English

Periodic Fourier representation of Boolean functions

Quantum Physics 2019-03-27 v3 Computational Complexity

Abstract

In this work, we consider a new type of Fourier-like representation of Boolean function f ⁣:{+1,1}n{+1,1}f\colon\{+1,-1\}^n\to\{+1,-1\} f(x)=cos(πS[n]ϕSiSxi). f(x) = \cos\left(\pi\sum_{S\subseteq[n]}\phi_S \prod_{i\in S} x_i\right). This representation, which we call the periodic Fourier representation, of Boolean function is closely related to a certain type of multipartite Bell inequalities and non-adaptive measurement-based quantum computation with linear side-processing (NMQC\mathrm{NMQC}_\oplus). The minimum number of non-zero coefficients in the above representation, which we call the periodic Fourier sparsity, is equal to the required number of qubits for the exact computation of ff by NMQC\mathrm{NMQC}_\oplus. Periodic Fourier representations are not unique, and can be directly obtained both from the Fourier representation and the F2\mathbb{F}_2-polynomial representation. In this work, we first show that Boolean functions related to Z/4Z\mathbb{Z}/4\mathbb{Z}-polynomial have small periodic Fourier sparsities. Second, we show that the periodic Fourier sparsity is at least 2degF2(f)12^{\mathrm{deg}_{\mathbb{F}_2}(f)}-1, which means that NMQC\mathrm{NMQC}_\oplus efficiently computes a Boolean function ff if and only if F2\mathbb{F}_2-degree of ff is small. Furthermore, we show that any symmetric Boolean function, e.g., ANDn\mathsf{AND}_n, Modn3\mathsf{Mod}^3_n, Majn\mathsf{Maj}_n, etc, can be exactly computed by depth-2 NMQC\mathrm{NMQC}_\oplus using a polynomial number of qubits, that implies exponential gaps between NMQC\mathrm{NMQC}_\oplus and depth-2 NMQC\mathrm{NMQC}_\oplus.

Keywords

Cite

@article{arxiv.1803.09947,
  title  = {Periodic Fourier representation of Boolean functions},
  author = {Ryuhei Mori},
  journal= {arXiv preprint arXiv:1803.09947},
  year   = {2019}
}

Comments

18 pages, 2 figures, 2 tables

R2 v1 2026-06-23T01:06:04.187Z