Asymptotic analysis on positive solutions of the Lane-Emden system with nearly critical exponents

TL;DR

This paper analyzes the asymptotic behavior of positive solutions to the Lane-Emden system near critical exponents, revealing complex bubbling phenomena and establishing new methods for understanding blow-up rates and locations.

Contribution

It provides a detailed qualitative and quantitative analysis of bubbling solutions for the Lane-Emden system near critical exponents, including new techniques for blow-up analysis.

Findings

Multiple bubbling phenomena can occur under energy conditions.

Interaction between bubbles is strongly influenced by the parameter p.

One-bubble solutions are characterized for certain parameter ranges.

Abstract

We concern a family $\{(u_{\varepsilon},v_{\varepsilon})\}_{\varepsilon > 0}$ of solutions of the Lane-Emden system on a smooth bounded convex domain $\Omega$ in $\mathbb{R}^N$ \[\begin{cases} -\Delta u_{\varepsilon} = v_{\varepsilon}^p &\text{in } \Omega,\\ -\Delta v_{\varepsilon} = u_{\varepsilon}^{q_{\varepsilon}} &\text{in } \Omega,\\ u_{\varepsilon},\, v_{\varepsilon} > 0 &\text{in } \Omega,\\ u_{\varepsilon} = v_{\varepsilon} =0 &\text{on } \partial\Omega \end{cases}\] for $N \ge 4$, $\max\{1,\frac{3}{N-2}\} < p < q_{\varepsilon}$ and small \[\varepsilon := \frac{N}{p+1} + \frac{N}{q_{\varepsilon}+1} - (N-2) > 0.\] This system appears as the extremal equation of the Sobolev embedding $W^{2,(p+1)/p}(\Omega) \hookrightarrow L^{q_{\varepsilon}+1}(\Omega)$, and is also closely related to the Calder\'on-Zygmund estimate. Under the a natural energy condition \[\sup_{\varepsilon > 0} \left(\|u_{\varepsilon}\|_{W^{2,{p+1 \over p}}(\Omega)} + \|v_{\varepsilon}\|_{W^{2,{q_{\varepsilon}+1 \over q_{\varepsilon}}}(\Omega)}\right) < \infty,\] we prove that the multiple bubbling phenomena may arise for the family $\{(u_{\varepsilon},v_{\varepsilon})\}_{\varepsilon > 0}$, and establish a detailed qualitative and quantitative description. If $p < \frac{N}{N-2}$, the nonlinear structure of the system makes the interaction between bubbles so strong, so the determination process of the blow-up rates and locations is completely different from that of the classical Lane-Emden equation. If $p \ge \frac{N}{N-2}$, the blow-up scenario is relatively close to (but not the same as) that of the classical Lane-Emden equation, and only one-bubble solutions can exist. Even in the latter case, the standard approach does not work well, which forces us to devise a new method. Using our analysis, we also deduce a general existence theorem valid on any smooth bounded domains.