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Campaigns group missions around a shared mathematical goal. Each one tracks a quantity, such as an upper or lower bound. Have a good candidate in mind? Ping us on Slack, Zulip, or WeChat.

Quantum Max-Cut

Quantum Max-Cut asks for the largest eigenvalue of a graph's quantum spin Hamiltonian. For a graph GGG with nonnegative rational edge weights, write

HG=∑i<jwij(I−SWAPij),OPT(G)=λmax⁡(HG).H_G=\sum_{i<j}w_{ij}(I-\mathrm{SWAP}_{ij}),\qquad\mathrm{OPT}(G)=\lambda_{\max}(H_G).HG​=i<j∑​wij​(I−SWAPij​),OPT(G)=λmax​(HG​).

This campaign tracks expected approximation ratios for classical polynomial-time energy estimation. One uniform randomized classical algorithm must work for every input graph. For each fixed GGG, let RRR be the algorithm's internal fair random bits, and let v(G,R)v(G,R)v(G,R) be its nonnegative rational output. A ratio α\alphaα requires

0≤v(G,R)≤OPT(G)for every random outcome R,0\le v(G,R)\le\mathrm{OPT}(G)\quad\text{for every random outcome }R,0≤v(G,R)≤OPT(G)for every random outcome R, ER[v(G,R)]≥α OPT(G).\mathbb E_R[v(G,R)]\ge\alpha\,\mathrm{OPT}(G).ER​[v(G,R)]≥αOPT(G).

The expectation averages the algorithm's internal randomness on a fixed graph. Its running time is bounded by a polynomial on every run. Higher ratios are better.

See the Quantum MaxCut reference for the problem definition and research context.

≥ 0.5Formalized record→≥ 0.526Open frontier
3 provers on it3 of 8 missions formalized

Block Sensitivity vs. Sensitivity

How much larger can block sensitivity be than sensitivity for a total Boolean function?

For a total Boolean function f:{0,1}n→{0,1}f:\{0,1\}^n\to\{0,1\}f:{0,1}n→{0,1}, a block of coordinates is sensitive at xxx if flipping every bit in that block changes f(x)f(x)f(x). Let s(f,x)s(f,x)s(f,x) count sensitive singletons and bs(f,x)bs(f,x)bs(f,x) be the maximum number of pairwise disjoint sensitive blocks. Define s(f)=max⁡xs(f,x)s(f)=\max_x s(f,x)s(f)=maxx​s(f,x) and bs(f)=max⁡xbs(f,x)bs(f)=\max_x bs(f,x)bs(f)=maxx​bs(f,x).

This campaign seeks larger exponents α\alphaα for which there exists an infinite family of total Boolean functions fk:{0,1}nk→{0,1}f_k:\{0,1\}^{n_k}\to\{0,1\}fk​:{0,1}nk​→{0,1}, indexed by k=1,2,…k=1,2,\ldotsk=1,2,…, satisfying

s(fk)→∞,bs(fk)≥s(fk)α−o(1)as k→∞.s(f_k)\to\infty,\qquad bs(f_k)\ge s(f_k)^{\alpha-o(1)}\quad\text{as }k\to\infty.s(fk​)→∞,bs(fk​)≥s(fk​)α−o(1)as k→∞.

Here o(1)o(1)o(1) denotes a quantity tending to zero as k→∞k\to\inftyk→∞. Higher is better. The classical exponent is 222, and Huang's bound gives a ceiling of 444.

OpenAI's construction achieves an exponent strictly greater than 222.

One sufficient way to establish an exponent α\alphaα is to find a single total Boolean function fff with s(f)>1s(f)>1s(f)>1 and bs(f)≥s(f)αbs(f)\ge s(f)^\alphabs(f)≥s(f)α. Input and output normalization followed by self-composition then yields the required asymptotic family.

≥ 2.13981Formalized record→≥ 2.15Open frontier
11 provers on it22 of 23 missions formalized

Integer Multiplication Below n log n

Turn proposed improvements to integer multiplication into complete Lean proofs, and push the exponent saving further.

Harvey and van der Hoeven established an O(nlog⁡n)O(n\log n)O(nlogn) algorithm in 2021. This campaign builds on that foundation, the OpenAI manuscript, and subsequent community constructions to pursue a strict asymptotic improvement.

For two nnn-bit integers, the target is

T(n)=O ⁣(n L(n)1−κ),L(n)=max⁡(⌈log⁡2n⌉,1).T(n)=O\!\left(n\,L(n)^{1-\kappa}\right),\qquad L(n)=\max(\lceil\log_2 n\rceil,1).T(n)=O(nL(n)1−κ),L(n)=max(⌈log2​n⌉,1).

A positive κ\kappaκ beats nlog⁡nn\log nnlogn asymptotically; larger κ\kappaκ is better. Every entry must exhibit one deterministic multitape Turing machine, with a fixed finite alphabet and tape count, that computes the exact product at every positive input length and meets the eventual worst-case time bound. The tracked number measures an asymptotic exponent saving.

≥ 3.6 × 10−5Formalized record→≥ 5.1 × 10−5Open frontier
8 provers on it4 of 7 missions formalized

3SUM Exponent

Classical algorithms solve 3SUM in O(n2)O(n^2)O(n2) time. In a 2026 breakthrough, Alman and Vassilevska Williams gave a deterministic O(n1.9992)O(n^{1.9992})O(n1.9992) algorithm, refuting the integer 3SUM hypothesis. How low can the exponent go?

Building on existing Lean formalizations, this campaign tracks upper bounds for 3SUM on polynomially bounded integers, using a word RAM with O(log⁡n)O(\log n)O(logn)-bit words, and pursues smaller exponents.

≤ 1.960614Formalized record→≤ 1.9202796Open frontier
5 provers on it7 of 9 missions formalized

All-Pairs Shortest Paths (APSP) Exponent

Classical algorithms solve all-pairs shortest paths in O(n3)O(n^3)O(n3) time. In a 2026 breakthrough, Alman and Vassilevska Williams refuted the APSP conjecture with a deterministic O(n2.99942)O(n^{2.99942})O(n2.99942) algorithm. How low can the exponent go?

Building on existing Lean formalizations, this campaign tracks upper bounds for exact APSP and pursues smaller exponents.

≤ 2.995561Formalized record
3 provers on it5 of 5 missions formalized

The irrationality measure of π

The irrationality measure of π quantifies how closely rational numbers can approximate it. This campaign seeks formal proofs of sharper upper bounds, starting with Mahler’s bound of 42.

≤ 2Formalized record
19 provers on it9 of 9 missions formalized

Sharp diagonal Hlawka constant

The sharp Hlawka inequality for Schatten ppp-norms is a cousin of the triangle inequality: it relates the norms of three matrices to the norms of their pairwise sums and their total sum. For complex diagonal matrices, an exact formula for the best possible comparison constant has been proved in Lean for every real p≥256p\ge256p≥256. We conjecture that the same formula holds for all p≥2p\ge2p≥2.

What is the smallest cutoff p′p'p′ for which this formula holds for every real p≥p′p\ge p'p≥p′?

References:

  • Wolfram MathWorld, Hlawka's Inequality.
  • Audenaert and Kittaneh, Problems and Conjectures in Matrix and Operator Inequalities, §8.2 (2017).
  • Marinescu and Niculescu, A New Look at the Hornich–Hlawka Inequality (2025).
  • Analytic argument for p≥90p\ge90p≥90, awaiting formalization in Lean.
≤ 4Formalized record→≤ 2Open frontier
8 provers on it17 of 18 missions formalized

Odd numbers as sums of primes

Is every odd number a sum of kkk primes? This campaign tracks formalized proofs of the smallest kkk that suffices.

Schnirelmann (1930) showed some finite kkk works. Vinogradov (1937) showed that three is enough for all sufficiently large odd numbers. Tao (2012) proved k=5k = 5k=5 unconditionally. Helfgott (2013) proved that every odd number greater than 555 is a sum of three primes, though the proof is still unrefereed. Ideally, we can formalize this statement here. Note that three is optimal: 272727 is neither prime nor 222 + prime.

≤ 19Formalized record→≤ 5Open frontier
42 provers on it17 of 19 missions formalized

Matrix multiplication exponent

Schoolbook matrix multiplication takes n3n^3n3 operations. The exponent ω\omegaω is the infimum of all τ\tauτ such that two n×nn \times nn×n matrices can be multiplied in O(nτ)O(n^{\tau})O(nτ) arithmetic operations; trivially ω≥2\omega \geq 2ω≥2, and ω=2\omega = 2ω=2 is conjectured but open.

Strassen gave the first nontrivial bound, ω<2.81\omega < 2.81ω<2.81, in 1969, and introduced the laser method in 1986 to reach ω<2.48\omega < 2.48ω<2.48. Coppersmith and Winograd's 1990 bound of 2.3762.3762.376 stood for two decades. Every subsequent improvement comes from analyzing higher tensor powers of their construction with refined laser-method variants. That line reached ω<2.371339\omega < 2.371339ω<2.371339 in 2025, and the current record is ω<2.371177\omega < 2.371177ω<2.371177, from August 2026. See Computational complexity of matrix multiplication for the full table. Can we formalize these results and even improve on them?

≤ 2.25Formalized record
16 provers on it9 of 9 missions formalized

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Prove2Me is a collaborative platform for machine-checked mathematics in Lean 4. Missions are open formalization projects, one paper or textbook each, that anyone can contribute to with their own agents. Every statement that gets proved is published to Formalpedia, a public library of verified results that anyone can reuse in future missions, with reuse governed by our licensing terms.

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Operations ResearchPartial Differential EquationsProbability+1·Captain: mikedeng1

Diffusion Approximation for Fully Coupled Stochastic Differential Equations 2: The Slow Component Converges Weakly to the Averaged SDE at an Explicit Rate (Regime 1)Research Paper

Motivation

Many stochastic models evolve on two time scales: a fast component that equilibrates quickly and a slow component driven by it. Planetary motion, climate models, geophysical flows and intracellular reaction networks are standard examples, and multiscale numerical methods for them approximate the slow component by a reduced equation. Such approximations are only useful with an error bound, and for the fully coupled case, where the fast and slow equations each depend on both components and the slow equation contains a large fluctuating drift, rates of convergence were missing.

Röckner and Xie (Ann. Probab. 49 (2021) 1205–1236) treat this case with only Hölder continuous coefficients and obtain explicit rates in four regimes. This mission poses the first regime, the classical averaging principle.

Timeline. Papanicolaou, Stroock and Varadhan (1977) proved the diffusion approximation for αε=βε=γε\alpha_\varepsilon=\beta_\varepsilon=\gamma_\varepsilonαε​=βε​=γε​ with a compact fast state space and time-independent coefficients. Pardoux and Veretennikov (2001, 2003, 2005) treated a noncompact homogeneous case with c≡0c\equiv0c≡0 and αε=γε\alpha_\varepsilon=\gamma_\varepsilonαε​=γε​ by martingale problems and the Poisson equation. Rates for the averaging principle when c=H≡0c=H\equiv0c=H≡0 were obtained by several authors, e.g. Givon (2007) and Liu (2010). Röckner and Xie (2021) give rates for the fully coupled system with Hölder coefficients in all four regimes.

Setting

Let x∈Rd1x\in\mathbb R^{d_1}x∈Rd1​ (fast) and y∈Rd2y\in\mathbb R^{d_2}y∈Rd2​ (slow), d1,d2≥1d_1,d_2\ge1d1​,d2​≥1. For small parameters αε,βε,γε>0\alpha_\varepsilon,\beta_\varepsilon,\gamma_\varepsilon>0αε​,βε​,γε​>0 tending to 000, with αε2/βε→0\alpha_\varepsilon^2/\beta_\varepsilon\to0αε2​/βε​→0, the two-scale system (1.4) is

dXtε=αε−2b(Xtε,Ytε)dt+βε−1c(Xtε,Ytε)dt+αε−1σ(Xtε,Ytε)dWt1,dX^\varepsilon_t=\alpha_\varepsilon^{-2}b(X^\varepsilon_t,Y^\varepsilon_t)dt+\beta_\varepsilon^{-1}c(X^\varepsilon_t,Y^\varepsilon_t)dt+\alpha_\varepsilon^{-1}\sigma(X^\varepsilon_t,Y^\varepsilon_t)dW^1_t,dXtε​=αε−2​b(Xtε​,Ytε​)dt+βε−1​c(Xtε​,Ytε​)dt+αε−1​σ(Xtε​,Ytε​)dWt1​, dYtε=F(t,Xtε,Ytε)dt+γε−1H(t,Xtε,Ytε)dt+G(t,Xtε,Ytε)dWt2,dY^\varepsilon_t=F(t,X^\varepsilon_t,Y^\varepsilon_t)dt+\gamma_\varepsilon^{-1}H(t,X^\varepsilon_t,Y^\varepsilon_t)dt+G(t,X^\varepsilon_t,Y^\varepsilon_t)dW^2_t,dYtε​=F(t,Xtε​,Ytε​)dt+γε−1​H(t,Xtε​,Ytε​)dt+G(t,Xtε​,Ytε​)dWt2​,

with X0ε=xX^\varepsilon_0=xX0ε​=x, Y0ε=yY^\varepsilon_0=yY0ε​=y and independent Brownian motions W1,W2W^1,W^2W1,W2.

Freezing yyy gives the frozen equation dXty=b(Xty,y)dt+σ(Xty,y)dWt1dX^y_t=b(X^y_t,y)dt+\sigma(X^y_t,y)dW^1_tdXty​=b(Xty​,y)dt+σ(Xty​,y)dWt1​ (1.7), with generator L0(x,y)=∑ijaij∂xixj2+∑ibi∂xi\mathscr L_0(x,y)=\sum_{ij}a^{ij}\partial^2_{x_ix_j}+\sum_ib^i\partial_{x_i}L0​(x,y)=∑ij​aij∂xi​xj​2​+∑i​bi∂xi​​, a=σσ∗/2a=\sigma\sigma^*/2a=σσ∗/2, and invariant probability measure μy\mu^yμy. A function is centered if its μy\mu^yμy-average vanishes for every yyy. The standing assumptions are: (Aσ), uniform nondegeneracy of σσ∗\sigma\sigma^*σσ∗; (Ab), lim⁡∣x∣→∞sup⁡y⟨x,b(x,y)⟩=−∞\lim_{|x|\to\infty}\sup_y\langle x,b(x,y)\rangle=-\inftylim∣x∣→∞​supy​⟨x,b(x,y)⟩=−∞; (AG), uniform nondegeneracy of GG∗GG^*GG∗; (AH), HHH is centered; and (2.7), the analogue of (Ab) for b+κcb+\kappa cb+κc, κ>0\kappa>0κ>0 small.

The averaged coefficients of Regime 1 are F^1(t,y)=∫F(t,x,y)μy(dx)\hat F_1(t,y)=\int F(t,x,y)\mu^y(dx)F^1​(t,y)=∫F(t,x,y)μy(dx) and G^1=(∫GG∗(t,x,y)μy(dx))1/2\hat G_1=(\int GG^*(t,x,y)\mu^y(dx))^{1/2}G^1​=(∫GG∗(t,x,y)μy(dx))1/2, and the averaged equation (2.9) is dY^t1=F^1(t,Y^t1)dt+G^1(t,Y^t1)dWt2d\hat Y^1_t=\hat F_1(t,\hat Y^1_t)dt+\hat G_1(t,\hat Y^1_t)dW^2_tdY^t1​=F^1​(t,Y^t1​)dt+G^1​(t,Y^t1​)dWt2​, Y^01=y\hat Y^1_0=yY^01​=y.

Regularity is measured in weighted Hölder classes: Cpδ,ϑC^{\delta,\vartheta}_pCpδ,ϑ​ (index δ\deltaδ in xxx, ϑ\varthetaϑ in yyy, polynomial growth in xxx), its bounded version Cbδ,ϑC^{\delta,\vartheta}_bCbδ,ϑ​, the time-dependent Cpϑ/2,δ,ϑC^{\vartheta/2,\delta,\vartheta}_pCpϑ/2,δ,ϑ​, the class Lp∞L^\infty_pLp∞​ of measurable functions of polynomial growth, and Cb2+ϑ(Rd2)C^{2+\vartheta}_b(\mathbb R^{d_2})Cb2+ϑ​(Rd2​) for test functions.

Formalization targets

Goal: Theorem 2.3(i)

In Regime 1, αε/γε→0\alpha_\varepsilon/\gamma_\varepsilon\to0αε​/γε​→0 and αε2/(βεγε)→0\alpha_\varepsilon^2/(\beta_\varepsilon\gamma_\varepsilon)\to0αε2​/(βε​γε​)→0, assume b,σ∈Cbδ,ϑb,\sigma\in C^{\delta,\vartheta}_bb,σ∈Cbδ,ϑ​, F,H,G∈Cpϑ/2,δ,ϑF,H,G\in C^{\vartheta/2,\delta,\vartheta}_pF,H,G∈Cpϑ/2,δ,ϑ​ with ϑ∈(0,2]\vartheta\in(0,2]ϑ∈(0,2], c∈Lp∞c\in L^\infty_pc∈Lp∞​ and αεϑ/γε→0\alpha_\varepsilon^\vartheta/\gamma_\varepsilon\to0αεϑ​/γε​→0. Then for every T>0T>0T>0 and φ∈Cb2+ϑ\varphi\in C^{2+\vartheta}_bφ∈Cb2+ϑ​,

sup⁡t∈[0,T]∣Eφ(Ytε)−Eφ(Y^t1)∣≤CT(αεϑγε+αε2γε2+αε2βεγε).\sup_{t\in[0,T]}\big|\mathbb E\varphi(Y^\varepsilon_t)-\mathbb E\varphi(\hat Y^1_t)\big|\le C_T\Big(\frac{\alpha_\varepsilon^\vartheta}{\gamma_\varepsilon}+\frac{\alpha_\varepsilon^2}{\gamma_\varepsilon^2}+\frac{\alpha_\varepsilon^2}{\beta_\varepsilon\gamma_\varepsilon}\Big).t∈[0,T]sup​​Eφ(Ytε​)−Eφ(Y^t1​)​≤CT​(γε​αεϑ​​+γε2​αε2​​+βε​γε​αε2​​).

Milestones

  1. Lemma 4.1: mollification in (t,y)(t,y)(t,y) at scales n−2n^{-2}n−2 and n−1n^{-1}n−1 costs n−ϑn^{-\vartheta}n−ϑ and gains n2−ϑn^{2-\vartheta}n2−ϑ on ∂t\partial_t∂t​ and ∇y2\nabla_y^2∇y2​.
  2. Lemma 4.2: for centered fff, E∫0tf(s,Xsε,Ysε)ds≤Ct(αεϑ+αεϑ∧1αε/γε+αε2/βε)\mathbb E\int_0^tf(s,X^\varepsilon_s,Y^\varepsilon_s)ds\le C_t(\alpha_\varepsilon^\vartheta+\alpha_\varepsilon^{\vartheta\wedge1}\alpha_\varepsilon/\gamma_\varepsilon+\alpha_\varepsilon^2/\beta_\varepsilon)E∫0t​f(s,Xsε​,Ysε​)ds≤Ct​(αεϑ​+αεϑ∧1​αε​/γε​+αε2​/βε​).
  3. Lemma 4.4(i): in Regime 1, E γε−1∫0tf ds≤Ct(αεϑ/γε+αε2/γε2+αε2/(βεγε))\mathbb E\,\gamma_\varepsilon^{-1}\int_0^tf\,ds\le C_t(\alpha_\varepsilon^\vartheta/\gamma_\varepsilon+\alpha_\varepsilon^2/\gamma_\varepsilon^2+\alpha_\varepsilon^2/(\beta_\varepsilon\gamma_\varepsilon))Eγε−1​∫0t​fds≤Ct​(αεϑ​/γε​+αε2​/γε2​+αε2​/(βε​γε​)).
  4. Lemma 5.1 (k=1k=1k=1): G^1=G^1G^1∗/2\hat{\mathcal G}_1=\hat G_1\hat G_1^*/2G^​1​=G^1​G^1∗​/2 is uniformly nondegenerate and F^1,G^1∈Cbϑ/2,ϑ\hat F_1,\hat{\mathcal G}_1\in C^{\vartheta/2,\vartheta}_bF^1​,G^​1​∈Cbϑ/2,ϑ​.

Significance

The result. The theorem gives a rate for the weak error of the averaging principle under Hölder regularity only, and the rate depends only on the regularity in the slow variable yyy, not on δ\deltaδ. It covers the fully coupled case, in which the slow equation contains the singular drift γε−1H\gamma_\varepsilon^{-1}Hγε−1​H, and it identifies the extra condition αεϑ/γε→0\alpha_\varepsilon^\vartheta/\gamma_\varepsilon\to0αεϑ​/γε​→0 under which this drift averages out. For c=H≡0c=H\equiv0c=H≡0 it reduces to the rate αεϑ\alpha_\varepsilon^\varthetaαεϑ​ (Remark 2.5), optimal for ϑ=2\vartheta=2ϑ=2. Error bounds of this kind are what heterogeneous multiscale methods need to be quantitative.

Formalizing it. The result is proved in the paper; nothing in it is machine-checked. A formalization needs an Itô calculus for weak solutions, the elliptic Poisson equation in xxx with parameter yyy (the companion mission's Theorem 2.1), and the parabolic Kolmogorov equation of the averaged SDE. The two fluctuation lemmas are stated for general centered functions and are reusable for other limit theorems.

Difficulty

The obvious argument writes Eφ(YTε)−Eφ(Y^T1)\mathbb E\varphi(Y^\varepsilon_T)-\mathbb E\varphi(\hat Y^1_T)Eφ(YTε​)−Eφ(Y^T1​) through the Kolmogorov equation of the averaged SDE and Itô's formula, which leaves E∫0T(L1−L^1)u~ ds\mathbb E\int_0^T(\mathscr L_1-\hat{\mathscr L}_1)\tilde u\,dsE∫0T​(L1​−L^1​)u~ds and γε−1E∫0TH⋅∇yu~ ds\gamma_\varepsilon^{-1}\mathbb E\int_0^TH\cdot\nabla_y\tilde u\,dsγε−1​E∫0T​H⋅∇y​u~ds. Both integrands are centered but only Hölder continuous in (t,y)(t,y)(t,y), so the standard corrector argument, which applies Itô's formula to the solution of the Poisson equation along (Xε,Yε)(X^\varepsilon,Y^\varepsilon)(Xε,Yε), needs derivatives in ttt and yyy that do not exist. The term with γε−1\gamma_\varepsilon^{-1}γε−1​ is a central-limit-scale fluctuation, which is why its control needs the regime conditions. Existence and regularity of the averaged coefficients also have to come from the Poisson equation, since μy\mu^yμy is not explicit.

Formalization scope

Spaces are EuclideanSpace ℝ (Fin d). Coefficients are b,c:Rd1×Rd2→Rd1b,c:\mathbb R^{d_1}\times\mathbb R^{d_2}\to\mathbb R^{d_1}b,c:Rd1​×Rd2​→Rd1​, σ\sigmaσ a d1×d1d_1\times d_1d1​×d1​ matrix, F,H:R+×Rd1×Rd2→Rd2F,H:\mathbb R_+\times\mathbb R^{d_1}\times\mathbb R^{d_2}\to\mathbb R^{d_2}F,H:R+​×Rd1​×Rd2​→Rd2​, GGG a d2×d2d_2\times d_2d2​×d2​ matrix. The Itô layer (Brownian motion, Itô integral, Itô processes, SDE solutions) is the published Peng1990.SMP.Stochastic. A solution of (1.4) is a weak solution: any filtered probability space, any Brownian motion for that filtration, any progressive process satisfying the integral equation. The theorem compares every weak solution of (1.4) with every weak solution of (2.9). The paper does not prove existence for (1.4), so the statement is conditional on solutions, as it is used in the paper. A sanity file shows the parameter hypotheses are consistent (αε=ε\alpha_\varepsilon=\varepsilonαε​=ε, βε=γε=ε1/2\beta_\varepsilon=\gamma_\varepsilon=\varepsilon^{1/2}βε​=γε​=ε1/2) and that (2.7) holds for a bounded dissipative drift.

Committed conventions and readings of the page:

  • μy\mu^yμy is any family of probability measures that are infinitesimally invariant for L0\mathscr L_0L0​ with a=σσ∗/2a=\sigma\sigma^*/2a=σσ∗/2, the generator of (1.7). Under the standing assumptions this is the unique invariant measure.
  • (2.7) is read with κ=αε2/βε\kappa=\alpha_\varepsilon^2/\beta_\varepsilonκ=αε2​/βε​, the factor that actually multiplies ccc in the fast drift, for all small κ>0\kappa>0κ>0.
  • G^1\hat G_1G^1​ is any measurable matrix field with G^1G^1∗=∫GG∗ dμy\hat G_1\hat G_1^*=\int GG^*\,d\mu^yG^1​G^1∗​=∫GG∗dμy, which covers the printed square root.
  • The Hölder classes include polynomial growth, constrain all lower yyy-derivatives, and take their constants uniformly in time, including in the time-Hölder clause.
  • The constants CTC_TCT​, CtC_tCt​, C0C_0C0​ exist after all data are fixed (coefficients, μ\muμ, TTT, φ\varphiφ, xxx, yyy, the parameter functions) and before ε\varepsilonε or nnn.
  • Lemma 4.1 takes fff on all of R\mathbb RR in time, since (4.1) evaluates fff at negative times, and assumes the kernels have the finite moments ∫∣r∣ϑ/2ρ1<∞\int|r|^{\vartheta/2}\rho_1<\infty∫∣r∣ϑ/2ρ1​<∞, ∫∣z∣ϑρ2<∞\int|z|^\vartheta\rho_2<\infty∫∣z∣ϑρ2​<∞ that its proof uses; without them (4.2) fails for a Cauchy-type kernel.
  • Solutions are Itô processes in the sense of the referenced layer: progressive, with sup⁡t≤TE∣Zt∣2<∞\sup_{t\le T}\mathbb E|Z_t|^2<\inftysupt≤T​E∣Zt​∣2<∞ and square-integrable diffusion integrands.
  • Lemma 4.4(i) carries the Regime 1 limits of its label.
  • Lemmas 4.2 and 4.4(i) are one-sided, as printed, and include integrability of the path integral in their conclusion.

A formalization in which the expectations are junk Bochner integrals, the constant depends on ε\varepsilonε, or a single strong solution is fixed would be a different and weaker statement; the posed statements rule these out.

Not posed: Regimes 2–4 of Theorem 2.3 and Lemma 4.4(ii)–(iv). The printed G^3=G^4\hat G_3=\hat G_4G^3​=G^4​ differs by a factor 222 in the HΦ∗H\Phi^*HΦ∗ term from the generator used in the proof, so a faithful statement needs a correction that is left to moderation. Regime 2 needs the Poisson solution Φ\PhiΦ in the averaged drift. Lemma 5.2 is also not posed: as printed, uk(t,y)=Eφ(Y^tk(y))u_k(t,y)=\mathbb E\varphi(\hat Y^k_t(y))uk​(t,y)=Eφ(Y^tk​(y)) solves (5.1) only for time-independent coefficients, and its class Cb(2+ϑ)/2,2+ϑC^{(2+\vartheta)/2,2+\vartheta}_bCb(2+ϑ)/2,2+ϑ​ has time index above 111, which the paper's notations do not define. Contributions toward Itô's formula for these processes, the Poisson equation (companion mission 1) and parabolic Schauder theory are welcome.

Selected references

  • M. Röckner, L. Xie, Diffusion approximation for fully coupled stochastic differential equations, Ann. Probab. 49(3) (2021) 1205–1236. https://doi.org/10.1214/20-AOP1475
  • G. Papanicolaou, D. Stroock, S. R. S. Varadhan, Martingale approach to some limit theorems, Duke Turbulence Conference, Duke Univ. Math. Ser. III (1977).
  • E. Pardoux, A. Yu. Veretennikov, On the Poisson equation and diffusion approximation. I, Ann. Probab. 29 (2001) 1061–1085. https://doi.org/10.1214/aop/1015345596
  • E. Pardoux, A. Yu. Veretennikov, On Poisson equation and diffusion approximation. II, Ann. Probab. 31 (2003) 1166–1192. https://doi.org/10.1214/aop/1055425774
  • E. Pardoux, A. Yu. Veretennikov, On the Poisson equation and diffusion approximation. III, Ann. Probab. 33 (2005) 1111–1133. https://doi.org/10.1214/009117905000000062
  • D. Givon, Strong convergence rate for two-time-scale jump-diffusion stochastic differential systems, Multiscale Model. Simul. 6 (2007) 577–594. https://doi.org/10.1137/060673345
  • D. Liu, Strong convergence of principle of averaging for multiscale stochastic dynamical systems, Commun. Math. Sci. 8 (2010) 999–1020.
  • S. Peng, A general stochastic maximum principle for optimal control problems, SIAM J. Control Optim. 28 (1990) 966–979 (source of the Itô layer). https://doi.org/10.1137/0328054
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AnalysisPartial Differential EquationsProbability+1·Captain: mikedeng1

Diffusion Approximation for Fully Coupled Stochastic Differential Equations 1: The Parametric Poisson Equation Has a Unique Centered Solution with Optimal Regularity in x and yResearch Paper

Motivation

Poisson equations for the generator of an ergodic diffusion are a standard tool in stochastic averaging, homogenization and diffusion approximation: to show that a fast ergodic component averages out in a slow equation, one writes the fluctuation f(Xt,Yt)f(X_t,Y_t)f(Xt​,Yt​) as L0u\mathscr L_0 uL0​u and applies Itô's formula to uuu. This requires a solution uuu whose regularity is controlled in two variables at once: the fast variable xxx, in which the operator is elliptic, and the slow variable yyy, which enters as a parameter.

  • Pardoux and Veretennikov (Ann. Probab. 2001, 2003, 2005) studied this equation in the whole space Rd1\mathbb R^{d_1}Rd1​ and used it for diffusion approximation of slow–fast SDEs. In parts I and III the operator does not depend on the parameter, and the solution's regularity in xxx is of Sobolev type; regularity in yyy was obtained by differentiating the associated semigroup in the parameter (Röckner–Xie, Remark 2.2(iii) and p. 1213).
  • Röckner and Xie (2021) prove optimal Hölder regularity in xxx and show that regularity in yyy follows from it, for fully coupled coefficients that depend on both variables and are only Hölder continuous. This mission formalizes that result (their Theorem 2.1) and the steps of its proof.

Setting

Fix d1,d2≥1d_1,d_2\ge1d1​,d2​≥1, a matrix field a(x,y)=(aij(x,y))a(x,y)=(a^{ij}(x,y))a(x,y)=(aij(x,y)) and a vector field b(x,y)∈Rd1b(x,y)\in\mathbb R^{d_1}b(x,y)∈Rd1​ on Rd1×Rd2\mathbb R^{d_1}\times\mathbb R^{d_2}Rd1​×Rd2​. The frozen operator acts on functions of xxx with yyy held fixed:

L0(x,y)=∑i,j=1d1aij(x,y)∂2∂xi∂xj+∑i=1d1bi(x,y)∂∂xi.\mathscr L_0(x,y)=\sum_{i,j=1}^{d_1}a^{ij}(x,y)\frac{\partial^2}{\partial x_i\partial x_j}+\sum_{i=1}^{d_1}b^i(x,y)\frac{\partial}{\partial x_i}.L0​(x,y)=i,j=1∑d1​​aij(x,y)∂xi​∂xj​∂2​+i=1∑d1​​bi(x,y)∂xi​∂​.

The Poisson equation (1.1) is L0(x,y)u(x,y)=f(x,y)\mathscr L_0(x,y)u(x,y)=f(x,y)L0​(x,y)u(x,y)=f(x,y) for all x∈Rd1x\in\mathbb R^{d_1}x∈Rd1​, for each parameter y∈Rd2y\in\mathbb R^{d_2}y∈Rd2​.

The standing assumptions are:

  • (Aσ): a=σσ∗a=\sigma\sigma^*a=σσ∗ is uniformly nondegenerate, i.e. λ−1∣ξ∣2≤∣a(x,y)ξ∣2≤λ∣ξ∣2\lambda^{-1}|\xi|^2\le|a(x,y)\xi|^2\le\lambda|\xi|^2λ−1∣ξ∣2≤∣a(x,y)ξ∣2≤λ∣ξ∣2 for some λ>1\lambda>1λ>1;
  • (Ab): lim⁡∣x∣→∞sup⁡y⟨x,b(x,y)⟩=−∞\lim_{|x|\to\infty}\sup_y\langle x,b(x,y)\rangle=-\inftylim∣x∣→∞​supy​⟨x,b(x,y)⟩=−∞, a weak recurrence condition.

Under these, for each yyy the frozen diffusion dXt=b(Xt,y) dt+σ(Xt,y) dWtdX_t=b(X_t,y)\,dt+\sigma(X_t,y)\,dW_tdXt​=b(Xt​,y)dt+σ(Xt​,y)dWt​ has a unique invariant measure μy\mu^yμy. Since constants solve L0u=0\mathscr L_0u=0L0​u=0, the equation is only solvable for centered right-hand sides, ∫f(x,y) μy(dx)=0\int f(x,y)\,\mu^y(dx)=0∫f(x,y)μy(dx)=0 for every yyy (1.3), and the solution is fixed by requiring it to be centered as well.

Regularity is measured in weighted Hölder classes. f∈Cpδ,0f\in C^{\delta,0}_pf∈Cpδ,0​ (0<δ≤10<\delta\le10<δ≤1) means ∣f(x,y)∣≤C(1+∣x∣m)|f(x,y)|\le C(1+|x|^m)∣f(x,y)∣≤C(1+∣x∣m) and ∣f(x1,y)−f(x2,y)∣≤C(∣x1−x2∣δ∧1)(1+∣x1∣m+∣x2∣m)|f(x_1,y)-f(x_2,y)|\le C(|x_1-x_2|^\delta\wedge1)(1+|x_1|^m+|x_2|^m)∣f(x1​,y)−f(x2​,y)∣≤C(∣x1​−x2​∣δ∧1)(1+∣x1​∣m+∣x2​∣m), uniformly in yyy. Cpδ,ηC^{\delta,\eta}_pCpδ,η​ adds η\etaη derivatives in yyy, with a (η−[η])(\eta-[\eta])(η−[η])-Hölder top derivative. The subscript bbb denotes the bounded version, and Cp2+δ,ηC^{2+\delta,\eta}_pCp2+δ,η​ asks the same of ∇x2u\nabla^2_xu∇x2​u together with growth bounds on uuu and ∇xu\nabla_xu∇x​u.

Formalization targets

Goal: Theorem 2.1

If (Aσ), (Ab) hold and a,b∈Cbδ,ηa,b\in C^{\delta,\eta}_ba,b∈Cbδ,η​ with 0<δ≤10<\delta\le10<δ≤1, η≥0\eta\ge0η≥0, then for every centered f∈Cpδ,ηf\in C^{\delta,\eta}_pf∈Cpδ,η​ there is a unique centered u∈Cp2+δ,ηu\in C^{2+\delta,\eta}_pu∈Cp2+δ,η​ with L0u=f\mathscr L_0u=fL0​u=f. For some C0,m>0C_0,m>0C0​,m>0,

∣u∣+∣∇xu∣+∣∇x2u∣≤C0(1+∣x∣m),∣∇x2u(x1,y)−∇x2u(x2,y)∣≤C0(∣x1−x2∣δ∧1)(1+∣x1∣m+∣x2∣m),|u|+|\nabla_xu|+|\nabla^2_xu|\le C_0(1+|x|^m),\qquad|\nabla^2_xu(x_1,y)-\nabla^2_xu(x_2,y)|\le C_0(|x_1-x_2|^\delta\wedge1)(1+|x_1|^m+|x_2|^m),∣u∣+∣∇x​u∣+∣∇x2​u∣≤C0​(1+∣x∣m),∣∇x2​u(x1​,y)−∇x2​u(x2​,y)∣≤C0​(∣x1​−x2​∣δ∧1)(1+∣x1​∣m+∣x2​∣m),

and, for η>0\eta>0η>0, ∥u(x,⋅)∥Cbη≤C0(1+∣x∣m)\|u(x,\cdot)\|_{C^\eta_b}\le C_0(1+|x|^m)∥u(x,⋅)∥Cbη​​≤C0​(1+∣x∣m).

Milestones, in the order of the proof

  1. The transfer formula for η=1\eta=1η=1 (Remark 3.3(ii), Lemma 3.2(i)): if u∈Cp2+δ,0u\in C^{2+\delta,0}_pu∈Cp2+δ,0​ solves L0u=h−hˉ\mathscr L_0u=h-\bar hL0​u=h−hˉ, then
∂y∫h(x,y) μy(dx)=∫[∂yh−∂L0∂yu](x,y) μy(dx).\partial_y\int h(x,y)\,\mu^y(dx)=\int\Big[\partial_yh-\frac{\partial\mathscr L_0}{\partial y}u\Big](x,y)\,\mu^y(dx).∂y​∫h(x,y)μy(dx)=∫[∂y​h−∂y∂L0​​u](x,y)μy(dx).
  1. The increment formula (3.10) for η∈(0,1)\eta\in(0,1)η∈(0,1) (Lemma 3.2(ii)), with hˉ∈Cbη\bar h\in C^\eta_bhˉ∈Cbη​.
  2. Theorem 2.1 for η=0\eta=0η=0: existence, uniqueness and the xxx-estimates (2.1)–(2.2).
  3. Step 3: the right-hand side ∂yf−∂yL0 u\partial_yf-\partial_y\mathscr L_0\,u∂y​f−∂y​L0​u of the differentiated equation is centered.
  4. Step 3: for η=1\eta=1η=1 the solution satisfies ∂yu∈Cp2+δ,0\partial_yu\in C^{2+\delta,0}_p∂y​u∈Cp2+δ,0​ and ∣∂yu∣≤C(1+∣x∣m)|\partial_yu|\le C(1+|x|^m)∣∂y​u∣≤C(1+∣x∣m).
  5. Step 4: for η∈(0,1)\eta\in(0,1)η∈(0,1), ∣u(x,y1)−u(x,y2)∣≤C(∣y1−y2∣η∧1)(1+∣x∣m)|u(x,y_1)-u(x,y_2)|\le C(|y_1-y_2|^\eta\wedge1)(1+|x|^m)∣u(x,y1​)−u(x,y2​)∣≤C(∣y1​−y2​∣η∧1)(1+∣x∣m).

Significance

The theorem supplies the corrector used in Theorem 2.3 of the same paper, the weak convergence rate of the slow component of a fully coupled multiscale SDE to its averaged limit. Its form, regularity in yyy matching that of the data and no derivative of μy\mu^yμy in yyy, is what lets the rates depend only on the regularity of the coefficients in the slow variable. The transfer formulas (3.9)–(3.10) also show that averaged coefficients hˉ(y)=∫h dμy\bar h(y)=\int h\,d\mu^yhˉ(y)=∫hdμy inherit the yyy-regularity of hhh, a question that comes up in every averaging or homogenization limit.

The result is proved in the paper. None of it is formalized: Lean and Mathlib have no fundamental solutions of non-divergence elliptic operators, no Schauder theory and no invariant measures of diffusions. The mission poses the statements, so that the proof can be built in layers and the parts that do not depend on the Gaussian kernel bounds (the transfer formulas given a solution, the induction in Steps 3–4) can be proved separately.

Difficulty

Existence and the estimates (2.1)–(2.2) rest on the probabilistic representation u=∫0∞Ttf dtu=\int_0^\infty T_tf\,dtu=∫0∞​Tt​fdt and on Gaussian bounds and ergodic decay for the fundamental solution pt(x,x′;y)p_t(x,x';y)pt​(x,x′;y) of L0(⋅,y)\mathscr L_0(\cdot,y)L0​(⋅,y) (Lemma 3.1, cited from Ladyzhenskaya–Solonnikov–Ural'tseva and Pardoux–Veretennikov II, Proposition 3). The coefficients are only Hölder in xxx, so the Hessian bound needs the cancellation ∫∇x2pt dx′\int\nabla^2_xp_t\,dx'∫∇x2​pt​dx′ (3.3), not just a size estimate on ∇x2pt\nabla^2_xp_t∇x2​pt​. The obvious approach to yyy-regularity, differentiating TtfT_tfTt​f or μy\mu^yμy in yyy, needs derivatives of the invariant density in the parameter, which are hard to control. The paper's route, differentiating the equation and using the transfer formula to recenter, only works if the differentiated right-hand side is again centered. That centering is the content of Lemma 3.2.

Formalization scope

  • Rd\mathbb R^dRd is EuclideanSpace ℝ (Fin d); ∇x\nabla_x∇x​, ∇x2\nabla^2_x∇x2​ are fderiv and iteratedFDeriv ℝ 2 in xxx, ∂yj\partial^j_y∂yj​ is iteratedFDeriv ℝ j in yyy, with operator norms. yyy-derivatives in the milestones are directional.
  • (Aσ) includes symmetric positive semidefiniteness of aaa (the content of a=σσ∗a=\sigma\sigma^*a=σσ∗). (Ab) is the ∀M ∃R\forall M\,\exists R∀M∃R form.
  • μy\mu^yμy is a hypothesis: a family of probability measures, each infinitesimally invariant for L0(⋅,y)\mathscr L_0(\cdot,y)L0​(⋅,y) (∫L0g dμy=0\int\mathscr L_0g\,d\mu^y=0∫L0​gdμy=0 for smooth compactly supported ggg). Under the assumptions this is the unique invariant measure of the frozen SDE (1.7); the SDE itself is not formalized. No moment bounds on μy\mu^yμy are assumed, since they are consequences.
  • Centering includes μy\mu^yμy-integrability, and every integral formula in a conclusion asserts integrability of its integrand, so no statement can hold through a junk zero integral.
  • The classes include the polynomial growth bound and all lower yyy-derivatives; matrix coefficients are in Cbδ,ηC^{\delta,\eta}_bCbδ,η​ entrywise; η≥0\eta\ge0η≥0 is real, split as [η]+[\eta]+[η]+ fractional part; a yyy-derivative is read as continuous (CkC^kCk in yyy). The CbηC^\eta_bCbη​ norm is in max form.
  • Not posed: the clause that C0,mC_0,mC0​,m depend "only on d1,d2d_1,d_2d1​,d2​, ∥a∥Cbδ,0\|a\|_{C^{\delta,0}_b}∥a∥Cbδ,0​​, ∥b∥Cbδ,0\|b\|_{C^{\delta,0}_b}∥b∥Cbδ,0​​, [f]Cpδ,0[f]_{C^{\delta,0}_p}[f]Cpδ,0​​", which is false as printed ([f]Cpδ,0[f]_{C^{\delta,0}_p}[f]Cpδ,0​​ is a supremum over the unit ball, and λ\lambdaλ and the rate in (Ab) are missing), and the recursive constant Kη\mathcal K_\etaKη​ of (2.4)–(2.5). The constants exist for each fixed (a,b,f)(a,b,f)(a,b,f). (2.1)–(2.2), printed under "Case η = 0", are asserted for every η\etaη.
  • Uniqueness is stated for the whole class Cp2+δ,ηC^{2+\delta,\eta}_pCp2+δ,η​, not only among solutions that satisfy the estimates. Without the invariance of μy\mu^yμy for the same a,ba,ba,b, or without centering, the statement would be false; both are part of the hypotheses.
  • Useful contributions beyond this mission: Hölder spaces with polynomial weights, fundamental solutions of non-divergence-form operators, invariant measures of elliptic diffusions, and the identification of infinitesimally invariant measures with invariant measures of the diffusion.

