Abstract

We calculate the polarization of prompt $\varUpsilon$($n$S) production in the improved color evaporation model at leading order employing the $k_T$-factorization approach. We present the polarization parameter $\lambda_\vartheta$ of prompt $\varUpsilon$($n$S) as a function of transverse momentum in $p+p$ and $p+\bar{p}$ collisions to compare with data in the helicity, Collins-Soper and Gottfried-Jackson frames. We also present calculations of the bottomonium production cross sections as a function of transverse momentum and rapidity. This is the first $p_T$-dependent calculation of bottomonium production and polarization in the improved color evaporation model. We find agreement with both bottomonium cross sections and polarization measurements.

Highlights

  • This paper is a continuation of our previous work [1] on quarkonium production and polarization in the improved color evaporation model using the kT-factorization approach

  • This paper is a continuation of that work where we extend our pT-dependent leading order (LO) ICEM calculation of quarkonium production and polarization in the kT-factorization approach to prompt ΥðnSÞ

  • We employ the scattering amplitudes calculated in Ref. [1] to compute the bbpartonic production cross section σ J;Jz according to the JP of each directly produced bottomonium state below the BBthreshold

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Summary

INTRODUCTION

This paper is a continuation of our previous work [1] on quarkonium production and polarization in the improved color evaporation model using the kT-factorization approach. We first developed our LO calculation of quarkonium polarization in the ICEM [2] in Refs. We performed the first pT-dependent polarization calculation in the ICEM [1] for prompt J=ψ production and polarization by employing the kT-factorization approach. This paper is a continuation of that work where we extend our pT-dependent leading order (LO) ICEM calculation of quarkonium production and polarization in the kT-factorization approach to prompt ΥðnSÞ. It assumed that no distinction is made between the spin states in the CEM

PRODUCTION OF POLARIZED
POLARIZATION OF PROMPT ΥðnSÞ
RESULTS
Unpolarized bottomonium production
Υð1SÞ pT distribution
Ratio of χ b2ð1PÞ to χ b1ð1PÞ production
ΥðnSÞ rapidity distribution
Frame dependence of λθ
CONCLUSIONS

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