department of physics, keio university › ... › 5473 › 6743 › 04_-_fukushima.pdf · color...
TRANSCRIPT
![Page 1: Department of Physics, Keio University › ... › 5473 › 6743 › 04_-_Fukushima.pdf · Color ∼O(Nc) Also diagrams ... Holographic Dual Sakai-Sugimoto model (dual to large-Nc](https://reader033.vdocuments.net/reader033/viewer/2022060402/5f0e57997e708231d43ec77d/html5/thumbnails/1.jpg)
Feb. 15 @ GSI 1
The Structure of QCD Phase Diagram
~ Facts and Fictions ~
Kenji Fukushima
Department of Physics, Keio University
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Feb. 15 @ GSI 2
Phase Diagram Candidates
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Feb. 15 @ GSI 3
Two Historical Phase Diagrams
Diagram-1982 Diagram-1983
Anomaly matching
BaymLattice
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Feb. 15 @ GSI 4
Color Superconductivity
Diagram-1999 Alford
Non-CFL includes: 2SC, dSC, uSC, etc... Crystalline SC
Chromomagnetic Instability Crystallography Gritch problem
Alford, Blaschke, Casalbuoni,KF, Huang, Kunihiro, Rajagopal,Rischke, Ruggieri, Schmitt,Shovkovy, etc...
Too difficult
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Feb. 15 @ GSI 5
Triple-Point-Like Structure
Diagram-2009
Andronic, Blaschke,Braun-Munzinger, Cleymans,KF, McLerran, Oeschler,Pisarski, Redlich, Sasaki,Satz, Stachel
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Feb. 15 @ GSI 6
Interpretation of Statistical Model
Freeze-out points are located by the particle yieldsTwo regimes in meson-dominance and baryon-dominance
Baryonic Regime
MesonicRegime
Mesonic Hagedorn Transition
Baryonic Hagedorn Transition
Z~∫ dmme−m /T
m ~em /T H
T c=T H
Z∼∫ dmρB (m)e−(mB−μB )/T
ρ(m)∼em B/T B
T c=(1−μB /mB)T B
Andronic-Blaschke-Braun-Munzinger-Cleymans-KF-McLerran-Oeschler-Pisarski-Redlich-Sasaki (2010)
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Feb. 15 @ GSI 7
Diagram-2010
KF-Hatsuda (2010)
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Feb. 15 @ GSI 8
Interweaving Chiral Spirals
Kojo-Hidaka-KF-Piarski-McLerran (2011)
Diagram-2011
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Feb. 15 @ GSI 9
Too Difficult Again
Let's get back to the basics!
Policy for simplification
If there is ANY counter-example (model or whatever), remove it from the phase diagram.
If there is NO concrete example to falsify, leave it on the phase diagram (however odd it looks).
This should be a fair and unbiased criterion
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Feb. 15 @ GSI 10
Diagram-2013
KF-Sasaki (2013)Remaining (so-far) “Facts”
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Feb. 15 @ GSI 11
Quarkyonic Matter (Regime)
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Feb. 15 @ GSI 12
Phase Diagram at Large Nc
McLerran-Pisarski (2007)
Nuclear Matter
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Feb. 15 @ GSI 13
Ordinary Nuclear Matter
Many-body problem T-matrix G-matrix...
Symmetric nuclear matterSaturation (self-binding)Exchanges of p, 2p, etc(Lattice-QCD; Aoki et al.)
Potentials in all interaction channelsincluding hyperons can be estimated from the lattice-QCD (H-dibaryons?)
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Feb. 15 @ GSI 14
Strong Baryon Interactions
One-mesonexchange
SameColor
∼O (N c)
Also diagramsinvolving gluonsto make the samecolor exchanges
Mesons~ free
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Feb. 15 @ GSI 15
Dense Nuclear Matter
HeavyBaryon
HeavyBaryon
HeavyBaryon
HeavyBaryon
HeavyBaryon
HeavyBaryon
Skyrme-Crystal
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Feb. 15 @ GSI 16
Dense Nuclear Matter
HeavyBaryon
Meson
Meson
Meson
Meson
Meson
Meson
Meson Meson
Meson
Meson
MesonMeson
Meson
Meson
Meson
HeavyBaryon
HeavyBaryon
HeavyBaryon
HeavyBaryon
HeavyBaryon
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Feb. 15 @ GSI 17
Quarkyonic Matter
HeavyBaryon
QuarkHeavyBaryon
HeavyBaryon
HeavyBaryon
HeavyBaryon
HeavyBaryon
AntiQuark
Quark
QuarkQuark
Quark
Quark
QuarkQuark Quark
Quark
Quark
Quark
Quark
AntiQuark
AntiQuark
AntiQuark
AntiQuark
AntiQuark
AntiQuark
AntiQuark Anti
Quark
AntiQuark
AntiQuark Anti
Quark
AntiQuark
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Feb. 15 @ GSI 18
Holographic Dual
Sakai-Sugimoto model (dual to large-Nc QCD)Same degrees of freedom and symmetry as QCD
D4 deconfiningDensity source from baryons than quarks
Bergman et al. (2007)
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Feb. 15 @ GSI 19
More on Holographic Dual
Ooguri-Park, Chuang-Dai-Kawamoto-Lin-Yeh (2010)
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Feb. 15 @ GSI 20
Definition: ~ Formal / Phenomenological ~
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Feb. 15 @ GSI 21
Formal Definition
A state of matter that satisfies the McLerran-Pisarski conjecture
Conjecture:
A dense system of strongly interacting baryonsbe a dual to a system of quarks
One manifestation of the “Quark-Hadron Duality”
KF-Sasaki (2013)
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Feb. 15 @ GSI 22
Quark-Hadron Dualities
Superfluid Nuclear MatterColor-Flavor-Locked State
Hadron Resonance GasQuasi-particles / PL
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Feb. 15 @ GSI 23
Similarity and Dissimilarity
Hadron resonance gas can describe thermodynamic properties (including fluctuations) up to the crossover regions.How free HRG melts into a quark-gluon plasma?
