Decoupling of deficiency indices and applications to Schrödinger-type operators with possibly strongly singular potentials (Q305753)

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scientific article; zbMATH DE number 6620640
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Decoupling of deficiency indices and applications to Schrödinger-type operators with possibly strongly singular potentials
scientific article; zbMATH DE number 6620640

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    Decoupling of deficiency indices and applications to Schrödinger-type operators with possibly strongly singular potentials (English)
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    30 August 2016
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    Schrödinger operator
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    strongly singular potentials
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    deficiency indices
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    essential self-adjointness
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    The study of deficiency indices of symmetric operators in Hilbert spaces is one of the central problems in spectral theory of unbounded linear operators. One of the main objects in the paper under review are closed symmetric realizations \(H\) in \(L^2(\mathbb{R}^n)\) of Schrödinger-type operators NEWLINE\[NEWLINE (-\Delta + V)\upharpoonright_{C_0^\infty(\mathbb{R}^n\setminus\Sigma)} NEWLINE\]NEWLINE whose potential \(V\) has a countable number of well-separated singularities on compact sets \(\Sigma_j\), \(j\in J\), of \(n\)-dimensional Lebesgue measure zero, with \(J\subseteq \mathbb{N}\) an index set and \(\Sigma=\bigcup_{j\in J}\Sigma_j\).NEWLINENEWLINEThe central result in the paper under review is an abstract approach to the question of decoupling of deficiency indices. Then the authors apply it to the concrete case of Schrödinger type operators in \(L^2(\mathbb{R}^n)\) and to second-order elliptic differential operators on \(\mathbb{R}^n\). For example, it is proved that under certain assumptions on \(V\) and \(\Sigma\) the defect \(\text{Def}(H)\) of \(H\) can be computed in terms of the individual defects \(\text{Def}(H_j)\) of \(H_j\), where \(H_j\) is a closed symmetric realization of \((-\Delta + V)\upharpoonright_{C_0^\infty(\mathbb{R}^n\setminus\Sigma_j)}\). More specifically, the authors derive the results that the defect of \(H\) can be computed as the sum of over the individual defects of \(H_j\), NEWLINE\[NEWLINE \text{Def}(H) = \sum_{j\in J} \text{Def}(H_j). NEWLINE\]NEWLINE The possibility that one and hence both sides equal \(\infty\) is included. Here NEWLINE\[NEWLINE \text{Def}(A):= \frac{n_+(A) + n_-(A)}{2}, NEWLINE\]NEWLINE and \(n_\pm(A)\) are the standard deficiency indices of \(A\). Notice that \(\text{Def}(A) = n_\pm(A)\) if \(n_+(A)=n_-(A)\) (the latter holds, in particular, when \(A\) is lower semibounded or commutes with a conjugation).NEWLINENEWLINEFinally, let us mention that applications to Schrödinger operators with multipolar inverse-square potentials allow to considerably improve the results obtained in [\textit{V. Felli} et al., J. Funct. Anal. 250, No. 2, 265--316 (2007; Zbl 1222.35074)].
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