US2188410A - Electron multiplier - Google Patents
Electron multiplier Download PDFInfo
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- US2188410A US2188410A US166491A US16649137A US2188410A US 2188410 A US2188410 A US 2188410A US 166491 A US166491 A US 166491A US 16649137 A US16649137 A US 16649137A US 2188410 A US2188410 A US 2188410A
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- 229910052751 metal Inorganic materials 0.000 description 6
- 239000002184 metal Substances 0.000 description 6
- 230000004048 modification Effects 0.000 description 6
- 238000012986 modification Methods 0.000 description 6
- 239000011248 coating agent Substances 0.000 description 3
- 238000000576 coating method Methods 0.000 description 3
- 238000010894 electron beam technology Methods 0.000 description 3
- 239000000463 material Substances 0.000 description 3
- 238000010276 construction Methods 0.000 description 2
- 230000007423 decrease Effects 0.000 description 2
- 230000002093 peripheral effect Effects 0.000 description 2
- 150000001664 caesium compounds Chemical class 0.000 description 1
- 230000008878 coupling Effects 0.000 description 1
- 238000010168 coupling process Methods 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
- 238000003780 insertion Methods 0.000 description 1
- 230000037431 insertion Effects 0.000 description 1
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J43/00—Secondary-emission tubes; Electron-multiplier tubes
- H01J43/04—Electron multipliers
- H01J43/06—Electrode arrangements
- H01J43/18—Electrode arrangements using essentially more than one dynode
- H01J43/20—Dynodes consisting of sheet material, e.g. plane, bent
Definitions
- This invention relates to electron discharge devices and more particularly to electron discharge devices of the electron multiplier type in which a primary electron cLu'rent derived from a thermionic, photo-electric, or other primary cathode is amplified or multiplied one or more times by secondary electron emission.
- a known form of electron multiplier such as is disclosed in U. S. Patent 2,073,599, Malter, and in which the present invention may be embodied, comprises in general a primary cathode, a row of secondary emitters, a parallel row of accelerating electrodes, and an output anode.
- the accelerat ing electrodes and the secondary electron emit- !5 ters are at positive potentials which increase toward the output anode and a magnetic field causes the stream of electrons from the cathode to bombard the first secondary emitter, the resulting stream of secondary electrons to bom- 0 bard the second emitter, and so on, electron multiplication occurring at each bombardment.
- Such an electron multiplier has an accelerating voltage-final output current characteristic curve, which over a range of accelerating voltage from !5 zero to about 600 volts between emitters rises to a maximum of about 300 volts and then falls away again, showing a pronounced though not very sharp peak.
- the principal object of the invention is to :0 provide an improved electron multiplier useful for frequency multiplication, particularly frequency doubling, and similar purposesv
- Another object of the invention is to provide an electron multiplier having improved properties and char- 5 acteristics, especially a characteristic curve in which the sharpness of the peak is substantially increased.
- a further object is to provide a simple frequency doubler in which the improved electron multiplier is utilized.
- At least one of the electrodes of the electron multiplier is so dimensioned or constructed that with an increase in the accelerating voltage beyond a predetermined critical value at which the output current 5 is a maximum and at which the multiplier is normally operated, the proportion of electrons in one or more of the electron streams which is utilized to contribute to the generation of secondary electrons and to the final output our- 3 rent substantially decreases so that the output current falls sharply with the increase in operating voltage beyond the critical or normal value and the peak in the characteristic curve is sharpened.
- the electron multiplier may, in accordance with the invention, be used for frequency multiplication, particularly frequency doubling, and to this end the electron multiplier is operated at an accelerating voltage near the value corresponding to the summit of the peak and the 5- positive half waves of a frequency which is to be doubled is superimposed upon the accelerating voltage.
- the increase in potential during each half wave will cause the output current first to increase to the maximum and then to decrease 10 the same way by operating the tube at an ac- 1 5 celerating voltage near but on the other side of the summit of the peak.
