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Polynomial relaxation time on trees (Kenyon--Mossel--Peres)

Proved
MarkovMixing.ising_tree_relaxation

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

markov-chainsmixing-timesprobability

Let Tb,kT_{b,k}Tb,k​ be the rooted bbb-ary tree of depth kkk (b≥2b\ge2b≥2, k≥1k\ge1k≥1): vertices are the words of length at most kkk over a bbb-letter alphabet, each word joined to its bbb one-letter extensions; write nkn_knk​ for its number of vertices. The Ising model on Tb,kT_{b,k}Tb,k​ at inverse temperature β>0\beta>0β>0 is the distribution π(σ)∝exp⁡(β∑{v,w}∈Eσ(v)σ(w))\pi(\sigma)\propto\exp\bigl(\beta\sum_{\{v,w\}\in E}\sigma(v)\sigma(w)\bigr)π(σ)∝exp(β∑{v,w}∈E​σ(v)σ(w)) on spin configurations, with Glauber dynamics re-sampling a uniformly chosen site from the conditional distribution. Among the eigenvalues of the dynamics (real λ\lambdaλ with Pf=λfPf=\lambda fPf=λf, f≠0f\ne0f=0), let λ⋆\lambda_\starλ⋆​ be the largest absolute value of an eigenvalue different from 111; the relaxation time is trel=(1−λ⋆)−1t_{\mathrm{rel}}=(1-\lambda_\star)^{-1}trel​=(1−λ⋆​)−1, as in Mission VII.

The theorem (Theorem 15.6, Kenyon–Mossel–Peres; Levin–Peres–Wilmer) asserts the polynomial bound

trel  ≤  nk  cT(β,b),cT(β,b)=2β(3b+1)log⁡b+1.t_{\mathrm{rel}}\;\le\;n_k^{\;c_T(\beta,b)},\qquad c_T(\beta,b)=\frac{2\beta(3b+1)}{\log b}+1.trel​≤nkcT​(β,b)​,cT​(β,b)=logb2β(3b+1)​+1.

On trees the relaxation time stays polynomial in the volume at every temperature — unlike the complete graph, where it becomes exponential below the critical temperature. The book's proof is an induction on depth powered by this mission's other tools: cutting the root's edges (the edge-removal proposition) splits the tree into independent subtrees whose product structure is handled by a block-dynamics comparison, at a per-level cost of e2β(3b+1)e^{2\beta(3b+1)}e2β(3b+1) — which telescopes to the stated exponent.

Preamble
import Definitions.Def_mm_ising
import Mathlib.Analysis.SpecialFunctions.Pow.Real
Formal statement
namespace MarkovMixing

/-- **Theorem 15.6** (Kenyon–Mossel–Peres; LPW): for the Glauber dynamics of
the Ising model on the rooted `b`-ary tree of depth `k`, with
`c_T(β,b) = 2β(3b+1)/log b + 1` and `n_k` the number of vertices,
`t_rel ≤ n_k^{c_T(β,b)}`. -/
theorem ising_tree_relaxation (b k : ℕ) (hb : 2 ≤ b) (hk : 1 ≤ k)
    (β : ℝ) (hβ : 0 < β) [inst : DecidableRel (aryTree b k).Adj] :
    relaxationTime (glauber (isingDist (aryTree b k) β)) ≤
      (Fintype.card (TreeVertex b k) : ℝ) ^
        (2 * β * (3 * (b : ℝ) + 1) / Real.log b + 1) := 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, Theorem 15.6, p. 207
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What the Lean code literally says, in plain math · claude-fable-5

Read-back: ising_tree_relaxation

Hypotheses. Naturals b,kb, kb,k with b≥2b \ge 2b≥2 and k≥1k \ge 1k≥1; a real β\betaβ with β>0\beta > 0β>0; and a (given, arbitrary) decidability instance for the adjacency of the tree graph below.

