US2281717A - Electron discharge apparatus - Google Patents

Electron discharge apparatus Download PDF

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Publication number
US2281717A
US2281717A US375114A US37511441A US2281717A US 2281717 A US2281717 A US 2281717A US 375114 A US375114 A US 375114A US 37511441 A US37511441 A US 37511441A US 2281717 A US2281717 A US 2281717A
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electrodes
discharge apparatus
chamber
electron beam
gap
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US375114A
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Arthur L Samuel
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AT&T Corp
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Bell Telephone Laboratories Inc
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Priority to US375114A priority Critical patent/US2281717A/en
Priority to GB4176/42A priority patent/GB555162A/en
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J23/00Details of transit-time tubes of the types covered by group H01J25/00
    • H01J23/16Circuit elements, having distributed capacitance and inductance, structurally associated with the tube and interacting with the discharge
    • H01J23/18Resonators
    • H01J23/20Cavity resonators; Adjustment or tuning thereof
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J25/00Transit-time tubes, e.g. klystrons, travelling-wave tubes, magnetrons
    • H01J25/02Tubes with electron stream modulated in velocity or density in a modulator zone and thereafter giving up energy in an inducing zone, the zones being associated with one or more resonators
    • H01J25/10Klystrons, i.e. tubes having two or more resonators, without reflection of the electron stream, and in which the stream is modulated mainly by velocity in the zone of the input resonator
    • H01J25/12Klystrons, i.e. tubes having two or more resonators, without reflection of the electron stream, and in which the stream is modulated mainly by velocity in the zone of the input resonator with pencil-like electron stream in the axis of the resonators

Definitions

  • One object of this invention is to achieve close,
  • Another object of this invention is to expedite the association of external circuits with the gaps in electron beam discharge apparatus.
  • a further object of this invention is to facilitate the exact tuning of external circuits associated with electron beam discharge devices.
  • the electrodes defining the gaps are provided with annular metallic portions sealed in the wall'of the enclosing vessel and extending therethrough, and the external circuits comprise chamber resonators contacting with the annular metallic portions.
  • the chamber resonators comprise separable halves adapted when joined to encompass the enclosing vessel of the device and to make good mechanical and electrical contact with the annular portions of the gap defining electrodes.
  • FIG. 1 is an elevational view mainly in section of electron beam discharge apparatus illustrative of one embodiment of this invention
  • Fig. 2 is a perspective view of one of the chamber resonators included in the apparatus shown in Fig. 1;
  • Fig. 3 is a fragmentary view mainly in section of electron beam discharge apparatus illustrative of another embodiment of this invention and particularly suitable for the generation of ultra-' high frequency oscillations.
  • the electron discharge apparatus illustrated in Fig. 1 comprises a highly evacuated enclosing vessel of ,vitreous material having an elongated tubular portion l0,
  • a target electrode ll mounted within the encloslng vessel'at one end thereof, and an electron gun II, which may be of the construction dis closed in the application Serial No. 327,826, filed April 4, 1940, of Arthur L. Samuel and Carlyle V. Parker, mounted within the vessel at the othar end thereof; the target electrode and electron gun being coaxial with the tubular portion In of the enclosing vessel.
  • a plurality of electrodes arranged in pairs as shown to define a pair of gaps l3 and Il.
  • Each of these electrodes includes a I central frusto-conical portion l5 and an outer annular portion i6 hermeticallysealed to and extending through the wall of the tubular portion Ill of the enclosing vessel.
  • the electron gun l2 when energized produces a concentrated electron beam which flows along the axis of the device to the target electrode ii and in so doing traverses the gaps l3 and Hi.
  • the beam may be controlled, by velocity variation, by potentials impressed upon or between the electrodes defining the gap l3 and energy ma be taken from the device by a circuit coupled to the electrodes defining the gap ll.
  • the input and output circuits comprise chamber resonators each of which, as shown more clearly in Fig. 2, includes two complementary semicircular metallic halves hinged together as shown at I1 and adapted to be locked together by a hook l8 and catch 19.
