[0001] This invention relates to a reflection mode alkali (bialkali or multialkali) photocathode,
and a photomultiplier using it.
[0002] Conventional photocathodes are in the form of transmission mode photocathodes which
emit electrons in the direction opposite to that of the incident light, i.e., incident
photons are converted into photoelectrons and transmitted, or of reflection mode photocathodes
which emit photoelectrons towards the incident light, i.e., incident photons are converted
into photoelectrons and emitted back towards the incident light. The reflection mode
photocathode comprises a base substrate, generally of a metal. Reflection mode bialkali
photocathodes and reflection mode multialkali photocathodes having a base substrates
of nickel (Ni) are known. In the reflection mode bialkali photocathode, antimony (Sb)
is deposited on the Ni base substrate and is activated by potassium (K) and cesium
(Cs). In the multialkali photocathode, Sb is deposited on a Ni base substrate and
is activated by K, Cs and sodium (Na). The amount of Sb deposition has generally been
above 200 µg/cm
2, as will be explained below.
[0003] EP-A-05 32 358 (which falls within the terms of Article 54(3) EPC) describes a reflection
type photocathode for use in a photomultiplier tube formed by sequentially depositing
three layers on a nickel substrate. The first layer is made of chromium, manganese
or magnesium as a major component and is deposited over the substrate. The second
layer is made of aluminium as a major component and is deposited over the first layer.
The third layer is made of antimony and at least one kind of alkali metal and is deposited
over the second layer.
[0004] "S-11 and S-20 photocathode research activity" by F. Gex et al., Proc. SPIE-The International
Society For Optical Engineering, 1985, USA, SPIE vol 491, pages 287-293, described
a reflection type photocathode formed by depositing upon a glass substrate a metal
comprising aluminium and nickel amongst others. Upon this metal is deposited an antimony
activated alkali photocathode of up to 90 mm thickness.
[0005] In the above-mentioned conventional reflection mode alkali photocathodes, e.g., bialkali
photocathodes, their radiant sensitivity S
k is about 80 µA/Lm. Even in a reflection mode bialkali photocathode having an intermediate
layer between the Sb layer and the base substrate, maximum radiant sensitivity S
k is 120 µA/Lm. Here µA/Lm represents sensitivity in lumens. Lumen is a unit of luminous
flux based on visual sensitivity, and 1 Lm/m
2 = 1 Lux. The radiant sensitivity S
k corresponds to a current density of the photocathode when the intensity of incident
light is expressed in Watts.
[0006] Photomultipliers are used in the field of measuring feeble light. The beneficial
properties of the photomultiplier are apparent in the limiting case where the light
to be detected is counted in photons. Accordingly, even some small percentage of sensitivity
improvement is significant.
[0007] From this viewpoint, the inventors have found that a good reflection mode alkali
photocathode can be realized by controlling the deposition weight of Sb.
[0008] The reflection mode alkali photocathode according to this invention comprises a thin
layer of antimony deposited directly on a base substrate, and activated by a plurality
of alkali metals, in which the thin layer of antimony is deposited in an amount below
100 µg/cm
2 and activated by the alkali metals. The reflection mode alkali photocathode according
to this invention is suitably usable in photomultipliers.
[0009] In the reflection mode alkali photocathode according to this invention, the layer
of Sb activated by the alkali metals is deposited sufficiently thin. This is a drastic
change from the conventional idea embodied in conventional reflection mode photocathodes.
That is, a reduction from the 200 µg/cm
2 deposition amount of the conventional Sb layer of the conventional reflection mode
photocathode to below 100 µg/cm
2 can produce sufficiently satisfactory results.
[0010] Attempts to improve the photosensitivities of photocathodes including Sb have included
the selection of materials of the base substrate of the photocathode surface, the
improvement of the surface treatment of the photocathode, and the fabrication conditions,
such as temperature and degree of vacuum for activating the photocathode surface with
alkali metals.
[0011] The inventors have noticed that the deposition weight of Sb is completely different
from previous devices and made studies on it.
[0012] The finding is that photosensitivities of the photocathode are very dependent on
the deposition weights of Sb. Analysis by electronic balance of the deposition weights
of the Sb content of photomultipliers (hereinafter called "PMT") marketed by Hamamatsu
Photonics K.K. have shown that the deposition weights of reflection mode photocathode
of both multialkali and bialkali types are about 200 µg/cm
2.
[0013] PMTs having various Sb deposition weights were then fabricated and the deposition
weight dependency of the radiant sensitivity was studied. The finding was that the
photocathode of these PMTs have peak photosensitivies at about 40 µg/cm
2 and are superior to the conventional photocathodes.
[0014] The inventors have therefore demonstrated experimentally that sufficient radiant
sensitivity can be obtained with a Sb deposition weight range of 10 µg/cm
2 - 100 µg/cm
2. As for radiant sensitivities at below 10 µg/cm
2, by extrapolating data of the experiments, radiant sensitivities of the fabricated
PMTs more than that of the conventional PMTs can be obtained at, e.g., even some µg/cm
2. Even in the case when the base substrate of the photocathode surface is formed of
aluminium (Al), high photosensitivities can be obtained even in a range of 5 µg/cm
2 - 10 µg/cm
2.
