Matches in SemOpenAlex for { <https://semopenalex.org/work/W1977022548> ?p ?o ?g. }
- W1977022548 endingPage "726" @default.
- W1977022548 startingPage "712" @default.
- W1977022548 abstract "We investigate the dependence of the QCD vacuum structure on the $theta$-angle and quark mass, using the Di-Vecchia--Veneziano model. Although the Di-Vecchia--Veneziano model is a chiral effective model, it contains the topological properties of the pure Yang--Mills theory. It is shown that within this model, the ground state energies for all $theta$ are continuous functions of quark mass from the chiral limit to the quenched limit, even including the first order phase transition at $theta = pi$. Based on this effective model, we discuss (i) how the ground state depends on quark mass, and (ii) why the phase transition at $theta = pi$ is present both in the chiral and quenched limit. In order to analyze the relation between quark mass and the $theta$-vacua, we calculate the chiral condensate as a function of quark mass. Also, considering the presence of the innate metastable states included in the QCD $theta$-vacuum, we also give a unified understanding of the phase transitions at $theta = pi$ in the chiral and quenched limit." @default.
- W1977022548 created "2016-06-24" @default.
- W1977022548 creator A5035076890 @default.
- W1977022548 date "2014-12-01" @default.
- W1977022548 modified "2023-09-30" @default.
- W1977022548 title "QCD θ -vacua from the chiral limit to the quenched limit" @default.
- W1977022548 cites W1561867150 @default.
- W1977022548 cites W1740296105 @default.
- W1977022548 cites W1762584651 @default.
- W1977022548 cites W1844019259 @default.
- W1977022548 cites W1921023200 @default.
- W1977022548 cites W194364720 @default.
- W1977022548 cites W1958894153 @default.
- W1977022548 cites W1968984039 @default.
- W1977022548 cites W196925666 @default.
- W1977022548 cites W1969396244 @default.
- W1977022548 cites W1980931786 @default.
- W1977022548 cites W1981234283 @default.
- W1977022548 cites W1989818853 @default.
- W1977022548 cites W1994101208 @default.
- W1977022548 cites W1995175048 @default.
- W1977022548 cites W1997902877 @default.
- W1977022548 cites W1998323214 @default.
- W1977022548 cites W1998474538 @default.
- W1977022548 cites W2001065717 @default.
- W1977022548 cites W2006780700 @default.
- W1977022548 cites W2015895943 @default.
- W1977022548 cites W2019930952 @default.
- W1977022548 cites W2025712550 @default.
- W1977022548 cites W2027123664 @default.
- W1977022548 cites W2028043408 @default.
- W1977022548 cites W2035928167 @default.
- W1977022548 cites W2041226112 @default.
- W1977022548 cites W2047911152 @default.
- W1977022548 cites W2054804077 @default.
- W1977022548 cites W2056463321 @default.
- W1977022548 cites W2059774580 @default.
- W1977022548 cites W2059847138 @default.
- W1977022548 cites W2061044423 @default.
- W1977022548 cites W2063237488 @default.
- W1977022548 cites W2087276725 @default.
- W1977022548 cites W2090153452 @default.
- W1977022548 cites W2094078806 @default.
- W1977022548 cites W2098002520 @default.
- W1977022548 cites W2146423825 @default.
- W1977022548 cites W2154010782 @default.
- W1977022548 cites W2169641865 @default.
- W1977022548 cites W2177787397 @default.
- W1977022548 cites W2209061280 @default.
- W1977022548 cites W2952951178 @default.
- W1977022548 cites W2963838362 @default.
- W1977022548 cites W3105734522 @default.
- W1977022548 cites W3106365705 @default.
- W1977022548 cites W882030661 @default.
- W1977022548 doi "https://doi.org/10.1016/j.nuclphysb.2014.11.002" @default.
- W1977022548 hasPublicationYear "2014" @default.
- W1977022548 type Work @default.
- W1977022548 sameAs 1977022548 @default.
- W1977022548 citedByCount "6" @default.
- W1977022548 countsByYear W19770225482017 @default.
- W1977022548 countsByYear W19770225482018 @default.
- W1977022548 countsByYear W19770225482020 @default.
- W1977022548 crossrefType "journal-article" @default.
- W1977022548 hasAuthorship W1977022548A5035076890 @default.
- W1977022548 hasBestOaLocation W19770225481 @default.
- W1977022548 hasConcept C10138342 @default.
- W1977022548 hasConcept C109214941 @default.
- W1977022548 hasConcept C117137515 @default.
- W1977022548 hasConcept C121332964 @default.
- W1977022548 hasConcept C134306372 @default.
- W1977022548 hasConcept C149288129 @default.
- W1977022548 hasConcept C151201525 @default.
- W1977022548 hasConcept C16090227 @default.
- W1977022548 hasConcept C162324750 @default.
- W1977022548 hasConcept C182306322 @default.
- W1977022548 hasConcept C3079626 @default.
- W1977022548 hasConcept C33923547 @default.
- W1977022548 hasConcept C3909970 @default.
- W1977022548 hasConcept C62520636 @default.
- W1977022548 hasConcept C69523127 @default.
- W1977022548 hasConcept C7602139 @default.
- W1977022548 hasConcept C89464430 @default.
- W1977022548 hasConcept C99077945 @default.
- W1977022548 hasConceptScore W1977022548C10138342 @default.
- W1977022548 hasConceptScore W1977022548C109214941 @default.
- W1977022548 hasConceptScore W1977022548C117137515 @default.
- W1977022548 hasConceptScore W1977022548C121332964 @default.
- W1977022548 hasConceptScore W1977022548C134306372 @default.
- W1977022548 hasConceptScore W1977022548C149288129 @default.
- W1977022548 hasConceptScore W1977022548C151201525 @default.
- W1977022548 hasConceptScore W1977022548C16090227 @default.
- W1977022548 hasConceptScore W1977022548C162324750 @default.
- W1977022548 hasConceptScore W1977022548C182306322 @default.
- W1977022548 hasConceptScore W1977022548C3079626 @default.
- W1977022548 hasConceptScore W1977022548C33923547 @default.
- W1977022548 hasConceptScore W1977022548C3909970 @default.
- W1977022548 hasConceptScore W1977022548C62520636 @default.
- W1977022548 hasConceptScore W1977022548C69523127 @default.