Asymmetric dihadron azimuthal correlations in Au+Au collisions at 200 GeV Joshua Konzer Purdue University STAR Collaboration.

Slides:



Advertisements
Similar presentations
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.
Advertisements

Photon-Jet Correlations at RHIC Saskia Mioduszewski Texas A&M University 18 July, 2007.
Measurements of long-range angular correlation and identified particle v 2 in 200 GeV d+Au collisions from PHENIX Shengli Huang Vanderbilt University for.
2009/Sep/15, flow workshop, ECT* TrentoShinIchi Esumi, Univ. of Tsukuba1 Jet - flow(v 2 ) correlation ShinIchi Esumi Inst. of Physics, Univ. of Tsukuba.
Cone is medium response, Ridge is medium itself. Fuqiang Wang Purdue University For the STAR Collaboration.
High-p T spectra and correlations from Cu+Cu and Au+Au collisions in STAR Marco van Leeuwen, LBNL for the STAR collaboration.
Ali Hanks - APS Direct measurement of fragmentation photons in p+p collisions at √s = 200GeV with the PHENIX experiment Ali Hanks for the PHENIX.
Understanding Jet Energy Loss with Angular Correlation Studies in PHENIX Ali Hanks for the PHENIX Collaboration 24 th Winter Workshop on Nuclear Dynamics.
Winter Workshop on Nuclear Dynamics, Feb 2011 Centrality dependence of number and transverse momentum correlations in Au+Au collisions at 200 GeV Monika.
Direct photons and Jet correlation in HI. Integrated I AA (0.4
STAR 1 Strange Particle Ratios on the Near- & Away-Side of Jets at RHIC Jiaxu Zuo BNL/SINAP with Paul Sorensen BNL For STAR Collaboration 23rd Winter Workshop.
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.
Jana Bielcikova (Yale University) for the STAR Collaboration 23 rd Winter Workshop on Nuclear Dynamics February 12-18, 2007 Two-particle correlations with.
Feb 2007 Big Sky, Montana Nuclear Dynamics 2007 Conference Is There A Mach Cone? For the STAR Collaboration Claude Pruneau Motivations/Goals Expectations/Models.
Two-, Three-, and Jet-Hadron Correlations at STAR Kolja Kauder for the STAR Collaboration Rencontres de Moriond – La Thuile, Mar
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.
Interaction between jets and dense medium in heavy-ion collisions Rudolph C. Hwa University of Oregon TsingHua University, Beijing, China May 4, 2009.
Charge Asymmetry Correlations Searching for Local Parity Violation Quan Wang, Purdue For STAR Collaboration.
Heavy-Ion Cafe, 30/Jun/2007, TokyoShinIchi Esumi, Inst. of Physics, Univ. of Tsukuba1 Jet correlation and modification at RHIC and 3 particle correlation.
Two particle correlations with respect to higher harmonic plane in Au+Au 200 GeV collisions at RHIC-PHENIX Takahito Todoroki for the PHENIX Collaboration.
KEK seminar, 5/Nov/2008Univ. of Tsukuba, ShinIchi Esumi1 Jet correlation (Mach-cone, Ridge) at RHIC ShinIchi Esumi Inst. of Physics, Univ. of Tsukuba Contents.
Nov 2001 Craig Ogilvie 1 Angular Correlations at High pt: Craig Ogilvie for the Phenix Collaboration Energy-loss: increased medium-induced gluon-radiation.
‘2+1’ correlation – Tagging of Back to Back Jets GREESHMA K M IIT Bombay ALICE-India Meet 27 th & 28 th April
Identified Particle Ratios at large p T in Au+Au collisions at  s NN = 200 GeV Matthew A. C. Lamont for the STAR Collaboration - Talk Outline - Physics.
ATLAS measurement of dipolar flow (v 1 ) in Pb-Pb collisions Jiangyong Jia for the ATLAS Collaboration WWND 2012 April 7 th - 14 rd Based on results in.
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,
Two Particle Correlations and Viscosity in Heavy Ion Collisions Monika Sharma for the Wayne State University STAR Collaboration Outline: Motivation Measurement.
The long-range pseudo-rapidity correlations in high-energy collisions 王福强 Purdue University.
Background introduction Model introduction Analysis method Results and discussions Conclusions Collaborators: S. Zhang, Y. G. Ma, H. Z. Huang, X. Z, Cai,
Winter Workshop on Nuclear Dynamics Jet studies in STAR via 2+1 correlations Hua Pei For the STAR Collaboration.
