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AnalysisDynamical SystemsProbability+1·Captain: mikedeng1

Averaging Dynamics Driven by Fractional Brownian Motion: Young Solutions of dxⁿ = fₙ(t, xⁿ)dB Converge in Probability in C^α to the Solution of dx = f̄(x)dB When |fₙ − f̄|_{−κ,γ} → 0Research Paper

Why oscillating coefficients matter

An equation driven by fractional Brownian motion can respond to a rapidly varying coefficient even when that coefficient has no useful pointwise limit. Hairer and Li study this issue for fractional Brownian motion with Hurst index above one half. Their Section 3 isolates a deterministic averaging statement: if the time antiderivatives of the coefficients approach those of a limiting coefficient in a suitable negative Hölder norm, the solutions approach the limiting solution in probability. This statement supplies a common target for averaging models whose fast variables have very different origins. The authors use it later with mixing fast processes, and also present a quasi-periodic example. The result and its role in the paper are stated in Hairer and Li, Section 3.

The problem sits at the boundary of two familiar views of differential equations. A pathwise Young equation is defined from individual sufficiently regular paths, whereas the available estimates for the oscillating coefficient and the fractional Brownian driver involve probability and conditional expectation. The mission records the precise point where these descriptions meet. It treats the published article, rather than a preprint, and targets its Theorem 3.13.

Driver, coefficients, and solutions

An mmm-dimensional fractional Brownian motion B=(B1,…,Bm)B=(B^1,\ldots,B^m)B=(B1,…,Bm) with index HHH is a centered Gaussian process with independent coordinates and covariance

E[BsiBtj]=1i=j∣s∣2H+∣t∣2H−∣t−s∣2H2.\mathbb E[B_s^iB_t^j]=\mathbf1_{i=j}\frac{|s|^{2H}+|t|^{2H}-|t-s|^{2H}}2.E[Bsi​Btj​]=1i=j​2∣s∣2H+∣t∣2H−∣t−s∣2H​.

The paper works with a two-sided process and 1/2<H<11/2<H<11/2<H<1. It uses a version whose sample paths are locally β\betaβ-Hölder for every β<H\beta<Hβ<H. The mission names that version condition separately, because the covariance law alone does not select particular sample paths. The relevant past sigma algebra at time sss is generated by increments Bu−BvB_u-B_vBu​−Bv​ with u,v≤su,v\le su,v≤s. These conventions come from pp. 1826 and 1831–1832 of the article.

For a path xxx on [0,T][0,T][0,T], write ∣x∣α|x|_\alpha∣x∣α​ for its homogeneous Hölder seminorm and ∣x∣∞|x|_\infty∣x∣∞​ for its supremum norm. The norm on Cα[0,T]C^\alpha[0,T]Cα[0,T] is ∣x∣∞+∣x∣α|x|_\infty+|x|_\alpha∣x∣∞​+∣x∣α​. A Young integral ∫stfr dbr\int_s^t f_r\,db_r∫st​fr​dbr​ is the limit of left-point sums over partitions of [s,t][s,t][s,t] as the largest cell shrinks to zero. A Young solution from x0x_0x0​ is an α\alphaα-Hölder path satisfying its integral equation at every time, with value x0x_0x0​ at time zero. Here BC2BC^2BC2 means bounded, twice continuously differentiable maps with bounded derivatives through order two; Cζ,2C^{\zeta,2}Cζ,2 means ζ\zetaζ-Hölder in time with values in BC2BC^2BC2. These are the paper's conventions on pp. 1829 and 1835–1838.

The negative Hölder bound ∣f∣−κ,γ≤K|f|_{-\kappa,\gamma}\le K∣f∣−κ,γ​≤K means that the time antiderivative of fff has increments bounded by K∣t−s∣1−κK|t-s|^{1-\kappa}K∣t−s∣1−κ, and that the difference of those increments at spatial points x,yx,yx,y is bounded by K∣t−s∣1−κ∣x−y∣γK|t-s|^{1-\kappa}|x-y|^\gammaK∣t−s∣1−κ∣x−y∣γ. Both bounds apply on the time window in question when ∣t−s∣≤1|t-s|\le1∣t−s∣≤1. This is equation (3.12) in the article. It measures cancellation over time; it does not require f(t,x)f(t,x)f(t,x) itself to be small.

Formalization targets

The goal is the dBdBdB part of Theorem 3.13. Let fnf_nfn​ be Cζ,2C^{\zeta,2}Cζ,2, let the limiting fˉ\bar ffˉ​ be autonomous and in BC2BC^2BC2, and suppose ∣fn−fˉ∣−κ,γ→0|f_n-\bar f|_{-\kappa,\gamma}\to0∣fn​−fˉ​∣−κ,γ​→0. The exponents satisfy 1/2<α<H−κ1/2<\alpha<H-\kappa1/2<α<H−κ, H−κ>1/2H-\kappa>1/2H−κ>1/2, H−κ+γα>1H-\kappa+\gamma\alpha>1H−κ+γα>1, and α<ζ≤1\alpha<\zeta\le1α<ζ≤1. For Young solutions with the same starting point,

dxtn=fn(t,xtn) dBt,dxt=fˉ(xt) dBt,dx_t^n=f_n(t,x_t^n)\,dB_t,\qquad dx_t=\bar f(x_t)\,dB_t,dxtn​=fn​(t,xtn​)dBt​,dxt​=fˉ​(xt​)dBt​,

the target is

∀ε>0,P(∥xn−x∥Cα[0,T]>ε)⟶0.\forall\varepsilon>0,\qquad P\bigl(\|x^n-x\|_{C^\alpha[0,T]}>\varepsilon\bigr)\longrightarrow0.∀ε>0,P(∥xn−x∥Cα[0,T]​>ε)⟶0.

The milestone list follows the statements used around this target: the Hölder composition estimate of Lemma 2.1, the RKHS estimate of Lemma 3.3, the fractional Brownian integral estimate of Lemma 3.4, the stochastic sewing lemma of Lemma 3.5, the Young case of (3.18) from Lemmas 3.10 and 3.12, the Kolmogorov inclusions (3.24), and the deterministic stability estimate of Lemma 2.2. Each is a separate formal theorem. The authors' proofs follow their statements in Sections 2 and 3 and the Appendix; Lemma 3.5 is quoted from Lê, Theorem 2.1 without proof in the article.

What the result provides

The target gives convergence of entire solution paths in a Hölder topology, in probability. In the paper, this lets a model-specific estimate of the negative Hölder distance be used to conclude convergence of the corresponding dynamical system. Theorem A is obtained by adding such an estimate for a stationary mixing fast process; the deterministic statement here isolates the part independent of that model. These uses are described in Sections 1 and 3.

The published paper proves the result. This mission asks for machine-checked proofs of the stated Lean theorems. Its reusable work would include a pathwise Young integral over arbitrary partitions, Hölder norms that retain the value +∞+\infty+∞, a two-sided vector fractional Brownian motion interface, and stochastic estimates for time-dependent integrands. The goal and milestones in this proposal are statements with proof placeholders; the local build checks their types, not their proofs.

Main obstruction

Pointwise control of fn−fˉf_n-\bar ffn​−fˉ​ is unavailable: a rapidly oscillating function can be large at most times and still have small time antiderivatives. Applying a pathwise Young stability estimate directly to fn−fˉf_n-\bar ffn​−fˉ​ therefore leaves a coefficient norm that need not tend to zero. The integral estimate must connect cancellation measured by ∣⋅∣−κ,γ|\cdot|_{-\kappa,\gamma}∣⋅∣−κ,γ​ with LpL^pLp bounds on the driven equation. The dependence on the past of the fractional Brownian motion makes this step more delicate than an estimate for a deterministic integrand. The required estimates and their domains appear in Lemmas 3.4–3.12.

Formalization scope

Time is R\mathbb RR for the two-sided driver; coefficient and solution assertions use [0,T][0,T][0,T] with T>0T>0T>0. State spaces are finite-dimensional real Euclidean spaces. The goal takes H∈(1/2,1)H\in(1/2,1)H∈(1/2,1) from the standing setting of Section 3.1, and it assumes the locally Hölder version of BBB described on p. 1826. The solutions are required almost surely to satisfy the Young equation from the same x0x_0x0​. This requirement fixes the processes to the equations; the convergence claim cannot be obtained by choosing arbitrary paths. Probability of the norm event uses the measure of that set, and the conclusion is convergence in probability in the full CαC^\alphaCα norm.

The Lean definitions use [0,∞][0,\infty][0,∞] for path and process seminorms, so unbounded suprema are not replaced by a default real value. The negative Hölder hypothesis uses real bounds Kn→0K_n\to0Kn​→0 instead of an infimum that could be meaningless on an empty class. The Young integral quantifies over every monotone partition and the mesh limit of its left-point sums. The fBm definition includes Gaussianity, means, and every cross-coordinate covariance; its path version is explicit. Interval integrals in the coefficient bound are applied to time-continuous coefficients in the goal. Lemmas 3.4 and 3.10 use the increment filtration, the case needed for this theorem.

The paper's Lemma 2.2 needs a common initial value for its homogeneous-seminorm estimate; the formal statement includes it and records the printed issue. The paper writes the limiting coefficient with a time argument but uses an autonomous coefficient in (3.23), which the goal adopts. This proposal covers the dBdBdB equation. The final dtdtdt extension in Theorem 3.13 and the conditional-expectation estimate (3.19) remain outside its current items. Contributions that close these gaps, or supply a general conditional Wiener integral matching the article's notation, would extend the development.

Selected references

  • M. Hairer and X.-M. Li, Averaging dynamics driven by fractional Brownian motion, Annals of Probability 48(4), 2020, 1826–1860. DOI.
  • K. Lê, A stochastic sewing lemma and applications, 2018, arXiv:1810.10500, cited as [23] in Hairer and Li. arXiv.
9 thms1 active userReviewed
🏆Completed
Actuarial ScienceProbability·Captain: WillR

Actuarial Mathematics II: Term Assurance Present Values and MomentsTextbook

Motivation

An nnn-year term assurance pays a benefit if the insured person dies in one of the first nnn policy years. It can pay only once. This matters when calculating the second moment: claims in different years cannot both occur, so the cross-products between them are zero.

Actuarial Mathematics I established finite expected present values, second moments and variances for general collections of contingent payments. This mission applies those results to one life and a fixed-term death benefit. It proves the familiar term-assurance formulas from reusable death-year events, rather than treating them as isolated actuarial notation.

Mathematical setting

Let (Ω,F,P)(\Omega,\mathcal F,P)(Ω,F,P) be a probability space and let K:Ω→NK:\Omega\to\mathbb NK:Ω→N be a measurable curtate future lifetime: the number of complete future years lived before death. For k∈Nk\in\mathbb Nk∈N, define the event of death during policy year k+1k+1k+1 by

Dk={ω∈Ω:K(ω)=k}.D_k=\{\omega\in\Omega:K(\omega)=k\}.Dk​={ω∈Ω:K(ω)=k}.

Each event DkD_kDk​ is measurable. The events are pairwise disjoint: if i≠ji\ne ji=j, then Di∩Dj=∅D_i\cap D_j=\varnothingDi​∩Dj​=∅.

Fix a policy term n∈Nn\in\mathbb Nn∈N and a constant annual discount factor vvv. A unit benefit is payable at time k+1k+1k+1 if death occurs during year k+1k+1k+1, for 0≤k<n0\leq k<n0≤k<n. Its random present value is

Zn(ω)=∑k=0n−1vk+11Dk(ω).Z_n(\omega)=\sum_{k=0}^{n-1}v^{k+1}\mathbf1_{D_k}(\omega).Zn​(ω)=k=0∑n−1​vk+11Dk​​(ω).

When n=0n=0n=0, the sum is zero. The implementation uses the previously published `ActuarialValuation.presentValue` definition with the schedule of death-year events, reusing the general valuation machinery. The theorem statements allow any real vvv, so the finite algebra also holds beyond the economic setting 0<v≤10<v\leq10<v≤1. The positive discount factors customary in the source are a special case.

Main theorem

The capstone proves these three identities together.

Expected present value:

EP[Zn]=∑k=0n−1vk+1P(Dk).\mathbb E_P[Z_n]=\sum_{k=0}^{n-1}v^{k+1}P(D_k).EP​[Zn​]=k=0∑n−1​vk+1P(Dk​).

Second moment:

EP[Zn2]=∑k=0n−1v2(k+1)P(Dk).\mathbb E_P[Z_n^2]=\sum_{k=0}^{n-1}v^{2(k+1)}P(D_k).EP​[Zn2​]=k=0∑n−1​v2(k+1)P(Dk​).

Variance:

Var⁡P(Zn)=∑k=0n−1v2(k+1)P(Dk)−(∑k=0n−1vk+1P(Dk))2.\operatorname{Var}_P(Z_n)= \sum_{k=0}^{n-1}v^{2(k+1)}P(D_k) -\left(\sum_{k=0}^{n-1}v^{k+1}P(D_k)\right)^2.VarP​(Zn​)=k=0∑n−1​v2(k+1)P(Dk​)−(k=0∑n−1​vk+1P(Dk​))2.

The second-moment simplification comes from the mutual exclusivity of distinct death-year events, not from independence. In the general double sum from Actuarial Mathematics I, every off-diagonal intersection of death-year events is empty, leaving a single sum.

Formalisation milestones

The milestones proceed from measurability of each death-year event to disjointness across years, vanishing products of distinct death-year indicators, the finite present-value representation, the expected value, the second moment and the variance. The proposal gives each mathematical statement and Lean target type separately. The capstone combines the three moment identities for the same KKK, vvv, nnn and PPP.

The project uses the existing `ActuarialValuation` namespace and imports published Mission I results where they apply. All dates are annual, and benefits are payable at the end of the year of death. Multiple lives, benefits payable immediately on death, stochastic discounts, select-life models and whole-of-life infinite sums are outside the scope of this capstone.

Why these results matter

A complete proof provides a reusable one-life mortality event model and a verified finite-term insurance valuation formula. The model can support a later mission on pure endowments and endowment assurances, where survival-to-term events complement death-in-term events, and another on temporary annuities, where survival events are nested rather than disjoint.

The results also make it straightforward to compare the traditional actuarial single-sum variance formula with the general dependent-cashflow theorem proved in Mission I.

Source and scope

The main mathematical source is Life Contingencies: The Mathematics, Statistics, and Economics of Life Insurance, Chapter 2 §2.4.3 for curtate future lifetime, Chapter 3 §3.1.1 equation (3.4) for disjoint-event moments, and §3.2.2 equation (3.8) for term-assurance present value, mean and variance.

  • https://openacttextdev.github.io/LifeCon/C-ModelingLifeTimes.html
  • https://openacttextdev.github.io/LifeCon/C-SimpleBenefit.html
  • https://actuaries.org.uk/media/yfnkmkbq/cm1_syllabus-2026-_final-proof.pdf (CM1 2026, life-contingency valuation objectives)
  • Actuarial Mathematics I: Present Values of Contingent Cashflows

These established actuarial formulas are not new mathematical conjectures. The contribution is a precise formal link in Lean from a curtate-lifetime model to the general contingent-payment valuation layer.

Formalisation challenges

The death-year set must be shown measurable from the measurability of KKK. The disjointness arguments must also cover degenerate cases such as n=0n=0n=0. The generic second-moment theorem uses an ordered double sum. The proof must remove only terms justified by Di∩Dj=∅D_i\cap D_j=\varnothingDi​∩Dj​=∅, retain the diagonal terms and use the correct end-of-year exponent k+1k+1k+1.

All formal declarations are written for Prove2Me's pinned Mathlib revision `0df444a360eaa60ab8c11dca51a86af692955474`. No local Lean compiler is used. Any private preflight compilation, if needed, is performed through Prove2Me's remote system.

15 thms1 active userReviewed
Computational GeometryLinear algebraMachine Learning·Captain: mikedeng1

Turning Big Data into Tiny Data: Constant-Size Coresets for k-Means, PCA, and Projective Clustering II: An SVD Coreset of at Most 2(j + ⌈j/ε⌉ − 1) Weighted Points for Affine j-SubspacesResearch Paper

Motivation

Principal component analysis (PCA) asks for the jjj-dimensional affine subspace that best fits a cloud of nnn points in Rd\mathbb R^dRd in the least-squares sense. When nnn is very large, or the points arrive as a stream or are spread over many machines, one wants to replace the data by a small summary on which the cost of every candidate subspace can still be evaluated, up to a factor 1+ε1+\varepsilon1+ε. Such a summary is a coreset. Coresets for the jjj-subspace problem are the building block of the streaming and distributed PCA and projective clustering algorithms of Feldman, Schmidt and Sohler (SIAM J. Comput. 49(3), 2020), whose sizes depend on jjj and ε\varepsilonε only, not on nnn or ddd.

For linear subspaces (through the origin) the paper's Theorem 17 gives a deterministic coreset of m=O(j/ε)m=O(j/\varepsilon)m=O(j/ε) points read off the singular value decomposition. Data are rarely centred, though, and subtracting the mean before the computation does not survive the union of coresets with different means (p. 616). Section 4 of the paper repairs this: Theorem 19 gives a coreset for affine jjj-subspaces whose points already carry the mean, at the price of doubling the size and weighting the points. This mission formalizes Theorem 19.

Setting

A data set of nnn points in Rd\mathbb R^dRd is a matrix A∈Rn×dA\in\mathbb R^{n\times d}A∈Rn×d whose rows Ai∗A_{i*}Ai∗​ are the points. For a nonempty set C⊆RdC\subseteq\mathbb R^dC⊆Rd and a point ppp, dist⁡(p,C)=inf⁡c∈C∥p−c∥2\operatorname{dist}(p,C)=\inf_{c\in C}\|p-c\|_2dist(p,C)=infc∈C​∥p−c∥2​. The cost of CCC is

dist⁡2(A,C)=∑i=1ndist⁡2(Ai∗,C),\operatorname{dist}^2(A,C)=\sum_{i=1}^n\operatorname{dist}^2(A_{i*},C),dist2(A,C)=i=1∑n​dist2(Ai∗​,C),

and for weights w1,…,wr≥0w_1,\ldots,w_r\ge0w1​,…,wr​≥0 on the rows of S∈Rr×dS\in\mathbb R^{r\times d}S∈Rr×d the weighted cost is ∑iwidist⁡2(Si∗,C)\sum_i w_i\operatorname{dist}^2(S_{i*},C)∑i​wi​dist2(Si∗​,C). The squared Frobenius norm is ∥M∥F2=∑i,kMik2\|M\|_F^2=\sum_{i,k}M_{ik}^2∥M∥F2​=∑i,k​Mik2​.

A singular value decomposition (SVD) of AAA is a factorization A=UΣVTA=U\Sigma V^TA=UΣVT with U∈Rn×nU\in\mathbb R^{n\times n}U∈Rn×n and V∈Rd×dV\in\mathbb R^{d\times d}V∈Rd×d orthogonal and Σ∈Rn×d\Sigma\in\mathbb R^{n\times d}Σ∈Rn×d rectangular diagonal with nonnegative, nonincreasing diagonal entries σ1≥σ2≥⋯\sigma_1\ge\sigma_2\ge\cdotsσ1​≥σ2​≥⋯. Σ(m)\Sigma^{(m)}Σ(m) keeps the first mmm diagonal entries and sets the rest to 000; the mmm-rank approximation is A(m)=UΣ(m)VTA^{(m)}=U\Sigma^{(m)}V^TA(m)=UΣ(m)VT (Definition 1).

The mean row is μ(A)=1n∑iAi∗\mu(A)=\frac1n\sum_iA_{i*}μ(A)=n1​∑i​Ai∗​ and the centred matrix is A′=A−1⋅μ(A)A'=A-\mathbb 1\cdot\mu(A)A′=A−1⋅μ(A), whose rows are Ai∗−μ(A)A_{i*}-\mu(A)Ai∗​−μ(A).

Algorithm 1, subspace-Coreset(A,j,ε)(A,j,\varepsilon)(A,j,ε), sets m=min⁡{n,d,j+⌈j/ε⌉−1}m=\min\{n,d,j+\lceil j/\varepsilon\rceil-1\}m=min{n,d,j+⌈j/ε⌉−1}, returns the matrix SSS of the first mmm rows of Σ(m)VT\Sigma^{(m)}V^TΣ(m)VT (all other rows are zero), the weights wi=1w_i=1wi​=1, and Δ=∥A−A(m)∥F2\Delta=\|A-A^{(m)}\|_F^2Δ=∥A−A(m)∥F2​.

Algorithm 2, affine-jjj-subspace-Coreset(A,j,ε)(A,j,\varepsilon)(A,j,ε), runs Algorithm 1 on A′A'A′, obtaining (S′,Δ)(S',\Delta)(S′,Δ) with m=∣S′∣m=|S'|m=∣S′∣, and returns

S=1⋅μ(A)+mn⋅[S′−S′]∈R2m×d,w=(n2m,…,n2m),S=\mathbb 1\cdot\mu(A)+\sqrt{\frac mn}\cdot\begin{bmatrix}S'\\-S'\end{bmatrix}\in\mathbb R^{2m\times d},\qquad w=\Bigl(\frac n{2m},\ldots,\frac n{2m}\Bigr),S=1⋅μ(A)+nm​​⋅[S′−S′​]∈R2m×d,w=(2mn​,…,2mn​),

together with Δ\DeltaΔ.

Formalization targets

Goal: Theorem 19 (p. 617)

Let n≥1n\ge1n≥1, j∈[1,d−1]j\in[1,d-1]j∈[1,d−1] and ε>0\varepsilon>0ε>0, and let (S,Δ,w)(S,\Delta,w)(S,Δ,w) be the output of Algorithm 2 for any SVD of A′A'A′. Then S∈R(2m)×dS\in\mathbb R^{(2m)\times d}S∈R(2m)×d, m≤j+⌈j/ε⌉−1m\le j+\lceil j/\varepsilon\rceil-1m≤j+⌈j/ε⌉−1, Δ≥0\Delta\ge0Δ≥0, and for every affine jjj-dimensional subspace CCC of Rd\mathbb R^dRd,

dist⁡2(A,C)≤∑i=12mwidist⁡2(Si∗,C)+Δ≤(1+ε)dist⁡2(A,C).\operatorname{dist}^2(A,C)\le\sum_{i=1}^{2m}w_i\operatorname{dist}^2(S_{i*},C)+\Delta\le(1+\varepsilon)\operatorname{dist}^2(A,C).dist2(A,C)≤i=1∑2m​wi​dist2(Si∗​,C)+Δ≤(1+ε)dist2(A,C).

Milestones

  1. Theorem 17 (p. 615): for any SVD of AAA, the output of Algorithm 1 satisfies dist⁡2(A,L)≤∑i=1mdist⁡2(Si∗,L)+Δ≤(1+ε)dist⁡2(A,L)\operatorname{dist}^2(A,L)\le\sum_{i=1}^m\operatorname{dist}^2(S_{i*},L)+\Delta\le(1+\varepsilon)\operatorname{dist}^2(A,L)dist2(A,L)≤∑i=1m​dist2(Si∗​,L)+Δ≤(1+ε)dist2(A,L) for every jjj-dimensional linear subspace LLL.
  2. Lemma 18 (p. 616): if μ(M)=0⃗\mu(M)=\vec0μ(M)=0, LLL is a linear jjj-subspace and t∈L⊥t\in L^\perpt∈L⊥, then dist⁡2(M,t+L)=dist⁡2(M,L)+n∥t∥2\operatorname{dist}^2(M,t+L)=\operatorname{dist}^2(M,L)+n\|t\|^2dist2(M,t+L)=dist2(M,L)+n∥t∥2.
  3. Display (7) (p. 618): with S′′=m/n [S′;−S′]S''=\sqrt{m/n}\,[S';-S']S′′=m/n​[S′;−S′], dist⁡2(A′,L)≤n2mdist⁡2(S′′,L)+Δ≤(1+ε)dist⁡2(A′,L)\operatorname{dist}^2(A',L)\le\frac n{2m}\operatorname{dist}^2(S'',L)+\Delta\le(1+\varepsilon)\operatorname{dist}^2(A',L)dist2(A′,L)≤2mn​dist2(S′′,L)+Δ≤(1+ε)dist2(A′,L) for every linear jjj-subspace LLL.

Theorem 17 rests on Corollary 16 and Claim 3 of the paper; those are milestones of the companion mission Turning Big Data into Tiny Data … I and are not posed again here.

Significance

The result. Theorem 19 gives a deterministic summary of 2m≤2(j+⌈j/ε⌉−1)2m\le2(j+\lceil j/\varepsilon\rceil-1)2m≤2(j+⌈j/ε⌉−1) weighted points and one scalar that preserves the cost of every affine jjj-subspace within 1+ε1+\varepsilon1+ε, for arbitrary data, with no assumption on the mean. Because its points carry the mean, coresets of different data sets can be merged, which the merge-and-reduce streaming constructions of the paper's later sections need. Any (1+ε′)(1+\varepsilon')(1+ε′)-approximate PCA solution computed on the coreset is then a (1+ε)(1+ε′)(1+\varepsilon)(1+\varepsilon')(1+ε)(1+ε′)-approximate solution for the full data.

Formalizing it. The theorem is proved in the paper; no machine-checked proof of it, or of any coreset theorem, exists on the platform. A complete development would produce the cost identities for sums of squared distances to linear and affine subspaces in Lean, the effect of centring and orthogonal translation on these costs, and the use of the SVD truncation as a summary, all of which are reusable for other PCA, low-rank approximation and projective clustering results.

Difficulty

The obvious construction, centring the data, computing the linear coreset of the centred data and adding the mean back, fails: the linear coreset S′S'S′ need not have mean 0⃗\vec00, and translating a subspace by t⊥Lt\perp Lt⊥L changes the cost of a point set by a multiple of ∥t∥2\|t\|^2∥t∥2 that depends on the number of points (p. 617). The paper's construction has to match both the mean and the total weight of the original data while keeping the linear-subspace guarantee, and the formal proof has to carry this through the reduction of an arbitrary affine subspace to a linear one plus an orthogonal translation. Beneath it lies Theorem 17, which needs the SVD-based estimate of the companion mission (Corollary 16) and the passage from the nnn-row matrix A(m)=UΣ(m)VTA^{(m)}=U\Sigma^{(m)}V^TA(m)=UΣ(m)VT to the mmm nonzero rows of Σ(m)VT\Sigma^{(m)}V^TΣ(m)VT. Distances to subspaces in Lean are infima over sets, so the identities dist⁡2(A,L)=∥AY∥F2\operatorname{dist}^2(A,L)=\|AY\|_F^2dist2(A,L)=∥AY∥F2​ for an orthonormal basis YYY of L⊥L^\perpL⊥ must themselves be established.

Formalization scope

  • Representation. Points are rows of Matrix (Fin n) (Fin d) ℝ, read as points of EuclideanSpace ℝ (Fin d). dist⁡\operatorname{dist}dist is Metric.infDist. Linear jjj-subspaces are Submodules of finrank jjj; affine ones are AffineSubspaces whose direction has finrank jjj, and t+Lt+Lt+L is AffineSubspace.mk' t L. The SVD and A(m)A^{(m)}A(m) are the published ProjLikeRetr.FixedRank.IsSVD and truncSVD. Every statement holds for an arbitrary SVD; none is chosen.
  • Pinned hypotheses and readings.
    1. The page's "Δ>0\Delta>0Δ>0" (Theorems 17 and 19) is false when rank⁡A′≤m\operatorname{rank}A'\le mrankA′≤m, for instance when all points coincide; the statements claim Δ≥0\Delta\ge0Δ≥0.
    2. n≥1n\ge1n≥1 is added to Theorem 19 and (7), since Algorithm 2 divides by nnn.
    3. "subspace-Coreset(P,j,ε)(P,j,\varepsilon)(P,j,ε)" is read with P=AP=AP=A.
    4. Theorem 17's S∈Rm×dS\in\mathbb R^{m\times d}S∈Rm×d is the first mmm rows of Σ(m)VT\Sigma^{(m)}V^TΣ(m)VT, as the text before it says, although Algorithm 1, line 3 writes the whole matrix.
    5. Lemma 18's "affine jjj-dimensional subspace LLL" is a linear subspace: the lemma uses L⊥L^\perpL⊥, and the proof of Theorem 19 applies it to linear LLL.
    6. Theorem 19's affine subspace CCC is also required to be nonempty; this follows from j≥1j\ge1j≥1 and guards against Mathlib's convention that the distance to ∅\emptyset∅ is 000.
  • Conventions. m≤j+⌈j/ε⌉−1m\le j+\lceil j/\varepsilon\rceil-1m≤j+⌈j/ε⌉−1 is written m+1≤j+⌈j/ε⌉m+1\le j+\lceil j/\varepsilon\rceilm+1≤j+⌈j/ε⌉. Diagonal positions of Σ\SigmaΣ are 0-based in Lean. The 2m2m2m output rows are μ+m/n Si∗′\mu+\sqrt{m/n}\,S'_{i*}μ+m/n​Si∗′​ followed by μ−m/n Si∗′\mu-\sqrt{m/n}\,S'_{i*}μ−m/n​Si∗′​. Weights are the real number n/(2m)n/(2m)n/(2m) with m=∣S′∣m=|S'|m=∣S′∣, not the cap j+⌈j/ε⌉−1j+\lceil j/\varepsilon\rceil-1j+⌈j/ε⌉−1.
  • Not trivializable. The goal quantifies over affine, not linear, subspaces; the coreset is built from an SVD of the centred matrix A′A'A′ and Δ\DeltaΔ is the residual of A′A'A′, so neither the mean nor the centring can be dropped; and no hypothesis is vacuous (any data matrix with any of its SVDs satisfies them).
  • Not formalized. The running-time clauses ("O(min⁡{nd2,dn2})O(\min\{nd^2,dn^2\})O(min{nd2,dn2}) time") and §4.1 (weighted inputs).
  • Welcome contributions. Lemmas computing dist⁡2\operatorname{dist}^2dist2 to subspaces via orthogonal projections, invariance of these costs under orthogonal maps, and the cost identity for symmetric point sets.

Selected references

  • D. Feldman, M. Schmidt, C. Sohler, Turning Big Data into Tiny Data: Constant-Size Coresets for k-Means, PCA, and Projective Clustering, SIAM J. Comput. 49(3):601–657, 2020. https://doi.org/10.1137/18M1209854
  • P.-A. Absil, J. Malick, Projection-like Retractions on Matrix Manifolds, SIAM J. Optim. 22(1):135–158, 2012 (source of the published SVD definition used here). https://doi.org/10.1137/100802529
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Bandit AlgorithmsMachine LearningProbability+1·Captain: mikedeng1

The Multi-Armed Bandit Problem with Covariates II: Adaptively Binned Successive Elimination Has Regret at Most Cn(K log K/n)^{β(α+1)/(2β+d)} Under Smoothness and Margin ConditionsResearch Paper

Motivation

An online decision maker often sees information about a customer, patient, or request before choosing an action. A bandit with covariates models this setting when the reward of every available action is initially unknown and only the reward of the chosen action is observed. A method must learn which action works best for which covariates while paying for exploratory choices. Perchet and Rigollet studied this problem for smooth reward functions and measured how quickly a policy can approach the performance of an oracle that knows every arm's mean reward Perchet and Rigollet, 2013.

A fixed grid divides the covariate space at one resolution everywhere. It can spend pulls distinguishing arms in regions where their difference is already large, while leaving too few observations in regions where they are close. Adaptively binned successive elimination (ABSE) instead refines a region only while several arms remain plausible there. The paper proves a regret rate controlled jointly by the smoothness of the reward functions and the probability of encountering near ties. Its Theorem 5.1 is the target of this mission.

Setting

There are K≥2K\ge2K≥2 arms and covariates XtX_tXt​ in the unit cube X=[0,1]d⊂Rd\mathcal X=[0,1]^d\subset\mathbb R^dX=[0,1]d⊂Rd, with d≥1d\ge1d≥1. At time ttt, the policy sees XtX_tXt​, chooses an arm, and sees that arm's reward. The random vectors consisting of the covariate and all potential arm rewards are independent across times. Covariates have a common probability law PXP_XPX​ with a density between constants 0<c‾≤c‾0<\underline c\le\overline c0<c​≤c. Every reward lies in [0,1][0,1][0,1]; for arm iii its conditional mean given Xt=xX_t=xXt​=x is f(i)(x)∈[0,1]f^{(i)}(x)\in[0,1]f(i)(x)∈[0,1]. The paper does not require the complete reward vectors to be identically distributed across time. These conventions come from §3.1, pp. 10–11.

At xxx, write f∗(x)=max⁡if(i)(x)f^*(x)=\max_i f^{(i)}(x)f∗(x)=maxi​f(i)(x). Write f♯(x)f^\sharp(x)f♯(x) for the largest mean strictly below f∗(x)f^*(x)f∗(x), and set f♯(x)=f∗(x)f^\sharp(x)=f^*(x)f♯(x)=f∗(x) when every arm ties. The difference f∗(x)−f♯(x)f^*(x)-f^\sharp(x)f∗(x)−f♯(x) is the positive gap wherever a genuinely suboptimal arm exists. The smoothness condition requires ∣f(i)(x)−f(i)(x′)∣≤L∥x−x′∥β|f^{(i)}(x)-f^{(i)}(x')|\le L\|x-x'\|^\beta∣f(i)(x)−f(i)(x′)∣≤L∥x−x′∥β for every arm, with the Euclidean norm, 0<β≤10<\beta\le10<β≤1, and L>0L>0L>0. The margin condition, with α>0\alpha>0α>0, 0<δ0<10<\delta_0<10<δ0​<1, and C0>0C_0>0C0​>0, says

PX{0<f∗(X)−f♯(X)≤δ}≤C0δα(0≤δ≤δ0).P_X\{0<f^*(X)-f^\sharp(X)\le\delta\}\le C_0\delta^\alpha\qquad(0\le\delta\le\delta_0).PX​{0<f∗(X)−f♯(X)≤δ}≤C0​δα(0≤δ≤δ0​).

These are the assumptions defining the paper's class MXK(α,β,L)\mathcal M^K_{\mathcal X}(\alpha,\beta,L)MXK​(α,β,L) §3.2, pp. 12–13.

ABSE starts with the whole cube. Each live dyadic cell runs a copy of successive elimination on its inherited arms. One round pulls each remaining arm once. After a complete round, an arm is eliminated if its empirical mean falls more than twice the radius U(s,n∣B∣d)U(s,n|B|^d)U(s,n∣B∣d) below the largest empirical mean, where ∣B∣|B|∣B∣ is the cell's side length and UUU uses log⁡‾(x)=max⁡{log⁡x,1}\overline{\log}(x)=\max\{\log x,1\}log​(x)=max{logx,1}. The cell splits after its specified stopping round if it has at least two active arms and is below the maximum depth k0k_0k0​. Each child receives the survivors. The policy takes d,β,L,K,nd,\beta,L,K,nd,β,L,K,n as parameters and uses the current covariate and rewards it actually observed Policy 3, p. 22.

Formalization targets

Goal: Theorem 5.1, finite margin exponent

The goal is the finite-α\alphaα part of Theorem 5.1, p. 22. Fix d≥1d\ge1d≥1, 0<β≤10<\beta\le10<β≤1, L>0L>0L>0, α>0\alpha>0α>0 with αβ≤d\alpha\beta\le dαβ≤d, 0<δ0<10<\delta_0<10<δ0​<1, C0>0C_0>0C0​>0 and 0<c‾≤c‾0<\underline c\le\overline c0<c​≤c. There is one constant C>0C>0C>0, depending on these parameters but not on KKK, nnn or the machine, such that for every K≥2K\ge2K≥2, every n≥Klog⁡Kn\ge K\log Kn≥KlogK and every machine of the class,

ERn(π~)≤Cn(Klog⁡Kn)β(α+1)2β+d.\mathbb E R_n(\widetilde\pi)\le Cn\left(\frac{K\log K}{n}\right)^{\frac{\beta(\alpha+1)}{2\beta+d}}.ERn​(π)≤Cn(nKlogK​)2β+dβ(α+1)​.

