The Ginzburg–Landau equations in a semi-infinite superconducting film in the large κ limit

1997 ◽  
Vol 8 (4) ◽  
pp. 347-367 ◽  
Author(s):  
CATHERINE BOLLEY ◽  
BERNARD HELFFER

Following our preceding papers [1, 2] concerning semi-infinite superconducting films, we consider new a priori estimates on the exterior magnetic field h=A′(0), when (f, A) is a solution of the corresponding Ginzburg–Landau system. The main new results concern the limit as κ→∞, but we prove also the existence of a finite superheating field. We also discuss recent results [3] concerning the superheating field in the large κ limit, and show how to relate these formal solutions to suitable subsolutions and supersolutions giving the existence of a solution for h<1/√2 and κ large enough. We also analyse the same problem by variational techniques and get the existence of a locally stable solution for h<1/√2 and any κ>0.

1966 ◽  
Vol 145 (1) ◽  
pp. 231-236 ◽  
Author(s):  
V. D. Arp ◽  
R. S. Collier ◽  
R. A. Kamper ◽  
H. Meissner

2001 ◽  
Vol 03 (01) ◽  
pp. 1-14 ◽  
Author(s):  
A. AFTALION ◽  
E. N. DANCER

In this paper, we study the Ginzburg–Landau equations for a two dimensional domain which has small size. We prove that if the domain is small, then the solution has no zero, that is no vortex. More precisely, we show that the order parameter Ψ is almost constant. Additionnally, we obtain that if the domain is a disc of small radius, then any non normal solution is symmetric and unique. Then, in the case of a slab, that is a one dimensional domain, we use the same method to derive that solutions are symmetric. The proofs use a priori estimates and the Poincaré inequality.


1996 ◽  
Vol 08 (01) ◽  
pp. 43-83 ◽  
Author(s):  
CATHERINE BOLLEY ◽  
BERNARD HELFFER

In continuation with our preceding paper [10] concerning the superconducting film, we present in this article rigorous results concerning the superheating in the weak κ limit. The principal result is an important step toward the rigorous proof of a formula due to P. De Gennes [26] . This paper is complementary to our paper [11] where numerical results are presented and approximate models are discussed. Most of the results have been announced in [12] and [13].


1996 ◽  
Vol 06 (09) ◽  
pp. 1665-1671 ◽  
Author(s):  
J. BRAGARD ◽  
J. PONTES ◽  
M.G. VELARDE

We consider a thin fluid layer of infinite horizontal extent, confined below by a rigid plane and open above to the ambient air, with surface tension linearly depending on the temperature. The fluid is heated from below. First we obtain the weakly nonlinear amplitude equations in specific spatial directions. The procedure yields a set of generalized Ginzburg–Landau equations. Then we proceed to the numerical exploration of the solutions of these equations in finite geometry, hence to the selection of cells as a result of competition between the possible different modes of convection.


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