US3787747A - Periodic magnetically focused beam tube - Google Patents
Periodic magnetically focused beam tube Download PDFInfo
- Publication number
- US3787747A US3787747A US00278408A US3787747DA US3787747A US 3787747 A US3787747 A US 3787747A US 00278408 A US00278408 A US 00278408A US 3787747D A US3787747D A US 3787747DA US 3787747 A US3787747 A US 3787747A
- Authority
- US
- United States
- Prior art keywords
- slab
- disposed
- major face
- sheet
- magnetizable
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Lifetime
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Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J21/00—Vacuum tubes
- H01J21/02—Tubes with a single discharge path
- H01J21/18—Tubes with a single discharge path having magnetic control means; having both magnetic and electrostatic control means
-
- 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
- H01J23/0873—Magnetic focusing arrangements with at least one axial-field reversal along the interaction space, e.g. P.P.M. focusing
Definitions
- the periodic magnet structure for a periodically focused beam tube is formed by a single pair of homogeneous slabs of magnetizable material that are permanently magnetized with a pattern of magnetic poles of alternating polarity taken along the direction of the beam path.
- a pair of ceramic slabs are disposed to straddle the sheet beam and the internal planar faces of the ceramic slabs have circuits printed thereon for: electrical connections to all elements, beam forming electrodes, microwave interaction structure, edge focusing electrodes, and the beam collector electrode structure.
- the permanently magnetized slabs are disposed external to the vacuum envelope, straddling the printed circuit ceramic slabs, for focusing the beam.
- the present invention relates to the field of periodic permanent magnet focused microwave beam tubes such as traveling wave tubes and klystrons.
- tubular or sheet electron beams may be magnetically focused by means of a periodic magnetic focusing structure having a pole pattern which is characterized by poles of alternating polarity taken in the direction of the beam path.
- periodic magnetic focusing structures two types of geometries have been employed; one of which employs magnetic poles of the same polarity disposed in registration transversely across the beam and the second geometry wherein poles of opposite polarity are disposed in transverse registration across the beam path.
- the magnetic focusing structure of the first type having poles of the same polarity disposed transversely of the beam path is disclosed in U. S. Pat. No. 3,102,211 (see FIG. 13) issued Aug. 27, 1963.
- the second type of geometry wherein the poles are of opposite polarity taken transversely of the beam path is disclosed and claimed in U. S. Pat. No. 3,013,173 issued Dec. l2, 1961.
- the magnet structure has been relatively complicated because it requires a plurality of permanently magnetized magnets separated by magnetically permeable material or spacers of a different magnetic property.
- the resultant structure is relatively complicated requiring a relatively large number of parts which must be assembled around the envelope of the tube to provide a composite periodic permanent magnet beam focusing structure.
- the principal object of the present invention is the provision of an improved periodic magnetically focusedbeam tube.
- the periodic magnetic focusing structure comprises a structure of generally homogeneous permanently magnetizable material magnetized in a pattern of periodic permanent poles of alternating polarity taken in a direction along the beam path, whereby a relatively complicated periodic permanent pole geometry is obtained with an extremely simple magnetic structure.
- a microwave beam tube includes a microwave interaction structure formed on a major face of a dielectric slab facing the electron beam and a permanently magnetized pair of slabs of generally homogeneous magnetic material forms the beam focusing structure disposed external of the vacuum envelope of the tube adjacent the outside wall of the dielectric slab for causing the magnetic fields to permeate the dielectric slab and microwave interaction structure to focus the beam internally of the vacuum envelope of the tube.
- a microwave interaction structure, electrostatic beam edge focusing electrodes, electrical connections, beam forming electrode structure, and beam collector electrode structure are all formed, as by printing, on the common face of a dielectric slab facing a sheet-shaped electron beam.
- a pair of slabs of homogeneous permanently magnetizable material is disposed overlaying the dielectric slab externally of the vacuum envelope.
