We discuss the truncation of low energy effective action of QCD below the chiral symmetry breaking (CSB) scale, including all operators of dimensionality less or equal to 6 which can be built with quark and chiral fields. We perform its bosonization in the scalar, pseudoscalar, vector and axial-vector channels in the large-N_c and leading-log approximation. Constraints on the coefficients of the effective lagrangian are derived from the requirement of Chiral Symmetry Restoration (CSR) at energies above the CSB scale in the scalar-pseudoscalar and vector-axial-vector channels, from matching to QCD at intermediate scales, and by fitting some hadronic observables. In this truncation two types of pseudoscalar states (massless pions and massive ...
I report on recent progress in calculating electroweak processes within the framework of QCD in the ...
We assume a Gaussian approximation for QCD and discuss the heavy-light quark system. Spontaneous chi...
We present the first Nf=2+1+1 results for the matrix elements of the operators describing neutral K ...
We extend our previous formulation of low-energy QCD in terms of an effective lagrangian containing ...
We calculate the coefficients in the chiral Lagrangian approximately from QCD based on a previous st...
We estimate the couplings in the Heavy Hadron Chiral Theory (HHCT) lagrangian from the QCD sum rules...
We investigate the interplay of chiral and heavy quark symmetries by using the NJL quark model. Heav...
The Global Colour Model (GCM) of QCD is a very successful model. Not only is it formally derivable f...
Dynamical chiral symmetry breaking (DCSB) is one of the keystones of low-energy hadronic phenomena. ...
Strong hadronic decays are discussed in the 't Hooft model for the two-dimensional QCD in the limit ...
We calculate the leading non-analytic quark-mass dependence in the moments of isovector quark distri...
We consider the low energy effective action of QCD below the chiral symmetry breaking scale, includi...
We present results of a high-statistics study of scalar and pseudoscalar meson propagators in quench...
We assume a Gaussian approximation for QCD and discuss the heavy-light quark system. Spontaneous chi...
To describe pion as a bound state of two quark, when their current masses are non equal to zero, is ...
I report on recent progress in calculating electroweak processes within the framework of QCD in the ...
We assume a Gaussian approximation for QCD and discuss the heavy-light quark system. Spontaneous chi...
We present the first Nf=2+1+1 results for the matrix elements of the operators describing neutral K ...
We extend our previous formulation of low-energy QCD in terms of an effective lagrangian containing ...
We calculate the coefficients in the chiral Lagrangian approximately from QCD based on a previous st...
We estimate the couplings in the Heavy Hadron Chiral Theory (HHCT) lagrangian from the QCD sum rules...
We investigate the interplay of chiral and heavy quark symmetries by using the NJL quark model. Heav...
The Global Colour Model (GCM) of QCD is a very successful model. Not only is it formally derivable f...
Dynamical chiral symmetry breaking (DCSB) is one of the keystones of low-energy hadronic phenomena. ...
Strong hadronic decays are discussed in the 't Hooft model for the two-dimensional QCD in the limit ...
We calculate the leading non-analytic quark-mass dependence in the moments of isovector quark distri...
We consider the low energy effective action of QCD below the chiral symmetry breaking scale, includi...
We present results of a high-statistics study of scalar and pseudoscalar meson propagators in quench...
We assume a Gaussian approximation for QCD and discuss the heavy-light quark system. Spontaneous chi...
To describe pion as a bound state of two quark, when their current masses are non equal to zero, is ...
I report on recent progress in calculating electroweak processes within the framework of QCD in the ...
We assume a Gaussian approximation for QCD and discuss the heavy-light quark system. Spontaneous chi...
We present the first Nf=2+1+1 results for the matrix elements of the operators describing neutral K ...