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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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Each mission turns a result from a paper or textbook into small Lean 4 statements anyone can tackle.

Campaigns (experimental)

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.

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.

≤ 1.999074Formalized record
3 provers on it4 of 4 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.

≤ 7.103205334138Formalized record→≤ 2Open frontier
9 provers on it7 of 8 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.
≤ 80Formalized record→≤ 70Open frontier
3 provers on it7 of 8 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.

≤ 27Formalized record→≤ 5Open frontier
35 provers on it13 of 15 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

Steady-State Analysis of the Join-the-Shortest-Queue Model in the Halfin-Whitt Regime 2: The JSQ Diffusion Limit Satisfies a Foster-Lyapunov Drift ConditionResearch Paper

Motivation

Join-the-shortest-queue (JSQ) is the basic load-balancing rule for a system of nnn parallel single-server queues: every arriving customer joins a queue of minimal length. It is optimal in several senses for homogeneous servers and is the reference policy against which cheaper rules (power-of-ddd choices, join-the-idle-queue) are measured. In the Halfin–Whitt regime, where the arrival rate is nλn\lambdanλ with λ=1−β/n\lambda = 1-\beta/\sqrt nλ=1−β/n​ for a fixed β>0\beta>0β>0, Eschenfeldt and Gamarnik (arXiv:1502.00999) proved that the suitably centred and scaled numbers of queues of length at least one and at least two converge, on finite time intervals, to a two-dimensional reflected diffusion. Braverman (arXiv:1801.05121) justified the interchange of limits (the stationary distributions of the nnn-server chains converge to the stationary distribution of the diffusion). One ingredient of that result is that the diffusion is exponentially ergodic, so it has a unique stationary distribution that is approached at a geometric rate. This mission formalizes the analytic core of that ingredient: a Foster–Lyapunov drift condition for the diffusion's generator.

Timeline. Eschenfeldt and Gamarnik (2015) proved the process-level diffusion limit, the first analysis of JSQ in this regime. Mukherjee, Borst, van Leeuwaarden and Whiting (J. Appl. Probab. 53, 2016) showed that a class of load-balancing schemes shares the same diffusion limit. Braverman (arXiv 2018, v2 2019; Math. Oper. Res. 45(3), 2020) proved tightness of the scaled stationary distributions and exponential ergodicity of the limit, which together give the interchange of limits.

Setting

The state space is the closed quadrant Ω=(−∞,0]×[0,∞)\Omega = (-\infty,0]\times[0,\infty)Ω=(−∞,0]×[0,∞). For f:Ω→Rf:\Omega\to\mathbb Rf:Ω→R write f1=∂f/∂x1f_1 = \partial f/\partial x_1f1​=∂f/∂x1​, f2=∂f/∂x2f_2 = \partial f/\partial x_2f2​=∂f/∂x2​, f11=∂f1/∂x1f_{11} = \partial f_1/\partial x_1f11​=∂f1​/∂x1​. On the boundary ∂Ω\partial\Omega∂Ω these are one-sided derivatives, and C2(Ω)C^2(\Omega)C2(Ω) denotes the twice continuously differentiable functions in this sense.

The diffusion limit Y=(Y1,Y2)Y=(Y_1,Y_2)Y=(Y1​,Y2​) solves

Y1(t)=Y1(0)+2W(t)−βt+∫0t(−Y1(s)+Y2(s)) ds−U(t),Y2(t)=Y2(0)+U(t)−∫0tY2(s) ds,Y_1(t)=Y_1(0)+\sqrt2W(t)-\beta t+\int_0^t(-Y_1(s)+Y_2(s))\,ds-U(t),\qquad Y_2(t)=Y_2(0)+U(t)-\int_0^tY_2(s)\,ds,Y1​(t)=Y1​(0)+2​W(t)−βt+∫0t​(−Y1​(s)+Y2​(s))ds−U(t),Y2​(t)=Y2​(0)+U(t)−∫0t​Y2​(s)ds,

with WWW a standard Brownian motion and UUU a nondecreasing regulator that increases only when Y1=0Y_1=0Y1​=0. For f∈C2(Ω)f\in C^2(\Omega)f∈C2(Ω) with the reflection condition f1(0,x2)=f2(0,x2)f_1(0,x_2)=f_2(0,x_2)f1​(0,x2​)=f2​(0,x2​), its generator acts by

GYf(x)=(−x1+x2−β)f1(x)−x2f2(x)+f11(x),x∈Ω.G_Yf(x)=(-x_1+x_2-\beta)f_1(x)-x_2f_2(x)+f_{11}(x),\qquad x\in\Omega .GY​f(x)=(−x1​+x2​−β)f1​(x)−x2​f2​(x)+f11​(x),x∈Ω.

The construction of the Lyapunov function uses an auxiliary integer n≥1n\ge1n≥1 and the fluid operator

Lf(x)=(−x1+x2−βn)f1(x)−x2f2(x),Lf(x)=\Big(-x_1+x_2-\frac{\beta}{\sqrt n}\Big)f_1(x)-x_2f_2(x),Lf(x)=(−x1​+x2​−n​β​)f1​(x)−x2​f2​(x),

the generator of the deterministic fluid path v1′=−v1+v2−β/nv_1'=-v_1+v_2-\beta/\sqrt nv1′​=−v1​+v2​−β/n​, v2′=−v2v_2'=-v_2v2′​=−v2​. A smoothed indicator ϕ(ℓ,u)\phi^{(\ell,u)}ϕ(ℓ,u) (a piecewise cubic that rises from 000 at ℓ\ellℓ to 111 at uuu) and two levels β<κ1<κ2\beta<\kappa_1<\kappa_2β<κ1​<κ2​ define the PDEs

Lf(1)(x)=−ϕ(κ1/n,κ2/n)(−x1),Lf(2)(x)=−ϕ(κ1/n,κ2/n)(x2),x∈Ω,Lf^{(1)}(x)=-\phi^{(\kappa_1/\sqrt n,\kappa_2/\sqrt n)}(-x_1),\qquad Lf^{(2)}(x)=-\phi^{(\kappa_1/\sqrt n,\kappa_2/\sqrt n)}(x_2),\qquad x\in\Omega,Lf(1)(x)=−ϕ(κ1​/n​,κ2​/n​)(−x1​),Lf(2)(x)=−ϕ(κ1​/n​,κ2​/n​)(x2​),x∈Ω,

each with the reflection condition. Their solutions are written explicitly in terms of the fluid hitting times τ~(κ)\tilde\tau^{(\kappa)}τ~(κ) (through the Lambert W function) and τ\tauτ, and the curves Γ(κ)\Gamma^{(\kappa)}Γ(κ) that split Ω\OmegaΩ into regions S0,…,S3S_0,\dots,S_3S0​,…,S3​.

Formalization targets

Goal: Theorem 4

For every β>0\beta>0β>0 there exist c>0c>0c>0, d>0d>0d>0, a compact set KKK and V∈C2(Ω)V\in C^2(\Omega)V∈C2(Ω) with V≥1V\ge1V≥1 on Ω\OmegaΩ, V(x)→∞V(x)\to\inftyV(x)→∞ as ∣x∣→∞|x|\to\infty∣x∣→∞ in Ω\OmegaΩ, and V1(0,x2)=V2(0,x2)V_1(0,x_2)=V_2(0,x_2)V1​(0,x2​)=V2​(0,x2​), such that

GYV(x)≤−cV(x)+d 1(x∈K),x∈Ω.G_YV(x)\le -cV(x)+d\,1(x\in K),\qquad x\in\Omega .GY​V(x)≤−cV(x)+d1(x∈K),x∈Ω.

The constants are unspecified and depend only on β\betaβ; the statement involves no nnn.

Milestones

  1. (5.6)–(5.7): ϕ(ℓ,u)\phi^{(\ell,u)}ϕ(ℓ,u) has an absolutely continuous derivative with ϕ′(ℓ)=ϕ′(u)=0\phi'(\ell)=\phi'(u)=0ϕ′(ℓ)=ϕ′(u)=0, ∣ϕ′∣≤4/(u−ℓ)|\phi'|\le 4/(u-\ell)∣ϕ′∣≤4/(u−ℓ) and ∣ϕ′′∣≤12/(u−ℓ)2|\phi''|\le12/(u-\ell)^2∣ϕ′′∣≤12/(u−ℓ)2.
  2. Lemma 10: τ~(κ)\tilde\tau^{(\kappa)}τ~(κ) extends to {x2=0}\{x_2=0\}{x2​=0}, vanishes on {x1=−κ/n}\{x_1=-\kappa/\sqrt n\}{x1​=−κ/n​}, and has explicit one-sided partial derivatives.
  3. Lemma 11: the explicit f(1)f^{(1)}f(1) is nonnegative, lies in C2(Ω)C^2(\Omega)C2(Ω), and has explicit first partials.
  4. Lemma 12: the explicit six-case f(2)f^{(2)}f(2) is well defined, lies in C2(Ω)C^2(\Omega)C2(Ω), and has the partials (C.8)–(C.9).
  5. Lemma 8: for ϵ>0\epsilon>0ϵ>0, κ1=β+ϵ\kappa_1=\beta+\epsilonκ1​=β+ϵ, κ2=β+2ϵ\kappa_2=\beta+2\epsilonκ2​=β+2ϵ, both PDEs have C2(Ω)C^2(\Omega)C2(Ω) solutions with
f(1)≤log⁡2,f(2)≤log⁡2+ϵβ on a box,∣f1(1)∣≤4nϵlog⁡2, ∣f11(1)∣≤12nϵ2log⁡2, ∣f1(2)∣≤nβ, ∣f11(2)∣≤nβϵ(1+4β+ϵϵ).f^{(1)}\le\log2,\quad f^{(2)}\le\log2+\tfrac{\epsilon}{\beta}\ \text{on a box},\qquad |f^{(1)}_1|\le\tfrac{4\sqrt n}{\epsilon}\log2,\ |f^{(1)}_{11}|\le\tfrac{12n}{\epsilon^2}\log2,\ |f^{(2)}_1|\le\tfrac{\sqrt n}{\beta},\ |f^{(2)}_{11}|\le\tfrac{n}{\beta\epsilon}\big(1+4\tfrac{\beta+\epsilon}{\epsilon}\big).f(1)≤log2,f(2)≤log2+βϵ​ on a box,∣f1(1)​∣≤ϵ4n​​log2, ∣f11(1)​∣≤ϵ212n​log2, ∣f1(2)​∣≤βn​​, ∣f11(2)​∣≤βϵn​(1+4ϵβ+ϵ​).

Significance

By the criterion of Down, Meyn and Tweedie (Ann. Probab. 23, 1995, Theorem 5.2), a drift inequality of the form (5.2) with compact KKK and V→∞V\to\inftyV→∞ implies that the diffusion is positive Harris recurrent and exponentially ergodic in the VVV-norm (Theorem 3 and Corollary 1 of the paper). Together with tightness of the prelimit stationary distributions (mission 1 of this series), this gives convergence of the stationary distributions of the JSQ chains to that of the diffusion. That justifies approximating steady-state JSQ performance by the diffusion.

The construction itself is reusable. Solving the fluid-model PDE Lf=−(smoothed indicator)Lf=-(\text{smoothed indicator})Lf=−(smoothed indicator) and exponentiating the solution is a general route from fluid stability to exponential ergodicity of a diffusion. This mission writes that route out for one reflected diffusion with explicit hitting-time formulas.

Status: the result is proved in the paper; no part of it has a machine-checked proof. Theorem 3 and Corollary 1 are not posed, because they rest on the cited Down–Meyn–Tweedie theory and on the existence of the reflected process, neither of which Mathlib has.

Difficulty

The reflecting boundary rules out the first candidates. The condition V1(0,x2)=V2(0,x2)V_1(0,x_2)=V_2(0,x_2)V1​(0,x2​)=V2​(0,x2​) excludes exponentials of linear functions such as ea(x2−x1)e^{a(x_2-x_1)}ea(x2​−x1​) unless a=0a=0a=0. The natural candidate from the fluid model, the exponential of the fluid time needed to reach a box, has a discontinuous integrand and is not in C2(Ω)C^2(\Omega)C2(Ω), so GYG_YGY​ cannot be applied to it. The milestone functions f(1)f^{(1)}f(1), f(2)f^{(2)}f(2) are given piecewise across the curves Γ(κ1)\Gamma^{(\kappa_1)}Γ(κ1​), Γ(κ2)\Gamma^{(\kappa_2)}Γ(κ2​) and the lines x1=−κi/nx_1=-\kappa_i/\sqrt nx1​=−κi​/n​, through implicitly defined hitting times. Three things are hard: C2C^2C2 regularity across these interfaces, the Lambert W asymptotics as x2↓0x_2\downarrow0x2​↓0, and second-derivative bounds that hold uniformly on the unbounded domain Ω\OmegaΩ with the stated dependence on nnn and ϵ\epsilonϵ.

Formalization scope

  • Points of Ω\OmegaΩ are pairs ℝ × ℝ, and Ω\OmegaΩ is Set.Iic 0 ×ˢ Set.Ici 0. Partials are fderivWithin ℝ f Ω in the coordinate directions, which are one-sided at boundary points. C2(Ω)C^2(\Omega)C2(Ω) is ContDiffOn ℝ 2 f Ω.
  • GYG_YGY​ is the generator formula of p. 16, and every statement applies it only to C2(Ω)C^2(\Omega)C2(Ω) functions with the reflection condition. The process (2.1) and the extended generator are not constructed. V∈C2(Ω)V\in C^2(\Omega)V∈C2(Ω) is part of the conclusion of Theorem 4, so a VVV whose derivatives within Ω\OmegaΩ are undefined (and default to 000) cannot satisfy (5.2) vacuously. Dropping V≥1V\ge1V≥1, V→∞V\to\inftyV→∞, the compactness of KKK, or c,d>0c,d>0c,d>0 would make (5.2) trivial, and all four are kept.
  • The auxiliary nnn is an integer n≥1n\ge1n≥1; no relation between β\betaβ and n\sqrt nn​ is assumed.
  • The Lambert W function (principal branch) is defined locally, since Mathlib has none. τ\tauτ takes values in WithTop ℝ, with ∞\infty∞ when no solution exists, and its real value is used only where it is finite. ν∗\nu^*ν∗ (the curve Γ(κ)\Gamma^{(\kappa)}Γ(κ)) is the solution of a nonlinear system whose uniqueness is Lemma 5.
  • Two printed misprints are corrected. Lemma 8's "for every ϵ>0\epsilon>0ϵ>0" is formalized with κ1=β+ϵ\kappa_1=\beta+\epsilonκ1​=β+ϵ, κ2=β+2ϵ\kappa_2=\beta+2\epsilonκ2​=β+2ϵ, the choice its proof makes; read literally, the printed statement is false. In (C.5) of Lemma 10 the identity τ~2=−τ~1τ~\tilde\tau_2=-\tilde\tau_1\tilde\tauτ~2​=−τ~1​τ~ is formalized as τ~2=τ~1τ~\tilde\tau_2=\tilde\tau_1\tilde\tauτ~2​=τ~1​τ~, which is what implicit differentiation gives.
  • Lemmas 5, 6 and 9 (properties of Γ(κ)\Gamma^{(\kappa)}Γ(κ), τ\tauτ and WWW) are milestones of mission 1; here their objects are only definitions. Contributions proving those facts in this namespace, or general lemmas on the Lambert W function, are welcome.

Selected references

  • A. Braverman, Steady-State Analysis of the Join-the-Shortest-Queue Model in the Halfin-Whitt Regime, Math. Oper. Res. 45(3), 2020; preprint arXiv:1801.05121v2, 2019. https://arxiv.org/abs/1801.05121, https://doi.org/10.1287/moor.2019.1023
  • P. Eschenfeldt, D. Gamarnik, Join the Shortest Queue with Many Servers. The Heavy-Traffic Asymptotics, 2015 (Math. Oper. Res. 43(3), 2018). https://arxiv.org/abs/1502.00999
  • D. Down, S. P. Meyn, R. L. Tweedie, Exponential and Uniform Ergodicity of Markov Processes, Ann. Probab. 23, 1671–1691, 1995. https://doi.org/10.1214/aop/1176987798
  • D. Mukherjee, S. C. Borst, J. S. H. van Leeuwaarden, P. A. Whiting, Universality of Load Balancing Schemes on the Diffusion Scale, J. Appl. Probab. 53, 1111–1124, 2016. https://projecteuclid.org/euclid.jap/1481132840
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ProbabilityStatistics·Captain: mikedeng1

Central Limit Theorems and Bootstrap in High Dimensions 2: Gaussian Multiplier Bootstrap for Simple Convex Sets with Error C[Δ̄ₙ^{1/3} log^{2/3}(pn) + n⁻¹ log^{1/2}(pn)]Research Paper

Motivation

Many procedures in high-dimensional statistics reduce to computing the probability that a normalized sum of independent random vectors falls into a set: simultaneous confidence intervals for many means, max-type tests, multiple testing with family-wise error control, and inference after model selection. When the dimension ppp is comparable to or much larger than the sample size nnn, these probabilities are approximated by those of a Gaussian vector with the same covariance, the high-dimensional central limit theorem. That Gaussian law is not available in practice, because its covariance matrix is unknown. The Gaussian multiplier bootstrap replaces it by a Gaussian vector built from the data, whose covariance is the sample covariance, and simulates from it.

Chernozhukov, Chetverikov and Kato, Central limit theorems and bootstrap in high dimensions (Ann. Probab. 45 (2017)), prove that this bootstrap is valid uniformly over hyperrectangles and over simple convex sets (sets sandwiched between a polytope with polynomially many facets and its small enlargement), with error depending on ppp only through log⁡p\log plogp. This mission formalizes their abstract multiplier bootstrap theorem, Theorem 4.1.

Timeline:

  • 2013: the same authors prove Gaussian approximation and multiplier bootstrap validity for maxima of sums of high-dimensional vectors (Ann. Statist. 41 (2013)).
  • 2015: comparison and anti-concentration bounds for maxima of Gaussian vectors (Probab. Theory Related Fields 162 (2015)), reference [20] of the paper; its Theorem 1 is the Gaussian-to-Gaussian comparison used here.
  • 2017: the present paper extends both the CLT and the bootstrap from maxima to hyperrectangles and simple convex sets.

Setting

Let n≥4n\ge4n≥4 and p≥3p\ge3p≥3. Let X1,…,XnX_1,\dots,X_nX1​,…,Xn​ be independent random vectors in Rp\mathbb R^pRp with coordinates XijX_{ij}Xij​, centred (E[Xij]=0\mathrm E[X_{ij}]=0E[Xij​]=0) with E[Xij2]<∞\mathrm E[X_{ij}^2]<\inftyE[Xij2​]<∞. Let Y1,…,YnY_1,\dots,Y_nY1​,…,Yn​ be independent Gaussian vectors with Yi∼N(0,E[XiXi′])Y_i\sim N(0,\mathrm E[X_iX_i'])Yi​∼N(0,E[Xi​Xi′​]) and set

SnY=1n∑i=1nYi.S_n^Y=\frac1{\sqrt n}\sum_{i=1}^nY_i .SnY​=n​1​i=1∑n​Yi​.

The multiplier bootstrap: let e1,…,ene_1,\dots,e_ne1​,…,en​ be i.i.d. N(0,1)N(0,1)N(0,1), independent of the data X1n={X1,…,Xn}X_1^n=\{X_1,\dots,X_n\}X1n​={X1​,…,Xn​}, let Xˉ=n−1∑iXi\bar X=n^{-1}\sum_iX_iXˉ=n−1∑i​Xi​, and

SneX=1n∑i=1nei(Xi−Xˉ).S_n^{eX}=\frac1{\sqrt n}\sum_{i=1}^ne_i(X_i-\bar X).SneX​=n​1​i=1∑n​ei​(Xi​−Xˉ).

Given the data, SneXS_n^{eX}SneX​ is Gaussian with covariance Σ^=n−1∑i(Xi−Xˉ)(Xi−Xˉ)′\widehat\Sigma=n^{-1}\sum_i(X_i-\bar X)(X_i-\bar X)'Σ=n−1∑i​(Xi​−Xˉ)(Xi​−Xˉ)′, while SnYS_n^YSnY​ has covariance Σ=n−1∑iE[XiXi′]\Sigma=n^{-1}\sum_i\mathrm E[X_iX_i']Σ=n−1∑i​E[Xi​Xi′​].

A hyperrectangle is a set {w:aj≤wj≤bj ∀j}\{w:a_j\le w_j\le b_j\ \forall j\}{w:aj​≤wj​≤bj​ ∀j} with −∞≤aj≤bj≤∞-\infty\le a_j\le b_j\le\infty−∞≤aj​≤bj​≤∞. For a finite set V\mathcal VV of unit vectors and thresholds s(v)s(v)s(v), the polyhedron Am=⋂v∈V{w:w′v≤s(v)}A^m=\bigcap_{v\in\mathcal V}\{w:w'v\le s(v)\}Am=⋂v∈V​{w:w′v≤s(v)} has the enlargement Am,ϵ=⋂v∈V{w:w′v≤s(v)+ϵ}A^{m,\epsilon}=\bigcap_{v\in\mathcal V}\{w:w'v\le s(v)+\epsilon\}Am,ϵ=⋂v∈V​{w:w′v≤s(v)+ϵ}. For constants a,d>0a,d>0a,d>0, a Borel set AAA satisfies condition (C) if Am⊆A⊆Am,a/nA^m\subseteq A\subseteq A^{m,a/n}Am⊆A⊆Am,a/n for some such polyhedron with m≤(pn)dm\le(pn)^dm≤(pn)d facets; Am(A)A^m(A)Am(A) denotes this polyhedron and V(Am)\mathcal V(A^m)V(Am) its normals. Condition (M.1′) with constant b>0b>0b>0 asks n−1∑iE[(v′Xi)2]≥bn^{-1}\sum_i\mathrm E[(v'X_i)^2]\ge bn−1∑i​E[(v′Xi​)2]≥b for every v∈V(Am)v\in\mathcal V(A^m)v∈V(Am). Finally,

Δn(A)=sup⁡A∈Amax⁡v1,v2∈V(Am(A))∣v1′(Σ^−Σ)v2∣,Δn,r=max⁡j,k∣Σ^jk−Σjk∣.\Delta_n(\mathcal A)=\sup_{A\in\mathcal A}\max_{v_1,v_2\in\mathcal V(A^m(A))}\big|v_1'(\widehat\Sigma-\Sigma)v_2\big|,\qquad \Delta_{n,r}=\max_{j,k}|\widehat\Sigma_{jk}-\Sigma_{jk}| .Δn​(A)=A∈Asup​v1​,v2​∈V(Am(A))max​​v1′​(Σ−Σ)v2​​,Δn,r​=j,kmax​∣Σjk​−Σjk​∣.

Formalization targets

Goal: Theorem 4.1

Let A\mathcal AA be a class of sets satisfying (C) and (M.1′). There is CCC depending only on a,b,da,b,da,b,d such that for every Δˉn>0\bar\Delta_n>0Δˉn​>0, on the event Δn(A)≤Δˉn\Delta_n(\mathcal A)\le\bar\Delta_nΔn​(A)≤Δˉn​,

ρnMB(A)=sup⁡A∈A∣P(SneX∈A∣X1n)−P(SnY∈A)∣≤C{Δˉn1/3log⁡2/3(pn)+n−1log⁡1/2(pn)}.\rho_n^{MB}(\mathcal A)=\sup_{A\in\mathcal A}\big|P(S_n^{eX}\in A\mid X_1^n)-P(S_n^Y\in A)\big|\le C\big\{\bar\Delta_n^{1/3}\log^{2/3}(pn)+n^{-1}\log^{1/2}(pn)\big\}.ρnMB​(A)=A∈Asup​​P(SneX​∈A∣X1n​)−P(SnY​∈A)​≤C{Δˉn1/3​log2/3(pn)+n−1log1/2(pn)}.

The theorem is deterministic in the data: it holds at every realization on the event, and turning it into a rate requires only a bound on Δn(A)\Delta_n(\mathcal A)Δn​(A).

Milestones

In the order of the proof (App. E.2, p. 2342):

  1. Conditional Gaussianity: given X1nX_1^nX1n​, SneX∼N(0,Σ^)S_n^{eX}\sim N(0,\widehat\Sigma)SneX​∼N(0,Σ).
  2. Display (21): 0≤Fβ(w)−max⁡j(wj−yj)≤β−1log⁡p0\le F_\beta(w)-\max_j(w_j-y_j)\le\beta^{-1}\log p0≤Fβ​(w)−maxj​(wj​−yj​)≤β−1logp for the smooth max Fβ(w)=β−1log⁡∑jeβ(wj−yj)F_\beta(w)=\beta^{-1}\log\sum_je^{\beta(w_j-y_j)}Fβ​(w)=β−1log∑j​eβ(wj​−yj​).
  3. The comparison display ∣E[g(Fβ(SneX))∣X1n]−E[g(Fβ(SnY))]∣≤(∥g′′∥∞/2+β∥g′∥∞)Δn,r|\mathrm E[g(F_\beta(S^{eX}_n))\mid X_1^n]-\mathrm E[g(F_\beta(S^Y_n))]|\le(\|g''\|_\infty/2+\beta\|g'\|_\infty)\Delta_{n,r}∣E[g(Fβ​(SneX​))∣X1n​]−E[g(Fβ​(SnY​))]∣≤(∥g′′∥∞​/2+β∥g′∥∞​)Δn,r​.
  4. Lemma A.1 (Nazarov's inequality): P(Y≤y+a)−P(Y≤y)≤Calog⁡pP(Y\le y+a)-P(Y\le y)\le Ca\sqrt{\log p}P(Y≤y+a)−P(Y≤y)≤Calogp​ for a centred Gaussian YYY with variances at least bbb.
  5. The smoothed step: ∣P(SneX≤y−ϕ−1∣X1n)−P(SnY≤y−ϕ−1)∣≤C{ϕ−1log⁡1/2p+(ϕ2+βϕ)Δn,r}|P(S^{eX}_n\le y-\phi^{-1}\mid X_1^n)-P(S^Y_n\le y-\phi^{-1})|\le C\{\phi^{-1}\log^{1/2}p+(\phi^2+\beta\phi)\Delta_{n,r}\}∣P(SneX​≤y−ϕ−1∣X1n​)−P(SnY​≤y−ϕ−1)∣≤C{ϕ−1log1/2p+(ϕ2+βϕ)Δn,r​} with β=ϕlog⁡p\beta=\phi\log pβ=ϕlogp.
  6. Display (39): sup⁡y∣P(SneX≤y∣X1n)−P(SnY≤y)∣≤CΔn,r1/3log⁡2/3p\sup_y|P(S^{eX}_n\le y\mid X_1^n)-P(S^Y_n\le y)|\le C\Delta_{n,r}^{1/3}\log^{2/3}psupy​∣P(SneX​≤y∣X1n​)−P(SnY​≤y)∣≤CΔn,r1/3​log2/3p under (M.1): n−1∑iE[Xij2]≥bn^{-1}\sum_i\mathrm E[X_{ij}^2]\ge bn−1∑i​E[Xij2​]≥b.
  7. Remark 4.1 = (38): ρnMB(Are)≤CΔˉn1/3log⁡2/3p\rho_n^{MB}(\mathcal A^{re})\le C\bar\Delta_n^{1/3}\log^{2/3}pρnMB​(Are)≤CΔˉn1/3​log2/3p on Δn,r≤Δˉn\Delta_{n,r}\le\bar\Delta_nΔn,r​≤Δˉn​, CCC depending only on bbb.
  8. The reduction display: for one simple convex set, the error at AAA is at most Cϵlog⁡1/2(pn)+ρˉC\epsilon\log^{1/2}(pn)+\bar\rhoCϵlog1/2(pn)+ρˉ​, where ρˉ\bar\rhoρˉ​ is the larger error at AmA^mAm and Am,ϵA^{m,\epsilon}Am,ϵ.

Significance

Theorem 4.1 is the abstract step behind the paper's explicit multiplier bootstrap rates: Proposition 4.1 combines it with maximal inequalities that bound Δn(A)\Delta_n(\mathcal A)Δn​(A) with high probability, and obtains, with probability at least 1−α1-\alpha1−α, the rate (Bn2log⁡5(pn)log⁡2(1/α)/n)1/6(B_n^2\log^5(pn)\log^2(1/\alpha)/n)^{1/6}(Bn2​log5(pn)log2(1/α)/n)1/6 for simple convex sets with sparse facet normals. In applications it justifies bootstrap critical values for max-type statistics and simultaneous confidence regions when p≫np\gg np≫n. Remark 4.1, the hyperrectangle case, is the version most used in practice.

The results are proved on paper; none is formalized on the platform. A formal development produces machine-checked versions of the smooth-max sandwich, a Gaussian anti-concentration bound (Nazarov's inequality), a quantitative Gaussian comparison inequality and the bootstrap theorem itself. The comparison display and Lemma A.1 are proved in the paper only by citation ([20] and Klivans–O'Donnell–Servedio, Thm. 20), so formal proofs of them are new work rather than transcriptions.

Difficulty

The obvious route compares SneXS^{eX}_nSneX​ and SnYS^Y_nSnY​ through the Kolmogorov distance of their laws or through a total-variation bound between two Gaussians. Both depend polynomially on ppp and fail when p≫np\gg np≫n. The proof instead compares smooth functionals of the coordinatewise maximum, where the error depends on ppp only through β∼log⁡p\beta\sim\log pβ∼logp, and then converts back to probabilities of orthants with an anti-concentration inequality whose constant grows like log⁡p\sqrt{\log p}logp​. Both conversions must hold uniformly in the threshold yyy, and the final bound for simple convex sets requires passing to the mmm-dimensional vectors (v′Xi)v∈V(v'X_i)_{v\in\mathcal V}(v′Xi​)v∈V​ with m≤(pn)dm\le(pn)^dm≤(pn)d, which is why log⁡(pn)\log(pn)log(pn) appears. The comparison inequality for g∘Fβg\circ F_\betag∘Fβ​ is the step with the least existing infrastructure: it is a Slepian–Stein interpolation between two Gaussian laws with explicit control of second derivatives of FβF_\betaFβ​.

Formalization scope

  • Vectors live in EuclideanSpace ℝ (Fin p); N(0,Σ)N(0,\Sigma)N(0,Σ) is Mathlib's multivariateGaussian 0 Σ. Independence is iIndepFun; YiY_iYi​'s law is fixed by P.map (Y i) = multivariateGaussian 0 (covMat P (X i)), and square integrability of each XijX_{ij}Xij​ makes covMat positive semidefinite, so this is the genuine Gaussian law.
  • n≥4n\ge4n≥4 and p≥3p\ge3p≥3 (the paper's standing assumption) are hypotheses of every theorem.
  • P(⋅∣X1n)P(\cdot\mid X_1^n)P(⋅∣X1n​) is read per realization: the bootstrap law mbLaw x is the push-forward of N(0,1)⊗nN(0,1)^{\otimes n}N(0,1)⊗n under e↦n−1/2∑iei(xi−xˉ)e\mapsto n^{-1/2}\sum_ie_i(x_i-\bar x)e↦n−1/2∑i​ei​(xi​−xˉ), and the bound is asserted at every ω\omegaω on the event, for the data X(ω)X(\omega)X(ω). Since eee is independent of the data, this is a version of the conditional law; no conditional expectation appears.
  • Suprema over the class, over v1,v2v_1,v_2v1​,v2​ and over hyperrectangles are encoded as bounds for every member.
  • The class A\mathcal AA is an indexed family of measurable sets, each with its approximating polyhedron given by a finite set of unit vectors and real thresholds. The page uses facet normals and support values; allowing any finite family of unit vectors is a mild generalization that implies the page's theorem.
  • Constants: CCC is quantified after a,b,da,b,da,b,d (after bbb alone for (38), (39), Lemma A.1 and the smoothed step) and before nnn, ppp, the probability space, the data, the class, Δˉn\bar\Delta_nΔˉn​ and the realization. A constant chosen after nnn or ppp would trivialize the goal.
  • Moments enter only through lower bounds ((M.1), (M.1′)) on integrals of square-integrable functions, so no integral takes a default value; the comparison display integrates continuous functions of linear growth against Gaussian laws. The goal does not mention FβF_\betaFβ​, ggg, ϱnMB\varrho_n^{MB}ϱnMB​, (38) or (39).

Infrastructure needed: multivariate Gaussian laws and their linear images, Gaussian integration by parts or Slepian interpolation, Nazarov's inequality, and properties of log-sum-exp. Lemma A.1, display (21) and the comparison display are reusable beyond this mission, for the high-dimensional CLT of the companion mission and for any max-type Gaussian approximation. Proofs of any milestone are welcome, as are proofs of the conditional Gaussianity identity from Mathlib's Gaussian API.

Selected references

  • V. Chernozhukov, D. Chetverikov, K. Kato, Central limit theorems and bootstrap in high dimensions, Ann. Probab. 45(4):2309–2352, 2017. https://doi.org/10.1214/16-AOP1113
  • V. Chernozhukov, D. Chetverikov, K. Kato, Comparison and anti-concentration bounds for maxima of Gaussian random vectors, Probab. Theory Related Fields 162:47–70, 2015. https://doi.org/10.1007/s00440-014-0565-9
  • V. Chernozhukov, D. Chetverikov, K. Kato, Gaussian approximations and multiplier bootstrap for maxima of sums of high-dimensional random vectors, Ann. Statist. 41(6):2786–2819, 2013. https://doi.org/10.1214/13-AOS1161
  • A. Klivans, R. O'Donnell, R. Servedio, Learning geometric concepts via Gaussian surface area, FOCS 2008. https://doi.org/10.1109/FOCS.2008.64
  • F. Nazarov, On the maximal perimeter of a convex set in ℝⁿ with respect to a Gaussian measure, Geometric Aspects of Functional Analysis, Lecture Notes in Math. 1807, 169–187, 2003. https://doi.org/10.1007/978-3-540-36428-3_14
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ProbabilityStatistics·Captain: mikedeng1

Central Limit Theorems and Bootstrap in High Dimensions 1: Gaussian Approximation of Normalized Sums over All Hyperrectangles with Error K₁[(L̄ₙ² log⁷p/n)^{1/6} + Mₙ(φₙ)/L̄ₙ]Research Paper

Motivation

Many statistical procedures look at a large number of averages at once: simultaneous confidence intervals for ppp means, multiple testing of ppp hypotheses, the maximum of ppp ttt-statistics. Their calibration needs the joint law of a ppp-dimensional normalized sum, and in modern applications ppp is comparable to, or much larger than, the sample size nnn. Classical multivariate central limit theorems with explicit error, such as Bentkus's bound over convex sets (Bentkus 2003), require ppp to grow slowly with nnn (roughly p=o(n1/7)\sqrt p = o(n^{1/7})p​=o(n1/7)), which rules out these applications.

Chernozhukov, Chetverikov and Kato showed that when the class of sets is restricted to hyperrectangles, the Gaussian approximation error depends on the dimension only through log⁡p\log plogp (Ann. Probab. 45 (2017)).

Timeline. In 2013 the same authors proved a Gaussian approximation for the maximum of a sum (sets of the form {w:wj≤a ∀j}\{w : w_j \le a \ \forall j\}{w:wj​≤a ∀j}) with rate n−1/8n^{-1/8}n−1/8 (Ann. Statist. 41 (2013)). The 2017 paper extends this to all hyperrectangles, improves the rate to n−1/6n^{-1/6}n−1/6, and adds bootstrap results.

Setting

Let n≥4n \ge 4n≥4 and p≥3p \ge 3p≥3. Let X1,…,XnX_1, \dots, X_nX1​,…,Xn​ be independent random vectors in Rp\mathbb R^pRp with coordinates XijX_{ij}Xij​, each centred (E[Xij]=0\mathrm E[X_{ij}] = 0E[Xij​]=0) with E[Xij2]<∞\mathrm E[X_{ij}^2] < \inftyE[Xij2​]<∞. Let Y1,…,YnY_1, \dots, Y_nY1​,…,Yn​ be independent centred Gaussian vectors with Yi∼N(0,E[XiXi′])Y_i \sim N(0, \mathrm E[X_iX_i'])Yi​∼N(0,E[Xi​Xi′​]), the same covariance as XiX_iXi​. The normalized sums are

SnX:=1n∑i=1nXi,SnY:=1n∑i=1nYi.S^X_n := \frac{1}{\sqrt n}\sum_{i=1}^n X_i, \qquad S^Y_n := \frac{1}{\sqrt n}\sum_{i=1}^n Y_i.SnX​:=n​1​i=1∑n​Xi​,SnY​:=n​1​i=1∑n​Yi​.

A hyperrectangle is a set A={w∈Rp:aj≤wj≤bj for all j}A = \{w \in \mathbb R^p : a_j \le w_j \le b_j \text{ for all } j\}A={w∈Rp:aj​≤wj​≤bj​ for all j} with −∞≤aj≤bj≤∞-\infty \le a_j \le b_j \le \infty−∞≤aj​≤bj​≤∞; Are\mathcal A^{\mathrm{re}}Are is the class of all of them. The quantity to bound is

ρn(Are):=sup⁡A∈Are∣P(SnX∈A)−P(SnY∈A)∣.\rho_n(\mathcal A^{\mathrm{re}}) := \sup_{A \in \mathcal A^{\mathrm{re}}}\big|\mathrm P(S^X_n \in A) - \mathrm P(S^Y_n \in A)\big|.ρn​(Are):=A∈Aresup​​P(SnX​∈A)−P(SnY​∈A)​.

The error is measured through the third-moment parameter Ln:=max⁡jn−1∑iE∣Xij∣3L_n := \max_j n^{-1}\sum_i \mathrm E|X_{ij}|^3Ln​:=maxj​n−1∑i​E∣Xij​∣3 and the truncated maximal moments

Mn,X(ϕ):=1n∑i=1nE[max⁡j∣Xij∣3 1{max⁡j∣Xij∣>n4ϕlog⁡p}],M_{n,X}(\phi) := \frac1n\sum_{i=1}^n \mathrm E\Big[\max_j|X_{ij}|^3\,1\Big\{\max_j|X_{ij}| > \frac{\sqrt n}{4\phi\log p}\Big\}\Big],Mn,X​(ϕ):=n1​i=1∑n​E[jmax​∣Xij​∣31{jmax​∣Xij​∣>4ϕlogpn​​}],

Mn,Y(ϕ)M_{n,Y}(\phi)Mn,Y​(ϕ) the same with YYY, and Mn(ϕ):=Mn,X(ϕ)+Mn,Y(ϕ)M_n(\phi) := M_{n,X}(\phi) + M_{n,Y}(\phi)Mn​(ϕ):=Mn,X​(ϕ)+Mn,Y​(ϕ). Here log⁡\loglog is the natural logarithm.