  • Each of the metallic halves includes semicircular end walls 20 joined to a semicylindrical outer wall 2 I, and an inner semicylindrical wall 22 having thereon a flange 23. All of these walls may be of a suitable metal, such as copper.
  • a semicylindrical wing bolt 29 threaded into metallic member 24, for example or tinned sheet copper, having a flexible slotted edge portion 25.
  • metallic member 24 for example or tinned sheet copper
  • semicylindrical metallic members 26, for example or tinned copper, having a slotted flexible edge portion 21 are secured to the flanges 23.
  • each chamber resonator when joined define an axially symmetrical structure which may be mounted readily on the tubular portion ll! of the enclosing vessel, with the flexible portions 25 and 21 making a good electrical contact with the annular portions of one pair of the gap defining electrodes, as shown in. Fig. 1.
  • a low resistance, close and highly efilcient coupling free from discontinuities is established between the gaps and the resonating chambers.
  • the resonating chambers in a particularly advantageous form are so constructed as to be substantially resonant to the frequency at which the device with which they are associated is to be operated. Exact tuning of each chamber to a desired frequency may be efiected by a metallic plate 28 mounted in adjustable parallel relation to one of the end walls 2b of the chamber by a the opposite end wall 2d.
  • An input or output circuit may be coupled to each chamber resonator through a metallic loop 30 one end of which is fitted in'an aperture in a metallic eyelet 3i fitted in one wall it of the chamber and the other end of which extends through an insulating member 32 within the eyelet Si, the eyelet being secured to the wall 26 by a locking ring 33 and set screw 36.
  • the loops 3d are constructed to provide the desired impedance and coupling for any particular application or use and, as will be understood, loops of cllfierent impedances may be used interchangeably to meet particular requirements.
  • each resonating chamber together with the electrodes 15, it associated therewith defines a conductive structure electrically symmetrical with respect to the longitudinal axis of the electron beam and the gaps l3 and id so that uniform transmission of energy between the beam and the resonating chambers is realized and faithful translation is obtained. Furthermore, as noted heretofore, a low resistance, low loss coupling free from discontinuities is achieved between the electron beam and the chamber resonators.
  • a chamber resonator suitable for use in apparatus for generating ultra-high frequency oscillations is illustrated in Fig. 3 and comprises coaxial cylindrical conductors 35 and 36.
  • the inner conductor 35 may be in one piece and of tinned sheet copper and is provided at its ends with flexible slotted portions 31 for grasping the annular portions 5 of two of the gap forming electrodes. Electrical connection to the inner conductor 35 may be established through a conductor 38 secured to I coupling between thethe conductor. midway between the ends thereot.
  • the outer conductor 36 may be composed of two metallic, e. 3., copper, halves hinged together as in the resonator illustrated in Fig. 2 and provided with inwardly extending flanges 39 to which metallic sleeves having flexible end portions 40 are secured, these end portions grasping the annular portions lb of two of the gap defining electrodes as shown. 'lhe resonating chamber, therefore, provides a low impedance, low loss gaps i3 and i4 and symmetrical with respect to the longitudinal axis of the electron beam.
  • Electron discharge apparatus comprising an enclosing vessel having a tubular insulating portion, means opposite one end of said portion for producing an electron beam, a target electrode opposite the other end of said portion, a pair of electrodes between said means and said electrode defining a gap to be traversed by said beam and having portions sealed 'in and extending through said insulating portion, a second pair of electrodes between said means and said .tar-
  • electrode defining a gap to be traversed by said beam and having portions sealed in and extending through said insulating portion, and a chamber resonator outside of said vessel including a wall electrically connecting one of said first pair of electrodes and one or said second pair of electrodes and a second wall electrically connecting the other electrodes of said pairs.
