qcd phase transitions and green’s functionspawlowsk/delta10/talks/...hoehler et al., npb...
TRANSCRIPT
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7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal | 1
QCD Phase Transitions and Green’s Functions
Heidelberg, 7 May 2010
Lorenz von Smekal
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7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
European Commission
2
Special Credit and Thanks to:
ExtreMe Matter InstituteHelmholtz Alliance 'Cosmic Matter in the Laboratory'
Reinhard AlkoferJens BraunChristian FischerHolger GiesLisa Haas Axel MaasKim MaltmanFlorian MarhauserJens MüllerJan PawlowskiBernd-Jochen SchaeferDaniel SpielmannNucu StamatescuAndre SternbeckJochen Wambach
Helmholtz Young Investigator Group 'Nonperturbative Phenomena in QCD'
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7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Contents
• Introduction: why Green’s functions?
• Functional methods
• What do we know?(zero temperature and density)
• Applications to QCD phase transitions(deconfinement and chiral symmetry restoration)
• Summary and Outlook: what may we expect?
2
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• quantum field theoretic building blocks for hadron phenomenologyhadron masses, decay constants, form factors, magnetic moments, charge radii etc.from covariant bound state equations (Bethe-Salpeter and Faddeev)
covariant Faddeev equation for baryons
need QCD quark and gluonGreen’s functions as input
−→ G. Eichmann, PhD Thesis, Graz (2009)[arXiv:0909.0703 [hep-ph]]
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Introduction
Why QCD Green’s Functions?
0.0 0.5 1.0 1.5 2.0Q2 [GeV2]
0.0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1.0
1.1
1.2
GE
Proton Electric Form Factormq=0.43 GeV, msc=0.60 GeV, max=0.83 GeV
Hoehler et al., NPB 114(1976), 505Bosted et al., PRL 68(1992), 3841All contributions2 loop contributions
0 0.5 1 1.5 2 2.5 3 3.5Q2 [GeV2]
0
0.5
1
1.5
2
µpG
E/GM
The Ratio µpGE/GM
JLab Hall A Coll, PRL 84 (2000), 1398mq=0.36, msc=0.63, max=0.68mq=0.43, msc=0.60, max=0.83
Oettel, Pichowsky, LvS, EPJA 8 (2000) 251Oettel, Alkofer, LvS, EPJA 8 (2000) 553
3
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• confinement, dynamical mass generation, chiral symmetry breakingand Goldstone’s theorem
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Introduction
Why QCD Green’s Functions?
Alkofer & LvS, Phys. Rept. 353/5-6 (2001) 281Fischer, J. Phys. G 32 (2006) 253Massen der Quarks: Numerische Lösung der DSE
10-2 10-1 100 101 102 103
p2 [GeV2]
10-4
10-3
10-2
10-1
100
101
Qua
rk M
ass F
unct
ion:
M(p
2 )
Bottom quarkCharm quarkStrange quarkUp/Down quarkChiral limit
M(p2): impulsabhängig!
Dynamische MasseMstark (0) ! 400MeV
Flavour-Abhängigkeitwegen Mschwach
C. F. and R. Alkofer, Phys. Rev. D 67 (2003)
Christian S. Fischer (TU Darmstadt) Landau gauge QCD 16. März 2007 27 / 39
Fischer, Alkofer, PRD 67 (2003) 094020
Pionen und Rho-Mesonen II
0 200 400 600 800 1000 1200M
! [MeV]
600
800
1000
1200
1400
1600
M" [
MeV
]
Nf=3, DSENf=2, JLQCD(2003)Nf=2, CP-Pacs (2002/4)
C. F., P. Watson and W. Cassing, Phys. Rev. D 72 (2005) 094025
Christian S. Fischer (TU Darmstadt) Landau gauge QCD 16. März 2007 38 / 39
Fischer, Watson, Cassing, PRD 72 (2005) 094025
4
TOPCITE 500+
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• confinement, dynamical mass generation, chiral symmetry breakingand Goldstone’s theorem
• chiral symmetry restoration and deconfinement transition . . .
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Introduction
Why QCD Green’s Functions?
Alkofer & LvS, Phys. Rept. 353/5-6 (2001) 281Fischer, J. Phys. G 32 (2006) 253
Here:
Massen der Quarks: Numerische Lösung der DSE
10-2 10-1 100 101 102 103
p2 [GeV2]
10-4
10-3
10-2
10-1
100
101
Qua
rk M
ass F
unct
ion:
M(p
2 )
Bottom quarkCharm quarkStrange quarkUp/Down quarkChiral limit
M(p2): impulsabhängig!
Dynamische MasseMstark (0) ! 400MeV
Flavour-Abhängigkeitwegen Mschwach
C. F. and R. Alkofer, Phys. Rev. D 67 (2003)
Christian S. Fischer (TU Darmstadt) Landau gauge QCD 16. März 2007 27 / 39
Fischer, Alkofer, PRD 67 (2003) 094020
Pionen und Rho-Mesonen II
0 200 400 600 800 1000 1200M
! [MeV]
600
800
1000
1200
1400
1600
M" [
MeV
]
Nf=3, DSENf=2, JLQCD(2003)Nf=2, CP-Pacs (2002/4)
C. F., P. Watson and W. Cassing, Phys. Rev. D 72 (2005) 094025
Christian S. Fischer (TU Darmstadt) Landau gauge QCD 16. März 2007 38 / 39
Fischer, Watson, Cassing, PRD 72 (2005) 094025
4
TOPCITE 500+
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Z(T, V, µ) =�D[A, c,ψ] δ(∂A) exp
�−
� 1/T
0dt
�
Vd3x
�14F 2 + c̄ ∂Dc + ψ̄(−D/ + m−µγ0)ψ
��
Lorenz condition, ∂µAµ = 0
c̄, c � Det(−∂µDµ(A))
Fµν = ∂µAν − ∂νAµ + ig[Aµ, Aν ]
ψ(1/T, �x) = −ψ(0, �x)
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Generalities - Partition Function
Landau gauge:
Faddeev-Popov ghosts and determinant:
Field strengths:Quark fields with a.p. b.c.’s:
5
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∂A = 0 for A = Atr, many copies!
