FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2076264294> ?p ?o ?g. }

• W2076264294 endingPage "139" @default.
• W2076264294 startingPage "120" @default.
• W2076264294 abstract "In order to gain a better understanding of the Ising model in higher dimensions we have made a comparative study of how the boundary, open versus cyclic, of a d-dimensional simple lattice, for d=1,...,5, affects the behaviour of the specific heat C and its microcanonical relative, the entropy derivative -dS/dU. In dimensions 4 and 5 the boundary has a strong effect on the critical region of the model and for cyclic boundaries in dimension 5 we find that the model displays a quasi first order phase transition with a bimodal energy distribution. The latent heat decreases with increasing systems size but for all system sizes used in earlier papers the effect is clearly visible once a wide enough range of values for K is considered. Relations to recent rigorous results for high dimensional percolation and previous debates on simulation of Ising models and gauge fields are discussed." @default.
• W2076264294 created "2016-06-24" @default.
• W2076264294 creator A5024726931 @default.
• W2076264294 creator A5035765654 @default.
• W2076264294 date "2011-04-01" @default.
• W2076264294 modified "2023-10-18" @default.
• W2076264294 title "Non-vanishing boundary effects and quasi-first-order phase transitions in high dimensional Ising models" @default.
• W2076264294 cites W1590167836 @default.
• W2076264294 cites W1969758109 @default.
• W2076264294 cites W1971986650 @default.
• W2076264294 cites W1992240203 @default.
• W2076264294 cites W1995436153 @default.
• W2076264294 cites W1997601212 @default.
• W2076264294 cites W2008637411 @default.
• W2076264294 cites W2016285684 @default.
• W2076264294 cites W2040094758 @default.
• W2076264294 cites W2042068487 @default.
• W2076264294 cites W2052978120 @default.
• W2076264294 cites W2072453195 @default.
• W2076264294 cites W2072868068 @default.
• W2076264294 cites W2074121902 @default.
• W2076264294 cites W2074670256 @default.
• W2076264294 cites W2083442073 @default.
• W2076264294 cites W2089498317 @default.
• W2076264294 cites W2127210480 @default.
• W2076264294 cites W2163932869 @default.
• W2076264294 cites W2285867887 @default.
• W2076264294 cites W2596824449 @default.
• W2076264294 cites W2746834873 @default.
• W2076264294 cites W3100525495 @default.
• W2076264294 cites W3101328473 @default.
• W2076264294 cites W3102096359 @default.
• W2076264294 cites W3103525440 @default.
• W2076264294 cites W3104492478 @default.
• W2076264294 cites W3121297229 @default.
• W2076264294 doi "https://doi.org/10.1016/j.nuclphysb.2010.12.002" @default.
• W2076264294 hasPublicationYear "2011" @default.
• W2076264294 type Work @default.
• W2076264294 sameAs 2076264294 @default.
• W2076264294 citedByCount "28" @default.
• W2076264294 countsByYear W20762642942012 @default.
• W2076264294 countsByYear W20762642942013 @default.
• W2076264294 countsByYear W20762642942014 @default.
• W2076264294 countsByYear W20762642942015 @default.
• W2076264294 countsByYear W20762642942016 @default.
• W2076264294 countsByYear W20762642942017 @default.
• W2076264294 countsByYear W20762642942018 @default.
• W2076264294 countsByYear W20762642942019 @default.
• W2076264294 countsByYear W20762642942020 @default.
• W2076264294 countsByYear W20762642942021 @default.
• W2076264294 countsByYear W20762642942022 @default.
• W2076264294 countsByYear W20762642942023 @default.
• W2076264294 crossrefType "journal-article" @default.
• W2076264294 hasAuthorship W2076264294A5024726931 @default.
• W2076264294 hasAuthorship W2076264294A5035765654 @default.
• W2076264294 hasBestOaLocation W20762642942 @default.
• W2076264294 hasConcept C106301342 @default.
• W2076264294 hasConcept C121332964 @default.
• W2076264294 hasConcept C121864883 @default.
• W2076264294 hasConcept C149288129 @default.
• W2076264294 hasConcept C169760540 @default.
• W2076264294 hasConcept C182310444 @default.
• W2076264294 hasConcept C188324986 @default.
• W2076264294 hasConcept C24890656 @default.
• W2076264294 hasConcept C26873012 @default.
• W2076264294 hasConcept C2780457167 @default.
• W2076264294 hasConcept C2781204021 @default.
• W2076264294 hasConcept C44280652 @default.
• W2076264294 hasConcept C51329190 @default.
• W2076264294 hasConcept C62520636 @default.
• W2076264294 hasConcept C65494353 @default.
• W2076264294 hasConcept C86803240 @default.
• W2076264294 hasConcept C97355855 @default.
• W2076264294 hasConceptScore W2076264294C106301342 @default.
• W2076264294 hasConceptScore W2076264294C121332964 @default.
• W2076264294 hasConceptScore W2076264294C121864883 @default.
• W2076264294 hasConceptScore W2076264294C149288129 @default.
• W2076264294 hasConceptScore W2076264294C169760540 @default.
• W2076264294 hasConceptScore W2076264294C182310444 @default.
• W2076264294 hasConceptScore W2076264294C188324986 @default.
• W2076264294 hasConceptScore W2076264294C24890656 @default.
• W2076264294 hasConceptScore W2076264294C26873012 @default.
• W2076264294 hasConceptScore W2076264294C2780457167 @default.
• W2076264294 hasConceptScore W2076264294C2781204021 @default.
• W2076264294 hasConceptScore W2076264294C44280652 @default.
• W2076264294 hasConceptScore W2076264294C51329190 @default.
• W2076264294 hasConceptScore W2076264294C62520636 @default.
• W2076264294 hasConceptScore W2076264294C65494353 @default.
• W2076264294 hasConceptScore W2076264294C86803240 @default.
• W2076264294 hasConceptScore W2076264294C97355855 @default.
• W2076264294 hasIssue "1" @default.
• W2076264294 hasLocation W20762642941 @default.
• W2076264294 hasLocation W20762642942 @default.
• W2076264294 hasOpenAccess W2076264294 @default.
• W2076264294 hasPrimaryLocation W20762642941 @default.
• W2076264294 hasRelatedWork W16992684 @default.
• W2076264294 hasRelatedWork W1714818406 @default.
• W2076264294 hasRelatedWork W2032967918 @default.

• next