  • Electron discharge apparatus comprising an enclosing vessel having a tubular insulating portion, an electron gun opposite one end of said portion for projecting an electron beam axially thereof, a target electrode opposite the other end of said portion, two pairs of axially aligned electrodes within said insulating portion and defining a pair of gaps'to be traversed by the electron beam, each of said electrodes including an annular metallic member extending through said insulating portion and hermetically sealed thereto, and a cylindrical chamber resonator encompassing said tubular portion and including an inner cylindrical conductor contacting one of the annular members of the electrodes in each said pairs of electrodes and including also an outer cylindrical conductor electrically connected to the annular members of the other electrodes in said pairs of electrodes.
  • An electron beam discharge apparatus comprising an enclosing vessel having a tubular insulating portion, an electron gun opposite one end of said portion for projecting an electron beam therethrough, a target electrode opposite the other end of said portion, and means in energy transferring relation with said beam comprising a pair of spaced electrodes having portions defining a gap to be traversed by said beam and having also conductive members extending through said portion and hermetically sealed thereto and a chamber resonator encompassing said portion, said resonator including a pair of complementary halves each having resilient me- ;allio portions contacting said conductive memers.
  • Electron beam discharge apparatus including an enclosing vessel having a tubular insulating portion, means opposite one end oi said portion for projecting an electron beam there through, a target electrode opposite the other end of said portion, and means in energy translating relation with said beam comprising a pair of annular metallic discs extending through the wall of said insulating portion and hermetically sealed thereto, electrodes electrically integral with said discs and defining a gap to be traversed by said beam, and a cylindrical chamber resonator encompassing said insulating portion and including two complementary separable halves each having spaced walls each 01 which has ailixed thereto substantially semicylindrical flexible members grasping the periphery of one of said discs.
  • Electron beam discharge apparatus in ac cordance with claim 4 comprising means for tuning said chamber resonator including a metallic plate opposite and in parallel relation to one of said walls and means for varying the spacing between said plate and said one wall carried by the opposite wall.

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Description

y 1942- A. L. SAMUEL 23mm ELECTRON DISCHARGE APPARATUS Filed Jan. 2.1., 1941 /NVENTOR By ALSAMUEL WW6. M
AT TORNE Y Patented May 5, 1942 UNITED STATE 5 PATENT orFlca 2,281,717 I ELECTRON DISCHARGE APPARATUS Arthur L. Samuel, Summit, N. 1.. assignor to Bell Telephone Lahorato rice, 1 Incorporated,
New York, N. Y., a corporation of New York Application January 21, 1941, Serial No. 375,114
5 Claims.
with reference to the accompanying drawing, in
which:
or more gaps traversed by the beam at which a signal is impressed for controlling the beam or at' which energy is taken from the beam. Heretofore, external circuits have been associated with the beam by mounting elements of the circuit externally of the vessel and in the vicinity of the gap or gaps mentioned, the coupling path be.- I
tween the circuit and gap including the insulating material of the enclosing vessel. Such association of the external circuits with the gaps, it has been found, does not provide an eiilcient coupling between these circuits and gaps due in part to the physical and conductive segregation thereof and to losses, particularly at ultra-high frequencies, in the insulating material of the enclosing vessel. In addition, such association renders difficult, at best, the attainment of electrical symmetry between the beam, and the electrical circuits and the exact tuning of the circuits.
One object of this invention is to achieve close,
' efficient and symmetrical coupling between the circuits and the gaps in electron beam discharge apparatus.
Another object of this invention is to expedite the association of external circuits with the gaps in electron beam discharge apparatus.
A further object of this invention is to facilitate the exact tuning of external circuits associated with electron beam discharge devices.
In accordance with one feature of this invention, the electrodes defining the gaps are provided with annular metallic portions sealed in the wall'of the enclosing vessel and extending therethrough, and the external circuits comprise chamber resonators contacting with the annular metallic portions.
In accordance with another feature of this invention the chamber resonators comprise separable halves adapted when joined to encompass the enclosing vessel of the device and to make good mechanical and electrical contact with the annular portions of the gap defining electrodes.
