BACKGROUND OF THE INVENTION
Field of The Invention
[0001] The present invention relates to a photomultiplier of so-called side-on type into
which light to be measured is incident through a side of a container.
Related Background Art
[0002] Fig. 1 is a side view, partly in vertical section, of a conventional side-on type
photomultiplier which is generally used, and Fig.. 2 is a cross-sectional view of
the photomultiplier. In this photomultiplier, light to be measured enters through
a side of a glass bulb 1 which is a transparent closed container. The incident light
passing through the glass bulb 1 impinges on a photosurface of a reflection type photocathode
2, whereby photoelectrons are emitted from the photosurface. The photoelectrons are
then delivered to an electron multiplying unit constituted of plural stages of dynodes
3a, 3b, 3c ···. The electron multiplying unit successively multiplies the photoelectrons,
and the multiplied electrons are collected as an output signal in an anode 4.
[0003] A grid electrode 6 is provided between a light entrance portion 5 of the glass bulb
1 and the photocathode 2 so as to guide the photoelectrons emitted from the photocathode
2 to dynode 3a of the first stage. The potential of the grid electrode 6 is set to
be equal to that of the photocathode 2. There are various types of grid electrodes
which may be employed as the grid electrode 6. For example, the grid electrode 6 may
be a grid electrode (not shown) constituted in a manner that fine conductive wires
are placed in a grid-shaped configuration, or a grid electrode constituted in a manner
that one fine conductive wire 6c is helically wound around two supporting rods 6a
and 6b as shown in Fig. 1.
[0004] There is also known a side-on type photomultiplier disclosed in JP-B-53-18864. As
shown in Fig. 3, in this side-on type photomultiplier, a glass plate 7 on which a
transparent conductive film is formed is employed instead of the grid electrode 6.
[0005] There is also known a side-on type photomultiplier disclosed in JP-A-4-292843. JP-A-4-292843
discloses a structure in which a conductive portion such as an aluminum-evaporated
film is formed on an inside wall surface of a glass bulb except for a light entrance
portion. Further, JP-A-4-292843 also discloses that the conductive portion is formed
also on the light entrance portion when the conductive portion is transparent. The
conductive portion reduces a resistance of the inside wall surface of the glass bulb,
so that a time constant formed by stray capacitance and the surface resistance of
the inside wall surface of the glass bulb is small. Since the time constant is small,
the unstableness of the potential on the inside wall surface of the glass bulb is
eliminated. As a result, an influence upon an electron track of photoelectrons is
reduced, whereby a hysteresis characteristic is improved. The hysteresis is a phenomenon
that an output signal rises not suddenly but gradually to reach stability when an
optical pulse enters a photomultiplier.
SUMMARY OF THE INVENTION
[0006] According to the present invention, there is provided a photomultiplier comprising:
a transparent closed container including a light entrance portion; a reflection type
photocathode, provided in the closed container, for emitting photoelectrons in response
to an incident light transmitted through the light entrance portion; a transparent
conductive film formed on an inside wall surface of the light entrance portion of
the closed container, a predetermined potential being applied to the film; an electron
multiplying unit, including plural stages of dynodes, for electron-multiplying the
photoelectrons emitted from the reflection type photocathode; and an anode for collecting
the multiplied electrons.
[0007] The transparent conductive film may be formed on the entire inside wall surface of
the closed container.
[0008] The present invention will become more fully understood from the detailed description
given hereinbelow and the accompanying drawings which are given by way of illustration
only, and thus are not to be considered as limiting the present invention.
[0009] 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 become apparent to
those skilled in the art from this detailed description.
