STAR Analysis Meeting - BNL

Slides:



Advertisements
Similar presentations
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.
Advertisements

Multiparticle Correlations and Charged Jet Studies in p+p, d+Au, and Au+Au Collisions at  s NN =200 GeV. Michael L. Miller Yale University For the STAR.
Photon-Hadron Correlations at RHIC Saskia Mioduszewski Texas A&M University E-M Workshop of RHIC/AGS Users’ Meeting 27 May, 2008.
Photon-Jet Correlations at RHIC Saskia Mioduszewski Texas A&M University 18 July, 2007.
Measurement of the inclusive jet cross section in p+p collisions at E CM =200 GeV Mike Miller (MIT) For the STAR collaboration.
BNL Seminar 10/02 High p t Hadrons in STAR: Past, Present, and Future Michael L. Miller Yale University For the STAR Collaboration.
1 N. Davidson E/p single hadron energy scale check with minimum bias events Jet Note 8 Meeting 15 th May 2007.
Ali Hanks - APS Direct measurement of fragmentation photons in p+p collisions at √s = 200GeV with the PHENIX experiment Ali Hanks for the PHENIX.
1 High pt particle spectra and correlations of strange particles in pp, dA, and AA in STAR Rene Bellwied Wayne State University (for M.Heinz, J.Adams,
Oana Catu, Yale University for the STAR Collaboration Quark Matter 2008, February 4-10, Jaipur, India System size dependence of dihadron correlations and.
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.
Direct photons and jet correlations in heavy ion collisions Andrew Adare University of Colorado For the PHENIX Collaboration WWND, February 2007.
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.
Xiaoyan LinQuark Matter 2006, Shanghai, Nov , Study B and D Contributions to Non- photonic Electrons via Azimuthal Correlations between Non-
Alán Dávila for the STAR Collaboration WWND February, 8, 2011.
‘2+1’ correlation – Tagging of Back to Back Jets GREESHMA K M IIT Bombay ALICE-India Meet 27 th & 28 th April
Photon-Jet Correlations at RHIC Saskia Mioduszewski Texas A&M University 19 June, 2007.
Jet Studies in STAR via Di-jet Triggered (2+1) Multi-hadron Correlations Kolja Kauder for the STAR collaboration Kolja Kauder for the STAR collaboration,
Winter Workshop on Nuclear Dynamics Jet studies in STAR via 2+1 correlations Hua Pei For the STAR Collaboration.
What Can be Learned from Identifying Leading Hadrons of Jets in STAR? Kolja Kauder for the STAR Collaboration.
1 34th International Conference on High Energy Physics (ICHEP 2008) ‏ The STAR Experiment Texas A&M University A. Hamed for the STAR collaboration Direct.
Elena Bruna for the STAR Collaboration Yale University Quark Matter 09, Knoxville 03/29 -04/
STAR Christine Nattrass (STAR Collaboration), Yale University DNP, Nashville, 28 October Two particle azimuthal correlations in Cu+Cu collisions.
1 Correlations between J/ψ and charged hadrons Chun Zhang / Jiangyong Jia.
1 Away-side Modification and Near-side Ridge Relative to Reaction Plane at 200 GeV Au+Au Collisions 第十届全国粒子物理学术会议 (南京) Apr. 28th, 2008 Aoqi Feng, Fuqiang.
C ONTROL STUDY OF SURFACE BIAS EMISSION IN 2- PARTICLE CORRELATIONS IN A U +A U AT √ S NN = 200 G E V IN PHENIX Eric Vazquez 2012 APS-Division of Nuclear.
Mike Miller First measurement of the inclusive jet cross section in p+p collisions at E CM =200 GeV M.L. Miller (MIT) Motivations: 1.Baseline for inclusive.
Ti Results: Energy and system dependence Conclusions Ridge Jet Figure 1: Sample di-hadron correlation showing the jet-like correlation and the ridge [1]
