203,722 research outputs found
Scalable explicit implementation of anisotropic diffusion with Runge-Kutta-Legendre super-time-stepping
An important ingredient in numerical modelling of high temperature magnetised
astrophysical plasmas is the anisotropic transport of heat along magnetic field
lines from higher to lower temperatures.Magnetohydrodynamics (MHD) typically
involves solving the hyperbolic set of conservation equations along with the
induction equation. Incorporating anisotropic thermal conduction requires to
also treat parabolic terms arising from the diffusion operator. An explicit
treatment of parabolic terms will considerably reduce the simulation time step
due to its dependence on the square of the grid resolution () for
stability. Although an implicit scheme relaxes the constraint on stability, it
is difficult to distribute efficiently on a parallel architecture. Treating
parabolic terms with accelerated super-time stepping (STS) methods has been
discussed in literature but these methods suffer from poor accuracy (first
order in time) and also have difficult-to-choose tuneable stability parameters.
In this work we highlight a second order (in time) Runge Kutta Legendre (RKL)
scheme (first described by Meyer et. al. 2012) that is robust, fast and
accurate in treating parabolic terms alongside the hyperbolic conversation
laws. We demonstrate its superiority over the first order super time stepping
schemes with standard tests and astrophysical applications. We also show that
explicit conduction is particularly robust in handling saturated thermal
conduction. Parallel scaling of explicit conduction using RKL scheme is
demonstrated up to more than processors.Comment: 15 pages, 9 figures, incorporated comments from the referee. This
version is now accepted for publication in MNRA
Modification of Angular Velocity by Inhomogeneous MRI Growth in Protoplanetary Disks
We have investigated evolution of magneto-rotational instability (MRI) in
protoplanetary disks that have radially non-uniform magnetic field such that
stable and unstable regions coexist initially, and found that a zone in which
the disk gas rotates with a super-Keplerian velocity emerges as a result of the
non-uniformly growing MRI turbulence. We have carried out two-dimensional
resistive MHD simulations with a shearing box model. We found that if the
spatially averaged magnetic Reynolds number, which is determined by widths of
the stable and unstable regions in the initial conditions and values of the
resistivity, is smaller than unity, the original Keplerian shear flow is
transformed to the quasi-steady flow such that more flattened (rigid-rotation
in extreme cases) velocity profile emerges locally and the outer part of the
profile tends to be super-Keplerian. Angular momentum and mass transfer due to
temporally generated MRI turbulence in the initially unstable region is
responsible for the transformation. In the local super-Keplerian region,
migrations due to aerodynamic gas drag and tidal interaction with disk gas are
reversed. The simulation setting corresponds to the regions near the outer and
inner edges of a global MRI dead zone in a disk. Therefore, the outer edge of
dead zone, as well as the inner edge, would be a favorable site to accumulate
dust particles to form planetesimals and retain planetary embryos against type
I migration.Comment: 28 pages, 11figures, 1 table, accepted by Ap
Sparse non-negative super-resolution -- simplified and stabilised
The convolution of a discrete measure, , with
a local window function, , is a common model for a measurement
device whose resolution is substantially lower than that of the objects being
observed. Super-resolution concerns localising the point sources
with an accuracy beyond the essential support of
, typically from samples , where indicates an inexactness in the sample
value. We consider the setting of being non-negative and seek to
characterise all non-negative measures approximately consistent with the
samples. We first show that is the unique non-negative measure consistent
with the samples provided the samples are exact, i.e. ,
samples are available, and generates a Chebyshev system. This is
independent of how close the sample locations are and {\em does not rely on any
regulariser beyond non-negativity}; as such, it extends and clarifies the work
by Schiebinger et al. and De Castro et al., who achieve the same results but
require a total variation regulariser, which we show is unnecessary.
Moreover, we characterise non-negative solutions consistent with
the samples within the bound . Any such
non-negative measure is within of the discrete
measure generating the samples in the generalised Wasserstein distance,
converging to one another as approaches zero. We also show how to make
these general results, for windows that form a Chebyshev system, precise for
the case of being a Gaussian window. The main innovation of these
results is that non-negativity alone is sufficient to localise point sources
beyond the essential sensor resolution.Comment: 59 pages, 7 figure
Renormalization Group Flows from Gravity in Anti-de Sitter Space versus Black Hole No-Hair Theorems
Black hole no-hair theorems are proven using inequalities that govern the
radial dependence of spherically symmetric configurations of matter fields. In
this paper, we analyze the analogous inequalities for geometries dual to
renormalization group flows via the AdS/CFT correspondence. These inequalities
give much useful information about the qualitative properties of such flows.
For Poincare invariant flows, we show that generic flows of relevant or
irrelevant operators lead to singular geometries. For the case of irrelevant
operators, this leads to an apparent conflict with Polchinski's decoupling
theorem, and we offer two possible resolutions to this problem.Comment: 13 pages, 3 figures, harvmac, epsf, references and comments adde
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