

A stable gravitational collapse code is constructed under
the assumption of axisymmetry in an effort to study black
hole critical collapse of various matter sources. A unigrid,
Crank-Nicholson scheme is implemented with a multigrid
elliptic solver to evolve a scalar field along with electric
and magnetic fields. Stable and convergent evolutions for
weak and strong field are found. For the strong field
regime, black hole excision succeeds in yielding
long-lasting, stable evolutions in the presence of a black
hole. Studies of the threshold of black hole formation
(critical phenomena) await the implementation of adaptive
mesh refinement (AMR).
[B13.002] Relativistic Hydrodynamics with AMR
Orhan Donmez, Joan Centrella (Drexel University and NASA/Goddard Space Flight Center)
Modeling astrophysical sources of gravitational radiation
requires fully 3-D numerical simulations. Due to the range
of scales involved, adaptive mesh refinement (AMR) is a
critical component for successful modeling. We present a
progress report on the development of a fully general
relativistic hydrodynamics code for modeling such sources.
Results from 3-D runs involving shocks using AMR will be
shown.
[B13.003] Three-dimensional Adaptive Evolutions of Strong Gravitational Waves
Dae-Il Choi, Joan Centrella (Drexel University and NASA/Goddard Space Flight Center)
General relativistic research is entering a new era with the installation of several worldwide gravitational wave (GW) observatories based on laser interferometers. These include ground-based detectors such as LIGO, VIRGO, GEO, and TAMA and a space-based detector LISA.
Theoretical challenges for numerical relativists include calculating accurate waveforms generated by the sources likely to be detected by these GW observatories. These waveforms will greatly enhance the successful detection and interpretation of the signals.
The final goal of our research program is to calculate waveforms for one such candidate--inspiralling binary neutron star system. The full Einstein equations in 3-D must be solved to follow both the dynamics of the binaries from initial inspiral to final merger, and the generation and propagation of gravitational waves into the wave zone.
One of the crucial requirements for this kind of simulation
is AMR (Adaptive Mesh Refinement). My talk is based on
work-in-progress that solves the vacuum Einstein equations
with strong gravitational waves as initial data. This
problem constitutes a first step towards full simulations
and allows us to test our AMR code without involving the
complexity of hydrodynamics. 2-level AMR runs show that the
fine grid tracks the features of the gravitational waves
well.
[B13.004] Isolated horizons in numerical relativity
Olaf Dreyer, Badri Krishnan, Eric Schnetter, Deirdre Shoemaker (Center for Gravitational Physics and Geometry, Pennsylvania State University)
The notion of isolated horizons was recently introduced to
describe the near horizon geometry of a black hole. We use
this framework to extract invariant physical information
from the numerical simulations of black hole collisions. In
particular we calculate the mass and angular momentum only
using quantities intrinsic to the horizon. To extract this
physical information, we do not need to embed the spacetime
in a Kerr solution. This is a significant advantage because
one does not know what Kerr parameters to use or how the
physical geometry is to approach Kerr.
[B13.005] Generic T^2 Symmetric Cosmologies: A Precision Numerical Laboratory for Local Mixmaster Dynamics
Beverly K. Berger (Oakland U.), James Isenberg (U. of Oregon), Marsha Weaver (AEI)
Unlike the velocity dominated special case of vacuum Gowdy cosmological spacetimes, generic T^2 symmetric (twisted Gowdy) models appear to exhibit local mixmaster dynamics (LMD) (of an unusual type). Numerical simulations of these models are sufficiently accurate to allow precise comparison between predicted quantitative signatures of LMD and the actual behavior of the solutions. Implications for more general cosmological spacetimes will be discussed.
[B13.006] Adaptive Mesh Refinement for Collapsing Cosmological Spacetimes
Zackery Belanger, Beverly K. Berger (Oakland U.), Milo Dorr, Xabier Garaizar (LLNL)
Gravitational wave amplitudes in collapsing cosmological spacetimes are characterized by narrowing spiky features which challenge any fixed spatial resolution computer simulation. This points to the possible usefulness of adaptive mesh refinement (AMR). Using Godunov's method in combination with the Structured Adaptive Mesh Refinement Algorithm Infrastructure (SAMRAI) of Lawrence Livermore National Laboratory, a fully-functional code using AMR has been developed and applied to the collapse of twisted Gowdy cosmologies to explore their local mixmaster dynamics.
[B13.007] Numerical simulation of generic singularities
David Garfinkle (Oakland University)
This talk is on a numerical simulation of the approach to
the singularity with a scalar field as the matter. The
simulation is done using a 3+1 code that uses harmonic
coordinates. The asymptotic behavior of the metric is found.
Since the metric has no symmetries, it is expected that the
behavior found is the generic behavior of singularities with
this type of matter.
[B13.008] Numerical evolution of constant mean curvature foliations of single black hole spacetimes
Pablo Laguna (Penn State University), Adrian Gentle, Warner Miller (Los Alamos National Laboratory), Deirdre Shoemaker (Penn State University)
We investigate the convergence and long-term stability
properties of numerical evolutions of single black holes
spacetimes using time independent foliations constructed
from hypersurfaces of constant mean curvature. We focus our
attention on foliations that are asymptotic to future null
infinity because of their potential to facilitate radiation
extraction in more complicated settings. We consider both,
foliations with and without singularity avoidance
properties. We discuss the extension and possible advantages
of these foliations in the numerical evolutions of multiple
black holes systems.