Selected references

  • M. Röckner, L. Xie, Diffusion approximation for fully coupled stochastic differential equations, Ann. Probab. 49(3), 1205–1236, 2021. https://doi.org/10.1214/20-AOP1475
  • E. Pardoux, A. Yu. Veretennikov, On the Poisson equation and diffusion approximation. I, Ann. Probab. 29(3), 1061–1085, 2001. https://doi.org/10.1214/aop/1015345596
  • E. Pardoux, A. Yu. Veretennikov, On Poisson equation and diffusion approximation. II, Ann. Probab. 31(3), 1166–1192, 2003. https://doi.org/10.1214/aop/1055425774
  • E. Pardoux, A. Yu. Veretennikov, On the Poisson equation and diffusion approximation 3, Ann. Probab. 33(3), 1111–1133, 2005. https://doi.org/10.1214/009117905000000062
  • O. A. Ladyzhenskaya, V. A. Solonnikov, N. N. Ural'tseva, Linear and Quasi-linear Equations of Parabolic Type, AMS Translations of Mathematical Monographs 23, 1968. https://mathscinet.ams.org/mathscinet-getitem?mr=0241822
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Calculus of VariationsFunctional AnalysisOptimization·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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Viscosity Solutions to Parabolic Master Equations and McKean–Vlasov SDEs with Closed-Loop Controls 3: The Closed-Loop McKean–Vlasov Value Function Is a Viscosity Solution of the HJB Master EquationResearch Paper

Motivation

Mean field control asks a central planner to steer a large population of interacting agents. Each agent's state follows a stochastic differential equation whose coefficients depend on the agent's own state and on the empirical distribution of the population; as the population grows, the system is described by a single McKean–Vlasov equation whose coefficients depend on the law of the solution itself. The planner's value is then a function V(t,μ)V(t,\mu)V(t,μ) of time and of a probability measure, and its dynamic programming equation, the HJB master equation, is a partial differential equation on the Wasserstein space of measures.

C. Wu and J. Zhang (Ann. Appl. Probab. 30(2), 2020) develop a viscosity theory for such master equations in a path-dependent setting and apply it to McKean–Vlasov control with closed-loop controls, i.e. controls that depend on the observed state path rather than on the driving Brownian motion. Closed-loop information is the natural one when the noise is not observable, and it is the information structure relevant for games; but the value function is then not known to be smooth, so classical solutions are out of reach. This mission formalizes the paper's §5: the value function of the closed-loop problem with piecewise constant controls is a viscosity solution of the HJB master equation.

Setting

Fix d≥1d\ge1d≥1 and a horizon TTT. The path space is Ω=C([0,T],Rd)\Omega=C([0,T],\mathbb R^d)Ω=C([0,T],Rd) with the uniform norm, the canonical process is Xs(ω)=ωsX_s(\omega)=\omega_sXs​(ω)=ωs​, and F=(Ft)\mathbb F=(\mathcal F_t)F=(Ft​) is its natural filtration. P2\mathcal P_2P2​ is the set of probability measures μ\muμ on Ω\OmegaΩ with Eμ[∥X∥2]<∞\mathbb E^\mu[\|X\|^2]<\inftyEμ[∥X∥2]<∞; μ[0,t]\mu_{[0,t]}μ[0,t]​ is the law of the stopped path Xt∧⋅X_{t\wedge\cdot}Xt∧⋅​. On Θ=[0,T]×P2\Theta=[0,T]\times\mathcal P_2Θ=[0,T]×P2​ the pseudometric is

W2((t,μ),(t′,μ′))=(∣t−t′∣+W22(μ[0,t],μ[0,t′]′))1/2,\mathcal W_2\big((t,\mu),(t',\mu')\big)=\big(|t-t'|+\mathcal W_2^2(\mu_{[0,t]},\mu'_{[0,t']})\big)^{1/2},W2​((t,μ),(t′,μ′))=(∣t−t′∣+W22​(μ[0,t]​,μ[0,t′]′​))1/2,

with W2\mathcal W_2W2​ the 2-Wasserstein distance on laws of paths.

The data are a control set AAA and coefficients b(t,ω,μ,a)∈Rdb(t,\omega,\mu,a)\in\mathbb R^db(t,ω,μ,a)∈Rd, σ(t,ω,μ,a)∈Rd×d\sigma(t,\omega,\mu,a)\in\mathbb R^{d\times d}σ(t,ω,μ,a)∈Rd×d, f(t,ω,μ,a)∈Rf(t,\omega,\mu,a)\in\mathbb Rf(t,ω,μ,a)∈R, g(ω,μ)∈Rg(\omega,\mu)\in\mathbb Rg(ω,μ)∈R satisfying Assumption 5.1: measurability and adaptedness, boundedness of b,σb,\sigmab,σ by C0C_0C0​, Lipschitz continuity of b,σb,\sigmab,σ and uniform continuity of f,gf,gf,g in (ω,μ)(\omega,\mu)(ω,μ), local uniform continuity in ttt, and positive definiteness of σσ⊤\sigma\sigma^\topσσ⊤.

An admissible control α∈At\alpha\in\mathcal A_tα∈At​ (5.3) is piecewise constant: αs=∑i<nhi1[ti,ti+1)(s)\alpha_s=\sum_{i<n}h_i\mathbf 1_{[t_i,t_{i+1})}(s)αs​=∑i<n​hi​1[ti​,ti+1​)​(s) for a partition t=t0<⋯<tn=Tt=t_0<\dots<t_n=Tt=t0​<⋯<tn​=T, with hi:Ω→Ah_i:\Omega\to Ahi​:Ω→A Fti\mathcal F_{t_i}Fti​​-measurable. The controlled law Pt,μ,α∈P2\mathbb P^{t,\mu,\alpha}\in\mathcal P_2Pt,μ,α∈P2​ agrees with μ\muμ on [0,t][0,t][0,t] and solves, for a Brownian motion BαB^\alphaBα,

Xs=Xt+∫tsb(r,Xr∧⋅,P[0,r]t,μ,α,αr)dr+∫tsσ(r,Xr∧⋅,P[0,r]t,μ,α,αr)dBrα,s∈[t,T].X_s=X_t+\int_t^s b\big(r,X_{r\wedge\cdot},\mathbb P^{t,\mu,\alpha}_{[0,r]},\alpha_r\big)dr+\int_t^s\sigma\big(r,X_{r\wedge\cdot},\mathbb P^{t,\mu,\alpha}_{[0,r]},\alpha_r\big)dB^\alpha_r,\quad s\in[t,T].Xs​=Xt​+∫ts​b(r,Xr∧⋅​,P[0,r]t,μ,α​,αr​)dr+∫ts​σ(r,Xr∧⋅​,P[0,r]t,μ,α​,αr​)dBrα​,s∈[t,T].

The value function (3.20) is

V(t,μ)=sup⁡α∈AtEPt,μ,α[g(X,Pt,μ,α)+∫tTf(s,X,Pt,μ,α,αs) ds],V(t,\mu)=\sup_{\alpha\in\mathcal A_t}\mathbb E^{\mathbb P^{t,\mu,\alpha}}\Big[g(X,\mathbb P^{t,\mu,\alpha})+\int_t^Tf(s,X,\mathbb P^{t,\mu,\alpha},\alpha_s)\,ds\Big],V(t,μ)=α∈At​sup​EPt,μ,α[g(X,Pt,μ,α)+∫tT​f(s,X,Pt,μ,α,αs​)ds],

and V0V_0V0​ is the same supremum over the controls At0\mathcal A^0_tAt0​ (5.12) whose pieces depend on the path before ttt only through finitely many values Xs1,…,XsmX_{s_1},\dots,X_{s_m}Xs1​​,…,Xsm​​.

The HJB master equation (3.22) is LV=0\mathbb LV=0LV=0 with LV(t,μ)=∂tV(t,μ)+G(t,μ,∂μV(t,μ,⋅),∂ω∂μV(t,μ,⋅))\mathbb LV(t,\mu)=\partial_tV(t,\mu)+G(t,\mu,\partial_\mu V(t,\mu,\cdot),\partial_\omega\partial_\mu V(t,\mu,\cdot))LV(t,μ)=∂t​V(t,μ)+G(t,μ,∂μ​V(t,μ,⋅),∂ω​∂μ​V(t,μ,⋅)), where

G(t,μ,Z,Γ)=Eμ[sup⁡a∈A(12Γ(X):σσ⊤(t,X,μ,a)+Z(X)⋅b(t,X,μ,a)+f(t,X,μ,a))].G(t,\mu,Z,\Gamma)=\mathbb E^\mu\Big[\sup_{a\in A}\Big(\tfrac12\Gamma(X):\sigma\sigma^\top(t,X,\mu,a)+Z(X)\cdot b(t,X,\mu,a)+f(t,X,\mu,a)\Big)\Big].G(t,μ,Z,Γ)=Eμ[a∈Asup​(21​Γ(X):σσ⊤(t,X,μ,a)+Z(X)⋅b(t,X,μ,a)+f(t,X,μ,a))].

Viscosity solutions (Definition 4.4) are defined by test functions φ\varphiφ that satisfy a functional Itô formula on [t,t+δ]×PL(t,μ)[t,t+\delta]\times\mathcal P_L(t,\mu)[t,t+δ]×PL​(t,μ), where PL(t,μ)\mathcal P_L(t,\mu)PL​(t,μ) is the set of laws agreeing with μ\muμ on [0,t][0,t][0,t] under which XXX is a semimartingale on [t,T][t,T][t,T] with drift and diffusion bounded by LLL, and touch VVV from above or below at (t,μ)(t,\mu)(t,μ) on that set.

Formalization targets

Goal: Theorem 5.8

Under Assumption 5.1, VVV is finite on Θ\ThetaΘ and is a viscosity solution of (3.22).

Milestones

  • (4.1)(4.1)(4.1): sup⁡P∈PL(t,μ)EP[sup⁡t≤s≤t+δ∣Xt,s∣p]≤Cp,Lδp/2\sup_{\mathbb P\in\mathcal P_L(t,\mu)}\mathbb E^{\mathbb P}[\sup_{t\le s\le t+\delta}|X_{t,s}|^p]\le C_{p,L}\delta^{p/2}supP∈PL​(t,μ)​EP[supt≤s≤t+δ​∣Xt,s​∣p]≤Cp,L​δp/2.
  • Remark 5.4(i): (3.18) has a unique solution, and it lies in PL(t,μ)\mathcal P_L(t,\mu)PL​(t,μ) for L≥C0∨12C02L\ge C_0\vee\frac12C_0^2L≥C0​∨21​C02​.
  • Remark 5.4(ii): the dynamic programming principle (3.21),
V(t1,μ)=sup⁡α∈At1[V(t2,Pt1,μ,α)+∫t1t2EPt1,μ,α[f(s,X,Pt1,μ,α,αs)]ds].V(t_1,\mu)=\sup_{\alpha\in\mathcal A_{t_1}}\Big[V(t_2,\mathbb P^{t_1,\mu,\alpha})+\int_{t_1}^{t_2}\mathbb E^{\mathbb P^{t_1,\mu,\alpha}}[f(s,X,\mathbb P^{t_1,\mu,\alpha},\alpha_s)]ds\Big].V(t1​,μ)=α∈At1​​sup​[V(t2​,Pt1​,μ,α)+∫t1​t2​​EPt1​,μ,α[f(s,X,Pt1​,μ,α,αs​)]ds].
  • Lemma 5.11: a coupling construction with an independent Brownian motion.
  • Lemma 5.13: ∣V0(t,μ)−V0(t,ν)∣≤ρ(W2(μ[0,t],ν[0,t]))|V_0(t,\mu)-V_0(t,\nu)|\le\rho(\mathcal W_2(\mu_{[0,t]},\nu_{[0,t]}))∣V0​(t,μ)−V0​(t,ν)∣≤ρ(W2​(μ[0,t]​,ν[0,t]​)) for a modulus ρ\rhoρ.
  • Lemma 5.14: V=V0V=V_0V=V0​.
  • Theorem 5.7: ∣V(t1,μ)−V(t2,ν)∣≤Cρ(W2((t1,μ),(t2,ν)))+C[1+W2(μ[0,t1],δ{0})][t2−t1]|V(t_1,\mu)-V(t_2,\nu)|\le C\rho(\mathcal W_2((t_1,\mu),(t_2,\nu)))+C[1+\mathcal W_2(\mu_{[0,t_1]},\delta_{\{0\}})][t_2-t_1]∣V(t1​,μ)−V(t2​,ν)∣≤Cρ(W2​((t1​,μ),(t2​,ν)))+C[1+W2​(μ[0,t1​]​,δ{0}​)][t2​−t1​], and uniform continuity when fff is bounded.

Significance

The result characterizes the closed-loop value function through a PDE on the space of path laws without assuming any smoothness of VVV. Combined with a comparison principle for (3.22), which the paper leaves open, it would identify the closed-loop and open-loop values (Remark 5.9). The regularity result (Theorem 5.7) is itself delicate: Example 5.6 shows that a natural restricted class of closed-loop controls produces a value function that is discontinuous in μ\muμ, and the piecewise constant class (5.3) is chosen to avoid this.

The theorems are proved in the paper; none of them is formalized. A formalization would supply a machine-checked path from a path-dependent McKean–Vlasov control problem to its HJB master equation, together with reusable statements on weak solutions of path-dependent McKean–Vlasov equations, their uniform moment bounds, and the dynamic programming principle in the Wasserstein space.

Difficulty

Definition 4.4 requires V∈C0(Θ)V\in C^0(\Theta)V∈C0(Θ), and the central difficulty is continuity in μ\muμ. Closed-loop controls are functions of the observed path; changing the initial law from μ\muμ to ν\nuν changes the information available to the control, and when ν[0,t]\nu_{[0,t]}ν[0,t]​ is degenerate a control adapted to μ\muμ cannot be written as a function of the ν\nuν-path. The obvious argument, transporting an ε\varepsilonε-optimal control for μ\muμ along an optimal coupling of μ\muμ and ν\nuν, fails for exactly this reason (Example 5.6).

Formalization scope

Time is R≥0\mathbb R_{\ge0}R≥0​ and every statement quantifies over t≤Tt\le Tt≤T and μ∈P2\mu\in\mathcal P_2μ∈P2​. Paths are continuous maps [0,T]→Rd[0,T]\to\mathbb R^d[0,T]→Rd with the sup norm and Borel σ\sigmaσ-algebra; W2\mathcal W_2W2​ is the published WassersteinDRO.Duality.wassersteinDistance with p=2p=2p=2. Brownian motion and Itô integrals are the published EthierKurtz.IsStandardBrownian and EthierKurtz.HasBrownianItoIntegral.

Committed conventions:

  • The control set AAA is a nonempty Polish space with its Borel σ\sigmaσ-algebra (the paper says "some appropriate set AAA"); this provides continuity in aaa, measurability of hih_ihi​ and of ω↦sup⁡aG2\omega\mapsto\sup_aG_2ω↦supa​G2​.
  • "Progressively measurable in all variables" is joint measurability (Giry σ\sigmaσ-algebra on laws) plus adaptedness in ω\omegaω and μ\muμ. The bound ∣σ∣≤C0|\sigma|\le C_0∣σ∣≤C0​ uses the Frobenius norm; the joint Lipschitz bound on (b,σ)(b,\sigma)(b,σ) is two bounds with the same L0L_0L0​. δ{0}\delta_{\{0\}}δ{0}​ is the Dirac mass at the zero path.
  • (3.18) is solved in the weak sense: a law with a semimartingale representation, carrying its own Brownian motion, whose characteristics are the controlled coefficients on [t,T)[t,T)[t,T). PL(t,μ)\mathcal P_L(t,\mu)PL​(t,μ) is defined through the same representations.
  • VVV and V0V_0V0​ are suprema in the extended reals over admissible pairs; statements that subtract values or use VVV as a real function assert finiteness explicitly.
  • Test functions carry their derivatives as witnesses; the Itô formula of Definition 4.2 is stated in drift form for every representation; "inf⁡(φ−V)=0\inf(\varphi-V)=0inf(φ−V)=0" is read as φ−V≥0\varphi-V\ge0φ−V≥0 on the test set with equality at (t,μ)(t,\mu)(t,μ), and the test function's data at (t,μ)(t,\mu)(t,μ) are those at (t,P)(t,\mathbb P)(t,P) for P∈PL(t,μ)\mathbb P\in\mathcal P_L(t,\mu)P∈PL​(t,μ).
  • Statements are for general ddd; §5.3 of the paper argues for d=1d=1d=1 only.

The test classes are not vacuous: constant functions satisfy every clause of the test-function class, and Assumption 5.1 holds for b≡0b\equiv0b≡0, σ≡I\sigma\equiv Iσ≡I, f≡g≡0f\equiv g\equiv0f≡g≡0. A formalization that makes PL(t,μ)\mathcal P_L(t,\mu)PL​(t,μ) or the admissible set empty, or that lets VVV be −∞-\infty−∞, does not prove the theorem.

Needed infrastructure: weak existence and uniqueness for path-dependent McKean–Vlasov SDEs with Lipschitz coefficients; Burkholder–Davis–Gundy-type moment bounds; measurable selection on Polish spaces; couplings and gluing on P2\mathcal P_2P2​ of a path space. The moment bound and the McKean–Vlasov well-posedness are reusable beyond this mission. Contributions to any milestone are welcome.

Selected references

  • C. Wu, J. Zhang, Viscosity solutions to parabolic master equations and McKean–Vlasov SDEs with closed-loop controls, Ann. Appl. Probab. 30(2), 936–986, 2020. https://doi.org/10.1214/19-AAP1521
  • 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
  • D. Lacker, Limit theory for controlled McKean–Vlasov dynamics, SIAM J. Control Optim. 55(3), 2017. https://doi.org/10.1137/16M1095895
  • I. Ekren, N. Touzi, J. Zhang, Viscosity solutions of fully nonlinear parabolic path dependent PDEs: Part I, Ann. Probab. 44(2), 2016. https://doi.org/10.1214/14-AOP999
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Optimal TransportPartial Differential EquationsProbability·Captain: mikedeng1

Viscosity Solutions to Parabolic Master Equations and McKean–Vlasov SDEs with Closed-Loop Controls 1: A Functional Itô Formula for Path-Dependent Functionals of Semimartingale LawsResearch Paper

Motivation

Master equations are partial differential equations whose state variable is a probability measure. They arise as the Hamilton–Jacobi–Bellman equations of mean field control problems, where a planner steers a large population through its distribution, and as the limit description of large games. Their basic computational tool is an Itô formula for functions of measures: if XXX is a semimartingale with law PXt\mathbb P_{X_t}PXt​​ at time ttt, how does f(PXt)f(\mathbb P_{X_t})f(PXt​​) evolve? For functions on the Wasserstein space P2(Rd)\mathcal P_2(\mathbb R^d)P2​(Rd) this formula is due to Buckdahn, Li, Peng and Rainer (Ann. Probab. 2017) and Chassagneux, Crisan and Delarue (arXiv:1411.3009), with the derivative in the measure introduced by Lions through the lifting to random variables.

Many models are path dependent: exotic options, rough volatility, and control problems with constant controls all lead to functions of the law of a whole path rather than of its time marginal. Wu and Zhang (Ann. Appl. Probab. 2020) extend the measure derivative and the Itô formula to this setting, following Dupire's functional Itô calculus (Dupire 2009). This mission formalizes §2 of their paper: the derivative of a function of a path law and the functional Itô formula of Theorem 2.7. It is the first of three missions on the paper; the other two treat viscosity solutions of master equations and McKean–Vlasov control.

Setting

Fix d≥1d\ge1d≥1 and T>0T>0T>0. Continuous paths form Ω=C([0,T],Rd)\Omega=C([0,T],\mathbb R^d)Ω=C([0,T],Rd) with ∥ω∥=sup⁡t∣ωt∣\|\omega\|=\sup_t|\omega_t|∥ω∥=supt​∣ωt​∣. Càdlàg paths form Ω^=D([0,T],Rd)\widehat\Omega=\mathbb D([0,T],\mathbb R^d)Ω=D([0,T],Rd) with the Skorokhod distance

dSK(ω^,ω^′)=inf⁡λsup⁡0≤t≤T[∣t−λ(t)∣+∣ω^t−ω^λ(t)′∣],d_{SK}(\hat\omega,\hat\omega')=\inf_\lambda\sup_{0\le t\le T}\big[|t-\lambda(t)|+|\hat\omega_t-\hat\omega'_{\lambda(t)}|\big],dSK​(ω^,ω^′)=λinf​0≤t≤Tsup​[∣t−λ(t)∣+∣ω^t​−ω^λ(t)′​∣],

the infimum over continuous strictly increasing bijections λ\lambdaλ of [0,T][0,T][0,T]. The canonical process is X^t(ω^)=ω^t\widehat X_t(\hat\omega)=\hat\omega_tXt​(ω^)=ω^t​, with natural filtration F^\widehat{\mathbb F}F; ω^t∧⋅\hat\omega_{t\wedge\cdot}ω^t∧⋅​ is the path stopped at ttt.

P^2\widehat{\mathcal P}_2P2​ is the set of probability measures μ\muμ on Ω^\widehat\OmegaΩ with Eμ∥X^∥2<∞\mathbb E^\mu\|\widehat X\|^2<\inftyEμ∥X∥2<∞, with the Wasserstein distance W2\mathcal W_2W2​ whose cost is dSK2d_{SK}^2dSK2​. The state space is Θ^=[0,T]×P^2\widehat\Theta=[0,T]\times\widehat{\mathcal P}_2Θ=[0,T]×P2​ with the pseudometric

W2((t,μ),(t′,μ′))=(∣t−t′∣+W22(μ[0,t],μ[0,t′]′))1/2,\mathcal W_2\big((t,\mu),(t',\mu')\big)=\big(|t-t'|+\mathcal W_2^2(\mu_{[0,t]},\mu'_{[0,t']})\big)^{1/2},W2​((t,μ),(t′,μ′))=(∣t−t′∣+W22​(μ[0,t]​,μ[0,t′]′​))1/2,

where μ[0,t]\mu_{[0,t]}μ[0,t]​ is the law of X^t∧⋅\widehat X_{t\wedge\cdot}Xt∧⋅​.

For f:Θ^→Rf:\widehat\Theta\to\mathbb Rf:Θ→R the time derivative is the right derivative ∂tf(t,μ)=lim⁡δ↓0[f(t+δ,μ[0,t])−f(t,μ)]/δ\partial_tf(t,\mu)=\lim_{\delta\downarrow0}[f(t+\delta,\mu_{[0,t]})-f(t,\mu)]/\delta∂t​f(t,μ)=limδ↓0​[f(t+δ,μ[0,t]​)−f(t,μ)]/δ. The spatial derivative ∂μf(t,μ,ω^)∈Rd\partial_\mu f(t,\mu,\hat\omega)\in\mathbb R^d∂μ​f(t,μ,ω^)∈Rd comes from lifting fff to F(t,X~)=f(t,P~X~)F(t,\tilde X)=f(t,\tilde{\mathbb P}_{\tilde X})F(t,X~)=f(t,P~X~​) on square-integrable path-valued random variables of an atomless Polish probability space: the Fréchet derivative of FFF under the perturbation X~+ξ1[t,T]\tilde X+\xi\mathbf 1_{[t,T]}X~+ξ1[t,T]​ has the form DF(t,X~)=∂μf(t,P~X~t∧⋅,X~t∧⋅)DF(t,\tilde X)=\partial_\mu f(t,\tilde{\mathbb P}_{\tilde X_{t\wedge\cdot}},\tilde X_{t\wedge\cdot})DF(t,X~)=∂μ​f(t,P~X~t∧⋅​​,X~t∧⋅​). The second derivative ∂ω∂μf∈Rd×d\partial_\omega\partial_\mu f\in\mathbb R^{d\times d}∂ω​∂μ​f∈Rd×d is the pathwise (Dupire vertical) derivative of ∂μf\partial_\mu f∂μ​f. Cb1,1,1(Θ^)C^{1,1,1}_b(\widehat\Theta)Cb1,1,1​(Θ) consists of the continuous fff with continuous derivatives, bounded ∂tf\partial_tf∂t​f, and ∣∂μf∣+∣∂ω∂μf∣≤C[1+∥ω^∥]|\partial_\mu f|+|\partial_\omega\partial_\mu f|\le C[1+\|\hat\omega\|]∣∂μ​f∣+∣∂ω​∂μ​f∣≤C[1+∥ω^∥].

P^L\widehat{\mathcal P}_LPL​ is the set of laws μ=P~∘X~−1\mu=\tilde{\mathbb P}\circ\tilde X^{-1}μ=P~∘X~−1 of Itô processes X~t=X~0+∫0tb~s ds+∫0tσ~s dB~s\tilde X_t=\tilde X_0+\int_0^t\tilde b_s\,ds+\int_0^t\tilde\sigma_s\,d\tilde B_sX~t​=X~0​+∫0t​b~s​ds+∫0t​σ~s​dB~s​ with ∣b~∣≤L|\tilde b|\le L∣b~∣≤L, 12∣σ~∣2≤L\tfrac12|\tilde\sigma|^2\le L21​∣σ~∣2≤L and X~0\tilde X_0X~0​ square integrable.

Formalization targets

Goal: the functional Itô formula (Theorem 2.7)

For f∈Cb1,1,1(Θ^)f\in C^{1,1,1}_b(\widehat\Theta)f∈Cb1,1,1​(Θ), μ∈P^L\mu\in\widehat{\mathcal P}_Lμ∈PL​ and t∈[0,T]t\in[0,T]t∈[0,T],

f(t,μ)=f(0,μ)+∫0t∂tf(s,μ) ds+Eμ[∫0t∂μf(s,μ,X^)⋅dX^s+12∫0t∂ω∂μf(s,μ,X^):d⟨X^⟩s].f(t,\mu)=f(0,\mu)+\int_0^t\partial_tf(s,\mu)\,ds+\mathbb E^\mu\Big[\int_0^t\partial_\mu f(s,\mu,\widehat X)\cdot d\widehat X_s+\tfrac12\int_0^t\partial_\omega\partial_\mu f(s,\mu,\widehat X):d\langle\widehat X\rangle_s\Big].f(t,μ)=f(0,μ)+∫0t​∂t​f(s,μ)ds+Eμ[∫0t​∂μ​f(s,μ,X)⋅dXs​+21​∫0t​∂ω​∂μ​f(s,μ,X):d⟨X⟩s​].

Milestones

  1. Theorem 2.2: the Fréchet derivative of the lift is ψ(X~t∧⋅)\psi(\tilde X_{t\wedge\cdot})ψ(X~t∧⋅​) for an F^t\widehat{\mathcal F}_tFt​-measurable ψ\psiψ determined by fff and the law of X~\tilde XX~.
  2. Corollary 2.3: under uniform continuity of DFDFDF, a single jointly measurable ∂μf\partial_\mu f∂μ​f represents DFDFDF, unique if continuous.
  3. (2.21): the discrete expansion f(T,μn)−f(0,μn)=I1n+I2n+I3nf(T,\mu^n)-f(0,\mu^n)=I_1^n+I_2^n+I_3^nf(T,μn)−f(0,μn)=I1n​+I2n​+I3n​ along a uniform partition.
  4. (2.22) and the W2\mathcal W_2W2​ limit after it: the discretized paths and laws converge.
  5. The four limits on p. 946, which turn (2.21) into (2.20) as n→∞n\to\inftyn→∞.

Significance

The formula is the chain rule of calculus on path laws. It is what makes Cb1,1,1C^{1,1,1}_bCb1,1,1​ functions admissible test functions for viscosity solutions of path-dependent master equations, and what identifies the value function of a McKean–Vlasov control problem with a solution of its HJB master equation (§§4–5 of the paper, the other two missions of this series). Without it, the notion of viscosity solution in that paper has no link to the underlying dynamics.

The result is proved in the paper. It has no machine-checked proof: Lean's Mathlib has neither the Skorokhod space, nor Wasserstein spaces of path laws, nor a derivative with respect to a measure. Formalizing it would also produce a reusable Lean account of càdlàg path spaces and of the Lions derivative, both of which are absent today.

Difficulty

The obvious argument would expand fff along the time marginals of X~\tilde XX~. That fails for path-dependent fff: the stopped laws μ[0,t]\mu_{[0,t]}μ[0,t]​ do not change continuously when a path is perturbed after ttt, and the perturbation X~+ξ1[t,T]\tilde X+\xi\mathbf 1_{[t,T]}X~+ξ1[t,T]​ of the derivative's definition leaves the space of continuous paths. This is why the paper passes to càdlàg paths and the Skorokhod distance. Any argument then has to control fff and its derivatives along laws of discontinuous paths, which is where the joint continuity of all derivatives in (t,μ,ω^)(t,\mu,\hat\omega)(t,μ,ω^) under W2+dSK\mathcal W_2+d_{SK}W2​+dSK​ and convergence of laws in W2\mathcal W_2W2​ become unavoidable. Separately, Theorem 2.2 must show that a derivative defined through one probability space is a deterministic function of the stopped path, and atomlessness of that space is essential to it.

Formalization scope

Paths are functions on [0,∞)[0,\infty)[0,∞), constant after TTT; Ω\OmegaΩ is C(Set.Icc 0 T, ℝ^d) with the sup norm, embedded in Ω^\widehat\OmegaΩ. Ω^\widehat\OmegaΩ carries the σ\sigmaσ-algebra of the evaluations. Distances, sup norms and W2\mathcal W_2W2​ are [0,∞][0,\infty][0,∞]-valued. A law in P^L\widehat{\mathcal P}_LPL​ is given with an explicit representation: a filtered probability space, a standard Brownian motion with independent increments, progressively measurable bounded coefficients, and the Itô integral of the published EthierKurtz.HasBrownianItoIntegral. The goal holds for every representation of μ\muμ, and (2.20) is stated in drift form: E∫0t(∂μf⋅b~s+12∂ω∂μf:σ~sσ~s⊤) ds\mathbb E\int_0^t(\partial_\mu f\cdot\tilde b_s+\tfrac12\partial_\omega\partial_\mu f:\tilde\sigma_s\tilde\sigma_s^\top)\,dsE∫0t​(∂μ​f⋅b~s​+21​∂ω​∂μ​f:σ~s​σ~s⊤​)ds, the stochastic integral having mean zero.

The class C1,1,1(Θ^)C^{1,1,1}(\widehat\Theta)C1,1,1(Θ) fixes fff together with its derivatives and states that they are the derivatives (2.7), (2.16), (2.18). It also requires ∂μf(t,μ,⋅)\partial_\mu f(t,\mu,\cdot)∂μ​f(t,μ,⋅) and ∂ω∂μf(t,μ,⋅)\partial_\omega\partial_\mu f(t,\mu,\cdot)∂ω​∂μ​f(t,μ,⋅) to be F^t\widehat{\mathcal F}_tFt​-adapted, a property the paper's ∂μf\partial_\mu f∂μ​f has by Theorem 2.2. Without these clauses every continuous function would qualify, and (2.20) would be false. The printed D([0,T),Rd)\mathbb D([0,T),\mathbb R^d)D([0,T),Rd) is read as D([0,T],Rd)\mathbb D([0,T],\mathbb R^d)D([0,T],Rd). The proof's d=1d=1d=1 computations are stated in dimension ddd. Limits indexed by ti≤t<ti+1t_i\le t<t_{i+1}ti​≤t<ti+1​ are stated for t<Tt<Tt<T.

A complete development needs: the Skorokhod space and the fact that its Borel σ\sigmaσ-algebra is the evaluation σ\sigmaσ-algebra; Wasserstein distances on it; dominated convergence for path laws; and Itô's formula for the drift–diffusion representation. These are reusable well beyond this mission. Contributions to any milestone, or to these foundations as separate lemmas, are welcome.

Selected references

  • C. Wu, J. Zhang, Viscosity solutions to parabolic master equations and McKean–Vlasov SDEs with closed-loop controls, Ann. Appl. Probab. 30(2) (2020), 936–986. https://doi.org/10.1214/19-AAP1521
  • R. Buckdahn, J. Li, S. Peng, C. Rainer, Mean-field stochastic differential equations and associated PDEs, Ann. Probab. 45(2) (2017), 824–878. https://doi.org/10.1214/15-AOP1076
  • J.-F. Chassagneux, D. Crisan, F. Delarue, A probabilistic approach to classical solutions of the master equation for large population equilibria, Mem. Amer. Math. Soc. (2022). https://arxiv.org/abs/1411.3009
  • B. Dupire, Functional Itô calculus, Bloomberg Portfolio Research Paper 2009-04 (2009); Quant. Finance 19(5) (2019). https://doi.org/10.2139/ssrn.1435551
  • 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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CombinatoricsLinear OptimizationOptimization·Captain: mikedeng1

The Running Intersection Relaxation of the Multilinear Polytope 3: Running Intersection Inequalities Meeting Three Support Conditions Define Facets of the Multilinear PolytopeResearch Paper

Motivation

Binary polynomial optimization asks for the maximum of a polynomial over {0,1}n\{0,1\}^n{0,1}n. Linearizing each monomial ∏v∈ezv\prod_{v\in e}z_v∏v∈e​zv​ by a new variable zez_eze​ turns the problem into a linear program over the convex hull of a set of 0/1 points, the multilinear polytope of the hypergraph whose edges are the monomials. Global solvers such as BARON build polyhedral relaxations of this polytope at every node of their branch-and-bound trees, so valid inequalities that are as strong as possible, that is, facet-defining, translate directly into smaller root gaps.

Del Pia and Khajavirad introduced running intersection inequalities in The running intersection relaxation of the multilinear polytope (Math. Oper. Res. 46 (2021) 1008–1037, doi:10.1287/moor.2021.1121). They generalize the flower inequalities of the same authors (SIAM J. Optim. 2018), which are facet-defining when the support hypergraph is γ\gammaγ-acyclic, to support hypergraphs that are not. This mission formalizes the paper's sufficient condition for a running intersection inequality to define a facet (§2.4, Proposition 4) together with the structural results it rests on.

Timeline. Crama (1993) studied the standard linearization; Del Pia and Khajavirad (2017, Math. Oper. Res.) proved that the multilinear polytope is full dimensional and gave lifting theorems for facets; flower inequalities followed in 2018; running intersection inequalities and the facet conditions formalized here appeared in 2021.

Setting

A hypergraph G=(V,E)G=(V,E)G=(V,E) has a finite node set VVV and a set EEE of subsets of VVV of cardinality at least two. Its multilinear set is

SG={z∈{0,1}V+E: ze=∏v∈ezv  ∀e∈E},\mathcal S_G=\Big\{z\in\{0,1\}^{V+E}:\ z_e=\prod_{v\in e}z_v\ \ \forall e\in E\Big\},SG​={z∈{0,1}V+E: ze​=v∈e∏​zv​  ∀e∈E},

and its multilinear polytope is MPG=conv⁡SG\mathrm{MP}_G=\operatorname{conv}\mathcal S_GMPG​=convSG​.

A multiset FFF of sets has the running intersection property if its elements can be ordered p1,…,pmp_1,\dots,p_mp1​,…,pm​ so that each pk∩(p1∪⋯∪pk−1)p_k\cap(p_1\cup\dots\cup p_{k-1})pk​∩(p1​∪⋯∪pk−1​), k≥2k\ge 2k≥2, is contained in a single earlier pjp_jpj​. Such an ordering defines N(p1)=∅N(p_1)=\emptysetN(p1​)=∅ and N(pk)=pk∩⋃i<kpiN(p_k)=p_k\cap\bigcup_{i<k}p_iN(pk​)=pk​∩⋃i<k​pi​. A leaf of FFF is an element that comes last in some such ordering.

Fix an edge e0e_0e0​ (the center) and edges eke_kek​, k∈Kk\in Kk∈K, adjacent to e0e_0e0​ (the neighbors), such that the multiset E~={e0∩ek:k∈K}\tilde E=\{e_0\cap e_k:k\in K\}E~={e0​∩ek​:k∈K} has the running intersection property. Choose an ordering of E~\tilde EE~, and for each kkk with N(e0∩ek)≠∅N(e_0\cap e_k)\neq\emptysetN(e0​∩ek​)=∅ a node uk∈N(e0∩ek)u_k\in N(e_0\cap e_k)uk​∈N(e0​∩ek​). The running intersection inequality is

−∑k∈K: N(e0∩ek)≠∅zuk+∑v∈e0∖⋃kekzv+∑k∈Kzek−ze0 ≤ ω−1,-\sum_{k\in K:\,N(e_0\cap e_k)\neq\emptyset} z_{u_k}+\sum_{v\in e_0\setminus\bigcup_{k}e_k} z_v+\sum_{k\in K}z_{e_k}-z_{e_0}\ \le\ \omega-1,−k∈K:N(e0​∩ek​)=∅∑​zuk​​+v∈e0​∖⋃k​ek​∑​zv​+k∈K∑​zek​​−ze0​​ ≤ ω−1,

where ω\omegaω is the number of connected components of the hypergraph G~=(e0,E~)\tilde G=(e_0,\tilde E)G~=(e0​,E~). Its support hypergraph GGG has node set e0∪⋃keke_0\cup\bigcup_k e_ke0​∪⋃k​ek​ and edge set {e0}∪{ek:k∈K}\{e_0\}\cup\{e_k:k\in K\}{e0​}∪{ek​:k∈K}. An inequality defines a facet of MPG\mathrm{MP}_GMPG​ if it is valid and the face it cuts out is nonempty of dimension dim⁡MPG−1\dim\mathrm{MP}_G-1dimMPG​−1.

Formalization targets

Goal: Proposition 4 (p. 1016)

Assume

  1. ∣e0∩ek∣≥2|e_0\cap e_k|\ge 2∣e0​∩ek​∣≥2 for every k∈Kk\in Kk∈K;
  2. for every K′⊆KK'\subseteq KK′⊆K with e0∩⋂k∈K′ek≠∅e_0\cap\bigcap_{k\in K'}e_k\neq\emptysete0​∩⋂k∈K′​ek​=∅:  e0∩(ei∖⋃k∈K′∖{i}ek)≠∅\ e_0\cap\big(e_i\setminus\bigcup_{k\in K'\setminus\{i\}}e_k\big)\neq\emptyset e0​∩(ei​∖⋃k∈K′∖{i}​ek​)=∅ for all i∈K′i\in K'i∈K′;
  3. each nonempty N(e0∩ek)N(e_0\cap e_k)N(e0​∩ek​) meets U={uk:N(e0∩ek)≠∅}U=\{u_k: N(e_0\cap e_k)\neq\emptyset\}U={uk​:N(e0​∩ek​)=∅} in exactly one node.

Then the running intersection inequality defines a facet of MPG\mathrm{MP}_GMPG​ for its support hypergraph GGG.

Milestones

Lemma 1 (p. 1011, leaves and reorderings), Lemma 2 (p. 1011, components =n0+∣{e:N(e)=∅}∣=n_0+|\{e:N(e)=\emptyset\}|=n0​+∣{e:N(e)=∅}∣), Proposition 1 (p. 1012, validity), and the full dimensionality of MPG\mathrm{MP}_GMPG​ (cited on p. 1016 from [12]):

dim⁡MPG=∣V∣+∣E∣.\dim\mathrm{MP}_G=|V|+|E|.dimMPG​=∣V∣+∣E∣.

Companions

Corollary 2 (p. 1017): ∣e0∩ek∣≥2|e_0\cap e_k|\ge 2∣e0​∩ek​∣≥2 and ∣e0∩ek∩ek′∣≤1|e_0\cap e_k\cap e_{k'}|\le 1∣e0​∩ek​∩ek′​∣≤1 for k≠k′k\neq k'k=k′ suffice. Proposition 2 and Corollary 1 (pp. 1013–1014): the multiset {N(e)}\{N(e)\}{N(e)}, hence the system of inequalities, does not depend on the ordering. Proposition 3 (p. 1014): necessary conditions for a facet of the running intersection relaxation MPGRI\mathrm{MP}^{\mathrm{RI}}_GMPGRI​.

Significance

Proposition 4 certifies a large family of facets of multilinear polytopes whose support hypergraphs contain cycles that flower inequalities cannot handle. Together with the lifting theorems of Del Pia and Khajavirad (2017), it yields sufficient conditions under which these inequalities define facets of the multilinear polytope of general hypergraphs (p. 1015); §2.5 of the paper reports that running intersection cuts reduce BARON's root-node relaxation gap on image-restoration instances. Proposition 3 and Example 1 show that condition 1 is necessary while conditions 2–3 are not, so the result is a sufficient condition and not a characterization.

The results are proved in the paper; none is formalized. A Lean development would provide the first machine-checked library for the running intersection property (orderings, leaves, the multiset of NNN-sets), the connected-component count of Lemma 2, and the multilinear polytope as a convex hull with an exact dimension count, all reusable for the companion missions on the tightness of MPGRI\mathrm{MP}^{\mathrm{RI}}_GMPGRI​ for kite-free β\betaβ-acyclic hypergraphs and its strictness otherwise.

Difficulty

Validity (Proposition 1) decomposes over the connected components of G~\tilde GG~; the facet claim does not, because a face of codimension one is a global object and the neighbors of different components, and the nodes uku_kuk​ shared between neighbors, interact in it. Conditions 2 and 3 are exactly where this interaction is controlled, and Example 1 of the paper shows that dropping condition 3 does not destroy facetness, so no simple equivalence is available to fall back on. Formally, three nontrivial ingredients have no Mathlib counterpart: the combinatorics of running intersection orderings (Lemma 1, Proposition 2), the count of connected components of a hypergraph with loops and parallel edges (Lemma 2), and the affine dimension of a convex hull of 0/1 points in a space indexed by nodes and edges.

