Utilizing 2712.4 ±14.3 million 𝜓(3686) events accumulated by the BESIII experiment, we perform a partial wave analysis of 𝜓(3686) →𝛾𝜒𝑐𝐽 →𝛾ΛΛbar decay (𝐽 =0, 1, 2). The ratio of the helicity amplitudes with same (++) and opposite (+-) helicity for 𝜒𝑐2 →ΛΛbar decay is determined for the first time to be 𝑅𝜒𝑐2 =0.575 ±0.048 ±0.018, with a relative phase angle ΔΦ𝜒𝑐2 =0.37 ±0.15 ±0.05 rad. The parameters of the angular distribution of 𝜒𝑐2 are determined to be 𝛼𝜒𝑐2 =−0.211 ±0.100 ±0.050 and 𝛽𝜒𝑐2 =−0.039 ±0.089 ±0.033, based on the distribution 𝑑𝑁/𝑑cos𝜃 =1 +𝛼𝜒𝑐2cos2𝜃 +𝛽𝜒𝑐2cos4𝜃. The width of 𝜒𝑐0 is determined to be 12.31 ±0.26 ±0.12 MeV. Additionally, the branching fractions for 𝜒𝑐𝐽 →ΛΛbar are measured to be (3.662 ±0.048 ±0.111) ×10−4, (1.182 ±0.026 ±0.042) ×10−4, and (1.704 ±0.035 ±0.057) ×10−4 for 𝜒𝑐0, 𝜒𝑐1 and 𝜒𝑐2, respectively, where the first uncertainty is statistical and the second systematic.
Helicity amplitude and branching fraction measurement of χ cJ → ΛΛbar
Garzia, I.;Melendi, F. M.;
2026
Abstract
Utilizing 2712.4 ±14.3 million 𝜓(3686) events accumulated by the BESIII experiment, we perform a partial wave analysis of 𝜓(3686) →𝛾𝜒𝑐𝐽 →𝛾ΛΛbar decay (𝐽 =0, 1, 2). The ratio of the helicity amplitudes with same (++) and opposite (+-) helicity for 𝜒𝑐2 →ΛΛbar decay is determined for the first time to be 𝑅𝜒𝑐2 =0.575 ±0.048 ±0.018, with a relative phase angle ΔΦ𝜒𝑐2 =0.37 ±0.15 ±0.05 rad. The parameters of the angular distribution of 𝜒𝑐2 are determined to be 𝛼𝜒𝑐2 =−0.211 ±0.100 ±0.050 and 𝛽𝜒𝑐2 =−0.039 ±0.089 ±0.033, based on the distribution 𝑑𝑁/𝑑cos𝜃 =1 +𝛼𝜒𝑐2cos2𝜃 +𝛽𝜒𝑐2cos4𝜃. The width of 𝜒𝑐0 is determined to be 12.31 ±0.26 ±0.12 MeV. Additionally, the branching fractions for 𝜒𝑐𝐽 →ΛΛbar are measured to be (3.662 ±0.048 ±0.111) ×10−4, (1.182 ±0.026 ±0.042) ×10−4, and (1.704 ±0.035 ±0.057) ×10−4 for 𝜒𝑐0, 𝜒𝑐1 and 𝜒𝑐2, respectively, where the first uncertainty is statistical and the second systematic.I documenti in SFERA sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.


