“…Remark 10. A Lorentzian metric on a manifold M is called geodesically connected [17,18] if any two points in M can be connected by a future directed nonspacelike geodesic. For any left-invariant Lorentzian metric on Aff + (R) we have J + (Id) = Aff + (R), so such a metric is not geodesically connected.…”
Section: Inverse Of the Exponential Mapping And Optimal Synthesismentioning
Left-invariant Lorentzian structures on the 2D solvable non-Abelian Lie group are studied. Sectional curvature, attainable sets, Lorentzian length maximizers, distance, spheres, and infinitesimal isometries are described.
“…Remark 10. A Lorentzian metric on a manifold M is called geodesically connected [17,18] if any two points in M can be connected by a future directed nonspacelike geodesic. For any left-invariant Lorentzian metric on Aff + (R) we have J + (Id) = Aff + (R), so such a metric is not geodesically connected.…”
Section: Inverse Of the Exponential Mapping And Optimal Synthesismentioning
Left-invariant Lorentzian structures on the 2D solvable non-Abelian Lie group are studied. Sectional curvature, attainable sets, Lorentzian length maximizers, distance, spheres, and infinitesimal isometries are described.
“…Geodesic nonimprisonment and pseudoconvexity of all geodesics together with the absence of conjugate points implies geodesic connectedness and serve as conditions for a pseudo-Riemannian version of the Hadamard-Cartan theorem [7], [5, chapter 11]. For a recent generalization see [11].…”
We consider pseudoconvexity properties in Lorentzian and Riemannian manifolds and their relationship in static spacetimes. We provide an example of a causally continuous and maximal null pseudoconvex spacetime that fails to be causally simple. Its Riemannian factor provides an analogous example of a manifold that is minimally pseudoconvex, but fails to be convex.
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