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Campaigns (experimental)

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

Block Sensitivity vs. Sensitivity

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

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

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

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

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

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

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

≥ 2.131121719190Formalized record→≥ 2.15Open frontier
9 provers on it18 of 19 missions formalized

Integer Multiplication Below n log n

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

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

For two nnn-bit integers, the target is

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

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

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

3SUM Exponent

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

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

≤ 1.960614Formalized record→≤ 1.9202796Open frontier
4 provers on it7 of 8 missions formalized

All-Pairs Shortest Paths (APSP) Exponent

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

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

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

The irrationality measure of π

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

≤ 7.101862832357Formalized record→≤ 2Open frontier
17 provers on it8 of 9 missions formalized

Sharp diagonal Hlawka constant

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

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

References:

  • Wolfram MathWorld, Hlawka's Inequality.
  • Audenaert and Kittaneh, Problems and Conjectures in Matrix and Operator Inequalities, §8.2 (2017).
  • Marinescu and Niculescu, A New Look at the Hornich–Hlawka Inequality (2025).
  • Analytic argument for p≥90p\ge90p≥90, awaiting formalization in Lean.
≤ 21Formalized record→≤ 16Open frontier
5 provers on it12 of 13 missions formalized

Odd numbers as sums of primes

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

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

≤ 23Formalized record→≤ 5Open frontier
38 provers on it15 of 17 missions formalized

Matrix multiplication exponent

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

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

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

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

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Control TheoryOperations ResearchProbability+1·Captain: mikedeng1

A Mean Field Game of Optimal Portfolio Liquidation 2: The Value Functions of the Penalized Mean Field Games Converge in L¹ to the Value Function of the Liquidation-Constrained GameResearch Paper

Motivation

Optimal portfolio liquidation asks how a trader should unwind a position of X\mathcal XX shares over a horizon [0,T][0,T][0,T] when trading moves prices. Since Almgren and Chriss (2001) the standard model charges a quadratic cost ηtξt2\eta_t\xi_t^2ηt​ξt2​ for trading at rate ξt\xi_tξt​ (temporary impact) and a risk penalty λtXt2\lambda_tX_t^2λt​Xt2​ on the open position, and imposes the liquidation constraint XT=0X_T=0XT​=0. When many traders liquidate at once, each one's costs also depend on the others' aggregate trading rate μt\mu_tμt​ through a permanent impact term κtμtXt\kappa_t\mu_tX_tκt​μt​Xt​. Fu, Graewe, Horst and Popier (arXiv:1804.04911) model this as a mean field game (MFG) with common noise and prove that, under a weak-interaction condition, the game has a unique equilibrium.

The liquidation constraint makes the problem singular: the value function blows up at TTT, and the equilibrium is described by a forward-backward system whose decoupling field AAA satisfies a Riccati BSDE with terminal value AT=+∞A_T=+\inftyAT​=+∞. A natural question is whether the constraint can be replaced by a finite penalty nXT2nX_T^2nXT2​ on the unliquidated position, a non-singular problem of the type studied in the MFG literature, and whether the penalized equilibria approach the constrained one as n→∞n\to\inftyn→∞. Section 4 of the paper answers this at the level of values. In the single-agent case, singular terminal conditions of this type were studied by Ankirchner, Jeanblanc and Kruse (SIAM J. Control Optim., 2014) and Graewe, Horst and Séré (Stochastic Process. Appl., 2018), references [3] and [28] of the paper.

Setting

Fix T>0T>0T>0, an mmm-dimensional Brownian motion W~=(W0,W)\widetilde W=(W^0,W)W=(W0,W) whose first coordinate W0W^0W0 is common noise, and an initial position X∈L2\mathcal X\in L^2X∈L2 independent of W~\widetilde WW. Let F0\mathbb F^0F0 be the filtration of W0W^0W0 and F\mathbb FF that of (X,W~)(\mathcal X,\widetilde W)(X,W), both augmented. The coefficients κ,λ,η\kappa,\lambda,\etaκ,λ,η are bounded, nonnegative, F\mathbb FF-progressive processes, with λ\lambdaλ and η\etaη bounded below by positive constants. Write κmax⁡\kappa_{\max}κmax​, η⋆\eta_\starη⋆​, λ⋆\lambda_\starλ⋆​ for the essential supremum of κ\kappaκ and the essential infima of η\etaη and λ\lambdaλ, ∥η∥\|\eta\|∥η∥ for the essential supremum of ∣η∣|\eta|∣η∣, and α=η⋆/∥η∥∈(0,1]\alpha=\eta_\star/\|\eta\|\in(0,1]α=η⋆​/∥η∥∈(0,1]. Assumption 2.3 adds the weak-interaction condition: some θ>0\theta>0θ>0 satisfies κmax⁡<4η⋆θ\kappa_{\max}<4\eta_\star\thetaκmax​<4η⋆​θ and θκmax⁡<4λ⋆\theta\kappa_{\max}<4\lambda_\starθκmax​<4λ⋆​.

