The generalized lambda function Λk=W[k,2,1]\Lambda_k=W_{[k,2,1]} is the ratio of differences of Weierstrass ℘\wp-values (℘(k/N;τ)−℘(1/N;τ))/(℘(2/N;τ)−℘(1/N;τ))\big(\wp(k/N;\tau)-\wp(1/N;\tau)\big)/\big(\wp(2/N;\tau)-\wp(1/N;\tau)\big), a modular function for the congruence subgroup Γ1(N)\Gamma_1(N) introduced in Lang's framework. Ishii (2011 preprint arXiv:1110.4429, generalized in Ramanujan J. 33 (2014)) proved that Λk\Lambda_k together with the modular invariant jj generates the modular function field of Γ1(N)\Gamma_1(N), so that CM values of Λk\Lambda_k generate ray class fields, and proved that, writing δ=gcd⁡(k,N)\delta=\gcd(k,N), whenever δ=1\delta=1, or δ>1\delta>1 with 3∤δ3\nmid\delta and N/δN/\delta not a prime power, every SL2(Z)\mathrm{SL}_2(\mathbb{Z})-transform of Λk\Lambda_k has qq-expansion over Z[ζN]\mathbb{Z}[\zeta_N] and every CM value Λk(α)\Lambda_k(\alpha) is an algebraic integer. In the complementary regime, δ>1\delta>1 with 3∣δ3\mid\delta or N/δN/\delta a prime power, the status of both the qq-expansion integrality and the algebraic integrality of the CM values is open.

Background

A central theme of explicit class field theory for imaginary quadratic fields is to produce, in the spirit of Hilbert's twelfth problem, concrete modular functions whose special values generate the abelian extensions of such a field KK. If α\alpha lies in the complex upper half plane H\mathbb{H} and Q(α)=K\mathbb{Q}(\alpha)=K is imaginary quadratic, α\alpha is called an imaginary quadratic point or CM point; the classical singular moduli j(α)j(\alpha) generate the Hilbert class field (the maximal unramified abelian extension) of KK. Refinements with level structure generate ray class fields, the abelian extensions classified by class field theory with a prescribed modulus, and are sought as class invariants: generators with small height that are algebraic integers, so that their minimal polynomials over Z\mathbb{Z} (class polynomials) have integer coefficients.

Fix an integer N≥6N\ge 6 and let Γ1(N)={(abcd)∈SL2(Z) : a≡1, c≡0(modN)},\Gamma_1(N)=\left\{\begin{pmatrix}a&b\\c&d\end{pmatrix}\in\mathrm{SL}_2(\mathbb{Z})\ :\ a\equiv 1,\ c\equiv 0 \pmod{N}\right\}, a congruence subgroup of SL2(Z)\mathrm{SL}_2(\mathbb{Z}); denote by A1(N)\mathcal{A}_1(N) its field of modular functions (meromorphic functions on H\mathbb{H} invariant under Γ1(N)\Gamma_1(N) with compatible behavior at the cusps). Write Lτ=Z+ZτL_\tau=\mathbb{Z}+\mathbb{Z}\tau for the lattice generated by 11 and τ\tau, and ℘(z;L)\wp(z;L) for the Weierstrass ℘\wp-function of a lattice LL. In his book Elliptic Functions, Lang introduced the generalized lambda functions: for a triple a=[a1,a2,a3]a=[a_1,a_2,a_3] of distinct integers with 0<ai≤N/20<a_i\le N/2, Wa(τ)=℘(a1/N;Lτ)−℘(a3/N;Lτ)℘(a2/N;Lτ)−℘(a3/N;Lτ),W_a(\tau)=\frac{\wp(a_1/N;L_\tau)-\wp(a_3/N;L_\tau)}{\wp(a_2/N;L_\tau)-\wp(a_3/N;L_\tau)}, a family generalizing the classical elliptic modular lambda function (the squared elliptic modulus parametrizing elliptic curves with a basis of 22-torsion, itself the corresponding ratio of ℘\wp-differences at the half-periods). Lang proposed investigating the special values of these functions at imaginary quadratic points, in particular whether they generate ray class fields. The function studied in Ishii's preprint arXiv:1110.4429 is Λk:=W[k,2,1]\Lambda_k:=W_{[k,2,1]} (note that the related display (℘(kτ/N;τ)−℘(τ/N;τ))/(℘(2τ/N;τ)−℘(τ/N;τ))\big(\wp(k\tau/N;\tau)-\wp(\tau/N;\tau)\big)/\big(\wp(2\tau/N;\tau)-\wp(\tau/N;\tau)\big), which appears in Corollary 3.3 of the preprint and Corollary 4.6 of the published version, equals Λk∘S\Lambda_k\circ S for S=(0−110)∈SL2(Z)S=\begin{pmatrix}0&-1\\1&0\end{pmatrix}\in\mathrm{SL}_2(\mathbb{Z}) by the transformation of ℘\wp under the homothety L−1/τ=(−1/τ)LτL_{-1/\tau}=(-1/\tau)L_\tau, not Λk\Lambda_k itself); the surrounding theory of modular units is relevant here: a modular unit is a modular function with no zeros or poles on H\mathbb{H}, and for congruence subgroups such units are generated by Siegel functions, explicit qq-products built from the Dedekind eta function.

Put ζ=e2πi/N\zeta=e^{2\pi i/N} and q=e2πiτ/Nq=e^{2\pi i\tau/N}. The standard route from qq-expansion arithmetic to integrality of special values is the modular equation argument: if ff is a modular function for Γ1(N)\Gamma_1(N) with no poles on H\mathbb{H} and every transform f∘Af\circ A (A∈SL2(Z)A\in\mathrm{SL}_2(\mathbb{Z})) has Laurent expansion f∘A∈Z[ζ]((q))f\circ A\in\mathbb{Z}[\zeta]((q)) (a formal Laurent series in qq with coefficients in the ring of cyclotomic integers Z[ζ]\mathbb{Z}[\zeta]), then the product Φ(X,j)=∏A(X−f∘A)\Phi(X,j)=\prod_{A}(X-f\circ A) over coset representatives of SL2(Z)/Γ1(N){±I}\mathrm{SL}_2(\mathbb{Z})/\Gamma_1(N)\{\pm I\} is a monic polynomial with coefficients in Z[ζ][j]\mathbb{Z}[\zeta][j]; Galois invariance gives Φ∈Z[j][X]\Phi\in\mathbb{Z}[j][X], so ff is integral over Z[j]\mathbb{Z}[j], and since j(α)j(\alpha) is an algebraic integer at every CM point α\alpha (a classical fact of complex multiplication), f(α)f(\alpha) is an algebraic integer.

The lineage of results is as follows. Ishida and Ishii built the function-field machinery of A1(N)\mathcal{A}_1(N); Hong and Koo obtained ray class field generators from singular values of Γ1(N)\Gamma_1(N)-modular functions; Ishii and Kobayashi proved that WaW_a is integral over Z[j]\mathbb{Z}[j] (with algebraic-integer CM values) under a strong coprimality condition on the triple, essentially a1a2a3(a1±a3)(a2±a3)a_1a_2a_3(a_1\pm a_3)(a_2\pm a_3) prime to NN. Ishii's preprint arXiv:1110.4429 and its generalization in Ramanujan J. 33 (2014) 121-130 (arXiv:1110.6489) prove that Λk,ℓ=W[k,ℓ,1]\Lambda_{k,\ell}=W_{[k,\ell,1]} generates A1(N)\mathcal{A}_1(N) over C(j)\mathbb{C}(j) for all 1<ℓ≠k<N/21<\ell\ne k<N/2, and that consequently Λk(α)\Lambda_k(\alpha) together with ζ\zeta generates the ray class field of K=Q(α)K=\mathbb{Q}(\alpha) modulo NN over its Hilbert class field whenever Z[α]\mathbb{Z}[\alpha] is the maximal order (via the Gee-Stevenhagen form of Shimura reciprocity, which computes the Galois action on such special values). For the integrality statements, with δ=gcd⁡(k,N)\delta=\gcd(k,N), the hypothesis is: (i) δ=1\delta=1, or (ii) δ>1\delta>1, (δ,3)=1(\delta,3)=1 and N/δN/\delta is not a power of a prime. Under it, Λk∘A∈Z[ζ]((q))\Lambda_k\circ A\in\mathbb{Z}[\zeta]((q)) for every A∈SL2(Z)A\in\mathrm{SL}_2(\mathbb{Z}), Λk\Lambda_k is integral over Z[j]\mathbb{Z}[j], and all CM values of all transforms are algebraic integers. Where the hypothesis bites: the leading coefficient of Λk∘A\Lambda_k\circ A is a product of ratios of the shape (1−ζa)/(1−ζb)(1-\zeta^a)/(1-\zeta^b), whose integrality is governed by the cyclotomic-unit lemma that 1−ζk1-\zeta^k is a unit of Z[ζ]\mathbb{Z}[\zeta] exactly when N/gcd⁡(k,N)N/\gcd(k,N) is not a prime power (used in the branch c≡0(modN)c\equiv 0\pmod N of the transform computation), while the branch 2c=c{2c}={c} (here {x}\{x\} denotes the integer with 0≤{x}≤N/20\le\{x\}\le N/2 such that x≡±{x}(modN)x\equiv\pm\{x\}\pmod N, as defined in Section 2 of the preprint), possible only when 3∣N3\mid N, introduces a denominator 1−ζ3d1-\zeta^{3d} and thereby the condition (δ,3)=1(\delta,3)=1.

