U.S. patent number 3,808,494 [Application Number 05/243,893] was granted by the patent office on 1974-04-30 for flexible channel multiplier.
This patent grant is currently assigned to Matsushita Electric Industrial Co., Ltd.. Invention is credited to Masashi Hashimoto, Tomonao Hayashi, Hiroshi Moriga, Toshio Shimizu, Wataru Shimotsuma, Kazumasa Yamamoto.
United States Patent |
3,808,494 |
Hayashi , et al. |
April 30, 1974 |
FLEXIBLE CHANNEL MULTIPLIER
Abstract
A flexible channel secondary electron multiplier tube for use in
detector of a mass spectrometer, a detector for the photons and
charged particles in the cosmic space and an image intensifier,
which is made up of electron-conductive polymers having a secondary
electron emitting effect and which, therefore, can easily be
produced by extrusion molding and which do not require the inner
surface thereof to be coated with a secondary electron emitting
substance. The secondary electron emission coefficient .delta. of
the tube is 2.0 with respect to primary electron of 250 eV, and the
gain thereof is higher than that of conventional glass tube channel
secondary electron multipliers. The tube can be used by bending it
at an optional curvature so as to eliminate the undesirable
influence of ion feedback, and can be produced at a lower cost than
a conventional one.
Inventors: |
Hayashi; Tomonao (Munashino,
JA), Hashimoto; Masashi (Tokyo, JA),
Yamamoto; Kazumasa (Toyonska, JA), Shimotsuma;
Wataru (Osaka, JA), Moriga; Hiroshi (Mortiguchi,
JA), Shimizu; Toshio (Daito, JA) |
Assignee: |
Matsushita Electric Industrial Co.,
Ltd. (Osaka, JA)
|
Family
ID: |
26333671 |
Appl.
No.: |
05/243,893 |
Filed: |
April 13, 1972 |
Related U.S. Patent Documents
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Application
Number |
Filing Date |
Patent Number |
Issue Date |
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887052 |
Dec 22, 1969 |
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Foreign Application Priority Data
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Dec 27, 1968 [JA] |
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43-654 |
Dec 27, 1968 [JA] |
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43-656 |
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Current U.S.
Class: |
313/103R;
252/500; 252/511; 252/514; 313/105R; 313/103CM; 313/105CM |
Current CPC
Class: |
H01J
49/025 (20130101); H01J 43/24 (20130101); G01T
1/28 (20130101) |
Current International
Class: |
H01J
49/02 (20060101); H01J 43/00 (20060101); H01J
43/24 (20060101); G01T 1/28 (20060101); G01T
1/00 (20060101); H01j 043/22 (); H01j 043/24 () |
Field of
Search: |
;313/95,103,104,105 |
References Cited
[Referenced By]
U.S. Patent Documents
Foreign Patent Documents
Other References
Chem. Abstracts, Vol. 70, 1969.
|
Primary Examiner: Segal; Robert
Attorney, Agent or Firm: Stevens, Davis, Miller &
Mosher
Parent Case Text
This is a continuation of application Ser. No. 887,052, filed Dec.
22, 1969, now abandoned.
Claims
1. A flexible channel secondary electron multiplier comprising at
least one flexible pipe fixed in an arcuate shape as a unitary
piece, said at least one pipe having a conically or
pyramidally-shaped injection port, said pipe and injection port
being molded of a composition comprising at least one thermosetting
resin selected from the group consisting of polyvinyl chloride and
polyethylene having a large secondary electron emission coefficient
and at least one selected from the group consisting of an
electron-conductive charge transfer complex and carbon black, said
composition thus possessing a volume resistivity no greater than
3.0 .times.10.sup.10 ohm-cm and wherein said electron-conductive
charge transfer complex is a salt selected from the group
consisting of potassium-tetracyano-paraquinodimethane,
sodium-tetracyano-paraquinodimethane,
lithium-tetracyano-paraquinodimethane and
polyvinylpyridine-tetracyano-paraquinodimethane.
