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Séminaire d'Analyse

The Dirichlet problem without the maximum principle

Tom ter Elst (Oakland)

Salle de Conférences

16 mars 2023 à 14:00

"The maximum principle plays an important role for the solution of the Dirichlet problem. Now consider the Dirichlet problem with respect to an elliptic operator A=−∑k,l=1d∂k akl ∂l−∑k=1d∂k bk+∑k=1dck ∂k+c0 A = - \sum_{k,l=1}^d \partial_k \, a_{kl} \, \partial_l - \sum_{k=1}^d \partial_k \, b_k + \sum_{k=1}^d c_k \, \partial_k + c_0 on a sufficiently regular open set Ω⊂Rd\Omega \subset \mathbb{R}^d, where akl,ck∈L∞(Ω,R)a_{kl}, c_k \in L_\infty(\Omega,\mathbb{R}) and bk,c0∈L∞(Ω,C)b_k,c_0 \in L_\infty(\Omega,\mathbb{C}). Suppose that the associated operator on L2(Ω)L_2(\Omega) with Dirichlet boundary conditions is invertible. Note that in general this operator does not satisfy the maximum principle. Nevertheless, we show that for all φ∈C(∂Ω)\varphi \in C(\partial \Omega) there exists a unique u∈C(Ω‾)∩Hloc1(Ω)u \in C(\overline \Omega) \cap H^1_{\rm loc}(\Omega) such that u∣∂Ω=φu|_{\partial \Omega} = \varphi and Au=0A u = 0. In the case when Ω\Omega has a Lipschitz boundary and φ∈C(Ω‾)∩H1/2(Ω‾)\varphi \in C(\overline \Omega) \cap H^{1/2}(\overline \Omega), then we show that uu coincides with the variational solution in H1(Ω)H^1(\Omega). This is joint work with Wolfgang Arendt."