New estimates for the Hardy constants of multipolar Schrödinger operators
arXiv:1402.5933 · doi:10.1142/S0219199715500935
Abstract
In this paper we study the optimization problem $$μ^\star(Ω):=\inf_{u\in \semi}\frac{\into |\n u|^2 \dx}{\into V u^2 \dx}$$ in a suitable functional space $\semi$. Here, is the multi-singular potential given by and all the singular poles , , arise either in the interior or at the boundary of a smooth open domain $Ω\subset \rr^N$, with or , respectively. For a bounded domain containing all the singularities in the interior, we prove that $μ^\star(Ω)>μ^\star(\rr^N)$ when and $μ^\star(Ω)=μ^\star(\rr^N)$ when (It is known from \cite{cristi1} that $μ^\star(\rr^N)=(N-2)^2/n^2)$. In the situation when all the poles are located on the boundary we show that if is either a ball, the exterior of a ball or a half-space. Our results do not depend on the distances between the poles. In addition, in the case of boundary singularities we obtain that is attained in $\hoi$ when is a ball and . Besides, is attained in $\semi$ when is the exterior of a ball with and whereas in the case of a half-space is attained in $\semi$ when . We also analyze the critical constants in the so-called \textit{weak} Hardy inequality which characterizes the range of ensuring the existence of a lower bound for the spectrum of the Schrödinger operator . In the context of both interior and boundary singularities we show that the critical constants in the weak Hardy inequality are and , respectively.
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