2015/05/31 by Qi-Li Liao, Yan Yu, Ya Deng +2 · 2 citations
Physics and Astronomy · #hep-ph
paper · pdf · doi:10.1103/physrevd.91.114030
published as Phys. Rev. D 91, 114030 (2015) · 10 pages, 13 figures. arXiv admin note: substantial text overlap with arXiv:1408.5563
arxiv created 2015/06/26 · arxiv updated 2015/07/01
We present a systematic study of the production of the heavy quarkonium, i.e., |(cc)[n] ⟩ , |(bc)[n] ⟩ (or |(cb)[n] ⟩), and |(bb)[n] ⟩ quarkonium [|(QQ')[n]⟩ quarkonium for short], through Z0 boson semi-exclusive decays with new parameters \citelx for the heavy quarkonium under the framework of the NRQCD, where [n] stands for n1S0, n3S1, n1P0, n3PJ (n=1, ⋯, 6; J=(0, 1, 2)). "Improved trace technology" is adopted to derive the simplified analytic expressions at the amplitude level, which shall be useful for dealing with these decay channels. If all higher |(QQ')[n]⟩ quarkonium states decay to the ground state |(QQ')[11S0]⟩ with 100% efficiency via electromagnetic or hadronic interactions, we obtain Γ(Z0→ |(cc)[11S0]⟩)=1476 KeV, Γ(Z0→ |(bc)[11S0]⟩)=1485 KeV, Γ(Z0→ |(bb)[11S0]⟩)=127.5 KeV. At the LHC and ILC with the luminosity \cal L∝ 1034cm-2s-1, sizable heavy quarkonium events can be produced through Z0 boson decays, i.e., about 5.9~×105 (cc), 6.0~×105 (bc) (or (cb)), 5.1~×104 (bb) events per year can be obtained.