Is There Only One Solution of the Dyson-Schwinger Equation for Quark Propagator in the Case of Non-zero Current Quark Mass
arXiv:hep-ph/0402164 · doi:10.1088/0256-307X/22/12/014
Abstract
In this letter it is shown on general ground that there exist two qualitatively distinct solutions of the Dyson-Schwinger equation for the quark propagator in the case of non-zero current quark mass. One solution corresponds to the ``Nambu-Goldstone'' phase and the other one corresponds to the ``Wigner'' phase in the chiral limit.
arXiv comment7 pages
References in corpus (6)
- Dyson-Schwinger Equations and the Application to Hadronic Physics
- Dyson-Schwinger Equations: Density, Temperature and Continuum Strong QCD
- Hadron Physics from the Global Color Model of QCD
- The Calculation of Vacuum Properties from the Global Color Symmetry Model
- Pion susceptibility of the QCD vacuum from an effective quark-quark interaction
- Tensor susceptibility of the QCD vacuum from an effective quark-quark interaction
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