Matches in SemOpenAlex for { <https://semopenalex.org/work/W2034540217> ?p ?o ?g. }
- W2034540217 abstract "A thorough study of 4-dimensional SU(2) Yang-Mills theory in Coulomb gauge is performed using large scale lattice simulations. The (equal-time) transverse gluon propagator, the ghost form factor d(p) and the Coulomb potential V_{coul} (p) ~ d^2(p) f(p)/p^2 are calculated. For large momenta p, the gluon propagator decreases like 1/p^{1+eta} with eta =0.5(1). At low momentum, the propagator is weakly momentum dependent. The small momentum behavior of the Coulomb potential is consistent with linear confinement. We find that the inequality sigma_{coul} ge sigma comes close to be saturated. Finally, we provide evidence that the ghost form factor d(p) and f(p) acquire IR singularities, i.e., d(p) propto 1/sqrt{p} and f(p) propto 1/p, respectively. It turns out that the combination g_0^2 d_0(p) of the bare gauge coupling g_0 and the bare ghost form factor d_0(p) is finite and therefore renormalization group invariant." @default.
- W2034540217 created "2016-06-24" @default.
- W2034540217 creator A5015756372 @default.
- W2034540217 creator A5045459961 @default.
- W2034540217 date "2004-10-13" @default.
- W2034540217 modified "2023-10-16" @default.
- W2034540217 title "Propagators in Coulomb gauge from SU(2) lattice gauge theory" @default.
- W2034540217 cites W1514487823 @default.
- W2034540217 cites W1605113314 @default.
- W2034540217 cites W1987863892 @default.
- W2034540217 cites W1994969983 @default.
- W2034540217 cites W1997241615 @default.
- W2034540217 cites W1998620850 @default.
- W2034540217 cites W2001790848 @default.
- W2034540217 cites W2002765685 @default.
- W2034540217 cites W2006577223 @default.
- W2034540217 cites W2011500808 @default.
- W2034540217 cites W2013699130 @default.
- W2034540217 cites W2018850201 @default.
- W2034540217 cites W2021984131 @default.
- W2034540217 cites W2025720005 @default.
- W2034540217 cites W2029301184 @default.
- W2034540217 cites W2032451690 @default.
- W2034540217 cites W2032641545 @default.
- W2034540217 cites W2038584293 @default.
- W2034540217 cites W2044694400 @default.
- W2034540217 cites W2044879294 @default.
- W2034540217 cites W2045163697 @default.
- W2034540217 cites W2056785266 @default.
- W2034540217 cites W2059798761 @default.
- W2034540217 cites W2069440073 @default.
- W2034540217 cites W2081683262 @default.
- W2034540217 cites W2091045653 @default.
- W2034540217 cites W2092617456 @default.
- W2034540217 cites W2097343631 @default.
- W2034540217 cites W2099708120 @default.
- W2034540217 cites W2131835095 @default.
- W2034540217 cites W2139213325 @default.
- W2034540217 cites W2148384901 @default.
- W2034540217 cites W2291978477 @default.
- W2034540217 cites W2953259908 @default.
- W2034540217 cites W3104625665 @default.
- W2034540217 cites W4256142438 @default.
- W2034540217 doi "https://doi.org/10.1103/physrevd.70.074507" @default.
- W2034540217 hasPublicationYear "2004" @default.
- W2034540217 type Work @default.
- W2034540217 sameAs 2034540217 @default.
- W2034540217 citedByCount "62" @default.
- W2034540217 countsByYear W20345402172012 @default.
- W2034540217 countsByYear W20345402172013 @default.
- W2034540217 countsByYear W20345402172014 @default.
- W2034540217 countsByYear W20345402172015 @default.
- W2034540217 countsByYear W20345402172016 @default.
- W2034540217 countsByYear W20345402172017 @default.
- W2034540217 countsByYear W20345402172018 @default.
- W2034540217 countsByYear W20345402172020 @default.
- W2034540217 countsByYear W20345402172021 @default.
- W2034540217 crossrefType "journal-article" @default.
- W2034540217 hasAuthorship W2034540217A5015756372 @default.
- W2034540217 hasAuthorship W2034540217A5045459961 @default.
- W2034540217 hasBestOaLocation W20345402172 @default.
- W2034540217 hasConcept C10138342 @default.
- W2034540217 hasConcept C104416048 @default.
- W2034540217 hasConcept C117137515 @default.
- W2034540217 hasConcept C121332964 @default.
- W2034540217 hasConcept C123579102 @default.
- W2034540217 hasConcept C138817895 @default.
- W2034540217 hasConcept C147120987 @default.
- W2034540217 hasConcept C162324750 @default.
- W2034540217 hasConcept C166124518 @default.
- W2034540217 hasConcept C181830111 @default.
- W2034540217 hasConcept C24890656 @default.
- W2034540217 hasConcept C2781204021 @default.
- W2034540217 hasConcept C3079626 @default.
- W2034540217 hasConcept C31593994 @default.
- W2034540217 hasConcept C37914503 @default.
- W2034540217 hasConcept C40263606 @default.
- W2034540217 hasConcept C42238305 @default.
- W2034540217 hasConcept C60718061 @default.
- W2034540217 hasConcept C62520636 @default.
- W2034540217 hasConcept C68532491 @default.
- W2034540217 hasConcept C9342510 @default.
- W2034540217 hasConceptScore W2034540217C10138342 @default.
- W2034540217 hasConceptScore W2034540217C104416048 @default.
- W2034540217 hasConceptScore W2034540217C117137515 @default.
- W2034540217 hasConceptScore W2034540217C121332964 @default.
- W2034540217 hasConceptScore W2034540217C123579102 @default.
- W2034540217 hasConceptScore W2034540217C138817895 @default.
- W2034540217 hasConceptScore W2034540217C147120987 @default.
- W2034540217 hasConceptScore W2034540217C162324750 @default.
- W2034540217 hasConceptScore W2034540217C166124518 @default.
- W2034540217 hasConceptScore W2034540217C181830111 @default.
- W2034540217 hasConceptScore W2034540217C24890656 @default.
- W2034540217 hasConceptScore W2034540217C2781204021 @default.
- W2034540217 hasConceptScore W2034540217C3079626 @default.
- W2034540217 hasConceptScore W2034540217C31593994 @default.
- W2034540217 hasConceptScore W2034540217C37914503 @default.
- W2034540217 hasConceptScore W2034540217C40263606 @default.
- W2034540217 hasConceptScore W2034540217C42238305 @default.
- W2034540217 hasConceptScore W2034540217C60718061 @default.