Jana Bielcikova (Yale University) for the STAR Collaboration 23 rd Winter Workshop on Nuclear...

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Jana Bielcikova (Yale University) for the STAR Collaboration 23 rd Winter Workshop on Nuclear Dynamics February 12-18, 2007 Two-particle correlations with strange baryons and mesons at RHIC
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Transcript of Jana Bielcikova (Yale University) for the STAR Collaboration 23 rd Winter Workshop on Nuclear...

Jana Bielcikova (Yale University) for the STAR Collaboration

23rd Winter Workshop on Nuclear Dynamics February 12-18, 2007

Two-particle correlations with strange baryons and mesons at

RHIC

Jana Bielcikova 23rd Winter Workshop on Nuclear Dynamics

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Outline:

• Physics motivation• Correlations with identified strange trigger

particles (Λ, Λ and K0

S) in d+Au and Au+Au collisions

• Correlations with identified strange associated particles

(Λ, Λ and K0S) in central Au+Au collisions

• Summary

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RCP:• intermediate pT : baryon/meson splitting independent of strangeness content• high pT (pT > 5 GeV/c) : all particles have similar RCP and appear to show similar suppression •large enhancement of baryon/meson ratio in central Au+Au relative to p+p collisions - reaches maximum at pT~3 GeV/c

• jet fragmentation is not a dominant source of particle production

Baryon/meson anomaly at intermediate pT

Jana Bielcikova 23rd Winter Workshop on Nuclear Dynamics

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Parton recombination at intermediate pT

• in vacuo fragmentation of a high momentum quark to produce hadrons competes with in medium recombination of lower momentum quarks to produce hadrons

•6 GeV/c particle via : fragmentation from high pT

meson - 2 quarks at pT~3 GeV/c baryon - 3 quarks at pT~2 GeV/cRecombination produces more baryons than mesons at intermediate pT

R.J. Fries et al., PRL 90 (202303) 2003V. Greco et al., PRL 90 (202302) 2003

baryon

meson

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Jet-like correlations at RHIC

central Au+Au collisions @ 200 GeV:

• disappearance of away-side correlations observed at intermediate pT

• d+Au and p+p similar -> jet suppression is a final state effect

• lowering associated pT :

- resurrects correlated yield at away side

- near and away-side yields are enhanced with respect to d+Au

0.15<pT(assoc)<4.0 GeV/c4 <pT(trig)<6 GeV/c 2 GeV/c <pT(assoc)<pT(trig)

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Correlations with identified particles

provide additional information on:• baryon/meson enhancement • medium modification of jet shape • particle production mechanisms

coalescence/recombination mechanisms

and/or (modified) fragmentation of high-pT partons?

parton

hadrons

hadrons

Λ, Λ, K0S, γ … ?

Λ, Λ, K0S, γ … ?

parton

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Correlations at near-side

a.u.

pTtrig=3-6 GeV/c, 1.5 GeV/c <pT

assoc< pTtrig

Au+Au central @ 200 GeV

ridge

ridge

jetjet+ridge

after v2 subtraction

jetridge

v2 + away-side peak h-h

Au+Au: long-range correlations at near side (“the ridge”)

Near-side yield : Δɸ (J+R) = Δɸ (J) + Δɸ (R) Jet yield : Δɸ (J) = Δɸ (|Δη| < 0.7) - Δɸ (|Δη| > 0.7) Ridge yield : Δɸ (R) = Δɸ (J+R) - Δɸ(J)

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before elliptic flow subtraction

Correlations with strange particle triggers in Au+Au at 200 GeV

Selection criteria:• 3.0 GeV/c < pT

trigger < 3.5 GeV/c • 1 GeV/c < pT

associated < 2 GeV/c• || < 1

Correlation function:• normalized per trigger particle• corrected for reconstruction efficiency of associated charged particles• acceptance corrected

