PPG067 Physics Statements Michael P. McCumber and Barbara Jacak August + September, 2006.

Slides:



Advertisements
Similar presentations
What do we Learn From Azimuthal Correlation Measurements in PHENIX Roy. A. Lacey Nuclear Chemistry, SUNY, Stony Brook.
Advertisements

Elliptic flow of thermal photons in Au+Au collisions at 200GeV QNP2009 Beijing, Sep , 2009 F.M. Liu Central China Normal University, China T. Hirano.
1 Jet Structure of Baryons and Mesons in Nuclear Collisions l Why jets in nuclear collisions? l Initial state l What happens in the nuclear medium? l.
TJH: ISMD 2005, 8/9-15 Kromeriz, Czech Republic TJH: 1 Experimental Results at RHIC T. Hallman Brookhaven National Laboratory ISMD Kromeriz, Czech Republic.
Photon-Hadron Correlations at RHIC Saskia Mioduszewski Texas A&M University E-M Workshop of RHIC/AGS Users’ Meeting 27 May, 2008.
Probing Properties of the QCD Medium via Heavy Quark Induced Hadron Correlations Huan Zhong Huang Department of Physics and Astronomy University of California.
References to Study the New Matter. Study QGP in different Centrality Most Central events (highest multiplicity), e.g. top 5% central, i.e. 5% of the.
Motivation One of the major findings at the Relativistic Heavy Ion Collider (RHIC) is the suppression of the highly energetic particles which raises the.
Jet Propagation and Mach-Cone Formation in (3+1)-dimensional Ideal Hydrodynamics Barbara Betz and Miklos Gyulassy, Jorge Noronha, Dirk Rischke, Giorgio.
High-p T spectra and correlations from Cu+Cu and Au+Au collisions in STAR Marco van Leeuwen, LBNL for the STAR collaboration.
Understanding Jet Energy Loss with Angular Correlation Studies in PHENIX Ali Hanks for the PHENIX Collaboration 24 th Winter Workshop on Nuclear Dynamics.
Michael P. McCumber for the PHENIX Collaboration Quark Matter 2008 Jaipur, India 5 February 2008 The “Shoulder” and the “Ridge” in PHENIX: Medium Response.
Oana Catu, Yale University for the STAR Collaboration Quark Matter 2008, February 4-10, Jaipur, India System size dependence of dihadron correlations and.
Luan Cheng (Institute of Particle Physics, Huazhong Normal University) I. Introduction II. Interaction Potential with Flow III. Flow Effects on Light Quark.
Hard Probes at RHIC Saskia Mioduszewski Texas A&M University Winter Workshop on Nuclear Dynamics 8 April, 2008.
WWND 03/13/06 N Grau1 Jet Correlations from PHENIX Focus entirely on A+A collisions High-trigger p T correlations –Can we do jet tomography? Low-trigger.
Jana Bielcikova (Yale University) for the STAR Collaboration 23 rd Winter Workshop on Nuclear Dynamics February 12-18, 2007 Two-particle correlations with.
Jet Propagation and Mach-Cone Formation in (3+1)-dimensional Ideal Hydrodynamics Barbara Betz Thanks goes to: Miklos Gyulassy, Igor Mishustin, Jorge Noronha,
Do We Understand Interactions of Hard Probes With Dense Matter ? Joint EIC & Hot QCD Workshop on Future Prospects of QCD at High Energy BNL - 20 July 2006.
A derivation of the source term induced by a fast parton from the quark energy-momentum tensor Bryon Neufeld, LANL Winter Workshop on Nuclear Dynamics.
STAR Back-to-Back Di-Jet Triggered Multi-Hadron Correlations as Medium Probes in STAR Back-to-Back Di-Jet Triggered Multi-Hadron Correlations as Medium.
Interaction between jets and dense medium in heavy-ion collisions Rudolph C. Hwa University of Oregon TsingHua University, Beijing, China May 4, 2009.
Sonic Mach Cones Induced by Fast Partons in a Perturbative Quark-Gluon Plasma [1] Presented by Bryon Neufeld (of Duke University) on March 20 th 2008 in.
J. RuppertFocus talk on interactions between jets and medium #1 Focus talk on interactions between jets and medium Jörg Ruppert Nuclear Theory, Duke University.
The conical flow Where the energy of quenched jets go? Edward Shuryak (with Jorge Casalderrey-Solana, Derek Teaney) Department of Physics and Astronomy,
Nov 2001 Craig Ogilvie 1 Angular Correlations at High pt: Craig Ogilvie for the Phenix Collaboration Energy-loss: increased medium-induced gluon-radiation.
What’s Missing in our Current Picture from High p T Measurements at RHIC? Saskia Mioduszewski Texas A&M University 23 March, 2007.
1 Identified Di-hadron Correlation in Au+Au & PYTHIA Simulation Jiaxu Zuo Shanghai Institute of Applied Physics & BNL CCAST Beijing,
Background introduction Model introduction Analysis method Results and discussions Conclusions Collaborators: S. Zhang, Y. G. Ma, H. Z. Huang, X. Z, Cai,
Precision Probes for Hot QCD Matter Rainer Fries Texas A&M University & RIKEN BNL QCD Workshop, Washington DC December 15, 2006.
November 18, Shanghai Anomalous Viscosity of an Expanding Quark-Gluon Plasma Masayuki ASAKAWA Department of Physics, Osaka University S. A.
