Phase space analysis of the Hermite semigroup and applications to nonlinear global well-posedness

Abstract

We study the Hermite operator $H=-\Delta +|x{|}^2$ in ${\mathbb{R}}^d$ and its fractional powers $H^{\beta }$, $\beta >0$ in phase space. Namely, we represent functions $f$ via the so-called short-time Fourier, alias Fourier-Wigner or Bargmann transform $V_{g}f$ ($g$ being a fixed window function), and we measure their regularity and decay by means of mixed Lebesgue norms in phase space of $V_{g}f$, that is in terms of membership to modulation spaces $M^{p,q}$, $0<p,q\le \infty$. We prove the complete range of fixed-time estimates for the semigroup $e^{-t{H}^{\beta }}$ when acting on $M^{p,q}$, for every $0<p,q\le \infty$, exhibiting the optimal global-in-time decay as well as phase-space smoothing. As an application, we establish global well-posedness for the nonlinear heat equation for $H^{\beta }$ with power-type nonlinearity (focusing or defocusing), with small initial data in modulation spaces or in Wiener amalgam spaces. We show that such a global solution exhibits the same optimal decay $e^{-ct}$ as the solution of the corresponding linear equation, where $c=d^{\beta }$ is the bottom of the spectrum of $H^{\beta }$. This is in sharp contrast to what happens for the nonlinear focusing heat equation without potential, where blow-up in finite time always occurs for (even small) constant initial data - hence in $M^{\infty ,1}$.

18 pages