2005
DOI: 10.1016/j.sysconle.2004.07.005
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On the realization of periodic functions

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Cited by 7 publications
(14 citation statements)
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“…A computer simulation would essentially reduce the problem to a finite-dimensional approximation, and thus the simulation would (at best) represent a solution of a finitedimensional output regulation problem. From the practical point of view this problem is compounded by the fact that little research on approximation of infinite-dimensional output regulation problems for infinite-dimensional exosystems has been reported [24,25].…”
Section: The Exogenous Systemmentioning
confidence: 99%
“…A computer simulation would essentially reduce the problem to a finite-dimensional approximation, and thus the simulation would (at best) represent a solution of a finitedimensional output regulation problem. From the practical point of view this problem is compounded by the fact that little research on approximation of infinite-dimensional output regulation problems for infinite-dimensional exosystems has been reported [24,25].…”
Section: The Exogenous Systemmentioning
confidence: 99%
“…the search for a space W, operators S and Q, and a suitable initial state w 0 -for a specific function u(t) is called realization. This procedure is discussed in the articles [5,6,13,16,18]. The following example shows that the function generator approach includes inputs in various subspaces of BUC(R + , U) [2,7,23].…”
Section: Function Generators In Banach Spacesmentioning
confidence: 99%
“…Such realizations play a central role in some regulator problems of modern control theory [8]. The realizationsoccasionally also called state space realizations-that we consider are of the forṁ Here x(t) is the state of the system (which lies in some Hilbert space H ) while y(t) is the output of the system.…”
Section: Introduction and Some Definitionsmentioning
confidence: 99%
“…System (1.1) is denoted Σ(A, −, C, −) [3]. One possible approach to constructing an infinite-dimensional realization for a given 2π -periodic function y ∈ C 1 [0, 2π] is as follows [8]. Choose the state space H to be L 2 [0, 2π], select the C 0 -semigroup T (·) to be the 2π -periodic left shift on H (such that T (τ )f = f (· + τ − 2π ·+τ 2π ) for each f ∈ H ), select x 0 = y and finally set the observation operator C to be the (ordinary) point evaluation operator at the origin.…”
Section: Introduction and Some Definitionsmentioning
confidence: 99%
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