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Strong solutions of the steady nonlinear Navier-Stokes system in domains with exits to infinity

K. Pileckas (1997)

Rendiconti del Seminario Matematico della Università di Padova

Strong superconvergence of finite element methods for linear parabolic problems.

Wang, Kening, Li, Shuang (2009)

International Journal of Mathematics and Mathematical Sciences

Strong unique continuation for second order elliptic differential operators

Rachid Regbaoui (1996/1997)

Séminaire Équations aux dérivées partielles

Strong unique continuation for the Lamé system with Lipschitz coefficients in three dimensions

Hang Yu (2011)

ESAIM: Control, Optimisation and Calculus of Variations

This paper studies the strong unique continuation property for the Lamé system of elasticity with variable Lamé coefficients λ, µin three dimensions, $div (μ (\nabla u + \nabla u^{t})) + \nabla (λ div u) + V u = 0$ whereλ and μ are Lipschitz continuous and V∈L∞. The method is based on the Carleman estimate with polynomial weights for the Lamé operator.

Strong unique continuation for the Lamé system with Lipschitz coefficients in three dimensions*

Hang Yu (2011)

ESAIM: Control, Optimisation and Calculus of Variations

This paper studies the strong unique continuation property for the Lamé system of elasticity with variable Lamé coefficients λ, µ in three dimensions, $div (μ (\nabla u + \nabla u^{t})) + \nabla (λ div u) + V u = 0$ where λ and μ are Lipschitz continuous and V∈L∞. The method is based on the Carleman estimate with polynomial weights for the Lamé operator.

Strong unique continuation of eigenfunctions for $p$ -Laplacian operator.

Hadi, Islam Eddine, Tsouli, N. (2001)

International Journal of Mathematics and Mathematical Sciences

Strongly elliptic linear operators without coercive quadratic forms I. Constant coefficient operators and forms

Gregory C. Verchota (2014)

Journal of the European Mathematical Society

A family of linear homogeneous 4th order elliptic differential operators $L$ with real constant coefficients, and bounded nonsmooth convex domains $Ω$ are constructed in $ℝ^{6}$ so that the $L$ have no constant coefficient coercive integro-differential quadratic forms over the Sobolev spaces $W^{2, 2} (Ω)$ .