For a rank-rr EXE\to X over a paracompact Hausdorff space, its Stiefel–Whitney classes are classes

wi(E)Hi(X;Z/2),i0,w_i(E)\in H^i(X;\mathbb Z/2),\qquad i\ge0,

depending only on the bundle isomorphism class. As a family over all such bundles and bases they are characterized by all of the following axioms:

  1. Degree and rank normalization: w0(E)=1w_0(E)=1 and wi(E)=0w_i(E)=0 for i>ri>r.
  2. Naturality: for every continuous f:YXf:Y\to X with YY paracompact Hausdorff, wi(fE)=fwi(E)w_i(f^*E)=f^*w_i(E).
  3. Whitney product: w(EF)=w(E)w(F)w(E\oplus F)=w(E)\smile w(F), where w(E)=i=0rwi(E)w(E)=\sum_{i=0}^r w_i(E), direct sums are fiberwise direct sums with their local product topology, and multiplication is the mod-22 .
  4. Line normalization: the tautological real line bundle γ1\gamma^1 over RP1\mathbb{RP}^1 has w1(γ1)w_1(\gamma^1) equal to the nonzero element of H1(RP1;Z/2)H^1(\mathbb{RP}^1;\mathbb Z/2). Its fiber over a line R2\ell\subset\mathbb R^2 is \ell itself.

The class w(E)w(E) is the total Stiefel–Whitney class. These axioms include the normalization that distinguishes this canonical family from other natural mod-22 classes.

Basic properties

If f:YXf:Y\to X is continuous, then

wi(fE)=fwi(E).w_i(f^*E)=f^*w_i(E).

The Whitney product formula implies that a fiberwise exact sequence of real vector bundles

0EEE00\longrightarrow E'\longrightarrow E\longrightarrow E''\longrightarrow0

satisfies w(E)=w(E)w(E)w(E)=w(E')\smile w(E''), since such a sequence of real vector bundles splits after choosing a continuous fiber metric. Trivial bundles have total class 11.

These axioms uniquely determine the classes and make them insensitive to choices of metrics, connections, or .

Geometric meaning

The first class w1(E)w_1(E) vanishes exactly when EE is orientable. For an oriented positive-rank bundle, w2(E)w_2(E) obstructs a lift of its oriented orthonormal frame bundle through Spin(r)SO(r)\operatorname{Spin}(r)\to\operatorname{SO}(r); for tangent bundles this is a . More generally, nonzero higher classes obstruct the existence of many everywhere linearly independent sections: if EE has kk pointwise independent sections, then the top kk Stiefel–Whitney classes vanish.

For a closed smooth nn-manifold MM, evaluating degree-nn products of the classes of TMTM on the mod-2 gives Stiefel–Whitney numbers. These numbers are central invariants in unoriented cobordism.

Examples

For n1n\ge1, the tautological real line bundle γ1RPn\gamma^1\to\mathbb{RP}^n, w(γ1)=1+aw(\gamma^1)=1+a, where aa is the generator of H1(RPn;Z/2)H^1(\mathbb{RP}^n;\mathbb Z/2). For the of the sphere,

TSnRRn+1,TS^n\oplus\underline{\mathbb R}\cong\underline{\mathbb R}^{\,n+1},

so the Whitney formula gives w(TSn)=1w(TS^n)=1.

Because coefficients are mod 22, no orientation is required to define these classes. Integral lifts or refinements, when they exist, are additional structure and are not part of the definition.

Conventions and scope

The singular title “Stiefel–Whitney class” refers to any component wi(E)w_i(E); the plural refers to the whole family. These are invariants of real vector bundles. Chern classes play the analogous role for complex bundles, although reduction mod 22 relates the even Stiefel–Whitney classes of an underlying real bundle to Chern classes.

References
  1. J. W. Milnor and J. D. Stasheff, Characteristic Classes, Annals of Mathematics Studies 76, Princeton University Press, 1974. DOI record. Relevant: Chapters 4 and 8, axioms, examples, and obstruction-theoretic properties.
  2. D. Husemoller, Fibre Bundles, 3rd ed., Springer, 1994. DOI record. Relevant: Chapter 17, characteristic classes of real vector bundles.