1 evidence for multi-parton dynamics in hadronization of bulk partonic matter at rhic huan zhong...
TRANSCRIPT
1
Evidence for Multi-parton Dynamics in Hadronization of Bulk Partonic Matter at RHIC
Huan Zhong Huang (黄焕中 )Department of Physics and Astronomy
University of California Los Angeles
Department of Engineering PhysicsTsinghua University
7th Annual Conference of Chinese High Energy Physics Society
2
Outline
• Relativistic Heavy Ion Collider (RHIC) and Quark-Gluon Plasma (QGP)
• Fragmentation Scheme • Hadronization of Bulk Partonic Matter• Recent Results of High pT Probes• Outlook
3
STAR
Relativistic Heavy Ion Collider --- RHIC
Au+Au 200 GeV N-N CM energyPolarized p+p up to 500 GeV CM energy
4
Quark-Hadron Phase Transition
5
Au + Au Collisions at RHIC
STARSTAR
Central Event
(real-time Level 3)
6
Nucleus-Nucleus Collisions and Volcanic Eruption
Volcanic high pT -- Strombolian eruption Volcanic mediate pT – Spatter (clumps)
Volcanic low pT – Bulk matter flows
7
The The Field & FeynmanField & Feynman picture of cascade fragmentation picture of cascade fragmentation
Kretzer@ISMD04
8
Baryon Production from pQCD
K Kp p
e+e-jet fragmentation from SLD
Normal Fragmentation Cannot Produce the Large Baryon Yield
9
Too Many Baryons at Intermediate pT
10
Elliptic Flow Parameter v2
y
x
py
px
coordinate-space-anisotropy momentum-space-anisotropy
Initial/final conditions, dof, EOS
1i
Ritttt
))ψcos(i(2v1dydpp
dN
2π
1
dyddpp
dN
11
Elliptic Flow: ultra-cold Fermi-GasElliptic Flow: ultra-cold Fermi-Gas
• Li-atoms released from an optical trap exhibit elliptic flow analogous to what is observed in ultra-relativistic heavy-ion collisions
Elliptic flow is a general feature of strongly interacting systems!
12
Hydro calculations break-down at higher pT (as expected).
How is v2 established at pT above 2 GeV/c?
Why is baryon v2 larger than meson v2?
PRL 92 (2004) 052302; PRL 91 (2003) 182301
Elliptic Flow v2
13
Constituent Quark Degree of Freedom
KS – two quark coalescence– three quark coalescence from the partonic matter surface?!
Particle v2 may be related to quark matter anisotropy !!
pT < 1 GeV/c may be affected by hydrodynamic flow !
Hadronization Scheme for Bulk Partonic Matter:
Quark Coalescence – (ALCOR-J.Zimanyi et al, AMPT-Lin et al, Rafelski+Danos, Molnar+Voloshin …..)
Quark Recombination – (R.J. Fries et al, R. Hwa et al)
14
Constituent Quark Scaling
Constituent (n) Quark Scaling-- Meson n=2 and Baryon n=3 grouping
Some deviation due to internal hadron structure
15
Nuclear Modification Factor
ddp
Nd
collddpNd
TAA
T
pp
T
AA NpR 2
2
/)(
Peripheralcoll
T
Centralcoll
TTCP
NddpNd
NddpNd
pR]/[
]/[
)( 2
2
N-binary Scaling RAA or RCP = 1 simple superposition of independent N-N collisions !
16
Strangeness from Bulk Partonic MatterRCP
Constituent Quark Number Scaling-- Hadronization through quark clustering-- Effective DOF – constituent quarks quasi-hadrons at Tc ? Lattice QCD picture?
17
Intermediate pT Dynamics
Multi-parton dynamics – clustering of quarks – could be responsible for -- increased baryon production -- strange baryon enhancement -- strong elliptic flow at intermediate pT !!!
Hadronization of bulk partonic matter -- different phenomenon from e+e- collisions !
18
pT Scales and Physical Processes
RCPThree PT Regions:
-- Fragmentation
-- multi-parton dynamics (recombination or coalescence or …)
-- Hydrodynamics (constituent quarks ? parton dynamics from gluons to constituent quarks? )
19
Multi-Parton Dynamics for Bulk Matter Hadronization
Essential difference:Traditional fragmentation particle properties mostly determined by the leading quark !Emerging picture from RHIC data (RAA/RCP and v2) all
constituent quarks are almost equally important in determining particle properties !
v2 of hadron comes from v2 of all constituent quarks !
The fact that in order to explain the v2 of hadrons individual constituent quarks (n=2-meson,3-baryon) must have a collective elliptic flow v2 and the hadron v2 is the sum of quark v2 Strong Evidence for Deconfiement !
20
Recombination+Fragmentation ModelRecombination+Fragmentation Model
basic assumptions:
• at low pt, the quarks and antiquark spectrum is thermal and they recombine into hadrons locally “at an instant”:
features of the parton spectrum are shifted to higher pt in the hadron spectrum
• at high pt, the parton spectrum is given by a pQCD power law, partons suffer jet energy loss and hadrons are formed via fragmentation of quarks and gluons
qq M qqq B
• shape of parton spectrum determines if recombination is more effective than fragmentation• baryons are shifted to higher pt than mesons, for same quark distribution understand behavior of baryons!
