Heavy Ion Physics with CMS Bolek Wyslouch MIT. May 19 01Bolek Wyslouch2 Holy Grail of High Energy Nuclear Physics: Quark Gluon Plasma quarks and gluons,

Slides:



Advertisements
Similar presentations
Open beauty production in pp collisions at 7 TeV with CMS Kajari Mazumdar Tata Institute of Fundamental Research Mumbai, India. on behalf of CMS Collaboration,
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.
CMS Heavy Ion Physics Edwin Norbeck University of Iowa.
Jet probes of nuclear collisions: From RHIC to LHC Dan Magestro, The Ohio State University Midwest Critical Mass October 21-22, 2005.
Measurement of charmonia at mid-rapidity at RHIC-PHENIX  c  J/   e + e -  in p+p collisions at √s=200GeV Susumu Oda CNS, University of Tokyo For.
Results from PHENIX on deuteron and anti- deuteron production in Au+Au collisions at RHIC Joakim Nystrand University of Bergen for the PHENIX Collaboration.
A probe for hot & dense nuclear matter. Lake Louise Winter Institute 21 February, 2000 Manuel Calderón de la Barca Sánchez.
Relativistic Heavy-Ion Collisions: Recent Results from RHIC David Hardtke LBNL.
24/04/2007ALICE – Masterclass Presentation1 ALICE Hannah Scott University of Birmingham.
Winter Workshop on Nuclear Dynamics, Heavy Ion Physics with CMS: Day-One Measurements Olga Barannikova for the CMS Collaboration.
Identification of Upsilon Particles Using the Preshower Detector in STAR Jay Dunkelberger, University of Florida.
1 The CMS Heavy Ion Program Michael Murray Kansas.
ALICE EMCal Physics and Functional Requirements Overview.
March 1, 2003University of Rochester - Graduate Student Days1 Nuclear Physics at the University of Rochester Steven Manly Grad. Student Days March 1, 2003.
Formation and decay of resonances Motivation Formation time Resonance Correlation Summary and Future Plans Motivation Formation time Resonance Correlation.
Christina Markert Physics Workshop UT Austin November Christina Markert The ‘Little Bang in the Laboratory’ – Accelorator Physics. Big Bang Quarks.
The forward detectors of CMS Experiment at LHC Bolek Wyslouch MIT
RHIC program and machine performances Hugo Pereira Da Costa, CEA Saclay, PHENIX Collaboration, 3 Juillet 2006.
JSPS Research Fellow / University of Tsukuba T. Horaguchi Oct for HAWAII /10/15HAWAII
RHIC R.K. CHOUDHURY BARC. Relativistic Heavy Ion Collider at Brookhaven National Laboratory (BNL), USA World’s First Heavy Ion Collider became.
ISMD31 / Sept. 4, 2001 Toru Sugitate / Hiroshima Univ. The 31 st International Symposium on Multiparticle Dynamics on 1-7, Sept in Datong, China.
Sean Kelly, QWG 9/03 Prospects for Quarkonia Physics In Media at the LHC.
High p T  0 Production in p+p, Au+Au, and d+Au Stefan Bathe UC Riverside for the Collaboration Topics in Heavy Ion Collisions McGill University, Montreal,
Mark D. Baker What have we learned from RHIC? Mark D. Baker Chemistry Department Thanks to: W. Busza, Axel Drees, J. Katzy, B. Lugo, P. Steinberg, N. Xu,
Hard vs. Soft Physics at RHIC - Insights from PHENIX l Why hard vs. soft? l Soft physics: thermal, flow effects l Hard processes at RHIC l Conclusion Barbara.
An experimental perspective on first jet measurements at LHC: Lessons from RHIC Dan Magestro, The Ohio State University ALICE-USA Collaboration Meeting.
US participation in Heavy Ion Physics with Compact Muon Solenoid at LHC M. Ballintijn,K Barish,R Betts, BE Bonner, W.Busza, D.Cebra, G.Eppley, E.Garcia,
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.
J/psi production in Au+Au and Cu+Cu collisions at RHIC-PHENIX Susumu Oda (Doctor course student) Hamagaki group, CNS, University of Tokyo 2007/08/28 CISS07,
Summer Student Practice, Dubna, 2009 Analysis of UrQMD Data Obtained for Relativistic Au+Au Collisions at 17.3 GeV for STAR detector F. Nemulodi, M.W.
Quest for omega mesons by their radiative decay mode in √s=200 GeV A+A collisions at RHIC-PHENIX ~Why is it “Quest”?~ Simulation Study Real Data Analysis.
09/15/10Waye State University1 Elliptic Flow of Inclusive Photon Ahmed M. Hamed Midwest Critical Mass University of Toledo, Ohio October, 2005 Wayne.
Photon 2003Falk Meissner, LBNL Falk Meissner Lawrence Berkeley National Laboratory For the STAR Collaboration Photon 2003 April 2003 Coherent Electromagnetic.
Relativistic Heavy Ion Collider and Ultra-Dense Matter.
