{"title":"实线上三次塞格格方程的矩阵解","authors":"Ruoci Sun","doi":"10.1007/s11040-025-09500-8","DOIUrl":null,"url":null,"abstract":"<div><p>This paper is dedicated to studying matrix solutions of the cubic Szegő equation on the real line, which is introduced in Pocovnicu [Anal PDE 4(3):379–404, 2011; Dyn Syst A 31(3):607–649, 2011] and Gérard–Pushnitski (Commun Math Phys 405:167, 2024), leading to the following cubic matrix Szegő equation on <span>\\({\\mathbb {R}}\\)</span>, </p><div><div><span>$$\\begin{aligned} i \\partial _t U = \\Pi _{\\ge 0} \\left( U U ^* U \\right) , \\quad \\widehat{\\left( \\Pi _{\\ge 0} U\\right) }(\\xi )= {\\textbf{1}}_{\\xi \\ge 0}{\\hat{U}}(\\xi )\\in {\\mathbb {C}}^{M \\times N}. \\end{aligned}$$</span></div></div><p>Inspired by the space-periodic case in Sun (The matrix Szegő equation, arXiv:2309.12136), we establish its Lax pair structure via double Hankel operators and Toeplitz operators. Then the explicit formula in Gérard–Pushnitski (Commun Math Phys 405:167, 2024) can be extended to two equivalent formulas in the matrix equation case, which both express every solution explicitly in terms of its initial datum and the time variable.</p></div>","PeriodicalId":694,"journal":{"name":"Mathematical Physics, Analysis and Geometry","volume":"28 1","pages":""},"PeriodicalIF":0.9000,"publicationDate":"2025-03-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Matrix Solutions of the Cubic Szegő Equation on the Real Line\",\"authors\":\"Ruoci Sun\",\"doi\":\"10.1007/s11040-025-09500-8\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>This paper is dedicated to studying matrix solutions of the cubic Szegő equation on the real line, which is introduced in Pocovnicu [Anal PDE 4(3):379–404, 2011; Dyn Syst A 31(3):607–649, 2011] and Gérard–Pushnitski (Commun Math Phys 405:167, 2024), leading to the following cubic matrix Szegő equation on <span>\\\\({\\\\mathbb {R}}\\\\)</span>, </p><div><div><span>$$\\\\begin{aligned} i \\\\partial _t U = \\\\Pi _{\\\\ge 0} \\\\left( U U ^* U \\\\right) , \\\\quad \\\\widehat{\\\\left( \\\\Pi _{\\\\ge 0} U\\\\right) }(\\\\xi )= {\\\\textbf{1}}_{\\\\xi \\\\ge 0}{\\\\hat{U}}(\\\\xi )\\\\in {\\\\mathbb {C}}^{M \\\\times N}. \\\\end{aligned}$$</span></div></div><p>Inspired by the space-periodic case in Sun (The matrix Szegő equation, arXiv:2309.12136), we establish its Lax pair structure via double Hankel operators and Toeplitz operators. Then the explicit formula in Gérard–Pushnitski (Commun Math Phys 405:167, 2024) can be extended to two equivalent formulas in the matrix equation case, which both express every solution explicitly in terms of its initial datum and the time variable.</p></div>\",\"PeriodicalId\":694,\"journal\":{\"name\":\"Mathematical Physics, Analysis and Geometry\",\"volume\":\"28 1\",\"pages\":\"\"},\"PeriodicalIF\":0.9000,\"publicationDate\":\"2025-03-09\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Mathematical Physics, Analysis and Geometry\",\"FirstCategoryId\":\"100\",\"ListUrlMain\":\"https://link.springer.com/article/10.1007/s11040-025-09500-8\",\"RegionNum\":3,\"RegionCategory\":\"数学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"MATHEMATICS, APPLIED\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Mathematical Physics, Analysis and Geometry","FirstCategoryId":"100","ListUrlMain":"https://link.springer.com/article/10.1007/s11040-025-09500-8","RegionNum":3,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"MATHEMATICS, APPLIED","Score":null,"Total":0}
引用次数: 0
摘要
本文主要研究实数线上三次塞格格方程的矩阵解,在Pocovnicu [j] . PDE 4(3): 379-404, 2011;[j]和gsamrrad - pushnitski (comm Math Phys 405: 167,2024),推导出以下三次矩阵的塞格格方程 \({\mathbb {R}}\), $$\begin{aligned} i \partial _t U = \Pi _{\ge 0} \left( U U ^* U \right) , \quad \widehat{\left( \Pi _{\ge 0} U\right) }(\xi )= {\textbf{1}}_{\xi \ge 0}{\hat{U}}(\xi )\in {\mathbb {C}}^{M \times N}. \end{aligned}$$受太阳的空间周期情况的启发(矩阵塞格格方程,arXiv:2309.12136),我们利用双Hankel算子和Toeplitz算子建立了它的Lax对结构。然后,gsamrad - pushnitski (common Math Phys 405:167, 2024)中的显式公式可以推广为矩阵方程情况下的两个等效公式,它们都以初始基准和时间变量显式地表示每个解。
Matrix Solutions of the Cubic Szegő Equation on the Real Line
This paper is dedicated to studying matrix solutions of the cubic Szegő equation on the real line, which is introduced in Pocovnicu [Anal PDE 4(3):379–404, 2011; Dyn Syst A 31(3):607–649, 2011] and Gérard–Pushnitski (Commun Math Phys 405:167, 2024), leading to the following cubic matrix Szegő equation on \({\mathbb {R}}\),
$$\begin{aligned} i \partial _t U = \Pi _{\ge 0} \left( U U ^* U \right) , \quad \widehat{\left( \Pi _{\ge 0} U\right) }(\xi )= {\textbf{1}}_{\xi \ge 0}{\hat{U}}(\xi )\in {\mathbb {C}}^{M \times N}. \end{aligned}$$
Inspired by the space-periodic case in Sun (The matrix Szegő equation, arXiv:2309.12136), we establish its Lax pair structure via double Hankel operators and Toeplitz operators. Then the explicit formula in Gérard–Pushnitski (Commun Math Phys 405:167, 2024) can be extended to two equivalent formulas in the matrix equation case, which both express every solution explicitly in terms of its initial datum and the time variable.
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