Coexistence of local magnetism and superconductivity in the heavy-fermion CeRhAs revealed by SR studies
arXiv:2406.16575 · doi:10.1103/PhysRevB.111.115134
Abstract
The superconducting (SC) state ( = 0.3 K) of the heavy-fermion compound CeRhAs, which undergoes an unusual field-induced transition to another high-field SC state, emerges from an unknown ordered state below = 0.55 K. While an electronic multipolar order of itinerant Ce-4 states was proposed to account for the phase, the exact order parameter has not been known to date. Here, we report on muon spin relaxation (SR) studies of the magnetic and SC properties in CeRhAs single crystals at low temperatures. We reveal a magnetic origin of the order by identifying a spontaneous internal field below = 0.55 K. Furthermore, we find evidence of a microscopic coexistence of local magnetism with bulk superconductivity. Our findings open the possibility that the phase involves both dipole and higher order Ce-4 moment degrees of freedom and accounts for the unusual non-Fermi liquid behavior.
7 pages, 4 figures, and supplemental material
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Cited by in corpus (12)
- Unified picture of superconductivity and magnetism in CeRhAs
- Inversion-asymmetric itinerant antiferromagnets by the space group symmetry
- The phase diagram of CeRhAs for out-of-plane magnetic field
- Thermodynamics, elastic anomalies and excitations in the field induced phases of CeRh2As2
- Incommensuration in odd-parity antiferromagnets
- Conventional -wave Superconductivity in LaRhAs; the Analog without the 4 Electrons of CeRhAs
- Unveiling the superconducting scenario in multiphase superconductor CeRhAs from space-group symmetry analysis and DFT calculations
- Coulomb blockade thermometry based nanocalorimetry
- Composite Superconducting Orders and Magnetism in CeRhAs
- Quasiclassical theory of vortex states in locally non-centrosymmetric superconductors: application to CeRhAs
- La substitution studies on the heavy-fermion superconductor CeRhAs
- Multipolar fluctuations from localized 4f electrons in CeRh2As2