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Gluon mass generation in the presence of dynamical quarks

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arxiv 1304.5936 v2 pith:VVTX46E5 submitted 2013-04-22 hep-ph hep-lathep-th

classification hep-phhep-lathep-th
keywords gluonmasspropagatorinfrareddiagramdynamicalequationfamilies
verification ladder T0 review T1 audit T2 compute T3 formal

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We study in detail the impact of dynamical quarks on the gluon mass generation mechanism, in the Landau gauge, for the case of a small number of quark families. As in earlier considerations, we assume that the main bulk of the unquenching corrections to the gluon propagator originates from the fully dressed quark-loop diagram. The nonperturbative evaluation of this diagram provides the key relation that expresses the unquenched gluon propagator as a deviation from its quenched counterpart. This relation is subsequently coupled to the integral equation that controls the momentum evolution of the effective gluon mass, which contains a single adjustable parameter; this constitutes a major improvement compared to the analysis presented in Phys. Rev. D86 (2012) 014032, where the behaviour of the gluon propagator in the deep infrared was estimated through numerical extrapolation. The resulting nonlinear system is then treated numerically, yielding unique solutions for the modified gluon mass and the quenched gluon propagator, which fully confirm the picture put forth recently in several continuum and lattice studies. In particular, an infrared finite gluon propagator emerges, whose saturation point is considerably suppressed, due to a corresponding increase in the value of the gluon mass. This characteristic feature becomes more pronounced as the number of active quark families increases, and can be deduced from the infrared structure of the kernel entering in the gluon mass equation.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Physics of the gluon mass gap

    hep-ph 2025-08 conditional novelty 6.0 of 10

    The gluon mass gap, defined as the complex pole of the gluon propagator, is linearly tied to the deconfinement temperature, and both Tc and fπ are insensitive to deep-infrared deformations below the infrared inflection point.

  2. Quark Propagator at one-loop in the Refined Gribov-Zwanziger framework

    hep-th 2025-05 conditional novelty 5.0 of 10

    At one loop in the Refined Gribov-Zwanziger framework, the quark mass function agrees roughly with lattice QCD after fitting the gluon propagator, but the dressing function disagrees in the infrared.

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