Description
The present invention relates to a flexible channel secondary
electron multiplier tube which is adapted for use in the detector
of a mass spectrometer, the detector of a device for measuring low
energy ions or electrons from cosmic space which is mounted in an
artificial satellite or space observation rocket, an image
intensifier or the like.
A secondary electron multiplier tube, when supplied with photons,
ions or electrons as an input, readily emits secondary electron and
amplifies them in a stable condition, and hence is applicable to
such an apparatus which measures or indicates a faint input signal
by amplifying the same. The flexible channel secondary electron
multiplier tube has the property of conducting electrons and is
produced by extrusion-molding a polymer composition, having a
secondary electron emission coefficient .delta. greater than 1,
into a tubular shape. By suitably selecting the electric field to
be applied, a gain of 10.sup.6 or greater can easily be
obtained.
The polymer compound of the type described itself has a secondary
emitting effect and has substantially the same processability,
moldability and flexibility as those of the commonly used plastics.
Therefore, the flexible channel secondary electron multiplier tube
can be produced very easily by simply molding the polymer
composition into a tubular shape, it being unnecessary to coat the
inner wall of the tube with an electron emitting substance. As
compared with a glass-made channel multiplier, the flexible channel
secondary electron multiplier tube of a polymer composition has the
advantages that it can be processed more easily and is more
resistive to shock and that it can be used by fixing at a curvature
at which the multiplying efficiency is highest. Furthermore, it is
not inferior to the glass-made multiplier tube in multiplication
gain.
Conventional channel multipliers are classified into parallel plate
multipliers and capillary multipliers. The parallel plate
multiplier is also called a continuous dynode multiplier and
comprises, as shown in FIG. 1 mentioned later, quartz plates of a
size, for example, of 25.4 mm in length, 9.5 mm in width and 1 mm
in thickness, arranged in parallel relation at an interval of 0.3
mm and each being coated with a film of a resistance of the order
of 10.sup.9 .OMEGA. which is formed by evaporation-depositing
alumina and molybdenum.
In this figure, numeral 1 designates a thus formed dynode, 2 a
collector, 3 an ammeter for output current and 4 an input current
path. The secondary electron emission coefficient .delta. is
normally 2.45 with respect to a primary electron of 150 eV. The
gain changes with the voltage impressed, which is shown as a
continuous dynode characteristic in FIG. 9 also mentioned later.
When a direct-current voltage of 3,000 V is impressed on the
dynodes, the gain is about 5 .times. 10.sup.5. This multiplier has
the drawback that, while the secondary electron emission
coefficient .delta. is large, the gain is small and further the
operation is unstable by reason of the positive feedback process
caused by using parallel plates.
The glass-made capillary multiplier has been developed for the
purpose of directly surveying the exosphere by mounting it on a
rocket or artificial satellite, by taking advantage of its high
gain, small size, light weight and simplicity. However, the most
serious drawbacks of this system are that it is extremely difficult
to coat on the inner surface of the fine pipe a resistance film on
the order of 10.sup.9 .OMEGA. which has a stable secondary electron
emitting effect, and that it is easily subject to breakage even
under a slight shock. The construction of the capillary multiplier
is shown in FIG. 2 mentioned later, in which numeral 5 designates a
glass tube, 6 resistance coating, 7 a secondary electron track, and
8 injected ion, and the gain characteristic thereof is shown as a
capillary multiplier characteristic in FIG. 9. The secondary
electron emission coefficient .delta. of the capillary multiplier
is 2.50 with respect to a primary electron of 150 eV. The gain of
the multiplier when impressed with an acceleration voltage of 3,000
V is 5.0 .times. 10.sup.7.
According to the present invention, a capillary second electron
multiplier can be obtained, simply by molding a polymer composition
into a tubular shape which has a secondary electron emitting
effect, and the multiplier thus obtained can be used by curling and
fixing it at a curvature at which the gain is highest, by taking
advantage of the flexibility of the material.
