U.S. patent application number 09/772931 was filed with the patent office on 2001-06-28 for optical filter and optical device provided with this optical filter.
This patent application is currently assigned to NIKON CORPORATION. Invention is credited to Osawa, Keiji, Shibazaki, Kiyoshige.
Application Number | 20010005283 09/772931 |
Document ID | / |
Family ID | 27282277 |
Filed Date | 2001-06-28 |
United States Patent
Application |
20010005283 |
Kind Code |
A1 |
Osawa, Keiji ; et
al. |
June 28, 2001 |
Optical filter and optical device provided with this optical
filter
Abstract
Light emitted from a taking lens 20 enters a first birefringent
plate la to be spatially divided along a first direction extending
perpendicular to the direction in which the light advances to
achieve two separate rays L10 and L20. The vibrational planes of
the two light fluxes L10 and L20 emitted from the first
birefringent plate 1a are converted to a circularly polarized light
by a phase plate 1c. The two light fluxes L10' and L20' emitted
from the phase plate 1c are each spatially divided into two by a
second birefringent plate 1d along a second direction extending
perpendicular to the first direction to achieve four separate rays
L11, L12, L21 and L22, to be guided to an imaging plane 15a of an
imaging device 15. At least either the first birefringent plate or
the second birefringent plate is constituted of lithium niobate,
rutile. Chilean nitrate, or the like.
Inventors: |
Osawa, Keiji; (Chuou-ku,
JP) ; Shibazaki, Kiyoshige; (Higashimurayama-shi,
JP) |
Correspondence
Address: |
OLIFF & BERRIDGE, PLC
277 S. WASHINGTON STREET, SUITE 500
ALEXANDRIA
VA
22314
US
|
Assignee: |
NIKON CORPORATION
|
Family ID: |
27282277 |
Appl. No.: |
09/772931 |
Filed: |
January 31, 2001 |
Related U.S. Patent Documents
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Application
Number |
Filing Date |
Patent Number |
|
|
09772931 |
Jan 31, 2001 |
|
|
|
09281324 |
Mar 30, 1999 |
|
|
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Current U.S.
Class: |
359/489.19 ;
348/E5.028 |
Current CPC
Class: |
G02B 5/3083 20130101;
G02B 27/46 20130101; H04N 5/2254 20130101; G02B 27/288 20130101;
G02B 17/0856 20130101 |
Class at
Publication: |
359/497 ;
359/494; 359/495 |
International
Class: |
G02B 005/30; G02B
027/28 |
Foreign Application Data
Date |
Code |
Application Number |
Mar 31, 1998 |
JP |
10-101822 |
Jul 13, 1998 |
JP |
10-197610 |
Jan 27, 1999 |
JP |
11-018596 |
Claims
What is claimed is:
1. An optical filter comprising: a first birefringent plate
constituting an optical element that spatially divides incident
light along a first direction extending perpendicular to a
direction in which the incident light advances to achieve two
separate light fluxes; a vibrational plane converting plate that
changes the vibrational plane of each of the two light fluxes
emitted from said first birefringent plate; and a second
birefringent plate constituting an optical element that spatially
divides each of the two light fluxes emitted from said vibrational
plane converting plate into two light fluxes along a second
direction which is different from said first direction, to achieve
a total of four separate light fluxes, wherein: at least either
said first birefringent plate or said second birefringent plate is
constituted of a material with a larger difference between the
extraordinary ray refractive index and the ordinary ray refractive
index compared to that of quartz.
2. An optical filter according to claim 1, further comprising: an
IR blocking filter constituting an optical element provided between
said first birefringent plate and said second birefringent
plate.
3. An optical filter according to claim 1, wherein: an
anti-reflection coating is applied to a boundary surface of said
first birefringent plate and an optical element provided adjacent
to said first birefringent plate and to a boundary surface of said
second birefringent plate and an optical element provided adjacent
to said second birefringent plate.
4. An optical filter according to claim 1, wherein: said first
birefringent plate and said second birefringent plate are both
thinner than other optical elements.
5. An optical filter according to claim 1, wherein: said
vibrational plane converting plate is constituted of a phase plate
that is capable of creating a specific quantity of phase difference
between a light component vibrating in one vibrating direction and
a light component vibrating in another vibrating direction
extending perpendicular to the one vibrating direction for the two
light fluxes emitted from said first birefringent plate.
6. An optical filter according to claim 1, wherein: said
vibrational plane converting plate is constituted of an optical
rotatory plate provided as an optical element for rotating
vibrating directions of vibrational planes of the two light fluxes
emitted from said first birefringent plate by a specific
degree.
7. An optical apparatus comprising: an imaging device for
converting an object image formed by an image forming lens mounted
in said optical apparatus to an image signal, and an optical filter
which is provided between said image forming lens and said imaging
device, said optical filter having: a first birefringent plate
constituting an optical element that spatially divides incident
light along a first direction extending perpendicular to a
direction in which the incident light advances to achieve two
separate light fluxes; a vibrational plane converting plate that
changes the vibrational plane of each of the two light fluxes
emitted from said first birefringent plate; and a second
birefringent plate constituting an optical element that spatially
divides each of the two light fluxes emitted from said vibrational
plane converting plate into two light fluxes along a second
direction which is different from said first direction, to achieve
a total of four separate light fluxes, wherein: at least either
said first birefringent plate or said second birefringent plate is
constituted of a material with a larger difference between the
extraordinary ray refractive index and the ordinary ray refractive
index compared to that of quartz.
8. An optical apparatus according to claim 7, further comprising: a
quick return mirror; a focal plane shutter; and a TTL focus
detection device that detects a focal point position of said image
forming lens, wherein: said optical filter is provided outside an
optical path between said taking lens and said TTL focus detecting
device.
9. An optical filter comprising: a first birefringent plate that
spatially divides light emitted from an image forming lens along a
first direction into two separate light fluxes; a phase plate that
is capable of creating a specific quantity of phase difference
between a light component vibrating in one vibrating direction and
a light component vibrating in another vibrating direction
extending perpendicular to said one vibrating direction for the two
light fluxes emitted from said first birefringent plate; and a
second birefringent plate having a thickness and a refractive index
both almost equal to a thickness and a refractive index of said
first birefringent plate and provided to spatially divide each of
the two light fluxes emitted from said phase plate along a second
direction which is different from said first direction to achieve
two separate light fluxes to be guided to an imaging plane of an
imaging device, wherein: with A representing an image height at a
corner of an focal plane and PO representing an air equivalent
optical path length from said imaging plane to an exit pupil of
said image forming lens, the thickness t1 and the refractive index
n1 of said first birefringent plate and said second birefringent
plate satisfy the conditional equation below, when
A/PO.gtoreq.0.15. 24 t1 C .times. n1 Y ( n1 ) ( 55 ) with 25 Y ( n1
) = 1 - cos cos 1 ( 56 ) C = 1 2 .times. { K .times. B .times. d
.times. Fno - ( 1 - cos cos 2 ) .times. t2 n2 } ( 57 ) sin 1 = sin
n1 ( 58 ) 1 = sin - 1 ( sin n1 ) ( 59 ) 2 = sin - 1 ( n1 .times.
sin n2 ) ( 60 ) 0.25 K 0.35 ( 61 ) 1 B 3 ( 62 ) t1: thicknesses of
the first birefringent plate and the second birefringent plate n1:
refractive indices of the first birefringent plate and the second
birefringent plate t2: thickness of the phase plate n2: refractive
index of phase plate d: pixel pitch at the imaging device .phi.:
Angle of incidence at a first birefringent plate of light flux
entering corner of the imaging plane of the imaging device from the
center of the exit pupil of the taking lens Fno: F number of the
taking lens
10. An optical filter comprising: a first birefringent plate that
spatially divides light emitted from an image forming lens along a
first direction into two separate light fluxes; a phase plate that
is capable of creating a specific quantity of phase difference
between a light component vibrating in one vibrating direction and
a light component vibrating in another vibrating direction
extending perpendicular to said one vibrating direction for the two
light fluxes emitted from said first birefringent plate; and a
second birefringent plate having a refractive index almost equal to
a refractive index of said first birefringent plate and provided to
spatially divide each of the two light fluxes emitted from said
phase plate along a second direction which is different from said
first direction to achieve two separate light fluxes to be guided
to an imaging plane of an imaging device, wherein: with A
representing an image height at a corner of an focal plane and PO
representing an air equivalent optical path length from said
imaging plane to an exit pupil of said image forming lens, a
thickness t11 and the refractive index n1 of said first
birefringent plate and a thickness t12 and a refractive index n1 of
said second birefringent plate satisfy the conditional equation
below, when A/PO.gtoreq.0.15. 26 t11 + t12 C1 .times. n1 Y ( n1 ) (
63 ) with 27 Y ( n1 ) = 1 - cos cos 1 ( 64 ) C1 = K .times. B
.times. d .times. Fno - ( 1 - cos cos 2 ) .times. t2 n2 ( 65 ) sin
1 = sin n1 ( 66 ) 1 = sin - 1 ( sin n1 ) ( 67 ) 2 = sin - 1 ( n1
.times. sin n2 ) ( 68 ) 0.25 K 0.35 ( 69 ) 1 B 3 ( 70 ) t11:
thickness of the first birefringent plate t12 : thickness of the
second birefringent plate n1: refractive indices of the first
birefringent plate and the second birefringent plate t2: thickness
of the phase plate n2: refractive index of phase plate d: pixel
pitch at the imaging device .phi.: Angle of incidence at a first
birefringent plate of light flux entering corner of the imaging
plane of the imaging device from the center of the exit pupil of
the taking lens Fno: F number of the taking lens
11. An optical filter comprising: a first birefringent plate that
spatially divides light emitted from an image forming lens along a
first direction into two separate light fluxes; a phase plate that
is capable of creating a specific quantity of phase difference
between a light component vibrating in one vibrating direction and
a light component vibrating in another vibrating direction
extending perpendicular to said one vibrating direction for the two
light fluxes emitted from said first birefringent plate; and a
second birefringent plate having a thickness and a refractive index
both different from a thickness and a refractive index of said
first birefringent plate and provided to spatially divide each of
the two light fluxes emitted from said phase plate in a second
direction which is different from said first direction to achieve
two separate light fluxes from each of the two light fluxes to be
guided to an imaging plane of an imaging device, wherein: with A
representing an image height at a corner of an focal plane and PO
representing an air equivalent optical path length from said
imaging plane to an exit pupil of said image forming lens, the
thickness t11 and the refractive index n11 of said first
birefringent plate and the thickness t12 and the refractive index
n12 of said second birefringent plate satisfy the conditional
equation below. when A/PO.gtoreq.0.15. 28 ( 1 - cos cos 1 ) .times.
t11 n11 + ( 1 - cos cos 3 ) .times. t12 n12 C2 ( 71 ) with 29 C2 =
K .times. B .times. d .times. Fno - ( 1 - cos cos 2 ) .times. t2 n2
( 72 ) sin 1 = sin n11 ( 73 ) 1 = sin - 1 ( sin n11 ) ( 74 ) 2 =
sin - 1 ( n11 .times. sin 1 n2 ) ( 75 ) 3 = sin - 1 ( n2 .times.
sin 2 n12 ) ( 76 ) 0.25 K 0.35 ( 77 ) 1 B 3 ( 78 ) t11: thickness
of the first birefringent plate t12: thickness of the second
birefringent plate n11: refractive index of the first birefringent
plate n12: refractive index of the second birefringent plate t2:
thickness of the phase plate n2: refractive index of phase plate d:
pixel pitch at the imaging device .phi.: Angle of incidence at a
first birefringent plate of light flux entering corner of the
imaging plane of the imaging device from the center of the exit
pupil of the taking lens Fno: F number of the taking lens
12. An optical filter according to claim 1, further comprising: a
neutralizing circuit for neutralizing electrical charge stored at
said first birefringent plate and said second birefringent
plate.
13. An optical apparatus according to claim 7, further comprising:
a neutralizing circuit for neutralizing an electrical charge stored
at, at least, one of said optical filter, said image forming lens
and said imaging device.
14. An optical apparatus comprising: a photoelectric conversion
device that converts an optical image guided to a photosensitive
portion of said photoelectric conversion device to an electrical
signal, provided with a cover member to cover said photosensitive
portion; a transparent electrode formed at a front surface of said
cover member; and a conductive member electrically connected to
said transparent electrodes for neutralizing an electrical charge
occurring at said photoelectric conversion device caused by an
electrical charge.
15. An optical apparatus comprising: a photoelectric conversion
device that converts an optical image formed by an image forming
lens to an electrical signal; an optical member provided in an
optical path between said image forming lens and said photoelectric
conversion device; a transparent electrode provided, at least, at a
front surface of said optical member located close to an image
forming plane of said image forming lens; and a conductive member
electrically connected to said transparent electrode and provided
to neutralize an electrical charge occurring at said optical member
caused by an electrical charge.
16. An optical apparatus according to claim 14, further comprising:
a voltage source for reducing an adhesive force with which foreign
matter adheres to said photoelectric conversion device by applying
a voltage to said conductive member.
17. An optical apparatus according to claim 15, further comprising:
a shutter that can be switched between a light blocking state in
which light flux entering said photoelectric conversion device is
blocked and an open state in which the light flux is allowed to
pass, wherein: said conductive member neutralizes an electrical
charge occurring at said photoelectric conversion device during an
operation of said shutter.