- FIG. 1 One way of carrying out the invention is illustrated in the accompanying Figure 1 showing a known type of electron multiplier comprising an indirectly heated primary cathode I with a control electrode l I, a row of secondary emitter electrodes 2, 3, 4, and 5, a parallel row of accelerating electrodes 6, l, 8, 9, and I 0 in a plane parallel to the plane of the emitters, and an output anode I 2.
- the multiplier is connected in the usual way to a source l6 of operating potential, and if used for frequency doubling is also connected to a source of alternating voltage 13, a rectifier M, a resistance l5, and a tuned load circuit l1.
- each accelerating electrode may be connected internally of the envelope l8 to the next secondary emitting electrode so that electrode 6 is connected to emitter 2, electrode 1 to emitter 3, and so on, as shown in the patent above mentioned, which also shows a magnetic field system which may be used such as the magnetic system M.
- this conventional electron multiplier is modified by making the accelerating electrodes and the secondary emitters not, as hitherto, all of the same size, but of graduated size. As shown in Figure 1 these electrodes, except the accelerating electrode 6, are of greater size as their distance from the -5 the peak primary cathode 1 increases. At each step of electron multiplication, the electron beam becomes progressively larger in cross-section, hence the graduation of size in electrodes 2 to 5 and I to It) may be a graduation in length or in width, or both.
- Constructing the tube in accordance with this invention with electrodes of increasing size insures that the electron beams will just cover the emitters at normal operating voltage and will tend to overshoot their targets or overflow the edges of the emitters when a critical potential, slightly above normal operating voltage and the same for all the beams, is reached. In this way the peak of the characteristic at the critical voltage is considerably sharpened.
- the multiplier of Figure 1 is modified in accordance with this invention by the use of multiplying electrodes or emitters 2, 3, and 4, which arev of the same size, but are rendered secondary electron emitting, not over their whole surfaces, but over areas smaller than the whole surfaces.
- These areas, indicated at 2a, 3a, and 4a, are coated with a secondary electron emitting mate rial, such as caesium compounds and are graduated in size, increasing with distance from the cathode i and with proximity to anode 18.
- a secondary electron emitting mate rial such as caesium compounds
- the proportion of electrons in the beams which strike the coated or electron emitting areas is reduced.
- the peak of the characteristic may be exaggerated by coating the peripheral area of the output anode with a secondary electron emissive coating lZa.
- the emitters 2, 3 and 4-. and the accelerating electrodes 6, I, 8 and 9 are of the same size but adjacent each secondary emitter or multiplying electrode except the last and, for example, adjacent each emitter 2 and 3 is an auxiliary electrode i9 between the corresponding emitter and the output anode.
- Each auxiliary electrode lii is preferably tilted somewhat so as to face partly toward the accelerating electrode opposite the corresponding secondary emitter electrode to which the auxiliary electrode is adjacent.
- Each auxiliary electrode is connected to the next secondary emitter in the series, the first auxiliary electrode it? being connected to emitter 3 and the second to emitter 3.
- increasing the accelerating potential beyond a predetermined critical value causes increasing proportions of the electrons in the electron streams to fall upon the auxiliary electrodes and thus not contribute to further secondary emission.
- the auxiliary electrodes marked lga; 29a in this figure may, instead of being slightly tilted, be positioned between successive secondary emitter electrodes and somewhat behind them, so as to be further away than the emitters from the plane of the accelerating electrodes.
- the auxiliary electrodes may, as indicated in Figure l, be provided with separate external connections to enable the applied potentials to be individually adjusted.
- auxiliary electrodes. 2 I 22 in the form of small plates placed behind and beside the output anode l2. These auxiliary electrodes are connected to a source of higher potential than the output anode.
- the size of the output anode i2 is critically chosen in dependence upon the point at which the peak of the characteristic curve is required to occur, so that at the critical accelerating voltage all the discharge reaches the output 5 anode.
- the cross section of the discharge becomes greater than the area of the output anode I3, and an increasing number of the electrons miss and overflow the edge of the output anode and are taken up by the auxiliary electrodes 2 i, 22.
- An electron multiplier as described may be employed as a frequency multiplier by superimposing upon the usual accelerating potentials applied to the various electrodes a unidirectional potential derived by rectifying alternating current voltage of a frequency to be doubled, as shown in Figure 1.
