Please use this identifier to cite or link to this item: http://bura.brunel.ac.uk/handle/2438/12541
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dc.contributor.authorFyodorov, YV-
dc.contributor.authorSavin, DV-
dc.date.accessioned2016-04-20T14:36:23Z-
dc.date.available2015-05-01-
dc.date.available2016-04-20T14:36:23Z-
dc.date.issued2015-
dc.identifier.citationEPL, 110, (4), (2015)en_US
dc.identifier.issnhttp://iopscience.iop.org/article/10.1209/0295-5075/110/40006/meta;jsessionid=C59A5B40793FA61166DFD6C92CDC1A1F.c1-
dc.identifier.issn0295-5075-
dc.identifier.issn1286-4854-
dc.identifier.urihttp://bura.brunel.ac.uk/handle/2438/12541-
dc.description.abstractWe employ the random matrix theory (RMT) framework to revisit the distribution of resonance widths in quantum chaotic systems weakly coupled to the continuum via a finite number M of open channels. In contrast to the standard first-order perturbation theory treatment we do not a priori assume the resonance widths being small compared to the mean level spacing. We show that to the leading order in weak coupling the perturbative χ<inf>M</inf><sup>2</sup> distribution of the resonance widths (in particular, the Porter-Thomas distribution at M = 1) should be corrected by a factor related to a certain average of the ratio of square roots of the characteristic polynomial ("spectral determinant") of the underlying RMT Hamiltonian. A simple single-channel expression is obtained that properly approximates the width distribution also at large resonance overlap, where the Porter-Thomas result is no longer applicable.en_US
dc.language.isoenen_US
dc.publisherIOP Publishingen_US
dc.titleResonance width distribution in RMT: Weak-coupling regime beyond Porter-Thomasen_US
dc.typeArticleen_US
dc.identifier.doihttp://dx.doi.org/10.1209/0295-5075/110/40006-
dc.relation.isPartOfEPL-
pubs.issue4-
pubs.publication-statusPublished-
pubs.volume110-
Appears in Collections:Dept of Mathematics Research Papers

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