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Symmetrization and moments of the adjacency difference

PDF p. 33: Proof of Proposition 6.3, first paragraphs

Statement

Let n≥1 and p∈[0,1]. Let A be the adjacency matrix of the loop-free Erdős–Rényi graph G(n,p), and let A′ be an independent copy. Thus the entries indexed by distinct unordered pairs of distinct vertices are independent Bernoulli(p) variables, A is symmetric, and its diagonal is zero. Let I be the identity matrix, J the all-ones matrix, ΔA=A−pJ, and W=A−A′. The norm ∥⋅∥ is the operator norm induced by the Euclidean norm; Tr⁡ denotes the sum of diagonal entries.

Then EA=p(J−I) and E∥ΔA∥≤E∥W∥+p. For each x≠y and each positive integer k, EWx,yk=0 when k is odd and EWx,yk=2p(1−p) when k is even. With the zeroth power interpreted as the constant one, EWx,y0=1. The diagonal entries of W are zero. For every integer ℓ≥1, E∥W∥≤(ETr⁡W2ℓ)1/(2ℓ).

The stronger inequality E∥ΔA∥≤E∥W∥ can fail even when n≥2 and 0<p<1. For instance it fails at p=1−[4n(n−1)]−1.

Facts & Assumptions

[F1]

The centered-matrix and operator-norm conventions give ΔA=A−pJ for reference degree pn and define the induced operator norm (Centered graph matrices and reference degree, Loewner order, Hermitian inner product, and operator norm).

[F2]

The independent-copy construction gives a symmetric zero-diagonal W whose off-diagonal entries are differences of independent Bernoulli(p) variables (Independent-copy symmetrization matrix).

[F3]

Independent-copy norm symmetrization gives E∥A−EA∥≤E∥A−A′∥ and, for this graph, EA=p(J−I) (Norm symmetrization at the actual matrix mean).

[F4]

A difference of two independent Bernoulli(p) variables has odd positive moments zero, positive even moments 2p(1−p), and zeroth moment one (Finite Bernoulli difference laws and parity of moments).

[F5]

For a real symmetric matrix and ℓ≥1, ∥W∥2ℓ≤Tr⁡W2ℓ pointwise (Trace powers, closed walks and independent edge moments).

[F6]

Finite Jensen gives f(∑iqixi)≤∑iqif(xi) for a convex real function and nonnegative weights qi summing to one (Finite Jensen inequality for a convex function and nonnegative weights summing to one).

Proof

Given: The graph, independent copy, and integers in the statement.

Goal: Prove the corrected symmetrization and moment assertions, the trace bound, and the stated counterexample to the stronger inequality.

1.1F1F3givenalgebra

By [F3], ΔA=(A−EA)−pI. The operator norm of I is one, since n≥1 and If=f for every vector. The triangle inequality, followed by [F3], yields E∥ΔA∥≤E∥A−EA∥+p≤E∥W∥+p.

1.2F2F4given

The off-diagonal description in [F2] permits direct application of [F4] to every x≠y. It gives the positive odd and even moments and the separately stated zeroth moment. The diagonal assertion follows from [F2].

1.3F5F6givenalgebra

The finite graph sample space makes X=∥W∥ a nonnegative finite-valued random variable. Put m=2ℓ≥2. For s,t≥0, direct polynomial multiplication gives tm−sm−msm−1(t−s)=(t−s)2∑j=0m−2(j+1)tm−2−jsj≥0, where zeroth powers are constant one. Given x,y≥0 and q∈[0,1], apply this inequality at s=qx+(1−q)y with t=x and t=y, and multiply the two inequalities by q and 1−q. The linear terms cancel, yielding sm≤qxm+(1−q)ym. Thus f(t)=t2ℓ is convex on [0,∞). Apply [F6] to this function with weights equal to the outcome probabilities. Thus (EX)2ℓ≤EX2ℓ≤ETr⁡W2ℓ by [F5]. Taking the nonnegative 2ℓ-th root proves the trace bound.

2.1F1F2F4givenalgebra∎

For n≥2, each diagonal entry of ΔA is −p, so applying ΔA to a standard unit vector shows ∥ΔA∥≥p. On the other hand, the operator norm is at most the sum of the absolute values of all matrix entries: each matrix unit has norm one, and the triangle inequality applies. By [F2] and [F4], E∣Wxy∣=2p(1−p) for x≠y and the diagonal is zero. Hence E∥W∥≤2n(n−1)p(1−p). At p=1−[4n(n−1)]−1 this upper bound is p/2<p≤E∥ΔA∥. These steps establish all assertions.

Source notes

The article's proof of Proposition 6.3 displays the stronger symmetrization inequality and states the even-moment formula for all ℓ≥0. The corrected bounds above retain the positive-moment and trace claims while accounting for the nonzero mean EΔA=−pI and the zeroth moment. The article is cited for attribution, not as a proof of this lemma.

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