Appell–Humbert theorem

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Template:Short description In mathematics, the Appell–Humbert theorem describes the line bundles on a complex torus or complex abelian variety. It was proved for 2-dimensional tori by Template:Harvs and Template:Harvs, and in general by Template:Harvs

Statement

Suppose that T is a complex torus given by V/Λ where Λ is a lattice in a complex vector space V. If H is a Hermitian form on V whose imaginary part E=Im(H) is integral on Λ×Λ, and α is a map from Λ to the unit circle U(1)={z∈ℂ:|z|=1}, called a semi-character, such that

α(u+v)=eiπE(u,v)α(u)α(v) 

then

α(u)eπH(z,u)+H(u,u)π/2 

is a 1-cocycle of Λ defining a line bundle on T. For the trivial Hermitian form, this just reduces to a character. Note that the space of character morphisms is isomorphic with a real torus

Hom𝐀𝐛(Λ,U(1))≅ℝ2n/ℤ2n

if Λ≅ℤ2n since any such character factors through ℝ composed with the exponential map. That is, a character is a map of the form

exp(2πi⟨l∗,−⟩)

for some covector l∗∈V∗. The periodicity of exp(2πif(x)) for a linear f(x) gives the isomorphism of the character group with the real torus given above. In fact, this torus can be equipped with a complex structure, giving the dual complex torus.

Explicitly, a line bundle on T=V/Λ may be constructed by descent from a line bundle on V (which is necessarily trivial) and a descent data, namely a compatible collection of isomorphisms u∗𝒪V→𝒪V, one for each u∈Λ. Such isomorphisms may be presented as nonvanishing holomorphic functions on V, and for each u the expression above is a corresponding holomorphic function.

The Appell–Humbert theorem Template:Harv says that every line bundle on T can be constructed like this for a unique choice of H and α satisfying the conditions above.

Ample line bundles

Lefschetz proved that the line bundle L, associated to the Hermitian form H is ample if and only if H is positive definite, and in this case L⊗3 is very ample. A consequence is that the complex torus is algebraic if and only if there is a positive definite Hermitian form whose imaginary part is integral on Λ×Λ

See also

References