BRIEF DESCRIPTION OF THE DRAWINGS
[0010]
Fig. 1 is a side view, partly in vertical section, of a conventional photomultiplier
which is generally used;
Fig. 2 is a cross-sectional view of the conventional photomultiplier which is generally
used;
Fig. 3 is a cross-sectional view showing an example of another conventional photomultiplier;
Fig. 4 is a side view, partly in vertical section, of a photomultiplier according
to a first embodiment of the present invention;
Fig. 5 is a cross-sectional view of the photomultiplier according to the first embodiment;
Fig. 6 is a cross-sectional view showing an example of a variant of a transparent
conductive film in the first embodiment;
Fig. 7 is a cross-sectional view of a photomultiplier according to a second embodiment
of the present invention;
Fig. 8 is a diagram showing an electron track of photoelectrons in a conventional
structure;
Fig. 9 is a diagram showing an electron track of photoelectrons in a structure according
to the second embodiment;
Fig. 10 is a side view, partly in vertical section, of a photomultiplier according
to a third embodiment of the present invention;
Fig. 11 is a cross-sectional view of the photomultiplier according to the third embodiment;
Fig. 12 is a perspective view showing a shape of a dynode in the third embodiment;
Fig. 13 is a side view, partly in vertical section, of a photomultiplier according
to a fourth embodiment of the present invention;
Fig. 14 is a cross-sectional view showing an example of a structure of a transparent
conductive film in the fourth embodiment; and
Fig. 15 is a cross-sectional view showing another example of a structure of the transparent
conductive film in the fourth embodiment.
DESCRIPTION OF THE PREFERRED EMBODIMENTS
[0011] Figs. 4 and 5 show a photomultiplier of so-called side-on type to which an embodiment
of the present invention is applied. A glass bulb 11 is a transparent closed container.
Specifically, the glass bulb 11 is a transparent cylinder closed at the upper and
lower ends. Insulating material substrates 12a and 12b are provided at the upper and
lower positions in the glass bulb 11, respectively. The substrates 12a and 12b support
various electrodes. The various electrodes are led to the outside through terminals
14 provided on a base 13 placed at the bottom of the glass bulb 11. A photocathode
16, an electron multiplying unit 17 and an anode 18 for collecting an output signal
are supported between the insulating material substrates 12a and 12b. The photocathode
16 is placed so as to be inclined at a predetermined angle to a light entrance portion
15 of the glass bulb 11. The electron multiplying unit 17 is constituted of plural
stages of dynodes 17a, 17b, 17c for successively multiplying photoelectrons emitted
from the photocathode 16.
[0012] A transparent conductive film 19 is partically formed on an inside wall surface of
the light entrance portion 15 of the glass bulb 11. Although the transparent conductive
film 19 may be formed in various manners, the film 19 is preferably formed in a manner
that chromium (Cr) is selectively evaporated onto the inside wall surface of the glass
bulb 11. The transparent conductive film 19 electrically contacts with a pad 20 adhered
to the inside wall surface of the light entrance portion 15 of the glass bulb 11.
The pad 20 is led through the terminal 14 to the outside.
[0013] In this arrangement, predetermined potentials are applied to the photocathode 16
and the anode 18 through the terminals 14, respectively. For example, a potential
of - 1KV is applied to the photocathode 16, and a ground potential is applied to the
anode 18. An appropriate potential which divides a voltage between the photocathode
16 and the anode 18 is applied through the terminal 14 to each of the plural stages
of dynodes 17a, 17b, 17c···. For example, the same potential as the photocathode 16,
that is, the potential of -1KV is applied to the transparent conductive film 19 through
the terminal 14 and the pad 20. In such a state, incident light directly impinges
on the photocathode 16 through the light entrance portion 15 of the glass bulb 11
and the transparent conductive film 19. At this time, there is no grid electrode between
the light entrance portion 15 and the photocathode 16 like the prior art, and therefore
the incident light reaches the photocathode 16 with not being interfered at all. That
is, in the conventional photomultiplier as shown in Figs. 1 and 2, since the grid
electrode 6 is placed in front of the photocathode 2, a part of the light which is
to be entered into the photocathode 2 through the glass bulb 1 is scattered or absorbed
by the conductive wire 6c of the grid electrode 6. Therefore, even if the incident
light is uniform, a part of the incident light does not reach the photocathode 2.
Further, loss is caused due to absorption or scattering when light passes through
a glass material. Therefore, when the glass plate 7 is placed in the glass bulb 1
like the conventional photomultiplier as shown in Fig. 3, there arises a problem that
the loss becomes twofold since the light passes through a glass material two times.
However, in the present embodiment, as described above, the incident light reaches
the photocathode 16 with not being interfered at all.
