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Prompt charmonia hadroproduction in High Energy Factorization with tree-level NLO corrections

A. A. Prokhorov, S. P. Baranov, A. V. Lipatov, M. A. Malyshev

Oct 21, 2026arXiv:2610.29297v1
hep-ph
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Scorecard· 16/16
4.0/10 impact

Competent, comprehensive but incremental extension of the authors' own NLO† kT-factorization scheme to J/ψ and ηc, with niche impact and mediocre fit quality on several datasets.

Abstract

We consider prompt J/ψJ/ψ, χcJχ_{cJ} and ηcη_c production in high energy pppp collisions in the framework of non-relativistic QCD. We apply high-energy factorization with taking into account tree-level next-to-leading order corrections to the production amplitudes. Using several CCFM-evolved gluon densities in the proton and a previously proposed matching scheme to merge the leading and higher-order contributions, we extract the long-distance matrix elements for the entire charmonium family from a simultaneous fit to available LHC data. We provide predictions for the transverse momentum spectra and relative production rates σ(ψ′)/σ(J/ψ)σ(ψ^\prime)/σ(J/ψ) and σ(χcJ)/σ(J/ψ)σ(χ_{cJ})/σ(J/ψ) and find them to be in good agreement with the LHC data within the theoretical and experimental uncertainties across a wide kinematic region. We demonstrate that taking into account the tree-level NLO corrections improves the global description of the data.

AI Impact Assessments

(1 model)

Paper type: Phenomenological, empirical fit. It applies an existing theoretical framework (kT-factorization + NRQCD + the NLO† merging scheme) to a broad dataset.

Core Contribution

The paper extends the authors' earlier NLO† scheme, which merges tree-level 2→1 and 2→2 off-shell amplitudes with a double-counting-exclusion cut, from ψ′ and χcJ to prompt J/ψ and ηc. It fits color-octet LDMEs for the whole charmonium family to a large LHC dataset, about 983 J/ψ points and 59 χcJ points. The main technical devices are:

  • a two-step fit that avoids χ² bias from the dominant J/ψ data;
  • a linear combination of the 1S0[8] and 3P_J[8] LDMEs, which is needed because the two are strongly anticorrelated;
  • linear regression relations linking J/ψ direct and χcJ feed-down contributions;
  • HQSS relations used to predict ηc parameter-free;
  • an alternative scenario with independent |R′χc1|² and |R′χc2|².
  • The headline physics findings are:

  • Tree-level NLO† corrections improve the global description relative to LO.
  • Allowing HQSS violation in the χc1/χc2 wave functions describes σ(χc2)/σ(χc1) well. The required violation is about ±50%, well beyond expected O(v²) corrections, though NLO† reduces it by up to a factor of two relative to LO.
  • ηc production at LHCb is overestimated, which confirms the known ηc/HQSS puzzle. The paper also notes a discrepancy between the two LHCb 13 TeV analyses.
  • Methodological Rigor

    Strengths:

  • Very broad dataset: 11 J/ψ datasets spanning 5–13 TeV and central and forward rapidity.
  • Two CCFM gluon densities (A0 and JH'2013 set 2).
  • Theory uncertainty bands that include the soft-gluon-energy and renormalization scale variations.
  • ψ′/J/ψ ratios used as an out-of-fit validation.
  • Weaknesses:

  • χ²/n.d.f. for J/ψ is poor. It is 3.8 for A0 and 3.3 for JH'2013 after a pT>6 GeV cut. Individual datasets reach 12–18 (LHCb 5 TeV and 13 TeV, ATLAS 13 TeV, CMS 5 TeV).
  • The claim of "good agreement" rests on theory uncertainty bands, and the fit χ² uses experimental errors only.
  • The JH'2013 gluon requires a pT>6 GeV cut to match A0, which shows gluon-density dependence at low kT.
  • The χcJ fit has few points (59, or 50 after cuts) and many free parameters in the neq scenario. The χ²/n.d.f. values well below 1 (e.g. 0.07) suggest overfitting or overestimated errors.
  • The ad hoc rule of dropping the spin-alignment uncertainty for χc1+χc2 sums is an assumption.
  • The ηc "prediction" is not truly parameter-free. The authors choose ⟨Oηc(3S1[8])⟩=0 and ⟨Oηc(1P1[8])⟩=3⟨l.c.⟩ to improve agreement, so the ηc result is a conditional range, not a clean test.
  • The linear-combination and regression tricks hide the separate CO contributions, so the LDMEs are not individually extractable and are hard to compare with collinear NLO NRQCD fits.
  • The claim that NLO† improves on LO is shown mainly in Fig. 1, as χ² versus pT cutoff. A systematic LO-versus-NLO† comparison is limited, and the scheme depends on a model-dependent soft-gluon emission picture.
  • The polarization puzzle is not addressed here, though the paper is explicit about deferring it.
  • Potential Impact

    This is a specialized contribution within the small kT-factorization/CCFM quarkonium community, with some relevance to the NRQCD community more broadly. It provides a useful global LDME set within a framework that effectively resums high-energy logarithms and uses tree-level NLO amplitudes, which is an alternative to collinear NLO. The χc1/χc2 HQSS-violation finding and the ηc discrepancy feed ongoing debates (the heavy-quark spin symmetry puzzle). It is unlikely to change how the broader field approaches quarkonium production, since conclusions depend on the CCFM gluon choice and on the authors' soft-gluon model. Real-world application is minimal, beyond serving as input for Monte Carlo generators (CASCADE, PEGASUS) and for predictions at future colliders or in heavy-ion baselines.

    Timeliness

    Charmonium production remains an open issue. New LHC data (ATLAS 13 TeV 2024, LHCb ηc 2024) and the updated BESIII ηc→γγ width make a global reanalysis timely. The ηc data-tension observation is useful to experimentalists.

    Strengths

  • The most comprehensive simultaneous fit of the whole charmonium family within kT-factorization.
  • A transparent discussion of limitations, including the ηc and HQSS tensions.
  • Consistent reuse of an established scheme.
  • Flags the inconsistency between the LHCb ηc measurements.
  • Limitations

  • Incremental over the authors' own prior papers (2024 and 2025). The new elements are the J/ψ and ηc application and the combined fit.
  • High χ² on key datasets, and a gluon-density-dependent low-pT cut.
  • Model-dependent soft-gluon treatment.
  • The "NLO" corrections are only tree-level real emission, with no loop corrections.
  • Inherently limited reach beyond a niche community.
  • No public code or data table is mentioned. The inputs are public, but the amplitude calculation is complex, so replication is difficult.
  • Overall: A solid but incremental phenomenology paper of modest, niche impact.

    Rating:4/ 10
    Significance 3.5Rigor 5Novelty 3.5Clarity 6

    Generated Oct 22, 2026

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