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Functional Analysis

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Operations ResearchProbability·Captain: mikedeng1

Combined Custom Hedging: Optimal Design, Noninsurable Exposure, and Operational Risk Management: A Unique Optimal Combined Custom Hedge Exists When the Maximal Correlation Is Below OneResearch Paper

Motivation

Firms carry risks they cannot insure directly. A farmer's revenue depends on local yield and on local price; an airline's cost depends on jet fuel at a specific airport; an energy retailer's margin depends on load and on weather. Exchange-traded derivatives are written on standardized indices, so the exposure that matters is only partly claimable. Guiotto and Roncoroni (Operations Research 2022) study the design of a combined custom hedge: one over-the-counter claim written on the claimable part XXX of the firm's risk, plus a second claim written on a side index III that is correlated with the unclaimable part. The question is when such a pair is well defined, that is, when the firm's mean–variance hedging problem has one and only one optimal pair of claims.

Single-claim custom hedging goes back to Chowdhry and Howe (1999) and Caldentey and Haugh (2006; 2009, Operations Research 57(1)), whose framework prices claims through a pricing kernel dQ/dPdQ/dPdQ/dP known to the firm; that framework is adopted here. With two claims on two different random elements the optimal pair is coupled, and existence and uniqueness are no longer automatic.

Setting

Fix a probability space (Ω,F,P)(\Omega,\mathcal F,P)(Ω,F,P) carrying three random elements, valued in arbitrary measurable spaces: the claimable term XXX, the nonclaimable term YYY and the side index III. Write FX=σ(X)\mathcal F_X=\sigma(X)FX​=σ(X) and FI=σ(I)\mathcal F_I=\sigma(I)FI​=σ(I). The firm's business position is π=π(X,Y)\pi=\pi(X,Y)π=π(X,Y) for a Borel revenue function π\piπ, assumed square-integrable.

A claim on XXX is a random variable HHH that is FX\mathcal F_XFX​-measurable and has finite variance; the set of such claims is HX\mathcal H_XHX​, and HI\mathcal H_IHI​ is defined likewise. The centered subspace HX⊆HX\mathbb H_X\subseteq\mathcal H_XHX​⊆HX​ consists of claims with E[H]=0\mathbb E[H]=0E[H]=0.

Claims are priced by a pricing kernel dQ/dPdQ/dPdQ/dP, the density of an equivalent martingale measure QQQ: it is positive almost surely, has mean one and is square-integrable, and EQ[Z]=E[Z dQ/dP]\mathbb E_Q[Z]=\mathbb E[Z\,dQ/dP]EQ​[Z]=E[ZdQ/dP]. The firm ranks positions by the mean–variance criterion

U(Z)=ϱ E[Z]−a2Var⁡[Z],ϱ≥0, a>0.\mathcal U(Z)=\varrho\,\mathbb E[Z]-\tfrac a2\operatorname{Var}[Z],\qquad \varrho\ge 0,\ a>0 .U(Z)=ϱE[Z]−2a​Var[Z],ϱ≥0, a>0.

The value-centered design problem is

max⁡{U(π+[H+G]) : H∈HX, G∈HI, EQ[H]=EQ[G]=0}.(4)\max\Big\{\mathcal U\big(\pi+[H+G]\big)\ :\ H\in\mathcal H_X,\ G\in\mathcal H_I,\ \mathbb E_Q[H]=\mathbb E_Q[G]=0\Big\}.\qquad(4)max{U(π+[H+G]) : H∈HX​, G∈HI​, EQ​[H]=EQ​[G]=0}.(4)

A maximizer (H∗,G∗)(H^*,G^*)(H∗,G∗) is an optimal combined claim pair. The dependence between XXX and III is measured by the maximal correlation

rXI=sup⁡{ρ(ϕ,ψ) : ϕ∈HX, ψ∈HI}∈[0,1],(6)r_{XI}=\sup\big\{\rho(\phi,\psi)\ :\ \phi\in\mathbb H_X,\ \psi\in\mathbb H_I\big\}\in[0,1],\qquad(6)rXI​=sup{ρ(ϕ,ψ) : ϕ∈HX​, ψ∈HI​}∈[0,1],(6)

with ρ\rhoρ the Pearson correlation. Finally K=π+(ϱ/a) dQ/dP\mathcal K=\pi+(\varrho/a)\,dQ/dPK=π+(ϱ/a)dQ/dP is the optimal hedging kernel, Π0X=−E[K−E[K∣FI]∣FX]\Pi^X_0=-\mathbb E\big[\mathcal K-\mathbb E[\mathcal K\mid\mathcal F_I]\mid\mathcal F_X\big]Π0X​=−E[K−E[K∣FI​]∣FX​], and T[Z]=E[E[Z∣FI]∣FX]T[Z]=\mathbb E\big[\mathbb E[Z\mid\mathcal F_I]\mid\mathcal F_X\big]T[Z]=E[E[Z∣FI​]∣FX​].

Formalization targets

Goal: Theorem 1 (p. 11)

If rXI<1r_{XI}<1rXI​<1, then

  1. an optimal combined claim pair (H∗,G∗)(H^*,G^*)(H∗,G∗) of (4) exists;
  2. it is unique up to PPP-null sets, and so is the hedge H∗+G∗H^*+G^*H∗+G∗;
  3. the value-centered optimal claim H0∗=H∗−E[H∗]H^*_0=H^*-\mathbb E[H^*]H0∗​=H∗−E[H∗] solves
H0∗=Π0X+E[E[H0∗∣FI]∣FX].(7)H^*_0=\Pi^X_0+\mathbb E\big[\mathbb E[H^*_0\mid\mathcal F_I]\mid\mathcal F_X\big].\qquad(7)H0∗​=Π0X​+E[E[H0∗​∣FI​]∣FX​].(7)

Milestones

  • Proposition 1 (p. 9): every optimal pair is H∗=H0∗−EQ[H0∗]H^*=H^*_0-\mathbb E_Q[H^*_0]H∗=H0∗​−EQ​[H0∗​], G∗=G0∗−EQ[G0∗]G^*=G^*_0-\mathbb E_Q[G^*_0]G∗=G0∗​−EQ​[G0∗​] with PPP-centered (H0∗,G0∗)(H^*_0,G^*_0)(H0∗​,G0∗​) solving the first-order system (5).
  • (EC.25)–(EC.26) (p. ec24): a centered solution of (5) satisfies H0=Π0+T[H0]H_0=\Pi_0+T[H_0]H0​=Π0​+T[H0​].
  • TTT on HX\mathbb H_XHX​ (p. ec24): E[T[Z]]=E[Z]\mathbb E[T[Z]]=\mathbb E[Z]E[T[Z]]=E[Z], T(HX)⊆HXT(\mathbb H_X)\subseteq\mathbb H_XT(HX​)⊆HX​, and Π0∈HX\Pi_0\in\mathbb H_XΠ0​∈HX​.
  • Inner-product bound (p. ec25): ⟨E[ϕ∣FI],ψ⟩≤rXI∥ϕ∥2∥ψ∥2\langle\mathbb E[\phi\mid\mathcal F_I],\psi\rangle\le r_{XI}\|\phi\|_2\|\psi\|_2⟨E[ϕ∣FI​],ψ⟩≤rXI​∥ϕ∥2​∥ψ∥2​ for ϕ∈HX\phi\in\mathbb H_Xϕ∈HX​, ψ∈HI\psi\in\mathbb H_Iψ∈HI​.
  • (EC.28) (p. ec25): ∥E[ϕ∣FI]∥2≤rXI∥ϕ∥2\|\mathbb E[\phi\mid\mathcal F_I]\|_2\le r_{XI}\|\phi\|_2∥E[ϕ∣FI​]∥2​≤rXI​∥ϕ∥2​.
  • ∥T∥≤rXI\|T\|\le r_{XI}∥T∥≤rXI​ (p. ec25) on HX\mathbb H_XHX​.
  • (EC.27) (p. ec25): if rXI<1r_{XI}<1rXI​<1, H0=Π0+T[H0]H_0=\Pi_0+T[H_0]H0​=Π0​+T[H0​] has a unique solution in HX\mathbb H_XHX​.

Significance

The result. Theorem 1 makes the combined hedge an object: without it the optimal pair may fail to exist or may be non-unique (the paper points to Appendix EC.1(F) for non-uniqueness), and the paper's later results, the design integral equation (Theorem 2) and the value of combining claims (Theorem 3 and Definitions 1–3), are stated for the optimal pair whose existence and uniqueness Theorem 1 provides. Equation (7) separates the optimal claim into a part determined by the kernel K\mathcal KK alone and a cross-claim feedback through III. The condition rXI<1r_{XI}<1rXI​<1 is checkable: for jointly lognormal (X,I)(X,I)(X,I) it reduces to ∣ρZ,W∣<1|\rho_{Z,W}|<1∣ρZ,W​∣<1 for the underlying normals (Example 4).

Formalizing it. The theorem is proved in the paper; no machine-checked version exists. A formal proof needs a Hilbert-space treatment of conditional expectations onto two σ-algebras, a formal maximal-correlation index, and an existence argument for the maximization problem itself, which the paper's proof leaves implicit (see below). The intermediate statements are general facts about pairs of σ-algebras with maximal correlation below one and are reusable outside hedging.

Difficulty

The optimal pair is coupled: the claim on XXX depends on the conditional expectation of the claim on III given XXX and conversely, so neither can be computed first. When XXX and III share information, the two claim spaces overlap and the sum HX+HI\mathcal H_X+\mathcal H_IHX​+HI​ need not be closed in L2L^2L2; a maximizing sequence can then escape, and two different pairs can produce the same hedge. The condition rXI<1r_{XI}<1rXI​<1 excludes this, and the work lies in turning it into a quantitative bound on the alternating conditional-expectation operator.

A second difficulty is a gap in the printed argument. The paper derives the first-order system (5) as a necessary condition and then proves that the resulting fixed-point equation has a unique solution. It does not show that the pair built from that solution is optimal for (4), so existence of a maximizer needs a separate argument that the first-order condition is also sufficient or that the maximum is attained. The goal is stated for maximizers of (4), so this step cannot be skipped.

Formalization scope

Everything lives in the namespace CustomHedge.Exist. A Market bundles PPP, XXX, YYY, III, the revenue function, the kernel D =dQ/dP=dQ/dP=dQ/dP, rho =ϱ=\varrho=ϱ and a; Standing collects the assumptions above. Conventions:

  • Claims are random variables Ω→R\Omega\to\mathbb RΩ→R, strongly measurable for σ(X)\sigma(X)σ(X) (resp. σ(I)\sigma(I)σ(I)) and in L2(P)L^2(P)L2(P), not payoff functions x↦H(x)x\mapsto H(x)x↦H(x).
  • Optimality is maximization of U over all feasible pairs; uniqueness and the equations (5), (7), (EC.25), (EC.27) hold PPP-almost surely.
  • EQ\mathbb E_QEQ​ centers the budget constraint; E=EP\mathbb E=\mathbb E_PE=EP​ centers H0∗H^*_0H0∗​, HX\mathbb H_XHX​ and the maximal correlation.
  • The paper allows a≥0a\ge0a≥0; the formalization requires a>0a>0a>0, because K\mathcal KK divides by aaa and with a=0a=0a=0 problem (4) generally has no maximizer. ϱ=0\varrho=0ϱ=0 is allowed.
  • The maximal correlation is a real supremum over pairs with positive variances (where ρ\rhoρ is defined), with sup⁡∅=0\sup\emptyset=0sup∅=0; the set is bounded by one.
  • ∥Z∥2=(E[Z2])1/2\|Z\|_2=(\mathbb E[Z^2])^{1/2}∥Z∥2​=(E[Z2])1/2; conditional expectation is Mathlib's condExp.

A trivializing formalization is ruled out: the goal quantifies over maximizers of (4), not over solutions of the first-order system or of (EC.27), which are separate milestones. A sorry-free check confirms the standing assumptions and rXI<1r_{XI}<1rXI​<1 hold together with a non-trivial σ(X)\sigma(X)σ(X).

Needed infrastructure: L2L^2L2 conditional expectation as an orthogonal projection, the identity E[E[ϕ∣G]ψ]=E[ϕψ]\mathbb E[\mathbb E[\phi\mid\mathcal G]\psi]=\mathbb E[\phi\psi]E[E[ϕ∣G]ψ]=E[ϕψ] for G\mathcal GG-measurable ψ\psiψ, Banach's fixed-point theorem on a closed subspace of L2L^2L2, and concave maximization over a closed affine subspace. The maximal-correlation file is reusable beyond this mission. Proofs of individual milestones, and a proof of the goal by any route, are welcome.

Selected references

  • P. Guiotto and A. Roncoroni, Combined custom hedging: optimal design, noninsurable exposure, and operational risk management, Operations Research 70(3), 2022. https://doi.org/10.1287/opre.2021.2133 (cited from manuscript OPRE-2019-01-058.R3)
  • R. Caldentey and M. Haugh, Optimal control and hedging of operations in the presence of financial markets, Mathematics of Operations Research 31(2), 2006. https://doi.org/10.1287/moor.1060.0193
  • B. Chowdhry and J. T. B. Howe, Corporate risk management for multinational corporations: financial and operational hedging policies, European Finance Review 2, 229–246, 1999 (as cited in the paper; no link verified).
  • A. Rényi, On measures of dependence, Acta Mathematica Academiae Scientiarum Hungarica 10, 1959. https://doi.org/10.1007/BF02024507
  • B. Schweizer and E. F. Wolff, On nonparametric measures of dependence for random variables, Annals of Statistics 9(4), 1981. https://doi.org/10.1214/aos/1176345528
10 thms1 active userReviewed
Algorithmic Game TheoryConvex OptimizationEconomics·Captain: mikedeng1

Infinite-Dimensional Fisher Markets and Tractable Fair Division 1: The Eisenberg–Gale Programs Attain Their Optima, One at a Pure Allocation, and Optimal Pairs Are Exactly the Market EquilibriaResearch Paper

Why continuum Fisher markets matter

A Fisher market divides a supply of goods among buyers with fixed budgets. In a finite market, each good is a separate coordinate. Fair division can instead involve a continuum of items, such as locations along an interval or points in a region, where a buyer's valuation varies measurably from point to point. Finite dimensional existence and duality arguments do not automatically apply: the allocation is now a function, and the feasible set need not be compact in its natural function space. Gao and Kroer formulate a market and two Eisenberg–Gale programs for this setting, then prove that their optima exist and characterize equilibrium Gao and Kroer, §3.

The result also connects market equilibrium to fair division. A pure allocation assigns measurable regions of the item space to buyers, allowing overlap only on null sets. Existence of a pure optimizer means that a market outcome can be represented by such a division, rather than by fractional shares at each item. The same paper derives Pareto optimality, budget weighted envy freeness, and proportionality for equilibrium allocations Gao and Kroer, Theorems 1 and 3.

Market, allocations, and programs

The item space Θ\ThetaΘ is a compact subset of Rd\mathbb R^dRd with restricted Lebesgue measure μ\muμ. There are nnn buyers. Buyer iii has a budget Bi>0B_i>0Bi​>0 and a nonnegative integrable valuation density viv_ivi​ with ∫Θvi dμ>0\int_\Theta v_i\,d\mu>0∫Θ​vi​dμ>0. The utility of a bounded nonnegative bundle xix_ixi​ is ⟨vi,xi⟩=∫Θvixi dμ\langle v_i,x_i\rangle=\int_\Theta v_i x_i\,d\mu⟨vi​,xi​⟩=∫Θ​vi​xi​dμ. An allocation x=(xi)x=(x_i)x=(xi​) is feasible when ∑ixi≤1\sum_i x_i\le1∑i​xi​≤1 almost everywhere. It is pure when each xix_ixi​ equals the indicator of a measurable set Θi⊆Θ\Theta_i\subseteq\ThetaΘi​⊆Θ, up to almost everywhere equality, and these sets are pairwise disjoint up to null sets. Leftover items are allowed.

A nonnegative integrable price density ppp defines a buyer's affordable bundles by ⟨p,xi⟩≤Bi\langle p,x_i\rangle\le B_i⟨p,xi​⟩≤Bi​. A market equilibrium (x,p)(x,p)(x,p) is a feasible allocation and price at which every buyer maximizes utility among affordable bundles and ⟨p,1−∑ixi⟩=0\langle p,1-\sum_i x_i\rangle=0⟨p,1−∑i​xi​⟩=0. Thus unallocated supply may remain only where it has zero price. The paper's primal Eisenberg–Gale program, PEG\mathcal P_{EG}PEG​, maximizes weighted log utility over feasible allocations. Its dual program, DEG\mathcal D_{EG}DEG​, minimizes total price minus weighted log multipliers subject to p≥βivip\ge\beta_i v_ip≥βi​vi​ almost everywhere Gao and Kroer, pp. 6–8.

Formalization targets

The goal is the three part Theorem 1. In the notation above, it asserts attainment of the primal objective at a pure allocation, attainment of the dual objective with a unique multiplier vector β∗\beta^*β∗ and price p∗=max⁡iβi∗vip^*=\max_i\beta_i^*v_ip∗=maxi​βi∗​vi​ almost everywhere, and the equivalence

(x,p) is a market equilibrium⟺x optimizes PEG and (p,β∗) optimizes DEG.(x,p)\text{ is a market equilibrium} \quad\Longleftrightarrow\quad x\text{ optimizes }\mathcal P_{EG}\ \text{and}\ (p,\beta^*)\text{ optimizes }\mathcal D_{EG}.(x,p) is a market equilibrium⟺x optimizes PEG​ and (p,β∗) optimizes DEG​.

The milestone list follows the results the paper uses to reach that goal. Lemma A.1 gives a convex, compact range for utility matrices and, under atomlessness, identifies mixed and partition based ranges. Lemma 1 specializes this to the market's feasible utility set UUU, proving that UUU is compact and convex and equals the pure utility set U′U'U′. Lemma 2 establishes attainment and uniqueness in the finite dimensional reduction of the dual problem. Lemma 3 gives weak duality with the paper's constant C=∑iBi−∑iBilog⁡BiC=\sum_i B_i-\sum_i B_i\log B_iC=∑i​Bi​−∑i​Bi​logBi​ and its three optimality conditions. Theorem 2 expands the equivalence between optimality and equilibrium, including budget exhaustion and the utility formula ⟨vi,xi⟩=Bi/βi\langle v_i,x_i\rangle=B_i/\beta_i⟨vi​,xi​⟩=Bi​/βi​. These are the paper's numbered results on pp. 8–10 and a1 Gao and Kroer, §3 and Appendix A.1.

The proposal also states Theorem 3, Lemma 4, and Corollaries 1–3 as companion results. They record the resulting fairness properties, normalized equilibrium bounds, winning sets, a construction of dual prices from a pure optimum, and a test for a pure equilibrium Gao and Kroer, pp. 10–11.

What the result provides

Theorem 1 shows that the two programs give actual allocations and prices in the continuum market, not merely limiting objective values. The pure optimizer provides measurable regions for buyers. The dual multipliers give a unique utility price for each buyer, while the price density is determined almost everywhere. Theorem 2 makes these program outputs economically interpretable: each buyer exhausts its budget at equilibrium. Theorem 3 then supplies efficiency and fairness guarantees for those allocations Gao and Kroer, Theorems 1–3.

These results are proved in the cited paper. This mission asks for machine checked Lean proofs of those mathematical statements. Its definitions of allocations, demand, equilibrium, the two programs, and feasible utilities could also support formalization of the paper's later geometric and quasilinear results. The draft declarations compile as open statements; compilation does not establish the theorems.

Why the proof is difficult

The feasible allocations are bounded in an infinite dimensional function space, but that does not make the set compact in the topology used for the optimization problem. The paper instead needs compactness of the finite dimensional set of achievable utility vectors. The range result in Lemma A.1 is therefore central, and its atomless conclusion must be strong enough to replace fractional allocations by measurable partitions Gao and Kroer, Lemma 1 and Appendix A.1.

Standard constraint qualification arguments also do not supply the required duality theorem here: the positive cone in L1(Θ)L^1(\Theta)L1(Θ) has empty interior. The proposal consequently asks for the paper's specific weak duality inequality, attainment, and optimality characterization rather than assuming a general finite dimensional duality theorem applies Gao and Kroer, Remark 1.

Formalization scope

Lean uses real valued measurable functions on the ambient Euclidean space with measure μ=volume∣Θ\mu=\mathrm{volume}|_\Thetaμ=volume∣Θ​. It identifies prices and allocations up to μ\muμ almost everywhere equality, as the paper identifies L1L^1L1 and L∞L^\inftyL∞ equivalence classes. Bundles must belong to L∞(μ)L^\infty(\mu)L∞(μ) and prices and valuations must be integrable; these conditions prevent a nonintegrable product from receiving Lean's default integral value of zero. The number of buyers may be zero, consistent with the finite index formulation, while the standing positivity hypotheses apply to every buyer present.

The real logarithm in Lean returns zero at zero. The optimization predicates instead require positive utility or positive dual multipliers and compare only with other positive points, matching the paper's log⁡0=−∞\log 0=-\inftylog0=−∞ objective convention. The maximization over buyers is the finite supremum sup⁡iβivi\sup_i\beta_i v_isupi​βi​vi​. Price and allocation uniqueness is stated almost everywhere; multiplier uniqueness is exact. Lemma A.1 uses the paper's divisible measure condition for atomlessness and fixes its unnamed almost everywhere partition convention by requiring ∑jxj=1\sum_jx_j=1∑j​xj​=1 everywhere. Corollary 3 explicitly requires each denominator vi(Θi)v_i(\Theta_i)vi​(Θi​) to be positive. Lemma 4 alone assumes the normalizations vi(Θ)=1v_i(\Theta)=1vi​(Θ)=1 and ∑iBi=1\sum_iB_i=1∑i​Bi​=1, which the paper recalls before its statement.

The goal remains the full three part theorem. It does not assume the range theorem, duality equality, or optimality conditions it is meant to establish. Contributions to the measure range theorem, utility set compactness, the dual reduction, and the equilibrium characterization are all within scope.

Selected references

  • Yuan Gao and Christian Kroer, Infinite-Dimensional Fisher Markets and Tractable Fair Division, Operations Research, 2023; formalization follows arXiv:2010.03025v5, 2021, §§2–3 and Appendix A.1.
9 thms1 active userReviewed
Algorithmic Game TheoryMechanism DesignOperations Research+1·Captain: mikedeng1

Contextual Standard Auctions with Budgets: Revenue Equivalence and Efficiency Guarantees 1: A Value Pacing-Based Symmetric First Price Equilibrium ExistsResearch Paper

Motivation

Most online advertising is sold by auction, one impression at a time, to advertisers who manage a budget over many auctions rather than a value for a single one. Since 2019 the major ad exchanges have moved from second price to first price auctions, in which the winner pays its own bid. A budget-constrained advertiser in a first price auction must therefore shade its bids twice: once because of the budget, and once because of the payment rule. Whether these two effects admit a coherent equilibrium, and of what form, is the question behind Balseiro, Kroer and Kumar, Contextual Standard Auctions with Budgets: Revenue Equivalence and Efficiency Guarantees (Management Science, 2023, doi:10.1287/mnsc.2023.4719).

Earlier work on pacing equilibria treated second price auctions, where truthful bidding is dominant without budgets (Balseiro, Besbes and Weintraub 2015; Conitzer et al. 2022). In first price auctions with a single deterministic item, an equilibrium may fail to exist (the paper's Online Appendix A). The paper restores existence by letting items carry a random context and values depend on it linearly. This mission formalizes its first main result, Theorem 1: an equilibrium of a simple, interpretable form exists.

Setting

An item has a context α∈A⊂R+d\alpha\in A\subset\mathbb R^d_{+}α∈A⊂R+d​, a feature vector drawn from a law FFF with a density. There are nnn buyers. Each buyer has a type θ=(w,B)\theta=(w,B)θ=(w,B), a weight vector www and a budget BBB, drawn independently from a law GGG with a density on

Θ=(0,U)d×(Bmin⁡,U).\Theta=(0,U)^d\times(B_{\min},U).Θ=(0,U)d×(Bmin​,U).

Buyer (w,B)(w,B)(w,B) values item α\alphaα at wTαw^T\alphawTα, and ω:=sup⁡(w,B)∈Θ,α∈AwTα\omega:=\sup_{(w,B)\in\Theta,\alpha\in A}w^T\alphaω:=sup(w,B)∈Θ,α∈A​wTα. The seller reveals α\alphaα, then runs a first price auction with a public reserve price r(α)r(\alpha)r(α): a bid b(α)b(\alpha)b(α) wins if b(α)≥max⁡(r(α),{β(θi,α)}i)b(\alpha)\ge\max(r(\alpha),\{\beta(\theta_i,\alpha)\}_i)b(α)≥max(r(α),{β(θi​,α)}i​), where β\betaβ is the strategy of the n−1n-1n−1 competitors, and the winner pays its bid. A budget only needs to hold in expectation over α\alphaα and the competitors' types.

A strategy β∗:Θ×A→R≥0\beta^*:\Theta\times A\to\mathbb R_{\ge0}β∗:Θ×A→R≥0​ is a symmetric first price equilibrium (SFPE, Definition 1) if for GGG-almost every type (w,B)(w,B)(w,B) the bid function β∗(w,B,⋅)\beta^*(w,B,\cdot)β∗(w,B,⋅) solves

max⁡b:A→R≥0 E[(wTα−b(α))1{b(α)≥max⁡(r(α),{β∗(θi,α)}i)}]  s.t.  E[b(α)1{⋯ }]≤B.\max_{b:A\to\mathbb R_{\ge0}}\ \mathbb E\big[(w^T\alpha-b(\alpha))\mathbb 1\{b(\alpha)\ge\max(r(\alpha),\{\beta^*(\theta_i,\alpha)\}_i)\}\big]\ \ \text{s.t.}\ \ \mathbb E\big[b(\alpha)\mathbb 1\{\cdots\}\big]\le B .b:A→R≥0​max​ E[(wTα−b(α))1{b(α)≥max(r(α),{β∗(θi​,α)}i​)}]  s.t.  E[b(α)1{⋯}]≤B.

A pacing function μ:Θ→R≥0\mu:\Theta\to\mathbb R_{\ge0}μ:Θ→R≥0​ scales values down to paced values wTα/(1+μ(w,B))w^T\alpha/(1+\mu(w,B))wTα/(1+μ(w,B)). Let HαμH^\mu_\alphaHαμ​ be the distribution function of the highest of n−1n-1n−1 i.i.d. paced values, and for x≥r(α)x\ge r(\alpha)x≥r(α) let

σαμ(x)=x−∫r(α)xHαμ(s)Hαμ(x) ds,\sigma^\mu_\alpha(x)=x-\int_{r(\alpha)}^x\frac{H^\mu_\alpha(s)}{H^\mu_\alpha(x)}\,ds,σαμ​(x)=x−∫r(α)x​Hαμ​(x)Hαμ​(s)​ds,

with σαμ(x)=0\sigma^\mu_\alpha(x)=0σαμ​(x)=0 if Hαμ(x)=0H^\mu_\alpha(x)=0Hαμ​(x)=0 and σαμ(x)=x\sigma^\mu_\alpha(x)=xσαμ​(x)=x if x<r(α)x<r(\alpha)x<r(α). The value pacing–based strategy (Definition 2) is

βμ(w,B,α)=σαμ(wTα1+μ(w,B)).\beta^\mu(w,B,\alpha)=\sigma^\mu_\alpha\Big(\frac{w^T\alpha}{1+\mu(w,B)}\Big).βμ(w,B,α)=σαμ​(1+μ(w,B)wTα​).

For a buyer facing competitors who use βμ\beta^\muβμ, the dual function is qμ(w,B,t)=sup⁡bE[(wTα−(1+t)b(α))1{⋯ }]+tBq^\mu(w,B,t)=\sup_b\mathbb E[(w^T\alpha-(1+t)b(\alpha))\mathbb 1\{\cdots\}]+tBqμ(w,B,t)=supb​E[(wTα−(1+t)b(α))1{⋯}]+tB for t≥0t\ge0t≥0.

Formalization targets

Goal: Theorem 1 (p. 7)

∃ μ:Θ→R≥0such thatβμ is an SFPE.\exists\,\mu:\Theta\to\mathbb R_{\ge0}\quad\text{such that}\quad \beta^\mu\ \text{is an SFPE}.∃μ:Θ→R≥0​such thatβμ is an SFPE.

Milestones

  • Lemma 1 (p. 8): for every type and every t≥0t\ge0t≥0, σαμ(wTα/(1+t))\sigma^\mu_\alpha(w^T\alpha/(1+t))σαμ​(wTα/(1+t)) maximizes the Lagrangian E[(wTα/(1+t)−b(α))1{⋯ }]\mathbb E[(w^T\alpha/(1+t)-b(\alpha))\mathbb 1\{\cdots\}]E[(wTα/(1+t)−b(α))1{⋯}].
  • Proposition 1 (p. 8): on a set Θ′\Theta'Θ′ of full GGG-measure, for every μ\muμ, a minimizer t∗t^*t∗ of qμ(w,B,⋅)q^\mu(w,B,\cdot)qμ(w,B,⋅) over t≥0t\ge0t≥0 makes σαμ(wTα/(1+t∗))\sigma^\mu_\alpha(w^T\alpha/(1+t^*))σαμ​(wTα/(1+t∗)) optimal for the budget-constrained problem Qμ(w,B)Q^\mu(w,B)Qμ(w,B).
  • Lemma 2 (p. 10): the smallest minimizer ℓμ(w,B)\ell^\mu(w,B)ℓμ(w,B) of qμ(w,B,⋅)q^\mu(w,B,\cdot)qμ(w,B,⋅) over [0,ω/Bmin⁡][0,\omega/B_{\min}][0,ω/Bmin​] is nondecreasing in each wiw_iwi​ and nonincreasing in BBB.
  • Lemma 3 (p. 10): ℓμ∈L1(Θ)\ell^\mu\in L_1(\Theta)ℓμ∈L1​(Θ) and its total variation is at most V0=(d+1)max⁡(Ud,Ud+1) ω/Bmin⁡V_0=(d+1)\max(U^d,U^{d+1})\,\omega/B_{\min}V0​=(d+1)max(Ud,Ud+1)ω/Bmin​. The paper prints (d+1)Ud+1ω/Bmin⁡(d+1)U^{d+1}\omega/B_{\min}(d+1)Ud+1ω/Bmin​, which agrees when U≥1U\ge1U≥1. For U<1U<1U<1 the printed bound fails by a rescaling argument, and the mission corrects the exponent to ddd there.
  • Lemma 4 (p. 10): X0={μ∈L1(Θ):0≤μ≤ω/Bmin⁡, V(μ,Θ)≤V0}\mathcal X_0=\{\mu\in L_1(\Theta):0\le\mu\le\omega/B_{\min},\ V(\mu,\Theta)\le V_0\}X0​={μ∈L1​(Θ):0≤μ≤ω/Bmin​, V(μ,Θ)≤V0​} is nonempty, compact and convex in L1(Θ)L_1(\Theta)L1​(Θ); f(μ,μ^)=EG[qμ(w,B,μ^(w,B))]f(\mu,\hat\mu)=\mathbb E_G[q^\mu(w,B,\hat\mu(w,B))]f(μ,μ^​)=EG​[qμ(w,B,μ^​(w,B))] is continuous; C0∗(μ)=arg⁡min⁡μ^∈X0f(μ,μ^)C^*_0(\mu)=\arg\min_{\hat\mu\in\mathcal X_0}f(\mu,\hat\mu)C0∗​(μ)=argminμ^​∈X0​​f(μ,μ^​) is upper hemicontinuous with nonempty, convex, compact values.
  • Lemma 5 (p. 10): a fixed point μ∈C0∗(μ)\mu\in C^*_0(\mu)μ∈C0∗​(μ) satisfies μ(w,B)∈arg⁡min⁡t∈[0,ω/Bmin⁡]qμ(w,B,t)\mu(w,B)\in\arg\min_{t\in[0,\omega/B_{\min}]}q^\mu(w,B,t)μ(w,B)∈argmint∈[0,ω/Bmin​]​qμ(w,B,t) almost surely.
  • Proposition 2 (p. 9): some μ\muμ satisfies μ(w,B)∈arg⁡min⁡t≥0qμ(w,B,t)\mu(w,B)\in\arg\min_{t\ge0}q^\mu(w,B,t)μ(w,B)∈argmint≥0​qμ(w,B,t) almost surely.

The paper states that Proposition 2 combined with Proposition 1 implies Theorem 1.

Significance

Theorem 1 says that budget-constrained buyers in contextual first price auctions have an equilibrium that is described by one scalar per type: shade the value by the factor 1/(1+μ(w,B))1/(1+\mu(w,B))1/(1+μ(w,B)), then bid as an unconstrained buyer would in an i.i.d. first price auction against paced competitors. This is the object on which the rest of the paper is built: revenue equivalence across standard auctions (Theorem 2) and a liquid-welfare price of anarchy of at least 1/21/21/2 (Theorem 3) are both statements about pacing-based equilibria. Practically, it supports the use of pacing for budget management in first price auctions, with pacing multipliers computed as for second price auctions.

The result is proved in the paper; every proof is in its online appendix, which is not part of the source this mission cites. Nothing in the paper is formalized. A formalization would check a strong-duality argument for a non-convex problem and an infinite-dimensional fixed-point argument whose topology the authors chose with care, and it would produce reusable pieces: multivariate total variation, compactness of bounded-variation sets in L1L_1L1​, and the first price equilibrium bid against an arbitrary (possibly atomic) value distribution with a reserve price.

Difficulty

The buyer's problem Qμ(w,B)Q^\mu(w,B)Qμ(w,B) is not convex in the bid function, so standard convex duality does not give strong duality; Proposition 1 needs a direct argument combining Lagrangian optimality (Lemma 1), differentiability of qμq^\muqμ in ttt, and complementary slackness. Lemma 1 itself cannot quote the textbook first price equilibrium, because the paced value distribution λαμ\lambda^\mu_\alphaλαμ​ may have atoms and the reserve price creates discontinuities.

The fixed point lives in an infinite-dimensional space of pacing functions. The obvious topologies fail: the set X\mathcal XX of bounded pacing functions is not compact in any LpL_pLp​, and in the weak-* topology of L∞L_\inftyL∞​ upper hemicontinuity of the best-response correspondence is hard to obtain; restricting to Lipschitz functions loses the property that best responses stay in the set. The paper restricts to functions of bounded total variation, which requires the monotonicity of Lemma 2 and the variation bound of Lemma 3.

Formalization scope

Contexts are Fin d → ℝ, types are pairs (w, B) : (Fin d → ℝ) × ℝ, and wTαw^T\alphawTα is the explicit sum ∑iwiαi\sum_i w_i\alpha_i∑i​wi​αi​. A single Model structure holds d,n,U,Bmin⁡,A,F,G,rd,n,U,B_{\min},A,F,G,rd,n,U,Bmin​,A,F,G,r, and Model.Standing collects the assumptions of §2.2 together with four that the paper uses without stating them: n≥2n\ge2n≥2, Bmin⁡<UB_{\min}<UBmin​<U, AAA nonempty and bounded (so ω<∞\omega<\inftyω<∞), and measurability of AAA and rrr. Pacing functions are measurable functions on Rd×R\mathbb R^d\times\mathbb RRd×R that are nonnegative on Θ\ThetaΘ; values off Θ\ThetaΘ are irrelevant since G(Θc)=0G(\Theta^c)=0G(Θc)=0.

The conventions fixed in Lean:

  • Ties win: the indicator is b(α)≥max⁡(⋯ )b(\alpha)\ge\max(\cdots)b(α)≥max(⋯), as in the paper's tie-breaking rule.
  • An admissible bid function is measurable, nonnegative on AAA, and has an integrable payment integrand. The problem of Definition 1, QμQ^\muQμ, qμq^\muqμ and the Lagrangian of Lemma 1 all range over this class.
  • An SFPE is jointly measurable in (θ,α)(\theta,\alpha)(θ,α), so Theorem 1 must produce a measurable strategy.
  • qμq^\muqμ is the supremum over bids of p. 7, not the closed form of p. 8. σαμ\sigma^\mu_\alphaσαμ​ has an explicit branch for Hαμ(x)=0H^\mu_\alpha(x)=0Hαμ​(x)=0.
  • Argmins are stated as membership plus IsMinOn, over t≥0t\ge0t≥0 in Propositions 1–2 and over [0,ω/Bmin⁡][0,\omega/B_{\min}][0,ω/Bmin​] in Lemma 5 and ℓμ\ell^\muℓμ, as printed.
  • V(u,Ω)V(u,\Omega)V(u,Ω) takes values in EReal, with Euclidean ∥ϕ(x)∥≤1\|\phi(x)\|\le1∥ϕ(x)∥≤1 and test fields supported in Ω\OmegaΩ; L1(Θ)L_1(\Theta)L1​(Θ) is with respect to Lebesgue measure. Lemma 4 is stated on the image of X0\mathcal X_0X0​ in Lp ℝ 1 (volume.restrict Θ), in its norm topology.

A formalization in which qμq^\muqμ is defined by its closed form, in which non-integrable payments count as zero, or in which the strategy need not be measurable would make the milestones easier without proving the paper's theorem; these readings are excluded by the definitions above.

A complete development needs: first price equilibrium bids for general atomic distributions with reserves; measurability of parametric integrals; a duality argument for one-dimensional Lagrangian relaxations; multivariate bounded variation and its compact embedding in L1L_1L1​ of a box; and the Kakutani–Fan–Glicksberg theorem in a locally convex space. The bounded-variation and fixed-point parts are reusable beyond this mission. Proofs of any milestone, and alternative arguments, are welcome.

Selected references

  • S. R. Balseiro, C. Kroer, R. Kumar, Contextual Standard Auctions with Budgets: Revenue Equivalence and Efficiency Guarantees, Management Science, Articles in Advance, 2023. https://doi.org/10.1287/mnsc.2023.4719
  • S. R. Balseiro, O. Besbes, G. Y. Weintraub, Repeated Auctions with Budgets in Ad Exchanges: Approximations and Design, Management Science 61(4), 2015. https://doi.org/10.1287/mnsc.2014.2022
  • V. Conitzer, C. Kroer, E. Sodomka, N. E. Stier-Moses, Multiplicative Pacing Equilibria in Auction Markets, Operations Research 70(2), 2022. https://doi.org/10.1287/opre.2021.2167
  • V. Krishna, Auction Theory, 2nd ed., Academic Press, 2009.
  • L. C. Evans, R. F. Gariepy, Measure Theory and Fine Properties of Functions, revised ed., CRC Press, 2015.
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Operations ResearchOptimizationPartial Differential Equations·Captain: mikedeng1

Optimality Conditions in Control Problems with Random State Constraints in Probabilistic or Almost Sure Form IV: Radon-Measure Optimality Conditions for Robust State ConstraintsResearch Paper

Motivation

Optimal control problems governed by partial differential equations (PDEs) often carry uncertainty in their data, for example a random source term. When the state must stay below a threshold, there are several ways to impose the constraint: with high probability (chance constraints), almost surely, or for every value in a fixed uncertainty set (robust constraints). C. Geiersbach and R. Henrion (arXiv:2306.03965v2, Math. Oper. Res. 2025) derive first-order optimality conditions for all three models for the same elliptic model problem. This mission covers the robust model of §3.2 (pp. 23–25). Its Karush–Kuhn–Tucker (KKT) system has a Radon measure as multiplier, and it is related to the semi-infinite programming view of the same problem.

Robust state constraints are also the limiting case of the almost-sure model: by Lemma 3.4 of the paper (p. 19), an almost-sure constraint and the constraint for every parameter in the support of the distribution coincide when the constraint function is lower semicontinuous in the parameter. The robust multipliers live in C(Dˉ×Ξ)∗C(\bar D\times\Xi)^*C(Dˉ×Ξ)∗, which is a space of measures, whereas the almost-sure multipliers of §3.1 contain singular functionals with no such representation.

Setting

Let D⊆RdD\subseteq\mathbb R^dD⊆Rd, d∈{1,2,3}d\in\{1,2,3\}d∈{1,2,3}, be open, bounded and of class S: there are γ∈(0,1)\gamma\in(0,1)γ∈(0,1) and r0>0r_0>0r0​>0 such that meas⁡(Br(x)∖D)≥γmeas⁡(Br(x))\operatorname{meas}(B_r(x)\setminus D)\ge\gamma\operatorname{meas}(B_r(x))meas(Br​(x)∖D)≥γmeas(Br​(x)) for all x∈∂Dx\in\partial Dx∈∂D and 0<r<r00<r<r_00<r<r0​. Let Ξ⊂Rm\Xi\subset\mathbb R^mΞ⊂Rm be compact, let f0,φ1,…,φm∈L2(D)f_0,\varphi_1,\dots,\varphi_m\in L^2(D)f0​,φ1​,…,φm​∈L2(D), and set f(x,z)=f0(x)+∑i=1mziφi(x)f(x,z)=f_0(x)+\sum_{i=1}^m z_i\varphi_i(x)f(x,z)=f0​(x)+∑i=1m​zi​φi​(x) (Assumption 1.1, eq. (3)). The solution operator A−1:L2(D)→C(Dˉ)A^{-1}:L^2(D)\to C(\bar D)A−1:L2(D)→C(Dˉ) maps FFF to the unique weak solution y∈H01(D)∩C(Dˉ)y\in H^1_0(D)\cap C(\bar D)y∈H01​(D)∩C(Dˉ) of −Δy=F-\Delta y=F−Δy=F in DDD, y=0y=0y=0 on ∂D\partial D∂D.

