t. hatsuda (university of tokyo)
DESCRIPTION
QCD Phase Structure at High Baryon Density. T. Hatsuda (University of Tokyo). contents Introduction Ginzburg-Landau approach to Dense QCD (1) Continuity in Dense QCD (2,3) UCA/QCD Correspondence (4) Summary. - PowerPoint PPT PresentationTRANSCRIPT
T. Hatsuda (University of Tokyo)
QCD Phase StructureQCD Phase Structure
at High Baryon Density at High Baryon Density
contents• Introduction • Ginzburg-Landau approach to Dense QCD (1)
• Continuity in Dense QCD (2,3)
• UCA/QCD Correspondence (4)
• Summary
(1) Tachibana, Yamamoto, Baym & T.H., PRL 97 (2006) 122001; PRD 76 (2007) 074001.
(2) Tachibana, Yamamoto & T.H., PRD 78 (2008) 011501.
(3) Maeda, Baym and T.H., PRL 103 (2009) 085301
(4) Abuki, Baym, Yamamoto and T.H., arXiv: 1003.0408 [hep-ph]
NFQCD, March 10, 2010
Physics Today, Dec. vol.58 (2005)
http://www.lsbu.ac.uk/water/phase.html H2O H2O
4He 4He
Symmetry realization in hot/dense QCD ( for mu,d,s=0 case )
Symmetry realization in hot/dense QCD ( for mu,d,s=0 case )
QGP
0 RtRL
tL CqqCqqCFL :
Alford, Rajagopal & Wilczek, NP B537 (1999)
BRLC USUSUSU )1(])3()3([)3(
QGP :
Collins & Perry, PRL 34 (1975)
SB :
Nambu, PRL 4 (1960)
BRLC USUSU )1()3()3( RLRLC ZZSU )2()2()3(
0RLqq
QCD and high temperature superconductivityQCD and high temperature superconductivity
SB CSC
QGP
1. Competition between different orders
2. Strong coupling
Common features
• Kitazawa, Nemoto, Kunihiro, PTP (‘02)• Abuki, Itakura & Hatsuda, PRD (’02) • Chen, Stajic, Tan & Levin, Phys. Rep. (’05)
Dirac
Fermi
Transition at Finite T
SB CSC
QGP
Chiral field: ~
Chiral transformation:
Pisarski & Wilczek (’84)
Symmetry:
Ginzburg-Landau-Wilson analysis in hot QCD Ginzburg-Landau-Wilson analysis in hot QCD
SU(Nf)LxSU(Nf)RxU(1)A
SU(Nf)LxSU(Nf)R
quark mass term
Axial anomaly
XAfNZ )2(
Pisarski and Wilczek, PRD29 (’84)
Svetitsky & Yaffe, NPB210 (’82)Order of the thermal QCD transition (μ=0) Order of the thermal QCD transition (μ=0)
1st
1st
cross over
2nd
ms
small
larg
e
mu,dsmall large
Nf=0
Nf=1
Nf=2
Nf=3
Transition at Finite T
SB CSC
QGP
Asakawa-Yazaki CP
Transition at finite μ
SB CSC
QGP
CP
Thermonuclear Burst in X-ray Binaries4U 1608-248 EXO 1745-248 4U 1820-30
Mass-Radius relation of Neutron Stars and dense EOS Mass-Radius relation of Neutron Stars and dense EOS
1
42
2 21
R
GM
fD
RA
c
2/1
2
21
4
R
GM
D
GMF
csedd
(i) Apparent surface area
(ii) Eddington limit
Ozel, Baym & Guver, arXiv: 1002.3153 [astro-ph.HE]
Color superconductivity at high densityColor superconductivity at high density
major differences from the standard BCS superconductor
1. Relativistic fermi system color-magnetic int. dominant
High Tc : Tc/F ~ 0.1Compact pair : r~ 1-10 fm
Son, PRD59 (’99), Schafer & Wilczek, PRD60 (’99)Pisarski & Rischke, PRD61 (’00)Hong, Miransky, Shovkovy & Wijewardhana, PRD61 (’00)
2. Color-flavor entanglement
Various phases (c.f. Ice, 3He) 2SC, uSC, dSC, CFL etc
flavor color
u
d s
u
d s
u
d s
u
d s
CFLdSCuSC2SC
Pisarski & Wilczek, PRD29 (’84)
Iida & Baym, PRD63 (’01) Yamamoto, Tachibana, Baym & T.H., PRL97 (’06)
GL analysis for chiral-super interplay in QCD (Nf=3) GL analysis for chiral-super interplay in QCD (Nf=3)
Symmetry:
Chiral field: diquark field:
AZ )6(
Complete classification of the GL potential (mu,d,s=0)Complete classification of the GL potential (mu,d,s=0)Yamamoto, Tachibana, Baym & T.H., PRL 97 (’06), PRD 76 (‘07)
Axial anomaly
RL ZZ )2()2( broken explicitly
Chiral-CFL interplay in NChiral-CFL interplay in Nff=3 =3
Natural parameter relations
phase diagram (without d-σphase diagram (without d-σ coupling)coupling)
μ
T
phase diagram (with d-σ coupling)phase diagram (with d-σ coupling)
Low T critical point driven by the axial anomalyLow T critical point driven by the axial anomaly
T
μ
phase diagram (with d-σ coupling & quark mass)phase diagram (with d-σ coupling & quark mass)
h
Low T critical point driven by the axial anomalyLow T critical point driven by the axial anomalyHigh T critical point driven by Higgs condensateHigh T critical point driven by Higgs condensate
T
μ
NJL model with axial anomaly (mu=md=ms) NJL model with axial anomaly (mu=md=ms) Abuki, Baym, Yamamoto and T.H.,arXiv: 1003.0408 [hep-ph]
Spectral continuity at finite μ
SB CSC
QGPCP induced by Higgs
CP induced by anomaly
co
nden
sate
s Continuity in the ground state
Generalized Gell-Mann-Oakes-Renner relation :
Yamamoto, Tachibana, Baym & T.H., PR D76 (’07)
○
Tachibana, Yamamoto and T.H., PRD78 (2008)
○
Continuity in excitation modes
Vector meson – CFL gluon continuity (QCD sum rules):
diquark BCS
Baryon BCS
diquark BEC
UCA/QCD correspondenceUCA/QCD correspondence
“Simulating dense QCD matter with Ultracold atoms ?” Maeda, Baym and Hatsuda, Phys. Rev. Lett. 103 (2009) 085301
Neutron matter
quarkMatter?
b fσ
s-wave boson-fermion
scattering length
+0
-0
strong
weak
0weak
strong
0
Maeda, Baym and Hatsuda, Phys. Rev. Lett. 103 (2009) 085301Atomic BF mixtureAtomic BF mixture
Induced superfluidity of composite fermions -- a novel analogy between cold atoms and QCD --
Induced superfluidity of composite fermions -- a novel analogy between cold atoms and QCD --
Maeda, Baym & Hatsuda,Phys. Rev. Lett. 103 (’09)
CompositeFermion
cold atoms dense QCD
weak (bf)-(bf) attraction ⇔ strong b-f attraction baryon superfluidity ⇔ strong diqark correlation
Phase structure and symmetryPhase structure and symmetry
N-BCS b-BEC
Broken and residual symmetries (continuous symmetries)
broken
residual
b,f normal gas
N normal gas b-BEC
N-BCS
0
T
strong couplingstrong coupling weak couplingweak coupling
b,f normal gas
//( )b f1 31 n a
The Hamiltonian density has symmetry.
Y. Nambu, Nobel Lecture (Dec.8, 2008), page 24/25
1.1. QCD phase structureQCD phase structure ・ Three major phases in QCD: χSB, QGP and CSC ・ Axial anomaly plays crucial roles everywhere ・ Close similarity with high Tc supercond. & multi-comp. cold atoms
2.2. Chiral-super interplay driven by axial anomalyChiral-super interplay driven by axial anomaly ・ A new critical point at low T and high μ
・ Continuity of χSB phase and CSC phase
3.3. Spectral continuity in high density QCDSpectral continuity in high density QCD・ Pions are pions.
・ Vector mesons are gluons.
4. Future4. Future・ Real location of the new critical point ? ・ How to detect critical lines and points in lab. experiment ?
・ Tabletop simulations of high density QCD using cold atoms ?
Summary and FutureSummary and Future