Here π~\widetilde\piπ is ABSE and RnR_nRn​ is its cumulative regret against an arm of maximum conditional mean at each covariate. The goal asserts the shape of the rate with an unspecified constant, which is the paper's form.

Milestones

In attack order:

  1. Lemma A.1 (p. 28): a maximal Hoeffding–Azuma inequality, P{∃t≤T:Zˉt≥2(b−a)2t−1log⁡(4T/(δt))}≤δ\mathbb P\{\exists t\le T:\bar Z_t\ge\sqrt{2(b-a)^2t^{-1}\log(4T/(\delta t))}\}\le\deltaP{∃t≤T:Zˉt​≥2(b−a)2t−1log(4T/(δt))​}≤δ for bounded martingale differences.
  2. (5.3) (p. 21): ℓB≤Cℓ∣B∣−2β log⁡‾(n∣B∣2β+d)\ell_B\le C_\ell|B|^{-2\beta}\,\overline{\log}(n|B|^{2\beta+d})ℓB​≤Cℓ​∣B∣−2βlog​(n∣B∣2β+d), the number of rounds a cell spends before it may split.
  3. (5.10) (p. 26): if arm iii has gap above 8c0∣B∣β8c_0|B|^\beta8c0​∣B∣β at a point of BBB, then the cell mean of the arm ıˇ\check\imathˇ that is best at that point exceeds the cell mean of iii by at least 32εB,ℓB\tfrac32\varepsilon_{B,\ell_B}23​εB,ℓB​​.
  4. The display before (5.6) (p. 25): ∑∣B∣=2−kqB≤c22k(d−βα)\sum_{|B|=2^{-k}}q_B\le c_2 2^{k(d-\beta\alpha)}∑∣B∣=2−k​qB​≤c2​2k(d−βα), where qBq_BqB​ is the conditional probability of a near tie inside BBB.
  5. (5.5) (p. 24): the pathwise decomposition rnborn(B)=rnlive(B)+∑B′∈burst(B)rnborn(B′)r_n^{\mathrm{born}}(B)=r_n^{\mathrm{live}}(B)+\sum_{B'\in\mathrm{burst}(B)}r_n^{\mathrm{born}}(B')rnborn​(B)=rnlive​(B)+∑B′∈burst(B)​rnborn​(B′) of regret along the tree.
  6. Theorem 5.1, α=∞\alpha=\inftyα=∞ (p. 22): when the margin region {0<f⋆−f♯≤δ0}\{0<f^\star-f^\sharp\le\delta_0\}{0<f⋆−f♯≤δ0​} has probability zero, ERn(π~)≤CKlog⁡n\mathbb E R_n(\widetilde\pi)\le CK\log nERn​(π)≤CKlogn.

Significance

The result provides a performance guarantee for a policy that adapts its spatial resolution to observed evidence, under a class of nonparametric reward functions. It permits a direct comparison with a fixed-bin policy under the same smoothness and margin conditions. The paper proves the rate and discusses optimality in a minimax sense when K=2K=2K=2 §5, pp. 22–27. This mission asks for a machine-checked proof of the stated finite-α\alphaα regime; the Lean goal and milestones are currently open statements, so the paper's proof is the mathematical source rather than a completed formal proof.

A completed development would make the stochastic model, adaptive policy, cell geometry, and concentration estimates reusable for other contextual bandit analyses.

Difficulty

The main difficulty is the feedback loop between decisions and observations. A cell receives samples only when the covariate lands there, and its available arms depend on eliminations in its ancestors. Applying an ordinary concentration inequality to a fixed sequence of arm rewards does not by itself justify the bound at these random birth and stopping times. The formal proof must track the inherited active sets and the samples collected after each birth, then combine local error bounds across the tree. The appendix's maximal inequality controls a range of round counts; the regret argument also uses the small probability of covariates with nearly tied arm means §5, pp. 23–27 and Lemma A.1, p. 28.

Formalization scope

Lean uses EuclideanSpace ℝ (Fin d) and a probability measure on its unit cube. The lower density bound ensures every valid dyadic cell has positive probability, so its conditional mean is defined by a real quotient. A consistent half-open boundary assignment turns the paper's cells, which are specified up to Lebesgue-null boundaries, into a partition on every path. The policy is a recursive state machine: at time ttt it receives XtX_tXt​, chooses an arm from its prior state, and updates with only the reward of that arm. It does not receive the unknown means or any unobserved potential reward. The existential constant in the goal is quantified before KKK, nnn, the sample space, and the machine.

The finite-α\alphaα goal includes αβ≤d\alpha\beta\le dαβ≤d. The printed theorem omits it, although the proof uses it. Without it, a two-arm machine with constant means 111 and 000 has regret from the policy's first exploratory round, while the printed bound tends to zero when α\alphaα is large. The α=∞\alpha=\inftyα=∞ clause reads the margin condition as PX(0<f⋆−f♯≤δ0)=0P_X(0<f^\star-f^\sharp\le\delta_0)=0PX​(0<f⋆−f♯≤δ0​)=0, the limit of C0δαC_0\delta^\alphaC0​δα for δ<1\delta<1δ<1, because the page does not define it. The (5.3) milestone uses log⁡‾\overline{\log}log​: the printed ordinary logarithm can be nonpositive at a finest cell, while the left side is a positive integer. The cell parameter TB=n∣B∣dT_B=n|B|^dTB​=n∣B∣d and bursting after a full round follow Policy 3 and the proof where nearby prose or pseudocode differs. Lemma A.1 adds EZ1=0\mathbb EZ_1=0EZ1​=0 and a<ba<ba<b, both implicit on the page. The constants c2c_2c2​ and CℓC_\ellCℓ​ are existential and placed after the class parameters, because the page's explicit c2=c1α/c‾c_2=c_1^\alpha/\underline cc2​=c1α​/c​ omits the margin constant C0C_0C0​.

The probabilistic error displays (5.6)–(5.9) and (5.11)–(5.14) are not milestones. They are statements about the events AB={I‾B⊆IB⊆IˉB}\mathcal A_B=\{\underline{\mathcal I}_B\subseteq\mathcal I_B\subseteq\bar{\mathcal I}_B\}AB​={I​B​⊆IB​⊆IˉB​} and GB\mathcal G_BGB​, which the page leaves undefined for cells that are never born or never finish ℓB\ell_BℓB​ rounds. The decomposition (5.8) also leaves out arms of I‾B\underline{\mathcal I}_BI​B​ that were eliminated at an ancestor of BBB. A faithful encoding of these events is welcome as a contribution.

A complete proof needs measurable recursive policies, conditional expectations and independence, dyadic-cell volume and nesting facts, concentration for arm observations at adaptive times, and sums over tree depths. Contributions establishing these interfaces and the paper's intermediate bounds are welcome. The result must apply to every machine in the stated class. Each of the following would change the theorem: a policy that reads the unknown f(i)f^{(i)}f(i) or unobserved rewards (the oracle has zero regret), a constant chosen after the machine, a covariate law that is not a probability measure on the cube, Hölder continuity in the sup norm instead of the Euclidean norm, or dropping the density lower bound (cells of zero mass would make fˉB\bar f_Bfˉ​B​ a junk value). The paper's proofs are in §5 (pp. 23–27) and its Appendix (p. 28).

Selected references

  • Jean-Yves Audibert and Alexandre B. Tsybakov, Fast learning rates for plug-in classifiers, Annals of Statistics 35(2):608–633, 2007, DOI:10.1214/009053606000001217.
  • Eyal Even-Dar, Shie Mannor and Yishay Mansour, Action elimination and stopping conditions for the multi-armed bandit and reinforcement learning problems, Journal of Machine Learning Research 7:1079–1105, 2006, jmlr.org/papers/v7/evendar06a.
  • Philippe Rigollet and Assaf Zeevi, Nonparametric bandits with covariates, COLT 2010, pp. 54–66, arXiv:1003.1630.
  • Vianney Perchet and Philippe Rigollet, The multi-armed bandit problem with covariates, Annals of Statistics 41(2):693–721, 2013, pinned arXiv:1110.6084v3, DOI:10.1214/13-AOS1101.
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🏆Completed
Actuarial ScienceProbability·Captain: WillR

Actuarial Mathematics I: Present Values of Contingent CashflowsTextbook

Motivation

Life insurers and pension schemes promise cashflows whose payment depends on future events. A term assurance pays if the insured dies within a stated period. A pension pays when a member survives to an instalment date. A contingent survivor pension may continue after the member dies. These liabilities differ in the events triggering payment, but share one mathematical operation: discount the amounts payable and aggregate them to obtain a random present value. Expected present value is used in premium setting and liability valuation, while the second moment and variance quantify how much the discounted liability can vary.

The open textbook Life Contingencies: The Mathematics, Statistics, and Economics of Life Insurance, Chapter 3, §3.1, introduces uncertain discounted cashflows using indicators, and derives their expected values in equation (3.3). Its treatment also distinguishes independent indicators from indicators connected through death or survival. This mission establishes a finite-horizon generalisation of those identities that handles arbitrary dependencies among payment-triggering events.

Setting

Fix a measurable sample space (Ω,F)(\Omega,\mathcal F)(Ω,F) with a probability measure PPP. A finite set III indexes distinct payment obligations. Each obligation i∈Ii\in Ii∈I has a non-negative integer payment date ti∈Nt_i\in\mathbb Nti​∈N, a deterministic cashflow amount ci∈Rc_i\in\mathbb Rci​∈R, and a measurable event Ai∈FA_i\in\mathcal FAi​∈F that triggers payment. The deterministic discount function d:N→Rd:\mathbb N\to\mathbb Rd:N→R assigns a multiplier to each date. Write 1Ai(ω)\mathbf 1_{A_i}(\omega)1Ai​​(ω) for the real-valued event indicator, equal to one on AiA_iAi​ and zero otherwise.

The random present value is

Z(ω)=∑i∈Id(ti)ci1Ai(ω).Z(\omega)=\sum_{i\in I}d(t_i)c_i\mathbf 1_{A_i}(\omega).Z(ω)=i∈I∑​d(ti​)ci​1Ai​​(ω).

The same date can support multiple obligations with distinct contingencies, such as member and survivor payments, pension tranches and expenses. The index distinguishes obligations even when their payment times coincide. Amounts may be positive, zero or negative and triggering events can be mutually exclusive, nested, independent or arbitrarily dependent. Finite schedules also allow no obligations. Each present value is bounded and has finite first and second moments because the schedule is finite, amounts are deterministic real numbers, and indicators are bounded.

Formalisation targets

The capstone theorem proves the expected present value, second moment and variance identities for the same random variable ZZZ. The expected present value is

EP[Z]=∑i∈Id(ti)ciP(Ai).\mathbb E_P[Z]=\sum_{i\in I}d(t_i)c_iP(A_i).EP​[Z]=i∈I∑​d(ti​)ci​P(Ai​).

The second moment retains all dependence terms, including pairs of different obligations payable on the same date:

EP[Z2]=∑i∈I∑j∈Id(ti)ci d(tj)cj P(Ai∩Aj).\mathbb E_P[Z^2]=\sum_{i\in I}\sum_{j\in I} d(t_i)c_i\,d(t_j)c_j\,P(A_i\cap A_j).EP​[Z2]=i∈I∑​j∈I∑​d(ti​)ci​d(tj​)cj​P(Ai​∩Aj​).

Consequently,

Var⁡P(Z)=∑i∈I∑j∈Id(ti)ci d(tj)cj (P(Ai∩Aj)−P(Ai)P(Aj)).\operatorname{Var}_P(Z)=\sum_{i\in I}\sum_{j\in I} d(t_i)c_i\,d(t_j)c_j\, \left(P(A_i\cap A_j)-P(A_i)P(A_j)\right).VarP​(Z)=i∈I∑​j∈I∑​d(ti​)ci​d(tj​)cj​(P(Ai​∩Aj​)−P(Ai​)P(Aj​)).

The finite identity for expected present value specialises the textbook's equation (3.3). The general joint-event second-moment identity extends its §3.1.1 discussion to arbitrary dependence. The goal combines all three formulas in a single result, with supporting milestone theorems for integrability, square-integrability, one-event expectation, the finite-schedule expectation formula, pairwise event interactions, the second moment and the variance.

Significance

A single reusable statement should allow a future mission to specify the trigger events and payment schedule of a policy and immediately obtain its discounted mean and variance. A life assurance can use disjoint death-year events, and an annuity can use nested survival-to-payment events. A guaranteed pension, deferred benefit, survivor pension or multiple-decrement model can use more general indicators. Later missions can also specialise the variance expression when events are known to be independent or mutually exclusive.

Examples of why the dependence assumptions matter. Write wi=d(ti)ciw_i=d(t_i)c_iwi​=d(ti​)ci​ for each discounted obligation amount:

  • Mutually exclusive death-year benefits: If Ai∩Aj=∅A_i\cap A_j=\varnothingAi​∩Aj​=∅ for every distinct pair i≠ji\ne ji=j, the general second moment simplifies to EP[Z2]=∑i∈Iwi2P(Ai)\mathbb E_P[Z^2]=\sum_{i\in I}w_i^2P(A_i)EP​[Z2]=∑i∈I​wi2​P(Ai​). This is the event structure behind term-assurance death-year payments.
  • Nested survival payments: For an annuity whose AiA_iAi​ denotes survival to time tit_iti​, whenever ti≤tjt_i\leq t_jti​≤tj​ we have Aj⊆AiA_j\subseteq A_iAj​⊆Ai​, and hence P(Ai∩Aj)=P(Aj)P(A_i\cap A_j)=P(A_j)P(Ai​∩Aj​)=P(Aj​). The later-survival probability therefore appears in the cross-term.
  • Different benefits at the same date: Two obligations indexed 111 and 222 may both have payment time 555, while depending on different events. Their second moment includes the cross-term 2w1w2P(A1∩A2)2w_1w_2P(A_1\cap A_2)2w1​w2​P(A1​∩A2​), even though t1=t2t_1=t_2t1​=t2​.

These specialisations use the same capstone rather than different definitions of actuarial present value.

The mathematical identities are established results of elementary probability and financial mathematics. The formalisation contribution is a stable actuarial cashflow interface connecting the relevant Lean measure-theoretic and probability results. It does not assert that the classical equations are newly discovered, or that general insurance reserving, stochastic interest rates or continuous-time survival models have already been formalised.

Difficulty

The event indicator is a bounded random variable, but its mathematical expectation is represented in Lean by integration against a measure. The development must reconcile the real-valued integrals with event probabilities represented as extended non-negative reals. Moreover, expanding the square of a finite random cashflow sum requires pairwise intersections without adding an independence assumption. The usual simplification that removes cross-terms is invalid for nested survival events or arbitrary dependent payment events.

The target also uses the real-valued variance from Mathlib. Its general API permits variables outside L2L^2L2, so a faithful proof must establish square-integrability for the finite event-based present value rather than use any default value for an undefined or infinite variance.

Formalisation scope

The initial development is discrete-time and finite-horizon, with distinct payment obligations indexed by a finite set. Each obligation has a nonnegative integer payment time. Different obligations may have the same payment time. Discount multipliers and payments are deterministic real values; no positivity assumption is needed for the algebraic identities. Each trigger is a measurable event and the underlying measure is a probability measure. Empty index sets and zero or negative payments are included. The joint-event formula remains valid when the same outcome triggers more than one payment.

Use Mathlib's existing MeasureTheory.Measure, MeasurableSet, integration and ProbabilityTheory.variance rather than redefining them. A lightweight namespace ActuarialValuation should define the random present value and retain clear time and cashflow parameter names. Supporting results should be small and import only genuine mathematical dependencies. The formalisation uses a generic obligation index type and a payment-time function into the natural numbers. The event family and amounts are indexed by obligations rather than by time.

There is no finite-to-infinite inference in the target; infinite sums require separate convergence results. There are no mortality rates, hazard functions, Markov transition kernels or stochastic discount factors in this mission. Those are targets for later missions, building on the valuation layer.

Selected references

  • Life Contingencies: The Mathematics, Statistics, and Economics of Life Insurance, Chapter 3, §3.1, equations (3.1)–(3.3) and §3.1.1, https://openacttextdev.github.io/LifeCon/C-SimpleBenefit.html.
  • Lean community, Mathlib 4: ProbabilityTheory.variance, https://leanprover-community.github.io/mathlib4_docs/Mathlib/Probability/Moments/Variance.html.
  • Prove2Me, Captain tour, https://prove2.me/tour/mission-captain.
9 thms1 active userReviewed
Control TheoryDynamical SystemsPartial Differential Equations·Captain: mikedeng1

Local Exponential H² Stabilization of a 2 × 2 Quasilinear Hyperbolic System Using Backstepping 3: The Feedback with Dynamic Extension Locally Exponentially Stabilizes the Quasilinear System in H²Research Paper

Motivation

First-order hyperbolic systems of balance laws zt+Λ(z,x)zx+f(z,x)=0z_t+\Lambda(z,x)z_x+f(z,x)=0zt​+Λ(z,x)zx​+f(z,x)=0 model open-channel flow (the Saint-Venant equations), gas pipelines, traffic and heat exchangers. In most of these applications the state can be acted on only at one end of the domain, so stabilizing an equilibrium is a boundary control problem. For 2×22\times22×2 systems without source term (f=0f=0f=0), static boundary feedback built from a Lyapunov function works (Coron–Bastin–d'Andréa-Novel 2008); with a source term, Lyapunov functions of the diagonal form ∫01zTQ(x)z dx\int_0^1z^{\mathsf T}Q(x)z\,dx∫01​zTQ(x)zdx can fail (Bastin and Coron 2011, recalled in Remark 1 of the paper). Backstepping, introduced for parabolic equations by Krstic and Smyshlyaev, replaces the search for a Lyapunov function by an invertible integral change of variables that maps the linearized plant to a target system whose stability is evident.

Coron, Vazquez, Krstic and Bastin (arXiv:1208.6475v1, 2012; SIAM J. Control Optim. 51(3), 2013) design such a feedback for the linearization of a 2×22\times22×2 quasilinear system and prove that it stabilizes the nonlinear system locally in H2H^2H2. This mission formalizes that main result, Theorem 4.1.

Setting

The state is z(x,t)=(z1,z2)∈R2z(x,t)=(z_1,z_2)\in\mathbb R^2z(x,t)=(z1​,z2​)∈R2 on x∈[0,1]x\in[0,1]x∈[0,1], t≥0t\ge0t≥0, governed by

zt+Λ(z,x)zx+f(z,x)=0,z1(0,t)=G0(z2(0,t)),z2(1,t)=U(t).z_t+\Lambda(z,x)z_x+f(z,x)=0,\qquad z_1(0,t)=G_0(z_2(0,t)),\qquad z_2(1,t)=U(t).zt​+Λ(z,x)zx​+f(z,x)=0,z1​(0,t)=G0​(z2​(0,t)),z2​(1,t)=U(t).

The standing assumptions (§2) are: Λ\LambdaΛ, fff, G0G_0G0​ are C2C^2C2; Λ(0,x)=diag⁡(Λ1(x),Λ2(x))\Lambda(0,x)=\operatorname{diag}(\Lambda_1(x),\Lambda_2(x))Λ(0,x)=diag(Λ1​(x),Λ2​(x)) with Λ1>0>Λ2\Lambda_1>0>\Lambda_2Λ1​>0>Λ2​ on [0,1][0,1][0,1]; f(0,x)=0f(0,x)=0f(0,x)=0; G0(0)=0G_0(0)=0G0​(0)=0. Write fij=∂fi/∂zj(0,x)f_{ij}=\partial f_i/\partial z_j(0,x)fij​=∂fi​/∂zj​(0,x) and q=G0′(0)q=G_0'(0)q=G0′​(0); the paper treats q≠0q\ne0q=0.

The scaling w=Φz=(φ1z1,φ2z2)w=\Phi z=(\varphi_1z_1,\varphi_2z_2)w=Φz=(φ1​z1​,φ2​z2​), φ1=exp⁡∫0xf11/Λ1\varphi_1=\exp\int_0^xf_{11}/\Lambda_1φ1​=exp∫0x​f11​/Λ1​, φ2=exp⁡∫0xf22/Λ2\varphi_2=\exp\int_0^xf_{22}/\Lambda_2φ2​=exp∫0x​f22​/Λ2​, removes the diagonal of the linearization, which becomes wt=Σwx+Cww_t=\Sigma w_x+Cwwt​=Σwx​+Cw with Σ=diag⁡(−ϵ1,ϵ2)\Sigma=\operatorname{diag}(-\epsilon_1,\epsilon_2)Σ=diag(−ϵ1​,ϵ2​), ϵ1=Λ1\epsilon_1=\Lambda_1ϵ1​=Λ1​, ϵ2=−Λ2\epsilon_2=-\Lambda_2ϵ2​=−Λ2​, and CCC antidiagonal with entries c1=−f12φ1/φ2c_1=-f_{12}\varphi_1/\varphi_2c1​=−f12​φ1​/φ2​, c2=−f21φ2/φ1c_2=-f_{21}\varphi_2/\varphi_1c2​=−f21​φ2​/φ1​. The kernels Kvu,KvvK^{vu},K^{vv}Kvu,Kvv solve a pair of first-order hyperbolic equations on the triangle T={0≤ξ≤x≤1}\mathcal T=\{0\le\xi\le x\le1\}T={0≤ξ≤x≤1} with boundary data on its diagonal and on the edge ξ=0\xi=0ξ=0 ((3.32), (3.33), (3.36), (3.37)). The gain is k(x)=(φ1(x)Kvu(1,x),φ2(x)Kvv(1,x))/φ2(1)k(x)=(\varphi_1(x)K^{vu}(1,x),\varphi_2(x)K^{vv}(1,x))/\varphi_2(1)k(x)=(φ1​(x)Kvu(1,x),φ2​(x)Kvv(1,x))/φ2​(1).

The closed loop adds a dynamic extension:

z2(1,t)=∫01k(ξ)Tz(ξ,t) dξ+a(t)+b(t),a˙=−d1a,b˙=−d2b,z_2(1,t)=\int_0^1k(\xi)^{\mathsf T}z(\xi,t)\,d\xi+a(t)+b(t),\qquad \dot a=-d_1a,\quad \dot b=-d_2b,z2​(1,t)=∫01​k(ξ)Tz(ξ,t)dξ+a(t)+b(t),a˙=−d1​a,b˙=−d2​b,

with d1,d2>0d_1,d_2>0d1​,d2​>0, d1≠d2d_1\ne d_2d1​=d2​, and a(0)a(0)a(0), b(0)b(0)b(0) determined by the initial profile z0z_0z0​ through two linear functionals P1(z0)P_1(z_0)P1​(z0​), P2(z0)P_2(z_0)P2​(z0​). The norm is ∥z∥H2=∥z∥L2+∥zx∥L2+∥zxx∥L2\|z\|_{H^2}=\|z\|_{L^2}+\|z_x\|_{L^2}+\|z_{xx}\|_{L^2}∥z∥H2​=∥z∥L2​+∥zx​∥L2​+∥zxx​∥L2​ on [0,1][0,1][0,1].

Formalization targets

Goal: Theorem 4.1

For every 0<λ<2min⁡(d1,d2)0<\lambda<2\min(d_1,d_2)0<λ<2min(d1​,d2​) there are δ,c>0\delta,c>0δ,c>0 such that every classical solution with ∥z0∥H2≤δ\|z_0\|_{H^2}\le\delta∥z0​∥H2​≤δ satisfying the compatibility conditions (4.16), (4.18) obeys

∥z(⋅,t)∥H22+a2(t)+b2(t)≤c e−λt(∥z0∥H22+a2(0)+b2(0))(t≥0).\|z(\cdot,t)\|_{H^2}^2+a^2(t)+b^2(t)\le c\,e^{-\lambda t}\big(\|z_0\|_{H^2}^2+a^2(0)+b^2(0)\big)\qquad(t\ge0).∥z(⋅,t)∥H22​+a2(t)+b2(t)≤ce−λt(∥z0​∥H22​+a2(0)+b2(0))(t≥0).

Milestones, in the order the proof uses them

Write γ=(α,β)=K[Φz]=Φz−∫0xK(x,ξ)Φz(ξ)dξ\gamma=(\alpha,\beta)=\mathcal K[\Phi z]=\Phi z-\int_0^xK(x,\xi)\Phi z(\xi)d\xiγ=(α,β)=K[Φz]=Φz−∫0x​K(x,ξ)Φz(ξ)dξ for the full 2×22\times22×2 kernel KKK, η=γt\eta=\gamma_tη=γt​, θ=γtt\theta=\gamma_{tt}θ=γtt​, and ∥γ∥∞=sup⁡x(∣α∣+∣β∣)\|\gamma\|_\infty=\sup_x(|\alpha|+|\beta|)∥γ∥∞​=supx​(∣α∣+∣β∣).

  1. H2H^2H2 equivalence (p. 12): ∥γ∥H2\|\gamma\|_{H^2}∥γ∥H2​ and ∥z∥H2\|z\|_{H^2}∥z∥H2​ are equivalent.
  2. Proposition 5.1: for V1=∫01γTDγV_1=\int_0^1\gamma^{\mathsf T}D\gammaV1​=∫01​γTDγ and small ∥γ∥∞\|\gamma\|_\infty∥γ∥∞​, V˙1≤−λ1V1−λ2(α2(1,t)+β2(0,t))+C1V13/2+C2∥γx∥∞V1+C3(a2+b2)\dot V_1\le-\lambda_1V_1-\lambda_2(\alpha^2(1,t)+\beta^2(0,t))+C_1V_1^{3/2}+C_2\|\gamma_x\|_\infty V_1+C_3(a^2+b^2)V˙1​≤−λ1​V1​−λ2​(α2(1,t)+β2(0,t))+C1​V13/2​+C2​∥γx​∥∞​V1​+C3​(a2+b2).
  3. Lemma B.6: the sup and L2L^2L2 norms of η\etaη and γx\gamma_xγx​ are comparable.
  4. Proposition 5.3: for V2=∫01ηTR[γ]ηV_2=\int_0^1\eta^{\mathsf T}R[\gamma]\etaV2​=∫01​ηTR[γ]η, V˙2≤−λ3V2−λ4(η12(1,t)+η22(0,t))+K1V2∥η∥∞+K2(a2+b2)\dot V_2\le-\lambda_3V_2-\lambda_4(\eta_1^2(1,t)+\eta_2^2(0,t))+K_1V_2\|\eta\|_\infty+K_2(a^2+b^2)V˙2​≤−λ3​V2​−λ4​(η12​(1,t)+η22​(0,t))+K1​V2​∥η∥∞​+K2​(a2+b2).
  5. Proposition 5.4: for V3=∫01θTR[γ]θV_3=\int_0^1\theta^{\mathsf T}R[\gamma]\thetaV3​=∫01​θTR[γ]θ and small ∥γ∥∞+∥η∥∞\|\gamma\|_\infty+\|\eta\|_\infty∥γ∥∞​+∥η∥∞​, V˙3≤−λ5V3−λ6(θ12(1,t)+θ22(0,t))+K1V3V21/2+K2V2V31/2+K3V33/2+K4∥η∥∞η22(0,t)+K5(a2+b2)\dot V_3\le-\lambda_5V_3-\lambda_6(\theta_1^2(1,t)+\theta_2^2(0,t))+K_1V_3V_2^{1/2}+K_2V_2V_3^{1/2}+K_3V_3^{3/2}+K_4\|\eta\|_\infty\eta_2^2(0,t)+K_5(a^2+b^2)V˙3​≤−λ5​V3​−λ6​(θ12​(1,t)+θ22​(0,t))+K1​V3​V21/2​+K2​V2​V31/2​+K3​V33/2​+K4​∥η∥∞​η22​(0,t)+K5​(a2+b2).
  6. Proposition B.5: the norms of θ\thetaθ and γxx\gamma_{xx}γxx​ are comparable.

Significance

Theorem 4.1 shows that a feedback computed entirely from the linearization, by solving linear kernel equations, is a valid local stabilizer of the quasilinear system in H2H^2H2, the natural space for classical C1C^1C1 solutions of quasilinear hyperbolic systems. The dynamic extension (a,b)(a,b)(a,b) is what makes the result usable: without it, the static feedback imposes artificial compatibility conditions (4.17), (4.19) on the initial data.

The result is proved in the paper (§5 and Appendix B); none of it is machine-checked. A formal proof needs a rigorous treatment of the Volterra transformation and its inverse in H2H^2H2, the three-level Lyapunov argument (V1V_1V1​, V2V_2V2​, V3V_3V3​), and the comparison of these functionals with the H2H^2H2 norm. The formalization also records corrections to the printed formulas: the sign of φ2\varphi_2φ2​ in (4.1), the entries of CCC in (4.7), the initial values (4.26), and the admissible decay rates (see below).

Difficulty

The obvious argument — the linear closed loop is exponentially stable, so the nonlinear one is locally stable — fails for hyperbolic systems: the nonlinear terms ΛNL(w,x)wx\Lambda_{NL}(w,x)w_xΛNL​(w,x)wx​ contain a derivative of the state, so they are not small in L2L^2L2 relative to ∥w∥L2\|w\|_{L^2}∥w∥L2​, and an L2L^2L2 estimate does not close. One must control γ\gammaγ, γt\gamma_tγt​ and γtt\gamma_{tt}γtt​ simultaneously, each with its own Lyapunov functional whose weight R[γ]R[\gamma]R[γ] depends on the state, and exchange time derivatives for space derivatives through the equation, which is possible only while ∥γ∥∞\|\gamma\|_\infty∥γ∥∞​ and ∥γt∥∞\|\gamma_t\|_\infty∥γt​∥∞​ stay small.

Formalization scope

States are Fin 2 → ℝ, matrices Matrix (Fin 2) (Fin 2) ℝ, indices 0-based. A solution is one C2C^2C2 function z:R×R→R2z:\mathbb R\times\mathbb R\to\mathbb R^2z:R×R→R2 (space first) with the PDE imposed on [0,1]×[0,∞)[0,1]\times[0,\infty)[0,1]×[0,∞) and the boundary conditions for t≥0t\ge0t≥0; this is the theorem restricted to classical solutions, since Mathlib has no Sobolev spaces. Global existence is not asserted. Coefficient functions are defined on all of R\mathbb RR with global C2C^2C2 regularity and sign conditions on [0,1][0,1][0,1]. H1H^1H1, H2H^2H2 norms are sums of L2L^2L2 norms, as on p. 11; ∥⋅∥∞\|\cdot\|_\infty∥⋅∥∞​ uses ∣α∣+∣β∣|\alpha|+|\beta|∣α∣+∣β∣.

Added or corrected relative to the page, all disclosed in the items:

  • q≠0q\neq0q=0 (the case the paper proves; q=0q=0q=0 is a remark);
  • φ2=exp⁡(+∫f22/Λ2)\varphi_2=\exp(+\int f_{22}/\Lambda_2)φ2​=exp(+∫f22​/Λ2​), c1=−f12φ1/φ2c_1=-f_{12}\varphi_1/\varphi_2c1​=−f12​φ1​/φ2​, c2=−f21φ2/φ1c_2=-f_{21}\varphi_2/\varphi_1c2​=−f21​φ2​/φ1​, a(0)=(P2−d2P1)/(d1−d2)a(0)=(P_2-d_2P_1)/(d_1-d_2)a(0)=(P2​−d2​P1​)/(d1​−d2​), b(0)=(d1P1−P2)/(d1−d2)b(0)=(d_1P_1-P_2)/(d_1-d_2)b(0)=(d1​P1​−P2​)/(d1​−d2​);
  • 0<λ<2min⁡(d1,d2)0<\lambda<2\min(d_1,d_2)0<λ<2min(d1​,d2​) instead of "every λ>0\lambda>0λ>0", which fails for fixed d1,d2d_1,d_2d1​,d2​ because a(t)=a(0)e−d1ta(t)=a(0)e^{-d_1t}a(t)=a(0)e−d1​t;
  • milestones take a full C2C^2C2 kernel (the page's claim via Theorem A.2, guaranteed for C3C^3C3 data); the goal takes only C1C^1C1 kernels Kvu,KvvK^{vu},K^{vv}Kvu,Kvv;
  • Proposition 5.3's last term is K2(a2+b2)K_2(a^2+b^2)K2​(a2+b2) (printed K2b2K_2b^2K2​b2).
  • Proposition 5.4 is stated for closed-loop solutions of class C3C^3C3, since V˙3\dot V_3V˙3​ involves γttt\gamma_{ttt}γttt​.

Trivializing formalizations are ruled out: δ\deltaδ, ccc and every milestone constant are quantified after the data and before the solution; the kernels are pinned down by all their equations and boundary conditions (unique by Theorem A.1 of the paper); the corrected a(0)a(0)a(0), b(0)b(0)b(0) are the ones every classical solution has, so no small initial profile is excluded; and the H2H^2H2 norm contains ∥zxx∥L2\|z_{xx}\|_{L^2}∥zxx​∥L2​.

Not formalized: Lemma 5.2 (its printed bound (5.38), ∥γ∥∞(1+∥γx∥∞)\|\gamma\|_\infty(1+\|\gamma_x\|_\infty)∥γ∥∞​(1+∥γx​∥∞​), fails for profiles with small ∥γ∥∞\|\gamma\|_\infty∥γ∥∞​ and large ∥γx∥∞\|\gamma_x\|_\infty∥γx​∥∞​, and (5.37) compares a matrix with a scalar), and Lemmas B.1–B.4, B.7, B.8. Contributions of a reusable theory of Volterra integral transformations on [0,1][0,1][0,1] with C2C^2C2 kernels, and of the comparison between sup and L2L^2L2 norms of solutions of hyperbolic systems, are welcome.

Selected references

  • J.-M. Coron, R. Vazquez, M. Krstic, G. Bastin, Local Exponential H² Stabilization of a 2 × 2 Quasilinear Hyperbolic System Using Backstepping, arXiv:1208.6475v1, 2012; SIAM J. Control Optim. 51(3), 2013. https://arxiv.org/abs/1208.6475v1
  • G. Bastin, J.-M. Coron, On boundary feedback stabilization of non-uniform linear 2 × 2 hyperbolic systems over a bounded interval, Systems and Control Letters 60, 2011, pp. 900–906 (reference [1] of arXiv:1208.6475v1). https://arxiv.org/abs/1208.6475v1
  • M. Krstic, A. Smyshlyaev, Boundary Control of PDEs: A Course on Backstepping Designs, SIAM, 2008. https://doi.org/10.1137/1.9780898718607
  • J.-M. Coron, G. Bastin, B. d'Andréa-Novel, Dissipative boundary conditions for one-dimensional nonlinear hyperbolic systems, SIAM J. Control Optim. 47(3), 2008. https://doi.org/10.1137/060650222
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Spectral Statistics of Erdős–Rényi Graphs I: Local Semicircle Law: Local Semicircle Law for the Sparse Noncentered Matrix A = H + f|e⟩⟨e| Down to Spectral Scale η ≈ 1/NResearch Paper

Motivation

The adjacency matrix of an Erdős–Rényi random graph contains a large deterministic mean as well as random fluctuations. The mean affects the largest eigenvalue, while the centered fluctuations determine much of the remaining spectrum. A local spectral law must describe both pieces at a resolution fine enough to distinguish eigenvalues within a narrow energy window. Erdős, Knowles, Yau and Yin established such estimates for a broader class of sparse symmetric matrices and their noncentered rank-one deformations in Spectral statistics of Erdős–Rényi graphs I. This mission formalizes the paper's Theorem 2.9, with the centered-matrix law and eleven intermediate results of the paper as milestones.

The paper treats the graph matrix through a model that also allows other sparse distributions. Its parameters qNq_NqN​ and fNf_NfN​ separate sparsity from the size of the deterministic mean. That separation matters: the normalized resolvent trace can obey a local semicircle law even when the deformation produces a distinguished top eigenvalue. The formal target therefore concerns the deformed matrix itself, rather than replacing it with the centered matrix.

