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On the structure of the scalar mesons $f_0(975)$ and $a_0(980)$

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arxiv nucl-th/9411021 v1 pith:TK34HKT3 submitted 1994-11-22 nucl-th hep-ph

classification nucl-thhep-ph
keywords modelsoverlinepolestructuredescriptiongammamesonsmodel
verification ladder T0 review T1 audit T2 compute T3 formal
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abstract

We investigate the structure of the scalar mesons $f_0(975)$ and $a_0(980)$ within realistic meson-exchange models of the $\pi\pi$ and $\pi\eta$ interactions. Starting from a modified version of the J\"ulich model for $\pi\pi$ scattering we perform an analysis of the pole structure of the resulting scattering amplitude and find, in contrast to existing models, a somewhat large mass for the $f_0(975)$ ($m_{f_0}=1015$ MeV, $\Gamma_{f_0}=30$ MeV). It is shown that our model provides a description of $J/\psi\rightarrow\phi\pi\pi/\phi KK$ data comparable in quality with those of alternative models. Furthermore, the formalism developed for the $\pi\pi$ system is consistently extended to the $\pi\eta$ interaction leading to a description of the $a_0(980)$ as a dynamically generated threshold effect (which is therefore neither a conventional $q\overline{q}$ state nor a $K\overline{K}$ bound state). Exploring the corresponding pole position the $a_0(980)$ is found to be rather broad ($m_{a_0}=991$ MeV, $\Gamma_{a_0}=202$ MeV). The experimentally observed smaller width results from the influence of the nearby $K\overline{K}$ threshold on this pole.

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Cited by 1 Pith paper

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  1. Revisiting the $\Lambda_c^+ \to n\pi^+\eta$ decay in light of the BESIII measurement

    hep-ph 2026-08 conditional novelty 5.0 of 10

    The measured π+η mass spectrum of Λc+ → n π+ η is best reproduced by chiral-unitary models that include the N(1440) nucleon excitation; the a2(1320) tensor meson does not improve the fit.

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