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Double charm production e^+ e^- to J/psi + c bar{c} at B factories with next-to-leading order QCD corrections

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arxiv hep-ph/0611086 v4 pith:NEZABLMN submitted 2006-11-07 hep-ph hep-ex

Double charm production e^+ e^- to J/psi + c bar{c} at B factories with next-to-leading order QCD corrections

classification hep-ph hep-ex
keywords correctionsorderproductioncharmcontributionscrossdoublefactor
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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The inclusive $J/\psi$ production in $e^+ e^- \to J/\psi c\bar c$ at B factories is one of the most challenging open problems in heavy quarkonium physics. The observed cross section of this double charm production process is larger than existing leading order (LO) QCD predictions by a factor of 5. In the nonrelativistic QCD (NRQCD) factorization formalism, we calculate the next-to-leading order (NLO) QCD virtual and real corrections to this process, and find that these corrections can substantially enhance the cross section with a $K$ factor of about 1.8. We further take into account the feeddown contributions from higher charmonium states (mainly the $\psi(2S)$ as well as $\chi_{cJ}$) and the two-photon contributions, and find that the discrepancy between theory and experiment can be largely removed.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Revisiting relativistic corrections to inclusive $J/\psi$ production at B factories: Complete expansion for three-body quarkonium production

    hep-ph 2026-07 conditional novelty 6.0

    Full final-state kinematic expansion yields scheme-independent O(v²) corrections of about −14.6% (cc̄) and +12% (non-cc̄) for inclusive J/ψ at B factories, yet tension with Belle data remains.

  2. Semi-analytical results for $e^+e^-\to J/\psi + X_{{\rm non\,}c\bar{c}}$ up to $\mathcal{O}(\alpha_s v^2)$ at B factories

    hep-ph 2026-06 unverdicted novelty 6.0

    NRQCD calculation of O(α_s), O(v²) and first-time O(α_s v²) corrections to e⁺e⁻ → J/ψ + X_non c c̄, with r = m_c/√s expansions to r⁴⁰, yielding cross section 0.530 pb consistent with Belle but angular parameter deviating >2σ.