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Starting the Energy Scan - First Results from 62.4 GeV Au+Au Collisions

Starting the Energy Scan - First Results from 62.4 GeV Au+Au Collisions. Introduction. High p T . Bulk matter observations. Collective motion. Summary. The story so far.

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Starting the Energy Scan - First Results from 62.4 GeV Au+Au Collisions

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  1. Starting the Energy Scan - First Results from 62.4 GeV Au+Au Collisions • Introduction. • High pT. • Bulk matter observations. • Collective motion. • Summary

  2. The story so far. • We have discovered a strongly interacting medium with extremelyhigh energy density which cannot be described in terms of simple hadronic degrees of freedom. Phobos

  3. Nuclear modification factor at 200 GeV Charged Hadrons d2N/dpTd (Au+Au) RAA = NColld2N/dpTd (p+p) High pT suppression and loss of back-to-back signal inAu+Au but not ind+Au showed that effect due to Jet Quenching in final state NOT initial state parton saturation (GCG). BRAHMS Can we turn this effect off? Observed by all 4 experiments

  4. Need for an energy scan Varying the beam energy changes: • Initial state: sNN, Nbin/Npart, Qs(?) • System: , mB, Nch • Partonic: xT, dE/dx • Provide constraints on jet quenching models. • Study the excitation function of baryon transport. • Constrain models for hadron production at intermediate pT. Why 62.4 GeV? • Located (on log scale) mid-way between SPS and RHIC top energies. • Many reference data from ISR.

  5. Ncoll definition Au+Au b ~ 10.5 fm Glauber Monte Carlo Npart “Participants” Npart/2 ~ A L~A1/3 Ncoll= # of NN collisions:~A4/3 “Collisions” At 62.4 GeV Ncoll very different to 200 GeV

  6. First immediate result… Paddle Counter Signal top 50% of cross-section 200 GeV PHOBOS Preliminary 62.4 GeV Significant decrease in maximal multiplicity

  7. Charged hadron spectra and yields PHOBOS Expect 62.4 GeV fit into √s systematics

  8. Jet quenching predictions at 62.4 GeV I. Vitev nucl-th/0404052 Adil & Gyulassy nucl-th/0405036 RAA (p0) ~ 0.5 - 0.3 at pT = 4 GeV

  9. RAA charged particles same results from all 4 experiments BRAHMS Preliminary Maximum significantly higher than at 200 GeV. There is a suppression for most central data Similar shape evolution with centrality

  10. Universal centrality evolution? 62.4 GeV 200 GeV PHOBOS • But, varying the beam energy changes: • Initial state: sNN, Ncoll/Npart • System : , mB, Nch, • Partonic : xT, dE/dx • Energy-independent • Weak function of Npart, pT . • Use central A+A as denominator • Scale with 1/<Npart> • Allows comparison between different experiments nucl-ex/0405003

  11. PID spectra STAR Preliminary p BRAHMS Phenix preliminary p0 W- X-

  12. RAA for p0 for central data Predictions 0.3 - 0.5 at 4 GeV/c Again maximum > 200 GeV STAR Preliminary Charged ISR reference used for p0 Still discrepancy between charged and p0 Large baryon contribution up to at least 4 GeV/c

  13. Rcp of baryons and mesons Stat. Errors Only STAR preliminary STAR Preliminary (stat. errors only) The RCP(baryon) > RCP(meson) at intermediate pT. Problem with limited statistics.

