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Disorder-Induced Revival of the Bose-Einstein Condensation in Ni(Cl1-xBrx)(2)-4SC(NH2)(2) at High Magnetic Fields

机译:Ni(Cl1-xBrx)(2)-4SC(NH2)(2)中高磁场下玻色-爱因斯坦凝聚的无序诱导复兴

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摘要

Building on recent NMR experiments [A. Orlova et al., Phys. Rev. Lett. 118, 067203 (2017).], we theoretically investigate the high magnetic field regime of the disordered quasi-one-dimensional S = 1 antiferromagnetic material Ni(Cl1-xBrx)(2)-4SC(NH2)(2). The interplay between disorder, chemically controlled by Br-doping, interactions, and the external magnetic field, leads to a very rich phase diagram. Beyond the well-known antiferromagnetically ordered regime, an analog of a Bose condensate of magnons, which disappears when H >= 12.3 T, we unveil a resurgence of phase coherence at a higher field H similar to 13.6 T, induced by the doping. Interchain couplings stabilize the finite temperature long-range order whose extension in the field-temperature space is governed by the concentration of impurities x. Such a "minicondensation" contrasts with previously reported Bose-glass physics in the same regime and should be accessible to experiments.
机译:基于最近的NMR实验[A. Orlova等,《物理学报》。牧师118,067203(2017)。],我们从理论上研究了无序准一维S = 1反铁磁材料Ni(Cl1-xBrx)(2)-4SC(NH2)(2)的高磁场状态。由Br掺杂化学控制的无序,相互作用和外部磁场之间的相互作用导致了非常丰富的相图。除了众所周知的反铁磁有序机制之外,当H> = 12.3 T时,类似的强力磁玻色子凝结物消失,我们还发现了由掺杂引起的相干在与13.6 T相似的更高磁场H下的复活。链间偶联稳定了有限的温度远程范围,其在现场温度空间中的扩展由杂质x的浓度控制。这种“缩聚”与先前报道的玻色玻璃物理学在相同状态下形成对比,并且应该易于实验。

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    《Physical review letters》 |2017年第6期|067204.1-067204.6|共6页
  • 作者单位

    Univ Toulouse, CNRS, Lab Phys Theor, IRSAMC, F-31062 Toulouse, France;

    Univ Toulouse, CNRS, Lab Phys Theor, IRSAMC, F-31062 Toulouse, France;

    Univ Toulouse, CNRS, Lab Phys Theor, IRSAMC, F-31062 Toulouse, France;

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