hawking radiations and anomalies
DESCRIPTION
Hawking Radiations and Anomalies. Satoshi Iso (KEK) based on collaborations while I was staying at MIT(05/03-06/01) with Hiroshi Umetsu (OIQP) and Frank Wilczek (MIT) hep-th/0602146 hep-th/0603???. [1] Introduction. Hawking radiation is the most prominent quantum effect - PowerPoint PPT PresentationTRANSCRIPT
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Hawking Radiations and Anomalies
Satoshi Iso (KEK)
based on collaborations
while I was staying at MIT(05/03-06/01)
with Hiroshi Umetsu (OIQP) and Frank Wilczek (MIT)
hep-th/0602146
hep-th/0603???
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Hawking radiation is the most prominent quantum effectto arise for quantum fields in a background space-time with an event horizon. Hawking (1975) : calculate Bogoliubov coefficients for particle creations between in- and out- states in a collapsing star.
[1] Introduction
(1) Vacuum in curved backgrounds is not unique.
a(n)|vac> =0 How can we identify annihilation ops.?
(2) Only outgoing modes come out of the horizon. Ingoing modes are decoupled from the exterior world. decoherence(thermal distribution)
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BH
Basic facts about black holes
M(mass) Q(charge) a (angular mom.)
Schwarzshild (Q=a=0)Reissner-Nordstrom (with Q)Kerr (with a)Kerr-Newman (with Q and a)
Schwarzshild
r
t=Schwartshild time
r=2M
light cone at each radius
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Kruskal coordinates U,V : regular coordinates around horizon
where
r=const
tr=0
r=0
II: BH
IV: WH
I: exterior region
U V
III
U=0, V=0 at horizon
U=0 future horizonV=0 past horizon
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Horizon is not a singular point but a null hypersurface. No information comes out of the horizon.
Physical picture of Hawking radiation
BH
××
virtual pair creationof particles
E-E
××-E E
Hawking radiation
real pair creation
Hawking temperature
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Various derivations of Hawking radiation
(1)Hawking (1975) calculate Bogoliubov coefficinents Unruh (1976) B.coeff. in eternal BH, Unruh effect
(2) Euclidean method (Gibbons Hawking 1977)
Periodicity of the metric along the imaginary time direction=KMS condition
(4) Christensen Fulling (1977)
(3) Tunneling (Parikh Wilczek 2000)
calculate WKB amplitude for classically forbidden trajectories
Obtain each component of EM tensor in Schwarzshild BHusing conformal anomalies.
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Christensen Fulling method in d=2
Symmetries (stationary, rotational inv.) Conservation law of EM tensor
where
Then we need to determine 2 constants K, Q.
Trace of EM tensor is known from trace anomaly.
restrict the form of EM tensor as
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Determination of K and Q Impose 2 conditions
(1) regularity at future horizon
EM tensor should be regular at future horizon. Q=0
(2) No ingoing flux at r → ∞
Typical form of EM for radiation from blackbody with temp. T is
Hence K can be determined by asymptotic form of H2(r).
Flux of Hawking radiation
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92 constants K, Q and 2 functions trace(r), Θ(r)
D=4 case is more complicated and we can not determine all the components.
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Determination of Hawking flux in d=4 needs non-universal function Θ(r).
Hawking radiation is a universal phenomena and the Hawking flux should be determined only by a few macroscopic parameter of BH.
Furthermore, it is much more complicated to extend the treatmentto Reissner-Nordstrom or Kerr BH.
Instead of conformal anomaly, we will use gauge or gravitational anomalies to determine the Hawking flux.
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Plan of the talk
[2] Basic idea
[3] Reissner-Nordstrom black hole
[4] Kerr or Kerr-Newman black hole
[5] Effective action approach to Hawking radiation
[5] Summary and Discussions
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[2] Basic idea
r=0
r=0
BH
(1)Near horizon, each partial wave of d-dim quantum field behaves as d=2 massless free field.
Quantum fields in black holes.
Outgoing modes = right moving Ingoing modes = left moving
Effectively 2-dim conformal fields
(different from Robinson-Wilczek 2005)
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(2) Ingoing modes are decoupled once they are inside the horizon.
These modes are classically irrelevant for the physics in exterior region.
So we first neglect ingoing modes near the horizon.
The effective theory becomes chiral in the two-dimensional sense.
gauge and gravitational anomalies = breakdown of gauge and general coordinate invariance
(3) But the underlying theory is NOT anomalous.
Anomalies must be cancelled by quantum effects of the classically irrelevant ingoing modes. ( ~ Wess-Zumino term)
flux of Hawking radiation
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Analogy with anomaly inflow mechanism
Quantum Halldroplet
Chern-Simons term for gauge potential is induced in the bulk.
Gauge symmetry will be broken at the boundary.
