EMMI workshop, St. Goar, 31 Aug  3 Sep, 2009 Kai Schweda 1/26 (Some) Bulk Properties at RHIC Kai Schweda, University of Heidelberg / GSI Darmstadt Many.

Slides:



Advertisements
Similar presentations
PID v2 and v4 from Au+Au Collisions at √sNN = 200 GeV at RHIC
Advertisements

Mass, Quark-number, Energy Dependence of v 2 and v 4 in Relativistic Nucleus- Nucleus Collisions Yan Lu University of Science and Technology of China Many.
TJH: ISMD 2005, 8/9-15 Kromeriz, Czech Republic TJH: 1 Experimental Results at RHIC T. Hallman Brookhaven National Laboratory ISMD Kromeriz, Czech Republic.
Aug , 2005, XXXV ISMD, Czech X.Dong, USTC 1 Open charm production at RHIC Xin Dong University of Science and Technology of China - USTC  Introduction.
First Alice Physics Week, Erice, Dec 4  9, Heavy  Flavor (c,b) Collectivity at RHIC and LHC Kai Schweda, University of Heidelberg A. Dainese,
ISMD’05, Kromeriz, Aug 09  15, Heavy  Flavor (c,b) Collectivity – Light  Flavor (u,d,s) Thermalization at RHIC Kai Schweda, University of Heidelberg.
Jet probes of nuclear collisions: From RHIC to LHC Dan Magestro, The Ohio State University Midwest Critical Mass October 21-22, 2005.
Charm & bottom RHIC Shingo Sakai Univ. of California, Los Angeles 1.
Dilepton Forum, GSI, Feb 27, 2007 Kai Schweda 1 Heavy-Flavor Production at RHIC Kai Schweda, University of Heidelberg / GSI Darmstadt.
RHIC & AGS Annual User’s Meeting, May 2003 Nu Xu 1 Recent Results from STAR Nu Xu Lawrence Berkeley National Laboratory For the STAR Collaboration.
Heavy Quark Probes of QCD Matter at RHIC Huan Zhong Huang University of California at Los Angeles ICHEP-2004 Beijing, 2004.
HD lunch talk, 30 Apr 2008 Kai Schweda 1 Heavy-Quarks with ALICE  Some Highlights from the ALICE Physics Week in Prague March 2008 Kai Schweda, University.
Physics of High Baryon Density,Trento, May 29  June 2, Charm with STAR Kai Schweda, University of Heidelberg A. Dainese, X. Dong, J. Faivre, Y.
RNM meeting FIAS, Frankfurt, 22 Feb Hunt for the QGP at RHIC Kai Schweda, University of Heidelberg S. Blyth, A. Dainese, T. Dietel, X. Dong, J.
R. L. Thews Hard Probes 2004 Lisbon QUARKONIUM FORMATION IN STATISTICAL AND KINETIC MODELS R. L. THEWS UNIVERSITY OF ARIZONA HARD PROBES 2004 LISBON November.
DNP03, Tucson, Oct 29, Kai Schweda Lawrence Berkeley National Laboratory for the STAR collaboration Hadron Yields, Hadrochemistry, and Hadronization.
ISMD, Paraty, Brazil, Sep 2  Sep 8, 2006 Kai Schweda 1 D – D Correlations as a Sensitive Probe of Light – quark Thermalization Kai Schweda, University.
XXIII Graduate Days, Heidelberg, 5  9 Oct, 2009 Kai Schweda 1/62 Bulk Properties of QCD Matter Kai Schweda, University of Heidelberg / GSI Darmstadt Many.
STAR upgrade workshop, Yale, Jun , People: F. Bieser, R. Gareus, L. Greiner, H. Matis, M. Oldenburg, F. Retiere, H.G. Ritter, K.S., A. Shabetai(IReS),
Nu XuInternational Conference on Strangeness in Quark Matter, UCLA, March , 20061/20 Search for Partonic EoS in High-Energy Nuclear Collisions Nu.
5-12 April 2008 Winter Workshop on Nuclear Dynamics STAR Particle production at RHIC Aneta Iordanova for the STAR collaboration.
ISMD, Berkeley, Aug 4  9, 2007 Kai Schweda 1 Bulk Properties of QCD – matter at Highest Colider Energies Kai Schweda, University of Heidelberg / GSI Darmstadt.
DPG spring meeting, Tübingen, March Kai Schweda Lawrence Berkeley National Laboratory for the STAR collaboration Recent results from STAR at RHIC.
USTC, Hefei, Nov 22, Heavy  Flavor (c,b) Collectivity at RHIC and LHC Kai Schweda, University of Heidelberg A. Dainese, X. Dong, J. Faivre, Y.
WWND, San Diego1 Scaling Characteristics of Azimuthal Anisotropy at RHIC Michael Issah SUNY Stony Brook for the PHENIX Collaboration.
Outline Charm physics in NN collisions – some remarks
17 Sep 2012 Erice, 34th Course Open charm production with ALICE at the LHC Kai Schweda (for the ALICE Collaboration) Physikalisches Institut University.
Strange and Charm Probes of Hadronization of Bulk Matter at RHIC International Symposium on Multi-Particle Dynamics Aug 9-15, 2005 Huan Zhong Huang University.
Masashi Kaneta, LBNL Masashi Kaneta for the STAR collaboration Lawrence Berkeley National Lab. First results from STAR experiment at RHIC - Soft hadron.
Nu Xu1/28VIII International Workshop on Relativistic Aspects of Nuclear Physics, Rio de Janeiro, Brazil, 3-6, November, 2008 Explore the QCD Phase Diagram.
Rashmi Raniwala Hot & Dense Matter in RHIC-LHC Era, February 12-14, 2008, TIFR, Mumbai 1 Rashmi Raniwala Department of Physics University of Rajasthan.
