Abstract
The physical masses of the lowest scalar mesons strongly disagree with the calculated $q\overline{q}$ pole values. It is the purpose of this paper to explain theoretically the unusual spectrum of scalar mesons for both the ground and excited states, using the known spectra of the corresponding $q\overline{q}$ states and their connection to the meson resonances. The well-known Cornell coupled-channel mechanism is exploited for this connection together with the quark-chiral Lagrangian without fitting parameters. In addition to the scalars previously obtained using this method, ${f}_{0}(500)$, ${f}_{0}(980)$, ${a}_{0}(980)$, we predict all ground and first excited scalar states, ${f}_{0}(500)$, ${f}_{0}(980)$, ${a}_{0}(980)$, ${a}_{0}(1450)$, ${K}_{0}^{*}(700)$, ${K}_{0}^{*}(1430)$, ${f}_{0}(1370)$, ${f}_{0}(1710)$, which are in reasonably good agreement with experimental data.
Highlights
The QCD theory of hadrons has been a highly developed resource for treating hadron properties and has explained a majority of observed hadrons far [1]
They can hardly be associated with the lowest conventional qqscalars, for several reasons: (a) their masses are strongly displaced relative to expected qqmasses, and (b) in some cases two observed scalar resonances can be identified with a single qqstate with the same quantum numbers
In this paper we further extend PPM theory to include the radial excitations of the qqstates and find the resulting scalar resonances
Summary
The QCD theory of hadrons has been a highly developed resource for treating hadron properties and has explained a majority of observed hadrons far [1]. In [42] the basic formalism was combined to explain the possible connection of the basic qqpoles to the scalar resonances f0ð500Þ, f0ð980Þ, a0ð980Þ via the quark-chiral coefficients and the qq -meson-meson channel-coupling interaction. In these calculations [42] one fitting parameter in all cases was used—the channel radius λ in the qq -meson-meson transition. The main element of the Cornell formalism [43] is the expression for the total quark-meson Green’s function (resolvent) GðEÞ via the qqresolvent Gqqand the meson-meson resolvent Gφφ, GðEÞ
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