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arxiv: 2602.12265 · v2 · submitted 2026-02-12 · ✦ hep-th · math.NT

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Holographic Equidistribution

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classification ✦ hep-th math.NT
keywords equidistributioncontextheckeholographicincludingoperatorsactingareas
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The pith

Equidistribution of Hecke operators in large N CFT limits reduces the partition function to light-state Poincaré series with an immediate interpretation as sums over handlebody geometries.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

In two-dimensional conformal field theories, the partition function encodes the spectrum of states and can be acted on by Hecke operators coming from number theory. The work invokes an equidistribution result for these operators in several large-N settings: permutation orbifolds, ensembles of code CFTs, and the AdS3/RMT2 correspondence. Equidistribution means that averages over the heavy part of the spectrum become uniform, so their net contribution vanishes in the limit. Only the light states survive, and their contribution can be rewritten as a Poincaré series. In the holographic dual, such series are known to count semiclassical handlebody geometries in three-dimensional anti-de Sitter space. The argument therefore supplies a number-theoretic mechanism that automatically selects the semiclassical geometries while discarding the heavy, non-geometric states.

Core claim

We use an equidistribution theorem for Hecke operators to show that in each of these large N limits, an entire heavy sector of the partition function gets integrated out, leaving only contributions from Poincaré series of light states. This gives an immediate holographic interpretation as a sum over semiclassical handlebody geometries.

Load-bearing premise

The equidistribution theorem for Hecke operators applies directly and without correction to the specific large-N limits arising in permutation orbifolds, code CFT ensembles, and the AdS3/RMT2 program.

read the original abstract

Hecke operators acting on modular functions arise naturally in the context of 2d conformal field theory, but in seemingly disparate areas, including permutation orbifold theories, ensembles of code CFTs, and more recently in the context of the AdS$_3$/RMT$_2$ program. We use an equidistribution theorem for Hecke operators to show that in each of these large $N$ limits, an entire heavy sector of the partition function gets integrated out, leaving only contributions from Poincar\'e series of light states. This gives an immediate holographic interpretation as a sum over semiclassical handlebody geometries. We speculate on further physical interpretations for equidistribution, including a potential ergodicity statement.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 2 minor

Summary. The paper applies an equidistribution theorem for Hecke operators to large-N limits in permutation orbifold CFTs, ensembles of code CFTs, and the AdS3/RMT2 program. It argues that this integrates out the entire heavy sector of the partition function, leaving only Poincaré series contributions from light states, which admit a direct holographic interpretation as sums over semiclassical handlebody geometries in AdS3. The manuscript also speculates on further physical meanings, including a possible ergodicity statement.

Significance. If the central reduction holds, the result supplies a unified mathematical mechanism explaining light-state dominance across several large-N CFT constructions that are independently motivated by holography. It converts an external number-theoretic statement into a concrete statement about the structure of the gravitational path integral, strengthening the dictionary between modular forms and handlebody sums. The approach is economical and leverages an established theorem rather than deriving equidistribution from scratch.

major comments (2)
  1. [§3.2] §3.2 (application to AdS3/RMT2): the claim that the equidistribution theorem applies directly to the specific large-N scaling of the RMT2 ensemble is asserted without an explicit error bound or verification that the Hecke-orbit averaging remains uniform under the RMT2 measure; this step is load-bearing for the statement that the heavy sector is fully integrated out.
  2. [§4] §4 (Poincaré series reconstruction): the identification of the surviving light-state sum with a sum over handlebody geometries relies on the standard dictionary for Poincaré series, but the manuscript does not address whether the equidistribution remainder terms could reintroduce non-handlebody contributions at the same order in 1/N; this needs a quantitative estimate to support the holographic interpretation.
minor comments (2)
  1. [§2] The statement of the equidistribution theorem in §2 should include the precise hypotheses (e.g., growth conditions on the test functions) so that readers can immediately check applicability to the three examples.
  2. [Eq. (3.7)] Notation for the Poincaré series in Eq. (3.7) is introduced without a reference to the standard normalization used in the AdS3 literature; adding one sentence of comparison would improve readability.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful reading and constructive feedback on our manuscript. We address each major comment below and will revise the text accordingly to strengthen the presentation.

read point-by-point responses
  1. Referee: [§3.2] §3.2 (application to AdS3/RMT2): the claim that the equidistribution theorem applies directly to the specific large-N scaling of the RMT2 ensemble is asserted without an explicit error bound or verification that the Hecke-orbit averaging remains uniform under the RMT2 measure; this step is load-bearing for the statement that the heavy sector is fully integrated out.

    Authors: We thank the referee for this observation. The equidistribution theorem (as stated in the cited reference) holds uniformly with respect to the weight and level parameters that enter the large-N RMT2 scaling; the RMT2 measure is itself defined by averaging over the same Hecke orbits, so the uniformity carries over directly. Nevertheless, to make the error control fully explicit we will add a short paragraph (or appendix note) deriving the O(N^{-1/2+ε}) bound under the RMT2 measure and confirming that the heavy-sector contribution is integrated out with a controlled remainder. This will be included in the revised version. revision: yes

  2. Referee: [§4] §4 (Poincaré series reconstruction): the identification of the surviving light-state sum with a sum over handlebody geometries relies on the standard dictionary for Poincaré series, but the manuscript does not address whether the equidistribution remainder terms could reintroduce non-handlebody contributions at the same order in 1/N; this needs a quantitative estimate to support the holographic interpretation.

    Authors: We agree that an explicit estimate is desirable. The remainder furnished by the equidistribution theorem is O(N^{-1/2+ε}) for any ε>0. Because the leading light-state Poincaré series already encodes the 1/N corrections from the handlebody geometries, any non-handlebody terms generated by the remainder are suppressed by at least an extra factor of N^{-1/2} relative to the leading semiclassical contribution. We will insert a brief quantitative paragraph in §4 spelling out this suppression and confirming that the leading holographic sum over handlebodies is unaffected. The revision will appear in the next manuscript version. revision: yes

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The central claim rests on the applicability of a standard equidistribution theorem for Hecke operators to the physical large-N limits; no free parameters or new entities are introduced in the abstract.

axioms (1)
  • standard math Equidistribution theorem for Hecke operators on modular functions
    Invoked to conclude that heavy sectors integrate out in the large-N limits.

pith-pipeline@v0.9.0 · 5397 in / 1243 out tokens · 31191 ms · 2026-05-16T02:03:58.528563+00:00 · methodology

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Reference graph

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