Matches in SemOpenAlex for { <https://semopenalex.org/work/W1966108495> ?p ?o ?g. }
- W1966108495 abstract "The disorder-driven phase transition of the RFIM is observed using exact ground-state computer simulations for hyper cubic lattices in d=5,6,7 dimensions. Finite-size scaling analyses are used to calculate the critical point and the critical exponents of the specific heat, magnetization, susceptibility and of the correlation length. For dimensions d=6,7 which are larger or equal to the assumed upper critical dimension, d_u=6, mean-field behaviour is found, i.e. alpha=0, beta=1/2, gamma=1, nu=1/2. For the analysis of the numerical data, it appears to be necessary to include recently proposed corrections to scaling at and beyond the upper critical dimension." @default.
- W1966108495 created "2016-06-24" @default.
- W1966108495 creator A5005760050 @default.
- W1966108495 creator A5009888211 @default.
- W1966108495 date "2011-01-31" @default.
- W1966108495 modified "2023-10-01" @default.
- W1966108495 title "Critical behavior of the random-field Ising model at and beyond the upper critical dimension" @default.
- W1966108495 cites W124595874 @default.
- W1966108495 cites W1966640192 @default.
- W1966108495 cites W1973262677 @default.
- W1966108495 cites W1977391274 @default.
- W1966108495 cites W1987840821 @default.
- W1966108495 cites W1996568365 @default.
- W1966108495 cites W2004318687 @default.
- W1966108495 cites W2008658663 @default.
- W1966108495 cites W2027386874 @default.
- W1966108495 cites W2028576516 @default.
- W1966108495 cites W2032271728 @default.
- W1966108495 cites W2038945486 @default.
- W1966108495 cites W2057460263 @default.
- W1966108495 cites W2058769212 @default.
- W1966108495 cites W2059700943 @default.
- W1966108495 cites W2065755562 @default.
- W1966108495 cites W2067292582 @default.
- W1966108495 cites W2078520118 @default.
- W1966108495 cites W2081842692 @default.
- W1966108495 cites W2082979244 @default.
- W1966108495 cites W2085984146 @default.
- W1966108495 cites W2090359754 @default.
- W1966108495 cites W2143573616 @default.
- W1966108495 cites W2497720895 @default.
- W1966108495 cites W3100973346 @default.
- W1966108495 cites W3103008581 @default.
- W1966108495 cites W3105353949 @default.
- W1966108495 cites W3191407898 @default.
- W1966108495 cites W32103840 @default.
- W1966108495 doi "https://doi.org/10.1103/physrevb.83.014205" @default.
- W1966108495 hasPublicationYear "2011" @default.
- W1966108495 type Work @default.
- W1966108495 sameAs 1966108495 @default.
- W1966108495 citedByCount "29" @default.
- W1966108495 countsByYear W19661084952012 @default.
- W1966108495 countsByYear W19661084952013 @default.
- W1966108495 countsByYear W19661084952014 @default.
- W1966108495 countsByYear W19661084952015 @default.
- W1966108495 countsByYear W19661084952016 @default.
- W1966108495 countsByYear W19661084952017 @default.
- W1966108495 countsByYear W19661084952018 @default.
- W1966108495 countsByYear W19661084952019 @default.
- W1966108495 countsByYear W19661084952023 @default.
- W1966108495 crossrefType "journal-article" @default.
- W1966108495 hasAuthorship W1966108495A5005760050 @default.
- W1966108495 hasAuthorship W1966108495A5009888211 @default.
- W1966108495 hasBestOaLocation W19661084952 @default.
- W1966108495 hasConcept C114614502 @default.
- W1966108495 hasConcept C115260700 @default.
- W1966108495 hasConcept C121332964 @default.
- W1966108495 hasConcept C121864883 @default.
- W1966108495 hasConcept C134306372 @default.
- W1966108495 hasConcept C149288129 @default.
- W1966108495 hasConcept C164154869 @default.
- W1966108495 hasConcept C177407944 @default.
- W1966108495 hasConcept C194807282 @default.
- W1966108495 hasConcept C196298200 @default.
- W1966108495 hasConcept C207789793 @default.
- W1966108495 hasConcept C2524010 @default.
- W1966108495 hasConcept C26873012 @default.
- W1966108495 hasConcept C32546565 @default.
- W1966108495 hasConcept C33676613 @default.
- W1966108495 hasConcept C33923547 @default.
- W1966108495 hasConcept C51329190 @default.
- W1966108495 hasConcept C62520636 @default.
- W1966108495 hasConcept C99844830 @default.
- W1966108495 hasConceptScore W1966108495C114614502 @default.
- W1966108495 hasConceptScore W1966108495C115260700 @default.
- W1966108495 hasConceptScore W1966108495C121332964 @default.
- W1966108495 hasConceptScore W1966108495C121864883 @default.
- W1966108495 hasConceptScore W1966108495C134306372 @default.
- W1966108495 hasConceptScore W1966108495C149288129 @default.
- W1966108495 hasConceptScore W1966108495C164154869 @default.
- W1966108495 hasConceptScore W1966108495C177407944 @default.
- W1966108495 hasConceptScore W1966108495C194807282 @default.
- W1966108495 hasConceptScore W1966108495C196298200 @default.
- W1966108495 hasConceptScore W1966108495C207789793 @default.
- W1966108495 hasConceptScore W1966108495C2524010 @default.
- W1966108495 hasConceptScore W1966108495C26873012 @default.
- W1966108495 hasConceptScore W1966108495C32546565 @default.
- W1966108495 hasConceptScore W1966108495C33676613 @default.
- W1966108495 hasConceptScore W1966108495C33923547 @default.
- W1966108495 hasConceptScore W1966108495C51329190 @default.
- W1966108495 hasConceptScore W1966108495C62520636 @default.
- W1966108495 hasConceptScore W1966108495C99844830 @default.
- W1966108495 hasIssue "1" @default.
- W1966108495 hasLocation W19661084951 @default.
- W1966108495 hasLocation W19661084952 @default.
- W1966108495 hasOpenAccess W1966108495 @default.
- W1966108495 hasPrimaryLocation W19661084951 @default.
- W1966108495 hasRelatedWork W1584656853 @default.
- W1966108495 hasRelatedWork W16992684 @default.
- W1966108495 hasRelatedWork W2027999159 @default.