Single-gap isotropic $s-$wave superconductivity in single crystals AuSn$_4$
Sunil Ghimire, Kamal R. Joshi, Elizabeth H. Krenkel, Makariy A. Tanatar, Marcin Kończykowski, Romain Grasset, Paul C. Canfield, Ruslan Prozorov
SciPost Phys. 17, 116 (2024) · published 21 October 2024
- doi: 10.21468/SciPostPhys.17.4.116
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Abstract
London, $\lambda_L (T)$, and Campbell, $\lambda_{C} (T)$, penetration depths were measured in single crystals of a topological superconductor candidate AuSn$_4$. At low temperatures, $\lambda_L (T)$ is exponentially attenuated and, if fitted with the power law, $\lambda(T) \sim T^n$, gives exponents $n>4$, indistinguishable from the isotropic single $s-$wave gap Bardeen-Cooper-Schrieffer (BCS) asymptotic. The superfluid density fits perfectly in the entire temperature range to the BCS theory. The superconducting transition temperature, $T_c = 2.40 ± 0.05$ K, does not change after 2.5 MeV electron irradiation, indicating the validity of the Anderson theorem for isotropic $s-$wave superconductors. Campbell penetration depth before and after electron irradiation shows no hysteresis between the zero-field cooling (ZFC) and field cooling (FC) protocols, consistent with the parabolic pinning potential. Interestingly, the critical current density estimated from the original Campbell theory decreases after irradiation, implying that a more sophisticated theory involving collective effects is needed to describe vortex pinning in this system. In general, our thermodynamic measurements strongly suggest that the bulk response of the AuSn$_4$ crystals is fully consistent with the isotropic $s-$wave weak-coupling BCS superconductivity.
Authors / Affiliations: mappings to Contributors and Organizations
See all Organizations.- 1 2 Sunil Ghimire,
- 1 2 Kamal R. Joshi,
- 1 2 Elizabeth H. Krenkel,
- 1 2 Makariy Tanatar,
- 3 4 5 6 7 8 Marcin Konczykowski,
- 3 4 5 6 7 8 Romain Grasset,
- 1 2 Paul Canfield,
- 1 2 Ruslan Prozorov
- 1 Ames Laboratory
- 2 Iowa State University [ISU]
- 3 École Polytechnique
- 4 Institut Polytechnique de Paris / Institut Polytechnique de Paris
- 5 Laboratoire des Solides Irradiés / Irradiated Solids Laboratory [LSI]
- 6 Commissariat à l'énergie atomique / CEA Saclay [CEA Saclay]
- 7 Institut Rayonnement-Matière de Saclay / Institut Rayonnement-Matière de Saclay [IRAMIS]
- 8 Centre National de la Recherche Scientifique / French National Centre for Scientific Research [CNRS]