Matches in SemOpenAlex for { <https://semopenalex.org/work/W2082924322> ?p ?o ?g. }
- W2082924322 endingPage "532" @default.
- W2082924322 startingPage "522" @default.
- W2082924322 abstract "Exact solutions are rare for non-Markovian random walk models even in 1D, and much more so in 2D. Here we propose a 2D genuinely non-Markovian random walk model with a very rich phase diagram, such that the motion in each dimension can belong to one of 3 categories: (i) subdiffusive, (ii) superdiffusive, or (iii) normally diffusive. The main advance reported here is a different method, and the consequent physical insight, for analytically solving this model. Simpler non-Markovian models, such as Levy walks, have been solved in 2D, but it is not clear if the method of solution could be made to work for more complicated models such as the one studied here. We also report the exact solutions for the first two moments of the random walk propagator, along with the complete phase diagram. The latter is surprisingly rich and admits diverse diffusion regimes. Finally we discuss these results in the context of theoretical underpinnings as well as possible applications." @default.
- W2082924322 created "2016-06-24" @default.
- W2082924322 creator A5014553407 @default.
- W2082924322 creator A5026864148 @default.
- W2082924322 creator A5035730907 @default.
- W2082924322 date "2015-03-01" @default.
- W2082924322 modified "2023-10-16" @default.
- W2082924322 title "A two-dimensional non-Markovian random walk leading to anomalous diffusion" @default.
- W2082924322 cites W1964322893 @default.
- W2082924322 cites W1970119229 @default.
- W2082924322 cites W1970948529 @default.
- W2082924322 cites W1973400757 @default.
- W2082924322 cites W1977360274 @default.
- W2082924322 cites W1987732838 @default.
- W2082924322 cites W1992026911 @default.
- W2082924322 cites W1998904894 @default.
- W2082924322 cites W2000217017 @default.
- W2082924322 cites W2006417751 @default.
- W2082924322 cites W2011239886 @default.
- W2082924322 cites W2021977816 @default.
- W2082924322 cites W2025843255 @default.
- W2082924322 cites W2030765885 @default.
- W2082924322 cites W2040273793 @default.
- W2082924322 cites W2044058219 @default.
- W2082924322 cites W2045514685 @default.
- W2082924322 cites W2047341193 @default.
- W2082924322 cites W2051620101 @default.
- W2082924322 cites W2058946062 @default.
- W2082924322 cites W2062842298 @default.
- W2082924322 cites W2067439107 @default.
- W2082924322 cites W2080649465 @default.
- W2082924322 cites W2091464855 @default.
- W2082924322 cites W2111271983 @default.
- W2082924322 cites W2114121779 @default.
- W2082924322 cites W2129447992 @default.
- W2082924322 cites W2143423258 @default.
- W2082924322 cites W2145287259 @default.
- W2082924322 cites W2159720520 @default.
- W2082924322 cites W2160570224 @default.
- W2082924322 cites W2170633964 @default.
- W2082924322 cites W2171420116 @default.
- W2082924322 cites W3100759076 @default.
- W2082924322 cites W3105835323 @default.
- W2082924322 doi "https://doi.org/10.1016/j.physa.2014.11.047" @default.
- W2082924322 hasPublicationYear "2015" @default.
- W2082924322 type Work @default.
- W2082924322 sameAs 2082924322 @default.
- W2082924322 citedByCount "6" @default.
- W2082924322 countsByYear W20829243222016 @default.
- W2082924322 countsByYear W20829243222018 @default.
- W2082924322 countsByYear W20829243222019 @default.
- W2082924322 countsByYear W20829243222022 @default.
- W2082924322 crossrefType "journal-article" @default.
- W2082924322 hasAuthorship W2082924322A5014553407 @default.
- W2082924322 hasAuthorship W2082924322A5026864148 @default.
- W2082924322 hasAuthorship W2082924322A5035730907 @default.
- W2082924322 hasConcept C104416048 @default.
- W2082924322 hasConcept C105795698 @default.
- W2082924322 hasConcept C114614502 @default.
- W2082924322 hasConcept C121194460 @default.
- W2082924322 hasConcept C121332964 @default.
- W2082924322 hasConcept C121864883 @default.
- W2082924322 hasConcept C151730666 @default.
- W2082924322 hasConcept C154072304 @default.
- W2082924322 hasConcept C155155215 @default.
- W2082924322 hasConcept C159886148 @default.
- W2082924322 hasConcept C164602753 @default.
- W2082924322 hasConcept C2779343474 @default.
- W2082924322 hasConcept C3017618536 @default.
- W2082924322 hasConcept C33676613 @default.
- W2082924322 hasConcept C33923547 @default.
- W2082924322 hasConcept C37914503 @default.
- W2082924322 hasConcept C41008148 @default.
- W2082924322 hasConcept C44280652 @default.
- W2082924322 hasConcept C56739046 @default.
- W2082924322 hasConcept C62520636 @default.
- W2082924322 hasConcept C69357855 @default.
- W2082924322 hasConcept C85906118 @default.
- W2082924322 hasConcept C86803240 @default.
- W2082924322 hasConceptScore W2082924322C104416048 @default.
- W2082924322 hasConceptScore W2082924322C105795698 @default.
- W2082924322 hasConceptScore W2082924322C114614502 @default.
- W2082924322 hasConceptScore W2082924322C121194460 @default.
- W2082924322 hasConceptScore W2082924322C121332964 @default.
- W2082924322 hasConceptScore W2082924322C121864883 @default.
- W2082924322 hasConceptScore W2082924322C151730666 @default.
- W2082924322 hasConceptScore W2082924322C154072304 @default.
- W2082924322 hasConceptScore W2082924322C155155215 @default.
- W2082924322 hasConceptScore W2082924322C159886148 @default.
- W2082924322 hasConceptScore W2082924322C164602753 @default.
- W2082924322 hasConceptScore W2082924322C2779343474 @default.
- W2082924322 hasConceptScore W2082924322C3017618536 @default.
- W2082924322 hasConceptScore W2082924322C33676613 @default.
- W2082924322 hasConceptScore W2082924322C33923547 @default.
- W2082924322 hasConceptScore W2082924322C37914503 @default.
- W2082924322 hasConceptScore W2082924322C41008148 @default.
- W2082924322 hasConceptScore W2082924322C44280652 @default.
- W2082924322 hasConceptScore W2082924322C56739046 @default.