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Amplification via Non-Abelian Characters

Updated 18 November 2025
  • The paper presents an amplification argument using non-abelian characters to achieve a power-saving of c⁻¹/₁₂ in bilinear Kloosterman sum bounds, breaking classical limits in analytic number theory.
  • The technique leverages the representation theory of SL₂(Z/cZ) through character orthogonality and combinatorial group estimates to refine results beyond traditional Weil and Fourier bounds.
  • This method not only sharpens L-function moment asymptotics and large sieve inequalities but also paves the way for constructing infinite-dimensional, traceable non-abelian representations.

An amplification argument with non-abelian characters is an analytic technique leveraging the representation theory of non-abelian finite groups, specifically through character orthogonality and convolution, to obtain power-saving bounds in bilinear sums, especially when the natural Fourier methods stagnate. Recent advances show the utility of these methods in bounding Type II (bilinear) sums involving Kloosterman sums at composite moduli, breaking longstanding barriers in analytic number theory, with ramifications for LL-function moment asymptotics and large sieve inequalities.

1. Context: Bilinear Kloosterman Sums and Classical Barriers

Type II (bilinear) sums of Kloosterman sums,

S=mInJαmβn  Kl(am,n;c),S = \sum_{m \in I}\sum_{n \in J} \alpha_m \beta_n \; \mathrm{Kl}(am, n; c),

with Kl(m,n;c)=x(Z/cZ)×e(mx+nx1c)\mathrm{Kl}(m, n; c) = \sum_{x \in (\mathbb{Z}/c\mathbb{Z})^\times} e\left( \frac{m x + n x^{-1}}{c} \right), are central in analytic number theory, notably in studies of automorphic LL-functions and equidistribution. Previous approaches rely either on the Weil bound (Kl()c\mathrm{Kl}(\cdot) \ll \sqrt{c}) or Fourier analysis on the abelian group (Z/cZ)×(\mathbb{Z}/c\mathbb{Z})^\times (Pólya–Vinogradov), which yield “trivial” bounds of order min(c,MNc)\min(c, \sqrt{MNc}) up to co(1)c^{o(1)}. When MNcMN \approx c, surpassing these bounds has been classically difficult, especially for composite cc (notably near-primes S=mInJαmβn  Kl(am,n;c),S = \sum_{m \in I}\sum_{n \in J} \alpha_m \beta_n \; \mathrm{Kl}(am, n; c),0, squares S=mInJαmβn  Kl(am,n;c),S = \sum_{m \in I}\sum_{n \in J} \alpha_m \beta_n \; \mathrm{Kl}(am, n; c),1). The recent non-abelian amplification argument saves a power S=mInJαmβn  Kl(am,n;c),S = \sum_{m \in I}\sum_{n \in J} \alpha_m \beta_n \; \mathrm{Kl}(am, n; c),2 at critical range S=mInJαmβn  Kl(am,n;c),S = \sum_{m \in I}\sum_{n \in J} \alpha_m \beta_n \; \mathrm{Kl}(am, n; c),3 for such S=mInJαmβn  Kl(am,n;c),S = \sum_{m \in I}\sum_{n \in J} \alpha_m \beta_n \; \mathrm{Kl}(am, n; c),4, pushing beyond previous limits (Pascadi, 11 Nov 2025).

2. Non-Abelian Group-Theoretic Framework

The amplification builds on Fourier analysis over the non-abelian group S=mInJαmβn  Kl(am,n;c),S = \sum_{m \in I}\sum_{n \in J} \alpha_m \beta_n \; \mathrm{Kl}(am, n; c),5, which acts by Möbius transformations on the projective line S=mInJαmβn  Kl(am,n;c),S = \sum_{m \in I}\sum_{n \in J} \alpha_m \beta_n \; \mathrm{Kl}(am, n; c),6. The permutation representation

S=mInJαmβn  Kl(am,n;c),S = \sum_{m \in I}\sum_{n \in J} \alpha_m \beta_n \; \mathrm{Kl}(am, n; c),7

possesses character S=mInJαmβn  Kl(am,n;c),S = \sum_{m \in I}\sum_{n \in J} \alpha_m \beta_n \; \mathrm{Kl}(am, n; c),8. The relevant subrepresentation, after orthogonal projection by Möbius inversion to “sift” coprimality and oldforms, is

