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trel(G∗)≍thit(G)t_{\mathrm{rel}}(G^\ast)\asymp t_{\mathrm{hit}}(G)trel​(G∗)≍thit​(G) for lamplighter chains

Proved
MarkovMixing.lamplighter_relaxation

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

markov-chainsmixing-timesprobability

Let (Gn)(G_n)(Gn​) be any sequence of connected graphs with ∣Vn∣→∞|V_n|\to\infty∣Vn​∣→∞. Over each GnG_nGn​ two chains are compared. The base walk is the lazy simple random walk on GnG_nGn​ (hold with probability 12\tfrac1221​, else move to a uniform neighbour), with maximal hitting time thit(Gn)=max⁡x,yEx(τy)t_{\mathrm{hit}}(G_n)=\max_{x,y}\mathbb E_x(\tau_y)thit​(Gn​)=maxx,y​Ex​(τy​), the worst expected time to reach one vertex from another (Mission VI). The lamplighter chain Gn∗G_n^\astGn∗​ has states (lamp configuration in {0,1}Vn\{0,1\}^{V_n}{0,1}Vn​, lamplighter position); one step randomizes the lamp at the current position, moves the lamplighter one step of the base walk, and randomizes the lamp at the new position. Among the eigenvalues of a chain (real λ\lambdaλ with Pf=λfPf=\lambda fPf=λf, f≠0f\ne0f=0), λ⋆\lambda_\starλ⋆​ is the largest absolute value of an eigenvalue ≠1\ne1=1, and the relaxation time is trel=(1−λ⋆)−1t_{\mathrm{rel}}=(1-\lambda_\star)^{-1}trel​=(1−λ⋆​)−1 (Mission VII).

The theorem (Theorem 19.1 of Levin–Peres–Wilmer) asserts: there are constants c1,c2>0c_1,c_2>0c1​,c2​>0 such that for all sufficiently large nnn,

c1 thit(Gn)  ≤  trel(Gn∗)  ≤  c2 thit(Gn).c_1\,t_{\mathrm{hit}}(G_n)\;\le\;t_{\mathrm{rel}}(G_n^\ast)\;\le\;c_2\,t_{\mathrm{hit}}(G_n).c1​thit​(Gn​)≤trel​(Gn∗​)≤c2​thit​(Gn​).

The lamplighter's slowest mode is governed by the base walk's worst hitting time: to decorrelate, the lamplighter must revisit far-away lamps. The lower bound tests the variational characterization of the gap (Mission VII) with an eigenfunction built from an unvisited-vertex indicator; the upper bound is a coupling-contraction estimate. Together with the companion theorem (tmix≍tcovt_{\mathrm{mix}}\asymp t_{\mathrm{cov}}tmix​≍tcov​), the lamplighter ties the hitting, cover, relaxation, and mixing parameters of the whole series into one family.

Preamble
import Definitions.Def_mm_cutoff
Formal statement
namespace MarkovMixing

/-- **Theorem 19.1** (LPW): the relaxation time of the lamplighter chain is
comparable to the maximal hitting time of the underlying lazy walk: there
are constants `c₁, c₂ > 0` such that for all sufficiently large `n`,
`c₁ t_hit(G_n) ≤ t_rel(G_n⁎) ≤ c₂ t_hit(G_n)`. -/
theorem lamplighter_relaxation {Vf : ℕ → Type*} [∀ n, Fintype (Vf n)]
    [∀ n, DecidableEq (Vf n)] [∀ n, Nonempty (Vf n)]
    (G : ∀ n, SimpleGraph (Vf n)) [∀ n, DecidableRel (G n).Adj]
    (hconn : ∀ n, (G n).Connected)
    (hcard : Filter.Tendsto (fun n => Fintype.card (Vf n))
      Filter.atTop Filter.atTop) :
    ∃ c₁ c₂ : ℝ, 0 < c₁ ∧ 0 < c₂ ∧ ∃ N : ℕ, ∀ n : ℕ, N ≤ n →
      c₁ * hitTimeMax (lazy (graphWalk (G n))) ≤
        relaxationTime (lamplighter (G n)) ∧
      relaxationTime (lamplighter (G n)) ≤
        c₂ * hitTimeMax (lazy (graphWalk (G n))) := 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 19.2, Theorem 19.1, Eq. (19.2), p. 258
Read-back

What the Lean code literally says, in plain math · claude-fable-5

Read-back: lamplighter_relaxation

Fix, for every natural number nnn, a finite nonempty vertex type Vn\mathcal{V}_nVn​ (decidable equality) and a simple graph GnG_nGn​ on Vn\mathcal{V}_nVn​ (decidable adjacency), and assume: every GnG_nGn​ is connected, and ∣Vn∣→∞|\mathcal{V}_n| \to \infty∣Vn​∣→∞ as n→∞n \to \inftyn→∞ (no other link between the index nnn and the graph is assumed). Let Qn=12I+12WnQ_n = \tfrac12 I + \tfrac12 W_nQn​=21​I+21​Wn​ be the lazy simple random walk on GnG_nGn​, with Wn(x,y)=(deg⁡Gnx)−1W_n(x,y) = (\deg_{G_n} x)^{-1}Wn​(x,y)=(degGn​​x)−1 for x∼yx \sim yx∼y and 000 otherwise (0−1=00^{-1}=00−1=0 on isolated vertices). Define two quantities.

