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Analytic versus numerical regular-expander bounds — Remark 1.5

PDF p. 7: Remark 1.5; PDF p. 29: Section 5, paragraph following the numerical table

Statement

Assume countable choice: every countable family of nonempty sets has a choice function. Let G=(V,E) be a finite undirected graph with n=∣V∣>0 vertices, at most one edge between each pair, and self-loops allowed. Its binary symmetric adjacency matrix A has Axy=1 when x and y are adjacent and 0 otherwise; a diagonal entry records a self-loop. Assume G is d-regular with d>0: every row sum ∑y∈VAxy equals d, so a loop contributes once to its vertex degree. Write J for the all-ones matrix. An (n,d,α)-expander satisfies ∥A−(d/n)J∥≤αd, in the Euclidean operator norm. The graph is globally synchronizing if, for phase-volume almost every initial state of the homogeneous Kuramoto system, the rotating-frame trajectory converges to a state in which all phases agree.

If G is an (n,d,α)-expander with α≤0.0068, then it is globally synchronizing. In the article's convention, a d-regular Ramanujan graph is an (n,d,2d−1/d)-expander; it is globally synchronizing when d≥85730.

The article contrasts the 0.0068 consequence of Theorem 1.10 with its stronger 0.0816 regular-expander bound, whose proof uses numerical computations. The degree conclusion follows by applying Theorem 1.10 directly at a slightly larger parameter, not by asserting that 2d−1/d≤0.0068 at d=85730.

Facts & Assumptions

[F1]

A d-regular (n,d,a)-expander is an (n,d,a,−a,a)-expander (Regular adjacency expansion supplies two-sided expansion). The adjacency predicate remains true if its nonnegative parameter is enlarged (Adjacency spectral expander — Definition 1.3).

[F2]

Under countable choice, Theorem 1.10 makes an (n,d,a,c−,c+)-expander globally synchronizing when d>0, c−>−1, 0<a≤1/5, and 32a(1+4c+−3c−)(1+c−)2log⁡ ⁣(1+c++a2a)<1 (General two-sided spectral criterion — Theorem 1.10, The Axiom of Countable Choice (AC_ω)).

[F3]

For real t, exp⁡(t)=∑k=0∞tk/k!; log⁡ is its inverse on positive reals, and exp⁡ is strictly increasing (The real exponential function and the number e by a power series, The natural logarithm as the inverse of the exponential function, The exponential function is strictly increasing).

Proof

Given: The graph and hypotheses in the Statement, with countable choice.

Goal: Establish the two consequences of Theorem 1.10 and distinguish the parameter calculations.

1.1F3algebra

Put b=85383/12500000 and t=107669/25000. Exact rational arithmetic gives 0.0068<b<1/5, ∑k=020tk/k!>(1+2b)/(2b), and 32b(1+7b)(1−b)2t=481633281478542348481633485177153125<1. All terms after the twentieth in the exponential series are positive, so [F3] gives log⁡((1+2b)/(2b))<t. Hence 32b(1+7b)(1−b)2log⁡((1+2b)/(2b))<1.

2.1givenF1F2step 1.1algebra

If the graph is an (n,d,α)-expander with α≤0.0068, its norm inequality and d>0 force α≥0; enlargement makes it an (n,d,b)-expander. By [F1] it is an (n,d,b,−b,b)-expander. The hypotheses of [F2] hold: d>0, −b>−1, 0<b<1/5, and the numerical expression is the one bounded in step 1.1. Thus the graph is globally synchronizing.

3.1givenF1F2step 1.1algebra∎

Let D=85730 and d≥D. Since d and D are positive integers and D≥2, (d−1)/d2≤(D−1)/D2: after multiplying by the positive denominators, the difference is (d−D)((D−1)d−D)≥0. Also b2D2−4(D−1)=854109194681/1562500000000>0. Consequently 2d−1/d<b. The Ramanujan definition therefore supplies an (n,d,b)-expander, and the same application of [F1] and [F2] as in step 2.1 gives global synchrony. At d=D, the separate inequality 25000000(D−1)>289D2 shows 2D−1/D>17/2500=0.0068, explaining why the degree conclusion uses the direct application.

Source notes

The comparison of the numerical and analytic bounds and the degree threshold are attributed to Expander graphs are globally synchronizing, Remark 1.5 and the opening of Section 5. The proof above is a local application of the stated suppliers; the article's 0.0816 proof is mentioned for context and is not a premise of this deduction.

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