For a control u∈L2(D)u\in L^2(D)u∈L2(D), a cost F:L2(D)→RF:L^2(D)\to\mathbb RF:L2(D)→R and a threshold α∈R\alpha\in\mathbb Rα∈R, the robust problem (63) is

min⁡u∈L2(D)F(u)s.t.−Δy^(⋅,z)=u+f(⋅,z) in D,y^(⋅,z)=0 on ∂D,y^(x,z)≤α  ∀(x,z)∈D×Ξ.\min_{u\in L^2(D)}F(u)\quad\text{s.t.}\quad -\Delta\hat y(\cdot,z)=u+f(\cdot,z)\ \text{in }D,\quad \hat y(\cdot,z)=0\ \text{on }\partial D,\quad \hat y(x,z)\le\alpha\ \ \forall (x,z)\in D\times\Xi.u∈L2(D)min​F(u)s.t.−Δy^​(⋅,z)=u+f(⋅,z) in D,y^​(⋅,z)=0 on ∂D,y^​(x,z)≤α  ∀(x,z)∈D×Ξ.

The state is S^(u)∈C(Dˉ×Ξ)\hat{\mathcal S}(u)\in C(\bar D\times\Xi)S^(u)∈C(Dˉ×Ξ), [S^(u)](x,z)=[A−1(u+f(⋅,z))](x)[\hat{\mathcal S}(u)](x,z)=[A^{-1}(u+f(\cdot,z))](x)[S^(u)](x,z)=[A−1(u+f(⋅,z))](x), and G^(u)=S^(u)−α\hat{\mathcal G}(u)=\hat{\mathcal S}(u)-\alphaG^​(u)=S^(u)−α. The cone is K^={y∈C(Dˉ×Ξ):y≤0}\hat{\mathcal K}=\{y\in C(\bar D\times\Xi):y\le0\}K^={y∈C(Dˉ×Ξ):y≤0} and its polar cone is K^−={y∗∈C(Dˉ×Ξ)∗:⟨y∗,y⟩≤0 ∀y∈K^}\hat{\mathcal K}^-=\{y^*\in C(\bar D\times\Xi)^*:\langle y^*,y\rangle\le0\ \forall y\in\hat{\mathcal K}\}K^−={y∗∈C(Dˉ×Ξ)∗:⟨y∗,y⟩≤0 ∀y∈K^}. The linear part of the state is [A^−1B^h](x,z)=[A−1h](x)[\hat{\mathcal A}^{-1}\hat{\mathcal B}h](x,z)=[A^{-1}h](x)[A^−1B^h](x,z)=[A−1h](x). The active set is M(u)={(x,z)∈Dˉ×Ξ:[S^(u)](x,z)=max⁡Dˉ×ΞS^(u)}M(u)=\{(x,z)\in\bar D\times\Xi:[\hat{\mathcal S}(u)](x,z)=\max_{\bar D\times\Xi}\hat{\mathcal S}(u)\}M(u)={(x,z)∈Dˉ×Ξ:[S^(u)](x,z)=maxDˉ×Ξ​S^(u)}.

Formalization targets

Goal: Lemma 3.14 refined to (66), pp. 23–24

Let FFF be convex and continuously Fréchet differentiable, and assume the constraint qualification 0∈int⁡{G^(L2(D))−K^}0\in\operatorname{int}\{\hat{\mathcal G}(L^2(D))-\hat{\mathcal K}\}0∈int{G^​(L2(D))−K^}. Then u∗u^*u∗ is a solution of (63) if and only if there is a nonnegative finite Borel measure μ∗\mu^*μ∗ on Dˉ×Ξ\bar D\times\XiDˉ×Ξ with, for y∗=S^(u∗)y^*=\hat{\mathcal S}(u^*)y∗=S^(u∗),

⟨DF(u∗),h⟩+∫Dˉ×Ξ[A−1h](x) dμ∗(x,z)=0∀h∈L2(D),\langle DF(u^*),h\rangle+\int_{\bar D\times\Xi}[A^{-1}h](x)\,d\mu^*(x,z)=0\quad\forall h\in L^2(D),⟨DF(u∗),h⟩+∫Dˉ×Ξ​[A−1h](x)dμ∗(x,z)=0∀h∈L2(D), y∗≤α on Dˉ×Ξ,∫Dˉ×Ξ(y∗−α) dμ∗=0.y^*\le\alpha\ \text{on }\bar D\times\Xi,\qquad\int_{\bar D\times\Xi}(y^*-\alpha)\,d\mu^*=0.y∗≤α on Dˉ×Ξ,∫Dˉ×Ξ​(y∗−α)dμ∗=0.

The page derives (66) from the abstract system (65) of Lemma 3.14 (necessity). Sufficiency is the converse direction of Lemma 3.14, since a nonnegative measure defines a multiplier in K^−\hat{\mathcal K}^-K^− by integration. Both directions are part of the goal.

Milestones

  1. Lemma 3.13: unique solvability of (63b)–(63c) in C(Dˉ×Ξ)C(\bar D\times\Xi)C(Dˉ×Ξ) with the bound (64).
  2. Lemma 3.14: the abstract KKT system (65) with λ∗∈C(Dˉ×Ξ)∗\lambda^*\in C(\bar D\times\Xi)^*λ∗∈C(Dˉ×Ξ)∗.
  3. The identification C(Dˉ×Ξ)∗≅M(Dˉ×Ξ)C(\bar D\times\Xi)^*\cong\mathcal M(\bar D\times\Xi)C(Dˉ×Ξ)∗≅M(Dˉ×Ξ) (p. 23): every λ∗\lambda^*λ∗ is integration against a signed measure.
  4. Nonnegativity (p. 24): λ∗∈K^−\lambda^*\in\hat{\mathcal K}^-λ∗∈K^− gives a nonnegative μ∗\mu^*μ∗.
  5. Lemma 3.15: (66) is equivalent to the scalar-multiplier form (67): λ∗≥0\lambda^*\ge0λ∗≥0 and a probability measure μ~\tilde\muμ~​ on M(u∗)M(u^*)M(u∗) with ⟨DF(u∗),h⟩+λ∗∫[A−1h](x) dμ~=0\langle DF(u^*),h\rangle+\lambda^*\int[A^{-1}h](x)\,d\tilde\mu=0⟨DF(u∗),h⟩+λ∗∫[A−1h](x)dμ~​=0, max⁡y∗≤α\max y^*\le\alphamaxy∗≤α, λ∗(max⁡y∗−α)=0\lambda^*(\max y^*-\alpha)=0λ∗(maxy∗−α)=0.
  6. Lemma 3.16: the convex-hull condition (68) is equivalent to the existence of such a μ~\tilde\muμ~​.
  7. Lemma 3.4: for lower semicontinuous hhh, h(ξ)≤0h(\xi)\le0h(ξ)≤0 almost surely if and only if h≤0h\le0h≤0 on the support of the law of ξ\xiξ.

Significance

The goal gives the robust problem a KKT system whose multiplier is a nonnegative measure on Dˉ×Ξ\bar D\times\XiDˉ×Ξ that is carried by the points where the constraint is active. Lemmas 3.15 and 3.16 turn this into a scalar multiplier times a probability measure on the active set, and into a convex-hull condition. These are the forms used by semi-infinite programming algorithms and by discretizations that approximate the measure by finitely many atoms. Together with Lemma 3.4, they say when the KKT system of the almost-sure model (§3.1, with its singular multipliers) can be replaced by the measure-valued system of the robust model.

All statements of the mission are proved in the paper, some by reference: Lemma 3.14's proof refers to the argument of Lemma 3.7, and Lemma 3.16 relies on Phelps's barycenter theorem. None of them is formalized. A formal development would also check two points that the page leaves implicit. Lemma 3.15's proof divides by the total mass of μ∗\mu^*μ∗ and does not treat μ∗=0\mu^*=0μ∗=0. Condition (68) is printed per direction hhh, while (67a) needs one measure for all hhh.

Difficulty

The necessity direction of the goal needs a Lagrange multiplier theorem in a Banach space whose constraint cone K^\hat{\mathcal K}K^ has nonempty interior. The multiplier is a priori only an element of C(Dˉ×Ξ)∗C(\bar D\times\Xi)^*C(Dˉ×Ξ)∗, and the Riesz–Markov–Kakutani theorem on the compact space Dˉ×Ξ\bar D\times\XiDˉ×Ξ turns it into a measure. The state S^(u)\hat{\mathcal S}(u)S^(u) must also be shown to lie in C(Dˉ×Ξ)C(\bar D\times\Xi)C(Dˉ×Ξ). Continuity of each slice in xxx is the regularity of Lemma 1.2 (continuity of H01H^1_0H01​ solutions up to the boundary for class-S domains, from Kinderlehrer–Stampacchia), and joint continuity needs the bound (64), uniform in zzz. Working pointwise in zzz does not give these: a family of continuous slices need not be jointly continuous without an estimate that is uniform in the parameter.

Formalization scope

Dˉ\bar DDˉ and Ξ\XiΞ are subtypes of Euclidean spaces with CompactSpace instances, so C(Dˉ×Ξ)C(\bar D\times\Xi)C(Dˉ×Ξ) carries its sup norm. Measures on Dˉ×Ξ\bar D\times\XiDˉ×Ξ are Borel measures; on this compact metric space every finite Borel measure is regular, so "regular Borel (Radon) measure" is IsFiniteMeasure, and nonnegativity (66c) is built into Lean's Measure type. The solution operator is a hypothesis: a bounded linear map L2(D)→C(Dˉ)L^2(D)\to C(\bar D)L2(D)→C(Dˉ) such that A−1FA^{-1}FA−1F is, for every FFF, the weak solution in H01(D)∩C(Dˉ)H^1_0(D)\cap C(\bar D)H01​(D)∩C(Dˉ), encoded with the published weak-derivative definitions HunterPDE.Shared.WeakDeriv. The page's "≤0\le0≤0 in D×ΞD\times\XiD×Ξ" is encoded on Dˉ×Ξ\bar D\times\XiDˉ×Ξ, the same condition for continuous functions. "Solution" means global minimizer over the feasible set. L2(D)∗L^2(D)^*L2(D)∗ is identified with L2(D)L^2(D)L2(D) through the Riesz map. In Lemma 3.16 the clco of (68) is the norm closure of the convex hull, which equals the weak closure.

Added hypotheses: DDD and Ξ\XiΞ nonempty in Lemmas 3.15 and 3.16 (no probability measure exists on an empty set). Pinned reading: (68) is posed as one inclusion 0∈DF(u∗)+λ∗ co⁡‾{ux:(x,z)∈M(u∗)}0\in DF(u^*)+\lambda^*\,\overline{\operatorname{co}}\{u_x:(x,z)\in M(u^*)\}0∈DF(u∗)+λ∗co{ux​:(x,z)∈M(u∗)} in L2(D)L^2(D)L2(D), where uxu_xux​ represents h↦[A−1h](x)h\mapsto[A^{-1}h](x)h↦[A−1h](x). The page derives (68) from exactly this inclusion. The closed hull is kept because the page's remark that "co" suffices is not proved in infinite dimension.

Several trivializing formalizations are ruled out. The state operator is tied to the PDE and is never an arbitrary map into C(Dˉ×Ξ)C(\bar D\times\Xi)C(Dˉ×Ξ). The multiplier carries its sign (a nonnegative measure, or λ∗∈K^−\lambda^*\in\hat{\mathcal K}^-λ∗∈K^−) together with complementarity. Optimality is global minimality, not a stationarity condition. All integrands are continuous functions on a compact space against finite measures, so no integral takes a junk value.

A complete development needs elliptic regularity in C(Dˉ)C(\bar D)C(Dˉ) for class-S domains, a Banach-space Lagrange multiplier theorem under a Robinson-type constraint qualification, the Riesz–Markov–Kakutani theorem for C(K)∗C(K)^*C(K)∗ with signed measures (the platform's FamousTheorems.riesz_markov_kakutani covers positive functionals on CcC_cCc​), and barycenters of probability measures on compact convex sets. The last three are reusable beyond this mission. Contributions of proofs for any of them are welcome.

Selected references

  • C. Geiersbach, R. Henrion, Optimality conditions in control problems with random state constraints in probabilistic or almost-sure form, arXiv:2306.03965v2, 2024; Math. Oper. Res., 2025. https://arxiv.org/abs/2306.03965
  • F. Clarke, Optimization and Nonsmooth Analysis, Wiley, 1983. https://doi.org/10.1137/1.9781611971309
  • D. Kinderlehrer, G. Stampacchia, An Introduction to Variational Inequalities and Their Applications, Academic Press, 1980 (SIAM reprint 2000). https://doi.org/10.1137/1.9780898719451
  • R. R. Phelps, Lectures on Choquet's Theorem, 2nd ed., Lecture Notes in Mathematics 1757, Springer, 2001. https://doi.org/10.1007/b76887
  • H. W. Alt, Lineare Funktionalanalysis, Springer, 2012. https://doi.org/10.1007/978-3-662-08386-4
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Operations ResearchOptimizationPartial Differential Equations+1·Captain: mikedeng1

Optimality Conditions in Control Problems with Random State Constraints in Probabilistic or Almost Sure Form III: Absolutely Continuous and Singular Multipliers for Almost Sure State ConstraintsResearch Paper

Motivation

Optimal control of partial differential equations under uncertainty asks for a single deterministic control uuu that performs well when the data of the PDE are random. When a constraint on the state must hold, the modeller has to decide how strictly: with high probability (a probabilistic constraint), for almost every realization (an almost-sure constraint), or for every realization in a support set (a robust constraint). C. Geiersbach and R. Henrion (arXiv:2306.03965v2, Math. Oper. Res. 2025) derive optimality conditions for all three forms on a common model problem. This mission covers §3.1 of that paper, the almost-sure case.

Almost-sure state constraints are the natural model when a bound (a temperature, a stress, a concentration) must never be violated, and they appear throughout risk-averse PDE-constrained optimization (Geiersbach and Wollner, SIAM J. Optim. 2021; Geiersbach and Hintermüller, ESAIM:COCV 2022). Their difficulty is functional-analytic: the constraint lives in LP∞(Ω,C(Dˉ))L^\infty_{\mathbb P}(\Omega,\mathcal C(\bar D))LP∞​(Ω,C(Dˉ)), a space whose dual is not a function space, so Lagrange multipliers are a priori only finitely additive objects.

Setting

Let D⊆RdD\subseteq\mathbb R^dD⊆Rd, d∈{1,2,3}d\in\{1,2,3\}d∈{1,2,3}, be open, bounded and of class S: there are γ∈(0,1)\gamma\in(0,1)γ∈(0,1) and r0>0r_0>0r0​>0 with meas⁡(Br(x)∖D)≥γmeas⁡(Br(x))\operatorname{meas}(B_r(x)\setminus D)\ge\gamma\operatorname{meas}(B_r(x))meas(Br​(x)∖D)≥γmeas(Br​(x)) for all x∈∂Dx\in\partial Dx∈∂D and 0<r<r00<r<r_00<r<r0​. For F∈L2(D)F\in L^2(D)F∈L2(D) the Dirichlet problem −Δy=F-\Delta y=F−Δy=F in DDD, y=0y=0y=0 on ∂D\partial D∂D has a unique weak solution y∈H01(D)∩C(Dˉ)y\in H^1_0(D)\cap\mathcal C(\bar D)y∈H01​(D)∩C(Dˉ); the solution map is a continuous linear operator A−1:L2(D)→C(Dˉ)A^{-1}:L^2(D)\to\mathcal C(\bar D)A−1:L2(D)→C(Dˉ).

Let (Ω,F,P)(\Omega,\mathcal F,\mathbb P)(Ω,F,P) be a probability space and f~∈LP∞(Ω,L2(D))\tilde f\in L^\infty_{\mathbb P}(\Omega,L^2(D))f~​∈LP∞​(Ω,L2(D)) a random source. For a control u∈L2(D)u\in L^2(D)u∈L2(D) the random state y(⋅,ω)y(\cdot,\omega)y(⋅,ω) solves −Δy(⋅,ω)=u+f~(⋅,ω)-\Delta y(\cdot,\omega)=u+\tilde f(\cdot,\omega)−Δy(⋅,ω)=u+f~​(⋅,ω), y(⋅,ω)=0y(\cdot,\omega)=0y(⋅,ω)=0 on ∂D\partial D∂D. With B\mathcal BB the embedding of L2(D)L^2(D)L2(D) into constant elements of LP∞(Ω,L2(D))L^\infty_{\mathbb P}(\Omega,L^2(D))LP∞​(Ω,L2(D)) and [A−1y](ω)=A−1y(⋅,ω)[\mathcal A^{-1}y](\omega)=A^{-1}y(\cdot,\omega)[A−1y](ω)=A−1y(⋅,ω), the control-to-state operator is S(u)=A−1(Bu+f~)\mathcal S(u)=\mathcal A^{-1}(\mathcal Bu+\tilde f)S(u)=A−1(Bu+f~​) and the constraint map is G(u)=S(u)−α\mathcal G(u)=\mathcal S(u)-\boldsymbol\alphaG(u)=S(u)−α, where α\boldsymbol\alphaα is the constant function α∈R\alpha\in\mathbb Rα∈R. The problem is

min⁡u∈L2(D)F(u)s.t.G(u)∈K,(51)\min_{u\in L^2(D)}F(u)\quad\text{s.t.}\quad\mathcal G(u)\in\mathcal K,\qquad(51)u∈L2(D)min​F(u)s.t.G(u)∈K,(51)

with the cone K={y∈LP∞(Ω,C(Dˉ)):y(x,ω)≤0 on Dˉ, P-a.s.}\mathcal K=\{y\in L^\infty_{\mathbb P}(\Omega,\mathcal C(\bar D)):y(x,\omega)\le0\text{ on }\bar D,\ \mathbb P\text{-a.s.}\}K={y∈LP∞​(Ω,C(Dˉ)):y(x,ω)≤0 on Dˉ, P-a.s.} and its polar K−⊆(LP∞(Ω,C(Dˉ)))∗\mathcal K^-\subseteq(L^\infty_{\mathbb P}(\Omega,\mathcal C(\bar D)))^*K−⊆(LP∞​(Ω,C(Dˉ)))∗. The cost FFF is convex and continuously Fréchet differentiable.

For a separable Banach space XXX, a functional v∈(LP∞(Ω,X))∗v\in(L^\infty_{\mathbb P}(\Omega,X))^*v∈(LP∞​(Ω,X))∗ is absolutely continuous if ⟨v,x⟩=∫Ω⟨x∗(ω),x(ω)⟩ dP\langle v,x\rangle=\int_\Omega\langle x^*(\omega),x(\omega)\rangle\,d\mathbb P⟨v,x⟩=∫Ω​⟨x∗(ω),x(ω)⟩dP for a weakly measurable x∗:Ω→X∗x^*:\Omega\to X^*x∗:Ω→X∗ with ∫∥x∗∥ dP<∞\int\|x^*\|\,d\mathbb P<\infty∫∥x∗∥dP<∞ (the set Λ1(X∗)\Lambda_1(X^*)Λ1​(X∗) of such x∗x^*x∗), and singular if it vanishes on every xxx that vanishes on some FnF_nFn​, for a decreasing sequence of events with P(Fn)→0\mathbb P(F_n)\to0P(Fn​)→0 (the set Λ∘(X∗)\Lambda_\circ(X^*)Λ∘​(X∗)).

Formalization targets

Goal: Theorem 3.10

Under the constraint qualification 0∈int⁡{G(L2(D))−K}0\in\operatorname{int}\{\mathcal G(L^2(D))-\mathcal K\}0∈int{G(L2(D))−K}, u∗u^*u∗ solves (51) if and only if there are λ∈Λ1(C(Dˉ)∗)\lambda\in\Lambda_1(\mathcal C(\bar D)^*)λ∈Λ1​(C(Dˉ)∗), λ∘∈Λ∘(C(Dˉ)∗)\lambda^\circ\in\Lambda_\circ(\mathcal C(\bar D)^*)λ∘∈Λ∘​(C(Dˉ)∗) and a state y∗y^*y∗ with

DF(u∗)+E[A−∗λ]+B∗A−∗λ∘=0,Ay∗(⋅,ω)=u∗+f~(⋅,ω),DF(u^*)+\mathbb E[A^{-*}\lambda]+\mathcal B^*\mathcal A^{-*}\lambda^\circ=0,\qquad Ay^*(\cdot,\omega)=u^*+\tilde f(\cdot,\omega),DF(u∗)+E[A−∗λ]+B∗A−∗λ∘=0,Ay∗(⋅,ω)=u∗+f~​(⋅,ω), y∗(⋅,ω)≤α,λ(⋅,ω)≥0,⟨λ(⋅,ω),y∗(⋅,ω)−α⟩=0  P-a.s.,λ∘∈K−,⟨λ∘,y∗−α⟩=0.y^*(\cdot,\omega)\le\alpha,\quad\lambda(\cdot,\omega)\ge0,\quad\langle\lambda(\cdot,\omega),y^*(\cdot,\omega)-\boldsymbol\alpha\rangle=0\ \ \mathbb P\text{-a.s.},\qquad\lambda^\circ\in\mathcal K^-,\quad\langle\lambda^\circ,y^*-\boldsymbol\alpha\rangle=0.y∗(⋅,ω)≤α,λ(⋅,ω)≥0,⟨λ(⋅,ω),y∗(⋅,ω)−α⟩=0  P-a.s.,λ∘∈K−,⟨λ∘,y∗−α⟩=0.

Milestones

  1. Lemma 3.6: the random state exists, is a.s. unique, lies in LP∞(Ω,C(Dˉ))L^\infty_{\mathbb P}(\Omega,\mathcal C(\bar D))LP∞​(Ω,C(Dˉ)), and obeys the bound (52).
  2. Lemma 3.7: the abstract KKT system (53) with a multiplier λ∗∈(LP∞(Ω,C(Dˉ)))∗\lambda^*\in(L^\infty_{\mathbb P}(\Omega,\mathcal C(\bar D)))^*λ∗∈(LP∞​(Ω,C(Dˉ)))∗.
  3. Theorem 3.9 (Ioffe–Levin): every v∗∈(LP∞(Ω,X))∗v^*\in(L^\infty_{\mathbb P}(\Omega,X))^*v∗∈(LP∞​(Ω,X))∗ splits uniquely as va+v∘v^a+v^\circva+v∘ with ∥v∗∥=∥va∥+∥v∘∥\|v^*\|=\|v^a\|+\|v^\circ\|∥v∗∥=∥va∥+∥v∘∥.
  4. The splitting ⟨λ∗,A−1Bh⟩=E[⟨λ,A−1h⟩]+⟨λ∘,A−1Bh⟩\langle\lambda^*,\mathcal A^{-1}\mathcal Bh\rangle=\mathbb E[\langle\lambda,A^{-1}h\rangle]+\langle\lambda^\circ,\mathcal A^{-1}\mathcal Bh\rangle⟨λ∗,A−1Bh⟩=E[⟨λ,A−1h⟩]+⟨λ∘,A−1Bh⟩.
  5. (57): λ∗∈K−\lambda^*\in\mathcal K^-λ∗∈K− passes to both parts.
  6. (59) and pointwise complementarity: λ(ω)≥0\lambda(\omega)\ge0λ(ω)≥0 and ⟨λ(ω),y∗(ω)−α⟩=0\langle\lambda(\omega),y^*(\omega)-\boldsymbol\alpha\rangle=0⟨λ(ω),y∗(ω)−α⟩=0 almost surely.

Significance

The result. Lemma 3.7 gives a multiplier in the dual of L∞L^\inftyL∞, which cannot be evaluated scenario by scenario. Theorem 3.10 shows that, for this problem, the multiplier consists of an honest random variable λ(ω)∈C(Dˉ)∗\lambda(\omega)\in\mathcal C(\bar D)^*λ(ω)∈C(Dˉ)∗ (a random signed measure on Dˉ\bar DDˉ) satisfying sign and complementarity conditions for almost every realization, plus a singular remainder. This is the form needed to write adjoint equations and to design discretizations and algorithms (Proposition 3.12 of the paper). As Remark 3.11 notes, the derivation does not require reflexivity of the state space, unlike earlier work on LP∞(Ω,X)L^\infty_{\mathbb P}(\Omega,X)LP∞​(Ω,X)-constraints.

Formalizing it. The paper's argument is complete, but it rests on two cited results: the regularity theory behind Lemma 1.2/3.6 (Stampacchia-type continuity of weak solutions on class-S domains, Kinderlehrer–Stampacchia) and the Ioffe–Levin decomposition of (LP∞(Ω,X))∗(L^\infty_{\mathbb P}(\Omega,X))^*(LP∞​(Ω,X))∗ (Ioffe–Levin, Appendix 1, Theorem 3, and Levin 1974). Neither is in Mathlib. A formal development produces machine-checked versions of both, of a Robinson-type KKT theorem in Banach spaces, and of the multiplier refinement itself. None of these results has a machine-checked proof as far as the platform's catalog shows.

Difficulty

The obvious route is to apply the Riesz representation pointwise in ω\omegaω. It fails: (LP∞(Ω,C(Dˉ)))∗(L^\infty_{\mathbb P}(\Omega,\mathcal C(\bar D)))^*(LP∞​(Ω,C(Dˉ)))∗ contains purely finitely additive functionals that are not given by any integrand, so λ∗\lambda^*λ∗ has no density in general. The decomposition theorem isolates them, and the proof of Theorem 3.10 must then show that the sign condition λ∗∈K−\lambda^*\in\mathcal K^-λ∗∈K− and the complementarity condition pass to each part separately. The step from E[⟨λ,y⟩]≤0\mathbb E[\langle\lambda,y\rangle]\le0E[⟨λ,y⟩]≤0 for all y∈Ky\in\mathcal Ky∈K to "λ(ω)≥0\lambda(\omega)\ge0λ(ω)≥0 for almost every ω\omegaω, simultaneously for all nonnegative test functions" requires the separability of C(Dˉ)\mathcal C(\bar D)C(Dˉ); a version with a null set depending on the test function is weaker and is not the statement. Lemma 3.6 needs C(Dˉ)\mathcal C(\bar D)C(Dˉ)-regularity of weak solutions, which is where class S and d≤3d\le3d≤3 enter.

Formalization scope

Rd\mathbb R^dRd is EuclideanSpace ℝ (Fin d). L2(D)L^2(D)L2(D) is Lp ℝ 2 (volume.restrict D) and LP∞(Ω,X)L^\infty_{\mathbb P}(\Omega,X)LP∞​(Ω,X) is Lp X ⊤ P; their elements are a.e. classes, so every pointwise statement in ω\omegaω is stated P\mathbb PP-a.s. C(Dˉ)\mathcal C(\bar D)C(Dˉ) is C(closure D, ℝ) with [CompactSpace (closure D)] as an instance argument (implied by boundedness). Weak derivatives use the published HunterPDE.Shared.HasWeakDeriv; a weak solution in H01(D)∩C(Dˉ)H^1_0(D)\cap\mathcal C(\bar D)H01​(D)∩C(Dˉ) is encoded as continuity on Dˉ\bar DDˉ, zero boundary values, L2L^2L2 weak gradient and the weak form. A−1A^{-1}A−1 is a hypothesis: a continuous linear map L2(D)→C(Dˉ)L^2(D)\to\mathcal C(\bar D)L2(D)→C(Dˉ) whose values are weak solutions. "≤0\le0≤0 a.e. in DDD" for a function continuous on Dˉ\bar DDˉ is read as "≤0\le0≤0 on Dˉ\bar DDˉ"; "λ(⋅,ω)≥0\lambda(\cdot,\omega)\ge0λ(⋅,ω)≥0" as positivity of the functional. "Solution of (51)" is a global minimizer. (56a) is stated applied to every direction hhh.

Trivializing formalizations are ruled out: the state operator is tied to the PDE, not an arbitrary bounded operator; the multipliers carry their sign and complementarity conditions; absolutely continuous functionals require a weakly measurable, integrable density; singular functionals are concentrated on a decreasing sequence of events of vanishing probability, not merely "not absolutely continuous"; optimality is global.

Needed infrastructure: Lax–Milgram on H01(D)H^1_0(D)H01​(D) and continuity of weak solutions (Lemma 3.6); a KKT theorem under Robinson's constraint qualification (Lemma 3.7); the Yosida–Hewitt decomposition for finitely additive measures and a weak*-measurable representation of L1(Ω,X)∗L^1(\Omega,X)^*L1(Ω,X)∗ (Theorem 3.9). The decomposition theorem is reusable far beyond this mission; contributions toward any of these are welcome.

Selected references

  • C. Geiersbach, R. Henrion, Optimality conditions in control problems with random state constraints in probabilistic or almost-sure form, arXiv:2306.03965v2, 2024; Math. Oper. Res. 2025. https://arxiv.org/abs/2306.03965
  • A. D. Ioffe, V. L. Levin, Subdifferentials of convex functions, Trudy Moskov. Mat. Obshch. 26, 3–73, 1972 (Appendix 1, Theorem 3).
  • V. L. Levin, The Lebesgue decomposition for functionals on the vector-function space LX∞L^\infty_XLX∞​, Funct. Anal. Appl. 8(4), 314–317, 1974. https://doi.org/10.1007/bf01075488
  • K. Yosida, E. Hewitt, Finitely additive measures, Trans. Amer. Math. Soc. 72, 1952. https://doi.org/10.1090/S0002-9947-1952-0045194-X
  • J. F. Bonnans, A. Shapiro, Perturbation Analysis of Optimization Problems, Springer, 2000. https://doi.org/10.1007/978-1-4612-1394-9
  • C. Geiersbach, W. Wollner, Optimality conditions for convex stochastic optimization problems in Banach spaces with almost sure state constraints, SIAM J. Optim. 31(4), 2455–2480, 2021.
  • C. Geiersbach, M. Hintermüller, Optimality conditions and Moreau–Yosida regularization for almost sure state constraints, ESAIM: COCV 28, Paper No. 80, 2022. https://doi.org/10.1051/cocv/2022070
  • D. Kinderlehrer, G. Stampacchia, An Introduction to Variational Inequalities and Their Applications, Academic Press, 1980 (Chapter II, Appendices B and C). https://doi.org/10.1137/1.9780898719451
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Calculus of VariationsOptimization·Captain: mikedeng1

Nonlinear Quasi-hemivariational Inequalities: Existence and Optimal Control: Existence of Solutions to the Generalized Quasi-Hemivariational InequalityResearch Paper

Motivation

Hemivariational inequalities were introduced by Panagiotopoulos in the 1980s to model mechanical problems whose energy functional is neither convex nor smooth: nonmonotone friction, adhesion, delamination and unilateral contact with nonmonotone multivalued laws. Where a variational inequality expresses the optimality condition of a convex energy, a hemivariational inequality expresses a stationarity condition of a locally Lipschitz energy through Clarke's generalized directional derivative. When in addition the admissible set depends on the unknown state, as in contact problems with a solution-dependent gap or in Nash-type equilibrium problems with coupled constraints, the problem becomes a quasi-hemivariational inequality.

Zeng, Migórski and Khan (SIAM J. Control Optim. 59 (2021)) treat a general form of this problem that contains a multivalued operator TTT, a bifunction φ\varphiφ and a constraint map KKK at once. Their existence theorem for it, Theorem 3.8, is the base of an optimal control result (Section 4) and of an application to a frictional contact problem in elasticity (Section 5). This mission formalizes the existence part, Sections 2 and 3 of the paper.

Setting

Let VVV be a real reflexive Banach space with dual V∗V^*V∗ and pairing ⟨⋅,⋅⟩\langle\cdot,\cdot\rangle⟨⋅,⋅⟩, and let XXX, YYY be real Banach spaces. The data are: a nonempty closed convex set C⊆VC\subseteq VC⊆V; a multivalued constraint map K:C→2CK:C\to2^CK:C→2C; a multivalued operator T:C→2V∗T:C\to2^{V^*}T:C→2V∗; a function φ:V×V→R\varphi:V\times V\to\mathbb Rφ:V×V→R; a locally Lipschitz functional J:X→RJ:X\to\mathbb RJ:X→R; bounded linear operators γ:V→X\gamma:V\to Xγ:V→X and π:V→Y\pi:V\to Yπ:V→Y; a functional f∈Y∗f\in Y^*f∈Y∗; and an auxiliary function h:V→Rh:V\to\mathbb Rh:V→R.

For a locally Lipschitz JJJ, the Clarke generalized directional derivative and the generalized gradient are

J0(u;v)=lim sup⁡λ→0+, w→uJ(w+λv)−J(w)λ,∂J(u)={ξ∈X∗: J0(u;v)≥⟨ξ,v⟩ ∀v∈X}.J^0(u;v)=\limsup_{\lambda\to0^+,\ w\to u}\frac{J(w+\lambda v)-J(w)}{\lambda},\qquad \partial J(u)=\{\xi\in X^*:\ J^0(u;v)\ge\langle\xi,v\rangle\ \forall v\in X\}.J0(u;v)=λ→0+, w→ulimsup​λJ(w+λv)−J(w)​,∂J(u)={ξ∈X∗: J0(u;v)≥⟨ξ,v⟩ ∀v∈X}.

Problem 1.1 asks for u∈Cu\in Cu∈C and u∗∈T(u)u^*\in T(u)u∗∈T(u) such that u∈K(u)u\in K(u)u∈K(u) and

⟨u∗,v−u⟩+φ(v,u)+J0(γu;γ(v−u))≥⟨f,π(v−u)⟩Y∗×Yfor all v∈K(u).\langle u^*,v-u\rangle+\varphi(v,u)+J^0(\gamma u;\gamma(v-u))\ge\langle f,\pi(v-u)\rangle_{Y^*\times Y}\quad\text{for all }v\in K(u).⟨u∗,v−u⟩+φ(v,u)+J0(γu;γ(v−u))≥⟨f,π(v−u)⟩Y∗×Y​for all v∈K(u).

Its solution set is Γ(f)\Gamma(f)Γ(f). Fixing the constraint set gives Problem 3.3: find u∈Cu\in Cu∈C and u∗∈T(u)u^*\in T(u)u∗∈T(u) with the same inequality for all v∈Cv\in Cv∈C; its solution set is SOL(C;T,J,φ,f)\mathrm{SOL}(C;T,J,\varphi,f)SOL(C;T,J,φ,f). The variational selection S:C→2CS:C\to2^CS:C→2C maps w∈Cw\in Cw∈C to the solution set of Problem 3.3 with CCC replaced by K(w)K(w)K(w); its fixed points are exactly the solutions of Problem 1.1.

The hypotheses of the paper (p. 1250) are: TTT has nonempty, compact, convex values and is upper semicontinuous; T(⋅)+γ∗∂J(γ ⋅)T(\cdot)+\gamma^*\partial J(\gamma\,\cdot)T(⋅)+γ∗∂J(γ⋅) is (φ,h)(\varphi,h)(φ,h)-stably pseudomonotone with respect to π∗f\pi^*fπ∗f, where lim sup⁡t→0+h(tu)/t≥0\limsup_{t\to0^+}h(tu)/t\ge0limsupt→0+​h(tu)/t≥0 and hhh is weakly sequentially upper semicontinuous in the limsup sense (3.1); φ\varphiφ is convex and l.s.c. in its first argument, concave and u.s.c. in its second, and vanishes on the diagonal; KKK has nonempty closed convex values and satisfies two Mosco-type conditions (HK); a bounded set C0C_0C0​ meets every K(u)K(u)K(u) and, if CCC is unbounded, a coercivity condition (3.2) holds at each point of C0C_0C0​. Theorem 3.8 adds that γ\gammaγ is compact, hhh is convex, and lim sup⁡nφ(vn,un)≤φ(v,u)\limsup_n\varphi(v_n,u_n)\le\varphi(v,u)limsupn​φ(vn​,un​)≤φ(v,u) whenever vn→vv_n\to vvn​→v strongly and un⇀uu_n\rightharpoonup uun​⇀u weakly (3.19).

Formalization targets

Goal: Theorem 3.8 (ii)

Under all hypotheses of Theorem 3.8,

Γ(f)≠∅,Γ(f) is bounded,Γ(f) is weakly closed in V.\Gamma(f)\neq\emptyset,\qquad \Gamma(f)\ \text{is bounded},\qquad \Gamma(f)\ \text{is weakly closed in }V.Γ(f)=∅,Γ(f) is bounded,Γ(f) is weakly closed in V.

Milestones

  1. Proposition 2.5 (i)–(iii): J0(x;⋅)J^0(x;\cdot)J0(x;⋅) is sublinear, J0(x;v)=max⁡{⟨ξ,v⟩:ξ∈∂J(x)}J^0(x;v)=\max\{\langle\xi,v\rangle:\xi\in\partial J(x)\}J0(x;v)=max{⟨ξ,v⟩:ξ∈∂J(x)}, and (u,v)↦J0(u;v)(u,v)\mapsto J^0(u;v)(u,v)↦J0(u;v) is upper semicontinuous.
  2. Theorem 2.7 (Kluge): a multivalued self-map of a nonempty closed convex subset of a reflexive Banach space, with nonempty closed convex values and a sequentially weakly closed graph, has a fixed point if its domain or its range is bounded.
  3. Theorem 3.4 (i)–(iii): for Problem 3.3, the Minty-type characterization
⟨v∗,v−u⟩+φ(v,u)+⟨ηv,γ(v−u)⟩≥⟨f,π(v−u)⟩+h(v−u)∀v∈C, v∗∈T(v), ηv∈∂J(γv);\langle v^*,v-u\rangle+\varphi(v,u)+\langle\eta_v,\gamma(v-u)\rangle\ge\langle f,\pi(v-u)\rangle+h(v-u)\quad\forall v\in C,\ v^*\in T(v),\ \eta_v\in\partial J(\gamma v);⟨v∗,v−u⟩+φ(v,u)+⟨ηv​,γ(v−u)⟩≥⟨f,π(v−u)⟩+h(v−u)∀v∈C, v∗∈T(v), ηv​∈∂J(γv);

nonemptiness, boundedness and weak closedness of SOL(C;T,J,φ,f)\mathrm{SOL}(C;T,J,\varphi,f)SOL(C;T,J,φ,f); and its convexity when hhh is convex. 4. Theorem 3.8 (i): the same characterization for Problem 1.1, with CCC replaced by K(u)K(u)K(u). 5. Two claims from the proof of Theorem 3.8 (ii): the graph of SSS is sequentially weakly closed, and S(C)=⋃w∈CS(w)S(C)=\bigcup_{w\in C}S(w)S(C)=⋃w∈C​S(w) is bounded.

Significance

Theorem 3.8 is the existence result on which the rest of the paper rests: the optimal control problem of Section 4 minimizes F(f)=inf⁡u∈Γ(f)g(u,f)F(f)=\inf_{u\in\Gamma(f)}g(u,f)F(f)=infu∈Γ(f)​g(u,f) over f∈Y∗f\in Y^*f∈Y∗, and Section 5 casts an approximate static elastic contact model, with a multivalued normal compliance condition and a frictional law with slip-dependent friction coefficient, in the form of Problem 1.1 on a space of displacements. The theorem unifies several existence results for variational, hemivariational and quasi-variational inequalities: for single-valued TTT, J=0J=0J=0, π=id\pi=\mathrm{id}π=id, h=0h=0h=0 and φ(v,u)=ϕ(v)−ϕ(u)\varphi(v,u)=\phi(v)-\phi(u)φ(v,u)=ϕ(v)−ϕ(u), its Corollary 3.9 reduces to an earlier existence result for quasi-variational inequalities (Remark 3.10), and Theorem 3.4 removes the compactness of γ\gammaγ required in earlier work (Remark 3.6).

The results are proved in the paper. None of them, nor Clarke's calculus on a Banach space, nor Kluge's fixed point theorem, has a machine-checked proof to our knowledge. A formalization adds a checked version of a proof that combines a KKM-type fixed point theorem, Minty's trick for pseudomonotone multivalued operators, and a fixed point argument for the variational selection.

Difficulty

The obvious route to Problem 1.1 is to fix www, solve the inequality on K(w)K(w)K(w), and take a fixed point of the solution map. Two steps resist. First, the solution map is multivalued and its values are only weakly closed, so a Schauder- or Kakutani-type theorem in the norm topology does not apply; the fixed point theorem must work with sequentially weakly closed graphs, and the graph closedness of SSS has to be proved by passing to the limit in inequalities in which unu_nun​ converges only weakly while the test points vn∈K(wn)v_n\in K(w_n)vn​∈K(wn​) must converge strongly. That passage uses the compactness of γ\gammaγ, the upper semicontinuity of J0J^0J0, condition (3.19) and the Mosco-type conditions together. Second, in the "there exists u∗∈T(u)u^*\in T(u)u∗∈T(u)" form of the problem the inequality is not stable under weak limits in uuu, which is why the Minty reformulation and the stable pseudomonotonicity with the auxiliary function hhh are needed.

Formalization scope

All spaces are real normed spaces with CompleteSpace; V∗V^*V∗ is V →L[ℝ] ℝ with the operator-norm topology; reflexivity is surjectivity of NormedSpace.inclusionInDoubleDual ℝ V. No inner product and no finite dimension is assumed. Multivalued maps are total functions V → Set _, constrained on CCC only. Weak convergence xn⇀xx_n\rightharpoonup xxn​⇀x means ℓ(xn)→ℓ(x)\ell(x_n)\to\ell(x)ℓ(xn​)→ℓ(x) for every ℓ∈V∗\ell\in V^*ℓ∈V∗; "weakly closed" is sequential weak closedness, which for the bounded sets Γ(f)\Gamma(f)Γ(f) and SOL\mathrm{SOL}SOL in a reflexive space agrees with weak closedness. Adjoints are composition: ⟨γ∗η,w⟩=η(γw)\langle\gamma^*\eta,w\rangle=\eta(\gamma w)⟨γ∗η,w⟩=η(γw), ⟨π∗f,w⟩=f(πw)\langle\pi^*f,w\rangle=f(\pi w)⟨π∗f,w⟩=f(πw). J0J^0J0 is a real Filter.limsup and is used only under LocallyLipschitz J. Every lim sup⁡\limsuplimsup, infimum and limit in the hypotheses (lim sup⁡t→0+h(tu)/t≥0\limsup_{t\to0^+}h(tu)/t\ge0limsupt→0+​h(tu)/t≥0, (3.1), (3.2), (3.19)) is written with explicit ε\varepsilonε–NNN quantifiers, so no default value of a real lim sup⁡\limsuplimsup or inf⁡\infinf can make a hypothesis vacuous.

