Titlebook: Sobolev Spaces in Mathematics III; Applications in Math Victor Isakov Book 2009 Springer-Verlag New York 2009 Ginzburg-Landau model.Sobolev

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narcotic

密切关系

Finsler Structures and Wave Propagation,ing in such study can enhance one‘s understanding of Finsler geometry. We also discuss a problem in harmonic analysis motivated by a construction of Katok in Finsler geometry, which gives rise to an interesting variant of the Pinsky phenomenon, for pointwise Fourier inversion.

佛刊

Geometrization of Rings as a Method for Solving Inverse Problems, hyperbolic Dirichlet-to-Neumann map, spectral data, etc). We show that for a class of elliptic and hyperbolic problems the required manifold is identical with the spectrum of a certain algebra determined by the inverse data and, consequently, to recover the manifold it suffices to represent the cor

Middle-Ear

MOAT

Carleman Estimates with Second Large Parameter for Second Order Operators,arameter, from results for scalar equations we derive Carleman estimates for dynamical Lamé system with residual stress. These estimates are used to prove the Hölder and Lipschitz stability for the continuation of solutions under pseudoconvexity assumptions. So, the first uniqueness and stability of

DEVIL

,Linear Hyperbolic and Petrowski Type PDEs with Continuous Boundary Control → Boundary Observation Oerential equations with variable coefficients (in space), as a consequence of the continuity (boundedness) of the corresponding purely Boundary Control → Boundary observation open-loop map of dissipative character, of interest in its own right. The interior is assumed inaccessible. There are explici

权宜之计

Finsler Structures and Wave Propagation,of Finsler geometry. In particular, we investigate how understanding of the behavior of differential operators (and pseudodifferential operators) arising in such study can enhance one‘s understanding of Finsler geometry. We also discuss a problem in harmonic analysis motivated by a construction of K

CANE

Motilin

,Linear Hyperbolic and Petrowski Type PDEs with Continuous Boundary Control → Boundary Observation Ove and unexpected consequences. In particular, when accompanied by exact controllability of the corresponding open-loop linear model, it implies uniform stabilization with optimal decay rates—when a nonlinear function of the boundary observation closes up the loop, to generate the corresponding boundary feedback dissipative problem.