6533b860fe1ef96bd12c393a

RESEARCH PRODUCT

Low-lying even parity meson resonances and spin-flavor symmetry revisited

Lorenzo Luis SalcedoEn WangJu-jun XieLi-sheng GengCarmen Garcia-recioJ. Nieves

subject

QuarkNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryMesonNuclear TheoryHigh Energy Physics::LatticeFOS: Physical sciences01 natural sciencesNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)Chiral perturbation theoryInvers Amplitude Method0103 physical sciencesSymmetry breaking010306 general physicsPhysicsQuantum chromodynamics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaParity (physics)Quantum numberHigh Energy Physics - PhenomenologyChiral symmetry breaking

description

We review and extend the model derived in Garcia-Recio et al. [Phys. Rev. D 83, 016007 (2011)] to address the dynamics of the low-lying even-parity meson resonances. This model is based on a coupled-channels spin-flavor extension of the chiralWeinberg-Tomozawa Lagrangian. This interaction is then used to study the S-wave meson-meson scattering involving members not only of the pi octet, but also of the rho nonet. In this work, we study in detail the structure of the SU(6)-symmetry-breaking contact terms that respect (or softly break) chiral symmetry. We derive the most general local (without involving derivatives) terms consistent with the chiral-symmetry-breaking pattern of QCD. After introducing sensible simplifications to reduce the large number of possible operators, we carry out a phenomenological discussion of the effects of these terms. We show how the inclusion of these pieces leads to an improvement of the description of the J(P) = 2(+) sector, without spoiling the main features of the predictions obtained in the original model in the JP = 0(+) and J(P) = 1(+) sectors. In particular, we find a significantly better description of the I-G(J(PC)) =0(+)(2(++)), 1(-)(2(++)) and the I(JP)=1/2(2(+)) sectors, which correspond to the f(2)(1270), a(2)(1320), and K-2(*)(1430) quantum numbers, respectively.

10.1103/physrevd.87.096006http://hdl.handle.net/10550/39185