TY - JOUR
T1 - First Observation of a Three-Resonance Structure in 𝑒+𝑒−→Nonopen Charm Hadrons
AU - The BESIII collaboration
AU - Ablikim, M.
AU - Achasov, M.N.
AU - Adlarson, P.
AU - Aliberti, R.
AU - Calcaterra, A.
AU - Begzsuren, K.
AU - Holtmann, T.
AU - Kavatsyuk, Myroslav
AU - Kalantar-Nayestanaki, Nasser
AU - Kappert, Rosa
AU - Messchendorp, Johan
AU - Rodin, Viktor
PY - 2024/5/9
Y1 - 2024/5/9
N2 - We report the measurement of the inclusive cross sections for 𝑒+𝑒−→nOCH (where nOCH denotes non-open charm hadrons) with improved precision at center-of-mass (c.m.) energies from 3.645 to 3.871 GeV. We observe three resonances: ℛ(3760), ℛ(3780), and ℛ(3810) with significances of 8.1𝜎, 13.7𝜎, and 8.8𝜎, respectively. The ℛ(3810) state is observed for the first time, while the ℛ(3760) and ℛ(3780) states are observed for the first time in the nOCH cross sections. Two sets of resonance parameters describe the energy-dependent line shape of the cross sections well. In set I [set II], the ℛ(3810) state has mass (3805.7±1.1±2.7) [(3805.7±1.1±2.7)] MeV/𝑐2, total width (11.6±2.9±1.9) [(11.5±2.8±1.9)] MeV, and an electronic width multiplied by the nOCH decay branching fraction of (10.9±3.8±2.5) [(11.0±3.4±2.5)] eV. In addition, we measure the branching fractions ℬ[ℛ(3760)→nOCH]=(25.2±16.1±30.4)%[(6.4±4.8±7.7)%] and ℬ[ℛ(3780)→nOCH]=(12.3±6.6±8.3)%[(10.4±4.8±7.0)%] for the first time. The ℛ(3760) state can be interpreted as an open-charm (OC) molecular state, but containing a simple four-quark state component. The ℛ(3810) state can be interpreted as a hadrocharmonium state.
AB - We report the measurement of the inclusive cross sections for 𝑒+𝑒−→nOCH (where nOCH denotes non-open charm hadrons) with improved precision at center-of-mass (c.m.) energies from 3.645 to 3.871 GeV. We observe three resonances: ℛ(3760), ℛ(3780), and ℛ(3810) with significances of 8.1𝜎, 13.7𝜎, and 8.8𝜎, respectively. The ℛ(3810) state is observed for the first time, while the ℛ(3760) and ℛ(3780) states are observed for the first time in the nOCH cross sections. Two sets of resonance parameters describe the energy-dependent line shape of the cross sections well. In set I [set II], the ℛ(3810) state has mass (3805.7±1.1±2.7) [(3805.7±1.1±2.7)] MeV/𝑐2, total width (11.6±2.9±1.9) [(11.5±2.8±1.9)] MeV, and an electronic width multiplied by the nOCH decay branching fraction of (10.9±3.8±2.5) [(11.0±3.4±2.5)] eV. In addition, we measure the branching fractions ℬ[ℛ(3760)→nOCH]=(25.2±16.1±30.4)%[(6.4±4.8±7.7)%] and ℬ[ℛ(3780)→nOCH]=(12.3±6.6±8.3)%[(10.4±4.8±7.0)%] for the first time. The ℛ(3760) state can be interpreted as an open-charm (OC) molecular state, but containing a simple four-quark state component. The ℛ(3810) state can be interpreted as a hadrocharmonium state.
U2 - 10.1103/PhysRevLett.132.191902
DO - 10.1103/PhysRevLett.132.191902
M3 - Article
SN - 0031-9007
VL - 132
JO - Physical Review Letters
JF - Physical Review Letters
IS - 19
M1 - 191902
ER -