U.S. patent number 3,637,931 [Application Number 04/881,463] was granted by the patent office on 1972-01-25 for optic relay for use in television.
This patent grant is currently assigned to U.S. Philips Corporation. Invention is credited to Jacques Donjon, Auguste Raymond Le Pape, Gerard Joseph Marcel Marie.
United States Patent |
3,637,931 |
Donjon , et al. |
January 25, 1972 |
OPTIC RELAY FOR USE IN TELEVISION
Abstract
An optical relay device with an insulating plate which is
ferroelectric below its Curie temperature. The plate is scanned by
an electron beam. The plane of polarization of light incident on
the plate is variably rotated in dependence upon the electric field
created by means of the interaction between the electron beam and a
signal voltage applied to the plate, due to the Pockels effect. The
temperature of the plate is stabilized in the proximity of its
Curie temperature. This stabilizing device uses a capacitor as a
temperature sensing element. The dielectric of the capacitor is
formed by a material having a Curie temperature differing from that
of the plate by between 1.degree. and 20.degree..
Inventors: |
Donjon; Jacques (Yerres,
FR), Le Pape; Auguste Raymond (Vitry Chatillon,
FR), Marie; Gerard Joseph Marcel (L'Hay les Roses,
FR) |
Assignee: |
U.S. Philips Corporation (New
York, NY)
|
Family
ID: |
27244923 |
Appl.
No.: |
04/881,463 |
Filed: |
December 2, 1969 |
Foreign Application Priority Data
|
|
|
|
|
Dec 20, 1968 [FR] |
|
|
179505 |
Dec 20, 1968 [FR] |
|
|
179504 |
Feb 5, 1969 [FR] |
|
|
690611 |
|
Current U.S.
Class: |
348/767; 359/262;
348/748; 348/768; 348/E5.14 |
Current CPC
Class: |
H04N
5/7425 (20130101); G02F 1/0525 (20130101); G02F
1/00 (20130101); G02F 1/05 (20130101) |
Current International
Class: |
G02F
1/01 (20060101); G02F 1/05 (20060101); G02F
1/00 (20060101); H04N 5/74 (20060101); H04n
005/38 () |
Field of
Search: |
;178/5.4BD,7.5D ;250/199
;350/150 |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Griffin; Robert L.
Assistant Examiner: Stout; Donald E.
Claims
What is claimed is:
1. An optical relay device, comprising a plate of electrically
insulating material positioned in an optical path between a
polarizer and an analyzer, said material consisting of an acid salt
which is ferroelectric below the Curie temperature thereof, said
material being enriched with deuterium whereby the Curie
temperature thereof is higher than in the absence of deuterium,
means for applying a variable electric field across the plate with
a direction parallel to the general direction of propogation of
light in said path whereby the plane of polarization of the light
is variably rotated in dependence upon said field, means for
generating an electron beam, means for scanning the electron beam
across a major face of said plate, an anode for collecting
secondary electrons released from said plate by said electron beam,
and a temperature control device for stabilizing the temperature of
the plate at a value differing at most 5.degree. from the Curie
temperature of the plate, said temperature device comprising a
capacitor as a temperature-determining element the capacity of
which varies as a function of the temperature, the dielectric of
the capacitor comprising a material having a Curie temperature
differing from that of the plate by between 1.degree. and
20.degree..
2. A device as claimed in claim 1, wherein said anode is a gridlike
anode between the major face of said plate and said scanning means,
said anode being disposed parallel to and within 1 mm. from said
surface, said device further comprising means for applying a
potential to said anode, a gridlike electrode disposed parallel to
said gridlike anode on the side of said scanning means and means
for applying a potential to said gridlike electrode having a
voltage higher than the potential applied to said anode.
3. A device as claimed in claim 1, wherein the dielectric of the
capacitor has a Curie temperature which is between 5.degree. and
20.degree. lower than the Curie temperature of the said plate.
4. A device as claimed in claim 1, wherein in that the dielectric
of the capacitor consists of the same acid salt as the said plate
but is enriched with a lower percentage of deuterium than the
material of the said plate.
5. A device as claimed in claim 2, wherein said gridlike electrode
comprises parallel wires stretched perpendicular to the lines of
the scanning.
6. A device as claimed in claim 5, wherein the gridlike electrode
has a wider pitch than said anode.
