{ "id": "quant-ph/0306019", "version": "v1", "published": "2003-06-03T07:49:13.000Z", "updated": "2003-06-03T07:49:13.000Z", "title": "Decoherence without dissipation?", "authors": [ "Dominique Gobert", "Jan von Delft", "Vinay Ambegaokar" ], "comment": "8 pages, 4 figures", "doi": "10.1103/PhysRevA.70.026101", "categories": [ "quant-ph" ], "abstract": "In a recent article, Ford, Lewis and O'Connell (PRA 64, 032101 (2001)) discuss a thought experiment in which a Brownian particle is subjected to a double-slit measurement. Analyzing the decay of the emerging interference pattern, they derive a decoherence rate that is much faster than previous results and even persists in the limit of vanishing dissipation. This result is based on the definition of a certain attenuation factor, which they analyze for short times. In this note, we point out that this attenuation factor captures the physics of decoherence only for times larger than a certain time t_mix, which is the time it takes until the two emerging wave packets begin to overlap. Therefore, the strategy of Ford et al of extracting the decoherence time from the regime t < t_mix is in our opinion not meaningful. If one analyzes the attenuation factor for t > t_mix, one recovers familiar behaviour for the decoherence time; in particular, no decoherence is seen in the absence of dissipation. The latter conclusion is confirmed with a simple calculation of the off-diagonal elements of the reduced density matrix.", "revisions": [ { "version": "v1", "updated": "2003-06-03T07:49:13.000Z" } ], "analyses": { "keywords": [ "dissipation", "decoherence time", "attenuation factor captures", "emerging wave packets begin", "times larger" ], "tags": [ "journal article" ], "publication": { "publisher": "APS", "journal": "Phys. Rev. A" }, "note": { "typesetting": "TeX", "pages": 8, "language": "en", "license": "arXiv", "status": "editable" } } }