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Concentration and influences

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Abstract

Consider the discrete cube Ω={0,1}N, provided with the uniform probabilityP. We denote byd(x, A) the Hamming distance of a pointx of Ω and a subsetA of Ω. We define the influenceI(A) of theith coordinate onA as follows. Forx in Ω, consider the pointT i (x) obtained by changing the value of theith coordinate. Then\(I_i (A) = P(\{ x \in A;T_i (x) \notin A\} ).\)

We prove that we always have\(P(A)\int_\Omega {d(x,A)dP(x) \leqslant \frac{1}{2}\sum\limits_{i \leqslant N} {I_i (A).} } \)

Since it is easy to see that\(\sum\nolimits_{i \leqslant N} {I_i (A)^2 \leqslant \frac{1}{4}} \), this recovers the well known fact that ∫Ω d(x, A)dP(x) is at most of order\(\sqrt N \) whenP(A)≥1/2. The new information is that ∫Ω d(x, A)dP(x) can be of order\(\sqrt N \) only ifA reassembles the Hamming ball {x; ∑1≤N x i N/2}.

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Correspondence to Michel Talagrand.

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Talagrand, M. Concentration and influences. Isr. J. Math. 111, 275–284 (1999). https://doi.org/10.1007/BF02810688

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  • DOI: https://doi.org/10.1007/BF02810688

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