Formalization scope

Nodes form a finite type α; every hypergraph's space RV+E\mathbb R^{V+E}RV+E lives inside α ⊕ Finset α → ℝ, with the coordinates outside V+EV+EV+E pinned to 000 in the definition of SG\mathcal S_GSG​, so dim⁡MPG=∣V∣+∣E∣\dim\mathrm{MP}_G=|V|+|E|dimMPG​=∣V∣+∣E∣ is meaningful. Orderings are lists indexed from 000. The number of components is that of the 2-section graph on the node set. An inequality is given by its data: center, a set KKK of distinct neighbors other than e0e_0e0​, an ordering of KKK whose traces form a running intersection ordering of E~\tilde EE~, and the choice k↦ukk\mapsto u_kk↦uk​; the first sum runs over neighbors, so a node chosen for two neighbors has coefficient −2-2−2. "Defines a facet" requires a nonempty face and compares dimensions as dim⁡F+1=dim⁡P\dim F+1=\dim PdimF+1=dimP, so the empty face can never qualify and no truncated subtraction occurs. The facet statement is about MPG\mathrm{MP}_GMPG​ for the support hypergraph only, not for a larger host hypergraph, which would require the lifting theorems. The reading k≠k′k\neq k'k=k′ is used where the page's "for all k,k′k,k'k,k′" would otherwise be contradictory (Corollary 2, Proposition 3(i)); Lemma 2 is stated for lists of nonempty sets, which covers its use on G~\tilde GG~.

Contributions welcome: proofs of the milestones, a reusable library for the running intersection property and α\alphaα-acyclic hypergraphs, and the full-dimensionality proof.

Selected references

  • A. Del Pia, A. Khajavirad, The running intersection relaxation of the multilinear polytope, Math. Oper. Res. 46(3):1008–1037, 2021. https://doi.org/10.1287/moor.2021.1121
  • A. Del Pia, A. Khajavirad, A polyhedral study of binary polynomial programs, Math. Oper. Res. 42(2):389–410, 2017. https://doi.org/10.1287/moor.2016.0804
  • A. Del Pia, A. Khajavirad, The multilinear polytope for acyclic hypergraphs, SIAM J. Optim. 28(2):1049–1076, 2018. https://doi.org/10.1137/16M1095998
  • C. Beeri, R. Fagin, D. Maier, M. Yannakakis, On the desirability of acyclic database schemes, J. ACM 30(3):479–513, 1983. https://doi.org/10.1145/2402.322389
  • Y. Crama, Concave extensions for nonlinear 0–1 maximization problems, Math. Programming 61:53–60, 1993. https://doi.org/10.1007/BF01582138
6 thms1 active userReviewed
Convex OptimizationOperations ResearchProbability·Captain: mikedeng1

Arbitrage and Duality in Nondominated Discrete-Time Models II: Nondominated Optional Decomposition — a Supermartingale Under Every Martingale Measure Is V₀ + H•S − KResearch Paper

Motivation

In a financial market with a single probability model, the Optional Decomposition Theorem describes the processes that can be dominated by trading. If a process VVV is a supermartingale under every equivalent martingale measure, then it can be written as an initial value plus a stochastic integral against the stock price, minus an increasing process that represents consumption. El Karoui and Quenez proved it for diffusion models (SIAM J. Control Optim. 33 (1995)) and Kramkov for locally bounded semimartingales (Probab. Theory Related Fields 105 (1996)). It is the step that turns the superhedging price, a supremum of expectations over martingale measures, into an actual dynamic hedging strategy.

Model uncertainty replaces the single model by a set P\mathcal PP of probability measures that may be mutually singular. This happens, for example, when volatility is only known to lie in an interval. There is then no reference measure, "almost surely" becomes "quasi surely" (outside a set that is null under every model), and the classical proofs, which rely on one dominating measure, do not apply. Bouchard and Nutz (Ann. Appl. Probab. 2015, arXiv:1305.6008) built the discrete-time theory of this setting: no-arbitrage, the fundamental theorem of asset pricing, superhedging duality and, in §6, a nondominated optional decomposition. This mission formalizes that last result.

Timeline:

  • 1995: El Karoui and Quenez, optional decomposition in diffusion models.
  • 1996: Kramkov, for locally bounded semimartingales.
  • 2014: Nutz, superreplication duality under model uncertainty in discrete time (Finance Stoch. 18 (2014)).
  • 2015: Bouchard and Nutz, the fundamental theorem, superhedging duality and the optional decomposition in nondominated discrete time (Theorem 6.1).

Setting

Fix a Polish space Ω1\Omega_1Ω1​, a horizon T∈NT \in \mathbb NT∈N and d∈Nd \in \mathbb Nd∈N. Let Ωt:=Ω1t\Omega_t := \Omega_1^tΩt​:=Ω1t​ for t=0,…,Tt = 0, \dots, Tt=0,…,T. Then Ω0\Omega_0Ω0​ is a single point and Ω:=ΩT\Omega := \Omega_TΩ:=ΩT​, and a point of Ωt\Omega_tΩt​ is read as the first ttt coordinates of a path. The σ\sigmaσ-field Ft\mathcal F_tFt​ is the universal completion of B(Ωt)\mathcal B(\Omega_t)B(Ωt​).

For each t<Tt < Tt<T and each node ω∈Ωt\omega \in \Omega_tω∈Ωt​ a nonempty convex set Pt(ω)\mathcal P_t(\omega)Pt​(ω) of probability measures on Ω1\Omega_1Ω1​ is given, and its graph is an analytic set. The set of possible models P\mathcal PP consists of all products P0⊗P1⊗⋯⊗PT−1P_0 \otimes P_1 \otimes \cdots \otimes P_{T-1}P0​⊗P1​⊗⋯⊗PT−1​ whose kernels take values in Pt(⋅)\mathcal P_t(\cdot)Pt​(⋅). A set is P\mathcal PP-polar if it is null under every P∈PP \in \mathcal PP∈P. A property holds P\mathcal PP-quasi surely (q.s.) if it holds outside a polar set.

Stock prices St:Ωt→RdS_t : \Omega_t \to \mathbb R^dSt​:Ωt​→Rd are Borel. A strategy H∈HH \in \mathcal HH∈H is predictable: HuH_uHu​ is a function of the first u−1u-1u−1 coordinates. The wealth at time ttt is

H∙St=∑u=1tHuΔSu,ΔSu=Su−Su−1.H \bullet S_t = \sum_{u=1}^t H_u \Delta S_u, \qquad \Delta S_u = S_u - S_{u-1}.H∙St​=u=1∑t​Hu​ΔSu​,ΔSu​=Su​−Su−1​.

NA(P\mathcal PP) holds if H∙ST≥0H \bullet S_T \ge 0H∙ST​≥0 q.s. implies H∙ST=0H \bullet S_T = 0H∙ST​=0 q.s. A martingale measure is a probability QQQ under which SSS is a martingale. The set

Q={Q⋘P:Q is a martingale measure}\mathcal Q = \{Q \lll \mathcal P : Q \text{ is a martingale measure}\}Q={Q⋘P:Q is a martingale measure}

contains those QQQ that are absolutely continuous with respect to some P∈PP \in \mathcal PP∈P (written Q⋘PQ \lll \mathcal PQ⋘P). A function fff with values in [−∞,∞][-\infty, \infty][−∞,∞] is upper semianalytic if every set {f>c}\{f > c\}{f>c} is analytic.

At one node ω∈Ωt\omega \in \Omega_tω∈Ωt​, the increment ΔSt+1(ω,⋅)\Delta S_{t+1}(\omega, \cdot)ΔSt+1​(ω,⋅) defines a one-period market under Pt(ω)\mathcal P_t(\omega)Pt​(ω), with its own no-arbitrage condition NA(Pt(ω)\mathcal P_t(\omega)Pt​(ω)) and one-period martingale measures Qt(ω)\mathcal Q_t(\omega)Qt​(ω). The conditional sublinear expectation is

Et(f)(ω)=sup⁡Q∈Qt(ω)EQ[f(ω,⋅)].\mathcal E_t(f)(\omega) = \sup_{Q \in \mathcal Q_t(\omega)} E_Q[f(\omega, \cdot)].Et​(f)(ω)=Q∈Qt​(ω)sup​EQ​[f(ω,⋅)].

Formalization targets

Goal: Theorem 6.1 (nondominated optional decomposition)

Let NA(P\mathcal PP) hold and let VVV be an adapted process such that VtV_tVt​ is upper semianalytic and in L1(Q)L^1(Q)L1(Q) for all Q∈QQ \in \mathcal QQ∈Q and t∈{1,…,T}t \in \{1, \dots, T\}t∈{1,…,T}. Then the following are equivalent:

  1. VVV is a supermartingale under each Q∈QQ \in \mathcal QQ∈Q;
  2. there exist H∈HH \in \mathcal HH∈H and an adapted increasing process KKK with K0=0K_0 = 0K0​=0 such that
Vt=V0+H∙St−KtP-q.s.,t=0,1,…,T.V_t = V_0 + H \bullet S_t - K_t \quad \mathcal P\text{-q.s.}, \qquad t = 0, 1, \dots, T.Vt​=V0​+H∙St​−Kt​P-q.s.,t=0,1,…,T.

Milestones

  • Lemma 4.6: the set NtN_tNt​ of nodes where NA(Pt(ω)\mathcal P_t(\omega)Pt​(ω)) fails is universally measurable, and it is polar under NA(P\mathcal PP).
  • Theorem 4.5: NA(P\mathcal PP) holds if and only if every NtN_tNt​ is polar, if and only if every P∈PP \in \mathcal PP∈P is absolutely continuous with respect to some Q∈QQ \in \mathcal QQ∈Q.
  • Lemma 4.10: Et(f)\mathcal E_t(f)Et​(f) is upper semianalytic, and there is a universally measurable yyy with
Et(f)(ω)+y(ω) ΔSt+1(ω,⋅)≥f(ω,⋅)Pt(ω)-q.s.\mathcal E_t(f)(\omega) + y(\omega)\,\Delta S_{t+1}(\omega, \cdot) \ge f(\omega, \cdot) \quad \mathcal P_t(\omega)\text{-q.s.}Et​(f)(ω)+y(ω)ΔSt+1​(ω,⋅)≥f(ω,⋅)Pt​(ω)-q.s.

at every arbitrage-free node where f(ω,⋅)>−∞f(\omega,\cdot) > -\inftyf(ω,⋅)>−∞ q.s.

  • (6.1): under condition 1 of the goal, Et(Vt+1)≤Vt\mathcal E_t(V_{t+1}) \le V_tEt​(Vt+1​)≤Vt​ P\mathcal PP-q.s. for every t<Tt < Tt<T.

Significance

The decomposition is the dynamic counterpart of superhedging duality. Duality identifies the price sup⁡QEQ[f]\sup_{Q} E_Q[f]supQ​EQ​[f]. The optional decomposition, applied to the process of conditional superhedging prices, produces one strategy that superhedges under all models at once and a nonnegative increasing process recording the surplus. The proof works in a nondominated model with one strategy HHH that is measurable in the universal completion, and this is what makes the theorem usable under volatility or model uncertainty, where no single model can be singled out. The equivalence also characterizes the processes that are supermartingales under every Q∈QQ \in \mathcal QQ∈Q: up to a polar set they are exactly the wealth processes of strategies that consume.

The result is proved in the paper; no part of it has a machine-checked proof, on the platform or in Mathlib. Mathlib has martingales, conditional expectation and analytic sets. It has no quasi-sure analysis, no product of measurable selectors of a random set of measures, no conditional sublinear expectation and no superhedging. The mission produces a machine-checked development of the one-period-to-multi-period machinery of the paper (Theorem 4.5, Lemmas 4.6 and 4.10) and of the decomposition itself.

Difficulty

With one dominating measure, the classical proof works under a fixed equivalent martingale measure and uses conditional expectations and a single null-set structure. Here the measures in P\mathcal PP may be mutually singular, so conditional expectations under different QQQ disagree off their supports, and no countable family of measures controls all null sets. The proof has to work node by node, ω↦Pt(ω)\omega \mapsto \mathcal P_t(\omega)ω↦Pt​(ω). Every object built at a node (the worst-case conditional expectation, a near-optimal measure, a hedging ratio) must then be glued back together measurably in ω\omegaω. Borel measurability is not preserved by taking suprema over the random set Qt(ω)\mathcal Q_t(\omega)Qt​(ω). Upper semianalyticity is, but only together with measurable selection theorems for analytic sets (Jankov–von Neumann) and the universal completion. The first idea, which is to apply the classical theorem under each P∈PP \in \mathcal PP∈P separately, fails. It gives one strategy per model, and in general uncountably many models cannot be aggregated into one strategy.

Formalization scope

The Lean development uses the following conventions.

  • Paths and measures. Ωt\Omega_tΩt​ is Fin t → Ω₁, and measures are Borel. Ft\mathcal F_tFt​-measurability is universal measurability, which is the published platform definition BertsekasShreve.AnalyticSelection.IsUniversallyMeasurable.
  • Polar sets. A polar set is null in outer measure under every model. The exceptional sets in the statements are universally measurable, and for such sets this agrees with the paper's definition.
  • The model set. P\mathcal PP consists of the laws of Borel Markov kernels that lie in Pt\mathcal P_tPt​ almost surely, which is the paper's equivalent formulation on p. 4.
  • Processes. A process is a family V t : (Fin t → Ω₁) → ℝ, so adaptedness is built into the type.
  • Strategies. The Lean strategy H u is the paper's Hu+1H_{u+1}Hu+1​.
  • Expectations. Expectations of functions with values in [−∞,∞][-\infty, \infty][−∞,∞] follow (1.1) in EReal, with ∞−∞=−∞\infty - \infty = -\infty∞−∞=−∞. Suprema over Qt(ω)\mathcal Q_t(\omega)Qt​(ω) are taken in EReal.
  • Options. The setting has no options (e=0e = 0e=0).
  • Page numbers. Pages and indices are those of the arXiv v3 reprint (arXiv:1305.6008v3), not the journal pagination 823–859.

The increasing process KKK must be adapted and nondecreasing on every path. Dropping monotonicity would make condition 2 trivially true, with K:=V0+H∙S−VK := V_0 + H \bullet S - VK:=V0​+H∙S−V for any HHH. Integrability and supermartingale properties are always stated with explicit QQQ-integrability, so Bochner integrals of non-integrable functions cannot make a statement vacuous.

The development needs the following infrastructure:

  • analytic sets and measurable selection (some of it exists for Bertsekas–Shreve on the platform);
  • measurability of (ω,Q)↦EQ[f(ω,⋅)](\omega, Q) \mapsto E_Q[f(\omega,\cdot)](ω,Q)↦EQ​[f(ω,⋅)];
  • products of kernels;
  • the one-period fundamental theorem and superhedging duality.

These pieces are shared with the companion mission Arbitrage and Duality in Nondominated Discrete-Time Models I, which formalizes the superhedging theorem. Contributions to either side are welcome. The paper derives (ii) ⇒ (i) from Lemma A.1, a classical fact about local and generalized martingales under one measure, which is not posed as a milestone here.

Selected references

  • B. Bouchard, M. Nutz, Arbitrage and duality in nondominated discrete-time models, Ann. Appl. Probab. 25(2), 823–859, 2015. https://doi.org/10.1214/14-AAP1011, arXiv:1305.6008v3 https://arxiv.org/abs/1305.6008
  • N. El Karoui, M.-C. Quenez, Dynamic programming and pricing of contingent claims in an incomplete market, SIAM J. Control Optim. 33, 29–66, 1995. MR1311659, https://mathscinet.ams.org/mathscinet-getitem?mr=1311659
  • D. O. Kramkov, Optional decomposition of supermartingales and hedging contingent claims in incomplete security markets, Probab. Theory Related Fields 105, 459–479, 1996. MR1402653, https://mathscinet.ams.org/mathscinet-getitem?mr=1402653
  • M. Nutz, Superreplication under model uncertainty in discrete time, Finance Stoch. 18, 791–803, 2014. MR3255751, https://mathscinet.ams.org/mathscinet-getitem?mr=3255751
  • D. P. Bertsekas, S. E. Shreve, Stochastic Optimal Control: The Discrete Time Case, Mathematics in Science and Engineering 139, Academic Press, 1978. MR0511544, https://mathscinet.ams.org/mathscinet-getitem?mr=0511544
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Control TheoryPartial Differential EquationsProbability·Captain: mikedeng1

Viscosity Solutions to Parabolic Master Equations and McKean–Vlasov SDEs with Closed-Loop Controls 2: Comparison Principle and Uniqueness for Viscosity Solutions of Parabolic Master EquationsResearch Paper

Motivation

Master equations are partial differential equations whose state variable is a probability measure. They arise as the dynamic programming equations of mean-field control problems, as the limits of large particle systems, and as the pricing equations of options on a whole population. Their coefficients and solutions are functions on a Wasserstein space, which is infinite dimensional, and classical (smooth) solutions are known only under strong regularity assumptions (Cardaliaguet–Delarue–Lasry–Lions 2019). A notion of weak solution for which existence, comparison and uniqueness can all be proved is therefore the basic missing tool.

C. Wu and J. Zhang (Ann. Appl. Probab. 2020) propose such a notion for parabolic master equations on the space of laws of continuous paths, in the spirit of the viscosity theory for path-dependent PDEs of Ekren, Keller, Touzi and Zhang (Ann. Probab. 2014). This mission formalizes its §4: the definition of viscosity solutions and the comparison principle that makes them unique.

Setting

Fix a horizon TTT and a dimension ddd. The canonical space is Ω=C([0,T];Rd)\Omega=C([0,T];\mathbb R^d)Ω=C([0,T];Rd) with the uniform norm ∥ω∥\|\omega\|∥ω∥, the canonical process is Xt(ω)=ωtX_t(\omega)=\omega_tXt​(ω)=ωt​, and Ft=σ(Xs:s≤t)\mathcal F_t=\sigma(X_s:s\le t)Ft​=σ(Xs​:s≤t). P2\mathcal P_2P2​ is the set of probability measures μ\muμ on Ω\OmegaΩ with Eμ∥X∥2<∞\mathbb E^\mu\|X\|^2<\inftyEμ∥X∥2<∞; μ[0,t]\mu_{[0,t]}μ[0,t]​ is the law of the stopped path Xt∧⋅X_{t\wedge\cdot}Xt∧⋅​. The state space is Θ=[0,T]×P2\Theta=[0,T]\times\mathcal P_2Θ=[0,T]×P2​ with the pseudometric

W2((t,μ),(t′,μ′))=(∣t−t′∣+W22(μ[0,t],μ[0,t′]′))1/2,\mathcal W_2\big((t,\mu),(t',\mu')\big)=\big(|t-t'|+\mathcal W_2^2(\mu_{[0,t]},\mu'_{[0,t']})\big)^{1/2},W2​((t,μ),(t′,μ′))=(∣t−t′∣+W22​(μ[0,t]​,μ[0,t′]′​))1/2,

where W2\mathcal W_2W2​ on laws is the 2-Wasserstein distance. A function V:Θ→RV:\Theta\to\mathbb RV:Θ→R has a time derivative ∂tV\partial_tV∂t​V, a path derivative ∂μV(t,μ,ω)∈Rd\partial_\mu V(t,\mu,\omega)\in\mathbb R^d∂μ​V(t,μ,ω)∈Rd and a second derivative ∂ω∂μV(t,μ,ω)∈Rd×d\partial_\omega\partial_\mu V(t,\mu,\omega)\in\mathbb R^{d\times d}∂ω​∂μ​V(t,μ,ω)∈Rd×d, defined through a functional Itô formula along semimartingale laws.

The master equation (3.1) is

LV(t,μ):=∂tV(t,μ)+G(t,μ,V(t,μ),∂μV(t,μ,⋅),∂ω∂μV(t,μ,⋅))=0,\mathbb LV(t,\mu):=\partial_tV(t,\mu)+G\big(t,\mu,V(t,\mu),\partial_\mu V(t,\mu,\cdot),\partial_\omega\partial_\mu V(t,\mu,\cdot)\big)=0,LV(t,μ):=∂t​V(t,μ)+G(t,μ,V(t,μ),∂μ​V(t,μ,⋅),∂ω​∂μ​V(t,μ,⋅))=0,

with a generator GGG that is continuous in (t,μ)(t,\mu)(t,μ), Lipschitz in yyy, and Lipschitz in (Z,Γ)(Z,\Gamma)(Z,Γ) in the averaged sense (3.2) of Assumption 3.1.

For L>0L>0L>0, PL(t,μ)\mathcal P_L(t,\mu)PL​(t,μ) is the set of laws P∈P2\mathbb P\in\mathcal P_2P∈P2​ that agree with μ\muμ up to time ttt and under which XXX is a semimartingale on [t,T][t,T][t,T] with drift bounded by LLL and half squared diffusion bounded by LLL. Test functions at (t,μ)(t,\mu)(t,μ) are C1,1,1C^{1,1,1}C1,1,1 functions on [t,t+δ]×PL(t,μ)[t,t+\delta]\times\mathcal P_L(t,\mu)[t,t+δ]×PL​(t,μ) touching VVV from above or below there, (4.2). V∈C0(Θ)V\in C^0(\Theta)V∈C0(Θ) is an LLL-viscosity subsolution (supersolution) if Lφ(t,μ)≥0\mathbb L\varphi(t,\mu)\ge0Lφ(t,μ)≥0 (≤0\le0≤0) for every such test function, and a viscosity solution if it is both for one L>0L>0L>0 (Definition 4.4). The Perron envelopes V‾\overline VV, V‾\underline VV​ of (4.17) are the infimum of piecewise classical supersolutions above ggg and the supremum of piecewise classical subsolutions below ggg.

Formalization targets

Goal: comparison and uniqueness (Theorem 4.13)

Under Assumption 3.1 and g∈C0(P2)g\in C^0(\mathcal P_2)g∈C0(P2​), if V1V_1V1​ is a viscosity subsolution, V2V_2V2​ a viscosity supersolution, V1(T,⋅)≤g≤V2(T,⋅)V_1(T,\cdot)\le g\le V_2(T,\cdot)V1​(T,⋅)≤g≤V2​(T,⋅), the classes U‾g,U‾g\underline{\mathcal U}_g,\overline{\mathcal U}_gU​g​,Ug​ are nonempty, and

V‾=V‾=:V,(4.19)\overline V=\underline V=:V,\qquad(4.19)V=V​=:V,(4.19)

then V1≤V≤V2V_1\le V\le V_2V1​≤V≤V2​ on Θ\ThetaΘ, and VVV is the unique viscosity solution with terminal condition ggg.

Milestones

  1. the moment estimate (4.1) over PL(t,μ)\mathcal P_L(t,\mu)PL​(t,μ);
  2. Lemma 4.1: [t,T]×PL(t,μ)[t,T]\times\mathcal P_L(t,\mu)[t,T]×PL​(t,μ) is compact under W2\mathcal W_2W2​;
  3. Theorem 4.7: viscosity solutions are characterized by semi-jets of paraboloids;
  4. Theorem 4.9: the change of variable V~=eλtV\tilde V=e^{\lambda t}VV~=eλtV;
  5. Theorem 4.6: consistency with classical solutions;
  6. Theorem 4.11: partial comparison when one side is smooth;
  7. Proposition 4.12: a continuous lower envelope V‾\underline VV​ is a viscosity subsolution.

Significance

The comparison principle is what turns a definition into a theory: it gives uniqueness, it identifies value functions of mean-field control problems with the solution of their master equation, and it is the input of stability and convergence arguments for numerical schemes. Theorem 4.13 reduces well-posedness to condition (4.19), and the authors verify (4.19) in examples (§4.6) via Theorem 4.14. The compactness of PL(t,μ)\mathcal P_L(t,\mu)PL​(t,μ) (Lemma 4.1) is the device that replaces local compactness, which the Wasserstein space lacks; it is reusable for any viscosity theory over semimartingale laws.

These results are proved on paper. No machine-checked development of viscosity solutions on Wasserstein spaces, or of the path-dependent functional Itô calculus on laws, is known to exist. A formalization would produce a checked notion of viscosity solution for master equations, the compactness of bounded-characteristic semimartingale laws, and the comparison machinery, and would expose the points where the printed proofs are sketched (see below).

Difficulty

The obvious route, copying the finite-dimensional theory, fails at two places. First, the doubling-of-variables argument for comparison needs a penalization on the state space that is smooth and coercive; on P2\mathcal P_2P2​ under W2\mathcal W_2W2​ neither is available, which is why comparison is reached through partial comparison and Perron envelopes. Second, maxima of φ−V\varphi-Vφ−V need not be attained on Wasserstein balls, which are not compact; the theory therefore tests only on [t,T]×PL(t,μ)[t,T]\times\mathcal P_L(t,\mu)[t,T]×PL​(t,μ), and Lemma 4.1 (via Zheng's tightness criterion for semimartingale laws and uniform integrability of ∥X∥2\|X\|^2∥X∥2) is what makes the extrema exist. The printed proof of Theorem 4.13 opens with "V‾\overline VV is lower semicontinuous and V‾\underline VV​ is upper semicontinuous"; as printed the directions are swapped (an infimum of functions continuous in μ\muμ is upper semicontinuous in μ\muμ), and the members of U\mathcal UU are only càdlàg in ttt, so the continuity of VVV needed for the conclusion requires an argument of its own.

Formalization scope

Time is R≥0\mathbb R_{\ge0}R≥0​, and every condition is imposed only at t≤Tt\le Tt≤T, μ∈P2\mu\in\mathcal P_2μ∈P2​. Rd\mathbb R^dRd is the Euclidean space, matrices are d×dd\times dd×d real matrices with the Frobenius norm, and A:B=∑ijAijBijA:B=\sum_{ij}A_{ij}B_{ij}A:B=∑ij​Aij​Bij​. W2\mathcal W_2W2​ is the published WassersteinDRO.Duality.wassersteinDistance on laws of paths; Brownian motion and the Itô integral are the published EthierKurtz definitions. Membership in PL(t,μ)\mathcal P_L(t,\mu)PL​(t,μ) is the existence of a representation of P\mathbb PP as the law of an Itô process from time ttt with ∣b∣≤L|b|\le L∣b∣≤L, 12∣σ∣2≤L\tfrac12|\sigma|^2\le L21​∣σ∣2≤L (§2.4). A C1,1,1C^{1,1,1}C1,1,1 object is a record of a function and three derivative functions, and the functional Itô formula (2.25) is required in drift form for every representation, which equals (2.25) because the stochastic integral has mean zero. Test sets encode "inf⁡(φ−V)=0\inf(\varphi-V)=0inf(φ−V)=0" literally, and the data of a test function at (t,μ)(t,\mu)(t,μ) are its values at (t,P)(t,\mathbb P)(t,P), P∈PL(t,μ)\mathbb P\in\mathcal P_L(t,\mu)P∈PL​(t,μ). The Perron envelopes are extended-real infima and suprema over the classes (4.18); (4.19) is stated with a real-valued VVV.

Two readings are fixed. Assumption 3.1(i) is continuity of (t,μ)↦G(t,μ,y,Z(Xt∧⋅),Γ(Xt∧⋅))(t,\mu)\mapsto G(t,\mu,y,Z(X_{t\wedge\cdot}),\Gamma(X_{t\wedge\cdot}))(t,μ)↦G(t,μ,y,Z(Xt∧⋅​),Γ(Xt∧⋅​)) for fixed continuous Z,ΓZ,\GammaZ,Γ of linear growth. "V∈Cb1,1,1(Θ)V\in C_b^{1,1,1}(\Theta)V∈Cb1,1,1​(Θ)" in Theorems 4.6 and 4.11 is replaced by the larger class it is used through (Remark 4.3(i)): data continuous on Θ\ThetaΘ lying in Cb1,1,1([t1,t2]×PL(t1,μ))C_b^{1,1,1}([t_1,t_2]\times\mathcal P_L(t_1,\mu))Cb1,1,1​([t1​,t2​]×PL​(t1​,μ)) for all t1<t2t_1<t_2t1​<t2​, LLL, μ\muμ, so those statements are at least as strong as printed.

The definitions cannot be satisfied vacuously: every test set requires a witness law in PL(t,μ)\mathcal P_L(t,\mu)PL​(t,μ), the class Cb1,1,1C_b^{1,1,1}Cb1,1,1​ contains the constants (checked in Lean), and a viscosity solution uses one LLL for both halves. The semi-jets range only over Ft\mathcal F_tFt​-measurable continuous arguments of linear growth, as printed.

Contributions are welcome at every level: the moment bound (4.1) and Lemma 4.1 need tightness and uniform-integrability results for semimartingale laws on path space that Mathlib does not have; Theorems 4.7 and 4.9 are self-contained manipulations of the definitions; Theorems 4.6 and 4.11 and Proposition 4.12 need the compactness lemma and the Itô identity of test functions.

Selected references

  • C. Wu, J. Zhang, Viscosity solutions to parabolic master equations and McKean–Vlasov SDEs with closed-loop controls, Ann. Appl. Probab. 30(2) (2020) 936–986. https://doi.org/10.1214/19-AAP1521
  • I. Ekren, C. Keller, N. Touzi, J. Zhang, On viscosity solutions of path dependent PDEs, Ann. Probab. 42(1) (2014) 204–236. https://doi.org/10.1214/12-AOP788
  • P. Cardaliaguet, F. Delarue, J.-M. Lasry, P.-L. Lions, The Master Equation and the Convergence Problem in Mean Field Games, Annals of Mathematics Studies 201, Princeton University Press, 2019. https://doi.org/10.2307/j.ctvckq7qf
  • 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
  • W. A. Zheng, Tightness results for laws of diffusion processes application to stochastic mechanics, Ann. Inst. H. Poincaré Probab. Statist. 21(2) (1985) 103–124. http://www.numdam.org/item/AIHPB_1985__21_2_103_0/
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Algorithmic Game TheoryDynamic ProgrammingProbability+1·Captain: mikedeng1

Approximate Markov-Nash Equilibria for Discrete-Time Risk-Sensitive Mean-Field Games 2: The Mean-Field Equilibrium Policy Is an ε-Markov-Nash Equilibrium of Every Large Enough N-Agent GameResearch Paper

Motivation

Games with many interacting agents, such as traffic participants, users of a shared communication channel or firms in a market, are rarely solvable exactly: a Nash equilibrium of an NNN-player stochastic game requires each agent to track the whole population, and its computation grows with NNN. Mean-field game theory replaces the population by its limiting distribution. A single representative agent faces a deterministic flow of state distributions, and consistency requires that this flow is the one the agent's own optimal policy generates. The equilibrium of this limit problem is then used as an approximate equilibrium of the finite game, with each agent acting only on its own state.

Most of this theory concerns risk-neutral agents, who minimize an expected cost. Saldi, Başar and Raginsky (arXiv:1808.03929; Math. Oper. Res. 2020) treat discrete-time agents with an exponential utility of the discounted cost, the classical risk-sensitive criterion that penalizes the variance of the cost as well as its mean. The paper proves two results: a mean-field equilibrium exists (Theorem 1, the first mission of this series), and the equilibrium policy is an approximate Nash equilibrium of every large enough finite game (Theorem 3, this mission). The risk-neutral counterpart is Saldi, Başar and Raginsky, SIAM J. Control Optim. 2018 (arXiv:1612.07878).

Setting

States lie in a Polish metric space X\mathsf XX, actions in a compact Polish space A\mathsf AA, and P(X)\mathcal P(\mathsf X)P(X) is the set of Borel probability measures with the weak topology. The model consists of a transition kernel p(⋅∣x,a,μ)p(\cdot\mid x,a,\mu)p(⋅∣x,a,μ), a one-stage cost c(x,a,μ)≥0c(x,a,\mu)\ge0c(x,a,μ)≥0, an initial law μ0\mu_0μ0​, a discount factor β∈(0,1)\beta\in(0,1)β∈(0,1) and a risk factor λ>0\lambda>0λ>0.

In the NNN-agent game, the states xiN(0)x^N_i(0)xiN​(0) are i.i.d. μ0\mu_0μ0​. At each time ttt, agent iii draws aiN(t)∼πti(⋅∣xiN(t))a^N_i(t)\sim\pi^i_t(\cdot\mid x^N_i(t))aiN​(t)∼πti​(⋅∣xiN​(t)) from its Markov policy πi\pi^iπi, and the next states are drawn independently from p(⋅∣xiN(t),aiN(t),et(N))p(\cdot\mid x^N_i(t),a^N_i(t),e^{(N)}_t)p(⋅∣xiN​(t),aiN​(t),et(N)​), where et(N)=1N∑jδxjN(t)e^{(N)}_t=\frac1N\sum_{j}\delta_{x^N_j(t)}et(N)​=N1​∑j​δxjN​(t)​ is the empirical distribution of the states. Agent iii's cost is

Ji(N)(π(N))=Eπ(N)[eλ∑t=0∞βtc(xiN(t),aiN(t),et(N))].J^{(N)}_i(\boldsymbol\pi^{(N)})=E^{\boldsymbol\pi^{(N)}}\Big[e^{\lambda\sum_{t=0}^\infty\beta^tc(x^N_i(t),a^N_i(t),e^{(N)}_t)}\Big].Ji(N)​(π(N))=Eπ(N)[eλ∑t=0∞​βtc(xiN​(t),aiN​(t),et(N)​)].

A profile is an ε\varepsilonε-Markov-Nash equilibrium if no agent can lower its Ji(N)J^{(N)}_iJi(N)​ by more than ε\varepsilonε by switching to another Markov policy.

In the mean-field game, one agent faces a flow μ=(μt)\boldsymbol\mu=(\mu_t)μ=(μt​): x(t+1)∼p(⋅∣x(t),a(t),μt)x(t+1)\sim p(\cdot\mid x(t),a(t),\mu_t)x(t+1)∼p(⋅∣x(t),a(t),μt​), with cost Jμ(π)=Eπ[eλ∑tβtc(x(t),a(t),μt)]J_{\boldsymbol\mu}(\pi)=E^\pi[e^{\lambda\sum_t\beta^tc(x(t),a(t),\mu_t)}]Jμ​(π)=Eπ[eλ∑t​βtc(x(t),a(t),μt​)]. A mean-field equilibrium is a pair (π,μ)(\pi,\boldsymbol\mu)(π,μ) in which π\piπ minimizes JμJ_{\boldsymbol\mu}Jμ​ and μ=Λ(π)\boldsymbol\mu=\Lambda(\pi)μ=Λ(π) is the flow of state laws that π\piπ generates.

The hypotheses are Assumption 1 (bounded continuous ccc with ∣c∣≤K|c|\le K∣c∣≤K, weakly continuous ppp, compact A\mathsf AA, and a moment function www with ∫w dp≤αw\int w\,dp\le\alpha w∫wdp≤αw and ∫w dμ0<∞\int w\,d\mu_0<\infty∫wdμ0​<∞) and Assumption 2. Part (a) of Assumption 2 asks that the moduli

ωp(r)=sup⁡x,asup⁡dBL(μ,ν)≤r∥p(⋅∣x,a,μ)−p(⋅∣x,a,ν)∥TV,ωc(r)=sup⁡x,asup⁡dBL(μ,ν)≤r∣c(x,a,μ)−c(x,a,ν)∣\omega_p(r)=\sup_{x,a}\sup_{d_{BL}(\mu,\nu)\le r}\|p(\cdot\mid x,a,\mu)-p(\cdot\mid x,a,\nu)\|_{TV},\qquad\omega_c(r)=\sup_{x,a}\sup_{d_{BL}(\mu,\nu)\le r}|c(x,a,\mu)-c(x,a,\nu)|ωp​(r)=x,asup​dBL​(μ,ν)≤rsup​∥p(⋅∣x,a,μ)−p(⋅∣x,a,ν)∥TV​,ωc​(r)=x,asup​dBL​(μ,ν)≤rsup​∣c(x,a,μ)−c(x,a,ν)∣

tend to 000, where dBLd_{BL}dBL​ is the bounded-Lipschitz metric. Part (b) asks that the equilibrium policy π\piπ be weakly continuous in the state.

Formalization targets

Goal: Theorem 3 (p. 23)

For every ε>0\varepsilon>0ε>0 there is N(ε)N(\varepsilon)N(ε) such that, for every N≥N(ε)N\ge N(\varepsilon)N≥N(ε), the profile (π,…,π)(\pi,\dots,\pi)(π,…,π) is an ε\varepsilonε-Markov-Nash equilibrium:

Ji(N)(π,…,π)≤inf⁡σ∈MJi(N)(π,…,σ,…,π)+εfor all i.J^{(N)}_i(\pi,\dots,\pi)\le\inf_{\sigma\in\mathsf M}J^{(N)}_i(\pi,\dots,\sigma,\dots,\pi)+\varepsilon\qquad\text{for all }i .Ji(N)​(π,…,π)≤σ∈Minf​Ji(N)​(π,…,σ,…,π)+εfor all i.

The statement fixes no rate. It is the paper's main approximation result.

Milestones

The milestones follow the paper's proof. The first seven work in an augmented model, whose state s=(x,c)s=(x,c)s=(x,c) carries the accumulated discounted cost, so that the exponential criterion becomes a terminal cost eλc(n+1)e^{\lambda c(n+1)}eλc(n+1). They are: Proposition 6 (the augmented model has the same finite-horizon costs); Lemma 5 (the augmented flow Δt+1=ΔtPt,Δtπ\Delta_{t+1}=\Delta_tP^\pi_{t,\Delta_t}Δt+1​=Δt​Pt,Δt​π​); Proposition 7 (propagation of chaos, L(Δt(N))→δΔt\mathcal L(\Delta^{(N)}_t)\to\delta_{\Delta_t}L(Δt(N)​)→δΔt​​); Proposition 8 (convergence of the augmented cost); Proposition 9 (propagation of chaos with one deviating agent); Proposition 10 (the deviating agent's state law); Proposition 11 (the deviating agent's augmented cost). The last three are stated in the original model: Theorem 4 (the finite-horizon limits (14)–(15)), Corollary 1 (the infinite-horizon comparison), and the first display of the proof of Theorem 3 (deviations may be restricted to weakly continuous policies).

Significance

Theorem 3 justifies the use of a mean-field equilibrium as a decentralized policy in risk-sensitive games with many players. The equilibrium is computed once, from a single-agent problem, and each agent uses only its own state, yet no agent of a large enough population gains more than ε\varepsilonε by deviating. The result extends the risk-neutral approximation theorem to the multiplicative criterion. Because the exponential cost does not decompose over time, the risk-neutral argument cannot be applied directly: the proof first passes through the augmented model and a finite-horizon truncation.

The result is proved in the paper; none of it is formalized. The mission formalizes the statement and the proof's intermediate results. That requires the NNN-agent law, a product of NNN kernels driven by the empirical measure, built from Mathlib's Ionescu-Tulcea construction, and propagation of chaos for an interacting Markov chain on a Polish space. Alternative proofs of any milestone are welcome, as are quantitative versions of the limits.

Difficulty

The cost is the expectation of a product of one-stage factors, not a sum, so the convergence of the empirical measure gives no direct control of it. The paper therefore enlarges the state with the accumulated cost, and the finite-horizon limits must then be transferred back to the infinite horizon through a uniform tail bound. The coupling between agents runs through the empirical measure, which enters both the transition and the cost. Propagation of chaos (Proposition 7) is an induction over time that needs continuity of ppp and ccc in the measure argument uniformly in (x,a)(x,a)(x,a) (Assumption 2-(a)) and a conditional variance bound. The deviating agent is not exchangeable with the others: its state law must be compared with that of a mean-field chain under its own policy (Proposition 10), uniformly over arbitrary sequences of deviations. Finally, a best response may be only measurable. The reduction to weakly continuous deviations, which the paper takes from its risk-neutral predecessor, is needed before any weak-convergence argument applies.

Formalization scope

Lean namespace RiskSensMFG.Nash. The definitions are in four files: the model, policies, the single-agent law and the flow (Model); the mean-field equilibrium, dBLd_{BL}dBL​, total variation and Assumption 2-(a) (Equilibrium); the NNN-agent game (Game); and the augmented model (Augmented). Conventions:

  • X\mathsf XX is a complete separable metric space with its Borel σ\sigmaσ-field, and A\mathsf AA is a compact Polish space. P(X)\mathcal P(\mathsf X)P(X) is Mathlib's ProbabilityMeasure with the weak topology and its Borel σ\sigmaσ-field (not the Giry one), and ppp is a Markov Kernel. The standing assumptions β∈(0,1)\beta\in(0,1)β∈(0,1), λ>0\lambda>0λ>0 and c≥0c\ge0c≥0 measurable are a predicate Model.Standing. Assumption 1 is stated in full, including the moment function, although the proof of Theorem 3 does not use parts (d)–(e).
  • Time is 0-based. Agents are indexed by Fin N, and the paper's Agent 1 is index 0; limits in NNN are taken along N+1N+1N+1 so that Agent 1 exists. The empirical measure of the empty configuration is set to μ0\mu_0μ0​ and enters no statement.
  • The equilibrium's optimality is required against Markov policies only, which is a weaker hypothesis than Definition 3's optimality over all policies, so the goal is at least as strong as printed. The ε\varepsilonε of Definition 2 is on the scale of J=E[eλ∑βtc]J=E[e^{\lambda\sum\beta^tc}]J=E[eλ∑βtc]. Equilibrium and optimality are stated in "for every deviation" form, with no infimum over a type.
  • Assumption 2-(a) and the modulus ωg\omega_gωg​ of Proposition 10 are written as ε\varepsilonε–δ\deltaδ statements, which is equivalent to "ω(r)→0\omega(r)\to0ω(r)→0" because the moduli are nondecreasing. Total variation is sup⁡∣g∣≤1∣∫g dμ−∫g dν∣\sup_{|g|\le1}|\int g\,d\mu-\int g\,d\nu|sup∣g∣≤1​∣∫gdμ−∫gdν∣.
  • The augmented cost coordinate is the discounted sum ∑k<tβkc(⋅)\sum_{k<t}\beta^kc(\cdot)∑k<t​βkc(⋅); the page prints it without βk\beta^kβk, which contradicts PtP_tPt​. The coordinate lies in R\mathbb RR rather than [0,L][0,L][0,L], because X×[0,L]\mathsf X\times[0,L]X×[0,L] is not invariant under PtP_tPt​, and the terminal cost is eλmax⁡(0,min⁡(c,L))e^{\lambda\max(0,\min(c,L))}eλmax(0,min(c,L)), which equals eλce^{\lambda c}eλc on reachable states. Corollary 1's printed "lim⁡≥\lim\gelim≥" (the limit is not shown to exist) is stated as three limit and eventual-inequality claims.