18. An optical apparatus according to claim 17, further comprising:
a voltage source for reducing an adhesive force with which foreign
matter adheres to said optical member by applying a voltage to said
conductive member.
19. An optical apparatus according to claim 17, further comprising:
a control circuit that applies a voltage to said optical member
while sustaining an open state for said shutter.
Description
INCORPORATION BY REFERENCE
[0001] The disclosures of the following priority applications are
herein incorporated by reference:
[0002] Japanese Patent Application No. 10-101822, filed Mar. 31,
1998
[0003] Japanese Patent Application No. 10-197610, filed Jul. 13,
1998
[0004] Japanese Patent Application No. 11-18596, filed Jan. 27,
1999
BACKGROUND OF THE INVENTION
[0005] 1. Field of the Invention
[0006] The present invention relates to an optical filter and an
optical device provided with this optical filter.
[0007] 2. Description of the Related Art
[0008] In a digital still camera employing an imaging device such
as a CCD (hereafter a digital still camera is simply referred to as
a "DSC" in this specification), "beat" interference may occur as a
result of a certain relationship between the spatial frequency of
the subject image and the repetitive pitch of dot-type on-chip
color separation filters provided at the front surface of the
imaging device. In order to prevent any false color signals from
being generated by the beat, i.e., in order to prevent the
so-called "color moire," an optical low-pass filter is provided
between the taking lens and the imaging device. The optical
low-pass filter, which is constituted by employing a birefringent
plate achieving birefringence, reduces the generation of the beat
through the birefringent effect provided by the birefringent plate.
Normally, quartz is employed to constitute the birefringent
plate.
[0009] Japanese Examined Patent Publication No. 1994-20316 proposes
an optical low-pass filter employing two birefringent plates such
as that described above, which is suited for application in an
imaging device provided with dot-type on-chip color separation
filters. This optical low-pass filter is constituted by enclosing a
quarter-wave plate between two birefringent plates with the
directions in which the image becomes shifted through the
birefringence offset by approximately 90.degree. from each
other.
[0010] Now, the so-called direct image forming system, in which the
imaging device is directly provided at the primary image forming
plane of the taking lens without employing a reduction lens system
or the like is becoming the mainstay in single lens reflex type
DSCs that allow interchange of the taking lens among DSCs in recent
years. The advent of the direct image forming system has been
realized through the utilization of imaging devices having a large
image area of approximately 15.5 mm.times.22.8 mm that have been
manufactured in recent years to replace 2/3" size (approximately
6.8 mm.times.8.8 mm) and 1" size (approximately 9.3 mm.times.14 mm)
imaging devices that have been conventionally used in television
cameras and the like. With this size of image area available, an
image plane having a size (approximate aspect ratio 2:3=15.6
mm.times.22.3 mm), which is comparable to the image plane size of
the C-type silver halide film IX240 system (APS), is achieved. By
employing an imaging device achieving a relatively large image
area, it becomes possible to adopt a camera system that employs the
135-type photographic film in a DSC. To explain this point,
providing a 2/3" size or 1" size imaging device at the field of a
camera using the 135-type film only achieves a small image plane
size for the imaging device compared to the image plane size of the
135-type film (24 mm.times.36 mm). As a result, a large difference
will manifest in the angle of field achieved by a taking lens
having a specific focal length, to cause the photographer to feel
restricted. This problem becomes eliminated as the image area of
the imaging device increases and becomes closer to the image plane
size of the 135-type film.
[0011] However, as the image area in a single lens reflex type DSC,
which forms the primary image with the taking lens at an image
device directly, increases, the problems explained below arise to a
degree to which they cannot be neglected.
[0012] Imaging devices in DSCs in recent years have evolved in two
directions, i.e., toward a higher concentration of pixels and
toward a larger image plane. When the number of pixels is increased
to exceed 1 million pixels while maintaining the size of the image
plane at approximately 1/3" to 1/2" as in the prior art, the pixel
pitch becomes reduced. For instance, in an imaging device having
approximately 1,300,000 pixels, with its image plane size at
approximately 1/3," the pixel pitch is approximately 4 .mu.m.
Generally speaking, the pixel pitch "p" at an imaging device and
the thickness "t" of the birefringent plates constituting the
optical low-pass filter which is employed to support the pixel
pitch "p" achieve the relationship expressed through the following
equation (1)
P=t(ne.sup.2-no.sup.2)/(2ne.times.no) (1)
[0013] with
[0014] t: birefringent plate thickness
[0015] ne: extraordinary ray refractive index at birefringent
plate
[0016] no: ordinary ray refractive index at birefringent plate
[0017] When a quartz plate, which is most commonly employed to
constitute a birefringent plate, is used in an imaging device with
a pixel pitch of approximately 4 .mu.m, the thickness "t" required
of the quartz plate is concluded to be approximately 0.7 mm by
working backward with "p" in equation (1) set at 4 .mu.m, since the
refractive indices of quartz for light having a wavelength of 589
nm are ne=1.55336 and no=1.54425. Since the thickness of the
quarter-wave plate needs to be approximately 0.5 mm regardless of
the pixel pitch p, the entire thickness achieved when constituting
an optical low-pass filter by pasting together three plates, i.e.,
two quartz plates (birefringent plates) and one quarter-wave plate,
will be approximately 2 mm.
[0018] However, when the area of the photosensitive surface of an
imaging device increases, as in the case of, in particular, an
imaging device employed in a single lens reflex type DSC, it
becomes necessary to increase the thickness of the optical low-pass
filter for the reasons detailed below.
[0019] While the size of the image plane of a 1/3" imaging device
is approximately 3.6 mm.times.4.8 mm, let us now consider an
imaging device having an image plane size equivalent to that of the
C-type (aspect ratio 2:3=16 mm.times.24 mm) in an IX240 system
(advanced photo system (APS)) with silver halide film. When pixels
are arrayed at a pixel pitch of approximately 4 .mu.m on this
imaging device, the total number of pixels for the entire image
plane will exceed 20 million by simple calculation, and it is
considered that the current technical level is not high enough to
realize such a large number of pixels for practical use from the
viewpoints of the yield in imaging device production, the scale and
processing speed of the image information processing circuit and
the like. As a result, it is assumed that it is appropriate to set
the number of pixels at approximately two million and several
hundreds of thousands in an imaging device having a large image
plane equivalent to that of the APS-C type, which sets the pixel
pitch at 10 and several .mu.m.
[0020] For instance, when an APS-C size imaging device (16
mm.times.24 mm) is prepared at a pixel pitch set to 12 .mu.m, the
number of pixels in the imaging device will be approximately
2,670,000. When constituting the birefringent plates of the optical
low-pass filter employed in combination with the imaging device
having the pixel pitch of 12 .mu.m with quartz, the thickness of a
single quartz plate is calculated to be "t"=2.04 mm by
incorporating "p"=12 .mu.m in equation (1). By adding the
thicknesses of two such quartz plates and a quarter-wave plate (0.5
mm), the thickness of the optical low-pass filter is calculated to
be 4.58 mm, which is more than twice as large as the thickness of
an optical low-pass filter (thickness: 2 mm) with the pixel pitch
set at 4 .mu.m.
[0021] In addition, since the spectral sensitivity of an imaging
device is different from the spectral sensitivity of the human eye,
an IR blocking filter is normally provided to cut off infrared
light within the imaging optical path in a DSC employing an imaging
device. This IR blocking filter (thickness; approximately 0.8 mm)
is also provided pasted to the optical low-pass filter. Thus, the
entire thickness of the optical low-pass filter supporting the
pixel pitch of 12 .mu.m will go up to 5.38 mm when the thickness of
the IR blocking filter is included.
[0022] It is difficult to place an optical low-pass filter having
such a thickness between a taking lens and an imaging device. Even
in the case of a regular lens shutter type DSC, which does not
require any member to be provided between the rear end of the
taking lens and the photosensitive surface of the imaging device
except for the optical low-pass filter, it must be ensured in
design that the minimum value (the so-called back focal distance)
of the distance between the rearmost end of the taking lens and the
imaging device is larger than the thickness of the optical low-pass
filter. Setting the length of the back focal distance of the taking
lens larger than the focal length of the taking lens imposes
restrictions in terms of the optical design.
[0023] Furthermore, in the case of a single lens reflex type DSC,
which directly forms an image of the subject achieved by a taking
lens on a large size imaging device without employing a reduction
lens system, a quick return mirror for switching the optical path
between the viewfinder and the imaging system or a fixed
semitransparent mirror (beam splitter) is needed between the taking
lens and the imaging device. In addition, a mechanical shutter is
required for defining an exposure time and for blocking the imaging
device from exposure during an image signal read operation at the
imaging device. While this structure having a mirror and a shutter
provided between the taking lens and its image forming plane is
also adopted in a single lens reflex camera that employs regular
silver halide film, it is difficult to provide an optical low-pass
filter having a thickness exceeding 5 mm in addition while ensuring
that it does not present any obstacle in the operation or the
mirror at the shutter. It merits particular note that more and more
cameras in recent years adopt the autofocus (AF) function, and that
a single lens reflex camera with the AF function adopts a structure
having a sub mirror provided to the rear of the quick return
mirror, i.e., between the quick return mirror and the shutter, to
guide light flux to a focal point detection device. This makes it
even more difficult to position an optical low-pass filter having a
thickness exceeding 5 mm.
[0024] In addition to the problem of an increased thickness of the
optical low-pass filter resulting from a larger pixel pitch in a
larger imaging device as described above, another problem arises as
detailed below.
[0025] Normally, the length of the air equivalent optical path
achieved when light is transmitted and advances through a medium
having a thickness "t" and a refractive index "n" is expressed as
t/n. In other words, the air equivalent optical path lengths
achieved when light advances through media having the same
refractive index "n" but having different thicknesses "t", vary.
Now, let us consider light emitted from one point on the optical
axis of a photographic optical system toward an imaging device to
reach the center of the image plane of the imaging device and light
emitted from the same point on the optical axis of the photographic
optical system toward the imaging device to reach the periphery of
the image plane.
[0026] Since the light that reaches the center of the image plane
enters the light entry surface of the optical low-pass filter at
almost a right angle, "t" roughly equals the thickness of the
optical low-pass filter. In contrast, since the light reaching the
periphery of the image plane advances diagonally through the
optical low-pass filter, "t" here is larger than the "t"
encountered by the light reaching the center of the image plane.
Since the lengths of the air equivalent optical paths achieved by
light being transmitted through the optical low-pass filter are
different for the light reaching the center of the image plane and
the light reaching the periphery of the image plane as explained
above, a focus misalignment occurs in the direction of the optical
axis between the image plane center and the image plane periphery.
The degree of this focus misalignment increases as the thickness of
the optical low-pass filter increases as described above, which may
result in a reduced image quality at the peripheral area of the
image plane.
[0027] As the size of the imaging device is increased, a problem of
foreign matter becoming transferred as explained next, i.e., a
problem of foreign matter such as dust and lint adhering to the
photosensitive surface of the imaging device to cast a shadow onto
the image captured by the imaging device, tends to occur readily,
in addition to the problems discussed above. In particular, in an
interchangeable lens type DSC in which foreign matter such as dust
and lint readily enters the mirror box when the taking lens is
detached, this problem is more pronounced.
[0028] A similar problem occurs in optical devices such as
facsimile machines and image scanners when foreign matter such as
dust and lint materialize as a document is transmitted or the
document read unit moves, which may become adhered to the vicinity
of the photosensitive surface of the photoelectric conversion
element or the glass (platen glass) upon which the document is
placed to result in a shadow being cast on the input image, as in
the interchangeable lens type DSC.
[0029] Now, since the crystal of quartz employed to constitute
birefringent plates imparts a piezoelectric effect, the crystal
itself is caused to become electrically charged readily by
vibration or the like. The quartz crystal also has a property that
does not allow a stored electrical charge to be discharged easily.
In addition, since an insulating material such as plastic, ceramic
or the like is employed to constitute the imaging device package,
the electrical charge stored at the imaging device cannot be
released with ease.
[0030] Vibration and air currents occurring as a result of an
operation of an optical device sometimes cause the foreign matter
discussed above to become suspended inside the optical device,
which may ultimately become adhered to the electrically charged
birefringent plates, imaging device or the like, as explained
above. Consequently, the operator of the optical device is required
to clean the optical device frequently to prevent shadows from
being cast as explained earlier.
SUMMARY OF THE INVENTION
[0031] A first object of the present invention is to provide an
optical filter achieving a small thickness and an optical device
provided with the optical filter.
[0032] A second object of the present invention is to provide an
optical low-pass filter which is capable of preventing the loss of
image quality at the periphery of the image plane even when the
image area at the imaging device is expanded or even when the pixel
pitch is increased, and an optical device provided with the optical
low-pass filter.
[0033] A third object of the present invention is to prevent
foreign matter from becoming adhered to the optical filter
described above, a photoelectric conversion element and the like to
cast shadows thereupon, by neutralizing an electrical charge
occurring as a result of the optical filter, the photoelectric
conversion element and the like becoming electrically charged.
