Image intensifier

In an image intensifier comprising an entrance faceplate, made of a material transparent to light, having a photoelectric surface, formed on a surface opposite to a light entrance surface, for photoelectrically converting incident light into an electron; and an optical fiber block, constituted by a plurality of optical fibers bundled together, having a phosphor face at an end face of each optical fiber on the light entrance side, for emitting light in response to the electron incident thereon; the photoelectric surface of the entrance faceplate and the phosphor face of the optical fiber block opposing each other, while a vacuum atmosphere being formed therebetween; the optical fiber block is provided with a pit in which an end face of a core portion of each optical fiber is recessed from an end face of a cladding portion thereof, the bottom of the pit is filled with a phosphor, the surface of this phosphor is provided with a metal back layer, the cladding portion projects from the surface of the phosphor toward the entrance surface by a predetermined height, and the projecting surface of the cladding portion is provided with a metal film.

BACKGROUND OF THE INVENTION 
1. Field of the Invention 
The present invention relates to an image intensifier. 
2. Related Background Art 
FIG. 2 is a configurational view showing a typical proximity-type image 
intensifier. 
The image intensifier shown in FIG. 2 is constituted, successively in a row 
from its light entrance surface side, by a photoelectric plate 1, an 
microchannel plate (MCP) 2, and an optical fiber block 4. An output 
phosphor face 3 is formed on the surface of the optical fiber block 4 on 
the entrance surface side. When light is incident on the entrance surface 
of the photoelectric plate 1, due to photoelectric conversion, an electron 
is emitted from the surface of the photoelectric plate 1 opposite to the 
entrance surface. This electron is accelerated and amplified by the MCP 2, 
and then impinges on the phosphor face 3, thus emitting fluorescent light. 
The emitted light is guided through the optical fiber block 4 to the 
output side, whereby the incident light is amplified so as to yield output 
light. In the proximity-type image intensifier, the phosphor face 3 and 
the MCP 2 are disposed close to each other, thereby enhancing image 
reproducibility while attaining a compact configuration. 
In order to improve the output resolution of the image intensifier, various 
proposals have been made concerning the improvement of the output phosphor 
face. For example, one such proposal is disclosed in Japanese Patent 
Application Laid-Open No. 62-252043. According to the technique disclosed 
therein, as shown in FIG. 3, a core portion 42 on the entrance surface 
side of the optical fiber block 4 is formed with a pit 44 with respect to 
a cladding portion 43, and after the pit 44 is filled with a phosphor 45, 
a metal back layer 46 is formed on the surface on the entrance side. 
In contrast to the case where a phosphor layer is uniformly applied to the 
whole surface of the optical fiber block on the entrance surface side, a 
higher ratio of light generated in the phosphor 45 is made incident on the 
core portion 42, and the loss caused by the light leaked into and absorbed 
by the cladding portion 43 can be reduced. This enhances transmission 
efficiency, while light from leaking into the adjacent core, thereby 
improving the resolution as well. 
Nevertheless, the following problems may occur due to the fact that the 
electron is reflected on the output phosphor face. A part of the electrons 
accelerated from the MCP 2 are diffusely reflected by the surface of the 
metal back layer 46 of the phosphor face 3 when impinging thereon. FIG. 4 
shows a state of this diffuse reflection. Between the MCP 2 and the 
phosphor face 3, an electric field is generated by virtue of a voltage 
applied thereto. As shown in FIG. 4, the path of the diffusely reflected 
electron is deflected use to this electric field. As such the electron may 
re-impinge on a wide area of the phosphor face 3. 
Consequently, when a strong spot light enters the image intensifier, it 
allows a large amount of electrons to be incident on a narrow area of the 
phosphor face 3 from the MCP 2, and the electron, diffusely reflected on 
the phosphor face 3, may re-impinge on the phosphor face 3 over a much 
wider area than the initial incident area. As a result, a fluorescence 
effect may be generated in and outputted from an area wider than the 
incident area of the original spot light, thus deteriorating output 
resolution. This deterioration is commonly known as the halo phenomenon of 
output light. 
This halo phenomenon can be reduced when the distance between the MCP 2 and 
the phosphor face 3 is decreased. Nevertheless, because there is a limit 
to the minimal distance therebetween, due to pressure resistance, it has 
conventionally been difficult to suppress the halo phenomenon. As such, 
output resolution with respect to strong spot light has been hard to 
improve. 