[0015] The Sb deposition weights were quantitatively determined by the following method.
[0016] Antimony (Sb) can be deposited on a nickel plate functioning as the base substrate
by, e.g., the following method. First, a target made of Sb is placed on a heater as
the evaporation source in a vacuum vessel. Eight sheets of nickel plates are set respectively
at the same distance from the evaporation source. Then, the heater is turned on to
vaporize the Sb. Then based on a vaporizing amount of the Sb from the heater and a
distance from the evaporation source to the nickel plates, a deposition weight of
the Sb per unit area can be easily given.
[0017] The evaporation of the Sb is not always uniform in all directions, and the evaporation
of all the Sb is not assured. Accordingly it is difficult to measure an accurate deposition
weight by the above-described indirect method. Then, to improve the reliability of
the tests, the following direct method was used.
[0018] An evaporation source was prepared including a wire heater 101 and Sb target adhered
to the wire heater. The wire heater 101 was vertical as shown in FIG. 1. Eight nickel
plates 201 - 208 were set upright on a evaporation ring 102 which was rotatable around
the wire heater 101. The respective nickel plates 201 - 208 were positioned at the
same distance from the wire heater 101. A direct current was supplied to the wire
heater through electrodes 103, 104 and the evaporation ring 102 was rotated so that
the Sb was slowly evaporated. Thus the Sb could be deposited evenly on all the nickel
plates 201 - 208.
[0019] A deposition weight of the Sb was measured as follows. Weights of the 8 sheets of
nickel plates before the deposition were measured by an electronic balance type measurement
device of high precision with the zero point adjusted. Then the Sb was evaporated
by the method of FIG. 1. The deposition weight could be controlled with high precision
by adjusting the amount of solid Sb on the wire heater, and also by adjusting evaporation
times or heating temperatures with the wire heater. Then the 8 nickel plates with
the deposited Sb were measured by the electronic balance type measurement device with
the zero point adjusted.
[0020] A deposition weight of the Sb per unit area could be determined based on differences
of weights of the measured nickel plates before and after deposition, and the deposition
areas of the nickel plates. The data of FIGs. 2, 3 and 4 were thus obtained.
[0021] The base substrate, which is in direct contact with the Sb thin layer, is formed
of, e.g., Ni, Al or stainless steel. K, Ca, Rb and Na are suitable as the alkali metals.
Thus a reflection mode alkali photocathode of high radiant sensitivity can be realized
with high yields.
[0022] The present invention according to claim 1 will become more fully understood from
the detailed description given below and the accompanying drawings which are given
by way of illustration.
[0023] In the accompanying drawings.
FIG. 1 is a view of the device for evaporating Sb used by the inventors for high precision
measurement of the deposition weights of Sb;
FIG. 2 is a graph of the radiant sensitivity characteristic of one bialkali photocathode
fabricated for the tests;
FIG. 3 is a graph of the radiant sensitivity characteristic of another bialkali photocathcde
fabricated for the tests;
FIG. 4 is a graph of the radiant sensitivity characteristic of one of the multialkali
photocathode surfaces fabricated for the tests;
FIG. 5 is a side view of a side-on PMT with the glass bulb partially broken; and
FIG. 6 is a sectional view of the PMT of FIG. 5 along the line X1 - X2.
[0024] The reflection mode alkali photocathode according to this invention comprises a base
substrate of Ni, Al or stainless steel plate and a photosensitive layer containing
Sb activated by alkali metals, such as cesium (Cs), potassium (K), sodium (Na) and
rubidium (Rb). The deposition weight of Sb is below 100 µg/cm
2.
[0025] A photomultiplier having such reflection mode alkali photocathode is fabricated as
follows. A glass vacuum vessel is prepared, and Sb is evaporated on the part on which
the reflection mode photocathode is to be formed. Sb is deposited as a thin film in
a deposition weight of below 100 µg/cm
2. Subsequently when the photocathode surface portion is of a bialkali, Cs, Na and/or
K are introduced to activate the photocathode surface and the photocathode is sintered.
Temperature conditions and times for activation and sintering are known. Generally,
the temperature is selected from 140 - 220 °C.
[0026] The other components of the photomultiplier (PMT), such as dynodes, microchannel
plates, anode, etc. are mounted in the conventional prccedure. When the reflection
mode alkali photocathode is formed, and the other components are assembled the vacuum
vessel is closed, and the reflection mode alkali photocathode is finished.
[0027] One structure of a photomultiplier containing a reflection mode alkali photocathode
according to this invention is shown in FIGs. 5 and 6. As shown in FIG. 5, a glass
bulb 2 is mounted on a support 1, and stem pins 3A - 3F are provided extending downwardly
from the support 1. As shown in the sectional view along the line X
1 - X
2 of FIG. 5, the glass bulb 2 houses a cathode 4 of a nickel base substrate with a
photocathode surface formed on it, a metal mesh electrode 5 provided on the front
surface of the glass bulb 2, a circular cage-type 9-stage dynodes 61 - 69, and an
anode 7. In this PMT light passing the metal mesh electrode 5 enters the cathode 4.
