# Polarization of prompt $J/\psi$ and $\Upsilon$(1S) production in the color evaporation model

## TL;DR

This paper calculates the polarization of prompt $J/\psi$ and $\Upsilon$(1S) production in proton-proton and fixed-target collisions using the color evaporation model, providing predictions and comparisons with experimental data.

## Contribution

It presents the first leading-order polarization calculations for prompt $J/\psi$ and $\Upsilon$(1S) within the color evaporation model, including energy and rapidity dependence.

## Key findings

- Prompt $J/\psi$ and $\Upsilon$(1S) are longitudinally polarized at high energies.
- Polarization varies with rapidity, becoming transverse at forward rapidities.
- Model predictions align with some experimental results and provide new predictions for future tests.

## Abstract

We calculate the polarization of prompt $J/\psi$ and $\Upsilon$(1S) production using the color evaporation model at leading order. We present the polarization parameter $\lambda_\vartheta$ as a function of center of mass energy and rapidity in $p+p$ collisions. We also compare the $x_F$ dependence to experimental results in $p$+Cu and $\pi$+W collisions, and predict the $x_F$ dependence in $p$+Pb collisions at fixed-target energies. At energies far above the $Q\overline{Q}$ production threshold, we find the prompt $J/\psi$ and $\Upsilon$(1S) production to be longitudinally polarized with $\lambda_\vartheta^{J/\psi}=-0.51^{+0.05}_{-0.16}$ and $\lambda_\vartheta^{\Upsilon \rm{(1S)}}=-0.69^{+0.03}_{-0.02}$. Both prompt $J/\psi$ and prompt $\Upsilon$(1S) are also longitudinally polarized at central rapidity, becoming transversely polarized at the most forward rapidities.