{ "id": "0802.4235", "version": "v1", "published": "2008-02-28T16:46:31.000Z", "updated": "2008-02-28T16:46:31.000Z", "title": "Generalized Bloch analysis and propagators on Riemannian manifolds with a discrete symmetry", "authors": [ "P. Kocabova", "P. Stovicek" ], "doi": "10.1063/1.2898484", "categories": [ "math-ph", "math.MP" ], "abstract": "We consider an invariant quantum Hamiltonian $H=-\\Delta_{LB}+V$ in the $L^{2}$ space based on a Riemannian manifold $\\tilde{M}$ with a countable discrete symmetry group $\\Gamma$. Typically, $\\tilde{M}$ is the universal covering space of a multiply connected Riemannian manifold $M$ and $\\Gamma$ is the fundamental group of $M$. On the one hand, following the basic step of the Bloch analysis, one decomposes the $L^{2}$ space over $\\tilde{M}$ into a direct integral of Hilbert spaces formed by equivariant functions on $\\tilde{M}$. The Hamiltonian $H$ decomposes correspondingly, with each component $H_{\\Lambda}$ being defined by a quasi-periodic boundary condition. The quasi-periodic boundary conditions are in turn determined by irreducible unitary representations $\\Lambda$ of $\\Gamma$. On the other hand, fixing a quasi-periodic boundary condition (i.e., a unitary representation $\\Lambda$ of $\\Gamma$) one can express the corresponding propagator in terms of the propagator associated to the Hamiltonian $H$. We discuss these procedures in detail and show that in a sense they are mutually inverse.", "revisions": [ { "version": "v1", "updated": "2008-02-28T16:46:31.000Z" } ], "analyses": { "keywords": [ "riemannian manifold", "generalized bloch analysis", "quasi-periodic boundary condition", "propagator", "unitary representation" ], "tags": [ "journal article" ], "publication": { "journal": "Journal of Mathematical Physics", "year": 2008, "month": "Mar", "volume": 49, "number": 3, "pages": "033518" }, "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable", "inspire": 791096, "adsabs": "2008JMP....49c3518K" } } }