Let E be a complex vector bundle over a compact smooth manifold M. Let \nabla^E be a (C-linear) connection on E and let R^E denote its curvature.
The Chern character form associated to \nabla^E is defined by
ch\left(E,\nabla^E\right)=tr\left[ \exp\left(\frac{\sqrt{-1}}{2\pi}R^E\right)\right]\in\Omega^{even}(M).
Obviously, ch\left(E,\nabla^E\right) is a closed form. We denote the association cohomology class by ch(E) which is called the Chern character of E.
- ch(E\oplus F)= ch(E)+ch(F); \qquad (\oplus is Whithney direct sum)
- ch(E\otimes F)=ch(E)\times ch(F);
- If E\cong F, then ch(E)=ch(F).
The crux of the proof is that the calculate does not depend on the representative element.
Denote by Vector(M) the set of all complex vector bundles over M, then under the Whitney direct sum operation, Vect(M) becomes a semi-abelian group. And (Vect(M), \otimes, \oplus) is a semi-ring. Now we introduce an equivalence relation ‘\sim’ in Vect(M) such that
E \sim F\Leftrightarrow E\cong F.
So the following map
ch : Vect(M)\rightarrow H^{even}_dR(M,C)
is a homomorphism between semi-groups. there is a nature method for extending a semi-abelian group to a abelian group. The fundamental ideal: let N be the natural number(0 \not\in N). Now we extend semi-abelian group (N,+) to a abelian group.
i) Take
N\times N=\set{(m,n)|m,n\in N}.
In N\times N, there have a natural sum ‘+’ as follows:
\bigg( \forall m_1,m_2,n_1,n_2 \in N \bigg) \quad (m_1,n_1)+(m_2,n_2)=(m_1+m_2, n_1+n_2).
One introduces an equivalence relation ‘\sim’ in N\times N as follows:
(m_1,n_1)\sim (m_2,n_2) \Leftrightarrow m_1+n_2=m_2+n_1.
Please note there is not subtract. Let Z=N\times N /\sim, it is easily proved that Z is a abelian group. The zero element is [(m,m)],m\in N. And [(m,n)]^{-1}=[(n,m)].
ii)Make a map
\phi : N \rightarrow Z, \qquad \phi(m)=[(m+1,1)].
Obviously, the map \phi is isomorphism from N to a semi-subgroup \set{[(m+1,1)]}. So Z is a dilation of N. then we can denote
m=[(m+1,1)],\quad 0=[(m,m)],\quad -m=[(1,m+1)],\quad\forall m \in N.
One can prove this dilation is the smallest.
Now we can extend semi-abelian group Vect(M)/\sim to a group K(M) which is called the K-group of M. Naturally, the map ch is extended a group homomorphism,
ch: K(M) \rightarrow H^{even}_dR(M,\C).
Atiyah and Hirzebruch prove this homomorphism is an isomorphism if one ignores the torsion elements in K(M). This theory belongs the K-theory.
\langle \hat{A}(TM)ch(E),[M] \rangle =\int_M \hat{A}(TM,\nabla^{TM})ch(E,\nabla^E)\in \C.
If M is an even dimensional oriented spin closed manifold(see[milnor]), the characteristic number
\langle \hat{A}(TM)ch(E),[M] \rangle
is a integer.(Atiyah, Hirzebruch, Borel theorem)
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