Formalization targets

Goal: Theorem 2.1

If n−1∑iE[Xij2]≥b>0n^{-1}\sum_i \mathrm E[X_{ij}^2] \ge b > 0n−1∑i​E[Xij2​]≥b>0 for all jjj, there are constants K1,K2>0K_1, K_2 > 0K1​,K2​>0 depending only on bbb such that for every Lˉn≥Ln\bar L_n \ge L_nLˉn​≥Ln​,

ρn(Are)≤K1[(Lˉn2log⁡7pn)1/6+Mn(ϕn)Lˉn],ϕn:=K2(Lˉn2log⁡4pn)−1/6.\rho_n(\mathcal A^{\mathrm{re}}) \le K_1\left[\left(\frac{\bar L_n^2\log^7 p}{n}\right)^{1/6} + \frac{M_n(\phi_n)}{\bar L_n}\right], \qquad \phi_n := K_2\left(\frac{\bar L_n^2\log^4 p}{n}\right)^{-1/6}.ρn​(Are)≤K1​[(nLˉn2​log7p​)1/6+Lˉn​Mn​(ϕn​)​],ϕn​:=K2​(nLˉn2​log4p​)−1/6.

The constants are left existential, as on the page: the goal asserts the shape of the bound, not particular values.

Milestones

  1. Display (21): the smooth maximum Fβ(w)=β−1log⁡∑jeβ(wj−yj)F_\beta(w) = \beta^{-1}\log\sum_j e^{\beta(w_j - y_j)}Fβ​(w)=β−1log∑j​eβ(wj​−yj​) is within β−1log⁡p\beta^{-1}\log pβ−1logp of max⁡j(wj−yj)\max_j(w_j - y_j)maxj​(wj​−yj​).
  2. Lemma B.1: association inequalities for nondecreasing nonnegative functions, including (20) without independence.
  3. Lemma A.1 (Nazarov's inequality): P(Y≤y+a)−P(Y≤y)≤Calog⁡p\mathrm P(Y \le y + a) - \mathrm P(Y \le y) \le Ca\sqrt{\log p}P(Y≤y+a)−P(Y≤y)≤Calogp​ for a centred Gaussian YYY with E[Yj2]≥b\mathrm E[Y_j^2] \ge bE[Yj2​]≥b.
  4. Lemma 5.1, the key lemma: a recursive bound on ϱn:=sup⁡y,v∈[0,1]∣P(vSnX+1−vSnY≤y)−P(SnY≤y)∣\varrho_n := \sup_{y, v\in[0,1]}|\mathrm P(\sqrt v S^X_n + \sqrt{1-v}S^Y_n \le y) - \mathrm P(S^Y_n \le y)|ϱn​:=supy,v∈[0,1]​∣P(v​SnX​+1−v​SnY​≤y)−P(SnY​≤y)∣.
  5. Corollary 5.1: the same bound for ϱn′\varrho_n'ϱn′​, the supremum over hyperrectangles.
  6. Lemma C.1: an exponential tail bound gives E[ξ31{ξ>t}]≤6A(t+B)3e−t/B\mathrm E[\xi^3 1\{\xi > t\}] \le 6A(t+B)^3e^{-t/B}E[ξ31{ξ>t}]≤6A(t+B)3e−t/B.

Companion: Proposition 2.1

Under the moment conditions (M.1)–(M.2) and either an exponential (E.1) or a polynomial (E.2) moment bound with parameter Bn≥1B_n \ge 1Bn​≥1,

ρn(Are)≤C(Bn2log⁡7(pn)n)1/6orρn(Are)≤C{(Bn2log⁡7(pn)n)1/6+(Bn2log⁡3(pn)n1−2/q)1/3}.\rho_n(\mathcal A^{\mathrm{re}}) \le C\Big(\frac{B_n^2\log^7(pn)}{n}\Big)^{1/6} \quad\text{or}\quad \rho_n(\mathcal A^{\mathrm{re}}) \le C\Big\{\Big(\frac{B_n^2\log^7(pn)}{n}\Big)^{1/6} + \Big(\frac{B_n^2\log^3(pn)}{n^{1-2/q}}\Big)^{1/3}\Big\}.ρn​(Are)≤C(nBn2​log7(pn)​)1/6orρn​(Are)≤C{(nBn2​log7(pn)​)1/6+(n1−2/qBn2​log3(pn)​)1/3}.

Significance

The result. Under the exponential moment condition (E.1), Proposition 2.1 makes the Gaussian approximation error tend to zero when Bn2log⁡7(pn)=o(n)B_n^2\log^7(pn) = o(n)Bn2​log7(pn)=o(n), allowing ppp much larger than nnn. Under the polynomial moment condition (E.2), its second error term must also tend to zero. Theorem 2.1 is the probabilistic basis of the paper's multiplier and empirical bootstrap results for simultaneous inference (Chernozhukov, Chetverikov and Kato 2017).

Formalizing it. The result is proved on paper; no machine-checked version of this theorem was found in the platform catalog during this mission's prior-art search. A formal proof needs interpolation between SnXS^X_nSnX​ and SnYS^Y_nSnY​, Gaussian anti-concentration (Nazarov's inequality), and third-order Taylor estimates of smooth approximations of indicator functions. Nazarov's inequality is used in the paper by citation, so its formal proof is a separate milestone.

Difficulty

The obvious route, a Lindeberg replacement of each XiX_iXi​ by YiY_iYi​ after smoothing the indicator of a hyperrectangle coordinate by coordinate, loses a polynomial factor in ppp: the derivatives of a product of ppp smoothed one-dimensional indicators add up over coordinates, so the error grows like a power of ppp rather than of log⁡p\log plogp. Any smoothing must also be paid for by the probability that the Gaussian vector falls in a thin neighbourhood of the boundary of a hyperrectangle, and a dimension-free bound on that probability is not available for general hyperrectangles; the log⁡p\sqrt{\log p}logp​ anti-concentration bound is the best one can use. Finally, a direct comparison yields an inequality in which the quantity to be bounded appears on both sides, and the rate n−1/6n^{-1/6}n−1/6 is obtained only after that inequality is solved; a one-shot estimate gives a worse power of nnn. The truncation in Mn(ϕ)M_n(\phi)Mn​(ϕ) handles coordinates too large for a third-order Taylor expansion, since no moment condition beyond third moments is assumed.

Formalization scope

Vectors live in EuclideanSpace ℝ (Fin p) and the coordinate XijX_{ij}Xij​ is X i ω j. The Gaussian comparison vectors satisfy P.map (Y i) = multivariateGaussian 0 (covMat P (X i)) with covMat P Z = (E[Z_j Z_k])_{j,k}, which is positive semidefinite, so this is the genuine N(0,E[XiXi′])N(0, \mathrm E[X_iX_i'])N(0,E[Xi​Xi′​]); the YiY_iYi​ are independent. Hyperrectangle endpoints are extended reals used only in comparisons. Every theorem carries the standing assumptions n≥4n \ge 4n≥4, p≥3p \ge 3p≥3, independence, centring and finite second moments. Items that involve LnL_nLn​ or MnM_nMn​ add E∣Xij∣3<∞\mathrm E|X_{ij}|^3 < \inftyE∣Xij​∣3<∞; when a third moment is infinite the paper's bounds are vacuous, so this loses nothing. Mn(ϕ)M_n(\phi)Mn​(ϕ) is defined by its formula for every real ϕ\phiϕ, because Theorem 2.1 evaluates it at ϕn\phi_nϕn​, which may be below 111. Lemma 5.1 and Corollary 5.1 assume the YYY's independent of the XXX's, as the definition of ϱn\varrho_nϱn​ does; Theorem 2.1 and Proposition 2.1 do not. A bound on a supremum is stated set by set.

Constants that the paper says depend only on bbb (or on bbb and qqq) are quantified after bbb and before nnn, ppp, the probability space and every random vector; a constant chosen after nnn, ppp or the law would trivialize every statement. Upper bounds on expectations in hypotheses ((M.2), (E.1), (E.2)) and in Lemma C.1's conclusion are lower Lebesgue integrals, so a non-integrable function cannot make a hypothesis hold with a junk value of 000. Dropping the independence of the YiY_iYi​ or using a wrong covariance would make the goal false.

A complete development needs: a multivariate Stein or Slepian interpolation, third-order Taylor expansion with remainder for functions on Rp\mathbb R^pRp, Gaussian integration by parts, and Nazarov's inequality. The anti-concentration and smooth-max lemmas are reusable for any max-type Gaussian approximation, including the bootstrap results of the second mission of this series. Proofs of individual milestones, of Nazarov's inequality in particular, are welcome on their own.

Selected references

  • V. Chernozhukov, D. Chetverikov, K. Kato, Central limit theorems and bootstrap in high dimensions, Ann. Probab. 45(4):2309–2352, 2017. https://doi.org/10.1214/16-AOP1113
  • V. Chernozhukov, D. Chetverikov, K. Kato, Gaussian approximations and multiplier bootstrap for maxima of sums of high-dimensional random vectors, Ann. Statist. 41(6):2786–2819, 2013. https://doi.org/10.1214/13-AOS1161
  • V. Bentkus, On the dependence of the Berry–Esseen bound on dimension, J. Statist. Plann. Inference 113:385–402, 2003. MR1965117, https://mathscinet.ams.org/mathscinet-getitem?mr=1965117
  • F. Nazarov, On the maximal perimeter of a convex set in ℝⁿ with respect to a Gaussian measure, Geometric Aspects of Functional Analysis, Lecture Notes in Math. 1807, 169–187, Springer, 2003. MR2083397, https://mathscinet.ams.org/mathscinet-getitem?mr=2083397
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CombinatoricsOperations ResearchOptimization·Captain: mikedeng1

Scheduling Problems with Two Competing Agents 9: Total Completion Time Against a Maximum Cost Has at Most n_A·n_B + 1 Nondominated PairsResearch Paper

Motivation

Many scheduling decisions are not owned by a single decision maker. A machine shared by two departments, a production line serving two customers, or a computing resource shared by two users must process the jobs of two agents, each of which judges a schedule by its own criterion. Agnetis, Mirchandani, Pacciarelli and Pacifici introduced this model in Scheduling Problems with Two Competing Agents (Operations Research, 2004, doi:10.1287/opre.1030.0092), and it became the starting point of the literature on multi-agent scheduling (surveyed in Agnetis, Billaut, Gawiejnowicz, Pacciarelli and Soukhal, Multiagent Scheduling, Springer, 2014, doi:10.1007/978-3-642-41880-8).

When neither agent can impose its criterion on the other, the natural object to compute is the set of compromises that cannot be improved for one agent without hurting the other: the Pareto frontier. Section 11 of the paper asks how large that frontier can be for each pair of criteria it studies, because the size of the frontier decides whether it can be listed in polynomial time. This mission formalizes the answer for one agent minimizing its total completion time against the other agent's maximum cost.

Setting

Agent AAA owns jobs J1A,…,JnAAJ^A_1,\dots,J^A_{n_A}J1A​,…,JnA​A​ and agent BBB owns jobs J1B,…,JnBBJ^B_1,\dots,J^B_{n_B}J1B​,…,JnB​B​, with nB≥1n_B\ge 1nB​≥1. Every job JjJ_jJj​ has a positive processing time pjp_jpj​, is available at time 000, and is processed without interruption on a single machine that handles one job at a time. Since both criteria below are nondecreasing in completion times, a schedule σ\sigmaσ is a sequence of all nA+nBn_A+n_BnA​+nB​ jobs processed in that order from time 000 without idle time, and Cj(σ)C_j(\sigma)Cj​(σ) denotes the completion time of JjJ_jJj​.

  • Agent AAA wants to minimize its total completion time ∑h=1nAChA(σ)\sum_{h=1}^{n_A} C^A_h(\sigma)∑h=1nA​​ChA​(σ).
  • Each BBB-job has a nondecreasing cost function fkBf^B_kfkB​ of its completion time, and agent BBB wants to minimize its maximum cost fmax⁡B(σ)=max⁡kfkB(CkB(σ))f^B_{\max}(\sigma)=\max_k f^B_k(C^B_k(\sigma))fmaxB​(σ)=maxk​fkB​(CkB​(σ)).

A schedule σ\sigmaσ is nondominated if no schedule σˉ\bar\sigmaσˉ has ∑ChA(σˉ)≤∑ChA(σ)\sum C^A_h(\bar\sigma)\le\sum C^A_h(\sigma)∑ChA​(σˉ)≤∑ChA​(σ) and fmax⁡B(σˉ)≤fmax⁡B(σ)f^B_{\max}(\bar\sigma)\le f^B_{\max}(\sigma)fmaxB​(σˉ)≤fmaxB​(σ) with at least one inequality strict. Its nondominated pair is (∑ChA(σ),fmax⁡B(σ))\bigl(\sum C^A_h(\sigma),f^B_{\max}(\sigma)\bigr)(∑ChA​(σ),fmaxB​(σ)). The constrained problem 1∥∑CiA:fmax⁡B≤Q1\|\sum C^A_i : f^B_{\max}\le Q1∥∑CiA​:fmaxB​≤Q asks for a schedule with fkB(CkB)≤Qf^B_k(C^B_k)\le QfkB​(CkB​)≤Q for every BBB-job that minimizes ∑ChA\sum C^A_h∑ChA​ among such schedules; such a schedule is optimal for the bound QQQ.

The AAA-jobs of a schedule follow the SPT order when they appear by nondecreasing processing time, equal lengths in index order. A BBB-job overtakes an AAA-job when it moves from after it to before it.

Formalization targets

Goal: Theorem 11.6, corrected

∣{(∑ChA(σ), fmax⁡B(σ)):σ nondominated}∣ ≤ nA nB+1.\bigl|\{(\textstyle\sum C^A_h(\sigma),\,f^B_{\max}(\sigma)) : \sigma\ \text{nondominated}\}\bigr|\ \le\ n_A\,n_B+1.​{(∑ChA​(σ),fmaxB​(σ)):σ nondominated}​ ≤ nA​nB​+1.

The paper prints the bound nAnBn_An_BnA​nB​. That bound is false: with one job per agent, unit processing times and fB(t)=tf^B(t)=tfB(t)=t, the schedules ABABAB and BABABA give the two nondominated pairs (1,2)(1,2)(1,2) and (2,1)(2,1)(2,1). The corrected bound nAnB+1n_An_B+1nA​nB​+1 is the one the printed argument supports.

Milestones

  1. Lemma 5.4 (p. 234): if no BBB-job can complete last within the bound, every optimal schedule ends with a longest AAA-job. This is the reason the AAA-jobs of optimal schedules are in SPT order.
  2. Lemma 11.4 (p. 240): for Q′<QQ'<QQ′<Q and optimal schedules σ,σ′\sigma,\sigma'σ,σ′ for QQQ and Q′Q'Q′ whose AAA-jobs follow the SPT order, Cj(σ′)≥Cj(σ)C_j(\sigma')\ge C_j(\sigma)Cj​(σ′)≥Cj​(σ) for every AAA-job jjj.
  3. Lemma 11.5 (p. 240): under the same hypotheses, if a BBB-job precedes an AAA-job in σ\sigmaσ, it precedes it also in σ′\sigma'σ′.

Significance

A frontier of size at most nAnB+1n_An_B+1nA​nB​+1 means that the scheme the paper calls PP, which solves the constrained problem for a decreasing sequence of bounds, lists every nondominated pair with polynomially many calls to a polynomial algorithm (Theorem 5.5 of the paper). The contrast with the other criteria of §11 is the point: for two total-completion-time agents the paper exhibits an exponential frontier (Example 11.7). The bound therefore separates criteria whose compromises can be negotiated over an explicit list from those where they cannot.

Formalizing it adds three things. First, the printed statements need corrections: the bound is off by one, and Lemmas 11.4 and 11.5 are false when identical AAA-jobs may be ordered differently in the two schedules. A machine-checked version fixes the exact hypotheses. Second, the monotonicity of overtakes (Lemma 11.5) is a reusable structural fact about parametric scheduling under a tightening constraint. Third, no part of this paper or of two-agent scheduling has been machine-checked before, to our knowledge; the published sequence model the mission builds on comes from the formalization of Moore's 1968 algorithm.

Difficulty

The obvious argument counts overtakes: as the bound decreases, each BBB-job overtakes each AAA-job at most once, so consecutive frontier points differ by at least one new overtake. The step that does not go through as printed is "at most once". Optimal schedules for a given bound are not unique, and two optimal schedules can disagree on the order of identical AAA-jobs and on the position of a BBB-job between them. Then an "overtake" can be undone between two bounds without any change in the objectives. The counting is valid only for a consistently chosen family of schedules, and turning the comparison of optimal schedules for two different bounds into a strict improvement needs an exchange argument with careful bookkeeping of which jobs shift. A second, smaller gap is the base case: the first schedule of the chain carries no overtake and must be counted separately.

Formalization scope

Jobs are Fin nA ⊕ Fin nB, 0-based, and a schedule is a duplicate-free list of all jobs; completion times come from the published definition MooreLateJobs.Shared.completionTime (Moore 1968 series), referenced rather than redefined. Processing times are real and strictly positive, the paper's standing convention, which the exchange arguments use. The bound QQQ is real; the paper's integer QQQ is a special case. Feasibility for the bound is stated job by job. The maximum cost fmax⁡Bf^B_{\max}fmaxB​ is a finite maximum and requires nB≥1n_B\ge 1nB​≥1.

Explicit readings of the paper's phrases:

  • "Nondominated schedules" in Theorem 11.6 is read as nondominated pairs, one schedule per pair, as §11 defines the set it enumerates. Counting schedules would count swaps of identical jobs separately.
  • The count is Set.encard of a set of real pairs, so the goal asserts finiteness as well as the bound; it is not a Set.ncard, which would be 000 on an infinite set.
  • "The AAA-jobs are always SPT ordered" (p. 240) is read as the SPT order with ties broken by index, imposed as a hypothesis on both schedules in Lemmas 11.4 and 11.5. Without a fixed tie-break both lemmas are false.
  • Lemma 5.4 is restated with nA≥1n_A\ge 1nA​≥1, since an empty schedule has no last job. It is also a milestone of mission 3 of this series and is restated here identically because draft items cannot import each other.

Nothing in the statements is trivial by construction. The goal is about every instance with positive data, its hypotheses are satisfiable, and the counterexample to the printed bound is checked in Lean. The milestones' SPT hypotheses are met by some optimal schedule of every feasible instance, so they are not vacuous. Running times, including the polynomiality of PP and the choice of the decrement ϵ\epsilonϵ in Figure 4, are not formalized.

A complete development needs exchange lemmas for single-machine sequences (moving a job, swapping two adjacent jobs, and their effect on completion times), the existence of SPT-ordered optimal schedules, and a chain-counting argument for nested sets of overtakes. The exchange lemmas are reusable for any single-machine sequencing mission. Contributions of any of these, and of a proof of the corrected bound that avoids the scheme PP, are welcome.

Selected references

  • A. Agnetis, P. B. Mirchandani, D. Pacciarelli, A. Pacifici, Scheduling Problems with Two Competing Agents, Operations Research 52(2), 229–242, 2004. https://doi.org/10.1287/opre.1030.0092
  • J. M. Moore, An n Job, One Machine Sequencing Algorithm for Minimizing the Number of Late Jobs, Management Science 15(1), 102–109, 1968. https://doi.org/10.1287/mnsc.15.1.102
  • A. Agnetis, J.-C. Billaut, S. Gawiejnowicz, D. Pacciarelli, A. Soukhal, Multiagent Scheduling: Models and Algorithms, Springer, 2014. https://doi.org/10.1007/978-3-642-41880-8
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Operations ResearchOptimization·Captain: mikedeng1

Semismooth and Semiconvex Functions in Constrained Optimization III: With Semiconvex Problem Functions, a Stationary Point Is Optimal Unless There Is No Strictly Feasible PointResearch Paper

Motivation

Many constrained optimization problems in operations research have objective and constraint functions that are continuous but not differentiable: maxima of finitely many smooth functions, value functions of inner optimization problems, piecewise-linear costs. For such problems the classical Karush–Kuhn–Tucker theory does not apply directly, and algorithms need a nonsmooth replacement for the condition "the gradient of the Lagrangian vanishes". R. Mifflin's report Semismooth and semiconvex functions in constrained optimization (IIASA RR-76-21, 1976; SIAM J. Control Optim. 15(6), 1977) supplies one. It introduces a point-to-set map MMM built from Clarke's generalized gradients and shows, in §5, that 0∈M(xˉ)0 \in M(\bar x)0∈M(xˉ) is necessary for optimality of locally Lipschitz problems and, for a class of semiconvex functions, also sufficient as soon as a strictly feasible point exists. The map MMM goes back to Merrill's fixed-point work on differentiable and convex problems; Mifflin's own algorithm for semismooth problems converges to points satisfying 0∈M(xˉ)0 \in M(\bar x)0∈M(xˉ), so the sufficiency result says when such points are actual minimizers.

This mission is the third of three on the report. Mission I treats pointwise maxima of compact families of smooth functions, mission II the chain rule for semismooth compositions.

Setting

Write Rn\mathbb R^nRn for Euclidean space with inner product ⟨⋅,⋅⟩\langle\cdot,\cdot\rangle⟨⋅,⋅⟩. For F:Rn→RF:\mathbb R^n\to\mathbb RF:Rn→R, a point xxx and a direction ddd, the generalized directional derivative is

F0(x;d)=lim sup⁡h→0, t↓0F(x+h+td)−F(x+h)t,F^0(x;d)=\limsup_{h\to 0,\ t\downarrow 0}\frac{F(x+h+td)-F(x+h)}{t},F0(x;d)=h→0, t↓0limsup​tF(x+h+td)−F(x+h)​,

and the generalized gradient is the set ∂F(x)={g:⟨g,d⟩≤F0(x;d) for all d}\partial F(x)=\{g:\langle g,d\rangle\le F^0(x;d)\text{ for all }d\}∂F(x)={g:⟨g,d⟩≤F0(x;d) for all d}. When lim⁡t↓0[F(x+td)−F(x)]/t\lim_{t\downarrow 0}[F(x+td)-F(x)]/tlimt↓0​[F(x+td)−F(x)]/t exists it is the directional derivative F′(x;d)F'(x;d)F′(x;d); FFF is quasidifferentiable at xxx if F′(x;d)F'(x;d)F′(x;d) exists and equals F0(x;d)F^0(x;d)F0(x;d) for every ddd.

Let X⊆RnX\subseteq\mathbb R^nX⊆Rn. FFF is semiconvex at x∈Xx\in Xx∈X with respect to XXX (Definition 2) if (a) FFF is Lipschitz on a ball about xxx, (b) FFF is quasidifferentiable at xxx, and (c) x+d∈Xx+d\in Xx+d∈X and F′(x;d)≥0F'(x;d)\ge 0F′(x;d)≥0 imply F(x+d)≥F(x)F(x+d)\ge F(x)F(x+d)≥F(x). It is semiconvex on XXX if this holds at every point of XXX. Convex functions and differentiable pseudoconvex functions are semiconvex.

The problem of §5 is to minimize f(x)f(x)f(x) subject to h(x)≤0h(x)\le 0h(x)≤0, where h(x)=max⁡1≤i≤mhi(x)h(x)=\max_{1\le i\le m}h_i(x)h(x)=max1≤i≤m​hi​(x). A point is feasible if h(x)≤0h(x)\le 0h(x)≤0 and strictly feasible if h(x)<0h(x)<0h(x)<0; xˉ\bar xxˉ is optimal if it is feasible and f(xˉ)≤f(x)f(\bar x)\le f(x)f(xˉ)≤f(x) for every feasible xxx. The map MMM is

M(x)={∂f(x)h(x)<0,conv⁡{∂f(x)∪∂h(x)}h(x)=0,∂h(x)h(x)>0,M(x)=\begin{cases}\partial f(x) & h(x)<0,\\ \operatorname{conv}\{\partial f(x)\cup\partial h(x)\} & h(x)=0,\\ \partial h(x) & h(x)>0,\end{cases}M(x)=⎩⎨⎧​∂f(x)conv{∂f(x)∪∂h(x)}∂h(x)​h(x)<0,h(x)=0,h(x)>0,​

and xˉ\bar xxˉ is stationary if h(xˉ)≤0h(\bar x)\le 0h(xˉ)≤0 and 0∈M(xˉ)0\in M(\bar x)0∈M(xˉ). In Lean these are genGrad, HasDirDeriv, QuasidiffAt, SemiconvexAt/SemiconvexOn, IsFeasible, IsOptimal, Mmap and IsStationary in the namespace MifflinSemismooth.Optimality; F0F^0F0 is the published ClarkeGradients.Shared.genDirDeriv.

Formalization targets

Goal: Theorem 9 (p. 20)

Suppose fff and hhh are semiconvex on Rn\mathbb R^nRn and 0∈M(xˉ)0\in M(\bar x)0∈M(xˉ). Then

h(xˉ)>0 ⟹ h(x)≥h(xˉ)>0  for all x,h(\bar x)>0\ \Longrightarrow\ h(x)\ge h(\bar x)>0\ \text{ for all }x,h(xˉ)>0 ⟹ h(x)≥h(xˉ)>0  for all x, h(xˉ)≤0 ⟹ xˉ is optimal, or h(x)≥0 for all x.h(\bar x)\le 0\ \Longrightarrow\ \bar x\text{ is optimal, or } h(x)\ge 0\text{ for all }x.h(xˉ)≤0 ⟹ xˉ is optimal, or h(x)≥0 for all x.

The first alternative says the problem is infeasible, the last that it has no strictly feasible point. The theorem carries no constants and holds for any constraint function hhh, not only a finite maximum.

Milestones

The proof uses, in order: a point with 0∈∂F(xˉ)0\in\partial F(\bar x)0∈∂F(xˉ) minimizes a semiconvex FFF over Rn\mathbb R^nRn (p. 20); on the boundary h(xˉ)=0h(\bar x)=0h(xˉ)=0, the condition 0∈M(xˉ)0\in M(\bar x)0∈M(xˉ) yields λ∈[0,1]\lambda\in[0,1]λ∈[0,1], gˉ∈∂f(xˉ)\bar g\in\partial f(\bar x)gˉ​∈∂f(xˉ), g^∈∂h(xˉ)\hat g\in\partial h(\bar x)g^​∈∂h(xˉ) with λgˉ+(1−λ)g^=0\lambda\bar g+(1-\lambda)\hat g=0λgˉ​+(1−λ)g^​=0 (p. 20); Proposition 1(b), F0(x;d)=max⁡{⟨g,d⟩:g∈∂F(x)}F^0(x;d)=\max\{\langle g,d\rangle:g\in\partial F(x)\}F0(x;d)=max{⟨g,d⟩:g∈∂F(x)} (p. 3); Theorem 8, for FFF semiconvex on a convex XXX, F(x+d)≤F(x)F(x+d)\le F(x)F(x+d)≤F(x) implies F′(x;d)≤0F'(x;d)\le 0F′(x;d)≤0 (p. 19); and, if λ>0\lambda>0λ>0, ⟨gˉ,x−xˉ⟩≥0\langle\bar g,x-\bar x\rangle\ge 0⟨gˉ​,x−xˉ⟩≥0 for every feasible xxx (p. 21).

Companion results

Theorem 7 (p. 18): for locally Lipschitz f,hf,hf,h, an optimal point is stationary. Theorem 6 (p. 17): for locally Lipschitz h1,…,hmh_1,\dots,h_mh1​,…,hm​, h=max⁡ihih=\max_i h_ih=maxi​hi​ is locally Lipschitz with ∂h(x)⊆conv⁡⋃i∈A(x)∂hi(x)\partial h(x)\subseteq\operatorname{conv}\bigcup_{i\in A(x)}\partial h_i(x)∂h(x)⊆conv⋃i∈A(x)​∂hi​(x), where A(x)={i:h(x)=hi(x)}A(x)=\{i:h(x)=h_i(x)\}A(x)={i:h(x)=hi​(x)}; semismoothness, semiconvexity and quasidifferentiability on XXX pass from the hih_ihi​ to hhh, and in the last two cases the inclusion is an equality at points of XXX.

Significance

Theorems 7 and 9 together give a nonsmooth Karush–Kuhn–Tucker theory: for semiconvex problem functions with a strictly feasible point, stationarity in the sense of MMM is equivalent to global optimality. For differentiable functions this recovers the sufficiency of the Fritz John conditions for pseudoconvex objectives and constraints (Mangasarian, Nonlinear Programming, Theorem 10.1.1); for convex functions it recovers the saddle-point characterization. Since Mifflin's algorithm produces stationary points, Theorem 9 is the certificate that turns its output into a global minimizer. Theorem 6 lets the constraint max⁡ihi≤0\max_i h_i\le 0maxi​hi​≤0 stand for a finite system hi≤0h_i\le 0hi​≤0.

The results are proved in the report. None of them, and neither the notion of semiconvexity nor the map MMM, has a machine-checked proof on Prove2Me or in Mathlib as far as the platform search shows; Mathlib has no Clarke generalized gradient. The work is to formalize the known proofs, which also produces reusable facts about ∂F\partial F∂F (nonemptiness, compactness, the max formula) and about semiconvex functions on convex sets.

Difficulty

The case analysis of Theorem 9 is short; the weight sits in its ingredients. Theorem 8 is the delicate step. Semiconvexity constrains FFF only along directions where F′(x;d)≥0F'(x;d)\ge 0F′(x;d)≥0, so it says nothing directly about a direction along which FFF does not increase; and a mean value inequality along the segment from xxx to x+dx+dx+d ignores quasidifferentiability and does not determine the sign of F′(x;d)F'(x;d)F′(x;d). Proposition 1(b) is an attainment statement for a sublinear function whose finiteness rests on the Lipschitz hypothesis, and it fails for the real-valued limsup without that hypothesis. The convex-combination step depends on ∂f(xˉ)\partial f(\bar x)∂f(xˉ) and ∂h(xˉ)\partial h(\bar x)∂h(xˉ) being nonempty and convex: the convex hull of a union of two sets need not consist of two-point combinations otherwise. Theorem 7 needs M(xˉ)M(\bar x)M(xˉ) to be closed, which in the boundary case is a statement about the convex hull of two compact sets.

Formalization scope

Rn\mathbb R^nRn is EuclideanSpace ℝ (Fin n). F0F^0F0 is a real limsup and equals 000 when the difference quotient is unbounded; every statement therefore has a Lipschitz hypothesis at the points where F0F^0F0 or ∂F\partial F∂F is used, and semiconvexity includes "Lipschitz on a ball". ∂F\partial F∂F is the paper's support-set definition, not the hull of gradient limits. F′(x;d)F'(x;d)F′(x;d) is a relation (HasDirDeriv), never a function with a default value, so Definition 2(c) cannot hold vacuously. "Semiconvex on Rn\mathbb R^nRn" means with respect to X=RnX=\mathbb R^nX=Rn. "max" is IsGreatest, which asserts attainment. Lipschitz constants are nonnegative reals, which is equivalent to the page's positive constants.

The goal, Theorems 7, 8 and 9 are stated for an arbitrary constraint function hhh; the paper's h=max⁡ihih=\max_i h_ih=maxi​hi​ is the special case maxConstraint hs with m≥1m\ge 1m≥1, and Theorem 6 is the bridge. Theorem 9's hypothesis is 0∈M(xˉ)0\in M(\bar x)0∈M(xˉ) alone, without feasibility. Theorem 6(c) as printed asserts ∂h(x)=conv⁡⋃i∈A(x)∂hi(x)\partial h(x)=\operatorname{conv}\bigcup_{i\in A(x)}\partial h_i(x)∂h(x)=conv⋃i∈A(x)​∂hi​(x) "for each x∈Rnx\in\mathbb R^nx∈Rn"; that is false when X≠RnX\neq\mathbb R^nX=Rn (h1=−∣x∣h_1=-|x|h1​=−∣x∣, h2=−2∣x∣h_2=-2|x|h2​=−2∣x∣, X=(1,2)X=(1,2)X=(1,2), x=0x=0x=0), so it is stated for x∈Xx\in Xx∈X. A formalization with the hull-of-limits ∂\partial∂, a junk-valued F′F'F′, a feasibility hypothesis added to Theorem 9, or semiconvexity with respect to a smaller set would prove a different and weaker theorem, and is ruled out.

A complete development needs the basic theory of the generalized gradient (Proposition 1(a), (b)), a Lebourg-type mean value theorem for case analysis along segments, and the finite-max rule. These are reusable beyond this mission, by missions I and II of the series in particular. Proofs of the milestones in any order are welcome, as are proofs of Proposition 1(a) as an auxiliary lemma.

Selected references

  • R. Mifflin, Semismooth and semiconvex functions in constrained optimization, IIASA Research Report RR-76-21, December 1976, https://pure.iiasa.ac.at/id/eprint/524/ ; journal version: SIAM J. Control Optim. 15(6) (1977) 959–972, https://doi.org/10.1137/0315061
  • F. H. Clarke, Generalized gradients and applications, Trans. Amer. Math. Soc. 205 (1975) 247–262. https://doi.org/10.1090/S0002-9947-1975-0367131-6
  • O. L. Mangasarian, Nonlinear Programming, McGraw-Hill, 1969 (SIAM Classics reprint 1994). https://doi.org/10.1137/1.9781611971255
  • G. Lebourg, Valeur moyenne pour gradient généralisé, C. R. Acad. Sci. Paris Sér. A 281 (1975) 795–797.
  • B. N. Pshenichnyi, Necessary Conditions for an Extremum, Marcel Dekker, 1971.
10 thms1 active userReviewed
AnalysisOptimization·Captain: mikedeng1

Semismooth and Semiconvex Functions in Constrained Optimization II: A Semismooth Composition of Semismooth Functions Is Semismooth, with a Chain Rule for Generalized GradientsResearch Paper

Why composition matters

Optimization models often build an objective from several intermediate quantities: constraints, penalties, and transformed measurements are evaluated first, then combined by an outer function. These intermediate and outer functions can be Lipschitz without being differentiable at the point of interest. Ordinary differentiation supplies no chain rule there. The generalized-gradient framework gives a set of possible first-order slopes, while semismoothness provides stronger directional behavior along sequences approaching the point. Mifflin's IIASA report asks whether this behavior survives such compositions and how the generalized gradient of the result relates to those of its ingredients.

The report first establishes basic properties of the generalized gradient in §2, including almost-everywhere differentiability and a nonsmooth mean value theorem. Section 4 then states a chain-rule inclusion as Theorem 4 and the semismooth composition result as Theorem 5. The report is dated December 1976; a journal version appeared in 1977. The mission cites theorem numbers and pages from the report version throughout. No claim about differences between the report and journal texts is needed here.

Setting and definitions

Work in finite-dimensional Euclidean spaces. Let fi:Rn→Rf_i:\mathbb R^n\to\mathbb Rfi​:Rn→R, for i=1,…,mi=1,\ldots,mi=1,…,m, be component functions, and let E:Rm→RE:\mathbb R^m\to\mathbb RE:Rm→R be an outer function. Define the component map YYY and the composite FFF by

Y(x)=(f1(x),…,fm(x)),F(x)=E(Y(x)).Y(x)=(f_1(x),\ldots,f_m(x)),\qquad F(x)=E(Y(x)).Y(x)=(f1​(x),…,fm​(x)),F(x)=E(Y(x)).

The functions are locally Lipschitz in the report's precise sense: on each bounded subset of their Euclidean domain they have a finite Lipschitz constant. For a scalar function HHH, a point xxx, and a direction ddd, the generalized directional derivative H0(x;d)H^0(x;d)H0(x;d) is the joint upper limit of [H(x+h+td)−H(x+h)]/t[H(x+h+td)-H(x+h)]/t[H(x+h+td)−H(x+h)]/t as h→0h\to0h→0 and t↓0t\downarrow0t↓0. Its associated generalized gradient is the support set

∂H(x)={g:⟨g,d⟩≤H0(x;d) for every direction d}.\partial H(x)=\{g:\langle g,d\rangle\le H^0(x;d)\text{ for every direction }d\}.∂H(x)={g:⟨g,d⟩≤H0(x;d) for every direction d}.

This is the definition used in Mifflin's report, not an identification assumed in advance with a hull of ordinary gradient limits. Proposition 1(c) supplies that identification under the paper's Lipschitz assumption. The ordinary one-sided directional derivative H′(x;d)H'(x;d)H′(x;d) is the limit of [H(x+td)−H(x)]/t[H(x+td)-H(x)]/t[H(x+td)−H(x)]/t for t↓0t\downarrow0t↓0, when that limit exists.

Mifflin calls HHH semismooth at xxx if it is Lipschitz on a ball about xxx and the scalar sequence ⟨gk,d⟩\langle g_k,d\rangle⟨gk​,d⟩ has exactly one accumulation point whenever tk>0t_k>0tk​>0 tends to zero, θk/tk→0\theta_k/t_k\to0θk​/tk​→0, and gk∈∂H(x+tkd+θk)g_k\in\partial H(x+t_kd+\theta_k)gk​∈∂H(x+tk​d+θk​). The quantification is over every direction and every such sequence. This pointwise condition is Definition 1 of the report, and its link to one-sided directional derivatives is Lemma 2.

To state the chain rule, form the set

G(x)=conv⁡{∑i=1mwigi:gi∈∂fi(x) for every i,w∈∂E(Y(x))}.G(x)=\operatorname{conv}\left\{\sum_{i=1}^{m}w_i g^i:g^i\in\partial f_i(x)\text{ for every }i,\quad w\in\partial E(Y(x))\right\}.G(x)=conv{i=1∑m​wi​gi:gi∈∂fi​(x) for every i,w∈∂E(Y(x))}.

The same www is used across all components. The sum is the action of the report's matrix [g1⋯gm][g^1\cdots g^m][g1⋯gm] on www.

Formalization targets

Generalized-gradient chain rule

Theorem 4 asserts that FFF is locally Lipschitz and that, at every point,

∂F(x)⊆G(x).\partial F(x)\subseteq G(x).∂F(x)⊆G(x).

This is an inclusion, not a general equality. The report gives an example immediately after Theorem 4 in which the inclusion is strict: two identical absolute-value components cancel under an outer difference, while G(0)G(0)G(0) remains larger than ∂F(0)\partial F(0)∂F(0).

Semismooth composition

The goal, Theorem 5, assumes the setting of Theorem 4. If each fif_ifi​ is semismooth at a selected xxx and EEE is semismooth at Y(x)Y(x)Y(x), then

E∘Y is semismooth at x.E\circ Y\text{ is semismooth at }x.E∘Y is semismooth at x.

The conclusion is pointwise. It does not assert semismoothness throughout Rn\mathbb R^nRn from hypotheses at one point. The milestone list contains the chain rule and the source's stated support results: Proposition 2, Lemma 1, Proposition 1(c) and (d), Lemma 2, and the claims (4.2) and (4.11)–(4.12) from the proofs.

What the results provide

Theorem 5 permits composite nonsmooth objectives to be treated within the same semismooth class as their components. Theorem 4 gives a concrete set built from component generalized gradients that contains the composite's generalized gradient. Together, they let later statements about a composite use first-order information from its stated ingredients, subject to the inclusion's possible strictness. These are results proved in Mifflin's report, not open mathematical conjectures.

This mission drafts machine-checkable statements of those known results and their definition layer. The local Lean modules compile with proof placeholders; this staging does not supply machine-checked proofs of the theorems. A complete development would formalize the known arguments or another proof of the same statements. The reusable output would include the support-set generalized gradient, sequence-based semismoothness, the nonsmooth mean value result, and the chain-rule inclusion, all with their source assumptions exposed.

