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Ca$_3$Ir$_4$Sn$_{13}$: A weakly correlated nodeless superconductor

Superconductivity 2016-05-02 v1 Materials Science Strongly Correlated Electrons

Abstract

We report detailed Seebeck coefficient, Hall resistivity as well as specific heat measurement on Ca3_3Ir4_4Sn13_{13} single crystals. The Seebeck coefficient exhibits a peak corresponding to the anomaly in resistivity at TT^*, and the carrier density is suppressed significantly below TT^*. This indicates a significant Fermi surface reconstruction and the opening of the charge density wave gap at the supperlattice transition. The magnetic field induced enhancement of the residual specific heat coefficient γ(H)\gamma(H) exhibits a nearly linear dependence on magnetic field, indicating a nodeless gap. In the temperature range close to TcT_c the Seebeck coefficient can be described well by the diffusion model. The zero-temperature extrapolated thermoelectric power is very small, implying large normalized Fermi temperature. Consequently the ratio TcTF\frac{T_c}{T_F} is very small. Our results indicate that Ca3_3Ir4_4Sn13_{13} is a weakly correlated nodeless superconductor.

Keywords

Cite

@article{arxiv.1604.08948,
  title  = {Ca$_3$Ir$_4$Sn$_{13}$: A weakly correlated nodeless superconductor},
  author = {Kefeng Wang and C. Petrovic},
  journal= {arXiv preprint arXiv:1604.08948},
  year   = {2016}
}

Comments

5 pages, 5 figures