Setting

For each size NNN, let HN=(hij)H_N=(h_{ij})HN​=(hij​) be a real symmetric random matrix. Entries indexed by the upper triangle are independent, centered, and have variance 1/N1/N1/N. Their higher moments obey

E∣hij∣p≤CpNqNp−2,3≤p≤(log⁡N)A0log⁡log⁡N.\mathbf E|h_{ij}|^p\le\frac{C^p}{Nq_N^{p-2}},\qquad 3\le p\le(\log N)^{A_0\log\log N}.E∣hij​∣p≤NqNp−2​Cp​,3≤p≤(logN)A0​loglogN.

The sparsity parameter qNq_NqN​ lies between (log⁡N)3ξN(\log N)^{3\xi_N}(logN)3ξN​ and CNC\sqrt NCN​, and the logarithmic parameter satisfies 1+a0≤ξN≤A0log⁡log⁡N1+a_0\le\xi_N\le A_0\log\log N1+a0​≤ξN​≤A0​loglogN, with a0>0a_0>0a0​>0 and A0≥10A_0\ge10A0​≥10. Define eN=N−1/2(1,…,1)e_N=N^{-1/2}(1,\ldots,1)eN​=N−1/2(1,…,1) and the noncentered matrix AN=HN+fN∣eN⟩⟨eN∣A_N=H_N+f_N|e_N\rangle\langle e_N|AN​=HN​+fN​∣eN​⟩⟨eN​∣, where 0≤fN≤NC0\le f_N\le N^C0≤fN​≤NC. The projection ∣eN⟩⟨eN∣|e_N\rangle\langle e_N|∣eN​⟩⟨eN​∣ has every entry equal to 1/N1/N1/N. These are Definitions 2.1 and 2.2 of the source paper, pp. 5–6.

For a complex number z=E+iηz=E+i\etaz=E+iη with η>0\eta>0η>0, the resolvents are G(z)=(HN−zI)−1G(z)=(H_N-zI)^{-1}G(z)=(HN​−zI)−1 and G~(z)=(AN−zI)−1\widetilde G(z)=(A_N-zI)^{-1}G(z)=(AN​−zI)−1. Their normalized traces are m(z)=N−1Tr⁡G(z)m(z)=N^{-1}\operatorname{Tr}G(z)m(z)=N−1TrG(z) and m~(z)=N−1Tr⁡G~(z)\widetilde m(z)=N^{-1}\operatorname{Tr}\widetilde G(z)m(z)=N−1TrG(z). The comparison object is the semicircle density ρsc(x)=(2π)−1[4−x2]+\rho_{\mathrm{sc}}(x)=(2\pi)^{-1}\sqrt{[4-x^2]_+}ρsc​(x)=(2π)−1[4−x2]+​​ and its Stieltjes transform msc(z)=∫Rρsc(x)/(x−z) dxm_{\mathrm{sc}}(z)=\int_{\mathbb R}\rho_{\mathrm{sc}}(x)/(x-z)\,dxmsc​(z)=∫R​ρsc​(x)/(x−z)dx. Put κE=∣∣E∣−2∣\kappa_E=\bigl||E|-2\bigr|κE​=​∣E∣−2​ and D={E+iη:∣E∣≤Σ, 0<η≤3}D=\{E+i\eta:|E|\le\Sigma,\ 0<\eta\le3\}D={E+iη:∣E∣≤Σ, 0<η≤3} for a fixed Σ≥3\Sigma\ge3Σ≥3. These definitions appear in Section 2, pp. 7–9.

An NNN-dependent event has (ξ,ν)(\xi,\nu)(ξ,ν)-high probability when its failure probability is at most exp⁡[−ν(log⁡N)ξN]\exp[-\nu(\log N)^{\xi_N}]exp[−ν(logN)ξN​] for all sufficiently large NNN. The spectral estimates below refer to single events on which the claimed bound holds at every z∈Dz\in Dz∈D simultaneously.

Formalization targets

Main goal: the local law for A

Theorem 2.9 assumes ξN∼(A0/2)log⁡log⁡N\xi_N\sim(A_0/2)\log\log NξN​∼(A0​/2)loglogN and qN≥(log⁡N)C1ξNq_N\ge(\log N)^{C_1\xi_N}qN​≥(logN)C1​ξN​. Its first conclusion is that, with (ξ,ν)(\xi,\nu)(ξ,ν)-high probability, every z=E+iη∈Dz=E+i\eta\in Dz=E+iη∈D satisfies

∣m~(z)−msc(z)∣≤(log⁡N)C2ξN(min⁡{1qN2κE+η,1qN}+1Nη).|\widetilde m(z)-m_{\mathrm{sc}}(z)|\le(\log N)^{C_2\xi_N}\left(\min\left\{\frac1{q_N^2\sqrt{\kappa_E+\eta}},\frac1{q_N}\right\}+\frac1{N\eta}\right).∣m(z)−msc​(z)∣≤(logN)C2​ξN​(min{qN2​κE​+η​1​,qN​1​}+Nη1​).

Under the additional bound fN≤C0Nf_N\le C_0\sqrt NfN​≤C0​N​, its second conclusion controls every entry at every z∈Dz\in Dz∈D:

∣G~ij(z)−δijmsc(z)∣≤(log⁡N)C2ξN(1qN+Im⁡msc(z)Nη+1Nη).|\widetilde G_{ij}(z)-\delta_{ij}m_{\mathrm{sc}}(z)|\le(\log N)^{C_2\xi_N}\left(\frac1{q_N}+\sqrt{\frac{\operatorname{Im}m_{\mathrm{sc}}(z)}{N\eta}}+\frac1{N\eta}\right).∣Gij​(z)−δij​msc​(z)∣≤(logN)C2​ξN​(qN​1​+NηImmsc​(z)​​+Nη1​).

The constants C1,C2C_1,C_2C1​,C2​ are universal and positive. The probability exponent ν>0\nu>0ν>0 may depend on the fixed parameters named in the theorem. Both conclusions, including the extra condition on fNf_NfN​ in the second, are retained from Theorem 2.9, pp. 9–10.

Milestones

The milestones follow the paper's own sequence of numbered results.

  1. Properties of mscm_{\mathrm{sc}}msc​ (Lemma 3.2): ∣msc∣∼1|m_{\mathrm{sc}}|\sim1∣msc​∣∼1, ∣1−msc2∣∼κE+η|1-m_{\mathrm{sc}}^2|\sim\sqrt{\kappa_E+\eta}∣1−msc2​∣∼κE​+η​, and the size of Im⁡msc\operatorname{Im}m_{\mathrm{sc}}Immsc​ inside and outside the spectrum.
  2. Resolvent identities for minors (Lemma 3.4) and the self-consistent equation Gii=1/(−z−msc−([v]−Υi))G_{ii}=1/(-z-m_{\mathrm{sc}}-([v]-\Upsilon_i))Gii​=1/(−z−msc​−([v]−Υi​)) (Lemma 3.10); both are deterministic.
  3. Large deviation bounds for linear and quadratic forms in independent variables with the sparse moment decay (Lemma 3.8 (ii)).
  4. The weak local semicircle law for HHH (Theorem 3.1) on DL={∣E∣≤Σ, (log⁡N)LN−1≤η≤3}D_L=\{|E|\le\Sigma,\ (\log N)^LN^{-1}\le\eta\le3\}DL​={∣E∣≤Σ, (logN)LN−1≤η≤3}, L≥8ξL\ge8\xiL≥8ξ.
  5. Fluctuation averaging (Lemma 4.1 (4.2)): the average [Z]=N−1∑iZi[Z]=N^{-1}\sum_iZ_i[Z]=N−1∑i​Zi​ of the fluctuation terms is much smaller than each ZiZ_iZi​.
  6. The a priori norm bound ∥H∥≤2+(log⁡N)ξq−1/2\|H\|\le2+(\log N)^\xi q^{-1/2}∥H∥≤2+(logN)ξq−1/2 (Lemma 4.3) and the strong local law for HHH (Theorem 2.8, the analogue of the goal for f=0f=0f=0).
  7. Interlacing of the eigenvalues of HHH and AAA (Lemma 6.1) and the near-orthogonality ∑α≠N∣⟨vα,e⟩∣2=O(f−2)\sum_{\alpha\ne N}|\langle v_\alpha,e\rangle|^2=O(f^{-2})∑α=N​∣⟨vα​,e⟩∣2=O(f−2) of eee to the non-top eigenvectors of AAA (Corollary 6.7).
  8. The trace comparison ∣Λ~−Λ∣≤π/(Nη)|\widetilde\Lambda-\Lambda|\le\pi/(N\eta)∣Λ−Λ∣≤π/(Nη) (Lemma 7.1), which yields the first conclusion of the goal from Theorem 2.8.
  9. Entrywise control of G~\widetilde GG on the event Ω~(η)\widetilde\Omega(\eta)Ω(η) that Λ~d+Λ~o≤(log⁡N)−ξ\widetilde\Lambda_d+\widetilde\Lambda_o\le(\log N)^{-\xi}Λd​+Λo​≤(logN)−ξ on the line Im⁡z=η\operatorname{Im}z=\etaImz=η: the off-diagonal bound Λ~o≤CΦ\widetilde\Lambda_o\le C\PhiΛo​≤CΦ (Proposition 7.6 (7.14)) and the diagonal bounds of Lemma 7.7, with Φ=(log⁡N)ξ/q+(log⁡N)2ξ(Im⁡m~/(Nη)+1/(Nη))\Phi=(\log N)^\xi/q+(\log N)^{2\xi}(\sqrt{\operatorname{Im}\widetilde m/(N\eta)}+1/(N\eta))Φ=(logN)ξ/q+(logN)2ξ(Imm/(Nη)​+1/(Nη)).

Significance

The trace estimate gives quantitative control over spectral mass at local scales, including near the edges E=±2E=\pm2E=±2. The entrywise estimate says more: each resolvent entry is close to the diagonal semicircle approximation with an error that records both sparsity and finite-size effects. The paper's later results derive density-of-states and eigenvector statements from these local controls. Those consequences are outside this mission's goal.

The intended formal development supplies reusable definitions of sparse symmetric ensembles, high-probability events, semicircle transforms, and complex resolvents, followed by exact statements of the paper's estimates. Mathlib contains no local semicircle law, for Wigner or for sparse matrices, and no Stieltjes transform of the semicircle distribution; the local law, the large deviation bounds and the interlacing lemma are each reusable beyond this paper.

Difficulty

The deterministic rank-one comparison controls the normalized trace but does not by itself control each entry of G~\widetilde GG. The entrywise estimate must account for the deformation and for fluctuations caused by sparse entries. Near the spectral edges, the stability scale of the semicircle transform changes with κE+η\kappa_E+\etaκE​+η; a bound that is uniform in the bulk does not automatically retain the paper's edge behavior. The theorem also asks for one event covering a continuum of zzz values, so a collection of separate fixed-zzz probability bounds has the wrong quantifier order. These are substantive parts of Sections 3–7, beyond algebraic manipulation of resolvents.

Formalization scope

Lean represents all HNH_NHN​ on one probability space and takes their entries to be real, symmetric, measurable random variables, independent in the upper triangle. Conditions involving log⁡log⁡N\log\log NloglogN and the moments hold for all sufficiently large NNN; this avoids impossible small-NNN parameter bounds and matches the asymptotic theorem. The moment order ppp is real, as in the paper. Each finite expectation has an explicit integrability condition. A single positive constant CCC is used for the moment, sparsity, and deformation bounds: replacing several fixed constants by their maximum preserves all three inequalities.

Matrix indices use Fin N rather than the paper's 1,…,N1,\ldots,N1,…,N. The resolvent is a complex matrix formed by coercing the real matrix before subtracting zIzIzI. Every result that uses it restricts η>0\eta>0η>0 eventually or explicitly; its inverse at a singular input is never used to make a claim. The semicircle transform is defined by the paper's integral, and 4−x2\sqrt{4-x^2}4−x2​ uses Lean's nonnegative square root, implementing the positive part. The high-probability predicate evaluates the measure of arbitrary sets, so it can state the intersection over all zzz without a separate measurability assumption on that intersection. Positive qNq_NqN​ and positive square-root arguments follow eventually from the model and z∈Dz\in Dz∈D.

The deterministic Lemmas 3.2, 3.4, 3.10, 6.1 and 7.1 are stated for every real symmetric matrix and every zzz with η>0\eta>0η>0 (Lemma 3.2 on DDD); the paper's DLD_LDL​ is contained there. Minors keep the original index names, and Gkl(T)G^{(\mathbb T)}_{kl}Gkl(T)​ is only used for k,l∉Tk,l\notin\mathbb Tk,l∈/T. ZiZ_iZi​ is the explicit expression of (3.15). Ordered eigenvalues are the sorted roots of the characteristic polynomial. Statements the paper makes "for fixed zzz" (Lemmas 4.1, 7.7, Proposition 7.6) are uniform in zzz: one threshold N0N_0N0​ serves every zzz. The unnamed constants CCC, ν\nuν, KKK are chosen after the fixed parameters and before the random matrices; the universal C1,C2C_1,C_2C1​,C2​ come first.

Trivializing encodings are ruled out: every resolvent is taken at η>0\eta>0η>0, so the junk inverse of a singular matrix never enters; the model is satisfiable (independent Rademacher signs divided by N\sqrt NN​ with qN=Nq_N=\sqrt NqN​=N​ and ξN=(A0/2)log⁡log⁡N\xi_N=(A_0/2)\log\log NξN​=(A0​/2)loglogN satisfy it for large NNN); each event of the goal is one intersection over all z∈Dz\in Dz∈D, not a family of pointwise bounds; the constants appear in the paper's order; and the goal is about A=H+f∣e⟩⟨e∣A=H+f|e\rangle\langle e|A=H+f∣e⟩⟨e∣ with fff allowed to be large, so it does not reduce to Theorem 2.8.

Part (iii) of Lemma 3.8 is not a milestone: the printed (3.22) omits the diagonal variance term (N−2∑i∣Bii∣2)1/2(N^{-2}\sum_i|B_{ii}|^2)^{1/2}(N−2∑i​∣Bii​∣2)1/2, without which it fails for Rademacher variables with q≍Nq\asymp\sqrt Nq≍N​. Contributions of proofs of any milestone, and of the missing groundwork (Stieltjes transforms of measures, Schur complements of resolvents, moment bounds for sums of independent variables), are welcome.

Selected references

  • L. Erdős, A. Knowles, H.-T. Yau and J. Yin, Spectral statistics of Erdős–Rényi graphs I: Local semicircle law, Annals of Probability 41(3B), 2013, pp. 2279–2375. arXiv:1103.1919v5; DOI:10.1214/11-AOP734.
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Machine LearningMarkov ChainProbability+1·Captain: mikedeng1

Nonasymptotic Convergence Analysis for the Unadjusted Langevin Algorithm: Explicit Total-Variation Bound for ULA with Nonincreasing Step Sizes When the Potential Is Strongly Convex Outside a BallResearch Paper

Why sampling from e−Ue^{-U}e−U needs non-asymptotic guarantees

Bayesian inference, statistical physics and machine learning all ask for samples from a probability distribution π\piπ on Rd\mathbb R^dRd whose density is known only up to a constant, π(dx)∝e−U(x)dx\pi(dx)\propto e^{-U(x)}dxπ(dx)∝e−U(x)dx. The unadjusted Langevin algorithm (ULA) is the Euler–Maruyama discretisation of the Langevin diffusion, whose invariant law is π\piπ. It needs only gradients of UUU, has no accept/reject step, and is therefore cheap in high dimension. Without the Metropolis correction, however, the chain does not leave π\piπ invariant, so its usefulness rests on quantitative bounds: how far, in total variation, the law of the ppp-th iterate is from π\piπ, as an explicit function of the dimension ddd, the step sizes and the regularity of UUU.

Durmus and Moulines (arXiv:1507.05021, Ann. Appl. Probab. 27(3), 2017) gave such bounds for constant and decreasing step sizes. Earlier work of Dalalyan (arXiv:1412.7392, 2017) treated strongly log-concave targets with constant steps. Durmus and Moulines cover nonincreasing step sequences and, among other regimes, potentials that are only strongly convex outside a ball; this mission formalizes that case.

Setting

Write ∥⋅∥\|\cdot\|∥⋅∥ and ⟨⋅,⋅⟩\langle\cdot,\cdot\rangle⟨⋅,⋅⟩ for the Euclidean norm and inner product of Rd\mathbb R^dRd. The total variation norm of a difference of probability measures is

∥μ−ν∥TV=sup⁡{∣∫f dμ−∫f dν∣:f Borel, ∣f∣≤1},\|\mu-\nu\|_{\mathrm{TV}}=\sup\Big\{\Big|\int f\,d\mu-\int f\,d\nu\Big|: f\text{ Borel},\ |f|\le1\Big\},∥μ−ν∥TV​=sup{​∫fdμ−∫fdν​:f Borel, ∣f∣≤1},

which ranges in [0,2][0,2][0,2].

The potential U:Rd→RU:\mathbb R^d\to\mathbb RU:Rd→R satisfies two assumptions:

  • L1: UUU is differentiable and ∇U\nabla U∇U is LLL-Lipschitz;
  • H3(MsM_sMs​): UUU is convex and ⟨∇U(x)−∇U(y),x−y⟩≥m∥x−y∥2\langle\nabla U(x)-\nabla U(y),x-y\rangle\ge m\|x-y\|^2⟨∇U(x)−∇U(y),x−y⟩≥m∥x−y∥2 whenever ∥x−y∥≥Ms\|x-y\|\ge M_s∥x−y∥≥Ms​, for some Ms≥0M_s\ge0Ms​≥0, m>0m>0m>0.

The point x⋆x^\starx⋆ is a minimiser of UUU, and π(dx)=e−U(x)dx/∫e−U\pi(dx)=e^{-U(x)}dx/\int e^{-U}π(dx)=e−U(x)dx/∫e−U.

The Langevin diffusion is dYt=−∇U(Yt)dt+2 dBtddY_t=-\nabla U(Y_t)dt+\sqrt2\,dB^d_tdYt​=−∇U(Yt​)dt+2​dBtd​, with BdB^dBd a standard ddd-dimensional Brownian motion. Its transition semigroup is Pt(x,A)=P(Yt(x)∈A)P_t(x,A)=\mathbb P(Y_t(x)\in A)Pt​(x,A)=P(Yt​(x)∈A).

ULA with step sizes (γk)k≥1(\gamma_k)_{k\ge1}(γk​)k≥1​ is the chain

Xk+1=Xk−γk+1∇U(Xk)+2γk+1Zk+1,X_{k+1}=X_k-\gamma_{k+1}\nabla U(X_k)+\sqrt{2\gamma_{k+1}}Z_{k+1},Xk+1​=Xk​−γk+1​∇U(Xk​)+2γk+1​​Zk+1​,

with (Zk)(Z_k)(Zk​) i.i.d. standard Gaussian. Its one-step kernel is Rγ(x,⋅)=N(x−γ∇U(x),2γId)R_\gamma(x,\cdot)=\mathcal N(x-\gamma\nabla U(x),2\gamma I_d)Rγ​(x,⋅)=N(x−γ∇U(x),2γId​), and δxQγn=δxRγ1⋯Rγn\delta_xQ^n_\gamma=\delta_xR_{\gamma_1}\cdots R_{\gamma_n}δx​Qγn​=δx​Rγ1​​⋯Rγn​​ is the law of XnX_nXn​ started at xxx. Write Γn,p=∑k=npγk\Gamma_{n,p}=\sum_{k=n}^p\gamma_kΓn,p​=∑k=np​γk​, and let A(γ,x)=sup⁡k≥0∫∥∇U∥2 d(δxQγk)A(\gamma,x)=\sup_{k\ge0}\int\|\nabla U\|^2\,d(\delta_xQ^k_\gamma)A(γ,x)=supk≥0​∫∥∇U∥2d(δx​Qγk​).

The explicit constants use

  • F(λ,a,c,γ,w)=λaw+c(−λγlog⁡λ)−1F(\lambda,a,c,\gamma,w)=\lambda^aw+c(-\lambda^\gamma\log\lambda)^{-1}F(λ,a,c,γ,w)=λaw+c(−λγlogλ)−1 and G(λ,c,γ,w)=w+c(−λγlog⁡λ)−1G(\lambda,c,\gamma,w)=w+c(-\lambda^\gamma\log\lambda)^{-1}G(λ,c,γ,w)=w+c(−λγlogλ)−1;
  • ω(ε,R)=R2/{2Φ−1(1−ε/2)}2\omega(\varepsilon,R)=R^2/\{2\Phi^{-1}(1-\varepsilon/2)\}^2ω(ε,R)=R2/{2Φ−1(1−ε/2)}2, with Φ\PhiΦ the standard Gaussian distribution function;
  • λ=e−2m+γˉL2\lambda=e^{-2m+\bar\gamma L^2}λ=e−2m+γˉ​L2 and c=2(d+mMs2)c=2(d+mM_s^2)c=2(d+mMs2​).

Formalization targets

Goal: Theorem 21 (p. 16)

Let d≥1d\ge1d≥1, and let (γk)(\gamma_k)(γk​) be positive and nonincreasing with γ1≤γˉ<2mL−2\gamma_1\le\bar\gamma<2mL^{-2}γ1​≤γˉ​<2mL−2. Then for all 0≤n<p0\le n<p0≤n<p and xxx,

∥δxQγp−π∥TV≤2−1/2L(∑k=np−1{γk+133A(γ,x)+dγk+12})1/2+C(δxQγn)κΓn+1,p.\|\delta_xQ^p_\gamma-\pi\|_{\mathrm{TV}}\le2^{-1/2}L\Big(\sum_{k=n}^{p-1}\Big\{\tfrac{\gamma^3_{k+1}}3A(\gamma,x)+d\gamma^2_{k+1}\Big\}\Big)^{1/2}+C(\delta_xQ^n_\gamma)\kappa^{\Gamma_{n+1,p}}.∥δx​Qγp​−π∥TV​≤2−1/2L(k=n∑p−1​{3γk+13​​A(γ,x)+dγk+12​})1/2+C(δx​Qγn​)κΓn+1,p​.

The three constants are explicit:

  • the rate, log⁡κ=−m2log⁡2 [log⁡{(1+emω(1/2,max⁡(1,Ms))/4)(1+max⁡(1,Ms))}+log⁡2]−1\log\kappa=-\frac m2\log2\,[\log\{(1+e^{m\omega(1/2,\max(1,M_s))/4})(1+\max(1,M_s))\}+\log2]^{-1}logκ=−2m​log2[log{(1+emω(1/2,max(1,Ms​))/4)(1+max(1,Ms​))}+log2]−1;
  • the constant of the first term, A(γ,x)≤L2G(λ,c,γ1,∥x−x⋆∥2)A(\gamma,x)\le L^2G(\lambda,c,\gamma_1,\|x-x^\star\|^2)A(γ,x)≤L2G(λ,c,γ1​,∥x−x⋆∥2);
  • the constant of the second term, C(δxQγn)≤6+2(d/m+Ms2)1/2+2F1/2(λ,Γ1,n,c,γ1,∥x−x⋆∥2)C(\delta_xQ^n_\gamma)\le6+2(d/m+M_s^2)^{1/2}+2F^{1/2}(\lambda,\Gamma_{1,n},c,\gamma_1,\|x-x^\star\|^2)C(δx​Qγn​)≤6+2(d/m+Ms2​)1/2+2F1/2(λ,Γ1,n​,c,γ1​,∥x−x⋆∥2).

Milestones, in the order of the proof (§5.1, p. 34)

  1. (56), p. 30: for dXt=b(Xt)dt+dBtddX_t=b(X_t)dt+dB^d_tdXt​=b(Xt​)dt+dBtd​ with bbb Lipschitz and monotone (G1), sup⁡∥x−y∥≤R∥Pt(x,⋅)−Pt(y,⋅)∥TV≤2(1−ε)\sup_{\|x-y\|\le R}\|P_t(x,\cdot)-P_t(y,\cdot)\|_{\mathrm{TV}}\le2(1-\varepsilon)sup∥x−y∥≤R​∥Pt​(x,⋅)−Pt​(y,⋅)∥TV​≤2(1−ε) for t≥ω(ε,R)t\ge\omega(\varepsilon,R)t≥ω(ε,R).
  2. Theorem 36, p. 33: under G1 and the contraction G3, ∥Pt(x,⋅)−Pt(y,⋅)∥TV≤2{(1−ε)−1+1+∥x−y∥}κt\|P_t(x,\cdot)-P_t(y,\cdot)\|_{\mathrm{TV}}\le2\{(1-\varepsilon)^{-1}+1+\|x-y\|\}\kappa^t∥Pt​(x,⋅)−Pt​(y,⋅)∥TV​≤2{(1−ε)−1+1+∥x−y∥}κt with an explicit κ\kappaκ.
  3. §5.1, p. 34: ∥Pt(x,⋅)−π∥TV≤2{3+∥x−x⋆∥+∫∥y−x⋆∥dπ(y)}κt\|P_t(x,\cdot)-\pi\|_{\mathrm{TV}}\le2\{3+\|x-x^\star\|+\int\|y-x^\star\|d\pi(y)\}\kappa^t∥Pt​(x,⋅)−π∥TV​≤2{3+∥x−x⋆∥+∫∥y−x⋆∥dπ(y)}κt for the Langevin semigroup.
  4. §5.1, p. 34: ∫∥y−x⋆∥2dπ(y)≤d/m+Ms2\int\|y-x^\star\|^2d\pi(y)\le d/m+M_s^2∫∥y−x⋆∥2dπ(y)≤d/m+Ms2​.
  5. Proposition 20, p. 16: V(x)=∥x−x⋆∥2V(x)=\|x-x^\star\|^2V(x)=∥x−x⋆∥2 satisfies RγV≤λγV+γcR_\gamma V\le\lambda^\gamma V+\gamma cRγ​V≤λγV+γc for γ∈(0,γˉ]\gamma\in(0,\bar\gamma]γ∈(0,γˉ​].
  6. Lemma 1, p. 5: such a drift gives QγnV(x)≤F(λ,Γn,c,γ1,V(x))Q^n_\gamma V(x)\le F(\lambda,\Gamma_n,c,\gamma_1,V(x))Qγn​V(x)≤F(λ,Γn​,c,γ1​,V(x)).
  7. Proposition 2, p. 5: the decomposition bound (10), given the geometric ergodicity (3) of the diffusion.

The paper's proofs follow each statement in the body of the paper (§4.1, §4.12, §5, §5.1).

Significance

The theorem bounds the sampling error of ULA in total variation non-asymptotically, with a dimension-free contraction rate κ\kappaκ and constants polynomial in ddd. With steps decreasing to zero and cumulative step size diverging, its bound gives convergence of δxQγp\delta_xQ^p_\gammaδx​Qγp​ to π\piπ; for constant steps, the paper reports iteration counts of order dlog⁡dd\log ddlogd at a prescribed precision in Table 2. H3 covers log-concave targets whose potential can lack strong convexity inside a ball.

The result is proved in the paper but, as far as the platform's catalogue shows, not formalized anywhere. A formalization adds machine-checked versions of several reusable pieces:

  • a Foster–Lyapunov moment bound for time-inhomogeneous Markov chains (Lemma 1);
  • a Girsanov–Pinsker discretisation estimate for Euler schemes (Proposition 2);
  • a reflection-coupling contraction for diffusions with monotone drift (56), Theorem 36.

Difficulty

The ULA chain is not reversible with respect to π\piπ, so the spectral and Dirichlet-form tools of reversible MCMC do not apply to it directly. The bound must instead compare the chain with the continuous diffusion.

That comparison needs Girsanov's theorem on path space and a uniform control of ∫∥∇U∥2\int\|\nabla U\|^2∫∥∇U∥2 along a time-inhomogeneous chain.

The rate of the diffusion itself is the second obstacle. Without global strong convexity, synchronous coupling gives no contraction inside the ball ∥x−y∥<Ms\|x-y\|<M_s∥x−y∥<Ms​. An explicit rate requires a reflection coupling together with return-time estimates, and it has to be transferred through the time change between dY=−∇U dt+2dBdY=-\nabla U\,dt+\sqrt2dBdY=−∇Udt+2​dB and dX=−12∇U dt+dBdX=-\frac12\nabla U\,dt+dBdX=−21​∇Udt+dB.

Formalization scope

The state space is the published EthierKurtz.SDEState d, i.e. EuclideanSpace ℝ (Fin d), and Brownian motion and strong solutions are the published EthierKurtz.IsStandardBrownian and EthierKurtz.SolvesBrownianSDE. The conventions are:

  • Semigroup. A semigroup is pinned down by the laws of solutions. PPP is the semigroup of dX=b(X)dt+s dBdX=b(X)dt+s\,dBdX=b(X)dt+sdB when every strong solution from xxx, on every probability space, has time-ttt law Pt(x,⋅)P_t(x,\cdot)Pt​(x,⋅). The Langevin case is b=−∇Ub=-\nabla Ub=−∇U, s=2s=\sqrt2s=2​.
  • Total variation. It is the sup⁡∣f∣≤1\sup_{|f|\le1}sup∣f∣≤1​ norm. Using sup⁡A∣μ(A)−ν(A)∣\sup_A|\mu(A)-\nu(A)|supA​∣μ(A)−ν(A)∣ instead would halve every bound.
  • ULA. The laws δxQγn\delta_xQ^n_\gammaδx​Qγn​ are iterated Measure.bind with the Gaussian kernel N(x−γ∇U(x),2γId)\mathcal N(x-\gamma\nabla U(x),2\gamma I_d)N(x−γ∇U(x),2γId​). Steps are indexed from 111, and Γn,p=0\Gamma_{n,p}=0Γn,p​=0 for p<np<np<n.
  • Moments. Upper-bounded moments (QγnVQ^n_\gamma VQγn​V, ∫∥∇U∥2\int\|\nabla U\|^2∫∥∇U∥2, ∫∥y−x⋆∥2dπ\int\|y-x^\star\|^2d\pi∫∥y−x⋆∥2dπ) are lower Lebesgue integrals, so a non-integrable function cannot make a bound free. A(γ,x)≤aA(\gamma,x)\le aA(γ,x)≤a is a bound for every kkk, not a real supremum.
  • Normalisation of π\piπ. No hypothesis ∫e−U<∞\int e^{-U}<\infty∫e−U<∞ is added; it follows from L1 and H3.
  • Quantile. Φ−1(u)=inf⁡{z:Φ(z)≥u}\Phi^{-1}(u)=\inf\{z:\Phi(z)\ge u\}Φ−1(u)=inf{z:Φ(z)≥u}.
  • Logarithms and powers. λ\lambdaλ, κ\kappaκ lie in (0,1)(0,1)(0,1), so the logarithms and real powers are genuine.

Several hypotheses are added or read in a particular way, and each is disclosed in the item's statement:

  • x⋆x^\starx⋆. It is a bound variable with the hypothesis that it minimises UUU; the paper uses x⋆x^\starx⋆ in §3.3 without defining it.
  • Proposition 20. The dimension is positive so its printed c=2(d+mMs2)c=2(d+mM_s^2)c=2(d+mMs2​) satisfies (6)'s requirement c>0c>0c>0; this is stated in Lean.
  • Lemma 1. It carries the §2 standing assumption L1, which makes the Euler transition family measurable in its starting point. It is stated for Borel V≥0V\ge0V≥0 rather than V≥1V\ge1V≥1, because Theorem 21 applies it to ∥x−x⋆∥2\|x-x^\star\|^2∥x−x⋆∥2.
  • Proposition 2. It assumes (3) only at μ0=δxQγn\mu_0=\delta_xQ^n_\gammaμ0​=δx​Qγn​, with finite CCC and a finite bound on A(γ,x)A(\gamma,x)A(γ,x).
  • (11). The printed Qγk(y,dz)Q^k_\gamma(y,dz)Qγk​(y,dz) is read as Qγk(x,dz)Q^k_\gamma(x,dz)Qγk​(x,dz).

The citations [20] (existence of solutions), [27] (Lindvall), [32] (Meyn–Tweedie) and Girsanov's theorem are used inside the proofs and are not restated.

The library work needed is substantial: Itô calculus for the reflection coupling, Girsanov's theorem, Pinsker's inequality in this norm, and generator–drift arguments for the moments of π\piπ. Contributions of any of these as standalone platform theorems are welcome.

Selected references

  • A. Durmus, É. Moulines, Nonasymptotic convergence analysis for the unadjusted Langevin algorithm, Ann. Appl. Probab. 27(3), 2017; cited as arXiv:1507.05021v3. https://arxiv.org/abs/1507.05021
  • A. S. Dalalyan, Theoretical guarantees for approximate sampling from smooth and log-concave densities, J. R. Stat. Soc. B 79(3), 2017. https://arxiv.org/abs/1412.7392
  • T. Lindvall, L. C. G. Rogers, Coupling of multidimensional diffusions by reflection, Ann. Probab. 14(3), 1986. https://doi.org/10.1214/aop/1176992436
  • S. P. Meyn, R. L. Tweedie, Stability of Markovian processes III: Foster–Lyapunov criteria for continuous-time processes, Adv. Appl. Probab. 25(3), 1993. https://doi.org/10.2307/1427522
  • G. O. Roberts, R. L. Tweedie, Exponential convergence of Langevin distributions and their discrete approximations, Bernoulli 2(4), 1996. https://doi.org/10.2307/3318418
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Control TheoryDynamic ProgrammingProbability+1·Captain: mikedeng1

McKean–Vlasov Optimal Control: The Dynamic Programming Principle 1: The Weak Formulation's Value Function Is Upper Semi-Analytic and Satisfies the DPPResearch Paper

Motivation

A McKean–Vlasov control problem asks a planner to steer a stochastic differential equation whose coefficients depend not only on the current path of the state but also on its (conditional) distribution. Such problems describe the cooperative optimum of a large population of interacting agents: when each agent reacts to the empirical distribution of all others and a social planner chooses everybody's control, the limit as the population grows is a McKean–Vlasov control problem (Lacker 2017). When all agents are also exposed to a common noise (a shared source of randomness, such as a market factor), the relevant distribution is the conditional law of the state given that noise.

Bellman's dynamic programming principle (DPP) is the standard route from a control problem to its Hamilton–Jacobi–Bellman equation and to verification arguments. For McKean–Vlasov dynamics it fails in the naive state variable, because the problem is time-inconsistent; it can be recovered by taking the (conditional) law of the state as the state.

Timeline. Laurière and Pironneau (2014) and Bensoussan, Frehse and Yam (2013–2017) proved a DPP for densities of the state law. Pham and Wei (2017, SICON) proved a DPP over closed-loop controls in a Markovian setting with a common-noise filtration, under regularity assumptions; Pham and Wei (2018, ESAIM:COCV) treated the case without common noise. Bayraktar, Cosso and Pham (2018, Trans. AMS) obtained a randomised DPP, again Markovian and without common noise. Djete, Possamaï and Tan (2022) proved the DPP for the general non-Markovian problem with common noise, under Borel measurability of the coefficients only. This mission formalizes their DPP for the weak formulation.

