{"title":"On the intertwining map between Coulomb and hyperbolic scattering","authors":"Nicholas Lohr","doi":"arxiv-2408.16248","DOIUrl":null,"url":null,"abstract":"We construct a unitary operator between Hilbert spaces of generalized\neigenfunctions of Coulomb operators and the Laplace-Beltrami operator of\nhyperbolic space that intertwines their respective Poisson operators on\n$L^2(\\mathbb{S}^{d-1})$. The constructed operator generalizes Fock's unitary\ntransformation, originally defined between the discrete spectra of the\nattractive Coulomb operator and the Laplace-Beltrami operator on the sphere, to\nthe setting of continuous spectra. Among other connections, this map explains\nwhy the scattering matrices are the same in these two different settings, and\nit also provides an explicit formula for the Poisson operator of the Coulomb\nHamiltonian.","PeriodicalId":501373,"journal":{"name":"arXiv - MATH - Spectral Theory","volume":"1 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-08-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - MATH - Spectral Theory","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2408.16248","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
We construct a unitary operator between Hilbert spaces of generalized
eigenfunctions of Coulomb operators and the Laplace-Beltrami operator of
hyperbolic space that intertwines their respective Poisson operators on
$L^2(\mathbb{S}^{d-1})$. The constructed operator generalizes Fock's unitary
transformation, originally defined between the discrete spectra of the
attractive Coulomb operator and the Laplace-Beltrami operator on the sphere, to
the setting of continuous spectra. Among other connections, this map explains
why the scattering matrices are the same in these two different settings, and
it also provides an explicit formula for the Poisson operator of the Coulomb
Hamiltonian.