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Zapiski Nauchnykh Seminarov POMI, 2025, Volume 541, Pages 16–29
(Mi znsl7559)
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Abstract dynamical system with boundary control. IV
M. I. Belisheva, S. A. Simonovabc a St. Petersburg Department of Steklov Mathematical Institute of Russian Academy of Sciences
b Alferov Federal State Budgetary Institution of Higher Education and Science Saint Petersburg National Research Academic University of the Russian Academy of Sciences, St. Petersburg
c ITMO University
Abstract:
The paper continues the study of the general properties of evolutionary dynamical systems of the type \begin{align*} & u''(t)+L_0^*u(t) = 0 && \text{ in } {{\mathscr H}}, t\in(0,T), & u(0)=u'(0)=0 && \text{ in } {{\mathscr H}}, &\Gamma_1 u(t) = f(t) && \text{ in } {{\mathscr K}}, t\in[0,T], \end{align*} where $\mathscr H$ is a Hilbert space, $L_0$ is a positive-definite symmetric operator in $\mathscr H$, $\Gamma_1:{\mathrm {Dom}}\,L_0^*\to \mathscr K:={\mathrm {Ker}}\,L_0^*$ is one of the boundary operators from the Green formula $({L_0^*} u,v)-(u,{L_0^*}v)=(\Gamma_1u,\Gamma_2v)-(\Gamma_2u,\Gamma_1v)$, $f=f(t)$ is a $\mathscr K$-valued function of time (boundary control), $u=u^f(t)$ is the solution (trajectory), which is an $\mathscr H$-valued function of time. Compared to previous works on this topic, the novelty lies in the properties of the response operator $R^T: f\mapsto \Gamma_2 u^f(\cdot)$, which acts in $\mathscr F^T:=L_2([0,T];\mathscr K)$ on a relevant ${\mathrm{Dom}}\,R^T$.
Key words and phrases:
triangular factorization of operators, nest theory, functional models.
Received: 05.10.2025
Citation:
M. I. Belishev, S. A. Simonov, “Abstract dynamical system with boundary control. IV”, Mathematical problems in the theory of wave propagation. Part 54, Zap. Nauchn. Sem. POMI, 541, POMI, St. Petersburg, 2025, 16–29
Linking options:
https://www.mathnet.ru/eng/znsl7559 https://www.mathnet.ru/eng/znsl/v541/p16
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