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Search for a new state of matter – the Quark-Gluon Plasma

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Recent Results from RHIC

Huan Zhong Huang

黄焕中

Department of Physics and Astronomy

University of California Los Angeles



Department of Engineering Physics

Tsinghua University



Jan 9, 2008 @IHEP

1

Outline



• Formation of Dense Partonic Matter

• High pT and Heavy Quark Measurements

• Hadronization of Bulk Partonic Matter

• Searches for Exotic Particles and

Phenomenon

• Outlook





2

Au + Au Collisions at RHIC







Central Event









3

STAR (real-time Level 3)

Nucleus-Nucleus Collisions and Volcanic Eruption









Volcanic high pT -- Strombolian eruption Volcanic mediate pT – Spatter (clumps)









4

Volcanic low pT – Bulk matter flows

Hard Scattering and Jet Quenching



leading particle suppressed









back-to-back jets disappear





Hard Scattering in p+p Parton Energy Loss in A+A





Reduction of high pT particles

Disappearance of back-to-back high pT particle correlations

5

High pT Phenomena at RHIC

Very dense matter has been created

in central Au+Au collisions!



This dense matter is responsible for the

disappearance of back-to-back correlation

and the suppression of high pT particles !



Is the energy loss due to parton or hadron stage?

Is there a noticeable difference in experimental

phenomenon related to quarks versus gluons?

What is the flavor dependence of energy loss?

6

The Suppression is the Same for p0

and h – parton level effect









No suppression for direct photons – photons do not participant !

7

No Significant Difference Between

Quarks and Gluons at High pT









Baryons more likely from gluon fragmentations in the pQCD region

8

No Significant Difference Between

Heavy Quark Meson and Light Quark Mesons



Non-photonic electrons Charged hadrons

from heavy quark decays



STAR









9

Heavy quark energy loss: Early Expectations

Heavy quark has less dE/dx due Y. Dokshitzer & D. Kharzeev PLB 519(2001)199



to suppression of small angle dP 

 s C F d 2 2

k  dk 



dP0

gluon radiation p  (k    0 )

2 2 2 2

(1   0 /  2 ) 2

2





M k

“Dead Cone” effect 0 

E

,  









M. Djordjevic, et. al. PRL 94(2005)112301

J. Adams et. al, PRL 91(2003)072304









Radiative energy loss of heavy

quarks and light quarks

--- Probe the medium property !







What went wrong?10

Radiative Energy Loss not Enough

Moore & Teaney, PRC 71, 064904 (2005)









Large collisional (not radiative) interactions also

11

produce large suppression and v2

Does Charm Quark Flow Too ?









Reduce Experimental Uncertainties !!

Suppression in RAA  Non-zero azimuthal anisotropy 122 !

v

B and D contributions to electrons



Experimental

measurement of

B and D

contributions to

non-photonic

electrons !



Direct measurement

of D and B mesons









13

B and D contributions compatible







Bottom quarks

may suffer

considerable

energy loss

in the dense

partonic medium

too !



14

STAR preliminary data motivated sonic-boom prediction

pTtrig=4-6 GeV/c, pTassoc=0.15-4 GeV/c Casalderrey-Solana, Shuryak, Teaney,

hep-ph/0411315









Actually sonic-boom was first predicted

in the 70’s by the Frankfurt school.



Many recent studies:

H. Stoecker, nucl-th/0406018.

Muller, Ruppert, nucl-th/0507043.

F. Wang (STAR), QM’04 talk, nucl-ex/0404010.

Chaudhuri, Heinz, nucl-th/0503028.

Now published: STAR, PRL 95, 152301 (2005).

Y.G. Ma, et al. nucl-th/0601012. 15

Does Heavy Quark Energy Loss

Generate Mach Cone Emission?

Trigger on non-photonic electrons from

heavy quark decays --



AWAY

AWAY

SIDE

SIDE

NEAR

SIDE









Preliminary STAR data show a broadening peak at the away side !

16

High pT Phenomena at RHIC

Very dense matter has been created

in central Au+Au collisions!



This dense matter is responsible for the

disappearance of back-to-back correlation

and the suppression of high pT particles !



The mechanism for parton energy loss is yet to

be understood !



The nature for the broad peak on the away-side

requires more studies !

17

Intermediate pT Region









Volcanic mediate pT – Spatter (clumps)





At RHIC intriguing experimental features:

multi-quark clustering

 enhanced baryon over meson production

strangeness equilibration

 increased multi-strange hypeons 18

Elliptic Flow Parameter v2

coordinate-space-anisotropy  momentum-space-anisotropy



y







x









Initial/final conditions, dof, EOS



dN 1 dN  

 1   2v icos(i(  ψR ))

p t dp t dyd 2π p t dp t dy  i1  19

Constituent Quark Scaling



STAR

Baryon







Meson





PHENIX









Constituent (n) Quark Scaling

-- Meson n=2 and Baryon n=3 grouping

Saturation of v2 at Intermediate pT

20

Constituent Quark Degree of Freedom









Hadronization Scheme for

Bulk Partonic Matter:

KS – two quark coalescence

– three quark coalescence

from the partonic matter surface?!



Particle v2 may be related to

quark matter anisotropy !!



pT nK 

a feature not present in single

parton fragmentation !





Multi-parton dynamics:

coalescence,

recombination and

gluon junctions.



39

Particle Dependence of v2



STAR

Baryon



Meson





PHENIX









Why saturation at intermediate pT ?

Why baryon and meson difference ? 40

Spin Physics Program

The Spin Structure of the Proton:



½ = ½ SDq + DG +



q  up, down and strange quarks

G  gluons

L  angular momentum of quarks and gluons



Experimentally:

1) total spin in quarks ~ 30%

2) sea quarks are polarized too

3) little info about the gluon polarization

4) even less know about and how to measure

41



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