Title: ???
1QCD 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
- Tachibana, Yamamoto, Baym T.H., PRL 97
(2006) 122001 PRD 76 (2007) 074001. - Tachibana, Yamamoto T.H., PRD 78
(2008) 011501. - 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
2 H2O
3Symmetry realization in hot/dense QCD(for
mu,d,s0 case)
4QCD and high temperature superconductivity
5(No Transcript)
6 Transition at Finite T
7Ginzburg-Landau-Wilson analysis in hot QCD
Pisarski Wilczek (84)
Symmetry
Chiral field
Chiral transformation
8Order of the thermal QCD transition (µ0)
9 Transition at Finite T
Asakawa-Yazaki CP
10 Transition at finite µ
CP
11Mass-Radius relation of Neutron Stars and dense
EOS
Thermonuclear Burst in X-ray Binaries 4U 1608-248
EXO 1745-248 4U 1820-30
Ozel, Baym Guver, arXiv 1002.3153 astro-ph.HE
12Color superconductivity at high density
13GL analysis for chiral-super interplay in QCD
(Nf3)
Symmetry
14Yamamoto, Tachibana, Baym T.H., PRL 97
(06), PRD 76 (07)
Complete classification of the GL potential
(mu,d,s0)
15 Chiral-CFL interplay in Nf3
16phase diagram (without d-s coupling)
17phase diagram (with d-s coupling)
18phase diagram (with d-s coupling quark mass)
19NJL model with axial anomaly (mumdms)
Abuki, Baym, Yamamoto and T.H., arXiv 1003.0408
hep-ph
20 Spectral continuity at finite µ
CP induced by Higgs
CP induced by anomaly
21(No Transcript)
22 UCA/QCD correspondence
23Maeda, Baym and Hatsuda, Phys. Rev. Lett. 103
(2009) 085301
Atomic BF mixture
s-wave boson-fermion scattering length
strong
0
0
weak
0
-0
weak
strong
24Induced superfluidity of composite fermions -- a
novel analogy between cold atoms and QCD --
Maeda, Baym Hatsuda, Phys. Rev. Lett. 103 (09)
weak (bf)-(bf) attraction ? strong b-f attraction
baryon superfluidity ? strong diqark
correlation
25Phase structure and symmetry
Broken and residual symmetries (continuous
symmetries)
The Hamiltonian density has
symmetry.
N-BCS b-BEC
broken
residual
26Y. Nambu, Nobel Lecture (Dec.8, 2008), page 24/25
27Summary and Future
- QCD phase structure
- Three major phases in QCD ?SB, QGP
and CSC - Axial anomaly plays crucial roles
everywhere - Close similarity with high Tc
supercond. multi-comp. cold atoms - Chiral-super interplay driven by axial anomaly
- A new critical point at low T and
high µ - Continuity of ?SB phase and CSC phase
- Spectral continuity in high density QCD
- Pions are pions.
- Vector mesons are gluons.
- 4. Future
- Real location of the new critical point ?
- How to detect critical lines and points in
lab. experiment ?