Description
The invention relates to a device having an optic relay,
particularly for use in television. The relay comprises a plate of
electrically insulating material consisting of an acid salt which
becomes ferroelectric below the Curie temperature thereof. The salt
is enriched with deuterium to increase the Curie temperature
thereof. The plate rotates the plane of polarization of light
transmitted by a polarizer in accordance with a variable electric
field which is applied by means of a control electrode, so that it
appears substantially parallel to the direction of propagation of
said light across the plate. An analyzer transmits a selected
component of the light originating from the plate. Means are
provided for scanning a surface of said plate by an electron beam.
An anode receives the secondary electrons produced by the electron
beam. A temperature control device for stabilizing the temperature
of the plate at a value in the proximity of the Curie temperature
of the plate is provided. The temperature control device comprising
as a temperature-determining element a capacity, the capacity of
which is measured as a measure of the temperature.
In the picture tube of a television receiver the electron beam
usually fulfills the following three fundamental functions:
A. the beam supplies the energy to be converted into light (the
light-transmitting power of the tube hence is always lower than the
power transferred by the beam).
B. The beam scans the surface of the picture;
C. The beam transmits the video information.
With respect to functions (b) and (c), the power of the beam and
hence the brightness of the picture cannot be increased to such an
extent as would be necessary for projection on a large screen.
It has therefore been suggested to separate these functions and to
have the function (a) fulfilled, for example, by an arc lamp and
the functions (b) and (c) by a so-called "optic relay." Various
types of such relays have been designed. The most frequently used
relay(Eidophore) is heavy, bulky and hard to actuate. Another relay
has been proposed by Rissmann and Vosahlo ("Untersuchungen zur
Lichtsteuerung und Bildschriebung mit Hilfe elektrooptischer
Einkristalle," Jenar Jahrbuch 1960, first volume p. 228). In this
case a crystal is used which has an electro-optic effect, the
so-called "Pockels" effect. A crystal of KH.sub.2 PO.sub.4 has
proved suitable. This material will hereinafter be referred to as
KDP.
In so far as necessary, this effect can briefly be explained as
follows: when the electrically insulating crystal is exposed to an
electric field parallel to its crystal axis c (the three crystal
axes a, b and c constitute a trihedron of three rectangles; in this
case the axis c forms the optical axis) the index of refraction of
this crystal for light rays in the c-direction with linear
polarization in the plane ab depends upon the direction of
polarization. If X and Y denote the bisectors of the axes a and b,
and if the parameters of the crystal with respect to these various
directions are represented by the letters denoted for these
directions, it can be said that the diagram of the indices in the
plane ab becomes an ellipse with the axes X and Y instead of a
circle and that the difference nx-ny is proportional to the applied
electric field. From this it follows that if the incident light
rays are polarized parallel to the axis a, the intensity of the
light I which traverses an output polarizer is I=I.sub.o sin.sup. 2
kV if the direction of polarization of this polarizer is parallel
to the axis b, and is I=I.sub.o cos.sup.2 kV if the said direction
is parallel to the axis a, while I.sub.o is equal to the incident
light intensity, if no parasitic absorption occurs, wherein V is
the electric potential difference between the two faces of the
crystal and K is a coefficient which depends upon the crystalline
material used.
For the last-mentioned optic relay a thin monocrystalline plate of
KDP is used the thickness of which extends parallel to the axis c,
said plate being provided between two polarizers. In order to
obtain a projected picture by means of a lamp with this device, it
is sufficient, as described above, to apply an electric field
parallel to the axis c and to cause the value of the field to
correspond at any point with the brightness of the corresponding
point of the picture to be obtained. For this purpose, an electron
beam from an electron gun is caused to scan the plate by means of
conventional deflection members so that the beam fulfills the
function b. The function c, here the control of the electric field,
is likewise fulfilled by the beam and that in the following manner.
The electrons of the beam which are incident on the surface of the
plate produce secondary electrons but with a secondary emission
coefficient smaller than 1. As a result of this, negative charges
are formed at the points of the insulating plate on which the beam
was incident, which charges vary the electric field perpendicular
to the plate at the relative points. The charges thus produced
depend upon the accelerating voltage of the electron beam and in
particular on the anode voltage and the quantity of electricity
supplied by the beam. This quantity is the product of the beam
intensity and the duration of the passage of the beam over the
relative point of the plate. The term "point" in this case has the
meaning of an elementary plane. The video signal can previously be
used for the modulation of one of these four quantities. In the
relay described, either the anode voltage or the beam intensity can
be modulated but only the latter possibility is found to be
realizable. This possibility, however, has also several drawbacks.
