Nu Xu1/35 RNC Meeting, Berkeley, February 21, 2012 Beam Energy Scan at RHIC - A status report from STAR Nu Xu (1) Nuclear Science Division, Lawrence Berkeley National Laboratory, USA (2) College of Physical Science & Technology, Central China Normal University, China

Nu Xu2/35 RNC Meeting, Berkeley, February 21, 2012 QCD in Twenty-One Century (1)Higgs Particle – - Origin of Mass - SM  The Theory (2) QCD Phase Structure – - Critical point, phase boundaries - Confinement - χ C symmetry - Nucleon helicity structure - … - Non-linear QCD at small-x - … - Emerging properties of QCD

2 T E, Quarkyonic RHIC, SPS, FAIR 1 T ini, T C LHC, RHIC 3 Phase Boundary RHIC, FAIR, NICA The QCD Phase Diagram and High-Energy Nuclear Collisions 1 2 3

Nu Xu4/35 RNC Meeting, Berkeley, February 21, 2012 Phase Diagram: Water Phase diagram: A map shows that, at given degrees of freedom, how matter organize itself under external conditions. Water: H 2 O The QCD phase diagram: structure of matter with quark- and gluon-degrees (color degrees) of freedom.

Nu Xu5/35 RNC Meeting, Berkeley, February 21, 2012 QCD Phase Diagram (2010) Experiments: Systematic measurements (E beam, A size ) : extract numbers that are related to the phase diagram K. Fukushima and T. Hatsuda, Rept. Prog. Phys. 74, (2011); arXiv:

Nu Xu6/35 RNC Meeting, Berkeley, February 21, 2012 Outline (1) Introduction (2) Recent Results and Beam Energy Scan at RHIC (3) Summary and Outlook

Nu Xu7/35 RNC Meeting, Berkeley, February 21, 2012 BNL PAC, , 2010 *Heavy Flavor Tracker (HFT) 2013 *Time Projection Chamber (TPC) FGT 2011 STAR Detectors Fast and Full azimuthal particle identification EMC+EEMC+FMS (-1 ≤  ≤ 4) MRPC Time Of Flight DAQ1000 MTD 2013

Nu Xu8/35 RNC Meeting, Berkeley, February 21, 2012 Particle Identification at STAR STAR TPC STAR ToF STAR EMC STAR HFT Neutral particles Strange Jets Heavy Quark hyperons Hadrons Multiple-fold correlations for both HI and Spin physics! e, μ π K p d TPC ToF TPC Log 10 (p) STAR MTD

PID: (π ±, K ±, p) from Au+Au Collisions at 7.7, 39, 200 GeV Au+Au at 7.7 GeV Au+Au at 39 GeV Au+Au at 200 GeV

Nu Xu10/35 RNC Meeting, Berkeley, February 21, 2012 STAR Physics Focus Polarized p+p program - Study proton intrinsic properties Forward program - Study low-x properties, initial condition, search for CGC - Study elastic and inelastic processes in pp2pp 1) At 200 GeV at RHIC - Study medium properties, EoS - pQCD in hot and dense medium 2) RHIC beam energy scan (BES) - Search for the QCD critical point - Chiral symmetry restoration eRHIC (eSTAR) eRHIC (eSTAR)

Nu Xu11/35 RNC Meeting, Berkeley, February 21, 2012 STAR Di-electron Program Bulk-penetrating probe ~ 270M events 1)Reasonable agreement between data and cocktail. No dramatic enhancement in the low mass region: - η, ω, J/ψ from PHENIX - π 0, ( π ±) ϕ, from STAR - ρ contribution not included 2) Topics – the centrality dependence of: - slope parameter vs. mass - v 2 (p T ) vs. mass - R AA (p T ) vs. mass - spin-alignment vs. mass

Nu Xu12/35 RNC Meeting, Berkeley, February 21, 2012 y x pypy pxpx coordinate-space-anisotropy  momentum-space-anisotropy Anisotropy Parameter v 2 Initial/final conditions, EoS, degrees of freedom

Nu Xu13/35 RNC Meeting, Berkeley, February 21, 2012 Low p T (≤ 2 GeV/c): hydrodynamic mass ordering High p T (> 2 GeV/c): number of quarks scaling  Partonic Collectivity, necessary for QGP!  De-confinement in Au+Au collisions at RHIC! Partonic Collectivity at RHIC STAR: preliminary QM09: arXiv

Nu Xu14/35 RNC Meeting, Berkeley, February 21, 2012 Comparison with Model Results  Small value of specific viscosity over entropy η/s  Model uncertainty dominated by initial eccentricity ε Model: Song et al. arXiv:

Nu Xu15/35 RNC Meeting, Berkeley, February 21, 2012 Low η/s for QCD Matter at RHIC 1) η/s ≥ 1/4π 2) η/s(QCD matter) < η/s(QED matter) RHIC results

Nu Xu16/35 RNC Meeting, Berkeley, February 21, 2012 Antimatter Discoveries at RHIC “Observation of the Antimatter Helium-4 Nucleus” by STAR Collaboration Nature, 473, 353(2011). April, 2011March, 2010 “Observation of an Antimatter Hypernucleus” by STAR Collaboration Science, 328, 58(2010).

