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Anomalies and Transport
Karl LandsteinerInstituto de Física Teórica, UAM-CSIC
in collaboration withI. Amado, E. Megías, L. Melgar, F. Peña-Benitez,
arXiv:1102.4577 (JHEP 1105.5006)arXiv:1103.5006 (Phys. Rev. Lett. 107 (2011) 021601)
arXiv:1107.0368 (JHEP 1109 (2011) 121 )
8th Central European Seminar on Particle Physics and QFT, Vienna, 20111Tuesday, November 22, 2011
OutlineThe Chiral Magnetic Effect
Kubo formulas I
Kubo formulas II
Hydrodynamics
Strong coupling (Holography)
Observable gravitational anomaly?
Summary
[Kharzeev, McLarren, Warringa, Nucl. Phys A803,227, arXiv:0706.1026][Fukushima, Kharzeev, Warringa, Phys. Rev. D78, 074033, arXiv:0706.1026][Kharzeev, Warringa, Phys. Rev. D80 (2009) 034028, arXiv:0907.5007]
2Tuesday, November 22, 2011
The Chiral Magnetic Effect
B+
-
[Kharzeev, McLarren, Warringa]
[parity violating currents: Vilenkin ’80, Giovannini, Shaposhnikov ’98, Alekseev, Chaianov, Frohlich ’98]
-
3Tuesday, November 22, 2011
The Chiral Magnetic Effect
B+
-
Magnetic Field
[Kharzeev, McLarren, Warringa]
[parity violating currents: Vilenkin ’80, Giovannini, Shaposhnikov ’98, Alekseev, Chaianov, Frohlich ’98]
-
3Tuesday, November 22, 2011
The Chiral Magnetic Effect
B+
-
Net chirality
Magnetic Field
[Kharzeev, McLarren, Warringa]
[parity violating currents: Vilenkin ’80, Giovannini, Shaposhnikov ’98, Alekseev, Chaianov, Frohlich ’98]
-
3Tuesday, November 22, 2011
The Chiral Magnetic Effect
B+
-
Electric current
J i =µ5
2π2Bi
Net chirality
Magnetic Field
[Kharzeev, McLarren, Warringa]
[parity violating currents: Vilenkin ’80, Giovannini, Shaposhnikov ’98, Alekseev, Chaianov, Frohlich ’98]
-
3Tuesday, November 22, 2011
The Chiral Magnetic Effect
B+
-
Electric current
J i =µ5
2π2Bi
Net chirality
Magnetic Field
P-odd charge separation
[Kharzeev, McLarren, Warringa]
[parity violating currents: Vilenkin ’80, Giovannini, Shaposhnikov ’98, Alekseev, Chaianov, Frohlich ’98]
-
3Tuesday, November 22, 2011
Kubo formulas IChiral magnetic conductivity
Kubo formula, general symmetry group
[Kharzeev, Warringa]�J = σ �B
σAB = limpj→0
�
i,k
i
2pj�ijk�JA
i JBk �
����ω=0
4Tuesday, November 22, 2011
Kubo formulas I chiral fermions
chemical potentials and Cartan generators
1-loop calculation
[Newman, Son], [Newman]5Tuesday, November 22, 2011
Kubo formulas I chiral fermions
chemical potentials and Cartan generators
1-loop calculationAnomalycoeff
[Newman, Son], [Newman]5Tuesday, November 22, 2011
Kubo formulas I
∼ dABC
TA
TB TC
AμA pure gauge
AνB AρC
6Tuesday, November 22, 2011
Kubo formulas IIfinite density: charge transport => energy transport
energy flux sourced by magnetic fields
at ω=0 reverse order of operators
7Tuesday, November 22, 2011
Kubo formulas IIfinite density: charge transport => energy transport
energy flux sourced by magnetic fields
at ω=0 reverse order of operators
conductivity ?7Tuesday, November 22, 2011
Tμν sourced by metric
Ag “gravitomagnetic field” -> chiral gravitomagnetic effect
chiral vortical effect: fluid velocities
Kubo formulas II
8Tuesday, November 22, 2011
Kubo formulas IIas before: general symmetry group
9Tuesday, November 22, 2011
Kubo formulas IIas before: general symmetry group
Integration constantgravitational anomaly!
