WEKO3
アイテム
ファウシュモトロンの電子運動の軌道包絡線
http://hdl.handle.net/10105/2784
http://hdl.handle.net/10105/278496e048d2-83f9-483e-8d84-0c6e6f4c87df
| 名前 / ファイル | ライセンス | アクション |
|---|---|---|
NUE21_2_71-80.pdf (341.9 kB)
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| アイテムタイプ | 紀要論文 / Departmental Bulletin Paper(1) | |||||||||
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| 公開日 | 2010-03-19 | |||||||||
| タイトル | ||||||||||
| タイトル | ファウシュモトロンの電子運動の軌道包絡線 | |||||||||
| 言語 | ||||||||||
| 言語 | jpn | |||||||||
| 資源タイプ | ||||||||||
| 資源タイプ | departmental bulletin paper | |||||||||
| 著者 |
吉田, 武尚
× 吉田, 武尚
× 楠, 陽
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| 著者(ヨミ) | ||||||||||
| 姓名 | ヨシダ, タケヒサ | |||||||||
| 著者(ヨミ) | ||||||||||
| 姓名 | クスノキ, アキラ | |||||||||
| 著者別名 | ||||||||||
| 姓名 | YOSHIDA, Takehisa | |||||||||
| 著者別名 | ||||||||||
| 姓名 | KUSUNOKI, Akira | |||||||||
| 抄録 | ||||||||||
| 内容記述タイプ | Abstract | |||||||||
| 内容記述 | When electrons travel in a longitudinal direction within a transversal parabolic potential distribution undergoing the effect of high frequency field, a disturbance is induced in the electron beam and propagats constituting the two waves, fast- and slow-waves, called the simple harmonic motion waves. The fast electron wave of this type is not only used as a parametric amplifier, but also a microwave oscillator without a slow wave circuit. We call these microwave devices by the ter of the "Fawshmotron", especially the Parametric amplifier by the "A-type "Fawshmotron". A theoritical investigation of the pumping region of this device has been described with both the coupled mode and the electron motion theories. The sign of phase velocity of the fast wave is either positive or negative depending on wether ωo/ω is greater or less than unity. The microwave devices employing an interaction between the fast wave with positive phase velocity and the circuit wave are called the "B-type Fawshmotron". On the other hand, the "C-type Fawshmotron" uses the interaction between the fast wave with negative phase velocity and the circuit wave. The operation properties of these devices were described both theoritically and experimentaly. The purpose of this paper is conserned with an envelope of the electron orbit in the interaction region to the various types of the "Fawshmotron". For the "A-type Fawshmotron", these curves are given for quantities the square of frequencies ratio A and voltage modulation coefficients. For the "B- and C-type Fawshmotron" these curves are also given for the initial phase angles of the electron injection into the interaction space. | |||||||||
| 書誌情報 |
奈良教育大学紀要. 自然科学 en : BULLETIN OF NARA UNIVERSITY OF EDUCATION. NATURAL SCIENCE 巻 21, 号 2, p. 71-80, 発行日 1972-11-15 |
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| ISSN | ||||||||||
| 収録物識別子タイプ | ISSN | |||||||||
| 収録物識別子 | 05472407 | |||||||||
| 書誌レコードID | ||||||||||
| 収録物識別子タイプ | NCID | |||||||||
| 収録物識別子 | AN00181070 | |||||||||
| 著者版フラグ | ||||||||||
| 出版タイプ | VoR | |||||||||
| その他のタイトル | ||||||||||
| その他のタイトル | Electron Orbit of the "Fawshmotron" | |||||||||
| 出版者 | ||||||||||
| 出版者 | 奈良教育大学 | |||||||||