May, 20, 2010Exotics from Heavy Ion Collisions KE T and Quark Number Scaling of v 2 Maya Shimomura University of Tsukuba Collaborated with Yoshimasa Ikeda,
Partonic Collectivity at RHIC ShuSu Shi for the STAR collaboration Lawrence Berkeley National Laboratory Central China Normal University.
//Talk/2004/11MIT/nxu_mit_26oct04// LNS, November 15, 2004 Nu Xu 1 / 40 Recent Results from STAR at RHIC Nu Xu Lawrence Berkeley National Laboratory X.
In-Kwon YOO Pusan National University Busan, Republic of KOREA SPS Results Review.
Aug. 4-9, 2005, QM2005, Budapest X.Dong, USTC 1 Open charm production at RHIC Xin Dong University of Science and Technology of China - USTC.
M. Oldenburg Strange Quark Matter 2006 — March 26–31, Los Angeles, California 1 Centrality Dependence of Azimuthal Anisotropy of Strange Hadrons in 200.
Heavy flavour capabilities with the ALICE TRD Benjamin Dönigus ISNP 2008 Erice/Sicily.
Open charm hadron production via hadronic decays at STAR
J/Ψ PRODUCTION IN A+A COLLISIONS AT STAR Ota Kukral for the STAR Collaboration Czech Technical University in Prague RHIC & AGS Annual Users’ Meeting 17.
Helen Caines Yale University Soft Physics at the LHC - Catania - Sept Questions for the LHC resulting from RHIC Strangeness Outline Chemistry Yields.
//Nxu/tex3/TALK/2004/10USTC Collective Dynamics in High-Energy Collisions, USTC, October 18-19, 2004 Nu Xu 1 Charm Production at RHIC (1) Introduction.
CCAST, Beijing, China, 2004 Nu Xu //Talk/2004/07USTC04/NXU_USTC_8July04// 1 / 26 Collective Expansion in Relativistic Heavy Ion Collisions -- Search for.
Masashi Kaneta, First joint Meeting of the Nuclear Physics Divisions of APS and JPS 1 / Masashi Kaneta LBNL
Ralf Averbeck Stony Brook University Hot Quarks 2004 Taos, New Mexico, July 19-24, 2004 for the Collaboration Open Heavy Flavor Measurements with PHENIX.
HIRSCHEGG, January , 2005 Nu Xu //Talk/2005/01Hirschegg05// 1 / 24 Search for Partonic EoS in High-Energy Collisions Nu Xu Lawrence Berkeley National.
Peter Kolb, CIPANP03, May 22, 2003what we learn from hydro1 What did we learn, and what will we learn from Hydro CIPANP 2003 New York City, May 22, 2003.
John Harris (Yale) LHC Conference, Vienna, Austria, 15 July 2004 Heavy Ions - Phenomenology and Status LHC Introduction to Rel. Heavy Ion Physics The Relativistic.
OPEN HEAVY FLAVORS 1. Heavy Flavor 2 Heavy quarks produced in the early stages of the collisions (high Q2)  effective probe of the high-density medium.
1 Guannan Xie Nuclear Modification Factor of D 0 Mesons in Au+Au Collisions at √s NN = 200 GeV Lawrence Berkeley National Laboratory University of Science.
Strange Probes of QCD Matter Huan Zhong Huang Department of Physics and Astronomy University of California Los Angeles, CA Oct 6-10, 2008; SQM2008.
Quantitative Comparison of Viscous Hydro with Data What is needed to make progress: the STAR-flavored view Nu Xu (for STAR Collaboration) Nuclear Science.
Bulk properties at RHIC Olga Barannikova (Purdue University) Motivation Freeze-out properties at RHIC STAR perspective STAR  PHENIX, PHOBOS Time-span.
Christina MarkertHirschegg, Jan 16-22, Resonance Production in Heavy Ion Collisions Christina Markert, Kent State University Resonances in Medium.
Japanese Physics Society meeting, Hokkaido Univ. 23/Sep/2007, JPS meeting, Sapporo, JapanShinIchi Esumi, Inst. of Physics, Univ. of Tsukuba1 Collective.
Nu Xu“Hot and Dense Matter in the RHIC-LHC Era”, Mumbai, India, February 12-14, 20081/27 Many Thanks to the Conference Organizers Partonic EoS at RHIC.
Department of Physics, Oregon University, 7 October, 2004 Nu Xu //Nxu/tex3/TALK/2004/10OU 1 The `Big Bang’ in the Laboratory -- The Physics of High-energy.
Nu Xu1/36 International School of Nuclear Physics, 30 th Course, Erice-Sicily, September 2008 Explore the QCD Phase Diagram - Partonic Equation.
Yuting Bai (for the Collaboration) Anisotropic Flow and Ideal Hydrodynamic Limit International Conference on Strangeness in Quark Matter 2008 Oct ,
Strange hadrons and resonances at LHC energies with the ALICE detector INPC 2013 Firenze, Italy 2 -7 June 2013 A. Badalà (INFN Sezione di Catania) for.
Heavy-ion group at Heidelberg
Building Blocks of Matter
Outline Introduction LHC and ALICE Heavy-quark production in pp
Experimental Overview of Open Heavy Flavor
Open charm production in pp and Pb-Pb collisions in ALICE at the LHC
Collective Dynamics at RHIC
Strangeness in Collisions, BNL, February , 2006
Open charm production with ALICE at the LHC
Many Thanks to Organizers!
Dipartimento Interateneo di Fisica, Bari (Italy)
Presentation transcript:

EMMI workshop, St. Goar, 31 Aug  3 Sep, 2009 Kai Schweda 1/26 (Some) Bulk Properties at RHIC Kai Schweda, University of Heidelberg / GSI Darmstadt Many thanks to organizers !

EMMI workshop, St. Goar, 31 Aug  3 Sep, 2009 Kai Schweda 2/26 Outline  Introduction  Collectivity at RHIC - transverse radial flow - tranverse elliptic flow - extracting  /s  Heavy  quark dynamics  Summary

EMMI workshop, St. Goar, 31 Aug  3 Sep, 2009 Kai Schweda Operated modes: Au 9, 20, 64, 130, 200 GeV/2n Cu + 22, 62, 200 GeV/2n d GeV/2n p + 22, 62, 200, 500 GeV Planned or possible modes: Au 5 GeV/2n p GeV/2n

EMMI workshop, St. Goar, 31 Aug  3 Sep, 2009 Kai Schweda 4/26 Hadron spectra from RHIC p+p and Au+Au collisions at 200 GeV White papers - STAR: Nucl. Phys. A757, p102. Full kinematic reconstruction of (multi-) strange hadrons in large acceptance of STAR

EMMI workshop, St. Goar, 31 Aug  3 Sep, 2009 Kai Schweda HI - Collision History Plot: R. Stock, arXiv: [nucl-ex].  T c(ritical) : quarks and gluon  hadrons  T ch(emical) : hadron abundancies freeze out  T fo : particle spectra freeze out

EMMI workshop, St. Goar, 31 Aug  3 Sep, 2009 Kai Schweda Hadron Yield  Ratios 1) At RHIC: T ch = 160 ± 10 MeV  B = 25 ± 5 MeV 2)  S = 1.  The hadronic system is thermalized at RHIC. 3) Short-lived resonances show deviations.  There is life after chemical freeze-out. RHIC white papers , Nucl. Phys. A757, STAR: p102; PHENIX: p184; Statistical Model calculations: P. Braun-Munzinger et al. nucl-th/

