lattice fermion with chiral c hemical potential
DESCRIPTION
Lattice Fermion with Chiral C hemical Potential. Arata Yamamoto (University of Tokyo). AY, Phys. Rev. Lett . 107, 031601 (2011) AY, Phys. Rev. D 84, 114504 (2011) . NTFL workshop, Feb. 17, 2012. Introduction. In lattice QCD at finite density,. “sign problem”. - PowerPoint PPT PresentationTRANSCRIPT
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Lattice Fermionwith Chiral Chemical Potential
NTFL workshop, Feb. 17, 2012
Arata Yamamoto(University of Tokyo)
AY, Phys. Rev. Lett. 107, 031601 (2011)AY, Phys. Rev. D 84, 114504 (2011)
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Introduction
“sign problem”
In lattice QCD at finite density,
For small chemical potential,
reweighting, Taylor expansion, canonical ensemble,imaginary chemical potential, density of states, …
two-color QCD, isospin chemical potential,chiral chemical potential
For large chemical potential,
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[K.Fukushima, D.E.Kharzeev, H.J.Warringa (2008)]
Chiral chemical potential
Chiral chemical potential produces a chirally imbalanced matter.
right-handedFermi sea
left-handedFermi sea
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Wilson-Dirac operator
NO sign problem !!
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Chiral Magnetic Effect[D.E.Kharzeev, L.D.McLerran, H.J.Warringa (2007)]
Early Universe
[from NASA’s web page]
[from BNL’s web page]
heavy-ion collision (RHIC&LHC)
[from KEK’s web page]
chiral magnetic effect:
charge separation induced by a strong magnetic field
via the axial anomaly, i.e., nontrivial topology
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cf.) permanent magnet ~ 102 eV2 magnetar ~ 10 MeV2
magnetic field ~ 104 MeV2
non-central collision of heavy ions
beam
beam
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magnetic field
assumption: quarks are massless and deconfined.
electric current electric current
If L = R, the net current is zero.If L R, the net current is nonzero.
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the index theorem:
Globally,
Locally,
topological fluctuation in lattice QCD [from D.Leinweber’s web
page]
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topological fluctuation
beam
magnetic field
beam
“event-by-event” charge separation
electric current
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• SU(2) quenched QCD with the overlap fermion
Chiral magnetic effect in lattice QCD
[P.V.Buividovich, M.N.Chernodub, E.V.Luschevskaya, M.I.Polikarpov (2009)]
• instanton solution & 2+1 flavor QCD with the domain-wall fermion
[M.Abramczyk, T.Blum, G.Petropoulos, R.Zhou (2009)]
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magnetic field
electric current
positive helicity
negative helicity
Chiral chemical potential
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[K.Fukushima, D.E.Kharzeev, H.J.Warringa (2008)]
the Dirac equation coupled with a background magnetic field
Induced current
magnetic field
electric current induced electric current
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Lattice QCD Simulation
full QCD simulation with a finite chiral chemical potential
external magnetic field vector current
chirally imbalanced matter L R
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• the Wilson gauge action + the Wilson fermion
action
• flavor:
• lattice size:
• lattice spacing: fm
• pion/rho-meson mass:
• deconfinement phase
Simulation setup
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Chiral charge density
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Induced current
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Induced current
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[K.Fukushima, D.E.Kharzeev, H.J.Warringa (2008)]
by fitting the lattice data
from the Dirac equation
Induced current
lattice artifacts
e.g. dielectric correction [K.Fukushima, M.Ruggieri (2010)]
e.g. renormalization
physical effects
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Systematic Analysisquenched QCD simulation
lattice spacing dependencevolume dependencequark mass dependence
of
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Renormalization
renormalization factor:
cf.) nonperturbative renormalization
[L.Maiani, G.Martinelli (1986)]
The local vector current is renormalization-group variant on the lattice.
discretization artifact:
In the continuum limit ,
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Lattice spacing
The induced current depends on the lattice spacing.
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Spatial volume Quark mass
The induced current is independent of volume and quark mass.
chiral limit
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Summary
• We have performed a lattice QCD simulation with the chiral chemical potential.
• By applying an external magnetic field, we have obtained the induced current by the chiral magnetic effect.
• The continuum extrapolation is quantitatively important.
• chiral symmetry ?