[0001] This invention relates to a reflection mode alkali (bialkali or multialkali) photocathode,
and a photomultiplier using the same.
[0002] In conventional photocathode, there are a transmission mode photocathode which emits
electrons to the side opposite to a side of light incidence, i.e., converts incident
photons into photoelectron and transmits the photoelectron, and the reflection mode
photocathode which emits photoelectron to the side of light incidence, i.e., converts
incident photons into photoelectron and emits the photoelectron back to the side of
light incidence. The reflection mode photocathode comprises the base substrate mainly
of a metal. The reflection mode bialkali photocathode and reflection mode multialkali
photocathode having the base substrates of nickel (N) are known. In the reflection
mode bialkali photocathode, antimony (Sb) is deposited on a Ni base substrate and
is activated by alkali metals of potassium (K) and cesium (Cs) . In the multialkali
photocathode surface as well, Sb is deposited on a Ni base substrate and is activated
by K, Cs and sodium (Na). The Sb deposition amount has been generally above 200 µg/cm²
as will be explained later.
[0003] In the above-mentioned conventional reflection mode alkali photocathode, e.g., bialkali
photocathode, their radiant sensitivity is about S
k = 80 µA/Lm. Even in a reflection mode bialkali photocathode having an intermediate
layer between the Sb layer and the base substrate, its radiant sensitivity is S
k = 120 µA/Lm at maximum. Here µA/Lm represents a sensitivity in the unit of lumen.
Lumen is a unit of luminous flux based on the visual sensitivity, and 1 Lm/m² = 1
Lux. The radiant sensitivity S
k corresponds to a current density of the photocathode given when an intensity of incident
light is expressed by Watts.
[0004] The photomultiplier is used in the field of measuring feeble light. Properties of
the photomultiplier is exhibited in the limit region where light to be detected is
counted in photons. Accordingly even some percentage of sensitivity improvement is
significant.
[0005] Form this viewpoint, we, the inventors, made studies, and find that a good reflection
mode alkali photocathode can be realized by controlling a deposition weight of Sb.
[0006] The reflection mode alkali photocathode according to this invention comprises a thin
layer of antimony deposited on a base substrate, and activated by a plurality of kinds
of alkali metals, in which the thin layer of antimony being deposited in an amount
below 100 µg/cm² and activated by the alkali metals. The reflection mode alkali photocathode
according to this invention is suitably usable in photomultipliers.
[0007] In the reflection mode alkali photocathode according to this invention, the thin
layer of Sb activated by the alkali metals is deposited sufficiently thin. This is
a drastic change of a conventional idea involved in the conventional reflection mode
photocathode. That is, a reduction of a 200 µg/cm² deposition amount of the conventional
Sb layer of the conventional reflection mode photocathode µg/cm² to below 100 µg/cm²
can produce sufficiently satisfactory results.
[0008] To improve photosensitivities of the photocathode including Sb, the selection of
materials of the base substrate of the photocathode surface, the improvement of the
surface treatment of the photocathode, and the fabrication conditins, such as temperatures
and degrees of vacuum for activating the photocathode surface with alkali metals are
tried.
[0009] But we, the inventors, notice the deposition weight of Sb which is means completely
different from the above-mentioned means, and made studies on it. We, the inventors
believe that nobody has studied this means nor published results of his studies. Our
finding is that photosensitivities of the photocathode is very dependent on deposition
weights of Sb. First, they analyze by an electron balance the deposition weights of
the Sb of photomultipliers (hereinafter called "PMT") marketed by Hamamatsu Photonics
K.K. The results of their analyses show that the deposition weights of the reflection
mode photocathode of both multialkali and bialkali types are about 200 µg/cm².
[0010] Then, we, the inventors, fabricated for tests PMTs having various Sb deposition weights
and studied the deposition weight dependency of the radiant sensitivity. Our finding
is that the photocathode of these PMTs have peak photosensitivies at about 40 µg/cm²
and are superior to the conventional photocathode.