Main difficulty

At a point where FFF is differentiable, the component functions fif_ifi​ need not be differentiable, and the outer function EEE need not be differentiable at Y(x)Y(x)Y(x). The ordinary smooth chain rule therefore cannot simply multiply ordinary gradients. The candidate G(x)G(x)G(x) is a convex set of combinations of generalized gradients; a single chosen combination does not in general describe all nearby limiting slopes. The report's strict-inclusion example also shows why replacing Theorem 4 by equality would be false. For semismoothness, the condition concerns every admissible sequence of generalized gradients near the point, so checking just one path or one gradient selection does not establish Theorem 5.

Formalization scope

The Lean domain is EuclideanSpace ℝ (Fin n) and the outer domain is EuclideanSpace ℝ (Fin m). The report's norm is the Euclidean norm and its pairing is the real inner product. An index of type Fin m represents the mmm components; m=0m=0m=0 is admitted, in which case the component space is a point and the composite is constant. A finite sum represents the column-matrix product. The generalized gradient is defined by all directional support inequalities, so Proposition 1(c) remains a theorem rather than becoming true by definition.

The generalized directional derivative is imported from the published definition matching the report's joint limit. Lean's real limsup has a default value for an unbounded quotient; Lipschitz hypotheses are carried wherever that operation is used. “Locally Lipschitz” is imported as Lipschitzness on every bounded subset, and the explicit constants of §2 use nonnegative reals, equivalent to the report's positive constants by enlarging them. The directional derivative is a relation asserting a limit, so no value is assigned when the limit fails. “Exactly one accumulation point” remains an existence-and-uniqueness assertion about cluster points. The report's tk↓0t_k\downarrow0tk​↓0 means positive convergence to zero, as its proof of Lemma 2 says explicitly. These choices exclude a vacuous formulation that only asks about one convenient sequence or gives a default directional value.

The scope includes the two local definition files and the cited theorem statements, including both conclusions of Theorem 4 and Lemma 2. Proof contributions would need finite-dimensional Lipschitz and differentiability infrastructure, limiting-gradient compactness, convex hull and separation facts, and sequence convergence facts. Results about the alternative Qi–Sun vector-valued semismoothness notion are outside this mission's definition layer.

Selected references

  • R. Mifflin, Semismooth and Semiconvex Functions in Constrained Optimization, IIASA Research Report RR-76-21, December 1976. Report PDF.
  • R. Mifflin, “Semismooth and Semiconvex Functions in Constrained Optimization,” SIAM Journal on Control and Optimization 15(6), 1977. DOI. This mission's page and theorem references are to the IIASA report.
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Control TheoryMachine LearningOperations Research+2·Captain: mikedeng1

Convergence Analysis of Machine Learning for Mean Field Control, Finite Horizon: The N-Agent Discrete-Time Neural-Net Value Is Within O(N^{-1/max(d,4)} + n_in^{-1/(3(d+1))} + √Δt) of the MKV OptimumResearch Paper

Motivation

Mean field control studies the optimal control of a very large population of interacting agents through the limit in which the population is replaced by its distribution. The limit problem is a McKean–Vlasov (MKV) control problem: the dynamics and the cost of a representative agent depend on the law of its own state. Such problems arise in systemic risk, crowd motion, energy management and the planning of large distributed systems; the reference account is Carmona and Delarue, Probabilistic Theory of Mean Field Games with Applications I–II (Springer, 2018).

MKV control problems are rarely solvable in closed form, and grid-based numerical methods suffer from the dimension of the state. A practical alternative is to simulate a finite population on a time grid, parametrize the feedback control by a neural network, and minimize the simulated cost by stochastic gradient descent. Carmona and Laurière, Convergence analysis of machine learning algorithms for the numerical solution of mean field control and games: II — the finite horizon case (Ann. Appl. Probab. 32(6), 2022, doi:10.1214/21-AAP1715), quantify how close this computable proxy is to the true optimum. This mission formalizes the statement of their main result and of the propositions and lemmas its proof is built from.

Setting

Fix a horizon T>0T>0T>0, a state dimension ddd, a control dimension kkk (controls take values in A=RkA=\mathbb R^kA=Rk), an initial law μ0\mu_0μ0​ on Rd\mathbb R^dRd, a drift b(t,x,μ,α)b(t,x,\mu,\alpha)b(t,x,μ,α), a volatility σ(t,x,μ)\sigma(t,x,\mu)σ(t,x,μ) (not controlled), a running cost f(t,x,μ,α)f(t,x,\mu,\alpha)f(t,x,μ,α) and a terminal cost g(x,μ)g(x,\mu)g(x,μ); μ\muμ ranges over P2(Rd)\mathcal P_2(\mathbb R^d)P2​(Rd), the probability measures with finite second moment, compared with the Wasserstein distance W2W_2W2​.

Problem 1 (the MKV problem). On a probability space carrying a ddd-dimensional Wiener process WWW and an independent X0∼μ0X_0\sim\mu_0X0​∼μ0​, minimize over progressively measurable square-integrable controls α∈A\alpha\in\mathbb Aα∈A

J(α)=E[∫0Tf(t,Xt,L(Xt),αt) dt+g(XT,L(XT))],dXt=b(t,Xt,L(Xt),αt) dt+σ(t,Xt,L(Xt)) dWt,J(\alpha)=\mathbb E\Big[\int_0^Tf(t,X_t,\mathcal L(X_t),\alpha_t)\,dt+g(X_T,\mathcal L(X_T))\Big],\qquad dX_t=b(t,X_t,\mathcal L(X_t),\alpha_t)\,dt+\sigma(t,X_t,\mathcal L(X_t))\,dW_t,J(α)=E[∫0T​f(t,Xt​,L(Xt​),αt​)dt+g(XT​,L(XT​))],dXt​=b(t,Xt​,L(Xt​),αt​)dt+σ(t,Xt​,L(Xt​))dWt​,

where L(Xt)\mathcal L(X_t)L(Xt​) is the law of XtX_tXt​.

Problem 3 (the NNN-agent problem). NNN agents with independent Wiener processes WiW^iWi and i.i.d. initial states X0i∼μ0X^i_0\sim\mu_0X0i​∼μ0​ use a common feedback function v(t,x)v(t,x)v(t,x); the law is replaced by the empirical measure μtN=1N∑jδXtj\mu^N_t=\frac1N\sum_j\delta_{X^j_t}μtN​=N1​∑j​δXtj​​, and the cost is JN(v)=1N∑iE[∫0Tf(t,Xti,μtN,v(t,Xti)) dt+g(XTi,μTN)]J^N(v)=\frac1N\sum_i\mathbb E[\int_0^Tf(t,X^i_t,\mu^N_t,v(t,X^i_t))\,dt+g(X^i_T,\mu^N_T)]JN(v)=N1​∑i​E[∫0T​f(t,Xti​,μtN​,v(t,Xti​))dt+g(XTi​,μTN​)].

Problem 2 (the computable proxy). With Δt=T/NT\Delta t=T/N_TΔt=T/NT​ and tn=nΔtt_n=n\Delta ttn​=nΔt, the NNN agents follow the Euler scheme

Xˇtn+1i=Xˇtni+b(tn,Xˇtni,μˇtn,φ(tn,Xˇtni))Δt+σ(tn,Xˇtni,μˇtn)ΔWˇni\check X^i_{t_{n+1}}=\check X^i_{t_n}+b(t_n,\check X^i_{t_n},\check\mu_{t_n},\varphi(t_n,\check X^i_{t_n}))\Delta t+\sigma(t_n,\check X^i_{t_n},\check\mu_{t_n})\Delta\check W^i_nXˇtn+1​i​=Xˇtn​i​+b(tn​,Xˇtn​i​,μˇ​tn​​,φ(tn​,Xˇtn​i​))Δt+σ(tn​,Xˇtn​i​,μˇ​tn​​)ΔWˇni​

with i.i.d. Gaussian increments ΔWˇni∼N(0,Δt Id)\Delta\check W^i_n\sim\mathcal N(0,\Delta t\,I_d)ΔWˇni​∼N(0,ΔtId​), and JˇN(φ)\check J^N(\varphi)JˇN(φ) is the expected time-discretized cost. The feedback φ\varphiφ ranges over Nd+1,nin,kψ\mathbf N^\psi_{d+1,n_{\rm in},k}Nd+1,nin​,kψ​, the one-hidden-layer neural networks from (t,x)∈Rd+1(t,x)\in\mathbb R^{d+1}(t,x)∈Rd+1 to Rk\mathbb R^kRk with ninn_{\rm in}nin​ hidden neurons and activation ψ\psiψ; ψ\psiψ is 2π2\pi2π-periodic, of class C3\mathcal C^3C3, with ψ^1=∫−ππψ(x)e−ix dx≠0\hat\psi_1=\int_{-\pi}^{\pi}\psi(x)e^{-ix}\,dx\ne0ψ^​1​=∫−ππ​ψ(x)e−ixdx=0.

The standing assumptions (§2.2 and Appendix A of the paper) make b,σb,\sigmab,σ affine in (x,μˉ,α)(x,\bar\mu,\alpha)(x,μˉ​,α) (A1), make f,gf,gf,g differentiable in (x,α,μ)(x,\alpha,\mu)(x,α,μ) (in μ\muμ in the sense of the L-derivative) with Lipschitz derivatives (A2)–(A3), make fff strongly convex in α\alphaα (A4), and add the regularity (B1)–(B3), (C1)–(C3). Under them the reduced Hamiltonian b⋅y+fb\cdot y+fb⋅y+f has a minimizer α^(t,x,μ,y)\hat\alpha(t,x,\mu,y)α^(t,x,μ,y), the Pontryagin forward–backward system has a solution (X,Y,Z)(X,Y,Z)(X,Y,Z) with marginal flow μt\mu_tμt​, and Yt=V(t,Xt)Y_t=V(t,X_t)Yt​=V(t,Xt​) for a regular decoupling field VVV. The optimal feedback is v^(t,x)=α^(t,x,μt,V(t,x))\hat v(t,x)=\hat\alpha(t,x,\mu_t,V(t,x))v^(t,x)=α^(t,x,μt​,V(t,x)).

Formalization targets

Goal: Theorem 3 (p. 4070)

inf⁡α∈AJ(α) ≥ inf⁡φ∈Nd+1,nin,kψJˇN(φ)−C(N−1/max⁡(d,4)1+ln⁡(N)1{d=4}+nin−1/(3(d+1))+Δt)\inf_{\alpha\in\mathbb A}J(\alpha)\ \ge\ \inf_{\varphi\in\mathbf N^\psi_{d+1,n_{\rm in},k}}\check J^N(\varphi)-C\Big(N^{-1/\max(d,4)}\sqrt{1+\ln(N)\mathbf 1_{\{d=4\}}}+n_{\rm in}^{-1/(3(d+1))}+\sqrt{\Delta t}\Big)α∈Ainf​J(α) ≥ φ∈Nd+1,nin​,kψ​inf​JˇN(φ)−C(N−1/max(d,4)1+ln(N)1{d=4}​​+nin−1/(3(d+1))​+Δt​)

for a constant CCC depending only on the data and on ψ\psiψ, for all N,nin,NT≥1N,n_{\rm in},N_T\ge1N,nin​,NT​≥1.

The three steps

  1. Proposition 7 (finite population): inf⁡αJ(α)≥JN(v^)−c1N−2/max⁡(d,4)(1+ln⁡(N)1{d=4})\inf_\alpha J(\alpha)\ge J^N(\hat v)-c_1\sqrt{N^{-2/\max(d,4)}(1+\ln(N)\mathbf 1_{\{d=4\}})}infα​J(α)≥JN(v^)−c1​N−2/max(d,4)(1+ln(N)1{d=4}​)​.
  2. Proposition 8 (network class): some φ^∈Nd+1,nin,kψ\hat\varphi\in\mathbf N^\psi_{d+1,n_{\rm in},k}φ^​∈Nd+1,nin​,kψ​ with bounded Lipschitz constants has JN(v^)≥JN(φ^)−K2nin−1/(3(d+1))J^N(\hat v)\ge J^N(\hat\varphi)-K_2n_{\rm in}^{-1/(3(d+1))}JN(v^)≥JN(φ^​)−K2​nin−1/(3(d+1))​.
  3. Proposition 15 (time step): ∣JN(φ)−JˇN(φ)∣≤CΔt|J^N(\varphi)-\check J^N(\varphi)|\le C\sqrt{\Delta t}∣JN(φ)−JˇN(φ)∣≤CΔt​ for regular feedbacks.

Supporting results

Lemma 18 (Lipschitz continuity of α^\hat\alphaα^), Proposition 10 (network approximation of a function and its first two xxx-derivatives at rate nin−1/(2(d+1))n_{\rm in}^{-1/(2(d+1))}nin−1/(2(d+1))​ on [0,T]×Bˉd(0,R)[0,T]\times\bar B_d(0,R)[0,T]×Bˉd​(0,R)), (C.2) (moment bounds uniform in NNN), Proposition 13 (stability of JNJ^NJN under feedbacks close on a ball), Lemma 19 (time regularity of the particle system) and Lemma 14 (strong error CNΔtCN\Delta tCNΔt of the Euler scheme).

Significance

The theorem certifies the standard deep-learning approach to mean field control: the value computed by minimizing the simulated finite-population, discrete-time cost over networks is, up to an explicit error with separate rates for population size, network width and time step, no larger than the true MKV value. The rates also expose where the method loses: the nin−1/(3(d+1))n_{\rm in}^{-1/(3(d+1))}nin−1/(3(d+1))​ term is a curse of dimensionality in the network step (Remark 11).

The result is proved in the paper (§3 and Appendices B–D); the proof of Proposition 7 is a modification of Carmona–Delarue, Vol. II, Theorem 6.17. None of it is formalized. A formal development would provide the first machine-checked bridge between a stochastic control problem of McKean–Vlasov type and a concrete learning architecture, and its intermediate results (moment and stability estimates for interacting particle systems, the strong error of an Euler scheme with constants independent of the number of particles, simultaneous approximation of a function and its derivatives by periodic networks) are reusable on their own.

Difficulty

Each step rests on research-level analysis. Proposition 7 needs the Pontryagin principle for McKean–Vlasov control, the propagation of chaos for the optimally controlled system, and the Fournier–Guillin rate for empirical measures, whose max⁡(d,4)\max(d,4)max(d,4) exponent and logarithmic correction at d=4d=4d=4 appear in the bound. Proposition 8 requires approximating the optimal feedback together with its first two derivatives in xxx, because the time-discretization step needs regularity of the approximating network; standard universal approximation results give no control of derivatives, and the available simultaneous approximation results hold only for periodic functions, which forces a localization to a ball whose radius must be balanced against the approximation rate. Proposition 15 cannot be obtained from classical Euler estimates for a system of NdNdNd equations, whose constants grow with NNN: the estimates must be done agent by agent through the empirical measure.

Formalization scope

Rd\mathbb R^dRd is Fin d → ℝ with the sup norm; every constant is existential, so all statements are norm-independent. Time is ℝ≥0 for processes. Solutions of (2.2) and (3.2) use the published Itô-process predicate Peng1990.SMP.IsItoProcess (for X−X0X-X_0X−X0​, with continuous paths and the natural filtration of the initial data and the noise); the backward equation of the Pontryagin system uses Peng1990.SMP.SolvesBSDE; W2W_2W2​ is the published WassersteinDRO.Duality.wassersteinDistance. Problem 2 is law-level: the Euler scheme is a deterministic map of initial positions and increments, integrated against μ0⊗N⊗N(0,ΔtId)⊗NNT\mu_0^{\otimes N}\otimes\mathcal N(0,\Delta t I_d)^{\otimes NN_T}μ0⊗N​⊗N(0,ΔtId​)⊗NNT​; Lemma 14 couples it with the continuous system through the Brownian increments, as the paper does.

The hypotheses are bundled as Coeff ((A1)–(A4), (B1), (B3), (C1), with witnesses for every derivative; the L-derivative is the Fréchet derivative of the lift on L2([0,1])L^2([0,1])L2([0,1])) and DecouplingField ((2.6), existence of a solution of (2.7) on some Problem-1 space, Yt=V(t,Xt)Y_t=V(t,X_t)Yt​=V(t,Xt​), (B2), (C2), (C3)). Disclosed readings: ggg's L-convexity is (A4) without α\alphaα and with right-hand side 000; unique solvability of (2.7), uniqueness and Lipschitz continuity of α^\hat\alphaα^ are not assumed (the last is Lemma 18); Proposition 13 lets its constant depend on bounds for ∣v(0,0)∣,∣w(0,0)∣|v(0,0)|,|w(0,0)|∣v(0,0)∣,∣w(0,0)∣, as its proof does; Proposition 15 reads the first bound of (3.16) as C1(1+∣(t,x)∣)C_1(1+|(t,x)|)C1​(1+∣(t,x)∣). Infima are stated pointwise (∀α ∀η>0 ∃φ\forall\alpha\,\forall\eta>0\,\exists\varphi∀α∀η>0∃φ), never as a real ⨅, and N,nin,NT≥1N,n_{\rm in},N_T\ge1N,nin​,NT​≥1 throughout. The hypothesis bundle is not vacuous: a sorry-free check exhibits the model b=σ=0b=\sigma=0b=σ=0, f=∣α∣2f=|\alpha|^2f=∣α∣2, g=0g=0g=0, μ0=δ0\mu_0=\delta_0μ0​=δ0​ with α^=0\hat\alpha=0α^=0, V=0V=0V=0 satisfying every assumption on any Problem-1 space. Junk values cannot trivialize the goal: the costs are Bochner integrals whose integrability follows from the assumptions, so a non-integrable cost would only make the claimed inequality harder, never vacuous.

Contributions are welcome at every level: proofs of the milestones, in particular the self-contained Lemmas 14 and 19, (C.2) and Proposition 13; infrastructure for the L-derivative, Itô's formula for the published Itô processes, empirical-measure convergence rates, and trigonometric approximation of Cr\mathcal C^rCr periodic functions.

Selected references

  • R. Carmona, M. Laurière, Convergence analysis of machine learning algorithms for the numerical solution of mean field control and games: II — the finite horizon case, Ann. Appl. Probab. 32(6) (2022), 4065–4105. https://doi.org/10.1214/21-AAP1715
  • R. Carmona, F. Delarue, Probabilistic Theory of Mean Field Games with Applications I–II, Springer (2018). https://doi.org/10.1007/978-3-319-58920-6
  • N. Fournier, A. Guillin, On the rate of convergence in Wasserstein distance of the empirical measure, Probab. Theory Relat. Fields 162 (2015), 707–738. https://doi.org/10.1007/s00440-014-0583-7
  • S. Peng, A general stochastic maximum principle for optimal control problems, SIAM J. Control Optim. 28(4) (1990), 966–979. https://doi.org/10.1137/0328054
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Mechanism DesignOperations ResearchOptimization·Captain: mikedeng1

Double Counting in Supply Chain Carbon Footprinting I: With Joint Carbon Production, Every Differentiable Increasing Payment Rule That Makes the Social First-Best a Nash Equilibrium Double-CountsResearch Paper

Motivation

Carbon accounting assigns emissions from a shared supply-chain process to firms that can reduce them. If more than one firm can change the same emissions, charging each firm only a share may leave each with too little incentive to abate. Caro, Corbett, Tan and Zuidwijk study the conflict between avoiding double counting in an emissions ledger and inducing the effort a social planner would choose. Their working paper, published in Manufacturing & Service Operations Management in 2013, states an impossibility result for differentiable, increasing carbon-payment rules. It covers multiple firms, processes, and abatement actions, where a process can be influenced by several firms.

The question matters when a carbon footprint is used as a payment base rather than only as a report. A payment rule changes a firm's private incentive to exert costly effort. The rule may also include transfers between firms, so its incentive effect cannot be judged by looking at a single firm's allocated emissions alone. The paper asks what aggregate marginal payment is necessary if decentralized choices are to reproduce the social first best.

Timeline. Holmström (1982) showed for a team with one joint output and one-dimensional efforts that no budget-balanced sharing rule supports the efficient efforts as a Nash equilibrium (stated in the paper as Proposition 1, p. 11). Charging every team member the full social cost ("charging everything to everyone") is known to restore efficiency, as the paper recalls on p. 12. Caro, Corbett, Tan and Zuidwijk (2012 working paper, 2013 journal version) extend the impossibility to many processes, many abatement actions per firm and an explicit influence structure between firms and processes. They also characterize the linear rules that achieve the first best.

Setting

Let NNN be a finite set of firms and III a finite set of emission-producing processes. Firm nnn chooses a vector en=(en,j)je_n=(e_{n,j})_jen​=(en,j​)j​ of abatement efforts in [0,A]mn[0,A]^{m_n}[0,A]mn​, with A>0A>0A>0. The full profile is e=(en)ne=(e_n)_ne=(en​)n​. Firm nnn's profit before carbon payments is Vn(en)V_n(e_n)Vn​(en​), concave and componentwise decreasing in its effort. Process iii's footprint is fi(e)f_i(e)fi​(e), convex and componentwise decreasing in the collective effort, and nonnegative on the feasible box. The functions are differentiable, as assumed in the paper's model.

The influence matrix B=(bn,i)B=(b_{n,i})B=(bn,i​) has entries in {0,1}\{0,1\}{0,1}. An entry is one when the sum of the partial derivatives of fif_ifi​ with respect to firm nnn's actions is negative. The paper treats this matrix as independent of the effort profile. Joint carbon production means that a process has at least two influencing firms: for some iii, ∑nbn,i≥2\sum_n b_{n,i}\ge 2∑n​bn,i​≥2.

The societal cost per unit of footprint is pS>0p_S>0pS​>0. The social first best e∗e^*e∗ maximizes

S(e)=∑n∈NVn(en)−pS∑i∈Ifi(e)S(e)=\sum_{n\in N}V_n(e_n)-p_S\sum_{i\in I}f_i(e)S(e)=n∈N∑​Vn​(en​)−pS​i∈I∑​fi​(e)

over the effort box. The paper assumes that this solution is unique and that the effort bound is large enough for the relevant optimum to be interior. The first-best footprint is f(e∗)=(fi(e∗))i∈If(e^*)=(f_i(e^*))_{i\in I}f(e∗)=(fi​(e∗))i∈I​.

A carbon-based payment rule hn(ϕ)h_n(\phi)hn​(ϕ) charges firm nnn as a function of the observed footprint vector ϕ\phiϕ, rather than the unobserved effort profile. In the social-planner setting of equation (5), hn(ϕ)=pSf^n(ϕ)+gn(ϕ)h_n(\phi)=p_S\widehat f_n(\phi)+g_n(\phi)hn​(ϕ)=pS​f​n​(ϕ)+gn​(ϕ), where f^n\widehat f_nf​n​ is its footprint allocation and the transfers balance: ∑ngn(ϕ)=0\sum_n g_n(\phi)=0∑n​gn​(ϕ)=0 for ϕ≥0\phi\ge0ϕ≥0. A Nash equilibrium is a feasible effort profile where no firm improves Vn(en)−hn(f(e))V_n(e_n)-h_n(f(e))Vn​(en​)−hn​(f(e)) by changing its own entire effort vector while the other firms hold theirs fixed. At a footprint vector ϕ\phiϕ, the rule double-counts process iii when ∑n∂hn/∂fi(ϕ)>pS\sum_n \partial h_n/\partial f_i(\phi)>p_S∑n​∂hn​/∂fi​(ϕ)>pS​.

Formalization targets

The goal is Proposition 2, evaluated at the first-best footprint:

joint production ∧ e∗ is Nash under differentiable increasing h⟹∃i∈I: ∑n∂hn∂fi(f(e∗))>pS.\text{joint production}\ \land\ e^*\text{ is Nash under differentiable increasing }h \quad\Longrightarrow\quad \exists i\in I:\ \sum_n\frac{\partial h_n}{\partial f_i}(f(e^*))>p_S.joint production ∧ e∗ is Nash under differentiable increasing h⟹∃i∈I: n∑​∂fi​∂hn​​(f(e∗))>pS​.

The paper defines double counting existentially over footprint levels. Its Appendix A.1 proves the stronger assertion at f(e∗)f(e^*)f(e∗), which is the target here. The rule remains of the form (5), with balanced internal transfers on the nonnegative footprint domain.

Two source statements form the milestone list. The necessary part of Lemma 7 gives equation (14): at an interior first best that is also a Nash equilibrium, the sum over processes of each footprint derivative times the gap between the firm's marginal payment and pSp_SpS​ is zero, both with and without the influence indicator bn,ib_{n,i}bn,i​. Equation (18) says that if aggregate marginal payments do not exceed pSp_SpS​ at f(e∗)f(e^*)f(e∗), every individual process contribution to that sum is zero. The mission also drafts the sufficient part of Lemma 7 and Proposition 3, which characterizes the linear rules h=pSAmatf+kh=p_S A_{\mathrm{mat}}f+kh=pS​Amat​f+k with 0≤Amat≤10\le A_{\mathrm{mat}}\le10≤Amat​≤1: they implement e∗e^*e∗ precisely when Amat≥BA_{\mathrm{mat}}\ge BAmat​≥B.

Significance

Proposition 2 identifies a limit on footprint-based incentives under joint production. With more than one firm able to lower a process's emissions, a differentiable increasing rule that implements the first best cannot keep every aggregate marginal charge at or below the social carbon price. Balanced transfers among firms do not remove that requirement. Proposition 3 supplies a complementary characterization for linear payments, identifying which firms must bear the full marginal charge for the processes they influence. These are results proved in the paper, not open conjectures.

The formalization contributes a precise, reusable model of finite effort profiles, process footprints, unilateral deviations, and coordinate marginal payments. It also separates a global Nash best-response condition from first-order identities, so the necessary condition in Lemma 7 has mathematical content. The listed Lean theorems are draft statements with proof holes; they do not yet have machine-checked proofs. Completing them would formally verify the paper's stated claims under the declared model conventions.

Difficulty

The obstacle is the interaction between a shared footprint and unilateral decisions. A firm's payment derivative with respect to a process footprint is multiplied by that firm's own effect on the process, while the social objective prices the total footprint at pSp_SpS​. A condition on the sum of marginal payments alone does not specify the charge faced by each influential firm. With several actions and processes, the necessary condition is a sum over process contributions, so it cannot simply be read as a coordinatewise equality without further assumptions. These issues occur even though all effort and process index sets are finite.

Formalization scope

Lean represents firms, each firm's action indices, and processes by finite types. Efforts and footprints are real-valued functions. The firm and collective effort boxes are closed coordinatewise intervals, with A>0A>0A>0; optimality and Nash equilibrium quantify over all feasible profiles or unilateral deviations. Coordinate partial derivatives use one-variable derivatives after replacing the corresponding coordinate. Payment rules are functions on real footprint vectors and “increasing” means componentwise nondecreasing.

The source's sign test for bn,ib_{n,i}bn,i​ does not name an effort profile. The formalization pins it to every profile in the effort box, matching the paper's use of a fixed influence matrix. Interiority is required only of the named first best. The paper's “without loss of generality” nonempty row and column sums for BBB are omitted because the results do not use them; the strict part of its cost monotonicity is likewise unused. Its participation condition (3) is outside the decentralized game (4) and is not added to Nash equilibrium. Equation (5) and transfer balance are imposed only for nonnegative footprint vectors, as printed. The effort bound AAA and Proposition 3's matrix AmatA_{\mathrm{mat}}Amat​ have distinct names.

The first best is a feasible global maximum, not a default-valued real supremum; Nash equilibrium tests full unilateral deviations, not stationarity. These choices rule out a vacuous first-best target and a first-order surrogate for the game. The supporting definitions of finite effort boxes, coordinate derivatives, social value, and Nash best response are useful beyond the final impossibility statement. Contributions that prove the source's necessary and sufficient conditions, the linear characterization, or the goal against these definitions are within scope.

Selected references

  • B. Holmström, Moral Hazard in Teams, Bell Journal of Economics 13(2), 324–340, 1982. DOI.
  • F. Caro, C. J. Corbett, T. Tan and R. Zuidwijk, Double-Counting in Supply Chain Carbon Footprinting, working paper dated December 21, 2012, especially §§3–4 and Appendix A. Author-hosted manuscript. Published in Manufacturing & Service Operations Management 15(4), 2013. DOI.
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Mathematical PhysicsProbability·Captain: mikedeng1

The Two-Dimensional KPZ Equation in the Entire Subcritical Regime: For Every β̂ ∈ (0, 1) the Rescaled Log-Partition Function of the 2D Directed Polymer Has Edwards–Wilkinson Gaussian FluctuationsResearch Paper

Motivation

The two-dimensional directed polymer is a random walk whose paths are reweighted by a random space-time environment. Its logarithmic partition function is a discrete counterpart of the height field of the two-dimensional Kardar–Parisi–Zhang equation. At the intermediate-disorder scale, the random weighting becomes weaker as the walk grows, yet its fluctuations remain visible. Caravenna, Sun and Zygouras prove that throughout the subcritical regime 0<β^<10<\hat\beta<10<β^​<1, spatial averages of the centred log-partition function converge to Gaussian fluctuations described by an additive stochastic heat equation (Theorem 1.6, p. 6).

The polymer formulation matters because it is a concrete finite-path model: each partition function is an average over finitely many nearest-neighbour walks, while its limit retains the effect of disorder at every scale. The same paper treats the continuum KPZ equation separately; this mission takes its stated polymer theorem as the target. Earlier work in dimension 1+11+11+1 studied a different intermediate-disorder scaling and a Wiener-chaos limit (Alberts, Khanin and Quastel, 2014). The two-dimensional result concerns a distinct regime and a different limit.

Setting

Let SSS be the simple symmetric random walk on Z2\mathbb Z^2Z2. Starting at xxx, it chooses each of its four nearest-neighbour steps with probability 1/41/41/4. Write qn(z)=P0(Sn=z)q_n(z)=P_0(S_n=z)qn​(z)=P0​(Sn​=z), and let S~\widetilde SS be an independent copy. Their expected overlap through time NNN is

RN=∑n=1NP(Sn=S~n)=∑n=1N∑z∈Z2qn(z)2.R_N=\sum_{n=1}^N P(S_n=\widetilde S_n)=\sum_{n=1}^N\sum_{z\in\mathbb Z^2}q_n(z)^2.RN​=n=1∑N​P(Sn​=Sn​)=n=1∑N​z∈Z2∑​qn​(z)2.

For a fixed β^∈(0,1)\hat\beta\in(0,1)β^​∈(0,1), the disorder strength is βN=β^/RN\beta_N=\hat\beta/\sqrt{R_N}βN​=β^​/RN​​. The environment ω(n,z)\omega(n,z)ω(n,z) consists of independent, identically distributed real random variables with mean zero, variance one and finite exponential moments at all sufficiently small positive arguments. Its logarithmic moment generating function is λ(b)=log⁡E[ebω]\lambda(b)=\log\mathbb E[e^{b\omega}]λ(b)=logE[ebω]. The law also obeys the paper's concentration assumption (1.20): convex 1-Lipschitz functions of any finite collection of environment variables have stretched-exponential deviations from a median, measured with Euclidean distance (pp. 5–6).

For a length-NNN walk from xxx, sum βNω(n,Sn)−λ(βN)\beta_N\omega(n,S_n)-\lambda(\beta_N)βN​ω(n,Sn​)−λ(βN​) over times 1,…,N1,\ldots,N1,…,N, exponentiate, and average over paths. The result is the partition function ZN(x)Z_N(x)ZN​(x). Where λ(βN)\lambda(\beta_N)λ(βN​) is finite, its centring gives EZN(x)=1\mathbb E Z_N(x)=1EZN​(x)=1. A restricted function ZΛ,b(x)Z_{\Lambda,b}(x)ZΛ,b​(x) samples disorder only from the space-time sites in Λ\LambdaΛ. Section 2 uses an early window ANxA_N^xANx​ near the start and a late window BN≥B_N^{\ge}BN≥​ to define ZNA(x)Z_N^A(x)ZNA​(x), its remainder Z^NA(x)=ZN(x)−ZNA(x)\widehat Z_N^A(x)=Z_N(x)-Z_N^A(x)ZNA​(x)=ZN​(x)−ZNA​(x), and ZNB≥(x)Z_N^{B\ge}(x)ZNB≥​(x) (pp. 7–9).

At macroscopic time t>0t>0t>0 and position y∈R2y\in\mathbb R^2y∈R2, the fluctuation field is

hN(t,y)=log⁡Z⌊tN⌋(⌊Ny⌋)−E[log⁡Z⌊tN⌋(0)]βN.\mathfrak h_N(t,y)=\frac{\log Z_{\lfloor tN\rfloor}(\lfloor\sqrt N y\rfloor)-\mathbb E[\log Z_{\lfloor tN\rfloor}(0)]}{\beta_N}.hN​(t,y)=βN​logZ⌊tN⌋​(⌊N​y⌋)−E[logZ⌊tN⌋​(0)]​.

The floor of a vector is componentwise. In the numerator, Z⌊tN⌋Z_{\lfloor tN\rfloor}Z⌊tN⌋​ uses the disorder strength β⌊tN⌋\beta_{\lfloor tN\rfloor}β⌊tN⌋​; the field is divided by βN\beta_NβN​, exactly as in (1.23).

Formalization targets

For every t>0t>0t>0 and smooth compactly supported test function ϕ\phiϕ, Theorem 1.6 asserts

∫R2hN(t,y)ϕ(y) dy→d⟨v(2cβ^)(t/2,⋅),ϕ⟩,cβ^=11−β^2.\int_{\mathbb R^2}\mathfrak h_N(t,y)\phi(y)\,dy\xrightarrow{d}\langle v^{(\sqrt2c_{\hat\beta})}(t/2,\cdot),\phi\rangle,\qquad c_{\hat\beta}=\sqrt{\frac1{1-\hat\beta^2}}.∫R2​hN​(t,y)ϕ(y)dyd​⟨v(2​cβ^​​)(t/2,⋅),ϕ⟩,cβ^​​=1−β^​21​​.

The tested limit is centred Gaussian. Its variance is (2cβ^)2σϕ2(t/2)(\sqrt2c_{\hat\beta})^2\sigma_\phi^2(t/2)(2​cβ^​​)2σϕ2​(t/2), where

σϕ2(s)=∬ϕ(x)Ks(x,y)ϕ(y) dx dy,Ks(x,y)=∫0se−∣x−y∣2/(4u)4πu du.\sigma_\phi^2(s)=\iint\phi(x)K_s(x,y)\phi(y)\,dx\,dy,\qquad K_s(x,y)=\int_0^s\frac{e^{-|x-y|^2/(4u)}}{4\pi u}\,du.σϕ2​(s)=∬ϕ(x)Ks​(x,y)ϕ(y)dxdy,Ks​(x,y)=∫0s​4πue−∣x−y∣2/(4u)​du.

The milestone list follows the paper's stated results: second-moment bounds (3.2)–(3.4), higher moments for some p>2p>2p>2 (3.12), a left-tail bound (Proposition 3.1) and the negative and logarithmic moments it yields (3.14)–(3.16), vanishing spatial averages for two error terms (Propositions 2.1–2.2), replacement by the late-window term (Proposition 2.3), and the Gaussian limit for that term (Proposition 2.4). These are the exact result labels used in Sections 2 and 3 (pp. 8–13).

Significance

The theorem identifies the fluctuation law of the logarithm of the polymer partition function for every β^\hat\betaβ^​ strictly below the critical value 111. The coefficient cβ^c_{\hat\beta}cβ^​​ records the disorder strength in the limiting covariance, and the time t/2t/2t/2 reflects the two-dimensional walk's covariance convention. Without the spatial averaging and normalization, the statement would concern a different observable; the theorem characterizes a field tested against compactly supported functions (Theorem 1.6 and Remark 1.7).

The result is proved in the cited paper. This mission asks for a machine-checked proof of that known result and its curated supporting statements. The reusable output includes a finite-path polymer model on Z2\mathbb Z^2Z2, a precise restricted partition function, the disorder concentration assumption, and the Gaussian covariance functional. The published atomic polymer model already supplies the space-time cells, steps, walk positions and log moment generating function; this mission extends that common base to the centred, spatially shifted model of this paper.

Difficulty

Pointwise size does not identify the limiting spatial fluctuations. The early-window partition function captures much of ZN(x)Z_N(x)ZN​(x) at a fixed site, yet its averaged logarithm vanishes at the target scale. The small remainder cannot simply be discarded: after division by the early-window function, its late-time component carries the Gaussian limit. The paper separates these effects in Propositions 2.1–2.4 and needs moment and left-tail control to keep the logarithmic expression meaningful (Sections 2–4). A direct Taylor expansion of log⁡ZN\log Z_NlogZN​ around its mean would lose this distinction.

Formalization scope

Lean uses finite sequences of four-neighbour steps and the Euclidean norm on R2\mathbb R^2R2. Disorder is a family indexed by positive walk times and lattice sites; the time-zero row of its ambient type is unused. The full and restricted partition functions are finite walk averages. The concentration assumption quantifies over Euclidean 1-Lipschitz convex functions and their medians. The test class of Theorem 1.6 is Cc∞(R2)C_c^\infty(\mathbb R^2)Cc∞​(R2); the four Section 2 propositions use Cc(R2)C_c(\mathbb R^2)Cc​(R2). Treating “smooth” as analytic would make compactly supported tests trivial, so the Lean statement uses the smooth differentiability order.

The target additive stochastic heat observable is represented by its Gaussian law and the kernel above; the random field v(c)v^{(c)}v(c) itself is not formalized, and the statement does not need it. The kernel takes extended nonnegative values because it is infinite on the diagonal; the diagonal has zero area in the tested covariance integral. Moments and L1/L2L^1/L^2L1/L2 convergence use extended nonnegative integrals. The paper assumes exponential moments only near zero, so bounds whose printed form quantifies over every NNN are stated for all sufficiently large NNN, avoiding default values of the logarithmic moment generating function at early indices. The spatial sums have finite support because the test functions do. Replacing the Euclidean norm by the sup norm would change the early window (a square instead of a disc), the kernel and the class of 1-Lipschitz functions in (1.20), so all of these are Euclidean. The polymer propositions are stated for every window exponent below a threshold, as in (2.2), and the passage from the time-1 lattice averages of Propositions 2.1–2.4 to the general-time integral of Theorem 1.6 is part of the proof work, not of the statements. Contributions to the polymer moments, left-tail estimate, replacement propositions and Gaussian limit all feed the stated goal.

Selected references

  • Francesco Caravenna, Rongfeng Sun and Nikos Zygouras, The two-dimensional KPZ equation in the entire subcritical regime, Annals of Probability 48(3), 2020; formalization source: arXiv:1812.03911v3.
  • Tom Alberts, Konstantin Khanin and Jeremy Quastel, The intermediate disorder regime for directed polymers in dimension 1+1, Annals of Probability 42(3), 2014, DOI:10.1214/13-AOP895.
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Operations ResearchOptimizationProbability·Captain: mikedeng1

Retail Assortment Planning in the Presence of Consumer Search IV: Under Overlapping-Assortment Search, the Full Assortment Is Optimal Once Search Is Cheap EnoughResearch Paper

Assortment planning when consumers can shop elsewhere

A retailer that decides which variants of a product to stock (its assortment) trades off the revenue each variant brings against the operational cost of carrying it. The classical model of this trade-off uses the multinomial logit (MNL) model of consumer choice: a consumer who does not like what the store offers simply buys nothing (van Ryzin & Mahajan 1999). In practice a consumer who does not like what the store offers can also go elsewhere. Cachon, Terwiesch and Xu (working paper, December 2002; published in MSOM 7(4), 2005) add this consumer search to the MNL model and ask how it changes the retailer's optimal assortment.

