Please use this identifier to cite or link to this item: http://bura.brunel.ac.uk/handle/2438/11082
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dc.contributor.authorBrody, DC-
dc.contributor.authorHook, DW-
dc.contributor.authorHughston, LP-
dc.date.accessioned2015-06-30T11:03:37Z-
dc.date.available2005-06-20-
dc.date.available2015-06-30T11:03:37Z-
dc.date.issued2005-
dc.identifier.citation2005en_US
dc.identifier.urihttp://arxiv.org/abs/quant-ph/0506163v1-
dc.identifier.urihttp://bura.brunel.ac.uk/handle/2438/11082-
dc.description.abstractThe standard assumption for the equilibrium microcanonical state in quantum mechanics, that the system must be in one of the energy eigenstates, is weakened so as to allow superpositions of states. The weakened form of the microcanonical postulate thus asserts that all quantum states giving rise to the same energy expectation value must be realised with equal probability. The consequences that follow from this assertion are investigated. In particular, a closed-form expression for the density of states associated with any system having a nondegenerate energy spectrum is obtained. The result is applied to a variety of examples, for which the behaviour of the state density, as well as the relation between energy and temperature, are determined. Numerical studies indicate that the density of states converges to a distribution when the number of energy levels approaches infinity.en_US
dc.language.isoenen_US
dc.subjectquant-phen_US
dc.titleMicrocanonical distributions for quantum systemsen_US
dc.typeArticleen_US
pubs.notes16 pages, 8 figures-
pubs.notes16 pages, 8 figures-
Appears in Collections:Dept of Mathematics Research Papers

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