Abstract
In Chap. 5 we have established the notion of a ray-optical structure on a bare manifold \( \mathcal{M} \). From now on we shall assume that there is a Lorentzian metric g given on \( \mathcal{M} \). This metric is to be interpreted as a spacetime metric in the sense of general relativity, although for the mathematical formalism it will not be necessary to specialize to the case dim\( (\mathcal{M}) = 4 \). We shall assume, however, that dim\( (\mathcal{M}) > 2 \) > 2 to exclude some pathologies.
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© 2000 Springer-Verlag Berlin Heidelberg
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(2000). Ray-optical structures on Lorentzian manifolds. In: Ray Optics, Fermat’s Principle, and Applications to General Relatively. Lecture Notes in Physics, vol 61. Springer, Berlin, Heidelberg. https://doi.org/10.1007/3-540-46662-2_6
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DOI: https://doi.org/10.1007/3-540-46662-2_6
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