US3896329A - Permanent magnet beam focus structure for linear beam tubes - Google Patents
Permanent magnet beam focus structure for linear beam tubes Download PDFInfo
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- US3896329A US3896329A US291117A US29111772A US3896329A US 3896329 A US3896329 A US 3896329A US 291117 A US291117 A US 291117A US 29111772 A US29111772 A US 29111772A US 3896329 A US3896329 A US 3896329A
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- electron gun
- permanent magnet
- pole piece
- beam path
- collector
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J23/00—Details of transit-time tubes of the types covered by group H01J25/00
- H01J23/02—Electrodes; Magnetic control means; Screens
- H01J23/08—Focusing arrangements, e.g. for concentrating stream of electrons, for preventing spreading of stream
- H01J23/087—Magnetic focusing arrangements
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- ABSTRACT A light-weight permanent magnet beam focus structure for linear beam microwave tubes, such as klystrons and traveling wave tubes, employs a pair of centrally apertured generally cylindrical pole pieces disposed at opposite ends of the tube.
- the pole pieces are energized by means of a pair of high BXH product, radially polarized, permanently magnetized rings which are surrounded by a magnetically permeable cylindrical yoke.
- the magnet material is magnetized and loaded such as to have a ratio of Bm/Hm within the range of 0.8 to 1.3.
- Suitable magnets include the rare earth cobalt magnets, especially samarium cobalt.
- X-band medium power CW klystrons have had their beams magnetically focused by means of a pair of centrally apertured pole pieces disposed at opposite ends of the beampath and energized by means of transversely polarized bar magnets of Alnico IX material energized and loaded such as to have a Bm/Hm ratio of approximately 9.0.
- the beam of ing specification taken in connection with the accoma microwave tube may be focused by means of a permanent magnet structure utilizing radially polarized an- *nular permanent magnets at oppositeends of the tube and enclosed in a cylindrical magnetic yoke.
- a beam focusingmagnetic structure is disclosed in US. Pat. No. 3,205,415 issued Sept. 7, 1965.
- the permanently magnetized SUMMARY OF THE PRESENT INVENTION The principal object of the present invention is the provision of an improved permanent magnet beam focus structure for linear beam tubes.
- a pair of pole pieces at opposite ends of the beam path are energized by first and second radially polarized permanent magnets interconnected by a surrounding cylindrical magnetic yoke, whereby certain undesired leakage flux is eliminated to achieve a substantial reduction in the weight of the magnetic focus structure.
- the permanent magnet material is rare earth cobalt or mixtures of same energized and loaded to have a Bm/Hm ratio falling within the range of 0.8 to 1.3.
- the pole piece structure at the gun end of the tube includes a tubular axial projection projecting around the cathode for shaping the magnetic field in the region of the gun to provide a confined flow type of magnetic beam focusing.
- FIG. 1 is a longitudinal sectional view, partly in elevation, depicting a klystron tube employing a prior art magnetic beam focus structure
- FIGS. 1 and 2 there is shown an X- band klystron tube 1 employing a prior art permanent magnet beam focus structure 2.
- the tube 1 includes an electron gun assembly 3 for forming and projecting a beam of electrons 4 over an elongated beam path to a beam collector structure 5 disposed at the terminal end of the beam path for collecting and dissipating the energy of the collected electrons.
- a microwave circuit 6 is disposed along the. beam path 4 intermediate the electron gun 3 and beam collector 5 in energy exchanging relation with the beam to produce an output microwave signal which is coupled from the circuit 6 to a suitable load, such as an antenna, not shown.
- the microwave circuit.6 comprises an electrically conductive block body portion 7, as of copper, having a plurality of reentrant cavity resonators 8 formed therein.
- the cavities 8 include a deformable wall portion defining a tuning diaphragm, not shown, which is moved in and out (relative to the plane of the paper) for changing the volume of the cavity and thus tuning the resonant frequency of the cavity.
- the diaphragm is deformed by means of a tuning bridge structure 9 projecting out from the body of the tube along one side thereof.
