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Friedman spectral expansion in the uniform simple model

Statement

Fix d≥3 and ε>0. For a uniformly sampled labelled simple d-regular graph on n vertices, P(max⁡{λ2(A),∣λn(A)∣}≥2d−1+ε)→0 as n→∞ along nd even. This includes all nonconstant eigenvalues with multiplicity. It gives a fixed-degree, asymptotic bound, not an exact Ramanujan conclusion.

Here d is an integer, ε is fixed before the limit, and n≥d+1. The eigenvalues of the adjacency matrix A are ordered d=λ1≥⋯≥λn with multiplicity. The finite graph space exists by Feasible labelled simple regular graph orders, and its relation to conditional pairings is the exact event identity in Simple-model spectral events as conditional pairing counts. The spectral maximum is ρ0(A)=∥A−(d/n)J∥op by Ordered eigenvalues and the centered regular norm. In particular extra eigenvalues d from disconnection and −d from a bipartite component are retained, as made explicit in Disconnected and bipartite spectral witnesses. The equivalent normalized threshold is 2d−1/d+ε/d by Exact normalized spectral threshold transfer, with all asymptotic quantifiers as in Asymptotic quantifiers and uniform parameter ranges.

External input

Bordenave, Section 1, Theorem 1 (PDF/printed p. 2), explicitly imports the outstanding probabilistic estimate for a uniform member of Gd(n) stated above. The preceding definition on that page specifies labelled simple graphs. Its ordered eigenvalues are denoted μi there; replacing that letter by λi changes no hypothesis or conclusion. The five local intermediate items establish feasibility, ordered deflation, obstruction witnesses, normalization, and exact event/model encoding before this import. They do not prove the probability bound.

Application is direct: the graph law is precisely the uniform simple law by Simple-model spectral events as conditional pairing counts, the spectral event is exactly the source's ordered event by Ordered eigenvalues and the centered regular norm, and the limits keep d and ε fixed by Asymptotic quantifiers and uniform parameter ranges. Thus Theorem 1 applies without an additional connectedness condition, a permutation-model identification, or any claimed local reconstruction of its proof. The assertion about exceptional eigenvalues follows from Disconnected and bipartite spectral witnesses, and the normalized version follows from Exact normalized spectral threshold transfer. The exact source contract and actual reading limits are recorded in the reference metadata.

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Used by · 1

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External dependencies

Charles Bordenave, A new proof of Friedman’s second eigenvalue Theorem and its extension to random lifts · arXiv:1502.04482v4 (5 March 2019), Section 1, simple ensemble definition and Theorem 1, PDF/printed p. 2; eigenvalue ordering on p. 1

For fixed integer $d\ge3$, $G$ uniform on the labelled simple graph set $\mathcal G_d(n)$, and every fixed $\varepsilon>0$, $\mathbb P(\max\{\lambda_2(A),|\lambda_n(A)|\}\ge2\sqrt{d-1}+\varepsilon)\to0$ along every sequence $n\to\infty$ with $nd$ even. The eigenvalues are decreasingly ordered with multiplicity, so only one copy of the top eigenvalue is excluded.

Hypotheses: Fixed integer degree d at least 3; fixed positive epsilon; n tends to infinity through orders with nd even and n at least d+1; uniform distribution on all labelled simple d-regular graphs with vertex set {1,...,n}. No conditioning on connectedness or nonbipartiteness.

Reading limits: Freshly read extracted PDF pp. 1–2, including the eigenvalue ordering, definition of G_d(n), and full Theorem 1; visually inspected PDF p. 2. Read extracted overview pp. 3–5 as context only. Did not reconstruct or audit the probabilistic proof in Sections 2.3–2.6, quantitative bound (2), or random-lift results. The five local helper arguments establish model and spectral interfaces, not Friedman’s probabilistic estimate.

Sources