- the source l3 of the alternating voltage to be doubled is connected in series with the rectifier l4 across the resistance 95 inserted in series with the operating potential source it for the electrodes, the place of insertion being so chosen that the unidirectional superimposed potential is superimposed on all the electrodes to which the operating source it is connected.
- the output anode is connected in the usual way to the positive terminal of the potential source l5, preferably through the parallel tuned circuit H resonant to a frequency double the frequency of the source i3.
- the auxiliary electrodes 2!, 22 may, as shown in Figure 6, be connected together and through a coil 23 to the positive terminal of the operating potential source Hi, this coil being coupled to a coil 24- which is connected in series with a rectifier M and also a source of frequency 53 to be doubled across a resistance inserted in series with the operating potential source it.
- the output circuit includes a tuned output circuit ll tuned to double the frequency of the source E3. The arrangement is such that the circuit in which the auxiliary electrodes 2i and 22 are connected is back coupled to the input circuit, this back coupling tending to exaggerate the peak in the characteristic.
- the extra accelerating electrode being marked NJ and the extra emitter 5.
- An electron multiplier comprising a primary cathode, an output anode, a pair of opposed electrodes on opposite sides of the path of the electron stream from said cathode to said anode, one
- said electrodes comprising a metal sheet posim tioned to intercept said stream and having a coating of high secondary electron emissivity smaller than said metal sheet and of substantially the size of the cross-section of said electron stream to said electrode at the critical accelerat- 6! with material having secondary electron emission greater than unity at normal operating voltage to provide active surfaces no greater in size than the cross-section of the electron discharge which impinges on said emitters at the critical operating voltage at which maximum output of the multiplier occurs.
- An electron multiplier comprising a primary cathode, an output anode, a pair of opposed electrodes on opposite sides of the path of the electron stream from said cathode to said anode, one of said electrodes being positioned to intercept said stream and comprising a metal sheet having an oxide coated secondary emissive portion of no greater size than the electron stream which impinges on said electrode at the critical accelerating voltage at which maximum output of the multiplier occurs and a non-emissive conductive metal portion adjacent the edge of said oxide coated portion for collecting the part of said electron stream which overflows said coated portion.
- An electron multiplier comprising a primary cathode, an output anode, a row of emitter electrodes between said cathode and said anode, a row of discrete accelerating electrodes in a plane parallel to the plane of said row of emitters and adapted to be connected to a source of operating voltage, one of said emitters comprising an oxide coated metal surface of high secondary emissivity no greater in area than the cross-section of the electron discharge which impinges on said emitter at the critical operating voltage at which maximum output of the multiplier occurs, and a clean metal surface adjacent the edge or" said oxide coated surface and in the path of that part of the electron discharge which passes the edge of said oxide coated surface.
- An electron multiplier comprising a primary cathode, an output anode, a row of discrete accelerating electrodes between said cathode and i said anode and adapted to be connected to a source of operating voltage, a row of emitter electrodes in a plane parallel to the plane of said row of accelerating electrodes, each emitter electrode comprising an oxide coated emitter portion and a non-emitting conductive portion positioned adjacent and extending beyond the edge of the oxide coated portion to intercept and collect that part of the discharge which misses said oxide coated portion of said emitter at an accelerating voltage higher than the critical value at which maximum output of the multiplier occurs.
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Description
- Jan. 30, 1940 A, LINSELL ELECTRON MULTIPLIER 2 Sheets-Sheet 1 Filed Sept. 50, 1937 K my E m m E H m W M m Jan. 30, 1940. A, UNSELL 2,188,410
' ELECTRON MULTiPLIER Filed Sept. 30; 1937 2 Sheets-Sheet 2 INVENTOR. ALFRED .4. L/NSELL BY W ATTORNEY.
Patented Jan. 30, 1940 UNETED STATES PATENT orrics ELECTRON MULTIPLIER Application September 30, 1937, Serial No. 166,491 In Great Britain October 26, 1936 6 Claims.