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Note on Gribov Copies
A
A
Al
tr
tr
• Gribov, Singer (1978):
• Fujikawa, Hirschfeld (1979):
• Sharpe (1984), Neuberger (1987), Schaden (1998):
• LvS (2008):
gauge copies unavoidable.
average over copies (sign-weighted).
perfect cancellation, produces 0!
can be avoided → non-perturbative Becchi-Rouet-Stora-Tyutin (BRST) symmetry (on the lattice, but with sign problem).
6
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7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Non-Perturbative Tools
• Functional Methods:(a) Dyson-Schwinger Equations (DSEs)
Partition Function ➞ Generating Functional ➞ Equations of Motion for Green’s Functions
(b) Functional Renormalisation Group (FRG)Effective Action ➞ Energy-Momentum Cutoff➞ RG Flow ➞ Wetterich Equation
• Lattice Gauge Theory
+ chiral fermions+ no sign problem+ dynamical hadronisation
+ no truncations+ manifest gauge invariance
7
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7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Non-Perturbative Tools
• Functional Methods:(a) Dyson-Schwinger Equations (DSEs)
Partition Function ➞ Generating Functional ➞ Equations of Motion for Green’s Functions
(b) Functional Renormalisation Group (FRG)Effective Action ➞ Energy-Momentum Cutoff➞ RG Flow ➞ Wetterich Equation
• Lattice Gauge Theory
+ chiral fermions+ no sign problem+ dynamical hadronisation
+ no truncations+ manifest gauge invariance
— combine & compare —
7
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Dgluon ∝σ
p4, V (�r) ∝ σr
p2 [(GeV)2]
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Historical Note
)(rV
r
0 1 2 3 4
x = k2
/!
0
5Gluon
Ghost
Historically: infrared enhanced gluon exchange,
but no – it’s ghosts that dominate the long-range/infrared correlations!LvS, Hauck, Alkofer (1997)
)(rV
r
0 1 2 3 4
x = k2
/!
0
5Gluon
Ghost
2 conditions for confinement:Kugo, Ojima (1979)
(a) avoid Higgs mechanism
(b) mass gap
all physical states are color singlets.
8
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Dgluon ∝σ
p4, V (�r) ∝ σr
p2 [(GeV)2]
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Historical Note
)(rV
r
0 1 2 3 4
x = k2
/!
0
5Gluon
Ghost
Historically: infrared enhanced gluon exchange,
but no – it’s ghosts that dominate the long-range/infrared correlations!LvS, Hauck, Alkofer (1997)
)(rV
r
0 1 2 3 4
x = k2
/!
0
5Gluon
Ghost
2 conditions for confinement:Kugo, Ojima (1979)
(a) avoid Higgs mechanism
(b) mass gap
all physical states are color singlets.
F. Coester:
“Farbloser Quark zusammengeleimt von Gespenstern mit farbigem Leim”
8
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Pure Yang-Mills, T = 0
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Gluon Propagator
Z(p2)
p [GeV]
2
3
4
1
0 5 64321
!"!! #"$
%&!! #"$
!"!! '"(
'#!! '"(
%&!! '""
Sternbeck et al., PoS LAT2006, 76
�Aµ(x)Aν(y)� : Dµν(p) =Z(p2)
p2
�δµν −
pµpν
p2
�
9
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7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Gluon Propagator
2
3
4
1
0 5 64321
!"!! #"$
%&!! #"$
!"!! '"(
'#!! '"(
%&!! '""
Z(p2)
p [GeV]
Sternbeck et al., PoS LAT2006, 76
LvS, Hauck, Alkofer, Phys. Rev. Lett. 79 (1997) 3591
9
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7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Gluon Propagator
2
3
4
1
0 5 64321
!"!! #"$
%&!! #"$
!"!! '"(
'#!! '"(
%&!! '""
Z(p2)
p [GeV]
Sternbeck et al., PoS LAT2006, 76
LvS, Hauck, Alkofer, Phys. Rev. Lett. 79 (1997) 3591Lerche, LvS, Phys. Rev. D 65 (2002) 125006Fischer, Alkofer, Phys. Rev. D 65 (2002) 094008
9
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7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Gluon Propagator
2
3
4
1
0 5 64321
!"!! #"$
%&!! #"$
!"!! '"(
'#!! '"(
%&!! '""
Z(p2)
p [GeV]
Sternbeck et al., PoS LAT2006, 76
LvS, Hauck, Alkofer, Phys. Rev. Lett. 79 (1997) 3591Lerche, LvS, Phys. Rev. D 65 (2002) 125006Fischer, Alkofer, Phys. Rev. D 65 (2002) 094008Pawlowski, Litim, Nedelko, LvS, Phys. Rev. Lett. 93 (2004) 152002; Pawlowski (2006), unp.
