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晶格效应和熵释放在 spin-liquid 候选物 kappa-(BEDT-TTF)2Cu2(CN)3 的低温相变中。

Lattice effects and entropy release at the low-temperature phase transition in the spin-liquid candidate kappa-(BEDT-TTF)2Cu2(CN)3.

机构信息

Physikalisches Institut, J. W. Goethe-Universität Frankfurt(M), SFB/TR49, D-60438 Frankfurt(M), Germany.

出版信息

Phys Rev Lett. 2010 Jan 8;104(1):016403. doi: 10.1103/PhysRevLett.104.016403. Epub 2010 Jan 7.

Abstract

The spin-liquid candidate kappa-(BEDT-TTF)2Cu2(CN)3 has been studied by measuring the uniaxial expansion coefficients alpha(i), the specific heat, and magnetic susceptibility. Special emphasis was placed on the mysterious anomaly around 6 K--a potential spin-liquid instability. Distinct and strongly anisotropic lattice effects have been observed at 6 K, clearly identifying this feature as a second-order phase transition. Owing to the large anomalies in alpha(i), the application of Grüneisen scaling has enabled us to determine the corresponding specific heat contribution and the entropy release. Comparison of the latter with available spin models suggests that spin degrees of freedom alone cannot account for the phase transition. Scenarios involving charge degrees of freedom are discussed.

摘要

κ-(BEDT-TTF)2Cu2(CN)3 自旋液体候选材料的各向异性晶格效应和相变的研究:通过测量单轴各向异性系数 α(i)、比热和磁化率来研究。特别关注 6K 左右的神秘异常现象——这可能是一个自旋液体不稳定性的潜在迹象。在 6K 时观察到了明显且强烈各向异性的晶格效应,这清楚地将该特征标识为二级相变。由于 α(i)的大异常,格林艾森标度的应用使我们能够确定相应的比热贡献和熵释放。将后者与现有的自旋模型进行比较表明,仅自旋自由度不能解释相变。讨论了涉及电荷自由度的情况。

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