Abstract
We investigate the \( \mathcal{O}\left( {{\alpha_s}} \right) \) corrections to e + e − → J/ψ(ψ′) + χ cJ (J =0, 1, 2) in the NRQCD factorization approach. These next-to-leading order (NLO) corrections are calculated at the level of helicity amplitude. We have made a detailed analysis for both polarized and unpolarized cross sections, and compared our predictions with the measurements at the B factories. We also derive the asymptotic expressions for each of the NLO helicity amplitudes, and confirm the earlier speculation that at NLO in α s , the double logarithm of type \( {\ln^2}\left( {{{s} \left/ {{m_c^2}} \right.}} \right) \) appearing in the NRQCD short-distance coefficient is always associated with the helicity-suppressed channels.
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ArXiv ePrint: 1107.4351
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Dong, HR., Feng, F. & Jia, Y. \( \mathcal{O}\left( {{\alpha_s}} \right) \) corrections to J/ψ + χ cJ production at B factories. J. High Energ. Phys. 2011, 141 (2011). https://doi.org/10.1007/JHEP10(2011)141
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DOI: https://doi.org/10.1007/JHEP10(2011)141