9
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7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Gluon Propagator
2
3
4
1
0 5 64321
!"!! #"$
%&!! #"$
!"!! '"(
'#!! '"(
%&!! '""
Z(p2)
p [GeV]
Sternbeck et al., PoS LAT2006, 76
LvS, Hauck, Alkofer, Phys. Rev. Lett. 79 (1997) 3591Lerche, LvS, Phys. Rev. D 65 (2002) 125006Fischer, Alkofer, Phys. Rev. D 65 (2002) 094008Pawlowski, Litim, Nedelko, LvS, Phys. Rev. Lett. 93 (2004) 152002; Pawlowski (2006), unp.Fischer, Maas, Pawlowski, Annals Phys. 324 (2009) 2408; Pawlowski, in prep.
9
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7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Landau gauge QCD Propagators
Alkofer, Aguilar, Binosi, Bicudo, Bloch, Boucaud, Bogolubsky, Bornyakov, Bowman, Braun, Cucchieri, De Soto, Dudal, Fischer, Gies, Gracey, Huber, Ilgenfritz, Langfeld, Leinweber, Leroy, Litim, Llanes-Estrada, Nakamura, Natale, Nedelko, Maas, Mendes, Micheli, Mitrjushkin, Müller-Preußker, Oliveira, Papavassiliou,
Pawlowski, Pene, Petreczky, Quandt, Reinhardt, Rodriguez-Quintero, Schwenzer, Silva, Skullerud, Sorella, Stamatescu, Sternbeck, Vandersickel, Verschelde, LvS, Wambach, Williams, Zwanziger, ....
• Since 1997, DSEs, FRGEs, Stochastic Quantisation, Lattice Simulations:
• Numerical solutions & analytic infrared asymptotics(infrared-scaling, confinement criteria, Gribov ambiguity ...).
10
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7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Gluon Propagator
2
3
4
1
0 5 64321
!"!! #"$
%&!! #"$
!"!! '"(
'#!! '"(
%&!! '""
Z(p2)
p [GeV]
perturbativenon-perturbativeand relevant
Gribov ambiguity, offundamental interest(mass gap, Kugo-Ojima),but phenomenologicallynot relevant!
11
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7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Gluon Propagator
2
3
4
1
0 5 64321
!"!! #"$
%&!! #"$
!"!! '"(
'#!! '"(
%&!! '""
Z(p2)
p [GeV]
perturbativenon-perturbativeand relevant
Gribov ambiguity, offundamental interest(mass gap, Kugo-Ojima),but phenomenologicallynot relevant!
• Combine functional methods (FRGEs + DSEs).• Compare with lattice simulations where possible.
11
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αMMS (p2) =
g2
4πZ(p2)G2(p2)
p2 → 02.97
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Running Coupling
• From Landau gauge gluon and ghost propagators:
LvS, Hauck, Alkofer, Annals Phys. 267 (1998) 1Lerche, LvS, Phys. Rev. D 65 (2002) 125006
(infrared-scaling)
12
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αMMS (p2) =
g2
4πZ(p2)G2(p2)
p2 → 02.97
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Running Coupling
• From Landau gauge gluon and ghost propagators:
LvS, Maltman, Sternbeck, Phys. Lett. B 681 (2009) 336
LvS, Hauck, Alkofer, Annals Phys. 267 (1998) 1
• “MiniMOM” schemeprecise definition, known to 4 loops
Lerche, LvS, Phys. Rev. D 65 (2002) 125006
(infrared-scaling)
12
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αMMS (p2) =
g2
4πZ(p2)G2(p2)
p2 → 02.97
αs
not a fit!
r0Λ(0)
MS= 0.62(1), r0Λ
(2)
MS= 0.60(3)(2)
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Running Coupling
• From Landau gauge gluon and ghost propagators:
LvS, Maltman, Sternbeck, Phys. Lett. B 681 (2009) 336
LvS, Hauck, Alkofer, Annals Phys. 267 (1998) 1
• “MiniMOM” schemeprecise definition, known to 4 loops
0.05
0.10
0.15
0.20
0.25
0.30
0.35
0.40
1 10 100 1000 10000
!M
ML
(p2)
p2 [GeV2]
Nf = 0
(!, N4) = (6.0, 324)(6.2, 324)(6.4, 324)(6.6, 324)(6.9, 484)(7.2, 644)(7.5, 644)(8.5, 484)
!MMs (p2)
Lerche, LvS, Phys. Rev. D 65 (2002) 125006
(infrared-scaling)
• Lattice determination ofSternbeck et al. (LvS), PoS LAT2009, 210
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P (�x) = P exp�
ig
� 1/T
0dtA0(t, �x)
�
P (�x)→ ZP (�x) ,
Z ∈ {1, exp 2πi/3, exp 4πi/3}
→�
Φ = 0, confined, (center) symmetric, disorderedΦ �= 0, deconfined, spontan. broken Z3, ordered
Φ =13
�trP (�x)
�∼ e−Fq/T
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Applications I
Deconfinement Transition
• Pure gauge theory with static quarks:
and (global) Z3 center symmetry:
• Order parameter:
13
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Φ[a] =13�1 + 2 cos
a
2�,a =
1T
�gA30� ,
p [GeV]
p0 = 2πT (n− ν a/4π) ,
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Effective Potential
!t!k["] = 1
2
!
"
!
• Constant background:
V [a] =�
k
� �
p [GeV]
G(p2)Z(p2)
Braun, Gies, Pawlowski, Phys. Lett. B 684 (2010) 262
with:ν = {0,±1,±2}
14
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Φ[a] =13�1 + 2 cos
a
2�,a =
1T
�gA30� ,
p [GeV]
p0 = 2πT (n− ν a/4π) , O(V ��[a])(suppressed at Tc)
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Effective Potential
!t!k["] = 1
2
!
