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Theorem 5.2 and Corollary 5.3 -- the coupling bound

Proved
MarkovMixing.coupling_bound

by Shuze Chen · Aug 21, 2026 · Mathlib c5ea003 (Lean v4.30.0)

markov-chainsmixing-timesprobability

Let PPP be a Markov chain on a finite state space VVV with stationary distribution π\piπ, and write Pt(x,⋅)P^t(x,\cdot)Pt(x,⋅) for the distribution at time ttt started at xxx, ∥μ−ν∥TV=max⁡A⊆V∣μ(A)−ν(A)∣\|\mu-\nu\|_{TV}=\max_{A\subseteq V}|\mu(A)-\nu(A)|∥μ−ν∥TV​=maxA⊆V​∣μ(A)−ν(A)∣ for the total variation distance, and d(t)=max⁡x∥Pt(x,⋅)−π∥TVd(t)=\max_x\|P^t(x,\cdot)-\pi\|_{TV}d(t)=maxx​∥Pt(x,⋅)−π∥TV​ for the worst-case distance to stationarity. A Markovian coupling of PPP is a Markov chain on ordered pairs of states each of whose two coordinates, viewed on its own, moves according to PPP, and which keeps the two coordinates together once they coincide. For such a coupling started at the pair (x,y)(x,y)(x,y), the coupling time τcouple\tau_{\mathrm{couple}}τcouple​ is the first time the pair chain reaches the diagonal {(v,v)}\{(v,v)\}{(v,v)} — the moment the two copies meet.

Suppose a Markovian coupling Qx,yQ_{x,y}Qx,y​ of PPP is given for every pair of starting states. The theorem (Theorem 5.2 and Corollary 5.3 of Levin–Peres–Wilmer) asserts:

  1. for every pair x,yx,yx,y and time ttt, the rows of PtP^tPt are close whenever the coupling has probably met: ∥Pt(x,⋅)−Pt(y,⋅)∥TV≤Px,y{τcouple>t}\bigl\|P^t(x,\cdot)-P^t(y,\cdot)\bigr\|_{TV}\le\mathbb P_{x,y}\{\tau_{\mathrm{couple}}>t\}​Pt(x,⋅)−Pt(y,⋅)​TV​≤Px,y​{τcouple​>t};
  2. consequently d(t)≤max⁡x,yPx,y{τcouple>t}d(t)\le\max_{x,y}\mathbb P_{x,y}\{\tau_{\mathrm{couple}}>t\}d(t)≤maxx,y​Px,y​{τcouple​>t}.

This is the engine of the coupling method: to bound mixing, build a coupling that meets fast.

Preamble
import Definitions.Def_mm_coupling
Formal statement
namespace MarkovMixing

/-- **Theorem 5.2 and Corollary 5.3** (LPW): if each pair of starting states
carries a Markovian coupling of the chain (staying together after meeting),
then `‖P^t(x,·) − P^t(y,·)‖_TV ≤ P_{x,y}{τ_couple > t}`, and hence
`d(t) ≤ max_{x,y} P_{x,y}{τ_couple > t}`, where `τ_couple` is the hitting
time of the diagonal for the pair chain. -/
theorem coupling_bound {V : Type*} [Fintype V] [DecidableEq V] [Nonempty V]
    (P : Matrix V V ℝ) (hP : IsStochastic P)
    (π : V → ℝ) (hπ : IsStationary P π)
    (Q : V → V → Matrix (V × V) (V × V) ℝ)
    (hQ : ∀ x y : V, IsMarkovianCoupling P (Q x y)) (t : ℕ) :
    (∀ x y : V, tvDist (rowDist P t x) (rowDist P t y) ≤
      setAvoidTailProb (Q x y) (x, y) (pairDiagonal V) t) ∧
    distStationary P π t ≤
      ⨆ p : V × V, setAvoidTailProb (Q p.1 p.2) p (pairDiagonal V) t := 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 5.2, Theorem 5.2 and Corollary 5.3, pp. 64-65
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What the Lean code literally says, in plain math · claude-fable-5

