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Captain: mikedeng1

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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Captain: mikedeng1

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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Captain: mikedeng1

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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Captain: mikedeng1

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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Wasserstein Distributionally Robust Optimization V: The Wasserstein Shrinkage Estimator and Robust MMSE EstimationTextbook

Motivation

Minimum mean square error (MMSE) estimation — predicting a signal xxx from a noisy observation yyy by minimizing expected squared prediction error — underlies linear systems theory, linear regression, Kalman filtering, and multiple-input multiple-output signal processing. Its classical solution assumes the joint distribution of (x,y)(x,y)(x,y) is known exactly; in practice it is estimated from data, and the estimator inherits sampling error and model risk. Kuhn, Mohajerin Esfahani, Nguyen & Shafieezadeh-Abadeh's 2019 INFORMS TutORials chapter shows that hedging the MMSE objective against every distribution in a Wasserstein ball around the empirical distribution — an infinite-dimensional worst case over an intractable set of measures, a priori — collapses to a tractable, finite-dimensional convex semidefinite program (Theorem 25, p. 29), building on the Gelbrich-hull machinery of Section 2.3. This mission formalizes that reduction.

Setting

Fix mx,my∈Nm_x, m_y \in \mathbb{N}mx​,my​∈N and let ξ=(x,y)∈Rmx×Rmy\xi = (x,y) \in \mathbb{R}^{m_x} \times \mathbb{R}^{m_y}ξ=(x,y)∈Rmx​×Rmy​ be a random vector: xxx the signal to be estimated, yyy the observation. An estimator is a measurable function ψ:Rmy→Rmx\psi : \mathbb{R}^{m_y} \to \mathbb{R}^{m_x}ψ:Rmy​→Rmx​; write Ψ\PsiΨ for the family of all estimators. The distribution of ξ\xiξ is only known to lie in a type-2 Wasserstein ball Bε,2(P^N)B_{\varepsilon,2}(\hat P_N)Bε,2​(P^N​) centered at an elliptical nominal distribution P^N=Eg(μ^,Σ^)\hat P_N = E_g(\hat\mu,\hat\Sigma)P^N​=Eg​(μ^​,Σ^) with nominal mean μ^∈Rm\hat\mu \in \mathbb{R}^mμ^​∈Rm (m=mx+mym=m_x+m_ym=mx​+my​), nominal covariance Σ^∈S+m\hat\Sigma \in S^m_+Σ^∈S+m​, and density generator ggg. The distributionally robust MMSE estimation problem is

inf⁡ψ∈Ψsup⁡Q∈Bε,2(P^N)EQ[∥x−ψ(y)∥22].(35)\inf_{\psi \in \Psi} \sup_{Q \in B_{\varepsilon,2}(\hat P_N)} E_Q\big[\|x-\psi(y)\|_2^2\big]. \tag{35}ψ∈Ψinf​Q∈Bε,2​(P^N​)sup​EQ​[∥x−ψ(y)∥22​].(35)

Writing Σ^=(Σ^xxΣ^xyΣ^yxΣ^yy)\hat\Sigma = \begin{pmatrix}\hat\Sigma_{xx}&\hat\Sigma_{xy}\\\hat\Sigma_{yx}& \hat\Sigma_{yy}\end{pmatrix}Σ^=(Σ^xx​Σ^yx​​Σ^xy​Σ^yy​​) blockwise, the nonlinear convex SDP

max⁡Sf(S)=Tr[Sxx−SxySyy−1Syx]s.t.S=(SxxSxySyxSyy)⪰0,  Sxx⪰0,  Syy⪰0,  Tr[S+Σ^−2(Σ^1/2SΣ^1/2)1/2]≤ε2,  S⪰λmin⁡(Σ^)I(36)\max_S f(S) = \mathrm{Tr}[S_{xx} - S_{xy}S_{yy}^{-1}S_{yx}] \quad \text{s.t.} \quad S = \begin{pmatrix}S_{xx}&S_{xy}\\S_{yx}&S_{yy}\end{pmatrix} \succeq 0,\; S_{xx} \succeq 0,\; S_{yy} \succeq 0,\; \mathrm{Tr}[S+\hat\Sigma-2(\hat\Sigma^{1/2}S\hat\Sigma^{1/2})^{1/2}] \le \varepsilon^2,\; S \succeq \lambda_{\min}(\hat\Sigma) I \tag{36}Smax​f(S)=Tr[Sxx​−Sxy​Syy−1​Syx​]s.t.S=(Sxx​Syx​​Sxy​Syy​​)⪰0,Sxx​⪰0,Syy​⪰0,Tr[S+Σ^−2(Σ^1/2SΣ^1/2)1/2]≤ε2,S⪰λmin​(Σ^)I(36)

is the finite-dimensional relaxation the chapter builds toward.

Formalization targets

Goal (Theorem 25, distributionally robust MMSE estimator). If Σ^≻0\hat\Sigma \succ 0Σ^≻0, then the optimal value of problem (35) equals the optimal value of SDP (36). Moreover, if S⋆S^\starS⋆ is optimal in (36) with Syy⋆S^\star_{yy}Syy⋆​ invertible, then the affine function

ψ⋆(y)=Sxy⋆(Syy⋆)−1(y−μ^y)+μ^x\psi^\star(y) = S^\star_{xy}(S^\star_{yy})^{-1}(y-\hat\mu_y) + \hat\mu_xψ⋆(y)=Sxy⋆​(Syy⋆​)−1(y−μ^​y​)+μ^​x​

attains the outer infimum of (35) — it is a distributionally robust MMSE estimator, exhibited in closed form from an SDP optimizer.

Significance

Theorem 25 reduces an a priori infinite-dimensional, worst-case functional optimization problem (an infimum over all measurable estimators of a supremum over all distributions within a Wasserstein ball) to a finite convex program with one linear matrix inequality, one Loewner-order lower bound, and one trace/matrix-square-root constraint — solvable in polynomial time, with the optimal estimator recovered in closed form from the SDP's optimal block matrix. It shows that robustifying MMSE estimation against distributional ambiguity does not sacrifice tractability: the resulting estimator remains affine, the same functional form as the classical (non-robust) best linear unbiased estimator, only with its coefficients drawn from a regularized covariance estimate rather than the raw sample covariance. Formalizing it fixes, machine-checkably, the exact shape of that regularization — which SDP constraints are load-bearing (the Loewner lower bound in particular rules out a numerically unstable near-singular SyyS_{yy}Syy​) and which conditions (Σ^≻0\hat\Sigma \succ 0Σ^≻0, Syy⋆S^\star_{yy}Syy⋆​ invertible) the closed-form estimator formula actually needs.

Difficulty

The paper's own remark (p. 29) names the two nontrivial steps: first, "establishing a minimax theorem for (35) and exploiting the properties of elliptical distributions" to show the outer infimum is attained by an affine estimator — a priori (35) ranges over all measurable ψ\psiψ, and there is no obvious reason the worst case forces linearity. Second, "combining this structural insight with Theorem 16" (the SDP-representability result for indefinite quadratic losses under an elliptical nominal distribution, itself a nontrivial closed-form reduction of an infinite-dimensional worst-case risk) to convert the now-restricted problem over affine estimators into the finite SDP (36). Neither step is a routine consequence of the ambiguity-set definitions alone; each requires structural facts about elliptical distributions and quadratic losses proved earlier in the chapter.

Formalization scope

The signal-observation space is EuclideanSpace ℝ (Fin mx ⊕ Fin my), with xxx and yyy recovered as the two summand projections; the block matrix SSS is Matrix (Fin mx ⊕ Fin my) (Fin mx ⊕ Fin my) ℝ, and Matrix.toBlocks₁₁/toBlocks₁₂/toBlocks₂₁/toBlocks₂₂ give its four blocks. The constraint "Sxy=Syx⊤S_{xy}=S_{yx}^\topSxy​=Syx⊤​" is not stated as a separate hypothesis: it follows automatically once SSS is symmetric (implied by S.PosSemidef), so encoding the feasible set from a single symmetric S rather than four independently-quantified blocks makes it structurally impossible to drop — see pitfall 4 of BRIEF.md. The outer infimum of problem (35) ranges only over measurable ψ\psiψ (Measurable ψ on the binder), matching the paper's own definition of Ψ\PsiΨ as "the family of all possible measurable estimators" (p. 29) exactly. λ_min(Σ̂) is taken as a hypothesis parameter characterized by the two properties that make it the minimum ("≤ every eigenvalue of Σ̂, and attained by some eigenvalue"), rather than invoking a specific Mathlib min-eigenvalue API by name. S_{yy}⁻¹ uses the ordinary matrix inverse (junk zero matrix when singular), matching the paper's literal notation; S^\star_{yy} invertible is stated as an added hypothesis, not present verbatim on the page, because the paper leaves the formula's well-definedness implicit — disclosed per pitfall 5 rather than silently assumed away. The paper's own "which is always solvable" clause is not asserted: Theorem 25 states, as part of itself, that SDP (36) attains its maximum (an unconditional existence claim for an optimal S⋆S^\starS⋆); this formalization states only the conditional consequences of such an S⋆S^\starS⋆ existing, not that one does — proving or asserting solvability is out of this mission's scope, so the Lean statement is strictly weaker than Theorem 25's own conclusion on this point, disclosed rather than silently dropped. All risk-style suprema are EReal-valued and Integrable-guarded, matching the series' convention. No milestone theorem is included: the paper's own proof sketch derives (33)'s and by extension (36)'s SDP "via Theorem 16", but Theorem 16 (indefinite quadratic loss and p=2p=2p=2, eq. 23) was itself judged too heavy to state faithfully in 02-gelbrich's time budget and is not redefined here either — see STATUS.md. Theorem 24 (the Wasserstein shrinkage estimator, this chapter's originally recommended goal) is out of scope: its closed-form eigenvalue transformation (eq. 34a/34b) requires transcribing nested square roots from a rendered PDF page that this session's time budget did not allow verifying to the standard the brief demands (pitfall 1); the brief's own documented fallback to Theorem 25 was taken instead.

Selected references

  • Kuhn, D., Mohajerin Esfahani, P., Nguyen, V. A., & Shafieezadeh-Abadeh, S. (2019). Wasserstein Distributionally Robust Optimization: Theory and Applications in Machine Learning. INFORMS TutORials in Operations Research. https://doi.org/10.1287/educ.2019.0198
  • Nguyen, V. A., Shafieezadeh-Abadeh, S., Yue, M.-C., Kuhn, D., & Wiesemann, W. (2021). Optimistic distributionally robust optimization for nonparametric likelihood approximation. Advances in Neural Information Processing Systems, 32.
  • Shafieezadeh-Abadeh, S., Nguyen, V. A., Kuhn, D., & Mohajerin Esfahani, P. (2018). Wasserstein distributionally robust Kalman filtering. Advances in Neural Information Processing Systems, 31.
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Machine LearningOperations ResearchOptimization·Captain: mikedeng1

Wasserstein Distributionally Robust Optimization II: The Gelbrich Ambiguity Set and Elliptical TractabilityTextbook

Motivation

Distributionally robust optimization (DRO) hedges a decision against every distribution within some ambiguity set around an estimated (nominal) distribution, rather than trusting the estimate exactly. When the ambiguity set is a ball of radius ε\varepsilonε around the empirical distribution P^N\hat P_NP^N​ in the type-ppp Wasserstein metric, the resulting worst-case risk problem inherits attractive statistical guarantees (Mohajerin Esfahani & Kuhn 2018) but is, in general, an optimization problem over an infinite-dimensional space of measures. Kuhn, Mohajerin Esfahani, Nguyen & Shafieezadeh-Abadeh's 2019 INFORMS TutORials chapter surveys when this problem becomes computationally tractable. One route — the subject of this mission — discards everything about the nominal distribution except its mean vector and covariance matrix and replaces the Wasserstein ball with a set built only from these two moments, the Gelbrich hull. The construction is due to Gelbrich (1990), who first bounded the Wasserstein distance between two distributions using only their means and covariances.

