Charge Asymmetry Correlations Searching for Local Parity Violation Quan Wang, Purdue For STAR Collaboration.

Slides:



Advertisements
Similar presentations
1 A novel method of looking for the parity violation signal N. N. Ajitanand (SUNYSB Nuclear Chemistry) for the PHENIX Collaboration Joint CATHIE/TECHQM.
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.
STAR 1 Azimuthal Anisotropy: The Higher Harmonics Art Poskanzer for the Collaboration STAR.
Spontaneous Parity Violation in Strong Interactions Dhevan Gangadharan (UCLA) On behalf of the STAR Collaboration WWND
Measurements of long-range angular correlation and identified particle v 2 in 200 GeV d+Au collisions from PHENIX Shengli Huang Vanderbilt University for.
Ultra Peripheral Collisions at RHIC Coherent Coupling Coherent Coupling to both nuclei: photon~Z 2, Pomeron~A 4/3 Small transverse momentum p t ~ 2h 
Winter Workshop on Nuclear Dynamics, Feb 2011 Centrality dependence of number and transverse momentum correlations in Au+Au collisions at 200 GeV Monika.
 Transverse Polarization in STAR Au-Au Collisions Polarization definition and models E896 results STAR analysis STAR results Significance of results Future.
/home/vkoch/Desktop/INT2010/parity_ta lk.odp 1 Have we seen Local Parity Violation at RHIC? ● Introduction ● What the present data tell us ● Alternative.
Feb 2007 Big Sky, Montana Nuclear Dynamics 2007 Conference Is There A Mach Cone? For the STAR Collaboration Claude Pruneau Motivations/Goals Expectations/Models.
 production in d+Au collisions at STAR Haidong Liu University of California, Davis For the STAR Collaboration.
Gang Wang (WWND2010)1 Search for local parity violation with STAR ZDC-SMD Gang Wang (UCLA) for STAR Collaboration.
Measurement of Charge Asymmetry Correlations in Heavy Ion Collisions Quan Wang, Purdue For STAR Collaboration 111/4/2010DNP 2010.
High p T identified charged hadron v 2 and v 4 in 200GeV AuAu collisions by the PHENIX experiment Shengli Huang Vanderbilt University for the PHENIX Collaboration.
Nov 2001 Craig Ogilvie 1 Angular Correlations at High pt: Craig Ogilvie for the Phenix Collaboration Energy-loss: increased medium-induced gluon-radiation.
Event-by-event flow from ATLAS Jiangyong Jia. Initial geometry & momentum anisotropy 2 Single particle distribution hydrodynamics by MADAI.us Momentum.
Masashi Kaneta, LBNL Masashi Kaneta for the STAR collaboration Lawrence Berkeley National Lab. First results from STAR experiment at RHIC - Soft hadron.
Sevil Salur for STAR Collaboration, Yale University WHAT IS A PENTAQUARK? STAR at RHIC, BNL measures charged particles via Time Projection Chamber. Due.
Jinghua Fu Institute of Particle Physics, CCNU, Wuhan TUHEP, Tsinghua University, Beijing On the Measurement of Event Mean Pt Fluctuations Motivation Analytical.
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.
Asymmetric dihadron azimuthal correlations in Au+Au collisions at 200 GeV Joshua Konzer Purdue University STAR Collaboration.
Two Particle Correlations and Viscosity in Heavy Ion Collisions Monika Sharma for the Wayne State University STAR Collaboration Outline: Motivation Measurement.
QM’05 Budapest, HungaryHiroshi Masui (Univ. of Tsukuba) 1 Anisotropic Flow in  s NN = 200 GeV Cu+Cu and Au+Au collisions at RHIC - PHENIX Hiroshi Masui.
Centrality Determination and Reaction plane reconstruction with MPD D.Dryablov, V. Zhezher, M.Kapishin, G.Musulmanbekov XIV GDRE Workshop, Dubna
Longitudinal de-correlation of anisotropic flow in Pb+Pb collisions Victor Roy ITP Goethe University Frankfurt In collaboration with L-G Pang, G-Y Qin,
1 Search for effects related to Chiral Magnetic Wave at STAR Gang Wang (UCLA) for STAR Collaboration.
SQM2004, Cape Town, Sept. 16, 2004 STAR 1 Cronin Effect for the identified particles from 200 GeV d+Au collisions Xiangzhou Cai Shanghai INstitute of Applied.
 Production at forward Rapidity in d+Au Collisions at 200 GeV The STAR Forward TPCs Lambda Reconstruction Lambda Spectra & Yields Centrality Dependence.
1 Identified Particle Dependence of Nuclear Modification Factors in d+Au Collisions at RHIC. Lee Barnby - University of Birmingham For the STAR Collaboration.
Higher moments of net-charge multiplicity distributions at RHIC energies in STAR Nihar R. Sahoo, VECC, India (for the STAR collaboration) 1 Nihar R. Sahoo,