- the magnet structure is permanently magnetized in a pattern of periodic permanent poles of alternating polarity taken in a direction along the beam path, whereby an extremely simplified tube structure is obtained.
- a thermionic cathode is disposed intermediate the ends of two printed microwave interaction structures carried from the same face of a dielectric slab for projecting electron beams in opposite directions over the printed circuits to provide two microwave tubes within a common envelope.
- plural microwave tubes are provided within a single envelope by printing a plurality of interaction circuits in side-byside relation on a common dielectric slab and projecting a stream of electrons over the printed circuits to obtain-a plurality of microwave tubes within a common envelope.
- the permanently magnetized homogeneous slab of magnet material is flexible such that after a pattern of poles has been charged into the slab it is deformed, such as into a cylinder, to match the contour of the envelope of the beam to be focused.
- FIG. 1 is an exploded schematic perspective view of a microwave tube incorporating features of the present invention
- FIG. 1A is an enlarged detail view of an alternative edge seal embodiment for a portion of the structure of FIG. 1 delineated by line lA-IA,
- FIG. 2A is a perspective schematic view of a periodic magnetic focusing pole structure useful in the tube of FIG. 1,
- FIG. 2B is a perspective plot of the axial magnetic field intensity for the structure of FIG. 2A
- FIG. 3A is a view similar to that of-FIG. 2 depicting an alternative embodiment of the magnetic focusing structure for the tube of FIG. 1, I
- FIG. 3B is a perspective plot of the transverse magnetic field intensity for the structure of FIG. 3A.
- FIG. 4 is a schematic cross-sectional view of a sheet electron beam depicting the space charge focusing forces
- FIG. Si is a plot of transverse and lateral electric defocusing field forces versus transverse extent of the electron beam of FIG. 4,
- FIG. 6 is an enlarged cross-sectional view of a beam edge portion of the tube structure of FIG. 1 depicting the beam edge electrostatic focusing electrode structrue and its edge focusing electric field,
- FIG. 7 is a plot of collector current in milliamps versus voltage on the electrostatic beam edge focusing electrode structure,-
- FIG. 8 is a view similar to that of FIG. 1 depicting an alternative tube structure of the present invention.
- FIG. 9 is a schematic plan view of a combination oscillator and amplifier printed circuit tube incorporating features of the present invention.
- a tube 11 includes a pair of ceramic slabs l2 and 13, as of alumina or beryllia ceramic, sealed together in a gas-tight manner in spaced apart relation via the intermediary of a suitable gastight spacing structure such as spacing ring 14 as of metal or ceramic.
- the ceramic slabs l2 and 13 are sealed at their peripheries, as by brazing, to metallic sealing frames 15 and 16 which in turn are sealed together as by heliarc welding at 20.
- the frames 15 and 16 replace spacer l4 and serve as a means for sealing the vacuum envelope of the tube.
- a thermionic cathode emitter 17 is mounted to one of the ceramic plates 12 and 13, such as the lower plate 12, by soldering the heater leads of the thermionic cathode 17 to metalized leads 10 formed on the inner face of the lower ceramic plate 12.
- the thermionic cathode assembly 17 is preferably disposed at one end of the ceramic tube 11 in the space between the spaced ceramic plates 12 and 13 respectively.
- a microwave interaction structure 18, such as a meanderline, an interdigital line, a double meanderline, or an array of distributed interaction klystron cavities or the like is formed on each of the opposed inner faces of the ceramic plates 12 and 13, respectively, and a beam collector electrode plate 119 is similarly formed on both of the lower and upper ceramic plates 12 and 13.
- a pair of beam edge electrostatic beam focusing electrodes 21 are disposed at the side of each of the microwave interaction structures 18 on both the opposed inner surfaces of the lower and upper ceramic plates 12 and 13, respectively.
- a pair of sheet-shaped magnets 23 and 24 are disposed externally of the vacuum envelope abutting the outside faces of the lower and upper dielectric ceramic slabs l2 and 13, respectively.
