1 Paul Chung ( for the PHENIX Collaboration ) Nuclear Chemistry, SUNY, Stony Brook Evidence for a long-range pion emission source in Au+Au collisions at.

Slides:



Advertisements
Similar presentations
PID v2 and v4 from Au+Au Collisions at √sNN = 200 GeV at RHIC
Advertisements

Azimuthal Correlation Studies Via Correlation Functions and Cumulants N. N. Ajitanand Nuclear Chemistry, SUNY, Stony Brook.
Anomalous Pion Production in High Energy Particle Collisions Alexander Bylinkin, Andrey Rostovtsev XV Moscow School of Physics XXXX ITEP Winter School.
Yorito Yamaguchi For the PHENIX collaboration CNS, University of Tokyo 10/14/2008ATHIC2008 1/13.
Identified particle transverse momentum distributions in 200 GeV Au+Au collisions at RHIC 刘海东 中国科技大学.
Bingchu Huang, USTC/BNL 1 Bingchu Huang (for STAR Collaboration) University of Science and Technology of China (USTC) Brookhaven National Laboratory (BNL)
1 How to measure flow and the reaction plane? N. N. Ajitanand Nuclear Chemistry, SUNY, Stony Brook.
Julia VelkovskaMoriond QCD, March 27, 2015 Geometry and Collective Behavior in Small Systems from PHENIX Julia Velkovska for the PHENIX Collaboration Moriond.
1 Roy Lacey & Paul Chung Nuclear Chemistry, SUNY, Stony Brook Evidence for a long-range pion emission source in Au+Au collisions at.
1 Systematic studies of freeze-out source size in relativistic heavy-ion collisions by RHIC-PHENIX Akitomo Enokizono Lawrence Livermore National Laboratory.
4/23/06 Ali Hanks - APS 1 A method for directly measuring bremsstrahlung photons from jets Ali Hanks APS Conference April 23, 2006.
UCRL-PRES-?????? CorAL and the Future of Imaging This work was performed under the auspices of the U.S. Department of Energy by University of California,
Roy A. Lacey, Stony Brook; 24 th Winter Workshop on Nuclear Dynamics, April 5-12, Roy A. Lacey Prospects for locating the QCD Critical End Point.
Collision system dependence of 3-D Gaussian source size measured by RHIC-PHENIX Akitomo Enokizono Lawrence Livermore National Laboratory 23 rd Winter Workshop.
WPCF07, Sonoma, California, August Observation of Extended Pion Sources in Relativistic Heavy Ion Collisions: extraction of source breakup time.
1 P. Chung Nuclear Chemistry, SUNY, Stony Brook Evidence for a long-range pion emission source in Au+Au Collisions at.
12 th Zimányi Winter School on Heavy Ion Physics Kaon source imaging with the STAR experiment in 200 GeV Au+Au collisions at RHIC Róbert Vértesi (for the.
PHENIX measurements of reaction plane dependence of high p T photons and pions in Au+Au collisions Vladislav Pantuev, University at Stony Brook for PHENIX.
Zbigniew Chajęcki National Superconducting Cyclotron Laboratory Michigan State University Probing reaction dynamics with two-particle correlations.
Nov 2001 Craig Ogilvie 1 Angular Correlations at High pt: Craig Ogilvie for the Phenix Collaboration Energy-loss: increased medium-induced gluon-radiation.
QM2006 Shanghai, China 1 High-p T Identified Hadron Production in Au+Au and Cu+Cu Collisions at RHIC-PHENIX Masahiro Konno (Univ. of Tsukuba) for the PHENIX.
Roy A. Lacey, Stony Brook; EDT-HIC, McGill, Montreal, Canada, July 16-19, Roy A. Lacey New Prospects for locating the Critical End Point (CEP) in.
BNL/ Tatsuya CHUJO CNS workshop, Tokyo Univ. Identified Charged Single Particle Spectra at RHIC-PHENIX Tatsuya Chujo (BNL) for the PHENIX.
1 Roy Lacey ( for the PHENIX Collaboration ) Nuclear Chemistry Group Stony Brook University PHENIX Measurements of 3D Emission Source Functions in Au+Au.
M. Issah QM04 1 Azimuthal Anisotropy Measurements in PHENIX via Cumulants of Multi-particle Azimuthal Correlations Michael Issah (SUNY Stony Brook ) for.
July 21, 2011M.Š. EPS-HEP 2011, Grenoble11 Three-dimensional Kaon Source Extraction from STAR Experiment at RHIC Michal Šumbera NPI ASCR Prague (for the.
November 29, 2010Zimanyi Winter School 2010, Budapest11 3D Pion & Kaon Source Imaging from 200 AGeV Au+Au collisions Paul Chung (STAR Collaboration) NPI.
QM06, Shanghai, China, Nov Evidence of non-Gaussian tail in Pion Emission SPS: Sensitivity to source formation & emission duration Paul.
November 6, 2012M.Š. STAR regional mtg., Warsaw11 Kaon Freeze-out Dynamics in √s NN =200GeV Au+Au Collisions at RHIC Michal Šumbera NPI ASCR, Prague (for.
Hadron emission source functions measured by PHENIX Workshop on Particle Correlations and Fluctuations The University of Tokyo, Hongo, Japan, September.
