BCS theory for s+g-wave superconductivity borocarbides Y(Lu)NiBC
arXiv:cond-mat/0301290 · doi:10.1103/PhysRevB.68.174501
Abstract
The s+g mixed gap function Δ_k=Δ{[(1-x)-x\sin^4θ\cos4ϕ]} (x: weight of g-wave component) has been studied within BCS theory. By suitable consideration of the pairing interaction, we have confirmed that the coexistence of s- and g-wave, as well as the state with equal s and g amplitudes (i.e., x=1/2) may be stable. This provides the semi-phenomenological theory for the s+g-wave superconductivity with point nodes which has been observed experimentally in borocarbides YNi_2B_2C and possibly in LuNi_2B_2C.
5 pages, 3 figures
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Cited by in corpus (7)
- Evidence of gap anisotropy in superconducting YNi2B2C using directional point contact spectroscopy
- Comparative analysis of specific heat of YNi2B2C using nodal and two-gap models
- Pressure dependence of the upper critical field of MgB2 and of YNi2B2C
- Magnetic field dependence of superconducting energy gaps in YNi2B2C: Evidence of multiband superconductivity
- Superconducting order parameter in nonmagnetic borocarbides RNiBC (R=Y, Lu) probed by point-contact Andreev reflection spectroscopy
- Evolution of ground state and upper critical field in R(1-x)GdxNi2B2C (R = Lu, Y): Coexistence of superconductivity and spin-glass state
- Boron isotope effect in single crystals of ErNiBC superconductor