Four corrections to the printed hypotheses are built in and stated in each item's note: the pairing in (3.2) is ⟨ηu,γ(u−v0)⟩\langle\eta_u,\gamma(u-v_0)\rangle⟨ηu​,γ(u−v0​)⟩ (the page's ⟨ηu,u−v0⟩\langle\eta_u,u-v_0\rangle⟨ηu​,u−v0​⟩ does not typecheck); T(u)T(u)T(u) is nonempty for u∈Cu\in Cu∈C; the condition (3.2) assumed in Theorem 3.4 refers to a bounded set C0C_0C0​ that meets CCC; and for Theorem 3.8 (ii) and the boundedness of S(C)S(C)S(C), (3.2) in (HC0) holds uniformly in v0∈C0v_0\in C_0v0​∈C0​ (one RRR for each MMM), which is what the proof on pp. 1260–1261 uses. With (3.2) only at each fixed v0∈C0v_0\in C_0v0​∈C0​, as printed, Γ(f)\Gamma(f)Γ(f) can be unbounded; the counterexample is in the note of Theorem 3.8 (ii). Theorem 3.8 (i) and the graph-closedness of SSS keep (HC0) as printed. A formalization in which TTT may have empty values, C0C_0C0​ may be empty or disjoint from CCC, VVV is a Hilbert or finite-dimensional space, a real lim sup⁡\limsuplimsup default value makes the conditions on hhh or (3.19) vacuous, or "bounded" or "weakly closed" is dropped from the conclusion, would be a different and weaker theorem.

The development needs Clarke's calculus on a Banach space (Proposition 2.5, which relies on the Hahn–Banach theorem), Eberlein–Šmulian or Kakutani's theorem on weak compactness of bounded closed convex sets in reflexive spaces, Mazur's lemma, a KKM-type fixed point theorem in Hausdorff topological vector spaces, and Kluge's fixed point theorem. These pieces are reusable beyond this mission: Clarke's calculus for every nonsmooth optimization statement on Banach spaces, and the fixed point theorems for variational and quasi-variational inequalities in general. Contributions of any of them, of alternative proofs, and of proofs of the milestones in any order are welcome.

Selected references

  • S. Zeng, S. Migórski, A. A. Khan, Nonlinear quasi-hemivariational inequalities: existence and optimal control, SIAM J. Control Optim. 59(2) (2021) 1246–1274. https://doi.org/10.1137/19M1282210
  • F. H. Clarke, Optimization and Nonsmooth Analysis, Wiley, 1983; reprinted SIAM Classics in Applied Mathematics 5, 1990. https://doi.org/10.1137/1.9781611971309
  • R. Kluge, Nichtlineare Variationsungleichungen und Extremalaufgaben, VEB Deutscher Verlag der Wissenschaften, Berlin, 1979.
  • S. Migórski, A. Ochal, M. Sofonea, Nonlinear Inclusions and Hemivariational Inequalities, Springer, 2013. https://doi.org/10.1007/978-1-4614-4232-5
  • P. D. Panagiotopoulos, Hemivariational Inequalities: Applications in Mechanics and Engineering, Springer, 1993. https://doi.org/10.1007/978-3-642-51677-1
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Numerical AnalysisOptimization·Captain: mikedeng1

A Forward-Backward Splitting Method for Monotone Inclusions Without Cocoercivity 3: With Linesearch and Locally Lipschitz B the Method Converges to a Zero in Finite DimensionsResearch Paper

Motivation

Many problems in optimization, variational inequalities and saddle-point computation can be written as a monotone inclusion: find xxx with 0∈A(x)+B(x)0 \in A(x) + B(x)0∈A(x)+B(x), where AAA is a set-valued maximally monotone operator (a subdifferential, a normal cone) and BBB is single-valued (a gradient, a skew saddle operator). Splitting methods treat AAA only through its resolvent and BBB only through forward evaluations. The classical forward-backward method needs BBB to be cocoercive, which rules out saddle-point operators; Tseng's forward-backward-forward method removes this but needs two evaluations of BBB per step.

Malitsky and Tam (arXiv:1808.04162, SIAM J. Optim. 30(2), 2020) introduced the forward-reflected-backward method, which needs only monotonicity and Lipschitz continuity of BBB and one new evaluation of BBB per iteration. Its step size in Section 2 depends on a global Lipschitz constant LLL of BBB. Such a constant is often unknown, expensive to estimate, overly conservative, or nonexistent when BBB is only locally Lipschitz. Section 3 of the paper replaces the fixed step by a linesearch (backtracking) and proves convergence for locally Lipschitz BBB in finite dimensions. This mission formalizes that result.

Setting

Let HHH be a finite-dimensional real inner product space. An operator A:H⇉HA : H \rightrightarrows HA:H⇉H is monotone if ⟨x−y,u−v⟩≥0\langle x - y, u - v\rangle \ge 0⟨x−y,u−v⟩≥0 whenever u∈A(x)u \in A(x)u∈A(x), v∈A(y)v \in A(y)v∈A(y), and maximally monotone if moreover its graph is not properly contained in the graph of another monotone operator. For t>0t > 0t>0 the resolvent JtA=(I+tA)−1J_{tA} = (I + tA)^{-1}JtA​=(I+tA)−1 is the map with t−1(w−JtAw)∈A(JtAw)t^{-1}(w - J_{tA}w) \in A(J_{tA}w)t−1(w−JtA​w)∈A(JtA​w) for every www. A map B:H→HB : H \to HB:H→H is monotone if ⟨x−y,B(x)−B(y)⟩≥0\langle x - y, B(x) - B(y)\rangle \ge 0⟨x−y,B(x)−B(y)⟩≥0, and locally Lipschitz if every point has a neighbourhood on which BBB is Lipschitz. The zero set is (A+B)−1(0)={x:−B(x)∈A(x)}(A+B)^{-1}(0) = \{x : -B(x) \in A(x)\}(A+B)−1(0)={x:−B(x)∈A(x)}.

Fix δ∈(0,1)\delta \in (0,1)δ∈(0,1) and σ∈(0,1)\sigma \in (0,1)σ∈(0,1). Given xkx_kxk​, xk−1x_{k-1}xk−1​ and the previous step λk−1\lambda_{k-1}λk−1​, the trial point at step ttt is

xk+1(t)=JtA(xk−tB(xk)−λk−1(B(xk)−B(xk−1))).x_{k+1}(t) = J_{tA}\big(x_k - tB(x_k) - \lambda_{k-1}(B(x_k) - B(x_{k-1}))\big).xk+1​(t)=JtA​(xk​−tB(xk​)−λk−1​(B(xk​)−B(xk−1​))).

Algorithm 1 starts from arbitrary x0,x−1∈Hx_0, x_{-1} \in Hx0​,x−1​∈H and λ−1>0\lambda_{-1} > 0λ−1​>0. In each iteration it chooses ρ∈{1,σ−1}\rho \in \{1, \sigma^{-1}\}ρ∈{1,σ−1}, sets λk=ρλk−1σi\lambda_k = \rho\lambda_{k-1}\sigma^iλk​=ρλk−1​σi with iii the smallest nonnegative integer for which

λk∥B(xk+1)−B(xk)∥≤δ2∥xk+1−xk∥,xk+1=xk+1(λk).(30)\lambda_k \|B(x_{k+1}) - B(x_k)\| \le \frac{\delta}{2}\|x_{k+1} - x_k\|, \qquad x_{k+1} = x_{k+1}(\lambda_k). \tag{30}λk​∥B(xk+1​)−B(xk​)∥≤2δ​∥xk+1​−xk​∥,xk+1​=xk+1​(λk​).(30)

The choice of ρ\rhoρ may change from one iteration to the next; ρ=σ−1\rho = \sigma^{-1}ρ=σ−1 allows the step to grow.

Formalization targets

Goal: Theorem 3.4

If AAA is maximally monotone, BBB is monotone and locally Lipschitz, and (A+B)−1(0)≠∅(A+B)^{-1}(0) \ne \emptyset(A+B)−1(0)=∅, then every sequence generated by Algorithm 1 satisfies

∃ xˉ∈(A+B)−1(0):xk→xˉ.\exists\, \bar x \in (A+B)^{-1}(0): \qquad x_k \to \bar x .∃xˉ∈(A+B)−1(0):xk​→xˉ.

The statement fixes no constant: it holds for every δ,σ∈(0,1)\delta, \sigma \in (0,1)δ,σ∈(0,1), every λ−1>0\lambda_{-1} > 0λ−1​>0, every initial pair and every sequence of choices of ρ\rhoρ.

Milestones

  1. Lemma 3.2 (any real Hilbert space, BBB only locally Lipschitz): at any iteration state, some iii satisfies (30), so the linesearch terminates.
  2. Lemma 3.3: for a zero xxx there is ε>0\varepsilon > 0ε>0 with
∥xk+1−x∥2+2λk⟨B(xk+1)−B(xk),x−xk+1⟩+(12+ε)∥xk+1−xk∥2≤∥xk−x∥2+2λk−1⟨B(xk)−B(xk−1),x−xk⟩+12∥xk−xk−1∥2,\|x_{k+1}-x\|^2+2\lambda_k\langle B(x_{k+1})-B(x_k),x-x_{k+1}\rangle+\big(\tfrac12+\varepsilon\big)\|x_{k+1}-x_k\|^2 \le \|x_k-x\|^2+2\lambda_{k-1}\langle B(x_k)-B(x_{k-1}),x-x_k\rangle+\tfrac12\|x_k-x_{k-1}\|^2,∥xk+1​−x∥2+2λk​⟨B(xk+1​)−B(xk​),x−xk+1​⟩+(21​+ε)∥xk+1​−xk​∥2≤∥xk​−x∥2+2λk−1​⟨B(xk​)−B(xk−1​),x−xk​⟩+21​∥xk​−xk−1​∥2,

stated for k≥1k \ge 1k≥1 (see Formalization scope). 3. The iterates are bounded and ∥xk−xk+1∥→0\|x_k - x_{k+1}\| \to 0∥xk​−xk+1​∥→0. 4. (33): there is L>0L > 0L>0 with ∥B(xk+1)−B(xk)∥≤L∥xk+1−xk∥\|B(x_{k+1}) - B(x_k)\| \le L\|x_{k+1} - x_k\|∥B(xk+1​)−B(xk​)∥≤L∥xk+1​−xk​∥ for all kkk. 5. The step sizes (λk)(\lambda_k)(λk​) are bounded away from zero.

Significance

The theorem makes the forward-reflected-backward method usable without any knowledge of a Lipschitz constant, and extends it to operators that are only locally Lipschitz, such as gradients of C1C^1C1 functions without globally Lipschitz gradient or saddle operators of smooth non-quadratic convex-concave functions. The linesearch costs one resolvent and one evaluation of BBB per trial, and the adaptive factor ρ=σ−1\rho = \sigma^{-1}ρ=σ−1 lets the steps recover after a conservative phase. The same template (an energy inequality where the linesearch test stands in for the Lipschitz bound, followed by a lower bound on the step sizes) recurs in adaptive and backtracking variants of many first-order methods.

The result is proved in the paper; to our knowledge it has no machine-checked proof. The mission produces a formal account of Algorithm 1 including the minimality of the backtracking index, which is where informal accounts of linesearch methods tend to be imprecise. It also records one correction: Lemma 3.3 as printed asserts (32) for all k∈Nk \in \mathbb Nk∈N, but at k=0k = 0k=0 the bound concerns initial data that Algorithm 1 never tests, and it fails there. Theorem 3.4 is unaffected.

Difficulty

Two steps do not transfer directly from the constant-step analysis. First, termination of the linesearch requires the limit behaviour of resolvents as the step tends to zero (JtA(y)→Pdom A‾(y)J_{tA}(y) \to P_{\overline{\mathrm{dom}\,A}}(y)JtA​(y)→PdomA​(y), Bauschke–Combettes, Theorem 23.47), combined with continuity of BBB at the current point; local Lipschitz continuity enters only here and in the last step. Second, the step sizes must be bounded below. The obvious argument combines the accepted test (30) with the Lipschitz bound (33) along the iterates, but (33) concerns accepted points, while a rejected trial step concerns a trial point that is not an iterate. One must show that the rejected trial points also stay in a fixed bounded set, on which BBB is Lipschitz. Finite dimensionality is used exactly to pass from local Lipschitz continuity to Lipschitz continuity on bounded sets.

Formalization scope

HHH is a type with [NormedAddCommGroup H] [InnerProductSpace ℝ H] [FiniteDimensional ℝ H]; it is never specialised to EuclideanSpace ℝ (Fin n). The operator vocabulary (monotone, maximally monotone, resolvent) is the published module ThreeOpSplitting.Accel.MonotoneOperators; local Lipschitz continuity is Mathlib's LocallyLipschitz. Conventions committed to:

  • Resolvent as hypothesis. The resolvent is a family J : ℝ → H → H with IsResolventFamily A J; for maximally monotone AAA it exists (Minty) and is unique on t>0t > 0t>0. The goal keeps maximal monotonicity of AAA as well.
  • Index shift. Lean's x j is xj−1x_{j-1}xj−1​ and lam j is λj−1\lambda_{j-1}λj−1​, so lam 0 =λ−1=\lambda_{-1}=λ−1​. Algorithm 1's initialization also names a λ0\lambda_0λ0​ that the iteration never uses; it is not a parameter.
  • Run predicate. IsLinesearchRun J B δ σ lam x requires at every iteration some ρ∈{1,σ−1}\rho \in \{1, \sigma^{-1}\}ρ∈{1,σ−1} and an index iii such that λk=ρλk−1σi\lambda_k = \rho\lambda_{k-1}\sigma^iλk​=ρλk−1​σi, xk+1x_{k+1}xk+1​ is the trial point at λk\lambda_kλk​, (30) holds, and (30) fails at every smaller index. Every sequence of ρ\rhoρ choices is admitted.
  • Mode of convergence. Norm convergence, Filter.Tendsto x atTop (nhds xs).
  • Lemma 3.3 for k≥1k \ge 1k≥1. A disclosed correction of the printed "for all k∈Nk \in \mathbb Nk∈N".
  • Hypothesis relaxations in milestones. Lemma 3.3 uses only monotonicity of AAA and no completeness; the boundedness milestone drops finite dimensionality. Both are stronger than the page.

Trivializing encodings are ruled out: the resolvent is tied to AAA by IsResolventFamily rather than left free; the minimality clause prevents arbitrarily small accepted steps; ρ\rhoρ is not fixed; convergence is in norm, not weak; and a global Lipschitz hypothesis on BBB, which would reduce the goal to mission 1 of this series in finite dimension, is not assumed. The hypotheses are satisfiable (a sanity file checks A≡{0}A \equiv \{0\}A≡{0}, J=idJ = \mathrm{id}J=id, B=0B = 0B=0).

A complete development needs: nonexpansiveness and continuity in the step of resolvents of maximally monotone operators, including the small-step limit to the projection onto dom A‾\overline{\mathrm{dom}\,A}domA; Lipschitz continuity on compact sets of locally Lipschitz maps; the telescoping argument of Theorem 2.5; and a finite-dimensional closedness argument for the graph of A+BA + BA+B. The resolvent facts are reusable well beyond this mission. Proofs of individual milestones, and of the resolvent lemmas as separate items, are welcome.

Selected references

  • Y. Malitsky, M. K. Tam, A Forward-Backward Splitting Method for Monotone Inclusions Without Cocoercivity, SIAM J. Optim. 30(2):1451–1472, 2020. arXiv:1808.04162v4, doi:10.1137/18M1207260
  • H. H. Bauschke, P. L. Combettes, Convex Analysis and Monotone Operator Theory in Hilbert Spaces, 2nd ed., Springer, 2017. doi:10.1007/978-3-319-48311-5
  • P. Tseng, A modified forward-backward splitting method for maximal monotone mappings, SIAM J. Control Optim. 38(2):431–446, 2000. doi:10.1137/S0363012998338806
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Numerical AnalysisOptimization·Captain: mikedeng1

Projected Reflected Gradient Methods for Monotone Variational Inequalities 3: The Adaptive-Step Method Converges Weakly to a Solution Without Knowing the Lipschitz ConstantResearch Paper

Motivation

A variational inequality asks for a point of a convex set at which a vector field points "inward" against every feasible direction. It covers constrained convex minimization (with F=∇fF = \nabla fF=∇f), saddle-point problems, Nash equilibria of convex games and complementarity problems, which is why projection methods for it are a standard topic in optimization and numerical analysis.

The classical methods for a monotone, LLL-Lipschitz field (Korpelevich's extragradient method, Tseng's forward–backward–forward method, the subgradient extragradient method of Censor, Gibali and Reich) use a constant step λ<1/L\lambda < 1/Lλ<1/L or a backtracking search for one. Yu. Malitsky's paper (arXiv:1502.04968v1; SIAM J. Optim. 25(1), 2015, doi:10.1137/14097238X) introduces the projected reflected gradient method, which needs one projection and one evaluation of FFF per iteration. Its constant-step version requires λ<(2−1)/L\lambda < (\sqrt2 - 1)/Lλ<(2​−1)/L, and so requires knowing LLL, which is rarely available in practice (§4, p. 8). Section 4 removes that requirement: Algorithm 4.2 chooses its step from local information only and corrects it when a computable test fails. This mission formalizes the paper's convergence theorem for that algorithm, Theorem 4.4.

Setting

Let HHH be a real Hilbert space with inner product ⟨⋅,⋅⟩\langle\cdot,\cdot\rangle⟨⋅,⋅⟩, C⊆HC \subseteq HC⊆H nonempty, closed and convex, and F:H→HF : H \to HF:H→H. Write PCP_CPC​ for the metric projection onto CCC. The variational inequality (1.1) asks for x∗∈Cx^* \in Cx∗∈C with

⟨F(x∗),x−x∗⟩≥0for all x∈C,\langle F(x^*), x - x^*\rangle \ge 0 \quad\text{for all } x \in C,⟨F(x∗),x−x∗⟩≥0for all x∈C,

and SSS denotes its solution set. The standing conditions (p. 1) are (C1) S≠∅S \ne \emptysetS=∅; (C2) FFF is monotone, ⟨F(x)−F(y),x−y⟩≥0\langle F(x) - F(y), x - y\rangle \ge 0⟨F(x)−F(y),x−y⟩≥0; (C3) FFF is LLL-Lipschitz, ∥F(x)−F(y)∥≤L∥x−y∥\|F(x) - F(y)\| \le L\|x - y\|∥F(x)−F(y)∥≤L∥x−y∥, with L>0L > 0L>0.

Algorithm 4.2 (pp. 8–9) has parameters α∈(0,2−1)\alpha \in (0, \sqrt2 - 1)α∈(0,2​−1), λ−1>0\lambda_{-1} > 0λ−1​>0 and a cap λˉ>0\bar\lambda > 0λˉ>0, and adopts the convention 0/0=+∞0/0 = +\infty0/0=+∞. It starts from x0∈Cx_0 \in Cx0​∈C with y0=PC(x0−λ−1F(x0))y_0 = P_C(x_0 - \lambda_{-1}F(x_0))y0​=PC​(x0​−λ−1​F(x0​)), λ0=min⁡{α∥x0−y0∥/∥F(x0)−F(y0)∥,λˉ}\lambda_0 = \min\{\alpha\|x_0 - y_0\|/\|F(x_0) - F(y_0)\|, \bar\lambda\}λ0​=min{α∥x0​−y0​∥/∥F(x0​)−F(y0​)∥,λˉ}, τ0=1\tau_0 = 1τ0​=1 and x1=PC(x0−λ0F(y0))x_1 = P_C(x_0 - \lambda_0F(y_0))x1​=PC​(x0​−λ0​F(y0​)). For n≥1n \ge 1n≥1 it uses the step rule

λ(y,τ)=min⁡{α∥y−yn−1∥∥F(y)−F(yn−1)∥, 1+τn−1τλn−1, λˉ},(4.1)\lambda(y,\tau) = \min\Big\{\frac{\alpha\|y - y_{n-1}\|}{\|F(y) - F(y_{n-1})\|},\ \frac{1+\tau_{n-1}}{\tau}\lambda_{n-1},\ \bar\lambda\Big\}, \qquad (4.1)λ(y,τ)=min{∥F(y)−F(yn−1​)∥α∥y−yn−1​∥​, τ1+τn−1​​λn−1​, λˉ},(4.1)

forms the trial values yn=2xn−xn−1y_n = 2x_n - x_{n-1}yn​=2xn​−xn−1​, λn=λ(yn,1)\lambda_n = \lambda(y_n, 1)λn​=λ(yn​,1), xn+1=PC(xn−λnF(yn))x_{n+1} = P_C(x_n - \lambda_nF(y_n))xn+1​=PC​(xn​−λn​F(yn​)), and evaluates a test quantity tnt_ntn​ built from these. If tn≤0t_n \le 0tn​≤0 the trial is accepted. Otherwise, in step (4.i) (λn≥λn−1\lambda_n \ge \lambda_{n-1}λn​≥λn−1​) the step is replaced by some λn′∈[λn−1,λn]\lambda'_n \in [\lambda_{n-1}, \lambda_n]λn′​∈[λn−1​,λn​] satisfying (4.2), and in step (4.ii) (λn<λn−1\lambda_n < \lambda_{n-1}λn​<λn−1​) the reflection is replaced by yn′=xn+τn′(xn−xn−1)y'_n = x_n + \tau'_n(x_n - x_{n-1})yn′​=xn​+τn′​(xn​−xn−1​) for some τn′∈(0,1]\tau'_n \in (0,1]τn′​∈(0,1] satisfying (4.3), with a step λn′\lambda'_nλn′​ satisfying (4.4); xn+1x_{n+1}xn+1​ is then recomputed. The values yn,λn,τny_n, \lambda_n, \tau_nyn​,λn​,τn​ kept after iteration nnn are the corrected ones. A sequence produced this way is a run of Algorithm 4.2. The Lipschitz constant LLL appears nowhere in the algorithm.

Formalization targets

Goal: Theorem 4.4 (p. 12)

Under (C1)–(C3), for every run of Algorithm 4.2 there is x∗∈Sx^* \in Sx∗∈S with

xn⇀x∗andyn⇀x∗,x_n \rightharpoonup x^* \qquad\text{and}\qquad y_n \rightharpoonup x^*,xn​⇀x∗andyn​⇀x∗,

where ⇀\rightharpoonup⇀ is weak convergence in HHH.

Milestones

In the order the proof uses them:

  1. Lemma 4.1 (p. 9): step (4.i) is well-defined.
  2. Lemma 4.2 (p. 9): step (4.ii) is well-defined.
  3. The bound λ(y,τ)≥α/L\lambda(y,\tau) \ge \alpha/Lλ(y,τ)≥α/L from the proof of Lemma 4.2 (p. 9), given λn−1≥α/L\lambda_{n-1} \ge \alpha/Lλn−1​≥α/L and λˉ≥α/L\bar\lambda \ge \alpha/Lλˉ≥α/L.
  4. Along every run, 0<λn≤λˉ0 < \lambda_n \le \bar\lambda0<λn​≤λˉ and τn∈(0,1]\tau_n \in (0,1]τn​∈(0,1] (p. 12).
  5. Lemma 2.4 (p. 3): PM(xˉ+λ(x−xˉ))=xˉP_M(\bar x + \lambda(x - \bar x)) = \bar xPM​(xˉ+λ(x−xˉ))=xˉ for xˉ=PMx\bar x = P_Mxxˉ=PM​x and λ>0\lambda > 0λ>0.
  6. Lemma 4.3, the energy inequality (4.5) for z∈Sz \in Sz∈S (p. 10).
  7. The bound τnλn≤(1+τn−1)λn−1\tau_n\lambda_n \le (1 + \tau_{n-1})\lambda_{n-1}τn​λn​≤(1+τn−1​)λn−1​ and the decrease (4.10) (p. 12).
  8. Boundedness of (xn)(x_n)(xn​) and ∥xn+1−yn∥→0\|x_{n+1} - y_n\| \to 0∥xn+1​−yn​∥→0, ∥xn+1−xn∥→0\|x_{n+1} - x_n\| \to 0∥xn+1​−xn​∥→0 (p. 12).

The supporting lemmas 2.2 (Minty), 2.3 (Opial) and 2.7 are included as plain items, together with a statement that runs exist from every x0∈Cx_0 \in Cx0​∈C.

Significance

The result shows that the projected reflected gradient method keeps its weak convergence guarantee when the step is chosen adaptively, without knowledge of LLL, at a cost of at most two projections per iteration (one in most iterations, per the experiments of §5). Adaptive step rules of this kind, based on the local ratio ∥y−y′∥/∥F(y)−F(y′)∥\|y - y'\|/\|F(y) - F(y')\|∥y−y′∥/∥F(y)−F(y′)∥, recur in later work on reflected and golden-ratio methods for variational inequalities (e.g. Malitsky 2020, arXiv:1803.08832), so a formal treatment of the run predicate and its energy inequality is reusable beyond this paper.

The theorem is proved in the paper; it has no machine-checked proof that this mission knows of. The work here is to formalize the definitions of Algorithm 4.2, its well-definedness, the energy inequality and the closing weak-limit argument in a general Hilbert space. The proof as printed has a gap, described under Difficulty; a formal proof would either close it or show that the statement needs an extra hypothesis.

Difficulty

Lemma 4.3 is the bookkeeping core. It has five cases depending on how λn\lambda_nλn​ compares with λn−1\lambda_{n-1}λn−1​ and on the sign of a norm expression. In the case where the reflection is changed, the previous iterate must be reinterpreted as the projection of a point on a segment (via Lemma 2.4) before the estimate of the constant-step method applies.

The closing argument needs the step sizes to stay away from zero, so that the limit can be taken in the optimality inequality for the iterates. The paper asserts that α/L\alpha/Lα/L is a lower bound of (λn)(\lambda_n)(λn​), "from Lemma 4.2" (p. 12). The proof of Lemma 4.2 shows only that the step rule λ(y,τ)\lambda(y,\tau)λ(y,τ) is at least α/L\alpha/Lα/L, and that only under λˉ≥α/L\bar\lambda \ge \alpha/Lλˉ≥α/L. In step (4.ii) the algorithm allows any τn′∈(0,1]\tau'_n \in (0,1]τn′​∈(0,1] satisfying (4.3) and any λn′≥τn′λn−1\lambda'_n \ge \tau'_n\lambda_{n-1}λn′​≥τn′​λn−1​, so an admissible run can take λn\lambda_nλn​ arbitrarily small at such steps. The step regrows by the factor 1+τn−11 + \tau_{n-1}1+τn−1​ at later steps, but the printed proof does not control this. The obvious first attempt, citing a uniform lower bound λn≥α/L\lambda_n \ge \alpha/Lλn​≥α/L, does not work as stated.

Formalization scope

All objects live in one definitions item. HHH is a general real Hilbert space, never Rn\mathbb R^nRn. The projection PCP_CPC​ is a nearest point chosen by choice, with a junk value when none exists. Every theorem that uses it assumes CCC closed and convex together with a nonemptiness source, so the junk branch is never reached. Weak convergence is ⟨xn,v⟩→⟨x∗,v⟩\langle x_n, v\rangle \to \langle x^*, v\rangle⟨xn​,v⟩→⟨x∗,v⟩ for all vvv. (C3) uses a real constant L>0L > 0L>0. The convention 0/0=+∞0/0 = +\infty0/0=+∞ is encoded by omitting the ratio term from the minimum when its denominator is zero, never by Lean's x/0=0x/0 = 0x/0=0.

A run is a relation: the corrections λn′\lambda'_nλn′​, τn′\tau'_nτn′​ range over all admissible values, and nothing selects the largest. The stopping rule of step 3 is not encoded. A run whose residual vanishes continues as a constant sequence through the branch tn≤0t_n \le 0tn​≤0. Indices n−1n - 1n−1 are used only for n≥1n \ge 1n≥1, and λ−1\lambda_{-1}λ−1​ is a separate parameter.

The goal assumes exactly (C1)–(C3), α∈(0,2−1)\alpha \in (0, \sqrt2 - 1)α∈(0,2​−1), λ−1>0\lambda_{-1} > 0λ−1​>0 and λˉ>0\bar\lambda > 0λˉ>0. It assumes neither λˉ≥α/L\bar\lambda \ge \alpha/Lλˉ≥α/L nor any lower bound on (λn)(\lambda_n)(λn​). Adding such a bound would assume the unproved step of the paper's argument. The milestone on λ(y,τ)≥α/L\lambda(y,\tau) \ge \alpha/Lλ(y,τ)≥α/L carries λn−1≥α/L\lambda_{n-1} \ge \alpha/Lλn−1​≥α/L and λˉ≥α/L\bar\lambda \ge \alpha/Lλˉ≥α/L as explicit, disclosed hypotheses. Lemma 4.3 and (4.10) are stated without (C1) and (C3), which their proofs do not use. A formalization that concluded norm convergence, specialized HHH to finite dimension, or fixed one particular choice of corrections would be a different theorem.

The development needs the existence and characterization of the metric projection onto a closed convex set, Minty's lemma, Opial's inequality and weak sequential compactness of bounded sets in Hilbert space. These pieces are reusable for other projection methods. Contributions toward any milestone are welcome, as is a resolution of the lower-bound question for (λn)(\lambda_n)(λn​).

Selected references

  • Yu. Malitsky, Projected Reflected Gradient Methods for Monotone Variational Inequalities, SIAM J. Optim. 25(1) (2015); read as arXiv:1502.04968v1. https://arxiv.org/abs/1502.04968v1, https://doi.org/10.1137/14097238X
  • G. M. Korpelevich, The extragradient method for finding saddle points and other problems, Ekonomika i Matematicheskie Metody 12 (1976), 747–756.
  • P. Tseng, A modified forward-backward splitting method for maximal monotone mappings, SIAM J. Control Optim. 38(2) (2000), 431–446. https://doi.org/10.1137/S0363012998338806
  • Y. Censor, A. Gibali, S. Reich, The subgradient extragradient method for solving variational inequalities in Hilbert space, J. Optim. Theory Appl. 148 (2011), 318–335. https://doi.org/10.1007/s10957-010-9757-3
  • Yu. Malitsky, Golden ratio algorithms for variational inequalities, Math. Program. 184 (2020), 383–410. https://arxiv.org/abs/1803.08832
  • Z. Opial, Weak convergence of the sequence of successive approximations for nonexpansive mappings, Bull. Amer. Math. Soc. 73 (1967), 591–597. https://doi.org/10.1090/S0002-9904-1967-11761-0
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Harmonic Analysis·Captain: mikedeng1

Isotropic Gaussian Random Fields on the Sphere: Regularity, Fast Simulation and Stochastic Partial Differential Equations I: u ∈ V^η(−1,1) iff Σ u_ℓ²(2ℓ+1)(1+ℓ^{2η}) < ∞Research Paper

Motivation

A centered isotropic Gaussian random field TTT on the unit sphere S2\mathbb S^2S2 is determined by its angular power spectrum (Aℓ)ℓ≥0(A_\ell)_{\ell \ge 0}(Aℓ​)ℓ≥0​: its covariance is

E(T(x)T(y))=∑ℓ=0∞Aℓ 2ℓ+14π Pℓ(⟨x,y⟩)=kI(⟨x,y⟩),\mathbb E\big(T(x)T(y)\big) = \sum_{\ell=0}^\infty A_\ell\,\frac{2\ell+1}{4\pi}\,P_\ell(\langle x,y\rangle) = k_I(\langle x, y\rangle),E(T(x)T(y))=ℓ=0∑∞​Aℓ​4π2ℓ+1​Pℓ​(⟨x,y⟩)=kI​(⟨x,y⟩),

with PℓP_\ellPℓ​ the Legendre polynomials. Such fields model the cosmic microwave background and other data on the sphere (Marinucci and Peccati, 2011). In applications one often prescribes the kernel kIk_IkI​ rather than the spectrum, while simulation and error analysis (the Karhunen–Loève truncation, sample regularity, approximation of stochastic PDEs on the sphere) are governed by the decay of AℓA_\ellAℓ​. Section 3 of Lang and Schwab (2015) connects the two: the regularity of kIk_IkI​ on [−1,1][-1,1][−1,1], measured in weighted Sobolev spaces, is equivalent to weighted square summability of (Aℓ)(A_\ell)(Aℓ​). The authors call this result, Theorem 3.1, their main result.

This mission is the first of four from the same paper; the others treat sample Hölder regularity, Karhunen–Loève truncation rates and a stochastic heat equation.

Setting

Functions are real functions on the open interval (−1,1)(-1,1)(−1,1).

  • The Legendre polynomials are Pℓ(μ)=2−ℓ1ℓ!∂ℓ∂μℓ(μ2−1)ℓP_\ell(\mu) = 2^{-\ell}\frac{1}{\ell!}\frac{\partial^\ell}{\partial\mu^\ell}(\mu^2-1)^\ellPℓ​(μ)=2−ℓℓ!1​∂μℓ∂ℓ​(μ2−1)ℓ, ℓ∈N0\ell \in \mathbb N_0ℓ∈N0​.
  • The Fourier–Legendre coefficients of u∈L2(−1,1)u \in L^2(-1,1)u∈L2(−1,1) are uℓ=∫−11u(x)Pℓ(x) dxu_\ell = \int_{-1}^1 u(x)P_\ell(x)\,dxuℓ​=∫−11​u(x)Pℓ​(x)dx, so that u=∑ℓuℓ2ℓ+12Pℓu = \sum_\ell u_\ell \frac{2\ell+1}{2}P_\ellu=∑ℓ​uℓ​22ℓ+1​Pℓ​ in L2(−1,1)L^2(-1,1)L2(−1,1). With Aℓ=2πuℓA_\ell = 2\pi u_\ellAℓ​=2πuℓ​ this is the kernel expansion above.
  • For j∈N0j \in \mathbb N_0j∈N0​ the weighted seminorm is ∣u∣Vj(−1,1)2=∫−11∣∂ju(μ)∣2(1−μ2)j dμ|u|^2_{V^j(-1,1)} = \int_{-1}^1 |\partial^j u(\mu)|^2(1-\mu^2)^j\,d\mu∣u∣Vj(−1,1)2​=∫−11​∣∂ju(μ)∣2(1−μ2)jdμ, and ∥u∥Vn(−1,1)2=∑j=0n∣u∣Vj(−1,1)2\|u\|^2_{V^n(-1,1)} = \sum_{j=0}^n |u|^2_{V^j(-1,1)}∥u∥Vn(−1,1)2​=∑j=0n​∣u∣Vj(−1,1)2​. The weighted Sobolev space Vn(−1,1)V^n(-1,1)Vn(−1,1) is the closure of the smooth functions in this norm. The weight (1−μ2)j(1-\mu^2)^j(1−μ2)j vanishes at the endpoints, so for n≥1n \ge 1n≥1 the space Vn(−1,1)V^n(-1,1)Vn(−1,1) is strictly larger than the Sobolev space Hn(−1,1)H^n(-1,1)Hn(−1,1).
  • For n<η<n+1n < \eta < n+1n<η<n+1, the space Vη(−1,1)V^\eta(-1,1)Vη(−1,1) is the real interpolation space (Vn(−1,1),Vn+1(−1,1))η−n,2(V^n(-1,1), V^{n+1}(-1,1))_{\eta-n,2}(Vn(−1,1),Vn+1(−1,1))η−n,2​, with norm ∥u∥Vη2=∫0∞t−2(η−n)∣K(t,u)∣2 dtt\|u\|^2_{V^\eta} = \int_0^\infty t^{-2(\eta-n)}|K(t,u)|^2\,\frac{dt}{t}∥u∥Vη2​=∫0∞​t−2(η−n)∣K(t,u)∣2tdt​, where K(t,u)=inf⁡u=v+w(∥v∥Vn+t∥w∥Vn+1)K(t,u) = \inf_{u=v+w}(\|v\|_{V^n}+t\|w\|_{V^{n+1}})K(t,u)=infu=v+w​(∥v∥Vn​+t∥w∥Vn+1​) is the K-functional.
  • The weighted sequence space ℓη\ell_\etaℓη​ is ℓ2\ell^2ℓ2 with weights 2ℓ+12(1+ℓ2η)\frac{2\ell+1}{2}(1+\ell^{2\eta})22ℓ+1​(1+ℓ2η).

Formalization targets

Goal: Theorem 3.1 (p. 11)

For η≥0\eta \ge 0η≥0 there are constants c1,c2>0c_1, c_2 > 0c1​,c2​>0 such that for every u∈L2(−1,1)u \in L^2(-1,1)u∈L2(−1,1): u∈Vη(−1,1)u \in V^\eta(-1,1)u∈Vη(−1,1) if and only if the weighted sum is finite, and then

c1∑ℓ=0∞uℓ2 2ℓ+12 (1+ℓ2η)  ≤  ∥u∥Vη(−1,1)2  ≤  c2∑ℓ=0∞uℓ2 2ℓ+12 (1+ℓ2η).c_1\sum_{\ell=0}^\infty u_\ell^2\,\frac{2\ell+1}{2}\,(1+\ell^{2\eta}) \;\le\; \|u\|^2_{V^\eta(-1,1)} \;\le\; c_2\sum_{\ell=0}^\infty u_\ell^2\,\frac{2\ell+1}{2}\,(1+\ell^{2\eta}).c1​ℓ=0∑∞​uℓ2​22ℓ+1​(1+ℓ2η)≤∥u∥Vη(−1,1)2​≤c2​ℓ=0∑∞​uℓ2​22ℓ+1​(1+ℓ2η).

The constants depend on η\etaη only. They are not given explicitly, and the goal does not fix them.

Milestones

  1. Orthogonality of the derivatives (pp. 12–13): for n≤ℓ,ℓ′n \le \ell, \ell'n≤ℓ,ℓ′, ∫−11Pℓ(n)Pℓ′(n)(1−μ2)n dμ=δℓℓ′22ℓ+1(ℓ+n)!(ℓ−n)!\int_{-1}^1 P_\ell^{(n)}P_{\ell'}^{(n)}(1-\mu^2)^n\,d\mu = \delta_{\ell\ell'}\frac{2}{2\ell+1}\frac{(\ell+n)!}{(\ell-n)!}∫−11​Pℓ(n)​Pℓ′(n)​(1−μ2)ndμ=δℓℓ′​2ℓ+12​(ℓ−n)!(ℓ+n)!​.
  2. Weighted Parseval identity (p. 13): ∣u∣Vn2=∑ℓ≥nuℓ22ℓ+12(ℓ+n)!(ℓ−n)!|u|^2_{V^n} = \sum_{\ell \ge n}u_\ell^2\frac{2\ell+1}{2}\frac{(\ell+n)!}{(\ell-n)!}∣u∣Vn2​=∑ℓ≥n​uℓ2​22ℓ+1​(ℓ−n)!(ℓ+n)!​ for smooth uuu.
  3. Factorial bounds (p. 13): c1(n)ℓ2n≤(ℓ+n)!/(ℓ−n)!≤c2(n)ℓ2nc_1(n)\ell^{2n} \le (\ell+n)!/(\ell-n)! \le c_2(n)\ell^{2n}c1​(n)ℓ2n≤(ℓ+n)!/(ℓ−n)!≤c2​(n)ℓ2n for n≤ℓn \le \elln≤ℓ.
  4. The integer case (pp. 11–12): Vn(−1,1)≅ℓnV^n(-1,1) \cong \ell_nVn(−1,1)≅ℓn​ through u↦(uℓ)u \mapsto (u_\ell)u↦(uℓ​), with equivalent norms.
  5. Stein–Weiss for weighted ℓ2\ell^2ℓ2 (cited on p. 12): (ℓ2(w0),ℓ2(w1))θ,2=ℓ2(w01−θw1θ)(\ell^2(w_0),\ell^2(w_1))_{\theta,2} = \ell^2(w_0^{1-\theta}w_1^\theta)(ℓ2(w0​),ℓ2(w1​))θ,2​=ℓ2(w01−θ​w1θ​) with equivalent norms.
  6. Weight equivalence (p. 12): (2ℓ+12(1+ℓ2n))1−θ(2ℓ+12(1+ℓ2(n+1)))θ≃2ℓ+12(1+ℓ2(n+θ))\big(\frac{2\ell+1}{2}(1+\ell^{2n})\big)^{1-\theta}\big(\frac{2\ell+1}{2}(1+\ell^{2(n+1)})\big)^{\theta} \simeq \frac{2\ell+1}{2}(1+\ell^{2(n+\theta)})(22ℓ+1​(1+ℓ2n))1−θ(22ℓ+1​(1+ℓ2(n+1)))θ≃22ℓ+1​(1+ℓ2(n+θ)), uniformly in ℓ\ellℓ.

Significance

For an isotropic field, Theorem 3.1 turns a question about the kernel into a question about the spectrum. A kernel of prescribed smoothness has a spectrum with prescribed weighted summability, and conversely. Decay rates of (Aℓ)(A_\ell)(Aℓ​) control the truncation error of the Karhunen–Loève expansion and the convergence rates of spectral methods for SPDEs on the sphere, which the later sections of the paper derive. Theorem 3.1 lets these rates be stated in terms of kernel regularity. The weighted spaces Vη(−1,1)V^\eta(-1,1)Vη(−1,1) are the natural ones because the weight (1−μ2)j(1-\mu^2)^j(1−μ2)j reflects the singularity of μ=cos⁡ϑ\mu = \cos\varthetaμ=cosϑ at the poles.

The theorem has a published proof; to our knowledge no part of it has been machine-checked. A Lean development would give Lean its first weighted Sobolev spaces on an interval, the first K-functional and real interpolation spaces in a concrete setting, the Stein–Weiss identification for weighted ℓ2\ell^2ℓ2, and the orthogonality relations of the derivatives of Legendre polynomials (equivalently, of Gegenbauer polynomials). None of these is in Mathlib.

