We report an observation of the process Jpsi --> gamma X(1835) -->amma K0S K0S eta at low K0SK0S mass with a statistical significance larger than 12.9 sigma using a data sample of 1.31 x 10^9 Jpsi events collected with the BESIII detector. In this region of phase space the K0SK0S system is dominantly produced through the f0(980). By performing a partial wave analysis, we determine the spin parity of the X(1835) to be JPC= 0-+. The mass and width of the observed X(1835) are 1844 ± 9(stat)+16-25(syst) MeV/c2 and 192+20-17(stat)+62-43(syst) MeV, respectively, which are consistent with the results obtained by BESIII in the channel Jpsi --> gamma pi+pi-eta'.
Observation and spin-parity determination of the X(1835) in Jpsi --> gamma K0S K0S eta
Garzia, I.;
2015
Abstract
We report an observation of the process Jpsi --> gamma X(1835) -->amma K0S K0S eta at low K0SK0S mass with a statistical significance larger than 12.9 sigma using a data sample of 1.31 x 10^9 Jpsi events collected with the BESIII detector. In this region of phase space the K0SK0S system is dominantly produced through the f0(980). By performing a partial wave analysis, we determine the spin parity of the X(1835) to be JPC= 0-+. The mass and width of the observed X(1835) are 1844 ± 9(stat)+16-25(syst) MeV/c2 and 192+20-17(stat)+62-43(syst) MeV, respectively, which are consistent with the results obtained by BESIII in the channel Jpsi --> gamma pi+pi-eta'.File | Dimensione | Formato | |
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2015.observation and spin-parity.pdf
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PhysRevLett.115.091803-accepted.pdf
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