1963
DOI: 10.1063/1.3050816
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The Calculus of Variations

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Cited by 41 publications
(44 citation statements)
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“…Taking into account that only stable phase configurations, corresponding to minima of (3), are physically observable, the problem one has to solve can be formulated as follows: Find all solutions to (7), (8) that minimize (at least locally) (3) at given H ≥ 0. To resolve this problem, we have to turn to sufficient conditions of the minimum, 18 which requires an analysis of the second variation of (3).…”
Section: Introductionmentioning
confidence: 99%
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“…Taking into account that only stable phase configurations, corresponding to minima of (3), are physically observable, the problem one has to solve can be formulated as follows: Find all solutions to (7), (8) that minimize (at least locally) (3) at given H ≥ 0. To resolve this problem, we have to turn to sufficient conditions of the minimum, 18 which requires an analysis of the second variation of (3).…”
Section: Introductionmentioning
confidence: 99%
“…The main property of the functional (3) follows from the fact that it belongs to the class of regular functionals, i.e., satisfies a necessary condition of the minimum; 18 hence, all stationary points of (3) are either minima of saddle points. [Unfortunately, the statement of Ref.…”
Section: Introductionmentioning
confidence: 99%
“…However, contrary to popular belief, many other physical laws do not have a mechanistic 500 SASCHA E. ENGELBRECHT 2 An introduction to the calculus of variations can be found in Dreyfus (1965), and in-dept treatments are provided by Akhiezer (1962) and Bliss (1946). For a history of the calculus of variations, see Goldstine (1980).…”
mentioning
confidence: 99%
“…To eliminate any questions about the actual equilibrium field configurations in layered superconductors at H > 0, we present an explicit mathematical proof that the Meissner (0-soliton) and vortex-plane (soliton) configurations are unique solutions that satisfy the conditions of the minimum (1), (2). Moreover, we show that all the minima are strict and strong [19]. For the sake of diversification, we employ a new method of exact minimization of the Gibbs free-energy functional that, in contrast to Refs.…”
Section: Introductionmentioning
confidence: 99%
“…Mathematically, a classification of stable solutions amounts to the determination of all points of local minima of the energy functionals. A local minimum of the Gibbs free-energy functional of layered superconductors is determined by the relations [18,19] …”
Section: Introductionmentioning
confidence: 99%