N. N. Ajitanand Nuclear Chemistry, SUNY, Stony Brook For the PHENIX Collaboration Two and Three particle Flavor Dependent Correlations Remember the hungarian.
13/Aug/2013, Fluc. & Corr. Workshop, Chengdu, China ShinIchi Esumi, Univ. of Tsukuba1 Flow and Jet-correlation ShinIchi Esumi Univ. of Tsukuba Flow originated.
20-25 May 2007 The Berkeley School STAR Study of Jets with 2+1 multi-particle correlations Richard Hollis* for the STAR Collaboration * in close collaboration.
Three-Particle Azimuthal Correlations Jason Glyndwr Ulery 23 March 2007 High-pT Physics at LHC.
Background introduction Model introduction Analysis method Results and discussions Conclusions G.L. Ma, S. Zhang, YGM et al., Phys Lett B 641, 362 (2006)
STAR Christine Nattrass (STAR Collaboration), Yale University DNP, Nashville, 28 October Two particle azimuthal correlations in Cu+Cu collisions.
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.
Wuhan meeting, 4-6/Dec/2008ShinIchi Esumi, Univ. of Tsukuba1 Jet study at RHIC and Jet reconstruction study at LHC energy for ALICE experiment ShinIchi.
Characterizing the away-side jet, devoid of flow background, via two- and three-particle correlations in Au+Au collisions at 200 GeV in STAR Kun Jiang,
Measurement of correlations between elliptic and higher order flow in Pb+Pb collisions Soumya Mohapatra Columbia University Quark Matter May.
Ti Results: Energy and system dependence Conclusions Ridge Jet Figure 1: Sample di-hadron correlation showing the jet-like correlation and the ridge [1]
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,
Near-side  correlations of high-p t hadrons from STAR Jörn Putschke for the STAR collaboration Lawrence Berkeley National Laboratory Weisshorn (4505m),
2008/04/12APS April Meeting 1 Decomposition of Awayside Components of Dijet Correlation in Au+Au Collisions at √S NN = 200 GeV at PHENIX Chin-Hao Chen.
The Double Ridge Phenomenon in p-Pb Collisions Measured with ALICE Jan Fiete Grosse-Oetringhaus, CERN for the ALICE Collaboration Moriond QCD 2013.
06/Feb/2009 High pT Physics, PragueShinIchi Esumi, Univ. of Tsukuba1 Interplay between jet and v 2 ShinIchi Esumi Inst. of Physics, Univ. of Tsukuba measurements.
Alice Ohlson Yale University. Jets at RHIC 15 July 2013Jets at RHIC -- Alice Ohlson2 Hard-scattered partons fragment into collimated “jets” of hadrons.
1 Jets in PHENIX Jiangyong Jia, Columbia Univerisity How to measure jet properties using two particle correlation method (In PHENIX)? Discuss formula for.
Kirill Filimonov, ISMD 2002, Alushta 1 Kirill Filimonov Lawrence Berkeley National Laboratory Anisotropy and high p T hadrons in Au+Au collisions at RHIC.
Yen-Jie Lee (CERN) 1 MBUE working group 2012 Yen-Jie Lee (CERN) for the CMS Collaboration MBUE working group CERN 3 rd Dec, 2012 Two-particle correlations.
Jet-Medium Interactions from RHIC/STAR to LHC/ALICE Fuqiang Wang Purdue University What have been learnt at RHIC? What can be done at LHC?
Jet-medium interaction in heavy-ion collisions Rudolph C. Hwa University of Oregon Hua-Zhong Normal University, Wuhan, China April, 2009.
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.
TWO PARTICLE CORRELATION MEASUREMENTS AT PHENIX Takahito Todoroki For the PHENIX Collaboration University of Tsukuba & RIKEN Nishina Center Hard Probes.
The near-side in STAR Christine Nattrass (Yale University) for the STAR Collaboration.
Monika Sharma Wayne State University for the STAR Collaboration
PHENIX Measurement on High pT h-h and g-h Azimuthal Correlations
ATLAS vn results vn from event plane method
Jets and Jet-like Correlations in STAR
Heavy Ion Ohsaka University Takahito Todoroki
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
Two particle hadron correlations with higher harmonic reaction plane in Au+Au 200 GeV collisions at RHIC-PHENIX T. Todoroki for the PHENIX Collaboration.
Presentation transcript:

Asymmetric dihadron azimuthal correlations in Au+Au collisions at 200 GeV Joshua Konzer Purdue University STAR Collaboration

QM 2009 Results AuAu √s NN = 200GeV; 20-60% Centrality Dihadron Correlations separated into 12 different groups/slices depending on φ s = φ Trig – ψ EP in-plane trigger pt=3-4 GeV/c Jet Ridge  s |=  trig – ψ RP Out- plane CEM model Ridge: assoc pt=1-1.5 GeV/c Ridge: assoc pt=1.5-2 GeV/c Jet: assoc pt=1.5-2 GeV/c STAR Preliminary Jet is symmetric and remains constant as φ s →90 o. Ridge is Asymmetric and decreases as φ s →90 o ! Ridge may be due to jet-flow alignment. 2

4-Gaussian Fit RP Trig. Jet Ridge Away 2 Away 1 Jia et al, PRL 103 (2009) Flow subtracted signal includes jet, ridge, away-side ridge?, and away-side double peak Need to remove jet to get to ridge; Δη > 0.7 Away-side asymmetry Fit with 4 Gauss to analyze features Away-side pathlength sensitivity 3

4-Gaussian Fits ∆ φ (radians) Away-side peak 1Near-side “ridge” Away-side “ridge” (dashed) Data points Away-side peak 2 4 Gaussian is a good fit to data ; χ 2 ≈ 1.0 Possible away-side ridge 1/N trig dNdΔφ φ s – in-plane φ s – out-of-plane STAR Preliminary 4

4-Gaussian Data Peak locations reflect Event Plane influence Away-side peak areas similarity; inconsistent with absorption Peak width differences may be result of medium interaction showing sensitivity to medium pathlength φsφs φsφs φsφs Peak Location φ Gaussian AreasGaussian Sigmas STAR Preliminary 5 Near-side Ridge Away-side RidgeAway-side 1Away-side 2

v 3 estimates from AMPT – Phys. Rev. C 81, (2010) UrQMD - arXiv: arXiv: STAR data- arXiv: arXiv: Raw Dihadron Correlation v 2 & v 4 background v 3 background All inclusive Background v 3 inclusion has very little effect on Background v 2 & v 4 from calculation Theorized that away side peak and dip at 1 radian could change ZYAM and create away-side double peak v 3 Estimation φφφφφφ 1/N trig dNdΔφ v 3 has very little effect on final Dihadron Correlation STAR Preliminary 6 Signal w/ v3 Signal w/o STAR Preliminary 1/N trig dNdΔφ φφφφφφ

Minbias ZYAM Estimation Raw CorrelationBackground v 2 average Background v 2 maximumBackground v 2 minimum Minbias data is used to give most unbiased estimation of ZYAM Background is obtained from mixed events with v 2 added on top ZYAM values align very well with raw correlation at ≈ 1 radian STAR Preliminary 7

Conclusions 4 Gauss fit seems to suggest back-to-back ridge Away-side peaks seem to be effected by medium but not absorbed Ridge decreases as φ s progresses from in-plane to out- of-plane ZYAM is an assumption. Minimum bias data study indicates ZYAM appears reasonable. Present study suggests that v 3 has very little affect on final dihadron correlations. 8

Backup Slides

Previous Studies Previous research involved Dihadron correlation with Reaction Plane orientation; MAGNITUDE ONLY Ridge decreased as φ Trig progressed from in-plane to out-of-plane Jet Remains constant 10 arXiv:

Centrality Dependence Peripheral Most Central Progression toward more central shows the development of ridge peak and impact of medium interaction. φsφs AsAs Centrality 9 Centrality 5 Centrality 3 Asymmetry appears to peak at different φ s Sigma does not appear to change at different φ s 11

ZYAM Estimation Method 1 : v2 and ZYAM are calculated from this large centrality and applied respectively. Method 2 : v2 and ZYAM are calculated and applied for each of the centralities individually. The background-subtracted signals are the added together, with proper trigger weighting, to form the larger centrality chunk. Method 3 : v2 is calculated and recorded for each centrality. Raw signals for each centrality are combined as are the representative v2 background functions, with proper trigger weighting. The ZYAM is then calculated from the conglomerate Raw and v2 background functions. φφφφφφ 1/N trig dNdΔφ STAR Preliminary 12

Fourier Fit χ 2 /ndf = 31.05/39 χ 2 /ndf = 46.84/39 χ 2 /ndf = 57.28/39 χ 2 /ndf = 27.1/39 χ 2 /ndf = 45.9/39 χ 2 /ndf = 51.89/39 χ 2 /ndf = 46.94/43 χ 2 /ndf = 46.47/43 χ 2 /ndf = 57.44/43 χ 2 /ndf = 41.13/43 χ 2 /ndf = 60.62/43 χ 2 /ndf = 64.26/43 13

Fourier Fits to Data V1V1 V2V2 V3V3 V4V4 Fit values don’t necessarily agree with calculated values from data RP-dep. w/o direction Dependence RP-dep. w/ direction Dependence Calculated values: RP-dep. w/o direction dep. v 2 (assoc.)*v 2 (trig)= V 2 (fit) – V 2 (meas) 14

Jet Correlation Effect on EP ∆ φ (radians) Away-side peak 1Near-side “ridge” Away-side “ridge” (dashed) Data points Away-side peak 2 1/N trig dNdΔφ φ s – in-plane φ s – out-of-plane STAR Preliminary No Leading particle (|Δη|>0.5) cut when constructing Event Plane At trigger p T of 3-4 GeV (shown), jet impact on the Event Plane calculation has little effect on final signal 15