[0034] In order to achieve the objects described above, the present
invention comprises a first birefringent plate constituting an
optical element that spatially divides incident light into two
separate light fluxes along a first direction extending
perpendicular to the direction in which the incident light
advances, a vibrational plane converting plate that changes the
vibrational planes of the two light fluxes emitted from the first
birefringent plate and a second birefringent plate constituting an
optical element that spatially divides each of the two light fluxes
emitted from the vibrational plane converting plate into two light
fluxes along a second direction that is different from the first
direction to achieve a total of four separate light fluxes, with at
least either the first birefringent plate or the second
birefringent plate, constituted of a material having a larger
difference between the extraordinary ray refractive index and the
ordinary ray refractive index compared to that of quartz.
[0035] In addition, according to the present invention, an
anti-reflection coating is applied to a boundary surface of the
first birefringent plate and an optical element provided adjacent
to the first birefringent plate and a boundary surface of the
second birefringent plate and an optical element provided adjacent
to the second birefringent plate.
[0036] Furthermore, according to the present invention, the
vibrational plane converting plate is constituted of a phase plate
that is capable of creating a phase difference of a specific
quantity between a light component that vibrates in one vibrating
direction and a light component that vibrates in another vibrating
direction extending perpendicular to the one vibrating direction
for each of the two light fluxes emitted from the first
birefringent plate.
[0037] According to the present invention, the vibrational plane
converting plate may be constituted of an optical rotatory plate
provided as an optical element that rotates the directions of
vibration of the two light fluxes emitted from the first
birefringent plate at the vibrational plane by a specific
degree.
[0038] Alternatively, the present invention comprises a first
birefringent plate for spatially dividing light emitted from an
image forming lens along a first direction to achieve two separate
light fluxes, a phase plate that creates a phase difference of a
specific quantity between a light component that vibrates in one
vibrating direction and a light component that vibrates in another
vibrating direction extending perpendicular to the one vibrating
direction for each of the two light fluxes emitted from the first
birefringent plate and a second birefringent plate having almost
the same thickness and almost the same refractive index as those of
the first birefringent plate, provided for spatially dividing each
of the two light fluxes emitted from the phase plate along a second
direction that is different from the first direction to achieve two
separate light fluxes to be guided to the imaging plane of the
imaging device, with the thickness t1 and the refractive index n1
of the first birefringent plate and the second birefringent plate
satisfying the following conditional equation, with A representing
the image height at the image plane corners, PO representing the
air equivalent optical path length extending from the imaging plane
to the exit pupil of the image forming lens and A/PO.gtoreq.0.15
satisfied. 1 t1 C .times. n1 Y ( n1 ) ( 2 )
[0039] with 2 Y ( n1 ) = 1 - cos cos 1 ( 3 ) C = 1 2 .times. { K
.times. B .times. d .times. Fno - ( 1 - cos cos 2 ) .times. t2 n2 }
( 4 ) sin 1 = sin n1 ( 5 ) 1 = sin - 1 ( sin n1 ) ( 6 ) 2 = sin 1 (
n1 .times. sin n2 ) ( 7 ) 0.25 K 0.35 ( 8 ) 1 B 3 ( 9 )
[0040] t1: thicknesses of the first birefringent plate and the
second birefringent plate
[0041] n1: refractive indices of the first birefringent plate and
the second birefringent plate
[0042] t2: thickness of the phase plate
[0043] n2: refractive index of phase plate
[0044] d: pixel pitch at the imaging device
[0045] .phi.: Angle of incidence at a first birefringent plate of
light flux entering corner of the imaging plane of the imaging
device from the center of the exit pupil of the taking lens
[0046] Fno: F number of the taking lens
[0047] Alternatively, the present invention may comprise a first
birefringent plate for spatially dividing light emitted from an
image forming lens along a first direction to achieve two separate
light fluxes, a phase plate that creates a phase difference of a
specific quantity between a light component that vibrates in one
vibrating direction and a light component that vibrates in another
vibrating direction extending perpendicular to the one vibrating
direction for each of the two light fluxes emitted from the first
birefringent plate and a second birefringent plate is having almost
the same refractive index as that of the first birefringent plate,
provided for spatially dividing each of the two light fluxes
emitted from the phase plate along a second direction that is
different from the first direction to achieve two separate light
fluxes to be guided to the imaging plane of the imaging device,
with the thickness t11 and the refractive index n1 of the first
birefringent plate and the thickness t12 and the refractive index
n1 of the second birefringent plate satisfying the following
conditional equation, with A representing the image height at the
image plane corners, PO representing the air equivalent optical
path length extending from the imaging plane to the exit pupil of
the image forming lens and A/PO.gtoreq.0.15 satisfied. 3 t11 + t12
C1 .times. n1 Y ( n1 ) ( 10 )
[0048] with 4 Y ( n1 ) = 1 - cos cos 1 ( 11 ) C1 = K .times. B
.times. d .times. Fno - ( 1 - cos cos 2 ) .times. t2 n2 ( 12 ) sin
1 = sin n1 ( 13 ) 1 = sin - 1 ( sin n 1 ) ( 14 ) 2 = sin - 1 ( n1
.times. sin n2 ) ( 15 ) 0.25 K 0.35 ( 16 ) 1 B 3 ( 17 )
[0049] t11: thickness of the first birefringent plate
[0050] t12: thickness of the second birefringent plate
[0051] n1: refractive indices of the first birefringent plate and
the second birefringent plate
[0052] t2: thickness of the phase plate
[0053] n2: refractive index of phase plate
[0054] d: pixel pitch at the imaging device
[0055] .phi.: Angle of incidence at a first birefringent plate of
light flux entering corner of the imaging plane of the imaging
device from the center of the exit pupil of the taking lens
[0056] Fno: F number of the taking lens
[0057] Alternatively, the present invention may comprise a first
birefringent plate for spatially dividing light emitted from an
image forming lens along a first direction to achieve two separate
light fluxes, a phase plate that creates a phase difference of a
specific quantity between a light component that vibrates in one
vibrating direction and a light component that vibrates in another
vibrating direction extending perpendicular to the one vibrating
direction for each of the two light fluxes emitted from the first
birefringent plate and a second birefringent plate having a
different thickness and a different refractive index from those of
the first birefringent plate, provided for spatially dividing each
of the two light fluxes emitted from the phase plate along a second
direction that is different from the first direction to achieve two
separate light fluxes to be guided to the imaging plane of the
imaging device, with the thickness t11 and the refractive index n11
of the first birefringent plate and the thickness t12 and the
refractive index n12 of the second birefringent plate satisfying
the following conditional equation, with A representing the image
height at the image plane corners, PO representing the air
equivalent optical path length extending from the imaging plane to
the exit pupil of the image forming lens and A/PO.gtoreq.0.15
satisfied. 5 ( 1 - cos cos 1 ) .times. t11 n11 + ( 1 - cos cos 3 )
.times. t12 n12 C2 ( 18 )
[0058] with 6 C2 = K .times. B .times. d .times. Fno - ( 1 - cos
cos 2 ) .times. t2 n2 ( 19 ) sin 1 = sin n11 ( 20 ) 1 = sin - 1 (
sin n 11 ) ( 21 ) 2 = sin - 1 ( n11 .times. sin 1 n2 ) ( 22 ) 3 =
sin - 1 ( n2 .times. sin 2 n12 ) ( 23 ) 0.25 K 0.35 ( 24 ) 1 B 3 (
25 )
[0059] t11: thickness of the first birefringent plate
[0060] t12: thickness of the second birefringent plate
[0061] n11: refractive index of the first birefringent plate
[0062] n12: refractive index of the second birefringent plate
[0063] t2: thickness of the phase plate
[0064] n2: refractive index of phase plate
[0065] d: pixel pitch at the imaging device
[0066] .phi.: Angle of incidence at a first birefringent plate of
light flux entering corner of the imaging plane of the imaging
device from the center of the exit pupil of the taking lens
[0067] Fno: F number of the taking lens
[0068] The present invention is further provided with a
neutralizing circuit for neutralizing electrical charges stored at
the first birefringent plate and the second birefringent plate.
[0069] In addition, the present invention is provided with a
neutralizing circuit for neutralizing at least one of the
electrical charges stored at the optical filter, the image forming
lens and the imaging device.
[0070] The present invention is provided with a photoelectric
conversion element for converting an optical image guided to a
photosensitive portion of the photoelectric conversion element to
an electrical signal, having a cover member covering the
photosensitive portion, a transparent electrode formed at a front
surface of the cover member and a conductive circuit electrically
connected with the transparent electrode and provided to neutralize
any electrical charge occurring at the photoelectric conversion
element caused by the operation of the electrical system.
[0071] Furthermore, the present invention is provided with a
photoelectric conversion element for converting an optical image
formed by an image forming lens to an electrical signal, an optical
member provided in an optical path between the image forming lens
and the photoelectric conversion element, a transparent electrode
provided, at least, at a surface of an optical member located in
the vicinity of the image forming plane of the image forming lens
and a conductive member electrically connected with the transparent
electrode and provided for neutralizing the electrical charge
occurring at the optical member.
[0072] The present invention may be further provided with a voltage
source that reduces the force with which matter adhering to the
photoelectric conversion element by applying a voltage to a
conductive member.
[0073] The present invention is further provided with a shutter
that can be switched between a light blocking state in which a
light flux entering the photoelectric conversion element is blocked
and an open state in which the light flux is allowed to pass, with
the conductive circuit provided to neutralize the electrical charge
occurring at the photoelectric conversion element as a result of a
shutter operation.
[0074] In addition, the present invention may be further provided
with a voltage source that reduces the force with which foreign
matter adheres to the optical member by applying a voltage to the
conductive member.
[0075] The present invention is further provided with a control
circuit that sustains the open state of the shutter and applies the
voltage to the optical member.
BRIEF DESCRIPTION OF THE DRAWINGS
[0076] FIG. 1 illustrates the structure of the optical filter
according to the present invention;
[0077] FIG. 2 is a schematic illustration of the structure and the
principle of the optical filter according to the present
invention;
[0078] FIG. 3 is a longitudinal sectional view illustrating an
example of the structure of a single lens reflex type digital still
camera provided with the optical filter according to the present
invention;
[0079] FIG. 4 illustrates the relationship between the thickness of
the optical filter and the pixel pitch at the imaging device;
[0080] FIG. 5 is a longitudinal sectional view illustrating another
example of the structure of a single lens reflex type digital still
camera provided with the optical filter according to the present
invention;
[0081] FIG. 6 presents a schematic structure of the optical filter
in an embodiment of the present invention, illustrating an example
of the combination of two birefringent plates having equal
thicknesses and refractive indices;
[0082] FIG. 7 illustrates focus misalignment caused by an optical
low-pass filter;
[0083] FIG. 8 illustrates the relationship between the angle of
incidence of a ray of light entering the optical low-pass filter
and the focus misalignment quantity;
[0084] FIG. 9 illustrates the relationship between the angle of
incidence of a ray of light entering the optical low-pass filter
and the focus misalignment quantity;
[0085] FIG. 10 illustrates a method for selecting the combination
of the refractive indices and the thicknesses of the birefringent
plates;
[0086] FIG. 11 illustrates another method for selecting the
combination of the refractive indices and the thicknesses of the
birefringent plates;
[0087] FIG. 12 illustrates yet another method for selecting the
combination of the refractive indices and the thicknesses of the
birefringent plates;
[0088] FIG. 13 presents a schematic structure of the optical
low-pass filter in an embodiment of the present invention,
illustrating an example of a combination of two birefringent plates
having equal refractive indices and different thicknesses;
[0089] FIG. 14 presents a schematic structure of the optical
low-pass filter in an embodiment of the present invention,
illustrating an example of a combination of two birefringent plates
having different thicknesses and refractive indices;
[0090] FIG. 15 illustrates an example in which the present
invention is adopted in a camera;
[0091] FIG. 16 is an enlargement of the area in which the optical
filter and the imaging device are provided in the camera;
[0092] FIGS. 17A-17D illustrate structural examples of the
conductive connection portions through which the electrical charge
stored at the optical filter is released;
[0093] FIG. 18 illustrates an essential portion of another example
in which the present invention is adopted in a camera;
[0094] FIG. 19 illustrates an essential portion of yet another
example in which the present invention is adopted in a camera;
[0095] FIG. 20 illustrates an example in which the present
invention is adopted in a camera having a relay lens system;
and
[0096] FIG. 21 illustrates an example in which the present
invention is adopted in an image reading device (image
scanner).
DESCRIPTION OF THE PREFERRED EMBODIMENTS
Advantage of Space Saving Achieved by Reducing the Total Thickness
of the Optical Filter
[0097] FIG. 1 is a perspective illustrating an example of the
optical filter according to the present invention. The optical
filter 1 in FIG. 1 comprises four main components, i.e., four
optical elements each formed in a plate shape, i.e., a first
birefringent plate 1a, an IR blocking filter 1b, a phase plate 1c
and a second birefringent plate 1d. The first birefringent plate 1a
and the second birefringent plate 1d are positioned by ensuring
that the direction in which an image shift occurs as a result of
the birefringence achieved by the first birefringent plate 1a and
the direction in which the image shift occurs as a result of the
birefringence achieved by the second birefringent plate 1d are
offset from each other by 90.degree.. The IR blocking filter 1b for
cutting off infrared light and the phase plate 1c for converting
linearly polarized light to circularly polarized light are provided
between the two birefringent plates 1a and 1d. The phase plate 1c
may be constituted of, for instance, a quarter-wave plate. It is
necessary that the phase plate 1c be provided between the two
birefringent plates 1a and 1d in this manner, and in addition,
since the IR blocking filter 1b turns milky when it comes in
contact with air, it is normally enclosed by substrates to ensure
that its surface does not come in contact with air. It is to be
noted that while the IR blocking filter 1b may be constituted by
vapor-depositing a multilayer film having an IR blocking effect on
the surface of a glass substrate, a multilayer film similar to that
mentioned above may be provided at a surface of the first
birefringent plate 1a or the second birefringent plate 1d, instead.
