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Resonant X-ray magnetic diffraction experiments on SmB$$_2$$C$$_2$$

SmB$$_2$$C$$_2$$のX線共鳴磁気回折実験

稲見 俊哉; 本間 徹生*; 筒井 智嗣*; 犬童 健太郎*; 小野寺 秀也*; 石井 賢司; 大和田 謙二; 葛下 かおり*; 中尾 裕則*; 村上 洋一*

Inami, Toshiya; Homma, Tetsuo*; Tsutsui, Satoshi*; Indo, Kentaro*; Onodera, Hideya*; Ishii, Kenji; Owada, Kenji; Kuzushita, Kaori*; Nakao, Hironori*; Murakami, Yoichi*

われわれはSmB$$_2$$C$$_2$$$$T_{rm N2}$$=37Kと$$T_{rm N1}$$=51Kの逐次相転移を共鳴X線回折で調べた。強い共鳴回折がSmの$$L_3$$吸収端で$$T_{rm N2}$$以下では101反射に観測され、一方、中間相では、非整合な$${vec Q}$$=(1$$pmdelta$$, $$pmdelta$$,1)の位置に観測された($$delta$$=0.13)。したがって、SmB$$_2$$C$$_2$$の逐次相転移は整合-非整合磁気相転移であることがわかった。

We investigated successive phase transitions in SmB$$_2$$C$$_2$$ at $$T_{rm N2}$$=37K and $$T_{rm N1}$$=51K by means of resonant X-ray diffraction. Strong resonant diffraction signal is observed at the 101 reflection below $$T_{rm N2}$$ at the Sm $$L_3$$ edge, whereas in the intermediate phase signals appear at incommensurate positions $${vec Q}$$=(1$$pmdelta$$, $$pmdelta$$,1) where $$delta$$=0.13. Accordingly, the successive phase transitions in SmB$$_2$$C$$_2$$ is found to be commensurate-to-incommensurate magnetic phase transitions.

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