On the Hardy constant of some non-convex planar domains

preprint2014arXivOpen access

Abstract

The Hardy constant of a simply connected domain Ω⊂R2Ω\subset\mathbf{R}^2 is the best constant for the inequality ∫Ω∣∇u∣2dx≥c∫Ωu2dist(x,∂Ω)2 dx  ,    u∈Cc∞(Ω). \int_Ω|\nabla u|^2dx \geq c\int_Ω \frac{u^2}{{\rm dist}(x,\partialΩ)^2}\, dx \; , \;\;\quad u\in C^{\infty}_c(Ω). After the work of Ancona where the universal lower bound 1/16 was obtained, there has been a substantial interest on computing or estimating the Hardy constant of planar domains. In \cite{BT} we have determined the Hardy constant of an arbitrary quadrilateral in the plane. In this work we continue our investigation and we compute the Hardy constant for other non-convex planar domains. In all cases the Hardy constant is related to that of a certain infinite sectorial region which has been studied by E.B. Davies.

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