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Algorithmic Game TheoryOperations ResearchOptimization·Captain: mikedeng1

A Supply Chain Theory of Factoring and Reverse Factoring 1: The Supplier's Equilibrium Choice Among Recourse, Non-Recourse and Reverse FactoringResearch Paper

Motivation

Small and medium-sized suppliers that sell to large retailers typically ship first and are paid weeks or months later. Until the invoice is paid, the supplier's cash is trapped in accounts receivable, while production has to be financed up front. Factoring (selling or pledging the receivable to a financial intermediary for immediate cash) and reverse factoring (a buyer-initiated program in which the retailer approves the invoice and the supplier is paid early by the retailer's bank) are the standard remedies, and reverse factoring programs of large buyers are often coupled with an extension of payment terms. Which of these instruments a supplier should use, and how the answer depends on the credit ratings of the two firms, is the question addressed by Kouvelis and Xu, "A Supply Chain Theory of Factoring and Reverse Factoring", Management Science 67(10):6071–6088, 2021 (doi:10.1287/mnsc.2020.3788). The paper embeds each financing scheme in the pull wholesale-price game of Cachon (2004) and compares the resulting equilibria.

Setting

A retailer (the Stackelberg leader) offers a wholesale price www to a capital-constrained supplier (the follower), who then chooses a production quantity q≥0q \ge 0q≥0 and carries the inventory; the retail price ppp is fixed, and 0<c<p0 < c < p0<c<p is the unit production cost. Demand D≥0D \ge 0D≥0 has density fff, complementary distribution function Fˉ\bar FFˉ, finite mean, f>0f > 0f>0 on [0,Z][0, \mathbb Z][0,Z] (Z≤+∞\mathbb Z \le +\inftyZ≤+∞), and a strictly increasing failure rate z=f/Fˉz = f/\bar Fz=f/Fˉ (strict IFR). Expected sales are S(q)=∫0qFˉ(ξ) dξS(q) = \int_0^q \bar F(\xi)\,d\xiS(q)=∫0q​Fˉ(ξ)dξ, and k(q)=S(q)/Fˉ(q)k(q) = S(q)/\bar F(q)k(q)=S(q)/Fˉ(q).

Each firm j∈{s,r}j \in \{s, r\}j∈{s,r} has a credit rating Cj∈(Cmin⁡,Cmax⁡)C_j \in (C_{\min}, C_{\max})Cj​∈(Cmin​,Cmax​). The default probability ρj=ρ(Cj)∈[0,1]\rho_j = \rho(C_j) \in [0,1]ρj​=ρ(Cj​)∈[0,1] is strictly decreasing in the rating, and the interest-rate premium ηj=η(Cj)>0\eta_j = \eta(C_j) > 0ηj​=η(Cj​)>0 is decreasing. Production takes a lead time t1t_1t1​, payment follows after a term t2t_2t2​, and the supplier faces a Poisson liquidity shock of rate λs\lambda_sλs​ during production (the retailer, rate λr\lambda_rλr​). Under a scheme i∈{F,N,R}i \in \{\mathcal F, \mathcal N, \mathcal R\}i∈{F,N,R} (recourse, non-recourse, reverse factoring, the last with a payment extension τ≥0\tau \ge 0τ≥0), the supplier's expected profit is

πi(q;w)=(1−ρs)(Λie−λst1wS(q)−cqeηst1),\pi_i(q; w) = (1-\rho_s)\big(\Lambda_i e^{-\lambda_s t_1} w S(q) - c q e^{\eta_s t_1}\big),πi​(q;w)=(1−ρs​)(Λi​e−λs​t1​wS(q)−cqeηs​t1​),

with coefficients ΛF=(1−ρr)+(1−ρs)−eηst2\Lambda_{\mathcal F} = (1-\rho_r) + (1-\rho_s) - e^{\eta_s t_2}ΛF​=(1−ρr​)+(1−ρs​)−eηs​t2​, ΛN=e−ηrt2(1−ρr)\Lambda_{\mathcal N} = e^{-\eta_r t_2}(1-\rho_r)ΛN​=e−ηr​t2​(1−ρr​), ΛR=e−ηr(t2+τ)\Lambda_{\mathcal R} = e^{-\eta_r(t_2+\tau)}ΛR​=e−ηr​(t2​+τ), and effective unit cost ci=c e(ηs+λs)t1/Λic_i = c\,e^{(\eta_s+\lambda_s)t_1}/\Lambda_ici​=ce(ηs​+λs​)t1​/Λi​. The retailer's profit is e−λst1(1−ρr)(p−w)S(q)e^{-\lambda_s t_1}(1-\rho_r)(p-w)S(q)e−λs​t1​(1−ρr​)(p−w)S(q) under factoring and carries the extra factor 2−e−λrτ2 - e^{-\lambda_r \tau}2−e−λr​τ under reverse factoring.

Formalization targets

Goal: Proposition 5

For a given τ≥0\tau \ge 0τ≥0, let C3\mathbb C_3C3​ be the unique supplier rating with ΛF=ΛR\Lambda_{\mathcal F} = \Lambda_{\mathcal R}ΛF​=ΛR​, C1\mathbb C_1C1​ the one with ΛF=ΛN\Lambda_{\mathcal F} = \Lambda_{\mathcal N}ΛF​=ΛN​, and CF,CN,CR\mathbb C_{\mathcal F}, \mathbb C_{\mathcal N}, \mathbb C_{\mathcal R}CF​,CN​,CR​ the feasibility thresholds (ci=pc_i = pci​=p). With all three schemes available,

e−ηrτ<1−ρr:F adopted  ⟺  Cs>CF∨C1,N adopted  ⟺  CN<Cs≤C1;e^{-\eta_r\tau} < 1-\rho_r:\quad \mathcal F \text{ adopted} \iff C_s > \mathbb C_{\mathcal F}\vee\mathbb C_1,\qquad \mathcal N \text{ adopted} \iff \mathbb C_{\mathcal N} < C_s \le \mathbb C_1;e−ηr​τ<1−ρr​:F adopted⟺Cs​>CF​∨C1​,N adopted⟺CN​<Cs​≤C1​; 1−ρr≤e−ηrτ:F adopted  ⟺  Cs>CF∨C3,R adopted  ⟺  CR<Cs≤C3.1-\rho_r \le e^{-\eta_r\tau}:\quad \mathcal F \text{ adopted} \iff C_s > \mathbb C_{\mathcal F}\vee\mathbb C_3,\qquad \mathcal R \text{ adopted} \iff \mathbb C_{\mathcal R} < C_s \le \mathbb C_3.1−ρr​≤e−ηr​τ:F adopted⟺Cs​>CF​∨C3​,R adopted⟺CR​<Cs​≤C3​.

Milestones

  1. Proposition 2 (p. 6078): recourse factoring is feasible iff Cs>CFC_s > \mathbb C_{\mathcal F}Cs​>CF​, and then the unique equilibrium solves pFˉ(q)=cF[1+z(q)k(q)]p\bar F(q) = c_{\mathcal F}[1+z(q)k(q)]pFˉ(q)=cF​[1+z(q)k(q)], w=cF/Fˉ(q)w = c_{\mathcal F}/\bar F(q)w=cF​/Fˉ(q).
  2. Proposition 3 (p. 6079): the same for non-recourse factoring with cNc_{\mathcal N}cN​.
  3. §5.2 (p. 6082, Proposition EC.2): the same for reverse factoring with cR(τ)c_{\mathcal R}(\tau)cR​(τ).
  4. §4.4 (p. 6080, Lemma EC.2): between feasible schemes, the supplier's equilibrium profits are ordered as the Λi\Lambda_iΛi​.
  5. Proposition 4 (p. 6080): the choice between F\mathcal FF and N\mathcal NN alone.

A follow-on item states Corollary 1(i) (p. 6081): when the retailer's rating is at least the supplier's, non-recourse factoring strictly dominates recourse factoring whenever the latter is feasible.

Significance

Proposition 5 is the paper's main prediction: non-recourse factoring is the choice of medium-rated suppliers, recourse factoring of highly rated ones, and reverse factoring with a fixed payment extension is chosen only by low-to-medium-rated suppliers and only if the retailer's rating is not too high relative to the extension. The paper uses it to explain the documented reluctance of suppliers to join reverse-factoring programs that come with extended payment terms (Wuttke, Rosenzweig and Heese 2019; Corsten 2010, a teaching case), and it is the starting point of the paper's Proposition 6 on the retailer's optimal payment extension, which is the subject of the second mission of this series.

The results are proved in the paper's Online Appendix B. To the best of available knowledge none of them, and no model of supply chain finance, has a machine-checked proof. A formal development would also supply a reusable treatment of the pull wholesale-price game under a strictly IFR demand with an arbitrary effective unit cost, of which Propositions 2, 3 and EC.2 are three instances.

Difficulty

The case analysis of Proposition 5 is short once the milestones are available; the substance lies in them. Proposition 2 requires solving a bilevel problem: the follower's best response has to be identified for every wholesale price, including prices at which the supplier produces nothing, and the leader's objective has to be shown to have a single maximizer. The natural route through the first-order condition needs the IFR property to exclude multiple stationary points, and it has to cope with a support end Z\mathbb ZZ that may be finite (where Fˉ\bar FFˉ vanishes and kkk, zzz lose meaning) or infinite. Lemma EC.2 requires the equilibrium supplier profit as an explicit function of the effective cost and a monotonicity argument for it; comparing the Λi\Lambda_iΛi​ directly, without the equilibrium, does not prove it. The proofs themselves are not in the main text.

Formalization scope

Demand is a probability measure μ on ℝ with a density f, the support end Z : EReal, and the complementary distribution function Fbar μ x = μ((x, ∞)). The model data, the coefficients coef, the effective costs cF, cN, cR, the two profit functions, best responses, equilibria, feasibility and adoption are definitions; all theorems are for arbitrary data satisfying Params.Valid and DemandModel. Readings fixed by the formalization:

  • "Feasible": some wholesale price w≥0w \ge 0w≥0 with a supplier best response gives the retailer strictly positive profit. It is not defined as ci<pc_i < pci​<p, which is what Propositions 2 and 3 prove.
  • "Adopted" / "should be adopted": the scheme is feasible and its equilibrium supplier profit is best among the feasible available schemes, with ties resolved R≻N≻F\mathcal R \succ \mathcal N \succ \mathcal FR≻N≻F, the order forced by the paper's boundaries (Cs=C1C_s = \mathbb C_1Cs​=C1​, Cs=C3C_s = \mathbb C_3Cs​=C3​, Cr=C2C_r = \mathbb C_2Cr​=C2​). Profits are compared, not the Λi\Lambda_iΛi​.
  • "The unique value of CsC_sCs​ that satisfies …": a point of (Cmin⁡,Cmax⁡)(C_{\min}, C_{\max})(Cmin​,Cmax​) satisfying the equation and the only such point. The equation cF=pc_{\mathcal F} = pcF​=p is cross-multiplied, c e(ηs+λs)t1=pΛFc\,e^{(\eta_s+\lambda_s)t_1} = p\Lambda_{\mathcal F}ce(ηs​+λs​)t1​=pΛF​, since ΛF\Lambda_{\mathcal F}ΛF​ may be ≤0\le 0≤0.
  • "Cr>C2C_r > \mathbb C_2Cr​>C2​" is read through the paper's equivalence τ>−ηr−1ln⁡(1−ρr)\tau > -\eta_r^{-1}\ln(1-\rho_r)τ>−ηr−1​ln(1−ρr​), i.e. e−ηrτ<1−ρre^{-\eta_r\tau} < 1-\rho_re−ηr​τ<1−ρr​: the stated assumptions give no single crossing in CrC_rCr​.
  • "The unique equilibrium can be derived from …": the equilibrium exists and is unique, and it is exactly the solution of the system with q∈(0,Z)q \in (0, \mathbb Z)q∈(0,Z); this part is stated under feasibility.
  • "Increasing/decreasing" is weak unless stated (p. 6075); ρ\rhoρ is strictly decreasing, η\etaη weakly.
  • Continuity of fff is read on [0,Z][0,\mathbb Z][0,Z], and Z\mathbb ZZ as the upper end of the support.
  • Additions: wholesale prices are nonnegative; the retailer's reverse-factoring profit is the last line of the p. 6082 display (the middle line has a stray factor www).
  • Corollary 1(i): "higher credit rating" is read as Cr≥CsC_r \ge C_sCr​≥Cs​, "dominates" as a strictly larger equilibrium supplier profit whenever recourse is feasible.

A formalization in which feasibility or adoption is defined by the inequalities being proved (ci<pc_i < pci​<p, largest Λi\Lambda_iΛi​) makes the propositions trivial and is ruled out by the definitions above. The profit functions (7), (10) and the p. 6082 display are taken as the model; the derivation from bank and factor pricing (Eqs. (1), (5), (6), Lemma 1) is not formalized, and the unstated assumptions of Table EC.2 are not included. Contributions of reusable lemmas on SSS, kkk and zzz under strict IFR are welcome.

Selected references

  • P. Kouvelis and F. Xu, A Supply Chain Theory of Factoring and Reverse Factoring, Management Science 67(10):6071–6088, 2021. https://doi.org/10.1287/mnsc.2020.3788
  • G. P. Cachon, The Allocation of Inventory Risk in a Supply Chain: Push, Pull, and Advance-Purchase Discount Contracts, Management Science 50(2):222–238, 2004. https://doi.org/10.1287/mnsc.1030.0189
  • D. A. Wuttke, E. Rosenzweig, H. S. Heese, An Empirical Analysis of Supply Chain Finance Adoption, Journal of Operations Management 65(3):242–261, 2019.
  • P. Kouvelis and W. Zhao, Who Should Finance the Supply Chain? Impact of Credit Ratings on Supply Chain Decisions, Manufacturing & Service Operations Management 20(1):19–35, 2018.
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Dynamical SystemsNumber Theory·Captain: mysticflounder

Tao 2022: Almost All Collatz Orbits Attain Almost Bounded ValuesResearch Paper

Motivation

The Collatz map sends an even positive integer nnn to n/2n/2n/2 and an odd one to 3n+13n+13n+1. The Collatz conjecture asserts that every orbit of this map eventually reaches 111. It remains an open problem.

Because the conjecture is open, a large part of the literature proves weaker statements that hold for almost all starting values. These results bound how small an orbit gets, not whether it reaches 111. They are the strongest unconditional evidence for the conjecture. Terence Tao's 2022 theorem is the strongest result of this type: outside a set of logarithmic density zero, every orbit drops below any prescribed function that tends to infinity, however slowly (Tao 2022).

Timeline

Attributions follow the survey in Tao 2022, Section 1. Here Colmin⁡(N)\mathrm{Col}_{\min}(N)Colmin​(N) is the least value in the orbit of NNN.

  • 1976 to 1979, Terras and Everett. Colmin⁡(N)<N\mathrm{Col}_{\min}(N) < NColmin​(N)<N for almost all NNN, in natural density.
  • 1979, Allouche. Colmin⁡(N)<Nθ\mathrm{Col}_{\min}(N) < N^{\theta}Colmin​(N)<Nθ for almost all NNN, for every θ>0.869\theta > 0.869θ>0.869.
  • 1994, Korec. The same bound for every θ>log⁡3/log⁡4≈0.7924\theta > \log 3/\log 4 \approx 0.7924θ>log3/log4≈0.7924.
  • 2019 preprint, 2022 publication, Tao. The power NθN^{\theta}Nθ is replaced by any f(N)→∞f(N) \to \inftyf(N)→∞, in logarithmic density instead of natural density (Forum of Mathematics, Pi 10, e12).
  • 2026, ProofAtlas. A complete machine-checked proof of Tao's theorem in Lean 4 is published (formalization record).

Setting

Let collatzStep:N→N\mathrm{collatzStep} : \mathbb{N} \to \mathbb{N}collatzStep:N→N be

collatzStep(n)={n/2n even,3n+1n odd.\mathrm{collatzStep}(n) = \begin{cases} n/2 & n \text{ even},\\ 3n+1 & n \text{ odd}. \end{cases}collatzStep(n)={n/23n+1​n even,n odd.​

Write collatzStep[k]\mathrm{collatzStep}^{[k]}collatzStep[k] for the kkk-fold iterate, with collatzStep[0](n)=n\mathrm{collatzStep}^{[0]}(n) = ncollatzStep[0](n)=n. The orbit of nnn is the set of values collatzStep[k](n)\mathrm{collatzStep}^{[k]}(n)collatzStep[k](n) for k≥0k \ge 0k≥0. It includes nnn itself.

The Syracuse map acts on odd integers. It sends an odd nnn to the odd part of 3n+13n+13n+1, which is syracuseStep(n)=(3n+1)/2ν2(3n+1)\mathrm{syracuseStep}(n) = (3n+1)/2^{\nu_2(3n+1)}syracuseStep(n)=(3n+1)/2ν2​(3n+1). The Syracuse orbit minimum syracuseOrbitMin(n)\mathrm{syracuseOrbitMin}(n)syracuseOrbitMin(n) is the least value syracuseStep[k](n)\mathrm{syracuseStep}^{[k]}(n)syracuseStep[k](n) over k≥0k \ge 0k≥0.

For a set AAA of positive integers and a real cutoff x≥2x \ge 2x≥2, the logarithmic mass of AAA up to xxx is

weightedLogMassReal(x)=1log⁡x∑1≤n≤xn∈A1n.\mathrm{weightedLogMassReal}(x) = \frac{1}{\log x} \sum_{\substack{1 \le n \le x \\ n \in A}} \frac{1}{n}.weightedLogMassReal(x)=logx1​1≤n≤xn∈A​∑​n1​.

A set of positive integers has logarithmic density ddd when this quantity tends to ddd as x→∞x \to \inftyx→∞. Since ∑n≤x1/n=log⁡x+O(1)\sum_{n \le x} 1/n = \log x + O(1)∑n≤x​1/n=logx+O(1), all positive integers together have logarithmic density 111, and the odd positive integers have logarithmic density 1/21/21/2.

A function f:N→Rf : \mathbb{N} \to \mathbb{R}f:N→R tends to infinity on positive inputs when for every real MMM there is an NNN such that f(n)>Mf(n) > Mf(n)>M for all n≥Nn \ge Nn≥N with n>0n > 0n>0.

Formalization targets

Goal: Tao's Theorem 1.3

For every fff that tends to infinity on positive inputs,

lim⁡x→∞1log⁡x∑1≤n≤x∃k, collatzStep[k](n)<f(n)1n=1.\lim_{x \to \infty} \frac{1}{\log x} \sum_{\substack{1 \le n \le x \\ \exists k,\ \mathrm{collatzStep}^{[k]}(n) < f(n)}} \frac{1}{n} = 1.x→∞lim​logx1​1≤n≤x∃k, collatzStep[k](n)<f(n)​∑​n1​=1.

This is the Lean theorem collatz_almost_bounded_logarithmic. It fixes no rate and no constant, so later improvements do not invalidate it.

Syracuse form: Tao's Theorem 1.6

For every fff that tends to infinity on odd positive inputs, the odd nnn whose Syracuse orbit contains a value below f(n)f(n)f(n) have logarithmic density 1/21/21/2, which is all of the odd integers. This is syracuse_almost_bounded_logarithmic.

Quantitative form: Tao's Theorem 3.1

There are constants C,c>0C, c > 0C,c>0 such that for all real M≥2M \ge 2M≥2 and x≥2x \ge 2x≥2,

1log⁡x∑1≤n≤x, n oddsyracuseOrbitMin(n)>M1n≤C(log⁡M)c.\frac{1}{\log x} \sum_{\substack{1 \le n \le x,\ n \text{ odd} \\ \mathrm{syracuseOrbitMin}(n) > M}} \frac{1}{n} \le \frac{C}{(\log M)^{c}}.logx1​1≤n≤x, n oddsyracuseOrbitMin(n)>M​∑​n1​≤(logM)cC​.

This is syracuse_uniform_logarithmic_tail_bound. The three targets are listed from weakest to strongest. In Tao's paper, the goal and Theorem 1.6 both follow from Theorem 3.1.

Significance

The result. Theorem 1.3 improves the earlier almost-all bounds on Collatz orbit minima from a power of NNN to any function that tends to infinity. For example, Colmin⁡(N)<log⁡log⁡log⁡log⁡N\mathrm{Col}_{\min}(N) < \log\log\log\log NColmin​(N)<loglogloglogN for almost all NNN. The theorem does not settle the conjecture. A single divergent orbit or nontrivial cycle is not excluded, because its predecessors form a set with bounded orbit minima.

The formalization. The theorem is proved, and a complete formalization already exists. The ProofAtlas record Tao's Almost-Bounded Collatz Orbits proves the statement taoAlmostBoundedColMin_checked with the same step map and an orbit that includes its starting value. That package has 397 first-party Lean files and about 124,000 source lines. ProofAtlas records a passing build with no sorry and the axiom profile propext, Classical.choice, Quot.sound. The source is released under the Apache-2.0 licence at commit d53c8de00056fb05999e44589f2399d7efa026e4, with copyright held by Advameg, Inc. It was built with Lean v4.30.0-rc2.

The remaining work for this mission is therefore a port, not new mathematics. The existing Lean development must be moved to Lean v4.33.1 and Mathlib 0df444a, and then connected to the goal statement above.

Difficulty

The mathematical difficulty is already resolved in the existing proof. The classical first-descent argument shows that a typical orbit drops below its starting value. Repeating that argument fails, because after one descent the new value is no longer distributed like a random integer of its size, and the error compounds at each repetition. That is why earlier results stop at a power bound NθN^{\theta}Nθ.

The difficulty of this mission is engineering. The port moves a development of about 124,000 lines forward across three minor Lean releases and the corresponding Mathlib changes. Lemma renames, deprecations, and changes in tactic behaviour must be repaired file by file without changing any statement.

Formalization scope

  • Step map. collatzStep n = if Even n then n / 2 else 3 * n + 1, so collatzStep(0)=0\mathrm{collatzStep}(0) = 0collatzStep(0)=0. This is the same definition as in the ProofAtlas source.
  • Orbit. The witness kkk ranges over all natural numbers, including k=0k = 0k=0.
  • Density. The goal uses weightedLogMassReal: a real cutoff xxx, the natural indices 0≤n≤⌊x⌋0 \le n \le \lfloor x \rfloor0≤n≤⌊x⌋, weights 1/n1/n1/n, and normalization by log⁡x\log xlogx. The ProofAtlas statement instead uses integer cutoffs and normalization by the harmonic sum ∑n≤N1/n\sum_{n \le N} 1/n∑n≤N​1/n. A short bridge between the two normalizations is part of the required work.
  • Threshold. The hypothesis on fff constrains only positive inputs. The value f(0)f(0)f(0) is irrelevant.
  • Non-triviality. The case k=0k = 0k=0 alone covers only inputs with n<f(n)n < f(n)n<f(n). For slowly growing fff this set is finite, so the goal is not satisfied by the starting value.

The goal is already reduced, through accepted proofs, to the single open statement syracuse_uniform_logarithmic_tail_bound. Two routes therefore close the mission. The first is to port the ProofAtlas development and prove the goal directly through the density bridge. The second is to prove Theorem 3.1 in its stated form. Contributions welcome include ported modules as reusable solutions, the density bridge, and a proof of Theorem 3.1. Every ported file must keep the Apache-2.0 notice and attribution to the ProofAtlas source.

Selected references

  • Terence Tao, Almost all orbits of the Collatz map attain almost bounded values, Forum of Mathematics, Pi 10 (2022), e12. https://doi.org/10.1017/fmp.2022.8 and https://arxiv.org/abs/1909.03562
  • ProofAtlas, Tao's Almost-Bounded Collatz Orbits, Lean 4 formalization, source commit d53c8de00056fb05999e44589f2399d7efa026e4, Apache-2.0, 2026. https://proofatlas.ai/formalizations/tao-almost-bounded-orbits/
  • Jeffrey C. Lagarias (editor), The Ultimate Challenge: The 3x+1 Problem, American Mathematical Society, 2010. https://bookstore.ams.org/MBK/78
7 thms1 active userReviewed
Control TheoryDynamical SystemsOperations Research+1·Captain: mikedeng1

Stabilization of Hybrid Systems by Feedback Control Based on Discrete-Time State Observations I: Almost Sure Asymptotic StabilityResearch Paper

Motivation

Many engineered systems switch between a finite number of operating modes at random times: a power grid after a line failure, a networked controller whose links drop, a manufacturing plant whose machines break down and are repaired. A standard model for such systems is a hybrid stochastic differential equation, also called an SDE with Markovian switching: the state follows an Itô equation whose coefficients depend on a mode that evolves as a continuous-time Markov chain. The monograph of Mao and Yuan (Stochastic Differential Equations with Markovian Switching, 2006) develops the stability theory of these equations.

