Dynamical System with Boundary Control Associated with Symmetric Semi-Bounded Operator

preprint2012arXivOpen access

Abstract

Let L0L_0 be a closed densely defined symmetric semi-bounded operator with nonzero defect indexes in a separable Hilbert space H\cal H. It determines a {\it Green system} {H,B;L0,Γ1,Γ2}\{{\cal H}, {\cal B}; L_0, Γ_1, Γ_2\}, where B{\cal B} is a Hilbert space, and Γi:H→BΓ_i: {\cal H} \to \cal B are the operators related through the Green formula (L0∗u,v)H−(u,L0∗v)H=(Γ1u,Γ2v)B−(Γ2u,Γ1v)B.(L_0^*u, v)_{\cal H}-(u,L_0^*v)_{\cal H}=(Γ_1 u, Γ_2 v)_{\cal B} - (Γ_2 u, Γ_1 v)_{\cal B}. The {\it boundary operators} ΓiΓ_i are chosen canonically in the framework of the Vishik theory. With the Green system one associates a {\it dynamical system with boundary control} (DSBC) {align*} & u_{tt}+L_0^*u = 0 && {\rm in}\,\,\,{\cal H}, \,\,\,t>0 & u|_{t=0}=u_t|_{t=0}=0 && {\rm in}\,\,\,{\cal H} & Γ_1 u = f && {\rm in}\,\,\,{\cal B},\,\,\,t \geqslant 0. {align*} We show that this system is {\it controllable} if and only if the operator L0L_0 is completely non-self-adjoint. A version of the notion of a {\it wave spectrum} of L0L_0 is introduced. It is a topological space determined by L0L_0 and constructed from reachable sets of the DSBC.

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