They study two search models. In the overlapping assortment model (§3.1), a consumer who searches pays a search cost bbb and then finds a competitor carrying every variant, so search can only reveal variants the store does not carry. This mission formalizes the paper's Theorem 6 about that model: when search is cheap, the store's best response is to carry everything.

Setting

There are nnn variants, N={1,…,n}N = \{1,\dots,n\}N={1,…,n}, and an assortment is a subset S⊆NS \subseteq NS⊆N; write Sˉ=N−S\bar S = N - SSˉ=N−S for the variants the store does not carry. A consumer's utility for variant iii is Ui=(ui−pi)+ζiU_i = (u_i - p_i) + \zeta_iUi​=(ui​−pi​)+ζi​, where ui−piu_i - p_iui​−pi​ is the variant's expected net utility and the shocks ζi\zeta_iζi​ are independent with the zero-mean Gumbel distribution function F(x)=exp⁡[−exp⁡(−(x/μ+γ))]F(x) = \exp[-\exp(-(x/\mu + \gamma))]F(x)=exp[−exp(−(x/μ+γ))], with scale μ>0\mu > 0μ>0 and γ\gammaγ Euler's constant. The no-purchase option is a "faux variant" 000 with utility U0U_0U0​. Its preference is vi=exp⁡((ui−pi)/μ)>0v_i = \exp((u_i - p_i)/\mu) > 0vi​=exp((ui​−pi​)/μ)>0, and v0>0v_0 > 0v0​>0 is the preference of not buying.

Without search, variant i∈Si \in Si∈S has the MNL demand (2), qim(S)=vi/(∑k∈Svk+v0)q_i^m(S) = v_i / (\sum_{k\in S} v_k + v_0)qim​(S)=vi​/(∑k∈S​vk​+v0​). Following Theorem 1, put λ(u)=exp⁡[−(u/μ+γ)]\lambda(u) = \exp[-(u/\mu + \gamma)]λ(u)=exp[−(u/μ+γ)] and

H(u,S)=exp⁡(−λ(u)(v0+∑j∈Svj)),H(u, S) = \exp\Big(-\lambda(u)\big(v_0 + \textstyle\sum_{j\in S} v_j\big)\Big),H(u,S)=exp(−λ(u)(v0​+∑j∈S​vj​)),

the probability that every option the store offers, including not buying, has utility at most uuu. The best utility outside the store, max⁡i∈SˉUi\max_{i\in\bar S} U_imaxi∈Sˉ​Ui​, has a density w(yˉ,S)w(\bar y, S)w(yˉ​,S). A consumer whose best in-store utility is yyy searches when the expected gain exceeds the cost,

ΦS(y)=∫y∞(yˉ−y) w(yˉ,S) dyˉ ≥ b,(5)\Phi_S(y) = \int_y^\infty (\bar y - y)\, w(\bar y, S)\, d\bar y \ \ge\ b, \qquad (5)ΦS​(y)=∫y∞​(yˉ​−y)w(yˉ​,S)dyˉ​ ≥ b,(5)

and the search threshold Uˉ(S)\bar U(S)Uˉ(S) is the solution of ΦS(Uˉ(S))=b\Phi_S(\bar U(S)) = bΦS​(Uˉ(S))=b, equation (4). Theorem 3 gives the resulting demand,

qiso(S)=qim(S)(1−H(Uˉ(S),S)),i∈S, S≠N.q_i^{so}(S) = q_i^m(S)\big(1 - H(\bar U(S), S)\big), \qquad i \in S,\ S \ne N.qiso​(S)=qim​(S)(1−H(Uˉ(S),S)),i∈S, S=N.

When the store carries everything there is nothing to search for (p. 28: "If the retailer offers the full assortment, there will be no consumer search"), so qiso(N)=qim(N)q_i^{so}(N) = q_i^m(N)qiso​(N)=qim​(N).

Variant iii earns margin mim_imi​ per unit and costs c(qi)c(q_i)c(qi​) to carry, where ccc is concave and increasing (economies of scale). The retailer's profit is

π(S)=∑i∈S[mi qiso(S)−c(qiso(S))],(1), (13).\pi(S) = \sum_{i\in S}\big[m_i\, q_i^{so}(S) - c(q_i^{so}(S))\big], \qquad (1),\ (13).π(S)=i∈S∑​[mi​qiso​(S)−c(qiso​(S))],(1), (13).

As printed, the second line of (13) writes qiso(S)(1−H(Uˉ(S),S))q_i^{so}(S)(1 - H(\bar U(S), S))qiso​(S)(1−H(Uˉ(S),S)) where qim(S)(1−H(Uˉ(S),S))q_i^m(S)(1 - H(\bar U(S), S))qim​(S)(1−H(Uˉ(S),S)) is meant; the definition uses the latter.

Formalization targets

Goal: Theorem 6 (p. 18)

If the full assortment is profitable, π(N)>0\pi(N) > 0π(N)>0, then there is a bˉ>0\bar b > 0bˉ>0 such that

πb(S)≤πb(N)for every S⊆N and every search cost 0<b≤bˉ.\pi_b(S) \le \pi_b(N) \qquad \text{for every } S \subseteq N \text{ and every search cost } 0 < b \le \bar b .πb​(S)≤πb​(N)for every S⊆N and every search cost 0<b≤bˉ.

The threshold bˉ\bar bbˉ depends on the data v,v0,μ,m,cv, v_0, \mu, m, cv,v0​,μ,m,c but is one number for all assortments SSS.

Milestones

  1. w(⋅,S)w(\cdot, S)w(⋅,S) is the density of max⁡i∈SˉUi\max_{i\in\bar S} U_imaxi∈Sˉ​Ui​ (proof of Theorem 3, p. 11).
  2. For S≠NS \ne NS=N, the gain ΦS(y)\Phi_S(y)ΦS​(y) is finite and strictly decreasing in yyy (proof of Theorem 3, p. 11).
  3. For S≠NS \ne NS=N and b>0b > 0b>0, Uˉ(S)\bar U(S)Uˉ(S) is the unique solution of (4) (Theorem 3, p. 11).
  4. Uˉ(S)\bar U(S)Uˉ(S) is strictly decreasing in bbb (proof of Theorem 6, p. 18).
  5. Uˉ(S)→−∞\bar U(S) \to -\inftyUˉ(S)→−∞ as b→∞b \to \inftyb→∞ and Uˉ(S)→∞\bar U(S) \to \inftyUˉ(S)→∞ as b→0+b \to 0^+b→0+ (p. 18).
  6. H(Uˉ(S),S)→1H(\bar U(S), S) \to 1H(Uˉ(S),S)→1 and qiso(S)→0q_i^{so}(S) \to 0qiso​(S)→0 as b→0+b \to 0^+b→0+ (p. 18).

Significance

Theorem 6 separates the overlapping model sharply from the no-search MNL model and from the paper's independent-assortment model. In those two models every variant in an optimal assortment must earn a strictly positive profit, because dropping a loss-making variant only shifts demand to the remaining ones. In the overlapping model the assortment also controls whether consumers leave: carrying an unprofitable variant can pay because it removes a reason to search. Theorem 6 is the extreme form of this effect, stating that the motive to prevent search can override the profitability of individual variants entirely (§4.3, p. 17).

The paper gives only a short sketch of the proof. The steps it asserts without proof are the existence and uniqueness of Uˉ(S)\bar U(S)Uˉ(S), its monotonicity and limits in bbb, and the explicit density www. This mission states each of them as a milestone. No machine-checked version of any of these results is known.

Difficulty

The search threshold Uˉ(S)\bar U(S)Uˉ(S) is defined only implicitly, through an improper integral of the density of a maximum of Gumbel variables. Each property the theorem needs (that the equation has exactly one root, that the root moves monotonically with bbb, and that it escapes to +∞+\infty+∞ as b→0b \to 0b→0) has to be read off the integral. That means controlling ΦS\Phi_SΦS​ on the whole real line: its convergence, its strict decrease, and its limits at ±∞\pm\infty±∞.

The final comparison is not a direct consequence of qiso(S)→0q_i^{so}(S) \to 0qiso​(S)→0 either. A variant's profit miq−c(q)m_i q - c(q)mi​q−c(q) tends to −c(0)-c(0)−c(0) rather than to 000, so the conclusion depends on the sign of c(0)c(0)c(0), and bˉ\bar bbˉ must be chosen uniformly over all 2n2^n2n assortments.

Formalization scope

The shared model is the definition AssortSearch.FullAssort.Model, which builds on the published MNL share RetailVariety.Structure.share. Its conventions:

  • Variants are Fin n, numbered from 0; the paper's variant iii is index i−1i-1i−1. The no-purchase option is not a variant: v0v_0v0​ is a separate positive real.
  • Preferences vi>0v_i > 0vi​>0, v0>0v_0 > 0v0​>0 and the scale μ>0\mu > 0μ>0 are free data ("for any given set of preference"). γ\gammaγ is Real.eulerMascheroniConstant.
  • Assortments are arbitrary Finset (Fin n), including ∅\emptyset∅, whose profit is 000.
  • w(yˉ,S)w(\bar y, S)w(yˉ​,S) is given by its explicit formula (VˉS/μ) λ(yˉ)exp⁡(−λ(yˉ)VˉS)(\bar V_S/\mu)\,\lambda(\bar y)\exp(-\lambda(\bar y)\bar V_S)(VˉS​/μ)λ(yˉ​)exp(−λ(yˉ​)VˉS​) with VˉS=∑i∈Sˉvi\bar V_S = \sum_{i\in\bar S} v_iVˉS​=∑i∈Sˉ​vi​. Milestone 1 proves that it is the density of the maximum.
  • ΦS(u)\Phi_S(u)ΦS​(u) is the Lebesgue integral over (u,∞)(u, \infty)(u,∞). Its integrability is part of milestone 2, so no result relies on Lean's value 000 for a non-integrable function.
  • Uˉ(S)\bar U(S)Uˉ(S) is defined as inf⁡{u:ΦS(u)≤b}\inf\{u : \Phi_S(u) \le b\}inf{u:ΦS​(u)≤b}; milestone 3 proves that it solves (4). The demand for S=NS = NS=N is the no-search MNL share, and Uˉ(N)\bar U(N)Uˉ(N) is never used.
  • The cost c:R→Rc : \mathbb R \to \mathbb Rc:R→R is concave and monotone on [0,1][0,1][0,1], where all demands lie. The hypothesis c(0)≥0c(0) \ge 0c(0)≥0 is added to Theorem 6; without it the theorem fails (a counterexample is in the goal's statement).
  • Search costs are positive: 0<b≤bˉ0 < b \le \bar b0<b≤bˉ.
  • The margins mim_imi​ are reals that satisfy §3's standing assumption of monotone margins (p. 6): mj≥mkm_j \ge m_kmj​≥mk​ whenever vj≥vkv_j \ge v_kvj​≥vk​ (equivalently uj−pj≥uk−pku_j - p_j \ge u_k - p_kuj​−pj​≥uk​−pk​). §3's labelling of variants by decreasing net utility is a labelling without loss of generality and is not encoded, since assortments are arbitrary subsets.

Several formalizations would make the goal trivial or empty, and each is excluded:

  • taking Uˉ(S)\bar U(S)Uˉ(S) as a free parameter instead of the solution of (4);
  • concluding ∃bˉ\exists \bar b∃bˉ without bˉ>0\bar b > 0bˉ>0;
  • defining qso(N)q^{so}(N)qso(N) through a junk value of Uˉ(N)\bar U(N)Uˉ(N);
  • dropping the hypothesis π(N)>0\pi(N) > 0π(N)>0;
  • fixing a specific cost function.

A complete development needs the integral calculus of the Gumbel tail (∫u∞(yˉ−u)w\int_u^\infty (\bar y - u) w∫u∞​(yˉ​−u)w and its derivative in uuu) and the product-measure computation of the law of a maximum of independent variables. Both are reusable beyond this paper, for instance in other search and extreme-value models. Contributions are welcome on any milestone, and on helper lemmas such as the continuity of ΦS\Phi_SΦS​ and its limits at ±∞\pm\infty±∞.

Selected references

  • G. P. Cachon, C. Terwiesch, Y. Xu, Retail Assortment Planning in the Presence of Consumer Search, Wharton working paper, December 20, 2002; published in Manufacturing & Service Operations Management 7(4):330–346, 2005. https://doi.org/10.1287/msom.1050.0088
  • G. van Ryzin, S. Mahajan, On the Relationship Between Inventory Costs and Variety Benefits in Retail Assortments, Management Science 45(11):1496–1509, 1999. https://doi.org/10.1287/mnsc.45.11.1496
  • D. McFadden, Conditional Logit Analysis of Qualitative Choice Behavior, in P. Zarembka (ed.), Frontiers in Econometrics, Academic Press, 1974.
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CombinatoricsGraph Theory·Captain: mikedeng1

Three-Coloring and List Three-Coloring of Graphs Without Induced Paths on Seven Vertices 3: In a Lemma 11 Instance, Two Vertices of Xᵢ Have Neighbor Triples Joined by an EdgeResearch Paper

Motivation

A graph is 3-colorable if its vertices can be colored with three colors so that adjacent vertices get different colors. Deciding 3-colorability is NP-complete in general, and one of the standard ways to map the boundary between easy and hard cases is to forbid an induced subgraph. For the path PtP_tPt​ on ttt vertices, 3-colorability of P6P_6P6​-free graphs was known to be polynomial (Randerath and Schiermeyer, 2004, reference [21] of the paper), and Randerath, Schiermeyer and Tewes asked in 2002 whether the same holds for t=7t = 7t=7.

Bonomo, Chudnovsky, Maceli, Schaudt, Stein and Zhong (Combinatorica, 2017) answered this question. Their Theorem 1 states that the list version, in which every vertex vvv may only receive a color from a prescribed list L(v)⊆{1,2,3}L(v) \subseteq \{1,2,3\}L(v)⊆{1,2,3}, can be decided for P7P_7P7​-free graphs in time O(∣V(G)∣21(∣V(G)∣+∣E(G)∣))O(|V(G)|^{21}(|V(G)|+|E(G)|))O(∣V(G)∣21(∣V(G)∣+∣E(G)∣)). The algorithm first reduces the instance to a polynomial number of configurations described by a seed, and then calls Lemma 11 (p. 14) on each configuration. Lemma 11 rests on one structural fact about P7P_7P7​-free graphs, Claim 13 (p. 16), which is the goal of this mission.

Timeline:

  • 2002: Randerath, Schiermeyer and Tewes ask whether 3-colorability of P7P_7P7​-free graphs is polynomial.
  • 2004: Randerath and Schiermeyer give a polynomial algorithm for P6P_6P6​-free graphs.
  • 2017: Bonomo et al. give a polynomial algorithm for list 3-coloring of P7P_7P7​-free graphs; Claims 12 and 13 are its structural core.
  • As of the paper, no ttt is known for which 3-coloring PtP_tPt​-free graphs is NP-complete (p. 2); the case t=8t = 8t=8 is open.

Setting

All graphs are finite and simple. For a set SSS of vertices of a graph GGG, N(S)N(S)N(S) is the set of vertices outside SSS with a neighbor in SSS, and S‾=S∪N(S)\overline{S} = S \cup N(S)S=S∪N(S). A graph is PtP_tPt​-free if it has no induced subgraph isomorphic to PtP_tPt​.

A palette LLL assigns each vertex a list L(v)⊆{1,2,3}L(v) \subseteq \{1,2,3\}L(v)⊆{1,2,3}. A seed of (G,L)(G,L)(G,L) is a nonempty set SSS that induces a connected subgraph, is 2-dominating (every vertex is at distance at most 222 from SSS), and satisfies ∣L(v)∣=1|L(v)| = 1∣L(v)∣=1 for v∈Sv \in Sv∈S and ∣L(v)∣=2|L(v)| = 2∣L(v)∣=2 for v∈N(S)v \in N(S)v∈N(S).

The Lemma 11 setting consists of a graph GGG, a palette LLL and a seed SSS such that

  1. GGG is connected and P7P_7P7​-free;
  2. adjacent v∈Sv \in Sv∈S and w∈N(S)w \in N(S)w∈N(S) have disjoint lists;
  3. the set XXX of vertices with ∣L(v)∣=3|L(v)| = 3∣L(v)∣=3 is stable and anticomplete to V(G)∖(S‾∪X)V(G) \setminus (\overline{S} \cup X)V(G)∖(S∪X);
  4. no vertex of XXX has a connected neighborhood.

For i∈{1,2,3}i \in \{1,2,3\}i∈{1,2,3}, DiD_iDi​ is the set of v∈N(S)v \in N(S)v∈N(S) with L(v)={1,2,3}∖{i}L(v) = \{1,2,3\} \setminus \{i\}L(v)={1,2,3}∖{i}, and Ni(x)=N(x)∩DiN_i(x) = N(x) \cap D_iNi​(x)=N(x)∩Di​. For {i,j,k}={1,2,3}\{i,j,k\} = \{1,2,3\}{i,j,k}={1,2,3}, XiX_iXi​ is the set of x∈Xx \in Xx∈X for which Nj(x)N_j(x)Nj​(x) is not complete to Nk(x)N_k(x)Nk​(x), and for x∈Xix \in X_ix∈Xi​ the paper fixes non-adjacent nj(x)∈Nj(x)n_j(x) \in N_j(x)nj​(x)∈Nj​(x), nk(x)∈Nk(x)n_k(x) \in N_k(x)nk​(x)∈Nk​(x).

Formalization targets

Goal: Claim 13 (p. 16)

In the Lemma 11 setting, let {i,j,k}={1,2,3}\{i,j,k\} = \{1,2,3\}{i,j,k}={1,2,3}, x,y∈Xix, y \in X_ix,y∈Xi​, and let nj∈Nj(x)n_j \in N_j(x)nj​∈Nj​(x), nk∈Nk(x)n_k \in N_k(x)nk​∈Nk​(x) be non-adjacent. Then

∃ a∈{x,nj,nk}, ∃ b∈{y,nj(y),nk(y)}:ab∈E(G).\exists\, a \in \{x, n_j, n_k\},\ \exists\, b \in \{y, n_j(y), n_k(y)\}:\quad ab \in E(G).∃a∈{x,nj​,nk​}, ∃b∈{y,nj​(y),nk​(y)}:ab∈E(G).

Milestones

  1. Display (1), p. 6. For a seed SSS and two non-adjacent v,w∈N(S)v, w \in N(S)v,w∈N(S) there is an induced vvv–www path on at least 333 vertices whose inner vertices lie in SSS.
  2. p. 15. For d∈Did \in D_id∈Di​ and s∈S∩N(d)s \in S \cap N(d)s∈S∩N(d), L(s)={i}L(s) = \{i\}L(s)={i}.
  3. p. 15. No vertex of XXX has a neighbor in SSS.
  4. Claim 12, p. 15. For i≠ji \ne ji=j, ui,vi∈Diu_i, v_i \in D_iui​,vi​∈Di​, uj,vj∈Dju_j, v_j \in D_juj​,vj​∈Dj​ with {ui,vi,uj,vj}\{u_i, v_i, u_j, v_j\}{ui​,vi​,uj​,vj​} stable, there is an induced path PPP with ends a,ba, ba,b among them such that {a,b}≠{ui,uj}\{a,b\} \ne \{u_i,u_j\}{a,b}={ui​,uj​}, {a,b}≠{vi,vj}\{a,b\} \ne \{v_i,v_j\}{a,b}={vi​,vj​}, the interior P∗P^*P∗ lies in SSS, and P∗P^*P∗ is anticomplete to the other two vertices.

Significance

Claim 13 says that the neighbor triples {x,nj(x),nk(x)}\{x, n_j(x), n_k(x)\}{x,nj​(x),nk​(x)} of the vertices of XiX_iXi​ pairwise touch. This is what allows the proof of Lemma 11 (Claims 14 to 17) to refine the palette of all of XiX_iXi​ simultaneously with only polynomially many guesses: without it, the vertices of XiX_iXi​ could interact independently and the number of cases would be exponential. Claim 12 and display (1) are the general tools for building long induced paths through a seed, used throughout §3.1.

The paper's result is proved and published. None of it is formalized in a proof assistant as far as the platform's index shows. This mission produces a machine-checked version of the structural core of Lemma 11, and the definitions it needs (seeds, the Lemma 11 setting, the sets DiD_iDi​ and Ni(x)N_i(x)Ni​(x)) are reusable for the rest of the paper's argument.

Difficulty

The proof of Claim 13 is short on paper, but it assembles an induced P7P_7P7​ from three pieces: the path through SSS given by Claim 12 and the two short paths nj−x−nkn_j - x - n_knj​−x−nk​ and nj(y)−y−nk(y)n_j(y) - y - n_k(y)nj​(y)−y−nk​(y). Showing that the union is induced requires every non-adjacency between the pieces, and these come from different hypotheses: the stability of XXX, the fact that XXX has no neighbor in SSS, the list structure of the vertices of SSS next to DiD_iDi​, and part (c) of Claim 12. Claim 12 itself is an extremal argument (choose the neighbor closest to an end of a path), which in a formal setting requires explicit manipulation of paths as sequences of vertices: splitting, reversing and concatenating them while keeping them induced. The obvious approach of taking any shortest path through SSS between two of the four vertices fails, because such a path can have interior vertices adjacent to the other two.

Formalization scope

Graphs are SimpleGraph V on a finite type V with decidable equality; vertex sets are Finset V. The colors 1,2,31,2,31,2,3 are 0,1,2 in Fin 3, and a palette is V → Finset (Fin 3). P7P_7P7​-freeness is the negation of Mathlib's induced containment IsIndContained of pathGraph 7; ordinary subgraph containment would be a different, much stronger condition. Connectedness uses Mathlib's Connected, which includes nonemptiness. An induced path is the published platform definition StrongPerfectGraph.Main.IsInducedPath (a nonempty list of distinct vertices in which two vertices are adjacent exactly when consecutive); its ends are the first and last list entries and its interior P∗P^*P∗ is the list with both ends removed.

The Lemma 11 setting is a structure Lemma11Hyp G L S bundling its hypotheses. Lemma 11's own conclusion, a decision procedure with running time O(∣V(G)∣9(∣V(G)∣+∣E(G)∣))O(|V(G)|^9(|V(G)|+|E(G)|))O(∣V(G)∣9(∣V(G)∣+∣E(G)∣)), and the running time of Theorem 1 are not formalized, since there is no machine model. The paper's arbitrary choice of nj(y),nk(y)n_j(y), n_k(y)nj​(y),nk​(y) is replaced by quantification over every non-adjacent pair mj∈Nj(y)m_j \in N_j(y)mj​∈Nj​(y), mk∈Nk(y)m_k \in N_k(y)mk​∈Nk​(y), which is Claim 13 for every possible choice. The case x=yx = yx=y is allowed.

One hypothesis is added to Claim 12: the four vertices ui,vi,uj,vju_i, v_i, u_j, v_jui​,vi​,uj​,vj​ are pairwise distinct, and the ends a,ba, ba,b of the path are required to be distinct. The paper's proof and its use in Claim 13 take the four vertices distinct; without the assumption the claim can fail, and without a≠ba \ne ba=b a one-vertex path would satisfy it vacuously.

The following trivializing readings are excluded: dropping the overline in "anticomplete to V(G)∖(S‾∪X)V(G) \setminus (\overline{S} \cup X)V(G)∖(S∪X)" (which, together with milestone 3, would force XXX to be isolated); a one-vertex path or repeated vertices in Claim 12; and subgraph instead of induced-subgraph containment for P7P_7P7​-freeness. The setting is satisfiable with X≠∅X \neq \emptysetX=∅: the 5-cycle y−a−s−t−b−yy - a - s - t - b - yy−a−s−t−b−y with S={s,t}S = \{s,t\}S={s,t}, L(s)={2}L(s) = \{2\}L(s)={2}, L(t)={3}L(t) = \{3\}L(t)={3}, L(a)={1,3}L(a) = \{1,3\}L(a)={1,3}, L(b)={1,2}L(b) = \{1,2\}L(b)={1,2}, L(y)={1,2,3}L(y) = \{1,2,3\}L(y)={1,2,3} satisfies every hypothesis, with y∈X1y \in X_1y∈X1​.

Proofs of the milestones and the goal are welcome, as are general lemmas about induced paths as lists (subpaths, concatenation through a connected set) that would serve other graph-theory missions.

Selected references

  • F. Bonomo, M. Chudnovsky, P. Maceli, O. Schaudt, M. Stein and M. Zhong, Three-coloring and list three-coloring of graphs without induced paths on seven vertices, Combinatorica 38 (2018) 779–801 (OnlineFirst 2017). https://doi.org/10.1007/s00493-017-3553-8
  • B. Randerath and I. Schiermeyer, 3-Colorability ∈ P for P₆-free graphs, Discrete Applied Mathematics 136 (2004) 299–313 (reference [21] of the paper).
  • B. Randerath, I. Schiermeyer and M. Tewes, Three-colorability and forbidden subgraphs. II: polynomial algorithms, Discrete Mathematics 251 (2002) 137–153 (reference [22] of the paper).
  • E. Camby and O. Schaudt, A new characterization of PkP_kPk​-free graphs, Algorithmica (reference [2] of the paper; the source of Theorem 4, which the other missions of this series use).
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CombinatoricsDiscrete GeometryGraph Theory·Captain: mikedeng1

Twin-width I: Tractable FO Model Checking 2: Every Subgraph of a Unit d-Dimensional Ball Graph with Clique Number k Has Twin-width at Most (3⌈√d⌉)^d·kResearch Paper

Motivation

Twin-width is a graph parameter introduced by Bonnet, Kim, Thomassé and Watrigant in Twin-width I: Tractable FO Model Checking (J. ACM 69(1), Article 3, 2021; arXiv:2004.14789). Its main theorem says that first-order model checking is fixed-parameter tractable on every class of graphs of bounded twin-width, provided a witnessing contraction sequence is given. This turns every class shown to have bounded twin-width into a class on which a whole logic becomes algorithmically tractable, so the question "which natural classes have bounded twin-width?" has direct algorithmic content.

Section 4 of the paper answers that question for several classes. This mission covers the geometric part of Section 4: ddd-dimensional grids, grids with diagonals, and unit ddd-dimensional ball graphs with bounded clique number. Geometric intersection graphs are a standard source of hard instances in parameterized algorithms. Width parameters designed for dense graphs (rank-width, clique-width, boolean-width) are unbounded already on the planar n×nn\times nn×n grid, whereas twin-width stays bounded on grids of every fixed dimension and transfers from there to ball graphs.

Setting

All graphs are finite and simple. Two vertex sets X,YX,YX,Y of a graph GGG are homogeneous if every pair (x,y)∈X×Y(x,y)\in X\times Y(x,y)∈X×Y is an edge or no pair is. For a partition P\mathcal PP of V(G)V(G)V(G), the red degree of a part XXX is the number of other parts not homogeneous to XXX; P\mathcal PP is a ddd-partition if every red degree is at most ddd. The graph GGG has twin-width at most ddd, tww⁡(G)≤d\operatorname{tww}(G)\le dtww(G)≤d, if there is a sequence P0,…,PN\mathcal P_0,\dots,\mathcal P_NP0​,…,PN​ of ddd-partitions of V(G)V(G)V(G) that starts with the partition into singletons, ends with at most one part, and in which each partition arises from the previous one by merging two parts. This is the paper's partition form of its definition by contractions of trigraphs (graphs with black and red edges, §3).

For the all-red trigraph Hr=(V,∅,E(H))H^r=(V,\emptyset,E(H))Hr=(V,∅,E(H)), in which every edge of HHH is red, the paper's contraction rule never produces a black edge, and two parts are red-adjacent exactly when some edge of HHH joins them. The red twin-width tww⁡(Hr)≤d\operatorname{tww}(H^r)\le dtww(Hr)≤d is defined as above with this adjacency.

For d,n≥1d,n\ge 1d,n≥1, the ddd-dimensional nnn-grid PndP^d_nPnd​ has vertex set [n]d[n]^d[n]d, with x∼yx\sim yx∼y iff ∑i∣xi−yi∣=1\sum_{i}|x_i-y_i|=1∑i​∣xi​−yi​∣=1. The grid with diagonals Kn,dK_{n,d}Kn,d​ has the same vertices, with distinct x∼yx\sim yx∼y iff max⁡i∣xi−yi∣≤1\max_i|x_i-y_i|\le 1maxi​∣xi​−yi​∣≤1, and Kn,drK^r_{n,d}Kn,dr​ is its all-red trigraph; RndR^d_nRnd​ is the all-red trigraph of PndP^d_nPnd​.

Given centres c(v)∈Rdc(v)\in\mathbb R^dc(v)∈Rd for vvv in a finite set VVV, the unit ball graph GGG joins distinct u,vu,vu,v iff the closed unit balls around c(u)c(u)c(u) and c(v)c(v)c(v) meet, that is ∥c(u)−c(v)∥2≤2\|c(u)-c(v)\|_2\le 2∥c(u)−c(v)∥2​≤2. Its clique number is the largest size of a set of pairwise adjacent vertices. A subgraph of GGG is obtained by deleting vertices and edges.

Formalization targets

Goal: Theorem 4.5 (p. 3:15)

For every d,kd,kd,k, every subgraph HHH of a unit ddd-dimensional ball graph GGG with clique number at most kkk satisfies

tww⁡(H)≤(3⌈d ⌉)d k.\operatorname{tww}(H)\le (3\lceil\sqrt d\,\rceil)^d\,k .tww(H)≤(3⌈d​⌉)dk.

Milestones, in the order the paper uses them

  1. Red paths have twin-width at most 222 (§3, p. 3:12).
  2. Induced subgraphs do not increase twin-width, for graphs and for all-red trigraphs (§4.1, p. 3:12).
  3. tww⁡(Rnd)≤3d\operatorname{tww}(R^d_n)\le 3dtww(Rnd​)≤3d for positive d,nd,nd,n (the statement proved inside Theorem 4.3, p. 3:15).
  4. Theorem 4.3: tww⁡(Pnd)≤3d\operatorname{tww}(P^d_n)\le 3dtww(Pnd​)≤3d for positive d,nd,nd,n.
  5. Every subgraph of PndP^d_nPnd​ has twin-width at most 3d3d3d (p. 3:15).
  6. Lemma 4.4: every subgraph of Kn,drK^r_{n,d}Kn,dr​ has twin-width at most 2(3d−1)2(3^d-1)2(3d−1).
  7. In a unit ball graph without a clique of size k+1k+1k+1, each half-open cell of side 2/d2/\sqrt d2/d​ contains at most kkk centres (proof of Theorem 4.5, p. 3:16).

A companion item, Theorem 4.1 (p. 3:13, graph case), states that adding one vertex joined to an arbitrary set at most changes twin-width from ttt to 2(t+1)2(t+1)2(t+1).

Significance

The goal theorem places unit ball graphs of bounded clique number, in every fixed dimension, among the classes of bounded twin-width. Combined with the paper's main theorem, and with the paper's remark that a contraction sequence can be computed in polynomial time from a geometric representation, it gives fixed-parameter tractable first-order model checking on these graphs. The clique-number hypothesis is needed: unit disk graphs without a clique bound have unbounded twin-width (p. 3:16), as shown in Twin-width II. Theorem 4.3 and Lemma 4.4 are of independent use as twin-width bounds for grids, and the subgraph statements show that grids are an exception to the general fact that bounded twin-width is not preserved by taking (non-induced) subgraphs (p. 3:13).

All results here are proved in the paper. To our knowledge none of them, and no notion of twin-width with red degree, is machine-checked in Lean or Mathlib. The work is to formalize the paper's arguments: the parallel contraction of grid layers, the supercell contraction, and the geometric counting.

Difficulty

Twin-width is not monotone under subgraphs, so the obvious route, "a unit ball graph of bounded clique number is a subgraph of a grid-like graph, hence has bounded twin-width", fails as stated. The paper repairs it by working with all-red trigraphs throughout: for an all-red trigraph, removing edges can only remove red adjacencies, and this is why Theorem 4.3 is proved in its red form and Lemma 4.4 is stated for Kn,drK^r_{n,d}Kn,dr​. A second difficulty is bookkeeping: the bound 3d3d3d comes from contracting the nnn layers of PndP^d_nPnd​ "in parallel" and tracking the red degree of every vertex at each step, and Lemma 4.4 is asserted "by the arguments of Theorem 4.3" without a separate proof, so its argument has to be reconstructed.

Formalization scope

Lean represents twin-width by the predicates TwinWidthLE G d and RedTwinWidthLE H d on finite vertex types: an explicit sequence of Finpartitions of the vertex set from ⊥ (singletons) to at most one part, consecutive partitions differing by one merge of two distinct parts. Twin-width is never a number, so no infimum over an empty set enters. [n]d[n]^d[n]d is Fin d → Fin n; centres live in EuclideanSpace ℝ (Fin d) with the Euclidean distance; balls are closed of radius 111, so centres at distance exactly 222 are adjacent. ⌈d ⌉\lceil\sqrt d\,\rceil⌈d​⌉ is the natural-number ceiling of the real square root. "Clique number kkk" is encoded as CliqueFree (k+1) (clique number at most kkk), which is the same theorem because the bound is monotone in kkk; subgraphs are a finite vertex set SSS together with a graph H≤G[S]H\le G[S]H≤G[S] on it.

The hypotheses 1≤d1\le d1≤d, 1≤n1\le n1≤n appear in Theorem 4.3, its red form, and the grid-subgraph statement, as on the page ("positive integers"). No other hypothesis is added; Lemma 4.4, the cell bound and the goal hold as stated also for d=0d=0d=0 or n=0n=0n=0. The red-degree count uses "some edge joins the two parts", which is derived from the paper's contraction rule for trigraphs without black edges and is used only for all-red trigraphs; the twin-width of graphs counts non-homogeneous parts. This rules out the trivializing readings: a twin-width defined as an infimum that defaults to 000, a sequence allowed to jump to one part, homogeneity counted as adjacency for graphs, or a bound depending on the graph. The polynomial-time sentence of Theorem 4.5 is not formalized.

Reusable infrastructure: the partition-form twin-width predicates (shared with the other missions of this series), grids and grids with diagonals in coordinates, and unit ball graphs. Contributions are welcome on the general lemmas (induced subgraphs, red-to-black transfer, small explicit sequences) as well as on the grid theorems themselves.

Selected references

  • É. Bonnet, E. J. Kim, S. Thomassé, R. Watrigant, Twin-width I: Tractable FO Model Checking, Journal of the ACM 69(1), Article 3, 2021. https://doi.org/10.1145/3486655 (preprint: https://arxiv.org/abs/2004.14789)
  • É. Bonnet, C. Geniet, E. J. Kim, S. Thomassé, R. Watrigant, Twin-width II: small classes, Combinatorial Theory 2(2), 2022. https://arxiv.org/abs/2006.09877
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CombinatoricsGraph TheoryMathematical Logic·Captain: mikedeng1

Twin-width I: Tractable FO Model Checking 5: First-Order Interpretations of a Class of Graphs of Bounded Twin-width Have Bounded Twin-widthResearch Paper

Why interpretations

Twin-width is a graph parameter introduced by Bonnet, Kim, Thomassé and Watrigant in Twin-width I: Tractable FO Model Checking (J. ACM 69(1), Article 3, 2021; arXiv:2004.14789). Its main algorithmic consequence is that first-order model checking is fixed-parameter tractable on graphs given with a contraction sequence of bounded width. A parameter of this kind is useful only if the classes it bounds are closed under the constructions that arise in practice. Many such constructions are first-order definable: the complement of a graph, its square (join vertices at distance at most two), the map graph of a planar map. Section 8 of the paper shows that twin-width is stable under every such construction: a first-order interpretation of a class of bounded twin-width has bounded twin-width. Bounded VC-dimension, by contrast, is not preserved (interval graphs have VC-dimension at most two but interpret every graph, p. 3:41).

The result has since become the basis of the "model-theoretic" view of twin-width: bounded twin-width classes are closed under first-order transductions (Theorem 8.1 of the paper), and later work identifies them, among ordered structures, with the monadically dependent classes (Twin-width IV, Bonnet, Giocanti, Ossona de Mendez, Simon, Thomassé and Toruńczyk).

Setting

Let GGG be a finite simple graph on a vertex set VVV.

Two vertex sets X,YX,YX,Y are homogeneous if all pairs in X×YX\times YX×Y are edges or none is. For a partition P\mathcal PP of VVV, the red graph GPG_{\mathcal P}GP​ has the parts as vertices, two distinct parts being adjacent when they are not homogeneous. P\mathcal PP is a ddd-partition if GPG_{\mathcal P}GP​ has maximum degree at most ddd. The graph GGG has twin-width at most ddd, tww⁡(G)≤d\operatorname{tww}(G)\le dtww(G)≤d, if there is a sequence of ddd-partitions from the partition into singletons to a partition with at most one part, each obtained from the previous one by merging two parts (p. 3:32).

A prenex formula of depth ℓ\ellℓ with two free variables is

φ(x,y)=Q1x1 Q2x2⋯Qℓxℓ φ∗,Qi∈{∀,∃},\varphi(x,y)=Q_1x_1\,Q_2x_2\cdots Q_\ell x_\ell\ \varphi^*,\qquad Q_i\in\{\forall,\exists\},φ(x,y)=Q1​x1​Q2​x2​⋯Qℓ​xℓ​ φ∗,Qi​∈{∀,∃},

with φ∗\varphi^*φ∗ a Boolean combination of atoms u=vu=vu=v and E(u,v)E(u,v)E(u,v), u,v∈{x1,…,xℓ,x,y}u,v\in\{x_1,\dots,x_\ell,x,y\}u,v∈{x1​,…,xℓ​,x,y}. The interpretation φ(G)\varphi(G)φ(G) is the graph on VVV in which distinct u,vu,vu,v are adjacent iff G⊨φ(u,v)∧φ(v,u)G\models\varphi(u,v)\wedge\varphi(v,u)G⊨φ(u,v)∧φ(v,u). For a class G\mathcal GG, φ(G)\varphi(\mathcal G)φ(G) is the class of all induced subgraphs of the graphs φ(G)\varphi(G)φ(G), G∈GG\in\mathcal GG∈G.

The proof works with morphism-trees. The complete tree MTk(V)MT_k(V)MTk​(V) has as nodes all tuples (v1,…,vi)(v_1,\dots,v_i)(v1​,…,vi​) of vertices with i≤ki\le ki≤k, the parent of a tuple being its prefix. Two sibling nodes are equivalent in (G,P)(G,\mathcal P)(G,P) if an automorphism of the tree swaps them, preserving equalities and adjacencies among the entries of every tuple and the part of P\mathcal PP of every entry. A reduction deletes one of two equivalent siblings with its subtree, repeatedly; a reduct admits no further reduction. Two vertices u,u′u,u'u,u′ are adjacent in Eℓ+2(G,P)E_{\ell+2}(G,\mathcal P)Eℓ+2​(G,P) when (u)(u)(u) and (u′)(u')(u′) are equivalent in some reduction of MTℓ+2(V)MT_{\ell+2}(V)MTℓ+2​(V), and Iℓ+2(G,P)I_{\ell+2}(G,\mathcal P)Iℓ+2​(G,P) is the partition into the connected components of Eℓ+2(G,P)E_{\ell+2}(G,\mathcal P)Eℓ+2​(G,P).