SUMMARY OF THE INVENTION 
It is an object of the present invention to provide an image intensifier 
which can yield an improved output resolution even with respect to strong 
spot light. 
The present invention provides an image intensifier comprising an entrance 
faceplate, made of a material transparent to light, having a photoelectric 
surface, formed on a surface opposite to a light entrance surface, for 
photoelectrically converting incident light into an electron. Also 
provided is an optical fiber block, constituted by a plurality of optical 
fibers bundled together, having a phosphor face at an end face of each 
optical fiber on the light entrance side, for emitting light in response 
to the electron incident thereon. The photoelectric surface of the 
entrance faceplate and the phosphor face of the optical fiber block oppose 
each other, while a vacuum atmosphere is formed therebetween. The phosphor 
face of the optical fiber block is provided with a pit in which an end 
face of a core portion of each optical fiber constituting the optical 
fiber block is recessed from an end face of a cladding portion thereof, 
and a phosphor is embedded in each pit, while the cladding portion 
projects from a surface of the phosphor by a predetermined height, the 
projecting surface of the cladding portion being provided with a metal 
film. 
Consequently, the pit formed at the core portion of each optical fiber on 
the entrance-side end face of the optical fiber block is provided with a 
phosphor face, whereas the formed phosphor faces are connected to each 
other through the metal film formed on the projecting surface of the 
cladding portion at the entrance-side end face of the optical fiber block. 
Accordingly, individual phosphor faces partitioned so as to correspond to 
the respective optical fibers are provided, while being recessed from the 
entrance surface and separated from each other. Because all of these 
phosphor faces are electrically connected to each other, the same voltage 
can be applied to all the phosphor faces. 
Also, a metal film may be formed on the phosphor face. This metal film 
functions as a metal back layer with respect to the phosphor face, whereby 
the light generated in the phosphor is effectively guided to the optical 
fiber. 
Further, the projecting height of the cladding portion is preferably at 
least 0.5 times diameter of the core portion. In particular, it is 
preferably at least 1.0 times diameter of the core portion. Consequently, 
each phosphor face can be separated from its adjacent phosphor face more 
securely, thus suppressing mutual influences among the phosphor faces. 
The present invention will be more fully understood from the detailed 
description given hereinbelow and the accompanying drawings, which are 
given by way of illustration only and are not to be considered as limiting 
the present invention. 
Further scope of applicability of the present invention will become 
apparent from the detailed description given hereinafter. However, it 
should be understood that the detailed description and specific examples, 
while indicating preferred embodiments of the invention, are given by way 
of illustration only, since various changes and modifications within the 
spirit and scope of the invention will be apparent to those skilled in the 
art from this detailed description.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS 
In the following, an embodiment of the present invention will be explained 
with reference to the accompanying drawings. FIG. 1 is an enlarged view 
showing the optical fiber block in accordance with this embodiment. 
Since the basic configuration of the image intensifier in this embodiment 
is the same as the typical proximity-type image intensifier shown in FIG. 
2, no explanation will be provided for the overall configuration and 
operation thereof. First, the configuration of its optical fiber block 4 
will be explained with reference to FIG. 1. Basically, the optical fiber 
block 4 has a configuration in which a number of optical fibers 41, each 
comprising a core portion 42 and a cladding portion 43 with a lower 
refractive index covering the core portion 42, are bundled together. 
Consequently, light incident on the core portion 42 can be efficiently be 
transmitted to the output side. 
The end face of the core portion 42 on the entrance surface side is 
recessed from the end face of the cladding portion 43 so as to form a pit 
44, whose bottom is filled with a phosphor 45 which emits light upon 
electron bombardment. The part filled with the individual phosphor 45 
corresponds to the phosphor face 3 shown in FIG. 2. Accordingly, the 
individual phosphor faces 3 are respectively provided for the individual 
optical fibers 41. The surface of the phosphor 45 is provided with a metal 
back layer 46. The cladding portion 43 projects from the surface of the 
phosphor 45 toward the entrance surface, and its tip end is rounded. The 
individual phosphor faces 3 are separated from each other by the cladding 
portion 43. The surface of the projecting part of the cladding portion 43 
is provided with a metal film 47. Accordingly, the individual phosphors 45 
embedded within the respective pits 44 are electrically connected to each 
other through the metal film 47. Current is supplied to the metal back 
layer 46 through the metal film 47, whereby a voltage is applied between 
the metal back layer 46 and the MCP 2 shown in FIG. 2, thus forming an 
electric field therebetween. 
