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ℓPart 2· Theorem F

Theorem F — Spectral Stability

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

Theorem F. Let ∥δW∥∞:=max⁡i,j∣Wt′(i,j)−Wt(i,j)∣\|\delta W\|_\infty:=\max_{i,j}|W'_t(i,j)-W_t(i,j)|.

(i) ∣ϕt′(F)−ϕt(F)∣≤C1∥δW∥∞∣V∣2/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)≤θ−ϵ\phi_t(F)\le\theta-\epsilon with ϵ>0\epsilon>0, then F∈Ft′F\in\mathfrak{F}'_t provided ∥δW∥∞<ϵ⋅volt(F)/(C1∣V∣2)\|\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: ∣Δcut∣≤∣F∣⋅∣Fˉ∣⋅∥δW∥∞≤∣V∣2∥δW∥∞|\Delta_{\mathrm{cut}}|\le|F|\cdot|\bar F|\cdot\|\delta W\|_\infty\le|V|^2\|\delta W\|_\infty.

Denominator perturbation: ∣Δvol∣≤∣F∣⋅∣V∣⋅∥δW∥∞≤∣V∣2∥δW∥∞|\Delta_{\mathrm{vol}}|\le|F|\cdot|V|\cdot\|\delta W\|_\infty\le|V|^2\|\delta W\|_\infty.

∣ϕ′−ϕ∣=∣cut+Δcvol+Δv−cutvol∣=∣Δc⋅vol−cut⋅Δv(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: ∣Δc⋅vol−cut⋅Δv∣≤∥δW∥∞∣V∣2(vol+cut)≤∥δW∥∞∣V∣2(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)⋅vol≥vol2/2(\mathrm{vol}+\Delta_v)\cdot\mathrm{vol}\ge\mathrm{vol}^2/2 for ∣Δv∣≤vol/2|\Delta_v|\le\mathrm{vol}/2.

Result: ∣ϕ′−ϕ∣≤2(1+θ)∥δW∥∞∣V∣2/vol=C1∥δW∥∞∣V∣2/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/(C1∣V∣2/volt(F))\delta_0=\epsilon/(C_1|V|^2/\mathrm{vol}_t(F)). Then ∣ϕ′−ϕ∣<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∥∞<ϵ vol(F)2.2 ∣V∣2\|\delta W\|_\infty<\frac{\epsilon\,\mathrm{vol}(F)}{2.2\,|V|^2}, or equivalently ∥δW∥∞⋅∣V∣2vol(F)<ϵ2.2\|\delta W\|_\infty\cdot\frac{|V|^2}{\mathrm{vol}(F)}<\frac{\epsilon}{2.2}.