Formalization targets

Goal: Theorem 8.3 (graphs)

For every prenex formula φ(x,y)\varphi(x,y)φ(x,y) and every ddd there is DDD such that

tww⁡(G)≤d ⟹ tww⁡(φ(G)[S])≤Dfor every graph G and every S⊆V(G).\operatorname{tww}(G)\le d\ \Longrightarrow\ \operatorname{tww}\bigl(\varphi(G)[S]\bigr)\le D\quad\text{for every graph } G \text{ and every } S\subseteq V(G).tww(G)≤d ⟹ tww(φ(G)[S])≤Dfor every graph G and every S⊆V(G).

The bound DDD depends on φ\varphiφ and ddd only. No explicit function is asserted: the paper gives none (the proof goes through a tower-type bound on reducts).

Milestones

  1. Lemma 5.2 in graph form (p. 3:18, applied on p. 3:43): rrr-refining hhh-partitions from the finest to the coarsest partition give tww⁡(G)≤r(h+1)\operatorname{tww}(G)\le r(h+1)tww(G)≤r(h+1).
  2. Lemma 7.3 (p. 3:32): reducts of MTℓ(G)MT_\ell(G)MTℓ​(G) have size bounded by a function of ℓ\ellℓ.
  3. Lemmas 7.11–7.14 (pp. 3:35–3:38): restriction to connected tuples rooted at a part and the pruned shuffle commute with reductions; the pruned shuffle of all MTℓ(G,P,X)MT_\ell(G,\mathcal P,X)MTℓ​(G,P,X) is MTℓ(G,P)MT_\ell(G,\mathcal P)MTℓ​(G,P), and that of reducts is a reduction of it.
  4. Lemma 8.4 (p. 3:41) and its extension to reductions (p. 3:42): equivalent nodes (u,v),(u,v′)(u,v),(u,v')(u,v),(u,v′) of MTℓ+2MT_{\ell+2}MTℓ+2​ satisfy the same prenex formulas of depth ℓ\ellℓ.
  5. Iℓ+2I_{\ell+2}Iℓ+2​ refines P\mathcal PP and is monotone under coarsening (p. 3:42).
  6. Lemma 8.5 (p. 3:42): a part of a ddd-partition meets boundedly many components of Eℓ+2(G,P)E_{\ell+2}(G,\mathcal P)Eℓ+2​(G,P).
  7. Lemma 8.6 (p. 3:43): parts of Iℓ+2(G,P)I_{\ell+2}(G,\mathcal P)Iℓ+2​(G,P) inside parts at distance at least 3ℓ+23^{\ell+2}3ℓ+2 in GPG_{\mathcal P}GP​ are homogeneous in φ(G)\varphi(G)φ(G).

Significance

Theorem 8.3 turns every first-order definable graph construction into a source of bounded-twin-width classes: squares and fixed powers of planar graphs, complements, map graphs (as transductions, via Theorem 8.1), kkk-planar graphs and bounded-degree string graphs. Combined with the model-checking algorithm it gives FPT first-order model checking on all these classes, provided a contraction sequence is available. The theorem is also the first step of the model-theoretic characterisations of bounded twin-width in the later papers of the series.

The result is proved in the paper; no machine-checked proof of it, or of any twin-width bound, exists to our knowledge, and Mathlib has no notion of twin-width or of first-order interpretations of graphs. The mission asks for a formal proof of the graph case. The morphism-tree milestones are also the combinatorial core of the paper's linear-time model-checking algorithm (Theorems 7.5, 7.15), whose running-time statements are not part of this mission.

Difficulty

The obvious approach refines the ddd-partitions Pi\mathcal P_iPi​ of GGG by the "type" of each vertex with respect to φ\varphiφ. The number of such types is not bounded: a vertex's behaviour depends on the whole graph through the quantifiers. The paper replaces types by the components of Eℓ+2(G,Pi)E_{\ell+2}(G,\mathcal P_i)Eℓ+2​(G,Pi​), defined through reductions of morphism-trees that respect Pi\mathcal P_iPi​. Two facts must then be shown, and neither is local in an obvious way. First, the number of components inside a part is bounded (Lemma 8.5); this needs the pruned shuffle, which assembles a reduction of the whole tree MTℓ+2(G,P)MT_{\ell+2}(G,\mathcal P)MTℓ+2​(G,P) from reductions of the local trees MTℓ+2(G,P,X)MT_{\ell+2}(G,\mathcal P,X)MTℓ+2​(G,P,X), and the fact that it commutes with reductions (Lemma 7.12), where an automorphism of one local tree must be extended to the shuffle without breaking adjacency between non-homogeneous parts. Second, far-apart components are homogeneous in φ(G)\varphi(G)φ(G) (Lemma 8.6), which needs the evaluation argument of Lemma 8.4 inside a reduction of the partitioned tree.

Formalization scope

  • Graphs are SimpleGraph V on a Fintype with decidable equality. Twin-width is the predicate TwinWidthLE G d in the paper's partition form (pp. 3:12, 3:32); trigraphs are not formalized, and twin-width is never an infimum, so no junk value of sInf can make a bound vacuous. Merge steps merge exactly two distinct parts, so a sequence cannot jump to one part.
  • Formulas are Mathlib's FirstOrder.Language.graph.Formula (Fin 2), evaluated in G.structure; variable 0 is xxx, variable 1 is yyy. Prenex is Mathlib's IsPrenex; quantifier depth qdepth is defined in the mission (∃=¬∀¬\exists=\neg\forall\neg∃=¬∀¬ counts once).
  • The interpretation requires u≠vu\neq vu=v for an edge (a simple graph has no loops). The goal is the graph case of Theorem 8.3, which the page states for augmented binary structures; Section 8 itself says it works with undirected graphs (p. 3:40).
  • In the goal the bound DDD is chosen after φ\varphiφ and ddd and before the graph: a bound chosen after the graph would make the statement trivial. The hereditary closure (induced subgraphs on every SSS) is part of the statement.
  • Morphism-trees are sets of tuples (Set (List V)), the paper's identification of a node with its current path (p. 3:30), which is exact for reductions of complete trees. Equivalent siblings are distinct. Distances in GPG_{\mathcal P}GP​ are in N∪{∞}\mathbb N\cup\{\infty\}N∪{∞}, so disconnected parts are far apart. The sequence graph uses 0-based indices, hence the exponent 3ℓ−(k+1)3^{\ell-(k+1)}3ℓ−(k+1). The pruned shuffle is defined by its characterisation (each component of the sequence graph of a tuple lies in the tree of its local root). Lemmas of §7.3 carry its standing assumption ℓ>0\ell>0ℓ>0.
  • Lemma 5.2 is posed for graphs with the bound r(h+1)r(h+1)r(h+1) (the matrix lemma's rtrtrt with t=h+1t=h+1t=h+1).
  • Not in the mission: Theorem 8.1 (transductions), Lemma 8.2 and Lemma 5.1 (augmented binary structures), and all running-time statements (Theorems 1.1, 7.1, 7.5, 7.15, Corollaries 7.16–7.17).

Reusable beyond this mission: the partition form of twin-width, quantifier depth of first-order formulas, and the morphism-tree machinery (reductions, pruned shuffles), which formalizes the algorithmic core of first-order model checking on bounded twin-width. Contributions welcome: proofs of the §7 lemmas, of Lemma 8.4 by induction on the quantifier prefix, and the closure of twin-width under induced subgraphs.

Selected references

  • É. Bonnet, E. J. Kim, S. Thomassé, R. Watrigant, Twin-width I: Tractable FO Model Checking, J. ACM 69(1), Article 3, 2021. https://doi.org/10.1145/3486655 (arXiv:2004.14789, https://arxiv.org/abs/2004.14789)
  • É. Bonnet, U. Giocanti, P. Ossona de Mendez, P. Simon, S. Thomassé, S. Toruńczyk, Twin-width IV: Ordered Graphs and Matrices, J. ACM, 2024. https://arxiv.org/abs/2102.03117
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Graph TheoryOperations ResearchProbability+1·Captain: mikedeng1

Graphon Mean Field Systems V: On Percolated Graphs Sampled From a Lipschitz Graphon the Mean-Square Error Is at Most κ(q)/(nβₙ)^{1/q}Research Paper

Motivation

Large systems of interacting diffusions — neurons, oscillators, agents in a network game, particles in a queueing or load-balancing model — are usually analysed through their mean-field limit: as the population grows, each particle interacts with the empirical law of the others, and the system is replaced by a single nonlinear (McKean–Vlasov) equation. The classical theory assumes that every particle interacts with every other one with the same strength. Real networks are heterogeneous and sparse: particle iii interacts with particle jjj only through an edge of a random graph, and the number of neighbours of a particle is much smaller than the population size.

Bayraktar, Chakraborty and Wu (Ann. Appl. Probab. 33(5), 2023) describe the heterogeneity by a graphon and prove laws of large numbers and rates of convergence for such systems. This mission is the fifth of a series formalizing that paper. Its subject is the paper's quantitative result for not-so-dense graphs: when the edges are sampled from a Lipschitz graphon and then thinned by a sparsity factor βn\beta_nβn​, the average mean-square distance between each particle and its graphon limit is of order (nβn)−1/q(n\beta_n)^{-1/q}(nβn​)−1/q for every q>1q>1q>1.

Setting

Let I=[0,1]I=[0,1]I=[0,1] with Lebesgue measure. A graphon is a measurable symmetric function G:I×I→[0,1]G:I\times I\to[0,1]G:I×I→[0,1]. Fix a horizon T>0T>0T>0 and write Cd=C([0,T]:Rd)\mathcal C_d=C([0,T]:\mathbb R^d)Cd​=C([0,T]:Rd) with the norm ∥x∥∗,T=sup⁡0≤s≤T∣xs∣\|x\|_{*,T}=\sup_{0\le s\le T}|x_s|∥x∥∗,T​=sup0≤s≤T​∣xs​∣.

One probability space carries, for every label u∈Iu\in Iu∈I, an initial state Xu(0)X_u(0)Xu​(0) with law μu(0)\mu_u(0)μu​(0) and a standard ddd-dimensional Brownian motion BuB_uBu​, the whole family {Xu(0),Bu:u∈I}\{X_u(0),B_u:u\in I\}{Xu​(0),Bu​:u∈I} being independent. The limit system (4.2) is a continuum of diffusions, one per label:

Xu(t)=Xu(0)+∫0t ⁣∫I ⁣∫Rdb(Xu(s),x) G(u,v) μv,s(dx) dv ds+∫0tσ(Xu(s)) dBu(s),μu,t=L(Xu(t)).X_u(t)=X_u(0)+\int_0^t\!\int_I\!\int_{\mathbb R^d}b(X_u(s),x)\,G(u,v)\,\mu_{v,s}(dx)\,dv\,ds+\int_0^t\sigma(X_u(s))\,dB_u(s),\qquad \mu_{u,t}=\mathcal L(X_u(t)).Xu​(t)=Xu​(0)+∫0t​∫I​∫Rd​b(Xu​(s),x)G(u,v)μv,s​(dx)dvds+∫0t​σ(Xu​(s))dBu​(s),μu,t​=L(Xu​(t)).

The particles are independent but not identically distributed; their laws are coupled through the dvdvdv-integral.

The not-so-dense nnn-particle system (4.1) uses the same initial states and Brownian motions at the labels i/ni/ni/n:

Xin(t)=Xi/n(0)+∫0t1nβn∑j=1nξijn b(Xin(s),Xjn(s)) ds+∫0tσ(Xin(s)) dBi/n(s),i=1,…,n.X^n_i(t)=X_{i/n}(0)+\int_0^t\frac{1}{n\beta_n}\sum_{j=1}^n\xi^n_{ij}\,b(X^n_i(s),X^n_j(s))\,ds+\int_0^t\sigma(X^n_i(s))\,dB_{i/n}(s),\qquad i=1,\dots,n.Xin​(t)=Xi/n​(0)+∫0t​nβn​1​j=1∑n​ξijn​b(Xin​(s),Xjn​(s))ds+∫0t​σ(Xin​(s))dBi/n​(s),i=1,…,n.

The edges are percolated samples of GGG (Condition 4.3): ξijn=ξjin∼Bernoulli(βnG(i/n,j/n))\xi^n_{ij}=\xi^n_{ji}\sim\mathrm{Bernoulli}(\beta_nG(i/n,j/n))ξijn​=ξjin​∼Bernoulli(βn​G(i/n,j/n)), independent for 1≤i≤j≤n1\le i\le j\le n1≤i≤j≤n and independent of the noise. A particle has about nβnn\beta_nnβn​ neighbours, which is why the interaction is scaled by 1/(nβn)1/(n\beta_n)1/(nβn​).

The standing hypotheses are Condition 4.1 — u↦μu(0)u\mapsto\mu_u(0)u↦μu​(0) measurable with bounded second moments; bbb bounded and Lipschitz; σ\sigmaσ bounded, Lipschitz and invertible with bounded inverse; βn∈(0,1]\beta_n\in(0,1]βn​∈(0,1] and nβn→∞n\beta_n\to\inftynβn​→∞ — and Condition 2.3: on finitely many intervals I1,…,INI_1,\dots,I_NI1​,…,IN​ covering III, the map u↦μu(0)u\mapsto\mu_u(0)u↦μu​(0) is Lipschitz in the Wasserstein distance W2W_2W2​, and GGG is Lipschitz on every block Ii×IjI_i\times I_jIi​×Ij​.

Formalization targets

Goal: Theorem 4.2

Under Conditions 2.3, 4.1 and 4.3, for each q∈(1,∞)q\in(1,\infty)q∈(1,∞) there is κ(q)∈(0,∞)\kappa(q)\in(0,\infty)κ(q)∈(0,∞) with

1n∑i=1nE∥Xin−Xi/n∥∗,T2≤κ(q)(nβn)1/qfor all n∈N.\frac1n\sum_{i=1}^n\mathbb E\big\|X^n_i-X_{i/n}\big\|_{*,T}^2\le\frac{\kappa(q)}{(n\beta_n)^{1/q}}\qquad\text{for all }n\in\mathbb N .n1​i=1∑n​E​Xin​−Xi/n​​∗,T2​≤(nβn​)1/qκ(q)​for all n∈N.

The constant depends on qqq and on the data, never on nnn. The bound is on the average over particles, not on the maximum.

Milestones

  1. Lemma 7.1: all moments of the coupling error are bounded uniformly in nnn and iii.
  2. (7.10): E[ξijn∣Xjn(s)−Xj/n(s)∣2]≤(2E∣Xjn(s)−Xj/n(s)∣2+κ(q)(nβn)−1/q)βnG(i/n,j/n)\mathbb E[\xi^n_{ij}|X^n_j(s)-X_{j/n}(s)|^2]\le\big(2\mathbb E|X^n_j(s)-X_{j/n}(s)|^2+\kappa(q)(n\beta_n)^{-1/q}\big)\beta_nG(i/n,j/n)E[ξijn​∣Xjn​(s)−Xj/n​(s)∣2]≤(2E∣Xjn​(s)−Xj/n​(s)∣2+κ(q)(nβn​)−1/q)βn​G(i/n,j/n).
  3. (7.15): the interaction error Rsn,2R^{n,2}_sRsn,2​ is at most (κ/n)∑jE∣Xjn(s)−Xj/n(s)∣2+κ(q)(nβn)−1/q(\kappa/n)\sum_j\mathbb E|X^n_j(s)-X_{j/n}(s)|^2+\kappa(q)(n\beta_n)^{-1/q}(κ/n)∑j​E∣Xjn​(s)−Xj/n​(s)∣2+κ(q)(nβn​)−1/q.
  4. Theorem 2.1(b) for (4.2): W2,T(μu,μv)≤κ∣u−v∣W_{2,T}(\mu_u,\mu_v)\le\kappa|u-v|W2,T​(μu​,μv​)≤κ∣u−v∣ for u,vu,vu,v in one interval IiI_iIi​.
  5. §7.3 display: the discretization error Rsn,4R^{n,4}_sRsn,4​ is at most κ/n2\kappa/n^2κ/n2.

Significance

Theorem 4.2 gives an explicit rate for the convergence of a particle system on a sparse random graph to its graphon limit. Its companion, Theorem 4.1 (mission IV), proves the law of large numbers under weaker hypotheses but without a rate. The rate says that the effective sample size is nβnn\beta_nnβn​, the typical degree, not nnn: graphs with βn→0\beta_n\to0βn​→0 still approximate the graphon system as long as the degree grows. Results of this type justify replacing a large heterogeneous network by its graphon limit in control and game problems, such as graphon mean-field games, where the error of the replacement must be quantified.

The paper proves the theorem by hand; none of its results has a machine-checked proof. The formalization produces precise statements of the not-so-dense model, of the estimates of §7.1 that hold for any sparsity, and of the discretization bound, each usable on its own. The milestones (7.10) and (7.15) are the paper's key estimates for sparse interactions and are shared with mission IV.

Difficulty

The obvious approach is to compare each XinX^n_iXin​ with Xi/nX_{i/n}Xi/n​ by Gronwall's inequality, after bounding the difference of drifts. That step fails at the interaction term: the edge ξijn\xi^n_{ij}ξijn​ and the error Xjn−Xj/nX^n_j-X_{j/n}Xjn​−Xj/n​ are dependent, because the edge enters the dynamics of particle jjj. A plain Cauchy–Schwarz bound loses a factor 1/βn1/\beta_n1/βn​ and gives nothing when βn→0\beta_n\to0βn​→0. Estimates (7.10) and (7.15) quantify how weak this dependence is, and they are where the hypotheses that σ\sigmaσ is invertible with bounded inverse and that nβn→∞n\beta_n\to\inftynβn​→∞ are needed. The discretization term needs the Lipschitz regularity of the limit laws in the label (Theorem 2.1(b)), itself a fixed-point estimate on a space of measure-valued maps.

Formalization scope

The Lean development uses Mathlib's unitInterval for III, Fin d → ℝ with its sup norm for Rd\mathbb R^dRd (all constants are existential, so the choice of norm does not matter), time ℝ≥0, and the path space Cd\mathcal C_dCd​ as continuous maps on [0,T][0,T][0,T] with the sup norm. Brownian motions, Itô integrals and Itô processes are those of the published Peng1990.SMP.Stochastic; Wasserstein distances are the published WassersteinDRO.Duality.wassersteinDistance, valued in [0,∞][0,\infty][0,∞]. Particle iii is Lean's i : Fin n with label (i+1)/n(i+1)/n(i+1)/n.

Committed conventions:

  • A solution of (4.2) has continuous paths, AE-measurable path maps, and path laws in the class M\mathcal MM (measurable in uuu, bounded second moments); each XuX_uXu​ is a strong solution for the filtration of (Xu(0),Bu)(X_u(0),B_u)(Xu​(0),Bu​). A solution of (4.1) is a strong solution for the filtration of the edges, the initial states and the Brownian motions of the nnn labels.
  • The edges are {0,1}\{0,1\}{0,1}-valued, symmetric, with the diagonal included, mutually independent over i≤ji\le ji≤j, and independent of the σ-algebra of the noise.
  • Condition 4.1(d) is required for n≥1n\ge1n≥1; the invertibility of σ\sigmaσ is that of a d×dd\times dd×d matrix; the intervals of Condition 2.3 are order-connected subsets of III.
  • Expectations of nonnegative quantities are lower Lebesgue integrals, so no expectation is silently 000 for a non-integrable integrand.

The solution predicates are not vacuous: the zero-coefficient system Xu(t)=Xu(0)X_u(t)=X_u(0)Xu​(t)=Xu​(0) satisfies both, Condition 4.1 and Condition 4.3 are satisfiable, and every statement quantifies over solutions rather than assuming the conclusion. The constant κ(q)\kappa(q)κ(q) is chosen after qqq and before nnn, so it cannot depend on nnn, and the bound is the paper's average over iii, not a weaker or a stronger form. At n=0n=0n=0 both sides of every rate are 000.

The paper's proofs are in its §5 (Theorem 2.1), §7.1 (Lemma 7.1, (7.10), (7.15)) and §7.3 (Theorem 4.2). Stochastic analysis at that level — Burkholder–Davis–Gundy and Rosenthal inequalities, Girsanov's theorem for these SDEs, Gronwall arguments for measure-valued fixed points — is mostly absent from Mathlib, and contributions of such infrastructure are welcome, as are proofs of any milestone.

Selected references

  • E. Bayraktar, S. Chakraborty, R. Wu, Graphon mean field systems, Ann. Appl. Probab. 33(5):3587–3619, 2023. https://doi.org/10.1214/22-AAP1901
  • L. Lovász, Large Networks and Graph Limits, AMS Colloquium Publications 60, 2012. https://doi.org/10.1090/coll/060
  • B. Bollobás, C. Borgs, J. Chayes, O. Riordan, Percolation on dense graph sequences, Ann. Probab. 38(1):150–183, 2010. https://doi.org/10.1214/09-AOP478
  • S. Peng, A general stochastic maximum principle for optimal control problems, SIAM J. Control Optim. 28(4):966–979, 1990. https://doi.org/10.1137/0328054
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Operations ResearchProbabilityStochastic Systems·Captain: mikedeng1

Steady-State Analysis of the Join-the-Shortest-Queue Model in the Halfin-Whitt Regime 1: Diffusion-Scaled Stationary Queue Lengths Have Expectations Bounded Uniformly in nResearch Paper

Motivation

Join-the-shortest-queue (JSQ) is the load-balancing rule in which each arriving job is sent to a server with the fewest jobs. It is a baseline in the design of server farms and data centers, and in the many-server Halfin–Whitt regime, where the load per server approaches one at rate 1/n1/\sqrt n1/n​, it combines near-full utilization with vanishing waiting. Eschenfeldt and Gamarnik (arXiv:1502.00999, 2015) proved that the suitably scaled JSQ process converges, over bounded time intervals, to a two-dimensional reflected diffusion; Mukherjee, Borst, van Leeuwaarden and Whiting (J. Appl. Probab. 53, 2016) gave the form of the result that Braverman quotes as Theorem 1. Process-level convergence over bounded time intervals says nothing about the stationary distribution. To conclude that the stationary distributions converge as well, one needs tightness of the scaled stationary distributions, uniformly in the number of servers nnn.

Braverman (arXiv:1801.05121, Math. Oper. Res. 45(3), 2020) supplied this, together with positive recurrence of the diffusion limit. This mission formalizes the first of the two main results, Theorem 2, and the chain of lemmas the paper uses to prove it.

Setting

There are nnn identical servers, each with its own infinite buffer. Jobs arrive as a Poisson process of rate nλn\lambdanλ and service times are i.i.d. exponential with mean one. An arriving job joins a server with the fewest jobs, ties broken arbitrarily. The Halfin–Whitt regime is

λ=1−β/n,β>0 fixed.\lambda = 1 - \beta/\sqrt n,\qquad \beta > 0 \text{ fixed}.λ=1−β/n​,β>0 fixed.

For i≥1i \ge 1i≥1, QiQ_iQi​ is the number of servers with at least iii jobs. The process Q=(Q1,Q2,… )Q = (Q_1, Q_2, \dots)Q=(Q1​,Q2​,…) is a continuous-time Markov chain on

S={q∈{0,1,…,n}∞ ∣ qi≥qi+1, ∑iqi<∞}.S = \Big\{ q \in \{0,1,\dots,n\}^\infty \ \Big|\ q_i \ge q_{i+1},\ \textstyle\sum_i q_i < \infty \Big\}.S={q∈{0,1,…,n}∞ ​ qi​≥qi+1​, ∑i​qi​<∞}.

Its generator GQG_QGQ​ sends qqq to q+e(i)q + e^{(i)}q+e(i) at rate nλn\lambdanλ when q1=⋯=qi−1=n>qiq_1 = \dots = q_{i-1} = n > q_iq1​=⋯=qi−1​=n>qi​, and to q−e(i)q - e^{(i)}q−e(i) at rate qi−qi+1q_i - q_{i+1}qi​−qi+1​. The fluid-scaled coordinates are X1=(Q1−n)/n≤0X_1 = (Q_1 - n)/n \le 0X1​=(Q1​−n)/n≤0, the negative of the fraction of idle servers, and Xi=Qi/nX_i = Q_i/nXi​=Qi​/n for i≥2i \ge 2i≥2. The diffusion-scaled coordinates are nXi\sqrt n X_in​Xi​. Expectations E\mathbb EE are taken under a stationary distribution π\piπ of the chain.

The proof works with functions on Ω=(−∞,0]×[0,∞)\Omega = (-\infty, 0] \times [0, \infty)Ω=(−∞,0]×[0,∞) and with the first-order operator

Lf(x)=(−x1+x2−β/n)f1(x)−x2f2(x),Lf(x) = (-x_1 + x_2 - \beta/\sqrt n) f_1(x) - x_2 f_2(x),Lf(x)=(−x1​+x2​−β/n​)f1​(x)−x2​f2​(x),

where fif_ifi​ is the partial derivative in xix_ixi​, taken one-sided on ∂Ω\partial\Omega∂Ω.

Formalization targets

Goal: Theorem 2

For each β>0\beta > 0β>0 there is a constant C(β)C(\beta)C(β) such that for all n≥1n \ge 1n≥1 with β<n\beta < \sqrt nβ<n​ and every stationary distribution,

E∣nXi∣≤C(β),  i=1,2,E∣nXi∣≤C(β),  i≥3.\mathbb E\big|\sqrt n X_i\big| \le C(\beta),\ \ i = 1, 2,\qquad \mathbb E\big|n X_i\big| \le C(\beta),\ \ i \ge 3.E​n​Xi​​≤C(β),  i=1,2,E​nXi​​≤C(β),  i≥3.

The constant depends on β\betaβ only, not on nnn, the stationary distribution, or iii.

Milestones, in the order the proof uses them

  1. Lemma 1: E GQf(Q)=0\mathbb E\,G_Q f(Q) = 0EGQ​f(Q)=0 whenever E∣f(Q)∣<∞\mathbb E|f(Q)| < \inftyE∣f(Q)∣<∞.
  2. Lemma 2: EQ1=nλ\mathbb E Q_1 = n\lambdaEQ1​=nλ and EQi=nλ P(Q1=⋯=Qi−1=n)\mathbb E Q_i = n\lambda\,\mathbb P(Q_1 = \dots = Q_{i-1} = n)EQi​=nλP(Q1​=⋯=Qi−1​=n).
  3. Lemma 3: the generator, applied to f(x1,x2)f(x_1, x_2)f(x1​,x2​), equals Lf(x)+(f2−f1)(x)λ1(x1=0)+ε(x)Lf(x) + (f_2 - f_1)(x)\lambda 1(x_1 = 0) + \varepsilon(x)Lf(x)+(f2​−f1​)(x)λ1(x1​=0)+ε(x) with an explicit remainder ε\varepsilonε built from second weak derivatives.
  4. Lemmas 5 and 6: the curve Γ(κ)\Gamma^{(\kappa)}Γ(κ) and the hitting time τ(x)\tau(x)τ(x) of the fluid model; existence and uniqueness, finiteness, derivative formulas and monotonicity in κ\kappaκ.
  5. Lemma 7 and Lemma 4: for κ>β\kappa > \betaκ>β, the explicit function f∗f^*f∗ of (4.14) solves
Lf(x)=−((x2−κ/n)∨0) on Ω,f1(0,x2)=f2(0,x2),Lf(x) = -\big((x_2 - \kappa/\sqrt n)\vee 0\big)\ \text{on } \Omega,\qquad f_1(0, x_2) = f_2(0, x_2),Lf(x)=−((x2​−κ/n​)∨0) on Ω,f1​(0,x2​)=f2​(0,x2​),

with f11∗,f12∗,f22∗≥0f^*_{11}, f^*_{12}, f^*_{22} \ge 0f11∗​,f12∗​,f22∗​≥0, vanishing second derivatives for x2≤κ/nx_2 \le \kappa/\sqrt nx2​≤κ/n​, and explicit upper bounds of order n/β\sqrt n/\betan​/β above that level. 6. (3.18): E((X2−κ/n)∨0)≤1βn(12+6κκ−β)P(X2≥κ/n−1/n)\mathbb E\big((X_2 - \kappa/\sqrt n)\vee 0\big) \le \frac{1}{\beta\sqrt n}\big(12 + \frac{6\kappa}{\kappa - \beta}\big)\mathbb P(X_2 \ge \kappa/\sqrt n - 1/n)E((X2​−κ/n​)∨0)≤βn​1​(12+κ−β6κ​)P(X2​≥κ/n​−1/n). 7. Theorem 2, (2.2): the i=1,2i = 1, 2i=1,2 half of the goal.

Significance

Theorem 2 shows that in steady state the number of idle servers and the number of servers holding two or more jobs are O(n)O(\sqrt n)O(n​) on average, and the number of servers holding i≥3i \ge 3i≥3 jobs is O(1)O(1)O(1) on average, uniformly in nnn. Combined with the process-level limit and the positive recurrence of the limiting diffusion (Theorem 3, the companion mission), it yields Proposition 1: the diffusion-scaled stationary distribution converges to the stationary distribution of the diffusion. This justifies the diffusion as a steady-state approximation for JSQ.

The method is the generator-comparison or Stein's-method approach: a Lyapunov function solving a first-order PDE for the fluid model, with explicit bounds on its derivatives. It applies to other many-server systems, and the paper is an example of that approach on an infinite-dimensional chain whose diffusion limit is two-dimensional.

The result is proved in the paper; no machine-checked proof is known to exist. The work remaining is to formalize the known proof: the adjoint relation for a countable-state chain with bounded rates, the Taylor expansion of the generator, and the explicit analysis of f∗f^*f∗ through the fluid curves.

Difficulty

The obvious route is to bound P(Q1=⋯=Qi−1=n)\mathbb P(Q_1 = \dots = Q_{i-1} = n)P(Q1​=⋯=Qi−1​=n) in Lemma 2 directly. The paper notes that no good handle on these probabilities exists. The PDE route needs a solution whose second derivatives are bounded by O(n)O(\sqrt n)O(n​). General results that give such bounds require a continuous fluid vector field, and the JSQ fluid model is discontinuous because of the reflection at x1=0x_1 = 0x1​=0. So f∗f^*f∗ is constructed explicitly from the fluid paths, and its derivatives must be bounded by hand through the implicitly defined τ(x)\tau(x)τ(x) and ν∗(x1)\nu^*(x_1)ν∗(x1​).

A second difficulty is dimensional: the chain is infinite-dimensional while the PDE is two-dimensional, so the remainder of Lemma 3 contains a term with q3q_3q3​ that is controlled only by combining Lemma 2 with the monotonicity of f2∗f^*_2f2∗​.

Formalization scope

  • Model. States are functions ℕ → ℕ with 0-based indices: Lean q.1 i is the paper's qi+1q_{i+1}qi+1​, so the goal's "i≥3i \ge 3i≥3" is Lean index ≥2\ge 2≥2. Each state is bounded by nnn, nonincreasing and eventually zero. The generator genQ is the displayed formula on p. 6.
  • Stationarity. No process is constructed. A stationary distribution is a probability π\piπ on SSS satisfying global balance πGQ=0\pi G_Q = 0πGQ​=0, which characterizes stationarity for this chain with bounded rates. Such a π\piπ exists, since the chain is positive recurrent for λ<1\lambda < 1λ<1 (Bramson 2011), so statements quantifying over it are not vacuous. Expectations are sums against π\piπ. Lemma 1 keeps its integrability hypothesis, and all other expectations are of bounded functions.
  • Parameters. λ=1−β/n\lambda = 1 - \beta/\sqrt nλ=1−β/n​ with 0<β<n0 < \beta < \sqrt n0<β<n​, so that λ>0\lambda > 0λ>0; λ\lambdaλ is free in Lemmas 1–2. Constants are quantified as ∃C\exists C∃C after β\betaβ and before nnn.
  • Misprint. The printed Theorem 2 omits E\mathbb EE. Read as an almost-sure bound it is false, so the expectation version, which the paper proves, is the target.
  • Derivatives. Points of Ω\OmegaΩ are pairs in ℝ × ℝ. Partial derivatives are named functions asserted to be one-sided derivatives along coordinate lines (HasDerivWithinAt on Set.Iic 0 or Set.Ici 0). Weak second derivatives are a.e. derivatives of absolutely continuous functions, in integral form on compact intervals. A "solution" of the PDE whose derivatives are the junk values of a derivative operator is thereby excluded. The PDE needs genuine derivatives, and Lemma 7 is about the explicit f∗f^*f∗ of (4.14), not about an arbitrary function.
  • Fluid objects. ν∗,η∗\nu^*, \eta^*ν∗,η∗ are the components of the unique solution of (4.8). τ\tauτ is valued in WithTop ℝ, with ∞\infty∞ as ⊤, so a missing solution is never read as 000. f∗f^*f∗ is an if cascade, and Lemma 7 states the agreement of its branches. f∗f^*f∗ is defined by the closed form (4.14), not through the fluid model (4.1).
  • Not included. Lemma 9 (via the Lambert W function, which Mathlib lacks), the bootstrapping argument of App. A.4 (not a numbered result), Theorems 1 and 3, and Proposition 1.

Contributions of reusable infrastructure are welcome: the adjoint relation for countable-state chains with bounded rates, and FTC/Taylor lemmas for absolutely continuous first derivatives.

Selected references

  • A. Braverman, Steady-State Analysis of the Join-the-Shortest-Queue Model in the Halfin–Whitt Regime, Math. Oper. Res. 45(3), 2020; arXiv:1801.05121v2. https://arxiv.org/abs/1801.05121
  • P. Eschenfeldt, D. Gamarnik, Join the Shortest Queue with Many Servers. The Heavy Traffic Asymptotics, arXiv preprint, 2015. https://arxiv.org/abs/1502.00999
  • D. Mukherjee, S. C. Borst, J. S. H. van Leeuwaarden, P. A. Whiting, Universality of Load Balancing Schemes on the Diffusion Scale, J. Appl. Probab. 53, 1111–1124, 2016. https://projecteuclid.org/euclid.jap/1481132840
  • M. Bramson, Stability of Join the Shortest Queue Networks, Ann. Appl. Probab. 21, 1568–1625, 2011. https://doi.org/10.1214/10-AAP726
  • S. Halfin, W. Whitt, Heavy-Traffic Limits for Queues with Many Exponential Servers, Oper. Res. 29(3), 1981. https://doi.org/10.1287/opre.29.3.567
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Graph TheoryOperations ResearchProbability+1·Captain: mikedeng1

Graphon Mean Field Systems IV: Law of Large Numbers for Particle Systems on Percolated Not-So-Dense Graphs With nβₙ → ∞Research Paper

Motivation

Large networks are often modeled through a graphon, a measurable function that records how likely two labeled vertices are to interact. For interacting diffusions, this lets one ask whether a finite random network has a predictable population limit. Bayraktar, Chakraborty and Wu study that question for graphon weighted systems, including graphs obtained by independently retaining potential edges with a sparsity parameter βn\beta_nβn​. Their not-so-dense regime allows βn\beta_nβn​ to decrease, provided the typical interaction scale nβnn\beta_nnβn​ diverges. Theorem 4.1 is the paper's law of large numbers for this regime; its two conclusions distinguish convergence of the population's empirical law from mean-square closeness of each particle to a coupled graphon limit. Bayraktar, Chakraborty and Wu, 2023.

The authors present three main convergence results: continuity of the continuum graphon system in Section 2, a dense-system law of large numbers in Section 3, and the percolated-system law of large numbers in Section 4. Section 7 establishes the latter. The graphon and cut-metric framework used here follows the graph-limit treatment cited by the paper. Bayraktar, Chakraborty and Wu, 2023; Lovász, 2012.

Setting

Let I=[0,1]I=[0,1]I=[0,1]. A graphon is a symmetric measurable G:I2→[0,1]G:I^2\to[0,1]G:I2→[0,1]. The cut norm ∥W∥□\|W\|_\square∥W∥□​ measures the largest absolute integral of WWW over a measurable rectangle S×US\times US×U. A sequence of step graphons GnG_nGn​ approaches GGG when ∥Gn−G∥□→0\|G_n-G\|_\square\to0∥Gn​−G∥□​→0. The related operator norm ∥W∥∞→1\|W\|_{\infty\to1}∥W∥∞→1​ measures the effect of WWW on bounded measurable functions. Remark 2.1 says cut convergence implies convergence in this operator norm. Bayraktar, Chakraborty and Wu, 2023, Remark 2.1.

Fix a dimension d≥1d\ge1d≥1 and horizon T>0T>0T>0. A label u∈Iu\in Iu∈I has an initial state Xu(0)∈RdX_u(0)\in\mathbb R^dXu​(0)∈Rd and an independent ddd-dimensional Brownian motion BuB_uBu​. The initial states are independent of each other and of the Brownian motions. The limiting graphon particle XuX_uXu​ is a continuous path whose drift averages b(Xu(s),x)G(u,v)b(X_u(s),x)G(u,v)b(Xu​(s),x)G(u,v) against the time-sss laws of all labels vvv, and whose diffusion matrix is σ(Xu(s))\sigma(X_u(s))σ(Xu​(s)). The time-sss law at label vvv is μv,s=L(Xv(s))\mu_{v,s}=\mathcal L(X_v(s))μv,s​=L(Xv​(s)). The family of path laws μu=L(Xu)\mu_u=\mathcal L(X_u)μu​=L(Xu​) is measurable in uuu and has uniformly bounded second moments. Bayraktar, Chakraborty and Wu, 2023, (4.2).

For nnn particles, label iii means i/ni/ni/n, with 1≤i≤n1\le i\le n1≤i≤n. Each undirected edge weight ξijn=ξjin\xi^n_{ij}=\xi^n_{ji}ξijn​=ξjin​ is Bernoulli with mean βnGn(i/n,j/n)\beta_nG_n(i/n,j/n)βn​Gn​(i/n,j/n); diagonal weights are included. These edge variables are independent of the Brownian motions and initial states. The finite particle XinX_i^nXin​ uses the same initial state and Brownian motion as Xi/nX_{i/n}Xi/n​. Its drift is the sum of ξijnb(Xin,Xjn)\xi^n_{ij}b(X_i^n,X_j^n)ξijn​b(Xin​,Xjn​) divided by nβnn\beta_nnβn​; its diffusion is σ(Xin)\sigma(X_i^n)σ(Xin​). The coefficients bbb and σ\sigmaσ are bounded and Lipschitz, and σ(x)\sigma(x)σ(x) is invertible with uniformly bounded inverse. Initial laws have uniformly bounded second moments, 0<βn≤10<\beta_n\le10<βn​≤1, and nβn→∞n\beta_n\to\inftynβn​→∞. Bayraktar, Chakraborty and Wu, 2023, Conditions 4.1–4.2.

