000057024 001__ 57024
000057024 005__ 20240610121140.0
000057024 0247_ $$2DOI$$a10.1088/1742-5468/2006/11/P11001
000057024 0247_ $$2WOS$$aWOS:000243165200003
000057024 037__ $$aPreJuSER-57024
000057024 041__ $$aeng
000057024 082__ $$a530
000057024 084__ $$2WoS$$aMechanics
000057024 084__ $$2WoS$$aPhysics, Mathematical
000057024 1001_ $$0P:(DE-HGF)0$$aRakos, A.$$b0
000057024 245__ $$aDynamical scaling for probe particles in a driven fluid
000057024 260__ $$aBristol$$bIOP Publ.$$c2006
000057024 300__ $$aP11001
000057024 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article
000057024 3367_ $$2DataCite$$aOutput Types/Journal article
000057024 3367_ $$00$$2EndNote$$aJournal Article
000057024 3367_ $$2BibTeX$$aARTICLE
000057024 3367_ $$2ORCID$$aJOURNAL_ARTICLE
000057024 3367_ $$2DRIVER$$aarticle
000057024 440_0 $$013281$$aJournal of Statistical Mechanics : Theory and Experiment$$v$$x1742-5468
000057024 500__ $$aRecord converted from VDB: 12.11.2012
000057024 520__ $$aWe investigate two distinct universality classes for probe particles that move stochastically in a one-dimensional driven system. If the random force that drives the probe particles is fully generated by the current fluctuations of the driven fluid, such as when the probe particles are embedded in a ring, they inherit the dynamical exponent of the fluid, which generically is z = 3/2. On the other hand, if the random force has a part that is temporally uncorrelated, the resulting motion can be described by a dynamical exponent z = 2 as considered in previous work.
000057024 536__ $$0G:(DE-Juel1)FUEK414$$2G:(DE-HGF)$$aKondensierte Materie$$cP54$$x0
000057024 588__ $$aDataset connected to Web of Science
000057024 650_7 $$2WoSType$$aJ
000057024 65320 $$2Author$$adriven diffusive systems (theory)
000057024 65320 $$2Author$$astochastic particle dynamics (theory)
000057024 7001_ $$0P:(DE-HGF)0$$aLevine, E.$$b1
000057024 7001_ $$0P:(DE-HGF)0$$aMukamel, D.$$b2
000057024 7001_ $$0P:(DE-Juel1)130966$$aSchütz, G. M.$$b3$$uFZJ
000057024 773__ $$0PERI:(DE-600)2138944-5$$a10.1088/1742-5468/2006/11/P11001$$gp. P11001$$pP11001$$qP11001$$tJournal of statistical mechanics: theory and experiment$$x1742-5468$$y2006
000057024 8567_ $$uhttp://dx.doi.org/10.1088/1742-5468/2006/11/P11001
000057024 909CO $$ooai:juser.fz-juelich.de:57024$$pVDB
000057024 9131_ $$0G:(DE-Juel1)FUEK414$$bMaterie$$kP54$$lKondensierte Materie$$vKondensierte Materie$$x0$$zentfällt   bis 2009
000057024 9141_ $$aNachtrag$$y2006
000057024 915__ $$0StatID:(DE-HGF)0010$$aJCR/ISI refereed
000057024 9201_ $$0I:(DE-Juel1)VDB31$$d31.12.2006$$gIFF$$kIFF-TH-II$$lTheorie II$$x1
000057024 970__ $$aVDB:(DE-Juel1)89723
000057024 980__ $$aVDB
000057024 980__ $$aConvertedRecord
000057024 980__ $$ajournal
000057024 980__ $$aI:(DE-Juel1)ICS-2-20110106
000057024 980__ $$aUNRESTRICTED
000057024 981__ $$aI:(DE-Juel1)IBI-5-20200312
000057024 981__ $$aI:(DE-Juel1)IAS-2-20090406
000057024 981__ $$aI:(DE-Juel1)ICS-2-20110106