9Tuesday, November 22, 2011
Kubo formulas II
∼ tr (TA)TA
gμν gλρ
AμA pure gauge
10Tuesday, November 22, 2011
Anomalies
11Tuesday, November 22, 2011
Jµ = nuµ + σPµν∂ν� µ
T
�uλ + νµ
Hydrodynamicsalso energy flux
hydrodynamics:
[Son,Surowka], [Eling, Neiman, Oz], [Erdmenger, Haack, Kaminski, Yarom], [Banerjee, Bhattacharya, Bahattacharya, Dutta Loganayagam, Surowka], [Loganayagam] [Kharzeev, Yee] [Sadovyev, Isachenkov, Zakharov]
limpj→0
i
2pj
�
i,k
�ijk �T0iT0k�|ω=0 �= 0
Tµν = (�+ P )uµuν + Pgµν + ησµν + ζPµν∂λuλ +Qµuν +Qνuµ
12Tuesday, November 22, 2011
anomalous contributions
Jµ = nuµ + σPµν∂ν� µ
T
�uλ + νµ
Hydrodynamicsalso energy flux
hydrodynamics:
[Son,Surowka], [Eling, Neiman, Oz], [Erdmenger, Haack, Kaminski, Yarom], [Banerjee, Bhattacharya, Bahattacharya, Dutta Loganayagam, Surowka], [Loganayagam] [Kharzeev, Yee] [Sadovyev, Isachenkov, Zakharov]
limpj→0
i
2pj
�
i,k
�ijk �T0iT0k�|ω=0 �= 0
Tµν = (�+ P )uµuν + Pgµν + ησµν + ζPµν∂λuλ +Qµuν +Qνuµ
12Tuesday, November 22, 2011
νµA = σBABBB,µ + σV
Aωµ
Qµ = ρBABA,µ + ρVAωµ
BA,µ =1
2�µνρλuνFA
ρλ
ωµ = �µνρλuν∂ρuλ
σBAB =
1
4π2dABCµ
C
σVA = ρBA =
1
8π2dABCµ
BµC +T 2
24bA
ρV =1
12π2dABCµ
AµBµC +T 2
12bAµ
A
Hydrodynamics
13Tuesday, November 22, 2011
Holographymixed gauge gravitational Chern Simons term
current
on-shell we recover the anomaly
[H.U. Yee], [Gynther, KL,Pena-Benitez, Rebhan] [Kalayhdzian, Kirsch], [Gorski, Zayakin]
14Tuesday, November 22, 2011
HolographyKubo formulas: fluctuations
background: charged AdS black hole
correlators are
coeffs consistent with weak coupling
no T^3 terms !
�JJ� = −ipz� κ
2πGµ− κ
6πGβ�
15Tuesday, November 22, 2011
T 0i =µ5
6T 2ωi
J i5 =
�µ2 + µ2
5
4π2+
T 2
6
�ωi
Observe grav. Anomaly?
[Karen-Zur, Oz]
ωi
Enhanced Ω_ Production
Better Observable? Energy!
Eup > Edown
measurable effect?
16Tuesday, November 22, 2011
SummaryAnomalies -> parity violating transport
Magnetic fields or vortices
We have derived Kubo formulas
(non)-renormalizaton
Surprise: mixed gauge gravitational anomaly contributes
Hydrodynamics and derivative expansion? (fluid/gravity)
Holography with gravitational CS term
Observable effects? [Karen-Zur, Oz], [Kharzeev, Son], [Kharzeev, Yee]
[Oz, Neiman], [Son], [Kharzeev, Yee], [Loganayagam]
17Tuesday, November 22, 2011