light-front dynamic application to the rhic physics
DESCRIPTION
Light-Front Dynamic Application to the RHIC Physics. Korea University, June 16, 2007. In collaboration with Prof. Byungsik Hong. Motivation. QGP is thought to have existed ten millionths of second after the Big Bang ; creating the primordial matter of universe in the laboratory. - PowerPoint PPT PresentationTRANSCRIPT
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Light-Front Dynamic Application to the RHIC Physics
Korea University, June 16, 2007In collaboration with Prof. Byungsik Hong
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Motivation• QGP is thought to have existed ten millionths of second after the Big Bang; creating the primordial matter of universe in the laboratory.
• RHIC obtained distinguished results from CERN SPS._ Jet Quenching and Bulk Hadronization (BARYONS07)• LHC ALICE (CMS, ATLAS) would need theoretical predictions at energy 30-fold energy increase from RHIC.
• LFD has progressed last several years._ Trecherous points exist and correct use is required.
Time to investigate the application and make a progress….
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Outline• Brief Overview on State Changes
Chemical and Thermal Freeze-outs
• Hadronization Mechanisms
Quark Recombination and Fragmentation
• Numerical Results
Wavefunction Dependence on PT Spectra,
Ratio between proton and antiproton, etc...
• Elliptic Flow
Preliminary V2 calculation
• Conclusion
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Nuclear Phase DiagramT(MeV)
Density(n0)
~150
~10
Early Universe(RHIC)
Color SuperconductorNeutron Star
Hadron Gas
Quark-Gluon Plasma
Phase Transition
Atomic NucleiSIS explores high baryon density hadronic matter.
RHIC & future LHC explore high temperature & low baryon density partonic matter.
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Heavy-Ion Accelerators
Acceleratorc.m. Energy
(GeV)Status
SIS 18
(GSI, Germany)
2A
(A=mass number)Running
AGS
(BNL, USA)5A Finished
SIS 300
(GSI, Germany)8A Plan to run from ~2014
SPS
(CERN, Switzerland)20A Finish soon
RHIC
(BNL, USA)200A Running
LHC
(CERN, Switzerland)5500A Plan to run from ~2007
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Relativistic Heavy Ion Collider
Brookhaven National Lab.Brookhaven National Lab. in New Yorkin New York
Circumference: 3.83 km First collision: 2000 100A GeV Au+Au(2X1026/cm2/s) 250 GeV p + p (2X1032/cm2/s)
PHENIPHENIXX STARSTAR
PHOBOPHOBOSS
BRAHMBRAHMSS
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QuickTime™ and aYUV420 codec decompressor
are needed to see this picture.
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• Expansion and Cooling
- T → TC• Hadronization from QGP- Intermediate PT (2-5 GeV) Recombination• Chemical Equilibrium and Freeze-out (TC ≈ 175 MeV)
- Inelastic Channels (e.g. Δ↔pπ)- Number of each hadron species doesn’t change
• Thermal Equilibrium - Elastic Scatterings Dominant- Interaction still exists (MFP > DBP)
• Continued Expansion and Thermal Freeze-out- Particle distance gets larger (DBP > MFP)- No further elastic collisions but still heavy particles can decay into light particles (e.g. Δ→Ρπ): Tfreeze-out≈120 MeV
• Formation of QGP
- T T≫ C ≈ 175 MeV
• Heavy Ion Collision- Hard Scattering and High PT Fragmentation
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Hadronization MechanismsR.J. Fries, nucl-th/0403036, PRC 68, 044902 (2003)
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Recombination of a Quark-Antiquark Pair
><=∑∫ PMPMPd
N abab
M ;|ˆ|;)2( 3
3
ρπ
FormalismFunction in Wigner ),()(
where
),)1(;(|),(|),;()2()2(
)(
)2
;()()2
;()2()2(
)(
3
23
2
3
3
3
3
3
3
3
∫
∫ ∫
∫ ∫
Φ=Φ
−−⋅
=
+Φ−⋅
=
⊥+
⊥⊥+
Σ
⊥+
Σ
qrrdq
kPxRwkxkxPRwkdPdxRuPRd
C
qP
RwqqP
RwqdRuPRd
CPd
dNE
WM
WM
bMaM
bWMaM
M
ψππ
ππ
)(),(
),();(
0
2//)( 22
ρρφρφργ η
−Θ≈= Δ−⋅−
ffeepRw TRvp
aa
R.Fries,B.Muller,C.Nonaka and S.Bass, PRC68, 044902(2003); PRL90, 202303(2003)
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Extended Recombination Formalism
{ } ⎥⎦
⎤⎢⎣
⎡⎥⎦⎤
⎢⎣⎡ −−++++=
⎥⎦
⎤⎢⎣
⎡=
⊥⊥⊥
⊥⊥
∞
⊥
=∫ ∫
22221
21
0 0
203
0
2
)1()(cosh
),,(
where
),,(),(sinh
2)2(
kPxmkxPmT
KPkxk
PkxkkxkddxT
PI
VMC
dyPd
dN
TbTaT
TM
TMTT
baTM
yT
M
η
ψη
γγπ
nbaPower
baGauss
x
km
x
kmkx
x
km
x
kmkx
)1
/(1),(
]/)1
([Exp),(
22222
22222
αψ
βψ
+−+
++
=
−+
++
−=
⊥⊥⊥
⊥⊥⊥
B.Hong, C.Ji, D.-P.Min, PRC73, 054901 (2006)
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Light-Front Wavefunctions
ψK
x
k⊥
ψD
x
k⊥
ψπ
x
k⊥
β2 (GeV2) = 0.026 0.26 2.6
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Gaussian vs. Power Law)2,5.0( 2 == nPower αψ π
)825.0( 2 =βψ πGauss
)1,825.0( 2 == nPower αψ π
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Ref.8: R.Fries,B.Muller,C.Nonaka,S.Bass,PRC68,044902(2003)
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Fragmentation and Jet Quenching
κ)/1(
)(
0
2
1
0 323
Bp
CK
dypd
dN
pd
dNEzD
z
dz
Pd
dNE
TyT
perta
a a
aaha
h
+=
=
=
→∑∫ - Parameters of the parton distribution function
D.K. Srivastava, et al., PRC 67, 034903 (2003)
- Parameters of the Fragmentation function
B.A. Kniel, et al., NPB 582, 514 (2000)D. De Florian, et al., PRD 57, 5811 (1998)
ATTT R
Lpbpbp
><=Δ )(),( ε
R. Baier, et al., JHEP 0109, 033 (2001)B. Mueller, PRC 67, 061901 (2003)
Striking results from STAR:BARYONS07
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Single Spectra of Mesons
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Single Spectra of Baryons
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Comparison of Particle Ratios
--- R.Fries,B.Muller,C.Nonaka,S.Bass,PRC68,044902(2003) B.Hong,C.Ji,D.-P.Min,PRC74,054901(2006)
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Enhanced sea quark contribution to the fragmentation of p and pbar.