[0011] That is, we have experimentally proved that sufficient radiant sensitivities can
be obtained in a Sb deposition weight range of 10 µg/cm² - 100 µg/cm². As for radiant
sensitivities at below 10 µg/cm², we find out, by extrapolating data of the experiments,
that radiant sensitivities of the fabricated PMTs more than that of the conventional
PMTs can be obtained at, e.g., even some µg/cm². Especially in the case the base substrate
of a photocathode surface is formed of aluminium (Al), high photosensitivities can
be obtained even in a range of 5 µg/cm² - 10 µg/cm².
[0012] The Sb deposition weights were quantitatively determined by the following method.
[0013] 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 a unit area can be easily given.
[0014] The evaporation of the Sb is not always uniform in all the directions, and the evaporation
of all the Sb is not secured. Accordingly it is difficult to measure an accurate deposition
weight by the above-described indirect method. Then, to improve the reliability of
the tests, we, the inventors, used the following direct method.
[0015] A evaporation source including a wire heater 101 and Sb target adhered to the wire
heater 101 in a uniform thickness was prepared. The wire heater 101 was set 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 101 through electrodes 103, 104 with the evaporation
ring 102 set on rotation, so that the Sb was slowly evaporated. Thus the Sb could
be deposited evenly on all the nickel plates 201 - 208.
[0016] 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 electron balance type measurement
device of high precision with the zero point adjusted. Then the Sb was evaporated
by the method of FIG. 1. A deposition weight could be controlled with high precision
by adjusting a deposition amount of the solid Sb to the wire heater, and also by adjusting
evaporation times or heating temperatures with the wire heater with the same adhesion
amount. Then the 8 nickel plates with the Sb adhered to were measured by the electron
balance type meausrement device with the zero point adjusted.
[0017] A deposition weight of the Sb per a unit area could be determined based on differences
of weights of the measured nickel plates between before and after the deposition,
and deposition areas of the nickel plates. The data of FIGs. 2, 3 and 4 were thus
obtained.
[0018] It is preferred that 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.
[0019] 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.
[0020] 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 form this detailed description.
[0021] FIG. 1 is a view of the device for evaporating Sb used by the inventors of this invention
for high precision of measuring the deposition weights of the Sb.
[0022] FIG. 2 is a graph of the radiant sensitivity characteristic of one bialkali photocathode
fabricated for the tests.
[0023] FIG. 3 is a graph of the radiant sensitivity characteristic of another bialkali photocathode
fabricated for the tests.
[0024] FIG. 4 is a graph of the radiant sensitivity characteristic of one of the multialkali
photocathode surfaces fabricated for the tests.
[0025] FIG. 5 is a side view of a side-on PMT with the glass bulb partially broken.
[0026] FIG. 6 is a sectional view of the PMT of FIG. 5 along the line X₁ - X₂.
[0027] This invention will be explained below in more detail. The reflection mode alkali
photocathode according to this invention comprises a base substrate of Ni or others,
and a photosensitive layer containing Sb activated by alkali metals, such as cesium
(Cs), potassium (K), sodium (Na) and rubidium (Rb). A deposition weight of the Sb
is below 100 µg/cm².
[0028] A photomultiplier having such reflection mode alkali photocathode is fabricated as
follows. A glass vacuum vessel is prepared, and Sb is evaporated on a part for the
reflection mode photocathode to be formed on. Sb is deposited as a thin film in deposition
weight of a below 100 µg/cm², or a porous film. Subsequently when in the photocathode
surface portion made of a bialkali, Cs, Na, K are introduced to activate the photocathode
surface portion, and the photocathode is sintered. Temperature condicitons and times
for the activation and the sintering are set suitably as known. Incidentally a temperature
is selected from 140 - 220 °C.
[0029] The other members of a photomultiplier (PMT), such as dynodes, microchannel plates,
an anode, etc. are mounted in the conventional procedure. When the reflection mode
alkali photocathode is formed, and the members are mounted, the vacuum vessel is closed,
and the reflection mode alkali photocathode is finished.
[0030] A structure of a photomultiplier having the 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 downwardly on the support
1. As in the sectional view along the line X₁ - X₂ of FIG. 5, the glass bulb 2 houses
a cathode 4 of a nickel base substrate with a photocathode surface formed on, 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. Photoelectron thus emitted impinge on the respective
dynodes 61, 62, ..., ..., 68,69 one after another, and a number of the electrons is
rapidly increased by the emission of secondary electrons. Then all the electrons are
collected by the anode 7 and are taken outside as electric signals through one of
the stem pins 3A - 3F.