Given an aggregate rate μ\muμ, a trading rate ξ∈LF2\xi\in L^2_{\mathbb F}ξ∈LF2​ yields the position Xtξ=X−∫0tξs dsX^\xi_t=\mathcal X-\int_0^t\xi_s\,dsXtξ​=X−∫0t​ξs​ds. The constrained problem minimizes

J(X,ξ;μ)=E[∫0T(κsμsXsξ+ηsξs2+λs(Xsξ)2)ds ∣ X]J(\mathcal X,\xi;\mu)=\mathbb E\Big[\int_0^T\big(\kappa_s\mu_sX^\xi_s+\eta_s\xi_s^2+\lambda_s(X^\xi_s)^2\big)ds\,\Big|\,\mathcal X\Big]J(X,ξ;μ)=E[∫0T​(κs​μs​Xsξ​+ηs​ξs2​+λs​(Xsξ​)2)ds​X]

over ξ\xiξ with ∫0Tξs ds=X\int_0^T\xi_s\,ds=\mathcal X∫0T​ξs​ds=X; its value is V(X;μ)V(\mathcal X;\mu)V(X;μ). The penalized problem (4.1) drops the constraint and minimizes

Jn(ξ;μ)=E[∫0T(κtμtXtξ+ηtξt2+λt(Xtξ)2)dt+n(XTξ)2 ∣ X]J^n(\xi;\mu)=\mathbb E\Big[\int_0^T\big(\kappa_t\mu_tX^\xi_t+\eta_t\xi_t^2+\lambda_t(X^\xi_t)^2\big)dt+n(X^\xi_T)^2\,\Big|\,\mathcal X\Big]Jn(ξ;μ)=E[∫0T​(κt​μt​Xtξ​+ηt​ξt2​+λt​(Xtξ​)2)dt+n(XTξ​)2​X]

over all ξ∈LF2\xi\in L^2_{\mathbb F}ξ∈LF2​, with value Vn(X;μ)V^n(\mathcal X;\mu)Vn(X;μ). An equilibrium is a fixed point μt=E[ξt∗∣Ft0]\mu_t=\mathbb E[\xi^*_t|\mathcal F^0_t]μt​=E[ξt∗​∣Ft0​].

The constrained equilibrium is given by the FBSDE (2.3), dXt=−Yt2ηtdtdX_t=-\frac{Y_t}{2\eta_t}dtdXt​=−2ηt​Yt​​dt, −dYt=(κtE[Yt2ηt∣Ft0]+2λtXt)dt−Zt dW~t-dY_t=\big(\kappa_t\mathbb E[\frac{Y_t}{2\eta_t}|\mathcal F^0_t]+2\lambda_tX_t\big)dt-Z_t\,d\widetilde W_t−dYt​=(κt​E[2ηt​Yt​​∣Ft0​]+2λt​Xt​)dt−Zt​dWt​, X0=XX_0=\mathcal XX0​=X, XT=0X_T=0XT​=0, decoupled as Y=AX+BY=AX+BY=AX+B where

−dAt=(2λt−At22ηt)dt−ZtA dW~t,AT=+∞.-dA_t=\Big(2\lambda_t-\frac{A_t^2}{2\eta_t}\Big)dt-Z^A_t\,d\widetilde W_t,\qquad A_T=+\infty .−dAt​=(2λt​−2ηt​At2​​)dt−ZtA​dWt​,AT​=+∞.

The penalized equilibria are given by the FBSDE (4.2) with YTn=2nXTnY^n_T=2nX^n_TYTn​=2nXTn​, decoupled by AnA^nAn, the solution of the same Riccati BSDE with ATn=2nA^n_T=2nATn​=2n. The solutions live in weighted spaces: Hl\mathcal H_lHl​ with norm (Esup⁡t∣Yt/(T−t)l∣2)1/2\big(\mathbb E\sup_t|Y_t/(T-t)^l|^2\big)^{1/2}(Esupt​∣Yt​/(T−t)l∣2)1/2, and the penalized analogue Hln\mathcal H^n_lHln​ with weight (T−t+η⋆/n)−l(T-t+\eta_\star/n)^{-l}(T−t+η⋆​/n)−l. Assumption 4.1 requires a constant CCC with exp⁡(−∫rsAu2ηudu)≤CT−sT−r\exp\big(-\int_r^s\frac{A_u}{2\eta_u}du\big)\le C\frac{T-s}{T-r}exp(−∫rs​2ηu​Au​​du)≤CT−rT−s​ for all 0≤r≤s<T0\le r\le s<T0≤r≤s<T, almost surely.