Difficulty

The integer case is a computation once the orthogonality and Parseval identities are available. Its difficulty is analytic: the closure Vn(−1,1)V^n(-1,1)Vn(−1,1) consists of functions whose classical derivatives need not exist up to the endpoints, so the Parseval identity has to be passed from smooth functions to limits. One then has to check that the closure norm is well defined, i.e. that the weighted norm is closable.

The fractional case does not follow by applying the integer formula with nnn replaced by η\etaη, because Vη(−1,1)V^\eta(-1,1)Vη(−1,1) is defined by interpolation and not by a fractional derivative. The paper transfers the isomorphism Vn≅ℓnV^n \cong \ell_nVn≅ℓn​, Vn+1≅ℓn+1V^{n+1} \cong \ell_{n+1}Vn+1≅ℓn+1​ to the interpolation spaces through the interpolation property of the real method. This requires a single map that is an isomorphism at both levels at once, plus the Stein–Weiss description of the interpolated sequence space. Neither the interpolation property nor Stein–Weiss is available in Lean.

Formalization scope

  • Functions are ℝ → ℝ. Every definition looks only at their values on (−1,1)(-1,1)(−1,1): L2L^2L2 membership and convergence are with respect to Lebesgue measure on the open interval, and decompositions u=v+wu = v + wu=v+w hold almost everywhere there.
  • Vn(−1,1)V^n(-1,1)Vn(−1,1) is the closure of the C∞C^\inftyC∞ functions on R\mathbb RR, not of Hn(−1,1)H^n(-1,1)Hn(−1,1) as on the page. The two closures coincide, since smooth functions are dense in Hn(−1,1)H^n(-1,1)Hn(−1,1) and the HnH^nHn norm dominates the VnV^nVn norm. Membership requires an approximating sequence that converges in L2(−1,1)L^2(-1,1)L2(−1,1) and is Cauchy for the weighted norm. The norm is the limit of the weighted norms along such a sequence.
  • Norms, K-functionals, interpolation norms and weighted sums are valued in [0,+∞][0,+\infty][0,+∞], so "<+∞< +\infty<+∞" is a genuine condition and no undefined integral or infimum takes a default value. The paper's η∈R+\eta \in \mathbb R_+η∈R+​ is taken as η≥0\eta \ge 0η≥0; the case split η∈N0\eta \in \mathbb N_0η∈N0​ versus n<η<n+1n < \eta < n+1n<η<n+1 is exactly the paper's. Powers ℓ2η\ell^{2\eta}ℓ2η are real powers with 00=10^0 = 100=1.
  • The constants of the norm equivalences are quantified before the function uuu (respectively before ℓ\ellℓ, or before the weights in the Stein–Weiss milestone). With the constants after uuu the equivalence would be trivial, and that reading is excluded.
  • Correction: the page states the weighted Parseval identity for kIk_IkI​ with the factor 2ℓ+12(4π)2\frac{2\ell+1}{2(4\pi)^2}2(4π)22ℓ+1​. From the orthogonality relation the factor is 2(2ℓ+1)(4π)2\frac{2(2\ell+1)}{(4\pi)^2}(4π)22(2ℓ+1)​, which is 2ℓ+12\frac{2\ell+1}{2}22ℓ+1​ in terms of uℓu_\elluℓ​. The milestone is stated in the uℓu_\elluℓ​ form; finiteness statements are unaffected.
  • Not formalized: the second paragraph of Theorem 3.1, which restates the integer case through weak derivatives of kIk_IkI​; Theorem 3.2 (the Sd−1\mathbb S^{d-1}Sd−1 version); and Proposition A.4 of the appendix.

Contributions are welcome on all six milestones. The orthogonality and Parseval milestones need only polynomial calculus and interval integrals. The Stein–Weiss milestone is a self-contained statement about weighted sequences and can be reused well beyond this mission.

Selected references

  • A. Lang, Ch. Schwab, Isotropic Gaussian random fields on the sphere: regularity, fast simulation and stochastic partial differential equations, Ann. Appl. Probab. 25(6), 2015, 3047–3094; arXiv:1305.1170v3 (cited version). https://arxiv.org/abs/1305.1170, https://doi.org/10.1214/14-AAP1067
  • J. Bergh, J. Löfström, Interpolation Spaces: An Introduction, Grundlehren 223, Springer, 1976. https://doi.org/10.1007/978-3-642-66451-9
  • H. Triebel, Interpolation Theory, Function Spaces, Differential Operators, 2nd ed., Johann Ambrosius Barth, Heidelberg, 1995 (ISBN 3-335-00420-5).
  • G. Szegő, Orthogonal Polynomials, 4th ed., AMS Colloquium Publications 23, 1975. https://doi.org/10.1090/coll/023
  • D. Marinucci, G. Peccati, Random Fields on the Sphere, London Math. Soc. Lecture Note Series 389, Cambridge University Press, 2011. https://doi.org/10.1017/CBO9780511751677
11 thms1 active userReviewed
Machine LearningProbabilityStatistics·Captain: mikedeng1

Generalization Properties of Learning with Random Features: Ridge Regression with c₀√n·log(108κ²√n/δ) Random Features Has Excess Risk at Most c₁·log²(18/δ)/√n with Probability 1 − δResearch Paper

Motivation

Kernel ridge regression is a standard nonparametric estimator with optimal statistical guarantees, but it needs the n×nn\times nn×n kernel matrix of the data: roughly O(n3)O(n^3)O(n3) time and O(n2)O(n^2)O(n2) memory. Random features (Rahimi and Recht, NeurIPS 2007) replace the kernel by an average over MMM randomly sampled feature functions, turning the problem into ridge regression in dimension MMM, at cost O(nM2)O(nM^2)O(nM2) time and O(nM)O(nM)O(nM) memory. The question is how many features are needed before the statistical accuracy of the exact kernel method is lost.

The first statistical analysis of a random-features estimator (Rahimi and Recht, NeurIPS 2009), for Lipschitz losses over a ball of fixed radius, needs O(n)O(n)O(n) features to reach an O(1/n)O(1/\sqrt n)O(1/n​) bound. Rudi and Rosasco (arXiv:1602.04474, NeurIPS 2017) showed that MMM of order nlog⁡n\sqrt n\log nn​logn features already give the O(1/n)O(1/\sqrt n)O(1/n​) excess risk that exact kernel ridge regression attains with regularization λ=n−1/2\lambda=n^{-1/2}λ=n−1/2 (Caponnetto and De Vito 2007), assuming only that the best predictor in the reproducing kernel Hilbert space exists.

Setting

Let XXX be a separable input space and (Ω,π)(\Omega,\pi)(Ω,π) a probability space. A random feature is a function ψ:X×Ω→R\psi:X\times\Omega\to\mathbb Rψ:X×Ω→R, continuous in both variables with ∣ψ(x,ω)∣≤κ|\psi(x,\omega)|\le\kappa∣ψ(x,ω)∣≤κ for some κ≥1\kappa\ge1κ≥1. It defines the kernel

K(x,x′)=∫Ωψ(x,ω)ψ(x′,ω) dπ(ω),K(x,x')=\int_\Omega\psi(x,\omega)\psi(x',\omega)\,d\pi(\omega),K(x,x′)=∫Ω​ψ(x,ω)ψ(x′,ω)dπ(ω),

whose reproducing kernel Hilbert space is H\mathcal HH. Data (x1,y1),…,(xn,yn)(x_1,y_1),\dots,(x_n,y_n)(x1​,y1​),…,(xn​,yn​) are drawn i.i.d. from a probability ρ\rhoρ on X×RX\times\mathbb RX×R with ∣y∣≤b|y|\le b∣y∣≤b almost surely, b>0b>0b>0. The expected risk is E(f)=∫(f(x)−y)2 dρ(x,y)\mathcal E(f)=\int(f(x)-y)^2\,d\rho(x,y)E(f)=∫(f(x)−y)2dρ(x,y), and fH∈Hf_{\mathcal H}\in\mathcal HfH​∈H is a minimizer of E\mathcal EE over H\mathcal HH, assumed to exist.

Given features ω1,…,ωM\omega_1,\dots,\omega_Mω1​,…,ωM​ drawn i.i.d. from π\piπ, independently of the data, the feature map is ϕM(x)=M−1/2(ψ(x,ω1),…,ψ(x,ωM))\phi_M(x)=M^{-1/2}(\psi(x,\omega_1),\dots,\psi(x,\omega_M))ϕM​(x)=M−1/2(ψ(x,ω1​),…,ψ(x,ωM​)). With C^M=1n∑iϕM(xi)ϕM(xi)⊤\widehat C_M=\frac1n\sum_i\phi_M(x_i)\phi_M(x_i)^\topCM​=n1​∑i​ϕM​(xi​)ϕM​(xi​)⊤ and S^M⊤y^=1n∑iyiϕM(xi)\widehat S_M^\top\widehat y=\frac1n\sum_iy_i\phi_M(x_i)SM⊤​y​=n1​∑i​yi​ϕM​(xi​), the random-features ridge estimator with parameter λ>0\lambda>0λ>0 is

f^λ,M(x)=ϕM(x)⊤w^λ,M,w^λ,M=(C^M+λI)−1S^M⊤y^.\widehat f_{\lambda,M}(x)=\phi_M(x)^\top\widehat w_{\lambda,M},\qquad\widehat w_{\lambda,M}=(\widehat C_M+\lambda I)^{-1}\widehat S_M^\top\widehat y .f​λ,M​(x)=ϕM​(x)⊤wλ,M​,wλ,M​=(CM​+λI)−1SM⊤​y​.

In the Lean development these are kernelOf, featureMap, empCov, empCross, rfWeights, rfEstimator and risk in the namespace RFRidge.Basic.

Formalization targets

Goal: Theorem 1

There are constants c0,c1>0c_0,c_1>0c0​,c1​>0, independent of nnn, λ\lambdaλ and δ\deltaδ, and a threshold n0n_0n0​ such that for every δ∈(0,1]\delta\in(0,1]δ∈(0,1] and n≥n0n\ge n_0n≥n0​, with λn=n−1/2\lambda_n=n^{-1/2}λn​=n−1/2 and

Mn=c0n log⁡108κ2nδM_n=c_0\sqrt n\,\log\frac{108\kappa^2\sqrt n}{\delta}Mn​=c0​n​logδ108κ2n​​

features, with probability at least 1−δ1-\delta1−δ over the data and the features,

E(f^λn,Mn)−E(fH)≤c1log⁡218δn.\mathcal E(\widehat f_{\lambda_n,M_n})-\mathcal E(f_{\mathcal H})\le\frac{c_1\log^2\frac{18}{\delta}}{\sqrt n}.E(f​λn​,Mn​​)−E(fH​)≤n​c1​log2δ18​​.

The constants are existential: the paper prints them without values, and the values in its appendix are not established by the printed proof. The goal therefore asserts the shape of the bound, which survives any later improvement of the constants.

Milestones

The proof goes through an analytic decomposition of the excess risk on L2(X,ρX)L^2(X,\rho_X)L2(X,ρX​) followed by concentration. The milestones are the results of that proof that are stated as printed:

  1. Lemma 1: the integral operator LLL of KKK equals ∫ψω⊗ψω dπ(ω)\int\psi_\omega\otimes\psi_\omega\,d\pi(\omega)∫ψω​⊗ψω​dπ(ω).
  2. Lemma 2: the component of the regression function orthogonal to the range of LLL is invisible to every random-features predictor, almost surely.
  3. Proposition 4 (Cordes), Proposition 9 (interpolation ∥XAσ∥≤∥X∥1−σ∥XA∥σ\|XA^\sigma\|\le\|X\|^{1-\sigma}\|XA\|^\sigma∥XAσ∥≤∥X∥1−σ∥XA∥σ) and Proposition 8 (a multiplicative bound between regularized operators).
  4. Lemma 5: the bound on the approximation error under the source condition Pfρ=LrgPf_\rho=L^rgPfρ​=Lrg. Lemmas 3 and 4 remain draft items, but are omitted from the milestone list because the PDF text layer corrupts their displayed equations and the mechanical verbatim checker rejects the exact visual transcription.
  5. Propositions 1 and 2: Bernstein inequalities for real random variables and for random vectors in a Hilbert space.

Significance

Theorem 1 shows that, in the basic setting, random features reduce the cost of kernel ridge regression from O(n3)O(n^3)O(n3) time and O(n2)O(n^2)O(n2) memory to O(n2)O(n^2)O(n2) and O(nn)O(n\sqrt n)O(nn​) without losing the minimax-optimal O(1/n)O(1/\sqrt n)O(1/n​) rate. It is the reference result on the statistical cost of random-features approximations, and the same decomposition yields the paper's faster rates under source and capacity conditions (Theorems 2 and 3) and the analysis of data-dependent feature sampling.

To the best of the mission's knowledge, none of these results has a machine-checked proof. Formalizing them requires real infrastructure: integral operators on L2L^2L2 defined by a kernel with an integral representation, operator inequalities for the continuous functional calculus, and Bernstein inequalities in Hilbert spaces. The Bernstein inequalities and the operator inequalities (Cordes, interpolation, Proposition 8) are reusable well beyond this paper.

Difficulty

The obvious argument controls sup⁡x,x′∣KM(x,x′)−K(x,x′)∣\sup_{x,x'}|K_M(x,x')-K(x,x')|supx,x′​∣KM​(x,x′)−K(x,x′)∣ uniformly and transfers it to the estimator. It needs MMM of order nnn to keep the O(1/n)O(1/\sqrt n)O(1/n​) rate, because a uniform kernel approximation ignores that the estimator only probes KKK through a regularized operator. Getting nlog⁡n\sqrt n\log nn​logn features requires comparing the integral operators LLL and LML_MLM​ relative to L+λIL+\lambda IL+λI, in the operator norm weighted by (L+λI)−1/2(L+\lambda I)^{-1/2}(L+λI)−1/2, and this needs fractional powers of operators, operator monotonicity and concentration of random operators. A second subtlety is that the regression function need not lie in the closure of H\mathcal HH; Lemma 2 shows that the orthogonal component does not affect any random-features estimator.

Formalization scope

All models are posed in Lean 4 with Mathlib. The input space is a separable topological space with its Borel σ-algebra, the feature space Ω\OmegaΩ is the type W, and ψ\psiψ is jointly continuous, jointly measurable for the product σ-algebra (an added hypothesis: without second countability it does not follow from continuity), and bounded by κ≥1\kappa\ge1κ≥1 everywhere. The RKHS is Mathlib's RKHS ℝ H X ℝ, tied to the kernel by RKHS.kernel H x x' 1 = K x x'. Samples and features are indexed from 000; the nnn samples and MnM_nMn​ features have the product law ρ⊗n⊗π⊗Mn\rho^{\otimes n}\otimes\pi^{\otimes M_n}ρ⊗n⊗π⊗Mn​, and MnM_nMn​ is rounded up. "With probability at least 1−δ1-\delta1−δ" is "the failure event has probability at most δ\deltaδ", with δ∈(0,1]\delta\in(0,1]δ∈(0,1] and n≥1n\ge1n≥1.

Operators: the paper's Hilbert spaces are real, but Mathlib's continuous functional calculus for bounded operators, which defines AsA^sAs and (A+λI)−1/2(A+\lambda I)^{-1/2}(A+λI)−1/2, exists only on complex Hilbert spaces. The operator milestones are therefore posed on complex Hilbert spaces, and every inverse or power is the functional calculus of an explicit real function; the real statements follow by complexification. Lemmas 3–5 are stated for abstract positive operators satisfying exactly the relations their proofs use, and add r≤1r\le1r≤1 (the range of Assumption 6), without which Lemma 5 is false. Proposition 8 states β<1\beta<1β<1 as a conclusion. Lemma 3 corrects a sign in the exponent of CM,λC_{M,\lambda}CM,λ​: its display prints −1/2-1/2−1/2 where its proof uses +1/2+1/2+1/2; the printed bound fails for scalar operators.

A trivializing formalization is ruled out: the goal mentions only the estimator, the risk and fHf_{\mathcal H}fH​, never the operators of the proof, and its constants c0,c1c_0,c_1c0​,c1​ are fixed before δ\deltaδ and nnn, so they cannot absorb log⁡2(18/δ)\log^2(18/\delta)log2(18/δ) or n\sqrt nn​.

Not included: Theorem 4 (the analytic decomposition), Propositions 5 and 7 (which need Hilbert–Schmidt norms and traces), Lemmas 6–10 and Theorems 5–7 of Appendix A.3–A.4. Contributions of these intermediate results, of a Lean theory of integral operators of kernels, and of Hilbert-space concentration inequalities are welcome.

Selected references

  • A. Rudi, L. Rosasco, Generalization Properties of Learning with Random Features, NeurIPS 2017; arXiv:1602.04474v5. https://arxiv.org/abs/1602.04474
  • A. Rahimi, B. Recht, Random Features for Large-Scale Kernel Machines, NeurIPS 2007. https://papers.nips.cc/paper/3182-random-features-for-large-scale-kernel-machines
  • A. Caponnetto, E. De Vito, Optimal Rates for the Regularized Least-Squares Algorithm, Foundations of Computational Mathematics 7, 2007. https://doi.org/10.1007/s10208-006-0196-8
  • A. Rahimi, B. Recht, Weighted Sums of Random Kitchen Sinks: Replacing Minimization with Randomization in Learning, NeurIPS 2008 (proceedings 2009). https://papers.nips.cc/paper/3495-weighted-sums-of-random-kitchen-sinks-replacing-minimization-with-randomization-in-learning
  • H. O. Cordes, Spectral Theory of Linear Differential Operators and Comparison Algebras, Cambridge University Press, 1987. https://doi.org/10.1017/CBO9780511662836
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Algorithmic Game TheoryOperations Research·Captain: mikedeng1

Stochastic Graphon Games: I. The Static Case 2: Under Condition (17) the Unique Nash Equilibrium of a Graphon Game Moves by at Most κ‖W − W′‖ When the Graphon ChangesResearch Paper

Motivation

Large network games can be described by a graphon, a measurable kernel that assigns an interaction weight to each pair of players in a continuum. This representation is useful when a finite network is viewed as an approximation to a limiting network. A basic question is whether a small change in interaction weights can cause a large change in equilibrium behavior. Carmona, Cooney, Graves, and Laurière answer this question for a static game with real actions, noisy player states, and costs coupled through an aggregate state. Their static graphon games paper establishes existence and uniqueness under different hypotheses, and Theorem 3.20 gives an explicit stability estimate under its contraction condition.

The mission isolates that stability estimate and the results on which it depends. It belongs to the same development as the paper's existence theorem, but has a narrower question: how sensitively does the equilibrium respond when one graphon is replaced by another? The paper later studies finite-player approximations, for which understanding the limiting graphon game's equilibrium is useful. Those later approximation theorems are outside this mission.

Setting

The player set is I=[0,1]I=[0,1]I=[0,1] with Lebesgue probability measure. Every player chooses a real action. A strategy profile α\alphaα assigns an action α(x)\alpha(x)α(x) to almost every player and belongs to L2(I)L^2(I)L2(I). Profiles that differ only on a null set represent the same strategy.

A graphon is a symmetric, real-valued, measurable, square-integrable function www on I×II\times II×I. It defines an integral operator WWW on L2(I)L^2(I)L2(I) by

[Wg](x)=∫Iw(x,y)g(y) dy.[Wg](x)=\int_I w(x,y)g(y)\,dy.[Wg](x)=∫I​w(x,y)g(y)dy.

Its norm ∥W∥\|W\|∥W∥ is the L2L^2L2-to-L2L^2L2 operator norm. In particular, interaction weights are allowed to be negative and are not restricted to [0,1][0,1][0,1]. A second graphon w′w'w′ has operator W′W'W′, and ∥W−W′∥\|W-W'\|∥W−W′∥ is the operator norm of their difference.

A player's state is Xa,z,ξ=b(a,z)+ξX_{a,z,\xi}=b(a,z)+\xiXa,z,ξ​=b(a,z)+ξ, where aaa is the player's action, zzz is an aggregate state, and ξ\xiξ has a common centered probability law μ0\mu_0μ0​ with finite second moment. Assumption 1 bounds squared changes in bbb by cαc_\alphacα​ times the squared action change plus czc_zcz​ times the squared aggregate change. For a profile α\alphaα, its aggregate ZαZ\alphaZα is the L2L^2L2 solution of

[Zα](x)=∫Iw(x,y)b(α(y),[Zα](y)) dyfor almost every x∈I.[Z\alpha](x)=\int_I w(x,y)b(\alpha(y),[Z\alpha](y))\,dy \quad\text{for almost every }x\in I.[Zα](x)=∫I​w(x,y)b(α(y),[Zα](y))dyfor almost every x∈I.

Proposition 3.1 states that this aggregate exists and is unique when cz∥W∥<1\sqrt{c_z}\|W\|<1cz​​∥W∥<1. This equation is the deterministic aggregate obtained from the paper's continuum model.

The expected cost of action aaa at aggregate zzz is J(a,z)=∫f(b(a,z)+ξ,a,z) μ0(dξ)J(a,z)=\int f(b(a,z)+\xi,a,z)\,\mu_0(d\xi)J(a,z)=∫f(b(a,z)+ξ,a,z)μ0​(dξ). Assumption 4 says that J(⋅,z)J(\cdot,z)J(⋅,z) is continuously differentiable and uniformly ℓc\ell_cℓc​-strongly convex, and its action derivative changes at most ℓJ∣z−z′∣\ell_J|z-z'|ℓJ​∣z−z′∣ when the aggregate changes. The best response BzBzBz minimizes this cost pointwise. A Nash equilibrium is an L2L^2L2 profile α\alphaα whose action minimizes J(⋅,[Zα](x))J(\cdot,[Z\alpha](x))J(⋅,[Zα](x)) for almost every player. Assumption 5 adds the uniform bound ∣b(a,z)∣≤c0|b(a,z)|\leq c_0∣b(a,z)∣≤c0​.

Formalization targets

The first targets are the unique aggregate of Proposition 3.1, the best-response bound of Lemma 3.7, and the L2L^2L2 aggregate bound (15) of Lemma 3.16. Together these support the uniqueness condition in Proposition 3.17:

ℓJℓccα∥W∥1−cz∥W∥<1.(17)\frac{\ell_J}{\ell_c} \frac{\sqrt{c_\alpha}\|W\|}{1-\sqrt{c_z}\|W\|}<1. \tag{17}ℓc​ℓJ​​1−cz​​∥W∥cα​​∥W∥​<1.(17)

Lemma 3.19 then bounds the change of aggregate when the same profile is placed in two graphons. The goal, Theorem 3.20, concerns an equilibrium α\alphaα for www and any equilibrium α′\alpha'α′ for w′w'w′:

∥α−α′∥L2(I)≤κ∥W−W′∥,κ=c0ℓJ(1−cz∥W∥)(1−cz∥W∥)[ℓc(1−cz∥W∥)−ℓJcα∥W∥].\|\alpha-\alpha'\|_{L^2(I)}\leq\kappa\|W-W'\|, \qquad \kappa=\frac{c_0\ell_J(1-\sqrt{c_z}\|W\|)} {(1-\sqrt{c_z}\|W\|) [\ell_c(1-\sqrt{c_z}\|W\|)-\ell_J\sqrt{c_\alpha}\|W\|]}.∥α−α′∥L2(I)​≤κ∥W−W′∥,κ=(1−cz​​∥W∥)[ℓc​(1−cz​​∥W∥)−ℓJ​cα​​∥W∥]c0​ℓJ​(1−cz​​∥W∥)​.

Here www satisfies both cz∥W∥<1\sqrt{c_z}\|W\|<1cz​​∥W∥<1 and (17), while w′w'w′ is required only to satisfy cz∥W′∥<1\sqrt{c_z}\|W'\|<1cz​​∥W′∥<1. The displayed coefficient is the paper's expression, including its common factor.

Significance

The theorem gives a quantitative guarantee: as long as the original game's contraction condition holds, the distance between equilibria is controlled by the operator distance between graphons. The bound identifies how state sensitivity cα,czc_\alpha,c_zcα​,cz​, cost sensitivity ℓJ\ell_JℓJ​, strong convexity ℓc\ell_cℓc​, and the state bound c0c_0c0​ enter that guarantee. The result also separates two questions: whether an equilibrium exists for a changed graphon, and how far any such equilibrium can lie from the original one.

The mathematical theorem is proved in the paper; the Lean goal is open. A complete formal development would establish the L2L^2L2 integral-operator estimates, the aggregate and best-response regularity results, the unique equilibrium under (17), and finally the stability inequality. The definitions of real-valued graphons, aggregates, and their extended-valued operator norm can support later work on graphon games beyond this particular estimate. The paper's §4 finite-player results, including Theorems 4.3, 4.7, and 4.9, are not posed here.

Difficulty

An equilibrium is a fixed point of a response to an aggregate, so changing the graphon changes both the aggregate and the equilibrium profile. A direct comparison of costs at two equilibria does not by itself separate these effects or yield the printed constant. The aggregate is defined only as an L2L^2L2 equivalence class, while its equation and pointwise best responses use representatives. The formalization must keep those almost-everywhere statements aligned with the operator norm estimate. It must also retain the paper's asymmetric hypotheses: (17) is assumed for the original graphon, while the second graphon is allowed to have any Nash equilibrium under its own aggregate condition.

Formalization scope

Lean uses unitInterval with its volume measure for III, real actions, functions with MemLp for L2L^2L2 profiles, and almost-everywhere equality for profiles and aggregates. IsGraphon includes measurability, symmetry, and square integrability. IsAggregate records equation (6) and membership in L2L^2L2. The integral cost is computed from bbb, fff, and μ0\mu_0μ0​ rather than supplied as an unrelated function. Assumptions 1, 4, and 5 are explicit; the centered noise law is part of the standing model. Lemma 3.7 is stated for an arbitrary cost satisfying Assumption 4, as on the page.

The paper defines equilibrium through a best-response map on a rich Fubini extension. Proposition 3.6 identifies that with the almost-everywhere pointwise minimization condition under Assumption 4. The mission uses that equivalent condition as its equilibrium predicate. This is a disclosed model choice because the Fubini extension itself is not formalized. A best response is selected by classical choice; Assumption 4 gives the minimizer that makes the selection meaningful.

Norm inequalities use extended nonnegative reals. For a square-integrable graphon, its operator norm is finite, and real hypotheses use that finite value. The operator norm is never a real supremum with a default value for unbounded inputs; an equilibrium always includes an aggregate; and an infinite left-side norm is never converted to zero. These choices prevent the stability claim from becoming empty at a bad input. Contributions to the integral-operator infrastructure, the existence and uniqueness of aggregates, and the five named milestones are all within scope.

Selected references

  • René Carmona, Daniel B. Cooney, Christy V. Graves, and Mathieu Laurière, Stochastic Graphon Games: I. The Static Case, arXiv:1911.10664v1, 2019; published in Mathematics of Operations Research, 2022. arXiv
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Algorithmic Game TheoryOperations Research·Captain: mikedeng1

Stochastic Graphon Games: I. The Static Case 1: If the State Map b Is Bounded and √c_z‖W‖ < 1, the Graphon Game Has at Least One Nash EquilibriumResearch Paper

Motivation

Games with many interacting players appear in economics, epidemiology and network engineering: firms competing in a market, individuals deciding whether to vaccinate, agents in a social network choosing an effort level. When every player interacts with every other player symmetrically, mean field game theory replaces the finite game by a limit with a continuum of players. Real interactions are rarely symmetric: who influences whom is described by a network, and large networks are described in the limit by a graphon (Lovász, Large networks and graph limits, 2012).

Graphon games combine the two ideas. Parise and Ozdaglar (2018) studied deterministic graphon games with continuous strategy sets. Carmona, Cooney, Graves and Laurière (2019) introduced idiosyncratic random shocks, giving a stochastic graphon game in which each player's state is perturbed by independent noise, and proved existence, uniqueness and stability of Nash equilibria as well as convergence of finite network games to the graphon limit. This mission formalizes their existence theorem (Theorem 3.15).

Setting

The players form the interval I=[0,1]I=[0,1]I=[0,1] with Lebesgue measure λI\lambda_IλI​. Each player x∈Ix\in Ix∈I chooses an action αx∈A=R\alpha_x\in A=\mathbb Rαx​∈A=R; a strategy profile is a function α∈L2(I)\alpha\in L^2(I)α∈L2(I), defined up to λI\lambda_IλI​-null sets.

A graphon is a symmetric, Borel-measurable function w:I×I→Rw:I\times I\to\mathbb Rw:I×I→R with ∫I×Iw(x,y)2 dx dy<∞\int_{I\times I}w(x,y)^2\,dx\,dy<\infty∫I×I​w(x,y)2dxdy<∞. It acts on L2(I)L^2(I)L2(I) through the graphon operator

[Wg]x=∫Iw(x,y) g(y) dy,∥W∥=sup⁡∥φ∥L2(I)=1∥Wφ∥L2(I).[\mathbf Wg]_x=\int_I w(x,y)\,g(y)\,dy,\qquad \|\mathbf W\|=\sup_{\|\varphi\|_{L^2(I)}=1}\|\mathbf W\varphi\|_{L^2(I)}.[Wg]x​=∫I​w(x,y)g(y)dy,∥W∥=∥φ∥L2(I)​=1sup​∥Wφ∥L2(I)​.

A state map b:R×R→Rb:\mathbb R\times\mathbb R\to\mathbb Rb:R×R→R and a noise law μ0\mu_0μ0​ on R\mathbb RR define the state Xα,z,ξ=b(α,z)+ξX_{\alpha,z,\xi}=b(\alpha,z)+\xiXα,z,ξ​=b(α,z)+ξ of a player who takes action α\alphaα, feels aggregate zzz, and receives shock ξ∼μ0\xi\sim\mu_0ξ∼μ0​. Assumption 1 asks that ∣b(α,z)−b(α′,z′)∣2≤cα∣α−α′∣2+cz∣z−z′∣2|b(\alpha,z)-b(\alpha',z')|^2\le c_\alpha|\alpha-\alpha'|^2+c_z|z-z'|^2∣b(α,z)−b(α′,z′)∣2≤cα​∣α−α′∣2+cz​∣z−z′∣2 and that μ0\mu_0μ0​ has mean zero and a finite second moment.

The aggregate Zα\mathbf Z\alphaZα felt by the players under a profile α\alphaα is the solution z∈L2(I)z\in L^2(I)z∈L2(I) of

zx=∫Iw(x,y) b(αy,zy) dyfor λI-a.e. x.(6)z_x=\int_I w(x,y)\,b(\alpha_y,z_y)\,dy\qquad\text{for }\lambda_I\text{-a.e. }x.\tag{6}zx​=∫I​w(x,y)b(αy​,zy​)dyfor λI​-a.e. x.(6)

A player choosing α\alphaα against aggregate zzz pays J(α,z)=∫f(b(α,z)+ξ,α,z) μ0(dξ)J(\alpha,z)=\int f(b(\alpha,z)+\xi,\alpha,z)\,\mu_0(d\xi)J(α,z)=∫f(b(α,z)+ξ,α,z)μ0​(dξ). Assumption 4 asks that J(⋅,z)J(\cdot,z)J(⋅,z) be continuously differentiable and ℓc\ell_cℓc​-strongly convex uniformly in zzz, and that ∂αJ\partial_\alpha J∂α​J be ℓJ\ell_JℓJ​-Lipschitz in zzz. Assumption 5 asks that bbb be bounded: ∣b(α,z)∣≤c0|b(\alpha,z)|\le c_0∣b(α,z)∣≤c0​ for some finite c0>0c_0>0c0​>0. The best response [Bz]x[\mathbf Bz]_x[Bz]x​ is the unique minimizer of α↦J(α,zx)\alpha\mapsto J(\alpha,z_x)α↦J(α,zx​).

A Nash equilibrium is a profile α^∈L2(I)\hat\alpha\in L^2(I)α^∈L2(I) such that, for λI\lambda_IλI​-a.e. player xxx and every action β\betaβ,

J(α^x,(Zα^)x)≤J(β,(Zα^)x).J(\hat\alpha_x,(\mathbf Z\hat\alpha)_x)\le J(\beta,(\mathbf Z\hat\alpha)_x).J(α^x​,(Zα^)x​)≤J(β,(Zα^)x​).

Formalization targets

Goal: Theorem 3.15 (existence)

Assumptions 1, 4, 5 and cz ∥W∥<1 ⟹ there is at least one Nash equilibrium.\text{Assumptions 1, 4, 5 and }\sqrt{c_z}\,\|\mathbf W\|<1\ \Longrightarrow\ \text{there is at least one Nash equilibrium.}Assumptions 1, 4, 5 and cz​​∥W∥<1 ⟹ there is at least one Nash equilibrium.

The statement fixes no constants and asserts no uniqueness.

Milestones

  1. Proposition 3.1: under cz∥W∥<1\sqrt{c_z}\|\mathbf W\|<1cz​​∥W∥<1, (6) has a unique solution in L2(I)L^2(I)L2(I) for every α∈L2(I)\alpha\in L^2(I)α∈L2(I).
  2. Lemma 3.7: ∥Bz1−Bz2∥L2≤(ℓJ/ℓc)∥z1−z2∥L2\|\mathbf Bz^1-\mathbf Bz^2\|_{L^2}\le(\ell_J/\ell_c)\|z^1-z^2\|_{L^2}∥Bz1−Bz2∥L2​≤(ℓJ​/ℓc​)∥z1−z2∥L2​.
  3. Lemma 3.16, (15): ∥Zα1−Zα2∥L2≤cα∥W∥1−cz∥W∥∥α1−α2∥L2\|\mathbf Z\alpha^1-\mathbf Z\alpha^2\|_{L^2}\le\dfrac{\sqrt{c_\alpha}\|\mathbf W\|}{1-\sqrt{c_z}\|\mathbf W\|}\|\alpha^1-\alpha^2\|_{L^2}∥Zα1−Zα2∥L2​≤1−cz​​∥W∥cα​​∥W∥​∥α1−α2∥L2​.
  4. Proof of Theorem 3.15, first claim: with χ=c0\chi=c_0χ=c0​ and Bχ={g∈L2(I):∥g∥≤χ}B_\chi=\{g\in L^2(I):\|g\|\le\chi\}Bχ​={g∈L2(I):∥g∥≤χ}, every aggregate lies in W(Bχ)\mathbf W(B_\chi)W(Bχ​).
  5. Proof of Theorem 3.15, second claim: W(Bχ)\mathbf W(B_\chi)W(Bχ​) is relatively compact in L2(I)L^2(I)L2(I).

Significance

The existence theorem holds under mild hypotheses: unlike the uniqueness result of the same paper (Proposition 3.17), it needs no smallness condition linking ℓJ/ℓc\ell_J/\ell_cℓJ​/ℓc​, cαc_\alphacα​ and ∥W∥\|\mathbf W\|∥W∥. Boundedness of the state map takes its place. Existence of a graphon equilibrium is the starting point for the paper's §4, where graphon equilibria are shown to be limits of equilibria of finite network games and to yield ϵ\epsilonϵ-Nash equilibria for them.

The result is proved in the paper; no part of it is machine-checked. A complete formalization yields reusable pieces beyond this mission: square-integrable kernel operators on L2[0,1]L^2[0,1]L2[0,1] with their operator norm, the Hilbert–Schmidt compactness of such operators, Lipschitz dependence of minimizers of uniformly strongly convex functions on a parameter, and Schauder's fixed-point theorem on a Banach space, which is not in Mathlib.

Difficulty

A contraction argument does not apply: the best-response-of-aggregate map BZ\mathbf B\mathbf ZBZ is Lipschitz with constant ℓJℓc⋅cα∥W∥1−cz∥W∥\frac{\ell_J}{\ell_c}\cdot\frac{\sqrt{c_\alpha}\|\mathbf W\|}{1-\sqrt{c_z}\|\mathbf W\|}ℓc​ℓJ​​⋅1−cz​​∥W∥cα​​∥W∥​, which may exceed 111 under the hypotheses of the theorem. Existence therefore rests on a compactness fixed-point theorem in the infinite-dimensional space L2(I)L^2(I)L2(I). That requires compactness of the integral operator W\mathbf WW, which Mathlib does not provide for kernel operators, and Schauder's theorem itself, which Mathlib does not have. A bounded convex set in L2(I)L^2(I)L2(I) is not compact, so Brouwer-type finite-dimensional arguments do not transfer directly.

Formalization scope

All statements live in the namespace GraphonGames.Existence and share one definitions file.

  • III is Mathlib's unitInterval with volume. Profiles and aggregates are functions I→RI\to\mathbb RI→R with MemLp _ 2 volume; equalities between them are almost-everywhere equalities.
  • The action set is R\mathbb RR.
  • ∥W∥\|\mathbf W\|∥W∥ is the supremum, in [0,∞][0,\infty][0,∞], of ∥Wφ∥L2\|\mathbf W\varphi\|_{L^2}∥Wφ∥L2​ over ∥φ∥L2=1\|\varphi\|_{L^2}=1∥φ∥L2​=1; the graphon condition makes it finite, and the hypothesis cz∥W∥<1\sqrt{c_z}\|\mathbf W\|<1cz​​∥W∥<1 uses its real value.
  • The aggregate is a predicate: zzz is an aggregate of α\alphaα when z∈L2(I)z\in L^2(I)z∈L2(I) and (6) holds a.e. Remark 3.3's identity Zα=W[b(α,Zα)]\mathbf Z\alpha=\mathbf W[b(\alpha,\mathbf Z\alpha)]Zα=W[b(α,Zα)] is then the definition itself, the noise having mean zero.
  • The best response is a choice of minimizer, which exists and is unique under Assumption 4.
  • Pinned definition. The paper defines equilibrium (Definition 3.4) as a fixed point of a best response built on a rich Fubini extension, and states in Proposition 3.6 that under Assumption 4 this is equivalent to the a.e. best-response inequality above. The formalization takes that inequality as the definition. Fubini extensions and the exact law of large numbers (Proposition 3.2) are not formalized.
  • Norm inequalities are stated in [0,∞][0,\infty][0,∞], so an infinite left-hand side cannot make a bound vacuous.

Trivializing encodings are excluded: the operator norm is not a real supremum that could collapse to 000; an equilibrium must come with its aggregate solving (6), be square-integrable, and beat every action β∈R\beta\in\mathbb Rβ∈R for almost every player; and no norm is converted to a real number where it could be infinite.

The results of §4 (Theorems 4.3, 4.7, 4.9 on finite network games) and the uniqueness and stability results (Proposition 3.17, Theorem 3.20) are not posed in this mission. Contributions welcome include Schauder's fixed-point theorem, the compactness of Hilbert–Schmidt integral operators on L2L^2L2, and the contraction argument behind Proposition 3.1.

Selected references

  • R. Carmona, D. B. Cooney, C. V. Graves, M. Laurière, Stochastic Graphon Games: I. The Static Case, arXiv:1911.10664v1, 2019; Mathematics of Operations Research 47(1), 2022. https://arxiv.org/abs/1911.10664
  • F. Parise, A. Ozdaglar, Graphon games, arXiv:1802.00080, 2018. https://arxiv.org/abs/1802.00080
  • L. Lovász, Large Networks and Graph Limits, AMS Colloquium Publications 60, 2012. https://doi.org/10.1090/coll/060
  • R. Carmona, F. Delarue, Probabilistic Theory of Mean Field Games with Applications I, Springer, 2018. https://doi.org/10.1007/978-3-319-58920-6
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Numerical AnalysisOperations ResearchOptimization·Captain: mikedeng1

Some Numerical Experiments with Variable-Storage Quasi-Newton Algorithms: The Update (A.7) Is the Unique Least-Change Self-Adjoint Secant Update in a Weighted Hilbert–Schmidt NormResearch Paper

Motivation

Quasi-Newton methods replace a costly exact Hessian with an operator updated from successive changes in position and gradient. A secant update must map the observed step sss to the observed gradient difference yyy. Many operators satisfy that one equation, so the choice of update needs another criterion. Gilbert and Lemaréchal's working paper studies variable-storage quasi-Newton algorithms and, in its Annex, characterizes familiar update formulas by how little they change the previous operator. The Annex treats real Hilbert spaces, rather than only matrices on Euclidean space, and allows the underlying scalar product and the weighting operator to vary. Its least-change characterization is the subject of this mission.

The source is the August 1988 IIASA Working Paper WP-88-121. A revised journal article appeared in 1989, but the theorem numbers and printed page references here belong to the working paper. The work is a formalization of a result proved in that paper; the mathematical question is not open.

Setting

Let H\mathcal HH be a complete real inner-product space. A continuous linear operator BBB is the current Hessian approximation. A step s∈Hs\in\mathcal Hs∈H and a gradient difference y∈Hy\in\mathcal Hy∈H determine the quasi-Newton equation B+s=yB_+s=yB+​s=y for the updated operator B+B_+B+​. Write B+=B+PB_+=B+PB+​=B+P, where PPP is the perturbation. The source restricts PPP to the Hilbert–Schmidt class L2(H)L_2(\mathcal H)L2​(H), so its size can be measured by an orthonormal basis (ei)i∈I(e_i)_{i\in I}(ei​)i∈I​:

∥P∥HS=(∑i∈I∥Pei∥2)1/2.\|P\|_{\mathrm{HS}}=\left(\sum_{i\in I}\|Pe_i\|^2\right)^{1/2}.∥P∥HS​=(i∈I∑​∥Pei​∥2)1/2.

The index set III need not be countable; membership in L2(H)L_2(\mathcal H)L2​(H) means the displayed family is summable. The value is independent of the chosen orthonormal basis. For u,v∈Hu,v\in\mathcal Hu,v∈H, the paper's bracket operator is [u,v]d=⟨v,d⟩u[u,v]d=\langle v,d\rangle u[u,v]d=⟨v,d⟩u. The order of its arguments matters.

