thermal phase transitions in realistic dense quark matter
DESCRIPTION
Thermal phase transitions in realistic dense quark matter. Taeko Matsuura (Tokyo) K. Iida (RIKEN BNL) M. Tachibana (RIKEN) T. Hatsuda (Tokyo). Physical Review Letters 93 (2004) 132001 hep-ph/0411356 (to appear in PRD). - PowerPoint PPT PresentationTRANSCRIPT
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Thermal phase transitions in realistic dense quark matter
Taeko Matsuura (Tokyo)
K. Iida (RIKEN BNL)
M. Tachibana (RIKEN)
T. Hatsuda (Tokyo)
Physical Review Letters 93 (2004) 132001
hep-ph/0411356 (to appear in PRD)
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μ
T mu,d,s =0
Color superconductor (CFL)
Idealized QCD phase diagram (Nf=3)Idealized QCD phase diagram (Nf=3)
Hadron
QGP
mu,d ~0 and ms ~200 MeV beta equilibriumcharge neutral
Realistic QCD phase diagram (Nf=3)Realistic QCD phase diagram (Nf=3)
““external fields”external fields”
μ
T
dSC2SC
QGP
Hadron mCFL
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system External field pairings New phases
liquid 3He
A phase
magnetic field A1-A2
electron super
conductor
magneticimpurity
pairing with different moms
Crystalline
Structure
(FFLO)
color super conductor near Tc
m and unequal Fermi moms for
different flavors (u,d,s)
dSC
unequal Fermi moms for ( ) and ( )
Examples of new phases driven by external fields Examples of new phases driven by external fields
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Color Superconductor (without m, ) Color Superconductor (without m, )
Entangled pairing in color-flavor space
PJ 0 Color antisym
Flavor antisym
ab a bij i 5 jq C q (m
omen
tum
)
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Realistic quark matter at T~TcRealistic quark matter at T~Tc
quark mass ms >> mu,d 0,
beta equilibrium
i= - qi e (i=u, d, s)
electric neutrality
Q = Qquark +Qelectron= 0
color neutrality
nR = nB = nG
major role
minor role
Why we consider T~Tc ? Effect of the ext. field (m, ) prominent Ginzburg-Landau expansion possible (Δ<< Tc )
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Color Superconductor (with m, ) near TcColor Superconductor (with m, ) near Tc
・ ・ What kind of phase structure near TWhat kind of phase structure near Tcc? ?
・ ・ What are the quark & gluon spectra ?What are the quark & gluon spectra ?
2
4sm
2
2sm
2
2sm
2
4sm
Tc
Ext. fields:0
0 =u
d
s s
m
m
ms2
μ
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Ginzburg-Landau free energyGinzburg-Landau free energy
Near Tc (Δ << Tc)
2 4 6S( ) +O( ) , 0C
C
T -Ta b a b
T
Corrections fromquark mass &charge neutrality
Corrections fromcolor neutrality
T<TcT>Tc
ΔΔ
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m=0, =0 Iida & Baym, PRD (`01)
3E 0
0
QCD at finite temperature & density
1S ( ( ) )
4a ad d r iD m F F
small external fields
22 2 21
4 4 42
ud ds su
ud ds su
β
β
2 2 2Cud ds su
C
T -T
T 2
4
( )
( )
O
O
22
1 2 =4 , ( / )2 cT
High density QCD → GL free energyHigh density QCD → GL free energy
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m≠0, ≠0 Iida,Matsuura,Tachibana,&Hatsuda, PRL (2004)
2lnFij
ijij C
p
T
2
F Fi jF
ij
p pp
2lnFijC
ijij C C
pT -T
T T
Flavor dependent shift of the GL free energy
O(Δ2ms2)
Flavor
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1 lnFijijc
c c
pT
T T
Larger averaged Fermi mom.
ud ds suF F Fp p p ud ds su
c c cT T T
shift of shift of critical temperaturecritical temperature
More stable pairing
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22
2
3
8 2sm
g
New phase : dSCNew phase : dSC
T
dSC
2 cT
3 cT
mCFL
2SCCFL
normal normal
m ,=0 m , ≠0
Second order phase transitions (MFA)
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elementary excitation spectraelementary excitation spectra
Gluons Quasi fermions (Nambu-Goldstone bosons)
●Gluons (Meissner masses)
number of
massive gluons
mCFL 8
dSC 8
2SC 5
2 2 2A1,2
2 2 2A4,5
2 2 2A6,7
2 2 2 2 2 22
A 2 28
4 4 2 22
2 2A
γ g ( + )
γ g ( + )
γ g ( + )
4γ g
3 +
+4γ g
3 +
ds us
ds ud
us ud
ds us ds ud us ud
ds us
ds us ds us
ds us
m
m
m
m
m
2( / )cT
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● Gapless quasi-fermions
T
normal phase
2SC mCFL dSC
Cf. Alford, Berges & Rajagopal (`99),
M.Huang & I.Shovkovy (`03)
p p
Unpaired case Paired case
0 2 0 4 0 3 1paired 9 5 5 2 2 0 0unpaired
2
smonly
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summarysummary
We studied the phase structure near CSC ⇔ QGP boundary with strange quark mass and charge neutrality using Ginzburg-Landau theory
m and lead to Flavor dependent pF
Pairing occur between quarkswith different pF
ij ij
c FT p
gapless fermion appearsat very close to Tc
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μ
T
dSC2SC
QGP
Hadron mCFL
gCFL,g2SC, uSC,CFLK,FFLO, BEC, ・・・
thermal phase structure in the mean-field approx. (MFA)& new dSC phase (this work)
Order of the phase transition may change. (beyond MFA)
Matsuura, Iida, Hatsuda, and Baym, PRD 074012(2004)
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back up
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Ginzburg-Landau (T ~Tc) local coupling to gluons mA
2 >0 (always)
QCD nonlocal coupling to gluons
k k
Giannakis & Ren (hep-ph/0412015)
2δ
δ > 0.3041 ×2πkB T mA8
2 , κ < 0 unstable to FFLO δ < 0.3041 ×2πkB T ← our case mA8
2 , κ > 0 stable to FFLO
κ:momentum susceptibility
Meissner mass
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Why color neutrality does not play role ?
T normal
super
μe, μ8
μe
μ8
2( )O
(1)O
Tc
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FFLO pairing
“BCS” pairing(zero free energy condition) F=E-μN
μu < μd
ku=q + pkd=q – p
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22
2
3
8 2sm
g
Order of Δ and δT
~σTc
Δ~ σTc
T μ Effect of Fluctuation
⇒ T ~ g2 Tc or gTc
>> σTc
(at high density)
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T ~0 vs T ~Tc
ACB
P
T ~0 difference is important
T ~Tc average is important
δ<< Tc