As the optical fiber 41, either an optical fiber whose core portion 42 has 
a square cross section as shown in FIGS. 5A and 5B or an optical fiber 
whose core portion 42 has a circular cross section as shown in FIGS. 5C 
and 5D, may be used. In the case of an optical fiber having a square cross 
section, the length of one side thereof will be heretofore referred to as 
the diameter. Therefore, the diameter of the core portion and the 
projecting height of the cladding portion will be hereinafter referred to 
as d and L, respectively. 
Thus, the optical fiber block 4 can be configured, for example, as follows. 
First, a number of optical fibers are bundled, and end faces of the core 
portion 42 and cladding portion 43 are processed into flat surfaces while 
being aligned with each other. Then, the formed bundle is etched with an 
acid or alkali solution which can selectively erode the core portion 42, 
so as to form a desired depth of the pit 44. The depth of the pit 44 can 
be controlled by a precision of .mu.m unit when the concentration, 
reaction time, and reaction temperature of the etching solution are 
regulated. After the pit 44 is formed, the tip of the cladding portion 43 
is rounded by etching, and then the metal film 47 is deposited on the 
exposed surface of the cladding 43. 
Subsequently, the bottom portion of thus formed pit 44 is forcibly filled 
with the grains of phosphor 45 by centrifugal sedimentation. Such as type 
P11 (ZnS: Ag), P20 ((Zn, Cd)S: Ag), P24 (ZnO: Zn), P43 (Gd.sub.2 O.sub.2 
S: Tb.sup.3+), P46 (Y.sub.3 Al.sub.5 O.sub.12 : Ce.sup.3+) or P47 (Y.sub.2 
SiO.sub.5 : Ce.sup.3+) fluorescent material can be used for the phosphor 
45. Preferably the grain of the phosphor 45 has 2.0 .mu.m mean diameter. 
Because it is difficult to fill the bigger grain to the pit 44 and smaller 
grain has smaller light conversion efficiency than this grain. 
Here, as the amount of phosphor 45 is adjusted, the height of the cladding 
portion 43 projecting from the surface of the phosphor 45 can be 
regulated. Since, as stated above the tip of the cladding portion 43 is 
rounded the grains of phosphor 45 naturally drop into the pit 44 from the 
tip of the cladding portion 43 without adhering to the surface of the 
cladding portion 43. 
Subsequently, a solution comprising a heat-decomposable polymer compound 
such as nitrocellulose or acrylic resin dissolved in an organic solvent 
fills up the pit 44 to the surface of the phosphor 45. The filling is 
forcibly effected by use of a centrifuge. After the polymer compound is 
dried, aluminum is deposited on its surface. Thereafter, as being heated 
at 350.degree. C. in the atmosphere, the polymer compound is decomposed 
and eliminated. Consequently, the metal back layer 46 made of Al is 
formed. 
In the following, with reference to FIGS. 6 and 7, explanation will be 
provided for operations of the optical fiber block 4 in accordance with 
this embodiment when an electron is incident on the phosphor face 3 from 
the MCP 2 shown in FIG. 2. FIGS. 6 and 7 are views each showing tracks of 
incident and reflected electrons in the vicinity of the entrance surface 
of the optical fiber block 4. 
The incident electron directed toward the phosphor face 3 from the MCP 2 
shown in FIG. 2 reaches the entrance surface (corresponding to a plane 
connecting the respective tips of the cladding portions 43) of the optical 
fiber block 4 as shown in FIG. 6. A portion of the incident electrons 
reach the metal back layer 46, whereas the rest reach the metal layer 47 
on the top and wall surfaces of the cladding portion 43 projecting toward 
the entrance surface from the metal back layer 46. A major portion of the 
electrons that reached the surface of the metal back layer 46 pass through 
the metal back layer 46 so as to impinge on the phosphor 45, thereby 
generating light. As the metal back layer 46 reflects the light generated 
in the phosphor 45 toward the core portion 42, the light is efficiently 
transmitted toward the core portion 42. About 3% of the electrons that 
reached the metal back layer 46 are diffusely reflected by its surface. On 
the other hand, a major portion of the electrons that directly reached the 
cladding portion 43 are absorbed by the metal film 47, leaving about 3% 
thereof to be diffusely reflected. 
