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Finite-Prime Weil Quadratic Form

Updated 18 February 2026
  • Finite-prime Weil quadratic forms are cyclic quadratic modules defined by q(a)=a²/(2p^r) that underpin the arithmetic of vector-valued modular forms.
  • They feature explicit Weil representations with closed-form generating weight formulas and bi-modal multiplicity distributions reflecting deep modular symmetries.
  • Computational methods leveraging quadratic Gauss sums and algebraic reductions enable efficient determination of invariants and basis elements in these representations.

A finite-prime Weil quadratic form refers, in the context of the arithmetic theory of modular forms and automorphic representations, to a specific class of finite quadratic modules and their associated Weil representations, particularly those arising from cyclic groups of order 2pr2p^r for a prime p5p\geq 5. The associated quadratic forms, their induced bilinear forms, and the symmetries of the resulting module algebra encode rich arithmetic and geometric information, especially concerning vector-valued modular forms of half-integral weight, their generating weights, and their module structures over rings of modular forms. Recent research has achieved explicit, closed-form descriptions of the corresponding Weil representations and their modular form modules, including limiting multiplicity distributions, geometric interpretations on stacks, and computational algorithms for invariants.

1. Finite Cyclic Quadratic Modules: Definition and Structure

For a prime p5p\geq 5 and integer r1r\geq 1, set m=2prm=2p^r. The cyclic quadratic module in question is A=Z/mZA=\mathbb{Z}/m\mathbb{Z}. The quadratic form q:AQ/Zq:A\to\mathbb{Q}/\mathbb{Z} is defined by q(a)=a2/(2pr)mod1q(a) = a^2/(2p^r) \bmod 1. The associated symmetric bilinear form is b(a,b)=q(a+b)q(a)q(b)=ab/prmod1b(a,b)=q(a+b)-q(a)-q(b) = ab/p^r \bmod 1.

This module and form fit the general theory of finite quadratic modules (A,q)(A,q), where AA is a finite abelian group and qq satisfies q(x)=q(x)q(-x)=q(x) and yields a Z\mathbb{Z}-bilinear map B(x,y)=q(x+y)q(x)q(y)B(x,y)=q(x+y)-q(x)-q(y) (Ehlen et al., 2017). When the bilinear form bb is nondegenerate, (A,q)(A,q) is called nondegenerate. The level of (A,q)(A,q) is the minimal positive integer NN with Nq(x)ZN q(x)\in\mathbb{Z} for all xAx\in A.

For these cyclic modules, the signature sig(A)=1\mathrm{sig}(A)=1 mod $8$, which informs transformation properties of the associated representations under the modular group (Candelori et al., 2016).

2. The Weil Representation for Finite-Prime Modules

The Weil representation ρA\rho_A of the metaplectic group Mp2(Z)\mathrm{Mp}_2(\mathbb{Z}) acts naturally on the group algebra C[A]\mathbb{C}[A] with the standard delta basis {δx}xA\{\delta_x\}_{x\in A} and e(x)=e2πixe(x)=e^{2\pi i x}. The action of the standard generators TT and SS is:

  • ρA(T)δx=e(q(x))δx\rho_A(T)\cdot\delta_x = e(-q(x))\delta_x
  • ρA(S)δx=ΩA(1)A1/2yAe(b(x,y))δy\rho_A(S)\cdot\delta_x = \Omega_A(1) |A|^{-1/2}\sum_{y\in A} e(b(x,y))\delta_y

with A=2pr|A|=2p^r and ΩA(1)=i\Omega_A(1)=\sqrt{i} because sig(A)=1\mathrm{sig}(A)=1 (mod 8). These formulas are specific instances of the general Weil representation on finite quadratic modules (Ehlen et al., 2017, Zhu, 17 Dec 2025). Notably, ρA(S)4=iId\rho_A(S)^4 = i\cdot \mathrm{Id}, reflecting the metaplectic double cover and parity structure (Candelori et al., 2016).

The explicit computation of these operators reduces in particular cyclic and diagonal cases to elementary expressions involving Gauss sums (see below for generalizations) (Zhu, 17 Dec 2025).

3. Vector-Valued Modular Forms and Module Structure

For k12Zk\in\frac{1}{2}\mathbb{Z}, the space of vector-valued modular forms of weight kk transforming under ρA\rho_A can be constructed as the sheaf VkV_k on the metaplectic orbifold, which in this context is identified with the weighted projective line P(8,12)\mathbb{P}(8,12). The graded module of such forms,

M(ρA)=k12ZMk(ρA),M(\rho_A) = \bigoplus_{k\in\frac12\mathbb{Z}} M_k(\rho_A),

is a free module of rank 2pr2p^r over M(1)=C[E4,E6]M(1)=\mathbb{C}[E_4,E_6], the ring of (scalar) modular forms for SL2(Z)\mathrm{SL}_2(\mathbb{Z}). If k1k2k2prk_1\leq k_2\leq\cdots\leq k_{2p^r} are the generating weights,

jkj=12Tr(L),\sum_j k_j = 12\cdot \mathrm{Tr}(L),

where LL is an exponent matrix determined by the action of TT. The standard exponents satisfy 0kj23/20 \leq k_j \leq 23/2 (Candelori et al., 2016).

4. Explicit Formulas for Generating Weights and Multiplicities

The generating weights have closed-form expressions as functions of pp and rr via an explicit trace-of-exponents formula:

Tr(L)=pr{pr/4}pr/2+p(r+1)/212(p1)Cp,r\mathrm{Tr}(L) = p^r - \{p^r/4\}\cdot p^{\lfloor r/2\rfloor} + \frac{p^{\lfloor (r+1)/2\rfloor}-1}{2(p-1)}\cdot C_{p,r}

where Cp,rC_{p,r} encodes data from Dirichlet class numbers and pp modulo $8$.

