naoki yamamoto (university of tokyo) 高密度 qcd における カイラル対称性 contents...
TRANSCRIPT
Naoki Yamamoto (University of Tokyo)
高密度 QCD におけるカイラル対称性
contents
• Introduction: color superconductivity• The role of U(1)A anomaly and chiral symmetry
breaking• Partition function zeros and chiral symmetry
breaking• Summary & Outlook(1) T. Hatsuda, M. Tachibana, N.Y. and G. Baym, Phys. Rev. Lett. 97 (2006) 122001.(2) N.Y., JHEP 0812 (2008) 060.(3) N.Y. and T. Kanazawa, Phys. Rev. Lett. 103 (2009) 032001.
KEK 理論センター研究会「原子核・ハドロン物理」 2009.8.11.
QCD phase diagram
T
mB
Quark-Gluon Plasma
Hadrons
RHIC/LHC
CFL
Color superconductivity
quark matter
Neutron star
Color Superconductivity
QCD at high density → asymptotic free Fermi surface
Attractive channel → Cooper instability
[3]C×[3]C=[6]C+[3]C
E
p
μ
q q
3
“diquark condensate”
“Fermi sea”
“Dirac sea”
Color-Flavor Locking (CFL)
ud s
r,g,bu,d,s
Pairing channel • s-wave pairing, spin singlet → Dirac antisymmetric• Attractive channel → color antisymmetric• Pauli principle → flavor antisymmetric• U(1)A anomaly → Lorentz scalar
3-flavor limit: Color-Flavor Locking (CFL) Alford-Rajagopal-Wilczek (NPB1999)
Gauge-invariant order parameter
e.g.)
Symmetry breaking pattern:
CFL is positive parity
... due to the presence of U(1)A anomaly.
Consider the Kobayashi-Maskawa-’t Hooft (KMT) vertex with quark mass:
VKMT is minimized when
and the positive parity state is energetically favored.
Alford-Rajagopal-Wilczek (NPB1999)
Kobayashi-Maskawa (PTP1970);‘t Hooft (PRD1976)
G G
T. Schafer (PRD2002)
Chiral symmetry breaking in CFL
The chiral condensate:
Exactly calculated thanks to the screening of instantons at high μ:
[Point]
1. Chiral symmetry is broken not only by the diquark condensate but also the chiral condensate in CFL.
2. Nonzero chiral condensate in CFL is model-independent.
3. Chiral-super interplay of the type is inevitable.
Alford-Rajagopal-Wilczek (NPB1999)
T. Schafer (PRD2002); NY (JHEP2008)
Possible phase structure I
Anomaly-induced critical point at high μ. Hatsuda-Tachibana-NY-Baym (PRL2006) A realization of quark-hadron continuity. Schafer-Wilczek (PRL1999) Critical point(s) of other origins. Kitazawa-Koide-Kunihiro-Nemoto
(PTP2002); Zhang-Fukushima-Kunihiro (PRD2009);
Zhang-Kunihiro, arXiv:0904.1062.
T
mB
Quark-Gluon Plasma
HadronsColor
superconductivity
Possible phase structure III
Is there this possibility? [see also Hidaka-san’s talk]
T
mB
Quark-Gluon Plasma
Hadrons CFLquark matter
Phase diagram of “instantons” (Nf=3)
T
mB
“instanton liquid”
“instanton molecule”
“instanton gas“
Chiral phase transition at high μ: instanton-induced crossover. 4-dim. generalization of Kosterlitz-Thouless transition.
NY (JHEP2008)
Another viewpoint: Lee-Yang zeros
The partition function zeros in the complex plane at V<∞ reflects the information of the chiral condensate at V=∞:
Nonzero chiral condensate at V=∞ requires a cut through m=0.
Halasz-Jackson-Verbaarschot (PRD97)
[Lee-Yang zeros at μ=0] Leutwyler-Smilga (PRD92)
Predictions of Random Matrix Theory (RMT)
Halasz-Jackson-Verbaarschot (PRD97); Halasz, et al. (PRD98) RMT predictions:
1. Chiral symmetry restores at μ=μc.
2. The cut will move away from origin as μ increases.
→ Is it consistent with the chiral symmetry breaking at high μ?
[Random Matrix Theory → Ohtani-san’s talk]
Finite-volume QCD at high density
QCD in a large but finite torus:
ε-regime:
Elementary excitations in CFL;• 9 quarks: mass gap~Δ due to the color superconductivity. • 8 gluons: mass gap~Δ due to the Higgs mechanism.• 8+1(+1) Nambu-Goldstone (NG) modes: nearly (or exactly) massless.
