Matches in SemOpenAlex for { <https://semopenalex.org/work/W2012398413> ?p ?o ?g. }
- W2012398413 endingPage "11765" @default.
- W2012398413 startingPage "11755" @default.
- W2012398413 abstract "The relaxational dynamics of the d-dimensional, classical anisotropic Heisenberg (Ising-Heisenberg) model near the percolation bicritical point (p=${p}_{c}$, T=0) is considered. As in the corresponding Ising system, the relevant physical process involves the activation of domain walls over a hierarchy of energy barriers. In this system the domain boundaries are quasi-one-dimensional Bloch walls and we show that a simple scaling theory gives exact results for the Bloch-wall energy and length across the whole range of anisotropy. These results are used to derive explicit expressions for the characteristic time ${ensuremath{tau}}_{c}$ in the various scaling regimes of interest. In particular, it is found that the conventional dynamic scaling hypothesis for ${ensuremath{tau}}_{c}$ is violated at sufficiently low temperatures in all cases of nonvanishing anisotropy, and the crossover to singular dynamic scaling behavior is demonstrated explicitly." @default.
- W2012398413 created "2016-06-24" @default.
- W2012398413 creator A5043846314 @default.
- W2012398413 creator A5077850411 @default.
- W2012398413 date "1988-12-01" @default.
- W2012398413 modified "2023-09-24" @default.
- W2012398413 title "Bloch walls and anomalous longitudinal Glauber dynamics of dilute anisotropic magnets at the percolation threshold" @default.
- W2012398413 cites W1964526053 @default.
- W2012398413 cites W1968776099 @default.
- W2012398413 cites W1970146924 @default.
- W2012398413 cites W1972204862 @default.
- W2012398413 cites W1974906217 @default.
- W2012398413 cites W1977323460 @default.
- W2012398413 cites W1977597626 @default.
- W2012398413 cites W1982872965 @default.
- W2012398413 cites W1983272724 @default.
- W2012398413 cites W1987424527 @default.
- W2012398413 cites W1988335285 @default.
- W2012398413 cites W1998752817 @default.
- W2012398413 cites W2000593257 @default.
- W2012398413 cites W2003178155 @default.
- W2012398413 cites W2005702383 @default.
- W2012398413 cites W2006025940 @default.
- W2012398413 cites W2006219183 @default.
- W2012398413 cites W2009455826 @default.
- W2012398413 cites W2010372371 @default.
- W2012398413 cites W2023579765 @default.
- W2012398413 cites W2059584681 @default.
- W2012398413 cites W2061989541 @default.
- W2012398413 cites W2066359652 @default.
- W2012398413 cites W2067520303 @default.
- W2012398413 cites W2068155490 @default.
- W2012398413 cites W2076045134 @default.
- W2012398413 cites W2079218525 @default.
- W2012398413 cites W2111201101 @default.
- W2012398413 cites W2138085462 @default.
- W2012398413 cites W4255039614 @default.
- W2012398413 doi "https://doi.org/10.1103/physrevb.38.11755" @default.
- W2012398413 hasPubMedId "https://pubmed.ncbi.nlm.nih.gov/9946062" @default.
- W2012398413 hasPublicationYear "1988" @default.
- W2012398413 type Work @default.
- W2012398413 sameAs 2012398413 @default.
- W2012398413 citedByCount "0" @default.
- W2012398413 crossrefType "journal-article" @default.
- W2012398413 hasAuthorship W2012398413A5043846314 @default.
- W2012398413 hasAuthorship W2012398413A5077850411 @default.
- W2012398413 hasConcept C115260700 @default.
- W2012398413 hasConcept C121332964 @default.
- W2012398413 hasConcept C121864883 @default.
- W2012398413 hasConcept C122507166 @default.
- W2012398413 hasConcept C134306372 @default.
- W2012398413 hasConcept C154945302 @default.
- W2012398413 hasConcept C169760540 @default.
- W2012398413 hasConcept C181686392 @default.
- W2012398413 hasConcept C191486275 @default.
- W2012398413 hasConcept C201665358 @default.
- W2012398413 hasConcept C2524010 @default.
- W2012398413 hasConcept C26873012 @default.
- W2012398413 hasConcept C2729557 @default.
- W2012398413 hasConcept C2780457167 @default.
- W2012398413 hasConcept C2780708879 @default.
- W2012398413 hasConcept C32546565 @default.
- W2012398413 hasConcept C33923547 @default.
- W2012398413 hasConcept C36503486 @default.
- W2012398413 hasConcept C41008148 @default.
- W2012398413 hasConcept C51329190 @default.
- W2012398413 hasConcept C62520636 @default.
- W2012398413 hasConcept C69990965 @default.
- W2012398413 hasConcept C82217956 @default.
- W2012398413 hasConcept C85725439 @default.
- W2012398413 hasConcept C86803240 @default.
- W2012398413 hasConcept C99844830 @default.
- W2012398413 hasConceptScore W2012398413C115260700 @default.
- W2012398413 hasConceptScore W2012398413C121332964 @default.
- W2012398413 hasConceptScore W2012398413C121864883 @default.
- W2012398413 hasConceptScore W2012398413C122507166 @default.
- W2012398413 hasConceptScore W2012398413C134306372 @default.
- W2012398413 hasConceptScore W2012398413C154945302 @default.
- W2012398413 hasConceptScore W2012398413C169760540 @default.
- W2012398413 hasConceptScore W2012398413C181686392 @default.
- W2012398413 hasConceptScore W2012398413C191486275 @default.
- W2012398413 hasConceptScore W2012398413C201665358 @default.
- W2012398413 hasConceptScore W2012398413C2524010 @default.
- W2012398413 hasConceptScore W2012398413C26873012 @default.
- W2012398413 hasConceptScore W2012398413C2729557 @default.
- W2012398413 hasConceptScore W2012398413C2780457167 @default.
- W2012398413 hasConceptScore W2012398413C2780708879 @default.
- W2012398413 hasConceptScore W2012398413C32546565 @default.
- W2012398413 hasConceptScore W2012398413C33923547 @default.
- W2012398413 hasConceptScore W2012398413C36503486 @default.
- W2012398413 hasConceptScore W2012398413C41008148 @default.
- W2012398413 hasConceptScore W2012398413C51329190 @default.
- W2012398413 hasConceptScore W2012398413C62520636 @default.
- W2012398413 hasConceptScore W2012398413C69990965 @default.
- W2012398413 hasConceptScore W2012398413C82217956 @default.
- W2012398413 hasConceptScore W2012398413C85725439 @default.
- W2012398413 hasConceptScore W2012398413C86803240 @default.
- W2012398413 hasConceptScore W2012398413C99844830 @default.