# Ir 5$d$-band Derived Superconductivity in LaIr$_3$

## TL;DR

This study investigates the superconducting properties of LaIr$_3$, revealing weak-coupling, fully gapped s-wave superconductivity with a transition at 2.5 K and detailed insights into its magnetic and electronic characteristics.

## Contribution

First comprehensive analysis of LaIr$_3$'s superconductivity using muon-spin rotation and heat capacity, highlighting weak-coupling s-wave behavior and detailed magnetic properties.

## Key findings

- Superconducting transition at 2.5 K
- Type-II superconductivity with Hc2(0) = 3.84 T
- Weak-coupling s-wave superconductivity with 2Δ(0)/kBTc = 3.31

## Abstract

We have studied the superconducting properties of LaIr$_3$ with a rhombohedral structure using magnetization, heat capacity, and muon-spin rotation/relaxation ($\mu$SR) measurements. The zero-field cooled and field cooled susceptibility measurements exhibit a superconducting transition below $T_{\mathrm{C}}$ = 2.5 K. Magnetization measurements indicate bulk type-II superconductivity with upper critical field $\mu_0H_{\mathrm{c2}}(0)$ = 3.84 T. Two successive transitions are observed in heat capacity data, one at $T_{\mathrm{C}}$ = 2.5 K and a second at 1.2 K below $T_{\mathrm{C}}$ whose origin remain unclear. The heat capacity jump reveals $\Delta C$/$\gamma T_{\mathrm{C}} \sim$ 1.0 which is lower than 1.43 expected for BCS weak coupling limit. Transverse field-$\mu$SR measurements reveal a fully gapped $s-$wave superconductivity with 2$\Delta(0)/k_{\mathrm{B}}T_{\mathrm{C}}$ = 3.31, which is small compared to BCS value 3.56, suggesting weak coupling superconductivity. Moreover the study of the temperature dependence of the magnetic penetration depth estimated using the transverse field-$\mu$SR measurements gives a zero temperature value of the magnetic penetration depth $\lambda_{\mathrm{L}}(0)$ = 386(3) nm, superconducting carrier density $n_{\mathrm{s}}$ = 2.9(1) $\times$10$^{27}$ carriers $m^{-3}$ and the carriers' effective-mass enhancement $m^{*}$ = 1.53(1) $m_{\mathrm{e}}$. Our zero-field-$\mu$SR measurements do not reveal the spontaneous appearance of an internal magnetic field below the transition temperature, which indicates that time-reversal symmetry is preserved in the superconducting state of LaIr$_3$.