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Edge removal perturbs the spectral gap by at most e2β(Δ+2r)e^{2\beta(\Delta+2r)}e2β(Δ+2r)

Proved
MarkovMixing.ising_edge_removal

by Shuze Chen · Aug 22, 2026 · Mathlib c5ea003 (Lean v4.30.0)

markov-chainsmixing-timesprobability

Let GGG be a graph with maximum degree Δ\DeltaΔ on a finite vertex set, and let G′⊆GG'\subseteq GG′⊆G be a subgraph obtained by deleting rrr edges (all vertices kept). For a graph HHH, the Ising model at inverse temperature β>0\beta>0β>0 is the distribution πH(σ)∝exp⁡(β∑{v,w}∈E(H)σ(v)σ(w))\pi_H(\sigma)\propto\exp\bigl(\beta\sum_{\{v,w\}\in E(H)}\sigma(v)\sigma(w)\bigr)πH​(σ)∝exp(β∑{v,w}∈E(H)​σ(v)σ(w)) on spin configurations σ:V→{±1}\sigma:V\to\{\pm1\}σ:V→{±1}, and its Glauber dynamics re-samples a uniformly chosen site from the conditional distribution. The spectral gap of a chain is γ=1−λ2\gamma=1-\lambda_2γ=1−λ2​, where λ2\lambda_2λ2​ is the largest eigenvalue different from 111 (an eigenvalue being a real λ\lambdaλ with Pf=λfPf=\lambda fPf=λf for some nonzero fff, as in Mission VII).

The theorem (Proposition 15.7 of Levin–Peres–Wilmer) asserts that deleting the rrr edges changes the spectral gap by at most an explicit exponential factor:

γG′  ≤  e 2β(Δ+2r)  γG,\gamma_{G'}\;\le\;e^{\,2\beta(\Delta+2r)}\;\gamma_{G},γG′​≤e2β(Δ+2r)γG​,

where γH\gamma_HγH​ denotes the gap of the Glauber dynamics for the Ising model on HHH.

The proof is a direct comparison of Dirichlet forms (Mission VII): removing rrr edges changes every Gibbs weight by at most e2βre^{2\beta r}e2βr and every transition probability by at most e2βΔe^{2\beta\Delta}e2βΔ. In the book this is the key surgery step for the tree bound: cutting the root's edges splits the tree into independent subtrees, at a bounded cost in the gap.

Preamble
import Definitions.Def_mm_ising
Formal statement
namespace MarkovMixing

/-- **Proposition 15.7** (LPW): removing `r` edges from a graph of maximal
degree `Δ` changes the spectral gap of the Ising Glauber dynamics by at most
a factor `e^{2β(Δ + 2r)}`:  `γ̃ ≤ e^{2β(Δ+2r)} γ` is equivalent to the
stated `1/γ ≤ e^{2β(Δ+2r)}/γ̃`. -/
theorem ising_edge_removal {Vv : Type*} [Fintype Vv] [DecidableEq Vv]
    [Nonempty Vv] (G G' : SimpleGraph Vv) [DecidableRel G.Adj]
    [DecidableRel G'.Adj] (hsub : G' ≤ G) (β : ℝ) (hβ : 0 < β) :
    spectralGap (glauber (isingDist G' β)) ≤
      Real.exp (2 * β * ((G.maxDegree : ℝ) +
        2 * ((G.edgeFinset \ G'.edgeFinset).card : ℝ))) *
      spectralGap (glauber (isingDist G β)) := by
  sorry

end MarkovMixing
Source
D. A. Levin, Y. Peres, E. L. Wilmer, Markov Chains and Mixing Times, AMS 2009, https://documents.epfl.ch/groups/i/ip/ipg/www/2013-2014/Random_Walks/markovmixing.pdf, Section 15.4, Proposition 15.7, p. 207
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What the Lean code literally says, in plain math · claude-fable-5

Read-back: ising_edge_removal

Setting. Let VVV be a finite, nonempty type with decidable equality, and let G,G′G, G'G,G′ be two simple graphs on VVV (each with decidable adjacency) satisfying G′≤GG' \le GG′≤G, i.e. every edge of G′G'G′ is an edge of GGG. Let β\betaβ be a real with β>0\beta > 0β>0.

