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.
Let X and Y be oriented smooth closed manifolds,and f: X → Y a continuous map.Let vf=f*(TY) - TX in the K-group K(X).If dim(X) ≡ dim(Y) mod 2, then
ch(fK*(x))=fH*(ch(x)
d(vf)/2 | |
e |
\hat{A}(vf)),
The theorem is proven by considering several special cases.[3] If Y is the Thom space of a vector bundle V over X,then the Gysin maps are just the Thom isomorphism.Then, using the splitting principle, it suffices to check the theorem via explicit computation for linebundles.
If f: X → Y is an embedding, then the Thom space of the normal bundle of X in Y can be viewed as a tubular neighborhood of Xin Y, and excision gives a map
u:H*(B(N),S(N))\toH*(Y,Y-B(N))\toH*(Y)
v:K(B(N),S(N))\toK(Y,Y-B(N))\toK(Y)
Finally, we can factor a general map f: X → Yinto an embedding
i:X\toY x S2n
p:Y x S2n\toY.
Atiyah and Hirzebruch then 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.