2017
DOI: 10.1103/physrevd.95.114503
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Refining the detection of the zero crossing for the three-gluon vertex in symmetric and asymmetric momentum subtraction schemes

Abstract: This article reports on the detailed study of the three-gluon vertex in four-dimensional SU (3) Yang-Mills theory employing lattice simulations with large physical volumes and high statistics. A meticulous scrutiny of the so-called symmetric and asymmetric kinematical configurations is performed and it is shown that the associated form-factor changes sign at a given range of momenta. The lattice results are compared to the model independent predictions of Schwinger-Dyson equations and a very good agreement amo… Show more

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Cited by 73 publications
(118 citation statements)
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References 95 publications
(125 reference statements)
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“…At zero temperature, the three-gluon vertex shows a zero crossing in four as well as in three dimensions [2,6,46,49,[51][52][53]59,[132][133][134][135]. Analytical studies show that it is caused by the divergent ghost triangle diagram.…”
Section: Three-gluon Vertex and Its Zero Crossingmentioning
confidence: 96%
“…At zero temperature, the three-gluon vertex shows a zero crossing in four as well as in three dimensions [2,6,46,49,[51][52][53]59,[132][133][134][135]. Analytical studies show that it is caused by the divergent ghost triangle diagram.…”
Section: Three-gluon Vertex and Its Zero Crossingmentioning
confidence: 96%
“…Finally, details on the Landau gauge computation of the gauge fields, and the correlation functions defined in Eqs. (2.1) and (2.3), may be found in [35,69]. In addition, the treatment of the O(4)-breaking artifacts has been carried out as described in [56,[70][71][72].…”
Section: B the Lattice Observablesmentioning
confidence: 99%
“…More specifically, in the case of the three-gluon vertex, the left panel of Fig. 6 shows a compilation of the lattice data of this form factor in the symmetric configuration (defined as q 2 = p 2 = r 2 and q · p = q · r = p · r = −q 2 /2, e.g., with a 2π/3 angle between each pair of momenta) [72,73], properly normalized by dividing out the coupling [g = 2 at μ = 4.3 GeV for the data set at hand, corresponding to α s = 0.32]. Notice, in particular, the suppression of the vertex with respect to its tree-level value, as well as the sign reversal (the so-called "zero crossing") at small momenta, followed by a (logarithmic) divergence at the origin.…”
Section: Numerical Analysismentioning
confidence: 99%