U.S. patent number RE38,943 [Application Number 09/671,674] was granted by the patent office on 2006-01-24 for compound objective lens for optical disks having different thicknesses.
This patent grant is currently assigned to Matsushita Electric Industrial Co., Ltd.. Invention is credited to Yoshiaki Komma, Sadao Mizuno, Seiji Nishino.
United States Patent |
RE38,943 |
Komma , et al. |
January 24, 2006 |
**Please see images for:
( Certificate of Correction ) ** |
Compound objective lens for optical disks having different
thicknesses
Abstract
A compound objective lens is composed of a hologram lens or
transmitting a part of incident light without any diffraction to
form a beam of transmitted light and diffracting a remaining part
of the incident light to form a beam of first-order diffracted
light, and an objective lens for converging the transmitted light
to form a first converging spot on a front surface of a thin type
of first information medium and converging the diffracted light to
form a second converging spot on a front surface of a thick type of
second information medium. Because the hologram selectively
functions as a concave lens for the diffracted light, a curvature
of the transmitted light differs from that of the diffracted light.
Therefore, even though the first and second information mediums
have different thicknesses, the transmitted light incident on rear
surface of the first information medium is converged on the its
front surface, and the diffracted light incident on a rear surface
of the second information medium is converged on the its front
surface. That is, the compound objective lens has two focal
points.
Inventors: |
Komma; Yoshiaki (Osaka,
JP), Mizuno; Sadao (Osaka, JP), Nishino;
Seiji (Osaka, JP) |
Assignee: |
Matsushita Electric Industrial Co.,
Ltd. (Osaka, JP)
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Family
ID: |
27280636 |
Appl.
No.: |
09/671,674 |
Filed: |
September 27, 2000 |
Related U.S. Patent Documents
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Application
Number |
Filing Date |
Patent Number |
Issue Date |
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08190520 |
Feb 1, 1994 |
5446565 |
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Reissue of: |
08455934 |
May 31, 1995 |
05815293 |
Sep 29, 1998 |
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Foreign Application Priority Data
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Feb 1, 1993 [JP] |
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5-14432 |
Aug 4, 1993 [JP] |
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5-193353 |
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Current U.S.
Class: |
359/19; 359/565;
359/569; 359/570; 359/721; 359/743; 369/103; 369/112.05; 369/112.1;
369/112.12; 369/112.15; 369/44.23 |
Current CPC
Class: |
G02B
3/10 (20130101); G02B 5/18 (20130101); G02B
5/1814 (20130101); G02B 5/1842 (20130101); G02B
5/1871 (20130101); G02B 5/1876 (20130101); G02B
5/1895 (20130101); G02B 5/32 (20130101); G02B
21/025 (20130101); G02B 21/18 (20130101); G02B
21/20 (20130101); G02B 27/4238 (20130101); G03F
9/70 (20130101); G03F 9/7049 (20130101); G03F
9/7069 (20130101); G03F 9/7088 (20130101); G11B
7/08511 (20130101); G11B 7/131 (20130101); G11B
7/1353 (20130101); G11B 7/1374 (20130101); G11B
7/139 (20130101); G11B 19/12 (20130101); G11B
19/127 (20130101); G11B 2007/0006 (20130101); G11B
2007/13727 (20130101) |
Current International
Class: |
G02B
5/32 (20060101); G02B 7/00 (20060101); G02B
3/08 (20060101); G02B 3/10 (20060101); G11B
7/12 (20060101) |
Field of
Search: |
;359/19,565,569,570,571,574,575,721,743
;369/44.23,94,103,112.02,112.03,112.04,112.06,112.07,112.08,112.1,112.11,112.12,112.13,112.15,112.25,286 |
References Cited
[Referenced By]
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06 215406 |
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May 1994 |
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JP |
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06-325405 |
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Nov 1994 |
|
JP |
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Other References
"Optical Design with Diffractive Lenses" by D. Falkis, et al.,
Designer's Handbook; Photonics Spectra, Nov. 1991, pp. 205-208.
cited by examiner .
"Diffractive Lenses in Broadband Optical Design" by D. Falkis, et
al., Designer's Handbook; Photonics Spectra, Dec. 1991, pp.
131-134. cited by examiner .
"Sperical Grating Objective Lenses for Optical Disk Pick-Ups", K.
Goto, et al., Proc. Int. Symp. on Optical Memory, 1987; Japanese J.
Appl. Phys., vol. 26 (1987) Supplement 26-4, pp. 135-140. cited by
examiner .
"APO-Tele Lenses with Kinoform Elements" by M.A. Gan, et al., SPIE
vol. 1507 Holographic Optics III; Principles and Applications
(1991), pp. 116-125. cited by examiner .
"Design of Some Achromatic Imaging Hybrid Diffractive-Refractive
Lenses", by P. Twardowski, et al., SPIE vol. 1507 Holographic
Optics III; Principles and Applications (1991); pp. 55-56. cited by
examiner .
Applied Optics, vol. 29, No. 7, Mar. 1, 1990, New York, US, pp.
994-997; XP000101359, Ojeda-Castaneda & Berriel-Valdos "Zone
plate for arbitrarity high focal depth". cited by examiner.
|
Primary Examiner: Juba, Jr.; John
Attorney, Agent or Firm: Gopstein; Israel Clark &
Brody
Parent Case Text
CROSS-REFERENCE TO RELATED APPLICATIONS
This application is a continuation-in-part of U.S. Pat. application
Ser. No. 08/190,520, filed Feb. 1, 1994 now U.S. Pat. No.
5,446,565.
Claims
What is claimed is:
1. A compound objective lens, comprising: lens means, having a
first convex surface and a second convex surface opposite to each
other, for receiving a beam of incident light of one particular
wavelength passing through an optical axis at the first convex
surface, refracting the beam of incident light and emitting a beam
of refracted light from the second convex surface; and plural focal
point generating means for receiving the beam of incident light not
yet refracted by the lens means, generating from the beam of
incident light a plurality of beams of divided light including a
first beam of divided light and a second beam of divided light,
converging the beams of divided light at a plurality of focal
points which are placed on the optical axis on a side facing the
second convex surface of the lens means on condition that the first
beam of divided light transmits through a first substrate and is
converged on an information recording plane placed at a first
distance T1 from a surface of the first substrate at a diffraction
limit and that the second beam of divided light transmits through a
second substrate and is converged on an information recording plane
placed at a second distance T2 (T1.apprxeq.T2) from a surface of
the second substrate at a diffraction limit.
2. A compound objective lens according to claim 1 in which the
plural focal point generating means is a hologram generating from
the incident light as the beams of divided light a plurality of
beams of diffracted light having different diffraction orders.
3. A compound objective lens according to claim 2 in which the
first beam of divided light is a beam of transmitted light which
agrees with a beam of zero-order diffracted light generated by the
hologram, and the second beam of divided light is a beam of
first-order diffracted light generated by the hologram.
4. A compound objective lens according to claim 2 in which the
hologram is a phase modulation relief type of diffraction device, a
grating pattern of the hologram has a step-wise cross section and
is formed in a concentric circle shape, the grating pattern of the
hologram is concentrically partitioned into a plurality of blocks,
a phase modulation degree of the incident light passing through the
grating pattern of the hologram varies in a step-wise shape of four
stairs for each of the blocks, and a ratio of an etching width of a
top stair to a length of the corresponding block and another ratio
of an etching width of a bottom stair to the length of the
corresponding block are respectively lowered toward an outer
direction of the grating pattern of the hologram.
5. A compound objective lens according to claim 2 in which the
hologram is a phase modulation relief type of diffraction device, a
grating pattern of the hologram is formed in a concentric circle
shape and is concentrically partitioned into a plurality of blocks,
a phase modulation degree of the incident light passing through an
inner portion of the grating pattern of the hologram varies in a
step-wise shape of four inside stairs for each of the blocks, the
four inside stairs are composed of a top stair, a second stair, a
third stair and a bottom stair in that order, a ratio of an etching
width of the top stair to a length of the corresponding block and
another ratio of an etching width of the bottom stair to the length
of the corresponding block are respectively lowered toward an outer
direction of the grating pattern in the inner portion of the
hologram, another phase modulation degree of the incident light
passing through an outer portion of the grating pattern of the
hologram varies in a step-wise shape of two outside stairs for each
of the blocks, and a difference in width between the outside stairs
is increased toward the outer direction of the grating pattern in
the outer portion of the hologram.
6. A compound objective lens according to claim 2 in which the
hologram is a phase modulation relief type of diffraction device, a
grating pattern of the hologram has a step-wise cross section and
is formed in a concentric circle shape, the grating pattern of the
hologram is concentrically partitioned into a plurality of blocks,
a phase modulation degree of the incident light passing through the
grating pattern of the hologram varies in a step-wise shape of four
stairs for each of the blocks, and a ratio of an etching width of a
top stair to a length of the corresponding block and another ratio
of an etching width of a bottom stair to the length of the
corresponding block are respectively lowered toward an inner
direction of the grating pattern of the hologram.
7. A compound objective lens according to claim 2 in which the
hologram is a phase modulation relief type of diffraction device, a
grating pattern of the hologram is formed in a concentric circle
shape and is concentrically partitioned into a plurality of blocks,
a phase modulation degree of the incident light passing through an
outer portion of the grating pattern of the hologram varies in a
step-wise shape of four inside stairs for each of the blocks, the
four inside stairs are composed of a top stair, a second stair, a
third stair and a bottom stair in that order, a ratio of an etching
width of the top stair to a length of the corresponding block and
another ratio of an etching width of the bottom stair to the length
of the corresponding block are respectively lowered toward an inner
direction of the grating pattern in the outer portion of the
hologram, another phase modulation degree of the incident light
passing through an inner portion of the grating pattern of the
hologram varies in a step-wise shape of two inside stairs for each
of the blocks, and a difference in width between the inside stairs
is increased toward the inner direction of the grating pattern in
the inner portion of the hologram.
8. A compound objective lens according to claim 2 in which the
hologram is a phase modulation type of diffraction device and is
made of a liquid crystal cell.
9. A compound objective lens according to claim 2 in which the
hologram is a phase modulation type of diffraction device and is
placed on a substrate of a birefringence material.
10. A compound objective lens according to claim 2 in which a
positional relationship between the lens means and the hologram is
fixed.
11. A compound objective lens according to claim 10 in which the
hologram is formed on a lens surface of the lens means.
12. A compound objective lens according to claim 11 in which the
hologram is placed on a lens surface of the lens means of which a
curvature is higher than those of other lens surfaces of the lens
means.
13. A compound objective lens according to claim 11 in which the
hologram is placed on a lens surface of the lens means of which a
curvature is lower than those of other lens surfaces of the lens
means.
14. A compound objective lens according to claim 1 in which a
numerical aperture of the lens means for the incident light
converged at one focal point of the focal points differs from that
for the incident light converged at another focal point of the
focal points.
15. A compound objective lens according to claim 2 in which a
grating pattern is formed in a first portion of a light-passing
area of the hologram corresponding to an aperture of the lens
means, and any grating pattern is not formed in a second portion of
the light-passing area of the hologram.
16. A compound objective lens according to claim 15 in which a
phase of the incident light passing through the second portion of
the light-passing area of the hologram almost agrees with an
average value of phases of the incident light passing through the
first portion of the light-passing area of the hologram.
17. A compound objective lens according to claim 15 in which the
grating pattern is formed in a step-wise shape having a plurality
of stairs, a surface height of the second portion of the
light-passing area of the hologram in an optical direction is the
same as a height of a stair selected from the stairs except a top
stair and a bottom stair.
18. A compound objective lens according to claim 1 in which a
numerical aperture of the lens means is equal to or higher than
0.6.
.Iadd.19. A compound objective lens according to claim 1 in which
the focal points of the beams of divided light generated by the
plural focal point generating means correspond to focal positions
differing from each other in an optical axis
direction..Iaddend.
.Iadd.20. A compound objective lens according to claim 1 in which
two focal points selected from among the focal points of the beams
of divided light generated by the plural focal point generating
means correspond to two different positions from one of the first
and second substrates..Iaddend.
.Iadd.21. A compound objective lens according to claim 2 in which a
numerical aperture of the lens means for the incident light
converged at one focal point of the focal points differs from that
for the incident light converged at another focal point of the
focal points..Iaddend.
.Iadd.22. A compound objective lens according to claim 2 in which
the focal points generated by the hologram correspond to focal
positions differing from each other in an optical axis
direction..Iaddend.
.Iadd.23. A compound objective lens according to claim 2 in which
two focal points selected from among the focal points correspond to
two positions placed far from a substrate at two different
thicknesses..Iaddend.
.Iadd.24. A compound objective lens according to claim 2 in which a
numerical aperture of the lens means is equal to or higher than
0.6..Iaddend.
.Iadd.25. An image optical system, comprising: a light source for
radiating a beam of incident light of one particular wavelength;
lens means having a first convex surface and a second convex
surface opposite to each other, for receiving the beam of incident
light, which is radiated from the light source and passes through
an optical axis, at the first convex surface, refracting the beam
of incident light and emitting a beam of refracted light from the
second convex surface; and plural focal point generating means for
receiving the beam of incident light not yet refracted by the lens
means, generating from the beam of incident light a plurality of
beams of divided light including a first beam of divided light and
a second beam of divided light, converging the beams of divided
light at a plurality of focal points which are placed on the
optical axis on a side facing the second convex surface of the lens
means on condition that the first beam of divided light transmits
through a first substrate and is converged on an information
recording plane placed at a first distance T1 from a surface of the
first substrate at a diffraction limit and that the second beam of
divided light transmits through a second substrate and is converged
on an information recording plane placed at a second distance T2
(T1.apprxeq.T2) from a surface the second substrate at a
diffraction limit..Iaddend.
.Iadd.26. An image optical system according to claim 25 in which
the plural focal point generating means is a hologram..Iaddend.
.Iadd.27. An image optical system according to claim 26 in which a
plurality of beams of diffracted light having different diffraction
orders are generated from the incident light in the hologram, and
the beams of the diffracted light are converged at the focal points
in one-to-one correspondence..Iaddend.
.Iadd.28. An image optical system according to claim 27 in which a
beam of transmitted light which agrees with a beam of zero-order
diffracted light generated by the hologram is converged at a first
focal point of the focal points, and a beam of diffracted light
generated by the hologram is converged at a second focal point of
the focal points..Iaddend.
.Iadd.29. An image optical system according to claim 26 in which a
grating pattern is formed in the hologram in a concentric circle
shape..Iaddend.
.Iadd.30. A compound objective lens according to claim 26 in which
a positional relationship between the lens means and the hologram
is fixed..Iaddend.
.Iadd.31. An image optical system according to claim 30 in which
the hologram is formed on a lens surface of the lens
means..Iaddend.
.Iadd.32. An image optical system according to claim 31 in which
the hologram is placed on a lens surface of the lens means which
has a higher curvature than those of other lens surfaces of the
lens means and is placed at a position nearer than those of the
other lens surfaces of the lens means..Iaddend.
.Iadd.33. An image optical system according to claim 31 in which
the hologram is placed on a lens surface of the lens means which
has a lower curvature than those of other lens surfaces of the lens
means..Iaddend.
.Iadd.34. An image optical system according to claim 25 in which a
numerical aperture of the lens means for the incident light
converted at one focal point of the focal points differs from that
for the incident light converged at another focal point of the
focal points..Iaddend.
.Iadd.35. An image optical system according to claim 34 in which
the plural focal point generating means is a hologram..Iaddend.
.Iadd.36. An image optical system according m claim 35 in which a
grating pattern is formed in a first portion of a light-passing
area of the hologram corresponding to an aperture of the lens
means, and any grating pattern is not formed in a second portion of
the light-passing area of the hologram..Iaddend.
.Iadd.37. An image optical system according to claim 36 in which a
phase of the incident light passing through the second portion of
the light-passing area of the hologram almost agrees with an
average value of phases of the incident light passing through the
first portion of the light-passing area of the
hologram..Iaddend.
.Iadd.38. An image optical system according to claim 35 in which a
first diffraction efficiency of the hologram at a first region for
the incident light differs from a second diffraction efficiency of
the hologram at a second region for the incident
light..Iaddend.
.Iadd.39. An image optical system according to claim 25 in which a
far field pattern of the incident light radiated from the light
source is distributed to decrease an intensity of the incident
light toward a peripheral portion of the beam, an intensity of the
incident light passing through a central portion of the lens means
is two or more times that of the incident light passing through
peripheral portion of the lens mean..Iaddend.
.Iadd.40. An image optical system according to claim 25 in which
the focal points generated by the plural focal point generating
correspond to focal positions differing from each other in an
optical axis direction..Iaddend.
.Iadd.41. An image optical system according to claim 40 in which
the plural focal point generating means is a hologram..Iaddend.
.Iadd.42. An image optical system according to claim 25 in which
two focal points selected from among the focal points correspond to
two positions placed far from a substrate at two different
thicknesses..Iaddend.
.Iadd.43. An image optical system according to claim 42 in which
the plural focal point generating means is a hologram..Iaddend.
.Iadd.44. An optical head apparatus comprising: a light source for
radiating a beam or incident light of one particular wavelength;
lens means, having a first convex surface and a second convex
surface opposite to each other, for receiving the beam of incident
light, which is radiated from the light source and passes through
an optical axis, at the first convex surface, refracting the beam
of incident light and emitting a beam of refracted light from the
second convex surface; and plural focal point generating means for
receiving the beam of incident light not yet refracted by the lens
means, generating from the beam of incident light a plurality of
beams of divided light including a first beam of divided light and
a second beam of divided light converging the beams of divided
light at a plurality of focal points which are placed on the
optical axis on a side facing the second convex surface of the lens
means on condition that the first beam of divided light transmits
through a first substrate and is converged on an information
recording plane placed at a first distance T1 from a surface of the
first substrate at a diffraction limit and that the second beam of
divided light transmits through a second substrate and is converged
on an information recording plane placed at a second distance T2
(T1.apprxeq.T2) from a surface of the second substrate at a
diffraction limit; and a photo detector for receiving a plurality
of beams of reflected light obtained by reflecting the beams of
divided light converged on the information recording planes of the
substrates by the plural focal point generating means and
outputting an electric signal generated according to intensities of
the beans of reflected light..Iaddend.
.Iadd.45. An optical head apparatus according to claim 44 in which
the plural focal point generating means is a hologram..Iaddend.
.Iadd.46. An optical head apparatus according to claim 45 in which
a plurality of beams of diffracted light having different
diffraction orders are generated from the incident light in the
hologram and the beams of the diffracted light are converged at the
focal points in one-to-one correspondence..Iaddend.
.Iadd.47. An optical head apparatus according to claim 46 in which
a beam of transmitted light which agrees with a beam of zero-order
diffracted light generated by the hologram is converged at a first
focal point of the focal points, and a beam of diffracted light
generated by the hologram is convened at a second focal point of
the focal points..Iaddend.
.Iadd.48. An optical head apparatus according to claim 45 in which
the hologram is arranged on a plane, and an optical axis of the
lens means is not in parallel with a normal line of the
plane..Iaddend.
.Iadd.49. An optical head apparatus according to claim 45 in which
a positional relationship between the lens means and the hologram
is fixed..Iaddend.
.Iadd.50. An optical head apparatus according to claim 49 in which
the hologram is formed on a lens surface of the lens
means..Iaddend.
.Iadd.51. An optical head apparatus according to claim 50 in which
the hologram is placed on a lens surface of the lens means of which
a curvature is higher than those of other lens surfaces of the lens
means..Iaddend.
.Iadd.52. An optical head apparatus according to claim 50 in which
the hologram is placed on a lens surface of the lens means of which
a curvature is lower than those of other lens surfaces of the lens
means..Iaddend.
.Iadd.53. An optical head apparatus according to claim 45 in which
a grating pattern is formed in the hologram in a concentric circle
shape..Iaddend.
.Iadd.54. An optical head apparatus according to claim 53 in which
the grating pattern is formed in a first portion of a light-passing
area of the hologram corresponding to an aperture of the lens mean,
and another grating pattern is non-concentrically formed in a
second portion of the light-passing area of the hologram to
diffract the incident light..Iaddend.
.Iadd.55. An optical head apparatus according to claim 45 in which
the hologram is a phase modulation type of diffraction
device..Iaddend.
.Iadd.56. An optical head apparatus according to claim 55 in which
a phase modulation degree of light passing through the hologram is
lower than 2.pi. radians..Iaddend.
.Iadd.57. An optical head apparatus according to claim 55 in which
the hologram is a relief type of diffraction device..Iaddend.
.Iadd.58. An optical head apparatus according to claim 57 in which
a height H of relief formed in the hologram is set to:
H<.lamda./(n(.lamda.)-1), where a symbol .lamda. denotes a
wavelength of the incident light and a symbol n(.lamda.) denotes a
refractive index of a material of the hologram for the incident
light having the wavelength .lamda., and a difference in phase
modulation degree of the incident light passing through the
hologram is lower than 2.pi. radians..Iaddend.
.Iadd.59. An optical head apparatus according to claim 57 in which
a grating pattern of the hologram is formed in a step-wise cross
sectional shape..Iaddend.
.Iadd.60. An optical head apparatus according to claim 59 in which
the grating pattern of the hologram is formed in a concentric
circle shape and is concentrically partitioned into a plurality of
blocks, a phase modulation degree of the incident light passing
through the grating pattern of the hologram varies in a step-wise
shape of four stairs for each of blocks, and a ratio of an etching
width of a top stair to a length of the block and another ratio of
an etching width of a bottom stair to the length of the block are
respectively lowered toward an outer direction of the grating
pattern of the hologram..Iaddend.
.Iadd.61. An optical head apparatus according to claim 59 in which
the grating pattern of the hologram is formed in a concentric
circle shape and is concentrically partitioned into a plurality of
blocks, a phase modulation degree of the incident light passing
through an inner portion of the grating pattern of the hologram
varies in a step-wise shape of four inside stairs for each of
blocks, the four inside stairs are composed of a top stair, a
second stair, a third stair and a bottom stair in that order, a
ratio of an etching width of a top stair to a length of the block
and another ratio of an etching width of a bottom stair to the
length of the block are respectively lowered toward an outer
direction of the grating pattern in the inner portion of the
hologram, another phase modulation degree of the incident light
passing through an outer portion of the grating pattern of the
hologram varies in a step-wise shape of two outside stairs for each
of blocks, a height of an upper stair of the outside stairs agrees
with that of the second stair, a height of a lower stair of the
outside stairs agrees with that of the third stair, and a
difference in width between the upper and lower stairs is increased
toward the outer direction of the grating pattern in the outer
portion of the hologram..Iaddend.
.Iadd.62. An optical head apparatus according to claim 59 in which
the grating pattern of the hologram is formed in a concentric
circle shape and is concentrically partitioned into a plurality of
blocks, a phase modulation degree of the incident light passing
through the grating pattern of the hologram varies in a step-wise
shape of four stairs for each of blocks, and a ratio of an etching
width of a top stair to a length of the block and another ratio of
an etching width of a bottom stair to the length of the block are
respectively lowered toward an inner direction of the grating
pattern of the hologram..Iaddend.
.Iadd.63. An optical head apparatus according to claim 59 in which
the grating pattern of the hologram is formed in a concentric
circle shape and is concentrically partitioned into a plurality of
blocks, a phase modulation degree of the incident light passing
through an outer portion of the grating pattern of the hologram
varies in a step-wise shape of four outside stairs for each of
blocks, the four outside stairs are composed of a top stair, a
second stair, a third stair and a bottom stair in that order, a
ratio of an etching width of a top stair to a length of the block
and another ratio of an etching width of a bottom stair to the
length of the block are respectively lowered toward an inner
direction of the grating pattern in the outer portion of the
hologram, another phase modulation degree of the incident light
passing through an inner portion of the grating pattern of the
hologram varies in a step-wise shape of two inside stairs for each
of blocks, a height of an upper stair of the inside stairs agrees
with that of the second stair, a height of a lower stair of the
inside stairs agrees with that of the third stair; and a difference
in width between the upper and lower stairs is increased toward the
inner direction of the grating pattern in the inner portion of the
hologram..Iaddend.
.Iadd.64. An optical head apparatus according to claim 55 in which
the hologram a phase modulation type of diffraction device made of
a liquid crystal cell..Iaddend.
.Iadd.65. An optical head apparatus according to claim 55 in which
the hologram means is a phase modulation type of diffraction device
placed on a substrate made of a birefringence
material..Iaddend.
.Iadd.66. An optical head apparatus according to claim 44 in which
a numerical aperture of the lens means for the incident light
converged at one focal point of the focal points differs from that
fat the incident light converged at another focal point of the
focal points..Iaddend.
.Iadd.67. An optical head apparatus according to claim 66 in which
the plural focal point generating means is a hologram..Iaddend.
.Iadd.68. An optical head apparatus according to claim 67 in which
a grating pattern is formed in a first portion of a light-passing
area of the hologram corresponding to an aperture of the lens
means, and any grating pattern is not formed in a second portion of
the light-passing area of the hologram..Iaddend.
.Iadd.69. An optical head apparatus according to claim 68 in which
a phase of the incident light passing through the second portion of
the light-passing area of the hologram almost agrees with an
average value of phases of the incident light passing through the
first portion of the light-passing area of the
hologram..Iaddend.
.Iadd.70. An optical head apparatus according to claim 68 in which
the grating pattern is formed in a step-wise shape having a
plurality of stairs, a surface height of the second portion of the
light-passing area of the hologram in an optical axis direction is
the same as a height of a stair selected from the stairs except a
top stair and a bottom stair..Iaddend.
.Iadd.71. An optical head apparatus according to claim 67 in which
a first diffraction efficiency of the hologram at first region for
the incident light differs from a second diffraction efficiency of
the hologram at a second region for the incident
light..Iaddend.
.Iadd.72. An optical head apparatus according to claim 71 in which
a grating pattern of the hologram is concentrically formed, the
hologram is a phase modulation type of diffraction device, and a
phase modulation degree in an outer portion of the grating pattern
of the hologram is lower than that in an inner portion of the
grating pattern of the hologram..Iaddend.
.Iadd.73. An optical head apparatus according to claim 71 in which
a grating pattern of the hologram is concentrically formed, the
hologram is a phase modulation type of diffraction device, and a
phase modulation degree in an inner portion of the grating pattern
of the hologram is lower than that in an outer portion of grating
pattern of the hologram..Iaddend.
.Iadd.74. An optical head apparatus according to claim 44 in which
a far field pattern of the incident light radiated from the light
source is distributed to decrease an intensity of the incident
light toward a peripheral portion of the beam, an intensity of the
incident light passing through a central portion of the lens means
is two or more times that of the incident light passing through a
peripheral portion of the lens means..Iaddend.
.Iadd.75. An optical head apparatus according to claim 44 in which
the focal points generated by the plural focal point generating
means correspond to focal positions differing from each other in an
optical axis direction..Iaddend.
.Iadd.76. An optical head apparatus according to claim 75 in which
the plural focal point generating means is a hologram..Iaddend.
.Iadd.77. An optical head apparatus according to claim 44 in which
two focal points selected from among the focal points correspond to
two positions placed inside a substrate at two different
thicknesses..Iaddend.
.Iadd.78. An optical head apparatus according to claim 77 in which
the plural focal point generating means is a hologram..Iaddend.
.Iadd.79. An optical head apparatus according to claim 78 in which
the lens means converges a beam of transmitted light obtained by
passing the incident light through the hologram on an information
recording plane placed far from a substrate surface by a first
thickness T1, and the hologram converges a beam of diffracted light
obtained by diffracting the incident light in the hologram and
refracting the incident light in the lens means on another
information recording plane placed far from the substrate surface
by a second thickness T2(T1<T2)..Iaddend.
.Iadd.80. An optical head apparatus according to claim 78 in which
the hologram converges a beam of diffracted light obtained by
diffracting the incident light in the hologram and refracting the
incident light in the lens means on another information recording
plane placed far from the substrate surface by a first thickness
T1, and the lens means converges a beam of transmitted light
obtained by passing the incident light through the hologram on an
information recording plane placed far from a substrate surface by
a second thickness T2(T1<T2)..Iaddend.
.Iadd.81. An optical head apparatus according to claim 44 in which
the photo detector is arranged close to the light
source..Iaddend.
.Iadd.82. An optical head apparatus according to claim 44 in which
the incident light linearly polarized is radiated from the light
source, and the optical head apparatus, further comprising: a
polarized beam splitter for totally transmitting beam of light
linearly polarized in a first direction and totally reflecting a
beam of light linearly polarized at a second direction
perpendicular to the first direction; and a 1/4-.lamda. plate for
changing the light transmitting through or reflected by the
polarized beam splitter to a beam of light circularly polarized in
a rotational direction wherein the incident light linearly
polarized in a third direction agreeing with the first or second
direction is circularly polarized in a first rotational direction
by the 1/4-.lamda. plate, the light circularly polarized in the
first rotational direction is converged on the information mediums
by the lens means and the plural focal point generating means to
form a beam of light circularly polarized in a second rotational
direction opposite to the first rotational direction, the light
circularly polarized in the second rotational direction is changed
to the light linearly polarized in a fourth direction perpendicular
to the first direction by the 1/4-.lamda. plate, and the light
linearly polarized in the fourth direction is totally reflected by
or transmits through the polarized beam splitter to be incident on
the photo detector..Iaddend.
.Iadd.83. An optical head apparatus according to claim 44 in which
the photo deflector comprises: a servo signal detector for
detecting a servo signal included in one of the reflected light;
and another signal detector arranged at a periphery of the servo
signal detector for detecting another signal included in another
one of the reflected light..Iaddend.
.Iadd.84. An optical head apparatus according to claim 44 in which
the photo detector comprises: a signal detector for detecting a
focus error signal and a tracking error signal included in the
reflected light..Iaddend.
.Iadd.85. An optical head apparatus according to claim 44, further
comprising: reshaping means for reshaping the incident light
radiated from the light source, the incident light reshaped being
refracted by the lens means..Iaddend.
.Iadd.86. A compound objective lens, comprising a region to produce
a focal point on an information plane through a layer, wherein the
region of the lens is divided into a plurality of regions including
at least both of a first region and a second region by dividing the
region of the lens depending on differences in a distance from an
optical axis of the lens, the first region being located at a
position farther from the optical axis than a position of the
second region, the second region being optimized so that the lens
has a numerical aperture NA2 to produce a focal point through a
second layer on an information plane placed at a distance T2 from a
surface of the second layer, and both of the first region and the
second region being optimized so that the lens has a numerical
aperture NA1 (NA1 is not equal to NA2) to produce a focal point
through a first layer on an information plane placed at a distance
T1 (T1 is not equal to T2) from the surface of the first layer,
wherein the compound objective lens has a first convex surface and
a second convex surface opposite to each other, for receiving a
beam of incident light of one particular wavelength passing through
the optical axis at the first convex surface, and the compound
objective lens refracts the beam of incident light and emits a beam
of refracted light from the second convex surface, and the region
of the lens receives the beam of incident light not yet refracted
by the lens and generates from the incident light a plurality of
beams of divided light, and generates a plurality of focal points
which are placed on the optical axis on a side facing the second
convex surface..Iaddend.
.Iadd.87. A compound objective lens according to claim 86, wherein
the second region has an optical relief, the numerical aperture NA1
is larger than the numerical aperture NA2, and the distance T1 is
smaller than the distance T2..Iaddend.
.Iadd.88. A compound objective lens according to claim 87, in which
the optical relief is formed concentrically in the second region of
the compound objective lens..Iaddend.
.Iadd.89. A compound objective lens according to claim 87, in which
the optical relief is provided on a side of the compound objective
lens opposite to an optical disk..Iaddend.
.Iadd.90. A compound objective lens according to claim 87, in which
the first region has an optical relief formed therein..Iaddend.
.Iadd.91. A compound objective lens according to claim 90, in which
the optical relief of the first region is higher in height than the
optical relief of the second region..Iaddend.
.Iadd.92. A compound objective lens according to claim 87,
comprising an objective lens on which the plurality of regions are
provided..Iaddend.
.Iadd.93. A compound objective lens according to claim 87,
comprising an objective lens and a relief lens on which the
plurality of regions are provided..Iaddend.
.Iadd.94. A compound objective lens according to claim 87, in which
the distance T1 is larger than 0.4 millimeter and smaller than 0.8
millimeter..Iaddend.
.Iadd.95. A compound objective lens according to claim 87, in which
a height H of the optical relief formed in the second region is set
to: H<.lamda./(,(.lamda.)-1), where a symbol .lamda. denotes a
wavelength of a light beam passing through the second region and a
symbol n(.lamda.) denotes a refractive index of a material of the
optical relief at the wavelength .lamda. of the light
beam..Iaddend.
.Iadd.96. A compound objective lens according to claim 95, in which
a difference in phase modulation degree of the light beam passing
through the second region is lower than 2.pi. radian..Iaddend.
.Iadd.97. A compound objective lens according to claim 87, in which
the optical relief of the second region is a hologram..Iaddend.
.Iadd.98. A compound objective lens according to claim 97, in which
the hologram of the second region has a diffraction efficiency
lower than 100%..Iaddend.
.Iadd.99. A compound objective lens according to claim 97, in which
the hologram of the second region is formed to function as a convex
lens..Iaddend.
.Iadd.100. A compound objective lens according to claim 97, in
which the hologram of the second region has slopes inclining to the
same direction as a surface of a convex lens..Iaddend.
.Iadd.101. A compound objective lens according to claim 97, in
which the plurality of regions include at least one region having
no optical hologram..Iaddend.
.Iadd.102. A compound objective lens according to claim 101, in
which the first region has no hologram..Iaddend.
.Iadd.103. A compound objective lens according to claim 97, in
which the first region has a hologram..Iaddend.
.Iadd.104. A compound objective lens according to claim 103, in
which the first region is higher in a diffraction efficiency than
the second region..Iaddend.
.Iadd.105. A compound objective lens according to claim 97, in
which the hologram of the second region is formed into a blazed
hologram lens..Iaddend.
.Iadd.106. A compound objective lens according to claim 105, in
which the hologram is formed into saw-teeth in a section
thereof..Iaddend.
.Iadd.107. An optical head apparatus for performing at least one of
recording and reproduction of pieces of information on and from an
optical disk placed to face the optical head apparatus, comprising
(i) an optical source for radiating a light beam; and (ii) a
compound objective lens receiving the light beam and comprising a
region to produce a focal point on an information plane through a
layer, wherein the region of the lens is divided into a plurality
of regions including at least both of a first region and a second
region by dividing the region of the lens depending on differences
in a distance from an optical axis of the lens, the first region
being located at a position farther from the optical axis than a
position of the second region, the second region being optimized so
that the lens has a numerical aperture NA2 to produce a focal point
through a second layer on an information plane placed at a distance
T2 from a surface of the second layer, and both of the first region
and the second region being optimized so that the lens has a
numerical aperture NA1 (NA1 is not equal to NA2) to produce a focal
point through a first layer on an information plane placed at a
distance T1 (T1 is not equal to T2) from the surface of the first
layer, wherein the compound objective lens has a first convex
surface and a second convex surface opposite to each other, for
receiving a beam of incident light of one particular wavelength
passing through the optical axis at the first convex surface, and
the compound objective lens refracts the beam of incident light and
emits a beam of refracted light from the second convex surface, and
the region of the lens receives the beam of incident light not yet
refracted by the lens, and generates from the incident light a
plurality of beams of divided light, and generates a plurality of
focal points which are placed on the optical axis on a side facing
the second convex surface..Iaddend.
.Iadd.108. An optical head apparatus according to claim 107,
comprising: a collimate lens to change the light beam from the
optical source into an approximately parallel light; and an optical
detector to receive light from both of the information planes
placed at a distance T1 from the surface of the first layer and
placed at a distance T2 from the surface of the second layer;
wherein the compound objective lens receives the approximately
parallel light..Iaddend.
.Iadd.109. An optical head apparatus according to claim 107 wherein
the numerical aperture NA1 is larger than the numerical aperture
NA2 (NA1>NA2) and the distances T1 and T2 correspond to
thicknesses T1 and T2 of the first and second layers composed of,
respectively, first and second information media included in the
optical disk, the thickness T1 being smaller the thickness T2
(T1<T21)..Iaddend.
.Iadd.110. An optical head apparatus according to claim 109,
comprising: a photo detector for detecting the light beam, which is
converged at an information recording plane, serving as the
information plane, of the first information medium having the
thickness T1 and at an information recording plane, serving as the
information plane, of the second information medium having the
thickness T2 by the compound objective lens and is reflected by the
first information medium and the second information medium,
respectively, to obtain first information recorded in the
information recording plane of the first information medium and
second information recorded in the information recording plane of
the second information medium..Iaddend.
