2005
DOI: 10.1016/j.jfa.2005.05.013
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On the wave equation with a large rough potential

Abstract: International audienc

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Cited by 84 publications
(68 citation statements)
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“…Several results are available for the equations i∂ t u − ∆u + V (x)u = 0, u + V (x)u = 0. We cite among the others [8], [15], [16], [19], [32] and the recent survey [33] for Schrö-dinger; and [5], [6], [10], [12], [13] for the wave equation. We must also mention the wave operator approach of Yajima (see [2], [39], [40], [41]) which permits to deal with the above equations in a unified way, although under nonoptimal assumptions on the potential in dimensions 1 and 3.…”
Section: Introductionmentioning
confidence: 99%
“…Several results are available for the equations i∂ t u − ∆u + V (x)u = 0, u + V (x)u = 0. We cite among the others [8], [15], [16], [19], [32] and the recent survey [33] for Schrö-dinger; and [5], [6], [10], [12], [13] for the wave equation. We must also mention the wave operator approach of Yajima (see [2], [39], [40], [41]) which permits to deal with the above equations in a unified way, although under nonoptimal assumptions on the potential in dimensions 1 and 3.…”
Section: Introductionmentioning
confidence: 99%
“…This is all technically justified by a work of Jensen and Nakamura, [8], (see also a more recent result Theorem 5.2, [1])…”
Section: Wave Equations With Time Dependent Potentialsmentioning
confidence: 73%
“…This is usually restricted to either time independent or very small time dependent potentials and in some cases are dimensionally restrictive. This was done (mostly in the physically important 3 D case) in the context of the Schrödinger equation in a series of papers by Rodnianski-Schlag [13], Goldberg-Schlag [6], and in the wave equation context by Georgiev-Visciglia [4], D'Ancona -Pierfelice [1], and others.…”
Section: ∂ Tt U(x T) − U + V (X T)u = F (X T) (X T) ∈ R N × Rmentioning
confidence: 99%
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