Abstract

We discuss gluon-gluon mechanisms for production of mesons with hidden strangeness, such as $\eta'$ and $\phi$ meson, in proton-proton collisions at large energies. The $g^* g^* \to \eta'$ and $g^* g^* \to \phi g$ mechanisms are considered only and the corresponding cross sections are calculated in the $k_t$-factorization approach. The $F_{\gamma^* \gamma^* \to \eta'}$ and $F_{g^* g^* \to \eta'}$ form factors are calculated from quark-antiquark $\eta'$ light-cone wave function including quark/antiquark transverse momenta. The result for two-photon transition form factor demonstrates that higher twists may survive even to large photon virtualities. The result is compared with the result of a recent leading-twist NLO analysis which uses phenomenological distribution amplitudes fitted to exclusive production of $\eta'$ in $e^+ e^- \to e^+ e^- \eta'$ reaction. We calculate transverse momentum distributions of both $\eta'$ and $\phi$ mesons in proton-proton collisions for RHIC and LHC energies. The results are compared to experimental data whenever available. The results of the Lund string model are shown for comparison for $\eta'$ production at LHC energies. It seems that the two-gluon fusion is not the dominant mechanism for both $\phi$ and $\eta'$ production, although the situation for $\eta'$, especially at larger energies, is less clear due to lack of experimental data.

Highlights

  • The mechanism of the particle production in protonproton collisions was studied continously for five decades

  • The result of calculation is below the experimental data. This suggests that the gluongluon fusion is not the dominant production mechanism of φ meson production

  • The fragmentation mechanism is considered in Refs. [34,35], and it may be the dominant mechanism of φ meson production

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Summary

INTRODUCTION

The mechanism of the particle production in protonproton collisions was studied continously for five decades. Quarkonium production at high energies is studied considering the two-gluon process. The situation with hidden strangeness mesons was not discussed carefully in the literature. We wish to explore whether the two-gluon fusion may be an important production mechanism. The presence of the two-gluon component in η0 may be relevant in the context of its production in the hadronic reaction. The gluon content in a meson may occur, e.g., via mixing with glueballs. Mixing of scalar glueball with the scalar-isoscalar “quarkonia” was discussed, e.g., in Ref. A low mass pseudoscalar glueball is discussed in Ref. The hadronization process for η0 production has not been discussed carefully in the literature. We shall discuss possible consequences of the gluonic component in η0 for its production in protonproton collisions. We shall compare our results with both experimental data as well as with results of the Lund string model

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