For example, the negative charge produced on the plate is not a
linear function of the beam intensity: a further important drawback
is that it is necessary for the variation of the picture that said
charge is dissipated at least partly between two successive
pictures. This dissipation involves flicker of the picture seen by
the spectator the effect of which usually is reduced only by a
complication of the scanning system (interlacing). The dissipation
furthermore has for its result that the transparency is always low.
When a KDP crystal is used, it is necessary in order to dissipate
the charges within less than one-tenth of a second to operate at
the ambient temperature which involves important variations of the
potential of the screen of a few kV., as a result of which the
focusing of the electron beam is seriously hampered.
It is already known to avoid the said drawbacks by a device of the
type mentioned in the first paragraph. This device is described in
U.S. Pat. No. 3,520,589, the contents of which are herein
incorporated by reference. In the target plate described in this
application to be scanned by the electron beam and showing the
Pockels effect, a temperature is used in the proximity of the Curie
temperature thereof. This is possible in that the target plate
consists of a salt of the KDP type, for example, a double acid
phosphate or arsenate of potassium, rubidium or caesium which is
enriched with deuterium, as a result of which enrichment the Curie
temperature is considerably increased. The dielectric constant
.epsilon. reaches a very high value, so that, in order to obtain an
adequate modulation of the light, small control voltages (V) can be
applied across the target plate by means of a control electrode,
since the Pockels effect is proportional to the product .epsilon.
V. It has been proposed to control the temperature by means of a
temperature control device which comprises as a
temperature-determining element a capacitor the capacitance of
which is measured as a measure of the temperature, the dielectric
of said capacitor being formed by a plate cut out of the same
material as the said target plate. This has the advantage that the
measured capacity is proportional to the dielectric constant of the
crystal and hence proportional to the electro-optic sensitivity
which is to be stabilized. However, it is difficult to approach the
optimum operating temperature, since the optimum operating
temperature lies at the temperature at which the dielectric
constant of the target plate and hence also of the capacitor has a
maximum.
It is the object of the invention to avoid this drawback and to
provide a device which comprises an efficaceous control device
which is simple of construction and with which the optimum
operating temperature can also be adjusted.
According to the invention, in a device of the type mentioned in
the first paragraph the dielectric of the capacitor is formed by a
material the Curie temperature of which differs from that of the
said plate by a few degrees. Thus the capacity of the capacitor
varies uniformly in the proximity of the optimum operating
temperature. The dielectric of the capacitor preferably has a Curie
temperature which is lower than the Curie temperature of the target
plate between 5.degree. and 20.degree.. The capacity of the
capacitor varies in a particularly suitable manner as a function of
the temperature in the neighborhood of the optimum operating
temperature and that in such manner that the capacity is always
increasing, when the temperature is decreasing, and the control
device can be very simple. The device is of particular advantage
if, according to a further aspect of the invention, it has the
particular characteristic that the dielectric consists of the same
acid salt as the said plate but is enriched with a lower percentage
of deuterium than the material of the plate. The plate may consist,
for example, of a double-acid phosphate or arsenate of potassium,
rubidium or caesium enriched with 80 to 100 percent deuterium and
the dielectric of the capacitor may consist of the salt of the same
chemical composition enriched with from 5 to 20 percent less
deuterium.
In order that the invention may be readily carried into effect,
embodiment of the device according to the invention will now be
described in greater detail, by way of example, with reference to
FIGS. 1 to 13 of the accompanying drawings. Corresponding
components are referred to by the same reference numerals in the
various Figures.
FIG. 1 is a diagrammatic representation, partly in a perspective
view and partly as a block diagram, of a known part of an
embodiment in which the light traverses the target plate only
once.
FIG. 2 shows a known part of an embodiment in which the light is
reflected at a surface of the target plate.
FIG. 3 shows a known modification of a part of the device shown in
FIG. 2.
FIG. 4 is the cross-sectional view of the known vacuum tube shown
in FIG. 2.
FIG. 5 is a diagrammatic cross-sectional view of the screen of the
tube shown in FIG. 4.
FIGS. 6 and 7 show a front elevation of two elements of the tube
shown in FIG. 4.
FIG. 8 is a block diagram of an embodiment of the thermal control
device in a device according to the invention.
FIGS. 9 and 10 show modifications of the embodiment shown in FIG.
2,
FIG. 11 shows the beam separation polarization device shown in FIG.
10,
FIGS. 12 and 13 show modifications of parts of FIGS. 9 and 10.