In this case, it is desirable that a protective layer be provided
to ensure that the multilayer film does not come in contact with
air. By providing a multilayer film at the surface of the first
birefringent plate 1a or the second birefringent plate 1d in this
manner, the total thickness of the optical filter 1 can be
reduced.
[0098] Next, in reference to FIG. 2, the functions achieved by the
optical filter 1 structured as illustrated in FIG. 1 are explained.
It is to be noted that in FIG. 2, the IR blocking filter 1b is not
shown to achieve simplicity in the explanation and that the first
birefringent plate 1a and the phase plate 1c, and the phase plate
1c and the second birefringent plate 1d are shown separate from
each other.
[0099] When a light ray L that has been transmitted through a
taking lens 20 enters the first birefringent plate 1a, it is
separated into linear light (an ordinary ray L10) that vibrates in
a direction perpendicular to the direction in which the light flux
advances and linear light (extraordinary ray L20) that vibrates
perpendicular to the ordinary ray L10). Since the first
birefringent plate 1a has different refractive indices for the
ordinary ray L10 and the extraordinary ray L20, the photographic
light ray L that becomes the ordinary ray L10 and the extraordinary
ray L20 after entering the birefringent plate 1a travel through two
separate optical paths, achieves a double image. In this structure,
with the direction in which the extraordinary ray L20 is shifted
relative to the ordinary ray L10 (the horizontal direction in the
figure) referred to as a first direction, the first birefringent
plate 1a can be considered to be an optical element that spatially
divides input light along the first direction extending
perpendicular to the direction in which the input light flux
advances to achieve two separate light fluxes. These two light
fluxes, i.e., the ordinary ray L10 and the extraordinary ray L20
are linear light fluxes achieving a light intensity ratio of 1:1
and having polarization planes intersecting each other
orthogonally, since the light ray L is natural light.
[0100] Next, the ordinary ray L10 and the extraordinary ray L20
enter the phase plate 1c. The phase plate 1c, which is provided to
convert linear light to circular light, converts the ordinary ray
L10 and the extraordinary ray L20 to circular ray L10' and circular
ray L20 ' respectively with their phases offset from each other by
90.degree.. Since a birefringent plate has an effect on circular
light that is similar to its effect on natural light under normal
circumstances, the circular ray L10' and the circular ray L20' that
have entered the second birefringent plate 1d are respectively
divided into an ordinary ray L11 and an extraordinary ray L12
having intensities equal to each other, and into an ordinary ray
L21 and an extraordinary ray L22 having intensities equal to each
other. The direction in which the extraordinary ray L12 is shifted
relative to the ordinary ray L11 and the direction in which the
extraordinary ray L22 is shifted relative to the ordinary ray L21
both constitute a second direction extending perpendicular to the
first direction discussed earlier (the vertical direction in the
figure).
[0101] Thus, the photographic light ray L that is originally a
single light flux is first separated into the ordinary ray L10 and
the extraordinary ray L20 at the first birefringent plate 1a, and
then after they are converted to circular light fluxes at the phase
plate 1c by changing the vibrational planes of the light fluxes,
they are separated into four light fluxes, i.e., the ordinary rays
L11 and L21 and the extraordinary rays L12 and L22 at the second
birefringent plate 1d. As a result, a quadruple image is formed on
an imaging plane 15a of an imaging device 15. Since the first and
second birefringent plate 1a and 1d are combined by assuring that
the directions in which images are shifted as a result of the
birefringence achieved by the two birefringent plates are offset
from each other by 90.degree. as explained earlier, the quadruple
image on the imaging plane 15a constitutes a near square shape with
the individual points achieving equal intensity. When the distance
between the individual points, which corresponds to the length of
one side of the square shape, is referred to as a separating
distance d, the separating distance d is calculated through the
following equation (26)
d=t(ne.sup.2-no.sup.2)/(2ne.times.no) (26)
[0102] with
[0103] t: birefringent plate thickness
[0104] ne: extraordinary ray refractive index
[0105] no: ordinary ray refractive index
[0106] The optical filter 1 according to the present invention is
constituted of the first birefringent plate 1a, the IR blocking
filter 1b, the phase plate 1c and the second birefringent plate 1d.
While the phase plate 1c is provided between the first birefringent
plate 1a and the second birefringent plate 1d in the structure, the
position of the IR blocking filter 16 may be set freely. In other
words, the IR blocking filter 1b may be provided between the first
birefringent plate 1a and the phase plate 1c, as illustrated in
FIG. 1, or it may be provided between the phase plate 1c and the
second birefringent plate 1d. Alternatively, the IR blocking filter
1b may be provided between a taking lens 20 and the first
birefringent plate 1a, or between the second birefringent plate 1d
and the imaging plane 15a.
[0107] Next, the materials that may be employed to constitute the
first birefringent plate 1a and the second birefringent plate 1d
constituting the optical filter 1 according to the present
invention are explained. Apart from quartz, lithium niobate
(LiNbO.sub.3) is a substance known as having a birefringent effect.
While lithium niobate is employed to constitute a surface acoustic
wave filter in communication devices by taking advantage of its
property whereby it becomes distorted when a voltage is applied and
is also employed to constitute a light guide for laser light by
taking advantage of its properties of having a high refractive
index and being transparent, there are almost no examples in which
its birefringent effect is utilized. However, LiNbO.sub.3, which
achieves a refractive index ne=2.2238 for extraordinary ray of
light having a wavelength of 550 nm and a refractive index
no=2.3132 for ordinary ray at a temperature of 25.degree. C. with a
larger difference between the extraordinary ray refractive index
and the ordinary ray refractive index compared to that of quartz
will realize a larger separating distance d compared to that of
quartz at the same thickness, when its property of causing
birefringence is utilized in an optical filter. For instance, in
order to achieve a separating distance d of 12 .mu.m, "t" is
calculated to be 0.3 mm using equation (26) and the values of the
refractive index ne and the refractive index no given above. This
amounts to only 15% of 2.04 mm required when quartz is used to
constitute the birefringent plates.
[0108] FIG. 3 illustrates an example in which the optical filter 1
having its birefringent plates constituted of LiNbO.sub.3 according
to the present invention is mounted in a single lens reflex type
digital still camera (DSC). It is to be noted that the figure shows
a longitudinal sectional view illustrating the structure of the
DSC.
[0109] In the DSC in FIG. 3, a mount 11 for mounting an
interchangeable taking lens 20 (see FIG. 3) is provided at its
front portion (on the left side in the figure). However, FIG. 3
illustrates a state in which the taking lens is removed. Subject
light L that has been transmitted through the taking lens 20 is
separated into transmitted ray L1 for autofocus (AF) and reflected
ray L2 for viewfinder monitoring by a semitransparent quick return
mirror 12. When the quick return mirror 12 is lowered, i.e., in a
viewfinder monitoring state, the transmitted ray L1 is reflected
downward in FIG. 3 by a sub mirror 13 provided as part of the quick
return mirror 12 to enter a TTL focus detection device 14 provided
at the bottom of the mirror box. The TTL focus detection device
receives the impinging light through the taking lens, and detects
the focal point of the taking lens. The reflected ray L2, on the
other hand, forms an image of the subject on a focal plane 21a of a
viewing screen 21 provided at a position that is conjugate with the
position of the plane of the imaging device 15 (to be detailed
later) and this image is enlarged by an ocular 23 via a penta-prism
22 to be monitored.
[0110] When a release button (not shown) is pressed, the quick
return mirror 12 is caused to swing upward around its pivot portion
12a together with the sub mirror 13, to recede to the position
indicated by the 2-point chain line 12' in the figure. This allows
the subject light L that has been transmitted through the taking
lens 20 to travel toward the imaging plane 15a (to be detailed
later).
[0111] An imaging device package 16 is provided at the rear portion
of the DSC (on the right side in the figure). The imaging device
package 16 is provided with the imaging device 15 and a seal glass
2 that covers the front of the imaging plane 15a of the imaging
device 15. The optical filter 1 according to the present invention
is provided in close proximity to the front surface of the seal
glass 2. The imaging device package 16 is held by a bracket 17. The
bracket 17 is secured to the camera main body 19 with screws 18.
The bracket 17 and the surface of the camera main body 19 at which
the bracket 17 is mounted are machined with a high degree of
accuracy so that the imaging plane 15a of the imaging device
package 16 is positioned with a high degree of optical
accuracy.
[0112] A shutter unit 3 is provided between the optical filter 1
and the quick return mirror 12 to block light during an imaging
signal read operation (signal brigade operation) at the imaging
device 15. FIG. 3 illustrates a state during a signal read
following exposure, with a light blocking screen 3a closed. The
shutter unit 3 is formed in such a manner that it opens its light
blocking screen 3a at a start of imaging device exposure to allow
the subject light L to reach the imaging plane 15a.
[0113] To explain the thickness of the optical filter 1 by
referring to FIG. 1 again, the total of the thicknesses of the four
plate-like optical elements 1a, 1b, 1c and 1d constituting the
optical filter 1 under normal circumstances will be 1.6-1.9 mm
since the thickness of both the first and second birefringent
plates 1a and 1d constituted of LiNbO.sub.3 is 0.3 mm, the
thickness of the phase plate 1c constituted of quartz or the like
is approximately 0.5 mm and the thickness of the IR blocking filter
1b is approximately 0.5-0.8 mm with the pixel pitch at the imaging
device 15 set at 12 .mu.m, for instance. Even when the total
thickness is at its largest at 1.9 mm, it only amounts to 35% of
the total thickness 5.38 mm of an optical filter having its first
and second birefringent plates 1a and 1b constituted of quartz, to
achieve a great advantage in space saving. In particular, since
only a limited degree of freedom in design is allowed in regard to
the position of the imaging device 15, whose imaging plane 15a must
be provided at the image forming plane of the taking lens 20 and,
as a result, the space available for providing the shutter unit 3
and the optical filter 1 becomes limited, the advantage of space
saving thus achieved in comparison with the space required when the
first birefringent plate 1a and the second birefringent plate 1d
are constituted of quartz is significant. Most single lens reflex
cameras in recent years are provided with an autofocus adjustment
mechanism, with the sub mirror 13 provided at the rear of the quick
return mirror 12. Thus, there is no large space between the rear
end of the sub mirror 13 and the shutter unit 3 or between the rear
surface of the shutter unit 3 and the lens image forming plane and,
as a result, it is extremely difficult to mount an optical filter
having a large thickness of 5.38 mm in a conventional silver halide
AF camera structure.
[0114] However, the optical filter 1 according to the present
invention described above, which saves space, can be mounted in
such a structure. Thus, while basically still utilizing the
conventional silver halide type single lens reflex camera
structure, a DSC employing an imaging device having a large image
plane with a pixel pitch exceeding 10 .mu.m can be realized.
[0115] It is to be noted that while LiNbO.sub.3 constituting the
first and second birefringent plates 1a and 1d in the present
invention has a cleaving property, this shortcoming can be
sufficiently compensated by bonding them together with the phase
plate 1c and the like to achieve an integrated unit.
[0116] In the optical filter 1 structured as described above, an
optical rotatory plate for rotating the plane of polarization of
light by 45.degree. may be employed in place of the phase plate 1c.
Examples in which an optical rotatory plate is used in an optical
filter in the prior art provided with birefringent plates
constituted of quartz include that disclosed in Japanese Examined
Patent Publication No. 1994-20316 mentioned earlier. According to
the present invention, advantages similar to those achieved when
the phase plate 1c explained earlier is employed can be realized by
adopting a structure in which such an optical rotatory plate is
used in combination with the first and second birefringent plates
1a and 1d constituted of LiNbO.sub.3. This allows for a greater
degree of freedom in regard to the structural features other than
the first and second birefringent plates 1a and 1d. Furthermore, it
goes without saying that an optical element other than the phase
plate 1c or the optical rotatory plate may be employed as long as
it provides an effect equivalent to that achieved by the phase
plate 1c and the optical rotatory plate.
[0117] FIG. 4 presents a graph illustrating the relationship
between the pixel pitch at the imaging device 15 and the thickness
of the optical filter 1 achieved in a structure having its first
and second birefringent plates constituted of quartz and that
achieved in a structure having its first and second birefringent
plates constituted of LiNbO.sub.3. With the thicknesses of the
members other than the birefringent plates 1a and 1d, i.e., the
thickness of the IR blocking filter 1b and the thickness of the
phase plate 1c set at 0.6 mm and 0.5 mm respectively and the
thickness of the birefringent plates 1a and 1d which is calculated
through equation (26) indicated as t, the thickness "t" of the
entire optical filter is 1.1+340 p (p: pixel pitch at the imaging
device) using quartz to constitute the birefringent plates whereas
the thickness "t" of the entire optical filter using LiNbO.sub.3 to
constitute the birefringent plates is 1.1+50.7 p. As the pixel
pitch "p" increases, the difference between their thicknesses (see
.DELTA.1 and .DELTA.2 in FIG. 4) clearly becomes larger. For
instance, .DELTA.1 is 1.16 mm with "p" at 4 .mu.m, .DELTA.2 is 4.63
mm with "p" at 16 .mu.m and, thus FIG. 4 demonstrates that the
larger the pixel pitch, the larger the space saving advantage
achieved by constituting the birefringent plates 1a and 1d with
LiNbO.sub.3.