Enhanced production of direct photons in Au+Au collisions at =200 GeV Y. Akiba (RIKEN/RBRC) for PHENIX Collaboration
Sergey Panitkin Current Status of the RHIC HBT Puzzle Sergey Panitkin Brookhaven National Lab La Thuile, March 18, 2005.
M. Muniruzzaman University of California Riverside For PHENIX Collaboration Reconstruction of  Mesons in K + K - Channel for Au-Au Collisions at  s NN.
Measurement of photons via conversion pairs with PHENIX at RHIC - Torsten Dahms - Stony Brook University HotQuarks 2006 – May 18, 2006.
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.
 Measurement of  x E  (Fig. 4) Assorted correlations between a fixed high-p T trigger hadron (  p Ttrig  =4.7GeV/c) and lower p T associated hadrons.
2Roy A. Lacey, Stony Brook University, SEWM2010 Study of the properties of the QGP is a central goal at RHIC “The major discoveries in the first five.
1 Roy Lacey Nuclear Chemistry, SUNY, Stony Brook Proofing the Source Imaging Technique.
School of Collective Dynamics in High-Energy CollisionsLevente Molnar, Purdue University 1 Effect of resonance decays on the extracted kinetic freeze-out.
S. PrattNSCL/MSU Deciphering the Space-Time Evolution of Heavy-Ion Collisons with Correlation Measurements Scott Pratt Michigan State University.
R. Lednicky: Joint Institute for Nuclear Research, Dubna, Russia I.P. Lokhtin, A.M. Snigirev, L.V. Malinina: Moscow State University, Institute of Nuclear.
Roy A. Lacey, Stony Brook University; QM11, Annecy, France 2011.
Scott PrattMichigan State University Femtoscopy: Theory ____________________________________________________ Scott Pratt, Michigan State University.
Roy A. Lacey, Stony Brook, ISMD, Kromĕříž, Roy A. Lacey What do we learn from Correlation measurements at RHIC.
21 st WWND, W. Holzmann Wolf Gerrit Holzmann (Nuclear Chemistry, SUNY Stony Brook) for the Collaboration Tomographic Studies of the sQGP at RHIC: the next.
Measurement of photons via conversion pairs with the PHENIX experiment at RHIC - Torsten Dahms - State University of New York at Stony Brook for the PHENIX.
The hypernuclei program at RHIC-STAR Jinhui Chen for the STAR Collaboration Shanghai Institute of Applied Physics, CAS The 11 th International Conference.
BNL/ Tatsuya CHUJO JPS RHIC symposium, Chuo Univ., Tokyo Hadron Production at RHIC-PHENIX Tatsuya Chujo (BNL) for the PHENIX Collaboration.
Measurement of photons via conversion pairs with the PHENIX experiment at RHIC - Torsten Dahms - Master of Arts – Thesis Defense Stony Brook University.
T. Csörgő 1,2 for the PHENIX Collaboration Femtoscopic results in Au+Au & p+p from PHENIX at RHIC 1 MTA KFKI RMKI, Budapest,
PHENIX Results from the RHIC Beam Energy Scan Brett Fadem for the PHENIX Collaboration Winter Workshop on Nuclear Dynamics 2016.
Paul Chung for the STAR Collaboration Nuclear Physics Institute ASCR Prague WPCF 2011, Tokyo 3D kaon source extraction from 200GeV Au+Au collisions.
Analysis of the anomalous tail of pion production in Au+Au collisions as measured by the PHENIX experiment at RHIC M. Nagy 1, M. Csanád 1, T. Csörgő 2.
IOPB Dipak Mishra (IOPB), ICPAQGP5, Kolkata Feb 8 – 12 1 Measurement of  ++ Resonance Production in d+Au sqrt(s NN ) = 200 GeV Dipak Mishra.
A generalized Buda-Lund model M. Csanád, T. Csörgő and B. Lörstad (Budapest & Lund) Buda-Lund model for ellipsoidally symmetric systems and it’s comparison.
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.
What do the scaling characteristics of elliptic flow reveal about the properties of the matter at RHIC ? Michael Issah Stony Brook University for the PHENIX.
Fall DNP Meeting,  meson production in Au-Au and d-Au collision at \ /s NN = 200 GeV Dipali Pal Vanderbilt University (for the PHENIX collaboration)
M. J. TannenbaumQuarkMatter M. J. Tannenbaum Brookhaven National Laboratory Upton, NY USA for the PHENIX Collaboration Event-by-Event Average.
Richard Petti For the PHENIX Collaboration
Monika Sharma Wayne State University for the STAR Collaboration
High-pT Identified Hadron Production in Au+Au and Cu+Cu Collisions
ATLAS vn results vn from event plane method
Example analysis of toy model
Takafumi Niida from Univ. of Tsukuba for the PHENIX Collaborations
for the PHENIX collaboration
Identified Charged Hadron Production
Directed Flow from Au+Au Collisions at 200 GeV
Stony Brook University
Presentation transcript:

