For example, for $$ -\Delta u=f(u) \quad \text { in } \Omega, $$ we call a solution is stable if $$ Q_u(\varphi):=\int_{\Omega}|\nabla \varphi|^2 d x-\int_{\Omega} f^{\prime}(u) \varphi^2 d x \geq 0, \quad \forall \varphi \in C_c^1(\Omega) . $$ Here $Q_u(\varphi)$ is the second variation of its energy functional.
And the Morse index is defined by the maximal dimension of space $K_\varphi$ in which $Q_u(\varphi) <0$.
I want to ask a naive question about the stable solution. $Q_u(\varphi) \ge0$ means local minimum, the Morse index is defined by the maximal dimension of space $K_\varphi$ in which $Q_u(\varphi) <0$, if we consider infinite Morse index, it should be possible that $Q_u(\varphi) <0, \forall \varphi \in C_c^1(\Omega)$, so a local maximum. Is there something I misunderstood, thank you!
My thoughts: For the questions that we have proved no stable solution (so no local minimum), maybe we should set $v=-u$ and study the $$ -\Delta v=-f(-v) \quad \text { in } \Omega $$ again. I think the method should be the same, so local minimum of $u$ is the local maximum of $v$, local maximum of $u$ is the local minimum of $v$, so no local maximum for $u$?