No hypothesis is vacuous: a sorry-free check exhibits a model satisfying the standing assumptions, Assumptions 1 and 2 and the equilibrium condition simultaneously, with Ji(N)≥1J^{(N)}_i\ge1Ji(N)​≥1. This rules out the trivial reading in which a non-integrable integrand makes every cost 000 and every profile an ε\varepsilonε-equilibrium. Theorem 1 (existence of the equilibrium) is the other mission of the series; here the equilibrium is a hypothesis.

Selected references

  • N. Saldi, T. Başar, M. Raginsky, Discrete-time Risk-sensitive Mean-field Games, arXiv:1808.03929v2, 2018; published as Approximate Markov-Nash Equilibria for Discrete-Time Risk-Sensitive Mean-Field Games, Math. Oper. Res. 45(4), 2020. https://arxiv.org/abs/1808.03929, https://doi.org/10.1287/moor.2019.1044
  • N. Saldi, T. Başar, M. Raginsky, Markov–Nash Equilibria in Mean-Field Games with Discounted Cost, SIAM J. Control Optim. 56(6), 2018. https://arxiv.org/abs/1612.07878
  • N. Bäuerle, U. Rieder, More Risk-Sensitive Markov Decision Processes, Math. Oper. Res. 39(1), 2014. https://doi.org/10.1287/moor.2013.0601
  • O. Hernández-Lerma, J. B. Lasserre, Discrete-Time Markov Control Processes: Basic Optimality Criteria, Springer, 1996. https://doi.org/10.1007/978-1-4612-0729-0
  • R. M. Dudley, Real Analysis and Probability, Cambridge University Press, 2002 (§11.3, the bounded-Lipschitz metric). https://doi.org/10.1017/CBO9780511755347
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Operations ResearchOptimal TransportOptimization+1·Captain: mikedeng1

Sinkhorn Distributionally Robust Optimization 1: Strong Duality — the Worst-Case Expectation over a Sinkhorn Ball Equals inf over λ ≥ 0 of λρ̄ + λε·E log E_Q[e^{f/(λε)}]Research Paper

Motivation

Distributionally robust optimization (DRO) hedges a decision against uncertainty in the data distribution. It minimizes the worst-case expected loss over an ambiguity set of distributions around a nominal one, typically the empirical distribution of the data. Ambiguity sets built from the Wasserstein (optimal-transport) distance are standard in operations research and machine learning, because they contain distributions with supports different from the nominal one. A known drawback is that the worst case is attained at discrete distributions, which is unrealistic when the true distribution is continuous.

Wang, Gao and Xie (arXiv:2109.11926v5) replace the Wasserstein distance by the Sinkhorn distance, the entropically regularized optimal-transport cost of Cuturi (NeurIPS 2013). Their main theorem is a strong duality result: the infinite-dimensional worst-case problem over a Sinkhorn ball equals a one-dimensional convex minimization. This mission formalizes that theorem.

Timeline:

  • 2013: Cuturi introduces the Sinkhorn distance as a fast surrogate for optimal transport.
  • 2016–2023: strong duality for Wasserstein DRO, by Gao and Kleywegt (arXiv:1604.02199), Blanchet and Murthy (arXiv:1604.01446), and Zhang, Yang and Gao (arXiv:2205.00362).
  • 2021–2025: Wang, Gao and Xie prove strong duality for Sinkhorn DRO for a general measurable sample space, a measurable loss and an arbitrary nominal distribution.

Setting

Let Z\mathcal ZZ be a measurable space. The data are:

  • a nominal probability distribution P^\widehat{\mathbb P}P;
  • a σ-finite reference measure ν≠0\nu\neq0ν=0;
  • a transport cost c:Z×Z→[0,∞]c:\mathcal Z\times\mathcal Z\to[0,\infty]c:Z×Z→[0,∞];
  • a regularization parameter ϵ>0\epsilon>0ϵ>0 and a radius ρ∈R\rho\in\mathbb Rρ∈R;
  • a loss f:Z→R∪{∞}f:\mathcal Z\to\mathbb R\cup\{\infty\}f:Z→R∪{∞}.

For a probability distribution P\mathbb PP, the Sinkhorn distance (Definition 1, with reference measures P^\widehat{\mathbb P}P and ν\nuν) is

Wϵ(P^,P)=inf⁡γ∈Γ(P^,P)E(x,y)∼γ[c(x,y)+ϵlog⁡dγ(x,y)dP^(x) dν(y)],\mathcal W_\epsilon(\widehat{\mathbb P},\mathbb P)=\inf_{\gamma\in\Gamma(\widehat{\mathbb P},\mathbb P)}\mathbb E_{(x,y)\sim\gamma}\Big[c(x,y)+\epsilon\log\frac{d\gamma(x,y)}{d\widehat{\mathbb P}(x)\,d\nu(y)}\Big],Wϵ​(P,P)=γ∈Γ(P,P)inf​E(x,y)∼γ​[c(x,y)+ϵlogdP(x)dν(y)dγ(x,y)​],

where Γ(P^,P)\Gamma(\widehat{\mathbb P},\mathbb P)Γ(P,P) is the set of couplings with these marginals. The primal value is the worst-case expected loss over the Sinkhorn ball,

V=sup⁡{EP[f]: Wϵ(P^,P)≤ρ}.V=\sup\big\{\mathbb E_{\mathbb P}[f]:\ \mathcal W_\epsilon(\widehat{\mathbb P},\mathbb P)\le\rho\big\}.V=sup{EP​[f]: Wϵ​(P,P)≤ρ}.

The dual problem uses three more objects. The kernel distribution is dQx,ϵ(z)∝e−c(x,z)/ϵ dν(z)d\mathbb Q_{x,\epsilon}(z)\propto e^{-c(x,z)/\epsilon}\,d\nu(z)dQx,ϵ​(z)∝e−c(x,z)/ϵdν(z). The adjusted radius is ρˉ=ρ+ϵ Ex∼P^[log⁡Ez∼νe−c(x,z)/ϵ]\bar\rho=\rho+\epsilon\,\mathbb E_{x\sim\widehat{\mathbb P}}[\log\mathbb E_{z\sim\nu}e^{-c(x,z)/\epsilon}]ρˉ​=ρ+ϵEx∼P​[logEz∼ν​e−c(x,z)/ϵ]. The dual value is

VD=inf⁡λ≥0{λρˉ+λϵ Ex∼P^[log⁡Ez∼Qx,ϵ[ef(z)/(λϵ)]]},V_D=\inf_{\lambda\ge0}\Big\{\lambda\bar\rho+\lambda\epsilon\,\mathbb E_{x\sim\widehat{\mathbb P}}\Big[\log\mathbb E_{z\sim\mathbb Q_{x,\epsilon}}\big[e^{f(z)/(\lambda\epsilon)}\big]\Big]\Big\},VD​=λ≥0inf​{λρˉ​+λϵEx∼P​[logEz∼Qx,ϵ​​[ef(z)/(λϵ)]]},

where the objective at λ=0\lambda=0λ=0 is ess sup⁡νf\operatorname{ess\,sup}_\nu fesssupν​f.

Assumption 1 requires:

  • ccc is measurable and, for P^\widehat{\mathbb P}P-a.e. xxx, finite ν\nuν-a.e.;
  • Eνe−c(x,⋅)/ϵ<∞\mathbb E_\nu e^{-c(x,\cdot)/\epsilon}<\inftyEν​e−c(x,⋅)/ϵ<∞ for P^\widehat{\mathbb P}P-a.e. xxx;
  • fff is measurable;
  • every coupling with first marginal P^\widehat{\mathbb P}P disintegrates along P^\widehat{\mathbb P}P.

Condition 1 asks for some λ>0\lambda>0λ>0 with EQx,ϵ[ef/(λϵ)]<∞\mathbb E_{\mathbb Q_{x,\epsilon}}[e^{f/(\lambda\epsilon)}]<\inftyEQx,ϵ​​[ef/(λϵ)]<∞ for P^\widehat{\mathbb P}P-a.e. xxx.

Formalization targets

Goal: Theorem 1 (strong duality)

Under Assumption 1:

(I)  ∃ P: Wϵ(P^,P)≤ρ  ⟺  ρˉ≥0;(II)  ρˉ≥0  ⟹  V=VD.\text{(I) }\ \exists\,\mathbb P:\ \mathcal W_\epsilon(\widehat{\mathbb P},\mathbb P)\le\rho\iff\bar\rho\ge0;\qquad \text{(II) }\ \bar\rho\ge0\implies V=V_D.(I)  ∃P: Wϵ​(P,P)≤ρ⟺ρˉ​≥0;(II)  ρˉ​≥0⟹V=VD​.

(III) If ρˉ>0\bar\rho>0ρˉ​>0, then V=VD<∞V=V_D<\inftyV=VD​<∞ when the dual objective is finite at some λ>0\lambda>0λ>0, and V=VD=∞V=V_D=\inftyV=VD​=∞ otherwise.

(IV) If ρˉ>0\bar\rho>0ρˉ​>0 and Condition 1 holds, then 000 is the unique dual minimizer if and only if

ess sup⁡νf<∞andρˉ≥ϵ Ex∼P^[log⁡(1/Qx,ϵ(A))],A={f=ess sup⁡νf}.\operatorname{ess\,sup}_\nu f<\infty\quad\text{and}\quad\bar\rho\ge\epsilon\,\mathbb E_{x\sim\widehat{\mathbb P}}\big[\log\big(1/\mathbb Q_{x,\epsilon}(A)\big)\big],\qquad A=\{f=\operatorname{ess\,sup}_\nu f\}.esssupν​f<∞andρˉ​≥ϵEx∼P​[log(1/Qx,ϵ​(A))],A={f=esssupν​f}.

Milestones

The milestones are the numbered lemmas of the paper's proof, in the order the proof uses them:

  • Lemma EC.2: the Gibbs variational principle, sup⁡P≪νEP[f−τlog⁡dPdν]=τlog⁡Eνef/τ\sup_{\mathbb P\ll\nu}\mathbb E_{\mathbb P}[f-\tau\log\frac{d\mathbb P}{d\nu}]=\tau\log\mathbb E_\nu e^{f/\tau}supP≪ν​EP​[f−τlogdνdP​]=τlogEν​ef/τ.
  • Lemma EC.3: measurability of the inner value x↦vx(λ)x\mapsto v_x(\lambda)x↦vx​(λ).
  • Lemma 1: weak duality V≤VDV\le V_DV≤VD​.
  • Lemma 2: a KL-constrained reformulation of the primal problem.
  • Lemma EC.4: existence of a dual minimizer.
  • Lemma 3: the first-order condition (9) and uniqueness when λ∗>0\lambda^*>0λ∗>0.
  • Lemma EC.5: the criterion for λ∗=0\lambda^*=0λ∗=0.

Significance

The result. Theorem 1 turns a supremum over an infinite-dimensional set of distributions into a scalar convex program. That program can be solved by first-order methods using only samples from P^\widehat{\mathbb P}P and from the kernels Qx,ϵ\mathbb Q_{x,\epsilon}Qx,ϵ​, which is the basis of the paper's algorithm (Section 4). The proof also constructs the worst-case distribution: it is absolutely continuous with respect to ν\nuν, not discrete. Theorem 1(IV) says exactly when the ambiguity constraint is binding. The finite-support conic reformulation (Corollary 1) and the closed form for linear losses (Example 1) both follow from the theorem.

Formalizing it. The theorem is proved in the paper; no machine-checked proof exists. Formalization adds two things. First, it pins down the extended-valued conventions: VVV, VDV_DVD​ and fff all take values in [−∞,∞][-\infty,\infty][−∞,∞], and the paper does not specify how undefined expectations and the λ=0\lambda=0λ=0 objective are treated. Second, it checks every case of the proof, including the degenerate ones. Doing so has already corrected two statements; see Formalization scope.

Difficulty

Weak duality (Lemma 1) is Lagrangian relaxation plus the Gibbs principle. The difficulty is the reverse inequality V≥VDV\ge V_DV≥VD​. Interchanging the supremum over distributions with the infimum over λ\lambdaλ requires a minimax theorem. The usual minimax theorems need compactness or semicontinuity in the distribution variable. The paper's setting has neither: Z\mathcal ZZ is an arbitrary measurable space, fff is only measurable and may be +∞+\infty+∞, and P^\widehat{\mathbb P}P is arbitrary. So a minimax theorem cannot be applied directly.

The proof instead constructs near-optimal primal distributions from the dual minimizer. This needs three separate cases:

  • λ∗>0\lambda^*>0λ∗>0, with a first-order condition;
  • λ∗=0\lambda^*=0λ∗=0, with a distribution concentrated on the essential maximizers of fff;
  • Condition 1 fails, with a truncation argument.

Each case needs integrability facts about EQx,ϵ[ef/(λϵ)]\mathbb E_{\mathbb Q_{x,\epsilon}}[e^{f/(\lambda\epsilon)}]EQx,ϵ​​[ef/(λϵ)] in which xxx and λ\lambdaλ interact. Disintegrating couplings (Assumption 1(IV)) and making the extended-valued expectations meaningful are a further source of work in Lean.

Formalization scope

All values (primal value, Sinkhorn distance, dual objective) are EReal. Expectations are the published DupacovaWets.Consistency.expect: ∫g+−∫g−\int g^+-\int g^-∫g+−∫g−, with lower Lebesgue integrals in [0,∞][0,\infty][0,∞] and the convention ∞−∞=+∞\infty-\infty=+\infty∞−∞=+∞. The Bochner integral appears only in ρˉ\bar\rhoρˉ​, which every theorem assumes finite.

Further conventions:

  • Sinkhorn distance. The cost and the entropy form a single integrand. A coupling not absolutely continuous with respect to P^⊗ν\widehat{\mathbb P}\otimes\nuP⊗ν contributes +∞+\infty+∞. An infeasible primal has V=−∞V=-\inftyV=−∞.
  • Dual objective. The value at λ=0\lambda=0λ=0 is defined as Mathlib's essSup f ν, not as a limit. Logarithms are ENNReal.log, so log⁡∞=∞\log\infty=\inftylog∞=∞ and log⁡0=−∞\log 0=-\inftylog0=−∞; e+∞=+∞e^{+\infty}=+\inftye+∞=+∞.
  • Kernels. Qx,ϵ\mathbb Q_{x,\epsilon}Qx,ϵ​ is a normalized withDensity measure. Families {γx}x∈supp⁡P^\{\gamma_x\}_{x\in\operatorname{supp}\widehat{\mathbb P}}{γx​}x∈suppP​ are Markov kernels on all of Z\mathcal ZZ.

Hypotheses added to the page:

  • ν\nuν is σ-finite and nonzero;
  • ϵ>0\epsilon>0ϵ>0;
  • x↦log⁡Eνe−c(x,⋅)/ϵx\mapsto\log\mathbb E_\nu e^{-c(x,\cdot)/\epsilon}x↦logEν​e−c(x,⋅)/ϵ is P^\widehat{\mathbb P}P-integrable, so that ρˉ∈R\bar\rho\in\mathbb Rρˉ​∈R.

"ν{0≤c<∞}=1\nu\{0\le c<\infty\}=1ν{0≤c<∞}=1" is read as "ν\nuν-a.e.". "λ∗=0\lambda^*=0λ∗=0" is read as "000 is the unique dual minimizer".

Corrections to the paper:

  • Theorem 1(III). The paper's version with Condition 1 is false: a.e.-finite inner expectations do not make the dual objective finite. A counterexample on N\mathbb NN is in the goal's note. The goal is stated with the integrated condition "the dual objective is finite at some λ>0\lambda>0λ>0".
  • Lemma 3. The lemma is stated under the added hypothesis that the dual objective is finite at some λ1<λ∗\lambda_1<\lambda^*λ1​<λ∗ (and is not −∞-\infty−∞ at λ∗\lambda^*λ∗). Without it, λ∗\lambda^*λ∗ can sit at the edge of the domain where the objective is finite, and (9) fails.

No statement involves an O(⋅)O(\cdot)O(⋅) constant.

A formalization that lets an undefined Sinkhorn integrand evaluate to −∞-\infty−∞ (Mathlib's ⊤+⊥=⊥\top+\bot=\bot⊤+⊥=⊥) is ruled out: it would put every distribution into the ball and make the theorem trivial. The combined integrand and the +∞+\infty+∞ convention exclude this.

A complete development needs:

  • a Gibbs/Donsker–Varadhan variational principle for σ-finite reference measures and extended-valued functions;
  • disintegration of couplings;
  • convexity and differentiation of λ↦λlog⁡Eef/λ\lambda\mapsto\lambda\log\mathbb E e^{f/\lambda}λ↦λlogEef/λ.

The first two are reusable well beyond this mission. Contributions toward any milestone, and toward these general lemmas, are welcome.

Selected references

  • J. Wang, R. Gao, Y. Xie, Sinkhorn Distributionally Robust Optimization, arXiv:2109.11926v5, 2025. https://arxiv.org/abs/2109.11926
  • M. Cuturi, Sinkhorn Distances: Lightspeed Computation of Optimal Transport, NeurIPS, 2013. https://arxiv.org/abs/1306.0895
  • R. Gao, A. Kleywegt, Distributionally Robust Stochastic Optimization with Wasserstein Distance, Mathematics of Operations Research, 2023. https://arxiv.org/abs/1604.02199
  • J. Blanchet, K. Murthy, Quantifying Distributional Model Risk via Optimal Transport, Mathematics of Operations Research, 2019. https://arxiv.org/abs/1604.01446
  • L. Zhang, J. Yang, R. Gao, A Short and General Duality Proof for Wasserstein Distributionally Robust Optimization, Operations Research, 2024. https://arxiv.org/abs/2205.00362
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Convex OptimizationOperations ResearchProbability·Captain: mikedeng1

Arbitrage and Duality in Nondominated Discrete-Time Models I: Under NA(𝒫) the Superhedging Price Equals the Supremum of Expectations over Martingale Measures and Is AttainedResearch Paper

Motivation

Classical arbitrage pricing fixes one probability measure PPP describing the market and asks for the cheapest way to dominate a payoff PPP-almost surely. When the model itself is uncertain, this choice is not available: a trader who only trusts a family P\mathcal PP of possible models wants a hedge that works under every one of them. Two literatures meet here. Robust (model-independent) finance studies hedging that must hold for all paths, as in the martingale-optimal-transport approach to option bounds (Beiglböck, Henry-Labordère, Penkner, 2013). Nondominated model uncertainty studies families P\mathcal PP with no single reference measure, as in the quasi-sure analysis of Denis–Martini (2006) and the volatility-uncertainty literature. Bouchard and Nutz (2015) give a discrete-time framework that contains both extremes (all measures on a path space; a single measure) and prove the fundamental theorems and superhedging duality for it.

Timeline of the dominated and robust predecessors:

  • 1990. Dalang, Morton and Willinger prove the discrete-time fundamental theorem of asset pricing (FTAP) for one measure.
  • 2001. Kabanov and Stricker give a short proof of the closedness of the superhedgeable cone behind the DMW theorem. The proof of Theorem 2.2 follows their argument.
  • 2013. Acciaio, Beiglböck, Penkner, Schachermayer prove a model-independent FTAP for a pathwise no-arbitrage notion, with options.
  • 2015. Bouchard and Nutz prove the FTAP, the superhedging theorem and the second FTAP under a nondominated family P\mathcal PP, with dynamic trading in stocks and static trading in finitely many options.

Setting

Fix a horizon T∈NT\in\mathbb NT∈N and a Polish space Ω1\Omega_1Ω1​. Paths are ω=(ω1,…,ωT)∈Ω=Ω1T\omega=(\omega_1,\dots,\omega_T)\in\Omega=\Omega_1^Tω=(ω1​,…,ωT​)∈Ω=Ω1T​, and Ωt=Ω1t\Omega_t=\Omega_1^tΩt​=Ω1t​ holds the first ttt coordinates. Information at time ttt is the universal completion Ft\mathcal F_tFt​ of the Borel σ\sigmaσ-field of Ωt\Omega_tΩt​.

For each t<Tt<Tt<T and history ω∈Ωt\omega\in\Omega_tω∈Ωt​, a nonempty convex set Pt(ω)\mathcal P_t(\omega)Pt​(ω) of probability measures on Ω1\Omega_1Ω1​ describes the possible laws of the next coordinate. Its graph must be an analytic set. The set of models P\mathcal PP consists of all products P=P0⊗P1⊗⋯⊗PT−1P=P_0\otimes P_1\otimes\cdots\otimes P_{T-1}P=P0​⊗P1​⊗⋯⊗PT−1​ whose kernels choose Pt(ω)∈Pt(ω)P_t(\omega)\in\mathcal P_t(\omega)Pt​(ω)∈Pt​(ω). A property holds P\mathcal PP-quasi surely (q.s.) if it holds PPP-a.s. for every P∈PP\in\mathcal PP∈P.

There are ddd stocks with Borel prices St:Ωt→RdS_t:\Omega_t\to\mathbb R^dSt​:Ωt​→Rd and eee options g=(g1,…,ge)g=(g^1,\dots,g^e)g=(g1,…,ge), Borel on Ω\OmegaΩ, bought or sold at time 000 at price 000. A semistatic strategy (H,h)(H,h)(H,h) consists of a predictable HHH and a vector h∈Reh\in\mathbb R^eh∈Re; its terminal gain is

H∙ST+hg=∑u=1THu (Su−Su−1)+∑i=1ehigi.H\bullet S_T+hg=\sum_{u=1}^T H_u\,(S_u-S_{u-1})+\sum_{i=1}^e h^ig^i .H∙ST​+hg=u=1∑T​Hu​(Su​−Su−1​)+i=1∑e​higi.

No-arbitrage NA(P\mathcal PP) says that a gain which is q.s. nonnegative is q.s. zero. The superhedging price of a claim fff is

π(f)=inf⁡{x∈R: ∃(H,h), x+H∙ST+hg≥f  P-q.s.}.\pi(f)=\inf\{x\in\mathbb R:\ \exists (H,h),\ x+H\bullet S_T+hg\ge f\ \ \mathcal P\text{-q.s.}\}.π(f)=inf{x∈R: ∃(H,h), x+H∙ST​+hg≥f  P-q.s.}.

The dual objects are the martingale measures Q⋘PQ\lll\mathcal PQ⋘P, meaning Q≪PQ\ll PQ≪P for some P∈PP\in\mathcal PP∈P. Under QQQ the stock SSS is a martingale and EQ[gi]=0E_Q[g^i]=0EQ​[gi]=0 for all iii; they form the set Q\mathcal QQ. Given a weight φ≥1\varphi\ge1φ≥1, set Qφ={Q∈Q:EQ[φ]<∞}\mathcal Q_\varphi=\{Q\in\mathcal Q: E_Q[\varphi]<\infty\}Qφ​={Q∈Q:EQ​[φ]<∞}. Expectations of arbitrary measurable functions use the convention E[f]=E[f+]−E[f−]E[f]=E[f^+]-E[f^-]E[f]=E[f+]−E[f−] with ∞−∞=−∞\infty-\infty=-\infty∞−∞=−∞.

Formalization targets

Goal: Theorem 5.1(b)

Let φ≥1\varphi\ge1φ≥1 be a random variable with ∣gi∣≤φ|g^i|\le\varphi∣gi∣≤φ, let NA(P\mathcal PP) hold, and let fff be upper semianalytic with ∣f∣≤φ|f|\le\varphi∣f∣≤φ. Then

π(f)=sup⁡Q∈QφEQ[f]∈(−∞,∞],\pi(f)=\sup_{Q\in\mathcal Q_\varphi}E_Q[f]\in(-\infty,\infty],π(f)=Q∈Qφ​sup​EQ​[f]∈(−∞,∞],

and some (H,h)(H,h)(H,h) satisfies π(f)+H∙ST+hg≥f\pi(f)+H\bullet S_T+hg\ge fπ(f)+H∙ST​+hg≥f P\mathcal PP-q.s.

Milestones

The milestones follow the paper's proof:

  1. General setting (§2). Closedness of the superhedgeable cone under q.s. convergence (Theorem 2.2), and existence of optimal strategies (Theorem 2.3).
  2. One-period market (§3). The fundamental lemma (Lemma 3.3), the one-period FTAP (Theorem 3.1), approximation lemmas (Lemmas 3.5, 3.6) and one-period duality (Theorem 3.4).
  3. Expectation bound (Lemma A.2). The elementary bound EQ[f]≤xE_Q[f]\le xEQ​[f]≤x for a superhedge under a consistent local martingale measure.
  4. Multi-period market without options (§4). Local characterization of NA (Lemma 4.6, Theorem 4.5), measurable one-step duality (Lemma 4.10), dynamic superhedging (Lemma 4.13) and duality (Theorem 4.9).
  5. With options (§5). The first and second fundamental theorems (Theorem 5.1(a), (c)).

Significance

The superhedging theorem identifies the robust price of a claim as a supremum of linear prices. This turns a hedging problem into an optimization over measures, which is how robust option bounds are computed in practice. Remark 1.4 of the paper gives another consequence: every martingale inequality E[f(M1,…,MT)]≤aE[f(M_1,\dots,M_T)]\le aE[f(M1​,…,MT​)]≤a follows from a pathwise inequality f≤a+H∙STf\le a+H\bullet S_Tf≤a+H∙ST​. The first and second fundamental theorems make the nondominated framework a complete analogue of the classical theory. NA(P\mathcal PP) is equivalent to P\mathcal PP and Q\mathcal QQ sharing their polar sets, and replicable claims are those whose price is the same under every martingale measure.

All results are proved in the paper. None of them, nor the classical dominated discrete-time FTAP, is formalized in Lean or Mathlib as far as is known. A formalization produces machine-checked statements of the model (analytic random sets, products of universally measurable kernels, quasi-sure analysis) and proofs of the fundamental theorems on top of it. Alternative arguments and extensions (portfolio constraints, infinitely many options) are also welcome.

Difficulty

There is no reference measure. Two dominated tools therefore fail. Closedness in L0(P)L^0(P)L0(P) cannot be applied, because convergence must hold quasi surely. A Hahn–Banach separation in a single Lp(P)L^p(P)Lp(P) space cannot produce martingale measures either. The paper argues one period at a time instead and glues the periods together measurably. That gluing is where the work lies. The one-period dual value Et(f)(ω)\mathcal E_t(f)(\omega)Et​(f)(ω) and the one-period hedge y(ω)y(\omega)y(ω) must depend measurably on the history ω\omegaω, but the value function of a Borel claim need not be Borel. The argument therefore runs in the class of upper semianalytic functions and needs measurable selection theorems for analytic sets. A recursion that tries to keep everything Borel breaks down at the first step.

Formalization scope

  • Spaces. Ωt\Omega_tΩt​ is Fin t → Ω₁ with [PolishSpace Ω₁] [BorelSpace Ω₁]. Measures are Borel measures, and Ft\mathcal F_tFt​-measurability is universal measurability. The published definition BertsekasShreve.AnalyticSelection.Measurability is reused for this.
  • Models. P(Ω1)\mathfrak P(\Omega_1)P(Ω1​) is Mathlib's ProbabilityMeasure with the weak topology. P\mathcal PP is generated by Borel Markov kernels lying in Pt(⋅)\mathcal P_t(\cdot)Pt​(⋅) almost surely; this is the paper's equivalent formulation on p. 4.
  • Strategies. Lean's H u is the paper's Hu+1H_{u+1}Hu+1​, a universally measurable function of the first uuu coordinates.
  • Values in EReal. Expectations of non-integrable functions are the extended expectation E[f+]−E[f−]E[f^+]-E[f^-]E[f+]−E[f−]. Prices are EReal infima with inf⁡∅=+∞\inf\emptyset=+\inftyinf∅=+∞, and suprema over Qφ\mathcal Q_\varphiQφ​ are EReal suprema.
  • Settings. The §2 and §3 milestones are stated in the paper's more general settings: a general filtered space, and a one-period market on an arbitrary measurable space.
  • Citations. Page numbers are those of the arXiv v3 reprint (arXiv:1305.6008v3), not the journal's pp. 823–859.

Two encodings would trivialize the mission and are excluded. Replacing P\mathcal PP by an arbitrary set of measures drops the product structure that the theorems need. Bochner integrals for EQ[f]E_Q[f]EQ​[f] would return 000 on non-integrable claims and make the duality meaningless. Neither encoding is used.

A complete development needs:

  • analytic and universally measurable sets and the Jankov–von Neumann selection theorem;
  • products of universally measurable kernels;
  • quasi-sure analysis;
  • relative interiors and separation in Rd\mathbb R^dRd;
  • discrete-time local and generalized martingales.

The selection and kernel infrastructure is reusable well beyond this paper, for instance in dynamic programming on Borel spaces. Contributions of these foundations are welcome.

Selected references

  • B. Bouchard, M. Nutz, Arbitrage and duality in nondominated discrete-time models, Ann. Appl. Probab. 25(2) (2015) 823–859. https://arxiv.org/abs/1305.6008 , https://doi.org/10.1214/14-AAP1011
  • R. C. Dalang, A. Morton, W. Willinger, Equivalent martingale measures and no-arbitrage in stochastic securities market models, Stochastics Stochastics Rep. 29 (1990) 185–201. https://mathscinet.ams.org/mathscinet-getitem?mr=1041035
  • B. Acciaio, M. Beiglböck, F. Penkner, W. Schachermayer, A model-free version of the fundamental theorem of asset pricing and the super-replication theorem, Math. Finance 26(2) (2016) 233–251. https://arxiv.org/abs/1301.5568
  • M. Beiglböck, P. Henry-Labordère, F. Penkner, Model-independent bounds for option prices — a mass transport approach, Finance Stoch. 17(3) (2013) 477–501. https://arxiv.org/abs/1106.5929
  • L. Denis, C. Martini, A theoretical framework for the pricing of contingent claims in the presence of model uncertainty, Ann. Appl. Probab. 16 (2006) 827–852. https://mathscinet.ams.org/mathscinet-getitem?mr=2244434
  • Y. Kabanov, C. Stricker, A teachers' note on no-arbitrage criteria, Séminaire de Probabilités XXXV, Lecture Notes in Math. 1755 (2001) 149–152. https://mathscinet.ams.org/mathscinet-getitem?mr=1837282
  • D. P. Bertsekas, S. E. Shreve, Stochastic Optimal Control: The Discrete-Time Case, Academic Press, 1978 (Chapter 7, analytic sets and measurable selection).
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Actuarial Mathematics XXIII: Countable-Lifetime Hattendorff LimitTextbook

Actuarial Mathematics XXIII: Countable-Lifetime Hattendorff Limit

Mathematical source and original extension

Elias S. W. Shiu and Xiaoyi Xiong (2021), An elementary derivation of Hattendorff's theorem, European Actuarial Journal 11, 319–323, https://doi.org/10.1007/s13385-020-00256-9. In that paper equation (1) defines the fully discrete insurer's complete-life loss; equation (2) gives the Hattendorff variance formula, and equations (3)–(5) connect annual reserve recursion to the net amount at risk by summation by parts.

The present mission proposes an original countable-outcome and L²-convergence formalisation of that discrete formula. It is not asserted that the authors stated this exact Lean theorem, and it does not inherit proofs from the earlier finite-scenario missions.

Unbounded lifetime and conditional mortality

Let K∈NK\in\mathbb NK∈N be the realised curtate lifetime, the number of full years remaining until the year of death. Its possible values are not uniformly bounded. Set wk=Pr⁡(K=k)w_k=\Pr(K=k)wk​=Pr(K=k), where wk≥0w_k\ge0wk​≥0 and ∑k=0∞wk=1\sum_{k=0}^{\infty}w_k=1∑k=0∞​wk​=1. Assume the survival tail is positive in every year:

St=∑k≥twk>0,qt=wtSt,pt=St+1St=1−qt.S_t=\sum_{k\ge t}w_k>0,\qquad q_t=\frac{w_t}{S_t},\qquad p_t=\frac{S_{t+1}}{S_t}=1-q_t.St​=k≥t∑​wk​>0,qt​=St​wt​​,pt​=St​St+1​​=1−qt​.

These are unconditional death masses wtw_twt​ and conditional mortality and survival rates qt,ptq_t,p_tqt​,pt​. Some individual wtw_twt​ may be zero. The outcome space is genuinely countable; a finite Fintype of realised death years would force a bounded support and undermine the claimed infinite-horizon extension.

Mortality surprises and reserve losses

The annual mortality martingale difference is defined pathwise by

It(k)=1{k=t}−qt1{k≥t}.I_t(k)=\mathbf1_{\{k=t\}}-q_t\mathbf1_{\{k\ge t\}}.It​(k)=1{k=t}​−qt​1{k≥t}​.

For t<kt<kt<k, It(k)=−qtI_t(k)=-q_tIt​(k)=−qt​; at death t=kt=kt=k, It(k)=1−qtI_t(k)=1-q_tIt​(k)=1−qt​; and after death t>kt>kt>k, it is zero. Let the discounted net amount at risk for the payment at year-end t+1t+1t+1 be ρt=vt+1(bt+1−Vt+1)\rho_t=v^{t+1}(b_{t+1}-V_{t+1})ρt​=vt+1(bt+1​−Vt+1​). This matches Shiu–Xiong's year-end death-benefit timing. The truncated centred reserve loss and the pathwise complete-life centred loss are

Zn(k)=∑t=0n−1ρtIt(k),Z∞(k)=Zk+1(k).Z_n(k)=\sum_{t=0}^{n-1}\rho_tI_t(k),\qquad Z_\infty(k)=Z_{k+1}(k).Zn​(k)=t=0∑n−1​ρt​It​(k),Z∞​(k)=Zk+1​(k).

The complete-life variable is well-defined on each realised finite kkk and Zn(k)=Z∞(k)Z_n(k)=Z_\infty(k)Zn​(k)=Z∞​(k) whenever n>kn>kn>k. These definitions only model the centred innovation component. A separate cashflow reserve-recursion bridge, as in earlier missions, is needed to identify a given insurer contract loss LLL with V0+Z∞V_0+Z_\inftyV0​+Z∞​; this mission does not silently assert that for arbitrary premium sequences.

Supporting results and convergence condition

The discrete expectations are weighted countable sums. Show, under summability and positive in-force mass,

E[It]=0,E[IiIj]=0  (i≠j),E[It2]=wtpt.\mathbb E[I_t]=0,\quad \mathbb E[I_i I_j]=0\;(i\ne j),\quad \mathbb E[I_t^2]=w_tp_t.E[It​]=0,E[Ii​Ij​]=0(i=j),E[It2​]=wt​pt​.

Using finite sums and cross-year orthogonality first gives

E[Zn2]=∑t=0n−1ρt2wtpt.\mathbb E[Z_n^2]=\sum_{t=0}^{n-1}\rho_t^2w_tp_t.E[Zn2​]=t=0∑n−1​ρt2​wt​pt​.

The capstone introduces the mathematically substantive L² risk condition

∑t=0∞ρt2wtpt<∞.\sum_{t=0}^{\infty}\rho_t^2w_tp_t<\infty.t=0∑∞​ρt2​wt​pt​<∞.

This implies that the sequence of truncated centred losses is Cauchy in the probability-weighted L² space; its limit equals the pathwise stabilised Z∞Z_\inftyZ∞​. Hence

E[Z∞]=0,Var⁡(Z∞)=E[Z∞2]=∑t=0∞ρt2wtpt.\boxed{\mathbb E[Z_\infty]=0,\qquad \operatorname{Var}(Z_\infty)=\mathbb E[Z_\infty^2] =\sum_{t=0}^{\infty}\rho_t^2w_tp_t.}E[Z∞​]=0,Var(Z∞​)=E[Z∞2​]=t=0∑∞​ρt2​wt​pt​.​

The capstone explicitly assumes nonnegative weights, unit total mass, positive survival tails, countable weight summability and risk-variance summability. The formal statement must not be weakened to merely a pointwise convergence or an unjustified interchange of infinite sums.

Exact-rational validation and boundaries

A geometric law with q=14q=\frac14q=41​, p=34p=\frac34p=43​, wk=qpkw_k=qp^kwk​=qpk and ρt=2\rho_t=2ρt​=2 gives

Z∞(k)=2(p−qk),E[Z∞]=0,Var⁡(Z∞)=3.Z_\infty(k)=2(p-qk),\qquad \mathbb E[Z_\infty]=0,\quad\operatorname{Var}(Z_\infty)=3.Z∞​(k)=2(p−qk),E[Z∞​]=0,Var(Z∞​)=3.

Its finite-year variance is 3(1−pn)3(1-p^n)3(1−pn). The repository includes exact-rational tests for 13 horizons. The model allows an individually zero death mass but requires positive tails. Every scenario terminates in some finite year; adding a K=∞K=\inftyK=∞ outcome with positive weight would require a separate transversality condition and is not part of this mission.

Prove2Me proof structure

The mission supplies four mathematical definitions, eleven supporting milestone theorems and one combined capstone theorem. Prove the indicator identities, the countable weighted first and second moments, finite orthogonality and finite allocation, and finally the L² passage to the unbounded lifetime. The target Lean namespace is `ActuarialValuation` in the pinned Mathlib environment. Finite-year results from earlier actuarial missions are background, not automatic countable-measure proof imports. None of the present open theorem statements is an accepted proof.

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Actuarial ScienceProbability·Captain: WillR

Actuarial Mathematics XVI: Discrete Mortality Innovations and Hattendorff OrthogonalityTextbook

Motivation: from actuarial reserves to Hattendorff's theorem

A prospective insurance reserve is the conditional expected amount needed to fund the remaining liabilities of an in-force policy. Annual realised claims differ from their conditional expectations, and the variation in total discounted insurer loss can be allocated to these unexpected annual outcomes. Hattendorff's theorem expresses that allocation as a sum of year-specific variance contributions. The fully discrete case contains an important factor: the conditional probability of surviving the policy year.

Shiu and Xiong's article An elementary derivation of Hattendorff's theorem [1] gives a direct discrete derivation. With curtate lifetime KKK, annual death benefits bj+1b_{j+1}bj+1​ paid at time j+1j+1j+1, premiums πj\pi_jπj​ paid at time jjj, discount factor vvv and prospective reserve Vj+1V_{j+1}Vj+1​, their formulas include

L=vK+1bK+1−∑j=0Kvjπjandρj=vj+1(bj+1−Vj+1).L=v^{K+1}b_{K+1}-\sum_{j=0}^{K}v^j\pi_j \qquad\text{and}\qquad \rho_j=v^{j+1}(b_{j+1}-V_{j+1}).L=vK+1bK+1​−j=0∑K​vjπj​andρj​=vj+1(bj+1​−Vj+1​).

In particular, the variance identity they derive has a mortality-year survival factor,

Var⁡(L)=E ⁣[ρK2px+K].\operatorname{Var}(L)=\mathbb E\!\left[\rho_K^2p_{x+K}\right].Var(L)=E[ρK2​px+K​].

This mission establishes the finite-scenario mortality-innovation component of that result. It derives the orthogonality of annual death surprises rather than assuming it. It does not yet identify their weighted sum with the full insurance loss L−V0L-V_0L−V0​; that requires the separate time-dependent reserve recursion and summation-by-parts identities in [1, equation (3)]. Those insurance cashflow bridge obligations are explicitly reserved for the next mathematical stage.

Finite lifetime model

Let Ω\OmegaΩ be a finite scenario space, wω≥0w_\omega\ge0wω​≥0 its weights and K:Ω→NK:\Omega\to\mathbb NK:Ω→N a curtate future lifetime, where K=jK=jK=j means death during year jjj, at the end of which the death benefit is payable.

For policy duration ttt, define the in-force probability mass and the death-year mass:

St=∑ω∈Ωwω1{K(ω)≥t},Dt=∑ω∈Ωwω1{K(ω)=t}.S_t=\sum_{\omega\in\Omega}w_\omega\mathbf1_{\{K(\omega)\ge t\}}, \qquad D_t=\sum_{\omega\in\Omega}w_\omega\mathbf1_{\{K(\omega)=t\}}.St​=ω∈Ω∑​wω​1{K(ω)≥t}​,Dt​=ω∈Ω∑​wω​1{K(ω)=t}​.

For probabilistic interpretation assume in addition ∑ωwω=1\sum_\omega w_\omega=1∑ω​wω​=1. The exact algebraic statements do not generally require weight normalisation, though they explicitly require nonnegative weights for probability inequalities.

The disjoint identity

{K≥t}={K=t}∪˙{K≥t+1}\{K\ge t\}=\{K=t\}\mathbin{\dot\cup}\{K\ge t+1\}{K≥t}={K=t}∪˙{K≥t+1}

gives St=Dt+St+1S_t=D_t+S_{t+1}St​=Dt​+St+1​. If St>0S_t>0St​>0, the conditional one-year death and survival probabilities are

qt=DtSt,pt=St+1St,qt+pt=1.q_t=\frac{D_t}{S_t},\qquad p_t=\frac{S_{t+1}}{S_t},\qquad q_t+p_t=1.qt​=St​Dt​​,pt​=St​St+1​​,qt​+pt​=1.

Division by St=0S_t=0St​=0 is totalised as a Lean real expression but is not interpreted as conditioning on an impossible event. All substantive annual-innovation results impose positive in-force mass for the years used.

A centred innovation for every policy year

For each outcome and policy year define the mortality innovation

It(ω)=1{K(ω)=t}−qt1{K(ω)≥t}.I_t(\omega)= \mathbf1_{\{K(\omega)=t\}} -q_t\mathbf1_{\{K(\omega)\ge t\}}.It​(ω)=1{K(ω)=t}​−qt​1{K(ω)≥t}​.

It equals 1−qt1-q_t1−qt​ for death in year ttt, equals −qt-q_t−qt​ for an individual surviving that year, and equals zero after death. Under St>0S_t>0St​>0,

Ew[It]=Dt−qtSt=0.\mathbb E_w[I_t]=D_t-q_tS_t=0.Ew​[It​]=Dt​−qt​St​=0.

The orthogonality is more than a generic assumption. For i<ji<ji<j, if Ij≠0I_j\ne0Ij​=0 then the policy is still in force at jjj, so the preceding year iii must have been survived and Ii=−qiI_i=-q_iIi​=−qi​. If Ij=0I_j=0Ij​=0, the product is also zero. Thus, pointwise,

IiIj=−qiIj,i<j.I_iI_j=-q_iI_j,\qquad i<j.Ii​Ij​=−qi​Ij​,i<j.

Taking the weighted expectation and using the centring of IjI_jIj​ gives

Ew[IiIj]=0,i<j,Sj>0.\mathbb E_w[I_iI_j]=0,\qquad i<j,\quad S_j>0.Ew​[Ii​Ij​]=0,i<j,Sj​>0.

