By analyzing existing data on pseudoscalar charmonium decays,we obtain the ratio of the branching fractions of η_(c)(2S) and η_(c) decays into ten different final states with light hadrons.For the first time,we test...By analyzing existing data on pseudoscalar charmonium decays,we obtain the ratio of the branching fractions of η_(c)(2S) and η_(c) decays into ten different final states with light hadrons.For the first time,we test the two existing theoretical predictions of these decays and find that the experimental data are significantly different from both of them.The lack of observation of any decay mode with higher rate in η_(c)(2S)than in η_(c) decays suggests very unusual decay dynamics in pseudoscalar charmonium decays to be identified.We also report the first model-independent evaluation of the partial width of η_(c)(2S)→yy(2.21^(+0.88)_(-0.64)keV)and improve determination of that of η_(c)→yy(5.43^(+0.41)_(-0.38)KeV).The latter shows a tension with the most recent lattice QCD calculation.展开更多
基金Supported in part by National Key Research and Development Program of China(2020YFA0406301)National Natural Science Foundation of China(NSFC)(11961141012,11835012,11521505)。
文摘By analyzing existing data on pseudoscalar charmonium decays,we obtain the ratio of the branching fractions of η_(c)(2S) and η_(c) decays into ten different final states with light hadrons.For the first time,we test the two existing theoretical predictions of these decays and find that the experimental data are significantly different from both of them.The lack of observation of any decay mode with higher rate in η_(c)(2S)than in η_(c) decays suggests very unusual decay dynamics in pseudoscalar charmonium decays to be identified.We also report the first model-independent evaluation of the partial width of η_(c)(2S)→yy(2.21^(+0.88)_(-0.64)keV)and improve determination of that of η_(c)→yy(5.43^(+0.41)_(-0.38)KeV).The latter shows a tension with the most recent lattice QCD calculation.