This invention relates to electron discharge devices and more particularly to electron discharge devices of the electron multiplier type in which a primary electron cLu'rent derived from a thermionic, photo-electric, or other primary cathode is amplified or multiplied one or more times by secondary electron emission.
A known form of electron multiplier, such as is disclosed in U. S. Patent 2,073,599, Malter, and in which the present invention may be embodied, comprises in general a primary cathode, a row of secondary emitters, a parallel row of accelerating electrodes, and an output anode. The accelerat ing electrodes and the secondary electron emit- !5 ters are at positive potentials which increase toward the output anode and a magnetic field causes the stream of electrons from the cathode to bombard the first secondary emitter, the resulting stream of secondary electrons to bom- 0 bard the second emitter, and so on, electron multiplication occurring at each bombardment. Such an electron multiplier has an accelerating voltage-final output current characteristic curve, which over a range of accelerating voltage from !5 zero to about 600 volts between emitters rises to a maximum of about 300 volts and then falls away again, showing a pronounced though not very sharp peak.
The principal object of the invention is to :0 provide an improved electron multiplier useful for frequency multiplication, particularly frequency doubling, and similar purposesv Another object of the invention is to provide an electron multiplier having improved properties and char- 5 acteristics, especially a characteristic curve in which the sharpness of the peak is substantially increased. A further object is to provide a simple frequency doubler in which the improved electron multiplier is utilized.
0 According to the invention at least one of the electrodes of the electron multiplier is so dimensioned or constructed that with an increase in the accelerating voltage beyond a predetermined critical value at which the output current 5 is a maximum and at which the multiplier is normally operated, the proportion of electrons in one or more of the electron streams which is utilized to contribute to the generation of secondary electrons and to the final output our- 3 rent substantially decreases so that the output current falls sharply with the increase in operating voltage beyond the critical or normal value and the peak in the characteristic curve is sharpened. Owing to the peak in the character- 5 istic curve, the electron multiplier may, in accordance with the invention, be used for frequency multiplication, particularly frequency doubling, and to this end the electron multiplier is operated at an accelerating voltage near the value corresponding to the summit of the peak and the 5- positive half waves of a frequency which is to be doubled is superimposed upon the accelerating voltage. The increase in potential during each half wave will cause the output current first to increase to the maximum and then to decrease 10 the same way by operating the tube at an ac- 1 5 celerating voltage near but on the other side of the summit of the peak.
For a better understanding of my invention, reference may be had to the accompanying drawings in which some embodiments of the inven- 0 tion are illustrated diagrammatically, and in which Figure 1 shows one form of multiplier used as a frequency doubler, Figures 2, 3, 4 and 5 show modifications, and Figure 6 shows a modification used as a frequency doubler.
One way of carrying out the invention is illustrated in the accompanying Figure 1 showing a known type of electron multiplier comprising an indirectly heated primary cathode I with a control electrode l I, a row of secondary emitter electrodes 2, 3, 4, and 5, a parallel row of accelerating electrodes 6, l, 8, 9, and I 0 in a plane parallel to the plane of the emitters, and an output anode I 2. The multiplier is connected in the usual way to a source l6 of operating potential, and if used for frequency doubling is also connected to a source of alternating voltage 13, a rectifier M, a resistance l5, and a tuned load circuit l1. In use, the accelerating electrodes 6 to H! are maintained at increasingly positive potentials in the usual way, not shown; for example, each accelerating electrode may be connected internally of the envelope l8 to the next secondary emitting electrode so that electrode 6 is connected to emitter 2, electrode 1 to emitter 3, and so on, as shown in the patent above mentioned, which also shows a magnetic field system which may be used such as the magnetic system M.
In accordance with the invention this conventional electron multiplier is modified by making the accelerating electrodes and the secondary emitters not, as hitherto, all of the same size, but of graduated size. As shown in Figure 1 these electrodes, except the accelerating electrode 6, are of greater size as their distance from the -5 the peak primary cathode 1 increases. At each step of electron multiplication, the electron beam becomes progressively larger in cross-section, hence the graduation of size in electrodes 2 to 5 and I to It) may be a graduation in length or in width, or both. Constructing the tube in accordance with this invention with electrodes of increasing size insures that the electron beams will just cover the emitters at normal operating voltage and will tend to overshoot their targets or overflow the edges of the emitters when a critical potential, slightly above normal operating voltage and the same for all the beams, is reached. In this way the peak of the characteristic at the critical voltage is considerably sharpened.