A controller that stabilizes such a system usually needs the current state. In practice the state is sampled: it is observed at times 0,τ,2τ,…0,\tau,2\tau,\dots0,τ,2τ,… and the control is held between observations. Mao (Automatica 49, 2013) showed that, under a global Lipschitz condition on the drift and diffusion, a feedback control based on discrete-time observations stabilizes a hybrid SDE in the sense of mean-square exponential stability when τ\tauτ is small enough. You, Liu, Lu, Mao and Qiu (SIAM J. Control Optim. 53(2), 2015) replaced that condition by local Lipschitz continuity plus linear growth, gave an explicit bound (3.5) on the admissible observation interval τ\tauτ, and proved H∞H_\inftyH∞​-stability, mean-square asymptotic stability, almost sure asymptotic stability and exponential stability of the controlled system. This mission formalizes the almost sure asymptotic stability result, Theorem 3.4, and the results it is built on.

Setting

Let (Ω,F,{Ft}t≥0,P)(\Omega,\mathcal F,\{\mathcal F_t\}_{t\ge0},\mathbb P)(Ω,F,{Ft​}t≥0​,P) be a probability space with a filtration satisfying the usual conditions (increasing, right-continuous, F0\mathcal F_0F0​ contains the null sets). On it live an mmm-dimensional {Ft}\{\mathcal F_t\}{Ft​}-Brownian motion www and a right-continuous {Ft}\{\mathcal F_t\}{Ft​}-Markov chain rrr on S={1,…,N}S=\{1,\dots,N\}S={1,…,N} with generator Γ=(γij)\Gamma=(\gamma_{ij})Γ=(γij​) (γij≥0\gamma_{ij}\ge0γij​≥0 for i≠ji\ne ji=j, zero row sums), independent of www. Fix τ>0\tau>0τ>0 and the sampling time δt=[t/τ]τ\delta_t=[t/\tau]\tauδt​=[t/τ]τ, the last observation time up to ttt. The controlled system is

dx(t)=(f(x(t),r(t),t)+u(x(δt),r(t),t))dt+g(x(t),r(t),t) dw(t),x(0)=x0, r(0)=r0,(2.1)dx(t)=\big(f(x(t),r(t),t)+u(x(\delta_t),r(t),t)\big)dt+g(x(t),r(t),t)\,dw(t),\qquad x(0)=x_0,\ r(0)=r_0,\tag{2.1}dx(t)=(f(x(t),r(t),t)+u(x(δt​),r(t),t))dt+g(x(t),r(t),t)dw(t),x(0)=x0​, r(0)=r0​,(2.1)

with f,u:Rn×S×R+→Rnf,u:\mathbb R^n\times S\times\mathbb R_+\to\mathbb R^nf,u:Rn×S×R+​→Rn and g:Rn×S×R+→Rn×mg:\mathbb R^n\times S\times\mathbb R_+\to\mathbb R^{n\times m}g:Rn×S×R+​→Rn×m. The feedback uuu sees the state only at the observation times.

The hypotheses are:

  • Assumption 2.1: f,gf,gf,g locally Lipschitz in xxx, and ∣f(x,i,t)∣≤K1∣x∣|f(x,i,t)|\le K_1|x|∣f(x,i,t)∣≤K1​∣x∣, ∣g(x,i,t)∣≤K2∣x∣|g(x,i,t)|\le K_2|x|∣g(x,i,t)∣≤K2​∣x∣ (∣g∣|g|∣g∣ the trace norm).
  • Assumption 2.2: ∣u(x,i,t)−u(y,i,t)∣≤K3∣x−y∣|u(x,i,t)-u(y,i,t)|\le K_3|x-y|∣u(x,i,t)−u(y,i,t)∣≤K3​∣x−y∣ and u(0,i,t)=0u(0,i,t)=0u(0,i,t)=0.
  • Assumption 3.1: there are U∈C2,1(Rn×S×R+;R+)U\in C^{2,1}(\mathbb R^n\times S\times\mathbb R_+;\mathbb R_+)U∈C2,1(Rn×S×R+​;R+​) and λ1,λ2>0\lambda_1,\lambda_2>0λ1​,λ2​>0 with LU(x,i,t)+λ1∣Ux(x,i,t)∣2≤−λ2∣x∣2\mathcal LU(x,i,t)+\lambda_1|U_x(x,i,t)|^2\le-\lambda_2|x|^2LU(x,i,t)+λ1​∣Ux​(x,i,t)∣2≤−λ2​∣x∣2, where
LU=Ut+Ux[f+u]+12trace⁡[gTUxxg]+∑jγijU(x,j,t).\mathcal LU=U_t+U_x[f+u]+\tfrac12\operatorname{trace}[g^TU_{xx}g]+\sum_j\gamma_{ij}U(x,j,t).LU=Ut​+Ux​[f+u]+21​trace[gTUxx​g]+j∑​γij​U(x,j,t).
  • Condition (3.5): λ2>τK32λ1[2τ(K12+2K32)+K22]\lambda_2>\frac{\tau K_3^2}{\lambda_1}\big[2\tau(K_1^2+2K_3^2)+K_2^2\big]λ2​>λ1​τK32​​[2τ(K12​+2K32​)+K22​] and τ≤14K3\tau\le\frac1{4K_3}τ≤4K3​1​.

In Lean these are Assumption21, Assumption22, C21, LU, Assumption31, Condition35, in the namespace You2015.Asymp; the basis is HybridSetup, the Itô integral IsItoIntegral, the sampling time delta, and solutions SolvesSampledHybridSDE, in the namespace You2015.Shared shared with the companion mission.

Formalization targets

Goal: Theorem 3.4 (almost sure asymptotic stability)

Under the hypotheses above, every solution of (2.1) satisfies

lim⁡t→∞x(t)=0a.s.\lim_{t\to\infty}x(t)=0\quad\text{a.s.}t→∞lim​x(t)=0a.s.

for all x0∈Rnx_0\in\mathbb R^nx0​∈Rn and r0∈Sr_0\in Sr0​∈S. No rate is claimed; the statement is the qualitative convergence of almost every path.

Milestones, in the order the proof uses them

  1. (3.15) E∣x(t)−x(δt)∣2≤2E∫δtt[τ∣f+u(x(δs),⋅)∣2+∣g∣2]ds\mathbb E|x(t)-x(\delta_t)|^2\le2\mathbb E\int_{\delta_t}^t[\tau|f+u(x(\delta_s),\cdot)|^2+|g|^2]dsE∣x(t)−x(δt​)∣2≤2E∫δt​t​[τ∣f+u(x(δs​),⋅)∣2+∣g∣2]ds.
  2. Theorem 3.2 (H∞H_\inftyH∞​-stability): ∫0∞E∣x(s)∣2ds<∞\int_0^\infty\mathbb E|x(s)|^2ds<\infty∫0∞​E∣x(s)∣2ds<∞.
  3. (3.21) E∣x(s)−x(δs)∣2≤3(τK12+K22)1−6τ2K32∫δssE∣x(z)∣2dz+6τ2K321−6τ2K32E∣x(s)∣2\mathbb E|x(s)-x(\delta_s)|^2\le\frac{3(\tau K_1^2+K_2^2)}{1-6\tau^2K_3^2}\int_{\delta_s}^s\mathbb E|x(z)|^2dz+\frac{6\tau^2K_3^2}{1-6\tau^2K_3^2}\mathbb E|x(s)|^2E∣x(s)−x(δs​)∣2≤1−6τ2K32​3(τK12​+K22​)​∫δs​s​E∣x(z)∣2dz+1−6τ2K32​6τ2K32​​E∣x(s)∣2.
  4. (3.23) sup⁡t≥0E∣x(t)∣2<∞\sup_{t\ge0}\mathbb E|x(t)|^2<\inftysupt≥0​E∣x(t)∣2<∞.
  5. ∣E∣x(t2)∣2−E∣x(t1)∣2∣≤C(t2−t1)|\mathbb E|x(t_2)|^2-\mathbb E|x(t_1)|^2|\le C(t_2-t_1)∣E∣x(t2​)∣2−E∣x(t1​)∣2∣≤C(t2​−t1​).
  6. Theorem 3.3: lim⁡t→∞E∣x(t)∣2=0\lim_{t\to\infty}\mathbb E|x(t)|^2=0limt→∞​E∣x(t)∣2=0.
  7. (3.24)–(3.25): E∫0∞∣x(t)∣2dt<∞\mathbb E\int_0^\infty|x(t)|^2dt<\inftyE∫0∞​∣x(t)∣2dt<∞ and lim inf⁡t→∞∣x(t)∣=0\liminf_{t\to\infty}|x(t)|=0liminft→∞​∣x(t)∣=0 a.s.
  8. (3.28): P(∃t:∣x(t)∣≥h)≤C/h2\mathbb P(\exists t:|x(t)|\ge h)\le C/h^2P(∃t:∣x(t)∣≥h)≤C/h2 for h>∣x0∣h>|x_0|h>∣x0​∣.

Significance

The result. Theorem 3.4 says that a controller sampling the state at rate 1/τ1/\tau1/τ makes almost every trajectory of the switching system converge to the equilibrium, with an explicit, checkable bound (3.5) on τ\tauτ. Mean-square convergence (Theorem 3.3) does not imply almost sure convergence in general, and a single trajectory is what an operator observes, so the pathwise statement is the one relevant to a deployed system. Condition (3.5) is stated in terms of the constants of Assumptions 2.1, 2.2 and 3.1, so for a concrete system (Section 6 of the paper) it gives a numerical bound on the observation interval.

Formalizing it. The results are proved in the paper; none of them is machine-checked. Mathlib has real Brownian motion but no Itô integral, no stochastic differential equations and no continuous-time Markov chains. The mission therefore also produces a reusable definition layer: a filtration under the usual conditions, a multidimensional {Ft}\{\mathcal F_t\}{Ft​}-Brownian motion, an {Ft}\{\mathcal F_t\}{Ft​}-Markov chain with a given generator, the L2L^2L2 Itô integral of vector-valued integrands, and the solution notion of an SDE with Markovian switching and a sampled-state delay. A related but different layer exists on Prove2Me for Ethier–Kurtz (EthierKurtz_IsStandardBrownian, EthierKurtz_HasBrownianItoIntegral, EthierKurtz_SolvesBrownianSDE); it has no mode switching and no sampled state, so it cannot express (2.1).

Difficulty

Equation (2.1) is a stochastic differential delay equation with the delay t−δtt-\delta_tt−δt​, which is bounded but jumps at every observation time and has derivative 111 in between. The stability theorems for hybrid delay equations in the literature require a differentiable delay with derivative less than one (Mao–Yuan, p. 285), so they do not apply. Applying LU\mathcal LULU directly to U(x(t),r(t),t)U(x(t),r(t),t)U(x(t),r(t),t) leaves the term Ux[u(x(t))−u(x(δt))]U_x[u(x(t))-u(x(\delta_t))]Ux​[u(x(t))−u(x(δt​))], which has no sign and depends on the path over a whole observation interval, so a Lyapunov function of the current state alone does not close the argument.

For the goal, the natural first idea, deducing almost sure convergence from E∣x(t)∣2→0\mathbb E|x(t)|^2\to0E∣x(t)∣2→0 or from ∫0∞∣x(t)∣2dt<∞\int_0^\infty|x(t)|^2dt<\infty∫0∞​∣x(t)∣2dt<∞ a.s., fails: both are compatible with paths that make ever shorter excursions away from 000. The obstacle is to exclude infinitely many excursions of a fixed size, which neither moment statement controls.

Formalization scope

Conventions committed to in Lean:

  • The state space is EuclideanSpace ℝ (Fin n), so ∣x∣|x|∣x∣ is the Euclidean norm; the explicit constants in (3.5) and (3.21) depend on it. The diffusion ggg is given by its mmm columns and ∣g∣2=∑k∣gk∣2|g|^2=\sum_k|g_k|^2∣g∣2=∑k​∣gk​∣2 (trace norm). Modes are Fin N (0-based). Time is ℝ≥0; time integrals are over subsets of R\mathbb RR at s.toNNReal.
  • Every expectation E∣⋅∣2\mathbb E|\cdot|^2E∣⋅∣2 and every time integral of a nonnegative quantity is a lower Lebesgue integral in [0,∞][0,\infty][0,∞], so a non-integrable process cannot produce a junk value 000.
  • "The solution of (2.1)" is read as every process satisfying the solution definition: progressively measurable, almost surely continuous paths, E∣x(t)∣2<∞\mathbb E|x(t)|^2<\inftyE∣x(t)∣2<∞ for each ttt, and for each ttt, almost surely, the integral equation with Itô integrals in the L2L^2L2 sense. Existence and uniqueness (cited from Mao–Yuan on p. 908) are not asserted.
  • "An mmm-dimensional Brownian motion" and "a Markov chain with generator Γ\GammaΓ" are read in the Mao–Yuan framework the paper cites: an {Ft}\{\mathcal F_t\}{Ft​}-Brownian motion with independent coordinates and increments independent of the past, and an {Ft}\{\mathcal F_t\}{Ft​}-Markov chain with transition matrix etΓe^{t\Gamma}etΓ. The usual conditions are kept as hypotheses.
  • "Locally Lipschitz" is uniform in the mode and time on each ball. C2,1C^{2,1}C2,1 carries its derivatives Ut,Ux,UxxU_t,U_x,U_{xx}Ut​,Ux​,Uxx​ as witnesses tied to UUU by derivative relations and joint continuity.
  • "τ>0\tau>0τ>0 sufficiently small for (3.5)" means every τ>0\tau>0τ>0 satisfying both inequalities of (3.5). U,λ1,λ2,τU,\lambda_1,\lambda_2,\tauU,λ1​,λ2​,τ are data of each statement. The paper's "CCC denotes a positive constant" is an existential chosen after x0x_0x0​, r0r_0r0​ and the solution, and before the time variables and hhh.
  • (3.15) and (3.21) are stated under fewer hypotheses than the surrounding proof has (Assumptions 2.1, 2.2, τ>0\tau>0τ>0, and for (3.21) τ≤1/(4K3)\tau\le1/(4K_3)τ≤1/(4K3​)), because their derivations use no more. Misprints on the page (for example g(x,i,s)=f(x,i,0)g(x,i,s)=f(x,i,0)g(x,i,s)=f(x,i,0) on p. 909 and the swapped definitions of ∨,∧\vee,\wedge∨,∧ on p. 907) are not formalized.

A trivializing formalization is ruled out: the expectations are not Bochner integrals (which vanish for non-integrable integrands), the solution notion admits the true solution and requires path continuity, the derivative witnesses of UUU are tied to UUU, and a sorry-free check shows that the data hypotheses (Assumptions 2.1, 2.2, 3.1, C2,1C^{2,1}C2,1, (3.5)) are satisfiable, for example by n=m=N=1n=m=N=1n=m=N=1, f=g=0f=g=0f=g=0, u(x)=−xu(x)=-xu(x)=−x, U=∣x∣2U=|x|^2U=∣x∣2, λ1=1/4\lambda_1=1/4λ1​=1/4, λ2=1\lambda_2=1λ2​=1, τ=1/10\tau=1/10τ=1/10.

Welcome contributions: the Itô isometry and Itô's formula for the L2L^2L2 integral defined here, a generalized Itô formula for functions of a Markov-modulated Itô process, and Doob's maximal inequality in continuous time. These are reusable far beyond this mission. Section 4 of the paper (exponential stability) is a separate mission of the same series.

Selected references

  • S. You, W. Liu, J. Lu, X. Mao, Q. Qiu, Stabilization of Hybrid Systems by Feedback Control Based on Discrete-Time State Observations, SIAM J. Control Optim. 53(2), 905–925, 2015. https://doi.org/10.1137/140985779
  • X. Mao, C. Yuan, Stochastic Differential Equations with Markovian Switching, Imperial College Press, 2006. https://doi.org/10.1142/p473
  • X. Mao, Stabilization of continuous-time hybrid stochastic differential equations by discrete-time feedback control, Automatica 49(12), 3677–3681, 2013. https://doi.org/10.1016/j.automatica.2013.09.005
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Control TheoryOperations ResearchOptimization+1·Captain: mikedeng1

A General Stochastic Maximum Principle for Optimal Control Problems: The Maximum Principle with First- and Second-Order Adjoint ProcessesResearch Paper

Motivation

Pontryagin's maximum principle gives necessary conditions for optimality in deterministic optimal control: along an optimal trajectory, the optimal control maximizes (or minimizes) a Hamiltonian built from an adjoint process. For a system driven by Brownian noise the analogous statement was open in full generality for two decades. The difficulty appears exactly when the diffusion coefficient depends on the control and the control domain is not convex, the situation of controlled volatility in finance, of controlled noise intensity in engineering, and of any problem whose admissible actions form a discrete or otherwise nonconvex set.

Shige Peng's 1990 paper (SIAM J. Control Optim. 28(4)) closed that case. It introduced the second-order adjoint process and a second-order variational inequality, and it is the starting point of the modern theory of stochastic Hamiltonian systems and of backward stochastic differential equations as a tool in control.

Timeline.

  • 1972: Kushner obtains necessary conditions for diffusions whose diffusion coefficient does not depend on the control (SIAM J. Control 10).
  • 1973–1978: Bismut introduces the adjoint equation as a linear backward stochastic differential equation and develops duality methods (SIAM Review 20).
  • Early 1980s: Bensoussan and Haussmann prove maximum principles for convex control domains or control-independent diffusion, using the first-order adjoint equation only.
  • 1990: Peng proves the general principle, with control-dependent diffusion and an arbitrary nonempty control domain (this mission). In the same year Pardoux and Peng prove existence and uniqueness for nonlinear backward SDEs (Systems Control Lett. 14).
  • 1999: Yong and Zhou give a textbook account of the theory (Springer).

Setting

Let (Ω,F,P)(\Omega,\mathcal F,P)(Ω,F,P) be a probability space carrying a standard ddd-dimensional Wiener process B=(B1,…,Bd)B=(B^1,\dots,B^d)B=(B1,…,Bd), and let Ft=σ{B(s);0≤s≤t}\mathcal F^t=\sigma\{B(s);0\le s\le t\}Ft=σ{B(s);0≤s≤t} be its natural filtration. Fix a horizon T>0T>0T>0, an initial state x0∈Rnx_0\in\mathbb R^nx0​∈Rn and a nonempty control domain U⊆RkU\subseteq\mathbb R^kU⊆Rk. The data are

g:Rn×Rk→Rn,σ=(σ1,…,σd), σj:Rn×Rk→Rn,l:Rn×Rk→R,h:Rn→R.g:\mathbb R^n\times\mathbb R^k\to\mathbb R^n,\quad \sigma=(\sigma^1,\dots,\sigma^d),\ \sigma^j:\mathbb R^n\times\mathbb R^k\to\mathbb R^n,\quad l:\mathbb R^n\times\mathbb R^k\to\mathbb R,\quad h:\mathbb R^n\to\mathbb R .g:Rn×Rk→Rn,σ=(σ1,…,σd), σj:Rn×Rk→Rn,l:Rn×Rk→R,h:Rn→R.

An admissible control vvv is a progressively measurable UUU-valued process with sup⁡t≤TE∣v(t)∣m<∞\sup_{t\le T}E|v(t)|^m<\inftysupt≤T​E∣v(t)∣m<∞ for every m≥1m\ge1m≥1. Its trajectory solves the state equation

dx(t)=g(x(t),v(t)) dt+∑j=1dσj(x(t),v(t)) dBj(t),x(0)=x0,dx(t)=g(x(t),v(t))\,dt+\sum_{j=1}^d\sigma^j(x(t),v(t))\,dB^j(t),\qquad x(0)=x_0,dx(t)=g(x(t),v(t))dt+j=1∑d​σj(x(t),v(t))dBj(t),x(0)=x0​,

and its cost is J(v)=E∫0Tl(x(t),v(t)) dt+E h(x(T))J(v)=E\int_0^Tl(x(t),v(t))\,dt+E\,h(x(T))J(v)=E∫0T​l(x(t),v(t))dt+Eh(x(T)). A pair (y,u)(y,u)(y,u) is optimal when J(u)≤J(v)J(u)\le J(v)J(u)≤J(v) for every admissible vvv.

Assumption (3): g,σ,l,hg,\sigma,l,hg,σ,l,h are C2C^2C2 in xxx, jointly continuous in (x,v)(x,v)(x,v) together with their first and second xxx-derivatives; gx,gxx,σx,σxx,lxx,hxxg_x,g_{xx},\sigma_x,\sigma_{xx},l_{xx},h_{xx}gx​,gxx​,σx​,σxx​,lxx​,hxx​ are bounded; and g,σ,lx,hxg,\sigma,l_x,h_xg,σ,lx​,hx​ grow at most like C(1+∣x∣+∣v∣)C(1+|x|+|v|)C(1+∣x∣+∣v∣).

The Hamiltonian is H(x,v,p,K)=l(x,v)+(p,g(x,v))+∑j(Kj,σj(x,v))H(x,v,p,K)=l(x,v)+(p,g(x,v))+\sum_j(K_j,\sigma^j(x,v))H(x,v,p,K)=l(x,v)+(p,g(x,v))+∑j​(Kj​,σj(x,v)). The first-order adjoint process (p,K)(p,K)(p,K) solves the backward equation

−dp=[gx∗p+∑jσxj∗Kj+lx]dt−∑jKj dBj,p(T)=hx(y(T)),-dp=\Big[g_x^*p+\sum_j\sigma_x^{j*}K_j+l_x\Big]dt-\sum_jK_j\,dB^j,\qquad p(T)=h_x(y(T)),−dp=[gx∗​p+j∑​σxj∗​Kj​+lx​]dt−j∑​Kj​dBj,p(T)=hx​(y(T)),

and the second-order adjoint process (P,Q)(P,Q)(P,Q), symmetric-matrix valued, solves

−dP=[gx∗P+Pgx+∑jσxj∗Pσxj+∑jσxj∗Qj+∑jQjσxj+Hxx]dt−∑jQj dBj,P(T)=hxx(y(T)),-dP=\Big[g_x^*P+Pg_x+\sum_j\sigma_x^{j*}P\sigma_x^j+\sum_j\sigma_x^{j*}Q_j+\sum_jQ_j\sigma_x^j+H_{xx}\Big]dt-\sum_jQ_j\,dB^j,\qquad P(T)=h_{xx}(y(T)),−dP=[gx∗​P+Pgx​+j∑​σxj∗​Pσxj​+j∑​σxj∗​Qj​+j∑​Qj​σxj​+Hxx​]dt−j∑​Qj​dBj,P(T)=hxx​(y(T)),

with all coefficients evaluated along (y(t),u(t))(y(t),u(t))(y(t),u(t)) and both solutions adapted to Ft\mathcal F^tFt.

Formalization targets

Goal: Theorem 3 (p. 975)

If (y,u)(y,u)(y,u) is optimal, then adjoint processes (p,K)(p,K)(p,K) and (P,Q)(P,Q)(P,Q) exist in LF2L^2_{\mathcal F}LF2​, solving the two equations above, such that for every v∈Uv\in Uv∈U, for almost every τ∈[0,T]\tau\in[0,T]τ∈[0,T], almost surely,

H(y,v,p,K−Pσ(y,u))+12tr⁡(σσ∗(y,v)P) ≥ H(y,u,p,K−Pσ(y,u))+12tr⁡(σσ∗(y,u)P),H\big(y,v,p,K-P\sigma(y,u)\big)+\tfrac12\operatorname{tr}\big(\sigma\sigma^*(y,v)P\big)\ \ge\ H\big(y,u,p,K-P\sigma(y,u)\big)+\tfrac12\operatorname{tr}\big(\sigma\sigma^*(y,u)P\big),H(y,v,p,K−Pσ(y,u))+21​tr(σσ∗(y,v)P) ≥ H(y,u,p,K−Pσ(y,u))+21​tr(σσ∗(y,u)P),

all evaluated at time τ\tauτ.

Milestones

  1. Lemma 1: the spike-perturbed state equals y+y1+y2y+y_1+y_2y+y1​+y2​ up to o(ε2)o(\varepsilon^2)o(ε2) in mean square, where y1,y2y_1,y_2y1​,y2​ solve the first- and second-order variational equations (5), (6).
  2. Lemma 2: the cost expansion (11) is ≥o(ε)\ge o(\varepsilon)≥o(ε) at an optimal control.
  3. Eq. (13): existence and uniqueness of (p,K)(p,K)(p,K) as a Riesz representer.
  4. Eq. (14): the cost expansion in Hamiltonian form is ≥o(ε)\ge o(\varepsilon)≥o(ε).
  5. Eq. (17): existence and uniqueness of (P,Q)(P,Q)(P,Q) as a Riesz representer.
  6. Eq. (18): the variational inequality for these representers.
  7. Eq. (19): (p,K)(p,K)(p,K) is the unique solution of the first-order adjoint equation.
  8. Eq. (20): (P,Q)(P,Q)(P,Q) solves the second-order adjoint equation.