"
!
• Constant background:
V [a] =�
k
� �
p [GeV]
G(p2)Z(p2)
Braun, Gies, Pawlowski, Phys. Lett. B 684 (2010) 262
with: • Up to terms
ν = {0,±1,±2}
14
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a
2π
V [a]/T 4
Φ[a] = 0
Tc/√
σ = 0.658± 0.023
Tc = 289.5± 10 MeV ,
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Effective Potential
Braun, Gies, Pawlowski, Phys. Lett. B 684 (2010) 262
285 MeV
295 MeV
300 MeV
310 MeV
289.5 MeV
289.5 MeV SU(3)
(consistent with lattice average)
15
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a
2π
V [a]/T 4
Φ[a] = 0
Tc/√
σ = 0.658± 0.023
Tc = 289.5± 10 MeV ,
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Effective Potential
Braun, Gies, Pawlowski, Phys. Lett. B 684 (2010) 262
285 MeV
295 MeV
300 MeV
310 MeV
289.5 MeV
289.5 MeV SU(3)
(consistent with lattice average)
Φ[amin]
T/Tc
0.90 0.95 1.00 1.05 1.10 1.15 1.20 1.25
0.0
0.2
0.4
0.6
0.8
1.0
15
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Tc = 305+40−55MeV
V ��[amin] ∝ |t|2ν , ν = 0.65(2) [νIsing = 0.63]
V [a] = −�
kflow
�V ��[a], αMM
s (k)�
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Order Parameter
Universal properties & gauge independence
JMP, Marhauser ‘08
Φ[A0]
T/Tc
Marhauser, Pawlowski, arXiv:0812.1144• Polyakov gauge:
• critical exponent from screening mass:
Φ[amin]
= t + 1
16
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Dµν(p) =ZT(p2)
p2PT
µν +ZL(p2)
p2P L
µν
3-dim. fixed-point behavior for p < T ,only weakly T -dependent otherwise,Nf dependence
T = 0 : ZT = ZL = Z
T > 0 : ZT � Z
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Finite Temperature Propagators
• Pure (Landau) gauge:
Maas, Wambach, Grüter, Alkofer, EPJC 37 (2004) 335
• Lattice & DSEs:
Maas, Wambach, Alkofer, EPJC 42 (2005) 93
Cucchieri, Karsch, Petreczky, Phys. Lett. B 497 (2001) 80Cucchieri, Karsch, Petreczky, Phys. Rev. D 64 (2001) 036001
Cucchieri, Maas, Mendes, Phys. Rev. D 75 (2007) 076003Maas, arXiv:0911.0348
• Running coupling, FRG:
Braun, Gies, Phys. Lett. B 645 (2007) 53Braun, Gies, JHEP 06 (2006) 024
Marhauser, Pawlowski, arXiv:0812.1144
17
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DL(0)−1/2
ν = 0.60(1)∝ (T/Tc − 1)ν ,
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Electric Screening Mass
0
0.2
0.4
0.6
0.8
1
1.2
1.4
0 0.5 1 1.5 2 2.5
SU(2)SU(3)
Maas, LvS, in progress
[νIsing = 0.63]
T/Tc
• finite volume
• Gribov copies
(well established)• critical behavior?
18
�ν = 0.62(2)
∝�
T
Tc− (1 + δ) ,
Maas, private communicationFischer, Maas, Müller, arXiv:1003.1960
Data:
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7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Applications II
Deconfinement & Chiral Symmetry Restoration
— quenched —
19
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ψ(1/T, �x) = −e2πiθψ(0, �x)
O(θ) =�O[ψθ]
�e.g., θ-dependent quark condensate,
mass function, density . . .
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Applications II
Deconfinement & Chiral Symmetry Restoration
— quenched —
• Allow quarks with b.c.’s:
• in observables:
19
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ψ(1/T, �x) = −e2πiθψ(0, �x)
O(θ) =�O[ψθ]
�e.g., θ-dependent quark condensate,
mass function, density . . .