Photoelectrons thus emitted impinge on the respective dynodes 61, 62, ..., ..., 68,
69 one after another, and the number of electrons is rapidly increased by the emission
of secondary electrons. Then all the electrons are collected by the anode 7 and are
transmitted as electric signals through one of the stem pins 3A - 3F.
[0028] Next, examples of fabrication for tests of the bialkali photocathode surface will
be explained. In all the examples the conditions, such as temperatures, vacuum degrees,
times, etc. are the same irrespective of deposition weights of Sb. In the examples,
base substrates were Ni plates having their surfaces (weakly) oxidized, and Sb layers
were formed on the washed oxidized surfaces.
[0029] In the examples, the Sb layers were deposited in 6 different thicknesses (deposition
weights) from 15 - 230 µg/cm
2. Then K and Cs were introduced to activate the Sb layers to obtain a bialkali (K-Cs-Sb)
photocathode. Twenty photocathode surfaces (totally 120) were prepared at the respective
set deposition weights.
[0030] The sample photocathode surfaces exhibited the radiant sensitivity characteristic
of FIG. 2. The average luminous sensitivity was below about 80(µA/1m) at a deposition
weight of Sb of above 100 µg/cm
2. At a deposition weight of 20 - 80 µg/cm
2, the average luminous sensitivity was above 115 (µA/1m).
[0031] As apparent in FIG. 2, the deposition of Sb in 40 µg/cm
2 provides especially good improvement of the radiant sensitivity. The sample photocathode
surfaces exhibited a maximum value of 193 µA/1m. A 150 µA/1m radiant sensitivity could
be stably realized. This high sensitivity widely ranged from near infrared radiation
to ultraviolet radiation.
[0032] Furthermore, there were fabricated for test bialkali photocathode surfaces, using
nickel, stainless steel and aluminium as the base substrates, and potassium, cesium,
rubidium, etc. as the alkali metals.
[0033] Sample A: A nickel plate having the surface weakly oxidized was used, and K-Cs were
used as the alkali metals.
[0034] Sample B: A nickel plate having the surface nonoxidized, and K-Cs were used as the
alkali metals.
[0035] Sample C: A nickel plate having the surface oxidized, and Rb-Cs were used as the
alkali metals.
[0036] Sample D: A stainless steel (non-magnetic material) plate which had undergone no
oxidizing step, and K-Cs were used as the alkali metals.
[0037] Sample E: An aluminium plate which had undergone no oxidizing step, and K-Cs were
used as the alkali metals.
[0038] Five PMTs were prepared for each of 10, 20, 50, 80 and 160 µg/cm
2 Sb deposition weights of each of Samples A, B, D and E. Three PMTs were prepared
for each cf the above-stated Sb deposition weights for Sample C. Average radiant sensitivities
were determined.
[0039] The results are shown in FIG. 3. As shown in FIG. 3, in the cases where the base
substrates are formed of nickel or stainless steel, high radiant sensitivities can
be obtained at an Sb deposition weight of 10 - 100 µg/cm
2. In the case where the base substrate is formed of aluminium, a high sensitivity
can be obtained at 5 - 100 µg/cm
2.
[0040] In further examples the base substrates were Al plates having Al deposited on the
surfaces, and Sb layers were deposited on the washed surfaces of the Al plates.
[0041] In the examples, the Sb layers were deposited in 7 different thicknesses (deposition
weights) from 15 - 205 µg/cm
2. Then Na, K, Cs were introduced to activate the Sb layers to obtain multialkali (Cs-Na-K-Sb)
photocathodes. Five photocathodes (totally 35) were prepared at the respective deposition
weights.
[0042] The sample photocathode surfaces exhibited the radiant sensitivity characteristic
of FIG. 4. The average luminous sensitivity was below about 120 (µA/1m) at a deposition
weight of Sb of above 100 µg/cm
2. At a deposition weight of 20 - 8C µg/cm
2, the average luminous sensitivity was above 140 - 150 (µA/1m).
[0043] As apparent in FIG. 4, the deposition weight of Sb of about 40 µg/cm
2 can attain especially good improvement of the radiant sensitivities. In the examples,
radiant sensitivities of about 200 µA/1m can be stably realized. The high radiant
sensitivities widely range from the near infrared to the ultraviolet. It is apparent
from the examples and the test results that base substrates of nickel, stainless steel,
aluminium or others can be used as the multialkali photocathode surfaces.
[0044] The alkali photocathode according to this invention includes the Sb layer in a deposition
weight of below 100 µg/cm
2, whereby reflection mode alkali photocathode of a high sensitivity can be realized
with high yields. As alkali metals used in the photocathode surface according to this
invention, some elements other than cesium, potassium, rubidium and sodium are available.
As the base substrate of the photocathode surface according to this invention, some
metals other than aluminium, nickel and stainless steel are available. Although the
inventors have not obtained experimental data on all combinations of these materials,
the results of their experiments on combinations of typical materials showed characteristics
commcn to the experiments, i.e., the Sb depositicn weight dependency of the radiant
sensitivity as shown in FIGs. 2-4.