Using a sample of (10087±44)×106 J/ψ events accumulated with the BESIII detector, we analyze the decays η→π+π-l+l-(l=e or μ) via the process J/ψ→γη. The branching fraction of η→π+π-e+e-is measured to be B(η→π+π-e+e-)=(3.07±0.12stat±0.19syst)×10-4. No signal events are observed for the η→π+π-μ+μ-decay, leading to an upper limit on the branching fraction of B(η→π+π-μ+μ-)<4.0×10-7 at the 90% confidence level. Furthermore, the CP-violation asymmetry parameter is found to be ACP(η→π+π-e+e-)=(-4.04±4.69stat±0.14syst)%, showing no evidence of CP-violation with current statistics. Additionally, we extract the transition form factor from the decay amplitude of η→π+π-e+e-. Finally, axionlike particles are searched for via the decay η→π+π-A,a→e+e-, and upper limits on this branching fraction relative to that of η→π+π-e+e-are presented as a function of the axionlike particle mass in the range 5-200 MeV/c2.
Study of η →π+π-l+l-
Garzia, I.;
2025
Abstract
Using a sample of (10087±44)×106 J/ψ events accumulated with the BESIII detector, we analyze the decays η→π+π-l+l-(l=e or μ) via the process J/ψ→γη. The branching fraction of η→π+π-e+e-is measured to be B(η→π+π-e+e-)=(3.07±0.12stat±0.19syst)×10-4. No signal events are observed for the η→π+π-μ+μ-decay, leading to an upper limit on the branching fraction of B(η→π+π-μ+μ-)<4.0×10-7 at the 90% confidence level. Furthermore, the CP-violation asymmetry parameter is found to be ACP(η→π+π-e+e-)=(-4.04±4.69stat±0.14syst)%, showing no evidence of CP-violation with current statistics. Additionally, we extract the transition form factor from the decay amplitude of η→π+π-e+e-. Finally, axionlike particles are searched for via the decay η→π+π-A,a→e+e-, and upper limits on this branching fraction relative to that of η→π+π-e+e-are presented as a function of the axionlike particle mass in the range 5-200 MeV/c2.| File | Dimensione | Formato | |
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PhysRevD.111.072008.pdf
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