Formalization targets

Goal: Theorem 4.6

Under Assumptions 2.3 and 4.1, with μ∗=E[Y/(2η)∣F0]\mu^*=\mathbb E[Y/(2\eta)|\mathcal F^0]μ∗=E[Y/(2η)∣F0] the constrained equilibrium and μn=E[Yn/(2η)∣F0]\mu^n=\mathbb E[Y^n/(2\eta)|\mathcal F^0]μn=E[Yn/(2η)∣F0] the penalized ones,

lim⁡n→∞E∣Vn(X;μn)−V(X;μ∗)∣=0.\lim_{n\to\infty}\mathbb E\big|V^n(\mathcal X;\mu^n)-V(\mathcal X;\mu^*)\big|=0 .n→∞lim​E​Vn(X;μn)−V(X;μ∗)​=0.

Milestones

  1. Lemma 4.2 (first condition). If η\etaη is deterministic, Assumption 4.1 holds.
  2. Lemma A.3. AnA^nAn exists uniquely, Atn≥(12n+E[∫tTds2ηs∣Ft])−1A^n_t\ge\big(\frac1{2n}+\mathbb E[\int_t^T\frac{ds}{2\eta_s}|\mathcal F_t]\big)^{-1}Atn​≥(2n1​+E[∫tT​2ηs​ds​∣Ft​])−1, An↑AA^n\uparrow AAn↑A, and ∥An∥M−1+∥An∥M−1n≤C\|A^n\|_{\mathcal M_{-1}}+\|A^n\|_{\mathcal M^n_{-1}}\le\mathfrak C∥An∥M−1​​+∥An∥M−1n​​≤C uniformly in nnn.
  3. Theorem 4.3. The FBSDE (4.4), with parameter p∈[0,1]\mathfrak p\in[0,1]p∈[0,1] and data f∈L2f\in L^2f∈L2, has a unique solution in Hαn×Hγn×S2×L2×L2\mathcal H^n_\alpha\times\mathcal H^n_\gamma\times S^2\times L^2\times L^2Hαn​×Hγn​×S2×L2×L2.
  4. Lemma 4.4. ∥Xn∥n,α+∥Bn∥n,γ+E∫0T∣Ytn∣2dt≤C‾\|X^n\|_{n,\alpha}+\|B^n\|_{n,\gamma}+\mathbb E\int_0^T|Y^n_t|^2dt\le\overline{\mathfrak C}∥Xn∥n,α​+∥Bn∥n,γ​+E∫0T​∣Ytn​∣2dt≤C uniformly in nnn.
  5. (4.8). Under Assumption 4.1 the constrained equilibrium position satisfies ∥X∗∥1<∞\|X^*\|_1<\infty∥X∗∥1​<∞.
  6. Lemma 4.5. (Xn,Bn,Yn)→(X,B,Y)(X^n,B^n,Y^n)\to(X,B,Y)(Xn,Bn,Yn)→(X,B,Y) in L2(dt⊗dP)L^2(dt\otimes d\mathbb P)L2(dt⊗dP).

Significance

The result is a consistency statement between two models of liquidation. Penalized models are what a numerical scheme or a standard MFG solver can handle, since their FBSDEs have finite terminal data. Theorem 4.6 says that equilibrium values computed with a large penalty approximate the value of the hard-constrained game, and Lemma 4.5 says the same for positions and trading rates. Without it, a penalized model would be an unrelated object rather than an approximation of the constrained one.

The result is proved in the paper; it is not formalized anywhere. A machine-checked development would need, beyond the paper, the theory of quadratic BSDEs with finite and singular terminal values, conditional mean-field FBSDEs with common noise, and conditional essential infima of control problems. The milestones isolate reusable pieces: the monotone approximation of a singular Riccati BSDE (Lemma A.3) and uniform estimates in nnn-dependent weighted spaces (Lemma 4.4).

