EP0082769A1 - Multiplicateur de fréquence - Google Patents
Multiplicateur de fréquence Download PDFInfo
- Publication number
- EP0082769A1 EP0082769A1 EP82402296A EP82402296A EP0082769A1 EP 0082769 A1 EP0082769 A1 EP 0082769A1 EP 82402296 A EP82402296 A EP 82402296A EP 82402296 A EP82402296 A EP 82402296A EP 0082769 A1 EP0082769 A1 EP 0082769A1
- Authority
- EP
- European Patent Office
- Prior art keywords
- frequency
- cavity
- frequency multiplier
- axis
- magnetic field
- 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.)
- Withdrawn
Links
- 238000010894 electron beam technology Methods 0.000 claims abstract description 6
- 230000003993 interaction Effects 0.000 claims description 5
- 230000005672 electromagnetic field Effects 0.000 claims description 2
- 230000001902 propagating effect Effects 0.000 claims 1
- 238000004519 manufacturing process Methods 0.000 abstract description 3
- 238000005259 measurement Methods 0.000 abstract description 2
- 210000002381 plasma Anatomy 0.000 abstract description 2
- 230000010349 pulsation Effects 0.000 description 6
- 230000010355 oscillation Effects 0.000 description 2
- 230000001133 acceleration Effects 0.000 description 1
- 230000005540 biological transmission Effects 0.000 description 1
- 230000008878 coupling Effects 0.000 description 1
- 238000010168 coupling process Methods 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
Images
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J25/00—Transit-time tubes, e.g. klystrons, travelling-wave tubes, magnetrons
- H01J25/02—Tubes 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
- H01J25/025—Tubes 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 with an electron stream following a helical path
Definitions
- the invention relates to a frequency multiplier for the production of millimeter and sub-millimeter radio waves, operating by interaction of an electron beam and an electromagnetic wave.
- This type of tube is used for the production of high powers in the range of millimeter and sub-millimeter waves mentioned.
- the subject of the invention is a frequency multiplication arrangement making it possible to avoid these difficulties.
- the seat circuit of the electromagnetic wave in interaction with the beam is provided in two parts, the first of which resonates on a frequency close to the cyclotronic frequency f, and the second on a frequency multiple whole of this frequency, in the conditions which will be described.
- This figure shows in schematic section a frequency multiplier of the invention.
- an electron beam 6 passes through a first cavity 1, resonating with a pulsation ⁇ ) J close to ⁇ c .
- This cavity extends over such a length and has an impedance whose value is such that an oscillation at this frequency occurs there.
- This oscillation is in low amplitude operating conditions, so that in this section of the multiplier tube only a small fraction of the beam energy is expended in the interaction of the latter with the electromagnetic field of the cavity. Given the high overvoltages that we know to achieve for such cavities, it is perfectly possible nevertheless to obtain at the output 8 of the cavity 1 a beam having a large modulation depth, in the sense that it is understood in the interaction tubes in general, and speed modulation in particular.
- a part bearing the mark 5, located in front of the cavity 1 comprises, according to the art known in the art, one or more traps intended to avoid any influence of the high frequency wave on the gun whose optics is particularly delicate in this kind of tube.
- This part can also include, always according to the art, attenuating zones for the high frequency wave, for the same purpose. It consists of a slip space, equipotential for the accelerated beam; it is practically at the same continuous potential as anode 4.
- the beam then enters the cavity 2 resonating at a frequency multiple whole of the self-oscillation frequency corresponding to the previous pulsation W.
- the beam gives up a significant fraction of its energy in the form of electromagetic energy at the harmonic frequency nf (n integer); this energy is evacuated by the output guide 7, while the electrons are captured by a collector not shown in the drawing.
- the distance between the ends 8 and 9 of the two cavities can be increased compared to that of the example, so as to constitute an equipotential tunnel 10 for sliding, as in a klystron, allowing an improvement in the grouping of the electrons within the beam.
- the tunnel is advantageously at the potential of the anode, as are the cavities 1 and 2.
- the cavity l instead of being self-oscillating, can be modified (length and reduced overvoltage) so as to no longer self-oscillate; in this case it is excited by an external microwave source, not shown, operating in the vicinity of the cyclotonic frequency.
- This requires the addition to the cavity 1 of a source coupling member (loop in the case of a coaxial, iris in that of a guide, etc.).
- the frequency multiplier of the present intention preferably operates in TE mode, preferably in TE mode o, n, l
- n 2 ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ ⁇ respectively the pulsation and the wavelength considered corresponding to the frequency f for the first cavity and nf for the second.