Evidence from a sibling setting points to genuine arithmetic sensitivity of exactly the excluded regimes: for the principal-congruence analogue Λ(τ;Q1,Q2)\Lambda(\tau;Q_1,Q_2) (the same ratio of ℘\wp-differences at points Q1,Q2,Q1+Q2Q_1,Q_2,Q_1+Q_2 with {Q1,Q2}\{Q_1,Q_2\} a basis of (Z/N)2(\mathbb{Z}/N)^2), Ishii proved that CNΛC_N\Lambda is integral over Z[j]\mathbb{Z}[j] with CN=1C_N=1 precisely when NN is not a prime power (CN=p2C_N=p^2 for p=2,3p=2,3, CN=pC_N=p for p>3p>3 otherwise), sharpened this to (1−ζ)3Λ(α)(1-\zeta)^3\Lambda(\alpha) and (1−ζ)3/Λ(α)(1-\zeta)^3/\Lambda(\alpha) being algebraic integers at all CM points α\alpha, proved Λ(α)\Lambda(\alpha) is a unit when NN is not a prime power, and exhibited explicit CM values that are not algebraic integers when NN is a prime power (norm 3−33^{-3} at N=3N=3, norm 1/21/2 at N=4N=4). Those results, however, are proved for a different group and a different function and do not transfer to Λk=W[k,2,1]\Lambda_k=W_{[k,2,1]}.

Problem Statement

Let N≥6N\ge 6, let kk be an integer with 2<k<N/22<k<N/2, put δ=gcd⁡(k,N)\delta=\gcd(k,N), and let Λk(τ)=W[k,2,1](τ)=℘(k/N;Lτ)−℘(1/N;Lτ)℘(2/N;Lτ)−℘(1/N;Lτ),\Lambda_k(\tau)=W_{[k,2,1]}(\tau)=\frac{\wp(k/N;L_\tau)-\wp(1/N;L_\tau)}{\wp(2/N;L_\tau)-\wp(1/N;L_\tau)}, where Lτ=Z+ZτL_\tau=\mathbb{Z}+\mathbb{Z}\tau is the lattice generated by 11 and τ\tau, ℘(z;L)\wp(z;L) denotes the Weierstrass ℘\wp-function of a lattice LL, ζ=e2πi/N\zeta=e^{2\pi i/N}, q=e2πiτ/Nq=e^{2\pi i\tau/N}, Z[ζ]((q))\mathbb{Z}[\zeta]((q)) is the ring of formal Laurent series in qq with coefficients in the cyclotomic integer ring Z[ζ]\mathbb{Z}[\zeta], jj denotes the classical elliptic modular invariant, and an imaginary quadratic point is an α\alpha in the complex upper half plane H\mathbb{H} such that Q(α)\mathbb{Q}(\alpha) is an imaginary quadratic field. It is known that if δ=1\delta=1, or if δ>1\delta>1 with (δ,3)=1(\delta,3)=1 and N/δN/\delta not a power of a prime, then Λk∘A∈Z[ζ]((q))\Lambda_k\circ A\in\mathbb{Z}[\zeta]((q)) for every A∈SL2(Z)A\in\mathrm{SL}_2(\mathbb{Z}), Λk\Lambda_k is integral over Z[j]\mathbb{Z}[j], and Λk(α)\Lambda_k(\alpha) is an algebraic integer for every imaginary quadratic point α\alpha. Determine the complementary regime, namely δ>1\delta>1 with 3∣δ3\mid\delta or N/δN/\delta a power of a prime:

(a) for which such pairs (k,N)(k,N) does Λk∘A∈Z[ζ]((q))\Lambda_k\circ A\in\mathbb{Z}[\zeta]((q)) hold for every A∈SL2(Z)A\in\mathrm{SL}_2(\mathbb{Z});

(b) for which such pairs (k,N)(k,N) is Λk\Lambda_k integral over Z[j]\mathbb{Z}[j], and in particular Λk(α)\Lambda_k(\alpha) an algebraic integer at every imaginary quadratic point α\alpha.

The two prongs are linked parts of one objective, completing the integrality picture of the family: (a) implies (b) through the modular equation argument, while failure of (a) at some transform does not by itself decide (b), since denominators may cancel in the Galois-invariant product ∏A(X−Λk∘A)\prod_A(X-\Lambda_k\circ A). A complete answer either proves that (a) and (b) hold throughout the regime, or establishes exactly which pairs (k,N)(k,N) fail, with explicit witnesses for the failing pairs (an imaginary quadratic point α\alpha with Λk(α)\Lambda_k(\alpha) not an algebraic integer, or a transform AA with Λk∘A∉Z[ζ]((q))\Lambda_k\circ A\notin\mathbb{Z}[\zeta]((q))) together with the corresponding statements for the remaining pairs.

References

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