Concentric bubbles concentrating in finite time for the energy critical wave maps equation

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Hauptverfasser: Jendrej, Jacek, Krieger, Joachim
Format: Preprint
Veröffentlicht: 2025
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author Jendrej, Jacek
Krieger, Joachim
author_facet Jendrej, Jacek
Krieger, Joachim
contents We show that the energy critical Wave Maps equation from $\mathbb{R}^{2+1}$ to $\mathbb{S}^2$ and restricted to the co-rotational setting with co-rotation index $k = 2$ admits finite time blow up solutions of finite energy on $(0, t_0]\times \mathbb{R}^2$, $t_0>0$, and concentrating two concentric bubble profiles at the frequency scales $λ_1(t) = e^{α(t)},\,α(t)\sim \big|\log t\big|^{β+1}$, as well as $λ_2(t) = t^{-1}\cdot \big|\log t\big|^β$. The parameter $β>\frac32$ can be chosen arbitrarily. This shows that soliton resolution scenarios with finite time blow up and $N = 2$ collapsing profiles, i. e. bubble trees, do occur for this equation.
format Preprint
id arxiv_https___arxiv_org_abs_2501_08396
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle Concentric bubbles concentrating in finite time for the energy critical wave maps equation
Jendrej, Jacek
Krieger, Joachim
Analysis of PDEs
35L05, 35B40
We show that the energy critical Wave Maps equation from $\mathbb{R}^{2+1}$ to $\mathbb{S}^2$ and restricted to the co-rotational setting with co-rotation index $k = 2$ admits finite time blow up solutions of finite energy on $(0, t_0]\times \mathbb{R}^2$, $t_0>0$, and concentrating two concentric bubble profiles at the frequency scales $λ_1(t) = e^{α(t)},\,α(t)\sim \big|\log t\big|^{β+1}$, as well as $λ_2(t) = t^{-1}\cdot \big|\log t\big|^β$. The parameter $β>\frac32$ can be chosen arbitrarily. This shows that soliton resolution scenarios with finite time blow up and $N = 2$ collapsing profiles, i. e. bubble trees, do occur for this equation.
title Concentric bubbles concentrating in finite time for the energy critical wave maps equation
topic Analysis of PDEs
35L05, 35B40
url https://arxiv.org/abs/2501.08396