{ "id": "1508.07747", "version": "v1", "published": "2015-08-31T10:03:17.000Z", "updated": "2015-08-31T10:03:17.000Z", "title": "Eigenfunction expansions for the Schrödinger equation with inverse-square potential", "authors": [ "A. G. Smirnov" ], "comment": "20 pages, to appear in a special issue of Theoretical and Mathematical Physics dedicated to I.V. Tyutin on the occasion of his 75th birthday", "categories": [ "math-ph", "math.MP", "math.SP" ], "abstract": "The one-dimensional Schr\\\"odinger equation $-f\"+q_\\kappa f = Ef$ on the positive semi-axis with the potential $q_\\kappa(r)=(\\kappa^2-1/4)r^{-2}$ is considered. For each complex number $\\vartheta$, we construct a solution $u^\\kappa_\\vartheta(E)$ of this equation that is analytic in $\\kappa$ in a complex neighborhood of the interval $(-1,1)$ and, in particular, at the \"singular\" point $\\kappa = 0$. For $-1<\\kappa<1$ and real $\\vartheta$, the solutions $u^\\kappa_\\vartheta(E)$ determine a unitary eigenfunction expansion operator $U_{\\kappa,\\vartheta}\\colon L_2(0,\\infty)\\to L_2(\\mathbb R,\\mathcal V_{\\kappa,\\vartheta})$, where $\\mathcal V_{\\kappa,\\vartheta}$ is a positive measure on $\\mathbb R$. It is shown that every self-adjoint realization of the formal differential expression $-\\partial^2_r + q_\\kappa(r)$ for the Hamiltonian is diagonalized by the operator $U_{\\kappa,\\vartheta}$ for some $\\vartheta\\in\\mathbb R$. Using suitable singular Titchmarsh-Weyl $m$-functions, we explicitly find the measures $\\mathcal V_{\\kappa,\\vartheta}$ and prove their continuity in $\\kappa$ and $\\vartheta$.", "revisions": [ { "version": "v1", "updated": "2015-08-31T10:03:17.000Z" } ], "analyses": { "keywords": [ "schrödinger equation", "inverse-square potential", "unitary eigenfunction expansion operator", "formal differential expression", "complex number" ], "note": { "typesetting": "TeX", "pages": 20, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2015arXiv150807747S" } } }