Prerequisites : Theorem A (energy isolation), Chapter 8.
Theorem F. Let ∥ δ W ∥ ∞ : = max i , j ∣ W t ′ ( i , j ) − W t ( i , j ) ∣ \|\delta W\|_\infty:=\max_{i,j}|W'_t(i,j)-W_t(i,j)| ∥ δ W ∥ ∞ := max i , j ∣ W t ′ ( i , j ) − W t ( i , j ) ∣ .
(i) ∣ ϕ t ′ ( F ) − ϕ t ( F ) ∣ ≤ C 1 ∥ δ W ∥ ∞ ∣ V ∣ 2 / v o l t ( F ) |\phi'_t(F)-\phi_t(F)|\le C_1\|\delta W\|_\infty|V|^2/\mathrm{vol}_t(F) ∣ ϕ t ′ ( F ) − ϕ t ( F ) ∣ ≤ C 1 ∥ δ W ∥ ∞ ∣ V ∣ 2 / vol t ( F ) , where C 1 = 2 ( 1 + θ ) ≤ 4 C_1=2(1+\theta)\le 4 C 1 = 2 ( 1 + θ ) ≤ 4 .
(ii) If ϕ t ( F ) ≤ θ − ϵ \phi_t(F)\le\theta-\epsilon ϕ t ( F ) ≤ θ − ϵ with ϵ > 0 \epsilon>0 ϵ > 0 , then F ∈ F t ′ F\in\mathfrak{F}'_t F ∈ F t ′ provided ∥ δ W ∥ ∞ < ϵ ⋅ v o l t ( F ) / ( C 1 ∣ V ∣ 2 ) \|\delta W\|_\infty<\epsilon\cdot\mathrm{vol}_t(F)/(C_1|V|^2) ∥ δ W ∥ ∞ < ϵ ⋅ vol t ( F ) / ( C 1 ∣ V ∣ 2 ) .
Proof. (Complete; reproduced from Chapter 8.)
(i) Write ϕ = c u t / v o l \phi=\mathrm{cut}/\mathrm{vol} ϕ = cut / vol (under (F1), denominator is v o l ( F ) \mathrm{vol}(F) vol ( F ) ).
Numerator perturbation: ∣ Δ c u t ∣ ≤ ∣ F ∣ ⋅ ∣ F ˉ ∣ ⋅ ∥ δ W ∥ ∞ ≤ ∣ V ∣ 2 ∥ δ W ∥ ∞ |\Delta_{\mathrm{cut}}|\le|F|\cdot|\bar F|\cdot\|\delta W\|_\infty\le|V|^2\|\delta W\|_\infty ∣ Δ cut ∣ ≤ ∣ F ∣ ⋅ ∣ F ˉ ∣ ⋅ ∥ δ W ∥ ∞ ≤ ∣ V ∣ 2 ∥ δ W ∥ ∞ .
Denominator perturbation: ∣ Δ v o l ∣ ≤ ∣ F ∣ ⋅ ∣ V ∣ ⋅ ∥ δ W ∥ ∞ ≤ ∣ V ∣ 2 ∥ δ W ∥ ∞ |\Delta_{\mathrm{vol}}|\le|F|\cdot|V|\cdot\|\delta W\|_\infty\le|V|^2\|\delta W\|_\infty ∣ Δ vol ∣ ≤ ∣ F ∣ ⋅ ∣ V ∣ ⋅ ∥ δ W ∥ ∞ ≤ ∣ V ∣ 2 ∥ δ W ∥ ∞ .
∣ ϕ ′ − ϕ ∣ = ∣ c u t + Δ c v o l + Δ v − c u t v o l ∣ = ∣ Δ c ⋅ v o l − c u t ⋅ Δ v ( v o l + Δ v ) ⋅ v o l ∣ . |\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|. ∣ ϕ ′ − ϕ ∣ = vol + Δ v cut + Δ c − vol cut = ( vol + Δ v ) ⋅ vol Δ c ⋅ vol − cut ⋅ Δ v .
Numerator: ∣ Δ c ⋅ v o l − c u t ⋅ Δ v ∣ ≤ ∥ δ W ∥ ∞ ∣ V ∣ 2 ( v o l + c u t ) ≤ ∥ δ W ∥ ∞ ∣ V ∣ 2 ( 1 + θ ) v o l |\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} ∣ Δ c ⋅ vol − cut ⋅ Δ v ∣ ≤ ∥ δ W ∥ ∞ ∣ V ∣ 2 ( vol + cut ) ≤ ∥ δ W ∥ ∞ ∣ V ∣ 2 ( 1 + θ ) vol .
Denominator: ( v o l + Δ v ) ⋅ v o l ≥ v o l 2 / 2 (\mathrm{vol}+\Delta_v)\cdot\mathrm{vol}\ge\mathrm{vol}^2/2 ( vol + Δ v ) ⋅ vol ≥ vol 2 /2 for ∣ Δ v ∣ ≤ v o l / 2 |\Delta_v|\le\mathrm{vol}/2 ∣ Δ v ∣ ≤ vol /2 .
Result: ∣ ϕ ′ − ϕ ∣ ≤ 2 ( 1 + θ ) ∥ δ W ∥ ∞ ∣ V ∣ 2 / v o l = C 1 ∥ δ W ∥ ∞ ∣ V ∣ 2 / v o l |\phi'-\phi|\le 2(1+\theta)\|\delta W\|_\infty|V|^2/\mathrm{vol}=C_1\|\delta W\|_\infty|V|^2/\mathrm{vol} ∣ ϕ ′ − ϕ ∣ ≤ 2 ( 1 + θ ) ∥ δ W ∥ ∞ ∣ V ∣ 2 / vol = C 1 ∥ δ W ∥ ∞ ∣ V ∣ 2 / vol .
(ii) Set δ 0 = ϵ / ( C 1 ∣ V ∣ 2 / v o l t ( F ) ) \delta_0=\epsilon/(C_1|V|^2/\mathrm{vol}_t(F)) δ 0 = ϵ / ( C 1 ∣ V ∣ 2 / vol t ( F )) . Then ∣ ϕ ′ − ϕ ∣ < ϵ |\phi'-\phi|<\epsilon ∣ ϕ ′ − ϕ ∣ < ϵ , so ϕ t ′ ( F ) < θ \phi'_t(F)<\theta ϕ t ′ ( F ) < θ . Volume condition preserved similarly. □ \square □
Explicit constant. C 1 = 2 ( 1 + θ ) C_1=2(1+\theta) C 1 = 2 ( 1 + θ ) . For θ = 0.1 \theta=0.1 θ = 0.1 , C 1 = 2.2 C_1=2.2 C 1 = 2.2 . The perturbation size requirement is ∥ δ W ∥ ∞ < ϵ v o l ( F ) 2.2 ∣ V ∣ 2 \|\delta W\|_\infty<\frac{\epsilon\,\mathrm{vol}(F)}{2.2\,|V|^2} ∥ δ W ∥ ∞ < 2.2 ∣ V ∣ 2 ϵ vol ( F ) , or equivalently ∥ δ W ∥ ∞ ⋅ ∣ V ∣ 2 v o l ( F ) < ϵ 2.2 \|\delta W\|_\infty\cdot\frac{|V|^2}{\mathrm{vol}(F)}<\frac{\epsilon}{2.2} ∥ δ W ∥ ∞ ⋅ vol ( F ) ∣ V ∣ 2 < 2.2 ϵ .