The aforesaid moldable and flexible secondary electron emission
polymer composition can be produced by any one of the following
three processes:
1. A charge transfer complex consisting of metals in Group I of the
Periodic Table or onium compounds as electron donor and
tetracyanoparaquinodimethane or tetracyanoethylene as electron
acceptor, has excellent secondary electron emitting effect and is
capable of conducting electrons. An organic charge transfer complex
is fully compatible and can homogeneously be blended with
thermoplastic or thermosetting resins. A moldable and flexible
secondary electron emitting polymer composition having a large
secondary electron emission coefficient .delta. can be produced by
blending such an organic charge transfer complex having a high
secondary electron emitting effect with a matrix polymer.
2. The polymeric charge transfer complex consisting of
poly-2-vinylpyridine as donor and tetracyanoparaquinodimethane as
acceptor, has a secondary electron emission coefficient .delta. of
2.0 or greater and is electron-conductive, the volume resistivity
being 2.0 .times. 10.sup.10 .OMEGA. cm. This polymeric charge
transfer complex is moldable but poor in flexibility. Therefore, by
copolymerizing vinylpyridine with styrene, ethylacrylate, etc., a
flexible polymeric charge transfer complex can be synthetized.
A secondary electron emitting polymer composition can be produced
by using this polymeric charge transfer complex along or by
blending it with other polymers for the purpose of further
improving the moldability and flexibility.
3. Polyethylene, polystyrene, polyvinyl chloride and epoxy resin
which are insulating polymers, have a secondary electron emitting
effect and are moldable and flexible. Therefore, these compounds
can easily be molded into a multiplier tube. However, the
multiplier tube thus produced does not show a stable multiplying
effect because it is charged in a positive polarity due to the lack
of electrons which will result upon emitting secondary electrons.
Therefore, a secondary electron emitting polymer composition can be
produced by adding carbon black or a fine metal powder to the
insulating polymers for the purpose of imparting conductivity
thereto.
The secondary electron multipliers made of the secondary electron
emitting polymer compositions produced by the processes described
above are believed to be much superior to the glass-made capillary
secondary electron multipliers in the following six points:
1. The structural material itself has the property of emitting
secondary electrons.
2. They can be produced in large quantities and with a uniform
quality.
3. The production cost is low.
4. Owing to their flexibility, they can be used at an optional
curvature and hence stable operation can be obtained.
5. They have great mechanical strengths and are highly resistant to
shock.
6. The available percentage is high. Gain characteristics for
channel multiplier is high.
The present invention will appear more clearly from the following
detailed description when taken in conjunction with the
accompanying drawings, showing the examples of the invention, in
which:
FIGS. 1 and 2 are diagrams showing the theoretical structures of
conventional multipliers, the former being a view of a continuous
dynode multiplier and the latter being a view of a capillary
multiplier;
FIG. 3 is a set of views showing the structure of an embodiment of
the flexible channel multiplier of the present invention, in which
FIG. 3a shows an input cone for ions or electrons and FIG. 3b shows
a side elevation;
FIGS. 4 and 5 are sets of views showing other embodiments of the
flexible channel multiplier of the invention respectively, in which
FIGS. 4a and 5a show input cones for ions or electrons and FIGS. 4b
and 5b shows the side elevations of the respective multipliers;
FIG. 6 is a diagram exemplifying the use of a flexible channel
multiplier, similar to those shown in FIG. 4, which is formed in a
spiral shape;
FIG. 7 is a diagram showing an experimental arrangement in counting
mode;
FIG. 8 is an output wave-form diagram of the multiplier of FIG. 3
in the single electron injection;
FIG. 9 is a diagram showing in comparison the relationships between
the acceleration voltage and the gain, of the present flexible
channel multiplier and the conventional one;
FIG. 10 is a diagram showing the relationship between the primary
electron energy and the secondary electron emission coefficient
.delta., of the flexible channel multiplier of Example 5; and
FIG. 11 is a diagram showing the relationship between the
acceleration voltage and the gain, of the multiplier of Example
5.