S=mInJαmβn  Kl(am,n;c),S = \sum_{m \in I}\sum_{n \in J} \alpha_m \beta_n \; \mathrm{Kl}(am, n; c),9

with Kl(m,n;c)=x(Z/cZ)×e(mx+nx1c)\mathrm{Kl}(m, n; c) = \sum_{x \in (\mathbb{Z}/c\mathbb{Z})^\times} e\left( \frac{m x + n x^{-1}}{c} \right)0 the projection to functions constant on Kl(m,n;c)=x(Z/cZ)×e(mx+nx1c)\mathrm{Kl}(m, n; c) = \sum_{x \in (\mathbb{Z}/c\mathbb{Z})^\times} e\left( \frac{m x + n x^{-1}}{c} \right)1-orbits. This Kl(m,n;c)=x(Z/cZ)×e(mx+nx1c)\mathrm{Kl}(m, n; c) = \sum_{x \in (\mathbb{Z}/c\mathbb{Z})^\times} e\left( \frac{m x + n x^{-1}}{c} \right)2 is of dimension Kl(m,n;c)=x(Z/cZ)×e(mx+nx1c)\mathrm{Kl}(m, n; c) = \sum_{x \in (\mathbb{Z}/c\mathbb{Z})^\times} e\left( \frac{m x + n x^{-1}}{c} \right)3 and decomposes into irreducibles with dimensions Kl(m,n;c)=x(Z/cZ)×e(mx+nx1c)\mathrm{Kl}(m, n; c) = \sum_{x \in (\mathbb{Z}/c\mathbb{Z})^\times} e\left( \frac{m x + n x^{-1}}{c} \right)4.

3. Amplifier Construction and Character Orthogonality

With smoothing and abelian Fourier transforms in Kl(m,n;c)=x(Z/cZ)×e(mx+nx1c)\mathrm{Kl}(m, n; c) = \sum_{x \in (\mathbb{Z}/c\mathbb{Z})^\times} e\left( \frac{m x + n x^{-1}}{c} \right)5, the Kloosterman matrix is reduced to an operator norm Kl(m,n;c)=x(Z/cZ)×e(mx+nx1c)\mathrm{Kl}(m, n; c) = \sum_{x \in (\mathbb{Z}/c\mathbb{Z})^\times} e\left( \frac{m x + n x^{-1}}{c} \right)6, for

Kl(m,n;c)=x(Z/cZ)×e(mx+nx1c)\mathrm{Kl}(m, n; c) = \sum_{x \in (\mathbb{Z}/c\mathbb{Z})^\times} e\left( \frac{m x + n x^{-1}}{c} \right)7

where Kl(m,n;c)=x(Z/cZ)×e(mx+nx1c)\mathrm{Kl}(m, n; c) = \sum_{x \in (\mathbb{Z}/c\mathbb{Z})^\times} e\left( \frac{m x + n x^{-1}}{c} \right)8 are standard generators. The non-abelian amplifier is inserted as follows:

Kl(m,n;c)=x(Z/cZ)×e(mx+nx1c)\mathrm{Kl}(m, n; c) = \sum_{x \in (\mathbb{Z}/c\mathbb{Z})^\times} e\left( \frac{m x + n x^{-1}}{c} \right)9

where LL0 is a normal subgroup (typically LL1), and LL2 are traces of irreducible representations. By exploiting character orthogonality and positivity, for even LL3,

LL4

Irreducibility and subgroup normality underpin the bound, reducing the problem to explicit evaluations on LL5 and combinatorial counts in LL6.

4. Analytical Ingredients and Combinatorial Estimates

Three principal analytic inputs:

  • Character sum over LL7: By Clifford theory, for LL8,

LL9

delivering a large denominator for the amplifier.

  • Pointwise bounds for characters: For Kl()c\mathrm{Kl}(\cdot) \ll \sqrt{c}0, Kl()c\mathrm{Kl}(\cdot) \ll \sqrt{c}1, with Kl()c\mathrm{Kl}(\cdot) \ll \sqrt{c}2, Kl()c\mathrm{Kl}(\cdot) \ll \sqrt{c}3; so typically large on-diagonal, small off-diagonal.
  • Solution counting in Kl()c\mathrm{Kl}(\cdot) \ll \sqrt{c}4: For Kl()c\mathrm{Kl}(\cdot) \ll \sqrt{c}5,

Kl()c\mathrm{Kl}(\cdot) \ll \sqrt{c}6

saving a factor of Kl()c\mathrm{Kl}(\cdot) \ll \sqrt{c}7 over the naive Kl()c\mathrm{Kl}(\cdot) \ll \sqrt{c}8 total.