[B13.009] Solving the Constraint Equations of General Relativity
Harald P. Pfeiffer, Lawrence E. Kidder, Mark A. Scheel, Saul A. Teukolsky (Cornell University), Gregory B. Cook (Wake Forest University)
Posing initial data for general relativity requires solving
the so-called constraint equations, a set of coupled partial
differential equations. Work towards a new solver for these
constraint equations is presented. The new code is based on
the pseudospectral collocation method. Ultimately it will
solve the full coupled initial data equations with no
simplifying assumptions.
[B13.010] Numerical Simulations of Black Holes with Excision
Deirdre Shoemaker, Gioel Calabrese, David Garrison, Bernard Kelly, Pablo Laguna, Keith Lockitch, Jorge Pullin, Kenneth Smith, Manuel Tiglio (Penn State University)
We present results from numerical simulations of single
black holes in three dimensions using the Maya code. We
focus on how to numerically solve the Einstein's field
equations in three dimensions written in an ADM like system
including the ramifications that the equations and gauge
choice have on numerical stability. One of the key
ingredients in simulating a black hole in a long term stable
manner is excising the black hole's singularity. Two of the
design features of the Maya code are flexibility and
readability. These features are exploited in our excision
algorithm design. This talk includes a discussion of the
excision scheme accompanied by results from numerically
solving the ADM equations for a black hole while excising
the singularity.
[B13.011] Gravitation, Symmetry and Undergraduates
Jamie Jorgensen (Utah State University), Formal Geometry and Mathematical Physics Team
This talk will discuss "Project Petrov" Which is designed to
investigate gravitational fields with symmetry. Project
Petrov represents a collaboration involving physicists,
mathematicians as well as graduate and undergraduate math
and physics students. An overview of Project Petrov will be
given, with an emphasis on students' contributions,
including software to classify and generate Lie algebras, to
classify isometry groups, and to compute the isometry group
of a given metric.
[B13.012] Internal-structure dependent coefficients in the post-Newtonian equations of motion
Eanna Flanagan (Cornell University)
The post-3-Newtonian equation of motion for "point
particles" recently derived by Damour, Jaranowski and
Schafer and by Blanchet and Faye contains a term whose
numerical coefficient has not yet been determined by the
methods used to date to derive the equations of motion. One
might speculate that the coefficient depends on the internal
structure of the bodies, so that, for example, it would have
different values for polytropic stellar models with
different polytropic indices. We show here that this is not
the case -- the coefficient must take the same value for all
spherically symmetric bodies -- and that such
internal-structure dependent coefficients cannot arise at
orders below the 5th post Newtonian order. The argument is
based on an earlier, matched asymptotic expansion based
analysis of the interaction of the orbital motion and
internal degrees of freedom in binary stellar systems.
[B13.013] Fast travel in spherically symmetric geometries
Belkis Cabrera Palmer, Donald Marolf (Syracuse University)
We investigate spherically symmetric configurations that
allow the fastest possible travel between two spatial
points. The end points are chosen unambiguously by fixing
the metric to be "Schwarzschild" for values of the
area-radius coordinate r bigger than R. Thus, the end points
of the path are in the "Schwarzschild" external region. We
demand also that such geometries should satisfy the weak
energy condition (WEC). The result shows that, provided the
WEC is satisfied, the fastest travel is achieved by setting
the metric in the interior (r<R) equal to that of Minkowski
space. Then, the mass that enters the Schwarszchild metric
is concentrated in a thin shell at r=R.
[B13.014] Neutron Star Structure In The Presence of Scalar Fields
James Crawford (Penn State - Fayette), Demosthenes Kazanas (NASA/Goddard Space Flight Center, Code 661)
Motivated by the possible presence of scalar fields on
astrophysical scales, suggested by the recent measurement of
the deceleration parameter by distance supernovae surveys,
we present models of neutron star structure under the
assumption that a scalar field makes a significant
contribution to the stress energy momentum tensor, in
addition to that made by the normal matter. To that end we
solve the coupled Einstein - scalar field - hydrostatic
balance equations to compute the effect of the presence of
the scalar field on the neutron star structure. We find that
the presence of the scalar field does change the structure
of the neutron star, especially in cases of strong coupling
between the scalar field and the matter density. We present
the neutron star radius as a function of the matter--scalar
field coupling constant for different values of the neutron
star central density. The presence of the scalar field does
affect both the maximum neutron star mass and its radius,
the latter increasing with the value of the above coupling
constant. Our results may be testable with the recent timing
observations of accreting neutron stars.
[B13.015] Weak Field Limit of a Scale Invariant Yang-Mills Theory of Gravity
James P. Crawford (Pennsylvania State University)
A theory of gravity where the action is taken to be in Yang-Mills form ("square of the Riemann tensor") is discussed. If we demand that the spin-connection field be treated as an "ordinary" gauge field, then it must remain invariant under scale transformations. This implies invariance of the Riemann tensor and the gravitational action, but the torsion tensor transforms inhomogeneously. To construct a scale invariant action for a scalar field requires terms quadratic in the torsion, but this action is not uniquely determined by the demand of scale invariance since it is only the vector ("trace") part of the torsion which transforms inhomogeneously, the remaining pieces being invariant. This ambiguity is lifted by the further demand that in the weak field limit the field equations reduce to the weak field limit of Einstein's equation. Thus we obtain a classically viable alternative to Einsteinian gravity, but whose construction as a Yang-Mills theory may ameliorate the notoriously difficult problem of quantization.