- a pair of waveguides, not shown, project out from the first and last cavity on the opposite side of the body 7 from the tuners 9.
- the permanent magnet beam focus structure 2 includes a centrally apertured electron gun pole piece 11 disposed at the upstream end of the beam 4 and a similar collector pole piece 12 disposed adjacent the collector 5.
- pole pieces 11 and 12 are madeof soft iron.
- The. pole pieces are energized by transversely directed pairs of permanent bar-shaped magnets 13 and 14, said pairs of permanent magnets 13 and 14 being transversely polarized as indicated by the arrows to make one of the magnetic poles ll of one polarity such as north, and the other magnetic pole piece 12 of opposite polarity, such as south, to produce a beam focusing magnetic field within the beam 4 which is longitudinally directed of the beam and of generally uniform magnitude as of 2,200 gauss.
- a pair of magnetically permeable rectangular plates 15, as of soft iron, are disposed on opposite sides of the body of the tube 7 interconnecting thepairs of permanent magnets 13 and 14 to provide a magnetic flux return path.
- the magnets 13 and 14 of the prior art were made of Alnico IX and energized and loaded such as to have an operating point with a ratio of Bm/Hm of approxiing structure for focusing an X-band klystron of the type shown in FIG. 1 having a gap length between poles ll and'l2 of 1.8 inches and providing a magnetic field of an averageintensity of 2,200 gauss within'the beam path weighs approximately 14 pounds.
- Several problems, aside from weight, are encountered in the structure of FIG. 2. One of these problems is that if the magnets 13 and 14 are not properly balanced, i.e., of equal prior art magnet structure of FIG.
- the Bm v. Hm curve for samarium cobalt is shown by line 23.
- the load line 24 (Bm/Hm) ratio is chosen within the range of 0.8 to 1.3. This yields a higher energy product magnet than that offered by Alnico IX.
- the beam focus structure 31 includes an annular gun pole piece 32 disposed at the gun end of the tube and-having an axially directed tubular projecting portion 33 surrounding the thermionic cathode emitter 34 of the electron gun 3.
- An annular collector pole piece 35 is disposed at the collector end of the interaction circuit region 6.
- a pair of annular radially polarized permanent magnets 36 and 37 are dis-- posed encircling the respective gun and the collector pole piece structures 32 and 35.
- a cylindrical magnetic return yoke 38 as of soft iron surrounds both the gun and collector permanent magnets 36 and 37 and the intervening region therebetween. The yoke 38 is apertured for access to the tuners 9 and for'passage of the wave-guides through the yoke.
- the permanent magnets 36 and 37 are preferably rare earth cobalt magnets operated in a region having a ratio of (Bm/Hm)within the range of 0.8 to 1.3, as indicated by the cross-hatched region of the plot of FIG. 3. Magnets 36 and'37 are oppositely radially polarized as shown by the arrows of FIG. 4 to produce an axial magnetic focusing field B in the gap between the pole pieces 33 and 35.
- the mutually opposed inner faces 41 and 42 of the gun pole piece and collector pole piece, respectively, are planar and parallel to facilitate emitter of the gun such that the magnetic flux lines pass through the emitting surface perpendicular thereto to obtain a confined flow type of magnetic beam focusing.
- the magnetic beam focusing structure 31 of the present invention results in reducing the weight of the beam focus magnetic structure by a factor of 3.5. That is, the weight is cut from 14 pounds to 4 pounds.
- a better beam focusing field is obtained because the cylindrical yoke 38 in combination with the annular permanent magnets 36 and 37 yields cylindrical symmetry which assures that the opposite sides of the yoke are operating at the same magnetic potential as the yoke constitutes a magnetic equipotential member.
