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Stefan Kunkel

Publications and source records attributed to Stefan Kunkel.

2 recordsLinked to original sources

Diffusion with nonlocal Robin boundary conditions

We investigate a second order elliptic differential operator $A_{β, μ}$ on a bounded, open set $Ω\subset\mathbb{R}^{d}$ with Lipschitz boundary subject to a nonlocal boundary condition of Robin type. More precisely we have $0\leq β\in L^{\infty}(\partialΩ)$ and $μ\colon \partial Ω\to \mathscr{M}(\overlineΩ)$, and boundary conditions of the form \[ \partial_ν^{\mathscr{A}}u(z)+β(z)u(z)=\int_{\overlineΩ}u(x)μ(z)(dx),\ z\in\partialΩ, \] where $\partial_ν^{\mathscr{A}}$ denotes the weak conormal derivative with respect to our differential operator. Under suitable conditions on the coefficients of the differential operator and the function $μ$ we show that $A_{β, μ}$ generates a holomorphic semigroup $T_{β,μ}$ on $L^{\infty}(Ω)$ which enjoys the strong Feller property. In particular, it takes values in $C(\overlineΩ)$. Its restriction to $C(\overlineΩ)$ is strongly continuous and holomorphic. We also establish positivity and contractivity of the semigroup under additional assumptions and study the asymptotic behavior of the semigroup.

math.FA

Diffusion with nonlocal boundary conditions

We consider second order differential operators $A_μ$ on a bounded, Dirichlet regular set $Ω\subset \mathbb{R}^d$, subject to the nonlocal boundary conditions \[ u(z) = \int_Ωu(x)\, μ(z, dx)\quad \mbox{for } z \in \partial Ω. \] Here the function $μ: \partialΩ\to \mathscr{M}^+(Ω)$ is $σ(\mathscr{M} (Ω), C_b(Ω))$-continuous with $0\leq μ(z,Ω) \leq 1$ for all $z\in \partial Ω$. Under suitable assumptions on the coefficients in $A_μ$, we prove that $A_μ$ generates a holomorphic positive contraction semigroup $T_μ$ on $L^\infty(Ω)$. The semigroup $T_μ$ is never strongly continuous, but it enjoys the strong Feller property in the sense that it consists of kernel operators and takes values in $C(\barΩ)$. We also prove that $T_μ$ is immediately compact and study the asymptotic behavior of $T_μ(t)$ as $t \to \infty$.

math.FA