Setting

Fix a horizon T>0T>0T>0, dimensions n,d,ℓ∈Nn,d,\ell\in\mathbb Nn,d,ℓ∈N, a nonempty Polish space (U,ρ)(U,\rho)(U,ρ) of control values, a point u0∈Uu_0\in Uu0​∈U and an exponent p≥0p\ge0p≥0. Let Ck:=C([0,T],Rk)\mathcal C^k:=C([0,T],\mathbb R^k)Ck:=C([0,T],Rk) with the uniform norm, P(E)\mathcal P(E)P(E) the Borel probability measures on EEE with the weak topology, and xt∧⋅x_{t\wedge\cdot}xt∧⋅​ the path xxx stopped at time ttt. The coefficients b,σ,σ0,Lb,\sigma,\sigma_0,Lb,σ,σ0​,L are maps [0,T]×Cn×P(Cn×U)×U→Rn,Rn×d,Rn×ℓ,R[0,T]\times\mathcal C^n\times\mathcal P(\mathcal C^n\times U)\times U\to\mathbb R^n,\mathbb R^{n\times d},\mathbb R^{n\times\ell},\mathbb R[0,T]×Cn×P(Cn×U)×U→Rn,Rn×d,Rn×ℓ,R, and g:Cn×P(Cn)→Rg:\mathcal C^n\times\mathcal P(\mathcal C^n)\to\mathbb Rg:Cn×P(Cn)→R; all are Borel measurable, and b,σ,σ0,Lb,\sigma,\sigma_0,Lb,σ,σ0​,L depend on the path and the measure only through their restrictions to [0,t][0,t][0,t] (non-anticipative).

A weak control γ\gammaγ with initial condition (t,ν)∈[0,T]×P(Cn)(t,\nu)\in[0,T]\times\mathcal P(\mathcal C^n)(t,ν)∈[0,T]×P(Cn) consists of a probability space carrying two filtrations Fγ⊇Gγ\mathbb F^\gamma\supseteq\mathbb G^\gammaFγ⊇Gγ (the second models the common noise), a state XγX^\gammaXγ, Brownian motions WγW^\gammaWγ (idiosyncratic) and BγB^\gammaBγ (common) on [t,T][t,T][t,T], a predictable UUU-valued control αγ\alpha^\gammaαγ, and measure-valued processes μsγ=L(Xs∧⋅γ∣Gsγ)\mu^\gamma_s=\mathcal L(X^\gamma_{s\wedge\cdot}\mid\mathcal G^\gamma_s)μsγ​=L(Xs∧⋅γ​∣Gsγ​) and μˉsγ=L((Xs∧⋅γ,αsγ)∣Gsγ)\bar\mu^\gamma_s=\mathcal L((X^\gamma_{s\wedge\cdot},\alpha^\gamma_s)\mid\mathcal G^\gamma_s)μˉ​sγ​=L((Xs∧⋅γ​,αsγ​)∣Gsγ​), such that Xt∧⋅γ∼ν(t)X^\gamma_{t\wedge\cdot}\sim\nu(t)Xt∧⋅γ​∼ν(t), an integrability condition of order ppp holds, a compatibility condition between the two filtrations holds, and

dXsγ=b(s,Xγ,μˉsγ,αsγ) ds+σ(s,Xγ,μˉsγ,αsγ) dWsγ+σ0(s,Xγ,μˉsγ,αsγ) dBsγ,s∈[t,T].dX^\gamma_s=b(s,X^\gamma,\bar\mu^\gamma_s,\alpha^\gamma_s)\,ds+\sigma(s,X^\gamma,\bar\mu^\gamma_s,\alpha^\gamma_s)\,dW^\gamma_s+\sigma_0(s,X^\gamma,\bar\mu^\gamma_s,\alpha^\gamma_s)\,dB^\gamma_s,\qquad s\in[t,T].dXsγ​=b(s,Xγ,μˉ​sγ​,αsγ​)ds+σ(s,Xγ,μˉ​sγ​,αsγ​)dWsγ​+σ0​(s,Xγ,μˉ​sγ​,αsγ​)dBsγ​,s∈[t,T].

The reward and the value function are

J(t,γ)=E[∫tTL(s,Xs∧⋅γ,μˉsγ,αsγ) ds+g(XT∧⋅γ,μTγ)],VW(t,ν)=sup⁡γ∈ΓW(t,ν)J(t,γ),J(t,\gamma)=\mathbb E\Big[\int_t^TL(s,X^\gamma_{s\wedge\cdot},\bar\mu^\gamma_s,\alpha^\gamma_s)\,ds+g(X^\gamma_{T\wedge\cdot},\mu^\gamma_T)\Big],\qquad V_W(t,\nu)=\sup_{\gamma\in\Gamma_W(t,\nu)}J(t,\gamma),J(t,γ)=E[∫tT​L(s,Xs∧⋅γ​,μˉ​sγ​,αsγ​)ds+g(XT∧⋅γ​,μTγ​)],VW​(t,ν)=γ∈ΓW​(t,ν)sup​J(t,γ),

with ∞−∞:=−∞\infty-\infty:=-\infty∞−∞:=−∞ and sup⁡∅=−∞\sup\emptyset=-\inftysup∅=−∞. Each weak control also carries Asγ=∫ts∨tπ(αrγ) drA^\gamma_s=\int_t^{s\vee t}\pi(\alpha^\gamma_r)\,drAsγ​=∫ts∨t​π(αrγ​)dr, where π\piπ is a Borel isomorphism of UUU onto a subset of [0,1][0,1][0,1], and the continuous conditional-law process μ^γ\hat\mu^\gammaμ^​γ of (Xγ,Aγ,Wγ,Bγ)(X^\gamma,A^\gamma,W^\gamma,B^\gamma)(Xγ,Aγ,Wγ,Bγ) given Gγ\mathbb G^\gammaGγ.

Formalization targets

Goal: Theorem 3.1

VW:[0,T]×P(Cn)→[−∞,∞]V_W:[0,T]\times\mathcal P(\mathcal C^n)\to[-\infty,\infty]VW​:[0,T]×P(Cn)→[−∞,∞] is upper semi-analytic (every superlevel set {VW>c}\{V_W>c\}{VW​>c} is analytic), and for every stopping time τ⋆\tau^\starτ⋆ of the canonical filtration of Ω⋆:=Cℓ×C([0,T],P(Cn×C×Cd×Cℓ))\Omega^\star:=\mathcal C^\ell\times C([0,T],\mathcal P(\mathcal C^n\times\mathcal C\times\mathcal C^d\times\mathcal C^\ell))Ω⋆:=Cℓ×C([0,T],P(Cn×C×Cd×Cℓ)) with values in [t,T][t,T][t,T], setting τγ:=τ⋆(Bγ,t,μ^γ)\tau^\gamma:=\tau^\star(B^{\gamma,t},\hat\mu^\gamma)τγ:=τ⋆(Bγ,t,μ^​γ),

VW(t,ν)=sup⁡γ∈ΓW(t,ν)E[∫tτγL(s,Xs∧⋅γ,μˉsγ,αsγ) ds+VW(τγ,μτγγ)].V_W(t,\nu)=\sup_{\gamma\in\Gamma_W(t,\nu)}\mathbb E\Big[\int_t^{\tau^\gamma}L(s,X^\gamma_{s\wedge\cdot},\bar\mu^\gamma_s,\alpha^\gamma_s)\,ds+V_W(\tau^\gamma,\mu^\gamma_{\tau^\gamma})\Big].VW​(t,ν)=γ∈ΓW​(t,ν)sup​E[∫tτγ​L(s,Xs∧⋅γ​,μˉ​sγ​,αsγ​)ds+VW​(τγ,μτγγ​)].

Milestones

The canonical reformulation on Ωˉ:=Ω^×C([0,T],P(Ω^))\bar\Omega:=\hat\Omega\times C([0,T],\mathcal P(\hat\Omega))Ωˉ:=Ω^×C([0,T],P(Ω^)) with weak control rules PˉW(t,ν)\bar{\mathcal P}_W(t,\nu)PˉW​(t,ν) (Definition 4.1): Lemma 4.4(i) (weak controls and weak control rules correspond), Corollary 4.6 (VW(t,ν)=sup⁡Pˉ∈PˉW(t,ν)J(t,Pˉ)V_W(t,\nu)=\sup_{\bar{\mathbb P}\in\bar{\mathcal P}_W(t,\nu)}J(t,\bar{\mathbb P})VW​(t,ν)=supPˉ∈PˉW​(t,ν)​J(t,Pˉ)), Lemma 4.7 (analytic graphs, VWV_WVW​ u.s.a.), Lemma 4.8 (stability under conditioning at a stopping time), Lemma 4.9 (dependence on the initial law only through ν^(t)\hat\nu(t)ν^(t)), (4.10) (moment truncation VWM↗VWV^M_W\nearrow V_WVWM​↗VW​, analytic and u.s.a.) and Lemma 4.10 (universally measurable ε\varepsilonε-optimal families and concatenation).

Significance

The result. The theorem gives the DPP for McKean–Vlasov control with common noise in a non-Markovian setting, with no regularity on the coefficients beyond Borel measurability and no integrability on the rewards. It is the starting point for the dynamic programming (HJB) equation on the space of probability measures, for the Markovian corollaries of §3.2 of the paper, and, through the equivalence of formulations in the companion work, for the strong formulations treated in the second mission of this series.

Formalizing it. The result is proved on paper; nothing of it is machine-checked. A formal development needs a working theory of weak controls with conditional laws, a controlled martingale problem on a space of measure-valued paths, and analytic-set measurability in continuous time. None of these exists in Mathlib, and the analytic-selection layer on Prove2Me (Bertsekas–Shreve, Chapter 7) is stated but not yet proved.

Difficulty

The obvious argument conditions an optimal-ish control on its information at the stopping time and pastes in near-optimal controls from the conditioned states. Each step fails without additional structure: VWV_WVW​ is not known to be measurable, so E[VW(τγ,μτγγ)]\mathbb E[V_W(\tau^\gamma,\mu^\gamma_{\tau^\gamma})]E[VW​(τγ,μτγγ​)] is not obviously meaningful; conditioning a weak control on its information at τγ\tau^\gammaτγ need not yield a weak control, because the conditional-law constraint involves the common-noise filtration and a compatibility condition between filtrations; and choosing a near-optimal control for each conditioned state is a selection problem over an uncountable family of probability spaces. The state of the problem is a law, which is itself defined only up to null sets, so random-time evaluations such as μτγγ\mu^\gamma_{\tau^\gamma}μτγγ​ need a continuous version.

Formalization scope

The Lean development lives in the namespace MKVDPP.Weak. Conventions:

  • Times are in R≥0\mathbb R_{\ge0}R≥0​; paths are elements of C([0,T],Rk)C([0,T],\mathbb R^k)C([0,T],Rk) with Rk\mathbb R^kRk Euclidean; a path is read at times beyond TTT as its value at TTT.
  • Expectations and time integrals are E[ξ+]−E[ξ−]\mathbb E[\xi^+]-\mathbb E[\xi^-]E[ξ+]−E[ξ−] in [−∞,∞][-\infty,\infty][−∞,∞] with ∞−∞=−∞\infty-\infty=-\infty∞−∞=−∞, computed as lower integrals.
  • The supremum defining VWV_WVW​ ranges over weak controls on probability spaces in Type (universe 0).
  • "The integrals are implicitly assumed to be well-defined" is pinned to local Itô integrals (EthierKurtz.HasBrownianItoIntegral) of integrands that are a.s. square integrable on [t,T][t,T][t,T], taken against the shifted Brownian motions Wγ,tW^{\gamma,t}Wγ,t, Bγ,tB^{\gamma,t}Bγ,t; no L2(P)L^2(\mathbb P)L2(P) condition, which would shrink ΓW\Gamma_WΓW​.
  • The conditional-law requirement "for dP⊗dsd\mathbb P\otimes dsdP⊗ds-a.e. (s,ω)(s,\omega)(s,ω)" is read in Fubini form; μTγ\mu^\gamma_TμTγ​ and μτγγ\mu^\gamma_{\tau^\gamma}μτγγ​ are the XXX-marginals of the continuous process μ^γ\hat\mu^\gammaμ^​γ.
  • "Local martingale on [t,T][t,T][t,T]" in Definition 4.1 is pinned to: every localised process Sφ,mS^{\varphi,m}Sφ,m, m≥1m\ge1m≥1, is an (Fˉ,Pˉ)(\bar{\mathbb F},\bar{\mathbb P})(Fˉ,Pˉ)-martingale on [t,T][t,T][t,T]. The page integrates ∣Sˉ∣|\bar S|∣Sˉ∣ and Sˉφ\bar S^\varphiSˉφ from 000. Here they run from the initial time ttt, because before ttt the canonical control may be ∂\partial∂, where the coefficients are undefined, and a coefficient that is not integrable before ttt would empty P^W(t,⋅)\hat{\mathcal P}_W(t,\cdot)P^W​(t,⋅).
  • The cemetery value ∂\partial∂ of the canonical control is read as u0u_0u0​ inside the coefficients (a null set under Definition 4.1).
  • In (3.2), (+∞)+(−∞)(+\infty)+(-\infty)(+∞)+(−∞) inside the expectation is −∞-\infty−∞.
  • Lemma 4.4(i)'s converse carries the hypothesis that the canonical AAA is a.s. ∫t⋅∨tπ(αˉr) dr\int_t^{\cdot\vee t}\pi(\bar\alpha_r)\,dr∫t⋅∨t​π(αˉr​)dr; without it the converse is false, because Definition 4.1 leaves AAA before ttt unconstrained.

The goal does not mention the canonical space Ωˉ\bar\OmegaΩˉ, weak control rules or any selection; a formalization of ΓW\Gamma_WΓW​ that is empty, or a value function that is constant, would trivialize it. A sanity file exhibits a weak control in the degenerate case n=d=ℓ=0n=d=\ell=0n=d=ℓ=0 for every t≤Tt\le Tt≤T, so the structure is satisfiable.

Infrastructure a complete development needs: conditional laws and r.c.p.d. on Polish spaces, the predictable σ\sigmaσ-algebra, stochastic integrals against a filtration, the Stroock–Varadhan martingale problem, Itô's formula, and analytic sets with the Jankov–von Neumann selection theorem. The analytic-selection results and the martingale-problem/SDE correspondence are reusable well beyond this mission. Contributions on any milestone, and on proving the referenced Bertsekas–Shreve selection theorems, are welcome. Out of scope: Theorem 3.4 (it rests on the companion paper), the Markovian results of §3.2, and the HJB discussion of §3.3.

Selected references

  • M. F. Djete, D. Possamaï, X. Tan, McKean–Vlasov optimal control: the dynamic programming principle, Ann. Probab. 50(2), 2022; cited as arXiv:1907.08860v2. https://arxiv.org/abs/1907.08860v2
  • H. Pham, X. Wei, Dynamic programming for optimal control of stochastic McKean–Vlasov dynamics, SIAM J. Control Optim. 55(2):1069–1101, 2017. https://arxiv.org/abs/1604.04057
  • D. Lacker, Limit theory for controlled McKean–Vlasov dynamics, SIAM J. Control Optim. 55(3):1641–1672, 2017. https://arxiv.org/abs/1609.08064
  • N. El Karoui, X. Tan, Capacities, measurable selection and dynamic programming part II: application in stochastic control problems, 2013. https://arxiv.org/abs/1310.3364
  • E. Bayraktar, A. Cosso, H. Pham, Randomized dynamic programming principle and Feynman–Kac representation for optimal control of McKean–Vlasov dynamics, Trans. Amer. Math. Soc. 370(3):2115–2160, 2018. https://doi.org/10.1090/tran/7118
  • M. Laurière, O. Pironneau, Dynamic programming for mean-field type control, C. R. Math. Acad. Sci. Paris 352(9):707–713, 2014. https://doi.org/10.1016/j.crma.2014.07.008
  • A. Bensoussan, J. Frehse, S. Yam, Mean Field Games and Mean Field Type Control Theory, SpringerBriefs in Mathematics, Springer, 2013. https://doi.org/10.1007/978-1-4614-8508-7
  • D. Bertsekas, S. Shreve, Stochastic Optimal Control: The Discrete-Time Case, Academic Press, 1978. https://web.mit.edu/dimitrib/www/SOC_1978.pdf
  • D. Stroock, S. Varadhan, Multidimensional Diffusion Processes, Springer, 1997. https://doi.org/10.1007/3-540-28999-2
14 thms1 active userReviewed
Control TheoryDynamic ProgrammingProbability+1·Captain: mikedeng1

McKean–Vlasov Optimal Control: The Dynamic Programming Principle 2: Under Lipschitz Coefficients the Common-Noise-Adapted Strong Formulation Satisfies the DPPResearch Paper

Why common noise changes the control problem

A controller may act on a large population of interacting particles while all particles also experience a shared random disturbance. In the population limit, the state of a representative particle depends on the distribution of states conditional on the common noise. The controller therefore influences both its own state and the conditional population law. The usual state variable for dynamic programming must carry that law, and a future decision may use only information available from common noise. Djete, Possamaï and Tan establish a dynamic programming principle for this setting in McKean–Vlasov optimal control: the dynamic programming principle, Theorem 3.2. Their result permits path dependent coefficients and merely Borel reward functions, so ordinary continuity arguments do not determine the value function's measurability.

The paper distinguishes a weak formulation, in which the stochastic basis varies with the control, from a strong formulation on a fixed space. This mission concerns the latter, restricted to controls predictable from common noise, under the paper's Lipschitz and growth Assumption 2.8. The companion mission treats the weak dynamic programming principle, Theorem 3.1. The present mission asks for a machine checked account of the strong formulation and of the transfer between its intrinsic, fixed space and canonical descriptions.

State, noise and admissible controls

Fix a horizon T>0T>0T>0. A state trajectory belongs to Cn=C([0,T],Rn)\mathcal C^n=C([0,T],\mathbb R^n)Cn=C([0,T],Rn). The two driving noises are a ddd dimensional idiosyncratic Brownian motion WWW and an ℓ\ellℓ dimensional common Brownian motion BBB. The control space UUU is nonempty and Polish. At time sss, the controlled drift bbb and diffusions σ,σ0\sigma,\sigma_0σ,σ0​ may depend on the stopped state path Xs∧⋅X_{s\wedge\cdot}Xs∧⋅​, the control αs\alpha_sαs​, and the conditional law μˉs\bar\mu_sμˉ​s​ of the stopped state and control given common noise. The running and terminal rewards are LLL and ggg.

A B\mathbb BB strong control has a continuous state satisfying the controlled stochastic equation, the conditional laws required by the paper, finite quadratic control energy, and an α\alphaα predictable for the common noise filtration. Its reward J(t,γ)J(t,\gamma)J(t,γ) is the expected running reward from ttt to TTT plus the terminal reward. The value VSB(t,ν)V_S^{\mathbb B}(t,\nu)VSB​(t,ν) is the supremum of these rewards over such controls from initial path law ν\nuν. The initial law lies in P2(Cn)\mathcal P_2(\mathcal C^n)P2​(Cn), the laws with a finite second moment. The coefficient hypothesis uses the quadratic Wasserstein distance W2W_2W2​ and one constant C>0C>0C>0 for both a Lipschitz bound and a quadratic growth bound. These conditions are Assumption 2.8 of the source paper, p. 8.

The paper also fixes a canonical probability space Ωt\Omega^tΩt carrying an initial path and Brownian increments after ttt. Its common noise predictable controls form A2B(t,ν)\mathcal A_2^{\mathbb B}(t,\nu)A2B​(t,ν). Proposition 2.10 says this fixed space computes the same value as the intrinsic strong formulation. The precise probability law on Ωt\Omega^tΩt is characterized by the initial stopped path law and independent standard Brownian increments; the paper does not choose a unique construction.

Formalization targets

The goal is Theorem 3.2, p. 10. It first asserts that the value on [0,T]×P2(Cn)[0,T]\times\mathcal P_2(\mathcal C^n)[0,T]×P2​(Cn) is upper semi analytic: each strict superlevel set {(t,ν):VSB(t,ν)>c}\{(t,\nu):V_S^{\mathbb B}(t,\nu)>c\}{(t,ν):VSB​(t,ν)>c} is analytic. For an initial pair (t,ν)(t,\nu)(t,ν) and a stopping time τ∈[t,T]\tau\in[t,T]τ∈[t,T] for the raw common noise filtration on Ωt\Omega^tΩt, it then asserts

VSB(t,ν)=sup⁡α∈A2B(t,ν)E ⁣[∫tτL(s,Xs∧⋅α,μˉsα,αs) ds+VSB(τ,μτα)].V_S^{\mathbb B}(t,\nu)=\sup_{\alpha\in\mathcal A_2^{\mathbb B}(t,\nu)} \mathbb E\!\left[\int_t^\tau L(s,X^\alpha_{s\wedge\cdot},\bar\mu_s^\alpha,\alpha_s)\,ds +V_S^{\mathbb B}(\tau,\mu_\tau^\alpha)\right].VSB​(t,ν)=α∈A2B​(t,ν)sup​E[∫tτ​L(s,Xs∧⋅α​,μˉ​sα​,αs​)ds+VSB​(τ,μτα​)].

Here μτα\mu_\tau^\alphaμτα​ is the law of the stopped state conditional on information from common noise at τ\tauτ. The milestone sequence follows the paper's supporting results: strong solution existence and uniqueness (Theorem A.3(i)); equivalence of intrinsic and fixed space values (Proposition 2.10); induction of canonical rules from strong controls (the forward clause of Lemma 4.4(ii)); the canonical value identity (Corollary 4.6); the Wiener represented rule class and its value (Lemma 4.11); analytic rule graphs and value measurability (Lemma 4.12); and stability of a strong rule under conditioning at a stopping time (Lemma 4.13(i)). Each is a source indexed target, rather than an invented intermediate assertion.

What the result provides

The identity permits the value after a random common noise stopping time to be evaluated from the stopped conditional state law. This is the form needed to compare control decisions before and after a random observation time. Upper semi analyticity supplies measurable superlevel sets for the value even when LLL and ggg lack continuity. The paper proves these statements mathematically; the mission seeks their Lean formalization, not a new theorem about the underlying control problem.

A complete formalization would also provide reusable definitions of conditional measure valued flows, Brownian motion relative to a filtration over a shifted interval, a local Itô equation, and canonical martingale control rules. The two published Ethier–Kurtz definitions supply the local Itô relation and probability augmentation of a filtration. They are shared infrastructure rather than new statements of this paper.

Where the difficulty lies

The state law in the coefficients is conditional on common noise and changes with the control. A pathwise solution of the state equation must therefore remain consistent with its own conditional law. A naive argument that restarts an ordinary diffusion at τ\tauτ does not establish that consistency for a restarted control. It also does not ensure that a restarted control remains predictable from common noise. The paper's canonical rule formulation and its conditioning and measurability results address those obstructions. The reward may be unbounded and extended real valued, so the expectation convention and its behavior at infinite positive and negative parts matter to the statement itself.

Formalization scope and conventions

Paths are continuous maps on compact real intervals with uniform norm; Rk\mathbb R^kRk is Mathlib's Euclidean space, including k=0k=0k=0. Probability measures carry weak convergence topology, and P2\mathcal P_2P2​ is its finite second moment subtype. The product of path space and UUU uses Mathlib's product metric; matrix norms are Frobenius. Supremums range over admissible controls, solutions and conditional law versions. They are EReal valued, so the empty supremum is −∞-\infty−∞. The signed expectation is positive part minus negative part with ∞−∞=−∞\infty-\infty=-\infty∞−∞=−∞, as in the paper. The model fixes a Borel embedding of UUU into [0,1][0,1][0,1] and a cemetery control for invalid reconstructed paths.

The Lean statements pin the paper's implicit “well defined” stochastic integral to a pathwise square integrable local Itô relation and almost surely integrable drift. A conditional law equality stated for dP⊗dsd\mathbb P\otimes dsdP⊗ds almost every pair is expressed in Fubini form. The localized processes printed in Definition 4.1 define its local martingale requirement. The terminal law and the stopped law in the target are quantified as versions of their stated conditional distributions. The fixed canonical law is any law satisfying the paper's initial distribution and Brownian conditions; the target is stated for every such family. These conventions rule out free conditional laws, arbitrary future stopping times, and a value that is −∞-\infty−∞ solely because a formalization made the control class empty. A full development must establish nonemptiness and version independence as part of the cited supporting theory.

The scope ends with Theorem 3.2 and the listed milestones. Lemma 4.13(ii), the more involved measurable selection and concatenation result, remains a future contribution. Theorem 3.4 uses a separate companion result; the Markovian corollaries and the heuristic Hamilton–Jacobi discussion of §3.3 are outside this mission.

Selected references

  • M. F. Djete, D. Possamaï and X. Tan, McKean–Vlasov optimal control: the dynamic programming principle, arXiv:1907.08860v2, 2020; published in Annals of Probability 50(2), 2022. Preprint. This mission cites the preprint's page and theorem numbering.
14 thms1 active userReviewed
Control TheoryDynamical SystemsPartial Differential Equations·Captain: mikedeng1

Local Exponential H² Stabilization of a 2 × 2 Quasilinear Hyperbolic System Using Backstepping 2: Backstepping Feedback Makes a 2 × 2 Linear Hyperbolic System Vanish in Finite TimeResearch Paper

Motivation

Systems of two first-order hyperbolic equations with opposite transport speeds model open-channel flow (the Saint-Venant equations), gas pipelines, heat exchangers and traffic. In such systems one boundary is actuated, the other boundary reflects, and the coupling terms move energy between the two families of waves. Boundary feedback design for them is a standard problem of distributed-parameter control.

The backstepping method designs a feedback by means of an invertible Volterra integral transformation that turns the plant into a target system whose behaviour is known in closed form. Coron, Vazquez, Krstic and Bastin (arXiv:1208.6475; SIAM J. Control Optim. 51(3), 2013) carry out this design for a general linear 2×22\times22×2 hyperbolic system with spatially varying speeds and couplings, in §3 of their paper. The resulting linear feedback is the controller they later apply to a quasilinear system. This mission formalizes the linear result.

Timeline:

  • 2008: Krstic and Smyshlyaev, Backstepping boundary control for first-order hyperbolic PDEs and application to systems with actuator and sensor delays (Systems & Control Letters 57), give the scalar transport case.
  • 2012/2013: Coron, Vazquez, Krstic and Bastin treat the 2×22\times22×2 case. The kernel equations of the transformation form a Goursat-type system on a triangle, and they prove it is well-posed in their Appendix A.

Setting

Let ϵ1,ϵ2\epsilon_1,\epsilon_2ϵ1​,ϵ2​ be C1C^1C1 functions on [0,1][0,1][0,1] with ϵ1,ϵ2>0\epsilon_1,\epsilon_2>0ϵ1​,ϵ2​>0, let c1,c2c_1,c_2c1​,c2​ be continuous, and let q∈Rq\in\mathbb Rq∈R. The state w(x,t)=[u v]T∈R2w(x,t)=[u\ v]^T\in\mathbb R^2w(x,t)=[u v]T∈R2 solves

wt=Σ(x)wx+C(x)w,Σ=(−ϵ100ϵ2),C=(0c1c20),x∈[0,1], t≥0,w_t=\Sigma(x)w_x+C(x)w,\qquad \Sigma=\begin{pmatrix}-\epsilon_1&0\\0&\epsilon_2\end{pmatrix},\quad C=\begin{pmatrix}0&c_1\\c_2&0\end{pmatrix},\qquad x\in[0,1],\ t\ge0,wt​=Σ(x)wx​+C(x)w,Σ=(−ϵ1​0​0ϵ2​​),C=(0c2​​c1​0​),x∈[0,1], t≥0,

so uuu travels to the right and vvv to the left. The boundary conditions are u(0,t)=q v(0,t)u(0,t)=q\,v(0,t)u(0,t)=qv(0,t) and v(1,t)=U(t)v(1,t)=U(t)v(1,t)=U(t), where UUU is the control. The norm is ∥w(⋅,t)∥L2=∫01(u2+v2) dξ\|w(\cdot,t)\|_{L^2}=\sqrt{\int_0^1(u^2+v^2)\,d\xi}∥w(⋅,t)∥L2​=∫01​(u2+v2)dξ​.

The kernels Kvu,KvvK^{vu},K^{vv}Kvu,Kvv are functions on the triangle T={(x,ξ):0≤ξ≤x≤1}\mathcal T=\{(x,\xi):0\le\xi\le x\le1\}T={(x,ξ):0≤ξ≤x≤1} that solve

ϵ2(x)Kxvu−ϵ1(ξ)Kξvu=ϵ1′(ξ)Kvu+c2(ξ)Kvv,ϵ2(x)Kxvv+ϵ2(ξ)Kξvv=−ϵ2′(ξ)Kvv+c1(ξ)Kvu,\epsilon_2(x)K^{vu}_x-\epsilon_1(\xi)K^{vu}_\xi=\epsilon_1'(\xi)K^{vu}+c_2(\xi)K^{vv},\qquad \epsilon_2(x)K^{vv}_x+\epsilon_2(\xi)K^{vv}_\xi=-\epsilon_2'(\xi)K^{vv}+c_1(\xi)K^{vu},ϵ2​(x)Kxvu​−ϵ1​(ξ)Kξvu​=ϵ1′​(ξ)Kvu+c2​(ξ)Kvv,ϵ2​(x)Kxvv​+ϵ2​(ξ)Kξvv​=−ϵ2′​(ξ)Kvv+c1​(ξ)Kvu,

with Kvu(x,x)=−c2(x)/(ϵ1(x)+ϵ2(x))K^{vu}(x,x)=-c_2(x)/(\epsilon_1(x)+\epsilon_2(x))Kvu(x,x)=−c2​(x)/(ϵ1​(x)+ϵ2​(x)) and Kvv(x,0)=(qϵ1(0)/ϵ2(0))Kvu(x,0)K^{vv}(x,0)=(q\epsilon_1(0)/\epsilon_2(0))K^{vu}(x,0)Kvv(x,0)=(qϵ1​(0)/ϵ2​(0))Kvu(x,0). The control law (3.48) is

U(t)=∫01Kvu(1,ξ)u(ξ,t) dξ+∫01Kvv(1,ξ)v(ξ,t) dξ.U(t)=\int_0^1K^{vu}(1,\xi)u(\xi,t)\,d\xi+\int_0^1K^{vv}(1,\xi)v(\xi,t)\,d\xi .U(t)=∫01​Kvu(1,ξ)u(ξ,t)dξ+∫01​Kvv(1,ξ)v(ξ,t)dξ.

The target system is γt=Σ(x)γx\gamma_t=\Sigma(x)\gamma_xγt​=Σ(x)γx​ with α(0,t)=qβ(0,t)\alpha(0,t)=q\beta(0,t)α(0,t)=qβ(0,t) and β(1,t)=0\beta(1,t)=0β(1,t)=0, for γ=[α β]T\gamma=[\alpha\ \beta]^Tγ=[α β]T. The direct transformation is γ=w−∫0xK(x,ξ)w(ξ,t) dξ\gamma=w-\int_0^xK(x,\xi)w(\xi,t)\,d\xiγ=w−∫0x​K(x,ξ)w(ξ,t)dξ (3.23), with the full 2×22\times22×2 kernel KKK of (3.30)–(3.37). The inverse transformation is w=γ+∫0xL(x,ξ)γ(ξ,t) dξw=\gamma+\int_0^xL(x,\xi)\gamma(\xi,t)\,d\xiw=γ+∫0x​L(x,ξ)γ(ξ,t)dξ (3.38), with LLL solving (3.40)–(3.47). The finite time is

tF=∫01(1ϵ1(ξ)+1ϵ2(ξ))dξ.t_F=\int_0^1\left(\frac1{\epsilon_1(\xi)}+\frac1{\epsilon_2(\xi)}\right)d\xi .tF​=∫01​(ϵ1​(ξ)1​+ϵ2​(ξ)1​)dξ.

Formalization targets

Goal: Theorem 3.2 (pp. 6–7)

For q≠0q\neq0q=0, every classical solution of the closed loop satisfies

∀λ>0 ∃c>0:∥w(⋅,t)∥L2≤c e−λt∥w(⋅,0)∥L2(t≥0),andw(x,t)=0  (x∈[0,1], t≥tF).\forall\lambda>0\ \exists c>0:\quad \|w(\cdot,t)\|_{L^2}\le c\,e^{-\lambda t}\|w(\cdot,0)\|_{L^2}\quad(t\ge0),\qquad\text{and}\qquad w(x,t)=0\ \ (x\in[0,1],\ t\ge t_F).∀λ>0 ∃c>0:∥w(⋅,t)∥L2​≤ce−λt∥w(⋅,0)∥L2​(t≥0),andw(x,t)=0  (x∈[0,1], t≥tF​).

Here ccc depends on λ\lambdaλ and the data but not on the solution.

Milestones

  1. Proposition 3.1 (p. 3): the same two conclusions for the target system under the section's q≠0q\neq0q=0 assumption.
  2. §3.2 (p. 5): if KKK solves (3.30)–(3.37), the transformation (3.23) maps every closed-loop solution to a target solution.
  3. §3.3 (p. 6): if LLL solves (3.40)–(3.47), the transformation (3.38) maps every solution of γt=Σγx\gamma_t=\Sigma\gamma_xγt​=Σγx​, α(0,t)=qβ(0,t)\alpha(0,t)=q\beta(0,t)α(0,t)=qβ(0,t), to a solution of (3.1) with u(0,t)=qv(0,t)u(0,t)=qv(0,t)u(0,t)=qv(0,t).
  4. §3.5 (p. 8): the conclusion of Theorem 3.2 for q=0q=0q=0, where (3.37) reads Kvv(x,0)=0K^{vv}(x,0)=0Kvv(x,0)=0.

Significance

The theorem shows that a single linear boundary feedback, computed once from the coefficients, drives every state of the system to zero in exactly the time tFt_FtF​. That time is the sum of the travel times of the two characteristic families across [0,1][0,1][0,1]. Exponential stability at every rate follows. The same feedback, rescaled, is the controller of the paper's main result, Theorem 4.1: local exponential H2H^2H2 stabilization of a quasilinear 2×22\times22×2 system, the subject of mission 3 of this series. The well-posedness of the kernel equations, Theorem A.1, is mission 1.

The result is proved in the paper. As far as is known, none of it has been machine-checked. A formal proof needs Volterra transformations of vector-valued functions with differentiation under a variable-limit integral, explicit solutions of transport equations along characteristics, and L2L^2L2 estimates for integral operators with continuous kernels. These tools apply to backstepping designs well beyond this paper.

Difficulty

Proposition 3.1 and the two mapping statements are calculations: an integration by parts and the explicit solution along characteristics. The difficulty of Theorem 3.2 is the step "the transformation is invertible", which the paper's proof takes for granted. The goal hypothesizes only Kvu,KvvK^{vu},K^{vv}Kvu,Kvv, so it is not enough to state the mapping and the inverse separately. The solver has to recover the full state from the target state: either build the remaining kernels Kuu,KuvK^{uu},K^{uv}Kuu,Kuv and the inverse kernel LLL, or argue directly from the closed (Kvu,Kvv)(K^{vu},K^{vv})(Kvu,Kvv) subsystem. Both routes need existence or uniqueness for Goursat-type problems, which the paper proves only in Appendix A. A second, routine obstacle is that the uniform constant ccc must be extracted from the finite-time interval [0,tF][0,t_F][0,tF​] using bounds on the kernels.

Formalization scope

  • States are w : ℝ → ℝ → Fin 2 → ℝ, space first, with Lean index 0 for the paper's first component.
  • Solutions are classical: jointly C1C^1C1 on R2\mathbb R^2R2, with the equations imposed on [0,1]×[0,∞)[0,1]\times[0,\infty)[0,1]×[0,∞). The value w(⋅,0)w(\cdot,0)w(⋅,0) replaces the paper's initial condition w0∈L2w_0\in L^2w0​∈L2. This is the theorem restricted to classical solutions; Mathlib has no Sobolev-space solution theory for these equations.
  • The coefficients and kernels are functions on R\mathbb RR and R2\mathbb R^2R2 with global regularity, and positivity is assumed only on [0,1][0,1][0,1].
  • The goal and Proposition 3.1 assume q≠0q\neq0q=0, the standing assumption of §§3.1–3.4. The separate §3.5 milestone covers q=0q=0q=0.
  • The right boundary condition of the closed loop is the feedback (3.48) evaluated on the same state, not a free input.
  • Only the "if" direction of the §3.2 equivalence is formalized.

