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Level-One Modular Forms and the j-Invariant

1 · Prerequisites

2 · Summary

This page builds the classical theory of level-one modular forms from the action of the modular group. The group PSL2(Z) acts on the upper half-plane by Möbius transformations, and the reduction argument produces the standard fundamental domain D with its boundary identifications and its two elliptic classes, represented by i, ω and ω+1 in its closure; the quotient chart lemma then gives Γ\H a Riemann surface structure, with the ν-th-power chart at an elliptic point, and the cusp chart and compactness lemma adjoin the orbit of ∞ so that X(1)=PSL2(Z)\H∗ is a compact Riemann surface. On this curve a modular form of weight k is defined as a holomorphic function on H transforming by the factor (cτ+d)k and bounded at the cusp; equivalently its q-expansion has no negative powers, and the q-expansion principle records how the growth condition descends to the quotient.

The supply of forms comes from the lattice sums. The Eisenstein series Gk(τ)=∑′(mτ+n)−k converge absolutely and normally for even k≥4, uniformly on compact subsets of the half-plane, and the Lipschitz formula turns the sum into 2ζ(k) plus an explicit power series in q=e2πiτ, so that the normalised series Ek=Gk/(2ζ(k)) has q-expansion beginning 1+O(q) with coefficients −2kBkσk−1(n). The transformation law Gk(γτ)=(cτ+d)kGk(τ) then makes E4 and E6 modular forms of weights four and six, while the weight-two series is treated separately: its regularisation satisfies a transformation law with a non-vanishing correction term, so it is quasimodular rather than modular, and it is used in the discriminant computation.

The analytic heart of the page is the valence formula. Subtracting the contributions of the cusp and of the elliptic points from the boundary term of the argument principle gives ∑Pord⁡P(f)/νP+ord⁡∞(f)=k/12 for every nonzero weight-k form, and the boundary arc computation is what produces the k/12. The valence formula yields the location of the zeros of E4 and E6, the dimension formula dim⁡Mk=⌊k/12⌋+1 for even k≥0 with k≢2(mod12) and dim⁡Mk=⌊k/12⌋ for k≡2(mod12), with dim⁡Sk=dim⁡Mk−1 for even k≥4, and the fact that Δ=(E43−E62)/1728 is a cusp form of weight twelve with no zeros on H. The logarithmic derivative of the infinite product and the E2 transformation law give the product formula Δ=q∏n≥1(1−qn)24 and the integrality of its Fourier coefficients.

The final block assembles the graded ring and the invariant. The monomials E4aE6b with 4a+6b=k form a basis of Mk, so M∗=C[E4,E6] with E4 and E6 algebraically independent; the function j=E43/Δ is holomorphic on H, invariant under the modular group, and has a simple pole at the cusp, and the q-expansion j=q−1+744+196884q+⋯ has integral coefficients. The resulting map jˉ:X(1)→C^ is a biholomorphism, and through it the j-invariant classifies complex tori up to biholomorphism, with the square and hexagonal tori realising the values 1728 and 0.

3 · Logical flowchart

4 · Definitions, theorems and proofs

DefinitionDefinition: Literature-sourcedProof: Not applicablejudge pass (gpt-6.1-sol)Open item page →

The modular group and its action on the upper half-plane

Definition

Let

SL2(Z)={γ=(abcd):a,b,c,d∈Z, ad−bc=1},

a subgroup of GL2(R)⊆GL2(C) (Invertible matrices and the general linear group GL⁡n(F), GL⁡n(F) is a group under matrix multiplication, including the trivial group GL⁡0(F), The integers as equivalence classes of pairs of naturals, For same-sized finite square matrices over a commutative ring, det⁡(AB)=det⁡(A)det⁡(B)). Its centre is {±I}: the inclusion {±I}⊆Z(SL2(Z)) is immediate, {±I} is normal (The center of a group is a normal subgroup, Normal subgroup: invariance under conjugation), and conversely every 2×2 matrix commuting with all of SL2(Z) is scalar — in particular a matrix A=(abcd) commuting with both U=(1101) and L=(1011) satisfies c=0 and a=d from AU=UA, and then b=0 from AL=LA, by comparing entries of the two products, so A=aI is scalar; a scalar matrix λI of determinant 1 has λ2=1, so λ=±1 (Rectangular matrix multiplication and the identity matrix In, including zero-sized shapes). The modular group is the quotient

PSL2(Z):=SL2(Z)/{±I},

a group by For N⊴G, the cosets form a group with identity N and inverse (gN)−1=g−1N, The quotient group G/N and coset product (gN)(hN)=ghN, The canonical projection π:G→G/N, π(g)=gN, is a surjective group homomorphism.

For γ∈SL2(R) and τ∈H set γ⋅τ:=aτ+bcτ+d, the Möbius transformation attached to γ (Möbius transformations of the Riemann sphere, The unit disc, the upper half-plane, and Blaschke factors). The denominator does not vanish: cτ+d=0 would give τ=−d/c∈R when c≠0, and when c=0 invertibility gives d≠0. Writing cτ+d=(cRe⁡τ+d)+icIm⁡τ and using cτ+d‾=cτˉ+d, a direct computation gives

Im⁡(γ⋅τ)=Im⁡τ∣cτ+d∣2>0,

so H is stable under each γ, and γ↦γ⋅ is the restriction of the matrix-to-Möbius map, a group homomorphism (Möbius transformations form a group and identify with the projective linear quotient of GL_2(C), Actions of G on X correspond exactly to homomorphisms G→Sym⁡(X)); hence γ↦(τ↦γ⋅τ) is a left action of SL2(R) on H by biholomorphisms (Left group actions, transitive actions, and faithful actions, Every Möbius transformation is a biholomorphism of the Riemann sphere, Complex differentiability at a point, the complex derivative, holomorphic functions, and entire functions, Conjugation is an involutive real-field automorphism, zz‾=∣z∣2, and modulus is definite, multiplicative, and subadditive, Real and imaginary parts, complex conjugation, and modulus)).

The kernel of the restricted action of SL2(Z) is exactly {±I}: ±I act trivially, while a matrix acting trivially fixes the three distinct points i, i+1, 2i∈H, so it is the identity Möbius transformation and hence scalar — knowing that a Möbius transformation is determined by its values at three distinct points and that the kernel of the matrix-to-Möbius map is the scalar subgroup (A unique Möbius transformation carries any ordered triple of distinct sphere points to any other, Möbius transformations form a group and identify with the projective linear quotient of GL_2(C)) — and a scalar in SL2(Z) is ±I. The action therefore descends to a faithful action of PSL2(Z), the quotient by the normal subgroup {±I} (First isomorphism theorem for groups: G/ker⁡f≅im⁡f).

The elements S=(0−110) and T=(1101) act by S⋅τ=−1/τ and T⋅τ=τ+1. In SL2(Z) one computes S2=−I and (ST)3=−I: ST=(0−111) has (ST)2−ST+I=0 by direct multiplication, whence (ST)3=(ST)(ST−I)=−I. Hence S and ST have order 2 and 3 in PSL2(Z), so S2=1 and (ST)3=1 there.

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Reduction of orbits to the standard domain

Statement

Let Γ′=⟨S,T⟩≤PSL2(Z) and D‾={τ∈H:∣ℜτ∣≤1/2, ∣τ∣≥1}. (a) Every τ∈H is Γ′-equivalent to a point of D‾: among the points of the orbit Γ′⋅τ some point τ0 has maximal imaginary part; after applying a power of T one has ∣ℜτ0∣≤1/2, and then necessarily ∣τ0∣≥1. (b) For fixed τ∈H and N>0 there are only finitely many pairs (c,d)∈Z2 with ∣cτ+d∣≤N.

Facts & Assumptions

Given: τ=x+iy∈H, so y>0, and the action of Γ′ with ℑ(γ⋅τ)=ℑτ/∣cτ+d∣2 for the bottom row (c,d) of γ; T⋅τ=τ+1, S⋅τ=−1/τ (The modular group and its action on the upper half-plane).

[F1]

For z∈C, ∣Re⁡z∣≤∣z∣, ∣Im⁡z∣≤∣z∣, and ∣z∣2=zzˉ (Conjugation is an involutive real-field automorphism, zz‾=∣z∣2, and modulus is definite, multiplicative, and subadditive, Real and imaginary parts, complex conjugation, and modulus).

[F2]

A nonempty subset of Z that is bounded above has a greatest element and one that is bounded below has a least element; in particular the integers in a bounded interval form a finite set (A nonempty set of integers bounded above has a greatest element, and a nonempty set of integers bounded below has a least element). Every real has an integer part ⌊u⌋ with ⌊u⌋≤u<⌊u⌋+1 (Integer part: for every real x there is exactly one integer m with m≤x<m+1).

[F3]

If 0<r<1 then 1/r2>1 (Basic properties of the absolute value).

Proof

1.1F1F2givenalgebra

Fix N>0 and suppose ∣cτ+d∣≤N. Since Im⁡(cτ+d)=cy and Re⁡(cτ+d)=cx+d, [F1] gives ∣c∣y≤N, that is ∣c∣≤N/y; by [F2] only finitely many integers c satisfy this. For each such c, [F1] gives ∣cx+d∣≤N, so −N−cx≤d≤N−cx, and [F2] leaves only finitely many integers d. Hence only finitely many pairs (c,d) satisfy ∣cτ+d∣≤N.

2.1F1F2F3step 1.1givenalgebra∎

The set V:={∣cτ+d∣:γ∈Γ′ with bottom row (c,d)} is nonempty (the identity has value ∣0⋅τ+1∣=1) and every element is positive. Applying 1.1 with N=1 shows that the elements of V are among the finitely many numbers ∣cτ+d∣ attached to pairs with ∣cτ+d∣≤1, together with values >1; hence V has a least element m>0, realized by some γ0∈Γ′. Since ℑ(γ⋅τ)=y/∣cτ+d∣2, the point τ0:=γ0⋅τ of the orbit has maximal imaginary part y/m2: for every γ∈Γ′ with bottom row (c,d) one has ∣cτ+d∣≥m, so ℑ(γ⋅τ)=y/∣cτ+d∣2≤y/m2=ℑτ0. Choose n∈Z with ∣ℜτ0−n∣≤1/2, possible by taking n=⌊ℜτ0+1/2⌋ [F2]; then τ1:=T−n⋅τ0 satisfies ℑτ1=ℑτ0 (translation does not change the imaginary part) and ∣ℜτ1∣=∣ℜτ0−n∣≤1/2. If ∣τ1∣<1, then Sτ1∈Γ′⋅τ and ℑ(Sτ1)=ℑτ1/∣τ1∣2>ℑτ1 by [F1] and [F3], contradicting the maximality of ℑτ0=ℑτ1. Hence ∣τ1∣≥1, and τ1∈D‾ is the required Γ′-equivalent point.

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The standard fundamental domain, boundary identifications and elliptic stabilisers

Statement

Let D={τ∈H:∣ℜτ∣<1/2, ∣τ∣>1} and let D‾ be its closure in H. (a) D is a fundamental domain for PSL2(Z): every orbit meets D‾, no two points of D are equivalent, and two distinct points z,z′∈D‾ are equivalent if and only if either z′=z±1 with ℜz=∓1/2, or z′=−1/z with ∣z∣=1. (b) The only points of D‾ with nontrivial stabiliser are i, ω:=e2πi/3 and ω+1=eiπ/3: Stab⁡(i)=⟨S⟩ has order 2, Stab⁡(ω)=⟨ST⟩ has order 3, and Stab⁡(ω+1)=⟨TS⟩ has order 3 in PSL2(Z). (c) PSL2(Z)=⟨S,T⟩.

Facts & Assumptions

[F1]

Every Γ′-orbit meets D‾ (Reduction of orbits to the standard domain), and for γ=(abcd)∈SL2(Z) one has ℑ(γ⋅z)=ℑz/∣cz+d∣2, so ℑ(γ⋅z)≥ℑz is equivalent to ∣cz+d∣≤1 (The modular group and its action on the upper half-plane).

[F2]

Every z∈D‾ satisfies ∣ℜz∣≤1/2 and ∣z∣≥1, hence Im⁡z≥3/2 (The modular group and its action on the upper half-plane, Reduction of orbits to the standard domain).

Proof

1.1F1F2givenalgebra

Every Γ-orbit meets D‾, because Γ′≤Γ and every Γ′-orbit does [F1]. Suppose z,z′∈D‾ satisfy z′=γ⋅z with γ=(abcd)∈SL2(Z) and Im⁡z′≥Im⁡z; replacing γ by −γ, which gives the same element of Γ, we may assume c≥0. Then ∣cz+d∣≤1 by [F1], while Im⁡z≥3/2 by [F2]; hence ∣c∣ 32≤∣c∣Im⁡z=∣Im⁡(cz+d)∣≤∣cz+d∣≤1, so ∣c∣≤2/3<2 and therefore c∈{0,1}.

2.1F1F2step 1.1givencasesalgebra

Case c=0. Then d=±1 and γ=±(1m01), so z′=z+m with m∈Z. Since both points lie in D‾, ∣m∣=∣ℜz′−ℜz∣≤1. If m=0 then z′=z. If m=1 then ℜz′=ℜz+1≤1/2 and ℜz≥−1/2 force ℜz=−1/2; conversely for z∈D‾ with ℜz=−1/2 the point z′=z+1 lies in D‾, since 1/2≥ℜz′ and ∣z′∣=∣z−(−1)∣=∣ ∣z∣ ∣=∣z∣ holds because ∣z′∣2=∣z∣2+2Re⁡z+1=∣z∣2. The case m=−1 is the mirror image with ℜz=1/2.

2.2F1F2step 1.1givencasesalgebra

Case c=1. First suppose d=0. Then b=ad−1=−1 and ∣z∣=∣cz+d∣≤1≤∣z∣ shows ∣z∣=1; the map is z′=a−1/z=a−zˉ with a∈Z, and ∣ℜz′∣≤1/2, ∣ℜz∣≤1/2 give ∣a∣≤1. For a=0 this is z′=−1/z with ∣z∣=1; for a=−1 the condition ℜz′=−1−ℜz≥−1/2 forces ℜz=−1/2, so z=ω and z′=−1−zˉ=z; for a=1 we get ℜz′=1−ℜz≥1/2, forcing ℜz′=1/2 and ℜz=1/2, after which ∣z′∣2=1−2ℜz+∣z∣2=∣z∣2=1 and z′=1−zˉ=1−(12−iy)=12+iy=z. So for d=0 the only new identification is z′=−1/z when ∣z∣=1. Now suppose d≥1. Since ∣cz+d∣2−∣z∣2=2dRe⁡z+d2≤1−1=0, we get ℜz≤−d/2≤−1/2, so d=1 and ℜz=−1/2; then ∣z+1∣2=∣z∣2 and 1≤∣z∣, ∣z+1∣≤1 force ∣z+1∣=1=∣z∣, whence z=ω. Here b=a−1 and z′=a+ω (because 1/(1+ω)=−ω), so ℜz′=a−1/2∈[−1/2,1/2] gives a∈{0,1}: for a=0 one has z′=z, and for a=1 one has z′=ω+1=z+1. If d≤−1, write d=−k, k≥1; then ∣cz+d∣2−∣z∣2=−2kℜz+k2≤0 gives ℜz≥k/2≥1/2, so k=1, d=−1, ℜz=1/2, and ∣z−1∣=∣z∣=1 forces z=ω+1; with b=−a−1 and ω=ω+1−1 one computes z′=a+1+ω, so ℜz′=a+1/2∈[−1/2,1/2] gives a∈{−1,0}: for a=0 one has z′=z, and for a=−1 one has z′=ω=z−1.

