Centrality Dependence of Charged Antiparticle to Particle Ratios from Abigail Bickley Univ. of Maryland, Chemistry Dept. for the Collaboration DNP, October.

Slides:



Advertisements
Similar presentations
ICHEP 2002, AmsterdamGerrit van Nieuwenhuizen/MIT Scaling of Charged Hadron p T distributions in Au+Au collisions at 200 GeV Gerrit van Nieuwenhuizen MIT.
Advertisements

Tokaj, Hungary, March 17, 2008Gábor VeresHigh-p T physics at the LHC, Tokaj ’08 1 Correlations with a high-p T trigger over a broad η range Gábor Veres.
Peter Steinberg PHOBOS The Landscape of Particle Production: Results from. Peter Steinberg Brookhaven National Laboratory SPS FNALRHICSppS AGS.
Gunther Roland - MITPHOBOS QM2005 Structure and Fine Structure of Hadron Production at RHIC Gunther Roland Massachusetts Institute of Technology New Results.
Gunther Roland - MITPHOBOS ISMD’05 3 Remarks on Fluctuations in Hadron Production at RHIC Gunther Roland Massachusetts Institute of Technology New Results.
Systematics of Soft Particle Production at RHIC: George S.F. Stephans Massachusetts Institute of Technology Lessons from (And some thoughts for the future)
S. Manly – U. Rochester Quark Matter, Budapest, Hungary - August System size, energy and  dependence of directed and elliptic flow Steven Manly.
Rachid Nouicer1 The Latest Results from RHIC Rachid NOUICER University of Illinois at Chicago and Brookhaven National Laboratory for the Collaboration.
Gábor Veres Strangeness in Quark Matter ‘06, UCLA, March 27, Strangeness measurements with the Experiment Gábor Veres Eötvös Loránd University,
S. Manly – U. Rochester Gordon Conf. 2006, New London, New Hampshire1 The simple geometric scaling of flow – perhaps it’s not so simple after all Steven.
S. Manly – U. Rochester Xi’an, China, Nov. 23, The eccentricities of flow S. Manly University of Rochester International Workshop on Hadron Physics.
Conor Henderson, MIT APS April 2001 Measurement Of Charged Antiparticle To Particle Ratios by the PHOBOS Experiment at RHIC Conor Henderson Massachusetts.
Charged particle multiplicity studies with PHOBOS Birger Back Argonne National Laboratory for the PHOBOS Collaboration.
Results from PHOBOS at RHIC David Hofman University of Illinois at Chicago For the Collaboration European Physical Society HEP2005 International Europhysics.
Multiplicity Fluctuations in 200 GeV Au-Au Collisions Zhengwei Chai Brookhaven National Laboratory for the Collaboration APS April Meeting, Denver, 2004.
1 - S. Manly, Univ. of Rochester APS - Washington D.C. - April 2001 Results from the PHOBOS experiment at RHIC Steve Manly (Univ. of Rochester) for the.
Gábor I. VeresQuark Matter 2006, Shanghai, November 14-20, Anti-particle to particle ratios in p+p, Cu+Cu and Au+Au collisions at RHIC Gábor I.
Gábor I. Veres Massachusetts Institute of Technology for the Collaboration International Workshop on Hot and Dense Matter in Relativistic Heavy Ion Collisions.
Update on flow studies with PHOBOS S. Manly University of Rochester Representing the PHOBOS collaboration Flow Workshop BNL, November 2003.
Femtoscopy BNL Workshop 6/21/2005George Stephans Very Low p T in x Past, Present, and Prospects.
Performance of the PHOBOS Trigger Detectors in 200 GeV pp Collisions at RHIC Joseph Sagerer University of Illinois at Chicago for the Collaboration DNP.
Wit Busza DoE Review of RHIC Program 9 July 2003.
Christof Roland/MITMoriond,March, Results from the PHOBOS experiment at RHIC Christof Roland (MIT) for the PHOBOS Collaboration.
Measuring Mid-Rapidity Multiplicity in PHOBOS Aneta Iordanova University of Illinois at Chicago For the collaboration.
Centrality measurement and the centrality dependence of dN charged /d  at mid-rapidity Judith Katzy (MIT) for the PHOBOS collaboration.
Birger Back/ANLBreckenridge, Feb 5-12, Recent results from PHOBOS Birger Back Argonne National Laboratory for the PHOBOS Collaboration.
Multiplicity as a measure of Centrality in Richard S Hollis University of Illinois at Chicago.
Conor Henderson, MIT Division of Nuclear Physics, Chicago, 2004 Charged Hadron p T Spectra from Au+Au at  s NN = 62.4 GeV Conor Henderson, MIT For the.
EPS Meeting AachenGerrit van Nieuwenhuizen Charged Particle Production in Au+Au at RHIC Gerrit van Nieuwenhuizen Massachusetts Institute of Technology.
Anti-particle to Particle Ratios in Cu+Cu RHIC Vasundhara Chetluru University of Illinois, Chicago For the collaboration Division of Nuclear.
Limiting Fragmentation Observations at Richard S Hollis University of Illinois at Chicago For the Collaboration.
Performance of PHOBOS Vertex Finders in 200GeV pp Collisions at RHIC Richard S Hollis University of Illinois at Chicago For the PHOBOS Collaboration Fall.
Phobos Collaboration and Management Wit Busza Phobos Technical Cost and Schedule Review November 1998.