The invention and the foregoing and other features thereof will be understood more clearly and fully from the following detailed description Fig. 1 is an elevational view mainly in section of electron beam discharge apparatus illustrative of one embodiment of this invention;
Fig. 2 is a perspective view of one of the chamber resonators included in the apparatus shown in Fig. 1; and
Fig. 3 is a fragmentary view mainly in section of electron beam discharge apparatus illustrative of another embodiment of this invention and particularly suitable for the generation of ultra-' high frequency oscillations.
Referring now to the drawing, the electron discharge apparatus illustrated in Fig. 1 comprises a highly evacuated enclosing vessel of ,vitreous material having an elongated tubular portion l0,
a target electrode ll mounted within the encloslng vessel'at one end thereof, and an electron gun II, which may be of the construction dis closed in the application Serial No. 327,826, filed April 4, 1940, of Arthur L. Samuel and Carlyle V. Parker, mounted within the vessel at the othar end thereof; the target electrode and electron gun being coaxial with the tubular portion In of the enclosing vessel.- Mounted between the target electrode and electrongun and coaxial therewith are a plurality of electrodes arranged in pairs as shown to define a pair of gaps l3 and Il. Each of these electrodes includes a I central frusto-conical portion l5 and an outer annular portion i6 hermeticallysealed to and extending through the wall of the tubular portion Ill of the enclosing vessel.
The electron gun l2 when energized produces a concentrated electron beam which flows along the axis of the device to the target electrode ii and in so doing traverses the gaps l3 and Hi. The beam may be controlled, by velocity variation, by potentials impressed upon or between the electrodes defining the gap l3 and energy ma be taken from the device by a circuit coupled to the electrodes defining the gap ll.
In the apparatus shown in Fig.1, the input and output circuits comprise chamber resonators each of which, as shown more clearly in Fig. 2, includes two complementary semicircular metallic halves hinged together as shown at I1 and adapted to be locked together by a hook l8 and catch 19. Each of the metallic halves includes semicircular end walls 20 joined to a semicylindrical outer wall 2 I, and an inner semicylindrical wall 22 having thereon a flange 23. All of these walls may be of a suitable metal, such as copper.
Secured to the upper wall 20 is a semicylindrical wing bolt 29 threaded into metallic member 24, for example or tinned sheet copper, having a flexible slotted edge portion 25. Similarly, semicylindrical metallic members 26, for example or tinned copper, having a slotted flexible edge portion 21 are secured to the flanges 23.
The two halves of each chamber resonator when joined define an axially symmetrical structure which may be mounted readily on the tubular portion ll! of the enclosing vessel, with the flexible portions 25 and 21 making a good electrical contact with the annular portions of one pair of the gap defining electrodes, as shown in. Fig. 1. Hence, it will be appreciated'that a low resistance, close and highly efilcient coupling free from discontinuities is established between the gaps and the resonating chambers.
n The resonating chambers in a particularly advantageous form are so constructed as to be substantially resonant to the frequency at which the device with which they are associated is to be operated. Exact tuning of each chamber to a desired frequency may be efiected by a metallic plate 28 mounted in adjustable parallel relation to one of the end walls 2b of the chamber by a the opposite end wall 2d.
An input or output circuit may be coupled to each chamber resonator through a metallic loop 30 one end of which is fitted in'an aperture in a metallic eyelet 3i fitted in one wall it of the chamber and the other end of which extends through an insulating member 32 within the eyelet Si, the eyelet being secured to the wall 26 by a locking ring 33 and set screw 36. The loops 3d are constructed to provide the desired impedance and coupling for any particular application or use and, as will be understood, loops of cllfierent impedances may be used interchangeably to meet particular requirements.
When the loop 38 in the resonating chamber nearest the gun i2 is energized by the application of a potential or slgnalthereto, this resonating chamber is excited accordingly and a corresponding controlling action is exerted on the electron beam, at the gap id. The beam in passing through the gap id excites the resonating chamber associated with this gap and an output current corresponding to the input signal is obtained from the loop 39 associated with the'output resonating cavity.
