@Article{Garcia-Recio_etal2013,
author="Garcia-Recio, C.
and Geng, L. S.
and Nieves, J.
and Salcedo, L. L.
and Wang, E.
and Xie, J. J.",
title="Low-lying even parity meson resonances and spin-flavor symmetry revisited",
journal="Physical Review D",
year="2013",
publisher="Amer Physical Soc",
volume="87",
number="9",
pages="096006--18pp",
abstract="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.",
optnote="WOS:000319059500004",
optnote="exported from refbase (https://references.ific.uv.es/refbase/show.php?record=1450), last updated on Thu, 20 Jun 2013 12:02:16 +0000",
issn="1550-7998",
doi="10.1103/PhysRevD.87.096006",
opturl="http://arxiv.org/abs/1304.1021",
opturl="https://doi.org/10.1103/PhysRevD.87.096006",
archivePrefix="arXiv",
eprint="1304.1021",
language="English"
}