- I In a linear beam tube: electron gun means for forming and projecting a beam of electrons over an elongated beam path; collector means at the terminal end of the beam path for collecting and dissipating the energy of the collected electrons; electrical circuit means disposed along the beam path I intermediate said cathode means and said collector means in energy exchanging relation with the beam to produce an output signal; magnet means for magnetically focusing the beam over said beam path between said electron gun means and said collector means, said magnet 7 means including, electron gun and collector pole piece structures coaxially disposed of the beam path in axially spaced relation, said pole piece structures each being centrally apertured for passage of the beam therethrough and each being made of a magnetically permeable material, magnetically permeable magnetic yoke means coaxially disposed of said beam path and including axially spaced portions surrounding said electron gun and collector pole piece structures respectively in radially spaced relation therefrom, permanent magnet means for energizing said pole piece structures, said permanent magnet means comprising essentially only first
Abstract
A light-weight permanent magnet beam focus structure for linear beam microwave tubes, such as klystrons and traveling wave tubes, employs a pair of centrally apertured generally cylindrical pole pieces disposed at opposite ends of the tube. The pole pieces are energized by means of a pair of high BXH product, radially polarized, permanently magnetized rings which are surrounded by a magnetically permeable cylindrical yoke. The magnet material is magnetized and loaded such as to have a ratio of Bm/Hm within the range of 0.8 to 1.3. Suitable magnets include the rare earth cobalt magnets, especially samarium cobalt.
Description
United States Patent [1 1 Lien [ 1 July 22, 1975 PERMANENT MAGNET BEAM FOCUS STRUCTURE FOR LINEAR BEAM TUBES Primary ExaminerJames W. Lawrence Assistant ExaminerSaxfield Chatmon, Jr. Attorney, Agent, or FirmStanley Z. Cole; D. R. Pressman; R. K. Stoddard [57] ABSTRACT A light-weight permanent magnet beam focus structure for linear beam microwave tubes, such as klystrons and traveling wave tubes, employs a pair of centrally apertured generally cylindrical pole pieces disposed at opposite ends of the tube. The pole pieces are energized by means of a pair of high BXH product, radially polarized, permanently magnetized rings which are surrounded by a magnetically permeable cylindrical yoke. The magnet material is magnetized and loaded such as to have a ratio of Bm/Hm within the range of 0.8 to 1.3. Suitable magnets include the rare earth cobalt magnets, especially samarium cobalt.
7 Claims, 4 Drawing Figures [52] US. Cl. 315/35; 313/84; 315/535 [51] Int. Cl. H0lj 25/34 [58] Field of Search 315/35, 5.35; 313/84 [56] References Cited UNITED STATES PATENTS 2,936,394 5/1960 Brewer 315/3.5 2,956,193 10/1960 De Wit 315/3.5 X 3,133,226 5/1964 Buck et al... 315/35 3,141,116 7/1964 Henne 315/35 X 3,255,370 6/1966 Geppert... 315/535 X 3,324,433 6/1967 Kimura.... 315/35 X 3,375,400 3/1968 Schrumpf 3l5/3.5
sm Bill e s4? H Brn //lllllllllll"l 7/// PERMANENT MAGNET BEAM FOCUS STRUCTURE FOR LINEAR BEAM TUBES DESCRIPTION OF THE PRIOR ART Heretofore, X-band medium power CW klystrons have had their beams magnetically focused by means of a pair of centrally apertured pole pieces disposed at opposite ends of the beampath and energized by means of transversely polarized bar magnets of Alnico IX material energized and loaded such as to have a Bm/Hm ratio of approximately 9.0. Two such bar magnets were provided at opposite lateral sides of each pole piece and a pair of magnetically permeable yoke plates interconnected the two energized pole piece assemblies to provide a return flux path therebetween. In a typical X-band CW klystron tube, the aforedescribed magnet structure, which is capable of providing an average focusing magnetic field of 2,200 gauss over a beam path length of 1.8 inches, weighs approximately 14 pounds.
It would be desirable to substantially reduce the weight of the beam focus magnetic structure, especially for airborne applications. i
It is also known from the prior art that certain rare earth cobalt magnet materials, such as samarium cobalt, can provide a higher energy product permanent magnet than that offered by Alnico IX.