Formalization targets

Let Cd=C([0,T];Rd)\mathcal C_d=C([0,T];\mathbb R^d)Cd​=C([0,T];Rd), μn=n−1∑i=1nδXin\mu^n=n^{-1}\sum_{i=1}^{n}\delta_{X_i^n}μn=n−1∑i=1n​δXin​​, and μˉ=∫Iμu du\bar\mu=\int_I\mu_u\,duμˉ​=∫I​μu​du. The main target, Theorem 4.1, first asserts convergence in probability in the weak topology on P(Cd)\mathcal P(\mathcal C_d)P(Cd​):

μn→Pμˉ.\mu^n\xrightarrow{\mathbb P}\bar\mu.μnP​μˉ​.

This uses Condition 2.2(a): on each of finitely many intervals covering III, the initial law varies continuously in Wasserstein distance W2W_2W2​. If the graphon also satisfies Condition 2.2(b), its stated sectional continuity outside null sets, the theorem adds

1n∑i=1nE∥Xin−Xi/n∥∗,T2⟶0,∥x∥∗,T=sup⁡0≤s≤T∣xs∣.\frac1n\sum_{i=1}^{n}\mathbb E\|X_i^n-X_{i/n}\|_{*,T}^2\longrightarrow0, \qquad \|x\|_{*,T}=\sup_{0\le s\le T}|x_s|.n1​i=1∑n​E∥Xin​−Xi/n​∥∗,T2​⟶0,∥x∥∗,T​=0≤s≤Tsup​∣xs​∣.

The milestones record the paper's cut-to-operator observation, uniform coupling moments, the one-edge and two-edge estimates, the bound on the second interaction-error term, the quantitative coupling lemma, and the empirical law of large numbers for the independent limiting particles. The second displayed limit is conditional on 2.2(b); the first is not. Bayraktar, Chakraborty and Wu, 2023, Theorem 4.1.

Significance

The first conclusion identifies the population-level limit even when the sampled network has a decreasing edge-retention probability. It gives a deterministic law on path space, rather than only a limit at one time. The second conclusion is stronger: it compares each finite particle with the limiting particle built from the same initial state and Brownian motion, averaged over all labels. This comparison is available when the extra graphon continuity assumption holds. Bayraktar, Chakraborty and Wu, 2023, Theorem 4.1 and Remark 4.1.

The mathematical results were proved in the published paper. The present mission asks for machine-checked Lean proofs of its specified statements; the draft theorems themselves currently contain sorry. Reusable outputs would include the percolated-edge model, a path-law formulation of graphon diffusions, and estimates for random interactions that depend on the particle states they influence. The paper's proofs appear in Sections 5–7, with the sparse-system argument in Section 7. Bayraktar, Chakraborty and Wu, 2023.

Difficulty

The edge variables are independent of the driving noise, but a particle's state depends on its incident edges. Therefore an expression such as E[ξijn∣Xjn−Xj/n∣2]\mathbb E[\xi^n_{ij}|X_j^n-X_{j/n}|^2]E[ξijn​∣Xjn​−Xj/n​∣2] cannot be factored into the edge mean times the error moment. The same dependence affects pairs of edges in the squared interaction sum. Equations (7.10), (7.14), and (7.15) quantify the discrepancy. A second difficulty is that cut convergence controls integrals against fixed bounded tests, while the dynamics and their path laws supply tests that vary with the system. The paper's regularity conditions and quantitative estimates are needed to connect those forms of control. Bayraktar, Chakraborty and Wu, 2023, Sections 7.1–7.2.

Formalization scope

Lean represents III by Mathlib's unit interval, Rd\mathbb R^dRd by Fin d → ℝ, and continuous paths by maps from [0,T][0,T][0,T] into that vector space. The chosen vector and matrix norms are fixed sup-type norms; finite-dimensional norm equivalence preserves the limit statements and the estimates with existential constants. The horizon and dimension are explicitly positive. Particle index i : Fin n denotes the paper's (i+1)(i+1)(i+1)st particle, and empirical laws use positive sizes n+1n+1n+1 to avoid division by zero. Wasserstein distances use extended nonnegative reals, while nonnegative expectations use lower integrals.

The noise lives on one probability space. The continuum equation uses the natural filtration of its own initial state and Brownian motion. The finite equation uses the natural filtration of its edge array, sampled initial states, and Brownian motions. A solution carries a measurable continuous-path law family in the paper's class M\mathcal MM; this prevents a nonmeasurable pushforward or a default-zero integral from silently satisfying an equation. Edge symmetry, Bernoulli marginals, independence, and diagonal self-loops are explicit. The zero-coefficient system has a separate sorry-free Lean witness for both solution predicates, ruling out a vacuous solution concept.

The formalization uses the published Peng1990.SMP.Stochastic Itô interface and WassersteinDRO.Duality.wassersteinDistance definition. Contributions can prove the listed estimates, strengthen their reusable stochastic and measure-theoretic infrastructure, or connect this mission's local setting to the other graphon missions after their definitions are published. The auxiliary changed-measure particles of Section 7.1 are outside the initial milestone list. Bayraktar, Chakraborty and Wu, 2023, Sections 4 and 7.

Selected references

  • E. Bayraktar, S. Chakraborty and R. Wu, Graphon mean field systems, Annals of Applied Probability 33(5):3587–3619, 2023. DOI.
  • L. Lovász, Large Networks and Graph Limits, American Mathematical Society Colloquium Publications 60, 2012. DOI.
13 thms1 active userReviewed
CombinatoricsGraph TheoryTheoretical Computer Science·Captain: mikedeng1

A c^k n 5-Approximation Algorithm for Treewidth 2: X Is a Balanced S-Separator iff V(G)∖X Splits into Three Mutually Non-Adjacent Parts Each Holding at Most |S|/2 Vertices of SResearch Paper

Motivation

The paper of Bodlaender, Drange, Dregi, Fomin, Lokshtanov and Pilipczuk (2016) has an algorithmic headline. This mission concerns one of its finite graph lemmas, Lemma 2.9. The lemma translates a condition phrased separately for every connected component into a condition on three vertex sets. A reader of graph decompositions encounters both forms: components express what remains connected after deleting vertices, while a small fixed number of parts gives a compact way to state constraints on a partition. Lemma 2.9 identifies exactly when the two forms agree for the half-balance threshold. The same result appears again in the paper as Lemma 6.2, where the authors use it in a later section.

The result does not require a tree decomposition or a treewidth hypothesis. It holds for every finite graph. That generality makes it a useful standalone target: the definitions of deletion, connected components, and the weighted three-partition can be reused wherever graph separators are studied. The mission follows the published SIAM article, with printed page 328 for the main lemma and pages 363–364 for its restatement and the supporting combinatorial observation.

Setting

Let GGG be a finite simple graph with vertex set V(G)V(G)V(G). Let SSS and XXX be subsets of its vertices. The deleted graph G∖XG\setminus XG∖X retains precisely the vertices outside XXX and the edges joining them. Two remaining vertices are in the same connected component when a walk joins them without passing through any vertex of XXX. Write CX(u)C_X(u)CX​(u) for the vertex set of the component containing u∉Xu\notin Xu∈/X. This interpretation follows the paper's notation on page 320.

A balanced SSS-separator is a set XXX for which each component of G∖XG\setminus XG∖X contains at most half the vertices of SSS:

∣CX(u)∩S∣≤∣S∣2for every u∈V(G)∖X.|C_X(u)\cap S|\le\frac{|S|}{2}\qquad\text{for every }u\in V(G)\setminus X.∣CX​(u)∩S∣≤2∣S∣​for every u∈V(G)∖X.

The paper introduces this phrase on page 321. Here balance is a property of XXX relative to SSS; it imposes no bound on the size of XXX. The denominator counts all vertices of SSS, including any that lie in XXX.

A three-part partition of V(G)∖XV(G)\setminus XV(G)∖X is a triple (M1,M2,M3)(M_1,M_2,M_3)(M1​,M2​,M3​) of pairwise disjoint sets whose union is V(G)∖XV(G)\setminus XV(G)∖X. A part may be empty. Two parts have no edge between them if no edge of GGG joins a vertex of one to a vertex of the other. Since the graph is undirected, checking the three unordered pairs of distinct parts covers the requirement for every i≠ji\ne ji=j.

Formalization targets

Lemma 2.9: balanced separators and three parts

The goal is the equivalence stated on page 328, also restated as Lemma 6.2 on page 363:

X is a balanced S-separator⟺V(G)∖X=M1∪˙M2∪˙M3,no edge joins distinct Mi,∣Mi∩S∣≤∣S∣/2(i=1,2,3).X\text{ is a balanced }S\text{-separator} \quad\Longleftrightarrow\quad \begin{gathered} V(G)\setminus X=M_1\mathbin{\dot\cup}M_2\mathbin{\dot\cup}M_3,\\ \text{no edge joins distinct }M_i,\\ |M_i\cap S|\le |S|/2\quad(i=1,2,3). \end{gathered}X is a balanced S-separator⟺V(G)∖X=M1​∪˙M2​∪˙M3​,no edge joins distinct Mi​,∣Mi​∩S∣≤∣S∣/2(i=1,2,3).​

The equivalence is the target, including both directions. It applies even when SSS or V(G)∖XV(G)\setminus XV(G)∖X is empty. It does not include a bound on ∣X∣|X|∣X∣.

Lemma 6.3: three bounded sums

The main supporting result on page 363 says that nonnegative integers a1,…,apa_1,\ldots,a_pa1​,…,ap​ with total qqq and ai≤q/2a_i\le q/2ai​≤q/2 can be divided into three classes, each with sum at most q/2q/2q/2. The milestone list also records the paper's merge inequality and its assertion that a component cannot cross between parts having no edge between them. These are the specific claims used in the published discussion of Lemma 2.9.

Significance

Lemma 2.9 lets a componentwise balance condition be represented by three sets whose coverage, disjointness, edge separation, and cardinalities can be inspected directly. It gives an exact equivalence, so the three-part formulation loses no balanced separators and introduces none that fail the original definition. That is the mathematical content needed when a later argument represents a separator by a bounded number of regions rather than by a list of all its components. The result is already proved in the 2016 paper; the open work in this mission is a machine-checked formalization of that known result and its cited supporting claims.

Formalizing the equivalence also establishes reusable interfaces for vertex deletion and component membership in a finite simple graph. A future development can state a separator condition using IsBalancedSSep, or use the three-part conclusion without redefining what a component of G∖XG\setminus XG∖X means. The independent integer-partition lemma has uses whenever indivisible nonnegative weights, each no larger than half the total, must be grouped into three bounded classes. Nothing in that statement depends on graphs.

Difficulty

There may be arbitrarily many components of G∖XG\setminus XG∖X, although the conclusion permits only three parts. Simply assigning all components to one part can violate the half bound, while splitting a component between different parts may create forbidden edges. A component's weight is the number of its vertices in SSS, and those weights can be uneven or zero. The theorem has to accommodate all such patterns without changing the threshold ∣S∣/2|S|/2∣S∣/2. In the converse direction, the absence of edges between the three parts must control entire walks, not only their first edge; ordinary connectivity in GGG would allow a walk through XXX and would describe the wrong components.

Formalization scope

The Lean development uses SimpleGraph V with V : Type, [Fintype V], and [DecidableEq V]. Vertex sets are Finset V. The shared walk-based AvoidReach G X u v requires every vertex on a walk to lie outside XXX, including both endpoints; avoidComp G X u collects the vertices reachable in this way. It is used only for u∉Xu\notin Xu∈/X when quantifying over components. This shared definition matches the paper's G∖XG\setminus XG∖X. The graph itself need not have decidable adjacency, since the statements concern propositions rather than computations.

Half bounds are written as 2c≤∣S∣2c\le |S|2c≤∣S∣ or 2c≤q2c\le q2c≤q in natural-number arithmetic. This is equivalent to the paper's rational half bound and avoids any interpretation of natural-number division. The three parts may be empty, so X=V(G)X=V(G)X=V(G) is a genuine boundary case. The set SSS may meet XXX; the right-hand denominator remains ∣S∣|S|∣S∣. The graph may have no vertices. There is no treewidth parameter or size condition on XXX: adding one would change Lemma 2.9 and can make its reverse implication false. Nor may components be computed using connectivity in the original graph, where paths through deleted vertices could merge them.

The required infrastructure is finite graph walks, finite sets, cardinalities, sums over finite index types, and the three original claims in the milestone list. The graph-component definitions and the integer grouping theorem are reusable beyond this mission. Contributions that prove any milestone or the full equivalence under exactly these conventions are in scope.

Selected references

  • H. L. Bodlaender, P. G. Drange, M. S. Dregi, F. V. Fomin, D. Lokshtanov and M. Pilipczuk, A c^k n 5-approximation algorithm for treewidth, SIAM Journal on Computing 45(2):317–378, 2016. DOI: 10.1137/130947374.
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CombinatoricsGraph TheoryTheoretical Computer Science·Captain: mikedeng1

Twin-width I: Tractable FO Model Checking 3: Grid Minor Theorem for Twin-width — t-Twin-Ordered Matrices Are (2t+2)-Mixed Free, and t-Mixed Free Matrices Have Twin-width at Most 4c_t·α^(4c_t+2)Research Paper

Motivation

Twin-width is a graph and matrix invariant introduced by Bonnet, Kim, Thomassé and Watrigant (J. ACM 69(1), Article 3, 2021). Classes of bounded twin-width include bounded tree-width and clique-width graphs, proper minor-closed classes, posets of bounded width, and permutations avoiding a fixed pattern; on all of them, first-order model checking is fixed-parameter tractable once a contraction sequence is given. The difficulty in applying this framework is to bound twin-width for a concrete class, because a contraction sequence is an intricate object.

Section 5 of the paper supplies the tool that makes such bounds routine: the Grid Minor Theorem for twin-width (Theorem 5.4). It reduces bounding twin-width to finding an order of the rows and columns of a matrix (for a graph, an order of its vertices) in which no large mixed minor appears. The paper then uses it for pattern-avoiding permutations, posets of bounded width and KtK_tKt​-minor free graphs (Section 6, Table 1). The argument is modelled on the proof of the Stanley–Wilf conjecture by Marcus and Tardos (JCTA 107, 2004) and on its use by Guillemot and Marx for permutation pattern matching (SODA 2014).

Timeline. Füredi and Hajnal (1992) conjectured a linear bound on the number of 111s in a 0,10,10,1-matrix avoiding a permutation pattern. Marcus and Tardos (2004) proved it, with constant ct=2t4(t2t)c_t=2t^4\binom{t^2}{t}ct​=2t4(tt2​), via ttt-grid minors. Fox (arXiv:1310.8378) improved the constant to 3t 28t3t\,2^{8t}3t28t, and Cibulka and Kynčl (arXiv:1607.07491) to 83(t+1)224t\tfrac83(t+1)^22^{4t}38​(t+1)224t. Guillemot and Marx (2014) built from the grid structure a decomposition of permutations; Bonnet et al. (2020 preprint, 2021 journal) generalized it to arbitrary matrices over a finite alphabet, which is Theorem 5.4.

Setting

Let M=(mi,j)M=(m_{i,j})M=(mi,j​) be an n×mn\times mn×m matrix with entries in a finite alphabet AAA of size α\alphaα. For sets RRR of rows and CCC of columns, the zone R∩CR\cap CR∩C is the submatrix on those rows and columns; it is constant if all its entries are equal.

A partition of MMM is a pair (R,C)(\mathcal R,\mathcal C)(R,C) of a partition of the rows and a partition of the columns. Its error value is the largest number, over all parts RiR_iRi​ (respectively CjC_jCj​), of parts of the other side forming a non-constant zone with it. A contraction sequence is a sequence of partitions starting from the finest one (all singletons), ending at the coarsest one (one row part, one column part), each obtained from the previous by merging two row parts or two column parts. MMM has twin-width at most ttt, tww⁡(M)≤t\operatorname{tww}(M)\le ttww(M)≤t, if some contraction sequence has error value at most ttt throughout.

A division is a partition whose parts consist of consecutive indices. MMM is ttt-twin-ordered if it has a contraction sequence of error value at most ttt consisting of divisions.

A zone is vertical if its rows are all equal, horizontal if its columns are all equal, and mixed otherwise. A ttt-mixed minor is a division into ttt row intervals and ttt column intervals all of whose t2t^2t2 zones are mixed; MMM is ttt-mixed free if it has none. For 0,10,10,1-matrices, a ttt-grid minor is such a division in which every zone contains a 111. Finally ct=83(t+1)224tc_t=\tfrac83(t+1)^22^{4t}ct​=38​(t+1)224t.

Formalization targets

Goal: Theorem 5.4

For n,m≥1n,m\ge1n,m≥1:

$$M\ \text{ttt-twin-ordered}\ \Longrightarrow\ M\ \text{(2t+2)(2t+2)(2t+2)-mixed free},

t\ge1,\ M\ \text{ttt-mixed free}\ \Longrightarrow\ \operatorname{tww}(M)\le 4c_t,\alpha^{4c_t+2}.$$

The constant is the one the paper's proof produces; the paper's summary 22O(t)2^{2^{O(t)}}22O(t) is not formalized.

Milestones, in the order of the proof

  1. Lemma 5.5: a matrix is mixed iff it contains a corner, a mixed 2×22\times22×2 submatrix on consecutive rows and columns.
  2. Lemma 5.6: fusing two consecutive row parts does not increase the mixed value of a column interval (mixed zones plus mixed cuts).
  3. Lemma 5.2: a sequence of partitions, each rrr-refining the next, with error value at most ttt, certifies tww⁡(M)≤rt\operatorname{tww}(M)\le rttww(M)≤rt.
  4. Theorem 5.3 (Marcus–Tardos, constant of Cibulka–Kynčl): ctmax⁡(n,m)c_t\max(n,m)ct​max(n,m) entries 111 force a ttt-grid minor.
  5. Lemma 5.7: a ttt-mixed free matrix has a division sequence of mixed value at most 2ct2c_t2ct​.
  6. The first item of Theorem 5.4.
  7. The row-type count on p. 3:22: within a row part, rows restricted to the non-mixed zones take at most αt′+1\alpha^{t'+1}αt′+1 values.

Significance

Theorem 5.4 characterizes bounded twin-width of matrices, up to the order of rows and columns, by the exclusion of a mixed minor. Its second item is used in Section 6 of the same paper to show that KtK_tKt​-minor free graphs, posets of bounded width and pattern-avoiding permutations have bounded twin-width, and in later papers of the twin-width series as the standard route to twin-width upper bounds. Without it, each such bound needs its own explicit contraction sequence.

The result is proved in the paper; no machine-checked proof of it exists in Mathlib or on the platform. The mission produces a machine-checked statement and, once solved, a proof of the grid theorem with its explicit constant, a formal treatment of contraction sequences of matrices, and a statement of the Marcus–Tardos theorem with the Cibulka–Kynčl constant, which is itself absent from Mathlib.

Difficulty

The first item is comparatively short. The second item is where the work lies. The natural first idea — contract greedily as long as the error value stays below a bound depending on ttt — does not work: the error value is not monotone under fusions, and nothing in the absence of a mixed minor directly prevents a greedy sequence from getting stuck with large error. Any proof has to identify a quantity that is monotone under fusion and is bounded by a density argument, and then turn a sequence controlled by that quantity into a contraction sequence of bounded error value; the paper's choices (mixed value, Lemmas 5.6 and 5.7) are the milestones. The density argument rests on the Marcus–Tardos theorem with an explicit single-exponential constant, a substantial combinatorial result in its own right and not available in Mathlib.

Formalization scope

Matrices are Matrix (Fin n) (Fin m) A with [Fintype A], and α\alphaα is Fintype.card A. Partitions are Mathlib Finpartitions of univ; the finest is ⊥, and "coarsest" means at most one part. Twin-width is the partition form of p. 3:18, as a predicate MatTwinWidthLE M t with exactly one merge, of rows or of columns, per step; it is never an infimum over a possibly empty set. Divisions in minors are given by strictly increasing cut points 0=r0<⋯<rt=n0=r_0<\dots<r_t=n0=r0​<⋯<rt​=n, so all parts are non-empty. Vertical and horizontal mean "all rows (columns) of the zone agree". Grid minors use Bool entries. Since ctc_tct​ is not an integer, α4ct+2\alpha^{4c_t+2}α4ct​+2 is a real power, and the bound is ⌊4ctα4ct+2⌋\lfloor 4c_t\alpha^{4c_t+2}\rfloor⌊4ct​α4ct​+2⌋; the mixed-value bound of Lemma 5.7 is ⌊2ct⌋\lfloor 2c_t\rfloor⌊2ct​⌋.

Hypotheses added relative to the page: n,m≥1n,m\ge1n,m≥1 in Theorems 5.3, 5.4 and Lemma 5.7; t≥1t\ge1t≥1 in the second item of Theorem 5.4, in Theorem 5.3 and in Lemma 5.7, since for t=0t=0t=0 every non-empty matrix is vacuously 000-mixed free and the bound would be false; m≥1m\ge1m≥1 in the row-type count. Theorem 5.3 is stated with the explicit constant ctc_tct​ that the paper quotes and uses, not as a bare existence statement.

The statements are not trivializable by the usual routes: twin-width is not a junk infimum, a contraction sequence cannot jump to one part in a single step, the error value counts non-constant zones per part on both sides, minors range over divisions with non-empty interval parts rather than arbitrary partitions, and all bounds depend only on ttt and α\alphaα, never on MMM.

A complete development needs: finite partitions and their merges, divisions as interval partitions, the Marcus–Tardos theorem, and bookkeeping for sequences of partitions. The partition machinery and Theorem 5.3 are reusable beyond this mission (graph twin-width in the other missions of this series, pattern avoidance). Proofs of individual milestones, and of the Marcus–Tardos theorem from its original argument, are welcome.

Selected references

  • É. Bonnet, E. J. Kim, S. Thomassé, R. Watrigant, Twin-width I: Tractable FO Model Checking, J. ACM 69(1), Article 3, 2021. https://doi.org/10.1145/3486655
  • A. Marcus, G. Tardos, Excluded permutation matrices and the Stanley–Wilf conjecture, J. Combin. Theory Ser. A 107(1), 153–160, 2004. https://doi.org/10.1016/j.jcta.2004.04.002
  • J. Fox, Stanley–Wilf limits are typically exponential, arXiv:1310.8378, 2013. https://arxiv.org/abs/1310.8378
  • J. Cibulka, J. Kynčl, Füredi–Hajnal limits are typically subexponential, arXiv:1607.07491, 2016. https://arxiv.org/abs/1607.07491
  • S. Guillemot, D. Marx, Finding small patterns in permutations in linear time, SODA 2014, 82–101. https://doi.org/10.1137/1.9781611973402.7
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Operations ResearchOptimization·Captain: mikedeng1

Scheduling Problems with Two Competing Agents 3: The Least-Cost Backward Rule Gives a Nondominated Schedule Minimizing Total Completion Time Under a Maximum-Cost BoundResearch Paper

Motivation

Many scheduling situations involve more than one decision maker sharing a resource. Two departments of a firm may share a machine shop, two clients may share a contractor, or two users may share a processor, and each cares only about how its own jobs are served. Agnetis, Mirchandani, Pacciarelli and Pacifici (Oper. Res. 52(2), 2004) introduced a systematic study of such two-agent scheduling problems. Their framework has two questions. The constrained problem asks for the best schedule for one agent among those that keep the other agent's cost below a bound. The Pareto problem asks for the schedules whose cost pair cannot be improved for one agent without hurting the other. The paper settles the complexity of these questions for the standard scheduling objectives and gave rise to a large literature on multi-agent scheduling (see the survey by Perez-Gonzalez and Framinan, EJOR 235, 2014).

This mission covers §5.2 of the paper: agent AAA minimizes the total completion time of its jobs, and agent BBB requires that the maximum of its jobs' regular costs stay below a bound QQQ.

Setting

Agent AAA owns jobs J1A,…,JnAAJ^A_1,\dots,J^A_{n_A}J1A​,…,JnA​A​ and agent BBB owns jobs J1B,…,JnBBJ^B_1,\dots,J^B_{n_B}J1B​,…,JnB​B​. Job JjJ_jJj​ has a processing time pj>0p_j>0pj​>0. All jobs are available at time 000 and are processed one at a time, without interruption, on a single machine. Because every objective here is nondecreasing in the completion times, the machine is never left idle, and a schedule σ\sigmaσ is simply a sequence of all nA+nBn_A+n_BnA​+nB​ jobs; the completion time Cj(σ)C_j(\sigma)Cj​(σ) of a job is the total processing time of that job and the jobs before it. Write PAP_APA​ and PBP_BPB​ for the total processing times of the two agents.

Agent AAA's objective is the total completion time ∑hChA(σ)\sum_h C^A_h(\sigma)∑h​ChA​(σ). Each BBB-job has a nondecreasing cost function fkBf^B_kfkB​, and agent BBB's objective is the maximum cost

fmax⁡B(σ)=max⁡kfkB(CkB(σ)).f^B_{\max}(\sigma)=\max_k f^B_k\bigl(C^B_k(\sigma)\bigr).fmaxB​(σ)=kmax​fkB​(CkB​(σ)).

Given a bound QQQ, a schedule is feasible for the problem 1∥∑CiA:fmax⁡B≤Q1\|\sum C^A_i : f^B_{\max}\le Q1∥∑CiA​:fmaxB​≤Q if fkB(CkB)≤Qf^B_k(C^B_k)\le QfkB​(CkB​)≤Q for every BBB-job, and optimal if it is feasible and minimizes ∑ChA\sum C^A_h∑ChA​ among feasible schedules. The instance is feasible if a feasible schedule exists. A schedule is nondominated if no schedule is at least as good for both agents and strictly better for one.

The paper solves the problem with a backward rule (Figure 1). Fill the sequence from the end. With τ\tauτ the total length of the jobs not yet placed, place last any unplaced BBB-job with fkB(τ)≤Qf^B_k(\tau)\le QfkB​(τ)≤Q. If there is none, place last a longest unplaced AAA-job. If neither exists, the instance is infeasible. The least-cost variant of §5.2.1 chooses, among the BBB-jobs, one minimizing fkB(τ)f^B_k(\tau)fkB​(τ) over all unplaced BBB-jobs. A B-block of a schedule is a maximal run of consecutive BBB-jobs.

Formalization targets

Goal: Theorem 5.7

On a feasible instance with nB≥1n_B\ge1nB​≥1, every schedule σ~\tilde\sigmaσ~ produced by the least-cost variant, under any tie-breaking, satisfies

σ~ is optimal for 1∥∑CiA:fmax⁡B≤Qandσ~ is nondominated for (∑CiA, fmax⁡B).\tilde\sigma \text{ is optimal for } 1\|\textstyle\sum C^A_i : f^B_{\max}\le Q \quad\text{and}\quad \tilde\sigma \text{ is nondominated for } \bigl(\textstyle\sum C^A_i,\ f^B_{\max}\bigr).σ~ is optimal for 1∥∑CiA​:fmaxB​≤Qandσ~ is nondominated for (∑CiA​, fmaxB​).

The nondominance is the printed theorem; the optimality is how the paper introduces σ~\tilde\sigmaσ~, and rests on Theorem 5.5.

Milestones

  • Lemma 5.3: if some BBB-job JkˉBJ^B_{\bar k}JkˉB​ has fkˉB(PA+PB)≤Qf^B_{\bar k}(P_A+P_B)\le QfkˉB​(PA​+PB​)≤Q, some optimal schedule ends with JkˉBJ^B_{\bar k}JkˉB​ and no optimal schedule ends with an AAA-job.
  • Lemma 5.4: if every BBB-job has fkB(PA+PB)>Qf^B_k(P_A+P_B)>QfkB​(PA​+PB​)>Q, every optimal schedule ends with a longest AAA-job.
  • Theorem 5.5 (correctness): on a feasible instance every schedule of Figure 1 is optimal, and Figure 1 runs to completion exactly on feasible instances.
  • Lemma 5.6: all optimal schedules have the same partition of the BBB-jobs into B-blocks, and each B-block occupies the same time interval in all of them.

Significance

Theorem 5.5 shows that the constrained problem with total completion time against a maximum cost is solvable by sorting, in contrast to its weighted version, which the same section shows NP-hard. Lemma 5.6 describes all optimal schedules: they agree on the completion times of the AAA-jobs (up to permuting identical jobs) and on the B-blocks, and differ only inside each block. Theorem 5.7 turns this into a nondominated schedule. It is the building block for the Pareto problem 1∥∑CiA∘fmax⁡B1\|\sum C^A_i\circ f^B_{\max}1∥∑CiA​∘fmaxB​ of §11.2, where solving the constrained problem for a sequence of bounds enumerates the nondominated pairs.

The results are proved in the paper; none of them has a machine-checked proof that we know of. The mission formalizes the statements and asks for their proofs. The proof of Theorem 5.7 invokes "the very same proof of Lawler's algorithm (Lawler 1973) restricted to 1∥fmax⁡1\|f_{\max}1∥fmax​", applied inside each B-block. Lawler's rule is a separate statement on the platform, LawlerPrec.MinMax.lawler_rule_optimal, currently open. A solver may prove it and adapt it, but the goal does not need it in that exact form.

Difficulty

The interchange arguments of Lemmas 5.3 and 5.4 are short. The obstacle is Lemma 5.6. Two optimal schedules can differ in which BBB-job is placed at each step, and in the order of AAA-jobs of equal length. The paper's argument compares the completion time of each AAA-job across two optimal schedules and shows it cannot move earlier. That needs the fact that a BBB-job finishing before an AAA-job could not have been placed at that AAA-job's completion time, which comes from applying Lemma 5.3 to a prefix of the schedule. Formalizing it requires restricting optimality to prefixes and sub-instances, which the bare sequence model does not provide. The tempting shortcut of proving Theorem 5.7 from Lawler's rule on the whole schedule fails, since the bound QQQ and agent AAA's objective change which jobs may be placed where; the reduction is only to one Lawler instance per block.

Formalization scope

Jobs are Fin nA ⊕ Fin nB (0-based). A schedule is a duplicate-free list of all jobs, with completion times from the published sequence model MooreLateJobs.Shared.completionTime (Moore 1968 series), which this mission reuses. Processing times are real and strictly positive. Without positivity the second claim of Lemma 5.3 fails, because a zero-length BBB-job can sit anywhere. Cost functions are real-valued and nondecreasing, and QQQ is real (the paper's integer QQQ is a special case). Feasibility is stated job by job; fmax⁡Bf^B_{\max}fmaxB​ is a finite maximum and requires nB≥1n_B\ge1nB​≥1, which the goal assumes. Lemma 5.4 assumes nA≥1n_A\ge1nA​≥1, since "a longest AAA-job" presupposes one.

The paper's loose phrases are read as follows:

  • "the algorithm" is a property of a finished sequence. At position mmm, with the jobs at positions 0,…,m0,\dots,m0,…,m unplaced and τ\tauτ their total length, the job at mmm must be a choice the rule allows.
  • "Ties are broken arbitrarily" means that every sequence satisfying the rule is covered.
  • "no solution exists, STOP" leaves no allowed choice. Running to completion therefore means that some sequence satisfies the rule.
  • "the optimal schedule generated in this way" puts optimality into the goal as a conclusion, not a hypothesis.
  • "a longest A-job" is an AAA-job of maximal length; when several are tied, no statement fixes which one.
  • Nondominance quantifies over all schedules, not only those feasible for QQQ.
  • A B-block's interval runs from the earliest start to the latest completion of its jobs.

The running times of Theorems 5.5 and 5.8 (O(nAlog⁡nA+nBlog⁡nB)O(n_A\log n_A+n_B\log n_B)O(nA​lognA​+nB​lognB​) and O(nAlog⁡nA+nB2)O(n_A\log n_A+n_B^2)O(nA​lognA​+nB2​)) are not formalized. Nor is the claim (3) inside the proof of Lemma 5.6.

A trivializing formalization is ruled out: feasibility of the instance is a hypothesis and not built into the rule, the rule constrains every position, and the goal asserts nondominance against all schedules.

Useful infrastructure includes interchange lemmas for the sequence model (moving one job to the end, swapping two jobs), restriction of a schedule to a prefix, and Lawler's rule for 1∥fmax⁡1\|f_{\max}1∥fmax​ on a fixed time window. The interchange lemmas and the prefix restriction are reusable across the whole two-agent series.

Selected references

  • A. Agnetis, P. B. Mirchandani, D. Pacciarelli, A. Pacifici, Scheduling Problems with Two Competing Agents, Operations Research 52(2), 229–242, 2004. https://doi.org/10.1287/opre.1030.0092
  • E. L. Lawler, Optimal Sequencing of a Single Machine Subject to Precedence Constraints, Management Science 19(5), 544–546, 1973. https://doi.org/10.1287/mnsc.19.5.544
  • J. M. Moore, An n Job, One Machine Sequencing Algorithm for Minimizing the Number of Late Jobs, Management Science 15(1), 102–109, 1968. https://doi.org/10.1287/mnsc.15.1.102
  • R. L. Graham, E. L. Lawler, J. K. Lenstra, A. H. G. Rinnooy Kan, Optimization and Approximation in Deterministic Sequencing and Scheduling: A Survey, Annals of Discrete Mathematics 5, 287–326, 1979. https://doi.org/10.1016/S0167-5060(08)70356-X
  • P. Perez-Gonzalez, J. M. Framinan, A common framework and taxonomy for multicriteria scheduling problems with interfering and competing jobs: Multi-agent scheduling problems, European Journal of Operational Research 235(1), 1–16, 2014. https://doi.org/10.1016/j.ejor.2013.09.017
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Machine LearningNumerical AnalysisOptimization·Captain: mikedeng1

Conservative Set Valued Fields, Automatic Differentiation, Stochastic Gradient Methods and Deep Learning 2: Forward and Reverse Mode Automatic Differentiation Yield Conservative FieldsResearch Paper

Motivation

Training a neural network means running a first-order method on a loss that is built from compositions of elementary operations, many of them nonsmooth: ReLU, max-pooling, absolute values, sorting, norms. The gradient the optimizer uses is not computed by hand. It is computed by automatic differentiation (autodiff), most often in its reverse mode, backpropagation, which applies the chain rule of calculus operation by operation. When every operation is smooth, the output is the gradient. When some are not, each nonsmooth operation is assigned some "derivative" at its kinks (for ReLU at 000, typically 000), and the chain rule is applied anyway. The result is in general neither a gradient, nor a Clarke subgradient, nor an element of any classical subdifferential: the classical subdifferentials do not satisfy the chain rule that autodiff applies.

Bolte and Pauwels (TSE Working Paper 1044, 2019; Mathematical Programming, 2021) introduced conservative set-valued fields to give these outputs a meaning. A conservative field is a set-valued map whose circulation along every closed path vanishes, exactly as for a gradient field. It obeys a chain rule along absolutely continuous curves. This mission formalizes the paper's Theorem 8: forward-mode and reverse-mode automatic differentiation, run with conservative fields for the elementary operations, return a conservative field for the composed function. The companion mission of this series formalizes the paper's Theorem 1, that a conservative field equals the gradient of its potential almost everywhere.

Setting

Write Rn\mathbb R^nRn for Euclidean space and D:Rn⇉RnD:\mathbb R^n\rightrightarrows\mathbb R^nD:Rn⇉Rn for a set-valued map, assigning a subset D(x)⊆RnD(x)\subseteq\mathbb R^nD(x)⊆Rn to every point. A path γ:[0,1]→Rn\gamma:[0,1]\to\mathbb R^nγ:[0,1]→Rn is absolutely continuous, with derivative γ˙(t)\dot\gamma(t)γ˙​(t) for almost every ttt.

A conservative field (Definition 1) is a set-valued map DDD with closed graph and nonempty compact values such that for every absolutely continuous loop γ\gammaγ (γ(0)=γ(1)\gamma(0)=\gamma(1)γ(0)=γ(1)) the circulation t↦max⁡v∈D(γ(t))⟨γ˙(t),v⟩t\mapsto\max_{v\in D(\gamma(t))}\langle\dot\gamma(t),v\ranglet↦maxv∈D(γ(t))​⟨γ˙​(t),v⟩ is Lebesgue integrable with integral 000. A function f:Rn→Rf:\mathbb R^n\to\mathbb Rf:Rn→R is a potential for DDD, or DDD is a conservative field for fff (Definition 2), if DDD is conservative and f(x)=f(0)+∫01max⁡v∈D(γ(t))⟨γ˙(t),v⟩ dtf(x)=f(0)+\int_0^1\max_{v\in D(\gamma(t))}\langle\dot\gamma(t),v\rangle\,dtf(x)=f(0)+∫01​maxv∈D(γ(t))​⟨γ˙​(t),v⟩dt for every absolutely continuous path γ\gammaγ from 000 to xxx. A map JF:Rn⇉Rm×nJ_F:\mathbb R^n\rightrightarrows\mathbb R^{m\times n}JF​:Rn⇉Rm×n is a conservative mapping for F:Rn→RmF:\mathbb R^n\to\mathbb R^mF:Rn→Rm (Definition 4) if, along every absolutely continuous curve γ\gammaγ, for almost every ttt, ddtF(γ(t))=Vγ˙(t)\frac{d}{dt}F(\gamma(t))=V\dot\gamma(t)dtd​F(γ(t))=Vγ˙​(t) for all V∈JF(γ(t))V\in J_F(\gamma(t))V∈JF​(γ(t)).

An evaluation program (§5.1) has inputs x1,…,xpx_1,\dots,x_px1​,…,xp​ and intermediate nodes xp+1,…,xqx_{p+1},\dots,x_qxp+1​,…,xq​. Node kkk has a tuple parents(k)\mathtt{parents}(k)parents(k) of distinct earlier nodes and an elementary function gk:R∣parents(k)∣→Rg_k:\mathbb R^{|\mathtt{parents}(k)|}\to\mathbb Rgk​:R∣parents(k)∣→R. Algorithm 1 sets xk=gk(xparents(k))x_k=g_k(x_{\mathtt{parents}(k)})xk​=gk​(xparents(k)​) for k=p+1,…,qk=p+1,\dots,qk=p+1,…,q and returns f(x)=xqf(x)=x_qf(x)=xq​. Each gkg_kgk​ comes with a conservative field DkD_kDk​ (property (d)). Given a choice dk∈Dk(xparents(k))d_k\in D_k(x_{\mathtt{parents}(k)})dk​∈Dk​(xparents(k)​) for every kkk:

  • Algorithm 2 (forward mode) computes the rows ∂xk/∂x=∑j∈parents(k)(∂xj/∂x) dkj\partial x_k/\partial x=\sum_{j\in\mathtt{parents}(k)}(\partial x_j/\partial x)\,d_{kj}∂xk​/∂x=∑j∈parents(k)​(∂xj​/∂x)dkj​ and returns ∂xq/∂x1,…,p\partial x_q/\partial x_{1,\dots,p}∂xq​/∂x1,…,p​;
  • Algorithm 3 (reverse mode) starts from v=eq∈Rqv=e_q\in\mathbb R^qv=eq​∈Rq, sweeps t=q,…,p+1t=q,\dots,p+1t=q,…,p+1, adds v[t] dtjv[t]\,d_{tj}v[t]dtj​ to v[j]v[j]v[j] for each parent jjj of ttt, and returns (v[1],…,v[p])(v[1],\dots,v[p])(v[1],…,v[p]).

