The decay ψ(3686) → γπ+π−π0 is studied using a sample of (2712.4 ± 14.3) × 10⁶ ψ(3686) events collected with the BESIII detector. The decay η(1405) → π+π−π0 is observed for the first time in ψ(3686) decays via the intermediate state f0(980), and the product branching fraction B(ψ(3686) → γη(1405)) × B(η(1405) → f0(980)π0) × B(f0(980) → π+π−) is determined to be (3.77 ± 0.43 ± 0.30) × 10⁻⁷, where the first uncertainty is statistical and the second is systematic. The branching fraction of the isospin-violating decay ψ(3686) → γf1(1285) → γf0(980)π0 → γπ+π−π0 is determined to be (7.36 ± 2.25 ± 2.36) × 10⁻⁸, with a statistical significance of 2.9σ. Since no ηc signal is evident in either the π+π−π0 or f0(980)π0 mass spectrum, upper limits are set at B(ψ(3686) → γηc) × B(ηc → π+π−π0) < 3.09 × 10⁻⁷ and B(ψ(3686) → γηc) × B(ηc → f0(980)π0) × B(f0(980) → π+π−) < 7.97 × 10⁻⁸ at the 90% confidence level, respectively

Observation of 𝜓⁡(3686) →𝛾⁢𝜂⁡(1405) via 𝜂⁡(1405) →𝑓0⁡(980)⁢𝜋0

Garzia, I.;Melendi, F.  M.;
2026

Abstract

The decay ψ(3686) → γπ+π−π0 is studied using a sample of (2712.4 ± 14.3) × 10⁶ ψ(3686) events collected with the BESIII detector. The decay η(1405) → π+π−π0 is observed for the first time in ψ(3686) decays via the intermediate state f0(980), and the product branching fraction B(ψ(3686) → γη(1405)) × B(η(1405) → f0(980)π0) × B(f0(980) → π+π−) is determined to be (3.77 ± 0.43 ± 0.30) × 10⁻⁷, where the first uncertainty is statistical and the second is systematic. The branching fraction of the isospin-violating decay ψ(3686) → γf1(1285) → γf0(980)π0 → γπ+π−π0 is determined to be (7.36 ± 2.25 ± 2.36) × 10⁻⁸, with a statistical significance of 2.9σ. Since no ηc signal is evident in either the π+π−π0 or f0(980)π0 mass spectrum, upper limits are set at B(ψ(3686) → γηc) × B(ηc → π+π−π0) < 3.09 × 10⁻⁷ and B(ψ(3686) → γηc) × B(ηc → f0(980)π0) × B(f0(980) → π+π−) < 7.97 × 10⁻⁸ at the 90% confidence level, respectively
2026
Ablikim, M.; Achasov, M.  n.; Adlarson, P.; Ai, X.  c.; Aliberti, R.; Amoroso, A.; An, Q.; Bai, Y.; Bakina, O.; Ban, Y.; Bao, H. -R.; Batozskaya, V.; ...espandi
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11392/2634891
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