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Quark-Gluon Plasma Presented by: Paul Pryor and Michael Byrd December 8, 2010
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Overview Definitions Theory Signatures Detection Results 2
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Quark-Gluon Plasma Increasing the temperature of the hadronic system eventually leads to complete dissociation of quarks and gluons 3 full-energy collisions between gold ions at Brookhaven Lab's Relativistic Heavy Ion Collider (RHIC), as captured by the Solenoidal Tracker at RHIC (STAR) detector.
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Where do we stand? 4 Atoms Protons, neutrons, and electrons Baryons and mesons quarks Interaction Particles AffectedRange Relative Strength Particles ExchangedRole in Universe Strong Quarks ~10 -15 m1 Gluons Holds quarks together to form nucleons HadronsMesons Holds nucleons together to form atomic nuclei Electro- magnetic Charged particles ∞~10 -2 mPhotons Determines structures of atoms, molecules, solids, and liquids; is important factor in astronomical universe Weak Quarks and leptons ~10 -18 m~10 -5 m Intermediate bosons Mediates transformation of quarks and leptons; helps determine compositions of atomic nuclei GravitationalAll∞~10 -39 mGravitons Assembles matter into planets, stars, and galaxies
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Strong force 5 Primary expression The level between quarks Produces quark confinement color gluons Secondary expression The level between baryons flavor mesons
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Baryons and Mesons 6 Baryons Mass carriers Composed of three quarks Mesons Composed of a quark antiquark pair Alternative charge (flavor) carriers http://newscenter.lbl.gov/feature-stories/2010/01/14/jet/#hide
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There is an octet of ½ + baryons (1/2= spin, + = odd parity): - isospins of the same multiplet 7
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Quarks and Gluons Quarks Fermions Carry Color charge charges of ± 1/3e or ± 2/3e Gluons massless the mediator of color interactions carries color-anticolor charge quanta Absolute confinement 8
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Plasma A fully ionized gas 9
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Quantum Chromodynamics (QCD) The dynamical theory of quarks and gluons that describes color interactions Parton model 10
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QCD Phase Diagram 11
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Theory of strong interactions 12 QCD 4D SU (3) gauge theory Describes the interactions of quarks and gluons QCD is defined through the Lagrangian D - Dirac operator N f - Flavors Ψ f - Quark fields
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Hydrodynamics Perfect liquid Perfect gas 13
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Signatures 14 Enhancement of strangeness forward angles large rapidity measurements y= 5 – 8 Observables give information about different stages of the collision
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Post-plasma Observable 15 Detection of final state particles frozen out of the hot collision zone Freeze out
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Why look? 16 Help prove the validity of QCD If QGP is a reality, its further study may give insight into the processes of the early universe
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Experiment Signatures & Detection
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1. Jet Quenching Jet—a narrow cone of hadrons and other particles produced by the hadronization of a quark or gluon in a heavy ion experiment According to QCD, matter undergoing a phase crossover into quark gluon plasma losses significant energy, which effectively quenches the outgoing jet Strong suppression of inclusive hadron production Disappearance of the away-side jet Pedestal&flow subtracted Experimental Results 18
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2. Strangeness Strange quarks are not brought into the reaction by the colliding nuclei Strange quarks or antiquarks are made from the kinetic energy of colliding nuclei Strange quarks are naturally radioactive and decay by weak interactions into lighter quarks which can be detected relatively easily (Xi baryon(dss) into a pion(d) and a Lambda baryon(uds)) Experimental Results Cont. 19
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Relativistic Heavy Ion Collider Complex 1.Tandem Van de Graaff2a. Tandem-to-Booster line (TTB)2b. Linear Accelerator (Linac)3. Booster Synchrotron - 37% the speed of light 4. Alternating Gradient Synchrotron - 99.7% the speed of light 5. AGS-to-RHIC Line6. RHIC - 2.4 mile ring - six intersection points 20