The autodiff fields are Dfwd(x)D_{\mathrm{fwd}}(x)Dfwd​(x) and Drev(x)D_{\mathrm{rev}}(x)Drev​(x), the sets of outputs of Algorithm 2 and Algorithm 3 over all choices at xxx.

Formalization targets

Goal: Theorem 8

If every DkD_kDk​ is a locally bounded conservative field for gkg_kgk​, then

Dfwd and Drev are conservative fields for f.D_{\mathrm{fwd}}\ \text{and}\ D_{\mathrm{rev}}\ \text{are conservative fields for } f .Dfwd​ and Drev​ are conservative fields for f.

"Conservative field for fff" is meant in full: closed graph, nonempty compact values, zero circulation and the potential identity.

Milestones, in the order of the paper's proof

  1. Lemma 2: for a locally bounded, graph-closed DDD with nonempty values and a locally Lipschitz fff, DDD is a conservative field for fff iff ddtf(x(t))=⟨v,x˙(t)⟩\frac{d}{dt}f(x(t))=\langle v,\dot x(t)\rangledtd​f(x(t))=⟨v,x˙(t)⟩ for all v∈D(x(t))v\in D(x(t))v∈D(x(t)), for almost every ttt, along every absolutely continuous curve xxx.
  2. Lemma 3: stacking conservative fields of the coordinates of FFF row by row gives a conservative mapping for FFF.
  3. (10): with Gk(x)=x+ek(gk(xparents(k))−xk)G_k(x)=x+e_k(g_k(x_{\mathtt{parents}(k)})-x_k)Gk​(x)=x+ek​(gk​(xparents(k)​)−xk​) on Rq\mathbb R^qRq, the map Lk(x)={I−ekekT+ekdT:d∈Dk(x)}L_k(x)=\{I-e_ke_k^T+e_kd^T : d\in D_k(x)\}Lk​(x)={I−ek​ekT​+ek​dT:d∈Dk​(x)} is a conservative mapping for GkG_kGk​.
  4. Lemma 5: x↦J2(F1(x)) J1(x)x\mapsto J_2(F_1(x))\,J_1(x)x↦J2​(F1​(x))J1​(x) is a conservative mapping for F2∘F1F_2\circ F_1F2​∘F1​.
  5. Mk=Jk×⋯×Jp+1×JpM_k=J_k\times\cdots\times J_{p+1}\times J_pMk​=Jk​×⋯×Jp+1​×Jp​: the matrix of forward-mode rows up to node kkk is the product of the matrices Jj=I−ejejT+ejdjTJ_j=I-e_je_j^T+e_jd_j^TJj​=I−ej​ejT​+ej​djT​.
  6. Lemma 4: each row of a conservative mapping satisfies the chain rule for the corresponding coordinate.
  7. Reverse mode equals forward mode: for every choice, Algorithm 3 returns the output of Algorithm 2.

Significance

Theorem 8 says what backpropagation computes on a nonsmooth program: an element of a conservative field of the function, a set that behaves like a gradient along curves. This is what lets the paper's later results apply to deep learning: stochastic subgradient methods driven by such outputs converge, for definable losses, to points that are critical for the conservative field. It is also the reason why spurious outputs of autodiff (a nonzero "derivative" of a function that is identically zero) are harmless: by the companion Theorem 1 they occur only on a Lebesgue null set.

The result is proved in the paper, and nothing here is open. To our knowledge none of it has been machine-checked: there is no formal account of conservative fields, and the existing formalizations of backpropagation treat smooth layered networks only. This mission produces a formal model of evaluation programs and of both autodiff modes, a formal chain-rule calculus for conservative mappings (Lemmas 2–5), and the theorem itself. Formalizing it exposed three points the printed text leaves to the reader: the overwriting update of Algorithm 3, the nonempty-values hypothesis missing from Lemma 2, and the local boundedness that Theorem 8 needs (see Formalization scope).

Difficulty

The obvious argument is "autodiff applies the chain rule, and conservative fields satisfy the chain rule". The chain rule along curves (Lemmas 3–5) only gives the derivative identity of Definition 4 for each element of Dfwd(x)D_{\mathrm{fwd}}(x)Dfwd​(x). It does not give the set-valued properties of Definition 1. Passing back to a conservative field (Lemma 2) needs DfwdD_{\mathrm{fwd}}Dfwd​ to have closed graph, nonempty compact values and local boundedness. These depend on how the sets Dk(xparents(k))D_k(x_{\mathrm{parents}(k)})Dk​(xparents(k)​) vary with xxx through the forward pass, and they fail without local boundedness of the DkD_kDk​. Lemma 2 relates an integral identity along every path to a pointwise almost-everywhere identity, and both directions involve the measure theory of absolutely continuous curves that Mathlib supports only in part. The equality of reverse and forward modes is linear algebra, but the two algorithms traverse the graph in opposite orders, and the printed reverse update is not the one the equality needs.

Formalization scope

Rn\mathbb R^nRn is EuclideanSpace ℝ (Fin n), and the conservative-field layer is polymorphic in the dimension: each gkg_kgk​ lives on R∣parents(k)∣\mathbb R^{|\mathtt{parents}(k)|}R∣parents(k)∣. A path is a function ℝ → ℝ^n that is AbsolutelyContinuousOnInterval on [0,1][0,1][0,1], with γ˙\dot\gammaγ˙​ = deriv γ. Definitions 1–2 require the circulation to be interval-integrable, because Lean integrates a non-integrable function to 000. Definition 4 and the chain rule (5) assert HasDerivAt, not an equation for deriv, so they cannot hold by default at points of non-differentiability. Nodes are Fin q, numbered from 000. Parent tuples are duplicate-free lists of smaller nodes, and input nodes have none.

Dfwd(x)D_{\mathrm{fwd}}(x)Dfwd​(x) and Drev(x)D_{\mathrm{rev}}(x)Drev​(x) range over all admissible choices. A single fixed choice would give a map that is not a conservative field in general, and the formal statement does not use one.

Deviations from the printed text, each recorded with its item:

  • Algorithm 3's update "v[j]:=v[t]dtjv[j]:=v[t]d_{tj}v[j]:=v[t]dtj​" is implemented as v[j]:=v[j]+v[t]dtjv[j]:=v[j]+v[t]d_{tj}v[j]:=v[j]+v[t]dtj​, which is what the proof computes. The printed overwrite makes Theorem 8(ii) false whenever a node has two children.
  • Lemma 2 gets the hypothesis that DDD has nonempty values, without which its "if" direction fails for D≡∅D\equiv\emptysetD≡∅.
  • Theorem 8 gets the hypothesis that every DkD_kDk​ is locally bounded. The paper takes it from a citation in Remark 3(d), but a conservative field need not be locally bounded, and without it DfwdD_{\mathrm{fwd}}Dfwd​ can fail to have closed graph.
  • Lemma 4's "conservative field" is read in the chain-rule sense (5), since a conservative mapping need not have closed graph or nonempty values.
  • Lemma 5's domain of J2J_2J2​ is read as Rm\mathbb R^mRm.

Theorem numbers and pages are those of the TSE Working Paper 1044 (October 2019), the version this mission cites. The journal version is typeset differently.

The conservative-field definitions duplicate those of the companion mission and are meant to be merged with them. Contributions are welcome at every level: Lemma 2 and Lemmas 3–5 form a reusable nonsmooth chain-rule calculus, and the reverse-equals-forward identity is a standalone statement about backpropagation that holds for arbitrary weights.

Selected references

  • J. Bolte, E. Pauwels, Conservative set valued fields, automatic differentiation, stochastic gradient methods and deep learning, TSE Working Paper 1044, October 2019. https://publications.ut-capitole.fr/id/eprint/42324/1/wp_tse_1044.pdf
  • J. Bolte, E. Pauwels, Conservative set valued fields, automatic differentiation, stochastic gradient methods and deep learning, Mathematical Programming 188 (2021), 19–51. https://doi.org/10.1007/s10107-020-01501-5
  • A. Griewank, A. Walther, Evaluating Derivatives: Principles and Techniques of Algorithmic Differentiation, 2nd ed., SIAM, 2008. https://doi.org/10.1137/1.9780898717761
  • D. Davis, D. Drusvyatskiy, S. Kakade, J. D. Lee, Stochastic subgradient method converges on tame functions, Foundations of Computational Mathematics 20 (2020), 119–154. https://doi.org/10.1007/s10208-018-09409-5
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Adaptive Cubic Regularisation Methods for Unconstrained Optimization. Part II: Worst-Case Function- and Derivative-Evaluation Complexity 3: ARC(S) Reaches −λ_min(QᵀBQ) ≤ ε in O(ε^(−3)) IterationsResearch Paper

Second-order worst-case complexity of cubic regularisation

Unconstrained minimization of a smooth nonconvex function f:Rn→Rf:\mathbb R^n\to\mathbb Rf:Rn→R is the core subproblem of most nonlinear optimization software. Methods that only drive the gradient to zero may stall at saddle points, so a second-order guarantee (approximately nonnegative curvature) is the natural target for nonconvex problems. Worst-case evaluation complexity, meaning the number of function and derivative evaluations needed to reach a prescribed accuracy, is the standard way to compare such methods.

Timeline:

  • 1981. Griewank, in an unpublished report, proposed globally minimizing a cubic regularisation of the second-order Taylor model to obtain an affine-invariant Newton method converging to second-order critical points.
  • 2006. Nesterov and Polyak (Math. Program. 108) proved that, when the Hessian is globally Lipschitz and the step is the exact global minimizer of the cubic model with the exact Hessian, their method reaches approximate first-order criticality in O(ϵ−3/2)O(\epsilon^{-3/2})O(ϵ−3/2) iterations and approximate second-order criticality in O(ϵ−3)O(\epsilon^{-3})O(ϵ−3).
  • 2009–2011. Cartis, Gould and Toint introduced the Adaptive Regularisation with Cubics (ARC) framework (Part I, Math. Program. 127). It uses an adaptive weight, an approximate Hessian and inexact subspace minimization. In Part II (Math. Program. 130) they proved that its second-order variant ARC(S) matches the Nesterov–Polyak orders under these weaker requirements.

This mission formalizes the second-order bound of Part II, Corollary 5.4.

Setting

Write g(x)=∇f(x)g(x)=\nabla f(x)g(x)=∇f(x) and H(x)=∇2f(x)H(x)=\nabla^2 f(x)H(x)=∇2f(x), and let ∥⋅∥\|\cdot\|∥⋅∥ be the Euclidean norm. At iterate xkx_kxk​, given a symmetric operator BkB_kBk​ (an approximation of H(xk)H(x_k)H(xk​)) and a weight σk>0\sigma_k>0σk​>0, the cubic model is

mk(s)=f(xk)+s⊤gk+12s⊤Bks+13σk∥s∥3.m_k(s)=f(x_k)+s^\top g_k+\tfrac12 s^\top B_ks+\tfrac13\sigma_k\|s\|^3 .mk​(s)=f(xk​)+s⊤gk​+21​s⊤Bk​s+31​σk​∥s∥3.

Algorithm ARC computes a step sks_ksk​ that decreases mkm_kmk​ at least as much as the best step along −gk-g_k−gk​ (the Cauchy condition). It then forms the ratio ρk=(f(xk)−f(xk+sk))/(f(xk)−mk(sk))\rho_k=(f(x_k)-f(x_k+s_k))/(f(x_k)-m_k(s_k))ρk​=(f(xk​)−f(xk​+sk​))/(f(xk​)−mk​(sk​)). If ρk≥η1\rho_k\ge\eta_1ρk​≥η1​ it accepts the step, xk+1=xk+skx_{k+1}=x_k+s_kxk+1​=xk​+sk​, and the iteration is successful; otherwise xk+1=xkx_{k+1}=x_kxk+1​=xk​. Finally it updates σk+1\sigma_{k+1}σk+1​: it may shrink after a very successful step (ρk>η2\rho_k>\eta_2ρk​>η2​) and grows by a factor in [γ1,γ2][\gamma_1,\gamma_2][γ1​,γ2​] after an unsuccessful one. The parameters satisfy γ2≥γ1>1\gamma_2\ge\gamma_1>1γ2​≥γ1​>1, 1>η2≥η1>01>\eta_2\ge\eta_1>01>η2​≥η1​>0 and σ0>0\sigma_0>0σ0​>0.

ARC(S) further requires

gk⊤sk+sk⊤Bksk+σk∥sk∥3=0,sk⊤Bksk+σk∥sk∥3≥0,g_k^\top s_k+s_k^\top B_ks_k+\sigma_k\|s_k\|^3=0,\qquad s_k^\top B_ks_k+\sigma_k\|s_k\|^3\ge0,gk⊤​sk​+sk⊤​Bk​sk​+σk​∥sk​∥3=0,sk⊤​Bk​sk​+σk​∥sk​∥3≥0,

and the inner termination rule TC.s, ∥∇smk(sk)∥≤κθmin⁡(1,∥sk∥)∥gk∥\|\nabla_s m_k(s_k)\|\le\kappa_\theta\min(1,\|s_k\|)\|g_k\|∥∇s​mk​(sk​)∥≤κθ​min(1,∥sk​∥)∥gk​∥ with κθ∈(0,1)\kappa_\theta\in(0,1)κθ​∈(0,1). In Corollary 5.4 each step is moreover a global minimizer of mkm_kmk​ over a subspace Lk\mathcal L_kLk​ spanned by the orthonormal columns of a matrix QkQ_kQk​. The curvature measure is the leftmost eigenvalue

λk=λmin⁡(Qk⊤BkQk)=min⁡{v⊤Bkv:v∈Lk, ∥v∥=1}.\lambda_k=\lambda_{\min}(Q_k^\top B_kQ_k)=\min\{v^\top B_kv: v\in\mathcal L_k,\ \|v\|=1\}.λk​=λmin​(Qk⊤​Bk​Qk​)=min{v⊤Bk​v:v∈Lk​, ∥v∥=1}.

The assumptions are:

  • AF.3: f∈C2f\in C^2f∈C2;
  • AF.4: ggg is κH\kappa_HκH​-Lipschitz on an open convex set containing the iterates;
  • AF.6: HHH is LLL-Lipschitz on Rn\mathbb R^nRn;
  • AM.4: ∥(H(xk)−Bk)sk∥≤C∥sk∥2\|(H(x_k)-B_k)s_k\|\le C\|s_k\|^2∥(H(xk​)−Bk​)sk​∥≤C∥sk​∥2;
  • f(xk)≥flowf(x_k)\ge f_{\rm low}f(xk​)≥flow​ for all kkk;
  • σk≥σmin⁡>0\sigma_k\ge\sigma_{\min}>0σk​≥σmin​>0 for all kkk;
  • the standing assumption mk(sk)<f(xk)m_k(s_k)<f(x_k)mk​(sk​)<f(xk​) for every kkk (the paper's (2.6)).

Formalization targets

Goal: Corollary 5.4

Let

L0=max⁡(σ0,32γ2(C+L)),αcurv=σmin⁡6L03,κcurv=f(x0)−flowη1αcurv,L_0=\max\big(\sigma_0,\tfrac32\gamma_2(C+L)\big),\quad \alpha_{\rm curv}=\frac{\sigma_{\min}}{6L_0^3},\quad \kappa_{\rm curv}=\frac{f(x_0)-f_{\rm low}}{\eta_1\alpha_{\rm curv}},L0​=max(σ0​,23​γ2​(C+L)),αcurv​=6L03​σmin​​,κcurv​=η1​αcurv​f(x0​)−flow​​, κSu=log⁡(L0/σmin⁡)log⁡γ1,κcurvt=(1+κSu)κcurv+κSu.\kappa^u_S=\frac{\log(L_0/\sigma_{\min})}{\log\gamma_1},\qquad \kappa^t_{\rm curv}=(1+\kappa^u_S)\kappa_{\rm curv}+\kappa^u_S .κSu​=logγ1​log(L0​/σmin​)​,κcurvt​=(1+κSu​)κcurv​+κSu​.

For every ϵ>0\epsilon>0ϵ>0, the successful iterations with −λk>ϵ-\lambda_k>\epsilon−λk​>ϵ number at most

L2s=⌈κcurvϵ−3⌉.L^s_2=\lceil\kappa_{\rm curv}\epsilon^{-3}\rceil .L2s​=⌈κcurv​ϵ−3⌉.

Some iterate lll has −λl≤ϵ-\lambda_l\le\epsilon−λl​≤ϵ, and if −λk>ϵ-\lambda_k>\epsilon−λk​>ϵ for all k≤jk\le jk≤j, then at most L2sL^s_2L2s​ of the iterations 0,…,j0,\dots,j0,…,j are successful. When ϵ≤1\epsilon\le1ϵ≤1, every such jjj satisfies

j≤⌈κcurvtϵ−3⌉.j\le\lceil\kappa^t_{\rm curv}\epsilon^{-3}\rceil .j≤⌈κcurvt​ϵ−3⌉.

The constants are those printed in the paper.

Milestones

The milestones follow the paper's proof:

  • Theorems 2.1 and 2.2 (generic counting bounds for ARC);
  • Lemma 4.1 (properties of a subspace minimizer);
  • Lemma 4.2 (model decrease 16σk∥sk∥3\tfrac16\sigma_k\|s_k\|^361​σk​∥sk​∥3);
  • Lemma 5.1 (σk≤L0\sigma_k\le L_0σk​≤L0​);
  • the displays (5.28), (5.29), (5.30) and (5.32) from the proof of the corollary.

Significance

The corollary gives an explicit, dimension-free bound of order ϵ−3\epsilon^{-3}ϵ−3 on the number of iterations, and function evaluations, that a practical second-order method needs to reach approximate nonnegative curvature in its subspaces of minimization. The order is the one Nesterov and Polyak proved under much stronger requirements: exact Hessians and exact global minimization over Rn\mathbb R^nRn. Taking Lk=Rn\mathcal L_k=\mathbb R^nLk​=Rn and Bk=H(xk)B_k=H(x_k)Bk​=H(xk​) recovers their second-order guarantee. Corollary 5.5 of the paper combines this bound with the first-order bound of Corollary 5.3 into a joint first- and second-order complexity bound.

All results here are proved in the paper (some by citation of Part I). None has a machine-checked proof. A formal development would supply:

  • the counting arguments of §2;
  • the characterization of global minimizers of a cubic model over a subspace (Lemma 4.1, whose proof is in Part I);
  • the Taylor-type estimate that bounds σk\sigma_kσk​ (Lemma 5.1).

The neighbouring missions of this series formalize the first-order bounds (Corollaries 3.4 and 5.3).

Difficulty

The counting arguments are elementary once the per-iteration estimates are available. The substantial step is Lemma 4.1. Global minimality over a subspace must be turned into the identity (4.1), the inequality (4.2) and positive semidefiniteness of Qk⊤BkQk+σk∥sk∥IQ_k^\top B_kQ_k+\sigma_k\|s_k\|IQk⊤​Bk​Qk​+σk​∥sk​∥I. First-order stationarity of the reduced model gives only (4.1); the semidefiniteness needs the global characterization of minimizers of a nonconvex cubic, which a local second-order condition does not provide. Lemma 5.1 needs a third-order Taylor remainder bound under a Lipschitz Hessian. A second point of care is the bookkeeping between σk\sigma_kσk​ and σk+1\sigma_{k+1}σk+1​ in Theorem 2.1, where the printed hypothesis is one index short (see below).

Formalization scope

  • The space is Rn\mathbb R^nRn as EuclideanSpace ℝ (Fin n). The gradient is Mathlib's gradient, the Hessian is fderiv ℝ (gradient f), and BkB_kBk​ are self-adjoint continuous linear operators with the operator norm.
  • The algorithm is a predicate on sequences (xk,sk,σk,Bk)(x_k,s_k,\sigma_k,B_k)(xk​,sk​,σk​,Bk​), not a function, because the step and the new weight are choices. The Cauchy condition is stated as mk(sk)≤mk(−αgk)m_k(s_k)\le m_k(-\alpha g_k)mk​(sk​)≤mk​(−αgk​) for all α≥0\alpha\ge0α≥0. Successful means ρk≥η1\rho_k\ge\eta_1ρk​≥η1​, and the counts are cardinalities of filtered ranges.
  • λmin⁡(Qk⊤BkQk)\lambda_{\min}(Q_k^\top B_kQ_k)λmin​(Qk⊤​Bk​Qk​) is the Rayleigh-quotient infimum of BkB_kBk​ over unit vectors of Lk\mathcal L_kLk​, never the eigenvalue of BkB_kBk​ on all of Rn\mathbb R^nRn; for Lk={0}\mathcal L_k=\{0\}Lk​={0} Lean's empty infimum is 000. The subspace minimizer condition is sk∈Lks_k\in\mathcal L_ksk​∈Lk​ with mk(sk)≤mk(t)m_k(s_k)\le m_k(t)mk​(sk​)≤mk​(t) for all t∈Lkt\in\mathcal L_kt∈Lk​, and it is stated in addition to the ARC(S) conditions.
  • (2.6) is a hypothesis for every kkk; the paper assumes it "unless the algorithm terminates". Lean's x/0=0x/0=0x/0=0 would otherwise classify a zero predicted decrease as unsuccessful.
  • "Takes at most NNN iterations to reach −λl2+1≤ϵ-\lambda_{l_2+1}\le\epsilon−λl2​+1​≤ϵ" is stated as: every jjj with −λk>ϵ-\lambda_k>\epsilon−λk​>ϵ for all k≤jk\le jk≤j satisfies the bound; the existence of a first iterate with −λl2+1≤ϵ-\lambda_{l_2+1}\le\epsilon−λl2​+1​≤ϵ, which the corollary asserts, is stated separately. The total count is stated as finiteness of the set together with a bound on its cardinality.
  • Correction. Theorem 2.1 is stated with σk≤σˉ\sigma_k\le\bar\sigmaσk​≤σˉ for k≤j+1k\le j+1k≤j+1 instead of the printed k≤jk\le jk≤j. The printed version fails for j=0j=0j=0 when iteration 000 is unsuccessful and σˉ=σ0\bar\sigma=\sigma_0σˉ=σ0​.
  • A formalization in which the subspace measure is replaced by λmin⁡(Bk)\lambda_{\min}(B_k)λmin​(Bk​), the subspace minimizer condition is dropped, or (2.6) is weakened to a vacuous hypothesis does not count as this result; nor does one in which the constants are replaced by an existential.
  • Contributions are welcome on any milestone. Lemmas 4.1, 4.2 and 5.1 are reusable for every cubic-regularisation development.

Selected references

  • C. Cartis, N. I. M. Gould, Ph. L. Toint, Adaptive cubic regularisation methods for unconstrained optimization. Part II: worst-case function- and derivative-evaluation complexity, Math. Program. 130(2):295–319, 2011 (preprint rev. 15 Sep 2009). https://doi.org/10.1007/s10107-009-0337-y
  • C. Cartis, N. I. M. Gould, Ph. L. Toint, Adaptive cubic regularisation methods for unconstrained optimization. Part I: motivation, convergence and numerical results, Math. Program. 127(2):245–295, 2011. https://doi.org/10.1007/s10107-009-0286-5
  • Yu. Nesterov, B. T. Polyak, Cubic regularization of Newton method and its global performance, Math. Program. 108(1):177–205, 2006. https://doi.org/10.1007/s10107-006-0706-8
  • A. Griewank, The modification of Newton's method for unconstrained optimization by bounding cubic terms, Technical Report NA/12, DAMTP, University of Cambridge, 1981.
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Numerical AnalysisOperations ResearchOptimization·Captain: mikedeng1

Adaptive Cubic Regularisation Methods for Unconstrained Optimization. Part II: Worst-Case Function- and Derivative-Evaluation Complexity 2: ARC(S) Reaches ‖g‖ ≤ ε in O(ε^(−3/2)) IterationsResearch Paper

Motivation

Second-order methods for smooth nonconvex minimization are used in practice because they converge in far fewer iterations than gradient descent, yet for a long time their worst-case guarantee from an arbitrary starting point was no better than that of steepest descent. Nesterov and Polyak (Math. Program. 108, 2006) showed that adding a cubic term to Newton's quadratic model and minimizing that model globally at each step reaches a point with ∥∇f∥≤ϵ\|\nabla f\|\le\epsilon∥∇f∥≤ϵ in O(ϵ−3/2)O(\epsilon^{-3/2})O(ϵ−3/2) iterations when the Hessian is Lipschitz, against O(ϵ−2)O(\epsilon^{-2})O(ϵ−2) for steepest descent. Their analysis needs the exact Hessian and an exact global minimizer of a nonconvex model, both of which are too expensive in large-scale computation.

Cartis, Gould and Toint built the Adaptive Regularisation with Cubics (ARC) framework for that setting: the Hessian may be replaced by an approximation BkB_kBk​, the regularisation weight is adapted without knowledge of a Lipschitz constant, and the step only approximately minimizes the model over a subspace (in practice a Krylov subspace generated by the Lanczos method). Part I (Math. Program. 127, 2011) proved convergence and fast local rates. Part II (Math. Program. 130, 2011), the source of this mission, proved that the practical variant ARC(S) keeps the O(ϵ−3/2)O(\epsilon^{-3/2})O(ϵ−3/2) worst-case bound. Later work showed that this order is sharp for the method (Cartis, Gould & Toint, SIAM J. Optim. 2010) and cannot be improved by any method using derivatives up to second order (Carmon, Duchi, Hinder & Sidford, Math. Program. 2020).

Setting

Let f:Rn→Rf:\mathbb R^n\to\mathbb Rf:Rn→R be twice continuously differentiable, with gradient g=∇fg=\nabla fg=∇f, Hessian H=∇2fH=\nabla^2 fH=∇2f, and Euclidean norm ∥⋅∥\|\cdot\|∥⋅∥. At iterate xkx_kxk​, with gk=g(xk)g_k=g(x_k)gk​=g(xk​), a symmetric operator BkB_kBk​ and a weight σk>0\sigma_k>0σk​>0, the cubic model is

mk(s)=f(xk)+s⊤gk+12s⊤Bks+13σk∥s∥3.m_k(s)=f(x_k)+s^\top g_k+\tfrac12 s^\top B_k s+\tfrac13\sigma_k\|s\|^3 .mk​(s)=f(xk​)+s⊤gk​+21​s⊤Bk​s+31​σk​∥s∥3.

ARC (Algorithm 2.1) has parameters γ2≥γ1>1\gamma_2\ge\gamma_1>1γ2​≥γ1​>1, 1>η2≥η1>01>\eta_2\ge\eta_1>01>η2​≥η1​>0 and σ0>0\sigma_0>0σ0​>0. At each iteration it:

  1. chooses a step sks_ksk​ with mk(sk)≤mk(−αgk)m_k(s_k)\le m_k(-\alpha g_k)mk​(sk​)≤mk​(−αgk​) for every α≥0\alpha\ge0α≥0 (the Cauchy condition);
  2. computes ρk=f(xk)−f(xk+sk)f(xk)−mk(sk)\rho_k=\dfrac{f(x_k)-f(x_k+s_k)}{f(x_k)-m_k(s_k)}ρk​=f(xk​)−mk​(sk​)f(xk​)−f(xk​+sk​)​;
  3. accepts the step (xk+1=xk+skx_{k+1}=x_k+s_kxk+1​=xk​+sk​) if ρk≥η1\rho_k\ge\eta_1ρk​≥η1​, and otherwise sets xk+1=xkx_{k+1}=x_kxk+1​=xk​;
  4. picks σk+1\sigma_{k+1}σk+1​ in (0,σk](0,\sigma_k](0,σk​], [σk,γ1σk][\sigma_k,\gamma_1\sigma_k][σk​,γ1​σk​] or [γ1σk,γ2σk][\gamma_1\sigma_k,\gamma_2\sigma_k][γ1​σk​,γ2​σk​] according as ρk>η2\rho_k>\eta_2ρk​>η2​, η1≤ρk≤η2\eta_1\le\rho_k\le\eta_2η1​≤ρk​≤η2​ or ρk<η1\rho_k<\eta_1ρk​<η1​.

Iterations with ρk≥η1\rho_k\ge\eta_1ρk​≥η1​ are successful. Sj\mathcal S_jSj​ and Uj\mathcal U_jUj​ are the successful and unsuccessful iterations k≤jk\le jk≤j.

ARC(S) (Algorithm 4.1) additionally requires each step to satisfy

  • gk⊤sk+sk⊤Bksk+σk∥sk∥3=0g_k^\top s_k+s_k^\top B_ks_k+\sigma_k\|s_k\|^3=0gk⊤​sk​+sk⊤​Bk​sk​+σk​∥sk​∥3=0 (4.1);
  • sk⊤Bksk+σk∥sk∥3≥0s_k^\top B_ks_k+\sigma_k\|s_k\|^3\ge0sk⊤​Bk​sk​+σk​∥sk​∥3≥0 (4.2);
  • the termination rule TC.s: ∥gk+Bksk+σk∥sk∥sk∥≤κθmin⁡(1,∥sk∥) ∥gk∥\|g_k+B_ks_k+\sigma_k\|s_k\|s_k\|\le\kappa_\theta\min(1,\|s_k\|)\,\|g_k\|∥gk​+Bk​sk​+σk​∥sk​∥sk​∥≤κθ​min(1,∥sk​∥)∥gk​∥, with κθ∈(0,1)\kappa_\theta\in(0,1)κθ​∈(0,1).

The assumptions are:

  • AF.4: ggg is κH\kappa_HκH​-Lipschitz on an open convex set containing the iterates, κH≥1\kappa_H\ge1κH​≥1;
  • AF.6: HHH is LLL-Lipschitz on Rn\mathbb R^nRn, L>0L>0L>0;
  • AM.4: ∥(H(xk)−Bk)sk∥≤C∥sk∥2\|(H(x_k)-B_k)s_k\|\le C\|s_k\|^2∥(H(xk​)−Bk​)sk​∥≤C∥sk​∥2, C>0C>0C>0;
  • (2.11): σk≥σmin⁡>0\sigma_k\ge\sigma_{\min}>0σk​≥σmin​>0;
  • (2.6): mk(sk)<f(xk)m_k(s_k)<f(x_k)mk​(sk​)<f(xk​) for every kkk;
  • f(xk)≥flowf(x_k)\ge f_{\rm low}f(xk​)≥flow​ for every kkk.

Formalization targets

Goal: Corollary 5.3

With L0=max⁡(σ0,32γ2(C+L))L_0=\max(\sigma_0,\tfrac32\gamma_2(C+L))L0​=max(σ0​,23​γ2​(C+L)), κg=(1−κθ)/(12L+C+L0+κθκH)\kappa_g=\sqrt{(1-\kappa_\theta)/(\tfrac12L+C+L_0+\kappa_\theta\kappa_H)}κg​=(1−κθ​)/(21​L+C+L0​+κθ​κH​)​, αS=σmin⁡κg3/6\alpha_S=\sigma_{\min}\kappa_g^3/6αS​=σmin​κg3​/6, κSs=(f(x0)−flow)/(η1αS)\kappa^s_S=(f(x_0)-f_{\rm low})/(\eta_1\alpha_S)κSs​=(f(x0​)−flow​)/(η1​αS​), κSu=log⁡(L0/σmin⁡)/log⁡γ1\kappa^u_S=\log(L_0/\sigma_{\min})/\log\gamma_1κSu​=log(L0​/σmin​)/logγ1​ and κS=(1+κSu)(2+κSs)\kappa_S=(1+\kappa^u_S)(2+\kappa^s_S)κS​=(1+κSu​)(2+κSs​), the corollary has three parts:

  1. at most ⌈κSsϵ−3/2⌉\lceil\kappa^s_S\epsilon^{-3/2}\rceil⌈κSs​ϵ−3/2⌉ successful iterations have min⁡(∥gk∥,∥gk+1∥)>ϵ\min(\|g_k\|,\|g_{k+1}\|)>\epsilonmin(∥gk​∥,∥gk+1​∥)>ϵ;
  2. if ∥g0∥,∥g1∥>ϵ\|g_0\|,\|g_1\|>\epsilon∥g0​∥,∥g1​∥>ϵ, at most ⌈κSsϵ−3/2⌉+1\lceil\kappa^s_S\epsilon^{-3/2}\rceil+1⌈κSs​ϵ−3/2⌉+1 successful iterations precede the first l1l_1l1​ with ∥gl1+1∥≤ϵ\|g_{l_1+1}\|\le\epsilon∥gl1​+1​∥≤ϵ;
  3. if moreover ϵ≤1\epsilon\le1ϵ≤1, then
l1≤⌈κS ϵ−3/2⌉.l_1\le\left\lceil\kappa_S\,\epsilon^{-3/2}\right\rceil .l1​≤⌈κS​ϵ−3/2⌉.

Milestones

The milestones follow the proof:

  • Theorem 2.1, (2.13) and (2.14): unsuccessful iterations bounded by successful ones;
  • Theorem 2.2: a uniform model decrease bounds the number of successful iterations;
  • Lemma 4.2: f(xk)−mk(sk)≥16σk∥sk∥3f(x_k)-m_k(s_k)\ge\tfrac16\sigma_k\|s_k\|^3f(xk​)−mk​(sk​)≥61​σk​∥sk​∥3;
  • Lemma 5.1: σk≤L0\sigma_k\le L_0σk​≤L0​;
  • Lemma 5.2: ∥sk∥≥κg∥gk+1∥\|s_k\|\ge\kappa_g\sqrt{\|g_{k+1}\|}∥sk​∥≥κg​∥gk+1​∥​ on successful iterations;
  • the displayed steps (5.20), (5.22) and (5.23) of the corollary's proof.

Significance

The corollary shows that inexact subspace minimization and approximate Hessians cost nothing in worst-case order. The bound is the same O(ϵ−3/2)O(\epsilon^{-3/2})O(ϵ−3/2) count of iterations, function evaluations and gradient evaluations as for the exact cubic-regularised Newton method. It is the founding result of the evaluation-complexity theory of adaptive regularisation methods, and later results build on it: higher-order regularisation, constrained and stochastic variants, and the lower bounds showing that ϵ−3/2\epsilon^{-3/2}ϵ−3/2 is optimal for second-order methods.

The result is proved on paper; to the knowledge of this mission it has no machine-checked proof. Formalizing it fixes the exact hypotheses: the standing assumption (2.6), the Lipschitz set in AF.4, and the off-by-one in Theorem 2.1. It also yields reusable Lean statements of the counting arguments (Theorems 2.1 and 2.2) shared by every trust-region and adaptive-regularisation complexity proof.

Difficulty

The first idea is to bound the model decrease by ϵ3/2\epsilon^{3/2}ϵ3/2 directly from ∥gk∥>ϵ\|g_k\|>\epsilon∥gk​∥>ϵ. That fails: TC.s and the Taylor estimates bound the step length by the gradient at the next iterate, ∥gk+1∥\|g_{k+1}\|∥gk+1​∥, not by ∥gk∥\|g_k\|∥gk​∥. The count must therefore use min⁡(∥gk∥,∥gk+1∥)\min(\|g_k\|,\|g_{k+1}\|)min(∥gk​∥,∥gk+1​∥), and turning it into a bound on the first l1l_1l1​ with ∥gl1+1∥≤ϵ\|g_{l_1+1}\|\le\epsilon∥gl1​+1​∥≤ϵ needs care at the last iteration. The constant κg\kappa_gκg​ combines four sources of error: the Hessian approximation, the Lipschitz Hessian, the bound on σk\sigma_kσk​, and the inexact model gradient. The bound on σk\sigma_kσk​ itself (Lemma 5.1) needs a second-order Taylor estimate of fff along the step. Unsuccessful iterations do not decrease fff and are counted separately through the growth of σk\sigma_kσk​.

Formalization scope

The Lean development uses the following conventions:

  • Rn\mathbb R^nRn is EuclideanSpace ℝ (Fin n), ggg is gradient f and HHH is fderiv ℝ (gradient f);
  • BkB_kBk​ is a continuous linear operator with IsSelfAdjoint, and operator norms are Mathlib's;
  • runs of ARC and ARC(S) are predicates on the sequences x,s,σ,Bx,s,\sigma,Bx,s,σ,B, because the step and the new weight are choices;
  • the Cauchy condition is stated as mk(sk)≤mk(−αgk)m_k(s_k)\le m_k(-\alpha g_k)mk​(sk​)≤mk​(−αgk​) for all α≥0\alpha\ge0α≥0;
  • TC.s uses the explicit model gradient gk+Bksk+σk∥sk∥skg_k+B_ks_k+\sigma_k\|s_k\|s_kgk​+Bk​sk​+σk​∥sk​∥sk​;
  • powers ϵ±3/2\epsilon^{\pm3/2}ϵ±3/2 are real powers and ceilings are integer ceilings.

Hypotheses and quantifiers:

  • (2.6) is a hypothesis for every kkk, the paper's standing assumption for ARC(S) (p. 12). It also rules out the junk value ρk=0\rho_k=0ρk​=0 that Lean's division by zero would give.
  • "At most NNN iterations before ∥gl1+1∥≤ϵ\|g_{l_1+1}\|\le\epsilon∥gl1​+1​∥≤ϵ" is stated as: every jjj with ∥gk∥>ϵ\|g_k\|>\epsilon∥gk​∥>ϵ for all k≤jk\le jk≤j satisfies j≤Nj\le Nj≤N. This also asserts that l1l_1l1​ exists.
  • Theorem 2.1 is posed with σk≤σˉ\sigma_k\le\bar\sigmaσk​≤σˉ for k≤j+1k\le j+1k≤j+1: the printed range k≤jk\le jk≤j makes it false at j=0j=0j=0.

The constants are written out exactly as printed; replacing them with "there is a constant" would trivialize the goal and is excluded. Contributions are welcome:

  • Taylor estimates under a Lipschitz Hessian on EuclideanSpace;
  • a general counting lemma behind Theorems 2.1–2.2.

Both are reusable well beyond this mission.

Selected references

  • C. Cartis, N. I. M. Gould, Ph. L. Toint, Adaptive cubic regularisation methods for unconstrained optimization. Part II: worst-case function- and derivative-evaluation complexity, Math. Program. 130(2):295–319, 2011 (preprint rev. 15 Sep 2009). https://doi.org/10.1007/s10107-009-0337-y
  • C. Cartis, N. I. M. Gould, Ph. L. Toint, Adaptive cubic regularisation methods for unconstrained optimization. Part I: motivation, convergence and numerical results, Math. Program. 127(2):245–295, 2011. https://doi.org/10.1007/s10107-009-0286-5
  • C. Cartis, N. I. M. Gould, Ph. L. Toint, On the complexity of steepest descent, Newton's and regularized Newton's methods for nonconvex unconstrained optimization problems, SIAM J. Optim. 20(6):2833–2852, 2010. https://doi.org/10.1137/090774100
  • Y. Carmon, J. C. Duchi, O. Hinder, A. Sidford, Lower bounds for finding stationary points I, Math. Program. 184:71–120, 2020. https://doi.org/10.1007/s10107-019-01406-y
  • Yu. Nesterov, B. T. Polyak, Cubic regularization of Newton method and its global performance, Math. Program. 108(1):177–205, 2006. https://doi.org/10.1007/s10107-006-0706-8
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Dynamic ProgrammingOperations ResearchProbability·Captain: mikedeng1

Information Relaxations and Duality in Stochastic Dynamic Programs 2: With a Common Generating Function, a Looser Information Relaxation Gives a Weaker Dual BoundResearch Paper

Motivation

Many stochastic dynamic programs in operations research, such as inventory control with partially observed demand or the pricing of American options, are too large to solve exactly. A heuristic policy gives a lower bound on the optimal expected reward; to judge whether it is good enough one needs an upper bound. Brown, Smith and Sun (Oper. Res. 2010) build such bounds by information relaxation: let the decision maker see more than she would in reality, and charge a penalty for using the extra information. The construction generalizes the martingale duality for optimal stopping of Haugh and Kogan (Oper. Res. 2004), Rogers (Math. Finance 2002) and Andersen and Broadie (Manage. Sci. 2004).

