首页> 外文期刊>Physical review. B, Condensed Matter And Materals Physics >Bose-Einstein condensation of triplons in the 5 = 1 tetramer antiferromagnet K_2Ni_2(MoO_4)_3: A compound close to a quantum critical point
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Bose-Einstein condensation of triplons in the 5 = 1 tetramer antiferromagnet K_2Ni_2(MoO_4)_3: A compound close to a quantum critical point

机译:5 = 1四聚体反铁磁体K_2Ni_2(MoO_4)_3中三元的玻色-爱因斯坦凝聚:一种接近量子临界点的化合物

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摘要

The structure of K_2Ni_2(MoO_4)_3 consists of S = 1 tetramers formed by Ni~(2+) ions. The magnetic susceptibility X(T) and specific heat C_P(T) data on a single crystal show a broad maximum due to the low dimensionality of the system with short-range spin correlations. A sharp peak is seen in x(T) and C_P(T) at about 1.13 K, well below the broad maximum. This is an indication of magnetic long-range order, i.e., the absence of spin gap in the ground state. Interestingly, the application of a small magnetic field (H > 0.1 T) induces magnetic behavior akin to the Bose-Einstein condensation (BEC) of triplon excitations observed in some spin-gap materials. Our results demonstrate that the temperature-field (T-H) phase boundary follows a power law (T - T_N) ∝ H~(1/a) with the exponent 1/a close to 2/3, as predicted for the BEC scenario. The observation of BEC of triplon excitations in small H infers that K_2Ni_2(MoO_4)_3 is located in the proximity of a quantum critical point, which separates the magnetically ordered and spin-gap regions of the phase diagram.
机译:K_2Ni_2(MoO_4)_3的结构由Ni〜(2+)离子形成的S = 1个四聚体组成。由于具有短程自旋相关性的系统的低维数,单晶上的磁化率X(T)和比热C_P(T)数据显示出很大的最大值。在x(T)和C_P(T)中大约1.13 K处出现一个尖锐的峰,远低于宽最大值。这表明了磁远距离顺序,即在基态中不存在自旋间隙。有趣的是,施加小磁场(H> 0.1 T)会诱发类似于某些自旋间隙材料中三重激发的Bose-Einstein凝聚(BEC)的磁行为。我们的结果表明,温度场(T-H)相界遵循幂定律(T-T_N)∝ H〜(1 / a),指数1 / a接近2/3,如BEC情景所预测。对小H中三重激发的BEC的观察表明,K_2Ni_2(MoO_4)_3位于量子临界点附近,该量子临界点将相图的磁有序和自旋间隙区域分开。

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  • 来源
    《Physical review. B, Condensed Matter And Materals Physics》 |2017年第18期|180407.1-180407.5|共5页
  • 作者单位

    School of Physics, University of Hyderabad, Central University PO, Hyderabad 500046, India,Center of Condensed Matter Sciences, National Taiwan University, Taipei 10617, Taiwan;

    Max Planck Institute for Chemical Physics of Solids, 01187 Dresden, Germany,Department of Physics, Indian Institute of Technology Madras, Chennai 600036, India;

    Department of Physics, Indian Institute of Technology Bombay, Powai, Mumbai 400076, India,Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai 400005, India;

    Department of Physics, Indian Institute of Technology Bombay, Powai, Mumbai 400076, India;

    Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai 400005, India;

    Max Planck Institute for Chemical Physics of Solids, 01187 Dresden, Germany;

    Dresden High Magnetic Field Laboratory (HLD-EMFL), Helmholtz-Zentrum Dresden-Rossendorf, 01328 Dresden, Germany;

    Center of Condensed Matter Sciences, National Taiwan University, Taipei 10617, Taiwan;

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