It will be noted that each resonating chamber together with the electrodes 15, it associated therewith defines a conductive structure electrically symmetrical with respect to the longitudinal axis of the electron beam and the gaps l3 and id so that uniform transmission of energy between the beam and the resonating chambers is realized and faithful translation is obtained. Furthermore, as noted heretofore, a low resistance, low loss coupling free from discontinuities is achieved between the electron beam and the chamber resonators.
A chamber resonator suitable for use in apparatus for generating ultra-high frequency oscillations is illustrated in Fig. 3 and comprises coaxial cylindrical conductors 35 and 36. The inner conductor 35 may be in one piece and of tinned sheet copper and is provided at its ends with flexible slotted portions 31 for grasping the annular portions 5 of two of the gap forming electrodes. Electrical connection to the inner conductor 35 may be established through a conductor 38 secured to I coupling between thethe conductor. midway between the ends thereot.
The outer conductor 36 may be composed of two metallic, e. 3., copper, halves hinged together as in the resonator illustrated in Fig. 2 and provided with inwardly extending flanges 39 to which metallic sleeves having flexible end portions 40 are secured, these end portions grasping the annular portions lb of two of the gap defining electrodes as shown. 'lhe resonating chamber, therefore, provides a low impedance, low loss gaps i3 and i4 and symmetrical with respect to the longitudinal axis of the electron beam.
- Although specific embodiments of the invention have been shown and described, it will be understood, of course, that they are but illustrative and that various modifications may be made therein without departing from the scope and spirit of this invention as defined in the appended claims.
What is claimed is: l
1. Electron discharge apparatus comprising an enclosing vessel having a tubular insulating portion, means opposite one end of said portion for producing an electron beam, a target electrode opposite the other end of said portion, a pair of electrodes between said means and said electrode defining a gap to be traversed by said beam and having portions sealed 'in and extending through said insulating portion, a second pair of electrodes between said means and said .tar-
' get electrode defining a gap to be traversed by said beam and having portions sealed in and extending through said insulating portion, and a chamber resonator outside of said vessel including a wall electrically connecting one of said first pair of electrodes and one or said second pair of electrodes and a second wall electrically connecting the other electrodes of said pairs.
2. Electron discharge apparatus comprising an enclosing vessel having a tubular insulating portion, an electron gun opposite one end of said portion for projecting an electron beam axially thereof, a target electrode opposite the other end of said portion, two pairs of axially aligned electrodes within said insulating portion and defining a pair of gaps'to be traversed by the electron beam, each of said electrodes including an annular metallic member extending through said insulating portion and hermetically sealed thereto, and a cylindrical chamber resonator encompassing said tubular portion and including an inner cylindrical conductor contacting one of the annular members of the electrodes in each said pairs of electrodes and including also an outer cylindrical conductor electrically connected to the annular members of the other electrodes in said pairs of electrodes.
3. An electron beam discharge apparatus comprising an enclosing vessel having a tubular insulating portion, an electron gun opposite one end of said portion for projecting an electron beam therethrough, a target electrode opposite the other end of said portion, and means in energy transferring relation with said beam comprising a pair of spaced electrodes having portions defining a gap to be traversed by said beam and having also conductive members extending through said portion and hermetically sealed thereto and a chamber resonator encompassing said portion, said resonator including a pair of complementary halves each having resilient me- ;allio portions contacting said conductive memers.
4. Electron beam discharge apparatus including an enclosing vessel having a tubular insulating portion, means opposite one end oi said portion for projecting an electron beam there through, a target electrode opposite the other end of said portion, and means in energy translating relation with said beam comprising a pair of annular metallic discs extending through the wall of said insulating portion and hermetically sealed thereto, electrodes electrically integral with said discs and defining a gap to be traversed by said beam, and a cylindrical chamber resonator encompassing said insulating portion and including two complementary separable halves each having spaced walls each 01 which has ailixed thereto substantially semicylindrical flexible members grasping the periphery of one of said discs.