[0014] Further, if the transparent conductive film 19 is a chromium-evaporated film., the
loss of light caused when the incident light passes through the transparent conductive
film 19 is extremely small since the transparent conductive film 19 has a high transmittance
of 98%. In contrast, in the conventional photomultiplier as shown in Figs. 1 and 2,
since a grid electrode having a transmittance of 75% is generally employed as the
grid electrode 6, 25% of the incident light does not reach the photocathode 2. Therefore,
the transmittance for the incident light entering the photomultiplier according to
the present invention is extremely improved.
[0015] Furthermore, in the conventional photomultiplier as shown in Fig.3, there also arises
a problem associated with manufacture. That is, conventionally, in a manufacturing
process of the photocathode 2, an alkali metal used for producing a photosurface flows
and reaches the photosurface as shown by the dotted lines in Fig. 3. However, when
the glass pate 7 is placed in the flow-path of the alkali metal, the alkali metal
can not be uniformly led to the photocathode 2. As a result, in the conventional photomultiplier,
it is very difficult to form a uniform photosurface. In contrast, in the present embodiment,
since such a glass plate 7 is not employed, the uniform photosurface can be produced
readily.
[0016] In the present embodiment, there is no conventional grid electrode between the light
entrance portion 15 and the photocathode 16, and the transparent conductive film 19,
to which a predetermined potential is applied, formed on the light entrance portion
15 functions as a focusing electrode. Therefore, an electric field for focusing photoelectrons,
formed between the photocathode 16 and the dynode 17a of the first stage of the electron
multiplying unit 17, spreads up to the position near the inside wall surface of the
light entrance portion 15 of the glass bulb 11. As a result, the photoelectrons, which
are generated from the photocathode 16 and which exist in the vicinity of the photocathode
16, are guided due to the electric field for focusing and accelerated toward the dynode
17a of the first stage. Consequently, the photosensitivity of the photomultiplier
according to the present embodiment is improved when compared with that of the photomultiplier
shown in Figs. 1 and 2 by 20% or more, and the SN ratio which is the ratio of the
input signal to the noise is improved in the present embodiment.
[0017] In the present embodiment, since the predetermined potential is applied to the transparent
conductive film 19 formed on the inside wall surface of the light entrance portion
15 of the glass bulb 11, the unstableness of the potential on the inside wall surface
of the glass bulb 11 is eliminated. Therefore, even if the photoelectrons collide
with the inside wall surface of the glass bulb 11, the potential of the inside wall
surface of the glass bulb 11 immediately returns to the predetermined potential, that
is, -1KV, and hence the change of the potential of the inside wall surface of the
glass bulb 11 is performed at high speed. It is considered that the photoelectrons
from the photocathode 16 collide with the light entrance portion 15 of the glass bulb
11 and the portion is charged, whereby the potential of the portion becomes unstable
and an electron track of photoelectrons is influenced. Therefore, the hysteresis of
the photomultiplier becomes extremely small.
[0018] On the other hand, the conventional grid electrode 6 shown in Figs. 1 and 2 plays
not only a role as an electron lens but also a role for improving the hysteresis characteristic.
Therefore, in the conventional grid electrode 6 shown in Figs. 1 and 2, the photoelectrons
moving from the photocathode 2 to the light entrance portion 5 are intercepted by
stringing the conductive wire 6c on a plane in front of the entire front surface of
the photocathode 2. However, some photoelectrons pass between the lattices of the
grid electrode 6 and reach the light entrance portion 5, and hence the improvement
of the hysteresis characteristic has a limitation. Further, in the conventional photomultiplier
disclosed in JP-A-4-292843 in which the hysteresis characteristic is improved by forming
the conductive portion on the inside wall surface of the glass bulb, there also arises
the above-mentioned problem of the reduction in the transmittance since the grid electrode
is placed in front of the photocathode. However, in the photomultiplier according
to the present embodiment, as described above, the hysteresis of the photomultiplier
is exceedingly small.
[0019] In the above explanation of the embodiment, the case where the transparent conductive
film 19 is partly formed on the front of the light entrance portion 15 has been described.