Jet Physics in ALICE Mercedes López Noriega - CERN for the ALICE Collaboration Hot Quarks 2006 Villasimius, Sardinia - Italy.
1 Jeffery T. Mitchell – Quark Matter /17/12 The RHIC Beam Energy Scan Program: Results from the PHENIX Experiment Jeffery T. Mitchell Brookhaven.
Hadron Collider Physics 2012, 12/Nov/2012, KyotoShinIchi Esumi, Univ. of Tsukuba1 Heavy Ion results from RHIC-BNL ShinIchi Esumi Univ. of Tsukuba Contents.
Heavy Ion Physics with CMS Russell Betts - UIC. Studying QCD with Heavy Ions Quark Gluon Plasma: –QCD at High T, High Density –Phase Diagram of QCD Strongly-Interacting.
Measurement of J/  -> e + e - and  C -> J/  +   in dAu collisions at PHENIX/RHIC A. Lebedev, ISU 1 Fall 2003 DNP Meeting Alexandre Lebedev, Iowa State.
Report from India Topical Conference on Hadron Collider Physics XIII Jan 14-20, TIFR, India Naohito Saito RIKEN/ RIKEN BNL Research Center.
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:
Presentation for NFR - October 19, Trine S.Tveter Recent results from RHIC Systems studied so far at RHIC: - s NN 1/2 = 
Pablo Yepes, Rice U 0 HI May 19, 2001May 19, CMS Heavy Ion Physics Pablo Yepes Rice University oHadronic Collisions sQuarkonia Production sJet Collisions.
LHC Heavy-Ion Program a CMS Perspective Edwin Norbeck University of Iowa for the CMS Collaboration 20 th Winter Workshop on Nuclear Dynamics CMS HI groups:
Heavy Ion Physics with the ATLAS detector Helio Takai Brookhaven National Laboratory IV INTERNATIONAL SYMPOSIUM ON LHC PHYSICS AND DETECTORS.
The ALICE Experiment Event by Event fluctuations ALICE TOF Calibration 30th November 2007Chiara Zampolli1.
D.Arkhipkin, Y. Zoulkarneeva, Workshop of European Research Group on Ultra relativistic Heavy Ion Physics March 9 th 2006 Transverse momentum and centrality.
News from ALICE Jan PLUTA Heavy Ion Reaction Group (HIRG) Warsaw University of Technology February 22, XIII GDRE Workshop, SUBATECH, Nantes.
January 15, 2004CMS Heavy Ions Bolek Wyslouch1 Bolek Wyslouch MIT for the CMS Collaboration Quark Matter 2004, Oakland, CA CMS HI groups: Athens, Auckland,
1 Heavy Ion Physics at CMS Prashant Shukla Nuclear Physics Division BARC, Mumbai India 28 th February 2011, BARC.
1 Probing dense matter at extremely high temperature Rudolph C. Hwa University of Oregon Jiao Tong University, Shanghai, China April 20, 2009.
Mass states of light vector mesons are considered to be sensitive probes of partial chiral symmetry restoration theoretically expected in high energy and/or.
1 First results from PbPb collisions at CMS Prashant Shukla Nuclear Physics Division BARC, Mumbai India CMS collaboration India-CMS Meeting, 17 January,
PHOBOS at RHIC 2000 XIV Symposium of Nuclear Physics Taxco, Mexico January 2001 Edmundo Garcia, University of Maryland.
July 27, 2002CMS Heavy Ions Bolek Wyslouch1 Heavy Ion Physics with the CMS Experiment at the Large Hadron Collider Bolek Wyslouch MIT for the CMS Collaboration.
 -jet measurements Table of Contents:  Motivation  Preliminary QA of  -trigger Data  Shower Shape Analysis  Experimental Challenges  Summary  
Elliptic Flow of Inclusive Photon Elliptic Flow of Inclusive Photon Ahmed M. Hamed Midwest Critical Mass University of Toledo, Ohio Oct. 22,
SPHENIX Mid-rapidity extensions: Additional Tracking system and pre-shower Y. Akiba (RIKEN/RBRC) sPHENIX workfest July 29,
V. Pozdnyakov Direct photon and photon-jet measurement capability of the ATLAS experiment at the LHC Valery Pozdnyakov (JINR, Dubna) on behalf of the HI.
PHENIX J/  Measurements at  s = 200A GeV Wei Xie UC. RiverSide For PHENIX Collaboration.
Ultra-peripheral heavy ion results from CMS Michael Murray, DIS2015, 29 th April 2015 CMS: HIN :
Non-Prompt J/ψ Measurements at STAR Zaochen Ye for the STAR Collaboration University of Illinois at Chicago The STAR Collaboration:
Recent Results from ALICE E. Vercellin Dipartimento di Fisica dell’Università di Torino and INFN Torino.
Review of ALICE Experiments
Probing Quark Matter in the PHENIX Experiment at RHIC
Jet Physics in Heavy Ion Collisions with the ALICE Detector at the LHC
Jet Measurements with the EMCal of ALICE
Introduction of Heavy Ion Physics at RHIC
First Hints for Jet Quenching at RHIC
Dipartimento Interateneo di Fisica, Bari (Italy)
Presentation transcript:

Heavy Ion Physics with CMS Bolek Wyslouch MIT

May 19 01Bolek Wyslouch2 Holy Grail of High Energy Nuclear Physics: Quark Gluon Plasma quarks and gluons, the fundamental constituents of matter, are no longer confined within the dimensions of the nucleon, but free to move around over a volume in which a high enough temperature and/or density prevails plasma also exhibits the so-called "chiral symmetry" which in normal nuclear matter is spontaneously broken, resulting in effective quark masses which are much larger than the actual masses. Basically: physics of condensed nuclear matter: phase changes due to multiple interactions of energetic quarks and gluons

May 19 01Bolek Wyslouch3 p n z partons plasma mixed thermalisation hadronization freeze-out chiral symmetry thermal equilibrium chemical equilibrium deconfinement  k   t hadrons mass and width of resonances () thermal photons or dileptons (e + e    +   ) strangeness enhancement (K  energy loss of initial partons (jet quenching) suppression of heavy-quark bound states (J/, ’s  +   ) Particle production in Heavy Ion collision The “probes”

May 19 01Bolek Wyslouch4 Hard probes: cc, bb, jets High mass or high momentum objects created during formation phase via high Q 2 parton scattering Penetrate hot and dense matter Sensitive to state of hot and dense matter –Color screening –dE/dx by strong interactions Vacuum QGP ????? Quarkonia, Jets High pt particles J/  suppressed ?  ’/  ratio ?

May 19 01Bolek Wyslouch5 Today’s Experiments Relativistic Heavy Ion Collider on Long Island, a dedicated facility: –Collisions of Au-Au with up to 100 AGeV in each beam –Four Experiments: Brahms, Phenix, Phobos, Star So far about 1-2 weeks of data This year ~9 months Running 6-9 months per year Building on CERN/SPS results

May 19 01Bolek Wyslouch6 Recent results from RHIC Global features: charged multiplicity, particle production asymmetry (flow) indicate significant increase of energy density compared to pp Indication of importance of “hard probes” –Jet production may be suppressed (quenched), production of high pt particles is smaller than expected from pp Looking forward to see J/psi production at RHIC, suppression observed at SPS…

May 19 01Bolek Wyslouch7 Charged multiplicity at mid-rapidity

May 19 01Bolek Wyslouch8 Missing high pt particles at RHIC ? Effect seems to be stronger than “Cronin effect” observed in pA

May 19 01Bolek Wyslouch9 What to expect from RHIC within the next few years A very detailed study of most if not all “QGP signatures” at RHIC Many beam energies, ion species, very high luminosity But: maximum energy at RHIC is limited by ring radius and magnets Some measurements, especially high pt probes may require higher energies: LHC

May 19 01Bolek Wyslouch10 What To Expect from LHC LHC (Large Heavy ion Collider) is expected to provide pA and AA collisions. Energy: 5.5 GeV per nucleon pair in PbPb 6 weeks/year First heavy ion run in March 2007

May 19 01Bolek Wyslouch11 Main emphasis: Identified particles at low pt Add-ons for high pt physics

May 19 01Bolek Wyslouch12 CMS: High pt edge of HI physics

May 19 01Bolek Wyslouch13 Some CMS Assets of interest to HI CMS has excellent muon detection capabilities: –||<1.3 for barrel and ||<2.4 with endcaps. –Good mass resolution: 46 MeV for the Upsilon. –Efficient suppression of background from /K decays: Electromagnetic calorimeter at 1.3 m from beam axis. P T threshold at 3.5 GeV/c for a single muon to reach the -chambers. Large calorimeter coverage with good jet reconstruction capabilities.

