Lack of diamagnetism and the Little-Parks effect

Abstract

When a superconducting sample is submitted to a sufficiently strong external magnetic field, the superconductivity of the material is lost. In this paper we prove that this effect does not, in general, take place at a unique value of the external magnetic field strength. Indeed, for a sample in the shape of a narrow annulus the set of magnetic field strengths for which the sample is superconducting is not an interval. This is a rigorous justification of the Little-Parks effect. We also show that the same oscillation effect can happen for disc-shaped samples if the external magnetic field is non-uniform. In this case the oscillations can even occur repeatedly along arbitrarily large values of the Ginzburg--Landau parameter $\kappa$. The analysis is based on an understanding of the underlying spectral theory for a magnetic Schrödinger operator. It is shown that the ground state energy of such an operator is not in general a monotone function of the intensity of the field, even in the limit of strong fields.

References in corpus (2)

• On the third critical field in Ginzburg-Landau theory
• Sharp asymptotics for the Neumann Laplacian with variable magnetic field : case of dimension 2

Cited by in corpus (6)

• The breakdown of superconductivity in the presence of magnetic steps
• Counterexample to strong diamagnetism for the magnetic Robin Laplacian
• On the isoperimetric inequality for the magnetic Robin Laplacian with negative boundary parameter
• Semi-classical eigenvalue estimates under magnetic steps (Former title: Hearing the shape of a magnetic edge in the semiclassical limit)
• Magnetic steps on the threshold of the normal state
• Eigenvalues of the Neumann magnetic Laplacian in the unit disk