TY - JOUR
T1 - Ir 5d-band derived superconductivity in LaIr3
AU - Bhattacharyya, A.
AU - Adroja, D. T.
AU - Biswas, P. K.
AU - Sato, Y. J.
AU - Lees, M. R.
AU - Aoki, D.
AU - Hillier, A. D.
N1 - Publisher Copyright:
© 2019 IOP Publishing Ltd.
PY - 2020
Y1 - 2020
N2 - The superconducting properties of rhombohedral LaIr3 were examined using susceptibility, resistivity, heat capacity, and zero-field (ZF) and transverse-field (TF) muon spin relaxation and rotation (μSR) measurements. The susceptibility and resistivity measurements confirm a superconducting transition below Tc K. Two successive transitions are observed in the heat capacity data, one at Tc K and a second at 1.2 K below Tc. The heat capacity jump is ΔC/γTc 10, which is lower than 1.43 expected for Bardeen-Cooper-Schrieffer (BCS) weak-coupling limit. TF-μSR measurements reveal a fully gapped s-wave superconductivity with 2Δ(0)/kbTc=3.31(8), which is small compared to the BCS value of 3.56, suggesting weak-coupling superconductivity. The magnetic penetration depth, λl(0), estimated from TF-μSR gives λL(0)=386(3) nm, a superconducting carrier density ns=2.9(1)×1027 carriers m-3 and a carrier effective-mass enhancement factor m*=1.53(1)me. ZF-μSR data show no evidence for any spontaneous magnetic fields below Tc, which demonstrates that time-reversal symmetry is preserved in the superconducting state of LaIr3.
AB - The superconducting properties of rhombohedral LaIr3 were examined using susceptibility, resistivity, heat capacity, and zero-field (ZF) and transverse-field (TF) muon spin relaxation and rotation (μSR) measurements. The susceptibility and resistivity measurements confirm a superconducting transition below Tc K. Two successive transitions are observed in the heat capacity data, one at Tc K and a second at 1.2 K below Tc. The heat capacity jump is ΔC/γTc 10, which is lower than 1.43 expected for Bardeen-Cooper-Schrieffer (BCS) weak-coupling limit. TF-μSR measurements reveal a fully gapped s-wave superconductivity with 2Δ(0)/kbTc=3.31(8), which is small compared to the BCS value of 3.56, suggesting weak-coupling superconductivity. The magnetic penetration depth, λl(0), estimated from TF-μSR gives λL(0)=386(3) nm, a superconducting carrier density ns=2.9(1)×1027 carriers m-3 and a carrier effective-mass enhancement factor m*=1.53(1)me. ZF-μSR data show no evidence for any spontaneous magnetic fields below Tc, which demonstrates that time-reversal symmetry is preserved in the superconducting state of LaIr3.
KW - D-band superconductivity
KW - Muon spin spectroscopy
KW - Superconducting gap structure
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U2 - 10.1088/1361-648X/ab4389
DO - 10.1088/1361-648X/ab4389
M3 - Article
C2 - 31509814
AN - SCOPUS:85075814064
SN - 0953-8984
VL - 32
JO - Journal of Physics Condensed Matter
JF - Journal of Physics Condensed Matter
IS - 6
M1 - 065602
ER -