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Two Particle Interferometry at RHIC. Sergey Panitkin (Brookhaven National Laboratory). Outline. Introduction and Motivation Summary of Results from AuAu 130 GeV Results from AuAu 200 GeV PHOBOS PHENIX STAR (see talks by M. Lisa, V. Okorokov) Summary and outlook. q Side. q Out. p y. - PowerPoint PPT Presentation
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Sergey Panitkin
Two Particle Interferometry at RHIC
Sergey Panitkin
(Brookhaven National Laboratory)
Sergey Panitkin
Outline
Introduction and Motivation Summary of Results from AuAu 130 GeV Results from AuAu 200 GeV
– PHOBOS– PHENIX– STAR (see talks by M. Lisa, V. Okorokov)
Summary and outlook
Sergey Panitkin
Information:
•geometrical source size: Rside
•lifetime
(for simple sources!)
)( 222222
1),,( LongLongSideSideOutOut RqRqRqLongSideOut eqqqC
px
qOutpy
qSideDecomposition of the pair relative momentum
(measured in the LCMS frame; (p1+ p2)z=0)
Pratt-Bertsch Parameterization
Rside2=R0ut
2-(pair)2
Sergey Panitkin
Pion Correlation Functions at RHIC
Open symbols – No Coulomb
Solid – Coulomb corrected
Red line – Gaussian fit
Experimental effects that were evaluated:Single track cutsTrack mergingTrack splittingPID Impurities
Finite radius CoulombMomentum resolutionEvent vertex mixing
STAR 130 GeV
Sergey Panitkin
In Search of the QGP. Naïve expectations
QGP has more degrees of freedom than pion gas
Entropy should be conservedduring fireball evolution
Hence: Look in hadronic phasefor signs of: Large size, Large lifetime, Expansion……
Sergey Panitkin
In search of the QGP: Expectations
“Naïve” picture (no space-momentum correlations):
– Rout2=Rside
2+(pair)2
One step further:– Hydro calculation of Rischke
& Gyulassy expects Rout/Rside ~ 2->4 @ kt = 350 MeV.
– Looking for a “soft spot”
Rout
Rside
Sergey Panitkin
Excitation function of the HBT parameters
• ~10% Central AuAu(PbPb) events
• y ~ 0
• kT 0.17 GeV/c
no significant rise in spatio-temporal size of the emitting source at RHIC
Note ~100 GeV gap betweenSPS and RHIC !
Sergey Panitkin
The Rout/Rside Ratio at 130 GeV
Hydro +UrQMD
Smaller observed ratio than expected from theory.
Different KT dependence.Data -> Short freeze-outModel -> Extended freeze-out
(S. Soff et al)
RHIC HBT Puzzle
STAR
Sergey Panitkin
RHIC HBT PUZZLE
P.Kolb
Small Rout implies small
Large Rside implies large RSmall Rbeam impliessmall lifetime ~10 fm/c
But Hydro fits spectra and v2 nicely!
Sergey Panitkin
RHIC HBT Puzzle
Most “reasonable” models still do not reproduce RHIC √SNN = 130GeV HBT radii
“Blast wave” parameterization (Sollfrank
model) can approximately describe data at 130
GeV
…but emission duration must be small
= 0.6 (radial flow)
• T = 110 MeV
• R = 13.5 1fm (hard-sphere)
emission= 1.5 1 fm/c (Gaussian)
fromspectra, v2
√SNN = 130GeVPHENIX PRL 88 192302 (2002)
STAR 130 GeV
PHENIX 130 GeV
Hydro + RQMD
+-
Sergey Panitkin
PHENIX kT dependence of source radiiCentrality is in top 30%
Sergey Panitkin
PHENIX Centrality dependence @ 200 GeV
Fit with p0+p1*Npart^1/3
Rlong increases more rapidly with the Npart
than Rout.
0.2<kT<2.0GeV/c, <kT>=0.46GeV/c
Rlong ~ Rside
Sergey Panitkin
Centrality and mT dependence at 200 GeV
RL varies similar to RO, RS with centrality
HBT radii decrease with mT (flow)
Roughly parallel mT dependence for different centralities
RO/RS ~ 1 (short emission time)
Central
Midcentral
Peripheral
200GeV
STAR PRELIMINARY
Sergey Panitkin
Comparison to 130 GeV. Transverse radii
*
Central
Midcentral
Peripheral
PHENIX Central
200GeV - 130 GeV
Higher B-field higher pT
Transverse radii:
• similar but not identical• low-pT RO, RS larger at 200 GeV• steeper falloff in mT
(PHENIX 130GeV)• Ro falls steeper with mT
STAR PRELIMINARY
Statistical errors only
Sergey Panitkin
Rout/Rside Ratios at 200 GeV
Ratio is <1 at high Pt (but note different centralities!)