O(θ + 1) = O(θ)
O(θ + 1/3) = O(θ)
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Applications II
Deconfinement & Chiral Symmetry Restoration
— quenched —
• Allow quarks with b.c.’s:
• in observables:
, always � Fourier series
, in Z3-symmetric confined phase
• observe:
19
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�O =� 1
0dθ O(θ) e−2πiθ
, dual quark condensate,dual mass, density . . .�
Z3-symmetry, confinement⇒ �O = 0�
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Dual Order Parameters
• Order parameter for confinement:
• Originally from lattice
Gattringer, Phys. Rev. Lett. 97 (2006) 032003Synatschke, Wipf, Wozar, Phys. Rev. D 75 (2007) 114003Synatschke, Wipf, Langfeld, Phys. Rev. D 77 (2008) 114018Bilgici, Bruckmann, Gattringer, Hagen, Phys. Rev. D 77 (2008) 094007
20
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7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
T-dependent Gluon PropagatorT-dependent gluon
T -dependent gluon propagator from lattice data
0 5 10 15p2 [Gev2]
0
0.5
1
1.5
2
2.5
Z T(p2 )
T=0T=0.6 TcT=0.99 TcT=2.2 Tc
0 5 10 15p2 [Gev2]
0
0.5
1
1.5
2
2.5
Z L(p2 )
T=0T=0.6 TcT=0.99 TcT=2.2 Tc
C.F., Maas and Mueller, in preparation
Christian S. Fischer (TU Darmstadt / GSI) Phase transitions and spectral functions 25th of Feb. 2010 11 / 25
Fischer, Maas, Müller, arXiv:1003.1960
• Input for quark DSE:
Fischer, Phys. Rev. Lett. 103 (2009) 052003Fischer, Müller, Phys. Rev. D 80 (2009) 074029
21
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Tchiral ≈ Tconf ≈ 277 MeV
−→ Christian Fischer’s talk
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Chiral & Deconfinement Transition(s)Transition temperatures
0 0.5 1 1.5 2 2.5T/Tc
0.00
0.05
0.10Polyakov loopCondensate
0 0.5 1 1.5 2 2.5T/Tc
0.00
0.05
0.10Polyakov loopCondensate
C.F., Maas, Mueller in preparation
similar transition temperatures for chiral and deconfinementSU(2): T ! 305 MeV SU(3): T ! 270 MeVincreasing chiral condensate due to electric screening masses
Christian S. Fischer (TU Darmstadt / GSI) Phase transitions and spectral functions 25th of Feb. 2010 15 / 25
dual condensate (dressed Polyakov loop)
chiral condensate
Fischer, Maas, Müller, arXiv:1003.1960
SU(3), quenched
(chiral limit)
22
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7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Applications III
Full Dynamical QCD
— at zero & imaginary chemical potential —
23
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Oθ(θ) =�O[ψθ]
�θ observables in different theories,
built on θ-dependent ground states
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Applications III
Full Dynamical QCD
— at zero & imaginary chemical potential —
ψ(1/T, �x) = −e2πiθψ(0, �x)• Quarks with b.c.’s:
• but observables:
23
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Oθ(θ) =�O[ψθ]
�θ observables in different theories,
built on θ-dependent ground states
µ = 2πi Tθ
O(θ + 1/3) = O(θ)
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Applications III
Full Dynamical QCD
— at zero & imaginary chemical potential —
ψ(1/T, �x) = −e2πiθψ(0, �x)• Quarks with b.c.’s:
• but observables:
• observe: now always!
• imaginary chemical potential:
Roberge, Weiss, Nucl. Phys. B 257 (1986) 734
23
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a0 =1T
�gA30�θ=0 ,
aθ =1T
�gA30�θ , quark condensate, mass, density,
fπ,. . . , order parameters forchiral phase transition in QCDθ
(but no dual order parameters)
breaks Roberge-Weiss symmetry,→ dual observables, deconfinement transition
(dual condensate, dual density . . . )
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Full Dynamical QCD
• Landau gauge Yang-Mills with background, compare:
(a)
(b)
• include Nf = 2 dynamical quarks massless, chiral limit
• coupled to mesons dynamical hadronisation
24
c.f., quark meson model:
Schaefer, Wambach, Phys. Part. Nucl. 39 (2008) 1025Berges, Tetradis, Wetterich, Phys. Rept. 363 (2002) 223
![Page 42: QCD Phase Transitions and Green’s Functionspawlowsk/Delta10/talks/...Hoehler et al., NPB 114(1976), 505 Bosted et al., PRL 68(1992), 3841 All contributions 2ïloop contributions](https://reader036.vdocuments.net/reader036/viewer/2022070903/5f5e389fb8878118cd4ab8e1/html5/thumbnails/42.jpg)
Tchiral ≈ Tconf ≈ 180 MeV
±20 MeV
µ = 0
−→ Lisa Haas’ talk
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Full Dynamical QCD, Nf = 2, chiral limit
Braun, Haas, Marhauser, Pawlowski, arXiv:0908.0008
0
0.2
0.4
0.6
0.8
1
150 160 170 180 190 200 210 220 230
T [MeV]
f!(T)/f!(0)
Dual density
Polyakov Loop
160 180 200"
L,d
ual
a0 =1T
�gA30�θ=0 ,(a)
25
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change boundary conditions of confined quarks at no cost
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Full Dynamical QCD, Nf = 2, chiral limit
Braun, Haas, Marhauser, Pawlowski, arXiv:0908.0008
θ
• free energy difference:
f(T, θ)− f(T, 0)
26
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QCDθ ,
−→ Lisa Haas’ talk
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
QCDθ — imaginary chemical potential
(b) µ = 2πi Tθ
• Originally from lattice de Forcrand, Philipsen, Nucl. Phys. B 642 (2002) 290D’ Elia, Lombardo, Phys. Rev. D 67 (2003) 014505Kratochvila, de Forcrand, Phys. Rev. D 73 (2006) 114512Wu, Luo, Chen, Phys. Rev. D 76 (2007) 034505
no sign poblem
• Here
0
50
100
150
200
250
300
0 !/3 2!/3 ! 4!/3
T [M
eV
]
2!"
