Physics – High Energy Physics – High Energy Physics - Phenomenology
Scientific paper
2002-03-05
Phys.Rev. D66 (2002) 014019
Physics
High Energy Physics
High Energy Physics - Phenomenology
Further typos corrected, to appear in Phys. Rev. D
Scientific paper
10.1103/PhysRevD.66.014019
We calculate the coefficients in the chiral Lagrangian approximately from QCD based on a previous study of deriving the chiral Lagrangian from the first principles of QCD in which the chiral Lagrangian coefficients are defined in terms of certain Green's functions in QCD. We first show that, in the large N(c)-limit, the anomaly part contributions to the coefficients are exactly cancelled by certain terms in the normal part contributions, and the final results of the coefficients only concern the remaining normal part contributions depending on QCD interactions. We then do the calculation in a simple approach with the approximations of taking the large-N(c) limit, the leading order in dynamical perturbation theory, and the improved ladder approximation, thereby the relevant Green's functions are expressed in terms of the quark self energy. By solving the Schwinger-Dyson equation for the quark self energy, we obtain the approximate QCD predicted coefficients and the quark condensate which are consistent with the experimental values.
Kuang Yu-Ping
Lu Qin
Wang Qing
Yang Hua
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