Abstract
We discuss prompt production of $J/\ensuremath{\psi}$ mesons in proton-proton collisions at the LHC within the NRQCD ${k}_{t}$-factorization approach using Kimber-Martin-Ryskin (KMR) unintegrated gluon distributions (UGDF). We include both direct color-singlet production ($gg\ensuremath{\rightarrow}J/\ensuremath{\psi}g$) as well as a feed down from ${\ensuremath{\chi}}_{c}\ensuremath{\rightarrow}J/\ensuremath{\psi}\ensuremath{\gamma}$ and ${\ensuremath{\psi}}^{\ensuremath{'}}\ensuremath{\rightarrow}J/\ensuremath{\psi}X$ decays. The production of the decaying mesons (${\ensuremath{\chi}}_{c}$ or ${\ensuremath{\psi}}^{\ensuremath{'}}$) is also calculated within the NRQCD ${k}_{t}$-factorization approach. The corresponding matrix elements for $gg\ensuremath{\rightarrow}J/\ensuremath{\psi}\text{ }\text{ }\mathrm{g}$, $gg\ensuremath{\rightarrow}{\ensuremath{\psi}}^{\ensuremath{'}}g$ and $gg\ensuremath{\rightarrow}{\ensuremath{\chi}}_{c}$ include parameters of the nonrelativistic space wave functions of the quarkonia at $r=0$, which are taken from potential models in the literature. We get the ratio of the corresponding cross section ratio for ${\ensuremath{\chi}}_{c}(2)$-to-${\ensuremath{\chi}}_{c}(1)$ at midrapidities much closer to experimental data than obtained in a recent analysis. Differential distributions in rapidity and transverse momentum of $J/\ensuremath{\psi}$ and ${\ensuremath{\psi}}^{\ensuremath{'}}$ are calculated and compared with experimental data of the ALICE and LHCb Collaborations. We discuss a possible onset of gluon saturation effects in the production of $J/\ensuremath{\psi}$ and ${\ensuremath{\chi}}_{c}$ mesons at forward/backward rapidities. We show that it is necessary to modify the standard KMR UGDF to describe ALICE and LHCb data. A mixed UGDF scenario was proposed. Then, we can describe the experimental data for $J/\ensuremath{\psi}$ production within model uncertainties with a color-singlet component only. Therefore, our theoretical results leave only relatively small room for the color-octet contributions. We discuss relations to other models in the literature. The results for the so-called hybrid model are compared to the results of the original ${k}_{t}$-factorization approach.
Highlights
There is a long-standing lack of convergence in understanding production of J/ψ quarkonia in proton-proton or proton-antiproton collisions
We have focused on the calculation of cross sections for inclusive prompt production of J/ψ and ψ0 in forward directions within the kt-factorization approach
NR QCD matrix elements were used with parameters of quarkonia ccwave functions at the origin taken from potential model(s)
Summary
There is a long-standing lack of convergence in understanding production of J/ψ quarkonia in proton-proton or proton-antiproton collisions. In a very recent kt-factorization analysis of χc production [1], the authors found very different values of the nonrelativistic wave function at the origin for χcð1Þ and χcð2Þ, jR0χcð1Þð0Þj2 ≈ 5jR0χcð2Þð0Þj2; ð1:1Þ from a fit based on the kt-factorization approach to LHC data. This large modification would put in doubt either the NRQCD approach and/or validity of the leading-order kt-factorization. The ψ0 quarkonium has a sizeable branching fraction into J/ψX [4] This contribution is much smaller than the direct one as is discussed in this paper. We expect that color-singlet contributions may dominate in this region of the phase space
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