  14. Again, large proton contribution at intermediate pT Small difference as function of centrality (not very peripheral 30-60%) Baryon/meson ratios STAR Preliminary Lessp in central collisions at 62.4 GeV Ratios factor 2-3 higher than in p+p at pT= 2-4 GeV

  15. Ratios at mid-rapidity Clear systematic trend with collision energy Minbias (0-80%) 62.4 GeV STAR Preliminary Stat. Errors Only STAR Preliminary L/L -/ +: 1.017±0.002 K-/K+: 0.835±0.006 p/p: 0.458±0.005 confirm varying y same effect as varying √s. Ratios flat as function of pT

  16. Statistical model results Close to net-baryon free Tch flat with centrality ● p, K,p ● p, K,p ● p, K,p, L, X ● p, K,p, L, X Close to chem. equilibrium ! STAR preliminary Au+Au at √sNN=200GeV and 62 GeV TLQCD~160-170MeV TLQCD~160-170MeV Energy dependence but small Nch dependence…

  17. (In)dependence of mid-rapidity yields Preliminary Preliminary • T, µB, and V all vary with energy, but in such a way as to ensureyields stay ~constant Preliminary

  18. Radial flow Blastwave fit Shape of the mT spectrum depends on mass: Tch Radial flow! p K p STAR Preliminary STAR Preliminary STAR Preliminary Same flow as at 200 GeV

  19. Kaon Slopes Top 5% central collisions

  20. HBT probes space-time evolution of system and system size at freeze-out. Studies at √s=130, 200 GeV yielded similar HBT radii to SPS energies (“HBT puzzle”). Severe challenge to hydrodynamic calculations. At an intermediate energy, a larger expansion time might point to a long-lived mixed phase.  interferometry PRELIMINARY Systematics of central 0-5% Fully consistent Coulomb treatment in kT dependence same results from PHOBOS

  21. HBT from SPS to RHIC No sign of qualitatively different expansion dynamics at 62 GeV. Continues to be a severe challenge submitted to Phys. Rev. C Rapid Communications Same results from STAR

  22. Charged particle correlations PHENIX PRELIMINARY PHENIX PRELIMINARY pT Substantialsignals attributable to elliptic flow (v2 = <cos(2f)>) v2 apparently saturates and is the same as at 200 GeV Jets are going to be a challenge

  23. Longitudinal elliptic flow h’=|h|-ybeam Longitudinal scaling of v2 nucl-ex/0406021

  24. Identified Elliptic Flow sNN = 62.4 GeV Au+Au centrality : 0-84% sNN = 200 GeV Au+Au centrality : 0-92% v2 v2 stat. error only sys. error <15% stat. error only sys. error <20% Charged p,K,p : PRL91, 182301 (2003) p0 : work in progress PHENIX preliminary pT [GeV/c] pT [GeV/c] Although statistics not great again resembles 200 GeV

  25. Quark coalescence? 62.4 GeV Au+Au: PHENIX preliminary 200 GeV Au+Au, charged p,K,p : from PRL p0 : work in progress stat. error only sys. error <20% (62GeV) 15% (200GeV) Coalescence at intermediate pT leads to: v2 /nquark The scaling works as for 200 GeV Au+Au Seems to be slightly lower than 200 GeV for pT/nquark<1 GeV/c pT /nquark [GeV/c]

  26. Summary Many of the results indicate environment similar at 62.4 GeV to 200 GeV but it’s notidentical • Initial energy density lower • Evidence of jet quenching Cronin effect is stronger • HBT radii at ~6 fm • Chemical freeze-out conditions similar to 200 GeV (fn Nch) Baryon chemical potential much higher • Radial flow as strong as at 200 GeV (fn Nch) • Elliptic flow as strong as at 200 GeV (fncentrality) Consistent with Nquark scaling • Elliptic flow appears universal at forward rapidities • Jet contribution much weaker than at 200 GeV As yet un-answered questions: Are the gluon densities the same in both systems? Do they spend the same amount of time in each stage? i.e. do they reach the same freeze-out conditions in the same manner?

  27. back up

  28. Why an energy scan? Varying the beam energy changes: • Initial state: sNN, Ncoll/Npart, Qs(?) • System: , mB, Nch • Partonic: xT, dE/dx Varying the geometry (A,b): • jet quenching • vary overall path length • vary asymmetry • Elliptic (and directed) flow • Study A dependence at fixed eccentricity. Npart eccentricity

  29. p+p references +/-25% uncertainty p0reference p0reference chargedreference

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