Significance

The result. Theorem 3 is the necessary condition for optimal control of diffusions in its general form. When σ\sigmaσ does not depend on the control the trace terms cancel and it reduces to the classical first-order principle. When the control enters the diffusion, the first-order condition is false in general, and the second-order adjoint PPP is the correction. The theorem underlies stochastic linear-quadratic theory, the verification of optimal portfolio and volatility-control policies, and the relation between the maximum principle and the Hamilton–Jacobi–Bellman equation.

Formalizing it. The theorem is classical and proved; none of it is machine-checked. Mathlib has real Brownian motion but no stochastic integral, no SDE and no backward SDE. This mission produces the first formal statements on the platform of a controlled SDE, of a backward SDE and of the maximum principle, together with a precise definition layer (Itô integral, Itô process, BSDE solution) that later missions can reuse, e.g. for Peng's endpoint-constrained principle (§6 of the paper) or for the existence theory of BSDEs. A formal proof would also pin down the approximation arguments the paper leaves to the reader.

Difficulty

The obvious route perturbs the optimal control convexly, u+ε(v−u)u+\varepsilon(v-u)u+ε(v−u), and differentiates the cost. That needs UUU convex. For nonconvex UUU one uses a spike variation on a time interval of length ε\varepsilonε. For deterministic systems the state then moves by O(ε)O(\varepsilon)O(ε) and a first-order expansion suffices. With control-dependent diffusion the stochastic integral over the spike interval moves the state by order ε\sqrt\varepsilonε​ in L2L^2L2, so the first-order variational equation leaves an error of the same order as the effect being measured. Second-order terms in the state enter the cost at order ε\varepsilonε, and they are quadratic, so they cannot be handled by a single linear adjoint. The second-order expansion, the matrix-valued adjoint that represents the quadratic term, and the identification of both adjoints with backward SDEs are where the work lies. On the formal side, none of the stochastic calculus exists in Mathlib: the Itô isometry, Itô's formula for matrix-valued processes, moment estimates for linear SDEs and the martingale representation behind the backward equations all have to be built.

Formalization scope

Conventions committed to in Lean:

  • States, controls and noise are Fin n → ℝ, Fin k → ℝ, Fin d → ℝ with the sup norm; matrices are Matrix (Fin n) (Fin n) ℝ. Time is ℝ≥0, and time integrals are over [0, t] ⊂ ℝ.
  • The Wiener process is Rd\mathbb R^dRd-valued: the paper's "RnR^nRn-valued standard Wiener process" (p. 967) is a misprint, since σ(x,v)∈L(Rd,Rn)\sigma(x,v)\in\mathcal L(R^d,R^n)σ(x,v)∈L(Rd,Rn). Coordinates are independent real Brownian motions (Mathlib's IsBrownianReal).
  • The filtration is the natural filtration of BBB, not completed, as on p. 967.
  • "Adapted", for processes integrated in dtdtdt, is read as progressively measurable.
  • The Itô integral is a relation (an L2L^2L2 limit of elementary integrals, as in Ikeda–Watanabe), not an operator. SDE and BSDE solutions hold "for every ttt, almost surely", with sup⁡tE∣x(t)∣2<∞\sup_tE|x(t)|^2<\inftysupt​E∣x(t)∣2<∞ for forward solutions and LF2L^2_{\mathcal F}LF2​ membership for backward ones.
  • Optimality is among admissible controls of finite cost, and the optimal cost is finite; the paper never states finiteness, and a cost can be +∞+\infty+∞ under (3).
  • Lemma 1 is stated with o(ε2)o(\varepsilon^2)o(ε2) where the page prints "≤Cε2\le C\varepsilon^2≤Cε2" in (4). The proof (via (10)) establishes o(ε2)o(\varepsilon^2)o(ε2), and Lemma 2 needs it. Lemma 1, (13), (17), (19) and (20) are stated for any admissible pair, since their proofs do not use optimality.
  • "≥o(ε)\ge o(\varepsilon)≥o(ε)" means: some r(ε)=o(ε)r(\varepsilon)=o(\varepsilon)r(ε)=o(ε) as ε→0+\varepsilon\to0^+ε→0+ bounds the left side from below for small ε\varepsilonε. "∀v∈U\forall v\in U∀v∈U, a.e., a.s." quantifies vvv first, then τ\tauτ, then ω\omegaω.
  • PPP and QjQ_jQj​ are symmetric-valued (Rn,nR^{n,n}Rn,n is the space of symmetric matrices, p. 973). Stochastic integrals against the matrix σ\sigmaσ or QQQ are sums over the columns, ∑j(⋅)j dBj\sum_j(\cdot)_j\,dB^j∑j​(⋅)j​dBj.

Trivializing formalizations ruled out. Without adaptedness the backward equations have pathwise solutions with K=0K=0K=0 and the goal would be free; every adjoint and every solution is required to be progressive for the natural filtration of BBB. The hypotheses are satisfiable: a sorry-free check shows that the zero problem has an optimal pair and that the Itô relation holds for the zero integrand.

Infrastructure needed, and reusable. The Itô integral and isometry, Itô's formula (vector and matrix forms), existence, uniqueness and moment estimates for linear SDEs with bounded coefficients, Riesz representation in LF2L^2_{\mathcal F}LF2​, and existence and uniqueness for linear BSDEs (via martingale representation for the Brownian filtration). All of these are reusable well beyond this mission; contributions of any of them, as separate theorems, are welcome. Related platform definitions: the Ethier–Kurtz series (EthierKurtz_HasBrownianItoIntegral, EthierKurtz_SolvesBrownianSDE) formalizes an Itô integral by dyadic step approximation and uncontrolled SDEs over a completed filtration. The deterministic Pontryagin principle appears in Vector Space Methods XII and Dynamic Programming and Optimal Control III.

Selected references

  • S. Peng, A General Stochastic Maximum Principle for Optimal Control Problems, SIAM J. Control Optim. 28(4), 966–979, 1990. https://doi.org/10.1137/0328054
  • H. J. Kushner, Necessary Conditions for Continuous Parameter Stochastic Optimization Problems, SIAM J. Control 10(3), 550–565, 1972. https://doi.org/10.1137/0310041
  • J.-M. Bismut, An Introductory Approach to Duality in Optimal Stochastic Control, SIAM Review 20(1), 62–78, 1978. https://doi.org/10.1137/1020004
  • E. Pardoux and S. Peng, Adapted Solution of a Backward Stochastic Differential Equation, Systems & Control Letters 14(1), 55–61, 1990. https://doi.org/10.1016/0167-6911(90)90082-6
  • J. Yong and X. Y. Zhou, Stochastic Controls: Hamiltonian Systems and HJB Equations, Springer, 1999. https://doi.org/10.1007/978-1-4612-1466-3
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Operations ResearchOptimizationTheoretical Computer Science·Captain: mikedeng1

An Optimal On-Line Algorithm for Metrical Task System 2: The Randomized Competitive Ratio of the Uniform Task System Lies Between H(n) and 2H(n)Research Paper

Motivation

Metrical task systems, introduced by Borodin, Linial and Saks (J. ACM 39(4), 1992), are a common abstraction of on-line problems in which a server occupies one of finitely many states, pays a cost for each task depending on its current state, and may pay a transition cost to change state first. Paging, list update and the kkk-server problem all fit into this framework. The paper's first main result is that every deterministic on-line algorithm on an nnn-state metrical task system has competitive ratio at least 2n−12n-12n−1, and that 2n−12n-12n−1 is attained. The lower bound comes from an adversary that always charges the state the algorithm currently occupies. That adversary needs to know the algorithm's state, which suggests that randomization can help.

Section 7 of the paper makes this precise for the simplest system, the uniform task system, in which all transitions cost 111. There the randomized competitive ratio against an oblivious adversary is between H(n)H(n)H(n) and 2H(n)2H(n)2H(n), where H(n)=1+12+⋯+1nH(n)=1+\tfrac12+\cdots+\tfrac1nH(n)=1+21​+⋯+n1​ is between ln⁡n\ln nlnn and 1+ln⁡n1+\ln n1+lnn. This was the first logarithmic bound for a task system.

Timeline:

  • 1985: Sleator and Tarjan introduce competitive analysis for list update and paging (CACM 28(2)).
  • 1987/1992: Borodin, Linial and Saks define metrical task systems, prove the deterministic ratio 2n−12n-12n−1, and prove H(n)≤wˉ≤2H(n)H(n)\le\bar w\le 2H(n)H(n)≤wˉ≤2H(n) for the uniform system (conference version STOC 1987; journal version cited above).
  • 1991: Fiat, Karp, Luby, McGeoch, Sleator and Young prove the analogous 2Hk2H_k2Hk​ upper bound for randomized paging (J. Algorithms 12(4)).

Setting

A task system (S,d)(S,d)(S,d) is a finite set SSS of nnn states with a transition-cost matrix ddd: d(i,i)=0d(i,i)=0d(i,i)=0, d(i,j)>0d(i,j)>0d(i,j)>0 for i≠ji\ne ji=j, and d(i,k)≤d(i,j)+d(j,k)d(i,k)\le d(i,j)+d(j,k)d(i,k)≤d(i,j)+d(j,k). In the uniform task system, d(i,j)=1d(i,j)=1d(i,j)=1 for all i≠ji\neq ji=j. A task is a vector T∈R≥0ST\in\mathbb R_{\ge0}^ST∈R≥0S​ of processing costs. Given an initial state s0s_0s0​ and tasks T=T1⋯Tm\mathbf T=T^1\cdots T^mT=T1⋯Tm, a schedule is σ:{0,…,m}→S\sigma:\{0,\dots,m\}\to Sσ:{0,…,m}→S with σ(0)=s0\sigma(0)=s_0σ(0)=s0​, of cost

c(T;σ)=∑i=1md(σ(i−1),σ(i))+∑i=1mTi(σ(i)).c(\mathbf T;\sigma)=\sum_{i=1}^m d(\sigma(i-1),\sigma(i))+\sum_{i=1}^m T^i(\sigma(i)).c(T;σ)=i=1∑m​d(σ(i−1),σ(i))+i=1∑m​Ti(σ(i)).

The off-line optimum c0(T)c_0(\mathbf T)c0​(T) is the least cost over all schedules.

A deterministic on-line algorithm chooses σ(i)\sigma(i)σ(i) from s0s_0s0​ and T1,…,TiT^1,\dots,T^iT1,…,Ti. A randomized on-line algorithm RRR chooses σ(i)\sigma(i)σ(i) at random, with a distribution that depends on s0s_0s0​, on T1,…,TiT^1,\dots,T^iT1,…,Ti and on the states σ(0),…,σ(i−1)\sigma(0),\dots,\sigma(i-1)σ(0),…,σ(i−1) already visited. The task sequence is fixed before any random choice is made (an oblivious adversary). With pr(σ∣T)\mathrm{pr}(\sigma\mid\mathbf T)pr(σ∣T) the probability that RRR follows σ\sigmaσ, the expected cost is cˉR(T)=∑σc(T;σ) pr(σ∣T)\bar c_R(\mathbf T)=\sum_\sigma c(\mathbf T;\sigma)\,\mathrm{pr}(\sigma\mid\mathbf T)cˉR​(T)=∑σ​c(T;σ)pr(σ∣T). For w>0w>0w>0, RRR is expected www-competitive if there is a constant KKK with

cˉR(T)≤w c0(T)+K\bar c_R(\mathbf T)\le w\,c_0(\mathbf T)+KcˉR​(T)≤wc0​(T)+K

for every finite task sequence and every initial state. The randomized competitive ratio wˉ(S,d)\bar w(S,d)wˉ(S,d) is the infimum of all such www over all RRR.

Formalization targets

Goal: Theorem 7.1

For the uniform task system on n≥1n\ge1n≥1 states,

H(n)  ≤  wˉ(S,d)  ≤  2H(n).H(n)\;\le\;\bar w(S,d)\;\le\;2H(n).H(n)≤wˉ(S,d)≤2H(n).

Milestones

  1. Upper bound (p. 759). Some randomized on-line algorithm is expected 2H(n)2H(n)2H(n)-competitive on the uniform task system.
  2. Lemma 7.2 (p. 759). Let DDD be a distribution on infinite task sequences over a finite task alphabet, with E(c0(Tj))→∞E(c_0(\mathbf T^j))\to\inftyE(c0​(Tj))→∞, and let mj=inf⁡AE(cA(Tj))m_j=\inf_A E(c_A(\mathbf T^j))mj​=infA​E(cA​(Tj)) over deterministic on-line algorithms. Then every achievable www satisfies
lim sup⁡j→∞mjE(c0(Tj))≤w.\limsup_{j\to\infty}\frac{m_j}{E(c_0(\mathbf T^j))}\le w .j→∞limsup​E(c0​(Tj))mj​​≤w.
  1. mj≥j/nm_j\ge j/nmj​≥j/n (p. 760) when the tasks are independent uniformly random unit elementary tasks UsU_sUs​ (cost 111 in sss, 000 elsewhere).
  2. Coupon collector (p. 760). For i.i.d. uniform states on SSS, the expected number of draws until every state has appeared is nH(n)nH(n)nH(n).
  3. Off-line cost (p. 760). Under the same distribution, E(c0(Tj))≤j/(nH(n))+CE(c_0(\mathbf T^j))\le j/(nH(n))+CE(c0​(Tj))≤j/(nH(n))+C for a constant CCC independent of jjj.

Significance

The theorem shows that randomization reduces the competitive ratio of the uniform task system from 2n−12n-12n−1 to Θ(log⁡n)\Theta(\log n)Θ(logn). That is an exponential improvement, and it identifies the adversary's knowledge of the algorithm's state as the source of the deterministic lower bound. Lemma 7.2 is a form of Yao's principle adapted to the additive-constant definition of competitiveness. It is the standard tool for randomized lower bounds in on-line computation, and the same argument shape reappears for paging and kkk-server lower bounds.

On the formalization side, the result is proved but, as far as is known, has not been machine-checked. A complete development yields a reusable model of randomized on-line algorithms with oblivious adversaries, a Yao-type lemma usable for other on-line problems, and a coupon-collector expectation in the product-measure setting. The upper half additionally needs the continuous-time reduction of the paper's Lemma 3.1 in randomized form, or a direct discrete-time algorithm.

Difficulty

For the upper bound, the natural algorithm is continuous-time. It proceeds in phases, and inside a phase it stays in a state until that state has accumulated cost 111. A discrete task can saturate several states at once and straddle a phase boundary. So a discrete algorithm must either simulate the continuous one or be analyzed directly, and the expected transition count per phase must be controlled with the first phase starting in a deterministic state.

For the lower bound, the first obstacle is that the natural statement "wˉ≥lim sup⁡mj/E(c0)\bar w\ge\limsup m_j/E(c_0)wˉ≥limsupmj​/E(c0​)" silently assumes that a randomized algorithm's expected cost, averaged over random inputs, is at least that of the best deterministic algorithm. With the behavioural (kernel) definition used here, this requires converting a kernel into a mixture of deterministic algorithms, which is Kuhn's theorem on each finite horizon. The second obstacle is that the paper's claim E(c0(Tj))≤j/(nH(n))+O(1)E(c_0(\mathbf T^j))\le j/(nH(n))+O(1)E(c0​(Tj))≤j/(nH(n))+O(1) is supported only by the elementary renewal theorem, which gives a limit of ratios; the additive bound needs a sharper renewal estimate. Mathlib has no renewal theory. The hypothesis E(c0(Tj))→∞E(c_0(\mathbf T^j))\to\inftyE(c0​(Tj))→∞ of Lemma 7.2 must also be established for the uniform distribution; the paper does not prove it separately.

Formalization scope

  • States form a finite nonempty type S, and nnn = Fintype.card S; no n≥2n\ge2n≥2 assumption is made (at n=1n=1n=1 the goal reads 1≤wˉ≤21\le\bar w\le21≤wˉ≤2, and wˉ=1\bar w=1wˉ=1). H(n)H(n)H(n) is Mathlib's harmonic n, cast to R\mathbb RR. The uniform system has unit transition cost.
  • Tasks are finite and nonnegative. The paper also allows +∞+\infty+∞ entries; these are excluded. Task sequences are Fin m → S → ℝ and schedules are Fin (m+1) → S with σ 0 = s₀. c0c_0c0​ is a finite minimum.
  • A randomized algorithm is a kernel S → List (S → ℝ) → List S → PMF S. This is the paper's scheduler–taskmaster description (p. 758), equivalent to a distribution over deterministic algorithms on every finite task sequence. pr(σ∣T)\mathrm{pr}(\sigma\mid\mathbf T)pr(σ∣T) is the product of kernel probabilities, and cˉR\bar c_RcˉR​ is a finite sum. That pr(⋅∣T)\mathrm{pr}(\cdot\mid\mathbf T)pr(⋅∣T) sums to 111 has been checked locally.
  • wˉ(S,d)\bar w(S,d)wˉ(S,d) is the real sInf of {w:∃R, R expected w-competitive}\{w : \exists R,\ R \text{ expected } w\text{-competitive}\}{w:∃R, R expected w-competitive}. On the empty set this would be 000, so the upper bound is stated as the existence of an expected 2H(n)2H(n)2H(n)-competitive algorithm, and Lemma 7.2 is stated for every achievable www. The goal's lower half forces the set to be nonempty. Statements of the form "wˉ≤c\bar w\le cwˉ≤c" alone are therefore not acceptable substitutes for milestones 1 and 2.
  • Lemma 7.2 is restricted to task sequences over a finite alphabet, with the product σ\sigmaσ-algebra and measurable singletons. This makes every E(cA(Tj))E(c_A(\mathbf T^j))E(cA​(Tj)) a genuine integral for every deterministic AAA, and it covers the paper's application. The lim sup⁡\limsuplimsup of Lemma 7.2 is taken in EReal.
  • The coupon-collector time takes values in [0,∞][0,\infty][0,∞] and its expectation is a lower Lebesgue integral. Milestone 5 renders the paper's O(1)O(1)O(1) as an explicit constant CCC chosen before jjj.

Contributions welcome: proofs of any milestone; a discrete-time randomized phase algorithm; a general Kuhn-type conversion from kernels to mixtures of deterministic algorithms; renewal-theoretic lemmas.

Selected references

  • A. Borodin, N. Linial, M. Saks, An Optimal On-Line Algorithm for Metrical Task System, J. ACM 39(4):745–763, 1992. https://doi.org/10.1145/146585.146588
  • D. D. Sleator, R. E. Tarjan, Amortized Efficiency of List Update and Paging Rules, Commun. ACM 28(2):202–208, 1985. https://doi.org/10.1145/2786.2793
  • A. Fiat, R. M. Karp, M. Luby, L. A. McGeoch, D. D. Sleator, N. E. Young, Competitive Paging Algorithms, J. Algorithms 12(4):685–699, 1991. https://doi.org/10.1016/0196-6774(91)90041-V
  • A. C.-C. Yao, Probabilistic Computations: Toward a Unified Measure of Complexity, FOCS 1977, 222–227. https://doi.org/10.1109/SFCS.1977.24
  • S. M. Ross, Applied Probability Models with Optimization Applications, Holden-Day, 1970 (the elementary renewal theorem cited as [20] in the paper).
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Markov Processes: Characterization and Convergence V: Change of Variables for Continuous SemimartingalesTextbook

Change of variables along random paths

The ordinary chain rule describes how a smooth function changes along a differentiable path. A continuous stochastic path can have fluctuations whose accumulated squared increments remain visible even when the time partition becomes arbitrarily fine. The change of variables formula must account for these fluctuations as well as the part of the path with finite variation. Ethier and Kurtz give this identity for time-dependent functions of multidimensional continuous semimartingales in Chapter 5, Theorem 2.9, equations (2.40)–(2.41), of Markov Processes: Characterization and Convergence.

Processes and smooth functions

Work on a complete probability space with a filtration, an increasing family of sigma algebras describing the information available at each nonnegative time. The initial sigma algebra contains every ambient null set. For each coordinate, a continuous semimartingale has a decomposition

Xi(t)=Xi(0)+Vi(t)+Mi(t).X_i(t)=X_i(0)+V_i(t)+M_i(t).Xi​(t)=Xi​(0)+Vi​(t)+Mi​(t).

The initial vector is measurable with respect to the initial information. Each process ViV_iVi​ is continuous and adapted, starts at zero, and has bounded variation on every bounded time interval. Each MiM_iMi​ is a continuous adapted local martingale, initially zero almost surely: stopping along a suitable sequence of stopping times tending to infinity gives martingales. No Brownian driver or diffusion coefficient is specified.

Let f(t,x)f(t,x)f(t,x) be a real-valued function of nonnegative time and a vector in Rd\mathbb R^dRd. The regularity class C1,2C^{1,2}C1,2 requires joint continuity of the function, its first time derivative, all first spatial derivatives, and all second spatial derivatives. The time derivative at zero is interpreted from the right. The hypotheses impose no compact support, global derivative bound, or second time derivative.

The change of variables identity

The goal is the complete identity

f(t,X(t))−f(0,X(0))=∫0tft(s,X(s)) ds+∑i∫0tfxi(s,X(s)) dVi(s)+∑i∫0tfxi(s,X(s)) dMi(s)+12∑i,j∫0tfxixj(s,X(s)) d⟨Mi,Mj⟩s.\begin{aligned} f(t,X(t))-f(0,X(0))={}&\int_0^t f_t(s,X(s))\,ds\\ &+\sum_i\int_0^t f_{x_i}(s,X(s))\,dV_i(s)\\ &+\sum_i\int_0^t f_{x_i}(s,X(s))\,dM_i(s)\\ &+\frac12\sum_{i,j}\int_0^t f_{x_ix_j}(s,X(s))\,d\langle M_i,M_j\rangle_s. \end{aligned}f(t,X(t))−f(0,X(0))=​∫0t​ft​(s,X(s))ds+i∑​∫0t​fxi​​(s,X(s))dVi​(s)+i∑​∫0t​fxi​​(s,X(s))dMi​(s)+21​i,j∑​∫0t​fxi​xj​​(s,X(s))d⟨Mi​,Mj​⟩s​.​

It holds almost surely simultaneously for every nonnegative time. The quadratic covariation ⟨Mi,Mj⟩\langle M_i,M_j\rangle⟨Mi​,Mj​⟩ records the limit of sums of products of increments. Both diagonal and off-diagonal contributions occur. The bracket processes and integral versions are supplied by the conclusion, rather than imposed as additional restrictions on the input processes.

What the identity supplies

The formula determines how a smooth observation of the evolving state changes. Its terms separate explicit time dependence, finite-variation motion, martingale fluctuations, and their second-order correction. This is the calculus result for a given continuous semimartingale; existence or uniqueness of solutions to a stochastic differential equation is a separate mathematical question. The target is the known theorem in the cited book. Its mathematical assertion includes existence of the integral versions appearing in the displayed identity.

Why continuity does not give the ordinary chain rule

Continuity of the sample paths does not imply bounded variation of the martingale component. Consequently, ordinary pathwise integration against that component does not supply the needed calculus. The stochastic integral requires a probabilistic limiting interpretation. A further issue is the exceptional set: an identity established separately at each time does not by itself provide one event of full probability on which it holds at every time. The continuous versions and the order of the quantifiers address that distinction.

Representations and boundary conventions

Coordinates are indexed by Fin d, and time is nonnegative. Allowing zero coordinates also includes the consistent case of a function of time alone. A dyadic partition has 2n2^n2n intervals, so the denominators in the defining sums are nonzero, including at partition level zero. At time zero all increments vanish.

The finite-variation integrals are characterized pathwise by limits of left dyadic sums. The stochastic integrals are continuous adapted processes characterized by convergence of those sums in probability at each fixed time. The cross brackets are characterized by the corresponding increment-product sums and are required to have continuous adapted versions of locally bounded variation. These predicates do not assume the change of variables identity. The ordinary time integral has a continuous integrand on each compact interval, so its integrability follows from the stated hypotheses. The source's almost-sure version conventions are retained; right continuity of the filtration is not an additional hypothesis.

Selected reference

Stewart N. Ethier and Thomas G. Kurtz, Markov Processes: Characterization and Convergence, Wiley, 1986. Chapter 5, Stochastic Integral Equations, §2, Theorem 2.9, printed p.287 (held PDF p.296). Probability-space and version conventions: printed pp.279–280 and 286 (PDF pp.288–289 and 295).

