Quantitative quasi-invariance of Gaussian measures below the energy level for the 1D generalized nonlinear Schrödinger equation and application to global well-posedness
Alexis Knezevitch
TL;DR
This work proves almost-sure global well-posedness for the 1D periodic nonlinear Schrödinger equation with odd nonlinearities $p\ge 5$ for rough Gaussian initial data below the energy level. The authors blend a deterministic local Cauchy theory with a probabilistic globalization that leverages the quasi-invariance of Gaussian measures $\mu_s$ under the flow, together with $L^q$ bounds on Radon-Nikodym derivatives. Central to the approach are the renormalized energy and a Boué-Dupuis variational framework, augmented by a Poincaré-Dulac normal form reduction to control resonant interactions. The result yields a global flow for $\mu_s$-typical initial data with polynomial-in-time Sobolev-norm growth and establishes a robust probabilistic globalization parallel to Bourgain’s invariant-measure strategy, informed by recent developments on transport and quasi-invariance. The techniques provide a template for combining deterministic and probabilistic methods to achieve global behavior for dispersive PDEs with rough random data.
Abstract
We consider the Schrödinger equation on the one dimensional torus with a general odd-power nonlinearity $p \geq 5$, which is known to be globally well-posed in the Sobolev space $H^σ(\mathbb{T})$, for every $σ\geq 1$, thanks to the conservation and finiteness of the energy. For regularities $σ< 1$, where this energy is infinite, we explore a globalization argument adapted to random initial data distributed according to the Gaussian measures $μ_s$, with covariance operator $(1-Δ)^s$, for $s$ in a range $(s_p,\frac{3}{2}]$. We combine a deterministic local Cauchy theory with the quasi-invariance of Gaussian measures $μ_s$, with additional $L^q$-bounds on the Radon-Nikodym derivatives, to prove that the Gaussian initial data generate almost surely global solutions. These $L^q$-bounds are obtained with respect to Gaussian measures accompanied by a cutoff on a renormalization of the energy; the main tools to prove them are the Boué-Dupuis variational formula and a Poincaré-Dulac normal form reduction. This approach is similar in spirit to Bourgain's invariant argument and to a recent work by Forlano-Tolomeo.
