7,475 research outputs found
The Newtonian potential of thin disks
The one-dimensional, ordinary differential equation (ODE) by Hur\'e & Hersant
(2007) that satisfies the midplane gravitational potential of truncated, flat
power-law disks is extended to the whole physical space. It is shown that
thickness effects (i.e. non-flatness) can be easily accounted for by
implementing an appropriate "softening length" . The solution of this
"softened ODE" has the following properties: i) it is regular at the edges
(finite radial accelerations), ii) it possesses the correct long-range
properties, iii) it matches the Newtonian potential of a geometrically thin
disk very well, and iv) it tends continuously to the flat disk solution in the
limit . As illustrated by many examples, the ODE,
subject to exact Dirichlet conditions, can be solved numerically with
efficiency for any given colatitude at second-order from center to infinity
using radial mapping. This approach is therefore particularly well-suited to
generating grids of gravitational forces in order to study particles moving
under the field of a gravitating disk as found in various contexts (active
nuclei, stellar systems, young stellar objects). Extension to non-power-law
surface density profiles is straightforward through superposition. Grids can be
produced upon request.Comment: Accepted for publication in A&
A substitute for the singular Green kernel in the Newtonian potential of celestial bodies
The "point mass singularity" inherent in Newton's law for gravitation
represents a major difficulty in accurately determining the potential and
forces inside continuous bodies. Here we report a simple and efficient
analytical method to bypass the singular Green kernel 1/|r-r'| inside the
source without altering the nature of the interaction. We build an equivalent
kernel made up of a "cool kernel", which is fully regular (and contains the
long-range -GM/r asymptotic behavior), and the gradient of a "hyperkernel",
which is also regular. Compared to the initial kernel, these two components are
easily integrated over the source volume using standard numerical techniques.
The demonstration is presented for three-dimensional distributions in
cylindrical coordinates, which are well-suited to describing rotating bodies
(stars, discs, asteroids, etc.) as commonly found in the Universe. An example
of implementation is given. The case of axial symmetry is treated in detail,
and the accuracy is checked by considering an exact potential/surface density
pair corresponding to a flat circular disc. This framework provides new tools
to keep or even improve the physical realism of models and simulations of
self-gravitating systems, and represents, for some of them, a conclusive
alternative to softened gravity.Comment: Accepted for publication in A&A; 7 pages, color figure
A Lifshitz Black Hole in Four Dimensional R^2 Gravity
We consider a higher derivative gravity theory in four dimensions with a
negative cosmological constant and show that vacuum solutions of both Lifshitz
type and Schr\"{o}dinger type with arbitrary dynamical exponent z exist in this
system. Then we find an analytic black hole solution which asymptotes to the
vacuum Lifshitz solution with z=3/2 at a specific value of the coupling
constant. We analyze the thermodynamic behavior of this black hole and find
that the black hole has zero entropy while non-zero temperature, which is very
similar to the case of BTZ black holes in new massive gravity at a specific
coupling. In addition, we find that the three dimensional Lifshitz black hole
recently found by E. Ayon-Beato et al. has a negative entropy and mass when the
Newton constant is taken to be positive.Comment: 11 pages, no figure; v2, a minor error correcte
Non-relativistic metrics from back-reacting fermions
It has recently been pointed out that under certain circumstances the
back-reaction of charged, massive Dirac fermions causes important modifications
to AdS_2 spacetimes arising as the near horizon geometry of extremal black
holes. In a WKB approximation, the modified geometry becomes a non-relativistic
Lifshitz spacetime. In three dimensions, it is known that integrating out
charged, massive fermions gives rise to gravitational and Maxwell Chern-Simons
terms. We show that Schrodinger (warped AdS_3) spacetimes exist as solutions to
a gravitational and Maxwell Chern-Simons theory with a cosmological constant.
Motivated by this, we look for warped AdS_3 or Schrodinger metrics as exact
solutions to a fully back-reacted theory containing Dirac fermions in three and
four dimensions. We work out the dynamical exponent in terms of the fermion
mass and generalize this result to arbitrary dimensions.Comment: 26 pages, v2: typos corrected, references added, minor change
Asymptotic behaviour of a semilinear elliptic system with a large exponent
Consider the problem \begin{eqnarray*} -\Delta u &=& v^{\frac 2{N-2}},\quad
v>0\quad {in}\quad \Omega, -\Delta v &=& u^{p},\:\:\:\quad u>0\quad {in}\quad
\Omega, u&=&v\:\:=\:\:0 \quad {on}\quad \partial \Omega, \end{eqnarray*} where
is a bounded convex domain in with smooth boundary
We study the asymptotic behaviour of the least energy
solutions of this system as We show that the solution remain
bounded for large and have one or two peaks away form the boundary. When
one peak occurs we characterize its location.Comment: 16 pages, submmited for publicatio
Topologically Massive Gravity and Ricci-Cotton Flow
We consider Topologically Massive Gravity (TMG), which is three dimensional
general relativity with a cosmological constant and a gravitational
Chern-Simons term. When the cosmological constant is negative the theory has
two potential vacuum solutions: Anti-de Sitter space and Warped Anti-de Sitter
space. The theory also contains a massive graviton state which renders these
solutions unstable for certain values of the parameters and boundary
conditions. We study the decay of these solutions due to the condensation of
the massive graviton mode using Ricci-Cotton flow, which is the appropriate
generalization of Ricci flow to TMG. When the Chern-Simons coupling is small
the AdS solution flows to warped AdS by the condensation of the massive
graviton mode. When the coupling is large the situation is reversed, and warped
AdS flows to AdS. Minisuperspace models are constructed where these flows are
studied explicitly
Wide Field Photometry of the Galactic Globular Cluster M22
We present wide field photometry of the Galactic Globular Cluster M~22 in the
B, V and I passbands for more than 186,000 stars. The study is complemented by
the photometry in two narrowband filters centered on H and the
adjacent continuum, and by infrared J, H and K magnitudes derived from the 2
MASS survey for 2000 stars. Profiting from this huge database, we
completely characterized the evolved stellar sequences of the cluster by
determining a variety of photometric parameters, including new photometric
estimates of the mean metallicity, reddening and distance to the cluster. In
particular, from our multi-wavelength analysis, we re-examined the
long-standing metallicity spread problem in M~22. According to our dataset, we
conclude that most of the observed width of the red giant branch must be due to
differential reddening, which amounts to a maximum of , although the presence of a small metallicity spread cannot
be completely ruled out. More specifically, the maximum metallicity spread
allowed by our data is of the order of [Fe/H] dex,
i.e., not much more than what allowed by the photometric errors. Finally, we
identified most of the known variable stars and peculiar objects in our field
of view. In particular, we find additional evidence supporting previous optical
identifications of the central star of the Planetary Nebula IRAS 18333-2357,
which is associated with M~22.Comment: 15 pages, 16 figures, accepted for publication in MNRA
Maximal parabolic regularity for divergence operators including mixed boundary conditions
We show that elliptic second order operators of divergence type fulfill
maximal parabolic regularity on distribution spaces, even if the underlying
domain is highly non-smooth, the coefficients of are discontinuous and
is complemented with mixed boundary conditions. Applications to quasilinear
parabolic equations with non-smooth data are presented.Comment: 39 pages, 4 postscript figure
A boundary stress tensor for higher-derivative gravity in AdS and Lifshitz backgrounds
We investigate the Brown-York stress tensor for curvature-squared theories.
This requires a generalized Gibbons-Hawking term in order to establish a
well-posed variational principle, which is achieved in a universal way by
reducing the number of derivatives through the introduction of an auxiliary
tensor field. We examine the boundary stress tensor thus defined for the
special case of `massive gravity' in three dimensions, which augments the
Einstein-Hilbert term by a particular curvature-squared term. It is shown that
one obtains finite results for physical parameters on AdS upon adding a
`boundary cosmological constant' as a counterterm, which vanishes at the
so-called chiral point. We derive known and new results, like the value of the
central charges or the mass of black hole solutions, thereby confirming our
prescription for the computation of the stress tensor. Finally, we inspect
recently constructed Lifshitz vacua and a new black hole solution that is
asymptotically Lifshitz, and we propose a novel and covariant counterterm for
this case.Comment: 25 pages, 1 figure; v2: minor corrections, references added, to
appear in JHE
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