Anisotropic Physical Properties of the Kondo Semimetal CeCuAs
arXiv:2003.10794 · doi:10.7566/JPSCP.30.011020
Abstract
The recently proposed novel materials class called Weyl-Kondo semimetal (WKSM) is a time reversal invariant but inversion symmetry broken Kondo semimetal in which Weyl nodes are pushed to the Fermi level by the Kondo interaction. Here we explore whether CeCuAs may be a new WKSM candidate. We report on its single-crystal growth, structure determination and physical properties investigation. Previously published studies on polycrystalline samples suggest that it is indeed a Kondo semimetal, which is confirmed by our investigations on single crystals. X-ray diffraction reveals that CeCuAs crystallizes in a tetragonal centrosymmetric structure, although the inversion symmetry could still be broken locally due to partially occupied Cu sites. Chemical analysis results in an average occupation = 0.11(1). The electrical resistivity increases logarithmically with decreasing temperature, and saturates below 10 K. A Kondo temperature 4 K is extracted from entropy, estimated from the specific heat measurements. From Hall effect experiments, a charge carrier density of cm is extracted, a value characteristic of a semimetal. The magnetization shows pronounced anisotropy, with no evidence of magnetic ordering down to 0.4 K. We thus classify CeCuAs as a tetragonal Kondo semimetal with anisotropic magnetic properties, with a possibly broken inversion symmetry, thus fulfilling the necessary conditions for a WKSM state.
arXiv comment6 pages, 4 figures, Proceedings of the International Conference on Strongly Correlated Electron Systems (SCES2019)
References in corpus (5)
- Weyl-Kondo Semimetal in Heavy Fermion Systems
- Kondo Insulator to Semimetal Transformation Tuned by Spin-Orbit Coupling
- Anisotropic optical conductivity of the putative Kondo insulator CeRuSn
- Magnetic, electrical resistivity, heat-capacity and thermopower anomalies in CeCuAs2
- Phonon anomaly and anisotropic superconducting gap in non-centrosymmetric Li2(Pd1-xPtx)3B