Please use this identifier to cite or link to this item: http://hdl.handle.net/2289/2652
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dc.contributor.authorAnantha Ramakrishna, S.-
dc.contributor.authorKumar, N.-
dc.date.accessioned2007-06-11T04:31:25Z-
dc.date.available2007-06-11T04:31:25Z-
dc.date.issued2001-07-
dc.identifier.citationEuropean Physical Journal B, 2001, Vol.23, p515-519en
dc.identifier.issn1434-6028-
dc.identifier.issn1434-6036 (Online)-
dc.identifier.urihttp://hdl.handle.net/2289/2652-
dc.descriptionRestricted Access. An open-access version is available at arXiv.org (one of the alternative locations)en
dc.description.abstractWe re-examine and correct an earlier derivation of the distribution of the Wigner phase delay time for wave reflection from a long one-dimensional disordered conductor treated in the continuum limit. We then numerically compare the distributions of the Wigner phase delay time and the dwell time, the latter being obtained by the use of an infinitesimal imaginary potential as a clock, and investigate the effects of strong disorder and a periodic (discrete) lattice background. We find that the two distributions coincide even for strong disorder, but only for energies well away from the band-edges.en
dc.format.extent178319 bytes-
dc.format.mimetypeapplication/pdf-
dc.language.isoenen
dc.publisherEDP Sciencesen
dc.relation.urihttp://arxiv.org/abs/cond-mat/0106195en
dc.rights2001 EDP Sciencesen
dc.titleDistribution of the delay time and the dwell time for wave reflection from a long random potentialen
dc.typeArticleen
Appears in Collections:Research Papers (TP)

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