Disorder-dependent slopes of the upper critical field in nodal and nodeless superconductors
arXiv:2306.00259 · doi:10.1103/PhysRevB.108.064502
Abstract
We study the slopes of the upper critical field at in anisotropic superconductors with transport (non-magnetic) scattering employing the Ginzburg-Landau theory, developed for this situation by S. Pokrovsky and V. Pokrovsky, Phys. Rev. B 54, 13275 (1996). We found unexpected behavior of the slopes for a wave superconductor and in a more general case of materials with line nodes in the order parameter. Specifically, the presence of line nodes causes to decrease with increasing non-magnetic scattering parameter , unlike the nodeless case where the slope increases. In a pure wave case, the slope changes from decreasing to increasing when scattering parameter approaches , where at which that implies the the existence of a gapless state in wave superconductors with transport scattering in the interval, . Furthermore, we have considered the mixed order parameter that has 4 nodes on a cylindrical Fermi surface when a part is dominant, or no nodes at all when an phase is the major one. We find that presence of nodes causes the slope to decrease initially with increasing , whereas in the nodeless state, monotonically increases. Therefore, fairly straightforward experiments make it possible to decide whether or not the order parameter of a superconductor has nodes by measuring the disorder-dependence of the slope of at .
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