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Part 2· Theorem F

Theorem F — Spectral Stability

Prerequisites: Theorem A (energy isolation), Chapter 8.

Theorem F. Let δW:=maxi,jWt(i,j)Wt(i,j)\|\delta W\|_\infty:=\max_{i,j}|W'_t(i,j)-W_t(i,j)|.

(i) ϕt(F)ϕt(F)C1δWV2/volt(F)|\phi'_t(F)-\phi_t(F)|\le C_1\|\delta W\|_\infty|V|^2/\mathrm{vol}_t(F), where C1=2(1+θ)4C_1=2(1+\theta)\le 4.

(ii) If ϕt(F)θϵ\phi_t(F)\le\theta-\epsilon with ϵ>0\epsilon>0, then FFtF\in\mathfrak{F}'_t provided δW<ϵvolt(F)/(C1V2)\|\delta W\|_\infty<\epsilon\cdot\mathrm{vol}_t(F)/(C_1|V|^2).

Proof. (Complete; reproduced from Chapter 8.)

(i) Write ϕ=cut/vol\phi=\mathrm{cut}/\mathrm{vol} (under (F1), denominator is vol(F)\mathrm{vol}(F)).

Numerator perturbation: ΔcutFFˉδWV2δW|\Delta_{\mathrm{cut}}|\le|F|\cdot|\bar F|\cdot\|\delta W\|_\infty\le|V|^2\|\delta W\|_\infty.

Denominator perturbation: ΔvolFVδWV2δW|\Delta_{\mathrm{vol}}|\le|F|\cdot|V|\cdot\|\delta W\|_\infty\le|V|^2\|\delta W\|_\infty.

ϕϕ=cut+Δcvol+Δvcutvol=ΔcvolcutΔv(vol+Δv)vol.|\phi'-\phi|=\left|\frac{\mathrm{cut}+\Delta_c}{\mathrm{vol}+\Delta_v}-\frac{\mathrm{cut}}{\mathrm{vol}}\right|=\left|\frac{\Delta_c\cdot\mathrm{vol}-\mathrm{cut}\cdot\Delta_v}{(\mathrm{vol}+\Delta_v)\cdot\mathrm{vol}}\right|.

Numerator: ΔcvolcutΔvδWV2(vol+cut)δWV2(1+θ)vol|\Delta_c\cdot\mathrm{vol}-\mathrm{cut}\cdot\Delta_v|\le\|\delta W\|_\infty|V|^2(\mathrm{vol}+\mathrm{cut})\le\|\delta W\|_\infty|V|^2(1+\theta)\mathrm{vol}.

Denominator: (vol+Δv)volvol2/2(\mathrm{vol}+\Delta_v)\cdot\mathrm{vol}\ge\mathrm{vol}^2/2 for Δvvol/2|\Delta_v|\le\mathrm{vol}/2.

Result: ϕϕ2(1+θ)δWV2/vol=C1δWV2/vol|\phi'-\phi|\le 2(1+\theta)\|\delta W\|_\infty|V|^2/\mathrm{vol}=C_1\|\delta W\|_\infty|V|^2/\mathrm{vol}.

(ii) Set δ0=ϵ/(C1V2/volt(F))\delta_0=\epsilon/(C_1|V|^2/\mathrm{vol}_t(F)). Then ϕϕ<ϵ|\phi'-\phi|<\epsilon, so ϕt(F)<θ\phi'_t(F)<\theta. Volume condition preserved similarly. \square

Explicit constant. C1=2(1+θ)C_1=2(1+\theta). For θ=0.1\theta=0.1, C1=2.2C_1=2.2. The perturbation size requirement is δW<ϵvol(F)2.2V2\|\delta W\|_\infty<\frac{\epsilon\,\mathrm{vol}(F)}{2.2\,|V|^2}, or equivalently δWV2vol(F)<ϵ2.2\|\delta W\|_\infty\cdot\frac{|V|^2}{\mathrm{vol}(F)}<\frac{\epsilon}{2.2}.