{ "id": "1512.06182", "version": "v1", "published": "2015-12-19T03:10:08.000Z", "updated": "2015-12-19T03:10:08.000Z", "title": "Entanglement entropy of a Maxwell field on the sphere", "authors": [ "Horacio Casini", "Marina Huerta" ], "comment": "18 pages, 5 figures", "categories": [ "hep-th" ], "abstract": "We compute the logarithmic coefficient of the entanglement entropy on a sphere for a Maxwell field in $d=4$ dimensions. In spherical coordinates the problem decomposes into one dimensional ones along the radial coordinate for each angular momentum. We show the entanglement entropy of a Maxwell field is equivalent to the one of two identical massless scalars from which the mode of $l=0$ has been removed. This shows the relation $c^M_{\\log}=2 (c^S_{\\log}-c^{S_{l=0}}_{\\log})$ between the logarithmic coefficient in the entropy for a Maxwell field $c^M_{\\log}$, the one for a $d=4$ massless scalar $c_{\\log}^S$, and the logarithmic coefficient $c^{S_{l=0}}_{\\log}$ for a $d=2$ scalar with Dirichlet boundary condition at the origin. Using the accepted values for these coefficients $c_{\\log}^S=-1/90$ and $c^{S_{l=0}}_{\\log}=1/6$ we get $c^M_{\\log}=-16/45$, which coincides with Dowker's calculation, but does not match the coefficient $-\\frac{31}{45}$ in the trace anomaly for a Maxwell field. We have numerically evaluated these three numbers $c^M_{\\log}$, $c^S_{\\log}$ and $c^{S_{l=0}}_{\\log}$, verifying the relation, as well as checked they coincide with the corresponding logarithmic term in mutual information of two concentric spheres.", "revisions": [ { "version": "v1", "updated": "2015-12-19T03:10:08.000Z" } ], "analyses": { "keywords": [ "maxwell field", "entanglement entropy", "logarithmic coefficient", "dirichlet boundary condition", "massless scalar" ], "publication": { "doi": "10.1103/PhysRevD.93.105031" }, "note": { "typesetting": "TeX", "pages": 18, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2015arXiv151206182C", "inspire": 1410908 } } }