Errors are statistical + systematic
Sergey Panitkin
Evolution timescale from RL
(fit to STAR 200GeV data only)
Simple Mahklin/Sinyukov fit (assuming boost-invariant longitudinal flow)
T
KfoL m
TtR
Assuming TK=110 MeV(from spectra at 130 GeV)
fm/c 6.7t
fm/c 10t
periphfo
centralfo
Makhlin and Sinyukov,
Z. Phys. C 39 (1988) 69
STAR PRELIMINARY
Longitudinal radius:at 200GeV identical to 130 GeV
rapid evolution!!!
*
Central
Midcentral
Peripheral
PHENIX Central
200GeV - 130 GeV
Sergey Panitkin
What have we learned about pion source S(x,p) ?
Pion spectra shapes plus HBT RO,S,L(KT): T ~ 100 MeV <> ~ 0.6 R ~ 12 fm t0~10 fm/c Rout/Rside described by sharp radial cut-off and brief emission duration, ~2 fm/c which squeezes Rout
Increased pion phase space density (see talk by R. Lednicky)Azimuthal dependence points toward fast break up of the source (see talk by M. Lisa)
Sergey Panitkin
Comparison of kaons to pions
In the most 30% central
Mt scaling violation ?
Sergey Panitkin
STAR K0s Reconstruction
Number of K0s
Mean ~ 3.79 / Event
Nu
mb
er o
f ev
entsDCA – distance of closest approach
pT(GeV/c)
pT ~ 1 GeV/cmT ~ 1.12 GeV/c2c
ou
nts
DCA between daughters
DCA of daughters to primary vertex
DCA of V0 to primary vertex
Decay Length
Vo
Sergey Panitkin
K0sK0
s Correlations from STAR
STAR PRELIMINARY
S/N = 19.11
Minv (GeV/c2)
cou
nts
0.46 0.48 0.50 0.52
blue: signal from fit
red : noise
A promising low-Q correlation!
Qinv (GeV/c)
CF STAR PRELIMINARY
• no coulomb interaction
• less affected by long-lived resonance feed-down
• extend systematic to higher pT
• strangeness dynamics
• unique measurement
Large source for <mT> ~ 1.12 GeV/c2 ???systematic study underway…
=0.76 0.29Rinv=5.75 ± 1.0 fm
Sergey Panitkin
Summary
Lots of new data from all RHIC experiments ! So far no obvious inconsistencies in pion HBT data
interferometry:
sources sizes at 200 roughly same as at 130GeV, with similar systematics:
radii decrease with mT: consistent with radial flow mT dependence independent of centrality
RO/RS ~ 1 over large Pt range: short emission duration RL (mT): Sinyukov fits → evolution time: <> ≈ 10fm/c systematics study underway
Kaon interferometry: Mt scaling violation (Charged kaons –PHENIX, K0 – STAR) ? More data needed (coming soon!)
More data to come soon ! Need theoretical explanation!
Sergey Panitkin
Fireball dynamics: Collective expansion
tanh 1 r r (r) s f (r)
R
s
Flow profile used
r =s (r/R)0.5
dn
mT dmT r dr mT K1
mT coshT
0
R
I0pT sinh
T
Shape of the mT spectrum depends on particle mass
Inverse-slope depends on mT-range
where and
The model is from E.Schenedermann et al. PRC48 (1993) 2462 and based on Blast wave model
Description of freeze-out inspired by hydrodynamics
Sergey Panitkin
Blast wave at 200 GeV: Fails?
10% central negative pion HBT radii. Systematic uncertainty in the data is 8.2% for Rs, 16.1% for Ro, 8.3% for RL.
From the spectra (systematic errors):T = 0.7 ± 0.2 syst. Tfo = 110 23 syst. MeV
--
0 = 132 fm/cR = 9.7±0.2 fm
PHENIX PreliminaryRs (fm) Ro (fm) RL (fm)
J. Burward-Hoy(QM2002)
Model by Wiedemann, Scotto, Heinz, PRC 53 (No. 2), Feb. 1996