用扫描SQUID显微镜观察超导Dirac半金属PdTe2的中间态

P. Garcia-Campos, Y. Huang, A. de Visser, K. Hasselbach
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引用次数: 3

摘要

狄拉克半金属PdTe${}_2$在温度$T_{c}=1.6$~K时变为超导。热力学和介子自旋实验支持i型超导性,这对于二元化合物来说是不寻常的。i型超导体的一个关键性质是在低于热力学临界场$H_{c}$的磁场中超导畴和正常畴(通量结构)共存的中间态。利用扫描SQUID显微镜(SSM)观察了PdTe${}_2$超导状态下的磁通结构。磁通结构具有强烈的历史依赖性,随着磁场的增大,磁通结构由圆形向层流形状转变。在地表测得的磁场振幅表明存在朗道分支。确定了中间态的畴壁宽度。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Visualization by scanning SQUID microscopy of the intermediate state in the superconducting Dirac semimetal PdTe2
The Dirac semimetal PdTe${}_2$ becomes superconducting at a temperature $T_{c}=1.6$~K. Thermodynamic and muon spin rotation experiments support type-I superconductivity, which is unusual for a binary compound. A key property of a type-I superconductor is the intermediate state which presents a coexistence of superconducting and normal domains (flux structures) at magnetic fields lower than the thermodynamic critical field $H_{c}$. By means of scanning SQUID microscopy (SSM) we observe flux structures in the superconducting state of PdTe${}_2$. The flux structures are strongly history dependent with a transition from round shapes to laminar shapes as the magnetic field is more and more increased. The field amplitudes measured at the surface are indicative for the presence of Landau branching. The domain wall width in the intermediate state has been determined.
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