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Enhanced sea quark contribution to the fragmentation of p.
We do not expect for the recombination model to work for peripheral collisions.
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Enhanced sea quark contribution to the fragmentation of pbar.
We do not expect for the recombination model to work for peripheral collisions.
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Particle Ratios Data for central Au+Au collisions at √sNN
= 200 GeV
Open Squares: PHENIX Data-Phys. Rev. C 69, 034909 (2004)
Solid Circles: STAR Data-Phys. Rev. Lett. 97, 152301 (2006)
Solid Lines: Predictions by the present recombination model by using the fragmentation function determined by the
pp collisions data
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Anisotropy Parameter v2 Elliptic flow = v2 = 2nd Fourier coefficient of momentum anisotropy
dn/d ~ 1 + 2 v2(pT) cos (2) + …Initial spatial anisotropy is converted into momentum anisotropy. Efficiency of the conversion depends on the properties of the medium
x
yz
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Elliptic Flow Calculation
€
v2M (PT ) =
dx∫ d2k⊥ |ψ(x,k⊥ ) |2 {v2
a(xPT + k⊥ ) +v2b[(1−x)PT −k⊥]}kM (x,k⊥ ,PT )
dx∫ d2k⊥ |ψ(x,k⊥ ) |2 {1+ 2v2
a(xPT + k⊥ )v2b[(1−x)PT −k⊥ ]}kM (x,k⊥ ,PT )
NR⏐ → ⏐ v2
a(12
PT ) +v2b(12
PT )
1+ 2v2a(12
PT )v2b(12
PT )
€
v2a( pT ) = (cos2φ) =
dφ (cos2φ) I2[ pT sinhηT (φ)∫ /T]K1[mT coshηT (φ) /T]dφ I0[ pT sinhηT (φ)∫ /T]K1[mT coshηT (φ) /T]
€
ηT (φ) =ηT0 [1− f ( pT ) (cos2φ)] ; f ( pT ) =
α n
1+ ( pT / p0 )m; α =
w(b)−l(b)w(b) + l(b)
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Anisotropy Parameter v2
Au+Au at √sNN = 200 GeV
Data- Open Symbols for negatives- Solid Symbols for positives
Recombination model-No fragmentation-Dashed lines: α=0.50-Solid lines: α=0.42-Dotted lines: α=0.35
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Anisotropy Parameter v2
Au+Au at √sNN = 200 GeV
Data- Open Symbols for negatives- Solid Symbols for positives
Recombination model-Explicit model calculation for protons by the recombination for pT>4 GeV/c is still underway.-For preliminary result here, we assumed the simple quark number scaling for now. -Including the fragmentation part-Dashed lines: Recombination-Dotted lines: Fragmentation-Solid lines: Sum
preliminary
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Conclusions and Outlook• Extended the formulation of recombination model
– Intrinsic Transverse Momentum Effect– Light-Front Wavefunction
• Gaussian vs. Power Law
• Found the sensitivity of wavefunction dependence– Recombination favored by the larger size hadrons
• New results on yield ratios of K-/K+ and pbar/p– Jet Quenching Effect included
• Elliptic flow Extension possible and preliminary results obtained• Maybe useful for the analysis of other QGP nature
– Possible Formation of the Binary Systems– Crossover between BCS and BEC
• Feshbach Resonances – Heavy Hadron Production
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Food for Thoughts:Binary Bound States in QGP
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Effective
Mass
Pressure
T/Tc
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Bose-Einstein Condensation
Hydrodynamical Expansion of Trapped Atoms
Analogous to Elliptic Flows in RHIC Data
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Crossover between BCS and BEC
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Controlling Parameters
• High Tc Superconductors: Doping Holes• Ultracold Trapped Atoms: Applying Magnetic Fields • RHIC:
Changing sNN and Projectiles, etc.