Riemann-Roch theorem for smooth manifolds
- Riemann-Roch theorem for smooth manifolds
In mathematics, a Riemann-Roch theorem for smooth manifolds is a version of results such as the Hirzebruch-Riemann-Roch theorem or Grothendieck-Riemann-Roch theorem (GRR) without a hypothesis making the smooth manifolds involved carry a complex structure. Results of this kind were obtained by Michael Atiyah and Friedrich Hirzebruch in 1959, reducing the requirements to something like a spin structure.
In their paper "Riemann-Roch theorems for differentiable manifolds" (Bull. Amer. Math. Soc. 65 (1959) 276-281) they define, for oriented smooth closed manifolds "X" and "Y" and a continuous mapping
:"f": "Y" → "X"
that "f" is a "c"1-map if there is "c"1 in the integral cohomology group
:"H"2("Y", "Z")
such that for the Stiefel-Whitney classes "w"2 we have
:"c"1 = "w"2("Y") − "f"*("w"2("X") modulo 2
in
:"H"2("Y", "Z"/2"Z").
Writing "ch"("X") for the image in "H"*("X", Q) they showed that for "f" a "c"1-map there is
:"f"!: "ch"("Y") → "ch"("X")
which is a homomorphism of abelian groups, and satisfying
:"f"!("y")"A"^("X") = "f"*("y".exp("c"1)/2)"A"^("Y")),
where "A"^ is the A-hat genus and "f"* the Gysin homomorphism. This mimics the GRR theorem; but "f"! has only an implicit definition.
This they specialised and refined in the case "X" = a point, where the condition becomes the existence of a spin structure on "Y". Corollaries are on Pontryagin classes and the J-homomorphism.
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