It is also known from the prior art that the beam of ing specification taken in connection with the accoma microwave tube may be focused by means of a permanent magnet structure utilizing radially polarized an- *nular permanent magnets at oppositeends of the tube and enclosed in a cylindrical magnetic yoke. Such a beam focusingmagnetic structure is disclosed in US. Pat. No. 3,205,415 issued Sept. 7, 1965. In this latter magnetic focusing system, the permanently magnetized SUMMARY OF THE PRESENT INVENTION The principal object of the present invention is the provision of an improved permanent magnet beam focus structure for linear beam tubes.
In one feature of the present invention, a pair of pole pieces at opposite ends of the beam path are energized by first and second radially polarized permanent magnets interconnected by a surrounding cylindrical magnetic yoke, whereby certain undesired leakage flux is eliminated to achieve a substantial reduction in the weight of the magnetic focus structure.
In another feature of the present invention, the permanent magnet material is rare earth cobalt or mixtures of same energized and loaded to have a Bm/Hm ratio falling within the range of 0.8 to 1.3.
In another feature of the present invention, the pole piece structure at the gun end of the tube includes a tubular axial projection projecting around the cathode for shaping the magnetic field in the region of the gun to provide a confined flow type of magnetic beam focusing.
Other features and advantages of the present invention will become apparent upon a perusal of the followpanying drawings wherein:
BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a longitudinal sectional view, partly in elevation, depicting a klystron tube employing a prior art magnetic beam focus structure,
DESCRIPTION OF THE PREFERRED EMBODIMENTS Referring now to FIGS. 1 and 2, there is shown an X- band klystron tube 1 employing a prior art permanent magnet beam focus structure 2. The tube 1 includes an electron gun assembly 3 for forming and projecting a beam of electrons 4 over an elongated beam path to a beam collector structure 5 disposed at the terminal end of the beam path for collecting and dissipating the energy of the collected electrons. A microwave circuit 6 is disposed along the. beam path 4 intermediate the electron gun 3 and beam collector 5 in energy exchanging relation with the beam to produce an output microwave signal which is coupled from the circuit 6 to a suitable load, such as an antenna, not shown. The microwave circuit.6 comprises an electrically conductive block body portion 7, as of copper, having a plurality of reentrant cavity resonators 8 formed therein. The cavities 8 include a deformable wall portion defining a tuning diaphragm, not shown, which is moved in and out (relative to the plane of the paper) for changing the volume of the cavity and thus tuning the resonant frequency of the cavity. The diaphragm is deformed by means of a tuning bridge structure 9 projecting out from the body of the tube along one side thereof. A pair of waveguides, not shown, project out from the first and last cavity on the opposite side of the body 7 from the tuners 9.
As best shown in FIG. 2 the permanent magnet beam focus structure 2 includes a centrally apertured electron gun pole piece 11 disposed at the upstream end of the beam 4 and a similar collector pole piece 12 disposed adjacent the collector 5. In a typical example, pole pieces 11 and 12 are madeof soft iron. The. pole pieces are energized by transversely directed pairs of permanent bar- shaped magnets 13 and 14, said pairs of permanent magnets 13 and 14 being transversely polarized as indicated by the arrows to make one of the magnetic poles ll of one polarity such as north, and the other magnetic pole piece 12 of opposite polarity, such as south, to produce a beam focusing magnetic field within the beam 4 which is longitudinally directed of the beam and of generally uniform magnitude as of 2,200 gauss. A pair of magnetically permeable rectangular plates 15, as of soft iron, are disposed on opposite sides of the body of the tube 7 interconnecting thepairs of permanent magnets 13 and 14 to provide a magnetic flux return path.
