Production of Excited Doubly Heavy Baryons at the Super-ZZ Factory

Abstract

In the framework of nonrelativistic QCD, the PP-wave excited doubly heavy baryons are thoroughly studied via the channel e+eβˆ’β†’βŸ¨QQβ€²βŸ©[n]β†’ΞžQQβ€²+Qβ€²Λ‰+QΛ‰e^{+} e^{-}\rightarrow \langle QQ^{\prime}\rangle[n] \rightarrow \Xi_{QQ^{\prime}} +\bar{Q^{\prime}} +\bar{Q}, which takes place at the collision energy ZZ-pole. Q(β€²)Q^{(\prime)} represents bb or cc quark for the production of Ξcc\Xi_{cc}, Ξbc\Xi_{bc}, and Ξbb\Xi_{bb}, respectively. All of the intermediate diquark states ⟨QQβ€²βŸ©[n]\langle QQ'\rangle[n] in PP-wave, ⟨cc⟩[1P1]3Λ‰\langle cc\rangle[^{1}P_{1}]_{\mathbf{\bar 3}}, ⟨cc⟩[3PJ]6\langle cc\rangle[^{3}P_{J}]_{\mathbf{6}}, ⟨bc⟩[1P1]3Λ‰/6\langle bc\rangle[^{1}P_{1}]_{\mathbf{\bar 3}/ \mathbf{6}}, ⟨bc⟩[3PJ]3Λ‰/6\langle bc\rangle[^{3}P_{J}]_{\mathbf{\bar 3}/ \mathbf{6}}, ⟨bb⟩[1P1]3Λ‰\langle bb \rangle[^{1}P_{1}]_{\mathbf{\bar 3}}, and ⟨bb⟩[3PJ]6\langle bb\rangle[^{3}P_{J}]_{\mathbf{6}} with J=0J=0, 1, or 2, are taken into account. The cross sections and differential distributions, including the transverse momentum, rapidity, angular, and invariant mass, are discussed for the excited baryons production. The result is that the contributions of Ξcc\Xi_{cc}, Ξbc\Xi_{bc}, and Ξbb\Xi_{bb} in PP-wave are found to be 3.97%\%, 5.08%\%, and 5.89%\%, respectively, compared to SS-wave. Supposing that all PP-wave excited states can decay into the ground state 100\%, the total events NΞcc=8.48Γ—104βˆ’6N_{\Xi_{cc}}=8.48 \times10^{4-6}, NΞbc=2.26Γ—105βˆ’7N_{\Xi_{bc}}=2.26\times10^{5-7}, and NΞbb=4.12Γ—103βˆ’5N_{\Xi_{bb}}=4.12 \times10^{3-5} would be produced at the Super-ZZ Factory with a high luminosity up to L≃1034βˆ’36cmβˆ’2sβˆ’1{\cal L} \simeq 10^{34-36}{\rm cm}^{-2} {\rm s}^{-1}.Comment: 13 pages, 4 figures, 4 table

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