%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \documentclass[a4paper,11pt]{article} \def\ms{\textsc{2010 Mathematics Subject Classifications} : } \providecommand\key[1]{\par \textsc{Keywords :}#1 \vspace{0,5cm}} \providecommand\add[2]{\textsc{{#1}} {\newline \textbf{ E-mail : }#2}} \date{} \begin{document} \begin{center} \LARGE On the Spectral Theory of Multidimensional Schr\"{o}dinger Operator \end{center} \vspace{1cm} \normalsize \centerline{Setenay AKDUMAN} \vspace{.5cm} \centerline{Department of Mathematics, Faculty of Science, Dokuz Eyl\"{u}l University,} \centerline{T{\i}naztepe Camp., Buca, 35160, Izmir, Turkey} \centerline{setenayakduman@gmail.com} \vspace{.5cm} \begin{abstract} The main object of my talk is the Schr\"{o}dinger operator $L(V)$ with a matrix potential on a $d-$ dimensional rectangle with Neumann boundary conditions. The operator $L(V)$ is considered as a perturbation of the free Hamiltonian $L(0)$, when $V=0$. Perturbative analysis of eigenvalues and eigenfunctions of $L(V)$ meets a serious difficulty due to presence of the very close eigenvalues of unperturbed operator. In general, this leads to the so-called `small denominators' problem. However, the set of unperturbed eigenvalues can be splitted into two parts called resonance and non-resonance domains, respectively. This opens a door to study the perturbations of each group for obtaining various asymptotic formulas for the eigenvalues and eigenfunctions of $L(V)$. I will talk about this problem which is a part of my PhD dissertation. \end{abstract} \vspace{.5cm} \ms {47F05, 35P15} \key {Schr\"{o}dinger operator, Neumann condition, Perturbation theory.} \begin{thebibliography}{9} \bibitem{veliev}Veliev, O. (2015). Multidimensional Periodic Schrödinger Operator. Springer. \bibitem{Kato} Kato, T. \textit{Perturbation Theory for Linear Operators}, Springer, Berlin (1980) \bibitem{Karakilicsetenay} Karak{\i}l{\i}\c{c}, S. \& Akduman S. (2015). Eigenvalue Asymptotics for the Schr\"odinger Operator with a Matrix Potential in a Single Resonance Domain. \textit{Filomat, 29:1, 21-38}. \end{thebibliography} \end{document} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%