The magnets 13 and 14 of the prior art were made of Alnico IX and energized and loaded such as to have an operating point with a ratio of Bm/Hm of approxiing structure for focusing an X-band klystron of the type shown in FIG. 1 having a gap length between poles ll and'l2 of 1.8 inches and providing a magnetic field of an averageintensity of 2,200 gauss within'the beam path weighs approximately 14 pounds. Several problems, aside from weight, are encountered in the structure of FIG. 2. One of these problems is that if the magnets 13 and 14 are not properly balanced, i.e., of equal prior art magnet structure of FIG. 2 by substitution of more powerful permanent magnets, such as one of the rare earth cobalt magnets, for example samarium cobalt, .it is found that excessive leakage of magnetic flux around the permanent magnets is experienced. More particularly, as shown in FIG. 3, the Bm v. Hm curve for samarium cobalt is shown by line 23. In order to obtain a higher energy product (Bm X Hm) for a rare earth cobalt magnet material, the load line 24 (Bm/Hm) ratio is chosen within the range of 0.8 to 1.3. This yields a higher energy product magnet than that offered by Alnico IX. However, it requires that the magnet have a larger cross-sectional area and this results in producing more self leakage of flux around the = individual magnets 13 and 14 in the geometry of FIG.
It has been found that the self leakage associated with the end regions of the magnets at 26, in FIG. 2, can be substantially eliminated by shaping the magnets 13 and 14 to figures of revolution, i.e., annular members, such that there are no end portions 26.
Referring now to FIG. 4, there is shown a magnetic beam focusing structure 31 incorporating features of the present invention. The beam focus structure 31 includes an annular gun pole piece 32 disposed at the gun end of the tube and-having an axially directed tubular projecting portion 33 surrounding the thermionic cathode emitter 34 of the electron gun 3. An annular collector pole piece 35 is disposed at the collector end of the interaction circuit region 6. A pair of annular radially polarized permanent magnets 36 and 37 are dis-- posed encircling the respective gun and the collector pole piece structures 32 and 35. A cylindrical magnetic return yoke 38, as of soft iron surrounds both the gun and collector permanent magnets 36 and 37 and the intervening region therebetween. The yoke 38 is apertured for access to the tuners 9 and for'passage of the wave-guides through the yoke.
The permanent magnets 36 and 37 are preferably rare earth cobalt magnets operated in a region having a ratio of (Bm/Hm)within the range of 0.8 to 1.3, as indicated by the cross-hatched region of the plot of FIG. 3. Magnets 36 and'37 are oppositely radially polarized as shown by the arrows of FIG. 4 to produce an axial magnetic focusing field B in the gap between the pole pieces 33 and 35. The mutually opposed inner faces 41 and 42 of the gun pole piece and collector pole piece, respectively, are planar and parallel to facilitate emitter of the gun such that the magnetic flux lines pass through the emitting surface perpendicular thereto to obtain a confined flow type of magnetic beam focusing.
The magnetic beam focusing structure 31 of the present invention, as used for focusing the beam of the tube of FIG. 1, results in reducing the weight of the beam focus magnetic structure by a factor of 3.5. That is, the weight is cut from 14 pounds to 4 pounds. In addition, a better beam focusing field is obtained because the cylindrical yoke 38 in combination with the annular permanent magnets 36 and 37 yields cylindrical symmetry which assures that the opposite sides of the yoke are operating at the same magnetic potential as the yoke constitutes a magnetic equipotential member.
What is claimed is: I 1. In a linear beam tube: electron gun means for forming and projecting a beam of electrons over an elongated beam path; collector means at the terminal end of the beam path for collecting and dissipating the energy of the collected electrons; electrical circuit means disposed along the beam path I intermediate said cathode means and said collector means in energy exchanging relation with the beam to produce an output signal; magnet means for magnetically focusing the beam over said beam path between said electron gun means and said collector means, said magnet 7 means including, electron gun and collector pole piece structures coaxially disposed of the beam path in axially spaced relation, said pole piece structures each being centrally apertured for passage of the beam therethrough and each being made of a magnetically permeable material, magnetically permeable magnetic yoke means coaxially disposed of said beam path and including axially spaced portions surrounding said electron gun and collector pole piece structures respectively in radially spaced relation therefrom, permanent magnet means for energizing said pole piece structures, said permanent magnet means comprising essentially only first and second axially spaced centrally apertured radially polarized permanent magnet means of opposite radial polarity interposed between said respective pole piece structures and said respective surrounding yoke portions for producing an axially directed beam focus magnetic field within the beam path and extending axially between said pair of axially spaced electron gun and I manent magnet means has-a (Bm/Hm) ratio falling within the range of 0.8 to 1.3.
