Quasinormal modes and self-adjoint extensions of the Schroedinger operator
arXiv:2010.10674 · doi:10.1103/PhysRevD.103.045001
Abstract
We revisit here the analytical continuation approach usually employed to compute quasinormal modes (QNM) and frequencies of a given potential barrier starting from the bounded states and respective eigenvalues of the Schroedinger operator associated with the potential well corresponding to the inverted potential . We consider an exactly soluble problem corresponding to a potential barrier of the Poschl-Teller type with a well defined and behaved QNM spectrum, but for which the associated Schroedinger operator obtained by analytical continuation fails to be self-adjoint. Although admits self-adjoint extensions, we show that the eigenstates corresponding to the analytically continued QNM do not belong to any self-adjoint extension domain and, consequently, they cannot be interpreted as authentic quantum mechanical bounded states. Our result challenges the practical use of the this type of method when fails to be self-adjoint since, in such cases, we would not have in advance any reasonable criterion to choose the initial eigenstates of which would correspond to the analytically continued QNM.
arXiv comment& pages, 1 Figure. Accepted for its publication in Physical Review D
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