@Article{Lin_etal2024,
author="Lin, J. X.
and Li, J. T.
and Liang, W. H.
and Chen, H. X.
and Oset, E.",
title="J/$\psi$ decays into $\omega$($\phi$) f1(1285) and $\omega$($\phi$) {\textquoteleft}{\textquoteleft}f1(1420){\textquoteright}{\textquoteright}",
journal="European Physical Journal C",
year="2024",
publisher="Springer",
volume="84",
number="1",
pages="52--8pp",
abstract="We perform a theoretical study of the J/psi -> omega (Phi)K* K + c.c. -> omega(Phi)K-0 pi+ K- reactions with the assumption that the f1(1285) is dynamically generated from a single channel K*K + c.c interaction in the chiral unitary approach. Two peaks in the K-0 pi+ K- invariant mass distribution are observed, one clear peak locates at the f(1)(1285) nominal mass, the other peak locates at around 1420MeV with about 70MeV width. We conclude that the former peak is associated with the f(1)(1285) and the latter peak is not a genuine resonance but a manifestation of the kinematic effect in the higher energy region caused by the K* K + c.c. decay mode of the f(1)(1285).",
optnote="WOS:001145308000007",
optnote="exported from refbase (https://references.ific.uv.es/refbase/show.php?record=5911), last updated on Mon, 05 Feb 2024 07:58:13 +0000",
issn="1434-6044",
doi="10.1140/epjc/s10052-024-12405-5",
opturl="https://arxiv.org/abs/2310.19213",
opturl="https://doi.org/10.1140/epjc/s10052-024-12405-5",
language="English"
}