Fourier Entropy–Influence conjecture

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Subjects: Analysis and dynamics · Logic and computation

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The problem

A rule takes on/off switches and gives a yes-or-no answer. How much hidden structure can it have if changing one switch rarely changes that answer? For the two-switch AND rule, which says yes only when both are on, flipping one switch changes the answer exactly when the other is on. Under equally likely settings, that happens half the time for each switch. Adding those probabilities gives its total influence. A second description breaks the rule into patterns involving individual switches and combinations of switches. The conjecture asks whether influence always limits how widely that description is spread across patterns.[3] [4]

Scope

For every f:{−1,1}ⁿ→{−1,1}, let p(S)=f̂(S)², H=Σ p(S) log₂(1/p(S)) and I=Σ |S|p(S). Does H≤CI hold for one universal constant C?

What remains open

The required spread measure is Fourier entropy, which uses squared pattern weights, not just a count of switches. The conjecture needs one fixed constant that works for every Boolean rule and every number of switches, with settings equally likely. Results for particular rule families or bounds with an extra term do not establish that guarantee.[3] [4]

Why it matters

The flip test examines one switch at a time, but a rule can depend on combinations that this local view hides. A positive answer would connect stability under these small changes to a compact approximate description using a limited collection of important patterns. It would make local sensitivity informative about global structure.[3]

Definitions

3 terms
total influence

Under equally likely Boolean input settings, add for every input the probability that flipping just that input changes the output. These local flip probabilities form the total sensitivity measure used here.[3] [4]

Fourier weight

The square of a Fourier coefficient, where the coefficient is the average agreement of a sign-valued rule with one parity pattern. All these nonnegative weights sum to one.[3] [4]

Fourier entropy

The entropy of the squared Fourier weights: add each weight times the base-two logarithm of its reciprocal, with zero weights contributing zero. It measures spread over patterns, not simply the number of input variables.[3] [4]

Sources

  1. A new bound for the Fourier-Entropy-Influence conjecture Xiao Han · 2023-12-13
    Notes on A new bound for the Fourier-Entropy-Influence conjecture

    Original arXiv locator retains December 13, 2023 first submission. Definitions, concentration passage and the additional individual-influence term were read in v2, December 10, 2025, separately cited below. The extra term cannot be silently removed.

  2. Further evidence towards the Fourier Entropy-Influence conjecture María José González, Paul MacManus and María Cristina Pereyra · 2026-05-29
    Notes on Further evidence towards the Fourier Entropy-Influence conjecture

    Original arXiv locator retains May 29, 2026 first submission. The freshly read exact v2, June 9, 2026, is separately cited below. Selected splitting, separation and tribes classes are partial results, not the universal conjecture.

  3. A new bound for the Fourier-Entropy-Influence conjecture (arXiv v2) Xiao Han · 2025-12-10
    Notes on A new bound for the Fourier-Entropy-Influence conjecture (arXiv v2)

    Exact v2 revision date. Uniform Boolean definitions, the retained extra influence term and entropy concentration were freshly read. Basic identities and the illustrative example were independently computed; no removal of the extra term or full proof audit is claimed.

  4. Further evidence towards the Fourier Entropy-Influence conjecture (arXiv v2) María José González, Paul MacManus and María Cristina Pereyra · 2026-06-09
    Notes on Further evidence towards the Fourier Entropy-Influence conjecture (arXiv v2)

    Exact v2 revision date. Uniform Boolean setup and results for specified splitting/tribes/separation classes were read. The authored AND example explicitly uses +1 for yes, and is checked directly; it is not a proof of the universal bound.

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