The flexible channel secondary electron multipliers according to
the present invention are produced by molding flexible secondary
electron emitting polymer compositions having a large secondary
electron emission coefficient into the shapes described in the
following examples at a suitable temperature and under a suitable
pressure, by extrusion-molding, injection-molding or casting
methods. These flexible channel secondary electron multipliers are
respectively so designed as to incrase the gain, to elimiate the
undesirable effect of ion feedback and to enhance the collection
efficiency. The secondary electron emitting polymer composition
used in Examples 1--4, illustrated hereinafter, has the following
composition:
Lithium-tetracyano-paraquinodimethane-- 35 g.
Polyvinyl chloride (PVC) (Average
polymerization degree 1,200)--30 g.
Stabilizer (equivalent mixture of
tribasic lead sulfate and Cd-Ba type
stabilizer)--5 g.
Low molecular weight polyurethane
(Ultramole PU of Bayer)--30 g.
After weighing precisely, the component materials were thoroughly
blended for 30 minutes in a ribbon blender, while maintaining them
at a temperature of 60.degree. C. and successively thereafter the
blend was kneaded for 10 minutes on a mixing roll heated at a
temperature of 165.degree. - 170.degree. C. and taken out in the
shape of a sheet. The sheet material thus obtained was pelletized
by a pelletizer and used as a sample in the respective
Examples.
Example 1
The flexible secondary electron emitting polymer composition was
continuously molded into a tube by extrusion molding under the
conditions of a temperature of 180.degree. C. and a pressure of 200
kg/cm.sup.2, and the tube was cut in a length of 100 mm. The pipe
thus obtained had an inner diameter of 1 mm, an outer diameter of 2
mm and a total length of 100 mm as shown in FIG. 3. The electric
resistance of the pipe across the opposite ends thereof was 6.0
.times. 10.sup.11 .OMEGA. at room temperature and the secondary
electron emission coefficient .delta. thereof was 2.0 with respect
to a primary electron having an energy of 300 eV. These
measurements were taken by fixing the pipe at a radius of curvature
of 30 mm upon bending.
Example 2
The flexible secondary electron emitting polymer composition was
molded by extrusion-molding under the conditions of a temperature
of 180.degree. C. and a pressure of 200 kg/cm.sup.2 into a pipe of
the shape as shown in FIG. 4, which consists of a conical input
cone of 10 mm in diameter and 15 mm in depth and a tube of 1 mm in
inner diameter and 2 mm in outer diameter connected with each other
integrally.
The electric resistance of the pipe across the opposite ends
thereof at room temperature was 6.5 .times. 10.sup.11 .OMEGA. and
the secondary electron emission coefficient thereof was 2.0 with
respect to a primary electron having an energy of 300 eV. These
measurements were taken by fixing the pipe at a radius of curvature
of 30 mm upon bending.
Example 3
The flexible secondary electron emitting polymer composition was
molded by extrusion molding under the conditions of a temperature
of 180.degree. C. and a pressure of 200 kg/cm.sup.2, into a pipe of
the shape as shown in FIG. 5, which consists of a pyramidal input
cone of 10 .times. 4 mm in bottom surface area, 15 mm in height and
0.5 mm in thickness and a tube of 2 mm in outer diameter and 1 mm
in inner diameter, connected with each other integrally, and has a
total length of 115 mm. The electric resistance of the pipe across
the opposite ends thereof at room temperature was 6.5 .times.
10.sup.11 .OMEGA. and the secondary electron emission coefficient
was 2.0 with respect to a primary electron having an energy of 300
eV. These measurements were taken by fixing the pipe at a radius of
curvature of 30 mm upon bending.
Example 4
A multiplier which is the same as that of Example 2 except that the
length of the tube was 150 mm, was molded and fixed upon bending it
three turns at a radius of curvature of 5 mm into a spiral shape as
shown in FIG. 6, for use as a secondary electron multiplier, in
which the upper arrow mark indicates an injection part for
electrons and ions and the lower arrow marks indicate connection
with a synchroscope.