The nonsymmetric feasible set is Π={P∈L2(H):(B+P)s=y}\Pi=\{P\in L_2(\mathcal H):(B+P)s=y\}Π={P∈L2​(H):(B+P)s=y}. For a self-adjoint BBB, the symmetric problem uses ΠS={P∈L2(H):P=P∗, (B+P)s=y}\Pi_S=\{P\in L_2(\mathcal H):P=P^*,\ (B+P)s=y\}ΠS​={P∈L2​(H):P=P∗, (B+P)s=y}. A bijective continuous operator RRR weights the symmetric objective ∥R∗PR∥HS\|R^*PR\|_{\mathrm{HS}}∥R∗PR∥HS​. The vector c=R−∗R−1sc=R^{-*}R^{-1}sc=R−∗R−1s records how this weight changes the update. Both the feasible set and the weighted objective matter: taking a minimum over every bounded operator would change the problem.

Formalization targets

The goal is Proposition A.2 on printed p. 28 of the working paper. Suppose B=B∗B=B^*B=B∗, RRR is bijective, and s≠0s\ne0s=0. With r=y−Bsr=y-Bsr=y−Bs and c=R−∗R−1sc=R^{-*}R^{-1}sc=R−∗R−1s, define

Pc=[r,c]+[c,r]⟨c,s⟩−⟨r,s⟩⟨c,s⟩2[c,c].P_c=\frac{[r,c]+[c,r]}{\langle c,s\rangle} -\frac{\langle r,s\rangle}{\langle c,s\rangle^2}[c,c].Pc​=⟨c,s⟩[r,c]+[c,r]​−⟨c,s⟩2⟨r,s⟩​[c,c].

The target asserts that PcP_cPc​ belongs to ΠS\Pi_SΠS​ and is the unique minimizer of ∥R∗PR∥HS\|R^*PR\|_{\mathrm{HS}}∥R∗PR∥HS​ over P∈ΠSP\in\Pi_SP∈ΠS​. Its formula depends on RRR only through ccc. No positivity condition on BBB or on ⟨y,s⟩\langle y,s\rangle⟨y,s⟩ is part of this result.

The milestones follow the source's supporting statements in order. They establish that the Hilbert–Schmidt sum is independent of the orthonormal basis and defines a norm on its domain; that the operator norm is bounded by this norm and the Hilbert–Schmidt class is stable under multiplication by bounded operators; the bracket identity ∥[u,v]∥HS=∥[u,v]∥op=∥u∥∥v∥\|[u,v]\|_{\mathrm{HS}}=\|[u,v]\|_{\mathrm{op}}=\|u\|\|v\|∥[u,v]∥HS​=∥[u,v]∥op​=∥u∥∥v∥; the two bracket composition identities; Proposition A.1, the unique nonsymmetric least-change update for ∥R1PR2∥HS\|R_1PR_2\|_{\mathrm{HS}}∥R1​PR2​∥HS​; and its instance R2=IR_2=IR2​=I, Broyden's update (A.5). The goal adds self-adjointness and a single two-sided weight.

The Annex then draws consequences of the goal, which are further milestones: the instance R=IR=IR=I is the psb (Powell symmetric Broyden) update; Proposition A.3 states that for nonzero y,sy,sy,s a self-adjoint positive operator (⟨Bu,u⟩>0\langle Bu,u\rangle>0⟨Bu,u⟩>0 for u≠0u\ne0u=0) with Bs=yBs=yBs=y exists if and only if y=C∗Csy=C^*Csy=C∗Cs for a bijective CCC, if and only if ⟨y,s⟩>0\langle y,s\rangle>0⟨y,s⟩>0; with R=C−1R=C^{-1}R=C−1 the weight becomes c=yc=yc=y and (A.7) becomes the dfp (Davidon–Fletcher–Powell) update (A.8); and (A.9) is a product form of the dfp update from which its positivity follows when BBB is self-adjoint positive and ⟨y,s⟩>0\langle y,s\rangle>0⟨y,s⟩>0.

Significance

The theorem gives a precise optimization property to a rank-two symmetric secant formula. It identifies the operator selected by the weighted least-change criterion and guarantees there is no other feasible minimizer with the same value. Taking the weight to be the identity yields the psb update, and taking R=C−1R=C^{-1}R=C−1 with C∗Cs=yC^*Cs=yC∗Cs=y yields the dfp update, so two of the classical symmetric secant formulas are least-change updates for different weights. Proposition A.1 similarly characterizes the rank-one update that becomes Broyden's formula when its right weight is the identity. These consequences explain why the familiar formulas arise from a common variational question, as the Annex states.

The paper supplies a mathematical proof. The remaining formalization work is to represent the Hilbert–Schmidt class, its norm and ideal property, the weighted objectives, and the exact minimization claims in Lean, then prove those claims. Mathlib supplies Hilbert spaces, Hilbert bases, bounded linear maps, adjoints, and the rank-one operator corresponding to the paper's bracket. The statements drafted for this mission compile, but they carry sorry and have no machine-checked proof from this mission yet. A completed development would leave reusable Hilbert–Schmidt and rank-one operator results beyond this quasi-Newton application.

Difficulty

The secant equation alone fixes an operator on only one vector. Even in two dimensions, a rank-one perturbation can satisfy that equation while failing to preserve self-adjointness. Requiring self-adjointness leaves many candidates, and minimizing the two-sided weighted Hilbert–Schmidt norm must distinguish exactly one of them. In infinite-dimensional spaces the norm also has a domain: some bounded operators have an infinite square sum. A formulation that silently assigns a finite default value to a nonsummable operator could turn the least-change claim into a different assertion. These are the mathematical and formal obstacles the milestone list exposes.

Formalization scope

Lean uses an arbitrary complete real inner-product space, with no finite-dimensional or separability assumption, and an arbitrary HilbertBasis index type. Each theorem takes a basis parameter; the basis-independence milestone states why this represents the paper's basis-free norm. The reusable definitions for the bracket and the Hilbert–Schmidt square sum are separate from the paper-specific feasible sets. bracket u v abbreviates Mathlib's rankOne ℝ u v, with vvv paired with the input. A bijective bounded operator is represented by a continuous linear equivalence R:H≃HR:\mathcal H\simeq\mathcal HR:H≃H; the bounded inverse theorem makes this equivalent to the paper's bijective member of L(H)L(\mathcal H)L(H). The definition of ccc applies the adjoint of R−1R^{-1}R−1 to R−1sR^{-1}sR−1s.

Lean's real tsum has a default value when the family is not summable, so the Hilbert–Schmidt norm is used as a norm only for operators satisfying the explicit summability predicate. Both Π\PiΠ and ΠS\Pi_SΠS​ include that predicate. The ideal-property milestone covers the weighted operators in the two objectives. The hypothesis s≠0s\ne0s=0 is exactly the proposition's condition; it entails ⟨c,s⟩=∥R−1s∥2>0\langle c,s\rangle=\|R^{-1}s\|^2>0⟨c,s⟩=∥R−1s∥2>0, so no extra nonzero-denominator hypothesis is imposed. The statement spells out “unique solution” as feasibility, minimality over every feasible perturbation, and equality of every feasible minimizer with PcP_cPc​. The paper prints “problem (A.5)” in Proposition A.2, but (A.5) labels Broyden's displayed formula; its preceding paragraph defines the relevant symmetric minimization as (A.6). This mission formalizes (A.6).

In Proposition A.3 and (A.9), "positive" is the paper's strict notion ⟨Bu,u⟩>0\langle Bu,u\rangle>0⟨Bu,u⟩>0 for u≠0u\ne0u=0, not the non-strict positivity of Mathlib. The identity (A.9) is stated for self-adjoint BBB and ⟨y,s⟩≠0\langle y,s\rangle\ne0⟨y,s⟩=0, the setting of the Annex's symmetric problem; the paper's sentence before the psb formula repeats the "(A.5)" misprint and is read as (A.6) in the same way.

The definition layer, basis independence, operator-ideal property, bracket results, both least-change propositions, and the Broyden, psb, dfp and positivity statements are welcome proof targets. The scaling results of §4.1 are outside this mission.

Selected references

  • Jean Charles Gilbert and Claude Lemaréchal, Some numerical experiments with variable-storage quasi-Newton algorithms, IIASA Working Paper WP-88-121, August 1988, §2.1 and Annex, printed pp. 3 and 26–30. Working paper PDF.
  • Jean Charles Gilbert and Claude Lemaréchal, Some numerical experiments with variable-storage quasi-Newton algorithms, Mathematical Programming 45 (1989), 407–435. DOI 10.1007/BF01589113. Cited for publication history; all statement indices above follow the working paper.
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Differential GeometryOptimal TransportProbability·Captain: mikedeng1

Bakry–Émery Curvature-Dimension Condition and Riemannian Ricci Curvature Bounds 4: A Riemannian Energy Measure Space Satisfying BE(K,∞) Is an RCD(K,∞) SpaceResearch Paper

Why relate heat flow and curvature?

Heat flow gives an analytic way to describe how functions spread on a space. Optimal transport gives a metric way to describe how probability measures move on the same space. On a smooth Riemannian manifold, a lower Ricci curvature bound constrains both motions. The problem addressed by Ambrosio, Gigli and Savaré is to identify the corresponding relationship when the underlying space need not be a manifold. A Dirichlet form can specify a heat flow even when there are no smooth coordinates, while a Wasserstein distance can measure transport between probability measures. Theorem 4.17 connects these two descriptions for Riemannian energy measure spaces.

The paper proves the implication from the Bakry–Émery condition BE(K,∞)BE(K,\infty)BE(K,∞) to the Riemannian curvature-dimension condition RCD(K,∞)RCD(K,\infty)RCD(K,∞). Its printed theorem is an equivalence; the paper cites the reverse implication from earlier work in the proof on p. 58. This mission targets the implication established here, with the source's exact assumptions.

Setting

Let XXX be a complete, separable metric space with a Borel measure mmm. A Dirichlet form E\mathcal EE assigns a nonnegative energy to square-integrable functions, is quadratic and lower semicontinuous, and decreases under normal contractions. Its associated heat flow PtP_tPt​ evolves a function over time. The associated carré du champ Γ(f)\Gamma(f)Γ(f) measures the energy density of a function. Functions with energy density at most one define an intrinsic distance

dE(x,y)=sup⁡{∣ψ(y)−ψ(x)∣:ψ is continuous and Γ(ψ)≤1 m-a.e.}.d_{\mathcal E}(x,y)=\sup\{|\psi(y)-\psi(x)|:\psi\text{ is continuous and }\Gamma(\psi)\le1\ m\text{-a.e.}\}.dE​(x,y)=sup{∣ψ(y)−ψ(x)∣:ψ is continuous and Γ(ψ)≤1 m-a.e.}.

For the Riemannian energy measure space in this mission, this intrinsic distance is the metric of XXX. The structure also requires the paper's upper regularity and continuous-representative properties. The growth condition (MD.exp)(MD.exp)(MD.exp) controls the measure of large balls. In the BE(K,∞)BE(K,\infty)BE(K,∞) condition, a weak second-derivative inequality for the heat flow has curvature parameter KKK and no finite-dimensional correction term. These assumptions are stated at the start of §4 and govern the §4 milestones even when an individual theorem does not repeat them. See Definitions 3.6 and 3.16 and the opening of §4.

Write P2(X)\mathcal P_2(X)P2​(X) for the probability measures with finite second moment, W2W_2W2​ for their quadratic Wasserstein distance, and Ent⁡m(ρ)\operatorname{Ent}_m(\rho)Entm​(ρ) for entropy relative to mmm. The heat flow has a dual action HtH_tHt​ on measures. The target RCD(K,∞)RCD(K,\infty)RCD(K,∞) asks for a curve HtρH_t\rhoHt​ρ from every ρ∈P2(X)\rho\in\mathcal P_2(X)ρ∈P2​(X) that satisfies the following evolution variational inequality against every ν∈P2(X)\nu\in\mathcal P_2(X)ν∈P2​(X) of finite entropy, at every t>0t>0t>0:

d+dtW22(Htρ,ν)2+K2W22(Htρ,ν)+Ent⁡m(Htρ)≤Ent⁡m(ν).\frac{d^+}{dt}\frac{W_2^2(H_t\rho,\nu)}2 +\frac K2W_2^2(H_t\rho,\nu) +\operatorname{Ent}_m(H_t\rho) \le\operatorname{Ent}_m(\nu).dtd+​2W22​(Ht​ρ,ν)​+2K​W22​(Ht​ρ,ν)+Entm​(Ht​ρ)≤Entm​(ν).

The definition also includes full support, local finiteness, the exponential growth condition, and the length-space property. See Definition 3.1.

Formalization targets

The goal is the forward implication of Theorem 4.17:

Riemannian energy measure space+(MD.exp)+BE(K,∞)⟹RCD(K,∞).\text{Riemannian energy measure space}+(MD.exp)+BE(K,\infty) \quad\Longrightarrow\quad RCD(K,\infty).Riemannian energy measure space+(MD.exp)+BE(K,∞)⟹RCD(K,∞).

Three milestones supply central results from the paper. The final assertions of Theorem 3.17 give the dual measure flow and its absolute continuity after positive time. Corollary 3.18 identifies BE(K,∞)BE(K,\infty)BE(K,∞) with the W2W_2W2​ contraction W2((Ptf)m,(Ptg)m)≤e−KtW2(fm,gm)W_2((P_t f)m,(P_t g)m)\le e^{-Kt}W_2(fm,gm)W2​((Pt​f)m,(Pt​g)m)≤e−KtW2​(fm,gm) on probability densities. A companion item, Theorem 4.8, gives an entropy bound for HtμH_t\muHt​μ when μ\muμ has finite second moment:

Ent⁡m(Htμ)≤r2+∫Xd2(x,x0) dμ(x)2I2K(t)−log⁡m(Br(x0)),r,t>0.\operatorname{Ent}_m(H_t\mu) \le\frac{r^2+\int_X d^2(x,x_0)\,d\mu(x)}{2I_{2K}(t)} -\log m(B_r(x_0)),\qquad r,t>0.Entm​(Ht​μ)≤2I2K​(t)r2+∫X​d2(x,x0​)dμ(x)​−logm(Br​(x0​)),r,t>0.

The third milestone, Theorem 4.16, bounds the distance and entropy at the heat-evolved endpoint of a regular curve ρs\rho_sρs​:

W22(ρ0,Htρ1)+2tEnt⁡m(Htρ1)≤RK(t)2∫01∣ρ˙s∣2 ds+2tEnt⁡m(ρ0),RK(t)=t/IK(t).W_2^2(\rho_0,H_t\rho_1)+2t\operatorname{Ent}_m(H_t\rho_1) \le R_K(t)^2\int_0^1|\dot\rho_s|^2\,ds +2t\operatorname{Ent}_m(\rho_0),\qquad R_K(t)=t/I_K(t).W22​(ρ0​,Ht​ρ1​)+2tEntm​(Ht​ρ1​)≤RK​(t)2∫01​∣ρ˙​s​∣2ds+2tEntm​(ρ0​),RK​(t)=t/IK​(t).

The milestone list follows the source labels and constants in §4.

What the result provides

The conclusion turns an analytic curvature bound on a heat semigroup into a transport statement about entropy on probability measures. It therefore identifies a concrete set of Dirichlet-form hypotheses under which the heat evolution has the metric behavior demanded by RCD(K,∞)RCD(K,\infty)RCD(K,∞). The result applies in the paper's metric measure setting, where the space may lack a smooth tensor calculus. The RCDRCDRCD conclusion carries convergence from every initial measure in P2(X)\mathcal P_2(X)P2​(X) and the inequality for all finite-entropy comparison measures.

The mathematical implication is proved in the cited paper. The proposed Lean statements are open proof targets: their declarations compile with placeholders, and no machine-checked proof of this implication is asserted here. A complete development would connect Dirichlet-form calculus, probability measures, entropy, and Wasserstein geometry in reusable interfaces. The dual-flow and regular-curve definitions are especially useful beyond this theorem.

Main difficulty

The heat flow is initially specified on square-integrable functions, whereas the target is an inequality for probability measures, including measures without an initial density. A bound on Γ(Ptf)\Gamma(P_t f)Γ(Pt​f) by itself controls functions almost everywhere; it does not immediately produce the pointwise dual flow or the right derivative of W22W_2^2W22​ required by Definition 3.1. The action estimate also begins with regular curves, while the target quantifies over every initial measure in P2(X)\mathcal P_2(X)P2​(X). These changes of domain and regularity are the central mathematical obstacles; simply renaming the heat semigroup as a measure flow leaves the target unjustified.

Formalization scope

Lean uses real-valued function representatives for L2(X,m)L^2(X,m)L2(X,m), with almost-everywhere congruence in the Dirichlet form and heat flow. Measures use the Borel sigma algebra. The source uses its mmm-completion; the formalization treats quantities invariant under mmm-almost-everywhere equality, and this convention is explicit in the definition layer. The metric is complete and second countable, and its equality with dEd_{\mathcal E}dE​ is part of the energy-measure-space predicate. A sigma-finiteness instance is carried where entropy or measure operations need it; it follows from the source's measure-growth setting. The dual flow and the L1L^1L1 extension are bound by predicates that specify their action on densities. The mollifier for a regular curve is bound by the conditions of (2.17), while the action is the infimum of squared admissible speeds, which equals the integral of the squared metric derivative.

Wasserstein costs use R≥0∪{∞}\mathbb R_{\ge0}\cup\{\infty\}R≥0​∪{∞}, and entropy uses extended real values. Theorem 4.8 restricts r,tr,tr,t to positive numbers, so the ball mass and I2K(t)I_{2K}(t)I2K​(t) used in its formula have the intended domain. Theorem 4.16 also uses t>0t>0t>0, making RK(t)=t/IK(t)R_K(t)=t/I_K(t)RK​(t)=t/IK​(t) meaningful, including at K=0K=0K=0. The goal requires an EVI flow beginning at each ρ∈P2(X)\rho\in\mathcal P_2(X)ρ∈P2​(X) and the inequality at every positive time; allowing a vacuous flow or checking only almost every time would not express Definition 3.1. Contributions may establish the milestone statements and the companion Theorem 4.8, develop the omitted intermediate estimates from §4, or prove the goal from the source's full argument.

Selected references

  • L. Ambrosio, N. Gigli and G. Savaré, Bakry–Émery curvature-dimension condition and Riemannian Ricci curvature bounds, Annals of Probability 43(1), 2015, 339–404. arXiv:1209.5786v4.
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Optimal TransportProbability·Captain: mikedeng1

Bakry–Émery Curvature-Dimension Condition and Riemannian Ricci Curvature Bounds 3: Lipschitz and Pointwise Gradient Bounds on the Heat Semigroup Make Its Dual Semigroup a W₂ ContractionResearch Paper

Motivation

A lower bound on Ricci curvature can be expressed in two ways that make sense far beyond smooth manifolds. The Eulerian way bounds the gradient of the heat semigroup: Bakry and Émery's Γ2\Gamma_2Γ2​-calculus gives ∣∇Ptf∣2≤e−2Kt Pt∣∇f∣2|\nabla \mathsf P_t f|^2 \le e^{-2Kt}\,\mathsf P_t|\nabla f|^2∣∇Pt​f∣2≤e−2KtPt​∣∇f∣2. The Lagrangian way bounds how heat flow moves probability measures in optimal transport distance: W2(Htμ,Htν)≤e−KtW2(μ,ν)W_2(\mathsf H_t\mu,\mathsf H_t\nu)\le e^{-Kt}W_2(\mu,\nu)W2​(Ht​μ,Ht​ν)≤e−KtW2​(μ,ν). On Riemannian manifolds the two are equivalent (von Renesse–Sturm 2005). Kuwada (2010) showed that the equivalence is a general duality between a pointwise gradient bound with a constant C(t)C(t)C(t) and W2W_2W2​-contraction with the same constant, valid on length metric measure spaces.

Ambrosio, Gigli and Savaré (arXiv:1209.5786v4, Ann. Probab. 2015) needed this duality in a setting with no doubling or Poincaré inequality, where the semigroup comes from an abstract Dirichlet form and is only defined almost everywhere. Their §3.2 builds the dual semigroup on probability measures and proves the contraction (Theorem 3.5). Combined with their Theorem 3.17 it gives Corollary 3.18, the step that links the Bakry–Émery condition BE(K,∞)\mathrm{BE}(K,\infty)BE(K,∞) to W2W_2W2​-contraction and, later in the paper, to RCD(K,∞)\mathrm{RCD}(K,\infty)RCD(K,∞).

Setting

Let (X,d)(X,\mathsf d)(X,d) be a complete separable metric space with a Borel measure mmm of full support such that m(Br(x))<∞m(B_r(x))<\inftym(Br​(x))<∞ for every ball (condition (MD)). The space is a length space if d(x0,x1)\mathsf d(x_0,x_1)d(x0​,x1​) is the infimum of the lengths of curves joining x0x_0x0​ to x1x_1x1​ (3.2).

A Dirichlet form E\mathcal EE on L2(X,m)L^2(X,m)L2(X,m) is a lower semicontinuous quadratic form with dense domain that does not increase under normal contractions; it is strongly local if E(f,g)=0\mathcal E(f,g)=0E(f,g)=0 whenever f+af+af+a and ggg have disjoint supports. Its heat flow (Pt)t≥0(\mathsf P_t)_{t\ge0}(Pt​)t≥0​ solves ddtPtf=ΔEPtf\frac{d}{dt}\mathsf P_tf=\Delta_{\mathcal E}\mathsf P_tfdtd​Pt​f=ΔE​Pt​f in L2L^2L2. It is mass preserving if ∫Ptf dm=∫f dm\int\mathsf P_tf\,dm=\int f\,dm∫Pt​fdm=∫fdm (2.12).

Lipb(X)\mathrm{Lip}_b(X)Lipb​(X) denotes bounded Lipschitz functions, ∣Df∣(x)=lim sup⁡y→x∣f(y)−f(x)∣/d(y,x)|Df|(x)=\limsup_{y\to x}|f(y)-f(x)|/\mathsf d(y,x)∣Df∣(x)=limsupy→x​∣f(y)−f(x)∣/d(y,x) the slope, and P(X)\mathscr P(X)P(X) the Borel probability measures. The Wasserstein cost is

W22(μ,ν)=inf⁡{∫d2(x,y) dγ(x,y): γ a coupling of μ,ν}∈[0,∞].W_2^2(\mu,\nu)=\inf\Big\{\int\mathsf d^2(x,y)\,d\boldsymbol\gamma(x,y):\ \boldsymbol\gamma\text{ a coupling of }\mu,\nu\Big\}\in[0,\infty].W22​(μ,ν)=inf{∫d2(x,y)dγ(x,y): γ a coupling of μ,ν}∈[0,∞].

Two hypotheses on the semigroup, with C:[0,∞)→[0,∞)C:[0,\infty)\to[0,\infty)C:[0,∞)→[0,∞) bounded on every [0,T][0,T][0,T]:

(3.15)Ptf∈Lipb(X),  Lip(Ptf)≤C(t) Lip(f),(3.16)∣DP~tf∣2(x)≤C2(t) P~t∣Df∣2(x),\text{(3.15)}\quad \mathsf P_tf\in\mathrm{Lip}_b(X),\ \ \mathrm{Lip}(\mathsf P_tf)\le C(t)\,\mathrm{Lip}(f),\qquad \text{(3.16)}\quad |D\tilde{\mathsf P}_tf|^2(x)\le C^2(t)\,\tilde{\mathsf P}_t|Df|^2(x),(3.15)Pt​f∈Lipb​(X),  Lip(Pt​f)≤C(t)Lip(f),(3.16)∣DP~t​f∣2(x)≤C2(t)P~t​∣Df∣2(x),

for f∈Lipb(X)∩L2(X,m)f\in\mathrm{Lip}_b(X)\cap L^2(X,m)f∈Lipb​(X)∩L2(X,m). Under (3.15) the map fm↦(Ptf)mfm\mapsto(\mathsf P_tf)mfm↦(Pt​f)m extends uniquely to a weakly continuous dual semigroup Ht:P(X)→P(X)\mathsf H_t:\mathscr P(X)\to\mathscr P(X)Ht​:P(X)→P(X), and P~tf(x)=∫f dHtδx\tilde{\mathsf P}_tf(x)=\int f\,d\mathsf H_t\delta_xP~t​f(x)=∫fdHt​δx​ is the pointwise version of Pt\mathsf P_tPt​ (Proposition 3.2).

Formalization targets

Goal: Theorem 3.5 (forward direction)

Under (MD), the length property, (2.12), (3.15) and (3.16), for every t≥0t\ge0t≥0 and μ,ν∈P(X)\mu,\nu\in\mathscr P(X)μ,ν∈P(X),

W2(Htμ,Htν)≤C(t) W2(μ,ν).W_2(\mathsf H_t\mu,\mathsf H_t\nu)\le C(t)\,W_2(\mu,\nu).W2​(Ht​μ,Ht​ν)≤C(t)W2​(μ,ν).

The constant C(t)C(t)C(t) is left free; the goal is the duality itself, not a particular curvature bound.

Milestones

  • Proposition 3.2 (i): existence and uniqueness of Ht\mathsf H_tHt​, with W(β)(Htμ,Htν)≤(C(t)∨1)W(β)(μ,ν)W_{(\beta)}(\mathsf H_t\mu,\mathsf H_t\nu)\le(C(t)\vee1)W_{(\beta)}(\mu,\nu)W(β)​(Ht​μ,Ht​ν)≤(C(t)∨1)W(β)​(μ,ν) and W1(Htμ,Htν)≤C(t)W1(μ,ν)W_1(\mathsf H_t\mu,\mathsf H_t\nu)\le C(t)W_1(\mu,\nu)W1​(Ht​μ,Ht​ν)≤C(t)W1​(μ,ν).
  • Proposition 3.2 (ii)–(iv): P~t\tilde{\mathsf P}_tP~t​ preserves Cb(X)C_b(X)Cb​(X), agrees mmm-a.e. with Pt\mathsf P_tPt​, satisfies the duality ∫f dHtμ=∫P~tf dμ\int f\,d\mathsf H_t\mu=\int\tilde{\mathsf P}_tf\,d\mu∫fdHt​μ=∫P~t​fdμ, and is continuous at t=0t=0t=0.
  • Lemma 3.3: a Fatou-type upper bound lim sup⁡n∫fn dμn≤∫f dμ\limsup_n\int f_n\,d\mu_n\le\int f\,d\mulimsupn​∫fn​dμn​≤∫fdμ for weakly converging μn\mu_nμn​.
  • Lemma 3.4: for f∈Lipb(X)f\in\mathrm{Lip}_b(X)f∈Lipb​(X) nonnegative with bounded support and the Hopf–Lax map Q1f(x)=inf⁡yf(y)+12d2(y,x)Q_1f(x)=\inf_y f(y)+\tfrac12\mathsf d^2(y,x)Q1​f(x)=infy​f(y)+21​d2(y,x),
P~tQ1f(x)−P~tf(y)≤12C2(t) d2(x,y).\tilde{\mathsf P}_tQ_1f(x)-\tilde{\mathsf P}_tf(y)\le\tfrac12C^2(t)\,\mathsf d^2(x,y).P~t​Q1​f(x)−P~t​f(y)≤21​C2(t)d2(x,y).
  • (3.26): the contraction for Dirac masses, W22(Htδx,Htδy)≤C2(t) d2(x,y)W_2^2(\mathsf H_t\delta_x,\mathsf H_t\delta_y)\le C^2(t)\,\mathsf d^2(x,y)W22​(Ht​δx​,Ht​δy​)≤C2(t)d2(x,y).

Significance

The theorem turns a pointwise, infinitesimal estimate on functions into a global estimate on measures. In the paper, with C(t)=e−KtC(t)=e^{-Kt}C(t)=e−Kt it gives the W2W_2W2​-contraction of the heat flow under BE(K,∞)\mathrm{BE}(K,\infty)BE(K,∞) (Corollary 3.18). That contraction is an ingredient of the identification of the heat flow with the EVIK\mathrm{EVI}_KEVIK​ gradient flow of the entropy (Theorem 4.17). The argument of §3.2 avoids doubling and local Poincaré assumptions on the metric measure space (p. 26), which is what makes it usable for the general Energy measure spaces of the paper.

The result is proved in the literature: in Kuwada's paper, and in the form posed here in §3.2 of the source. As far as a search of the Prove2Me catalogue shows, none of it is formalized: there is no Wasserstein distance on a general metric space, no dual semigroup of a Dirichlet form, and no Hopf–Lax semigroup on metric spaces. The mission asks for formal proofs of the known argument; the dual semigroup, Lemma 3.3 and the Hopf–Lax estimates are reusable on their own.

Difficulty

The semigroup acts on L2L^2L2 classes, while (3.16) and the contraction are statements at every point; the bridge is the pointwise version P~t\tilde{\mathsf P}_tP~t​, which exists only through the dual semigroup and its weak continuity. The direct approach, applying the gradient bound along a geodesic between xxx and yyy, fails because W2W_2W2​ is not a supremum over Lipschitz functions of a linear quantity. The route goes through the quadratic Kantorovich duality and the Hopf–Lax semigroup on a metric space, neither of which is available in Mathlib, and through limits of integrals against varying measures Htδy\mathsf H_t\delta_{y}Ht​δy​. Passing from Dirac masses to arbitrary μ,ν\mu,\nuμ,ν needs a measurable selection of optimal plans.

Formalization scope

  • Elements of L2(X,m)L^2(X,m)L2(X,m) are functions; every predicate is invariant under mmm-a.e. equality. The σ-algebra is Borel rather than its mmm-completion.
  • The heat flow P\mathsf PP and the dual semigroup H\mathsf HH are binders pinned by predicates (IsHeatSemigroup, IsDualSemigroup), not constructions. IsDualSemigroup requires Ht(fm)=(Ptf)m\mathsf H_t(fm)=(\mathsf P_tf)mHt​(fm)=(Pt​f)m for probability densities f∈L1∩L2f\in L^1\cap L^2f∈L1∩L2 and weak continuity on P(X)\mathscr P(X)P(X), which determines Ht\mathsf H_tHt​ on P(X)\mathscr P(X)P(X). Choosing H\mathsf HH as anything else (e.g. the identity) does not satisfy the predicate, so the goal is not trivialized that way. Dropping the length property would change the statement.
  • (3.15) is stated as "every Lipschitz constant KKK of fff gives the Lipschitz constant C(t)KC(t)KC(t)K of a version of Ptf\mathsf P_tfPt​f". (3.16) and the conclusions are in [0,∞][0,\infty][0,∞]; W2W_2W2​ appears squared.
  • Mass preservation is stated on L1∩L2L^1\cap L^2L1∩L2, where the heat flow is pinned.
  • The paper states Theorem 3.5 as an equivalence; only the direction proved there is posed, the converse being cited from Kuwada.
  • The paper prints Lemma 3.4 with an absolute value, which fails at x=yx=yx=y; the one-sided inequality its proof gives, and (3.26) uses, is the stated form.
  • Lemma 3.3 assumes fff integrable; this only excludes the case ∫f dμ=+∞\int f\,d\mu=+\infty∫fdμ=+∞, where the claim is trivial.

Contributions welcome: the quadratic Kantorovich duality on Polish spaces, Hopf–Lax calculus on length spaces, measurable selection of optimal plans, and the portmanteau-type Lemma 3.3.

Selected references

  • L. Ambrosio, N. Gigli, G. Savaré, Bakry–Émery curvature-dimension condition and Riemannian Ricci curvature bounds, Ann. Probab. 43(1), 2015. https://arxiv.org/abs/1209.5786
  • K. Kuwada, Duality on gradient estimates and Wasserstein controls, J. Funct. Anal. 258, 2010. https://doi.org/10.1016/j.jfa.2010.01.010
  • M.-K. von Renesse, K.-T. Sturm, Transport inequalities, gradient estimates, entropy, and Ricci curvature, Comm. Pure Appl. Math. 58, 2005. https://doi.org/10.1002/cpa.20060
  • L. Ambrosio, N. Gigli, G. Savaré, Metric measure spaces with Riemannian Ricci curvature bounded from below, Duke Math. J. 163, 2014. https://arxiv.org/abs/1109.0222
  • D. Bakry, M. Émery, Diffusions hypercontractives, Séminaire de Probabilités XIX, LNM 1123, 1985. https://doi.org/10.1007/BFb0075847
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AnalysisDifferential GeometryProbability·Captain: mikedeng1

Bakry–Émery Curvature-Dimension Condition and Riemannian Ricci Curvature Bounds 2: The Dirichlet Form of an Energy Measure Space Is Twice the Cheeger Energy Iff It Is Upper-RegularResearch Paper

Motivation

There are two standard ways to do analysis on a non-smooth space. The first starts from an energy: a Dirichlet form E\mathcal EE on L2(X,m)L^2(X,m)L2(X,m), its heat semigroup and its carré du champ Γ\GammaΓ. This is the setting of Bakry–Émery Γ\GammaΓ-calculus and of the curvature-dimension condition BE(K,N)BE(K,N)BE(K,N). The second starts from a metric measure space (X,d,m)(X,d,m)(X,d,m): slopes of Lipschitz functions, the Cheeger energy, Wasserstein distances, and the synthetic Ricci bounds CD(K,∞)\mathrm{CD}(K,\infty)CD(K,∞) and RCD(K,∞)\mathrm{RCD}(K,\infty)RCD(K,∞) of Lott–Villani and Sturm.

Moving between the two requires a dictionary. A Dirichlet form defines a distance, the intrinsic distance dEd_{\mathcal E}dE​ (Biroli–Mosco, Sturm). That distance defines a Cheeger energy. The question is whether the energy rebuilt from dEd_{\mathcal E}dE​ is the energy we started from. Ambrosio, Gigli and Savaré answer this in §3.3 of their paper on the Bakry–Émery condition and Riemannian Ricci bounds (arXiv:1209.5786, Ann. Probab. 2015). Their answer is the identification used in the main theorem of the paper, BE(K,∞)⇒RCD(K,∞)BE(K,\infty)\Rightarrow\mathrm{RCD}(K,\infty)BE(K,∞)⇒RCD(K,∞).

Timeline:

  • 1991–1995: Biroli–Mosco and Sturm introduce the intrinsic distance of a strongly local regular Dirichlet form on a locally compact space and prove its length property there ([50, 52] of the paper).
  • 1999: Cheeger defines the energy that now bears his name (GAFA 9).
  • 2014: Ambrosio–Gigli–Savaré identify the minimal weak gradient with Cheeger's relaxed gradient on general metric measure spaces and introduce RCD(K,∞)\mathrm{RCD}(K,\infty)RCD(K,∞) (Invent. Math. 195; Duke 163).
  • 2015: the present paper sets up Energy measure spaces on Polish spaces, without local compactness, and proves Theorems 3.9–3.14.

Setting

Let XXX be a set with a σ-additive measure mmm. A Dirichlet form is a lower semicontinuous quadratic form E:L2(X,m)→[0,∞]\mathcal E:L^2(X,m)\to[0,\infty]E:L2(X,m)→[0,∞] with E(η∘f)≤E(f)\mathcal E(\eta\circ f)\le\mathcal E(f)E(η∘f)≤E(f) for every 1-Lipschitz η\etaη with η(0)=0\eta(0)=0η(0)=0, and with dense domain V={E<∞}\mathbb V=\{\mathcal E<\infty\}V={E<∞}. It is strongly local when E(f,g)=0\mathcal E(f,g)=0E(f,g)=0 whenever (f+a)g=0(f+a)g=0(f+a)g=0 a.e. for a constant aaa. A function f∈Vf\in\mathbb Vf∈V belongs to G\mathbb GG, with carré du champ Γ(f)∈L+1\Gamma(f)\in L^1_+Γ(f)∈L+1​, if E(f,fφ)−12E(f2,φ)=∫Γ(f)φ dm\mathcal E(f,f\varphi)-\frac12\mathcal E(f^2,\varphi)=\int\Gamma(f)\varphi\,dmE(f,fφ)−21​E(f2,φ)=∫Γ(f)φdm for all bounded φ∈V\varphi\in\mathbb Vφ∈V.

Let LC\mathbb L_CLC​ be the set of continuous ψ∈G\psi\in\mathbb Gψ∈G with Γ(ψ)≤1\Gamma(\psi)\le1Γ(ψ)≤1 a.e. The intrinsic distance is

dE(x,y)=sup⁡ψ∈LC∣ψ(y)−ψ(x)∣.d_{\mathcal E}(x,y)=\sup_{\psi\in\mathbb L_C}|\psi(y)-\psi(x)|.dE​(x,y)=ψ∈LC​sup​∣ψ(y)−ψ(x)∣.

An Energy measure space (X,τ,m,E)(X,\tau,m,\mathcal E)(X,τ,m,E) (Definition 3.6) is a strongly local Dirichlet form on a Polish space with a fully supported Borel measure such that dEd_{\mathcal E}dE​ is a finite complete distance inducing τ\tauτ, and a continuous θ≥0\theta\ge0θ≥0 has its truncations Sk∘θS_k\circ\thetaSk​∘θ in L\mathbb LL.

On the metric side, ∣Df∣(x)=lim sup⁡y→x∣f(y)−f(x)∣/d(y,x)|Df|(x)=\limsup_{y\to x}|f(y)-f(x)|/d(y,x)∣Df∣(x)=limsupy→x​∣f(y)−f(x)∣/d(y,x) is the slope, and the Cheeger energy is

Ch(f)=inf⁡{lim inf⁡n12∫∣Dfn∣2 dm: fn∈Lipb(X), fn→f in L2}.\mathrm{Ch}(f)=\inf\Big\{\liminf_n\tfrac12\int|Df_n|^2\,dm:\ f_n\in\mathrm{Lip}_b(X),\ f_n\to f\text{ in }L^2\Big\}.Ch(f)=inf{nliminf​21​∫∣Dfn​∣2dm: fn​∈Lipb​(X), fn​→f in L2}.

Condition (MD) asks that (X,d)(X,d)(X,d) be complete and separable, supp⁡m=X\operatorname{supp}m=Xsuppm=X, and balls have finite measure. Condition (ED) asks that every ψ∈LC\psi\in\mathbb L_Cψ∈LC​ be 1-Lipschitz for ddd (ED.a), and that every Lipschitz ψ\psiψ with ∣Dψ∣≤1|D\psi|\le1∣Dψ∣≤1 and bounded support lie in LC\mathbb L_CLC​ (ED.b). E\mathcal EE is upper-regular (Definition 3.13) if every fff in a dense subset of V\mathbb VV is an L2L^2L2 limit of bounded continuous fn∈Gf_n\in\mathbb Gfn​∈G with bounded upper semicontinuous gn≥Γ(fn)g_n\ge\sqrt{\Gamma(f_n)}gn​≥Γ(fn​)​ and lim sup⁡n∫gn2≤E(f)\limsup_n\int g_n^2\le\mathcal E(f)limsupn​∫gn2​≤E(f).

Formalization targets

Goal: Theorem 3.14

For an Energy measure space,

E(f)=2 Ch(f)∀f∈L2(X,m)⟺E is upper-regular,\mathcal E(f)=2\,\mathrm{Ch}(f)\quad\forall f\in L^2(X,m)\qquad\Longleftrightarrow\qquad\mathcal E\text{ is upper-regular},E(f)=2Ch(f)∀f∈L2(X,m)⟺E is upper-regular,

and in this case G=V\mathbb G=\mathbb VG=V.

Milestones

  • Theorem 3.9: an Energy measure space satisfies (MD) and (ED) for dEd_{\mathcal E}dE​; conversely, a distance with (MD) and (ED) makes the structure an Energy measure space and equals dEd_{\mathcal E}dE​.
  • Theorem 3.10: (X,dE)(X,d_{\mathcal E})(X,dE​) is a length space.
  • Proposition 3.11: if f∈G∩Cbf\in\mathbb G\cap C_bf∈G∩Cb​ and Γ(f)≤ζ2\Gamma(f)\le\zeta^2Γ(f)≤ζ2 with ζ\zetaζ bounded upper semicontinuous, then fff is Lipschitz and ∣D∗f∣≤ζ|D^*f|\le\zeta∣D∗f∣≤ζ.
  • Theorem 3.12: under (MD), (ED.b) holds iff every Lipschitz fff of bounded support has ∣Df∣2≥Γ(f)|Df|^2\ge\Gamma(f)∣Df∣2≥Γ(f); then 2Ch≥E2\mathrm{Ch}\ge\mathcal E2Ch≥E and ∣Dg∣w2≥Γ(g)|Dg|_w^2\ge\Gamma(g)∣Dg∣w2​≥Γ(g).
  • The remaining assertions of Theorem 3.14: Γ(f)=∣Df∣w2\Gamma(f)=|Df|_w^2Γ(f)=∣Df∣w2​ (3.41), density of V∩Lipb\mathbb V\cap\mathrm{Lip}_bV∩Lipb​ in V\mathbb VV, and mass preservation of (Pt)(P_t)(Pt​) under (MD.exp).

Significance

The identification E=2Ch\mathcal E=2\mathrm{Ch}E=2Ch lets every metric notion be applied to an energy structure. Once it holds, the Wasserstein gradient flow of the entropy, the EVIK\mathrm{EVI}_KEVIK​ formulation and RCD(K,∞)\mathrm{RCD}(K,\infty)RCD(K,∞) all make sense for the energy. That is the route by which the paper proves that BE(K,∞)BE(K,\infty)BE(K,∞) on a Riemannian Energy measure space implies RCD(K,∞)\mathrm{RCD}(K,\infty)RCD(K,∞), the converse of the earlier RCD⇒BE\mathrm{RCD}\Rightarrow BERCD⇒BE result. Theorem 3.12 gives the one-sided inequality 2Ch≥E2\mathrm{Ch}\ge\mathcal E2Ch≥E under the single condition (ED.b), and (3.41) says the energy density is the squared minimal weak gradient. Mass preservation is a standing hypothesis of several other results of the paper, and here it comes for free.

