{ "id": "hep-th/0007019", "version": "v4", "published": "2000-07-03T22:54:53.000Z", "updated": "2000-11-15T22:00:35.000Z", "title": "Non-Linear Electrodynamics in Curved Backgrounds", "authors": [ "Gary W. Gibbons", "Koji Hashimoto" ], "comment": "35 pages, LaTeX, Comments and references added, a part of Sec. 5.1 deleted, published version", "journal": "JHEP 0009:013,2000", "doi": "10.1088/1126-6708/2000/09/013", "categories": [ "hep-th" ], "abstract": "We study non-linear electrodynamics in curved space from the viewpoint of dualities. After establishing the existence of a topological bound for self-dual configurations of Born-Infeld field in curved space, we check that the energy-momentum tensor vanishes. These properties are shown to hold for general duality-invariant non-linear electrodynamics. We give the dimensional reduction of Born-Infeld action to three dimensions in a general curved background admitting a Killing vector. The SO(2) duality symmetry becomes manifest but other symmetries present in flat space are broken, as is U-duality when one couples to gravity. We generalize our arguments on duality to the case of n U(1) gauge fields, and present a new Lagrangian possessing SO(n) X SO(2)_elemag duality symmetry. Other properties of this model such as Legendre duality and enhancement of the symmetry by adding dilaton and axion, are studied. We extend our arguments to include a background b-field in the curved space, and give new examples including almost Kaehler manifolds and Schwarzshild black holes with a $b$-field.", "revisions": [ { "version": "v4", "updated": "2000-11-15T22:00:35.000Z" } ], "analyses": { "keywords": [ "curved space", "duality symmetry", "general duality-invariant non-linear electrodynamics", "energy-momentum tensor vanishes", "schwarzshild black holes" ], "tags": [ "journal article" ], "publication": { "publisher": "IOP", "journal": "J. High Energ. Phys." }, "note": { "typesetting": "LaTeX", "pages": 35, "language": "en", "license": "arXiv", "status": "editable", "inspire": 529614 } } }