Three trivializing readings are excluded. The constant ccc is quantified after the data and before the solution, so it cannot depend on the solution. The finite-time claim is vanishing for every t≥tFt\ge t_Ft≥tF​, with tFt_FtF​ exactly (3.8), not for some unspecified time. The kernels are pinned down by all four of (3.32), (3.33), (3.36), (3.37). With C1C^1C1 coefficients a solution exists (the paper's Theorem A.2), and a sanity file checks that the hypotheses admit a non-zero closed-loop solution.

Welcome contributions: lemmas on differentiating ∫0xK(x,ξ)w(ξ,t) dξ\int_0^xK(x,\xi)w(\xi,t)\,d\xi∫0x​K(x,ξ)w(ξ,t)dξ, transport equations along characteristics, and the invertibility of Volterra operators with continuous kernels.

The paper's proofs are on pp. 3–5 (Proposition 3.1), p. 5 (§3.2), p. 6 (§3.3) and p. 7 (Theorem 3.2).

Selected references

  • J.-M. Coron, R. Vazquez, M. Krstic, G. Bastin, Local Exponential H2H^2H2 Stabilization of a 2×22\times22×2 Quasilinear Hyperbolic System Using Backstepping, arXiv:1208.6475v1, 2012; SIAM J. Control Optim. 51(3), 2013. https://arxiv.org/abs/1208.6475
  • M. Krstic, A. Smyshlyaev, Backstepping boundary control for first-order hyperbolic PDEs and application to systems with actuator and sensor delays, Systems & Control Letters 57(9), 2008. https://doi.org/10.1016/j.sysconle.2008.02.005
  • M. Krstic, A. Smyshlyaev, Boundary Control of PDEs: A Course on Backstepping Designs, SIAM, 2008. https://doi.org/10.1137/1.9780898718607
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CombinatoricsGraph TheoryLinear algebra·Captain: mikedeng1

A Harary-Sachs Theorem for Hypergraphs: The Codegree-d Coefficient of the Characteristic Polynomial of a k-Graph as a Weighted Sum over Its Veblen InfragraphsResearch Paper

Motivation

The characteristic polynomial of an ordinary graph records spectral information in coefficients that can also be described by finite graph configurations. The classical Harary–Sachs theorem is an instance of this connection. For a uniform hypergraph, the adjacency object is a tensor rather than a matrix, and its characteristic polynomial is defined through a multivariate resultant. Clark and Cooper's hypergraph theorem gives a corresponding coefficient formula. It identifies the configurations that replace the elementary subgraphs of the graph case and assigns them weights determined by directed Eulerian structures. The result makes a tensor spectral invariant accessible through finite combinatorial objects.

The article appeared as Gregory J. Clark and Joshua N. Cooper, A Harary-Sachs theorem for hypergraphs, Journal of Combinatorial Theory, Series B (2021), DOI 10.1016/j.jctb.2021.01.002. This mission follows the pinned arXiv version 2, whose page and theorem numbers are used below.

Setting

A simple kkk-graph H=([n],E)\mathcal H=([n],E)H=([n],E) has a fixed vertex set of nnn labeled vertices and a set EEE of distinct edges, each containing exactly kkk vertices. Isolated vertices remain part of [n][n][n]. The normalized adjacency hypermatrix AH\mathcal A_{\mathcal H}AH​ gives an ordered kkk-tuple the value 1/(k−1)!1/(k-1)!1/(k−1)! when its underlying set is an edge, and zero otherwise. This normalization makes every ordering of the other k−1k-1k−1 vertices contribute the intended total weight.

The characteristic polynomial ϕ(H)\phi(\mathcal H)ϕ(H) is the multivariate resultant of the coordinates of (λI−AH)xk−1(\lambda\mathcal I-\mathcal A_{\mathcal H})x^{k-1}(λI−AH​)xk−1. The resultant is characterized by three conditions: it vanishes exactly when homogeneous coordinate polynomials have a nonzero common complex root, it evaluates to one on the coordinate monomials, and it is irreducible over the complex coefficient field. Its degree in λ\lambdaλ is t=n(k−1)n−1t=n(k-1)^{n-1}t=n(k−1)n−1. The codegree-ddd coefficient ϕd(H)\phi_d(\mathcal H)ϕd​(H) is the coefficient of λt−d\lambda^{t-d}λt−d; this degree is fixed from the source theorem and is not read from an implementation of ϕ\phiϕ.

A multi-hypergraph SSS is a multiset of kkk-element edges. It is Veblen when the degree of every vertex is divisible by kkk. Its flattening discards repeated edges, so SSS is an infragraph of H\mathcal HH when every edge of its flattening belongs to EEE. Components use only vertices covered by edges; a labeled object may still sit in a larger ambient vertex set with unused vertices.

A rooting of SSS is a sequence of its edges, each assigned a root vertex in that edge, with roots in nondecreasing order. An edge rooted at uuu contributes a directed arc u→vu\to vu→v to every other vertex vvv of the edge. Summing these arcs with multiplicity produces a directed multigraph DRD_RDR​. An Euler rooting has balanced in- and out-degrees and connected positive-degree vertices. Its arborescence number τ(DR)\tau(D_R)τ(DR​) counts spanning trees of these active vertices directed toward a specified root, with parallel arcs distinguished. For connected SSS, its associated coefficient is

CS=∑R: DR Eulerianτ(DR)∏v∈V(DR)deg⁡−(v).C_S=\sum_{R:\,D_R\text{ Eulerian}}\frac{\tau(D_R)}{\prod_{v\in V(D_R)}\deg^-(v)}.CS​=R:DR​ Eulerian∑​∏v∈V(DR​)​deg−(v)τ(DR​)​.

For disconnected SSS, CSC_SCS​ is the product of the coefficients of its connected components. These conventions follow Definitions 6–10 in the source.

Formalization targets

Differential trace and Euler rootings

The supporting targets identify when a monomial differential operator contributes to a matrix trace, and show that an Euler rooting determines a connected Veblen multi-hypergraph. The operator identity is counted by Euler tours with distinguishable parallel arcs. The resultant-to-trace identity quoted in the paper is also a milestone:

ϕd(H)=Pd(−Tr⁡1(H)/1,…,−Tr⁡d(H)/d).\phi_d(\mathcal H)=P_d\left(-\operatorname{Tr}_1(\mathcal H)/1,\ldots,-\operatorname{Tr}_d(\mathcal H)/d\right).ϕd​(H)=Pd​(−Tr1​(H)/1,…,−Trd​(H)/d).

Here PdP_dPd​ is the paper's sum over positive compositions of ddd, and Tr⁡j\operatorname{Tr}_jTrj​ is its differential trace from Equation (1).

Harary–Sachs coefficient formula

The goal uses the labeled form of Theorem 14. Let Tm(d,H)\mathscr T_m(d,\mathcal H)Tm​(d,H) be the set of ordered mmm-tuples (S1,…,Sm)(S_1,\ldots,S_m)(S1​,…,Sm​) of connected labeled Veblen infragraphs whose edge counts sum to ddd. Then

ϕd(H)=∑m=1d(−(k−1)n)mm!∑(S1,…,Sm)∈Tm(d,H)∏i=1mCSi.\phi_d(\mathcal H)=\sum_{m=1}^{d}\frac{\bigl(-(k-1)^n\bigr)^m}{m!}\sum_{(S_1,\ldots,S_m)\in\mathscr T_m(d,\mathcal H)}\prod_{i=1}^{m}C_{S_i}.ϕd​(H)=m=1∑d​m!(−(k−1)n)m​(S1​,…,Sm​)∈Tm​(d,H)∑​i=1∏m​CSi​​.

The paper prints the equivalent sum over isomorphism classes, using automorphism groups and the copy weight (#H⊆H)(\#H\subseteq\mathcal H)(#H⊆H). The labeled expression is the result before that grouping. The isomorphism-class statement is outside this mission's Lean target and remains a separate formalization task.

Significance

The theorem expresses a coefficient of a resultant, defined algebraically over complex common roots, as a finite rational weighted sum over hypergraph configurations. It extends the graph case while preserving the exact normalization, sign, component count, and coefficient index. The formula can be used to study low codegree coefficients by enumerating finite Veblen infragraphs and their Euler rootings. Clark and Cooper also use associated coefficients to compare different hypergraph structures in the paper.

The formal development separates the resultant, the differential trace, and the combinatorial counts into reusable definitions. It would provide machine-checked statements of the paper's main equality and several links between those definitions. The Lean theorems in this draft are open targets with sorry placeholders; compiling their statements does not constitute a machine-checked proof of the paper's claims.

Difficulty

The ordinary matrix determinant has a direct expansion by permutations. A tensor characteristic polynomial is a multivariate resultant, so that expansion does not directly reveal which hypergraphs contribute to a coefficient. The trace side uses repeated partial derivatives, and repeated hyperedges can create several distinct rootings with the same directed arc multiplicities. Counting only a multiset of root assignments loses those orderings and changes the coefficient. The Eulerian condition, arborescence multiplicities, and factorial factors must agree simultaneously for the algebraic and combinatorial expressions to match.

Formalization scope

The Lean representation uses Fin n vertices, finite sets of simple edges, multisets of repeated edges, rational adjacency weights, and complex polynomials only for the resultant criterion. It assumes k≥2k\ge2k≥2, n≥1n\ge1n≥1, and 1≤d≤n(k−1)n−11\le d\le n(k-1)^{n-1}1≤d≤n(k−1)n−1. The source fixes k≥2k\ge2k≥2, and the latter two bounds expose the domain in which the printed coefficient expansion and its proof use ddd. An isolated vertex of H\mathcal HH counts in nnn and in (k−1)n(k-1)^n(k−1)n, while isolated vertices do not pad a multi-hypergraph component.

The formalization takes a polynomial satisfying the resultant's common-root, normalization, and irreducibility properties as an input. Separate sanity proofs give witnesses in the one-variable degree-zero and degree-one cases; degree one covers the first goal-domain degree when k=2k=2k=2. The characteristic polynomial is evaluated from this polynomial, never defined by the trace identity. Rootings are sequences, arborescences are directed toward the least positive-degree vertex, and the associated coefficient is calculated on covered vertices. The goal uses the labeled sum, so no automorphism is computed on an ambient padded vertex set. Contributions formalizing the omitted isomorphism-class equivalence, the BEST circuit count, and proofs of the stated targets are welcome.

Selected references

  • Gregory J. Clark and Joshua N. Cooper, A Harary-Sachs theorem for hypergraphs, Journal of Combinatorial Theory, Series B, 2021. arXiv:1812.00468v2; DOI 10.1016/j.jctb.2021.01.002.
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CombinatoricsGraph TheoryGroup Theory·Captain: mikedeng1

Edge-Transitive Bi-Cayley Graphs 3: Every Connected Semisymmetric Bi-Dihedrant Has Valency at Least 6, and Semisymmetric Bi-Dihedrants of Valency 2k Exist for Each Odd k ≥ 3Research Paper

Motivation

A graph may have enough symmetry for every edge to look the same while its vertices still fall into two distinct classes. Such a graph is semisymmetric when it has constant valency, is edge-transitive, and is not vertex-transitive. Conder, Zhou, Feng and Zhang study this phenomenon among bi-Cayley graphs, graphs equipped with a group acting freely on two vertex orbits. Their dihedral case supplies examples related to questions of Marušič and Potočnik about semisymmetric tetracirculants. It also asks how small the valency of a semisymmetric graph with this specific group action can be. The paper states that six is the minimum and that examples occur at every valency 2k2k2k with odd k≥3k\ge3k≥3 (Conder et al., Theorem 1.5 and its introduction, p. 3).

The authors develop the bi-Cayley setting and the relevant automorphism actions before reaching the dihedral result. The lower bound appears as Theorem 6.1, while Example 6.2 defines a graph family and Proposition 6.4 gives a semisymmetry criterion for its odd-kkk members (Conder et al., pp. 11–13). This mission targets those claims within a single formal graph model. The final sentence of Theorem 1.5, concerning an edge-regular family, depends on the separate Theorem 6.5 and is outside this goal.

Setting

Let HHH be a finite group. Choose subsets R,L,S⊆HR,L,S\subseteq HR,L,S⊆H with R−1=RR^{-1}=RR−1=R, L−1=LL^{-1}=LL−1=L, 1∉R∪L1\notin R\cup L1∈/R∪L, and ∣R∣=∣L∣|R|=|L|∣R∣=∣L∣. The graph BiCay⁡(H,R,L,S)\operatorname{BiCay}(H,R,L,S)BiCay(H,R,L,S) has two labelled copies of each element of HHH, written h0h_0h0​ and h1h_1h1​. For each h∈Hh\in Hh∈H, it joins h0h_0h0​ to (xh)0(xh)_0(xh)0​ when x∈Rx\in Rx∈R, joins h1h_1h1​ to (yh)1(yh)_1(yh)1​ when y∈Ly\in Ly∈L, and joins h0h_0h0​ to (zh)1(zh)_1(zh)1​ when z∈Sz\in Sz∈S. These are unoriented edges. Right multiplication by HHH preserves the graph and acts regularly on each of its two vertex copies (Conder et al., pp. 1 and 4).

A bi-dihedrant is a bi-Cayley graph whose group is dihedral. Write Dn=⟨a,b∣an=b2=(ab)2=1⟩D_n=\langle a,b\mid a^n=b^2=(ab)^2=1\rangleDn​=⟨a,b∣an=b2=(ab)2=1⟩ for the dihedral group of degree n≥3n\ge3n≥3. Graph valency is the number of neighbours of a vertex. Connectedness is required throughout the paper. For a semisymmetric graph the common valency exists by definition, but the formal statements quantify over every vertex so that the numerical claims refer to the actual graph degree (Conder et al., definitions on p. 4 and Theorem 6.1 on p. 11).

The constructed family Γ(n,λ,2k)\Gamma(n,\lambda,2k)Γ(n,λ,2k) uses n≥5n\ge5n≥5, k≥2k\ge2k≥2, and a residue λ\lambdaλ of multiplicative order 2k2k2k modulo nnn whose even-power sum vanishes: ∑j=0k−1λ2j=0\sum_{j=0}^{k-1}\lambda^{2j}=0∑j=0k−1​λ2j=0. For 0≤i<k0\le i<k0≤i<k, put ci=∑j=0iλ2jc_i=\sum_{j=0}^{i}\lambda^{2j}ci​=∑j=0i​λ2j and di=λcid_i=\lambda c_idi​=λci​. Set S(n,λ,2k)={aci:0≤i<k}∪{badi:0≤i<k}S(n,\lambda,2k)=\{a^{c_i}:0\le i<k\}\cup\{ba^{d_i}:0\le i<k\}S(n,λ,2k)={aci​:0≤i<k}∪{badi​:0≤i<k}. Then Γ(n,λ,2k)=BiCay⁡(Dn,∅,∅,S(n,λ,2k))\Gamma(n,\lambda,2k)=\operatorname{BiCay}(D_n,\varnothing,\varnothing,S(n,\lambda,2k))Γ(n,λ,2k)=BiCay(Dn​,∅,∅,S(n,λ,2k)) (Conder et al., Example 6.2, pp. 12–13).

Right multiplication R(g):hi↦(hg)iR(g):h_i\mapsto(hg)_iR(g):hi​↦(hg)i​ gives a subgroup R(H)≤Aut⁡(Γ)R(H)\le\operatorname{Aut}(\Gamma)R(H)≤Aut(Γ), and X=NAut⁡(Γ)(R(H))X=N_{\operatorname{Aut}(\Gamma)}(R(H))X=NAut(Γ)​(R(H)) is its normaliser. For α∈Aut⁡(H)\alpha\in\operatorname{Aut}(H)α∈Aut(H) and g,x,y∈Hg,x,y\in Hg,x,y∈H the paper's permutations are σα,g:h0↦(hα)0, h1↦(ghα)1\sigma_{\alpha,g}:h_0\mapsto(h^\alpha)_0,\ h_1\mapsto(gh^\alpha)_1σα,g​:h0​↦(hα)0​, h1​↦(ghα)1​ and δα,x,y:h0↦(xhα)1, h1↦(yhα)0\delta_{\alpha,x,y}:h_0\mapsto(xh^\alpha)_1,\ h_1\mapsto(yh^\alpha)_0δα,x,y​:h0​↦(xhα)1​, h1​↦(yhα)0​; the sets F\mathrm FF and I\mathrm II of (2.2) collect those that preserve the edge rules. A graph is normal edge-transitive when XXX, not merely Aut⁡(Γ)\operatorname{Aut}(\Gamma)Aut(Γ), is transitive on edges (Conder et al., pp. 4–5).

Formalization targets

The milestones, in attack order, are Proposition 2.1(b) (one may assume 1∈S1\in S1∈S), Proposition 2.2 (the normaliser X=R(H)(F∪I)X=R(H)(\mathrm F\cup\mathrm I)X=R(H)(F∪I)), the opening step of the proof of Theorem 6.1 (R=L=∅R=L=\varnothingR=L=∅ for a semisymmetric graph), Theorem 6.1, the claims of Example 6.2, and Proposition 6.4.

Minimum valency

For every connected semisymmetric bi-dihedrant over DnD_nDn​, n≥3n\ge3n≥3, and every vertex vvv,

deg⁡Γ(v)≥6.\deg_{\Gamma}(v)\ge6.degΓ​(v)≥6.

This is Theorem 6.1 and the first claim of Theorem 1.5. The milestone for the proof's opening step records that semisymmetry forces R=L=∅R=L=\varnothingR=L=∅; the theorem itself still ranges over all valid R,L,SR,L,SR,L,S (Conder et al., Theorem 6.1, p. 11).

Examples at every odd index

For each odd integer k≥3k\ge3k≥3, there is a connected semisymmetric bi-dihedrant Γ\GammaΓ such that

deg⁡Γ(v)=2kfor every vertex v.\deg_{\Gamma}(v)=2k\qquad\text{for every vertex }v.degΓ​(v)=2kfor every vertex v.

Example 6.2 is the first milestone toward this claim: under its hypotheses Γ(n,λ,2k)\Gamma(n,\lambda,2k)Γ(n,λ,2k) is connected, ∣S∣=2k|S|=2k∣S∣=2k, every vertex has degree 2k2k2k, and σα,b\sigma_{\alpha,b}σα,b​ for α:(a,b)↦(aλ,ba)\alpha:(a,b)\mapsto(a^\lambda,ba)α:(a,b)↦(aλ,ba) lies in XXX and permutes the neighbours of 101_010​ cyclically, so the graph is normal edge-transitive (Conder et al., p. 13). Proposition 6.4 is the second: under the defining conditions for Γ(n,λ,2k)\Gamma(n,\lambda,2k)Γ(n,λ,2k), odd kkk and λk=−1\lambda^k=-1λk=−1 modulo nnn imply semisymmetry (Conder et al., Proposition 6.4, p. 13). An auxiliary arithmetic theorem states the parameter existence needed to apply it for every odd k≥3k\ge3k≥3.

Significance

The lower bound excludes semisymmetric bi-dihedrants of valency at most five. The existence assertion says that six is attained and places examples at an infinite sequence of larger valencies. Together these claims distinguish the restrictions imposed by a dihedral bi-Cayley action from edge transitivity alone. The construction also gives a concrete family on which questions about stronger automorphism properties can be posed (Conder et al., §6, pp. 11–14).

The result is proved in the cited paper; this mission seeks a machine-checked version of its first two Theorem 1.5 claims. The definition of a bi-Cayley graph, the precise graph symmetry predicates, and the arithmetic parameter family are reusable beyond this particular lower bound. The statements here are open proof targets in Lean, with their mathematical content fixed before proof development. The edge-regular claim from the theorem's final sentence requires additional source results and remains a separate formalization target.

Difficulty

Edge transitivity alone does not make a graph vertex-transitive: a semisymmetric graph is precisely the regular case where that inference fails. The lower bound therefore cannot be obtained by treating every vertex as lying in one automorphism orbit. In the dihedral case, the proof must account for both the rotations and reflections in the connection set, and for the constraints that connectedness and graph automorphisms impose on low-valency possibilities (Conder et al., proof of Theorem 6.1, pp. 11–12).

The existence statement has a distinct arithmetic requirement. Proposition 6.4 is conditional on n,λ,kn,\lambda,kn,λ,k satisfying Example 6.2 and λk=−1\lambda^k=-1λk=−1. The paper asserts examples for every odd k≥3k\ge3k≥3 without spelling out parameters for all such kkk. The auxiliary arithmetic statement records that remaining obligation explicitly; a proof of the conditional proposition alone would not establish the quantified existence claim.

Formalization scope

Lean represents the two vertex copies by H ⊕ H and the dihedral group by Mathlib's DihedralGroup n. The graph is a SimpleGraph built from the three edge rules above, with the inverse-closure and loop-exclusion conditions retained in BiCayData. Semisymmetry uses the full graph automorphism group, unoriented edge transitivity, and constant graph degree. The source's standing finite, connected, simple, and undirected conventions are explicit through finite groups, simple graphs, and connectedness hypotheses. The goal and Theorem 6.1 use n≥3n\ge3n≥3, the range of dihedral groups in §6; the existence examples are also required to be connected.

The definitions do not set valency equal to ∣S∣|S|∣S∣, replace a graph degree by a formula, or make an edge-transitivity claim true by ranging over an empty edge set. The setting requires valid inverse-closed side sets rather than silently symmetrising an invalid one. The arithmetic hypothesis uses the multiplicative order in Z/nZ\mathbb Z/n\mathbb ZZ/nZ and enumerates the indices of Zk\mathbb Z_kZk​ by 0,…,k−10,\ldots,k-10,…,k−1. Normal edge-transitivity in Example 6.2 is stated for the subgroup XXX and semisymmetry for the full group Aut⁡(Γ)\operatorname{Aut}(\Gamma)Aut(Γ); the two are not interchanged. The restriction n≥3n\ge3n≥3 in the lower bound is that of Theorem 6.1 and is a disclosed hypothesis of the goal: D1D_1D1​ and D2D_2D2​ are abelian, and the paper treats bi-Cayley graphs over abelian groups separately. The auxiliary parameter statement is not in the paper; it is supplied so that the existence claim has a complete proof path. The third sentence of Theorem 1.5 is not formalized. Contributions establishing the structural lower bound, the family criterion, or the arithmetic existence statement are all within scope.

Selected references

  • Marston Conder, Jin-Xin Zhou, Yan-Quan Feng and Mi-Mi Zhang, Edge-transitive bi-Cayley graphs, preprint arXiv:1606.04625v1, 2016; published in Journal of Combinatorial Theory, Series B, 2020. Preprint · DOI.
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Edge-Transitive Bi-Cayley Graphs 1: For Connected BiCay(H, ∅, ∅, S), the Normaliser of R(H) Is 2-Arc-Transitive Iff Three Conditions on Aut(H) Hold, and Never 3-Arc-TransitiveResearch Paper

Motivation

A graph is symmetric when its automorphism group moves any vertex, edge or arc to any other, and sss-arc-transitive when it moves any walk of length sss without immediate backtracking to any other. Tutte's work on cubic graphs made sss-arc-transitivity a central measure of symmetry in algebraic graph theory, and most constructions of highly symmetric graphs start from a group acting regularly on vertices (Cayley graphs) or semiregularly with a few orbits.

Bi-Cayley graphs are the case of two orbits: a group HHH acts semiregularly by right multiplication with exactly two vertex orbits. The Petersen graph, the Gray graph (the smallest cubic semisymmetric graph) and the smallest member of Bouwer's family of half-arc-transitive graphs are all bi-Cayley graphs, and all of them are edge-transitive. Deciding edge-transitivity of a bi-Cayley graph is hard in general, but the subgroup of automorphisms that normalise the semiregular group R(H)R(H)R(H) is explicitly known, which makes the "normal" version of the question tractable.

C. H. Li asked whether 3-arc-transitive bi-normal Cayley graphs exist and asked for a description of the 2-arc-transitive ones (Li, Proc. Amer. Math. Soc. 133, Question 1.2(a) and Problem 1.3(b), as cited in the paper, p. 2). M. Conder, J.-X. Zhou, Y.-Q. Feng and M.-M. Zhang answered both through their Theorem 1.1 (arXiv:1606.04625v1; J. Combin. Theory Ser. B, 2020). This mission formalizes that theorem and the lemmas its proof uses.

Setting

Let HHH be a finite group with identity 111. Let R,L,S⊆HR, L, S \subseteq HR,L,S⊆H with ∣R∣=∣L∣|R| = |L|∣R∣=∣L∣, 1∉R=R−11 \notin R = R^{-1}1∈/R=R−1 and 1∉L=L−11 \notin L = L^{-1}1∈/L=L−1. The bi-Cayley graph Γ=BiCay(H,R,L,S)\Gamma = \mathrm{BiCay}(H,R,L,S)Γ=BiCay(H,R,L,S) has vertex set H0∪H1H_0 \cup H_1H0​∪H1​, two disjoint copies of HHH (the copy of hhh in HiH_iHi​ is hih_ihi​), and edges {h0,(xh)0}\{h_0,(xh)_0\}{h0​,(xh)0​}, {h1,(yh)1}\{h_1,(yh)_1\}{h1​,(yh)1​} and {h0,(zh)1}\{h_0,(zh)_1\}{h0​,(zh)1​} for h∈Hh \in Hh∈H, x∈Rx \in Rx∈R, y∈Ly \in Ly∈L, z∈Sz \in Sz∈S. The main theorem concerns R=L=∅R = L = \emptysetR=L=∅, where Γ\GammaΓ is bipartite with parts H0H_0H0​, H1H_1H1​ and every vertex has ∣S∣|S|∣S∣ neighbours.

For g∈Hg \in Hg∈H, R(g):hi↦(hg)iR(g) : h_i \mapsto (hg)_iR(g):hi​↦(hg)i​ is an automorphism of Γ\GammaΓ; these form the subgroup R(H)≤Aut(Γ)R(H) \le \mathrm{Aut}(\Gamma)R(H)≤Aut(Γ), and

X=NAut(Γ)(R(H))X = N_{\mathrm{Aut}(\Gamma)}(R(H))X=NAut(Γ)​(R(H))

is its normaliser. For α∈Aut(H)\alpha \in \mathrm{Aut}(H)α∈Aut(H) (written as an exponent, h↦hαh \mapsto h^\alphah↦hα) and x,y,g∈Hx, y, g \in Hx,y,g∈H the paper defines the permutations

δα,x,y:h0↦(xhα)1, h1↦(yhα)0,σα,g:h0↦(hα)0, h1↦(ghα)1,\delta_{\alpha,x,y} : h_0 \mapsto (xh^\alpha)_1,\ h_1 \mapsto (yh^\alpha)_0, \qquad \sigma_{\alpha,g} : h_0 \mapsto (h^\alpha)_0,\ h_1 \mapsto (gh^\alpha)_1,δα,x,y​:h0​↦(xhα)1​, h1​↦(yhα)0​,σα,g​:h0​↦(hα)0​, h1​↦(ghα)1​,

and the sets I\mathrm{I}I of those δα,x,y\delta_{\alpha,x,y}δα,x,y​ with Rα=x−1LxR^\alpha = x^{-1}LxRα=x−1Lx, Lα=y−1RyL^\alpha = y^{-1}RyLα=y−1Ry, Sα=y−1S−1xS^\alpha = y^{-1}S^{-1}xSα=y−1S−1x, and F\mathrm{F}F of those σα,g\sigma_{\alpha,g}σα,g​ with Rα=RR^\alpha = RRα=R, Lα=g−1LgL^\alpha = g^{-1}LgLα=g−1Lg, Sα=g−1SS^\alpha = g^{-1}SSα=g−1S.

An sss-arc is a sequence (v0,…,vs)(v_0,\dots,v_s)(v0​,…,vs​) of vertices in which consecutive vertices are adjacent and vi−1≠vi+1v_{i-1} \ne v_{i+1}vi−1​=vi+1​. A subgroup K≤Aut(Γ)K \le \mathrm{Aut}(\Gamma)K≤Aut(Γ) is transitive on sss-arcs if any sss-arc can be mapped to any other by an element of KKK; 1-arcs are arcs. Γ\GammaΓ is normal edge-transitive if XXX is transitive on edges, and normal locally arc-transitive if the stabiliser X10X_{1_0}X10​​ is transitive on the neighbourhood Γ(10)\Gamma(1_0)Γ(10​). KKK acts semisymmetrically if it is edge-transitive but not vertex-transitive. Aut(H,Δ)\mathrm{Aut}(H,\Delta)Aut(H,Δ) is the setwise stabiliser of Δ⊆H\Delta \subseteq HΔ⊆H in Aut(H)\mathrm{Aut}(H)Aut(H).

Formalization targets

Goal: Theorem 1.1

Let Γ=BiCay(H,∅,∅,S)\Gamma = \mathrm{BiCay}(H,\emptyset,\emptyset,S)Γ=BiCay(H,∅,∅,S) be connected, with 1∈S1 \in S1∈S and ∣S∣≥2|S| \ge 2∣S∣≥2. Then

X is transitive on the 2-arcs of Γ  ⟺  (a)∧(b)∧(c),X \text{ is transitive on the 2-arcs of } \Gamma \iff \text{(a)} \wedge \text{(b)} \wedge \text{(c)},X is transitive on the 2-arcs of Γ⟺(a)∧(b)∧(c),

where (a) Sα=S−1S^\alpha = S^{-1}Sα=S−1 for some α∈Aut(H)\alpha \in \mathrm{Aut}(H)α∈Aut(H); (b) Aut(H,S∖{1})\mathrm{Aut}(H, S\setminus\{1\})Aut(H,S∖{1}) is transitive on S∖{1}S \setminus \{1\}S∖{1}; (c) Sβ=s−1SS^\beta = s^{-1}SSβ=s−1S for some s∈S∖{1}s \in S\setminus\{1\}s∈S∖{1} and β∈Aut(H)\beta \in \mathrm{Aut}(H)β∈Aut(H). Furthermore, if ∣S∣≥3|S| \ge 3∣S∣≥3, XXX is not transitive on the 3-arcs of Γ\GammaΓ.

Milestones

  • Proposition 2.2 (cited by the paper from Zhou and Feng): for connected Γ\GammaΓ, every element of F\mathrm{F}F and of I\mathrm{I}I is an automorphism in XXX, and X=R(H) (F∪I)X = R(H)\,(\mathrm{F} \cup \mathrm{I})X=R(H)(F∪I).
  • Proposition 2.2(a): for δα,x,y∈I\delta_{\alpha,x,y} \in \mathrm{I}δα,x,y​∈I, ⟨R(H),δα,x,y⟩\langle R(H),\delta_{\alpha,x,y}\rangle⟨R(H),δα,x,y​⟩ is vertex-transitive.
  • Lemma 3.2: X1011={σα,1∣α∈Aut(H,S∖{1})}X_{1_01_1} = \{\sigma_{\alpha,1} \mid \alpha \in \mathrm{Aut}(H,S\setminus\{1\})\}X10​11​​={σα,1​∣α∈Aut(H,S∖{1})}, and, for ∣S∣≥3|S| \ge 3∣S∣≥3, XXX is not 3-arc-transitive.
  • Proposition 3.3: Γ\GammaΓ is normal locally arc-transitive iff Γ(10)\Gamma(1_0)Γ(10​) is an orbit of F\mathrm{F}F; in that case XXX is arc-transitive iff Sα=S−1S^\alpha = S^{-1}Sα=S−1 for some α\alphaα, and semisymmetric otherwise.

A companion item, Lemma 3.1, shows that a connected normal edge-transitive BiCay(H,R,L,S)\mathrm{BiCay}(H,R,L,S)BiCay(H,R,L,S) has R=L=∅R = L = \emptysetR=L=∅; it explains why the goal is stated for BiCay(H,∅,∅,S)\mathrm{BiCay}(H,\emptyset,\emptyset,S)BiCay(H,∅,∅,S).

Significance

Combined with Lemma 3.1, Theorem 1.1 reduces 2-arc-transitivity of the normaliser of R(H)R(H)R(H) to three conditions on Aut(H)\mathrm{Aut}(H)Aut(H) and the single set SSS, all checkable in the group without building the graph. Its second part rules out normal 3-arc-transitive bi-Cayley graphs of valency at least 3, which settles Li's question on 3-arc-transitive bi-normal Cayley graphs negatively. Proposition 3.3 is the arc-transitive versus semisymmetric dichotomy for normal locally arc-transitive bi-Cayley graphs, the starting point of the paper's later constructions of semisymmetric and half-arc-transitive examples.

All results are proved in the paper (Proposition 2.2 by citation). None of them has a machine-checked proof that this mission knows of. Mathlib has simple graphs, graph isomorphisms and normalisers, but no bi-Cayley graphs, no sss-arcs and no transitivity notions for subgroups of Aut(Γ)\mathrm{Aut}(\Gamma)Aut(Γ). A formal proof would supply the first verified description of the normaliser of a semiregular group with two orbits, reusable for any bi-Cayley or bi-circulant result.

Difficulty

The bulk of the work is Proposition 2.2. That σα,g\sigma_{\alpha,g}σα,g​ and δα,x,y\delta_{\alpha,x,y}δα,x,y​ preserve edges exactly under the conditions of (2.2) is a direct computation. The converse is harder: every automorphism normalising R(H)R(H)R(H) must be one of these permutations composed with some R(h)R(h)R(h). That needs the conjugation action of XXX on R(H)R(H)R(H) to induce an automorphism of HHH, and XXX to preserve the partition {H0,H1}\{H_0, H_1\}{H0​,H1​} into R(H)R(H)R(H)-orbits.

The 3-arc clause looks like a stabiliser count, but it holds only once 111_111​ has at least two neighbours besides 101_010​: for ∣S∣=2|S| = 2∣S∣=2 the graph is a cycle of length 2∣H∣2|H|2∣H∣, the normaliser is the whole dihedral automorphism group, and that group is transitive on 3-arcs. Any proof must use ∣S∣≥3|S| \ge 3∣S∣≥3 at exactly this step.

Formalization scope

The vertex set is H ⊕ H (Sum.inl h =h0= h_0=h0​, Sum.inr h =h1= h_1=h1​). The data (R,L,S)(R, L, S)(R,L,S) is a structure of three Finsets carrying the side conditions R−1=RR^{-1} = RR−1=R, L−1=LL^{-1} = LL−1=L, 1∉R1 \notin R1∈/R, 1∉L1 \notin L1∈/L and ∣R∣=∣L∣|R| = |L|∣R∣=∣L∣. Adjacency is given directly by the three edge rules. Aut(Γ)\mathrm{Aut}(\Gamma)Aut(Γ) is the group Γ ≃g Γ, R(H)R(H)R(H) is the subgroup generated by the R(g)R(g)R(g), and XXX is its Subgroup.normalizer. Automorphisms of HHH are MulAut H, and Δα\Delta^\alphaΔα is the image of Δ\DeltaΔ under α\alphaα. σα,g\sigma_{\alpha,g}σα,g​ and δα,x,y\delta_{\alpha,x,y}δα,x,y​ are permutations of H ⊕ H, and "σα,g∈X\sigma_{\alpha,g} \in Xσα,g​∈X" means that some element of XXX has σα,g\sigma_{\alpha,g}σα,g​ as its vertex map. Products are written pointwise to avoid the composition-order convention of the group of graph automorphisms. An sss-arc is a function on Fin (s+1).

The paper assumes throughout that groups and graphs are finite and graphs connected; each theorem carries Fintype H and connectivity. Three hypotheses are added to the printed Theorem 1.1, each needed for the statement to be true or non-vacuous: 1∈S1 \in S1∈S (the paper's normalisation of a bi-Cayley triple, used by conditions (b) and (c) and by the proof); ∣S∣≥2|S| \ge 2∣S∣≥2 (for ∣S∣=1|S| = 1∣S∣=1 the graph is K2K_2K2​, which has no 2-arcs, so 2-arc-transitivity would hold vacuously while (c) fails); and ∣S∣≥3|S| \ge 3∣S∣≥3 for the 3-arc clause (false for cycles). Lemma 3.2 carries the same 1∈S1 \in S1∈S and ∣S∣≥3|S| \ge 3∣S∣≥3, and Proposition 3.3 carries 1∈S1 \in S1∈S.

