Alphabeta Math
ExampleConstruction: Literature-sourcedVerification: AI-adaptedPipeline-generatedprecheck passaudited 2026-10-02
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Oriented bases and SL2(Z)

Example

Let Λ=Z+iZ={m+ni:m,n∈Z}.

  1. The pairs (1,i) and (1+i,i) are bases of Λ of positive complex orientation and differ by an integer change-of-basis matrix of determinant 1;
  2. the pair (i,1) is a basis of Λ of negative orientation, and it differs from (1,i) by an integer matrix of determinant −1;
  3. all three pairs are bases of the same lattice, so they all define the same complex torus C/Λ and the same compact Riemann surface.

Facts & Assumptions

Given: The lattice Λ=Z+iZ, whose elements are the numbers m+ni with m,n∈Z and whose real-linear independence datum is i/1=i∉R.

[F1]

A basis of a lattice Λ is a pair (ω1,ω2) with Λ=Zω1+Zω2 and ω1,ω2 real-linearly independent; it is oriented when Im⁡(ω2/ω1)>0; two bases of the same lattice differ by a matrix in GL2(Z), and two oriented bases by a matrix in SL2(Z); the quotient torus and all its structure depend on the set Λ alone (Complex lattice and quotient torus).

[F2]

For a full lattice Λ the quotient TΛ=C/Λ is a compact Riemann surface with the quotient topology of the class map π, which is a holomorphic covering map (The quotient C/Λ is a compact Riemann surface).

Verification

1.1F1

The pair (1,i) is a basis of Λ: by definition Λ=Z⋅1+Z⋅i, and 1,i are real-linearly independent since i∉R; its orientation is positive because Im⁡(i/1)=1>0.

1.2F1algebra

The pair (1+i,i) is a basis of the same lattice: 1+i,i∈Λ, so Z(1+i)+Zi⊆Λ, while 1=(1+i)−i and i=i show the reverse inclusion; the change-of-basis matrix, whose columns are the new vectors in the old basis, expressing (1+i,i)=(ω1+ω2,ω2) in the basis (1,i) is (1011), of determinant 1, so the orientation is positive as well, and independently Im⁡(i/(1+i))=Im⁡((1+i)/2)=12>0.

1.3F1algebra

The pair (i,1) is a basis of Λ with change-of-basis matrix (0110) relative to (1,i), of determinant −1; its orientation is negative because Im⁡(1/i)=Im⁡(−i)=−1<0.

2.1F1F2step 1.1step 1.2step 1.3∎

By steps 1.1, 1.2 and 1.3 the three pairs are bases of the same lattice Λ, so they give the same quotient C/Λ and the same lattice sums, and by [F2] this quotient is a compact Riemann surface with holomorphic covering map π, independently of which basis is used to describe Λ.

The example illustrates that orientation is a property of an ordered basis, not of the lattice: (1,i) and (1+i,i) are related by the unipotent matrix (1011)∈SL2(Z), whereas swapping the two vectors multiplies the orientation sign by −1.

Depends on

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