{ "id": "quant-ph/0503134", "version": "v4", "published": "2005-03-15T15:38:40.000Z", "updated": "2006-02-23T21:42:43.000Z", "title": "Comment on \"On the temperature dependence of the Casimir effect\"", "authors": [ "V. B. Bezerra", "R. S. Decca", "E. Fischbach", "B. Geyer", "G. L. Klimchitskaya", "D. E. Krause", "D. López", "V. M. Mostepanenko", "C. Romero" ], "comment": "11 pages, 3 figures, changed in accordance with the final published version", "journal": "Phys.Rev. E73 (2006) 028101", "doi": "10.1103/PhysRevE.73.028101", "categories": [ "quant-ph", "cond-mat.stat-mech", "hep-th" ], "abstract": "Recently, Brevik et al. [Phys. Rev. E 71, 056101 (2005)] adduced arguments against the traditional approach to the thermal Casimir force between real metals and in favor of one of the alternative approaches. The latter assumes zero contribution from the transverse electric mode at zero frequency in qualitative disagreement with unity as given by the thermal quantum field theory for ideal metals. Those authors claim that their approach is consistent with experiments as well as with thermodynamics. We demonstrate that these conclusions are incorrect. We show specifically that their results are contradicted by four recent experiments and also violate the third law of thermodynamics (the Nernst heat theorem).", "revisions": [ { "version": "v4", "updated": "2006-02-23T21:42:43.000Z" } ], "analyses": { "subjects": [ "73.61.At", "77.22.Ch", "11.10.Wx", "05.30.-d" ], "keywords": [ "temperature dependence", "casimir effect", "thermal quantum field theory", "transverse electric mode", "assumes zero contribution" ], "tags": [ "journal article" ], "publication": { "publisher": "APS", "journal": "Phys. Rev. E" }, "note": { "typesetting": "TeX", "pages": 11, "language": "en", "license": "arXiv", "status": "editable", "inspire": 678646 } } }