2015
DOI: 10.1007/s12215-015-0204-z
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Polynomial decay rate estimate for bilinear parabolic systems under weak observability condition

Abstract: In this paper, we shall study the stability for distributed bilinear systems on a Hilbert state space that can be decomposed in two subspaces: unstable finite-dimensional and stable infinite-dimensional with respect to the evolution generator. Then, we shall show under a weaker observability assumption that stabilizing such a system with a feedback control of the form p r (t) = − y(t) −r y(t), By(t) for r < 2, reduces stabilizing only its projection on the finite-dimension subspace which make the whole system … Show more

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Cited by 3 publications
(2 citation statements)
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“…Furthermore, we set φfalse(x,tfalse)=normalcosfalse(tfalse),0.1emfalse(x,tfalse)false(0,1false)×false[π2,0false], which satisfies the hypothesis false(scriptHfalse).The operator A is an infinitesimal generator of a semigroup of contractions in L 2 (0,1). The spectrum of A is given by the simple eigenvalues λ j =− π 2 ( j −1) 2 , j ∈ IN * and associated to the eigenfunctions defined by ϕ 1 ( x )=1 and ϕjfalse(xfalse)=2normalcosfalse(false(j1false)πxfalse),j2, (see, e.g., [13]). Taking the compact operator of the form Bz=truej=1+1j2z,ϕjϕj. The family ( ϕ j ) j ≥ 1 is an orthonormal basis of L 2 (0,1) and the solution of the system () can be written as: zfalse(x,tfalse)=truej=1+zfalse(tfalse),ϕjL2false(0,1false)ϕjfalse(xfalse),.3emfalse(x,tfalse)false(0,1false)×false[0,+false). The operator A generates the semigroup of contractions S ( t ) defined by Sfalse(tfalse)z=truej=1+eλjtz,ϕjϕj, and we have BS(t…”
Section: Numerical Examplesmentioning
confidence: 99%
“…Furthermore, we set φfalse(x,tfalse)=normalcosfalse(tfalse),0.1emfalse(x,tfalse)false(0,1false)×false[π2,0false], which satisfies the hypothesis false(scriptHfalse).The operator A is an infinitesimal generator of a semigroup of contractions in L 2 (0,1). The spectrum of A is given by the simple eigenvalues λ j =− π 2 ( j −1) 2 , j ∈ IN * and associated to the eigenfunctions defined by ϕ 1 ( x )=1 and ϕjfalse(xfalse)=2normalcosfalse(false(j1false)πxfalse),j2, (see, e.g., [13]). Taking the compact operator of the form Bz=truej=1+1j2z,ϕjϕj. The family ( ϕ j ) j ≥ 1 is an orthonormal basis of L 2 (0,1) and the solution of the system () can be written as: zfalse(x,tfalse)=truej=1+zfalse(tfalse),ϕjL2false(0,1false)ϕjfalse(xfalse),.3emfalse(x,tfalse)false(0,1false)×false[0,+false). The operator A generates the semigroup of contractions S ( t ) defined by Sfalse(tfalse)z=truej=1+eλjtz,ϕjϕj, and we have BS(t…”
Section: Numerical Examplesmentioning
confidence: 99%
“…with 𝐵 𝑢 = 𝑃 𝑢 𝐵𝑃 𝑢 and 𝐵 𝑠 = 𝑃 𝑠 𝐵𝑃 𝑠 (see [20]). It has been shown in [6], under the spectrum growth assumption:…”
Section: Introductionmentioning
confidence: 99%