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Statistical Model Predictions for p+p and Pb+Pb Collisions at LHC

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Presentation on theme: "Statistical Model Predictions for p+p and Pb+Pb Collisions at LHC"— Presentation transcript:

1 Statistical Model Predictions for p+p and Pb+Pb Collisions at LHC
Ingrid Kraus Nikhef and TU Darmstadt

2 Heavy Ion Collisions School, Erice, Sept 18, 2008
Outline Predictions for Pb+Pb collisions at LHC Extrapolation of thermal parameters, predictions Experimental observables for T and μB determination From Pb+Pb to p+p: system size dependence Model ansatz with correlated, equilibrated clusters Analysed data and results Predictions for p+p collisions at LHC Driven by initial or final state? Summary in Collaboration with H. Oeschler, K. Redlich, J. Cleymans, S. Wheaton Ingrid Kraus, Nikhef Heavy Ion Collisions School, Erice, Sept 18, 2008

3 Hadron ratios in the grand canonical ensemble
large systems, large number of produced hadrons two parameters describe particle ratios in the hadronic final state T, V, m T, Vb, Nb A. Andronic, P. Braun-Munzinger, J. Stachel, Nucl. Phys. A772 (2006) 167 Ingrid Kraus, Nikhef Heavy Ion Collisions School, Erice, Sept 18, 2008

4 Thermal Parameters in Pb+Pb
Phys. Rev. C 73(2006) On the freeze-out curve: TLHC ≈ TRHIC ≈ 170 MeV T ≤ TC ≈ 170 MeV μB from parametrised freeze-out curve: μB (√(sNN) = 5.5TeV) = 1 MeV Phys. Rev. C 73 (2006) Grand canonical ensemble for Pb+Pb predictions Ingrid Kraus, Nikhef Heavy Ion Collisions School, Erice, Sept 18, 2008

5 Heavy Ion Collisions School, Erice, Sept 18, 2008
Predictions for Pb+Pb Reliable for stable particles Benchmark for resonances Errors: T = 170 +/- 5 MeV μB = MeV Phys. Rev. C 74 (2006) - 1 All calculations with THERMUS hep-ph/ Ingrid Kraus, Nikhef Heavy Ion Collisions School, Erice, Sept 18, 2008

6 T and μB dependence I: h / h ratios
_ T and μB dependence I: h / h ratios Sensitive on μB determine μB from p/p weakly dep. on T _ Ingrid Kraus, Nikhef Heavy Ion Collisions School, Erice, Sept 18, 2008

7 T dependence: ratios with large Dm
Ratios with larger mass differences are more sensitive T from W / p and/or W / K Ingrid Kraus, Nikhef Heavy Ion Collisions School, Erice, Sept 18, 2008

8 T and μB dependence II: mixed ratios
Controlled by masses Weakly dep. on μB and T K/p not usable for T and mB determination good test of predictions Ingrid Kraus, Nikhef Heavy Ion Collisions School, Erice, Sept 18, 2008

9 Canonical suppression
Canonical ensemble small systems / peripheral collisions, low energies suppressed phase-space for particles related to conserved charges Stronger suppression for multi-strange hadrons Suppression depends on strangeness content, not difference Ingrid Kraus, Nikhef Heavy Ion Collisions School, Erice, Sept 18, 2008

10 Canonical suppression
Canonical ensemble small systems / peripheral collisions, low energies suppressed phase-space for particles related to conserved charges Stronger suppression for multi-strange hadrons Suppression depends on strangeness content, not difference Suppressed strangeness production beyond canonical suppression SPS √(sNN) = 17 AGeV Ingrid Kraus, Nikhef Heavy Ion Collisions School, Erice, Sept 18, 2008

11 Modification of the model
Statistical Model approach: T and μB Volume for yields → radius R used here Deviations: strangeness undersaturation factor gS Fit parameter Alternative: small clusters (RC) in fireball (R): RC ≤ R Chemical equilibrium in subvolumes: canonical suppression RC free parameter Study p+p, C+C, Si+Si, Pb+Pb / Au+Au collisions at SPS and RHIC energies R RC Ingrid Kraus, Nikhef Heavy Ion Collisions School, Erice, Sept 18, 2008

12 System size and energy dep. of cluster size
Small clusters in all systems Small system size dependence p+p energy dependence? Pb+Pb / Au+Au data consistent with saturated strangeness production p+p C+C Si+Si Pb/Au Ingrid Kraus, Nikhef Heavy Ion Collisions School, Erice, Sept 18, 2008

13 System size and energy dep. of cluster size
RC= R Pb+Pb Au+Au A+A: clusters smaller than fireball RC not well defined for RC ≥ 2 fm because suppression vanishes Ingrid Kraus, Nikhef Heavy Ion Collisions School, Erice, Sept 18, 2008

14 System size and energy dep. of cluster size
RC= R Pb+Pb Au+Au Particle ratios saturate at RC ≈ fm no precise determination for weak strangeness suppression Ingrid Kraus, Nikhef Heavy Ion Collisions School, Erice, Sept 18, 2008

15 Extrapolation to LHC: T - mB – systematics
Chemical decoupling conditions extracted from SIS up to RHIC feature common behavior Extrapolation to LHC energy with parametrisation e.g. Nucl. Phys. A 697 (2002) 902 Phys. Rev. C 73(2006) Ingrid Kraus, Nikhef Heavy Ion Collisions School, Erice, Sept 18, 2008

16 System size and energy dep. of T and mB
T, μB weakly dependent on system size p+p C+C Si+Si Pb/Au Ingrid Kraus, Nikhef Heavy Ion Collisions School, Erice, Sept 18, 2008

17 Extrapolation to LHC: cluster size
what defines RC in p+p? initial size of p+p system relevant RC const final state of large number of produced hadrons relevant RC increases with multiplicity Ingrid Kraus, Nikhef Heavy Ion Collisions School, Erice, Sept 18, 2008

18 Heavy Ion Collisions School, Erice, Sept 18, 2008
Prediction for p+p significant increase of ratios at RC ≈ 1.5 fm RC will be determined with ALICE data Ingrid Kraus, Nikhef Heavy Ion Collisions School, Erice, Sept 18, 2008

19 Heavy Ion Collisions School, Erice, Sept 18, 2008
Extraction of RC Sensitivity increases with strangeness difference RC from W / p hep-ph Ingrid Kraus, Nikhef Heavy Ion Collisions School, Erice, Sept 18, 2008

20 Heavy Ion Collisions School, Erice, Sept 18, 2008
W / p For Pb+Pb ratio was proposed as a measure of T but … Sensitivity on canonical suppression is much stronger than on T Ingrid Kraus, Nikhef Heavy Ion Collisions School, Erice, Sept 18, 2008

21 Heavy Ion Collisions School, Erice, Sept 18, 2008
Summary Pb+Pb predictions for particle ratios with extrapolated parameters T, μB T, μB determination with p / p and W / K or W / p ratios p+p predictions difficult due to unknown degree of canonical suppression Cluster radius RC from data _ Ingrid Kraus, Nikhef Heavy Ion Collisions School, Erice, Sept 18, 2008

22 Heavy Ion Collisions School, Erice, Sept 18, 2008
Data and fits Ingrid Kraus, Nikhef Heavy Ion Collisions School, Erice, Sept 18, 2008


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