Blowup for Biharmonic NLS

TL;DR

This paper investigates finite-time blowup phenomena for the focusing biharmonic nonlinear Schrödinger equation across various dimensions and nonlinearities, introducing a new analytical tool called the localized Riesz bivariance.

Contribution

It establishes blowup results for radial data in $H^2$ for different nonlinear regimes and introduces the localized Riesz bivariance as a new analytical method.

Findings

Proves finite-time blowup for supercritical nonlinearities in any dimension.

Derives a universal upper bound for blowup rate in certain regimes.

Establishes a radial symmetry result for ground states of biharmonic NLS.

Abstract

We consider the Cauchy problem for the biharmonic (i.\,e.~fourth-order) NLS with focusing nonlinearity given by $i \partial_t u = \Delta^2 u - \mu \Delta u -|u|^{2 \sigma} u$ for $(t,x) \in [0,T) \times \mathbb{R}^d$, where $0 < \sigma <\infty$ for $d \leq 4$ and $0 < \sigma \leq 4/(d-4)$ for $d \geq 5$; and $\mu \in \mathbb{R}$ is some parameter to include a possible lower-order dispersion. In the mass-supercritical case $\sigma > 4/d$, we prove a general result on finite-time blowup for radial data in $H^2(\mathbb{R}^d)$ in any dimension $d \geq 2$. Moreover, we derive a universal upper bound for the blowup rate for suitable $4/d < \sigma < 4/(d-4)$. In the mass-critical case $\sigma=4/d$, we prove a general blowup result in finite or infinite time for radial data in $H^2(\mathbb{R}^d)$. As a key ingredient, we utilize the time evolution of a nonnegative quantity, which we call the (localized) Riesz bivariance for biharmonic NLS. This construction provides us with a suitable substitute for the variance used for classical NLS problems. In addition, we prove a radial symmetry result for ground states for the biharmonic NLS, which may be of some value for the related elliptic problem.