- the sheet-shaped magnets 23 and 24 are made of a generally homogeneous permanently magnetizable magnetic material, such as ferromagnetic material, or permanently magnetizable particles embedded in a suitable binder such as silicon rubber.
- Suitable magnet materials include barium ferrite Ba Fm- 0 preferably oriented, and barium ferrite embedded in silicon rubber. Such materials preferably have a high coercive force, as of 5 2,000 Oresteds.
- the sheet-shaped magnets 23 and 24 are permanently magnetized in a pattern generally indicated with respect to magnet 24, such pattern having a plurality of laterally directed magnetic poles of alternating polarity taken in a direction along the beam path as shown schematically in FIGS. 2 and 3.
- the permanent magnet pattern is readily charged into the slab-shaped magnet 24 by placing the magnetic sheet 24 over a suitable magnetizing fixture consisting of a generally comb-shaped magnetically permeable material, as of soft iron.
- the teeth of the comb have a vane shape generally conforming to the shape of the laterally directed poles to be charged into the magnetic sheet 24.
- Energizing coils are wound about the base of the individual vane-shaped teeth of the combshaped charging fixture with the direction of current through adjacent coils being in the opposite direction such as to generate, when energized with current, poles of alternating polarity taken in the direction down the spine of the comb-shaped charging fixture.
- the magnetic fixture 24, which is to be charged, can be disposed between the mutually opposed teeth of two such comb-shaped charging fixtures with the transversely aligned opposed teeth of the combs being of opposite magnetic polarity such that the magnetic sheet 24 is charged uniformly through the sheet with poles of alternating polarity.
- the sheet 24 may be disposed over a single charging comb and charged.
- the magnetic sheet 24 is permanently magnetized with transverse directed poles opposite the ends of each of the vane-shaped teeth of the charging fixture and with longitudinal polarization in the outer regions of the fringing field between adjacent poles.
- An advantage to making the magnet structure 23 and 24 by charging the desired pole pattern is that, once a charging fixture has been made the desired magnet structure can be duplicated exactly without assembly and fabrication of individual magnets and spacers. Also, the intensity and period of the periodic magnet structure is readily varied down the length of the magnet structure by varying the ampere turns around the individual vane-shaped teeth of the charging fixture and by varying the spacing between adjacent teeth of the charging fixture.
- the slow wave circuit 18 has a lateral width of approximately 0.80 inches and an axial length of approximately 5 inches.
- the electron beam has a lateral width of approximately 0.700 inches and a thickness of approximately 0.055 inches.
- Slow wave circuits 18 are formed as by printed circuit techniques on the inner major faces of the opposed ceramic sheets 12 and 13, each slab having a thickness of approximately 0.100 inches and being spaced apart from the opposed slab by approximately 0.120 inches.
- the electrostatic beam edge focusing electrodes 21 are spaced by approximately 0.060 inches from the adjacent edge of the slow wave circuit 18 and each electrode 21 has a lateral width of approximately 0.050 inches.
- the sheet-shaped magnets 23 and 24 each have a lateral width of approximately 1.00 inches and a thickness of approximately 0.100 inches and extend for substantially the entire axial length of the tube.
- the magnet structure had a period of 0.5 inch from one north pole to the succeeding north pole taken along the beam path.
- the periodic beam focusing field had a peak longitudinal component of magnetic field intensity in the midplane of the beam of 200 gauss.
- a magnetically permeable member such as a sheet of soft iron, not shown, is preferably disposed over the outer major face of the sheet-shaped magnets 23 and 24 to serve as a return magnetic flux path of high magnetic permeability.
- FIGS. 4-6 the effect of the beam edge electrostatic focusing electrodes 21 is shown.