May 19 01Bolek Wyslouch14 Selected Physics Topics first physics studies by CMS Event Characterization (centrality) Quarkonium Production: Upsilon and J/in the barrel Z detection Jet Production: –Single/Double jet ratios, jet quenching –Z and  tagged jets Ultra-Peripheral Collisions:  and - Pomeron Muon detector Calorimetry Studies conducted by existing HI group in CMS Pablo Yepes will present the details

May 19 01Bolek Wyslouch15 Stretching CMS Pb-Pb Detector designed for pp. However due to flexible design offers unique capabilities for AA   

May 19 01Bolek Wyslouch16 Centrality: Participants vs. Spectators “Spectators” Zero-degree Calorimeter “Spectators” Many things scale with N part : Transverse Energy Particle Multiplicity Particle Spectra “Participants” Only ZDCs measure N part Detectors at 90 o The collision geometry (i.e. the impact parameter) determines the number of nucleons that participate in the collision

May 19 01Bolek Wyslouch17 Event Characterization In spite of very strong magnetic field (4 Tesla) there is a good correlation between centrality and transverse energy.

May 19 01Bolek Wyslouch18 Alternative “centrality trigger” “Zero degree calorimeter” –Small fast calorimeters sensitive to forward neutrons –Very forward region, between two vacuum beam lines –Working at RHIC –Same design can be adopted for LHC Could be essential for some measurements

May 19 01Bolek Wyslouch19 Will the DAQ cope with the HI ? Pb-Pb at L=10 27 cm -2 s -1 (2 experiments running at the time) LHC HI is relatively low luminosity but the occupancy can be huge, O(100,000) particles Expected event size ~1.5 M Bytes (or larger, needs study) With mass storage of 100 MBytes/s one can write ~70 events/s

May 19 01Bolek Wyslouch20 Needs dedicated, continuing studies DAQ and trigger: configuration, length of DAQ buffers, trigger thresholds –Most likely need to be reconfigured for the HI run Lower magnetic field ? –Better jet acceptance –Lower pt threshold for J/psi (?) –functioning of trigger etc

May 19 01Bolek Wyslouch21 Software for Heavy Ion Collisions A real challenge ! PbPb min bias Multiplicity: dNch/dh=1500 time: 6 hours/ev space: 500Mb/ev For 3000 events (0.5 sec LHC) ~3 years for PII 400 MHz ~2Tb disk space. -> minimum 36 computers (for 1 month run). Example: Small MC PRODUCTION in 2001 The most interesting events are central dNch/dy=8000 (dNch/dh=6000). The time and the space will be ~24h/ev and ~2Gb/ev.

May 19 01Bolek Wyslouch22 US Politics CMS has a great potential to do good physics during Heavy Ion runs at LHC US Nuclear physics community endorsed US participation in LHC heavy ion program (NSAC Long Range Plan) Positive signs from DoE/Nuclear But no miracles: RHIC is big and very hungry Some of our colleagues prefer Alice CMS Heavy ion group: Lyon, Moscow, St. Petersburg, Dubna From the US: Rice, UC Davis Several US groups are considering participation (MIT, UIC, your colleagues) Schedule and level of participation are driven by RHIC commitments

May 19 01Bolek Wyslouch23 Schedule and Resources First HI run will be in 2007 Needed to get good HI physics in 2007: –Physics studies –DAQ, Trigger and software preparation –Zero-degree calorimeter construction There will be solid physics base learned at RHIC

May 19 01Bolek Wyslouch24 Possible plan Involvement in direct simulation and physics preparation work, ramping up in Involvement in US CMS computing together with HEP groups DoE Nuclear funding for Tier-2(+) size computing resources

May 19 01Bolek Wyslouch25 Summary LHC will be a natural continuation of the series of Heavy Ion accelerators CMS will have unique capabilities at the high transverse momentum frontier –, Z 0, , high pt jets CMS can provide a natural place to do these measurements in the late-RHIC and post-RHIC era Complementary to RHIC