Difficulty

The obvious argument compares the two problems control by control: the constrained optimizer is admissible for the penalized problem, so Vn≤VV^n\le VVn≤V up to the change of μ\muμ. The reverse inequality is where it fails. The penalized optimizer leaves a residual position XTn≠0X^n_T\neq0XTn​=0, and its cost has to be compared with the singular one, whose weight (T−t)−1(T-t)^{-1}(T−t)−1 explodes at TTT. Controlling this requires estimates uniform in nnn in spaces whose weights (T−t+η⋆/n)−l(T-t+\eta_\star/n)^{-l}(T−t+η⋆​/n)−l degenerate as n→∞n\to\inftyn→∞, and the bare exponent α=η⋆/∥η∥<1\alpha=\eta_\star/\|\eta\|<1α=η⋆​/∥η∥<1 of the constrained problem is not enough to make the boundary terms vanish. Assumption 4.1, which upgrades the state to H1\mathcal H_1H1​, is what closes the gap. In addition, the aggregate rate μn\mu^nμn changes with nnn, so both the controls and the cost functional move at once.

Formalization scope

Time is R≥0\mathbb R_{\ge0}R≥0​; processes are real-valued functions of (t,ω)(t,\omega)(t,ω); WWW is the m=k+1m=k+1m=k+1-dimensional W~\widetilde WW with coordinate 000 the common noise. Stochastic integrals and BSDEs come from the published definition Peng1990.SMP.Stochastic. BSDEs on [0,T)[0,T)[0,T) are imposed on every [0,τ][0,\tau][0,τ], τ<T\tau<Tτ<T; AT=+∞A_T=+\inftyAT​=+∞ is lim⁡t↑TAt=+∞\lim_{t\uparrow T}A_t=+\inftylimt↑T​At​=+∞ a.s. Conditional expectations inside drivers are F0\mathbb F^0F0-progressive versions of integrable processes. Weighted norms are computed in [0,∞][0,\infty][0,∞]. The explicit readings are:

  • κmax⁡,η⋆,λ⋆,∥η∥\kappa_{\max},\eta_\star,\lambda_\star,\|\eta\|κmax​,η⋆​,λ⋆​,∥η∥ are essential bounds over dt⊗dPdt\otimes d\mathbb Pdt⊗dP; (2.4) is stated without division; "1/λ,1/η∈L∞1/\lambda,1/\eta\in L^\infty1/λ,1/η∈L∞" is a positive essential lower bound.
  • Assumption 2.3 is a hypothesis of every statement, including Lemma A.3 (the appendix assumes only its boundedness part).
  • Assumption 4.1 holds almost surely with the constant chosen before ω\omegaω (as restated on p. 32).
  • The penalty index is an integer n≥1n\ge1n≥1; constants in Lemma A.3 and Lemma 4.4 are chosen before nnn.
  • The class of AnA^nAn is S2×L2S^2\times L^2S2×L2 on [0,T][0,T][0,T] (not printed in Lemma A.3).
  • The penalized control set is LF2L^2_{\mathbb F}LF2​, with no terminal constraint.
  • Values are conditional essential infima given σ(X)\sigma(\mathcal X)σ(X).
  • The equilibria μn,μ∗\mu^n,\mu^*μn,μ∗ of Theorem 4.6 are defined through the FBSDE solutions, as in the proof; uniqueness of penalized equilibria is not claimed.
  • The solution of Proposition 2.8 includes the relation Y=AX+BY=AX+BY=AX+B on [0,T)[0,T)[0,T); "Theorem 2.8" on pp. 25–29 means Proposition 2.8.
  • L1L^1L1 convergence means ∫∣Vn−V∣ dP→0\int|V^n-V|\,d\mathbb P\to0∫∣Vn−V∣dP→0, not convergence of expectations.

A trivializing formalization would quantify over all solutions of the penalized MFG (claiming a uniqueness the paper does not state) or define VVV by a pointwise infimum over all controls (which is −∞-\infty−∞ or junk); both are ruled out above. Contributions toward BSDE comparison principles and quadratic BSDE well-posedness on this stochastic-integral layer are welcome and reusable.

Selected references

  • G. Fu, P. Graewe, U. Horst, A. Popier, A Mean Field Game of Optimal Portfolio Liquidation, Math. Oper. Res. 46(4), 2021; preprint arXiv:1804.04911v3. https://arxiv.org/abs/1804.04911
  • R. Almgren, N. Chriss, Optimal execution of portfolio transactions, Journal of Risk 3, 2001. https://doi.org/10.21314/JOR.2001.041
  • S. Ankirchner, M. Jeanblanc, T. Kruse, BSDEs with singular terminal condition and a control problem with constraints, SIAM J. Control Optim. 52(2):893–913, 2014 (reference [3] of the paper).
  • P. Graewe, U. Horst, E. Séré, Smooth solutions to portfolio liquidation problems under price-sensitive market impact, Stochastic Process. Appl. 128(3):979–1006, 2018 (reference [28] of the paper).
  • S. Peng, A general stochastic maximum principle for optimal control problems, SIAM J. Control Optim. 28(4), 1990. https://doi.org/10.1137/0328054
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Linear OptimizationMachine LearningOperations Research+1·Captain: mikedeng1