- the sheet-shaped electron beam is shown at 27 with electrostatic space charge defocusing forces as indicated by the arrows radiating away from the beam 27. From the direction of the arrows, it is seen that the defocusing forces are substantially transverse in the midlateral sections of the beam 27 but, near the beam edges, the defocusing forces become substantially lateral.
- FIG. 5 there is shown the relative amplitude of the transverse and lateral spacecharged defocusing electric fields. From the curve it is shown that the transverse defocusing electric field falls off as the lateral defocusing field increases.
- the beam 27 will have a certain beam voltage, as of +900 volts relative to the cathode potential.
- the beam voltage is at ground potential which is also the potential on the slow wave circuit 18 and the cathode 17 is run at a negative potential.
- the difference between the slow wave circuit potential and the cathode potential corresponds to the beam voltage.
- the beam edge focusing electrodes 21 are operated at a potential negative with respect to the beam potential and potential of the circuit 18.
- the electrostatic force on the electrons is indicated by arrows 28 and it is seen that these arrows, in the mid-transverse plane of the beam at the edge of the beam, have a maximum amplitude tending to force the electrons back toward the mid-lateral plane of the beam 27.
- the potential on the edge focusing electrodes 21 relative to the beam potential and the potential on the circuit 18 is not critical. This is shown in FIG. 7 wherein collector currents in milliamps is plotted versus voltage on the edge focus electrodes 21. From the curve it is seen that once a minimum voltage has been established between the electrostatic focus electrode and the beam voltage and circuit potential, as of 50 volts, that a further increase of the voltage difference has very little effect on beam transmission. It is also seen that a relatively high beam transmission efficiency is obtained, as of 95 percent.
- FIG. 8 there is shown an alternative microwave tube embodiment 30 of the present invention.
- the tube 30 is substantially the same as that previously described with regard to FIG. 1 with the exception that the longitudinal and lateral extent of the ceramic plates 12 and 13 has been extended to accommodate a plurality of parallel microwave interaction circuits l8 and formed on both of the mutually opposed faces of the ceramic plates 12 and 13, respectively.
- the thermionic cathode emitter assembly 17 has been moved to the center of the tube and the collector electrodes 19 are disposed at opposite ends of the ceramic slabs 12 and 13 such that the electron beams are directed from both sides of the thermionic cathode emitter 17 toward opposite ends of the individual microwave interaction circuits 18 to the collector assemblies 19 at opposite ends of the tube.
- a single cathode emitter 17 can serve to provide an electron beam for a plurality of individual tubes connected in parallel.
- the microwave circuits and the connections for the individual tubes are readily formed by printed circuit techniques such that the fabrication cost for the 10 tubes is substantially the same as it would be for one tube.
- The'RF outputs of the individual circuits 18 are taken out through suitable RF output connectors 3]. arrayed at opposite ends of the composite tube 30.
- the individual RF outputs may be used individually or connected in parallel for increasing the power output capability of the tube 30.
- the thermionic cathode 17 may comprise, for example, a directly heated thoriated tungsten ribbon.
- the microwave circuit 18 includes two circuit portions, circuit portion 18 is a forward wave amplifier circuit, and circuit portion 18 is an interdigital backward wave oscillator circuit.
- the output of the backward wave oscillator circuit 18 is fed into the input of the forward wave slow wave circuit via printed circuit line 33 disposed at the upstream end of the electron beam.
- the beam is emitted by a thermionic emitter 17 such that the sheet beam is common to both slow wave circuits l8 and 18' and is collected by a common collector electrode 19.
- the magnet may comprise a hollow cylinder which is charged with a pattern of axially spaced ring-shaped pole regions of alternating magnetic polarity taken in the axial direction along the beam path.
- two such concentrically disposed cylindrical magnets may" be employed for focusing the annular beam passable coaxially of and between the pair of cylindrical permanently magnetized magnet structures.
- said beam forming means forms a sheet-shaped beam
- said homogeneous structure includes, a generally homagnetizable member being permanently magnetized in a pattern having periodic permanent poles of alternating polarity taken in a direction along the beam path.
