Observation of resonance structures in $e^+e^-\to Ï^+Ï^-Ï_2(3823)$ and mass measurement of $Ï_2(3823)$
arXiv:2203.05815 · doi:10.1103/PhysRevLett.129.102003
Abstract
Using a data sample corresponding to an integrated luminosity of 11.3 $\rm fb^{-1}$ collected at center-of-mass energies from $4.23$ to $4.70$ GeV with the BESIII detector, we measure the product of the $e^+e^-\to Ï^+Ï^-Ï_2(3823)$ cross section and the branching fraction $\mathcal{B}[Ï_2(3823)\to γÏ_{c1}]$. For the first time, resonance structure is observed in the cross section line shape of $e^+e^-\to Ï^+Ï^-Ï_2(3823)$ with significances exceeding $5Ï$. A fit to data with two coherent Breit-Wigner resonances modeling the $\sqrt{s}$-dependent cross section yields $M(R_1)=4406.9\pm 17.2\pm 4.5$ MeV/$c^2$, $Î(R_1)=128.1\pm 37.2\pm 2.3$ MeV, and $M(R_2)=4647.9\pm 8.6\pm 0.8$ MeV/$c^2$, $Î(R_2)=33.1\pm 18.6\pm 4.1$ MeV. Though weakly disfavored by the data, a single resonance with $M(R)=4417.5\pm26.2\pm3.5$ MeV/$c^2$, $Î(R)=245\pm48\pm13$ MeV is also possible to interpret data. This observation deepens our understanding of the nature of the vector charmoniumlike states. The mass of the $Ï_2(3823)$ state is measured as $(3823.12\pm 0.43\pm 0.13)$ MeV/$c^2$, which is the most precise measurement to date.
8 pages, 2 figures, Published in Phys. Rev. Lett