- the opening in the center of the first cavity can, without drawback, as in the drawing, have the same dimension as in the second cavity, or a dimension substantially greater; finally, in the example, the sliding tube, chosen very short, was a small fraction of the previous smallest radius r ..
- the multiplier tube of the invention allows the generation of high-end microwave energy, with high levels. It has the same applications as the prior art generators in millimeter and sub-millimeter waves, namely, in particular, measurement in plasmas, radar transmission and telecommunications.
Landscapes
- Particle Accelerators (AREA)
- Microwave Tubes (AREA)
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
FR8124167A FR2518803A1 (fr) | 1981-12-23 | 1981-12-23 | Multiplicateur de frequence |
FR8124167 | 1981-12-23 |
Publications (1)
Publication Number | Publication Date |
---|---|
EP0082769A1 true EP0082769A1 (fr) | 1983-06-29 |
Family
ID=9265365
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP82402296A Withdrawn EP0082769A1 (fr) | 1981-12-23 | 1982-12-14 | Multiplicateur de fréquence |
Country Status (3)
Country | Link |
---|---|
EP (1) | EP0082769A1 (enrdf_load_stackoverflow) |
JP (1) | JPS58116807A (enrdf_load_stackoverflow) |
FR (1) | FR2518803A1 (enrdf_load_stackoverflow) |
Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4554484A (en) * | 1983-08-29 | 1985-11-19 | The United States Of America As Represented By The Secretary Of The Navy | Complex cavity gyrotron |
EP0141525A3 (en) * | 1983-09-30 | 1987-10-28 | Kabushiki Kaisha Toshiba | Gyrotron device |
US5038077A (en) * | 1989-01-31 | 1991-08-06 | The United States Of American As Represented By The Secretary Of The Navy | Gyroklystron device having multi-slot bunching cavities |
US5281894A (en) * | 1990-09-28 | 1994-01-25 | The United States Of America As Represented By The Secretary Of The Navy | Dual cavity for a dual frequency gyrotron |
WO1999028943A1 (en) * | 1997-11-27 | 1999-06-10 | Eev Limited | Electron beam tubes |
KR101122098B1 (ko) * | 2003-06-24 | 2012-03-15 | 알베마를 코포레이션 | 가금 가공처리시의 살균 제어 |
Citations (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2492996A (en) * | 1945-08-25 | 1950-01-03 | Sperry Corp | Tunable high-frequency cavity resonator |
US3155868A (en) * | 1959-10-14 | 1964-11-03 | Nippon Electric Co | Plural resonator cavities tuned to integrally related frequencies |
US3363138A (en) * | 1964-11-04 | 1968-01-09 | Sperry Rand Corp | Electron beam-plasma device operating at multiple harmonics of beam cyclotron frequency |
US3373309A (en) * | 1962-10-03 | 1968-03-12 | Siemens Ag | Electron beam tube for frequency multiplication |
US3389347A (en) * | 1966-09-08 | 1968-06-18 | Army Usa | Microwave noise generator |
US3457450A (en) * | 1966-08-31 | 1969-07-22 | Varian Associates | High frequency electron discharge device |
US3474283A (en) * | 1967-03-22 | 1969-10-21 | Us Navy | Cyclotron wave upconverter |
-
1981
- 1981-12-23 FR FR8124167A patent/FR2518803A1/fr active Granted
-
1982
- 1982-12-14 EP EP82402296A patent/EP0082769A1/fr not_active Withdrawn
- 1982-12-22 JP JP22575182A patent/JPS58116807A/ja active Pending
Patent Citations (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2492996A (en) * | 1945-08-25 | 1950-01-03 | Sperry Corp | Tunable high-frequency cavity resonator |
US3155868A (en) * | 1959-10-14 | 1964-11-03 | Nippon Electric Co | Plural resonator cavities tuned to integrally related frequencies |
US3373309A (en) * | 1962-10-03 | 1968-03-12 | Siemens Ag | Electron beam tube for frequency multiplication |
US3363138A (en) * | 1964-11-04 | 1968-01-09 | Sperry Rand Corp | Electron beam-plasma device operating at multiple harmonics of beam cyclotron frequency |
US3457450A (en) * | 1966-08-31 | 1969-07-22 | Varian Associates | High frequency electron discharge device |
US3389347A (en) * | 1966-09-08 | 1968-06-18 | Army Usa | Microwave noise generator |
US3474283A (en) * | 1967-03-22 | 1969-10-21 | Us Navy | Cyclotron wave upconverter |
Non-Patent Citations (1)
Title |
---|
IEEE TRANSACTIONS ON MICROWAVE THEORY AND TECHNIQUES, vol. MTT-25, no. 6, juin 1977, pages 514-521, New York (USA); * |
