§ Vector fields over the 2 sphere
We assume that we already know the hairy ball theorem, which states that
no continuous vector field on S2 exists that is nowhere vanishing. Using
this, we wish to deduce (1) that the module of vector fields over S2 is
not free, and an explicit version of what the
Serre Swan theorem
tells us, that this module is projective
§ 1. Vector fields over the 2-sphere is projective
Embed the 2-sphere as a subset of R3. So at each point, we have
a tangent plane, and a normal vector that is perpendicular to the sphere:
for the point p∈S2, we have the vector p as being normal to TpS2 at p.
So the normal bundle is of the form:
N≡{{s}×{λs:λinR}:s∈S2}
- If we think of the trivial bundle, that is of the form Tr≡{s}×R:s∈S2}.
- We want to show an isomorphism between N and T.
- Consider a map f:N→Tr such that f((s,n))≡(s,∣∣n∣∣). The inverse is g:Tr→N given by g((s,r))≡(s,r⋅s). It's easy to check that these are inverses, so we at least have a bijection.
- To show that it's a vector bundle morphism, TODO.
- (This is hopelessly broken, I can't treat the bundle as a product. I can locally I guess by taking charts; I'm not sure how I ought to treat it globally!)
§ 1. Vector fields over the sphere is not free
- 1. Given two bundles E,F over any manifold M, a module isomorphism f:X(E)→X(F) of vector fields as C∞(M) modules is induced by a smooth isomorphism of vector bundles F:E→F.
- 2. The module X(M) is finitely generated as a C∞ module over M.
- Now, assume that X(S2) is a free module, so we get that X(S2)≃⊕iC∞(S2).
- By (2), we know that this must be a finite direct sum for some finite N: mathfrakX(S2)=⊕i=1NC∞(Sn).
- But having N different independent non-vanishing functions on S2 is the same as clubbing them all together into a vector of N values at each point at S2.
- So we get a smooth function S2→Rn, AKA a section of the trivial bundle Rn≡S2×Rn.
- This means that we have managed to trivialize the vector bundle over the sphere if vector fields over S2 were a free module.
- Now, pick the element S2×{(1,1,1,1,…)}∈S2×Rn. This is a nowhere vanishing vector field over S2. But such an object cannot exist, and hence vector fields over the sphere cannot be free.
§ References