The affine geometry of the Lanczos H-tensor formalism

Details The affine geometry of the Lanczos H-tensor formalism The affine geometry of the Lanczos H-tensor formalism

Jan 1993

adsabs.harvard.edu/cgi-bin/nph-data_query?bibcode=1993gregr..25...55h&link_type=abstract

General Relativity and Gravitation, Volume 25, Issue 1, pp.55-80

Mathematics

Differential Geometry

5

Scientific paper

We identify the fiber-bundle-with-connection structure that underlies the Lanczos H-tensor formulation of Riemannian geometrical structure. We consider linear connections to be type (1,2) affine tensor fields, and we sketch the structure of the appropriate fiber bundle that is needed to describe the differential geometry of such affine tensors, namely the affine frame bundleA {1/2} M with structure groupA {1/2} (4) =GL(4) ⓈT {1/2}ℝ4 over spacetimeM. Generalized affine connections on this bundle are in 1-1 correspondence with pairs(Γ, K) onM, where thegl(4)-componentΓ denotes a linear connection and the T{1/2}ℝ4-componentK is a type (1,3) tensor field onM. We show that the Lanczos H-tensor arises from a gauge fixing condition on this geometrical structure. The resulting translation gauge, theLanczos gauge, is invariant under the transformations found earlier by Lanczos. The other Lanczos variablesQ μmandq are constructed in terms of the translational component of the generalized affine connection in the Lanczos gauge. To complete the geometric reformulation we reconstruct the Lanczos Lagrangian completely in terms of affine invariant quantities. The essential field equations derived from ourA {1/2} (4)-invariant Lagrangian are the Bianchi and Bach-Lanczos identities for four-dimensional Riemannian geometry.

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