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Critical PSD kernel phases: quantitative tail growth

Statement

Let d>0, a>0, −1<c−≤0≤c+, w=c+−c−>0, s=1+c−, B=1+c++a. Suppose ∥A−(d/n)J∥≤ad and c−dI⪯L−dI+(d/n)J⪯c+dI. For normalized phases satisfying the preceding kernel inequality set Ct={x:∣θx∣≥t} and m0=∣Cπ/2∣>0. For 0<γ<β≤π/2, 0<ϵ<s, and u>0:

(a) if sin⁡(β−γ)≥2(1+u)a/(s−ϵ), then ∣Cγ∣≥min⁡{(1+ϵ/w)∣Cβ∣,uan,n/2};

(b) if sin⁡(β−γ)≥2Bm0/((s−ϵ)∣Cβ∣), then ∣Cγ∣≥min⁡{(1+ϵ/w)∣Cβ∣,n/2}.

Facts & Assumptions

[F1]

Use the graph, phase, algebraic and analytic interfaces of Regular critical PSD phases: kernel and half-circle, Two-sided spectral expander — Definition 1.9, Angular order and elementary inverse-trigonometric bounds. Every configuration assumed here is a critical point with positive-semidefinite Hessian; local minimality is never inferred from that condition.

[F2]

Sine is strictly increasing on [−π/2,π/2] and has range [−1,1] (Signs, monotonicity intervals, and ranges of sine and cosine).

[F3]

Sine is odd: sin⁡(−t)=−sin⁡t for every real t, and consequently sin⁡0=0 (Parity and the Pythagorean identity for sine and cosine).

Proof

Given: The hypotheses of the Statement.

Goal: Establish its conclusions directly for critical PSD phases.

1.1F1algebra

For sets define e(U,W)=∑x∈U,y∈WAxy and p(U)=e(U,Uc). Testing the centered-adjacency bound on 1U gives e(U,U)≤(d/n)∣U∣2+ad∣U∣. Testing the centered-Laplacian inequalities on 1U−(∣U∣/n)1 gives (1+c−)d∣U∣∣Uc∣/n≤p(U)≤(1+c+)d∣U∣∣Uc∣/n. Therefore e(U,V)=e(U,U)+p(U)≤Bd∣U∣, since c+≥0. These tests include loops under the stated degree convention.

1.2F1algebra

Suppose ∅≠X⊆Y, ∣Y∣<n/2, and ∣Y∣<(1+ϵ/w)∣X∣. Put x=∣X∣, y=∣Y∣, Z=Y∖X, z=∣Z∣<ϵx/w. The identity 2e(X,Yc)=p(X)+p(Y)−p(Z) and the two cut bounds give e(X,Yc)≥(1+c−)dx(n−y)/n−wdz(n−z)/(2n)>(s−ϵ)dx(n−y)/n. Indeed, z(n−z)<(ϵx/w)n<2(ϵx/w)(n−y). This inequality is strict also at z=0, because ϵx(n−y)>0.

1.3F1F2F3algebra

Sum the kernel inequality over y∈X=Cβ, and split x into X, Y∖X, Yc with Y=Cγ. On these regions the kernel is at most 1, 0, and −sin⁡(β−γ) respectively: for x∈Y∖X the sine argument lies in [−π/2,0], and for x∈Yc it lies in [−π/2,−(β−γ)]; monotonicity, oddness and the sine range give these bounds. Thus e(X,X)≥sin⁡(β−γ)e(X,Yc). A second bound is obtained from K(u,v)+K(v,u)≤1∣u∣≥π/2+1∣v∣≥π/2. If both absolute phases are below π/2 the sum is zero by oddness; if just one is above, the sum is at most 1 because the other kernel term is nonpositive; if both are above each term is at most 1. Symmetrizing the internal sum gives e(Cπ/2,X)≥sin⁡(β−γ)e(X,Yc).

2.1F1algebra∎

To prove (a), suppose the conclusion fails. Then y<n/2, y<(1+ϵ/w)x and y<uan, hence x<uan. Steps 1.1–1.2 yield e(X,X)≤(1+u)adx and e(X,Yc)>(s−ϵ)dx/2. The sine hypothesis and step 1.3 now give e(X,X)>(1+u)adx, a contradiction. To prove (b), failure gives the first two strict size inequalities. Steps 1.1–1.3 give Bdm0≥e(Cπ/2,X)≥sin⁡(β−γ)e(X,Yc)>Bdm0, also impossible. This proves both estimates.

Depends on

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