Setting

Fix Ξ⊆Rm\Xi \subseteq \mathbb{R}^mΞ⊆Rm, a nominal distribution P^N∈P(Ξ)\hat P_N \in \mathcal{P}(\Xi)P^N​∈P(Ξ), a radius ε>0\varepsilon > 0ε>0 and an exponent p≥1p \ge 1p≥1. The type-ppp Wasserstein distance between two probability measures Q,Q′Q, Q'Q,Q′ on Rm\mathbb{R}^mRm is

Wp(Q,Q′)=(inf⁡π∈Π(Q,Q′)∫∥ξ−ξ′∥p dπ(ξ,ξ′))1/p,W_p(Q,Q') = \Big(\inf_{\pi \in \Pi(Q,Q')} \int \|\xi-\xi'\|^p \, d\pi(\xi,\xi')\Big)^{1/p},Wp​(Q,Q′)=(π∈Π(Q,Q′)inf​∫∥ξ−ξ′∥pdπ(ξ,ξ′))1/p,

the infimum over couplings π\piπ (probability measures on Rm×Rm\mathbb{R}^m \times \mathbb{R}^mRm×Rm with marginals QQQ and Q′Q'Q′) of the ppp-th root of the expected ppp-th power of Euclidean distance. The Wasserstein ambiguity set is Bε,p(P^N)={Q∈P(Ξ):Wp(Q,P^N)≤ε}B_{\varepsilon,p}(\hat P_N) = \{Q \in \mathcal{P}(\Xi) : W_p(Q,\hat P_N) \le \varepsilon\}Bε,p​(P^N​)={Q∈P(Ξ):Wp​(Q,P^N​)≤ε}, and the worst-case risk of a loss function ℓ\ellℓ is Rε,p(P^N,ℓ)=sup⁡Q∈Bε,p(P^N)EQ[ℓ(ξ)]R_{\varepsilon,p}(\hat P_N,\ell) = \sup_{Q \in B_{\varepsilon,p}(\hat P_N)} E_Q[\ell(\xi)]Rε,p​(P^N​,ℓ)=supQ∈Bε,p​(P^N​)​EQ​[ℓ(ξ)].

Suppose P^N\hat P_NP^N​ has mean vector μ^\hat\muμ^​ and covariance matrix Σ^∈S+m\hat\Sigma \in S^m_+Σ^∈S+m​ (the positive semidefinite m×mm\times mm×m matrices). The mean-covariance uncertainty set is

Uε(μ^,Σ^)={(μ,Σ)∈Rm×S+m:∥μ^−μ∥22+Tr[Σ^+Σ−2(Σ^1/2ΣΣ^1/2)1/2]≤ε2},U_\varepsilon(\hat\mu,\hat\Sigma) = \Big\{(\mu,\Sigma) \in \mathbb{R}^m \times S^m_+ : \|\hat\mu-\mu\|_2^2 + \mathrm{Tr}\big[\hat\Sigma+\Sigma-2(\hat\Sigma^{1/2}\Sigma\hat\Sigma^{1/2})^{1/2}\big] \le \varepsilon^2\Big\},Uε​(μ^​,Σ^)={(μ,Σ)∈Rm×S+m​:∥μ^​−μ∥22​+Tr[Σ^+Σ−2(Σ^1/2ΣΣ^1/2)1/2]≤ε2},

where Σ1/2\Sigma^{1/2}Σ1/2 is the positive-semidefinite square root. The Gelbrich hull is Gε(μ^,Σ^)={Q∈P(Ξ):(EQ[ξ],CovQ[ξ])∈Uε(μ^,Σ^)}G_\varepsilon(\hat\mu,\hat\Sigma) = \{Q \in \mathcal{P}(\Xi) : (E_Q[\xi],\mathrm{Cov}_Q[\xi]) \in U_\varepsilon(\hat\mu,\hat\Sigma)\}Gε​(μ^​,Σ^)={Q∈P(Ξ):(EQ​[ξ],CovQ​[ξ])∈Uε​(μ^​,Σ^)}: the distributions on Ξ\XiΞ whose own mean and covariance lie in Uε(μ^,Σ^)U_\varepsilon(\hat\mu,\hat\Sigma)Uε​(μ^​,Σ^). An elliptical distribution Eg(μ,Σ)E_g(\mu,\Sigma)Eg​(μ,Σ) has density f(ξ)=C⋅det⁡(Σ)−1g((ξ−μ)⊤Σ−1(ξ−μ))f(\xi) = C \cdot \det(\Sigma)^{-1} g\big((\xi-\mu)^\top\Sigma^{-1}(\xi-\mu)\big)f(ξ)=C⋅det(Σ)−1g((ξ−μ)⊤Σ−1(ξ−μ)) for a density generator ggg and normalizing constant CCC; two elliptical distributions "have the same density generator" when their ggg coincide (e.g. both Gaussian, both Student-tνt_\nutν​ for the same ν\nuν).

Formalization targets

Goal (Theorem 13, Gelbrich hull). For every p≥2p \ge 2p≥2,

Bε,p(P^N)⊆Gε(μ^,Σ^).B_{\varepsilon,p}(\hat P_N) \subseteq G_\varepsilon(\hat\mu,\hat\Sigma).Bε,p​(P^N​)⊆Gε​(μ^​,Σ^).

This is an outer approximation: every distribution within ε\varepsilonε of P^N\hat P_NP^N​ in Wasserstein distance has a mean and covariance inside Uε(μ^,Σ^)U_\varepsilon(\hat\mu,\hat\Sigma)Uε​(μ^​,Σ^), so optimizing over the Gelbrich hull instead of the Wasserstein ball can only enlarge the feasible set, never shrink it below the truth.

Supporting results. Theorem 4 (Gelbrich bound) gives the moment-only lower bound on W2W_2W2​ that Theorem 13 is built from, with equality for elliptical distributions sharing a generator. Proposition 1 sharpens the goal's containment to an equality on the mean-covariance projection itself, under the same two conditions (Ξ=Rm\Xi = \mathbb{R}^mΞ=Rm, P^N\hat P_NP^N​ elliptical). Corollary 1 propagates the goal's set containment to the risk level: Rε,p(P^N,ℓ)≤Rε(μ^,Σ^,ℓ)R_{\varepsilon,p}(\hat P_N,\ell) \le R_\varepsilon(\hat\mu,\hat\Sigma,\ell)Rε,p​(P^N​,ℓ)≤Rε​(μ^​,Σ^,ℓ) for every ℓ\ellℓ, where Rε(μ^,Σ^,ℓ)=sup⁡Q∈Gε(μ^,Σ^)EQ[ℓ(ξ)]R_\varepsilon(\hat\mu,\hat\Sigma,\ell) = \sup_{Q \in G_\varepsilon(\hat\mu,\hat\Sigma)} E_Q[\ell(\xi)]Rε​(μ^​,Σ^,ℓ)=supQ∈Gε​(μ^​,Σ^)​EQ​[ℓ(ξ)] is the Gelbrich risk.

Significance

Theorem 13 is the hinge between an intractable infinite-dimensional worst-case-risk problem and a tractable one: the paper goes on (Theorem 16, outside this mission's scope) to show that for quadratic loss functions and elliptical nominal distributions the Gelbrich risk itself equals the optimal value of a semidefinite program with two linear matrix inequality constraints — and that, under those same conditions, the Wasserstein worst-case risk, the Gelbrich risk and the SDP value all coincide. Corollary 1 is what makes the Gelbrich risk usable as a conservative surrogate even outside that special case: it upper-bounds the true worst-case risk for any loss function and any p≥2p \ge 2p≥2, at the cost of discarding all but first- and second-order information about the nominal distribution. Formalizing the goal and Corollary 1 gives the exact scope in which this moment-relaxation is licensed — the p≥2p \ge 2p≥2 restriction and the outer-approximation direction are both easy to get backwards, and this mission's Lean encoding fixes both irreversibly.

Difficulty

The obvious first argument is to prove containment pointwise: fix Q∈Bε,p(P^N)Q \in B_{\varepsilon,p}(\hat P_N)Q∈Bε,p​(P^N​) and show its mean and covariance land in Uε(μ^,Σ^)U_\varepsilon(\hat\mu,\hat\Sigma)Uε​(μ^​,Σ^). That reduces Theorem 13 to Proposition 1's containment half, which in turn reduces to the Gelbrich bound (Theorem 4) applied to the pair (Q,P^N)(Q,\hat P_N)(Q,P^N​) — the inequality direction of Theorem 4 suffices for containment; only the sharper equality direction (needed for Proposition 1's own equality clause) requires the elliptical hypothesis. The non-obvious step is Theorem 4 itself: bounding W2(Q,Q′)W_2(Q,Q')W2​(Q,Q′) below by a closed-form expression in the two distributions' first two moments only, for arbitrary Q,Q′Q,Q'Q,Q′ with those moments, requires an argument that survives every coupling π\piπ — the paper's proof goes through a lower bound on the coupling's cross-covariance term via the eigenvalues of Σ1/2Σ′Σ1/2\Sigma^{1/2}\Sigma'\Sigma^{1/2}Σ1/2Σ′Σ1/2, not a direct manipulation of W2W_2W2​'s definition.

Formalization scope

Rm\mathbb{R}^mRm is EuclideanSpace ℝ (Fin m); a "distribution" is a MeasureTheory.Measure on it constrained by Q Set.univ = 1 (probability) and Q Ξᶜ = 0 (support in Ξ). The Wasserstein distance is ENNReal-valued (Definition 1's infimum over couplings, matching 01-duality's convention); the worst-case and Gelbrich risks are EReal-valued suprema restricted to loss functions integrable under the candidate distribution, avoiding Mathlib's junk value for a non-integrable Bochner integral. Σ1/2\Sigma^{1/2}Σ1/2 is the positive-semidefinite matrix square root, picked by choice from its defining existential and applied in this mission only to matrices hypothesized (or, per Section 2.3's standing assumption, given) positive semidefinite. Elliptical distributions (IsElliptical) are represented by the paper's own density formula (a measure equal to volume.withDensity of C·det(Σ)⁻¹·g((ξ-μ)ᵀΣ⁻¹(ξ-μ)) for some C>0), together with the mean/covariance facts every theorem in this chunk reads off directly; an earlier draft kept only the latter, under which "same density generator" held vacuously for any moment-matched pair — corrected after moderation flagged it (see STATUS.md). Because 01-duality (Wasserstein distance, ambiguity set, worst-case risk) is not yet a published mission, this chunk redefines those objects locally in its own namespace rather than importing an unpublished draft, per the series' definition-reuse policy; a future upload can retire the duplication once 01-duality is live. A formalization that dropped Theorem 4's "same density generator" condition from its equality clause, or that stated the goal's containment for all p≥1p\ge 1p≥1 rather than p≥2p \ge 2p≥2, would be trivializing or simply false — both are explicit hypotheses in the Lean statements. Matrix.PosSemidef and its Loewner order carry the S+mS^m_+S+m​ constraints; no elliptical-distribution or Gelbrich-hull infrastructure exists elsewhere on the platform, so this mission's definitions are original contributions reusable by any later extension (Theorem 16/17, Lemma 1/2's SDP representations) of this series.

