Upper Critical Field of the 3 Kelvin Phase in Sr2RuO4
arXiv:cond-mat/0304510 · doi:10.1143/JPSJ.72.1623
Abstract
The inhomogeneous 3 Kelvin phase is most likely a superconducting state nucleating at the interface between micrometer-sized Ru-metal inclusions and Sr2RuO4 above the bulk onset of superconductivity. This filamentary superconducting state yields a characteristic temperature dependence of the upper critical field which is sublinear, i.e., H_{c2} (T) \propto (T^* - T)^γ with 0.5 \leq γ< 1 (T^*: nucleation temperature). The Ginzburg-Landau theory is used to analyze the behavior of the nucleated spin-triplet phase in a field and the characteristic features of H_{c2} observed in the experiment are explained based on a two-component order parameter in the presence of a filament of enhanced superconductivity with a finite width.
4 pages, 3 figures
References in corpus (6)
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- Quasiparticle States near the Surface and the Domain Wall in a p_x\pm i p_y-Wave Superconductor
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Cited by in corpus (6)
- Evaluation of Spin-Triplet Superconductivity in Sr2RuO4
- Strong Peak in of SrRuO Under Uniaxial Pressure
- Tunneling properties at the interface between superconducting Sr2RuO4 and a Ru micro-inclusion
- Phase transition in the 3 Kelvin phase in the eutectic Sr2RuO4-Ru
- Large Enhancement of 3-K Phase Superconductivity in the Sr2RuO4-Ru Eutectic System by Uniaxial Pressure
- Evolution of the filamentary 3-Kelvin phase in Pb-Ru-Sr2RuO4 Josephson junctions