Maximal hitting time. thit(Qn)=sup⁡(x,y)∑t=0∞ax,y(t)t_{\mathrm{hit}}(Q_n) = \sup_{(x,y)} \sum_{t=0}^{\infty} a_{x,y}(t)thit​(Qn​)=sup(x,y)​∑t=0∞​ax,y​(t), the supremum over all ordered pairs (x,y)(x,y)(x,y) of vertices of the infinite sum over t∈Nt \in \mathbb{N}t∈N of ax,y(t)a_{x,y}(t)ax,y​(t), where ax,y(t)a_{x,y}(t)ax,y​(t) is the sum, over all trajectories ω=(ω0,…,ωt)\omega = (\omega_0,\dots,\omega_t)ω=(ω0​,…,ωt​) with ω0=x\omega_0 = xω0​=x and ωi≠y\omega_i \ne yωi​=y for every i≤ti \le ti≤t (including i=0i = 0i=0), of ∏i<tQn(ωi,ωi+1)\prod_{i<t} Q_n(\omega_i,\omega_{i+1})∏i<t​Qn​(ωi​,ωi+1​) — the probability that the walk started at xxx has avoided yyy through time ttt. Note that for the diagonal pairs x=yx = yx=y the condition fails at i=0i=0i=0, so those pairs contribute 000 to the supremum. The sum over ttt is Lean's tsum, equal to the junk value 000 if the family is not summable; the supremum is a real supremum over the finite nonempty set of pairs.

Relaxation time of the lamplighter chain. Let LnL_nLn​ be the lamplighter matrix on states (f,v)(f,v)(f,v), f:Vn→{off,on}f : \mathcal{V}_n \to \{\text{off},\text{on}\}f:Vn​→{off,on}, v∈Vnv \in \mathcal{V}_nv∈Vn​: transition probability from (f,v)(f,v)(f,v) to (g,u)(g,u)(g,u) equal to Qn(v,v)/2=1/4Q_n(v,v)/2 = 1/4Qn​(v,v)/2=1/4 if u=vu = vu=v and g=fg = fg=f off vvv (lamp at vvv unconstrained); Qn(v,u)/4Q_n(v,u)/4Qn​(v,u)/4 if u≠vu \ne vu=v and g=fg = fg=f off {v,u}\{v,u\}{v,u} (lamps at vvv and uuu unconstrained); 000 otherwise. Its relaxation time is

trel(Ln)  =  (1−λ⋆(Ln))−1,λ⋆(Ln)=sup⁡{∣λ∣:λ∈R, λ≠1, ∃f≠0, Lnf=λf},t_{\mathrm{rel}}(L_n) \;=\; \bigl(1 - \lambda^\star(L_n)\bigr)^{-1}, \qquad \lambda^\star(L_n) = \sup\bigl\{|\lambda| : \lambda \in \mathbb{R},\ \lambda \ne 1,\ \exists f \ne 0,\ L_n f = \lambda f\bigr\},trel​(Ln​)=(1−λ⋆(Ln​))−1,λ⋆(Ln​)=sup{∣λ∣:λ∈R, λ=1, ∃f=0, Ln​f=λf},

where the eigenvalue condition means there is a nonzero real vector fff on the lamplighter state space with the matrix acting on column vectors satisfying Lnf=λfL_n f = \lambda fLn​f=λf. Junk conventions: the real supremum of an empty set is 000; the inverse is total, so if λ⋆(Ln)=1\lambda^\star(L_n) = 1λ⋆(Ln​)=1 then trel(Ln)=0−1=0t_{\mathrm{rel}}(L_n) = 0^{-1} = 0trel​(Ln​)=0−1=0. Only real eigenvalues enter; λ=1\lambda = 1λ=1 is excluded but values >1> 1>1 or ≤−1\le -1≤−1, if any, are not.

Assertion. There exist reals c1>0c_1 > 0c1​>0 and c2>0c_2 > 0c2​>0 and a natural number NNN such that for all n≥Nn \ge Nn≥N,

c1⋅thit(Qn)  ≤  trel(Ln)andtrel(Ln)  ≤  c2⋅thit(Qn),c_1 \cdot t_{\mathrm{hit}}(Q_n) \;\le\; t_{\mathrm{rel}}(L_n) \quad\text{and}\quad t_{\mathrm{rel}}(L_n) \;\le\; c_2 \cdot t_{\mathrm{hit}}(Q_n),c1​⋅thit​(Qn​)≤trel​(Ln​)andtrel​(Ln​)≤c2​⋅thit​(Qn​),

both inequalities non-strict, with c1,c2,Nc_1, c_2, Nc1​,c2​,N uniform over n≥Nn \ge Nn≥N. Nothing is asserted or assumed about stochasticity of LnL_nLn​ or about any stationary distribution — the two sides are exactly the formulas above.

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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