color neutrality effects in the phase diagram of the pnjl model
DESCRIPTION
Color neutrality effects in the phase diagram of the PNJL model. A. Gabriela Grunfeld Tandar Lab. – Buenos Aires - Argentina. In collaboration with D. Blaschke D. Gomez Dumm N. N. Scoccola. Motivation. - PowerPoint PPT PresentationTRANSCRIPT
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Color neutrality effects in the phase Color neutrality effects in the phase diagram of the PNJL modeldiagram of the PNJL model
A. Gabriela GrunfeldTandar Lab. – Buenos Aires - Argentina
In collaboration with
D. BlaschkeD. Gomez Dumm N. N. Scoccola
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Motivation
Understanding of the behavior of strongly interacting matter at finite T and/or density is of fundamental interest and has important applications in cosmology, in the astrophysics of neutron stars and in the physics of URHIC.
CBM@FAIR
From RHIC
(from Jürgen Schaffner-Bielich)
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For a long time, QCD phase diagramrestricted to 2 phases
HADRONIC PHASE: “our world”color neutral hadrons, SB
QGP: S is restored
In recent years phase diagram richer and more complex structure T
Hadrons
QG Plasma
2SC CFL
E
T
Hadrons
QG Plasma
2SC CFL
E
Rajagopal
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The treatment of QCD at finite densities and temperatures is a problem of very high complexity for which rigorous approaches are not yet available
NJL model is the most simple and widely used model of this type.
• Development of effective models for interacting quark matter that obey the symmetry requirements of the QCD Lagrangian
• Inclusion of simplified quark interactions in a systematic way
local interactions
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Effective theories Lattice results at μ -> 0
Reproduce ?
extrapolate at high μ
Nambu Jona-Lasinio model + Polyakov loop dynamiccs
( , )U
Lattice simulations of P in a pure gauge theory
Chiral symmetry breaking
confinement
It reasonable to ask what happens with color neutrality in presence of PL• important in URHIC• could be extended to compact stars imposing electric charge neutrality + β decay
Higher Tc than NJL
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The model
NJL SU(2) flavor + quarks with a background color field related to the Polyakov loop Φ:
mc (current q mass), G and H parameters of the model
1
2 0t
C i
5 2 2Ci
In our case: SU(2) flavor + diquarks + color neutrality
H/G = ¾ from Fierz tr. OGE
diquarks
*S. Rößner, C. Ratti and W. Weise, PRD75, 034007 (2007)
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3 3 8 8
Polyakov loop:
quarks with a background color field aa tΑgiAiA
004
LTrN C
C
1
then
0
4exp AdiL
TiC eTr /
31
Polyakov gauge => diag representation
order parameter for confinement
conf
deconf
0
0
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We considered the polynomial form for the effective potential *:
2
0 00 1 2
3
03
( )
( )
T Ta T a a a
T T
Tb T b
T
with
2*33*** )(3)(461ln)()(21
),( tbTaTU
T0 = 270 MeV from lattice crit temp for deconf.
δSE (Φ,T) -> (V/T) U(Φ,T)
gluon dynamics,
effective potential, confinement-deconf. transition
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over Dirac, flavor and color indices
1 0 0 5 2 2*
5 2 2 0 0
. ( )( , )
. ( )n
n
n
i p iS i p
i p i
Matsubara frequencies ωn=(2n+1) π T
Then, we obtain the Euclidean effective action
where Matsubara frequencies ωn=(2n+1) π T
1
22 3
(4) 3( , ) ln ( ; )22 2 (2 )
MFAMFAE
nn jE
TU T Tr S i p
S d pV G H
• MFA -> drop the meson fluctuations• (+ Usual 2SC ansatz Δ5 = Δ7= 0 and Δ2 = Δ)
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Then, the thermodynamic potential per volume reads:
2 2
2ln 2 ln 1 exp( / )n
n
ET E T E T
T
22 3
(4) 3
1( , ) ln 1 exp ( / )
22
2 2 (2 )
MFAMFAE
f j jjE
U T E T ES d p
NV G H
1,2
2 23,4 3
2 25,6 3
2 2
( )
( )
b
r
E
E i
E i
where
p
8
8
3
23
r
b
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Thermodynamic equilibrium -> minimum of thermodynamic potential. The mean fields and are obtained from the coupled gap equations
together with
We impose color charge neutrality
We consider * 8 0 311 2cos
3 T
To Ω be real
0),(
;0),(
fc
MFAfc
MFA TT
0),(
3
fcMFA T
0),(
8
fcMFA T
=> μ3 = 0
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NUMERICAL RESULTS
we use the set of parameters from PRD75, 034007 (2007) • G = 10.1 GeV-2
• Λ = 0.65 GeV effective theory, fluctuations, at T = μ = 0• H = ¾ G, 0.8G• mc = 5.5• a0 = 3.51• a1 = -2.47• a2 = 15.2 from lattice• b3 = -1.75• T0 = 270.
Phase diagram: Low μ -> XSB and XSB + 2SCHigh μ -> 2SC
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Phase diagrams
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Low temperature expansion
11210
)()(3
20
2)(
2)(2
0
0
22
0
22
8
0
2
2
pdpH
SgSgpdp
SgSgEp
dpM
GmM
rrbb
rrbbc
)()()()(3
20
0
22
8rrbb SgSgSgSgpdp
3/
3/2
3200
00
80
MifM
MifM
M
T = 0
• for μ ≠ 0 (Δ still 0)
Trivially satisfied for a wide range of μ8
• for μ = 0, Δ = μ8= μr = μb = 0, Mo = 324.11 Mev
Step beyond: μ8 from fin T and then T -> 0 For μ < M0/3
2ln238 T
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For μ > M0 (before 1st order ph.tr)
2SC ->
HG
pdpG
0
22
112
G
f )(
• T = 0
If H/G > 0.783 f(Δ) ≠ 0
in region μr = cte f(Δ) ≠ 0
• T ≠ 0
in region μr = cte f(Δ) ≠ 0 untilT = 20 MeV, 2nd order
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Summary and outlookSummary and outlook
• we have studied a chiral quark model at finite T and µ NJL + diquarks + Polyakov loop + color neutrality• ansatz PRD75, 034007 (2007) ϕ8 = 0 => μ8 ≠ 0, then μ3 = 0• to enforce color neutr color neutrality => μ8 ≠ 0 • without PL, symmetric case, with PL non symmetric densities in color space• different quark matter phases can occur at low T and intermediate µ• coexisting phase XSB + 2SC region• Next step: starting with ϕ3 ϕ8 ≠ 0, => μ3 μ8 ≠ 0 more general…
فرامرز
Some ReferencesS. Rößner, C. Ratti and W. Weise, PRD75, 034007 (2007) F. Karsch and E. Laermann, Phys. Rev. D 50, 6954 (1994) [arXiv:hep-lat/9406008].C. Ratti, M. A. Thaler and W. Weise, Phys. Rev. D 73, 014019 (2006) [arXiv:hep-ph/0506234].M. Buballa, Phys. Rept. 407, 205 (2005) [arXiv:hep-ph/0402234].K. Fukushima Physics Letters B 591 (2004) 277–284S. Rößner, T. Hell, C. Ratti and W. Weise, arXiv:0712.3152v1 hep-ph
THANKS!