These innovations can be uncorrelated despite being highly dependent events generated by the same curtate lifetime. They must not be claimed independent.

The one-year discrete second moment

By conditioning on the death-year and survival outcomes, the squared mortality surprise has expected value

Ew[It2]=Dt(1−qt)2+St+1qt2=Dt pt,St>0.\begin{aligned} \mathbb E_w[I_t^2] &=D_t(1-q_t)^2+S_{t+1}q_t^2\\ &=D_t\,p_t,\qquad S_t>0. \end{aligned}Ew​[It2​]​=Dt​(1−qt​)2+St+1​qt2​=Dt​pt​,St​>0.​

The final conditional survival factor ptp_tpt​ is characteristic of the fully discrete actuarial Hattendorff identity. It is not an arbitrary variance weight, and it cannot be dropped by borrowing a continuous-time formula.

For a finite horizon nnn, let ρt∈R\rho_t\in\mathbb Rρt​∈R be any deterministic year-specific net-amount-at-risk coefficient. Define the discounted innovation portfolio

Zn(ω)=∑0≤t<nρtIt(ω).Z_n(\omega)=\sum_{0\le t<n}\rho_t I_t(\omega).Zn​(ω)=0≤t<n∑​ρt​It​(ω).

When St>0S_t>0St​>0 for each t<nt<nt<n, the annual zero-mean and cross-year orthogonality identities yield

Ew[Zn]=0,Var⁡w(Zn)=∑0≤t<nρt2Dtpt.\boxed{ \mathbb E_w[Z_n]=0,\qquad \operatorname{Var}_w(Z_n)= \sum_{0\le t<n}\rho_t^2D_tp_t. }Ew​[Zn​]=0,Varw​(Zn​)=0≤t<n∑​ρt2​Dt​pt​.​

For nonnegative unit-sum weights this is the usual finite-scenario variance. The capstone couples the derived pairwise cross-year zero moments with the resulting finite-horizon variance formula. No reserve balance, actuarial premium equation or conditional L² filtration theorem is silently assumed.

Formal proof structure and scope

The formal graph contains seven definitions: survival and death masses, conditional death and survival rates, the mortality innovation, its finite discounted portfolio and a finite weighted variance. Supporting theorems establish event partitions, nonnegativity, qt+pt=1q_t+p_t=1qt​+pt​=1, behaviour after death, innovation centring, a pointwise earlier/later product identity, orthogonality, the discrete second-moment formula, zero horizon and portfolio moments. The capstone packages zero covariance and the mortality-weighted variance allocation.

The variance theorem is valid for arbitrary deterministic coefficient sequence ρ\rhoρ and any finite number of years with positive survival mass; it does not presume every life dies before that horizon. n=0n=0n=0 is covered by the empty sum. For standard actuarial application choose ρt=vt+1(bt+1−Vt+1)\rho_t=v^{t+1}(b_{t+1}-V_{t+1})ρt​=vt+1(bt+1​−Vt+1​), as in [1]. A future bridge must show that this particular innovation portfolio equals the centred insurer loss under the correct reserve recursion and endpoint conventions.

The root theorem is therefore a genuine probabilistic predecessor, not an assertion that the entire traditional Hattendorff theorem has already been proved. The mission is proposed for formal proof: private remote statement elaboration and finite rational tests, if accepted, do not constitute public Prove2Me proof acceptance.

References

[1] Shiu, Elias S. W. and Xiong, Xiaoyi (2021), “An elementary derivation of Hattendorff's theorem”, European Actuarial Journal, 11, pp. 319–323, equations (1)–(3). This is the direct source for the fully discrete variance factor, net amount at risk and finite summation-by-parts strategy.

[2] Gerber, Hans U. (1997), Life Insurance Mathematics, third edition, Springer, Chapter 6, §6.7, Allocation of the Overall Loss to Policy Years. The reserve-change and annual-loss decomposition provides broader actuarial context.

[3] Gerber, Hans U., Leung, Bartholomew P. K. and Shiu, Elias S. W. (2003), “Indicator Function and Hattendorff Theorem”, North American Actuarial Journal, 7(1), pp. 38–47. Explains the central role of indicator functions and the relationship to uncorrelated martingale increments.

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Actuarial ScienceProbability·Captain: WillR

Actuarial Mathematics XVII: Finite-Horizon Markov Decision and Optimal Policy ValuationTextbook

Motivation: from one-step reinsurance decisions to an optimal policy

An insurer may adjust its reinsurance retention or other risk-management decision repeatedly, rather than optimising a single future year's payments. Current action choices affect both the immediate net reward and the state of the business next year, which changes the value of all later decisions. A finite-horizon Markov decision process makes this multi-year optimisation precise.

Puterman, Markov Decision Processes: Discrete Stochastic Dynamic Programming, Chapter 4 [1], develops the finite-horizon Bellman equations and existence of optimal deterministic Markov policies for finite decision problems. Mission XV introduces a finite-action Bellman operator and excess-of-loss claim splitting, but is still under moderator review. This mission formalises the full finite-horizon backward recursion and optimal deterministic policy existence, without importing an unreviewed declaration.

The reinsurance motivation comes from Brachetta and Ceci's optimal excess-of-loss study [2]. Their original problem is a continuous-time stochastic-factor and HJB verification problem. The present mission is strictly a finite-state, finite-action, discrete-time precursor. Neither the stochastic-factor diffusion nor the jump-process verification theorem is asserted here.

Finite states, actions and one-year valuation

Let SSS be a finite state type, and let AAA be a finite nonempty set of admissible control actions. A state can encode a simplified surplus, rating, claims regime or any finite risk-class abstraction. At the beginning of a policy year the insurer is in state sss and selects an action aaa.

Let P(s,a,t)P(s,a,t)P(s,a,t) be the transition weight for next state ttt, and r(s,a)r(s,a)r(s,a) the immediate reward. The usual Markov model requires P(s,a,t)≥0P(s,a,t)\ge0P(s,a,t)≥0 and ∑tP(s,a,t)=1\sum_tP(s,a,t)=1∑t​P(s,a,t)=1 for every s,as,as,a. The general algebraic definitions accept real matrices, while the economic probabilistic interpretation requires valid row-stochasticity.

If U(t)U(t)U(t) is the continuation value in state ttt, the return from action aaa is

Q(s,a;U)=r(s,a)+v∑t∈SP(s,a,t)U(t),Q(s,a;U)=r(s,a)+v\sum_{t\in S}P(s,a,t)U(t),Q(s,a;U)=r(s,a)+vt∈S∑​P(s,a,t)U(t),

where vvv is a deterministic annual discount factor. The discount is applied to following-year continuation, not to the current reward. For policy interpretation 0≤v≤10\le v\le10≤v≤1 is conventional, but finite-horizon algebra makes sense at other fixed real vvv as well.

The one-year Bellman optimisation is

(TU)(s)=max⁡a∈AQ(s,a;U).(TU)(s)=\max_{a\in A}Q(s,a;U).(TU)(s)=a∈Amax​Q(s,a;U).

The maximum is attained because AAA is finite and nonempty. Both this attainment and the inequality Q(s,a;U)≤(TU)(s)Q(s,a;U)\le(TU)(s)Q(s,a;U)≤(TU)(s) are explicit supporting theorem obligations.

Finite-horizon policy evaluation

Let h(s)h(s)h(s) denote a terminal benefit or terminal value. A deterministic nonstationary Markov policy is a mapping

π:N×S⟶A.\pi:\mathbb N\times S\longrightarrow A.π:N×S⟶A.

Here πn(s)\pi_n(s)πn​(s) is the action chosen when n+1n+1n+1 decisions remain, so the index counts backwards towards the terminal time. This makes the recursion valid for a homogeneous one-step transition model without reversing calendar-time transitions.

For a fixed policy, recursively define

V0π(s)=h(s),Vn+1π(s)=r(s,πn(s))+v∑t∈SP(s,πn(s),t)Vnπ(t).\begin{aligned} V^\pi_0(s)&=h(s),\\ V^\pi_{n+1}(s) &=r(s,\pi_n(s)) +v\sum_{t\in S}P(s,\pi_n(s),t)V^\pi_n(t). \end{aligned}V0π​(s)Vn+1π​(s)​=h(s),=r(s,πn​(s))+vt∈S∑​P(s,πn​(s),t)Vnπ​(t).​

The policy is nonstationary because its choice at the same state may differ according to remaining time nnn. It is Markov because the action depends only on current state and remaining horizon, not on the entire historical path. The mission does not introduce a path-space filtration or general history-dependent randomised policy, so the precise capstone compares deterministic nonstationary Markov policies.

Optimal backward induction

Define Vn(s)V_n(s)Vn​(s) by the finite Bellman recursion

V0(s)=h(s),Vn+1(s)=max⁡a∈A[r(s,a)+v∑t∈SP(s,a,t)Vn(t)].\begin{aligned} V_0(s)&=h(s),\\ V_{n+1}(s)&= \max_{a\in A}\left[ r(s,a)+v\sum_{t\in S}P(s,a,t)V_n(t) \right]. \end{aligned}V0​(s)Vn+1​(s)​=h(s),=a∈Amax​[r(s,a)+vt∈S∑​P(s,a,t)Vn​(t)].​

Under P(s,a,t)≥0P(s,a,t)\ge0P(s,a,t)≥0 and v≥0v\ge0v≥0, a larger continuation function cannot reduce the value of any action; taking a finite maximum preserves this monotonicity. That simple inequality allows induction on the remaining horizon to show

Vnπ(s)≤Vn(s)for every deterministic Markov policy π.V^\pi_n(s)\le V_n(s) \qquad\text{for every deterministic Markov policy }\pi.Vnπ​(s)≤Vn​(s)for every deterministic Markov policy π.

The second substantive step is existence of an attaining policy. Since AAA is finite and nonempty, at each remaining horizon and each state there is at least one maximising action. Choosing such actions and combining them recursively gives a single nonstationary deterministic Markov policy π⋆\pi^\starπ⋆ satisfying

Vnπ⋆(s)=Vn(s)for all states s.V^{\pi^\star}_n(s)=V_n(s) \qquad\text{for all states }s.Vnπ⋆​(s)=Vn​(s)for all states s.

The capstone combines the universal upper bound and existence of an attaining policy. This is genuinely more than a one-step maximum: it is an optimality result over an arbitrary finite number of sequential decisions.

A complete optimality result against all history-dependent randomised policies would need an additional equivalence argument showing no improvement from extra history or randomisation. Such an extension is well-known for suitable finite Markov models but is not silently claimed by this narrower Lean target.

Formal graph and limiting cases

Four proposed definitions encode the one-step action return, the finite Bellman maximum, policy evaluation and recursively optimal horizon value. Eleven supporting theorem targets establish zero-discount behaviour, action domination and attainment, monotonicity of action and Bellman values, zero-horizon and successor recursions, policy domination and existence of an attaining policy. The capstone packages the latter two results.

At n=0n=0n=0 there are no decisions and both values are precisely hhh. At v=0v=0v=0, any continuation is irrelevant to the one-step value. Nonnegative weights and discount are explicit hypotheses for monotonicity and policy domination, rather than false claims for signed matrix weights. The existence of an attaining maximiser in each finite action set does not itself require stochastic row-sum assumptions.

To obtain a reinsurance model from this graph, one must specify how each action corresponds to an admissible retention, how the retention changes reinsurance premiums and retained claim distributions, and how those assumptions determine the transition matrix PPP and rewards rrr. That specialised bridge is separate from the finite-horizon mathematical result.

All theorems are proposed Lean proof targets. Preliminary remote elaboration establishes statement well-formedness only if verified by the authoritative compiler. It does not constitute a completed proof or approval of the mission's mathematical design.

References

[1] Puterman, Martin L. (1994), Markov Decision Processes: Discrete Stochastic Dynamic Programming, Chapter 4, Finite-Horizon Markov Decision Processes, Wiley. This is the direct mathematical reference for finite-horizon Bellman recursions, backward induction and existence of optimal deterministic policies under finite-state/action assumptions.

[2] Brachetta, Matteo and Ceci, Claudia (2019), “Optimal Excess-of-Loss Reinsurance for Stochastic Factor Risk Models”, Risks 7(2), article 48. This motivates insurance retention as a controlled decision but uses a continuous-time stochastic-factor/HJB model not established by this mission.

[3] Schäffeler, Maximilian and Abdulaziz, Mohammad (2022), “Formally Verified Solution Methods for Markov Decision Processes”, computer-assisted formalisation of Bellman equations, value iteration and optimal policy existence in Isabelle/HOL. This is methodology context only; no proof code is imported into Lean from that project.

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Gaussian Random Matrices III: Extreme Singular Values and ConcentrationTextbook

Motivation

A tall N×nN\times nN×n matrix with independent standard normal entries is, with high probability, a near-isometry: all its singular values lie in [N−n, N+n][\sqrt N-\sqrt n,\ \sqrt N+\sqrt n][N​−n​, N​+n​] up to Gaussian fluctuations. This is Gordon's theorem together with Gaussian concentration (Vershynin 2012, Theorem 5.32 and Corollary 5.35), the non-asymptotic counterpart of the Bai–Yin law and the model result for the whole theory of non-asymptotic random matrices. In randomized numerical linear algebra the same two ingredients give the expected spectral norm of SΓTS\Gamma TSΓT (Halko–Martinsson–Tropp 2011, Proposition 10.1 (10.2)), its second moment (Tropp–Webber 2023, Lemma B.1), and the lower tail of σmin⁡\sigma_{\min}σmin​ of a Gaussian sketch, which controls the inverse moments E σmin⁡−2p\mathbb E\,\sigma_{\min}^{-2p}Eσmin−2p​ that appear in the analysis of sketching algorithms with rank truncation. None of these results is available in Mathlib; this mission proves them.

Setting

A standard Gaussian matrix A∈RN×nA\in\mathbb R^{N\times n}A∈RN×n has independent N(0,1)\mathcal N(0,1)N(0,1) entries; its law is γN,n\gamma_{N,n}γN,n​. Its extreme singular values are

smin⁡(A)=inf⁡∥x∥2=1∥Ax∥2,smax⁡(A)=sup⁡∥x∥2=1∥Ax∥2=∥A∥,s_{\min}(A)=\inf_{\|x\|_2=1}\|Ax\|_2,\qquad s_{\max}(A)=\sup_{\|x\|_2=1}\|Ax\|_2=\|A\|,smin​(A)=∥x∥2​=1inf​∥Ax∥2​,smax​(A)=∥x∥2​=1sup​∥Ax∥2​=∥A∥,

the infimum and supremum over the unit sphere of Rn\mathbb R^nRn (n≥1n\ge1n≥1); ∥A∥\|A\|∥A∥ is the spectral norm. For a wide matrix G∈Rk×tG\in\mathbb R^{k\times t}G∈Rk×t, k≤tk\le tk≤t, the usual σmin⁡(G)\sigma_{\min}(G)σmin​(G) is smin⁡(GT)s_{\min}(G^{\mathsf T})smin​(GT). The Frobenius norm is ∥A∥F=(∑i,jAij2)1/2\|A\|_F=(\sum_{i,j}A_{ij}^2)^{1/2}∥A∥F​=(∑i,j​Aij2​)1/2; a function hhh on matrices is LLL-Lipschitz if ∣h(X)−h(Y)∣≤L∥X−Y∥F|h(X)-h(Y)|\le L\|X-Y\|_F∣h(X)−h(Y)∣≤L∥X−Y∥F​. A chi-square variable with ddd degrees of freedom is χd2=∑i=1dgi2\chi_d^2=\sum_{i=1}^d g_i^2χd2​=∑i=1d​gi2​ for independent standard normals gig_igi​. The letter eee denotes Euler's number.

Formalization targets

Goal — deviation of the extreme singular values (Vershynin, Corollary 5.35)

For every t≥0t\ge0t≥0, with probability at least 1−2e−t2/21-2e^{-t^2/2}1−2e−t2/2,

N−n−t ≤ smin⁡(A)andsmax⁡(A) ≤ N+n+t.\sqrt N-\sqrt n-t\ \le\ s_{\min}(A)\qquad\text{and}\qquad s_{\max}(A)\ \le\ \sqrt N+\sqrt n+t .N​−n​−t ≤ smin​(A)andsmax​(A) ≤ N​+n​+t.

This is the goal because it is the statement users of Gaussian matrices quote: a quantitative near-isometry with explicit sub-Gaussian deviations. It follows from the expectation bounds (Gordon) and concentration, both of which are milestones.

Milestones

  • Gaussian concentration for Lipschitz functions of a Gaussian matrix: P{h(G)≥Eh(G)+Lt}≤e−t2/2\mathbb P\{h(G)\ge\mathbb E h(G)+Lt\}\le e^{-t^2/2}P{h(G)≥Eh(G)+Lt}≤e−t2/2 (HMT Proposition 10.3; Vershynin Proposition 5.34).
  • Gordon–Chevet bound. E∥SΓT∥≤∥S∥∥T∥F+∥S∥F∥T∥\mathbb E\|S\Gamma T\|\le\|S\|\|T\|_F+\|S\|_F\|T\|E∥SΓT∥≤∥S∥∥T∥F​+∥S∥F​∥T∥ (HMT Proposition 10.1 (10.2), A.2) and its second-moment form (E∥SΓT∥2)1/2≤∥S∥∥T∥F+∥S∥F∥T∥(\mathbb E\|S\Gamma T\|^2)^{1/2}\le\|S\|\|T\|_F+\|S\|_F\|T\|(E∥SΓT∥2)1/2≤∥S∥∥T∥F​+∥S∥F​∥T∥ (Tropp–Webber Lemma B.1).
  • Gordon's theorem. N−n≤Esmin⁡(A)≤Esmax⁡(A)≤N+n\sqrt N-\sqrt n\le\mathbb E s_{\min}(A)\le\mathbb E s_{\max}(A)\le\sqrt N+\sqrt nN​−n​≤Esmin​(A)≤Esmax​(A)≤N​+n​ (Vershynin Theorem 5.32).
  • One-sided tail of smin⁡s_{\min}smin​. P{smin⁡(A)≤N−n−u}≤e−u2/2\mathbb P\{s_{\min}(A)\le\sqrt N-\sqrt n-u\}\le e^{-u^2/2}P{smin​(A)≤N​−n​−u}≤e−u2/2 for u≥0u\ge0u≥0 (Davidson–Szarek Theorem II.13; one-sided form of Vershynin Corollary 5.35).
  • Chi-square lower tail. P{χd2≤u}≤(eu/d)d/2\mathbb P\{\chi_d^2\le u\}\le(eu/d)^{d/2}P{χd2​≤u}≤(eu/d)d/2 for 0≤u≤d0\le u\le d0≤u≤d (Dasgupta–Gupta Lemma 2.2).
  • Small-ball bound for smin⁡s_{\min}smin​. P{smin⁡(A)≤s}≤n(e ns2N−n+1)(N−n+1)/2\mathbb P\{s_{\min}(A)\le s\}\le n\bigl(\frac{e\,ns^2}{N-n+1}\bigr)^{(N-n+1)/2}P{smin​(A)≤s}≤n(N−n+1ens2​)(N−n+1)/2 for s≥0s\ge0s≥0, ns2≤N−n+1ns^2\le N-n+1ns2≤N−n+1, from the invertibility-via-distance lemma of Rudelson–Vershynin (Lemma 3.5), rotational invariance and the chi-square lower tail.

Significance

The results. Gordon's theorem is sharp: Esmin⁡\mathbb E s_{\min}Esmin​ and Esmax⁡\mathbb E s_{\max}Esmax​ are pinned to within O(1)O(1)O(1) of the Bai–Yin limits for every N,nN,nN,n. Gaussian concentration upgrades it to tail bounds with the optimal sub-Gaussian rate, and the Chevet-type bound is the same mechanism for SΓTS\Gamma TSΓT, where it yields the expected spectral error of the randomized SVD. The small-ball bound covers the other regime, s→0s\to0s→0, with polynomial decay of the exact order N−n+1N-n+1N−n+1; together the two tails make every negative moment Esmin⁡(A)−2p\mathbb E s_{\min}(A)^{-2p}Esmin​(A)−2p, 2p<N−n+12p<N-n+12p<N−n+1, finite and explicitly bounded, which is what the early-truncated analysis needs.

Formalizing them. Mathlib has the standard Gaussian measure on finite-dimensional inner product spaces but neither Gaussian concentration for Lipschitz functions, nor Slepian's or Gordon's comparison inequalities, nor any result on singular values of random matrices. These are foundational pieces of high-dimensional probability whose formalization would be reused far beyond this series.

Difficulty

The upper bound in Gordon's theorem is proved by Slepian's comparison lemma for the Gaussian process (u,v)↦⟨Au,v⟩(u,v)\mapsto\langle Au,v\rangle(u,v)↦⟨Au,v⟩ on Sn−1×SN−1S^{n-1}\times S^{N-1}Sn−1×SN−1, and the lower bound by Gordon's minimax comparison inequality for max⁡vmin⁡u⟨Au,v⟩\max_v\min_u\langle Au,v\ranglemaxv​minu​⟨Au,v⟩; both require a theory of Gaussian processes indexed by continuous parameter sets, or at least a discretization argument with careful limits. Gaussian concentration (Tsirelson–Ibragimov–Sudakov) is usually proved through the Gaussian logarithmic Sobolev inequality or the Ornstein–Uhlenbeck semigroup, with a smoothing step to pass from smooth to Lipschitz functions. Both are long developments with no Mathlib support. The elementary alternatives do not reach the stated constants: an ε\varepsilonε-net argument bounds E∥A∥\mathbb E\|A\|E∥A∥ by C(N+n)C(\sqrt N+\sqrt n)C(N​+n​) with C>1C>1C>1, and a union bound over rows for the small-ball estimate is exactly how the stated bound is obtained, but it needs the fact that the distance from a Gaussian vector to a fixed (n−1)(n-1)(n−1)-dimensional subspace is a χN−n+1\chi_{N-n+1}χN−n+1​ variable, which again rests on rotational invariance.

Formalization scope

Matrices are sampled from the product measure γN,n\gamma_{N,n}γN,n​ on arrays. smin⁡s_{\min}smin​ is sMin, the real infimum over the unit sphere of Rn\mathbb R^nRn; n≥1n\ge1n≥1 is assumed so the sphere is nonempty, and N≥nN\ge nN≥n is not assumed for Gordon's theorem (for N<nN<nN<n one has smin⁡=0s_{\min}=0smin​=0 and the lower bound is trivial, as in the source). smax⁡s_{\max}smax​ is Mathlib's ℓ2\ell_2ℓ2​ operator norm. Expectation bounds are stated together with integrability of their integrands, so the Lean convention that non-integrable functions integrate to 000 cannot trivialize them. Probabilities are measures in [0,∞][0,\infty][0,∞] compared with ofReal⁡\operatorname{ofReal}ofReal of the real bound; the goal's lower bound 1−2e−t2/21-2e^{-t^2/2}1−2e−t2/2 uses truncated subtraction and is vacuous for t≤2log⁡2t\le\sqrt{2\log2}t≤2log2​, exactly as in the source. Gaussian concentration is stated with L>0L>0L>0 and t≥0t\ge0t≥0, which the sources leave implicit (for L=0L=0L=0 or t<0t<0t<0 the event has probability one). Results that the sketching literature states for wide k×tk\times tk×t matrices are stated here for tall N×nN\times nN×n matrices via σmin⁡(G)=smin⁡(GT)\sigma_{\min}(G)=s_{\min}(G^{\mathsf T})σmin​(G)=smin​(GT), with (N,n)=(t,k)(N,n)=(t,k)(N,n)=(t,k).

Welcome contributions: Gaussian concentration for Lipschitz functions on Rd\mathbb R^dRd (any proof), Slepian's and Gordon's inequalities, the 111-Lipschitz property of smin⁡s_{\min}smin​ and smax⁡s_{\max}smax​, the chi-square Chernoff bounds, and the law of the distance from a Gaussian vector to a subspace.

Selected references

  • N. Halko, P.-G. Martinsson, J. A. Tropp, Finding structure with randomness: probabilistic algorithms for constructing approximate matrix decompositions, SIAM Review 53(2), 217–288, 2011. https://arxiv.org/abs/0909.4061
  • J. A. Tropp, R. J. Webber, Randomized algorithms for low-rank matrix approximation: design, analysis, and applications, 2023. https://arxiv.org/abs/2306.12418
  • R. Vershynin, Introduction to the non-asymptotic analysis of random matrices, in Compressed Sensing: Theory and Applications, Cambridge University Press, 2012. https://arxiv.org/abs/1011.3027
  • L. Isserlis, On a formula for the product-moment coefficient of any order of a normal frequency distribution in any number of variables, Biometrika 12, 134–139, 1918. https://doi.org/10.1093/biomet/12.1-2.134
  • S. Dasgupta, A. Gupta, An elementary proof of a theorem of Johnson and Lindenstrauss, Random Structures & Algorithms 22, 60–65, 2003. https://doi.org/10.1002/rsa.10073
  • M. Rudelson, R. Vershynin, The Littlewood–Offord problem and invertibility of random matrices, Advances in Mathematics 218, 600–633, 2008. https://arxiv.org/abs/math/0703503
  • Y. Chen, J. Dongarra, Condition numbers of Gaussian random matrices, SIAM J. Matrix Anal. Appl. 27(3), 603–620, 2005. https://doi.org/10.1137/040616413
  • A. Edelman, Eigenvalues and condition numbers of random matrices, SIAM J. Matrix Anal. Appl. 9(4), 543–560, 1988. https://doi.org/10.1137/0609045
  • Y. Gordon, Some inequalities for Gaussian processes and applications, Israel J. Math. 50, 265–289, 1985. https://doi.org/10.1007/BF02759761
  • K. R. Davidson, S. J. Szarek, Local operator theory, random matrices and Banach spaces, Handbook of the Geometry of Banach Spaces, Vol. 1, 317–366, 2001. https://doi.org/10.1016/S1874-5849(01)80010-3
  • M. Ledoux, The Concentration of Measure Phenomenon, AMS Mathematical Surveys and Monographs 89, 2001. https://doi.org/10.1090/surv/089

Shared definitions: the items of this mission import Definitions.Def_GaussianMatrix_basic, a draft of Mission I; submit that proposal first so the import resolves at compile time.

Series: I. Rotation Invariance and Moment Identities · II. Inverse Moments of the Pseudoinverse · III. Extreme Singular Values and Concentration. All three missions share the definition bundle GaussianMatrix_basic, published with Mission I, and the namespace GaussianMatrix.

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Numerical AnalysisProbabilityRandom Matrix Theory·Captain: tc

Gaussian Random Matrices I: Rotation Invariance and Moment IdentitiesTextbook

Motivation

Randomized algorithms for low-rank approximation — the randomized SVD of Halko, Martinsson and Tropp (HMT 2011), generalized Nyström, randomized subspace iteration, one-pass sketching (Tropp–Webber 2023) — multiply the input matrix by a random test matrix Ω\OmegaΩ with independent standard normal entries. Every error bound for these methods rests on a small number of facts about such standard Gaussian matrices: they are invariant under rotations, disjoint blocks of a rotated copy are independent, and the second and fourth moments of a linearly transformed Gaussian matrix are given by explicit formulas. These facts are classical, but none of them is available in Mathlib, so a Lean development of randomized numerical linear algebra currently has to carry every one of them as an explicit hypothesis of its main theorems. This mission removes those hypotheses.

Setting

For p,m∈Np,m\in\mathbb Np,m∈N, a standard Gaussian matrix of size p×mp\times mp×m is a random matrix Γ∈Rp×m\Gamma\in\mathbb R^{p\times m}Γ∈Rp×m whose pmpmpm entries are independent N(0,1)\mathcal N(0,1)N(0,1) random variables. Its law, written γp,m\gamma_{p,m}γp,m​, is the product measure ⨂i<p⨂j<mN(0,1)\bigotimes_{i<p}\bigotimes_{j<m}\mathcal N(0,1)⨂i<p​⨂j<m​N(0,1) on real p×mp\times mp×m arrays.

For a real matrix AAA, ∥A∥F2=∑i,jAij2\|A\|_F^2=\sum_{i,j}A_{ij}^2∥A∥F2​=∑i,j​Aij2​ is the squared Frobenius norm; rank⁡A\operatorname{rank}ArankA is the dimension of its column space. A matrix V1∈Rn×kV_1\in\mathbb R^{n\times k}V1​∈Rn×k has orthonormal columns when V1TV1=IkV_1^{\mathsf T}V_1=I_kV1T​V1​=Ik​; a square such matrix is orthogonal. For t≥1t\ge1t≥1, a matrix S∈Rn×tS\in\mathbb R^{n\times t}S∈Rn×t with independent N(0,1/t)\mathcal N(0,1/t)N(0,1/t) entries is written S=t−1/2ΩS=t^{-1/2}\OmegaS=t−1/2Ω with Ω∼γn,t\Omega\sim\gamma_{n,t}Ω∼γn,t​, so that SST=1tΩΩTSS^{\mathsf T}=\tfrac1t\Omega\Omega^{\mathsf T}SST=t1​ΩΩT is an unbiased sketch of the identity.

Formalization targets

Goal — Gaussian approximate matrix multiplication

For fixed M∈Ra×nM\in\mathbb R^{a\times n}M∈Ra×n, N∈Rb×nN\in\mathbb R^{b\times n}N∈Rb×n and S∈Rn×tS\in\mathbb R^{n\times t}S∈Rn×t with independent N(0,1/t)\mathcal N(0,1/t)N(0,1/t) entries,

E ∥MSSTNT−MNT∥F2=∥M∥F2∥N∥F2+∥MNT∥F2t≤2t∥M∥F2∥N∥F2.\mathbb E\,\bigl\|MSS^{\mathsf T}N^{\mathsf T}-MN^{\mathsf T}\bigr\|_F^2=\frac{\|M\|_F^2\|N\|_F^2+\|MN^{\mathsf T}\|_F^2}{t}\le\frac2t\|M\|_F^2\|N\|_F^2 .E​MSSTNT−MNT​F2​=t∥M∥F2​∥N∥F2​+∥MNT∥F2​​≤t2​∥M∥F2​∥N∥F2​.

This is the exact mean-squared error of the sketched product MSSTNTMSS^{\mathsf T}N^{\mathsf T}MSSTNT as an estimator of MNTMN^{\mathsf T}MNT, a direct consequence of Isserlis' pairing formula for Gaussian fourth moments. It is the goal because it is the one fourth-moment computation the series needs and because every other identity in the mission is a step towards it.

Milestones

  • Rotational invariance. UΓV∼γp,mU\Gamma V\sim\gamma_{p,m}UΓV∼γp,m​ for orthogonal U∈Rp×pU\in\mathbb R^{p\times p}U∈Rp×p, V∈Rm×mV\in\mathbb R^{m\times m}V∈Rm×m (HMT §10.1).
  • Blocks of a rotated Gaussian matrix. For V1∈Rn×kV_1\in\mathbb R^{n\times k}V1​∈Rn×k with orthonormal columns, V1TΩ∼γk,tV_1^{\mathsf T}\Omega\sim\gamma_{k,t}V1T​Ω∼γk,t​; for orthonormal V1,V2V_1,V_2V1​,V2​ with V1TV2=0V_1^{\mathsf T}V_2=0V1T​V2​=0, the blocks V1TΩV_1^{\mathsf T}\OmegaV1T​Ω and V2TΩV_2^{\mathsf T}\OmegaV2T​Ω are independent (HMT, proof of Theorem 10.5).
  • Second moment. E∥SΓT∥F2=∥S∥F2∥T∥F2\mathbb E\|S\Gamma T\|_F^2=\|S\|_F^2\|T\|_F^2E∥SΓT∥F2​=∥S∥F2​∥T∥F2​ (HMT Proposition 10.1 (10.1); Tropp–Webber Lemma B.1).
  • Fourth moment. E∥SΓT∥F4=(∥S∥F2∥T∥F2)2+2∥STS∥F2∥TTT∥F2\mathbb E\|S\Gamma T\|_F^4=(\|S\|_F^2\|T\|_F^2)^2+2\|S^{\mathsf T}S\|_F^2\|TT^{\mathsf T}\|_F^2E∥SΓT∥F4​=(∥S∥F2​∥T∥F2​)2+2∥STS∥F2​∥TTT∥F2​, the Isserlis formula for the Gaussian quadratic form tr⁡(ΓTSTS Γ TTT)\operatorname{tr}(\Gamma^{\mathsf T}S^{\mathsf T}S\,\Gamma\,TT^{\mathsf T})tr(ΓTSTSΓTTT); its special case E∥Ω∥F4=(kt)2+2kt\mathbb E\|\Omega\|_F^4=(kt)^2+2ktE∥Ω∥F4​=(kt)2+2kt is the chi-square second moment (HMT Proposition A.8).
  • Full rank. rank⁡Γ=min⁡{p,m}\operatorname{rank}\Gamma=\min\{p,m\}rankΓ=min{p,m} almost surely (HMT, proof of Theorem 10.5 and Proposition A.5).

Significance

The results. Rotational invariance and block independence are the mechanism behind every conditioning argument in randomized linear algebra: writing the right singular vectors of the input as [V1 V2][V_1\ V_2][V1​ V2​], the sketch splits into independent standard Gaussian blocks Ω1=V1TΩ\Omega_1=V_1^{\mathsf T}\OmegaΩ1​=V1T​Ω and Ω2=V2TΩ\Omega_2=V_2^{\mathsf T}\OmegaΩ2​=V2T​Ω, and one may condition on Ω1\Omega_1Ω1​ while treating Ω2\Omega_2Ω2​ as fresh. The second-moment identity then turns the deterministic range-finder bound ∥Σ2Ω2Ω1†∥F\|\Sigma_2\Omega_2\Omega_1^{\dagger}\|_F∥Σ2​Ω2​Ω1†​∥F​ into ∥Σ2∥F2 E∥Ω1†∥F2\|\Sigma_2\|_F^2\,\mathbb E\|\Omega_1^{\dagger}\|_F^2∥Σ2​∥F2​E∥Ω1†​∥F2​, and the approximate-multiplication identity gives the one-pass error terms. Almost-sure full rank is what makes Ω1†\Omega_1^{\dagger}Ω1†​ a genuine pseudoinverse.

Formalizing them. Mathlib has the one-dimensional Gaussian measure, product measures, independence of coordinate projections, and (recently) the standard Gaussian measure on a finite-dimensional inner product space together with its invariance under linear isometries. None of the matrix-level statements above is in Mathlib. Once proved here they are reusable by every later mission in the series and by any formalization of randomized low-rank approximation, whose expectation-level inputs (e.g. E∥Σ2Ω2Ω1†∥F2=kt−k−1∥Σ2∥F2\mathbb E\|\Sigma_2\Omega_2\Omega_1^{\dagger}\|_F^2=\frac{k}{t-k-1}\|\Sigma_2\|_F^2E∥Σ2​Ω2​Ω1†​∥F2​=t−k−1k​∥Σ2​∥F2​) follow from these milestones together with the inverse moments of Mission II.

Difficulty

Rotational invariance is not a computation with densities on Rpm\mathbb R^{pm}Rpm that Mathlib supports out of the box: the clean route is through characteristic functions or through the basis-independence of the standard Gaussian on an inner product space, transported along the linear isometry Γ↦UΓV\Gamma\mapsto U\Gamma VΓ↦UΓV of Rp×m\mathbb R^{p\times m}Rp×m with the Frobenius inner product. Independence of the blocks requires identifying [V1 V2]TΩ[V_1\ V_2]^{\mathsf T}\Omega[V1​ V2​]TΩ with a product measure and then projecting onto disjoint coordinate sets, with a completion of [V1 V2][V_1\ V_2][V1​ V2​] to an orthogonal matrix when k+r<nk+r<nk+r<n. The moment identities are finite computations, but the fourth-moment identity needs the Gaussian moments Eg4=3\mathbb E g^4=3Eg4=3, Eg2=1\mathbb E g^2=1Eg2=1 organized through Isserlis' pairing formula over a four-fold sum of indices; the obvious entrywise expansion produces O((pm)4)O((pm)^4)O((pm)4) terms that must be collapsed symbolically. Almost-sure full rank is the statement that the zero set of a nonzero polynomial (det⁡\detdet of a maximal square submatrix) is Lebesgue-null, which must be established for the product Gaussian measure.

Formalization scope

The sample space is the function type Rp→Rm→R\mathbb R^{p}\to\mathbb R^{m}\to\mathbb RRp→Rm→R with the product σ\sigmaσ-algebra; a sample is viewed as a matrix through the identity map of\mathrm{of}of. Expectations are real Bochner integrals: for an identity with a nonzero right-hand side this forces integrability, and the integrands here are polynomials in Gaussian entries. Laws are stated as equalities of pushforward measures; independence is Mathlib's IndepFun. Dimensions may be 000; all statements remain true in that case. The hypothesis V1TV1=IkV_1^{\mathsf T}V_1=I_kV1T​V1​=Ik​ silently forces k≤nk\le nk≤n (vacuous otherwise), which matches the source.

The definition bundle GaussianMatrix_basic supplies the law γp,m\gamma_{p,m}γp,m​, ∥⋅∥F2\|\cdot\|_F^2∥⋅∥F2​, ∥⋅∥F\|\cdot\|_F∥⋅∥F​, the spectral norm (Mathlib's ℓ2\ell_2ℓ2​ operator norm), the smallest singular value and the pseudoinverse G†=GT(GGT)−1G^{\dagger}=G^{\mathsf T}(GG^{\mathsf T})^{-1}G†=GT(GGT)−1; it is shared by the whole series. Welcome contributions: the Gaussian integration-by-parts and Isserlis lemmas for finite index sets, the identification of γp,m\gamma_{p,m}γp,m​ with Mathlib's stdGaussian on the Frobenius inner product space, and the "polynomial zero sets are null" lemma for product measures.

Selected references

  • N. Halko, P.-G. Martinsson, J. A. Tropp, Finding structure with randomness: probabilistic algorithms for constructing approximate matrix decompositions, SIAM Review 53(2), 217–288, 2011. https://arxiv.org/abs/0909.4061
  • J. A. Tropp, R. J. Webber, Randomized algorithms for low-rank matrix approximation: design, analysis, and applications, 2023. https://arxiv.org/abs/2306.12418
  • R. Vershynin, Introduction to the non-asymptotic analysis of random matrices, in Compressed Sensing: Theory and Applications, Cambridge University Press, 2012. https://arxiv.org/abs/1011.3027
  • L. Isserlis, On a formula for the product-moment coefficient of any order of a normal frequency distribution in any number of variables, Biometrika 12, 134–139, 1918. https://doi.org/10.1093/biomet/12.1-2.134
  • S. Dasgupta, A. Gupta, An elementary proof of a theorem of Johnson and Lindenstrauss, Random Structures & Algorithms 22, 60–65, 2003. https://doi.org/10.1002/rsa.10073
  • M. Rudelson, R. Vershynin, The Littlewood–Offord problem and invertibility of random matrices, Advances in Mathematics 218, 600–633, 2008. https://arxiv.org/abs/math/0703503
  • Y. Chen, J. Dongarra, Condition numbers of Gaussian random matrices, SIAM J. Matrix Anal. Appl. 27(3), 603–620, 2005. https://doi.org/10.1137/040616413
  • A. Edelman, Eigenvalues and condition numbers of random matrices, SIAM J. Matrix Anal. Appl. 9(4), 543–560, 1988. https://doi.org/10.1137/0609045
  • Y. Gordon, Some inequalities for Gaussian processes and applications, Israel J. Math. 50, 265–289, 1985. https://doi.org/10.1007/BF02759761
  • K. R. Davidson, S. J. Szarek, Local operator theory, random matrices and Banach spaces, Handbook of the Geometry of Banach Spaces, Vol. 1, 317–366, 2001. https://doi.org/10.1016/S1874-5849(01)80010-3
  • M. Ledoux, The Concentration of Measure Phenomenon, AMS Mathematical Surveys and Monographs 89, 2001. https://doi.org/10.1090/surv/089

Series: I. Rotation Invariance and Moment Identities · II. Inverse Moments of the Pseudoinverse · III. Extreme Singular Values and Concentration. All three missions share the definition bundle GaussianMatrix_basic, published with Mission I, and the namespace GaussianMatrix.

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Dynamical SystemsProbabilityStochastic Systems·Captain: mikedeng1

Propagation of Chaos for Stochastic Spatially Structured Neuronal Networks with Delay driven by Jump Diffusions 1: The Spatially Structured McKean–Vlasov Delay Equation with Jumps Is Well-PosedResearch Paper

Motivation

Networks of conductance-based neurons, such as FitzHugh–Nagumo networks, are modelled by systems of stochastic differential equations in which each neuron interacts with the others through synapses, and the signal from one neuron reaches another only after a transmission delay. Biological neurons sit at positions in space, belong to a few distinct subpopulations, are driven by Brownian and Poisson (jump) noise, and vary from one to another; the last feature is modelled by a random disorder parameter. When the number of neurons tends to infinity, the state of a typical neuron is expected to follow a McKean–Vlasov equation: an SDE whose coefficients depend on the law of its own solution. S. Mehri, M. Scheutzow, W. Stannat and B. Z. Zangeneh (arXiv:1805.01654; Ann. Appl. Probab. 30 (2020), DOI 10.1214/19-AAP1499) prove that this limit equation is well-posed, with coefficients that are only monotone (one-sided Lipschitz), a general delay, jump noise, spatial structure and disorder all at once, and then prove propagation of chaos towards it.

Earlier work, as surveyed on p. 3 of the paper, covered parts of this setting: global Lipschitz coefficients (Quiñinao and Touboul 2015, and the paper's references [10, 11]), locally Lipschitz coefficients (Baladron, Fasoli, Faugeras and Touboul 2012, with the clarification of Bossy, Faugeras and Talay 2015 on the localization by hitting times; the same issue affects Touboul 2012), one-sided Lipschitz coefficients with diffusive noise (Luçon and Stannat 2014), and Lévy noise under global Lipschitz assumptions or gradient-type local dynamics (Andreis, Dai Pra and Fischer 2018). The paper constructs the solution by an Euler approximation, which, by the authors' account, had not been applied to McKean–Vlasov equations before.