Let VVV be a finite, nonempty type with decidable equality, and let PPP be a real V×VV \times VV×V matrix assumed stochastic, meaning every entry satisfies P(x,y)≥0P(x,y) \ge 0P(x,y)≥0 and every row sums to 111: ∑yP(x,y)=1\sum_y P(x,y) = 1∑y​P(x,y)=1. Let π:V→R\pi : V \to \mathbb{R}π:V→R be assumed stationary for PPP, meaning π\piπ is a probability vector (π(x)≥0\pi(x) \ge 0π(x)≥0 for all xxx and ∑xπ(x)=1\sum_x \pi(x) = 1∑x​π(x)=1) and πP=π\pi P = \piπP=π (row-vector–matrix product). Let QQQ assign to every ordered pair (x,y)∈V×V(x,y) \in V \times V(x,y)∈V×V a real matrix Qx,yQ_{x,y}Qx,y​ indexed by (V×V)×(V×V)(V \times V) \times (V \times V)(V×V)×(V×V), and assume that for every x,yx, yx,y the matrix Qx,yQ_{x,y}Qx,y​ is a Markovian coupling of PPP, which here means all four of: (i) Qx,yQ_{x,y}Qx,y​ is stochastic (nonnegative entries, rows summing to 111); (ii) for every current pair p=(p1,p2)p = (p_1, p_2)p=(p1​,p2​) and every x′∈Vx' \in Vx′∈V, ∑y′Qx,y(p,(x′,y′))=P(p1,x′)\sum_{y'} Q_{x,y}\big(p, (x',y')\big) = P(p_1, x')∑y′​Qx,y​(p,(x′,y′))=P(p1​,x′) (first marginal moves by PPP from the first coordinate of the current pair); (iii) symmetrically, ∑x′Qx,y(p,(x′,y′))=P(p2,y′)\sum_{x'} Q_{x,y}\big(p, (x',y')\big) = P(p_2, y')∑x′​Qx,y​(p,(x′,y′))=P(p2​,y′); (iv) from any diagonal pair (z,z)(z,z)(z,z), the probability of moving to any off-diagonal pair is 000 (once coupled, the coupling never assigns positive weight off the diagonal in one step). Note that the starting pair (x,y)(x,y)(x,y) appears only as the index selecting which coupling matrix is used; conditions (i)–(iv) constrain each Qx,yQ_{x,y}Qx,y​ at all pairs ppp, not just at (x,y)(x,y)(x,y). Fix also an arbitrary time t∈{0,1,2,… }t \in \{0, 1, 2, \dots\}t∈{0,1,2,…}. Write DDD for the diagonal {(z,z):z∈V}⊆V×V\{(z,z) : z \in V\} \subseteq V \times V{(z,z):z∈V}⊆V×V, and for a stochastic-type matrix RRR on pairs, a starting pair ppp, and horizon ttt, define the diagonal-avoidance mass

AR(p,t)  =  ∑ω∏i=0t−1R(ωi,ωi+1),A_R(p, t) \;=\; \sum_{\omega} \prod_{i=0}^{t-1} R(\omega_i, \omega_{i+1}),AR​(p,t)=ω∑​i=0∏t−1​R(ωi​,ωi+1​),

the sum running over all sequences ω:{0,…,t}→V×V\omega : \{0,\dots,t\} \to V \times Vω:{0,…,t}→V×V with ω0=p\omega_0 = pω0​=p and ωi∉D\omega_i \notin Dωi​∈/D for every index i=0,…,ti = 0, \dots, ti=0,…,t — including i=0i = 0i=0, so if ppp itself lies on the diagonal (i.e. x=yx = yx=y) this quantity is 000, and at t=0t = 0t=0 it is exactly the indicator that ppp is off the diagonal (the empty product being 111). Write dTV(μ,ν)=sup⁡A⊆V∣∑z∈Aμ(z)−∑z∈Aν(z)∣\mathrm{d_{TV}}(\mu, \nu) = \sup_{A \subseteq V} \big| \sum_{z \in A} \mu(z) - \sum_{z \in A} \nu(z) \big|dTV​(μ,ν)=supA⊆V​​∑z∈A​μ(z)−∑z∈A​ν(z)​ (supremum of the absolute discrepancy over all finite subsets AAA of VVV, applied here to arbitrary real-valued vectors), and let Pt(x,⋅)P^t(x, \cdot)Pt(x,⋅) denote row xxx of the ttt-th matrix power of PPP. The theorem then asserts the conjunction of two claims: (1) for every pair of states x,y∈Vx, y \in Vx,y∈V,

dTV(Pt(x,⋅), Pt(y,⋅))  ≤  AQx,y((x,y), t),\mathrm{d_{TV}}\big(P^t(x,\cdot),\, P^t(y,\cdot)\big) \;\le\; A_{Q_{x,y}}\big((x,y),\, t\big),dTV​(Pt(x,⋅),Pt(y,⋅))≤AQx,y​​((x,y),t),

i.e. the total-variation distance between the time-ttt distributions started from xxx and from yyy is at most the mass, under the coupling chain Qx,yQ_{x,y}Qx,y​ started at (x,y)(x,y)(x,y), of length-ttt trajectories that stay off the diagonal at every time from 000 through ttt; and (2)

sup⁡x∈VdTV(Pt(x,⋅), π)  ≤  sup⁡(p1,p2)∈V×VAQp1,p2((p1,p2), t),\sup_{x \in V} \mathrm{d_{TV}}\big(P^t(x,\cdot),\, \pi\big) \;\le\; \sup_{(p_1,p_2) \in V \times V} A_{Q_{p_1,p_2}}\big((p_1,p_2),\, t\big),x∈Vsup​dTV​(Pt(x,⋅),π)≤(p1​,p2​)∈V×Vsup​AQp1​,p2​​​((p1​,p2​),t),

i.e. the worst-case (over starting states) total-variation distance to π\piπ at time ttt is at most the worst diagonal-avoidance mass over all starting pairs (p1,p2)(p_1, p_2)(p1​,p2​) — the supremum on the right ranging over all pairs, including diagonal ones (for which the avoidance mass is 000). The stationarity hypothesis on π\piπ is used only in claim (2), where π\piπ appears; no irreducibility or aperiodicity of PPP is assumed, and the claims hold for the single fixed ttt quantified in the statement (which is universally quantified, so effectively for all t≥0t \ge 0t≥0, including t=0t = 0t=0).

Human review
  • Endorsed by Community (Bot) · Aug 21, 2026

  • Endorsed by Shuze Chen · Aug 21, 2026

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

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