2 research outputs found
Future geodesic completeness of some spatially homogeneous solutions of the vacuum Einstein equations in higher dimensions
It is known that all spatially homogeneous solutions of the vacuum Einstein
equations in four dimensions which exist for an infinite proper time towards
the future are future geodesically complete. This paper investigates whether
the analogous statement holds in higher dimensions. A positive answer to this
question is obtained for a large class of models which can be studied with the
help of Kaluza-Klein reduction to solutions of the Einstein-scalar field
equations in four dimensions. The proof of this result makes use of a criterion
for geodesic completeness which is applicable to more general spatially
homogeneous models.Comment: 18 page
Die lineare InstabilitÀt der Uniform Black String Lösungen
Black strings are black hole solutions of Einsteinâs equations in more than
four dimensions. In spacetime dimensions n + 1 they have horizon topology
S^(nâ1) Ă S^1. Using numerical simulations, it was discovered in the 1990s
that black strings are linearly unstable. Since then, most research
surrounding this result was focused on understanding physical aspects of the
instability. In this thesis we will return to the original problem of linear
stability and prove an existence result for a special class of mode solutions.
This constitutes an important step towards proving linear instability.Black strings sind schwarze Löcher und Lösungen der Einsteinschen
Feldgleichungen in mehr als vier Dimensionen. In Raumzeitdimension n + 1 hat
ihr Ereignishorizont die Topologie S^(nâ1) Ă S^1. Durch numerische
Simulationen wurde in den 1990ern entdeckt, dass black strings linear instabil
sind. Ausgehend von diesem Resultat lag der Schwerpunkt der Forschung darauf,
die physikalischen Aspekte dieser InstabilitÀt zu verstehen. In dieser Arbeit
werden wir zu dem Problem der linearen InstabilitĂ€t zurĂŒckkehren und die
Existenz einer speziellen Familie von Lösungen beweisen. Dies ist ein
wichtiger Schritt fĂŒr den Beweis der linearen InstabilitĂ€t