12.07.2015 Views

Ivancevic_Applied-Diff-Geom

Ivancevic_Applied-Diff-Geom

Ivancevic_Applied-Diff-Geom

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

<strong>Applied</strong> Bundle <strong>Geom</strong>etry 695On the other hand, it follows from the Bianchi identity,R [abdc] + ∇ [a T bc] d + T [ab e T c]e d = 0,that2(p + q)P [ab] = −∇ c T ab c .The Rho–tensor P ab has the transformation equationˆP A′ B ′AB = P A′ B ′AB − ∇ A′A Υ B′B + Υ B′A Υ A′B . (4.172)We are most interested in the special case p = 2. Then the wholecomponent F c ab is irreducible and so it vanishes by our condition on thetrace, while the other component ˜F c ab of the torsion, together with thetrace–free part of U [A′ B ′ ]D(ABC)are the only local invariants of the structures.In all other cases 2 < p ≤ q, the two components of the torsion are the onlyinvariants.The totally symmetrized covariant derivatives of the Rho–tensors playa special role. We use the notationS a···b := ∇ (a ∇ b · · · ∇ d P ef)} {{ }sfor s = 2, 3 · · · .TwistorsVia the Cartan bundle G over M any P −module V gives rise to a naturalbundle (or induced bundle) V. Sections of V are identified with functionsf : G → V such that f(x.p) = ρ(p −1 )f(x), where x ↦→ x.p gives the actionof p ∈ P on x ∈ G while ρ is the action defining the P −module structure.Recall also that the Cartan bundle is equipped with a canonical connection,the so called normal Cartan connection ω. In view of this it isin our interests to work, where possible, with natural bundles V inducedfrom V where this is not merely a P −module but in fact a G−module.Then the Cartan connection induces an invariant linear connection on V.Let us write V α for the module corresponding to the standard representationof G on R p+q and write V α for the dual module. The index αis another Penrose-type abstract index and we write E α and E α for therespective bundles induced by these G-modules. All finite dimensionalG−modules are submodules in tensor products of the fundamental representationsV α and V α . Thus the bundles E α and E α play a special roleand we term these (local) twistor bundles [Bailey and Eastwood (1991);Penrose and Rindler (1986)]. In fact in line with the use of the word“tensor” we also describe any explicit subbundle of a tensor product of

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!