[0118] It is to be noted that since the refractive index of
LiNbO.sub.3 greatly differs from those of quartz and the
BK7-equivalent glass constituting the IR blocking filter, internal
reflection tends to occur more readily at its boundary surfaces
compared to a structure achieved by pasting together crystal
plates. Since this internal reflection can be prevented by applying
an anti-reflection coating to the boundary surface, it is desirable
that an anti-reflection coating be applied at the boundary surfaces
where the plates are pasted together, as well as at the front
surface as in a regular optical filter.
[0119] While the explanation has been given thus far on an example
in which the optical filter 1 is provided to the rear of the
shutter unit 3, now an example in which the position of the optical
filter 1 is changed, is explained below in reference to FIG. 5. It
is to be noted that in FIG. 5, the same reference numbers are
assigned to members and the like with the same structural features
and functions as those illustrated in FIG. 3 to preclude the
necessity of a repeated explanation thereof.
[0120] As illustrated in FIG. 5, a thin optical filter 1 employing
LiNbO.sub.3 may be provided at the front surface of the quick
return mirror 12 in a single lens reflex type DSC. In this case,
while the optical filter 1 is still positioned within the optical
path (the photographic light flux L) of the taking lens achieving a
similar optical effect in a photographing state with the quick
return mirror raised (indicated by the 2-point chain line in the
figure), the optical filter 1 is present in both the viewfinder
monitoring optical path and the AF detection optical path in a
viewfinder monitoring state with the quick return mirror 12 lowered
(indicated by the solid line and the figure). This is, strictly
speaking, not desirable since the effect of the image separation at
the optical filter 1 affects the viewfinder image and the AF
detection accuracy. However, even when there is hardly any gap
between the shutter unit 3 and the imaging device 15 and the
optical filter cannot be positioned between the shutter unit 3 and
the imaging device 15 even with the space saving effect achieved
through the use of LiNbO.sub.3, the optical filter can be mounted
between a locus 12s at the front end of the quick return mirror 12
during its operation and a trailing end LB of the taking lens by
reducing the radius of the locus 12s at the front end of the quick
return mirror 12 compared to that in a single lens reflex type
camera using the 135-type photographic film. If the size of the
imaging device is smaller (e.g., the APS size) than the image plane
size of the 135-type photographic film, the size of the quick
return mirror 12 can be also reduced correspondingly compared to
the size of the quick return mirror in a camera that employs the
135-type photographic film. Thus, the space for accommodating the
thin optical filter 1 constituted by using LiNbO.sub.3 is assured
by the reduced radius of the locus 12s at the front end of the
quick return mirror 12.
[0121] While the explanation has been given thus far on an example
in which both the first and second birefringent plates 1a and 1d in
the optical filter 1 are constituted of LiNbO.sub.3, a
corresponding degree of space saving effect can be achieved by
forming one of the two birefringent plates 1a and 1b with
LiNbO.sub.3 and forming the other birefringent plate with, for
instance, quartz. In other words, the technical scope of the
present invention includes a structure achieved by constituting
only one of the two birefringent plates 1a and 1d with LiNbO.sub.3,
as well as a structure which is achieved by constituting both the
birefringent plates 1a and 1d with LiNbO.sub.3.
Improvement in the Optical Performance Achieved by Reducing the
Total Thickness of the Optical Filter
[0122] As explained above, by constituting at least either the
first or second birefringent plate 1a or 1d in the optical filter 1
with LiNbO.sub.3, the total thickness of the optical filter 1 can
be reduced. In addition to the advantage explained earlier, the
optical filter 1 according to the present invention achieves an
advantage of reducing the focus misalignment occurring in the
direction of the optical axis between the central area of the image
plane and the periphery of the image plane as explained below.
[0123] FIG. 6 schematically illustrates the structure in which the
optical filter 1 is provided between the taking lens 20 and the
imaging device 15 inside the single lens reflex type DSC
illustrated in FIG. 3 or FIG. 5. It is to be noted that the
illustration of the IR blocking filter 1b is omitted in FIG. 6. In
the optical filter 1 in FIG. 6, the thickness of the first
birefringent plate 1a and the thickness of the second birefringent
plate 1d are equal to each other at t1. The thickness of the phase
plate 1c is t2. In addition, the refractive index of the first
birefringent plate 1a and the second birefringent plate 1d is n1,
whereas the refractive index of the phase plate is n2. A CCD, a MOS
type image sensor or the like is employed to constitute the imaging
device 15.
[0124] Now, a general principle is discussed in regard to the total
thickness of an optical filter in reference to a comparison of an
optical filter used in combination with an imaging device having a
2/3" image area size and approximately 1.3 million pixels and an
optical filter used in combination with an imaging device having a
15.5 mm.times.22.8 mm image area size and approximately 2 million
pixels. Then, optical problems occurring as a result of an increase
in the thickness of the optical filter are explained.
[0125] At an imaging device having image plane size of
approximately {fraction (2/3)}" and approximately 1.3 million
pixels, the pixel pitch will be approximately 6.6 .mu.m. The
thickness "t" required to achieve a separating distance for the
image corresponding to this level of pixel pitch by using quartz,
the most common material, to constitute the birefringent plates is
calculated as follows. Quartz has the following refractive indices
for light having a wavelength of 589 nm.
[0126] ne=1.55336
[0127] no=1.54425
[0128] The thickness "t" for each birefringent plate is calculated
to be approximately 1.12 mm by performing the reverse calculation
using equation (26) with d set at 6.6 .mu.m. As already explained,
since the thickness of the phase plate needs to be approximately
0.5 mm regardless of what the separating distance is, the thickness
of the optical filter constituted by pasting together the three
plates in this case will be approximately 2.74 mm.
[0129] Now, an imaging device having an image area of approximately
15.5 mm.times.22.8 mm and having approximately 2 million pixels,
which is comparable to the C-type in the IX240 system will have a
pixel pitch of approximately 13.2 .mu.m. The thickness "t" required
for achieving a separating distance for the image corresponding to
the pixel pitch of 13.2 .mu.m when constituting the birefringent
plates with quartz, as in the example featuring the 2/3" imaging
device, is calculated to be "t"=2.25 mm by performing reverse
calculation using equation (26) with d set at 13.2 .mu.m. The total
thickness of the optical filter is calculated to be approximately 5
mm by adding the thickness of the two birefringent plates and the
thickness 0.5 mm of the phase plate, which shows an approximately
82% increase over the thickness of the optical filter having a
pixel pitch of 6.6 .mu.m. When the thickness 0.5 mm of the IR
blocking filter is added, the optical filter supporting the pixel
pitch of 13.2 .mu.m will have a large thickness of 5.5 mm adding
together the thicknesses of the four elements including that of the
IR blocking filter.
[0130] The reason for focus misalignment occurring in the direction
of the optical axis between the central area of the image plane and
the periphery of the image plane as the thickness of the optical
filter increases in this manner is explained in reference to FIG.
7.
[0131] For the purpose of simplifying the explanation, it is
assumed that an optical filter OF having a total thickness "t"
which is provided between the taking lens 20 and the imaging device
15 has a uniform refractive index n. By providing the optical
filter OF between the taking lens 20 and the imaging device 15, the
air equivalent optical path length between the lens 20 and the
imaging plane 15a of the imaging device 15 changes as expressed in
the following equation (27) relative to a structure with no optical
filter OF present 7 1 = t .times. ( 1 - 1 n ) ( 27 )
[0132] The change quantity .DELTA.1 in the air equivalent optical
path length expressed through equation (27) relates to a beam of
light advancing on the optical axis Ax of the taking lens 20 and is
achieved only when the light flux enters the optical filter OF
perpendicularly. The angle of incidence .phi. of the light flux
entering the filter OF after passing through the center "P" of the
exit pupil L of the lens 20 is at its largest when the light flux
SR enters an off-axis corner 15f of the imaging plane 15a of the
imaging device 15. With .theta.1 representing the refractive angle
of the light flux SR after it enters the optical filter OF and L1
representing the optical path length of the light flux SR within
the optical filter OF, the change quantity .DELTA.3 of the air
equivalent optical path length along the direction in which the
light flux SR advances is calculated through the following equation
(28). Then, based upon equation (28) the change quantity .DELTA.2
of the air equivalent optical path length in the direction of the
optical axis is calculated through the following equation (29). 8 3
= t cos - L1 n = t cos - t n .times. cos 1 = t .times. ( 1 cos - 1
n .times. cos 1 ) ( 28 ) 2 = 3 .times. cos = t .times. ( 1 - cos n
.times. cos 1 ) ( 29 )
[0133] Equation (27) and equation (29) indicate that a difference
.DELTA.2-.DELTA.1 as expressed through the following equation (30)
is formed in the change quantity of the air equivalent optical path
length between the light flux reaching the center 15c of the
imaging plane 15a of the imaging device 15 and the light flux
reaching the diagonal corner 15f. This difference causes a focus
misalignment occurring between the image plane center and the image
plane periphery, resulting in the image forming plane of the taking
lens 20 becoming non-planar. As a result, as the difference
.DELTA.2-.DELTA.1 increases, the quality of image at the periphery
of the image plane deteriorates. 9 2 - 1 = t n .times. ( 1 - cos
cos 1 ) ( 30 )
[0134] As equation (30) clearly indicates, since it can be assumed
that .theta..apprxeq..phi. even in the case of a light flux
entering a diagonal corner 35a of the image plane as long as the
angle of incidence of the light flux at the optical filter OF is
not excessively large, the difference .DELTA.2-.DELTA.1 can be
considered to be 0.
[0135] The following two conditions must be satisfied to ensure
that the angle of incidence at the optical filter OF of a light
flux entering a diagonal corner of an image plane does not become
excessively large. Specifically, the first condition is that the
distance (PO) between the exit pupil L of the taking lens 20 and
the imaging plane 15a is large. The second condition is that the
image area of the imaging device 15 be small, i.e., that the area
of the imaging plane 15a be small with a small distance "A"
achieved between the image plane center 15c and the diagonal corner
15f of the image plane.
[0136] Since interchangeable lenses used in a camera employing the
135-type photographic film can be often directly utilized in a
single lens reflex type DSC, the lenses utilized in such a DSC may
have a relatively short PO of approximately 50 mm. The difference
.DELTA.2-.DELTA.1 explained above manifesting when the imaging size
of the imaging device is, for instance, 24 mm.times.16 mm (aspect
ratio; 3:2) and the pixel pitch is 13.2 mm and a taking lens 20
with a PO of 50 mm is mounted, is now calculated.
[0137] When the thickness of the optical filter OF is assumed to be
5 mm (the pixel pitch at 3.2 .mu.m, includes the thickness 0.5 mm
of the phase plate) and "n"=1.54 (quartz), the image height at the
image plane is calculated to be 14.4 mm with the angle of incidence
.phi. at the optical filter OF at 16.1.degree.. Based upon the law
of refraction, .theta.1 is calculated to be 10.4.degree., and based
upon equation (30), the focus misalignment quantity
.DELTA.2-.DELTA.1 at the image plane center 15c and the diagonal
corner 15f of the image plane is calculated to be approximately 75
.mu.m.
[0138] When the results of the calculation performed above are
compared with those achieved by an optical filter employed in
combination with an imaging device in the 2/3" size (the image
height 5.6 mm at the corner, the pixel pitch at 6.6 .mu.m)
described earlier and a lens with PO set at 100 mm, .theta.1 is
calculated to be 2.1.degree. based upon the angle of incidence
.phi.=3.2.degree.. Since the pixel pitch of the {fraction (2/3)}"
size imaging device is 6.6 .mu.m and the thickness of the optical
filter OF (n=1.54) is calculated to be approximately 2.7 mm
(includes the thickness of the phase plate), the focus misalignment
quantity .DELTA.2-.DELTA.1 at the diagonal corner of the image
plane in this case is calculated to be approximately 1.6 .mu.m,
which is only 2% of 75 .mu.m.
[0139] Now, when discussing the depth of focus achieved by imaging
with an imaging device, the setting of the allowable diameter of
the circle of confusion which constitutes a premise for the
discussion, i.e., the setting of the allowable circle of confusion
diameter, is an issue to be addressed. There is a theory that the
allowable circle of confusion diameter should be set to
approximately 33 .mu.m (={fraction (1/30)}mm) with the 135-type (35
mm full size) photographic film. At the same time, while there are
various theories in regard to how the allowable circle of confusion
diameter should be set when imaging is performed with an imaging
device, they all fall within a range of 1 time to approximately 3
times the pixel pitch of the imaging device. In this discussion we
shall assume the allowable circle of confusion diameter is twice
the pixel pitch.
