{ "id": "cond-mat/0408316", "version": "v1", "published": "2004-08-13T09:49:42.000Z", "updated": "2004-08-13T09:49:42.000Z", "title": "The quantum measurement process in an exactly solvable model", "authors": [ "Armen E. Allahverdyan", "Roger Balian", "Theo M. Nieuwenhuizen" ], "comment": "7 pages revtex, 2 figures", "doi": "10.1063/1.1874554", "categories": [ "cond-mat.stat-mech", "cond-mat.other", "quant-ph" ], "abstract": "An exactly solvable model for a quantum measurement is discussed which is governed by hamiltonian quantum dynamics. The $z$-component $\\hat s_z$ of a spin-1/2 is measured with an apparatus, which itself consists of magnet coupled to a bath. The initial state of the magnet is a metastable paramagnet, while the bath starts in a thermal, gibbsian state. Conditions are such that the act of measurement drives the magnet in the up or down ferromagnetic state according to the sign of $s_z$ of the tested spin. The quantum measurement goes in two steps. On a timescale $1/\\sqrt{N}$ the off-diagonal elements of the spin's density matrix vanish due to a unitary evolution of the tested spin and the $N$ apparatus spins; on a larger but still short timescale this is made definite by the bath. Then the system is in a `classical' state, having a diagonal density matrix. The registration of that state is a quantum process which can already be understood from classical statistical mechanics. The von Neumann collapse and the Born rule are derived rather than postulated.", "revisions": [ { "version": "v1", "updated": "2004-08-13T09:49:42.000Z" } ], "analyses": { "subjects": [ "03.65.Ta", "02.50.Cw" ], "keywords": [ "exactly solvable model", "quantum measurement process", "spins density matrix", "hamiltonian quantum dynamics", "von neumann collapse" ], "tags": [ "journal article" ], "note": { "typesetting": "RevTeX", "pages": 7, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2005AIPC..750...26A" } } }