FIG. 1 diagrammatically shows members of an optic relay and the
members which cooperate with said relay so as to obtain a visible
picture on a screen 2 via a projection lens 4. The light is
supplied by a lamp 6 shown in the drawing as a filament lamp; of
course, any other type may be used. The light passes a collimator
lens 8, then a space 10 which serves for suppressing the infrared
thermal rays. The optic relay is mainly constituted by a plate 12,
consisting of a parallelepiped-shaped monocrystal of KDP which
contains approximately 95 percent deuterium ions calculated on the
H-ions; this crystal the optical axis (c) of which is perpendicular
to the major planes is arranged between the two crossed polarizers
14 and 16 the planes of polarization of which are parallel to the
two other crystal axes (a and b) of the monocrystal. According to
the invention, the plate 12 is kept substantially at the value of
the Curie temperature (approximately -55.degree. C.) by means of
the temperature control device to be described below with reference
to FIG. 8. Of this control device, FIG. 1 shows only the known
thermal control 18. On the left-hand surface of the plate 12 in
FIG. 1, an electron beam impinges which is denoted by a broken line
and originates from an electron gun 20. This beam periodically
scans the whole effective surface of the plate 12 by means of
deflection means 22 which is controlled by scanning signals of a
receiver 24 which receiver receives the synchronization signals at
the input 26 with the actual video signal. A block 28 supplies the
required direct voltage for a few of the said members, as well as
to an anode 30. For the sake of clarity the anode is denoted by a
plate parallel to the light beam; it will be obvious that this
arrangement is very favorable for passing the light but not for
receiving the secondary electrons originating from all points of
the plate 12 on which the electron beam impinges. Therefore, in
practice the anode is provided parallel to the surface of the plate
12 and in the immediate proximity thereof. Since the incident
electron beam and the light beam have to traverse the anode, the
anode is constructed, for example, in the form of a grid.
FIG. 1 furthermore shows a thin plate 32 which is electrically
conductive and optically transparent and which in practice is
formed by a thin metal layer (gold, silver, chromium) and which is
surrounded by one or more metal oxide layers (SiO, SiO.sub.2,
Bi.sub.2 O.sub.3, Ag.sub.2 O) so as to improve the adherence.
Between this thin metal layer and the anode, the video information
signal is applied. It is possible to fix the potential of the layer
at a particular value, and to supply the information signal to the
anode, but in the example described the conductive transparent
layer receives the signal so that said layer constitutes a control
electrode.
The mechanism of this control may be described as follows.
When the electrons of the electron beam reach the surface of the
plate, they produce, if the energy lies within the desirable limits
and if the anode potential is sufficiently high, secondary
electrons the number of which is larger than that of the incident
electrons. As a result of this the potential of the point of
incidence is increased so that the potential difference between the
anode and the point of incidence becomes smaller. If the electrons
of the beam are incident on said point in a sufficient number, the
said potential difference becomes negative and reaches such a value
(-3V, for example) that every incident electron produces only one
single secondary electron. The potential of the point thus reaches
a limit value with respect to the anode potential. Dependent upon
the scanning rate, the intensity of the beam must for that purpose
be chosen to be sufficiently high. If the potential of the relative
point would initially not have been lower but higher than the said
limit value, the secondary emission would not have compensated for
the charges produced by the beam, so that said potential would have
gradually reduced to the said value.
The control electrode will now be considered; if the anode
potential is constant, every passage of the electron beam, as
described above, fixes the potential of an arbitrary point A of the
surface at a value V.sub.o independent of the point of incidence
and of the instant of passage. The corresponding electric charge at
the relative point, however, depends upon the potential of the
control electrode which is provided in the proximity of the other
surface of the plate. It is sufficient to consider the "capacitor"
the dielectric of which is formed by the said plate and the
electrodes by the control electrode and the element of the surface
of incidence around the point A to see that, if V.sub.A denotes the
potential of said electrode at the instant of passage, the charge
is proportional to V.sub.o -V.sub.a. Since the charge occurs on an
electrically insulating surface, this remains constant till the
next passage of the beam over the same point A as well as the
potential difference V.sub.o -V.sub.A between the two surfaces of
the plate at the relative point and the relative electric field
which is perpendicular to the plate and the control electrode. The
electric field which controls the passage of the light through the
plate at the point A hence is in itself constant between two
passages of the beam and during said passages is controlled by the
video information signals. This also holds good for a further point
B where the fixed potential difference when the beam passes is
V.sub.o -V.sub.B, V.sub.B being the value of the video information
signal at the instant of passage.
The constancy of the electric field between two successive passages
of the beam prevents flicker of the picture in such manner that, if
the picture to be reproduced is developed only very slowly, only a
few pictures per minute need be transmitted.
