A Boolean function takes each vector of bits to either zero or one. Use independent uniform input bits; the influence of a variable is the probability that flipping that bit changes the value. A quite fair Boolean function has . All logarithms in the estimates below are natural, except where a base is explicitly written.
Here is a balanced tribes construction with unused coordinates valid for every . For each put , and choose the largest with . Partition of the bits into blocks of size . Let be one when at least one block is all ones, and ignore the other bits. This is a tribes function. With , its zero probability is .
For the function is a single bit and has mean . For , and . The elementary inequalities giveThus both output probabilities are between one quarter and three quarters.
A used bit is pivotal exactly when the other bits of its block are one and every other block fails. Hence its influence is ; unused bits have zero influence. Maximality of gives . Also for : this is immediate for , while for one has . ThereforeThis proves the requested existence with room in the constant. The dimension-one boundary case cannot satisfy the printed logarithmic bound: a quite fair function of one bit is nonconstant and has influence one, whereas . Thus the statement requires the usual nontrivial range (or its intended large- interpretation).
Use normalized Fourier-Walsh transform coefficients . The Hamming weight counts the nonzero coordinates. Norms on the input cube use uniform probability, and a frequency integral here is counting over . A common alternative normalization multiplies both sides of the requested comparison by the same factor and does not change it.
Beckner's inequality states that for and , the noise operator on the Boolean hypercube, with coefficients , satisfies . In particular choose , , .
Let and . Then . On frequencies of weight at most two, , so Beckner's inequality and Parseval's identity give the low-degree Fourier mass of a sparse Boolean set estimateThe indicator function is real and the cube characters are real, so the displayed squares equal the squared absolute values. Total Fourier weight is . If , then and , since . ThereforeThis establishes the strict comparison for every power , not merely for an unspecified very large threshold. The original PDF supplies the density condition and Beckner request, both missing from the converted TeX.
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