.Iadd.111. An optical head apparatus according to claim 109, in
which the compound objective lens comprises an optical device for
minimizing an aberration occurring in the light beam in cases where
the light beam passing through the optical device transmits through
the first layer of the first information medium having the
thickness T1 and is focused on an information recording plane,
serving as the information plane, of the first information medium,
and a ring-shaped band, placed on at least one surface of the
optical device, for shifting a phase of the light beam passing
through the optical device to reduce a wavefront aberration caused
by a difference between the thicknesses T1 and T2 of the first and
second information media in cases where the light beam passing
through the optical device transmits through the second layer of
the second information medium having the thickness T2 and is
focused on an information recording plane, serving as the
information plane of the second information medium; the optical
head apparatus further comprising a photo detector for detecting
the light beam which is converged on the information recording
plane of the first information medium having the thickness T1 and
on the information recording plane of the second information medium
having the thickness T2 by the compound objective lens and is
reflected by the first information medium and second information
medium to reproduce information recorded in the first and second
information media, respectively..Iaddend.
.Iadd.112. An optical head apparatus according to claim 109, in
which the compound objective lens comprises a phase adjusting
device, formed in a ring-band shape, for shifting a part of the
light beam radiated from the optical source, the compound objective
lens having a light converging performance so as to converge the
light beam radiated from the optical source on an information
recording plane serving as the information plane of the first
information medium having the thickness T1 through the layer
thereof at a diffraction limit, to converge the light beam, of
which the part is shifted by the phase adjusting device, on an
information recording-plane, serving as the information plane, of
the second information medium having the thickness T2 or the
information recording plane of the first information medium having
the thickness T1 through the layer thereof, the optical head
apparatus further comprises a photo detector for detecting the
light beam, which is converged on the information recording plane
of the first and second information media each having the thickness
T1 or T2 by the compound objective lens and is reflected by the
first and second information media, respectively, to reproduce
information recorded in the first and second information media,
respectively..Iaddend.
.Iadd.113. An optical head apparatus according to claim 109, in
which the plurality of regions of the compound objective lens
include a third region, corresponding to a numerical aperture NA4
equal to or lower than the numerical aperture NA2 (NA4<NA2), for
changing the light beam radiated from the optical source to
converge the light beam on an information recording plane, serving
as the information plane, of the second information medium having
the thickness T2 through the layer thereof; and a photo detector
for detecting the beam light, which is converged on the information
recording plane of the first information medium having the
thickness T1 and on an information recording plane serving as the
information plane, of the second information medium having the
thickness T2 by the compound objective lens and is reflected by the
first and second information media having the thickness T1 and T2
respectively, to reproduce first information recorded in the first
information medium and second information recorded in the second
information medium, respectively..Iaddend.
.Iadd.114. An optical disk apparatus, comprising; (1) an optical
head apparatus for performing at least one of recording and
reproduction of pieces of information on and from an optical disk
placed to face the optical head apparatus, comprising: (i) an
optical source for radiating a light beam; and (ii) a compound
objective lens receiving the light beam and comprising: a region to
produce a focal point on an information plane through a layer,
wherein the region of the lens is divided into a plurality of
regions including, at least both of a first region and a second
region by dividing the region of the lens depending on differences
in a distance from an optical axis of the lens, the first region
being located at a position farther from the optical axis than a
position of the second region, the second region being optimized so
that the lens has a numerical aperture NA2 to produce a focal point
through a second layer on an information plane placed at a distance
T2 from a surface of the second layer, and both of the first region
and the second region being optimized so that the lens has a
numerical aperture NA1 (NA1 is not equal to NA2) to produce a focal
point through a first layer on an information plane placed at a
distance T1 (T1 is not equal to T2) from the surface of the first
layer, and wherein the compound objective lens has a first convex
surface and a second convex surface opposite to each other, for
receiving a beam of incident light of one particular wavelength
passing through the optical axis at the first convex surface, and
the compound objective lens refracts the beam of incident light and
emits a beam of refracted light from the second convex surface, and
the region of the lens receives the beam of incident light not yet
refracted by the lens, and generates from the incident light a
plurality of beams of divided light, and generates a plurality of
focal points which are placed on the optical axis on a side facing
the second convex surface; (2) a moving apparatus for moving the
optical head apparatus; and (3) a rotating apparatus for rotating
the optical disk..Iaddend.
.Iadd.115. An optical disk apparatus according to claim 114,
comprising: a focus controller to change a distance between the
optical disk and the compound objective lens and start focus
control when a focus error signal detected from the compound
objective lens surpasses a predetermined level so as to perform
focus control corresponding to the different distances T1 and
T2..Iaddend.
.Iadd.116. An optical disk apparatus according to claim 114,
wherein the numerical aperture NA1 is larger than the numerical
aperture NA2 (NA1>NA2) and the distances T1 and T2 correspond to
thicknesses T1 and T2 of the first and second layers composed of,
respectively, first and second information media included in the
optical disk, the thickness T1 being smaller the thickness T2
(T1<T2)..Iaddend.
.Iadd.117. An optical disk apparatus according to claim 116,
wherein the optical head apparatus is configured, through the
compound objective lens, to read an information signal, a focus
error signal and a tracking error signal from the optical disk
rotated by the rotating apparatus; the optical disk apparatus
further comprising: connecting means for connecting the rotating
apparatus and the moving apparatus with an electric source to
supply an electric power to the rotating apparatus and the moving
apparatus; actuating means for actuating the compound objective
lens of the optical head apparatus; focus control means for
controlling the actuating means to perform a first focus control of
the optical head apparatus corresponding to the thickness T1 of the
first information medium and a second focus control of the optical
head apparatus corresponding to the thickness T2 of the second
information medium according to the focus error signal read by the
optical head apparatus; tracking control means for controlling the
actuating means to perform a first tracking control of the optical
head apparatus corresponding to the thickness T1 of the first
information medium and a second tracking control of the optical
head apparatus corresponding to the thickness T2 of the second
information medium according to the tracking error signal read by
the optical head apparatus; detecting means for detecting whether
the optical disk has the first information medium having the
thickness T1 or the second information medium having the thickness
T2; and changing means for switching from the second focus and
tracking controls performed by the focus control means and the
tracking control means to the first focus and tracking controls
performed by the focus control means and the tracking control means
according to the detection of the detecting means..Iaddend.
.Iadd.118. An optical disk apparatus according to claim 116, in
which the optical head apparatus is configured, through the
compound objective lens, to read an information signal, a focus
error signal and a tracking error signal from the optical disk
rotated by the rotating apparatus; the optical disk apparatus
further comprising: connecting means for connecting the rotating
apparatus and the moving apparatus with an electric source to
supply an electric power to the rotating apparatus and the moving
apparatus; actuating means for actuating the compound objective
lens of the optical head apparatus; focus control means for
controlling the actuating means to perform a first focus control of
the optical head apparatus corresponding to the thickness T1 of the
first information medium and a second focus control of the optical
head apparatus corresponding to the thickness T2 of the second
information medium according to the focus error signal read by the
optical head apparatus; and tracking control means for controlling
the actuating means to perform a first tracking control of the
optical head apparatus corresponding to the thickness T1 of the
first information medium and a second tracking control of the
optical head apparatus corresponding to the thickness T2 of the
second information medium according to the tracking error signal
read by the optical head apparatus..Iaddend.
.Iadd.119. An optical disk apparatus according to claim 118 in
which the compound objective lens of the optical head apparatus is
moved in a direction to the optical disk by the moving apparatus,
and the compound objective lens of the optical head apparatus is
operated to focus the light beam on the first or second information
medium by the actuating means under the control of the focus
control means to decrease an intensity of the focus error signal to
zero in case where the intensity of the focus error signal exceeds
a threshold..Iaddend.
.Iadd.120. An optical disk apparatus according to claim 116,
comprising: a photo detector for detecting the light beam which is
converged at an information recording plane, serving as the
information plane, of the first information medium having the
thickness T1 and at an information recording plane, serving as the
information plane, of the second information plane having the
thickness T2 by the compound objective lens and is reflected by the
first information medium and the second information medium,
respectively; focus control means for performing a first focus
control of the optical head apparatus corresponding to the
thickness T1 of the and a second focus control of the optical head
apparatus corresponding to the thickness T2 according to the light
beam detected by the photo detector; tracking control means for
performing a first tracking control of the optical head apparatus
corresponding to the thickness T1 and a second tracking control of
the optical head apparatus corresponding to the thickness T2
according to the light beam detected by the photo detector; and
information detecting means for judging according to the light beam
detected by the photo detector, for which the first focus control
and the second focus control and the first tracking control and the
second tracking control are performed, whether the light beam
radiated from the light source is converged at the information
recording plane of the first information medium having the
thickness T1 or at the information recording plane of the second
information medium having the thickness T2, reproducing first
information recorded in the information recording plane of the
first information medium from the light beam detected by the photo
detector in cases where it is judged that the light beam is
converged at the information recording plane of the first
information medium, and reproducing second information recorded in
the information recording plane of the second information medium
from the light beam detected by the photo detector in cases where
it is judged that the light beam is converged at the information
recording plane of the second information medium..Iaddend.
.Iadd.121. An optical disk apparatus according to claim 116, in
which the plurality of regions of the compound objective lens
include: a third region which corresponds to a numerical aperture
NA3 satisfying a relationship of NA2.ltoreq.NA3<NA1 and is
unified with the first region of the objective lens through a
discontinuous plane, the optical head apparatus further comprising:
a photo detector for detecting the light beam which is converged at
an information recording plane, serving as the information plane,
of the first information medium having the thickness T1 and at an
information recording plane, serving as the information plane, of
the second information medium having the thickness T2 by the
compound objective lens and is reflected therefrom, respectively;
focus control means for performing a first focus control of the
optical head apparatus corresponding to the thickness T1 and a
second focus control of the optical head apparatus corresponding to
the thickness T2 according to the light beam detected by the photo
detector; tracking control means for performing a first tracking
control of the optical head apparatus corresponding to the
thickness T1 and a second tracking control of the optical head
apparatus corresponding to the thickness T2 according to the light
beam detected by the photo detector; and information detecting
means for judging according to the light beam detected by the photo
detector, for which the first focus control and the second focus
control and the first tracking control and the second tracking
control are performed, whether the light beam radiated from the
optical source is converged at the information recording plane of
the first or second information medium having either of the
thickness T1 or T2, reproducing first information recorded in the
information recording plane of the first information medium having
the thickness T1 from the light beam detected by the photo detector
in cases where it is judged that the light beam is converged at the
information recording plane of the first information medium, and
reproducing second information recorded in the information
recording plane of the second information medium having the
thickness T2 from the light beam detected by the photo detector in
cases where it is judged that the light beam is converged at the
information recording plane of the second information
medium..Iaddend.
.Iadd.122. An optical disk apparatus according to claim 116, in
which the optical head apparatus comprises an optical device for
minimizing an aberration occurring in the light beam in cases where
the light beam passing through the optical device transmits through
the layer of the first information medium having the thickness T1
and is focused on an information recording plane, serving as the
information plane, of the first information medium, a ring-shaped
band, placed on at least one surface of the optical device, for
shifting a phase of the light beam passing through the optical
device to reduce a wavefront aberration caused by a difference
between the thicknesses T1 and T2 of the first and second
information media in cases where the light beam passing through the
optical device transmits through the layer of the second
information medium having the thickness T2 and is focused on the
information recording plane thereof, and a photo detector for
detecting the light beam, which is converged on the information
recording planes of the first and second information media having
the thicknesses T1 and T2 by the compound objective lens and is
reflected by the first and second information media, respectively,
to reproduce information recorded in the first and second
information media, respectively; focus control means for performing
a first focus control of the optical head apparatus corresponding
to the thickness T1 of the first information medium and a second
focus control of the optical head apparatus corresponding to the
thickness T2 of the second information medium according to the
light beam detected by the photo detector; tracking control means
for performing a first tracking control of the optical head
apparatus corresponding to the thickness T1 and a second tracking
control of the optical head apparatus corresponding to the
thickness T2 according to the light beam detected by the photo
detector; and information detecting means for judging according to
the light beam detected by the photo detector, for which the first
focus control and the second focus control and the first tracking
control and the second tracking control are performed, whether the
light beam radiated from the optical source is converged at an
information recording plane, serving as the information plane, of
the first or second information medium having the thickness T1 or
T2 reproducing first information recorded in the information
recording plane of the first information medium having the
thickness T1 from the light beam detected by the photo detector in
cases where it is judged that the light beam is converged at the
information recording plane of the first information medium, and
reproducing second information recorded in the information
recording plane of the second information medium having the
thickness T2 from the light beam detected by the photo detector in
cases where it is judged that the light beam is converged at the
information recording plane of the second information
medium..Iaddend.
.Iadd.123. An optical disk apparatus according to claim 116, in
which the plurality of regions of the compound objective lens
include a third region, corresponding to a numerical aperture NA4
equal to or lower than the numerical aperture NA2 (NA4<NA2), for
changing the light beam radiated from the optical source to
converge the light beam on an information recording plane, serving
as the information plane, of the second information medium having
the thickness T2 through the layer thereof; a photo detector for
detecting the light beam, which is converged on the information
recording plane of the first and second information media each
having the thickness T1 or T2 by the compound objective lens and is
reflected by the first and second information media, respectively,
to reproduce information recorded in the first and second
information media, respectively; focus control means for performing
a first focus control of the optical head apparatus corresponding
to the thickness T1 of the first information medium and a second
focus control of the optical head apparatus corresponding to the
thickness T2 of the second information medium according to the
light beam detected by the photo detector; tracking control means
for performing a first tacking control of the optical head
apparatus corresponding to the thickness T1 of the first
information medium and a second tracking control of the optical
head apparatus corresponding to the thickness T2 of the second
information medium according to the light beam detected by the
photo detector; and information detecting means for judging
according to the light beam detected by the photo detector, for
which the first focus control and the second focus control and the
first tracking control and the second tracking control are
performed, whether the light beam radiated from the optical source
is converged at an information recording plane, serving as the
information plane, of the first information medium having the
thickness T1 or at an information recording plane, serving as the
information plane, of the second information medium having the
thickness T2, reproducing first information recorded in the
information recording plane of the first information medium from
the light beam detected by the photo detector in cases where it is
judged that the light beam is converged at the information
recording plane of the first information medium, and reproducing
second information recorded in the information recording plane of
the second information medium from the light beam detected by the
photo detector in cases where it is judged that the light beam is
converged at the information recording plane of the second
information medium..Iaddend.
Description
BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention relates to a compound objective lens composed
of an objective lens and a hologram lens which has two focal
points, an imaging optical system for converging light on two
converging spots placed at different depths of an information
medium with the compound objective lens, an optical head apparatus
for recording, reproducing or erasing information on or from an
information medium such as an optical medium or a magneto-optical
medium like an optical disk or an optical card with the imaging
optical system, an optical disk in which a series of high density
recording pits and a series of comparatively low density recording
pits are provided, an optical disk apparatus for recording or
reproducing information on or from the optical disk with the
compound objective lens, a binary focus microscope having two focal
points in which two types of images drawn at different depths are
simultaneously observed, and an alignment apparatus for aligning
two types of images drawn at different depths with the binary focus
microscope.
2. Description of the Related Art
An optical memory technique has been put to practical use to
manufacture an optical disk in which a pit pattern formed of a
series of pits is drawn to record information. The optical disk is
utilized as a high density and large capacity of information
medium. For example, the optical disk is utilized for a digital
audio disk, a video disk, a document file disk, and a data file
disk. To record information on the optical disk and to reproduce
the information from the optical disk, a light beam radiated from a
light source is minutely converged in an imaging optical system,
and the light beam minutely converged is radiated to the optical
disk through the imaging optical system. Therefore, the light beam
is required to be reliably controlled in the imaging optical system
with high accuracy.
The imaging optical system is utilized for an optical head
apparatus in which a detecting system is additionally provided to
detect the intensity of the light beam reflected from the optical
disk. Fundamental functions of the optical head apparatus are
classified into a converging performance for minutely converging a
light beam to form a diffraction-limited micro-spot of the light
beam radiated on the optical disk, a focus control in a focus servo
system, a tracking control in a tracking serve system, and the
detection of pit signals (or information signals) obtained by
radiating the light beam on a pit pattern of the optical disk. The
fundamental function of the optical head apparatus is determined by
the combination of optical sub-systems and a photoelectric transfer
detecting process according to a purpose and a use. Specifically,
an optical head apparatus in which a holographic optical element
(or hologram) is utilized to minimize and thin the optical head
apparatus has been recently proposed.
2.1. Previously Proposed Art
FIG. 1 is a constitutional view of a conventional optical head
apparatus proposed in Japanese Patent Application No. 46630 of 1991
which is applied by inventors of the present invention.
As shown in FIG. 1, a conventional optical head apparatus 11 for
recording or reproducing information on or from an information
medium 12 such as an optical disk is provided with a light beam
source 13 such as a semiconductor laser, a transmission type of
blazed hologram 14 for transmitting a light beam L1 radiated from
the light beam source 12 without any diffraction in an outgoing
optical path and diffracting a light beam L2 reflected on the
information medium 12 in a returning optical path, an objective
lens 15 for converging the light beam L1 transmitting through the
hologram 13 on the information medium 14 to read the information,
an actuator 16 for integrally moving the objective lens 15 with the
blazed hologram 13 to focus the light beam L1 on the information
medium 12 with the objective lens 15, and a photo detector 17 for
detecting the intensity of the light beam L2 reflected on the
information medium 12 to reproduce the information.
As shown in FIG. 2A, a relative position between the blazed
hologram 14 and the objective lens 15 is fixed by a fixing means
18. Or, as shown in FIG. 2B, a blazed pattern is formed on a side
of the objective lens 15 to integrally form the blazed hologram 14
with the objective lens 15.
In the above configuration, a light beam L1 (or a laser beam)
radiated from the light beam source 13 is radiated to the blazed
hologram 14, and the light beam L1 mainly transmits through the
blazed hologram 14 without any diffraction in an outgoing optical
path. The light beam L1 transmitting through the blazed hologram 14
is called zero-order diffracted light. Thereafter, the zero-order
diffracted light L1 is converged on the information medium 12 by
the objective lens 15. In the information medium 12, information
indicated by a series of patterned pits is recorded and read by the
zero-order diffracted light L1. Thereafter, a beam light L2 having
the information is reflected toward the objective lens 15 in a
returning optical path and is incident to the blazed hologram 14.
In the blazed hologram 14, the light L2 is mainly diffracted. The
light L2 diffracted is called first-order diffracted light.
Thereafter, the first-order diffracted light L2 is received in the
photo detector 17.
In the photo detector 17, the intensity distribution of the
first-order diffracted light L2 is detected. Therefore, a servo
signal for adjusting the position of the objective lens 15 by the
action of the actuator 16 is obtained. Also, the intensity of the
first-order diffracted light L2 is detected in the photo detector
17. Because the information medium 12 is rotated at high speed, the
patterned pits radiated by the light 17 are changed so that the
intensity of the first-order diffracted light L2 detected is
changed. Therefore, an information signal indicating the
information recorded in the information medium 12 is obtained by
detecting the change in intensity of the first-order diffracted
light L2.
In the above operation, a part of the light beam L1 is necessarily
diffracted in the blazed hologram 14 when the light beam L1 is
radiated to the blazed hologram 14 in the outgoing optical path.
Therefore, unnecessary diffracted light such as first-order
diffracted light and minus first-order diffracted light necessarily
occurs. In cases where the hologram 14 is not blazed, the
unnecessary diffracted light in the outgoing optical path also
reads the information recorded in the information medium 12, and
the unnecessary light is undesirably received in the photo detector
17. To prevent the unnecessary light from transmitting to the
information medium 12, the blazed hologram 14 is manufactured to
form a blazed hologram pattern on the surface thereof, so that the
intensity of the unnecessary light received in the photo detector
17 is decreased.
Also, because an objective lens of a conventional microscope has
only a focal point, images placed within a focal depth of the
objective lens can be only observed with the conventional
microscope.
Also, a minute circuit is formed on a semiconductor such as a group
III-V compound semiconductor to form a microwave circuit, an
opto-electronic detector or a solid state laser. In this case, a
photo-sensitive material is coated on a sample made of the
semiconductor. Thereafter, a relative position between the sample
and a photo mask covering the sample is adjusted by utilizing an
alignment apparatus, and the photo-sensitive material is exposed by
a beam of exposure light through the photo mask to transfer a
circuit pattern drawn on the photo mask to the photo-sensitive
material in an exposure process by utilizing an exposure apparatus.
For example, an alignment pattern is drawn on a reverse side of the
sample, and a relative position between the sample and the photo
mask is adjusted with high accuracy while simultaneously observing
the alignment pattern of the sample and the circuit pattern of the
photo mask with the conventional microscope. Thereafter, the
circuit pattern of the photo mask is transferred to a front side of
the sample.
In this case, because images placed within a focal depth of an
objective lens utilized in the conventional microscope can be only
observed with the conventional microscope, it is required to
utilize the conventional microscope having a deep focal depth in
the alignment apparatus in cases where the alignment pattern and
the circuit pattern are simultaneously observed with the
conventional microscope. Therefore, the magnification of the
conventional microscope having a deep focal depth is lowered.
2.2. Problems to be Solved by the Invention
An optical disk having a high density memory capacity has been
recently developed because of the improvement in a design technique
of an optical system and the shortening of the wavelength of light
radiated from a semiconductor laser. For example, a numerical
aperture at an optical disk side of an imaging optical system in
which a light beam converged on an optical disk is minutely
narrowed in diameter is enlarged to obtain the optical disk having
a high density memory capacity. In this case, the degree of
aberration occurring in the imaging optical system is increased
because an optical axis of the system tilts from a normal line of
the optical disk. As the numerical aperture is increased, the
degree of the aberration is enlarged. To prevent the increase of
the numerical aperture, it is effective to thin the thickness of
the optical disk. The thickness of the optical disk denotes a
distance from a surface of the optical disk (or an information
medium) radiated by a light beam to an information recording plane
on which a series of patterned pits are formed.
FIG. 3 shows a relationship between the thickness of the optical
disk and the numerical aperture on condition that the tilt of the
optical axis is constant.
As shown in FIG. 3, because the numerical aperture is 0.5 when the
thickness of the optical disk is 1.2 mm, it is effective to thin
the optical disk to 0.6 mm in thickness when the numerical aperture
is increased to 0.6. In this case, even though the numerical
aperture is increased on condition that the tilt of the optical
axis is not changed, the degree of the aberration is not increased.
Therefore, it is preferred that the thickness of the optical disk
be thinned to obtain the optical disk having a high density memory
capacity.
Accordingly, it is expected that the thickness of a prospective
optical disk having a high density memory capacity becomes thinner
than that of a present optical disk such as a compact disk
appearing on the market now. For example, the thickness of the
compact disk is about 1.2 mm, and the thickness of the prospective
optical disk is expected to range from 0.4 mm to 0.8 mm. In this
case, it is required to record or reproduce information on or from
an optical disk with an optical head system regardless of whether
the optical disk is the present optical disk or the prospective
optical disk having a high density memory capacity. That is, an
optical head apparatus having an imaging optical system in which a
light beam is converged on an optical disk within the diffraction
limit regardless of whether the optical disk is thick or thin is
required.
However, in a conventional optical head apparatus, a piece of
information is only recorded or reproduced on or from an optical
disk having a fixed thickness. For example, in cases where the
thickness of the information medium 12 is off a regular range by
about .+-.0.1 mm or more, an aberration such as a spherical
aberration occurs when the optical head apparatus 11 is operated.
Therefore, the recording or the reproduction of the information is
impossible. Accordingly, there is a drawback that an optical head
apparatus in which a piece of information is recorded or reproduced
on or from an optical disk regardless of whether the optical disk
is the present optical disk or the prospective optical disk having
a high density memory capacity cannot be manufactured in a
conventional technique.
Also, there is a problem in the conventional microscope. That is,
because an objective lens of the conventional microscope has only a
focal point and images placed within a focal depth of the objective
lens can be only observed with the conventional microscope, the
magnification of the conventional microscope and an observed range
in an optical axis direction are in a trade-off relationship.
Therefore, there is a drawback that it is impossible to observe the
images over a wide observed range in the optical axis direction at
high magnification
Also, there is a problem in the alignment apparatus. That is, when
a circuit pattern drawn on the photo mask is transferred to the
front side of the sample after an alignment pattern is drawn on the
reverse side of the sample, the alignment of the photomask and the
sample is performed by simultaneously observing the circuit pattern
of the photo mask and the alignment pattern of the sample with the
conventional microscope having a deep focal depth and a low
magnification. Therefore, because the conventional microscope has a
low magnification, there is a drawback that it is impossible to
align the photo mask with the sample at a high accuracy ranging
within 5 .mu.m.
SUMMARY OF THE INVENTION
A first object of the present invention is to provide, with due
consideration to the drawbacks of such a conventional objective
lens having a focal point, a compound objective lens having two
focal points.
A second object of the present invention is to provide an imaging
optical system having the compound objective lens in which light
transmitting through the compound objective lens is converged at a
diffraction limit on two converging spots placed at different
depths of an information medium.
A third object of the present invention is to provide an optical
head apparatus having the imaging optical system in which
information is recorded, reproduced or erased on or from one of the
converging spots of the information medium at which light is
converged by the action of the imaging optical system.
A fourth object of the present invention is to provide a high
density optical disk in which a series of first recording pits is
formed to record pieces of information at high density on a thin
substrate.
A fifth object of the present invention is to provide an optical
disk apparatus in which information is recorded or reproduced on or
from the optical disk with the compound objective lens regardless
of whether a series of recording pits expressing pieces of
information is recorded or reproduced on or from the high density
optical disk having a thin thickness or a conventional compact disk
having an ordinary thickness.
A sixth object of the present invention is to provide a binary
focus microscope having two focal points in which two types of
images drawn at different depths are simultaneously observed.
A seventh object of the present invention is to provide an
alignment apparatus in which two types of images drawn at different
depths are aligned with the binary focus microscope.
An eighth object of the present invention is to provide a focusing
method for focusing light on an information medium with the optical
head apparatus.
A ninth embodiment of the present invention is to provide an
information reproducing method for reproducing a piece of recording
information recorded on a high density optical disk having a thin
thickness.
The first object is achieved by the provision of a compound
objective lens having two focal points, comprising: hologram means
for transmitting a part of incident light without any diffraction
to form a beam of transmitted light and diffracting a remaining
part of the incident light to form a beam of diffracted light, the
hologram means functioning as a lens for the diffracted light to
diverge the diffracted light from the hologram means or converge
the diffracted light; and lens means for converging the transmitted
light formed in the hologram means to form a first converging spot
at a first focal point and converging the diffracted light formed
in the hologram means to form a second converging spot at a second
focal point, the second focal point differing from the first focal
point.
In the above configuration, a part of incident light transmits
through the hologram means without any diffraction. Therefore, a
beam of transmitted light not diverged from the hologram means or
not converging is formed. Thereafter, the transmitted light is
refracted and converged by the lens means, so that the transmitted
light is focused on a first converging spot positioned at a first
focal point.
In contrast, a remaining part of incident light is diffracted by
the hologram means. Therefore, a beam of diffracted light such as a
beam of first-order diffracted light which is diverged from the
hologram lens or converges is formed. Thereafter, the diffracted
light is refracted and converged by the lens means, so that the
diffracted light is focused on a second converging spot positioned
at a second focal point.
In this case, because a propagation direction of the transmitted
light differs from that of the diffracted light, the first focal
point of the compound objective lens for the transmitted light
differs from the second focal point of the compound objective lens
for the diffracted light. Therefore, the compound objective lens
has two focal points, and the incident light transmitting through
the compound objective lens are converged on two converging
points.
Accordingly, the incident light transmitting through the compound
objective lens can be reliably converged on an information medium
regardless whether the information medium has a first thickness or
a second thickness.
It is preferred that a grating pattern be drawn in the hologram
means in a concentric circle shape, the grating pattern of the
hologram means be formed in relief to concentrically form
alternating rows of bottom portions and top portions, a height H of
relief in the grating pattern be set to H<.lamda./(n(.lamda.)-1)
where a symbol .lamda. denotes a wavelength of the incident light
and a symbol n(.lamda.) denotes a refractive index of the hologram
means made of a glass material for the incident light having the
wavelength .lamda., and a difference in phase modulation degree
between the incident light transmitting through a bottom portion of
the grating pattern and the incident light transmitting through a
top portion of the grating pattern be lower than 2.pi. radians to
set a diffraction efficiency of the hologram means to a value lower
than 100%.
In the above configuration, because the height of the relief in the
grating pattern is lower than a value .lamda./(n(.lamda.)-1), the
difference in phase modulation degree is induced to be lower than
2.pi. radians. Therefore, the diffraction efficiency of the
hologram means is set to a value lower than 100% over the entire
grating pattern, so that the transmitted light and the diffracted
light are simultaneously formed in the hologram lens.
The first object is also achieved by the provision of a compound
objective lens, comprising: lens means for converging a beam of
first incident light on a front surface of a first information
medium having a first thickness T1 and converging a beam of second
incident light on a front surface of a second information medium
having a second thickness T2 (T2<T1), the first incident light
passing through the first information medium from its rear surface,
and the second incident light passing through the second
information medium from its rear surface; and aperture limiting
means for selectively limiting an aperture of the lens means for
the second incident light which is incident on the lens means, a
second numerical aperture of the lens means for the second incident
light which is incident on the lens means being lower than a first
numerical aperture of the lens means for the first incident light
which is incident on the lens means.
In the above configuration, an aperture of the lens means for the
second incident light is limited by the aperture limiting means,
and another aperture of the lens means for the first incident light
is limited. Thereafter, the first incident light is converged by
the lens means on the first information medium at a high numerical
aperture, and the second incident light is converged by the lens
means on the second information medium at a low numerical aperture.
Accordingly, the compound objective lens has two focal points.
Also, the intensity of the first incident light can be larger than
that of the second incident light.
The first object is also achieved by the provision of a compound
objective lens, comprising: lens means for converging a beam of
first incident light on a front surface of a first information
medium having a first thickness and converging a beam of second
incident light on a front surface of a second information medium
having a second thickness, the first incident light passing through
the first information medium from its rear surface, and the second
incident light passing through the second information medium from
its rear surface; and curvature changing means for changing a
curvature of spherical waves of a part of incident light to form
the first incident light which is incident on the lens means and
not changing a curvature of spherical waves of a remaining part of
incident light to form the second incident light which is incident
on the lens means.
In the above configuration, a curvature of spherical waves of a
part of incident light is changed by the curvature changing means
to form a beam of first incident light, and a curvature of
spherical waves of a remaining part of incident light is not
changed to form a beam of second incident light. Thereafter, the
first incident light is converged on the first information medium,
and the second incident light is converged on the second
information medium.
Accordingly, the compound objective lens has two focal points.
The second object is achieved by the provision of an imaging
optical system, comprising: a light source for radiating a beam of
incident light of which a far field pattern is distributed to
decrease intensity of the incident light toward a peripheral
portion of the beam; hologram means for transmitting a part of the
incident light radiated from the light source without any
diffraction to form a beam of transmitted light and diffracting a
remaining part of the incident light to form a beam of diffracted
light, a grating pattern being formed in relief in the hologram
means to concentrically form alternating rows of bottom portions
and top portions on condition that a height H of relief in the
grating pattern is set to H<.lamda./(n(.lamda.)-1) where a
symbol .lamda. denotes a wavelength of the incident light and a
symbol n(.lamda.) denotes a refractive index of the hologram means
made of a glass material for the incident light having the
wavelength .lamda., a difference in phase modulation degree between
the incident light transmitting through the bottom portions of the
grating pattern and the incident light transmitting through the top
portions of the grating pattern being lower than 2.pi. radians to
set a diffraction efficiency of the hologram means to a value lower
than 100%, the height H of the relief in the grating pattern being
gradually lowered toward an outer direction of a pattern region in
which the grating pattern is drawn, and the diffraction efficiency
of the hologram means for the incident light being gradually
lowered toward the outer direction of the pattern region to
distribute intensity of the transmitted light in a gently-sloping
shape; and lens means for converging the transmitted light formed
in the hologram means to form a first converging spot at a first
focal point and converging the diffracted light formed in the
hologram means to form a second converging spot at a second focal
point.
In the above configuration, a beam of incident light is radiated
from a light source. A far field pattern of the incident light is
distributed to decrease intensity of the incident light toward a
peripheral portion of the beam. For example, the light source is a
semiconductor laser, the far field pattern of the incident light is
distributed in the Gaussian distribution. Thereafter, the incident
light transmits through the hologram means. In this case, because a
grating pattern is drawn in relief in the hologram means and
because the height of the relief is lower than a value
.lamda./(n(.lamda.)-1), the difference in phase modulation degree
between the incident light transmitting through a bottom portion of
the grating pattern and the incident light transmitting through a
top portion of the grating pattern is induced to be lower than
2.pi. radians. Therefore, the diffraction efficiency of the
hologram means for the incident light is set to a value lower than
100% over the entire grating pattern, so that the transmitted light
and the diffracted light are simultaneously formed in the hologram
lens. In addition, because the height H of the relief in the
grating pattern is gradually lowered toward the outer direction of
the pattern region, the diffraction efficiency of the hologram
means for the incident light is gradually lowered toward the outer
direction of the pattern region. Therefore, the incident light
positioned at a center portion of its beam are mainly changed to
the diffracted light, and the incident light positioned at a
peripheral portion of its beam are mainly changed to the
transmitted light.
Thereafter, the transmitted light is refracted and converged by the
lens means, so that the transmitted light is focused on a first
converging spot positioned at a first focal point. Also, the
diffracted light is refracted and converged by the lens means, so
that the diffracted light is focused on a second converging spot
positioned at a second focal point. In this case, because a
propagation direction of the transmitted light differs from that of
the diffracted light, the first focal point for the transmitted
light differs from the second focal point for the diffracted
light.
Accordingly, even though the far field pattern of the incident
light is distributed in the Gaussian distribution, the far field
pattern of the transmitted light is distributed in a gently-sloping
shape. Therefore, secondary maxima (or side lobes) of the
transmitted light can be prevented from occurring at the first
converging spot.
Also, because the height H of the relief in the grating pattern is
gradually lowered over the entire pattern region, a numerical
aperture of the lens means for the diffracted light can be
sufficiently heightened.
The second object is also achieved by the provision of an imaging
optical system, comprising: a light source for radiating a beam of
incident light of which a far field pattern is distributed to
decrease intensity of the incident light toward a peripheral
portion of the beam; hologram means for transmitting a part of the
incident light radiated from the light source without any
diffraction to form a beam of transmitted light and diffracting a
remaining part of the incident light to form a beam of diffracted
light, a grating pattern being formed in relief in the hologram
means to concentrically form alternating rows of bottom portions
and top portions on condition that a height H of relief in the
grating pattern is set to H<.lamda./(n(.lamda.)-1) where a
symbol .lamda. denotes a wavelength of the incident light and a
symbol n(.lamda.) denotes a refractive index of the hologram means
made of a glass material for the incident light having the
wavelength .lamda., a difference in phase modulation degree between
the incident light passing through the bottom portions of the
grating pattern and the incident light passing through the top
portions of the grating pattern being lower than 2.pi. radians to
set a diffraction efficiency of the hologram means to a value lower
than 100%, the height H of the relief in the grating pattern being
gradually lowered toward an inner direction of a pattern region in
which the grating pattern is drawn, and the diffraction efficiency
of the hologram means for the incident light being gradually
lowered toward the inner direction of the pattern region to
distribute intensity of the diffracted light in a gently-sloping
shape; and lens means for converging the transmitted light formed
in the hologram means to form a first converging spot at a first
focal point and converging the diffracted light formed in the
hologram means to form a second converging spot at a second focal
point.
In the above configuration, the transmitted light and the
diffracted light are simultaneously formed in the hologram lens in
the same manner. Also, because the height H of the relief in the
grating pattern is gradually lowered toward the inner direction of
the pattern region, the diffraction efficiency of the hologram
means for the incident light is gradually lowered toward the inner
direction of the pattern region. Therefore, the incident light
positioned at a center portion of its beam are mainly changed to
the transmitted light, and the incident light positioned at a
peripheral portion of its beam are mainly changed to the diffracted
light.
Accordingly, even though the far field pattern of the incident
light is distributed in the Gaussian distribution, the far field
pattern of the diffracted light is distributed in a gently-sloping
shape. Therefore, secondary maxima (or side lobes) of the
diffracted light can be prevented from occurring at the second
converging spot.
Also, because the height H of the relief in the grating pattern is
gradually lowered over the entire pattern region, a numerical
aperture of the lens means for the transmitted light can be
sufficiently heightened.
