Abstract

As a topic of "quantum color dynamics", we study various mass generation of colored particles and gluonic dressing effect in a non-perturbative manner, using the Schwinger-Dyson (SD) formalism in (scalar) QCD. First, we review dynamical quark-mass generation in QCD in the SD approach as a typical fermion-mass generation via spontaneous chiral-symmetry breaking. Second, using the SD formalism for scalar QCD, we investigate the scalar diquark, a bound-state-like object of two quarks, and its mass generation, which is clearly non-chiral-origin. Here, the scalar diquark is treated as an extended colored scalar field, like a meson in effective hadron models, and its effective size $R$ is introduced as a form factor. As a diagrammatical difference, the SD equation for the scalar diquark has an additional 4-point interaction term, in comparison with the single quark case. The diquark size $R$ is taken to be smaller than a hadron, $R\sim 1$ fm, and larger than a constituent quark, $R\sim 0.3$ fm. We find that the compact diquark with $R\simeq 0.3$ fm has a large effective mass of about 900 MeV, and therefore such a compact diquark is not acceptable in effective models for hadrons. We also consider the artificial removal of 3- and 4-point interaction, respectively, to see the role of each term, and find that the 4-point interaction plays the dominant role of the diquark self-energy. From the above two different cases, quarks and diquarks, we guess that the mass generation of colored particles is a general result of non-perturbative gluonic dressing effect.

Highlights

  • Quantum chromodynamics (QCD) is the fundamental gauge theory of the strong interaction, and it is a longHow to cite this paper: Imai, S. and Suganuma, H. (2016) Non-Perturbative Analysis of Various Mass Generation by Gluonic Dressing Effect with the Schwinger-Dyson Formalism in QCD

  • It is notable that the same form of the running coupling for the quark/gluon coupling can be used even for the scalar diquark/gluon [93] [94]. (In particular, in the heavy mass limit of colored particles, the QCD interaction depends only on their color.) Since the scalar diquark corresponds to an antiquark in terms of the color representation, we may use the same form of the running coupling even for the scalar diquark case

  • We have studied various mass generation of colored particles and gluonic dressing effect in a non-perturbative manner, using the Schwinger-Dyson (SD) formalism in QCD

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Summary

Introduction

Quantum chromodynamics (QCD) is the fundamental gauge theory of the strong interaction, and it is a long. The point-like scalar-quark interacting with gluons acquires a large extra mass of about 1.5 GeV at the cutoff a−1 1 GeV , where a is the lattice spacing. Such a large-mass acquirement would be problematic in describing hadrons with scalar diquarks. Since it is a bound-state-like object inside a hadron, the diquark must have an effective size. This effect gives a natural UV cutoff of the theory, and reduces the large radiative correction.

Dynamical Mass Generation of Quarks in QCD
The Schwinger-Dyson Equation for the Scalar Diquark
The Parameter Setting
The Constant Bare Mass Case
Discussion on the Scalar Diquark Property
Mass Generation for Colored Scalar Particle
Conclusion and Discussion
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