[0140] The depth of focus is calculated as the product of aperture
value setting at the taking lens and the allowable circle of
confusion diameter. Thus, the depth of focus achieved when the
aperture value setting at the taking lens is F2.8 and the pixel
pitch is 13.2 .mu.m is calculated to be 2.8.times.13.2
.mu.m.times.2=74 .mu.m. In addition, the depth of focus achieved
when the aperture value setting at the taking lens is F 2.8 and the
pixel pitch is 6.6 .mu.m is calculated to be 2.8.times.6.6
.mu.m.times.2=36 .mu.m. While a focus misalignment of 1.6 .mu.m
relative to the depth of focus of 36 .mu.m does not present any
problem whatsoever, a focus misalignment of 75 .mu.m relative to
the depth of focus of 74 .mu.m poses a serious problem. Even if the
focal point matches perfectly without any error at the center of
the image plane, the focus misalignment attributable to the
thickness of the optical filter OF already exceeds the depth of
focus at the corners of the image plane, and if we also take into
consideration error factors in regard to the focal point matching
at the center of the image plane (positioning adjustment accuracy
at the imaging plane, lens focusing error and the like), there will
be no room for allowance for error factors left for the image at
the corners of the image plane.
[0141] FIG. 8 presents a graph illustrating the relationship
between the angle of incidence of a light flux at an optical filter
and the focus misalignment quantity discussed above with the
thickness of the optical filter is as a parameter. In the graph in
FIG. 8, a curve 1 represents the change in the focus misalignment
quantity observed when a relatively thick optical filter employing
quartz birefringent plates is used to support an imaging device
having a pixel pitch of 13.2 .mu.m, whereas curve 2 represents
change in the focus misalignment quantity observed when a
relatively thin optical filter employing quartz birefringent plates
is used to support an imaging device having a pixel pitch of 6.6
.mu.m. Point "T" indicates the results achieved when PO=50 mm, the
pixel pitch is 13.2 .mu.m and the image height at the corner is
14.4 mm, whereas point "S" indicates the results achieved when
PO=100 mm, the pixel pitch is 6.6 .mu.m and the image height at the
corner is 5.6 mm.
[0142] When the imaging device having a pixel pitch of 6.6 .mu.m is
enlarged to achieve the dimensions 24 mm.times.16 mm, the focus
misalignment quantity at the corners of the image plane increase
diagonally upward to the right along the curve 2 from the point "s"
to reach the value indicated by point "S1" with the angle of
incidence at 16.1.degree.. However, in a larger imaging device, the
pixel pitch is also set larger in consideration of the comparative
merits achieved by an increase in the number of pixels relative to
the production yield and also in order to improve the sensitivity.
As a result, the thickness of the optical filter constituted by
using quartz must be increased in correspondence.
[0143] Due to this increase in the thickness of the optical filter,
the focus misalignment quantity further increases upward from the
point "S1" on the curve 2 until the focus misalignment quantity is
at the point "T" on the curve 1 in the case of the imaging device
having a pixel pitch of 13.2 .mu.m. The focus misalignment quantity
at the corners of the image plane increases markedly in an imaging
device having a large image area in this manner, since the increase
in the angle of incidence at the filter of light entering the
corners of the image plane at the filter and the increase in the
pixel pitch resulting in an increase in the filter thickness are
factors which together introduce a greater effect than any one of
them alone.
[0144] FIG. 9 presents a graph similar to that presented in FIG. 8.
In FIG. 9, a curve representing the change in the focus
misalignment quantity observed when an optical filter employing
quartz birefringent plates is used to support an imaging device
having a pixel pitch of 13.2 .mu.m and a curve representing the
change in focus misalignment quantity observed when an optical
filter employing quartz birefringent plates is used to support an
imaging device having a pixel pitch of 9 .mu.m are presented.
[0145] Now, let us assume that the allowable value for the focus
misalignment described above is 1/3of the depth of focus. When the
aperture value setting at the taking lens is at F 2.8, the depth of
focus is calculated as 2.8.times.pixel pitch.times.2. Using the
pixel pitch, the allowable value for the focus misalignment is
expressed as 2.8.times.pixel pitch.times.2.div.3=1.9.times.pixel
pitch. FIG. 9 indicates that the 1.9.times.pixel pitch focus
misalignment (25.1 .mu.m with a pixel pitch of 13.2 .mu.m and 17.1
.mu.m with a pixel pitch of 9 .mu.m) occurs when the angle of
incidence is approximately 9.5.degree.. It is indicated that since
TAN 9.degree.=0.158, a filter that takes into consideration the
focus misalignment occurring at the corners of the image plane when
there is a possible combination of "PO"0 and the image height at
the corner "A" that results in TAN .phi. exceeding TAN
.phi.=A/PO.gtoreq.0.15 must be achieved.
[0146] Now, an explanation is given in regard to how the focus
misalignment described above is reduced by employing the optical
filter 1 in the embodiment of the present invention, again in
reference to FIG. 6. As illustrated in FIG. 6, the light flux SR
travels through the center of the exit pupil L of the taking lens
20 to enter the corner 15f along the diagonal of the imaging plane
15a, and .theta.1 represents the refractive angle of the light flux
SR after it enters the first birefringent plate 1a (since the first
birefringent plate 1a and the second birefringent plate 1d have the
same refractive index, the refractive angle of the light flux SR
after it enters the second birefringent plate 1d, too, is referred
to as .theta.1). Likewise, the refractive angle of the light flux
SR after it enters the phase plate 1c is indicated as .theta.2. In
addition, n1 represents the refractive index of the first
birefringent plate 1a and the second birefringent plate 1d, and n2
represents the refractive index of the phase plate 1c.
[0147] Based upon equation (30), the individual focus misalignment
quantities at the corners of the image plain occurring as a result
of the light being transmitted through the first birefringent plate
1a, the phase plate 1c and the second birefringent plate 1d, are
calculated, with the focus misalignment quantities corresponding to
the birefringent plates 1a and 1d calculated by using the following
equation (31) and the focus misalignment quantity corresponding to
the phase plate 1c calculated by using the following equation (32)
respectively. The focus misalignment quantity .DELTA.a occurring at
the corners of the image plane attributable to the entire optical
filter 1 is the total of the individual focus misalignment
quantities, which may be calculated through the following equation
(33). 10 r = t1 n1 .times. ( 1 - cos cos 1 ) ( 31 ) 11 p = t2 n2
.times. ( 1 - cos cos 2 ) ( 32 )
.DELTA.a=2.times..DELTA..GAMMA.+.DELTA..rho. (33)
[0148]
[0149] The concept of the allowance for the focus misalignment
quantity at the corners of the image plane is explained again. At
the focus position at the center of the image plane (=on the lens
optical axis), there is almost always a focusing error (the range
finding error and the lens stop position accuracy error
attributable to autofocus, or focusing error in manual range
finding), and it is also difficult to achieve zero error for the
mechanical accuracy with respect to the image plane position of the
camera itself. Thus, these errors must be ultimately covered with
the depth of focus at the image plane (=product of the aperture
value setting at the taking lens and the allowable circle of
confusion diameter). As a result, the allowable value for the focus
misalignment quantity cannot be set equal to the depth of focus,
and it must be ensured that the allowable value for the focus
misalignment quantity must be set equal to or less than a factor K
(K<1) of the depth of focus. By taking into consideration the
deviation factor of the focusing accuracy described above at the
center of the image plane, a value that is approximately
1/4-1/3(0.25.ltoreq.K.ltoreq.0.35) of the depth of focus may be
regarded as reasonable.
[0150] At the same time, since there are various theories in regard
to the length of the allowable circle of confusion diameter
relative to the pixel pitch at the imaging plane of an imaging
device, all of which fall within the range of approximately 1-3
times the pixel pitch, as explained earlier, the allowable circle
of confusion diameter is expressed as B.times.d
(1.ltoreq.B.ltoreq.3, d: pixel pitch).
[0151] With Fno representing the aperture value setting at the
taking lens 20, the relationship described above is numerically
expressed through equation (34). 12 2 .times. t1 n1 .times. ( 1 -
cos cos 1 ) + t2 n2 .times. ( 1 - cos cos 2 ) K .times. B .times. d
.times. Fno ( 0.25 K 0.35 1 B 3 ) ( 34 )
[0152] By fixing the distance from the exit pupil L of the taking
lens 20 to the imaging plane 15a and the image area size of the
imaging device 15 at constant values and by constituting the phase
plate with a specific material to a specific thickness (e.g., using
quartz which is a common material for this application, to achieve
a thickness of approximately 0.5 mm), constants, i.e., n2=1.54,
.theta.2=10.4.degree. and t2=0.5, are achieved. In addition, since
.phi., too, achieves a constant value, the second term in the left
side member of equation (34) becomes a constant. Thus, .theta.1 can
be expressed as a function of n1 so that equation (34) is
re-expressed with the following equation (35). 13 t1 C .times. n1 Y
( n1 ) ( 35 )
[0153] with 14 Y ( n1 ) = 1 - cos cos 1 ( 36 ) C = 1 2 .times. { K
.times. B .times. d .times. Fno - ( 1 - cos cos 2 ) .times. t2 n2 }
= const . ( 37 ) sin 1 = sin n1 ( 38 ) 1 = sin - 1 ( sin n1 ) ( 39
) 2 = sin - 1 ( n1 .times. sin n2 ) ( 40 )
[0154] Now, let us consider a case in which the image height is
14.4 mm (a diagonal of 24 mm.times.16 mm), the air equivalent
optical path length from the image plane to the exit pupil of the
lens is 50 mm, K=0.3, B=3, d=12 .mu.m and Fno=2.8. Y(n1) and C are
calculated using the following equations (41) and (42) with the
angle of the incidence .phi. at the filter at 16.1.degree. and
.theta.2 at 10.4.degree.. 15 Y ( n1 ) = 1 - 0.9608 cos { sin - 1 (
0.2773 / n1 ) } ( 41 ) C=0.006318 (42)
[0155]
[0156] By rendering in a graph the relationship expressed in
equation (35) with these values incorporated, the horizontal axis
representing n1 and the vertical axis representing t1, a curve G in
FIG. 10 is achieved. The combination of t1 and n1 that satisfies
the inequality expressed in equation (35) is present in the range
that is lower than the curve G in FIG. 10. By making an appropriate
selection for the material to constitute the first birefringent
plate 1a and the second birefringent plate 1d to ensure that the
combination of the refractive index n1 and the thickness t1
described above is achieved, the focus misalignment quantity at the
corners of the image plane is set to be equal to or lower than a
specific value (the allowable value set by selecting the values for
B and K). For instance, let us consider a case in which quartz is
used to constitute the first birefringent plate 1a and the second
birefringent plate 1d. t1q representing the thickness achieved by
constituting the first birefringent plate 1a and the second
birefringent plate 1d of quartz is calculated to be t1q=2.04 mm by
performing reverse calculation using equation (26) with d=12 .mu.m.
Since the refractive index n1q of quartz is 1.54, the coordinates
(n1q, t1q) in the graph in FIG. 10 correspond to the position of
point Q, thereby demonstrating that the focus misalignment quantity
at the corners of the image plane is not set to be equal to or less
than the allowable value.
[0157] Now, let us consider a case in which lithium niobate
(LiNbO.sub.3), which is known as a material having a birefringent
effect comparable to that achieved by quartz, is used to constitute
the first birefringent plate 1a and the second birefringent plate
1d. The extraordinary ray refractive index ne and the ordinary ray
refractive index no of lithium niobate are ne=2.2238 and no=2.3132
(=n1b) respectively. t1b representing the thickness of the
birefringent plates 1a and 1d with lithium niobate is calculated to
be t1b=0.3 mm by incorporating d=12 .mu.m and the value of ne and
no above in equation (26).
[0158] The position of the coordinates (n1b, t1b) is indicated at
point NB in the graph in FIG. 10. The point NB is located in the
range lower than the curve G, demonstrating that the focus
misalignment easily stays within the allowable value.
[0159] Next, FIG. 11 presents a graph with K=0.25 and B=1.5
adopting more rigorous criteria for evaluation. By these criteria
for evaluation, the point NB achieved by using lithium niobate to
constitute the birefringent plates 1a and 1d is located in the
range above the curve G', and the focus misalignment quantity is no
longer equal to or less than the allowable value. It is understood
that in this case, a focus misalignment quantity equal to or less
than the allowable value is achieved by using Chilean nitrate
(NaNO.sub.3, ne=1.34, no=1.60) indicated by a point NA or rutile
(TiO.sub.2, ne=2.9, no=2.61) indicated by a point TI in FIG. 11 to
constitute the birefringent plates 1a and 1d.
[0160] The level of rigor for the evaluation criteria is set
depending upon the selected values for K and B, the F-number and
the position of the exit pupil of a taking lens that can be
mounted, and the required image distance over which focusing should
be assured. In a camera that does not allow lens exchange, the open
F-number of the lens is naturally selected for the F-number,
whereas in an interchangeable lens type camera, the open F-number
of the lens achieving the brightest open F-number among lenses that
may be mounted is selected for the F-number, under normal
circumstances. The same principle applies to the position of the
exit pupil. In addition, K and B are set within the setting ranges
explained earlier, in reference to the overall target performance
level and the like of the electronic camera in which the optical
filter is mounted.
[0161] For instance, if a lens having an open F-number of 1.4,
which is included among the lineup of interchangeable lenses that
can be used is expected to be used, it is naturally necessary to
set the target performance corresponding to this open F-number.