Selected references

  • Kuhn, D., Mohajerin Esfahani, P., Nguyen, V. A., & Shafieezadeh-Abadeh, S. (2019). Wasserstein Distributionally Robust Optimization: Theory and Applications in Machine Learning. INFORMS TutORials in Operations Research. https://doi.org/10.1287/educ.2019.0198
  • Gelbrich, M. (1990). On a formula for the L2 Wasserstein metric between measures on Euclidean and Hilbert spaces. Mathematische Nachrichten, 147(1), 185–203.
  • Mohajerin Esfahani, P., & Kuhn, D. (2018). Data-driven distributionally robust optimization using the Wasserstein metric: performance guarantees and tractable reformulations. Mathematical Programming, 171(1), 115–166.
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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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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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Introduction to Stochastic Programming VII: Convergence Rates for Sample Average ApproximationTextbook

Motivation

Most stochastic programs cannot be solved exactly: the expectation defining the objective is an integral over a continuous or high-dimensional random parameter, and evaluating it exactly is as hard as the optimization itself. The standard remedy is Monte Carlo: draw a sample of size ν from the random parameter, replace the true expectation by the sample average, and solve the resulting finite-dimensional "sample average approximation" (SAA) instead. This only helps if the SAA's optimal value and optimal solution actually converge to the true problem's as ν → ∞, and if that convergence is fast enough to be useful with a sample size one can actually draw and solve. Birge & Louveaux's Chapter 9, §9.5, states the two central asymptotic results that justify this approach for a general (not necessarily linear, not necessarily two-stage) stochastic program: a central limit theorem describing the SAA optimal value's fluctuations around the truth (Theorem 6, after Shapiro [1991]), and an exponential-rate large-deviation bound on how quickly both the SAA value and the SAA solution concentrate near their true counterparts as the sample grows (Theorem 7, after Dai, Chen & Birge [2000]). This mission formalizes both statements.

Setting

Fix a feasible set X ⊆ ℝⁿ of first-stage decisions and an outcome space Ξ carrying a σ-algebra. The book considers the general stochastic program

z* = inf_{x ∈ X} ∫_Ξ g(x,ξ) P(dξ),                                                        (5.1)

with g : ℝⁿ × Ξ → ℝ an abstract integrand — no longer specialized to the two-stage recourse cost Q(x,ξ) of Chapters 3–7, matching the book's own level of generality at this point in §9.5 — and ξ a random element of (Ξ, 𝓑, P). Given an i.i.d. sample ξ₁, ξ₂, … from P, the sample average approximation of size ν is

zν = inf_{x ∈ X} (1/ν) Σᵢ₌₁^ν g(x,ξᵢ) .                                                    (5.2)

Both z* and zν are attained (an optimal solution x* of (5.1); a random optimal solution xν(ω) of (5.2) at each sample outcome ω). The two chapter results describe, in different regimes, how (zν, xν) relates to (z*, x*) as ν → ∞.

Formalized in this mission: X sits in EuclideanSpace ℝ (Fin n); the sample is a sequence ξ : ℕ → Ω → Ξ on an ambient probability space (Ω, P), independent and identically distributed (Mathlib's iIndepFun/IdentDistrib); z*, x*, zν, xν are given as hypotheses that pin them down as the optimal value and an optimal point of (5.1)/(5.2) (a lower bound over X plus attainment at the named point), rather than computed via sInf/sSup of an image set — Real's extended-real infimum returns the junk value 0 on an unbounded-below or empty set, which would silently misstate the theorems if X, g are only assumed as loosely as the book states them.

Formalization targets

Goal — Chapter 9, Theorem 7 (p. 412)

∀ ε>0, ∃ α>0, ∃ β>0,
  (∀ ν>0, P[|zν − z*| ≥ ε] ≤ α·e^{−βν})
  ∧ (x* the unique optimal solution of (5.1) → ∀ ν≥1, P[‖xν − x*‖ ≥ ε] ≤ α·e^{−βν})

under the moment hypothesis: there exist a>0, θ₀>0, η : Ξ → ℝ with |g(x,ξ)| ≤ a·η(ξ) for all x ∈ X, and E[e^{θ·η(ξ)}] < ∞ for every θ ∈ [0,θ₀]. This is the mission's goal because it is a clean, self-contained existential-constants statement — no algorithm to define, unlike most of the chapter's other convergence results — and because, like Chunk 03's Theorem 6(a), the book's own proof cites an external paper (Dai, Chen & Birge [2000], Theorems 3.1–3.2) and gives no in-text derivation: the statement itself, not a derivation from a preceding numbered result of this book, is the mission's content.

Milestone — Chapter 9, Theorem 6 (p. 411)

X compact, g(x,·) measurable ∀x∈X, g Lipschitz in x with an L²(μ) envelope a,
x0 the unique minimizer of x ↦ E g(x) over X
  ⟹ √ν·[zν − E g(x0)] converges in distribution to N(0, Var g(x0))

Included as a milestone (not used in Theorem 7's proof, which the book does not give — see above) because it is the chapter's other general SAA convergence result, standing on the same setup (5.1)–(5.2), and because Mathlib's MeasureTheory.Function.ConvergenceInDistribution (the TendstoInDistribution predicate) plus Probability.Distributions.Gaussian.Real (gaussianReal) and Mathlib's own i.i.d. central limit theorem (ProbabilityTheory.tendstoInDistribution_inv_sqrt_mul_sum_sub) supply exactly the vocabulary needed to state — not prove — a faithful weak-convergence-to-Gaussian conclusion. Chunk 09's BRIEF.md flagged this as a milestone to attempt "only if your workspace has enough of a weak-convergence/CLT toolkit in Mathlib to state it faithfully"; the toolkit is present (verified directly, not assumed from substrate.md, which predates this rev's addition of ConvergenceInDistribution.lean), so it is included.

Significance

Every practical Monte Carlo solution method for stochastic programming — every discretization, every scenario-reduction heuristic, every "solve on a sample and hope" approach used throughout the rest of the book and the wider literature — rests on exactly these two results: that the SAA converges at all (Theorem 6's CLT gives the asymptotic distribution of the error) and that it converges fast enough to bound the error at a finite, computable sample size (Theorem 7's exponential rate). Formalizing them gives Prove2Me a first foothold in convergence-rate theory for stochastic optimization under sampling, a genre distinct from the concentration-of-measure results already reachable via Mathlib's sub-Gaussian machinery (Probability/Moments/SubGaussian.lean): sub-Gaussian concentration bounds a fixed-size sample's deviation from its own mean, not the rate-in-ν convergence of a nested sequence of optimization problems' values and solutions to a limiting problem's — the object Theorem 7 is actually about.

Difficulty

Theorem 6 needs a functional/uniform argument over the whole feasible set X (not the plain i.i.d. CLT at the single point x0) to control the interaction between sampling noise and the optimization over x; the book states it without proof, citing Shapiro [1991]. Theorem 7's constants α, β are produced by a large-deviation argument specific to the exponential-moment condition, again cited rather than derived in the book. Both are left as sorry; the value of this mission is the faithful statement, matching the difficulty pattern already established for Chunk 03's Theorem 6(a) (a result the book itself only cites).

Formalization scope

  • Existential constants left abstract, never sharpened or weakened. Theorem 7's α, β are ∃-bound exactly as the book leaves them (trap 8 of reference/FAITHFULNESS_TRAPS.md: the existentials sit outside every quantifier they must be uniform over — in particular outside the ∀ ν). No closed form for α, β in terms of a, θ0, ε is invented.
  • The book's own typo is corrected, and the correction is flagged. The printed (5.8) reads P[E[zν − z*)] ≥ ε] ≤ αe^{−βν} — an unmatched parenthesis and a stray E[·] around a quantity that is already deterministic. milestones.yaml/MODERATION_NOTES.md quote the typo verbatim; the Lean and natural_language_statement use the unambiguous P[|zν − z*| ≥ ε] the surrounding prose (and every other occurrence of this quantity in the section) plainly intends.
  • g is left fully abstract, not specialized to the two-stage recourse cost Q(x,ξ) of Chunks 03–07, matching §9.5's own generality and keeping this mission independent of every other chunk's namespace (no cross-chunk import, per missions/README.md's "Prior art" column for this chunk: "none expected").
  • z*, x*, zν, xν are hypothesis-characterized, not sInf/sSup-defined, to avoid the real extended-value junk-value trap (trap 5) discussed under Setting above.
  • Measurability of zν, xν is an added hypothesis (hzSAA_meas/hxSAA_meas/hzSAA_meas in Theorem 6), not derivable from the other hypotheses since g is abstract; the book is silent on this technical point, standard for an applied convergence theorem, but Lean's P {ω | …} needs it for the displayed probability to be the actual measure of the event rather than an outer-measure value on a possibly non-measurable set.
  • Convergence in distribution (Theorem 6) is formalized via Mathlib's TendstoInDistribution, with the limiting Gaussian supplied as an explicit random variable Y on a separate probability space with HasLaw Y (gaussianReal 0 σ²) P' — the same pattern Mathlib's own CLT (tendstoInDistribution_inv_sqrt_mul_sum_sub) uses for its own conclusion.
  • Trivialization risk (this chapter's own, beyond paper.md's book-wide list item 5). A formalization that quantifies α, β universally, or with an invented closed form, would assert something the book's proof (cited, not given) does not establish; a formalization of Theorem 7 that used a computable sInf-defined zν on a set that is not shown bounded below would let the conclusion hold vacuously via the junk value 0, independent of the genuine large-deviation content — both are excluded by the choices above.

Selected references

  • Birge, J.R., Louveaux, F. Introduction to Stochastic Programming, 2nd ed., Springer 2011, Chapter 9, §9.5 (pp. 409–412).
  • Shapiro, A. "Asymptotic properties of statistical estimators in stochastic programming." Annals of Statistics 19 (1991), 1463–1466 — proof of Theorem 6 (their Theorem 3.3).
  • Dai, L., Chen, C.-H., Birge, J.R. "Convergence properties of two-stage stochastic programming." Journal of Optimization Theory and Applications 106 (2000), 489–509 — proof of Theorem 7 (their Theorems 3.1–3.2).
  • King, A.J., Rockafellar, R.T. "Asymptotic theory for solutions in statistical estimation and stochastic programming." Mathematics of Operations Research 18 (1993), 148–162 — the general theory of §9.5's opening (Theorem 5), the chapter's third general result, not formalized here (see STATUS.md for why it is out of scope).
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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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🏆Completed
Statistics·Captain: burkh4rt

Discriminative Kalman Filter asymptoticsResearch Paper

Motivation

Bayesian filtering estimates an unobserved state from measurements arriving over time. A filter combines what the state dynamics predict with what the newest observation says. In neural decoding, for example, the state may describe an intended movement while the observation contains activity from many recorded neurons. The observation can have many more coordinates than the state and need not follow a linear Gaussian observation model.

The Discriminative Kalman Filter (DKF) uses a Gaussian approximation to the state conditional on the newest observation. It combines that approximation with a Gaussian state transition and a correction for the stationary state distribution. The resulting recursion retains a mean vector and covariance matrix. Burkhart et al. developed this construction and proved an asymptotic justification in Theorem 2 of Appendix B.

The historical starting point is the linear Gaussian filter of Kalman (1960). The 2020 DKF paper changes how observation information enters the update and establishes a corresponding approximation theorem. The present mission concerns formal verification of that published theorem.

