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Titlebook: Linear and Nonlinear Aspects of Vortices; The Ginzburg-andau M Frank Pacard,Tristan Rivière Book 2000 Springer Science+Business Media New Y

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tial geometry, mathematical analysis, differential equations, mechanics, functional analysis that correspond to the temporary state of these disciplines without involving topological concepts. Therefore, it is essential to acquaint students with topo­ logical research methods already in the first un
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Qualitative Aspects of Ginzburg-Landau Equations,is diffeomorphic to the unit ball .. ⊃ ℝ., the functional has the following form:.Here the . is defined from Ω into ℂ, and A is a 1-form defined in Ω which represents the . in the material. The quantity |.|. is nothing but the density of cooper pairs of electrons that produce the superconductivity.
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,Elliptic Operators in Weighted Hölder Spaces,low up near each puncture .. at most at a certain prescribed rate. Then, we proceed to the investigation of the mapping properties of some class of elliptic operators which are defined between these spaces.
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,The Ginzburg-Landau Equation in ℂ,uation in all ℂ, and also .., the linearized Ginzburg-Landau operator about ... Next we carry out a careful study of all possible asymptotic behaviors of a solution of the homogeneous equation .. É = 0 both near the origin and near .. This yields a classification of all bounded solutions of .. É = 0
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Elliptic Operators in Weighted Sobolev Spaces,ription of the theory of elliptic operators in weighted Sobolev spaces but rather to provide simple proofs of some results that are needed in subsequent chapters. Further results can be found in the references already given in Chapter 2.
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Solving Uniqueness Questions,of the Ginzburg-Landau equation from Chapters 3 through 7 with the Pohozaev formula for the Ginzburg-Landau equation as established in Chapter 9. Indeed, using the machinery developed in Chapter 10, we are going to compare any sequence of solutions of the Ginzburg-Landau equation to the solutions co
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Qualitative Aspects of Ginzburg-Landau Equations,which represents the . in the material. The quantity |.|. is nothing but the density of cooper pairs of electrons that produce the superconductivity. Finally, .. denotes the . which is applied and then appears in the problem. The parameter . > 0 is usually called the ..
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