Chiral edge currents along the boundary rescue the gauge invariance.
chiral edgecurrent
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[3] Hawking radiation from charged black holes via gauge and gravitational anomalies
Metric and gauge potential of charged black hole (Reissner-Nordstrom)
Charged fields in RN BH. Partial wave decomposition
Each partial wave behaves as a d=2 free massless field.
Infinite set of d=2 quantum fields
IUWhep-th/0602146
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Note that
(1)The effective d=2 current or EM tensor are given by integrating d-dimensional ones over (d-2)-sphere.
(2) The effective 2-dim theory contains a dilaton background in addition to the d=2 metric.
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Hawking radiation from RN BH.
Planck distribution with a chemical potential
for fermoins
Fluxes of current and EM tensor are given by
e: charge of radiated particlesQ: charge of BH
( Extremal BH radiates charged particles~ Schwinger mechnism )
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Gauge current and gauge anomaly
horizon
ε
If we neglect ingoing modes in region H the theory becomes chiral there.
Gauge current has anomaly in region H.
consistent current
We can define a covariant current by
which satisfies
OH
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In region O,
In near horizon region H,
are integration constants.
Current is written as a sum of two regions.
where
= current at infinity
= value of consistent current at horizon
consistent current
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Variation of the effective action under gauge tr.
Using anomaly eq.
=0
impose
cancelled by WZ term
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・ Determination of
We assume that the covariant current to vanish at horizon.
Unruh vac.
Reproduces the correct Hawking flux
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EM tensor and Gravitational anomaly
Under diffeo. they transform
Effective d=2 theory contains background of graviton, gauge potential and dilaton.
Ward id. for the partition function
=anomaly
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Gravitational anomaly
consistent current
covariant current
In the presence of gauge and gravitational anomaly, Ward id. becomes
non-universal
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Solve component of Ward.id.
(1) In region O
(2) In region H
Using
(near horizon)
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Variation of effective action under diffeo.
(1) classical effect of background electric field
(1) (2) (3)
(2) cancelled by induced WZ term of ingoing modes
(3) Coefficient must vanish.
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Determination of
We assume that the covariant current to vanish at horizon.
since
we can determine
and therefore flux at infinity is given by
Reproduces the flux of Hawking radiation
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[4] Rotating black holes
Basic ideaKerr=axial symmetric
isometry
U(1) gauge symmetryin d=2
diffeo in axial direction
KK
partial wavewith m
charge m
a part of metric background electric field
(IUW, to appear)
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Kerr black hole
scalar field in Kerr geometry
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Near horizon, each partial wave is decoupled and can be treated as free massless d=2 field.
dilaton
metric
gauge potential
U(1) charge of is m.
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Results
Flux of angular momentum
Flux of energy
where(angular velocity at horizon)
These results are consistent with those for Hawking radiation.
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[5] Effective action approach to Hawking radiation (IU, to appear)
Quantum fields in BH background can be described by d=2 conformal fields near horizon.
For free d=2 free fields, we can calclate the effective actionof quantum fields in black hole background.
EM tensor or current can be explicitly obtained.
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Effective action of charged fields in electric and gravitational bkg.
gravity
gauge
The induced EM tensor and current are given by
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where
We need to impose boundary condition for
(Leutwyler 85)
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Boundary condition (for Unruh vacuum)
(1) Physical quantities must be regular at the future horizon.(2) There are no ingoing fluxes at infinity.
RN BH
tortoise coordinate
conformal metric
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・ U(1) gauge current in RN BH
B satisfies
It can be solved as
where
constant
hence
or
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Boundary condition
(1)Current is regular at future horizon in Kruskal coordinate
Metric is regular at outer horizon
regularity of JU at horizon imposes Since
(2) Ingoing current vanish at infinity
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Hence U(1) current is completely determined
Flux of U(1) charge
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Similarly EM tensor can be also determined.
Boundary conditions
EM tensor can be fully determined and the flux becomes
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[6] Summary and Discussions
(1) Hawking flux can be universally determined by demanding cancellation of gauge or gravitational anomalies at horizon.
Hawking radiation is a quantum effect to arise forquantum field in a background space-time with event-horizon.
quantum effect of classicallyirrelevant ingoing modes at horizon.(though anomaly)
outgoing
ingoing
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(2) The treatment can be applied to any type of black holes.
i.e. Schwarzshild Reissner-Nordstrom Kerr Kerr-Newman
Nonabelian gauge field?
(3) Planck distribution ?
(We have neglected the effect of grey body factor.)
anomaly for each frequency ?
RG analysis near horizon ?
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(4) Entropy of BH and Membrane paradigm
Horizon constraints entropy of BH as diffeo on horizon keeping the constraint
Quantum effect of ingoing modes
effective modes at horizon
cf. Carlip