Tconf
T#
Braun, Haas, Marhauser, Pawlowski, arXiv:0908.0008
27
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�M =� 1
0dθ M(θ) e−2πiθ Mθ(θ + 1/3) = Mθ(θ)
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Dual Observables vs. Chiral Transition in QCDθ
θ
• Quark mass parameter(a) dual mass, confinement (b) mass in QCDθ, chiral symmetry breaking
∆θ = 1/3
28
Mθ(θ)
M(θ)
![Page 46: QCD Phase Transitions and Green’s Functionspawlowsk/Delta10/talks/...Hoehler et al., NPB 114(1976), 505 Bosted et al., PRL 68(1992), 3841 All contributions 2ïloop contributions](https://reader036.vdocuments.net/reader036/viewer/2022070903/5f5e389fb8878118cd4ab8e1/html5/thumbnails/46.jpg)
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Summary & Outlook
29
• Propagators and Running Coupling of Landau Gauge QCDvery well understood at T=0, increasingly well at finite T
2
3
4
1
0 5 64321
!"!! #"$
%&!! #"$
!"!! '"(
'#!! '"(
%&!! '""
Z(p2)
p [GeV]
0.05
0.10
0.15
0.20
0.25
0.30
0.35
0.40
1 10 100 1000 10000
!M
ML
(p2)
p2 [GeV2]
Nf = 0
(!, N4) = (6.0, 324)(6.2, 324)(6.4, 324)(6.6, 324)(6.9, 484)(7.2, 644)(7.5, 644)(8.5, 484)
!MMs (p2)
![Page 47: QCD Phase Transitions and Green’s Functionspawlowsk/Delta10/talks/...Hoehler et al., NPB 114(1976), 505 Bosted et al., PRL 68(1992), 3841 All contributions 2ïloop contributions](https://reader036.vdocuments.net/reader036/viewer/2022070903/5f5e389fb8878118cd4ab8e1/html5/thumbnails/47.jpg)
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Summary & Outlook
29
• Propagators and Running Coupling of Landau Gauge QCDvery well understood at T=0, increasingly well at finite T
• 1st Applications of range from:deconfinement phase transition of the pure gauge theory
The hard part done!
deconfinement & chiral symmetry restoration in full QCD at zero and imaginary chemical potential
285 MeV
295 MeV
300 MeV
310 MeV
289.5 MeV
289.5 MeV SU(3)
0
0.2
0.4
0.6
0.8
1
150 160 170 180 190 200 210 220 230
T [MeV]
f!(T)/f!(0)
Dual density
Polyakov Loop
160 180 200
"L,d
ual
![Page 48: QCD Phase Transitions and Green’s Functionspawlowsk/Delta10/talks/...Hoehler et al., NPB 114(1976), 505 Bosted et al., PRL 68(1992), 3841 All contributions 2ïloop contributions](https://reader036.vdocuments.net/reader036/viewer/2022070903/5f5e389fb8878118cd4ab8e1/html5/thumbnails/48.jpg)
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Summary & Outlook
29
• Propagators and Running Coupling of Landau Gauge QCDvery well understood at T=0, increasingly well at finite T
• 1st Applications of range from:deconfinement phase transition of the pure gauge theory
The hard part done!
deconfinement & chiral symmetry restoration in full QCD at zero and imaginary chemical potential
• Tested against Lattice Results
![Page 49: QCD Phase Transitions and Green’s Functionspawlowsk/Delta10/talks/...Hoehler et al., NPB 114(1976), 505 Bosted et al., PRL 68(1992), 3841 All contributions 2ïloop contributions](https://reader036.vdocuments.net/reader036/viewer/2022070903/5f5e389fb8878118cd4ab8e1/html5/thumbnails/49.jpg)
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Summary & Outlook
29
• Propagators and Running Coupling of Landau Gauge QCDvery well understood at T=0, increasingly well at finite T
• 1st Applications of range from:deconfinement phase transition of the pure gauge theory
deconfinement & chiral symmetry restoration in full QCD at zero and imaginary chemical potential
• Continue to Combine Methods towards:- 2+1 dynamical quark flavors- real chemical potential: critical end point, triple point... ?- obtain model independent information on QCD phase diagram- refine and constrain effective hadronic theories
• Tested against Lattice Results
![Page 50: QCD Phase Transitions and Green’s Functionspawlowsk/Delta10/talks/...Hoehler et al., NPB 114(1976), 505 Bosted et al., PRL 68(1992), 3841 All contributions 2ïloop contributions](https://reader036.vdocuments.net/reader036/viewer/2022070903/5f5e389fb8878118cd4ab8e1/html5/thumbnails/50.jpg)
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Summary & Outlook
Thank You!
29
• Propagators and Running Coupling of Landau Gauge QCDvery well understood at T=0, increasingly well at finite T
• 1st Applications of range from:deconfinement phase transition of the pure gauge theory
deconfinement & chiral symmetry restoration in full QCD at zero and imaginary chemical potential
• Continue to Combine Methods towards:- 2+1 dynamical quark flavors- real chemical potential: critical end point, triple point... ?- obtain model independent information on QCD phase diagram- refine and constrain effective hadronic theories
• Tested against Lattice Results
![Page 51: QCD Phase Transitions and Green’s Functionspawlowsk/Delta10/talks/...Hoehler et al., NPB 114(1976), 505 Bosted et al., PRL 68(1992), 3841 All contributions 2ïloop contributions](https://reader036.vdocuments.net/reader036/viewer/2022070903/5f5e389fb8878118cd4ab8e1/html5/thumbnails/51.jpg)
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Extra Sides
38
Some Additional Material
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�ψ(x)ψ̄(y)� :
�c(x)c̄(y)� :
�Aµ(x)Aν(y)� :
(T = 0 here)
Dµν(p) =Z(p2)
p2
�δµν −
pµpν
p2
�
DG(p) = −G(p2)p2
S(p) =Zψ(p2)
ip/ + M(p2)
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Dyson-Schwinger Equations
39
-1=
-1- 1/2 - 1/2
- 1/6 - 1/2
+ +
-1=
-1
-1=
-1
glue:
ghost:
glue:
quark:
Z[j] = � exp(j,φ) �
Generating functional:
Green’s functions
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7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Functional RG (Flow) Equations
40
! "#$ S"#$ !k
k=%
k
"#$
k 0
IR UV
k- k&
0.5 1 1.5 2
0.2
0.4
0.6
0.8
1
0.5 1 1.5 2
2
4
6
8
!t!k["] = 1
2
!