Longitudinal Spin Asymmetry and Cross Section of Inclusive  0 Production in Polarized p+p Collisions at 200 GeV Outline  Introduction  Experimental.
Jeffery T. Mitchell (BNL) – Quark Matter The Evolution of Correlation Functions from Low to High p T : From HBT to Jets Quark Matter 2005 Jeffery.
Multi-strange Baryon Correlations in p+p and d+Au Collisions at √s NN = 200 GeV Betty Bezverkhny Yale University For the Collaboration Hot Quarks ’04,
1 Jets in PHENIX Jiangyong Jia, Columbia Univerisity How to measure jet properties using two particle correlation method (In PHENIX)? Discuss formula for.
 -jet measurements Table of Contents:  Motivation  Preliminary QA of  -trigger Data  Shower Shape Analysis  Experimental Challenges  Summary  
Jet Production in Au+Au Collisions at STAR Alexander Schmah for the STAR Collaboration Lawrence Berkeley National Lab Hard Probes 2015 in Montreal/Canada.
May 27 th, Questions: Does the presence of a jet deform the structure of the soft medium? Does the space-momentum correlation that causes v.
Toward a  +Jet Measurement in STAR Saskia Mioduszewski, for the STAR Collaboration Texas A&M University 1.
Direct Photon v 2 Study in 200 GeV AuAu Collisions at RHIC Guoji Lin (Yale) For STAR Collaboration RHIC & AGS Users’ Meeting, BNL, June 5-9.
What can we learn from high-p T azimuthal correlations of neutral strange baryons and mesons at RHIC ? Jana Bielcikova (Yale University) for the STAR Collaboration.
Is there a strange baryon/meson dependence in correlations in STAR? Marek Bombara for the STAR Collaboration (University of Birmingham) Strangeness in.
The near-side in STAR Christine Nattrass (Yale University) for the STAR Collaboration.
As a probe of the quark gluon plasma
Outline Motivation Analysis technique Results Conclusions.
Future prospects for NA61 heavy ions: rare observables
Time Independent Analysis
Monika Sharma Wayne State University for the STAR Collaboration
Jet Measurements with Neutral and Di-jet Triggers in Central Au+Au Collisions at √sNN = 200 GeV with STAR Nihar Ranjan Sahoo (for the STAR collaboration)
PHENIX Measurement on High pT h-h and g-h Azimuthal Correlations
Introduction and analysis method
NA61 and NA49 Collaboration Meeting May 14-19, 2012, Budapest
ATLAS vn results vn from event plane method
Jets and Jet-like Correlations in STAR
Recent STAR results on high-pT probes
Experimental Studies of Quark Gluon Plasma at RHIC
RAA predictions show enhancement highly sensitive to jet quenching
Tatsuya Chujo for the PHENIX collaboration
Heavy Ion Ohsaka University Takahito Todoroki
Scaling Properties of Fluctuation and Correlation Results from PHENIX
Multi-hadron cluster triggered correlations
Eitaro Hamada, Univ. of Tsukuba
“Hard” & “Soft” Interactions in Proton + Proton 200GeV
Two particle correlations with higher harmonic reaction plane in Au+Au 200 GeV collisions at RHIC-PHENIX T. Todoroki for the Collaboration.
ShinIchi Esumi, Univ. of Tsukuba
Third DNP/JPS Joint Meeting, 14th October 2009
ShinIchi Esumi, Univ. of Tsukuba
Identified Charged Hadron Production at High pT
ShinIchi Esumi, Univ. of Tsukuba
Two particle hadron correlations with higher harmonic reaction plane in Au+Au 200 GeV collisions at RHIC-PHENIX T. Todoroki for the PHENIX Collaboration.
Identified Particle Production at High Transverse Momentum at RHIC
Measurement of b-jet Shapes at CDF
Presentation transcript:

STAR Analysis Meeting - BNL Multi-hadron Triggered Azimuthal Correlations in Au+Au Collisions at √sNN = 200 GeV Brooke Haag UC Davis Outline Introduction / Analysis Technique Motivation & explanation of multi-hadron triggers Results Away side yields for different pT trigger bins: 10 to 12 GeV & 12 to 15 GeV Ratios of Cluster triggers to di-hadron triggers Away side yields (dAu) for pT trigger bins: 8 to 10 GeV & 12 to 15 GeV Cone radius study -- preview Conclusions and Outlook STAR Analysis Meeting - BNL October 15-19, 2007

STAR Analysis Meeting - BNL - Oct. 2007 Introduction Fragmentation function D(z) depends on z defined as pT/ET,jet Current method of Di-hadron correlation is insensitive to true fragmentation functions Try multi-hadron (cluster) trigger Better constrain ET,jet ~ pT(trig), better approximation of fragmentation function Gain statistics STAR, Phys. Rev. Let. 97 (2006),162301 STAR Analysis Meeting - BNL - Oct. 2007

STAR Analysis Meeting - BNL - Oct. 2007 Analysis Technique R Seed Associated track Collect arrays of seed and associated tracks with a minimum seed pT cut (5.0 GeV) and a minimum associated pT cut Define a cone radius (R=0.3) pT trigger = pT sum of all the associated tracks (secondary seeds) in that cone Plot  between the highest pT seed in the cone and associated tracks Subtract flat background for Au+Au Extract Yields: pT (trigger) = 8 to 10 GeV, 10 to 12 GeV & 12 to 15 GeV pT (assoc) = 3 to 4, … ,10 to 11 GeV Di-hadron correlation R Seed Secondary Seeds Associated track Multi-hadron trigger STAR Analysis Meeting - BNL - Oct. 2007

dN/d - jet pT, 12 to 15 GeV, associated pT, 3 to 4 GeV AuAu 0-12% Plot  between the highest pT seed in the cone and associated tracks Subtract flat background for Au+Au Extract Yields: pT (trigger) = 8 to 10 GeV, 10 to 12 GeV, & 12 to 15 GeV pT (assoc) = 3 to 4, … ,10 to 11 GeV Near side Away side STAR Analysis Meeting - BNL - Oct. 2007

Combinatorial Background Seed Secondary Seed Associated track pT seed > 5.0 GeV Vary minimum secondary seed pT to test effect of combinatorial background in AuAu 2.0 GeV 3.0 GeV 4.0 GeV STAR Analysis Meeting - BNL - Oct. 2007

Comparison of single vs. cluster trigger statistics - d+Au Minimum secondary seed cut = 2.0 GeV 291 66 Di-hadron correlation Multi-hadron triggers gain statistics by allowing clusters to add up to pT(trig), not just requiring a single particle to carry pT(trig) STAR Analysis Meeting - BNL - Oct. 2007

Away side yields Minimum secondary seed cut = 2.0 GeV 10 GeV < pT trig < 12 GeV 12 GeV < pT trig < 15 GeV STAR preliminary STAR preliminary Fraction of Multi-hadron triggers to Single+Multi triggers = 0.83 Fraction of Multi-hadron triggers to Single+Multi triggers = 0.86 Multi-hadron and Di-hadron curves match well for 10 < pT trig <12 GeV Multi-hadron and Di-hadron curves don’t match as well for 12 < pT trig <15 GeV, especially at lower pT assoc, likely effect of random clusters STAR Analysis Meeting - BNL - Oct. 2007

Away side yields Minimum secondary seed cut = 3.0 GeV 10 GeV < pT trig < 12 GeV 12 GeV < pT trig < 15 GeV STAR preliminary STAR preliminary Fraction of Multi-hadron triggers to Single+Multi triggers = 0.59 Fraction of Multi-hadron triggers to Single+Multi triggers = 0.64 Multi-hadron and Di-hadron curves match well in both pT trigger bins Fraction of Multi-hadron triggers decreases as secondary seed cut increases STAR Analysis Meeting - BNL - Oct. 2007

Away side yields Minimum secondary seed cut = 4.0 GeV 10 GeV < pT trig < 12 GeV 12 GeV < pT trig < 15 GeV STAR preliminary STAR preliminary Fraction of Multi-hadron triggers to Single+Multi triggers = 0.36 Fraction of Multi-hadron triggers to Single+Multi triggers = 0.21 Multi-hadron and Di-hadron curves match well for 12 < pT trig < 15 GeV For 10 < pT trig < 12 GeV, Multi-hadron triggers have slightly higher yield than Di-hadrons, possible effect of minimum seed/secondary seed cuts Fraction of Multi-hadron triggers decreases as secondary seed cut increases STAR Analysis Meeting - BNL - Oct. 2007

STAR Analysis Meeting - BNL - Oct. 2007 Ratios: Single+Multi-hadron triggers to Di-hadrons - 10 GeV < pT trig < 12 GeV - Min. secondary seed cut = 2.0 GeV Min. secondary seed cut = 3.0 GeV Min. secondary seed cut = 4.0 GeV STAR preliminary STAR preliminary STAR preliminary Ratio Cluster Analysis/di-hadron Analysis Ratios (statistical errors only) fall around unity and are relatively flat. No significant variation with increasing secondary seed cut. The single+multi-hadron triggers sample same kinematics as di-hadron correlations. STAR Analysis Meeting - BNL - Oct. 2007

