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

被引:16
|
作者
Isono, Takayuki [1 ,3 ]
Sugiura, Shiori [1 ]
Terashima, Taichi [1 ]
Miyagawa, Kazuya [2 ]
Kanoda, Kazushi [2 ]
Uji, Shinya [1 ]
机构
[1] Natl Inst Mat Sci, Tsukuba, Ibaraki 3050003, Japan
[2] Univ Tokyo, Dept Appl Phys, Bunkyo Ku, Tokyo 1138656, Japan
[3] RIKEN, Condensed Mol Mat Lab, Wako, Saitama 3510198, Japan
来源
NATURE COMMUNICATIONS | 2018年 / 9卷
关键词
STATE;
D O I
10.1038/s41467-018-04005-1
中图分类号
O [数理科学和化学]; P [天文学、地球科学]; Q [生物科学]; N [自然科学总论];
学科分类号
07 ; 0710 ; 09 ;
摘要
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 anti-ferromagnet, 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.
引用
收藏
页数:6
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