N. N. Ajitanand Nuclear Chemistry, SUNY, Stony Brook For the PHENIX Collaboration Two and Three particle Flavor Dependent Correlations Remember the hungarian.
U N C L A S S I F I E D 7 Feb 2005 Studies of Hadronic Jets with the Two-Particle Azimuthal Correlations Method Paul Constantin.
Detail study of the medium created in Au+Au collisions with high p T probes by the PHENIX experiment at RHIC Takao Sakaguchi Brookhaven National Laboratory.
Conical Flow induced by Quenched QCD Jets Jorge Casalderrey-Solana, Edward Shuryak and Derek Teaney, hep- ph/ SUNY Stony Brook.
20-25 May 2007 The Berkeley School STAR Study of Jets with 2+1 multi-particle correlations Richard Hollis* for the STAR Collaboration * in close collaboration.
1 Search for the Effects of the QCD Color Factor in High-Energy Collisions at RHIC Bedanga Mohanty LBNL  Motivation  Color Factors  Search for Color.
Jet Propagation and Mach Cones In (3+1)d Ideal Hydrodynamics Barbara Betz, Miklos Gyulassy, Dirk Rischke, Horst Stöcker and Giorgio Torrieri Quark Matter.
High Pt physics with TOF ALICE B.V.Zagreev ITEP
1 Olga Barannikova University of Illinois at Chicago LHC09, Prague Multi-hadron correlations at RHIC and LHC Olga Barannikova.
Jet Physics in ALICE Mercedes López Noriega - CERN for the ALICE Collaboration Hot Quarks 2006 Villasimius, Sardinia - Italy.
Background introduction Model introduction Analysis method Results and discussions Conclusions G.L. Ma, S. Zhang, YGM et al., Phys Lett B 641, 362 (2006)
Jet Propagation & Mach Cone Evolution in (3+1)d Ideal Hydrodynamics Barbara Betz, Miklos Gyulassy, Dirk Rischke, Horst Stöcker and Giorgio Torrieri 05.
1 Jet Fragmentation and Baryon Production l Jet fragmentation l Why we should expect medium effects l Energy loss effects on the fragmentation function.
U N C L A S S I F I E D Operated by the Los Alamos National Security, LLC for the DOE/NNSA Slide 0 Study of the Quark Gluon Plasma with Hadronic Jets What:
Flow effects on jet profile N. Armesto 2nd International Conference on Hard and Electromagnetic Probes of High-Energy Nuclear Collisions Asilomar Conference.
1 N. N. Ajitanand Nuclear Chemistry, SUNY Stony Brook 27 May 2008 AGS-RHIC Workshop 2008 Three Particle Correlations.
Hydrodynamic Flow from Fast Particles Jorge Casalderrey-Solana. E. V. Shuryak, D. Teaney SUNY- Stony Brook.
1 Mach Cones in Quark Gluon Plasma Jorge Casalderrey-Solana Lawrence Berkeley Laboratory.
Strange Probes of QCD Matter Huan Zhong Huang Department of Physics and Astronomy University of California Los Angeles, CA Oct 6-10, 2008; SQM2008.
The Art Poskanzer School 1. 2 Physics motivation To create and study QGP – a state of deconfined, thermalized quarks and gluons predicted by QCD at high.
21 st WWND, W. Holzmann Wolf Gerrit Holzmann (Nuclear Chemistry, SUNY Stony Brook) for the Collaboration Tomographic Studies of the sQGP at RHIC: the next.
2008/04/12APS April Meeting 1 Decomposition of Awayside Components of Dijet Correlation in Au+Au Collisions at √S NN = 200 GeV at PHENIX Chin-Hao Chen.
Kirill Filimonov, ISMD 2002, Alushta 1 Kirill Filimonov Lawrence Berkeley National Laboratory Anisotropy and high p T hadrons in Au+Au collisions at RHIC.
Enke Wang (Institute of Particle Physics, Huazhong Normal University) I. Introduction II. Ineraction Potential with Flow III.Flow Effects on Light Quark.
Xin-Nian Wang/LBNL QCD and Hadronic Physics Beijing, June 16-20, 2005 Xin-Nian Wang 王新年 Lawrence Berkeley National Laboratory Jet Tomography of Strongly.
1 High p T Hadron Correlation Rudolph C. Hwa University of Oregon Hard Probes 2006 Asilomar, CA, June 10, 2006 and No Correlation.
What have we learned from the RHIC experiments so far ? Berndt Mueller (Duke University) KPS Meeting Seoul, 22 April 2005.
Hadron RHIC at intermediate and high p T Conference on Intersections between Particle and Nuclear Physics New York, NY, May 20-23, 2003 Berndt.
Parton showers as a source of energy-momentum deposition and the implications for jet observables Bryon Neufeld, LANL 1Neufeld Based on the preprint R.B.
Jana Bielcikova (Yale)ISMD 2007, Berkeley1 Near-side di-hadron correlations at RHIC Jana Bielcikova (Yale University)
F. Dominguez, CM, A. Mueller, B. Xiao and B. Wu, arXiv:
Future prospects for NA61 heavy ions: rare observables
Recontres de Moriond, March
Medium properties and jet-medium interaction from STAR
In-Medium Properties of Jets
Experimental Studies of Quark Gluon Plasma at RHIC
Guo-Liang Ma Background introduction Model introduction
Jet Correlations from PHENIX: From Low-pT to High-pT
of Hadronization in Nuclei
Presentation transcript:

PPG067 Physics Statements Michael P. McCumber and Barbara Jacak August + September, 2006

25 September 2006Michael P. McCumber & Barbara Jacak 2 Figure 3 rms increases with npart kurtosis decreases rapidly from near- gaussian values away side peak dispacement is consistent with 0 in dAu & peripheral AuAu. rapidly increases to about 1 rad.

25 September 2006Michael P. McCumber & Barbara Jacak 3 Mechanisms for away-side modification Mach Cone Cherenkov Gluon-Radiation Wake Waves Medium-induced gluon radiation at large emission angles Damping of jet by strongly coupled medium (via AdS/CFT)

25 September 2006Michael P. McCumber & Barbara Jacak 4 Mach Cones – Renk & Ruppert hep-ph/ Mach cone survives expansion! Longitudinal flow → better Δφ signal from a Mach Cone Data → large fractional of energy deposited in collective, propagating mode AwayNear→

25 September 2006Michael P. McCumber & Barbara Jacak 5 Mach Cones – Chaudhuri & Heinz hydro simulations: assume lost energy instantaneously thermalized No Mach cone produced Large energy loss scenarios give “splash-back” signal rejected by data PRL97, (2006)

25 September 2006Michael P. McCumber & Barbara Jacak 6 Mach Cones – Jorge & Edward Modified away side peak shape is due to propagation of a sound wave Speed of sound intermediate between QGP (c s =  0.33) and hadron gas (c s =  0.2) First order phase transition causes existence of region with c s =0. This would give a reflected wave, and 2 nd peak at  =1.4 rad NP A774, 577 (2006) & hep-ph/

25 September 2006Michael P. McCumber & Barbara Jacak 7 Mach Cones – Jorge & Edward hep-ph/ No clear (or even unclear) evidence for second peak in ppg032 result

25 September 2006Michael P. McCumber & Barbara Jacak 8 Run 4 AuAu not here either… (maybe in 0-5% bin?)

25 September 2006Michael P. McCumber & Barbara Jacak 9 Cherenkov – Koch, Majumder, Wang Cherenkov production has “a strong dependence on the gluon momentum” & will “disappear for high-energy gluons” D values will “gradually” shrink as associated momentum is increased. Not consistent with our data PRL 96, (2006) Paul C’s AN

25 September 2006Michael P. McCumber & Barbara Jacak 10 Wake Waves – Ruppert, Muller Excite either a density wave or a plasma collective mode (plasmon) Sub-sonic partons drag along a screening cloud as a wake (the response of plasma to color charge) Super-sonic partons create Mach cone signal If plasma is strongly coupled, high p parton excites plasma oscillations analogous to Cherenkov radiation (but it looks like Mach cone…) PL B618, 123 (2005)

25 September 2006Michael P. McCumber & Barbara Jacak 11 Large angle gluon emission -- Vitev PL B630, 178 (2005) Predicted angles are typically smaller than observed. p T dependence in central collisions (like the data) Average scattering angle decreases with path length This contrasts our centrality dependence!

25 September 2006Michael P. McCumber & Barbara Jacak 12 large angle gluon emission #2 Polosa & Salgado hep-ph/ Look at symmetric & asymmetric gluon splittings (asym ~ like Vitev) p T trigger ~ p T associated restrict signal to a small number of splittings Smaller qhat & larger  radiated – gluons more collinear. So effects should disappear at smaller pTassoc at 62 than 200 GeV. can we say anything about this? Vitev does opacity expansion, they use BDMPS

25 September 2006Michael P. McCumber & Barbara Jacak 13 AdS/CFT correspondence of gravity in 5D string theory & field theory similar (but not identical) to QCD → field properties in limit of super strong coupling. Friess, et al. (hep-th/ ) stress tensor →wake of directional emission at p = several times the temperature see also Casalderry &Teaney (nucl-th/ ) Liu, Rajagopal, Wiedemann (hep-ph/ ) on qhat

25 September 2006Michael P. McCumber & Barbara Jacak 14 Figure 3 universal curve with N part ! data imply: away side jet splitting is a property of the medium, rather than the specific collision system successful models include strong medium response to jet