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Strange Baryon Production at RHIC Hui Long Department of Physics University of California, Los Angeles 1. Introduction 2. Strangeness measurement and results > results of bulk properties ( yield, freeze-out T, event anisotropy ) > results from intermediate P T ( <10 GeV/c) on Nuclear modification factor of Λ and Ks. 3. Summary

Strange Baryon Production at RHIC · 2003. 10. 15. · Strange Baryon Production at RHIC Hui Long Department of Physics University of California, Los Angeles 1. Introduction 2. Strangeness

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Page 1: Strange Baryon Production at RHIC · 2003. 10. 15. · Strange Baryon Production at RHIC Hui Long Department of Physics University of California, Los Angeles 1. Introduction 2. Strangeness

Strange Baryon Production at RHICHui Long

Department of PhysicsUniversity of California, Los Angeles

1. Introduction

2. Strangeness measurement and results

> results of bulk properties

( yield, freeze-out T, event anisotropy )

> results from intermediate PT ( <10 GeV/c) on

Nuclear modification factor of Λ and Ks.

3. Summary

Page 2: Strange Baryon Production at RHIC · 2003. 10. 15. · Strange Baryon Production at RHIC Hui Long Department of Physics University of California, Los Angeles 1. Introduction 2. Strangeness

(p, d,…Au)100 GeV/nucleon

PHOBOS BRAHMS

STARPHENIX

Page 3: Strange Baryon Production at RHIC · 2003. 10. 15. · Strange Baryon Production at RHIC Hui Long Department of Physics University of California, Los Angeles 1. Introduction 2. Strangeness

Introduction : Physics Goal of RHIC

Identify and study the properties of the matter with partonic degree of freedom:

- nuclear effects in the intermediate pT regioninitial conditions;parton energy loss due to interaction of dense matter.

- bulk propertiescollision dynamics;collective motion with the partonic degree of freedom;early thermalization (c-quark).

Strange particles can be good probes to both !!!

Page 4: Strange Baryon Production at RHIC · 2003. 10. 15. · Strange Baryon Production at RHIC Hui Long Department of Physics University of California, Los Angeles 1. Introduction 2. Strangeness

(GeV/c)tP

0 0.5 1 1.5 2

-2dy

(GeV

/c)

tN

/dP

2 d t1/

Pev

t1/

1/2

10-2

10-1

1

10

102

103

21×

(min-bias)Λ

(min-bias)Λ

(central)Λ

(central)Λ

Strange Baryon Measurement at RHIC ( 130 GeV)

Λ p + π-

Ξ− Λ + π-

Ω− Λ + κ-

-2 )2

dy

(GeV

/c⊥

N/d

m2 d ⊥

mπ1/

(2ev

t1/

N

10-6

10-5

10-4

10-3

10-2

10-1

1

-Ξ(a)

)2- m (GeV/c⊥m

+Ξ(b)

1 2

+Ω+-Ω(c)

[0-10%][0-10%] [10-25%] (/5) [25-75%] (/10)

01 201 20

STAR

PHENEX

Page 5: Strange Baryon Production at RHIC · 2003. 10. 15. · Strange Baryon Production at RHIC Hui Long Department of Physics University of California, Los Angeles 1. Introduction 2. Strangeness

Strange Baryon Yield at Mid-rapidity (130 GeV)

Ω+⎯Ω

STAR Preliminary

Nearly linear dependence on number of charged particles

Page 6: Strange Baryon Production at RHIC · 2003. 10. 15. · Strange Baryon Production at RHIC Hui Long Department of Physics University of California, Los Angeles 1. Introduction 2. Strangeness

Ratio of Particle Yield and Statistic Model:..T, µb γs

( integrated yield dominated by low pt particles)

One of the bulk properties: Tch ~ 176 MeV(Chemical freeze-out: particle’s yield remain unchanged since )

Page 7: Strange Baryon Production at RHIC · 2003. 10. 15. · Strange Baryon Production at RHIC Hui Long Department of Physics University of California, Los Angeles 1. Introduction 2. Strangeness

ρ = tanh−1 βr

R

β s

E.Schnedermann et al, PRC48 (1993) 2462

dnmT dmT

∝ r dr mT K1mT cosh ρ

T⎛ ⎝

⎞ ⎠

0

R

∫ I0pT sinh ρ

T⎛ ⎝

⎞ ⎠

where

βT =βs (r/R)n

Strange Baryon and Hydro-dynamic Fit (130 GeV)1 σ, 2σ , 3 σ contours

Ξ s behave differently !! Higher Tfo-- >Freeze-out earlier

Tfo ~ Tch -- transverse flow at/before chemical freeze-out, maybe at partonic stage ?

Hydro-dynamic fit: T, β ( Thermal + Transverse flow )

Thermal freeze-out: particle pT distribution stable since

βΤ

Page 8: Strange Baryon Production at RHIC · 2003. 10. 15. · Strange Baryon Production at RHIC Hui Long Department of Physics University of California, Los Angeles 1. Introduction 2. Strangeness

Event Anisotropy– What’s Elliptic Flow ?

