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Development of polarized positron source via laser-Compton scattering

Development of polarized positron source via laser-Compton scattering
通过激光康普顿散射开发偏振正电子源
批准号:
11554010
负责人:
OMORI Tsunehiko
金额:
$6.21万
依托单位国家:
日本
项目类别:
Grant-in-Aid for Scientific Research (B)
财政年份:
1999
资助国家:
日本
项目状态:
已结题
起止时间:
1999 至 2001

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中文摘要
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英文摘要
Studies were done at the Accelerator Test Facility (ATF) in KEK. A vacuum chamber, named Compton chamber, is developed to achieve efficient head-on collision of laser and electron beams. The results of collision experiment to generate γ-rays (Emax = 56 MeV) were as follows.1) number of generated γ-rays : 1 x 10^6/pulse2) pulse duration : about 30 p sec3) polarization of γ-ray the beam was measuredThis was the highest intensity of γ-rays generated in this energy region. And this was the first demonstration of polarization measurement of the γ-ray beam of such short pulse duration. It was demonstrated that our proposed method can generate high intensity γ-ray beam efficiently. We think this was the good progress for the development of the polarized positron source.
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K.Dobashi 他11名: "Design of polarized-positron generation system"Nuclear Instruments and Methods in Physics Research. A455. 32-35 (2000)
K. Dobashi 等 11 人:“极化正电子产生系统的设计”核仪器和物理研究方法 A455(2000)。
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T.Hirose 他8名: "Polarized Positron Source for the Linear Collider, JLC"Nuclear Instruments and Methods in Physics Research A. 455. 15-24 (2000)
T. Hirose 和其他 8 人:“线性对撞机的偏振正电子源,JLC”核仪器和物理研究方法 A. 455. 15-24 (2000)
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K.Dobashi 他11名: "Production of a Polarized positron and Measurement of Its Polarization"Nuclear Instruments and Methods in Physics Research A. 455. 32-35 (2000)
K. Dobashi 等人 11:“极化正电子的产生及其极化测量”核仪器和物理研究方法 A. 455. 32-35 (2000)
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Study of gamma-ray generation by using self-resonating enhancement optical cavity
Development of a three dimensional four mirror optical cavity for laser-Compton scattering
Efficient generation of polarized gamma-rays by using a pulse laser beam stacking cavity and an electron storage ring
Precision Study of Son-Linear QED by Observing an Energy-Angular 2D-Distribution
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