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Abstract

Notation. We continue to use the notation listed at the beginning of Chapter 2. As in earlier chapters, if \( \mathbb{T} \) is a strongly continuous semigroup on the Hilbert space X, with generator A, then the spaces X1 and X−1 are as in Section 2.10 and the extension of A to X is still denoted by A.

Keywords

Weak Solution Control Operator Inverse Semigroup Boundary Control Bernoulli Beam 
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Copyright information

© Birkhäuser Verlag AG 2009

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