As shown in FIG. 7, a portion of the reflected electrons travel along a 
track such as that indicated by A and directly impinge on the metal film 
47 on the wall surface of the cladding portion 43. Since the reflectivity 
of the metal film 47 is as low as about 3%, the amount of electrons 
jumping out of the entrance surface of the optical fiber block beyond the 
top part of the cladding portion 43, after being reflected by the wall 
surface of the cladding portion 43, is negligible. 
The reflected electrons that jump out of the entrance surface of the 
optical fiber block without directly impinging on the wall surface of the 
cladding portion 43 (see tracks B to D), return back toward the entrance 
surface of the optical fiber block due to the electric field formed 
between the MCP 2 and the phosphor face 3 (i.e. metal back layer 46 here). 
Since most of the returning electrons impinge on the top part (see track 
B) or wall surface (see track C) of the cladding portion without reaching 
the surface of the metal back layer 46, only a very small portion of all 
incident electrons contribute to fluorescence. This small portion is 
attributed to the returning electrons that impinge on the phosphor 45 
after being incident on the metal back layer 46 (see track D). 
While almost all the reflected electrons A to D are deemed to be made 
incident on the phosphor face 3 again in the conventional example, the 
amount of the reflected electrons reentering the phosphor face 3 is 
reduced in this embodiment. Consequently, the halo phenomenon caused by 
the reflected electrons can be suppressed, thus allowing a high resolution 
to be kept even with respect to strong incident spot light. 
The inventor conducted an experiment comparing the respective halo 
phenomena of the image intensifiers for the conventional example as shown 
in FIG. 3 and the present embodiment shown in FIG. 1. 
FIGS. 8A and 8B are perspective and sectional views showing the entrance 
surface of the optical fiber block in accordance with the present 
embodiment used for this experiment. The cross section of the core portion 
of each optical fiber is square with a diameter d of 6 .mu.m, whereas the 
cladding portion between the core portions has a thickness of 2 .mu.m and 
a height of 1.5 d, i.e., 9 .mu.m. The conventional example is 
substantially the same as this embodiment except that the height L of the 
cladding portion shown in FIGS. 8A and 8B is set to zero. In either case, 
the distance between the MCP outlet and the optical fiber block inlet is 
set to 0.7 mm, and a voltage of 6 kV is applied between the MCP and the 
optical fiber block inlet. The incident light is a spot light having a 
spot diameter of 0.4 mm with an output luminance of 150 nit. The output 
light from each optical fiber block is captured by a 2/3-inch CCD and then 
is subjected to image processing by an image processing apparatus DVS-2000 
manufactured by Hamamatsu Photonics K. K., whereby the samples are 
compared with each other in terms of spatial pattern and intensity 
distribution. 
The displayed images obtained as a result of the image processing are shown 
in FIGS. 9A to 9C. These photographs respectively show the incident light, 
the output light obtained by the conventional example, and the output 
light obtained by this embodiment. In each photograph, the upper and lower 
images respectively indicate the spatial pattern of the light and the 
intensity distribution of the light in a transverse section. It can be 
seen from FIGS. 9A to 9C that, when spot light having a very narrow range 
is given as incident light, output light spreads over a wide range in the 
conventional example. In particular, its intensity distribution resembles 
a skirt-like spread area on the periphery which is indicative of the halo 
phenomenon. In contrast the present embodiment did not generate a spread 
portion such as the above-mentioned skirt, and it can be seen that the 
boundary of light is cleaner and more vivid than that in the conventional 
example. As explained in the foregoing, it has been ascertained that the 
present embodiment can suppress the halo phenomenon and improve the 
resolution with respect to a strong spot light. 
