Localization of bubbling for high order nonlinear equations
Frédéric Robert
Abstract
We analyze the asymptotic pointwise behavior of families of solutions to the high-order critical equation $$P_αu_α=Δ_g^k u_α+\hbox{lot}=|u_α|^{2^\star-2-ε_α} u_α\hbox{ in }M$$ that behave like $$u_α=u_0+B_α+o(1)\hbox{ in }H_k^2(M)$$ where $B=(B_α)_α$ is a Bubble, also called a Peak. We give obstructions for such a concentration to occur: depending on the dimension, they involve the mass of the associated Green's function or the difference between $P_α$ and the conformally invariant GJMS operator. The bulk of this analysis is the proof of the pointwise control \begin{equation*} |u_α(x)|\leq C\Vert u_0\Vert_\infty^{(2^\star-1)^2}+C\left(\frac{μ_α^{2}}{μ_α^{2 }+d_g(x,x_α)^{2 }}\right)^{\frac{n-2k}{2}}\hbox{ for all }x\in M\hbox{ and }α\in\mathbb{N}, \end{equation*} where $|u_α(x_α)|=\max_M|u_α|\to +\infty$ and $μ_α:=|u_α(x_α)|^{-\frac{2}{n-2k}}$. The key to obtain this estimate is a sharp control of the Green's function for elliptic operators involving a Hardy potential.
