The relations among differential cross section, polarization and helicity density matrix elements in yN -+ nN and TN --L VN processes are given for the photon-vector-meson analogy model. For example, the differential cross sections of yN + ?rN processes are given in terms of density matrix elements
Pion Observables in the Extended NJL Model with Vector and Axial-Vector Mesons
✍ Scribed by Véronique Bernard; Alex H. Blin; Brigitte Hiller; Yuri P. Ivanov; Alexander A. Osipov; Ulf-G. Meißner
- Publisher
- Elsevier Science
- Year
- 1996
- Tongue
- English
- Weight
- 974 KB
- Volume
- 249
- Category
- Article
- ISSN
- 0003-4916
No coin nor oath required. For personal study only.
✦ Synopsis
The momentum-space bosonization method of a Nambu and Jona-Lasinio type model with vector and axial-vector mesons is applied to ?? scattering. Unlike the case in earlier published papers, we obtain the ?? scattering amplitude using the linear and nonlinear realizations of chiral symmetry and fully taking into account the momentum dependence of meson vertices. We show the full physical equivalence between these two approaches. The chiral expansion procedure in this model is discussed in detail. Chiral expansions of the quark mass, pion mass and constant f ? are obtained. The low-energy ?? phase shifts are compared to the available data. We also study the scalar form factor of the pion.
1996 Academic Press, Inc.
1. Introduction
Coloured quarks and gluons are the main objects in the fundamental theory of the strong interactions, quantum chromodynamics (QCD), which are not directly article no.
📜 SIMILAR VOLUMES
The general relation between pion electroproduction and vector meson production by pions is given under the assumption of the vector-meson-photon analogy model. We also propose how to check the off-mass-shell effect on the scattering amplitude for the nN + VN process. In a series of papers (Z)--(3)
An explicit operator construction of the axial vector current in the boson o-model is given in perturbation theory. This current is finite and satisfies the PCAC condition with the renormalized pion field. It also (at least formally) satisfies the SU, x SlJ, equal-time time-component current algebra