The third object is achieved by the provision of an optical head
apparatus for recording or reproducing a piece of information on or
from a thin type of first information medium having a first
thickness or a thick type of second information medium having a
second thickness larger than the first thickness, comprising: a
light source for radiating a beam of incident light; hologram means
for transmitting a part of the incident light radiated from the
light source without any diffraction on an outgoing path to form a
beam of transmitted light and diffracting a remaining part of the
incident light radiated from the light source on the outgoing path
to form a beam of diffracted light, the hologram means functioning
as a lens for the diffracted light to diverge the diffracted light
from the hologram means or converge the diffracted light; lens
means for converging the transmitted light formed in the hologram
means at a first focal length on the outgoing path to form a first
converging spot at a front surface of the first information medium
or converging the diffracted light formed in the hologram means at
a second focal length on the outgoing path to form a second
converging spot at a front surface of the second information
medium, the transmitted light being incident on a rear surface of
the first information medium and being converged at the front
surface of the first information medium, the transmitted light
being reflected at the rear surface of the first information medium
and again passing through the lens means and the hologram means on
an incoming path, the diffracted light being incident on a rear
surface of the second information medium and being converged at the
front surface of the second information medium, and the diffracted
light being reflected at the rear surface of the first information
medium and again passing through the lens means and the hologram
means on the incoming path; wavefront changing means for changing a
wavefront of the transmitted light or the diffracted light passing
through the lens means and the hologram means on the incoming path
to form one or more beams of information light; and detecting means
for detecting intensities of the information light formed by the
wavefront changing means and generating an information signal
according to the intensities of the information light, the
information signal expressing a piece of information recorded on
the first information medium or the second information medium.
In the above configuration, a beam of incident light is radiated
from the light source, and a part of the incident light transmits
through the hologram lens to form a beam of transmitted light.
Also, a remaining part of the incident light is diffracted by the
hologram lens to form a beam of diffracted light. Thereafter, the
transmitted light and the diffracted light are converged by the
converging means. In cases where a piece of information is recorded
or reproduced on or from the first information medium, the
transmitted light is incident on the rear surface of the first
information medium and is converged at the front surface of the
first information medium to form the first converging spot.
Thereafter, the transmitted light is reflected at the rear surface
of the first information medium and again passes through the lens
means and the hologram means without any diffraction. In contrast,
in cases where a piece of information is recorded or reproduced on
or from the second information medium, the diffracted light is
incident on the rear surface of the second information medium and
is converged at the front surface of the second information medium
to form the second converging spot. Thereafter, the diffracted
light is reflected at the rear surface of the second information
medium and again passes through the lens means. Thereafter, the
diffracted light is again diffracted by the hologram means.
Thereafter, a wavefront of the transmitted light or the diffracted
light is changed by the wavefront changing means to form a
plurality of beams of reflected light, and the intensities of the
reflected light is detected by the detecting means. Therefore, an
information signal expressing the information recorded on the first
or second information medium is generated according to the
intensities of the reflected light.
Accordingly, because the first converging spot of the transmitted
light differs from the second converging spot of the diffracted
light, a compound objective lens composed of the hologram lens and
the lens means has two focal points. Therefore, a piece of
information can be recorded or reproduced on or from an information
medium regardless of whether the information medium has the first
thickness or the second thickness.
The third object is also achieved by the provision of an optical
head apparatus for recording or reproducing a piece of information
on or from a first information medium having a first thickness T1
or a second information medium having a second thickness T2
(T1<T2), comprising: lens means for converging a beam of first
incident light on a front surface of a first information medium
having a first thickness T1 or converging a beam of second incident
light on a front surface of a second information medium having a
second thickness T2 (T2<T1), the first incident light passing
through the first information medium from its rear surface, and the
second incident light passing through the second information medium
from its rear surface;
aperture limiting means for selectively limiting an aperture of the
lens means for the second incident light which is incident on the
lens means, a second numerical aperture of the lens means for the
second incident light which is incident on the lens means being
lower than a first numerical aperture of the lens means for the
first incident light which is incident on the lens means, the first
incident light being reflected at the front surface of the first
information medium and again passing through the lens means and the
aperture limiting means on an incoming path, and the second
incident light being reflected at the front surface of the second
information medium and again passing through the lens means and the
aperture limiting means on the incoming path; a light source for
radiating the first incident light and the second incident light to
the aperture limiting means; wavefront changing means for changing
a wavefront of the first or second incident light passing through
the lens means and the aperture limiting means on the incoming path
to form one or more beams of information light; and detecting means
for detecting intensities of the information light formed by the
wavefront changing means and generating an information signal
according to the intensities of the information light, the
information signal expressing a piece of information recorded on
the first information medium or the second information medium.
In the above configuration, a compound objective lens composed of
the lens means and the aperture limiting means has two focal
points, and the intensity of the first incident light is larger
than that of the second incident light.
Accordingly, a piece of information can be recorded or reproduced
on or from an information medium regardless of whether the
information medium has the first thickness or the second thickness.
Also, a piece of information can be efficiently recorded on the
first information medium with the first incident light having a
high intensity, and a piece of information can be efficiently
reproduced from the second information medium with the second
incident light having a comparatively low intensity.
The third object is also achieved by the provision of an optical
head apparatus for recording or reproducing a piece of information
on or from a first information medium having a first thickness or a
second information medium having a second thickness, comprising:
lens means for converging a beam of first incident light on a front
surface of the first information medium and converging a beam of
second incident light on a front surface of the second information
medium, the first incident light passing through the first
information medium from its rear surface, and the second incident
light passing through the second information medium from its rear
surface; and curvature changing means for changing a curvature of
spherical waves of a part of incident light to form the first
incident light which is incident on the lens means and not changing
a curvature of spherical waves of a remaining part of incident
light to form the second incident light which is incident on the
lens means, the first incident light being reflected at the front
surface of the first information medium and again passing through
the lens means and the curvature changing means on an incoming
path, and the second incident light being reflected at the front
surface of the second information medium and again passing through
the lens means and the curvature changing means on the incoming
path; a light source for radiating the incident light to the
curvature changing means; wavefront changing means for changing a
wavefront of the first or second incident light passing through the
lens means and the curvature changing means on the incoming path to
form one or more beams of information light; and detecting means
for detecting intensities of the information light formed by the
wavefront changing means and generating an information signal
according to the intensities of the information light, the
information signal expressing a piece of information recorded on
the first information medium or the second information medium.
In the above configuration, because a compound objective lens is
composed of the lens means and the curvature changing means, the
compound objective lens has two focal points. Accordingly, a piece
of information can be recorded or reproduced on or from an
information medium regardless of whether the information medium has
the first thickness or the second thickness.
The fourth object is achieved by the provision of an optical disk,
comprising: an information recording substrate partitioned into a
first region and a second region, the first region having a first
thickness, and the second region having a second thickness smaller
than the first thickness; a plurality of first recording pits
placed at the first region of the information recording substrate
for recording pieces of recording information at a high recording
density, the first recording pits being formed at narrow intervals;
and a plurality of second recording pits placed at the second
region of the information recording substrate for recording pieces
of distinguishing information at an ordinary recording density of a
compact disk, the distinguishing information informing that the
recording information are recorded on the information recording
substrate having the first thickness, and the recording density of
the recording information being higher than that of the
distinguishing information.
In the above configuration, a substrate of a conventional compact
disk has the same second thickness as that of the second region of
the information recording substrate in the optical disk according
to the present invention. Therefore, in cases where a beam of
reproducing light is incident on a prescribed region of an unknown
disk selected from a group of the conventional compact disk and the
optical disk, the reproducing light is focused on a recording pit
of the conventional compact disk or one of the second recording
pits of the optical disk regardless of whether the unknown disk is
the conventional compact disk or the optical disk.
In cases where the unknown disk is the optical disk, a piece of
distinguishing information is read by the reproducing light.
Because the distinguishing information informs that pieces of
recording information are recorded on the information recording
substrate having the first thickness, a curvature of the
reproducing light is automatically changed to focus the reproducing
light on the information recording substrate having the first
thickness, and the reproducing light is automatically focused on
one of the first recording pits. Therefore, a piece of recording
information is reproduced.
In contrast, in cases where the unknown disk is the conventional
compact disk, a piece of recording information is read by the
reproducing light in the same manner as in a prior art.
Accordingly, a piece of recording information formed on an
information recording substrate can be reliably reproduced even
though the thickness of the information recording substrate is
unknown.
The fourth object is also achieved by the provision of an optical
disk, comprising: an information recording substrate having a thin
thickness, the thin thickness of the information recording
substrate being thinner than that of a compact disk; a plurality of
first recording pits placed at a first region of the information
recording substrate for recording pieces of recording information
at a high recording density, the first recording pits being formed
at narrow intervals; and a plurality of second recording pits
placed at a second region of the information recording substrate
for recording pieces of distinguishing information at a low
recording density, the distinguishing information informing that
the recording information are recorded on the information recording
substrate having the thin thickness, the recording density of the
recording information being higher than that of the distinguishing
information, each of the second recording pits being larger than
that of a recording pit in the compact disk, and a converging spot
of a beam of reproducing light, which is converged to focus on an
ordinary recording pit formed on a substrate having an ordinary
thickness of the compact disk, being formed in one of the second
recording pits to read the distinguishing information.
In the above configuration, a beam of reproducing light, of which a
curvature is adjusted to focus the reproducing light on a recording
pit formed on an information recording substrate of the compact
disk, is incident on a prescribed region of an unknown disk
selected from a group of the compact disk having an ordinary
thickness and the optical disk according to the present invention.
In cases where the unknown disk is the optical disk, the
reproducing light is converged on one of the second recording pits
in defocus because the information recording substrate of the
optical disk has the thin thickness. However, because each of the
second recording pits is large in size, a converging spot of the
reproducing light is formed in the second recording pit. Therefore,
a piece of distinguishing information is read by the reproducing
light. Because the distinguishing information informs that pieces
of recording information are recorded on the information recording
substrate having the thin thickness, a curvature of the reproducing
light is automatically changed to focus the reproducing light on
the information recording substrate having the thin thickness, and
the reproducing light is automatically focused on one of the first
recording pits. Therefore, a piece of recording information is
reproduced.
In contrast, in cases where the unknown disk is the compact disk, a
piece of recording information is read by the reproducing light in
the same manner as in a prior art.
Accordingly, a piece of recording information formed on an
information recording substrate can be reliably reproduced even
though the thickness of the information recording substrate is
unknown.
The fifth object is achieved by the provision of an optical disk
apparatus for recording or reproducing pieces of recording
information on or from an optical disk in which the recording
information are recorded or reproduced at a high density on or from
a first substrate having a first thickness and a piece of
distinguishing information informing that the recording information
are recorded or reproduced on or from the first substrate having
the first thickness is recorded at an ordinary density on a second
substrate having a second thickness larger than the first
thickness, comprising: rotating means for rotating the optical disk
at a regular speed; a light source for radiating a beam of incident
light; hologram means for transmitting a part of the incident light
radiated from the light source without any diffraction on an
outgoing path to form a beam of transmitted light and diffracting a
remaining part of the incident light radiated from the light source
on the outgoing path to form a beam of diffracted light, the
hologram means functioning as a lens for the diffracted light to
diverge the diffracted light from the hologram means; lens means
for converging the transmitted light formed in the hologram means
on the first substrate of the optical disk rotated by the rotating
means to record or reproduce a piece of recording information on or
from the optical disk and converging the diffracted light formed in
the hologram means on the second substrate of the optical disk
rotated by the rotating means to reproduce the distinguishing
information from the optical disk, the transmitted light being
reflected by the first substrate of the optical disk and again
passing through the lens means and the hologram means on an
incoming path, and the diffracted light being reflected by the
second substrate of the optical disk and again passing through the
lens means and the hologram means on the incoming path; wavefront
changing means for changing a wavefront of the transmitted light
passing through the lens means and the hologram means on the
incoming path to form one or more beams of recording information
light and changing a wavefront of the diffracted light passing
through the lens means and the hologram means on the incoming path
to form one or more beams of distinguishing information light;
detecting means for detecting intensities of the recording
information light formed by the wavefront changing means to
generate a recording information signal according to the
intensities of the recording information light and detecting
intensities of the distinguishing information light formed by the
wavefront changing means to generate a distinguishing information
signal according to the intensities of the distinguishing
information light, the distinguishing information signal expressing
the distinguishing information recorded on the second substrate of
the optical disk, and the recording information signal expressing
the recording information recorded on the first substrate of the
optical disk; and moving means for moving an optical head apparatus
comprising the light source, the hologram means, the lens means and
the detecting means to converge the diffracted light formed in the
hologram means on the second substrate of the optical disk and
moving the optical disk, in which the diffracted light formed in
the hologram means is converged on the second substrate of the
optical disk, to converge the transmitted light formed in the
hologram means on the first substrate of the optical disk in cases
where the distinguishing information is detected in the detecting
means.
In the above configuration, an optical head apparatus comprising
the light source, the hologram means, the lens means and the
detecting means has the same configuration as that described
before. Initially, the optical head apparatus is moved by the
moving means to converge in focus the diffracted light formed in
the hologram means on the second substrate of the optical disk
rotated by the rotating means. Therefore, the distinguishing
information recorded on the second substrate is reproduced in the
detecting means, and it is informed that pieces of recording
information are recorded or reproduced on or from the first
substrate having the first thickness. Thereafter, the optical head
apparatus is moved by the moving means to converge in focus the
transmitted light formed in the hologram means on the first
substrate of the optical disk rotated by the rotating means.
Therefore, a piece of recording information is recorded or
reproduced on or from the first substrate of the optical disk.
Accordingly, even though a high density type of optical disk, in
which pieces of recording information is recorded or reproduced on
or from the substrate having the first thickness smaller than the
second thickness of a conventional optical disk, is utilized, the
recording information can be reliably recorded or reproduced.
The fifth object is also achieved by the provision of an optical
disk apparatus for recording or reproducing pieces of recording
information on or from an optical disk in which the recording
information are recorded or reproduced at a high density on or from
a first substrate having a thin thickness thinner than that of a
compact disk and a piece of distinguishing information informing
that the recording information are recorded or reproduced on or
from the first substrate having the thin thickness is recorded at a
low density on a second substrate having the thin thickness,
comprising: rotating means for rotating the optical disk at a
regular speed; a light source for radiating a beam of incident
light; hologram means for transmitting a part of the incident light
radiated from the light source without any diffraction on an
outgoing path to form a beam of transmitted light and diffracting a
remaining part of the incident light radiated from the light source
on the outgoing path to form a beam of diffracted light, the
hologram means functioning as a lens for the diffracted light to
diverge the diffracted light from the hologram means; lens means
for converging in focus the transmitted light formed in the
hologram means on the first substrate of the optical disk rotated
by the rotating means to record or reproduce a piece of recording
information on or from the optical disk and converging in defocus
the diffracted light formed in the hologram means on the second
substrate of the optical disk rotated by the rotating means to
reproduce the distinguishing information from the optical disk, the
transmitted light being reflected by the first substrate of the
optical disk and again passing through the lens means and the
hologram means on an incoming path, and the diffracted light being
reflected by the second substrate of the optical disk and again
passing through the lens means and the hologram means on the
incoming path; wavefront changing means for changing a wavefront of
the transmitted light passing through the lens means and the
hologram means on the incoming path to form one or more beams of
recording information light and changing a wavefront of the
diffracted light passing through the lens means and the hologram
means on the incoming path to form one or more beams of
distinguishing information light; detecting means for detecting
intensities of the recording information light formed by the
wavefront changing means to generate a recording information signal
according to the intensities of the recording information light and
detecting intensities of the distinguishing information light
formed by the wavefront changing means to generate a distinguishing
information signal according to the intensities of the
distinguishing information light, the distinguishing information
signal expressing the distinguishing information recorded on the
second substrate of the optical disk, and the recording information
signal expressing the recording information recorded on the first
substrate of the optical disk; and moving means for moving an
optical head apparatus comprising the light source, the hologram
means, the lens means and the detecting means, to converge the
diffracted light formed in the hologram means in defocus on the
second substrate of the optical disk and moving the optical disk,
in which the diffracted light formed in the hologram means is
converged on the second substrate of the optical disk in defocus,
to converge the transmitted light formed in the hologram means on
the first substrate of the optical disk in focus in cases where an
intensity of the distinguishing information signal generated in the
detecting means is larger than a threshold value.
In the above configuration, an optical head apparatus comprising
the light source, the hologram means, the lens means and the
detecting means has the same configuration as that described
before. Initially, the optical head apparatus is moved by the
moving means to converge in defocus the diffracted light formed in
the hologram means on the second substrate of the optical disk
rotated by the rotating means. In this case, because the
distinguishing information is recorded at a low density, a
plurality of recording pits expressing the distinguishing
information are respectively large in size. Therefore, even though
the diffracted light is converged on each of the recording pits in
defocus, a converging spot of the diffracted light is formed in
each of the recording pits. Therefore, the distinguishing
information recorded on the second substrate is reproduced in the
detecting means, and it is informed that pieces of recording
information are recorded or reproduced on or from the first
substrate having the thin thickness. Thereafter, the optical head
apparatus is moved by the moving means to converge in focus the
transmitted light formed in the hologram means on the first
substrate of the optical disk rotated by the rotating means.
Therefore, a piece of recording information is recorded or
reproduced on or from the first substrate of the optical disk.
Accordingly, even though a high density type of optical disk, in
which pieces of recording information are recorded or reproduced on
or from the substrate having the thin thickness smaller than an
ordinary thickness of a conventional optical disk, is utilized, the
recording information can be reliably recorded or reproduced.
The sixth object is achieved by the provision of a binary focus
microscope for simultaneously observing a first image put on a
first image plane and a second image put on a second image plane,
comprising: an objective lens for refracting a beam of first light
diverging from the first image and a beam of second light diverging
from the second image, a first distance between the objective lens
and the first image of the first image plane differing from a
second distance between the objective lens and the second image of
the second image plane; a hologram lens for transmitting the first
light refracted by the objective lens without any diffraction to
form a beam of transmitted light and diffracting the second light
refracted by the objective lens to form a beam of diffracted light,
the hologram lens functioning as a lens for the second light to
pass the diffracted light through the same optical path as the
transmitted light passes through, and a beam of superposed light
being formed of the transmitted light and the diffracted light; an
inner lens for converging the superposed light formed by the
hologram lens at an image point of a third image plane to
simultaneously form the first image and the second image enlarged
on the third image plane; and an ocular lens for converging the
superposed light which is converged by the inner lens and diverges
from the image point to simultaneously form the first image and the
second image moreover enlarged.
In the above configuration, a beam of first light diverging from
the first image and a beam of second light diverging from the
second image are refracted together by the objective lens. In this
case, because a first distance between the objective lens and the
first image of the first image plane differs from a second distance
between the objective lens and the second image of the second image
plane, a curvature of the first light refracted differs from
another curvature of the second light refracted. Thereafter, the
first light refracted transmits through the hologram lens without
any diffraction to form a beam of transmitted light, and the second
light refracted is diffracted by the hologram lens to form a beam
of diffracted light. In this case, because the hologram lens
functions as a lens for the diffracted light, a curvature of the
diffracted light agrees with that of the transmitted light. In
other words, the diffracted light passes through the same optical
path as the transmitted light passes through. Therefore, a beam of
superposed light is formed of the transmitted light and the
diffracted light. Thereafter, the superposed light is converged by
the inner lens at an image point of a third image plane, so that
the first image and the second image enlarged are simultaneously
formed on the third image plane. Thereafter, the superposed light
diverging from the image point is converged by the ocular lens, so
that the first image and the second image moreover enlarged are
simultaneously formed.
Accordingly, an operator can observe the first image and the second
image sufficiently enlarged.
The sixth object is also achieved by the provision of a binary
focus microscope for simultaneously observing a first image put on
a first image plane and a second image put on a second image plane,
comprising: an objective lens for refracting a beam of first light
diverging from the first image and a beam of second light diverging
from the second image, a first distance between the objective lens
and the first image of the first image plane differing from a
second distance between the objective lens and the second image of
the second image plane; a hologram lens for transmitting the first
light refracted by the objective lens without any diffraction to
form a beam of transmitted light and diffracting the second light
refracted by the objective lens to form a beam of diffracted light,
the hologram lens functioning as a lens for the second light to
pass the diffracted light through the same optical path as the
transmitted light passes through, and a beam of superposed light
being formed of the transmitted light and the diffracted light; an
inner lens for converging the superposed light formed by the
hologram lens at an image point of a third image plane to
simultaneously form the first image and the second image enlarged
on the third image plane; and photographing means for photographing
a superposed image formed of the first and second images enlarged
on the third image plane by converging the superposed light in the
inner lens.
In the above configuration, the first image and the second image
enlarged are simultaneously formed on the third image plane in the
same manner. Thereafter, the first image and the second image
enlarged are photographed by the photographing means as a
superposed image.
Accordingly, the first image and the second image enlarged can be
observed.
The seventh embodiment is achieved by the provision of an alignment
apparatus for aligning a first reference image drawn on a photomask
with a second reference image drawn on a sample, comprising: a
light source for radiating beams of alignment light to illuminate
the first and second reference images; an objective lens for
refracting both a beam of first alignment light diverging from the
first reference image and a beam of second alignment light
diverging from the second reference image which are illuminated
with the alignment light radiated from the light source, a first
distance between the objective lens and the first reference image
of the photomask differing from a second distance between the
objective lens and the second reference image of the sample; a
hologram lens for transmitting the first alignment light refracted
by the objective lens without any diffraction to form a beam of
transmitted light and diffracting the second alignment light
refracted by the objective lens to form a beam of diffracted light,
the hologram lens functioning as a lens for the second alignment
light to pass the diffracted light through the same optical path as
the transmitted light passes through, and a beam of superposed
light being formed of the transmitted light and the diffracted
light; an inner lens for converging the superposed light formed by
the hologram lens at an image point of an image plane to
simultaneously form the first and second reference images enlarged
on the image plane, an optical axis passing through centers of the
objective lens, the hologram lens and the inner lens; photographing
means for photographing a superposed image formed of the first and
second images enlarged on the image plane by converging the
superposed light in the inner lens; and moving means for moving the
photomask or the sample according to the superposed image
photographed by the photographing means to align the first
reference image with the second reference image along the optical
axis.
In the above configuration, the objective lens, the hologram lens
and the inner lens are the same as those in the binary focus
microscope. Therefore, the first and second images enlarged on the
image plane is photographed by the photographing means as a
superposed image. Thereafter, the photomask or the sample is moved
in a direction perpendicular to the optical axis by the moving
means to align the first reference image with the second reference
image along the optical axis.
Accordingly, because the superposed image formed of the first and
second reference images enlarged is photographed by the
photographing means, a relative position between the first and
second reference images can be accurately observed. Therefore, the
first reference image can be accurately aligned with the second
reference image.
The eighth embodiment is achieved by the provision of a focusing
method for focusing light on a first information medium having a
first thickness or a second information medium having a second
thickness to record or reproduce a piece of information on or from
the first information medium or the second information medium,
comprising the steps of: moving an optical head apparatus in a
direction to decrease or increase the distance between the optical
head apparatus and the first or second information medium, the
optical head apparatus comprising a light source for radiating a
beam of incident light, hologram means for transmitting a part of
the incident light radiated from the light source without any
diffraction on an outgoing path to form a beam of transmitted light
and diffracting a remaining part of the incident light radiated
from the light source on the outgoing path to form a beam of
diffracted light, the hologram means functioning as a lens for the
diffracted light to diverge the diffracted light from the hologram
means or converge the diffracted light, lens means for converging
the transmitted light formed in the hologram means at a first focal
length on the outgoing path to form a first converging spot at a
front surface of the first information medium or converging the
diffracted light formed in the hologram means at a second focal
length on the outgoing path to form a second converging spot at a
front surface of the second information medium, the transmitted
light being incident on a rear surface of the first information
medium and being converged at the front surface of the first
information medium, the transmitted light being reflected at the
rear surface of the first information medium and again passing
through the lens means and the hologram means on an incoming path,
the diffracted light being incident on a rear surface of the second
information medium and being converged at the front surface of the
second information medium, and the diffracted light being reflected
at the rear surface of the first information medium and again
passing through the lens means and the hologram means on the
incoming path, wavefront changing means for changing a wavefront of
the transmitted light or the diffracted light passing through the
lens means and the hologram means on the incoming path to form one
or more beams of information light, and detecting means for
detecting intensities of the information light formed by the
wavefront changing means and generating an information signal and a
focus error signal according to the intensities of the information
light, the information signal expressing a piece of information
recorded on the first information medium or the second information
medium; judging whether or not an intensity of the focus error
signal generated in the detecting means is larger than a threshold
value; and adjusting the position of the optical head apparatus to
decrease the intensity of the focus error signal to zero when the
intensity of the focus error signal becomes larger than the
threshold value.
In the above steps, the focusing method is performed by utilizing
the optical head apparatus described above. The intensity of the
focus error signal is largely increased when the distance between
the lens means and the first or second information medium is near
to a focal length of the lens means. Therefore, when the intensity
of the focus error signal becomes larger than a threshold value,
the lens means is placed near to a just-focus point in which the
transmitted light or the diffracted light is converged on the first
or second information medium in focus.
Accordingly, in cases where the position of the optical head
apparatus is adjusted to decrease the intensity of the focus error
signal to zero when the intensity of the focus error signal becomes
larger than the threshold value, the transmitted light or the
diffracted light can be focused on the first or second information
medium.
The ninth embodiment is achieved by the provision of an information
reproducing method for reproducing a piece of recording information
from an optical disk in which the recording information are
recorded at a high density on a first substrate having a first
thickness and a piece of distinguishing information informing that
the recording information are recorded on the first substrate is
recorded at an ordinary density on a second substrate having a
second thickness larger than the first thickness, comprising the
step of: moving an optical disk apparatus under the second
substrate of the optical disk, the optical disk comprising rotating
means for rotating the optical disk at a regular speed, a light
source for radiating a beam of incident light; hologram means for
transmitting a part of the incident light radiated from the light
source without any diffraction on an outgoing path to form a beam
of transmitted light and diffracting a remaining part of the
incident light radiated from the light source on the outgoing path
to form a beam of diffracted light, the hologram means functioning
as a lens for the diffracted light to diverge the diffracted light
from the hologram means, lens means for converging the transmitted
light formed in the hologram means on the first substrate of the
optical disk rotated by the rotating means to record or reproduce a
piece of recording information on or from the optical disk and
converging the diffracted light formed in the hologram means on the
second substrate of the optical disk rotated by the rotating means
to reproduce the distinguishing information from the optical disk,
the transmitted light being reflected by the first substrate of the
optical disk and again passing through the lens means and the
hologram means on an incoming path, and the diffracted light being
reflected by the second substrate of the optical disk and again
passing through the lens means and the hologram means on the
incoming path, wavefront changing means for changing a wavefront of
the transmitted light passing through the lens means and the
hologram means on the incoming path to form one or more beams of
recording information light and changing a wavefront of the
diffracted light passing through the lens means and the hologram
means on the incoming path to form one or more beams of
distinguishing information light, and detecting means for detecting
intensities of the recording information light formed by the
wavefront changing means to generate a recording information signal
according to the intensities of the recording information light and
detecting intensities of the distinguishing information light
formed by the wavefront changing means to generate a distinguishing
information signal according to the intensities of the
distinguishing information light, the distinguishing information
signal expressing the distinguishing information recorded on the
second substrate of the optical disk, and the recording information
signal expressing the recording information recorded on the first
substrate of the optical disk; and converging the diffracted light
on the second substrate of the optical disk to reproduce the
distinguishing information; moving the optical disk apparatus to a
position under the first substrate of the optical disk to converge
the transmitted light on the first substrate of the optical disk
when the distinguishing information is detected in the detecting
means; and reproducing the recording information by generating the
recording information signal in the detecting means.
In the above steps, the information reproducing method is performed
by utilizing the optical disk apparatus described above. The
distinguishing information placed on the second substrate of the
optical disk is reproduce with the diffracted light. In this case,
because the second substrate has the second thickness, the
diffracted light is just focused on the second substrate.
Thereafter, when the distinguishing information is detected, the
optical disk apparatus is moved to a position under the first
substrate of the optical disk, and the transmitted light is
converged on the first substrate of the optical disk. In this case,
because the first substrate has the first thickness, the diffracted
light is just focused on the first substrate.
Accordingly, the recording information can be reliably
reproduced.
BRIEF DESCRIPTION OF THE DRAWINGS
The objects, features and advantages of the present invention will
be apparent from the following description taken in conjunction
with the accompanying drawings, in which:
FIG. 1 is a constitutional view of a conventional optical head
apparatus proposed in Japanese Patent Application No. 46630 of
1991;
FIGS. 2A, 2B are respectively a cross sectional view of a set of an
objective lens and a blazed hologram shown in FIG. 1;
FIG. 3 shows a relationship between the thickness of an optical
disk and a numerical aperture of an objective lens on condition
that the tilt of the optical axis is constant;
FIG. 4A is a constitutional view of an imaging optical system
having a compound objective lens according to a first embodiment of
the present invention, a beam of transmitted light not diffracted
being converged on a thin type of information medium;
FIG. 4B is a constitutional view of the imaging optical system
shown in FIG. 4A, a beam of first-order diffracted light being
converged on a thick type of information medium;
FIG. 5 is a plan view of a hologram lens shown in FIGS. 4A, 4B, a
grating pattern of the hologram lens being depicted;
FIG. 6 is a cross sectional view of the hologram lens shown in FIG.
5, the grating pattern formed in relief on the hologram lens being
shown;
FIG. 7 is an explanatory diagram showing an intensity distribution
of transmitted light L4 converged on a converging spot S1 of a
first information medium, a primary maximum and secondary maxima
suppressed occurring in the converging spot S1;
FIG. 8A is a cross sectional view of the hologram lens shown in
FIG. 5, the grating pattern approximating to a stepwise shape
composed of four stairs being shown;
FIG. 8B is a cross sectional view of the hologram lens shown in
FIG. 5, the grating pattern approximating to a stepwise shape
composed of a plurality of stairs being shown;
FIG. 9A is a constitutional view of an imaging optical system
having a compound objective lens according to a modification of the
first embodiment, a beam of first-order diffracted light being
converged on a thin type of information medium;
FIG. 9B is a constitutional view of the imaging optical system
shown in FIG. 9A, a beam of transmitted light not diffracted being
converged on a thick type of information medium;
FIG. 10A is a constitutional view of an imaging optical system
having a compound objective lens according to a second embodiment
of the present invention, a beam of transmitted light not
diffracted being converged on a thin type of information
medium;
FIG. 10B is a constitutional view of the imaging optical system
shown in FIG. 10A, a beam of first-order diffracted light being
converged on a thick type of information medium;
FIG. 11 shows a change of a diffraction efficiency of a hologram
lens shown in FIGS. 10A, 10B;
FIGS. 12A to 12E are respectively a cross sectional view of the
hologram lens shown in FIGS. 10A, 10B, the grating pattern of the
hologram lens approximating to a step-wise shape;
FIG. 13A shows an intensity distribution of incident light utilized
in the second embodiment, a far field pattern of the incident light
being distributed in a Gaussian distribution;
FIG. 13B shows an intensity distribution of transmitted light
transmitting through a hologram lens shown in FIGS. 10A, 10B, a far
field pattern of the incident light being distributed in a
gently-sloping shape;
FIGS. 14A to 14C show intensity distributions of transmitted light
and diffracted light transmitting through a hologram lens shown in
FIGS. 10A, 10B;
FIG. 15A is a plan view of a hologram lens according to a
modification of the second embodiment, a grating pattern of the
hologram lens being depicted;
FIGS. 15B, 15C are respectively a constitutional view of an imaging
optical system having a compound objective lens according to
another modification of the second embodiment;
FIG. 16A is a constitutional view of an imaging optical system
having a compound objective lens according to a third embodiment of
the present invention, a beam of first-order diffracted light being
converged on a thin type of information medium;
FIG. 16B is a constitutional view of the imaging optical system
shown in FIG. 16A, a beam of transmitted light not diffracted being
converged on a thick type of information medium;
FIG. 17 shows a change of a diffraction efficiency of a hologram
lens shown in FIGS. 16A, 16B;
FIGS. 18A to 18C show intensity distributions of transmitted light
and diffracted light transmitting through a hologram lens shown in
FIGS. 16A, 16B;
FIG. 19A is a cross sectional view of a compound objective lens
according to a fourth embodiment of the present invention;
FIG. 19B is a cross sectional view of a compound objective lens
according to a modification of the fourth embodiment of the present
invention;
FIG. 20 is a cross sectional view of a compound objective lens
according to a fifth embodiment of the present invention;
FIG. 21 is a constitutional view of an optical head apparatus
according to a sixth embodiment of the present invention;
FIG. 22 is a plan view of a wavefront changing device utilized in
the six, ninth and twelfth embodiments, a grating pattern of a
hologram lens utilized as the wavefront changing device being
depicted;
FIG. 23 shows a positional relation between focal points of
diffracted light occurring in the wavefront changing device shown
in FIG. 22 and a photo detector;
FIG. 24 is a plan view of a photo detector utilized in the six,
ninth, tenth, twelfth, thirteenth and seventeenth embodiments;
FIG. 25A and 25C respectively show a converging spot of first-order
diffracted light radiated to detecting sections SE1, SE2 and SE3 of
a sextant photo-detector shown in FIG. 24 and another converging
spot of minus first-order diffracted light radiated to detecting
sections SE4, SE5 and SE6 of the sextant photo-detector on
condition that an objective lens shown in FIG. 21 is defocused on
an information medium;
FIG. 25B shows a converging spot of first-order diffracted light
radiated to the detecting sections SE1, SE2 and SE3 of the sextant
photo-detector and another converging spot of minus first-order
diffracted light radiated to the detecting sections SE4, SE5 and
SE6 of the sextant photo-detector on condition that the objective
lens is just focused on the information medium;
FIG. 26 shows a relationship between beams of diffracted light
occurring in the wavefront changing device shown in FIG. 22 and the
photo detector shown in FIG. 24;
FIG. 27 is a constitutional view of an optical head apparatus
according to a seventh embodiment;
FIG. 28 is a plan view of a photo detector utilized in the seven,
ninth, tenth, twelfth and thirteenth embodiments;
FIGS. 29A, 29B, 29C show various shapes of converging spots
converged on the photo detector shown in FIG. 28;
FIG. 29D shows a radial direction Dr and a tangential direction
Dt;
FIG. 30 is a constitutional view of an optical head apparatus
according to a first modification of the seventh embodiment;
FIG. 31 is a constitutional view of an optical head apparatus
according to a second modification of the seventh embodiment;
FIG. 32 is a constitutional view of an optical head apparatus
according to a third modification of the seventh embodiment;
FIG. 33 is a constitutional view of an optical head apparatus
according to a forth modification of the seventh embodiment;
FIG. 34 shows a beam of transmitted light not diffracted on an
incoming optical path and a beam of transmitted light diffracted on
the incoming optical path, the beams being utilized to detect an
information signal;
FIG. 35A graphically shows a change of a focus error signal
obtained by detecting the intensity of transmitted light, the
strength of the focus error signal depending on a distance between
an objective lens and a first information medium;
FIG. 35B graphically shows a change of a focus error signal
obtained by detecting the intensity of diffracted light, the
strength of the focus error signal depending on a distance between
an objective lens and a second information medium.
FIG. 36A graphically shows a change of a focus error signal
obtained by detecting the intensity of diffracted light, the
strength of the focus error signal depending on a distance between
an objective lens and a first information medium;
FIG. 36B graphically shows a change of a focus error signal
obtained by detecting the intensity of transmitted light, the
strength of the focus error signal depending on a distance between
an objective lens and a second information medium;
FIG. 37 is a constitutional view of an optical head apparatus
according to a ninth embodiment;
FIG. 38 is a constitutional view of an optical head apparatus
according to a tenth embodiment;
FIG. 39 is a plan view of a beam splitter having a reflection type
of hologram utilized in the optical head apparatus shown in FIG.
38;
FIGS. 40A, 40B are respectively a constitutional view of an optical
head apparatus according an eleventh embodiment;
FIG. 41 is a plan view of a beam splitter having a reflection type
of hologram utilized in the optical head apparatus shown in FIG.