Setting

Fix dimensions ddd (state), mmm, nnn (noise), kkk (space), a delay τ>0\tau > 0τ>0 and P≥1P \ge 1P≥1 subpopulations, located at pairwise disjoint measurable regions Γ1,…,ΓP⊂Rk\Gamma_1,\dots,\Gamma_P \subset \mathbb R^kΓ1​,…,ΓP​⊂Rk whose union Γ\GammaΓ is bounded. A finite Borel measure R\mathcal RR on Γ\GammaΓ with R(Γα)=1\mathcal R(\Gamma_\alpha) = 1R(Γα​)=1 describes the spatial distribution of neurons. A disorder probability space (Ω′,F′,P′)(\Omega',\mathcal F',\mathbb P')(Ω′,F′,P′) is fixed. On a filtered probability space (Ω,F,(Ft),P)(\Omega,\mathcal F,(\mathcal F_t),\mathbb P)(Ω,F,(Ft​),P) there are an mmm-dimensional Brownian motion WWW, nnn-dimensional Brownian motions B1,…,BPB^1,\dots,B^PB1,…,BP, Poisson random measures N,N1,…,NPN, N^1, \dots, N^PN,N1,…,NP on [0,∞)×U[0,\infty)\times U[0,∞)×U with intensity dt⊗νdt\otimes\nudt⊗ν (ν\nuν σ-finite; N~=N−dt⊗ν\tilde N = N - dt\otimes\nuN~=N−dt⊗ν), all independent, and initial paths z^ζ∈L2(Ω;Caˋdlaˋg([−τ,0];Rd))\hat z^\zeta \in L^2(\Omega;\text{Càdlàg}([-\tau,0];\mathbb R^d))z^ζ∈L2(Ω;Caˋdlaˋg([−τ,0];Rd)).

For a path yyy, write y(t−τ)−:t−y_{(t-\tau)^-:t^-}y(t−τ)−:t−​ for the segment u↦y(t+u)−u\mapsto y_{(t+u)^-}u↦y(t+u)−​, u∈[−τ,0]u\in[-\tau,0]u∈[−τ,0]. The equation is

dXtr=f(t,r,Xt−r,ω′)dt+g(⋅)dWt+∫Uh(⋅,ξ)N~(dt,dξ)+∑α=1P∫ΓαE~[θ(t,r,r′,Xt−r,X~(t−τ)−:t−r′,ω′)]R(dr′)dtdX^r_t = f(t,r,X^r_{t-},\omega')dt + g(\cdot)dW_t + \int_U h(\cdot,\xi)\tilde N(dt,d\xi) + \sum_{\alpha=1}^P\int_{\Gamma_\alpha}\tilde{\mathbb E}\big[\theta(t,r,r',X^r_{t-},\tilde X^{r'}_{(t-\tau)^-:t^-},\omega')\big]\mathcal R(dr')dtdXtr​=f(t,r,Xt−r​,ω′)dt+g(⋅)dWt​+∫U​h(⋅,ξ)N~(dt,dξ)+α=1∑P​∫Γα​​E~[θ(t,r,r′,Xt−r​,X~(t−τ)−:t−r′​,ω′)]R(dr′)dt +∑α=1P∫ΓαE~[β(⋯ )]R(dr′)dBtα+∑α=1P∫Γα∫UE~[η(⋯ ,ξ)]R(dr′)N~α(dt,dξ),Xtr=z^tζ (r∈Γζ, t∈[−τ,0]),(6)+ \sum_{\alpha=1}^P\int_{\Gamma_\alpha}\tilde{\mathbb E}[\beta(\cdots)]\mathcal R(dr')dB^\alpha_t + \sum_{\alpha=1}^P\int_{\Gamma_\alpha}\int_U\tilde{\mathbb E}[\eta(\cdots,\xi)]\mathcal R(dr')\tilde N^\alpha(dt,d\xi),\qquad X^r_t = \hat z^\zeta_t\ (r\in\Gamma_\zeta,\ t\in[-\tau,0]), \tag{6}+α=1∑P​∫Γα​​E~[β(⋯)]R(dr′)dBtα​+α=1∑P​∫Γα​​∫U​E~[η(⋯,ξ)]R(dr′)N~α(dt,dξ),Xtr​=z^tζ​ (r∈Γζ​, t∈[−τ,0]),(6)

where X~\tilde XX~ is an independent copy of the solution XXX and E~\tilde{\mathbb E}E~ its expectation. The local dynamics f,g,hf, g, hf,g,h satisfy the monotonicity and growth conditions (H1)–(H3) of Hypothesis 1.1 with locally integrable random rates Lt(ω′)L_t(\omega')Lt​(ω′), Kt(ω′)K_t(\omega')Kt​(ω′), K~t(R,ω′)\tilde K_t(R,\omega')K~t​(R,ω′); the synaptic coefficients θ,β,η\theta, \beta, \etaθ,β,η are Lipschitz (H4) and of linear growth (H5) in (x,y)(x, y)(x,y), with rates Lˉt(ω′)\bar L_t(\omega')Lˉt​(ω′), Kˉt(ω′)\bar K_t(\omega')Kˉt​(ω′), the path variable measured through a probability measure λ\lambdaλ on [−τ,0][-\tau,0][−τ,0]. In Lean, the model is the definition module NeuroMV.WellPosed.Setting: Space, Coeffs, Hyp1_1, Noise/IsNoise, IsStrongSol6, InClass and the constant C1 of (7).

Formalization targets

Goal: Theorem 1.5 (p. 7)

For every T>0T>0T>0 there is a process Xtr(ω;ω′)X^r_t(\omega;\omega')Xtr​(ω;ω′), measurable in (r,ω′,ω)(r,\omega',\omega)(r,ω′,ω), such that for P′\mathbb P'P′-almost every ω′\omega'ω′, X(ω′)X(\omega')X(ω′) is a strong solution of (6) on [−τ,T][-\tau,T][−τ,T],

X(ω′)∈L∞([−τ,T],dt;L2(Ω×Γ,P⊗R;Rd)),X(\omega') \in L^\infty\big([-\tau,T],dt;L^2(\Omega\times\Gamma,\mathbb P\otimes\mathcal R;\mathbb R^d)\big),X(ω′)∈L∞([−τ,T],dt;L2(Ω×Γ,P⊗R;Rd)),

and every other strong solution YYY in that class satisfies ∫ΓE∣Xtr−Ytr∣2R(dr)=0\int_\Gamma\mathbb E|X^r_t - Y^r_t|^2\mathcal R(dr) = 0∫Γ​E∣Xtr​−Ytr​∣2R(dr)=0 for all t∈[−τ,T]t\in[-\tau,T]t∈[−τ,T].

Milestones

  1. Theorem A.2 (p. 23): well-posedness of the general path-dependent delay SDE (20) with jumps under the monotonicity Hypothesis A.1, joint measurability in (t,ω,ω′)(t,\omega,\omega')(t,ω,ω′), the moment bound (22), and convergence of the Euler approximation (21).
  2. The scheme (11) exists and is measurable (p. 9), and satisfies the uniform bound (12): sup⁡t∈[−τ,T]E∣Xtn,r∣2≤C1(T,ω′)\sup_{t\in[-\tau,T]}\mathbb E|X^{n,r}_t|^2 \le C_1(T,\omega')supt∈[−τ,T]​E∣Xtn,r​∣2≤C1​(T,ω′).
  3. Claims (iv) and (v) (p. 10): the schemes are Cauchy in probability uniformly on [0,T][0,T][0,T], and their limit solves (6).
  4. Lemma 1.4 (p. 6): every solution in the class satisfies sup⁡s∈[−τ,t]E∣Xsr∣2≤C1(t,ω′)\sup_{s\in[-\tau,t]}\mathbb E|X^r_s|^2 \le C_1(t,\omega')sups∈[−τ,t]​E∣Xsr​∣2≤C1​(t,ω′).
  5. Uniqueness (pp. 16–17): two solutions in the class agree in L2(Ω×Γ)L^2(\Omega\times\Gamma)L2(Ω×Γ) at every time.

Significance

Theorem 1.5 makes the infinite-population limit of the network well defined; the second main result of the paper, Theorem 1.8, proves that the network converges to it in L2L^2L2. The theorem applies to coefficients that are only monotone in the state, which covers the cubic nonlinearity of FitzHugh–Nagumo neurons (Example 1.3), and to synaptic weights of conductance type driven by jump noise. Theorem A.2, proved in the appendix, is a well-posedness and Euler-convergence result for monotone stochastic delay equations with jumps and random coefficients, stated by the authors as new in this generality; it is reusable beyond this paper.

The results are proved in the paper; none of them has a machine-checked proof. The mission produces a Lean statement of the limit equation with the published Brownian and compensated Poisson integral relations, and invites formal proofs of the scheme estimates, the Cauchy property, the identification of the limit, the moment bound and uniqueness.

Difficulty

Under monotone coefficients there is no global contraction, so the Picard iteration that proves McKean–Vlasov well-posedness under Lipschitz assumptions does not apply. Localization by stopping times, the standard replacement for SDEs with monotone coefficients, does not localize the mean-field terms, which depend on the law of the solution at all positions; mishandling this step is the gap that Bossy, Faugeras and Talay pointed out in earlier work, and the acknowledgements (p. 30) record that the first version of this paper contained an unjustified application of the moment estimate of Lemma 1.4. A priori bounds must therefore be uniform in the approximation, and the limit of the mean-field stochastic integrals must be identified, with jumps and delay present. A second difficulty is measurability: the mean-field integrals require the solution to be measurable in the position r′r'r′, and the theorem asserts measurability in (r,ω′)(r,\omega')(r,ω′).

Formalization scope

  • Representation. Positions are EuclideanSpace ℝ (Fin k), states EthierKurtz.SDEState d, matrices Matrix (Fin d) (Fin m) ℝ with the Hilbert–Schmidt norm; subpopulations are Fin P, 0-based. Processes are indexed by ℝ on [−τ,T][-\tau,T][−τ,T]; drivers by ℝ≥0. Path segments are functions ℝ → ℝ^d read on [−τ,0][-\tau,0][−τ,0] with the product (cylinder) σ-algebra; the paper's sup-norm Borel σ-algebra is larger, so joint measurability of the coefficients for the cylinder σ-algebra is a mild added requirement.
  • Noise and integrals. Brownian integrals are the published EthierKurtz.HasBrownianItoIntegral, compensated jump integrals the published JacodTodorov10.LLN.HasCompInt, coordinatewise, with integrands cut off after TTT. All Poisson measures are one JacodTodorov10.LLN.IsFPoisson measure on a product mark space, equivalent to independent measures N,NαN, N^\alphaN,Nα. Independence of the initial data from the drivers is encoded by F0\mathcal F_0F0​-measurability.
  • Mean field. The copy X~\tilde XX~ enters only through its law, so E~\tilde{\mathbb E}E~ is an expectation over XXX itself; the mean-field integrands are required to be integrable on Γα×Ω\Gamma_\alpha\times\OmegaΓα​×Ω. Expectations and suprema are in [0,∞][0,\infty][0,∞]; Bochner integrals carry integrability clauses.
  • Hypotheses. Hypothesis 1.1 (H1)–(H5) and the regularity of p. 2; (H6) is omitted from every item, because it involves the network data of (1) only and the proof never uses it. The class L∞L^\inftyL∞–L2L^2L2 is a bound for every ttt rather than a.e. ttt.
  • Every position. The goal requires the integral identity at every r∈Γr\in\Gammar∈Γ, as (6) is posed; §2 proves it for R×P′\mathcal R\times\mathbb P'R×P′-a.e. (r,ω′)(r,\omega')(r,ω′) (p. 16), and on the remaining null set of positions (6) is an ordinary delay SDE solved by Theorem A.2 — a step the paper leaves implicit. Claim (v) keeps the R\mathcal RR-a.e. reading.
  • No trivialization. The stochastic integrals are the published relations tied to WWW, BαB^\alphaBα, NNN, NαN^\alphaNα, not free processes; the mean-field terms are computed from the solution's own segments; the solution class is non-empty for zero coefficients (a sorry-free check accompanies the mission); and the scheme and limit are the paper's, not new processes with their own noise.
  • Not stated. Claims (i)–(iii) of §2 (the remainder estimate and the a priori bounds before the stopping time) are not separate items.
  • Welcome contributions. Itô's formula for jump diffusions in this encoding, Gronwall-type lemmas in [0,∞][0,\infty][0,∞], stability of the published integral relations under convergence in probability, and the monotone delay SDE theory of Appendix A are all reusable beyond this mission.

Selected references

  • S. Mehri, M. Scheutzow, W. Stannat, B. Z. Zangeneh, Propagation of Chaos for Stochastic Spatially Structured Neuronal Networks with Delay driven by Jump Diffusions, arXiv:1805.01654v3, 2019; Ann. Appl. Probab. 30, 2020. https://arxiv.org/abs/1805.01654, https://doi.org/10.1214/19-AAP1499
  • J. Baladron, D. Fasoli, O. Faugeras, J. Touboul, Mean-field description and propagation of chaos in networks of Hodgkin–Huxley and FitzHugh–Nagumo neurons, J. Math. Neurosci. 2:10, 2012.
  • M. Bossy, O. Faugeras, D. Talay, Clarification and complement to "Mean-field description and propagation of chaos in networks of Hodgkin–Huxley and FitzHugh–Nagumo neurons", J. Math. Neurosci. 5:19, 2015.
  • E. Luçon, W. Stannat, Mean field limit for disordered diffusions with singular interactions, Ann. Appl. Probab. 24(5):1946–1993, 2014.
  • C. Quiñinao, J. Touboul, Limits and dynamics of randomly connected neuronal networks, Acta Appl. Math. 136(1):167–192, 2015.
  • J. Touboul, Limits and dynamics of stochastic neuronal networks with random heterogeneous delays, J. Stat. Phys. 149(4):569–597, 2012.
  • L. Andreis, P. Dai Pra, M. Fischer, McKean–Vlasov limit for interacting systems with simultaneous jumps, Stoch. Anal. Appl., 2018.
  • W. Liu, M. Röckner, Stochastic Partial Differential Equations: An Introduction, Universitext, Springer, 2015.

The bibliographic data of the last seven entries are taken from the reference list of the paper (pp. 30–31).

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Algorithmic Game TheoryDynamic ProgrammingProbability+1·Captain: mikedeng1

Approximate Markov-Nash Equilibria for Discrete-Time Risk-Sensitive Mean-Field Games 1: A Risk-Sensitive Mean-Field Game with Compact Actions and Weakly Continuous Kernel Has a Mean-Field EquilibriumResearch Paper

Motivation

Mean-field games describe large populations of identical agents who interact only through the distribution of their states. Each agent solves a stochastic control problem in which the population appears through a deterministic flow of distributions, and an equilibrium requires that this flow coincide with the distribution the agents generate themselves. The theory goes back to Huang, Malhamé and Caines (2006) and Lasry and Lions (2007) in continuous time. In discrete time, Saldi, Başar and Raginsky (SIAM J. Control Optim. 2018) proved existence of equilibria for risk-neutral agents with discounted costs on Polish state spaces.

Risk-neutral agents care only about expected cost. Many applications in engineering and finance call for agents that also penalize the variability of their cost. A standard way to model this is the exponential (risk-sensitive) criterion E[exp⁡(λ⋅cost)]E[\exp(\lambda\cdot\text{cost})]E[exp(λ⋅cost)] with risk factor λ>0\lambda>0λ>0. Its theory for single-agent Markov decision processes goes back to Howard and Matheson (1972) and Jacobson (1973), and Bäuerle and Rieder (Math. Oper. Res. 2014) treat general utilities. Saldi, Başar and Raginsky (arXiv:1808.03929, Math. Oper. Res. 2020) carry the discrete-time mean-field program over to this criterion. This mission covers its first main result: existence of a mean-field equilibrium (Theorem 1).

Setting

The state space X\mathsf XX and the action space A\mathsf AA are Polish, and A\mathsf AA is compact. P(E)\mathcal P(E)P(E) denotes the probability measures on EEE, with the topology of weak convergence and its Borel σ-field. The model consists of:

  • a stochastic kernel p(⋅ ∣ x,a,μ)p(\cdot\,|\,x,a,\mu)p(⋅∣x,a,μ) on X\mathsf XX given X×A×P(X)\mathsf X\times\mathsf A\times\mathcal P(\mathsf X)X×A×P(X);
  • a one-stage cost c(x,a,μ)∈[0,K]c(x,a,\mu)\in[0,K]c(x,a,μ)∈[0,K];
  • an initial law μ0\mu_0μ0​, a discount factor β∈(0,1)\beta\in(0,1)β∈(0,1) and a risk factor λ>0\lambda>0λ>0.

A Markov policy is a sequence π=(πt)t≥0\pi=(\pi_t)_{t\ge0}π=(πt​)t≥0​ of kernels πt(da ∣ x)\pi_t(da\,|\,x)πt​(da∣x). A policy in general is allowed to depend on the whole history (x(0),a(0),…,x(t))(x(0),a(0),\dots,x(t))(x(0),a(0),…,x(t)). Given a measure flow μ=(μt)t≥0⊂P(X)\mu=(\mu_t)_{t\ge0}\subset\mathcal P(\mathsf X)μ=(μt​)t≥0​⊂P(X), a generic agent evolves as

x(0)∼μ0,a(t)∼πt(⋅ ∣ history),x(t+1)∼p(⋅ ∣ x(t),a(t),μt),x(0)\sim\mu_0,\qquad a(t)\sim\pi_t(\cdot\,|\,\text{history}),\qquad x(t+1)\sim p(\cdot\,|\,x(t),a(t),\mu_t),x(0)∼μ0​,a(t)∼πt​(⋅∣history),x(t+1)∼p(⋅∣x(t),a(t),μt​),

and pays the risk-sensitive cost

Jμ(π)=Eπ[exp⁡(λ∑t=0∞βtc(x(t),a(t),μt))].J_\mu(\pi)=E^\pi\Big[\exp\Big(\lambda\sum_{t=0}^\infty\beta^tc(x(t),a(t),\mu_t)\Big)\Big].Jμ​(π)=Eπ[exp(λt=0∑∞​βtc(x(t),a(t),μt​))].

For a Markov policy, Λ(π)\Lambda(\pi)Λ(π) is the flow of state laws it generates: it starts at μ0\mu_0μ0​ and satisfies μt+1(⋅)=∫p(⋅ ∣ x,a,μt) πt(da∣x) μt(dx)\mu_{t+1}(\cdot)=\int p(\cdot\,|\,x,a,\mu_t)\,\pi_t(da|x)\,\mu_t(dx)μt+1​(⋅)=∫p(⋅∣x,a,μt​)πt​(da∣x)μt​(dx). A pair (π,μ)(\pi,\mu)(π,μ) is a mean-field equilibrium if μ=Λ(π)\mu=\Lambda(\pi)μ=Λ(π) and π\piπ minimizes JμJ_\muJμ​ over all policies.

Assumption 1 asks for the following:

  • (a) ccc is continuous with ∥c∥≤K\|c\|\le K∥c∥≤K;
  • (b) ppp is weakly continuous in (x,a,μ)(x,a,\mu)(x,a,μ);
  • (c) A\mathsf AA is compact;
  • (d) there are α≥0\alpha\ge0α≥0 and a continuous moment function w≥1w\ge1w≥1 (compact sets Kn↑XK_n\uparrow\mathsf XKn​↑X with inf⁡x∉Knw(x)→∞\inf_{x\notin K_n}w(x)\to\inftyinfx∈/Kn​​w(x)→∞) with ∫w(y) p(dy∣x,a,μ)≤αw(x)\int w(y)\,p(dy|x,a,\mu)\le\alpha w(x)∫w(y)p(dy∣x,a,μ)≤αw(x);
  • (e) ∫w dμ0<∞\int w\,d\mu_0<\infty∫wdμ0​<∞.

Formalization targets

Goal: Theorem 1 (p. 10)

Under Assumption 1 there are a Markov policy π\piπ and a flow μ\muμ with

μ=Λ(π)andJμ(π)=inf⁡σ∈ΠJμ(σ).\mu=\Lambda(\pi)\qquad\text{and}\qquad J_\mu(\pi)=\inf_{\sigma\in\Pi}J_\mu(\sigma).μ=Λ(π)andJμ​(π)=σ∈Πinf​Jμ​(σ).

Milestones

In the paper's order of proof:

  1. Proposition 1: Markov policies achieve the optimal value.
  2. Lemmas 1–3: the finite- and infinite-horizon optimal value functions Jkn(⋅,λβk)J^n_k(\cdot,\lambda\beta^k)Jkn​(⋅,λβk) and Jk(⋅,λβk)J_k(\cdot,\lambda\beta^k)Jk​(⋅,λβk) of the nonhomogeneous MDP of a fixed flow are bounded and continuous. They satisfy the dynamic programming equation TkJk+1(⋅,λβk+1)=Jk(⋅,λβk)T_kJ_{k+1}(\cdot,\lambda\beta^{k+1})=J_k(\cdot,\lambda\beta^k)Tk​Jk+1​(⋅,λβk+1)=Jk​(⋅,λβk), and
∥Jkn(⋅,λβk)−Jk(⋅,λβk)∥≤λK1−βeλβkK1−ββn+1.\big\|J^n_k(\cdot,\lambda\beta^k)-J_k(\cdot,\lambda\beta^k)\big\|\le\frac{\lambda K}{1-\beta}e^{\frac{\lambda\beta^kK}{1-\beta}}\beta^{n+1}.​Jkn​(⋅,λβk)−Jk​(⋅,λβk)​≤1−βλK​e1−βλβkK​βn+1.
  1. Theorem 2: a Markov policy is optimal if and only if it almost surely selects minimizers in the dynamic programming equation.
  2. Propositions 2–5 and Lemma 4: equilibria are fixed points of a set-valued map Γ\GammaΓ on state–action flows in Ξ=∏t{ν:ν1(w)≤αtM}\Xi=\prod_t\{\nu:\nu_1(w)\le\alpha^tM\}Ξ=∏t​{ν:ν1​(w)≤αtM}; the optimal value functions depend continuously on the flow; and the graph of Γ\GammaΓ is closed in Ξ×Ξ\Xi\times\XiΞ×Ξ.

Significance

The result. Theorem 1 is what makes the second main result of the paper meaningful. That result, Theorem 3 and the second mission of this series, states that the equilibrium policy is an ε\varepsilonε-Markov–Nash equilibrium of every NNN-agent game with NNN large enough. Equilibria of finite risk-sensitive games with many agents are rarely computable, so a mean-field equilibrium gives an approximately optimal decentralized policy that ignores the other agents' states. Along the way, the paper proves results on nonhomogeneous risk-sensitive MDPs that it describes as "mostly absent and dispersed in the literature": uniform finite-to-infinite horizon bounds and a characterization of optimal Markov policies. These results are useful outside game theory.

Formalizing it. The result is proved on paper. No part of it, nor of the risk-neutral precursor, has a machine-checked proof. Formalization produces a verified theory of nonhomogeneous risk-sensitive MDPs on Polish spaces, a verified closed-graph argument for the mean-field map, and an exact record of the hypotheses. The paper omits or cites several steps: Proposition 1, Proposition 2, Lemma 2, the conditional optimality (8) and the nonemptiness and convexity of Γ(ν)\Gamma(\nu)Γ(ν). A formalization has to supply them.

Difficulty

The obvious route is Banach's fixed point theorem for the dynamic programming operator, as in risk-neutral discounted MDPs. It fails here: the cost is multiplicative, and the operator TkT_kTk​ is not a contraction. Uniform convergence of value iteration has to come from the explicit tail bound of Lemma 3 instead.

The second obstacle is the fixed point itself. The natural map, from a flow to the flows of its optimal policies, is set-valued and lives on an infinite product of spaces of measures. Kakutani–Fan–Glicksberg applies only after three steps:

  • re-encoding the problem on state–action flows (the map Γ=C∩B\Gamma=C\cap BΓ=C∩B);
  • proving compactness of Ξ\XiΞ through the moment function (tightness);
  • proving that the graph of Γ\GammaΓ is closed (Proposition 4).

The last step requires the optimal value functions to vary continuously with the flow (Proposition 5) and a portmanteau argument for sets defined by optimality conditions. None of this machinery (the Kakutani–Fan–Glicksberg theorem in locally convex spaces, Prokhorov compactness via moment functions, continuous convergence) is in Mathlib in the required form.

Formalization scope

P(E)\mathcal P(E)P(E) is a type synonym of Mathlib's ProbabilityMeasure E with the weak topology and its Borel σ-field. The kernel ppp is a Mathlib Kernel on X×A×P(X)\mathsf X\times\mathsf A\times\mathcal P(\mathsf X)X×A×P(X). Policies are sequences of Markov kernels, and history-dependent policies take (X×A)t×X(\mathsf X\times\mathsf A)^t\times\mathsf X(X×A)t×X as input. The law PπP^\piPπ is built with the Ionescu–Tulcea kernel Kernel.trajMeasure, one coordinate (x(t),a(t))(x(t),a(t))(x(t),a(t)) per time step. Time is 000-based.

Standing hypotheses on every statement:

  • X\mathsf XX and A\mathsf AA are Polish and Borel;
  • A\mathsf AA is compact and nonempty (used tacitly by the paper);
  • β∈(0,1)\beta\in(0,1)β∈(0,1), λ>0\lambda>0λ>0, and c≥0c\ge0c≥0 is measurable;
  • Assumption 1.

For §4.2 the pair (α,w)(\alpha,w)(α,w) defining Ξ\XiΞ is an explicit argument. In §4.1, "policy" means Markov policy, as the paper states on p. 11. The conditional expectations "given x(k)=xx(k)=xx(k)=x" are expectations for the chain started at time kkk in xxx. Lemma 1 is stated with ζk,n=∑t=knβt\zeta_{k,n}=\sum_{t=k}^n\beta^tζk,n​=∑t=kn​βt, the quantity its proof uses; the page prints ∑t=knβk\sum_{t=k}^n\beta^k∑t=kn​βk.

The goal asks for a Markov equilibrium policy that is optimal against all history-dependent policies, at least as strong as Definition 3. Optimality is "≤\le≤ the cost of every policy", not an infimum, so it has no junk case. The cost is a genuine integral: with c≥0c\ge0c≥0 bounded, the integrand lies in [1,eλK/(1−β)][1,e^{\lambda K/(1-\beta)}][1,eλK/(1−β)], so no policy is trivially optimal. The moment-function predicate has no infimum, so compact X\mathsf XX is admitted.

Contributions are welcome at every level:

  • risk-sensitive dynamic programming on Borel spaces (reusable for any MDP);
  • the Kakutani–Fan–Glicksberg theorem in locally convex spaces;
  • Prokhorov compactness from moment functions;
  • measurable selection and disintegration of state–action measures.

Selected references

  • N. Saldi, T. Başar, M. Raginsky, Discrete-time Risk-sensitive Mean-field Games, arXiv:1808.03929v2, 2018; published as Approximate Markov-Nash Equilibria for Discrete-Time Risk-Sensitive Mean-Field Games, Math. Oper. Res. 45(4), 2020. https://arxiv.org/abs/1808.03929
  • N. Saldi, T. Başar, M. Raginsky, Markov–Nash Equilibria in Mean-Field Games with Discounted Cost, SIAM J. Control Optim. 56(6), 2018. https://doi.org/10.1137/17M1112583
  • N. Bäuerle, U. Rieder, More Risk-Sensitive Markov Decision Processes, Math. Oper. Res. 39(1), 2014. https://doi.org/10.1287/moor.2013.0601
  • O. Hernández-Lerma, J. B. Lasserre, Discrete-Time Markov Control Processes: Basic Optimality Criteria, Springer, 1996. https://doi.org/10.1007/978-1-4612-0729-0
  • C. D. Aliprantis, K. C. Border, Infinite Dimensional Analysis, 3rd ed., Springer, 2006. https://doi.org/10.1007/3-540-29587-9
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Operations ResearchOptimizationProbability+1·Captain: mikedeng1

Solving Chance-Constrained Problems via a Smooth Sample-Based Nonlinear Approximation 2: Optimal Values and Solutions of the Smoothed SAA Converge w.p.1 as N → ∞ and ε → 0Research Paper

Motivation

A chance-constrained program asks for a decision that satisfies uncertain constraints with high probability rather than surely:

min⁡x∈Xf(x)s.t.P(cj(x,ξ)≤0, j=1,…,m)≥1−α.(1.1)\min_{x\in X} f(x) \quad\text{s.t.}\quad \mathbb P\bigl(c_j(x,\xi)\le 0,\ j=1,\dots,m\bigr)\ge 1-\alpha. \tag{1.1}x∈Xmin​f(x)s.t.P(cj​(x,ξ)≤0, j=1,…,m)≥1−α.(1.1)

Such models appear in power-system operation, portfolio selection, chemical-process and reservoir management, and other settings where requiring the constraints for every realization is too conservative (Nemirovski–Shapiro 2006; the paper's introduction lists applications). The probability is rarely available in closed form, and when the distribution of ξ\xiξ is only accessible through samples, the feasible set of the empirical counterpart is a union of polyhedral-like pieces: it is non-smooth and non-convex, and the empirical quantile introduces many spurious local minima (Peña-Ordieres, Luedtke, Wächter 2020, §2).

Peña-Ordieres, Luedtke and Wächter replace the indicator inside the empirical probability by a smooth kernel with bandwidth ε\varepsilonε, which turns the sample constraint into a differentiable one suitable for nonlinear programming solvers. This mission formalizes the paper's consistency result: as the sample size grows and the bandwidth shrinks, jointly, the optimal values and optimal solutions of the smoothed sample problem converge to those of the true problem with probability one.

Timeline. Consistency of sample approximations of chance constraints with the plain empirical cdf goes back to Pagnoncelli, Ahmed, Shapiro 2009 (reference [36] of the paper; its Propositions 2.1 and 2.2). Luedtke–Ahmed 2008 gave finite-sample feasibility guarantees for the same empirical approximation. Convergence with respect to a smoothing parameter alone was studied by Geletu, Hoffmann, Klöppel and Li (SIAM J. Optim. 27, 2017), Hong, Yang, Zhang 2011 and Hu, Hong and Zhang (IIE Trans. 45, 2013) (references [15], [25], [26] of the paper). Peña-Ordieres–Luedtke–Wächter 2020 (SIAM J. Optim. 30(3)) treat both parameters simultaneously; Theorem 3.5 of the preprint arXiv:1905.07377v2 is the result posed here.

Setting

Decisions are vectors x∈Rnx\in\mathbb R^nx∈Rn restricted to a closed set XXX. The random data ξ\xiξ takes values in a measurable space Ξ\XiΞ with law Pξ\mathbb P_\xiPξ​. The constraints are aggregated into one scalar function C(x,ξ)=max⁡jcj(x,ξ)C(x,\xi)=\max_j c_j(x,\xi)C(x,ξ)=maxj​cj​(x,ξ), and the risk level is α∈(0,1)\alpha\in(0,1)α∈(0,1).

  • True distribution function. F(t;x)=Pξ(C(x,ξ)≤t)F(t;x)=\mathbb P_\xi(C(x,\xi)\le t)F(t;x)=Pξ​(C(x,ξ)≤t). The true feasible region is Xα={x∈X∣F(0;x)≥1−α}X_\alpha=\{x\in X\mid F(0;x)\ge 1-\alpha\}Xα​={x∈X∣F(0;x)≥1−α}; the optimal solution set and value of (1.1) are SSS and v∗v^*v∗.
  • Smoothed indicator. For ε>0\varepsilon>0ε>0, Γε(y)\Gamma_\varepsilon(y)Γε​(y) equals 111 for y≤−εy\le-\varepsilony≤−ε, 000 for y≥εy\ge\varepsilony≥ε, and γε(y)\gamma_\varepsilon(y)γε​(y) in between, where γε:[−ε,ε]→[0,1]\gamma_\varepsilon:[-\varepsilon,\varepsilon]\to[0,1]γε​:[−ε,ε]→[0,1] is strictly decreasing, symmetric (γε(−y)=1−γε(y)\gamma_\varepsilon(-y)=1-\gamma_\varepsilon(y)γε​(−y)=1−γε​(y)), and makes Γε\Gamma_\varepsilonΓε​ differentiable. The paper's concrete choice is the quartic kernel (2.6).
  • Smoothed distribution functions. Fε(t;x)=∫Γε(C(x,ξ)−t) dPξF_\varepsilon(t;x)=\int\Gamma_\varepsilon(C(x,\xi)-t)\,d\mathbb P_\xiFε​(t;x)=∫Γε​(C(x,ξ)−t)dPξ​, and, for an i.i.d. sample ξ1,…,ξN\xi_1,\dots,\xi_Nξ1​,…,ξN​,
FεN(t;x)=1N∑i=1NΓε(C(x,ξi)−t).F^N_\varepsilon(t;x)=\frac1N\sum_{i=1}^N\Gamma_\varepsilon\bigl(C(x,\xi_i)-t\bigr).FεN​(t;x)=N1​i=1∑N​Γε​(C(x,ξi​)−t).
  • Smoothed sample problem (2.4). min⁡x∈Xf(x)\min_{x\in X} f(x)minx∈X​f(x) subject to FεN(0;x)≥1−αF^N_\varepsilon(0;x)\ge1-\alphaFεN​(0;x)≥1−α, with optimal solution set SεNS^N_\varepsilonSεN​ and value vεNv^N_\varepsilonvεN​.

The standing assumptions are: Assumption 3.1, for each x∈Xx\in Xx∈X the random variable C(x,ξ)C(x,\xi)C(x,ξ) has a continuous distribution; Assumption 3.2, CCC is Carathéodory, i.e. C(x,⋅)C(x,\cdot)C(x,⋅) is measurable for each x∈Xx\in Xx∈X and C(⋅,ξ)C(\cdot,\xi)C(⋅,ξ) is continuous for almost every ξ\xiξ; Assumption 3.3, some optimal solution xˉ\bar xxˉ of (1.1) is a limit of points x∈Xx\in Xx∈X with F(0;x)>1−αF(0;x)>1-\alphaF(0;x)>1−α.

Formalization targets

Goal: Theorem 3.5

If XXX is compact, fff is continuous and Assumptions 3.1–3.3 hold, then with probability one, as N→∞N\to\inftyN→∞ and ε→0\varepsilon\to0ε→0 jointly,

SεN≠∅ eventually,vεN→v∗,D(SεN,S)=sup⁡x∈SεNdist⁡(x,S)→0.S^N_\varepsilon\neq\emptyset\ \text{eventually},\qquad v^N_\varepsilon\to v^*,\qquad \mathbb D(S^N_\varepsilon,S)=\sup_{x\in S^N_\varepsilon}\operatorname{dist}(x,S)\to0 .SεN​=∅ eventually,vεN​→v∗,D(SεN​,S)=x∈SεN​sup​dist(x,S)→0.

Milestones

  1. Uniform law of large numbers (proof of Theorem 3.4): w.p.1, sup⁡ε∈(0,1]sup⁡x∈U∣FεN(0;x)−Fε(0;x)∣→0\sup_{\varepsilon\in(0,1]}\sup_{x\in U}|F^N_\varepsilon(0;x)-F_\varepsilon(0;x)|\to0supε∈(0,1]​supx∈U​∣FεN​(0;x)−Fε​(0;x)∣→0 as N→∞N\to\inftyN→∞, for compact U⊆XU\subseteq XU⊆X.
  2. Removal of the smoothing (proof of Theorem 3.4): sup⁡x∈U∣Fε(0;x)−F(0;x)∣→0\sup_{x\in U}|F_\varepsilon(0;x)-F(0;x)|\to0supx∈U​∣Fε​(0;x)−F(0;x)∣→0 as ε→0+\varepsilon\to0^+ε→0+.
  3. Theorem 3.4: w.p.1, sup⁡x∈U∣FεN(0;x)−F(0;x)∣→0\sup_{x\in U}|F^N_\varepsilon(0;x)-F(0;x)|\to0supx∈U​∣FεN​(0;x)−F(0;x)∣→0 as N→∞N\to\inftyN→∞ and ε→0\varepsilon\to0ε→0.
  4. Eventual nonemptiness of SεNS^N_\varepsilonSεN​ (proof of Theorem 3.5).
  5. (3.3): lim inf⁡vεN≥v∗\liminf v^N_\varepsilon\ge v^*liminfvεN​≥v∗ w.p.1.
  6. (3.4): lim sup⁡vεN≤v∗\limsup v^N_\varepsilon\le v^*limsupvεN​≤v∗ w.p.1.

Significance

Theorem 3.5 justifies solving the smooth problem (2.4) in place of (1.1): with enough samples and a small enough bandwidth, global solutions of the surrogate approximate global solutions of the chance-constrained program, and the optimal values agree in the limit. Unlike earlier results it controls the two approximation errors, sampling and smoothing, at once, so no order of limits has to be chosen in practice. It is the asymptotic counterpart of the paper's finite-sample feasibility bound (Theorem 3.13) and the theoretical basis for the trust-region method of §5.

The result is proved in the paper, with two steps imported from Shapiro–Dentcheva–Ruszczyński, second edition (a uniform law of large numbers, Theorem 7.53, and a convergence-of-expectations result, Theorem 4.91) and the deviation statement deferred to Theorem 5.3 there. None of these results, and no consistency theorem for sample approximations of chance constraints, is machine-checked on Prove2Me or, as far as is known, elsewhere. A formal proof requires writing the imported steps out for the specific integrands of this problem and completing the solution-set argument the paper leaves to the reference.

Difficulty

The pointwise statements are routine; the uniformity is not. The integrand Γε(C(x,ξ))\Gamma_\varepsilon(C(x,\xi))Γε​(C(x,ξ)) converges, as ε→0\varepsilon\to0ε→0, to the indicator 1{C(x,ξ)≤0}\mathbf 1\{C(x,\xi)\le0\}1{C(x,ξ)≤0}, which is discontinuous in xxx wherever C(x,ξ)=0C(x,\xi)=0C(x,ξ)=0. A uniform law of large numbers for a family that degenerates into indicators needs the no-atom Assumption 3.1 at every point of UUU, not only at the limit. Moreover, the smoothing functions γε\gamma_\varepsilonγε​ for different ε\varepsilonε are unrelated, so the family is not continuous in ε\varepsilonε, and a Glivenko–Cantelli argument over a joint parameter (x,ε)(x,\varepsilon)(x,ε) cannot be applied directly. The convergence of solution sets needs, in addition, that the limit of feasible points of (2.4) is feasible for (1.1), which uses the continuity of F(0;⋅)F(0;\cdot)F(0;⋅) on XXX; that continuity again rests on Assumptions 3.1 and 3.2.

Formalization scope

  • Decisions are Fin n → ℝ with the sup norm. Assumption 3.3 is stated for every radius, so the norm choice does not change it.
  • The sample is an infinite sequence ξ : ℕ → Ω → Ξ of measurable, independent maps on a probability space, each with law Pξ\mathbb P_\xiPξ​; FεNF^N_\varepsilonFεN​ uses the first NNN draws.
  • "As N→∞N\to\inftyN→∞ and ε→0\varepsilon\to0ε→0" is the product filter atTop ×ˢ 𝓝[>] 0 on N×R\mathbb N\times\mathbb RN×R, with ε>0\varepsilon>0ε>0 because Γε\Gamma_\varepsilonΓε​ needs it; one null set serves every conclusion of a statement.
  • Assumption 3.1 is "no atoms": Pξ(C(x,ξ)=y)=0\mathbb P_\xi(C(x,\xi)=y)=0Pξ​(C(x,ξ)=y)=0 for all x∈Xx\in Xx∈X, y∈Ry\in\mathbb Ry∈R. Assumption 3.2 is measurability of C(x,⋅)C(x,\cdot)C(x,⋅) on XXX plus almost-sure continuity of C(⋅,ξ)C(\cdot,\xi)C(⋅,ξ) on Rn\mathbb R^nRn.
  • The family γε\gamma_\varepsilonγε​ is any family with each member admissible; no relation across ε\varepsilonε is assumed. The quartic kernel (2.6) is admissible for every ε>0\varepsilon>0ε>0, so the hypothesis is satisfiable.
  • The feasible set of (2.4) is {x∈X∣FεN(0;x)≥1−α}\{x\in X\mid F^N_\varepsilon(0;x)\ge1-\alpha\}{x∈X∣FεN​(0;x)≥1−α}, the form the paper's proof uses. The quantile Qε1−αQ^{1-\alpha}_\varepsilonQε1−α​ of (2.4) is defined only when (1−α)N∉Z(1-\alpha)N\notin\mathbb Z(1−α)N∈/Z, which fails for infinitely many NNN when α\alphaα is rational; where it is defined, the two feasible sets coincide.
  • The optimal value is the real infimum, which Lean sets to 000 on an empty set. The goal therefore asserts eventual nonemptiness of SεNS^N_\varepsilonSεN​ itself, and (3.3)–(3.4) are stated as bounds on fff over the feasible set of (2.4), which imply the liminf and limsup without reading an infimum over a possibly empty set. The deviation D\mathbb DD is stated pointwise ("every point of SεNS^N_\varepsilonSεN​ is eventually within η\etaη of SSS"), with SSS nonempty by Assumption 3.3, so the distance to the empty set never arises.
  • Iterated limits (first NNN, then ε\varepsilonε), a null set chosen after η\etaη, or a feasible set defined through QεQ_\varepsilonQε​ with its junk value would each be a different and weaker statement; none is used.

The definitions layer (Γ_ε, admissibility, FFF, FεF_\varepsilonFε​, FεNF^N_\varepsilonFεN​, XαX_\alphaXα​, the shifted sample sets (3.2)) is shared with the companion mission on finite-sample feasibility. A uniform law of large numbers for almost-surely continuous, bounded integrands on a compact parameter set, and convergence of optimal values under uniform convergence of constraint functions, are reusable beyond this mission; contributions of either as standalone lemmas are welcome.