[0031] 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 the surfaces (weakly) oxidized, and Sb layers
were formed on the rinsed oxidized surfaces.
[0032] In the examples, the Sb layers were deposited in 6 different thicknesses (deposition
weights) from 15 - 230 µg/cm². Then K, 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.
[0033] The sample photocathode surfaces exhibited the radiant sensitivity characteristic
of FIG. 2. An average luminous sensitivity is below about 80(µA/1m) at a deposition
weight of Sb of above 100 µg/cm². At a deposition weight of 20 - 80 µg/cm², an average
luminous sensitivity is above 115 (µA/1m).
[0034] As apparent in FIG. 2, the deposition of Sb in 40 µg/cm² provides especially much
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 the near infrared radiation to the ultraviolet
radiation.
[0035] Furthermore, the inventors 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.
[0036] Sample A: A nickel plate having the surface weakly oxidized was used, and K-Cs was
used as the alkali metals.
[0037] Sample B: A nickel plate having the surface non-oxidized, and K-Cs was used as the
alkali metals.
[0038] Sample C: A nickel plate having the surface oxidized, and Rb-Cs was used as the alkali
metals.
[0039] Sample D: A stainless steel (non-magnetic material) plate which has undergone no
oxidizing step, and K-Cs was used as the alkali metals.
[0040] Sample E: An aluminium plate which has undergone no oxidizing step, and K-Cs was
used as the alkali metals.
[0041] Five PMTs were prepared for each of 10, 20, 50, 80 and 160 µg/cm² Sb deposition weights
of each of Samples A, B, D and E. Three PMTs were prepared for each of the above-stated
Sb deposition weights for Sample C. Average radiant sensitivities were determined.
[0042] The results are shown in FIG. 3. As shown in FIG. 3, in the cases that the base substrates
are formed of nickel and stainless steel, high radiant sensitivities can be obtained
at an Sb deposition weight of 10 - 100 µg/cm². In the case that the base substrate
is formed of aluminium, a high sensitivity can be obtained at 5 - 100 µg/cm².
[0043] Then samples of the multialkali photocathode surface will be explained. In the samples,
the base substrates were Al plates having Al deposited on the surfaces, and Sb layers
were deposited on the rinsed surfaces of the Al plates.
[0044] In the examples, the Sb layers were deposited in 7 different thicknesses (deposition
weights) from 15 - 205 µg/cm². Then Na, K, Cs were introduced into to activate the
Sb layers to obtain a multialkali (Cs-Na-K-Sb) photocathode. Five photocathode (totally
35) were prepared at the respective set deposition weights.
[0045] The sample photocathode surfaces exhibited the radiant sensitivity characteristic
of FIG. 4. An average luminous sensitivity is below about 120 (µA/1m) at a deposition
weight of Sb of above 100 µg/cm². At a deposition weight of 20 - 80 µg/cm², an average
luminous sensitivity is above 140 - 150 (µA/1m).
[0046] As apparent in FIG. 4, the deposition weight of Sb in about 40 µg/cm² can attain
especially much improvement of the radiant sensitivities. In the samples, radiant
sensitivities of about 200 µA/1m can be stably realized. The high radiant sensitivities
widely range from the near infrared radiation to the ultraviolet radiation. It is
apparent from the examples and the test results that base substrates of nickel, stainless,
aluminium or others can be used in the multialkali photocathode surface.
[0047] The alkali photocahode according to this invention includes the Sb layer in the deposition
weight of below 100 µg/cm², whereby reflection mode alkali photocathode of a high
sensitivity can be realized with high yields. As alakli 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 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 common to the experiments, i.e., the Sb deposition weight dependency
of the radiant sensitivity as shown in FIGs. 1 - 3.
[0048] Accordingly the photocathodes which are formed of not only the experimentally proved
materials, but also of materials equivalent to these materials, and which have Sb
deposition weights of below 100 µg/cm² are included in the coverage of this invention.
[0049] 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.