Long finite time bubble trees for two co-rotational wave maps

Abstract

We show that the energy critical Wave Maps equation from $\mathbb{R}^{2+1}$ into $\mathbb{S}^2$, restricted to the $k=2$ co-rotational setting, admits arbitrarily large numbers of concentrating concentric $n$ bubble profiles. For any $n\in\mathbb{N}$, we construct an $n$-bubble solution concentrating at scales $λ_1(t)\gg λ_2(t)\gg \ldots\gg λ_n(t)$, where $λ_n(t)=t^{-1}\vert \log t\vert^β$, and $λ_j(t)\gtrsim \exp( \int_t^{t_0} λ_{j+1}(s)ds)$, for any $j<n$. Here $β>\tfrac32$ is a parameter that can be chosen arbitrarily. This shows that, as far as finite time blow-up case is concerned, the entirety of cases postulated in the soliton resolution theorem indeed occur, provided the concentric collapsing bubbles have alternating signs.

Theorems & Definitions (45)

• Theorem 1.1
• Theorem 2.1
• Proposition 4.1: JenKri
• Proposition 4.2: JenKri
• Proposition 4.3
• Proposition 4.4: KST3
• Proposition 4.5
• Lemma 5.1
• proof
• Proposition 5.2