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We investigate the blow-up dynamics for the $L^2$ critical two-dimensional Zakharov-Kuznetsov equation \begin{equation*} \begin{cases} \partial_t u+\partial_{x_1} (\Delta u+u^3)=0, \mbox{ } x=(x_1,x_2)\in \mathbb{R}^2, \mbox{ } t \in…

Analysis of PDEs · Mathematics 2024-11-26 Francisc Bozgan , Tej-Eddine Ghoul , Nader Masmoudi , Kai Yang

We consider positive solutions for the fractional heat equation with critical exponent \begin{equation*} \begin{cases} u_t = -(-\Delta)^{s}u + u^{\frac{n+2s}{n-2s}}\text{ in } \Omega\times (0, \infty), u = 0\text{ on }…

Analysis of PDEs · Mathematics 2018-05-25 M. Musso , Y. Sire , J. Wei , Z. Zheng , Y. Zhou

We consider $L^2$-critical focusing nonlinear Schroedinger equations with Hartree type nonlinearity $$i \pr_t u = -\DD u - \big (\Phi \ast |u|^2 \big) u \quad {in $\RR^4$},$$ where $\Phi(x)$ is a perturbation of the convolution kernel…

Analysis of PDEs · Mathematics 2011-11-30 Joachim Krieger , Enno Lenzmann , Pierre Raphael

We prove the existence of energy solutions of the energy critical focusing wave equation in R^3 which blow up exactly at x=t=0. They decompose into a bulk term plus radiation term. The bulk is a rescaled version of the stationary "soliton"…

Analysis of PDEs · Mathematics 2007-05-23 Joachim Krieger , Wilhelm Schlag , Daniel Tataru

We prove that if $u(t)$ is a log-log blow-up solution, of the type studied by Merle-Rapha\"el (2001-2005), to the $L^2$ critical focusing NLS equation $i\partial_t u +\Delta u + |u|^{4/d} u=0$ with initial data $u_0\in H^1(\mathbb{R}^d)$ in…

Analysis of PDEs · Mathematics 2010-07-08 Justin Holmer , Svetlana Roudenko

We consider the energy-critical (corotational) 1-equivariant wave maps into the two-sphere. By the seminal work [53] of Rapha\"el and Rodnianski, there is an open set of initial data whose forward-in-time development blows up in finite time…

Analysis of PDEs · Mathematics 2023-09-11 Kihyun Kim

We consider closed immersed surfaces in R^3 evolving by the geometric triharmonic heat flow. Using local energy estimates, we prove interior estimates and a positive absolute lower bound on the lifespan of solutions depending solely on the…

Analysis of PDEs · Mathematics 2015-02-02 James McCoy , Scott Parkins , Glen Wheeler

We consider the energy super critical 4 dimensional semilinear heat equation $$\partial_tu=\Delta u+|u|^{p-1}u, \ \ x\in \Bbb R^4, \ \ p>5.$$ Let $\Phi(r)$ be a three dimensional radial self similar solution for the three supercritical…

Analysis of PDEs · Mathematics 2017-09-18 Frank Merle , Pierre Raphael , Jeremie Szeftel

In this paper we consider the slightly $L^2$-supercritical gKdV equations $\partial_t u+(u_{xx}+u|u|^{p-1})_x=0$, with the nonlinearity $5<p<5+\varepsilon$ and $0<\varepsilon\ll 1$ . We will prove the existence and stability of a blow-up…

Analysis of PDEs · Mathematics 2016-09-19 Yang Lan

We consider the energy critical Schrodinger map to the 2-sphere for equivariant initial data of homotopy number k=1. We show the existence of a set of smooth initial data arbitrarily close to the ground state harmonic map in the scale…

Analysis of PDEs · Mathematics 2011-02-25 Frank Merle , Pierre Raphael , Igor Rodnianski

We consider the energy critical four dimensional semi-linear heat equation \[ \partial_{t}v-\Delta v-v^{3}=0, \quad(t,x)\in \mathbb{R}\times \mathbb{R}^4. \] Formal computation of Filippas et al. (R. Soc. Lond. Proc. 2000) conjectures the…

Analysis of PDEs · Mathematics 2022-04-26 Tongtong Li , Liming Sun , Shumao Wang

In this paper, we consider the Yang-Mills heat flow on $\mathbb R^d \times SO(d)$ with $d \ge 11$. Under a certain symmetry preserved by the flow, the Yang-Mills equation can be reduced to: $$ \partial_t u =\partial_r^2 u +\frac{d+1}{r}…

Analysis of PDEs · Mathematics 2024-01-08 A. Bensouilah , G. K. Duong , T. E. Ghoul

We consider the semilinear heat equation \begin{eqnarray*} \partial_t u = \Delta u + |u|^{p-1} u \ln ^{\alpha}( u^2 +2), \end{eqnarray*} in the whole space $\mathbb{R}^n$, where $p > 1$ and $ \alpha \in \mathbb{R}$. Unlike the standard case…

Analysis of PDEs · Mathematics 2018-03-28 G. K. Duong , V. T. Nguyen , H. Zaag

In this paper, we will study the existence of finite time singularity to harmonic heat flow and their formation patterns. After works of Coron-Ghidaglia, Ding and Chen-Ding, one knows blow-up solutions under smallness of initial energy for…

Analysis of PDEs · Mathematics 2021-12-30 Shi-Zhong Du

We construct the first example of finite time blow-up solutions for the heat flow of the $H$-system, describing the evolution of surfaces with constant mean curvature \begin{equation*} \left\{ \begin{aligned} &u_t = \Delta u -…

Analysis of PDEs · Mathematics 2023-11-27 Yannick Sire , Juncheng Wei , Youquan Zheng , Yifu Zhou

The focusing cubic wave equation in three spatial dimensions has the explicit solution $\sqrt{2}/t$. We study the stability of the blowup described by this solution as $t \to 0$ without symmetry restrictions on the data. Via the conformal…

Analysis of PDEs · Mathematics 2017-05-16 Annegret Y. Burtscher , Roland Donninger

We construct finite time blow-up solutions to the 3-dimensional harmonic map flow into the sphere $S^2$, \begin{align*} u_t & = \Delta u + |\nabla u|^2 u \quad \text{in } \Omega\times(0,T) \\ u &= u_b \quad \text{on } \partial…

Analysis of PDEs · Mathematics 2019-02-12 Juan Davila , Manuel Del Pino , Catalina Pesce , Juncheng Wei

We fully revisit the near soliton dynamics for the mass critical (gKdV) equation. In Part I, for a class of initial data close to the soliton, we prove that only three scenario can occur: (BLOW UP) the solution blows up in finite time $T$…

Analysis of PDEs · Mathematics 2012-04-24 Yvan Martel , Frank Merle , Pierre Raphael

We construct a two-parameter continuum of type II blow up solutions for the energy-critical focusing NLS in dimension $ d = 3$. The solutions collapse to a single energy bubble in finite time, precisely they have the form $ u(t,x) = e^{i…

Analysis of PDEs · Mathematics 2025-10-03 Tobias Schmid

We consider the energy critical semilinear heat equation $$ \left\{\begin{aligned} &\partial_t u-\Delta u =|u|^{\frac{4}{n-2}}u &\mbox{in } {\mathbb R}^n\times(0,T),\\ &u(x,0)=u_0(x), \end{aligned}\right. $$ where $ n\geq 3$, $u_0\in…

Analysis of PDEs · Mathematics 2021-01-19 Kelei Wang , Juncheng Wei