Strong Mixed-Integer Programming Formulations for Trained Neural Networks 1: A ReLU Neuron over a Box Has an Ideal Formulation with One Binary Variable and the Exponential Family (6b)Research Paper

Why optimize over a trained ReLU neuron

A trained feed-forward neural network with ReLU activations, ReLU(v)=max⁡{0,v}\mathrm{ReLU}(v)=\max\{0,v\}ReLU(v)=max{0,v}, is a piecewise linear function of its input. Many tasks ask for an optimization over such a network with its weights held fixed: verifying that no small perturbation of an image changes its classification, finding adversarial examples, or embedding a learned model of demand or cost inside a decision problem ("predict, then optimize"). The standard way to solve such problems exactly is mixed-integer programming (MIP): each neuron is written as a small set of linear constraints with one binary variable, and the network is the composition of these neuron formulations. How strong each neuron formulation is decides how fast branch-and-bound can close the gap.

The formulation used in the literature up to 2018 is the big-M formulation. It is valid but weak. This mission formalizes the main result of Anderson, Huchette, Tjandraatmadja and Vielma, IPCO 2019 extended abstract (arXiv:1811.08359v2), which gives the strongest possible formulation of a single ReLU neuron that uses the original variables and one binary variable only.

Timeline. Big-M formulations of ReLU networks were used by several groups in 2017–2018 for verification and adversarial analysis (see §1.2 of the paper). Balas's disjunctive programming (1985, 1998) and the multiple choice formulation of piecewise linear functions (Vielma and Nemhauser, Math. Program. 2011) give an ideal formulation of the neuron that needs a copy of the input variables. Anderson et al. (2019) project out that copy and obtain the formulation (6) below; a longer journal version (Math. Program. 2020, with W. Ma) develops the analysis further, including interactions between neurons.

Setting

Fix η∈N\eta\in\mathbb Nη∈N, a weight vector w∈Rηw\in\mathbb R^\etaw∈Rη, a bias b∈Rb\in\mathbb Rb∈R, and bounds L,U∈RηL,U\in\mathbb R^\etaL,U∈Rη with Li<UiL_i<U_iLi​<Ui​ for every iii. The neuron computes ReLU(f(x))\mathrm{ReLU}(f(x))ReLU(f(x)) for the affine function f(x)=w⋅x+bf(x)=w\cdot x+bf(x)=w⋅x+b on the box [L,U]={x:L≤x≤U}[L,U]=\{x: L\le x\le U\}[L,U]={x:L≤x≤U}. Its graph is

gr⁡(ReLU∘f;[L,U])={(x,ReLU(f(x))):L≤x≤U}.\operatorname{gr}(\mathrm{ReLU}\circ f;[L,U])=\{(x,\mathrm{ReLU}(f(x))) : L\le x\le U\}.gr(ReLU∘f;[L,U])={(x,ReLU(f(x))):L≤x≤U}.

The sign-adjusted bounds are L˘i=Li\breve L_i=L_iL˘i​=Li​, U˘i=Ui\breve U_i=U_iU˘i​=Ui​ when wi≥0w_i\ge 0wi​≥0, and L˘i=Ui\breve L_i=U_iL˘i​=Ui​, U˘i=Li\breve U_i=L_iU˘i​=Li​ when wi<0w_i<0wi​<0. Then M+(f)=w⋅U˘+bM^+(f)=w\cdot\breve U+bM+(f)=w⋅U˘+b and M−(f)=w⋅L˘+bM^-(f)=w\cdot\breve L+bM−(f)=w⋅L˘+b are the maximum and minimum of fff on [L,U][L,U][L,U], and supp⁡(w)={i:wi≠0}\operatorname{supp}(w)=\{i: w_i\ne 0\}supp(w)={i:wi​=0}. Strict activity means M−(f)<0<M+(f)M^-(f)<0<M^+(f)M−(f)<0<M+(f): the neuron is neither always off nor always on. The paper assumes throughout that Li<UiL_i<U_iLi​<Ui​ and that strict activity holds.

A set RRR of points (x,y,z)(x,y,z)(x,y,z) with z∈[0,1]z\in[0,1]z∈[0,1], read together with the constraint z∈{0,1}z\in\{0,1\}z∈{0,1}, is a formulation of the graph if (x,y)(x,y)(x,y) lies on the graph exactly when (x,y,z)∈R(x,y,z)\in R(x,y,z)∈R for some z∈{0,1}z\in\{0,1\}z∈{0,1}; RRR is then its LP relaxation. The formulation is ideal if every extreme point of RRR has z∈{0,1}z\in\{0,1\}z∈{0,1}.

