Cayley graphs of the Boolean cube #
The Cayley graph of the cube ι → Bool with generators s₁, …, s_d joins each u to u + sⱼ
along its j-th edge (Cslib.RotationMap.cubeCayley). Every bit string is its own negative, so
this is an undirected d-regular multigraph and the rotation map is an involution.
Its walk operator multiplies the Fourier coefficient of each function at S by the bias of the
generators at S (Cslib.RotationMap.fourierCoeff_walk_cubeCayley). The characters are therefore
its eigenvectors, and by Plancherel's identity its spectral expansion is at most the bias of the
generators: if the uniform distribution over the generators is ε-biased with ε ≥ 0, then
λ(G) ≤ ε (Cslib.RotationMap.spectralExpansion_cubeCayley_le). The expander mixing lemma then
counts the edges between two sets (Cslib.RotationMap.card_interedges_cubeCayley_le), again for
ε ≥ 0. This is the mixing estimate (6.3) in the proof
of [OpenAI2026ETH, Lemma 6.1], whose bipartite double cover has left vertex u joined by its
j-th edge to right vertex u + sⱼ.
Main definitions #
Cslib.RotationMap.cubeCayley: the Cayley graph of the cube with given generators.
Main results #
Cslib.RotationMap.fourierCoeff_walk_cubeCayley: the walk is diagonal in the Fourier basis.Cslib.RotationMap.spectralExpansion_cubeCayley_le: small-bias generators give small spectral expansion.Cslib.RotationMap.card_interedges_cubeCayley_le: the edge count between two sets.
References #
The Cayley graph of the cube with generators s j: the j-th edge at u leads to u + s j,
where it is also the j-th edge.
Instances For
The walk operator of a Cayley graph of the cube multiplies each Fourier coefficient by the bias of the generators.
Small-bias generators give small spectral expansion: if the uniform distribution over the
generators is ε-biased, with ε ≥ 0, the spectral expansion of the Cayley graph is at most
ε.
Edges between two sets of a small-bias Cayley graph (the mixing estimate (6.3) of
[OAI26c]): if the generators are ε-biased, with ε ≥ 0, the number of edges from U to
V is at most d |U| |V| / 2^|ι| + ε d √(|U| |V|).