On the best possible remaining term in the Hardy Inequality

We give a necessary and sufficient condition on a radially symmetric potential $V$ on $\Omega$ that makes it an admissible candidate for an improved Hardy inequality of the following form: \begin{equation}\label{gen-hardy.0} \hbox{$\int_{\Omega}|\nabla u |^{2}dx - (\frac{n-2}{2})^{2} \int_{\Omega}\frac{|u|^{2}}{|x|^{2}}dx\geq c\int_{\Omega} V(|x|)|u|^{2}dx$ \quad for all $u \in H^{1}_{0}(\Omega)$.} \end{equation}Comment: 13 pages. Updated versions --if any-- of this author's papers can be downloaded at http://pims.math.ca/~nassif

On the critical dimension of a fourth order elliptic problem with negative exponent

We study the regularity of the extremal solution of the semilinear biharmonic equation $\beta \Delta^2 u-\tau \Delta u=\frac{\lambda}{(1-u)^2}$ on a ball $B \subset \R^N$, under Navier boundary conditions $u=\Delta u=0$ on $\partial B$, where $\lambda >0$ is a parameter, while $\tau>0$, $\beta>0$ are fixed constants. It is known that there exists a $\lambda^{*}$ such that for $\lambda>\lambda^{*}$ there is no solution while for $\lambda<\lambda^{*}$ there is a branch of minimal solutions. Our main result asserts that the extremal solution $u^{*}$ is regular ($\sup_{B}u^{*}<1$) for $N\leq 8$ and $\beta, \tau>0$ and it is singular ($\sup_{B}u^{*}=1$) for $N\geq 9$, $\beta>0$, and $\tau>0$ with $\frac{\tau}{\beta}$ small. Our proof for the singularity of extremal solutions in dimensions $N\geq 9$ is based on certain improved Hardy-Rellich inequalities