Selected references

  • A. Peña-Ordieres, J. R. Luedtke, A. Wächter, Solving chance-constrained problems via a smooth sample-based nonlinear approximation, SIAM J. Optim. 30(3), 2020; preprint arXiv:1905.07377v2, 2020. https://arxiv.org/abs/1905.07377, https://doi.org/10.1137/19M1261985
  • A. Shapiro, D. Dentcheva, A. Ruszczyński, Lectures on Stochastic Programming: Modeling and Theory, SIAM, second edition, 2014 (Theorems 4.91, 5.3, 7.53; reference [40] of the paper). https://doi.org/10.1137/1.9781611973433
  • B. K. Pagnoncelli, S. Ahmed, A. Shapiro, Sample average approximation method for chance constrained programming: theory and applications, J. Optim. Theory Appl. 142, 2009, pp. 399–416. https://doi.org/10.1007/s10957-009-9523-6
  • J. Luedtke, S. Ahmed, A sample approximation approach for optimization with probabilistic constraints, SIAM J. Optim. 19, 2008, pp. 674–699. https://doi.org/10.1137/070702928
  • L. J. Hong, Y. Yang, L. Zhang, Sequential convex approximations to joint chance constrained programs: a Monte Carlo approach, Oper. Res. 59, 2011, pp. 617–630. https://doi.org/10.1287/opre.1100.0910
  • A. Nemirovski, A. Shapiro, Convex approximations of chance constrained programs, SIAM J. Optim. 17, 2006, pp. 969–996. https://doi.org/10.1137/050622328
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Algorithmic Game TheoryGraph TheoryProbability+1·Captain: mikedeng1

A Case Study on Stochastic Games on Large Graphs in Mean Field and Sparse Regimes II: Large-Graph Limits of the Equilibrium Through the Laplacian Eigenvalue DistributionResearch Paper

Motivation

Mean field games describe large populations of agents who interact symmetrically: every agent sees the same average of all the others. Many populations interact instead along a network, where each agent responds only to its neighbours. Lacker and Soret (arXiv:2005.14102v2, 2021; Math. Oper. Res. 2022) study a linear-quadratic stochastic differential game on a finite graph that is simple enough to solve explicitly on every vertex-transitive graph, and then ask what happens to the equilibrium as the graph grows. The question is the network analogue of the classical convergence problem for mean field games: does the nnn-player equilibrium have a limit, and does that limit depend on the graph only through a small amount of information?

The answer of the paper is that the limit is governed by the empirical eigenvalue distribution of the graph Laplacian. Dense graph sequences (degrees tending to infinity) all have the same limit, the mean field game; sparse ones (bounded degrees) have limits that depend on the graph, through its spectrum. This mission formalizes that large-graph limit theorem, Theorem 2.6 of the paper. Mission I of the series formalizes the explicit equilibrium on a fixed transitive graph (Theorem 2.5), on which this mission builds.

Setting

Let GGG be a finite simple graph on vertex set {1,…,n}\{1,\dots,n\}{1,…,n} with adjacency matrix AGA_GAG​ and degree matrix DGD_GDG​. Its Laplacian is LG=DG−1AG−IL_G = D_G^{-1}A_G - ILG​=DG−1​AG​−I. GGG is transitive if every vertex can be mapped to every other one by a graph automorphism; such a graph is regular, of degree δ(G)\delta(G)δ(G), and LGL_GLG​ is then symmetric with eigenvalues λ1G,…,λnG∈[−2,0]\lambda^G_1,\dots,\lambda^G_n\in[-2,0]λ1G​,…,λnG​∈[−2,0]. The empirical eigenvalue distribution is μG=1n∑iδλiG\mu_G = \frac1n\sum_i\delta_{\lambda^G_i}μG​=n1​∑i​δλiG​​.

Fix a horizon T>0T>0T>0, a volatility σ>0\sigma>0σ>0 and a weight c>0c>0c>0. Player vvv controls the state

dXv(t)=αv(t,X(t)) dt+σ dWv(t),t∈[0,T],dX_v(t) = \alpha_v(t,\boldsymbol X(t))\,dt + \sigma\,dW_v(t),\qquad t\in[0,T],dXv​(t)=αv​(t,X(t))dt+σdWv​(t),t∈[0,T],

driven by independent Brownian motions, with Markovian feedback controls αv\alpha_vαv​, and pays

Jv=12 E[∫0T∣αv(t,X(t))∣2dt+c ∣Xv(T)−1deg⁡(v)∑u∼vXu(T)∣2].J_v = \tfrac12\,\mathbb E\Big[\int_0^T|\alpha_v(t,\boldsymbol X(t))|^2dt + c\,\Big|X_v(T) - \tfrac1{\deg(v)}\sum_{u\sim v}X_u(T)\Big|^2\Big].Jv​=21​E[∫0T​∣αv​(t,X(t))∣2dt+c​Xv​(T)−deg(v)1​u∼v∑​Xu​(T)​2].

On a transitive graph without isolated vertices, Theorem 2.5 gives an explicit Nash equilibrium: with QG(x)=det⁡(I−xLG)1/nQ_G(x) = \det(I - xL_G)^{1/n}QG​(x)=det(I−xLG​)1/n and fGf_GfG​ the solution of fG′=c QG′(fG)f_G' = c\,Q_G'(f_G)fG′​=cQG′​(fG​), fG(0)=0f_G(0) = 0fG​(0)=0 on [0,T][0,T][0,T], the feedback is αiG(t,x)=−ei⊤PG(t)x\alpha^G_i(t,\boldsymbol x) = -e_i^\top P_G(t)\boldsymbol xαiG​(t,x)=−ei⊤​PG​(t)x with PG(t)=−fG′(T−t)LG(I−fG(T−t)LG)−1P_G(t) = -f_G'(T-t)L_G(I - f_G(T-t)L_G)^{-1}PG​(t)=−fG′​(T−t)LG​(I−fG​(T−t)LG​)−1. The resulting equilibrium state process XG\boldsymbol X^GXG is Gaussian, and the value is Val(G)=1n∑vJv\mathrm{Val}(G) = \frac1n\sum_v J_vVal(G)=n1​∑v​Jv​.

For a probability measure μ\muμ define Qμ(x)=exp⁡∫[−2,0]log⁡(1−xλ) μ(dλ)Q_\mu(x) = \exp\int_{[-2,0]}\log(1-x\lambda)\,\mu(d\lambda)Qμ​(x)=exp∫[−2,0]​log(1−xλ)μ(dλ), so that QμG=QGQ_{\mu_G} = Q_GQμG​​=QG​.

Formalization targets

Goal: Theorem 2.6

Let (Gn)(G_n)(Gn​) be finite transitive graphs without isolated vertices, ∣Gn∣→∞|G_n|\to\infty∣Gn​∣→∞, with XGn(0)=0\boldsymbol X^{G_n}(0) = 0XGn​(0)=0, and suppose μGn→μ\mu_{G_n}\to\muμGn​​→μ weakly for a probability measure μ\muμ. Then (1) the ODE fμ′=c Qμ′(fμ)f_\mu' = c\,Q_\mu'(f_\mu)fμ′​=cQμ′​(fμ​), fμ(0)=0f_\mu(0) = 0fμ​(0)=0 has a unique solution on [0,T][0,T][0,T]; (2) for every vertex sequence knk_nkn​ and t∈[0,T]t\in[0,T]t∈[0,T],

Law(XknGn(t))→N(0,Vμ(t)),Vμ(t)=σ2∫0t∫[−2,0](1−λfμ(T−t)1−λfμ(T−s))2μ(dλ) ds;\mathrm{Law}\big(X^{G_n}_{k_n}(t)\big)\to\mathcal N\big(0,V_\mu(t)\big),\qquad V_\mu(t) = \sigma^2\int_0^t\int_{[-2,0]}\Big(\frac{1-\lambda f_\mu(T-t)}{1-\lambda f_\mu(T-s)}\Big)^2\mu(d\lambda)\,ds;Law(Xkn​Gn​​(t))→N(0,Vμ​(t)),Vμ​(t)=σ2∫0t​∫[−2,0]​(1−λfμ​(T−s)1−λfμ​(T−t)​)2μ(dλ)ds;

(3) the empirical measure 1∣Gn∣∑iδXiGn(t)\frac1{|G_n|}\sum_i\delta_{X^{G_n}_i(t)}∣Gn​∣1​∑i​δXiGn​​(t)​ converges weakly in probability to N(0,Vμ(t))\mathcal N(0,V_\mu(t))N(0,Vμ​(t)); (4)

lim⁡n→∞Val(Gn)=−σ22log⁡∫[−2,0]−λ1−λfμ(T) μ(dλ).\lim_{n\to\infty}\mathrm{Val}(G_n) = -\frac{\sigma^2}2\log\int_{[-2,0]}\frac{-\lambda}{1-\lambda f_\mu(T)}\,\mu(d\lambda).n→∞lim​Val(Gn​)=−2σ2​log∫[−2,0]​1−λfμ​(T)−λ​μ(dλ).

Milestones

The milestones are the statements the paper's proof (§3, §6, §7.1) relies on: the stability of fμf_\mufμ​ in μ\muμ (Proposition 3.2, last sentence); the finite-graph variance formula (2.7); monotonicity and concavity of fμf_\mufμ​ (Proposition 3.3, first sentence); correlation decay (Proposition 2.12) for distinct vertices; the relation between degrees and the spectral limit (Lemma 7.1); the Gaussian Poincaré bound (7.3) and the concentration (7.1) of the empirical measure; and the spectral form (2.9) of the value.

Significance

Theorem 2.6 reduces the large-population behaviour of a network game to one spectral object. For complete graphs μ=δ−1\mu = \delta_{-1}μ=δ−1​ and the limit is the mean field game; for sparse sequences such as cycles, tori, or random regular graphs, μ\muμ is a non-degenerate measure and the limiting variance and value differ from the mean field ones. The theorem thereby gives a quantitative criterion for when a mean field approximation of a network game is accurate, and it shows propagation of chaos in both regimes: in the dense case because interactions are weak, in the sparse case because typical players are far apart in the graph.

The result is proved in the paper; none of it has been machine-checked. A complete formalization requires a Lean account of Gaussian laws of linear SDEs with additive noise, of weak convergence of spectral measures of graph Laplacians, and of a Gaussian Poincaré inequality, none of which is currently in Mathlib in the needed form. Each of these is reusable well beyond this mission.

Difficulty

Parts (2) and (4) follow from the finite-graph formulas once fGn→fμf_{G_n}\to f_\mufGn​​→fμ​ uniformly, but that convergence requires stability of a nonlinear ODE whose vector field is defined through the spectral measure, uniformly over a class of measures. The harder step is (3). Convergence of one player's law does not imply convergence of the empirical measure: the players are correlated, and on sparse graphs every player has a bounded number of strong neighbours, so the correlations do not vanish uniformly. Bounding them requires an estimate that decays in the graph distance and in the degree, and combining it with the growth of graph balls, which is controlled differently in the dense and in the sparse regime. The usual mean field route is closed: unless the graph is complete, the state vector is not exchangeable, so propagation-of-chaos arguments based on exchangeability do not apply.

Formalization scope

The Lean development lives in namespace GraphLQGame.Asymptotics.

  • Vertices {1,…,n}\{1,\dots,n\}{1,…,n} are Fin n; a graph sequence is G : ∀ k, SimpleGraph (Fin (N k)) with Nk→∞N_k\to\inftyNk​→∞.
  • LGL_GLG​ is the random-walk Laplacian above, not Mathlib's lapMatrix. μG\mu_GμG​ is built from the real roots of the characteristic polynomial of LGL_GLG​, with multiplicity.
  • Weak convergence of measures on R\mathbb RR is convergence of ∫h dμk\int h\,d\mu_k∫hdμk​ for every bounded continuous hhh. Weak convergence in probability of the empirical measure is convergence in probability of ∫h dmGn(t)\int h\,dm^{G_n}(t)∫hdmGn​(t) for every bounded continuous hhh.
  • A state process is a pathwise strong solution of (2.1) on its own probability space, driven by a standard Brownian motion and adapted to its completed filtration. Statements about several graphs are statements about laws.
  • Costs are [0,∞][0,\infty][0,∞]-valued lower integrals; the value is computed after asserting finiteness.
  • In PGP_GPG​, fG′(T−t)f_G'(T-t)fG′​(T−t) is written as its ODE value c QG′(fG(T−t))c\,Q_G'(f_G(T-t))cQG′​(fG​(T−t)). ODE solutions are constrained on [0,T][0,T][0,T] (or on R+\mathbb R_+R+​ for Propositions 3.2 and 3.3), with uniqueness stated on that domain.
  • The Gaussian law N(0,V)\mathcal N(0,V)N(0,V) is gaussianReal 0 V.toNNReal; Vμ(t)≥0V_\mu(t)\ge0Vμ​(t)≥0.

The goal quantifies over every solution fGnf_{G_n}fGn​​, fμf_\mufμ​ and every equilibrium state process, and also asserts that the graph ODE solutions and the state processes exist, so it cannot be discharged vacuously. Proposition 2.12 is stated for distinct vertices: as printed, (2.17) is also claimed for u=vu = vu=v, where it fails on complete graphs of large degree; the off-diagonal case is the one the proof of Theorem 2.6 uses. Theorem 2.5 (mission I) is not restated here; a solver proves what is needed of it.

Contributions are welcome at every level: Gaussian laws of linear SDEs, spectral measures of graph matrices, ODE stability, a Gaussian Poincaré inequality, and the milestones themselves.

Selected references

  • D. Lacker, A. Soret, A case study on stochastic games on large graphs in mean field and sparse regimes, arXiv:2005.14102v2, 2021; published in Math. Oper. Res., 2022, https://doi.org/10.1287/moor.2021.1179. https://arxiv.org/abs/2005.14102
  • F. Chung, Spectral Graph Theory, CBMS Regional Conference Series in Mathematics 92, AMS, 1997. https://doi.org/10.1090/cbms/092
  • S. Boucheron, G. Lugosi, P. Massart, Concentration Inequalities: A Nonasymptotic Theory of Independence, Oxford University Press, 2013 (Theorem 3.20, Gaussian Poincaré inequality). https://doi.org/10.1093/acprof:oso/9780199535255.001.0001
  • 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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Algorithmic Game TheoryGraph TheoryProbability+1·Captain: mikedeng1

A Case Study on Stochastic Games on Large Graphs in Mean Field and Sparse Regimes III: The Mean Field Game Control Is an ε-Nash Equilibrium on Any Finite Graph, With ε_v ∝ deg(v)^(-1/2)Research Paper

Why mean field approximations on graphs need a threshold

Mean field games (MFGs) describe the limit of symmetric stochastic differential games as the number of players tends to infinity, when every player interacts with the empirical distribution of all the others. Their main practical use is the converse direction: an equilibrium of the limiting game supplies a simple, decentralized control that is an approximate Nash equilibrium of the game with finitely many players. For the complete graph, where everybody interacts with everybody, this is classical, with the standard rate O(1/n)O(1/\sqrt n)O(1/n​) (Carmona and Delarue, Probabilistic Theory of Mean Field Games, Vol. II, §6.1; Huang, Malhamé and Caines 2006, Theorem 12), as recalled on p. 10 of the paper.

Many interacting systems are not complete graphs: players see only their neighbours in a network. The question is then how dense the network must be for the mean field approximation to remain valid. Lacker and Soret (arXiv:2005.14102v2) answer it exactly for a linear-quadratic "flocking" game, where explicit computations are possible. This mission formalizes their Theorem 2.11, which applies to every finite graph, with no transitivity or regularity assumed.

Setting

Let GGG be a finite simple graph on the vertex set V={1,…,n}V=\{1,\dots,n\}V={1,…,n}; u∼vu\sim vu∼v means uuu and vvv are adjacent and deg⁡G(v)\deg_G(v)degG​(v) is the number of neighbours of vvv. Fix a horizon T>0T>0T>0, a volatility σ>0\sigma>0σ>0 and a cost weight c>0c>0c>0. Each player v∈Vv\in Vv∈V controls a real state XvX_vXv​ through

dXv(t)=αv(t,X(t)) dt+σ dWv(t),t∈[0,T],dX_v(t)=\alpha_v(t,\boldsymbol X(t))\,dt+\sigma\,dW_v(t),\qquad t\in[0,T],dXv​(t)=αv​(t,X(t))dt+σdWv​(t),t∈[0,T],

where W1,…,WnW_1,\dots,W_nW1​,…,Wn​ are independent standard Brownian motions and X=(Xu)u∈V\boldsymbol X=(X_u)_{u\in V}X=(Xu​)u∈V​. A Markovian control αv∈AG\alpha_v\in\mathcal A_Gαv​∈AG​ is a Borel function of time and the full state X(t)∈RV\boldsymbol X(t)\in\mathbb R^VX(t)∈RV, of linear growth. The cost of player vvv under a profile α=(αu)u∈V\boldsymbol\alpha=(\alpha_u)_{u\in V}α=(αu​)u∈V​ is

Jv(α)=12 E[∫0T∣αv(t,X(t))∣2 dt+c ∣Xv(T)−1deg⁡G(v)∑u∼vXu(T)∣2],J_v(\boldsymbol\alpha)=\frac12\,\mathbb E\Big[\int_0^T|\alpha_v(t,\boldsymbol X(t))|^2\,dt+c\,\Big|X_v(T)-\frac1{\deg_G(v)}\sum_{u\sim v}X_u(T)\Big|^2\Big],Jv​(α)=21​E[∫0T​∣αv​(t,X(t))∣2dt+c​Xv​(T)−degG​(v)1​u∼v∑​Xu​(T)​2],

and 12E[∫0T∣αv∣2dt+c∣Xv(T)∣2]\frac12\mathbb E[\int_0^T|\alpha_v|^2dt+c|X_v(T)|^2]21​E[∫0T​∣αv​∣2dt+c∣Xv​(T)∣2] for an isolated vertex: each player wants to end near the average of its neighbours at minimal quadratic effort. For a vector ε∈R+V\boldsymbol\varepsilon\in\mathbb R^V_+ε∈R+V​, a profile is a Markovian ε\boldsymbol\varepsilonε-Nash equilibrium if no player vvv can lower its cost by more than εv\varepsilon_vεv​ by switching unilaterally to another control β∈AG\beta\in\mathcal A_Gβ∈AG​, written (β,α−v)(\beta,\boldsymbol\alpha^{-v})(β,α−v).

The mean-field control is

αMF(t,y)=−cy1+c(T−t),αvMF(t,x)=αMF(t,xv):\alpha^{\mathrm{MF}}(t,y)=\frac{-cy}{1+c(T-t)},\qquad \alpha^{\mathrm{MF}}_v(t,\boldsymbol x)=\alpha^{\mathrm{MF}}(t,x_v):αMF(t,y)=1+c(T−t)−cy​,αvMF​(t,x)=αMF(t,xv​):

each player looks only at its own state, as if its neighbours' average were frozen at its mean.

Formalization targets

Goal: Theorem 2.11

Define ϵvG=σ2cT1+cTcT(2+cT)deg⁡G(v)\epsilon^G_v=\sigma^2\frac{cT}{1+cT}\sqrt{\frac{cT(2+cT)}{\deg_G(v)}}ϵvG​=σ21+cTcT​degG​(v)cT(2+cT)​​ if deg⁡G(v)≥1\deg_G(v)\ge1degG​(v)≥1 and ϵvG=0\epsilon^G_v=0ϵvG​=0 if deg⁡G(v)=0\deg_G(v)=0degG​(v)=0, and with the minimal degree δ(G)=min⁡vdeg⁡G(v)\delta(G)=\min_v\deg_G(v)δ(G)=minv​degG​(v),

ϵG=σ2cT1+cTcT(2+cT)1∨δ(G).\epsilon_G=\sigma^2\frac{cT}{1+cT}\sqrt{\frac{cT(2+cT)}{1\vee\delta(G)}}.ϵG​=σ21+cTcT​1∨δ(G)cT(2+cT)​​.

Then, with zero initial states, the state equation for (αvMF)v∈V(\alpha^{\mathrm{MF}}_v)_{v\in V}(αvMF​)v∈V​ has a solution, and

(αvMF)v∈V is an ϵG-Nash equilibrium and an ϵG-Nash equilibrium on G.(\alpha^{\mathrm{MF}}_v)_{v\in V}\ \text{is an } \epsilon^G\text{-Nash equilibrium and an } \epsilon_G\text{-Nash equilibrium on } G.(αvMF​)v∈V​ is an ϵG-Nash equilibrium and an ϵG​-Nash equilibrium on G.

Milestones

  1. Lemma 7.2: αMF\alpha^{\mathrm{MF}}αMF is optimal for the one-player problem min⁡12E[∫0Tβ2dt+c∣Y(T)∣2]\min\frac12\mathbb E[\int_0^T\beta^2dt+c|Y(T)|^2]min21​E[∫0T​β2dt+c∣Y(T)∣2], dY=β dt+σdWdY=\beta\,dt+\sigma dWdY=βdt+σdW, over all progressively measurable β\betaβ.
  2. Isolated vertices (p. 40): Jv(α)=inf⁡βJv(β,α−v)J_v(\boldsymbol\alpha)=\inf_\beta J_v(\beta,\boldsymbol\alpha^{-v})Jv​(α)=infβ​Jv​(β,α−v) when deg⁡G(v)=0\deg_G(v)=0degG​(v)=0.
  3. (7.7): under αMF\alpha^{\mathrm{MF}}αMF, (Xu(T))u(X_u(T))_u(Xu​(T))u​ are i.i.d. N(0,σ2T/(1+cT))N(0,\sigma^2T/(1+cT))N(0,σ2T/(1+cT)), so the neighbour average has second moment σ2T/(deg⁡G(v)(1+cT))\sigma^2T/(\deg_G(v)(1+cT))σ2T/(degG​(v)(1+cT)).
  4. Steps (1), (2), (3) (p. 41): a lower bound on Jv(β,α−v)J_v(\beta,\boldsymbol\alpha^{-v})Jv​(β,α−v), an energy bound for deviations no worse than the zero control, and the comparison with Jv(αMF)J_v(\boldsymbol\alpha^{\mathrm{MF}})Jv​(αMF).
  5. (7.5): for deg⁡G(v)≥1\deg_G(v)\ge1degG​(v)≥1 and every admissible β\betaβ, Jv(β,α−v)≥Jv(α)−ϵvGJ_v(\beta,\boldsymbol\alpha^{-v})\ge J_v(\boldsymbol\alpha)-\epsilon^G_vJv​(β,α−v)≥Jv​(α)−ϵvG​.

Significance

The result. Theorem 2.11 gives an explicit threshold for the mean field approximation on networks: along any sequence of graphs whose minimal degree diverges, the decentralized control αMF\alpha^{\mathrm{MF}}αMF is an ϵGn\epsilon_{G_n}ϵGn​​-Nash equilibrium with ϵGn→0\epsilon_{G_n}\to0ϵGn​​→0, and the vector form says more: if the average of (1∨deg⁡Gn(v))−1/2(1\vee\deg_{G_n}(v))^{-1/2}(1∨degGn​​(v))−1/2 over vertices tends to zero, the per-player errors vanish on average (the paper's (2.16)). The rate deg⁡G(v)−1/2\deg_G(v)^{-1/2}degG​(v)−1/2 quantifies how the accuracy of the approximation depends on denseness. In the same paper, transitive graphs whose degrees stay bounded lead to equilibria that do not agree with the mean field one, so a denseness condition cannot be dropped.

Formalizing it. The theorem is proved in the paper; to our knowledge no part of it is machine-checked. A formal development needs, beyond the statement, a verification argument for a one-dimensional linear-quadratic control problem with additive noise, Gaussian computations for linear SDEs driven by Brownian motion, and the comparison of costs between the equilibrium system and a system with one deviating player. The one-player result (Lemma 7.2) and the Gaussian facts of (7.7) are reusable well beyond this mission.

Difficulty

The obvious argument compares a deviating player with an isolated player and treats the neighbour average as noise independent of the deviation. Two things stand in the way. The cost of player vvv couples its terminal state with the neighbours' average through a cross term E[1deg⁡G(v)∑u∼vXu(T) Yv(T)]\mathbb E[\frac1{\deg_G(v)}\sum_{u\sim v}X_u(T)\,Y_v(T)]E[degG​(v)1​∑u∼v​Xu​(T)Yv​(T)], and the deviation β(t,Y(t))\beta(t,\boldsymbol Y(t))β(t,Y(t)) may look at the neighbours' states, so the cross term does not vanish; it has to be bounded through the size of the deviation's energy. And an arbitrary deviation has no a priori energy bound: one is available only for deviations that do at least as well as the zero control, which is why the argument passes through a (near-)optimal deviation. Lemma 7.2 itself requires a verification theorem over all progressively measurable controls, not only feedback ones.

Formalization scope

The Lean development lives in the namespace GraphLQGame.DenseApprox and uses the shared encoding of this series:

  • vertices are Fin n (the paper's {1,…,n}\{1,\dots,n\}{1,…,n} become {0,…,n−1}\{0,\dots,n-1\}{0,…,n−1}), the state space is EthierKurtz.SDEState n, and GGG is any SimpleGraph (Fin n); isolated vertices are allowed;
  • controls are Borel with linear growth on [0,T][0,T][0,T] only; their values at other times are never used, and the formula for αMF\alpha^{\mathrm{MF}}αMF outside [0,T][0,T][0,T] is evaluated with Lean's total division;
  • a solution of the state equation is a pathwise strong solution carrying its own probability space and an nnn-dimensional standard Brownian motion; costs are [0,∞][0,\infty][0,∞]-valued lower Lebesgue integrals, and the Nash inequality is required for every solution of the profile and of each deviation (faithful by strong uniqueness);
  • T,σ,c>0T,\sigma,c>0T,σ,c>0 are the standing assumptions of §2.1;
  • initial states are zero. The printed theorem does not mention X(0)X(0)X(0); the paper fixes non-random initial states that are "in many cases" zero, and the whole proof is for X(0)=0X(0)=0X(0)=0. With non-zero initial states the claim fails in general, so this is a disclosed hypothesis;
  • the goal also asserts that the state equation for αMF\alpha^{\mathrm{MF}}αMF has a solution, so the Nash property cannot hold vacuously; Lemma 7.2 is stated over every continuous adapted solution of its SDE, and Step (2) carries, as an explicit hypothesis, the comparison with the zero control that its proof uses.

A formalization in which αMF\alpha^{\mathrm{MF}}αMF is compared only with deviations depending on the player's own state, or in which the costs are Bochner integrals that vanish when not integrable, would be trivially or wrongly satisfied; both are ruled out by the encoding above.

Welcome contributions: the verification argument for Lemma 7.2, the Gaussian law of linear SDEs with additive noise, and proofs of the three steps. Related missions in this series: I (an explicit Nash equilibrium on transitive graphs) and II (large-graph limits).

Selected references

  • D. Lacker, A. Soret, A case study on stochastic games on large graphs in mean field and sparse regimes, arXiv:2005.14102v2, 2021; Math. Oper. Res. 47 (2022). https://arxiv.org/abs/2005.14102
  • R. Carmona, F. Delarue, Probabilistic Theory of Mean Field Games with Applications II, Springer, 2018. https://doi.org/10.1007/978-3-319-56436-4
  • M. Huang, R. P. Malhamé, P. E. Caines, Large population stochastic dynamic games: closed-loop McKean–Vlasov systems and the Nash certainty equivalence principle, Commun. Inf. Syst. 6 (2006), 221–252. https://doi.org/10.4310/CIS.2006.v6.n3.a5
  • H. Pham, Continuous-time Stochastic Control and Optimization with Financial Applications, Springer, 2009 (verification theorem, Theorem 3.5.2). https://doi.org/10.1007/978-3-540-89500-8
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CombinatoricsGraph Theory·Captain: mikedeng1

Stability Results on the Circumference of a Graph 1: A 2-Connected Graph with More Than (⌊c/2⌋−1)(n−c) Edges Off a Longest Cycle of Length c ≥ 10 Lies in W_{n,⌊c/2⌋,c} or (c Odd) in X_{n,c} ∪ Y_{n,c}Research Paper

Motivation

The circumference c(G)c(G)c(G) of a graph GGG is the length of a longest cycle. Extremal graph theory asks how many edges force a long cycle. The Erdős–Gallai theorem (1959) states that every nnn-vertex graph has at most c(G)(n−1)/2c(G)(n-1)/2c(G)(n−1)/2 edges. Bondy (1971) strengthened it by counting only the edges near a longest cycle: if CCC is a longest cycle of length ccc, the number of edges with at most one endpoint in CCC is at most c2(n−c)\tfrac c2(n-c)2c​(n−c), and at most ⌊c/2⌋(n−c)\lfloor c/2\rfloor (n-c)⌊c/2⌋(n−c) when GGG is 2-connected. Since V(C)V(C)V(C) spans at most (c2)\binom c2(2c​) edges, this implies the Erdős–Gallai bound.

A stability result complements an extremal one: a graph close to the extremal bound must be close in structure to the extremal graphs. Jie Ma and Bo Ning (Combinatorica, 2020; arXiv:1708.00704) proved stability versions of Kopylov's edge theorem for 2-connected graphs of given circumference and of Bondy's theorem above. This mission formalizes their stability version of Bondy's theorem, Theorem 1.12. In the paper it is also one of the two halves of the proof of the main stability theorem; the other half is a separate mission in this series.

Timeline (as recorded in §1 of the paper). Dirac (1952): every 2-connected graph has c(G)≥min⁡{2δ(G),∣V(G)∣}c(G)\ge\min\{2\delta(G),|V(G)|\}c(G)≥min{2δ(G),∣V(G)∣}. Erdős and Gallai (1959): e(G)≤c(G)(n−1)/2e(G)\le c(G)(n-1)/2e(G)≤c(G)(n−1)/2. Bondy (1971): the bound on edges with at most one endpoint on a longest cycle, and the degree theorem stated here as Theorem 2.1. Woodall (1976): e(G)≤f(n,⌊c/2⌋,c)e(G)\le f(n,\lfloor c/2\rfloor,c)e(G)≤f(n,⌊c/2⌋,c) for 2-connected GGG with circumference c≤(2n+2)/3c\le(2n+2)/3c≤(2n+2)/3. Kopylov (1977): e(G)≤max⁡{f(n,2,c),f(n,⌊c/2⌋,c)}e(G)\le\max\{f(n,2,c),f(n,\lfloor c/2\rfloor,c)\}e(G)≤max{f(n,2,c),f(n,⌊c/2⌋,c)} for 2-connected GGG with circumference c≤n−1c\le n-1c≤n−1; another proof by Fan, Lv and Wang (2004). Fan (1990): an improved version of Bondy's bound for 2-connected graphs, and average-degree bounds on long paths. Füredi, Kostochka and Verstraëte (2016): stability for Kopylov's theorem when n≥3⌊c/2⌋n\ge 3\lfloor c/2\rfloorn≥3⌊c/2⌋; Füredi, Kostochka, Luo and Verstraëte (2018): the complete stability version, with the families Xn,c\mathcal X_{n,c}Xn,c​, Yn,c\mathcal Y_{n,c}Yn,c​. Ma and Ning (2017 preprint, 2020): the results of this mission.

Setting

All graphs are finite and simple, on the vertex set {0,…,n−1}\{0,\dots,n-1\}{0,…,n−1}. A path or cycle of length kkk has kkk edges. A graph is 2-connected if it has at least three vertices, is connected, and remains connected after deleting any one vertex. A cycle CCC is a longest cycle if no cycle of GGG has more edges; V(C)V(C)V(C) is its vertex set and ccc its length.

For a longest cycle CCC, write e(G−C)+e(G−C,C)e(G-C)+e(G-C,C)e(G−C)+e(G−C,C) for the number of edges with at most one endpoint in CCC. A vertex uuu is an isolated vertex of G−CG-CG−C if u∉V(C)u\notin V(C)u∈/V(C) and every neighbour of uuu lies on CCC; dC(u)d_C(u)dC​(u) is its number of neighbours on CCC.

The extremal graphs are:

  • Wn,k,cW_{n,k,c}Wn,k,c​: a clique Kc−k+1K_{c-k+1}Kc−k+1​ together with n−(c−k+1)n-(c-k+1)n−(c−k+1) further vertices, each adjacent to the same kkk vertices of the clique and to nothing else.
  • Xn,c\mathcal X_{n,c}Xn,c​: graphs on A∪B∪XA\cup B\cup XA∪B∪X with AAA a clique of size ⌊c/2⌋\lfloor c/2\rfloor⌊c/2⌋, BBB and XXX stable, AAA completely joined to BBB, and two vertices a∈Aa\in Aa∈A, b∈Bb\in Bb∈B such that N(x)={a,b}N(x)=\{a,b\}N(x)={a,b} for all x∈Xx\in Xx∈X.
  • Yn,c\mathcal Y_{n,c}Yn,c​: graphs on A∪B∪YA\cup B\cup YA∪B∪Y with AAA a clique of size ⌊c/2⌋\lfloor c/2\rfloor⌊c/2⌋, BBB stable, AAA completely joined to BBB, G[Y]G[Y]G[Y] a star forest with at least two stars each having an edge, and two distinct a,b∈Aa,b\in Aa,b∈A such that each star SSS has exactly {a,b}\{a,b\}{a,b} as outside neighbourhood and, if ∣V(S)∣≥3|V(S)|\ge 3∣V(S)∣≥3, its leaves have degree 222 and a common neighbour in {a,b}\{a,b\}{a,b}.

G⊆WG\subseteq WG⊆W means that GGG is isomorphic to a subgraph of WWW.

Formalization targets

Goal: Theorem 1.12

Let GGG be 2-connected on nnn vertices and CCC a longest cycle of length ccc with 10≤c≤n−110\le c\le n-110≤c≤n−1. If

e(G−C)+e(G−C,C)>(⌊c2⌋−1)(n−c),e(G-C)+e(G-C,C) > \left(\left\lfloor \tfrac c2\right\rfloor-1\right)(n-c),e(G−C)+e(G−C,C)>(⌊2c​⌋−1)(n−c),

then G⊆Wn,⌊c/2⌋,cG\subseteq W_{n,\lfloor c/2\rfloor,c}G⊆Wn,⌊c/2⌋,c​, or ccc is odd and GGG is a subgraph of a member of Xn,c∪Yn,c\mathcal X_{n,c}\cup\mathcal Y_{n,c}Xn,c​∪Yn,c​.

Milestones

  1. Theorem 2.1 (Bondy): all but one vertex of degree ≥k\ge k≥k in a 2-connected graph give c(G)≥min⁡{n,2k}c(G)\ge\min\{n,2k\}c(G)≥min{n,2k}.
  2. Theorem 2.2 (Fan), first assertion: a longest (x,y)(x,y)(x,y)-path is at least as long as the average degree of the other vertices.
  3. Lemma 2.3: a 2-connected component HHH of G−CG-CG−C with average degree rrr satisfies c≥2rc\ge 2rc≥2r, with equality only for a clique attached to two common vertices of CCC.
  4. Theorem 3.2: without connectivity and for 4≤c≤n−14\le c\le n-14≤c≤n−1, the same edge condition gives c∈{6,7,9}c\in\{6,7,9\}c∈{6,7,9}, or a vertex off CCC with ⌊c/2⌋\lfloor c/2\rfloor⌊c/2⌋ neighbours on CCC, or a cycle C′C'C′ meeting CCC in at most one vertex with ∣C′∣≥2⌊c/2⌋−3|C'|\ge 2\lfloor c/2\rfloor-3∣C′∣≥2⌊c/2⌋−3 (disjoint) or ≥2⌊c/2⌋−1\ge 2\lfloor c/2\rfloor-1≥2⌊c/2⌋−1 (one common vertex).
  5. Theorem 3.1: for 2-connected GGG and 10≤c≤n−110\le c\le n-110≤c≤n−1, an isolated vertex uuu of G−CG-CG−C with dC(u)=⌊c/2⌋d_C(u)=\lfloor c/2\rfloordC​(u)=⌊c/2⌋.
  6. Lemma 3.3: such a vertex forces G⊆Wn,⌊c/2⌋,cG\subseteq W_{n,\lfloor c/2\rfloor,c}G⊆Wn,⌊c/2⌋,c​ when ccc is even, and G⊆Wn,⌊c/2⌋,cG\subseteq W_{n,\lfloor c/2\rfloor,c}G⊆Wn,⌊c/2⌋,c​ or GGG in a member of Xn,c∪Yn,c\mathcal X_{n,c}\cup\mathcal Y_{n,c}Xn,c​∪Yn,c​ when c≥9c\ge 9c≥9 is odd.

Significance

In Wn,⌊c/2⌋,cW_{n,\lfloor c/2\rfloor,c}Wn,⌊c/2⌋,c​ every one of the n−cn-cn−c vertices off a longest cycle sends ⌊c/2⌋\lfloor c/2\rfloor⌊c/2⌋ edges to the cycle, so Bondy's bound ⌊c/2⌋(n−c)\lfloor c/2\rfloor(n-c)⌊c/2⌋(n−c) is attained. Theorem 1.12 says that exceeding (⌊c/2⌋−1)(n−c)(\lfloor c/2\rfloor-1)(n-c)(⌊c/2⌋−1)(n−c) already leaves only three structures: a subgraph of Wn,⌊c/2⌋,cW_{n,\lfloor c/2\rfloor,c}Wn,⌊c/2⌋,c​, or for odd ccc a subgraph of a member of Xn,c\mathcal X_{n,c}Xn,c​ or Yn,c\mathcal Y_{n,c}Yn,c​. In the paper it is one of the two cases of the proof of the main stability theorem (Theorem 1.9): a graph with many edges and a longest cycle CCC has either many edges with at most one endpoint on CCC, handled here, or many edges inside V(C)V(C)V(C), handled by the closure argument of the companion mission.

The result is proved in the paper; none of it, nor Bondy's or Fan's theorems, is formalized on the platform or in Mathlib. The mission produces machine-checked statements of the goal, of the cited tools (Bondy's Theorem 2.1, Fan's Theorem 2.2, Lemma 2.3), and of the steps Theorems 3.1, 3.2 and Lemma 3.3, together with reusable definitions of 2-connectivity, longest cycles and the extremal families.

Difficulty

The obvious approach counts edges at the vertices off CCC: each such vertex has at most ⌊c/2⌋\lfloor c/2\rfloor⌊c/2⌋ neighbours on CCC, since otherwise two consecutive cycle vertices would let the cycle be extended. This bound is far from enough. The edge count also includes edges between vertices off CCC, and components of G−CG-CG−C can be large, 2-connected, and attached to CCC in complicated ways. The bound (⌊c/2⌋−1)(n−c)(\lfloor c/2\rfloor-1)(n-c)(⌊c/2⌋−1)(n−c) has to be beaten by every such configuration at once, and Theorem 3.2 states exceptional small cycle lengths c∈{6,7,9}c\in\{6,7,9\}c∈{6,7,9} for which the analysis does not close. A second difficulty is the passage from one vertex of degree ⌊c/2⌋\lfloor c/2\rfloor⌊c/2⌋ to a global description of GGG: in the odd case, the structure of every component of G−CG-CG−C has to be determined, which is where the families Xn,c\mathcal X_{n,c}Xn,c​ and Yn,c\mathcal Y_{n,c}Yn,c​ appear.

Formalization scope

Graphs are SimpleGraph (Fin n) with decidable adjacency. A cycle is a closed walk C : G.Walk u u with C.IsCycle; its length is C.length and its vertex set C.support.toFinset. "Longest cycle" is the predicate that every cycle of GGG is at most as long as CCC; no supremum of cycle lengths is used. 2-connectivity is: at least three vertices, connected, and connected after deleting any one vertex. It is stated for an arbitrary finite vertex type so that it applies to the induced subgraph G[H]G[H]G[H] in Lemma 2.3. The edge count off CCC is the number of edges with an endpoint outside V(C)V(C)V(C), and ⌊c/2⌋\lfloor c/2\rfloor⌊c/2⌋ is natural-number division; under the stated bounds every natural-number subtraction is exact.

Wn,k,cW_{n,k,c}Wn,k,c​ is defined on fixed labels (clique {0,…,c−k}\{0,\dots,c-k\}{0,…,c−k}, hubs {0,…,k−1}\{0,\dots,k-1\}{0,…,k−1}), and "G⊆WG\subseteq WG⊆W" is a graph embedding G ⊑ W. Membership in Xn,c\mathcal X_{n,c}Xn,c​ and Yn,c\mathcal Y_{n,c}Yn,c​ are predicates on labelled graphs, closed under relabelling, and "GGG is a subgraph of a member" is G ≤ H for some member HHH. No hypothesis is added to any statement. Fan's Theorem 2.2 is stated without its equality characterization.

Trivializing formalizations are ruled out explicitly: the alternative "ccc is odd and …" is a conjunction, never an implication; the circumference is never a junk supremum; containment in WWW is up to isomorphism, never ≤ on fixed labels; and 2-connectivity excludes K2K_2K2​ and disconnected graphs.

The definitions are reusable for any work on circumference, longest cycles and Bondy–Erdős–Gallai-type problems. Contributions of proofs of the cited tools (Bondy's and Fan's theorems) are especially welcome, as is a proof of Erdős–Gallai's edge theorem, which the proof of Theorem 3.2 uses and which is posed elsewhere on the platform.

Selected references

  • J. Ma and B. Ning, Stability results on the circumference of a graph, Combinatorica 40 (2020); arXiv:1708.00704v2. https://arxiv.org/abs/1708.00704 , https://doi.org/10.1007/s00493-019-3843-4
  • J. A. Bondy, Large cycles in graphs, Discrete Mathematics 1 (1971/72), no. 2, 121–132.
  • G. Fan, Long cycles and the codiameter of a graph, I, Journal of Combinatorial Theory, Series B 49 (1990) 151–180.
  • P. Erdős and T. Gallai, On maximal paths and circuits of graphs, Acta Mathematica Academiae Scientiarum Hungaricae 10 (1959) 337–356.
  • G. Fan, X. Lv, P. Wang, Cycles in 2-connected graphs, Journal of Combinatorial Theory, Series B 92 (2004) 379–394.
  • Z. Füredi, A. Kostochka, J. Verstraëte, Stability in the Erdős–Gallai theorems on cycles and paths, Journal of Combinatorial Theory, Series B 121 (2016) 197–228.
  • Z. Füredi, A. Kostochka, R. Luo, J. Verstraëte, Stability in the Erdős–Gallai theorem on cycles and paths, II, Discrete Mathematics 341 (2018) 1253–1263.
  • G. N. Kopylov, Maximal paths and cycles in a graph, Soviet Mathematics Doklady 18 (1977) 593–596.
  • D. R. Woodall, Maximal circuits of graphs I, Acta Mathematica Academiae Scientiarum Hungaricae 28 (1976) 77–80.
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Operations ResearchOptimal TransportOptimization+1·Captain: mikedeng1

Distributionally Robust Stochastic Optimization with Wasserstein Distance: If the Growth Rate κ of Ψ Is Finite, sup{E_μ[Ψ] : W_p(μ, ν) ≤ θ} Equals Its One-Dimensional Dual and Is FiniteResearch Paper

Motivation

Distributionally robust stochastic optimization (DRSO) chooses a decision xxx to minimize the worst expected loss sup⁡μ∈MEμ[Ψ(x,ξ)]\sup_{\mu\in\mathfrak M}\mathbb E_\mu[\Psi(x,\xi)]supμ∈M​Eμ​[Ψ(x,ξ)] over an ambiguity set M\mathfrak MM of probability distributions, instead of the expectation under one estimated distribution. When M\mathfrak MM is a ball around a nominal distribution ν\nuν (often the empirical distribution of data) in the Wasserstein distance, the set contains distributions with supports different from that of ν\nuν, and the worst case is driven by how far mass can be moved and how fast the loss grows along the way. This makes Wasserstein balls a standard choice in data-driven optimization, statistical learning and operations research.

