Refined Strichartz estimates and their orthornomal counterparts for Schrödinger equations on torus
The aim of the paper is twofold. We establish refined Strichartz estimates for the Schrödinger equation on tori within the framework of partial regularity. As a result, we reveal that the solution of the free Schrödinger equation has better regularity in mixed Lebesgue spaces. This complements the well-established theory over the past few decades, where initial data comes from the Sobolev space with respect to all spatial variables. As an application, we obtain local well-posedness for non-gauge-invariant nonlinearities with partially regular initial data. On the other hand, we extend refined Strichartz estimates for infinite systems of orthonormal functions, which generalizes the classical orthonormal Strichartz estimates on the torus by Nakamura [41] . As an application, we establish well-posedness for the Hartree equation for infinitely many fermions in some Schatten spaces. In the process, we develop several harmonic analysis tools for mixed Lebesgue spaces, e.g. Fourier multiplier transference principle, vector-valued Bernstein inequality, and vector-valued Littlewood–Paley theory for densities of operators, which may be of independent interest and complement the results of [45,55].
💡 Research Summary
The paper investigates the Schrödinger equation on the torus $\mathbb T^{d}$ from a novel “partial regularity’’ perspective and derives refined Strichartz estimates both for single functions and for orthonormal families. Classical Strichartz estimates on compact manifolds suffer from a loss of derivatives because the dispersive decay (the $L^\infty_x$ bound) is absent. Earlier works (Bourgain, Burq‑Gérard‑Tzvetkov, Dinh) obtained estimates with a $1/q$ loss in Sobolev regularity, but they require the initial data to belong to the full Sobolev space $H^{s}(\mathbb T^{d})$.
Partial regularity framework.
The authors split the spatial variable $z=(x,y)\in\mathbb T^{d-k}\times\mathbb T^{k}$ with $1\le k<d$ and introduce the mixed Sobolev space
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