( )( )3 2

31

1 1 2 cos2 n r

nt t

d N d NE v nd p p dp dy

ϕπ

=

⎛ ⎞= + −Ψ⎜ ⎟

⎝ ⎠∑

coordinate spacey

x

12 , tan ( )cos2( ) y

xrv

pp

ϕϕ −== −ΨMomentum space

py

pxEffected by pressure gradient, surface emission pattern, final re-scattering.

Page 9: Strange Baryon Production at RHIC · 2003. 10. 15. · Strange Baryon Production at RHIC Hui Long Department of Physics University of California, Los Angeles 1. Introduction 2. Strangeness

Features of Elliptic Flow at RHIC

Low pt : hydro-like collective behaviorHigh pt : lower than hydro-limit and the trend

consistent with expectation from jet-quenching due to parton energy loss.

Page 10: Strange Baryon Production at RHIC · 2003. 10. 15. · Strange Baryon Production at RHIC Hui Long Department of Physics University of California, Los Angeles 1. Introduction 2. Strangeness

Strange Hadron (Ks and Λ ) V2 (200 GeV)

Hydro behavior at pt<2 GeV

, V2(Λ) <V2(K)

When pt> 2.5GeV, V2(Λ) >V2(K) !!!

--Energy Loss ?--Coalescence ?

Partonic dof relevant ?

Page 11: Strange Baryon Production at RHIC · 2003. 10. 15. · Strange Baryon Production at RHIC Hui Long Department of Physics University of California, Los Angeles 1. Introduction 2. Strangeness

Strange Particle v2 and Coalescence

V2 ~ n

-> Ξ , Ω v2 = Λ v2

Partonic collectivityat RHIC ?

Z Lin, PRL, 89,202302(02)S. Voloshin, nu-ex/0210014R. Fries et al. nucl-th/0301087D. Molnar et al. nucl-th/0302014

Page 12: Strange Baryon Production at RHIC · 2003. 10. 15. · Strange Baryon Production at RHIC Hui Long Department of Physics University of California, Los Angeles 1. Introduction 2. Strangeness

Strange Baryon in Intermediate PT : Nuclear Modification

Npart: Number of participants number of incoming nucleons (participants) in the overlap region

ησηddpdT

ddpNdpRT

NNAA

TAA

TAA //)( 2

2

=

<Nbinary>/σinelp+p

N-N cross sectionNuclear Modification Factor:

If no “effects”:R < 1 in regime of soft physicsR = 1 at high-pt where hard

scattering dominates

Nbin: Number of binary collisions number of equivalent inelastic nucleon-nucleon collisions

Page 13: Strange Baryon Production at RHIC · 2003. 10. 15. · Strange Baryon Production at RHIC Hui Long Department of Physics University of California, Los Angeles 1. Introduction 2. Strangeness

Suppression of High pT Charged Hadrons

Preliminary √sNN = 200 GeV

1.0

1.0

1.0

Strong Suppressionin central Au+Au

N-Binary Scalingin peripheral Au+Au

Similar suppression pattern for π0 and for 130 GeV Au+Au dataand also observed by PHENIX

Used UA1 p+p 200 GeV data (pT<6 GeV/c) as reference

Page 14: Strange Baryon Production at RHIC · 2003. 10. 15. · Strange Baryon Production at RHIC Hui Long Department of Physics University of California, Los Angeles 1. Introduction 2. Strangeness

Rcp of Strange Particles

Different pt dependencesbetween Rcp(Λ) and Rcp(K)

At pt~5 GeV/c, all the Rcpapproach each other.

0-2 GeV, Flow effects ?

2-4 GeV, Coalescence ?

>5GeV, Fragmentation ?

partonicmatter

Page 15: Strange Baryon Production at RHIC · 2003. 10. 15. · Strange Baryon Production at RHIC Hui Long Department of Physics University of California, Los Angeles 1. Introduction 2. Strangeness

Summary (I)

bulk properties

Yield and Freeze-out T

-almost linear increase with charged hadrons ;

- earlier freeze-out and high freeze-out T of multi-

strange baryon Ξ - partonic radial flow ?

Event anisotropy

- hydro behavior of v2 at pt< 2GeV/c;

- heavier particle has larger saturated v2 at pt>2 Gev/c; ? Coalescence model ? Partonic Collectivity ?

Page 16: Strange Baryon Production at RHIC · 2003. 10. 15. · Strange Baryon Production at RHIC Hui Long Department of Physics University of California, Los Angeles 1. Introduction 2. Strangeness

Summary (II)

Nuclear Effects

-Suppression of charged hadron at pt<12 GeV/c ;

-Rcp dependent on particle type at pt< 5 GeV/c;

<- flow ( 0- 2 GeV/c) ?

<- Coalescence (2- 4 GeV/c) ? ( partonic matter ?)

<- fragmentation ( > 5 GeV/c) ?

Multi-strange v2 and Rcp measurement in AA and dA coming soon !!!