21
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?
22
The Suppression is the Same for and – parton level effect
No suppression for direct photons – photons do not participant !
23
No Significant Difference BetweenQuarks and Gluons at High pT
Baryons more likely from gluon fragmentations in the pQCD region
24
STARSTAR
No Significant Difference BetweenHeavy Quark Meson and Light Quark Mesons
Non-photonic electrons from heavy quark decays
Charged hadrons
25
Heavy quark energy loss: Early Expectations
k
E
M
dP
k
dkkdCdP Fs
,
)/1()(
0
2220
022
022
22
Y. Dokshitzer & D. Kharzeev PLB 519(2001)199
Radiative energy loss of heavy quarks and light quarks
--- Probe the medium property !
Heavy quark has less dE/dx due to suppression of small angle gluon radiation
“Dead Cone” effect
M. Djordjevic, et. al. PRL 94(2005)112301
J. Adams et. al, PRL 91(2003)072304
What went wrong?
26
B and D contributions to electrons
Experimental measurement of B and D contributions to non-photonic electrons !
Direct measurement of D and B mesons
27
Poor (Wo)Man’s Approach to Measure B/D Contributions to Electrons – e-h correlations
B
D
PYTHIA Simulations of e-h correlations from p+p
X. Lin hep-ph/0602067
28
STAR preliminary data motivated sonic-boom prediction
F. Wang (STAR), QM’04 talk, nucl-ex/0404010.Now published: STAR, PRL 95, 152301 (2005).
pTtrig=4-6 GeV/c, pT
assoc=0.15-4 GeV/c
Many recent studies:H. Stoecker, nucl-th/0406018.Muller, Ruppert, nucl-th/0507043.Chaudhuri, Heinz, nucl-th/0503028.Y.G. Ma, et al. nucl-th/0601012.
Casalderrey-Solana, Shuryak, Teaney, hep-ph/0411315
Actually sonic-boom was first predicted in the 70’s by the Frankfurt school.
29
High pT Phenomena at RHICVery 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 (Mach cone or not) !
30
Discoveries from Unexpected Areas?!
RHIC -- Frontier for bulk partonic matter formation (quark clustering and rapid hadronization) -- Factory for exotic particles/phenomena
Potential exotic particles/phenomena:penta-quark states (uudds, uudds!)
di-baryonsH – (, uuddss) [] (ssssss)
strange quark matter
meta-stable Parity/CP odd vacuum bubblesdisoriented chiral condensate……
31
STAR – Exciting Physics Program A full TOF upgrade will greatly enhance STAR’s capability !!
RHIC – Exotic Particle Factory
Full Barrel TOF Using MRPC
Chinese STAR Group SINAP Tsinghua University USTC CCNU, Wuhan IMP, Lan Zhou IHEP
Construction to be finished by 2008Full installation in 2009
32
RHIC Physics Outlook
Heavy Ion Physics: 1) Properties of high density QCD matter 2) Chiral symmetry at high temperature and density 3) Search for exotic particles/phenomena at RHIC 4) Search for critical point (low energy scan)
RHIC Spin Physics Using Polarized p+p Collisions: 1) the gluon spin structure function major milestone to understand the spin of the proton! 2) sea quark spin structure function 3) quark transverse spin distribution
33
End of Talk
34
Experimental Statistical and Systematic Errors
c-cbar production CS PHENIX0.92+-0.15+-0.54 mb0.567+-0.057+-0.224 mb
STAR1.4+-0.2+-0.4 mb
Errors taken seriously
High pT region does not contribute to total CS much. Difference between STAR and PHENIX has to be resolved !!
35
B does not seem dominant at pT 4.5 GeV/c
Preliminary STAR Data
Xiaoyan Lin – STAR presentation at Hard Probe 2006
36
Intriguing Situation Regarding Pentaquark States
pK+ and pK- from 18.4 M d+Au at 200 GeVBackground – Combinatorial and Correlated Pairs
Statistical significance ~ 4Intriguing ! Not conclusive yet !Another long d+Au run will resolve this uncertainty !
M (GeV/c2) M (GeV/c2)
37
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
38
Radiative Energy Loss not EnoughMoore & Teaney, PRC 71, 064904 (2005)
Large collisional (not radiative) interactions also produce large suppression and v2
39
Charm Quark in Dynamical Model (AMPT)
Large scattering cross sections needed !
40
Nuclear Modification Factor RAA RCP
Multi-parton dynamics predict baryon yield increases with centrality FASTER than mesons! Yield ~ n and n>nK a feature not present in single parton fragmentation !
Multi-parton dynamics: coalescence, recombination and gluon junctions.
RCP
RCP=[yield/N-N]central
[yield/N-N]peripheral
41
STAR
PHENIX
Particle Dependence of v2
Baryon
Meson
Why saturation at intermediate pT ?Why baryon and meson difference ?
42
Spin Physics Program
The Spin Structure of the Proton:
½ = ½ q + G + <L>
q up, down and strange quarksG gluonsL 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 <L> and how to measure <L>