In applications, the analyst chooses both the relaxation and the penalty, trading the quality of the bound against the cost of computing it. Proposition 2.3 of the paper collects four properties that govern this choice. The first is the subject of this mission.

Setting

Uncertainty is a probability space (Ω,F,P)(\Omega,\mathcal F,\mathbb P)(Ω,F,P), and decisions are made in periods t=0,…,Tt=0,\dots,Tt=0,…,T. The natural filtration F=(F0,…,FT)\mathbb F=(\mathcal F_0,\dots,\mathcal F_T)F=(F0​,…,FT​) records what is known in each period, with F0={∅,Ω}\mathcal F_0=\{\emptyset,\Omega\}F0​={∅,Ω}. An action sequence is a=(a0,…,aT)a=(a_0,\dots,a_T)a=(a0​,…,aT​), chosen from feasible sets At(a0,…,at−1)A_t(a_0,\dots,a_{t-1})At​(a0​,…,at−1​). Period rewards rt(a0,…,at)r_t(a_0,\dots,a_t)rt​(a0​,…,at​) are Ft\mathcal F_tFt​-measurable random variables and the total reward is r(a)=∑trt(a)r(a)=\sum_t r_t(a)r(a)=∑t​rt​(a).

A policy is a map α:Ω→A\alpha:\Omega\to Aα:Ω→A from outcomes to feasible action sequences. It is adapted to a filtration G\mathbb GG if the period-ttt action is Gt\mathcal G_tGt​-measurable; AG\mathcal A_{\mathbb G}AG​ denotes these policies. A filtration G\mathbb GG with Ft⊆Gt⊆F\mathcal F_t\subseteq\mathcal G_t\subseteq\mathcal FFt​⊆Gt​⊆F for all ttt is a relaxation of F\mathbb FF, written F⊆G\mathbb F\subseteq\mathbb GF⊆G. A penalty is a function z(a,ω)z(a,\omega)z(a,ω); it is dual feasible if E[z(αF)]≤0\mathbb E[z(\alpha_F)]\le0E[z(αF​)]≤0 for every αF∈AF\alpha_F\in\mathcal A_{\mathbb F}αF​∈AF​. For any relaxation G\mathbb GG and dual feasible zzz, the dual bound

sup⁡αG∈AGE[r(αG)−z(αG)]\sup_{\alpha_G\in\mathcal A_{\mathbb G}}\mathbb E\big[r(\alpha_G)-z(\alpha_G)\big]αG​∈AG​sup​E[r(αG​)−z(αG​)]

is at least the optimal value sup⁡αF∈AFE[r(αF)]\sup_{\alpha_F\in\mathcal A_{\mathbb F}}\mathbb E[r(\alpha_F)]supαF​∈AF​​E[r(αF​)] (weak duality, Lemma 2.1).

The paper's main source of penalties is Proposition 2.2. Given generating functions wt(a)w_t(a)wt​(a) depending only on a0,…,ata_0,\dots,a_ta0​,…,at​, set

zt(a)=E[wt(a)∣Gt]−E[wt(a)∣Ft],z(a)=∑t=0Tzt(a).z_t(a)=\mathbb E[w_t(a)\mid\mathcal G_t]-\mathbb E[w_t(a)\mid\mathcal F_t],\qquad z(a)=\sum_{t=0}^T z_t(a).zt​(a)=E[wt​(a)∣Gt​]−E[wt​(a)∣Ft​],z(a)=t=0∑T​zt​(a).

Such a penalty has zero mean along every nonanticipative policy, and its dual bound is computed by the backward recursion (10), the Bellman recursion with rewards rt−ztr_t-z_trt​−zt​ and conditional expectations given Gt\mathcal G_tGt​.

Formalization targets

Goal: Proposition 2.3(i)

For filtrations F⊆G1⊆G2\mathbb F\subseteq\mathbb G^1\subseteq\mathbb G^2F⊆G1⊆G2 and one common sequence of generating functions (w0,…,wT)(w_0,\dots,w_T)(w0​,…,wT​), let ziz^izi be the Proposition 2.2 penalty of (Gi,w)(\mathbb G^i,w)(Gi,w). Then

sup⁡αG∈AG1E[r(αG)−z1(αG)]≤sup⁡αG∈AG2E[r(αG)−z2(αG)].(12)\sup_{\alpha_G\in\mathcal A_{\mathbb G^1}}\mathbb E\big[r(\alpha_G)-z^1(\alpha_G)\big]\le\sup_{\alpha_G\in\mathcal A_{\mathbb G^2}}\mathbb E\big[r(\alpha_G)-z^2(\alpha_G)\big].\qquad(12)αG​∈AG1​sup​E[r(αG​)−z1(αG​)]≤αG​∈AG2​sup​E[r(αG​)−z2(αG​)].(12)

With a common generating function, a looser relaxation gives a weaker bound.

Milestones

  1. Equation (10). For a Proposition 2.2 penalty under a relaxation G\mathbb GG, the expectation of the initial dual value function V0GV^{\mathbb G}_0V0G​ equals the dual bound.
  2. Proposition 2.3(ii). For dual feasible z1,z2z^1,z^2z1,z2 and one relaxation G\mathbb GG, the difference of the two dual bounds lies between inf⁡αGE[z2(αG)−z1(αG)]\inf_{\alpha_G}\mathbb E[z^2(\alpha_G)-z^1(\alpha_G)]infαG​​E[z2(αG​)−z1(αG​)] and sup⁡αGE[z2(αG)−z1(αG)]\sup_{\alpha_G}\mathbb E[z^2(\alpha_G)-z^1(\alpha_G)]supαG​​E[z2(αG​)−z1(αG​)], eq. (13).
  3. Proposition 2.3(iii). For F⊆F′⊆G\mathbb F\subseteq\mathbb F'\subseteq\mathbb GF⊆F′⊆G, the penalty zt(a)=E[wt(a)∣Gt]−E[wt(a)∣Ft′]z_t(a)=\mathbb E[w_t(a)\mid\mathcal G_t]-\mathbb E[w_t(a)\mid\mathcal F'_t]zt​(a)=E[wt​(a)∣Gt​]−E[wt​(a)∣Ft′​] still satisfies the conclusions of Proposition 2.2.
  4. Proposition 2.3(iv). If z^t(a)\hat z_t(a)z^t​(a) are unbiased estimates of the terms zt(a)z_t(a)zt​(a) of a dual feasible penalty, E[z^t(a)∣Gt]=zt(a)\mathbb E[\hat z_t(a)\mid\mathcal G_t]=z_t(a)E[z^t​(a)∣Gt​]=zt​(a), and the relaxation G^\widehat{\mathbb G}G additionally reveals the estimates, then the dual bound of (G,z)(\mathbb G,z)(G,z) is at most that of (G^,z^)(\widehat{\mathbb G},\hat z)(G,z^), eq. (14).

Milestone 1 is on the goal's path; milestones 2–4 are the remaining parts of the same proposition.

Significance

Proposition 2.3(i) tells the analyst how to read a weak bound. If a cheap generating function (for instance wt=0w_t=0wt​=0, the zero penalty) gives a satisfactory bound under some relaxation, it will give a bound at least as tight under any less informative relaxation that still contains F\mathbb FF; conversely, moving to a looser relaxation without improving the generating function can only weaken the bound. Part (ii) is a continuity statement: penalties close to the ideal penalty give bounds close to the optimal value. Part (iii) permits the subtracted conditional expectation to be computed under an intermediate filtration, which the paper uses when volatility is unobserved in its option-pricing example. Part (iv) is the justification for estimating penalties by nested simulation, as in the methods of Haugh–Kogan and Andersen–Broadie: unbiased estimates yield valid, if weaker, upper bounds.

The results are proved in the paper's electronic companion. To our knowledge none of them, nor the information-relaxation duality framework itself, has a machine-checked proof. Formalizing them requires a usable theory of policies adapted to a filtration, penalties evaluated along random action sequences, and backward recursions with conditional expectations, all of which are reusable for other duality results in stochastic dynamic programming.

Difficulty

The obvious argument for (12) compares the two suprema policy by policy: AG1⊆AG2\mathcal A_{\mathbb G^1}\subseteq\mathcal A_{\mathbb G^2}AG1​⊆AG2​. This fails, because the two bounds use different penalties: for a fixed G1\mathbb G^1G1-adapted policy, E[z1(α)]\mathbb E[z^1(\alpha)]E[z1(α)] and E[z2(α)]\mathbb E[z^2(\alpha)]E[z2(α)] need not agree, so the larger policy set alone does not order the bounds. The penalty changes with the relaxation exactly so as to remove part of the value of the extra information, and the statement asserts that it never removes more than that information is worth. Even the representation (10) of a dual bound by a backward recursion is nontrivial: it requires near-optimal actions to be selected measurably in every period.

In Lean, the further difficulty is the composition of an action-indexed family of conditional expectations with a random action: ω↦zt(α(ω))(ω)\omega\mapsto z_t(\alpha(\omega))(\omega)ω↦zt​(α(ω))(ω), where each zt(a)z_t(a)zt​(a) is only defined almost surely. Countability of the action set is what makes this composite well defined up to null sets.

Formalization scope

Periods are Fin (T + 1); an action sequence is a function Fin (T + 1) → X for one countable action type X with the discrete σ-algebra (the disjoint union of the per-period action sets). Filtrations are Mathlib Filtrations of the ambient σ-algebra; a relaxation is 𝔽 ≤ 𝔾. Policies are maps Ω → (Fin (T + 1) → X) with values in the feasible set, adapted when each action is measurable for the corresponding σ-algebra. Conditional expectations are Mathlib's μ[f | m], so identities between them hold almost surely. Dual bounds are suprema in EReal over the adapted policy sets, so an infinite bound is represented and no junk value 000 arises from an unbounded supremum.

Pinned regularity, beyond the paper's text: period rewards and generating functions are uniformly bounded (almost surely for the latter) and measurable, so that every expectation exists; in part (iv), the estimates are measurable and uniformly bounded. In part (ii), the difference of two dual bounds is taken in EReal, and the case where both bounds are +∞+\infty+∞ (where the page's difference is undefined) is excluded.

The penalties z1,z2z^1,z^2z1,z2 of the goal are computed from www by the formula of Proposition 2.2; stating the goal for arbitrary penalties with Proposition 2.2's properties would be a different and false claim. Likewise G^\widehat{\mathbb G}G in part (iv) is constructed from G\mathbb GG and the estimates.

The definitions duplicate those of mission 1 of this series (the framework, the recursive model, the penalty construction); they are expected to be merged. Contributions of reusable lemmas about adapted policies over countable action sets and about backward recursions with conditional expectations are welcome.

Selected references

  • D. B. Brown, J. E. Smith, P. Sun, Information Relaxations and Duality in Stochastic Dynamic Programs, Operations Research, Articles in Advance, 2010. https://doi.org/10.1287/opre.1090.0796
  • M. B. Haugh, L. Kogan, Pricing American Options: A Duality Approach, Operations Research 52(2), 2004. https://doi.org/10.1287/opre.1030.0070
  • L. Andersen, M. Broadie, Primal-Dual Simulation Algorithm for Pricing Multidimensional American Options, Management Science 50(9), 2004. https://doi.org/10.1287/mnsc.1040.0258
  • L. C. G. Rogers, Monte Carlo Valuation of American Options, Mathematical Finance 12(3), 2002. https://doi.org/10.1111/1467-9965.02010
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Numerical AnalysisOperations ResearchOptimization·Captain: mikedeng1

On the Complexity of Steepest Descent, Newton's and Regularized Newton's Methods for Nonconvex Unconstrained Optimization Problems 2: Newton's Method Can Need ε^(−2+τ) Iterations to Reach ‖g‖ ≤ εResearch Paper

Motivation

Newton's method is the reference second-order method for unconstrained minimization of a smooth function f:Rn→Rf:\mathbb R^n\to\mathbb Rf:Rn→R. Near a nondegenerate local minimizer it converges quadratically, and in practice it often works well far from one. Its global behaviour on nonconvex functions is a different matter. The pure method may fail outright when the Hessian is singular or indefinite, and when every Hessian along the run is positive definite it is still not clear how fast the gradient goes to zero.

A natural question is how many iterations a method needs, in the worst case, to produce an iterate xkx_kxk​ with ∥∇f(xk)∥≤ε\|\nabla f(x_k)\|\le\varepsilon∥∇f(xk​)∥≤ε. For steepest descent on functions with a Lipschitz gradient the answer is known to be at most O(ε−2)O(\varepsilon^{-2})O(ε−2) (Nesterov 2004, p. 29). Cartis, Gould and Toint (SIAM J. Optim. 2010) showed that this bound is essentially sharp, and that Newton's method can be just as slow. A matching O(ε−3/2)O(\varepsilon^{-3/2})O(ε−3/2) bound holds for cubic regularization (Nesterov–Polyak 2006; Cartis–Gould–Toint 2011), so the Newton example separates plain Newton from its regularized variants in the worst case.

This mission is the second of three on that paper. It covers the Newton example of §3.

Setting

Work in the Euclidean plane R2\mathbb R^2R2, with coordinates [x]1,[x]2[x]_1,[x]_2[x]1​,[x]2​. For a twice continuously differentiable f:R2→Rf:\mathbb R^2\to\mathbb Rf:R2→R write g(x)=∇f(x)g(x)=\nabla f(x)g(x)=∇f(x) for the gradient and H(x)=∇2f(x)H(x)=\nabla^2 f(x)H(x)=∇2f(x) for the Hessian, a symmetric linear operator on R2\mathbb R^2R2 with operator norm ∥H(x)∥\|H(x)\|∥H(x)∥.

At an iterate xkx_kxk​, Newton's method (in its simplest form) minimizes the quadratic model

mk(xk+s)=f(xk)+g(xk)Ts+12sTH(xk)s.m_k(x_k+s)=f(x_k)+g(x_k)^Ts+\tfrac12 s^TH(x_k)s .mk​(xk​+s)=f(xk​)+g(xk​)Ts+21​sTH(xk​)s.

The method is well defined when H(xk)H(x_k)H(xk​) is positive definite. The model then has a unique global minimizer sks_ksk​, characterized by H(xk)sk=−g(xk)H(x_k)s_k=-g(x_k)H(xk​)sk​=−g(xk​), and the next iterate is xk+1=xk+skx_{k+1}=x_k+s_kxk+1​=xk​+sk​ (the unit Newton step). A run of the method from x0x_0x0​ is a sequence (xk)k≥0(x_k)_{k\ge0}(xk​)k≥0​ satisfying these two conditions at every kkk.

The paper aims at the standard assumptions under which globalized Newton methods are provably convergent:

AS.1 fff is twice continuously differentiable, bounded below, and has bounded and Lipschitz continuous second derivatives along each segment [xk,xk+1][x_k,x_{k+1}][xk​,xk+1​].

Fix τ∈(0,1)\tau\in(0,1)τ∈(0,1) and let η=τ/(4−2τ)\eta=\tau/(4-2\tau)η=τ/(4−2τ), so that 12+η=1/(2−τ)\tfrac12+\eta=1/(2-\tau)21​+η=1/(2−τ).

Formalization targets

Goal: Newton's method can need ⌊ε−(2−τ)⌋\lfloor\varepsilon^{-(2-\tau)}\rfloor⌊ε−(2−τ)⌋ iterations

For every τ∈(0,1)\tau\in(0,1)τ∈(0,1) there exist f:R2→Rf:\mathbb R^2\to\mathbb Rf:R2→R and a run (xk)(x_k)(xk​) of Newton's method on fff from x0=0x_0=0x0​=0 such that

  1. fff is twice continuously differentiable on R2\mathbb R^2R2 and bounded below, and sup⁡y∥H(y)∥<∞\sup_y\|H(y)\|<\inftysupy​∥H(y)∥<∞;
  2. there is one constant LLL with ∥H(y)−H(z)∥≤L∥y−z∥\|H(y)-H(z)\|\le L\|y-z\|∥H(y)−H(z)∥≤L∥y−z∥ for all y,zy,zy,z on a common segment [xk,xk+1][x_k,x_{k+1}][xk​,xk+1​];
  3. every step achieves the model value, f(xk+1)=mk(xk+1)f(x_{k+1})=m_k(x_{k+1})f(xk+1​)=mk​(xk+1​) (the paper's (3.8));
  4. for every k≥0k\ge0k≥0,
∥g(xk)∥ ≥ (1k+1)12−τ;\|g(x_k)\|\ \ge\ \Big(\frac1{k+1}\Big)^{\frac1{2-\tau}};∥g(xk​)∥ ≥ (k+11​)2−τ1​;
  1. for every ε∈(0,1)\varepsilon\in(0,1)ε∈(0,1) and every kkk, if ∥g(xk)∥≤ε\|g(x_k)\|\le\varepsilon∥g(xk​)∥≤ε then
k+1 ≥ ⌊1ε2−τ⌋.k+1\ \ge\ \Big\lfloor \frac1{\varepsilon^{2-\tau}}\Big\rfloor .k+1 ≥ ⌊ε2−τ1​⌋.

The goal fixes no constant: the bounds on the Hessian and its Lipschitz modulus are existential. The paper's explicit constants appear in the milestones.

Milestones

The milestones follow the paper's verification, in order:

  • the prescribed gradients satisfy the lower bound (2.3) (p. 6);
  • the prescribed data (xk,fk,gk,Hk)(x_k,f_k,g_k,H_k)(xk​,fk​,gk​,Hk​) of (3.2)–(3.4) satisfy the Newton conditions (3.6)–(3.8) (pp. 6–7);
  • ∣ψk∣∈(0,1)|\psi_k|\in(0,1)∣ψk​∣∈(0,1), the Hermite conditions (2.12)–(2.13) for the first-coordinate pieces pkp_kpk​ at αk=1\alpha_k=1αk​=1, and the bound (2.17) on pk′′p_k''pk′′​ (pp. 4–5, used on p. 7);
  • the interpolation conditions for the second-coordinate pieces qkq_kqk​, and ∣qk′′∣≤219|q_k''|\le219∣qk′′​∣≤219 (pp. 7–8);
  • the knot values (3.9)–(3.10) and the pieces pkp_kpk​, qkq_kqk​ on their intervals are nonnegative, so f2≥0f_2 \ge 0f2​≥0 (pp. 7–8);
  • the third derivative along each step is at most 858858858 (p. 9).

Significance

The result. Under the standard assumptions for which globalized Newton methods are known to converge, Newton's method can need nearly ε−2\varepsilon^{-2}ε−2 iterations to reduce the gradient below ε\varepsilonε, the same order as the worst case of steepest descent. Hence no worst-case complexity bound better than O(ε−2+τ)O(\varepsilon^{-2+\tau})O(ε−2+τ) can be proved for Newton's method under those assumptions, for any τ>0\tau>0τ>0. The identity f(xk+1)=mk(xk+1)f(x_{k+1})=m_k(x_{k+1})f(xk+1​)=mk​(xk+1​) makes the example robust (§6): every iteration is very successful in a trust-region framework, and the unit step is accepted by a linesearch, so the trust-region and linesearch globalizations of Newton's method are equally slow on it. The contrast with the O(ε−3/2)O(\varepsilon^{-3/2})O(ε−3/2) bound for cubic regularization is what makes regularized Newton methods the better choice from the worst-case point of view.

Formalizing it. The result is proved on paper but has no machine-checked proof that we know of. A formalization has to make several things precise that the paper treats briefly: the smooth extension of the construction to negative coordinates, the C2C^2C2 gluing of infinitely many polynomial pieces, the passage from bounded third derivatives to Lipschitz continuity of the Hessian along the path, and the counting step from the gradient bound to the iteration count. The result is closed mathematically; the open work is the formal proof.

Difficulty

There is no difficulty in writing down the iterates: the paper prescribes xkx_kxk​, f(xk)f(x_k)f(xk​), g(xk)g(x_k)g(xk​) and H(xk)H(x_k)H(xk​) explicitly, and checking that they are consistent with Newton's method is algebra. The difficulty is to find one function fff on all of R2\mathbb R^2R2 that takes these values, gradients and Hessians at the iterates and keeps the global properties: twice continuously differentiable everywhere, bounded below, bounded Hessian, Lipschitz Hessian along the path.

The first attempt fails at the Lipschitz requirement. The one-dimensional steepest-descent example of §2 with unit steplength already is a run of Newton's method, since its second derivative equals 111 at every iterate, and its gradients decay at the required rate. But its third derivative grows linearly with kkk (p. 5), so its second derivative is not Lipschitz continuous along the path, and AS.1 fails. The iterates of that example get closer together while the curvature must still return to 111 at each of them. Any construction has to reconcile the slow decay of the gradient with a Lipschitz modulus of the Hessian along the path that does not grow with kkk. A Lipschitz constant on the whole plane is neither claimed nor available for the paper's construction.

Formalization scope

  • The plane is EuclideanSpace ℝ (Fin 2). The gradient is gradient f, the Hessian is fderiv ℝ (gradient f), and its norm is the operator norm. Components are x 0 and x 1.
  • The run is part of the conclusion (∃ x), with positive definiteness at every iterate. It is not a hypothesis, so the statement cannot hold vacuously. The Hessian in the Newton rule is the true Hessian of fff, not a free sequence of matrices.
  • fff is required on all of R2\mathbb R^2R2; the paper builds it on the nonnegative quadrant and remarks that it extends.
  • Two choices are stronger than AS.1 as printed: the Hessian is bounded on all of R2\mathbb R^2R2, not only along the segments, and the Lipschitz constant along the segments is one constant for all kkk.
  • τ∈(0,1)\tau\in(0,1)τ∈(0,1): the paper says "for any τ>0\tau>0τ>0", but the construction needs τ<1\tau<1τ<1, and for ε<1\varepsilon<1ε<1 the cases τ<1\tau<1τ<1 imply the iteration bound for every τ>0\tau>0τ>0.
  • The count is posed as k+1≥⌊ε−(2−τ)⌋k+1\ge\lfloor\varepsilon^{-(2-\tau)}\rfloork+1≥⌊ε−(2−τ)⌋, counting the iterates x0,…,xkx_0,\dots,x_kx0​,…,xk​. Posed as k≥⌊ε−(2−τ)⌋k\ge\lfloor\varepsilon^{-(2-\tau)}\rfloork≥⌊ε−(2−τ)⌋ it is false: as printed, the paper's count is off by one.
  • Ruling out trivialization: the statement is existential in fff and in the run, and the run must satisfy Newton's rule with the true Hessian. Dropping positive definiteness, using a free matrix sequence, or replacing "≥\ge≥" in the gradient bound by a statement about one coordinate would each change the theorem.
  • Milestones are stated about explicit data: the prescribed values xk,fk,gk,Hkx_k,f_k,g_k,H_kxk​,fk​,gk​,Hk​ and the quintic pieces pk,qkp_k,q_kpk​,qk​, defined in two definition files. The goal does not mention them, and a solver may use any other construction.
  • Needed infrastructure: derivatives of polynomials, C2C^2C2 gluing of piecewise functions with matching values and first and second derivatives, convergence of ∑(k+1)−(1+2η)\sum (k+1)^{-(1+2\eta)}∑(k+1)−(1+2η), and the rpow identity 12+η=1/(2−τ)\tfrac12+\eta=1/(2-\tau)21​+η=1/(2−τ). The gluing lemma is reusable beyond this mission: missions 1 and 3 of the series use the same kind of construction.

Selected references

  • C. Cartis, N. I. M. Gould, Ph. L. Toint, On the complexity of steepest descent, Newton's and regularized Newton's methods for nonconvex unconstrained optimization problems, SIAM J. Optim. 20(6), 2833–2852, 2010. https://doi.org/10.1137/090774100 (preprint 15 Oct 2009 used here).
  • Yu. Nesterov, Introductory Lectures on Convex Optimization: A Basic Course, Kluwer, 2004. https://doi.org/10.1007/978-1-4419-8853-9
  • Yu. Nesterov, B. T. Polyak, Cubic regularization of Newton method and its global performance, Math. Program. 108, 177–205, 2006. https://doi.org/10.1007/s10107-006-0706-8
  • C. Cartis, N. I. M. Gould, Ph. L. Toint, Adaptive cubic regularisation methods for unconstrained optimization. Part II: worst-case function- and derivative-evaluation complexity, Math. Program. 130, 295–319, 2011. https://doi.org/10.1007/s10107-009-0337-y
  • J. E. Dennis, R. B. Schnabel, Numerical Methods for Unconstrained Optimization and Nonlinear Equations, Prentice-Hall, 1983. https://doi.org/10.1137/1.9781611971200
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AnalysisControl TheoryDynamical Systems+1·Captain: mikedeng1

Continuous-Time Average-Preserving Opinion Dynamics with Opinion-Dependent Communications 3: The n-Agent Model Approximates the Continuum Model Uniformly on Every Finite HorizonResearch Paper

Motivation

Bounded-confidence models describe a population of agents who repeatedly average their opinions with those of agents whose opinions are close to their own. They are used to study consensus and polarization in opinion formation, and in control as a primitive for decentralized rendezvous of mobile agents. Simulations of these models show a robust phenomenon: opinions converge to clusters, and the distances between clusters are typically close to twice the confidence radius rather than just above it. For finitely many agents this regularity has resisted proof.

V. D. Blondel, J. M. Hendrickx and J. N. Tsitsiklis (SIAM J. Control Optim. 48 (2010) 5214–5240) study a continuous-time version of the model in two forms: with nnn discrete agents, and with a continuum of agents indexed by [0,1][0,1][0,1]. For the continuum they prove that regular initial opinions converge to clusters whose separation obeys a lower bound depending on the cluster weights. To transfer such conclusions to finitely many agents one needs to know that the nnn-agent model is close to the continuum model when nnn is large. Section 4 of the paper proves this on every finite time horizon. This mission formalizes that result.

Setting

Discrete agents. There are n≥1n\ge1n≥1 agents with real opinions ξi(t)\xi_i(t)ξi​(t), t≥0t\ge0t≥0. Agents iii and jjj interact when ∣ξi−ξj∣<1|\xi_i-\xi_j|<1∣ξi​−ξj​∣<1. A solution of (2.1) is a continuous ξ:[0,∞)→Rn\xi:[0,\infty)\to\mathbb R^nξ:[0,∞)→Rn with

ξi(t)=ξi(0)+∫0t∑j: ∣ξi(τ)−ξj(τ)∣<1(ξj(τ)−ξi(τ)) dτ\xi_i(t)=\xi_i(0)+\int_0^t\sum_{j:\,|\xi_i(\tau)-\xi_j(\tau)|<1}\bigl(\xi_j(\tau)-\xi_i(\tau)\bigr)\,d\tauξi​(t)=ξi​(0)+∫0t​j:∣ξi​(τ)−ξj​(τ)∣<1∑​(ξj​(τ)−ξi​(τ))dτ

for all t≥0t\ge0t≥0 and all iii. The right-hand side is discontinuous when the interaction graph changes, so the integral form is used. A solution is proper if it is the unique solution from its initial value, its non-differentiability times have no accumulation point, and two agents that meet stay together.

Continuum agents. Agents are indexed by α∈I=[0,1]\alpha\in I=[0,1]α∈I=[0,1] with Lebesgue measure. YYY is the set of bounded measurable functions I→RI\to\mathbb RI→R. For m,M>0m,M>0m,M>0, XmMX_m^MXmM​ is the set of nondecreasing x~\tilde xx~ with m≤x~(β)−x~(α)β−α≤Mm\le\frac{\tilde x(\beta)-\tilde x(\alpha)}{\beta-\alpha}\le Mm≤β−αx~(β)−x~(α)​≤M for β≠α\beta\ne\alphaβ=α; such x~\tilde xx~ are regular. The interaction operator is

L(x~)(α)=∫I1[∣x~(α)−x~(γ)∣<1] (x~(γ)−x~(α)) dγ,\mathcal L(\tilde x)(\alpha)=\int_I \mathbf 1\bigl[|\tilde x(\alpha)-\tilde x(\gamma)|<1\bigr]\,\bigl(\tilde x(\gamma)-\tilde x(\alpha)\bigr)\,d\gamma ,L(x~)(α)=∫I​1[∣x~(α)−x~(γ)∣<1](x~(γ)−x~(α))dγ,

and a solution of (3.2) from x~0\tilde x_0x~0​ is a measurable x:(α,t)↦xt(α)x:(\alpha,t)\mapsto x_t(\alpha)x:(α,t)↦xt​(α) with every xt∈Yx_t\in Yxt​∈Y and xt(α)=x~0(α)+∫0tL(xτ)(α) dτx_t(\alpha)=\tilde x_0(\alpha)+\int_0^t\mathcal L(x_\tau)(\alpha)\,d\tauxt​(α)=x~0​(α)+∫0t​L(xτ​)(α)dτ for all t≥0t\ge0t≥0 and all α∈I\alpha\in Iα∈I.

The embedding. For ξ∈Rn\xi\in\mathbb R^nξ∈Rn, G(ξ)G(\xi)G(ξ) is the step function with G(ξ)(α)=ξiG(\xi)(\alpha)=\xi_iG(ξ)(α)=ξi​ on [i−1n,in)[\frac{i-1}n,\frac in)[ni−1​,ni​) and G(ξ)(1)=ξnG(\xi)(1)=\xi_nG(ξ)(1)=ξn​. It distributes the nnn agents over nnn blocks of III of length 1/n1/n1/n.

Formalization targets

Goal: Theorem 7 (finite-horizon approximation)

Let x~0∈XmM\tilde x_0\in X_m^Mx~0​∈XmM​, xxx the solution of (3.2) from x~0\tilde x_0x~0​, and for each n≥1n\ge1n≥1 let ξ⟨n⟩\xi^{\langle n\rangle}ξ⟨n⟩ be a proper solution of (2.1) with nondecreasing ξ⟨n⟩(0)\xi^{\langle n\rangle}(0)ξ⟨n⟩(0) and ∥G(ξ⟨n⟩(0))−x~0∥∞→0\|G(\xi^{\langle n\rangle}(0))-\tilde x_0\|_\infty\to0∥G(ξ⟨n⟩(0))−x~0​∥∞​→0. Then for every TTT and ε>0\varepsilon>0ε>0 there is n′n'n′ with

∥G(ξ⟨n⟩(t/n))−xt∥∞≤ε(t∈[0,T], n≥n′).\bigl\|G\bigl(\xi^{\langle n\rangle}(t/n)\bigr)-x_t\bigr\|_\infty\le\varepsilon\qquad(t\in[0,T],\ n\ge n').​G(ξ⟨n⟩(t/n))−xt​​∞​≤ε(t∈[0,T], n≥n′).

The statement fixes no rate in nnn and no dependence of n′n'n′ on TTT; it asserts only uniform convergence on bounded time intervals.

Milestones

  1. Lemma 1: for x~∈Xm\tilde x\in X_mx~∈Xm​ and y~∈Y\tilde y\in Yy~​∈Y, ∥L(x~)−L(y~)∥∞≤(2+8/m)∥x~−y~∥∞\|\mathcal L(\tilde x)-\mathcal L(\tilde y)\|_\infty\le(2+8/m)\|\tilde x-\tilde y\|_\infty∥L(x~)−L(y~​)∥∞​≤(2+8/m)∥x~−y~​∥∞​.
  2. Theorem 4, left inequality of (3.7): a solution from x~0∈XmM\tilde x_0\in X_m^Mx~0​∈XmM​ satisfies xt(β)−xt(α)≥me−t(β−α)x_t(\beta)-x_t(\alpha)\ge m e^{-t}(\beta-\alpha)xt​(β)−xt​(α)≥me−t(β−α) for all t≥0t\ge0t≥0, α<β\alpha<\betaα<β.
  3. Proposition 4: for every ε,T>0\varepsilon,T>0ε,T>0 there is δ>0\delta>0δ>0 such that every solution yyy of (3.2) with ∥y0−x~0∥∞≤δ\|y_0-\tilde x_0\|_\infty\le\delta∥y0​−x~0​∥∞​≤δ satisfies ∥yt−xt∥∞≤ε\|y_t-x_t\|_\infty\le\varepsilon∥yt​−xt​∥∞​≤ε on [0,T][0,T][0,T].
  4. Embedding (Section 4): if ξ\xiξ solves (2.1), then (α,t)↦G(ξ(t/n))(α)(\alpha,t)\mapsto G(\xi(t/n))(\alpha)(α,t)↦G(ξ(t/n))(α) solves (3.2) from G(ξ(0))G(\xi(0))G(ξ(0)).

Significance

The theorem says that the continuum model is the large-population limit of the nnn-agent model over any fixed time window. Combined with the paper's continuum convergence result (Theorem 6), it supports the paper's Conjecture 1 on intercluster distances for finitely many agents, and it is the first step of the paper's Proposition 5, which derives Conjecture 1 for random initial opinions from a stability conjecture for the continuum. It is a mean-field limit for a model whose interaction kernel is discontinuous, where standard Lipschitz mean-field arguments do not apply directly.

All four results and the goal are proved in the paper (with the time-scale correction described below). None of them has a machine-checked proof that this mission is aware of. The formalization contributes a checked continuous-dependence estimate for a discontinuous integral equation, a checked statement that the finite-agent dynamics embed in the continuum dynamics, and a precise record of the time normalization under which the two models agree.

Difficulty

The operator L\mathcal LL is not Lipschitz on YYY: moving one opinion across the confidence threshold changes the interaction set discontinuously. The obvious Gronwall argument for continuous dependence therefore fails for two arbitrary solutions. It works only around a trajectory that stays in some Xm′X_{m'}Xm′​, where few agents sit near the threshold, which is why the lower slope bound must hold at every time and not only at time 000. The perturbed trajectory, coming from nnn agents, is a step function and is never regular, so the estimate must be one-sided in this sense.

A literal reading of the page also fails. The page writes G(ξ⟨n⟩(t))G(\xi^{\langle n\rangle}(t))G(ξ⟨n⟩(t)), but for α\alphaα in block iii the continuum interaction L(G(ξ))(α)\mathcal L(G(\xi))(\alpha)L(G(ξ))(α) equals 1n\frac1nn1​ times the discrete right-hand side of (2.1). With x~0(α)=α/2\tilde x_0(\alpha)=\alpha/2x~0​(α)=α/2 and ξi⟨n⟩(0)=x~0(i/n)\xi^{\langle n\rangle}_i(0)=\tilde x_0(i/n)ξi⟨n⟩​(0)=x~0​(i/n), both models are linear; at t=1t=1t=1 the sup distance between G(ξ⟨n⟩(1))G(\xi^{\langle n\rangle}(1))G(ξ⟨n⟩(1)) and x1x_1x1​ tends to e−1/4e^{-1}/4e−1/4. The discrete time must be rescaled by 1/n1/n1/n.

Formalization scope

Namespace BHTOpinion.Approx. Agents of the discrete model are Fin n (0-based); the continuum index set is Set.Icc (0:ℝ) 1 with Lebesgue measure. Opinion functions are ℝ → ℝ, of which only the values on III matter; trajectories are written x t α, time first, with time in ℝ and explicit t≥0t\ge0t≥0 guards. In 0-based form, G(ξ)(α)=ξmin⁡(⌊nα⌋,n−1)G(\xi)(\alpha)=\xi_{\min(\lfloor n\alpha\rfloor,n-1)}G(ξ)(α)=ξmin(⌊nα⌋,n−1)​ on III; for n=0n=0n=0 the definition returns 000, and every statement assumes n≥1n\ge1n≥1.

Explicit readings of the paper's phrases:

  • Sup norms are written pointwise over III, including α=1\alpha=1α=1: a bound at every α∈I\alpha\in Iα∈I, never a real supremum.
  • "lim⁡n→∞∥G(ξ⟨n⟩(0))−x~0∥∞=0\lim_{n\to\infty}\|G(\xi^{\langle n\rangle}(0))-\tilde x_0\|_\infty=0limn→∞​∥G(ξ⟨n⟩(0))−x~0​∥∞​=0" is: for every δ>0\delta>0δ>0 there is NNN such that the pointwise bound δ\deltaδ holds for all n≥Nn\ge Nn≥N.
  • "There exists n′n'n′" is an explicit ∃ n′\exists\,n'∃n′ with the bound for all n≥n′n\ge n'n≥n′, t∈[0,T]t\in[0,T]t∈[0,T], α∈I\alpha\in Iα∈I.
  • "The solution xxx" of (3.2) is any solution from x~0\tilde x_0x~0​; the theorem holds for each.
  • "Proper initial condition, admitting a unique solution" is kept as printed: uniqueness from ξ⟨n⟩(0)\xi^{\langle n\rangle}(0)ξ⟨n⟩(0), finitely many non-differentiability times on every bounded interval, agents that meet stay together.
  • Solutions of (2.1) and (3.2) require the time integrand to be integrable; Lean's integral of a non-integrable function is 000.
  • The labelled correction: the discrete trajectory enters as ξ⟨n⟩(t/n)\xi^{\langle n\rangle}(t/n)ξ⟨n⟩(t/n) in the embedding claim and in Theorem 7. Equivalently, the page's statement holds for the weighted model (2.4) with weights 1/n1/n1/n; only the rescaled form is stated.
  • Only the left inequality of (3.7) is a milestone. The right inequality Me4t/mMe^{4t/m}Me4t/m is not used by Section 4.

A trivializing formalization is ruled out: the hypotheses are satisfied by x~0(α)=α∈X11\tilde x_0(\alpha)=\alpha\in X_1^1x~0​(α)=α∈X11​, the conclusion is not vacuous because GGG is evaluated at n≥1n\ge1n≥1 only, and the perturbed initial values y0y_0y0​ in Proposition 4 range over all of YYY, not over regular functions.

Infrastructure needed: Gronwall's inequality for a sup-norm difference, measure-theoretic bookkeeping for L\mathcal LL on step functions, and a change of variables τ↦τ/n\tau\mapsto\tau/nτ↦τ/n in interval integrals. The Lipschitz estimate on XmX_mXm​ and the slope bound are reusable for any continuum bounded-confidence model. Contributions to any milestone are welcome; the embedding milestone is independent of the other three.

Selected references

  • V. D. Blondel, J. M. Hendrickx, J. N. Tsitsiklis, Continuous-time average-preserving opinion dynamics with opinion-dependent communications, SIAM J. Control Optim. 48(8), 2010, 5214–5240. https://doi.org/10.1137/090766188
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