The big-M formulation (3) is y≥f(x)y\ge f(x)y≥f(x), y≤f(x)−M−(f)(1−z)y\le f(x)-M^-(f)(1-z)y≤f(x)−M−(f)(1−z), y≤M+(f)zy\le M^+(f)zy≤M+(f)z, (x,y,z)∈[L,U]×R≥0×{0,1}(x,y,z)\in[L,U]\times\mathbb R_{\ge0}\times\{0,1\}(x,y,z)∈[L,U]×R≥0​×{0,1}. The formulation of Proposition 1 is

y≥w⋅x+b(6a)y≤∑i∈Iwi(xi−L˘i(1−z))+(b+∑i∉IwiU˘i)z∀I⊆supp⁡(w)(6b)(x,y,z)∈[L,U]×R≥0×{0,1}.(6c)\begin{aligned} &y\ge w\cdot x+b &&(6a)\\ &y\le\sum_{i\in I}w_i\bigl(x_i-\breve L_i(1-z)\bigr)+\Bigl(b+\sum_{i\notin I}w_i\breve U_i\Bigr)z\qquad\forall I\subseteq\operatorname{supp}(w) &&(6b)\\ &(x,y,z)\in[L,U]\times\mathbb R_{\ge0}\times\{0,1\}. &&(6c) \end{aligned}​y≥w⋅x+by≤i∈I∑​wi​(xi​−L˘i​(1−z))+(b+i∈/I∑​wi​U˘i​)z∀I⊆supp(w)(x,y,z)∈[L,U]×R≥0​×{0,1}.​​(6a)(6b)(6c)​

Formalization targets

Goal: Proposition 1 (p. 6)

(6a)–(6c) is a formulation of gr⁡(ReLU∘f;[L,U]), and every extreme point of its LP relaxation has z∈{0,1}.\text{(6a)–(6c) is a formulation of }\operatorname{gr}(\mathrm{ReLU}\circ f;[L,U]),\ \text{and every extreme point of its LP relaxation has } z\in\{0,1\}.(6a)–(6c) is a formulation of gr(ReLU∘f;[L,U]), and every extreme point of its LP relaxation has z∈{0,1}.

Milestones (Appendix A.1 and §2.2)

  1. The multiple choice formulation (5), with copies x0,x1,y0,y1x^0,x^1,y^0,y^1x0,x1,y0,y1, has only integral zzz at extreme points in its lifted space and formulates the graph; projected to (x,y,z)(x,y,z)(x,y,z), its LP relaxation is the convex hull of its points with z∈{0,1}z\in\{0,1\}z∈{0,1} (§2.2, pp. 5–6).
  2. Projecting the copies out of the LP relaxation of (5) gives the linear system (7): (6a), (6b), a second exponential family (7c), and the bounds (7d) (App. A.1, p. 14).
  3. The family (7c) is implied by the other constraints (App. A.1, pp. 14–15).
  4. The LP relaxation of (6) is the convex hull of its points with z∈{0,1}z\in\{0,1\}z∈{0,1} (App. A.1, p. 14).

Companion results

  • M±(f)M^\pm(f)M±(f) are the maximum and minimum of fff on [L,U][L,U][L,U] (§1.3, p. 4).
  • Proposition 3 (p. 7): for (x^,y^,z^)∈[L,U]×R≥0×[0,1](\hat x,\hat y,\hat z)\in[L,U]\times\mathbb R_{\ge0}\times[0,1](x^,y^​,z^)∈[L,U]×R≥0​×[0,1], if some inequality of (6b) is violated, the one for I^={i∈supp⁡(w):wix^i<wi(L˘i(1−z^)+U˘iz^)}\hat I=\{i\in\operatorname{supp}(w): w_i\hat x_i<w_i(\breve L_i(1-\hat z)+\breve U_i\hat z)\}I^={i∈supp(w):wi​x^i​<wi​(L˘i​(1−z^)+U˘i​z^)} is the most violated.
  • The big-M formulation (3) is a formulation of the graph (p. 4); Examples 1 and 2 (p. 5) show that it is not ideal and that its gap grows like 12γη\tfrac12\gamma\eta21​γη; its inequalities (3b), (3c) are (6b) for I=supp⁡(w)I=\operatorname{supp}(w)I=supp(w) and I=∅I=\emptysetI=∅ (p. 7).

