f.s.n. and d.a. fogaça
DESCRIPTION
Gluon condensates and the equation of state of cold quark gluon plasmas. F.S.N. and D.A. Fogaça. IFUSP / BRAZIL. arXiv:1012.5266. Introduction. QCD phase diagram. Hot QGP. Cold QGP. Hot QGP. Ideal gas of weakly interacting quarks and gluons. (perturbative QCD). - PowerPoint PPT PresentationTRANSCRIPT
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F.S.N. and D.A. Fogaça
IFUSP / BRAZIL
Gluon condensates and the equation of state of cold quark gluon plasmas
arXiv:1012.5266
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Introduction
QCD phase diagram
Hot QGP
Cold QGP
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Ideal gas of weakly interacting quarks and gluons
Equation of state from the MIT bag model
(perturbative QCD)
Hot QGP
Lattice QCD: significant non-perturbative effects
RHIC: strongly interacting fluid
Non vanishing gluon condensate above deconfinement
David Miller, Phys. Rep. (2007) hep-ph/0608234
Borsanyi et al.,arXiv:1011.4229
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Equation of state MIT bag model
quarks vacuum
BBB
3/43/2
3/7
2
3)(
Bp BB
3/43/2
3/7
2
3
3
1)(
Cold QGP
MIT Bag
“Big Bag”
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Derive a simple EOS for the cold QGP
Assume that gluon condensates survive in cold QGP
Naively: they go asymptotically to zero ...
Non-trivial behavior: Metlitski, Zhitnitsky, Nucl. Phys. B (2005)
Estimate the effects of the gluon condensates A2 and A4
Our goal
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QGP at large densities and zero temperature :
Separation of the gluon fields in soft and hard modes:
aaa AG
a mean field approximation
(“Walecka”)
Hard gluons are generated by intense quark sources
They have large ocupation numbers and become classical
aa00
aA
aa AA
Soft gluons generate the condensates in the plasma
0 aA
0 cba AAA
baba AAAA
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Infinite matter: soft and hard fields are uniform !
0 aA 00 a
Soft gluons
Hard gluons
Quarks
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The effective Lagrangian :
)()()()( 00000000
2
eeddccbbedacbaaa AAAAffgFF
cbcbaaaa GGfgGGF
jjiaa
jijiiaa
QCD mGTgiFFL
)(4
1
cbcbaa GGfgF Uniform fields:
aaa AG Field decomposition :
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002 edcbedacba AAAffg
edcbedacba AAAAffg 2
000000
2 edcbedacba Affg
edcbedacba AAAffg 002
edcbedacba AAAffg 00
2 edcbedacba AAAffg 00
2
00002 edcbedacba AAffg 00
002
edcbedacba AAffg
edcbedacba AAffg 0000
2 0000
2 edcbedacba AAffg
edcbedacba AAffg 00
002
edcbedacba AAffg 00002
000000
2 edcbedacba Affg
000000
2 edcbedacba Affg
edcbedacba Affg 000000
2
00000000
2 edcbedacba ffg
A^4
A^3
A^2
A^1
A^0
mass term for the hard gluons
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Expectation values of the soft gluons in the “vacuum” :
dynamical gluon mass
2220
2 AAAgg aa
dimension 2 gluon condensate is a parameter !
22
2
2
240
40
2
)34(4
9F
gFF
gbg aas
dimension 4 gluon condensate is a parameter !
20
22
32
9 gmG
2032
1 gAA baba
0 cba AAA 0 aA
dbcadcbadcba ggggAAAA
[
)34)(32(
40
]cbdagg
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jjiaa
jijiiaaG
QCD mTgim
bL )(
2 000
0
240
soft gluons
hard gluons
quarks + hard gluons
Equations of motion
0)( 00 jji
aajiji mTgi
aaG gm 02
jajii
a T 0
Energy - momentum tensor
hard couplingg is a parameter !
The effective Lagrangian
00T
iiTp3
1LgL
T ii
)()(
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3/4
FkQ
G
mkkkdm
gb
0
2222
22
240 2
3
2
27)(
FkQ
G mk
kkd
m
gbp
022
4
22
2
240 22
27)(
326 F
Q k
MIT BagModel
From B we can infer thevalue of the condensate in the QGP !
3/43/23/7
2
3)(
B
3/43/23/7
2
3
3
1)(
Bp
The equation of state
When the two EOS coincide0g
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Parameters
20 % of the vacuum value
224 AAA20
20
15 % of the vacuum value
GeVm 02.0
3.0s
01.0s
43 )200(/200 MeVfmMeVB
240 444
1FFFFFbB
s
aas
s
aa
42 0006.0 GeVF
22 3.0 GeVA
MeVmG 290
quark mass :
hard coupling :
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Numerical results
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Pressure and sound velocity
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Pressure versus energy density
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F. Samarruca, arXiV:1009.1172 [nucl-th]
Comparison with the MIT bag model
200B
100B
0s
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Comparison with the MIT bag model
More pressure
More energy
Harder EOS
Hard gluons!
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Comparison with the MIT bag model
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Conclusion
Simple approach to dense and cold QGP
Weak gluon condensates in QGPBag constant
Massive gluons
Gluon field decomposition = soft + hard
Mean field approximation
Richer version of the MIT bag model with classical hard gluons
Condensates make the EOS softer
2F
2A
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Back ups
][)34)(32(
40 cbdadbcadcbadcba ggggggAAAA
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BV
V
m
gV 2
202
Compute the Lagrangian, energy-momentum tensor and obtain the EOS :
But we can estimate the Laplacian :
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Gluon condensate in a hot QGP :
Gluon condensate in dense and cold QGP ?
David Miller, Phys. Rep. (2007) hep-ph/0608234
Naively: goes asymptotically to zero !
Non-trivial behavior: Metlitski, Zhitnitsky, Nucl. Phys. B (2005)
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Introduction
RHIC (2003) : evidence of the strongly interacting QGP (sQGP)
How to include non-perturbative effects in the equation of state ?
Finite temperature: lattice QCD
Finite density: models !
Our model: effects of the gluon condensates in the QGP !
non-perturbative effects !
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Borsanyi et al.,arXiv:10114229
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The equation of state
MIT BagModel
3/4
From B we can infer thevalue of the condensate in the QGP !
BBB
3/43/2
3/7
2
3)(
Bp BB
3/43/2
3/7
2
3
3
1)(
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Finite temperature:
Finite density ?
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É difícil acreditar...