5. Main Bilinear Bounds and their Extensions

Merging the preceding arguments yields for intervals Kl()c\mathrm{Kl}(\cdot) \ll \sqrt{c}9 of lengths (Z/cZ)×(\mathbb{Z}/c\mathbb{Z})^\times0, with (Z/cZ)×(\mathbb{Z}/c\mathbb{Z})^\times1,

(Z/cZ)×(\mathbb{Z}/c\mathbb{Z})^\times2

For critical (Z/cZ)×(\mathbb{Z}/c\mathbb{Z})^\times3 (with (Z/cZ)×(\mathbb{Z}/c\mathbb{Z})^\times4, (Z/cZ)×(\mathbb{Z}/c\mathbb{Z})^\times5, (Z/cZ)×(\mathbb{Z}/c\mathbb{Z})^\times6), this gives a saving of (Z/cZ)×(\mathbb{Z}/c\mathbb{Z})^\times7 for (Z/cZ)×(\mathbb{Z}/c\mathbb{Z})^\times8. For general modulus (Z/cZ)×(\mathbb{Z}/c\mathbb{Z})^\times9, employing hybrid arguments (gluing results at prime factors), the bound improves over Pólya–Vinogradov for all min(c,MNc)\min(c, \sqrt{MNc})0 and all min(c,MNc)\min(c, \sqrt{MNc})1, specifically with

min(c,MNc)\min(c, \sqrt{MNc})2

for any min(c,MNc)\min(c, \sqrt{MNc})3.

6. Applications: min(c,MNc)\min(c, \sqrt{MNc})4-Function Moments and Large Sieve Bounds

Non-abelian amplification yields new asymptotics:

  • Twisted moments of cuspidal min(c,MNc)\min(c, \sqrt{MNc})5-functions: For fixed holomorphic newforms min(c,MNc)\min(c, \sqrt{MNc})6 and any modulus min(c,MNc)\min(c, \sqrt{MNc})7,

min(c,MNc)\min(c, \sqrt{MNc})8

  • Exceptional-spectrum large sieve for Maass forms: For min(c,MNc)\min(c, \sqrt{MNc})9 Maass forms co(1)c^{o(1)}0 with eigenvalues co(1)c^{o(1)}1, coefficients co(1)c^{o(1)}2, any co(1)c^{o(1)}3, and coprime sequence co(1)c^{o(1)}4,

co(1)c^{o(1)}5

substantially improving prior co(1)c^{o(1)}6 savings when co(1)c^{o(1)}7 and co(1)c^{o(1)}8 is composite.

7. Connections to Infinite Characters and Traceable Representations

Amplification arguments with non-abelian characters exploit deep representation-theoretic input, analogous to the infinite character constructions in non-amenable groups acting on trees and higher-rank arithmetic groups (Bekka, 2018). While the Kloosterman amplification operates in the setting of co(1)c^{o(1)}9, the existence of large irreducibles with strong orthogonality and traceability echoes the method of inducing representations from non-amenable subgroups and deforming permutation representations (Julg–Valette trick), which produce uncountably many infinite-dimensional, traceable irreducible representations for non-abelian groups. This highlights the overarching theme: leveraging non-abelian harmonic analysis to both extend the analytic toolkit of number theory—e.g., bounding exponential sums—and to construct new classes of representations with rich properties.


In summary, the amplification argument with non-abelian characters merges non-abelian Fourier techniques, explicit character sum bounds, combinatorial group theory, and analytic number theory to achieve unprecedented savings in bilinear Kloosterman sum estimates for composite moduli. This methodology directly translates to sharper asymptotics in MNcMN \approx c0-function moments and exceptional large sieve bounds, while also elucidating representation-theoretic phenomena such as infinite character construction for non-abelian groups (Pascadi, 11 Nov 2025, Bekka, 2018).

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