The electric resistance of the multiplier across the opposite ends
thereof was 9.0 .times. 10.sup.11 .OMEGA. at room temperature and
the secondary electron emission coefficient thereof with respect to
a primary electron having an energy of 300 eV was 2.0.
The construction of a measuring circuit, using the flexible channel
secondary electron multiplier of Example 1, is shown in FIG. 7. The
multiplier tube used had a total length L of 100 mm, an inner
diameter r.sub.i of 1 mm, an outer diameter r.sub.o of 2 mm and a
radius of curvature r.sub.c of 30 mm. In addition the arrow mark 9
indicates the flexible channel multiplier, 10 incident electrons
and 11 connection with a synchroscope. The resistance value of the
tube across the opposite ends thereof was 1 .times. 10.sup.9
.OMEGA.. The tube was connected to a direct-current source Va of a
voltage of 3,000 V through a load resistance (R.sub.L) of 50
.OMEGA.. Character C.sub.c designates a coupling condenser, the
electrostatic capacity of which is 0.01 .mu.F. While maintaining
the multiplier tube in a vacuum atmosphere of 1 .times.
10.sup.-.sup.6.sub. Torr, a faint electron stream of the order of
10.sup.-.sup.18 A having an energy of 300 eV was fed as an input
and the output was taken out from a cable which was connected to
the output end of the tube through the coupling condenser C.sub.c.
A voltage change corresponding to the output current was read by a
synchroscope through a 50.OMEGA. load resistance R.sub.L '. As will
be clear from FIG. 8, in which one scale represents 40 mV on the
axis of ordinates and one scale 10 n sec. on the axis of abscissa,
it was found that a pulse output of a width of about 30 n sec. can
be obtained for one electron injected, in case of the acceleration
voltage being 3,000 V. By calculating the area surrounded by the
output waveform, the gain of the multiplier tube can be obtained.
The curve of Example 1 in the diagram of FIG. 9 shows the
relationship between the thus obtained gain and the acceleration
voltage. In this case, a suitable value of the acceleration voltage
is in the proximity of 3,000 V because the expansion of pulse
height distribution is relatively small. The gain in this case was
6.0 .times. 10.sup.8. The gains of Examples 2, 3 and 4 were 7.0
.times. 10.sup.8, 6.5 .times. 10.sup.8 and 8.0 .times. 10.sup.8
respectively.
In Examples 2, 3 and 4, it was ascertained that the collecting
effect was enhanced due to the fact that the input ends of the
respective multiplier tubes are shaped in a trumpet-like
configuration. In Example 4, it is evident that the gain is
improved.
Other polymer compositions which are also suitable for use in the
production of the present secondary electron multiplier will be
described hereinafter:
Example 5
A mixture consisting of
Sodium-tetracyano-paraquinodimethane-- 35 g.
Polyvinyl chloride (PVC) (Average
polymerization degree 1,200)--45 g.
Low molecular weight polyurethane
(Ultramole PU of Bayer)--55 g.
Stabilizer (equivalent mixture of
tribasic lead sulfate and Cd-Ba
type stabilizer)--10 g.
was sufficiently agitated in a ribbon blender for about 30 minutes
at a temperature of 60.degree.C. Successively thereafter, the
mixture was kneaded on a hot roll heated at 165.degree. -
170.degree. C. and taken out in the form of a sheet having a
thickness of about 1 mm. The sheet was pelletized by a pelletizer.
Using the resultant pellets, a tube was molded continuously at a
temperature of 180.degree. C. under a pressure of 60 kg/cm.sup.2 by
an extruder of 1 mm in inner diameter and 2 mm in outer diameter,
and a multiplier having an inner diameter of 1 mm, an outer
diameter of 2 mm and a total length of 100 mm was obtained from the
tube. The electric resistance of the multiplier across the opposite
ends thereof was 6.5 .times. 10.sup.11 .OMEGA. at room temperature
and the secondary electron emission coefficient .delta. thereof was
2.0.
Example 6
A mixture consisting of
Potassium-tetracyano-paraquinodimethane-- 35 g.
Polyvinyl chloride (PVC) (Average
polymerization degree 1,200)--30 g.