- said magnetizable structure comprises a slab of substantially homogeneous permanently magnetizable material having a planar face facing said beam.
- said magnet slab is a slab of ferrite magnet material.
- said magnet slab is a slab of permanently magnetizable magnet particles embedded in a binder material.
- said permanently magnetizable structure includes a pair of said magnetizable slabs disposed on opposite sides of said sheet-shaped beam with their respective major faces disposed facing a corresponding major face of said sheet-shaped beam.
- the apparatus of claim 11 including, electrostatic edge focusing electrode means disposed adjacent the edge regions of said slow wave circuit in electrical insulative relation thereto and extending along the opposte edges of said sheet-shaped beam for constraining lateral expansion of said sheet-shaped beam.
- the apparatus of claim 15 including beam collector electrode means disposed on and lying substantially entirely on said planar major face of said dielectric slab at the terminal end of said beam path.
- the apparatus of claim 16 including, beam focus electrode structure disposed on and lying substantially entirely on said planar major face of said dielectirc slab at the upstream end of said beam path intermediate said cathode emitter means and said slow wave circuit means.
- said electrical circuit means includes a pair of elongated microwave interaction structure means disposed of said major face of said dielectirc slab in end-to-end relation, and wherein said beam forming and projecting means includes a thermionic cathode emitter disposed intermediate the adjacent ends of said pair of microwave interaction structure means for projecting a pair of electron beams in opposite direction along said pair of microwave interaction structure means.
- said electrical circuit means includes a plurality of elongated microwave interaction structure means disposed on and lying substantially entirely on said major face of said dielectric slab in side-by-side relation.
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- Microwave Tubes (AREA)
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US27840872A | 1972-08-07 | 1972-08-07 |
Publications (1)
Publication Number | Publication Date |
---|---|
US3787747A true US3787747A (en) | 1974-01-22 |
Family
ID=23064862
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
US00278408A Expired - Lifetime US3787747A (en) | 1972-08-07 | 1972-08-07 | Periodic magnetically focused beam tube |
Country Status (7)
Country | Link |
---|---|
US (1) | US3787747A (fr) |
JP (1) | JPS49124962A (fr) |
DE (1) | DE2338061A1 (fr) |
FR (1) | FR2195838B1 (fr) |
GB (1) | GB1406938A (fr) |
IL (1) | IL42696A (fr) |
IT (1) | IT992766B (fr) |
Cited By (16)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3909651A (en) * | 1974-08-15 | 1975-09-30 | Us Army | Low-cost periodic permanent magnet and electrostatic focusing scheme for electron tubes |
US3971965A (en) * | 1975-03-31 | 1976-07-27 | The United States Of America As Represented By The Secretary Of The Army | Internally-focused traveling wave tube |
US3982152A (en) * | 1974-11-25 | 1976-09-21 | Raytheon Company | Cascade crossed field device |
US4107573A (en) * | 1977-02-02 | 1978-08-15 | The United States Of America As Represented By The Secretary Of The Army | Printed circuit traveling wave tube |
US4232249A (en) * | 1978-09-28 | 1980-11-04 | Bell Telephone Laboratories, Incorporated | Beam-switched traveling wave tube |
