Home
Convex Optimization
Convex Optimization Group
Calculus of Inequalities
Conic Independence
Convex Cones
Convex, Affine, Conic Hulls
Convex Functions
Convex Geometry
Distance Geometry
Distance Matrix Cone
Dual Cones
Duality Gap
Euclidean Distance Matrices
Elliptope and Fantope
Extreme Directions
Eigenvalues/Eigenvectors
Farkas Lemma
Face Recognition
Fifth Metric Property
Kissing Number
Linear Algebra
Linear Matrix Inequality
Matrix Calculus
Manifold Learning
Molecular Conformation
Positive Semidefinite Cone
Projection
Quasiconvex Functions
Rank Constraint
Semidefinite Programming
Schoenberg Criterion
Sensor Network Localization
Optimization News
SEO Consultant
Video
Wikimization
Zeros of Polynomials
Contact Us
Wikimization     Meboo     Video     News     Contact     See
Felice crystal
Home arrow Optimization News arrow A dynamical system approach to inhomogeneous dust solutions. (arXiv:0709.1005v2 [gr-qc] CROSS...
A dynamical system approach to inhomogeneous dust solutions. (arXiv:0709.1005v2 [gr-qc] CROSS...

We examine numerically and qualitatively the Lema\^\i tre--Tolman--Bondi (LTB) inhomogeneous dust solutions as a 3--dimensional dynamical system characterized by six critical points. One of the coordinates of the phase space is an average density parameter, $<\Omega>$, which behaves as the ordinary $\Omega$ in Friedman-Lema\^\i tre--Robertson--Walker (FLRW) dust spacetimes. The other two coordinates, a shear parameter and a density contrast function, convey the effects of inhomogeneity. As long as shell crossing singularities are absent, this phase space is bounded or it can be trivially compactified. This space contains several invariant subspaces which define relevant particular cases, such as: ``parabolic'' evolution, FLRW dust and the Schwarzschild--Kruskal vacuum limit. We examine in detail the phase space evolution of several dust configurations: a low density void formation scenario, high density re--collapsing universes with open, closed and wormhole topologies, a structure formation scenario with a black hole surrounded by an expanding background, and the Schwarzschild--Kruskal vacuum case. Solution curves start expanding from a past attractor (source) in the plane $<\Omega>=1$, associated with self similar regime at an initial singularity. Depending on the initial conditions and specific configurations, the curves approach several saddle points as they evolve between this past attractor and other two possible future attractors: perpetually expanding curves terminate at a line of sinks at $<\Omega>=0$, while collapsing curves reach maximal expansion as $<\Omega>$ diverges and end up in sink that coincides with the past attractor and is also associated with self similar behavior.

Read more: http://arxiv.org/abs/0709.1005.

 

The Course

The Videos

See Inside

Convex Optimization

by Stephen Boyd 

& L. Vandenberghe 

Buy Book



See Figures

See Inside

Dattorro

by Dattorro

Buy Book



The Course

Bertsekas

by Dimitri Bertsekas 

Buy Book



See Inside

Hiriart-Urruty & Lemaréchal

by Hiriart-Urruty

& Lemaréchal

Buy Book



See Inside

Rockafellar

by Rockafellar

Buy Book



Optimization Newsletter
Subscription:

Email:

Receive HTML mailings?
Subscribe Unsubscribe