121 research outputs found
Entanglement entropy from surface terms in general relativity
Entanglement entropy in local quantum field theories is typically ultraviolet
divergent due to short distance effects in the neighbourhood of the entangling
region. In the context of gauge/gravity duality, we show that surface terms in
general relativity are able to capture this entanglement entropy. In
particular, we demonstrate that for 1+1 dimensional CFTs at finite temperature
whose gravity dual is the BTZ black hole, the Gibbons-Hawking-York term
precisely reproduces the entanglement entropy which can be computed
independently in the field theory.Comment: 6 pages 1 fig. Essay awarded honourable mention in the Gravity
Research Foundation 2013 Awards for Essays on Gravitation. v2: to appear in
IJMPD spl. issu
Fermion helicity flip by parity violating torsion
The helicity flip of a spin-1/2 Dirac fermion interacting with a torsion-
field endowed with a pseudo-tensorial extension is analysed. Taking the torsion
to be represented by a Kalb-Ramond field, we show that there is a finite
amplitude for helicity flip for massive fermions. The lowest order contribution
is proportional to the pseudo-tensor term.Comment: 5 pages, Revtex, Two figures, Title changed in the modified version.
Few discussions added.No change in the conclusion. Accepted for publication
In Physics Letters
Holographic stress tensor at finite coupling
We calculate one, two and three point functions of the holographic stress
tensor for any bulk Lagrangian of the form . Using the first law of entanglement, a simple method has
recently been proposed to compute the holographic stress tensor arising from a
higher derivative gravity dual. The stress tensor is proportional to a
dimension dependent factor which depends on the higher derivative couplings. In
this paper, we identify this proportionality constant with a B-type trace
anomaly in even dimensions for any bulk Lagrangian of the above form. This in
turn relates to , the coefficient appearing in the two point
function of stress tensors. We use a background field method to compute the two
and three point function of stress tensors for any bulk Lagrangian of the above
form in arbitrary dimensions. As an application we consider general situations
where for holographic plasmas is less than the KSS bound.Comment: v4: further typos correcte
On critical exponents without Feynman diagrams
In order to achieve a better analytic handle on the modern conformal
bootstrap program, we re-examine and extend the pioneering 1974 work of
Polyakov's, which was based on consistency between the operator product
expansion and unitarity. As in the bootstrap approach, this method does not
depend on evaluating Feynman diagrams. We show how this approach can be used to
compute the anomalous dimensions of certain operators in the model at
the Wilson-Fisher fixed point in dimensions up to .Comment: 27 pages, 1 figure, Comments added. Typos correcte
Non-classical paths in interference experiments
In a double slit interference experiment, the wave function at the screen
with both slits open is not exactly equal to the sum of the wave functions with
the slits individually open one at a time. The three scenarios represent three
different boundary conditions and as such, the superposition principle should
not be applicable. However, most well known text books in quantum mechanics
implicitly and/or explicitly use this assumption which is only approximately
true. In our present study, we have used the Feynman path integral formalism to
quantify contributions from non-classical paths in quantum interference
experiments which provide a measurable deviation from a naive application of
the superposition principle. A direct experimental demonstration for the
existence of these non-classical paths is hard. We find that contributions from
such paths can be significant and we propose simple three-slit interference
experiments to directly confirm their existence.Comment: v2: 5 pages + 3 pages supplementary, title changed, version to appear
in Physical Review Letter
Entanglement entropy in higher derivative holography
We consider holographic entanglement entropy in higher derivative gravity
theories. Recently Lewkowycz and Maldacena arXiv:1304.4926 have provided a
method to derive the equations for the entangling surface from first
principles. We use this method to compute the entangling surface in four
derivative gravity. Certain interesting differences compared to the two
derivative case are pointed out. For Gauss-Bonnet gravity, we show that in the
regime where this method is applicable, the resulting equations coincide with
proposals in the literature as well as with what follows from considerations of
the stress tensor on the entangling surface. Finally we demonstrate that the
area functional in Gauss-Bonnet holography arises as a counterterm needed to
make the Euclidean action free of power law divergences.Comment: 24 pages, 1 figure. v3: typos corrected, published versio
Analytic bootstrap at large spin
We use analytic conformal bootstrap methods to determine the anomalous
dimensions and OPE coefficients for large spin operators in general conformal
field theories in four dimensions containing a scalar operator of conformal
dimension . It is known that such theories will contain an
infinite sequence of large spin operators with twists approaching
for each integer . By considering the case where such
operators are separated by a twist gap from other operators at large spin, we
analytically determine the , dependence of the anomalous
dimensions. We find that for all , the anomalous dimensions are negative for
satisfying the unitarity bound. We further compute the first
subleading correction at large spin and show that it becomes universal for
large twist. In the limit when is large, we find exact agreement with the
AdS/CFT prediction corresponding to the Eikonal limit of a 2-2 scattering with
dominant graviton exchange.Comment: 34 pages, 4 figures. v6: JHEP versio
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