Phobos at RHIC Edmundo Garcia University of Illinois at Chicago for the PHOBOS Collaboration IV Latin American Symposium on Nuclear Physics Mexico City.
Latest Results From PHOBOS David Hofman University of Illinois at Chicago.
Rachid Nouicer1 University of Illinois at Chicago and Brookhaven National Laboratory for the Collaboration Seminar at BNL November 14, 2003 The Latest.
RHIC PHENOMENOLOGY AS SEEN BY Wit Busza QCD in the RHIC Era UCSB, April 2002.
Charged Particle Multiplicity Measurement in 200 GeV pp Collisions with PHOBOS Joseph Sagerer University of Illinois at Chicago for the Collaboration DNP.
Peter Steinberg Universal Behavior of Charged Particle Multiplicities in Heavy-Ion Collisions Peter Steinberg Brookhaven National Laboratory for the PHOBOS.
October 2005K.Woźniak TIME ‘ Vertex Reconstruction Algorithms in the PHOBOS Experiment at RHIC Krzysztof Woźniak for the PHOBOS Collaboration Institute.
Centrality Dependence of Charged Hadron Production at RHIC d+Au vs Au+Au Gunther Roland/MIT for the PHOBOS Collaboration BNL June 18, 2003.
Charged particle multiplicities from Cu+Cu, Au+Au and d+Au collisions at RHIC Richard S Hollis University of Illinois at Chicago detailed distribution:
Results from the Experiment at RHIC Abigail Bickley University of Maryland For the Collaboration Topics in Heavy Ion Collisions June 25-28, 2003, Montreal.
Recent Results from PHOBOS David Hofman – UIC For the Collaboration AGS/RHIC Users Meeting May 15-16, 2003, BNL.
(B) Find N part for d+Au collisions? 0-10%10-20%40-60%100-80% Aneta Iordanova University of Illinois at Chicago N part Determination and Systematic Studies.
1 1 Rachid Nouicer - BNL PHOBOS QM Energy and Centrality Dependence of Directed and Elliptic Flow in Au+Au and Cu+Cu Collisions at RHIC Energies.
PHOBOS WHITE PAPER REPORT Wit Busza on behalf of the PHOBOS Collaboration White paper report, June 2004.
RHIC results on cluster production in pp and heavy ion George S.F. Stephans Massachusetts Institute of Technology For the Collaboration.
Status of the Phobos experiment at RHIC S.Manly Univ. of Rochester ( for the Phobos Collaboration APS - Atlanta.
Spectrometer Based Ratio Analysis Technique Discussion of Corrections Absorption Correction – As the collision products pass through the detector, some.
Peter Steinberg Systematics of Charged Particle Production in 4  with the PHOBOS Detector at RHIC Peter A. Steinberg Brookhaven National Laboratory George.
For the Collaboration Charged Hadron Spectra and Ratios in d+Au and Au+Au Collisions from PHOBOS Experiment at RHIC Adam Trzupek The Henryk Niewodniczański.
S.Manly - RHIC Park City 3/00 Status of the Phobos experiment at RHIC S.Manly Univ. of Rochester ( for the.
For the Collaboration Low-p T Spectra of Identified Charged Particles in  s NN = 200 GeV Au+Au Collisions from PHOBOS Experiment at RHIC Adam Trzupek.
Gerrit J. van Nieuwenhuizen For the PHOBOS collaboration Experience & Upgrade RHIC future detectors R&D Workshop Brookhaven National Laboratory November.
1 1 Rachid Nouicer - BNL PHOBOS PANIC Global Observables from Au+Au, Cu+Cu, d+Au and p+p Collisions at RHIC Energies Rachid NOUICER Brookhaven National.
THE PHOBOS EXPERIMENT AT RHIC Judith Katzy for the PHOBOS Collaboration.
VERTEX2003, Low Hall, Cumbria The PHOBOS Detector “Design, Experience and Analysis” RUSSELL BETTS for The PHOBOS Collaboration.
Russell Betts (UIC) for the PHOBOS Collaboration Multiplicity Measurements with The PHOBOS Detector 18 th Winter Workshop on Nuclear Dynamics Nassau, Jan.
For the Collaboration Adam Trzupek The Henryk Niewodniczański Institute of Nuclear Physics Polish Academy of Sciences Kraków, Poland The 2007 Europhysics.
1 V Latin American Symposium on Nuclear Physics Brasil, Setembro 2003 Edmundo García University of Illinois at Chicago for the PHOBOS collaboration Recent.
Hadron Spectra from Gábor I. Veres / MIT for the PHOBOS Collaboration.
Properties of charged-particle production at mid-rapidity for Au+Au collisions at RHIC Aneta Iordanova University of Illinois at Chicago.
Centrality Dependence of Charged Antiparticle to Particle Ratios Near Mid-Rapidity in d+Au Collisions at √s NN = 200 GeV Abigail Bickley Univ. of Maryland,
June 18, 2004BNL - Elliptic Flow, S. Manly1 Au-Au event in the PHOBOS detector Energy dependence of elliptic flow over a large pseudorapidity range in.
Particle production in nuclear collisions over a broad centrality range Aneta Iordanova University of Illinois at Chicago for the PHOBOS collaboration.
Conor Henderson, MIT Strangeness Production in PHOBOS Conor Henderson Massachusetts Institute of Technology For the PHOBOS Collaboration RHIC/AGS Users’
Collective flow with PHOBOS
Adam Trzupek The Henryk Niewodniczański Institute of Nuclear Physics
RHIC Physics Through the Eyes of PHOBOS
Presentation transcript:

Centrality Dependence of Charged Antiparticle to Particle Ratios from Abigail Bickley Univ. of Maryland, Chemistry Dept. for the Collaboration DNP, October 31, 2003

Collaboration Birger Back, Mark Baker, Maarten Ballintijn, Donald Barton, Bruce Becker, Russell Betts, Abigail Bickley, Richard Bindel, Wit Busza (Spokesperson), Alan Carroll, Patrick Decowski, Edmundo Garcia, Tomasz Gburek, Nigel George, Kristjan Gulbrandsen, Stephen Gushue, Clive Halliwell, Joshua Hamblen, Adam Harrington, Conor Henderson, David Hofman, Richard Hollis, Roman Holynski, Burt Holzman, Aneta Iordanova, Erik Johnson, Jay Kane, Nazim Khan, Piotr Kulinich, Chia Ming Kuo, Jang Woo Lee, Willis Lin, Steven Manly, Alice Mignerey, Gerrit van Nieuwenhuizen, Rachid Nouicer, Andrzej Olszewski, Robert Pak, Inkyu Park, Heinz Pernegger, Corey Reed, Christof Roland, Gunther Roland, Joe Sagerer, Pradeep Sarin, Iouri Sedykh, Wojtek Skulski, Chadd Smith, Peter Steinberg, George Stephans, Andrei Sukhanov, Marguerite Belt Tonjes, Adam Trzupek, Carla Vale, Robin Verdier, Gábor Veres, Frank Wolfs, Barbara Wosiek, Krzysztof Wozniak, Alan Wuosmaa, Bolek Wyslouch, Jinlong Zhang ARGONNE NATIONAL LABORATORYBROOKHAVEN NATIONAL LABORATORY INSTITUTE OF NUCLEAR PHYSICS, KRAKOWMASSACHUSETTS INSTITUTE OF TECHNOLOGY NATIONAL CENTRAL UNIVERSITY, TAIWANUNIVERSITY OF ILLINOIS AT CHICAGO UNIVERSITY OF MARYLANDUNIVERSITY OF ROCHESTER

Motivation In d+Au collisions little reinteraction is expected thus the ratios should reflect the initially produced yields Recent results suggest conditions in Au+Au collisions are different than those observed in d+Au collisions Do these different conditions influence the measured particle ratios? Initial StateFinal State Interactions

Centrality Dependence The more collisions a participating nucleon suffers the greater the baryon number transport to mid-rapidity PeripheralCentral d+Au:Au+Au: N coll = # collisions, N part = # participants, N d part = # deuteron participants

 p  /p Ratio vs Centrality If the total proton yield is equal to the sum of the transported and produced components  Expect the  p/p  ratio to decrease with increasing number of collisions; i.e with centrality

Detector 2003 SPECTRIG mini-pCal pCal TOF Walls Rings T0 Paddle Spectrometer

Particle Identification Cut bands lie 3 RMS deviations from the expected mean Cutoffs minimize contamination from other particle species