FIG. 12 presents the results of the evaluation (NB) obtained by
using lithium niobate to constitute the first birefringent plate 1a
and the second birefringent plate 1d with K=0.33, B=3 and
Fno=1.4.
[0162] The explanation has been given thus far on an example in
which the optical filter 1 according to the present invention is
employed in combination with an imaging device constituted through
a so-called square pixel array whereby the pixels at the imaging
device 15 are arrayed in the same array pitch in both the
longitudinal and the lateral directions. However, the imaging
device 15 is not necessarily required to assume a square pixel
array. If the imaging device 15 does not assume a square pixel
array, it is necessary to set different separating distances for
the image effected by the two birefringent plates 1a and 1d
corresponding to the array pitches in the longitudinal and lateral
directions. In such a case, a method whereby the two birefringent
plates having different thicknesses are constituted of the same
material, a method whereby the two birefringent plates are
constituted of materials having different refractive indices to
achieve the same thickness or a method whereby the two birefringent
plates are formed to have different thicknesses and different
refractive indices from each other, may be adopted.
[0163] FIG. 13 illustrates an example in which a single material is
used to constitute the two birefringent plates, formed to have
different thicknesses. In FIG. 13, with t11 and t12 respectively
representing the thicknesses of a first birefringent plate 1Aa and
a second birefringent plate 1Ad constituting an optical filter 1A
provided between the taking lens 20 and an imaging device 15A, a
conditional equation corresponding to equation (35) is presented as
the following equation (43). 16 t11 + t12 C1 .times. n1 Y ( n1 ) (
43 )
[0164] with 17 Y ( n1 ) = 1 - cos cos 1 ( 44 ) 18 C1 = K .times. B
.times. d .times. Fno - ( 1 - cos cos 2 ) .times. t2 n2 = const . (
45 ) 19 sin 1 = sin n1 ( 46 ) 20 1 = sin - 1 ( sin n1 ) ( 47 ) 21 2
= sin - 1 ( n1 .times. sin n2 ) ( 48 )
[0165] When the thicknesses of the two birefringent plates are
different, a graph corresponding to that in FIG. 10 is drawn in a
similar manner by using (n1, t11+t12) as a variable. The selected
birefringent material is evaluated at a point with the X coordinate
value represented by its refractive index n1 and the Y coordinate
value represented by the total (t11+t12) of the thicknesses t11 and
t12 determined by the required image separating distances.
[0166] An example constituted of two birefringent plates having
different thicknesses and different refractive indices is
illustrated in FIG. 14. With t11 and t12, and n11 and n12
respectively representing the thicknesses and the refractive
indices of a first birefringent plate 1Ba and a second birefringent
plate 1Bd constituting an optical filter 1B provided between the
taking lens 20 and the imaging device 15A in FIG. 14, a conditional
equation corresponding to equation (35) is presented as the
following equation (49). 22 ( 1 - cos cos 1 ) .times. t11 n11 + ( 1
- cos cos 3 ) .times. t12 n12 C2 ( 49 )
[0167] with 23 C2 = K .times. B .times. d .times. Fno - ( 1 - cos
cos 2 ) .times. t2 n2 = const . ( 50 ) sin 1 = sin n11 ( 51 ) 1 =
sin - 1 ( sin n11 ) ( 52 ) 2 = sin - 1 ( n11 .times. sin 1 n2 ) (
53 ) 3 = sin - 1 ( n2 .times. sin 2 n12 ) ( 54 )
[0168] While the explanation has been given in reference to the
embodiments above on an example in which the present invention is
adopted in an optical filter for a DSC, the present invention may
be adopted in other types of cameras provided with a solid-state
imaging device such as a video camera or in an optical apparatus
such as an image scanner or the like.
[0169] While the explanation has been given above with respect to
the advantage of reducing the degree of focus misalignment
occurring in the direction of the optical axis between the central
area of the image plane and the periphery of the image plane by
reducing the thickness of the optical filter in reference to an
example in which only the optical filter is provided between the
taking lens 20 and the imaging device 15, an infrared blocking
filter may be provided together with the optical filter. It is
obvious that the focus misalignment attributable to the thickness
of the infrared blocking filter must also be taken into
consideration in this case.
[0170] In addition, in the explanation given above, the first
birefringent plate 1a and the second birefringent plate 1d
constituting the optical filter 1 utilized in combination with the
imaging device 15 having the square pixel array illustrated in FIG.
6 have the same thickness t1 and the same refractive index n1.
However, the present invention is not restricted to this example.
Namely, the separating distance achieved when an incident light
flux is separated into two spatially separate light fluxes by one
birefringent plate is determined by the product of the thickness
and the refractive index of the birefringent plate and thus, two
birefringent plates having different thicknesses and refractive
indices may be adopted in combination in an imaging device having a
square pixel array. Furthermore, the relative angle of the
directions in which the light is separated by the first and second
birefringent plates is not restricted to 90.degree., and various
angles may be set including 30.degree., 45.degree., 60.degree. and
so forth, depending upon the separation pattern to be achieved.
Prevention of Shadows of Foreign Matter Cast onto Input Image
[0171] FIG. 15 schematically illustrates an essential portion of an
interchangeable lens type single lens reflex type DSC in which the
present invention is adopted (hereafter, an interchangeable lens
type single lens reflex DSC is simply referred to as a "camera"). A
taking lens 20 which can be exchanged to suit particular purposes
of photographing is mounted at a camera main body 70. Inside a
mirror box 72 of the camera main body 70, a mirror 12, a shutter
unit 3, an optical filter 1, an imaging device 15 and the like are
provided. A focusing screen 21 is provided above the mirror box
72.
[0172] The mirror 12 is automatically switched between a lowered
state i.e., the state indicated by the solid line in FIG. 15, and a
raised state, i.e., the state indicated by the 2-point chain line
in FIG. 15, in correspondence to the operating state of the camera.
The shutter unit 3 blocks light during an imaging signal read
operation at the imaging device 15 which is provided, together with
the optical filter 1, to the rear of the shutter unit 3. Since the
optical filter 1 assumes a structure identical to that illustrated
in FIG. 1, its explanation is omitted.
[0173] FIG. 16 is an enlargement of the area where the optical
filter 1 and the imaging device 15 are provided in the camera
illustrated in FIG. 15. Transparent electrodes 38A and 38B
constituted of a Nesa film or the like are respectively formed at
the entry surface and the exit surface of the optical filter 1. A
transparent electrode 38C constituted of a Nesa film or the like is
also formed at the front surface of a seal glass 2 provided at the
photosensitive surface of the imaging device 15. These transparent
electrodes 38A-38C are connected to a conductive area of a casing
37 via a conductive connection portion 36a or 36b as detailed
later.
[0174] The optical filter 1 and the casing 37, the conductive
connection portions between the transparent electrodes 38A and 38B
formed at the front surface of the optical filter 1 and the casing
37 are explained in reference to FIGS. 17A-17D, which illustrate
these components in partial enlargements. In FIG. 17A, a through
hole 34a is bored at the optical filter 1. A conductive pin 91 is
inserted through the through hole 34a, and the pin 91 and the
transparent electrodes 38A and 38B are bonded by using a conductive
adhesive 90 such as silver paste. This achieves an electrically
continuous state for the pin 91 and the transparent electrodes 38A
and 38B. One end of a wire 92 is soldered onto the pin 91, with
another end of the wire 92 soldered to the conductive area of the
casing 37. It is to be noted that the wire 92 and the conductive
area of the casing 37 may be connected with each other by attaching
a lug plate or the like (not shown) to the wire 92 through
soldering or crimping and securing the lug plate or the like to the
casing 37 through screwing. Thus, the transparent electrodes 38A
and 38B are connected to the conductive area of the casing 37 so
that their potentials are set equal to the potential at the
conductive area. As described above, a conductive connection
portion 36aA in the example illustrated in FIG. 17A is constituted
of the conductive adhesive 90, the pin 91 and the wire 92.
[0175] The conductive connection portion at which the transparent
electrodes 38A and 38B are connected with the conductive area of
the casing 37 may assume a structure illustrated in FIG. 17B or
FIG. 17C, instead, and the following is an explanation of these
structures. In FIG. 17B, conductive members 94A and 94B having a
spring property are secured at the conductive area of the casing 37
in a state that allows electrical continuity. A resilient restoring
force imparted by the conductive members 94A and 94B presses the
transparent electrode 38A in contact against the conductive member
94A and the transparent electrode 38B in contact against the
conductive member 94B respectively. Thus, the transparent
electrodes 38A and 38B are both connected to the conductive area of
the casing 37 with their potentials set equal to that at the
conductive area. In other words, in the example illustrated in FIG.
17B, a conductive connection portion 36aB is constituted of the
conductive members 94A and 94B.
[0176] In FIG. 17C, the optical filter 1 is held by a frame body 95
having a conductive property, and the transparent electrodes 38A
and 38B are in contact with the frame body 95 in a state that
allows electrical continuity. The frame body 95 is retained at a
fixing portion 37a formed at the conductive area of the casing 37
through tightening of screws 96. Thus, the transparent electrodes
38A and 38B are both connected to the conductive area of the casing
37 with their potentials set equal to that at the conductive area.
In other words, a conductive connection portion 36aC in the example
presented in FIG. 17C is constituted of the frame body 95, the
screws 96 and the fixing portion 37a.
[0177] Now, in reference to FIG. 17D, the conductive connection
portion 36b at which the transparent electrode 38C formed at the
front surface of the seal glass 2 of the imaging device 15 and the
conductive area of the casing 37 are connected is explained. A
conductive member 94C having a spring property is secured at the
bracket 17 holding the imaging device 15, with the conductive
member 94C placed in contact with the transparent electrode 38C.
One end of a wire 97 is soldered onto the conductive member 94C,
with another end of the wire 97 soldered onto the conductive area
of the casing 37. As in the conductive connection portion 36aA
illustrated in FIG. 17A, the wire 97 and the casing 37 may be
connected by attaching a lug plate (not shown) to the wire 97
through soldering or crimping and by retaining the lug plate or the
like at the casing 37 through screwing. As explained above, the
conductive connection portion 36b in the example illustrated in
FIG. 17D is constituted of the conductive member 94C and the wire
97.
[0178] In the camera structured as described above, the mirror 12
is in a lowered state as illustrated in FIG. 15 during a
photographing preparation operation, i.e., when the photographer is
engaged in an operation related to framing (monitoring of a
viewfinder image), adjustment of the exposure value, focal point
adjustment and the like. Thus, the image of the subject formed by
the taking lens 20 is reflected upward by the mirror 12 so that an
image can be formed on the focusing screen 21. The photographer
monitors the subject image formed on the focusing screen 21 via a
viewfinder lens system (not shown).
[0179] During a photographing operation, the mirror 12 swings
upward and subsequently, after the shutter unit 3 has been engaged
in an open/close operation, the mirror 12 is lowered. Through this
sequence of operations, the light from the subject guided by the
taking lens 20 is transmitted through the optical filter 1 to enter
the imaging device 15.
[0180] In the camera described above, the transparent electrodes
38A and 38B formed at the two surfaces of the optical filter 1 and
the transparent electrode 38C formed at the front surface of the
seal glass 2 at the imaging device 15 are all connected to the
conductive area of the casing 37 via the conductive connection
portion 36a and the conductive connection portion 36b respectively.
This prevents the optical filter 1 and the imaging device 15 from
becoming electrically charged. As a result, dust and lint are
prevented from becoming adhered to the optical filter 1 and the
seal glass 2 located near the focal plane of the taking lens 1.
[0181] Now, a discharge may occur in a camera in the prior art when
its optical filter becomes electrically charged and the difference
in the potential occurring between the optical filter and the
photoelectric conversion element increases to a certain degree.
When such a discharge occurs, noise may be superimposed on a signal
output by the photoelectric conversion element. In addition,
depending upon the extent of the discharge, the photoelectric
conversion element itself may even be destroyed. In contrast, since
the optical filter 1 and the imaging device 15 are connected with
each other with their potentials set equal to each other via the
conductive area of the casing 37 in the camera in this embodiment,
there is no difference in the potential, thereby eliminating the
problem described above.
[0182] In the explanation given above in reference to FIGS. 15, 16
and 17A-17D, the transparent electrodes 38A and 38B formed at the
two surfaces of the optical filter 1 and the transparent electrode
38C formed at the front surface of the seal glass 2 are both
connected to the conductive area of the casing 37 in a continuous
state. The camera that is to be explained next differs from this
structure in that the transparent electrodes 38A-38C are connected
with one another to achieve equal potentials and that a voltage
source is connected between the transparent electrodes 38A-38C and
the conductive area of casing 37. Thus, the explanation is now
given mainly on these differences. Since the other structural
features are identical to those illustrated in FIGS. 15, 16 and
17A-17D, their explanation is omitted.
