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Cyclic Quadratic Modules

Updated 28 March 2026
  • Cyclic quadratic modules are finite abelian groups equipped with quadratic forms that satisfy bilinearity and nondegeneracy, providing a framework for studying Weil representations.
  • They decompose into cyclic modules, such as those of order 2p^r, with invariants like level, signature, and discriminant forms that influence half-integral weight modular forms.
  • In the large parameter limit, the generating weights converge to a symmetric, bi-modal distribution, revealing deep arithmetic and representation-theoretic symmetries.

A cyclic quadratic module is a finite abelian group equipped with a quadratic form satisfying specific bilinearity and nondegeneracy conditions, central to the study of the Weil representation and vector-valued modular forms. In particular, modules of order 2pr2p^r (with pp an odd prime, r1r\ge1) possess intricate arithmetic and representation-theoretic properties that control the structure of associated half-integral weight modular forms. The generating weights of these modules display remarkable uniformity in the large parameter limits, reflecting deep symmetries in the underlying arithmetic.

1. Definition and Invariants of Cyclic Quadratic Modules

Let MM be a finite abelian group, and q:MQ/Zq: M \to \mathbb{Q}/\mathbb{Z} a function such that:

  • For all xMx \in M and integers nn, q(nx)=n2q(x)q(nx) = n^2 q(x) in Q/Z\mathbb{Q}/\mathbb{Z}.
  • The associated bilinear form b(x,y)=q(x+y)q(x)q(y)b(x,y) = q(x+y) - q(x) - q(y) is Z\mathbb{Z}-bilinear and nondegenerate, in the sense that x(yb(x,y))x \mapsto (y \mapsto b(x,y)) yields an isomorphism MHom(M,Q/Z)M \cong \operatorname{Hom}(M, \mathbb{Q}/\mathbb{Z}).

Such a pair (M,q)(M,q) is a finite quadratic module. A module is cyclic of order NN if MZ/NZM \cong \mathbb{Z}/N\mathbb{Z}; every such module admits a generator $1$ with q(k)=ak2NmodZq(k) = \frac{a k^2}{N} \bmod \mathbb{Z} for unique a(Z/N)×a \in (\mathbb{Z}/N)^\times, denoted ANaA_N^a.

Key invariants include:

  • Level: The minimal NN such that Nq(x)ZN q(x) \in \mathbb{Z} for all xx.
  • Signature: sig(M)Z/8\operatorname{sig}(M) \in \mathbb{Z}/8, extracted from the Gauss sum

ΩM(1)=1MxMe(q(x))=(i)sig(M)\Omega_M(1) = \frac{1}{\sqrt{|M|}} \sum_{x \in M} e(q(x)) = (\sqrt{i})^{\,\operatorname{sig}(M)}

where e(u)=e2πiue(u) = e^{2\pi i u}.

  • Discriminant form: For an integral lattice LL, the quadratic module L/LL^*/L with q(x+L)=12(x,x)modZq(x+L) = \frac{1}{2}(x,x) \bmod \mathbb{Z}.

2. Structure of Even-Order Cyclic Modules of Order 2pr2p^r

Fixing an odd prime p5p\ge5 and r1r\ge1, the distinguished cyclic module is

D=A2pr=(Z/2prZ,q(x)x24prmodZ).D = A_{2p^r} = (\mathbb{Z}/2p^r\mathbb{Z},\, q(x) \equiv \tfrac{x^2}{4p^r} \bmod \mathbb{Z}).

By the Chinese Remainder Theorem, Z/2prZZ/2ZZ/prZ\mathbb{Z}/2p^r\mathbb{Z} \simeq \mathbb{Z}/2\mathbb{Z} \oplus \mathbb{Z}/p^r\mathbb{Z}, and the form splits orthogonally:

q2prq2qpr,withq2(xmod2)=x24mod1,  qpr(ymodpr)=y2prmod1.q_{2p^r} \cong q_2 \oplus q_{p^r}, \quad \text{with} \quad q_2(x \bmod 2) = \tfrac{x^2}{4} \bmod 1,\; q_{p^r}(y \bmod p^r) = \tfrac{y^2}{p^r} \bmod 1.

In Jordan decomposition, this is A21Apr4A_{2}^{\,1} \oplus A_{p^r}^{4}.

The signature is sig(A2pr)=1Z/8\operatorname{sig}(A_{2p^r}) = 1 \in \mathbb{Z}/8 (odd), excluding the existence of integral-weight modular forms for its Weil representation.

3. The Weil Representation Associated to DD

Let Mp2(Z)\mathrm{Mp}_2(\mathbb{Z}) denote the metaplectic double cover of SL2(Z)\mathrm{SL}_2(\mathbb{Z}), generated by (T,1)(T,1) and (S,τ)(S,\sqrt{\tau}) with relations S2=ZS^2=Z, Z2=(I,1)Z^2=(I,-1). The Weil representation ρD\rho_D is a unitary representation:

ρD:Mp2(Z)GL(C[D])\rho_D: \mathrm{Mp}_2(\mathbb{Z}) \longrightarrow \mathrm{GL}(\mathbb{C}[D])

on the group algebra C[D]\mathbb{C}[D] with basis {δx}xD\{\delta_x\}_{x\in D}, defined via:

  • ρD(T)δx=e(q(x))δx\rho_D(T)\,\delta_x = e(-q(x))\,\delta_x
  • ρD(S)δx=(i)sig(D)DyDe(b(x,y))δy\rho_D(S)\,\delta_x = \frac{(\sqrt{i})^{\,\operatorname{sig}(D)}}{\sqrt{|D|}} \sum_{y \in D} e(b(x,y))\,\delta_y

Here b(x,y)=q(x+y)q(x)q(y)b(x,y) = q(x+y) - q(x) - q(y). The representation respects all relations of Mp2(Z)\mathrm{Mp}_2(\mathbb{Z}).

