학술논문

Measurement of $$J/\psi $$ J / ψ decays into final states $$2(\pi ^{+}\pi ^{-})\pi ^{0},K^{+}K^{-}\pi ^{+}\pi ^{-}\pi ^{0},\,2(\pi ^{+}\pi ^{-})$$ 2 ( π + π - ) π 0 , K + K - π + π - π 0 , 2 ( π + π - ) and $$K^{+}K^{-}\pi ^{+}\pi ^{-}$$ K + K - π + π
Document Type
article
Author
V. V. AnashinO. V. AnchugovV. M. AulchenkoE. M. BaldinG. N. BaranovA. K. BarladyanA. Yu. BarnyakovM. Yu. BarnyakovS. E. BaruI. Yu. BasokA. M. BatrakovE. A. BekhtenevA. E. BlinovV. E. BlinovA. V. BobrovV. S. BobrovnikovA. V. BogomyagkovA. E. BondarA. R. BuzykaevP. B. CheblakovV. L. DorohovS. I. EidelmanS. A. GlukhovD. N. GrigorievV. V. KaminskiyS. E. KarnaevG. V. KarpovS. V. KarpovK. Yu. KarukinaD. P. KashtankinA. A. KatsinT. A. KharlamovaV. A. KiselevV. V. KolmogorovS. A. KononovK. Yu. KotovA. A. KrasnovE. A. KravchenkoV. N. KudryavtsevV. F. KulikovE. A. KuperG. Ya. KurkinI. A. KuyanovE. B. LevichevD. A. MaksimovV. M. MalyshevA. L. MaslennikovO. I. MeshkovS. I. MishnevI. A. MorozovI. I. MorozovN. Yu. MuchnoiV. V. NeufeldS. A. NikitinI. B. NikolaevI. N. OkunevA. P. OnuchinS. B. OreshkinA. A. OsipovI. V. OvtinS. V. PeleganchukV. V. PetrovP. A. PiminovS. G. PivovarovV. G. PrisekinO. L. RezanovaA. A. RubanV. K. SandyrevG. A. SavinovA. G. ShamovD. N. ShatilovL. I. ShekhtmanD. A. ShvedovB. A. ShwartzE. A. SimonovS. V. SinyatkinA. N. SkrinskyA. V. SokolovE. V. StarostinaD. P. SukhanovA. M. SukharevA. A. TalyshevV. A. TayurskyV. I. TelnovYu. A. TikhonovK. Yu. TodyshevA. G. TribendisG. M. TumaikinYu. V. UsovA. I. VorobiovV. N. ZhilichA. A. ZhukovV. V. ZhulanovA. N. Zhuravlev
Source
European Physical Journal C: Particles and Fields, Vol 82, Iss 10, Pp 1-11 (2022)
Subject
Astrophysics
QB460-466
Nuclear and particle physics. Atomic energy. Radioactivity
QC770-798
Language
English
ISSN
1434-6052
Abstract
Abstract Using the 1.32 $$\hbox {pb}^{-1}$$ pb - 1 statistics collected at the $$J/\psi $$ J / ψ peak with the KEDR detector at the VEPP-4M $$e^{+}e^{-\, }$$ e + e - collider, we measured the branching fractions of $$J/\psi $$ J / ψ meson decays to the final states 2( $$\pi ^{+}\pi ^{-})\pi ^{0}$$ π + π - ) π 0 , $$K^{+}K^{-}\pi ^{+}\pi ^{-}\pi ^{0}$$ K + K - π + π - π 0 , 2( $$\pi ^{+}\pi ^{-})$$ π + π - ) and $$K^{+}K^{-}\pi ^{+}\pi ^{-}$$ K + K - π + π - . The results obtained for the decays $$J/\psi \rightarrow $$ J / ψ → 2( $$\pi ^{+}\pi ^{-})\pi ^{0}$$ π + π - ) π 0 , $$J/\psi \rightarrow K^{+}K^{-}\pi ^{+}\pi ^{-}\pi ^{0}$$ J / ψ → K + K - π + π - π 0 contradict the measurements performed by other groups in the last century, but agree well with recent results of BABAR and BESIII collaborations.