Significance

Proposition 1 says that the convex hull of the graph, lifted with one binary variable, is described by (6a), (6b) and the bounds, with no auxiliary continuous variables. Optimizing a linear function over the LP relaxation of (6) therefore gives the tightest convex relaxation available for a single neuron, and Proposition 3 gives a separation routine linear in η\etaη, so the exponential family can be added on demand to a big-M model. The paper's experiments (§3, not formalized) report that separating over (6b) solves smaller MNIST verification instances faster than Gurobi's default cut generation by a factor of 7.

The result is proved in the paper; nothing here is open. To our knowledge none of these statements has a machine-checked proof. The work this mission asks for is the formalization of the known proof: an ideality statement for the multiple choice formulation, a Fourier–Motzkin projection carried out for an arbitrary index set with general-sign weights, and the passage from a hull identity to integrality of extreme points.

Difficulty

The formulation half of Proposition 1 is a short case analysis on z∈{0,1}z\in\{0,1\}z∈{0,1}; the content is ideality. The obvious attempt, characterizing the extreme points of the LP relaxation of (6) directly, is impractical: the polytope is cut out by 2∣supp⁡(w)∣2^{|\operatorname{supp}(w)|}2∣supp(w)∣ inequalities, and showing that every point with fractional zzz is a proper convex combination of feasible points means handling all patterns of tight inequalities of (6b) at once. Ideality of the extended formulation (5) is classical and passes to its projection onto (x,y,z)(x,y,z)(x,y,z), but that only helps once the projection is known to be exactly the LP relaxation of (6): it has to be computed for an arbitrary index set, and every inequality it produces must be shown to be one of (6a), (6b), the bounds, or implied by them. Weights of both signs must be handled throughout: the page treats negative weights by a change of variables, and a formal development has to carry the sign-adjusted bounds L˘,U˘\breve L,\breve UL˘,U˘ through every step.

Formalization scope

Inputs x∈Rηx\in\mathbb R^\etax∈Rη are Fin η → ℝ, so indices are 0-based; points (x,y,z)(x,y,z)(x,y,z) are (Fin η → ℝ) × ℝ × ℝ. A formulation is encoded by its LP relaxation RRR (with z∈[0,1]z\in[0,1]z∈[0,1]) and the predicate "(x,y)∈S(x,y)\in S(x,y)∈S iff (x,y,z)∈R(x,y,z)\in R(x,y,z)∈R for some z∈{0,1}z\in\{0,1\}z∈{0,1}"; ideality is ∀ p ∈ Set.extremePoints ℝ R, p.2.2 = 0 ∨ p.2.2 = 1. M±(f)M^\pm(f)M±(f) are defined by their closed forms, and a companion theorem proves that they are the maximum and minimum. In (6b) and (7c), "i∉Ii\notin Ii∈/I" ranges over all indices outside III, zero weights included. The system (7) is stated with L˘,U˘\breve L,\breve UL˘,U˘, i.e. after undoing the page's substitution x~i=−xi\tilde x_i=-x_ix~i​=−xi​; for w≥0w\ge 0w≥0 it is the page's display. The LP relaxation of (5) is represented both in its lifted space and projected to (x,y,z)(x,y,z)(x,y,z), with the copies quantified existentially in the latter, and constant bbb is scaled by 1−z1-z1−z in (5b) and by zzz in (5c).

The goal carries both standing assumptions of §1.3 (Li<UiL_i<U_iLi​<Ui​ and strict activity) and nothing else. Milestones that do not need strict activity omit it, which makes them stronger. Example 2 includes the page's γ=0\gamma=0γ=0 boundary: although its box then violates Li<UiL_i<U_iLi​<Ui​ when η>0\eta>0η>0, the example's three stated claims remain true.

Ideality is a statement about the LP relaxation, not about the set with z∈{0,1}z\in\{0,1\}z∈{0,1}: applied to the latter it would hold trivially, and a goal stating only that (6) is a formulation would omit the result's content. Both are ruled out by the statement of the goal.

A complete development needs: extreme points and convex hulls of polyhedra in product spaces (Mathlib), the hull of a union of two polytopes as a projection, Fourier–Motzkin elimination over an arbitrary finite index set, and finite-sum manipulations over subsets of supp⁡(w)\operatorname{supp}(w)supp(w). The Fourier–Motzkin and disjunctive-hull lemmas are reusable well beyond this mission; contributions of either are welcome, as are proofs of the companion results.

Source: the IPCO 2019 extended abstract, arXiv:1811.08359v2 (28 Feb 2019); all labels and pages refer to that version.