5. The apparatus of claim 4 wherein said permanent I magnet material is a rare-earth-cobalt.
rected tubular projection surrounding said electron gun for shaping the magnetic field in the region of said gun to cause the beam focusing magnetic field lines to pass through said concave emitting surface generally perpendicular to said surface, whereby a magnetically confined convergent flow electron gun is obtained.
Claims (7)
1. In a linear beam tube: electron gun means for forming and projecting a beam of electrons over an elongated beam path; collector means at the terminal end of the beam path for collecting and dissipating the energy of the collected electrons; electrical circuit means disposed along the beam path intermediate said cathode means and said collector means in energy exchanging relation with the beam to produce an output signal; magnet means for magnetically focusing the beam over said beam path between said electron gun means and said collector means, said magnet means including, electron gun and collector pole piece structures coaxially disposed of the beam path in axially spaced relation, said pole piece structures each being centrally apertured for passage of the beam therethrough and each being made of a magnetically permeable material, magnetically permeable magnetic yoke means coaxially disposed of said beam path and including axially spaced portions surrounding said electron gun and collector pole piece structures respectively in radially spaced relation therefrom, permanent magnet means for energizing said pole piece structures, said permanent magnet means comprising essentially only first and second axially spaced centrally apertured radially polarized permanent magnet means of opposite radial polarity interposed between said respective pole piece structures and said respective surrounding yoke portions for producing an axially directed beam focus magnetic field within the beam path and extending axially between said pair of axially spaced electron gun and collector pole piece structures, the magnetic field within said permanent magnet means being composed of flux lines which are substantially radially directed and centered substantially at the beam axis.
2. The apparatus of claim 1 wherein said first and second permanent magnet means are each figures of revolution with an axis of revolution along the axis of the beam path.
3. The apparatus of claim 1 wherein said yoke is a figure of revolution.
4. The apparatus of claim 1 wherein each of said permanent magnet means has a (Bm/Hm) ratio falling within the range of 0.8 to 1.3.
5. The apparatus of claim 4 wherein said permanent magnet material is a rare-earth-cobalt.
6. The apparatus of claim 1 wherein said electron gun and collector pole piece structures have opposed generally planar transverse inner faces.
7. The apparatus of claim 1 wherein said electron gun includes a thermionic cathode emitter having a generally spherically concave emitting surface, and wherein said electron gun pole piece includes an axially directed tubular projection surrounding said electron gun for shaping the magnetic field in the region of said gun to cause the beam focusing magnetic field lines to pass through said concave emitting surface generally perpendicular to said surface, whereby a magnetically confined convergent flow electron gun is obtained.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US291117A US3896329A (en) | 1972-09-21 | 1972-09-21 | Permanent magnet beam focus structure for linear beam tubes |
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| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US291117A US3896329A (en) | 1972-09-21 | 1972-09-21 | Permanent magnet beam focus structure for linear beam tubes |
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| US3896329A true US3896329A (en) | 1975-07-22 |
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| US291117A Expired - Lifetime US3896329A (en) | 1972-09-21 | 1972-09-21 | Permanent magnet beam focus structure for linear beam tubes |
