2011
DOI: 10.1090/conm/535/10542
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Abrikosov lattice solutions of the Ginzburg-Landau equations

Abstract: Building on the earlier work of Odeh, Barany, Golubitsky, Turski and Lasher we give a proof of existence of Abrikosov vortex lattices in the Ginzburg-Landau model of superconductivity.

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Cited by 14 publications
(55 citation statements)
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“…. 3843 vq =0 0.25 1.000 26 1.002 26 1.008 01 1.003 30 1.024 28 1.073 64 1.012 19 1.072 60 1.189 62 1.026 59 1.13093 1.305 52 1.061 25 1.229 95 1.47005 1.180 34 1.424 80 1.732 61 1.000 22 1. 002 20 1.…”
Section: Problem and Resultsmentioning
confidence: 99%
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“…. 3843 vq =0 0.25 1.000 26 1.002 26 1.008 01 1.003 30 1.024 28 1.073 64 1.012 19 1.072 60 1.189 62 1.026 59 1.13093 1.305 52 1.061 25 1.229 95 1.47005 1.180 34 1.424 80 1.732 61 1.000 22 1. 002 20 1.…”
Section: Problem and Resultsmentioning
confidence: 99%
“…023 70 1.073 02 1.010 89 1.071 05 1.188 27 1. 02401 1.128 43 1.303 64 1.056 28 1.226 21 1.467 61 1.171 95 1.419 71 1.729 61 1.000 18 1.002 02 1.007 69 1.002 34 1.021 96 1.071 17 1.008 94 1.066 42 1.184 23 1.020 15 1.120 89 1.297 94 1.048 90 1.214 89 1.460 24 1.159 60 1.404 24 1.720 53 . Sample [7].…”
Section: Problem and Resultsmentioning
confidence: 99%
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“…For a lattice L ⊂ R 2 , we denote by Ω L and |Ω L | the basic lattice cell and its area, respectively. The following results were proven in [31,32]:…”
Section: Introductionmentioning
confidence: 91%
“…Assume χ ∈ H 1 loc and is L−periodic (we say, χ ∈ H 1 per ). Following [31], we differentiate the equation E λ (e isχ ψ, α + s∇χ) = E λ (ψ, α), w.r.to s at s = 0, use that curl ∇χ = 0 and integrate by parts, to obtain Re −∆ a n +α ψ + κ 2 (|ψ| 2 − 1)ψ,iχψ + J(ψ, α), ∇χ = 0. (6.10) (Due to conditions (6.3) -(6.4) and the L−periodicity of χ, there are no boundary terms.)…”
Section: Setup Of the Bifurcation Problemmentioning
confidence: 99%