The above described device (FIG. 1) hence operates as follows: the
electron beam scans the plate 12; the resulting charge occurring at
every point of plate 12 depends upon the signal voltage applied to
the thin plate 32 at the moment when the electron beam passes that
point; in this way an image of electric field strengths is formed
on the plate 12, the electric field being directed perpendicular to
the plate 12. According to the Pockels effect the plane of
polarization of light incident on the plate 12 is variably rotated
in dependence upon said field. As a result of the crossed
polarizers 14 and 16 on either side of the plate 12, the amount of
light reaching a point of the screen 2 is dependent on the electric
field strength of the corresponding point of the plate 12, and in
this way an image is projected on screen 2 by the projection lens
4, corresponding with the image of electric field strengths on
plate 12. In consequence of the rotation of the plane of
polarization the amplitude of the light waves passing the polarizer
16 and projected on a point of the screen 2 is proportional with
the sin of the electric field strength of the corresponding point
of the plate 12, thus sin kV if V is the potential over the plate
and k is a constant. The light intensity is the square of this
amplitude and thus sin.sup.2 kV.
For clearness' sake the plate 12 in the Figure is shown
perpendicular to the light beam, only the electron beam is incident
at an acute angle. In practice, it may be preferable, as a result
of the presence of the grid in front of the screen which serves as
an anode 30, to use a minimum inclination of the beam in the axis
of the beam so that both beams are at an angle. It is found,
however, that the KDP crystal causes a phase shift as a result of
its double refraction when a light beam passes through it which
encloses a given angle with its optical axis c.
This phase shift is compensated by providing a crystal plate (not
shown) between the polarizer, 14 and 16, the optical axis of which
plate is parallel to that of the plate 12 and which shows a double
refraction of opposite signs.
In FIG. 2 the target plate (not shown) which rotates the plane of
polarization of the light and at the surface of which the light is
reflected, forms part of the screen 266 shown in the vacuum tube
50. The incident light originates from an arc lamp 6, A capacitor C
projects the picture of the arc on a small mirror (here a totally
reflecting prism R), which mirror is placed in the focus of an
optic system L having a focal distance f (for example, a doublet to
reduce the aberration and the chromatism). As a result of the small
dimensions of the picture of the source 6, the rays originating
from the optic system L and incident in the tube 50 are
substantially parallel. The normal to the screen 66 is slightly
inclined to the axis of the beam (approximately 1.degree.) so that
the reflected beam is focused on a plane near the mirror R prior to
the beam impinging upon the screen 2. The reciprocating paths can
be varied by using the mirror R for the projection on the screen 2.
The optic system L operates as a projection objective. The
adjustment is carried out by controlling the distance p between L
and the screen 266; in this case 1/ p' +1/ p must be equal to 1/ f,
where p' is the distance between the objective L and the screen 2.
In FIG. 2 the position is shown of the crossed polarizers P.sub.1
and P.sub.2 of the polaroid type, which are arranged in the forward
and return path, respectively.
In a known modification of this arrangement a beam separation
polarization device is used. This polarizer may comprise several
dielectric layers or be derived from the Glazebrook prism of spar
as is shown in FIG. 3. This polarizer or prism replaces the mirror
R of FIG. 2 and in this case the polaroids P.sub.1 and P.sub.2 may
be omitted. This has the advantage that overlapping forward and
return beams can be used as a result of which the angle between the
light beam and the screen of the tube 50 approaches 90.degree. even
more accurately. The electric field of the light beam has a
direction denoted by 267 on the left-hand side of the prism R in
FIG. 3 and denoted by 268 on the right-hand side of the prism
R.
The vacuum tube 50 of FIG. 2 can be constructed as shown in FIGS. 4
and 5 to which reference is now made. The target plate shown in
FIGS. 4 and 5 is of the same type as that of FIGS. 1 and according
to the invention is kept at the value of the Curie temperature by
means of the temperature control device to be described hereinafter
with reference to FIG. 8. The reference numerals 18 and 81 in FIG.
