# Nodeless superconductivity and preserved time-reversal symmetry in the   noncentrosymmetric Mo3P superconductor

**Authors:** T. Shang, J. Philippe, J. A. T. Verezhak, Z. Guguchia, J. Z. Zhao,, L.-J. Chang, M. K. Lee, D. J. Gawryluk, E. Pomjakushina, M. Shi, M. Medarde,, H.-R. Ott, and T. Shiroka

arXiv: 1905.04726 · 2019-05-24

## TL;DR

This study reveals that Mo3P is a nodeless superconductor with preserved time-reversal symmetry, exhibiting conventional BCS-like behavior and fully-gapped superconductivity at 5.5 K.

## Contribution

It provides the first comprehensive microscopic characterization of Mo3P, demonstrating its nodeless, spin-singlet superconductivity with preserved time-reversal symmetry.

## Key findings

- Superconducting transition temperature T_c = 5.5 K
- Fully-gapped superconducting state with Δ_0 = 0.83 meV
- No spontaneous magnetic fields indicating preserved time-reversal symmetry

## Abstract

We report a comprehensive study of the noncentrosymmetric superconductor Mo$_3$P. Its bulk superconductivity, with $T_c = 5.5$ K, was characterized via electrical resistivity, magnetization, and heat-capacity measurements, while its microscopic electronic properties were investigated by means of muon-spin rotation/relaxation ($\mu$SR) and nuclear magnetic resonance (NMR) techniques. In the normal state, NMR relaxation data indicate an almost ideal metallic behavior, confirmed by band-structure calculations, which suggest a relatively high electron density of states, dominated by the Mo $4d$-orbitals. The low-temperature superfluid density, determined via transverse-field $\mu$SR and electronic specific heat, suggest a fully-gapped superconducting state in Mo$_3$P, with $\Delta_0= 0.83$ meV, the same as the BCS gap value in the weak-coupling case, and a zero-temperature magnetic penetration depth $\lambda_0 = 126$ nm. The absence of spontaneous magnetic fields below the onset of superconductivity, as determined from zero-field $\mu$SR measurements, indicates a preserved time-reversal symmetry in the superconducting state of Mo$_3$P and, hence, spin-singlet pairing.

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Source: https://tomesphere.com/paper/1905.04726