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Petrow–Young Subconvexity Bound

Updated 25 January 2026
  • The paper establishes a Weyl-type subconvexity bound for Dirichlet L-functions with an exponent of 1/6, surpassing the classical convexity barrier.
  • It utilizes innovative analytic and spectral methods, including the approximate functional equation, delta method, and Kuznetsov formula.
  • The result leads to improved distribution exponents for divisor functions like d3(n) and d4(n), advancing equidistribution in arithmetic progressions.

The Petrow–Young subconvexity bound is a breakthrough in analytic number theory that establishes a Weyl-type subconvex estimate for Dirichlet LL-functions of primitive characters, with profound implications for the distribution of divisor functions in arithmetic progressions. The method enables significant improvements on classical “square root barrier” results, enabling new exponents of distribution for d3(n)d_3(n) and d4(n)d_4(n) and advancing the study of mean values of arithmetic functions in residue classes.

1. Formal Statement of the Petrow–Young Subconvexity Bound

Let χ\chi be a primitive Dirichlet character modulo a cube-free integer qq, and let L(s,χ)=n1χ(n)nsL(s,\chi) = \sum_{n \ge 1} \chi(n)n^{-s} for s=12+its = \tfrac12 + it. Petrow and Young prove the following Weyl-type subconvexity bound: L ⁣(12+it,χ)  ε  (q(1+t))16+εL\!\Bigl(\tfrac12+it,\chi\Bigr)\;\ll_{\varepsilon}\;(q(1+|t|))^{\tfrac16+\varepsilon} for every ε>0\varepsilon>0 (Parry, 2024, Aydemir et al., 18 Jan 2026).

Equivalently, the "exponent" θ=1/6\theta = 1/6 may be taken in the general form

L ⁣(12+it,χ)ε(q(1+t))θ+ε.L\!\left(\tfrac12+it,\chi\right) \ll_\varepsilon (q(1+|t|))^{\theta+\varepsilon}.

This subconvex estimate sits strictly below the classical convexity bound with exponent $1/4$, and permits a power-saving improvement crucial to arithmetic equidistribution problems.

2. Outline of the Proof and Main Techniques

The proof proceeds by several innovative analytic and spectral techniques:

  • Approximate Functional Equation: The LL-function is expressed in terms of two dual sums, each of length about (qT)1/2(qT)^{1/2}.
  • Circle/Delta Method: Detection of n=mn = m via a δ\delta-symbol or spectral trace formula on PGL2\mathrm{PGL}_2.
  • Reciprocity and Kuznetsov Formula: The sum is analyzed using Kloosterman sums, whose structure is accessed via the Kuznetsov trace formula on Γ0(q)\Gamma_0(q).
  • Spectral Reciprocity: Introduction of a duality between GL1\mathrm{GL}_1-twists and sums over GL2\mathrm{GL}_2 Fourier coefficients.
  • Amplification and Stationary Phase Analysis: An amplification method (inspired by Duke–Friedlander–Iwaniec) is used to harvest the central values, and oscillatory integrals are bounded by the stationary phase method.

The consequence is a “hybrid” subconvex bound, yielding θ=1/6\theta=1/6 in both qq-aspect and tt-aspect, and thus establishing the stated Weyl-type estimate (Aydemir et al., 18 Jan 2026).

3. Applications to Exponent of Distribution Beyond the Square-Root Barrier

The Petrow–Young bound serves as the analytic foundation for achieving exponents of distribution for divisor functions dk(n)d_k(n) beyond the $1/2$ barrier in arithmetic progressions:

  • Four-fold Divisor Function (d4(n)d_4(n)): Parry demonstrates that d4(n)d_4(n) possesses exponent of distribution $4/7$ on average over residue classes, breaking the qx1/2q \asymp x^{1/2} limit for the first time. The main steps involve smoothing, application of an Ivić multidimensional Voronoi formula, and separation into diagonal/off-diagonal terms. The off-diagonal regime is controlled by employing the Petrow–Young subconvexity in bounding bilinear forms involving LL-functions, culminating in the second-moment estimate

amodqA(a/q)2εx3/2+εq7/8\sum_{a\bmod q}\bigl|A(a/q)\bigr|^2 \ll_\varepsilon x^{3/2+\varepsilon}q^{7/8}

for prime qx4/7εq \le x^{4/7 - \varepsilon}. This leads to individual error terms E(x;q,a)E(x;q,a) of size x1δ\ll x^{1-\delta}, confirming equidistribution of d4(n)d_4(n) up to qx4/7q\le x^{4/7} (Parry, 2024).