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Stochastic Systems·Captain: mikedeng1

Markov Processes: Characterization and Convergence IV: Martingale characterization of Markov processesTextbook

From local evolution to a Markov process

A stochastic process can be described through the way functions of its state change over time. For a suitable pair of functions f and g, the difference between f evaluated along the process and the accumulated integral of g has zero conditional drift. A martingale problem specifies a collection of such pairs. The question is whether these local conditions determine the evolution of the process, including the dependence of its future on its past. Ethier and Kurtz's Chapter 4, Theorem 4.1 answers this question under analytic hypotheses on the collection of pairs and a separation condition on the functions being observed.

State space, functions, and histories

Let E be a separable metric space, with its Borel sigma algebra. Write B(E) for the bounded real Borel functions, equipped with the uniform norm. A linear relation A is a linear subspace of B(E) × B(E). A pair (f,g) in A prescribes g as the drift associated with f; the relation is allowed to be multivalued. It is dissipative when

a∥f∥≤∥af−g∥((f,g)∈A, a>0).a\|f\|\leq\|af-g\|\qquad ((f,g)\in A,\ a>0).a∥f∥≤∥af−g∥((f,g)∈A, a>0).

Let μ be a probability measure on E. A solution X of the martingale problem for (A,μ) is a jointly measurable process on a probability space with initial law μ, satisfying the compensated moment identities of Chapter 4, equation (3.4). Those identities test each compensated increment against products of bounded Borel functions of finitely many earlier states. The natural past at time s is the sigma algebra generated by all coordinates X(r) with r≤s.

A subspace L of B(E) is separating if two Borel probability measures that have the same integral against every function in L must be equal. This is a condition on measures, stronger in purpose than merely distinguishing individual states.

Characterization target

Suppose A′ is a linear subrelation of A and, for some λ>0,

R(λ−A′)‾=D(A′)‾=L,\overline{\mathcal R(\lambda-A')}=\overline{\mathcal D(A')}=L,R(λ−A′)​=D(A′)​=L,

where both closures use the uniform norm and L is separating. Given a solution X of (A,μ), the target is the existence of a strongly continuous contraction semigroup T on L generated by the closed relation A′‾\overline{A'}A′, together with

E[f(X(s+t))∣FsX]=(T(t)f)(X(s))(s,t≥0, f∈L).\mathbb E[f(X(s+t))\mid\mathcal F_s^X]=(T(t)f)(X(s))\quad(s,t\geq0,\ f\in L).E[f(X(s+t))∣FsX​]=(T(t)f)(X(s))(s,t≥0, f∈L).

The process is Markov: for every bounded Borel observable, conditioning a future observation on the entire past agrees almost surely with conditioning on the present state. In addition, any other solution with initial law μ has exactly the same finite-dimensional distributions as X. The competing solution may live on a different probability space. Existence of X is an assumption; the existence conclusion concerns its corresponding semigroup.

What the characterization establishes

The theorem joins an analytic description of evolution with a probabilistic one. The closed generator relation determines a semigroup, while the martingale identities identify the conditional evolution of the supplied process. Separation allows observables in L to determine probability laws. Uniqueness concerns every finite list of observation times, which is the source's convention for this martingale problem.

This is a known theorem of Ethier and Kurtz. The formalization target is its complete statement and eventually a machine-checked proof. The present theorem remains a proof obligation. Its expression infrastructure consists of bounded functions, the natural past, and the finite-history definition of a solution.

Mathematical difficulty

The observed functions initially lie in a subspace L, whereas the Markov conclusion ranges over all bounded Borel observations. Identifying only individual expectations does not by itself establish conditional evolution or equality of joint laws. The analytic part must also identify the entire generator graph: agreement on the original relation alone is weaker than the asserted equality with its closure. Both closure hypotheses and probability-measure separation are therefore part of the target.

Formalization scope

Bounded functions are actual pointwise real functions with the uniform norm. Borel measurability is imposed on the relation, and uniform limits preserve it. The construction does not use functions modulo almost-everywhere equality. The state space is separable and metric; completeness and local compactness are not additional hypotheses. Processes need no right-continuous or cadlag paths.

Histories may be empty, repeated, or unordered, with every history time at most the start of the increment. Products combine repeated observations. Boundedness and finite time intervals ensure the required integrability. Nonnegative real times index the processes. The semigroup is represented by a real-indexed family whose axioms concern nonnegative times; negative-time values have no mathematical role. Generator equality is a biconditional for the derivative limit from positive times. The target retains semigroup correspondence, the ordinary Markov property, and unrestricted finite-dimensional uniqueness as one theorem.

Selected references

Stewart N. Ethier and Thomas G. Kurtz, Markov Processes: Characterization and Convergence, Wiley, 1986, Chapter 4, Theorem 4.1, printed p.182 (PDF p.191); equations (3.4) and (4.2), printed pp.174 and 183. Separation conventions: Chapter 3, printed pp.112 and 116. Chapter 4.

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Stochastic Systems·Captain: mikedeng1

Ethier–Kurtz: Martingales with partially ordered time (Theorem 8.7)Textbook

Martingales with partially ordered time

Optional sampling relates a process observed at two random times. A martingale has a conditional expectation at an earlier index equal to its value there, but this defining property initially concerns deterministic indices. Random indices require a separate theorem. In Chapter 2, Section 8, Ethier and Kurtz extend optional sampling to a partially ordered family of indices for use in the time changes of Chapter 6. The target is their Theorem 8.7, printed pages 87–88.

Metric lattices and information

A metric lattice is a partially ordered metric space I in which each pair of points has a greatest lower bound and a least upper bound. These are written as the meet and join. Both operations are jointly continuous. Points need not be comparable. The interval between u ≤ v consists of all points w with u ≤ w ≤ v.

A subset is separable from above if it contains a sequence aₙ that approximates each of its points w by the finite meets of those aᵢ with w ≤ aᵢ and i ≤ n. Each such meet is taken once this finite set is nonempty. The resulting sequence of meets must converge to w. The theorem assumes this condition for each interval.

Let Ω carry a probability measure P and an ambient sigma algebra. A filtration assigns a sub-sigma algebra Fᵤ to each index u, increasing with the order. A real-valued process X is a martingale if each X(u) is Fᵤ-measurable and integrable and, whenever u ≤ v,

E[X(v)∣Fu]=X(u)almost surely.E[X(v)\mid F_u]=X(u)\quad\text{almost surely}.E[X(v)∣Fu​]=X(u)almost surely.

Right continuity here has a specific lattice meaning: for every u and every outcome ω, X(u ∨ v,ω) tends to X(u,ω) as v tends to u. A stopping time τ is a Borel-measurable I-valued random variable such that {τ ≤ u} belongs to Fᵤ for every u.

The optional-sampling target

Take stopping times τ₁ ≤ τ₂ pointwise. Suppose there are deterministic sequences uₙ and vₙ in I such that

P{un≤τ1≤τ2≤vn}⟶1,P\{u_n\leq\tau_1\leq\tau_2\leq v_n\}\longrightarrow1,P{un​≤τ1​≤τ2​≤vn​}⟶1,

and

E[∣X(vn)∣1{τ2≤vn}c]⟶0.E[|X(v_n)|\mathbf1_{\{\tau_2\leq v_n\}^{c}}]\longrightarrow0.E[∣X(vn​)∣1{τ2​≤vn​}c​]⟶0.

Assume also that X(τ₂) is integrable. The target is

E[X(τ2)∣Fτ1]=X(τ1)almost surely.E[X(\tau_2)\mid F_{\tau_1}]=X(\tau_1)\quad\text{almost surely}.E[X(τ2​)∣Fτ1​​]=X(τ1​)almost surely.

The sigma algebra Fτ consists of ambient-measurable events A for which A ∩ {τ ≤ u} belongs to Fᵤ for every u. This is the information used in the conclusion.

What the result provides

The conclusion extends the martingale identity to random lattice indices under explicit exhaustion and tail assumptions. Neither a deterministic bound on both stopping times nor a linear ordering of all indices is part of the statement. This is a known theorem in the cited book. The formal target retains the full conditional-expectation identity; its proof remains to be formalized.

Why the hypotheses matter

In a partially ordered space, the complement of {τ₂ ≤ vₙ} includes incomparable indices. Replacing this complement by {vₙ < τ₂} would change the tail assumption. Likewise, right continuity must use lattice joins, rather than a one-dimensional time convention. Controlling probabilities of the exhaustion events alone does not state the integrability control required by the second limit. Both limits belong to the theorem.

Mathematical scope and conventions

The index space has a metric and a lattice structure with continuous meet and join. No top, bottom, completeness of the metric, or linear order is required. The filtration need not be complete or right continuous. The stopping times are finite I-valued variables; their measurability is explicit. The sequences uₙ and vₙ need not be monotone. The nonnegative tail expectation uses extended nonnegative integration, avoiding a default value for a nonintegrable real integral. Indexwise integrability is retained explicitly, along with terminal integrability.

The two accompanying definitions express separation from above and the stopped sigma algebra. Together with the martingale and stopping-time conditions, they specify the single optional-sampling theorem. The target contains no additional supporting-theorem milestones.

Source

Stewart N. Ethier and Thomas G. Kurtz, Markov Processes: Characterization and Convergence, Wiley, 1986, Chapter 2 §8, Theorem 8.7, printed pp. 87–88 (supplied PDF pp. 96–97); definitions and equation (8.6), printed p. 85 (PDF p. 94). Chapter 2.

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Markov Processes: Characterization and Convergence 20: Two-type critical branching limitsTextbook

Why two types change the limit

Critical branching is a basic scaling model for populations whose expected size neither grows nor decays at leading order. A single-type population has one macroscopic direction, but a two-type population has two coupled directions. In the critical regime considered by Ethier and Kurtz, one weighted population mode survives on the diffusive scale while a second mode is pulled rapidly toward zero. The rapid mode still leaves a random integrated contribution and an initial boundary layer, so discarding it would lose part of the limiting dynamics. The mission packages all of these conclusions from Chapter 9, Section 2, Theorem 2.1 of Ethier and Kurtz as one formal target.

The branching model

The state is a pair of natural numbers recording the numbers of particles of types 1 and 2. A type-iii particle lives for an exponential time with positive rate λi\lambda_iλi​. At death it is replaced by a random pair of offspring with law ρi\rho_iρi​. The generator therefore applies the type-specific replacement rule at an intensity proportional to the current number of particles of that type. The formal predicate IsTwoTypeBranching records a measurable càdlàg process satisfying the corresponding natural-past martingale identities on finite-support tests, with an explicit integrability condition.

The offspring mean matrix has strictly positive entries. Its critical weighted rate matrix has a positive eigenvector ν\nuν with eigenvalue zero and an opposite-sign eigenvector μ\muμ with eigenvalue −η-\eta−η, where η>0\eta>0η>0. For the nnnth process, Lean consistently uses the positive index n+1n+1n+1. At accelerated time (n+1)t(n+1)t(n+1)t, the scaled modes are

Xn(t)=ν1Z1(n)((n+1)t)+ν2Z2(n)((n+1)t)n+1,Yn(t)=μ1Z1(n)((n+1)t)+μ2Z2(n)((n+1)t)n+1.X_n(t)=\frac{\nu_1 Z^{(n)}_1((n+1)t)+\nu_2 Z^{(n)}_2((n+1)t)}{n+1}, \qquad Y_n(t)=\frac{\mu_1 Z^{(n)}_1((n+1)t)+\mu_2 Z^{(n)}_2((n+1)t)}{n+1}.Xn​(t)=n+1ν1​Z1(n)​((n+1)t)+ν2​Z2(n)​((n+1)t)​,Yn​(t)=n+1μ1​Z1(n)​((n+1)t)+μ2​Z2(n)​((n+1)t)​.

The compensated fast coordinate is

Wn(t)=Yn(t)+∫0t(n+1)ηYn(s) ds.W_n(t)=Y_n(t)+\int_0^t (n+1)\eta Y_n(s)\,ds.Wn​(t)=Yn​(t)+∫0t​(n+1)ηYn​(s)ds.

Formalization target

The goal is the complete three-part statement of Theorem 2.1. First, (Xn,Wn)(X_n,W_n)(Xn​,Wn​) converges jointly in path law to a continuous two-dimensional diffusion (X,W)(X,W)(X,W). Its covariance matrix is built from the raw second moments of the two offspring replacement increments, and its generator has the form

Af(x,w)=x2(a11fxx+2a12fxw+a22fww)(x,w).Af(x,w)=\frac{x}{2}\left(a_{11}f_{xx}+2a_{12}f_{xw}+a_{22}f_{ww}\right)(x,w).Af(x,w)=2x​(a11​fxx​+2a12​fxw​+a22​fww​)(x,w).

Second, on every finite time interval the fast mode is uniformly close in probability to its exponentially decaying initial layer Yn(0)e−(n+1)ηtY_n(0)e^{-(n+1)\eta t}Yn​(0)e−(n+1)ηt. On every interval 0<t1<t20<t_1<t_20<t1​<t2​, its integrated drift converges weakly to W(t2)−W(t1)W(t_2)-W(t_1)W(t2​)−W(t1​). Third, the first population coordinate is uniformly reconstructed from XnX_nXn​ together with that same initial layer. The limit statement keeps the possibly nonzero initial fast coordinate and the separate nonnegativity conclusion for the slow coordinate.

What the result supplies

The theorem identifies both the persistent and collapsing directions of a critical multitype system. The slow direction produces population-scale diffusion, while the compensated fast direction records fluctuations that remain visible after the raw fast mode contracts. The reconstruction formula connects these mode coordinates back to the original particle count. Keeping the path limit, fast decay, integrated limit, and reconstruction together prevents an apparently simpler marginal statement from omitting the initial-layer behavior needed at time zero.

The textbook theorem is already mathematically proved. This mission asks for a Lean proof of the reviewed formal statement; the uploaded goal is intentionally a statement with a proof placeholder, not a claim of machine-checked completion. The concrete generator, branching-law predicate, scaling map, càdlàg condition, and diffusion martingale-problem predicate provide reusable vocabulary for related multitype limit theorems.

Where the formal difficulty lies

Coordinatewise convergence is insufficient. The result couples full path laws, a continuous diffusion martingale problem, compact-uniform control of an initial layer, and a positive-time integral of a rapidly changing mode. The naive step of simply setting the fast mode to zero fails at time zero and erases the exponential term needed in the population reconstruction. The covariance coefficients also come from replacement increments rather than centered offspring counts, so changing that convention alters the limiting operator.

Formalization scope and conventions

The state space is exactly N×N\mathbb N\times\mathbb NN×N; both offspring laws are probability measures, both coordinates have finite third moments under each parent law, and all four entries of the mean matrix are positive. Initial populations are deterministic floors of (n+1)zi(n+1)z_i(n+1)zi​ for nonnegative densities ziz_izi​. The positive indexing avoids division by zero in every scaling, clock, and exponential. Natural-number subtraction in the generator is used only with a zero event intensity when the relevant population is empty.

Path convergence is represented by a joint probability-space realization carrying the correct complete prelimit path laws and almost-sure uniform convergence on compact intervals to a continuous limit. This is the continuous-limit Skorohod convention used in the reviewed development. The definitions are concrete: none contains the target theorem or assumes its conclusions. The mission includes only expression-essential dependencies, reusing exact private book-wide definitions for càdlàg paths and the continuous diffusion generator law. It does not add proof-only lemmas or split the three source conclusions into separate missions.

Selected references

  • Stewart N. Ethier and Thomas G. Kurtz, Markov Processes: Characterization and Convergence, Wiley, 1986, Chapter 9, Section 2, Theorem 2.1, printed pp. 392–393. DOI
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Markov Processes: Characterization and Convergence 18: Countable spin-flip systemsTextbook

Why infinite spin systems need a generation theorem

A spin-flip system models a countable collection of two-state components whose transition rates may depend on the entire current configuration. Such systems are basic examples of interacting particle processes: each local move is simple, but infinitely many possible moves may be active and their rates interact through the configuration. The central analytic question is whether the formal sum of local flip operators determines a genuine time evolution on continuous observables. Chapter 8, Section 3 of Stewart N. Ethier and Thomas G. Kurtz, Markov Processes: Characterization and Convergence, answers this question under uniform rate and influence bounds Ethier--Kurtz, Theorem 3.5.

This mission states that result without replacing the countable system by a finite-state chain or assuming finite total jump intensity. It also retains the theorem's cylinder-function core, which identifies finitely coordinate-dependent observables as a sufficient starting class for recovering the closed generator.

Configuration space and coordinate variation

Let S be a countable type of sites. A configuration is a function η : S → Bool; false and true relabel the source spins -1 and 1. The product topology on these configurations is the one induced by the discrete topology on each coordinate. The Lean space C(S → Bool, ℝ) consists of real-valued continuous observables on this compact product space and carries its uniform norm.

For a site i, spinFlip i η agrees with η away from i and negates the Boolean value at i. For an observable f, its coordinate variation at i is

var⁡i(f)=sup⁡η∣f(flip⁡iη)−f(η)∣.\operatorname{var}_i(f)=\sup_{\eta}\left|f(\operatorname{flip}_i\eta)-f(\eta)\right|.vari​(f)=ηsup​∣f(flipi​η)−f(η)∣.

The domain used in the theorem is the full class of continuous observables for which ∑ i, var_i(f) is summable. This is a one-coordinate variation domain: it measures the effect of changing one spin, rather than exchanging two occupied sites.

For every site i, the flip rate c i is itself a continuous function of the configuration. Rates are nonnegative and uniformly bounded in the uniform norm. Their dependence on other coordinates is controlled by a second uniform bound: for each i, the series ∑ j, var_j(c i) is summable, with a bound independent of i. These are the two clauses of equation (3.24).

Formalization target

The pre-generator graph implements equation (3.25). For every pair (f,g) in that graph, f has summable coordinate variation and

g(η)=∑ici(η)(f(flip⁡iη)−f(η)).g(\eta)=\sum_i c_i(\eta)\bigl(f(\operatorname{flip}_i\eta)-f(\eta)\bigr).g(η)=i∑​ci​(η)(f(flipi​η)−f(η)).

The goal is Theorem 3.5 in full. It asserts that every function in the prescribed domain has a continuous image in the graph; the closure of the graph in the product uniform-norm topology is single-valued; and that closure is exactly the generator graph of a strongly continuous contraction semigroup. The semigroup is positive and preserves the constant function one, giving the conservative Feller conclusion used by the source.

The final clause retains the source's cylinder core. Restrict the initial graph to functions depending on a finite set of coordinates, expressed by the existence of a finite set F such that agreement on F forces equal function values. The closure of this restricted graph equals the full generator graph. Generation and the core are kept together because both are conclusions of the same theorem.

Significance of the result

The result turns an infinite formal sum of local moves into a closed, single-valued Markov generator. This is stronger than merely defining the pointwise series: it supplies the strongly continuous positive contraction evolution, conservativity, and the derivative characterization of the entire generator domain. The cylinder-core clause means that finite-coordinate observables are graph-norm dense enough to recover that generator, even though the state space and the total collection of possible flips are countable.

The theorem is already proved in the source. The formalization target is its precise Lean statement, including the infinite-site domain, the uniform influence hypothesis, generator closure, and core. The reusable infrastructure consists of the book-wide strongly continuous contraction-semigroup predicate and the mission-local flip, variation, and graph definitions.

Where the analytic difficulty lies

The naive finite-rate jump argument does not apply. A uniform bound on each individual rate does not bound the sum of rates over a countably infinite site set, so the system may have infinite total potential flip intensity. Pointwise notation for the generator also does not by itself show that its image is continuous or that its graph closure is single-valued. The coordinate-influence bound and summable-variation domain are therefore essential parts of the target rather than optional regularity decoration.

The neighboring exclusion-process theorem is not interchangeable with this one. A spin flip changes one coordinate and permits creation or destruction of occupation, whereas exclusion dynamics exchanges two coordinates and conserves particle number. Their domains and rate conditions are correspondingly different.

Formalization scope

The Lean statement allows empty, finite, and countably infinite S; it does not impose nonemptiness or finiteness. Bool is an exact two-state relabeling, not a restriction to a special numerical spin convention. spinVariation uses a real supremum over the nonempty compact configuration space. Explicit Summable hypotheses prevent divergent real tsum expressions from receiving an unintended default interpretation.

The operator graph uses the actual pointwise series and requires a continuous output. Closure is taken in C(S → Bool, ℝ) × C(S → Bool, ℝ). The semigroup is indexed by real time, but every law and bound uses nonnegative times; negative-time values carry no mathematical requirement. No finite-total-rate hypothesis, finite-site approximation, two-site exchange dynamics, or weakened core statement is admitted.

Selected references

  • Stewart N. Ethier and Thomas G. Kurtz, Markov Processes: Characterization and Convergence, Wiley, 1986, Chapter 1, Section 3; Chapter 4; Chapter 8, Section 3, Theorem 3.5, equations (3.24)--(3.25), printed p. 381. Wiley DOI
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Markov Processes: Characterization and Convergence 17: Nonlocal jump and Lévy generatorsTextbook

Why nonlocal generators matter

Markov processes with jumps model changes that cannot be represented by continuous diffusion paths: arrivals in queueing systems, sudden failures, population events, and discontinuous changes in financial or physical systems. Their infinitesimal descriptions are nonlocal generators, because the value of the operator at a state depends on test-function values at displaced states rather than only on derivatives at the current point. Chapter 8, Section 3 of Stewart N. Ethier and Thomas G. Kurtz, Markov Processes: Characterization and Convergence (Wiley, 1986), treats three complementary regimes. Theorem 3.1 covers finite-rate jumps on a general locally compact state space. Theorem 3.4 treats homogeneous Lévy operators on Euclidean space, including infinite jump activity and degenerate covariance. Theorem 3.3 gives the main target here: well-posedness for a time- and state-dependent compensated Lévy-type martingale problem.

These results connect concrete jump kernels and integro-differential operators to two standard descriptions of stochastic dynamics. Autonomous operators are realized as generators of conservative Feller semigroups, while time-dependent operators are characterized through martingale identities. Keeping all three source results in one mission records the nonlocal-generator theme without claiming that their distinct hypotheses imply one another.

The setting

For the Euclidean results, the state space is Rd\mathbb R^dRd, represented in Lean as EuclideanSpace ℝ (Fin d), with d>0d>0d>0. A covariance field a(t,x)a(t,x)a(t,x) is a continuous linear endomorphism, a drift field b(t,x)b(t,x)b(t,x) is a vector, and ν(t,x,dy)\nu(t,x,dy)ν(t,x,dy) is a measure of jump displacements. For a smooth compactly supported test function fff, the compensated Lévy-type operator is

Ltf(x)=12∑i,jaij(t,x) ∂ijf(x)+Df(x)[b(t,x)]+∫ ⁣(f(x+y)−f(x)−Df(x)[y]1+∥y∥2)ν(t,x,dy).L_t f(x)=\frac12\sum_{i,j}a_{ij}(t,x)\,\partial_{ij}f(x) +Df(x)[b(t,x)] +\int\!\left(f(x+y)-f(x)-\frac{Df(x)[y]}{1+\lVert y\rVert^2}\right)\nu(t,x,dy).Lt​f(x)=21​i,j∑​aij​(t,x)∂ij​f(x)+Df(x)[b(t,x)]+∫(f(x+y)−f(x)−1+∥y∥2Df(x)[y]​)ν(t,x,dy).

The denominator in the compensation term is part of the source convention. The covariance factor 1/21/21/2 applies only to the second-order term; the drift is unscaled. The weighted moment ∥y∥2/(1+∥y∥2)\lVert y\rVert^2/(1+\lVert y\rVert^2)∥y∥2/(1+∥y∥2) permits measures with infinite total mass while controlling the compensated integral.

A solution of the Lévy-type martingale problem is a jointly measurable process with the prescribed initial pushforward law whose integrated-generator increments have zero expectation against every bounded continuous function of any finite history. Smooth compactly supported functions are the spatial tests. This definition imposes no path-continuity requirement.

The finite-rate model uses a locally compact, noncompact, separable metric space EEE, a nonnegative rate λ(x)\lambda(x)λ(x), and a weakly continuous probability transition kernel μ(x,dy)\mu(x,dy)μ(x,dy). Its operator is Af(x)=λ(x)∫(f(y)−f(x))μ(x,dy)Af(x)=\lambda(x)\int(f(y)-f(x))\mu(x,dy)Af(x)=λ(x)∫(f(y)−f(x))μ(x,dy). Positive weights γ\gammaγ and η\etaη specify the graph domain and control behavior at infinity.

Formalization targets

Goal: nonautonomous Lévy-type well-posedness

The main target is Chapter 8, Section 3, Theorem 3.3. The covariance is continuous, symmetric, bounded, and strictly positive definite at every nonzero vector, without a uniform ellipticity constant. The drift is measurable and bounded. The weighted jump measure is integrable, and for every measurable set its weighted mass is a bounded continuous function of time and state.

