
When dealing with Schrödinger operators with non-locally-integrable potentials or with Schrö\-din\-ger operators on graphs, it is convenient to split the domain into intervals \(I_i\) \((i\in \Omega)\) on which the potential is locally integrable. Then consider the differential operator \(T\) on the direct sum Hilbert space \(\bigoplus_{i\in\Omega }L^2(I_i,\omega _i)\) of weighted Lebesgue spaces with weight \(\omega _i\). The operator \(T=\bigoplus_{i\in \Omega}T_i\) is the direct sum of self-adjoint realizations of quasi-differential operators given by Shin-Zettl matrices. Some results on spectral representations, cyclic vectors, and spectral multiplicities are presented and are illustrated by examples.
Schrödinger operator, Vector-operators ($v$-operators), quasi-differential operator, General theory of ordinary differential operators, Cyclic vectors, hypercyclic and chaotic operators, ordered representation, vector operator, General spectral theory of ordinary differential operators, Linear symmetric and selfadjoint operators (unbounded), 34L05, cyclic vector, multiplicity, spectral representation, unitary transformation, 47B25, 47B37, 47A16
Schrödinger operator, Vector-operators ($v$-operators), quasi-differential operator, General theory of ordinary differential operators, Cyclic vectors, hypercyclic and chaotic operators, ordered representation, vector operator, General spectral theory of ordinary differential operators, Linear symmetric and selfadjoint operators (unbounded), 34L05, cyclic vector, multiplicity, spectral representation, unitary transformation, 47B25, 47B37, 47A16
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