4 denote a known part hereof. The light denoted by the arrows 40
(FIG. 4) which impinges upon the plate 12 substantially
perpendicularly, is reflected on the rear surface of the plate by a
mirror 42 (FIG. 5) which is electrically nonconductive. This mirror
could be formed by a metal layer vapor deposited in a vacuum
through the grid 30; in the example shown, the mirror has a
multiple dielectric and is formed by seven layers alternately of
zinc sulphide and cryolite; the thickness of each layer is equal to
one-fourth wavelength of the light. In order to increase the
secondary emission coefficient a cryolite layer 44 with double
thickness is added. The rear surface of the plate 12 receives the
electron beam supplied by the gun 20. This beam is accelerated by a
voltage of 2,000 volt between the cathode 202 with the filament 204
and the electrode 206. The beam passes a gridlike electrode 30a and
the gridlike anode 30 before reaching the plate 12. The gridlike
anode 30 receives secondary electrons from the plate 12. Secondary
electrons not intercepted by the anode 30 are intercepted by the
gridlike electrode 30a having an appropriate potential. The beam is
then deflected magnetically by the four coils 22 after focusing by
means of the coil 46, so that in the case of an intensity of 26
.mu.a. the current density at the level of the layer 44 is
1A/sq.cm. In this manner a scanning of 600.times.800 discrete
points on a surface area of the plate 12 of 27 mm. .times. 36 mm.
is obtained.
The layer 44, the mirror 42 and the various other layers are
provided one after the other.
As a result of the use of the mirror 42, various advantages are
obtained with respect to the device shown in FIG. 1.
As a result of the use of the mirror 42 the light has to traverse
the plate 12 two times, as a result of which with a given thickness
of the plate and a given electric voltage the resulting phase shift
is doubled. The analysis by the electron beam is also facilitated
when said beam is incident perpendicularly. Moreover the light does
not traverse the anode 30, so that a better permeability is
obtained.
FIG. 5 shows on the right-hand side the anode 30 formed by a grid
and covered with a receiving member for the secondary electrons
originating from the layer 44, under the action of the incident
electrons of the beam transmitted by the gun 20. The receiving grid
consists of copper. The pitch is 50.mu. and the thickness is
approximately 10 .mu.. The diameter of the apertures is
approximately 45 .mu. so that the permeability for the incident
electrons lies between 60 and 70 percent. This grid is stretched on
an annular support 52 (FIG. 4) consisting of a copper-nickel alloy
having a coefficient of expansion which is approximately equal to
that of copper. This support has an effective circular passage of
40 mm. diameter and comprises a narrowed portion 54 in which a
copper-nickel ring can be accommodated. In order to secure the grid
to the support, the ring is forced into the narrow portion 54 while
the grid is taken along, after which the ring and the support are
secured together by spot-welds. After mounting the grid is
thermally hardened so as to obtain a suitable mechanical stress of
the grid.
The support 52 of the grid 30 comprises a gap 56 for passing the
connection wire 58 of the control grid 32 and six holes as denoted
by 60. The support is secured by screws 62 on a tray 64; both
components are applied to earth potential. The depth of the tray is
equal to the thickness of a disc 66, the function of which will be
described below. The disc has a thickness of 8 mm. and a diameter
of 5 cm. In order to maintain the space of 50 .mu. chosen between
the grid 30 and the layer 44, mica spacing members (not shown) are
provided between the support 52 and the tray 64. In front of the
plate 12 is arranged the control electrode 32 which must have a
sufficient thickness to have a low resistance per square which in
this case is lower than 500 ohm, (the resistance per square is
measured between two parallel sides of a square with the layer).
However, the electrode must be thin so as to obtain a good
transparency. In the example described, the electrode is formed by
a metal layer (gold, silver, chromium) coated with one or more
metal oxide layers 321 and 322 to improve the adherence (SiO,
SiO.sub.2, Bi.sub.2 O.sub.3, Ag.sub.2 O, for example).
Reference is now made to FIG. 6 and FIG. 7.
The sensitive layer 12 has substantially the shape of a rectangle
of 3.times.4 cm. (FIG. 6). An aluminum layer 70 which leaves an
effective aperture of 27 mm..times. 36 mm. and which enables a good
electrically conductive connection to the control electrode 32, is
provided at the edges of said rectangle on the rear surface. When
the plate 12 is provided on the disc 66, said layer 70 contacts an
aluminum layer 72 (see FIG. 7) which is provided in four sectors on
the front surface of the disc 66. These four sectors which are
separated from each other enable the electric contact between the
layers 70 and 72 to be checked after the provision. On the layer 72
the connection wire 58 is situated through which the video
information signal is supplied to the electrode 32. The thickness
of the plate 12 is 0.2 mm. which is compatible with the said
definition (600.times.800 points) in the proximity of the Curie
temperature the dielectric constant is much higher in the direction
of the optical axis of the crystal than in any other direction. As
a result of this the lines of force of the electric field cannot
deviate from the normal to the plate, while throughout the
thickness hereof the definition obtained in the division of the
charges on the layer 44 can be maintained.