Objects. The vertex type Tb,k=TreeVertex(b,k)T_{b,k} = \mathrm{TreeVertex}(b,k)Tb,k​=TreeVertex(b,k) consists of all strings of length at most kkk over a bbb-letter alphabet (pairs of a level j∈{0,…,k}j \in \{0,\dots,k\}j∈{0,…,k} and a map {0,…,j−1}→{0,…,b−1}\{0,\dots,j-1\}\to\{0,\dots,b-1\}{0,…,j−1}→{0,…,b−1}); its cardinality is ∑j=0kbj\sum_{j=0}^k b^j∑j=0k​bj. The graph aryTree(b,k)\mathrm{aryTree}(b,k)aryTree(b,k) joins two such vertices exactly when one is at the next level below the other and extends its address by one arbitrary letter — the complete rooted bbb-ary tree of depth kkk, with edges between each node and its bbb children. μ\muμ is the Ising measure on spin configurations σ:Tb,k→{±1}\sigma : T_{b,k} \to \{\pm1\}σ:Tb,k​→{±1}, proportional to exp⁡(β∑{v,w}∈Esσ(v)sσ(w))\exp\big(\beta \sum_{\{v,w\} \in E} s_\sigma(v)s_\sigma(w)\big)exp(β∑{v,w}∈E​sσ​(v)sσ​(w)) (the code's ordered double sum with factor 12\tfrac1221​), and P=glauber(μ)P = \mathrm{glauber}(\mu)P=glauber(μ) is the heat-bath single-site chain on these configurations (uniform random vertex of the tree, resample its spin from the conditional of μ\muμ).

The relaxation time as defined in this development is

trel(P)  =  (1−λ⋆(P))−1,λ⋆(P)=sup⁡{ ∣λ∣  :  ∃f≠0, Pf=λf, λ≠1 },t_{\mathrm{rel}}(P) \;=\; \Big(1 - \lambda^\star(P)\Big)^{-1}, \qquad \lambda^\star(P) = \sup\big\{\,|\lambda| \;:\; \exists f \ne 0,\ P f = \lambda f,\ \lambda \ne 1 \,\big\},trel​(P)=(1−λ⋆(P))−1,λ⋆(P)=sup{∣λ∣:∃f=0, Pf=λf, λ=1},

the reciprocal of the absolute spectral gap, where the supremum is the real sSup over the absolute values of all real eigenvalues of PPP other than the exact value 111. Junk conventions in force: if that eigenvalue set is empty or unbounded, the sSup is 000 (making trel=1t_{\mathrm{rel}} = 1trel​=1); and if λ⋆(P)=1\lambda^\star(P) = 1λ⋆(P)=1 the reciprocal is 0−1=00^{-1} = 00−1=0 by Lean's convention, so trelt_{\mathrm{rel}}trel​ would then be 000 and the asserted bound trivially satisfied. If λ⋆(P)>1\lambda^\star(P) > 1λ⋆(P)>1 the relaxation time is negative.

The claim.

trel(glauber(μ))  ≤  ∣Tb,k∣ 2β (3b+1)log⁡b + 1,t_{\mathrm{rel}}\big(\mathrm{glauber}(\mu)\big) \;\le\; \big|T_{b,k}\big|^{\,\frac{2\beta\,(3b+1)}{\log b} \,+\, 1},trel​(glauber(μ))≤​Tb,k​​logb2β(3b+1)​+1,

i.e. the relaxation time is at most the number of tree vertices (not configurations), cast to a real, raised to the real power 2β(3b+1)log⁡b+1\dfrac{2\beta(3b+1)}{\log b} + 1logb2β(3b+1)​+1 (real exponentiation with a real exponent; log⁡\loglog is the natural logarithm, and log⁡b>0\log b > 0logb>0 since b≥2b \ge 2b≥2). This is a single non-strict inequality — a polynomial-in-∣Tb,k∣|T_{b,k}|∣Tb,k​∣ upper bound whose exponent depends on β\betaβ and bbb but not on kkk. Nothing is asserted for b≤1b \le 1b≤1, k=0k = 0k=0, or β≤0\beta \le 0β≤0.

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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