In another construction shown in Figure 2 the multiplier of Figure 1 is modified in accordance with this invention by the use of multiplying electrodes or emitters 2, 3, and 4, which arev of the same size, but are rendered secondary electron emitting, not over their whole surfaces, but over areas smaller than the whole surfaces. These areas, indicated at 2a, 3a, and 4a, are coated with a secondary electron emitting mate rial, such as caesium compounds and are graduated in size, increasing with distance from the cathode i and with proximity to anode 18. When the electron beams increase in cross section with increasing voltage, the proportion of electrons in the beams which strike the coated or electron emitting areas is reduced. As also indicated in this figure, the peak of the characteristic may be exaggerated by coating the peripheral area of the output anode with a secondary electron emissive coating lZa.
In another modification shown in Figure 3 the emitters 2, 3 and 4-. and the accelerating electrodes 6, I, 8 and 9 are of the same size but adjacent each secondary emitter or multiplying electrode except the last and, for example, adjacent each emitter 2 and 3 is an auxiliary electrode i9 between the corresponding emitter and the output anode. Each auxiliary electrode liiis preferably tilted somewhat so as to face partly toward the accelerating electrode opposite the corresponding secondary emitter electrode to which the auxiliary electrode is adjacent. Each auxiliary electrode is connected to the next secondary emitter in the series, the first auxiliary electrode it? being connected to emitter 3 and the second to emitter 3. In a multiplier of this construction, increasing the accelerating potential beyond a predetermined critical value causes increasing proportions of the electrons in the electron streams to fall upon the auxiliary electrodes and thus not contribute to further secondary emission.
As illustrated in Figure l, the auxiliary electrodes marked lga; 29a in this figure may, instead of being slightly tilted, be positioned between successive secondary emitter electrodes and somewhat behind them, so as to be further away than the emitters from the plane of the accelerating electrodes. If desired, the auxiliary electrodes may, as indicated in Figure l, be provided with separate external connections to enable the applied potentials to be individually adjusted.
In a further modification illustrated in Figure in the characteristic curve is exaggerated by the use of auxiliary electrodes. 2 I 22 in the form of small plates placed behind and beside the output anode l2. These auxiliary electrodes are connected to a source of higher potential than the output anode. In this modification the size of the output anode i2 is critically chosen in dependence upon the point at which the peak of the characteristic curve is required to occur, so that at the critical accelerating voltage all the discharge reaches the output 5 anode. When the accelerating voltage corresponding to this peak is exceeded the cross section of the discharge becomes greater than the area of the output anode I3, and an increasing number of the electrons miss and overflow the edge of the output anode and are taken up by the auxiliary electrodes 2 i, 22.
An electron multiplier as described may be employed as a frequency multiplier by superimposing upon the usual accelerating potentials applied to the various electrodes a unidirectional potential derived by rectifying alternating current voltage of a frequency to be doubled, as shown in Figure 1. For this purpose the source l3 of the alternating voltage to be doubled is connected in series with the rectifier l4 across the resistance 95 inserted in series with the operating potential source it for the electrodes, the place of insertion being so chosen that the unidirectional superimposed potential is superimposed on all the electrodes to which the operating source it is connected. The output anode is connected in the usual way to the positive terminal of the potential source l5, preferably through the parallel tuned circuit H resonant to a frequency double the frequency of the source i3.
If the modification shown in Figure 5 is used for frequency doubling, the auxiliary electrodes 2!, 22 may, as shown in Figure 6, be connected together and through a coil 23 to the positive terminal of the operating potential source Hi, this coil being coupled to a coil 24- which is connected in series with a rectifier M and also a source of frequency 53 to be doubled across a resistance inserted in series with the operating potential source it. The output circuit includes a tuned output circuit ll tuned to double the frequency of the source E3. The arrangement is such that the circuit in which the auxiliary electrodes 2i and 22 are connected is back coupled to the input circuit, this back coupling tending to exaggerate the peak in the characteristic. In order to indicate that the invention is not limited to the use of any particular number of electron 5G multiplier stages one more stage is shown in Figures 1 and 6 than in the other figures, the extra accelerating electrode being marked NJ and the extra emitter 5.