4. Half-Integral Weight Modular Forms and Generating Weights

For any finite-dimensional representation ρ\rho of Mp2(Z)\mathrm{Mp}_2(\mathbb{Z}), the module of holomorphic ρ\rho-valued half-integral weight modular forms is

M(ρ)=k12ZMk(ρ),M(\rho) = \bigoplus_{k \in \tfrac{1}{2} \mathbb{Z}} M_k(\rho),

which is a free module of rank dimρ\dim \rho over C[E4,E6]\mathbb{C}[E_4, E_6], the ring of level-one modular forms. The fjMkj(ρ)f_j \in M_{k_j}(\rho) with M(ρ)j=1dimρC[E4,E6]fjM(\rho) \cong \bigoplus_{j=1}^{\dim\rho} \mathbb{C}[E_4,E_6]\langle f_j\rangle determine the generating weights k1kdimρk_1 \le \cdots \le k_{\dim\rho}, subject to the sum rule

jkj=12Tr(L),\sum_{j} k_j = 12\,\operatorname{Tr}(L),

where LL is any exponent matrix with ρ(T)=e2πiL\rho(T) = e^{2\pi i L}.

For ρ=ρA2pr\rho = \rho_{A_{2p^r}}, Tr(L)\operatorname{Tr}(L) is given by:

Tr(L)=pr{pr4}pr/2+p(r+1)/212(p1){hp,p1(mod4) 4hp+1,p3(mod8) 2hp+1,p7(mod8)\operatorname{Tr}(L) = p^r - \left\{ \frac{p^r}{4} \right\} p^{\lfloor r/2 \rfloor} + \frac{p^{\lfloor (r+1)/2 \rfloor}-1}{2(p-1)} \begin{cases} h_p, & p \equiv 1 \pmod{4} \ 4h_p^* + 1, & p \equiv 3 \pmod{8} \ 2h_p + 1, & p \equiv 7 \pmod{8} \end{cases}

where hph_p is the class number of Q(p)\mathbb{Q}(\sqrt{-p}).

It is established that M1/2(ρA2pr)=0M_{1/2}(\rho_{A_{2p^r}}) = 0 and M1(ρA2pr)=0M_{1}(\rho_{A_{2p^r}}) = 0 (by Skoruppa–Serre–Stark and parity), and a further check confirms M3/2M_{3/2} is unobstructed. Thus all dimensions dimMk\dim M_k can be extracted from the Euler characteristic. The multiplicity mkm_k of each weight kk, for k{3/2,5/2,,21/2}k \in \{3/2, 5/2, \dots, 21/2\}, is described by explicit linear combinations involving prp^r, Tr(L)\operatorname{Tr}(L), and small correction factors:

δ=18(2+(1pr)),ϵ±=16(1±(pr3)),\delta = \frac{1}{8}(2 + (\tfrac{-1}{p^r})), \quad \epsilon_\pm = \frac{1}{6}(1 \pm (\tfrac{p^r}{3})),

with mirror-symmetry mk=m23/2km_{k} = m_{23/2 - k}, and m1/2=m23/2=0m_{1/2} = m_{23/2} = 0.

5. Limiting Behavior of Generating Weights

As pp \to \infty (with rr fixed) or rr \to \infty (with pp fixed), dimρ=2pr\dim \rho = 2p^r increases, and hp=O(p1/2+ε)h_p = O(p^{1/2+\varepsilon}). One obtains:

Tr(L)dimρ12\frac{\operatorname{Tr}(L)}{\dim \rho} \to \frac{1}{2}

Consequently, the normalized multiplicities mk/dimρm_k / \dim \rho converge to a discrete, bi-modal distribution, symmetric and concentrated at the central weights:

mkdimρ{0k=1/2,23/2 148k=3/2,21/2 348k=5/2,19/2 548k=7/2,17/2 748k=9/2,15/2 848k=11/2,13/2 \frac{m_k}{\dim\rho} \to \begin{cases} 0 & k = 1/2,\,23/2 \ \frac{1}{48} & k = 3/2,\,21/2 \ \frac{3}{48} & k = 5/2,\,19/2 \ \frac{5}{48} & k = 7/2,\,17/2 \ \frac{7}{48} & k = 9/2,\,15/2 \ \frac{8}{48} & k = 11/2,\,13/2 \ \end{cases}

This limiting pattern highlights a pronounced symmetric "hump" at weights $11/2$ and $13/2$. This universal emergence of a discrete, symmetric measure for the generating weights as parameters grow suggests a deeper structural or representation-theoretic phenomenon, analogous to automorphic forms over large-level metaplectic groups (Candelori et al., 2016).

6. Context and Open Directions

The explicit computation of generating weights for vector-valued modular forms in the context of Weil representations of even-order cyclic quadratic modules, particularly those of order 2pr2p^r, deepens the understanding of the interplay between arithmetic invariants (such as class numbers and Gauss sums) and the algebraic structure of modular forms. The observed measure convergence suggests new potential "limit objects" for these representation-theoretic constructions, indicating directions for further research into discrete distributions and automorphic phenomena in the context of large-level metaplectic and modular theory.

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