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Observation of ηc(1S,2S) and χcJ decays to 2(π+π−)η via ψ(3686) radiative transitions. / The BESIII Collaboration ; Николаев, Иван Борисович; Мучной, Николай Юрьевич.
в: Physical Review D, Том 111, № 5, 052013, 31.03.2025.Результаты исследований: Научные публикации в периодических изданиях › статья › Рецензирование
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TY - JOUR
T1 - Observation of ηc(1S,2S) and χcJ decays to 2(π+π−)η via ψ(3686) radiative transitions
AU - BESIII Collaboration
AU - Achasov, M. n.
AU - Aliberti, R.
AU - Николаев, Иван Борисович
AU - Мучной, Николай Юрьевич
N1 - Observation of ηc(1S,2S) and χcJ decays to 2(π+π−)η via ψ(3686) radiative transitions / M. Ablikim, M. N. Achasov, P. Adlarson [et al.] // Physical Review D. – 2025. – Vol. 111, No. 5. – P. 052013. – DOI 10.1103/physrevd.111.052013.
PY - 2025/3/31
Y1 - 2025/3/31
N2 - Based on (2712.4±14.1)×106 ψ(3686) decays collected with the BESIII detector, we have observed, for the first time, the hadronic decays of S- and P-wave charmonium states into 2(π+π-)η via radiative transitions from ψ(3686). The branching fraction of the decay ηc(1S)→2(π+π-)η has a significant dependence on the interference pattern between ηc(1S) and non-ηc(1S) processes. We measure it in both the destructive and constructive interference scenarios for the first time. The mass and width of the ηc(1S) are measured to be M=(2984.14±0.13±0.38) MeV/c2 and Γ=(28.82±0.11±0.82) MeV, respectively. Clear signals for the decays of the χcJ(J=0,1,2) and the ηc(2S) to 2(π+π-)η are also observed for the first time, and the corresponding branching fractions are measured. The ratio of the branching fractions between the ηc(2S) and ηc(1S) decays is significantly lower than the theoretical prediction, which might suggest different dynamics in their decays.
AB - Based on (2712.4±14.1)×106 ψ(3686) decays collected with the BESIII detector, we have observed, for the first time, the hadronic decays of S- and P-wave charmonium states into 2(π+π-)η via radiative transitions from ψ(3686). The branching fraction of the decay ηc(1S)→2(π+π-)η has a significant dependence on the interference pattern between ηc(1S) and non-ηc(1S) processes. We measure it in both the destructive and constructive interference scenarios for the first time. The mass and width of the ηc(1S) are measured to be M=(2984.14±0.13±0.38) MeV/c2 and Γ=(28.82±0.11±0.82) MeV, respectively. Clear signals for the decays of the χcJ(J=0,1,2) and the ηc(2S) to 2(π+π-)η are also observed for the first time, and the corresponding branching fractions are measured. The ratio of the branching fractions between the ηc(2S) and ηc(1S) decays is significantly lower than the theoretical prediction, which might suggest different dynamics in their decays.
UR - https://www.scopus.com/record/display.uri?eid=2-s2.0-105003753552&origin=inward&txGid=5bc16dc43739d8775b93a6fb285aa9ef
UR - https://elibrary.ru/item.asp?id=82015402
UR - https://www.mendeley.com/catalogue/cfc44b42-9a77-319e-850a-1d2d2bbf63d2/
U2 - 10.1103/PhysRevD.111.052013
DO - 10.1103/PhysRevD.111.052013
M3 - Article
VL - 111
JO - Physical Review D
JF - Physical Review D
SN - 2470-0010
IS - 5
M1 - 052013
ER -
ID: 66126275