Point Contact Spectroscopy of Superconducting Gap Anisotropy in Nickel Borocarbide Compound LuNi2B2C

TL;DR

This study investigates the anisotropic superconducting gap in LuNi2B2C using point contact spectroscopy, revealing non-uniform gap distribution and the inadequacy of simple models, suggesting a continuous gap distribution over the Fermi surface.

Contribution

It introduces a continuous, dual-maxima model to better describe the superconducting gap anisotropy in LuNi2B2C, surpassing traditional one- and two-gap models.

Findings

Superconducting gap is non-uniformly distributed over the Fermi surface.

Largest contribution to conductivity varies with direction, with different gap sizes.

Deviation from BCS model is more pronounced in the c direction.

Abstract

Point contacts are used to investigate the anisotropy of the superconducting energy gap in LuNi2B2C in the ab plane and along the c axis. It is shown that the experimental curves should be described assuming that the superconducting gap is non-uniformly distributed over the Fermi surface. The largest and the smallest gaps have been estimated by two-gap fitting models. It is found that the largest contribution to the point-contact conductivity in the c direction is made by a smaller gap and, in the ab plane by a larger gap. The deviation from the one-gap BCS model is pronounced in the temperature dependence of the gap in both directions. The temperature range, where the deviation occurs, is for the c direction approximately 1.5 times more than in the ab plane. The \Gamma parameter, allowing quantitatively estimate the gap anisotropy by one-gap fitting, in c direction is also about 1.5 times greater than in the ab plane. Since it is impossible to describe satisfactorily such gap distribution either by the one- or two-gap models, a continuous, dual-maxima model of gap distribution over the Fermi surface should be used to describe superconductivity in this material.