All of these results are proved in the paper, partly by citation: the mass-preservation clause rests on [6, Theorem 4.20], and the length property uses a midpoint criterion from Burago–Burago–Ivanov. None of them has a machine-checked proof. Mathlib has no Dirichlet forms, no Cheeger energy and no theory of length spaces built from curve length. This mission produces precise Lean statements of the paper's identification theorem and of the lemmas its proof uses, so that the metric–energy dictionary can be built up and proved one piece at a time.

Difficulty

The inequality 2Ch≥E2\mathrm{Ch}\ge\mathcal E2Ch≥E is the easy direction once (3.32) is available. Proving (3.32) means bounding the energy density of the Hopf–Lax inf-convolution QtfQ_tfQt​f pointwise by D+(x,t)2/t2D^+(x,t)^2/t^2D+(x,t)2/t2. Only finite minima over a countable dense set lie in V\mathbb VV, so the bound has to pass to the limit through the lower semicontinuity (2.10) of Γ\sqrt\GammaΓ​.

The reverse inequality needs the opposite move: from an mmm-a.e. bound Γ(f)≤ζ2\Gamma(f)\le\zeta^2Γ(f)≤ζ2 to a pointwise bound on the metric slope at every point. That step is Proposition 3.11. It needs ζ\zetaζ to be upper semicontinuous and dEd_{\mathcal E}dE​ to be a length distance. Without upper semicontinuity, an a.e. bound says nothing about the slope at a given point. The obvious idea, testing E\mathcal EE against the Lipschitz functions given by (ED.b), produces only lower bounds on E\mathcal EE and cannot give 2Ch≤E2\mathrm{Ch}\le\mathcal E2Ch≤E. That is why upper regularity is the exact condition. The length property (Theorem 3.10) is itself proved by contradiction from a Lipschitz test function built from two disjoint balls. On a space that is not locally compact, this needs a completeness argument rather than Hopf–Rinow.

Formalization scope

Representation. Elements of L2(X,m)L^2(X,m)L2(X,m) are functions X→RX\to\mathbb RX→R. E\mathcal EE is ∞\infty∞ off L2L^2L2, and every predicate is invariant under mmm-a.e. equality. The σ-algebra is Borel (BorelSpace), standing in for its mmm-completion. The topology τ\tauτ is the topology of the metric of XXX, and condition (b) of Definition 3.6 says that this metric equals dEd_{\mathcal E}dE​. Completeness and separability are typeclass binders. The carré du champ is a predicate on a density, never a chosen function. Slopes, dEd_{\mathcal E}dE​, Ch\mathrm{Ch}Ch and curve lengths take values in [0,∞][0,\infty][0,∞]. The curve length is the total variation, which agrees with ∫∣γ˙∣\int|\dot\gamma|∫∣γ˙​∣. The truncation profile SSS of (3.27) is a parameter with the properties the paper fixes. "Dense in V\mathbb VV" means dense for the norm (∥f∥22+E(f))1/2(\|f\|_2^2+\mathcal E(f))^{1/2}(∥f∥22​+E(f))1/2. The minimal weak gradient is required to be nonnegative, which makes its two characterizing conditions determine it. Mass preservation is stated on L1∩L2L^1\cap L^2L1∩L2, with Ptf∈L1P_tf\in L^1Pt​f∈L1 part of the conclusion. In Theorem 3.9 the printed "distance on X×XX\times XX×X" is read as a distance on XXX.

Ruling out trivializations. The Cheeger energy is defined from slopes of bounded Lipschitz functions and never through E\mathcal EE. Upper regularity is Definition 3.13 with a dense approximating set, not the identity E=2Ch\mathcal E=2\mathrm{Ch}E=2Ch.

Infrastructure. A complete development needs carré du champ calculus for strongly local forms (chain rule, (2.9), (2.10)), the Hopf–Lax semigroup on metric spaces, relaxation and minimal weak gradients, and the midpoint characterization of length spaces. Mathlib has none of these, and all of them can be reused beyond this mission. Contributions of any of these pieces, and proofs of individual milestones, are welcome.

Selected references

  • L. Ambrosio, N. Gigli, G. Savaré, Bakry–Émery curvature-dimension condition and Riemannian Ricci curvature bounds, Ann. Probab. 43(1), 339–404, 2015. https://arxiv.org/abs/1209.5786 (v4 cited)
  • L. Ambrosio, N. Gigli, G. Savaré, Calculus and heat flow in metric measure spaces and applications to spaces with Ricci bounds from below, Invent. Math. 195, 289–391, 2014. https://doi.org/10.1007/s00222-013-0456-1
  • L. Ambrosio, N. Gigli, G. Savaré, Metric measure spaces with Riemannian Ricci curvature bounded from below, Duke Math. J. 163, 1405–1490, 2014. https://doi.org/10.1215/00127094-2681605
  • J. Cheeger, Differentiability of Lipschitz functions on metric measure spaces, Geom. Funct. Anal. 9, 428–517, 1999. https://doi.org/10.1007/s000390050094
  • K.-T. Sturm, Analysis on local Dirichlet spaces I. Recurrence, conservativeness and L^p-Liouville properties, J. Reine Angew. Math. 456, 173–196, 1994. https://doi.org/10.1515/crll.1994.456.173
  • N. Bouleau, F. Hirsch, Dirichlet Forms and Analysis on Wiener Space, de Gruyter, 1991. https://doi.org/10.1515/9783110858389
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Differential GeometryOptimal TransportProbability·Captain: mikedeng1

Bakry–Émery Curvature-Dimension Condition and Riemannian Ricci Curvature Bounds 6: BE(K,N) on Riemannian Energy Measure Spaces Is Stable Under Sturm–Gromov–Hausdorff ConvergenceResearch Paper

Motivation

Curvature bounds on a smooth Riemannian manifold control diffusion and the behavior of probability measures. Metric measure spaces extend these questions to limits that need not be smooth. A useful curvature condition must continue to hold when a sequence of spaces converges. Ambrosio, Gigli, and Savaré prove that their analytic Bakry–Émery curvature-dimension condition has this stability property for Riemannian energy measure spaces under Sturm–Gromov–Hausdorff convergence Ambrosio–Gigli–Savaré, Theorem 5.8. The result connects a condition stated through heat flow and Dirichlet forms with convergence stated through distances between probability measures.

The article's §5.2 first defines the convergence of spaces and of functions living in different L2L^2L2 spaces, then states the stability theorem. This order matters: the measure changes with the space, so ordinary convergence of functions on one fixed measured space cannot express the claim Ambrosio–Gigli–Savaré, Definitions 5.4 and 5.6.

Setting

A metric measure space (X,d,m)(X,d,m)(X,d,m) consists of a complete separable metric space (X,d)(X,d)(X,d) and a measure mmm. The class P2(X)\mathcal P_2(X)P2​(X) contains probability measures with finite second moment. The squared Wasserstein distance W22(μ,ν)W_2^2(\mu,\nu)W22​(μ,ν) is the infimum of the mean squared transport cost d(x,y)2d(x,y)^2d(x,y)2 over couplings of μ\muμ and ν\nuν.

A sequence (Xn,dn,mn)(X_n,d_n,m_n)(Xn​,dn​,mn​) Sturm–Gromov–Hausdorff converges to (X∞,d∞,m∞)(X_\infty,d_\infty,m_\infty)(X∞​,d∞​,m∞​) when there is a complete separable ambient metric space ZZZ and distance-preserving embeddings ιn:Xn→Z\iota_n:X_n\to Zιn​:Xn​→Z, including ι∞\iota_\inftyι∞​, such that W2((ιn)#mn,(ι∞)#m∞)→0W_2((\iota_n)_\#m_n,(\iota_\infty)_\#m_\infty)\to0W2​((ιn​)#​mn​,(ι∞​)#​m∞​)→0. The embeddings need not be onto. This definition compares measures on different spaces after placing them in one ambient space; it does not assume that the original spaces coincide Ambrosio–Gigli–Savaré, Definition 5.4.

An energy measure space has a strongly local Dirichlet form E\mathcal EE, its associated heat flow PtP_tPt​, a carré du champ Γ\GammaΓ, and an intrinsic distance dEd_{\mathcal E}dE​ agreeing with ddd. The Cheeger energy Ch⁡m\operatorname{Ch}_mChm​ is the relaxed integral of one half the squared local slope. A Riemannian energy measure space also has the upper-regularity and continuous-representative properties of Definition 3.16. The paper writes E=2Ch⁡m\mathcal E=2\operatorname{Ch}_mE=2Chm​ in this situation Ambrosio–Gigli–Savaré, Definitions 3.6 and 3.16 and Theorem 3.14.

The Bakry–Émery condition BE(K,N)\mathrm{BE}(K,N)BE(K,N) bounds a second-order expression involving the heat flow, the carré du champ, curvature parameter KKK, and dimension parameter NNN. The formalization uses the paper's weak distributional form (2.33), writing ν=1/N≥0\nu=1/N\ge0ν=1/N≥0; ν=0\nu=0ν=0 represents N=∞N=\inftyN=∞. This is the same KKK and NNN for every source space and for the limit Ambrosio–Gigli–Savaré, Definition 2.4 and (2.33).

Formalization targets

Supporting convergence results

Remark 5.5 asserts that the Cheeger energy is invariant under an isometric embedding. Lemma 5.7 supplies two criteria (squared norms, or entropies of bounded densities) for convergence of scalar functions across changing measures and shows that continuous maps of linear growth preserve this convergence. Lemma 5.9 says that, in the RCD setting, both heat-flow outputs and their generators converge. These are the mission's formal milestones Ambrosio–Gigli–Savaré, pp. 63–66.

Stability goal

For Riemannian energy measure spaces (Xn,dn,mn,En)(X_n,d_n,m_n,\mathcal E_n)(Xn​,dn​,mn​,En​) with mn∈P2(Xn)m_n\in\mathcal P_2(X_n)mn​∈P2​(Xn​) and BE(K,N)\mathrm{BE}(K,N)BE(K,N), Theorem 5.8 asks for

(Xn,dn,mn)→SGH(X∞,d∞,m∞)⟹(X∞,d∞,m∞,2Ch⁡m∞) is Riemannian and satisfies BE(K,N).(X_n,d_n,m_n)\xrightarrow{\mathrm{SGH}}(X_\infty,d_\infty,m_\infty) \quad\Longrightarrow\quad (X_\infty,d_\infty,m_\infty,2\operatorname{Ch}_{m_\infty}) \text{ is Riemannian and satisfies }\mathrm{BE}(K,N).(Xn​,dn​,mn​)SGH​(X∞​,d∞​,m∞​)⟹(X∞​,d∞​,m∞​,2Chm∞​​) is Riemannian and satisfies BE(K,N).

The goal includes the assertion that the limit energy is a Dirichlet form; quadraticity is part of the conclusion. It covers finite NNN and N=∞N=\inftyN=∞ with the same statement Ambrosio–Gigli–Savaré, Theorem 5.8.

Significance

The theorem permits analytic curvature-dimension bounds to survive convergence even when the carrier spaces, measures, and L2L^2L2 spaces vary. Without a stability statement, a bound verified separately on approximating spaces would give no such bound for their metric measure limit. The theorem also ensures that the limit Cheeger energy retains the quadratic structure required for the Riemannian theory Ambrosio–Gigli–Savaré, Theorem 5.8 and its proof.

The result is proved in the cited paper. The remaining work here is a machine-checked development of its definitions and proof, including the convergence of heat flows and generator terms across changing measures. The statements in this proposal are proof targets; they are not presented as already machine-checked. The definitions of SGH convergence and graph-law convergence can also support other stability questions for metric measure spaces.

Difficulty

The difficulty is that each PtnP_t^nPtn​ acts on a different L2(Xn,mn)L^2(X_n,m_n)L2(Xn​,mn​), while BE(K,N)\mathrm{BE}(K,N)BE(K,N) is an inequality involving the semigroup, its generator, and integrals against mnm_nmn​. Convergence of the underlying measures alone does not imply convergence of those functions or of their squared terms. In particular, pointwise convergence on a common carrier is not even a statement available before choosing embeddings and representatives. The paper's separate notion of function convergence addresses this gap Ambrosio–Gigli–Savaré, Definitions 5.4 and 5.6 and Lemma 5.9.

Formalization scope

Lean keeps the spaces indexed by nnn: Xn n, m n, E n, and P n. The goal uses SGH convergence as an existential ambient realization, rather than assuming the paper's common-space reduction (5.10). The source heat flows and the truncation profile SSS are named by their defining properties; they are the paper's determined objects. The limit heat flow is not assumed to exist: the BE(K,N)\mathrm{BE}(K,N)BE(K,N) conclusion is stated for every family satisfying the heat-flow characterization of 2Ch⁡m∞2\operatorname{Ch}_{m_\infty}2Chm∞​​. Functions represent L2L^2L2 classes, and the common Setting layer records almost-everywhere invariance. The measurable spaces are Borel; the paper's completed measurable structures are represented through measurable versions and almost-everywhere relations.

The formal goal assumes that m∞m_\inftym∞​ has full support on X∞X_\inftyX∞​. Definition 3.6 requires this, while §5.2 explicitly warns that the ambient SGH limit may fail to be fully supported. The full-support condition makes the theorem refer to the intended limit carrier. The goal does not assume that the limit already is a Riemannian energy measure space or satisfies BE(K,N)\mathrm{BE}(K,N)BE(K,N).

Function convergence uses graph laws on X×RkX\times\mathbb R^kX×Rk. The chosen product metric is Mathlib's max metric; any fixed finite product metric yields the same W2W_2W2​ convergence in this setting. The squared Wasserstein distance is extended nonnegative, so a missing finite coupling does not turn into a false real value. The limit energy is defined as 2Ch⁡m∞2\operatorname{Ch}_{m_\infty}2Chm∞​​, with no free energy parameter. Measurable representatives are explicit when forming pushforwards. Lemma 5.9 is stated on a common, fully supported RCD carrier; this narrows its ambient application and is recorded for review. Contributions to the Cheeger-energy invariance, changing-measure function convergence, heat-flow stability, and final BE passage are all within scope.

Selected references

  • Luigi Ambrosio, Nicola Gigli, Giuseppe Savaré, Bakry–Émery curvature-dimension condition and Riemannian Ricci curvature bounds, Annals of Probability 43(1), 2015, 339–404. arXiv:1209.5786v4, DOI:10.1214/14-AOP907.
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Optimal TransportProbabilityStatistics·Captain: mikedeng1

Computational Optimal Transport XI: For p = 1, 2 the p-Wasserstein Distance on ℝ^d with d ≥ 2 Is Not HilbertianTextbook

Why ask whether a Wasserstein distance is Hilbertian

Kernel methods, multidimensional scaling and low-distortion embeddings all work best on data whose distance comes from a Hilbert space. A distance ddd on a set Z\mathcal ZZ is Hilbertian when Z\mathcal ZZ can be mapped into a Hilbert space so that ddd becomes the norm distance; for such a ddd, the kernel e−dp/te^{-d^p/t}e−dp/t is positive definite for 0≤p≤20\le p\le 20≤p≤2 and t>0t>0t>0 (Berg, Christensen and Ressel, 1984), and the classical Euclidean toolbox applies. Optimal transport distances are popular for comparing probability measures, so it is natural to ask whether they are Hilbertian. In dimension one the answer is yes for W2\mathcal W_2W2​: the map sending a measure to its quantile function is an isometry into L2([0,1])L^2([0,1])L2([0,1]), and between univariate Gaussians W2\mathcal W_2W2​ is the Euclidean distance between (mean, standard deviation). Peyré and Cuturi, Computational Optimal Transport (FnT ML 2019), §8.3, show that this does not extend to the plane: for p=1,2p=1,2p=1,2 and d≥2d\ge2d≥2 the ppp-Wasserstein distance on Rd\mathbb R^dRd is not Hilbertian (Proposition 8.2, p. 507).

The tool is a classical characterization. Schoenberg (1938) proved that a distance is Hilbertian exactly when its square is conditionally negative definite; Berg, Christensen and Ressel (1984, Prop. 3.2) give the modern form. The easy direction turns non-embeddability into a finite check, and the book's proof of Proposition 8.2 performs that check numerically on 35 measures supported on the four corners of the unit square (Figure 8.6, p. 508). Stronger, quantitative statements are known: planar W1\mathcal W_1W1​ does not even embed into L1L^1L1 with bounded distortion (Naor and Schechtman, 2007), and Andoni, Naor and Neiman (2018) study which powers of Wasserstein distances embed.

Setting

Let Z\mathcal ZZ be a set. A function φ:Z×Z→R\varphi:\mathcal Z\times\mathcal Z\to\mathbb Rφ:Z×Z→R is negative definite (Definition 8.3, p. 501, in the conditional form used in §8.3) if it is symmetric and, for every n≥0n\ge0n≥0, every x1,…,xn∈Zx_1,\dots,x_n\in\mathcal Zx1​,…,xn​∈Z and every r∈Rnr\in\mathbb R^nr∈Rn with ∑iri=0\sum_ir_i=0∑i​ri​=0,

∑i,j=1nrirj φ(xi,xj)≤0.\sum_{i,j=1}^n r_ir_j\,\varphi(x_i,x_j)\le0 .i,j=1∑n​ri​rj​φ(xi​,xj​)≤0.

A function d:Z×Z→Rd:\mathcal Z\times\mathcal Z\to\mathbb Rd:Z×Z→R is Hilbertian (Definition 8.4, p. 506) if there are a real Hilbert space H\mathcal HH and a map ϕ:Z→H\phi:\mathcal Z\to\mathcal Hϕ:Z→H with d(z,z′)=∥ϕ(z)−ϕ(z′)∥Hd(z,z')=\|\phi(z)-\phi(z')\|_{\mathcal H}d(z,z′)=∥ϕ(z)−ϕ(z′)∥H​ for all z,z′z,z'z,z′.

On Rd\mathbb R^dRd with the Euclidean norm ∥⋅∥2\|\cdot\|_2∥⋅∥2​, let Pp(Rd)\mathcal P_p(\mathbb R^d)Pp​(Rd) be the Borel probability measures μ\muμ with ∫∥x∥2p dμ<∞\int\|x\|_2^p\,d\mu<\infty∫∥x∥2p​dμ<∞. A coupling of μ\muμ and ν\nuν is a measure π\piπ on Rd×Rd\mathbb R^d\times\mathbb R^dRd×Rd whose two marginals are μ\muμ and ν\nuν, and the ppp-Wasserstein distance (2.18) is

Wp(μ,ν)=(inf⁡π∫∥x−y∥2p dπ(x,y))1/p,\mathcal W_p(\mu,\nu)=\Big(\inf_{\pi}\int\|x-y\|_2^p\,d\pi(x,y)\Big)^{1/p},Wp​(μ,ν)=(πinf​∫∥x−y∥2p​dπ(x,y))1/p,

finite on Pp(Rd)\mathcal P_p(\mathbb R^d)Pp​(Rd). For points x1,…,xnx_1,\dots,x_nx1​,…,xn​ and a histogram a∈Σna\in\Sigma_na∈Σn​ (nonnegative, summing to one) the discrete measure is ∑iaiδxi\sum_ia_i\delta_{x_i}∑i​ai​δxi​​; for two histograms a,ba,ba,b, U(a,b)U(a,b)U(a,b) is the set of nonnegative matrices with row sums aaa and column sums bbb, and LC(a,b)=min⁡P∈U(a,b)∑i,jCi,jPi,jL_C(a,b)=\min_{P\in U(a,b)}\sum_{i,j}C_{i,j}P_{i,j}LC​(a,b)=minP∈U(a,b)​∑i,j​Ci,j​Pi,j​ (2.11).

The configuration of the book's proof consists of the corners x1=[0,0]x^1=[0,0]x1=[0,0], x2=[1,0]x^2=[1,0]x2=[1,0], x3=[0,1]x^3=[0,1]x3=[0,1], x4=[1,1]x^4=[1,1]x4=[1,1] of the unit square, the 35 histograms of Σ4\Sigma_4Σ4​ with entries in {0,14,12,34,1}\{0,\tfrac14,\tfrac12,\tfrac34,1\}{0,41​,21​,43​,1}, and the centering matrix J=In−1n1n,nJ=I_n-\tfrac1n\mathbb 1_{n,n}J=In​−n1​1n,n​.

Formalization targets

Goal: Proposition 8.2

For d≥2d\ge2d≥2 and p∈{1,2}p\in\{1,2\}p∈{1,2},

Wp on Pp(Rd) is not Hilbertian.\mathcal W_p \text{ on } \mathcal P_p(\mathbb R^d) \text{ is not Hilbertian.}Wp​ on Pp​(Rd) is not Hilbertian.

Milestones

  1. Proposition 8.1, proved direction (pp. 506–507): if ddd is Hilbertian then d2d^2d2 is negative definite.
  2. Squared distance (p. 507): Wp2\mathcal W_p^2Wp2​ on Pp(Rd)\mathcal P_p(\mathbb R^d)Pp​(Rd) is not negative definite, d≥2d\ge2d≥2, p=1,2p=1,2p=1,2.
  3. Reduction to the plane (proof of Prop. 8.2): if Wp2\mathcal W_p^2Wp2​ on Pp(Rd)\mathcal P_p(\mathbb R^d)Pp​(Rd), d≥2d\ge2d≥2, were negative definite, so would be Wp2\mathcal W_p^2Wp2​ on Pp(R2)\mathcal P_p(\mathbb R^2)Pp​(R2).
  4. Discrete measures (Remark 2.13, p. 375): Wp(∑iaiδxi,∑jbjδxj)p=LC(a,b)\mathcal W_p\big(\sum_ia_i\delta_{x_i},\sum_jb_j\delta_{x_j}\big)^p=L_C(a,b)Wp​(∑i​ai​δxi​​,∑j​bj​δxj​​)p=LC​(a,b) with Ci,j=∥xi−xj∥2pC_{i,j}=\|x_i-x_j\|_2^pCi,j​=∥xi​−xj​∥2p​.
  5. Centering criterion (proof of Prop. 8.2): a matrix MMM admits a zero-sum rrr with r⊤Mr>0r^\top Mr>0r⊤Mr>0 if and only if JMJJMJJMJ has a positive eigenvalue.
  6. The grid counterexample (proof of Prop. 8.2, Figure 8.6): for p=1,2p=1,2p=1,2 there are grid histograms a1,…,ana^1,\dots,a^na1,…,an and a zero-sum rrr with
∑i,jrirj Wp2(∑kakiδxk,∑kakjδxk)>0.\sum_{i,j}r_ir_j\,\mathcal W_p^2\Big(\sum_k a^i_k\delta_{x^k},\sum_k a^j_k\delta_{x^k}\Big)>0.i,j∑​ri​rj​Wp2​(k∑​aki​δxk​,k∑​akj​δxk​)>0.

Significance

A Hilbertian distance gives positive definite Gaussian and Laplace kernels, Euclidean multidimensional scaling and Johnson–Lindenstrauss dimension reduction for free. Proposition 8.2 says none of these can be obtained for W1\mathcal W_1W1​ or W2\mathcal W_2W2​ on Rd\mathbb R^dRd, d≥2d\ge2d≥2, by an isometric embedding; this is why the literature turned to approximate embeddings, sliced distances and entropic surrogates (pp. 507–508). The negative-definiteness test of milestone 1 is a reusable certificate for non-embeddability of any finite metric.

The result is known, and the book's proof is a floating-point eigenvalue computation. The formal content of this mission is a machine-checked proof with an exact certificate: rational or algebraic Wasserstein distances between explicit discrete measures and an explicit zero-sum vector. As far as this mission is aware, no formal proof of the statement exists in Mathlib or on the platform. Schoenberg's converse is cited by the book and is not part of the mission.

Difficulty

The abstract part is short: expanding ∥ϕ(zi)−ϕ(zj)∥2\|\phi(z_i)-\phi(z_j)\|^2∥ϕ(zi​)−ϕ(zj​)∥2 and using ∑iri=0\sum_ir_i=0∑i​ri​=0 gives milestone 1. The obstacle is the certificate. The book observes that JDp2JJ\mathbf D_p^2JJDp2​J has a positive top eigenvalue (about 1.21.21.2 for p=1p=1p=1 and 0.70.70.7 for p=2p=2p=2), but a proof needs exact transport costs between the chosen measures, each the value of a small linear program whose optimality has to be established (for instance by a dual certificate), together with a vector rrr for which the quadratic form is provably positive. For p=1p=1p=1 the costs involve 2\sqrt22​, the diagonal of the square. A second, separate difficulty is connecting the measure-theoretic Wp\mathcal W_pWp​ to the discrete program (milestone 4) and transporting a counterexample from R2\mathbb R^2R2 into Rd\mathbb R^dRd (milestone 3), both of which require working with couplings as measures on a product space.

Formalization scope

  • Rd\mathbb R^dRd is EuclideanSpace ℝ (Fin d); Wp\mathcal W_pWp​ is the published definition WassersteinDRO.Duality.wassersteinDistance (an [0,∞][0,\infty][0,∞]-valued infimum over all measures with the two marginals, raised to 1/p1/p1/p), converted to a real number. The distance is considered on Pp(Rd)\mathcal P_p(\mathbb R^d)Pp​(Rd), the set where it is finite; outside it the real conversion is a junk 000. The book names no domain; since the counterexample consists of finitely supported measures, the finite computation gives non-Hilbertianity on Pp\mathcal P_pPp​ and on every smaller set containing those measures.
  • Negative definiteness is conditional. Definition 8.3 as printed quantifies over all rrr; under that reading no nonzero squared distance is negative definite, so Proposition 8.1 would be false and "not negative definite" trivially true. The zero-sum condition, used by the book in the proof of Proposition 8.1, is part of the definition; this rules out the trivial formalization.
  • Hilbert spaces are real, complete inner-product spaces in the universe of Z\mathcal ZZ. Indices are 0-based (Fin n). Histograms are real vectors; the reduction milestone is stated for every p≥1p\ge1p≥1.
  • Discrete transport objects (U(a,b)U(a,b)U(a,b), LCL_CLC​) are redefined in this mission's namespace CompOT.NotHilbertian, duplicating chunk II of the series.

Contributions welcome: the forward direction of Schoenberg's characterization, the discrete-measure bridge (reusable wherever discrete optimal transport meets measure-theoretic couplings), the isometric-embedding invariance of Wp\mathcal W_pWp​, and exact certificates for the grid computation.

Selected references

  • G. Peyré and M. Cuturi, Computational Optimal Transport, Foundations and Trends in Machine Learning 11(5–6):355–607, 2019. https://doi.org/10.1561/2200000073
  • I. J. Schoenberg, Metric spaces and positive definite functions, Transactions of the AMS 44(3):522–536, 1938. https://doi.org/10.1090/S0002-9947-1938-1501980-0
  • C. Berg, J. P. R. Christensen and P. Ressel, Harmonic Analysis on Semigroups, Graduate Texts in Mathematics 100, Springer, 1984. https://doi.org/10.1007/978-1-4612-1128-0
  • A. Naor and G. Schechtman, Planar earthmover is not in L1L_1L1​, SIAM Journal on Computing 37(3):804–826, 2007. https://doi.org/10.1137/05064206X
  • A. Andoni, A. Naor and O. Neiman, Snowflake universality of Wasserstein spaces, Annales scientifiques de l'École normale supérieure 51(3):657–700, 2018. https://arxiv.org/abs/1509.08677
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AnalysisProbability·Captain: mikedeng1

Bakry–Émery Curvature-Dimension Condition and Riemannian Ricci Curvature Bounds 1: The Weak, Pointwise and Gradient Forms of the Bakry–Émery Condition BE(K,N) Are EquivalentResearch Paper

Motivation

On a Riemannian manifold, a lower bound Ric≥K\mathrm{Ric}\ge KRic≥K together with a dimension bound NNN can be read off from the heat flow alone. This is the Bakry–Émery curvature-dimension condition BE(K,N)BE(K,N)BE(K,N): Bochner's inequality Γ2(f)≥K Γ(f)+1N(Δf)2\Gamma_2(f)\ge K\,\Gamma(f)+\tfrac1N(\Delta f)^2Γ2​(f)≥KΓ(f)+N1​(Δf)2 for the iterated carré du champ. The condition makes sense for any diffusion: weighted manifolds, infinite-dimensional Gaussian spaces, and limits of manifolds where no Ricci tensor exists. For this reason it is one of the two main routes to synthetic curvature bounds, the other being the optimal-transport conditions of Lott–Villani and Sturm. Bakry–Émery 1985; Bakry–Gentil–Ledoux 2014.

Ambrosio, Gigli and Savaré prove that, on metric measure spaces, BE(K,∞)BE(K,\infty)BE(K,∞) for the Cheeger energy is equivalent to the transport condition RCD(K,∞)RCD(K,\infty)RCD(K,∞). Their first step (§2.2) is to state BE(K,N)BE(K,N)BE(K,N) for an abstract Dirichlet form, in a weak form and under minimal regularity, and to show that the usual ways of writing it are equivalent. That equivalence, Corollary 2.3, is the subject of this mission. Every later section of the paper and the remaining missions of this series use one of its forms. arXiv:1209.5786v4, §2.2, pp. 14–20.

Setting

Let (X,B)(X,\mathcal B)(X,B) be a measurable space with a σ\sigmaσ-additive measure mmm.

  • A symmetric Dirichlet form is a functional E:L2(X,m)→[0,∞]\mathcal E:L^2(X,m)\to[0,\infty]E:L2(X,m)→[0,∞] that is quadratic and L2L^2L2-lower semicontinuous, satisfies E(η∘f)≤E(f)\mathcal E(\eta\circ f)\le\mathcal E(f)E(η∘f)≤E(f) for every 1-Lipschitz η\etaη with η(0)=0\eta(0)=0η(0)=0, and has a dense domain V={f:E(f)<∞}\mathbb V=\{f:\mathcal E(f)<\infty\}V={f:E(f)<∞}.
  • Write E(f,g)\mathcal E(f,g)E(f,g) for its bilinear form and V∞=V∩L∞\mathbb V_\infty=\mathbb V\cap L^\inftyV∞​=V∩L∞.
  • E\mathcal EE is strongly local if E(f,g)=0\mathcal E(f,g)=0E(f,g)=0 whenever (f+a)g=0(f+a)g=0(f+a)g=0 a.e. for some constant aaa.
  • The generator ΔE\Delta_{\mathcal E}ΔE​ is defined by E(f,g)=−∫Xg ΔEf dm\mathcal E(f,g)=-\int_X g\,\Delta_{\mathcal E}f\,dmE(f,g)=−∫X​gΔE​fdm for all g∈Vg\in\mathbb Vg∈V, and the heat flow Pt\mathsf P_tPt​ solves ∂tPtf=ΔEPtf\partial_t\mathsf P_tf=\Delta_{\mathcal E}\mathsf P_tf∂t​Pt​f=ΔE​Pt​f with Ptf→f\mathsf P_tf\to fPt​f→f in L2L^2L2. By contraction, Pt\mathsf P_tPt​ extends to L1(X,m)L^1(X,m)L1(X,m).

For f,g,φ∈V∞f,g,\varphi\in\mathbb V_\inftyf,g,φ∈V∞​ set

Γ[f,g;φ]=12(E(f,gφ)+E(g,fφ)−E(fg,φ)),Γ[f;φ]=Γ[f,f;φ].\Gamma[f,g;\varphi]=\tfrac12\big(\mathcal E(f,g\varphi)+\mathcal E(g,f\varphi)-\mathcal E(fg,\varphi)\big),\qquad \Gamma[f;\varphi]=\Gamma[f,f;\varphi].Γ[f,g;φ]=21​(E(f,gφ)+E(g,fφ)−E(fg,φ)),Γ[f;φ]=Γ[f,f;φ].

By continuity, this extends to f,g∈Vf,g\in\mathbb Vf,g∈V, φ∈V∞\varphi\in\mathbb V_\inftyφ∈V∞​. The set G\mathbb GG consists of those f∈Vf\in\mathbb Vf∈V for which φ↦Γ[f;φ]\varphi\mapsto\Gamma[f;\varphi]φ↦Γ[f;φ] has a density Γ(f)∈L+1(X,m)\Gamma(f)\in L^1_+(X,m)Γ(f)∈L+1​(X,m), the carré du champ. The iterated form is

Γ2[f;φ]=12Γ[f;ΔEφ]−Γ[f,ΔEf;φ].\Gamma_2[f;\varphi]=\tfrac12\Gamma[f;\Delta_{\mathcal E}\varphi]-\Gamma[f,\Delta_{\mathcal E}f;\varphi].Γ2​[f;φ]=21​Γ[f;ΔE​φ]−Γ[f,ΔE​f;φ].

Along the heat flow, for t>0t>0t>0 and s∈[0,t]s\in[0,t]s∈[0,t], set

At[f;φ](s)=12 ⁣∫X(Pt−sf)2Psφ dm,AtΔ[f;φ](s)=12 ⁣∫X(ΔEPt−sf)2Psφ dm,\mathsf A_t[f;\varphi](s)=\tfrac12\!\int_X(\mathsf P_{t-s}f)^2\mathsf P_s\varphi\,dm,\qquad \mathsf A^\Delta_t[f;\varphi](s)=\tfrac12\!\int_X(\Delta_{\mathcal E}\mathsf P_{t-s}f)^2\mathsf P_s\varphi\,dm,At​[f;φ](s)=21​∫X​(Pt−s​f)2Ps​φdm,AtΔ​[f;φ](s)=21​∫X​(ΔE​Pt−s​f)2Ps​φdm,

Bt[f;φ](s)=Γ[Pt−sf;Psφ]\mathsf B_t[f;\varphi](s)=\Gamma[\mathsf P_{t-s}f;\mathsf P_s\varphi]Bt​[f;φ](s)=Γ[Pt−s​f;Ps​φ] and Ct[f;φ](s)=Γ2[Pt−sf;Psφ]\mathsf C_t[f;\varphi](s)=\Gamma_2[\mathsf P_{t-s}f;\mathsf P_s\varphi]Ct​[f;φ](s)=Γ2​[Pt−s​f;Ps​φ]. Finally IK(t)=∫0teKsdsI_K(t)=\int_0^te^{Ks}dsIK​(t)=∫0t​eKsds, IK,2(t)=∫0tIK(s)dsI_{K,2}(t)=\int_0^tI_K(s)dsIK,2​(t)=∫0t​IK​(s)ds, and ν=1/N≥0\nu=1/N\ge0ν=1/N≥0.

Formalization targets

Goal: Corollary 2.3

Let K∈RK\in\mathbb RK∈R and ν≥0\nu\ge0ν≥0. The following are equivalent:

  • (i) Γ2[f;φ]≥KΓ[f;φ]+ν∫X(ΔEf)2φ dm\Gamma_2[f;\varphi]\ge K\Gamma[f;\varphi]+\nu\int_X(\Delta_{\mathcal E}f)^2\varphi\,dmΓ2​[f;φ]≥KΓ[f;φ]+ν∫X​(ΔE​f)2φdm for every (f,φ)∈D(Γ2)(f,\varphi)\in D(\Gamma_2)(f,φ)∈D(Γ2​) with φ≥0\varphi\ge0φ≥0;
  • (ii) Ct[f;φ](s)≥KBt[f;φ](s)+2νAtΔ[f;φ](s)\mathsf C_t[f;\varphi](s)\ge K\mathsf B_t[f;\varphi](s)+2\nu\mathsf A^\Delta_t[f;\varphi](s)Ct​[f;φ](s)≥KBt​[f;φ](s)+2νAtΔ​[f;φ](s) for 0≤s<t0\le s<t0≤s<t;
  • (iii) the distributional inequality
∂s2At[f;φ]≥2K ∂sAt[f;φ]+4ν AtΔ[f;φ]in D′(0,t);\partial_s^2\mathsf A_t[f;\varphi]\ge2K\,\partial_s\mathsf A_t[f;\varphi]+4\nu\,\mathsf A^\Delta_t[f;\varphi]\quad\text{in }\mathscr D'(0,t);∂s2​At​[f;φ]≥2K∂s​At​[f;φ]+4νAtΔ​[f;φ]in D′(0,t);
  • (iv) Ptf∈G\mathsf P_tf\in\mathbb GPt​f∈G and I2K(t)Γ(Ptf)+2νI2K,2(t)(ΔEPtf)2≤12Pt(f2)−12(Ptf)2I_{2K}(t)\Gamma(\mathsf P_tf)+2\nu I_{2K,2}(t)(\Delta_{\mathcal E}\mathsf P_tf)^2\le\tfrac12\mathsf P_t(f^2)-\tfrac12(\mathsf P_tf)^2I2K​(t)Γ(Pt​f)+2νI2K,2​(t)(ΔE​Pt​f)2≤21​Pt​(f2)−21​(Pt​f)2 a.e.;
  • (v) G=V\mathbb G=\mathbb VG=V and, for f∈Vf\in\mathbb Vf∈V, t>0t>0t>0, 12Pt(f2)−12(Ptf)2+2νI−2K,2(t)(ΔEPtf)2≤I−2K(t)PtΓ(f)\tfrac12\mathsf P_t(f^2)-\tfrac12(\mathsf P_tf)^2+2\nu I_{-2K,2}(t)(\Delta_{\mathcal E}\mathsf P_tf)^2\le I_{-2K}(t)\mathsf P_t\Gamma(f)21​Pt​(f2)−21​(Pt​f)2+2νI−2K,2​(t)(ΔE​Pt​f)2≤I−2K​(t)Pt​Γ(f) a.e.;
  • (vi) G\mathbb GG is dense in L2L^2L2, and for f∈Gf\in\mathbb Gf∈G, t>0t>0t>0,
Γ(Ptf)+2νI−2K(t)(ΔEPtf)2≤e−2KtPtΓ(f)a.e.\Gamma(\mathsf P_tf)+2\nu I_{-2K}(t)(\Delta_{\mathcal E}\mathsf P_tf)^2\le e^{-2Kt}\mathsf P_t\Gamma(f)\quad\text{a.e.}Γ(Pt​f)+2νI−2K​(t)(ΔE​Pt​f)2≤e−2KtPt​Γ(f)a.e.

Any of them implies G=V\mathbb G=\mathbb VG=V. Condition (iii) is the paper's definition of BE(K,N)BE(K,N)BE(K,N) (Definition 2.4).

Milestones

  1. Lemma 2.1, in four parts:
    • A\mathsf AA is continuous, AΔ\mathsf A^\DeltaAΔ is continuous, and ∂sA=B\partial_s\mathsf A=\mathsf B∂s​A=B (2.25);
    • A\mathsf AA and AΔ\mathsf A^\DeltaAΔ are monotone for φ≥0\varphi\ge0φ≥0;
    • ∂sB=2C\partial_s\mathsf B=2\mathsf C∂s​B=2C (2.26).
  2. Lemma 2.2: four equivalent forms of the scalar inequality a′′≥2Ka′+νga''\ge2Ka'+\nu ga′′≥2Ka′+νg.
  3. Its integrated consequences (2.30) and (2.31).

Significance

The result. Condition (i) is the classical Bochner inequality. (iii) is the form that survives limits and is used as a definition. (iv), (v) and (vi) are pointwise estimates for the heat flow: the reverse and the local Poincaré inequalities, and the Bakry–Émery gradient bound Γ(Ptf)≤e−2KtPtΓ(f)\Gamma(\mathsf P_tf)\le e^{-2Kt}\mathsf P_t\Gamma(f)Γ(Pt​f)≤e−2KtPt​Γ(f). Section 3 of the paper uses (vi) to obtain Lipschitz regularization and to identify the intrinsic distance. Section 4 uses (iii) with ν=0\nu=0ν=0 to prove the RCD(K,∞)RCD(K,\infty)RCD(K,∞) property. The conclusion G=V\mathbb G=\mathbb VG=V means that a BEBEBE form automatically admits a carré du champ on its whole domain, so Γ\GammaΓ-calculus is available without extra assumptions.

Formalizing it. The equivalences are classical for smooth diffusions with an algebra of nice functions. The paper's contribution is to prove them for an arbitrary strongly local Dirichlet form, where no such algebra is assumed. The result is proved; it is not formalized. The mission produces a Lean interface for Dirichlet forms, their heat flows, the extended Γ\GammaΓ and Γ2\Gamma_2Γ2​, and the six conditions. Proofs of the milestones and of the goal are open.

Difficulty

The obvious argument differentiates s↦At[f;φ](s)s\mapsto\mathsf A_t[f;\varphi](s)s↦At​[f;φ](s) twice and reads off A′′=2Γ2\mathsf A''=2\Gamma_2A′′=2Γ2​. That requires fff, φ\varphiφ and ΔEφ\Delta_{\mathcal E}\varphiΔE​φ to be smooth enough for every term to be defined. For a general f∈L2f\in L^2f∈L2 only the first derivative exists, as Γ[⋅;⋅]\Gamma[\cdot;\cdot]Γ[⋅;⋅] on V×V∞\mathbb V\times\mathbb V_\inftyV×V∞​, and only through the continuity extension (2.20). The weak forms must therefore be reached by truncation and semigroup mollification.

The passage from the integrated inequality (iv) to the existence of the density Γ(Ptf)\Gamma(\mathsf P_tf)Γ(Pt​f) is not a computation either. It needs a Daniell-type construction of a measure from a positive functional on V∞\mathbb V_\inftyV∞​. The converse directions, from (iv) or (vi) back to (iii), require a second-order Taylor expansion in time of quantities whose regularity is only that of Lemma 2.1.