3.1F1F3step 2.1step 2.2givenalgebra

Combining 1.1, 2.1 and 2.2: for any two Γ-equivalent points z,z′∈D‾ one of them, say the one with larger imaginary part, is of the listed shape; the case analysis gives either z′=z, or z′=z±1 with ℜz=∓1/2, or z′=−1/z with ∣z∣=1. Since the two identifications force ∣z∣=1 or ∣ℜz∣=1/2, neither can occur for two distinct points of D, whose points have ∣ℜz∣<1/2 and ∣z∣>1; this proves (a). For (b), a stabiliser element is a case with z′=z in the same analysis: besides the identity, this happens exactly for z=i with γ=±S, for z=ω with γ representing ST or (ST)2, and for z=ω+1 with γ representing TS or (TS)2. Since S2=(ST)3=(TS)3=1 in Γ and S≠1, ST≠1, these give Stab⁡(i)=⟨S⟩ of order 2 and Stab⁡(ω)=⟨ST⟩, Stab⁡(ω+1)=⟨TS⟩ of order 3, by [F3]; all other points of D‾ have trivial stabiliser.

4.1F3step 3.1givenalgebra∎

For (c) let γ∈Γ and fix z0:=2i∈D. By 1.1 there is γ1∈Γ′ with γ1⋅(γ⋅z0)∈D‾; set δ:=γ1γ∈Γ. Then z0∈D⊆D‾ and δ⋅z0∈D‾ are equivalent, so by (a) either δ⋅z0=z0 or one of the two boundary identifications holds; the latter are impossible because ∣z0∣=2>1 and ∣ℜz0∣=0<1/2. Hence δ stabilises z0, and by (b) the only points of D‾ with nontrivial stabiliser are i,ω,ω+1, none of which equals z0; so δ=1 and γ=γ1−1∈Γ′. Therefore Γ=Γ′=⟨S,T⟩.

LemmaStatement: Literature-sourcedProof: AI-adaptedjudge pass (gpt-6.1-sol)Open item page →

Local charts and the Riemann surface structure of a modular quotient

Statement

Let Γ≤PSL2(Z) have finite index, with quotient map p:H→Γ\H. (a) For every τ there is an open neighbourhood U of τ such that {γ∈Γ:γU∩U≠∅}=Stab⁡Γ(τ); stabilisers are finite cyclic, distinct orbits have disjoint invariant neighbourhoods, and p is open with Hausdorff quotient. (b) Γ\H carries a Riemann surface structure for which p is holomorphic and which is unique with that property: at a point with trivial stabiliser the local inverse of p is a chart; at an elliptic point, in a local coordinate z centred at it in which a generator of the stabiliser acts by z↦e2πi/νz, the ν-th power zν descends to a chart on the quotient.

Facts & Assumptions

Given: A finite-index subgroup Γ≤G:=PSL2(Z) acting on H by biholomorphisms (The modular group and its action on the upper half-plane, Left group actions, transitive actions, and faithful actions).

[F1]

Every point of H is G-equivalent to a point of D‾={τ:∣ℜτ∣≤1/2,∣τ∣≥1}, and the only points of D‾ with nontrivial G-stabiliser are i,ω,ω+1, with stabilisers cyclic of orders 2,3,3; G acts faithfully (The standard fundamental domain, boundary identifications and elliptic stabilisers, The modular group and its action on the upper half-plane).

[F2]

For fixed τ and N>0 only finitely many pairs (c,d)∈Z2 satisfy ∣cτ+d∣≤N (Reduction of orbits to the standard domain).

[F3]

A nonidentity Möbius transformation with two fixed points is conjugate to z↦λz, λ≠0,1 (Nonidentity Möbius transformations are parabolic or conjugate to a dilation, with the projective trace invariant); in a coordinate centred at a fixed point of an element of finite order ν, that element acts as z↦ζz with ζ a primitive ν-th root of unity, and Möbius transformations are biholomorphisms (Biholomorphic maps between complex domains).

[F4]

If f is holomorphic near a with f′(a)≠0, then f is biholomorphic between suitable neighbourhoods of a and f(a) (A nonzero complex derivative gives a local biholomorphism); a nonconstant holomorphic function has the local normal form ϕ(z)m (Local normal form of a nonconstant holomorphic map).

Proof

1.1F1F2F6givenalgebra

For compact sets K,L⊂H, only finitely many γ∈Γ satisfy γK∩L≠∅. Write z∈K, w=γz∈L; if yK≤ℑz≤YK, ℑw≥yL>0 and ∣ℜz∣≤XK, the height formula gives ∣cz+d∣2≤YK/yL. Thus ∣c∣≤YK/yL/yK and ∣d∣≤YK/yL+∣c∣XK, leaving finitely many integer bottom rows. For any fixed bottom row, all determinant-one top rows are (a0,b0)+k(c,d), so the corresponding maps are γ0z+k; the real parts of γ0(K) and L are bounded, leaving finitely many k. Apply this to a closed small disc about τ. The stabiliser is finite cyclic: conjugation into D‾ and [F1, F6] identify it with a subgroup of a cyclic group of order 1,2 or 3. For each of the finitely many non-stabilising maps meeting that disc, disjointness of its image of τ and τ permits shrinking the neighbourhood. Intersect its images under the finite stabiliser to obtain an invariant open U with γU∩U≠∅ exactly for stabiliser elements.

2.1F5step 1.1givenalgebra

If q,q′∈Γ\H are distinct, choose τ,τ′ with p(τ)=q, p(τ′)=q′; the set {γ∈Γ:γB(τ,δ)∩B(τ′,δ)≠∅} is finite for small δ by the same boundedness argument as in 1.1, and no element of it carries τ to τ′ because q≠q′; shrinking δ therefore gives disjoint open neighbourhoods U,U′ of τ,τ′ with γU∩U′=∅ for all γ∈Γ. Then ΓU and ΓU′ are disjoint Γ-invariant open sets, so q,q′ have disjoint neighbourhoods and the quotient is Hausdorff. The map p is open: for open V⊆H, the preimage p−1(p(V))=⋃γ∈ΓγV is open, so p(V) is open by definition of the quotient topology.

3.1F3F4F5step 2.1givenalgebra

Construction of charts. If Stab⁡Γ(τ)={1}, take U as in 1.1; then p∣U is injective, p(U) is open by 2.1, and p∣U−1 is a homeomorphism onto its image by [F5]; declare it a chart, and p is the identity map in these coordinates. If Stab⁡Γ(τ)=⟨γ0⟩ has order ν>1, then ν∈{2,3} by 1.1; by [F3] there is a biholomorphic coordinate z on a disc Δ centred at τ, z(τ)=0, in which γ0 acts by z↦ζz with ζ a primitive ν-th root of unity. Choose Δ so that {γ:γΔ∩Δ≠∅}=⟨γ0⟩; then z1ν=z2ν for z1,z2∈Δ exactly when z2=ζkz1 for some k (both are ν-th roots of the same number), so ψ:=zν induces a bijection Δ/⟨γ0⟩→Δ′ onto a disc Δ′ and this bijection is a homeomorphism by [F5]; since p(Δ)=Δ/⟨γ0⟩, the induced map p(Δ)→Δ′ is a chart on the quotient. In these coordinates p is the holomorphic map z↦zν, so p is holomorphic for the atlas.

4.1F4F5F7step 3.1algebra∎

Transition maps are holomorphic away from elliptic centres by the local inverse theorem [F4]. At a centre of order ν, a quotient-coordinate function pulled back to the uniformising coordinate has a holomorphic Taylor series h(z) invariant under z↦ζz; coefficient comparison gives h(z)=∑m≥0amνzmν=g(zν), with g holomorphic. Indeed its power series converges for ∣zν∣<rν whenever h converges for ∣z∣<r. This proves transition holomorphy also at the centre. Any other surface structure making p holomorphic has the same property for the pullback of each of its charts, so its charts are holomorphic functions of our quotient charts. These functions are injective, since both charts are homeomorphisms; their derivatives are therefore nonzero and their inverses are holomorphic. The two maximal atlases agree, proving uniqueness. The quotient is second countable: images under the open map p of a countable disc basis of H form a basis; it is connected as the continuous image of H. Thus the atlas defines a Riemann surface with all the topological hypotheses.

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The cusp chart and compactness of X(1)

Statement

Let H∗=H∪Q∪{∞} be the space obtained by adding the cusps, topologised by the usual topology on H together with, at γ⋅∞, the images under γ∈PSL2(Z) of the basic neighbourhoods {ℑτ>N}∪{∞} of ∞. Then the PSL2(Z)-action extends continuously to H∗, the cusps form the single orbit Q∪{∞}=PSL2(Z)⋅∞, and X(1)=PSL2(Z)\H∗ is compact Hausdorff with Y(1)=PSL2(Z)\H as a dense open subset whose complement is the single cusp class. The function q(τ)=e2πiτ descends to a homeomorphism of a neighbourhood of the cusp class onto an open disc in C and provides the cusp chart, so that X(1) is a compact Riemann surface.

Facts & Assumptions

Given: The action of G:=PSL2(Z)=⟨S,T⟩ on H with Sτ=−1/τ, Tτ=τ+1, its fundamental domain D, and the identification of G with its Möbius transformations on C^ (The modular group and its action on the upper half-plane, The standard fundamental domain, boundary identifications and elliptic stabilisers).

[F1]

Every orbit meets D‾={τ:∣ℜτ∣≤1/2,∣τ∣≥1}, no two distinct points of D are equivalent, and two distinct z,z′∈D‾ are equivalent exactly when z′=z±1 with ℜz=∓1/2 or z′=−1/z with ∣z∣=1 (The standard fundamental domain, boundary identifications and elliptic stabilisers).

[F2]

For finite-index Γ≤G the quotient Γ\H has the properties of Local charts and the Riemann surface structure of a modular quotient; in particular its quotient map is open and the quotient is Hausdorff.

[F3]

Quotient topologies, continuous maps, homeomorphisms, compactness and Hausdorffness are as in The quotient topology of a surjection, quotient maps, saturated sets, and the quotient of a space by an equivalence relation with its canonical projection, For a quotient map q:X→Y, a map out of Y is continuous iff its composite with q is; a continuous map on X constant on the fibres of q factors uniquely through q; and a composite of quotient maps is a quotient map, Homeomorphism, open map, closed map, embedding, and what it means for a property to be topological, A continuous bijection is a homeomorphism iff it is open iff it is closed, and homeomorphy is an equivalence relation on spaces, Hausdorff space: distinct points have disjoint open neighbourhoods; every metrizable space is Hausdorff and the indiscrete topology on two points is not, Open cover, subcover, and compact topological space; a compact subset is a subspace that is compact in its own right, Subspace topology: the traces of the open sets, its closed sets and its bases, the continuity of the inclusion, and the characteristic property of a map into a subspace, For a metric space with its metric topology, compactness in the topological sense is compactness in the metric sense, and the two notions of compact subset coincide, A continuous image of a compact space is compact; a continuous real-valued map on a nonempty compact space attains a maximum and a minimum; and a continuous bijection from a compact space to a Hausdorff space is a homeomorphism, In a Hausdorff space a point and a disjoint compact set, and two disjoint compact sets, have disjoint open neighbourhoods; hence every compact subset is closed, and in a compact Hausdorff space the compact subsets are exactly the closed ones, A continuous image of a connected space is connected, and connectedness is a topological property; complex structures and holomorphic maps are as in Riemann surfaces and holomorphic atlases and Holomorphic maps and meromorphic functions on Riemann surfaces.

Proof

1.1F2F3givenconstructalgebra

The action extends to H∗: for γ∈G and a cusp γ0⋅∞=m/n with m,n coprime, Bézout gives b,d∈Z with md−nb=1, so (mbnd)∈SL2(Z) and γγ0⋅∞=γ⋅(m/n); Möbius maps are homeomorphisms of C^ carrying Q∪{∞} to itself and the basic cusp neighbourhoods of γ0⋅∞ to basic cusp neighbourhoods of γγ0⋅∞, so the extended action is continuous and well defined. Every rational m/n in lowest terms equals γ⋅∞ for the matrix above with γ=(mbnd), and ∞ itself is in the orbit, so the cusps form the single orbit Q∪{∞}=G⋅∞.

1.2F2F3F4givenconstructalgebra

Fix N>1 and put BN:={ℑτ>N}∪{∞}. If γ∈SL2(Z) has c≠0 and z,γz∈H with ℑz,ℑγz>N, then ℑ(γz)=ℑz/∣cz+d∣2≤ℑz/(cℑz)2=1/(c2ℑz)<1/N<N, a contradiction; hence every γ mapping a point of BN back into BN has c=0, i.e. lies in ⟨T⟩. Consequently the G-orbit of a point of BN meets BN exactly in its ⟨T⟩-orbit, and BN/⟨T⟩ is identified with its image p(BN). By [F4] the map q(τ)=e2πiτ realises H/⟨T⟩≅{0<∣q∣<1}, so it descends to a homeomorphism of p(BN) onto {∣q∣<e−2πN} sending the cusp class to 0; the topology at the cusp was defined exactly so that {ℑτ>N′} corresponds to {∣q∣<e−2πN′}, so this is a homeomorphism onto the open disc and provides the cusp chart.

2.1F1F3step 1.1givenalgebra

Put K:=D‾∪{∞} with its subspace topology in H∗. Given an intrinsic open cover U of K, take U∞∈U containing ∞; the subspace topology and the cusp neighbourhood basis give N>1 with K∩BN⊆U∞. The set L:=D‾∩{ℑτ≤N} is closed and bounded in C, with imaginary part at least 3/2, hence compact by Heine-Borel in Rn: with the Euclidean metric a subset of Rn is compact if and only if it is closed and bounded, and the proof by bisection uses no choice principle; the same holds on the real line and the metric/topological compactness agreement in [F3]. Since H has its usual topology inside H∗, the topology induced on L from K is its usual subspace topology. Thus {U∩L:U∈U} is an intrinsic open cover of L and has a finite subcover. The corresponding finitely many members of U, together with U∞, cover K, proving its compactness. The quotient map p is continuous, so p(D‾∪{∞}) is compact by [F3]; it equals X(1) because every point of H is G-equivalent to a point of D‾ by [F1] and every cusp lies in the orbit of ∞ by 1.1. Hence X(1) is compact.

3.1F1F2F3F4step 1.2step 2.1algebra∎

To separate the cusp from an interior point p(τ), choose a relatively compact open neighbourhood U of τ with 0<y0≤ℑz≤Y on U. For every γ∈G, its height on U is at most M=max⁡(Y,1/y0): if c=0 height is unchanged, while if c≠0, ℑ(γz)≤1/(c2ℑz)≤1/y0. For N>max⁡(1,M) the open sets p(U) and p(BN) are disjoint. The quotient map on H∗ is open, since the saturation of each open set is the union of its translates; hence these are open neighbourhoods in X(1). Two interior points are separated by [F2], so X(1) is Hausdorff. The interior quotient is open and dense, since every cusp neighbourhood meets H; its complement is the unique cusp class. Its atlas [F2] is compatible with the cusp coordinate: for N>1 stabilisers on BN∩H are trivial and q′=2πiq≠0, so the transition to any local lift chart and its inverse are holomorphic. The inherited countable interior basis plus p(Bn), n≥2, gives second countability; connectedness follows from the connected dense interior. Together with 2.1 this makes X(1) a compact Riemann surface.