38;
FIG. 42A and 42C respectively show a converging spot of first-order
diffracted light radiated to detecting sections SE1, SE2 and SE3 of
a sextant photo-detector shown in FIG. 24 and another converging
spot of minus first-order diffracted light radiated to detecting
sections SE4, SE5 and SE6 of the sextant photo-detector on
condition that diffracted light is converged in defocus on a second
information medium;
FIG. 42B shows a converging spot of first-order diffracted light
radiated to the detecting sections SE1, SE2 and SE3 of a sextant
photo-detector shown in FIG. 24 and another converging spot of
minus first-order diffracted light radiated to the detecting
sections SE4, SE5 and SE6 of the sextant photo-detector on
condition that diffracted light is converged in focus on a second
information medium;
FIG. 43 is a constitutional view of an optical head apparatus
according to a twelfth embodiment;
FIG. 44 is a constitutional view of an optical head apparatus
according to a thirteenth embodiment;
FIG. 45 is a constitutional view of an optical head apparatus
according to a fourteenth embodiment;
FIG. 46 is a plan view of a hologram lens utilized in the optical
head apparatus shown in FIG. 45;
FIG. 47 is a constitutional view of an optical head apparatus
according to a fifteenth embodiment;
FIG. 48 is a plan view of a hologram lens utilized in the optical
head apparatus shown in FIG. 47;
FIGS. 49A, 49B respectively show a positional relation between
unnecessary light occurring in the hologram lens shown in FIG. 48
and a photo detector shown in FIG. 47;
FIG. 50 is a constitutional view of an optical head apparatus
according to a sixteenth embodiment;
FIG. 51 is a diagonal view of a light source and photo detectors
utilized in the optical head apparatus shown in
FIG. 50;
FIG. 52 is a constitutional view of an optical head apparatus
according to a seventeenth embodiment;
FIG. 53 is a diagonal view of a high density optical disk according
to an eighteenth embodiment, a cross sectional view of the disk
being partially shown;
FIG. 54 is a diagonal view of a high density optical disk according
to a nineteenth embodiment, a cross sectional view of the disk
being partially shown;
FIG. 55 is a block diagram of an optical disk apparatus with one of
the optical head apparatuses shown in FIGS. 21, 27, 30, 31, 32, 33,
37, 38, 40A, 43, 44, 50 and 52 according to a twentieth
embodiment;
FIG. 56 is a flow chart showing the operation of the optical disk
apparatus shown in FIG. 55;
FIG. 57 is a block diagram of an optical disk apparatus with one of
the optical head apparatuses shown in FIGS. 21, 27, 30, 31, 32, 33,
37, 38, 40A, 43, 44, 50 and 52 according to a twenty-first
embodiment;
FIG. 58 is a flow chart showing the operation of the optical disk
apparatus shown in FIG. 57;
FIG. 59 is a constitutional view of a binary focus microscope
according to a twenty-second embodiment;
FIG. 60 is a partial view of the binary focus microscope shown in
FIG. 59 in cases where first and second samples are located at
bottoms of sample holders;
FIG. 61 is a constitutional view of a binary focus microscope
according to a modification of the twenty-second embodiment;
FIG. 62 is a constitutional view of an alignment apparatus
according to a twenty-third embodiment; FIG. 63 is a constitutional
view of the optical disk apparatus of which the block diagram is
shown in FIG. 55;
FIG. 64 is a constitutional view of an exposure apparatus in which
the alignment apparatus is included;
FIG. 65 is a diagonal view of an image reproducing apparatus for
which the optical disk apparatus 176 is provided;
FIG. 66 is a diagonal view of a voice reproducing apparatus for
which the optical disk apparatus 176 is provided;
FIG. 67 is a diagonal view of an information processing apparatus
for which the optical disk apparatus 176 is provided; and
FIG. 68 is a diagonal view of another information processing
apparatus for which the optical disk apparatus 176 is provided.
DETAIL DESCRIPTION OF THE PREFERRED EMBODIMENTS
Preferred embodiments of a compound objective lens, an imaging
optical system, an optical head apparatus, an optical disk, an
optical disk apparatus, a binary focus microscope and an alignment
apparatus according to the present invention are described with
reference to drawings.
(First Embodiment)
FIG. 4A is a constitutional view of an imaging optical system
having a compound objective lens according to a first embodiment of
the present invention, a beam of transmitted light not diffracted
being converged on a thin type of information medium. FIG. 4B is a
constitutional view of the imaging optical system shown in FIG. 4A,
a beam of first-order diffracted light being converged on a thick
type of information medium. FIG. 5 is a plan view of a hologram
lens shown in FIGS. 4A, 4B, a grating pattern of the hologram lens
being depicted.
As shown in FIGS. 4A, 4B, an imaging optical system 21 for
converging light on a first substrate 22 of a thin type of first
information medium 23 (a thickness T1) or a second substrate 24 of
a thick type of second information medium 25 (a thickness T2) to
form a diffraction-limited converging spot comprises a blazed
hologram lens 26 for transmitting a part of incident light L3
radiated from a light source without any diffraction to form a beam
of transmitted light L4 and diffracting a remaining part of the
incident light L3 to form a beam of first-order diffracted light
L5, and an objective lens 27 for converging the transmitted light
L4 on the first information medium 23 or converging the first-order
diffracted light L5 on the second information medium 25.
The first information medium 23 represents a prospective optical
disk having a high density memory capacity, and the thickness T1 of
the first information medium 23 ranges from 0.4 mm to 0.8 mm. The
second information medium 25 represents a compact disk or a laser
disk appearing on the market now, and the thickness T2 of the
second information medium 25 is about 1.2 mm.
The term "convergence" denotes in this specification that divergent
light or collimated light is focused to form a diffraction-limited
micro spot.
In the above configuration, a part of incident light L3 collimated
transmits through the hologram lens 26 without any diffraction, and
a beam of transmitted light L4 (that is, a beam of zero-order
diffracted light L4) is formed. Thereafter, the transmitted light
L4 is converged by the objective lens 27. Also, a remaining part of
the incident light L3 is diffracted and refracted by the hologram
lens 26, and a beam of first-order diffracted light L5 is formed.
In this case, the hologram lens 26 selectively functions as a
concave lens for the first-order diffracted light L5, so that the
first-order diffracted light L5 diverges from the hologram lens 26.
Thereafter, the first-order diffracted light L5 is converged by the
objective lens 27.
In cases where the thin type of first information medium 23 is
utilized to record or reproduce pieces of information on or from a
front surface of the medium 23, as shown in FIG. 4A, the
transmitted light L4 is incident on a rear surface of the first
information medium 23 and is focused on its front surface by the
objective lens 27 to form a diffraction-limited converging spot S1
on the first information medium 23. In contrast, in cases where the
thick type of second information medium 25 is utilized to record or
reproduce pieces of information on or from a front surface of the
medium 25, the diffracted light L5 is incident on a rear surface of
the second information medium 25 and is focused on its front
surface to form a diffraction-limited converging spot S2 on the
second information medium 25. Because the hologram lens 26
functions as a concave lens to diverge the first-order diffracted
light L5, the diffraction-limited converging spots S1, S2 are
formed even though the thickness T1 of the first information medium
23 differs from the thickness T2 of the second information medium
25. Therefore, a compound objective lens 29 composed of the
hologram lens 26 and the objective lens 27 has substantially two
focal points.
As shown in FIG. 5, the hologram lens 26 is formed by drawing a
grating pattern P1 in a pattern region 26A of a transparent
substrate 28 in a concentric circle shape. The pattern region 26A
is positioned in a center portion of the transparent substrate 28,
and a no-pattern region 26B is positioned in a peripheral portion
of the transparent substrate 28 to surround the pattern region 26A.
An optical axis of the imaging optical system 21 passes through a
central point of the grating pattern P1 and a central axis of the
objective lens 27.
In addition, as shown in FIG. 6, the grating pattern P1 of the
hologram lens 26 is formed in relief to produce a phase modulation
type of hologram lens. That is, blocks which each are composed of a
bottom portion and a top portion are concentrically formed in the
grating pattern P1. The height H of the relief in the grating
pattern P1 is set to: H<.lamda./(n(.lamda.)-1), (1) where the
symbol .lamda.denotes a wavelength of the incident light L3 and the
symbol n(.lamda.) denotes a refractive index of the transparent
substrate 28 for the incident light L3. In this case, a difference
in phase modulation degree between the incident light L3
transmitting through a bottom portion of the grating pattern P1 and
the incident light L3 transmitting through a top portion of the
grating pattern P1 is lower than 2.pi. radians. Therefore, a
diffraction efficiency of the hologram lens 26 for the incident
light L3 transmitting through the grating pattern P1 is less than
100% to generate the light L4 transmitting through the grating
pattern P1. Also, the incident light L3 transmitting through the
no-pattern region 26B is not diffracted. As a result, the intensity
of the transmitted light L4 can be sufficient to record or
reproduce pieces of information on or from the first information
medium 23.
Also, because the intensity of the transmitted light L4 is
sufficient over the entire surface of the hologram lens 26,
secondary maxima (side lobes) of the transmitted light L4
undesirably occurring in the converging spot S1 can be suppressed.
In detail, as an intensity distribution of the transmitted light L4
converged on the converging spot S1 is shown in FIG. 7, a primary
maximum (a main lobe) of the transmitted light L4 positioned in a
center of the converging spot S1 is utilized to record or reproduce
a piece of information on or from the first information medium 23,
and secondary maxima positioned around the primary maximum are
unnecessary because the secondary maxima deteriorate a recording
pit or a reproducing signal formed by the primary maximum.
The grating pattern P1 of hologram lens 26 formed in relief is
blazed as shown in FIG. 6, so that the occurrence of minus
first-order diffracted light is considerably suppressed. Therefore,
the intensity sum of the transmitted light L4 and the first-order
diffracted light L5 is maximized. In other words, a utilization
efficiency of the incident light L3 is enhanced.
The numerical aperture NA of the objective lens 27 is equal to or
more than 0.6. Also, when the transmitted light L4 is converged by
the objective lens 27, the diffraction-limited converging spot S1
is formed on the first information medium 23 having a thickness
T1.
A diameter of the hologram lens 26 is almost the same as an
aperture of the objective lens 27, so that a diameter of the
pattern region 26A is smaller than the aperture of the objective
lens 27. Because the incident light L3 transmitting through the
no-pattern region 26B is not diffracted, not only the light L4
transmitting through the pattern region 26A but also the light L4
transmitting through the no-pattern region 26B are converged on the
first information medium 23 by the objective lens 27 having a high
numerical aperture. Therefore, the intensity of the transmitted
light L4 converged at the converging point S1 can be increased. In
contrast to the transmitted light L4, only the incident light L3
transmitting through the pattern region 26A of the hologram lens 26
is changed to the first-order diffracted light L5, and the
first-order diffracted light L5 is converged on the second
information medium 25 by the objective lens 27 having substantially
a low numerical aperture.
The phase of the light L4 transmitting through the grating pattern
P1 of the pattern region 26A is determined by an average value of
the phase modulation degrees in the light L4 transmitting through
the bottom and top portions of the grating pattern P1. In contrast,
because the height of the no-pattern region 26B is constant, the
phase of the light L4 transmitting through the no-pattern region
26B is modulated at a phase modulation degree. Therefore, as shown
in FIG. 6, the height of the no-pattern region 26B is set even with
an average height of the grating pattern P1 to enhance the
convergence function of the objective lens 27.
For example, as shown in FIG. 8A, in cases where each block of the
grating pattern P1 in the hologram lens 26 shown in FIG. 6
approximates to a step-wise shape composed of four stairs, a first
step is etched at a depth h1+h2 and a width W1, a second step is
etched at a depth hi and a width W2, a third step is etched at a
depth h2 and a width W2, and a fourth step is etched at a width W1.
Therefore, the grating pattern P1 approximating to the step-wise
shape is formed in the pattern region 26A. Thereafter, a peripheral
portion of the transparent substrate 28 is etched by a depth h1 or
h2 to form the no-pattern region 26B. Therefore, the height of the
no-pattern region 26B is almost the same as an average height of
the pattern region 26A, so that the phase of the light L4
transmitting through the pattern region 26A is almost the same as
that of the light L4 transmitting through the no-pattern region
26B.
In addition, as shown in FIG. 8B, an ideal blazed shape of the
hologram lens 26 shown in FIG. 6 can approximate to a step-wise
shape which is obtained by etching a center portion of the
transparent substrate 28 many times. In this case, the height H0 of
the step-wise shape is set to satisfy an equation
H0<.lamda./(n(.lamda.)-1) so that the difference in phase
modulation degree is set to a value lower than 2x radians.
Specifically, in cases where the step-wise shape of the hologram
lens 26 is composed of a flight of N stairs having the same
difference no in level, the difference n.sub.o in level is set to
satisfy an equation n.sub.o<.lamda./I{(n(.lamda.)-1)*N} to set
the difference in phase modulation degree of each stairs to a value
lower than 2x/N radians. A peripheral portion of the transparent
substrate 28 is etched to set the thickness of the no-pattern
region 26B to a thickness of the pattern region 26A at one of the N
stairs which is not the top stair or the bottom stair. Therefore,
the height of the no-pattern region 26B is almost the same as an
average height of the pattern region 26A, so that the phase of the
light L4 transmitting through the pattern region 26A is almost the
same as that of the light L4 transmitting through the no-pattern
region 26B.
The grating pattern P1 of the hologram lens 26 is designed to
correct any aberration occurring in the objective lens 27 and the
second information medium 25, so that the first-order diffracted
light L5 transmits through the second information medium 25 having
a thickness T2 and is converged on the medium 25 to form the
diffraction-limited converging spot S2 without any aberration. A
method for designing the hologram lens 26 having an aberration
correcting function is described.
After the first-order diffracted light L5 is converged on the
second information medium 25, spherical waves diverge from the
converging spot S2 and transmit through the second substrate 24 and
the objective lens 27. Thereafter, the spherical waves transmit
through the transparent substrate 28 and optically interfere with
the incident light L3. Therefore, an interference pattern is formed
by the interference between the spherical waves and the incident
light L3. The interference pattern can be calculated by subtracting
the phase of the spherical waves from an inverted phase obtained by
inverting the phase of the incident light L3. Accordingly, the
grating pattern P1 of the hologram lens 26 which agrees with the
interference pattern calculated can be easily formed according to a
computer generated hologram technique.
Accordingly, because the compound objective lens 29 is composed of
the objective lens 27 and the hologram lens 26 in which a part of
the incident light L3 is diffracted and refracted, a
diffraction-limited converging spot can be reliably formed on an
information medium regardless of whether the information medium has
a thickness T1 or a thickness T2. Also, two diffraction-limited
converging spots can be simultaneously formed on an information
medium at difference depths. In other words, the compound objective
lens has substantially two focal points.
Also, because the diffraction efficiency of the hologram lens 26 is
less than 100% and the intensity of the light L4 transmitting
through the hologram lens 26 is sufficient to record or reproduce
information on or from the first information medium 23, the
secondary maxima of the transmitted light L4 converged on the
converging spot S1 can be suppressed.
Also, because the hologram lens 26 is blazed, the occurrence of
minus first-order diffracted light can be considerably suppressed.
Therefore, the intensity sum of the transmitted light L4 and the
first-order diffracted light L5 can be maximized, and a utilization
efficiency of the incident light L3 can be enhanced.
Also, because the hologram lens 26 functions as a lens only for the
first-order diffracted light, the position of the converging point
S1 formed by the transmitted light L4 differs from that of the
converging point S2 formed by the first-order diffracted light L5
in an optical axis direction. Therefore, when the transmitted light
L4 is converged in focus on an information recording plane of the
information medium 23 to record or read a piece of information, the
first-order diffracted light L5 converged on the information medium
23 is out of focus at the information recording plane. In the same
manner, when the first-order diffracted light L5 is converged in
focus on an information recording plane of the information medium
25, the transmitted light L4 converged on the information medium 25
is out of focus at the information recording plane. Accordingly,
when the light L4 (or L5) is converged on the converging spot S1
(or S2) in focus to record or read the information, the light L5
(or L4) not converged on the converging spot S1 (or S2)in focus
does not adversely influence on the recording or reading of the
information. To reliably prevent the adverse influence on the
recording or reading of the information, a difference in the
optical axis direction between the converging spots S1, S2 is
required to be equal to or more than 50 .mu.m. That is, when the
difference is equal to or more than 50 .mu.m, the light L5 (or L4)
largely diverges to reduce the intensity of the light L5 (or L4) at
an information recording plane when the light L4 (or L5) is
converged on the converging spot S1 (or S2) of the information
recording plane at a high intensity.
Also, because the thickness T2 of the second information medium 25
representing the compact disk or the laser disk is about 1.2 mm and
because the thickness T1 of the first information medium 23
representing a prospective optical disk ranges from 0.4 mm to 0.8
mm, the difference in the optical axis direction between the
converging points S1, S2 is required to be equal to or less than
1.0 mm by considering a moving range of an actuator with which the
position of the compound objective lens 29 composed of the
objective lens 27 and the hologram lens 26 is adjusted according to
a focus servo signal. Because the hologram lens 26 functions as a
concave lens for the first-order diffracted light, the difference
between the converging points S1, S2 can be increased to about 1
mm.
Accordingly, even though the transmitted light L4 and the
first-order diffracted light L5 are simultaneously converged by the
objective lens 27, no adverse influence is exerted on the recording
or reproduction of the information on condition that the difference
between the converging points S1, S2 ranges from 50 .mu.m to 1
mm.
Examples of the utilization of the imaging optical system 21 for
various types of optical disks are described.
In cases where the image optical system 21 is utilized for an
optical disk device in which pieces of information recorded in a
thin type of high density optical disk and a thick type of compact
disk are exclusively reproduced, the diffraction efficiency of the
hologram lens 26 for changing the incident light L3 to the
diffracted light L5 is set in a range from about 20% to 70%. In
this case, the intensity of the transmitted light L4 converged on
the high density optical disk is almost the same as that of the
first-order diffracted light L5 converged on the compact disk.
Therefore, the output power of the incident light L3 can be
minimized.
Also, in cases where the image optical system 21 is utilized for an
optical disk device in which pieces of information recorded in a
thin type of high density optical disk are recorded or reproduced
and pieces of information recorded in a thick type of optical disk
are exclusively reproduced, the diffraction efficiency of the
hologram lens 26 for changing the incident light L3 to the
first-order diffracted light L5 is set to a value equal to or lower
than 30%. In this case, even though a high intensity of transmitted
light L4 is required to record a piece of information on the high
density optical disk, the recording of the information can be
reliably performed without increasing the intensity of the incident
light L3 because a transmission efficiency of the hologram lens 26
for the incident light L3 is high. In other words, a utilization
efficiency of the incident light L3 can be enhanced when a piece of
information is recorded on the high density optical disk, so that
the output power of the incident light L3 can be minimized.
In the first embodiment, the hologram lens 26 functions as a
concave lens for the first-order diffracted light L5. However, it
is applicable that a hologram lens 26M functioning as a convex lens
for the first-order diffracted light L5 be utilized in place of the
hologram lens 26. That is, as shown in FIGS. 9A, 9B, the diffracted
light L5 is converged on the first information medium 23 by the
objective lens 27 to form the diffraction limited converging spot
S1, and the transmitted light L4 is converged on the second
information medium 25 by the objective lens 27 to form the
diffraction limited converging spot S2. In this case, the
difference between the converging points S1, S2 is required to be
equal to or less than 0.5 mm by considering the moving range of the
actuator. However, the occurrence of a chromatic aberration can be
prevented in an imaging optical system 21M in which the hologram
lens 26M functioning as a concave lens for the diffracted light L5
is utilized. The achromatization function in the imaging optical
system is described in detail.
When a focal length of the hologram lens 26M for the incident light
L3 having a wavelength .lamda..sub.o is represented by f.sub.Ho and
another focal length of the hologram lens 26M for the incident
light L3 having a wavelength .lamda..sub.r is represented by
f.sub.Hn an equation (2) is satisfied.
f.sub.Hf-f.sub.Ho.times..lamda..sub.of.lamda..sub.l (2)
The focal length fH of the hologram lens 22 is shortened as the
wavelength .lamda. of the incident light L3 becomes longer. Also,
when a refractive index of the objective lens 27 for the incident
light L3 having a wavelength .lamda..sub.o is represented by
n(.lamda..sub.o) and another refractive index of the objective lens
27 for the incident light L3 having a wavelength .lamda..sub.l is
represented by n(.lamda..sub.l), a focal length f.sub.D(.lamda.) of
the objective lens 27 for the incident light L3 having a wavelength
.lamda. is formulated by an equation (3).
f.sub.D(.lamda..sub.l)=f.sub.D(.lamda..sub.o).times.(n(.lamda..sub.o)-1)/-
(n(.lamda..sub.l)-1) (3)
The focal length f.sub.D(.lamda.) of the objective lens 27 is
lengthened as the wavelength .lamda. of the incident light L3
becomes longer. That is, the dependence of the focal length
f.sub.D(.lamda.) on the wavelength .lamda. in the objective lens 27
is opposite to that of the focal length f.sub.H on the wavelength
.lamda. in the hologram lens 26M. Therefore, a condition that the
compound objective lens 29M composed of the objective lens 27 and
the hologram lens 26M functions as an achromatic lens is formulated
by an equation (4).
1/f.sub.Ho+1/f.sub.D(.lamda..sub.o)=1/f.sub.Hf+1/(f.sub.D(.lamda..sub.f)=-
1/(f.sub.Ho.times..lamda..sub.of.pi..sub.f)+(n(.lamda..sub.f)-1)/{f.sub.D(-
.lamda..sub.n).times.(n(.lamda..sub.o)-1)} (4)
Accordingly, because the dependence of the focal length
f.sub.D(.lamda.) on the wavelength .lamda. in the objective lens 27
is opposite to that in the hologram lens 22, the compound objective
lens 29M having an achromatic function can be formed by the
combination of the lenses 26M, 27, and the occurrence of the
chromatic aberration can be prevented. Also, even though the
equation (4) is not strictly satisfied, the occurrence of the
chromatic aberration can be largely suppressed.
Also, a curvature of the objective lens 27 can be small because the
hologram lens 26M functions as a convex lens for the first-order
diffracted light L5. Also, because the hologram lens 26M is a plane
type of element, a lightweight type of compound objective lens
having an achromatic function can be made in large scale
manufacture. A principal of the achromatization has been proposed
in a first literature (D. Faklis and M. Morris, Photonics
Spectra(1991), November p.205 & December p. 131), a second
literature (M. A. Gan et al., S.P.I.E.(1991), Vol.1507, p. 116),
and a third literature (P. Twardowski and P. Meirucis,
S.P.I.E.(1991), Vol.1507, p.55).
(Second Embodiment)
FIG. 10A is a constitutional view of an imaging optical system
having a compound objective lens according to a second embodiment
of the present invention, a beam of transmitted light not
diffracted being converged on a thin type of information medium.
FIG. 10B is a constitutional view of the imaging optical system
shown in FIG. 10A, a beam of first-order diffracted light being
converged on a thick type of information medium.
As shown in FIGS. 10A, 10B, an imaging optical system 31 for
converging light on the first substrate 22 of the first information
medium 23 (the thickness T1) or the second substrate 24 of the
second information medium 25 (the thickness T2) to form a
diffraction-limited converging spot, comprises a blazed hologram
lens 32 for transmitting a part of incident light L3 without any
diffraction to form a beam of transmitted light L4 and diffracting
a remaining part of incident light L3 to form a beam of first-order
diffracted light L5, and the objective lens 27 for converging the
transmitted light L4 on the first information medium 23 or
converging the first-order diffracted light L5 on the second
information medium 25.
The hologram lens 32 is formed by drawing a grating pattern P2 in a
pattern region 32A of the transparent substrate 28 in a concentric
circle shape. The pattern region 32A is positioned in a center
portion of the transparent substrate 28. An diameter of the grating
pattern P2 is equal to or larger than an aperture of the objective
lens 27. Also, a diffraction efficiency of the hologram lens 32 for
the incident light L3 transmitting through the grating pattern P2
is less than 100% in the same manner as in the first embodiment, so
that the intensity of the transmitted light L4 is sufficient to
record or reproduce a piece of information on or from the first
information medium 23.
In addition, as shown in FIG. 11, the diffraction efficiency in a
central portion of the pattern region 32A is high, and the
diffraction efficiency is gradually decreased toward an outer
direction of the pattern region 32A. In other words, in cases where
the grating pattern P2 of the hologram lens 32 is formed in relief,
the height H of the relief in the grating pattern P2 is gradually
lowered toward the outer direction of the pattern region 32A. Or,
in cases where an ideal blazed shape of the hologram lens 26
approximates to a step-wise shape, each block of the grating
pattern P2 positioned in the central portion of the transparent
substrate 28 is formed in a step-wise shape shown in FIG. 12A in
which an inclined angle .theta..sub.1 of stairs is large and a
relationship W1>W2 between a first etching width W1 and a second
etching width W2 is satisfied, and the grating pattern P2 formed in
the step-wise shape shown in FIG. 12A is gradually changed by
decreasing the first etching width W1 and increasing the second
etching width W2 toward the outer direction of the pattern region
32A while the height H of the grating pattern P2 is gradually
decreased. Therefore, each block of the grating pattern P2
positioned in a peripheral portion of the transparent substrate 28
is formed in a step-wise shape shown in FIG. 12B in which an
inclined angle 82 of stairs is small and a relationship W1<W1
between the etching widths is satisfied. Also, each block of the
grating pattern P2 positioned in a middle portion between the
central and peripheral portions is formed in a step-wise shape
shown in FIG. 12C in which the etching widths W1, W2 is the
same.
In the above configuration of the imaging optical system 31, a part
of the incident light L3 transmits through the hologram lens 32
without any diffraction to form a beam of transmitted light L4, and
the transmitted light L4 is converged by the objective lens 27.
Also, a remaining part of the incident light L3 is diffracted and
refracted by the hologram lens 32. In this case, the hologram lens
32 functions as a concave lens for the incident light L3, so that a
first-order diffracted light L5 diverges from the hologram lens 32.
Thereafter, the first-order diffracted light L5 is converged by the
objective lens 27.
In cases where the thin type of first information medium 23 is
utilized to record or reproduce pieces of information on or from a
front surface of the medium 23, as shown in FIG. 10A, the
transmitted light L4 is incident on a rear surface of the first
information medium 23 and is focused on its front surface by the
objective lens 27 to form a diffraction-limited converging spot S3
on the first information medium 23. In this case, because the
diffraction efficiency in the central portion of the grating
pattern P2 is high and because the diffraction efficiency is
gradually decreased toward the outer direction of the grating
pattern P2, a diffraction probability of the incident light L3 is
lowered in the peripheral portion of the grating pattern P2.
Therefore, the light L4 transmits through the objective lens 27 on
condition that the numerical aperture NA of the objective lens 27
is high.
In contrast, in cases where the thick type of second information
medium 25 is utilized to record or reproduce pieces of information
on or from a front surface of the medium 25, the diffracted light
L5 is incident on a rear surface of the second information medium
25 and is focused on its front surface to form a
diffraction-limited converging spot S5 on the second information
medium 25. In this case, because the hologram lens 32 functions as
a concave lens to diverge the first-order diffracted light L5, the
diffraction-limited converging spots S3, S4 are formed even though
the thickness T1 of the first information medium 23 differs from
the thickness T2 of the second information medium 25. Therefore, a
compound objective lens 34 composed of the hologram lens 32 and the
objective lens 27 has substantially two focal points.
Accordingly, because the light L4 transmits through the objective
lens 27 on condition that the numerical aperture NA of the
objective lens 27 is high, the intensity of the transmitted light
L4 converged on the first information medium 23 can be high.
Also, in cases where the incident light L3 is radiated from a
semiconductor laser, a far field pattern of the incident light L3
is distributed in a Gaussian distribution as shown in FIG. 13A.
Therefore, because the diffraction efficiency is gradually
decreased toward the outer direction of the grating pattern P2, a
far field pattern of the transmitted light L4 is distributed in a
gently-sloping shape as shown in FIG. 13B. In contrast to the
second embodiment, because the incident light L3 is not diffracted
in the no-pattern region 26b of the hologram lens 26 in the first
embodiment, the intensity of the transmitted light L4 is suddenly
increased at the peripheral portion of the hologram lens 26.
Accordingly, secondary maxima of the transmitted light L4 converged
on the converging spot S3 can be moreover suppressed in the second
embodiment as compared with in the first embodiment. That is, the
recording and reproducing of the information can be performed
without any deterioration of the information by utilizing the
imaging optical system 31.
In addition, in cases where the first-order diffracted light L5 is
converged on the second information medium 25 to form the
diffraction-limited converging spot S4 , a numerical aperture of
the objective lens 27 for the first-order diffracted light L5 is
low because the diffraction efficiency of the hologram lens 32 is
decreased toward an outer direction of the pattern region 32A. As a
result, the intensity of the first-order diffracted light L5
becomes lowered. In cases where the diffraction efficiency of the
hologram lens 32 is heightened to increase the intensity of the
first-order diffracted light L5, the intensity of the transmitted
light L4 at its inner beam portion is largely decreased, and
secondary maxima (or side lobes) of the transmitted light L4 at the
converging spot S3 is undesirably increased. Therefore, the
incident light L3 of which the far field pattern is distributed in
the Gaussian distribution is radiated to the hologram lens 32 to
increase the intensity of the first-order diffracted light L5
without any increase of the second maxima. In detail, as shown in
FIG. 14A, the incident light L3 distributed not only in a central
portion of the Gaussian distribution but also in a peripheral
portion of the Gaussian distribution transmits through the hologram
lens 32 and is refracted by the objective lens 27 because the
diameter of the grating pattern P2 is equal to or larger than the
aperture of the objective lens 27. Therefore, a numerical aperture
NA of the objective lens 27 at a light source side for the incident
light L3 becomes higher than that in the first embodiment, and the
diffraction efficiency of the hologram lens 32 is heightened. As a
result, the intensity of the first-order diffracted light L5
converged on the second information medium 25 can be increased, as
shown in FIG. 14B. Also, because the intensity of the incident
light L3 at the peripheral portion of the Gaussian distribution is
low and because the diffraction efficiency of the hologram lens 32
is increased toward the inner direction of the grating pattern
region 32A, intensity of the transmitted light L4 is distributed in
a gently-sloping shape as shown in FIG. 14C. Accordingly, secondary
maxima of the transmitted light L4 at the converging spot S3 can be
suppressed.
Examples of the utilization of the imaging optical system 31 for
various types of optical disks are described.
In cases where the image optical system 31 is utilized for an
optical disk device in which pieces of information recorded in a
thin type of high density optical disk and a thick type of compact
disk are exclusively reproduced, the diffraction efficiency of the
hologram lens 32 for the incident light L3 is set in a range from
about 20% to 70%. In this case, the intensity of the transmitted
light L4 converged on the high density optical disk is almost the
same as that of the first-order diffracted light L5 converged on
the compact disk. Therefore, the output power of the incident light
L3 can be minimized.
Also, in cases where the image optical system 31 is utilized for an
optical disk device in which pieces of information recorded in a
thin type of high density optical disk are recorded or reproduced
and pieces of information recorded in a thick type of optical disk
are exclusively reproduced, the diffraction efficiency of the
hologram lens 32 for the incident light L3 is set to a value equal
to or lower than 30%. In this case, even though a high intensity of
transmitted light L4 is required to record a piece of information
on the high density optical disk, the recording of the information
can be reliably performed without increasing the intensity of the
incident light L3 because a transmission efficiency of the hologram
lens 32 for the incident light L3 is high. In other words, a
utilization efficiency of the incident light L3 can be enhanced
when a piece of information is recorded on the high density optical
disk, so that the output power of the incident light L3 can be
minimized.
In the second embodiment, the grating pattern P2 positioned in the
central portion of the transparent substrate 28 is gradually
changed toward the outer direction of the pattern region 32A from
the step-wise shape shown in FIG. 12A to the step-wise shape shown
in FIG. 12B through the step-wise shape shown in FIG. 12C. However,
because the occurrence of unnecessary diffracted light such as
minus first-order diffracted light can be effectively prevented in
the middle portion of the transparent substrate 28 in which the
grating pattern P2 is formed in the step-wise shape shown in FIG.
12C, it is preferred that the middle portion occupy a large part of
the pattern region 32A of the hologram lens 32. In this case, the
intensity sum of the transmitted light L4 and the first-order
diffracted light L5 can be maximized, so that a utilization
efficiency of the incident light L3 can be enhanced.
Also, because the first etching width W1 of the grating pattern P2
is gradually decreased toward the outer direction of the pattern
region 32A, it is applicable that the grating pattern P2 formed in
the step-wise shape shown in FIG. 12B be changed to a step-wise
shape shown in FIG. 12D when the first width W1 is decreased to a
value lower than about 1 .mu.m. That is, a flight of four stairs
shown in FIG. 12B is changed to a flight of two stairs. In this
case, the grating pattern P2 formed in the step-wise shape shown in
FIG. 12D can be easily made. In addition, in cases where a height
H4 of the grating pattern P2 formed in the step-wise shape shown in
FIG. 12D is moreover decreased toward the outer direction of the
pattern region 32A, it is preferred that the grating pattern P2 be
formed in a step-wise shape shown in FIG. 12E. That is, a third
etching width W3 is gradually decreased toward the outer direction
of the pattern region 32A while decreasing a height H5 of the
grating pattern P2. Therefore, the diffraction efficiency of the
hologram lens 32 can be gradually decreased toward the outer
direction of the pattern region 32A without any manufacturing
difficulty of the grating pattern P2.
In addition, as shown in FIG. 15A, it is applicable that a hologram
lens 33 be formed, in place of the hologram lens 32, by placing the
grating pattern P1 of the pattern region 32A in a central portion
of the transparent substrate 28 and placing four types of
diffraction regions 33A, 33B, 33C and 33D which surround the
grating pattern P1. A part of the incident light L3 transmitting
through each of the diffraction regions 33A to 33D is diffracted to
control a transmission efficiency of the hologram lens 33. In this
case, the intensity of the transmitted light L4 at its peripheral
portion is decreased, so that secondary maxima occurring in the
converging spot S3 can be suppressed. Also, it is applicable that
the grating pattern P1 of the hologram be replaced with the grating
pattern P2. Also, it is applicable that grating directions of the
diffraction regions 33A to 33D differ from each other. In this
case, even though the first-order diffracted light L5 diffracted in
the diffraction region 33A is, for example, incident on the
diffraction region 33c after the diffracted light L5 is reflected
by the second information medium 25, the diffracted light L5 again
diffracted in the diffraction region 33c does not pass in parallel
to the optical axis. Therefore, in cases where a piece of
information read from the second information medium 25 is detected
in a detector to reproduce the information, the first-order
diffracted light L5 diffracted in the diffraction regions 33A to
33D is not detected by the detector as stray light. Accordingly,
the reproduction of the information does not deteriorate.
Also, as shown in FIG. 15B, it is applicable that the hologram lens
32 function as a convex lens. In this case, the diffracted light L5
is converged on the first information medium 23, and the
transmitted light LA is converged on the second information medium
25, as shown in FIG. 15C.
(Third Embodiment)
FIG. 16A is a constitutional view of an imaging optical system
having a compound objective lens according to a third embodiment of
the present invention, a beam of first-order diffracted light being
converged on a thin type of information medium. FIG. 16B is a
constitutional view of the imaging optical system shown in FIG.
16A, a beam of transmitted light not diffracted being converged on
a thick type of information medium.
As shown in FIGS. 16A, 16B, an imaging optical system 41 for
converging light on the first substrate 22 of the first information
medium 23 (the thickness T1) or the second substrate 24 of the
second information medium 25 (the thickness T2) to form a
diffraction-limited converging spot comprises a blazed hologram
lens 42 for transmitting a part of incident light L3 without any
diffraction to form a beam of transmitted light L4 and diffracting
a remaining part of incident light L3 to form a beam of first-order
diffracted light L6, and the objective lens 27 for converging the
first-order diffracted light L6 on the first information medium 23
or converging the transmitted light LA on the second information
medium 25.
The hologram lens 42 is formed by drawing a grating pattern P3 in a
pattern region 42A of the transparent substrate 28 in a concentric
circle shape. The pattern region 42A is positioned in a center
portion of the transparent substrate 28. An diameter of the grating
pattern P3 is equal to or larger than an aperture of the objective
lens 27. Also, a diffraction efficiency of the hologram lens 42 for
the incident light L3 transmitting through the grating pattern P3
is less than 100% in the same manner as in the first embodiment, so
that the intensity of the transmitted light L4 is sufficient to
record or reproduce a piece of information on or from the second
information medium 25.
In addition, as shown in FIG. 17, the diffraction efficiency of the
hologram lens 42 is high in a peripheral portion of the pattern
region 42A, and the diffraction efficiency is gradually decreased
toward an inner direction of the pattern region 42A. In other
words, in cases where the grating pattern P3 of the hologram lens
42 is formed in relief, the height H of the relief in the grating
pattern P3 is gradually lowered toward the inner direction of the
pattern region 42A. Or, in cases where an ideal blazed shape of the
hologram lens 26 approximates to a step-wise shape, each pitch of
the grating pattern P3 positioned in the peripheral portion of the
transparent substrate 28 is formed in a step-wise shape shown in
FIG. 12A in which the inclined angle 81 of stairs is large and the
relationship Wl>W2 between the first and second etching widths
W1, W2 is satisfied, and the grating pattern P3 formed in the
step-wise shape shown in FIG. 12A is gradually changed by
decreasing the first etching width W1 and increasing the second
etching width W2 toward the inner direction of the pattern region
42A while the height H of the grating pattern P3 is gradually
decreased. Therefore, each pitch of the grating pattern P3
positioned in a central portion of the transparent substrate 28 is
formed in a stepwise shape shown in FIG. 12B in which the inclined
angle 82 of stairs is small and the relationship W1<W2 is
satisfied. Also, each pitch of the grating pattern P3 positioned in
a middle portion between the central and peripheral portions is
formed in a step-wise shape shown in FIG. 12C in which the etching
widths W1, W2 is the same.
