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2011 QCD and High Energy Interactions - Rencontres de Moriond ...

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EPOS 2 <strong>and</strong> LHC Results<br />

TanguyPierog (1) , Iu.Karpenko (2,3) , <strong>and</strong> K.Werner (3)<br />

(1) Karlsruhe Institut of Technology, Institut für Kernphysik, Postfach 3640, 76021 Karlsruhe Germany<br />

(2) Bogolyubov Institute for Theoretical Physics, Kiev 143, 03680, Ukraine<br />

(3) SUBATECH, University of Nantes – IN2P3/CNRS– EMN, Nantes, France<br />

To study the effects related to the formation of a Quark-Gluon-Plasma in heavy ion collisions,<br />

the proton-proton collisions are usually used as a reference. If this approach seems to be valid<br />

at RHIC or for very high transverse momentum at LHC, it might be different at intermediate<br />

pt for LHC energies, where some collective effects might be visible already in pp data (ridge,...).<br />

Within a global mo<strong>de</strong>l such as EPOS 2, where light <strong>and</strong> heavy systems are treated using the<br />

same physics, we can test the collective effects both in pp <strong>and</strong> lead-lead collisions at LHC. In<br />

this paper, it will be shown that the collective effect are not negligible already for pp at LHC.<br />

1 Introduction<br />

The CMS collaboration published recently results 1 on two particle correlations in ∆η <strong>and</strong> ∆φ,<br />

in pp scattering at 7 TeV. Most remarkable is the discovery of a ridge-like structure around<br />

∆η = 0, exten<strong>de</strong>d over many units in ∆η, referred to as “the ridge”, in high multiplicity pp<br />

events. A similar structure has been observed in heavy ion collisions at RHIC, <strong>and</strong> there is little<br />

doubt that the phenomenon is related to the hydrodynamical evolution of matter. This “fluid<br />

dynamical behavior” is actually consi<strong>de</strong>red to be the major discovery at RHIC 2 .<br />

1.5<br />

0.5<br />

-0.5<br />

∆φ<br />

R( ∆η,<br />

∆φ)<br />

1<br />

0<br />

4<br />

3<br />

2<br />

1<br />

0<br />

-1<br />

-3<br />

-2<br />

-1<br />

0<br />

1<br />

2<br />

3<br />

∆η<br />

R( ∆η,<br />

∆φ)<br />

Figure 1: (Color online) Two particle correlation function R versus ∆η <strong>and</strong> ∆φ for high multiplicity events in pp<br />

collisions at 7 TeV, as obtained from a hydrodynamical evolution based on flux tube initial conditions (lefth<strong>and</strong>si<strong>de</strong>).<br />

On the righth<strong>and</strong>-si<strong>de</strong> the calculation is done without hydro evolution .i.e. particle production directly<br />

from string (flux tube) <strong>de</strong>cay.We consi<strong>de</strong>r particles with pt between 1 <strong>and</strong> 3 GeV/c.<br />

So does pp scattering provi<strong>de</strong> as well a liquid, just ten times smaller than a heavy ion<br />

1.5<br />

∆φ<br />

1<br />

0.5<br />

0<br />

-0.5<br />

4<br />

3<br />

2<br />

1<br />

0<br />

-1<br />

-3 -2<br />

-1<br />

0<br />

1<br />

2<br />

3<br />

∆η

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