The Attractor and the Quantum States

dc.creatorElze, Hans-Thomas
dc.date2008-06-20
dc.date.accessioned2026-07-07T12:39:06Z
dc.date.available2026-07-07T12:39:06Z
dc.descriptionThe dissipative dynamics anticipated in the proof of 't Hooft's existence theorem -- "For any quantum system there exists at least one deterministic model that reproduces all its dynamics after prequantization" -- is constructed here explicitly. We propose a generalization of Liouville's classical phase space equation, incorporating dissipation and diffusion, and demonstrate that it describes the emergence of quantum states and their dynamics in the Schroedinger picture. Asymptotically, there is a stable ground state and two decoupled sets of degrees of freedom, which transform into each other under the energy-parity symmetry of Kaplan and Sundrum. They recover the familiar Hilbert space and its dual. Expectations of observables are shown to agree with the Born rule, which is not imposed a priori. This attractor mechanism is applicable in the presence of interactions, to few-body or field theories in particular.
dc.description14 pages; based on invited talk at 4th Workshop ad memoriam of Carlo Novero "Advances in Foundations of Quantum Mechanics and Quantum Information with Atoms and Photons", Torino, May 2008; submitted to Int J Qu Info
dc.identifierhttps://arxiv.org/abs/0806.3408
dc.identifierhttp://arxiv.org/abs/0806.3408
dc.identifierInt J Qu Info (IJQI) 7 (2009) 83-96
dc.identifierdoi:10.1142/S0219749909004700
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/218992
dc.subjectQuantum Physics
dc.subjectGeneral Relativity and Quantum Cosmology
dc.titleThe Attractor and the Quantum States
dc.typetext

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