I claim:
1. An electron multiplier comprising a primary cathode, an output anode, a pair of opposed electrodes on opposite sides of the path of the electron stream from said cathode to said anode, one
of said electrodes comprising a metal sheet posim tioned to intercept said stream and having a coating of high secondary electron emissivity smaller than said metal sheet and of substantially the size of the cross-section of said electron stream to said electrode at the critical accelerat- 6! with material having secondary electron emission greater than unity at normal operating voltage to provide active surfaces no greater in size than the cross-section of the electron discharge which impinges on said emitters at the critical operating voltage at which maximum output of the multiplier occurs.
3. An electron multiplier as defined in claim 1 in which the peripheral area of the output anode is coated with electron emissive material.
4. An electron multiplier comprising a primary cathode, an output anode, a pair of opposed electrodes on opposite sides of the path of the electron stream from said cathode to said anode, one of said electrodes being positioned to intercept said stream and comprising a metal sheet having an oxide coated secondary emissive portion of no greater size than the electron stream which impinges on said electrode at the critical accelerating voltage at which maximum output of the multiplier occurs and a non-emissive conductive metal portion adjacent the edge of said oxide coated portion for collecting the part of said electron stream which overflows said coated portion.
5. An electron multiplier comprising a primary cathode, an output anode, a row of emitter electrodes between said cathode and said anode, a row of discrete accelerating electrodes in a plane parallel to the plane of said row of emitters and adapted to be connected to a source of operating voltage, one of said emitters comprising an oxide coated metal surface of high secondary emissivity no greater in area than the cross-section of the electron discharge which impinges on said emitter at the critical operating voltage at which maximum output of the multiplier occurs, and a clean metal surface adjacent the edge or" said oxide coated surface and in the path of that part of the electron discharge which passes the edge of said oxide coated surface.
6. An electron multiplier comprising a primary cathode, an output anode, a row of discrete accelerating electrodes between said cathode and i said anode and adapted to be connected to a source of operating voltage, a row of emitter electrodes in a plane parallel to the plane of said row of accelerating electrodes, each emitter electrode comprising an oxide coated emitter portion and a non-emitting conductive portion positioned adjacent and extending beyond the edge of the oxide coated portion to intercept and collect that part of the discharge which misses said oxide coated portion of said emitter at an accelerating voltage higher than the critical value at which maximum output of the multiplier occurs.
AUBYN LJNSELL,
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
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GB2188410X | 1936-10-26 |
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US2188410A true US2188410A (en) | 1940-01-30 |
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US166491A Expired - Lifetime US2188410A (en) | 1936-10-26 | 1937-09-30 | Electron multiplier |
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Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2424289A (en) * | 1943-07-30 | 1947-07-22 | Rca Corp | Calculating device |
US2465342A (en) * | 1941-07-28 | 1949-03-29 | Int Standard Electric Corp | Electronic discharge device |
US2617968A (en) * | 1946-09-28 | 1952-11-11 | Csf | Magnetron tube |
US2841741A (en) * | 1956-02-17 | 1958-07-01 | Bendix Aviat Corp | Multi-anode high speed switching tube |
-
1937
- 1937-09-30 US US166491A patent/US2188410A/en not_active Expired - Lifetime
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2465342A (en) * | 1941-07-28 | 1949-03-29 | Int Standard Electric Corp | Electronic discharge device |
US2424289A (en) * | 1943-07-30 | 1947-07-22 | Rca Corp | Calculating device |
US2617968A (en) * | 1946-09-28 | 1952-11-11 | Csf | Magnetron tube |
US2841741A (en) * | 1956-02-17 | 1958-07-01 | Bendix Aviat Corp | Multi-anode high speed switching tube |
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