Sharp L^2 bounds for oscillatory integral operators with C^\infty phases

dc.creatorRychkov, Vyacheslav
dc.date1999-11-19
dc.date.accessioned2026-07-07T05:31:42Z
dc.date.available2026-07-07T05:31:42Z
dc.descriptionLet T be an oscillatory integral operator on L^2(R) with a smooth real phase function S(x,y). We prove that, in all cases but the one described below, after localization to a small neighborhood of the origin the norm of T decays like N^{-d/2} as the frequency N->infty, where d is the Newton decay rate introduced by Phong and Stein, which is determined by the Newton diagram of S(x,y). For real analytic phase functions this result was proved by Phong and Stein. For smooth phase functions the best known results so far contained a loss of epsilon in the exponent (implicit in the work of Seeger). The exceptional case mentioned above happens when the Taylor series of the mixed partial derivative S''(x,y) factorizes in R[[x,y]] as U(x,y)(y-f(x))^k, where U(x,y) is a unit, k\ge 2, and f(x) is a series in R[[x]] of the form Cx+(higher order), C\ne 0. In this case we prove an estimate with a loss of of a power of log N.
dc.description23 pages, 5 figures
dc.identifierhttps://arxiv.org/abs/math/9911153
dc.identifierhttp://arxiv.org/abs/math/9911153
dc.identifierMath. Z. 236 (2001), no. 3, 461-489
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/79445
dc.subjectClassical Analysis and ODEs
dc.subjectPrimary 35S30; Secondary 42B10, 47G10
dc.titleSharp L^2 bounds for oscillatory integral operators with C^\infty phases
dc.typetext

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