Stabilizer (equivalent mixture of
tribasic lead sulfate and Cd-Ba
type stabilizer)--5 g.
Low molecular weight polyurethane
(Ultramole PU of Bayer)--30 g.
was sufficiently agitated in a ribbon blender for about 30 minutes
at a temperature of 60.degree. C. Successively thereafter, the
mixture was kneaded for about 10 minutes on a hot roll at a
temperature of 165.degree. - 170.degree. C. and taken out in the
form of a sheet having a thickness of about 1 mm. The sheet was
pelletized by a pelletizer and using the resultant pellets, a tube
was molded continuously at a temperature of 180.degree. C. under a
pressure of 60 kg/cm.sup.2 by an extruder having an inner diameter
of 1 mm and an outer diameter of 2 mm. A multiplier tube having an
inner diameter of 1 mm, an outer diameter of 2 mm and a total
length of 10 cm was obtained from the tube. The electric resistance
of the tube across the opposite ends thereof was 5.0 .times.
10.sup.11 .OMEGA. at room temperature and the secondary electron
emission coefficient .delta. thereof was 2.2.
Example 7
A styrene-ethylacrylate-2-vinylpyridine copolymer (at a ratio of
40-40-20) was dissolved in toluene and quaternarized by the
addition of hydriodic acid in an amount 1.5 times the mol number of
the 2-vinylpryridine. The hydriodic acid-quaternarized
styrene-ethylacrylate-2-vinylpyridine copolymer was dissolved in
acetonitrile and reacted with
lithium-tetracyano-paraquinodimethane, to form a charge transfer
complex. This complex is high flexible and moldable, and is
electron-conductive, the volume resistivity being 5.0 .times.
10.sup.9 .OMEGA. cm. The complex was molded under the conditions of
a temperature of 130.degree. C. and a pressure of 30 kg/cm.sup.2,
using an extruder with a die having an inner diameter of 1 mm. and
an outer diameter of 2 mm. The resultant molding was cut into a
length of 10 cm and an electrode was formed at each end with silver
paint, to obtain a multiplier tube. The electric resistance of the
tube across the opposite ends thereof was 3.0 .times. 10.sup.11
.OMEGA. and the secondary electron emission coefficient .delta. was
2.1.
Example 8
100 g. of poly-2-vinylpyridine was dissolved in 200 ml. of ethanol
and quaternarized with 127 g. of 67 percent hydriodic acid. 100 g.
of the poly-2-vinylpyridine hydriodate was dissolved in 200 ml. of
an equivalent mixed solvent of water and ethanol. On the other
hand, 145 g. of lithium-tetracyano-paraquinodimethane was dissolved
in 500 ml. of water. Both solutions were mixed with each other and
the mixture was thoroughly stirred, whereby a dark bluish purple
precipitate was formed. This precipitate is the
poly-2-vinylpyridine-tetracyano-paraquinodimethane charge transfer
complex. This complex is highly conductive and highly moldable but
not sufficiently flexible. The complex was blended with polyvinyl
chloride which had been plasticized with low molecular weight
polyurethane. The blending ratio was as follows:
Poly-2-vinylpyridine-tetracyano-paraquinodimethane--50 g.
Polyvinyl chloride-- 30 g.
Stabilizer (tribasic lead sulfate,
Cd-Ba type stabilizer)--5 g.
Low molecular weight polyurethane
(Ultramole PU of Bayer)--25 g.
The blend was kneaded for about 10 minutes on a hot roll at a
temperature of 160.degree. - 170.degree. C. and formed into the
shape of a sheet. After pelletizing the sheet, the resultant
pellets were molded into a tube by an extruder. The molding was
effected at a temperature of 160.degree. C. under a pressure of 30
kg/cm.sup.2. The electric resistance of the thus produced
multiplier tube across the opposite ends thereof was 1.0 .times.
10.sup.11 .OMEGA. and the secondary electron emission coefficient
.delta. was 2.3.