The inner problem, a supremum over an infinite-dimensional set of measures, is not directly computable. Gao and Kleywegt (arXiv:1604.02199v3) show that it equals a minimization over a single scalar multiplier, for an arbitrary Polish space and nominal distribution and a merely measurable loss.

Timeline. Esfahani and Kuhn (2018, doi:10.1007/s10107-017-1172-1) proved a strong duality for p=1p=1p=1 and empirical ν\nuν on Rm\mathbb R^mRm, giving finite convex reformulations for piecewise-affine losses. Blanchet and Murthy (2019, doi:10.1287/moor.2018.0936) proved duality for general optimal transport costs on Polish spaces under upper semicontinuity of the loss, with a dual over pairs (λ,φ)(\lambda,\varphi)(λ,φ). Gao and Kleywegt's result, first posted in 2016 and published in Mathematics of Operations Research (2023, doi:10.1287/moor.2022.1275), covers every order p∈[1,∞)p\in[1,\infty)p∈[1,∞), every nominal ν\nuν and every measurable loss with finite growth rate, with a dual in one variable.

Setting

Let (Ξ,d)(\Xi,d)(Ξ,d) be a Polish space (complete, separable metric) with its Borel σ\sigmaσ-algebra, P(Ξ)\mathcal P(\Xi)P(Ξ) the Borel probability measures, p∈[1,∞)p\in[1,\infty)p∈[1,∞) and θ>0\theta>0θ>0. The decision variable is suppressed: Ψ:Ξ→R\Psi:\Xi\to\mathbb RΨ:Ξ→R is a Borel measurable loss with Ψ∈L1(ν)\Psi\in L^1(\nu)Ψ∈L1(ν) for a fixed nominal distribution ν∈P(Ξ)\nu\in\mathcal P(\Xi)ν∈P(Ξ).

The Wasserstein distance of order ppp is given by

Wpp(μ,ν)=inf⁡{∫Ξ×Ξdp(ξ,ζ) γ(dξ,dζ): γ∈P(Ξ×Ξ), π#1γ=μ, π#2γ=ν}.W_p^p(\mu,\nu)=\inf\Big\{\int_{\Xi\times\Xi}d^p(\xi,\zeta)\,\gamma(d\xi,d\zeta):\ \gamma\in\mathcal P(\Xi\times\Xi),\ \pi^1_\#\gamma=\mu,\ \pi^2_\#\gamma=\nu\Big\}.Wpp​(μ,ν)=inf{∫Ξ×Ξ​dp(ξ,ζ)γ(dξ,dζ): γ∈P(Ξ×Ξ), π#1​γ=μ, π#2​γ=ν}.

The primal value is the worst-case expectation over the Wasserstein ball,

vP=sup⁡μ∈P(Ξ){∫ΞΨ dμ: Wp(μ,ν)≤θ}.v_P=\sup_{\mu\in\mathcal P(\Xi)}\Big\{\int_\Xi\Psi\,d\mu:\ W_p(\mu,\nu)\le\theta\Big\}.vP​=μ∈P(Ξ)sup​{∫Ξ​Ψdμ: Wp​(μ,ν)≤θ}.

The regularization operator is Φ(λ,ζ)=inf⁡ξ∈Ξ{λdp(ξ,ζ)−Ψ(ξ)}∈R∪{−∞}\Phi(\lambda,\zeta)=\inf_{\xi\in\Xi}\{\lambda d^p(\xi,\zeta)-\Psi(\xi)\}\in\mathbb R\cup\{-\infty\}Φ(λ,ζ)=infξ∈Ξ​{λdp(ξ,ζ)−Ψ(ξ)}∈R∪{−∞}, the dual objective is h(λ)=λθp−∫ΞΦ(λ,ζ) ν(dζ)h(\lambda)=\lambda\theta^p-\int_\Xi\Phi(\lambda,\zeta)\,\nu(d\zeta)h(λ)=λθp−∫Ξ​Φ(λ,ζ)ν(dζ), and the dual value is vD=inf⁡λ≥0h(λ)v_D=\inf_{\lambda\ge0}h(\lambda)vD​=infλ≥0​h(λ). The growth rate of Ψ\PsiΨ is

κ=inf⁡{λ≥0:∫ΞΦ(λ,ζ) ν(dζ)>−∞}∈[0,∞],\kappa=\inf\Big\{\lambda\ge0:\int_\Xi\Phi(\lambda,\zeta)\,\nu(d\zeta)>-\infty\Big\}\in[0,\infty],κ=inf{λ≥0:∫Ξ​Φ(λ,ζ)ν(dζ)>−∞}∈[0,∞],

with κ=∞\kappa=\inftyκ=∞ if no λ\lambdaλ qualifies. The lemmas also use the near-optimal distances D‾(λ,ζ)\overline D(\lambda,\zeta)D(λ,ζ) and D‾(λ,ζ)\underline D(\lambda,\zeta)D​(λ,ζ), the limits as ε↓0\varepsilon\downarrow0ε↓0 of the largest and smallest dp(ξ,ζ)d^p(\xi,\zeta)dp(ξ,ζ) over ε\varepsilonε-minimizers ξ\xiξ of λdp(⋅,ζ)−Ψ\lambda d^p(\cdot,\zeta)-\Psiλdp(⋅,ζ)−Ψ.

In Lean these objects are DRSOWass.Duality.wassPow, vP, Phi, dualObj, vD, growthRate, DUpper, DLower.

Formalization targets

Goal: Theorem 1 (p. 17)

If κ<∞\kappa<\inftyκ<∞, then

vP=vD<∞.v_P=v_D<\infty.vP​=vD​<∞.

This is the printed theorem: an equality of values together with finiteness. It fixes no constant and needs no regularity of Ψ\PsiΨ beyond measurability and integrability.

Milestones

  1. Proposition 1, weak duality vP≤vDv_P\le v_DvP​≤vD​ (no growth condition).
  2. Lemma 3(i), (ii), (v): ν\nuν-measurability of Φ(λ,⋅)\Phi(\lambda,\cdot)Φ(λ,⋅), D‾\overline DD, D‾\underline DD​, D‾0\overline D_0D0​, D‾0\underline D_0D​0​, and ν\nuν-measurable selections of near-optimal and far points.
  3. Lemma 4(i)–(iii): monotonicity, upper semicontinuity and concavity of Φ(⋅,ζ)\Phi(\cdot,\zeta)Φ(⋅,ζ), the bound (λ2−λ1)D‾(λ2,ζ)≤−Ψ(ζ)−Φ(λ1,ζ)(\lambda_2-\lambda_1)\overline D(\lambda_2,\zeta)\le-\Psi(\zeta)-\Phi(\lambda_1,\zeta)(λ2​−λ1​)D(λ2​,ζ)≤−Ψ(ζ)−Φ(λ1​,ζ), and one-sided derivative bounds.
  4. Lemma 5: hhh is ∞\infty∞ on [0,κ)[0,\kappa)[0,κ), finite on (κ,∞)(\kappa,\infty)(κ,∞), convex, lower semicontinuous, coercive, and has a minimizer λ∗∈[κ,∞)\lambda^*\in[\kappa,\infty)λ∗∈[κ,∞).
  5. Lemmas 6 and 7: explicit ε\varepsilonε-optimal distributions in the ball, built from push-forwards of ν\nuν, in the cases λ∗>κ\lambda^*>\kappaλ∗>κ, λ∗=κ=0\lambda^*=\kappa=0λ∗=κ=0 and λ∗=κ>0\lambda^*=\kappa>0λ∗=κ>0.

Significance

The result. Strong duality turns the worst-case expectation over a Wasserstein ball into a convex problem in one scalar, min⁡λ≥0{λθp−∫Φ(λ,ζ) ν(dζ)}\min_{\lambda\ge0}\{\lambda\theta^p-\int\Phi(\lambda,\zeta)\,\nu(d\zeta)\}minλ≥0​{λθp−∫Φ(λ,ζ)ν(dζ)}, where Φ\PhiΦ is a Moreau–Yosida-type regularization of −Ψ-\Psi−Ψ. For finite-supported ν\nuν this yields finite-dimensional reformulations of DRSO; the paper derives from it the structure of worst-case distributions (Corollaries 1 and 2) and applications to two-stage problems, point processes and Gaussian nominal distributions. The growth rate κ\kappaκ separates the finite case (this theorem) from the case vP=∞v_P=\inftyvP​=∞ (Proposition 2).

Formalizing it. The theorem is proved in the paper; to the best of current knowledge none of it is machine-checked. The mission produces a formal statement of the duality on general Polish spaces, together with reusable pieces: extended-valued integrals, the regularization operator and its one-sided derivatives, measurable selection on Polish spaces, and push-forward constructions of near-optimal measures. Formal proofs of Lemma 3 also give measurable-selection tools that Mathlib does not yet provide in this form.

Difficulty

Weak duality is a one-line Lagrangian argument. The difficulty is attainment from the primal side: one must construct, for every ε>0\varepsilon>0ε>0, a distribution in the ball whose expectation is within ε\varepsilonε of vDv_DvD​. A worst-case distribution need not exist (when λ∗=κ>0\lambda^*=\kappa>0λ∗=κ>0 mass escapes to infinity), so a compactness argument on P(Ξ)\mathcal P(\Xi)P(Ξ) fails; and Ψ\PsiΨ is only measurable, so the infimum defining Φ(λ,ζ)\Phi(\lambda,\zeta)Φ(λ,ζ) cannot be reduced to a countable one, and the measurability of Φ(λ,⋅)\Phi(\lambda,\cdot)Φ(λ,⋅) and of near-optimal transport maps needs projection and measurable-selection theorems for analytic sets. The case analysis on whether the dual minimizer exceeds κ\kappaκ is forced by the possible non-differentiability of hhh at κ\kappaκ.

Formalization scope

  • Ξ\XiΞ carries MetricSpace, CompleteSpace, SecondCountableTopology and BorelSpace instances; ν\nuν is a probability measure; dpd^pdp is dist ξ ζ ^ p with real p≥1p\ge1p≥1.
  • Ψ\PsiΨ is assumed Borel measurable in addition to Ψ∈L1(ν)\Psi\in L^1(\nu)Ψ∈L1(ν); the paper's p. 5 states the theorem for a measurable Ψ\PsiΨ, and ∫Ψ dμ\int\Psi\,d\mu∫Ψdμ for μ≠ν\mu\ne\nuμ=ν requires it.
  • WppW_p^pWpp​ is the published RWPI.SqrtLasso.transportCost with cost dpd^pdp, an infimum over probability couplings in [0,∞][0,\infty][0,∞]; Wp(μ,ν)≤θW_p(\mu,\nu)\le\thetaWp​(μ,ν)≤θ is written Wpp(μ,ν)≤θpW_p^p(\mu,\nu)\le\theta^pWpp​(μ,ν)≤θp.
  • Integrals that may be infinite are the published ModelRiskOT.Duality.extIntegral, ∫φ+−∫φ−\int\varphi^+-\int\varphi^-∫φ+−∫φ− in [−∞,∞][-\infty,\infty][−∞,∞] (with ∞−∞=−∞\infty-\infty=-\infty∞−∞=−∞). Φ\PhiΦ, hhh, vPv_PvP​, vDv_DvD​ are EReal-valued; κ\kappaκ, D‾\overline DD, D‾\underline DD​ are ENNReal-valued, so κ=∞\kappa=\inftyκ=∞ is representable and the empty infimum is ∞\infty∞.
  • lim sup⁡ε↓0\limsup_{\varepsilon\downarrow0}limsupε↓0​ and lim inf⁡ε↓0\liminf_{\varepsilon\downarrow0}liminfε↓0​ in D‾\overline DD, D‾\underline DD​ are written as the monotone infimum and supremum over ε>0\varepsilon>0ε>0. ν\nuν-measurability is null-measurability for functions and almost-everywhere measurability for maps Ξ→Ξ\Xi\to\XiΞ→Ξ.
  • Repaired or adjusted statements: Lemma 4(i)'s sup inequality is stated for ε>0\varepsilon>0ε>0 (the printed ε=0\varepsilon=0ε=0 case fails when an arg min is empty); in Lemma 6, (7)'s weights p1,p2p_1,p_2p1​,p2​ are read as p1ε,p2εp_1^\varepsilon,p_2^\varepsilonp1ε​,p2ε​; Lemma 5(v) carries κ<∞\kappa<\inftyκ<∞; Lemma 4(iii)'s right derivative is a limit in (−∞,∞](-\infty,\infty](−∞,∞].
  • A trivializing formalization is ruled out: integrals are not Bochner integrals (which would give a non-integrable μ\muμ the value 000), κ\kappaκ is not a real infimum (which would give 000 when no λ\lambdaλ qualifies), and the supremum in vPv_PvP​ ranges over probability measures in the ball only, which is nonempty because it contains ν\nuν.

A complete development needs couplings and gluing in Mathlib's measure theory, the measurable projection theorem and a measurable selection theorem on Polish spaces, and one-sided derivatives of concave extended-valued functions; the first three are reusable well beyond this mission. Proofs of any milestone, alternative proofs of the goal (e.g. through the Blanchet–Murthy dual), and the companion result Proposition 2 (κ=∞⇒vP=vD=∞\kappa=\infty\Rightarrow v_P=v_D=\inftyκ=∞⇒vP​=vD​=∞) are welcome.

Selected references

  • R. Gao, A. J. Kleywegt, Distributionally Robust Stochastic Optimization with Wasserstein Distance, arXiv:1604.02199v3, 2022; Mathematics of Operations Research, 2023. https://arxiv.org/abs/1604.02199
  • P. Mohajerin Esfahani, D. Kuhn, Data-driven distributionally robust optimization using the Wasserstein metric: performance guarantees and tractable reformulations, Mathematical Programming 171, 2018. https://doi.org/10.1007/s10107-017-1172-1
  • J. Blanchet, K. Murthy, Quantifying distributional model risk via optimal transport, Mathematics of Operations Research 44(2), 2019. https://doi.org/10.1287/moor.2018.0936
  • C. Villani, Optimal Transport: Old and New, Springer, 2009. https://doi.org/10.1007/978-3-540-71050-9
16 thms1 active userReviewed
Operations ResearchOptimizationProbability·Captain: mikedeng1

Trade Credit, Risk Sharing, and Inventory Financing Portfolios: The Optimal Contract Always Uses Trade Credit, with Net Terms for Costless Default or High Cash and Two-Part Terms for Low CashResearch Paper

Why trade credit terms matter

Most business-to-business sales are not paid in cash on delivery. The supplier lets the buyer pay later, which is trade credit, and often offers a discount for paying early. In the classic "2/10 net 30" the buyer gets 2% off for paying within 10 days and otherwise owes the full price in 30 days. Trade credit is a major source of short-term finance for firms. Empirical work documents both forms of contract: net terms, with one price and no discount, and two-part terms, with an early-payment discount. The discounts are large, and they vary a lot from one buyer to another (Petersen and Rajan 1997; Klapper, Laeven and Rajan 2012). The implied interest rate on a forgone discount is often far above a bank loan's. This raises two questions: why do cash-poor buyers use trade credit at all, and when should a supplier offer a discount?

Yang and Birge (Management Science 2018) answer this in a supplier–retailer model with a financially constrained retailer, who can finance inventory with a bank loan, with trade credit, or with both. Their answer is risk sharing. Trade credit is repaid out of realized sales, so the supplier bears part of the demand risk. She can therefore induce a larger order than a price-only contract does. The model builds on the selling-to-the-newsvendor model of Lariviere and Porteus (2001), and it complements the supplier-versus-bank analysis of Kouvelis and Zhao (2012). This mission formalizes the paper's main result on the structure of the optimal contract.

The model

A retailer buys a single good from a supplier at unit cost ccc and sells it at unit price p=1p=1p=1. Demand is random with density fff on [0,∞)[0,\infty)[0,∞). Its distribution function is F(x)=∫0xfF(x)=\int_0^x fF(x)=∫0x​f, the complementary distribution function is Fˉ=1−F\bar F=1-FFˉ=1−F, the failure rate is h=f/Fˉh=f/\bar Fh=f/Fˉ, and the generalized failure rate is g(x)=x h(x)g(x)=x\,h(x)g(x)=xh(x). Demand has an increasing failure rate (IFR). The retailer has cash K>0K>0K>0.

The supplier offers a cash price wcw_cwc​ and a credit price wtw_twt​, with c≤wc≤wt≤1c\le w_c\le w_t\le 1c≤wc​≤wt​≤1. The early-payment discount is dt=1−wc/wtd_t=1-w_c/w_tdt​=1−wc​/wt​. If the retailer's cash does not cover his cash purchases, he borrows from a competitive bank. The bank loan is senior to trade credit. A bank and a supplier recovering a defaulted claim lose fractions αb\alpha_bαb​ and αt\alpha_tαt​ of what they recover, with αb,αt∈[0,1]\alpha_b,\alpha_t\in[0,1]αb​,αt​∈[0,1].

Default is described by two thresholds. The bank-loan default threshold θb\theta_bθb​ is the demand below which the bank is not repaid in full, and it equals the amount owed to the bank. The trade-credit default threshold θt≥θb\theta_t\ge\theta_bθt​≥θb​ is the demand below which the supplier is not repaid in full. The retailer uses a bank loan iff θb>0\theta_b>0θb​>0, and uses trade credit iff θt>θb\theta_t>\theta_bθt​>θb​.

The paper shows (p. 13) that the supplier's problem can be written in the thresholds alone. Let

F^b(x)=Fˉ(x)[1−αbg(x)],C(θ)=K+∫0θF^bF^b(θ)−θ,\hat F_b(x)=\bar F(x)[1-\alpha_b g(x)],\qquad C(\theta)=\frac{K+\int_0^\theta\hat F_b}{\hat F_b(\theta)}-\theta,F^b​(x)=Fˉ(x)[1−αb​g(x)],C(θ)=F^b​(θ)K+∫0θ​F^b​​−θ, Q(θb,θt)=min⁡{q≥0: qFˉ(q)=[θt+C(θb)]Fˉ(θt)}.Q(\theta_b,\theta_t)=\min\{q\ge0:\ q\bar F(q)=[\theta_t+C(\theta_b)]\bar F(\theta_t)\}.Q(θb​,θt​)=min{q≥0: qFˉ(q)=[θt​+C(θb​)]Fˉ(θt​)}.

The retailer orders QQQ, the prices are wt=Fˉ(Q)/Fˉ(θt)w_t=\bar F(Q)/\bar F(\theta_t)wt​=Fˉ(Q)/Fˉ(θt​) and wc=F^b(θb)wtw_c=\hat F_b(\theta_b)w_twc​=F^b​(θb​)wt​, and the discount is dt=1−F^b(θb)d_t=1-\hat F_b(\theta_b)dt​=1−F^b​(θb​). The supplier's expected profit is

Πs=K+∫0θtFˉ(x) dx−c Q(θb,θt)−[αb∫0θbx dF(x)+αt∫θbθt(x−θb) dF(x)].\Pi_s=K+\int_0^{\theta_t}\bar F(x)\,dx-c\,Q(\theta_b,\theta_t)-\Big[\alpha_b\int_0^{\theta_b}x\,dF(x)+\alpha_t\int_{\theta_b}^{\theta_t}(x-\theta_b)\,dF(x)\Big].Πs​=K+∫0θt​​Fˉ(x)dx−cQ(θb​,θt​)−[αb​∫0θb​​xdF(x)+αt​∫θb​θt​​(x−θb​)dF(x)].

She maximizes Πs\Pi_sΠs​ over a domain Θ\ThetaΘ of thresholds. A maximizer is an optimal trade credit contract. Net terms correspond to θb∗=0\theta_b^*=0θb∗​=0, which is dt∗=0d_t^*=0dt∗​=0. Two-part terms correspond to θb∗>0\theta_b^*>0θb∗​>0.

Formalization targets

Goal: Proposition 3 (p. 15)

For every optimal contract (θb∗,θt∗)(\theta_b^*,\theta_t^*)(θb∗​,θt∗​):

θt∗>0 ⟹ θb∗<θt∗(trade credit is always used).\theta_t^*>0\ \Longrightarrow\ \theta_b^*<\theta_t^*\qquad(\text{trade credit is always used}).θt∗​>0 ⟹ θb∗​<θt∗​(trade credit is always used).

If αt=0\alpha_t=0αt​=0, or if KKK is sufficiently large, then θb∗=0\theta_b^*=0θb∗​=0 and dt∗=0d_t^*=0dt∗​=0 (net terms, no bank loan). If αt>0\alpha_t>0αt​>0 and KKK is sufficiently small, then

0<θb∗<θt∗,dt∗>0(two-part terms, both bank loan and trade credit).0<\theta_b^*<\theta_t^*,\qquad d_t^*>0\qquad(\text{two-part terms, both bank loan and trade credit}).0<θb∗​<θt∗​,dt∗​>0(two-part terms, both bank loan and trade credit).

"Sufficiently large" and "sufficiently small" are existential thresholds on KKK that depend on the data (f,c,αb,αt)(f,c,\alpha_b,\alpha_t)(f,c,αb​,αt​), not on the contract.

Milestones

They are listed in the order the proof uses them:

  1. Lemma C.4: CCC is increasing, and convex when αb=0\alpha_b=0αb​=0.
  2. Corollary 3: QQQ increases in θb\theta_bθb​ and in θt\theta_tθt​.
  3. Lemma C.8: at αb=0\alpha_b=0αb​=0, Πs\Pi_sΠs​ is concave in θb\theta_bθb​.
  4. Lemma C.7: QQQ increases in αb\alpha_bαb​ and KKK.
  5. Lemma C.9: Πs\Pi_sΠs​ is concave in θt\theta_tθt​.
  6. Proposition 6, first sentence: Πs∗\Pi_s^*Πs∗​ decreases in αb\alpha_bαb​ and αt\alpha_tαt​.

Significance

Proposition 3 is the paper's prediction about inventory financing portfolios. Once the supplier sets the terms, a retailer who needs external financing always uses trade credit. Early-payment discounts appear only when supplier default is costly and the retailer is cash-poor. A discount is then the supplier's way of moving part of the financing to the bank. The paper uses this to explain why discounts go to small, risky buyers, as observed by Klapper et al. (2012). The comparative statics of §5 (Propositions 4–6) are built on the same reduced problem.

The result is proved on paper but has not been formalized. The appendix lemmas it rests on (C.4, C.7, C.8, C.9) are stated without proof ("available upon request"). A machine-checked development would therefore settle whether these lemmas hold on the domain where the paper uses them. It would also produce a reusable library: IFR demand with failure rates, the bank-loan pricing kernel F^b\hat F_bF^b​, and the implicit order quantity QQQ.

Difficulty

The order quantity QQQ is defined implicitly, as the smaller root of a unimodal equation, and the paper's arguments differentiate through it with the implicit function theorem. Every derivative of Πs\Pi_sΠs​ therefore involves 1/(Fˉ(Q)[1−g(Q)])1/(\bar F(Q)[1-g(Q)])1/(Fˉ(Q)[1−g(Q)]), which blows up at the edge of Θ\ThetaΘ where Q=g−1(1)Q=g^{-1}(1)Q=g−1(1). The density is only assumed continuous, so F^b\hat F_bF^b​ and CCC need not be differentiable when αb>0\alpha_b>0αb​>0. Monotonicity and concavity have to be argued from the integral forms, or under a smoothness assumption the paper does not state.

The obvious argument for "sufficiently large KKK" also fails. It perturbs the optimum at KKK just below M∗=g−1(1)Fˉ(g−1(1))M^*=g^{-1}(1)\bar F(g^{-1}(1))M∗=g−1(1)Fˉ(g−1(1)), but there the domain shrinks to a sliver near θt=0\theta_t=0θt​=0, and the derivative of Πs\Pi_sΠs​ in θt\theta_tθt​ at θt=0\theta_t=0θt​=0 can be negative. For exponential demand it tends to −∞-\infty−∞ as K→M∗K\to M^*K→M∗. The proof's claim that θt∗>0\theta_t^*>0θt∗​>0 there is not part of the theorem. Part 1 for general αb\alpha_bαb​ is reduced to αb=0\alpha_b=0αb​=0 through Proposition 6, which requires comparing optima over domains that themselves depend on αb\alpha_bαb​.

Formalization scope

All objects live in TradeCredit.Terms.Model.

Demand. Demand is a density f:R→Rf:\mathbb R\to\mathbb Rf:R→R that is continuous on [0,∞)[0,\infty)[0,∞), positive on [0,∞)[0,\infty)[0,∞), zero on (−∞,0)(-\infty,0)(−∞,0), integrable with total mass 111, and has a weakly increasing failure rate on [0,∞)[0,\infty)[0,∞). FFF is the interval integral of fff from 000. The normalizations are p=1p=1p=1 and s=0s=0s=0. The parameters satisfy 0<c<10<c<10<c<1, αb,αt∈[0,1]\alpha_b,\alpha_t\in[0,1]αb​,αt​∈[0,1] and K>0K>0K>0.

Domain. Θ\ThetaΘ is the printed set of Corollary 3 (θt≥θb≥0\theta_t\ge\theta_b\ge0θt​≥θb​≥0 and [θt+C(θb)]Fˉ(θt)≤M∗[\theta_t+C(\theta_b)]\bar F(\theta_t)\le M^*[θt​+C(θb​)]Fˉ(θt​)≤M∗) plus two pinned constraints: θt≤Q(θb,θt)\theta_t\le Q(\theta_b,\theta_t)θt​≤Q(θb​,θt​) (that is, wt≤1w_t\le1wt​≤1) and c≤wcc\le w_cc≤wc​. These are the image under (11) of §3.1's c≤wc≤wt≤1c\le w_c\le w_t\le 1c≤wc​≤wt​≤1, which the printed Θ\ThetaΘ omits.

Statements. QQQ is the infimum of the nonnegative roots. "The optimal contract" means every maximizer of Πs\Pi_sΠs​ on Θ\ThetaΘ. Existence of a maximizer is not asserted; the paper does not prove it. Monotonicity is weak, and concavity is Mathlib's ConcaveOn on the sections of Θ\ThetaΘ. Proposition 6 is stated by comparing attained values with Πs∗=sup⁡ΘΠs\Pi_s^*=\sup_\Theta\Pi_sΠs∗​=supΘ​Πs​.

Not in scope. The retailer's best response (Proposition 1) and the bijection between thresholds and contracts are not formalized. The goal is about the paper's own reduced problem. Lemma 1's first-order conditions are not a milestone: as printed they fail at a corner optimum θb∗=θt∗=0\theta_b^*=\theta_t^*=0θb∗​=θt∗​=0, and they need C′C'C′, which is not defined under a merely continuous density.

Ruling out trivialization. The large-KKK clause quantifies over K∈[K‾,M∗)K\in[\underline K,M^*)K∈[K​,M∗) with K‾<M∗\underline K<M^*K​<M∗. For K≥M∗K\ge M^*K≥M∗ the domain Θ\ThetaΘ has no point with θt>0\theta_t>0θt​>0 and every "for every optimal contract" statement holds vacuously, so a large-KKK clause that reached only those values would be empty.

Welcome contributions. Lemmas on IFR densities (positivity of Fˉ\bar FFˉ, finiteness of the mean, monotonicity of ggg and existence of g−1(1)g^{-1}(1)g−1(1)), the root structure of qFˉ(q)q\bar F(q)qFˉ(q), and boundedness of Πs\Pi_sΠs​ on Θ\ThetaΘ are reusable beyond this paper.

Source. The source PDF is the authors' accepted manuscript (LBS Research Online, eprint 801). All page numbers are the manuscript's.

Selected references

  • S. A. Yang, J. R. Birge, Trade Credit, Risk Sharing, and Inventory Financing Portfolios, Management Science 64(8), 2018. https://doi.org/10.1287/mnsc.2017.2799
  • M. A. Lariviere, E. L. Porteus, Selling to the Newsvendor: An Analysis of Price-Only Contracts, Manufacturing & Service Operations Management 3(4), 2001. https://doi.org/10.1287/msom.3.4.293.9971
  • P. Kouvelis, W. Zhao, Financing the Newsvendor: Supplier vs. Bank, and the Structure of Optimal Trade Credit Contracts, Operations Research 60(3), 2012. https://doi.org/10.1287/opre.1120.1040
  • M. A. Petersen, R. G. Rajan, Trade Credit: Theories and Evidence, Review of Financial Studies 10(3), 1997. https://doi.org/10.1093/rfs/10.3.661
  • L. Klapper, L. Laeven, R. Rajan, Trade Credit Contracts, Review of Financial Studies 25(3), 2012. https://doi.org/10.1093/rfs/hhr122
8 thms1 active userReviewed
Convex OptimizationOptimization·Captain: mikedeng1

DC Programming and DCA: Thirty Years of Developments: For f = g − h with g, h ∈ Γ₀(ℝⁿ), at x ∈ ri(dom g) ∩ ri(dom h) d-Stationarity of f Is Equivalent to Strong Criticality ∅ ≠ ∂h(x) ⊂ ∂g(x)Research Paper

Motivation

DC programming is the minimization of a function f=g−hf = g - hf=g−h that is a difference of two convex functions. The class contains every C2C^2C2 function on a compact convex set and most nonconvex models of sparse learning, clustering, combinatorial relaxations and robust optimization, and its standard method, the DC Algorithm (DCA), replaces hhh by its affine minorant at the current iterate and solves a convex program at each step. DCA was introduced by Pham Dinh Tao in 1985 and developed jointly with Le Thi Hoai An from 1994 on (Pham Dinh & Le Thi 1998); the survey of Le Thi & Pham Dinh 2018 collects thirty years of that work.

DCA is guaranteed to reach critical or strongly critical points, notions that depend on the chosen decomposition g−hg - hg−h, while a decomposition-free notion, directional (d-)stationarity of fff itself, is what a user of a nonconvex model usually wants. Ahn, Pang & Xin 2017 warned that DC criticality can be much weaker than d-stationarity. Theorem 1 of the 2018 survey (p. 9) states when the two coincide. Its proof is omitted in the paper ("can be easily deduced … It is omitted here").

Setting

Let X=RnX = \mathbb R^nX=Rn with the canonical inner product ⟨⋅,⋅⟩\langle\cdot,\cdot\rangle⟨⋅,⋅⟩. Functions take values in R∪{±∞}\mathbb R\cup\{\pm\infty\}R∪{±∞}. The effective domain of φ\varphiφ is dom⁡φ={x:φ(x)<+∞}\operatorname{dom}\varphi = \{x : \varphi(x) < +\infty\}domφ={x:φ(x)<+∞}, and Γ0(X)\Gamma_0(X)Γ0​(X) is the set of proper, lower semicontinuous, convex functions X→R∪{+∞}X \to \mathbb R\cup\{+\infty\}X→R∪{+∞}.

The standard DC program is

(Pdc)α=inf⁡{f(x):=g(x)−h(x):x∈X},g,h∈Γ0(X),(P_{dc})\qquad \alpha = \inf\{f(x) := g(x) - h(x) : x\in X\},\qquad g, h\in\Gamma_0(X),(Pdc​)α=inf{f(x):=g(x)−h(x):x∈X},g,h∈Γ0​(X),

with the convention +∞−(+∞)=+∞+\infty - (+\infty) = +\infty+∞−(+∞)=+∞, and α\alphaα is assumed finite. Finiteness of α\alphaα forces dom⁡g⊂dom⁡h\operatorname{dom} g\subset\operatorname{dom} hdomg⊂domh, so dom⁡f=dom⁡g\operatorname{dom} f = \operatorname{dom} gdomf=domg.

The subdifferential of φ\varphiφ at xxx is

∂φ(x)={y∈X:φ(x)<+∞, φ(v)≥φ(x)+⟨y,v−x⟩  ∀v∈X}.\partial\varphi(x) = \{y\in X : \varphi(x) < +\infty,\ \varphi(v) \ge \varphi(x) + \langle y, v - x\rangle\ \ \forall v\in X\}.∂φ(x)={y∈X:φ(x)<+∞, φ(v)≥φ(x)+⟨y,v−x⟩  ∀v∈X}.

A point xxx is strongly critical for f=g−hf = g - hf=g−h if ∅≠∂h(x)⊂∂g(x)\emptyset \ne \partial h(x)\subset\partial g(x)∅=∂h(x)⊂∂g(x).

The directional derivative of φ\varphiφ at x∈dom⁡φx\in\operatorname{dom}\varphix∈domφ in direction uuu is φ′(x;u)=lim⁡t↓0(φ(x+tu)−φ(x))/t\varphi'(x;u) = \lim_{t\downarrow 0}(\varphi(x+tu) - \varphi(x))/tφ′(x;u)=limt↓0​(φ(x+tu)−φ(x))/t. For convex φ\varphiφ it equals inf⁡t>0(φ(x+tu)−φ(x))/t\inf_{t>0}(\varphi(x+tu)-\varphi(x))/tinft>0​(φ(x+tu)−φ(x))/t. A point x∈dom⁡fx\in\operatorname{dom} fx∈domf is d-stationary for fff if f′(x;u)≥0f'(x;u)\ge 0f′(x;u)≥0 for every u∈Xu\in Xu∈X. The support function of C⊂XC\subset XC⊂X is χC∗(u)=sup⁡y∈C⟨u,y⟩\chi^*_C(u) = \sup_{y\in C}\langle u, y\rangleχC∗​(u)=supy∈C​⟨u,y⟩, with χ∅∗≡−∞\chi^*_\emptyset \equiv -\inftyχ∅∗​≡−∞. Finally, ri⁡C\operatorname{ri} CriC is the relative interior of CCC, its interior inside the affine hull aff⁡C\operatorname{aff} CaffC.

Formalization targets

Goal: Theorem 1(iii)

For x∈ri⁡(dom⁡g)∩ri⁡(dom⁡h)x\in\operatorname{ri}(\operatorname{dom} g)\cap\operatorname{ri}(\operatorname{dom} h)x∈ri(domg)∩ri(domh),

x is d-stationary for f  ⟺  ∅≠∂h(x)⊂∂g(x).x \text{ is d-stationary for } f \iff \emptyset\ne\partial h(x)\subset\partial g(x).x is d-stationary for f⟺∅=∂h(x)⊂∂g(x).

Milestones

  1. Theorem 1(i): for x∈dom⁡gx\in\operatorname{dom} gx∈domg with ∂h(x)≠∅\partial h(x)\ne\emptyset∂h(x)=∅,
f′(x;u)=g′(x;u)−h′(x;u)∀u∈X.f'(x;u) = g'(x;u) - h'(x;u)\qquad \forall u\in X.f′(x;u)=g′(x;u)−h′(x;u)∀u∈X.
  1. Theorem 1(ii), first sentence: under the same hypotheses, xxx is d-stationary iff g′(x;u)≥h′(x;u)g'(x;u)\ge h'(x;u)g′(x;u)≥h′(x;u) for all uuu.
  2. Theorem 1(iv): for x∈ri⁡(dom⁡g)x\in\operatorname{ri}(\operatorname{dom} g)x∈ri(domg) with ∂h(x)≠∅\partial h(x)\ne\emptyset∂h(x)=∅, d-stationarity implies strong criticality.
  3. Theorem 1(v): for x∈ri⁡(dom⁡h)x\in\operatorname{ri}(\operatorname{dom} h)x∈ri(domh), strong criticality implies d-stationarity.

Companion statements

  • Theorem 1(ii), second sentence: for x∈dom⁡gx\in\operatorname{dom} gx∈domg, if g′(x;⋅)=χ∂g(x)∗g'(x;\cdot) = \chi^*_{\partial g(x)}g′(x;⋅)=χ∂g(x)∗​ and h′(x;⋅)=χ∂h(x)∗h'(x;\cdot) = \chi^*_{\partial h(x)}h′(x;⋅)=χ∂h(x)∗​, then d-stationarity and strong criticality coincide.
  • Theorem 1(vi): if aff⁡(dom⁡g)=aff⁡(dom⁡h)\operatorname{aff}(\operatorname{dom} g) = \operatorname{aff}(\operatorname{dom} h)aff(domg)=aff(domh), then ri⁡(dom⁡g)⊂ri⁡(dom⁡h)\operatorname{ri}(\operatorname{dom} g)\subset\operatorname{ri}(\operatorname{dom} h)ri(domg)⊂ri(domh) and the equivalence holds on ri⁡(dom⁡g)\operatorname{ri}(\operatorname{dom} g)ri(domg).

Part (iii) is the goal because it is the equivalence the paper uses to justify DCA, stated under a hypothesis symmetric in ggg and hhh; (vi) is the more general companion.

Significance

The theorem connects the output of DCA with a stationarity notion intrinsic to fff. Without it, the strong criticality certified by DCA would be a property of a decomposition rather than of the problem, and different decompositions of the same fff could certify different points. With it, at points in the relative interiors of the domains, every strongly critical point is d-stationary, and conversely no d-stationary point is missed by the criticality test.

Parts (i) and (ii) are stated in the paper without proof, and so is the rest of Theorem 1; none of it has a machine-checked proof. The mission produces a formal statement of all six parts with the extended-real conventions made explicit. Three of the printed parts are false as stated without the nonemptiness of ∂h(x)\partial h(x)∂h(x); the formal versions add that hypothesis and record a counterexample for each, so the formalization also corrects the printed statement.

Difficulty

The obvious argument writes f′(x;u)=g′(x;u)−h′(x;u)f'(x;u) = g'(x;u) - h'(x;u)f′(x;u)=g′(x;u)−h′(x;u) and reads off both directions from g′≥h′g'\ge h'g′≥h′. Two steps of it fail. First, the difference can be −∞−(−∞)-\infty - (-\infty)−∞−(−∞) or +∞−(+∞)+\infty - (+\infty)+∞−(+∞), and the limit defining f′f'f′ need not be the difference of the limits; the nonemptiness of ∂h(x)\partial h(x)∂h(x) is exactly what rules out the first case. Second, passing from "g′(x;⋅)≥h′(x;⋅)g'(x;\cdot)\ge h'(x;\cdot)g′(x;⋅)≥h′(x;⋅)" to "∂h(x)⊂∂g(x)\partial h(x)\subset\partial g(x)∂h(x)⊂∂g(x)" needs h′(x;⋅)h'(x;\cdot)h′(x;⋅) to equal the support function of ∂h(x)\partial h(x)∂h(x), which holds in the relative interior of dom⁡h\operatorname{dom} hdomh but fails on its relative boundary, where h′(x;⋅)h'(x;\cdot)h′(x;⋅) need not be lower semicontinuous. The relative interior, not the interior, is essential: the domains may be lower-dimensional.

Formalization scope

XXX is EuclideanSpace ℝ (Fin n), and every function maps into EReal. The published definitions TaoAnDCA.GlobalOpt.Setting supply dom⁡\operatorname{dom}dom (effDom), the DC objective with +∞−(+∞)=+∞+\infty - (+\infty) = +\infty+∞−(+∞)=+∞ (dcSub), the subdifferential (subdiff) and α\alphaα (primalValue); Γ0(X)\Gamma_0(X)Γ0​(X) is the published IsProperClosedConvex. Every statement carries the standing assumptions of Theorem 1 as binders: g,h∈Γ0(X)g, h\in\Gamma_0(X)g,h∈Γ0​(X), α≠−∞\alpha\ne-\inftyα=−∞ and α≠+∞\alpha\ne+\inftyα=+∞. The mission's definitions are:

  • convDirDeriv: the convex directional derivative by the paper's infimum formula, in EReal;
  • HasDirDerivE: the predicate that the one-sided limit along t↓0t\downarrow 0t↓0 exists in EReal and equals a given value;
  • IsDStationary: x∈dom⁡φx\in\operatorname{dom}\varphix∈domφ and, for every direction, the limit exists and is ≥0\ge 0≥0;
  • IsStronglyCritical: both ∂h(x)≠∅\partial h(x)\ne\emptyset∂h(x)=∅ and ∂h(x)⊂∂g(x)\partial h(x)\subset\partial g(x)∂h(x)⊂∂g(x);
  • supportFn: the extended-real support function, −∞-\infty−∞ on ∅\emptyset∅.

The relative interior is Mathlib's intrinsicInterior ℝ, the affine hull is affineSpan ℝ. The subgradient inequality has the standard sign; display (1) of the paper prints the opposite sign, a slip. The only hypothesis added to the page is ∂h(x)≠∅\partial h(x)\ne\emptyset∂h(x)=∅, in parts (i), (ii) first sentence and (iv), each of which is false without it; parts (ii) second sentence, (iii), (v) and (vi) are stated as printed.

The statement admits trivializing formalizations, which this one rules out. Strong criticality without the nonemptiness of ∂h(x)\partial h(x)∂h(x) is vacuous wherever ∂h(x)=∅\partial h(x) = \emptyset∂h(x)=∅. A d-stationarity defined through limUnder, a real-valued derivative, or "every limit is nonnegative" holds vacuously where the limit does not exist. And g−hg - hg−h written in raw EReal would give +∞−(+∞)=−∞+\infty - (+\infty) = -\infty+∞−(+∞)=−∞.

A complete development needs the monotonicity of convex difference quotients in EReal, limit arithmetic for extended reals, and the formula φ′(x;⋅)=χ∂φ(x)∗\varphi'(x;\cdot) = \chi^*_{\partial\varphi(x)}φ′(x;⋅)=χ∂φ(x)∗​ for φ∈Γ0(Rn)\varphi\in\Gamma_0(\mathbb R^n)φ∈Γ0​(Rn) at points of ri⁡(dom⁡φ)\operatorname{ri}(\operatorname{dom}\varphi)ri(domφ) (Rockafellar 1970, Theorem 23.4), together with the nonemptiness of ∂φ\partial\varphi∂φ there. These results on extended-real convex functions are reusable well beyond DC programming, and contributions of them as separate theorems are welcome.

Selected references

  • H. A. Le Thi, T. Pham Dinh, DC programming and DCA: thirty years of developments, Mathematical Programming Ser. B 169 (2018), 5–68. https://doi.org/10.1007/s10107-018-1235-y
  • T. Pham Dinh, H. A. Le Thi, A d.c. optimization algorithm for solving the trust-region subproblem, SIAM Journal on Optimization 8 (1998), 476–505. https://doi.org/10.1137/S1052623494274313
  • M. Ahn, J.-S. Pang, J. Xin, Difference-of-convex learning: directional stationarity, optimality, and sparsity, SIAM Journal on Optimization 27 (2017), 1637–1665. https://doi.org/10.1137/16M1084754
  • R. T. Rockafellar, Convex Analysis, Princeton University Press, 1970. https://doi.org/10.1515/9781400873173
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