Further, the inventor conducted a simulation for investigating a 
relationship between the ratio of the reflected electrons reentering the 
phosphor face and the height of the cladding portion in the image 
intensifier of the embodiment shown in FIGS. 8A and 8B. In this 
simulation, when electrons are incident on one channel of the MCP, the 
behavior of the electrons reflected by the phosphor face are calculated 
three-dimensionally by virtue of a Monte Carlo simulation method. 
Except for the cladding height, the embodiment is similar as that used in 
the above-mentioned experiment. The classing height subjected to the 
calculation. The distance between the MCP outlet and the optical fiber 
block inlet and the applied voltage were the same as those mentioned 
above, i.e., 0.7 mm and 6 kV, respectively. It was assumed that electrons 
were incident with a distribution pattern determined by the electron track 
analysis when the electrons were incident on one channel of the MCP, and 
the reflection characteristic in the phosphor face and metal film followed 
a distribution of I.theta.=I.sub.o .alpha.cos.theta. wherein incident 
electron intensity is I.sub.o and reflected electron intensity is I.theta. 
and .alpha. is a constant. 
FIG. 10 shows the result of this calculation. In this graph, the solid line 
indicates, of the electrons reflected by the wall surface or top part of 
the cladding or the phosphor face, the ratio of those re-impinging on the 
phosphor face and thereby contributing to luminescence. The dashed line 
indicates, of the electrons emitted from the MCP, the ratio of those 
directly incident on the phosphor face. The chain line indicates, of the 
electrons emitted from the MCP, the ratio of those incident on the 
cladding wall. It can be seen from FIG. 10 that the reentrance of the 
reflected electrons into the phosphor face decreases to 50% or less when 
the cladding height L is 0.5 times diameter d of the core portion. As the 
cladding height L increases, the ratio of reentrance decreases. When L =1 
d, the ratio of reflected electrons incident on the phosphor face 
decreases to 9.3%. Further, when L is 6 times d, the ratio of electrons 
reentering the phosphor face decreases to 0.3%. Accordingly, L is 
preferably at least 0.5 d by which the amount of reentering electrons is 
reduced by at least 50%. More preferably, it is at least 1.0 d by which 
the amount of reentering electrons becomes 10% or less. Nevertheless, it 
is not preferable for L to be increased too much, in view of the fact that 
the ratio of electrons reaching the phosphor face from the MCP decreases 
and that the manufacture becomes difficult. Accordingly, L is preferably 
not greater than 6.0 d. 
Though the above-mentioned embodiment relates to a proximity-type image 
intensifier, the present invention is also applicable to image 
intensifiers of a type using no MCP or those using electronic lenses or 
the like other than the proximity type. Also, the phosphor face may not be 
provided with the metal film. The form and arrangement of the optical 
fibers should not be restricted to those shown in this embodiment. 
As explained in the foregoing, in accordance with the present invention, 
partitioned phosphor faces are provided so as to respectively correspond 
to individual optical fibers, and are recessed from the entrance surface. 
Accordingly, a major portion of the electrons reflected by the phosphor 
faces impinge on the cladding portions projecting from the phosphor faces 
and are absorbed therein, whereby the amount of electrons reentering the 
phosphor faces can be reduced. Consequently the halo phenomenon or more 
specifically, the fluorescence generated around the original spot light as 
the reflected electrons reenter the phosphor faces when strong spot light 
is incident, can be prevented. Namely, even when strong spot light is 
incident thereon, the image intensifier of the present invention can 
sustain a high resolution. Also, since the boundary of spot light becomes 
vivid, it is possible to measure the weak light in a region proximate to 
the spot light. Such weak light has been conventionally hard to measure, 
given their likelihood of being hidden by the halo. 
Also, because the phosphor face is provided with a metal film, the light 
generated in the phosphor is prevented from leaking into the inner surface 
of the optical fiber block, whereby the resolution and output can be kept 
from deteriorating. 
Further, the projecting height of the cladding portion is preferably set so 
as to be at least 0.5 times and, more preferably, at least 1.0 times 
diameter d of the core portion. Consequently, the halo phenomenon can 
effectively be suppressed without deteriorating the sensitivity of the 
light-receiving surface. 
From the invention thus described, it will be obvious that the invention 
may be varied in many ways. Such variations are not to be regarded as a 
departure from the spirit and scope of the invention, and all such 
modifications as would be obvious to one skilled in the art are intended 
for inclusion within the scope of the following claims.