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Sergey Panitkin Two Particle Interferometry at RHIC Sergey Panitkin (Brookhaven National Laboratory)

Two Particle Interferometry at RHIC

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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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Page 1: Two Particle Interferometry at RHIC

Sergey Panitkin

Two Particle Interferometry at RHIC

Sergey Panitkin

(Brookhaven National Laboratory)

Page 2: Two Particle Interferometry at RHIC

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

Page 3: Two Particle Interferometry at RHIC

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

Page 4: Two Particle Interferometry at RHIC

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

Page 5: Two Particle Interferometry at RHIC

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……

Page 6: Two Particle Interferometry at RHIC

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

Page 7: Two Particle Interferometry at RHIC

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 !

Page 8: Two Particle Interferometry at 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

Page 9: Two Particle Interferometry at RHIC

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!

Page 10: Two Particle Interferometry at RHIC

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

+-

Page 11: Two Particle Interferometry at RHIC

Sergey Panitkin

PHENIX kT dependence of source radiiCentrality is in top 30%

Page 12: Two Particle Interferometry at RHIC

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

Page 13: Two Particle Interferometry at RHIC

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

Page 14: Two Particle Interferometry at RHIC

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

Page 15: Two Particle Interferometry at RHIC

Sergey Panitkin

Rout/Rside Ratios at 200 GeV

Ratio is <1 at high Pt (but note different centralities!)

Errors are statistical + systematic

Page 16: Two Particle Interferometry at RHIC

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

Page 17: Two Particle Interferometry at RHIC

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)

Page 18: Two Particle Interferometry at RHIC

Sergey Panitkin

Comparison of kaons to pions

In the most 30% central

Mt scaling violation ?

Page 19: Two Particle Interferometry at RHIC

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

Page 20: Two Particle Interferometry at RHIC

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

Page 21: Two Particle Interferometry at RHIC

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!

Page 22: Two Particle Interferometry at RHIC

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

Page 23: Two Particle Interferometry at RHIC

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