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Multipole ordering in $$f$$-electron systems

$$f$$電子系における多極子秩序

久保 勝規 ; 堀田 貴嗣

Kubo, Katsunori; Hotta, Takashi

$$f$$電子系における多極子秩序を微視的観点から明らかにするために、われわれは$$j$$-$$j$$結合描像に基づいた$$Gamma_8$$モデルを、単純立方格子,体心立方格子,面心立方格子の3種類の格子の場合について解析した。このモデルは、$$(ffsigma)$$結合を介した跳び移り積分を持つが、われわれはその$$(ffsigma)$$に関する2次摂動論を用いて、それぞれの格子における有効モデルを導出した。さらに、それらの有効モデルに対して平均場近似を適用し、単純立方格子では$$Gamma_{3g}$$反強四極子転移、面心立方格子では$$Gamma_{2u}$$反強八極子転移、面心立方格子では縦型の三重変調$$Gamma_{5u}$$八極子転移が起こることがわかった。

In order to investigate multipole ordering in $$f$$-electron systems from a microscopic viewpoint, we study the so-called $$Gamma_8$$ models on three kinds of lattices, simple cubic (sc), bcc, and fcc, based on a $$j$$-$$j$$ coupling scheme with $$f$$-electron hopping integrals through $$(ffsigma)$$ bonding. From the $$Gamma_8$$ model, we derive an effective model for each lattice structure by using the second-order perturbation theory with respect to $$(ffsigma)$$. By further applying mean-field theory to the effective model, we find a $$Gamma_{3g}$$ antiferro-quadrupole transition for the sc lattice, a $$Gamma_{2u}$$ antiferro-octupole transition for the bcc lattice, and a longitudinal triple-$$q$$ $$Gamma_{5u}$$ octupole transition for the fcc lattice.

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パーセンタイル:22.76

分野:Physics, Condensed Matter

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