EMMI workshop, St. Goar, 31 Aug  3 Sep, 2009 Kai Schweda 7/26 Pressure, Flow, … Thermodynamic identity  – entropy p – pressure U – energy V – volume  = k B T, thermal energy per dof In A+A collisions, interactions among constituents and density distribution lead to: pressure gradient  collective flow  number of degrees of freedom (dof)  Equation of State (EOS)  cumulative – partonic + hadronic

EMMI workshop, St. Goar, 31 Aug  3 Sep, 2009 Kai Schweda 8/26 (anti-)Protons From RHIC (anti-)Protons From RHIC More central collisions Centrality dependence: - spectra at low momentum de-populated, become flatter at larger momentum  stronger collective flow in more central coll.! STAR: Phys. Rev. C70, (R).

EMMI workshop, St. Goar, 31 Aug  3 Sep, 2009 Kai Schweda 9/26 1) Multi-strange hadrons  and  freeze-out earlier than ( , K, p)  Collectivity prior to hadronization  Collectivity prior to hadronization 2) Sudden single freeze-out*: Resonance decays lower T fo for ( , K, p)  Collectivity prior to hadronization  Partonic Collectivity ?  Partonic Collectivity ? Kinetic Freeze-out at RHIC STAR Data: Nucl. Phys. A757, ( ), *A. Baran, W. Broniowski and W. Florkowski, Acta. Phys. Polon. B 35 (2004) 779. STAR Preliminary

Anisotropy Parameter v 2 y x pypy pxpx coordinate-space-anisotropy  momentum-space-anisotropy Initial/final conditions, EoS, degrees of freedom

EMMI workshop, St. Goar, 31 Aug  3 Sep, 2009 Kai Schweda 11/26 v 2 in the Low-p T Region P. Huovinen, private communications, v 2 approx. linear in p T, mass ordering from light  to heavier  àcharacteristic of hydrodynamic flow ! à sensitive to equation of state

EMMI workshop, St. Goar, 31 Aug  3 Sep, 2009 Kai Schweda 12/26 v 2 of  and multi-strange   Strange-quark flow - partonic collectivity at RHIC ! QM05 conference: M. Oldenburg; nucl-ex/

EMMI workshop, St. Goar, 31 Aug  3 Sep, 2009 Kai Schweda 13/26 Collectivity  Energy Dependence  Collectivity parameters and increase with collision energy  strong collective expansion at RHIC ! RHIC  0.6  expect strong partonic expansion at LHC, LHC  0.8, T fo  T ch K.S., ISMD07, arXiv: [nucl-ex].

EMMI workshop, St. Goar, 31 Aug  3 Sep, 2009 Kai Schweda 14/26 Elliptic Flow vs Collision Energy  Centrality dependence: - initial eccentricity  - overlap area S  Collision energy dep.: - multiplicity density dN ch /dy  in central collisions at RHIC, hydro-limit seems reached ! NA49, Phys. Rev. C68, (2003); STAR, Phys. Rev. C66, (2002); Hydro-calcs.: P. Kolb, J. Sollfrank, and U. Heinz, Phys. Rev.C62, (2000). Glauber initial conditions

EMMI workshop, St. Goar, 31 Aug  3 Sep, 2009 Kai Schweda 15/26 Non-ideal Hydro-dynamics M.Luzum and R. Romatschke, PRC (2008); P. Romatschke, arXiv:  finite shear viscosity  reduces elliptic flow  many caveats, e.g.: - initial eccentricity  (Glauber, CGC, …) - equation of state - hadronic contribution to  /s cf. talks by D. Fernandez-Fraile and D. Rischke

EMMI workshop, St. Goar, 31 Aug  3 Sep, 2009 Kai Schweda 16/26 Partonic Collectivity at RHIC 1) Copiously produced hadrons freeze-out ,K,p: T fo = 100 MeV,  T = 0.6 (c) >  T (SPS) 2) Multi-strange hadrons freeze-out: T fo = MeV (~ T ch ),  T = 0.4 (c) 3) Multi-strange v 2 :  and multi-strange hadrons  and  do flow! 4) Model - dependent  /s: (0?), x 1/4  Deconfinement & Partonic (u,d,s) Collectivity !