For every initial probability measure, the conclusion asserts existence of a measurable-process solution on some probability space and uniqueness of all finite-dimensional distributions among every solution on every probability space. Setwise continuity is retained exactly; it is not replaced by weak convergence of measures or by finite total jump intensity.

Related target: homogeneous Lévy generation

Theorem 3.4 freezes the coefficients in time and space. The covariance may be degenerate but is symmetric and nonnegative, and the jump measure needs only the finite weighted integral. The full C^2\widehat C^2C2 graph consists of functions, first derivatives, and second derivatives that vanish at infinity. Its closure is the exact generator of a positive conservative strongly continuous contraction semigroup on C0(Rd)C_0(\mathbb R^d)C0​(Rd), and smooth compactly supported functions form a core.

Related target: finite-rate jump generation

Theorem 3.1 retains the general-state-space jump model. The transition kernel is both setwise measurable and weakly continuous; the rate and weights satisfy the source's vanishing and signed integral bounds. The weighted graph closes to a single-valued conservative Feller generator, and compactly supported continuous functions form a core.

Significance

The main theorem says that the displayed nonlocal characteristics determine stochastic dynamics in distribution even when the drift is only measurable and jump activity need not be finite. The two autonomous theorems identify concrete domains whose closures are genuine Feller generators, including positivity, contraction, strong continuity, conservativity, and core statements. Together they distinguish finite-rate kernels, homogeneous compensated Lévy dynamics, and nonautonomous Lévy-type dynamics while sharing the same generator language.

The formal contribution is a machine-checkable statement layer, not a proof claim. It exposes the exact compensation, weighted-integrability, graph-domain, semigroup, and finite-history conventions on which later proofs depend. The common diffusion operator, bounded-pointwise closure, and strongly continuous contraction-semigroup predicate are reused from earlier private missions in the same textbook series rather than duplicated under conflicting identifiers.

Where the difficulty lies

The obvious finite-jump approximation does not by itself preserve the full conclusions. Infinite jump activity requires compensation near zero, and convergence of the associated operators must still identify the intended martingale problem or the exact closed Feller generator. In the nonautonomous theorem, setwise continuity of weighted jump masses must coexist with merely measurable drift, while uniqueness ranges over arbitrary probability-space realizations and all finite-dimensional laws. Strengthening to continuous drift, imposing finite total jump intensity, assuming uniform ellipticity, or comparing only continuous-path solutions would materially weaken or alter the source theorem.

Formalization scope and conventions

Nonnegative real time is represented by ℝ≥0; Euclidean coordinates use Fin d. Fréchet derivatives express both gradient and Hessian terms. The jump measure is a measure of displacements yyy, so the operator evaluates f(x+y)f(x+y)f(x+y). Integrable hypotheses prevent Lean's totalized integral from silently assigning zero to a divergent positive weighted moment. Positive dimension is explicit through [NeZero d].

The martingale predicate includes empty finite histories and repeated observation times. Its bounded continuous history tests determine the same finite-dimensional identities used by the source, and no sample-path regularity is inserted. The autonomous graphs live in C0×C0C_0\times C_0C0​×C0​; bounded-pointwise closure means closure under uniformly bounded pointwise sequential limits, not ordinary norm closure. The finite-rate theorem preserves its restriction of the additional integrability clause to states with positive rate. No vacuous solution predicate, unweighted moment assumption, hidden nonzero-rate condition, or proof-only theorem dependency is introduced.

Selected references

  • Stewart N. Ethier and Thomas G. Kurtz, Markov Processes: Characterization and Convergence, Wiley, 1986, Chapter 8, Section 3, Theorems 3.1, 3.3, and 3.4. Wiley DOI
  • Stewart N. Ethier and Thomas G. Kurtz, same volume, Chapter 4, Sections 2–3 for Feller and martingale-problem conventions, and Appendix 3 for bounded-pointwise closure. Wiley DOI
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Markov Processes: Characterization and Convergence 16: Degenerate diffusion on a simplexTextbook

Why simplex diffusions matter

Finite-dimensional simplices are the natural state spaces for proportions: allele frequencies, population shares, and other collections of nonnegative coordinates whose total cannot exceed one. A diffusion on such a space must do more than solve an unconstrained stochastic equation. Its covariance degenerates on the boundary, and its drift must respect every face so that the process remains in the simplex. Chapter 8 of Ethier and Kurtz develops generator results for this setting as part of the analytic foundation for Markov-process models with constrained state spaces Ethier and Kurtz, Chapter 8, §2.

This mission formalizes their Theorem 2.8, a known generation theorem rather than an open conjecture. The theorem treats arbitrary Lipschitz drift satisfying the inward boundary inequalities. It identifies the closed diffusion graph as a Feller generator and also states that polynomial restrictions form a core. The generality of the drift distinguishes this result from later population-model applications with particular mutation or selection coefficients.

The simplex and its boundary

For a positive integer ddd, the simplex state space is

Kd={x∈Rd:xi≥0 for every i,∑i=1dxi≤1}.K_d=\left\{x\in\mathbb R^d: x_i\ge 0\ \text{for every }i, \quad \sum_{i=1}^d x_i\le 1\right\}.Kd​={x∈Rd:xi​≥0 for every i,i=1∑d​xi​≤1}.

The missing mass 1−∑ixi1-\sum_i x_i1−∑i​xi​ may be viewed as an additional coordinate. In Lean, WFState d is the subtype of functions Fin d → ℝ satisfying precisely nonnegativity and the upper bound on the coordinate sum. These conditions already imply xi≤1x_i\le 1xi​≤1 for every coordinate.

Let b:Kd→Rdb:K_d\to\mathbb R^db:Kd​→Rd be the drift. The boundary conditions say that bi(x)≥0b_i(x)\ge 0bi​(x)≥0 whenever xi=0x_i=0xi​=0, while ∑ibi(x)≤0\sum_i b_i(x)\le 0∑i​bi​(x)≤0 whenever ∑ixi=1\sum_i x_i=1∑i​xi​=1. Thus the drift cannot point outward through a coordinate face or through the top face. No mutation–selection formula or extra smoothness condition is imposed: global Lipschitz continuity and these face inequalities are the complete drift hypotheses retained here.

The operator and target theorem

The covariance matrix is

aij(x)=xi(δij−xj),a_{ij}(x)=x_i(\delta_{ij}-x_j),aij​(x)=xi​(δij​−xj​),

and the associated simplex diffusion operator is

Gf(x)=12∑i,jxi(δij−xj) ∂i∂jf(x)+∑ibi(x) ∂if(x).Gf(x)=\frac12\sum_{i,j}x_i(\delta_{ij}-x_j) \,\partial_i\partial_j f(x)+\sum_i b_i(x)\,\partial_i f(x).Gf(x)=21​i,j∑​xi​(δij​−xj​)∂i​∂j​f(x)+i∑​bi​(x)∂i​f(x).

Only the second-order sum is multiplied by 1/21/21/2. The covariance becomes singular on boundary faces, so this is not an immediate instance of a uniformly elliptic whole-space theorem.

The formal target asserts that the uniform graph closure of

{(f,Gf):f∈C2(Kd)}\{(f,Gf):f\in C^2(K_d)\}{(f,Gf):f∈C2(Kd​)}

is single-valued and is exactly the generator graph of a positive, conservative, strongly continuous contraction semigroup on C(Kd)C(K_d)C(Kd​). Conservativity is expressed by preservation of the constant function 111. The generator is identified by the right derivative at time zero, not merely by containment of a convenient operator restriction.

The final clause says that polynomials restricted to KdK_dKd​ are a core: closing the graph obtained from polynomial first coordinates gives the same full generator graph. This is a graph-closure statement and is stronger than uniform density of polynomials as functions.

What the result provides

Single-valuedness shows that the closed graph behaves as an operator rather than a multivalued relation. Generation supplies a Feller semigroup whose positivity and preservation of constants give the Markov interpretation. The exact generator biconditional fixes the full infinitesimal domain, while the polynomial-core conclusion permits generator questions to be reduced to algebraically structured test functions without changing the closed operator.

The source theorem is already proved in the book. The formalization task is to recover its generator statement and core conclusion in Lean with all boundary, closure, and semigroup conventions explicit. The current mission contributes a source-reviewed statement and its expression-level definitions; it does not claim a completed Lean proof.

Why the formalization is delicate

The obvious route through standard elliptic diffusion generation does not apply because a(x)a(x)a(x) degenerates as coordinates approach the boundary. It is also insufficient to prove only that the displayed differential operator is contained in some generator: the theorem identifies the closure of the entire C2(Kd)C^2(K_d)C2(Kd​) graph and separately asserts the polynomial core.

Boundary semantics create another source of possible weakening. Dropping either inward condition would permit outward drift at a face. Replacing the arbitrary Lipschitz drift by a special population-genetics formula would narrow the theorem. Replacing graph equality by inclusion, or polynomial graph density by ordinary function density, would lose a stated conclusion. These distinctions are all preserved in the target.

Formalization scope

The Lean development uses the book-wide namespace EthierKurtz. The compact space C(Kd)C(K_d)C(Kd​) is represented by real-valued bounded continuous functions on WFState d; compactness makes this the intended continuous-function space with the uniform norm. A C2(Kd)C^2(K_d)C2(Kd​) function is represented through a globally twice continuously differentiable extension on the ambient finite-coordinate space, following the book’s Appendix 6 extension convention for closed convex sets.

The operator uses Fréchet derivatives evaluated on coordinate vectors, which represent the first and second partial derivatives in the finite-dimensional ambient space. The graph is closed in the product uniform norm. IsStronglyContinuousContractionSemigroup records identity at zero, the nonnegative-time semigroup law, contraction, and strong right continuity at zero. The target additionally records positivity, preservation of one, and equality between its derivative graph and the closed diffusion graph.

The scope excludes the zero-dimensional case, as required by 0 < d. It does not introduce a continuous-path hypothesis, a special drift parameterization, or uniform ellipticity. The only packaged declarations beyond the goal are the state space, operator, graph, and the already published semigroup predicate needed to state it. Proof-only lemmas and unrelated Chapter 8 results are outside this mission.

Selected references

  • Stewart N. Ethier and Thomas G. Kurtz, Markov Processes: Characterization and Convergence, Wiley, 1986, Chapter 8, §2, Theorem 2.8, printed p. 375; equation (1.15), printed p. 368; Appendix 6, printed pp. 499–500. DOI
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Markov Processes: Characterization and Convergence 14: One-dimensional boundary classificationTextbook

Why endpoint classification matters

A one-dimensional diffusion is governed in the interior by a second-order differential operator, but the interior coefficients alone do not determine what happens when the process approaches the edge of its state space. An endpoint may be reachable from the interior or inaccessible; after arrival it may absorb, reflect, or retain the process according to a boundary parameter. The same issue persists when an endpoint is infinite. Chapter 8 of Stewart N. Ethier and Thomas G. Kurtz, Markov Processes: Characterization and Convergence (Wiley, 1986), organizes these alternatives through scale and speed integrals and identifies the exact operator domain that generates the corresponding Feller evolution. This mission formalizes Chapter 8, Section 1, Theorem 1.1, printed page 367.

The setting

Let −∞≤r0<r1≤∞-\infty\le r_0<r_1\le\infty−∞≤r0​<r1​≤∞. The real state interval is I=[r0,r1]∩RI=[r_0,r_1]\cap\mathbb RI=[r0​,r1​]∩R, its interior is I∘=(r0,r1)I^\circ=(r_0,r_1)I∘=(r0​,r1​), and Iˉ\bar IIˉ is the closed interval in the extended real line. A function in C(Iˉ)C(\bar I)C(Iˉ) is represented by a continuous function on that compact extended interval, so finite endpoint limits are part of the object even when an endpoint is infinite.

The interior diffusion operator is

Gf(x)=a(x)2f′′(x)+b(x)f′(x),Gf(x)=\frac{a(x)}2 f''(x)+b(x)f'(x),Gf(x)=2a(x)​f′′(x)+b(x)f′(x),

where aaa and bbb are continuous on I∘I^\circI∘ and a(x)>0a(x)>0a(x)>0 there. Choose an interior reference point rrr. Define

B(x)=∫rx2b(y)a(y) dy,p(x)=∫rxe−B(y) dy,m(x)=∫rx2eB(y)a(y) dy.B(x)=\int_r^x \frac{2b(y)}{a(y)}\,dy, \qquad p(x)=\int_r^x e^{-B(y)}\,dy, \qquad m(x)=\int_r^x \frac{2e^{B(y)}}{a(y)}\,dy.B(x)=∫rx​a(y)2b(y)​dy,p(x)=∫rx​e−B(y)dy,m(x)=∫rx​a(y)2eB(y)​dy.

The corresponding endpoint tests uuu and vvv are nonnegative extended-real integrals. Their values may be +∞+\infty+∞; preserving that possibility is essential because the four boundary classes are distinguished precisely by which of the two tests are finite.

Formalization target

Theorem 1.1 — one-dimensional boundary diffusion generation

At either endpoint, the pair (u,v)(u,v)(u,v) gives the Feller boundary class:

classuvregular<∞<∞exit<∞=∞entrance=∞<∞natural=∞=∞.\begin{array}{c|cc} \text{class} & u & v\\ \hline \text{regular} & <\infty & <\infty\\ \text{exit} & <\infty & =\infty\\ \text{entrance} & =\infty & <\infty\\ \text{natural} & =\infty & =\infty. \end{array}classregularexitentrancenatural​u<∞<∞=∞=∞​v<∞=∞<∞=∞.​​

Entrance and natural endpoints are inaccessible, so the generator domain imposes no boundary equation there. At an exit endpoint the limiting generator value must be zero. At a regular endpoint rir_iri​, a parameter qi∈[0,1]q_i\in[0,1]qi​∈[0,1] determines the boundary condition

qilim⁡x→riGf(x)=(−1)i(1−qi)lim⁡x→rieB(x)f′(x).q_i\lim_{x\to r_i}Gf(x) =(-1)^i(1-q_i)\lim_{x\to r_i}e^{B(x)}f'(x).qi​x→ri​lim​Gf(x)=(−1)i(1−qi​)x→ri​lim​eB(x)f′(x).

The target states that the graph consisting of f∈C(Iˉ)f\in C(\bar I)f∈C(Iˉ) that are twice continuously differentiable in the interior, whose GfGfGf extends continuously to Iˉ\bar IIˉ, and that satisfy the applicable condition at both endpoints is exactly the infinitesimal generator of a Feller semigroup on C(Iˉ)C(\bar I)C(Iˉ). The conclusion includes the semigroup law, contraction, strong right continuity at zero, positivity, preservation of the constant function 111, and a biconditional identifying the complete generator graph rather than merely an included core or its closure.

Significance

The theorem translates local coefficients into a global Markov evolution while retaining every possible finite or infinite endpoint type. The endpoint tests determine which boundary behavior is available, and the regular-boundary parameter records absorbing, reflecting, and intermediate behavior in one equation. Without the classification, writing down the differential expression does not specify a unique Feller generator because distinct domains can encode different stochastic behavior at the same endpoint.

The formal contribution is a machine-checkable statement layer for the source theorem. It makes the compactified state space, improper endpoint integrals, one-sided endpoint filters, and exact generator graph explicit. The theorem itself remains an open proof obligation in this statement-only mission. The definitions can also support later formal work on hitting distributions, killed or reflected diffusions, and comparison of boundary regimes.

Where the difficulty lies

The main difficulty is that the classification cannot be reduced to ordinary finite integrals or to boundary values at finite real points. Infinite endpoints and divergent scale or speed tests carry mathematical information; replacing extended-real integrals by totalized real integrals would collapse boundary classes. A second difficulty is identifying the full closed generator domain. Showing that the differential expression is meaningful on smooth interior functions is insufficient: the proof must connect its endpoint asymptotics to positivity, conservativity, strong continuity, and exact generation on the uniform-norm space.

Formalization scope and conventions

Endpoints use EReal, and the state space is Set.Icc r₀ r₁ in the extended line. Coefficients are constrained only on the open real interior; no boundedness or uniform ellipticity is added. The drift primitive and scale/speed tests use oriented interval integrals internally and ENNReal endpoint integrals externally, retaining +∞+\infty+∞. Absolute values correct the orientation on the left of the reference point.

The graph stores continuous endpoint extensions of both fff and GfGfGf. Interior C2C^2C2 regularity is expressed by ContDiffOn ℝ 2, and endpoint limits use the one-sided neighborhood filter induced from the extended interval. The regular parameter is required to lie in [0,1][0,1][0,1] only when both boundary tests are finite. The mission does not replace the four cases by an opaque classifier, assume finite endpoints, add a pathwise stochastic differential equation, or weaken exact generation to graph inclusion. The shared book definition of a strongly continuous contraction semigroup is reused from the earlier semigroup-generation mission rather than redeclared.

Selected references

  • Stewart N. Ethier and Thomas G. Kurtz, Markov Processes: Characterization and Convergence, Wiley, 1986, Chapter 8, Section 1, Theorem 1.1 and equations (1.1)–(1.11), printed pp. 366–367. Wiley DOI
  • Stewart N. Ethier and Thomas G. Kurtz, same volume, Chapter 4, printed p. 166, for the Feller semigroup convention used in the conclusion. Wiley DOI
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Markov Processes: Characterization and Convergence 13: Whole-space diffusion generatorsTextbook

Why whole-space diffusion generators matter

Diffusion processes connect stochastic differential equations, partial differential equations, and Markov semigroups. On Euclidean space, their local behavior is encoded by a second-order operator built from a covariance field and a drift field. A central question is whether those local coefficients determine an actual Markov evolution, and whether the resulting evolution is unique. Ethier and Kurtz organize these questions through generator graphs and martingale problems, which allow the same language to cover smooth elliptic diffusions, degenerate models, and coefficients that vary measurably with time. This mission formalizes three complementary whole-space regimes from Chapter 8 of Stewart N. Ethier and Thomas G. Kurtz, Markov Processes: Characterization and Convergence (Wiley, 1986), principally Theorems 1.6, 1.7, and 2.5.

The setting

The state space is the finite-dimensional Euclidean space Rd\mathbb R^dRd, represented in Lean as EuclideanSpace ℝ (Fin d), with d>0d>0d>0. A covariance operator a(t,x)a(t,x)a(t,x) is a continuous linear endomorphism of this space, while a drift b(t,x)b(t,x)b(t,x) is a vector. For a smooth scalar test function fff, the diffusion operator is

Gtf(x)=12∑i,jaij(t,x) ∂ijf(x)+Df(x)[b(t,x)].G_t f(x)=\frac12\sum_{i,j} a_{ij}(t,x)\,\partial_{ij}f(x) + Df(x)[b(t,x)].Gt​f(x)=21​i,j∑​aij​(t,x)∂ij​f(x)+Df(x)[b(t,x)].

The factor 1/21/21/2 multiplies only the covariance-weighted second-order term. The formalization uses Fréchet derivatives evaluated in the standard coordinate directions. In the time-homogeneous cases, the smooth compactly supported graph consists of pairs (f,Gf)(f,Gf)(f,Gf) viewed in C0(Rd)×C0(Rd)C_0(\mathbb R^d)\times C_0(\mathbb R^d)C0​(Rd)×C0​(Rd), and its uniform closure is the candidate generator.

For time-dependent coefficients, a measurable process solves the time-inhomogeneous martingale problem when its initial pushforward law is prescribed and the integrated generator identity holds against every smooth compactly supported spatial test and every bounded continuous finite-history test. This formulation records the natural-past moment identities without imposing continuity of sample paths as an extra hypothesis.

Formalization targets

Goal: measurable-drift nonautonomous well-posedness

The main target is Chapter 8, Section 1, Theorem 1.7. The covariance and drift are jointly Borel measurable and locally bounded. The covariance is symmetric and nonnegative. At each fixed spatial point it is uniformly elliptic over every bounded positive time interval, and its spatial continuity is uniform over that interval. A common quadratic bound controls the covariance norm and the one-sided radial drift quantity ⟨x,b(t,x)⟩\langle x,b(t,x)\rangle⟨x,b(t,x)⟩.

For every initial probability measure, the conclusion asserts existence of a measurable-process solution on some probability space and uniqueness of all finite-dimensional distributions among every such solution on any probability space. The drift is not assumed continuous, and no stronger norm-growth condition on the drift or moment condition on the initial law is inserted.

Related target: uniformly elliptic Feller generation

Chapter 8, Section 1, Theorem 1.6 treats bounded Hölder continuous time-homogeneous coefficients with symmetric, globally uniformly elliptic covariance. It concludes that the closure of the smooth compactly supported graph is single-valued and is exactly the generator of a positive, strongly continuous contraction semigroup on C0(Rd)C_0(\mathbb R^d)C0​(Rd). Conservativity is retained through membership of the constant graph pair (1,0)(1,0)(1,0) in the bounded-pointwise closure.

Related target: degenerate smooth-core generation

Chapter 8, Section 2, Theorem 2.5 permits degenerate and unbounded covariance fields. Its assumptions are symmetry, nonnegativity, twice continuous differentiability of the matrix entries, bounded second partial derivatives, and a globally Lipschitz drift. Its conclusion is the same full Feller generation and conservativity statement. This regime is related to, but not implied by, the bounded uniformly elliptic regime.

Significance

Together the three statements separate distinct mechanisms for obtaining Markov dynamics from local diffusion data. The two autonomous theorems identify when a concrete smooth core closes to a Feller generator, including positivity, contraction, strong continuity, and conservativity. The nonautonomous theorem establishes existence and uniqueness in distribution under substantially rougher temporal behavior and merely measurable drift. Keeping the regimes together exposes the common operator while preserving their incompatible regularity hypotheses.

The formal contribution is a machine-checkable statement layer for these source results and their expression-essential definitions. It does not claim proofs of the theorems. The definitions make explicit the coordinate form of the generator, the C0C_0C0​ graph, the bounded-pointwise closure convention, and the complete finite-history martingale identities. These components can support later formal proofs and other diffusion or martingale-problem developments.

Where the difficulty lies

The source conclusions are not consequences of a single elementary continuity argument. In the Feller cases, identifying the closure of a graph with the generator requires simultaneous control of the operator domain, the semigroup properties, positivity, and conservativity. In the time-dependent case, measurability of the drift is deliberately weaker than continuity, while uniqueness must cover all measurable-process realizations and all finite collections of observation times. Replacing that conclusion by uniqueness only among continuous processes, or strengthening the drift hypotheses until a standard smooth theory applies, would change the theorem.

Formalization scope and conventions

The development uses nonnegative real time and finite-dimensional real Euclidean space. Covariance matrices act as continuous linear maps; their entries are recovered in the standard orthonormal basis. Smoothness is expressed with ContDiff, compact support with HasCompactSupport, and autonomous generator graphs in C₀. The bounded-pointwise closure is the smallest set closed under uniformly bounded pointwise sequential limits, not merely the set of one-step limits.

The martingale-problem predicate requires joint measurability of the process, equality of the initial pushforward measure, and all bounded continuous finite-history identities. Empty histories and repeated observation times are included. The goal compares the complete finite-dimensional laws of any two solutions. No vacuous solution predicate, arbitrary extension of the generator, chosen matrix square root, hidden path-continuity assumption, or proof-only theorem dependency is used.

Selected references

  • Stewart N. Ethier and Thomas G. Kurtz, Markov Processes: Characterization and Convergence, Wiley, 1986, Chapter 8, Theorems 1.6, 1.7, and 2.5. Wiley DOI
  • Stewart N. Ethier and Thomas G. Kurtz, same volume, Chapter 4 for martingale-problem well-posedness and Feller conventions, and Appendix 3 for bounded-pointwise closure. Wiley DOI
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Markov Processes: Characterization and Convergence 11: Stationary-sequence invariance principlesTextbook

Why stationary dependence matters

Classical central limit theorems begin with independent observations. Many stochastic models instead produce observations whose dependence persists across time: measurements from an equilibrium process, functions of a stationary Markov chain, and noise sequences in time-series models are standard examples. For such data, the variance of a long sum contains covariance terms from every lag, and independence cannot be used to discard them. Chapter 7, Section 3 of Stewart N. Ethier and Thomas G. Kurtz, Markov Processes: Characterization and Convergence (Wiley, 1986), gives a functional central limit theorem under a quantitative mixing condition. The conclusion is stronger than convergence of one normalized sum: the whole partial-sum path converges to Brownian motion.

