JPH0660819A - Millimeter wave band connecting cavity type traveling wave tube - Google Patents
Millimeter wave band connecting cavity type traveling wave tubeInfo
- Publication number
- JPH0660819A JPH0660819A JP20991492A JP20991492A JPH0660819A JP H0660819 A JPH0660819 A JP H0660819A JP 20991492 A JP20991492 A JP 20991492A JP 20991492 A JP20991492 A JP 20991492A JP H0660819 A JPH0660819 A JP H0660819A
- Authority
- JP
- Japan
- Prior art keywords
- type traveling
- cavity type
- mode
- traveling wave
- millimeter wave
- 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.)
- Pending
Links
Landscapes
- Microwave Tubes (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明は、ミリ波帯結合空胴型進
行波管に関し、特に高周波回路部を構成する空胴構造に
関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a millimeter wave band coupled cavity type traveling wave tube, and more particularly to a cavity structure constituting a high frequency circuit section.
【0002】[0002]
【従来の技術】従来のミリ波帯結合空胴型進行波管の高
周波回路部の空胴構造は、図2(a),(b)の断面図
に示すように、空胴1は空胴内に2πモードでの発振を
抑制するために2πモードでの周波数でマイクロ波の吸
収特性をもつロス体2と共に2πモード周波数から動作
周波数の間の高インピーダンス領域での発振防止用ロス
体3を配置していた。2. Description of the Related Art The cavity structure of a high frequency circuit of a conventional millimeter wave band coupled cavity type traveling wave tube has a cavity 1 as shown in the sectional views of FIGS. 2 (a) and 2 (b). In order to suppress the oscillation in the 2π mode, a loss body 2 having microwave absorption characteristics at a frequency in the 2π mode and a loss body 3 for preventing oscillation in a high impedance region between the 2π mode frequency and the operating frequency are provided. Had been placed.
【0003】[0003]
【発明が解決しようとする課題】上述した従来の結合空
胴型進行波管の空胴構造は、2πモードの周波数及び2
πモード周波数から動作周波数の間で吸収特性をもつ2
種類のロス体を配することにより発振を抑制していた
が、近年要求が高まってきているミリ波領域では、部品
寸法が非常に小さくなり、寸法精度のばらつきによりロ
ス体の吸収が所定の周波数で得られず発振が生ずるとか
動作帯域でロス量が増大し、所定の電気的特性が得られ
ないという問題点があった。The cavity structure of the conventional coupled cavity type traveling wave tube described above has a frequency of 2π mode and a frequency of 2π mode.
2 with absorption characteristics between π mode frequency and operating frequency
Oscillation was suppressed by arranging different types of loss bodies, but in the millimeter-wave region, where demand is increasing in recent years, component dimensions become extremely small, and variations in dimensional accuracy cause loss bodies to absorb a given frequency. However, there is a problem in that the amount of loss increases in the operating band and the predetermined electrical characteristics cannot be obtained.
【0004】[0004]
【課題を解決するための手段】本発明は、電子ビームを
放射,形成する電子銃部と、電子ビームとの相互作用に
よりマイクロ波を増幅させる高周波回路部と、マイクロ
波との相互作用を終えた電子ビームを一定の径に集束さ
せる集束装置部とを有するミリ波帯結合空胴型進行波管
において、高周波回路部を構成する空胴内に2πモード
の周波数及び2πモード近傍の高インピーダンスの周波
数領域での結合インピーダンスの不連続によって生ずる
発振を抑制するためのロス体として異なるSiC成分比
を有するものを配置している。SUMMARY OF THE INVENTION The present invention ends the interaction between an electron gun section that emits and forms an electron beam, a high-frequency circuit section that amplifies a microwave by the interaction with the electron beam, and the microwave. In a millimeter wave band coupled cavity type traveling wave tube having a focusing device section for focusing an electron beam to a constant diameter, a frequency of 2π mode and a high impedance near 2π mode are provided in a cavity forming a high frequency circuit section. Loss bodies having different SiC component ratios are arranged as the loss bodies for suppressing the oscillation caused by the discontinuity of the coupling impedance in the frequency domain.
