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Third Stiefel–Whitney Classes of Tangent and Normal Bundles
Statement
Let be a paracompact Hausdorff compactly generated weak Hausdorff space of CW homotopy type, and let be numerable finite-rank real vector bundles. Assume full AC as required by the imported characteristic-class and Bockstein suppliers. If
in mod-two singular cohomology, then
in . In particular, the equality applies to an oriented tangent bundle and its oriented normal bundle when their direct sum has vanishing .
Statement references
Facts & Assumptions
Given: Full AC; numerable finite-rank real bundles over the stated base, with and .
Stiefel–Whitney classes from the projective-bundle relation: are the Stiefel–Whitney classes of a numerable finite-rank real bundle .
Integral Third Stiefel–Whitney Class and Bockstein connecting operation: , with the integral connecting operation for .
Bockstein connecting operation and Singular cohomology with coefficients: the connecting homomorphism is computed by lifting a mod-two singular cocycle to an integral cochain and dividing its integral coboundary by .
The Bockstein is independent of lift and representative: this operation gives a well-defined cohomology class, independent of the cochain lift and cocycle representative.
The Axiom of Choice: every family of nonempty sets has a choice function; this is the full choice hypothesis of the imported Bockstein and characteristic-class suppliers.
Proof
The degree-two part of [F2] gives . The two degree-one classes vanish by the Given clause, and the left side vanishes by the Given clause, so . Since these classes have coefficients in , this says .
Apply the well-defined operation to the equality in step 1.1 and use [F3]. This gives .
Represent by a mod-two singular 2-cocycle . Lift each value of to its unique representative or , obtaining an integral 2-cochain . Because is a cocycle, every value of is even, so is an integral 3-cochain. By [F4] and the lift-independence in [F5], . Therefore , since is a coboundary.
Remarks
The equality uses the integral Bockstein, so torsion is retained. The proof does not assume a classification theorem for spin structures; its input is the explicit vanishing of .