Hadron emission source functions measured by PHENIX Workshop on Particle Correlations and Fluctuations The University of Tokyo, Hongo, Japan, September.
09/15/10Waye State University1 Elliptic Flow of Inclusive Photon Ahmed M. Hamed Midwest Critical Mass University of Toledo, Ohio October, 2005 Wayne.
July 19, FTPC and its Utility to PMD program OUTLINE 1.FTPC and PMD: A comparison 2.FTPC and PMD: Physics issues 3.Summary FTPC Review: BNL, July.
S.A. Voloshin School of Collective Dynamics in High Energy Collisions, LBNL, June 7-11, 2010 page 1 Local strong parity violation and new perspectives.
Search for the QCD Critical Point Gary D. Westfall Michigan State University For the STAR Collaboration Gary Westfall for STAR – Erice,
Jan. 13, 2004QM 2004 Poster Session1 The Geometry of Hadronization in Au-Au Collisions at s NN 1/2 = 130 and 200 GeV Studied with Two-Particle, Charge-Dependent.
Flow fluctuation and event plane correlation from E-by-E Hydrodynamics and Transport Model Victor Roy Central China Normal University, Wuhan, China Collaborators.
Forward-backward multiplicity correlations in PbPb, pPb and pp collisions from ATLAS Jiangyong Jia for the ATLAS collaboration 9/27-10/3, 2015
M. Muniruzzaman University of California Riverside For PHENIX Collaboration Reconstruction of  Mesons in K + K - Channel for Au-Au Collisions at  s NN.
STAR QM2009 Experimental study of spontaneous strong parity violation… S.A. Voloshinpage 1 Experimental study of spontaneous strong parity violation in.
Jan Balewski: Di-jet Sivers in 200 GeV 1 Outline Motivation Principle of measurement, trigger Model of Sivers asymmetry Measured SSA & DSA Comparison.
Azimuthal HBT measurement of charged pions With respect to 3 rd event plane In Au+Au 200GeV collisions at RHIC-PHENIX Takafumi Niida for the PHENIX Collaboration.
N. N. Ajitanand Nuclear Chemistry, SUNY Stony Brook For the PHENIX Collaboration RHIC & AGS Users Meeting June Investigation of Parity Violation.
July 16th-19th, 2007 McGill University AM 1 July 16th-19th, 2007 McGill University, Montréal, Canada July 2007 Early Time Dynamics Montreal AM for the.
1 February 8, 2008 Sunil Dogra QM2008 Jaipur 1 Sunil M. Dogra University of Jammu, India (For the STAR collaboration)‏ Outline Motivation STAR Experiment.
Search for Chiral Magnetic Effects in High-Energy Nuclear Collisions
Detector Effects and Backgrounds In the following, I examine the following possible sources of spurious signals which could simulate the parity signal:
Dhevan Gangadharan (for the STAR Collaboration) Postdoctoral Researcher at CERN--Ohio State University.
School of Collective Dynamics in High-Energy CollisionsLevente Molnar, Purdue University 1 Effect of resonance decays on the extracted kinetic freeze-out.
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,
Oct. 12, 2007 Imran Younus k T Asymmetry in Longitudinally Polarized p +p Collisions at PHENIX.
Hadronic resonance production in Pb+Pb collisions from the ALICE experiment Anders Knospe on behalf of the ALICE Collaboration The University of Texas.
Dhevan Gangadharan UCLA STAR Collaboration DNP meeting 10/25/08 1.
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.
PHENIX. Motivation Collaboration PHENIX Roy A. Lacey (SUNY Stony Brook) PHENIX Collaboration I N T E R N A T I O N A L W O R K S H O P O N T H E P H.
Dynamical modeling of the chiral magnetic effect in heavy-ion collisions [arXiv: ] Yuji Hirono [Stony Brook Univ.] Collaborators: T. Hirano[Sophia.
9/11/2003Tomoaki Nakamura - Hiroshima Univ.1 Event-by-event charge/neutral fluctuation at RHIC-PHENIX Tomoaki Nakamura / Kensuke Homma Hiroshima University.
Chiral Magnet Effect, where are we?
Monika Sharma Wayne State University for the STAR Collaboration
for STAR Collaboration
NA61 and NA49 Collaboration Meeting May 14-19, 2012, Budapest
ATLAS vn results vn from event plane method
W Charge Asymmetry at CDF
STAR Spin alignment of vector mesons (K*0, φ) in Au+Au and p+p collisions at RHIC Jin Hui Chen Shanghai Institute of Applied Physics and UCLA For the STAR.
Analisi del flow con il metodo dei coefficienti di Fourier
The Study of Elliptic Flow for PID Hadron at RHIC-PHENIX
Identified Charged Hadron Production at High pT
Directed Flow from Au+Au Collisions at 200 GeV
Stony Brook University
Presentation transcript:

Charge Asymmetry Correlations Searching for Local Parity Violation Quan Wang, Purdue For STAR Collaboration

Outline  Motivation: Local Parity Violation  Charge Asymmetry Observables  Analysis Details  Results  Toy Model PV Signal Embedding  Summary

Motivation  Chiral magnetic effect:  LPV + large magnetic field  charge separation along the system angular momentum.  Kharzeev et al. NPA 803 (2008) 227

Charge Asymmetry Observables UP DOWN LEFT RIGHT EP  LPV effects in UD. LR is null- reference.  LPV expectations:  A +UD and A -UD are anti- correlated → ‹A + A - › UD < ‹A + A - › LR  Additional dynamical fluctuation broadens A ±UD distributions → ‹A ± 2 › UD > ‹A ± 2 › LR

Analysis Details  Data set: – AuAu 2004 MinBias 200GeV (20M events)  Standard STAR event and track cuts  To avoid self-correlation effect: 1.EP: η 0 2.EP: η>0; Asym η<0 η>0η<0

‹A 2 ›, ‹A + A - › and Stat. Fluc.  Statistic fluctuation and detector effect, Dashed line.  Stat. Fluc. Shows only in ‹A 2 ›, and is larger then ‹A 2 ›  TPC Random Flip  STAR preliminary

 ‹A 2 ›  In peripheral, both  ‹A 2 › UD and  ‹A 2 › LR are positive.  Like-sign pairs more likely in same direction. (small- angle correlation)  In central, both negative.  Like-sign pair more likely back-to-back.  Small-angle same-sign correlation is stronger in UD than LR.

‹A + A - › o Both ‹A + A - › UD and ‹A + A - › LR are large and positive. o Positive and negative charge particles are strongly correlated. o Small-angle opposite-sign correlation is stronger in UD than LR.

Summary of  ‹A 2 › and ‹A + A - ›  In peripheral, particles are preferentially in same direction, regardless same- sign or opposite-sign charges.  In mid-central to central, opposite-sign prefer in the same direction, but same- sign prefer back-to-back.

UD-LR   ‹A 2 › UD >  ‹A 2 › LR  Same-sign broadening in UD is larger than LR, consistent with LPV expectation.  However, same-sign are preferentially back-to-back. STAR preliminary o ‹A + A - › UD > ‹A + A - › LR > 0  Opposite-sign are more strongly emitted in the same direction in UD than LR, which is inconsistent with LPV expectation  Similar centrality dep.

LR-UD Compared to 3-point Correlator  UD-LR: infinite number of harmonic terms.   ‹A 2 ›: Higher-order terms may be small. o  ‹A + A - ›: Higher-order terms are important. STAR preliminary

Toy Model: Embedding PV Signal Embedding PV signal to real event. PV signal: – Magnitude: 1%, or 0.2% of total multiplicity, Poisson distribution. – Shape: Gaussian distribution in UP and DOWN relative to event plane with  =15°,  =45°. – Event Plane resolution smearing

Embedding PV signal 1%,  =15° 1%,  =45° 0.2%,  =15°  Our charge asymmetry observables are sensitive to LPV signal.  LPV signal may be already present in the data, thus, the difference between embedding and real data would suggest that data should have the same magnitude of signal of the toy model. STAR preliminary

Summary  Dynamical charge asymmetry correlations are presented.  Same-sign (  ‹A 2 ›):  more small-angle correlation in peripheral.  more back-to-back in mid-central to central.  broadening more strongly in UD then LR.  Opposite-sign (‹A + A - ›):  always in the same direction.  More strongly in UD then LR.  Data can’t be explained by LPV, more experimental as well as theoretical works are needed to further investigate the underlying physics.  Toy model study also confirms the LPV expectation, and gives a rough estimation of the magnitude of LPV signal.