{ "id": "1710.11399", "version": "v1", "published": "2017-10-31T10:23:06.000Z", "updated": "2017-10-31T10:23:06.000Z", "title": "Unconditional well-posedness below energy norm for the Maxwell-Klein-Gordon system", "authors": [ "Hartmut Pecher" ], "comment": "26 pages", "categories": [ "math.AP" ], "abstract": "The Maxwell-Klein-Gordon equation $ \\partial^{\\alpha} F_{\\alpha \\beta} = -Im(\\Phi \\overline{D_{\\beta} \\Phi}) $ , $ D^{\\mu}D_{\\mu} \\Phi = m^2 \\Phi $ , where $F_{\\alpha \\beta} = \\partial_{\\alpha} A_{\\beta} - \\partial_{\\beta} A_{\\alpha}$, $D_{\\mu} = \\partial_{\\mu} - iA_{\\mu} $, in the (3+1)-dimensional case is known to be unconditionally well-posed in energy space, i.e. well-posed in the natural solution space. This was proven by Klainerman-Machedon and Masmoudi-Nakanishi in Coulomb gauge and by Selberg-Tesfahun in Lorenz gauge. The main purpose of the present paper is to establish that for both gauges this also holds true for data $\\Phi(0)$ in Sobolev spaces $H^s$ with less regularity, i.e. $s < 1$, but $s$ sufficently close to $1$. This improves the (conditional) well-posedness results in both cases, i.e. uniqueness in smaller solution spaces of Bourgain-Klainerman-Machedon type, which were essentially known by Cuccagna, Selberg and the author for $s > \\frac{3}{4}$ , and which in Coulomb gauge is also contained in the present paper. In fact, the proof consists in demonstrating that any solution in the natural solution space for some $s > s_0$ belongs to a Bourgain-Klainerman-Machedon space where uniqueness is known. Here $s_0 \\approx 0.914$ in Coulomb gauge and $s_0 \\approx 0.907$ in Lorenz gauge.", "revisions": [ { "version": "v1", "updated": "2017-10-31T10:23:06.000Z" } ], "analyses": { "subjects": [ "35Q40", "35L70" ], "keywords": [ "unconditional well-posedness", "energy norm", "maxwell-klein-gordon system", "coulomb gauge", "natural solution space" ], "note": { "typesetting": "TeX", "pages": 26, "language": "en", "license": "arXiv", "status": "editable" } } }