In the above configuration of the imaging optical system 41, as
shown in FIG. 16B, a part of the incident light L3 transmits
through the hologram lens 42 without any diffraction to form a beam
of transmitted light L4, and the transmitted light L4 is converged
by the objective lens 27. Also, a remaining part of the incident
light L3 is diffracted by the hologram lens 42 to form a beam of
first-order diffracted light L6. In this case, the hologram lens 42
functions as a convex lens for the incident light L3, so that a
first-order diffracted light L6 formed in the hologram lens 42
converges. Thereafter, the diffracted light L6 is converged by the
objective lens 27.
In cases where the thin type of first information medium 23 is
utilized to record or reproduce pieces of information on or from a
front surface of the medium 23, as shown in FIG. 16A, the
diffracted light L6 is incident on a rear surface of the first
information medium 23 and is focused on its front surface to form a
diffraction-limited converging spot S5 on the first information
medium 23. In contrast, in cases where the thick type of second
information medium 25 is utilized to record or reproduce pieces of
information on or from a front surface of the medium 25, the
transmitted light L4 is incident on a rear surface of the second
information medium 25 and is focused on its front surface to form a
diffraction-limited converging spot S6 on the second information
medium 25.
In this case, because the hologram lens 42 functions as a convex
lens to converge the diffracted light L6, the diffraction-limited
converging spots S5, S6 are formed even though the thickness T1 of
the first information medium 23 differs from the thickness T2 of
the second information medium 25. Therefore, a compound objective
lens 43 composed of the hologram lens 42 and the objective lens 27
has substantially two focal points.
Also, because the hologram lens 42 functions as a convex lens for
the diffracted light L6, the diffracted light L6 transmits through
the objective lens 27 on condition that the numerical aperture NA
of the objective lens 27 is substantially high.
In addition, because the diffraction efficiency in the peripheral
portion of the grating pattern P3 is high and because the
diffraction efficiency is gradually decreased toward the inner
direction of the grating pattern P3, a diffraction probability of
the incident light L3 is higher in the peripheral portion of the
grating pattern P3.
The grating pattern P3 of the hologram lens 42 is designed to
correct any aberration occurring in the objective lens 27 and the
first information medium 23, so that the diffracted light L6
transmits through the first information medium 23 having the
thickness T1 and is converged on the medium 23 to form the
diffraction-limited converging spot S5 without any aberration. A
method for designing the hologram lens 42 having an aberration
correcting function is described.
After the diffracted light L6 is converged on the first information
medium 23, spherical waves diverge from the converging spot S5 and
transmit through the first substrate 22 and the objective lens 27.
Thereafter, the spherical waves transmit through the transparent
substrate 28 and optically interfere with the incident light L3.
Therefore, an interference pattern is formed by the interference
between the spherical waves and the incident light L3. The
interference pattern can be calculated by adding the phase of the
spherical waves to an inverted phase obtained by inverting the
phase of the incident light L3. Accordingly, the grating pattern P3
of the hologram lens 42 which agrees with the interference pattern
calculated can be easily formed according to a computer generated
hologram technique.
Accordingly, because the hologram lens 42 functions as a convex
lens for the first-order diffracted light L6, a curvature of the
objective lens 27 can be lowered. Also, a glass material having a
high refractive index is not required to produce the objective lens
27.
Also, because the first-order diffracted light L6 formed in the
hologram lens 42 converges before the diffracted light L6 is
incident on the objective lens 27, the distance in an optical axis
direction between the converging spots 55, 56 can be lengthened to
about 1 mm. Therefore, even though the transmitted light L4 (or the
first-order diffracted light L6) is converged on the converging
spot S6 (or 55) in focus to record or read a piece of information,
the light L6 (or L4) is not converged on the converging spot S6 (or
55) in focus to reduce the intensity of the light L6 (or L4) at the
converging spot S6 (or S5). Accordingly, no adverse influence is
exerted on the recording or reproduction of the information
Also, because the hologram lens 42 functions as a convex lens for
the first-order diffracted light L6, the occurrence of a chromatic
aberration can be prevented in the imaging optical system 41. In
detail, the focal length of the hologram lens 42 is shortened as
the wavelength of the incident light L3 becomes longer. In
contrast, the focal length of the objective lens 27 is lengthened
as the wavelength of the incident light L3 becomes longer. That is,
the dependence of the focal length on the wavelength in the
objective lens 27 is opposite to that of the focal length on the
wavelength in the hologram lens 42. Therefore, the compound
objective lens 43 having an achromatic function can be formed by
the combination of the lenses 27, 42, and the occurrence of the
chromatic aberration can be prevented.
Also, because the hologram lens 42 is a plane type of element, a
lightweight type of compound objective lens can be made in large
scale manufacture.
Also, because the diffraction efficiency of the hologram lens 42 is
gradually decreased toward an inner direction of the pattern region
42A, the numerical aperture of the objective lens 27 for the
first-order diffracted light L6 becomes substantially enlarged.
Therefore, the intensity of the first-order diffracted light L6 can
be enlarged to record or reproduce a piece of information on or
from the first information medium 23.
Also, in cases where the incident light L3 is radiated from a
semiconductor laser, a far field pattern of the incident light L3
is distributed in a Gaussian distribution as shown in FIG. 13A.
Therefore, because the diffraction efficiency of the hologram lens
42 is gradually decreased toward the inner direction of the grating
pattern P2, a far field pattern of the first-order diffracted light
L6 is distributed in a gently-sloping shape. Accordingly, secondary
maxima of the first-order diffracted light L6 converged on the
converging spot S5 can be moreover suppressed in the third
embodiment as compared with in the first embodiment. That is, the
recording and reproducing of the information can be performed
without any deterioration of the information by utilizing the
imaging optical system 41.
In addition, in cases where the transmitted light L4 is converged
on the second information medium 25 to form the diffraction-limited
converging spot S6 , a numerical aperture of the objective lens 27
for the transmitted light L4 is low because the diffraction
efficiency of the hologram lens 42 is increased toward an outer
direction of the grating pattern 42A. As a result, the intensity of
the transmitted light L4 becomes lowered. In cases where a
transmission efficiency of the hologram lens 42 is heightened to
increase the intensity of the transmitted light L4, the intensity
of the first-order diffracted light L6 at its inner beam portion is
largely decreased, and secondary maxima (or side lobes) of the
first-order diffracted light L6 at the converging spot S6 is
undesirably increased. Therefore, the incident light L3 of which
the far field pattern is distributed in the Gaussian distribution
is radiated to the hologram lens 42 to increase the intensity of
the transmitted light L4 without any increase of the second maxima.
In detail, as shown in FIG. 18A, the incident light L3 distributed
in not only a central portion of the Gaussian distribution but also
a peripheral portion of the Gaussian distribution transmits through
the hologram lens 42 and is refracted by the objective lens 27
because the diameter of the grating pattern P3 is equal to or
larger than the aperture of the objective lens 27. Therefore, a
numerical aperture NA of the objective lens 27 at a light source
side for the incident light L3 becomes higher than that in the
first embodiment, and a transmission efficiency of the hologram
lens 42 is heightened. As a result, the intensity of the
transmitted light L4 converged on the second information medium 25
can be increased, as shown in FIG. 18B. Also, because the intensity
of the incident light L3 at the peripheral portion of the Gaussian
distribution is low and because the diffraction efficiency of the
hologram lens 42 is decreased toward the inner direction of the
grating pattern 42A, the first-order diffracted light L6 is
distributed in a gently-sloping shape as shown in FIG. 18C.
Accordingly, secondary maxima of the first-order diffracted light
L6 at the converging spot S5 can be suppressed.
Examples of the utilization of the imaging optical system 41 for
various types of optical disks are described.
In cases where the image optical system 41 is utilized for an
optical disk device in which pieces of information recorded in a
thin type of high density optical disk and a thick type of compact
disk are exclusively reproduced, the diffraction efficiency of the
hologram lens 42 for the incident light L3 is set in a range from
about 20% to 70%. In this case, the intensity of the transmitted
light L4 converged on the compact disk is almost the same as that
of the first-order diffracted light L6 converged on the high
density optical disk. Therefore, the output power of the incident
light L3 can be minimized.
Also, in cases where the image optical system 41 is utilized for an
optical disk device in which pieces of information recorded in a
thin type of high density optical disk are recorded or reproduced
and pieces of information recorded in a thick type of optical disk
are exclusively reproduced, the diffraction efficiency of the
hologram lens 42 for the incident light L3 is set to a value equal
to or higher than 55%. In this case, even though a high intensity
of the first-order diffracted light L6 is required to record a
piece of information on the high density optical disk, the
recording of the information can be reliably performed without
increasing the intensity of the incident light L3 because the
diffraction efficiency of the hologram lens 42 for changing the
incident light L3 to the first-order diffracted light L6 is high.
In other words, a utilization efficiency of the incident light L3
can be enhanced when a piece of information is recorded on the high
density optical disk, so that the output power of the incident
light L3 can be minimized. Also, because the diffraction efficiency
of the hologram lens 42 is gradually decreased toward an inner
direction of the pattern region 42A, the numerical aperture of the
objective lens 27 for the first-order diffracted light L6 becomes
substantially enlarged. Therefore, the intensity of the first-order
diffracted light L6 can be enlarged to record or reproduce a piece
of information on or from the high density optical disk.
In the third embodiment, the grating pattern P3 positioned in the
pattern region 42A of the transparent substrate 28 is gradually
changed toward the outer direction of the pattern region 42A from
the step-wise shape shown in FIG. 12B to the step-wise shape shown
in FIG. 12A through the stepwise shape shown in FIG. 12C while
increasing the height H of the grating pattern P3. However, because
the occurrence of unnecessary diffracted light such as minus
first-order diffracted light can be effectively prevented in the
middle portion of the transparent substrate 28 in which the grating
pattern P3 is formed in the step-wise shape shown in FIG. 12C, it
is preferred that the middle portion occupy a large part of the
pattern region 42A of the hologram lens 42. In this case, the
intensity sum of the transmitted light L4 and the first-order
diffracted light L6 can be maximized, so that a utilization
efficiency of the incident light L3 can be enhanced.
Also, because the first etching width W1 of the grating pattern P3
is gradually decreased toward the inner direction of the pattern
region 42A, it is applicable that the grating pattern P3 formed in
the step-wise shape shown in FIG. 12B be changed to a step-wise
shape shown in FIG. 12D when the first width W1 is decreased to a
value lower than about 1 .mu.m. In this case, the grating pattern
P3 formed in the step-wise shape shown in FIG. 12D can be easily
made. In addition, in cases where a height H4 of the grating
pattern P3 formed in the step-wise shape shown in FIG. 12D is
moreover decreased toward the inner direction of the pattern region
42A, it is preferred that the grating pattern P3 be formed in a
step-wise shape shown in FIG. 12E. In this case, a third etching
width W3 is gradually decreased toward the inner direction of the
pattern region 42A while decreasing a height H5 of the grating
pattern P3. Therefore, the diffraction efficiency of the hologram
lens 42 can be gradually decreased toward the inner direction of
the pattern region 42A without any manufacturing difficulty of the
grating pattern P3.
In the first to third embodiments of the image optical systems 21,
31 and 41, the grating patterns P1, P2 and P3 of the hologram
lenses 26, 32 and 42 are respectively formed on a front side of the
transparent substrate 28 not facing the objective lens 27.
Therefore, a beam of light reflected at the front side of the
transparent substrate 28 does not adversely influence as stray
light on the recording or reproduction of the information. In
detail, because the reflected light is diffracted by the hologram
lens, the reflected light is scattered. Also, even though the
first-order diffracted light L5 or L6 is reflected at a reverse
side of the transparent substrate 28, the diffracted light
reflected is again diffracted by the hologram lens and is
scattered. Therefore, the light reflected at the front or reverse
side of the hologram lens does not adversely influence on the
recording or reproduction of the information.
However, in cases where an anti-reflection film is coated on a
front side of the hologram lens 28 at which the grating pattern is
not formed, it is applicable that the grating patterns P1, P2 and
P3 of the hologram lenses 26, 32 and 42 be respectively formed on a
reverse side of the transparent substrate 28 facing the objective
lens 27. In this case, because the first-order diffraction light
L5, L6 is not refracted at the front side of the hologram lens 28,
the design of the image optical systems 21, 31 and 41 can be
simplified.
Also, in the first to third embodiments, the grating patterns P1,
P2 and P3 of the hologram lenses 26, 32 and 42 are respectively
formed in relief to produce a phase modulation type of hologram
lens. However, as is described in Provisional Publication No.
189504/86 (561-189504) and Provisional Publication No. 241735/88
(563-241735), the phase modulation type of hologram lens can be
produced by utilizing a liquid crystal cell. Also, the phase
modulation type of hologram lens can be produced by utilizing a
birefringece material such as lithium niobate. For example, the
phase modulation type of hologram lens can be produced by
proton-exchanging a surface part of a lithium niobate
substrate.
(Fourth Embodiment)
Also, in the first to third embodiments, the compound objective
lens 29, 34 or 43 having two focal points is composed of the
objective lens 27 and the hologram lens 26, 32 or 42. However, as a
compound objective lens according to a fourth embodiment is shown
in FIG. 19A, it is preferred that each of the hologram lenses 26,
32 and 42 and the objective lens 27 be unified with a packaging
means 44 to form a compound objective lens 45 in which a relative
position between each of the hologram lenses 26, 32 and 42 and the
objective lens 27 is fixed. In this case, the transmitted light L4
and the first-order diffracted light L5, L6 can be easily converged
on the first or second information medium 23, 25 by adjusting the
position of the packing means 44 with an actuator. Also, as another
compound objective lens according to a modified fourth embodiment
is shown in FIG. 19B, it is preferred that each of the grating
patterns P1, P2 and P3 be directly drawn on a curved side of the
objective lens 27 facing a light source side to form a compound
objective lens 46 in which each of the hologram lenses 26, 32 and
42 is integrally formed with the objective lens 27.
Accordingly, the central axis of the objective lens 27 can always
agree with that of each of the hologram lenses 26, 32 and 42, so
that abaxial aberrations of each of the hologram lenses 26, 32 and
42 such as a coma aberration and an astigmatic aberration occurring
in the first-order diffracted light can be prevented in the fourth
embodiment. Also, because the hologram lens 26, 32 or 42 is placed
on a lens surface of the objective lens 27 of which a curvature is
higher than those of other lens surfaces of the objective lens 27,
a sine condition for the hologram lens treated as a lens can be
easily satisfied. Therefore, the degree of aberrations resulting
from a constitutional error of an optical head apparatus can be
sufficiently reduced.
(Fifth Embodiment)
Also, as a compound objective lens according to a fifth embodiment
is shown in FIG. 20, it is preferred that each of the grating
patterns P1, P2 and P3 be directly drawn on a side of the objective
lens 27 facing the information medium 23 or 25 to form a compound
objective lens 47 in which each of the hologram lenses 26, 32 and
42 is integrally formed with the objective lens 27. In this case, a
curvature at the side of the objective lens 27 can be small or in a
plane shape. Therefore, each of the grating patterns P1, P2 and P3
can be made at a low cost. Also, in cases where an aberration is
caused by tilting the hologram lens from the optical axis, the
aberration can be prevented by fixing the hologram lens and a light
source of the incident light L3 on the same base.
(Sixth Embodiment)
An optical head apparatus with one of the compound objective lenses
29, 29M, 34, 43, 45, 46 and 47 shown in the first to fifth
embodiments is described with reference to FIGS. 21 to 26 according
to a sixth embodiment of the present invention. X, Y and Z
co-ordinates shown in FIGS. 21 to 26 are utilized in common.
FIG. 21 is a constitutional view of an optical head apparatus
according to a sixth embodiment.
As shown in FIG. 21, an optical head apparatus 51 for recording or
reproducing pieces of information on or from the information medium
23 or 25, comprises a light source 52 such as a semiconductor laser
for radiating the incident light L3, a collimator lens 53 for
collimating the incident light L3, a beam splitter 54 for
transmitting the incident light L3 on an outgoing optical path and
reflecting a beam of transmitted light L4 R formed by reflecting
the transmitted light L4 on the information medium 23 or 25 or a
beam of diffracted light L5R (or L6R) formed by reflecting the
diffracted light L5 (or L6) on the information medium 23 or 25 on
an incoming optical path, the compound objective lens 29 (or 29M,
34, 43, 45, 46 or 47) composed of the hologram lens 26 (or 26M, 32,
33 or 42) and the objective lens 27, a converging lens 55 for
converging the transmitted light L4R or the diffracted light L5R
reflected by the beam splitter 54, a wavefront changing device 56
such as a hologram for changing a wavefront of the transmitted
light L4R or the diffracted light L5R to form a plurality of
converging spots of the transmitted light L4R or the diffracted
light L5R, a photo detector 57 for detecting intensities of the
converging spots of the transmitted light L4R or the diffracted
light L5R of which the wavefront is changed by the wavefront
changing device 56 to obtain an information signal recorded on the
information medium 23 or 25 and servo signals such as a focus error
signal and a tracking error signal, and an actuating unit 58 for
moving the compound objective lens composed of the hologram lens 26
and the objective lens 27 according to the servo signals.
In the above configuration, a beam of incident light L3 radiated
from the light source 52 is collimated in the collimator lens 53
and transmits through the beam splitter 54. Thereafter, a part of
the incident light L3 transmits through the compound objective lens
29 without any diffraction, and a remaining part of the incident
light L3 is diffracted.
Thereafter, in cases where a piece of information is recorded or
reproduced on or from the first information medium 23, the
transmitted light L4 is converged on the first information medium
23 to form the first converging spot S1. That is, the transmitted
light LA is incident on a rear surface of the first information
medium 23, and the first converging spot S1 is formed on a front
surface of the first information medium 23. Thereafter, a beam of
transmitted light L4R reflected at the front surface of the first
information medium 23 passes through the same optical path in the
reverse direction. That is, a part of the transmitted light L4R
again transmits through the compound objective lens 29 without any
diffraction and is reflected by the beam splitter 54. In this case,
the transmitted light L4R is collimated. Thereafter, the
transmitted light L4R is converged by the converging lens 55, and
the wavefront of a large part of the transmitted light L4R is
changed to form a plurality of converging spots on the photo
detector 57. Thereafter, the intensities of the converging spots of
the transmitted light L4R are detected in the photo detector 57.
Therefore, an information signal and servo signals such as a focus
error signal and a tracking error signal are obtained. The
actuating unit 58 are operated according to the servo signals to
move the compound objective lens 29 at high speed, so that the
transmitted light L4 is converged on the first information medium
23 in focus.
Also, in cases where a piece of information is recorded or
reproduced on or from the second information medium 25, the
diffracted light L5 is converged on the second information medium
25 to form the second converging spot S2. That is, the diffracted
light L5 is incident on a rear surface of the second information
medium 25, and the second converging spot S2 is formed on a front
surface of the second information medium 25. Thereafter, a beam of
diffracted light L4R reflected at the front surface of the second
information medium 25 passes through the same optical path in the
reverse direction. That is, a part of the diffracted light L5R is
again diffracted by the hologram lens 26 and is reflected by the
beam splitter 54. In this case, the diffracted light L4R is
collimated. Thereafter, the diffracted light L5R is converged by
the converging lens 55, and the wavefront of a large part of the
diffracted light L5R is changed to form a plurality of converging
spots on the photo detector 57. In this case, the diffracted light
L5R incident on the converging lens 55 is collimated in the same
manner as the transmitted light L4R incident on the converging lens
55, the converging spots of the diffracted light L5R are formed at
the same positions as those of the transmitted light L4R.
Thereafter, the intensities of the converging spots of the
diffracted light L5R are detected in the photo detector 57.
Therefore, an information signal and servo signals such as a focus
error signal and a tracking error signal are obtained. The
actuating unit 58 are operated according to the servo signals to
move the compound objective lens 29 at high speed, so that the
diffracted light L5 is converged on the second information medium
25 in focus.
In this case, because the transmitted light L4R again transmits
through the compound objective lens without any diffraction and the
diffracted light L5R is again diffracted by the hologram lens 26,
the outgoing optical path agrees with the incoming optical path in
a range between the information medium 23 or 25 and the beam
splitter 54 even though the converging spot S1 differs from the
converging spot S2. Therefore, a converging spot S7 on the photo
detector 57 at which the light L4R or L5R not diffracted by the
wavefront changing device 56 is converged relates to a radiation
point of the light source 52 in a mirror image, so that the light
LAR and L5R not diffracted by the wavefront changing device 56 are
converged at the same converging point S7. In the same manner, the
light L4R and L5R diffracted by the wavefront changing device 56
are converged at the same other converging points.
Accordingly, even though the compound objective lens has two focal
points, the wavefront changing unit 56 and the photo detector 57
required to detect the intensity of the transmitted light L4R can
be utilized to detect the intensity of the diffracted light L5R.
Therefore, the number of parts required to manufacture the optical
head apparatus 51 can be reduced, and a small sized optical head
apparatus can be manufactured at a low cost and in light weight
even though pieces of information are recorded or reproduced on or
from an information medium by utilizing the optical head apparatus
51 regardless of whether the information medium is thick or
thin.
In cases where the hologram lens 26 (or 32, 33, 42) is integrally
formed with the objective lens 27 as shown in FIG. 19A, 19B or 20,
each of the compound objective lenses 45, 46 and 47 can be
manufactured in light weight because the hologram lens 26 (or 32,
33, 42) is a plane type of optical device. For example, the
hologram lens 26 (or 32, 33, 42) is less than several tens mg in
weight. Therefore, the hologram lens 26 integrally formed with the
objective lens 27 can be easily moved by the actuating unit 58.
Next, a detecting method of the servo signals is described. FIG. 22
is a plan view of the wavefront changing unit 56. FIG. 23 is an
enlarged view of first-order diffracted light and transmitted light
detected in the photo detector 57. As shown in FIG. 22, the
wavefront changing unit 56 is partitioned into as diffracted light
generating region 56a in which a grating pattern P4 is drawn and a
pair of diffracted light generating regions 55b, 56c in which a
pair of grating patterns P5, P6 are drawn. The light L4R or L5R
incident on the diffracted light generating region 56a is
diffracted to obtain a focus error signal. The light L4R or L5R
incident on each of the diffracted light generating regions 56b,
56c is diffracted to obtain a tracking error signal.
Initially, a spot size detection method utilized to detect a focus
error signal is described as an example of a detecting method of a
focus error signal. The method is proposed in Japanese Patent
Application No. 185722 of 1990. In short, in cases where the method
is adopted, an allowable assembly error in an optical head
apparatus can be remarkably enlarged, and the servo signal such as
a focus error signal can be stably obtained to adjust the position
of the compound objective lens even though the wavelength of the
incident light L3 varies.
In detail, as shown in FIG. 23, the grating pattern P4 is designed
to change the transmitted light L4R (or the diffracted light L5R)
transmitting through the diffracted light generating region 56a of
the wavefront changing unit 56 to a beam of first-order diffracted
light L7 and a beam of minus first-order diffracted light LB. The
diffracted light L7, L8 are expressed by two types of spherical
waves having different curvatures. That is, interference fringes
are produced by actually interfering a spherical wave having a
focal point FP1 in the front of the photo detector 57 with another
spherical wave diverging from the converging spot S7 according to a
two-beam interferometric process, so that the grating pattern P4
agreeing with the interference fringes is formed. In other case,
the interference fringes are calculated according to a computer
generated hologram method. As a result, the transmitted light L4R
(or the diffracted light L5R) transmitting through the diffracted
light generating region 56a of the wavefront changing unit 56 is
diffracted and changed to beams of conjugate diffracted light such
as a beam of first-order diffracted light L7 and a beam of minus
first-order diffracted light L8. The beam of first-order diffracted
light L7 has the focal point FP1 at the front surface of the photo
detector 57, and the beam of minus first-order diffracted light L8
has a focal point FP2 in the rear of the photo detector 57.
As shown in FIG. 24, the photo detector 57 comprises a sextant
photo-detector 59 (or a six-division photo detector) in which six
detecting sections SE1, SE2, SE3, SE4, SE5 and SE6 are provided.
The intensity of the first-order diffracted light L7 is detected by
each of the detecting sections SE1, SE2 and SE3 of the sextant
photo-detector 59 and is changed to electric current signals SC1,
SC2 and SC3. Also, the intensity of the minus first-order
diffracted light L8 is detected by each of the detecting sections
SE4, SE5 and SE6 of the sextant photo-detector 59 and is changed to
electric current signals SC4, SC5 and SC6.
FIG. 25A and 25C respectively show a converging spot of the
first-order diffracted light L7 radiated to the detecting sections
SE1, SE2 and SE3 of the sextant photo-detector 59 and another
converging spot of the minus first-order diffracted light L8
radiated to the detecting sections SE4, SE5 and SE6 of the sextant
photo-detector 59 on condition that the objective lens 27 is
defocused on the information medium 23 or 25. FIG. 25B shows a
converging spot of the first-order diffracted light L7 radiated to
the detecting sections SE1, SE2 and SE3 of the sextant
photo-detector 59 and another converging spot of the minus
first-order diffracted light L8 radiated to the detecting sections
SE4, SE5 and SE6 of the sextant photo-detector 59 on condition that
the objective lens 27 is just focused on the information medium 23
or 25.
As shown in FIGS. 25A to 25C, in cases where the transmitted light
L4 (or the diffracted light L5) is converged on the information
medium 23 (or 25) on condition that the objective lens 27 is
defocused on the information medium 23 (or 25), a converging spot
S8 of the diffracted light L7 shown at the left side of FIGS. 25A,
25C is formed on the sextant photo-detector 59, and another
converging spot S9 of the diffracted light L8 shown at the right
side of FIG. 25A or 25C is formed on the sextant photo-detector 59.
In contrast, in cases where the transmitted light L4 (or the
diffracted light L5) is converged on the information medium 23 (or
25) on condition that the objective lens 27 is just focused on the
information medium 23 (or 25), a converging spot S8 of the
diffracted light L7 shown at the left side of FIG. 25B is formed on
the sextant photo-detector 59, and another converging spot S9 of
the diffracted light L8 shown at the right side of FIG. 25B is
formed on the sextant photo-detector 59. The intensity of the
diffracted light L7 is detected in each of the detecting sections
SE1, SE2 and SE3 of the sextant photo-detector 59 and is changed to
electric current signals SC1, SC2, SC3. Also, the intensity of the
diffracted light L8 is detected in the detecting sections SE4, SE5
and SE6 of the sextant photo-detector 59 and is changed to electric
current signals SC4, SC5 and SC6. Thereafter, a focus error signal
S.sub.jo, is obtained according to the spot Size detection method
by calculating an equation (5).
S.sub.jo=(SC1+SC3-SC2)-(SC4+SC6-SC5) (5) Thereafter, the position
of the compound objective lens is moved in a direction along an
optical axis at high speed so as to minimize the absolute value of
the focus error signal S.sub.jo.
In the spot size detection method, the diffracted light L7, L8 are
expressed by two types of spherical waves having different
curvatures to detect the focus error signal S.sub.jo. However, two
beams of diffracted light L7, L8 radiated to the photo detector 57
are not limited to the spherical waves. That is, because the change
of the diffracted light L7, L8 in a Y-direction is detected by the
photo detector 57 according to the spot size detection method, it
is required that a one-dimensional focal point of the diffracted
light L7 is positioned in the front of the photo detector 57 and a
one-dimensional focal point of the diffracted light L8 is
positioned in the rear of the photo detector 57. Therefore, it is
applicable that diffracted light including astigmatic aberration be
radiated to the photo detector 57.
In addition, an information signal S.sub.in is obtained by adding
all of the electric current signals according to an equation (6).
S.sub.in=SC1+SC2+SC3+SC4+SC5+SC6 (6)
Because the information medium 23 or 25 is rotated at high speed, a
patterned track pit radiated by the converging spots S8, S9 of the
diffracted light L7,L8 is rapidly changed one after another, so
that the intensity of the information signal S.sub.in is changed.
Therefore, the information stored in the information medium 23 or
25 can be reproduced according to the information signal
S.sub.in.
Next, the detection of a tracking error signal depending on a
relative position between a converging spot and a patterned track
pit on the information medium 23 or 25 is described.
The grating pattern P5 drawn in the diffracted light generating
region 56b shown in FIG. 22 is designed to change the transmitted
light LR (or the diffracted light L5R) transmitting through the
diffracted light generating region 56b of the wavefront changing
unit 56 to a beam of first-order diffracted light L9 and a beam of
minus first-order diffracted light L10. Also, the grating pattern
P6 drawn in the diffracted light generating region 56c shown in
FIG. 22 is designed to change the transmitted light L4R (or the
diffracted light L5R) transmitting through the diffracted light
generating region 56c of the wavefront changing unit 56 to a beam
of first-order diffracted light L11 and a beam of minus first-order
diffracted light L12.
As shown in FIG. 24, the photo detector 57 further comprises four
tracking photo-detectors 60a to 60d for detecting intensities of
the diffracted light L9 to L12. As shown in FIG. 26, the intensity
of the diffracted light L9 is detected by the tracking
photo-detector 60a and is changed to an electric current signal
SC7, the intensity of the diffracted light L10 is detected by the
tracking photo-detector 60d and is changed to an electric current
signal SC10, the intensity of the diffracted light L11 is detected
by the tracking photo-detector 60b and is changed to an electric
current signal SC8, and the intensity of the diffracted light L12
is detected by the tracking photo-detector 60c and is changed to an
electric current signal SC 9. A tracking error signal
S.sub.r.theta. is calculated according to an equation (7).
S.sub.r.theta.=SC7-SC8-SC9+SC10 (7)
Therefore, the asymmetry of the intensity distribution of the
transmitted light L4R (or the diffracted light L5R) incident on the
wavefront changing unit 56, which changes in dependence on the
positional relation between the converging spot S1 (or S2) and a
patterned track pit radiated by the light L4 or L5, is expressed by
the tracking error signal S.sub.r.theta..
Thereafter, the objective lens 27 is moved in a radial direction so
as to reduce a tracking error indicated by the tracking error
signal S.sub.r.theta.. The radial direction is defined as a
direction perpendicular to both the optical axis and a series of
patterned track pits. Therefore, the converging spot S1 (or S2) of
the transmitted light L4 (or the diffracted light L5) on the
information medium 23 (or 25) can be formed in the middle of the
patterned track pit, so that the tracking error becomes zero.
Accordingly, focus and tracking servo characteristics can be stably
obtained in the optical head apparatus 51. That is, because the
wavefront changing unit 56 has a wavefront changing function, a
focus error signal can be easily obtained. Also, because the
diffracted light generating regions 56b, 56c are provided in the
wavefront changing unit 56, a tracking error signal can be easily
obtained. Therefore, the number of parts required to manufacture
the optical head apparatus 51 can be reduced, and the number of
manufacturing steps can be reduced. In addition, the optical head
apparatus can be manufactured at a low cost and in light
weight.
Also, because the compound objective lens having two focal points
is utilized in the optical head apparatus 51, pieces of information
can be reliably recorded or reproduced from an information medium
by utilizing the optical head apparatus 51 regardless of whether
the information medium is thick or thin.
(Seventh Embodiment)
Next, an optical head apparatus in which servo signals such as a
focus error signal and a tracking error signal are detected
according to an astigmatic aberration method is described according
to a seventh embodiment of the present invention.
FIG. 27 is a constitutional view of an optical head apparatus
according to a seventh embodiment.
As shown in FIG. 27, an optical head apparatus 61 for recording or
reproducing pieces of information on or from the information medium
23 or 25, comprises the light source 52, the collimator lens 53,
the beam splitter 54, the compound objective lens 29 (or 29M, 34,
43, 45, 46 or 47) composed of the hologram lens 26 (or 26M, 32, 33
or 42) and the objective lens 27, the actuating unit 58, the
converging lens 55, an astigmatic aberration generating unit 62
such as a plane parallel plate for generating an astigmatic
aberration in the transmitted light L4R or the diffracted light L5
R converged by the converging lens 55, and a photo detector 63 for
detecting the intensity of the transmitted light L4R or the
diffracted light L5R in which the astigmatic aberration is
generated to obtain an information signal and servo signals such as
a focus error signal and a tracking error signal.
The astigmatic aberration generating unit 62 is classified into one
of the wavefront changing unit 56 because a wavefront of the
transmitted light L4R or the diffracted light L5R is changed by the
generating unit 62 to generate the astigmatic aberration in the
light L4R or L5R. Also, a normal line of the unit 62 is tilted from
an optical axis.
As shown in FIG. 28, the photo detector 63 comprises a quadrant
photo-detector 64 in which four detecting sections SE7, SE8, SE9
and SE10 are provided.
In the above configuration, the transmitted light L4R (or the
diffracted light L5R) reflected by the information medium 23 (or
25) is converged by the converging lens 55 in the same manner as in
the sixth embodiment. Thereafter, the transmitted light L4R (or the
diffracted light L5R) transmits through the astigmatic aberration
generating unit 62 and is converged on the photo detector 57 to
form a converging spot S10 on the detecting sections SE7, SE8, SE9
and SE10 of the quadrant photo-detector 64. In this case, because
the transmitted light L4R (or the diffracted light L5R) converged
by the converging lens 55 is a spherical wave, an astigmatic
aberration is generated in the transmitted light L4R (or the
diffracted light L4R) by the astigmatic aberration generating unit
62. Therefore, as shown in FIGS. 29A to 29C, the shape of the
converging spot S10 considerably changes depending on a distance
between the compound objective lens 29 and the information medium
23 (or 25).
For example, in cases where the transmitted light L4 (or the
diffracted light L5) is converged on the information medium 23 (or
25) on condition that the objective lens 27 is defocused on the
information medium 23 (or 25), the converging spot S10 of the
transmitted light L4R (or the diffracted light L5R) is formed on
the quadrant photodetector 64 as shown in FIGS. 29A, 29C. In
contrast, in cases where the transmitted light L4 (or the
diffracted light L5) is converged on the information medium 23 (or
25) on condition that the objective lens 27 is just focused on the
information medium 23 (or 25), the converging spot S10 of the
transmitted light L4R (or the diffracted light L5R) is formed on
the quadrant photo-detector 64 as shown in FIG. 25B.
The intensity of the transmitted light L4R (or the diffracted light
L5R) is detected in the detecting sections SE7, SE8, SE9 and SE10
of the quadrant photo-detector 64 and is changed to electric
current signals SC11, SC12, SC13 and SC14. Thereafter, a focus
error signal S.sub.f.theta. is obtained according to an astigmatic
aberration method by calculating an equation (8).
S.sub.f.theta.=(SC11+SC14)-(SC12+SC13) (8) Thereafter, the position
of the compound objective lens 29 is moved in a direction parallel
to an optical axis at high speed so as to minimize the absolute
value of the focus error signal S.sub.f.theta..
Also, a tangential direction Dt agreeing with an extending
direction of patterned recording pits and a radial direction Dr
perpendicular to both the optical axis and the patterned recording
pits are defined as shown in FIG. 29D. In this case, when the
quadrant photo-detector 64 is directed as shown in FIGS. 29A to
29C, a tracking error signal S.sub.r.theta. is calculated according
to an equation (9) by utilizing an intensity distribution change of
the transmitted light L4R (or the diffracted light L5R) which
depends on a positional relation between the converging spot S10
and a recording pit radiated by the light L4 or L5.
S.sub.ro=SC11+SC13-(SC12+SC14) (9)
Thereafter, the objective lens 27 is moved in the radial direction
so as to reduce a tracking error indicated by the tracking error
signal S.sub.r.theta. . Therefore, the converging spot S1, (or S2)
of the transmitted light L4 (or the diffracted light L5) on the
information medium 23 (or 25) can be formed in the middle of the
recording pit, so that the tracking error becomes zero.
In other case, the tracking error signal S.sub.r.theta. is obtained
according to a phase difference method by utilizing the result
calculated in the equation (8).
In addition, an information signal S.sub.in is obtained by adding
all of the electric current signals according to an equation (10).
S.sub.in=SC11+SC12+SC13+SC14 (10)
Accordingly, focus and tracking servo characteristics can be stably
obtained in the optical head apparatus 61. That is, because an
astigmatic aberration is generated in the transmitted light L4R (or
the diffracted light L5R) by the astigmatic aberration generating
unit 62 made of a plane parallel plate, the servo signals such as a
focus error signal and a tracking error signal can be easily
obtained. Therefore, the number of parts required to manufacture
the optical head apparatus 61 can be reduced, and the number of
manufacturing steps can be reduced. In addition, the optical head
apparatus 61 can be manufactured at a low cost and in light
weight.
