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A Compact Smith-Purcell Free-Electron Laser with a Bragg Cavity
https://nitech.repo.nii.ac.jp/records/4758
https://nitech.repo.nii.ac.jp/records/475808431c21-fd6e-41fe-adcd-ea39178cc8a3
| 名前 / ファイル | ライセンス | アクション |
|---|---|---|
本文_fulltext (596.2 kB)
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Copyright (c) 1999 IEICE http://search.ieice.org/index.html
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| Item type | 学術雑誌論文 / Journal Article(1) | |||||||||||
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| 公開日 | 2013-06-25 | |||||||||||
| タイトル | ||||||||||||
| タイトル | A Compact Smith-Purcell Free-Electron Laser with a Bragg Cavity | |||||||||||
| 言語 | en | |||||||||||
| 言語 | ||||||||||||
| 言語 | eng | |||||||||||
| 資源タイプ | ||||||||||||
| 資源タイプ識別子 | http://purl.org/coar/resource_type/c_6501 | |||||||||||
| 資源タイプ | journal article | |||||||||||
| 著者 |
Thumvongskul, Tipyada
× Thumvongskul, Tipyada
× Hirata, Akimasa
× Shiozawa, Toshiyuki
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| 著者別名 | ||||||||||||
| 姓名 | 平田, 晃正 | |||||||||||
| bibliographic_information |
en : IEICE transactions on electronics 巻 E82-C, 号 11, p. 2094-2100, 発行日 1999-11-20 |
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| 出版者 | ||||||||||||
| 出版者 | Institute of Electronics, Information and Communication Engineers | |||||||||||
| 言語 | en | |||||||||||
| ISSN | ||||||||||||
| 収録物識別子タイプ | ISSN | |||||||||||
| 収録物識別子 | 0916-8524 | |||||||||||
| item_10001_source_id_32 | ||||||||||||
| 収録物識別子タイプ | NCID | |||||||||||
| 収録物識別子 | AA10826283 | |||||||||||
| 出版タイプ | ||||||||||||
| 出版タイプ | VoR | |||||||||||
| 出版タイプResource | http://purl.org/coar/version/c_970fb48d4fbd8a85 | |||||||||||
| 内容記述 | ||||||||||||
| 内容記述タイプ | Other | |||||||||||
| 内容記述 | The growth and saturation characteristics of an electromagnetic (EM) wave in a Smith-Purcell free-electron laser (FEL) with a Bragg cavity are investigated in detail with the aid of numerical simulation based upon the fluid model of the electron beam. To analyze the problem, a two-dimensional (2-D) model of the Smith-Purcell FEL is considered. The model consists of a planar relativistic electron beam and a parallel plate metallic waveguide, which has a uniform grating carved on one plate. For confinement and extraction of EM waves, a Bragg cavity is formed by a couple of reflector gratings with proper spatial period and length, which are connected at both ends of the waveguide. The results of numerical simulation show that a compact Smith-Purcell FEL can be realized by using a Bragg cavity composed of metallic gratings. | |||||||||||
| 言語 | en | |||||||||||