Trivializing formalizations are ruled out in four ways. 2-arc-transitivity is never vacuous, since ∣S∣≥2|S| \ge 2∣S∣≥2 guarantees 2-arcs. RRR and LLL are never symmetrised silently, since the side conditions are data rather than repairs. Every transitivity statement is about XXX, not the full Aut(Γ)\mathrm{Aut}(\Gamma)Aut(Γ). Valency is the degree in the graph, never a formula in ∣S∣|S|∣S∣.

Contributions are welcome at every level: proofs of the milestones, a general library of bi-Cayley graphs and their normalisers, and lemmas on sss-arcs and stabilisers in SimpleGraph. The definitions are repeated identically in the companion missions on bi-abelian graphs and bi-dihedrants.

Selected references

  • M. Conder, J.-X. Zhou, Y.-Q. Feng and M.-M. Zhang, Edge-transitive bi-Cayley graphs, arXiv:1606.04625v1, 2016; J. Combin. Theory Ser. B, 2020. https://arxiv.org/abs/1606.04625v1, https://doi.org/10.1016/j.jctb.2020.05.006
  • J.-X. Zhou and Y.-Q. Feng, The automorphisms of bi-Cayley graphs, J. Combin. Theory Ser. B 116 (2016) 504–532 (reference [55] of the paper; source of Proposition 2.2). https://doi.org/10.1016/j.jctb.2015.10.004
  • C. H. Li, Finite s-arc transitive Cayley graphs and flag transitive projective planes, Proc. Amer. Math. Soc. 133 (2005) 31–41 (reference [29] of the paper; Question 1.2(a) and Problem 1.3(b)). https://doi.org/10.1090/S0002-9939-04-07549-5
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Edge-Transitive Bi-Cayley Graphs 2: Edge-Transitive Bi-Cayley Graphs over Abelian Groups Are Vertex-Transitive, and Half-Arc-Transitive Ones Have Valency at Least 6Research Paper

Why bi-Cayley graphs over abelian groups matter

A Cayley graph turns multiplication in a group into adjacency between vertices. Every Cayley graph is vertex transitive: multiplying every vertex by the same group element moves any chosen vertex to any other. A bi-Cayley graph starts with two copies of a group and permits edges both within and between the copies. Its built-in group action is transitive on each copy, but it need not exchange them. This makes bi-Cayley graphs a setting for distinguishing edge, vertex, and arc transitivity. Conder, Zhou, Feng and Zhang study these distinctions and their consequences for graph constructions in Edge-transitive bi-Cayley graphs.

For abelian groups, the paper proves a strong restriction: once a connected bi-Cayley graph is edge transitive, it is also vertex transitive. Its half-arc-transitive examples face additional local restrictions, including a minimum valency of six. The paper exhibits a graph of valency six in Example 4.3, so the numerical bound is attained in its class. The result separates these graphs from semisymmetric graphs, which are edge transitive but not vertex transitive. The claims and example appear in Proposition 1.3 and §4.

Graphs, actions, and terminology

Let HHH be a finite group and let R,L,SR,L,SR,L,S be subsets of HHH. Require R=R−1R=R^{-1}R=R−1, L=L−1L=L^{-1}L=L−1, 1∉R∪L1\notin R\cup L1∈/R∪L, and ∣R∣=∣L∣|R|=|L|∣R∣=∣L∣. The graph Γ=BiCay⁡(H,R,L,S)\Gamma=\operatorname{BiCay}(H,R,L,S)Γ=BiCay(H,R,L,S) has vertices H0∪H1H_0\cup H_1H0​∪H1​, two labelled copies of HHH. For h∈Hh\in Hh∈H, an element x∈Rx\in Rx∈R gives an edge from h0h_0h0​ to (xh)0(xh)_0(xh)0​; an element y∈Ly\in Ly∈L gives an edge from h1h_1h1​ to (yh)1(yh)_1(yh)1​; and an element z∈Sz\in Sz∈S gives an edge from h0h_0h0​ to (zh)1(zh)_1(zh)1​. The inverse closure of RRR and LLL makes the within-copy edges undirected. Excluding 111 from those two sets excludes loops. This is the construction on p. 1.

Every g∈Hg\in Hg∈H acts by right multiplication R(g):hi↦(hg)iR(g):h_i\mapsto(hg)_iR(g):hi​↦(hg)i​. The subgroup R(H)R(H)R(H) of graph automorphisms has two vertex orbits, H0H_0H0​ and H1H_1H1​. Its normaliser in Aut⁡(Γ)\operatorname{Aut}(\Gamma)Aut(Γ) is useful for describing further symmetries. For a group automorphism α\alphaα and group elements g,x,yg,x,yg,x,y, the paper defines permutations σα,g\sigma_{\alpha,g}σα,g​, which preserve the two copies, and δα,x,y\delta_{\alpha,x,y}δα,x,y​, which exchange them. Their precise edge-preservation conditions are the sets FFF and III of equation (2.2). The mission includes those definitions and the relevant part of the normaliser characterization, Proposition 2.2.

A graph is vertex transitive if its full automorphism group can move any vertex to any other, and edge transitive if it can move any undirected edge to any other. Arc transitivity asks the same for ordered adjacent pairs. A graph is half-arc-transitive when it is vertex and edge transitive but not arc transitive. A semisymmetric graph has constant valency, is edge transitive, and is not vertex transitive. These are the paper's definitions on p. 4. Valency means the actual number of neighbours of a vertex.

Formalization targets

The central target is the corrected reading of Proposition 1.3: for connected Γ\GammaΓ over an abelian HHH,

Γ edge transitive  ⟹  Γ vertex transitive,\Gamma\text{ edge transitive}\implies\Gamma\text{ vertex transitive},Γ edge transitive⟹Γ vertex transitive,

and, if Γ\GammaΓ is half-arc-transitive,

R∪L≠∅,(∀x∈R∪L) ord⁡(x)≠2,∣R∣=∣L∣ is even,∣S∣>2,deg⁡Γ(v)≥6(v∈V(Γ)).R\cup L\ne\varnothing,\quad (\forall x\in R\cup L)\ \operatorname{ord}(x)\ne2, \quad |R|=|L|\text{ is even},\quad |S|>2,\quad \deg_{\Gamma}(v)\ge6\quad(v\in V(\Gamma)).R∪L=∅,(∀x∈R∪L) ord(x)=2,∣R∣=∣L∣ is even,∣S∣>2,degΓ​(v)≥6(v∈V(Γ)).

The attack path records the normaliser characterization in Proposition 2.2, both parts of Proposition 4.1, its explicit bipartition step, and Proposition 4.2. The companion Corollary 4.4 expresses the absence of connected semisymmetric examples over abelian groups.

What the result establishes

The vertex-transitivity conclusion collapses one apparent possibility in the symmetry classification: an edge-transitive bi-Cayley graph over an abelian group cannot be semisymmetric. For half-arc-transitive graphs, the theorem rules out involutions in the within-copy connection sets, forces even set sizes, and excludes valencies below six. Example 4.3 supplies an attained bound, with H=C28H=C_{28}H=C28​ and valency six. These are concrete restrictions on any later classification or construction in this family; they follow from §4.

The mathematical results are proved in the cited paper. The mission asks for machine-checked Lean proofs of their statements and for a reusable finite bi-Cayley graph interface. The setting includes the right regular action, its normaliser, the two families of candidate automorphisms, and the transitivity predicates. The proof obligations are open in this local proposal; a successful development would make the abelian argument and its underlying graph-action lemmas available for later formalizations of bi-Cayley graphs.

The main obstacle

The right multiplication action gives only two known vertex orbits, one for each copy of HHH. Edge transitivity alone does not name an automorphism that swaps them. Inversion is an automorphism of an abelian group, but its induced copy-swapping permutation preserves graph edges directly only in the relevant bipartite case R=L=∅R=L=\varnothingR=L=∅. The paper must account for edge-transitive graphs whose connection sets initially allow edges inside the copies. For the valency bound, the absence of arc transitivity restricts how a vertex stabiliser can permute its neighbours; degree counting without those orbit constraints cannot yield ∣S∣>2|S|>2∣S∣>2. These are the points at which a proof must use the full automorphism action rather than just the visible right regular subgroup.

Formalization scope

Lean uses the vertex type H⊔HH\sqcup HH⊔H, with Sum.inl h for h0h_0h0​ and Sum.inr h for h1h_1h1​. The group and graph are finite; the graph is simple and undirected by construction, and every theorem assumes it is connected. The finite sets R,L,SR,L,SR,L,S retain the conditions R=R−1R=R^{-1}R=R−1, L=L−1L=L^{-1}L=L−1, 1∉R∪L1\notin R\cup L1∈/R∪L, and ∣R∣=∣L∣|R|=|L|∣R∣=∣L∣. The graph's degree, rather than a separately defined cardinality formula, represents valency. “Involution” means an element of order exactly two. All graph-level transitivity predicates quantify over the full automorphism group; the normaliser appears only in the separate Proposition 2.2 milestone. The paper's exponent notation for group automorphisms is rendered as function application, while R(g)R(g)R(g) remains right multiplication.

The printed first sentence of Proposition 1.3 says every connected bi-Cayley graph over an abelian group is vertex transitive. That sentence is false: the connected generalized Petersen graph GP(7,2)GP(7,2)GP(7,2) is a bi-Cayley graph over C7C_7C7​ and is not vertex transitive. Proposition 4.1(b), which the paper uses to establish Proposition 1.3, includes the missing edge-transitivity condition. The Lean goal states that corrected condition explicitly. It does not add an assumption to the half-arc-transitive clause, since half-arc-transitivity already entails edge transitivity. Proposition 4.2 prints two clauses labelled “(a)”; they are treated as distinct clauses while its quotation retains the printed labels.

The definition of the graph keeps RRR and LLL inverse closed as data; no graph constructor silently symmetrises arbitrary sets. Transitivity is taken over actual edges or arcs, and the degree bound is checked at every vertex. Contributions to the graph-action lemmas, the normaliser result, Proposition 4.1, and the vertex-stabiliser analysis behind Proposition 4.2 are all within scope. The Cayley-graph isomorphism in Proposition 2.2(b) is outside this mission's stated milestone because it is not used by the target.

Selected references

  • M. Conder, J.-X. Zhou, Y.-Q. Feng, and M.-M. Zhang, Edge-transitive bi-Cayley graphs, Journal of Combinatorial Theory, Series B, 2020; arXiv:1606.04625v1; DOI:10.1016/j.jctb.2020.05.006.
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CombinatoricsDiscrete Geometry·Captain: mikedeng1

Many Non-Equivalent Realizations of the Associahedron 2: Two Hohlweg–Lange Associahedra Are Normally Isomorphic iff Their Sign Sequences Agree up to Reflection and ReversalResearch Paper

Motivation

The associahedron Assn\mathrm{Ass}_nAssn​ is the nnn-dimensional simple polytope whose faces correspond to the sets of pairwise non-crossing diagonals of a convex (n+3)(n+3)(n+3)-gon, ordered by reverse inclusion: its vertices are the triangulations of the polygon and its facets are the diagonals. It appears in homotopy theory (Stasheff), in the theory of cluster algebras of type AAA, and as the secondary polytope of a convex polygon. Many explicit realizations are known, and a natural question is which of them are genuinely different.

Ceballos, Santos and Ziegler (arXiv:1109.5544, Combinatorica 2014) compare realizations up to normal isomorphism: two polytopes are normally isomorphic if some linear isomorphism of the ambient spaces sends every cone of one normal fan to a cone of the other (their Definition 2.1). This notion ignores the right-hand sides of the defining inequalities and keeps only the linear structure of the facet normals, which is what the classical constructions fix.

One family of realizations is due to Hohlweg and Lange (arXiv:math/0510614, Discrete Comput. Geom. 2007): one associahedron AssnI(σ)\mathrm{Ass}^I_n(\sigma)AssnI​(σ) for every sign sequence σ∈{+,−}n−1\sigma \in \{+,-\}^{n-1}σ∈{+,−}n−1. The constant sequence gives Loday's associahedron (arXiv:math/0212126), and the alternating sequence gives, up to normal isomorphism, the Chapoton–Fomin–Zelevinsky associahedron (arXiv:math/0202004). This mission formalizes the classification of the Hohlweg–Lange family up to normal isomorphism, Theorem 4.9 of Ceballos–Santos–Ziegler.

Setting

Fix n≥0n \ge 0n≥0. The vertices of a convex (n+3)(n+3)(n+3)-gon are its positions 0,…,n+20, \dots, n+20,…,n+2 in counterclockwise order. A diagonal joins two distinct non-adjacent positions; two diagonals cross when their endpoints are distinct and alternate around the boundary. The dihedral symmetries are the 2(n+3)2(n+3)2(n+3) maps i↦r+ii \mapsto r + ii↦r+i and i↦r−ii \mapsto r - ii↦r−i modulo n+3n+3n+3.

For σ∈{+,−}n−1\sigma \in \{+,-\}^{n-1}σ∈{+,−}n−1, the sign word σ~={+,−,σ,−,+}\widetilde\sigma = \{+,-,\sigma,-,+\}σ={+,−,σ,−,+} assigns signs to the labels 0,1,…,n+20, 1, \dots, n+20,1,…,n+2. The polygon Pn+3(σ)P_{n+3}(\sigma)Pn+3​(σ) places the labels from left to right, positive ones above a horizontal line and negative ones below; going counterclockwise, it visits the negative labels in increasing order and then the positive labels in decreasing order. For a diagonal ijijij with labels i<ji < ji<j, the set Rij(σ)R_{ij}(\sigma)Rij​(σ) consists of the labels strictly below the diagonal, and Sij(σ)⊆[n+1]={1,…,n+1}S_{ij}(\sigma) \subseteq [n+1] = \{1,\dots,n+1\}Sij​(σ)⊆[n+1]={1,…,n+1} is obtained from it by replacing 000 by iii and n+2n+2n+2 by jjj. The facet of AssnI(σ)\mathrm{Ass}^I_n(\sigma)AssnI​(σ) for the diagonal δ\deltaδ has normal vector eSδ(σ)e_{S_\delta(\sigma)}eSδ​(σ)​, the characteristic vector of Sδ(σ)S_\delta(\sigma)Sδ​(σ) taken modulo e[n+1]=(1,…,1)e_{[n+1]} = (1, \dots, 1)e[n+1]​=(1,…,1). In coordinates this is the vector

vδ(σ)=(1[k∈Sδ(σ)]−1[n+1∈Sδ(σ)])k=1,…,n∈Rn.v_\delta(\sigma) = \big(\mathbf 1[k \in S_\delta(\sigma)] - \mathbf 1[n+1 \in S_\delta(\sigma)]\big)_{k = 1, \dots, n} \in \mathbb R^n .vδ​(σ)=(1[k∈Sδ​(σ)]−1[n+1∈Sδ​(σ)])k=1,…,n​∈Rn.

The normal fan of AssnI(σ)\mathrm{Ass}^I_n(\sigma)AssnI​(σ) is the collection of cones R≥0{vδ(σ):δ∈D}\mathbb R_{\ge 0}\{v_\delta(\sigma) : \delta \in D\}R≥0​{vδ​(σ):δ∈D}, one for each set DDD of pairwise non-crossing diagonals. Two facets are parallel when their normals are negative multiples of each other. The reflection of σ\sigmaσ is −σ-\sigma−σ (all signs flipped), and its reversal σt\sigma^tσt is σ\sigmaσ read backwards.

Formalization targets

Goal: Theorem 4.9

For all σ1,σ2∈{+,−}n−1\sigma_1, \sigma_2 \in \{+,-\}^{n-1}σ1​,σ2​∈{+,−}n−1,

AssnI(σ1) and AssnI(σ2) are normally isomorphic  ⟺  σ2∈{σ1,−σ1,σ1t,−σ1t}.\mathrm{Ass}^I_n(\sigma_1) \text{ and } \mathrm{Ass}^I_n(\sigma_2) \text{ are normally isomorphic} \iff \sigma_2 \in \{\sigma_1, -\sigma_1, \sigma_1^t, -\sigma_1^t\}.AssnI​(σ1​) and AssnI​(σ2​) are normally isomorphic⟺σ2​∈{σ1​,−σ1​,σ1t​,−σ1t​}.

Both directions are content.

Milestones

  1. Lemma 2.2. Every bijection of the diagonals that preserves crossing is induced by a dihedral symmetry; for n≥2n \ge 2n≥2, that symmetry is unique.
  2. The fan-isomorphism step. A linear isomorphism of the two normal fans induces a crossing-preserving bijection of the diagonals that maps parallel pairs to parallel pairs.
  3. Proposition 4.7. AssnI(σ)\mathrm{Ass}^I_n(\sigma)AssnI​(σ) has exactly nnn pairs of parallel facets, with normals e[j]e_{[j]}e[j]​ and e[j]‾e_{\overline{[j]}}e[j]​​. They are the diagonals of explicit quadrilaterals {i,j,j+1,k}\{i, j, j+1, k\}{i,j,j+1,k}.
  4. The four diagonals. The diagonals crossing at least one member of every parallel pair are those joining {0,1}\{0,1\}{0,1} to {n+1,n+2}\{n+1, n+2\}{n+1,n+2}.
  5. Rigidity. A dihedral symmetry mapping the parallel pairs of Pn+3(σ1)P_{n+3}(\sigma_1)Pn+3​(σ1​) onto those of Pn+3(σ2)P_{n+3}(\sigma_2)Pn+3​(σ2​) forces σ2∈{σ1,−σ1,σ1t,−σ1t}\sigma_2 \in \{\sigma_1, -\sigma_1, \sigma_1^t, -\sigma_1^t\}σ2​∈{σ1​,−σ1​,σ1t​,−σ1t​}.
  6. Reflection. AssnI(σ)≅AssnI(−σ)\mathrm{Ass}^I_n(\sigma) \cong \mathrm{Ass}^I_n(-\sigma)AssnI​(σ)≅AssnI​(−σ), with {Sδ(−σ)}={[n+1]∖Sδ(σ)}\{S_\delta(-\sigma)\} = \{[n+1] \setminus S_\delta(\sigma)\}{Sδ​(−σ)}={[n+1]∖Sδ​(σ)}.
  7. Reversal. AssnI(σ)≅AssnI(σt)\mathrm{Ass}^I_n(\sigma) \cong \mathrm{Ass}^I_n(\sigma^t)AssnI​(σ)≅AssnI​(σt), with {Sδ(σt)}={τ(Sδ(σ))}\{S_\delta(\sigma^t)\} = \{\tau(S_\delta(\sigma))\}{Sδ​(σt)}={τ(Sδ​(σ))} for τ(i)=n+2−i\tau(i) = n + 2 - iτ(i)=n+2−i.

Significance

The theorem gives an exact count. The number of normally non-isomorphic Hohlweg–Lange associahedra equals the number of sign sequences of length n−1n-1n−1 up to reflection and reversal, which is 2n−3+2⌊(n−3)/2⌋2^{n-3} + 2^{\lfloor (n-3)/2 \rfloor}2n−3+2⌊(n−3)/2⌋ for n≥3n \ge 3n≥3 (OEIS A005418). Together with Hohlweg–Lange's identification of the constant and alternating sequences, it shows that Loday's associahedron and the Chapoton–Fomin–Zelevinsky associahedron are not normally isomorphic for n≥3n \ge 3n≥3. It is one of the two classifications on which the paper's main result (Theorem 6.1, that the Hohlweg–Lange and Santos families meet only in the Chapoton–Fomin–Zelevinsky associahedron) rests.

Bergeron, Hohlweg, Lange and Thomas (Isometry classes of generalized associahedra, Sém. Lothar. Combin. 61A, 2009) classified the same family up to isometry of normal fans and obtained the same classes. As Remark 4.10 of the paper explains, that classification does not imply this one, because a normal isomorphism need not be an isometry. Combining the two gives Proposition 4.11, that normal isomorphism and isometry coincide for this family.

Theorem 4.9 is proved in the paper; no machine-checked version is known. A formalization would supply the first formal treatment of the crossing graph of polygon diagonals and its automorphisms (Lemma 2.2), of the Hohlweg–Lange normal vectors, and of linear isomorphisms of simplicial fans given by rays on diagonals.

Difficulty

The "if" direction needs two explicit linear isomorphisms. Their action on the sets SδS_\deltaSδ​ is not diagonal by diagonal: Pn+3(σ)P_{n+3}(\sigma)Pn+3​(σ) and Pn+3(−σ)P_{n+3}(-\sigma)Pn+3​(−σ) have different boundary edges, so the matching of diagonals goes through a mirror image and through the sign swaps of Remark 4.2. One must show that this matching preserves the cone structure, not just the set of normals.

The "only if" direction cannot compare the two polygons by label, since Pn+3(σ1)P_{n+3}(\sigma_1)Pn+3​(σ1​) and Pn+3(σ2)P_{n+3}(\sigma_2)Pn+3​(σ2​) order their labels differently around the boundary. A linear isomorphism of fans first has to be turned into a combinatorial object. Linearity has to be used twice: it maps rays to rays and preserves cones, which yields a crossing-preserving bijection, and it preserves opposite pairs of normals. Lemma 2.2 then reduces that bijection to one of 2n+62n+62n+6 dihedral symmetries. The remaining step is a case analysis showing that a symmetry preserving the parallel pairs, and the four distinguished diagonals they determine, is a reflection or reversal of σ~\widetilde\sigmaσ. Comparing the multisets of normal vectors alone is not enough: every σ\sigmaσ gives exactly nnn parallel pairs with the same normals ±e[j]\pm e_{[j]}±e[j]​.

Formalization scope

  • Polygon conventions. Polygon vertices are Fin (n + 3), diagonals are Sym2 (Fin (n + 3)), and crossing, diagonal and triangulation come from the published definition ChvatalArtGallery.FanPartition.Triangulation, used as a reference item. Signs are Bool, and σ\sigmaσ is a function Fin (n - 1) → Bool. Positions and labels are kept apart: hlLabel n σ p is the label at position p.
  • Fan-level encoding. All statements are about normal fans, not polytopes. The normal fan of AssnI(σ)\mathrm{Ass}^I_n(\sigma)AssnI​(σ) is encoded as the fan of the vectors vδ(σ)v_\delta(\sigma)vδ​(σ), with one cone per set of pairwise non-crossing diagonals. That this is its normal fan is Hohlweg–Lange's theorem (Proposition 4.3 of the paper, [17, Prop. 1.3]), assumed by the encoding and not proved. The projection modulo e[n+1]e_{[n+1]}e[n+1]​ is x↦(xk−xn+1)k≤nx \mapsto (x_k - x_{n+1})_{k \le n}x↦(xk​−xn+1​)k≤n​; linear-isomorphism classes do not depend on this choice.
  • Normal isomorphism. This is Definition 2.1 read literally: a LinearEquiv that sends every cone of the first fan to a cone of the second.
  • Corrected statements. Three printed slips are corrected:
    • In the four-diagonal claim, only those of the four label pairs that are diagonals count. For constant σ\sigmaσ one of them is a polygon edge.
    • The complement in milestone 6 is taken in [n+1][n+1][n+1], where the page prints [n][n][n].
    • The reversal in milestone 7 is τ(i)=n+2−i\tau(i) = n+2-iτ(i)=n+2−i, where the page prints n+1−in+1-in+1−i.
  • Dimension threshold. Lemma 2.2 applies n≥2n \ge 2n≥2 only to uniqueness, exactly as the page does; existence holds also for n=0,1n=0,1n=0,1.
  • Ruled-out trivializations. The isomorphism must be linear, since a homeomorphism or a bijection of cones would identify every pair. Cones are nonnegative spans of the actual vectors vδ(σ)v_\delta(\sigma)vδ​(σ), not index sets. Symmetries of the polygon are the 2(n+3)2(n+3)2(n+3) dihedral maps, not arbitrary permutations of the vertices.
  • What to build. Lemma 2.2 and the fan-isomorphism step are reusable for every classification of associahedra by normal fans, including the Santos family in the companion missions. Contributions to Lemma 2.2 and to the simplicial-fan step are particularly welcome.

Selected references

  • C. Ceballos, F. Santos, G. M. Ziegler, Many non-equivalent realizations of the associahedron, Combinatorica 34 (2014); arXiv:1109.5544v2. https://arxiv.org/abs/1109.5544
  • C. Hohlweg, C. E. M. C. Lange, Realizations of the associahedron and cyclohedron, Discrete Comput. Geom. 37 (2007). https://arxiv.org/abs/math/0510614
  • J.-L. Loday, Realization of the Stasheff polytope, Arch. Math. 83 (2004). https://arxiv.org/abs/math/0212126
  • F. Chapoton, S. Fomin, A. Zelevinsky, Polytopal realizations of generalized associahedra, Canad. Math. Bull. 45 (2002). https://arxiv.org/abs/math/0202004
  • N. Bergeron, C. Hohlweg, C. Lange, H. Thomas, Isometry classes of generalized associahedra, Sém. Lothar. Combin. 61A (2009).
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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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Convex OptimizationMachine LearningOptimization·Captain: mikedeng1

Katyusha: The First Direct Acceleration of Stochastic Gradient Methods 1: Katyusha Converges at the Accelerated Linear Rate (1+√(σ/(3Lm)))^(−Sm) on Strongly Convex Finite SumsResearch Paper

Motivation

A finite-sum optimization problem asks for one vector that performs well across many component objectives. In empirical risk minimization, each component can represent the loss from one data point. A full gradient uses every component, whereas a stochastic gradient uses one component and can be much cheaper per step. The latter carries sampling noise, so a method must control that noise while moving toward the optimum. Allen-Zhu's Katyusha paper gives a direct accelerated stochastic method for this setting. Its strongly convex result, Theorem 2.1, bounds the expected objective error of a specified algorithm after a specified number of epochs.

The problem is relevant when the number of terms is large enough that a full gradient at every iteration is costly, but individual component gradients and proximal steps remain practical. Katyusha combines a periodically refreshed full gradient with individual component gradients. The paper's result concerns the actual returned snapshot of Algorithm 1, Option I, whose weighted averaging rule matters to the claim. Formalizing a generic noisy gradient method would leave the paper's central algorithmic guarantee unstated.

Setting

Let f1,…,fn:Rd→Rf_1,\ldots,f_n:\mathbb R^d\to\mathbb Rf1​,…,fn​:Rd→R be differentiable functions, with n≥1n\ge1n≥1. Their finite-sum objective is f(x)=n−1∑i=1nfi(x)f(x)=n^{-1}\sum_{i=1}^n f_i(x)f(x)=n−1∑i=1n​fi​(x). A real-valued regularizer ψ\psiψ gives the composite objective

F(x)=f(x)+ψ(x).F(x)=f(x)+\psi(x).F(x)=f(x)+ψ(x).

Each fif_ifi​ is convex and LLL smooth: its gradient is LLL Lipschitz in the Euclidean norm. The regularizer is σ\sigmaσ strongly convex, with L,σ>0L,\sigma>0L,σ>0, in the paper's convention that the quadratic term has coefficient σ/2\sigma/2σ/2. The comparison point x∗x^*x∗ minimizes the full objective FFF.

Algorithm 1 starts from x0x_0x0​ and keeps three vectors: a snapshot x~\widetilde xx, a proximal sequence zzz, and another proximal sequence yyy. In each epoch it computes ∇f(x~)\nabla f(\widetilde x)∇f(x). At a current point xxx, it samples iii uniformly from {1,…,n}\{1,\ldots,n\}{1,…,n} and forms the gradient estimator

∇~=∇f(x~)+∇fi(x)−∇fi(x~).\widetilde\nabla=\nabla f(\widetilde x)+\nabla f_i(x)-\nabla f_i(\widetilde x).∇=∇f(x)+∇fi​(x)−∇fi​(x).

The algorithm then makes two proximal updates using ∇~\widetilde\nabla∇ and ψ\psiψ. Its next snapshot is a weighted average of the new yyy values, with weights (1+ασ)j(1+\alpha\sigma)^j(1+ασ)j for j=0,…,m−1j=0,\ldots,m-1j=0,…,m−1. The iterates yyy and zzz persist between epochs. In the theorem's run the epoch length is m=2nm=2nm=2n, and τ2=1/2\tau_2=1/2τ2​=1/2, τ1=min⁡{mσ/3L,1/2}\tau_1=\min\{\sqrt{m\sigma}/\sqrt{3L},1/2\}τ1​=min{mσ​/3L​,1/2}, and α=1/(3τ1L)\alpha=1/(3\tau_1L)α=1/(3τ1​L). The output after SSS epochs is x~S\widetilde x^SxS.

Formalization targets

Theorem 2.1: objective error after SSS epochs

For every starting point x0x_0x0​ and minimizer x∗x^*x∗ of FFF, the target is the paper's two-case expected bound:

EF(x~S)−F(x∗)≤{4(1+σ/(3Lm))−Sm(F(x0)−F(x∗)),mσ/L≤3/4,3(2/3)S(F(x0)−F(x∗)),mσ/L>3/4.\mathbb E F(\widetilde x^S)-F(x^*)\le\begin{cases}4(1+\sqrt{\sigma/(3Lm)})^{-Sm}\bigl(F(x_0)-F(x^*)\bigr),&m\sigma/L\le3/4,\\3(2/3)^S\bigl(F(x_0)-F(x^*)\bigr),&m\sigma/L>3/4.\end{cases}EF(xS)−F(x∗)≤{4(1+σ/(3Lm)​)−Sm(F(x0​)−F(x∗)),3(2/3)S(F(x0​)−F(x∗)),​mσ/L≤3/4,mσ/L>3/4.​

The expectation is over every independent uniform index sampled by the run. The two regimes meet at the threshold where the algorithm's minimum defining τ1\tau_1τ1​ changes branch. The milestone list follows Lemmas 2.3–2.7 and the displayed one-epoch inequalities of Section 2.2. It includes the variance bound, the proximal estimates, and the two regime-specific epoch estimates that feed the final theorem.

Significance

The theorem gives an accelerated linear reduction of the expected composite-objective error under the paper's strong convexity assumptions. It identifies how the rate depends on component count nnn, smoothness LLL, strong convexity σ\sigmaσ, and epoch count SSS. The author also translates the result into an iteration-complexity statement and uses it as a basis for later reductions and generalizations in the paper. The objective-error theorem is the stable mathematical claim formalized here; the complexity paraphrase is outside this mission's Lean goal.

Allen-Zhu proved Theorem 2.1 in the paper. The Lean declarations in this proposal are targets with proof placeholders, not machine-checked proofs of Katyusha's convergence. Completing them would produce a checked account of the exact algorithm, its finite probability space, and the conditional inequalities for an epoch. The finite-sum and proximal-point definitions reused here are already published in the SAGA formalization; Katyusha's weighted snapshot and coupling statements require their own development.

Difficulty

The estimator is unbiased, but that fact alone does not give the claimed acceleration. Its variance depends on the snapshot and current point, and a direct descent estimate retains a variance penalty. The bound in Lemma 2.4 expresses that penalty through a smooth convex gap which can have either sign before it is combined with other terms. The two proximal sequences and the snapshot therefore have to be accounted for together. Across an epoch, the yyy iterates are averaged with nonuniform weights, while yyy and zzz themselves are carried into the next epoch. Replacing the snapshot with the final yyy value or with a uniform average changes the algorithm and the theorem.

The two rate cases also reflect different parameter values. When mσ/L≤3/4m\sigma/L\le3/4mσ/L≤3/4, τ1\tau_1τ1​ is determined by a square root; above that threshold it is fixed at 1/21/21/2. A proof of only one branch would omit part of the source result. Treating the sampled indices as a single arbitrary path would ask for a false pathwise guarantee, whereas stating the result for a favorable path would lose the expectation bound.

Formalization scope

Vectors are EuclideanSpace ℝ (Fin d) and component indices are Fin n, translating the paper's one-based {1,…,n}\{1,\ldots,n\}{1,…,n} to a zero-based finite type. The goal fixes m=2nm=2nm=2n as Algorithm 1 does; the conditional one-epoch statements admit any positive mmm. The number of epochs SSS can be zero, in which case the output is the initial snapshot. The objective is real-valued. Thus ψ\psiψ may be nondifferentiable but does not include extended-valued indicator functions. The component gradient fields are required to be the actual gradients of their functions, and the comparison point minimizes FFF, not merely fff.

A proximal map P(γ,⋅)P(\gamma,\cdot)P(γ,⋅) is an explicit argument constrained, for every γ>0\gamma>0γ>0, to minimize the proximal objective of the given ψ\psiψ. The run computes the paper's two proximal updates with that map. The expectation is the finite uniform average over all nSmn^{Sm}nSm sequences, equivalent to SmSmSm independent uniform samples. It never quantifies over a convenient sequence. These links prevent a vacuous or unrelated encoding of the method.

The paper writes both rates using O(⋅)O(\cdot)O(⋅). Its Section 2.2 bounds yield the concrete coefficient 444 in the square-root regime and 333 in the 1.5−S1.5^{-S}1.5−S regime; these are the expressions in the Lean goal. For Case 1 the rate is represented by division by (1+σ/(3Lm))Sm(1+\sqrt{\sigma/(3Lm)})^{Sm}(1+σ/(3Lm)​)Sm, a positive denominator. For Case 2 it is 3(2/3)S3(2/3)^S3(2/3)S. The statement retains both conclusions at their stated boundary. The one-step lemmas average only a fresh sampled index with the current state fixed, and the epoch statements average the current epoch's mmm indices.

The development needs finite sums and finite expectations, Euclidean smooth and strong convexity facts, proximal minimizer inequalities, and algebra of the weighted snapshot. The finite-sum objective, averaged gradient, proximal-point predicate, and finite index expectation are shared definitions; the Katyusha run, progress value, potential, and epoch inequalities are specific to this algorithm. Contributions proving the milestone statements, establishing existence and uniqueness of the proximal map under these assumptions, or improving reusable proximal and finite-expectation lemmas are within scope.

Selected references

  • Zeyuan Allen-Zhu, Katyusha: The First Direct Acceleration of Stochastic Gradient Methods, Journal of Machine Learning Research 18 (2018), 1–51; arXiv:1603.05953v6. The formalization uses the pinned arXiv version, pp. 1, 6–13.
  • Aaron Defazio, Francis Bach, and Simon Lacoste-Julien, SAGA: A Fast Incremental Gradient Method With Support for Non-Strongly Convex Composite Objectives, Advances in Neural Information Processing Systems 27 (2014); arXiv:1407.0202. The published finite-sum and proximal-point definitions are reused as common objects.
6 thms1 active userReviewed
Control TheoryPartial Differential EquationsProbability+1·Captain: mikedeng1

Reflected Solutions of Backward SDE's, and Related Obstacle Problems for PDE's 3: Uniqueness for the Parabolic Obstacle ProblemResearch Paper

Motivation

Reflected backward stochastic differential equations describe processes that must remain above a prescribed obstacle. El Karoui, Kapoudjian, Pardoux, Peng and Quenez connect that probabilistic construction to a parabolic partial differential equation with an obstacle in their 1997 paper. A representation by a stochastic process is useful only if the associated differential equation identifies a definite function. The comparison result in Theorem 8.6 supplies that identification: within a specified growth class, two viscosity solutions cannot disagree. This mission isolates that deterministic uniqueness statement. The companion existence and stochastic representation result is Theorem 8.5 of the same paper.

Setting

Fix a terminal time T>0T>0T>0 and a spatial dimension d≥1d\ge1d≥1. At time t∈[0,T]t\in[0,T]t∈[0,T] and point x∈Rdx\in\mathbb R^dx∈Rd, the drift b(t,x)b(t,x)b(t,x) is a vector and the diffusion coefficient σ(t,x)\sigma(t,x)σ(t,x) is a d×dd\times dd×d matrix. Both are continuous and Lipschitz in xxx uniformly over ttt. A continuous terminal payoff g(x)g(x)g(x) has at most polynomial growth. The continuous generator f(t,x,r,z)f(t,x,r,z)f(t,x,r,z) depends on a scalar value rrr and a vector zzz; it has polynomial growth at (r,z)=(0,0)(r,z)=(0,0)(r,z)=(0,0) and is Lipschitz in (r,z)(r,z)(r,z). The continuous obstacle h(t,x)h(t,x)h(t,x) has a polynomial upper bound and satisfies h(T,x)≤g(x)h(T,x)\le g(x)h(T,x)≤g(x).