Setting

The state space is Rd\mathbb R^dRd for a positive finite dimension ddd. Write ηd(z;m,C)\eta_d(z;m,C)ηd​(z;m,C) for the ordinary multivariate Gaussian density with mean mmm and symmetric positive-definite covariance CCC. Densities and their L1L^1L1 distances are with respect to Lebesgue measure.

The state model has a matrix AAA and positive-definite covariance matrices Γ,S\Gamma,SΓ,S satisfying

S=ASA⊤+Γ.S=ASA^\top+\Gamma.S=ASA⊤+Γ.

Its stationary density and transition density are

p(z)=ηd(z;0,S),τ(y,z)=ηd(z;Ay,Γ).p(z)=\eta_d(z;0,S),\qquad \tau(y,z)=\eta_d(z;Ay,\Gamma).p(z)=ηd​(z;0,S),τ(y,z)=ηd​(z;Ay,Γ).

For an integrable density sss, prediction gives

(τs)(z)=∫τ(y,z)s(y) dy.(\tau s)(z)=\int\tau(y,z)s(y)\,dy.(τs)(z)=∫τ(y,z)s(y)dy.

The discriminative update combines a previous filtering density sss with a density uuu for the state given the current observation:

u τs/p∥u τs/p∥1.\frac{u\,\tau s/p}{\|u\,\tau s/p\|_1}.∥uτs/p∥1​uτs/p​.

This expression is a probability density when its nonnegative weight has a finite, strictly positive integral. Dividing by ppp is part of the standard DKF under consideration.

For Gaussian inputs with parameters (a,V)(a,V)(a,V) and (b,U)(b,U)(b,U), define

G=AVA⊤+Γ,T=(U−1+G−1−S−1)−1,G=AVA^\top+\Gamma,\qquad T=(U^{-1}+G^{-1}-S^{-1})^{-1},G=AVA⊤+Γ,T=(U−1+G−1−S−1)−1, c=T(U−1b+G−1Aa).c=T(U^{-1}b+G^{-1}Aa).c=T(U−1b+G−1Aa).

The DKF step returns mean ccc and covariance TTT when the precision is invertible and the covariance is positive definite. The recursive filter starts from mean zero and covariance SSS, using the current observation's functions fff and QQQ as the Gaussian input mean and covariance. These are the updates in equation (2.7) of the paper.

Formalization targets

Fix sequences of probability densities sn,uns_n,u_nsn​,un​, indexed by positive integers, whose exact normalized updates

pn=unτsn/p∥unτsn/p∥1p_n=\frac{u_n\tau s_n/p}{\|u_n\tau s_n/p\|_1}pn​=∥un​τsn​/p∥1​un​τsn​/p​

are well defined for every index. Fix Gaussian density sequences sn′,un′s'_n,u'_nsn′​,un′​, a point bbb, and a probability measure PPP. The five assumptions are

A1:sn⇒P,A2:∥sn−sn′∥1⟶0,A3:un⇒δb,A4:∥un−un′∥1⟶0,A5:pn⇒δb.\begin{aligned} \mathrm{A1}:&\quad s_n\Rightarrow P,\\ \mathrm{A2}:&\quad \|s_n-s'_n\|_1\longrightarrow0,\\ \mathrm{A3}:&\quad u_n\Rightarrow\delta_b,\\ \mathrm{A4}:&\quad \|u_n-u'_n\|_1\longrightarrow0,\\ \mathrm{A5}:&\quad p_n\Rightarrow\delta_b. \end{aligned}A1:A2:A3:A4:A5:​sn​⇒P,∥sn​−sn′​∥1​⟶0,un​⇒δb​,∥un​−un′​∥1​⟶0,pn​⇒δb​.​

Here ⇒\Rightarrow⇒ denotes weak convergence, characterized by convergence of expectations of every bounded continuous real function; δb\delta_bδb​ is the unit point mass at bbb. The measure PPP need not have a density and may be degenerate.

The main goal is the complete conjunction of Theorem 2's conclusions, with separate milestones for each:

  • C1: sn′⇒Ps'_n\Rightarrow Psn′​⇒P.
  • C2: un′⇒δbu'_n\Rightarrow\delta_bun′​⇒δb​.
  • C3: the specific update
pn′=un′τsn′/p∥un′τsn′/p∥1p'_n=\frac{u'_n\tau s'_n/p}{\|u'_n\tau s'_n/p\|_1}pn′​=∥un′​τsn′​/p∥1​un′​τsn′​/p​

is a well-defined Gaussian density for all sufficiently large nnn.

  • C4: pn′⇒δbp'_n\Rightarrow\delta_bpn′​⇒δb​.
  • C5: ∥pn−pn′∥1⟶0\|p_n-p'_n\|_1\longrightarrow0∥pn​−pn′​∥1​⟶0.

A sixth milestone is Lemma 1 (DKF equation): the normalized Gaussian-input update has the explicit mean and covariance above whenever valid, and the two input weak limits imply its eventual validity and convergence to δb\delta_bδb​. It includes both the exact equation and the asymptotic assertion from the source.

Significance

In addition to neurodecoding with intracortical brain-computer interfaces, the DKF has also found applications in optimization and sequential data augmentation (see references). The original study was successfully reproduced by Casco-Rodriguez, et al. in ReScience C.

Difficulty

The inverse stationary density can grow in the tails, so small L1L^1L1 errors in the input densities do not immediately control the error after division and renormalization. Normalizing constants must remain finite and nonzero. The candidate Gaussian covariance must also become positive definite as a conclusion of the assumptions, rather than through an extra validity assumption imposed at every index.

There is a second distinction between convergence to a point mass and approximation in L1L^1L1. Two sequences may concentrate at the same point while retaining different shapes at shrinking scales. The C5 target therefore requires the full approximation argument, beyond the weak-convergence conclusions.

Formalization scope

Lean represents states as Fin d → ℝ and covariance matrices as real square matrices. The Gaussian density is the standard determinant-and-quadratic-form formula. The definition of Gaussian PDF includes positive-definite covariance and equality of densities almost everywhere. Thus null-set changes do not constrain the theorem artificially.

Probability density validity explicitly includes nonnegativity almost everywhere, integrability and total integral one. The L1L^1L1 quantity is an extended nonnegative integral. The update's validity explicitly requires measurable weight and a finite, strictly positive normalizer. Total expressions outside that domain supply no assumed probability interpretation; C3 establishes validity on a tail.

All density sequences use positive integer indices. The limit measure is a Mathlib probability measure. Weak convergence is tested against Mathlib bounded continuous functions using the actual measures generated by the densities. The stationary model, standard recursive DKF, exact update and approximate update are defined independently of the theorem conclusions.

The mission addresses deterministic Theorem 2 of Appendix B. The random-sequence extension in Remark 4, conditions implying a Bernstein–von Mises theorem, and induction over filtering time are separate developments. The proof plan follows the appendix through C1–C2, Lemma 1, C3–C4, and the five-term comparison for C5.

Selected references

  • M. C. Burkhart, D. M. Brandman, B. Franco, L. R. Hochberg and M. T. Harrison, The Discriminative Kalman Filter for Bayesian Filtering with Nonlinear and Nongaussian Observation Models, Neural Computation 32(5), 969–1017, 2020. DOI: 10.1162/neco_a_01275.
  • R. E. Kalman, A New Approach to Linear Filtering and Prediction Problems, Journal of Basic Engineering 82(1), 35–45, 1960. DOI: 10.1115/1.3662552.
  • M. C. Burkhart, A Discriminative Approach to Bayesian Filtering with Applications to Human Neural Decoding, Ph.D. dissertation, Brown University, 2019. DOI: 10.26300/nhfp-xv22.
  • D. M. Brandman, M. C. Burkhart, J. Kelemen, B. Franco, M. T. Harrison and L. R. Hochberg, Robust Closed-Loop Control of a Cursor in a Person with Tetraplegia using Gaussian Process Regression, Neural Computation 30(11), 2986–3008, 2018. DOI: 10.1162/neco_a_01129.
  • D. M. Brandman, T. Hosman, J. Saab, M. C. Burkhart, B. E. Shanahan, J. G. Ciancibello et al., Rapid calibration of an intracortical brain–computer interface for people with tetraplegia, Journal of Neural Engineering 15(2), 026007, 2018. DOI: 10.1088/1741-2552/aa9ee7.
  • J. Casco-Rodriguez, C. Kemere and R. G. Baraniuk, [Re] The Discriminative Kalman Filter for Bayesian Filtering with Nonlinear and Non-Gaussian Observation Models, ReScience C 10(1), article 3, 2025. DOI: 10.5281/zenodo.15172014, published PDF.
  • M. C. Burkhart, Discriminative Bayesian filtering lends momentum to the stochastic Newton method for minimizing log-convex functions, Optimization Letters 17, 657–673, 2023. DOI: 10.1007/s11590-022-01895-5.
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Harmonic AnalysisMachine Learning·Captain: Elsie66

ClockRoPE: Random Fourier RotationsResearch Paper

Motivation

Transformer sequence models modulate attention scores by a function of the relative position between a query and a key: the attention logit between token mmm and token nnn is scaled by a fixed profile f(pm−pn)f(p_m - p_n)f(pm​−pn​). Realizing this modulation the naive way means evaluating fff once per pair (m,n)(m,n)(m,n) and materializing an L×LL\times LL×L adjustment over the whole sequence — quadratic in the sequence length LLL. Rotary Position Embedding (RoPE) Su et al. 2021 avoids this entirely: it rotates the query at position pmp_mpm​ and the key at position pnp_npn​ independently, each by an angle depending only on its own position, so that the pairwise quantity f(pm−pn)f(p_m-p_n)f(pm​−pn​) falls out of the dot product of the two separately rotated vectors — fff is never evaluated pairwise, and no L×LL\times LL×L matrix is ever built. This is what lets RoPE stay a linear, per-token preprocessing step compatible with efficient (sub-quadratic) attention implementations, rather than an O(L2)O(L^2)O(L2) modulation. The catch is that RoPE's specific log-linear frequency schedule bakes in one particular profile: a monotone, decaying fff. That schedule is a poor fit whenever the correlation structure of the data is not monotonically decaying with distance — the leading example being periodicity: in sequential recommendation, interactions separated by exactly one day or one week are more correlated than interactions separated by, say, half a day, and a decaying profile cannot express that "attention comes back" at the period.

Chen, Ainslie, Choromanski et al., ClockRoPE: Random Fourier Rotations for Temporal Routine Modeling (arXiv:2607.26369), ask a more general question first: which attention-modulation profiles fff can be realized at all by this same per-token, pairwise-iteration-free rotation trick — rotate each token once, on its own, and let the pairwise profile emerge from the dot product — and by what rotation-frequency schedule? Their answer is a random-features construction — sample the rotation frequencies from the kernel's own Fourier transform, rather than fixing them log-linearly — that realizes any continuous, normalized, positive-definite profile in expectation, with a quantified concentration rate, all while keeping the exact same per-token rotate-then-dot-product computation RoPE already uses. ClockRoPE is the periodic instance of this general theory, later deployed in a production-scale generative-retrieval system.

