{"title":"Decay of the radius of spatial analyticity for the modified KdV equation and the nonlinear Schrödinger equation with third order dispersion","authors":"Renata O. Figueira, Mahendra Panthee","doi":"10.1007/s00030-024-00960-5","DOIUrl":null,"url":null,"abstract":"<p>We consider the initial value problems (IVPs) for the modified Korteweg–de Vries (mKdV) equation </p><span>$$\\begin{aligned} \\left\\{ \\begin{array}{l} \\partial _t u+ \\partial _x^3u+\\mu u^2\\partial _xu =0, \\quad x\\in \\mathbb {R},\\; t\\in \\mathbb {R}, \\\\ u(x,0) = u_0(x), \\end{array}\\right. \\end{aligned}$$</span><p>where <i>u</i> is a real valued function and <span>\\(\\mu =\\pm 1\\)</span>, and the cubic nonlinear Schrödinger equation with third order dispersion (tNLS equation in short) </p><span>$$\\begin{aligned} \\left\\{ \\begin{array}{l} \\partial _t v+i\\alpha \\partial _x^2v+\\beta \\partial _x^3v+i\\gamma |v|^2v = 0, \\quad x\\in \\mathbb {R},\\; t\\in \\mathbb {R}, \\\\ v(x,0) = v_0(x), \\end{array}\\right. \\end{aligned}$$</span><p>where <span>\\(\\alpha , \\beta \\)</span> and <span>\\(\\gamma \\)</span> are real constants and <i>v</i> is a complex valued function. In both problems, the initial data <span>\\(u_0\\)</span> and <span>\\(v_0\\)</span> are analytic on <span>\\(\\mathbb {R}\\)</span> and have uniform radius of analyticity <span>\\(\\sigma _0\\)</span> in the space variable. We prove that the both IVPs are locally well-posed for such data by establishing an analytic version of the trilinear estimates, and showed that the radius of spatial analyticity of the solution remains the same <span>\\(\\sigma _0\\)</span> till some lifespan <span>\\(0<T_0\\le 1\\)</span>. We also consider the evolution of the radius of spatial analyticity <span>\\(\\sigma (t)\\)</span> when the local solution extends globally in time and prove that for any time <span>\\(T\\ge T_0\\)</span> it is bounded from below by <span>\\(c T^{-\\frac{4}{3}}\\)</span>, for the mKdV equation in the defocusing case (<span>\\(\\mu = -1\\)</span>) and by <span>\\(c T^{-(4+\\varepsilon )}\\)</span>, <span>\\(\\varepsilon >0\\)</span>, for the tNLS equation. The result for the mKdV equation improves the one obtained in Bona et al. (Ann Inst Henri Poincaré 22:783–797, 2005) and, as far as we know, the result for the tNLS equation is the new one.</p>","PeriodicalId":501665,"journal":{"name":"Nonlinear Differential Equations and Applications (NoDEA)","volume":"14 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-05-31","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Nonlinear Differential Equations and Applications (NoDEA)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1007/s00030-024-00960-5","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
We consider the initial value problems (IVPs) for the modified Korteweg–de Vries (mKdV) equation
where u is a real valued function and \(\mu =\pm 1\), and the cubic nonlinear Schrödinger equation with third order dispersion (tNLS equation in short)
where \(\alpha , \beta \) and \(\gamma \) are real constants and v is a complex valued function. In both problems, the initial data \(u_0\) and \(v_0\) are analytic on \(\mathbb {R}\) and have uniform radius of analyticity \(\sigma _0\) in the space variable. We prove that the both IVPs are locally well-posed for such data by establishing an analytic version of the trilinear estimates, and showed that the radius of spatial analyticity of the solution remains the same \(\sigma _0\) till some lifespan \(0<T_0\le 1\). We also consider the evolution of the radius of spatial analyticity \(\sigma (t)\) when the local solution extends globally in time and prove that for any time \(T\ge T_0\) it is bounded from below by \(c T^{-\frac{4}{3}}\), for the mKdV equation in the defocusing case (\(\mu = -1\)) and by \(c T^{-(4+\varepsilon )}\), \(\varepsilon >0\), for the tNLS equation. The result for the mKdV equation improves the one obtained in Bona et al. (Ann Inst Henri Poincaré 22:783–797, 2005) and, as far as we know, the result for the tNLS equation is the new one.