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Abel–Jacobi map

Construction in algebraic geometry

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Construction of the map

In complex algebraic geometry, the Jacobian of a curve C is constructed using path integration. Namely, suppose C has genus g, which means topologically that

H1(C,Z)≅Z2g.

Geometrically, this homology group consists of (homology classes of) cycles in C, or in other words, closed loops. Therefore, we can choose 2g loops γ1,…,γ2g generating it. On the other hand, another more algebro-geometric way of saying that the genus of C is g is that

H0(C,K)≅Cg,

where K is the canonical bundle on C.

By definition, this is the space of globally defined holomorphic differential forms on C, so we can choose g linearly independent forms ω1,…,ωg. Given forms and closed loops we can integrate, and we define 2g vectors

Ωj=(∫γjω1,…,∫γjωg)∈Cg.

It follows from the Riemann bilinear relations that the Ωj generate a nondegenerate lattice Λ (that is, they are a real basis for Cg≅R2g), and the Jacobian is defined by

J(C)=Cg/Λ.

The Abel–Jacobi map is then defined as follows. We pick some base point p0∈C and, nearly mimicking the definition of Λ, define the map

{u:C→J(C)u(p)=(∫p0pω1,…,∫p0pωg)modΛ

Although this is seemingly dependent on a path from p0 to p, any two such paths define a closed loop in C and, therefore, an element of H1(C,Z), so integration over it gives an element of Λ. Thus the difference is erased in the passage to the quotient by Λ. Changing base-point p0 does change the map, but only by a translation of the torus.

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