Setting

Fix an embedding dimension d=2nd = 2nd=2n and group a vector v∈Rdv \in \mathbb{R}^dv∈Rd into nnn consecutive feature pairs v(j)=(v2j,v2j+1)∈R2v^{(j)} = (v_{2j}, v_{2j+1}) \in \mathbb{R}^2v(j)=(v2j​,v2j+1​)∈R2 for j=0,…,n−1j = 0, \dots, n-1j=0,…,n−1. For an angle θ\thetaθ, let

R(θ)=(cos⁡θ−sin⁡θsin⁡θcos⁡θ)R(\theta) = \begin{pmatrix} \cos\theta & -\sin\theta \\ \sin\theta & \cos\theta \end{pmatrix}R(θ)=(cosθsinθ​−sinθcosθ​)

be the 2×22\times 22×2 (Givens) rotation matrix. A real kernel f:R→Rf : \mathbb{R} \to \mathbb{R}f:R→R is positive definite if for every finite family of points x1,…,xN∈Rx_1,\dots,x_N \in \mathbb{R}x1​,…,xN​∈R and complex coefficients c1,…,cNc_1,\dots,c_Nc1​,…,cN​, ∑i,jci‾cjf(xi−xj)\sum_{i,j} \overline{c_i} c_j f(x_i - x_j)∑i,j​ci​​cj​f(xi​−xj​) has nonnegative real part; it is normalized if f(0)=1f(0) = 1f(0)=1. When fff is also continuous and Lebesgue-integrable, its Fourier transform

τ(ξ)=∫Rf(x)e−i2πξx dx\tau(\xi) = \int_{\mathbb{R}} f(x) e^{-i2\pi\xi x}\,dxτ(ξ)=∫R​f(x)e−i2πξxdx

is (by Bochner's theorem) a genuine probability density on R\mathbb{R}R: this is the distribution the mission's rotation frequencies are sampled from.

Given a query qm∈R2nq_m \in \mathbb{R}^{2n}qm​∈R2n at position pmp_mpm​, a key kn∈R2nk_n \in \mathbb{R}^{2n}kn​∈R2n at position pnp_npn​, and nnn i.i.d. frequencies ξ0,…,ξn−1∼τ\xi_0, \dots, \xi_{n-1} \sim \tauξ0​,…,ξn−1​∼τ, the Random Fourier Rotation (RFR) estimator is

g^(qm,kn,pm,pn)=∑j=0n−1(R(2πξjpm) qm(j))⊤(R(2πξjpn) kn(j)).\hat g(q_m, k_n, p_m, p_n) = \sum_{j=0}^{n-1} \big(R(2\pi\xi_j p_m)\, q_m^{(j)}\big)^\top \big(R(2\pi\xi_j p_n)\, k_n^{(j)}\big).g^​(qm​,kn​,pm​,pn​)=j=0∑n−1​(R(2πξj​pm​)qm(j)​)⊤(R(2πξj​pn​)kn(j)​).

g^\hat gg^​ is exactly the modulated attention logit computed by rotating query/key feature pairs with per-pair, sampled RoPE frequencies — the same operation standard RoPE performs, but with ξj\xi_jξj​ drawn from τ\tauτ instead of fixed by a log-linear schedule.

Formalization targets

Goal — convergence of the RFR estimator (Proposition 3.2)

P ⁣(∣1ng^(qm,kn,pm,pn)−1n qm⊤knf(pm−pn)∣≥ϵ)≤2exp⁡ ⁣(−ϵ2(2n)28∑j=0n−1(∥qm(j)∥ ∥kn(j)∥)2)P\!\left(\left|\tfrac1n \hat g(q_m,k_n,p_m,p_n) - \tfrac1n\, q_m^\top k_n f(p_m-p_n)\right| \ge \epsilon\right) \le 2\exp\!\left(-\frac{\epsilon^2(2n)^2}{8\sum_{j=0}^{n-1}\big(\lVert q_m^{(j)}\rVert\, \lVert k_n^{(j)}\rVert\big)^2}\right)P(​n1​g^​(qm​,kn​,pm​,pn​)−n1​qm⊤​kn​f(pm​−pn​)​≥ϵ)≤2exp(−8∑j=0n−1​(∥qm(j)​∥∥kn(j)​∥)2ϵ2(2n)2​)

for every ϵ>0\epsilon > 0ϵ>0. This is the mission's central target: it upgrades the mean identity below into a quantitative, non-asymptotic guarantee that the sampled estimator is close to the target profile with high probability, at a rate that is exponential in the embedding dimension d=2nd = 2nd=2n.

Milestone — unbiasedness of the RFR estimator (Proposition 3.1)

Eξ0,…,ξn−1∼τ[g^(qm,kn,pm,pn)]=qm⊤kn f(pm−pn).\mathbb{E}_{\xi_0,\dots,\xi_{n-1}\sim\tau}\big[\hat g(q_m,k_n,p_m,p_n)\big] = q_m^\top k_n\, f(p_m-p_n).Eξ0​,…,ξn−1​∼τ​[g^​(qm​,kn​,pm​,pn​)]=qm⊤​kn​f(pm​−pn​).

The expectation identity that the concentration bound above sharpens; it is the feasibility half of the claim ("this construction is correct on average") that the convergence half needs as its starting point.

Milestone — periodic case via Herglotz's theorem (Corollary 3.3)

For a continuous, positive-definite, TTT-periodic fff with f(0)=1f(0)=1f(0)=1 and Fourier coefficients αk=1T∫0Tf(x)e−i2πkx/T dx\alpha_k = \frac1T \int_0^T f(x) e^{-i2\pi kx/T}\,dxαk​=T1​∫0T​f(x)e−i2πkx/Tdx,

αk≥0 for all k∈Z,∑k=−∞∞αk=f(0)=1.\alpha_k \ge 0 \text{ for all } k \in \mathbb{Z}, \qquad \sum_{k=-\infty}^{\infty} \alpha_k = f(0) = 1.αk​≥0 for all k∈Z,k=−∞∑∞​αk​=f(0)=1.

The periodic specialization needed to apply the goal and first milestone with a discrete frequency distribution over harmonics k/Tk/Tk/T — the regime ClockRoPE actually deploys, since daily/weekly routines are periodic rather than merely decaying.

Significance

The result gives a general recipe — sample, don't hand-design — for turning any admissible attention-modulation profile into a RoPE-compatible rotation schedule, with a concentration guarantee that says how many feature pairs are needed before the sampled schedule reliably approximates the target profile. Crucially, the recipe changes only which frequencies the per-token rotation uses — it never touches the computational shape of RoPE itself: each query and key is still rotated once, independently, by an angle depending only on its own position, and the target pairwise profile f(pm−pn)f(p_m-p_n)f(pm​−pn​) is still recovered purely from the dot product of the two rotated vectors. So realizing an arbitrary positive-definite fff this way costs exactly what realizing RoPE's own log-linear profile costs — linear in the sequence length, with no pairwise evaluation of fff and no L×LL\times LL×L matrix ever materialized — rather than the quadratic cost a direct, per-pair implementation of an arbitrary modulation function would require. This subsumes standard RoPE's log-linear schedule as one instance and explains, via the periodic corollary, why a schedule built from the kernel's own spectrum (rather than an arbitrary log-linear one) is the right way to encode periodicity: nothing about the construction, or its efficiency, is specific to decay. The paper reports this translated into measured gains in a production-scale generative-retrieval system, which is unusual weight of practical evidence behind a Bochner/Herglotz-style spectral argument.

At the time of writing, none of these three results have a machine-checked proof; this mission asks for the first formalization of all three, together with the shared scaffolding (feature-pair extraction, the rotation estimator, and the notion of a positive-definite kernel) they are stated over.

Difficulty

The natural first attempt at the concentration bound is a direct union bound or a naive variance argument, but the estimator g^\hat gg^​ is a sum of nnn terms that are each bounded (each rotated pair lies on a fixed-radius circle) rather than governed by a variance bound that shrinks with nnn under a fixed frequency; the source proof instead applies McDiarmid's bounded-differences inequality, treating each sampled frequency ξj\xi_jξj​ as one coordinate of the input and bounding the one-coordinate change in g^\hat gg^​ by 2∥qm(j)∥∥kn(j)∥2\lVert q_m^{(j)}\rVert\lVert k_n^{(j)}\rVert2∥qm(j)​∥∥kn(j)​∥ via the maximal distance between two points on the unit circle — not by directly bounding a variance term. Establishing Proposition 3.1 itself already requires care: it requires justifying that τ\tauτ, defined purely as an integral transform of fff, is in fact a legitimate probability density (Bochner's theorem), and then a real/complex bookkeeping argument identifying the real inner product of rotated pairs with the real part of a product of complex exponentials.

Formalization scope

The mission works over the reals and represents feature pairs as functions Fin (2 * n) → ℝ sliced into Fin n-indexed pairs, matching the "nnn feature pairs, dimension d=2nd = 2nd=2n" convention used throughout; 2×22\times22×2 rotations are ordinary Matrix (Fin 2) (Fin 2) ℝ values built with Matrix.mulVec/Matrix.dotProduct, and expectation over i.i.d. τ\tauτ-distributed frequencies is formalized as integration against the product measure MeasureTheory.Measure.pi of n independent copies of the measure with density τ\tauτ (MeasureTheory.Measure.withDensity) — this is mathematically equivalent to, and more directly usable in Lean than, introducing an abstract probability space with named i.i.d. random variables.

Since a general continuous positive-definite kernel need not have an integrable Fourier transform (the periodic case in Corollary 3.3 is exactly the counterexample: its "Fourier transform" is a discrete measure, not a density) — the goal and first milestone add Integrable f as an explicit hypothesis beyond what the paper states in prose, so that τ\tauτ is genuinely a density rather than a junk value. This is not a strengthening of the target profiles the paper cares about in practice (Gaussian, Laplace, and the cosine/Gaussian priors used by ClockRoPE itself are all integrable) and mirrors the paper's own split between the density case (Propositions 3.1–3.2) and the discrete, purely-periodic case (Corollary 3.3). A formalization that dropped this hypothesis and instead let the Fourier integral silently evaluate to Lean's junk value (0 for non-integrable integrands) would make the goal statement possible to "prove" vacuously and must be avoided.

Definitions needed: a positive-definite-kernel predicate, the real-valued Fourier transform of a kernel, feature-pair extraction, the 2×22\times22×2 rotation matrix, and the RFR estimator itself — all reusable by any future mission formalizing RoPE-family positional encodings (e.g. STRING, nD-RoPE) or other random-Fourier-feature results. McDiarmid's inequality, if not already in Mathlib in the needed form, is itself a independently reusable contribution.

Selected references

  • Yiwen Chen, Joshua Ainslie, Krzysztof Choromanski, Xiang Gao, Su-Lin Wu, Yiping Yuan, Qian Sun, ClockRoPE: Random Fourier Rotations for Temporal Routine Modeling, 2026. arXiv:2607.26369
  • Jianlin Su, Yu Lu, Shengfeng Pan, Ahmed Murtadha, Bo Wen, Yunfeng Liu, RoFormer: Enhanced Transformer with Rotary Position Embedding, arXiv, 2021. arXiv:2104.09864
  • Ali Rahimi, Benjamin Recht, Random Features for Large-Scale Kernel Machines, NeurIPS, 2007.
  • Salomon Bochner, Monotone Funktionen, Stieltjessche Integrale und harmonische Analyse, Springer, 1933.
  • Gustav Herglotz, Über Potenzreihen mit positivem, reellem Teil im Einheitskreis, Berichte über die Verhandlungen der Königlich Sächsischen Gesellschaft der Wissenschaften zu Leipzig, 1911.
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Harmonic AnalysisMathematical Physics·Captain: lisamegawatts

Finite Reflection Positivity Methods I: Split Weights and Infrared ModesTextbook

Motivation

Reflection positivity and infrared bounds form a standard finite-volume route from the geometry of a lattice reflection to quantitative control of long wavelength fluctuations. In the classical argument, reflection positivity supplies a Cauchy--Schwarz inequality for reflected observables, while Fourier diagonalization of the lattice Laplacian identifies the free covariance used in the infrared comparison. These ingredients underlie rigorous results on continuous-symmetry lattice systems in Fröhlich, Simon, and Spencer's development of infrared bounds and spontaneous symmetry breaking (1976), and the general theory of reflection positivity developed by Fröhlich, Israel, Lieb, and Simon (1978). Related technology appears in Fröhlich and Spencer's treatment of the two-dimensional Abelian spin systems and Coulomb gas (1981).