【0005】[0005]
【実施例】次に本発明について図面を参照して説明す
る。図1(a),(b)は、本発明の一実施例の高周波
回路部の空胴構造を示す断面図である。図に示すように
高周波回路部を構成する空胴1に2πモード発振防止用
ロス体2と共に2πモード周波数から動作周波数の間の
高インピーダンス領域での発振防止用ロス体3が配置さ
れている。このマイクロ波吸収用ロス体は、熱伝導率の
よいMgO−SiC,BeO−SiCなどの材質を用い
ているが、このロス体のSiCの成分比率を空胴1の単
品に合せて5±0.5%、2±0.3%の範囲で所定の
範囲数に吸収特性を得るように変化させる。例えば、図
に示すロス体2はSiCの成分比率が5%、ロス体2′
は5.1%、ロス体3は2%、ロス体3′は1.9%の
ようにする。これにより、空胴1の寸法精度のばらつき
による吸収特性の変化を補正でき、発振を抑制し安定な
ミリ波帯結合空胴型進行波管を提供できる。The present invention will be described below with reference to the drawings. 1 (a) and 1 (b) are cross-sectional views showing a cavity structure of a high frequency circuit section according to an embodiment of the present invention. As shown in the figure, a loss body 2 for preventing 2π mode oscillation and a loss body 3 for preventing oscillation in a high impedance region between the 2π mode frequency and the operating frequency are arranged in a cavity 1 forming a high frequency circuit section. The microwave absorbing loss body is made of a material such as MgO-SiC or BeO-SiC having good thermal conductivity, and the SiC component ratio of this loss body is 5 ± 0 depending on the cavity 1 alone. It is changed so as to obtain the absorption characteristic within a predetermined range number within the range of 0.5% and 2 ± 0.3%. For example, the loss body 2 shown in the figure has a SiC component ratio of 5%, and the loss body 2 '
Is 5.1%, the loss body 3 is 2%, and the loss body 3'is 1.9%. This makes it possible to correct a change in absorption characteristics due to variations in the dimensional accuracy of the cavity 1, suppress oscillation, and provide a stable millimeter-wave band coupled cavity traveling wave tube.
【0006】[0006]
【発明の効果】以上説明したように本発明は、2πモー
ド周波数および2πモードから動作周波数の間の高イン
ピーダンス領域で生ずる発振を抑制するためのロス体の
SiC成分比を変化させ、空胴寸法精度のばらつきによ
る吸収特性の補正をすることによって、発振を抑制でき
ると共に動作帯域のロス量を抑制し安定なミリ波帯結合
空胴型進行波管を得ることができるという効果を有す
る。As described above, according to the present invention, the SiC component ratio of the loss body for suppressing the oscillation generated in the high impedance region between the 2π mode frequency and the 2π mode to the operating frequency is changed, and the cavity size is changed. By correcting the absorption characteristics due to variations in accuracy, it is possible to suppress oscillation and suppress the loss amount in the operating band, and obtain a stable millimeter wave band coupled cavity type traveling wave tube.
【図1】(a),(b)は本発明の一実施例の空胴の断
面図である。1A and 1B are cross-sectional views of a cavity according to an embodiment of the present invention.
【図2】(a),(b)は従来の結合空胴型進行波管の
空胴の一例の断面図である。2 (a) and 2 (b) are cross-sectional views of an example of a cavity of a conventional coupled cavity type traveling wave tube.
1 空胴 2,2′,3,3′ ロス体 1 Cavity 2,2 ', 3,3' Loss body
Claims (1)
と、前記電子ビームとの相互作用によりマイクロ波を増
幅させる高周波回路部と、前記マイクロ波の相互作用を
終えた前記電子ビームを捕捉するコレクタ部と、前記電
子ビームを一定の径に集束させる集束装置とを有するミ
リ波帯結合空胴型進行波管において、前記高周波回路部
の空胴内に2πモード近傍の高インピーダンスの周波数
領域での結合インピーダンスの不連続によって生ずる発
振を抑制するためのロス体として異なるSiC成分比を
有するものを配置することを特徴とするミリ波帯結合空
胴型進行波管。1. An electron gun section that emits and forms an electron beam, a high-frequency circuit section that amplifies a microwave by the interaction of the electron beam, and an electron beam that has completed the interaction of the microwave. In a millimeter wave band coupled cavity type traveling wave tube having a collector section and a focusing device for focusing the electron beam to a constant diameter, in a cavity of the high frequency circuit section in a high impedance frequency region near a 2π mode. 2. A millimeter wave band coupled cavity type traveling wave tube, wherein loss bodies having different SiC component ratios are arranged to suppress oscillation caused by the discontinuity of the coupling impedance.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP20991492A JPH0660819A (en) | 1992-08-06 | 1992-08-06 | Millimeter wave band connecting cavity type traveling wave tube |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP20991492A JPH0660819A (en) | 1992-08-06 | 1992-08-06 | Millimeter wave band connecting cavity type traveling wave tube |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH0660819A true JPH0660819A (en) | 1994-03-04 |
Family
ID=16580752
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP20991492A Pending JPH0660819A (en) | 1992-08-06 | 1992-08-06 | Millimeter wave band connecting cavity type traveling wave tube |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0660819A (en) |
-
1992
- 1992-08-06 JP JP20991492A patent/JPH0660819A/en active Pending
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Legal Events
Date | Code | Title | Description |
---|---|---|---|
A02 | Decision of refusal |
Free format text: JAPANESE INTERMEDIATE CODE: A02 Effective date: 19990309 |