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September 2008 - June 2014
September 2008 - September 2012
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Publications (5)
In this work we will focus on the causal character of Carter Spacetime (see
B. Carter, Causal structure in space-time, Gen. Rel. Grav. 1 4 337-406, 1971).
The importance of this spacetime is the following: for the causally best well
behaved spacetimes (the globally hyperbolic ones), there are several
characterizations or alternative definitions. In...
En esta investigación nos enfocamos en el carácter causal del espaciotiempo de Carter (ver [2], [10]). Este espaciotiempo es importante por la siguiente razón: para los espaciotiempos con un comportamiento causal óptimo, es decir, los globalmente hiperbólicos, existen varias caracterizaciones o definiciones alternativas. En algunos casos se ha demo...
Second-order symmetric Lorentzian spaces, that is to say, Lorentzian
manifolds with vanishing second derivative of the curvature tensor R, are
characterized by several geometric properties, and explicitly presented.
Locally, they are a product M=M_1 x M_2 where each factor is uniquely
determined as follows: M_2 is a Riemannian symmetric space and M...
We give a summary of recent results on the explicit local form of the
second-order symmetric Lorentzian manifolds in arbitrary dimension, and its
global version. These spacetimes turn out to be essentially a specific subclass
of plane waves.
As a difference with the positive-definite Riemannian case, in the Lorentzian
case there exists proper second-order symmetric spacetimes, i.e., those with
vanishing second covariant derivative of the Riemannian tensor
($R_{\lambda\mu\nu\rho;\alpha;\beta}=0$) which are not locally symmetric
($R_{\lambda\mu\nu\rho;\alpha}\neq 0$). In fact, they lie i...