Percolations
In the quarkyonic regime baryons melt into quarks.Strong Interactions
We surely know that free HRG cannot be a right description of nuclear matter!
Mesons ~ free at large Nc
Baryons ~ O(Nc) at large Nc
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Feb. 15 @ GSI 24
Deviation from free HRG (baseline)
Critical fluctuationIf fluctuations are affected by criticality of chiral phase transition (that belongs to O(4) at zero density and Z2 at the QCD critical point), fluctuations (skewness, kurtosis, etc) should deviate from the estimate of free HRG.Strongly interacting baryonsIf interactions among particles dominate the system properties, free HRG breaks down.
Interactions in the framework of HRG
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Feb. 15 @ GSI 25
Van der Waals Corrections
V → V −∑ νi N i
μ → μ−∑ νi P i
This is not sufficient to take accountof interacting baryons
Theory needs to be established to access Quarkyonic Regime
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Ground State Structure
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Feb. 15 @ GSI 27
Charge and Spin Density Waves
Peierls Instability (Gross-Neveu model)
Overhauser Instability (Chiral Gross-Neveu model)
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Feb. 15 @ GSI 28
In-medium Confinement
Whenever a gap opens near the Fermi surface, the low-energy (smaller than the gap size) effective theory is a pure Yang-Mills theory that is a confining theory.
Color superconductor / Pion condensation Rischke-Son-Stephanov / Son-Stephanov (2000)
Inhomogeneous condensate → Gap → Confinement Dual chiral-density wave Nakano-Tatsumi / Buballa-Nickel-...
Quarkyonic chiral spiral Hidaka-Kojo-McLerran-Pisarski (2010)
Many chiral models have no critical point.Any chiral model (so far) favors inhomogeneity.
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Feb. 15 @ GSI 29
p-wave Pion Condensation
Sakai-Tatsumi et al. (2003)
p-wave pion condensation is still a likely possibility.
Determination ofLandau-Migdalparameters
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Feb. 15 @ GSI 30
Challenges at High Densities
Mechanism of DeconfinementQualitative change of major degrees of freedomDeviation from a free hadron resonance gas
Crystalline Structure of CondensatesCondensed matter physics of QCDMixed phase ~ Density fluctuationsSpiral in chiral circle / Local parity violation
Phenomena related to the Baryon NumberTopological configurations / anomaly
e.g. Chiral Magnetic Wave
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Feb. 15 @ GSI 31
Chiral Magnetic Wave
Burnier-Kharzeev-Liao-Yee (2011)
n≠0
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Feb. 15 @ GSI 32
Chiral Magnetic Wave
Burnier-Kharzeev-Liao-Yee (2011)
j5
n5>0
n5<0
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Feb. 15 @ GSI 33
Chiral Magnetic Wave
Burnier-Kharzeev-Liao-Yee (2011)
j
j
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Feb. 15 @ GSI 34
Chiral Magnetic Wave
Burnier-Kharzeev-Liao-Yee (2011)
+
+
--
(Charge) Quadratic Moment
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Chiral Magnetic Wave
STAR data presented at CPODD
v2±=v2∓
qeρ̄e
A±
A±=N̄ +− N̄ −
N̄ ++ N̄ −
So far so good... but the background?
qe: quadratic moment
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Feb. 15 @ GSI 36
Conclusion
Even without any sharp structure, the QCD phase diagram contains rich physics at high density. c.f. BEC-BCS crossover in a ultracold gas
I do not try to exclude anything.Only I did not assume anything.
Observable?Comparison with HRG / EM probes / LPV / ...
c.f. neutron star physicsBaym, Lattimer, Ozel...