Weak superconducting fluctuations and small anisotropy of the upper critical fields in an Fe1.05Te0.85Se0.15 single crystal
arXiv:1003.1171 · doi:10.1143/JPSJ.79.074706
Abstract
We have investigated the temperature dependence of the resistive upper critical fields () for an FeTeSe single crystal, which exhibit superconductivity at μ_{0}H_{\rm c2}^{ab}(T)H \parallel abμ_{0}H_{\rm c2}(0) \approx 47 T is seen for both and . This fact is almost identical to the results of FeTeSe single crystals reported previously. We have discussed that the small anisotropy of the upper critical field at low temperatures in Fe(Te,Se) systems against the variation of the Te/Se ratio.
10 pages, 4 figures
References in corpus (11)
- Superconductivity at 38 K in the iron arsenide (Ba1-xKx)Fe2As2
- Superconductivity at 36 K in beta-Fe1.01Se with the compression of the interlayer separation under pressure
- Density functional study of FeS, FeSe and FeTe: Electronic structure, magnetism, phonons and superconductivity
- Superconductivity at 27 K in tetragonal FeSe under high pressure
- Tellurium substitution effect on superconductivity of the alpha-phase Iron Selenide
- Nearly Isotropic superconductivity in (Ba,K)Fe2As2
- The challenge of unravelling magnetic properties in LaFeAsO
- Small anisotropy, weak thermal fluctuations, and high field superconductivity in Co-doped iron pnictide Ba(Fe1-xCox)2As2
- Structure and superconductivity of LiFeAs
- Superconductivity in S-substituted FeTe
- Critical Fields and Anisotropy of NdO0.82F0.18FeAs Single Crystals