Unfolding the custom notions: for a graph HHH, μH\mu_HμH​ denotes the Ising measure on configurations σ:V→{±1}\sigma : V \to \{\pm1\}σ:V→{±1}, μH(σ)=wH(σ)/∑τwH(τ)\mu_H(\sigma) = w_H(\sigma)/\sum_\tau w_H(\tau)μH​(σ)=wH​(σ)/∑τ​wH​(τ) with wH(σ)=exp⁡(β∑{v,w}∈E(H)sσ(v)sσ(w))w_H(\sigma) = \exp\big(\beta \sum_{\{v,w\} \in E(H)} s_\sigma(v)s_\sigma(w)\big)wH​(σ)=exp(β∑{v,w}∈E(H)​sσ​(v)sσ​(w)) (the code's ordered double sum with a factor 12\tfrac1221​). glauber(μH)\mathrm{glauber}(\mu_H)glauber(μH​) is the single-site heat-bath chain: from σ\sigmaσ, pick a uniform vertex vvv (probability 1/∣V∣1/|V|1/∣V∣ each) and resample the spin at vvv from μH\mu_HμH​ conditioned on the other spins. For any matrix PPP on configurations, the spectral gap as defined here is

γ(P)  =  1−sup⁡{λ∈R  :  ∃f≠0, Pf=λf, λ≠1},\gamma(P) \;=\; 1 - \sup\{\lambda \in \mathbb{R} \;:\; \exists f \ne 0,\ P f = \lambda f,\ \lambda \ne 1\},γ(P)=1−sup{λ∈R:∃f=0, Pf=λf, λ=1},

where the supremum is the real sSup, which takes the junk value 000 if the set of such eigenvalues is empty or unbounded above — in that case γ(P)=1\gamma(P) = 1γ(P)=1. Note this λ2\lambda_2λ2​ is the supremum of all real eigenvalues other than exactly 111 (negative eigenvalues and eigenvalues >1> 1>1 included; only the value 111 itself is excluded), with no reversibility or symmetry assumed in the definition.

The claim. Under these hypotheses,

γ(glauber(μG′))  ≤  exp⁡ ⁣(2β(ΔG+2 ∣E(G)∖E(G′)∣))⋅γ(glauber(μG)),\gamma\big(\mathrm{glauber}(\mu_{G'})\big) \;\le\; \exp\!\Big( 2\beta\big(\Delta_G + 2\,|E(G)\setminus E(G')|\big)\Big)\cdot \gamma\big(\mathrm{glauber}(\mu_{G})\big),γ(glauber(μG′​))≤exp(2β(ΔG​+2∣E(G)∖E(G′)∣))⋅γ(glauber(μG​)),

where ΔG\Delta_GΔG​ is the maximum degree of the larger graph GGG (a natural number cast to R\mathbb{R}R) and ∣E(G)∖E(G′)∣|E(G)\setminus E(G')|∣E(G)∖E(G′)∣ is the number of edges of GGG that are not edges of G′G'G′ (cardinality of the edge-finset difference, cast to R\mathbb{R}R).

Direction of the inequality: it is the gap of the chain on the subgraph G′G'G′ that is bounded above by e2β(ΔG+2∣E(G)∖E(G′)∣)e^{2\beta(\Delta_G + 2|E(G)\setminus E(G')|)}e2β(ΔG​+2∣E(G)∖E(G′)∣) times the gap of the chain on GGG. The exponential factor uses ΔG\Delta_GΔG​ (not ΔG′\Delta_{G'}ΔG′​) and counts each removed edge with weight 222. No hypothesis is placed on connectivity, on the number of removed edges, or on the sign of either spectral gap (the sSup-based gaps could a priori be negative or take the junk value described above); G′=GG' = GG′=G is allowed, in which case the factor is e2βΔG≥1e^{2\beta\Delta_G} \ge 1e2βΔG​≥1.

Human review
  • Endorsed by Community (Bot) · Aug 22, 2026

  • Endorsed by Shuze Chen · Aug 22, 2026

    Confirmed by the mission captain (proposal self-audit).

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