However, As shown in Fig. 6, a transparent conductive film 19a may be formed on the
side portion, including the light entrance portion 15, of the glass bulb 11 along
the perimeter of the glass bulb 11. However, a plate spring 41 (see Fig. 4) for fixing
the insulating material substrate 12a to the glass bulb 11 is fixed to an end of a
rod for supporting the dynode 17, and hence the plate spring 41 is electrically connected
to the dynode 17. Therefore, the transparent conductive film 19a is not formed on
the upper portion of the glass bulb 11 so that the transparent conductive film 19a
does not contact with the plate spring 41. Even if the transparent conductive film
19a is employed, advantages similar to the above-mentioned embodiment are obtained.
In Fig. 6, portions identical to those of Figs. 4 and 5 are referred to by the same
reference numerals, and therefore-will not be described.
[0020] Next, a photomultiplier according to a second embodiment of the present invention
will be described.
[0021] Fig. 7 is a cross-sectional view of the photomultiplier according to the second embodiment.
In Fig. 7, portions identical to those of Figs. 4 and 5 are referred to by the same
reference numerals, and therefore will not be described. The present embodiment differs
from the first embodiment in a shape of a photocathode 21. That is, in the present
embodiment, there is no rod on the light entrance portion 15 side of the photocathode
21, and an end of the light entrance side of the photocathode 21 is fixed to a shield
plate 22 by weld. In this way, the photocathode 21 has a structure which functions
also as a shield plate. Further, since there is no conventional grid electrode between
the light entrance portion 15 and the photocathode 21, the photocathode 21 can be
expanded to a portion interfered by the conventional grid electrode. That is, the
end of the light entrance portion 15 of the photocathode 21 can be extended to a position
extremely close to the inside wall surface of the glass bulb 11, so that the effective
light-receptive area is increased. For example, in the present embodiment, the width
of photocathode 21 in a direction perpendicular to the light entrance direction is
about 3mm wider than that of the photocathode 2 of the conventional photomultiplier
shown in Figs. 1 and 2. As a result, in the present embodiment, the photosensitivity
of the photomultiplier is increasingly improved.
[0022] Further, as is apparent from Figs. 8 and 9, in the second embodiment, the electric
field for focusing photoelectrons is extremely widespread. Fig. 8 shows the electric
field for focusing which is formed in the conventional photomultiplier shown in Figs.
1 and 2. In Fig. 8, portions identical or corresponding to those of Figs. 1 and 2
are referred to by the same reference numerals, and therefore will not be described.
Fig. 9 shows the electric field for focusing which is formed in the photomultiplier
according to the second embodiment. In Fig. 9, portions identical or corresponding
to those of Fig. 7 are referred to by the same reference numerals, and therefore will
not be described.
[0023] In the conventional structure shown in Fig. 8, the electric field for focusing photoelectrons
is formed by the photocathode 2, the grid electrode 6 and the dynodes 3a and 3b. Due
to this electric field, an electron lens is formed between the photocathode 2 and
the dynode 3a, thereby the photoelectrons trace the electron track shown in the figure.
However, in this conventional structure, since there is the grid electrode 6 between
the light entrance portion and the photocathode 2, the permeation of the electric
field for focusing photoelectrons is weak in a region A of the photocathode 2 in the
vicinity of the inside wall surface of the glass bulb 11. Therefore, the photoelectrons
which exit in this region A among the photoelectrons emitted from the photocathode
2 is not efficiently guided to the dynode 3a of the first stage.
[0024] On the other hand, in the structure according to the present embodiment shown in
Fig.9, since there is no grid electrode such as the conventional grid electrode between
the light entrance portion and the photocathode 21, as described above, the end of
the photocathode 21 can be extended to the vicinity of the inside wall surface of
the glass bulb 11 without being interfered by the grid electrode. Consequently, the
electric field for focusing photoelectrons is formed to expand to the vicinity of
the inside wall surface of the glass bulb 11, whereby the electric field sufficiently
permeates also in the region in which the permeation of the electric field is conventionally
weak so that the electron track shown in the figure is formed. As a result, most of
the photoelectrons emitted from the photocathode 21 having the large size of the effective
light-receiving area is efficiently guided to the dynode 17a of the fist stage, and
therefore the photosensitivity of the photomultiplier is increasingly improved so
that the SN ratio is extremely improved.