Stationary sequences and mixing

Fix a probability space (Ω,F,P)(\Omega,\mathcal F,P)(Ω,F,P) and a two-sided real sequence (Yk)k∈Z(Y_k)_{k\in\mathbb Z}(Yk​)k∈Z​. Strict stationarity means that shifting every integer index by the same amount leaves the joint law of the entire sequence unchanged. Each YkY_kYk​ is measurable and centered, so E[Yk]=0E[Y_k]=0E[Yk​]=0.

For a nonnegative lag mmm, let the past be the sigma-algebra generated by all YkY_kYk​ with k≤0k\le 0k≤0, and let the future be generated by all YkY_kYk​ with k≥mk\ge mk≥m. For p≥1p\ge 1p≥1, the book's LpL^pLp mixing coefficient φp(m)\varphi_p(m)φp​(m) is the supremum, over future events AAA, of

∥P(A∣past)−P(A)∥p.\left\|P(A\mid\text{past})-P(A)\right\|_p.∥P(A∣past)−P(A)∥p​.

Thus φp(m)\varphi_p(m)φp​(m) measures how far events at least mmm time units in the future remain from being independent of the complete past. The Lean definition constructs both coordinate-generated sigma-algebras explicitly and represents conditional probability as the conditional expectation of an indicator.

Formalization target

For n≥1n\ge 1n≥1, define the scaled partial-sum process

Xn(t)=1n∑k=1⌊nt⌋Yk,t≥0.X_n(t)=\frac{1}{\sqrt n}\sum_{k=1}^{\lfloor nt\rfloor}Y_k, \qquad t\ge 0.Xn​(t)=n​1​k=1∑⌊nt⌋​Yk​,t≥0.

The Lean sequence uses the index n+1n+1n+1 because Lean's natural numbers begin at zero; this is only a reindexing of the same positive scaling sequence. Suppose there is δ>0\delta>0δ>0 such that every coordinate has a finite (2+δ)(2+\delta)(2+δ) moment. Set

p=2+δ1+δ,∑m=0∞φp(m)δ/(1+δ)<∞.p=\frac{2+\delta}{1+\delta}, \qquad \sum_{m=0}^{\infty}\varphi_p(m)^{\delta/(1+\delta)}<\infty.p=1+δ2+δ​,m=0∑∞​φp​(m)δ/(1+δ)<∞.

The target is Theorem 3.1: the ordered covariance series converges and

σ2=E[Y12]+2∑k=2∞E[Y1Yk]\sigma^2=E[Y_1^2]+2\sum_{k=2}^{\infty}E[Y_1Y_k]σ2=E[Y12​]+2k=2∑∞​E[Y1​Yk​]

is nonnegative, while XnX_nXn​ converges to centered Brownian motion with variance parameter σ2\sigma^2σ2. The variance is allowed to be zero. The covariance sum is encoded as convergence of its ordered partial sums, not as the stronger and unrequested assertion of absolute summability.

What the conclusion provides

The result identifies the macroscopic fluctuation process of a stationary dependent sequence. It supplies both the long-run variance, including every lag covariance, and a Brownian path limit. Consequently, continuous functionals of the accumulated process can be studied through the limiting Brownian motion rather than only through one-time normal approximations.

The formal statement preserves the book's functional interpretation. ConvergesToContinuousGaussian records the complete prelimit path laws, centered Gaussian finite-dimensional laws with covariance σ2min⁡(s,t)\sigma^2\min(s,t)σ2min(s,t), and convergence to a continuous limit through a common realization. This avoids weakening the theorem to convergence of a single terminal sum or to separate finite-dimensional marginals. The declaration is a statement-only formalization: the theorem remains an open Lean goal, while the mixing coefficient and partial-sum process are concrete definitions.

Where the difficulty lies

The usual independent-sum argument does not apply because blocks of observations are not independent and their covariance terms need not vanish. Merely showing that dependence becomes small at large lags is insufficient: the decay must interact with the available (2+δ)(2+\delta)(2+δ) moment so that the total contribution of distant dependence is summable. A scalar central limit theorem would also leave tightness of the path sequence unresolved. The theorem packages both issues into the summability condition on the precise LpL^pLp coefficient and concludes a path-level Brownian limit.

Formalization scope and conventions

The formalization uses a two-sided sequence indexed by Z\mathbb ZZ, matching the source's convenient stationary extension. Stationarity is equality of the laws of the whole shifted and unshifted sequence, which entails every finite-dimensional shift identity without adding Markov or independence assumptions. The probability measure is explicit, and every coordinate has an explicit measurability hypothesis.

stationaryLpMixing uses the past through zero and the future beginning at lag mmm. Its codomain is the extended nonnegative reals, so an infinite norm or supremum is not silently totalized to an ordinary real. The summability hypothesis is an extended-real infinite sum strictly below infinity. stationaryPartialSums embeds the real sum in one-dimensional Euclidean space so it can reuse the book-wide continuous-Gaussian path-convergence definition. The exact floor, positive indexing, square-root normalization, covariance order, and degenerate zero-variance case are retained. No interpolation, absolute covariance summability, positive-variance assumption, Markov property, or independence condition is introduced.

The expression-essential infrastructure consists of the two definitions introduced here and the compatible book-wide ConvergesToContinuousGaussian definition already staged for the preceding diffusion-limit mission. The latter is imported rather than duplicated under a conflicting name. Useful future work includes proving the theorem from martingale approximation and developing reusable results relating concrete mixing bounds to the required summability hypothesis.

Selected references

  • Stewart N. Ethier and Thomas G. Kurtz, Markov Processes: Characterization and Convergence, Wiley, 1986, Chapter 7, Section 3, Theorem 3.1, printed pp. 350–351; mixing convention in Section 2, printed pp. 345–346. Wiley DOI
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Markov Processes: Characterization and Convergence 10: Martingale and state-dependent diffusion limitsTextbook

Why diffusion limits matter

Many stochastic models are built from small random changes occurring at high frequency. Queue lengths, population counts, particle systems, and numerical schemes may be discrete or have jumps at every finite scale, yet their large-scale behavior is often described by a continuous diffusion. A diffusion approximation replaces the detailed microscopic model by a process whose drift and covariance depend on its current state. This can make asymptotic probabilities and qualitative behavior accessible without claiming that the original model itself has continuous paths.

Chapter 7 of Stewart N. Ethier and Thomas G. Kurtz, Markov Processes: Characterization and Convergence, develops general limit theorems for this passage. The retained results in this mission are Theorem 1.4, a martingale functional central limit theorem with deterministic covariance, and Theorem 4.1, a state-dependent diffusion approximation from localized characteristics. They are related limit regimes, but the former is not presented here as a literal specialization of the latter: its covariance may vary deterministically with time, whereas the state-dependent theorem uses time-homogeneous coefficient fields evaluated along the evolving state.

The probabilistic setting

A càdlàg process is right-continuous and has a finite left limit at every positive time. For each index nnn, the state process XnX_nXn​ and its finite-variation characteristic BnB_nBn​ have càdlàg paths in Rd\mathbb R^dRd. A symmetric matrix process AnA_nAn​ has càdlàg entries and positive-semidefinite increments. The natural filtration records the histories of XnX_nXn​, BnB_nBn​, and AnA_nAn​ jointly.

The centered process Mn=Xn−BnM_n=X_n-B_nMn​=Xn​−Bn​ is required to be a local martingale coordinatewise. Its quadratic characteristic is represented by requiring every product

MniMnj−AnijM_n^i M_n^j-A_n^{ij}Mni​Mnj​−Anij​

to be a local martingale as well. These conditions identify BnB_nBn​ as the approximate drift and AnA_nAn​ as the approximate covariance accumulation. They do not impose independence of the coordinates or of the prelimit processes.

Localization uses the first time τnr\tau_n^rτnr​ at which either the current value Xn(t)X_n(t)Xn​(t) or its left limit Xn(t−)X_n(t-)Xn​(t−) reaches radius rrr. The jump and characteristic conditions are checked only up to T∧τnrT\wedge\tau_n^rT∧τnr​, for each radius r>0r>0r>0 and time horizon T>0T>0T>0. This is essential when coefficients are controlled locally but not globally.

Formalization targets

State-dependent diffusion approximation

Let a(x)a(x)a(x) be a continuous symmetric positive-semidefinite matrix field and let b(x)b(x)b(x) be a continuous vector field. For smooth compactly supported fff, define

Gf(x)=12∑i,jaij(x) ∂i∂jf(x)+∑ibi(x) ∂if(x).Gf(x)=\frac12\sum_{i,j}a_{ij}(x)\,\partial_i\partial_jf(x) +\sum_i b_i(x)\,\partial_i f(x).Gf(x)=21​i,j∑​aij​(x)∂i​∂j​f(x)+i∑​bi​(x)∂i​f(x).

Assume the continuous-path martingale problem for this operator is well posed for every initial probability law. The goal states that if the stopped squared jumps of XnX_nXn​ and BnB_nBn​ vanish in expected supremum, the stopped first-power jumps of each AnijA_n^{ij}Anij​ vanish, and the stopped characteristics converge in probability to

∫0tbi(Xn(s)) dsand∫0taij(Xn(s)) ds,\int_0^t b_i(X_n(s))\,ds \quad\text{and}\quad \int_0^t a_{ij}(X_n(s))\,ds,∫0t​bi​(Xn​(s))dsand∫0t​aij​(Xn​(s))ds,

then weak convergence of the initial laws implies convergence of the complete path laws to the unique continuous diffusion law.

Martingale functional central limit theorem

The retained milestone treats vector local martingales with deterministic limiting covariance C(t)C(t)C(t). It preserves both alternatives in the source: either first-power martingale jumps vanish and AnA_nAn​ is the actual cross variation, or the jumps of AnA_nAn​ and the squared jumps of the martingale vanish while MniMnj−AnijM_n^iM_n^j-A_n^{ij}Mni​Mnj​−Anij​ is locally martingale. Pointwise convergence in probability of Anij(t)A_n^{ij}(t)Anij​(t) to Cij(t)C_{ij}(t)Cij​(t) then yields the centered continuous Gaussian limit with covariance C(min⁡(s,t))C(\min(s,t))C(min(s,t)).

Significance

The state-dependent theorem packages a common diffusion-limit argument into conditions on observable local characteristics. It separates model-specific work—identifying the drift, covariance, localization, and jump bounds—from the general conclusion that the entire trajectory converges. The martingale theorem records the important deterministic-covariance regime without erasing either of its two source alternatives.

For formalization, the mission provides concrete predicates for càdlàg paths, stopped maximum jumps, localized characteristic discrepancies, the diffusion generator, continuous martingale-problem laws, and Gaussian process convergence. The result is statement-only: the theorem bodies remain open with sorry, while every expression dependency is a concrete definition. No theorem proof, adapter-equivalence proof, or claim of completed formal verification is included.

Where the difficulty lies

Finite-dimensional convergence alone does not control whole trajectories. The central obstacle is simultaneous control of oscillations, jumps, and characteristics after localization. A naive argument that replaces BnB_nBn​ and AnA_nAn​ by their limiting integrals pointwise misses the uniform stopped discrepancies and does not justify tightness of path laws. Likewise, ignoring the left limit in the exit rule can miss a jump that crosses the localization boundary.

Well-posedness is also substantive. Identifying every subsequential limit with a solution of the martingale problem gives uniqueness only when that problem is well posed for the relevant initial law. The formal statement therefore retains existence and uniqueness for every initial probability law rather than silently assuming a distinguished solution.

Formalization scope

Time is nonnegative and the sequence is indexed from zero rather than one. Expectations of jump suprema take values in R≥0∪{∞}\mathbb R_{\ge0}\cup\{\infty\}R≥0​∪{∞}, so no unmentioned integrability assumption is introduced. Matrix positivity is Matrix.PosSemidef, which includes the real symmetric positive-semidefinite condition used by the source. The exit time includes both the current value and the positive-time left limit, and an empty exit set gives infinity.

The diffusion law uses continuous canonical paths, smooth compactly supported tests, and bounded measurable functions of finitely many past states to express the natural-filtration martingale identities. Full process convergence is encoded by a joint realization that preserves every complete prelimit path law and converges almost surely uniformly on each compact interval to a continuous limit. This is the source-reviewed continuous-limit Skorohod representation convention, not merely convergence of finitely many observations.

The two shared definitions EthierKurtz.IsSourceLocalMartingale and EthierKurtz.HasCrossVariation are imported from the earlier book-wide stochastic-calculus package. All other definitions needed to state these two results are included here. Contributions should preserve the localization quantifiers, both central-limit jump alternatives, the full martingale-problem well-posedness hypothesis, and the complete path-law conclusions.

Selected references

  • Stewart N. Ethier and Thomas G. Kurtz, Markov Processes: Characterization and Convergence, Wiley, 1986, Chapter 7, Sections 1 and 4, Theorems 1.4 and 4.1. Wiley digital edition
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Markov Processes: Characterization and Convergence 09: Brownian stochastic equations: existence and uniquenessTextbook

Brownian equations as models of evolving systems

A Brownian stochastic equation describes a state that changes through a deterministic drift and random fluctuations. Such equations are basic models for diffusions and connect probabilistic sample paths with analytic operators. Chapter 5, Section 3 of Stewart Ethier and Thomas Kurtz's Markov Processes: Characterization and Convergence develops this connection in both directions and then separates three questions: whether a solution exists, whether it is unique when driven by fixed noise, and whether all solutions have the same distribution. The mission records four central results from that section as one coherent formalization target. The principal goal is the fixed-driver existence theorem, Theorem 3.11. Theorems 3.3, 3.6, and 3.10 retain the representation, uniqueness, and weak-existence variants without treating one as a consequence of another.

State space, coefficients, and solutions

Fix a dimension ddd. The state space is the Euclidean space Rd\mathbb R^dRd, represented in Lean as EuclideanSpace ℝ (Fin d). A diffusion coefficient

σ:[0,∞)×Rd⟶Rd×d\sigma:[0,\infty)\times\mathbb R^d\longrightarrow\mathbb R^{d\times d}σ:[0,∞)×Rd⟶Rd×d

controls the random fluctuations, and a drift coefficient

b:[0,∞)×Rd⟶Rdb:[0,\infty)\times\mathbb R^d\longrightarrow\mathbb R^db:[0,∞)×Rd⟶Rd

controls the finite-variation part. Given a ddd-dimensional Brownian motion WWW and initial state ξ\xiξ, a solution XXX satisfies, componentwise,

X(t)=X(0)+∫0tσ(s,X(s)) dW(s)+∫0tb(s,X(s)) ds.X(t)=X(0)+\int_0^t \sigma(s,X(s))\,dW(s)+\int_0^t b(s,X(s))\,ds.X(t)=X(0)+∫0t​σ(s,X(s))dW(s)+∫0t​b(s,X(s))ds.

The formal statement does not postulate an opaque stochastic-integral operator. The predicate HasBrownianItoIntegral uses bounded predictable dyadic step approximations, integrated squared-error convergence in probability, and convergence in probability of the corresponding stochastic sums. SolvesBrownianSDE requires continuous paths, adaptation to the completed natural past of WWW and ξ\xiξ, integrability of the drift, and one almost-sure equation holding for every time and coordinate.

A weak solution may choose its probability space, filtration, and Brownian driver. Its Brownian future increments are independent of the entire filtration past, its state process is adapted after completion, and its initial distribution is prescribed. Pathwise uniqueness compares two solutions on the same space with the same filtration and driver. Distribution uniqueness compares solutions that may live on different spaces and asks for equality of their whole coordinate-path laws.

Formalization targets

Theorem 3.3: martingale-problem representation

For locally bounded Borel coefficients, a given continuous solution of the diffusion martingale problem can be lifted to the completed product with an auxiliary Brownian space. On that specific extension there exists a Brownian motion making the lifted original process a weak solution of the stochastic equation. The generator is

Gf(t,x)=12∑i,j(σσT)ij(t,x) ∂i∂jf(x)+∑ibi(t,x) ∂if(x).Gf(t,x)=\frac12\sum_{i,j}(\sigma\sigma^{\mathsf T})_{ij}(t,x)\,\partial_i\partial_j f(x)+\sum_i b_i(t,x)\,\partial_i f(x).Gf(t,x)=21​i,j∑​(σσT)ij​(t,x)∂i​∂j​f(x)+i∑​bi​(t,x)∂i​f(x).

This target retains the factor 1/21/21/2, the complete drift term, possibly singular diffusion matrices, the given process, and the exact completed product filtration.

Theorem 3.6: uniqueness implication

For locally bounded Borel σ\sigmaσ and bbb and any initial probability law μ\muμ, pathwise uniqueness implies uniqueness in distribution. No existence, Lipschitz, ellipticity, or moment assumption is added.

Theorem 3.10: weak existence

When both coefficients are continuous and a constant KKK satisfies

∥σ(t,x)∥2≤K(1+∥x∥2),x⋅b(t,x)≤K(1+∥x∥2),\lVert\sigma(t,x)\rVert^2\le K(1+\lVert x\rVert^2),\qquad x\cdot b(t,x)\le K(1+\lVert x\rVert^2),∥σ(t,x)∥2≤K(1+∥x∥2),x⋅b(t,x)≤K(1+∥x∥2),

there is a weak solution for every initial probability law. The drift hypothesis is one-sided and does not bound ∥b(t,x)∥\lVert b(t,x)\rVert∥b(t,x)∥.

Theorem 3.11: strong existence on fixed noise

The main goal assumes locally bounded Borel coefficients, the preceding one-sided growth condition locally in time, and local Lipschitz control on each bounded state ball. For every Brownian motion WWW and every independent square-integrable initial variable ξ\xiξ already given on a probability space, there exists XXX solving the equation with respect to the completed natural past of WWW and ξ\xiξ. The quantifier order preserves the fixed driver and original probability space.

Why these results matter

The representation theorem connects the analytic martingale problem with the pathwise stochastic-integral formulation while preserving a given process on a prescribed extension. The uniqueness theorem explains when the apparently stronger same-noise comparison controls the law of arbitrary weak solutions. The weak-existence theorem supplies solutions under continuity and one-sided growth without local Lipschitz assumptions. The strong-existence theorem supplies a solution driven by noise and initial data that are fixed in advance, under local Lipschitz regularity.

Formalizing the group creates reusable definitions for completed filtrations, Brownian drivers, local Itô integration, weak solutions, pathwise uniqueness, and time-dependent diffusion generators. The source results are classical theorems, and this proposal records their reviewed Lean statements as open proof obligations. It does not claim machine-checked proofs.

Main formalization difficulty

The central difficulty is keeping the probabilistic quantifiers and filtrations exact. Replacing the local stochastic integral by an unconstrained witness would make the equation too weak. Replacing weak existence by existence on a fixed space would make Theorem 3.10 too strong. Conversely, existentially choosing a new driver in Theorem 3.11 would lose its fixed-noise content. The representation theorem also cannot be reduced to equality in law: it must retain the original process through first projection and use the completed product past specified in the source.

Formalization scope

Time is ℝ≥0, states are finite-dimensional real Euclidean spaces, and diffusion matrices use the Frobenius norm. Brownian motion is represented by independent scalar Brownian coordinates with measurable evaluations and continuous paths. Completion adds every subset of an ambient measurable null set. The local Itô relation uses left-endpoint dyadic step functions, interval integrability, and convergence in probability. Equality of path laws is expressed on the coordinate function space; for continuous Euclidean paths this matches the usual continuous-path law.

The main theorem keeps Borel measurability, compact-set local boundedness, one-sided drift growth, squared diffusion growth, local Lipschitz bounds, independence of ξ\xiξ and WWW, and the second moment of ξ\xiξ. The weak theorem keeps continuity and an arbitrary initial law. The representation target keeps compactly supported smooth tests and the exact covariance contraction. These conditions rule out vacuous solution predicates and default-valued integrals. Contributions may prove the four theorem statements or establish reusable lemmas for the concrete integral, completion, martingale, and path-law infrastructure.

Selected references

  • Stewart N. Ethier and Thomas G. Kurtz, Markov Processes: Characterization and Convergence, Wiley, 1986, Chapter 5, Section 3, Theorems 3.3, 3.6, 3.10, and 3.11. Wiley
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Markov Processes: Characterization and Convergence 08: Change of variables for continuous semimartingalesTextbook

Motivation

A continuous stochastic process may combine a finite-variation drift with a local martingale fluctuation. To understand a function of that process, one needs a change-of-variables rule that accounts for both parts and for their quadratic covariation. The ordinary chain rule has no term for covariation. The result here is the time-dependent, multidimensional Itô formula in Stewart N. Ethier and Thomas G. Kurtz, Markov Processes: Characterization and Convergence (Wiley, 1986), Chapter 5, Section 2, Theorem 2.9, printed page 287 (PDF page 296). It applies to arbitrary continuous semimartingales satisfying the stated decomposition; its input is not restricted to a particular stochastic differential equation.

Setting

Time is the nonnegative real half-line and the state has d real coordinates, indexed by Fin d. The sample space Ω has a complete probability measure P and a filtration ℱ. The initial sigma algebra contains every ambient measurable null set. For each coordinate i, V_i is a continuous adapted finite-variation process, zero at time zero; M_i is a continuous adapted local martingale, zero at time zero almost surely. The process X_i has an ℱ₀-measurable initial value and satisfies X_i(t)=X_i(0)+V_i(t)+M_i(t) for all times and samples.

The test function f(t,x) has a continuous first time derivative, continuous first spatial derivatives, and continuous second spatial derivatives. At time zero, the time derivative is taken within the nonnegative-time domain. The notation f_t, f_{x_i}, and f_{x_i x_j} denotes these derivative witnesses. The conclusion supplies processes representing the continuous cross variations and integrals; their existence is part of the theorem. The Stieltjes relations use pathwise left dyadic sums for continuous finite-variation integrators. Martingale integrals and cross variations use convergence in probability of their corresponding dyadic sums. The integral versions are continuous and adapted where the theorem requires those properties.

Formalization targets

Theorem 2.9 — time-dependent multidimensional Itô formula

For every t ≥ 0, outside one null set independent of t, the target is

f(t,X(t))−f(0,X(0))=∫0tft(s,X(s)) ds+∑i∫0tfxi(s,X(s)) dVi(s)+∑i∫0tfxi(s,X(s)) dMi(s)+12∑i,j∫0tfxixj(s,X(s)) d⟨Mi,Mj⟩s.\begin{aligned} f(t,X(t))-f(0,X(0))={}&\int_0^t f_t(s,X(s))\,ds\\ &+\sum_i\int_0^t f_{x_i}(s,X(s))\,dV_i(s)\\ &+\sum_i\int_0^t f_{x_i}(s,X(s))\,dM_i(s)\\ &+\frac12\sum_{i,j}\int_0^t f_{x_i x_j}(s,X(s))\,d\langle M_i,M_j\rangle_s. \end{aligned}f(t,X(t))−f(0,X(0))=​∫0t​ft​(s,X(s))ds+i∑​∫0t​fxi​​(s,X(s))dVi​(s)+i∑​∫0t​fxi​​(s,X(s))dMi​(s)+21​i,j∑​∫0t​fxi​xj​​(s,X(s))d⟨Mi​,Mj​⟩s​.​

The goal is EthierKurtz.ito_formula. It retains every term and both coordinate indices in the cross-variation sum. The bracket and integral witnesses are existential conclusions, so the statement does not require their existence as an extra hypothesis on X.

Significance

The formula identifies the effect of a smooth, time-dependent transformation on any process with the stated continuous semimartingale decomposition. In particular, it exposes the second-order correction that distinguishes stochastic change of variables from deterministic calculus. This makes it a general calculus result that can later be applied to diffusion equations, martingale problems, and transformed processes, independently of how the input process was constructed.

The cited theorem is established in the source book. This mission provides a compiled Lean statement and concrete expression dependencies; it does not provide a Lean proof. Formalizing the proof would require the stochastic-integral and covariation infrastructure to support the source's continuous local-martingale setting and version conventions. A solver's result should prove this full statement or develop reusable infrastructure that supports it without changing its hypotheses or conclusion.

Difficulty

The ordinary deterministic chain rule cannot account for the double sum of cross variations. A statement limited to Brownian motion, an absolutely continuous bracket, or a fixed stochastic differential equation would omit cases covered by the source. The local-martingale integral also needs a continuous adapted version with a common almost-sure interpretation over all times; merely obtaining a separate fixed-time limit does not by itself supply that final identity. These requirements make the exact scope of the integral and bracket relations central to the formalization.

Formalization scope

The Lean declaration uses ℝ≥0 for time, Fin d → ℝ for state vectors, Measure Ω for the probability law, and Filtration ℝ≥0 for the filtration. It includes completeness of P, the initial-null-set condition on ℱ 0, continuity and adaptation of V and M, local bounded variation of V, stopping-time localization for M, the full decomposition of X, and continuous derivative witnesses for f. The final almost-everywhere quantifier precedes the universal time quantifier. There is no Brownian driver, global square-integrability requirement, right-continuity assumption on the filtration, or diagonal-only bracket simplification.

