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08 December 2021
 
  » arxiv » nucl-ex/0602018

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Rapidity dependence of high p_T suppression at sqrt{s_{NN}}=62.4{GeV}
I. Arsene ; I. G. Bearden ; D. Beavis ; C. Besliu ; B. Budick ; H. Bøggild ; C. Chasman ; C. H. Christensen ; P. Christiansen ; J. Cibor ; R. Debbe ; E. Enger ; J. J. Gaardhøje ; K. Hagel ; H. Ito ; A. Jipa ; F. Jundt ; E.B. Johnson ; J. I. Jørdre ; C. E. Jørgensen ; R. Karabowicz ; E. J. Kim ; T. Kozik ; T. M. Larsen ; J. H. Lee ; Y. K. Lee ; S. Lindal ; R. Lystad ; G. Løvhøiden ; Z. Majka ; M. Mikelsen ; M. Murray ; J. Natowitz ; B. Neumann ; B. S. Nielsen ; D. Ouerdane ; R. Planeta ; F. Ramiires ; C. Ristea ; O. Ristea ; D. R{ö}hrich ; B. H. Samset ; D. Sandberg ; S. J. Sanders ; R. A. Scheetz ; P. Staszel ; T. S. Tveter ; F. Videbæk ; R. Wada ; Z. Yin ; H. Yang ; I. S. Zgura ; PostScript ; PDF ; Other formats ; SLAC-SPIRES HEP ; to ; by ;
Date 17 Feb 2006
AbstractWe present measurements of charged hadron p_T spectra from Au+Au collisions at sqrt(snn)=62.4 GeV for pseudorapidities eta=0, eta=1 and eta=3.2. Around midrapidity (eta=0, eta=1) we find nuclear modification factors at levels suggesting a smaller degree of high p_T suppression than in the same reaction at higher energy sqrt(snn)=200 GeV. At the high pseudorapidity, eta=3.2, where nuclear modification factors cannot be constructed due to the lack of p+p reference data, we find a significant reduction of R_{CP} (central to peripheral ratio) as compared to midrapidity.
Source arXiv, nucl-ex/0602018
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