$$\mathbb {R}^d\times \mathbb {T}^m$$ 上非线性薛定谔方程的 Legendre-Fenchel Identity : 理论与应用

Yongming Luo
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摘要

本文的灵感来源于作者之前的一项工作,即研究聚焦三次非线性薛定谔方程(NLS)在 \(\mathbb {R}^2\times \mathbb {T}\)上的大数据散射问题。然而,这篇论文的结果并不尖锐,因为我们甚至无法证明在所设定的阈值上存在基态解。通过利用半三次 Vanishing 几何学,我们在本文中建立了锐化散射结果。然而,由于模型的质量临界性质,我们遇到了一个重大挑战,即标准缩放论证无法扰动能量函数。我们通过证明具有规定质量和频率的变分问题的关键 Legendre-Fenchel 特性来克服这一困难。更准确地说,我们建立了一个基于 Legendre-Fenchel 特性的一般框架,并证明了在规定质量下更难甚至无法解决的变分问题,实际上可以通过考虑规定频率下更容易解决的变分问题来等效解决。作为显示域的几何形状如何影响基态解的存在的一个应用,我们还证明了虽然所有在\(\mathbb {R}^d\) 上的质量临界基态必须具有固定质量\({\widehat{M}}(Q)\),但在\(\mathbb {R}^d\times \mathbb {T}/)上的质量临界基态的存在对于质量数趋近于零的序列是有保证的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
A Legendre–Fenchel Identity for the Nonlinear Schrödinger Equations on $$\mathbb {R}^d\times \mathbb {T}^m$$ : Theory and Applications

The present paper is inspired by a previous work of the author, where the large data scattering problem for the focusing cubic nonlinear Schrödinger equation (NLS) on \(\mathbb {R}^2\times \mathbb {T}\) was studied. Nevertheless, the results from the companion paper are by no means sharp, as we could not even prove the existence of ground state solutions on the formulated threshold. By making use of the semivirial-vanishing geometry, we establish in this paper the sharpened scattering results. Yet due to the mass-critical nature of the model, we encounter the major challenge that the standard scaling arguments fail to perturb the energy functionals. We overcome this difficulty by proving a crucial Legendre–Fenchel identity for the variational problems with prescribed mass and frequency. More precisely, we build up a general framework based on the Legendre–Fenchel identity and show that the much harder or even unsolvable variational problem with prescribed mass, can in fact be equivalently solved by considering the much easier variational problem with prescribed frequency. As an application showing how the geometry of the domain affects the existence of the ground state solutions, we also prove that while all mass-critical ground states on \(\mathbb {R}^d\) must possess the fixed mass \({\widehat{M}}(Q)\), the existence of mass-critical ground states on \(\mathbb {R}^d\times \mathbb {T}\) is ensured for a sequence of mass numbers approaching zero.

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