Nu Xu17/35 RNC Meeting, Berkeley, February 21, 2012 Light Nuclei Productions at RHIC Production rate reduces by a factor of 1.6x10 3 (1.1x10 3 ) for each additional antinucleon added to the antinucleus (nucleus). STAR Experiment: Nature, 473, 353(2011), Top 100 by Discover Magazine 1)In high-energy nuclear collisions, N(d) >> N(α): QGP  (anti)light nuclei via coalescence 2)In the Universe, N(d) << N(α): N(anti-α)?

Nu Xu18/35 RNC Meeting, Berkeley, February 21, 2012 Beam Energy Scan at RHIC Observations: (1) Azimuthally HBT 1st order phase transition (2) Directed flow v 1 1st order phase transition (3) Dynamical correlations partonic vs. hadronic dof (4) v 2 - NCQ scaling partonic vs. hadronic dof (5) Fluctuations Critical point, correl. length - /public/sn arXiv: Study QCD Phase Structure - Signals of phase boundary - Signals for critical point

Nu Xu19/35 RNC Meeting, Berkeley, February 21, 2012 Bulk Properties at Freeze-out Kinetic Freeze-out: - Central collisions => lower value of T kin and larger collectivity β - Little energy dependence. Chemical Freeze-out: - Central collisions => higher values of T ch and μ B ! - The effect is stronger at lower energy.

Nu Xu20/35 RNC Meeting, Berkeley, February 21, 2012 Azimuthally Sensitive HBT vs. √s NN Freeze-out eccentricity w.r.t reaction plane: E895: PLB 496 (2000) 1 CERES: PRC 78 (2008) STAR: PRL 93 (2004) From √s NN = GeV, smooth trend observed for the freeze-out eccentricity ε f.o., as predicted by the transport model URQMD.

Nu Xu21/35 RNC Meeting, Berkeley, February 21, 2012 Dynamical Correlations (II) E-by-E PID Yield Ratios Au + Au collisions at RHIC (1)Historical observable: Ratios of identified particle yields. (2)In the observed energy range: √s NN = GeV, both baryon/pion and Strangeness/pion ratios vary smoothly as predicted by the transport model URQMD. (3)No strong enhancement in the strangeness ratio in new data.

Nu Xu22/35 RNC Meeting, Berkeley, February 21, 2012 Directed Flow Rapidity y v1v1 Mid-y v 1 is sensitive to: - Nuclear stopping - The mixture of initial and produced particles - Equation of state (EOS) - L.P. Csernai, D. Rohrich, PLB458, 454(99) - J. Brachmann et al., PRC61, 24909(00) - R. Snellings, et al., PRL (00) - M. Bleicher and H. Stöcker, PLB526, 309(02)

Nu Xu23/35 RNC Meeting, Berkeley, February 21, 2012 Mid-y v 1 slope vs. √s NN Mid-y v 1 is sensitive to: - Nuclear stopping - The mixture of initial and produced particles - Equation of state (EOS) At low beam energy, initial nucleons are dominant, v 1 > 0, by definition At higher beam energies, produced particles dominate the dynamics. Due to expansion, the sign of v 1 reverses (1)The sign change occurs between √s NN = 7.7 and 11.5 GeV indicating the change in the EOS around these beam energies (2)Transport models can NOT reproduced the trend and change properly

Nu Xu24/35 RNC Meeting, Berkeley, February 21, 2012 Search for Local Parity Violation in High Energy Nuclear Collisions The separation between the same-charge and opposite- charge correlations. - Strong external EM field - De-confinement and Chiral symmetry restoration L or B Voloshin, PR C62, (00). STAR; PRL103, (09); (PRC). Parity even observable Future tests with Beam Energy dependence & U+U collisions

Nu Xu25/35 RNC Meeting, Berkeley, February 21, 2012 Dynamical Correlations (1)Below √s NN = 11.5 GeV, the splitting between the same- and opposite-sign charge pairs disappeared (2)If QGP is the source for the observed splitting at high-energy nuclear collisions  hadronic interactions become dominant at √s NN ≤ 11.5 GeV STAR Preliminary

Nu Xu26/35 RNC Meeting, Berkeley, February 21, 2012 Observable*: NCQ Scaling in v 2 - m  ~ m p ~ 1 GeV - ss  φ not K + K -  φ -   h <<  p ,  In the hadronic case, no number of quark scaling and the value of v 2 of φ will be small. * Thermalization is assumed!  

