The Euler class of an oriented rank- vector bundle is the pullback of its Thom class along the zero section. Over it equals the top Stiefel-Whitney class.
For an -oriented real bundle of rank , pull its Thom class back along the zero section to obtain its Euler class in . It depends on the orientation and the actual bundle, not merely its stable isomorphism class. In complex cobordism the orientation may be supplied by a stable complex structure on a real vector bundle.
Normalize the section to the sphere bundle. Scaling it from zero to unit length gives a homotopy within the disk bundle from the zero section to this sphere-valued section. The image of the relative Thom class in absolute cohomology restricts to zero on the sphere bundle. Homotopy invariance therefore makes its zero-section pullback vanish.
// Target: geometry-and-topology.bigb
A complex rank- vector bundle has a canonical real orientation, and its Euler class equals its top Chern class. For a complex line this is . The splitting principle for complex vector bundles gives an injective cohomology pullback on which the bundle splits into lines. The Whitney product formula for Euler classes and Whitney sum formula for Chern classes then identify both sides with the product of those first Chern classes, proving the general equality.
For an oriented vector bundle of odd rank, multiplication by on each fiber identifies with the oppositely oriented bundle. Naturality and reversal of the Thom class giveso .
For oriented real vector bundles and , the ordered direct-sum orientation satisfiesThe formula follows because the Thom class of the direct sum is the fiberwise exterior product of the two Thom classes.
When an oriented rank- vector bundle has a closed oriented -dimensional base , its Euler number is the integer obtained by evaluating the Euler class of a vector bundle on the fundamental class of . A nonzero Euler number obstructs a nowhere-zero section and therefore obstructs a framing.
For a closed, oriented smooth manifold and a smooth vector field with isolated zeros, the Poincaré-Hopf theorem statesThe index of a vector field at an isolated zero is the mapping degree of on a small surrounding sphere, computed in an oriented coordinate chart. Thus local winding at the zeros adds up to the global Euler characteristic.[ref]
Manifolds, Transversality, and de Rham Cohomology by Peter Petersen. Theorem5.4.26, Poincaré-Hopf
For the gradient of height on a two-dimensional sphere, the north and south zeros each have index one; their sum is . For a compact manifold with boundary, the same sum requires an outward-pointing boundary condition. A constant nonzero vector field on a closed disk shows why unrestricted boundary behavior cannot be allowed.
At an isolated zero of a smooth vector field on an oriented -manifold, its index is the mapping degree of the normalized field on a sufficiently small surrounding coordinate sphere:The sphere contains no other zeros. Shrinking it without crossing another zero gives a homotopy of normalized maps, so the degree stays unchanged.
For a nondegenerate zero, the derivative is invertible and the index is . In the plane, sources and sinks therefore have index , while a saddle has index . Degenerate zeros can have other values: winds twice around a small circle and has index two.
The Poincaré-Hopf theorem sums these local indices to the Euler characteristic on a closed manifold, with the corresponding boundary condition needed when a boundary is present. Thus the local winding detects a global obstruction to a nowhere-zero field.[ref]
Manifolds, Transversality, and de Rham Cohomology by Peter Petersen. Theorem5.4.26, Poincaré-Hopf
The complex orientation turns a complex line bundle into an oriented real rank-two bundle, andMoreover and .
A Gysin sequence of a sphere bundle is the long exact sequence induced by the Gysin homomorphism and the Euler class of a vector bundle.
Let be an oriented real vector bundle of positive even rank , with zero Euler class, and suppose the integral cohomology of is torsion-free. The Gysin sequence gives . Choose an odd-degree class with . The projection formula for sphere bundle integration identifies the cohomology additively with . It is torsion-free, so graded commutativity of the cup product gives from . These facts establish the displayed ring isomorphism, not just a decomposition of groups.
For the sphere bundle of an oriented rank- real vector bundle, the integration map in the Gysin sequence lowers degree by . Its compatibility with the cup product is the displayed projection formula. The construction is the connecting map of the disk/sphere pair followed by the inverse Thom isomorphism theorem; the connecting map has its graded module sign, and the degree sign in the conventional fibre-integration map gives the displayed left-module formula.
For a real rank- vector bundle , the Thom isomorphism theorem with coefficients identifies the relative cohomology sequence of its disk bundle and sphere bundle withThe multiplier is the top Stiefel–Whitney class, also called the mod-two Euler class. No orientation of is required. For the real tautological line bundle, the sphere bundle is the antipodal cover of Real projective space; this sequence proves that all powers of the degree-one generator through the dimension of the base are nonzero.
For an integer , the diagonal quotient is the unit circle bundle of a complex line bundle over whose Euler class is times a generator. Its Gysin sequence giveswhile for prime , for .
Let be the standard basis of and let be an oriented circle bundle with Euler class . If , its Gysin sequence givesFor zero Euler class the bundle is trivial and its cohomology is that of .
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