On Hypermomentum in General Relativity II. The Geometry of Spacetime

In Part I** of this series we have introduced the new notion of hypermomentum Δ ijk as a dynamical quantity characterizing classical matter fields. In Part II, as a preparation for a general relativistic field theory, we look for a geometry of spacetime which will allow for the accomodation of hypermomentum into general relativity. A general linearly connected spacetime with a metric (L 4 , g) is shown to be the appropriate geometrical framework

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