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arXiv 2608.25093cond-mat.supr-con

中心对称碲掺杂PtBi₂单晶中的体超导性探测

Probing bulk superconductivity in centrosymmetric Te-doped PtBi$_2$ single crystals

Kilian Srowik, Pablo Pedrazzini, Soumen Ash, Oksana Kvitnitskaya, Andrii Kuibarov, Susmita Changdar, Oleksandr Suvorov, Volodymyr Bezguba, Alexander Kordyuk, Ra… 展开作者

Kilian Srowik, Pablo Pedrazzini, Soumen Ash, Oksana Kvitnitskaya, Andrii Kuibarov, Susmita Changdar, Oleksandr Suvorov, Volodymyr Bezguba, Alexander Kordyuk, Rafał Kurleto, Dawid Wutke, Reza Firouzmandi, Robert Kluge, Swarnamayee Mishra, Alexander Mistonov, Saicharan Aswartham, Jochen Geck, Sergey Borisenko, Laura T. Corredor, Bernd Büchner

AI总结:

本研究合成碲掺杂PtBi₂单晶,证实其为中心对称结构,观测到临界温度约2.4K的体超导性,点接触测量显示临界温度略升至约3K,为拓扑超导研究提供了中心对称体系的实验依据。

AI中文摘要:

外尔半金属γ-PtBi₂被证实是最具前景的新型材料之一,近期被提出作为拓扑i波超导体。观测该物理现象的关键要求是其三角晶系P31m晶体结构不存在反演对称性。已有研究表明,通过电子掺杂(仅用2%的Te部分替代Bi)可轻易将结构恢复为中心对称的P$\bar{3}$m1结构。本研究合成了碲掺杂PtBi$_{2-x}$Te$_x$样品,并对标称成分为PtBi$_{1.96}$Te$_{0.04}$的选定单晶的体超导性进行了全面研究,该样品展现出约100%的最高超导体积分数。单晶XRD测量证实样品为中心对称的P$\bar{3}$m1结构,而磁化率和比热测量观测到临界温度$T_\text{c} \u2248 2.4$K的体超导性。两个不同取向的上临界场测定为:面内磁场$H^{\u2228}_{\text{c2}}(0)\u2248 6.3$kOe,面外磁场$H^{\u22a5}_{\text{c2}}(0)\u2248 4.7$kOe。电阻和点接触测量中也发现了稳定的超导性,其中点接触测量显示临界温度略有提升至$T_\text{c} \u223c 3$K。最后,ARPES测量证实了样品的中心对称结构,呈现单一表面终止且无费米弧。

英文摘要:

The Weyl semimetal $γ$-PtBi$_2$ has been shown to be one of the most promising novel materials, recently proposed as a topological i-wave superconductor. A crucial requirement for observing this physics is the absence of inversion symmetry in its trigonal $P31m$ crystal structure. Centrosymmetry has been reported to be readily restored in the $P\overline{3}m1$ structure upon electron doping, partially substituting Bi with as little as 2% Te. In this work, we synthesized Te-doped PtBi$_{2-x}$Te$_{x}$ samples and thoroughly investigated the bulk superconductivity of selected single crystals with nominal composition PtBi$_{1.96}$Te$_{0.04}$, exhibiting the highest superconducting volume fraction of $\sim100$%. Single crystal XRD measurements confirm the centrosymmetric $P\overline{3}m1$ structure in our samples, whereas bulk superconductivity with a critical temperature of $T_\mathrm{c} \approx 2.4\,$K was observed in magnetization and specific heat measurements. The upper critical fields for two different orientations were determined as $H^{\parallel}_{\mathrm{c2}}(0)\approx 6.3\,$kOe for in-plane and $H^{\perp}_{\mathrm{c2}}(0)\approx 4.7\,$kOe for out-of-plane magnetic fields. Robust superconductivity was also found in resistance and point contact measurements, where the latter showed a slight enhancement of the critical temperature up to $T_\mathrm{c} \sim 3\,$K. Finally, ARPES measurements corroborate the centrosymmetric structure of our samples, showing a single surface termination and the absence of Fermi arcs.

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