Formalization scope

  • Representation. An element of L2L^2L2 is a function with MemLp f 2 m, and every predicate is invariant under a.e. equality. E\mathcal EE takes values in [0,∞][0,\infty][0,∞], with ∞\infty∞ off L2L^2L2. The completion of B\mathcal BB is not modelled.
  • Binders. The heat flow and its L1L^1L1 extension are binders, pinned by characterizing predicates. Generator values and carré du champ densities are witnesses, which are unique a.e.
  • Γ and Γ₂. They are predicates "the value is ccc": approximating sequences exist, and along each of them Γ\GammaΓ converges to ccc. The paper defines Γ\GammaΓ only on V×V×V∞\mathbb V\times\mathbb V\times\mathbb V_\inftyV×V×V∞​, so Γ2[f;φ]\Gamma_2[f;\varphi]Γ2​[f;φ] is undefined when ΔEφ∉V\Delta_{\mathcal E}\varphi\notin\mathbb VΔE​φ∈/V, and (i)–(ii) are required wherever it is defined.
  • Weak forms. Distributional inequalities are tested against nonnegative smooth functions compactly supported in (0,t)(0,t)(0,t), after integration by parts. This avoids derivatives at points where none exists.
  • Standing assumptions and constants. The strong locality and density assumptions of (2.1) are standing binders; there is no topology and no mass preservation. K∈RK\in\mathbb RK∈R is free and ν≥0\nu\ge0ν≥0. IKI_KIK​ is defined by its integral, so K=0K=0K=0 needs no separate case.
  • Departures from the page.
    • In condition (v) the coefficient of PtΓ(f)\mathsf P_t\Gamma(f)Pt​Γ(f) is I−2K(t)I_{-2K}(t)I−2K​(t). The page prints I−2K,2(t)I_{-2K,2}(t)I−2K,2​(t), which makes (v) false for small ttt already for the heat flow on R\mathbb RR; the paper's derivation of (v) from (2.31) gives I−2K(t)I_{-2K}(t)I−2K​(t). (v) is stated for t>0t>0t>0; at t=0t=0t=0 both sides vanish.
    • In Lemma 2.2 (iii), test functions are required to be nonnegative, since (2.27) fails for −ζ-\zeta−ζ.
    • In Lemma 2.2 (iv), s2<ts_2<ts2​<t is required.
  • Not a trivialization. The admissible test classes are nonempty, the conditions are not vacuous, and the hypotheses are satisfiable: the zero form with the identity flow satisfies them and BE(K,∞)BE(K,\infty)BE(K,∞) for every KKK, verified in Lean.
  • Shared layer. The setting module carries the paper's metric-measure definitions for the series and is reusable for any Dirichlet-form development, as is the interval lemma 2.2.

Proofs of any milestone are welcome. Each proved milestone is usable independently: Lemma 2.2, (2.30) and (2.31) are real-variable statements.

Selected references

  • L. Ambrosio, N. Gigli, G. Savaré, Bakry–Émery curvature-dimension condition and Riemannian Ricci curvature bounds, Ann. Probab. 43(1), 339–404, 2015. Pinned preprint arXiv:1209.5786v4, §2, pp. 10–20.
  • D. Bakry, M. Émery, Diffusions hypercontractives, Séminaire de Probabilités XIX, Lecture Notes in Math. 1123, 1985. https://doi.org/10.1007/BFb0075847
  • D. Bakry, I. Gentil, M. Ledoux, Analysis and Geometry of Markov Diffusion Operators, Springer, 2014. https://doi.org/10.1007/978-3-319-00227-9
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Partial Differential EquationsProbability·Captain: mikedeng1

From Nonlinear Fokker-Planck Equations to Solutions of Distribution Dependent SDE: Density-Dependent McKean–Vlasov SDEs Have Weak Solutions Whose Marginals Solve the Nonlinear FPEResearch Paper

Motivation

A McKean–Vlasov stochastic differential equation, or distribution dependent SDE, is an SDE whose coefficients depend on the law of the solution itself:

dX(t)=b(t,X(t),LX(t)) dt+σ(t,X(t),LX(t)) dW(t),dX(t) = b\big(t, X(t), \mathcal L_{X(t)}\big)\,dt + \sigma\big(t, X(t), \mathcal L_{X(t)}\big)\,dW(t),dX(t)=b(t,X(t),LX(t)​)dt+σ(t,X(t),LX(t)​)dW(t),

where LX(t)\mathcal L_{X(t)}LX(t)​ is the law of X(t)X(t)X(t). Such equations describe the limit of large systems of interacting particles (mean-field limits), and they are the probabilistic side of nonlinear Fokker–Planck equations: by Itô's formula the time marginals μt=LX(t)\mu_t = \mathcal L_{X(t)}μt​=LX(t)​ solve a Fokker–Planck equation whose coefficients depend on μt\mu_tμt​.

Most existence theory for McKean–Vlasov SDEs assumes that the coefficients are continuous, often Lipschitz, in the measure argument for a Wasserstein distance. That excludes the Nemytskii-type dependence b(X(t),u(t,X(t)))b(X(t), u(t, X(t)))b(X(t),u(t,X(t))), where u(t,⋅)u(t,\cdot)u(t,⋅) is the density of LX(t)\mathcal L_{X(t)}LX(t)​ evaluated at the current position. This dependence appears in models of nonlinear diffusion and porous media, where the diffusion speed depends on the local concentration. V. Barbu and M. Röckner (arXiv:1808.10706, Ann. Probab. 2020) reverse the usual direction: they first solve the nonlinear Fokker–Planck equation in L1L^1L1 by nonlinear semigroup theory and then construct the SDE from its solution.

Earlier results covered the case aij(x,u)=δijβ(u)a_{ij}(x,u) = \delta_{ij}\beta(u)aij​(x,u)=δij​β(u), as recorded in Remark 4.2 of the paper. Benachour, Chassaing, Roynette and Vallois (Ann. Sc. Norm. Sup. Pisa, 1996) treated d=1d = 1d=1, b≡0b \equiv 0b≡0, β(r)=r∣r∣m−1\beta(r) = r|r|^{m-1}β(r)=r∣r∣m−1. Blanchard, Röckner and Russo (Ann. Probab. 38, 2010) and Barbu, Röckner and Russo (Probab. Theory Relat. Fields, 2011) treated d=1d = 1d=1, b≡0b \equiv 0b≡0 with irregular β\betaβ, the latter in the degenerate case. Barbu and Röckner (SIAM J. Math. Anal. 50, 2018) treated a maximal monotone β\betaβ with a drift b(u)b(u)b(u) satisfying (H3)′.

Setting

Let d≥1d \ge 1d≥1, x∈Rdx \in \mathbb R^dx∈Rd, and let aij,bi:Rd×R→Ra_{ij}, b_i : \mathbb R^d \times \mathbb R \to \mathbb Raij​,bi​:Rd×R→R, 1≤i,j≤d1 \le i,j \le d1≤i,j≤d. The nonlinear Fokker–Planck equation (3.1) is

∂u∂t−∑i,j=1dDij2(aij(x,u)u)+div⁡(b(x,u)u)=0,u(0,⋅)=u0.\frac{\partial u}{\partial t} - \sum_{i,j=1}^d D^2_{ij}\big(a_{ij}(x,u)u\big) + \operatorname{div}\big(b(x,u)u\big) = 0, \qquad u(0,\cdot) = u_0 .∂t∂u​−i,j=1∑d​Dij2​(aij​(x,u)u)+div(b(x,u)u)=0,u(0,⋅)=u0​.

Two sets of hypotheses are considered. (H1)–(H3) (nondegenerate): aija_{ij}aij​ is C2C^2C2, bounded, with bounded xxx-gradient, symmetric; ∑i,j(aij+u ∂uaij)ξiξj≥γ∣ξ∣2\sum_{i,j}(a_{ij} + u\,\partial_ua_{ij})\xi_i\xi_j \ge \gamma|\xi|^2∑i,j​(aij​+u∂u​aij​)ξi​ξj​≥γ∣ξ∣2 for some γ>0\gamma > 0γ>0; bib_ibi​ is bounded, C1C^1C1, and bi(x,0)=0b_i(x,0) = 0bi​(x,0)=0. (H1)′–(H3)′ (degenerate): the coefficients do not depend on xxx, and the quadratic form above is only nonnegative.

The equation is written as an evolution equation u′+Au=0u' + Au = 0u′+Au=0 in L1(Rd)L^1(\mathbb R^d)L1(Rd), with the operator Au=−∑i,jDij2(aij(x,u)u)+div⁡(b(x,u)u)Au = -\sum_{i,j}D^2_{ij}(a_{ij}(x,u)u) + \operatorname{div}(b(x,u)u)Au=−∑i,j​Dij2​(aij​(x,u)u)+div(b(x,u)u) taken in the sense of distributions and domain D(A)={u∈L1:Au∈L1}D(A) = \{u \in L^1 : Au \in L^1\}D(A)={u∈L1:Au∈L1}. An operator is m-accretive if I+λAI + \lambda AI+λA is onto with a contractive inverse for every λ>0\lambda > 0λ>0. A mild solution is the uniform limit of the implicit Euler scheme uhi+hAuhi=uhi−1u_h^i + hAu_h^i = u_h^{i-1}uhi​+hAuhi​=uhi−1​. The paper calls a mild solution a weak solution of (3.1).

The SDE of the main theorem is

dX(t)=b(X(t),u(t,X(t))) dt+2 σ(X(t),u(t,X(t))) dW(t),0≤t≤T,u(t,⋅)=dLX(t)dx,(4.1)dX(t) = b\big(X(t), u(t,X(t))\big)\,dt + \sqrt2\,\sigma\big(X(t), u(t,X(t))\big)\,dW(t), \quad 0 \le t \le T, \qquad u(t,\cdot) = \frac{d\mathcal L_{X(t)}}{dx}, \tag{4.1}dX(t)=b(X(t),u(t,X(t)))dt+2​σ(X(t),u(t,X(t)))dW(t),0≤t≤T,u(t,⋅)=dxdLX(t)​​,(4.1)

with σ:Rd×R→L(Rd;Rd)\sigma : \mathbb R^d \times \mathbb R \to L(\mathbb R^d;\mathbb R^d)σ:Rd×R→L(Rd;Rd) measurable and a=σσTa = \sigma\sigma^Ta=σσT.

Formalization targets

Goal: Theorem 4.1

If a=σσTa = \sigma\sigma^Ta=σσT and bbb satisfy (H1)–(H3) or (H1)′–(H3)′ and u0u_0u0​ is a probability density, then (3.1) has a mild solution uuu with u(0)=u0u(0) = u_0u(0)=u0​, and for every T>0T > 0T>0 there is a weak solution XXX of (4.1) on [0,T][0,T][0,T] with

P∘X(t)−1(dx)=u(t,x) dx,0≤t≤T.P \circ X(t)^{-1}(dx) = u(t,x)\,dx, \qquad 0 \le t \le T .P∘X(t)−1(dx)=u(t,x)dx,0≤t≤T.

Milestones

  • The PDE layer for (H1)–(H3): Lemmas 3.2 and 3.3 (approximate and H1H^1H1 solutions of the resolvent equation under the extra smoothness (K)), the L1L^1L1 contraction (3.22), Proposition 3.1 (the resolvent equation in L1L^1L1, with contraction, positivity and mass conservation), density of D(A)D(A)D(A), m-accretivity of AAA, and Theorem 3.4 (existence and uniqueness of the mild solution, properties (3.36)–(3.39)), including preservation of probability densities.
  • The cited Crandall–Liggett theorem: an m-accretive operator generates a contraction semigroup of mild solutions.
  • The PDE layer for (H1)′–(H3)′: Lemma 3.6, the resolvent properties (3.52)–(3.54), Theorem 3.7.
  • The general scheme of §2: a weakly continuous probability solution of a linear Fokker–Planck equation with bounded coefficients is the marginal flow of a weak solution of the corresponding SDE.

Significance

The theorem gives weak existence for a class of distribution dependent SDEs whose coefficients are not continuous in the measure for any weak or Wasserstein topology: they are defined only on measures with a density and read that density at one point. The same construction gives a probabilistic representation of the nonlinear Fokker–Planck equation, which identifies its solutions as one-dimensional time marginals of a stochastic process and is the starting point for particle approximations.

The proofs are written in the literature. This mission formalizes them: the L1L^1L1 theory of a quasilinear elliptic operator in divergence form, the Crandall–Liggett generation theorem, and the passage from a Fokker–Planck solution to an SDE through the superposition principle. None of these is in Mathlib. The m-accretive operator layer and the superposition step are reusable well beyond this paper.

Difficulty

The natural first idea, a fixed point on the measure argument as in the Lipschitz McKean–Vlasov theory, fails: the map μ↦b(x,dμdx(x))\mu \mapsto b(x, \frac{d\mu}{dx}(x))μ↦b(x,dxdμ​(x)) is not continuous in any topology for which the law map of an SDE is compact, and it is not even defined at measures without density. The paper therefore solves the PDE first. There the obstacle is that AAA is nonlinear in the highest-order term and, under (H1)′–(H3)′, degenerate. Its resolvent has to be built from H1H^1H1 solutions on balls under extra smoothness. Its L1L^1L1 contraction comes from a sign-function argument that needs the monotonicity of u↦aij(x,u)uu \mapsto a_{ij}(x,u)uu↦aij​(x,u)u. Approximation arguments then remove (K) and the nondegeneracy. On the SDE side, the superposition principle needs a solution of the linear equation that is weakly continuous and consists of probability measures. Mass conservation and positivity of the semigroup supply exactly that.

Formalization scope

Rd\mathbb R^dRd is EthierKurtz.SDEState d, with indices Fin d (0-based) and Lebesgue measure volume. L1L^1L1 is MeasureTheory.Lp ℝ 1 volume. Coefficients are functions aij(x,r)a_{ij}(x,r)aij​(x,r), bi(x,r)b_i(x,r)bi​(x,r) of the point and of a real number. The degenerate case uses coefficients constant in xxx, and the operator A1A_1A1​ of (3.42) is then literally AAA. Operators are graphs X → X → Prop, and no resolvent is ever chosen. Mild solutions require that the Euler scheme can be run for all small steps, so the notion is not vacuous. Distributional derivatives are always moved onto smooth compactly supported test functions. H1H^1H1 uses the published weak derivative HunterPDE.Shared.HasWeakDeriv, and H01(BN)H^1_0(B_N)H01​(BN​) means "in H1(Rd)H^1(\mathbb R^d)H1(Rd) and zero outside BNB_NBN​". The SDE is the published EthierKurtz.IsWeakSDESolution on [0,∞)[0,\infty)[0,∞) with coefficients switched off after TTT. Its coefficients are evaluated on a jointly measurable version u~(t,x)\tilde u(t,x)u~(t,x) of the density, which must equal the law of X(t)X(t)X(t).

Deviations from the page, all disclosed in the statements:

  • a=σσTa = \sigma\sigma^Ta=σσT, not the printed 2σσT2\sigma\sigma^T2σσT. With noise 2σ\sqrt2\sigma2​σ the printed factor makes the theorem false (for d=1d = 1d=1, σ≡1/2\sigma \equiv 1/\sqrt2σ≡1/2​, b≡0b \equiv 0b≡0 the PDE has variance 2t2t2t and the SDE variance ttt).
  • In Lemmas 3.2 and 3.3 the explicit λ0=γ(b∞2+c∞2)−1\lambda_0 = \gamma(b_\infty^2 + c_\infty^2)^{-1}λ0​=γ(b∞2​+c∞2​)−1 is replaced by the existence of some λ0>0\lambda_0 > 0λ0​>0; (3.22) keeps the printed λ0\lambda_0λ0​, read as +∞+\infty+∞ when b∞=c∞=0b_\infty = c_\infty = 0b∞​=c∞​=0.
  • In §2 the coefficients are bounded instead of satisfying the integrability Hypothesis 2.1 (ii), and any measurable σˉ\bar\sigmaσˉ with σˉσˉT=aˉ\bar\sigma\bar\sigma^T = \bar aσˉσˉT=aˉ is allowed.
  • The typos "Cb(Rd×Rd)C_b(\mathbb R^d\times\mathbb R^d)Cb​(Rd×Rd)" in (H1) and "C1(Rd)C^1(\mathbb R^d)C1(Rd)" in (H3)′ are read as Cb(Rd×R)C_b(\mathbb R^d\times\mathbb R)Cb​(Rd×R) and C1(R)C^1(\mathbb R)C1(R).

A trivializing formalization is ruled out: the goal asserts the existence of the mild solution as well as the SDE for every mild solution, a mild solution must come from a run of the scheme, and the constant CCC of Lemma 3.3 is fixed before the data. Contributions are welcome at every layer, especially general results on m-accretive operators and the Crandall–Liggett theorem, L1L^1L1 estimates for quasilinear elliptic equations, and the superposition principle.

Selected references

  • V. Barbu, M. Röckner, From nonlinear Fokker–Planck equations to solutions of distribution dependent SDE, Ann. Probab. 48(4), 2020; arXiv:1808.10706v4. https://arxiv.org/abs/1808.10706
  • V. Barbu, M. Röckner, Probabilistic representation for solutions to nonlinear Fokker–Planck equations, SIAM J. Math. Anal. 50, 2588–2607, 2018.
  • Ph. Blanchard, M. Röckner, F. Russo, Probabilistic representation for solutions of an irregular porous media type equation, Ann. Probab. 38, 1870–1900, 2010.
  • V. Barbu, Nonlinear Differential Equations of Monotone Type in Banach Spaces, Springer, 2010. https://doi.org/10.1007/978-1-4419-5542-5
  • M. G. Crandall, T. M. Liggett, Generation of semi-groups of nonlinear transformations on general Banach spaces, Amer. J. Math. 93, 1971. https://doi.org/10.2307/2373376
  • D. Trevisan, Well-posedness of multidimensional diffusion processes with weakly differentiable coefficients, Electron. J. Probab. 21, 2016. https://doi.org/10.1214/16-EJP4453
  • D. W. Stroock, S. R. S. Varadhan, Multidimensional Diffusion Processes, Springer, 1979. https://doi.org/10.1007/3-540-28999-2
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Convex OptimizationDynamical SystemsOperations Research+1·Captain: mikedeng1

Tikhonov Regularization of a Second Order Dynamical System with Hessian Driven Damping 3: If ∫ ε(t)/t dt = +∞, the Trajectory Converges Strongly in the Ergodic Sense to the Minimum-Norm MinimizerResearch Paper

Motivation

Second order dynamical systems with vanishing damping are continuous-time models of accelerated first-order methods. The system x¨+αtx˙+∇g(x)=0\ddot x + \frac{\alpha}{t}\dot x + \nabla g(x) = 0x¨+tα​x˙+∇g(x)=0 is the continuous limit of Nesterov's accelerated gradient method (Su, Boyd, Candès 2016), and its trajectories converge weakly to a minimizer of a convex ggg when α>3\alpha>3α>3 (Attouch, Chbani, Peypouquet, Redont 2018). Two modifications of this system have been studied separately. A Hessian-driven damping term β∇2g(x)x˙\beta\nabla^2 g(x)\dot xβ∇2g(x)x˙ damps oscillations and keeps the fast rates (Attouch, Peypouquet, Redont 2016). A Tikhonov regularization term ϵ(t)x\epsilon(t)xϵ(t)x with ϵ(t)→0\epsilon(t)\to0ϵ(t)→0 selects one minimizer, the one of minimum norm, and can turn weak convergence into strong convergence (Attouch, Chbani, Riahi 2018).

Boţ, Csetnek and László (arXiv:1911.12845v2, Math. Program. 2021) study the system with both terms. Their results split into two regimes according to how fast ϵ\epsilonϵ decays. This mission covers the slow-decay regime of §4.1, where ∫+∞ϵ(t)/t dt=+∞\int^{+\infty}\epsilon(t)/t\,dt=+\infty∫+∞ϵ(t)/tdt=+∞ and the trajectory approaches the minimum-norm minimizer in a weighted average sense.

Timeline. 2016: Su, Boyd and Candès derive the continuous model of Nesterov's method. 2016: Attouch, Peypouquet and Redont add Hessian-driven damping (α≥3\alpha\ge3α≥3, β>0\beta>0β>0) and prove fast rates and weak convergence. 2018: Attouch, Chbani and Riahi add Tikhonov regularization without Hessian damping and prove, among other results, strong ergodic convergence to the minimum-norm minimizer when ∫ϵ(t)/t dt=+∞\int\epsilon(t)/t\,dt=+\infty∫ϵ(t)/tdt=+∞. 2020: Boţ, Csetnek and László combine both terms and extend that ergodic result (their Theorem 4.2).

Setting

Let H\mathcal HH be a real Hilbert space, t0>0t_0>0t0​>0, α>0\alpha>0α>0, β≥0\beta\ge0β≥0, and u0,v0∈Hu_0,v_0\in\mathcal Hu0​,v0​∈H. The data satisfy the paper's General assumption:

  • g:H→Rg:\mathcal H\to\mathbb Rg:H→R is convex and twice Fréchet differentiable, its gradient ∇g\nabla g∇g is Lipschitz continuous on bounded sets, and argmin⁡g≠∅\operatorname{argmin} g\neq\emptysetargming=∅;
  • ϵ:[t0,+∞)→[0,+∞)\epsilon:[t_0,+\infty)\to[0,+\infty)ϵ:[t0​,+∞)→[0,+∞) is nonincreasing, of class C1C^1C1, and lim⁡t→+∞ϵ(t)=0\lim_{t\to+\infty}\epsilon(t)=0limt→+∞​ϵ(t)=0.

A global C2C^2C2-solution of system (5) is a twice continuously differentiable x:[t0,+∞)→Hx:[t_0,+\infty)\to\mathcal Hx:[t0​,+∞)→H with

x¨(t)+αtx˙(t)+β∇2g(x(t))x˙(t)+∇g(x(t))+ϵ(t)x(t)=0(t≥t0),x(t0)=u0, x˙(t0)=v0.\ddot x(t)+\frac{\alpha}{t}\dot x(t)+\beta\nabla^2 g(x(t))\dot x(t)+\nabla g(x(t))+\epsilon(t)x(t)=0\quad(t\ge t_0),\qquad x(t_0)=u_0,\ \dot x(t_0)=v_0 .x¨(t)+tα​x˙(t)+β∇2g(x(t))x˙(t)+∇g(x(t))+ϵ(t)x(t)=0(t≥t0​),x(t0​)=u0​, x˙(t0​)=v0​.

The set argmin⁡g\operatorname{argmin} gargming is nonempty, closed and convex, so it has a unique element of minimum norm, the minimum-norm minimizer x∗=argmin⁡{∥x∥:x∈argmin⁡g}x^*=\operatorname{argmin}\{\|x\|:x\in\operatorname{argmin} g\}x∗=argmin{∥x∥:x∈argming}. For ϵ>0\epsilon>0ϵ>0 the Tikhonov approximation curve is

xϵ=argmin⁡x∈H(g(x)+ϵ2∥x∥2),x_\epsilon=\operatorname*{argmin}_{x\in\mathcal H}\Big(g(x)+\frac{\epsilon}{2}\|x\|^2\Big),xϵ​=x∈Hargmin​(g(x)+2ϵ​∥x∥2),

the unique minimizer of a strongly convex function. Finally, hx∗(t)=12∥x(t)−x∗∥2h_{x^*}(t)=\tfrac12\|x(t)-x^*\|^2hx∗​(t)=21​∥x(t)−x∗∥2 measures the distance of the trajectory to x∗x^*x∗, with derivative h˙x∗(t)=⟨x˙(t),x(t)−x∗⟩\dot h_{x^*}(t)=\langle\dot x(t),x(t)-x^*\rangleh˙x∗​(t)=⟨x˙(t),x(t)−x∗⟩.

Formalization targets

Goal: Theorem 4.2 (p. 18)

If ∫t0+∞ϵ(t)t dt=+∞\int_{t_0}^{+\infty}\frac{\epsilon(t)}{t}\,dt=+\infty∫t0​+∞​tϵ(t)​dt=+∞ and α>0\alpha>0α>0, then every global C2C^2C2-solution satisfies

lim⁡t→+∞1∫t0tϵ(s)s ds∫t0tϵ(s)s∥x(s)−x∗∥2 ds=0andlim inf⁡t→+∞∥x(t)−x∗∥=0.\lim_{t\to+\infty}\frac{1}{\int_{t_0}^{t}\frac{\epsilon(s)}{s}\,ds}\int_{t_0}^{t}\frac{\epsilon(s)}{s}\|x(s)-x^*\|^2\,ds=0 \qquad\text{and}\qquad \liminf_{t\to+\infty}\|x(t)-x^*\|=0 .t→+∞lim​∫t0​t​sϵ(s)​ds1​∫t0​t​sϵ(s)​∥x(s)−x∗∥2ds=0andt→+∞liminf​∥x(t)−x∗∥=0.

No rate and no constant is asserted, so the goal does not depend on any particular choice of ϵ\epsilonϵ.

Milestones

  1. Lemma 4.1 (p. 16): for α>0\alpha>0α>0, β≥0\beta\ge0β≥0, the velocity is bounded, 1t∥x˙(t)∥2∈L1([t0,+∞))\frac1t\|\dot x(t)\|^2\in L^1([t_0,+\infty))t1​∥x˙(t)∥2∈L1([t0​,+∞)), and sup⁡t≥t01t∣h˙x∗(t)∣<+∞\sup_{t\ge t_0}\frac1t|\dot h_{x^*}(t)|<+\inftysupt≥t0​​t1​∣h˙x∗​(t)∣<+∞ for every x∗∈argmin⁡gx^*\in\operatorname{argmin} gx∗∈argming.
  2. §4, p. 18: ∥xϵ∥≤∥x∗∥\|x_\epsilon\|\le\|x^*\|∥xϵ​∥≤∥x∗∥ for every ϵ>0\epsilon>0ϵ>0.
  3. §4, p. 18: lim⁡ϵ→0+xϵ=x∗\lim_{\epsilon\to0^+}x_\epsilon=x^*limϵ→0+​xϵ​=x∗ (stated in the paper as well known).
  4. (46) (p. 20): under the hypotheses of Theorem 4.2 there is C>0C>0C>0 with
∫t0tϵ(s)s(hx∗(s)−12(∥x∗∥2−∥xϵ(s)∥2))ds≤Cfor every t≥t0.\int_{t_0}^{t}\frac{\epsilon(s)}{s}\Big(h_{x^*}(s)-\frac12\big(\|x^*\|^2-\|x_{\epsilon(s)}\|^2\big)\Big)ds\le C\quad\text{for every }t\ge t_0 .∫t0​t​sϵ(s)​(hx∗​(s)−21​(∥x∗∥2−∥xϵ(s)​∥2))ds≤Cfor every t≥t0​.

Significance

The result shows that slow Tikhonov regularization still selects the minimum-norm minimizer when Hessian damping is added: the weighted time average of ∥x(t)−x∗∥2\|x(t)-x^*\|^2∥x(t)−x∗∥2 tends to zero and the trajectory comes arbitrarily close to x∗x^*x∗ infinitely often. The hypothesis is only α>0\alpha>0α>0, well below the threshold α≥3\alpha\ge3α≥3 that the paper needs for its fast rates, and no growth condition on ϵ\epsilonϵ beyond the divergence of ∫ϵ(t)/t dt\int\epsilon(t)/t\,dt∫ϵ(t)/tdt is imposed. It complements Theorem 4.4 of the same paper (a separate mission), which reaches full strong convergence under fast decay, ∫ϵ(t)/t dt<+∞\int\epsilon(t)/t\,dt<+\infty∫ϵ(t)/tdt<+∞, plus further conditions.

On the formal side, the theorem and its milestones are proved in the paper and in the cited literature, but none of them has a machine-checked proof. The work splits into an energy estimate for a nonautonomous second order ODE in a Hilbert space (Lemma 4.1), two facts about the Tikhonov curve that underlie the whole theory of Tikhonov regularization of convex problems (milestones 2 and 3), an integrated differential inequality (46), and a l'Hospital-type averaging step. The Tikhonov-curve facts are reusable for any formal treatment of viscosity selection and minimum-norm solutions.

Difficulty

The obvious attempt, a Lyapunov function that decreases along the trajectory and controls ∥x(t)−x∗∥\|x(t)-x^*\|∥x(t)−x∗∥, fails because x∗x^*x∗ is not a stationary point of the perturbed system: ∇g(x∗)+ϵ(t)x∗=ϵ(t)x∗≠0\nabla g(x^*)+\epsilon(t)x^*=\epsilon(t)x^*\neq0∇g(x∗)+ϵ(t)x∗=ϵ(t)x∗=0 in general. The distance to x∗x^*x∗ therefore need not decrease, and pointwise convergence is not available under the slow-decay hypothesis alone. The comparison point has to move along the Tikhonov curve xϵ(t)x_{\epsilon(t)}xϵ(t)​, whose convergence to x∗x^*x∗ comes without a rate. The available bound controls only a weighted integral of hx∗h_{x^*}hx∗​ corrected by ∥x∗∥2−∥xϵ(s)∥2\|x^*\|^2-\|x_{\epsilon(s)}\|^2∥x∗∥2−∥xϵ(s)​∥2, so the passage from (46) to the goal needs both xϵ(t)→x∗x_{\epsilon(t)}\to x^*xϵ(t)​→x∗ and the divergence of the weight. In the formal setting the Tikhonov-curve limit is itself a nontrivial weak-compactness argument in a Hilbert space, which the paper does not spell out.

Formalization scope

  • H\mathcal HH is a real Hilbert space (InnerProductSpace ℝ H, CompleteSpace H). ∇g\nabla g∇g is gradient g, and ∇2g(x)v\nabla^2 g(x)v∇2g(x)v is the Fréchet derivative of gradient g at xxx applied to vvv. "Twice Fréchet differentiable" means ggg and ∇g\nabla g∇g are differentiable; Lipschitz continuity on bounded sets is stated on every closed ball around the origin.
  • Trajectories are maps R→H\mathbb R\to\mathcal HR→H with explicit velocity and acceleration maps; derivatives are taken within [t0,+∞)[t_0,+\infty)[t0​,+∞) (one-sided at t0t_0t0​), the acceleration is continuous there, and values before t0t_0t0​ are irrelevant. The same holds for ϵ\epsilonϵ and its derivative.
  • Every theorem is stated for every global C2C^2C2-solution of (5). Existence and uniqueness of the solution is Theorem 2.1 of the paper, a milestone of the first mission of this series, so the hypothesis is not vacuous. The paper's standing α≥3\alpha\ge3α≥3 is replaced by each statement's own hypothesis α>0\alpha>0α>0.
  • The minimum-norm minimizer and the Tikhonov points are predicates on a candidate point; where the curve ϵ↦xϵ\epsilon\mapsto x_\epsilonϵ↦xϵ​ is needed, a selection that minimizes g+ϵ2∥⋅∥2g+\frac\epsilon2\|\cdot\|^2g+2ϵ​∥⋅∥2 for every ϵ>0\epsilon>0ϵ>0 is a hypothesis.
  • ∫t0+∞ϵ(t)/t dt=+∞\int_{t_0}^{+\infty}\epsilon(t)/t\,dt=+\infty∫t0​+∞​ϵ(t)/tdt=+∞ is stated as divergence of T↦∫t0Tϵ(t)/t dtT\mapsto\int_{t_0}^T\epsilon(t)/t\,dtT↦∫t0​T​ϵ(t)/tdt, never as an equation for a Bochner integral, which would take the value 000 on a non-integrable function. Likewise, lim inf⁡∥x(t)−x∗∥=0\liminf\|x(t)-x^*\|=0liminf∥x(t)−x∗∥=0 is stated as "for every δ>0\delta>0δ>0, ∥x(t)−x∗∥<δ\|x(t)-x^*\|<\delta∥x(t)−x∗∥<δ for arbitrarily large ttt", not through Filter.liminf, whose value on an unbounded function is a default. sup⁡<+∞\sup<+\inftysup<+∞ is boundedness from above of the image of [t0,+∞)[t_0,+\infty)[t0​,+∞), and L1L^1L1 membership is integrability on [t0,+∞)[t_0,+\infty)[t0​,+∞).
  • Definitions needed: argmin, the minimum-norm minimizer, Tikhonov points, the General assumption, the solution predicate for (5), and hx∗h_{x^*}hx∗​, h˙x∗\dot h_{x^*}h˙x∗​. These duplicate objects of the other two missions of the series, which are drafted independently.
  • Contributions welcome: proofs of the Tikhonov-curve facts in Mathlib generality, the energy estimate of Lemma 4.1, a continuous l'Hospital/Cesàro lemma for weighted averages, and the goal itself.

Selected references

  • R.I. Boţ, E.R. Csetnek, S.C. László, Tikhonov regularization of a second order dynamical system with Hessian driven damping, Mathematical Programming, 2021, https://doi.org/10.1007/s10107-020-01528-8 (cited from arXiv:1911.12845v2). https://arxiv.org/abs/1911.12845
  • H. Attouch, Z. Chbani, H. Riahi, Combining fast inertial dynamics for convex optimization with Tikhonov regularization, Journal of Mathematical Analysis and Applications 457(2), 1065–1094, 2018. https://arxiv.org/abs/1602.01973
  • H. Attouch, J. Peypouquet, P. Redont, Fast convex optimization via inertial dynamics with Hessian driven damping, Journal of Differential Equations 261(10), 5734–5783, 2016. https://arxiv.org/abs/1601.07113
  • H. Attouch, Z. Chbani, J. Peypouquet, P. Redont, Fast convergence of inertial dynamics and algorithms with asymptotic vanishing viscosity, Mathematical Programming 168, 123–175, 2018. https://arxiv.org/abs/1507.04782
  • W. Su, S. Boyd, E.J. Candès, A differential equation for modeling Nesterov's accelerated gradient method: theory and insights, Journal of Machine Learning Research 17(153), 1–43, 2016. https://arxiv.org/abs/1503.01243
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Operations ResearchProbability·Captain: mikedeng1

Conditional Risk Mappings: A Positively Homogeneous Lower Semicontinuous Conditional Risk Mapping Is the Supremum of Countably Many Conditional ExpectationsResearch Paper

Motivation

Risk measures quantify the danger of an uncertain cost XXX by a single number. The axiomatic theory of coherent and convex risk measures (Artzner, Delbaen, Eber and Heath, Coherent measures of risk, 1999; Föllmer and Schied, Convex measures of risk and trading constraints, 2002) is static: the risk is evaluated once, with no information beyond what is known at time zero. Multistage stochastic optimization and dynamic risk management need risk evaluated conditionally: at time 1 part of the uncertainty has been resolved, and the risk of a time-2 cost should be a function of what is known at time 1.

Ruszczyński and Shapiro, in Conditional risk mappings (preprint of February 21, 2004; journal version Mathematics of Operations Research 31(3), 2006), extend their earlier static theory (Optimization of convex risk functions, Math. Oper. Res. 31(3), 2006) to this conditional setting. They define conditional risk mappings by three axioms, derive a pointwise conjugate duality, and show that positively homogeneous conditional risk mappings are, under regularity conditions, suprema of countably many conditional expectations. The last result explains the word conditional: the conditional expectation is the prototype, and every positively homogeneous conditional risk mapping is a worst case over a countable family of them.

Setting

Let Ω\OmegaΩ be a set with σ\sigmaσ-algebras F1⊂F2\mathcal F_1\subset\mathcal F_2F1​⊂F2​; F1\mathcal F_1F1​ is the information available when risk is evaluated. Let X2\mathcal X_2X2​ be a real vector space of F2\mathcal F_2F2​-measurable functions X:Ω→RX:\Omega\to\mathbb RX:Ω→R, and X1⊂X2\mathcal X_1\subset\mathcal X_2X1​⊂X2​ a subspace of F1\mathcal F_1F1​-measurable ones. Let Y2\mathcal Y_2Y2​ be a real vector space of finite signed measures on (Ω,F2)(\Omega,\mathcal F_2)(Ω,F2​) with ∫∣X∣ d∣μ∣<∞\int|X|\,d|\mu|<\infty∫∣X∣d∣μ∣<∞, and pair them by

⟨μ,X⟩=∫ΩX dμ.\langle\mu,X\rangle=\int_\Omega X\,d\mu .⟨μ,X⟩=∫Ω​Xdμ.

Both spaces carry locally convex topologies that are compatible with this pairing: the continuous linear functionals on each space are exactly the pairings with elements of the other. Two standing conditions hold throughout: (C) if μ∈Y2\mu\in\mathcal Y_2μ∈Y2​ is not a nonnegative measure, some nonnegative X∈X2X\in\mathcal X_2X∈X2​ has ⟨μ,X⟩<0\langle\mu,X\rangle<0⟨μ,X⟩<0; (C′) 1B∈X1\mathbb 1_B\in\mathcal X_11B​∈X1​ for every B∈F1B\in\mathcal F_1B∈F1​.

A conditional risk mapping is a map ρ:X2→X1\rho:\mathcal X_2\to\mathcal X_1ρ:X2​→X1​ with, writing ρω(X)=[ρ(X)](ω)\rho_\omega(X)=[\rho(X)](\omega)ρω​(X)=[ρ(X)](ω):

  • (A1) convexity: ρω(tX+(1−t)Y)≤tρω(X)+(1−t)ρω(Y)\rho_\omega(tX+(1-t)Y)\le t\rho_\omega(X)+(1-t)\rho_\omega(Y)ρω​(tX+(1−t)Y)≤tρω​(X)+(1−t)ρω​(Y) for t∈[0,1]t\in[0,1]t∈[0,1];
  • (A2) monotonicity: Y(ω′)≥X(ω′)Y(\omega')\ge X(\omega')Y(ω′)≥X(ω′) for all ω′\omega'ω′ implies ρω(Y)≥ρω(X)\rho_\omega(Y)\ge\rho_\omega(X)ρω​(Y)≥ρω​(X);
  • (A3) translation equivariance: ρ(X+Y)=ρ(X)+Y\rho(X+Y)=\rho(X)+Yρ(X+Y)=ρ(X)+Y for every Y∈X1Y\in\mathcal X_1Y∈X1​.

Costs are minimised: smaller XXX is better. All inequalities hold at every ω∈Ω\omega\in\Omegaω∈Ω, not almost surely. ρ\rhoρ is positively homogeneous if ρ(tX)=tρ(X)\rho(tX)=t\rho(X)ρ(tX)=tρ(X) for t>0t>0t>0, and lower semicontinuous if each ρω\rho_\omegaρω​ is.

The conjugate is ρ∗(μ,ω)=sup⁡X{⟨μ,X⟩−ρω(X)}∈R‾\rho^*(\mu,\omega)=\sup_{X}\{\langle\mu,X\rangle-\rho_\omega(X)\}\in\overline{\mathbb R}ρ∗(μ,ω)=supX​{⟨μ,X⟩−ρω​(X)}∈R and the risk envelope is A(ω)={μ:ρ∗(μ,ω)<∞}\mathcal A(\omega)=\{\mu:\rho^*(\mu,\omega)<\infty\}A(ω)={μ:ρ∗(μ,ω)<∞}. PY2\mathcal P_{\mathcal Y_2}PY2​​ denotes the probability measures in Y2\mathcal Y_2Y2​, and PY2∣F1(ω)\mathcal P_{\mathcal Y_2|\mathcal F_1}(\omega)PY2​∣F1​​(ω) those ν\nuν with ν(B)=1B(ω)\nu(B)=\mathbb 1_B(\omega)ν(B)=1B​(ω) for all B∈F1B\in\mathcal F_1B∈F1​. A map ω↦μω\omega\mapsto\mu_\omegaω↦μω​ is weakly* F1\mathcal F_1F1​-measurable if every ω↦⟨μω,X⟩\omega\mapsto\langle\mu_\omega,X\rangleω↦⟨μω​,X⟩ is F1\mathcal F_1F1​-measurable. For such a selection of A\mathcal AA, the operator [Qμ(ν)](A)=∫μω(A) dν(ω)[\mathbb Q_\mu(\nu)](A)=\int\mu_\omega(A)\,d\nu(\omega)[Qμ​(ν)](A)=∫μω​(A)dν(ω) acts on Y2\mathcal Y_2Y2​. Assumption (K): PY2\mathcal P_{\mathcal Y_2}PY2​​ is compact, and every such Qμ\mathbb Q_\muQμ​ maps PY2\mathcal P_{\mathcal Y_2}PY2​​ into itself with a closed graph. Finally, μ(⋅)\mu(\cdot)μ(⋅) is the conditional probability of ν\nuν given F1\mathcal F_1F1​ if each ω↦μω(A)\omega\mapsto\mu_\omega(A)ω↦μω​(A) is F1\mathcal F_1F1​-measurable and ∫Sμω(A) dν=ν(A∩S)\int_S\mu_\omega(A)\,d\nu=\nu(A\cap S)∫S​μω​(A)dν=ν(A∩S) for S∈F1S\in\mathcal F_1S∈F1​, A∈F2A\in\mathcal F_2A∈F2​; then Eν[X∣F1](ω)=⟨μω,X⟩\mathbb E_\nu[X|\mathcal F_1](\omega)=\langle\mu_\omega,X\rangleEν​[X∣F1​](ω)=⟨μω​,X⟩.

Formalization targets

Goal: Theorem 2 (p. 11)

If X2\mathcal X_2X2​ is separable, (K) holds and ρ\rhoρ is a positively homogeneous, lower semicontinuous conditional risk mapping, then there are probability measures νi∈PY2\nu^i\in\mathcal P_{\mathcal Y_2}νi∈PY2​​, i∈Ni\in\mathbb Ni∈N, with

ρω(X)=sup⁡i∈NEνi[X∣F1](ω)for all X∈X2, ω∈Ω,\rho_\omega(X)=\sup_{i\in\mathbb N}\mathbb E_{\nu^i}[X|\mathcal F_1](\omega)\qquad\text{for all }X\in\mathcal X_2,\ \omega\in\Omega,ρω​(X)=i∈Nsup​Eνi​[X∣F1​](ω)for all X∈X2​, ω∈Ω,

each conditional expectation being the integral against a weakly* F1\mathcal F_1F1​-measurable conditional probability of νi\nu^iνi.