Also, because the compound objective lens having two focal points
is utilized in the optical head apparatus 61, pieces of information
can be reliably recorded or reproduced from an information medium
by utilizing the optical head apparatus 61 regardless of whether
the information medium is thick or thin.
In the seventh embodiment, the astigmatic aberration generating
unit 62 formed out of the plane parallel plate is arranged between
the converging lens 55 and the photo detector 63. However, as an
optical head apparatus 65 is shown in FIG. 30, it is applicable
that a cylindrical lens 66 integrally formed with the converging
lens 55 be arranged in place of the plane parallel plate to
generate an astigmatic aberration in the transmitted light L4R (or
the diffracted light L5R). In this case, because the cylindrical
lens 66 is integrally formed with the converging lens 55, the
optical head apparatus can be moreover manufactured at low cost. In
addition, as shown in FIG. 30, it is applicable that a normal line
of the hologram lens 26 (or 32, 33, 42) be tilted from an optical
axis passing through the center of the objective lens 27 by about
one degree to prevent stray light reflected in a surface of the
hologram lens 26 from being incident on the photo detector 57 or
63. Also, it is applicable that the hologram lens 26 (or 32, 33,
42) be coated with an anti-reflection coating to prevent the
occurrence of stray light.
Also, as an optical head apparatus 67 is shown in FIG. 31, it is
applicable that a polarized beam splitter 68 be arranged in place
of the beam splitter 54 to perfectly transmit the incident light L3
and a 1/4-.lamda. plate 69 be additionally placed between the
hologram lens 26 (or 32, 33, 42) and the polarized beam splitter
68. In this case, because the incident light L3 transmits through
the 1/4-.lamda. plate 69 in an outgoing optical path and because
the transmitted light L4R (or the diffracted light L5) again
transmits through the 1/4-.lamda. plate 69 in an incoming optical
path, the transmitted light L4R (or the diffracted light L5R) is
perfectly reflected by the polarized beam splitter 68. Accordingly,
a utilization efficiency of the incident light L3 can be enhanced.
Also, a signal-noise ratio of each of the servo signals and the
information signal can be enhanced.
Also, as an optical head apparatus 70 is shown in FIG. 32, it is
applicable that the polarized beam splitter 68 be arranged in place
of the beam splitter 54 to perfectly transmit the incident light L3
and the 1/4-.lamda. plate 69 be additionally placed between the
hologram lens 26 (or 32, 33, 42) and the objective lens 27. In this
case, the transmitted light L4R (or the diffracted light L5R) is
perfectly reflected by the polarized beam splitter 68 in the same
manner as the optical head apparatus shown in FIG. 31. In addition,
because stray light reflected from the hologram lens 26 (or 32, 33,
42) transmits through the polarized beam splitter 68, the stray
light is not incident on the photo detector 63. Accordingly, a
signal-noise ratio of each of the servo signals and the information
signal can be moreover enhanced.
Also, as an optical head apparatus 71 is shown in FIG. 33, it is
applicable that a wedge-like prism 72 for reshaping the incident
light L3 radiated from the light source 52 be additionally placed
between the collimator lens 53 and the polarized beam splitter 68.
In this case, an elliptic wavefront of the incident light L3 is
reshaped to a circular wavefront by the wedge-like prism 72.
Accordingly, a utilization efficiency of the incident light L3 can
be enhanced.
In the sixth and seventh embodiments, when the transmitted light L4
(that is, zero-order diffracted light L4) converged on the first
information medium 23 is reflected toward the compound objective
lens to reproduce a piece of information recorded on the first
information medium 23, a part of the transmitted light L4R is
diffracted in the hologram lens 26 (or 32, 33, 42) on the incoming
optical path, so that the part of the transmitted light L4R is
changed to a beam of first-order diffracted light L13. Therefore,
the first-order diffracted light L13 diverges from the hologram
lens 26, and a converging spot S11 of the diffracted light L13 is
formed on the photo detector 57 or 63 in a relatively large size,
as shown in FIG. 34. The size of the converging spot S11 is larger
than those of the sextant photo-detector 59 and the quadrant
photo-detector 64. Therefore, there is a drawback that a
signal-noise ratio in the information signal deteriorates.
To solve the drawback, it is preferred that the photo detector 57
(or 63) further comprise an information photodetector 73
surrounding the sextant photo-detector 59 (or the quadrant
photo-detector 64). The size of the information photo-detector 73
is equal to or larger than a 1 mm square. Therefore, in cases where
the information signal is determined by the sum of the intensity of
the transmitted light L4 detected in the sextant photo-detector 59
(or the quadrant photo-detector 64) and the intensity of the
diffracted light L13 detected in the information photo-detector 73,
the signal-noise ratio in the information signal can be enhanced,
and frequency characteristics of the information signal can be
enhanced.
(Eighth Embodiment)
Next, a method of focusing performed in the optical head
apparatuses 51, 61, 65, 67, 70 and 71 is described according to an
eighth embodiment of the present invention.
FIG. 35A graphically shows a change of the focus error signal
obtained by detecting the intensity of the transmitted light L4
formed in the hologram lens 26, 32 or 33, the strength of the focus
error signal depending on a distance between the objective lens 27
and the first information medium 23. FIG. 35B graphically shows a
change of the focus error signal obtained by detecting the
intensity of the diffracted light L5 formed in the hologram lens
26, 32 or 33, the strength of the focus error signal depending on a
distance between the objective lens 27 and the second information
medium 25.
The intensity of the transmitted light L4 is high because the
numerical aperture of the objective lens 27 for the transmitted
light L4 is large. Therefore, as shown in FIG. 35A, a change of a
focus error signal FE1 obtained in cases where the objective lens
27 is almost focused on the first information medium 23 is
considerably large as compared with a change of an unnecessary
focus error signal FE2 obtained in cases where the objective lens
27 is defocused on the first information medium 23. In addition, in
cases where the hologram lens 26, 32 or 33 is utilized in each of
the optical head apparatuses 51, 61, 65, 67, 70 and 71, the
unnecessary focus error signal FE2 is generated when the distance
between the objective lens 27 and the first information medium 23
is larger than the focal length of the objective lens 27 for the
transmitted light L4.
In contrast, the intensity of the diffracted light L5 is
comparatively low because the numerical aperture of the objective
lens 27 for the diffracted light L5 is comparatively small.
Therefore, as shown in FIG. 35B, a change of a focus error signal
FE3 obtained in cases where the objective lens 27 is almost focused
on the second information medium 25 is almost the same as that of
an unnecessary focus error signal FE4 obtained in cases where the
objective lens 27 is defocused on the second information medium 25.
In addition, in cases where the hologram lens 26, 32 or 33 is
utilized in each of the optical head apparatuses 51, 61, 65, 67, 70
and 71, the unnecessary focus error signal FE4 is generated when
the distance between the objective lens 27 and the second
information medium 25 is smaller than the focal length of the
objective lens 27 for the diffracted light L5.
Therefore, in cases where the focusing of the transmitted light L4
on the first information medium 23 is performed, the objective lens
27 placed far from the first information medium 23 is gradually
brought near to the first information medium 23. Thereafter, when
the strength of the focus error signal reaches a threshold value, a
focus servo loop provided in the photo detector 57 or 63 is set to
an operation condition, so that the objective lens 27 is set to be
focused on the first information medium 23. Also, in cases where
the focusing of the diffracted light L5 on the second information
medium 25 is performed, the objective lens 27 placed far from the
second information medium 25 is gradually brought near to the
second information medium 25 in the same manner. Thereafter, when
the strength of the focus error signal reaches a threshold value, a
focus servo loop provided in the photo detector 57 or 63 is set to
an operation condition, so that the objective lens 27 is set to be
focused on the second information medium 25.
Accordingly, the inverse influence of the unnecessary focus error
signal FE4 on the focusing of the diffracted light L5 can be
prevented. Also, because the objective lens 27 placed far from the
information medium 23 or 25 is gradually brought near to the
information medium 23 or 25 regardless of whether the information
medium is T1 or T2 in thickness, a focusing operation in each of
the optical head apparatuses 51, 61, 65, 67, 70 and 71 with the
hologram lens 26, 32 or 33 can be performed according to a common
procedure by changing the threshold value or performing an auto
gain control in which the focus error signal is normalized by
detecting the total intensity of the transmitted light L4R or the
diffracted light L4R. Therefore, a control circuit required to
perform the focusing operation can be made at a low cost.
FIG. 36A graphically shows a change of the focus error signal
obtained by detecting the intensity of the diffracted light L6
formed in the hologram lens 42, the strength of the focus error
signal depending on a distance between the objective lens 27 and
the first information medium 23. FIG. 36B graphically shows a
change of the focus error signal obtained by detecting the
intensity of the transmitted light L4 formed in the hologram lens
42, the strength of the focus error signal depending on a distance
between the objective lens 27 and the second information medium
25.
As shown in FIG. 36A, a change of a focus error signal FE5 obtained
in cases where the objective lens 27 is almost focused on the first
information medium 23 is considerably large as compared with a
change of an unnecessary focus error signal FE6 obtained in cases
where the objective lens 27 is defocused on the first information
medium 23. In addition, in cases where the hologram lens 42 is
utilized in each of the optical head apparatuses 51, 61, 65, 67, 70
and 71, the unnecessary focus error signal FE6 is generated when
the distance between the objective lens 27 and the first
information medium 23 is smaller than the focal length of the
objective lens 27 for the diffracted light L6.
In contrast, as shown in FIG. 36B, a change of a focus error signal
FE7 obtained in cases where the objective lens 27 is almost focused
on the second information medium 25 is almost the same as that of
an unnecessary focus error signal FES obtained in cases where the
objective lens 27 is defocused on the second information medium 25.
In addition, in cases where the hologram lens 42 is utilized in
each of the optical head apparatuses 51, 61, 65, 67, 70 and 71, the
unnecessary focus error signal FES is generated when the distance
between the objective lens 27 and the second information medium 25
is larger than the focal length of the objective lens 27 for the
transmitted light L4.
Therefore, in cases where the focusing of the diffracted light L6
on the first information medium 23 is performed, the objective lens
27 placed near to the first information medium 23 is gradually
moved away from the first information medium 23. Thereafter, when
the strength of the focus error signal reaches a threshold value, a
focus servo loop provided in the photo detector 57 or 63 is set to
an operation condition, so that the objective lens 27 is set to be
focused on the first information medium 23. Also, in cases where
the focusing of the transmitted light L4 on the second information
medium 25 is performed, the objective lens 27 placed near to the
second information medium 25 is gradually moved away from the
second information medium 25 in the same manner. Thereafter, when
the strength of the focus error signal reaches a threshold value, a
focus servo loop provided in the photo detector 57 or 63 is set to
an operation condition, so that the objective lens 27 is set to be
focused on the second information medium 25.
Accordingly, the inverse influence of the unnecessary focus error
signal FE8 on the focusing of the transmitted light L4 can be
prevented. Also, because the objective lens 27 placed near to the
information medium 23 or 25 is gradually moved away from the
information medium 23 or 25 regardless of whether the information
medium is T1 or T2 in thickness, a focusing operation in each of
the optical head apparatuses 51, 61, 65, 67, 70 and 71 with the
hologram lens 42 can be performed according to a common procedure
by changing the threshold value or performing the auto gain
control. Therefore, a control circuit required to perform the
focusing operation can be made at a low cost.
(Ninth Embodiment)
An optical head apparatus with the compound objective lens 29, 34,
45, 46 or 47 in which the incident light L3 is efficiently utilized
to obtain an information signal and servo signals is described with
reference to FIGS. 2, 37 according to a ninth embodiment of the
present invention.
FIG. 37 is a constitutional view of an optical head apparatus
according to a ninth embodiment.
As shown in FIG. 37, an optical head apparatus 81 for recording or
reproducing pieces of information on or from the information medium
23 or 25, comprises the light source 52, the collimator lens 53,
the beam splitter 54, the compound objective lens the compound
objective lens 29 (34, 45, 46 or 47) composed of the hologram lens
26 (or 32 or 33) and the objective lens 27, the actuating unit 58,
the converging lens 55, a beam splitter 82 for transmitting a beam
of diffracted light L4R or reflecting a beam of transmitted light
L4R, the photo detector 63 for detecting the intensity of the
diffracted light L5R transmitting through the beam splitter 82 to
obtain servo signals and an information signal recorded on the
second information medium 25, the wave-front changing device 56
such as a hologram for changing a wavefront of the transmitted
light L4R reflected by the beam splitter 82, and the photo detector
57 for detecting the intensity of the transmitted light L4R to
obtain servo signals and an information signal recorded on the
first information medium 23. The beam splitter 82 is made of a
plane parallel plate of which a normal line is tilted from an
optical path, so that an astigmatic aberration is generated in the
diffracted light L5R passing through the beam splitter 82. Also, a
coating is applied on a surface of the plane parallel plate.
In the above configuration, the transmitted light L4 (or the
diffracted light L5) are converged by the converging lens 27 in the
same manner as in the sixth embodiment. Thereafter, in cases where
a piece of information is recorded or reproduced on or from the
first information medium 23, the transmitted light L4 is converged
on the first information medium 23 to form the first converging
spot S1. Thereafter, a beam of transmitted light L4R reflected by
the first information medium 23 passes through the same optical
path in the reverse direction. That is, a great part of the
transmitted light L4R again transmits through the compound
objective lens without any diffraction and is reflected by the beam
splitter 54. Thereafter, the transmitted light L4R is converged by
the converging lens 55, and a part of the transmitted light L4R is
reflected by the beam splitter 82. Thereafter, the wavefront of a
great part of the transmitted light L4R is changed by the wavefront
changing unit 56, and the great part of the transmitted light L4R
is converged on the photo detector 57 to form the converging spots
S8, S9. Therefore, an information signal and servo signals such as
a focus error signal and a tracking error signal are obtained in
the same manner as in the sixth embodiment. Also, a remaining part
of the transmitted light L4R not changed its wavefront is converged
on the photo detector 57 to form the converging spot S7.
In contrast, in cases where a piece of information is recorded or
reproduced on or from the second information medium 25, the
diffracted light L5 is converged on the second information medium
25 to form the second converging spot S2. Thereafter, a beam of
diffracted light L4R reflected by the second information medium 25
passes through the same optical path in the reverse direction, and
a great part of the diffracted light L5R transmits through the
hologram lens 26 without any diffraction. Therefore, the diffracted
light L4R passes through the incoming optical path differing from
the outgoing optical path. Thereafter, the diffracted light L5R is
reflected by the beam splitter 54 and is converged by the
converging lens 55. Thereafter, a part of the diffracted light L5R
transmits through the beam splitter 82. In this case, an astigmatic
aberration is generated in the diffracted light L5R. Thereafter,
the diffracted light L5R is converged on the photo detector 63 to
form a converging spot S12 of which the shape is the same as the
converging spot S10 shown in FIGS. 29A to 29C, and the intensity of
the diffracted light L5R is detected in the photo detector 63.
Therefore, an information signal and servo signals such as a focus
error signal and a tracking error signal are obtained in the same
manner as in the seventh embodiment.
In this case, though a remaining part of the transmitted light L4R
transmits through the beam splitter 82, the remaining part of the
transmitted light L4R is not converged at the converging spot S12
because the transmitted light L4R passes through the same optical
path. Also, though a remaining part of the diffracted light L5R is
reflected the beam splitter 82, the remaining part of the
diffracted light L5R is not converged at the converging spot S7, S8
or S9 because the diffracted light L5R passes through the incoming
optical path differing from the outgoing optical path.
In the ninth embodiment, because the diffracted light L5R transmits
through the hologram lens 26 without any diffraction, the
converging spot S12 formed on the photo detector 63 does not relate
to a radiating point of the light source 52 in a mirror image,
while the converging spot S7 formed on the photo detector 57
relates to the radiating point of the light source 52 in the mirror
image. In other words, a focal point of the diffracted light L5R
converged by the converging lens 55 differs from that of the
transmitted light L4R converged by the converging lens 55.
Therefore, the photo detector 57 for detecting the intensity of the
transmitted light L4R and the photo detector 63 for detecting the
intensity of the diffracted light L4R are required.
Accordingly, because the compound objective lens having two focal
points is utilized in the optical head apparatus 81, pieces of
information can be reliably recorded or reproduced on or from an
information medium regardless of whether the information medium is
thick or thin.
An example of the utilization of the optical head apparatus 81 for
various types of optical disks is described.
In cases where the optical head apparatus 81 is utilized for an
optical disk device in which pieces of information recorded in a
thin type of high density optical disk 23 are recorded or
reproduced and pieces of information recorded in a thick type of
optical disk 25 are exclusively reproduced, the diffraction
efficiency of the hologram lens 26, 32 or 33 in the compound
objective lens 29, 34, 45, 46 or 47 for changing a beam of light to
a beam of first-order diffracted light is set to a value equal to
or lower than 30%. Therefore, in cases where a piece of information
recorded on the thick type of optical disk 25 is reproduced in the
photo detector 63, a signal-noise ratio of each of the servo
signals and the information signal obtained in the photo detector
63 can be enhanced because the diffracted light L4R transmitting
through the hologram lens 26, 32 or 33 at a high transmission
efficiency is utilized to obtain the servo signals and the
information signal. In other words, a utilization efficiency of the
incident light L3 can be enhanced when a piece of information
recorded on the thick type of optical disk 25 is reproduced, so
that the output power of the incident light L3 can be minimized.
Also, even though a high intensity of the transmitted light L4 is
required to record a piece of information on the high density
optical disk 23, the recording of the information can be reliably
performed without increasing the intensity of the incident light L3
because a transmission efficiency of the hologram lens 26, 32 or 33
for the incident light L3 is high. Also, in cases where a piece of
information recorded on the high density optical disk 23 is
reproduced in the photo detector 57, a signal-noise ratio of each
signal obtained in the photo detector 57 can be enhanced because
the transmission efficiency of the hologram lens 26, 32 or 33 for
the light L3, L4R is high.
(Tenth Embodiment)
An optical head apparatus with the compound objective lens 29, 34,
45, 46 or 47 in which the incident light L3 is efficiently utilized
to obtain an information signal and servo signals is described with
reference to FIGS. 38, 39 according to a tenth embodiment of the
present invention. X1 and Y1 coordinates shown in FIGS. 38, 39 are
utilized in common.
FIG. 38 is a constitutional view of an optical head apparatus
according to a tenth embodiment. FIG. 39 is a plan view of a beam
splitter having a reflection type of hologram utilized in the
optical head apparatus shown in FIG. 38.
As shown in FIG. 38, an optical head apparatus 91 for recording or
reproducing pieces of information on or from the information medium
23 or 25, comprises the light source 52, the collimator lens 53,
the beam splitter 54, the compound objective lens 29 (or 34, 45, 46
or 47) composed of the hologram lens 26 (or 32 or 33) and the
objective lens 27, the actuating unit 58, the converging lens 55, a
beam splitter 92 having a reflection type of hologram 93 for
transmitting a large part of the transmitted light L4R or
reflecting all of the diffracted light L5R incident on the hologram
93, the photo detector 63 for detecting the intensity of the
transmitted light L4R transmitting through the beam splitter 92 to
obtain servo signals and an information signal recorded in the
first information medium 23, and the photo detector 57 for
detecting the intensity of the diffracted light L5R to obtain servo
signals and an information signal recorded in the second
information medium 25.
The beam splitter 92 is made of a plane parallel plate inclined to
an optical path, so that an astigmatic aberration is generated in
the transmitted light L4R passing through the beam splitter 92.
Also, as shown in FIG. 39, the reflection type of hologram 93 is
arranged at a center portion of the beam splitter 92, and a light
transmitting region 92a is arranged at a peripheral portion of the
beam splitter 92 to surround the hologram 93. Light incident on the
light transmitting region 92a transmits without any diffraction.
The hologram 92 is partitioned into a diffracted light generating
region 93a in which a grating pattern P7 is drawn and a pair of
diffracted light generating regions 93b, 93c in which a pair of
grating patterns P8, P9 are drawn. The diffracted light L5R
incident on the diffracted light generating region 93a is
diffracted to obtain a focus error signal in the photo detector 57.
The diffracted light L5R incident on each of the diffracted light
generating regions 93b, 93c is diffracted to obtain a tracking
error signal in the photo detector 57.
In the above configuration, the transmitted light L4 and the
diffracted light L5 are converged by the converging lens 27 in the
same manner as in the sixth embodiment. Thereafter, in cases where
a piece of information is recorded or reproduced on or from the
first information medium 23, the transmitted light L4 is converged
on the first information medium 23 to form the first converging
spot S1. Thereafter, a beam of transmitted light L4R reflected by
the first information medium 23 passes through the same optical
path in the reverse direction. That is, a large part of the
transmitted light L4R again transmits through the compound
objective lens 29 without any diffraction and is reflected by the
beam splitter 54. Thereafter, the transmitted light L4R is
converged by the converging lens 55, and a large part of the
transmitted light L4R transmits through the beam splitter 92. In
this case, an astigmatic aberration is generated in the transmitted
light L4R. Thereafter, the transmitted light L4R is converged on
the photo detector 63 to form a converging spot S13 of which the
shape is the same as the converging spot S10 shown in FIGS. 29A to
29C, and the intensity of the transmitted light L4R is detected in
the photo detector 63. Therefore, an information signal and servo
signals such as a focus error signal and a tracking error signal
are obtained in the same manner as in the seventh embodiment.
In contrast, in cases where a piece of information is recorded or
reproduced on or from the second information medium 25, the
diffracted light L5 is converged on the second information medium
25 to form the second converging spot S2. Thereafter, a beam of
diffracted light L4R reflected by the second information medium 25
passes through the same optical path in the reverse direction, and
a large part of the diffracted light L5R transmits through the
hologram lens 26 without any diffraction. Therefore, the diffracted
light L4R transmits on the incoming optical path differing from the
outgoing optical path in the same manner as in the ninth
embodiment. Thereafter, the diffracted light L5R is reflected by
the beam splitter 54 and is converged by the converging lens 55 on
the beam splitter 92 to form a converging spot on the reflection
type of hologram 93 of the beam splitter 92. Therefore, all of the
diffracted light L5R is diffracted and reflected by the hologram 93
to be converged on the photo detector 57. That is, the diffracted
light L4R diffracted and reflected in the diffracted light
generating region 93a of the hologram 93 is splitted into two beams
and is converged on the detecting sections SE1 to SE6 of the
sextant photo-detector 59 in the photo detector 57 in the same
manner as in the sixth embodiment. Also, the diffracted light L5R
diffracted and reflected in the diffracted light generating region
93b of the hologram 93 is splitted into two beams, and the
intensity of the diffracted light L5R is detected in the tracking
photo-detectors 60a and 60d. Also, the diffracted light L5R
diffracted and reflected in the diffracted light generating region
93c of the hologram 93 is splitted into two beams, and the
intensity of the diffracted light L5R is detected in the tracking
photo-detectors 60b and 60c. Therefore, an information signal and
servo signals such as a focus error signal and a tracking error
signal are obtained in the same manner as in the sixth
embodiment.
In the tenth embodiment, because the transmitted light L4R
transmits through the hologram lens 26 without any diffraction, the
converging spot S13 formed on the photo detector 63 does not relate
to a radiating point of the light source 52 in a mirror image.
Therefore, the photo detector 57 for detecting the intensity of the
diffracted light L5R and the photo detector 63 for detecting the
intensity of the transmitted light L4R are required.
Accordingly, because the compound objective lens having two focal
points is utilized in the optical head apparatus 91, pieces of
information can be reliably recorded or reproduced on or from an
information medium regardless of whether the information medium is
thick or thin.
Also, because all of the diffracted light L5R is completely
diffracted and reflected by the hologram 93 of the beam splitter
92, the diffracted light L5R can be utilized at high efficiency.
Therefore, a signal-noise ratio of the signals obtained in the
photo detector 57 can be enhanced.
An example of the utilization of the optical head apparatus 91 for
various types of optical disks is described.
In cases where the optical head apparatus 91 is utilized for an
optical disk device in which pieces of information recorded in a
thin type of high density optical disk 23 are recorded or
reproduced and pieces of information recorded in a thick type of
optical disk 25 are exclusively reproduced, the diffraction
efficiency of the hologram lens 26, 32 or 33 in the compound
objective lens 29, 34, 45, 46 or 47 for changing a beam of light to
a beam of first-order diffracted light is set to a value equal to
or lower than 30%. Therefore, in cases where a piece of information
recorded on the thick type of optical disk 25 is reproduced in the
photo detector 57, a signal-noise ratio of each of the servo
signals and the information signal obtained in the photo detector
57 can be enhanced because the diffracted light L4R transmitting
through the hologram lens 26, 32 or 33 at a high transmission
efficiency is utilized to obtain the servo signals and the
information signal. In other words, a utilization efficiency of the
incident light L3 can be enhanced when a piece of information
recorded on the thick type of optical disk 25 is reproduced, so
that the output power of the incident light L3 can be minimized.
Also, even though a high intensity of the transmitted light L4 is
required to record a piece of information on the high density
optical disk 23, the recording of the information can be reliably
performed without increasing the intensity of the incident light L3
because a transmission efficiency of the hologram lens 26, 32 or 33
for the incident light L3 is high. Also, in cases where a piece of
information recorded on the high density optical disk 23 is
reproduced in the photo detector 63, a signal-noise ratio of each
signal obtained in the photo detector 63 can be enhanced because
the transmission efficiency of the hologram lens 26, 32 or 33 for
the light L3, L4R is high.
(Eleventh Embodiment)
An optical head apparatus with the compound objective lens 29, 34,
45, 46 or 47 in which the incident light L3 is efficiently utilized
to obtain an information signal and servo signals is described with
reference to FIGS. 40 to 42 according to an eleventh embodiment of
the present invention. X1 and Y1 co-ordinates shown in FIGS. 40, 41
are utilized in common, and X, Y and Z co-ordinates shown in FIGS.
40, 42 are utilized in common.
FIGS. 40A, 40B are respectively a constitutional view of an optical
head apparatus according an eleventh embodiment. FIG. 41 is a plan
view of a beam splitter having a reflection type of hologram
utilized in the optical head apparatus shown in FIG. 38.
As shown in FIGS. 40A, 40B, an optical head apparatus 101 for
recording or reproducing pieces of information on or from the
information medium 23 or 25, comprises the light source 52, the
collimator lens 53, the beam splitter 54, the compound objective
lens 29 (or 34, 45, 46 or 47) composed of the hologram lens 26 (or
32 or 33) and the objective lens 27, the actuating unit 58, the
converging lens 55, a beam splitter 102 having a transmission type
of hologram 103 for transmitting the transmitted light L4R
converged on the first information medium 23 and the diffracted
light L4R converged on the second information medium 25 and
diffracting the transmitted light L4R which is converged on the
second information medium 25 in defocus, a photo detector 104 for
detecting the intensity of the transmitted light L4R converged on
the first information medium 23 to obtain servo signals and an
information signal recorded in the first information medium 23,
detecting in defocus the intensity of the diffracted light L5R to
obtain an information signal recorded in the second information
medium 25, and detecting the intensity of the transmitted light L4R
converged on the second information medium 25 in defocus to obtain
a focus error signal.
The beam splitter 102 is made of a plane parallel plate inclined to
an optical path, so that an astigmatic aberration is generated in
the light L4R, L4R passing through the beam splitter 102. Also, as
shown in FIG. 41, the transmission type of hologram 103 is arranged
at a center portion of the beam splitter 102, and a light
transmitting region 102a is arranged at a peripheral portion of the
beam splitter 102 to surround the hologram 103. The transmitted
light L4R incident on the light transmitting region 102a transmits
without any diffraction. The hologram 102 is partitioned into
diffracted light generating regions 103a, 103b alternately arranged
to detect a focus error signal according to the spot size detection
method described in the sixth embodiment. That is, a grating
pattern P10 is drawn in each of the diffracted light generating
regions 103a, and a converging spot is formed by the transmitted
light L4R diffracted in the regions 103a. Also, a grating pattern
PH is drawn in each of the diffracted light generating regions
103b, and another converging spot is formed by the transmitted
light L4R diffracted in the regions 103b.
The photo detector 104 comprises the sextant photodetector 59 in
which the detecting sections SE1, SE2, SE3, SE4, SE5 and SE6 are
provided in the same manner as the photo detector 57.
In the above configuration, the transmitted light L4 and the
diffracted light L5 are converged by the converging lens 27 in the
same manner as in the sixth embodiment. Thereafter, in cases where
a piece of information is recorded or reproduced on or from the
first information medium 23, as shown in FIG. 40, the transmitted
light L4 is converged on the first information medium 23 to form
the first converging spot S1. Thereafter, a beam of transmitted
light L4R reflected by the first information medium 23 passes
through the same optical path in the reverse direction. That is,
the transmitted light L4R again transmits through the compound
objective lens without any diffraction and is reflected by the beam
splitter 54. Thereafter, the transmitted light L4R is converged by
the converging lens 55, and a major part of the transmitted light
L4R transmits through the beam splitter 103. In this case, an
astigmatic aberration is generated in the transmitted light L4R.
Thereafter, the transmitted light L4R is converged on the photo
detector 104 to form a converging spot S14 of which the shape is
the same as the converging spot S10 shown in FIGS. 29A to 29C, and
the intensity of the transmitted light L4R is detected in the photo
detector 104. Therefore, an information signal and servo signals
such as a focus error signal and a tracking error signal are
obtained in the same manner as in the seventh embodiment. In this
case, because the position of the photo detector 104 detecting the
transmitted light L4R relates to a radiation point of the light
source 52 in a mirror image, the transmitted light L4R is converged
on the photo detector 104 just in focus.
In contrast, in cases where a piece of information is recorded or
reproduced on or from the second information medium 25, as shown in
FIG. 40B, the diffracted light L5 is converged on the second
information medium 25 to form the second converging spot S2.
Thereafter, a beam of diffracted light L4R reflected by the second
information medium 25 passes through the same optical path in the
reverse direction and transmits through the hologram lens 26
without any diffraction. Therefore, the diffracted light L5R
transmits on the incoming optical path differing from the outgoing
optical path in the same manner as in the ninth embodiment.
Thereafter, the diffracted light L5R is reflected by the beam
splitter 54 and is converged by the converging lens 55. Thereafter,
a major part of the diffracted light L5R transmits through the beam
splitter 102, and the diffracted light L5R is converged on the
photo detector 57. In this case, an astigmatic aberration is
generated in the diffracted light L5R. Also, because the diffracted
light L5R is not diffracted by the hologram lens 26 on the incoming
optical path, the position of the photo detector 104 detecting the
diffracted light L5R does not relate to the radiation point of the
light source 52 in the mirror image. Therefore, the diffracted
light L5R is converged on the photo detector 104 in defocus.
However, because the entire intensity of the diffracted light L5R
converged in defocus is detected in the photo detector 104, an
information signal is obtained in the same manner as in the seventh
embodiment.
Also, the transmitted light L4 is converged on the second
information medium 25 in defocus as shown in FIG. 40B. That is, the
transmitted light L4 incident on the rear surface of the second
information medium 25 is converged at the front surface of the
second information medium 25. Thereafter, a beam of transmitted
light L4R reflected at the front surface of the second information
medium 25 again transmits through the compound objective lens
without any diffraction and is reflected by the beam splitter 54.
Thereafter, the transmitted light L4R is converged by the
converging lens 55 on the beam splitter 102 to form a converging
spot on the of hologram 103 of the beam splitter 102. Therefore,
all of the transmitted light L4R is diffracted by the hologram 103
and is converged on the photo detector 104. That is, the
transmitted light L4R diffracted in the diffracted light generating
regions 103a of the hologram 103 is changed to a first spherical
wave SW1 of which a focal point is placed at the front of the photo
detector 104, and the transmitted light L4R diffracted in the
diffracted light generating regions 103b of the hologram 103 is
changed to a second spherical wave SW2 of which a focal point is
placed at the rear of the photo detector 104. Thereafter, as shown
in FIGS. 42A to 42C, the first spherical wave SW1 is converged on
the detecting sections SE1 to SE3 of the sextant photo-detector 59
in the photo detector 104 to form a converging spot S15A, and the
second spherical wave SW2 is converged on the detecting sections
SE4 to SE6 of the sextant photo-detector 59 to form a converging
spot S15B. Because the regions 103a, 103b are divided into many
pieces, the converging spots S15A, S15B are respectively divided
into many pieces.
In cases where the diffracted light L5 is converged on the
information medium 25 in defocus, the converging spots S15A, S15B
of the transmitted light L4R shown in FIGS. 42A, 42C are formed on
the sextant photo-detector 59. In contrast, in cases where the
diffracted light L5 is converged on the information medium 25 in
focus, the converging spots S15A, S15B of the transmitted light L4R
shown in FIG. 42B are formed on the sextant photo-detector 59. The
intensity of the transmitted light L4R is detected in each of the
detecting sections SE1 to SE6 of the sextant photo-detector 59 and
is changed to electric current signals SC15 to SC20. Thereafter, a
focus error signal S.sub.f.theta. is obtained according to the spot
size detection method by calculating an equation (11).
S.sub.f.theta.=(SC15+SC17-SC16)-(SC18+SC20-SC19) (11) Thereafter,
the position of the compound objective lens is moved in a direction
along an optical axis at high speed so as to minimize the absolute
value of the focus error signal S.sub.f.theta.. Therefore, the
focus error signal is obtained in the same manner as in the sixth
embodiment.
Accordingly, because the compound objective lens having two focal
points is utilized in the optical head apparatus 101, pieces of
information can be reliably recorded or reproduced on or from an
information medium regardless of whether the information medium is
thick or thin.
Also, because all of the transmitted light L4R reflected by the
second information medium 25 is completely diffracted by the
hologram 103 of the beam splitter 102 to detect the focus error
signal, the transmitted light L4R can be utilized at high
efficiency. Therefore, a signal-noise ratio of the focus error
signal obtained in the photo detector 104 can be enhanced.
Also, the information signal and the servo signals can be obtained
in the photo detector 104 regardless of whether the information
medium 23 or 25 is thin or thick. Therefore, the number of parts
required to manufacture the optical head apparatus 101 can be
reduced, and a small sized optical head apparatus can be
manufactured at a low cost and in light weight even though pieces
of information are recorded or reproduced on or from an information
medium by utilizing the optical head apparatus 101 regardless of
whether the information medium is thick or thin.
An example of the utilization of the optical head apparatus 101 for
various types of optical disks is described. In cases where the
optical head apparatus 101 is utilized for an optical disk device
in which pieces of information recorded in a thin type of high
density optical disk 23 are recorded or reproduced and pieces of
information recorded in a thick type of optical disk 25 are
exclusively reproduced, the diffraction efficiency of the hologram
lens 26, 32 or 33 in the compound objective lens 29, 34, 45, 46 or
47 is set to a value equal to or lower than 30%. Therefore, in
cases where a piece of information recorded on the thick type of
optical disk 25 is reproduced in the photo detector 104, a
signal-noise ratio of each of the servo signals and the information
signal obtained in the photo detector 104 can be enhanced because
the diffracted light L5R transmitting through the hologram lens 26,
32 or 33 at a high transmission efficiency is utilized to obtain
the information signal. In other words, a utilization efficiency of
the incident light L3 can be enhanced when a piece of information
recorded on the thick type of optical disk 25 is reproduced, so
that the output power of the incident light L3 can be minimized.
Also, even though a high intensity of the transmitted light L4 is
required to record a piece of information on the high density
optical disk 23, the recording of the information can be reliably
performed without increasing the intensity of the incident light L3
because a transmission efficiency of the hologram lens 26, 32 or 33
for the incident light L3 is high.
Also, in cases where a piece of information recorded on the high
density optical disk 23 is reproduced in the photo detector 63, a
signal-noise ratio of each signal obtained in the photo detector 63
can be enhanced because the transmission efficiency of the hologram
lens 26, 32 or 33 for the light L3, L4R is high.
(Twelfth Embodiment)
An optical head apparatus with the compound objective lens 29M, 43,
45, 46 or 47 in which the incident light L3 is efficiently utilized
to obtain an information signal and servo signals is described with
reference to FIG. 43 according to a twelfth embodiment of the
present invention.
FIG. 43 is a constitutional view of an optical head apparatus
according to a twelfth embodiment.
As shown in FIG. 43, an optical head apparatus 111 for recording or
reproducing pieces of information on or from the information medium
23 or 25, comprises the light source 52, the collimator lens 53,
the beam splitter 54, the compound objective lens 29M (or 43, 45,
46 or 47) composed of the hologram lens 42 (or 26M or 32) and the
objective lens 27, the actuating unit 58, the converging lens 55,
the beam splitter 82, the photo detector 63, the wavefront changing
device 56, and the photo detector 57.
In the above configuration, a beam of incident light L3 radiated
from the light source 52 is collimated in the collimator lens 53
and transmits through the beam splitter 54. Thereafter, a part of
the incident light L3 transmits through the compound objective lens
29 without any diffraction, and a remaining part of the incident
light L3 is diffracted.
