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Analytic structure of QCD propagators in Minkowski space

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arxiv 1605.07357 v3 pith:UPV67ZZC submitted 2016-05-24 hep-ph hep-lathep-th

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

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Analytical functions for the propagators of QCD, including a set of chiral quarks, are derived by a one-loop massive expansion in the Landau gauge, deep in the infrared. By analytic continuation, the spectral functions are studied in Minkowski space, yielding a direct proof of positivity violation and confinement from first principles.The dynamical breaking of chiral symmetry is described on the same footing of gluon mass generation, providing a unified picture. While dealing with the exact Lagrangian, the expansion is based on massive free-particle propagators, is safe in the infrared and is equivalent to the standard perturbation theory in the UV. By dimensional regularization, all diverging mass terms cancel exactly without including mass counterterms that would spoil the gauge and chiral symmetry of the Lagrangian. Universal scaling properties are predicted for the inverse dressing functions and shown to be satisfied by the lattice data. Complex conjugated poles are found for the gluon propagator, in agreement with the i-particle scenario.

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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. The causal structure of the quark propagator

    hep-ph 2024-12 conditional novelty 7.0 of 10

    In a spectral DSE computation, the quark propagator develops complex-conjugate poles when the classical quark-gluon vertex strength exceeds a critical value, while the full QCD strength is predicted to stay below that value.

  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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