  • Ternary Divisor Function (d3(n)d_3(n)): The techniques transfer to d3(n)d_3(n), and by similar analysis the exponent of distribution is improved from $2/3$ to $8/11$ after averaging over residue classes modulo a prime qq. In this context, the Petrow–Young bound is invoked at several points:
    • Bounding bilinear sums involving d3(n)d_3(n) via Dirichlet character orthogonality,
    • Employing Perron's formula to express sums over d3(n)χ(n)d_3(n)\chi(n) in terms of L(s,χ)3L(s,\chi)^3,
    • Applying hybrid and averaged Weyl-type bounds for LL-functions within tt and qq-aspects.
    • The resulting mean square error is

a=1qEx(q,a)2εx3/2+εq11/16\sum_{a=1}^q |E_x(q,a)|^2 \ll_\varepsilon x^{3/2+\varepsilon} q^{11/16}

for qx8/11q \le x^{8/11}, thus confirming substantial progress over prior results (Aydemir et al., 18 Jan 2026).

4. Technical Preconditions and Functional Ranges

The subconvexity result and its applications are subject to several precise restrictions:

  • The character χ\chi must be primitive of conductor qq, with qq required to be cube-free in Petrow–Young (prime qq is allowed).
  • All bounds are uniform in tRt \in \mathbb{R} and for all ε>0\varepsilon > 0.
  • In distribution problems for dk(n)d_k(n), the modulus qq is required to satisfy qxθq \le x^{\theta}, with θ=4/7\theta=4/7 for d4(n)d_4(n), θ=8/11\theta=8/11 for d3(n)d_3(n) under averaging, as set by the detailed optimization of second moment bounds.

The principal consequences include:

  • d4(n)d_4(n) Equidistribution: Establishes equidistribution in prime modulus arithmetic progressions beyond the conventional range, achieving power-saving error terms for qx4/7q\le x^{4/7} (Parry, 2024).
  • d3(n)d_3(n) Improvements: Improves the exponent for equidistribution of d3(n)d_3(n) up to modulus qx8/11q\le x^{8/11} on average (Aydemir et al., 18 Jan 2026).
  • Framework for Higher Divisor Functions: The analytic structure provided by Petrow–Young suggests that, for k5k\geq5, any suitable subconvex bound for the relevant LL-functions could yield nontrivial distribution exponents for dk(n)d_k(n). This insight shows the generality and reach of the underlying analytic approach.

A table summarizing key exponents:

Function Classical Exponent With P-Y Bound Modulus Range
d3(n)d_3(n) $2/3$ $8/11$ qx8/11q \le x^{8/11}
d4(n)d_4(n) $1/2$ $4/7$ qx4/7q \le x^{4/7}

6. Key Formulas and Estimate Summary

The following central formulas encapsulate the main analytic advances:

  • Petrow–Young Weyl Bound:

L(12+it,χ)ε(q(1+t))1/6+εL(\tfrac12 + it, \chi) \ll_\varepsilon (q(1+|t|))^{1/6 + \varepsilon}

  • Fourth-Moment Bound (for d4(n)d_4(n)):

TTL(12+it,χ)4dtqT(qT)1/3+ε\int_{-T}^{T} |L(\tfrac12 + it, \chi)|^4\,dt \ll qT (qT)^{1/3+\varepsilon}

  • Second-Moment for Error Terms:

amodqE(x;q,a)2εx3/2+εq7/8\sum_{a\bmod q} |E(x;q,a)|^2 \ll_\varepsilon x^{3/2+\varepsilon} q^{7/8}

for d4(n)d_4(n), and

a=1qEx(q,a)2εx3/2+εq11/16\sum_{a=1}^q |E_x(q,a)|^2 \ll_\varepsilon x^{3/2+\varepsilon} q^{11/16}

for d3(n)d_3(n).

These expressions delineate the pathway from the subconvexity bound to explicit equidistribution results in arithmetic progressions.

7. Impact and Future Directions

The Petrow–Young subconvexity bound provides an essential analytic tool for advancing beyond natural convexity-barrier limits in the study of distribution of arithmetic functions. Its hybrid and uniformly sharp nature is indispensable for mean value theorems and divisor distribution problems. A plausible implication is that further enhancements in subconvex bounds for Dirichlet or related automorphic LL-functions would directly enable stronger exponents for various arithmetic function distribution results, particularly for higher dk(n)d_k(n) and analogous settings. The method’s paradigm—melding spectral reciprocity, advanced trace formulae, and optimized moment estimates—serves as a blueprint for subsequent progress in analytic number theory and automorphic forms.

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