Thereafter, in cases where a piece of information is recorded or
reproduced on or from the first information medium 23, the
diffracted light L6 is converged on the first information medium 23
to form the converging spot S5. That is, the diffracted light L6 is
incident on the rear surface of the first information medium 23,
and the converging spot S5 is formed on the front surface of the
first information medium 23. Thereafter, a beam of diffracted light
L6R reflected at the front surface of the first information medium
23 passes through the same optical path in the reverse direction,
and a great part of the diffracted light L6R is again diffracted by
the hologram lens 42. Therefore, the diffracted light L6R transmits
on the incoming optical path agreeing with the outgoing optical
path. Thereafter, the diffracted light L6R is reflected by the beam
splitter 54 and is converged by the converging lens 55. Thereafter,
a part of the diffracted light L6R transmits through the beam
splitter 82. In this case, an astigmatic aberration is generated in
the diffracted light L6R. Thereafter, the diffracted light L6R is
converged on the photo detector 63 to form the converging spot S10
of which the shape is shown in FIGS. 29A to 29C, and the intensity
of the diffracted light L6R is detected in the photo detector 63.
Therefore, an information signal and servo signals such as a focus
error signal and a tracking error signal are obtained in the same
manner as in the seventh embodiment.
In contrast, in cases where a piece of information is recorded or
reproduced on or from the second information medium 25, the
transmitted light L4 is converged on the second information medium
25 to form the converging spot S6. That is, the transmitted light
L4 is incident on the rear surface of the second information medium
25, and the converging spot S6 is formed on the front surface of
the second information medium 25. Thereafter, a beam of transmitted
light L4R reflected at the front surface of the second information
medium 25 passes through the same optical path in the reverse
direction. That is, the transmitted light L4R is collimated by the
objective lens 27 on the incoming optical path. Thereafter, a great
part of the transmitted light L4R is diffracted by the hologram
lens 42. Therefore, the transmitted light L4R transmits on the
incoming optical path differing from the outgoing optical path.
Thereafter, the transmitted light L4R is reflected by the beam
splitter 54 and is converged by the converging lens 55. Thereafter,
a part of the transmitted light L4R is reflected by the beam
splitter 82. Thereafter, the wavefront of a great part of the
transmitted light L4R is changed by the wavefront changing unit 56,
and the great part of the transmitted light L4R is converged on the
photo detector 57 to form converging spots S16, S17. Therefore, an
information signal and servo signals such as a focus error signal
and a tracking error signal are obtained in the same manner as in
the sixth embodiment. Also, a remaining part of the transmitted
light L4R not changed its wavefront by the wavefront changing unit
56 is converged on the photo detector 57 to form the converging
spot S18.
In the twelfth embodiment, because the transmitted light L4R is
diffracted by the hologram lens 42 on the incoming optical path,
the converging spot S18 formed on the photo detector 57 does not
relate to a radiation point of the light source 52 in a mirror
image, while the converging spot S10 formed on the photo detector
63 relates to the radiation point of the light source 52 in the
mirror image. In other words, a focal point of the transmitted
light L4R converged by the converging lens 55 differs from that of
the diffracted light L6R converged by the converging lens 55.
Therefore, the photo detector 57 for detecting the intensity of the
transmitted light L4R and the photo detector 63 for detecting the
intensity of the diffracted light L6R are required.
Accordingly, even though pieces of information are recorded or
reproduced on or from an information medium, the information can be
reliably recorded or reproduced on or from the information medium
regardless of whether the information medium is thick or thin.
Also, because the diffracted light L6 formed in the hologram lens
42 converges before the diffracted light L6 is incident on the
objective lens 27, the distance in an optical axis direction
between the converging spots S5, S6 can be lengthened to about 1
mm. Therefore, even though the transmitted light L4 (or the
diffracted light L6) is converged on the converging spot S6 (or S5)
in focus to record or read a piece of information, the light L6 (or
L4) is not converged on the converging spot S6 (or S5) in focus to
reduce the intensity of the light L6 (or L4) at the converging spot
S6 (or S5). Accordingly, no adverse influence is exerted on the
recording or reproduction of the information
Also, because the hologram lens 42 functions as a convex lens for
the first-order diffracted light L6, the occurrence of a chromatic
aberration can be prevented in the optical head apparatus 111.
An example of the utilization of the optical head apparatus 111 for
various types of optical disks is described. In cases where the
optical head apparatus 111 is utilized for an optical disk device
in which pieces of information recorded in a thin type of high
density optical disk 23 are recorded or reproduced and pieces of
information recorded in a thick type of optical disk 25 are
exclusively reproduced, the diffraction efficiency of the hologram
lens 26M or 42 in the compound objective lens 29M, 43, 45, 46 or 47
for changing a beam of light to a beam of first-order diffracted
light is set to a value equal to or higher than 55%. Therefore. in
cases where a piece of information recorded on the thick type of
optical disk 25 is reproduced in the photo detector 57, a
signal-noise ratio of each of the servo signals and the information
signal obtained in the photo detector 57 can be enhanced because
the transmitted light L4R diffracted by the hologram lens 26M or 42
at a high diffraction efficiency is utilized to obtain the servo
signals and the information signal. In other words, a utilization
efficiency of the incident light L3 can be enhanced when a piece of
information recorded on the thick type of optical disk 25 is
reproduced, so that the output power of the incident light L3 can
be minimized. Also, even though a high intensity of the diffracted
light L6 is required to record a piece of information on the high
density optical disk 23, the recording of the information can be
reliably performed without increasing the intensity of the incident
light L3 because the diffraction efficiency of the hologram lens
26M or 42 for the incident light L3 and the diffracted light L6R is
high. Also, in cases where a piece of information recorded on the
high density optical disk 23 is reproduced in the photo detector
63, a signal-noise ratio of each signal obtained in the photo
detector 63 can be enhanced because the diffraction efficiency of
the hologram lens 26M or 42 for the light L3, L6R is high.
(Thirteenth Embodiment)
An optical head apparatus with the compound objective lens 29M, 43,
45, 46 or 47 in which the incident light L3 is efficiently utilized
to obtain an information signal and servo signals is described with
reference to FIG. 44 according to a thirteenth embodiment of the
present invention.
FIG. 44 is a constitutional view of an optical head apparatus
according to a thirteenth embodiment.
As shown in FIG. 44, an optical head apparatus 121 for recording or
reproducing pieces of information on or from the information medium
23 or 25, comprises the light source 52, the collimator lens 53,
the beam splitter 54, the compound objective lens 43 (or 29M, 45,
46 or 47) composed of the hologram lens 42 (or 26M or 32) and the
objective lens 27, the actuating unit 58, the converging lens 55,
the beam splitter 92 having the reflection type of hologram 93, the
photo detector 63, and the photo detector 57.
In the above configuration, the transmitted light L4 and the
diffracted light L6 are converged by the converging lens 27 in the
same manner as in the twelfth embodiment. Thereafter, in cases
where a piece of information is recorded or reproduced on or from
the first information medium 23, the diffracted light L6 is
converged on the first information medium 23 to form the converging
spot S5. Thereafter, a beam of diffracted light L5R reflected by
the first information medium 23 passes through the same optical
path in the reverse direction, and a large part of the diffracted
light L6R is diffracted by the hologram lens 42. Therefore, the
diffracted light L6R transmits on the incoming optical path
agreeing with the outgoing optical path in the same manner as in
the twelfth embodiment. Thereafter, the diffracted light L6R is
reflected by the beam splitter 54 and is converged by the
converging lens 55 on the beam splitter 92 to form a converging
spot on the reflection type of hologram 93 of the beam splitter 92.
Therefore, all of the diffracted light L6R is diffracted and
reflected by the hologram 93 to be converged on the photo detector
57 in the same manner as in the tenth embodiment. Therefore, an
information signal and servo signals such as a focus error signal
and a tracking error signal are obtained in the same manner as in
the sixth embodiment.
In contrast, in cases where a piece of information is recorded or
reproduced on or from the second information medium 25, the
transmitted light L4 is converged on the second information medium
25 to form the converging spot S6. Thereafter, a beam of
transmitted light L4R reflected by the second information medium 25
passes through the same optical path in the reverse direction. That
is, a large part of the transmitted light L4R is collimated by the
objective lens 27 on the incoming optical path. Thereafter, a great
part of the transmitted light L4R is diffracted by the hologram
Lens 42. Therefore, the transmitted light L4R transmits on the
incoming optical path differing from the outgoing optical path in
the same manner as in the twelfth embodiment. Thereafter, the
transmitted light L4R is reflected by the beam splitter 54 and is
converged by the converging lens 55. Thereafter, a large part of
the transmitted light L4R transmits through the beam splitter 92.
In this case, an astigmatic aberration is generated in the
transmitted light L4R. Thereafter, the transmitted light L4R is
converged on the photo detector 63 to form a converging spot S19 of
which the shape is the same as the converging spot S10 shown in
FIGS. 29A to 29C, and the intensity of the transmitted light L4R is
detected in the photo detector 63. Therefore, an information signal
and servo signals such as a focus error signal and a tracking error
signal are obtained in the same manner as in the seventh
embodiment.
In the thirteenth embodiment, because the transmitted light L4R is
diffracted by the hologram lens 42, the converging spot S19 formed
on the photo detector 63 does not relate to a radiation point of
the light source 52 in a mirror image. Therefore, the photo
detector 57 for detecting the intensity of the diffracted light L6R
and the photo detector 63 for detecting the intensity of the
transmitted light L4R are required.
Accordingly, because the compound objective lens having two focal
points is utilized in the optical head apparatus 121, pieces of
information can be reliably recorded or reproduced on or from an
information medium regardless of whether the information medium is
thick or thin.
Also, because the diffracted light L6 formed in the hologram lens
42 converges before the diffracted light L6 is incident on the
objective lens 27, the distance in an optical axis direction
between the converging spots S5, S6 can be lengthened to about 1
mm. Therefore, even though the transmitted light L4 (or the
diffracted light L6) is converged on the converging spot S6 (or S5)
in focus to record or read a piece of information, the light L6 (or
L4) is not converged on the converging spot S6 (or S5) in focus to
reduce the intensity of the light L6 (or L4) at the converging spot
S6 (or S5). Accordingly, no adverse influence is exerted on the
recording or reproduction of the information
Also, because the hologram lens 42 functions as a convex lens for
the first-order diffracted light L6, the occurrence of a chromatic
aberration can be prevented in the optical head apparatus 121.
An example of the utilization of the optical head apparatus 121 for
various types of optical disks is described.
In cases where the optical head apparatus 121 is utilized for an
optical disk device in which pieces of information recorded in a
thin type of high density optical disk 23 are recorded or
reproduced and pieces of information recorded in a thick type of
optical disk 25 are exclusively reproduced, the diffraction
efficiency of the hologram lens 26M or 42 in the compound objective
lens 29M, 43, 45, 46 or 47 for changing a beam of light to a beam
of first-order diffracted light is set to a value equal to or
higher than 70%. Therefore, in cases where a piece of information
recorded on the thick type of optical disk 25 is reproduced in the
photo detector 57, a signal-noise ratio of each of the servo
signals and the information signal obtained in the photo detector
57 can be enhanced because the transmitted light L4R diffracted by
the hologram lens 26M or 42 at a high diffraction efficiency is
utilized to obtain the servo signals and the information signal. In
other words, a utilization efficiency of the incident light L3 can
be enhanced when a piece of information recorded on the thick type
of optical disk 25 is reproduced, so that the output power of the
incident light L3 can be minimized. Also, even though a high
intensity of the diffracted light L6 is required to record a piece
of information on the high density optical disk 23, the recording
of the information can be reliably performed without increasing the
intensity of the incident light L3 because the diffraction
efficiency of the hologram lens 26M or 42 for the incident light L3
and the diffracted light L6R is high. Also, in cases where a piece
of information recorded on the high density optical disk 23 is
reproduced in the photo detector 63, a signal-noise ratio of each
signal obtained in the photo detector 63 can be enhanced because
the diffraction efficiency of the hologram lens 26M or 42 for the
light L3, L6R is high.
(Fourteenth Embodiment)
An optical head apparatus in which noises included in an
information signal are reduced is described with reference to FIGS.
45, 46 according to a fourteenth embodiment of the present
invention.
FIG. 45 is a constitutional view of an optical head apparatus
according to a fourteenth embodiment. FIG. 46 is a plan view of a
hologram lens utilized in the optical head apparatus shown in FIG.
45.
As shown in FIG. 45, an optical head apparatus 131 for recording or
reproducing pieces of information on or from the information medium
23 or 25, comprises the light source 52, a beam splitter 132 having
a polarizing separation film 133 on its surface for reflecting the
incident light L3 radiated from the light source 52 on an outgoing
optical path and transmitting through the light L4R or L5R
reflected on the information medium 23 or 25 on an incoming optical
path, a collimator lens 134 for collimating the incident light L3
on the outgoing optical path and converging the light L4R or L5R on
the incoming optical path, a hologram lens 135 for transmitting a
part of the incident light L3 without any diffraction and
diffracting a remaining part of the incident light L3, the
1/4-.lamda. plate 69, the objective lens 27, the actuating unit 58,
and a photo detector 136 for detecting the light transmitting
through or diffracted by the hologram lens 135 on the incoming
optical path.
As shown in FIG. 46, the hologram lens 135 is formed by drawing the
grating pattern P1 in a central region 135a of the transparent
substrate 28 and a grating pattern P12 in a peripheral region 135b
surrounding the central region 135a. The grating pattern P12 is
drawn in a non-concentric shape. Because the grating pattern P1 are
drawn in the hologram lens 135, a compound objective lens 137
having two focal points is composed of the hologram lens 135 and
the objective lens 27. Light passing through the peripheral region
135b of the hologram lens 135 is detected by the photo detector 136
to cancel noises included in an information signal. An optical axis
of the optical head apparatus 131 passes through a central point of
the grating pattern P1 and a central axis of the objective lens
27.
The photo detector 136 comprises the quadrant photodetector 64
having the detecting sections SE7 to SE10 and a noise cancelling
photo detector 138 for detecting the intensity of light passing
through the peripheral region 135b of the hologram lens 135.
Because the grating pattern P12 of the peripheral region 135b is
drawn in the non-concentric shape, light diffracted in the
peripheral region 135b is not converged on the detecting sections
SE7 to SE10.
In the above configuration, the incident light L3 linearly
polarized in a first direction is radiated from the light source 52
and is reflected by the beam splitter 132 because the polarizing
separation film 133 functions as a mirror for the incident light L3
linearly polarized in the first direction. Therefore, the incident
light L3 is directed in an upper direction and is collimated by the
collimator lens 134. Thereafter, a part of the incident light L3
incident on the central region 135a of the hologram lens 135
transmits through the central region 135a without any diffraction
to form the transmitted light L4, and a remaining part of the
incident light L3 incident on the central region 135a of the
hologram lens 135 is diffracted in the central region 135a to form
the diffracted light L5. Also, a part of the incident light L3
incident on the peripheral region 135b of the hologram lens 135
transmits through the peripheral region 135b without any
diffraction to form a beam of noise cancelling light L14.
Thereafter, the light L4, L5 and L14 pass through the 1/4-.lamda.
plates so that the light L4, L5 and L14 linearly polarized in the
first direction is changed to the light L4, L5 and L14 circularly
polarized. Thereafter, the light L4, L5 and L14 are converged by
the converging lens 27.
Thereafter, in cases where a piece of information is recorded or
reproduced on or from the first information medium 23 (or the
second information medium 25), the transmitted light L4 (or the
diffracted light L5) is converged on the information medium 23 (or
25) to form the converging spot S1 (or S2 ). Thereafter, a beam of
transmitted light L4R (or a beam of diffracted light L5R) reflected
by the information medium 23 (or 25) passes through the same
optical path in the reverse direction. That is, the transmitted
light L4R (or the diffracted light L5R) is circularly polarized in
reverse and again passes through the converging lens 27 and the
1/4-.lamda. plate 69. Therefore, the light L4R (or L5R) is linearly
polarized in a second direction perpendicular to the first
direction. Thereafter, a part of the transmitted light L4R
transmits through the central region 135a of the hologram lens 135
without any diffraction, or a part of the diffracted light L5R is
again diffracted in the central region 135a. Thereafter, the
transmitted light L4R (or the diffracted light L5R) is converged by
the collimator lens 134 and passes through the beam splitter 132
without any reflection because the polarizing separation film 133
functions as a transparent plate for the light L4R (or L5R)
linearly polarized in the second direction. In this case, an
astigmatic aberration is generated in the transmitted light L4R (or
the diffracted light L5R) in the same manner as in the seventh
embodiment. Thereafter, the transmitted light L4R (or the
diffracted light L5R) is incident on the detecting sections SE7 to
SE10 of the photo detector 136 to form a converging spot S20 of
which the shape is the same as the converging spot S10 shown in
FIGS. 29A to 29C. The intensity of the transmitted light L4R (or
the diffracted light L5R) is changed to electric current signals
SC21 to SC24 in the detecting sections SE7 to SE10. Therefore,
servo signals such as a focus error signal and a tracking error
signal are obtained in the same manner as in the seventh
embodiment, so that the position of the compound objective lens 137
is adjusted to converge the transmitted light L4 (or the diffracted
light L5) on the information medium 23 (or 25) in focus. Also, an
information signal expressing a piece of information recorded on
the information medium 23 (or 25) is obtained according to an
equation (12). S.sub.in=SC21+SC22+SC23+SC24 (12)
Also, the noise cancelling light L14 is converged on the
information medium 23 to form a converging spot surrounding the
converging spot S1. Thereafter, a beam of noise cancelling light
L14R reflected by the first information medium 23 passes through
the same optical path in the reverse direction. That is, the noise
cancelling light L14R again passes through the converging lens 27
and the 1/4.lamda. plate 69, and a part of the noise cancelling
light L14R is diffracted and converged in the peripheral region
135b of the hologram lens 135 and is incident on the noise
cancelling photo detector 138. In the photo detector 138, an output
signal SC25 is generated according to the intensity of the noise
cancelling light L14R. Thereafter, a noise cancelled information
signal S.sub.nc expressing a piece of information recorded on the
first information medium 23 is obtained by adding all of the
signals according to an equation (13):
S.sub.nc=(SC21+SC22+SC23+SC24)+R.times.SC25 (13), where the symbol
R is a weighting factor.
In this case, because the term R.times..times.SC25 is added to
obtain the information signal S.sub.nc, inverse influence of noises
included in the term (SC21+SC22+SC23+SC24) on the noise cancelled
information signal S.sub.nc can be reduced. The reason is
described.
As is well known (for example, Japanese Patent Gazette No. 22452 of
1990 laid open to public inspection on Jul. 23, 1985 under
Provisional Publication No. 138748 of 1985 and Published Unexamined
Patent Application No. 131245 of 1986), signals expressing pieces
of information recorded on an optical disk shifts to a higher
frequency as the density of the information recorded becomes high.
Also, the amplitude of a signal having a high frequency becomes low
as compared with that of a signal having a low frequency in cases
where the signals are produced according to light passing through a
central region of a hologram lens. In contrast, the amplitude of a
signal having a high frequency is emphasized in cases where the
signal is produced according to light passing through a peripheral
region of the hologram lens. Therefore, in cases where the
information signal S.sub.nc is obtained according to the equation
(13), high frequency components included in the information signal
S.sub.nc is emphasized, and low frequency noise components included
in the term (SC21+SC22+SC23+SC24) are comparatively reduced. As a
result, a signal-noise ratio in the information signal S.sub.nc can
be enhanced.
Accordingly, because the compound objective lens having two focal
points is utilized in the optical head apparatus 131, pieces of
information can be reliably recorded or reproduced or or from an
information medium regardless of whether the information medium is
thick or thin.
Also, even though pieces of information are densely recorded in a
thin type of high density optical disk represented by the first
information medium 23, the information signal S.sub.nc can be
reliably reproduced at a high signal-noise ratio.
Also, because the intensity of the light L4R or L5R incident on the
detecting sections SE7 to SE10 of the photo detector 136 is reduced
by converging the noise cancelling light L14R on the photo detector
138, a positioning accuracy of the photo detector 136 can be
coarsely lowered to 1/100.
Also, in cases where the grating pattern P12 of the peripheral
region 135b functions as a lens for the incident light L3
diffracted in the peripheral region 135b, unnecessary diffracted
light generated in the peripheral region 135b on the outgoing
optical path forms a comparatively large converging spot in defocus
on the first information medium 23. Therefore, pieces of
information recorded on the first information medium 23 are read by
the unnecessary diffracted light, and the information are treated
as a piece of averaged information in the photo detector 136 even
though the unnecessary diffracted light is incident on the photo
detector 136. Accordingly, the information read by the unnecessary
diffracted light does not adversely influence on the information
signal S.sub.nc as a noise.
Also, in cases where a transmission efficiency of the peripheral
region 135b of the hologram lens 135 is set to agree with another
transmission efficiency of the central region 135a, secondary
maxima (or side lobes) occurring around the converging spot S1 can
be lowered as compared with the first embodiment. Accordingly, a
signal-noise ratio in the information signal S.sub.nc can be
enhanced.
(Fifteenth Embodiment)
An optical head apparatus in which noises included in an
information signal are reduced is described with reference to FIGS.
47 to 49 according to a fifteenth embodiment of the present
invention.
FIG. 47 is a constitutional view of an optical head apparatus
according to a fifteenth embodiment. FIG. 48 is a plan view of a
hologram lens utilized in the optical head apparatus shown in FIG.
47.
As shown in FIG. 47, an optical head apparatus 141 for recording or
reproducing pieces of information on or from the information medium
23 or 25, comprises the light source 52, the beam splitter 82, the
collimator lens 134, a hologram lens 142 for transmitting a part of
the incident light L3 without any diffraction and diffracting a
remaining part of the incident light L3, the objective lens 27, the
actuating unit 58, and a photo detector 143 for detecting the light
transmitting through or diffracted by the hologram lens 142 on the
incoming optical path.
As shown in FIG. 48, the hologram lens 142 is partitioned into a
central region 142a in which the grating pattern P1 is drawn, a
pair of side peripheral regions 142b, 142c in which grating
patterns P13, P14 are drawn to cancel noises included in an
information signal, and a pair of no-designed regions 142d, 142e in
which no grating pattern is drawn not to reduce the intensity of
light. Because the grating pattern P1 are drawn in the hologram
lens 135, a compound objective lens 144 having two focal points is
composed of the hologram lens 142 and the objective lens 27. An
optical axis of the optical head apparatus 141 passes through a
central point of the grating pattern P1 and a central axis of the
objective lens 27.
The photo detector 143 comprises the quadrant photodetector 64
having the detecting sections SE7 to SE10, a pair of noise
cancelling photo detector 138a, 138b for detecting the intensity of
light passing through the peripheral region 142b, 142c of the
hologram lens 142.
In the above configuration, the transmitted light L4 (or the
diffracted light L5) generated in the central region 142a of the
hologram lens 142 is converged on the first information medium 23
(or the second information medium 25) in an outgoing optical path
to form the converging spot S1 (or S2). Thereafter, the transmitted
light L4R (or the diffracted light L5R) passes through the same
optical path in the reverse direction. That is, the transmitted
light L4R (or the diffracted light L5R) again passes through the
converging lens 27, and a part of the transmitted light L4R
transmits through the central region 142a of the hologram lens 142
without any diffraction or a part of the diffracted light L5R is
again diffracted in the central region 142a. Thereafter, the
transmitted light L4R (or the diffracted light L5R) is converged by
the collimator lens 134 and passes through the beam splitter 82. In
this case, an astigmatic aberration is generated in the transmitted
light L4R (or the diffracted light L5R) in the same manner as in
the seventh embodiment. Thereafter, the transmitted light L4R (or
the diffracted light L5R) is incident on the detecting sections SE7
to SE10 of the photo detector 143 to form a converging spot S21 of
which the shape is the same as the converging spot S10 shown in
FIGS. 29A to 29C. The intensity of the transmitted light L4R (or
the diffracted light L5R) is changed to electric current signals
SC26 to SC29 in the detecting sections SE7 to SE10. Therefore,
servo signals such as a focus error signal and a tracking error
signal are obtained in the same manner as in the seventh
embodiment, so that the position of the compound objective lens 144
is adjusted to converge the transmitted light L4 (or the diffracted
light L5) on the information medium 23 (or 25) in focus. Also, an
information signal recorded on the second information medium 25 is
obtained according to an equation (14).
S.sub.in=SC26+SC27+SC28+SC29 (14)
Also, a part of the incident light L3 incident on the peripheral
region 142b of the hologram lens 142 transmits through the
peripheral region 142b without any diffraction to form a beam of
noise cancelling light L15, and a part of the incident light L3
incident on the peripheral region 142c of the hologram lens 142
transmits through the peripheral region 142c without any
diffraction to form a beam of noise cancelling light L16.
Thereafter, the noise cancelling light L15, L16 are converged on
the information medium 23 to form a converging spot surrounding the
converging spot S1. Thereafter, beams of noise cancelling light
LIL15R, L16R reflected by the first information medium 23 passes
through the same optical path in the reverse direction. That is,
the noise cancelling light LIL15R, L16R again passes through the
converging lens 27. A part of the noise cancelling light L15R is
diffracted and converged in the peripheral region 142b of the
hologram lens 142 and is incident on the noise cancelling photo
detector 138a, and a part of the noise cancelling light L16R is
diffracted and converged in the peripheral region 142c of the
hologram lens 142 and is incident on the noise cancelling photo
detector 138b. In the photo detector 138a, an output signal SC30 is
generated according to the intensity of the noise cancelling light
L15R. Also, an output signal SC31 is generated according to the
intensity of the noise cancelling light L16R in the photo detector
138b. Thereafter, a noise cancelled information signal S.sub.nc
expressing the information recorded on the first information medium
23 is obtained by adding all of the signals according to an
equation (15): S.sub.nc=(SC26+SC27+SC28+SC29)+R.times.(SC30+SC31)
(15), where the symbol R is a weighting factor.
Accordingly, because the compound objective lens having two focal
points is utilized in the optical head apparatus 141, pieces of
information can be reliably recorded or reproduced from an
information medium regardless of whether the information medium is
thick or thin.
Also, a signal-noise ratio in the information signal S.sub.nc can
be enhanced in the same manner as in the fourteenth embodiment.
Also, even though pieces of information are densely recorded in a
thin type of high density optical disk represented by the first
information medium 23, the information signal S.sub.nc can be
reliably reproduced at a high signal-noise ratio.
Also, because the intensity of the light L4R or L5R incident on the
detecting sections SE7 to SE10 of the photo detector 143 is reduced
by converging the noise cancelling light L15R, L16R on the photo
detectors 138a, 138b, a positioning accuracy of the photo detector
143 can be coarsely lowered to 1/100.
Also, in cases where the grating patterns P13, P14 of the
peripheral regions 142b, 142c functions as a lens for the incident
light L3 diffracted in the peripheral region 142b, 142c,
unnecessary diffracted light generated by diffracting the incident
light L3 in the peripheral regions 142b, 142c on the outgoing
optical path forms a comparatively large converging spot in defocus
on the first information medium 23. Also, an numerical number of
each of the peripheral regions 142b, 142c is lowered as compared
with that of the region 135b in the fourteenth embodiment because
the hologram lens 142 are partitioned into many fields. Therefore,
the size of the converging spot of the unnecessary diffracted light
formed in defocus on the first information medium 23 becomes larger
than that in the fourteenth embodiment. As a result, more pieces of
information recorded on the first information medium 23 are read by
the unnecessary diffracted light, and the information are treated
as a piece of averaged information in the photo detector 143 even
though the unnecessary diffracted light is incident on the photo
detector 143. Accordingly, the information read by the unnecessary
diffracted light is moreover averaged, and the averaged information
does not adversely influence on the information signal S.sub.nc as
a noise.
Also, as shown in FIGS. 49A, 49B, the unnecessary diffracted light
can be prevented from being incident on the photo detector 64 in
which each of the detecting sections SE7 to SE10 has SL0 square in
size. In detail, in cases where light generated in the peripheral
region 142c on the outgoing optical path is again diffracted in the
peripheral region 142b to form a beam of unnecessary diffracted
light Lu.sub.1, the light Lu.sub.1 is converged on a first position
PT1 spaced SP1 (SP1>SL0) from the center of the photo detector
64. In cases where light generated in the peripheral region 142b on
the outgoing optical path is again diffracted in the peripheral
region 142c to form a beam of unnecessary diffracted light
Lu.sub.2, the light Lu.sub.2 is converged on a second position PT2
spaced SP2 (SP2>SL0) from the center of the photo detector 64.
In cases where light generated in the peripheral regions 142b, 142c
on the outgoing optical path are again diffracted in the same
peripheral regions 142b, 142c to form beams of unnecessary
diffracted light Lu.sub.3, Lu.sub.4, the light Lu.sub.3, Lu.sub.4
are converged on third and fourth position PT3, PT4 spaced SP3
(SP3>SL0), SP4 (SP4>SL0) from the center of the photo
detector 64. Accordingly, the adverse influence of the unnecessary
diffracted light Lu.sub.1 to Lu.sub.4 can be prevented.
In cases where the light source 52 is formed of a semiconductor
laser, a far field pattern of the incident light L3 incident on the
hologram lens 142 is distributed in the Gaussian distribution as
shown in FIG. 13A, and a cross-sectional beam profile of the
incident light L3 distributed in the Gaussian distribution is in an
elliptic shape. That is, a beam divergent angle (or a full angle at
half maximum) of the incident light L3 in a perpendicular direction
is larger than that in a horizontal direction. In this embodiment,
the perpendicular direction of the incident light L3 is directed in
an X2 direction shown in FIG. 48, and the horizontal direction of
the incident light L3 is directed in a Y2 direction shown in FIG.
48. In this case, because a transmission efficiency of the regions
142b, 142c for the incident light L3 is smaller than that of the
regions 142d, 142e, the intensity of the incident light L3
transmitting through the hologram lens 142 without any diffraction
is largely reduced in the perpendicular direction as compared with
that in the horizontal direction. Therefore, the cross-sectional
beam profile of the incident light L3 is corrected to a circular
shape in the hologram lens 142. That is, the converging spot S1
formed on the first information medium 23 is corrected to the
circular shape. Accordingly, secondary maxima (or side lobes)
occurring around the converging spot S1 can be lowered, and a
signal-noise ratio of the information signal S.sub.nc can be
enhanced.
In the fifteenth embodiment, the noise cancelled information signal
S.sub.nc is obtained according to the equation (15). However, it is
preferred that the noise cancelled information signal S.sub.nc be
obtained according to the equation (16):
S.sub.nc=(SC26+SC27+SC28+SC29)+(R1.times.SC30+R2.times.SC31) (16),
where the symbols R1, R2 are weighting factors. In this case, the
noises included in the information can be moreover reduced.
(Sixteenth Embodiment)
An optical head apparatus manufactured in a small size and stably
operated is described with reference to FIGS. 50, 51 according to a
sixteenth embodiment of the present invention.
FIG. 50 is a constitutional view of an optical head apparatus
according to a sixteenth embodiment. FIG. 51 is a diagonal view of
a light source and photo detectors utilized in the optical head
apparatus shown in FIG. 50.
As shown in FIG. 50, an optical head apparatus 151 for recording or
reproducing pieces of information on or from the information medium
23 or 25, comprises the light source 52 for radiating the incident
light L3 linearly polarized in a non-diffracting direction parallel
to an X3 axis, an holographic element 152 for transmitting through
the incident light L3 without any diffraction on an outgoing
optical path and diffracting the transmitted light L4R or the
diffracted light L4R linearly polarized in a diffracting direction
parallel to a Y3 axis on an incoming optical path, the collimator
lens 53, the 1/4-.lamda. plate 69, the hologram lens 26 (or 26M,
32, 33, 42, 135 or 142), the objective lens 27, the actuating unit
58, and a photo detector 153 for detecting the intensity of the
light L4R or L5R diffracted by the holographic element 152. As
shown in FIG. 51, the light source 52 and the photo detector 153
are located on a substrate 154 to precisely fix a relative position
between the light source 52 and the photo detector 153. The photo
detector 153 comprises the sextant photo-detector 59 having the
detecting sections SE1 to SE6 and the tracking photo-detectors 60a
to 60d. Also, a mirror element 155 is located on the substrate 154
to direct the incident light L3 radiated from the light source 52
in a Z3 direction.
The holographic element 152 is produced by proton-exchanging
surface parts of a lithium niobate substrate or by utilizing a
liquid crystal cell, as is described in Provisional Publication No.
189504/86 (S61-189504) and Provisional Publication No. 241735/88
(S63-241735). Therefore, light linearly polarized in a
non-diffracting direction parallel to an X3 axis transmits through
the holographic element 152 without any diffraction. In contrast,
light linearly polarized in a diffracting direction parallel to a
Y3 axis which is perpendicular to the X3 axis is diffracted by the
holographic element 152.
In the above configuration, the incident light L3 linearly
polarized in a non-diffracting direction parallel to an X3 axis is
radiated from the light source 52 and transmits through the
holographic element 152 without any diffraction. Thereafter, the
incident light L3 is collimated by the collimator lens 53, and the
incident light L3 linearly polarized is changed to the incident
light L3 circularly polarized by the 1/4-.lamda. plate 69.
Thereafter, a part of the incident light L3 transmits through the
hologram lens 26 without any diffraction to form the transmitted
light L4, and a remaining part of the incident light L3 is
diffracted by the hologram lens 26 to form the diffracted light L5.
Thereafter, the light L4, L5 are converged by the objective lens
27, and the converging spot S1 of the transmitted light L4 (or the
converging spot S2 of the diffracted light L5) is formed on the
first information medium 23 (or the second information medium 25).
When the light L4 or L5 is reflected by the information medium 23
(or 25) and is changed to the light L4R (or L5R), a rotational
direction of the circular polarization in the light L4 is reversed.
Therefore, the light L4R (or L5R) having the reversed circular
polarization passes through the same optical path in the opposite
direction. That is, the transmitted light L4R (or the diffracted
light L5R) again passes through the converging lens 27, and a part
of the transmitted light L4R transmits through the hologram lens
142 without any diffraction or a part of the diffracted light L5R
is again diffracted by the hologram lens 142. Thereafter, the
transmitted light L4R (or the diffracted light L5R) circularly
polarized in reverse is changed to the light L4R (or L5R) linearly
polarized in a diffracting direction parallel to a Y3 axis by the
1/4-.lamda. plate 69. Thereafter, the light L4R (or L5R) is
converged by the collimator lens 53 and is diffracted by the
holographic element 152 to form a plurality of converging spots on
the photo detectors 153. Therefore, an information signal
expressing a piece of information recorded on the information
medium 23 (or 25) and servo signals such as a focus error signal
and a tracking error signal are obtained in the photo detector 153
in the same manner as in the sixth embodiment.
Accordingly, because the compound objective lens having two focal
points is utilized in the optical head apparatus 151, pieces of
information can be reliably recorded or reproduced or or from an
information medium regardless of whether the information medium is
thick or thin.
Also, because all of the incident light L3 transmits through the
holographic element 152 on the outgoing optical path and because
all of the light L4R or L5R is diffracted by the holographic
element 152 on the incoming optical path, a utilization efficiency
of the incident light L3 can be enhanced. Therefore, even though a
radiation intensity of the incident light L3 in the light source 52
is low, the information signal and the servo signals having a high
signal-noise ratio can be reliably obtained.
Also, because no beam splitter is utilized in the optical head
apparatus 151, the optical head apparatus 151 can be manufactured
at a small size, in a light weight, and at a low cost.
Also, because optical parts of the optical head apparatus 151 are
located along its optical axis, the optical head apparatus 151
stably operated can be obtained even though a circumstance
temperature largely varies and the apparatus is operated for a long
time.
Also, because the light L4R or L5R transmitting through the
holographic element 152 without any diffraction on the incoming
optical path is not required, it is preferred that a diffraction
efficiency of the holographic element 152 be heightened to set a
transmission efficiency of the holographic element 152 to almost
zero. In this case, a combination of the holographic element 152
and the 1/4-.lamda. plate 69 function functions as an isolator to
prevent the light L4R or L5R from returning to the light source 52.
Therefore, in cases where a semiconductor laser is utilized as the
light source 52, any light does not return to an active layer of
the semiconductor laser. Accordingly, noises induced by the light
returning to the semiconductor laser can be prevented.
Also, because the light source 52 and the photo detector 153 are
located on the same substrate 154, the light source 52 and the
photo detector 153 can be closely arranged each other. Therefore, a
relative position between the light source 52 and the photo
detector 153 can be easily set at a high accuracy. For example, the
relative position can be set at an accuracy within several .mu.m.
Accordingly, a manufacturing cost of the optical head apparatus 151
can be lowered, and the optical head apparatus 151 can be moreover
manufactured at a small size, in a light weight, and at a low
cost.
