Ultrasonic Team (T. Yanagisawa, Hokkaido Univ,)    

Ultrasonic Dispersion(s) due to Rattling
in the Filled-skutterudite ROs4Sb12

Jan 02, 2010

We are focusing on investigating ultrasonic dispersion (UD) due to rattling in the ROs4Sb12 (R = La, Pr, Nd, Sm) system in order to examine a possible relationship between the unconventional superconductivity in PrOs4Sb12 [1] or magnetically robust large residual entropy in low temperature specific heat in SmOs4Sb12 [2] and its local charge degrees of freedom due to anharmonic potential [1]. Intriguingly, NdOs4Sb12 and SmOs4Sb12 show double UD with different temperature and time scales, while non-4f system LaOs4Sb12 shows only a single UD. Most recently, we found that PrOs4Sb12 also show double UD. The another dispersion occurs at around Tc ~1.8 K, where the activation energy of the lower UD is estimated a one digit smaller value of ~5 K than the values obtained 67 K for NdOs4Sb12 and 105 K for SmOs4Sb12.
By monitoring a systematic change of the UD among the Sb-based filled skutterudites, we also find that both higher and lower activation energies E1 and E2 increase and corresponding attempt times τ0, (1), τ0, (2) decrease when the rare-earth ion changes from R = La to Sm in ROs4Sb12. When the rare-earth ion changes from R = La to Sm, not only the guest ion mass but also the amount of free space for the rattler in the atomic cage increases, owing to the lanhanide contraction, i.e., the ionic radius of the guest ion decreases, and relatively rigid character of the atomic cage of Sb-based filled skutterudites. We speculate that such changes in the guest ion conditions give rise to an additional anharmonicity of the potential,e.g., flat base or double wells, for the local ionic configuration, and result in the emergence of additional UD in 4f -electron system, R = Pr, Nd and Sm.

[1] E. D. Bauer et al., Phys. Rev. B 65 (2002) 100506(R).
[2] S. Sanada et al., J. Phys. Soc. Jpn. 74 (2005) 246.
[3] T. Yanagisawa et al., J. Phys. Soc. Jpn. 80 (2011) 043601.
[4] W. M. Yuhasz et al., Phys. Rev. B 71 (2005) 104402.
[5] Y. Aoki et al., Physica B 378-380 (2006) 54.

For more information please see our paper: T. Yanagisawa et al., J. Phys. Soc. Jpn. 80 (2011) 043601.

(also available on cond-mat/1010.1387)

An Auroral Temperature-Pressure Phase Diagram
of URu2Si2

Jan 01, 2010

重い電子系化合物URu2Si2の圧力下電気抵抗測定によって作られた温度ー圧力相図です。本物質は常圧においてT = 17.5 Kで、秩序変数・秩序波数共に不明の「隠れた秩序」を示す物質です。同研究室の日高助教がインデンター型圧力セルを用いて測定しました。電気抵抗の絶対値をグラデーションで表現すると、綺麗なオーロラのようなコントラストの中に隠れた秩序相が浮かび上がります。隠れた秩序相は静水圧下(P ≧ 1 GPa)で一次転移を伴って反強磁性相に転移することがわかっていますが、対応する領域で相境界線の勾配が変化し、相境界線が若干ブロードになっていることが相図からみてとれます。
もっと詳しく知りたい方は、強相関電子磁性1研究室の研究トピックス「URu2Si2 における隠れた秩序と微弱反強磁性」 をご覧下さい。

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