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Orbital stability : ウィキペディア英語版 | Orbital stability In mathematical physics or theory of partial differential equations, the solitary wave solution of the form is said to be orbitally stable if any solution with the initial data sufficiently close to forever remains in a given small neighborhood of the trajectory of . ==Formal definition== Formal definition is as follows. Let us consider the dynamical system : with a Banach space over , and . We assume that the system is -invariant, so that for any and any . Assume that , so that is a solution to the dynamical system. We call such solution a solitary wave. We say that the solitary wave is orbitally stable if for any there is such that for any with there is a solution defined for all such that , and such that this solution satisfies :
抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)』 ■ウィキペディアで「Orbital stability」の詳細全文を読む
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