Also, the light source 52 is electrically connected with an
external circuit through first wirings, and the photo detector 153
is electrically connected with another external circuit through
second wirings. In this case, because the light source 52 and the
photo detector 153 are located on the same substrate 154, the first
and second wirings can pass on an X3-Y3 plane in common. Therefore,
the light source 52 and the photo detector 153 can be easily and
automatically connected with the external circuits. In addition,
because reference lines required to connect the light source 52 and
the photo detector 153 with the external circuits are only drawn on
the X3-Y3 plane, the relative position between the light source 52
and the photo detector 153 can be easily set at a high
accuracy.
In the sixteenth embodiment, the optical head apparatus 151 with
the holographic element 152 is described. However, in cases where
the intensity of the incident light L3 is sufficient, it is
applicable that a hologram having a small grating pitch or a blazed
hologram be utilized in place of the holographic element 152. In
this case, pieces of information can be reliably recorded or
reproduced on or from an information medium regardless of whether
the information medium is thick or thin. Also, because no beam
splitter is utilized in the optical head apparatus 151, the optical
head apparatus 151 can be manufactured at a small size, in a light
weight, and at a low cost. Also, because optical parts of the
optical head apparatus 151 are located along its optical axis, the
optical head apparatus 151 stably operated can be obtained even
though a circumstance temperature largely varies and the apparatus
is operated for a long time.
(Seventeenth Embodiment)
An optical head apparatus manufactured in a small size and stably
operated is described with reference to FIG. 52 according to a
seventeenth embodiment of the present invention.
FIG. 52 is a constitutional view of an optical head apparatus
according to a seventeenth embodiment.
As shown in FIG. 52, an optical head apparatus 161 for recording or
reproducing pieces of information on or from the information medium
23 or 25, comprises the light source 52 for radiating the incident
light L3 linearly polarized in a first direction, the collimator
lens 53, a polarizing separation film 162 formed on a front surface
of a transparent substrate 162 for reflecting the incident light L3
linearly polarized in the first direction and transmitting light
linearly polarized in a second direction perpendicular to the first
direction, the 1/4-.lamda. plate 69, the hologram lens 26 (or 26M,
32, 33, 42, 135 or 142), the objective lens 27, the actuating unit
58, a reflection-type hologram 164 formed on a rear surface of the
transparent substrate 162 for diffracting and reflecting the light
L4R, L5R, and the photo detector 57.
In the above configuration, the incident light L3 linearly
polarized in a first direction is radiated from the light source 52
and is collimated by the collimator lens 53. Thereafter, all of the
incident light L3 is reflected by the polarizing separation film
162 because the incident light L3 is linearly polarized in the
first direction. Therefore, the incident light L3 is directed in an
upper direction. Thereafter, the linear polarization of the
incident light L3 is changed to a circular polarization in the
1/4-.lamda. plate 69, and a part of the incident light L3 transmits
through the hologram lens 26 to form the transmitted light L4.
Also, a remaining part of the incident light L3 is diffracted by
the hologram lens 26 to form the diffracted light L5. Thereafter,
the light L4, L5 are converged by the objective lens 27, and the
converging spot S1 of the transmitted light L4 (or the converging
spot S2 of the diffracted light L5) is formed on the first
information medium 23 (or the second information medium 25).
Thereafter, the transmitted light L4R (or the diffracted light L5R)
circularly polarized in reverse again passes through the converging
lens 27 in the same manner as in the sixteenth embodiment, and a
part of the transmitted light L4R transmits through the hologram
lens 26 without any diffraction or a part of the diffracted light
L4R is again diffracted by the hologram lens 26. Thereafter, the
transmitted light L4R (or the diffracted light L5R) circularly
Polarized in reverse is changed to the light L4R (or L5R) linearly
polarized in a second direction perpendicular to the first
direction by the 1/4-.lamda. plate 69. Thereafter, all of the light
L4R (or L4R) is refracted by the polarizing separation film 162 and
is diffracted and reflected by the hologram 164. Thereafter, the
light L4R (or L5R) transmits through the polarizing separation film
162 and is converged by the collimator lens 53 to form a plurality
of converging spots on the photo detector 57. Therefore, an
information signal expressing a piece of information recorded on
the information medium 23 (or 25) and servo signals such as a focus
error signal and a tracking error signal are obtained in the photo
detector 57 in the same manner as in the sixth embodiment.
Accordingly, because the compound objective lens having two focal
points is utilized in the optical head apparatus 161, pieces of
information can be reliably recorded or reproduced on or from an
information medium regardless of whether the information medium is
thick or thin.
Also, because the incident light L3 incident on the polarizing
separation film 162 is collimated, a reflectivity for the incident
light L3 is uniform over the entire film 162. Therefore, a
diffraction-limited spot of the light L4 or L5 can be easily formed
on the information medium 23 or 25. Also, because the light L4R,
L5R incident on the polarizing separation film 162 are collimated,
a transmissivity for the light L4R, L5R is uniform over the entire
film 162. Therefore, an offset occurring in the servo signals can
be prevented.
Also, because all of the incident light L3 transmits through the
hologram 164 on the outgoing optical path and because all of the
light L4R or L4R is diffracted by the hologram 164 on the incoming
optical path, a utilization efficiency of the incident light L3 can
be enhanced. Therefore, even though a radiation intensity of the
incident light L3 in the light source 52 is low, the information
signal and the servo signals having a high signal-noise ratio can
be reliably obtained.
Also, because a hybrid element composed of the film 162, the
substrate 163 and the hologram 164 functions as a beam splitter and
a rising mirror, the optical head apparatus 161 can be manufactured
at a small size, in a light weight, and at a low cost.
Also, because optical parts of the optical head apparatus 161 are
located along its optical axis, the optical head apparatus 161
stably operated can be obtained even though a circumstance
temperature largely varies and the apparatus is operated for a long
time.
Also, a combination of the film 162 and the 1/4-.lamda. plate 69
function functions as an isolator to prevent the light L4R or L5R
from returning to the light source 52. Therefore, in cases where a
semiconductor laser is utilized as the light source 52, any light
does not return to an active layer of the semiconductor laser.
Accordingly, noises induced by the light returning to the
semiconductor laser can be prevented. Also, it is preferred that
the hologram 164 be blazed. In this case, because the generation of
unnecessary diffracted light such as minus first-order diffracted
light in the hologram 164 is prevented, a diffraction efficiency of
the hologram 164 for changing light to first-order diffracted light
can be set to almost 100%. Therefore, the incident light L3 can be
efficiently utilized to obtain the signals.
Also, because light incident on the hologram 164 is diffracted to
first-order diffracted light, a chromatic aberration occurring in
the light L4R, L5R can be compensated in the hologram 164.
Therefore, the servo signals can be stably obtained.
In the seventeenth embodiment, the collimator lens 53 is located
between the light source 52 and the film 162. However, the
collimator lens 53 is not necessary in the optical head apparatus
161.
Also, the optical head apparatus 161 with the film 162 and the
1/4-.lamda. plate 69 is described. However, in cases where the
intensity of the incident light L3 is sufficient, it is applicable
that a reflection film having a reflectivity of almost 1/3 be
utilized in place of the film 162 and the 1/4-.lamda. plate 69 be
omitted. In this case, pieces of information can be reliably
recorded or reproduced on or from an information medium regardless
of whether the information medium is thick or thin. Also, because a
hybrid element composed of the film 162, the substrate 163 and the
hologram 164 functions as a beam splitter and a rising mirror, the
optical head apparatus 161 can be manufactured at a small size, in
a light weight, and at a low cost. Also, because optical parts of
the optical head apparatus 161 are located along its optical axis,
the optical head apparatus 161 stably operated can be obtained even
though a circumstance temperature largely varies and the apparatus
is operated for a long time.
In the sixth to seventeenth embodiments, pieces of information can
be reliably recorded or reproduced on or from an information medium
regardless of whether the information medium represents a
conventional optical disk such as a compact disk having a thickness
T2 of about 1.2 mm or a prospective high density optical disk
having a thickness T1 ranging from 0.4 mm to 0.8 mm. However, when
the information recorded or reproduced on or from the information
medium, it is required to examine the thickness of the information
medium in advance. Therefore, in cases where a piece of
distinguishing information is recorded on the information medium in
advance to distinguish the thickness of the information medium, it
is convenient for a user. Because no distinguishing information is
recorded on the conventional optical disk, it is preferred that the
distinguishing information be recorded on the prospective high
density optical disk appearing on the market in the future.
Therefore, a high density optical disk with the distinguishing
information is described according to eighteenth and nineteenth
embodiments.
(Eighteenth Embodiment)
FIG. 53 is a diagonal view of a high density optical disk according
to an eighteenth embodiment, a cross sectional view of the disk
being partially shown.
As shown in FIG. 53, a high density optical disk 171 is partitioned
into an outer region 171a and an inner region 171b. The outer
region 171a occupies a large part of the optical disk 171, and an
information recording substrate 171c of the outer region 171a has
the thickness T1, and the information recording substrate 171c of
the inner region 171b has the thickness T2. A plurality of first
recording pits 172 are formed on the information recording
substrate 171c of the outer region 171a at narrow intervals in
series to record pieces of information at a high density. Also, a
plurality of second recording pits 173 are formed on the
information recording substrate 171c of the inner region 171b at
ordinary intervals in series to record pieces of distinguishing
information at an ordinary density of a compact disk. The
distinguishing information inform that the optical disk 171 has the
thickness T1. The thickness T1 of the outer region 171a, for
example, ranges from 0.4 mm to 0.8 mm, and the thickness T2 of the
inner region is, for example, about 1.2 mm.
In the above configuration, the diffracted light L5 according to
the first or second embodiment (or the transmitted light L4
according to the third embodiment) is initially converged on an
inner region of the information medium 23, 25 while performing a
focus control corresponding to the second information medium 25
having the thickness T2. In cases where the information medium 23
or 25 is the optical disk 171, a piece of distinguishing
information informing that the optical disk 171 having the
thickness T1 is converged by the light L5 (or L4) is detected.
Thereafter, the transmitted light L4 (or the diffracted light L6)
is automatically converged on the outer region 171a of the optical
disk 171 while performing a focus control corresponding to the
first information medium 23 having the thickness T1.
In contrast, in cases where the information medium 23 or 25 is a
thick type of conventional optical disk having a thickness T2, no
distinguishing information is detected when the light L5 (or L4) is
converged on the inner region 171b of the conventional optical
disk. In this case, the focus control corresponding to the second
information medium 25 is continued to detect an information signal
expressing a piece of information recorded on the conventional
optical disk.
Accordingly, in cases where one of the optical head apparatuses
shown in FIGS. 21, 27, 30, 31, 32, 33, 37, 38, 40A, 43, 44, 50 and
52 is utilized, pieces of information can be automatically recorded
or reproduced on or from an information medium regardless of
whether the information medium is thin or thick.
Also, because only the distinguishing information is recorded in
the inner region, the inner region can be small. Therefore, a
memory capacity of the optical disk 171 is not lowered by the
addition of the second recording pit 173.
(Nineteenth Embodiment)
FIG. 54 is a diagonal view of a high density optical disk according
to a nineteenth embodiment, a cross sectional view of the disk
being partially shown.
As shown in FIG. 54, a high density optical disk 174 is partitioned
into an outer region 174a and an inner region 174b. The outer
region 174a occupies a large part of the optical disk 174. The
optical disk 174 has a uniform thickness of T1. The first recording
pits 172 are formed on an information recording substrate 174c of
the outer region 174a to record pieces of information at a high
density. Also, a plurality of second recording pits 175 having a
large size are formed on the information recording substrate 174c
of the inner region 174b at wide intervals to record pieces of
distinguishing information at a lower density than the ordinary
density. The distinguishing information inform that the entire
optical disk 174 has the thickness T1. The thickness T1 of the
optical disk 174, for example, ranges from 0.4 mm to 0.8 mm.
In the above configuration, the diffracted light L5 according to
the first or second embodiment (or the transmitted light L4
according to the third embodiment) is initially converged on an
inner region of the information medium 23 or 25 while performing a
focus control corresponding to the second information medium 25
having the thickness T2. In cases where the information medium 23
or 25 is the optical disk 174, the light L5 (or L4) is converged on
each of the second recording pits 175 in defocus. However, because
each of the second recording pits 175 is large in size, a
converging spot of the light L5 (or L4) is reliably formed in one
of the second recording pits 175. Therefore, a piece of
distinguishing information, which informs that the optical disk 174
having the thickness T1 is converged by the light L5 (or L4), is
detected. Thereafter, the transmitted light L4 (or the diffracted
light L6) is automatically converged on the outer region 174a of
the optical disk 174 while performing a focus control corresponding
to the first information medium 23 having the thickness T1.
In contrast, in cases where the information medium 23 or 25 is a
thick type of conventional optical disk having a thickness T2, no
distinguishing information is detected when the light L5 (or L4) is
converged on the inner region 174b of the conventional optical
disk. In this case, the focus control corresponding to the second
information medium 25 is continued to detect an information signal
expressing a piece of information recorded on the conventional
optical disk.
Accordingly, in cases where one of the optical head apparatuses
shown in FIGS. 21, 27, 30, 31, 32, 33, 37, 38, 40A, 43, 44, 50 and
52 is utilized, pieces of information can be automatically recorded
or reproduced on or from an information medium regardless of
whether the information medium is thin or thick.
Also, because only the distinguishing information is recorded in
the inner region of the optical disk 174, the inner region can be
small. Therefore, a memory capacity of the optical disk 174 is not
lowered by the addition of the second recording pit 173.
Also, because the thickness of the optical disk 174 is uniform, the
optical disk 174 can be easily manufactured at a low cost. Also,
the optical disk 174 can be thinned.
(Twentieth Embodiment)
An optical disk apparatus with one of the optical head apparatuses
in which it is automatically judged whether a high density optical
disk having the thickness T1 or a conventional optical disk having
the thickness T2 is utilized is described.
FIG. 55 is a block diagram of an optical disk apparatus with one of
the optical head apparatuses shown in FIGS. 21, 27, 30, 31, 32, 33,
37, 38, 40A, 43, 44, 50 and 52 according to a twentieth embodiment.
FIG. 56 is a flow chart showing the operation of the optical disk
apparatus shown in FIG. 55. FIG. 63 is a constitutional view of the
optical disk apparatus of which the block diagram is shown in FIG.
55.
As shown in FIG. 63, an optical disk apparatus 176 for recording or
reproducing pieces of information on or from the high density
optical disk 171 (or 174) or the conventional optical disk 25,
comprises the optical head apparatus 51 (or 61, 65, 67, 70, 71, 81,
91, 101, 111, 121, 151 or 161), a moving means 177 such as a feed
mechanism for moving the optical head apparatus 51 to a prescribed
position, a rotating means 178 such as a spindle motor for rotating
the high density optical disk 171 (or 174) or the conventional
optical disk 25, an actuating means representing the actuating unit
58 (not shown in FIG. 63), an electric circuit 179 representing a
focus control means and a tracking control means for controlling
the actuating means to perform a first focus control of the optical
head apparatus 51 corresponding to the first thickness T1 of the
optical disk 171 (or 174) and a second focus control of the optical
head apparatus 51 corresponding to the second thickness T2 of the
optical disk 171 (or 174) or 25 according to a focus error signal
read by the optical head apparatus 51 and controlling the actuating
means to perform a first tracking error control of the optical head
apparatus 51 corresponding to the first thickness T1 and a second
tracking error control of the optical head apparatus 51
corresponding to the second thickness T2 according to a tracking
error signal read by the optical head apparatus 51, and a
connecting means 180 for electrically connecting the rotating means
178, the moving means 177 and the electric circuit 179 with an
electric source (not shown) to supply an electric power to the
rotating means 178, the moving means 177 and the electric circuit
179.
In the above configuration, the high density optical disk 171 or
the conventional optical disk 25 is set to a prescribed position of
the optical disk apparatus 176, and the optical disk 171 or 25 is
rotated by the rotating means 178. Thereafter, the optical head
apparatus 51 is moved to a position just under an innermost
recording track of the optical disk 171 or 25 by the moving means
177 in a step 211, and the diffracted light L5 is converged on the
innermost recording track of the optical disk 171 or 25 while
performing a focus control corresponding to the conventional
optical disk 25 of the thickness T2 in a step 212. Thereafter, a
tracking control is performed, and a piece of information recorded
on the innermost recording track of the optical disk 171 or 25 is
detected in a step 213. In detail, a focus error signal and a
tracking error signal corresponding to a positional relationship
between the optical head apparatus 51 and the optical disk 171 or
25 are sent to the electric circuit 179. In the electric circuit
179, an actuating signal is generated according to the focus error
signal and the tracking error signal and is sent to the actuating
unit 58 to precisely move the compound objective lens 29 (or 29M,
34, 43, 45, 46 or 47) of the optical head apparatus 51. That is,
the second focus and tracking controls of the optical head
apparatus 51 corresponding to the second thickness T2 are performed
to read the information. Thereafter, it is judged in a step 214
whether the information agrees with a piece of distinguishing
information informing that the optical disk 171 having the
thickness T1 is set to the optical disk apparatus 176.
In cases where the high density optical disk 171 is set to the
optical disk apparatus 176, the distinguishing information is
detected. Thereafter, the transmitted light L4 is automatically
converged on the optical disk 171 while performing a focus control
corresponding to the optical disk 171 of the thickness T1 in a step
215. In detail, a focus error signal and a tracking error signal
corresponding to a positional relationship between the optical head
apparatus 51 and the optical disk 171 are sent to the electric
circuit 179. In the electric circuit 179, an actuating signal is
generated according to the focus error signal and the tracking
error signal and is sent to the actuating unit 58 to precisely move
the compound objective lens 29 (or 29M, 34, 43, 45, 46 or 47) of
the optical head apparatus 51. That is, the first focus and
tracking controls of the optical head apparatus 51 corresponding to
the first thickness T1 are performed. Therefore, pieces of
information are recorded or reproduced on or from the optical disk
171.
In contrast, in cases where the conventional optical head 25 is set
to the optical disk apparatus 176, the distinguishing information
is not detected. In this case, the convergence of the diffracted
light L5 on the conventional optical disk 25 is continued while
performing the focus control and the tracking control corresponding
to the conventional optical disk 25 in a step 216. Therefore,
pieces of information are recorded or reproduced on or from the
conventional optical disk 25.
Accordingly, the thickness of the optical disk set in the optical
disk apparatus 176 can be rapidly judged at a high accuracy. Also,
pieces of information can be stably recorded or reproduced on or
from an optical disk regardless of whether the optical disk is the
high density optical disk 171 (or 174) or the conventional optical
disk 25.
(Twenty-first Embodiment)
An optical disk apparatus with one of the optical head apparatuses
in which it is automatically judged whether a high density optical
disk having the thickness T1 or a conventional optical disk having
the thickness T2 is utilized is described.
FIG. 57 is a block diagram of an optical disk apparatus with one of
the optical head apparatuses shown in FIGS. 21, 27, 30, 31, 32, 33,
37, 38, 40A, 43, 44, 50 and 52 according 25 to a twenty-first
embodiment. FIG. 58 is a flow chart showing the operation of the
optical disk apparatus shown in FIG. 57.
As shown in FIG. 57, an optical disk apparatus 176 for recording or
reproducing pieces of information on or from a high density optical
disk 182 or the conventional optical disk 25, comprises the optical
head apparatus 51 (or 61, 65, 67, 70, 71, 81, 91, 101, 111, 121,
151 or 161), the moving means 177, and a rotating means 182 such as
a spindle motor for rotating the high density optical disk 182 or
the conventional optical disk 25. The high density optical disk 182
has no distinguishing information and has the thickness T1.
In the above configuration, the high density optical disk
182 or the conventional optical disk 25 is set to a prescribed
position of the optical disk apparatus 181, and the optical disk
182 or 25 is rotated by the rotating means 182. Thereafter, the
optical head apparatus 51 is moved to a position just under an
innermost recording track of the optical disk 182 or 25 in a step
221 because a piece of information is reliably recorded on the
innermost recording track, and the diffracted light L5 is converged
on the innermost recording track of the optical disk 182 or 25
while performing a focus control corresponding to the conventional
optical disk 25 of the thickness T2 in a step 222. Thereafter, a
tracking control is performed, and a piece of information recorded
on the innermost recording track of the optical disk 182 or 25 is
detected in a step 223. Thereafter, it is judged in a step 224
whether the intensity of an information signal expressing the
information detected is more than a threshold value. That is, the
intensity of the information signal more than the threshold value
denotes that the diffracted light L5 is converged in focus on the
optical disk 182 or 25, and the intensity of the information signal
not more than the threshold value denotes that the diffracted light
L5 is converged in defocus on the optical disk 182 or 25.
In cases where the high density optical disk 182 is set to the
optical disk apparatus 181, the intensity of the information signal
not more than the threshold value is detected. In this case, the
transmitted light L4 is automatically converged on the optical disk
182 while performing a focus control corresponding to the high
density optical disk 182 of the thickness T1 in a step 225.
Therefore, pieces of information are recorded or reproduced on or
from the optical disk 182.
In contrast, in cases where the conventional optical head 25 is set
to the optical disk apparatus 181, the intensity of the information
signal more than the threshold value is detected. In this case, the
convergence of the diffracted light L5 on the conventional optical
disk 25 is continued while performing the focus control and the
tracking control corresponding to the conventional optical disk 25
in a step 226. Therefore, pieces of information are recorded or
reproduced on or from the conventional optical disk 25.
Accordingly, the thickness of the optical disk set in the optical
disk apparatus 181 can be judged even though the optical disk 171
or 174 is not utilized. Also, pieces of information can be stably
recorded or reproduced on or from an optical disk regardless of
whether the optical disk is the high density optical disk 182 or
the conventional optical disk 25.
(Twenty-second Embodiment)
A binary focus microscope having two focal points in which two
images formed on different planes are simultaneously observed is
described according to a twenty-second embodiment.
FIG. 59 is a constitutional view of a binary focus microscope
according to a twenty-second embodiment.
As shown in FIG. 59, a binary focus microscope 191 for
simultaneously observing a first image of a first sample SP1 put on
a first sample plane PL1 and a second image of a second sample SP2
put on a second sample plane PL2, comprises an objective lens 192
having a first focal length F1 for refracting a beam of first light
L17 diverging from the first image and refracting a beam of second
light L18 diverging from the second image, the hologram lens 26 (or
26M, 32, 33 or 42) for transmitting through a part of the first
light L17 without any diffraction and diffracting a part of the
second light L18 to pass the second light L18 through the same
optical path as the first light L17 passes through, an inner lens
193 for converging a beam of superposed light L19 formed of the
first and second light L17, L18 at an inner focal point Pf1, an
ocular lens 194 for simultaneously forming the first and second
images by converging the superposed light L19 diverging from the
inner focal point Pf1, an inner lens-barrel 195 for moving a
combination element of the inner lens 193 and the hologram lens 26
along an optical axis to adjust a distance between the combination
element and the ocular lens 194, and an outer lens-barrel 196 for
moving the objective lens 192 along the optical axis to set the
distance between the first sample plane PL1 and the objective lens
192 to the focal length F1 of the objective lens 192.
The optical axis passes through the centers of the objective lens
192, the hologram lens 26, the inner lens 195 and the ocular lens
194. The position of the first sample plane PL1 differs from that
of the second sample plane PL2 along the optical axis.
In the above configuration, the position of the objective lens 192
is adjusted to set the distance between the first sample plane PL1
and the objective lens 192 to the first focal length F1 of the
objective lens 192. In this case, the distance between the second
sample plane PL2 and the objective lens 192 is set to a second
focal length F2. Also, the position of the combination element is
adjusted to clearly view the first and second images. That is, a
beam of first light L17 diverging from the first image on the first
sample plane PL1 is collimated in the objective lens 192, and a
part of the first light L17 transmits through the hologram lens 26.
Also, a beam of second light L18 diverging from the second image on
the second sample plane PL2 is refracted in the objective lens 192,
and a part of the second light L18 is diffracted in the hologram
lens 26 to pass the second light L18 through the same optical path
as the first light L17 passes through. Therefore, a beam of
superposed light L19 is formed of the first and second light L17,
L18. Thereafter, the superposed light L19 is converged by the inner
lens 193 at an inner focal point Pf1 to simultaneously form the
first and second images enlarged on an image plane PL3, and the
superposed light L19 diverging from the point Pf1 is converged by
the ocular lens 194 to simultaneously form the first and second
images moreover enlarged on an operator's eye.
Accordingly, because the hologram lens 26, 26M, 32, 33 or 42 is
utilized to form the superposed light L19, the first image of the
first sample SP1 put on the first sample plane PL1 and the second
image of the second sample SP2 put on the second sample plane PL2
can be simultaneously observed by simultaneously focusing the
binary focus microscope 191 on the first and second samples SP1,
SP2.
Also, even though the intensities of the first and second light
L17, L18 are reduced when the light L17, L18 pass through the
hologram lens 26, the intensity of the superposed light L19 is
sufficient to observe the first and second images because the
intensity of the superposed light L19 is determined by adding the
intensities of the first and second light L17, L18.
Also, because the hologram lens 26 is blazed as shown in FIG. 6,
the generation of unnecessary diffracted light such as minus
first-order diffracted light is reduced when the second light L18
is diffracted in the hologram lens 26. Therefore, the intensity of
the superposed light L19 can be increased, so that first and second
images observed can be moreover brightened.
Also, as shown in FIG. 60, in cases where the first sample SP1 is
placed at a bottom of a first sample holder 197 and in cases where
the second sample SP2 is placed at a bottom of a second sample
holder 198 located under the first sample holder 197, aberration
such as a chromatic aberration is generated in the first and second
light L17, L18 incident on the objective lens 192 because an
optical path length in the first sample holder 197 for the first
light L17 differs from that in the first and second sample holders
197, 198 for the second light L18. However, the aberration can
disappear in the hologram lens 26 by excessively correcting the
chromatic aberration in the hologram lens 26 as is described in the
first embodiment.
Also, the difference between the first and second focal lengths can
be changed by moving the inner and outer lens-barrels 195, 196
because the distance between the hologram lens 26 and the objective
lens 192 is changed. Therefore, even though the thickness of the
second sample holder 198 is changed, the first and second images
can be reliably observed.
In the twenty-second embodiment, the ocular lens 194 is utilized in
the binary focus microscope 191. However, the ocular lens 194 is
not necessarily required. Also, as shown in FIG. 61, it is
applicable that a camera 199 such as a charge-coupled device (CCD)
camera be placed on the image plane PL3 in place of the ocular lens
194. In this case, a superposed image formed of the first and
second images enlarged can be photographed with the CCD camera 199,
so that the first and second images can be simultaneously
recorded.
(Twenty-third Embodiment)
In cases where a minute circuit is formed on a semiconductor wafer,
a photosensitive material is coated on the semiconductor wafer, and
the photosensitive material covering the semiconductor wafer is
exposed to ultraviolet light through a photomask having a mask
pattern in an exposure process. Therefore, the mask pattern of the
photomask is transferred to the photosensitive material. In this
case, the semiconductor wafer is required to be aligned with the
photomask at a high accuracy in an alignment process performed
prior to the exposure process. Therefore, a reference image drawn
on the semiconductor wafer and the mask pattern drawn on the
photomask are simultaneously observed with a conventional
microscope having a deep focal depth. However, because the
magnification of the conventional microscope having a deep focal
depth is low, it is impossible to align the reference image and the
mask pattern at an accuracy within 5 .mu.m.
To solve the above drawback in the present invention, an alignment
apparatus utilized in the alignment process in which the
semiconductor wafer is aligned with the photomask at a high
accuracy while simultaneously observing a reference image drawn on
the semiconductor wafer and the mask pattern drawn on the photomask
is described according to a twenty-third embodiment.
FIG. 62 is a constitutional view of an alignment apparatus
according to a twenty-third embodiment.
As shown in FIG. 62, an alignment apparatus 201 for aligning a
first reference image RF1 of a mask pattern drawn on a bottom
surface of a photomask 202 with a second reference image RF2 drawn
on a bottom surface of a sample such as a semiconductor substrate
203, comprises a light source 204 for radiating beams of alignment
light having a particular wavelength to illuminate the first and
second reference images RF1, RF2, the objective lens 192 for
receiving a beam of first alignment light L20 diverging from the
first reference image RF1 illuminated with the alignment light and
receiving a beam of second alignment light L21 diverging from the
second reference image RF2 illuminated with the alignment light,
the hologram lens 26 (or 26M, 32, 33 or 42) for transmitting
through a part of the first alignment light L20 without any
diffraction and diffracting a part of the second alignment light
L21 to pass the second alignment light L21 through the same optical
path as the first alignment light L20 passes through, the inner
lens 193 for converging a beam of superposed alignment light L22
formed of the first and second alignment light L20, L21 at an inner
focal point Pf2, a camera 205 such as a charge-coupled device (CCD)
camera placed at the inner focal point Pf2 for simultaneously
photographing and recording the first and second reference images
RF1, RF2, the inner lens-barrel 195, the outer lens-barrel 196, a
moving means 206 for moving the photomask 202 in a horizontal
direction perpendicular to an optical axis to align the first
reference image RF1 with the second reference image RF2 along the
optical axis, and a control means 207 for controlling the movement
of the photomask 202 according to the first and second reference
images RF1, RF2 recorded in the camera 205.
The particular wavelength of the alignment light is determined on
condition that a transmissivity of the semiconductor substrate 203
for the alignment light is sufficiently high. The optical axis
passes through the centers of the objective lens 192, the hologram
lens 26 and the inner lens 193.
A binary microscope 208 is composed of the objective lens 192, the
hologram lens 26 (or 26M, 32, 33 or 42), the inner lens 193, the
inner lens-barrel 195 and the outer lens-barrel 196 in the same
manner as in the twenty-second embodiment.
In the above configuration, a beam of first alignment light L20
diverging from the first reference image RF1 is collimated in the
objective lens 192, and a part of the first alignment light L20
transmits through the hologram lens 26. Also, a beam of second
alignment light L21 diverging from the second reference image RF2
is refracted in the objective lens 192, and a part of the second
alignment light L21 is diffracted by the hologram lens 26 to pass
the second alignment light L21 through the same optical path as the
first alignment light L20 passes through. Therefore, a beam of
superposed alignment light L22 is formed of the first and second
alignment light L20, L21. Thereafter, the superposed alignment
light L22 is converged at an inner focal point Pf2 to
simultaneously form the first and second reference images RF1, RF2
enlarged. Thereafter, the first and second reference images RF1,
RF2 enlarged are photographed and recorded by the camera 205.
Thereafter, a relative position between the first and second
reference images RF1, RF2 is examined in the control means 207, and
the photomask 202 is moved in a horizontal direction by the moving
means 206 under control of the control means 207 to align the first
reference image RF1with the second reference image RF2. Thereafter,
as shown in FIG. 64, a photo sensitive material coated on the
semiconductor substrate 203 is exposed to exposure light radiated
from an exposure light source 211 through a reflecting mirror 212
and a shutter 213.
Accordingly, because the hologram lens 26, 26M, 32, 33 or 42 is
utilized to form the binary microscope 208 having two focal points,
the first reference image RF1 and the second reference image RF2
can be simultaneously observed even though a focal depth of the
binary microscope 208 is low. Also, because the focal depth of the
binary microscope 208 can be lowered, the magnification of the
binary microscope 208 can be heightened. Therefore, the first
reference image RF1 of the photomask 202 can be aligned with the
second reference image RF2 of the semiconductor substrate 203 at a
high accuracy.
(Twenty-fourth Embodiment)
FIG. 65 is a diagonal view of an image reproducing apparatus for
which the optical disk apparatus 176 is provided.
As shown in FIG. 65, an image reproducing apparatus 221 comprises
the optical disk apparatus 176 and a displaying unit 222 such as a
cathode ray tube or a liquid crystal display for displaying pieces
of image information recorded in the optical disk 171, 174 or 25 of
the optical disk apparatus 176 as an image.
In the above configuration, pieces of image information are
recorded in the outer region 171a of the optical disk 171 or in the
optical disk 174 at a high recording density, and the thickness T1
is, for example, 0.6 mm. Also, pieces of image information are
recorded in the conventional optical disk 25 having the thickness
T2 at an ordinary recording density. The conventional optical disk
25 represents a video compact disk having a thickness of 1.2 mm.
Because the optical disk apparatus 176 is provided for the image
reproducing apparatus 221, regardless of whether pieces of
particular image information are recorded in the optical disk 171
(or 174) or the conventional optical disk 25, the particular image
information are read from the optical disk 171, 174 or 25, and a
particular image can be displayed in the displaying unit 222.
Therefore, a user is not required to prepare both a conventional
image reproducing apparatus for reproducing the image information
recorded in the conventional optical disk 25 and an updated image
reproducing apparatus for reproducing the image information
recorded in an updated optical disk having a thickness of 0.6
mm.
FIG. 66 is a diagonal view of a voice reproducing apparatus for
which the optical disk apparatus 176 is provided.
As shown in FIG. 66, a voice reproducing apparatus 231 comprises
the optical disk apparatus 176 and a voice reproducing unit 232
such as a speaker for reproducing pieces of voice information
recorded in the optical disk 171, 174 or 25 of the optical disk
apparatus 176 as voices. The voice reproducing apparatus 231
additionally comprises a radio 233 and a cassette tape recorder
234.
In the above configuration, pieces of voice information are
recorded in the outer region 171a of the optical disk 171 or in the
optical disk 174 at a high recording density, and the thickness T1
is, for example, 0.6 mm. Also, pieces of voice information are
recorded in the conventional optical disk 25 having the thickness
T2 at an ordinary recording density. The conventional optical disk
25 represents an audio compact disk having a thickness of 1.2 mm.
Because the optical disk apparatus 176 is provided for the voice
reproducing apparatus 231, regardless of whether pieces of
particular voice information are recorded in the optical disk 171
(or 174) or the conventional optical disk 25, the particular voice
information are read from the optical disk 171, 174 or 25, and
particular voices can be reproduced by the voice reproducing unit
232. Therefore, a user is not required to prepare both a
conventional voice reproducing apparatus for reproducing the voice
information recorded in the conventional optical disk 25 and an
updated voice reproducing apparatus for reproducing the voice
information recorded in an updated optical disk having a thickness
of 0.6 mm.
FIG. 67 is a diagonal view of an information processing apparatus
for which the optical disk apparatus 176 is provided.
As shown in FIG. 67, an information processing apparatus 241
comprises the optical disk apparatus 176, an input apparatus 242
for inputting pieces of input information, a central processing
unit 243 placed on a circuit substrate 244 for processing pieces of
recorded information recorded in the optical disk 171, 174 or 25 of
the optical disk apparatus 176 or processing the input information
to record the input information in the optical disk 171, 174, and a
displaying unit 245 for displaying the recorded information
processed in the central processing unit 243.
In the above configuration, pieces of recorded information are
recorded in the outer region 171a of the optical disk 171 or in the
optical disk 174 at a high recording density, and the thickness T1
is, for example, 0.6 mm. Also, pieces of recorded information are
recorded in the conventional optical disk 25 having the thickness
T2 at an ordinary recording density. The conventional optical disk
25 represents a CD-ROM having a thickness of 1.2 mm. Because the
optical disk apparatus 176 is provided for the voice reproducing
apparatus 231, regardless of whether pieces of particular recorded
information are recorded in the optical disk 171 (or 174) or the
conventional optical disk 25, the particular recorded information
are read from the optical disk 171, 174 or 25, and a particular
image can be displayed in the displaying unit 245 according to the
recorded information. Also, when a user inputs pieces of input
information to the inputting apparatus 242, even though any of the
optical disks 171, 174 and 25 is set in the optical disk apparatus
176, the input information are recorded in the optical disk 171,
174 or 25. Therefore, the user is not required to prepare both a
conventional image reproducing apparatus for reproducing the image
information recorded in the conventional optical disk 25 and an
updated image reproducing apparatus for reproducing the image
information recorded in an updated optical disk having a thickness
of 0.6 mm.
In cases where a game program is recorded in the optical disk 171,
174 or 25, the user can play a game while observing a game image
displayed in the displaying unit 245 and inputting pieces of
operating data to the inputting apparatus 242 regardless of whether
the game program is recorded in any of the optical disks 171, 174
or 25.
Also, in cases where the information processing apparatus 241 is
utilized in a home, the information processing apparatus 241 can be
utilized as an information terminal for a domestic use.
Also, as shown in FIG. 68, in cases where a key board 245 is
utilized as the inputting apparatus 242, the information processing
apparatus 241 can be utilized as a computer system 246.
Having illustrated and described the principles of our invention in
a preferred embodiment thereof, it should be readily apparent to
those skilled in the art that the invention can be modified in
arrangement and detail without departing from such principles. We
claim all modifications coming within the spirit and scope of the
accompanying claims.
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