It has already been noted above that in the examples described the
plate 12 is kept substantially at the Curie temperature by means of
the control device to be described with reference to FIG. 8. In the
embodiments described, as shown, (only) in FIG. 4, the plate 12 is
for that purpose secured to a fluorine plate 66 having a
coefficient of expansion approaching that of KPD provided in a tray
62 of copper which is cooled by the hollow ring 80 which is
connected to a Joule-Thompson cryostat 18, to which nitrogen under
a pressure of 150 kg./sq.cm. is supplied. Only the plate 81 of the
cryostat is denoted in FIG. 4. With reference to FIG. 8, the
cryostat is formed by a narrow tube 82, which ends in a small
aperture and is wound within an inner tube 83 having a thermally
insulating wall. The gas expands via said aperture, so that it is
cooled and said gas in turn cools the in-flowing gas during its
escape along the narrow tube. The temperature gradually decreases.
The supply of nitrogen from a bottle 84 is controlled by an
electrically operated valve 86 which in itself is controlled on the
basis of the measured capacity of the capacitor 90 consisting of
the plate 88 covered with two electrodes. The plate 88 has a
diameter of from 3 to 10 mm., and a thickness of approximately 0.5
mm. It consists of KDP which is enriched with 5 to 20 percent less
deuterium than the plate 12 and is provided near the plate 12 (not
shown). In the tube shown in FIG. 4 it is adhered, for example, to
the free surface of the grid support 52. The characteristic of the
dielectric constant of the material of the plate 88 in accordance
with the temperature, enables the optimum operating temperature to
be adjusted for the plate 12.
The other elements of the control device are: an electric
oscillator 92 of 2 mc./s., a capacitor 94 which forms a capacitive
bridge with the capacitor 90, an amplifier 96, a detector 98, the
electromagnetic part 100 of the valve 86 and finally a controllable
threshold formed by a potentiometer 102 and a direct voltage
generator 104.
The device according to the invention can be improved by the
measure shown in FIGS. 9 to 13.
Whereas in FIG. 2 the optic system L operates as a collimator and
as a projection objective, FIG. 9, to which reference is now made,
shows the collimator separated from the objective. The collimator
is constituted by the plane-convex lens formed by the fluorine
plate 66 which also serves for the heat dissipation of the target
plate 12. A beam separation polarization device R is used. It may
comprise several dielectric layers or be derived from the
Glazebrook prism of spar as is shown in the Figure. The objective
125 is arranged between the beam separation polarization device R
and the projection screen 2. The lens 125 can as a result be
manufactured without special measures with respect to thermal or
mechanical stresses since it is avoided that the objective serves
as L in FIG. 2, as if it were placed between two crossed
polarizers, whereby each stress in the objective lens is expressed
in the appearance of parasitic light on the projection screen and
results in errors in the uniformity of the brightness of the
picture and a reduction of the contrast. Since the collimator 66 is
arranged substantially in the objective plane, it has only an
extremely weak influence on the operation of the objective 125. For
the calculation of the objective 125 only the curvature of the
field as a result of the collimator need be taken into account as
regards the collimator. The light source in FIG. 9 is of the film
projection type and consists of a lamp 6 having a mirror 123 in the
form of an ellipsoid of revolution.
The device shown in FIG. 9 may furthermore be improved by using the
measures shown in FIG. 10. Whereas in the device shown in FIG. 9
only half of the light intensity which is incident on the prism R
is used, since the surface 31 reflects only one of the polarized
components of the light to the plane 12, the whole light intensity
in the device shown in FIG. 10 is used by making use of a multiple
beam separation polarization device R, a plate 127 which shifts the
phase by half a wavelength, two flat mirrors 128 and 130 and one
concave mirror 129.
FIG. 11 shows in detail the multiple beam separation polarization
device R of FIG. 10 derived from the Glazebrook type of spar and
the direction of the electric vectors of the components of the
incident and emanating polarized light. The optic axis of the spar
is perpendicular to the plane of the drawing. Along the surfaces
131 and 132, three prisms equivalent to the two prism of R of FIG.
9 are combined by a glue the index of refraction of which lies in
the proximity of the extraordinary index of refraction of the spar
(n.sub.e = 1.486) which is lower than the ordinary index of
refraction (n.sub.o = 1.658). The prism 136 allows the light which
passes the surface 131 to emanate. This prism 136 is equivalent to
a layer with parallel surfaces for the projection beam and may
consist of glass or another transparent isotropic material which is
united with the three other prism by means of a suitable glue the
index of refraction of which may be different from the said index
of refraction n.sub.e.
