Some Questions about QGP July 2004. Basic Question Has Quark-Gluon Plasma been observed? or When and How will it be observed? The answer depends on the.

Slides:



Advertisements
Similar presentations
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.
Advertisements

Supported by DOE 11/22/2011 QGP viscosity at RHIC and LHC energies 1 Huichao Song 宋慧超 Seminar at the Interdisciplinary Center for Theoretical Study, USTC.
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.
The Phase Diagram of Nuclear Matter Oumarou Njoya.
Heavy Quark Probes of QCD Matter at RHIC Huan Zhong Huang University of California at Los Angeles ICHEP-2004 Beijing, 2004.
Forward-Backward Correlations in Relativistic Heavy Ion Collisions Aaron Swindell, Morehouse College REU 2006: Cyclotron Institute, Texas A&M University.
The speed of sound in a magnetized hot Quark-Gluon-Plasma Based on: Neda Sadooghi Department of Physics Sharif University of Technology Tehran-Iran.
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.
Relativistic Heavy-Ion Collisions: Recent Results from RHIC David Hardtke LBNL.
24/04/2007ALICE – Masterclass Presentation1 ALICE Hannah Scott University of Birmingham.
J/  nuclear modification factor in nucleus-nucleus collisions Xiao-Ming Xu.
1 Questions about sQGP Carlos Arguello Columbia University 24 th Winter Workshop on Nuclear Dynamics April 10 th 2008.
Quark recombination in high energy collisions for different energies Steven Rose Worcester Polytechnic Institute Mentor: Dr. Rainer Fries Texas A&M University.
200 GeV Au+Au Collisions, RHIC at BNL Animation by Jeffery Mitchell.
Identification of Upsilon Particles Using the Preshower Detector in STAR Jay Dunkelberger, University of Florida.
Has the critical temperature of the QCD phase transition been measured ?
Formation and decay of resonances Motivation Formation time Resonance Correlation Summary and Future Plans Motivation Formation time Resonance Correlation.
DPG spring meeting, Tübingen, March Kai Schweda Lawrence Berkeley National Laboratory for the STAR collaboration Recent results from STAR at RHIC.
Finite Size Effects on Dilepton Properties in Relativistic Heavy Ion Collisions Trent Strong, Texas A&M University Advisors: Dr. Ralf Rapp, Dr. Hendrik.
Output from this Series of Workshops: A science vision for the RHIC future 1.Provide a science case for the future RHIC program that makes clear its importance.
1 Debye screened QGP QCD : confined Chiral Condensate Quark Potential Deconfinement and Chiral Symmetry restoration expected within QCD mm symmetryChiral.
Christina Markert Physics Workshop UT Austin November Christina Markert The ‘Little Bang in the Laboratory’ – Accelorator Physics. Big Bang Quarks.
New States of Matter and RHIC Outstanding questions about strongly interacting matter: How does matter behave at very high temperature and/or density?
Frontiers of Nuclear Physics A Personal Outlook Huan Zhong Huang Department of Physics and Astronomy University of California, Los Angeles Department of.
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.
Relativistic Heavy Ion Physics: the State of the Art.
In-medium hadrons and chiral symmetry G. Chanfray, IPN Lyon, IN2P3/CNRS, Université Lyon I The Physics of High Baryon Density IPHC Strasbourg, september.
QCD Thermodynamics Jean-Paul Blaizot, CNRS and ECT* RHIC Physics in the Context of the Standard Model RBRC June 21,
A SCENIC OVERVIEW OF J/  PRODUCTION IN HEAVY ION COLLISIONS AT PHENIX Matthew Wysocki, University of Colorado For the PHENIX Collaboration.
T BB Hadronic matter Quark-Gluon Plasma Chiral symmetry broken Chiral symmetry restored Early universe A new view and on the QCD phase diagram Recent.
Axel Drees, Stony Brook University, Lectures at Trento June 16-20, 2008 Electromagnetic Radiation form High Energy Heavy Ion Collisions I.Lecture:Study.
EXPERIMENTAL EVIDENCE FOR HADRONIC DECONFINEMENT In p-p Collisions at 1.8 TeV * L. Gutay - 1 * Phys. Lett. B528(2002)43-48 (FNAL, E-735 Collaboration Purdue,
Chiral phase transition and chemical freeze out Chiral phase transition and chemical freeze out.
Relativistic Heavy Ion Collider and Ultra-Dense Matter.
Quark-Gluon Plasma Sijbo-Jan Holtman.
Some Questions about QGP August Basic Question Has Quark-Gluon Plasma been observed? The answer depends on definition. A proper definition should.
How To See the Quark-Gluon Plasma
Physics of Dense Matter in Heavy-ion Collisions at J-PARC Masakiyo Kitazawa J-PARC 研究会、 2015/8/5 、 J-PARC.
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:
Holographic QCD in the medium
Heavy Ions at the LHC Theoretical issues Super-hot QCD matter What have we learned from RHIC & SPS What is different at the LHC ? Goals of HI experiments.
And Mesons in Strange Hadronic Medium at Finite Temperature and Density Rahul Chhabra (Ph.D student) Department Of Physics NIT Jalandhar India In cooperation.
Olena Linnyk Charmonium in heavy ion collisions 16 July 2007.
The Quark-Gluon Plasma Marco van Leeuwen. 2 Elementary particles Atom Electron elementary, point-particle Protons, neutrons Composite particle  quarks.
Strange Probes of QCD Matter Huan Zhong Huang Department of Physics and Astronomy University of California Los Angeles, CA Oct 6-10, 2008; SQM2008.
Results from ALICE Christine Nattrass for the ALICE collaboration University of Tennessee at Knoxville.
24 Nov 2006 Kentaro MIKI University of Tsukuba “electron / photon flow” Elliptic flow measurement of direct photon in √s NN =200GeV Au+Au collisions at.
1 QCD at high T Future Opportunities in QCD SURA, December 15-16, 2006 The future is not what it used to be. Yogi Berra.
D ECONFINING E FFECTS AND D ISSOCIATION T EMPERATURE OF Q UARKONIA S TATES Palak D. Bhatt Sardar Patel University, Vallabh Vidyanagar 2 nd Heavy Flavour.
What have we learned from the RHIC experiments so far ? Berndt Mueller (Duke University) KPS Meeting Seoul, 22 April 2005.
Quark Gluon Plasma Presented by: Rick Ueno Welcome to the presentation of:
Axel Drees, University Stony Brook, PHY 551 S2003 Heavy Ion Physics at Collider Energies I.Introduction to heavy ion physics II.Experimental approach and.
Elliptic flow from initial states of fast nuclei. A.B. Kaidalov ITEP, Moscow (based on papers with K.Boreskov and O.Kancheli) K.Boreskov and O.Kancheli)
Review of ALICE Experiments
The 'Little Bang’ in the Laboratory - Physics at the LHC
for the ALICE collaboration University of Tennessee at Knoxville
Workshop on the physics of HL-LHC, and perspectives at HE-LHC
Probing Quark Matter in the PHENIX Experiment at RHIC
QCD (Quantum ChromoDynamics)
Heavy-Flavour Physics in Heavy-Ion Collisions
Special UCLA Nuclear Physics Seminar
Charm production at STAR
Current status of Thermalization from available STAR results
From Particle Data Book
QGP at RHIC: Seen through Modified Jet Fragmentation
of Hadronization in Nuclei
QCD and Heavy-ion Collisions
Introduction of Heavy Ion Physics at RHIC
Identified Particle Production at High Transverse Momentum at RHIC
Presentation transcript:

Some Questions about QGP July 2004

Basic Question Has Quark-Gluon Plasma been observed? or When and How will it be observed? The answer depends on the definition. A proper definition should catch the essential points.

Question 1: What is Plasma ?

2 kinds of plasma EM Plasma QG Plasma T - ρplot Normal Matter Nor- mal Mat- ter Plasma In normal matter Charge is bounded Colour is confined In Plasma Charge and Colour can move freely

EM Plasma Definition: Consists of a collection of free- moving electrons and ions Ions and Electrons move independently.

Some Examples of EM Plasma Tokamak plasma in action Princeton Plasma Physics Laboratory Nebula M1-67 a massive stellar wind NASA High-intensity plasma arc lamp Courtesy of OSRAM Sylvania, Danvers, MA Atmospheric Plasma Courtesy of J. Elston Litmas No (local) equilibrium is demanded for a plasma. Some of these plasmas are in or near thermal equilibrium, but some are not.

Question 2: Why RHIC ?

Workshop on BeV/n collisions of heavy ions – how and why, Bear Mountain, 1974

T.D.Lee & G. C. Wick Lee emphasized, whether the vacuum is a medium whose properties one could change; "we should investigate," he pointed out, “... by distributing high energy or high nucleon density over a relatively large volume." If in this way one could restore broken symmetries of the vacuum, then it might be possible to create abnormal dense states of nuclear matter

Our ultimate goal in doing Relativ. Heavy Ion Coll. is to Change the QCD vacuum Librate the confined quark-gluon Restore the chiral symmetry No (local) equilibrium is demanded too

The Definition of QGP A (locally) thermally equilibrated state of matter in which quarks and gluons are deconfined from hadrons, so that color degrees of freedom become manifest over nuclear, rather than merely nucleonic, volumes. The Prevalent DefinitionShould be changed into: hot and dense

X-N Wang ’ s Criteria: High density: є >> є C Large volume: V >> λ (mean-free-path) Long life-time: t >> λ Parton degrees of freedom Local thermal equilibration (interaction) approximately Debye screening of strong interaction: deconfinement Should be changed into: Multiple scattering (interaction) between partons (collective behavior)

Question 3: Has Quark DoF been observed yet? Has Color Deconfinement been observed yet? or

Direct Evidence v 2 scaling Parton recombination Partonic degrees of freedom The n’s here count the number of quarks that flowed. V 2 scaling tells us that they are the constituent quarks that started to flow at the early stage of collision. Constituent Quark Degree of Freedom

If this were the case, then all the flowing quarks would contribute to v 2 and the numbers of quarks in baryon and meson would not be 3 and 2 any more. The scaling breaks down. n >>3 Some model says that originally the current quarks flow, and they recombine into constituent quarks before hadronization.

Questions Are they really the constituent quarks that flow ? Is it the constituent quark DoF that shows up at the early stage of collision ? What kind of vacuum is that? We still cannot say for sure that Quark DoF has been observed.

Conclusion

Never forget that our ultimate goal in doing Relativ. Heavy Ion Coll. is to: Change the QCD vacuum Librate the confined quark-gluon Restore the chiral symmetry Our main effort should be concentrated in finding out direct, model-independent evidences for these 3 points.

The other properties of the produced system, e.g. thermalized or not are worthwhile investigating. But the results of this investigation do not affect the discovery or non-discovery of QGP.

Thanks!

A model-independent evidence of such a state of matter would be a great discovery. It would mean: The QCD vacuum has been successfully changed The Color Confinement has been successfully broken This discovery will become a milestone in the development of physics

Other Questions like Whether or not there is (local)equilibrium? Why there seems to be an expansion, but at the same time the volume measured by HBT is unchanged? ? can be left for further study.