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Stiefel-Whitney class

Stiefel-Whitney classes arise in mathematics as a type of characteristic class associated to real vector bundles E\rightarrow X. They are denoted wi(E), taking values in H^i(X,\mathbb Z_2), the cohomology groups with mod 2 coefficients. Naturally enough, we say that wi(E) is the ith Stiefel-Whitney class of E. As an example, over the circle, S1, there is a line bundle that is topologically non-trivial: that is, the line bundle associated to the Möbius band, usually thought of as having fibres [0,1]. The cohomology group

H^1(S^1,\mathbb Z/2\mathbb Z)

has just one element other than 0, this element being the first Steifel-Whitney class, w1, of that line bundle.

Contents

Axioms

Throughout, H^i(\;\cdot\;;G) denotes singular cohomology with coefficient group G.

  1. For every real vector bundle E\rightarrow X, there exist wi(E) in H^i(X;\mathbb Z/2\mathbb Z) which are natural, i.e., characteristic classes.
  2. w0(E) = 1 in H^0(X;\mathbb Z/2\mathbb Z).
  3. wi(E) = 0 whenever i > rank(E).
  4. w11) = x in H^1(\mathbb RP^1;\mathbb Z/2\mathbb Z)=\mathbb Z/2\mathbb Z (normalization condition). Here, γn is the canonical line bundle.
  5. w_k(E\oplus F)=\sum_{i+j=k}w_i(E)\cup w_j(F).
  6. If Ek has s_1,\ldots,s_{\ell} sections which are everywhere linearly independent then w_{k-\ell+1}=\cdots=w_k=0.

Some work is required to show that such classes do indeed exist and are unique.

Properties

The first Stiefel-Whitney class is zero if and only if the bundle is orientable.

The second Stiefel-Whitney class is zero if and only if the bundle admits a spin structure.

See also

References

J. Milnor & J. Stasheff, Characteristic Classes, Princeton, 1974.

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