The analytic and model-specific theorems are substantial, but their finite algebraic interface is sharply separable. This mission isolates that interface so later clock, XY, and Gaussian-domination developments can share one checked notion of reflection, one spectral covariance convention, and one treatment of the constant mode.

Setting

Let XXX be a finite set of configurations on one side of a reflection plane. A full split configuration is a pair (x,y)∈X×X(x,y)\in X\times X(x,y)∈X×X, and reflection exchanges its two entries. A plus-half observable is a function F:X→RF:X\to \mathbb RF:X→R lifted to X×XX\times XX×X through the first coordinate. Its reflected copy therefore depends on the second coordinate.

A split weight is specified by a finite feature index AAA, real coefficients cac_aca​, and features ϕa:X→R\phi_a:X\to\mathbb Rϕa​:X→R:

W(x,y)=∑a∈Acaϕa(x)ϕa(y).W(x,y)=\sum_{a\in A}c_a\phi_a(x)\phi_a(y).W(x,y)=a∈A∑​ca​ϕa​(x)ϕa​(y).

For a finite family of plus-half observables FiF_iFi​, the reflected kernel is

Kij=∑(x,y)∈X×XW(x,y)Fi(x)Fj(y).K_{ij}=\sum_{(x,y)\in X\times X} W(x,y)F_i(x)F_j(y).Kij​=(x,y)∈X×X∑​W(x,y)Fi​(x)Fj​(y).

A real matrix is positive semidefinite here when it is symmetric and its quadratic form is nonnegative on every real coordinate vector.

The spectral side uses a finite mode set III with a distinguished zero mode 000. An infrared spectrum consists of a function λ:I→R\lambda:I\to\mathbb Rλ:I→R that is nonnegative and vanishes exactly at 000. For β>0\beta>0β>0, the free mode covariance is diagonal, equals zero at the constant mode, and has entry

Gkk=1βλkG_{kk}=\frac{1}{\beta\lambda_k}Gkk​=βλk​1​

away from zero. Covariance domination is tested only on source vectors whose zero-mode coordinate vanishes. The concrete spectral fixture is the 4×44\times44×4 periodic square lattice, with tensor-product discrete Fourier modes and the nearest-neighbor graph Laplacian.

Formalization targets

Finite reflection positivity

The first target identifies the split reflection pairing with the explicit double sum over the two halves. Under ca≥0c_a\ge0ca​≥0, the resulting reflected kernel must be positive semidefinite:

∑i,juiKijuj≥0.\sum_{i,j}u_iK_{ij}u_j\ge0.i,j∑​ui​Kij​uj​≥0.

Every such kernel must satisfy the two-observable chessboard inequality

Kij2≤KiiKjj.K_{ij}^{2}\le K_{ii}K_{jj}.Kij2​≤Kii​Kjj​.

Typed finite spectrum

For every Torus-4 frequency kkk and site xxx, the registered Fourier mode ψk\psi_kψk​ must satisfy the pointwise eigenvalue equation

(ΔT4ψk)(x)=λkψk(x).(\Delta_{\mathrm{T4}}\psi_k)(x)=\lambda_k\psi_k(x).(ΔT4​ψk​)(x)=λk​ψk​(x).

The eigenvalues must be nonnegative and vanish exactly at the constant mode, and these laws must be packaged as the same spectrum type consumed by the infrared definitions.

Zero-mode-restricted infrared bound

The diagonal free covariance must be positive semidefinite for β>0\beta>0β>0. If an interacting covariance CCC is quadratically dominated by GGG on sources with u0=0u_0=0u0​=0, then every nonzero Fourier mode must satisfy

Ckk≤1βλk(k≠0).C_{kk}\le\frac{1}{\beta\lambda_k}\qquad(k\ne0).Ckk​≤βλk​1​(k=0).

Two finite counterfixtures are part of the target. They assert that an arbitrary full-vertex reflected two-point matrix need not be positive semidefinite, and that domination restricted away from the zero mode need not extend to full-matrix domination.

Significance

The resulting interface prevents three substitutions that otherwise look notational but change the theorem. Reflection positivity is tested on observables supported on one half rather than on an arbitrary matrix indexed by all vertices. The infrared comparison excludes the constant mode rather than forcing a fluctuating zero mode below a covariance with zero diagonal. The graph-Laplacian eigenvalue is connected to the Fourier mode by an explicit pointwise theorem rather than by assigning a function the name laplacianEigenvalue.

Several ingredients already have machine-checked Lean proofs in the LeanProofs repository: the finite matrix Cauchy--Schwarz theorem, the Torus-4 DFT diagonalization and zero-mode theorem, and the diagonal free-covariance calculation. This mission reorganizes those results around a corrected consumer boundary and adds the split-half and off-zero adapters. It does not present the finite statements as new mathematics.

Difficulty

The main difficulty is maintaining the correct domain at each interface. A reflection of lattice sites does not by itself imply positive semidefiniteness of a correlation matrix indexed by every site; the tested observables and their support are part of the assertion. Likewise, a free covariance whose constant-mode entry is defined to be zero cannot dominate an arbitrary covariance on all source vectors. Finally, a Fourier multiplier used for a pseudospectral derivative is not automatically the eigenvalue of the nearest-neighbor graph Laplacian. The formal statements must keep these three objects distinct.

Formalization scope

All configuration, feature, observable, and mode types are finite. Kernels, weights, coefficients, source vectors, and quadratic forms are real. Complex numbers occur only in the explicit discrete Fourier modes. Reflected pairings are unnormalized finite sums; no partition function or probability measure is introduced. The inverse temperature satisfies β>0\beta>0β>0. The distinguished zero mode is part of the spectrum interface, and infrared domination is restricted to source vectors that vanish at that coordinate.

The mission does not assert reflection positivity of a clock or XY Gibbs measure, nonnegative Fourier coefficients of a physical cross-bond weight, Gaussian domination, a thermodynamic limit, a Kosterlitz--Thouless transition, or a universal jump. It also does not identify the Torus-4 graph spectrum with the Grid3 pseudospectral multiplier from the Fourier--Hodge packet. Those are separate future missions requiring additional model and analytic input.

The reusable outputs are the split-weight RP interface, the finite positive-semidefinite kernel API, the typed spectrum object, and the zero-mode-restricted domination predicate. Contributions should preserve the explicit half support and zero-mode restrictions; a proof obtained by adding the desired conclusion as a hypothesis is outside scope.

Selected references

  • J. Fröhlich, B. Simon, and T. Spencer, Infrared bounds, phase transitions and continuous symmetry breaking, Communications in Mathematical Physics 50 (1976), 79--95. https://doi.org/10.1007/bf01608557
  • J. Fröhlich, R. Israel, E. H. Lieb, and B. Simon, Phase transitions and reflection positivity. I. General theory and long range lattice models, Communications in Mathematical Physics 62 (1978), 1--34. https://doi.org/10.1007/bf01940327
  • J. Fröhlich and T. Spencer, The Kosterlitz--Thouless transition in two-dimensional Abelian spin systems and the Coulomb gas, Communications in Mathematical Physics 81 (1981), 527--602. https://doi.org/10.1007/bf01208273
  • LeanProofs, ReflectionPositivityInfraredBound.lean, exact repository snapshot dbf503b2909cc17787d40a21eb75a0c9354cc6ef. https://github.com/MonumentalSystems/LeanProofs/blob/dbf503b2909cc17787d40a21eb75a0c9354cc6ef/LeanProofs/StatMech/ReflectionPositivityInfraredBound.lean
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Operations ResearchOptimization·Captain: StellaXin

Capped Base-Stock Policies: A 2.33-ApproximationResearch Paper

A performance guarantee for a simple replenishment rule

When replenishment takes several periods, an inventory decision commits stock before the demand that will consume it is known. Too much stock incurs holding costs; too little loses sales. An optimal decision can depend on the entire pipeline of outstanding orders. A rule with only two adjustable parameters is easier to implement, but its simplicity alone gives no guarantee on the cost it can incur.

Capped base-stock policies combine an inventory-position target with a maximum order quantity. The class was introduced and analyzed by Xin (2021). The present target is the finite-lead-time guarantee in Linwei Xin's Capped Base-Stock Policies: A 2.33-Approximation, specifically the author-supplied manuscript with source label thm-main. A public listing of the paper identifies the July 17, 2026 working paper; the supplied text is the authoritative version for this formalization.

Demand, stock, and delayed orders

Periods are discrete. Demand is a sequence of independent, identically distributed nonnegative real random variables DtD_tDt​ with finite, strictly positive mean μ\muμ. The deterministic lead time is an integer L≥1L\ge1L≥1. Holding and lost-sales rates are h>0h>0h>0 and p>0p>0p>0.

At the beginning of period ttt, ItI_tIt​ is on-hand inventory and x1,t,…,xL,tx_{1,t},\ldots,x_{L,t}x1,t​,…,xL,t​ are outstanding orders, with x1,tx_{1,t}x1,t​ due immediately. That arrival is received, an order qt≥0q_t\ge0qt​≥0 is placed, demand is realized, and costs are charged. The new order arrives LLL periods later. The equations are

It+1=(It+x1,t−Dt)+,xi,t+1=xi+1,t (i<L),xL,t+1=qt.I_{t+1}=(I_t+x_{1,t}-D_t)^+,\qquad x_{i,t+1}=x_{i+1,t}\ (i<L),\qquad x_{L,t+1}=q_t.It+1​=(It​+x1,t​−Dt​)+,xi,t+1​=xi+1,t​ (i<L),xL,t+1​=qt​.

Here u+=max⁡{u,0}u^+=\max\{u,0\}u+=max{u,0}. Unfilled demand is lost rather than backlogged. With ℓt=(Dt−It−x1,t)+\ell_t=(D_t-I_t-x_{1,t})^+ℓt​=(Dt​−It​−x1,t​)+, the period cost is hIt+1+pℓthI_{t+1}+p\ell_thIt+1​+pℓt​. Initial inventory and every pipeline coordinate are zero. A nonanticipative policy chooses orders using only information available before the current demand; policies may depend on the entire observed past and on independent private randomization.

For a policy π\piπ, its long-run expected average cost is

C(π)=lim sup⁡T→∞1T∑t=1TE[hIt+1π+pℓtπ],OPT=inf⁡π∈ΠC(π).C(\pi)=\limsup_{T\to\infty}\frac1T\sum_{t=1}^T\mathbb E[hI_{t+1}^\pi+p\ell_t^\pi],\qquad \mathrm{OPT}=\inf_{\pi\in\Pi}C(\pi).C(π)=T→∞limsup​T1​t=1∑T​E[hIt+1π​+pℓtπ​],OPT=π∈Πinf​C(π).

The capped rule is qt=min⁡{(S−It−∑i=1Lxi,t)+,r}q_t=\min\{(S-I_t-\sum_{i=1}^Lx_{i,t})^+,r\}qt​=min{(S−It​−∑i=1L​xi,t​)+,r} for finite S,r≥0S,r\ge0S,r≥0. Write CCBS∗=inf⁡S,r≥0C(πS,r)C^*_{\rm CBS}=\inf_{S,r\ge0}C(\pi_{S,r})CCBS∗​=infS,r≥0​C(πS,r​). Ordinary base stock is already included by taking r=Sr=Sr=S; no infinite order cap is required.