5. Electron beam discharge apparatus in ac cordance with claim 4 comprising means for tuning said chamber resonator including a metallic plate opposite and in parallel relation to one of said walls and means for varying the spacing between said plate and said one wall carried by the opposite wall.
AR'IHURL. SAMUEL
US375114A 1941-01-21 1941-01-21 Electron discharge apparatus Expired - Lifetime US2281717A (en)

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Cited By (30)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2420314A (en) * 1943-04-26 1947-05-13 Sperry Gyroscope Co Inc High-frequency resonator-tube
US2421635A (en) * 1943-03-20 1947-06-03 Gen Electric Ultra high frequency space resonant system
US2422695A (en) * 1943-05-07 1947-06-24 Bell Telephone Labor Inc Suppression of parasitic oscillations in high-frequency devices
US2423078A (en) * 1943-10-20 1947-07-01 Bell Telephone Labor Inc Harmonic generator
US2443907A (en) * 1943-01-11 1948-06-22 Gen Electric High-frequency cavity resonator apparatus
US2444066A (en) * 1940-05-11 1948-06-29 Int Standard Electric Corp Tuner for cavity resonators
US2447461A (en) * 1941-01-18 1948-08-17 Rca Corp Resonant cavity circuits
US2451328A (en) * 1941-02-14 1948-10-12 Standard Telephones Cables Ltd Ultra high frequency electron discharge device
US2454970A (en) * 1943-10-16 1948-11-30 Gen Electric Ultra high frequency electric discharge device
US2462856A (en) * 1942-05-19 1949-03-01 Sperry Corp Transmitter and/or receiver circuits
US2464349A (en) * 1943-05-27 1949-03-15 Bell Telephone Labor Inc Electronic high-voltage generator discharge device
US2466765A (en) * 1944-09-22 1949-04-12 Bell Telephone Labor Inc Magnetron inductive tuner employing variably spaced parallel plate transmission line
US2490845A (en) * 1945-01-20 1949-12-13 Sperry Corp High-frequency cavity resonator apparatus
US2498763A (en) * 1944-06-15 1950-02-28 Westinghouse Electric Corp Magnetron
US2501181A (en) * 1944-08-15 1950-03-21 Rca Corp High-frequency cavity resonator apparatus
US2506590A (en) * 1941-10-31 1950-05-09 Sperry Corp High-frequency tube structure
US2537862A (en) * 1943-07-09 1951-01-09 Bell Telephone Labor Inc High-voltage pulse generator
US2600278A (en) * 1945-08-02 1952-06-10 Louis D Smullin Variable capacity cavity tuning
US2619611A (en) * 1951-05-29 1952-11-25 Eitel Mccullough Inc Electron tube apparatus
US2639405A (en) * 1945-09-29 1953-05-19 Sylvania Electric Prod Electron discharge device
US2653300A (en) * 1945-10-10 1953-09-22 Louis D Smullin Wide band transmit receive switch
US2676787A (en) * 1949-06-22 1954-04-27 Howard L Johnson Drilling equipment
US2688107A (en) * 1950-01-25 1954-08-31 Collins Radio Co Electron beam device
US2774066A (en) * 1943-01-30 1956-12-11 Bell Telephone Labor Inc Transmitting and receiving circuits for wave transmission systems
US2904719A (en) * 1954-05-19 1959-09-15 Emi Ltd Electron discharge devices and electrical resonators therefor
US3076116A (en) * 1959-09-21 1963-01-29 Eitel Mccullough Inc Klystron apparatus
DE1243787B (en) * 1955-07-08 1967-07-06 Varian Associates Tunable electron tube in the manner of a klystron
DE1282197B (en) * 1955-09-21 1968-11-07 Varian Associates Reflex klystron
EP0390474A2 (en) * 1989-03-30 1990-10-03 Varian Associates, Inc. Klystron amplifier