Nu Xu27/35 RNC Meeting, Berkeley, February 21, 2012 Particle and Anti-particle v 2 vs. √s NN At √s NN ≤ 11.5 GeV: - v 2 ( baryon) > v 2 (anti-baryon) - v 2 ( π + ) < v 2 (π - ) - v 2 ( K - ) < v 2 (K + ) Hadronic interactions are dominant STAR: Quark Matter 2011

Sign Dependence and ϕ -meson v 2 - The φ v 2 falls off trend from other hadrons at 11.5 GeV -The v 2 -scaling holds for hadrons with same charge (?) “Effects of Hadronic Potential” by Xu, Chen, Ko, Lin,

Nu Xu29/35 RNC Meeting, Berkeley, February 21, 2012 Susceptibilities and Moments Thermodynamic function: The susceptibility: Thermodynamic function  Susceptibility  Moments Model calculations, e.g. LGT, HRG  Measurements Conserved Quantum Number S. Gupta, F. Karsch, V. Koch K. Redlich, M. Stephanov …

Nu Xu30/35 RNC Meeting, Berkeley, February 21, 2012 First Results on High Moments STAR: PRL, 105, 22302(2010) Energy Scan in Au+Au collisions: Run 10: 7.7, 11.5, 39 GeV Run 11: 19.6, 27 GeV 1)Centrality averaged events. In this analysis, effects of volume and detecting efficiencies are all canceled out. 2)Most transport model results values are higher than unity, except the Theminator result at 200GeV. LGT predicted values around )Test of thermalization with higher moments. 4)Critical point effect: non- monotonic dependence on collision energy. STAR: PRL105, 22302(2010) F. Karsch and K. Redlich, PLB695, 136(2011) 1)Centrality averaged events. In this analysis, effects of volume and detecting efficiencies are all canceled out. 2)Most transport model results values are higher than unity, except the Theminator result at 200GeV. LGT predicted values around )Test of thermalization with higher moments. 4)Critical point effect: non- monotonic dependence on collision energy. STAR: PRL105, 22302(2010) F. Karsch and K. Redlich, PLB695, 136(2011)

Nu Xu31/35 RNC Meeting, Berkeley, February 21, 2012 Comparing with LGT Results Assumptions: (a) Freeze-out temperature is close to LGT T C (b) Thermal equilibrium reached in central collisions (c) Taylor expansions, at μ B ≠0, on LGT results are valid  Lattice results are consistent with data for 20 < √s NN < 200 GeV  T C = (MeV) References: - STAR, PRL105, 22303(10) - R.V. Gavai and S. Gupta: PLB696, 459(11) - S. Gupta et al, Science, 332, 1525(2011)

Nu Xu32/35 RNC Meeting, Berkeley, February 21, 2012 Lattice: Phase Transition Temperature ActionTemperature Polyakov LoopT C conf ~ 170 MeV Chiral OperatorT C Chiral ~ 155 MeV RHIC DataT C Exp ~ MeV (T CH Exp ~ 160±5 MeV)

Nu Xu33/35 RNC Meeting, Berkeley, February 21, 2012 Summary (1)In √s NN = 200GeV Au+Au collisions, hot and dense matter, with partonic degrees of freedom and collectivity, has been formed (2)The matter behavior like a quantum liquid with small η/s (3) Partonic matter  antimatter -- =======-- (4) [partonic] < μ B ~110–320 (MeV) < [hadronic] (5) More results will come from PID v 2 and higher moments. (6) High statistics data for √s NN = GeV is important.

Nu Xu34/35 RNC Meeting, Berkeley, February 21, Phase boundary RHIC, FAIR, NICA Outlook: (7.7, 11.5, 15.5, 19.6, 27, 39,62, 200 GeV) 1 1 T ini, T C LHC, RHIC 2 2 T E RHIC, SPS, FAIR QGP Properties at RHIC (200 GeV AA and pA Collisions) - Upgrade for HF hadron measurements - di-leptons: v 2, p T spectra, R AA, … vs. mass QGP Properties at RHIC (200 GeV AA and pA Collisions) - Upgrade for HF hadron measurements - di-leptons: v 2, p T spectra, R AA, … vs. mass Patonic Matter Hadronic Matter

Thank You! Nu Xu

Nu Xu36/35 RNC Meeting, Berkeley, February 21, 2012 Atomic Nuclei Formation