[0025] Next, a photomultiplier according to a third embodiment of the present invention
will be described.
[0026] Fig. 10 is a side view, partly in vertical section, of the photomultiplier according
to the third embodiment, and Fig. 11 is a cross-sectional view thereof. In Figs. 10
and 11, portions identical or corresponding to those of Figs. 4, 5 and 7 are referred
to by the same reference numerals, and therefore will not described. The present embodiment
differs from the second embodiment in the structure of the electron multiplying unit
17. That is, in each of dynodes 17A, 17B, 17C and 17D of fist, second, third and fourth
stages constituting the electron multiplying unit 17, as shown in Fig. 12, the middle
portion of a supporting rod 31a which exists at the light entrance side between two
supporting rods 31a and 31b is eliminated. In Fig. 12, the dynode 17A is shown as
a representative of these dynodes. Since the middle portion of the supporting rod
31a is eliminated in this way, it is prevented that the photoelectrons accelerated
by the electric field for focusing is attracted by the supporting rod during the drift
to bend the electron track like the conventional structure shown in Fig. 8. Therefore,
the photoelectrons emitted from the photocathode 21 and the photoelectrons secondary-electron-multiplied
in the dynodes of the respective stages surely reach the dynodes of the next stages,
respectively. As a result, in the structure of the photomultiplier according to the
present embodiment, the photosensitivity is increasingly improved.
[0027] Next, a photomultiplier according to a fourth embodiment of the present invention
will be described.
[0028] Fig. 13 is a side view, partly in vertical section, of the photomultiplier according
to the fourth embodiment. In Fig. 13, portions identical or corresponding to those
of Figs. 4, 5 and 7 are referred to by the same reference numerals, and therefore
will not be described. The present embodiment differs from the above-mentioned second
embodiment in a structure for fixing the insulating material substrates 12a and 12b
supporting the photocathode 21 and dynodes 17 to the glass bulb 11. That is, in the
structure shown in Figs. 4 and 5, a part of the plate spring 41 having a shape extending
along a direction of a circumference of the insulating material substrate 12a is fixed
to an end of the supporting rods of the dynode 17. The plate spring 41 contacts with
the inside wall of the glass bulb 11 at a plurality of positions. Due to the elastic
force of the plate spring 41 toward the outside in a direction of a radius of the
insulating material substrate 12a, the supporting rods of the dynode 17 and the insulating
material substrate 12a fixed to the supporting rods are supported by and fixed to
the inside wall of the glass bulb 11.
[0029] However, in the photomultiplier shown in Fig. 13 according to the present embodiment,
a plurality of spring plates 51 is provided between the two insulating material substrates
12a and 12b at a plurality of positions. Two ends of each of the sprig plates 51 are
engaged with the circumference portions of the insulating material substrates 12a
and 12b, respectively. The middle portions of each of the spring plates 51 contact
with the inside wall of the glass bulb 11. Due to the elastic force of each of the
spring plates 51 toward the outside from the longitudinal center axis of the glass
bulb 11, the insulating material substrates 12a and 12b are supported by and fixed
to the inside wall of the glass bulb 11.
[0030] Since the spring plates 51 electrically float, in the present embodiment, even if
the transparent conductive film constituting the electrode for focusing contacts electrically
with the spring plates 51, the electron multiplying function is not influenced. That
is, in the present embodiment, the transparent conductive film 19 may be partly formed
on only the place corresponding to the light entrance portion 15 as shown in Fig.
14 in a manner similar to the second embodiment, and the transparent conductive film
19b may be formed on the whole of the inside wall surface of the glass bulb 11 as
shown in Fig. 15. In Figs. 14 and 15, portions identical or corresponding to those
of Fig. 7 are referred to by the same reference numerals, and therefore will not be
described. When the transparent conductive film 19b is formed on the whole of the
inside wall surface as shown in Fig. 15, the manufacturing process in which the transparent
conductive film is selectively formed on only the place corresponding to the light
entrance portion 15 is eliminated. Therefore, according to the photomultiplier having
the structure shown in Fig.15, an advantage that the manufacturing process is simplified
is obtained in addition to advantages similar to the above-mentioned second embodiment.
[0031] 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 to be included within the scope of the following claims.