STAR preliminarySTAR preliminary

STAR preliminarySTAR preliminarySTAR preliminarySTAR preliminary

STAR preliminarySTAR preliminary

trigger: baryon/meson baryon/antibaryon

after elliptic flow subtraction (using ZYAM method) Ajitanand et al, PRC72 (2005) 011902

systematic errors due to v2 uncertainty ~ 30%

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• steep increase of near-side yield with centrality in Au+Au• ratio of yields in central Au+Au/d+Au ~ 4-5

-> “jet” yield is independent of centrality and agrees with d+Au (effects of merged tracks under study)

JetJet + Ridge

-> “ridge” yield increases with centrality ridge of K0

S < ridge of Λ

Ridge

Centrality dependence of near-side yield

Jet

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pTtrigger dependence of jet and ridge

yields

• near-side associated yield is ridge dominated at intermediate pT

• jet yield: - increases steeply with pT

trigger

- smaller for Λ-triggers than for K0S-triggers ?

- baryon jet is wider than meson jet - effects of merged tracks under study • jet/ridge ratio increases with pT

trigger

Jet + Ridge Ridge Jet

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pT-distribution of associated particles

Trigger particle T(ridge) MeV T (jet) MeV

h+/- 438 ± 4 (stat.) 478 ± 8

K0S 406 ± 20 (stat.) 530 ± 61

Λ 416 ± 11 (stat.) 445 ± 49

STAR preliminary“jet” sloperidge slopeinclusive slope

J. Putschke (STAR), QM’06

h-h correlationspT

associated>2GeV/c

• Ridge spectra similar to particles from the bulk• Jet spectra are harder(T increases steeply with pT

trig)

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central-to-peripheral ratio (“ICP”): - ~ 3 at pT

associated = 1 GeV/c - decreases slowly with pT

associated

- jet yield is independent of centrality “ICP” is driven by long-range Δη correlations

• qualitative agreement with the parton recombination model BUT!• quantitative agreement requires same centrality and pT selection• check required on how well the “ridge” is reproduced by the model

• call for predictions for identified particles

What does a parton recombination model predict?

jet

ReCo: R. Hwa, Z.Tan: PRC72 (057902) 2005

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Particle composition in the ridge

/K0S ratio:

in the ridge: ~ 1.0 similar to that from inclusive pT spectra in the jet: ~ 0.5 consistent with p+p

|Δη|<2.0 |Δη|<0.7

STAR preliminary STAR preliminary

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What is the origin of the ridge ? 1) Parton radiation and its coupling to the longitudinal flow

• gluon bremsstrahlung of hard-scattered parton parton is shifted to lower pT

• radiated gluon contributes to broadening

2) Medium heating + parton recombination Chiu & Hwa Phys. Rev. C72:034903,2005

• hard parton passing through the medium enhanced thermal parton distribution (ΔT=15 MeV) recombination of thermal partons forms a pedestal (ridge)

• pedestal is not a part of the jet • enhanced baryon/meson ratio

3) Radial flow + trigger bias S.Voloshin, nucl-th/0312065, Nucl. Phys. A749, 287 (2005)

4) Longitudinal broadening of quenched jets in turbulent color field

A. Majumder, B. Mueller, S.A.Bass, hep-ph/0611135

• plasma instabilities in expanding medium broadening of jet cone

wide ridge in rapidity at low pTassoc

Armesto et al, PRL 93 (2004)

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Correlations with strange trigger particles:

- system size: strong increase (~4-5) of the near-side yield in central Au+Au in comparison to d+Au collisions due to long-range Δη correlations (“ridge”).

Ongoing studies of correlations in Cu+Cu. - ridge yield: steep increase with centrality, slope of pT spectra similar to that of “bulk”

- jet yield: consistent with d+Au, constant with centrality, increasing with pT

trigger

Correlations with strange associated particles:

B/M ratio in the ridge: close to the bulk

B/M ratio in the jet: consistent with p+p

The data qualitatively agree with recombination picture, but more detailed

comparisons are needed to draw final conclusions.

Summary

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BACKUP

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Analysis method

raw data correlation mixed events correlation corrected data correlation

h-K0S, 3 < pT

trig < 6 GeV/c, 2 < pTassoc < 3 GeV/c

ridge jetAu+Au, 0-10%