As shown in FIG. 10, the mirror 12 forms a picture of the source 6
in the beam separation polarization device R. The component of the
light the electric vector of which is parallel to the plane of the
drawing, is reflected at the surface 131 to the collimator 66 (see
FIGS. 10 and 11). The component the electric vector of which is
perpendicular to the plane of the drawing traverses R directly and
then the plate 127. Beyond the plate 127 the electric vector is
parallel to the plane of the drawing. By means of the flat mirrors
128 and 130 the concave mirror forms a second picture of the source
of the beam separation polarization device. The concave mirror
which operates with a magnification equal to 1, may be spherical.
By moving the concave mirror to the right or to the left in FIG. 10
only one of the flat mirrors 128 and 130 is sufficient.
The multiple beam separation polarization device R may also be
manufactured entirely from glass when several dielectric layers are
used at the separating surfaces 131 and 132. In this case the
directions of the electric vectors are the inverses of those which
are shown in FIG. 11.
With suitable choice of the indices of refraction the faces 131 and
132 may enclose angles of 45.degree. with the axis and, as shown in
FIG. 12, when a quarter wavelength plate 127 is used which is
passed two times, the prism 136 and the flat mirrors 128 and 130
may be omitted.
In the device shown in FIGS. 9 and 10 the light source 6 for the
mirror 123 a shadow which involves a nonuniform illumination of the
target plate and hence brightness errors on the screen 2. In order
to avoid this the devices may further be improved by using the
measure shown in FIG. 13. In FIG. 13 an assembly of two mirrors 141
and 142 which are shifted from each other by a few millimeters and
enclose an angle of a few degrees with each other is arranged
between the mirror 121 and the beam separation polarization device
R so that the light source 6 in front of the mirror 123 is not
visible when the mirror is observed through the beam separation
polarization device by means of the mirrors 141 and 142. The
mirrors 141 and 142 are preferably "cold mirrors," which are
transparent to infrared radiation so that heating of the beam
separation polarization device, of the target plate and of other
optical means used is counteracted.
In order to prevent that secondary electrons originating from the
point of the screen 266 hit by the electron beam impinge upon
points which may have higher potentials than the point of the grid
30, this grid may be provided, according to a known measure, very
close to the screen by adhering the grid 30 to the screen after the
surface of the grid has been covered with an insulating layer.
Furthermore, in order to prevent incident electrons on the screen
266, according to a known measure, a magnetic field perpendicular
to the surface of the screen is used. These measures prevent
efficaciously that the secondary electrons originating from the
point hit by the electron beam are received by adjacent points.
Upon using these measures alone, however, it remains possible that
secondary electrons, after having covered a path of several
millimeters or several centimeters, can return to all points of the
screen which have a potential equal to that or higher than that of
the screen. In order to remove this drawback, the last electrode of
the electron-optical lens system in the tube is preferably set up
at a potential which is equal to or higher than the highest
potential which any point of the screen can reach. Since this
highest potential with respect to the potential of the grid in
absolute value is equal to the potential difference between a
"white" point and a "black" point, a potential difference which is
at least equal to the maximum peak-to-peak control voltage must be
applied between the said last electrode and the grid. In practice
the last electrode then has a potential which is approximately 100
to 200 volts higher than that of the grid. The last electrode
preferably is a second grid provided in front of the first grid 30
at a few millimeters distance therefrom on the cathode side, to
which second grid a potential is applied which is 100 to 200 volt
higher than that of the first grid. This provides the advantage
that a particularly uniform collection of the secondary electrons
is also obtained. Since the second grid is not placed in the focal
plane of the beam it may have wider meshes than the first grid, the
advantage of a great transparency being obtained. The second grid
preferably consists of parallel wires stretched perpendicularly to
the direction of the scanning lines in order to avoid Moire
phenomena. When the first grid has a rectangular structure, the two
orthogonal directions of said structure preferably are oriented so
that they enclose angles of 45.degree. with the scanning lines and
with the direction of the wires of the second grid. When the first
grid has a "hexagonal" structure, the orientation thereof with
respect to the scanning lines and the wires of the second grid is
not critical. It is to be noted that the above-mentioned second
grid can be used together with a first grid secured to the screen
and a magnetic field, but, if desirable, for the sake of particular
requirements, may also serve to replace a first grid adhered to the
screen or a magnetic field.
* * * * *