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Periods of a complex torus

Statement

Assume the Axiom of Choice (The Axiom of Choice). Let Λ=Zω1+Zω2⊆C be a full lattice with oriented basis and let X=C/Λ be the associated complex torus with quotient map q:C→X (Complex lattice and quotient torus, The quotient C/Λ is a compact Riemann surface). Then:

  1. The translation-invariant differential dz descends to a nowhere-vanishing holomorphic differential on X; Ω(X)=C⋅dz, so X has genus 1, ℓ(K)=1 and deg⁡K=0 (The space of holomorphic differentials and the degree of the canonical divisor, Elliptic function for a lattice).
  2. With π1,π2 the loops t↦[tω1], t↦[tω2], the periods of dz are P(π1,dz)=ω1 and P(π2,dz)=ω2 (The period pairing and the period subgroup, Path integral of a holomorphic differential on a Riemann surface). Under the isomorphism Ω(X)∗≅C, α↦α(dz), the period lattice is exactly Λ, and Jac⁡(X)=C/Λ=X.
  3. For every base point p0∈X the point Abel-Jacobi map up0:X→Jac⁡(X)=X is a biholomorphism, and for D∈Div⁡0(X) one has u(D)=0 if and only if D is principal; equivalently Pic⁡0(X)≅X canonically (The Abel-Jacobi map embeds a positive-genus surface, Picard zero is the Jacobian). In particular, for points p,q∈X the class of the divisor (q)−(p) is the class of q−p in C/Λ.

Facts & Assumptions

Given: Full AC, a full lattice Λ=Zω1+Zω2, the torus X=C/Λ, and the loops π1,π2.

[F1]

X is a compact Riemann surface, the quotient map q is a holomorphic covering, and the charts are local inverses of q with translation transitions (The quotient C/Λ is a compact Riemann surface, Complex lattice and quotient torus).

[F2]

A holomorphic differential on X is equivalently a Λ-invariant holomorphic differential h(z) dz on C; the differential dz is invariant and nowhere vanishing, hence descends to a nowhere-vanishing holomorphic differential on X (Meromorphic differentials, orders and residues, Elliptic function for a lattice).

[F3]

If γ is a closed loop in X and γ~:[0,1]→C is a lift, then ∫γdz=γ~(1)−γ~(0)∈Λ: the integral of dz along a path is the difference of the endpoint values of any lift, because z is a primitive of dz on C and Λ is the group of deck translations. Conversely, for λ∈Λ the projection of t↦tλ is a loop with ∫dz=λ. Hence the period subgroup e(H1(X;Z)) equals Λ (Complex lattice and quotient torus, The quotient C/Λ is a compact Riemann surface, Path integral of a holomorphic differential on a Riemann surface).

[F4]

For a compact connected Riemann surface of genus g, dim⁡CΩ(X)=g and a nonzero holomorphic differential has exactly 2g−2 zeros counted with multiplicity (The space of holomorphic differentials and the degree of the canonical divisor).

[F5]

The path integral of a holomorphic differential is computed by local primitives; for dz on C a primitive is z, so the integral along a lifted path is the difference of its endpoints; the period pairing P agrees with integration over cycles and is additive (Path integral of a holomorphic differential on a Riemann surface, The period pairing and the period subgroup, The period pairing is well defined and computed by integration).

[F6]

The Jacobian is Ω(X)∗/Λ′ with Λ′=e(H1(X;Z)), the Abel-Jacobi map is represented by path integrals modulo Λ′, and for g=1 it is a biholomorphism onto the Jacobian; Pic⁡0(X)≅Jac⁡(X) canonically (The Jacobian of a compact Riemann surface, The Abel-Jacobi map, The Abel-Jacobi map is well defined and its degree-zero extension is base-point independent, The Abel-Jacobi map embeds a positive-genus surface, Picard zero is the Jacobian).

[F7]

Full AC is inherited from the Jacobian and classification interfaces; the example selects only the given lattice basis (The Axiom of Choice).

Verification

Given: The lattice, the torus and the two loops.

1.1F2F4

The translation action of Λ on C leaves dz invariant, so by [F2] dz descends to a holomorphic differential on X, and it is nowhere vanishing because its local expressions are the constant coefficient 1. Hence Ω(X)≠0, so g≥1 by [F4], and since a nonzero holomorphic differential has exactly 2g−2 zeros counted with multiplicity while dz has none, 2g−2=0 and g=1; then [F4] gives dim⁡CΩ(X)=1 and, since dz≠0, Ω(X)=C⋅dz with (dz)=0 of degree 0; in particular ℓ(K)=1 and deg⁡K=0.

1.2F3F5

The loops π1,π2 lift to the paths t↦tω1 and t↦tω2 on [0,1]; by [F5] the path integral of dz along π1 is ω1−0=ω1 and along π2 is ω2. By [F3] the period lattice is exactly e(H1(X;Z))=Λ; under Ω(X)∗≅C, α↦α(dz), the periods ω1,ω2 of the two standard loops are therefore the two generators of Λ. Hence Jac⁡(X)=C/Λ=X.

2.1F1F5F6step 1.1step 1.2

By [F5] the point map sends p=[z] to the class of the functional ω↦∫p0pω; under the identification Ω(X)=C dz of step 1.1 and Jac⁡(X)=C/Λ of step 1.2 this is the class of z−z0, that is, up0(p)=p−p0 in the group X. Hence up0 is the translation by −p0, a biholomorphism. Consequently u(D)=0 for D∈Div⁡0(X) exactly when ∑pnp(p−p0)=0 in C/Λ, i.e. when the group sum of D vanishes; by [F6] (Abel's criterion) this is exactly the condition that D is principal, and Pic⁡0(X)≅X. For D=(q)−(p) the class is q−p.

3.1F7step 1.1step 1.2step 2.1∎

The four displayed claims are steps 1.1, 1.2 and 2.1, under the inherited AC of [F7].

Source notes

Looijenga's Corollary 7.7 (Riemann Surfaces, printed p. 61) states that for genus one the point map is an isomorphism, so that S is isomorphic to a complex torus; McMullen (printed pp. 129 and 136) records that the periods of a one-form on a complex torus are its two generating periods. Forster's §20.8 (printed pp. 165-166) gives the doubly periodic Abel condition ∑ak≡∑bk(modΓ). The example spells out the invariant differential, the two period vectors and the resulting identification Jac⁡(X)=X.

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