FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2011276452> ?p ?o ?g. }

• W2011276452 abstract "We study the effects of twisted boundary conditions on the quark fields in the epsilon regime of chiral perturbation theory. We consider the $SU(2{)}_{L}ifmmodetimeselsetexttimesfi{}SU(2{)}_{R}$ chiral theory with nondegenerate quarks and the $SU(3{)}_{L}ifmmodetimeselsetexttimesfi{}SU(3{)}_{R}$ chiral theory with massless up and down quarks and massive strange quarks. The partition function and condensate are derived for each theory. Because flavor-neutral Goldstone bosons are unaffected by twisted boundary conditions chiral symmetry is still restored in finite volumes. The dependence of the condensate on the twisting parameters can be used to extract the pion decay constant from simulations in the epsilon regime. The relative contribution to the partition function from sectors of different topological charge is numerically insensitive to twisted boundary conditions." @default.
• W2011276452 created "2016-06-24" @default.
• W2011276452 creator A5008398136 @default.
• W2011276452 creator A5030966539 @default.
• W2011276452 date "2005-07-12" @default.
• W2011276452 modified "2023-10-05" @default.
• W2011276452 title "Quarks with twisted boundary conditions in the epsilon regime" @default.
• W2011276452 cites W1963699425 @default.
• W2011276452 cites W1967186877 @default.
• W2011276452 cites W1968760972 @default.
• W2011276452 cites W1973122949 @default.
• W2011276452 cites W1974898324 @default.
• W2011276452 cites W1977774147 @default.
• W2011276452 cites W1990520634 @default.
• W2011276452 cites W1991373977 @default.
• W2011276452 cites W1992554109 @default.
• W2011276452 cites W2005525227 @default.
• W2011276452 cites W2006970299 @default.
• W2011276452 cites W2007714141 @default.
• W2011276452 cites W2009672853 @default.
• W2011276452 cites W2014878137 @default.
• W2011276452 cites W2026657932 @default.
• W2011276452 cites W2028043408 @default.
• W2011276452 cites W2035825545 @default.
• W2011276452 cites W2039319561 @default.
• W2011276452 cites W2042538204 @default.
• W2011276452 cites W2044051520 @default.
• W2011276452 cites W2044704156 @default.
• W2011276452 cites W2052558151 @default.
• W2011276452 cites W2055288739 @default.
• W2011276452 cites W2056526142 @default.
• W2011276452 cites W2057866906 @default.
• W2011276452 cites W2068491716 @default.
• W2011276452 cites W2072738940 @default.
• W2011276452 cites W2084054364 @default.
• W2011276452 cites W2087579479 @default.
• W2011276452 cites W2092389467 @default.
• W2011276452 cites W2092617149 @default.
• W2011276452 cites W2099580529 @default.
• W2011276452 cites W2101032286 @default.
• W2011276452 cites W2113569916 @default.
• W2011276452 cites W2118939464 @default.
• W2011276452 cites W2159850928 @default.
• W2011276452 cites W2172104169 @default.
• W2011276452 cites W2192047738 @default.
• W2011276452 cites W3014594013 @default.
• W2011276452 cites W3097979751 @default.
• W2011276452 cites W3098036057 @default.
• W2011276452 cites W3098742702 @default.
• W2011276452 cites W3101560109 @default.
• W2011276452 cites W3102662747 @default.
• W2011276452 cites W3104639116 @default.
• W2011276452 cites W3105525605 @default.
• W2011276452 cites W3122198885 @default.
• W2011276452 cites W4240883129 @default.
• W2011276452 doi "https://doi.org/10.1103/physrevd.72.014501" @default.
• W2011276452 hasPublicationYear "2005" @default.
• W2011276452 type Work @default.
• W2011276452 sameAs 2011276452 @default.
• W2011276452 citedByCount "17" @default.
• W2011276452 countsByYear W20112764522012 @default.
• W2011276452 countsByYear W20112764522014 @default.
• W2011276452 countsByYear W20112764522016 @default.
• W2011276452 countsByYear W20112764522017 @default.
• W2011276452 crossrefType "journal-article" @default.
• W2011276452 hasAuthorship W2011276452A5008398136 @default.
• W2011276452 hasAuthorship W2011276452A5030966539 @default.
• W2011276452 hasBestOaLocation W20112764522 @default.
• W2011276452 hasConcept C109214941 @default.
• W2011276452 hasConcept C121332964 @default.
• W2011276452 hasConcept C151389596 @default.
• W2011276452 hasConcept C206094082 @default.
• W2011276452 hasConcept C2778401447 @default.
• W2011276452 hasConcept C3079626 @default.
• W2011276452 hasConcept C37914503 @default.
• W2011276452 hasConcept C52703039 @default.
• W2011276452 hasConcept C54937798 @default.
• W2011276452 hasConcept C62520636 @default.
• W2011276452 hasConcept C7602139 @default.
• W2011276452 hasConcept C79118098 @default.
• W2011276452 hasConcept C99077945 @default.
• W2011276452 hasConceptScore W2011276452C109214941 @default.
• W2011276452 hasConceptScore W2011276452C121332964 @default.
• W2011276452 hasConceptScore W2011276452C151389596 @default.
• W2011276452 hasConceptScore W2011276452C206094082 @default.
• W2011276452 hasConceptScore W2011276452C2778401447 @default.
• W2011276452 hasConceptScore W2011276452C3079626 @default.
• W2011276452 hasConceptScore W2011276452C37914503 @default.
• W2011276452 hasConceptScore W2011276452C52703039 @default.
• W2011276452 hasConceptScore W2011276452C54937798 @default.
• W2011276452 hasConceptScore W2011276452C62520636 @default.
• W2011276452 hasConceptScore W2011276452C7602139 @default.
• W2011276452 hasConceptScore W2011276452C79118098 @default.
• W2011276452 hasConceptScore W2011276452C99077945 @default.
• W2011276452 hasIssue "1" @default.
• W2011276452 hasLocation W20112764521 @default.
• W2011276452 hasLocation W20112764522 @default.
• W2011276452 hasOpenAccess W2011276452 @default.
• W2011276452 hasPrimaryLocation W20112764521 @default.
• W2011276452 hasRelatedWork W1560256990 @default.

• next