Cited By (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4554484A (en) * | 1983-08-29 | 1985-11-19 | The United States Of America As Represented By The Secretary Of The Navy | Complex cavity gyrotron |
EP0141525A3 (en) * | 1983-09-30 | 1987-10-28 | Kabushiki Kaisha Toshiba | Gyrotron device |
US5038077A (en) * | 1989-01-31 | 1991-08-06 | The United States Of American As Represented By The Secretary Of The Navy | Gyroklystron device having multi-slot bunching cavities |
US5281894A (en) * | 1990-09-28 | 1994-01-25 | The United States Of America As Represented By The Secretary Of The Navy | Dual cavity for a dual frequency gyrotron |
WO1999028943A1 (en) * | 1997-11-27 | 1999-06-10 | Eev Limited | Electron beam tubes |
US6465958B1 (en) | 1997-11-27 | 2002-10-15 | Eev Limited | Electron beam tubes |
KR101122098B1 (ko) * | 2003-06-24 | 2012-03-15 | 알베마를 코포레이션 | 가금 가공처리시의 살균 제어 |
Also Published As
Publication number | Publication date |
---|---|
JPS58116807A (ja) | 1983-07-12 |
FR2518803B1 (enrdf_load_stackoverflow) | 1984-10-26 |
FR2518803A1 (fr) | 1983-06-24 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
EP0013242B1 (fr) | Générateur d'ondes radioélectriques pour hyperfréquence | |
EP0413018B1 (fr) | Dispositif generateur d'ondes hyperfrequences a cathode virtuelle | |
FR2547456A1 (fr) | Tube a faisceau d'electrons module en densite avec un gain accru | |
EP0407558B1 (fr) | Dispositif amplificateur ou oscillateur fonctionnant en hyperfrequence | |
FR2499312A1 (fr) | Dispositif d'attenuation de modes pour des cavites de gyrotrons | |
EP0248689A1 (fr) | Klystron à faisceaux multiples | |
FR2760127A1 (fr) | Canon a electrons et klystron le comportant | |
EP0239466A1 (fr) | Circuit de sortie pour klystron, et klystron comportant un tel circuit de sortie | |
EP0082769A1 (fr) | Multiplicateur de fréquence | |
FR2970114A1 (fr) | Dispositif de generation d'ondes hyperfrequence ayant une cathode dont chaque extremite est raccordee a une source de tension | |
EP2472555A1 (fr) | Dispositif de génération d'ondes hyperfréquence comprenant une pluralité de magnétrons | |
FR3042063A1 (fr) | Dispositif pour generer des micro-ondes | |
EP0124396B1 (fr) | Dispositif d'injection d'un faisceau d'électrons pour générateur d'ondes radioélectriques pour hyperfréquences | |
EP2747118B1 (fr) | Cathode pour dispositif de génération d'ondes électromagnétiques, comprenant des régions d'émission mobiles les unes par rapport aux autres | |
EP0401066B1 (fr) | Dispositif d'onduleur hélicoîdal à aimants permanents pour application aux lasers à électrons libres | |
EP0124395A1 (fr) | Canon à électrons pour générateurs d'ondes radioélectriques pour hyperfréquences | |
EP0122186B1 (fr) | Générateur d'ondes radioélectriques pour hyperfréquences | |
EP1466343B1 (fr) | Tube electronique a collecteur simplifie | |
FR2526582A1 (fr) | Procede et appareil pour produire des micro-ondes | |
CA2044633A1 (fr) | Canon a electrons pour fournir des electrons groupes en impulsions courtes | |
EP2747117B1 (fr) | Dispositif de génération d'ondes hyperfréquences à double cathodes | |
FR2486305A1 (fr) | Tube amplificateur a champs croises a grand gain et ensemble d'emission radioelectrique muni d'un tel tube | |
FR2691287A1 (fr) | Nouveau circuit de sortie à interaction étendue pour un klystron relativiste large bande. | |
FR2588714A1 (fr) | Accelerateur d'ions a haute frequence | |
EP2743962B1 (fr) | Générateur d'ondes hyperfréquences et procédé de génération d'ondes associé |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
PUAI | Public reference made under article 153(3) epc to a published international application that has entered the european phase |
Free format text: ORIGINAL CODE: 0009012 |
|
AK | Designated contracting states |
Designated state(s): CH DE GB IT LI NL |
|
STAA | Information on the status of an ep patent application or granted ep patent |
Free format text: STATUS: THE APPLICATION IS DEEMED TO BE WITHDRAWN |
|
18D | Application deemed to be withdrawn |
Effective date: 19840302 |
|
RIN1 | Information on inventor provided before grant (corrected) |
Inventor name: EPSZTEIN, BERNARD |