3d pion & kaon source imaging from run4 and run7 200 agev au+au collisions
DESCRIPTION
Paul Chung (STAR Collaboration) NPI ASCR Prague. 3D Pion & Kaon Source Imaging from Run4 and Run7 200 AGeV Au+Au collisions. 1. PHENIX 1D Source Imaging. Phys.Rev.Lett.98:132301,2007. Phys.Rev.Lett.103:142301,2009. Outline. Run 4 Au+Au @ 200AGeV: 3D pion correlation functions - PowerPoint PPT PresentationTRANSCRIPT
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3D Pion & Kaon Source Imaging from Run4 and Run7 200 AGeV Au+Au collisions
Paul Chung (STAR Collaboration)NPI ASCR Prague
PHENIX 1D Source Imaging Phys.Rev.Lett.98:132301,2007
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Phys.Rev.Lett.103:142301,2009
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Outline
Run 4 Au+Au @ 200AGeV: 3D pion correlation functions Overview of 3D source shape analysis : Cartesian
Spherical Harmonic decomposition & Imaging Technique Correlation moments for low kT (0.25<kT<0.35 GeV)
pion pairs from peripheral collisions (50<cen<80%). 3D source function extraction: Moment Imaging & Fitting Therminator comparison for extracting pion source
lifetime & pion emission duration 3D Kaon correlation functions from Run 4 & Run 7
central Au+Au collisions Kaon source extraction & Therminator comparison
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Technique Devised by:
D. Brown, P. Danielewicz,PLB 398:252 (1997). PRC 57:2474 (1998).
Inversion of Linear integral equation to obtain source function
20( ) 1 ) (,4 ( )C K q r S rq drr
Source Source functionfunction
(Distribution of pair separations)
Encodes FSI
CorrelationCorrelationfunctionfunction
Inversion of this integral equation== Source Function
Emitting source
1D Koonin Pratt Eqn.
Extracted S(r) in pair CM frameHence Model-independent i.e Kernel independent of freeze-out conditions
No Shape assumption for S(r)
1D Imaging Formulation 1D Imaging Formulation
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Imaging : Inversion procedureImaging : Inversion procedure2( ) 4 ( , ) ( )C q drr K q r S r
( ) ( )j jj
S r S B r
( )
( , ) ( )
Thi ij j
j
ij j
C q K S
K dr K q r B r
2
22
( )
( )
Expti ij j
jExpt
i
C q K S
C q
Freeze-out occurs after last scattering Hence only Coulomb & BE effect included in kernel
Expansion in B-spline basis
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1 11
1 11
.... ........
.... ........
( ) ( ) (1)
( ) ( ) (2)
l ll
l ll
l lq
l
l lr
l
R q R q
S r S r
3( ) ( ) 1 4 ( , ) ( )R q C q dr K q r S r
(3)3D Koonin3D KooninPrattPratt
Plug in (1) and (2) into (3)1 1
2.... ....
( ) 4 ( , ) ( ) (4)l l
l llR q drr K q r S r
1 1
1 1
.... ....
.... ....
2 1 !!( ) ( ) ( ) (4)
! 42 1 !!
( ) ( ) ( ) (5)! 4
l l
l l
ql lq
l lrr
dlR q R q
ll dS r S rl
Invert (1)
Invert (2)
Expansion of R(q) and S(r) in Cartesian Harmonic basisExpansion of R(q) and S(r) in Cartesian Harmonic basis[Danielewicz and Pratt nucl-th/0501003 (v1)][Danielewicz and Pratt nucl-th/0501003 (v1)]
x=out-direction
y=side-direction
z=long-direction
3D Analysis Basics
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Monte Carlo Events:Phasemaker, Therminator
CRAB 3D C(q)
Correlation MomentsSource FITTING
Source IMAGING
SourceFunction
Model calculation from space points
SIMULATION PROCEDURE
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Fit Functions
Ellipsoid Fit (3D Gaussian) : G = lambda exp[-{ (x/2rx)2 + (y/2ry)2 + (z/2rz)2 }]
Hump Fit :H = exp[- Fs { (x/2rxs)2 + (y/2rys)2 + (z/2rzs)2 }] x
exp[- Fl { (x/2rxl)2 + (y/2ryl)2 + (z/2rzl)2 }]
Fs = 1/[1 + (r/r0)2 ]
Fl = 1 - Fs
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3D Imaging – S(r) & restored C(q)
STAR PRELIMINARY
STAR PRELIMINARY
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Ellipsoid vs Hump Fit : l=4 moments
STAR PRELIMINARYSTAR PRELIMINARY
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Therminator BW: Source lifetime & Pion emission duration extractionTherminator (Kisiel et al PRC
73, 064902 2006) : Production of particles from thermalized and expanding system with
Boost invariance & cylindrical symmetry
BW mode: Freeze-out hypersurface defined by constant laboratory time independent of transverse radius
Source extraction – central collisions PRL100, 232301 (2008) (PHENIX) Transverse dimension = 8.9fm
Source lifetime = 8.5fm/cEmission duration = 2fm/c
Source parameters larger for central collisions than for peripheral collisions
Full centrality dependence extraction underway
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Run 7 & Run 4 KK : C0 vs 1D C(qinv)
STAR PRELIMINARY STAR PRELIMINARY
Run 7 + Run 4 KK : l=2 & l=4 moments
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STAR PRELIMINARY STAR PRELIMINARY
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Conclusion
Correlation moments for low kT pion pairs from Run4 peripheral Au+Au collisions well described by the Hump Fit function.
For low kT pion pairs from peripheral collisions, inferred pion source lifetime ~ 3.5 fm/c & pion emission duration ~ 1 fm/c < central collisions.
Extracted Kaon source function essentially Gaussian – No significant non-Gaussian tail observed.
Kaon source dimension & lifetime smaller than for pion source; Kaon emission instantaneous (Therminator)