DefinitionDefinition: Literature-sourcedProof: Not applicablejudge pass (gpt-6.1-sol)Open item page →

The compactified level-one modular curve X(1)

Definition

Let H∗=H∪Q∪{∞} be the space of The cusp chart and compactness of X(1) with its cusp-neighbourhood topology and the action of PSL2(Z) (The modular group and its action on the upper half-plane, The quotient topology of a surjection, quotient maps, saturated sets, and the quotient of a space by an equivalence relation with its canonical projection). The compactified level-one modular curve is the quotient

X(1):=PSL2(Z)\H∗,

with the quotient topology and the structure of a compact Riemann surface whose interior quotient map H→X(1) is holomorphic and whose cusp coordinate is q=e2πiτ (The cusp chart and compactness of X(1), Riemann surfaces and holomorphic atlases); its single cusp is the class [∞]. The open modular curve is the dense open subset

Y(1):=PSL2(Z)\H=X(1)∖{[∞]},

whose Riemann surface structure is the one supplied by the local chart lemma for the quotient of the upper half-plane (Local charts and the Riemann surface structure of a modular quotient). More generally, for a finite-index subgroup Γ≤PSL2(Z) we write XΓ:=Γ\H∗ and YΓ:=Γ\H for the corresponding quotient spaces, with YΓ carrying the complex structure of Local charts and the Riemann surface structure of a modular quotient.

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The q-expansion principle at the cusp

Statement

Let f be holomorphic on H with f(τ+1)=f(τ) for all τ, and put q=e2πiτ. Then there is a unique holomorphic F on the punctured unit disc D∗={0<∣q∣<1} with f(τ)=F(e2πiτ). Moreover f is bounded on {ℑτ>Y0} for some Y0 if and only if F extends holomorphically to q=0, and then F(0)=lim⁡ℑτ→∞f(τ) and f(τ)−F(0)=O(e−2πδℑτ) for some δ>0 as ℑτ→∞. In particular f(τ)=∑n≥0anqn with an=(1/2πi)∮F(q)q−n−1 dq when the extension exists.

Facts & Assumptions

Given: A holomorphic, 1-periodic f on H and q=e2πiτ; the unit disc and half-plane are those of The unit disc, the upper half-plane, and Blaschke factors.

[F1]

∣e2πiτ∣=e−2πℑτ for every τ∈C (exp⁡(x+iy)=ex(cos⁡y+isin⁡y), ∣exp⁡(x+iy)∣=ex, and eiπ+1=0), and e2πiτ=e2πiτ′ if and only if τ−τ′∈Z (ker⁡(exp⁡)=2πiZ, and exp⁡z=exp⁡w exactly when z−w∈2πiZ).

[F2]

The principal logarithm L=Log⁡ is holomorphic on the slit plane C∖(−∞,0] and satisfies eL(w)=w there (The principal logarithm is the normalised holomorphic branch on the slit plane, Complex logarithms, the principal logarithm, and principal and multivalued complex powers).

[F4]

On a punctured disc 0<∣z−a∣<R, the singularity a is removable if and only if the function is bounded on some punctured neighbourhood of a; then the extension has value the limit at a (Characterizations of removable singularities).

[F5]

If a holomorphic function vanishes at a, then either it vanishes on a neighbourhood of a, or it has finite order m≥1 and factors locally as (z−a)mg with g holomorphic and g(a)≠0. In either case a function vanishing at 0 is q times a holomorphic function bounded near 0 (take the latter function to be zero in the first case) (The order of a zero is the exponent in its local holomorphic factorization).

[F6]

Every holomorphic function on an annulus has a convergent Laurent series (Laurent expansion on an annulus). The coefficients of a convergent Laurent series are the contour integrals 12πi∮f(ζ)(ζ−a)−n−1dζ, and they are unique (Laurent coefficients are given by contour integrals and are unique).

Proof

1.1F1F2F3givenconstruct

Let p(τ):=e2πiτ. For every q0∈D∗ there are an open disc V⊆D∗ about q0 and a holomorphic σ:V→H with p(σ(q))=q on V. Indeed, choose an angle α with e−iαq0∉(−∞,0] and let Sα={q:e−iαq∉(−∞,0]}; the function v(q):=L(e−iαq)+iα is holomorphic near q0 by [F2], and ev(q)=e−iαq⋅eiα=q by the addition law. Taking V a small disc contained in D∗∩Sα and setting σ(q):=−iv(q)/(2π) gives e2πiσ(q)=ev(q)=q, and σ is holomorphic by [F3]. Here ℑσ(q)>0 holds automatically: e−2πℑσ(q)=∣e2πiσ(q)∣=∣q∣<1 by [F1], so σ maps V into H.

2.1F1F3step 1.1givenalgebra

Define F(q):=f(σ(q)) for a local section σ as in 1.1; this is well defined. If σ,σ′ are two such sections near q, then p(σ(q))=q=p(σ′(q)), so σ(q)−σ′(q)∈Z by [F1], whence f(σ(q))=f(σ′(q)) by the periodicity of f. Since local sections exist near every q∈D∗, this gives a function F on all of D∗, holomorphic because near each point it is the composition f∘σ of holomorphic functions [F3]. If F~ is holomorphic on D∗ with f(τ)=F~(e2πiτ) for all τ, then for q∈D∗ and a local section σ with p(σ(q))=q we get F~(q)=F~(p(σ(q)))=f(σ(q))=F(q); hence F~=F and F is unique.

3.1F1F4F5step 1.1step 2.1givenalgebra

If F extends holomorphically to 0, then F is bounded on ∣q∣<δ for some δ>0; for ℑτ>−log⁡δ/(2π) one has ∣q∣<δ by [F1], so ∣f(τ)∣=∣F(q)∣ is bounded on that half-plane. Conversely, if ∣f∣≤M on {ℑτ>Y0}, then for 0<∣q∣<e−2πY0 any local section σ(q) of 1.1 satisfies ℑσ(q)=−log⁡∣q∣/(2π)>Y0 by [F1], so ∣F(q)∣=∣f(σ(q))∣≤M; by [F4] the singularity of F at 0 is removable, F extends holomorphically, and F(0)=lim⁡q→0F(q)=lim⁡ℑτ→∞f(τ) (given ε>0 choose δ with ∣F(q)−F(0)∣<ε for ∣q∣<δ; then ℑτ>−log⁡δ/(2π) gives ∣f(τ)−F(0)∣<ε). Finally, if the extension exists, either F−F(0) vanishes on a neighbourhood of 0, in which case take G:=0, or it vanishes to finite order m≥1 and [F5] writes F(q)−F(0)=qG(q) with G holomorphic near 0; in either case G is bounded near 0, so ∣f(τ)−F(0)∣=∣q∣ ∣G(q)∣≤Ce−2πℑτ for all large ℑτ, which is the asserted O(e−2πδℑτ) with δ=1.

4.1F4F6step 3.1algebra∎

Assume now that F extends holomorphically to 0. On the annulus 0<∣q∣<1 the holomorphic F has Laurent expansion ∑n∈Zanqn, and by [F6] an=12πi∮∣q∣=ρF(q)q−n−1dq for every 0<ρ<1. Since F is holomorphic at 0, all coefficients an with n<0 vanish (their principal part is zero, [F4] applied to the Laurent expansion), so F(q)=∑n≥0anqn and f(τ)=F(e2πiτ)=∑n≥0anqn converges for ∣q∣<1.

DefinitionDefinition: Literature-sourcedProof: Not applicablejudge pass (gpt-6.1-sol)Open item page →

Level-one modular forms and cusp forms

Definition

Fix an integer k. A modular form of weight k for PSL2(Z) is a holomorphic function f:H→C (Complex differentiability at a point, the complex derivative, holomorphic functions, and entire functions) such that

f(γ⋅τ)=(cτ+d)kf(τ)

for every γ=(abcd)∈SL2(Z) and every τ∈H (The modular group and its action on the upper half-plane), and such that the associated periodic function F of The q-expansion principle at the cusp is holomorphic at q=0. Since T=(1101) acts by τ↦τ+1 with factor 1, the law gives f(τ+1)=f(τ), so the q-expansion principle applies and F is the unique holomorphic function on 0<∣q∣<1 with f(τ)=F(e2πiτ). The form f is a cusp form if additionally F(0)=0.

Write Mk and Sk for the sets of modular and cusp forms of weight k. They are C-subspaces of the space of holomorphic functions on H: sums and scalar multiples of functions satisfying the transformation law satisfy it again, and the q-expansion condition is preserved because Faf+bg=aFf+bFg by uniqueness (Vector space over a field, Meromorphic functions on a plane domain). The transformation law is well posed: the factor (cτ+d)k depends only on γ and, by the cocycle identity for the Möbius action, the conditions for all γ are consistent (Möbius transformations form a group and identify with the projective linear quotient of GL_2(C)). Since −I∈SL2(Z) acts as the identity with factor (−1)k, one has f=(−1)kf, so Mk={0} for odd k. The weight condition is compatible with multiplication: MkMℓ⊆Mk+ℓ and SkMℓ⊆Sk+ℓ, because the products of the factors are (cτ+d)k+ℓ and the q-expansion of a product has constant term Ff(0)Fg(0).

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Absolute convergence and holomorphy of the lattice Eisenstein sums

Statement

For every even k≥4 and every τ∈H the family ((mτ+n)−k)(m,n)∈Z2∖{(0,0)} is absolutely summable, and the convergence is uniform on compact subsets of H. Consequently Gk(τ):=∑(m,n)′(mτ+n)−k defines a holomorphic function on H, and it depends only on the lattice Λτ=Z+Zτ assigned to τ.

Facts & Assumptions

Given: An even integer k≥4, the upper half-plane H with Im⁡>0 (The modular group and its action on the upper half-plane), and a compact K⊆H with Im⁡τ≥y0>0 and ∣Re⁡τ∣≤X for all τ∈K.

[F2]

If 0≤aj≤bj eventually and ∑bj converges then ∑aj converges (If 0≤ak≤bk eventually, convergence of ∑bk gives convergence of ∑ak, and divergence of ∑ak gives divergence of ∑bk); ∑jj−p converges for rational p>1 (For rational p>0, ∑1/kp converges iff p>1).

[F3]

For a complex double family with summable absolute values, apply the real double-series theorem separately to its real and imaginary parts. The family may then be summed in any order, in particular iterated or regrouped into shells (Fubini for double series: if ∑i∑j∣aij∣ converges then both iterated sums and the sum along every bijection N→N×N converge to one and the same value, If ∑∣ak∣ converges then ∑ak converges).

[F4]

If holomorphic functions on an open set converge locally uniformly, their limit is holomorphic (Locally uniform limits of holomorphic functions are holomorphic and their derivatives converge locally uniformly).

[F5]

∣z+w∣≥∣∣z∣−∣w∣∣, ∣zw∣=∣z∣∣w∣, and ∣Re⁡z∣≤∣z∣ (Conjugation is an involutive real-field automorphism, zz‾=∣z∣2, and modulus is definite, multiplicative, and subadditive, Real and imaginary parts, complex conjugation, and modulus).

Proof

1.1F5givenalgebra

Since mτ+n=0 with (m,n)≠(0,0) would give τ=−n/m∈R when m≠0 and n=0 when m=0, no denominator vanishes. Let cK:=min⁡(1/2, y0/max⁡(1,2X))>0. For (m,n)≠(0,0) and τ∈K we claim ∣mτ+n∣≥cKmax⁡(∣m∣,∣n∣). If ∣n∣≥2X∣m∣, then ∣Re⁡(mτ+n)∣=∣mRe⁡τ+n∣≥∣n∣−X∣m∣≥∣n∣/2 by [F5]; if moreover ∣n∣≥∣m∣ then ∣mτ+n∣≥∣n∣/2≥max⁡(∣m∣,∣n∣)/2, while if ∣n∣<∣m∣ then the imaginary part gives ∣mτ+n∣≥y0∣m∣=y0max⁡(∣m∣,∣n∣). If instead ∣n∣<2X∣m∣, then max⁡(∣m∣,∣n∣)≤max⁡(1,2X)∣m∣ and the imaginary part gives ∣mτ+n∣≥y0∣m∣≥y0max⁡(1,2X)max⁡(∣m∣,∣n∣). In all cases the claim holds.

2.1F1F2F3step 1.1givenalgebra

Regroup the nonzero pairs by the shell j:=max⁡(∣m∣,∣n∣)≥1; the shell has (2j+1)2−(2j−1)2=8j elements, and by 1.1 each contributes at most (cKj)−k, so shell j contributes at most 8cK−kj1−k. Since k≥4 gives k−1>1, the bound ∑j≥18cK−kj1−k<∞ follows from [F2]. The shell partial sums of the family are therefore nonnegative and bounded uniformly in τ∈K by an absolute constant, so they converge by the bounded-partial-sums criterion of [F1]; in the terminology of [F1] the family ((mτ+n)−k)(m,n)≠(0,0) is absolutely summable for each τ∈K, the regrouping being licensed by [F3], and the tail beyond shell J is bounded uniformly on K by 8cK−k∑j>Jj1−k.

3.1F3F4step 2.1givenalgebra∎

Each term τ↦(mτ+n)−k is holomorphic on H for (m,n)≠(0,0), being a power of the nonvanishing holomorphic function τ↦mτ+n. By 2.1 the partial sums over shells converge uniformly on every compact K⊆H (compactness supplies some y0,X), so [F4] makes the shell-sum limit Gk holomorphic on H, and this limit agrees with the (absolutely summable, hence order-independent by [F3]) family sum. Finally (m,n)↦mτ+n is a bijection of Z2 onto the lattice Λτ=Z+Zτ, so the summed family is exactly the family of values λ−k over the nonzero points λ∈Λτ; hence Gk(τ) depends only on Λτ and not on the enumeration.

DefinitionDefinition: Literature-sourcedProof: Not applicableOpen item page →

The divisor power sums σk

Definition

For an integer k≥0 and a positive integer n let

σk(n):=∑d∣n, 1≤d≤ndk,

the sum of the k-th powers of the positive divisors of n (Divisibility in Z: d∣a when a=dq for some integer q, Integer powers am, Finite sums and finite products, by recursion, The integers as equivalence classes of pairs of naturals). Thus σ0(n) is the number of positive divisors and σ1(n) is their sum. The sum is over the set of positive divisors of n, a finite set: it is nonempty because 1∣n, and it is bounded above by n when n≥1 (If d∣a and a≠0 then d≠0 and ∣d∣≤∣a∣; hence the set of divisors of a nonzero integer is bounded above by ∣a∣), so the displayed sum is a finite sum of integers. Each σk(n) is therefore a positive integer: by induction on k, d0=1>0 and dk+1=dkd>0 for every positive integer d, since positive integers are closed under multiplication (Integer powers am, The principle of mathematical induction, The integers form a totally ordered ring). The divisor d=1 contributes 1k=1, and adding the other positive integer summands preserves positivity by compatibility of the integer order with addition (The integers form a totally ordered ring). These functions are used only to express the Fourier coefficients of the Eisenstein series on this page.

DefinitionDefinition: Literature-sourcedProof: Not applicableOpen item page →

The level-one Eisenstein series E_k and the weight-two series E_2

Definition

For even k≥4 put

Gk(τ)=∑(m,n)∈Z2′(mτ+n)−k,τ∈H,

the prime excluding (m,n)=(0,0); this is an absolutely summable family whose sum is holomorphic in τ (Absolute convergence and holomorphy of the lattice Eisenstein sums). Define the normalised Eisenstein series

Ek:=Gk2ζ(k),ζ(k)=∑n≥1n−k,

the Riemann zeta value (The Riemann zeta function on the half-plane Re⁡s>1). For k>1 the series for ζ(k) converges (For rational p>0, ∑1/kp converges iff p>1), so 2ζ(k)>0 and the normalisation is well defined.

The constant term and the vanishing of the higher terms. Splitting the absolutely convergent sum into m=0 and m≠0, and bounding the latter with the Lipschitz formula (The Lipschitz formula for the reciprocal-power sums),

Gk(τ)=2ζ(k)+2∑m≥1(−2πi)k(k−1)!∑r≥1rk−1qmr,q=e2πiτ,

so Ek(τ)=1+O(q) as Im⁡τ→∞: the correction is a power series in q divisible by q, convergent for ∣q∣<1. The same computation yields the Fourier expansion of Eisenstein series are modular forms; their Fourier coefficients.

The weight-two series. Separately define

E2(τ):=1−24∑n≥1σ1(n)qn,q=e2πiτ,

with σ1(n) the sum of the positive divisors of n (The divisor power sums σk). Since σ1(n)≤n⋅n=n2 and ∑n≥1n2∣q∣n converges for ∣q∣<1 by the ratio test (Ratio test: lim sup⁡∣ak+1/ak∣<1 gives absolute convergence and hence convergence, and lim inf⁡∣ak+1/ak∣>1 gives divergence), the M-test (Weierstrass M-test for complex-valued function series, A complex power series converges absolutely and uniformly on every closed subdisc strictly inside its disc of convergence) makes E2 a holomorphic function of τ∈H. It is a quasimodular comparison object used in the discriminant product proof and in the counterexample item of the companion page; it is not itself a modular form, since its transformation law carries a nonzero correction term. The half-plane conventions are The modular group and its action on the upper half-plane.

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The Lipschitz formula for the reciprocal-power sums

Statement

For every integer k≥2 and every τ∈H, with q=e2πiτ, ∑n∈Z1(τ+n)k=(−2πi)k(k−1)!∑r=1∞rk−1qr, where the series on the left converges absolutely and the identity is independent of the order of summation.

Facts & Assumptions

Given: An integer k≥2, a point τ∈H, and q=e2πiτ.

[F1]

πcot⁡(πz)=1z+∑n≥1(1z−n+1z+n), and the series converges locally uniformly on C∖Z (The Mittag-Leffler expansion of pi cotangent).

[F2]

If the partial sums of ∑jgj of holomorphic functions converge locally uniformly to g, then g is holomorphic and g(m)=∑jgj(m) for every m, the derivative series again converging locally uniformly (A locally uniformly convergent series of holomorphic functions may be differentiated term by term, Complex analytic functions as locally representable by convergent power series).

[F3]

sin⁡z=eiz−e−iz2i, cos⁡z=eiz+e−iz2, and cot⁡z=cos⁡z/sin⁡z wherever sin⁡z≠0 (Complex sine, cosine, hyperbolic sine, and hyperbolic cosine from the complex exponential, Tangent, cotangent, secant, and cosecant on their exact natural domains).

[F4]

exp⁡(w+w′)=exp⁡(w)exp⁡(w′), exp⁡(2w)=exp⁡(w)2, exp⁡(−w)=1/exp⁡(w), and ∣exp⁡(x+iy)∣=ex for real x,y (exp⁡(z+w)=exp⁡z exp⁡w, and the complex exponential extends the real exponential, exp⁡(x+iy)=ex(cos⁡y+isin⁡y), ∣exp⁡(x+iy)∣=ex, and eiπ+1=0).

[F5]

exp⁡′=exp⁡; the chain rule and the algebra of derivatives give dmdwmeaw=ameaw and dmdwm1w+n=(−1)mm!(w+n)m+1 on their domains (The complex exponential is entire and its complex derivative is itself, The chain rule for complex derivatives, Linearity, product, reciprocal, and quotient rules for complex derivatives).

[F6]

Convergence in C is convergence in the metric d(z,w)=∣z−w∣ (The Euclidean metric, convergence, Cauchy sequences, and continuity on the complex plane); an absolutely convergent complex series converges, and every rearrangement of it has the same sum (Every absolutely convergent complex series converges, and rearrangements preserve its sum, Complex series, absolute convergence, complex power series, and radius of convergence).

Proof

1.1F1F3F4F6F7givenalgebra

The function z↦πcot⁡(πz) is holomorphic on the open set H⊆C∖Z, and by [F1] the partial sums of z−1+∑n≥1((z−n)−1+(z+n)−1) converge locally uniformly on H to it. Fix w with ∣w∣<1: the telescoping identity (1−w)∑m=0Nwm=1−wN+1, the convergence ∣w∣N+1→0 of [F7] and the metric description [F6] give ∣(1−w)∑m≤Nwm−1∣→0; dividing by the nonzero ∣1−w∣ proves ∑m≥0wm=1/(1−w). Now put u=eiπz and Q=u2=e2πiz by [F4]; then [F3] and [F4] give sin⁡(πz)=(u−u−1)/(2i)=(Q−1)/(2iu) and cos⁡(πz)=(u+u−1)/2=(Q+1)/(2u), so πcot⁡(πz)=πiQ+1Q−1=−πi(1+2∑r≥1Qr), because ∣Q∣=e−2πIm⁡z<1 for z∈H by [F4] and 1+Q1−Q=1+2∑r≥1Qr.

2.1F2F5step 1.1algebra

The series in 1.1 has holomorphic terms and locally uniformly convergent partial sums on H, so [F2] applies and, for m=k−1, differentiating termwise gives dk−1dzk−1πcot⁡(πz)=(−1)k−1(k−1)!∑n∈Z(z+n)−k on H, the displayed sum being understood through the absolutely convergent paired series of [F1] together with the term z−k differentiated from z−1; here dmdzm(z+n)−1=(−1)mm!(z+n)−m−1 by [F5]. On the other side the Q-series of 1.1 consists of entire terms with locally uniformly convergent partial sums, so differentiating it k−1 times termwise by [F2] and [F5] gives −2πi(2πi)k−1∑r≥1rk−1Qr as functions of z.

3.1F6F7step 2.1givenalgebra∎

Evaluating the two expressions of 2.1 at z=τ, where Q=e2πiτ=q, gives (−1)k−1(k−1)!∑n∈Z(τ+n)−k=−2πi(2πi)k−1∑r≥1rk−1qr. Dividing by the nonzero real number (−1)k−1(k−1)! yields the stated identity, since −2πi(2πi)k−1/(−1)k−1=(−2πi)k. Finally, for n≥2∣τ∣ one has ∣τ±n∣≥n−∣τ∣≥n/2, so ∑n≥1∣τ±n∣−k≤Cτ+2k+1∑n≥1n−k<∞ by [F7]; hence the family ((τ+n)−k)n∈Z is absolutely summable and, by [F6], every enumeration of it converges to the same sum, which is the order-independence asserted in the Statement.

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Eisenstein series are modular forms; their Fourier coefficients

Statement

For every even k≥4: (a) Ek is a modular form of weight k for PSL2(Z); (b) writing Bk for the k-th Bernoulli number, Ek(τ)=1−2kBk∑n≥1σk−1(n)qn, q=e2πiτ, with σk−1(n)=∑d∣ndk−1; (c) Ek(∞)=1, and Gk=2ζ(k)Ek; (d) in particular E4=1+240q+2160q2+O(q3) and E6=1−504q−16632q2+O(q3).

Facts & Assumptions

Given: Even k≥4, Gk(τ)=∑(m,n)′(mτ+n)−k and Ek=Gk/(2ζ(k)) (The level-one Eisenstein series E_k and the weight-two series E_2, The Riemann zeta function on the half-plane Re⁡s>1, The divisor power sums σk).

[F1]

The family ((mτ+n)−k) is absolutely summable with locally uniform convergence on H, and the action is by ℑ(γτ)=ℑτ/∣cτ+d∣2 with γ=(abcd) (Absolute convergence and holomorphy of the lattice Eisenstein sums, The modular group and its action on the upper half-plane).

[F2]

Lipschitz: ∑n∈Z(z+n)−k=(−2πi)k(k−1)!∑r≥1rk−1e2πirz for Im⁡z>0, absolutely convergent (The Lipschitz formula for the reciprocal-power sums).

[F3]

Mk is defined by the weight-k transformation law and holomorphy at the cusp, with Ek=1+O(q) (Level-one modular forms and cusp forms, The level-one Eisenstein series E_k and the weight-two series E_2); 2ζ(k)>0 and (m,n)↦(ma+nc,mb+nd) is a bijection of Z2 for γ∈SL2(Z) (The Riemann zeta function on the half-plane Re⁡s>1, Fubini for double series: if ∑i∑j∣aij∣ converges then both iterated sums and the sum along every bijection N→N×N converge to one and the same value).

[F4]

The even zeta values follow locally without a choice assumption. For ∣z∣<1, the cotangent expansion (The Mittag-Leffler expansion of pi cotangent) gives πzcot⁡(πz)=1−2∑m≥1ζ(2m)z2m: expand 2z2/(z2−n2) geometrically and interchange the sums, whose absolute total on ∣z∣≤r<1 is bounded by 2r2(1−r2)−1∑n≥1n−2. Put t=2πiz. The exponential definitions of sine and cosine give πzcot⁡(πz)=t/(et−1)+t/2. Comparing the coefficient of z2m in the Bernoulli generating series yields ζ(2m)=(−1)m+1B2m(2π)2m/(2(2m)!) (The Bernoulli numbers are defined by the generating series t/(et−1), Complex sine, cosine, hyperbolic sine, and hyperbolic cosine from the complex exponential, exp⁡(z+w)=exp⁡z exp⁡w, and the complex exponential extends the real exponential, Fubini for double series: if ∑i∑j∣aij∣ converges then both iterated sums and the sum along every bijection N→N×N converge to one and the same value, Ratio test: lim sup⁡∣ak+1/ak∣<1 gives absolute convergence and hence convergence, and lim inf⁡∣ak+1/ak∣>1 gives divergence).

Proof

1.1F1F3givenalgebra

Let γ=(abcd)∈SL2(Z). Writing mγτ+n=(ma+nc)τ+(mb+nd)cτ+d and using that (m,n)↦(ma+nc,mb+nd) is a bijection [F3], the absolute summability [F1] permits reindexing, so Gk(γτ)=(cτ+d)kGk(τ). Hence Ek(γτ)=(cτ+d)kEk(τ). By [F3], Ek=1+O(q) as Im⁡τ→∞, so in particular Ek is bounded near the cusp, and its periodic function F extends holomorphically to q=0 by the q-expansion principle; therefore Ek∈Mk and (a) holds.

1.2F2F3givenalgebra

Split the absolutely summable sum defining Gk into m=0 and m≠0. The m=0 part is ∑n≠0n−k=2ζ(k) because k is even. For m≠0 pair m with −m and n with −n; by [F3] this reindexing preserves the sum, and each remaining term with m≥1 is handled by [F2] applied to z=mτ (whose imaginary part is positive): ∑n∈Z(mτ+n)−k=(−2πi)k(k−1)!∑r≥1rk−1qmr. Therefore Gk=2ζ(k)+2(−2πi)k(k−1)!∑m≥1∑r≥1rk−1qmr=2ζ(k)+2(−2πi)k(k−1)!∑n≥1σk−1(n)qn, the last regrouping being the absolutely summable family (rk−1qmr)m,r≥1 grouped by n=mr [F3]: for ∣q∣≤ρ<1, its absolute sum is at most (1−ρ)−1∑r≥1rk−1ρr<∞ by the ratio test (Ratio test: lim sup⁡∣ak+1/ak∣<1 gives absolute convergence and hence convergence, and lim inf⁡∣ak+1/ak∣>1 gives divergence). Dividing by 2ζ(k) gives Ek=1+(−2πi)k(k−1)!ζ(k)∑n≥1σk−1(n)qn.

2.1F4step 1.2givenalgebra∎

For even k write k=2m. Then (−2πi)k=2kπk(−i)2m=(−1)m2kπk, and by [F4] ζ(2m)=(−1)m+1Bk(2π)k2k!, so (k−1)!ζ(k)=(−1)m+1Bk(2π)k2k and the coefficient of ∑σk−1(n)qn in 1.2 is (−1)m2kπk⋅2k(−1)m+1Bk(2π)k=−2kBk, proving (b). The constant term gives Ek(∞)=1 and Gk=2ζ(k)Ek, which is (c) (see [F3]). For (d): B4=−1/30 and B6=1/42, so −2⋅4B4=240 and −2⋅6B6=−504; with σ3(1)=1, σ3(2)=1+8=9 and σ5(1)=1, σ5(2)=1+32=33 this gives E4=1+240q+2160q2+O(q3) and E6=1−504q−16632q2+O(q3), as claimed. The special values used here are the local coefficient computation in [F4].

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The boundary arc contribution in the valence computation

Statement

Let k be even and let 0≠f∈Mk. On the unit-circle arc of the fundamental domain (away from the finitely many zeros and poles of f) one has the identity dlog⁡f(Sτ)=dlog⁡f(τ)+k dτ/τ with Sτ=−1/τ. Consequently, with the boundary orientation used in the argument-principle computation, the circular arc, traversed clockwise from ω to ω+1, of the positively oriented boundary of the truncated fundamental domain contributes the net amount πik/6 to ∮dlog⁡f (hence k/12 after division by 2πi), while the two vertical boundary sides cancel by T-invariance. If zeros lie on the boundary, these contributions mean limits after deleting paired neighbourhoods under S and T; the small indentation arcs are counted separately.

Facts & Assumptions

Given: Even k, a nonzero modular form f∈Mk (Level-one modular forms and cusp forms), and the standard domain D with Sτ=−1/τ, Tτ=τ+1, the arc being ∣τ∣=1 between ω=e2πi/3 and ω+1=eiπ/3 through i (The standard fundamental domain, boundary identifications and elliptic stabilisers).

[F1]

f(Sτ)=τkf(τ) for S=(0−110) and f(Tτ)=f(τ) (Level-one modular forms and cusp forms).

[F2]

Logarithmic derivative and the chain rule: on any region where a holomorphic g has no zeros, dlog⁡g=g′/g dτ; for c≠0, ddτlog⁡f(Sτ)=f′(Sτ)f(Sτ)⋅1τ2 (The logarithmic derivative of a meromorphic function, The chain rule for complex derivatives, Linearity, product, reciprocal, and quotient rules for complex derivatives).

[F3]

For a closed contour, ∮dlog⁡f is computed by the argument principle; reversal changes the sign, concatenation adds, and ∫γdτ/τ over a contour from a to b equals the increment of a logarithm, in particular ∫ωidτ/τ=log⁡i−log⁡ω (The integral of dz/(z−p) along a contour is the increment of a continuous logarithm, Rectifiable complex contours, reversal, concatenation, closedness, and orientation, The contour integral of a constant c is c times the endpoint displacement).

Proof

1.1F1F2givenalgebra

On a neighbourhood avoiding zeros, differentiate f(Sτ)=τkf(τ) and divide by that equality. The chain and product rules [F2] give f′(Sτ)f(Sτ)τ−2=f′(τ)f(τ)+k/τ, hence dlog⁡f(Sτ)=dlog⁡f(τ)+k dτ/τ. No global logarithm of f is required.

2.1F3step 1.1givenalgebra

Let L be the clockwise half-arc ω→i and R the half-arc i→ω+1. Since S(L) is R with reversed orientation, integrating 1.1 gives −∫Rdlog⁡f=∫Ldlog⁡f+k∫Ldτ/τ. Thus A:=∫Ldlog⁡f+∫Rdlog⁡f=−k∫Ldτ/τ=−k(iπ/2−2πi/3)=πik/6, and A/(2πi)=k/12. When boundary zeros occur, delete matching subarcs under S; the same equality holds on the remaining half-arcs, and the omitted integral of dτ/τ tends to zero. In particular it also applies when i or the endpoints are zeros.

3.1F1F3givenalgebra∎

Vertical sides: the right vertical side of the truncated domain is the image under T of the left vertical side, the map being orientation preserving on H; since f(Tτ)=f(τ) the logarithmic derivative is T-invariant, and the two sides are traversed in opposite directions as parts of the boundary, so their contributions to ∮dlog⁡f cancel. Hence the net contribution of the boundary pieces lying on ∂D is the arc contribution πik/6.

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The level-one valence formula

Statement

Let k be even and let f∈Mk with f≠0. Then ∑P∈PSL2(Z)\H1νPord⁡P(f)  +  ord⁡∞(f)  =  k12, where νP=2 if P is the class of i, νP=3 if P is the class of ω=e2πi/3, and νP=1 otherwise; ord⁡∞(f) is the order of vanishing at q=0 of the q-expansion from The q-expansion principle at the cusp.

Facts & Assumptions

Given: An even integer k, a nonzero f∈Mk, its q-expansion f(τ)=qng(q) with n=ord⁡∞(f), g holomorphic on ∣q∣<1 and g(0)≠0 (Level-one modular forms and cusp forms, The q-expansion principle at the cusp); the standard domain D with its closure D‾, the elliptic points i,ω,ω+1 and stabiliser orders νi=2, νω=νω+1=3 (The standard fundamental domain, boundary identifications and elliptic stabilisers).

[F1]

f is holomorphic on H; its zeros are isolated, and the identity theorem forces f≢0 on every connected open subset (Zeros of a nonzero holomorphic function are isolated, Identity theorem for holomorphic functions). Orders of zeros are defined by The order of a zero of a holomorphic function and the logarithmic derivative f′/f has a simple pole of residue m at a zero of order m (The logarithmic derivative has residue equal to local order, The logarithmic derivative of a meromorphic function, Meromorphic functions on a plane domain).

[F2]

Argument principle: for a meromorphic f admissible on a cycle Γ enclosing a region and nonvanishing on Γ, 12πi∫Γf′fdz=Z(f,Γ)−P(f,Γ) with the weighted counts of Zero and pole counts weighted by multiplicity and winding number (The argument principle for an admissible null-homologous cycle).

[F3]

On the truncated fundamental domain the circular arc contributes k/12 and the vertical sides cancel, in the sense of The boundary arc contribution in the valence computation; the truncation at height Y is legitimate because f=qng(q) with g(0)≠0 gives f′/f→2πin uniformly in Re⁡τ as Im⁡τ→∞.

[F4]

Representatives and angles: every class in PSL2(Z)\H has a representative in D‾, points of D have distinct classes, and the identifications of ∂D are only the T- and S-identifications; at i the domain subtends the angle π=2π/νi, at each of ω,ω+1 the angle π/3, and each of the two points is a representative of the single class of ω (The standard fundamental domain, boundary identifications and elliptic stabilisers, Local charts and the Riemann surface structure of a modular quotient, The compactified level-one modular curve X(1)).

Proof

1.1F1F2givenalgebra

Since f≢0 and f has isolated zeros, and since qng(q) with g(0)≠0 has no zeros for small ∣q∣, there are finitely many zeros of f in D‾∩{Im⁡τ≤Y} for each Y, and for large Y all zero classes have a representative there. Choose such a Y and ε>0 small, let R be the region obtained from D‾∩{Im⁡τ≤Y} by deleting the open discs of radius ε around each zero of f in that set (together with the strip Im⁡τ>Y), and let Γ=∂R with the positive orientation. Then f is holomorphic on a neighbourhood of R‾ and has no zeros on Γ, so by [F2] 12πi∮Γf′fdτ=0, and Γ consists of the top horizontal segment, the two vertical sides, the circular arc, cut where zeros occur, and the small circles (or circular arcs) around the zeros.

2.1F2F3step 1.1givenalgebra

The top segment is traversed from right to left; on it f′/f=2πin+o(1) uniformly in Re⁡τ as Y→∞ by [F3], so its contribution to 12πi∮ tends to −n. On the parts of Γ lying on the vertical sides of ∂D the integrand is T-invariant and the two sides are oppositely oriented, so they cancel exactly; the parts lying on the circular arc contribute k/12 in the limit ε→0 by [F3] (the cuts near zeros are accounted for with the small circles below).

2.2F1F4step 1.1givenalgebra

Consider a class P≠∞ with ord⁡P(f)=m>0 and all its representatives in the truncated domain. Near a zero τ0 of order m, f′/f=m/(τ−τ0)+holomorphic by [F1], so over a circular arc of angle θ around τ0 inside R the integral equals imθ+o(1) as ε→0, contributing −θm/(2π) to 12πi∮Γ (the boundary is traversed clockwise around the deleted disc). By [F4] the total angle of the sectors of R at all representatives of P is: 2π if P is a non-elliptic class (one interior representative, or two boundary representatives each contributing π), π=2π/νi for the class of i, and π/3+π/3=2π/3=2π/νω for the class of ω (represented by the two points ω and ω+1). Hence each class P≠∞ contributes −m/νP=−ord⁡P(f)/νP.

3.1F3step 2.1step 2.2givenalgebra∎

Summing 2.1 and 2.2 in the identity of 1.1 and letting Y→∞, ε→0 gives 0=k12−n−∑P≠∞ord⁡P(f)νP, that is ∑P≠∞1νPord⁡P(f)+ord⁡∞(f)=k12. All sums are finite by 1.1, and the term ord⁡∞(f)=n appears as the negative of the top-segment limit.

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The zeros of E4 and E6 at the elliptic points

Statement

E4 has a simple zero at the class of ω=e2πi/3 and no other zeros; E6 has a simple zero at the class of i and no other zeros. In particular E4 and E6 are nonzero modular forms with E4(∞)=E6(∞)=1, and E4 does not vanish at i while E6 does not vanish at ω.

Facts & Assumptions

Given: The Eisenstein series E4∈M4, E6∈M6 with E4(∞)=E6(∞)=1 (Eisenstein series are modular forms; their Fourier coefficients, The level-one Eisenstein series E_k and the weight-two series E_2), and the valence formula (The level-one valence formula).

[F1]

In the valence formula ∑Pord⁡P(f)/νP+ord⁡∞(f)=k/12, each summand ord⁡P(f)/νP is either 0 or at least 1/νP; the elliptic classes have νi=2 and νω=νω+1=3, all other classes have νP=1 (The level-one valence formula, The standard fundamental domain, boundary identifications and elliptic stabilisers).

Proof

1.1F1givenalgebra

For E4, k/12=1/3 and ord⁡∞(E4)=0 because E4(∞)=1≠0, so ∑Pord⁡P(E4)/νP=1/3. Every nonzero summand is at least 1/3 by [F1], with equality exactly for a simple zero at a class with νP=3, and the doubles 1/2,2/3,… and the integers 1,2,… are all strictly larger than 1/3. Hence exactly one summand is nonzero, namely a simple zero at a class with νP=3, and the only such class is that of ω. So E4 vanishes simply at the class of ω and nowhere else; in particular it does not vanish at i.

2.1F1step 1.1givenalgebra∎

For E6, k/12=1/2 and ord⁡∞(E6)=0, so ∑Pord⁡P(E6)/νP=1/2. A nonzero summand at the class of ω would be at least 1/3, leaving a total of at most 1/6 to be supplied by the remaining summands, of which every nonzero one is at least 1/2 (at i) or 1 (non-elliptic); this is impossible, so the class of ω is not a zero. The total 1/2 must then be a single summand at i (any non-elliptic zero contributes at least 1), and it equals 1/2 exactly for a simple zero at i. Hence E6 vanishes simply at the class of i and nowhere else, in particular not at ω.

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The dimension of the space of level-one modular forms

Statement

For even k≥0, dim⁡CMk={⌊k/12⌋+1,k≢2(mod12),⌊k/12⌋,k≡2(mod12), and dim⁡Sk=dim⁡Mk−1 for k≥4, while S0=0 and Sk=0 for 2≤k<12. In particular M0=C, M2=0, M4,M6,M8,M10 are one-dimensional, and M12 is two-dimensional. Moreover the forms E4aE6b with 4a+6b=k, a,b≥0, are linearly independent.

Facts & Assumptions

Given: The spaces Mk,Sk of level-one modular and cusp forms (Level-one modular forms and cusp forms), the valence formula, and the Eisenstein forms E4∈M4, E6∈M6 with constant term 1 at the cusp and zeros only at ω (for E4, simple) and i (for E6, simple) (The level-one valence formula, Eisenstein series are modular forms; their Fourier coefficients, The zeros of E4 and E6 at the elliptic points).

[F1]

Valence: for even k and 0≠f∈Mk, ∑P≠∞ord⁡P(f)/νP=k/12−ord⁡∞(f), all terms nonnegative with νP∈{1,2,3} (The level-one valence formula).

[F2]

The constant-term functional ε∞:Mk→C, f↦Ff(0)=f(∞), is linear and nonzero for k≥4 since ε∞(Ek)=1; Sk=ker⁡ε∞ by definition, and rank-nullity gives dim⁡Sk=dim⁡Mk−dim⁡im⁡ε∞ (Level-one modular forms and cusp forms, Eisenstein series are modular forms; their Fourier coefficients, Kernel and image of a linear map, The kernel and image are linear subspaces, and a linear map is injective if and only if its kernel is trivial, Rank and nullity of a linear map with finite-dimensional domain, Rank-nullity: dim⁡FV=nullity⁡T+rank⁡T, Vector space over a field).

[F3]

At the class of ω, ord⁡(E4)=1 and ord⁡(E6)=0; hence ord⁡ω(E4aE6b)=a for all a,b≥0 (The zeros of E4 and E6 at the elliptic points, The level-one valence formula).

Proof

1.1F1givenalgebra

Upper bound. Choose d:=⌊k/12⌋+1 distinct non-elliptic classes of points of H if k≢2(mod12), and d:=⌊k/12⌋ such classes if k≡2(mod12); such classes exist because non-elliptic classes are infinite. Suppose 0≠f∈Mk vanished at all chosen classes. Their total contribution to the valence sum is N≥d (each has νP=1). If k≢2(mod12) then d=⌊k/12⌋+1>k/12≥k/12−ord⁡∞(f), contradicting [F1]. If k≡2(mod12), write k=12q+2, so k/12=q+1/6 and d=q. If ord⁡∞(f)≥1 then the valence sum is at most q+1/6−1=q−5/6<q≤N, a contradiction. If ord⁡∞(f)=0, let m=ord⁡i(f), r=ord⁡ω(f) and N≥q the contribution of the remaining classes; multiplying the valence identity by 6 gives 6N+3m+2r=6q+1, so m is odd and r≡2(mod3); hence m≥1, r≥2 and N+m/2+r/3≥q+1/2+2/3=q+7/6>q+1/6=k/12, again contradicting [F1]. Therefore evaluation at the d chosen classes is injective on Mk, so dim⁡Mk≤d.

2.1F3step 1.1givenalgebra

Lower bound. If 4a+6b=4a′+6b′=k with a<a′ then ord⁡ω(E4aE6b)=a<a′=ord⁡ω(E4a′E6b′) by [F3], so in a linear relation ∑acaE4aE6b(a)=0 the term with least a, if its coefficient were nonzero, would give the sum the finite order a at the class of ω; since the sum is identically zero its order is infinite, so ca=0 for the least a, and induction gives that all coefficients vanish. Hence the monomials are linearly independent, so dim⁡Mk is at least their number. The pairs (a,b) with 4a+6b=k, a,b≥0, are indexed by the integers a≥0 with a≡k(mod3) and a≤k/4 (then b=(k−4a)/6≥0 is a nonnegative integer). Writing k=12q+s with s∈{0,2,4,6,8,10}, put a0∈{0,1,2} for the least nonnegative residue of s modulo 3. The solutions are a=a0+3j for 0≤j≤⌊(k/4−a0)/3⌋, so their number is max⁡(0,⌊(k/4−a0)/3⌋+1)=q+1 for s=0,4,6,8,10 and q for s=2; this is exactly ⌊k/12⌋+1 for k≢2(mod12) and ⌊k/12⌋ for k≡2(mod12). With 1.1 this proves the dimension formula.

3.1F2step 1.1step 2.1givenalgebra∎

Cusp forms and examples. For k≥4, ε∞ is nonzero and surjective onto C, so by [F2] dim⁡Sk=dim⁡Mk−1; for 0≤k<12 the formula gives dim⁡Mk=1 for k=0,4,6,8,10 and dim⁡M2=0, so Sk=0 there (for k=0,4,6,8,10 because the kernel of a nonzero functional on a one-dimensional space is zero, for k=2 because M2=0, and S0⊆M0). In particular M0=C (the constants lie in M0 and it is one-dimensional), M2=0, M4,M6,M8,M10 are one-dimensional, and M12 is two-dimensional. All the listed monomial counts are covered by 2.1, which also gives the asserted linear independence.

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The transformation law of the weight-two Eisenstein series E_2

Statement

The weight-two Eisenstein series E2(τ)=1−24∑n≥1σ1(n)qn satisfies E2(τ+1)=E2(τ) and, for every γ=(abcd)∈SL2(Z), E2 ⁣(aτ+bcτ+d)=(cτ+d)2E2(τ)−6icπ(cτ+d). In particular E2(−1/τ)=τ2E2(τ)−6iπτ, so E2 is not a modular form of weight 2.

Facts & Assumptions

Given: The series E2=1−24∑n≥1σ1(n)qn, q=e2πiτ, and its half-normalisation H:=(π2/6)E2, all on H (The level-one Eisenstein series E_k and the weight-two series E_2, The unit disc, the upper half-plane, and Blaschke factors).

[F1]

πcot⁡(πz)=1z+∑n≥12zz2−n2 with local uniform convergence on C∖Z (The Mittag-Leffler expansion of pi cotangent), and sin⁡w=w−w36+O(w5), cos⁡w=1−w22+O(w4) (The exponential definitions of complex sine, cosine, hyperbolic sine, and hyperbolic cosine equal their entire power series).

[F2]

Lipschitz: for τ∈H, ∑n∈Z(τ+n)−2=(−2πi)2∑r≥1rqr=−4π2∑r≥1rqr, absolutely on the left (The Lipschitz formula for the reciprocal-power sums).

[F3]

On every compact K⊆H there is cK>0 with ∣mz+n∣≥cKmax⁡(∣m∣,∣n∣) for all (m,n)≠(0,0) and z∈K This estimate is derived locally: if ℑz≥y0>0, ∣ℜz∣≤X, then ∣m∣≤∣mz+n∣/y0 and ∣n∣≤∣mz+n∣+X∣m∣≤(1+X/y0)∣mz+n∣, so one may take cK=min⁡(y0,(1+X/y0)−1).

[F5]

If G is differentiable on [n,n+1] with integrable G′=f, then ∫nn+1f=G(n+1)−G(n); consequently ∣f(n)−∫nn+1f∣≤2sup⁡[n,n+1]∣f′∣ (The second fundamental theorem: if G is differentiable on [a,b] with G′=f and f is integrable, then ∫abf=G(b)−G(a)).

[F6]

If φ(t,ε) and ∂εφ(t,ε) are continuous on R×I, one slice is absolutely integrable, and ∂εφ is dominated on each compact interval of ε by a t-integrable function, then Φ(ε)=∫Rφ(t,ε)dt is differentiable with Φ′(ε)=∫R∂εφ(t,ε)dt (Differentiation under an improper multiple integral under an integrable derivative bound).

Proof

1.1F1F4givenalgebra

We first record ζ(2)=π2/6. By [F1], πcot⁡(πz)=1z−2z∑n≥11n2−z2 for z∉Z; for ∣z∣≤1/2 one has 1n2−z2=1n2+z2n2(n2−z2) with ∣z∣2n2∣n2−z2∣≤2∣z∣2n4, so ∑n≥12zz2−n2=−2z∑n≥11n2+O(z3) by [F4] and πcot⁡(πz)=1z−2z∑n≥1n−2+O(z3). On the other hand [F1] gives πcot⁡(πz)=πcos⁡πzsin⁡πz=π1−(πz)2/2+O(z4)πz−(πz)3/6+O(z5)=1z−π23z+O(z3). Comparing coefficients of z and using ∑n−2>0 gives ∑n≥1n−2=π2/6.

2.1F2F3F4step 1.1givenalgebra

With q=e2πiτ and ∣q∣<1, [F2] gives ∑n∈Z(mτ+n)−2=−4π2∑r≥1rqmr for each m≥1, so ∑m≥1∑n∈Z(mτ+n)−2=−4π2∑m,r≥1rqmr=−4π2∑n≥1σ1(n)qn, the last step regrouping the absolutely summable family (rqmr)m,r≥1 by n=mr [F4]. Hence, by 1.1, H(τ)=ζ(2)+∑m≥1∑n∈Z(mτ+n)−2. For ε>0 define the regularised series Hε(z):=12∑(m,n)≠(0,0)′(mz+n)−2∣mz+n∣−2ε; pairing (m,n) with (−m,−n) and writing fm,ε(t):=(mz+t)−2∣mz+t∣−2ε, we have Hε(z)=ζ(2+2ε)+∑m≥1∑n∈Zfm,ε(n), and this family is absolutely summable for ε>0: on a compact K with c=cK, the shell of pairs with max⁡(∣m∣,∣n∣)=j has 8j elements each bounded by (cj)−2−2ε, so the shell sum is 8c−2−2εj−1−2ε, summable: compare with j−1−r for a rational 0<r<2ε and apply [F4].

3.1F3F4step 2.1givenalgebra

The regularised series satisfies Hε(γτ)=(cτ+d)2∣cτ+d∣2εHε(τ) for every γ=(abcd)∈SL2(Z). Indeed mγτ+n=m′τ+n′cτ+d with (m′,n′)=(ma+nc, mb+nd), and (m,n)↦(m′,n′) is a bijection of Z2 because its matrix (acbd) has determinant ad−bc=1; since (mγτ+n)−2∣mγτ+n∣−2ε=(cτ+d)2∣cτ+d∣2ε(m′τ+n′)−2∣m′τ+n′∣−2ε, the absolutely summable family of 2.1 may be reindexed and regrouped by [F4], giving the displayed law.

4.1F3F4F5step 3.1givenalgebra

Fix τ∈H, y:=Im⁡τ>0, and m≥1. Set Iε(mτ):=∫Rfm,ε(t) dt and Am(ε):=∑n∈Z[fm,ε(n)−∫nn+1fm,ε(t) dt]. The improper integral Iε(mτ) is the sum over n∈Z of ∫nn+1fm,ε, so ∑nfm,ε(n)=Iε(mτ)+Am(ε), and summing over m gives the exact identity Hε(τ)=ζ(2+2ε)+∑m≥1Am(ε)+∑m≥1Iε(mτ) for ε>0. The substitution mτ+t=my(u+i) shows Iε(mτ)=(my)−1−2εI(ε) with I(ε):=∫R(u+i)−2(1+u2)−εdu. Finally ∑m≥1Am(ε) converges uniformly for ε∈[−1/4,1/4]: by [F5], ∣fm,ε(n)−∫nn+1fm,ε∣≤2sup⁡[n,n+1]∣fm,ε′∣, and differentiating the product gives ∣fm,ε′(t)∣≤(2+2∣ε∣)∣mτ+t∣−3−2ε; on [n,n+1] the quantity ∣mτ+t∣ is comparable to ∣mτ+n∣ (their difference has modulus at most 1, and ∣mτ+t∣≥Im⁡mτ=my; for ∣mτ+n∣>2 this gives comparison, and only finitely many n fail it for a given m, none at all once my>2), so the absolute sum of all row differences is dominated uniformly in ε by a constant times ∑j≥18j j−5/2<∞ using [F3] and [F4]. The double series is thus uniformly convergent by the M-test; each row difference is continuous in ε, and regrouping into Am preserves the limit.

5.1F4F5F6step 2.1step 4.1givenalgebra

We let ε→0+. First, ζ(2+2ε)→ζ(2): for 0<ε≤1/4 and every N, ∣∑nn−2−2ε−∑nn−2∣≤∑n≤N∣n−2−2ε−n−2∣+2∑n>Nn−2, and the inner estimate is as small as desired for N large and then ε small. Second, ∑m≥1Am(ε)→∑m≥1Am(0) because the convergence is uniform on [−1/4,1/4] by 4.1 and each Am is continuous in ε; and Am(0)=∑n∈Z(mτ+n)−2 because I0(mτ)=∫R(mτ+t)−2dt=0, the primitive being −(mτ+t)−1. Third, I(0)=∫R(u+i)−2du=0 (same primitive) and I′(0)=−∫R(u+i)−2log⁡(1+u2) du=−π: the differentiation is licensed by [F6] separately on real and imaginary parts, with base slice ε=0 absolutely integrable (its modulus is (1+u2)−1), since for ∣ε∣≤1/4 the ε-difference quotients of (u+i)−2(1+u2)−ε are bounded by (1+u2)−3/4log⁡(1+u2), which is integrable on R, and a primitive of −log⁡(1+t2)/(t+i)2 is 1+log⁡(1+t2)t+i−arctan⁡t, whose endpoint difference is −π. Fourth, by [F5] and [F4] the decreasing function t↦t−1−2ε satisfies ∫1∞t−1−2εdt≤∑m≥1m−1−2ε≤1+∫1∞t−1−2εdt, that is ∑m≥1m−1−2ε=12ε+O(1). Hence ∑m≥1Iε(mτ)=y−1−2εI(ε)∑m≥1m−1−2ε→1y⋅(−π2)=−π2y as ε→0+, and therefore Hε(τ)→H(τ)−π2y, using 2.1, 4.1 and 2ε→0.

6.1step 3.1step 5.1givenalgebra∎

Taking ε→0+ in 3.1 and using 5.1 with ∣cτ+d∣2ε→1, H(γτ)−π2Im⁡(γτ)=(cτ+d)2(H(τ)−π2y). Since Im⁡(γτ)=y/∣cτ+d∣2, this rearranges to H(γτ)=(cτ+d)2H(τ)+π2y(∣cτ+d∣2−(cτ+d)2). Writing w:=cτ+d we have w2−∣w∣2=w(w−w‾)=2icy w, so the correction is −πic(cτ+d) and H(γτ)=(cτ+d)2H(τ)−πic(cτ+d). Multiplying by 6/π2 proves the stated transformation law; E2(τ+1)=E2(τ) is immediate from E2(τ+1)=1−24∑σ1(n)qn=E2(τ); and at γ=S, where c=1 and d=0, the law reads E2(−1/τ)=τ2E2(τ)−6iπτ, which differs from τ2E2(τ) for τ≠0, so E2 is not a modular form of weight 2.

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The discriminant is a nonvanishing cusp form of weight 12

Statement

Define Δ:=(E43−E62)/1728. Then Δ is a cusp form of weight 12 whose q-expansion is Δ(τ)=q−24q2+O(q3),q=e2πiτ; in particular Δ≠0 and ord⁡∞(Δ)=1, and the valence formula gives Δ(τ)≠0 for every τ∈H. Moreover E43 and E62 are linearly independent in M12, this space being two-dimensional with basis {E43,E62}.

Facts & Assumptions

Given: E4∈M4 and E6∈M6 with E4=1+240q+2160q2+O(q3) and E6=1−504q−16632q2+O(q3) (Eisenstein series are modular forms; their Fourier coefficients, The level-one Eisenstein series E_k and the weight-two series E_2, The divisor power sums σk).

[F1]

M12 is a two-dimensional complex vector space. Multiplication adds weights, with M4M4⊆M8, M8M4⊆M12 and M6M6⊆M12; the cusp forms are the kernel of the constant-term functional f↦f(∞) (The dimension of the space of level-one modular forms, Level-one modular forms and cusp forms).

[F2]

Valence formula: for even k and 0≠f∈Mk, ∑P≠∞ord⁡P(f)/νP=k/12−ord⁡∞(f) (The level-one valence formula).

Proof

1.1F1givenalgebra

E43∈M12 and E62∈M12 by [F1], hence Δ=(E43−E62)/1728∈M12. From the displayed expansions, E43=1+720q+(3⋅2160+3⋅2402)q2+O(q3)=1+720q+179280q2+O(q3) and E62=1−1008q+(5042−2⋅16632)q2+O(q3)=1−1008q+220752q2+O(q3). Therefore Δ=11728(1728q−41472q2+O(q3))=q−24q2+O(q3). In particular Δ≠0, Δ(∞)=0, so Δ is a cusp form, and ord⁡∞(Δ)=1.

2.1F1F2step 1.1givenalgebra∎

Applying the valence formula [F2] to Δ of weight 12 gives ∑P≠∞ord⁡P(Δ)/νP=12/12−1=0; every summand is a nonnegative multiple of 1/νP, so all vanish and Δ has no zeros on H. Finally, if aE43+bE62=0 then comparing constant terms gives a+b=0 and comparing q-coefficients gives 720a−1008b=0, whence (720+1008)a=0 and a=b=0; so E43,E62 are linearly independent in the two-dimensional space M12 and therefore form a basis.

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The modular discriminant and the j-invariant

Definition

The modular discriminant is

Δ(τ):=E4(τ)3−E6(τ)21728,

a cusp form of weight 12 with q-expansion q−24q2+O(q3) and without zeros on H (The discriminant is a nonvanishing cusp form of weight 12, Eisenstein series are modular forms; their Fourier coefficients). The j-invariant is the quotient

j(τ):=E4(τ)3Δ(τ),τ∈H,

which is holomorphic on H because Δ does not vanish there (Meromorphic functions on a plane domain). Since E43 and Δ both transform with the factor (cτ+d)12 under every γ∈SL2(Z), the quotient satisfies j(γ⋅τ)=j(τ) (Level-one modular forms and cusp forms).

The q-expansion and the cusp. From E43=1+720q+O(q2) and Δ=q(1−24q+O(q2)) (Eisenstein series are modular forms; their Fourier coefficients, The discriminant is a nonvanishing cusp form of weight 12),

j(τ)=q−11+720q+O(q2)1−24q+O(q2)=q−1+744+O(q),

so j has a simple pole at the cusp: its associated function of q is meromorphic at q=0 with a pole of order one. The special values follow from the zeros of E4,E6 (The zeros of E4 and E6 at the elliptic points): E6(i)=0 and E4(i)≠0 give j(i)=E4(i)3E4(i)3/1728=1728, while E4(ω)=0 gives j(ω)=0; the valence formula (The level-one valence formula) is what makes these the only relevant zeros.

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The graded ring of level-one modular forms

Statement

The graded C-algebra M∗=⨁k evenMk is freely generated by E4 and E6: the substitution X↦E4, Y↦E6 defines an isomorphism of graded C-algebras C[X,Y]→M∗, where deg⁡X=4 and deg⁡Y=6. Equivalently, for every even k≥0 the forms E4aE6b with 4a+6b=k, a,b≥0, form a basis of Mk, and the cusp forms form the principal ideal S∗=ΔM∗; explicitly Sk=ΔMk−12 for all k≥0 (with Mk−12=0 for k<12).

Facts & Assumptions

Given: The graded spaces Mk,Sk and the Eisenstein forms E4,E6 with E4(∞)=E6(∞)=1, together with Δ=(E43−E62)/1728∈S12 of order one at the cusp and without zeros on H (Level-one modular forms and cusp forms, Eisenstein series are modular forms; their Fourier coefficients, The discriminant is a nonvanishing cusp form of weight 12, The modular discriminant and the j-invariant).

[F1]

For even k the monomials E4aE6b with 4a+6b=k are linearly independent in Mk, and their number equals dim⁡Mk from the dimension formula; every such monomial has value 1 at the cusp (The dimension of the space of level-one modular forms, Eisenstein series are modular forms; their Fourier coefficients).

[F2]

A nonzero weight-k form has a well-defined constant term f(∞) at the cusp, and Sk is exactly the kernel of f↦f(∞) (Level-one modular forms and cusp forms).

[F3]

Δ has vanishing order 1 at the cusp and no zeros on H; therefore f↦f/Δ maps Sk bijectively onto Mk−12 for every even k: it is holomorphic on H, has the correct weight, and at the cusp the order drops by exactly 1; conversely Δh∈Sk for h∈Mk−12 (The discriminant is a nonvanishing cusp form of weight 12, The modular discriminant and the j-invariant, The level-one valence formula, The zeros of E4 and E6 at the elliptic points).

[F4]

For every even k≥4 there is a monomial of weight k (and for k=0 the empty monomial 1); M2=0 and Mk is one-dimensional for k=0,4,6,8,10 (The dimension of the space of level-one modular forms).

Proof

technique · induction on the weight $k$ in steps of $12$
1.1baseF1F2F4givenalgebra

Base cases: for k=0, M0=C consists of constants and the empty monomial 1 has weight 0; for k=2, M2=0; for k=4,6,8,10 the space Mk is one-dimensional and contains the monomial E4,E6,E42,E4E6 respectively, whose value at the cusp is 1, so every f∈Mk equals f(∞) times that monomial. Hence in these degrees the monomials span Mk.

1.2ihgiven

Assume, as induction hypothesis, that for some even k≥12 the weight-(k−12) monomials span Mk−12; equivalently every element of Mk−12 is a polynomial in E4,E6.

2.1F2F3F4step 1.1step 1.2givenalgebra

Let f∈Mk and choose a monomial P=E4aE6b of weight k [F4]; then P(∞)=1 and f−f(∞)P∈Mk has zero constant term at the cusp, so f−f(∞)P∈Sk [F2]. By [F3] there is h∈Mk−12 with f−f(∞)P=Δh; by the induction hypothesis 1.2 the form h is a polynomial in E4,E6, so f=f(∞)P+Δh is a polynomial in E4,E6 (using Δ=11728(E43−E62)). Hence the monomials span Mk for every even k≥0.

3.1F1F3step 2.1discharge-induction∎

The graded algebra map φ:C[X,Y]→M∗ with φ(X)=E4, φ(Y)=E6 is well defined because E4aE6b∈M4a+6b and multiplication of modular forms adds weights. In degree k the source is spanned by the monomials of weight k, whose images are linearly independent and as numerous as dim⁡Mk [F1]; since they also span Mk by the induction result, φ is an isomorphism in each degree and hence an isomorphism of graded algebras. Therefore the monomials form a basis and E4,E6 are algebraically independent. Finally [F3] gives Sk=ΔMk−12 for every k, that is S∗=ΔM∗.

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The j-invariant classifies complex tori

Statement

For a full lattice Λ⊂C with oriented basis (ω1,ω2) put τ=ω2/ω1∈H and j(Λ):=j(τ), with j the modular function of The modular discriminant and the j-invariant; this is well defined because another oriented basis changes τ by an element of SL2(Z) and j is invariant. For full lattices Λ,Λ′ the following are equivalent: (i) Λ′=cΛ for some c∈C× (the lattices are homothetic); (ii) the complex tori C/Λ and C/Λ′ are biholomorphic; (iii) j(Λ)=j(Λ′).

Facts & Assumptions

Given: Full lattices Λ,Λ′ with oriented bases, the complex tori TΛ,TΛ′ and their class maps π,π′ (Complex lattice and quotient torus, The quotient C/Λ is a compact Riemann surface), and the modular function j with j(γτ)=j(τ) for γ∈SL2(Z) (The modular discriminant and the j-invariant, The modular group and its action on the upper half-plane).

[F1]

A change of oriented basis is an element of SL2(Z) acting on τ=ω2/ω1 by the associated Möbius transformation; hence j(Λ) is well defined (Complex lattice and quotient torus, The modular discriminant and the j-invariant).

[F2]

For c∈C×, multiplication by c maps Λ onto cΛ and induces a biholomorphism TΛ→TcΛ; the oriented basis (cω1,cω2) has ratio τ=ω2/ω1 unchanged, so j is a homothety invariant (Complex lattice and quotient torus, Biholomorphic maps between complex domains).

[F3]

For a lattice Λ, π:C→TΛ is a holomorphic covering map and C is simply connected; hence for any continuous G:C→TΛ and basepoint there is a unique based lift f:C→C (The quotient C/Λ is a compact Riemann surface, Covering maps, evenly covered neighbourhoods, fibres, sheets, and trivial coverings, Every nonempty convex subset of Rn is simply connected, Lifting criterion for maps from path-connected locally path-connected spaces).

[F4]

Every biholomorphic self-map of C is affine f(z)=az+b, a≠0 (Every biholomorphic self-map of the complex plane is affine); an injective holomorphic map has nowhere-vanishing derivative (An injective holomorphic map has no critical point and is biholomorphic onto its image, Local normal form of a nonconstant holomorphic map).

[F5]

For f=E43−μΔ with finite μ, f(∞)=1 and the valence sum is 1. Moreover f=Δ(j−μ) and Δ is nonzero on H. The invariant holomorphic function j−μ factors in each elliptic chart through zν, where ν=2 or 3 (Local charts and the Riemann surface structure of a modular quotient); consequently each zero of f has order a positive multiple of ν at such a point, and weighted contribution at least 1. At ordinary points its order is at least 1. Thus f has exactly one zero class (The level-one valence formula, The discriminant is a nonvanishing cusp form of weight 12, The modular discriminant and the j-invariant).

[F6]

Λγτ=(cτ+d)−1Λτ for γ=(abcd)∈SL2(Z), directly from Z+Zγτ=Z+Zaτ+bcτ+d=(cτ+d)−1(Z(cτ+d)+Z(aτ+b)) (Complex lattice and quotient torus, The modular group and its action on the upper half-plane); and dim⁡M12=2 with E43,Δ a basis (The graded ring of level-one modular forms).

Proof

1.1F1F2givenalgebra

If Λ′=cΛ then multiplication by c is a biholomorphism TΛ→TΛ′ by [F2], so (i) implies (ii). Writing Λ=Zω1+Zω2=ω1Λτ with τ=ω2/ω1, the lattice Λ′ has the same normalised parameter τ, so j(Λ′)=j(τ)=j(Λ); hence (i) implies (iii). If Λ′′ is another basis of Λ, it is related to (ω1,ω2) by a matrix in SL2(Z) and the new parameter is γτ, so j is unchanged by [F1].

2.1F2F3F4step 1.1givenalgebra

Suppose (ii): let F:TΛ→TΛ′ be a biholomorphism. Composing with a translation of TΛ′ if necessary we may assume F([0])=[0], since translations are biholomorphisms. Put G:=F∘π:C→TΛ′; as C is simply connected and π′ is a holomorphic covering [F3], there is a unique based lift f:C→C with π′∘f=G and f(0)=0. Similarly the inverse F−1 admits a based lift f~ with f~(0)=0. Both f~∘f and the identity are based lifts of F−1∘F∘π=π=π∘id⁡, so by uniqueness f~∘f=id⁡, and symmetrically f∘f~=id⁡; thus f is a biholomorphism of C (it is holomorphic because locally it is a branch of the holomorphic covering π′ composed with G). By [F4] f(z)=az+b with a≠0, and f(0)=0 gives b=0, so f(z)=az. For every λ∈Λ, π′(f(z+λ))=G(z+λ)=G(z) because π is Λ-periodic, so f(z+λ)−f(z)=aλ∈ker⁡π′=Λ′; hence aΛ⊆Λ′. Applying the same argument to f~, whose affine form is a−1z, gives a−1Λ′⊆Λ, so aΛ=Λ′ and Λ′ is homothetic to Λ: (ii) implies (i).

3.1F5F6step 2.1givenalgebra∎

Suppose (iii): j(τ)=j(τ′) where Λ=ω1Λτ, Λ′=ω1′Λτ′; set μ=j(τ)=j(τ′). The form f:=E43−μΔ∈M12 has f(τ)=0=f(τ′) and f(∞)=1, so f≠0 and by [F5] all zeros of f, in particular τ and τ′, lie in one PSL2(Z)-class: there is γ∈SL2(Z) with τ′=γτ. Then Λτ′=Λγτ=(cτ+d)−1Λτ by [F6] is homothetic to Λτ, hence Λ′ is homothetic to Λ and (i) holds. The three implications close the equivalence.

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The j-invariant uniformizes X(1)

Statement

The function j descends to a holomorphic map jˉ:X(1)→C^ of compact Riemann surfaces, with jˉ([∞])=∞ and a simple pole at the cusp, and jˉ is a biholomorphism. Consequently X(1) is biholomorphic to the Riemann sphere and j is a Hauptmodul. The quotient map π:H→Y(1)⊂X(1) has local degree 2 at i and 3 at ω and ω+1, representatives of the classes of i and ω; more generally its local degree is 2 throughout PSL2(Z)⋅i, 3 throughout PSL2(Z)⋅ω, and 1 elsewhere. These ramification indices belong to π, while jˉ itself is unramified, so the composed map j=jˉ∘π:H→C^ has local degree 2 at i and 3 at ω and ω+1.

Facts & Assumptions

Given: The compact Riemann surface X(1)=PSL2(Z)\H∗ with its cusp [∞], the open part Y(1), and the quotient charts at elliptic points and at the cusp (The compactified level-one modular curve X(1), The cusp chart and compactness of X(1), Local charts and the Riemann surface structure of a modular quotient); the modular function j with j(γτ)=j(τ), holomorphic on H, and with j=q−1+744+O(q) at the cusp (The modular discriminant and the j-invariant).

[F1]

j is injective on PSL2(Z)-classes: if j(τ)=j(τ′) then the lattices Λτ,Λτ′ are homothetic, hence τ′=γτ for some γ∈SL2(Z) and [τ]=[τ′] in Y(1) (The j-invariant classifies complex tori).

[F2]

For λ∈C the form E43−λΔ∈M12 is nonzero with value 1 at the cusp, and its valence sum is 12/12=1>0, so it has a zero in H; hence j takes the value λ (The level-one valence formula, The modular discriminant and the j-invariant, The zeros of E4 and E6 at the elliptic points, The graded ring of level-one modular forms).

[F3]

Local normal form: a nonconstant holomorphic map of Riemann surfaces has, near a point, the form z↦zν in suitable coordinates; an injective holomorphic map of domains has nowhere-vanishing derivative and is biholomorphic onto its image (Local power-map normal form on Riemann surfaces, Ramification index, ramification order and branch value, An injective holomorphic map has no critical point and is biholomorphic onto its image, Biholomorphic maps between complex domains).

[F4]

In the quotient chart of Local charts and the Riemann surface structure of a modular quotient the map π near i is z↦z2 and near ω or ω+1 is z↦z3, these being the local degrees 2 and 3; jˉ will be unramified once it is shown biholomorphic, since biholomorphic maps have local degree one (Ramification index, ramification order and branch value).

Proof

1.1F4givenalgebra

On Y(1) the invariance and holomorphy of j produce a holomorphic function jˉ:Y(1)→C: at ordinary points use a local inverse of π; at a point of stabiliser order ν, the invariant Taylor series in a uniformising coordinate z has only powers zmν, so it is holomorphic in the quotient coordinate zν. Near the cusp, in the q-chart of The cusp chart and compactness of X(1), j is q−1(1+744q+O(q2)), a meromorphic function of q with a simple pole at q=0; since the cusp chart identifies the cusp with q=0, the formula q↦q−1(1+744q+⋯ ) defines a holomorphic map of a punctured disc into C^ extending to 0 with value ∞. Hence jˉ extends to a holomorphic map X(1)→C^ with jˉ([∞])=∞ and a simple pole in the q-coordinate.

2.1F1step 1.1givenalgebra

jˉ is injective. If jˉ([τ])=jˉ([τ′]) then j(τ)=j(τ′) (for τ,τ′∈H) and [F1] gives [τ]=[τ′]; on Y(1) this is the claim, and the cusp is the only remaining point, with jˉ([∞])=∞ not attained on Y(1) because j is holomorphic on H.

3.1F2step 2.1givenalgebra

jˉ is surjective: given λ∈C, [F2] provides τ∈H with j(τ)=λ, so λ is in the image, while ∞=jˉ([∞]); hence jˉ(X(1))=C^.

4.1F3F4step 3.1givenalgebra∎

A bijective holomorphic map of compact Riemann surfaces is a biholomorphism: at every point the local normal form is z↦zν, and injectivity forces ν=1, so the derivative is never zero and the map is locally biholomorphic by [F3]; a locally biholomorphic bijection has holomorphic inverse, so jˉ is biholomorphic and X(1)≅C^ with j a Hauptmodul. The local degrees of π at i and at ω,ω+1 are 2 and 3 by [F4], the same indices hold at all their modular translates because the group acts by biholomorphisms and π∘γ=π; outside these two orbits the stabilisers are trivial and the local degree is 1; since jˉ is unramified, the composition j=jˉ∘π has exactly these local degrees at the corresponding points, in particular 2 at i and 3 at ω and ω+1.

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Jacobi theta triple product and nonvanishing of the theta constant

Statement

For τ∈H, z∈C and Q=eπiτ, Θ(z∣τ):=∑m∈ZQm2e2πimz=∏n≥1(1−Q2n)(1+Q2n−1e2πiz)(1+Q2n−1e−2πiz). The series and product converge locally uniformly in each variable, uniformly on compact products. For fixed τ, Θ is entire in z with exactly the simple zeros z=(1+τ)/2+a+bτ, a,b∈Z. In particular θ(τ):=Θ(0∣τ)=∏n≥1(1−Q2n)(1+Q2n−1)2≠0. Here Q2=q; these cusp parameters must not be confused.

Facts & Assumptions

Given: τ∈H, z∈C and Q=eπiτ, so ∣Q∣=e−πIm⁡τ<1 (The unit disc, the upper half-plane, and Blaschke factors).

[F3]

Normally convergent products of holomorphic functions have holomorphic limits; on a compact set the zeros are exactly those of the finitely many factors that vanish there, and the tail is zero-free (Normally convergent products define holomorphic functions with the expected zeros, Normal convergence of holomorphic products).

[F4]
[F5]

If f is holomorphic near a and vanishes there to order one, then f=(z−a)g with g holomorphic and g(a)≠0 (The order of a zero is the exponent in its local holomorphic factorization).

[F6]

ker⁡exp⁡=2πiZ, exp⁡(w+w′)=exp⁡wexp⁡w′, exp⁡(2w)=exp⁡(w)2, exp⁡w≠0, and ∣exp⁡(x+iy)∣=ex for real x,y (ker⁡(exp⁡)=2πiZ, and exp⁡z=exp⁡w exactly when z−w∈2πiZ, exp⁡(z+w)=exp⁡z exp⁡w, and the complex exponential extends the real exponential).

[F7]

exp⁡′=exp⁡, and the chain rule and algebra of derivatives give ddze2πimz=2πim e2πimz (The complex exponential is entire and its complex derivative is itself, The chain rule for complex derivatives, Linearity, product, reciprocal, and quotient rules for complex derivatives).

Proof

1.1F1F2F6F7F8givenalgebra

Let K be a compact subset of the product, so Im⁡τ≥y0>0 and ∣Im⁡z∣≤M on K. Put r:=e−πy0<1. Then ∣Q∣≤r and ∣Qm2e2πimz∣≤rm2e2πM∣m∣ for every (m,z,τ) under consideration; the bounding series converges by [F8], since the ratio of consecutive terms is r2m+1e2πM→0. The M-test [F1] therefore gives uniform convergence on K; each term is entire in z and holomorphic in τ by [F6] and [F7], so [F2] shows that Θ is entire in z for fixed τ, holomorphic in τ, and that the series converges locally uniformly in each variable, uniformly on compact products. Termwise index shifts, licensed by absolute convergence [F8], give Θ(z+1∣τ)=Θ(z∣τ), since e2πim=1, and, using Qm2e2πimτ=Q(m+1)2−1, also Θ(z+τ∣τ)=Q−1e−2πizΘ(z∣τ).

1.2F3F6F7givenalgebra

Put Π(z∣τ):=∏n≥1(1−Q2n)(1+Q2n−1e2πiz)(1+Q2n−1e−2πiz) and gn(z,τ):=(1−Q2n)(1+Q2n−1e2πiz)(1+Q2n−1e−2πiz). For finite grouped products put Π0=1 (the empty product) and ΠN=∏1≤n≤Ngn for N≥1; normal convergence concerns this explicit sequence including its empty prefix. On K as above, with B:=e2πM, the estimate ∣gn−1∣≤(1+r2n)(1+Br2n−1)2−1≤CKr2n−1 shows ∑nsup⁡K∣gn−1∣<∞, so Π is normally convergent and [F3] makes it holomorphic in each variable with the displayed product. The factor 1−Q2n never vanishes because ∣Q2n∣<1. By [F6], 1+Q2n−1e2πiz=0 is equivalent to e2πiz=−Q−(2n−1)=eπi(1−(2n−1)τ), that is to z≡12−2n−12τ(modZ), and likewise 1+Q2n−1e−2πiz=0 is equivalent to z≡−12+2n−12τ(modZ). Writing a solution of the first type as 1+τ2+a+bτ with a=k and b=−n≤−1, and one of the second type with a=k−1 and b=n−1≥0, shows that the union of all solutions over n≥1 is exactly the coset 1+τ2+Z+τZ, each of whose points arises from exactly one n and one factor because the representation a+bτ with a,b∈Z is unique (Im⁡τ>0). At such a solution the derivative of the vanishing factor with respect to z is ±2πiQ2n−1e±2πiz≠0 by [F6] and [F7], so every zero of Π is simple and is a zero of exactly one factor. Finally, cancelling the shifted factors in the normally convergent product, with the reindexings n↦n+1 in the second product and n↦n±1 in the third, gives Π(z+1∣τ)=Π(z∣τ) and Π(z+τ∣τ)=1+Q−1e−2πiz1+Qe2πizΠ(z∣τ)=Q−1e−2πizΠ(z∣τ).

2.1F4F5F6F8step 1.1step 1.2givenalgebra

At z0:=1+τ2 we have Θ(z0∣τ)=∑m∈Z(−1)mQm2+m; the terms with indices m and −m−1 are negatives of each other, and the series is absolutely convergent by [F8], so it sums to 0. The shift laws of 1.1 then propagate the vanishing to all points of z0+Z+τZ, the multiplier Q−1e−2πiz being nonzero by [F6]. By 1.2 that coset is exactly the zero set of Π, all its zeros are simple, and Θ is entire in z by 1.1; hence Fτ:=Θ(⋅∣τ)/Π(⋅∣τ) is holomorphic off the coset and, by the Taylor series of its vanishing numerator and the simple-zero factorisation [F5] of its denominator at each zero, extends holomorphically across it to an entire function. The shift laws of 1.1 and 1.2 give Fτ(z+1)=Fτ(z) and Fτ(z+τ)=Fτ(z) off the coset, hence everywhere. Every z∈C is w+m+nτ with m,n∈Z and w in the compact parallelogram {s+tτ:0≤s,t≤1} (take m,n the integer parts of the coefficients of z in the basis 1,τ), so z↦Fτ(z) is bounded on C by its supremum on that compact set; [F4] gives Fτ≡c(τ) for a number c(τ) depending only on τ.

3.1F3F6F8step 2.1givenalgebra

Evaluating the constant of 2.1 at z=14, where no factor of Π vanishes, gives c(τ)=Θ(14∣τ)/Π(14∣τ). The series identity is Θ(14∣τ)=∑mQm2im=∑k(−1)kQ4k2=Θ(12∣4τ): the odd-m terms cancel in the pairs m↔−m, and the even ones m=2k contribute i2kQ4k2=(−1)kQ4k2, all licensed by [F8]. The product identity is Π(14∣τ)=∏n(1−Q2n)(1+Q4n−2)=∏k(1−Q4k)(1−Q8k−4)=∏j(1−Q8j)(1−Q8j−4)2=Π(12∣4τ), obtained from ∏n(1+Q4n−2)=∏n(1−Q8n−4)/∏n(1−Q4n−2) and from splitting ∏k(1−Q4k)=∏j(1−Q8j)∏j(1−Q8j−4); all rearrangements are legitimate by normal convergence [F3]. Hence c(τ)=c(4τ), and iteration gives c(τ)=c(4kτ) for every k≥0. Writing Qk:=Q4k→0, the evaluation of 2.1 at z=12 gives c(4kτ)=Θ(12∣4kτ)/Π(12∣4kτ) with Θ(12∣4kτ)=1+2∑m≥1(−1)mQkm2 and Π(12∣4kτ)=∏n(1−Qk2n)(1−Qk2n−1)2. Since ∣Qk∣→0, ∣Θ(12∣4kτ)−1∣≤2∣Qk∣/(1−∣Qk∣)→0, and with ρ=∣Qk∣, ∣Π(12∣4kτ)−1∣≤exp⁡(ρ(2+ρ)/(1−ρ2))−1→0 by the elementary product bound ∏(1+an)≤exp⁡∑an. Therefore c(τ)=lim⁡kc(4kτ)=1.

4.1F6step 2.1step 3.1givenalgebra∎

By 3.1, Θ(z∣τ)=Π(z∣τ) for all z, so by 2.1 the zeros of Θ in z are exactly the simple zeros z=1+τ2+a+bτ, a,b∈Z. Moreover Θ(0∣τ)=Π(0∣τ)=∏n(1−Q2n)(1+Q2n−1)2≠0, since ∣Q2n∣<1 and ∣Q2n−1∣<1 make every factor nonzero. This is the zero-free theta constant θ(τ), and Q2=q by the addition law [F6].

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Transformation laws of the Jacobi theta function

Statement

Assume countable choice. For τ∈H and z∈C, let Θ(z∣τ) and θ(τ)=Θ(0∣τ) be the functions of Jacobi theta triple product and nonvanishing of the theta constant, and set s(τ)=exp⁡(12Log⁡(τ/i)). The principal logarithm is defined here because Re⁡(τ/i)>0; thus s is the holomorphic square root of τ/i that is positive for τ=it, t>0. Then Θ(z∣−1/τ)=s(τ)eπiτz2Θ(τz∣τ),Θ(z∣τ+2)=Θ(z∣τ). In particular θ(−1/τ)=s(τ)θ(τ),θ(1−1/τ)=s(τ)∑n∈Zeπi(n+1/2)2τ. As Im⁡τ→∞, uniformly in Re⁡τ, θ(1−1/τ)=2s(τ)eπiτ/4(1+O(e−2πIm⁡τ)).

Facts & Assumptions

Given: Countable choice (The Axiom of Countable Choice (ACω)), τ∈H and z∈C.

[F1]

The theta series Θ(z∣τ)=∑n∈Zeπin2τ+2πinz converges absolutely and uniformly on compact products; it is entire in z and holomorphic in τ (Jacobi theta triple product and nonvanishing of the theta constant).

[F2]

Under countable choice, shifted Poisson summation for a Schwartz function f on R gives ∑nf(a+n)=∑mf^(m)e2πima, and both sums converge absolutely. For ft(u)=e−πtu2, t>0, the Fourier transform is t−1/2e−πξ2/t (Poisson summation for Schwartz functions, Euclidean Gaussian transform with the 2π normalization).

[F3]

Summable uniform majorants give uniformly convergent function series; locally uniform holomorphic limits are holomorphic, and holomorphic functions on a connected domain agreeing on a set with an interior accumulation point agree everywhere (Weierstrass M-test for complex-valued function series, Locally uniform limits of holomorphic functions are holomorphic and their derivatives converge locally uniformly, Identity theorem for holomorphic functions).

Proof

1.1F1F2F4givenalgebra

For t>0, every derivative of ft(u)=e−πtu2 is a polynomial times this Gaussian. Exponential domination (The exponential dominates every fixed nonnegative integer power at +∞) bounds each such derivative times every power of u, so ft is Schwartz in Schwartz space and its seminorms. Apply [F2] at the real shift a=x to obtain ∑ne−πt(n+x)2=t−1/2∑me−πm2/te2πimx. Multiplying by t and expanding (n+x)2 gives Θ(x∣i/t)=t e−πtx2Θ(itx∣it) for every real x. This is the asserted inversion identity for τ=it, since −1/(it)=i/t, s(it)=t and eπi(it)x2=e−πtx2. Countable choice is used precisely through the two suppliers in [F2].

2.1F1F3F4step 1.1algebra

Fix real x. Both sides of the claimed inversion identity are holomorphic in τ∈H. For the right-hand theta series, on any compact K⊂H its terms have modulus at most e−πy0n2+C∣n∣, where y0=min⁡KIm⁡τ>0 and C bounds 2π∣xIm⁡τ∣; this summable Gaussian majorant proves holomorphy by [F3]. The other factors are holomorphic by [F4], including s, since τ/i lies in the right half-plane. The left side is holomorphic by [F1] and composition with −1/τ. By 1.1 the two sides agree on the positive imaginary axis, whose points accumulate within H, so the identity theorem [F3] proves equality for all τ. Now fix such τ. The two sides are entire in z by [F1, F4] and agree for real z=x, so a second identity-theorem application proves the inversion formula for every z∈C.

3.1F1F4step 2.1algebra

Each term of the theta series is unchanged on replacing τ by τ+2, since e2πin2=1 for integral n; absolute convergence therefore proves the stated period-two identity. Setting z=0 in 2.1 gives θ(−1/τ)=s(τ)θ(τ). Since n2 and n have the same parity, [F1, F4] give θ(1+u)=Θ(1/2∣u) for u∈H. Apply 2.1 with z=1/2 and complete the square: eπiτ/4Θ(τ/2∣τ)=∑neπi(n+1/2)2τ. This proves the shifted-constant formula.

4.1F1F4step 3.1algebra∎

Pair n=j with n=−j−1, j≥0, in the absolutely convergent shifted series. Its value is 2eπiτ/4(1+∑j≥1eπiτj(j+1)). If y=Im⁡τ, then j(j+1)≥2j gives ∣∑j≥1eπiτj(j+1)∣≤e−2πy/(1−e−2πy). This proves the uniform asymptotic and its stated error term. The principal square root never vanishes on H; no alternative square-root sign, boundary point τ=0, or half-weight multiplier convention is implicit in any formula.

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The Jacobi product formula for the discriminant

Statement

For τ∈H and q=e2πiτ, Δ(τ)=q∏n=1∞(1−qn)24,Δ=(E43−E62)/1728. The product converges locally uniformly for ∣q∣<1; its factor after q is holomorphic and zero-free in the unit disc and equals 1 at q=0. Consequently Δ has integral Fourier coefficients and a simple zero at the cusp.

Facts & Assumptions

Given: Δ=(E43−E62)/1728∈S12 with q-expansion q−24q2+O(q3), and E2(τ)=1−24∑n≥1σ1(n)qn with its transformation law (The discriminant is a nonvanishing cusp form of weight 12, The level-one Eisenstein series E_k and the weight-two series E_2, The transformation law of the weight-two Eisenstein series E_2).

[F1]

A normally convergent product of holomorphic functions on a domain is holomorphic; on compacta all but finitely many factors are zero-free and the zeros come from the finitely many exceptional factors (Normally convergent products define holomorphic functions with the expected zeros).

[F2]

Locally uniform limits of holomorphic functions have locally uniformly convergent derivatives (Locally uniform limits of holomorphic functions are holomorphic and their derivatives converge locally uniformly).

[F3]

If a holomorphic function on a domain has zero derivative it is constant (A holomorphic function with zero derivative on a domain is constant).

[F4]

∑r≥0wr=1/(1−w) for ∣w∣<1 and the same geometric identity for complex w follows from the finite geometric sum and ∣w∣N+1→0; absolutely convergent complex double families may be regrouped by applying the real double-series theorem to real and imaginary parts (For ∣r∣<1, ∑k≥0rk=1/(1−r), and for ∣r∣≥1 the series diverges, Fubini for double series: if ∑i∑j∣aij∣ converges then both iterated sums and the sum along every bijection N→N×N converge to one and the same value); finite products of (1−qn)24 have integer coefficients by the binomial theorem (The binomial theorem over the complex field).

[F6]

F∈S12 means: F holomorphic on H, F(γτ)=(cτ+d)12F(τ) for all γ∈SL2(Z), and the associated function of q is holomorphic at 0 with value 0 (Level-one modular forms and cusp forms).

Proof

1.1F1F2F4givenalgebra

Put P0(q)=1 for the empty product, PN(q)=∏1≤n≤N(1−qn)24 for N≥1, P(q):=lim⁡NPN(q) and F(τ):=qP(q). For ∣q∣≤r<1 we have ∣(1−qn)24−1∣≤(224−1)rn, a summable majorant independent of q, so the product is normally convergent on the disc and [F1] makes P holomorphic and zero-free there with P(0)=1; hence F is holomorphic and zero-free on H and F(τ)=q+O(q2) (as a function of q). By [F2] the logarithmic derivative of P may be computed from the finite products and the geometric series [F4]: 12πiF′F=1−24∑n≥1nqn1−qn=1−24∑n≥1∑r≥1nqnr=1−24∑m≥1σ1(m)qm=E2(τ), the regrouping being justified by the bound ∑n,rn∣q∣nr≤(1−r)−1∑nnrn<∞ on ∣q∣≤r<1 [F4]; the last series converges by the ratio test.

2.1F3F5F6step 1.1givenalgebra

For γ=(abcd)∈SL2(Z) put Rγ(τ):=F(γτ)/[(cτ+d)12F(τ)]; this is holomorphic and zero-free on H. Its logarithmic derivative, divided by 2πi, equals E2(γτ)(cτ+d)2−12c2πi(cτ+d)−E2(τ) by 1.1, and by the E2 transformation law this is [E2(τ)−6icπ(cτ+d)]−[−6icπ(cτ+d)]−E2(τ)=0 (using 12c2πi(cτ+d)=−6icπ(cτ+d)). Hence Rγ is constant, Cγ, by [F3], and Cγδ=CγCδ because (cγδτ+dγδ)=(cγδτ+dγ)(cδτ+dδ). For T we have F(τ+1)=F(τ), so CT=1; for S we have RS(τ)=F(−1/τ)/[τ12F(τ)] and at τ=i, where −1/i=i and i12=1, this gives CS=F(i)/F(i)=1. Since S,T generate SL2(Z) [F5] and (−I) acts with factor (−1)12=1, multiplicativity gives Cγ=1 for every γ; thus F(γτ)=(cτ+d)12F(τ) for all γ, and since F=q+O(q2) it satisfies the cusp condition. Hence F∈S12 by [F6].

3.1F5step 2.1givenalgebra

By [F5], S12 is one-dimensional and contains the nonzero Δ=q−24q2+O(q3); so F=cΔ for some c∈C. Comparing q-coefficients, 1=c⋅1, so F=Δ, which is the product formula.

4.1F1F2F4step 2.1givenalgebra∎

Integrality of the coefficients: the coefficient of qN in P equals the coefficient of qN in the finite product ∏n≤N(1−qn)24, because all factors with n>N are congruent to 1 modulo qN+1; the finite product has integer coefficients by [F4], and its coefficients agree with those of the analytic expansion of P because the finite products converge locally uniformly, with all derivatives, to P near 0 by [F1] and [F2]. Hence every Taylor coefficient of P is an integer, and the coefficients of Δ=qP are integers as well; the simple zero at the cusp is ord⁡∞(Δ)=1 from the expansion q−24q2+⋯, consistent with [F5].

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Integrality of the Fourier coefficients of the j-invariant

Statement

With q=e2πiτ, the j-invariant has a Laurent expansion convergent for 0<∣q∣<1, j(τ)=q−1+744+196884q+21493760q2+∑n≥3c(n)qn,c(n)∈Z. Equivalently qj is holomorphic in the unit disc with integer Taylor coefficients and constant term 1.

Facts & Assumptions

Given: Δ=qP(q) with P holomorphic and zero-free on ∣q∣<1 and P(q)=∏n≥1(1−qn)24 (The Jacobi product formula for the discriminant), and j=E43/Δ (The modular discriminant and the j-invariant).

[F1]
[F2]

E4=1+240∑n≥1σ3(n)qn, with σ3(n)∈Z and σ3(1)=1, σ3(2)=9, σ3(3)=28 (Eisenstein series are modular forms; their Fourier coefficients, The divisor power sums σk).

[F3]

A holomorphic function on a disc has a convergent Taylor expansion with the coefficients given by the derivatives at the centre (A holomorphic function equals its Taylor series throughout the largest centred disc in its domain); locally uniform convergence passes to all derivatives (Locally uniform limits of holomorphic functions are holomorphic and their derivatives converge locally uniformly); the coefficient sequence of a product of two absolutely convergent complex series is the Cauchy product, absolutely convergent (The Cauchy product of two absolutely convergent complex series converges absolutely to the product of their sums, The binomial theorem over the complex field).

Proof

1.1F1F2F3givenalgebra

Since P is zero-free on the unit disc and Δ=qP, the function qj=E4(q)3/P(q) is holomorphic on ∣q∣<1. The powers E43 have integer Taylor coefficients: by [F2] the expansion of E4 has integer coefficients, and the coefficients of the cube are finite sums of products of integers, which by [F3] are exactly the Cauchy-product coefficients.

2.1F1F2F3step 1.1givenalgebra

Write P(q)=1+∑n≥1pnqn with pn∈Z by [F1], and let P(q)−1=∑n≥0bnqn be its Taylor expansion at 0, which exists and converges on ∣q∣<1 because P is holomorphic and zero-free there [F3]. Comparing coefficients in P⋅P−1=1 gives b0=1 and bn=−∑r=1nprbn−r for n≥1; by induction on n every bn is an integer. Hence qj=E43⋅P−1 has integer Taylor coefficients by the Cauchy product [F3], and its constant term is 1⋅1=1. Since j=q−1(qj), the Laurent expansion of j on 0<∣q∣<1 has the stated integer coefficients.

3.1F2F3step 2.1givenalgebra∎

The displayed coefficients are obtained by computing finitely many terms. From [F2] and σ3(1)=1, σ3(2)=9, σ3(3)=28: E4=1+240q+2160q2+6720q3+O(q4), so E43=1+720q+179280q2+16954560q3+O(q4); from the product formula Δ=q(1−24q+252q2−1472q3+O(q4)), so P=1−24q+252q2−1472q3+O(q4) and its inverse begins P−1=1+24q+324q2+3200q3+O(q4) (coefficient comparison, as in 2.1). Multiplying, qj=E43P−1=1+744q+196884q2+21493760q3+O(q4), hence j=q−1+744+196884q+21493760q2+∑n≥3c(n)qn with the stated initial coefficients.

5 · Examples, counterexamples and false statements

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