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Color Glass Condensate at the LHC: hadron multiplicities in $pp$, $pA$ and $AA$ collisions

Dmitri Kharzeev, Eugene Levin, Marzia Nardi

TL;DR

This paper develops predictions for hadron multiplicities at LHC energies within the Color Glass Condensate framework, emphasizing parton saturation via the saturation scale $Q_s$ as the controlling parameter. It combines a Glauber-based collision geometry with CGC-inspired gluon production, including running-coupling effects, to yield rapidity and centrality-dependent multiplicities for $pp$, $pA$, and $AA$ collisions. The authors fix the nonperturbative inputs using RHIC data and GW/BK/JIMWLK-inspired reasoning, and they provide quantified uncertainties, notably a relatively modest energy growth of multiplicities compared to many alternative models. Their results offer concrete, testable predictions for LHC measurements that can validate or constrain the CGC picture and $Q_s$ evolution, while highlighting larger uncertainties in proton-proton scenarios.

Abstract

We make quantitative predictions for the rapidity and centrality dependencies of hadron multiplicities in $AA$, $pA$ and $pp$ collisions at the LHC energies basing on the ideas of parton saturation in the Color Glass Condensate.

Color Glass Condensate at the LHC: hadron multiplicities in $pp$, $pA$ and $AA$ collisions

TL;DR

This paper develops predictions for hadron multiplicities at LHC energies within the Color Glass Condensate framework, emphasizing parton saturation via the saturation scale as the controlling parameter. It combines a Glauber-based collision geometry with CGC-inspired gluon production, including running-coupling effects, to yield rapidity and centrality-dependent multiplicities for , , and collisions. The authors fix the nonperturbative inputs using RHIC data and GW/BK/JIMWLK-inspired reasoning, and they provide quantified uncertainties, notably a relatively modest energy growth of multiplicities compared to many alternative models. Their results offer concrete, testable predictions for LHC measurements that can validate or constrain the CGC picture and evolution, while highlighting larger uncertainties in proton-proton scenarios.

Abstract

We make quantitative predictions for the rapidity and centrality dependencies of hadron multiplicities in , and collisions at the LHC energies basing on the ideas of parton saturation in the Color Glass Condensate.

Paper Structure

This paper contains 16 sections, 34 equations, 8 figures, 3 tables.

Figures (8)

  • Figure 1: The CGC approach for nucleus - nucleus collision with the saturation of parton density.
  • Figure 2: Rapidity dependence $dN/d\eta$ of charged hadron multiplicities in proton - proton (antiproton) collisions as a function of the pseudorapidity at different energies. The data are taken from Ref. RTABL.
  • Figure 3: Energy dependence of charged hadron multiplicity $dN/d\eta$ at $\eta =0$ in proton - proton (antiproton) collisions and of charged hadron multiplicities per participant pair $(2/N_{part})\,dN/d\eta$ at $\eta =0$ for central nucleus-nucleus collisions. The vertical dotted lines mark the LHC energies for nucleus-nucleus collisions ($W = 5500\,GeV$) and for proton-proton collisions ($W= 14000\,GeV$). collisions. The experimental data are from Ref. RTABLREF1.
  • Figure 4: Energy dependence of total multiplicity in proton - proton (antiproton) collisions. The vertical dotted line marks the LHC energies for proton-proton collisions ($W= 14000\,GeV$). collisions. The experimental data are taken from Ref. REF2.
  • Figure 5: Rapidity dependence of $d N/d \eta$ lead-lead collisions at the LHC energy at different centrality cuts. The solid lines corresponds to the prediction using Eq. (\ref{['QS']}) for the energy dependence of the saturation scale while the dotted lines show the predictions for Eq. (\ref{['QSRUNF']}) for running QCD coupling. The shadowed area shows the prediction for the minimal bias event.
  • ...and 3 more figures