EMMI workshop, St. Goar, 31 Aug  3 Sep, 2009 Kai Schweda Heavy  flavor: a unique probe X. Zhu, M. Bleicher, S.L. Huang, K.S., H. Stöcker, N. Xu, and P. Zhuang, PLB 647 (2007) 366. m c,b >>  QCD : new scale m c,b  const., m u,d,s ≠ const. initial conditions:  test pQCD,  R,  F probe gluon distribution early partonic stage: diffusion (  ), drag (  ), flow probe thermalization hadronization: chiral symmetry restoration confinement statistical coalescence J/  enhancement / suppression Q2Q2 time

EMMI workshop, St. Goar, 31 Aug  3 Sep, 2009 Kai Schweda 18/26 Heavy  quark Correlations  c-cbar mesons are correlated Pair creation: back to back Gluon splitting: forward Flavor excitation: flat  Exhibits strong correlations !  Baseline at zero: clear measure of vanishing correlations !  probe thermalization among partons ! PYTHIA: p + 14 TeV X. Zhu, M. Bleicher, S.L. Huang, K.S., H. Stöcker, N. Xu, and P. Zhuang, PLB 647 (2007) 366. G. Tsildeakis, H. Appelshäuser, K.S., J. Stachel, arXiv:

EMMI workshop, St. Goar, 31 Aug  3 Sep, 2009 Kai Schweda 19/26 Where does all the charm go? D0D0 DD DsDs cc J   Total charm cross section: open charm hadrons, e.g. D 0, D *,  c, … or c,b  e(  ) + X  Hidden-charm mesons, e.g. J/  carry ~ 1 % of total charm Statistics plot: H. Yang and Y. Wang, U Heidelberg.

EMMI workshop, St. Goar, 31 Aug  3 Sep, 2009 Kai Schweda 20/26 How to measure Heavy- Quark Production  e.g., D 0, c  = 123  m  displaced decay vertex is signature of heavy-quark decay  need precise pointing to collision vertex

EMMI workshop, St. Goar, 31 Aug  3 Sep, 2009 Kai Schweda 21/26 Heavy  Flavor production at RHIC  large discrepancy between STAR and PHENIX: factor > 2 (!)  need Si-vertex upgrades (> 2011)  large theoretical uncertainties (factor > 10)  Measure charm production at RHIC, LHC, FAIR and provide input to theory: - gluon distribution, - scales  R,  F Plot: J. Dunlop (STAR), QM2009, Open Heavy-flavor in heavy-ion collisions, Calcs: R. Vogt,Eur. Phys. J. C, s x (2008), M. Cacciari, 417th Heraeus Seminar, Bad Honnef (2008).

EMMI workshop, St. Goar, 31 Aug  3 Sep, 2009 Kai Schweda 22/26 STAR MicroVertex Tracker Active pixel sensors (APS) Two layers of thin silicon - Full open charm measurements - Full resonance measurements with both hadron and lepton decays STAR and PHENIX Si - Upgrades PHENIX Silcon Vertex Tracker 2 layers of pixel sensors (ALICE-type) 2 layers of thin silicon strip - Full open charm measurements  High-statistics Au+Au 200GeV: 2012* *T. Roser, RHIC Retreat, Mystic, CT, July 2009.

EMMI workshop, St. Goar, 31 Aug  3 Sep, 2009 Kai Schweda 23/26 ALICE at LHC TPC TRD 1000 scientists, 30 nations ITS: measures secondary vertex, open heavy-flavor, c and b TPC: tracks and identifies charged particles, (e,  ), , K, p TRD: identifies electrons above 1 GeV, fast trigger (6  s) ITS

EMMI workshop, St. Goar, 31 Aug  3 Sep, 2009 Kai Schweda 24/26 resolution at 10 GeV: measured 6.5% design 4.5% TPC commissioning performance at design, TPC ready for collisions transverse momentum resolution, B=0.5 Tparticle identification via dE/dx resolution: measured <5% design 5.5% –TPC installed in ALICE, running continuously May-October 2008, and since Aug 2009 –60 million events (cosmics, krypton, and laser) recorded

ITS: installed & commissioned SSD: charge correlation p-side vers. n-side Drift speed constant for hours SDD: Drift speed calibration & monitoring versus time after alignment before alignment SPD: Point resolution (σ spatial ) σ Δx = √2 x σ spatial ‏ Data: 14 μm Simulation: 11 μm

EMMI workshop, St. Goar, 31 Aug  3 Sep, 2009 Kai Schweda 26/26 Summary  Strong collective expansion at RHIC = 0.6 c, = 0.07  Small  /s < 10 x 1/4   Large uncertainty (exp. and theory) in  at RHIC need Si - upgrades  Measure spectra, correlations and v 2 of: e ±, D 0, D +, D *, D s, J/  c,  b,  to identify and characterize QGP !  LHC ready for Physics !