Physics – High Energy Physics – High Energy Physics - Phenomenology
Scientific paper
2003-04-08
Eur.Phys.J.C39:S1-S8,2005
Physics
High Energy Physics
High Energy Physics - Phenomenology
15 pages, Revtex, published version, Eur. Phys. J. C (2004) (DOI) 10.1140/epjcd/s2004-01-001-3
Scientific paper
10.1140/epjcd/s2004-01-001-3
Based on the (approximate) chiral symmetry of QCD Lagrangian and the bound state assumption of effective meson fields, a nonlinearly realized effective chiral Lagrangian for meson fields is obtained from integrating out the quark fields by using the new finite regularization method. As the new method preserves the symmetry principles of the original theory and meanwhile keeps the finite quadratic term given by a physically meaningful characteristic energy scale $M_c$, it then leads to a dynamically spontaneous symmetry breaking in the effective chiral field theory. The gap equations are obtained as the conditions of minimal effective potential in the effective theory. The instanton effects are included via the induced interactions discovered by 't Hooft and found to play an important role in obtaining the physical solutions for the gap equations. The lightest nonet scalar mesons($\sigma$, $f_0$, $a_0$ and $\kappa$) appearing as the chiral partners of the nonet pseudoscalar mesons are found to be composite Higgs bosons with masses below the chiral symmetry breaking scale $\Lambda_{\chi} \sim 1.2$ GeV. In particular, the mass of the singlet scalar (or the $\sigma$) is found to be $m_{\sigma} \simeq 677$ MeV.
Dai Yuan-Ben
Wu Yue-Liang
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