2016/11/10 by Daniele Binosi, Craig D. Roberts, J. Rodrı́guez-Quintero +1 · 49 citations
Physics and Astronomy · #Chiral symmetry breaking #High-Energy Particle Collisions Research #Infrared fixed point #Mathematical physics #Particle physics #Particle physics theoretical and experimental studies #Physics #Quantum Chromodynamics and Particle Interactions #Quantum chromodynamics #Quark #Renormalization #Renormalization group #Symmetry breaking #hep-lat #hep-ph #nucl-th
paper · pdf · doi:10.1103/physrevd.95.114009
published in Physical review. D/Physical review. D. 95(11) (American Physical Society) · 8 pages, 4 figures, 2 tables
arxiv created 2016/11/10 · openalex created_date 2017/03/23 · openalex publication_date 2017/06/13 · arxiv updated 2017/06/21 · openalex updated_date 2026/08/05
We determine the flavor dependence of the renormalization-group-invariant running interaction through judicious use of both unquenched Dyson-Schwinger equation and lattice results for QCD's gauge-sector two-point functions. An important step is the introduction of a physical scale setting procedure that enables a realistic expression of the effect of different numbers of active quark flavours on the interaction. Using this running interaction in concert with a well constrained class of dressed--gluon-quark vertices, we estimate the critical number of active lighter-quarks above which dynamical chiral symmetry breaking becomes impossible: nfcr\ensuremath≈9; and hence in whose neighborhood QCD is plausibly a conformal theory.