Watanabe Daiki, Sugii Kaori, Shimozawa Masaaki, Suzuki Yoshitaka, Yajima Takeshi, Ishikawa Hajime, Hiroi Zenji, Shibauchi Takasada, Matsuda Yuji, Yamashita Minoru
Institute for Solid State Physics, University of Tokyo, Chiba 277-8581, Japan; Department of Physics, Kyoto University, Kyoto 606-8502, Japan;
Institute for Solid State Physics, University of Tokyo, Chiba 277-8581, Japan;
Proc Natl Acad Sci U S A. 2016 Aug 2;113(31):8653-7. doi: 10.1073/pnas.1524076113. Epub 2016 Jul 20.
When quantum fluctuations destroy underlying long-range ordered states, novel quantum states emerge. Spin-liquid (SL) states of frustrated quantum antiferromagnets, in which highly correlated spins fluctuate down to very low temperatures, are prominent examples of such quantum states. SL states often exhibit exotic physical properties, but the precise nature of the elementary excitations behind such phenomena remains entirely elusive. Here, we use thermal Hall measurements that can capture the unexplored property of the elementary excitations in SL states, and report the observation of anomalous excitations that may unveil the unique features of the SL state. Our principal finding is a negative thermal Hall conductivity [Formula: see text] which the charge-neutral spin excitations in a gapless SL state of the 2D kagomé insulator volborthite Cu3V2O7(OH)2[Formula: see text]2H2O exhibit, in much the same way in which charged electrons show the conventional electric Hall effect. We find that [Formula: see text] is absent in the high-temperature paramagnetic state and develops upon entering the SL state in accordance with the growth of the short-range spin correlations, demonstrating that [Formula: see text] is a key signature of the elementary excitation formed in the SL state. These results suggest the emergence of nontrivial elementary excitations in the gapless SL state which feel the presence of fictitious magnetic flux, whose effective Lorentz force is found to be less than 1/100 of the force experienced by free electrons.
当量子涨落破坏潜在的长程有序状态时,新型量子态就会出现。受挫量子反铁磁体的自旋液体(SL)态,其中高度相关的自旋波动到非常低的温度,就是这类量子态的突出例子。SL态通常表现出奇异的物理性质,但这类现象背后基本激发的精确性质仍然完全难以捉摸。在这里,我们使用能够捕捉SL态中基本激发未被探索性质的热霍尔测量,并报告对可能揭示SL态独特特征的反常激发的观测。我们的主要发现是二维 Kagomé 绝缘体硫钒铜矿Cu3V2O7(OH)2·2H2O的无隙SL态中的电荷中性自旋激发表现出负的热霍尔电导率[公式:见原文],其方式与带电电子表现出传统电霍尔效应的方式非常相似。我们发现,在高温顺磁态中不存在[公式:见原文],并且随着进入SL态,随着短程自旋关联的增长而出现,这表明[公式:见原文]是SL态中形成的基本激发的关键特征。这些结果表明,在无隙SL态中出现了非平凡的基本激发,它们感受到虚拟磁通量的存在,其有效洛伦兹力被发现小于自由电子所经历力的1/100。