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dc.contributor.authorStariolo, Daniel Adrianpt_BR
dc.contributor.authorFabricius, Gabrielpt_BR
dc.date.accessioned2020-01-28T04:12:10Zpt_BR
dc.date.issued2006pt_BR
dc.identifier.issn0021-9606pt_BR
dc.identifier.urihttp://hdl.handle.net/10183/205008pt_BR
dc.description.abstractParticle motion of a Lennard-Jones supercooled liquid near the glass transition is studied by molecular dynamics simulations. We analyze the wave vector dependence of relaxation times in the incoherent self-scattering function and show that at least three different regimes can be identified and its scaling properties determined. The transition from one regime to another happens at characteristic length scales. The length scale associated with the onset of Fickian diffusion corresponds to the maximum size of heterogeneities in the system, and the characteristic time scale is several times larger than the alpha relaxation time. A second crossover length scale is observed, which corresponds to the typical time and length of heterogeneities, in agreement with results from four point functions. The different regimes can be traced back to the behavior of the van Hove distribution of displacements, which shows a characteristic exponential regime in the heterogeneous region before the crossover to Gaussian diffusion and should be observable in experiments. Our results show that it is possible to obtain characteristic length scales of heterogeneities through the computation of two point functions at different times.en
dc.format.mimetypeapplication/pdfpt_BR
dc.language.isoengpt_BR
dc.relation.ispartofThe journal of chemical physics. New York. Vol. 125, no. 6 (Aug. 2006), 064505, 7p.pt_BR
dc.rightsOpen Accessen
dc.subjectTransicao vitreapt_BR
dc.subjectDinâmica molecularpt_BR
dc.titleFickian crossover and length scales from two point functions in supercooled liquidspt_BR
dc.typeArtigo de periódicopt_BR
dc.identifier.nrb000556798pt_BR
dc.type.originEstrangeiropt_BR


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