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Centrality dependence of hadronization and chemical freeze-out conditions in heavy ion collisions at \sqrt s_{NN} = 2.76 TeV

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arxiv 1405.0710 v3 pith:BJG2Q5HJ submitted 2014-05-04 nucl-th hep-ph

classification nucl-thhep-ph
keywords centralitychemicalcollisionshadronizationmodeltemperaturedependencefreeze-out
verification ladder T0 review T1 audit T2 compute T3 formal

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We present an analysis of hadronic multiplicities measured in Pb-Pb collisions at \sqrt s_{NN} = 2.76 TeV as a function of the collision centrality within the statistical hadronization model. Evidence is found of a dependence of the chemical freeze-out temperature as a function of centrality, with a slow rise from central to peripheral collisions, which we interpret as an effect of post-hadronization inelastic scatterings. Using correction factors calculated by means of a simulation based on the UrQMD model, we are able to obtain a significant improvement in the statitical model fit quality and to reconstruct the primordial chemical equilibrium configuration. This is characterized by a nearly constant temperature of about 164 MeV which we interpret as the actual hadronization temperature.

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Cited by 4 Pith papers

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    Simulations show a peak in the proxy mass M_(d/2)K only when deuterons form by coalescence of protons from Λ(1520) decays, not in thermal models.

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    PYTHIA and Thermal FIST predict the same proton-deuteron balance scaling but differ sharply in its transverse-momentum dependence, so deuteron-triggered balance functions can in principle tell coalescence from statist...

  3. Kinetic freeze-out temperature from yields of short-lived resonances

    hep-ph 2019-08 conditional novelty 6.0 of 10

    The kinetic freeze-out temperature in Pb-Pb collisions at 2.76 TeV is extracted from ALICE yields of stable hadrons and short-lived resonances using a partial-chemical-equilibrium hadron resonance gas model, dropping ...

  4. What is the Quark-Gluon Plasma made of?

    nucl-th 2025-06 accept novelty 2.0 of 10

    The quark-gluon plasma is best described as a strongly coupled liquid of massive, very short-lived quark and gluon quasiparticles, with sound (phonon) modes becoming the most well-defined collective excitation at low momenta.

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