Stiefel–Whitney class
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In mathematics, the Stiefel–Whitney class arises as a type of characteristic class associated to real vector bundles
. It is denoted by w(E), taking values in
, the cohomology groups with mod 2 coefficients. The component of w(E) in
is denoted by wi(E) and called the ith Stiefel-Whitney class of E, so that
. 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
has just one element other than 0, this element being the first Stiefel-Whitney class, w1, of that line bundle.
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[edit] Axioms
Throughout, Hi(X;G) denotes singular cohomology of a space X with coefficients in the group G.
- Naturality: w(f * E) = f * w(E) for any bundle
and map f:X' − > X - w0(E) = 1 in
. - w1(γ1) is the generator of
(normalization condition). Here, γn is the canonical line bundle.
(Whitney product formula).
Some work is required to show that such classes do indeed exist and are unique (at least for paracompact spaces X); see section 3.5 and 3.6 in Husemoller or section 8 in Milnor and Stasheff.
[edit] Line bundles
Let X be a paracompact space, and let Vectn(X) denote the set of real vector bundles over X of dimension n for some fixed positive integer n. For any vector space V, let Grn(V) denote the Grassmannian
. Set
. Define the tautological bundle
by
; this is a real bundle of dimension n, with projection
given by
. For any map
, the induced bundle
. Since any two homotopic maps
have f * γn and g * γn isomorphic, the map
given by
is well-defined, where [X;Grn] denotes the set of homotopy equivalence classes of maps
. It's not difficult to prove that this map α is actually an isomorphism (see Sections 3.5 and 3.6 in Husemoller, for example). As a result, Grn is called the classifying space of real n-bundles.
Now consider the space Vect1(X) of line bundles over X. For n = 1, the Grassmannian Gr1 is just
, where the nonzero element of
acts by
. The quotient map
is therefore a double cover. Since
is contractible, we have
for i > 1 and
; that is,
. Hence
is the Eilenberg-Maclane space
. Hence
for any X, with the isomorphism given by
, where η is the generator
. Since
is also a bijection, we have another bijection
. This map w1 is precisely the Stiefel-Whitney class w1 for a line bundle. (Since the corresponding classifying space
for complex bundles is a
, the same argument shows that the Chern class defines a bijection between complex line bundles over X and
.) For example, since
, there are only two line bundles over the circle up to bundle isomorphism: the trivial one, and the open Möbius strip (i.e., the Möbius strip with its boundary deleted). If Vect1(X) is considered as a group under the operation of tensor product, then α is an isomorphism:
for all line bundles
.
[edit] Higher dimensions
The bijection above for line bundles implies that any functor θ satisfying the four axioms above is equal to w. Let
be an n-bundle. Then ξ admits a splitting map, a map
for some space X' such that
is injective and
for some line bundles
. Any line bundle over X is of the form g * γ1 for some map g, and θ(g * γ1) = g * θ(γ1) = 1 + w1(g * γ1) by naturality. Thus θ = w on Vect1(X). It follows from the fourth axiom above that
Since f * is injective, θ = w Thus the Stiefel-Whitney class is the unique functor satisfying the four axioms above.
Although the map
is a bijection, the corresponding map is not necessarily injective in higher dimensions. For example, consider the tangent bundle TSn for n even. With the canonical embedding of Sn in
, the normal bundle ν to Sn is a line bundle. Since Sn is orientable, ν is trivial. The sum
is just the restriction of
to Sn, which is trivial since
is contractible. Hence
. But
is not trivial; its Euler class
, where [Sn] denotes a fundamental class of Sn and χ the Euler characteristic.
[edit] Stiefel–Whitney numbers
If we work on a manifold of dimension n, then any product of Stiefel-Whitney classes of total degree n can be paired with the
-fundamental class of the manifold to give an element of
, a Stiefel-Whitney number of the vector bundle. For example, if the manifold has dimension 3, there are three linearly independent Stiefel-Whitney numbers, given by
. In general, if the manifold has dimension n, the number of possible independent Stiefel-Whitney numbers is the number of partitions of n.
The Stiefel-Whitney numbers of the tangent bundle of a smooth manifold are called the Stiefel-Whitney numbers of the manifold, and are important invariants.
[edit] Properties
- If Ek has
sections which are everywhere linearly independent then
. - wi(E) = 0 whenever i > rank(E).
- The first Stiefel-Whitney class is zero if and only if the bundle is orientable. In particular, a manifold M is orientable if and only if w1(TM) = 0.
- The bundle admits a spin structure if and only if both the first and second Stiefel-Whitney classes are zero.
- For an orientable bundle, the second Stiefel-Whitney class is in the image of the natural map
(equivalently, the so-called third integral Stiefel-Whitney class is zero) if and only if the bundle admits a spinc structure. - All the Stiefel-Whitney numbers of a smooth compact manifold X vanish if and only if the manifold is a boundary (unoriented) of a smooth compact manifold.
[edit] Integral Stiefel-Whitney classes
The element
is called the i + 1 integral Stiefel-Whitney class, where β is the Bockstein homomorphism, corresponding to reduction modulo 2,
:
For instance, the third integral Stiefel-Whitney class is the obstruction to a Spinc structure.
[edit] References
- D. Husemoller, Fibre Bundles, Springer-Verlag, 1994.
- J. Milnor & J. Stasheff, Characteristic Classes, Princeton, 1974.