Five definitions are expression dependencies: IsSourceLocalMartingale, HasCrossVariation, itoStepSum, HasContinuousStieltjesIntegral, and HasContinuousMartingaleIntegral. Their staged declarations retain the reviewed source definitions under a consistent EthierKurtz namespace. The dyadic-sum definitions do not embed the change-of-variables identity, so the theorem cannot be discharged by unfolding a definition of the desired answer. The mission asks for a proof of the stated result, not a weakened special case. The empty-coordinate case is admitted consistently; no positive-dimensional source case is excluded.

Selected references

  • Stewart N. Ethier and Thomas G. Kurtz, Markov Processes: Characterization and Convergence, Wiley, 1986 (held reprint 1986/2005), Chapter 5, Section 2, Theorem 2.9, printed p. 287 (PDF p. 296), equations (2.40)–(2.41). Conventions: printed pp. 279–280 and 286 (PDF pp. 288–289 and 295). Cross variation: Chapter 2, equation (6.4), printed p. 79 (PDF p. 88).
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Functional Analysis·Captain: mikedeng1

Markov Processes: Characterization and Convergence 01: Contraction semigroup generationTextbook

Motivation

Continuous-time Markov processes are often studied through operators that describe how observables evolve. The generation question asks when an operator specified on a domain actually determines a strongly continuous family of contractions. Ethier and Kurtz place this question at the start of Markov Processes: Characterization and Convergence because the resulting semigroup language supports their later treatment of processes and convergence. This mission records the full generation characterization in Chapter 1, Theorem 2.6, and retains the related perturbation result in Theorem 7.1.

Setting

Let (E) be a real Banach space. A linear operator (A) has a linear domain (D(A)\subseteq E), which need not equal (E). A family (T(t)), for nonnegative real (t), consists of bounded linear maps (E\to E). It is a strongly continuous contraction semigroup when (T(0)) is the identity, (T(s+t)=T(s)T(t)), every (T(t)) has norm at most one, and (T(t)x\to x) as (t\downarrow0) for every (x\in E). Its infinitesimal generator has exactly those (x) for which the right-hand difference quotient (t^{-1}(T(t)x-x)) converges, and sends each such (x) to the limit.

An operator is dissipative here when

r∥x∥≤∥rx−Ax∥(x∈D(A), r>0).r\lVert x\rVert\leq\lVert rx-Ax\rVert \quad(x\in D(A),\ r>0).r∥x∥≤∥rx−Ax∥(x∈D(A), r>0).

The range condition for a positive (r) says every vector in (E) is (rx-Ax) for some (x\in D(A)). Density means that vectors in (D(A)) approximate every vector in (E). These are independent requirements in the formal statement; neither the domain nor the operator is assumed closed or bounded.

For the related perturbation theorem, (A) and (B) may have different domains. Their sum uses the intersection of those domains. Closure is closure of the graph in (E\times E). A graph closure is required to be the graph of a single-valued operator before it can be called a generator.

Formalization targets

Theorem 2.6: generation characterization

The goal is the equivalence

A generates a strongly continuous contraction semigroup⟺D(A)‾=E,A is dissipative,Ran⁡(rI−A)=E for some r>0.A\text{ generates a strongly continuous contraction semigroup} \quad\Longleftrightarrow\quad \overline{D(A)}=E,\quad A\text{ is dissipative},\quad \operatorname{Ran}(rI-A)=E\text{ for some }r>0.A generates a strongly continuous contraction semigroup⟺D(A)​=E,A is dissipative,Ran(rI−A)=E for some r>0.

The left side uses the full infinitesimal-generator domain, rather than agreement with a generator only on a smaller subdomain. The right side includes dissipativity for every positive parameter and full surjectivity for at least one positive parameter.

Theorem 7.1: relatively bounded perturbation

The retained related result assumes that the closure of (A) is single-valued and generates a strongly continuous contraction semigroup, (D(A)\subseteq D(B)), and (B) is dissipative. It further assumes

∥Bx∥≤α∥Ax∥+β∥x∥(x∈D(A)),0≤α<1,β≥0.\lVert Bx\rVert\leq\alpha\lVert Ax\rVert+\beta\lVert x\rVert \quad(x\in D(A)),\qquad 0\leq\alpha<1,\quad\beta\geq0.∥Bx∥≤α∥Ax∥+β∥x∥(x∈D(A)),0≤α<1,β≥0.

It concludes that the closure of (A+B) is single-valued and generates such a semigroup, and that its entire graph equals the sum of the graph closures of (A) and (B). This theorem is a related generation variant within the same mission, not a separate main goal.

Significance

The equivalence turns an existence question about a family of operators into conditions on a single potentially unbounded operator. In particular, it preserves the exact-domain requirement: proving only that a semigroup generator extends (A) would answer a weaker question. The perturbation theorem then identifies circumstances under which an already generating operator remains useful after adding a dissipative term that need not itself be bounded.

The textbook proves both statements. The Lean files supplied here are statements with intentional proof holes; they do not claim machine-checked proofs. A completed formalization would supply proofs of these source results while keeping the domain, range, closure, and relative-bound conditions shown in the statements.

Difficulty

The hypotheses describe a linear map on only part of the Banach space, while the conclusion requires bounded operators on all of (E) at every nonnegative time. Checking a semigroup law on a convenient subspace is insufficient unless the resulting operators and generator have the stated full domains. For perturbations, graph closure can enlarge a domain. An equality of formulas on (D(A)) alone would therefore omit the theorem's graph and domain conclusion.

Formalization scope

Lean uses NormedAddCommGroup E, NormedSpace ℝ E, and CompleteSpace E for the real Banach space; Submodule ℝ E for each domain; D →ₗ[ℝ] E for an operator that need not be bounded; and E →L[ℝ] E for each semigroup operator. Semigroup values at negative real times are unconstrained. The derivative is the right limit through positive times. Graph closure is topological closure in the ambient product, and graph sum requires a common input. The strict relative bound (\alpha<1) and positive resolvent parameter remain explicit.

The reusable definitions are the semigroup predicate, full generator predicate, operator graph, and graph sum. The mission welcomes proofs of the two stated theorems and genuinely source-based supporting lemmas. A model with an empty operator domain, an operator restricted from a larger generator, or a conclusion that drops the graph equality would not satisfy the target.

Selected references

  • Stewart N. Ethier and Thomas G. Kurtz, Markov Processes: Characterization and Convergence, Wiley, 1986, Chapter 1, Sections 2 and 7, Theorems 2.6 and 7.1. Book record.
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Machine LearningStatistics·Captain: mikedeng1

High-Dimensional Statistics XIII: A Localized Uniform LawTextbook

Motivation

Every consistency guarantee for an empirical-risk-minimization procedure — the Lasso, kernel ridge regression, maximum likelihood — ultimately rests on relating an empirical average to its population expectation, uniformly over the class of candidate functions or parameters being searched. Chapter 4 established the classical form of this connection: a uniform law of large numbers, bounding sup⁡f∈F∣∥f∥n2−∥f∥22∣\sup_{f\in F}|\|f\|_n^2-\|f\|_2^2|supf∈F​∣∥f∥n2​−∥f∥22​∣ by an absolute quantity governed by the (unlocalized) complexity of FFF. Such a bound is often wasteful: it treats a function with small population norm the same as one with large population norm, when intuitively the empirical and population norms of a small function should already agree closely. This mission formalizes the sharper, localized form of this uniform law — the same localization principle Chapter 13 used for nonparametric least squares, now applied directly to the empirical-versus-population norm comparison itself, giving relative rather than absolute control and recovering optimal convergence rates that the unlocalized theory misses.

Setting

Fix a probability distribution PPP over a covariate space XXX and nnn i.i.d. samples x1,…,xn∼Px_1,\dots,x_n\sim Px1​,…,xn​∼P. For f:X→Rf:X\to\mathbb Rf:X→R, the population norm is ∥f∥22:=∫Xf(x)2 P(dx)\|f\|_2^2:=\int_Xf(x)^2\,P(dx)∥f∥22​:=∫X​f(x)2P(dx) and the empirical norm is ∥f∥n2:=1n∑i=1nf(xi)2\|f\|_n^2:=\frac1n\sum_{i=1}^nf(x_i)^2∥f∥n2​:=n1​∑i=1n​f(xi​)2; by linearity of expectation, E[∥f∥n2]=∥f∥22\mathbb E[\|f\|_n^2]=\|f\|_2^2E[∥f∥n2​]=∥f∥22​, so the question is how tightly ∥f∥n2\|f\|_n^2∥f∥n2​ concentrates around ∥f∥22\|f\|_2^2∥f∥22​, uniformly over a function class FFF. A class FFF is star-shaped around the origin if f∈F,α∈[0,1]  ⟹  αf∈Ff\in F,\alpha\in[0,1]\implies\alpha f\in Ff∈F,α∈[0,1]⟹αf∈F, and bbb-uniformly bounded if ∥f∥∞≤b\|f\|_\infty\le b∥f∥∞​≤b for every f∈Ff\in Ff∈F. The relevant complexity measure is the population localized Rademacher complexity

Rn(δ;F):=Eε,x[ sup⁡f∈F, ∥f∥2≤δ ∣1n∑i=1nεif(xi)∣ ],R_n(\delta;F) := \mathbb E_{\varepsilon,x}\Big[\ \sup_{f\in F,\ \|f\|_2\le\delta}\ \Big| \tfrac1n\sum_{i=1}^n\varepsilon_if(x_i)\Big|\ \Big],Rn​(δ;F):=Eε,x​[ f∈F, ∥f∥2​≤δsup​ ​n1​i=1∑n​εi​f(xi​)​ ],

where ε1,…,εn\varepsilon_1,\dots,\varepsilon_nε1​,…,εn​ are i.i.d. Rademacher signs independent of the samples — note that, unlike Chapter 13's Gaussian complexity for fixed design points, this expectation integrates out the randomness of the samples themselves, since this chapter treats {xi}\{x_i\}{xi​} as genuinely random throughout. A critical radius δn\delta_nδn​ is any positive solution of Rn(δ;F)≤δ2/bR_n(\delta;F)\le\delta^2/bRn​(δ;F)≤δ2/b.

Formalization targets

Theorem 14.1 (goal). Given FFF star-shaped and bbb-uniformly bounded, and δn\delta_nδn​ solving the critical inequality, for any t≥δnt\ge\delta_nt≥δn​,

∣∥f∥n2−∥f∥22∣≤12∥f∥22+t22for all f∈F,\Big|\|f\|_n^2-\|f\|_2^2\Big|\le\frac12\|f\|_2^2+\frac{t^2}2 \qquad\text{for all }f\in F,​∥f∥n2​−∥f∥22​​≤21​∥f∥22​+2t2​for all f∈F,

with probability at least 1−c1e−c2nt2/b21-c_1e^{-c_2nt^2/b^2}1−c1​e−c2​nt2/b2; and if additionally nδn2≥2c2log⁡(4log⁡(1/δn))n\delta_n^2\ge\frac2{c_2}\log(4\log(1/\delta_n))nδn2​≥c2​2​log(4log(1/δn​)),

∣∥f∥n−∥f∥2∣≤c0δnfor all f∈F,\big|\|f\|_n-\|f\|_2\big|\le c_0\delta_n \qquad\text{for all }f\in F,​∥f∥n​−∥f∥2​​≤c0​δn​for all f∈F,

with probability at least 1−c1′e−c2′nδn2/b21-c_1'e^{-c_2'n\delta_n^2/b^2}1−c1′​e−c2′​nδn2​/b2.

Significance

Theorem 14.1 is the technical engine behind two of the book's other sharp results: Example 14.2's derivation of the optimal n−1/2n^{-1/2}n−1/2 rate for bounded quadratic function classes (where the unlocalized analogue of this theorem only achieves the slower n−1/4n^{-1/4}n−1/4 rate), and, more broadly, every later argument in the book that needs to translate an empirical-norm guarantee (as produced directly by an M-estimator's optimality, e.g. Chapter 13's nonparametric least-squares bounds) into a population-norm guarantee, or vice versa. The gap between the "absolute" uniform law of Chapter 4 and the "relative" one here is exactly the difference between a bound that is only informative for functions of order-one population norm, and one that remains sharp arbitrarily close to the origin — which is precisely where a consistent estimator's error eventually lives. Formalizing the statement produces, for the first time on the platform, the localized-Rademacher-complexity vocabulary at the population level (as opposed to Chapter 13's fixed-design Gaussian-complexity version), reusable by any future mission needing to pass between empirical and population norms.

Difficulty

The naive approach — apply Hoeffding's inequality to ∣∥f∥n2−∥f∥22∣|\|f\|_n^2-\|f\|_2^2|∣∥f∥n2​−∥f∥22​∣ for a fixed fff, then union-bound (or apply the unlocalized Rademacher-complexity uniform law of Chapter 4) over FFF — gives a bound whose complexity term does not shrink as ∥f∥2→0\|f\|_2\to0∥f∥2​→0, since it uses the complexity of all of FFF regardless of a given function's own size. This is exactly the sub-optimality Example 14.2 exhibits concretely: the naive bound gives rate n−1/4n^{-1/4}n−1/4 where the truth is n−1/2n^{-1/2}n−1/2. The fix is not merely technical bookkeeping — it requires a genuine peeling argument over dyadic norm-scales (exactly as in Chapter 13's proof of Theorem 13.13), applying the localized complexity Rn(δ;F)R_n(\delta;F)Rn​(δ;F) at the scale δ=∥f∥2\delta=\|f\|_2δ=∥f∥2​ appropriate to each individual fff, and controlling the resulting geometric sum of tail probabilities across scales. A reader's first instinct — bound ∥f∥2\|f\|_2∥f∥2​ in terms of ∥f∥n\|f\|_n∥f∥n​ and substitute — is circular, since ∥f∥n\|f\|_n∥f∥n​ is itself the random quantity being controlled.

Formalization scope

The covariate space X carries an arbitrary MeasurableSpace structure (no topology needed for the statement); the sample sequence and the Rademacher signs are both represented as families of measurable functions on a shared probability space Ω, with their joint independence stated as a single IndepFun between the two vector-valued sequences (rather than building a combined-index iIndepFun), since it is the two sequences — not each pair of individual variables — whose independence the book invokes. The two conclusions of Theorem 14.1 are stated as a conjunction with the second gated behind its own extra hypothesis, never collapsed into a single implication, since the book's own statement keeps them syntactically and logically distinct (the second requires a strictly stronger and additional condition on top of the first's). The universal constants (c1,c2,c0,c1',c2') are quantified before every instance object, so they cannot secretly depend on the function class, sample size, or radius. Every f ∈ F is required measurable (hF_meas, added in revision): the book's own framing implicitly restricts to measurable, square-integrable f throughout (p. 454), and without this hypothesis the population norm popNormSq, which appears directly in the goal's conclusion, could silently take Mathlib's Bochner-integral junk value 0 for a non-measurable, pointwise-bounded member of a star-shaped, uniformly-bounded F. The trivializing formalization ruled out here is stating the localization constraint at the empirical rather than population norm in popRademacherComplexity — this chapter's whole point (contrast Chapter 13's Gn, correctly localized at the empirical norm since there the design is fixed) is that Rn(δ;F)R_n(\delta;F)Rn​(δ;F)'s localization is a population-level object, precisely because the samples are random here. Welcome future contributions: Corollary 14.3's covering-number sufficient condition for the empirical version of the critical inequality, and Theorem 14.20's Lipschitz/strongly-convex cost-function uniform law, both deferred from this mission (see STATUS.md) as they need substantial additional apparatus (metric entropy integrals; cost functions and strong convexity) beyond what Theorem 14.1 itself requires.

Selected references

  • M. Wainwright, High-Dimensional Statistics: A Non-Asymptotic Viewpoint, Cambridge University Press, 2019, Chapter 14. https://doi.org/10.1017/9781108627771
  • P. Bartlett, O. Bousquet and S. Mendelson, "Local Rademacher complexities," Annals of Statistics, 33(4):1497-1537, 2005. https://doi.org/10.1214/009053605000000282
  • V. Koltchinskii, "Local Rademacher complexities and oracle inequalities in risk minimization," Annals of Statistics, 34(6):2593-2656, 2006. https://doi.org/10.1214/009053606000001019
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Machine LearningStatistics·Captain: mikedeng1

High-Dimensional Statistics X: Graph Selection Consistency for Gaussian Graphical ModelsTextbook

Motivation

Many high-dimensional data sets — gene-expression profiles, sensor networks, social interactions — come with no natural ordering of variables, only pairwise dependencies whose structure is itself the object of interest. A graphical model encodes these dependencies as an undirected graph: vertices are variables, and edges mark direct (conditional) dependence. Recovering the graph from samples — graphical model selection — is a combinatorial problem masquerading as a statistical one: there are 2(d2)2^{\binom{d}{2}}2(2d​) candidate graphs on ddd vertices, far too many to search directly. For Gaussian data, however, graph structure is exactly the sparsity pattern of the inverse covariance (precision) matrix, which turns graph selection into ddd coupled sparse-regression problems — one per vertex — each of which the Lasso theory of Chapter 7 already knows how to solve. This mission formalizes the theorem, due to Meinshausen and Bühlmann (2006), that shows this reduction actually works: solving ddd independent Lasso problems and combining the results recovers the exact graph with high probability, at a sample complexity governed by the same kind of incoherence condition that governs Lasso support recovery itself.

Setting

An undirected graphical model on a finite vertex set VVV pairs a graph G=(V,E)G=(V,E)G=(V,E) with a random vector X=(Xj)j∈VX=(X_j)_{j\in V}X=(Xj​)j∈V​. Two equivalent structural properties connect XXX to GGG (Theorem 11.8, Hammersley-Clifford): XXX factorizes according to GGG if its density is a product of nonnegative functions, one per clique of GGG, each depending only on the variables in that clique (Definition 11.1); XXX is Markov with respect to GGG if, for every vertex cutset SSS separating VVV into disjoint pieces AAA and BBB, the sub-vectors XAX_AXA​ and XBX_BXB​ are conditionally independent given XSX_SXS​ (Definition 11.5). For a strictly positive density, these are the same condition.

For a zero-mean ddd-dimensional Gaussian vector with covariance Σ∗\Sigma^*Σ∗ and precision matrix Θ∗=(Σ∗)−1\Theta^*=(\Sigma^*)^{-1}Θ∗=(Σ∗)−1, the graph structure is exactly the support of Θ∗\Theta^*Θ∗: (j,k)∈E  ⟺  Θjk∗≠0(j,k)\in E \iff \Theta^*_{jk}\ne0(j,k)∈E⟺Θjk∗​=0. The neighborhood N(j):={k∣(j,k)∈E}N(j):=\{k\mid(j,k)\in E\}N(j):={k∣(j,k)∈E} of each vertex is itself a vertex cutset (separating {j}\{j\}{j} from everything else), so the conditional independence Xj⊥XV∖N+(j)∣XN(j)X_j\perp X_{V\setminus N^+(j)}\mid X_{N(j)}Xj​⊥XV∖N+(j)​∣XN(j)​ holds, and — by standard Gaussian conditioning — XjX_jXj​ decomposes as a linear function of XV∖{j}X_{V\setminus\{j\}}XV∖{j}​ plus independent Gaussian noise, with regression coefficients supported exactly on N(j)N(j)N(j). Neighborhood regression exploits this directly: for each vertex jjj, solve the Lasso

θ^j∈arg⁡min⁡θ∈Rd−1 12n∥Xj−X∖{j}θ∥22+λn∥θ∥1,\hat\theta_j \in \arg\min_{\theta\in\mathbb R^{d-1}}\ \frac1{2n}\|X_j-X_{\setminus\{j\}}\theta\|_2^2 +\lambda_n\|\theta\|_1,θ^j​∈argθ∈Rd−1min​ 2n1​∥Xj​−X∖{j}​θ∥22​+λn​∥θ∥1​,

read off N^(j):={k∣θ^j,k≠0}\hat N(j):=\{k\mid\hat\theta_{j,k}\ne0\}N^(j):={k∣θ^j,k​=0}, and combine the ddd per-vertex estimates into a single edge set via the OR rule ((j,k)∈E^OR(j,k)\in\hat E_{\mathrm{OR}}(j,k)∈E^OR​ iff k∈N^(j)k\in\hat N(j)k∈N^(j) or j∈N^(k)j\in\hat N(k)j∈N^(k)) or the more conservative AND rule (iff both hold). The relevant incoherence condition, analogous to Chapter 7's, is stated for a positive definite matrix Γ\GammaΓ and subset SSS: Γ\GammaΓ is α\alphaα-incoherent with respect to SSS if max⁡k∉S∥ΓkS(ΓSS)−1∥1≤1−α\max_{k\notin S}\|\Gamma_{kS}(\Gamma_{SS})^{-1}\|_1\le1-\alphamaxk∈/S​∥ΓkS​(ΓSS​)−1∥1​≤1−α.

Formalization targets

Theorem 11.8 (Hammersley-Clifford). Factorizes G p ↔ IsMarkov G X P for any strictly positive density ppp.

Theorem 11.12 (goal — graph selection consistency). Suppose for every jjj, Σ∖{j}∗\Sigma^*_{\setminus\{j\}}Σ∖{j}∗​ is α\alphaα-incoherent with respect to N(j)N(j)N(j), and ∣ ⁣∣ ⁣∣(ΣN(j),N(j)∗)−1∣ ⁣∣ ⁣∣∞≤b|\!|\!|(\Sigma^*_{N(j),N(j)})^{-1}|\!|\!|_\infty\le b∣∣∣(ΣN(j),N(j)∗​)−1∣∣∣∞​≤b. With λn=c01α(log⁡d/n+δ)\lambda_n=c_0\frac1\alpha(\sqrt{\log d/n}+\delta)λn​=c0​α1​(logd/n​+δ), the neighborhood-Lasso estimate combined via either rule satisfies, with probability at least 1−c2e−c3nmin⁡(δ2,1/m)1-c_2e^{-c_3n\min(\delta^2,1/m)}1−c2​e−c3​nmin(δ2,1/m):

E^⊆Eand∀(j,k): ∣Θjk∗∣≥7bλn  ⟹  (j,k)∈E^.\hat E\subseteq E \qquad\text{and}\qquad \forall (j,k):\ |\Theta^*_{jk}|\ge7b\lambda_n \implies (j,k)\in\hat E.E^⊆Eand∀(j,k): ∣Θjk∗​∣≥7bλn​⟹(j,k)∈E^.

Significance

Theorem 11.12 is the statistical justification for one of the two standard approaches to Gaussian graphical model selection (the other being the penalized-likelihood "graphical Lasso" of §11.2.1). Its significance is computational as much as statistical: rather than solving one ddd-dimensional penalized-likelihood problem, neighborhood regression solves ddd independent, embarrassingly parallel Lasso problems, each of dimension d−1d-1d−1 — a substantial practical advantage at scale, with (as this theorem shows) no loss in statistical guarantee. Formalizing it produces, for the first time on the platform, statement-level infrastructure for undirected graphical models (Hammersley-Clifford, the Markov property via vertex cutsets, neighborhood structure) together with the random-design analogue of the Lasso support-recovery machinery — a genuinely different technical regime from Chapter 7's fixed-design Lasso theory, since here the "design matrix" X∖{j}X_{\setminus\{j\}}X∖{j}​ is itself Gaussian and statistically coupled to the response XjX_jXj​ through the very covariance structure being estimated. As with the other missions in this series, only the statements are formalized here; the proofs (an extension of the primal-dual witness technique to random design, per the book's own proof sketch) are left as the draft goal for future proof contributions.

Difficulty

The proof of Theorem 7.21 (Chapter 7's Lasso support-recovery guarantee) is for a deterministic design matrix, with all randomness confined to the additive noise. Here the "design" X∖{j}X_{\setminus\{j\}}X∖{j}​ is itself random and Gaussian, and — critically — it is statistically dependent on the very quantity (N(j)N(j)N(j), encoded in Θ∗\Theta^*Θ∗'s support) the Lasso is trying to recover, since X∖{j}X_{\setminus\{j\}}X∖{j}​'s own covariance structure is exactly what the incoherence condition constrains. The naive approach of just conditioning on the realized design matrix and invoking Theorem 7.21 fails, because the deterministic-design incoherence condition would then need to hold for the sample covariance Γ=1nX∖{j}TX∖{j}\Gamma=\frac1n X_{\setminus\{j\}}^TX_{\setminus\{j\}}Γ=n1​X∖{j}T​X∖{j}​, not the population covariance Σ∖{j}∗\Sigma^*_{\setminus\{j\}}Σ∖{j}∗​ that is actually assumed — and controlling the gap between sample and population incoherence under the joint (not fixed) randomness of predictors and response is exactly the extra step the book's proof needs, handled via an extension of the primal-dual witness technique that tracks both sources of randomness together.