US4392078A (en) * | 1980-12-10 | 1983-07-05 | General Electric Company | Electron discharge device with a spatially periodic focused beam |
US5227691A (en) * | 1989-05-24 | 1993-07-13 | Matsushita Electric Industrial Co., Ltd. | Flat tube display apparatus |
US5712537A (en) * | 1993-01-11 | 1998-01-27 | Real Time Electronics, Corporation | High frequency scan converter |
US6700454B2 (en) | 2001-06-29 | 2004-03-02 | Zvi Yaniv | Integrated RF array using carbon nanotube cathodes |
US20040251652A1 (en) * | 2003-06-10 | 2004-12-16 | Hutchinson | Method of fabricating a magnetic coder device, and the device obtained thereby |
US20050062424A1 (en) * | 2003-06-30 | 2005-03-24 | Chiping Chen | Photonic crystal ribbon-beam traveling wave amplifier |
WO2005017938A3 (fr) * | 2003-08-12 | 2005-05-26 | Genvac Aerospace Corp | Procede et appareil pour oscillateur a ondes regressives biplanaire |
US7193485B2 (en) | 2003-08-12 | 2007-03-20 | James A. Dayton, Jr. | Method and apparatus for bi-planar backward wave oscillator |
WO2008008504A2 (fr) * | 2006-07-13 | 2008-01-17 | Manhattan Technologies, Llc | Appareil et procédé pour produire des oscillations électromagnétiques |
US20100045160A1 (en) * | 2008-08-20 | 2010-02-25 | Manhattan Technologies Ltd. | Multibeam doubly convergent electron gun |
US8723137B1 (en) * | 2012-10-17 | 2014-05-13 | Innosys, Inc | Hybrid magnet for vacuum electronic device |
Citations (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2812470A (en) * | 1954-10-22 | 1957-11-05 | Bell Telephone Labor Inc | Periodic focusing in traveling wave tubes |
US2911555A (en) * | 1957-09-04 | 1959-11-03 | Hughes Aircraft Co | Traveling-wave tube |
US3231780A (en) * | 1960-10-14 | 1966-01-25 | Sfd Lab Inc | Meandering slow wave circuit having high impedance stub support means |
US3504222A (en) * | 1966-10-07 | 1970-03-31 | Hitachi Ltd | Slow-wave circuit including meander line and shielding therefor |
US3610999A (en) * | 1970-02-05 | 1971-10-05 | Varian Associates | Slow wave circuit and method of fabricating same |
US3670196A (en) * | 1971-02-24 | 1972-06-13 | Raytheon Co | Helix delay line for traveling wave devices |
US3705327A (en) * | 1971-06-02 | 1972-12-05 | Allan W Scott | Microwave generator with interleaved focusing and interaction structures |
Family Cites Families (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3102211A (en) * | 1959-08-19 | 1963-08-27 | Varian Associates | Adiabatic beam condenser method and apparatus |
-
1972
- 1972-08-07 US US00278408A patent/US3787747A/en not_active Expired - Lifetime
-
1973
- 1973-07-09 IL IL42696A patent/IL42696A/en unknown
- 1973-07-26 DE DE19732338061 patent/DE2338061A1/de active Pending
- 1973-07-31 IT IT27320/73A patent/IT992766B/it active
- 1973-08-03 FR FR7328509A patent/FR2195838B1/fr not_active Expired
- 1973-08-03 GB GB3700473A patent/GB1406938A/en not_active Expired
- 1973-08-07 JP JP48088748A patent/JPS49124962A/ja active Pending
Patent Citations (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2812470A (en) * | 1954-10-22 | 1957-11-05 | Bell Telephone Labor Inc | Periodic focusing in traveling wave tubes |
US2911555A (en) * | 1957-09-04 | 1959-11-03 | Hughes Aircraft Co | Traveling-wave tube |
US3231780A (en) * | 1960-10-14 | 1966-01-25 | Sfd Lab Inc | Meandering slow wave circuit having high impedance stub support means |
US3504222A (en) * | 1966-10-07 | 1970-03-31 | Hitachi Ltd | Slow-wave circuit including meander line and shielding therefor |