1 Paul Chung ( for the PHENIX Collaboration ) Nuclear Chemistry, SUNY, Stony Brook Evidence for a long-range pion emission source in Au+Au collisions at

P. Chung, SUNY Stony Brook 2 Outline 1. Motivation 2. Brief Review of Apparatus & analysis technique 3.1D Results Angle averaged correlation function Angle averaged source function 4.3D analysis Correlation moments Source moments 5.Conclusion/s

P. Chung, SUNY Stony Brook 3 initial state pre-equilibrium QGP and hydrodynamic expansion hadronization hadronic phase and freeze-out Conjecture of collisions at RHIC : Motivation Which observables & phenomena connect to the de-confined stage? Courtesy S. Bass

P. Chung, SUNY Stony Brook 4 QGP and hydrodynamic expansion One Scenario : Motivation Expectation: A de-confined phase leads to an emitting system characterized by a much larger space-time extent than would be expected from a system which remained in the hadronic phase Increased System Entropy that survives hadronization

P. Chung, SUNY Stony Brook 5 Experimental Setup PHENIX Detector Several Subsystems exploited for the analysis Excellent Pid is achieved

P. Chung, SUNY Stony Brook 6 Analysis Summary Image analysis in PHENIX Follows three basic steps. I. Track selection II. Evaluation of the Correlation Functions (with pair-cuts etc. III.Analysis of correlation functions: Imaging Direct fits 1D & 3D analysis

P. Chung, SUNY Stony Brook 7 Cuts Dphi (rad) Dz (cm)

P. Chung, SUNY Stony Brook 8 Cuts Dz (cm) Dphi (rad)

P. Chung, SUNY Stony Brook 9 Imaging Technique Technique Devised by: D. Brown, P. Danielewicz, PLB 398:252 (1997). PRC 57:2474 (1998). Inversion of Linear integral equation to obtain source function Source function (Distribution of pair separations) Encodes FSI Correlationfunction Inversion of this integral equation ==  Source Function Emitting source 1D Koonin Pratt Eqn.

