4,276 research outputs found
Schwarzschild-De Sitter black holes in 4+1 dimensional bulk
We construct a static solution for 4+1 dimensional bulk such that the 3+1
dimensional world has a linear warp factor and describes the
Schwarzschild-dS_{4} black hole. For m=0 this four dimensional universe and
Friedmann Robertson Walker universe are related with an explicit coordinate
transformation. We emphasize that for linear warp factors the effect of bulk on
the brane world shows up as the dS_{4} background which is favored by the big
bang cosmology.Comment: 6 page
MGDLT5: Proceedings of the Fifth International Conference on Modern Greek Dialects and Linguistic Theory (Ghent, Belgium, September 20-22, 2012)
Accelerated Born-Infeld Metrics in Kerr-Schild Geometry
We consider Einstein Born-Infeld theory with a null fluid in Kerr-Schild
Geometry. We find accelerated charge solutions of this theory. Our solutions
reduce to the Plebanski solution when the acceleration vanishes and to the
Bonnor-Vaidya solution as the Born-Infeld parameter b goes to infinity. We also
give the explicit form of the energy flux formula due to the acceleration of
the charged sources.Comment: Latex file (12 pp
Static Cylindrical Matter Shells
Static cylindrical shells composed of massive particles arising from matching
of two different Levi-Civita space-times are studied for the shell satisfying
either isotropic or anisotropic equation of state. We find that these solutions
satisfy the energy conditions for certain ranges of the parameters.Comment: 9 pages, 3 figures, Latex; Final version, To appear in General
Relativity and Gravitatio
Closed timelike curves and geodesics of Godel-type metrics
It is shown explicitly that when the characteristic vector field that defines
a Godel-type metric is also a Killing vector, there always exist closed
timelike or null curves in spacetimes described by such a metric. For these
geometries, the geodesic curves are also shown to be characterized by a lower
dimensional Lorentz force equation for a charged point particle in the relevant
Riemannian background. Moreover, two explicit examples are given for which
timelike and null geodesics can never be closed.Comment: REVTeX 4, 12 pages, no figures; the Introduction has been rewritten,
some minor mistakes corrected, many references adde
Killing Vector Fields in Three Dimensions: A Method to Solve Massive Gravity Field Equations
Killing vector fields in three dimensions play important role in the
construction of the related spacetime geometry. In this work we show that when
a three dimensional geometry admits a Killing vector field then the Ricci
tensor of the geometry is determined in terms of the Killing vector field and
its scalars. In this way we can generate all products and covariant derivatives
at any order of the ricci tensor. Using this property we give ways of solving
the field equations of Topologically Massive Gravity (TMG) and New Massive
Gravity (NMG) introduced recently. In particular when the scalars of the
Killing vector field (timelike, spacelike and null cases) are constants then
all three dimensional symmetric tensors of the geometry, the ricci and einstein
tensors, their covariant derivatives at all orders, their products of all
orders are completely determined by the Killing vector field and the metric.
Hence the corresponding three dimensional metrics are strong candidates of
solving all higher derivative gravitational field equations in three
dimensions.Comment: 25 pages, some changes made and some references added, to be
published in Classical and Quantum Gravit
Dynamic connectivity algorithms for Monte Carlo simulations of the random-cluster model
We review Sweeny's algorithm for Monte Carlo simulations of the random
cluster model. Straightforward implementations suffer from the problem of
computational critical slowing down, where the computational effort per edge
operation scales with a power of the system size. By using a tailored dynamic
connectivity algorithm we are able to perform all operations with a
poly-logarithmic computational effort. This approach is shown to be efficient
in keeping online connectivity information and is of use for a number of
applications also beyond cluster-update simulations, for instance in monitoring
droplet shape transitions. As the handling of the relevant data structures is
non-trivial, we provide a Python module with a full implementation for future
reference.Comment: Contribution to the "XXV IUPAP Conference on Computational Physics"
proceedings; Corrected equation 3 and error in the maximal number of edge
level
Fragmentation of Fractal Random Structures
We analyze the fragmentation behavior of random clusters on the lattice under
a process where bonds between neighboring sites are successively broken.
Modeling such structures by configurations of a generalized Potts or
random-cluster model allows us to discuss a wide range of systems with fractal
properties including trees as well as dense clusters. We present exact results
for the densities of fragmenting edges and the distribution of fragment sizes
for critical clusters in two dimensions. Dynamical fragmentation with a size
cutoff leads to broad distributions of fragment sizes. The resulting power laws
are shown to encode characteristic fingerprints of the fragmented objects.Comment: Thoroughly revised version. Final version published in Physical
Review Letter
Corner contribution to cluster numbers in the Potts model
For the two-dimensional Q-state Potts model at criticality, we consider
Fortuin-Kasteleyn and spin clusters and study the average number N_Gamma of
clusters that intersect a given contour Gamma. To leading order, N_Gamma is
proportional to the length of the curve. Additionally, however, there occur
logarithmic contributions related to the corners of Gamma. These are found to
be universal and their size can be calculated employing techniques from
conformal field theory. For the Fortuin-Kasteleyn clusters relevant to the
thermal phase transition we find agreement with these predictions from
large-scale numerical simulations. For the spin clusters, on the other hand,
the cluster numbers are not found to be consistent with the values obtained by
analytic continuation, as conventionally assumed.Comment: 9 pages, 6 figure
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