[0032] The basic Japanese Application No.309371/1993 filed on December 9, 1993 is hereby
incorporated by reference.
1. A photomultiplier comprising:
a transparent closed container including a light entrance portion;
a reflection type photocathode, provided in said closed container, for emitting
photoelectrons in response to an incident light transmitted through said light entrance
portion;
a transparent conductive film formed on an inside wall surface of said light entrance
portion of said closed container, a predetermined potential being applied to said
film;
an electron multiplying unit, including plural stages of dynodes, for electron-multiplying
said photoelectrons emitted from said reflection type photocathode; and
an anode for collecting said multiplied electrons.
2. A photomultiplier according to claim 1, wherein said transparent conductive film is
formed in a manner that chromium is evaporated onto said inside wall surface of said
closed container.
3. A photomultiplier according to claim 1 or 2, further comprising:
a pad adhered to said inside wall surface of said closed container so as to electrically
contact with said transparent conductive film; and
a terminal electrically contacting with said pad, a part of said terminal being
exposed to an outside of said closed container;
wherein said predetermined potential is applied through said pad and said terminal
to said transparent conductive film.
4. A photomultiplier according to any preceding claim, wherein the same negative-polarity
potential is applied and said photocathode and said transparent conductive film, a
ground potential is applied to said anode, and an appropriate potential which divides
a voltage between said negative-polarity potential and said ground potential is applied
to each of said dynodes, respectively.
5. A photomutiplier according to any preceding claim, further comprising a shield plate
provided at the rear of said photocathode, wherein an end of a light entrance side
of said photocathode is fixed to an end of a light entrance side of said shield plate.
6. A photomultiplier according to claim 1, further comprising:
a pair of insulating material substrates for supporting said photocathode, said
electron multiplying unit and said anode; and
a plate spring having a shape extending along a direction of a circumference of
said insulating material substrate, a part of said plate spring being fixed to an
end of a supporting rod of said dynode constituting said electron multiplying unit,
a part of said plate spring contacting with said inside wall of said closed container;
wherein said supporting rod and said insulating material substrate fixed to the
supporting rod are supported by and fixed to said inside wall of said closed container,
due to an elastic force of said plate spring toward an outside of said closed container
in a direction of a radius of said insulating material substrate.
7. A photomultiplier according to claim 6, wherein said transparent conductive film is
formed on a side wall of an inside of said closed wall at a area in which said transparent
conductive film does not electrically contact with said plate spring, said area including
said place corresponding to said light entrance portion.
8. A photomultiplier according to claim 1, further comprising:
a pair of insulating material substrates for supporting said photocathode, said
electron multiplying unit and said anode; and
a spring plate of which two ends are engaged with said insulating material substrates,
respectively, a middle portion of said spring plate contacting with said inside wall
of said closed container;
wherein said insulating material substrates are supported by and fixed to said
inside wall of said closed container, due to an elastic force of said spring plate
toward an outside of said closed container from a longitudinal center axis of said
closed container.
9. A photomultiplier according to claim 8, wherein said transparent conductive film is
formed on the whole of said inside wall surface of said closed container.
10. A photomultiplier comprising:
a transparent closed container including a light entrance portion;
a reflection type photocathode, provided in said closed container, for emitting
photoelectrons in response to an incident light transmitted through said light entrance
portion;
an electron multiplying unit, including plural stages of dynodes, for electron-multiplying
said photoelectrons emitted from said reflection type photocathode;
an anode for collecting said multiplied electrons; and
a pair of insulating material substrates for supporting said photocathode, said
electron multiplying unit and said anode;
wherein a middle portion of light entrance side one of a pair of supporting rods
for supporting said dynodes constituting said electron multiplying unit to said insulating
material substrates is eliminated, and a dynode constituting portion which is wound
around said supporting rod of the light entrance side is eliminated.
11. A photomultiplier according to claim 10, wherein said dynode of which said middle
portion and said dynode constituting portion are eliminated is at least the dynode
of a first stage into which said photoelectrons emitted from said photocathode enters
directly.
12. A photomultiplier in which a transparent conductive film is formed over the inner
surface of a light entrance portion of a container for the photomultiplier to receive
a photoelectron guiding potential thereon.