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Relating high-energy lepton-hadron, proton-nucleus and nucleus-nucleus collisions through geometric scaling

Nestor Armesto, Carlos A. Salgado, Urs Achim Wiedemann

TL;DR

The empirical finding that the same A dependence accounts for the centrality evolution of the multiplicities measured in Au+Au collisions at RHIC and allows one to parametrize the high-p(t) particle suppression in d+AU collisions at forward rapidities is made.

Abstract

A characteristic feature of small-x lepton-proton data from HERA is geometric scaling -- the fact that over a wide range of x and Q^2 all data can be described by a single variable $Q^2/Q_{sat}^2(x)$, with all x-dependence encoded in the so-called saturation momentum $Q_{sat}(x)$. Here, we observe that the same scaling ansatz accounts for nuclear photoabsorption cross sections and favors the nuclear dependence $Q_{sat,A}^2\propto A^αQ_{sat}^2$, $α\simeq 4/9$. We then make the empirical finding that the same A-dependence accounts for the centrality evolution of the multiplicities measured in Au+Au collisions at RHIC. It also allows to parametrize the high-p_t particle suppression in d+Au collisions at forward rapidities. If these geometric scaling properties have a common dynamical origin, then this A-dependence of $Q_{sat,A}^2$ should emerge as a consequence of the underlying dynamical model.

Relating high-energy lepton-hadron, proton-nucleus and nucleus-nucleus collisions through geometric scaling

TL;DR

The empirical finding that the same A dependence accounts for the centrality evolution of the multiplicities measured in Au+Au collisions at RHIC and allows one to parametrize the high-p(t) particle suppression in d+AU collisions at forward rapidities is made.

Abstract

A characteristic feature of small-x lepton-proton data from HERA is geometric scaling -- the fact that over a wide range of x and Q^2 all data can be described by a single variable , with all x-dependence encoded in the so-called saturation momentum . Here, we observe that the same scaling ansatz accounts for nuclear photoabsorption cross sections and favors the nuclear dependence , . We then make the empirical finding that the same A-dependence accounts for the centrality evolution of the multiplicities measured in Au+Au collisions at RHIC. It also allows to parametrize the high-p_t particle suppression in d+Au collisions at forward rapidities. If these geometric scaling properties have a common dynamical origin, then this A-dependence of should emerge as a consequence of the underlying dynamical model.

Paper Structure

This paper contains 11 equations, 3 figures.

Figures (3)

  • Figure 1: Geometric scaling for $\gamma^*p$ (upper panel, data from proton), $\gamma^*A$ (middle panel, data from Adams:1995isArneodo:1995cs) and the ratio of data for $\gamma^*A$ divided by the scaling curve (\ref{['eqscalf']}) (lower panel). Also shown in the lower panel are the data from Arneodo:1996rv for ratios over $C$.
  • Figure 2: Energy and centrality dependence of the multiplicity of charged particles in AuAu collisions (\ref{['eqmult']}) compared to PHOBOS data Back:2002uc. Also shown in the lower panel are the ${\bar{p}}p$ data protmult and results for $\sqrt{s}=$ 62.5 and 5500 GeV/A.
  • Figure 3: Normalized ratios of central and semi-central to peripheral dAu collisions measured by BRAHMS Arsene:2004ux compared to results from Eq. (\ref{['eqratpt']}). The bands represent the uncertainty in the determination of $N_{\rm coll}$Arsene:2004ux. Results for the same centrality classes at the LHC are given in the lower panel.