P. Chung, SUNY Stony Brook 10 Imaging Inversion procedure

P. Chung, SUNY Stony Brook 11 Correlation Fits Parameters of the source function Minimize Chi-squared [Theoretical correlation function] convolute source function with kernel (P. Danielewicz) Measured correlation function

P. Chung, SUNY Stony Brook 12 Input source function recovered Procedure is Robust ! Quick Test with simulated source

P. Chung, SUNY Stony Brook 13 Fitting correlation functions Kinematics “Spheroid/Blimp” Ansatz Brown & Danielewicz PRC 64, (2001)

P. Chung, SUNY Stony Brook 14 Evidence for long-range source at RHIC 1D Source imaging PHENIX Preliminary

P. Chung, SUNY Stony Brook 15 Extraction of Source Parameters Fit Function (Pratt et al.) This fit function allows extraction of both the short- and long-range components of the source image This fit function allows extraction of both the short- and long-range components of the source image Bessel Functions Radii Pair Fractions

P. Chung, SUNY Stony Brook 16 Source functions from spheroid and Gaussian + Exponential are in excellent agreement Comparison of Source Functions

P. Chung, SUNY Stony Brook 17 PHENIX Preliminary Centrality dependence incompatible with resonance decay

P. Chung, SUNY Stony Brook 18 Short and long-range components of the source Short-range  Long-range  T. Csorgo M. Csanad

P. Chung, SUNY Stony Brook 19 Short and long-range components of the source T. Csorgo M. Csanad

P. Chung, SUNY Stony Brook 20 Pair fractions associated with long- and short-range structures T. Csorgo M. Csanad Core Halo assumption Expt  Contribution from decay insufficient to account for long- range component.

P. Chung, SUNY Stony Brook 21 New 3D Analysis 1D analysis  angle averaged C(q) & S(r) info only no directional information Need 3D analysis to access directional information Correlation and source moment fitting and imaging

P. Chung, SUNY Stony Brook 22 3D Analysis (3) 3D Koonin Pratt Plug in (1) and (2) into (3) (1) (2) Expansion of R(q) and S(r) in Cartesian Harmonic basis Basis of Analysis (Danielewicz and Pratt nucl-th/ (v1) 2005)

P. Chung, SUNY Stony Brook 23 3D Analysis How to calculate correlation function and Source function in any direction Source function/Correlation function obtained via moment summation

P. Chung, SUNY Stony Brook 24 PHENIX Preliminary 3D Source imaging Deformed source in pair cm frame: Origin of deformation Kinematics ? or Time effect Instantaneous Freeze-out LCMS implies kinematics PCMS implies time effect

P. Chung, SUNY Stony Brook 25 PHENIX Preliminary 3D Source imaging Spherically symmetric source in pair cm. frame (PCMS) Isotropic emission in the pair frame

P. Chung, SUNY Stony Brook 26 Extensive study of two-pion source Extensive study of two-pion source images and moments in Au+Au collisions at RHIC images and moments in Au+Au collisions at RHIC First observation of a long-range source having an First observation of a long-range source having an extension in the out direction for pions extension in the out direction for pions First explicit determination of a spherical proton source First explicit determination of a spherical proton source Further Studies underway to quantify extent of long-range source!

P. Chung, SUNY Stony Brook 27

P. Chung, SUNY Stony Brook 28 Two source fit function This is the single particle distribution

P. Chung, SUNY Stony Brook 29 Simulation tests of the method Very clear proof of principle Procedure Generate moments for source. Carryout simultaneous Fit of all moments input output

P. Chung, SUNY Stony Brook 30 Two source fit function This is the two particle distribution