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Detectors 21
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Solenoidal Tracker at RHIC (STAR) 22
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1. Time Projection Chamber Strong E-field: 130V/cm Multi-wire proportional chamber end caps Drift Gas: Argon/methane mixture (90:10) @ 1atm. 2. Silicon Vertex Tracker Res.:18 million pixels (72576 channels x 256 time samples) capabilities below transverse momenta of 150 MeVIc Sub-detectors 23
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3. Electromagnetic Calorimeter (EMC) Energy Deposition Measurements 4. Time-of-Flight (TOF) Detector Shingle design Tiled outer TPC cage w/ 7716 single ended scintillators in 216 trays 5. External Time-Projection Chambers (TPC) Sub-detectors Cont. 24
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What now? 25 Discovery of QGP not yet conclusive because signatures are indirect results predicted by theory Develop methods and hardware for direct detection of total deconfinement Determine if and where a definite transition exists Charm production Charm quarks, unlike the strange quarks, are predicted to be produced early in QGP formation at sufficient energies Looking to the LHC at CERN for detection
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STAR Collaboration Institutions (49) Argonne National Laboratory, Argonne, Illinois 60439, USA University of Bern, 3012 Bern, Switzerland University of Birmingham, Birmingham, United Kingdom Brookhaven National Laboratory, Upton, New York 11973, USA California Institute of Technology, Pasadena, California 91125, USA University of California, Berkeley, California 94720, USA University of California, Davis, California 95616, USA University of California, Los Angeles, California 90095, USA Carnegie Mellon University, Pittsburgh, Pennsylvania 15213, USA Creighton University, Omaha, Nebraska 68178, USA Nuclear Physics Institute AS CR, 250 68 ˇ Reˇz/Prague, Czech Republic Laboratory for High Energy (JINR), Dubna, Russia Particle Physics Laboratory (JINR), Dubna, Russia University of Frankfurt, Frankfurt, Germany Institute of Physics, Bhubaneswar 751005, India Indian Institute of Technology, Mumbai, India Indiana University, Bloomington, Indiana 47408, USA Institut de Recherches Subatomiques, Strasbourg, France University of Jammu, Jammu 180001, India Kent State University, Kent, Ohio 44242, USA Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA Massachusetts Institute of Technology, Cambridge, MA 02139-4307 Max-Planck-Institut f¨ur Physik, Munich, Germany Michigan State University, East Lansing, Michigan 48824, USA Moscow Engineering Physics Institute, Moscow Russia City College of New York, New York City, New York 10031, USA NIKHEF and Utrecht University, Amsterdam, The Netherlands Ohio State University, Columbus, Ohio 43210, USA Panjab University, Chandigarh 160014, India Pennsylvania State University, University Park, Pennsylvania 16802, USA Institute of High Energy Physics, Protvino, Russia Purdue University, West Lafayette, Indiana 47907, USA University of Rajasthan, Jaipur 302004, India Rice University, Houston, Texas 77251, USA Universidade de Sao Paulo, Sao Paulo, Brazil University of Science & Technology of China, Anhui 230027, China Shanghai Institute of Applied Physics, Shanghai 201800, China SUBATECH, Nantes, France Texas A&M University, College Station, Texas 77843, USA University of Texas, Austin, Texas 78712, USA Tsinghua University, Beijing 100084, China Valparaiso University, Valparaiso, Indiana 46383, USA Variable Energy Cyclotron Centre, Kolkata 700064, India Warsaw University of Technology, Warsaw, Poland University of Washington, Seattle, Washington 98195, USA Wayne State University, Detroit, Michigan 48201, USA Institute of Particle Physics, CCNU (HZNU), Wuhan 430079, China Yale University, New Haven, Connecticut 06520, USA University of Zagreb, Zagreb, HR-10002, Croatia 26
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Sources Adams, J. et al. The STAR Collaboration’s Critical Assessment of the Evidence from RHIC Collisions. Tech. 2008. Print Beddo, M. E. et al. STAR Conceptual Design Report. Tech. no. 5347. Print. Braun-Munzinger, Peter, and Johanna Stachel. "The Quest for the Quark– gluon Plasma." Nature 448 (2007): 302-09. Web. 15 Nov. 2010. "Quark–gluon Plasma." Online Reference - Information Articles & Reference Resources. Web. 22 Nov. 2010.. 27
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