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Cited By (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE3149254A1 (en) * | 1980-12-15 | 1982-12-30 | Varian Associates, Inc., 94303 Palo Alto, Calif. | MAGNETIC CONSTRUCTION FOR FOCUSING A LINEAR ELECTRON BEAM |
| US5378988A (en) * | 1993-01-22 | 1995-01-03 | Pulyer; Yuly M. | MRI system having high field strength open access magnet |
| US5805044A (en) * | 1994-02-15 | 1998-09-08 | The United States Of America As Represented By The Secretary Of The Army | Field free chamber in permanent magnet solenoids |
| US6147447A (en) * | 1997-06-13 | 2000-11-14 | Thomson Tubes Electroniques | Electronic gun for multibeam electron tube and multibeam electron tube with the electron gun |
| US20070164841A1 (en) * | 2006-01-18 | 2007-07-19 | Prime Electronics And Satellitics Incorporation | High-frequency filter |
| US20160078992A1 (en) * | 2014-09-11 | 2016-03-17 | Larry R. Barnett | Compact magnet system for a high-power millimeter-wave gyrotron |
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| US2936394A (en) * | 1955-07-18 | 1960-05-10 | Hughes Aircraft Co | Electron gun |
| US2956193A (en) * | 1957-07-11 | 1960-10-11 | Philips Corp | Magnet system for travelling wave tubes |
| US3133226A (en) * | 1960-10-07 | 1964-05-12 | Westinghouse Electric Corp | Magnetic structure for traveling wave tubes |
| US3141116A (en) * | 1961-04-27 | 1964-07-14 | Telefunken Patent | Magnetic device for focusing an electron beam |
| US3255370A (en) * | 1961-11-17 | 1966-06-07 | Sylvania Electric Prod | High convergence electron gun with magnetically shielded cathode |
| US3324433A (en) * | 1963-12-27 | 1967-06-06 | Hitachi Ltd | Electron lens system excited by at least one permanent magnet |
| US3375400A (en) * | 1964-11-02 | 1968-03-26 | Gen Electric | Radial magnet beam focusing system |
-
1972
- 1972-09-21 US US291117A patent/US3896329A/en not_active Expired - Lifetime
Patent Citations (7)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US2936394A (en) * | 1955-07-18 | 1960-05-10 | Hughes Aircraft Co | Electron gun |
| US2956193A (en) * | 1957-07-11 | 1960-10-11 | Philips Corp | Magnet system for travelling wave tubes |
| US3133226A (en) * | 1960-10-07 | 1964-05-12 | Westinghouse Electric Corp | Magnetic structure for traveling wave tubes |
| US3141116A (en) * | 1961-04-27 | 1964-07-14 | Telefunken Patent | Magnetic device for focusing an electron beam |
| US3255370A (en) * | 1961-11-17 | 1966-06-07 | Sylvania Electric Prod | High convergence electron gun with magnetically shielded cathode |
| US3324433A (en) * | 1963-12-27 | 1967-06-06 | Hitachi Ltd | Electron lens system excited by at least one permanent magnet |
| US3375400A (en) * | 1964-11-02 | 1968-03-26 | Gen Electric | Radial magnet beam focusing system |
Cited By (8)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE3149254A1 (en) * | 1980-12-15 | 1982-12-30 | Varian Associates, Inc., 94303 Palo Alto, Calif. | MAGNETIC CONSTRUCTION FOR FOCUSING A LINEAR ELECTRON BEAM |
| US4387323A (en) * | 1980-12-15 | 1983-06-07 | Varian Associates, Inc. | Permanent magnet structure for linear-beam electron tubes |
| US5378988A (en) * | 1993-01-22 | 1995-01-03 | Pulyer; Yuly M. | MRI system having high field strength open access magnet |
| US5805044A (en) * | 1994-02-15 | 1998-09-08 | The United States Of America As Represented By The Secretary Of The Army | Field free chamber in permanent magnet solenoids |
| US6147447A (en) * | 1997-06-13 | 2000-11-14 | Thomson Tubes Electroniques | Electronic gun for multibeam electron tube and multibeam electron tube with the electron gun |
| US20070164841A1 (en) * | 2006-01-18 | 2007-07-19 | Prime Electronics And Satellitics Incorporation | High-frequency filter |
| US20160078992A1 (en) * | 2014-09-11 | 2016-03-17 | Larry R. Barnett | Compact magnet system for a high-power millimeter-wave gyrotron |
| US9711314B2 (en) * | 2014-09-11 | 2017-07-18 | Larry R. Barnett | Compact magnet system for a high-power millimeter-wave gyrotron |
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