Index des auteurs, volumes 25-50. Author index, volumes 25-50
(1989)
Annales de l'I.H.P. Physique théorique
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(1989)
Annales de l'I.H.P. Physique théorique
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Amar Heminna (2010)
ESAIM: Control, Optimisation and Calculus of Variations
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The problem of boundary stabilization for the isotropic linear elastodynamic system and the wave equation with Ventcel's conditions are considered (see [12]). The boundary observability and the exact controllability were etablished in [11]. We prove here the enegy decay to zero for the elastodynamic system with stationary Ventcel's conditions by introducing a nonlinear boundary feedback. We also give a boundary feedback leading to arbitrarily large energy decay rates for the elastodynamic...
Masao Nagasawa (1993)
Séminaire de probabilités de Strasbourg
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David P. Levadoux, Bastiaan L. Michielsen (2010)
ESAIM: Mathematical Modelling and Numerical Analysis
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We present an integral equation method for solving boundary value problems of the Helmholtz equation in unbounded domains. The method relies on the factorisation of one of the Calderón projectors by an operator approximating the exterior admittance (Dirichlet to Neumann) operator of the scattering obstacle. We show how the pseudo-differential calculus allows us to construct such approximations and that this yields integral equations without internal resonances and being well-conditioned at...
Kim-Dang Phung (2010)
ESAIM: Control, Optimisation and Calculus of Variations
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We consider the Laplace equation in a smooth bounded domain. We prove logarithmic estimates, in the sense of John [5] of solutions on a part of the boundary or of the domain without known boundary conditions. These results are established by employing Carleman estimates and techniques that we borrow from the works of Robbiano [8,11]. Also, we establish an estimate on the cost of an approximate control for an elliptic model equation.
F. Bethuel, G. Orlandi, D. Smets (2004)
Journées Équations aux dérivées partielles
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We discuss the asymptotics of the parabolic Ginzburg-Landau equation in dimension Our only asumption on the initial datum is a natural energy bound. Compared to the case of “well-prepared” initial datum, this induces possible new energy modes which we analyze, and in particular their mutual interaction. The two dimensional case is qualitatively different and requires a separate treatment.
(1998)
Annales Polonici Mathematici
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