Formalization scope

The vertex set V is an arbitrary finite type; the covariate space for X is ℝ throughout (all variables jointly Gaussian). The Gaussian design is characterized via its one-dimensional projections (every linear combination is univariate Gaussian with the matching variance) rather than via Mathlib's multivariate-Gaussian machinery directly, to keep the definition self-contained. IsAlphaIncoherent's ambient index set is realized as a subset of the full vertex type rather than as a literal submatrix, since the book's condition never references an entry outside it. The theorem states the conclusion jointly for both the OR-rule and AND-rule estimated edge sets on one shared high-probability event, matching "based on either rule" literally rather than picking one. The trivializing formalization ruled out here is treating the neighborhood-Lasso estimate as a fixed-design Lasso problem (silently dropping the joint randomness of predictors and response) — every design realization in this formalization is the actual random vector Xdes i ω, not a deterministic parameter, and the Gaussian design hypothesis (IsIIDGaussianDesign) is stated over the same probability space Ω as the least-squares residual. Theorem 11.8 (Hammersley–Clifford) is formalized only for the continuous case — a random vector with a density with respect to Lebesgue measure — matching what the Gaussian goal (Theorem 11.12) actually needs; the book's own Definition 11.1 also permits a discrete (counting-measure) density, with the Ising model (Example 11.4) as a worked instance, which this mission does not cover. Contributions welcome: the graphical Lasso's own guarantees (Propositions 11.9, 11.10, deferred from this mission — see STATUS.md), and the proof of Theorem 11.12 itself via the primal-dual witness extension the book sketches.

Selected references

  • M. Wainwright, High-Dimensional Statistics: A Non-Asymptotic Viewpoint, Cambridge University Press, 2019, Chapter 11. https://doi.org/10.1017/9781108627771
  • N. Meinshausen and P. Bühlmann, "High-dimensional graphs and variable selection with the Lasso," Annals of Statistics, 34(3):1436-1462, 2006. https://doi.org/10.1214/009053606000000281
  • J. Hammersley and P. Clifford, "Markov fields on finite graphs and lattices," unpublished manuscript, 1971.
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Machine LearningRandom Matrix TheoryStatistics·Captain: mikedeng1

High-Dimensional Probability XI: Dvoretzky-Milman's TheoremTextbook

Motivation

A striking fact discovered by Dvoretzky in the 1960s (conjectured by Grothendieck, and sharpened into its modern quantitative form by Milman in 1971) is that every high-dimensional convex body, however irregular, contains a round slice: a random low-dimensional section (or projection) of any bounded convex set in Rn\mathbb R^nRn is, with high probability, close to a Euclidean ball — provided the dimension of the slice is small enough relative to a single geometric parameter of the body. This is remarkable because it holds for every bounded set, arbitrarily irregular; no special structure is assumed beyond boundedness. This chapter proves the theorem in its Gaussian form, as a culmination of every geometric and probabilistic tool the book develops: chaining and Dudley's inequality (Chapter 8), the matrix deviation inequality (Chapter 9), and Gaussian width and the stable dimension (Chapter 7) all combine into a single closing argument.

Setting

Fix a subset T⊆RnT\subseteq\mathbb R^nT⊆Rn. For a standard Gaussian vector g∼N(0,In)g\sim N(0,I_n)g∼N(0,In​), the Gaussian width of TTT is w(T):=Esup⁡x∈T⟨g,x⟩w(T) := \mathbb E\sup_{x\in T}\langle g,x\ranglew(T):=Esupx∈T​⟨g,x⟩ (Chapter 7), and the stable dimension of a bounded TTT is d(T):=w(T)2/diam(T)2d(T) := w(T)^2/\mathrm{diam}(T)^2d(T):=w(T)2/diam(T)2 up to an absolute constant factor (Definition 7.6.2) — a robust substitute for the ordinary linear-algebraic dimension of TTT, which can jump discontinuously under a small perturbation of TTT, unlike d(T)d(T)d(T).

An m×nm\times nm×n Gaussian random matrix with i.i.d. N(0,1)N(0,1)N(0,1) entries is a random matrix AAA each of whose mnmnmn entries is an independent standard normal random variable.

Formalization targets

Goal (Theorem 11.3.3, Dvoretzky-Milman's theorem, Gaussian form)

∃ c>0:m≤cε2d(T)  ⟹  P[(1−ε)B⊆conv(AT)⊆(1+ε)B]≥0.99\exists\,c>0:\quad m\le c\varepsilon^2 d(T) \;\Longrightarrow\; \mathbb P\bigl[(1-\varepsilon)B \subseteq \mathrm{conv}(AT) \subseteq (1+\varepsilon)B\bigr] \ge 0.99∃c>0:m≤cε2d(T)⟹P[(1−ε)B⊆conv(AT)⊆(1+ε)B]≥0.99

for every m×nm\times nm×n Gaussian random matrix AAA with i.i.d. N(0,1)N(0,1)N(0,1) entries, every bounded T⊆RnT\subseteq\mathbb R^nT⊆Rn containing the origin, and every ε∈(0,1)\varepsilon\in(0,1)ε∈(0,1), where BBB is the Euclidean ball of radius w(T)w(T)w(T) centered at the origin. The probability 0.990.990.99 is the book's own literal numeral, not a free parameter — this is the theorem the book actually states, not a family of theorems indexed by a confidence level.

Significance

Dvoretzky-Milman's theorem is one of the foundational results of the local theory of Banach spaces (asymptotic geometric analysis): it says every nnn-dimensional normed space contains an almost-Euclidean subspace of dimension proportional to (a geometric invariant closely related to) log⁡n\log nlogn in the worst case, and much larger for spaces whose unit ball is already well-behaved (the stable dimension of the cube [−1,1]n[-1,1]^n[−1,1]n, for instance, is proportional to nnn itself — Example 11.3.6). This underlies results throughout convex geometry, compressed sensing, and high-dimensional statistics wherever a random low-dimensional projection needs to be shown to preserve geometric structure. The book's own framing makes clear why this chapter is placed last: the theorem's proof is a genuine capstone, invoking Chevet's inequality (itself built from the matrix deviation inequality of Chapter 9, which is built from chaining, Chapter 8) as its main technical tool.

The theorem and its proof are classical (Milman 1971; this book's specific route via Chevet's inequality is a standard modern exposition). This mission formalizes the goal theorem's statement — including its two supporting geometric quantities, Gaussian width and stable dimension, and the notion of a Gaussian random matrix — as a complete, faithful target for a solver, in the book's own sub-namespace built for this chapter (no dependency here is reusable from an earlier chunk, since none of this book series' Chapter 7 or Chapter 9 definitions has yet been published).

Difficulty

The natural first idea — bound conv(AT)\mathrm{conv}(AT)conv(AT) directly using concentration of ∥Ax∥2\|Ax\|_2∥Ax∥2​ for each fixed x∈Tx\in Tx∈T — runs into exactly the uniform-supremum obstacle the whole book has been building tools to overcome: a bound that holds for one xxx at a time, even with a union bound over a net of TTT, does not obviously extend to the full convex hull without first controlling sup⁡x∈T∣⟨Ax,y⟩−w(T)∥y∥2∣\sup_{x\in T}|\langle Ax,y\rangle - w(T)\|y\|_2|supx∈T​∣⟨Ax,y⟩−w(T)∥y∥2​∣ uniformly over both x∈Tx\in Tx∈T and yyy on the unit sphere of the target space — a two-parameter supremum. The book's actual route goes through Chevet's inequality, itself proved using the matrix deviation inequality's own chaining-based argument, to control this two-sided supremum, and then converts the resulting inequality into the containment (1−ε)B⊆conv(AT)⊆(1+ε)B(1-\varepsilon)B\subseteq\mathrm{conv}(AT)\subseteq(1+\varepsilon)B(1−ε)B⊆conv(AT)⊆(1+ε)B via a support- function duality argument (a convex body is pinned down by its support function, so bounding sup⁡x∈T⟨Ax,y⟩\sup_{x\in T}\langle Ax,y\ranglesupx∈T​⟨Ax,y⟩ uniformly over yyy on the sphere is exactly what is needed).

Formalization scope

A is Ω → Matrix (Fin m) (Fin n) ℝ with an explicit IsGaussianMatrix hypothesis (entries i.i.d. N(0,1)N(0,1)N(0,1), formalized entrywise with joint independence). conv(AT) is convexHull ℝ of the image of T under A's mulVec, round-tripped through EuclideanSpace's continuous linear equivalence with the underlying function type. w(T) reuses this mission series' ExpSup/GaussianWidth convention (redefined locally, per the drafts-cannot-import-drafts rule, following the same ProbabilityTheory.stdGaussian-based realization of a standard Gaussian vector as 08-matrix-deviation). The stable dimension d(T)d(T)d(T) is formalized directly as w(T)2/diam(T)2w(T)^2/ \mathrm{diam}(T)^2w(T)2/diam(T)2 rather than via the book's literal (but only asymptotically equivalent, per Exercise 7.6.1) definition through a squared Gaussian width h(T−T)2h(T-T)^2h(T−T)2 — the goal theorem's own proof uses only the inequality direction of that equivalence, and the goal's hypothesis already carries an unpinned absolute constant that absorbs the equivalence constant, so this substitution preserves the theorem's exact truth content (see StableDimension's own doc-comment and MODERATION_NOTES.md for the full argument) rather than approximating it.

Ball-center deviation, disclosed. The book's printed theorem statement carries no hypothesis that TTT contains the origin; its proof opens by translating TTT so that it does ("Translating TTT if necessary, we can assume that TTT contains the origin"), and Remark 11.3.4 then confirms the ball is centered at the origin in that case. This mission states the WLOG-reduced case directly — adding 0∈T0\in T0∈T as an explicit hypothesis — rather than also formalizing the translation argument that recovers the fully general (untranslated) statement. This is disclosed as a genuine narrowing of the literal printed statement, though not of what the book's own proof actually establishes.

This mission covers Theorem 11.3.3 only, with no milestones: BRIEF.md explicitly instructs that if the chapter's full proof chain (general matrix deviation inequality, Chevet's inequality, random projections of sets — Theorems 11.1.5, 11.2.4, 11.3.1) proves too heavy for the session, milestones should be cut rather than the goal substituted. All three are left out, not approximated, given this chapter's five from-scratch definitions already needed for the goal's own statement. ExpSup, GaussianWidth, StableDimension and IsGaussianMatrix are reusable by any later development needing Gaussian width, the stable dimension, or a Gaussian random matrix. Solvers' contributions are welcome on the goal theorem itself and, beyond this mission's current scope, on the three named milestones.

Selected references

  • A. Dvoretzky, Some results on convex bodies and Banach spaces, Proc. Internat. Sympos. Linear Spaces (Jerusalem, 1960), 123–160.
  • V. D. Milman, A new proof of A. Dvoretzky's theorem on cross-sections of convex bodies, Funkcional. Anal. i Priložen. 5 (1971), 28–37.
  • R. Vershynin, High-Dimensional Probability: An Introduction with Applications in Data Science, Cambridge University Press, 2018, Chapter 11. https://doi.org/10.1017/9781108231596
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AnalysisStochastic Systems·Captain: naimengye

Probability Theory and Examples VI: Donsker's TheoremTextbook

Motivation

The central limit theorem says that Sn/nS_n/\sqrt nSn​/n​ converges to a normal random variable. Donsker's theorem says something much stronger: the whole rescaled path of the random walk converges to the whole path of a Brownian motion, as a random element of C[0,1]C[0,1]C[0,1].

The payoff is a machine. Once S(n⋅)/n⇒B(⋅)S(n\cdot)/\sqrt n\Rightarrow B(\cdot)S(n⋅)/n​⇒B(⋅) in C[0,1]C[0,1]C[0,1], every functional of the path that is continuous — or merely continuous at almost every Brownian path — transfers automatically. The maximum of the walk converges to the maximum of Brownian motion; the fraction of time the walk spends above a level converges to the corresponding occupation time; the last zero before time nnn converges to the last Brownian zero before time 111, which is how the arcsine law escapes the simple random walk it was proved for. This is the invariance principle of Erdős and Kac: the asymptotic behaviour of a functional of SnS_nSn​ should not depend on the step distribution, as long as the central limit theorem applies.

Chapter 8 of Rick Durrett's Probability: Theory and Examples (Version 5, 2019) proves this by embedding rather than by the usual tightness argument. Skorokhod's representation theorem puts a mean-zero, finite-variance random variable inside a Brownian motion as the value at a stopping time; iterating puts the whole walk inside one Brownian motion at a sequence of stopping times whose gaps are i.i.d.; and the law of large numbers then forces the embedded walk to be uniformly close to the Brownian path.

Setting

Let X1,X2,…X_1,X_2,\dotsX1​,X2​,… be i.i.d. with mean 000 and variance 111, and Sm=X1+⋯+XmS_m=X_1+\dots+X_mSm​=X1​+⋯+Xm​. Define S(u)S(u)S(u) to be SmS_mSm​ at integer u=mu=mu=m and linear in between, and set

Wn(t) = S(nt)n,t∈[0,1],W_n(t)\ =\ \frac{S(nt)}{\sqrt n},\qquad t\in[0,1],Wn​(t) = n​S(nt)​,t∈[0,1],

a random element of C[0,1]C[0,1]C[0,1], the continuous functions on the unit interval with the uniform norm and its Borel σ\sigmaσ-algebra.

On the Brownian side, let BBB be a Brownian motion, and write B(⋅)B(\cdot)B(⋅) for its restriction to [0,1][0,1][0,1], again a random element of C[0,1]C[0,1]C[0,1].

Formalization targets

Goal — Theorem 8.1.4, Donsker's theorem

S(n⋅)n ⟹ B(⋅)in C[0,1],\frac{S(n\cdot)}{\sqrt n}\ \Longrightarrow\ B(\cdot)\qquad\text{in }C[0,1],n​S(n⋅)​ ⟹ B(⋅)in C[0,1],

that is, the laws of WnW_nWn​ on C[0,1]C[0,1]C[0,1] converge weakly to the law of Brownian motion. This is a statement about measures on a function space, not about finite-dimensional marginals: it is exactly the extra content over the central limit theorem.

Supporting levels

Theorem 8.1.1, Skorokhod's representation theorem: a mean-zero, square-integrable law is the law of BTB_TBT​ for a stopping time TTT with ET=EX2\mathbb ET=\mathbb EX^2ET=EX2; Theorem 8.1.2, the embedding of the whole walk, giving stopping times T0=0,T1,…T_0=0,T_1,\dotsT0​=0,T1​,… with (B(Tn))n(B(T_n))_n(B(Tn​))n​ distributed as the walk and with i.i.d. gaps; Theorem 8.1.5, the continuous mapping theorem for almost surely continuous functionals; and its two workhorse instances, Example 8.1.6 on maxima and Example 8.1.8 on occupation times of half-lines.

Significance

The results themselves. Donsker's theorem is the reason the arcsine law, the distribution of the maximum, and the occupation-time law are universal rather than artefacts of the simple random walk for which they were first computed. It is also the prototype for every later functional limit theorem — for martingales in Durrett's section 8.2, for stationary sequences in 8.3, for the empirical process converging to a Brownian bridge in 8.4.

Skorokhod's embedding deserves separate billing. It says any centred law with finite variance sits inside Brownian motion, which is what makes the path-space comparison possible at all, and it is the tool behind the law of the iterated logarithm in Durrett's section 8.5. The construction is a two-point mixture: write the law as a mixture of two-point laws μu,v\mu_{u,v}μu,v​ with mean zero, use the exit time of (u,v)(u,v)(u,v) for each, and the exit-time identity ETa,b=−ab\mathbb ET_{a,b}=-abETa,b​=−ab integrates to EX2\mathbb EX^2EX2.

Formalizing them. Mathlib has the i.i.d. central limit theorem, convergence in distribution for random elements of an arbitrary topological space (TendstoInDistribution, with the continuous mapping theorem and Slutsky), Brownian motion as a process with its invariances, and the machinery of stopping times for filtered spaces. It has no functional limit theorem of any kind, no Wiener measure on C[0,1]C[0,1]C[0,1], no Skorokhod embedding, and no continuous-time optional stopping. Nothing in the library relates a random walk to a Brownian path.

Difficulty

The goal is the hardest item in this series, and the embedding route is the reason the mission is stated the way it is. Durrett's proof: with Xn,m=Xm/nX_{n,m}=X_m/\sqrt nXn,m​=Xm​/n​ and stopping times τmn\tau^n_mτmn​ realizing (Sn,1,…,Sn,n)(S_{n,1},\dots,S_{n,n})(Sn,1​,…,Sn,n​) as (B(τ1n),…,B(τnn))(B(\tau^n_1),\dots,B(\tau^n_n))(B(τ1n​),…,B(τnn​)), Lemma 8.1.9 says that if τ⌊ns⌋n→s\tau^n_{\lfloor ns\rfloor}\to sτ⌊ns⌋n​→s in probability for each s∈[0,1]s\in[0,1]s∈[0,1], then ∥Sn,(n⋅)−B(⋅)∥∞→0\|S_{n,(n\cdot)}-B(\cdot)\|_\infty\to0∥Sn,(n⋅)​−B(⋅)∥∞​→0 in probability. The hypothesis is the weak law applied to the i.i.d. gaps of Theorem 8.1.2 after Brownian scaling; the conclusion plus the converging-together lemma gives the theorem. The work is uniform control of the Brownian path over shrinking time windows — the modulus of continuity — together with the bookkeeping of the polygonal interpolation.

Skorokhod's theorem needs the two exit-time facts for Brownian motion, Durrett's Theorems 7.5.3 and 7.5.5: BTa,bB_{T_{a,b}}BTa,b​​ takes the values aaa and bbb with probabilities b/(b−a)b/(b-a)b/(b−a) and −a/(b−a)-a/(b-a)−a/(b−a), and ETa,b=−ab\mathbb ET_{a,b}=-abETa,b​=−ab. Both come from optional stopping applied to BtB_tBt​ and Bt2−tB_t^2-tBt2​−t, and continuous-time optional stopping is itself not in the library. The mixture identity,

∫φ dF=c−1∫0∞dF(v)∫−∞0dF(u) (v−u)[vv−uφ(u)+−uv−uφ(v)],c=∫0∞v dF(v),\int\varphi\,dF=c^{-1}\int_0^\infty dF(v)\int_{-\infty}^0 dF(u)\,(v-u) \Bigl[\tfrac{v}{v-u}\varphi(u)+\tfrac{-u}{v-u}\varphi(v)\Bigr], \qquad c=\int_0^\infty v\,dF(v),∫φdF=c−1∫0∞​dF(v)∫−∞0​dF(u)(v−u)[v−uv​φ(u)+v−u−u​φ(v)],c=∫0∞​vdF(v),

is elementary but needs Fubini and the two expressions for ccc.

Theorem 8.1.5 is the Mann–Wald theorem in the form that allows a discontinuous ψ\psiψ: Mathlib's TendstoInDistribution.continuous_comp handles genuinely continuous maps, and the extension to maps continuous almost everywhere with respect to the limit law is the milestone. Given it, the two examples are short — the maximum is continuous outright, and the occupation-time functional is continuous at every path spending no time at the level aaa, which Fubini shows is almost every Brownian path.

Formalization scope

C[0,1]C[0,1]C[0,1] is C(Set.Icc (0:ℝ) 1, ℝ), whose compact-open topology is the uniform one because the domain is compact, with the Borel σ\sigmaσ-algebra — Mathlib has no measurable-space instance on a space of continuous maps, so the mission supplies it, and a BorelSpace instance with it.

The polygonal interpolation is written as a finite sum,

S(u)=∑k<nXk⋅clamp⁡(u−k),clamp⁡(x)=max⁡(0,min⁡(1,x)),S(u)=\sum_{k<n}X_k\cdot\operatorname{clamp}(u-k),\qquad \operatorname{clamp}(x)=\max(0,\min(1,x)),S(u)=k<n∑​Xk​⋅clamp(u−k),clamp(x)=max(0,min(1,x)),

which agrees with SmS_mSm​ at integer m≤nm\le nm≤n and is linear in between, and is manifestly continuous, so walkPath is a genuine element of C[0,1]C[0,1]C[0,1] with no side condition. Both properties were proved in Lean before publishing rather than assumed. Indexing is from zero, so Sm=X0+⋯+Xm−1S_m=X_0+\dots+X_{m-1}Sm​=X0​+⋯+Xm−1​.

The Brownian limit is brownianPath B, the restriction of the path to [0,1][0,1][0,1]. Restriction is a total function: it returns the zero path for a discontinuous argument. That junk branch is never reached, because every statement assumes every path of BBB is continuous, not merely almost every one — one may always modify a Brownian motion on a null set to achieve this, and Durrett's canonical construction on C[0,∞)C[0,\infty)C[0,∞) has it by definition. Without it there would be no C[0,1]C[0,1]C[0,1]-valued random variable to speak of.

Weak convergence is Mathlib's TendstoInDistribution, the same predicate mission II used for the Lindeberg–Feller theorem, instantiated at C[0,1]C[0,1]C[0,1] rather than at R\mathbb RR.

Skorokhod's theorem and the embedding of the walk are stated as existence of a probability space carrying the Brownian motion, a filtration and the stopping times. This is how Durrett states them — the construction needs an independent pair (U,V)(U,V)(U,V) alongside the Brownian motion, and he notes himself that TU,VT_{U,V}TU,V​ is a stopping time only for the enlarged filtration. The filtration is therefore an explicit family FtF_tFt​ that is increasing, sits inside the ambient σ\sigmaσ-field, and contains σ(Bs:s≤t)\sigma(B_s:s\le t)σ(Bs​:s≤t) — the pastSigma of mission V, which this mission imports as a reference. The stopping-time property is {T ≤ t} ∈ F_t, stated directly rather than through a bundled filtration structure.

Theorem 8.1.2's conclusion "Sn=dB(Tn)S_n=_d B(T_n)Sn​=d​B(Tn​)" is read as equality of the laws of the whole processes: the push-forward of ω↦(n↦B(Tnω))\omega\mapsto(n\mapsto B(T_n\omega))ω↦(n↦B(Tn​ω)) equals the law of the partial-sum process of an i.i.d. sequence with step law μ\muμ, taken on the infinite product measure. The gaps are required to be independent and identically distributed, as the book says.

The counting in Example 8.1.8 is a sum of indicators rather than a filtered cardinality, to keep a decidability side condition out of the statement, and the limit is the Lebesgue measure of {t∈[0,1]:Bt>a}\{t\in[0,1]:B_t>a\}{t∈[0,1]:Bt​>a} as a real number. Example 8.1.6 takes the maximum over 0≤m≤n0\le m\le n0≤m≤n, which includes S0=0S_0=0S0​=0, and the limit is the supremum of BBB over [0,1][0,1][0,1], attained because the path is continuous on a compact interval.

Existence of a Brownian motion is a hypothesis, not a claim, exactly as in mission V, except in Theorems 8.1.1 and 8.1.2 where the existence of a suitable space is the content of the statement and a Brownian motion must be produced; that is Durrett's Theorem 7.1.1, which the library does not yet have, so those two items subsume it.

Contributions welcome beyond the listed items: Lemma 8.1.9 on its own; Theorem 8.1.3, the CLT derived from the embedding; Example 8.1.7, the last zero before time nnn and the arcsine law; continuous-time optional stopping and the exit identities 7.5.3 and 7.5.5 that Skorokhod's theorem rests on; the extension to C[0,∞)C[0,\infty)C[0,∞); and the martingale, stationary-sequence and empirical-process versions of sections 8.2 to 8.4.

Selected references

  • Rick Durrett, Probability: Theory and Examples, Version 5 (11 January 2019), chapter 8, section 8.1 (pp. 389–395); Theorems 8.1.1, 8.1.2, 8.1.4, 8.1.5, Examples 8.1.6 and 8.1.8. Published as the 5th edition, Cambridge University Press, 2019, DOI 10.1017/9781108591034
  • M. D. Donsker, An invariance principle for certain probability limit theorems, Memoirs of the American Mathematical Society 6 (1951).
  • A. V. Skorokhod, Studies in the Theory of Random Processes, Addison-Wesley, 1965.
  • P. Erdős and M. Kac, On certain limit theorems of the theory of probability, Bulletin of the American Mathematical Society 52 (1946), 292–302. DOI 10.1090/S0002-9904-1946-08560-2
  • P. Billingsley, Convergence of Probability Measures, 2nd ed., Wiley, 1999, chapters 2 and 8. DOI 10.1002/9780470316962
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