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

Research output: Contribution to conference › Paper › peer-review

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.

Original language	English
Pages	14-15
Number of pages	2
Publication status	Published - 1997 Jan 1
Externally published	Yes
Event	Proceedings of the 1997 Pacific Rim Conference on Lasers and Electro-Optics, CLEO/Pacific Rim - Chiba, Jpn Duration: 1997 Jul 14 → 1997 Jul 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

Electronic, Optical and Magnetic Materials
Atomic and Molecular Physics, and Optics
Condensed Matter Physics
Electrical and Electronic Engineering

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Pico second CO₂ laser system as a laser-Compton scattering source for high power and high repetition-rated γ-ray generation. / Tsunemi, Akira; Endo, Akira; Washio, Masakazu; Hirose, Tachishige; Kurihara, Yoshimasa; Oomori, Tsunehiko; Urakawa, Junji.

1997. 14-15 Paper presented at Proceedings of the 1997 Pacific Rim Conference on Lasers and Electro-Optics, CLEO/Pacific Rim, Chiba, Jpn, .

Research output: Contribution to conference › Paper › peer-review

Tsunemi, Akira ; Endo, Akira ; Washio, Masakazu ; Hirose, Tachishige ; Kurihara, Yoshimasa ; Oomori, Tsunehiko ; Urakawa, Junji. / Pico second CO₂ laser system as a laser-Compton scattering source for high power and high repetition-rated γ-ray generation. Paper presented at Proceedings of the 1997 Pacific Rim Conference on Lasers and Electro-Optics, CLEO/Pacific Rim, Chiba, Jpn, .2 p.

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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.",

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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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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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