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超越 $\sigma=2p$ 的临界拟线性 Hartree 方程的相变、尖锐渐近与对称性

Phase transition, sharp asymptotics and symmetry for critical quasilinear Hartree equations beyond $σ=2p$

Phuong Le

arXiv 2610.00339首次发表:更新:

发表机构

University of Economics and Law; Vietnam National University(经济与法律大学; 越南国立大学)

机构由 AI 辅助整理,请以论文原文为准。

AI 中文总结

本文研究互补范围 $2p<\sigma<N$ 内临界拟线性 Hartree 方程的尖锐渐近与对称性,揭示了由 $\sigma(p-2)+2p$ 符号控制的相变,并证明解径向对称且严格递减。

AI 中文摘要

我们建立了临界拟线性 Hartree 方程 \\[ -\Delta_pu=\big(|x|^{-\sigma}*u^{p^*_{\sigma}}\big)u^{p^*_{\sigma}-1} \quad\text{在 }\mathbb R^N \text{ 中}, \qquad p^*_{\sigma}=\frac{p(2N-\sigma)}{2(N-p)}, \\] 在互补范围 $2p<\sigma<N$ 内的尖锐渐近与对称性理论,超越了先前适用于 $\sigma\le2p$ 的拟线性理论 [Math. Ann., 391(2):2653--2708, 2025]。该范围在结构上有所不同:$p^*_{\sigma}<p$,因此通过提取因子 $u^{p-1}$ 得到的有效势在 $u\to0$ 时变得奇异。尽管如此,只要 $p^*_{\sigma}>1$,每个非负有限能量弱解自动局部有界。我们的证明提供了一种适用于该互补范围的拟线性正则性机制,而适用于 $\sigma\le2p$ 的位势论途径在此失效。对于满足 $p^*_{\sigma}>1$ 的正有限能量解,我们还揭示了由 $\sigma(p-2)+2p$ 的符号控制的尖锐转变。若该量为正,则经典的 $p$-调和轮廓得以保持。在阈值处,\\[ u(x)\simeq |x|^{-\gamma_h}(\log|x|)^{1/(p-p^*_{\sigma})}, \qquad \gamma_h=\frac{N-p}{p-1}, \\] 并具有匹配的双侧梯度速率。低于阈值时,\\[ u(x)=A_*|x|^{-\gamma_*}+o(|x|^{-\gamma_*}), \qquad \gamma_*=\frac{2(N-p)(\sigma-p)}{p(\sigma-2p)}<\gamma_h, \\] 且重标度后的梯度一致收敛到相应的径向轮廓。在所有三种情形中,解关于某一点径向对称,并沿径向变量严格递减。

英文摘要

We establish the sharp asymptotic and symmetry theory for the critical quasilinear Hartree equation \[ -Δ_pu=\big(|x|^{-σ}*u^{p^*_σ}\big)u^{p^*_σ-1} \quad\text{in }\mathbb R^N, \qquad p^*_σ=\frac{p(2N-σ)}{2(N-p)}, \] in the complementary range $2p<σ<N$, beyond the quasilinear theory previously available for $σ\le2p$ [Math. Ann., 391(2):2653--2708, 2025]. This range is structurally different: $p^*_σ<p$, so the effective potential obtained by factoring out $u^{p-1}$ becomes singular as $u\to0$. Nevertheless, whenever $p^*_σ>1$, every nonnegative finite-energy weak solution is automatically locally bounded. Our proof provides a quasilinear regularity mechanism adapted to this complementary range, where the potential-theoretic route available for $σ\le2p$ breaks down. For positive finite-energy solutions with $p^*_σ>1$ we moreover uncover a sharp transition governed by the sign of $σ(p-2)+2p$. If this quantity is positive, the classical $p$-harmonic profile persists. At the threshold, \[ u(x)\simeq |x|^{-γ_h}(\log|x|)^{1/(p-p^*_σ)}, \qquad γ_h=\frac{N-p}{p-1}, \] with the matching two-sided gradient rate. Below the threshold, \[ u(x)=A_*|x|^{-γ_*}+o(|x|^{-γ_*}), \qquad γ_*=\frac{2(N-p)(σ-p)}{p(σ-2p)}<γ_h, \] and the rescaled gradients converge uniformly to the corresponding radial profile. In all three regimes the solutions are radially symmetric about some point and strictly decreasing in the radial variable.

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