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Structure of glasses for $$^{3}$$He neutron spin filter cells

$$^{3}$$Heスピンフィルター用ガラスセルの構造

坂口 佳史; 吉良 弘; 奥 隆之; 篠原 武尚; 鈴木 淳市; 酒井 健二 ; 中村 充孝; 鈴谷 賢太郎; 相澤 一也; 新井 正敏; 武田 全康; 遠藤 康夫; Chang, L.-J.; 有本 靖*; 猪野 隆*; 清水 裕彦*; 神山 崇; 大山 研司*; 平賀 晴弘*; 堤 健之*; 山田 和芳; 尾原 幸治*; 加倉井 和久

Sakaguchi, Yoshifumi; Kira, Hiroshi; Oku, Takayuki; Shinohara, Takenao; Suzuki, Junichi; Sakai, Kenji; Nakamura, Mitsutaka; Suzuya, Kentaro; Aizawa, Kazuya; Arai, Masatoshi; Takeda, Masayasu; Endo, Yasuo; Chang, L.-J.; Arimoto, Yasushi*; Ino, Takashi*; Shimizu, Hirohiko*; Kamiyama, Takashi; Oyama, Kenji*; Hiraka, Haruhiro*; Tsutsumi, Kenji*; Yamada, Kazuyoshi; Ohara, Koji*; Kakurai, Kazuhisa

In spin-exchange optical pumping, there is unknown excess relaxation, called the X-factor, that limits attainable $$^{3}$$He polarization. It is known that the X-factor depends on the glass containers. Hence, it is expected that there are cell-to-cell variations in microscopic structure among the cells and that these variations affect the attainable $$^{3}$$He polarization. However, microscopic structure of the glasses for $$^{3}$$He neutron spin filters has not been clarified yet. In this paper, we have performed precise X-ray diffraction measurements for the glasses at SPring-8 using synchrotron radiation. The structural differences are observed between several types of glasses, and also, between the GE180 glass pieces with different thermal treatment. Based on the results, the structural influence on the performance of $$^{3}$$He neutron spin filters is discussed.

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