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三角格子量子自旋液体中的自旋晶格去耦

Spin-lattice decoupling in a triangular-lattice quantum spin liquid.

机构信息

National Institute for Materials Science, Tsukuba, Ibaraki, 305-0003, Japan.

Condensed Molecular Materials Laboratory, RIKEN, Wako, Saitama, 351-0198, Japan.

出版信息

Nat Commun. 2018 Apr 17;9(1):1509. doi: 10.1038/s41467-018-04005-1.

Abstract

A quantum spin liquid (QSL) is an exotic state of matter in condensed-matter systems, where the electron spins are strongly correlated, but conventional magnetic orders are suppressed down to zero temperature because of strong quantum fluctuations. One of the most prominent features of a QSL is the presence of fractionalized spin excitations, called spinons. Despite extensive studies, the nature of the spinons is still highly controversial. Here we report magnetocaloric-effect measurements on an organic spin-1/2 triangular-lattice antiferromagnet, showing that electron spins are decoupled from a lattice in a QSL state. The decoupling phenomena support the gapless nature of spin excitations. We further find that as a magnetic field is applied away from a quantum critical point, the number of spin states that interact with lattice vibrations is strongly reduced, leading to weak spin-lattice coupling. The results are compared with a model of a strongly correlated QSL near a quantum critical point.

摘要

量子自旋液体(QSL)是凝聚态系统中一种奇特的物质状态,其中电子自旋强烈相关,但由于强量子涨落,传统的磁有序被抑制到零温度。QSL 的最突出特征之一是存在分数化的自旋激发,称为自旋子。尽管进行了广泛的研究,但自旋子的性质仍然存在很大争议。在这里,我们报告了对有机自旋 1/2 三角晶格反铁磁体的磁热效应测量,结果表明电子自旋在 QSL 状态下与晶格解耦。这种去耦现象支持了自旋激发的无能隙性质。我们进一步发现,当磁场偏离量子临界点施加时,与晶格振动相互作用的自旋态的数量会大大减少,导致自旋-晶格耦合较弱。结果与量子临界点附近强关联 QSL 的模型进行了比较。

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