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<mrnumber>MR2918149</mrnumber>
<author>Kentarou YOSHII</author>
<author_utf8>Kentarou YOSHII</author_utf8>
<title>Classical Solutions to a Linear Schr&#246;dinger Evolution Equation Involving a Coulomb Potential with a Moving Center of Mass</title>
<journal>Funkcialaj Ekvacioj. Serio Internacia</journal>
<volume>54</volume>
<year>2011</year>
<page>485--493</page>
<url_pdf>http://fe.math.kobe-u.ac.jp/FE/FullPapers/54-3/54_485.pdf</url_pdf>
<mathsci_link>http://www.ams.org/mathscinet-getitem?mr=MR2918149</mathsci_link>
<abstract>This paper is concerned with Cauchy problems for the linear Schr&#246;dinger evolution equation $(i(\partial/\partial t)+\Delta+|x-a(t)|^{-1}+V_1(x,t))u(x,t)=f(x,t)$ in $\mathbb{R}^N \times[0,T]$, subject to initial condition: $u(\cdot,0)\in H^2(\mathbb{R}^N)\cap H_2(\mathbb{R}^N)$, where $i :=\sqrt{-1}$, $N\ge 3$, $T>0$ and $a: [0,T]\to\mathbb{R}^N$ expresses the center of the Coulomb potential, $V_1$ and $f$ are another real-valued potential and an inhomogeneous term, respectively, while $H_2(\mathbb{R}^N) :=\{v\in L^2(\mathbb{R}^N); |x|^2 v\in L^2(\mathbb{R}^N)\}$. We show that under some conditions on $V_1$ and $f$ the equation has a classical solution $u(\cdot)\in C^1([0,T];L^2(\mathbb{R}^N))\cap C([0,T];H^2(\mathbb{R}^N)\cap H_2(\mathbb{R}^N))$.</abstract>
<keywords>Schr&#246;dinger equation, Coulomb potential with a moving center of mass, Potentials singular at infinity, Existence and uniqueness of classical solutions, Energy estimates.</keywords>
<subject>35Q41, 35A09.</subject>
<fesi_info>
  <FILE>54-485</FILE>
  <YEAR>2011</YEAR>
  <TITLE>Classical Solutions to a Linear Schr&#246;dinger Evolution Equation Involving a Coulomb Potential with a Moving Center of Mass</TITLE>
  <AUTHOR>Kentarou YOSHII</AUTHOR>
  <AUTHOR_utf8>Kentarou YOSHII</AUTHOR_utf8>
</fesi_info>

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