{ "id": "1209.2021", "version": "v1", "published": "2012-09-10T15:06:59.000Z", "updated": "2012-09-10T15:06:59.000Z", "title": "Dirac operator on spinors and diffeomorphisms", "authors": [ "Ludwik Dabrowski", "Giacomo Dossena" ], "comment": "13 pages", "journal": "Class. Quantum Grav. 30 015006 (2013)", "doi": "10.1088/0264-9381/30/1/015006", "categories": [ "math-ph", "math.MP" ], "abstract": "The issue of general covariance of spinors and related objects is reconsidered. Given an oriented manifold $M$, to each spin structure $\\sigma$ and Riemannian metric $g$ there is associated a space $S_{\\sigma, g}$ of spinor fields on $M$ and a Hilbert space $\\HH_{\\sigma, g}= L^2(S_{\\sigma, g},\\vol{M}{g})$ of $L^2$-spinors of $S_{\\sigma, g}$. The group $\\diff{M}$ of orientation-preserving diffeomorphisms of $M$ acts both on $g$ (by pullback) and on $[\\sigma]$ (by a suitably defined pullback $f^*\\sigma$). Any $f\\in \\diff{M}$ lifts in exactly two ways to a unitary operator $U$ from $\\HH_{\\sigma, g} $ to $\\HH_{f^*\\sigma,f^*g}$. The canonically defined Dirac operator is shown to be equivariant with respect to the action of $U$, so in particular its spectrum is invariant under the diffeomorphisms.", "revisions": [ { "version": "v1", "updated": "2012-09-10T15:06:59.000Z" } ], "analyses": { "subjects": [ "53C27", "15A66", "34L40", "57S05" ], "keywords": [ "diffeomorphisms", "riemannian metric", "spin structure", "spinor fields", "general covariance" ], "tags": [ "journal article" ], "publication": { "publisher": "IOP", "journal": "Classical and Quantum Gravity", "year": 2013, "month": "Jan", "volume": 30, "number": 1, "pages": "015006" }, "note": { "typesetting": "TeX", "pages": 13, "language": "en", "license": "arXiv", "status": "editable", "inspire": 1185172, "adsabs": "2013CQGra..30a5006D" } } }