FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2171878145> ?p ?o ?g. }

• W2171878145 endingPage "618" @default.
• W2171878145 startingPage "612" @default.
• W2171878145 abstract "We develop a simple model for coupling the pseudo-Goldstone bosons of QCD Or's, K's, -q) to quark fields. This nonlocal model incorporates a momentum dependent dynamical quark mass ,~ (p) in a manner consistent with global chiral symmetry. Explicit current quark masses and gauge fields are also introduced. All low energy parameters of the chiral lagrangian are expressed in terms of ~(p). In particular we obtain the ten coefficients of order pa terms in the energy expansion. The physical values for too, mR +, inK0 , f#, and fn are used to determine the three current quark masses, the constituent quark mass, and the quark condensate. The results are in surprisingly good agreement with the experimental values. In this paper we will present a simple nonlocal model for pseudo-Goldstone bosons (PGBs) coupled to massive quarks. Upon integrating out the quarks and performing a derivative expansion the model yields an effective low energy chiral lagrangian. We will make no attempt to derive the model as a controlled approximation to QCD, and there is no reason a priori why the chiral lagrangian we obtain should resemble the low energy effective theory of QCD. But the model does incorporate a nontrivial momentum dependence for the quark mass and thereby represents the dynamical quark mass in QCD. This is accomplished in a manner consistent with the dynamical breakdown of chiral symmetry and it improves previous derivations of chiral lagrangians in chiral quark models. We find, rather surprisingly, that the model does well at reproducing what is currently known about low energy QCD. An effective chiral lagrangian may be used to encode the physics of the PGBs of QCD in a systematic low-energy expansion. In the notation of Gasser and Leutwyler [ 1 ], for QCD with three light quarks the leading (order p~) and next-to-leading (order p4) terms of the chiral lagrangian are the following: L = ]Fo2{(V ~ U+V~. + (X+ U + X U+)} + L, (V ~ U+V. 2 + L2(V~ U+V. U)(V ~' U+V U) + La(V g UtV~, UVU+V." @default.
• W2171878145 created "2016-06-24" @default.
• W2171878145 creator A5017262644 @default.
• W2171878145 creator A5071883428 @default.
• W2171878145 creator A5083149563 @default.
• W2171878145 date "1990-08-01" @default.
• W2171878145 modified "2023-09-24" @default.
• W2171878145 title "Chiral lagrangian from quarks with dynamical mass" @default.
• W2171878145 cites W1988373960 @default.
• W2171878145 cites W1991030422 @default.
• W2171878145 cites W1995758984 @default.
• W2171878145 cites W2003714477 @default.
• W2171878145 cites W2007484939 @default.
• W2171878145 cites W2012093868 @default.
• W2171878145 cites W2013058961 @default.
• W2171878145 cites W2013713498 @default.
• W2171878145 cites W2016076332 @default.
• W2171878145 cites W2020878299 @default.
• W2171878145 cites W2021242349 @default.
• W2171878145 cites W2028596933 @default.
• W2171878145 cites W2034928797 @default.
• W2171878145 cites W2042248841 @default.
• W2171878145 cites W2047153943 @default.
• W2171878145 cites W2058839247 @default.
• W2171878145 cites W2075654402 @default.
• W2171878145 cites W2081122760 @default.
• W2171878145 cites W2083629111 @default.
• W2171878145 cites W2091013442 @default.
• W2171878145 cites W2124141606 @default.
• W2171878145 cites W4235893598 @default.
• W2171878145 doi "https://doi.org/10.1016/0370-2693(90)90700-g" @default.
• W2171878145 hasPublicationYear "1990" @default.
• W2171878145 type Work @default.
• W2171878145 sameAs 2171878145 @default.
• W2171878145 citedByCount "51" @default.
• W2171878145 countsByYear W21718781452016 @default.
• W2171878145 crossrefType "journal-article" @default.
• W2171878145 hasAuthorship W2171878145A5017262644 @default.
• W2171878145 hasAuthorship W2171878145A5071883428 @default.
• W2171878145 hasAuthorship W2171878145A5083149563 @default.
• W2171878145 hasBestOaLocation W21718781452 @default.
• W2171878145 hasConcept C109214941 @default.
• W2171878145 hasConcept C121332964 @default.
• W2171878145 hasConcept C2778564446 @default.
• W2171878145 hasConcept C3079626 @default.
• W2171878145 hasConcept C37914503 @default.
• W2171878145 hasConcept C53469067 @default.
• W2171878145 hasConcept C7602139 @default.
• W2171878145 hasConceptScore W2171878145C109214941 @default.
• W2171878145 hasConceptScore W2171878145C121332964 @default.
• W2171878145 hasConceptScore W2171878145C2778564446 @default.
• W2171878145 hasConceptScore W2171878145C3079626 @default.
• W2171878145 hasConceptScore W2171878145C37914503 @default.
• W2171878145 hasConceptScore W2171878145C53469067 @default.
• W2171878145 hasConceptScore W2171878145C7602139 @default.
• W2171878145 hasIssue "3-4" @default.
• W2171878145 hasLocation W21718781451 @default.
• W2171878145 hasLocation W21718781452 @default.
• W2171878145 hasOpenAccess W2171878145 @default.
• W2171878145 hasPrimaryLocation W21718781451 @default.
• W2171878145 hasRelatedWork W2010075806 @default.
• W2171878145 hasRelatedWork W2058383649 @default.
• W2171878145 hasRelatedWork W2086948415 @default.
• W2171878145 hasRelatedWork W2092852450 @default.
• W2171878145 hasRelatedWork W2143478461 @default.
• W2171878145 hasRelatedWork W2238229723 @default.
• W2171878145 hasRelatedWork W2316477781 @default.
• W2171878145 hasRelatedWork W2732235149 @default.
• W2171878145 hasRelatedWork W2916760050 @default.
• W2171878145 hasRelatedWork W621198837 @default.
• W2171878145 hasVolume "245" @default.
• W2171878145 isParatext "false" @default.
• W2171878145 isRetracted "false" @default.
• W2171878145 magId "2171878145" @default.
• W2171878145 workType "article" @default.