Abstract:We study the origins of the inaccuracies of Schwinger's nonet mass, and the Sakurai mass-mixing angle, formulae for the pseudoscalar meson nonet, and suggest new versions of them, modified by the inclusion of the pseudoscalar decay constants. We use these new formulae to determine the pseudoscalar decay constants and mixing angle. The results obtained, f 8 /f π = 1.185± 0.040, f 9 /f π = 1.095 ± 0.020, f η /f π = 1.085 ± 0.025, f η ′ /f π = 1.195 ± 0.035, θ = (−21.4 ± 1.0) o , are in excellent agreement with e… Show more
“…We will not compare our prediction with the results from the two-mixing-angle schemes [4,5,8,12] since different mixing schemes are employed. Our result for the ratio f 8 /f π being 0.94±0.07 is smaller than the prediction from Chiral perturbation theory (ChPT) f 8 /f π = 1.28 [2,8] and most phenomenological analyses [1,3,9,12,13], but is larger than the result given in Ref. [5] f 8 /f π = 0.71.…”
contrasting
confidence: 84%
“…The recent experimental measurements on the productions of η and η ′ from the CLEO collaboration [15] and L3 collaboration [16] have stimulated more phenomenological studies on this issue [11][12][13][14]. The theoretical analyses are usually model dependent, and the predictions for θ vary from −12 • [4,13] to −20 • [2,9]. Besides the mixing angle θ, another two parameters f 8 and f 1 , the decay constants of η 8 and η 1 , are usually introduced.…”
We obtained two analytical constraints on the η-η ′ mixing parameters by considering two-photon decays of η and η ′ [η (η ′ ) → γγ], and productions of η and η ′ in the e + e − scattering at large momentum transfer (Q 2 → ∞). Using the data given in the PDG98 for the decay processes and recent CLEO measurements on the mesonphoton transition form factors, we estimate for the η 8 -η 1 mixing scheme the mixing angle to be θ = −14.5 • ± 2.0 • and the ratio of the decay constants of singlet to octet to be f 1 /f 8 = 1.17 ± 0.08. Applying our approach to the recently proposed qq-ss mixing scheme, we obtain the mixing angle to be φ = 39.8 • ± 1.8 • and the ratio of the decay constants of ss state to qq state to be f s /f q = 1.20 ± 0.10.
“…We will not compare our prediction with the results from the two-mixing-angle schemes [4,5,8,12] since different mixing schemes are employed. Our result for the ratio f 8 /f π being 0.94±0.07 is smaller than the prediction from Chiral perturbation theory (ChPT) f 8 /f π = 1.28 [2,8] and most phenomenological analyses [1,3,9,12,13], but is larger than the result given in Ref. [5] f 8 /f π = 0.71.…”
contrasting
confidence: 84%
“…The recent experimental measurements on the productions of η and η ′ from the CLEO collaboration [15] and L3 collaboration [16] have stimulated more phenomenological studies on this issue [11][12][13][14]. The theoretical analyses are usually model dependent, and the predictions for θ vary from −12 • [4,13] to −20 • [2,9]. Besides the mixing angle θ, another two parameters f 8 and f 1 , the decay constants of η 8 and η 1 , are usually introduced.…”
We obtained two analytical constraints on the η-η ′ mixing parameters by considering two-photon decays of η and η ′ [η (η ′ ) → γγ], and productions of η and η ′ in the e + e − scattering at large momentum transfer (Q 2 → ∞). Using the data given in the PDG98 for the decay processes and recent CLEO measurements on the mesonphoton transition form factors, we estimate for the η 8 -η 1 mixing scheme the mixing angle to be θ = −14.5 • ± 2.0 • and the ratio of the decay constants of singlet to octet to be f 1 /f 8 = 1.17 ± 0.08. Applying our approach to the recently proposed qq-ss mixing scheme, we obtain the mixing angle to be φ = 39.8 • ± 1.8 • and the ratio of the decay constants of ss state to qq state to be f s /f q = 1.20 ± 0.10.
“…Thus, introducing only the anomalous shift of the η 0 mass still yields the usual Schwinger relation, as noted by Ref. [51] in a different approach. The pion remains decoupled from the etas as long as one stays in the isospin limit; i.e., after one adds the anomalous contributionM 2 A (35) to Eq.…”
Section: A Masses In the η-η ′ Complexmentioning
confidence: 88%
“…(29). The usual Schwinger formula is known to be satisfied well for the vector and tensor nonets, but not for the pseudoscalar nonet [51]. Equation (38) reduces to the usual Schwinger pseudoscalar-meson relation for the limit of no anomaly, 3β → 0, but also for just X → 1, the limit of no influence of the flavor symmetry breaking on the anomalous mass shifts.…”
The study of light pseudoscalar quark-antiquark bound states in the Dyson-Schwinger approach with the effective QCD coupling enhanced by the interplay of the dimension 2 gluon condensate A 2 and dimension 4 gluon condensate F 2 , is extended to the η-η ′ complex. We include the effects of the gluon axial anomaly into the Dyson-Schwinger approach to mesons. The calculated masses, mixing and two-photon decay widths of η and η ′ mesons are in agreement with experiment. Also, in a model-independent way, we give the modification of the Gell-Mann-Okubo and Schwinger nonet relations due to the interplay of the gluon anomaly and SU(3) flavor symmetry breaking.
“…This value is in contrast to the experimentally still inaccurately determined mixing angle θ P , which has been subject of several investigations [1,2,3,4,5,6,7,8,9,10,11,12] and was found to be between −9 and −20…”
Abstract. The η ′ meson production in the reaction pp → ppη ′ has been studied at excess energies of Q = 26.5, 32.5 and 46.6 MeV using the internal beam facility COSY-11 at the cooler synchrotron COSY. The total cross sections as well as one angular distribution for the highest Q-value are presented. The excitation function of the near threshold data can be described by a pure s-wave phase space distribution with the inclusion of the proton-proton final state interaction and Coulomb effects. The obtained angular distribution of the η ′ mesons is also consistent with pure s-wave production.
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