[0183] FIG. 18 is an enlargement similar to that in FIG. 16, which
illustrates the portion of the camera where the optical filter 1
and the imaging device 15 are provided. In FIG. 16, the same
reference numbers are assigned to components identical to those
illustrated in FIGS. 16 and 17A-17D to preclude the necessity for
an explanation thereof. While the transparent electrodes 38A and
38B are connected to a terminal 50a of a voltage source 50 via a
conductive connection portion 36aA, the transparent electrode 38C
is connected to the terminal 50a of the voltage source 50 via a
conductive connection portion 36b. A terminal 50b of the voltage
source 50 is connected to the conductive area of the casing 37. It
is to be noted that while the voltage source 50 is illustrated as a
DC source for purposes of achieving maximum convenience in
illustration, with the side on which the terminal 50b is present
set to (+), the present invention is not restricted to this
example. Specifically, the potential resulting from an electrical
charge varies depending upon the material constituting the optical
filter 1, and it is desirable to adjust the polarity and the
voltage at the voltage source 50 to achieve the maximum effect in
preventing an electrical charge in correspondence to the specific
type of material used.
[0184] In addition, the voltage generated by the voltage source 50
may be an AC voltage instead of a DC voltage. If an AC voltage is
generated by the voltage source 50, its frequency should be set
within the range of approximately several kHz to twenty kHz.
[0185] By adopting the structure described above, the potential
generated by the voltage source 50 is applied to the transparent
electrodes 38A-38C relative to the casing 37 to inhibit any
electrical charge from occurring at the optical filter 1 and the
imaging device 15.
[0186] FIG. 19 is an enlargement similar to that in FIG. 16, which
illustrates the portion of the camera where the optical filter 1
and the imaging device 15 are provided. In FIG. 19, the same
reference numbers are assigned to components identical to those
illustrated in FIGS. 16 and 17A-17D to preclude the necessity for
an explanation thereof. In addition, since the structural features
other than that illustrated in FIG. 19 are similar to those
illustrated in FIG. 15, their explanation is omitted.
[0187] When the movable members such as a blade 3a and the like in
the shutter unit 3 are constituted of non-conductive materials,
static electricity may be generated by the movement of the movable
members to result in an electrical charge occurring at the shutter
unit 3 and the optical filter 1 provided near the shutter unit 3.
The structure illustrated in FIG. 19 achieves prevention of an
electrical charge from occurring at the shutter unit 3 and the
optical filter 1 during the operation of the shutter unit 3.
[0188] A base plate 3b of the shutter unit 3 is constituted of a
conductive material such as aluminum, brass or plastic containing a
carbon fiber. A lug plate (not shown), for instance, is connected
to one end of a wire 98 so that the wire 98 is screwed onto the
base plate 3b via the lug plate. Thus, the base plate 3b and the
wire 98 become electrically connected with each other. Another end
of the wire 98 is connected to a terminal 60a of a voltage source
60. While the transparent electrodes 38A and 38B are connected to a
terminal 60b of the voltage source 60 via a conductive connection
portion 36aA, the transparent electrode 38C is connected to the
terminal 60b of the voltage source 60 via a conductive connection
portion 36b. It is to be noted that as explained earlier in
reference to FIG. 18, selections are made in regard to the polarity
of the voltage source 60, whether a DC voltage or an AC voltage is
to be generated, the frequency of the voltage if an AC voltage is
generated and the voltage level, to achieve an optimal state for
preventing the shutter unit 3, the optical filter 1 and the imaging
device 15 from becoming electrically charged.
[0189] By adopting the structure described above, static
electricity is prevented from being generated during the operation
of the movable members in the shutter unit 3.
[0190] It is to be noted that while none of the shutter unit 3, the
optical filter 1 and the imaging device 15 is connected to the
conductive area of the casing 37 in FIG. 19, the terminal 60a or
60b of the voltage source 60 may be connected to the conductive
area of the casing 37. For instance, by connecting the terminal 60b
to the conductive area of the casing 37, static electricity that
may be generated at the optical filter 1 and the imaging device 15
can be suppressed without having to generate a voltage with the
voltage source 60.
[0191] Now, foreign matter tends to enter the mirror box 72 (see
FIG. 15) during a lens exchange or the like in a single lens reflex
type DSC which allows taking lens exchange. Thus, it is desirable
that the inside of the mirror box 72 be cleaned on a regular basis.
During such a cleaning process, foreign matter that has become
adhered to the optical filter 1 and the like may not be readily
removed even with air blown by using a blower or the like. However,
the camera explained above in reference to FIG. 19 facilitates the
cleaning process as explained below.
[0192] In FIG. 19, a taking lens detection unit 101 for detecting
whether or not the taking lens 20 (see FIG. 15) is attached, a
cleaning mode setting switch 102 for setting the cleaning mode for
the camera, a release switch 103, a mirror actuator 104 for moving
the mirror 12 (see FIG. 15) vertically by interlocking with the
photographing operation and a shutter actuator 105 for driving the
shutter unit 3 are connected to a CPU 100 that controls the camera
operation. This CPU 100 is further connected with the voltage
source 60.
[0193] The camera user removes the taking lens 20 from the camera
main body 70, sets the cleaning mode for the camera by operating
the cleaning mode setting switch 102 and turns on the release
switch 103. In response to this, the CPU 100 provides a control
signal to the mirror actuator 104 and the shutter actuator 105 to
set the member 12 in a raised state, i.e., the state indicated by
the 2-point chain line in FIG. 15 and to set the shutter unit 3 in
an open state. Next, the CPU 100 provides a control signal to the
voltage source 60 to cause the voltage source 60 to generate a
specific voltage. At this time, either an AC voltage or a DC
voltage may be generated by the voltage source 60. This neutralizes
electrical charges at the shutter unit 3, the optical filter 1 and
the imaging device 5 to reduce the force with which foreign matter
adheres to the optical filter 1 and the imaging device 15 (the
attractive force generated by static electricity).
[0194] In addition, the foreign matter that is adhering to the
optical filter 1, the imaging device 15 and the like may itself be
electrically charged. In such a case, the foreign matter may be
lifted off the optical filter 1 or the imaging device 15 by
generating an AC voltage with the voltage source 60 or by applying
a DC voltage having a polarity which will generate a repulsive
force against the adhering foreign matter. The foreign matter can
be removed with ease by the camera user with a blower or the like
to blow air into the inside of the mirror box 72 in the state in
which the voltage is being generated by the voltage source 60 as
described above. At this time, the foreign matter can be removed
even more effectively by employing an apparatus that electrically
charges the air blown out of the blower to generate an attractive
force to attract the foreign matter with the electrically charged
air blown out of the apparatus.
[0195] After the cleaning process is completed as described above,
the CPU 100 interlocks with the camera user operation in which the
release switch 103 is turned on again to transmit a control signal
to the voltage source 60, the mirror actuator 104 and the shutter
actuator 105. This stops the voltage generation at the voltage
source 60, closes the shutter unit 3 and lowers the mirror 12.
[0196] The cleaning mode described above may be also adopted in the
camera explained earlier in reference to FIG. 18. In addition,
while the source 50 in the camera explained in reference to FIG. 18
and the source 60 in the camera explained in reference to FIG. 19
are provided inside the cameras, these voltage sources 50 and 60
may be omitted to supply a voltage from an external source provided
outside the camera. In that case, the terminals 50a and 50b or the
terminals 60a and 60b should be set in a shorted state during
normal operation. Then, when the cleaning mode is set, a voltage is
applied by the external voltage source to the terminals 50a and 50b
or the terminals 60a and 60b. By adopting this structure, a more
compact, lighter and less costly camera is achieved with ease. At
the same time, the removal of foreign matter is facilitated.
[0197] While the explanation given above in reference to FIGS.
15-19 uses an example in which the present invention is adopted in
an interchangeable lens type DSC, the present invention may also be
adopted in a fixed taking lens type DSC. In addition, while the
explanation is given on an example of a direct image forming type
camera constituted by providing the optical filter 1 and the
imaging device 15 near the primary image forming plane of the
taking lens, the present invention may be adopted in a DSC provided
with a relay lens system as explained below in reference to FIG.
20.
[0198] FIG. 20 illustrates a schematic structure of an
interchangeable lens type DSC provided with a relay lens system
comprising a field lens 42 and a relay lens 45, with the same
reference numbers assigned to components identical to those in the
interchangeable lens type DSC illustrated in FIG. 15 so that the
explanation can be focused on the differences from the camera
illustrated in FIG. 15.
[0199] The following explanation is given in reference to an
assumed state, i.e. the photographing state in which the mirror 12
is as indicated by the 2-point chain line in FIG. 20 and the
shutter unit 3 is open. The field lens 42 is provided near the
primary image forming plane of the taking lens 20. Behind the field
lens 42, mirrors 43 and 44 for bending the optical path are
provided, and behind the mirror 44, the relay lens 45 is provided.
An image of the subject formed on the primary image forming plane
of the taking lens 20 is transmitted through the field lens 42, the
mirror 43, the mirror 44, the relay lens 45 and the optical filter
1 to become reformed on the photosensitive surface of the imaging
device 15 in a reduced size. In other words, the photosensitive
surface of the imaging device 15 constitutes the secondary image
forming plane of the taking lens 20. On an optical path "p"
indicated by the 1-point chain line in FIG. 20, a shadow will be
cast on the subject image formed on the photosensitive surface of
the photoelectric conversion element 15 even by foreign matter such
as dust and lint present near either the primary image forming
plane or the secondary image forming plane. In order to eliminate
this concern, it is desirable to provide transparent electrodes on
the front surface of the field lens 12 and on the exit surface of
the relay lens 15 and to connect the transparent electrodes to the
conductive area of the casing 37, the voltage source 50 (see FIG.
18) or the voltage source 60 (see FIG. 19).
[0200] While the explanation has been given above on an example of
application of the present invention in a camera, the present
invention may be adopted in other optical apparatuses. The
following is an explanation of an example in which the present
invention is adopted in an image input apparatus (image scanner)
given in reference to FIG. 21.
[0201] In FIG. 21, which illustrates a schematic structure of an
image input apparatus, an image input unit 250 comprises a mirror
162, an image forming lens 164, and imaging device 252, a housing
258 for housing these members and the like. At the imaging device
252, pixels are arrayed along a single column or over a plurality
of columns along the direction extending perpendicular to the page
on which FIG. 21 is printed. A ribbed belt (timing belt) 158 is
provided connecting between wheels 154 and 156. The image input
unit 250 is secured at the ribbed belt 158. The wheel 154 is driven
to rotate by a stepping motor 152 to drive the image input unit 250
in the horizontal direction relative to the page on which FIG. 21
is printed in a reciprocal movement. These components are housed in
a casing 172. A platen glass 166 is provided at an opening at the
top of the casing 172, and a document holder 168 which is capable
of covering the entire platen glass 166 is further provided.
[0202] A host computer (not shown) is connected to the image input
apparatus 150 structured as described above. In response to an
operation of the host computer by the operator after he sets a
document M to be read on the platen glass 166, the host computer
issues an image input command to the image input apparatus 150. In
response to this image input command, the image input apparatus 150
starts an image input of the document M and transfers the image
data to the host computer. In other words, an operation in which an
image of the document M formed by the image forming lens 164 is
linearly read by the imaging device 252 and then the image input
unit 250 is made to move in the horizontal direction relative to
the surface of the page on which FIG. 21 is printed at a specific
moving pitch is repeated to input a two-dimensional image of the
document M.
[0203] During this process, if foreign matter is adhering to the
front surface (document mounting surface) or the rear surface of
the platen glass 166, the exit surface of the image forming lens
164 or the photosensitive surface of the imaging device 252, the
shadow of the foreign matter will be transferred. In particular, if
foreign matter adheres to the exit surface of the image forming
lens 114 or the photosensitive surface of the imaging device 252, a
shadow will be cast constantly on the image input at specific
pixels of the imaging device 252 a line will be transferred onto
the input image resulting in a faulty picture.
[0204] To deal with this problem, a transparent electrode (not
shown) is formed at the rear surface of the platen glass 166 in the
image input apparatus illustrated in FIG. 21. This transparent
electrode is connected to an electrically conductive area of the
casing 172 via a conductive connection portion 170. Likewise, a
transparent electrode (not shown) formed at the exit surface of the
image forming lens 164 and a transparent electrode (not shown)
formed at the front surface of a seal glass 252a of the imaging
device 252 are respectively connected to the electrically
conductive area of the housing 258 via a conductive connection
portion 256 and a conductive connection portion 254. The structure
illustrated in FIG. 17B or FIG. 17C, for instance, may be adopted
in the conductive connection portions 170, 256 and 254.
[0205] The electrically conductive area of the housing 258 and the
electrically conductive area of the casing 172 are connected with
each other by a conductive member 260 which can be deformed freely,
such as a curled or slack flexible printed circuit board (FPC). As
a result, even when the image input unit 250 moves in the left and
right direction on the page on which FIG. 21 is printed, the
electrically continuous state can be maintained for the
electrically conductive area of the housing 258 and the
electrically conductive area of the casing 172. By adopting the
structure explained above, in which the platen glass 166, the exit
surface of the image forming lens 164 and the imaging device 252
are all connected with the casing 172 with their potentials set
equal to that of the casing 172, generation of static electricity
is suppressed. Thus, it becomes possible to prevent foreign matter
from adhering to the platen glass 166, the image forming lens 164
or the imaging device 252 to cast a shadow on the input image.
[0206] The present invention may be adopted in optical apparatuses
other than those in the examples explained above. For instance, it
may be adopted in an image input apparatus without an image forming
lens, which reads the document to be read by placing the imaging
device in close proximity to the document or an image input
apparatus that is provided with a light guide constituted in the
form of a fiber scope between the object of image input and the
imaging device.
* * * * *