Thermal Model at RHIC: Multiple Sources Analysis
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Investigating if there is one thermal source or many at RHIC using a grand canonical ensemble and multiple sources concept to describe quark mixtures. Analyzing rapidity dependence of temperature and chemical potential. Conclusions drawn from fitting data to theoretical model.
Thermal Model at RHIC: Multiple Sources Analysis
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Presentation Transcript
Is there one thermal source or many @ RHIC I.G. Bearden7, D. Beavis1, C. Besliu10, Y. Blyakhman6, J.Brzychczyk4, B. Budick6, H. Bøggild7 ,C. Chasman1, C. H. Christensen7, P. Christiansen7,J.Cibor4, R.Debbe1, J. J. Gaardhøje7,M. Germinario7,K. Grotowski4 , K. Hagel8, O. Hansen7, B. Harris11 , A.K. Holme12, H. Ito11, E. Jacobsen7, A. Jipa10, J. I. Jordre10, F. Jundt2, C.E.Jørgensen7, T. Keutgen9, E. J. Kim5, T. Kozik3, T.M.Larsen12, J. H. Lee1, Y. K.Lee5, G. Løvhøjden2, Z. Majka3, A. Makeev8, B. McBreen1, M. Murray11, J. Natowitz8, B.S.Nielsen7, K. Olchanski1, D. Ouerdane7, R.Planeta4, F. Rami2, D. Roehrich9, B. H. Samset12, S. J. Sanders11, I. S. Sgura10, R.A.Sheetz1, Z.Sosin3, P. Staszel7, T.S. Tveter12, F.Videbæk1, R. Wada8 and A.Wieloch3 1BNL, 2Strasbourg,3Jagiellonian University,, 4INP, Krakov, 5Johns Hopkins, 6CUNY 7Niels Bohr,8Texas A&M, 9Bergen, 10Bucharest,11Kansas,12 Oslo Michael Murray University of Kansas
95° 30° 2.3° 30° 15° The BRAHMS Experiment Michael Murray University of Kansas
Thermal Model (Becattini) • Use a grand-cononical ensemble to describe the mixture of u,d and s quarks. • Conserve strangeness & electic charge • Hadronization based on quark ratios • Include weak decays of all resonances. Michael Murray University of Kansas
Minimze 2 by searching over B and T 2 Michael Murray University of Kansas
Rapidity Dependence of Temperature and Chemical Potential Michael Murray University of Kansas
Picture will be clearer when final data are used Fit to dN/dy and volume directly Use a grid that extends to T=185MeV or so. Thermal model with multiple sources gives a reasonable description of our data. This hints that strangeness is locally conserved Temperature and µB increase with rapidity. Conclusions Michael Murray University of Kansas