"
!
k∂kΓk[φ]Wetterich, Phys. Lett. B 301 (1993) 90
Γ[φj ] = (j,φj)− lnZ[j]Effective action:Legendre transform
Γ(n)(x1, . . . xn)
φj = �φ�j
1PI vertex functions
free energy with
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7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Functional RG (Flow) Equations
41
k !k!1 = !
"!
"+1
2
"+1
2
"
!12
"
+
"
k !k!1 =
"+
"
!12
"
+
"
glue:
ghost:
Landau gauge QCD propagators,
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Z[j] = � exp(j,φ) �
φ = {A, c, c̄, ψ, ψ̄}
�φ(x)φ(y)�, �φ(x)φ(y)φ(z)�, . . .
Γ[φj ] = (j,φj)− lnZ[j]
Γ(n)(x1, . . . xn)
φj = �φ�j
7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Generating Functional and Effective Action
42
Introduce sources:
Fields:
Green’s functions
Effective action: 1PI vertex functions
free energy with
Legendre transform
Kopplung der QCD II (Definition)
!gg(p2) =g2
4" G2(p2)Z (p2)
!3g(p2) =g2
4" [!3g(p2)]2 Z 3(p2)
!4g(p2) =g2
4" [!4g(p2)]Z 2(p2)
R. Alkofer, C.F., F. Llanes-Estrada, Phys.Lett.B611:279-288,2005
Christian S. Fischer (TU Darmstadt) Landau gauge QCD 16. März 2007 11 / 39
Kopplung der QCD II (Definition)
!gg(p2) =g2
4" G2(p2)Z (p2)
!3g(p2) =g2
4" [!3g(p2)]2 Z 3(p2)
!4g(p2) =g2
4" [!4g(p2)]Z 2(p2)
R. Alkofer, C.F., F. Llanes-Estrada, Phys.Lett.B611:279-288,2005
Christian S. Fischer (TU Darmstadt) Landau gauge QCD 16. März 2007 11 / 39
Kopplung der QCD II (Definition)
!gg(p2) =g2
4" G2(p2)Z (p2)
!3g(p2) =g2
4" [!3g(p2)]2 Z 3(p2)
!4g(p2) =g2
4" [!4g(p2)]Z 2(p2)
R. Alkofer, C.F., F. Llanes-Estrada, Phys.Lett.B611:279-288,2005
Christian S. Fischer (TU Darmstadt) Landau gauge QCD 16. März 2007 11 / 39
Laufende Kopplung: ’IR-slavery’
!qg(p2) ! (p2)!1/2!! , Zf (p2) ! const , Z (p2) ! (p2)2!
!qg(p2) = !µ [!qg(p2)]2 [Zf (p2)]2 Z (p2) ! constqgNc
1p2
0.01 0.1 1 10 100Q [GeV]
0
1
2
3
4
5
!(Q) YM-couplingsQuark-gluon coupling
Christian S. Fischer (TU Darmstadt) Landau gauge QCD 16. März 2007 32 / 39
ΓcAc̄ ΓψAψ̄Γ3A Γ4A
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p2 [GeV2]
L = 13.6 fm
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Ghost Propagator
43
13
10-4 10-3 10-2 10-1 100 101 102
p2 [GeV2]
10-4
10-3
10-2
10-1
100
Z(p2 )
scalingdecoupling
10-4 10-3 10-2 10-1 100 101 102
p2 [GeV2]
100
101
102
G(p
2 )
scalingdecoupling
FIG. 5: Numerical solutions for the ghost and gluon dress-ing function with di!erent boundary conditions G(0). The(artificial) longitudinal components of the gluon propagatorare not displayed, since they are of the order of less than onepermille, i.e. of the order of the numerical error of our cal-culations. All results shown here are obtained from our noveltruncation scheme. Di!erences to the scheme defined in [5, 70]are, however, only very small and would not be visible in theplots.
E. Numerical results
Our numerical solutions for the ghost and gluon dress-ing functions are shown in Fig. 5. The correspondingmomentum scale has been fixed by best-possible match-ing of the gluon dressing function to the correspondingone on the lattice, cf.
V. SEC:LATTICE
. Thus we inherit the lattice scale. All results displayedare obtained from our novel truncation scheme. Di!er-ences to the scheme defined in [5, 70] are, however, onlyvery small and would not be visible in the plots. This pro-vides additional justification that the old scheme alreadyrepresented a reliable result. Transversality is manifest inour new truncation scheme; the longitudinal components
10-4 10-3 10-2 10-1 100 101 102
p2 [GeV2]
10-2
10-1
100
101
!(p
2 )
scalingdecoupling, G2Z
10-4 10-3 10-2 10-1 100 101 102
p2 [GeV2]
10-1
100
101
!(p
2 )
scalingdecoupling, G2Z
FIG. 6: The running coupling for the two types of solu-tions, defined as !(p2) = !(µ2)G(p2)2Z(p2) (top diagram)and !(p2) = !(µ2)G(p2)2Z̄(p2) (bottom diagram).
of the propagator (not shown in the figure) are smallerthan one permille and therefore of the same size as thenumerical error of our calculation. Quadratic divergen-cies do not appear and the numerical solutions respectmultiplicative renormalizability, see appendix B.