The dimension-generating series is

k12ZdimMk(ρA)tk=tk1++tk2pr(1t4)(1t6).\sum_{k\in\frac12\mathbb{Z}} \dim M_k(\rho_A) t^k = \frac{t^{k_1} + \cdots + t^{k_{2p^r}}}{(1-t^4)(1-t^6)}.

Multiplicity formulas for each allowed half-integral weight kk (excluding the parity-forbidden k=1k=1 and negative integers) are presented as:

m1/2=m23/2=0, m3/2=1324(pr+1)12Tr(L)δϵ+,  m21/2=1124(pr1)+12Tr(L)δ+ϵ,\begin{align*} &m_{1/2}=m_{23/2}=0, \ &m_{3/2} = \frac{13}{24}(p^r+1) - \frac{1}{2}\mathrm{Tr}(L) - \delta - \epsilon_+,\ &\cdots\ &m_{21/2}= -\frac{11}{24}(p^r-1) + \frac{1}{2}\mathrm{Tr}(L) - \delta + \epsilon_-, \end{align*}

where δ=(2+(1pr))/8\delta = (2 + (-1|p^r))/8 and ϵ±=(1±(pr3))/6\epsilon_\pm = (1 \pm (p^r|3))/6 (with appropriate Legendre symbols). Full explicit expressions are given in [(Candelori et al., 2016), Table 4.1].

5. Limiting Profile and Distribution of Generating Weights

By analyzing the lower-order terms and taking pp\to\infty (for fixed rr), or rr\to\infty (for fixed pp), the multiplicity ratios mk/(2pr)m_k/(2p^r) stabilize to a bi-modal profile:

0for k=1/2,23/2 1/48for k=3/2,21/2 3/48for k=5/2,19/2 5/48for k=7/2,17/2 7/48for k=9/2,15/2 8/48for k=11/2,13/2 \begin{array}{ll} 0 & \text{for } k=1/2,\,23/2 \ 1/48 & \text{for } k=3/2,\,21/2 \ 3/48 & \text{for } k=5/2,\,19/2 \ 5/48 & \text{for } k=7/2,\,17/2 \ 7/48 & \text{for } k=9/2,\,15/2 \ 8/48 & \text{for } k=11/2,\,13/2 \ \end{array}

As a consequence, the generating weights of the free module M(ρA)M(\rho_A) "pile up" around $11/2$ and $13/2$ in the large-dimension limit, offering a refined structural view of the modular form landscape for these representations (Candelori et al., 2016).

6. Quadratic Gauss Sums and the Weil Representation: Prime and Composite Moduli

The matrix elements of the Weil representation, especially for cyclic quadratic modules over Z/pZ\mathbb{Z}/p\mathbb{Z}, are expressible by explicit quadratic Gauss sums. For a symmetric integral n×nn\times n matrix GG and prime pp, reduction brings Q(x)=aixi2/2Q(x)=\sum a_i x_i^2/2 modulo pp. General Gauss sums Gp(λ)G_p(\lambda) factor as products of classical 1D Gauss sums, with

gp(a;)=xFpe((ax2+x)/p)=ϵp(a/p)pe(2(4a)1/p),g_p(a;\ell) = \sum_{x\in\mathbb{F}_p} e((a x^2 + \ell x)/p) = \epsilon_p (a/p)\sqrt{p} e(-\ell^2 (4a)^{-1}/p),

where (a/p)(a/p) is the Legendre symbol, and ϵp=1\epsilon_p=1 or ii for p1,3mod4p\equiv 1,3 \bmod 4 (Zhu, 17 Dec 2025).

More generally, for D=Zn/pZnD=\mathbb{Z}^n/p\mathbb{Z}^n and quadratic form QQ, the Weil representation acts by:

ρ(T)α,β=δα,βe(Q(α)),ρ(S)α,β=e(n/8)/pn/2e(αTβ/p).\rho(T)_{\alpha,\beta} = \delta_{\alpha,\beta} e(Q(\alpha)),\qquad \rho(S)_{\alpha,\beta} = e(n/8)/p^{n/2} e(-\alpha^T\beta/p).

Such formulas unify the representation theory across prime and composite moduli, avoiding the necessity of local data or theta-series limits (Zhu, 17 Dec 2025).

7. Geometric and Computational Methods

The vector bundle aspects of the theory are formulated on the stacky curve P(8,12)\mathbb{P}(8,12). The free module structure is proved via geometric arguments, employing Riemann–Roch for Deligne–Mumford stacks and Serre duality to determine vanishing and non-vanishing of the relevant cohomology groups. The critical weights are handled by results of Skoruppa–Serre–Stark. Closed-form counting of generating weights ultimately depends on explicit evaluation of Gauss sum traces and class number formulae (Candelori et al., 2016).

Algorithmically, invariants and bases of the Weil representation for arbitrary finite quadratic modules can be computed via linear algebra methods. Efficiency improvements stem from symmetrizations and splitting into pp-parts, with the global invariant space recovered as a tensor product of local ones. Under integrality and suitable reduction, the dimensions and bases remain unchanged modulo suitable primes (Ehlen et al., 2017).


The finite-prime Weil quadratic form thus exhibits a highly explicit and computable structure, both algebraically and geometrically, with direct consequences for the arithmetic of vector-valued modular forms and the representation theory of the modular and metaplectic groups (Candelori et al., 2016, Ehlen et al., 2017, Zhu, 17 Dec 2025).

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