Write a(t,x)=σ(t,x)σ(t,x)⊤a(t,x)=\sigma(t,x)\sigma(t,x)^\topa(t,x)=σ(t,x)σ(t,x)⊤. The associated second order spatial operator is Ltϕ=12Tr⁡(aD2ϕ)+b⋅DϕL_t\phi=\tfrac12\operatorname{Tr}(aD^2\phi)+b\cdot D\phiLt​ϕ=21​Tr(aD2ϕ)+b⋅Dϕ. The obstacle problem asks for a function whose terminal value is ggg and whose interior value obeys

min⁡{u−h, −∂tu−Ltu−f(t,x,u,Du σ)}=0.\min\{u-h,\,-\partial_tu-L_tu-f(t,x,u,Du\,\sigma)\}=0.min{u−h,−∂t​u−Lt​u−f(t,x,u,Duσ)}=0.

A parabolic superjet or subjet at an interior point is a triple (p,q,X)(p,q,X)(p,q,X) of a time slope, spatial slope and symmetric second order matrix that bounds the function locally above or below by the associated quadratic expansion, up to o(∣s−t∣+∣y−x∣2)o(|s-t|+|y-x|^2)o(∣s−t∣+∣y−x∣2). These jets let a continuous function satisfy the differential inequality without having ordinary derivatives. A viscosity subsolution uses superjets and a terminal upper bound; a viscosity supersolution uses subjets and a terminal lower bound. A viscosity solution satisfies both definitions.

Formalization targets

Uniqueness in the polynomial growth class

The goal is the paper's Theorem 8.6. Under the coefficient assumptions above and condition (27), every pair of continuous viscosity solutions with polynomial growth agrees on the entire closed time strip:

(u,v solve (24) and have polynomial growth)⟹u(t,x)=v(t,x)for every (t,x)∈[0,T]×Rd.\bigl(u,v\text{ solve (24) and have polynomial growth}\bigr) \Longrightarrow u(t,x)=v(t,x)\quad\text{for every }(t,x)\in[0,T]\times\mathbb R^d.(u,v solve (24) and have polynomial growth)⟹u(t,x)=v(t,x)for every (t,x)∈[0,T]×Rd.

Condition (27) gives a continuous modulus mRm_RmR​ for the change in fff between bounded spatial points, with argument ∣x−y∣(1+∣z∣)|x-y|(1+|z|)∣x−y∣(1+∣z∣) and mR(0)=0m_R(0)=0mR​(0)=0. The quantifiers include every radius R>0R>0R>0, every bounded scalar argument, and every gradient vector zzz. The milestone is Lemma 8.7, which controls the location and separation of the maximizers of the paper's doubled-variable function Φα(t,x,y)=u(t,x)−v(t,y)−α∣x−y∣2/2\Phi_\alpha(t,x,y)=u(t,x)-v(t,y)-\alpha|x-y|^2/2Φα​(t,x,y)=u(t,x)−v(t,y)−α∣x−y∣2/2.

Significance

The theorem shows that the obstacle PDE has at most one solution in the natural class allowed by polynomially growing coefficients and payoffs. Together with Theorem 8.5, which identifies the reflected backward SDE value as a viscosity solution, and the growth estimate at the end of Section 8, it yields the paper's probabilistic representation of the unique solution. Theorem 8.6 alone asserts uniqueness, so it makes no existence claim.

The formal development provides reusable interfaces for parabolic jets, viscosity inequalities, the obstacle operator and uniform polynomial growth on a finite time strip. Those interfaces can serve other comparison theorems and other parabolic obstacle problems. The mathematical result is proved in the 1997 article; this mission asks for a Lean proof of its deterministic uniqueness statement. The proposal declares the theorem with a proof placeholder and includes the comparison lemma as an intermediate target.

Difficulty

The first obstruction is that the candidate solutions need only be continuous. Subtracting their PDE expressions directly would assume derivatives they may not possess. The paper instead uses viscosity jets, and its comparison argument invokes the theorem of sums from Crandall, Ishii and Lions' viscosity-solutions guide. The generator's spatial modulus must control a gradient argument that grows as the two spatial points approach each other. Lemma 8.7 provides the necessary separation limit for the maximizers. The argument also treats a polynomial growth class on all of Rd\mathbb R^dRd, so a comparison confined to one fixed bounded ball would not establish the stated result.

Formalization scope

Lean uses nonnegative real time and functions on Rd\mathbb R^dRd represented by Fin d → ℝ. The terminal time and dimension are positive. Bounds with existential constants use the finite-dimensional sup norm, which is equivalent to the Euclidean norm in the paper. The displayed quadratic form, Tr⁡(aX)\operatorname{Tr}(aX)Tr(aX) and qσq\sigmaqσ are written by coordinate sums, so their signs, factor 12\tfrac1221​, and matrix order are exact. The obstacle is bounded only above in the data assumptions, exactly as condition (22) states. Condition (27) is imposed only on uniqueness, not folded into the definition of viscosity solution.

Jets are taken at 0<t<T0<t<T0<t<T through a one-sided little-ooo bound in the relative neighborhood of the interior strip. The terminal equality comes from the two terminal inequalities; the viscosity tests impose no separate condition at t=0t=0t=0. The printed text calls S(d)S(d)S(d) “symmetric nonnegative matrices,” but the proof of Theorem 8.6 uses arbitrary symmetric matrices produced by the theorem of sums. The formal definition therefore uses all symmetric matrices and records this correction for review.

The mission permits every continuous solution of polynomial growth. It does not restrict candidates to smooth, bounded or stochastic-representation functions. The companion reflected SDE construction, penalization limit and existence theorem are outside this mission's goal; the general stochastic interface Peng1990.SMP.Stochastic is listed as series context but is not imported by the deterministic statements. Useful contributions include the comparison proof, the lemma on doubled-variable maximizers, and reusable lemmas about jet transformations and the matrix trace inequality.

Selected references

  • N. El Karoui, C. Kapoudjian, É. Pardoux, S. Peng and M.-C. Quenez, Reflected solutions of backward SDE's, and related obstacle problems for PDE's, The Annals of Probability 25(2), 1997, pp. 702–737. DOI.
  • M. G. Crandall, H. Ishii and P.-L. Lions, User's guide to viscosity solutions of second order partial differential equations, Bulletin of the American Mathematical Society 27(1), 1992, pp. 1–67. DOI.
14 thms1 active userReviewed
Algorithmic Game TheoryControl TheoryProbability·Captain: mikedeng1

On the Convergence of Closed-Loop Nash Equilibria to the Mean Field Game Limit 4: In the Mean-Sign Game the Sign Feedback Is an ε_n-Nash Equilibrium and the Mean Converges in Law to ½δ_{H⁺}+½δ_{H⁻}Research Paper

Motivation

Mean field games describe the limit of symmetric stochastic differential games with nnn players as n→∞n\to\inftyn→∞. A basic question of the theory is which mean field equilibria are limits of Nash equilibria of the nnn-player games. For closed-loop equilibria, in which each player's control may depend on the states of all players, this question was open in general until D. Lacker, On the convergence of closed-loop Nash equilibria to the mean field game limit (arXiv:1808.02745, Ann. Appl. Probab. 2020). That paper shows that limits of closed-loop εn\varepsilon_nεn​-Nash equilibria are weak mean field equilibria, a class that can be strictly larger than the classical (strong) one.

Section 7.3 of the paper gives an explicit game in which the difference is visible. It has exactly three strong equilibria (Lacker, Probab. Theory Related Fields 165, 2016, Proposition 3.6, cited as [43] in the paper) and infinitely many weak ones. The weak equilibria form a family indexed by a switching time t0∈[0,T]t_0\in[0,T]t0​∈[0,T], and for t0∈(0,T)t_0\in(0,T)t0​∈(0,T) they are not mixtures of strong equilibria (Remark 7.1). Proposition 7.2, the subject of this mission, treats t0=0t_0=0t0​=0: the natural symmetric feedback is an nnn-player approximate Nash equilibrium, and its population mean selects the equal mixture of the two strong equilibria m±1m^{\pm1}m±1 rather than the third one, m0m^0m0. The selection mechanism is regularization by noise: the mean of the population solves an ill-posed ODE, and the small noise of the nnn-player system picks out a particular random solution (Trevisan, Electron. Commun. Probab. 18, 2013, cited as [57] in the paper).

Setting

Fix a horizon T>0T>0T>0. In the mean-sign game each of nnn players controls a real state

Xti=∫0tαsi ds+Wti,X0i=0,X^i_t = \int_0^t \alpha^i_s\,ds + W^i_t,\qquad X^i_0=0,Xti​=∫0t​αsi​ds+Wti​,X0i​=0,

with controls αsi∈A=[−1,1]\alpha^i_s\in A=[-1,1]αsi​∈A=[−1,1] and independent standard Brownian motions W1,…,WnW^1,\dots,W^nW1,…,Wn. The mean process is μ‾tn=1n∑k=1nXtk\overline\mu^n_t=\frac1n\sum_{k=1}^n X^k_tμ​tn​=n1​∑k=1n​Xtk​, the mean of the empirical measure μtn=1n∑kδXtk\mu^n_t=\frac1n\sum_k\delta_{X^k_t}μtn​=n1​∑k​δXtk​​. Player iii maximizes the expected terminal reward

Jin=E[XTi μ‾Tn],J^n_i=\mathbb E\big[X^i_T\,\overline\mu^n_T\big],Jin​=E[XTi​μ​Tn​],

that is, b(t,x,m,a)=ab(t,x,m,a)=ab(t,x,m,a)=a, f≡0f\equiv0f≡0, g(x,m)=x m‾g(x,m)=x\,\overline mg(x,m)=xm with m‾=∫y m(dy)\overline m=\int y\,m(dy)m=∫ym(dy), and initial law λ=δ0\lambda=\delta_0λ=δ0​.

A Markovian control of player iii is a Borel function β:[0,T]×Rn→[−1,1]\beta:[0,T]\times\mathbb R^n\to[-1,1]β:[0,T]×Rn→[−1,1] of time and the current states of all players. A profile (α1,…,αn)(\alpha^1,\dots,\alpha^n)(α1,…,αn) is a Markovian ε\varepsilonε-Nash equilibrium if no player can raise their payoff by more than ε\varepsilonε by switching to another Markovian control while the others keep theirs (Definition 2.1).

With sgn⁡(x)=1,−1,0\operatorname{sgn}(x)=1,-1,0sgn(x)=1,−1,0 for x>0x>0x>0, x<0x<0x<0, x=0x=0x=0, the sign feedback (7.13) with t0=0t_0=0t0​=0 is

α0n,i(t,x1,…,xn)=sgn⁡(1n∑k=1nxk)1(0,T](t),\alpha^{n,i}_0(t,x_1,\dots,x_n)=\operatorname{sgn}\Big(\frac1n\sum_{k=1}^n x_k\Big)\mathbf 1_{(0,T]}(t),α0n,i​(t,x1​,…,xn​)=sgn(n1​k=1∑n​xk​)1(0,T]​(t),

the same for every player. Finally H0±(t)=±tH^\pm_0(t)=\pm tH0±​(t)=±t on [0,T][0,T][0,T] (7.11).

Formalization targets

Goal: Proposition 7.2

For the profile αn=(α0n,1,…,α0n,n)\alpha^n=(\alpha^{n,1}_0,\dots,\alpha^{n,n}_0)αn=(α0n,1​,…,α0n,n​):

∃ εn≥0, εn→0:αn is a Markovian εn-Nash equilibrium for each n,\exists\,\varepsilon_n\ge0,\ \varepsilon_n\to0:\quad \alpha^n\ \text{is a Markovian }\varepsilon_n\text{-Nash equilibrium for each }n,∃εn​≥0, εn​→0:αn is a Markovian εn​-Nash equilibrium for each n, L((μ‾tn[αn])t∈[0,T]) ⟹ 12δH0++12δH0−on C([0,T];R).\mathcal L\big((\overline\mu^n_t[\alpha^n])_{t\in[0,T]}\big)\ \Longrightarrow\ \tfrac12\delta_{H^+_0}+\tfrac12\delta_{H^-_0}\quad\text{on }C([0,T];\mathbb R).L((μ​tn​[αn])t∈[0,T]​) ⟹ 21​δH0+​​+21​δH0−​​on C([0,T];R).

The goal also asserts that the nnn-player system under αn\alpha^nαn has a solution, so that the equilibrium property cannot hold vacuously.

Milestones

  1. The equilibrium payoff: J1n(αn)=E[∣μ‾Tn∣2]→T2J^n_1(\alpha^n)=\mathbb E[|\overline\mu^n_T|^2]\to T^2J1n​(αn)=E[∣μ​Tn​∣2]→T2 (proof of Proposition 7.2, p. 49).
  2. Lemma 7.4, the part about the mean YnY^nYn and player 1's noise W1W^1W1 when player 1 deviates to a 1n\frac1nn1​-optimal control (7.15): the laws of (Yn,W1)(Y^n,W^1)(Yn,W1) are tight, and every limit (Y,W)(Y,W)(Y,W) has L(Y)=12δH0++12δH0−\mathcal L(Y)=\tfrac12\delta_{H^+_0}+\tfrac12\delta_{H^-_0}L(Y)=21​δH0+​​+21​δH0−​​, solves Yt=∫0tsgn⁡(Ys) dsY_t=\int_0^t\operatorname{sgn}(Y_s)\,dsYt​=∫0t​sgn(Ys​)ds, and has YYY independent of WWW.
  3. The upper bound (7.14): lim sup⁡nsup⁡βJ1n(β,α0n,2,…,α0n,n)≤T2\limsup_n\sup_{\beta}J^n_1(\beta,\alpha^{n,2}_0,\dots,\alpha^{n,n}_0)\le T^2limsupn​supβ​J1n​(β,α0n,2​,…,α0n,n​)≤T2.

Significance

Proposition 7.2 is a concrete instance of the paper's main theme. Theorem 2.7 says that limits of closed-loop equilibria are weak equilibria; this example exhibits explicit, symmetric, Markovian approximate equilibria whose limit is a genuinely random equilibrium (the sign of the mean is a fair coin), selected by noise among infinitely many candidates, and it identifies the limiting law of the population mean exactly. The paper states that the analogous claim for t0∈(0,T)t_0\in(0,T)t0​∈(0,T), where the limit would be a weak equilibrium that is not a mixture of strong ones, is not resolved; a formal treatment of the t0=0t_0=0t0​=0 case makes the structure of that question precise.

Nothing of this proposition is machine-checked. Formalizing it requires weak solutions of SDEs with discontinuous drift, Nash equilibria over Markovian feedback controls, and weak convergence of laws on path space, all stated so that the junk values of Lean's total functions never enter. The objects defined here (the nnn-player game with quantified weak solutions, its payoffs and Markovian ε\varepsilonε-Nash equilibria) are shared with the other missions of this series.

Difficulty

The obvious argument for εn→0\varepsilon_n\to0εn​→0 compares player 1's payoff under a deviation with T2T^2T2. A deviation changes the drift of the mean only by O(1/n)O(1/n)O(1/n), but the dynamics of the mean, dYt=sgn⁡(Yt)dt+n−1/2dW‾tdY_t=\operatorname{sgn}(Y_t)dt+n^{-1/2}d\overline W_tdYt​=sgn(Yt​)dt+n−1/2dWt​, is ill-posed in the limit: the ODE y˙=sgn⁡(y)\dot y=\operatorname{sgn}(y)y˙​=sgn(y), y0=0y_0=0y0​=0, has infinitely many solutions ±(t−s)+\pm(t-s)^+±(t−s)+. Continuity of the solution map, the usual tool, is unavailable, and one must instead identify the limit law, which comes from the vanishing noise, and show that it is unchanged by the deviation. The second difficulty is that the payoff XT1YTX^1_TY_TXT1​YT​ is unbounded, so convergence of laws does not give convergence of payoffs without a uniform integrability estimate. The proof in the paper is short, but relies on a cited result on the vanishing-noise limit and on a compactness argument in a weak L2L^2L2 topology for the deviating controls.

Formalization scope

  • Dimension and state. d=1d=1d=1; R1\mathbb R^1R1 is EuclideanSpace ℝ (Fin 1) (the platform's EthierKurtz.SDEState 1) and its coordinate is y 0. Controls are real, A=[−1,1]A=[-1,1]A=[−1,1].
  • Pathwise equations. Volatility is the identity, so the SDE of each player is stated as Xti=X0i+∫0tb ds+WtiX^i_t=X^i_0+\int_0^t b\,ds+W^i_tXti​=X0i​+∫0t​bds+Wti​ almost surely for all t∈[0,T]t\in[0,T]t∈[0,T], with a Lebesgue integral of a bounded measurable integrand.
  • Solutions are quantified. A weak solution of the nnn-player system is a structure (probability space, filtration, independent F\mathbb FF-Brownian motions, i.i.d. initial states independent of the noise, adapted path-valued states, the empirical flow). Payoffs are functions of a solution; the Nash inequality and every limit statement are required for every solution. Solutions exist and are unique in law, so this matches the paper's definitions; the goal asserts existence explicitly.
  • Index shift. Term nnn of every sequence is the (n+1)(n+1)(n+1)-player game; the factor 1n\frac1nn1​ in the controls and the mean is then 1n+1\frac1{n+1}n+11​.
  • sgn and time. sgn⁡\operatorname{sgn}sgn is Real.sign (sgn⁡0=0\operatorname{sgn}0=0sgn0=0), and the control vanishes at t=0t=0t=0, both as printed.
  • Unbounded payoff. Assumption A fails (ggg is unbounded) and is not assumed anywhere. Payoffs are Bochner integrals; XTiμ‾TnX^i_T\overline\mu^n_TXTi​μ​Tn​ is integrable on every solution (bounded drift, X0i=0X^i_0=0X0i​=0), which is a fact to be proved rather than an assumption.
  • Laws. Laws on C([0,T];R)C([0,T];\mathbb R)C([0,T];R) carry the topology of weak convergence; the mean path is a continuous function of the state paths, so its law is a probability measure by construction.
  • Lemma 7.4. Only the (Y,W)(Y,W)(Y,W) coordinates are stated: tightness, (i), the equation for YYY in (ii), and (iv). The coordinates XXX and β\betaβ, which need the weak topology of L2([0,T];[−1,1])L^2([0,T];[-1,1])L2([0,T];[−1,1]), and item (iii) are not stated; the norm topology must not be substituted, because the deviating controls are not tight in it.
  • Ruled out. A statement in which the profiles have no solutions would make the Nash clause vacuous; the existence clause of the goal excludes it.

Contributions welcome: the existence of weak solutions for bounded measurable Markovian drifts, the vanishing-noise limit of dZ=sgn⁡(Z)dt+ϵ dWdZ=\operatorname{sgn}(Z)dt+\epsilon\,dWdZ=sgn(Z)dt+ϵdW, and Girsanov-type change-of-measure estimates are all reusable beyond this mission.

Selected references

  • D. Lacker, On the convergence of closed-loop Nash equilibria to the mean field game limit, Ann. Appl. Probab. 30(4), 2020; arXiv:1808.02745v1, 2018. https://arxiv.org/abs/1808.02745
  • D. Lacker, A general characterization of the mean field limit for stochastic differential games, Probab. Theory Related Fields 165(3–4), 581–648, 2016 (reference [43] of the paper).
  • D. Trevisan, Zero noise limits using local times, Electron. Commun. Probab. 18, 2013 (reference [57] of the paper).
  • R. Carmona, D. Lacker, A probabilistic weak formulation of mean field games and applications, Ann. Appl. Probab. 25(3), 2015. https://arxiv.org/abs/1307.1152
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Markov ChainMathematical PhysicsProbability·Captain: mikedeng1

The Endpoint Distribution of Directed Polymers 2: Geometric Localization with Positive Density Holds Exactly in the Low-Temperature PhaseResearch Paper

Motivation

A directed polymer in random environment is a random walk path reweighted by a random potential that is refreshed at every time step. It is a basic model of a one-dimensional object (a polymer, an interface, a flux line) pinned by impurities, and a discrete version of the KPZ universality class in dimension 1+11+11+1. A central question is localization: whether the walk's endpoint at time nnn, under the random Gibbs measure, concentrates on a few sites or spreads out like a simple random walk.

For a fixed disorder law there is a critical inverse temperature βc\beta_cβc​ (Comets–Yoshida, Ann. Probab. 2006). In the low-temperature phase β>βc\beta>\beta_cβ>βc​ the endpoint has atoms of positive mass, in the Cesàro sense, at a positive fraction of times (Carmona–Hu 2002, Comets–Shiga–Yoshida 2003); in the high-temperature phase it does not. Atoms alone say nothing about geometry: the mass could sit on a few sites that are far apart. Bates and Chatterjee (arXiv:1612.03443v5, Ann. Probab. 2020) prove that in the low-temperature phase the mass also sits on a region of bounded diameter at a positive fraction of times, in every dimension and for every disorder law with exponential moments. Before this, geometric localization was known only for the integrable log-gamma polymer in 1+11+11+1 dimensions (Comets–Nguyen 2016).

Setting

Fix d≥1d\ge1d≥1. Let (Xu)u∈N×Zd(X_u)_{u\in\mathbb N\times\mathbb Z^d}(Xu​)u∈N×Zd​ be i.i.d. real random variables with law L\mathfrak LL, not supported on a single point, such that λ(α)=log⁡E eαXu<∞\lambda(\alpha)=\log\mathbf E\,e^{\alpha X_u}<\inftyλ(α)=logEeαXu​<∞ for α∈[−2β,2β]\alpha\in[-2\beta,2\beta]α∈[−2β,2β] (assumption (1.1)), where β≥0\beta\ge0β≥0 is the inverse temperature. For a nearest-neighbour path γ\gammaγ of length nnn from the origin, its weight is exp⁡(β∑i=1nXi,γ(i))\exp(\beta\sum_{i=1}^n X_{i,\gamma(i)})exp(β∑i=1n​Xi,γ(i)​). The endpoint distribution fn(x)=ρn(ωn=x)f_n(x)=\rho_n(\omega_n=x)fn​(x)=ρn​(ωn​=x) is the total weight of paths ending at xxx divided by the total weight of all (2d)n(2d)^n(2d)n paths. The partition function is Zn=(2d)−n∑γexp⁡(β∑i=1nXi,γ(i))Z_n=(2d)^{-n}\sum_\gamma\exp(\beta\sum_{i=1}^nX_{i,\gamma(i)})Zn​=(2d)−n∑γ​exp(β∑i=1n​Xi,γ(i)​) and the free energy is Fn=1nlog⁡ZnF_n=\frac1n\log Z_nFn​=n1​logZn​. The limit p(β)=lim⁡EFnp(\beta)=\lim\mathbf E F_np(β)=limEFn​ exists, and βc\beta_cβc​ is characterised by p(β)=λ(β)p(\beta)=\lambda(\beta)p(β)=λ(β) for 0≤β≤βc0\le\beta\le\beta_c0≤β≤βc​ and p(β)<λ(β)p(\beta)<\lambda(\beta)p(β)<λ(β) for β>βc\beta>\beta_cβ>βc​.

For δ>0\delta>0δ>0 and K≥0K\ge0K≥0 let Gδ,K\mathcal G_{\delta,K}Gδ,K​ be the set of probability mass functions on Zd\mathbb Z^dZd that give mass greater than 1−δ1-\delta1−δ to some set DDD with diam⁡(D)=sup⁡x,y∈D∥x−y∥1≤K\operatorname{diam}(D)=\sup_{x,y\in D}\|x-y\|_1\le Kdiam(D)=supx,y∈D​∥x−y∥1​≤K.

The proofs work on the space S\mathcal SS of partitioned subprobability measures: functions f≥0f\ge0f≥0 on N×Zd\mathbb N\times\mathbb Z^dN×Zd with ∑f≤1\sum f\le1∑f≤1, modulo translations of each copy of Zd\mathbb Z^dZd, with a metric ddd that makes S\mathcal SS compact. The update fn↦fn+1f_n\mapsto f_{n+1}fn​↦fn+1​ induces a Markov kernel T\mathcal TT on S\mathcal SS; K\mathcal KK is its set of invariant probability measures and M⊂K\mathcal M\subset\mathcal KM⊂K the minimisers of a free-energy functional R\mathcal RR. On S\mathcal SS the mission uses the functionals max⁡(f)=max⁡uf(u)\max(f)=\max_uf(u)max(f)=maxu​f(u), the support number N(f)N(f)N(f) (number of copies carrying mass), Wδ(f)W_\delta(f)Wδ​(f) (the least diameter of a region of one copy with mass >1−δ>1-\delta>1−δ), m(f)=max⁡nqn(f)m(f)=\max_nq_n(f)m(f)=maxn​qn​(f) and Q(f)=∑nqn(f)/(1−qn(f))Q(f)=\sum_nq_n(f)/(1-q_n(f))Q(f)=∑n​qn​(f)/(1−qn​(f)), where qn(f)q_n(f)qn​(f) is the mass of copy nnn.

Formalization targets

Goal: Theorem 1.2 (= Theorem 7.3(a),(c))

If β>βc\beta>\beta_cβ>βc​, then for every δ>0\delta>0δ>0 there are K<∞K<\inftyK<∞ and θ>0\theta>0θ>0, depending only on δ,L,β,d\delta,\mathfrak L,\beta,dδ,L,β,d, such that

lim inf⁡n→∞1n∑i=0n−11{fi∈Gδ,K}≥θa.s.\liminf_{n\to\infty}\frac1n\sum_{i=0}^{n-1}\mathbb 1_{\{f_i\in\mathcal G_{\delta,K}\}}\ge\theta\quad\text{a.s.}n→∞liminf​n1​i=0∑n−1​1{fi​∈Gδ,K​}​≥θa.s.

If 0≤β≤βc0\le\beta\le\beta_c0≤β≤βc​, then for every KKK and every δ∈(0,1)\delta\in(0,1)δ∈(0,1),

lim⁡n→∞1n∑i=0n−11{fi∈Gδ,K}=0a.s.\lim_{n\to\infty}\frac1n\sum_{i=0}^{n-1}\mathbb 1_{\{f_i\in\mathcal G_{\delta,K}\}}=0\quad\text{a.s.}n→∞lim​n1​i=0∑n−1​1{fi​∈Gδ,K​}​=0a.s.

The goal fixes no constants: KKK and θ\thetaθ are only asserted to exist.

Milestones

  1. Lemma 5.4: max⁡\maxmax is continuous on S\mathcal SS.
  2. Theorem 5.3: the Cesàro average of max⁡xfi(x)\max_xf_i(x)maxx​fi​(x) tends to 000 a.s. at high temperature and has lim inf⁡≥c>0\liminf\ge c>0liminf≥c>0 a.s. at low temperature.
  3. Lemma 7.1: WδW_\deltaWδ​ is upper semicontinuous; mmm and QQQ are lower semicontinuous.
  4. Lemma 7.2: at low temperature ∫Q dν=∞\int Q\,d\nu=\infty∫Qdν=∞ for every ν∈M\nu\in\mathcal Mν∈M.
  5. Theorem 7.3(b): under the single-copy condition ν(N=1)=1\nu(N=1)=1ν(N=1)=1 for all ν∈M\nu\in\mathcal Mν∈M (7.4), localization holds with full density θ≥1−δ\theta\ge1-\deltaθ≥1−δ.
  6. Proposition 7.4: under (7.4), lim⁡K→∞lim inf⁡n1n∑i<nρi(ωi∈CiK)=1\lim_{K\to\infty}\liminf_n\frac1n\sum_{i<n}\rho_i(\omega_i\in\mathcal C_i^K)=1limK→∞​liminfn​n1​∑i<n​ρi​(ωi​∈CiK​)=1 a.s., where CiK\mathcal C_i^KCiK​ is the set of sites within distance KKK of every mode of fif_ifi​.

Significance

The theorem shows that the low-temperature phase is detected by the shape of the endpoint distribution, not only by its largest atom: positive-density geometric localization holds if and only if β>βc\beta>\beta_cβ>βc​. The determinism of KKK and θ\thetaθ makes the statement uniform over all environments with the given law. The conditional results 5 and 6 reduce full-density and favourite-region localization to a single property of the limit set M\mathcal MM, which is open.

The result is proved on paper; nothing in it is machine-checked. A formalization would produce a checked development of the compact space S\mathcal SS, of the Markov kernel T\mathcal TT, and of the variational characterisation of the free energy, which also underlies the companion mission on asymptotic pure atomicity of the same paper.

Difficulty

The obvious approach, tracking fnf_nfn​ in ℓ1(Zd)\ell^1(\mathbb Z^d)ℓ1(Zd), fails because mass escapes to infinity: the sequence (fn)(f_n)(fn​) has no convergent subsequence in any space of probability measures on Zd\mathbb Z^dZd. The paper's compactification keeps pieces of mass that drift apart as separate copies, so a limit point can split one copy's mass over several. The semicontinuity of WδW_\deltaWδ​, mmm and QQQ (Lemma 7.1) only goes one way for this reason, and positivity of the localized fraction needs the separate identity of Lemma 7.2, which uses strict convexity and the non-degeneracy of L\mathfrak LL. Theorem 5.3 already requires the full variational machinery of §4 (convergence of empirical measures to M\mathcal MM), which is the companion mission's subject.

Formalization scope

Points are Zd=\mathbb Z^d=Zd= Fin d → ℤ, cells are ℕ × (Fin d → ℤ), and paths are sequences of nnn signed coordinate steps. The environment is a family of independent measurable random variables, each with law L\mathfrak LL, on an arbitrary probability space. The phases are encoded through Theorem A as lim⁡EFn<λ(β)\lim\mathbf E F_n<\lambda(\beta)limEFn​<λ(β) (β>βc\beta>\beta_cβ>βc​) and lim⁡EFn=λ(β)\lim\mathbf EF_n=\lambda(\beta)limEFn​=λ(β) (0≤β≤βc0\le\beta\le\beta_c0≤β≤βc​), with EFn\mathbf EF_nEFn​ computed under the canonical product environment. Elements of S\mathcal SS are represented by their representatives, with the topology generated by ddd-balls (no quotient). In the goal, KKK and θ\thetaθ are chosen before the probability space. Part (a) is stated for all δ>0\delta>0δ>0 and part (c) for δ∈(0,1)\delta\in(0,1)δ∈(0,1), as printed.

Trivializing encodings are ruled out: Gδ,K\mathcal G_{\delta,K}Gδ,K​ requires total mass exactly 111; WδW_\deltaWδ​ and NNN take values in N∪{∞}\mathbb N\cup\{\infty\}N∪{∞} so that an empty infimum is ∞\infty∞; QQQ is computed in [0,∞][0,\infty][0,∞] so that 1/0=∞1/0=\infty1/0=∞; the sum in F~\widetilde FF is taken in [0,∞][0,\infty][0,∞]; M\mathcal MM avoids a real infimum over K\mathcal KK; L\mathfrak LL is non-degenerate; and the phase hypotheses are limits that exist.

A complete development needs: the metric space (S,d)(\mathcal S,d)(S,d) and its compactness, the measurability and continuity of T\mathcal TT, the Wasserstein space P(S)\mathcal P(\mathcal S)P(S) (here through the published RWPI.SqrtLasso.transportCost), and the convergence W(μn,M)→0\mathcal W(\mu_n,\mathcal M)\to0W(μn​,M)→0 (Theorem 4.9) together with M={δ0}\mathcal M=\{\delta_0\}M={δ0​} at high temperature (Theorem 5.2), both posed in the companion mission. Contributions to any milestone, and to the shared infrastructure of S\mathcal SS, are welcome.

Selected references

  • E. Bates, S. Chatterjee, The endpoint distribution of directed polymers, Ann. Probab. 48 (2020); arXiv:1612.03443v5. https://arxiv.org/abs/1612.03443
  • F. Comets, N. Yoshida, Directed polymers in random environment are diffusive at weak disorder, Ann. Probab. 34 (2006). https://doi.org/10.1214/009117905000000828
  • F. Comets, T. Shiga, N. Yoshida, Directed polymers in a random environment: path localization and strong disorder, Bernoulli 9 (2003). https://doi.org/10.3150/bj/1065444233
  • P. Carmona, Y. Hu, On the partition function of a directed polymer in a Gaussian random environment, Probab. Theory Related Fields 124 (2002). https://doi.org/10.1007/s004400200213
  • F. Comets, V.-L. Nguyen, Localization in log-gamma polymers with boundaries, Probab. Theory Related Fields 166 (2016). https://doi.org/10.1007/s00440-015-0662-4
  • F. Comets, Directed Polymers in Random Environments, Lecture Notes in Math. 2175, Springer (2017). https://doi.org/10.1007/978-3-319-50487-2
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Differential GeometryFunctional AnalysisOptimal Transport+1·Captain: mikedeng1

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

Why relate heat flow and curvature?

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

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

Setting

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

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

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

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

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

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

Formalization targets

The goal is the forward implication of Theorem 4.17:

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

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

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

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

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

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

What the result provides

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

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

Main difficulty

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

Formalization scope

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

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

Selected references

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

On the Convergence of Closed-Loop Nash Equilibria to the Mean Field Game Limit 2: Every Strong MFE Is the Limit in Law of Markovian ε_n-Nash Equilibria of the n-Player GamesResearch Paper

Motivation

Mean field games (Lasry–Lions 2006, Huang–Malhamé–Caines 2006) describe Nash equilibria of stochastic differential games with very many symmetric players. In this description each player interacts with the others only through the empirical distribution of their states. The mean field game is meant to be the limit of the nnn-player games as n→∞n\to\inftyn→∞. Making that link rigorous has two halves:

  • a limit theorem: every limit of nnn-player equilibria is a mean field equilibrium;
  • a converse: every mean field equilibrium is the limit of nnn-player approximate equilibria.

For closed-loop equilibria, where players react to the observed states of all others, both halves are harder than for open-loop equilibria. A single player's deviation changes the feedback of the whole system.

This mission covers the converse half of D. Lacker, On the convergence of closed-loop Nash equilibria to the mean field game limit (arXiv:1808.02745v1, 2018; Ann. Appl. Probab. 30(4), 2020).

Timeline.

  • Carmona–Delarue (2013) and Huang–Malhamé–Caines constructed ϵn\epsilon_nϵn​-Nash equilibria from mean field equilibria, under Lipschitz or linear-quadratic structure, with continuous feedbacks.
  • Cardaliaguet–Delarue–Lasry–Lions (2015, arXiv:1509.02505) obtained such a converse implicitly from a smooth master equation.
  • Lacker (2018) proved the converse for every strong mean field equilibrium. His hypotheses are bounded continuous coefficients and a drift that is Lipschitz in total variation, and the feedback may be discontinuous. The key input is a propagation-of-chaos result in total variation (Lacker, On a strong form of propagation of chaos for McKean–Vlasov equations, arXiv:1805.04476).

Setting

Fix a horizon T>0T>0T>0, a compact convex action set AAA in a real normed space, an initial law λ∈P(Rd)\lambda\in\mathcal P(\mathbb R^d)λ∈P(Rd) and coefficients

b:[0,T]×Rd×P(Rd)×A→Rd,f:[0,T]×Rd×P(Rd)×A→R,g:Rd×P(Rd)→R.b:[0,T]\times\mathbb R^d\times\mathcal P(\mathbb R^d)\times A\to\mathbb R^d,\quad f:[0,T]\times\mathbb R^d\times\mathcal P(\mathbb R^d)\times A\to\mathbb R,\quad g:\mathbb R^d\times\mathcal P(\mathbb R^d)\to\mathbb R .b:[0,T]×Rd×P(Rd)×A→Rd,f:[0,T]×Rd×P(Rd)×A→R,g:Rd×P(Rd)→R.

