In Part I** of this series we have introduced the new notion of hypermomentum Δijk 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 (L4, g) is shown to be the appropriate geometrical framework
Received: 1976-3-29
Published Online: 2014-6-2
Published in Print: 1976-6-1
© 1946 – 2014: Verlag der Zeitschrift für Naturforschung
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