Spectrometer Acceptance Contours represent where the acceptance has fallen to 10% of the maximal value d+Au Bend towards beampipeBend away from beampipe

Magnetic Field Reversals Bending toward beampipe: h - B -, h + B + near mid-rapidity Z Field Polarity: B -  - -  + +  - -  + + near mid-rapidity Z Field Polarity: B +  + +  + +  - -  - - Bending away from beampipe: h - B +, h + B -

Corrections Protons: –Absorption  3.5% ± 1.4% (syst.) –Secondary  1.6% ± 0.3% (stat.) ± 0.2% (syst.) –Feed-down  -0.5% ± 1% (syst.) Kaons: total correction <1% Pions: total correction <0.5%

Systematic Uncertainties Kaon and Proton Ratios: –Centrality Measure: 2% –Kinematic Acceptance (p T and y): 1% Proton Ratios: –Dead & hot spectrometer channels: 0.5% –Spectrometer arm asymmetries: 1% –Polarity-dependent vertex correction: 1% Pion Ratios: –Electron Contamination: < 0.1%

Particle Ratios vs Centrality - No evidence observed that final state effects in Au+Au collisions modify the produced meson yields  -  /  + ,  K -  /  K +  d+Au ~  -  /  + ,  K -  /  K +  Au+Au Colored points  d+Au Black points  Au+Au

Particle Ratios vs Centrality Au+Au proton ratio is significantly lower than d+Au ratios All d+Au particle ratios appear to be independent of centrality Colored points  d+Au Black points  Au+Au

Model Comparison Models agree with the expectation that baryon transport increases with increasing thus resulting in a decreased  p/p  ratio Data does not exhibit this behavior d+Au

Conclusions Do the different conditions in Au+Au and d+Au collisions influence the measured particle ratios? d+Au and Au+Au  and K ratios are consistent  no evidence that final state interactions in Au+Au collisions modify the ratio of initially produced meson yields is observed d+Au particle-antiparticle ratios show a surprising lack of centrality dependence Results are in clear disagreement with AMPT, HIJING and RQMD predictions nucl-ex/

Backup Slides

Raw Particle Yields TriggerCentrality % Evts (M) -- ++ K-K- K+K+ ppEvt (M) -- ++ K-K- K+K+ pp dAVertex dAVertex dAVertex dAVertex dAPeriph dAPeriph dAVertex: 30M evts; required T0 coincidence and |vz|<50cm dAPeriph: 20M evts; required dAVertex and Paddle occupancy <50%

Final Particle Ratios TriggerCentrality %  -  /  +  K -  /  K + p/pp/p dAVertex (1.3)0.995    0.07   0.04  0.04 dAVertex (1.8)1.004    0.03   0.02  0.03 dAVertex (1.8)1.008    0.02   0.02  0.03 dAVertex (2.0)1.016    0.03   0.02  0.03 dAPeriph (1.3)0.996    0.04   0.03  0.03 dAPeriph (1.6)1.014    0.03   0.02  0.03 Au+Au0-12~    0.03   0.02  0.03 Superscript = statistical uncertainty; Subscript = systematic uncertainty

Trigger Elements Normal Trigger: (dAVertex) –30M events collected –required T0 coincidence and |vz|<50cm Peripheral Trigger: (dAPeriph) –20M events collected –required dAVertex and Paddle occupancy <50% Negative Paddles Positive Paddles dAu x z PP PNT0NT0P Positive T0s Negative T0s

Energy (arb. units) Pseudorapidity Glauber Calculation Hijing Hulthen w.f.  inelastic = 41mb Full GEANT Simulation HIJING Simulation dN/d  Trigger% Centrality  N coll  dAVertex (1.7)2.2(1.3)0.20 dAVertex (3.0)4.0(1.8)0.61 dAVertex (3.6)6.1(1.8)0.78 dAVertex0-1016(4.0)8.1(2.0)0.84 dAPeriph (1.7)2.2(1.3)0.18 dAPeriph (2.7)3.7(1.6)0.24 Measuring Centrality in d+Au

Raw Particle Ratios Assumptions: the following must be the same for antiparticles and particles for each bending direction and centrality bin –Acceptance and tracking efficiency Field strength (B+/B-) : agree within 0.2% Centrality Fractions (E Ring ) : agree within 1% –Kinematic distributions  p T ,  p T 2  and  y  : agree within 2%

Baryon Transport d+Au vs Au+Au comparison: – central d+Au > central Au+Au BUT !! –(p/p) central d+Au > (p/p) central Au+Au Relative fraction of transported protons in central d+Au collisions is half that in central Au+Au collisions! 