U.S. patent number 3,854,066 [Application Number 05/418,001] was granted by the patent office on 1974-12-10 for electron device incorporating a microchannel secondary emitter.
This patent grant is currently assigned to The United States of America as represented by the Secretary of the Army. Invention is credited to Wesley J. Payne.
United States Patent |
3,854,066 |
Payne |
December 10, 1974 |
ELECTRON DEVICE INCORPORATING A MICROCHANNEL SECONDARY EMITTER
Abstract
An electron device incorporating a microchannel plate as a
secondary emission electron source which in addition to the primary
current provided by an electron emitter, such as a thermionic
emitter, will provide high gains. By impressing the proper voltages
thereon, the entrance and exit surfaces of the microchannel plate
serve respectively as equivalents to the control grid and screen
grid in a conventional type tube.
Inventors: |
Payne; Wesley J. (Bath,
NY) |
Assignee: |
The United States of America as
represented by the Secretary of the Army (Washington,
DC)
|
Family
ID: |
23656251 |
Appl.
No.: |
05/418,001 |
Filed: |
November 21, 1973 |
Current U.S.
Class: |
313/105R;
313/105CM; 330/42 |
Current CPC
Class: |
H01J
3/023 (20130101); H01J 21/02 (20130101) |
Current International
Class: |
H01J
3/02 (20060101); H01J 3/00 (20060101); H01J
21/00 (20060101); H01J 21/02 (20060101); H01j
043/02 () |
Field of
Search: |
;250/213VT
;313/103-105,67-68,95 ;330/42 |
References Cited
[Referenced By]
U.S. Patent Documents
Other References
Panitz, J. A., "Wide Aperture Channel Plate Electron Multipliers
for Mass ectrometer," Rev. Sci. Instrum., 42, 5-1971, pp.
724-725..
|
Primary Examiner: Lynch; Michael J.
Assistant Examiner: Punter; Wm. H.
Attorney, Agent or Firm: Edelberg; Nathan Lee; Milton W.
Claims
I claim:
1. A high gain electron device comprising:
a planar surface electron source having means associated therewith
for causing electrons to be emitted therefrom;
a microchannel plate having parallel conductive entrance and exit
faces positioned proximate said surface with said entrance face and
said planar surface in parallel relationship;
anode means positioned to receive electrons from the exit face of
said microchannel plate;
means associated with said entrance face for receiving a modulating
voltage;
means associated with said exit face for receiving a biasing
voltage, whereby the voltages impressed upon said faces control the
gain of the device by causing the entrance and exit faces to
function as a control grid and screen grid respectively; and
a suppressor grid located between said exit face and anode for
preventing anode electrons from returning to said exit face.
2. The high gain electron device according to claim 1 wherein said
electron source and associated means comprise an indirectly heated
planar thermionic emitter.
Description
BACKGROUND OF THE INVENTION
The invention described is directed to an electron device for
obtaining voltage gain, oscillation, frequency mixing, detection,
power transfer and for various other uses by utilizing the
characteristics of the microchannel plate.
DESCRIPTION OF THE PRIOR ART
It is present practice in electron devices to use thermionic
emitters as a sole source of electrons for the purpose of obtaining
voltage gain, oscillation, frequency mixing, detection, power
transfer and other purposes. The thermionic emitter is usually, but
not necessarily, in the form of an indirectly heated cathode coated
with mixture of carbonates, which when reduced provide electrons.
Concentric with this cathode are located grids and anodes which
provide the necessary control, suppression, focusing and collection
of the electrons emitted by the thermionic emitter. A plurality of
the electrons emitted by the cathode are collected by the anode or
plate concentric with the cathode, while a minority of these
electrons are collected by other electrodes such as the screen grid
or other accelerating electrodes. For a given amount of electrons
or current from the emitter, the efficiency or gain of an electron
device is dependent upon the extent of change in plate (anode)
current relative to the change of voltage impressed on the first or
control grid. This is referred to as the transconductance (G.sub.M
= dI.sub.b /dE.sub.ci) of the device; and the higher this
characteristic the higher the gain of the device. To obtain higher
levels of transconductance it has been common practice to utilize
control grids which embody a large number of turns per inch of very
fine wire (lateral wire) which permits large changes in electrons
passing through or between these wires for very discrete changes in
the voltage applied to them. For a device having a given control
grid construction, the transconductance may be increased by
increasing the number of electrons thus creating a higher level of
current to be varied by the given control grid construction. This
has the disadvantage of requiring an emitter of large physical size
which is not always desirable, particularly in high frequency
applications where interelectrode capacities become an important
part of the required circuitry. Another disadvantage is that more
power is required to bring the emitter up to the required
temperature to obtain electron emission.
