The fourth moment of Dirichlet L-functions along a coset and the Weyl bound
Pith reviewed 2026-05-24 16:04 UTC · model grok-4.3
The pith
A fourth moment bound along cosets of characters yields the Weyl subconvex bound for Dirichlet L-functions of every conductor.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
We prove a Lindelof-on-average upper bound for the fourth moment of Dirichlet L-functions of conductor q along a coset of the subgroup of characters modulo d when q* divides d. As a consequence we establish a Weyl-strength subconvex bound for all Dirichlet L-functions with no restrictions on the conductor.
What carries the argument
The fourth moment of L-functions along a coset of characters modulo d, under the divisibility condition q* divides d, which supplies the average input needed for amplification.
If this is right
- The Weyl subconvex bound holds for L(1/2 + it, chi) uniformly in the conductor q.
- All previous conductor restrictions on the Weyl bound for Dirichlet L-functions are removed.
- The same average input can be fed into amplification to reach the individual bound at any height t.
Where Pith is reading between the lines
- If the coset condition q* divides d can be removed, the fourth-moment result would apply to a larger set of averages.
- The method might extend to produce similar average bounds for other moments or for L-functions in different families.
- The resulting subconvexity could be inserted into existing zero-density estimates to improve error terms in prime-number theorems.
Load-bearing premise
The fourth-moment bound holds only when q* divides d, and the passage from this average to the individual Weyl bound relies on amplification techniques whose applicability without further restrictions is taken from prior work.
What would settle it
An explicit numerical check, for a small prime q where q* does not divide d, showing that the fourth moment over the coset exceeds the Lindelof average size, or an explicit Dirichlet L-function whose central value exceeds the Weyl bound.
read the original abstract
We prove a Lindel\"of-on-average upper bound for the fourth moment of Dirichlet $L$-functions of conductor $q$ along a coset of the subgroup of characters modulo $d$ when $q^*|d$, where $q^*$ is the least positive integer such that $q^2|(q^*)^3$. As a consequence, we finish the previous work of the authors and establish a Weyl-strength subconvex bound for all Dirichlet $L$-functions with no restrictions on the conductor.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper proves a Lindelöf-on-average upper bound for the fourth moment of Dirichlet L-functions of conductor q along a coset of the subgroup of characters modulo d when q^* divides d (with q^* the least positive integer such that q^2 divides (q^*)^3). As a consequence, the authors claim to complete their prior work and obtain a Weyl-strength subconvex bound for every Dirichlet L-function with no restrictions on the conductor.
Significance. If the deduction from the restricted coset moment to the unrestricted individual bound holds, the result would be a substantial advance: it would remove all conductor restrictions from the Weyl bound for Dirichlet L-functions, a longstanding goal with implications for many applications in analytic number theory. The coset-average approach itself appears technically novel.
major comments (1)
- [Abstract / consequence section] Abstract and the section deriving the consequence: the fourth-moment bound is established only under the condition q^* | d, yet the central claim is that this yields the Weyl bound for arbitrary q with no restrictions. The manuscript must explicitly verify that the specific form of the coset (modulo d with the divisibility constraint) is compatible with the amplification or related techniques from the authors' earlier work without introducing fresh conditions on q; this compatibility is load-bearing for the unrestricted conclusion but is presented as immediate.
Simulated Author's Rebuttal
We thank the referee for their careful reading and for identifying this point about the deduction from the coset moment to the unrestricted Weyl bound. We address the concern directly below.
read point-by-point responses
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Referee: [Abstract / consequence section] Abstract and the section deriving the consequence: the fourth-moment bound is established only under the condition q^* | d, yet the central claim is that this yields the Weyl bound for arbitrary q with no restrictions. The manuscript must explicitly verify that the specific form of the coset (modulo d with the divisibility constraint) is compatible with the amplification or related techniques from the authors' earlier work without introducing fresh conditions on q; this compatibility is load-bearing for the unrestricted conclusion but is presented as immediate.
Authors: We agree that the compatibility of the coset (under the condition q^* | d) with the amplification from our prior work should be verified explicitly rather than left implicit. In the earlier paper the amplification applies to any coset of characters modulo d and requires no further conditions on q once such a d is fixed. One may always choose d to be a multiple of q^* (for instance d = q^*), which satisfies the divisibility hypothesis without restricting the conductor q in any way. The resulting coset is admissible for the amplification method, and no new constraints on q arise. We will add a short paragraph in the consequence section spelling out this choice of d and confirming that the prior amplification applies verbatim. revision: yes
Circularity Check
Minor self-citation to prior work completes the subconvexity claim; new fourth-moment estimate under q^*|d supplies independent content
full rationale
The abstract presents a new Lindelöf-on-average fourth-moment bound that holds precisely when q^* divides d. The passage to an unrestricted Weyl bound is described as finishing the authors' previous work via amplification or related techniques. This constitutes one minor self-citation that is not load-bearing for the novel moment estimate itself. No equation or derivation in the provided text reduces a claimed prediction to a fitted input or prior result by construction, and the central moment bound retains independent mathematical content against external benchmarks.
Axiom & Free-Parameter Ledger
axioms (2)
- standard math Dirichlet L-functions admit analytic continuation and satisfy a functional equation
- standard math Approximate functional equations express central values via Dirichlet polynomials
Lean theorems connected to this paper
-
IndisputableMonolith/Foundation/RealityFromDistinction.leanreality_from_one_distinction unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
We prove a Lindelöf-on-average upper bound for the fourth moment of Dirichlet L-functions of conductor q along a coset of the subgroup of characters modulo d when q^*|d ... establish a Weyl-strength subconvex bound for all Dirichlet L-functions with no restrictions on the conductor.
-
IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
The sum g(χ,ψ) is multiplicative ... bound g(χ,ψ) ≪ p follows from the theory of ℓ-adic sheaves and trace functions, and in particular the Riemann hypothesis of Deligne.
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Reference graph
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discussion (0)
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