By varying the boundary condition G(0, µ2) we areable to generate both, a solution of the scaling type I, eq.(15)), with G!1(0, µ2) = 0 and a continuous set of decou-pling solutions characterized by a finite value G(0, µ2).Shown are results for three di!erent values of G(0, µ2).The corresponding gluon propagator is either massive inthe sense that D(0) = limp2"0 Z(p2)/p2 = const. fordecoupling, or has the power like behavior (15) with! = !C = (93 !
"1201)/98 # 0.595353 [4] in the case
of scaling. In the ultraviolet momentum region, bothtypes of solutions are almost identical, as expected. Therunning couplings are shown in Fig. 6. For the scal-ing solution one observes the infrared fixed point knownfrom previous studies, whereas the coupling for the de-coupling solution falls with p2 in the infrared when themass-independent definition (40) is used (top diagramof Fig. 6). If, however, we employ the mass-dependentdefinition (43) (bottom diagram of Fig. 6) the resulting
7
8
9
10
11
12
188
180
172
164
156
D(0
)[G
eV!
2]
1/L
Figure 3: Zero-momentum gluon propagator D(0) versus 1/L.
4. Ghost propagator
The Landau-gauge ghost propagator is defined by
Gab(q) = a2!
x,y
"e!2!ik·(x!y)/L[M!1]ab
xy
#
= !abG(q2) , (6)
where M denotes the lattice Faddeev-Popov operator, be-ing the Hessian of the gauge functional (2) with respect togx, in the background of the gauge-fixed links Uxµ
Mabxy =
!
µ
$Aab
x,µ !x,y ! Babx,µ !x+µ̂,y ! Cab
x,µ !x!µ̂,y
%(7)
with
Aabx,µ = Re Tr
${T a, T b}(Ux,µ + Ux!µ̂,µ)
%,
Babx,µ = 2 · Re Tr
$T bT a Ux,µ
%,
Cabx,µ = 2 · Re Tr
$T aT b Ux!µ̂,µ
%.
T a, a = 1, . . . , 8 are the (Hermitian) generators of thesu(3) Lie algebra satisfying Tr [T aT b] = !ab/2.
To invert M we use the conjugate gradient (CG) al-
gorithm with plane-wave sources "#c with colour and po-sition components #a
c (x) = !ac exp(2$i k·x/L). In fact,we apply a pre-conditioned CG algorithm (PCG) to solveMab
xy%b(y) = #ac (x) where as pre-conditioning matrix we
use the inverse Laplacian operator !!1 with diagonal coloursubstructure (for details see [23, 42]).
For the large lattice sizes as considered here, we areconfident that finite-volume distortions for all lattice mo-menta besides the two minimal ones do not change consid-erably with increasing L (see Fig. 4 and [37] for details).In this figure the ghost dressing function J(q2) = q2G(q2)is presented in a log-log scale. We do not see any power-like singular behaviour in the limit q2 " 0. Instead, wehave a good indication that J(q2) reaches a plateau justas the decoupling solution of DS and FRG equations does(see also [28, 33]).
4
3
2
10.001 0.01 0.1 1 10 100
J(q
2)
q2 [GeV2]
! = 5.7 644 (14 conf.)804 (11 conf.)804 (5 conf.)
Figure 4: Bare ghost dressing function J(q2) versus q2 for L = 64, 80at ! = 5.70. Errors are not shown at the two lowest q2 (squares).
5. Running coupling
Finally, let us present the running coupling defined asthe renormalization group (RG) invariant product
&s(q2) =
g20
4$Z(q2)J2(q2) , (8)
of the Landau-gauge gluon and ghost dressing functions.This definition is based on the ghost-gluon vertex in amomentum-subtraction scheme with the vertex renormal-isation constant (in Landau gauge) set to one. This ispossible [43], since the vertex is known to be regular [44](see also the lattice studies [45, 46]). Note that the rela-tion of &s in this scheme to the running coupling in the MSscheme is known to four loops and it can provide a valu-able alternative to the MS coupling in phenomenologicalapplications [43].
Beyond perturbation theory, the behaviour of &s dif-fers at low scales for the scaling and decoupling solutions.Based on our propagator data we can calculate &s for in-termediate and lower scales, and it clearly shows a decreasetowards q2 " 0 (see Fig. 5). This is again consistent withthe decoupling DS and FRG solutions.
6. Conclusions
The progress achieved on the lattice during the lasttwo years in studying the IR limit of gluodynamics andchecking the well-known scenarios of confinement in termsof Landau-gauge Green’s functions leads us to the follow-ing conclusions. Within the standard lattice approach asdescribed above only the decoupling-type solution of DSand FRG equations seems to survive. Since for this solu-tion the gluon propagator tends to a non-zero IR value, itcorresponds to a massive gluon. It has been argued thatthis behaviour contradicts global BRST invariance [12].
4
Bogolubsky et al., Phys. Lett. B 676 (2009) 69
Fischer, Maas, Pawlowski, Annals Phys. 324 (2009) 2408Maas, arXiv:0907.5185
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7. Mai 2010 | Fachbereich 5 | Institut für Kernphysik | Lorenz von Smekal |
Imaginary Chemical Potential
44
• Polyakov-NJL model:
Sakai, Kashiwa, Kouno, Matsuzaki, Yahiro, Phys. Rev. D 79 (2009) 096001Wu, Luo, Chen, Phys. Rev. D 76 (2007) 034505Lattice data: