# Nodeless Superconductivity and its Evolution with Pressure in the Layered Dirac Semimetal 2M-WS_2

## TL;DR

This study investigates the superconducting properties of 2M-WS2, a Dirac semimetal, under pressure, revealing a single-gap s-wave symmetry, a strong negative pressure effect on Tc, and weak pressure influence on superfluid density, highlighting complex superconductivity behavior.

## Contribution

The paper provides the first microscopic analysis of 2M-WS2's superconductivity under pressure, linking electronic structure changes to superconducting properties and revealing unique pressure effects.

## Key findings

- Superconductivity in 2M-WS2 has s-wave symmetry.
- Tc decreases strongly with pressure.
- Superfluid density is weakly affected by pressure.

## Abstract

The interaction between superconductivity and band topology can lead to various unconventional superconducting (SC) states, and represents a new frontier in condensed matter physics research. Recently, the transition metal dichalcogenide (TMD) system 2M-WS2 has been identified as a Dirac semimetal exhibiting both superconductivity with the highest Tc = 8.5 K among all the TMD materials and topological surface states with a single Dirac cone. Here we report on muon spin rotation (muSR) and density functional theory studies of microscopic SC properties and the electronic structure in 2M-WS2 at ambient and under hydrostatic pressures (p_max = 1.9 GPa). The SC order parameter in 2M-WS2 is determined to have single-gap s-wave symmetry. We further show a strong negative pressure effect on Tc and on the SC gap. This may be partly caused by the pressure induced reduction of the size of the electron pocket around the Gamma-point, at which a band inversion appears up to the highest applied pressure. We also find that the superfluid density ns is very weakly affected by pressure. The absence of a strong pressure effect on the superfluid density and the absence of a correlation between ns and Tc in 2M-WS2, in contrast to the other SC TMDs Td-MoTe2 and 2H-NbSe2, is explained in terms of its location in the optimal (ambient pressure) and above the optimal (under pressure) superconducting regions of the phase diagram and its large distance to the other possible competing or cooperating orders. These results hint towards a complex nature of the superconductivity in TMDs, despite the observed s-wave order parameter.