Energy Dependence of Intrinsic Charm Production: What is the Best Energy for Observation?

TL;DR

This paper investigates the energy dependence of intrinsic charm production in high-energy collisions, combining perturbative QCD with intrinsic charm models to identify optimal energies for experimental observation.

Contribution

It introduces a comprehensive calculation of $J/eta$ and $ar D$ meson production incorporating intrinsic charm and cold nuclear matter effects, highlighting the best energy range for detection.

Findings

Good agreement with fixed-target data when including intrinsic charm.

Intrinsic charm signal is strongest at midrapidity for low-energy fixed target experiments.

Provides predictions for $J/\psi$ and $\bar D$ meson distributions across energies.

Abstract

Background: A nonperturbative charm production contribution, known as intrinsic charm, was predicted in the early 1980s. Recent results have provided new evidence for its existence but further confirmation is needed. Purpose: $J/\psi$ and $\bar D$ meson production are calculated with a combination of perturbative QCD and intrinsic charm to determine the best energy range to study intrinsic charm production. Methods: $J/\psi$ and $\bar D$ meson production are calculated in perturbative QCD to next-to-leading order in the cross section. Cold nuclear matter effects, including nuclear modification of the parton densities and $p_T$ broadening by multiple scattering are taken into account in the production of both; absorption by nucleons is also included for the $J/\psi$. Contributions from intrinsic charm are calculated assuming production from a $|uud c \bar c \rangle$ Fock state. Results: The $J/\psi$ and $\bar D$ meson rapidity and $p_T$ distributions are calculated as a function of rapidity and transverse momentum $p_T$ over a wide range of center-of-mass energies with and without intrinsic charm in $p+p$ collisions. The nuclear modification factor, $R_{pA}$, is also calculated for $p+{\rm Pb}$ interactions at appropriate energies. Previous fixed-target data as a function of Feynman $x$, $x_F$, are also compared to calculations within the approach. Good agreement with the data is found when intrinsic charm is included. Conclusions: The intrinsic charm signal may be largest at midrapidity for future low energy fixed target experiments such as the proposed NA60+.