STAR Analysis Meeting - BNL - Oct. 2007 Ratios: Single+Multi-hadron triggers to Di-hadrons - 12 GeV < pT trig < 15 GeV - Min. secondary seed cut = 2.0 GeV Min. secondary seed cut = 3.0 GeV Min. secondary seed cut = 4.0 GeV STAR preliminary STAR preliminary STAR preliminary Ratio Cluster Analysis/di-hadron Analysis Excluding lowest pT associated bins affected by random clusters, ratios (statistical errors only) fall around unity and are relatively flat. No significant variation with increasing secondary seed cut. The single+multi-hadron triggers sample same kinematics as di-hadron correlations. STAR Analysis Meeting - BNL - Oct. 2007

Away side yields - dAu Minimum secondary seed cut = 2.0 GeV 8 GeV < pT trig < 10 GeV 12 GeV < pT trig < 15 GeV STAR preliminary STAR preliminary Fraction of Multi-hadron triggers to Single+Multi triggers = 0.39 Fraction of Multi-hadron triggers to Single+Multi triggers = 0.67 Run out of statistics with increasing pT associated, especially in higher pT trig bin. STAR Analysis Meeting - BNL - Oct. 2007

Cone Radius Study - AuAu Minimum secondary seed cut = 2.0 GeV Minimum secondary seed cut = 3.0 GeV Minimum secondary seed cut = 4.0 GeV STAR Analysis Meeting - BNL - Oct. 2007

Cone Radius Study - dAu Minimum secondary seed cut = 2.0 GeV STAR Analysis Meeting - BNL - Oct. 2007

Conclusions and Outlook Investigated Multi-hadron triggers as a method of better approximating fragmentation functions Multi-hadron triggers and Di-hadron correlations mostly give very similar results Also ratios of Single+Multi-hadron trigger yields to di-hadron yields show slopes not different, kinematics not very different Multi-hadron triggers yield the same physics as di-hadron correlations with improved statistics Method is promising, more work is needed Pythia simulations to understand expectations for multi-hadron trigger yields Study yields for different jet cone radii Look at higher pT trigger > 15 GeV STAR Analysis Meeting - BNL - Oct. 2007

Backup Slides

STAR Analysis Meeting - BNL - Oct. 2007 Away side yields - AuAu cone radius study Minimum secondary seed cut = 2.0 GeV 8 GeV < pT trig < 10 GeV 8 GeV < pT trig < 10 GeV R = 0.3 R = 0.1 STAR preliminary STAR preliminary Fraction of Multi-hadron triggers to Single+Multi triggers = 0.72 Fraction of Multi-hadron triggers to Single+Multi triggers = 0.25 Vary radius to study effect of combinatoric background. Fraction of Multi-hadron triggers decreases with smaller cone radius. STAR Analysis Meeting - BNL - Oct. 2007

Away side yields Minimum secondary seed cut = 2.0 GeV 8 GeV < pT trig < 10 GeV 10 GeV < pT trig < 12 GeV STAR preliminary STAR preliminary Fraction of Multi-hadron triggers to Single+Multi triggers = 0.72 Fraction of Multi-hadron triggers to Single+Multi triggers = 0.83 STAR Analysis Meeting - BNL - Oct. 2007

Away side yields Minimum secondary seed cut = 3.0 GeV 8 GeV < pT trig < 10 GeV 10 GeV < pT trig < 12 GeV STAR preliminary STAR preliminary Fraction of Multi-hadron triggers to Single+Multi triggers = 0.24 Fraction of Multi-hadron triggers to Single+Multi triggers = 0.59 STAR Analysis Meeting - BNL - Oct. 2007

Away side yields Minimum secondary seed cut = 4.0 GeV 10 GeV < pT trig < 12 GeV 8 GeV < pT trig < 10 GeV STAR preliminary STAR preliminary Fraction of Multi-hadron triggers to Single+Multi triggers = 0.04 Fraction of Multi-hadron triggers to Single+Multi triggers = 0.36 STAR Analysis Meeting - BNL - Oct. 2007

STAR Analysis Meeting - BNL - Oct. 2007 Ratios: Single+Multi-hadron triggers to Di-hadrons - 8 GeV < pT trig < 10 GeV - Min. secondary seed cut = 2.0 GeV Min. secondary seed cut = 3.0 GeV Min. secondary seed cut = 4.0 GeV STAR preliminary STAR preliminary STAR preliminary Ratio Cluster Analysis/di-hadron Analysis STAR Analysis Meeting - BNL - Oct. 2007