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Article type: Research Article
Authors: Kachmar, Aymana | Nasrallah, Marwab; c; *
Affiliations: [a] Department of Mathematics, Lebanese University, Nabatieh, Lebanon. E-mail: [email protected] | [b] Lebanese International University, Beirut, Lebanon. E-mail: [email protected] | [c] Faculty of Sciences, Section IV, Lebanese University, Bekaa, Lebanon
Correspondence: [*] Corresponding author. E-mail: [email protected].
Abstract: The energy of a type II superconductor placed in a strong non-uniform, smooth and signed magnetic field is displayed via a universal reference function defined by means of a simplified two dimensional Ginzburg–Landau functional. We study the asymptotic behavior of this functional in a specific asymptotic regime, thereby linking it to a one dimensional functional, using methods developed by Almog–Helffer and Fournais–Helffer devoted to the analysis of surface superconductivity in the presence of a uniform magnetic field. As a result, we obtain an asymptotic formula reminiscent of the one for the surface superconductivity regime, where the zero set of the magnetic field plays the role of the superconductor’s surface.
Keywords: Superconductivity, Ginzburg–Landau functional, ground state energy, vanishing magnetic field, Montgomery operator
DOI: 10.3233/ASY-171424
Journal: Asymptotic Analysis, vol. 103, no. 3, pp. 135-163, 2017
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