The nnn-player game.

  • A Markovian control is a Borel map α:[0,T]×(Rd)n→A\alpha:[0,T]\times(\mathbb R^d)^n\to Aα:[0,T]×(Rd)n→A.
  • Under a profile α=(α1,…,αn)\alpha=(\alpha^1,\dots,\alpha^n)α=(α1,…,αn) the states solve
dXti=b(t,Xti,μtn,αi(t,Xt))dt+dWti,μtn=1n∑kδXtk,dX^i_t=b\big(t,X^i_t,\mu^n_t,\alpha^i(t,X_t)\big)dt+dW^i_t,\qquad \mu^n_t=\tfrac1n\textstyle\sum_{k}\delta_{X^k_t},dXti​=b(t,Xti​,μtn​,αi(t,Xt​))dt+dWti​,μtn​=n1​∑k​δXtk​​,

with independent Brownian motions WiW^iWi and i.i.d. initial states of law λ\lambdaλ.

  • Player iii receives Jin(α)=E[∫0Tf(t,Xti,μtn,αi(t,Xt))dt+g(XTi,μTn)]J^n_i(\alpha)=\mathbb E\big[\int_0^Tf(t,X^i_t,\mu^n_t,\alpha^i(t,X_t))dt+g(X^i_T,\mu^n_T)\big]Jin​(α)=E[∫0T​f(t,Xti​,μtn​,αi(t,Xt​))dt+g(XTi​,μTn​)].
  • The profile is a Markovian ϵ\epsilonϵ-Nash equilibrium if no player gains more than ϵ\epsilonϵ by switching to another Markovian control.
  • Relaxed controls take values in P(A)\mathcal P(A)P(A) and average bbb and fff against them.

The mean field game. A flow m∈C([0,T];P(Rd))m\in C([0,T];\mathcal P(\mathbb R^d))m∈C([0,T];P(Rd)) is a strong MFE if some Borel feedback α∗:[0,T]×Rd→A\alpha^*:[0,T]\times\mathbb R^d\to Aα∗:[0,T]×Rd→A satisfies two conditions:

  • the state dXt∗=b(t,Xt∗,mt,α∗(t,Xt∗))dt+dWtdX^*_t=b(t,X^*_t,m_t,\alpha^*(t,X^*_t))dt+dW_tdXt∗​=b(t,Xt∗​,mt​,α∗(t,Xt∗​))dt+dWt​, X0∗∼λX^*_0\sim\lambdaX0∗​∼λ, has law mtm_tmt​ at every time;
  • α∗\alpha^*α∗ maximizes E[∫0Tf(t,Xt,mt,α(t,Xt))dt+g(XT,mT)]\mathbb E[\int_0^Tf(t,X_t,m_t,\alpha(t,X_t))dt+g(X_T,m_T)]E[∫0T​f(t,Xt​,mt​,α(t,Xt​))dt+g(XT​,mT​)] among all Borel feedbacks α\alphaα.

A strong RMFE is the relaxed analogue.

The assumptions are:

  • Assumption A: AAA compact convex; b,f,gb,f,gb,f,g bounded and jointly continuous.
  • Assumption B: the sets {(b(t,x,m,a),z):a∈A, z≤f(t,x,m,a)}\{(b(t,x,m,a),z):a\in A,\ z\le f(t,x,m,a)\}{(b(t,x,m,a),z):a∈A, z≤f(t,x,m,a)} are convex.
  • Assumption C: ∣b(t,x,m,a)−b(t,x,m′,a)∣≤c ∥m−m′∥TV|b(t,x,m,a)-b(t,x,m',a)|\le c\,\|m-m'\|_{TV}∣b(t,x,m,a)−b(t,x,m′,a)∣≤c∥m−m′∥TV​, with ∥m−m′∥TV=sup⁡∣φ∣≤1∫φ d(m−m′)\|m-m'\|_{TV}=\sup_{|\varphi|\le1}\int\varphi\,d(m-m')∥m−m′∥TV​=sup∣φ∣≤1​∫φd(m−m′).

Formalization targets

Goal: Theorem 2.11

Under Assumptions A, B and C, if mmm is a strong MFE, there are two families of objects:

  • numbers ϵn≥0\epsilon_n\ge0ϵn​≥0 with ϵn→0\epsilon_n\to0ϵn​→0;
  • for each nnn, Markovian ϵn\epsilon_nϵn​-Nash equilibria αn\alpha^nαn;

such that

μn[αn] → law  min C([0,T];P(Rd)).\mu^n[\alpha^n]\ \xrightarrow{\ \text{law}\ }\ m\quad\text{in }C([0,T];\mathcal P(\mathbb R^d)).μn[αn]  law ​ min C([0,T];P(Rd)).

The goal asserts no rate, so any quantitative improvement still implies it.

Milestones

  • Proposition 3.7 (strong part): under A and B, strong MFE and strong RMFE are the same flows.
  • Theorem 2.14 (Markovian projection): a drift process can be replaced by a Markovian drift b^(t,x)=E[bt∣Xt=x]\hat b(t,x)=\mathbb E[b_t\mid X_t=x]b^(t,x)=E[bt​∣Xt​=x] with the same one-dimensional marginals.
  • (7.2): for the symmetric profile Λn,i(t,x)=Λ∗(t,xi)\Lambda^{n,i}(t,x)=\Lambda^*(t,x^i)Λn,i(t,x)=Λ∗(t,xi), μn→m\mu^n\to mμn→m in law and ∫φ dμtn→∫φ dmt\int\varphi\,d\mu^n_t\to\int\varphi\,dm_t∫φdμtn​→∫φdmt​ in probability for bounded measurable φ\varphiφ.
  • νn→m\nu^n\to mνn→m (§7.1, p. 45): after one player deviates, the empirical flow still converges to mmm in probability.
  • Theorem 3.10: the relaxed converse, under A and C only.
  • Proposition 3.4(a): under A and B, a relaxed Markovian ϵ\epsilonϵ-Nash equilibrium can be replaced by a strict one with the same state law.

Significance

The result. Theorem 2.11 says that the strong MFE is a faithful idealization: every classical mean field equilibrium is approximately realized by Markovian feedback equilibria of large finite games. No continuity of the equilibrium feedback and no master equation are required. Together with the paper's main limit theorem (mission 1 of this series), it locates strong MFE inside the set of limits of closed-loop equilibria. The paper's Section 2.4 explains why the same converse is open for weak MFE.

Formalizing it. The result is proved on paper but has no machine-checked proof. A complete development would produce several reusable pieces:

  • pathwise formulations of SDEs with bounded measurable drift;
  • the Markovian projection theorem;
  • total-variation propagation of chaos;
  • relaxed-control purification by measurable selection.

None of these is in Mathlib.

Difficulty

The obvious argument has every player use α∗(t,Xti)\alpha^*(t,X^i_t)α∗(t,Xti​), invokes the McKean–Vlasov limit, and passes optimality to the limit. It fails at two places:

  • Discontinuous feedback. α∗\alpha^*α∗ is only measurable, so weak convergence of μn\mu^nμn does not give convergence of payoffs. Convergence in probability of ∫φ dμtn\int\varphi\,d\mu^n_t∫φdμtn​ for discontinuous φ\varphiφ is needed, and that is exactly what the total-variation Lipschitz Assumption C provides.
  • Arbitrary deviations. A deviating player's control βn\beta^nβn is arbitrary and depends on all nnn states. Its limit is a relaxed, non-Markovian control. Comparing it with the mean field optimum requires a projection back onto Markovian feedbacks, without losing the marginal laws.

Formalization scope

Representation.

  • States live in EuclideanSpace ℝ (Fin d).
  • P(⋅)\mathcal P(\cdot)P(⋅) is Mathlib's ProbabilityMeasure with the weak topology and the Borel σ\sigmaσ-field.
  • Paths and flows are continuous maps on Set.Icc 0 T with the compact-open (uniform) topology.
  • Unit volatility makes every SDE a pathwise integral equation Xt=X0+∫0t(drift)ds+WtX_t=X_0+\int_0^t(\text{drift})ds+W_tXt​=X0​+∫0t​(drift)ds+Wt​ a.s., with no stochastic integral.
  • Solutions are quantified, not chosen. Payoffs are functions of a solution, and every equilibrium inequality, consistency condition and convergence statement is required for every solution. This equals the paper's definitions because solutions exist and are unique in law (Girsanov; Veretennikov; Krylov–Röckner).
  • The game with n+1n+1n+1 players is indexed by nnn.

Committed choices.

  • The paper's consistency condition "mt=L(Xt)m_t=\mathcal L(X_t)mt​=L(Xt​)" is read as L(Xt∗)\mathcal L(X^*_t)L(Xt∗​).
  • "Strong RFME" in Proposition 3.7 is read as strong RMFE.
  • Theorem 2.14's "unique strong solution" is a strong solution adapted to the completed filtration of (X0,W)(X_0,W)(X0​,W); its existence is part of the conclusion.
  • The νn\nu^nνn milestone is stated for arbitrary relaxed Markovian deviations, which include the paper's near-optimal ones.
  • Coefficients and controls are defined at all real times; only [0,T][0,T][0,T] matters.

Ruled out. Because equilibria quantify over solutions, a profile whose state system has no solution would be an equilibrium vacuously. For this reason every existence conclusion (the goal, Theorem 3.10, Proposition 3.4(a)) also asserts that the chosen profiles have solutions, and strong (R)MFE requires the equilibrium SDE to have one.

Infrastructure. A complete proof needs Girsanov's theorem, strong existence for SDEs with bounded measurable drift, measurable selection, tightness on path space, and total-variation propagation of chaos. Each is reusable well beyond this mission, and contributions of any of them are welcome. Proposition 3.4(b), the weak half of Proposition 3.7, and Theorem 2.7 are outside this mission.

Selected references

  • D. Lacker, On the convergence of closed-loop Nash equilibria to the mean field game limit, arXiv:1808.02745v1, 2018; Ann. Appl. Probab. 30(4), 2020. https://arxiv.org/abs/1808.02745
  • D. Lacker, On a strong form of propagation of chaos for McKean–Vlasov equations, Electron. Commun. Probab. 23, 2018. https://arxiv.org/abs/1805.04476
  • I. Gyöngy, Mimicking the one-dimensional marginal distributions of processes having an Itô differential, Probab. Theory Related Fields 71, 1986. https://doi.org/10.1007/BF00699039
  • G. Brunick, S. Shreve, Mimicking an Itô process by a solution of a stochastic differential equation, Ann. Appl. Probab. 23(4), 2013. https://arxiv.org/abs/1011.0111
  • R. Carmona, F. Delarue, Probabilistic analysis of mean-field games, SIAM J. Control Optim. 51(4), 2013. https://arxiv.org/abs/1210.5780
  • P. Cardaliaguet, F. Delarue, J.-M. Lasry, P.-L. Lions, The master equation and the convergence problem in mean field games, Annals of Math. Studies 201, 2019. https://arxiv.org/abs/1509.02505
  • A. Yu. Veretennikov, On strong solutions and explicit formulas for solutions of stochastic integral equations, Math. USSR Sb. 39, 1981. https://doi.org/10.1070/SM1981v039n03ABEH001518
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Universality in Polytope Phase Transitions and Message Passing Algorithms 3: Projected Cross-Polytopes Have Weak Neighborliness ρ∗(δ) for Sub-Gaussian Matrices with a Gaussian ComponentResearch Paper

Why this phase transition matters

Sparse recovery asks when a vector with few nonzero coordinates can be reconstructed from fewer linear measurements than unknowns. A related geometric question asks how many faces of a high-dimensional cross-polytope survive a random linear projection. The two questions meet at the same threshold: uniqueness of a minimum-one-norm solution corresponds to a face of the projected cross-polytope. For Gaussian measurement matrices this threshold was known before the work of Bayati, Lelarge and Montanari, from Donoho's face-counting analysis (Donoho 2006); the same curve was later identified as the transition of approximate message passing (Donoho, Maleki and Montanari 2009). Their 2015 paper establishes the same weak-neighborliness curve for a broader class of independent sub-Gaussian entries with a nonzero Gaussian component. The result addresses the universality question posed for these projections: does the asymptotic transition depend on the full entry distribution or only on broad features of the matrix law?

The mathematical theorem is established in that paper. This mission records its statement in Lean and leaves the machine-checked proof open. The relevant statement is Theorem 2 on page 5 of the pinned arXiv version 2, rather than a claim about every random projection without a Gaussian component.

Polytopes, faces, and random matrices

The cross-polytope CnC_nCn​ is the unit ball for the coordinate one-norm in Rn\mathbb R^nRn:

Cn={x∈Rn:∑i=1n∣xi∣≤1}.C_n=\left\{x\in\mathbb R^n:\sum_{i=1}^n|x_i|\leq1\right\}.Cn​={x∈Rn:i=1∑n​∣xi​∣≤1}.

For an m×nm\times nm×n matrix AAA, the projected polytope ACnAC_nACn​ consists of all AxAxAx with x∈Cnx\in C_nx∈Cn​. Write F(Q;ℓ)F(Q;\ell)F(Q;ℓ) for the number of nonempty faces of QQQ whose affine dimension is ⌊ℓ⌋\lfloor\ell\rfloor⌊ℓ⌋. The weak neighborliness level ρ∈(0,1)\rho\in(0,1)ρ∈(0,1) of a random sequence Qn⊆Rm(n)Q_n\subseteq\mathbb R^{m(n)}Qn​⊆Rm(n) means that, for every ξ>0\xi>0ξ>0, the ratio F(Qn;m(n)ρ(1−ξ))/F(Cn;m(n)ρ(1−ξ))F(Q_n;m(n)\rho(1-\xi))/F(C_n;m(n)\rho(1-\xi))F(Qn​;m(n)ρ(1−ξ))/F(Cn​;m(n)ρ(1−ξ)) converges in probability to one, while the analogous ratio with 1+ξ1+\xi1+ξ converges in probability to zero. Both limits belong to the definition; the first alone would record only survival below a candidate threshold.

The matrices have m(n)=⌊nδ⌋m(n)=\lfloor n\delta\rfloorm(n)=⌊nδ⌋ rows for a fixed sampling ratio δ∈(0,1)\delta\in(0,1)δ∈(0,1). Within each matrix, the entries are independent, centered, unit-variance, and sub-Gaussian with one scale factor independent of nnn. They also admit a decomposition A(n)=A~(n)+ν0G(n)A(n)=\widetilde A(n)+\nu_0G(n)A(n)=A(n)+ν0​G(n), where ν0>0\nu_0>0ν0​>0 and the entries of G(n)G(n)G(n) are independent standard normal variables, jointly independent of A~(n)\widetilde A(n)A(n). The theorem imposes no independence between matrices with different values of nnn Bayati–Lelarge–Montanari, Theorem 2.

Formalization targets

Let ϕ\phiϕ and Φ\PhiΦ be the density and distribution function of a standard normal random variable. The paper defines its phase boundary through a positive parameter α\alphaα:

fδ(α)=2ϕ(α)α+2(ϕ(α)−αΦ(−α)),fρ(α)=1−αΦ(−α)ϕ(α).f_\delta(\alpha)=\frac{2\phi(\alpha)}{\alpha+2\bigl(\phi(\alpha)-\alpha\Phi(-\alpha)\bigr)},\qquad f_\rho(\alpha)=1-\frac{\alpha\Phi(-\alpha)}{\phi(\alpha)}.fδ​(α)=α+2(ϕ(α)−αΦ(−α))2ϕ(α)​,fρ​(α)=1−ϕ(α)αΦ(−α)​.

Footnote 3 states that fδf_\deltafδ​ decreases from one to zero on the nonnegative half-line, so each δ∈(0,1)\delta\in(0,1)δ∈(0,1) has exactly one positive parameter. The goal, Theorem 2, says that whenever fδ(α)=δf_\delta(\alpha)=\deltafδ​(α)=δ, the sequence A(n)CnA(n)C_nA(n)Cn​ has weak neighborliness fρ(α)f_\rho(\alpha)fρ​(α) in probability. The Lean theorem spells out this parameter relation; it does not apply an inverse function at an argument outside a proved range.

The milestone list covers the two scalar results identifying the boundary, a deterministic condition for exact recovery, and the compressed-sensing transition. With ZZZ standard normal and u+=max⁡(u,0)u_+=\max(u,0)u+​=max(u,0), the scalar function is

Gε(α)=ε(1+α2)+2(1−ε)E[(Z−α)+2].G_\varepsilon(\alpha)=\varepsilon(1+\alpha^2)+2(1-\varepsilon)\mathbb E[(Z-\alpha)_+^2].Gε​(α)=ε(1+α2)+2(1−ε)E[(Z−α)+2​].

Lemma 8 gives its unique positive minimizer and its minimum value. Lemma 9 relates that minimum to both sides of the boundary. The scalar state evolution σt+12=F(σt2,ασt)\sigma_{t+1}^2=\mathsf F(\sigma_t^2,\alpha\sigma_t)σt+12​=F(σt2​,ασt​), with F(σ2,θ)=δ−1E{[η(X+σZ;θ)−X]2}\mathsf F(\sigma^2,\theta)=\delta^{-1}\mathbb E\{[\eta(X+\sigma Z;\theta)-X]^2\}F(σ2,θ)=δ−1E{[η(X+σZ;θ)−X]2} and η(u;θ)=sign⁡(u)(∣u∣−θ)+\eta(u;\theta)=\operatorname{sign}(u)(|u|-\theta)_+η(u;θ)=sign(u)(∣u∣−θ)+​ soft thresholding, has slope Gε(α)/δG_\varepsilon(\alpha)/\deltaGε​(α)/δ at the origin and is concave (Lemma 7). Lemma 10 shows that a two-time correlation map Fα,ε\mathcal F_{\alpha,\varepsilon}Fα,ε​ satisfies Fα,ε(Q)>Q\mathcal F_{\alpha,\varepsilon}(Q)>QFα,ε​(Q)>Q on [0,1)[0,1)[0,1). Theorem 10, cited from Bürgisser and Cucker, bounds the probability that a Gaussian-perturbed rectangular matrix has a small least singular value:

P{σN(B+νG)≤νz}≤(a1z)M−N+1.\mathbb P\{\sigma_N(B+\nu G)\le\nu z\}\le(a_1z)^{M-N+1}.P{σN​(B+νG)≤νz}≤(a1​z)M−N+1.

Lemma 5 gives a recovery condition based on an approximate dual certificate and singular-value bounds. Theorem 8 states that minimum-one-norm recovery succeeds with probability tending to one below the boundary and fails with probability tending to one above it Bayati–Lelarge–Montanari, pp. 39–41, 60–61.

What a formal proof would establish

The goal would certify that the same face-count transition applies to every entry law in the stated class, including laws that are not identically distributed across the matrix. The conclusion is geometric: it counts faces of an actual projected one-norm ball. The recovery milestone provides a second way to state the threshold for sparse signals. Together they make the normalization and the two sides of the transition explicit, so future variants can compare their assumptions and conclusions with a fixed formal statement.

No machine-checked proof of Theorem 2 or of the selected milestones is known. The declarations are open Lean statements over explicit definitions. A complete development would formalize the known argument in the paper, including the probabilistic estimates and the bridge from recovery probabilities to face counts. Sharper results that remove the Gaussian component would be separate theorems with their own hypotheses.

Where the difficulty lies

The count of surviving faces depends on many supports and sign patterns simultaneously. Matching means and variances of matrix entries does not make their finite-dimensional face counts equal. Likewise, controlling recovery for one fixed signal does not immediately control the fraction of all faces. Near the boundary, exact recovery also requires uniform singular-value information for many column submatrices. These are the points where elementary concentration for a single entry or a single support is insufficient. The source paper treats the geometric statement and the recovery transition under a Gaussian-component condition; a proof that silently assumes full Gaussianity would miss its universality claim.

Formalization scope

Vectors are functions on Fin n, and every one-norm is an explicit sum of absolute values. The squared Euclidean norm is a sum of coordinate squares; the default norm on Fin n → ℝ is not used for it. Face counts reuse the published Grunbaum2003.faceCount definition, with dimension ⌊ℓ⌋\lfloor\ell\rfloor⌊ℓ⌋ for nonnegative ℓ\ellℓ; negative dimensions have zero nonempty faces. The two limits in weak neighborliness use convergence in measure, which expresses convergence in probability here. The printed lower ratio has a zero denominator for ξ>1\xi>1ξ>1, so that limit is stated for 0<ξ≤10<\xi\leq10<ξ≤1. Ratios at small nnn may involve zero denominators, but the asymptotic assertion concerns arbitrarily large nnn.

Theorem 2 uses variance one and an N(0,1)N(0,1)N(0,1) Gaussian component. Theorem 8 instead uses variance 1/m(n)1/m(n)1/m(n) and an N(0,1/m(n))N(0,1/m(n))N(0,1/m(n)) component, exactly as printed. Sub-Gaussianity uses Mathlib's moment-generating-function predicate for all real parameters; this is the operative two-sided reading of the paper's stated scale condition. The scalar Gaussian expectation in GεG_\varepsilonGε​ is accompanied by an explicit integrability conclusion in Lemma 8, excluding Lean's zero value for a nonintegrable integral. The restricted least singular value is the infimum of output norms on unit column vectors. This gives zero when a wide submatrix has a kernel and is the bound needed by Lemma 5. The state-evolution map is written as a function of σ2\sigma^2σ2, and its derivative at 000 is a right derivative. In Lemma 10 the law of X∞X_\inftyX∞​ is the three-atom mixture on {0,+∞,−∞}\{0,+\infty,-\infty\}{0,+∞,−∞}, with the split of the mass ε\varepsilonε between the two infinite atoms left free. The page's clause Fα,ε′(1)<1\mathcal F'_{\alpha,\varepsilon}(1)<1Fα,ε′​(1)<1 is stated for α>α∗(ε)\alpha>\alpha_*(\varepsilon)α>α∗​(ε), since the derivative equals 111 at α=α∗\alpha=\alpha_*α=α∗​. Theorem 10 quantifies ν>0\nu>0ν>0 and z>0z>0z>0, which the page leaves implicit.

The random-matrix predicates require measurability, independence within each nnn, the stated marginal laws, and independence of G(n)G(n)G(n) from A~(n)\widetilde A(n)A(n). They leave the matrix law otherwise arbitrary. The weak-neighborliness predicate contains both face-ratio limits and 0<ρ<10<\rho<10<ρ<1; neither the goal nor a milestone defines the threshold by assuming its conclusion. A full proof needs reusable facts about Gaussian integrals, independence of finite arrays, random face counts, restricted singular values, and the relation between projected faces and unique one-norm recovery. Contributions establishing those facts or closing any of the listed theorem statements are within scope.

Selected references

  • Mohsen Bayati, Marc Lelarge and Andrea Montanari, Universality in polytope phase transitions and message passing algorithms, Annals of Applied Probability 25(2), 2015. arXiv:1207.7321v2
  • David L. Donoho, High-dimensional centrally symmetric polytopes with neighborliness proportional to dimension, Discrete & Computational Geometry 35, 617–652, 2006. MR2225676
  • David L. Donoho, Arian Maleki and Andrea Montanari, Message-passing algorithms for compressed sensing, Proceedings of the National Academy of Sciences 106, 18914–18919, 2009. doi:10.1073/pnas.0909892106
  • Peter Bürgisser and Felipe Cucker, Smoothed analysis of Moore–Penrose inversion, SIAM Journal on Matrix Analysis and Applications 31, 2769–2783, 2010. MR2740632
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Algorithmic Game TheoryControl TheoryProbability·Captain: mikedeng1

On the Convergence of Closed-Loop Nash Equilibria to the Mean Field Game Limit 1: Empirical Measure Flows of Closed-Loop ε_n-Nash Equilibria Are Tight and Every Limit in Law Is a Weak MFEResearch Paper

Motivation

Mean field games (MFG) were introduced by Lasry and Lions (2007) and by Huang, Malhamé and Caines (2006) as limits of stochastic differential games with many symmetric players. The model is only meaningful if equilibria of the nnn-player games actually converge to equilibria of the limit game. That convergence depends on what information the players use. For open-loop equilibria, where controls are functions of the noise, it was established in general by Lacker (2016) and Fischer (2017). For closed-loop equilibria, where a player's control is a feedback on the observed states of all players, the deviation of one player changes the state processes of all others, and the only general results before this paper (Cardaliaguet, Delarue, Lasry and Lions, 2019) required a unique MFE and a smooth solution of the master equation.

Timeline:

  • 2006–2007: Lasry–Lions and Huang–Malhamé–Caines introduce MFG and construct approximate nnn-player equilibria from an MFE.
  • 2016–2017: Lacker and Fischer characterize limits of open-loop nnn-player equilibria as (weak) MFE, under continuity and compactness assumptions.
  • 2015/2019: Cardaliaguet–Delarue–Lasry–Lions prove convergence of closed-loop Markovian equilibria with a rate, assuming the master equation has a smooth solution (in particular, monotone data).
  • 2018: Lacker (arXiv:1808.02745, Ann. Appl. Probab. 2020) proves the closed-loop limit theorem without uniqueness or master equation, under bounded continuous data and a convexity condition. This mission formalizes that result.

Setting

Fix a dimension ddd, a horizon T>0T>0T>0, a compact convex control set AAA in a normed space, an initial law λ\lambdaλ on Rd\mathbb R^dRd, and bounded continuous functions b(t,x,m,a)∈Rdb(t,x,m,a)\in\mathbb R^db(t,x,m,a)∈Rd, f(t,x,m,a)∈Rf(t,x,m,a)\in\mathbb Rf(t,x,m,a)∈R, g(x,m)∈Rg(x,m)\in\mathbb Rg(x,m)∈R, where mmm ranges over the probability measures P(Rd)\mathcal P(\mathbb R^d)P(Rd) with the weak topology (Assumption A). Assumption B asks that {(b(t,x,m,a),z):a∈A, z≤f(t,x,m,a)}\{(b(t,x,m,a),z): a\in A,\ z\le f(t,x,m,a)\}{(b(t,x,m,a),z):a∈A, z≤f(t,x,m,a)} be convex for each (t,x,m)(t,x,m)(t,x,m).

In the nnn-player game, player iii picks an admissible closed-loop control αi(t,x)\alpha^i(t,x)αi(t,x): a measurable, non-anticipating function of time and of the paths of all nnn states. The states solve

dXti=b(t,Xti,μtn,αi(t,X))dt+dWti,μtn=1n∑k=1nδXtk,dX^i_t=b\big(t,X^i_t,\mu^n_t,\alpha^i(t,X)\big)dt+dW^i_t,\qquad \mu^n_t=\frac1n\sum_{k=1}^n\delta_{X^k_t},dXti​=b(t,Xti​,μtn​,αi(t,X))dt+dWti​,μtn​=n1​k=1∑n​δXtk​​,

with independent Brownian motions and i.i.d. initial states of law λ\lambdaλ, and player iii receives Jin(α)=E[∫0Tf(t,Xti,μtn,αi(t,X))dt+g(XTi,μTn)]J^n_i(\alpha)=\mathbb E\big[\int_0^Tf(t,X^i_t,\mu^n_t,\alpha^i(t,X))dt+g(X^i_T,\mu^n_T)\big]Jin​(α)=E[∫0T​f(t,Xti​,μtn​,αi(t,X))dt+g(XTi​,μTn​)]. A closed-loop ε\varepsilonε-Nash equilibrium is a profile from which no player gains more than ε\varepsilonε by a unilateral deviation. The random empirical measure flow μn=(μtn)t∈[0,T]\mu^n=(\mu^n_t)_{t\in[0,T]}μn=(μtn​)t∈[0,T]​ is an element of C([0,T];P(Rd))C([0,T];\mathcal P(\mathbb R^d))C([0,T];P(Rd)).

A function of (t,x,m)(t,x,m)(t,x,m), with mmm a measure flow, is semi-Markov if it depends on mmm only through (ms)s≤t(m_s)_{s\le t}(ms​)s≤t​. A weak MFE is a filtered probability space carrying a random flow μ\muμ, a Brownian motion WWW and a state X∗X^*X∗ with X0∗∼λX^*_0\sim\lambdaX0∗​∼λ, with X0∗,μ,WX^*_0,\mu,WX0∗​,μ,W independent, a semi-Markov control α∗(t,Xt∗,μ)\alpha^*(t,X^*_t,\mu)α∗(t,Xt∗​,μ) driving X∗X^*X∗, optimality of α∗\alpha^*α∗ against every semi-Markov alternative (the alternative state being driven by the same WWW and μ\muμ), and the consistency condition μt=P(Xt∗∈⋅∣Ftμ)\mu_t=\mathbb P(X^*_t\in\cdot\mid\mathcal F^\mu_t)μt​=P(Xt∗​∈⋅∣Ftμ​). When μ\muμ is deterministic this is the usual (strong) MFE.

Formalization targets

Goal: Theorem 2.7

Under Assumptions A and B, if εn≥0\varepsilon_n\ge0εn​≥0, εn→0\varepsilon_n\to0εn​→0, and αn\alpha^nαn is a closed-loop εn\varepsilon_nεn​-Nash equilibrium of the nnn-player game, then

{L(μn[αn])}n is tight in P(C([0,T];P(Rd))),\big\{\mathcal L(\mu^n[\alpha^n])\big\}_n\ \text{is tight in}\ \mathcal P\big(C([0,T];\mathcal P(\mathbb R^d))\big),{L(μn[αn])}n​ is tight in P(C([0,T];P(Rd))),

and every subsequential limit in law is the law of the flow of a weak MFE. No constant and no rate is asserted.

Milestones

Without convexity (Theorem 3.9) the same holds with weak relaxed MFE, and Proposition 3.7 identifies weak relaxed MFE flows with weak MFE flows under Assumption B. The proof path of Section 5 is: tightness of the path-space empirical measures (Lemma 5.1), a projection lemma (Lemma 5.2), the realization of a randomized Fokker–Planck equation by a semi-Markov relaxed control (Lemma 5.3), identification of the limiting dynamics with the limiting average value (Theorem 5.4), approximation of relaxed by continuous controls (Lemma 5.5), and the limit of unilateral deviations (Proposition 5.6). Two supporting results come from Section 2.1 (well-posedness of the nnn-player system) and Appendix A (Corollary A.7).

Significance

The theorem shows that the mean field game is the correct limit of closed-loop nnn-player games without any uniqueness assumption, which is the regime where the master-equation method is unavailable. The price is the limit object: a weak MFE, whose measure flow may be random and whose control may depend on the past of the flow. The paper also shows (Proposition 7.2) that this randomness genuinely occurs, so the result cannot be strengthened to strong MFE in general. Combined with the converse (Theorem 2.11, mission 2 of this series), it characterizes which MFE arise as closed-loop limits.

The result is proved in the paper; nothing in it is machine-checked. A formalization produces a checked definition of closed-loop nnn-player games and of weak semi-Markov MFE, which are reusable for any MFG convergence result, and it would make explicit the measurability bookkeeping (semi-Markov controls, completed filtrations, conditional laws) that the paper outsources to its appendices.

Difficulty

The obvious argument fails at the deviation step. In the open-loop setting a deviating player leaves the other players' states unchanged; here the other players' feedback controls react to the deviation, so the state of every player changes. The paper's way around this is to identify the limit with semi-Markov controls and show that the value of a deviation can be approximated by nnn-player deviations of a specific form; making this work requires relaxed controls, a measurable projection onto the filtration of the (random) flow, and well-posedness of SDEs with bounded measurable drift and random coefficients. A newcomer's first idea, passing the Nash inequality to the limit with Markovian limit controls, does not work, because the limit flow is random and the limit control must see its past.

Formalization scope

  • States, laws, paths. Rd\mathbb R^dRd is the platform's EthierKurtz.SDEState d; Brownian motion is the platform's EthierKurtz.IsStandardBrownian. P(E)\mathcal P(E)P(E) is Mathlib's ProbabilityMeasure with the weak topology and the Borel σ\sigmaσ-field of that topology. Paths and flows are continuous maps on [0,T][0,T][0,T] with the uniform topology.
  • Pathwise equations. The volatility is the identity (footnote 4), so every SDE is stated as Xt=X0+∫0tdrift ds+WtX_t=X_0+\int_0^t\text{drift}\,ds+W_tXt​=X0​+∫0t​driftds+Wt​ for all ttt, almost surely; no Itô integral is needed.
  • Solutions are quantified, not chosen. JinJ^n_iJin​ is computed on a given weak solution, and the Nash inequality is required for every solution of the original and of the deviated profile; this is the paper's definition because solutions exist and are unique in law (a milestone).
  • The alternative state in the weak MFE ranges over the solutions adapted to the completed filtration generated by (X0∗,W,μ)(X^*_0,W,\mu)(X0∗​,W,μ) (Remark 2.6), not over all adapted solutions.
  • Indexing. Term nnn of every sequence is the game with n+1n+1n+1 players; "every limit in distribution" quantifies over all subsequences.
  • Explicit hypotheses and corrected misprints. Lemma 5.3 needs μ0=λ\mu_0=\lambdaμ0​=λ a.s.; the paper omits it, and the statement adds it. Lemma 5.3(a) uses Λ∗(s,⋅,μ)\Lambda^*(s,\cdot,\mu)Λ∗(s,⋅,μ) inside ∫0t⋯ds\int_0^t\cdots ds∫0t​⋯ds, where the paper prints ttt. Lemma 5.5 states convergence of (μ,X[βn])(\mu,X[\beta^n])(μ,X[βn]), where the paper prints X[Λn]X[\Lambda^n]X[Λn]. In Definition 3.6(5) the alternative starts from X0∗X^*_0X0∗​, where the paper prints X0∼λX_0\sim\lambdaX0​∼λ. Theorem 5.4's value identity (5.8) is stated along a further subsequence: as printed, along the whole subsequence, it fails for an arbitrary sequence of controls, and the paper's proof passes to a further subsequence. Measurability of every process is explicit, so laws and conditional expectations are never degenerate. Proposition 3.7 is posed for its weak part only.
  • Not a trivialization. The solution class NSol is inhabited and the weak MFE predicate is satisfiable (checked for d=0d=0d=0), so neither the hypotheses nor the conclusion of the goal holds vacuously; the conclusion asserts the existence of a weak MFE with the limiting flow law, not a property of an arbitrary one.
  • Welcome contributions. Weak existence and uniqueness for SDEs with bounded measurable drift (Girsanov, Veretennikov), Prokhorov-type tightness on path space, relaxed-control compactness, and measurable selection are all missing from Mathlib and reusable well beyond this mission.

Selected references

  • D. Lacker, On the convergence of closed-loop Nash equilibria to the mean field game limit, arXiv:1808.02745v1, 2018; Ann. Appl. Probab. 30(4), 2020. https://arxiv.org/abs/1808.02745
  • J.-M. Lasry, P.-L. Lions, Mean field games, Japanese Journal of Mathematics 2(1), 2007. https://doi.org/10.1007/s11537-007-0657-8
  • M. Huang, R. Malhamé, P. Caines, Large population stochastic dynamic games: closed-loop McKean–Vlasov systems and the Nash certainty equivalence principle, Communications in Information and Systems 6(3), 2006. https://doi.org/10.4310/CIS.2006.v6.n3.a5
  • D. Lacker, A general characterization of the mean field limit for stochastic differential games, Probab. Theory Related Fields 165, 2016. https://arxiv.org/abs/1408.2708
  • M. Fischer, On the connection between symmetric N-player games and mean field games, Ann. Appl. Probab. 27(2), 2017. https://arxiv.org/abs/1405.1345
  • P. Cardaliaguet, F. Delarue, J.-M. Lasry, P.-L. Lions, The master equation and the convergence problem in mean field games, Annals of Mathematics Studies 201, 2019. https://arxiv.org/abs/1509.02505
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