Example 9
An electron-conductive polymer composition consisting of 90 g. of
an intermediate density polyethylene and 10 g. of carbon black
blended therewith, was used. Namely, the polyethylene was used to
make use of its own secondary electron emitting effect, and the
electron-conductive carbon black was added in a small quantity as
electron carrier, for quickly neutralizing the hole after the
emission of electrons. The composition had excellent moldability
and flexibility as it consisted essentially of polyethylene. The
material was molded by extrusion-molding into a pipe having an
inner diameter of 1 mm, an outer diameter of 2 mm and a total
length of 100 mm, at a temperature of 110.degree. C. under a
pressure of 60 kg/cm.sup.2.
The electric resistance of the pipe across the opposite ends
thereof was 1.0 .times. 10.sup.11 .OMEGA. and the secondary
electron emission coefficient .delta. was 1.9.
Example 10
30 g. of polyamine (Thomaid of Fuji Polymer Chemical Company) was
added to 100 g. of an epoxy resin (Epikote of Shell International
Chemicals Corporation), to which was added by stirring 10 g. of a
conductive silver powder for painting with stirring. The mixture
was poured into a tubular metal mold and cured therein for 1 hour
at a temperature of about 60.degree. C.
A multiplier tube having an inner diameter of 1.0 mm, an outer
diameter of 2.0 mm and a total length of 100 mm was obtained. The
resistance across the terminal ends of the tube was 1.0 .times.
10.sup.11 .OMEGA. and the secondary electron emission coefficient
.delta. was 1.7.
The secondary electron emission coefficients .delta. of the
secondary electron emitting polymer compositions produced by the
processes of the respective Examples were measured in a superhigh
vacuum from a sample film of each composition having a thickness of
20 .mu. and a diameter of 20 mm. The gains of the respective
multiplier tubes were measured by incorporating the tube in a
measuring circuit as shown in FIG. 7.
Referring to FIG. 10, there is shown the relationship between the
secondary electron emission coefficient .delta. and the primary
electron energy, which was obtained on a film of the secondary
electron emitting polymer composition produced by the process of
Example 5. Namely, the circuit of FIG. 7 was formed using the
secondary electron multiplier tube molded of the composition and a
faint electron stream of the order of 10.sup.-.sup.18 A having an
energy of 300 eV was fed to the multiplier tube as the input. To
the output side was connected a load resistance of 820 .OMEGA. and
a voltage change corresponding to the output current was observed
on a synchroscope. The relationship between the voltage impressed
and the gain is shown in FIG. 11. A noise-free, stable emitting
effect is obtained in the proximity of 3,000 V. The gain at this
time is 3.0 .times. 10.sup.8.
The secondary electron emission coefficients .delta. of the
multiplier tubes of Examples 5-10 with respect to a primary
electron having an energy of 300 eV and the gains of the same at an
acceleration voltage of 3,000 V were measured, the results of which
are summarized in Table 1 below: ##SPC1##
As has been described hereinabove, the flexible channel multiplier
of the present invention is superior to the prior art multipliers
in gain and is less inferior in characteristics. Further, the
flexible channel multiplier of the invention is far superior in the
uniformity of surface condition to the glass multiplier with a
coating on the inner surface thereof, owing to the fact that the
material of the tube itself is a uniform polymer composition having
a secondary electron emitting effect. Another advantage of the
present multiplier tube is that because of its flexibility, it is
highly resistive to shock, has excellent mechanical strengths and
can be used at a suitable curvature for the purpose of eliminating
the instability caused by ion feedback. The material can easily be
synthetized and simply molded by applying the techniques which are
commonly used for processing plastics. The flexible channel
secondary electron multiplier is adapted to mass production and is
of high industrial value. The flexible channel secondary electron
multiplier can be used as a detector element of such measuring
instruments which are mounted in an artificial satellite, space
observation rocket or the like for the measurement of ions,
electrons an photons, or as an ion detector of a mass spectrometer.
It is also expected to find practical use in an image intensifier
in the future which utilizes the secondary electron emitting
effect.
* * * * *