Superconducting state in the non-centrosymmetric Mg_{9.3}Ir_{19}B_{16.7} and Mg_{10.5}Ir_{19}B_{17.1} revealed by NMR
arXiv:0908.2894 · doi:10.1103/PhysRevB.80.060503
Abstract
We report ^{11}B NMR measurements in non-centrosymmetric superconductors Mg_{9.3}Ir_{19}B_{16.7} (T_c=5.8 K) and Mg_{10.5}Ir_{19}B_{17.1} (T_c=4.8 K). The spin lattice relaxation rate and the Knight shift indicate that the Cooper pairs are predominantly in the spin-singlet state with an isotropic gap. However, Mg_{10.5}Ir_{19}B_{17.1} is found to have more defects and the spin susceptibility remains finite even in the zero-temperature limit. We interpret this result as that the defects enhance the spin-orbit coupling and bring about more spin-triplet component.
for a proper, high-resolution Fig.5, contact the corresponding author
References in corpus (8)
- Spin Triplet Superconducting State due to Broken Inversion Symmetry in Li_2Pt_3B
- Physical properties of the noncentrosymmetric superconductor Mg_10Ir_19B_16
- Superconductivity in RhGa and IrGa without Inversion Symmetry
- Gap structure in noncentrosymmetric superconductors
- Physical properties of noncentrosymmetric superconductor RuB
- Nodeless Superconductivity in the Noncentrosymmetric Superconductor
- Possible nodeless superconductivity in the noncentrosymmetric superconductor Mg_(12-delta)Ir_19B_16
- Signature of superconducting states in cubic crystal without inversion symmetry
Cited by in corpus (6)
- Abrupt enhancement of non-centrosymmetry and appearance of the spin-triplet superconducting state in Li_2(Pd_{1-x}Pt_{x})_3B beyond x=0.8
- Spin-singlet superconductivity with a full gap in locally non-centrosymmetric SrPtAs
- Full-gap superconductivity in non-centrosymmetric ReZr, ReZr and ReZr
- Antiferromagnetic spin fluctuations and superconductivity in NbRhB and TaRhB with a chiral crystal structure
- Pressure study of the noncentrosymmetric 5d-electron superconductors CaMSi3 (M= Ir, Pt)
- Multi-band effect in the noncentrosymmetric superconductors Mg_{12-δ}Ir_{19}B_{16} revealed by Hall effect and magnetoresistance measurements