Formalization targets

For 0≤r≤μ0\le r\le\mu0≤r≤μ and m≥1m\ge1m≥1, set

Irm=max⁡0≤k≤m∑i=1k(r−Di),Gm(r,z)=E[(Irm+∑i=1m(Di−r)−z)+].I_r^m=\max_{0\le k\le m}\sum_{i=1}^k(r-D_i),\qquad G_m(r,z)=\mathbb E\left[\left(I_r^m+\sum_{i=1}^m(D_i-r)-z\right)^+\right].Irm​=0≤k≤mmax​i=1∑k​(r−Di​),Gm​(r,z)=E[(Irm​+i=1∑m​(Di​−r)−z)+].

Empty sums are zero. The lower certificate is

C‾=inf⁡{hz+p(μ−r):0≤r≤μ, z≥0, GL(r,z)≤L(μ−r), GL+1(r,z)≤(L+1)(μ−r)}.\underline C=\inf\{hz+p(\mu-r):0\le r\le\mu,\ z\ge0,\ G_L(r,z)\le L(\mu-r),\ G_{L+1}(r,z)\le(L+1)(\mu-r)\}.C​=inf{hz+p(μ−r):0≤r≤μ, z≥0, GL​(r,z)≤L(μ−r), GL+1​(r,z)≤(L+1)(μ−r)}.

The pair (0,0)(0,0)(0,0) is feasible. Both horizon constraints are retained. With

κL=1+4L2(L+1)(3L−1),\kappa_L=1+\frac{4L^2}{(L+1)(3L-1)},κL​=1+(L+1)(3L−1)4L2​,

the goal is Theorem 1's complete assertion:

CCBS∗≤κLC‾,CCBS∗≤κLOPT≤73OPT.C^*_{\rm CBS}\le\kappa_L\underline C,\qquad C^*_{\rm CBS}\le\kappa_L\mathrm{OPT}\le\frac73\mathrm{OPT}.CCBS∗​≤κL​C​,CCBS∗​≤κL​OPT≤37​OPT.

The exact rational constant is used; the title's 2.33 is a rounded description. Multiplicative inequalities also make sense when the optimal cost is zero.

Five supporting targets reproduce selected source statements: Proposition 1's lower-certificate bound; Proposition 2's finite-cap cost conclusion; Lemma 2's bound on a consecutive block in the greedy recursion; Proposition 3's ordinary-base-stock cost bound; and Proposition 4's two-branch inequality. The finite-cap and ordinary-base-stock parameters remain exactly (S,r)=((L+1)r+z,r)(S,r)=((L+1)r+z,r)(S,r)=((L+1)r+z,r) and S=(L+1)r+2zS=(L+1)r+2zS=(L+1)r+2z, respectively. Labels accompany the printed numbering so the supplied source is unambiguous.

What completing the mission establishes

The result gives a uniform cost guarantee for this policy class across all positive holding and penalty rates, every positive integer lead time, and arbitrary nonnegative demand laws with finite positive mean. It bounds the infimum of costs over the policy parameters; it does not by itself provide an algorithm for selecting parameters or assert that the infimum is attained. At L=1L=1L=1 the displayed coefficient is 2, while its uniform upper bound is 7/37/37/3.

The manuscript supplies mathematical proofs. This mission asks for checked proofs of their formal statements. Compiling the declarations confirms that they are well formed, not that the claims are proved. A completed development would provide reusable delayed-inventory dynamics, measurable history policies, average-cost optimization objects, finite-horizon demand envelopes, and policy-comparison results.

Where the formal work lies

The pipeline carries consequences of past decisions across multiple demand periods. Nonanticipativity and independence must be stated precisely before expectation and convexity arguments can be used. Also, existence of a stationary distribution alone does not identify its expected cost with a long-run cost from an empty initial system. The manuscript invokes stationary results from prior inventory work, including Xin and Goldberg (2016), and uses stationary CBS quantities in intermediate arguments. Their needed hypotheses and connections to the original objective require proof within a complete development.

The two cost bounds depend on both coordinates of a feasible lower-certificate pair. Losing either horizon constraint changes that certificate. Replacing it with an arbitrary scalar lower bound or assuming the policy comparisons would remove substantive parts of the result.

Formalization scope and conventions

Stock, orders, and demand take arbitrary nonnegative real values. Time is represented from zero in the operational model, corresponding to period one in the manuscript. The formal representation uses a canonical probability model with independent demand coordinates and an independent uniform private seed; measurable time-dependent decision functions use only preceding demands and that seed. Connecting arbitrary standard-Borel randomized controls to this canonical realization is a representation obligation. The zero-start optimum ranges over these general history policies, not only stationary or capped policies.

Expected nonnegative costs, their upper limits, and cost infima are represented in the extended nonnegative reals. Thus a policy with infinite expected cost does not acquire a fictitious zero value through a totalized real integral. The finite-horizon envelope expectations use the original integrable demand law. The greedy lemma uses integer-indexed sequences so subtraction of earlier times has no natural-number truncation; its blocks are nonempty, as required to define their maximum.

Definitions contain no unproved facts. In particular, stationarity, convergence from the empty initial state, lower bounds, and upper policy comparisons are not fields assumed by the model. Contributions to these intermediate obligations and to any of the five source targets support the central theorem.

Selected references

  • Linwei Xin, Capped Base-Stock Policies: A 2.33-Approximation, working paper, 2026. SSRN listing. Author-supplied LaTeX is authoritative: Theorem 1 (thm-main), Proposition 1 (lemma-lb), Proposition 2 (prop-finite-cap-bound), Lemma 2 (lem-greedy-window), Proposition 3 (prop-base-stock-bound), Proposition 4 (lem-two-branch). Source SHA-256: f353793c255e1ebed5f3ec541037284bd926183e3e5b71941f13e79c2d67cb7a.
  • Linwei Xin, Technical Note—Understanding the Performance of Capped Base-Stock Policies in Lost-Sales Inventory Models, Operations Research 69(1), 61–70, 2021. DOI.
  • Linwei Xin and David A. Goldberg, Optimality Gap of Constant-Order Policies Decays Exponentially in the Lead Time for Lost Sales Models, Operations Research 64(6), 1556–1565, 2016. DOI.
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Operations Research·Captain: viratkota

Coherent Measures of Risk: the axioms, and why Value-at-Risk fails themResearch Paper

Motivation

In 1999 Artzner, Delbaen, Eber and Heath asked what a risk measure ought to satisfy, wrote down four axioms, and observed that the industry standard of the day -- Value-at-Risk -- fails one of them. The failing axiom is subadditivity: merging two positions should never require more capital than holding them apart. VaR can violate it, so under VaR a diversified book can appear riskier than its parts.

That observation did not stay academic. It is the reason the Basel framework moved its market-risk capital standard from Value-at-Risk to Expected Shortfall. Few results in mathematical finance have had a more direct regulatory consequence, and the mathematics is elementary enough to state completely.

Setting

A position is a payoff X : Fin (n+1) -> R across finitely many equally-weighted states, and a risk measure rho sends it to the capital that must be added to make it acceptable. Following Definition 2.4 of the paper, rho is coherent when it is translation-invariant, subadditive, positively homogeneous and monotone. Nonemptiness of the state space is carried in the index type so the worst case is always attained; no probability measure is needed for these four axioms, which is faithful to the paper -- Artzner et al. state T, S, PH and M without reference to one.

Value-at-Risk is defined here at an integer tolerance k rather than a probability level, which keeps the quantile unambiguous on a finite space: VaR X k is the least capital leaving at most k states in loss, corresponding to level k/(n+1).

The goal

The mission's goal theorem is the negative result: Value-at-Risk is not subadditive. A witness is 25 equiprobable states with X losing 100 in state 0 alone and Y losing 100 in state 1 alone. Each has one losing state in twenty-five, so at tolerance k = 1 both have VaR = 0; their sum loses in two states, exceeding the tolerance, so VaR (X+Y) 1 = 100 > 0 + 0. The witness was checked numerically before this mission was drafted; what is open is the Lean proof.

The milestones establish the positive contrast on the same footing: worst-case risk, the most conservative measure, satisfies all four axioms, so the failure is specific to VaR rather than inherent to risk measurement.

Source

P. Artzner, F. Delbaen, J.-M. Eber and D. Heath, Coherent Measures of Risk, Mathematical Finance 9 (1999) 203-228. Axioms T, S, PH and M are Definition 2.4; the failure of subadditivity for VaR and the diversification consequence are discussed in Section 3.

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Machine LearningStatistics·Captain: willma

Don't Label Twice: Game, Set, MatchOpen Problem

The problem

(a) In a tennis match, you are the favorite, and win each point independently with probability q∈(1/2,1)q\in(1/2,1)q∈(1/2,1). Let n,mn,mn,m be odd positive integers greater than 111. You have the choice between playing a best-of-nmnmnm (i.e., you play nmnmnm points and whoever wins the majority of points wins the match), or a best-of-nnn of best-of-mmm's (i.e., the match is won by winning the majority of nnn "sets", and each "set" is won by winning the majority of mmm points). Prove that your probability of winning the match is strictly greater by playing the best-of-nmnmnm.

(b) We now consider two generalizations: m1,…,mkm_1,\ldots,m_km1​,…,mk​ are odd positive integers, while nnn is any positive integer, with all integers being greater than 111. You have the choice between playing a best-of-nm1⋯mknm_1\cdots m_knm1​⋯mk​, or a best-of-nnn of "sets", which are best-of-m1m_1m1​'s of "games", …, which are best-of-mkm_kmk​'s of "points". In both cases, now that nnn may be even, it is possible for the players to tie, in which case the match winner is determined by an independent fair coin. Prove again that your probability of winning the match is strictly greater by playing the best-of-nm1⋯mknm_1\cdots m_knm1​⋯mk​.

(c) We consider a further generalization where each completed "set" counts toward the match score in an independently random way:

  • with probability aaa, the winner gains 111 in the match score, as usual;
  • with probability bbb, the set is ignored and does not count toward the match score;
  • with probability ccc, the loser gains 111 in the match score;

with a+b+c=1a+b+c=1a+b+c=1 and a>ca>ca>c, so players are still incentivized to win sets (previously we had a=1a=1a=1, b=c=0b=c=0b=c=0). This random scoring rule is applied once per completed set, at the outermost layer only: the games and points inside a set are decided by plain majorities, with no randomness, and only the set's final result is scored. If you choose to play the best-of-nm1⋯mknm_1\cdots m_knm1​⋯mk​, then each individual point counts as a set and is subject to the same randomness with probabilities a,b,ca,b,ca,b,c. Prove that your probability of winning the match is still strictly greater by playing the best-of-nm1⋯mknm_1\cdots m_knm1​⋯mk​ (the fair-coin-on-ties convention continues).

(d) Continue from part (c), but change the fair-coin-on-ties convention so that you only win the match if you have a strictly greater match score than your opponent. Assuming b≥1/2b\ge1/2b≥1/2, prove that your probability of winning the match is strictly greater by playing the best-of-nm1⋯mknm_1\cdots m_knm1​⋯mk​.

Source and connection to Dorner–Hardt

Florian E. Dorner and Moritz Hardt, Don't Label Twice: Quantity Beats Quality when Comparing Binary Classifiers on a Budget, ICML 2024. arXiv:2402.02249 (v3, 8 April 2026).

