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Antiferromagnetic ordering and chiral crystal structure transformation in Nd$$_3$$Rh$$_4$$Sn$$_{13}$$

Nd$$_3$$Rh$$_4$$Sn$$_{13}$$における反強磁性秩序とカイラル結晶構造転移

下田 愛海*; 岩佐 和晃*; 桑原 慶太郎*; 佐賀山 基*; 中尾 裕則*; 石角 元志*; 中尾 朗子*; 河村 聖子   ; 村井 直樹  ; 大原 高志   ; 南部 雄亮*

Shimoda, Ami*; Iwasa, Kazuaki*; Kuwahara, Keitaro*; Sagayama, Hajime*; Nakao, Hironori*; Ishikado, Motoyuki*; Nakao, Akiko*; Kawamura, Seiko; Murai, Naoki; Ohara, Takashi; Nambu, Yusuke*

The detailed electronic superlattice structure of the Remeika phase compound Nd$$_3$$Rh$$_4$$Sn$$_{13}$$ was investigated. The material undergoes a structural phase transition at $$T_{rm D} simeq 338$$~K between the high temperature phase ($$Pmbar{3}n$$) and the low temperature chiral structure phase ($$I2_{1}$$3), which is the same symmetry change as that of the La- and Ce-based Remeika phase compounds. The inequivalent Nd-ion sites in the chiral phase are occupied by different crystalline electronic field splitting schemes of the 4$$f^3$$ electronic configuration with the total angular moment $$J = 9/2$$, which results in two-sublattice antiferromagnetic ordering below $$T_{rm N}$$ = 1.65 K. The one-dimensional Nd-ion chains in which the magnetic moments are alternately arranged are connected via the second-neighbor triangular lattice in the chiral phase, which suggests a magnetic frustration effect.

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パーセンタイル:52.00

分野:Materials Science, Multidisciplinary

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