Helicity Amplitude Analysis of e+e-→ψ(2S) →γχcJ→γΛ-Λ→γ pπ--pπ+
LIAO Guang-Rui1,2, PING Rong-Gang1, YANG Yong-Xu2
1Institute of High Energy Physics, Chinese Academy of Sciences, PO BOX 918(1), Beijing 1000492Department of Physics, Guangxi Normal University, Guilin 541004
Helicity Amplitude Analysis of e+e-→ψ(2S) →γχcJ→γΛ-Λ→γ pπ--pπ+
LIAO Guang-Rui1,2, PING Rong-Gang1, YANG Yong-Xu2
1Institute of High Energy Physics, Chinese Academy of Sciences, PO BOX 918(1), Beijing 1000492Department of Physics, Guangxi Normal University, Guilin 541004
摘要An analysis of the helicity amplitude is performed on the process e+e-→ψ(2S) →γχcJ→γΛ-Λ→γ pπ--pπ+. The joint angular distributions for each decay chain are given, and we focus on discussing the E1 contributions to ψ(2S) radiative decays, and the violation of the helicity selection rule in χcJ decays into hyperon pairs, together with the possibility of observing parity violation in successive hyperon decays.
Abstract:An analysis of the helicity amplitude is performed on the process e+e-→ψ(2S) →γχcJ→γΛ-Λ→γ pπ--pπ+. The joint angular distributions for each decay chain are given, and we focus on discussing the E1 contributions to ψ(2S) radiative decays, and the violation of the helicity selection rule in χcJ decays into hyperon pairs, together with the possibility of observing parity violation in successive hyperon decays.
[1] Karl G, Meshkov S and Rosner J L 1976 Phys. Rev. D 13 1203 Karl G, Meshkov S and Rosner J L 1980 Phys. Rev. Lett.45 215 Novikov V A et al 1978 Phys. Rep. 41 C 1 [2] Geffen D A and Wilson W 1980 Phys. Rev. Lett. 44 370. [3] Chauvat et al 1985 Phys. Lett 163 B 273 Asbyrt et al 1975 Nucl. Phys. B 99 30 [4] Brodsky S J and Lepage G P 1981 Phys. Rev. D 242848 [5] Chen H and Ping R G 2007 Phys. Rev. D 76036005 [6] Ablikim M, et al. (BES Collaboration) 2004 Phys.Rev. D 70 092004 [7] Karl G, Meshkov J and Rosner J L 1976 Phys. Rev. D 13 1203 [8] Particle Data Group 2008 Phys. Lett. B 667 1 [9] Bai J Z et al (BES Collaboration) 2003 Phys. Rev. D 67 112001