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Fully charm tetraquark production at hadronic collisions with gluon radiation effects

Yefan Wang, Ruilin Zhu

Abstract

We have performed, for the first time, a complete next-to-leading order QCD calculation for processes involving fully charm tetraquark states, revealing that the renormalization constant of the color-singlet four charm quark operator is exactly unity at this order. By resumming over various gluon radiation effects, we have improved the precision of their hadroproduction cross-section to the order of ${\cal O}(α_s^5)$. Through symmetry analysis, we investigated the possible quark configurations of the fully charm tetraquark and expanded its states in the color symmetry-antisymmetry basis. By combining LHCb data on the total cross section of the exotic hadron X(6900) and CMS measurements of its spin-parity, we extracted the non-perturbative but universal long-distance matrix elements. The rapidity and transverse momentum distributions are also predicted, which await further experimental verification.

Fully charm tetraquark production at hadronic collisions with gluon radiation effects

Abstract

We have performed, for the first time, a complete next-to-leading order QCD calculation for processes involving fully charm tetraquark states, revealing that the renormalization constant of the color-singlet four charm quark operator is exactly unity at this order. By resumming over various gluon radiation effects, we have improved the precision of their hadroproduction cross-section to the order of . Through symmetry analysis, we investigated the possible quark configurations of the fully charm tetraquark and expanded its states in the color symmetry-antisymmetry basis. By combining LHCb data on the total cross section of the exotic hadron X(6900) and CMS measurements of its spin-parity, we extracted the non-perturbative but universal long-distance matrix elements. The rapidity and transverse momentum distributions are also predicted, which await further experimental verification.

Paper Structure

This paper contains 14 equations, 5 figures.

Figures (5)

  • Figure 1: Typical Feynman diagrams for the gluon-gluon fusion to fully charm tetraquark up to NLO. The thick black lines stand for the massive charm quarks. The Feynman diagrams from the quark-antiquark annihilation or (anti)quark-gluon scattering can be plotted similarly.
  • Figure 2: NLO cross-section results for the fully charm tetraquark dependence on the hadron-hadron center-of-mass energy $\sqrt{S}$. $X(6900)$ is assumed to be $2^{++}$ and its $0^{++}$ partner is also plotted. The comparison with three choices of renormalization and factorization scales are given.
  • Figure 3: NLO differential cross-sections for the fully charm tetraquark with different quark configurations dependence on the rapidity $y$.
  • Figure 4: NLO and Resum(NLO after resummation) differential cross-sections for the fully charm tetraquark with different quark configurations dependence on the transverse momentum $P_\perp$.
  • Figure 5: Distribution of the polar angle $\theta^{\prime *}$ between the $J/\psi$ and the fully charm tetraquark momenta. The CMS 25 data is from the very recent measurement by the CMS experiment CMS:2025fpt.