Pico second CO2 laser system as a laser-Compton scattering source for high power and high repetition-rated γ-ray generation

Akira Tsunemi; Akira Endo; Masakazu Washio; Tachishige Hirose; Yoshimasa Kurihara; Tsunehiko Oomori; Junji Urakawa

Pico second CO₂ laser system as a laser-Compton scattering source for high power and high repetition-rated γ-ray generation

Akira Tsunemi^*, Akira Endo, Masakazu Washio, Tachishige Hirose, Yoshimasa Kurihara, Tsunehiko Oomori, Junji Urakawa

^*この研究の対応する著者

研究成果: Paper › 査読

抄録

A high power pico second CO₂ laser system is proposed for the generation of high power and high repetition-rated γ-ray beams by Compton scattering. The γ-ray is adopted for the production of positron beams in the Japan Linear Collider (JLC). One hundred independently operated p-sec CO₂ laser systems are placed around the Compton interaction point and triggered with the repetition rate of 150 Hz. A reflection mirror system composed of 100 flat mirrors corresponding to each laser unit is placed around the axis of the electron beams. Each p-sec CO₂ laser system is composed of a cw-CO₂ oscillator, an optical switching section, a pre-amplifier with a regenerative amplifier system and a multiple pass main amplifier.

本文言語	English
ページ	14-15
ページ数	2
出版ステータス	Published - 1997 1月 1
外部発表	はい
イベント	Proceedings of the 1997 Pacific Rim Conference on Lasers and Electro-Optics, CLEO/Pacific Rim - Chiba, Jpn 継続期間: 1997 7月 14 → 1997 7月 18

Other

Other	Proceedings of the 1997 Pacific Rim Conference on Lasers and Electro-Optics, CLEO/Pacific Rim
City	Chiba, Jpn
Period	97/7/14 → 97/7/18

ASJC Scopus subject areas

電子材料、光学材料、および磁性材料
原子分子物理学および光学
凝縮系物理学
電子工学および電気工学

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引用スタイル

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abstract = "A high power pico second CO2 laser system is proposed for the generation of high power and high repetition-rated γ-ray beams by Compton scattering. The γ-ray is adopted for the production of positron beams in the Japan Linear Collider (JLC). One hundred independently operated p-sec CO2 laser systems are placed around the Compton interaction point and triggered with the repetition rate of 150 Hz. A reflection mirror system composed of 100 flat mirrors corresponding to each laser unit is placed around the axis of the electron beams. Each p-sec CO2 laser system is composed of a cw-CO2 oscillator, an optical switching section, a pre-amplifier with a regenerative amplifier system and a multiple pass main amplifier.",

author = "Akira Tsunemi and Akira Endo and Masakazu Washio and Tachishige Hirose and Yoshimasa Kurihara and Tsunehiko Oomori and Junji Urakawa",

year = "1997",

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T1 - Pico second CO2 laser system as a laser-Compton scattering source for high power and high repetition-rated γ-ray generation

AU - Tsunemi, Akira

AU - Endo, Akira

AU - Washio, Masakazu

AU - Hirose, Tachishige

AU - Kurihara, Yoshimasa

AU - Oomori, Tsunehiko

AU - Urakawa, Junji

PY - 1997/1/1

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N2 - A high power pico second CO2 laser system is proposed for the generation of high power and high repetition-rated γ-ray beams by Compton scattering. The γ-ray is adopted for the production of positron beams in the Japan Linear Collider (JLC). One hundred independently operated p-sec CO2 laser systems are placed around the Compton interaction point and triggered with the repetition rate of 150 Hz. A reflection mirror system composed of 100 flat mirrors corresponding to each laser unit is placed around the axis of the electron beams. Each p-sec CO2 laser system is composed of a cw-CO2 oscillator, an optical switching section, a pre-amplifier with a regenerative amplifier system and a multiple pass main amplifier.

AB - A high power pico second CO2 laser system is proposed for the generation of high power and high repetition-rated γ-ray beams by Compton scattering. The γ-ray is adopted for the production of positron beams in the Japan Linear Collider (JLC). One hundred independently operated p-sec CO2 laser systems are placed around the Compton interaction point and triggered with the repetition rate of 150 Hz. A reflection mirror system composed of 100 flat mirrors corresponding to each laser unit is placed around the axis of the electron beams. Each p-sec CO2 laser system is composed of a cw-CO2 oscillator, an optical switching section, a pre-amplifier with a regenerative amplifier system and a multiple pass main amplifier.

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