US5239272A (en) * 1990-03-09 1993-08-24 Eev Limited Electron beam tube arrangements having primary and secondary output cavities

Cited By (31)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2444066A (en) * 1940-05-11 1948-06-29 Int Standard Electric Corp Tuner for cavity resonators
US2447461A (en) * 1941-01-18 1948-08-17 Rca Corp Resonant cavity circuits
US2451328A (en) * 1941-02-14 1948-10-12 Standard Telephones Cables Ltd Ultra high frequency electron discharge device
US2506590A (en) * 1941-10-31 1950-05-09 Sperry Corp High-frequency tube structure
US2462856A (en) * 1942-05-19 1949-03-01 Sperry Corp Transmitter and/or receiver circuits
US2443907A (en) * 1943-01-11 1948-06-22 Gen Electric High-frequency cavity resonator apparatus
US2774066A (en) * 1943-01-30 1956-12-11 Bell Telephone Labor Inc Transmitting and receiving circuits for wave transmission systems
US2421635A (en) * 1943-03-20 1947-06-03 Gen Electric Ultra high frequency space resonant system
US2420314A (en) * 1943-04-26 1947-05-13 Sperry Gyroscope Co Inc High-frequency resonator-tube
US2422695A (en) * 1943-05-07 1947-06-24 Bell Telephone Labor Inc Suppression of parasitic oscillations in high-frequency devices
US2464349A (en) * 1943-05-27 1949-03-15 Bell Telephone Labor Inc Electronic high-voltage generator discharge device
US2537862A (en) * 1943-07-09 1951-01-09 Bell Telephone Labor Inc High-voltage pulse generator
US2454970A (en) * 1943-10-16 1948-11-30 Gen Electric Ultra high frequency electric discharge device
US2423078A (en) * 1943-10-20 1947-07-01 Bell Telephone Labor Inc Harmonic generator
US2498763A (en) * 1944-06-15 1950-02-28 Westinghouse Electric Corp Magnetron
US2501181A (en) * 1944-08-15 1950-03-21 Rca Corp High-frequency cavity resonator apparatus
US2466765A (en) * 1944-09-22 1949-04-12 Bell Telephone Labor Inc Magnetron inductive tuner employing variably spaced parallel plate transmission line
US2490845A (en) * 1945-01-20 1949-12-13 Sperry Corp High-frequency cavity resonator apparatus
US2600278A (en) * 1945-08-02 1952-06-10 Louis D Smullin Variable capacity cavity tuning
US2639405A (en) * 1945-09-29 1953-05-19 Sylvania Electric Prod Electron discharge device
US2653300A (en) * 1945-10-10 1953-09-22 Louis D Smullin Wide band transmit receive switch
US2676787A (en) * 1949-06-22 1954-04-27 Howard L Johnson Drilling equipment
US2688107A (en) * 1950-01-25 1954-08-31 Collins Radio Co Electron beam device
US2619611A (en) * 1951-05-29 1952-11-25 Eitel Mccullough Inc Electron tube apparatus
US2904719A (en) * 1954-05-19 1959-09-15 Emi Ltd Electron discharge devices and electrical resonators therefor
DE1243787B (en) * 1955-07-08 1967-07-06 Varian Associates Tunable electron tube in the manner of a klystron
DE1282197B (en) * 1955-09-21 1968-11-07 Varian Associates Reflex klystron
US3076116A (en) * 1959-09-21 1963-01-29 Eitel Mccullough Inc Klystron apparatus
EP0390474A2 (en) * 1989-03-30 1990-10-03 Varian Associates, Inc. Klystron amplifier
EP0390474A3 (en) * 1989-03-30 1991-06-12 Varian Associates, Inc. Klystron amplifier
US5239272A (en) * 1990-03-09 1993-08-24 Eev Limited Electron beam tube arrangements having primary and secondary output cavities

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