Please use this identifier to cite or link to this item: http://hdl.handle.net/2289/5130
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dc.contributor.authorHeinrichs, J.-
dc.contributor.authorKumar, N.-
dc.date.accessioned2012-08-03T04:56:00Z-
dc.date.available2012-08-03T04:56:00Z-
dc.date.issued1984-02-
dc.identifier.citationJournal of Physics C: Solid State Physics, 1984, Vol. 17, p769-774en
dc.identifier.issn0022-3719-
dc.identifier.urihttp://hdl.handle.net/2289/5130-
dc.descriptionRestricted Accessen
dc.description.abstractThe probability distribution for the displacement x of a particle moving in a one-dimensional continuum is derived exactly for the general case of combined static and dynamic gaussian randomness of the applied force. The dynamics of the particle is governed by the high-friction limit of Brownian motion discussed originally by Einstein and Smoluchowski. In particular, the mean square displacement of the particle varies as t2 for t to infinity . This ballistic motion induced by the disorder does not give rise to a 1/f power spectrum, contrary to recent suggestions based on the above dynamical model.en
dc.language.isoenen
dc.publisherInsitutute of Physicsen
dc.relation.urihttp://dx.doi.org/10.1088/0022-3719/17/5/008en
dc.relation.urihttp://adsabs.harvard.edu/abs/1984JPhC...17..769Hen
dc.rights1984 Institute of Physicsen
dc.subjectclassical transporten
dc.subjectprobability theoryen
dc.subjectbrownian motionen
dc.subjectcomputational physicsen
dc.subjectstatistical physicsen
dc.subjectnonlinear systemsen
dc.titleNon-diffusive classical transport in a medium with static randomnessen
dc.typeArticleen
Appears in Collections:Research Papers (TP)

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