The paper asks how to spend a fixed budget of noisy crowdworker labels when comparing two binary classifiers: one label each for many data points, or several labels per data point aggregated by majority vote. It proves, via Cramér's theorem, that one label each is asymptotically optimal, and states the finite-sample version as an open conjecture (Section 5, Conjecture 1), still open in the April 2026 revision. Its Section 3 displays the finite-sample inequality for the independent, homogeneous-label case and verifies it numerically over about five billion parameter settings.

Part (d) of this mission with one level of sets is that Section 3 inequality in tennis language. A point is a single crowdworker label being correct (qqq is the label accuracy); a set is a data point, whose test label is the majority of its mmm labels; and the scoring rule is what the two classifiers do with that label. Writing ppp for the worse classifier's accuracy and p+ϵp+\epsilonp+ϵ for the better one's, a set is scored to its winner when the better classifier alone matches the test label, ignored when the two classifiers agree, and scored to its loser when the worse classifier alone matches:

a=(p+ϵ)(1−p),c=p(1−p−ϵ),b=1−a−c,a=(p+\epsilon)(1-p),\qquad c=p(1-p-\epsilon),\qquad b=1-a-c,a=(p+ϵ)(1−p),c=p(1−p−ϵ),b=1−a−c,

so that a−c=ϵ>0a-c=\epsilon>0a−c=ϵ>0, and b≥1/2b\ge1/2b≥1/2 always holds because two classifiers of accuracy at least 1/21/21/2 agree on at least half the data. Substituting into the paper's Proposition 1 recovers its gap-indicator probabilities exactly: Pr⁡(+1)=qϵ+p(1−p−ϵ)\Pr(+1)=q\epsilon+p(1-p-\epsilon)Pr(+1)=qϵ+p(1−p−ϵ), Pr⁡(−1)=(1−q)ϵ+p(1−p−ϵ)\Pr(-1)=(1-q)\epsilon+p(1-p-\epsilon)Pr(−1)=(1−q)ϵ+p(1−p−ϵ). The paper's inequality also allows n=1n=1n=1 and q=1q=1q=1, which parts (c)–(d) exclude only because the inequality can fail to be strict at b=0b=0b=0 there; for b≥1/2b\ge1/2b≥1/2 the same argument covers those edge cases. The paper's Conjecture 1 as literally stated concerns a correlated-error setting (its Section 3.2) and is not claimed here.

Parts (a)–(c) go beyond the paper's setting: arbitrary nesting depth, a fair-coin tie rule, and no constraint on the ignore rate bbb. The hypothesis b≥1/2b\ge1/2b≥1/2 in part (d) cannot be dropped: with one level, (a,b,c)=(0.9,0.1,0)(a,b,c)=(0.9,0.1,0)(a,b,c)=(0.9,0.1,0), q=0.6q=0.6q=0.6, m=3m=3m=3, n=1n=1n=1, the single best-of-3 finishes strictly ahead with probability 0.58320.58320.5832 while three single points do so with probability 0.57610.57610.5761.

Timeline

  • Feb 2024 — arXiv v1; ICML 2024. Asymptotic theorem via Cramér; finite-sample statement conjectured; ~5·10⁹-configuration numerical sweep.
  • Oct 2024 — arXiv v2.
  • Apr 2026 — arXiv v3; conjecture still stated as open.
  • Aug 2026 — private proof of the Section 3 inequality (strict win, b≥1/2b\ge1/2b≥1/2, one level) via exponential tilting of the tie probability.
  • Sep 2026 — private proof of the fair-coin version with no constraint on bbb (Bernstein degree elevation and a hypergeometric parity argument), then of the full four-part statement via a pairing lemma for player-symmetric rules. This mission formalizes that proof.

Conventions in the formal statement

"Greater than 111" is read as n≥2n\ge2n≥2 and each mi≥3m_i\ge3mi​≥3 odd; the list of set sizes in (b)–(d) is nonempty. Laws are functions Z→R\mathbb Z\to\mathbb RZ→R and every probability is a finite sum — no measure theory. The goal theorem is the conjunction of the four parts.

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Functional AnalysisOperations ResearchOptimization+1·Captain: Shuze Chen

Vector Space Methods II: Gauss–Markov EstimationTextbook

Motivation

Chapter 4 of Luenberger's Optimization by Vector Space Methods (Wiley, 1969) develops linear least-squares estimation as an application of the Hilbert space projection theorem formalized in Mission I of this series. The chapter's centerpiece is the classical Gauss–Markov theorem: among all linear unbiased estimators of an unknown parameter vector from noisy linear measurements, the estimator (W⊤Q−1W)−1W⊤Q−1y(W^\top Q^{-1} W)^{-1} W^\top Q^{-1} y(W⊤Q−1W)−1W⊤Q−1y has minimum variance — componentwise, not merely in trace. This result is foundational for statistics and econometrics, and its Hilbert-space derivation is the cleanest known.

Setting

Measurements are modeled as y=Wβ+εy = W\beta + \varepsilony=Wβ+ε, where yyy is an mmm-dimensional data vector, WWW a known m×nm \times nm×n matrix (n<mn < mn<m) with linearly independent columns, β\betaβ an unknown nnn-dimensional parameter vector, and ε\varepsilonε a random mmm-vector of measurement errors with Eε=0E\varepsilon = 0Eε=0 and covariance E[εε⊤]=QE[\varepsilon\varepsilon^\top] = QE[εε⊤]=Q, positive definite. A linear estimate is β^=Ky\hat\beta = Kyβ^​=Ky for a constant n×mn \times mn×m matrix KKK; it is unbiased when Eβ^=βE\hat\beta = \betaEβ^​=β for every β\betaβ, which holds iff KW=IKW = IKW=I. The optimality criterion is the error second moment E∥β^−β∥2E\|\hat\beta - \beta\|^2E∥β^​−β∥2, and the book's key observation (p. 85) is that the problem splits into nnn independent minimum norm problems, one per component, each solvable by the dual approximation theorem of Mission I.

Formally, randomness is carried by an abstract probability space: a measure space (Ω,μ)(\Omega, \mu)(Ω,μ) with μ\muμ a probability measure, random vectors as functions Ω→Rm\Omega \to \mathbb{R}^mΩ→Rm with explicit integrability hypotheses for all first and second moments, and E[⋅]=∫⋅ dμE[\cdot] = \int \cdot \, d\muE[⋅]=∫⋅dμ.

Formalization targets

The goal is §4.4 Theorem 1 (Gauss–Markov): with K0=(W⊤Q−1W)−1W⊤Q−1K_0 = (W^\top Q^{-1} W)^{-1} W^\top Q^{-1}K0​=(W⊤Q−1W)−1W⊤Q−1,

K0W=I,E[(K0y−β)i2]≤E[(Ky−β)i2]for every i and every K with KW=I,K_0 W = I, \qquad E\big[(K_0 y - \beta)_i^2\big] \le E\big[(K y - \beta)_i^2\big] \quad \text{for every } i \text{ and every } K \text{ with } KW = I,K0​W=I,E[(K0​y−β)i2​]≤E[(Ky−β)i2​]for every i and every K with KW=I,

with error covariance

E[(K0y−β)(K0y−β)⊤]=(W⊤Q−1W)−1.E\big[(K_0 y - \beta)(K_0 y - \beta)^\top\big] = (W^\top Q^{-1} W)^{-1}.E[(K0​y−β)(K0​y−β)⊤]=(W⊤Q−1W)−1.

Milestones: the deterministic least-squares estimate β^=(W⊤W)−1W⊤y\hat\beta = (W^\top W)^{-1} W^\top yβ^​=(W⊤W)−1W⊤y (§4.3 Theorem 1); the book's deterministic reduction — minimize the diagonal entries of KQK⊤KQK^\topKQK⊤ subject to KW=IKW = IKW=I (p. 85); the minimum-variance estimate β^=E[βy⊤](E[yy⊤])−1y\hat\beta = E[\beta y^\top] (E[y y^\top])^{-1} yβ^​=E[βy⊤](E[yy⊤])−1y for random β\betaβ (§4.5 Theorem 1); and the information-form identities RW⊤(WRW⊤+Q)−1=(W⊤Q−1W+R−1)−1W⊤Q−1RW^\top(WRW^\top + Q)^{-1} = (W^\top Q^{-1}W + R^{-1})^{-1}W^\top Q^{-1}RW⊤(WRW⊤+Q)−1=(W⊤Q−1W+R−1)−1W⊤Q−1 and R−RW⊤(WRW⊤+Q)−1WR=(W⊤Q−1W+R−1)−1R - RW^\top(WRW^\top+Q)^{-1}WR = (W^\top Q^{-1}W + R^{-1})^{-1}R−RW⊤(WRW⊤+Q)−1WR=(W⊤Q−1W+R−1)−1 (§4.5 Corollary 2).

Significance

The Gauss–Markov theorem justifies weighted least squares as the optimal linear unbiased procedure and is the standard benchmark against which biased and nonlinear estimators are measured. The minimum-variance estimate of §4.5 is the Bayesian counterpart with prior covariance RRR; the information-form identities connect the two and exhibit Gauss–Markov as the limit R−1→0R^{-1} \to 0R−1→0. Mission III builds the recursive (Kalman) estimator directly on these results.

All results are classical and proved in the source. Mathlib has mature measure-theoretic integration but, to date, no Gauss–Markov theorem and no linear estimation theory; the matrix milestones (trace reduction, information form) are also absent as stated. The probabilistic statements here are deliberately phrased with elementary integrals of products of real-valued components — no Bochner integration of vector-valued maps — so they are approachable with MeasureTheory.integral alone.

Difficulty

The subtlety is bookkeeping, not depth. Unbiasedness must be encoded as the algebraic constraint KW=IKW = IKW=I (the book proves the equivalence with Eβ^=βE\hat\beta = \betaEβ^​=β for all β\betaβ); the componentwise variance claim is strictly stronger than the trace claim and requires the per-component minimum norm argument, not a single matrix inequality. Positive definiteness of QQQ enters through invertibility of W⊤Q−1WW^\top Q^{-1} WW⊤Q−1W, which itself needs the linear independence of the columns of WWW — dropping either hypothesis makes the goal false. In the probabilistic statements every integral needs an integrability hypothesis; the drafts supply integrability of all pairwise products of components, from which integrability of every derived expression follows.

Formalization scope

Random vectors are plain functions Ω → Fin m → ℝ on a MeasurableSpace Ω with a probability measure μ; second moments are hypotheses of the form ∫ ω, ε ω i * ε ω j ∂μ = Q i j with explicit Integrable assumptions; no independence, Gaussianity, or distributional assumptions are used anywhere. Matrices are Matrix (Fin m) (Fin n) ℝ with Mathlib's Matrix.PosDef, nonconstructive inverse ⁻¹, and mulVec. Norms on parameter space are written as explicit finite sums of squares, avoiding any ambiguity between Euclidean and supremum norms on pi types. The estimators under comparison are strictly linear (β^=Ky\hat\beta = Kyβ^​=Ky, no affine offset), exactly as in the source; §4.5's affine extension (its Problem 6) is out of scope.

Selected references

  • David G. Luenberger, Optimization by Vector Space Methods, John Wiley & Sons, 1969. Chapter 4, pp. 78–102. ISBN 0-471-55359-X.
  • A. C. Aitken, On least squares and linear combination of observations, Proc. Roy. Soc. Edinburgh 55 (1935), 42–48 (the weighted-least-squares form of Gauss–Markov).
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