Statement

Let EXE\to X be an oriented real rank-nn with n2n\ge2 over a . If EE admits a continuous section s:XEs:X\to E satisfying πs=idX\pi s=\operatorname{id}_X and s(x)0xs(x)\ne0_x for all xx, then

e(E)=0Hn(X;Z).e(E)=0\in H^n(X;\mathbb Z).

Here e(E)e(E) is the . More precisely, e(E)e(E) is the primary obstruction to a section of the unit sphere bundle S(E)={v:v=1}XS(E)=\{v:\|v\|=1\}\to X for any continuous positive-definite fiber metric (the topological unit sphere is defined by the displayed norm equation). Consequently, when dimXn\dim X\leq n, the Euler class is the complete obstruction: such a section exists if and only if e(E)=0e(E)=0. For bases of dimension greater than nn, higher obstruction classes may remain after e(E)e(E) vanishes.

Obstruction-theoretic mechanism

A continuous positive-definite fiber metric turns a nowhere-zero section into a section of the unit sphere bundle S(E)S(E), whose fiber is Sn1S^{n-1}. Since Sn1S^{n-1} is (n2)(n-2)-connected, a section extends through the (n1)(n-1)-skeleton. The first possible obstruction lies in degree nn, with coefficients πn1(Sn1)Z\pi_{n-1}(S^{n-1})\cong\mathbb Z. The orientation trivializes this local coefficient system, and the resulting class is e(E)e(E). There are no cells on which a higher obstruction could live when dimXn\dim X\le n.

Geometric interpretation

For a smooth bundle over a closed oriented smooth base, a smooth section transverse to the has a zero set representing the Poincaré dual of e(E)e(E). When the base and bundle both have dimension nn, the signed count of isolated zeros equals

e(E),[X].\langle e(E),[X]\rangle.

Applied to E=TME=TM on a closed oriented manifold, this is the Poincaré–Hopf theorem: the total index of a is χ(M)\chi(M). Thus S2mS^{2m}, for m1m\ge1, has no nowhere-zero tangent vector field.

Rank zero and rank one

An oriented real line bundle over a CW complex is trivial, so it has a nowhere-zero section and Euler class zero in every base dimension. The displayed obstruction argument using πn1(Sn1)Z\pi_{n-1}(S^{n-1})\cong\mathbb Z is for n2n\ge2. A rank-zero bundle over a nonempty base has no nowhere-zero section and has Euler class 1H0(X;Z)1\in H^0(X;\mathbb Z).

Scope and near-misses

For a nonorientable bundle, the primary obstruction lives in cohomology with the orientation local system rather than ordinary integral cohomology. A section that vanishes somewhere is not a counterexample: the required condition is nowhere-zero, not merely nonzero as an element of the .

References
  1. John W. Milnor and James D. Stasheff, Characteristic Classes, Princeton University Press, 1974. DOI record. Relevant: Euler classes, zero sections, and the obstruction interpretation.
  2. Dale Husemoller, Fibre Bundles, 3rd ed., Springer, 1994. DOI record. Relevant: sphere bundles, cross-sections, and obstruction theory for vector bundles.