362 research outputs found

    Irrotational dust with Div H=0

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    For irrotational dust the shear tensor is consistently diagonalizable with its covariant time derivative: σab=0=σ˙ab,  a≠b\sigma_{ab}=0=\dot{\sigma}_{ab},\; a\neq b, if and only if the divergence of the magnetic part of the Weyl tensor vanishes: div H=0div~H = 0. We show here that in that case, the consistency of the Ricci constraints requires that the magnetic part of the Weyl tensor itself vanishes: Hab=0H_{ab}=0.Comment: 19 pages. Latex. Also avaliable at http://shiva.mth.uct.ac.za/preprints/text/lesame2.te

    Horizon area bound and MOTS stability in locally rotationally symmetric solutions

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    In this paper, we study the stability of marginally outer trapped surfaces (MOTS), foliating horizons of the form r=X(Ï„)r=X(\tau), embedded in locally rotationally symmetric class II perfect fluid spacetimes. An upper bound on the area of stable MOTS is obtained. It is shown that any stable MOTS of the types considered in these spacetimes must be strictly stably outermost, that is, there are no MOTS ``outside" of and homologous to S\mathcal{S}. Aspects of the topology of the MOTS, as well as the case when an extension is made to imperfect fluids, are discussed. Some non-existence results are also obtained. Finally, the ``growth" of certain matter and curvature quantities on certain unstable MOTS are provided under specified conditions.Comment: 21 pages, Submitted to CQG, comments are welcom

    Shear-Free Gravitational Waves in an Anisotropic Universe

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    We study gravitational waves propagating through an anisotropic Bianchi I dust-filled universe (containing the Einstein-de-Sitter universe as a special case). The waves are modeled as small perturbations of this background cosmological model and we choose a family of null hypersurfaces in this space-time to act as the histories of the wavefronts of the radiation. We find that the perturbations we generate can describe pure gravitational radiation if and only if the null hypersurfaces are shear-free. We calculate the gauge-invariant small perturbations explicitly in this case. How these differ from the corresponding perturbations when the background space-time is isotropic is clearly exhibited.Comment: 32 pages, accepted for publication in Physical Review
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