Vacuum Structure and Chiral Symmetry Breaking
نویسنده
چکیده
We relate here the vacuum structure of chiral symmetry breaking to a wide class of low energy hadronic properties to examine consistency with experimental results. Phase transition of chiral symmetry breaking is described through explicit vacuum realignment. We find that for the present ansatz, vacuum structure of the light quark sector can be determined from f π = 92 MeV, which then yields that Γ(π 0 → 2γ) = 8.3 eV and, R ch = 0.67 fms, in agreement with experiments. This amounts to three independent 'observa-tions' of the vacuum structure of the light quark sector. For the calculation of Γ(π 0 → 2γ), we do not use the anomaly equation-local gauge invariance for vacuum realignment becomes adequate. The above width is sensitive to the vacuum structure, and can give evidence regarding progress towards chiral symmetry restoration in QGP. The corresponding results for s quark sector are moderately good. We also exploit similar ideas for heavy quarks, but here the experimental data are rare, and the theoretical techniques are likely to need refinements.
منابع مشابه
Gluon Condensates , Chiral Symmetry Breaking And Pion Wave - function
We consider here chiral symmetry breaking in quantum chromodynamics arising from gluon condensates in vacuum. Through coherent states of gluons simulating a mean field type of approximation, we show that the off-shell gluon condensates of vacuum generate a mass-like contribution for the quarks, giving rise to chiral symmetry breaking. We next note that spontaneous breaking of global chiral symm...
متن کاملNo massless boson in chiral symmetry breaking in NJL and Thirring models
We show that the chiral symmetry breaking occurs in the vacuum of the massless Nambu-Jona-Lasinio (NJL) and Thirring models without a Goldstone boson. The basic reason of non-existence of the massless boson is due to the fact that the new vacuum after the symmetry breaking acquires nonzero fermion mass which inevitably leads to massive bosons. The new vacuum has a finite condensate of 〈ψ̄ψ〉 with...
متن کاملA Mechanism for Instanton induced Chiral Symmetry Breaking in QCD
We propose a mechanism for instanton induced chiral symmetry breaking in QCD with fundamental scalars. The model Lagragian that we use has the same symmetry properties as QCD. The scalar fields develop vacuum expectation values at a non-trivial minimum and generate masses for thhe light quarks. The minimization condition is also used to break the SU(Nf ) flavour symmetry in order to make the s ...
متن کاملPhase transition in two-flavor dense QCD from the Schwinger-Dyson equation
We investigate the phase structure of the two-flavor dense QCD using the SchwingerDyson equation (SDE) with the improved ladder approximation in the Landau gauge. The SDE for diquark condensate (color superconducting condensate) and that for quarkantiquark condensate (chiral condensate) are solved separately. In the low density region both the SDE’s have nontrivial solutions which correspond to...
متن کاملFoundations of the Constituent Quark Model
‘Constituent quarks’ means massive quarks, in contrast to the nearly massless u, d, s quarks of the QCD lagrangian. The dynamical or constituent masses appear owing to the spontaneous chiral symmetry breaking in QCD. A realistic mechanism of the chiral symmetry breaking is provided by instantons. Therefore, I review the present status of the QCD instanton vacuum, emphasizing the mechanism of ch...
متن کامل