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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 p≥5p\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 p≥5p\geq 5 and integer r≥1r\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:A→Q/Zq:A\to\mathbb{Q}/\mathbb{Z} is defined by q(a)=a2/(2pr) mod 1q(a) = a^2/(2p^r) \bmod 1. The associated symmetric bilinear form is b(a,b)=q(a+b)−q(a)−q(b)=ab/pr mod 1b(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 p≥5p\geq 50 is a finite abelian group and p≥5p\geq 51 satisfies p≥5p\geq 52 and yields a p≥5p\geq 53-bilinear map p≥5p\geq 54 (Ehlen et al., 2017). When the bilinear form p≥5p\geq 55 is nondegenerate, p≥5p\geq 56 is called nondegenerate. The level of p≥5p\geq 57 is the minimal positive integer p≥5p\geq 58 with p≥5p\geq 59 for all p≥5p\geq 50.

For these cyclic modules, the signature p≥5p\geq 51 mod p≥5p\geq 52, 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 p≥5p\geq 53 of the metaplectic group p≥5p\geq 54 acts naturally on the group algebra p≥5p\geq 55 with the standard delta basis p≥5p\geq 56 and p≥5p\geq 57. The action of the standard generators p≥5p\geq 58 and p≥5p\geq 59 is:

  • r≥1r\geq 10
  • r≥1r\geq 11

with r≥1r\geq 12 and r≥1r\geq 13 because r≥1r\geq 14 (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, r≥1r\geq 15, 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 r≥1r\geq 16, the space of vector-valued modular forms of weight r≥1r\geq 17 transforming under r≥1r\geq 18 can be constructed as the sheaf r≥1r\geq 19 on the metaplectic orbifold, which in this context is identified with the weighted projective line m=2prm=2p^r0. The graded module of such forms,

m=2prm=2p^r1

is a free module of rank m=2prm=2p^r2 over m=2prm=2p^r3, the ring of (scalar) modular forms for m=2prm=2p^r4. If m=2prm=2p^r5 are the generating weights,

m=2prm=2p^r6

where m=2prm=2p^r7 is an exponent matrix determined by the action of m=2prm=2p^r8. The standard exponents satisfy m=2prm=2p^r9 (Candelori et al., 2016).

4. Explicit Formulas for Generating Weights and Multiplicities

The generating weights have closed-form expressions as functions of A=Z/mZA=\mathbb{Z}/m\mathbb{Z}0 and A=Z/mZA=\mathbb{Z}/m\mathbb{Z}1 via an explicit trace-of-exponents formula:

A=Z/mZA=\mathbb{Z}/m\mathbb{Z}2

where A=Z/mZA=\mathbb{Z}/m\mathbb{Z}3 encodes data from Dirichlet class numbers and A=Z/mZA=\mathbb{Z}/m\mathbb{Z}4 modulo A=Z/mZA=\mathbb{Z}/m\mathbb{Z}5.

The dimension-generating series is

A=Z/mZA=\mathbb{Z}/m\mathbb{Z}6

Multiplicity formulas for each allowed half-integral weight A=Z/mZA=\mathbb{Z}/m\mathbb{Z}7 (excluding the parity-forbidden A=Z/mZA=\mathbb{Z}/m\mathbb{Z}8 and negative integers) are presented as:

A=Z/mZA=\mathbb{Z}/m\mathbb{Z}9

where q:A→Q/Zq:A\to\mathbb{Q}/\mathbb{Z}0 and q:A→Q/Zq:A\to\mathbb{Q}/\mathbb{Z}1 (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 q:A→Q/Zq:A\to\mathbb{Q}/\mathbb{Z}2 (for fixed q:A→Q/Zq:A\to\mathbb{Q}/\mathbb{Z}3), or q:A→Q/Zq:A\to\mathbb{Q}/\mathbb{Z}4 (for fixed q:A→Q/Zq:A\to\mathbb{Q}/\mathbb{Z}5), the multiplicity ratios q:A→Q/Zq:A\to\mathbb{Q}/\mathbb{Z}6 stabilize to a bi-modal profile:

q:A→Q/Zq:A\to\mathbb{Q}/\mathbb{Z}7

As a consequence, the generating weights of the free module q:A→Q/Zq:A\to\mathbb{Q}/\mathbb{Z}8 "pile up" around q:A→Q/Zq:A\to\mathbb{Q}/\mathbb{Z}9 and q(a)=a2/(2pr) mod 1q(a) = a^2/(2p^r) \bmod 10 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 q(a)=a2/(2pr) mod 1q(a) = a^2/(2p^r) \bmod 11, are expressible by explicit quadratic Gauss sums. For a symmetric integral q(a)=a2/(2pr) mod 1q(a) = a^2/(2p^r) \bmod 12 matrix q(a)=a2/(2pr) mod 1q(a) = a^2/(2p^r) \bmod 13 and prime q(a)=a2/(2pr) mod 1q(a) = a^2/(2p^r) \bmod 14, reduction brings q(a)=a2/(2pr) mod 1q(a) = a^2/(2p^r) \bmod 15 modulo q(a)=a2/(2pr) mod 1q(a) = a^2/(2p^r) \bmod 16. General Gauss sums q(a)=a2/(2pr) mod 1q(a) = a^2/(2p^r) \bmod 17 factor as products of classical 1D Gauss sums, with

q(a)=a2/(2pr) mod 1q(a) = a^2/(2p^r) \bmod 18

where q(a)=a2/(2pr) mod 1q(a) = a^2/(2p^r) \bmod 19 is the Legendre symbol, and b(a,b)=q(a+b)−q(a)−q(b)=ab/pr mod 1b(a,b)=q(a+b)-q(a)-q(b) = ab/p^r \bmod 10 or b(a,b)=q(a+b)−q(a)−q(b)=ab/pr mod 1b(a,b)=q(a+b)-q(a)-q(b) = ab/p^r \bmod 11 for b(a,b)=q(a+b)−q(a)−q(b)=ab/pr mod 1b(a,b)=q(a+b)-q(a)-q(b) = ab/p^r \bmod 12 (Zhu, 17 Dec 2025).

More generally, for b(a,b)=q(a+b)−q(a)−q(b)=ab/pr mod 1b(a,b)=q(a+b)-q(a)-q(b) = ab/p^r \bmod 13 and quadratic form b(a,b)=q(a+b)−q(a)−q(b)=ab/pr mod 1b(a,b)=q(a+b)-q(a)-q(b) = ab/p^r \bmod 14, the Weil representation acts by:

b(a,b)=q(a+b)−q(a)−q(b)=ab/pr mod 1b(a,b)=q(a+b)-q(a)-q(b) = ab/p^r \bmod 15

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 b(a,b)=q(a+b)−q(a)−q(b)=ab/pr mod 1b(a,b)=q(a+b)-q(a)-q(b) = ab/p^r \bmod 16. 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 b(a,b)=q(a+b)−q(a)−q(b)=ab/pr mod 1b(a,b)=q(a+b)-q(a)-q(b) = ab/p^r \bmod 17-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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