The production of J/ψ and Υ mesons in pp collisions at √ s = 8 TeV is studied with the LHCb detector. The J/ψ and Υ mesons are reconstructed in the µ + µ − decay mode and the signal yields are determined with a fit to the µ + µ − invariant mass distributions. The analysis is performed in the rapidity range 2.0 < y < 4.5 and transverse momentum range 0 < p T < 14 (15) GeV/c of the J/ψ (Υ ) mesons. The J/ψ and Υ production crosssections and the fraction of J/ψ mesons from b-hadron decays are measured as a function of the meson p T and y. The LHCb collaboration 27
IntroductionSuccessfully describing heavy quarkonium production is a long-standing problem in QCD. An effective field theory, non-relativistic QCD (NRQCD) [1,2], provides the foundation for much of the current theoretical work. According to NRQCD, the production of heavy quarkonium factorises into two steps: a heavy quark-antiquark pair is first created at short distances and subsequently evolves non-perturbatively into quarkonium at long distances. The NRQCD calculations depend on the colour-singlet (CS) and colour-octet (CO) matrix elements, which account for the probability of a heavy quark-antiquark pair in a particular colour state to evolve into a heavy quarkonium state. The CS model (CSM) [3,4], which provides a leading-order description of quarkonium production, was initially used to describe experimental data. However, it underestimates the observed cross-section for single J/ψ production at high transverse momentum (p T ) at the Tevatron [5]. To resolve this discrepancy, the CO mechanism was introduced [6]. The corresponding matrix elements were determined from the high-p T data, as the CO cross-section decreases more slowly with p T than that predicted by CS. More recent higher-order calculations [7][8][9][10] close the gap between the CS predictions and the experimental data [11], reducing the need for large CO contributions.