US3610999A (en) * | 1970-02-05 | 1971-10-05 | Varian Associates | Slow wave circuit and method of fabricating same |
US3670196A (en) * | 1971-02-24 | 1972-06-13 | Raytheon Co | Helix delay line for traveling wave devices |
US3705327A (en) * | 1971-06-02 | 1972-12-05 | Allan W Scott | Microwave generator with interleaved focusing and interaction structures |
Cited By (21)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3909651A (en) * | 1974-08-15 | 1975-09-30 | Us Army | Low-cost periodic permanent magnet and electrostatic focusing scheme for electron tubes |
US3982152A (en) * | 1974-11-25 | 1976-09-21 | Raytheon Company | Cascade crossed field device |
US3971965A (en) * | 1975-03-31 | 1976-07-27 | The United States Of America As Represented By The Secretary Of The Army | Internally-focused traveling wave tube |
US4107573A (en) * | 1977-02-02 | 1978-08-15 | The United States Of America As Represented By The Secretary Of The Army | Printed circuit traveling wave tube |
US4232249A (en) * | 1978-09-28 | 1980-11-04 | Bell Telephone Laboratories, Incorporated | Beam-switched traveling wave tube |
US4392078A (en) * | 1980-12-10 | 1983-07-05 | General Electric Company | Electron discharge device with a spatially periodic focused beam |
US5227691A (en) * | 1989-05-24 | 1993-07-13 | Matsushita Electric Industrial Co., Ltd. | Flat tube display apparatus |
US5712537A (en) * | 1993-01-11 | 1998-01-27 | Real Time Electronics, Corporation | High frequency scan converter |
US6700454B2 (en) | 2001-06-29 | 2004-03-02 | Zvi Yaniv | Integrated RF array using carbon nanotube cathodes |
US7452492B2 (en) * | 2003-06-10 | 2008-11-18 | Hutchinson | Method of fabricating a magnetic coder device, and the device obtained thereby |
US20040251652A1 (en) * | 2003-06-10 | 2004-12-16 | Hutchinson | Method of fabricating a magnetic coder device, and the device obtained thereby |
US20050062424A1 (en) * | 2003-06-30 | 2005-03-24 | Chiping Chen | Photonic crystal ribbon-beam traveling wave amplifier |
US7538608B2 (en) | 2003-06-30 | 2009-05-26 | Massachusetts Institute Of Technology | Photonic crystal ribbon-beam traveling wave amplifier |
US7193485B2 (en) | 2003-08-12 | 2007-03-20 | James A. Dayton, Jr. | Method and apparatus for bi-planar backward wave oscillator |
WO2005017938A3 (fr) * | 2003-08-12 | 2005-05-26 | Genvac Aerospace Corp | Procede et appareil pour oscillateur a ondes regressives biplanaire |
CN1871764B (zh) * | 2003-08-12 | 2012-07-11 | 曼哈顿技术有限责任公司 | 双平面返波振荡器的方法和装置 |
WO2008008504A2 (fr) * | 2006-07-13 | 2008-01-17 | Manhattan Technologies, Llc | Appareil et procédé pour produire des oscillations électromagnétiques |
WO2008008504A3 (fr) * | 2006-07-13 | 2008-11-27 | Manhattan Technologies Llc | Appareil et procédé pour produire des oscillations électromagnétiques |
US7679462B2 (en) | 2006-07-13 | 2010-03-16 | Manhattan Technologies, Llc | Apparatus and method for producing electromagnetic oscillations |
US20100045160A1 (en) * | 2008-08-20 | 2010-02-25 | Manhattan Technologies Ltd. | Multibeam doubly convergent electron gun |
US8723137B1 (en) * | 2012-10-17 | 2014-05-13 | Innosys, Inc | Hybrid magnet for vacuum electronic device |
Also Published As
Publication number | Publication date |
---|---|
IT992766B (it) | 1975-09-30 |
FR2195838B1 (fr) | 1977-02-25 |
FR2195838A1 (fr) | 1974-03-08 |
IL42696A (en) | 1976-02-29 |
JPS49124962A (fr) | 1974-11-29 |
GB1406938A (en) | 1975-09-17 |
IL42696A0 (en) | 1973-10-25 |
DE2338061A1 (de) | 1974-02-21 |
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