The fundamental scale of QCD
arXiv:2103.08223 · doi:10.1134/S1063778821130342
Abstract
There are several scales in the QCD as the theory of strong interaction: the vacuum gluonic condensate (as the divergence of the dilatation current), the nucleon mass as the basic mass scale in our universe, which is connected to the string tension , and the perturbative QCD scale , which defines the scale of the renormalized perturbative expansions. In this paper we connect all these scales to the vacuum condensate, using the field correlator method, where the string tension is expressed in terms of nonlocal field correlators, which are connected to the local condensates, while the perturbative is connected to in the framework of the Background Perturbation Theory (BPT). We also demonstrate how the IR singularities and IR renormalons disappear in BPT making the resulting theory internally consistent.
arXiv comment17 pages,3 figures
References in corpus (19)
- Renormalons
- Analytic Model for the QCD Running Coupling with Universal Value
- The 2009 World Average of
- Field correlators in QCD. Theory and applications
- Optimization of R(e+e-) and "Freezing" of the QCD Couplant at Low Energies
- The Confinement
- Casimir scaling as a test of QCD vacuum
- Gluelump spectrum in the QCD string model
- Perturbative expansions in QCD and analytic properties of alpha_s
- Puzzles in Hadronic Physics and Novel Quantum Chromodynamics Phenomenology
- Asymptotic freedom and IR freezing in QCD: the role of gluon paramagnetism
- Fourth-order QCD renormalization group quantities in the {\rm{V}}-scheme and the relation of the -function to the Gell-Mann--Low function in QED
- Perturbative QCD of hard and soft processes
- Analytic calculation of field-strength correlators
- Field Correlator Method for the confinement in QCD
- Confinement Mechanism in the Field Correlator Method
- Nonperturbative quark dynamics in a baryon
- Boosting QED and QCD bound states in the path integral formalism
- Novel solutions of RG equations for alpha(s) and beta(alpha) in the large N_c limit