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Enhanced spin correlations in the Bose-Einstein condensate compound Sr_3Cr_2O_8

机译:增强Bose-Einstein缩合物化合物SR_3CR_2O_8中的增强旋转相关性

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摘要

Combined experimental and modeling studies of the magnetocaloric effect, ultrasound, and magnetostriction were performed on single-crystal samples of the spin-dimer system Sr_3Cr_2O_8 in large magnetic fields to probe the spin-correlated regime in the proximity of the field-induced XT-type antiferromagnetic order also referred to as a Bose-Einstein condensate of magnons. The magnetocaloric effect, measured under adiabatic conditions, reveals details of the field-temperature (H, T) phase diagram, a dome characterized by critical magnetic-fields H_(c1) = 30.4. H_(c2) = 62 T, and a single maximum ordering temperature T_(max)(45 T) ≃ 8 K. The sample temperature was observed to drop significantly as the magnetic field is increased, even for initial temperatures above T_(max), indicating a significant magnetic entropy associated with the field-induced closure of the spin gap. The ultrasound and magnetostriction experiments probe the coupling between the lattice degrees of freedom and the magnetism in Sr_3Cr_2O_8. Our experimental results are qualitatively reproduced by a minimalistic phenomenological model of the exchange striction by which sound waves renormalize the effective exchange couplings.
机译:在大磁场中的旋转二聚体系统SR_3CR_2O_8的单晶样品对大磁场中的单晶样品进行磁热效应,超声波和磁致伸缩的组合实验和建模研究,以探测现场诱导的XT型接近的旋转相关的状态反铁磁性阶层还称为千吨浓缩胶剂的Bose-Einstein凝结物。在绝热条件下测量的磁热效应揭示了由临界磁场H_(C1)= 30.4的临界磁场特征的穹顶的细节。 H_(C2)= 62 T,以及单个最大排序温度T_(MAX)(45t)÷8k。由于磁场增加,即使对于高于T_(MAX)的初始温度,也观察到样品温度显着下降,表示与旋转间隙的场诱导的闭合相关联的显着磁熵。超声和磁致伸缩实验在SR_3CR_2O_8中探测晶格自由度与磁性之间的耦合。我们的实验结果是通过声波重整有效交换联轴器的简约现象模型来定性再现。

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  • 来源
    《Physical review》 |2020年第16期|165144.1-165144.9|共9页
  • 作者单位

    Dresden High Magnetic Field Laboratory (HLD-EMFL) and Wuerzburg-Dresden Cluster of Excellence ct.qmat Helmholtz-Zentrum Dresden-Rossendorf 01328 Dresden Germany Institute for Solid Slate Physics University of Tokyo Kashiwa Chiba 277-8581 Japan;

    Dresden High Magnetic Field Laboratory (HLD-EMFL) and Wuerzburg-Dresden Cluster of Excellence ct.qmat Helmholtz-Zentrum Dresden-Rossendorf 01328 Dresden Germany;

    Helmholtz-Zentrum Berlin fuer Materialien und Energie 14109 Berlin Germany Department of Mathematics and Physics University of Stavanger 4036 Stavanger Norway;

    Max-Planck-Institut fuer Physik komplexer Systeme Noethnitzer Strasse 38 D-01187 Dresden Germany B.I. Verkin Institute for Low Temperature Physics and Engineering of the National Academy of Sciences of Ukraine Nauky Avenue 47 Kharkiv 61103 Ukraine;

    National High Magnetic Field Laboratory Tallahassee Florida 32310 USA;

    Dresden High Magnetic Field Laboratory (HLD-EMFL) and Wuerzburg-Dresden Cluster of Excellence ct.qmat Helmholtz-Zentrum Dresden-Rossendorf 01328 Dresden Germany;

    Dresden High Magnetic Field Laboratory (HLD-EMFL) and Wuerzburg-Dresden Cluster of Excellence ct.qmat Helmholtz-Zentrum Dresden-Rossendorf 01328 Dresden Germany College of Engineering and Technology American University of the Middle East Kuwait;

    Dresden High Magnetic Field Laboratory (HLD-EMFL) and Wuerzburg-Dresden Cluster of Excellence ct.qmat Helmholtz-Zentrum Dresden-Rossendorf 01328 Dresden Germany;

    Institute for Solid State Physics University of Tokyo Kashiwa Chiba 277-8581 Japan;

    Helmholtz-Zentrum Berlin fuer Materialien und Energie 14109 Berlin Germany;

    Helmholtz-Zentrum Berlin fuer Materialien und Energie 14109 Berlin Germany Institut fuer Festkoerperphysik Technische Universitaet Berlin 10623 Berlin Germany;

    Institute for Solid State Physics University of Tokyo Kashiwa Chiba 277-8581 Japan;

    Dresden High Magnetic Field Laboratory (HLD-EMFL) and Wuerzburg-Dresden Cluster of Excellence ct.qmat Helmholtz-Zentrum Dresden-Rossendorf 01328 Dresden Germany;

    MPA-Maglab Los Alamos National Laboratory MS-E536 Los Alamos New Mexico 87545 USA;

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