In ε-regime,• Non-NG modes negligible since . • Kinetic terms of NG modes negligible.
NY-Kanazawa (PRL2009)
Partition functions in ε-regime
Chiral Lagrangian at high μ (flavor-symmetric): Son-Stephanov (PRD2000)
Exact partition function at high μ:
a novel correspondence between hadronic phase and CFL phase
related to quark-hadron continuity!
Dirac spectrum...
at μ=0.
at high μ.
NY-Kanazawa (PRL2009)
Exact Lee-Yang zeros at high density
Asymptotic partition function and Lee-Yang zeros at μ=∞:
Chiral condensate vanishes at μ=∞. However, many Lee-Yang zeros exist near origin even at high μ
and the chiral condensate can be nonzero for μ<∞.
NY-Kanazawa (PRL2009)
1. Phases in dense QCD• The U(1)A anomaly (or instanton) plays crucial role.• Non-vanishing chiral condensate even at high μ.• Chiral-super interplay is inevitable.• Possible critical point(s) in dense QCD.
2. Partition function zeros in dense QCD• Exact X-shaped cut in the complex mass plane at μ=∞.• Chiral condensate can be nonzero for μ<∞.
3. Future problems• Phases at lower or intermediate densities?• Anomaly-induced interplay in NJL. Baym-Hatsuda-NY, in progress.
• Confinement-deconfinement transition?• Microscopic understanding based on QCD?
Summary & Outlook
Back up slides
Chiral vs. Diquark condensates
E
p
pF
-pF
Diquark condensate Chiral condensate
Y. Nambu (‘60)
Hadrons (3-flavor)
SU(3)L×SU(3)R
→ SU(3) L+R
Chiral condensate
NG bosons (π etc)
Vector mesons (ρ etc)
Baryons
Color-flavor locking
SU(3)L×SU(3)R×SU(3)C×U(1)B
→ SU(3)L+R+C
Diquark condensate
NG bosons
Gluons
Quarks
Phases
Symmetry breaking
Order parameter
Elementaryexcitations
quark-hadron continuity
Continuity between hadronic matter and quark matter (color-flavor locking)
Conjectured by Schäfer & Wilczek, PRL 1999
Instantons and chiral symmetry breaking
Why instanton? : mechanism for chiral symm. breaking/restoration
T=0 T>Tc
“instanton liquid” (metal) “instanton molecule” (insulator)
Schäfer-Shuryak, Rev. Mod. Phys. (‘97)
See, e.g., Hell-Rößner-Cristoforetti-Weise, arXiv: 0810.1099
nonlocal NJL model
Origin of NJL model:
Then, χSB in dense QCD from instantons?
Dense QCD : U(1)A is asymptotically restored.
Low-energy dynamics in dense QCD
convergent!
Low-energy effective Lagrangian of η’
Manuel-Tytgat, PL(‘00)Son-Stephanov-Zhitnitsky, PRL(‘01)Schäfer, PRD(‘02)
Coulomb gas representation
: topological charge
: 4-dim Coulomb potential
Instanton density, topological susceptibility
Witten-Veneziano relation :
Renormalization group analysis
Fluctuations :
Change of potential after RG :
RG trans. :
RG scale :
kinetic vs. potential
D = 2 : potential irrelevant → vortex molecule phase potential relevant → vortex plasma phase
D 3≧ : potential relevant → plasma phase
Phase transition induced by instantons
Unpaired instanton plasma in dense QCD
→Coexistence phase:
Actually,
System parameter α Topological excitations Order of trans.
2D O(2) spin system vortex 2nd
3D compact QED magnetic monopole crossover
4D dense QCD instanton crossover
D-dim sine-Gordon model :
Note: weak coupling QCD:
Color superconductivity at large Nc
qq scattering
qq scattering
Double-line notation
★ Diquarks are suppressed at large Nc!
Deryagin-Grigoriev-Rubakov (‘92)
Shuster-Son (‘00)
Ohnishi-Oka-Yasui (‘07)
0 ≾ mu,d<ms ∞ (realistic quark masses)≪
Realistic QCD phase structure?
2nd critical point
Critical pointAsakawa & Yazaki, 89
mu,d,s = 0 (3-flavor limit) mu,d = 0, ms=∞ (2-flavor limit)≿ ≿T
μ
T
μT
μ
Hatsuda, Tachibana, Yamamoto & Baym 06
Possible phase structure II
T
mB
Quark-Gluon Plasma
HadronsColor
superconductivity
Of course, 1st order chiral phase transition at T=0 is still possible.