
A central assumption in general relativity is that the underlying geometry of spacetime is pseudo-Riemannian. Given the recent attempts at generalizations of general relativity, motivated both by theoretical and observational considerations, an important question is whether the spacetime geometry can also be made more general and yet still remain compatible with observations? Here I briefly summarize some earlier results which demonstrate that there are special classes of Finsler geometry, which is a natural metrical generalization of the Riemannian geometry, that are strictly compatible with the observations regarding the motion of idealised test particles and light rays. I also briefly summarize some recent attempts at employing Finsler geometries motivated by more recent developments such as those in String theory, whereby Lorentz invariance is partially broken.
Global differential geometry of Finsler spaces and generalizations (areal metrics), string theory, Local differential geometry of Finsler spaces and generalizations (areal metrics), String and superstring theories in gravitational theory, Einstein's equations (general structure, canonical formalism, Cauchy problems), Riemannian geometry, space-time geometry
Global differential geometry of Finsler spaces and generalizations (areal metrics), string theory, Local differential geometry of Finsler spaces and generalizations (areal metrics), String and superstring theories in gravitational theory, Einstein's equations (general structure, canonical formalism, Cauchy problems), Riemannian geometry, space-time geometry
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