Milestones

  1. dom⁡ρ∗(⋅,ω)⊆PY2∣F1(ω)\operatorname{dom}\rho^*(\cdot,\omega)\subseteq\mathcal P_{\mathcal Y_2|\mathcal F_1}(\omega)domρ∗(⋅,ω)⊆PY2​∣F1​​(ω) (proof of Theorem 1, pp. 5–6).
  2. Theorem 1 (p. 5): ρω(X)=sup⁡μ∈PY2∣F1(ω){⟨μ,X⟩−ρ∗(μ,ω)}\rho_\omega(X)=\sup_{\mu\in\mathcal P_{\mathcal Y_2|\mathcal F_1}(\omega)}\{\langle\mu,X\rangle-\rho^*(\mu,\omega)\}ρω​(X)=supμ∈PY2​∣F1​​(ω)​{⟨μ,X⟩−ρ∗(μ,ω)}, and its converse.
  3. (3.8) (p. 6): for positively homogeneous ρ\rhoρ, ρ∗(⋅,ω)\rho^*(\cdot,\omega)ρ∗(⋅,ω) is the indicator of a closed convex A(ω)\mathcal A(\omega)A(ω) and ρω(X)=sup⁡μ∈A(ω)⟨μ,X⟩\rho_\omega(X)=\sup_{\mu\in\mathcal A(\omega)}\langle\mu,X\rangleρω​(X)=supμ∈A(ω)​⟨μ,X⟩.
  4. Lemma 1 (p. 11): for separable X2\mathcal X_2X2​, countably many weakly* measurable selections of A\mathcal AA suffice.
  5. Under (K), each Qμ\mathbb Q_\muQμ​ has a fixed point in PY2\mathcal P_{\mathcal Y_2}PY2​​ (p. 10).
  6. Proposition 3 (p. 9): a fixed point νˉ\bar\nuνˉ of Qμ\mathbb Q_\muQμ​ has μ\muμ as its conditional probability given F1\mathcal F_1F1​.

Corollary 1 (p. 10, singleton envelopes give a conditional expectation) and Proposition 2 (p. 7, ρ(YX)=Yρ(X)\rho(YX)=Y\rho(X)ρ(YX)=Yρ(X) for nonnegative F1\mathcal F_1F1​-step functions YYY) are included as further statements.

Significance

Theorem 2 identifies the positively homogeneous conditional risk mappings with suprema of conditional expectations. It is the conditional analogue of the representation of a coherent risk measure as a worst-case expectation over a set of probability measures. It shows that the axioms (A1)–(A3), stated at every ω\omegaω, are the right abstraction of "conditional": nothing beyond conditional expectations and a supremum is needed to generate them. Theorem 1, the pointwise duality on which it rests, is what makes conditional risk mappings usable in multistage problems. Its envelope form (3.8) is what the paper's composition results and dynamic programming equations in §5–§7 manipulate.

The results are proved in the paper, partly by reference: the duality of Theorem 1 by applying the authors' earlier unconditional theorem "verbatim" at each ω\omegaω, Lemma 1 through a measurable-selection theorem, and Theorem 2 through Kakutani's fixed-point theorem. None of them is formalized. A formalization would check these deferred steps. In particular the passage, in the proof of Lemma 1, from a dense subset of X2\mathcal X_2X2​ to all of X2\mathcal X_2X2​ uses only lower semicontinuity of ρω\rho_\omegaρω​, and whether that suffices in every separable paired space is open to scrutiny.

Difficulty

Theorem 1 needs the Fenchel–Moreau theorem in a general locally convex space, paired through integrals against signed measures. Mathlib's convex duality is mostly finite-dimensional or normed, and the extended-real bookkeeping of conjugates is delicate. The main obstacle is Lemma 1. The envelope A(ω)\mathcal A(\omega)A(ω) can be uncountable, and choosing countably many selections that are simultaneously measurable in ω\omegaω and exhaust the supremum for every XXX requires a measurable-selection theorem for multifunctions with values in Y2\mathcal Y_2Y2​, a space that need not be metrizable. The obvious argument fixes a dense sequence XnX_nXn​, picks ε\varepsilonε-optimal measures for each XnX_nXn​, and passes to general XXX by semicontinuity. As written, that last step appears to need more than the proof supplies: approximation of ⟨μ,X⟩\langle\mu,X\rangle⟨μ,X⟩ by ⟨μ,Xn⟩\langle\mu,X_n\rangle⟨μ,Xn​⟩ uniformly over the chosen μ\muμ needs more than lower semicontinuity of ρω\rho_\omegaρω​. The fixed-point step needs a Kakutani-type theorem in a locally convex space, which Mathlib does not provide.

Formalization scope

X2\mathcal X_2X2​ and Y2\mathcal Y_2Y2​ are abstract real vector spaces with their own topologies (instances of IsTopologicalAddGroup, ContinuousSMul ℝ, LocallyConvexSpace ℝ), realised by injective linear maps into Ω→R\Omega\to\mathbb RΩ→R and into Mathlib's SignedMeasure Ω. They are not subspaces of Ω→R\Omega\to\mathbb RΩ→R with the pointwise topology. The ambient MeasurableSpace Ω is F2\mathcal F_2F2​; F1≤F2\mathcal F_1\le\mathcal F_2F1​≤F2​ is a structure field. The pairing is ∫X dμ+−∫X dμ−\int X\,d\mu^+-\int X\,d\mu^-∫Xdμ+−∫Xdμ−, and integrability against ∣μ∣|\mu|∣μ∣ is a field, so no integral takes a junk value. Compatibility includes continuity of both pairings as well as the representation of continuous functionals. The paper's space Y1\mathcal Y_1Y1​ is not modelled; no statement uses it.

Committed conventions:

  • every statement holds at every ω\omegaω; there are no a.e. classes;
  • the conjugate and the supremum in (3.6) are in EReal;
  • suprema of real numbers ((3.8), (4.7), (4.9)) are least upper bounds (IsLUB), never sSup on R\mathbb RR;
  • (K) is taken in its closed-graph form and quantifies over every weakly* measurable selection;
  • separability is that of the topology of X2\mathcal X_2X2​.

Two hypotheses are added where the page relies on them implicitly. Ω\OmegaΩ is nonempty in the goal, Corollary 1 and the fixed-point milestone. 1A∈X2\mathbb 1_A\in\mathcal X_21A​∈X2​ for every A∈F2A\in\mathcal F_2A∈F2​ is assumed in the goal, Proposition 3 and Corollary 1, because the paper derives measurability of ω↦μω(A)\omega\mapsto\mu_\omega(A)ω↦μω​(A) from weak* measurability.

The goal cannot be satisfied by an almost-everywhere version of a conditional expectation chosen separately for each XXX, which would allow ρ\rhoρ itself as a "version". Each Eνi[⋅∣F1]\mathbb E_{\nu^i}[\cdot|\mathcal F_1]Eνi​[⋅∣F1​] is integration against one kernel κi\kappa^iκi that is a conditional probability of νi\nu^iνi. The goal mentions no selection, fixed point or Kakutani; Qμ\mathbb Q_\muQμ​ appears only inside (K).

Contributions are welcome on all of the following:

  • Fenchel–Moreau duality for paired locally convex spaces;
  • measurable selections of weakly* measurable multifunctions;
  • a Kakutani–Fan–Glicksberg or Schauder–Tychonoff fixed-point theorem.

All three are reusable beyond this mission.

Selected references

  • A. Ruszczyński, A. Shapiro, Conditional risk mappings, preprint dated February 21, 2004; Mathematics of Operations Research 31(3):544–561, 2006. https://doi.org/10.1287/moor.1060.0204
  • A. Ruszczyński, A. Shapiro, Optimization of convex risk functions, Mathematics of Operations Research 31(3):433–452, 2006. https://doi.org/10.1287/moor.1050.0186
  • P. Artzner, F. Delbaen, J.-M. Eber, D. Heath, Coherent measures of risk, Mathematical Finance 9(3):203–228, 1999. https://doi.org/10.1111/1467-9965.00068
  • H. Föllmer, A. Schied, Convex measures of risk and trading constraints, Finance and Stochastics 6(4):429–447, 2002. https://doi.org/10.1007/s007800200072
  • P. Billingsley, Probability and Measure, 3rd ed., Wiley, 1995 (conditional probability, pp. 430–431).
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ProbabilityStochastic Systems·Captain: mikedeng1

Affine Processes on Positive Semidefinite Matrices II: Every Admissible Parameter Set Determines a Unique Affine Process on the PSD Cone with Generator (2.12)Research Paper

Motivation

Stochastic models of covariance matrices need processes that stay in the cone of positive semidefinite matrices. Wishart processes (Bru, 1991) and their extensions underlie multivariate stochastic-volatility and term-structure models in finance (see §1 of Cuchiero et al. for the literature). They are used because their Laplace transforms are explicit: they are exponential-affine in the initial state, and their exponents solve matrix Riccati equations. Cuchiero, Filipović, Mayerhofer and Teichmann (arXiv:0910.0137, Ann. Appl. Probab. 2011) classify all such affine processes on the cone. Theorem 2.4 of that paper says that affine processes on Sd+S_d^+Sd+​ correspond one-to-one to admissible parameter sets. This mission formalizes the converse direction of that correspondence: every admissible parameter set is realized by exactly one affine process.

Timeline:

  • Bru (1991, MR1132135) constructs Wishart processes for specific parameters.
  • Duffie, Filipović and Schachermayer (Ann. Appl. Probab. 2003, MR1994043) characterize affine processes on the canonical state space R+m×Rn\mathbb R_+^m\times\mathbb R^nR+m​×Rn, with existence through the martingale problem.
  • Cuchiero et al. (2011) give the full characterization on Sd+S_d^+Sd+​. The necessity of admissibility and the existence-and-uniqueness converse are proved in separate sections (§4 and §5).

Setting

Let SdS_dSd​ be the real symmetric d×dd\times dd×d matrices with ⟨x,y⟩=Tr⁡(xy)\langle x,y\rangle=\operatorname{Tr}(xy)⟨x,y⟩=Tr(xy), let Sd+S_d^+Sd+​ be the positive semidefinite cone, and let Sd++S_d^{++}Sd++​ be its interior. Write x⪯yx\preceq yx⪯y when y−x∈Sd+y-x\in S_d^+y−x∈Sd+​. A time-homogeneous, possibly killed Markov process on Sd+S_d^+Sd+​ with transition kernels pt(x,dξ)p_t(x,d\xi)pt​(x,dξ) is affine if it is stochastically continuous and

∫Sd+e−⟨u,ξ⟩pt(x,dξ)=e−φ(t,u)−⟨ψ(t,u),x⟩,t≥0, u,x∈Sd+,\int_{S_d^+}e^{-\langle u,\xi\rangle}p_t(x,d\xi)=e^{-\varphi(t,u)-\langle\psi(t,u),x\rangle},\qquad t\ge0,\ u,x\in S_d^+,∫Sd+​​e−⟨u,ξ⟩pt​(x,dξ)=e−φ(t,u)−⟨ψ(t,u),x⟩,t≥0, u,x∈Sd+​,

for functions φ≥0\varphi\ge0φ≥0 and ψ∈Sd+\psi\in S_d^+ψ∈Sd+​.

An admissible parameter set (α,b,βij,c,γ,m,μ)(\alpha,b,\beta^{ij},c,\gamma,m,\mu)(α,b,βij,c,γ,m,μ) (Definition 2.3) consists of the following:

  • a diffusion matrix α∈Sd+\alpha\in S_d^+α∈Sd+​;
  • a drift b⪰(d−1)αb\succeq(d-1)\alphab⪰(d−1)α;
  • killing rates c≥0c\ge0c≥0 and γ∈Sd+\gamma\in S_d^+γ∈Sd+​;
  • a jump measure mmm with ∫(∥ξ∥∧1) m(dξ)<∞\int(\|\xi\|\wedge1)\,m(d\xi)<\infty∫(∥ξ∥∧1)m(dξ)<∞;
  • a matrix of finite measures μ\muμ, which gives the state-dependent jump kernel M(x,dξ)=⟨x,μ(dξ)⟩/(∥ξ∥2∧1)M(x,d\xi)=\langle x,\mu(d\xi)\rangle/(\|\xi\|^2\wedge1)M(x,dξ)=⟨x,μ(dξ)⟩/(∥ξ∥2∧1);
  • linear drift coefficients βij\beta^{ij}βij, with the inward-pointing conditions (2.9) and (2.11) on ∂Sd+\partial S_d^+∂Sd+​.

These data define the operator (2.12),

Af(x)=12∑Aijkl(x)∂ij,kl2f+∑(bij+Bij(x))∂ijf−(c+⟨γ,x⟩)f+∫(f(x+ξ)−f(x))m(dξ)+∫(f(x+ξ)−f(x)−⟨χ(ξ),∇f⟩)M(x,dξ),\mathcal Af(x)=\tfrac12\sum A_{ijkl}(x)\partial^2_{ij,kl}f+\sum(b_{ij}+B_{ij}(x))\partial_{ij}f-(c+\langle\gamma,x\rangle)f+\int(f(x+\xi)-f(x))m(d\xi)+\int(f(x+\xi)-f(x)-\langle\chi(\xi),\nabla f\rangle)M(x,d\xi),Af(x)=21​∑Aijkl​(x)∂ij,kl2​f+∑(bij​+Bij​(x))∂ij​f−(c+⟨γ,x⟩)f+∫(f(x+ξ)−f(x))m(dξ)+∫(f(x+ξ)−f(x)−⟨χ(ξ),∇f⟩)M(x,dξ),

with Aijkl(x)=xikαjl+xilαjk+xjkαil+xjlαikA_{ijkl}(x)=x_{ik}\alpha_{jl}+x_{il}\alpha_{jk}+x_{jk}\alpha_{il}+x_{jl}\alpha_{ik}Aijkl​(x)=xik​αjl​+xil​αjk​+xjk​αil​+xjl​αik​. They also define the functions F(u)F(u)F(u) and R(u)R(u)R(u) of (2.16)–(2.17), which drive the generalized Riccati equations ∂tφ=F(ψ)\partial_t\varphi=F(\psi)∂t​φ=F(ψ), φ(0,u)=0\varphi(0,u)=0φ(0,u)=0 and ∂tψ=R(ψ)\partial_t\psi=R(\psi)∂t​ψ=R(ψ), ψ(0,u)=u\psi(0,u)=uψ(0,u)=u.

Formalization targets

Goal: Theorem 2.4, second part (= Proposition 5.9)

For every admissible parameter set there is a transition family (pt)(p_t)(pt​) and there are exponents (φ,ψ)(\varphi,\psi)(φ,ψ) such that:

(i) p is affine with exponents (φ,ψ);(ii) S+⊂D(Ap), Apf=(2.12);(iii) (φ,ψ) solves (2.14)–(2.15);\text{(i) } p \text{ is affine with exponents } (\varphi,\psi);\quad\text{(ii) } \mathcal S_+\subset D(\mathcal A_p),\ \mathcal A_pf=\text{(2.12)};\quad\text{(iii) } (\varphi,\psi) \text{ solves (2.14)–(2.15)};(i) p is affine with exponents (φ,ψ);(ii) S+​⊂D(Ap​), Ap​f=(2.12);(iii) (φ,ψ) solves (2.14)–(2.15); (iv) every affine p′ whose generator equals (2.12) on S+ satisfies pt′=pt for t≥0.\text{(iv) every affine } p' \text{ whose generator equals (2.12) on } \mathcal S_+ \text{ satisfies } p'_t=p_t \text{ for } t\ge0.(iv) every affine p′ whose generator equals (2.12) on S+​ satisfies pt′​=pt​ for t≥0.

Milestones, in attack order

  1. Theorem 4.8: a comparison theorem for matrix ODEs whose vector field is quasi-monotone increasing (Volkmann).
  2. Lemma 5.1: RRR is analytic on Sd++S_d^{++}Sd++​ and quasi-monotone increasing on Sd+S_d^+Sd+​.
  3. Lemma 5.2: the growth bound ⟨u,R(u)⟩≤K2(∥u∥2+1)\langle u,R(u)\rangle\le\frac K2(\|u\|^2+1)⟨u,R(u)⟩≤2K​(∥u∥2+1).
  4. Proposition 5.3: unique global R+×Sd++\mathbb R_+\times S_d^{++}R+​×Sd++​-valued Riccati solutions, analytic in (t,u)(t,u)(t,u).
  5. Lemma 5.5: the regularized operators Aε,δ,n\mathcal A^{\varepsilon,\delta,n}Aε,δ,n converge to A\mathcal AA uniformly on S+\mathcal S_+S+​.
  6. Lemma 5.7 (second part): the boundary condition ⟨b−12∑Dσklσkl,u⟩≥0\langle b-\frac12\sum D\sigma^{kl}\sigma^{kl},u\rangle\ge0⟨b−21​∑Dσklσkl,u⟩≥0 on ∂Sd+\partial S_d^+∂Sd+​.
  7. Lemma 5.6: the regularized martingale problems have Sd+S_d^+Sd+​-valued càdlàg solutions.
  8. Lemma 5.8: the martingale problem for A\mathcal AA has an Sd+∪{Δ}S_d^+\cup\{\Delta\}Sd+​∪{Δ}-valued càdlàg solution.

Significance

Together with the necessity direction (companion mission I in this series), the goal makes admissibility an exact characterization. Every admissible parameter set, including those with jumps of infinite activity and state-dependent killing, defines a well-posed Markov model on Sd+S_d^+Sd+​. Its Laplace transform is then given by the Riccati flow, which is what makes the model computationally tractable. The intermediate results are reusable on their own:

  • the matrix comparison theorem applies to any ODE on symmetric matrices;
  • the Riccati well-posedness on Sd++S_d^{++}Sd++​ holds for vector fields that need not be Lipschitz at ∂Sd+\partial S_d^+∂Sd+​;
  • the martingale-problem framework on a one-point compactification is used beyond this paper.

The theorem is proved in the paper; it is not formalized anywhere. No formal library contains affine processes, generalized Riccati equations on matrix cones, quasi-monotone comparison theorems or martingale problems with jumps. Formalizing them requires all of that infrastructure.

Difficulty

The obvious route is to solve the Riccati equation (2.15) on Sd+S_d^+Sd+​ by Picard iteration and to show invariance of the cone from the inward-pointing condition. That route fails because RRR need not be Lipschitz at ∂Sd+\partial S_d^+∂Sd+​: the integral term can have unbounded derivative there (Remark 5.4). Standard invariance theorems therefore do not apply. Instead, quasi-monotonicity keeps the solution away from the boundary.

The obvious construction of the process is also blocked. Stroock's existence and uniqueness theory for martingale problems needs Rn\mathbb R^nRn and a uniformly elliptic diffusion part, and neither holds on the cone, where the diffusion degenerates at the boundary. Existence must go through regularized operators with bounded smooth coefficients, then tightness in the Skorokhod space of Sd+∪{Δ}S_d^+\cup\{\Delta\}Sd+​∪{Δ} and a limit. Uniqueness in law comes from the Riccati solutions. The killing terms ccc and γ\gammaγ are added last.

Formalization scope

Conventions committed to in Lean:

  • MdM_dMd​ is the function type Fin d → Fin d → ℝ, with ⟨x,y⟩=∑ijxijyji\langle x,y\rangle=\sum_{ij}x_{ij}y_{ji}⟨x,y⟩=∑ij​xij​yji​ and its norm.
  • Sd+S_d^+Sd+​ is the subtype of positive semidefinite matrices, with the subspace topology and Borel structure.
  • Partial derivatives ∂/∂xij\partial/\partial x_{ij}∂/∂xij​ are taken in the symmetrized directions 12(Eij+Eji)\tfrac12(E^{ij}+E^{ji})21​(Eij+Eji).
  • The matrix measure μ\muμ is encoded as H dνH\,d\nuHdν with a finite measure ν\nuν and a positive semidefinite density HHH. This encoding is equivalent; take ν=∑iμii\nu=\sum_i\mu_{ii}ν=∑i​μii​.
  • The test space S+\mathcal S_+S+​ is represented by Schwartz functions on MdM_dMd​, restricted to the cone. The generator is the uniform limit of (Ptf−f)/t(P_tf-f)/t(Pt​f−f)/t.
  • Transition families are indexed by t∈Rt\in\mathbb Rt∈R, and only t≥0t\ge0t≥0 enters. Uniqueness is equality for t≥0t\ge0t≥0, never ∃!.
  • Analyticity on Sd++S_d^{++}Sd++​ is analyticity of y↦G((y+y⊤)/2)y\mapsto G((y+y^\top)/2)y↦G((y+y⊤)/2) on an open subset of MdM_dMd​.
  • Martingale problems carry an existentially quantified probability space, the natural filtration and càdlàg paths (the platform predicate EthierKurtz.HasCadlagPaths).
  • The cut-offs ϕn\phi_nϕn​ and ηε\eta_\varepsilonηε​ of §5.2 are arbitrary functions with the properties the paper lists. The paper fixes some and uses only those properties.
  • The case condition of (5.7) is tested on ϕn(x)x\phi_n(x)xϕn​(x)x, the argument of ηε\eta_\varepsilonηε​, rather than on xxx as printed. The printed reading makes sε,ns_{\varepsilon,n}sε,n​ discontinuous off Sd+S_d^+Sd+​, which contradicts the paper's claim sε,n∈Cb∞(Sd,Sd)s_{\varepsilon,n}\in C_b^\infty(S_d,S_d)sε,n​∈Cb∞​(Sd​,Sd​). The two readings agree on Sd+S_d^+Sd+​.
  • In Theorem 4.8, "locally Lipschitz" is read as Lipschitz in the state variable, locally uniformly in time. This is weaker than joint local Lipschitz continuity in (t,x)(t,x)(t,x).
  • Every statement that contains one of the integrals of (2.12), (2.16), (2.17) or (5.10) also asserts that its integrand is integrable.
  • Hypotheses not present on the page: none. Lemmas 5.1 and 5.2 assume less than the section's standing assumptions (not the drift condition (2.4)).

Trivializing formalizations are excluded:

  • Lean's value 000 for a non-integrable integral is ruled out by the integrability conclusions.
  • A pointwise generator would be weaker than the paper's notion, so the generator is the uniform limit.
  • An ∃! over transition families would be false at negative times, so uniqueness is stated for t≥0t\ge0t≥0.
  • A martingale problem is not posed for a fixed probability space, and X0=xX_0=xX0​=x is required almost surely.

Needed infrastructure, reusable beyond this mission: matrix calculus on SdS_dSd​ (square roots, spectral derivatives), comparison theorems for quasi-monotone ODEs, analytic dependence of ODE solutions, tightness in Skorokhod space, and martingale problems on locally compact spaces. Contributions are welcome at any of these levels, as are alternative proofs of the milestones.

Selected references

  • C. Cuchiero, D. Filipović, E. Mayerhofer, J. Teichmann, Affine processes on positive semidefinite matrices, Ann. Appl. Probab. 21 (2011) 397–463; cited from arXiv:0910.0137v3. https://arxiv.org/abs/0910.0137v3
  • D. Duffie, D. Filipović, W. Schachermayer, Affine processes and applications in finance, Ann. Appl. Probab. 13 (2003) 984–1053. https://mathscinet.ams.org/mathscinet-getitem?mr=1994043
  • M.-F. Bru, Wishart processes, J. Theoret. Probab. 4 (1991) 725–751. https://mathscinet.ams.org/mathscinet-getitem?mr=1132135
  • S. N. Ethier, T. G. Kurtz, Markov Processes: Characterization and Convergence, Wiley, New York, 1986. https://mathscinet.ams.org/mathscinet-getitem?mr=0838085
  • P. Volkmann, Über die Invarianz konvexer Mengen und Differentialungleichungen in einem normierten Raume, Math. Ann. 203 (1973) 201–210. https://mathscinet.ams.org/mathscinet-getitem?mr=0322305
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ProbabilityStochastic Systems·Captain: mikedeng1

Affine Processes on Positive Semidefinite Matrices III: For d ≥ 2, a Markov Family Is Infinitely Decomposable Iff It Is Affine with Zero Diffusion Iff It Is Affine and Infinitely DivisibleResearch Paper

Motivation

Affine processes are Markov processes whose Laplace transform depends exponential-affinely on the initial state. On the cone Sd+S_d^+Sd+​ of positive semidefinite matrices they model stochastic covariance matrices in multivariate stochastic volatility, interest-rate and credit models. Examples include the Wishart process of Bru (Bru 1991) and Ornstein–Uhlenbeck processes driven by matrix Lévy subordinators (Barndorff-Nielsen and Stelzer 2007, reference [3] of the paper). Cuchiero, Filipović, Mayerhofer and Teichmann (2011) characterize all affine processes on Sd+S_d^+Sd+​ by admissible parameter sets.

On the canonical state space R+m×Rn\mathbb R_+^m\times\mathbb R^nR+m​×Rn, Duffie, Filipović and Schachermayer (2003) showed that regular affine processes are exactly the infinitely decomposable Markov processes: the law started at x(1)+⋯+x(k)x^{(1)}+\dots+x^{(k)}x(1)+⋯+x(k) is a kkk-fold convolution of laws started at the x(i)x^{(i)}x(i). That property drives their existence proof. On Sd+S_d^+Sd+​ with d≥2d\ge2d≥2 it fails. The Wishart marginals are not infinitely divisible, a classical result of Paul Lévy. This mission formalizes the exact characterization: Theorem 2.9 of Cuchiero et al.

Setting

MdM_dMd​ is the space of real d×dd\times dd×d matrices and SdS_dSd​ the symmetric ones. SdS_dSd​ carries the pairing ⟨x,y⟩=Tr(xy)\langle x,y\rangle=\mathrm{Tr}(xy)⟨x,y⟩=Tr(xy) and the norm ∥x∥=⟨x,x⟩\|x\|=\sqrt{\langle x,x\rangle}∥x∥=⟨x,x⟩​. Sd+S_d^+Sd+​ is the closed convex cone of positive semidefinite matrices, and Sd+∪{Δ}S_d^+\cup\{\Delta\}Sd+​∪{Δ} its one-point compactification. The point Δ\DeltaΔ is the cemetery, where a killed process goes.

A transition family (pt)t≥0(p_t)_{t\ge0}(pt​)t≥0​ consists of sub-stochastic kernels on Sd+S_d^+Sd+​ satisfying p0(x,⋅)=δxp_0(x,\cdot)=\delta_xp0​(x,⋅)=δx​ and the Chapman–Kolmogorov equations. It is stochastically continuous if ps(x,⋅)→pt(x,⋅)p_s(x,\cdot)\to p_t(x,\cdot)ps​(x,⋅)→pt​(x,⋅) weakly as s→ts\to ts→t. The process is affine (Definition 2.1) if there are φ≥0\varphi\ge0φ≥0 and ψ∈Sd+\psi\in S_d^+ψ∈Sd+​ with

∫e−⟨u,ξ⟩pt(x,dξ)=e−φ(t,u)−⟨ψ(t,u),x⟩,t≥0, u,x∈Sd+.\int e^{-\langle u,\xi\rangle}p_t(x,d\xi)=e^{-\varphi(t,u)-\langle\psi(t,u),x\rangle},\qquad t\ge0,\ u,x\in S_d^+.∫e−⟨u,ξ⟩pt​(x,dξ)=e−φ(t,u)−⟨ψ(t,u),x⟩,t≥0, u,x∈Sd+​.

Theorem 2.4 of the paper attaches to every affine process a unique admissible parameter set (α,b,βij,c,γ,m,μ)(\alpha,b,\beta^{ij},c,\gamma,m,\mu)(α,b,βij,c,γ,m,μ). In it, α∈Sd+\alpha\in S_d^+α∈Sd+​ is the diffusion parameter, b⪰(d−1)αb\succeq(d-1)\alphab⪰(d−1)α the constant drift, ccc and γ\gammaγ the killing rates, and mmm and μ\muμ the jump measures. The exponents solve the generalized Riccati equations ∂tφ=F(ψ)\partial_t\varphi=F(\psi)∂t​φ=F(ψ), ∂tψ=R(ψ)\partial_t\psi=R(\psi)∂t​ψ=R(ψ), with F,RF,RF,R given by (2.16)–(2.17).

The canonical space Ω\OmegaΩ consists of paths ω:R+→Sd+∪{Δ}\omega:\mathbb R_+\to S_d^+\cup\{\Delta\}ω:R+​→Sd+​∪{Δ} that stay at Δ\DeltaΔ once they reach it, with coordinate process Xt(ω)=ω(t)X_t(\omega)=\omega(t)Xt​(ω)=ω(t). P\mathcal PP is the set of families (Px)x∈Sd+(P_x)_{x\in S_d^+}(Px​)x∈Sd+​​ of laws on Ω\OmegaΩ under which XXX is a stochastically continuous Markov process with Px[X0=x]=1P_x[X_0=x]=1Px​[X0​=x]=1. The convolution P∗QP*QP∗Q is the image of P×QP\times QP×Q under (ω,ω′)↦ω+ω′(\omega,\omega')\mapsto\omega+\omega'(ω,ω′)↦ω+ω′. A family (Px)∈P(P_x)\in\mathcal P(Px​)∈P is infinitely decomposable (Definition 2.7) if for every k≥1k\ge1k≥1 there is (Px(k))∈P(P^{(k)}_x)\in\mathcal P(Px(k)​)∈P with Px(1)+⋯+x(k)=Px(1)(k)∗⋯∗Px(k)(k)P_{x^{(1)}+\dots+x^{(k)}}=P^{(k)}_{x^{(1)}}*\dots*P^{(k)}_{x^{(k)}}Px(1)+⋯+x(k)​=Px(1)(k)​∗⋯∗Px(k)(k)​. It is infinitely divisible if every marginal Px∘Xt−1P_x\circ X_t^{-1}Px​∘Xt−1​ is.

Formalization targets

Goal: Theorem 2.9 (p. 12)

For d≥2d\ge2d≥2 and (Px)∈P(P_x)\in\mathcal P(Px​)∈P, the following are equivalent:

(i) (Px) is infinitely decomposable  ⟺  (ii) X is affine with α=0  ⟺  (iii) X is affine and infinitely divisible.\text{(i) }(P_x)\text{ is infinitely decomposable}\iff\text{(ii) }X\text{ is affine with }\alpha=0\iff\text{(iii) }X\text{ is affine and infinitely divisible}.(i) (Px​) is infinitely decomposable⟺(ii) X is affine with α=0⟺(iii) X is affine and infinitely divisible.

Milestones

  • Lemma 6.1. An additive g:Sd+→Rg:S_d^+\to\mathbb Rg:Sd+​→R extends to an additive f:Sd→Rf:S_d\to\mathbb Rf:Sd​→R. If ggg is measurable, then f(x)=⟨c,x⟩f(x)=\langle c,x\ranglef(x)=⟨c,x⟩ for some c∈Sdc\in S_dc∈Sd​.
  • Lemma 6.2. A measurable, strictly positive hhh with h(x+y)=h(x)h(y)h(x+y)=h(x)h(y)h(x+y)=h(x)h(y) on Sd+S_d^+Sd+​ has the form h(x)=e−⟨c,x⟩h(x)=e^{-\langle c,x\rangle}h(x)=e−⟨c,x⟩, c∈Sdc\in S_dc∈Sd​. If h≤1h\le1h≤1, then c∈Sd+c\in S_d^+c∈Sd+​.
  • Lemma 6.4. For k≥2k\ge2k≥2, Px(1)(1)∗⋯∗Px(k)(k)=Px(0)P^{(1)}_{x^{(1)}}*\dots*P^{(k)}_{x^{(k)}}=P^{(0)}_{x}Px(1)(1)​∗⋯∗Px(k)(k)​=Px(0)​ holds iff every finite-dimensional Laplace functional has the form Ex(j)[e−∑i⟨u(i),Xti⟩]=ρ(j)e−⟨ψ,x⟩\mathbb E^{(j)}_x[e^{-\sum_i\langle u^{(i)},X_{t_i}\rangle}]=\rho^{(j)}e^{-\langle\psi,x\rangle}Ex(j)​[e−∑i​⟨u(i),Xti​​⟩]=ρ(j)e−⟨ψ,x⟩ with ∏i≥1ρ(i)=ρ(0)\prod_{i\ge1}\rho^{(i)}=\rho^{(0)}∏i≥1​ρ(i)=ρ(0).
  • Lemma 5.10. The cones C\mathcal CC (Lévy–Khintchine exponents plus a constant) and CS\mathcal C^SCS are closed under composition and pointwise limits. For α=0\alpha=0α=0, truncating small jumps of μ\muμ approximates RRR locally uniformly.
  • Proposition 5.11. For an admissible parameter set with α=0\alpha=0α=0, (φ(t,⋅),ψ(t,⋅))∈(C,CS)(\varphi(t,\cdot),\psi(t,\cdot))\in(\mathcal C,\mathcal C^S)(φ(t,⋅),ψ(t,⋅))∈(C,CS) for every t≥0t\ge0t≥0.

Significance

The theorem separates two classes that coincide on R+m×Rn\mathbb R_+^m\times\mathbb R^nR+m​×Rn. On Sd+S_d^+Sd+​ with d≥2d\ge2d≥2, a diffusion component, which must satisfy b⪰(d−1)αb\succeq(d-1)\alphab⪰(d−1)α, is incompatible with taking kkk-th roots, because the root would need drift b/kb/kb/k. So the existence proof of Duffie–Filipović–Schachermayer, which builds a process from infinitely divisible kernels, covers exactly the pure-jump affine processes on Sd+S_d^+Sd+​. Processes with a diffusion part need the martingale-problem approach of the paper's §5. Proposition 5.11 gives the alternative existence proof for α=0\alpha=0α=0 (§5.3).

The theorem is proved in the paper. As far as is known, none of it has been machine-checked: no formal library has affine processes on matrix cones, convolution of path measures, or the Lévy–Khintchine form on Sd+S_d^+Sd+​. Formalization contributes a checked equivalence that rests on the paper's other main theorem (Theorem 2.4), together with reusable statements about Cauchy's equations on cones and Laplace functionals of Markov families. It is the third mission of a series. Missions I and II formalize the two halves of Theorem 2.4.

Difficulty

The equivalence links three layers: path-space laws, one-dimensional kernels, and Riccati exponents. (i) ⇒\Rightarrow⇒ (ii) first needs the multiplicative structure of Laplace functionals in the initial state. That gives affinity of the process and of each kkk-th root, with exponents (φ/k,ψ)(\varphi/k,\psi)(φ/k,ψ). Then it needs the fact that the root's parameter set is (α,b/k,… )(\alpha,b/k,\dots)(α,b/k,…) and is again admissible, so b/k⪰(d−1)αb/k\succeq(d-1)\alphab/k⪰(d−1)α for all kkk. The second step relies on the full necessity theorem, in particular Proposition 4.18. The first fails without strict positivity of the Laplace functional: Cauchy's exponential equation has non-exponential solutions that vanish somewhere (Remark 6.3). (ii) ⇒\Rightarrow⇒ (iii) requires every Riccati solution to stay in the Lévy–Khintchine cone. This is clear for finite-variation jumps via Picard iteration, but the general case needs the approximation Rδ→RR^\delta\to RRδ→R. (iii) ⇒\Rightarrow⇒ (i) must produce a Markov family of kkk-th roots on path space, not merely roots of each marginal. The case d=1d=1d=1 shows that d≥2d\ge2d≥2 cannot be dropped: there the Cox–Ingersoll–Ross process has α≠0\alpha\ne0α=0 and is infinitely decomposable.

Formalization scope

  • Matrices. MdM_dMd​ is Fin d → Fin d → ℝ, with ⟨x,y⟩=∑i,jxijyji\langle x,y\rangle=\sum_{i,j}x_{ij}y_{ji}⟨x,y⟩=∑i,j​xij​yji​ and ∥x∥=⟨x,x⟩\|x\|=\sqrt{\langle x,x\rangle}∥x∥=⟨x,x⟩​. Sd+S_d^+Sd+​ is the subtype of matrices with Mathlib's PosSemidef.
  • Parameters. The matrix measure μ\muμ is encoded as H dνH\,d\nuHdν, with ν\nuν finite and HHH a positive semidefinite density. This is equivalent to the paper's μ\muμ; take ν=∑iμii\nu=\sum_i\mu_{ii}ν=∑i​μii​. Exponents are functions on R×Md\mathbb R\times M_dR×Md​, evaluated at t≥0t\ge0t≥0 and positive semidefinite uuu. Time derivatives at t=0t=0t=0 are one-sided.
  • Path space. Sd+∪{Δ}S_d^+\cup\{\Delta\}Sd+​∪{Δ} is OnePoint of the cone, with its Borel σ-algebra. Addition is extended with Δ\DeltaΔ absorbing. Ω\OmegaΩ is the space of all paths R≥0→Sd+∪{Δ}\mathbb R_{\ge0}\to S_d^+\cup\{\Delta\}R≥0​→Sd+​∪{Δ} with the product σ-algebra; every notion in the theorem depends only on finite-dimensional distributions. Absorption at Δ\DeltaΔ and the Markov property with transition family ppp are imposed through finite-dimensional distributions. The path-sum map is measurable, which is checked in Lean, so the convolution is a genuine push-forward.
  • Marginals. Infinite divisibility of a marginal is that of the sub-probability kernel pt(x,⋅)p_t(x,\cdot)pt​(x,⋅). Killed mass sits at Δ\DeltaΔ, so roots are sub-probabilities.
  • The parameter set. "Affine with α=0\alpha=0α=0" refers to the unique admissible parameter set whose F,RF,RF,R drive the Riccati equations. The truncation function χ\chiχ is arbitrary.
  • Corrections to the page. Lemma 6.4 carries the hypothesis k≥2k\ge2k≥2, from its proof ("Fix k>1k>1k>1"). For k=1k=1k=1 the statement is false. In Proposition 5.11, "the solutions" are the jointly continuous ones.
  • Ruled out. A kernel-level identity in place of infinite decomposability is ruled out: (i) is stated on path space. The goal keeps the hypothesis d≥2d\ge2d≥2.
  • Reusable work. Contributions are welcome on Cauchy's equations on cones (Lemmas 6.1–6.2), on the measure theory of path convolutions, and on Lévy–Khintchine exponents on Sd+S_d^+Sd+​. All three are useful beyond this mission.

Selected references

  • C. Cuchiero, D. Filipović, E. Mayerhofer, J. Teichmann, Affine processes on positive semidefinite matrices, Ann. Appl. Probab. 21 (2011) 397–463; arXiv:0910.0137v3. https://arxiv.org/abs/0910.0137
  • D. Duffie, D. Filipović, W. Schachermayer, Affine processes and applications in finance, Ann. Appl. Probab. 13 (2003) 984–1053. https://doi.org/10.1214/aoap/1060202833
  • M.-F. Bru, Wishart processes, J. Theoret. Probab. 4 (1991) 725–751. https://doi.org/10.1007/BF01259552
  • O. E. Barndorff-Nielsen, R. Stelzer, Positive-definite matrix processes of finite variation, Probab. Math. Statist. 27 (2007) 3–43.
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Captain: marwahaha

Midpoint convexity from bounded tree potentials and path costsOpen Problem

Motivation

A positive averaged midpoint modulus need not supply a positive one-sided asymptotic modulus. Tree-potential norms give explicit spaces in which to separate those notions. The pinned manuscript supplies the research context.

Setting

Coordinates are finite lists of natural numbers. Tests have bounded prefix potentials, one of the specified quadratic budgets and a budget-dependent support condition; the normed space is completed.

Formalization target

The selected goal is OAI.BoundedTreePotentials.TreeCalculus.main_counterexample. Its central assertion is

δ‾X(t)≥1+t2/4−1(0<t<1).\overline\delta_X(t)\geq\sqrt{1+t^2/4}-1\qquad(0<t<1).δX​(t)≥1+t2/4​−1(0<t<1).

The theorem states that, for every choice of a Boolean flag r (whether the root node, the empty list, is included as a coordinate) and every quadratic kind k among sibling, antichain and global, the following hold for the Banach space X = TestCompletion(treeTestFamily r k). Here nodes are finite lists of natural numbers, the potential of a coefficient function f at a node s is the sum of f over all prefixes of s, and a coefficient function f is a tree test if f vanishes at the root when r is false, every potential satisfies |potential f s| ≤ 1, a quadratic budget holds, and a support condition holds. The budget says that the sum of f(s)² over every admissible finite set B of nodes is at most 1, where admissible means: all of B are children of one common parent (sibling), pairwise prefix-incomparable (antichain), or any finite set (global). The support condition is vacuous for sibling, finite support for antichain, and square-summability for global. The tree test family is the set of such functions on the coordinates, and each finitely supported vector x is given the norm sup over tests f of |Σ x_i f_i|; X is the completion of this normed space. First, X is complete, separable, and not finite-dimensional over ℝ. Second, for every 0 < t < 1, the averaged modulus of X, defined as the infimum over unit vectors x of the supremum over closed finite-codimension subspaces F of the infimum over y in F with ‖y‖ ≥ 1 of (‖x+ty‖+‖x−ty‖)/2 − 1, is at least √(1+t²/4) − 1. Third, for every real normed space Y that is linearly homeomorphic to X, Y does not satisfy IsAUCReal, meaning it is false that the one-sided modulus (defined like the averaged one but with ‖y‖ = 1 and the quantity ‖x+ty‖ − 1) is positive for every t > 0.

Significance and status

The formal statement quantifies over both root flags and all three encoded quadratic kinds. Its claims are completeness, separability, infinite dimension, the stated modulus bound and no linearly equivalent AUC space. The target is currently Open on Prove2Me. The manuscript's mathematical argument and a machine-checked proof of the selected statement are separate deliverables.

Difficulty

The lower estimate must coexist with an obstruction to every equivalent AUC norm, not just failure for the original tree norm.

Formalization scope

The exact published goal, its hypotheses and its referenced definition blocks specify the requested formalization. The explanatory formula above is a summary; all quantifiers and additional clauses in the linked statement remain required.

The available published material supplies this goal and its necessary definitions. Additional manuscript lemmas are not represented as attached milestones.

Selected references

  • OpenAI, Midpoint convexity from bounded tree potentials and path costs, preprint, 2026. Manuscript.
  • OpenAI, accompanying formal statements, commit adc7f1241b42. Selected goal source.
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