FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2044693670> ?p ?o ?g. }

• W2044693670 abstract "When the symmetries of homogenous isotropic turbulent flows are broken, different sets of modes with different physical roles emerge. In particular, choosing a forcing which puts more weight on one or the other of these sets may result in different statistics for the energy transfers. We use the general method of computing a partition function restricted to a portion of phase space to study analytically these different statistics. We illustrate this method in the case of parity symmetry breaking, measured by helicity. It is shown that when helicity is sign definite at all scales, an inverse cascade is expected for the energy. When sign-definiteness is lost, even for a small set of modes, this cascade disappears and there is a sharp phase transition to the standard helical equipartition spectra." @default.
• W2044693670 created "2016-06-24" @default.
• W2044693670 creator A5025888920 @default.
• W2044693670 date "2014-01-15" @default.
• W2044693670 modified "2023-10-14" @default.
• W2044693670 title "Restricted partition functions and inverse energy cascades in parity symmetry breaking flows" @default.
• W2044693670 cites W1967758385 @default.
• W2044693670 cites W1978995203 @default.
• W2044693670 cites W1985352787 @default.
• W2044693670 cites W1985626529 @default.
• W2044693670 cites W1998844365 @default.
• W2044693670 cites W2002952727 @default.
• W2044693670 cites W2003028297 @default.
• W2044693670 cites W2009461740 @default.
• W2044693670 cites W2012393256 @default.
• W2044693670 cites W2012672107 @default.
• W2044693670 cites W2013004558 @default.
• W2044693670 cites W2016447323 @default.
• W2044693670 cites W2025844876 @default.
• W2044693670 cites W2045444659 @default.
• W2044693670 cites W2046093611 @default.
• W2044693670 cites W2049234180 @default.
• W2044693670 cites W2050154297 @default.
• W2044693670 cites W2050962398 @default.
• W2044693670 cites W2061087839 @default.
• W2044693670 cites W2064882198 @default.
• W2044693670 cites W2066609626 @default.
• W2044693670 cites W2073524977 @default.
• W2044693670 cites W2077674352 @default.
• W2044693670 cites W2086667100 @default.
• W2044693670 cites W2102258350 @default.
• W2044693670 cites W2107809760 @default.
• W2044693670 cites W2124575407 @default.
• W2044693670 cites W2137497682 @default.
• W2044693670 cites W2138427209 @default.
• W2044693670 cites W2565064665 @default.
• W2044693670 cites W3099035077 @default.
• W2044693670 cites W3100685719 @default.
• W2044693670 cites W3102475271 @default.
• W2044693670 cites W4229698746 @default.
• W2044693670 cites W4237691679 @default.
• W2044693670 cites W4244283885 @default.
• W2044693670 cites W4251401595 @default.
• W2044693670 cites W4361807458 @default.
• W2044693670 doi "https://doi.org/10.1103/physreve.89.013010" @default.
• W2044693670 hasPubMedId "https://pubmed.ncbi.nlm.nih.gov/24580323" @default.
• W2044693670 hasPublicationYear "2014" @default.
• W2044693670 type Work @default.
• W2044693670 sameAs 2044693670 @default.
• W2044693670 citedByCount "9" @default.
• W2044693670 countsByYear W20446936702014 @default.
• W2044693670 countsByYear W20446936702015 @default.
• W2044693670 countsByYear W20446936702018 @default.
• W2044693670 crossrefType "journal-article" @default.
• W2044693670 hasAuthorship W2044693670A5025888920 @default.
• W2044693670 hasBestOaLocation W20446936702 @default.
• W2044693670 hasConcept C115260700 @default.
• W2044693670 hasConcept C121332964 @default.
• W2044693670 hasConcept C121864883 @default.
• W2044693670 hasConcept C184050105 @default.
• W2044693670 hasConcept C185592680 @default.
• W2044693670 hasConcept C204795200 @default.
• W2044693670 hasConcept C207467116 @default.
• W2044693670 hasConcept C2524010 @default.
• W2044693670 hasConcept C2775859700 @default.
• W2044693670 hasConcept C2777151079 @default.
• W2044693670 hasConcept C2778401447 @default.
• W2044693670 hasConcept C33923547 @default.
• W2044693670 hasConcept C34146451 @default.
• W2044693670 hasConcept C43617362 @default.
• W2044693670 hasConcept C62520636 @default.
• W2044693670 hasConcept C96469262 @default.
• W2044693670 hasConcept C99742106 @default.
• W2044693670 hasConceptScore W2044693670C115260700 @default.
• W2044693670 hasConceptScore W2044693670C121332964 @default.
• W2044693670 hasConceptScore W2044693670C121864883 @default.
• W2044693670 hasConceptScore W2044693670C184050105 @default.
• W2044693670 hasConceptScore W2044693670C185592680 @default.
• W2044693670 hasConceptScore W2044693670C204795200 @default.
• W2044693670 hasConceptScore W2044693670C207467116 @default.
• W2044693670 hasConceptScore W2044693670C2524010 @default.
• W2044693670 hasConceptScore W2044693670C2775859700 @default.
• W2044693670 hasConceptScore W2044693670C2777151079 @default.
• W2044693670 hasConceptScore W2044693670C2778401447 @default.
• W2044693670 hasConceptScore W2044693670C33923547 @default.
• W2044693670 hasConceptScore W2044693670C34146451 @default.
• W2044693670 hasConceptScore W2044693670C43617362 @default.
• W2044693670 hasConceptScore W2044693670C62520636 @default.
• W2044693670 hasConceptScore W2044693670C96469262 @default.
• W2044693670 hasConceptScore W2044693670C99742106 @default.
• W2044693670 hasIssue "1" @default.
• W2044693670 hasLocation W20446936701 @default.
• W2044693670 hasLocation W20446936702 @default.
• W2044693670 hasLocation W20446936703 @default.
• W2044693670 hasOpenAccess W2044693670 @default.
• W2044693670 hasPrimaryLocation W20446936701 @default.
• W2044693670 hasRelatedWork W1626003387 @default.
• W2044693670 hasRelatedWork W1988726653 @default.
• W2044693670 hasRelatedWork W2003043223 @default.
• W2044693670 hasRelatedWork W2023968175 @default.

• next