Ir 5d-band derived superconductivity in LaIr3

被引:10
作者
Bhattacharyya, A. [1 ]
Adroja, D. T. [2 ,3 ]
Biswas, P. K. [2 ]
Sato, Y. J. [4 ,5 ]
Lees, M. R. [6 ]
Aoki, D. [5 ]
Hillier, A. D. [2 ]
机构
[1] Ramakrishna Mission Vickananda Educ & Res Inst, Dept Phys, Belur Math, Howrah 711202, W Bengal, India
[2] Rutherford Appleton Lab, ISIS Facil, Didcot OX11 0QX, Oxon, England
[3] Univ Johannesburg, Highly Correlated Matter Res Grp, Phys Dept, POB 524, ZA-2006 Auckland Pk, South Africa
[4] Tohoku Univ, Grad Sch Engn, Sendai, Miyagi 9808577, Japan
[5] Tohoku Univ, Inst Mat Res, Oarai, Ibaraki 3111313, Japan
[6] Univ Warwick, Dept Phys, Coventry CV4 7AL, W Midlands, England
基金
日本学术振兴会;
关键词
superconducting gap structure; d-band superconductivity; muon spin spectroscopy; MU-SR; MOTT STATE; TRANSITION; TEMPERATURE;
D O I
10.1088/1361-648X/ab4389
中图分类号
O469 [凝聚态物理学];
学科分类号
070205 ;
摘要
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 (SR) measurements. The susceptibility and resistivity measurements confirm a superconducting transition below K. Two successive transitions are observed in the heat capacity data, one at K and a second at 1.2 K below . The heat capacity jump is , which is lower than 1.43 expected for Bardeen-Cooper-Schrieffer (BCS) weak-coupling limit. TF-SR measurements reveal a fully gapped s-wave superconductivity with , which is small compared to the BCS value of 3.56, suggesting weak-coupling superconductivity. The magnetic penetration depth, , estimated from TF-SR gives nm, a superconducting carrier density carriers m(-3) and a carrier effective-mass enhancement factor . ZF-SR data show no evidence for any spontaneous magnetic fields below , which demonstrates that time-reversal symmetry is preserved in the superconducting state of LaIr3.
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页数:7
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