To acquire high values of G.sub.M, secondary emission has been
employed to multiply the electron current after it has passed
through the control grid. This has been done by deflecting the
electrons (after passing through the control grid) onto
appropriately treated surfaces at the appropriate angle of
incidences where secondary electrons are generated and are
subsequently collected by the anode. The transconductance or gain
of these tubes is thus increased by a factor equal to the number of
secondary electrons generated by each primary electron. If four
secondary electrons are obtained for each primary the
transconductances is increased by a factor of four. While this has
the advantage of requiring smaller electron emitting surfaces to
obtain very high values of transconductance, there are inherent
disadvantages to this device, such as the much more complex
mechanical construction, treatment and care in handling the
secondary emission surfaces. Due to these and other disadvantages,
this type of device has found limited usage.
SUMMARY OF THE INVENTION
It is the object of this invention to provide an electron device
which will incorporate a microchannel plate as a secondary emission
electron source which in addition to the primary current provided
by an electron emitter, as for example, a thermionic emitter, will
provide extremely high gains. It is a further object of this
disclosure to utilize the conducting surfaces of the microchannel
plate as the control and screen grid electrodes necessary for the
proper functioning of the device.
The advantages of this invention are as follows:
1. The gain of the microchannel multiplied by the gain realized
from using the input electrode as a control grid permits design of
a device of enormous gain.
2. Use of the input microchannel electrode as a control grid and
the output microchannel electrodes as a screen grid greatly
simplifies the construction since electrodes are in perfect
alignment; no grid adjusting is required and screen current
(microchannel exit surface) is minimal.
3. Due to the large numbers of secondaries generated by the
microchannel plate, the primary current can be low; in fact the
lower the primary current the higher the microchannel gain since
they have a tendency to saturate at higher current densities. A
very low heater power is thus required to provide this minimal
primary current density. It is conceivable that cold emitters might
even be used to furnish the required current density.
4. Microphonics characteristics would also be improved due to the
solid construction and the absence of flimsy wire parts
incorporated in conventional tubes.
5. The lower heater power requirements reduces the power supply
demands, hence increasing the portability of equipment
incorporating these devices.
6. Construction is simplified making it more adaptable to automatic
assembly procedures.
7. Since the gain is high, and the device may be made very small
and compact, it is ideally suited for high frequency
application.
BRIEF DESCRIPTION OF THE DRAWING
The drawing shows the arrangement of components for one
contemplated embodiment of the disclosed invention.
DESCRIPTION OF THE PREFERRED EMBODIMENT
As shown in the Figure, a thermionic emitter 11, for example, is
used to provide the primary electrons. This emitter is of the
planar type to permit uniform spacing with the microchannel plate
12. The entrance surface 13 of the microchannel plate 12 by being
made conductive is used as the control grid and will permit
electrons to enter or not, depending upon the potential impressed
upon it by a voltage source V.sub.MCP . A signal to be amplified
could also be added at this point. Since the tubes or channels of
the microchannel plate 12 are very small, discrete changes in this
voltage will result in large changes in primary electrons entering
the microchannel. After the primary electrons pass through the
entrance surface 13 they generate secondaries in the microchannel
plate as is known in the art. The exit surface 14, being made an
electrically positive surface in relation to the entrance surface
13, the electrons are accelerated from the exit surface to be
collected by the anode 15. The exit surface 14 is thus performing
the function of a screen grid in a conventional tube. The gains
realized, however, are increased to very high values due to the
secondary multiplication. Thus, if the gain of the microchannel is
10.sup.4, the overall gain would equal G.sub.M .times. 10.sup.4 ;
G.sub.M in this case being that at the entrance surface 13.
A suppressor grid 16 with voltage V.sub.s is shown between the exit
surface 14 and the anode 15 which has voltage V.sub.a applied
thereto. The function of the suppressor 16 is to provide a negative
going field to prevent anode secondary electrons from returning to
the exit microchannel surface. Anode secondaries are those which
are released from the anode surface by electrons impinging thereon
from the microchannel exit surface. By selecting appropriate
distances between the microchannel exit surface and the anode, the
suppressor may not be required.
While only one embodiment of the contemplated invention has been
described, it is to be understood that many variations,
substitutions and alterations may be made while remaining within
the spirit and scope of the invention which is limited only by the
following claims.
* * * * *