Selected references

  • R. Anderson, J. Huchette, C. Tjandraatmadja, J. P. Vielma, Strong mixed-integer programming formulations for trained neural networks, IPCO 2019 (LNCS 11480), extended abstract. arXiv:1811.08359v2
  • R. Anderson, J. Huchette, W. Ma, C. Tjandraatmadja, J. P. Vielma, Strong mixed-integer programming formulations for trained neural networks, Mathematical Programming 183 (2020) 3–39. doi:10.1007/s10107-020-01474-5, arXiv:1811.01988
  • J. P. Vielma, G. Nemhauser, Modeling disjunctive constraints with a logarithmic number of binary variables and constraints, Mathematical Programming 128 (2011) 49–72. doi:10.1007/s10107-009-0295-4
  • E. Balas, Disjunctive programming and a hierarchy of relaxations for discrete optimization problems, SIAM Journal on Algebraic and Discrete Methods 6(3) (1985) 466–486. doi:10.1137/0606047
  • E. Balas, Disjunctive programming: properties of the convex hull of feasible points, Discrete Applied Mathematics 89 (1998) 3–44. doi:10.1016/S0166-218X(98)00136-X
  • J. P. Vielma, Mixed integer linear programming formulation techniques, SIAM Review 57(1) (2015) 3–57. doi:10.1137/130915303
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Convex OptimizationOptimization·Captain: mikedeng1

A Block Successive Upper-Bound Minimization Method of Multipliers for Linearly Constrained Convex Optimization 1: Cyclic BSUM-M Converges to Primal-Dual Optimal SolutionsResearch Paper

Motivation

Many problems in signal processing, machine learning and power systems have the form of a convex objective that is a sum of a smooth coupled term and nonsmooth block-separable terms, minimized subject to linear equality constraints that couple KKK blocks of variables: basis pursuit, demand response control in smart grids, and distributed estimation are the examples of Hong, Chang, Wang, Razaviyayn, Ma, Luo. The alternating direction method of multipliers (ADMM) handles two blocks well, but for K≥3K\ge3K≥3 blocks the directly extended Gauss–Seidel ADMM can diverge (Chen, He, Ye, Yuan, 2016), and convergence proofs for multi-block schemes usually need strong convexity or extra correction steps.

The block successive upper-bound minimization method of multipliers (BSUM-M) is the paper's answer: each block is updated by minimizing a local upper bound of the augmented Lagrangian, which makes the subproblems simple (for instance closed-form proximal steps), and the multiplier is updated by a dual gradient step with a small or diminishing stepsize. The main theorem shows that this scheme converges to primal and dual optimal solutions for any number of blocks without strong convexity, under an error bound.

Setting

The variable is x=(x1,…,xK)x=(x_1,\dots,x_K)x=(x1​,…,xK​), xk∈Rnkx_k\in\mathbb R^{n_k}xk​∈Rnk​, with the Euclidean norm ∥x∥2=∑k∥xk∥2\|x\|^2=\sum_k\|x_k\|^2∥x∥2=∑k​∥xk​∥2. Problem (1.1) is

min⁡x f(x)=g(x)+∑k=1Khk(xk)s.t.Ex=∑k=1KEkxk=q,xk∈Xk.\min_x\ f(x)=g(x)+\sum_{k=1}^K h_k(x_k)\quad\text{s.t.}\quad Ex=\sum_{k=1}^KE_kx_k=q,\quad x_k\in X_k .xmin​ f(x)=g(x)+k=1∑K​hk​(xk​)s.t.Ex=k=1∑K​Ek​xk​=q,xk​∈Xk​.

Under the standing Assumption A, g(x)=ℓ(Ax)+⟨x,b⟩g(x)=\ell(Ax)+\langle x,b\rangleg(x)=ℓ(Ax)+⟨x,b⟩ with ℓ\ellℓ strictly convex and continuously differentiable and AAA any matrix; hk(xk)=λk∥xk∥1+∑JwJ∥xk,J∥2h_k(x_k)=\lambda_k\|x_k\|_1+\sum_Jw_J\|x_{k,J}\|_2hk​(xk​)=λk​∥xk​∥1​+∑J​wJ​∥xk,J​∥2​ is a mixed ℓ1/ℓ2\ell_1/\ell_2ℓ1​/ℓ2​ norm with nonnegative weights; each Xk={xk∣Ckxk≤ck}X_k=\{x_k\mid C_kx_k\le c_k\}Xk​={xk​∣Ck​xk​≤ck​} is a compact polyhedron and X=∏kXkX=\prod_kX_kX=∏k​Xk​; the problem is feasible and the dual optimal value is attained.

For ρ>0\rho>0ρ>0, the augmented Lagrangian is L(x;y)=f(x)+⟨y,q−Ex⟩+ρ2∥q−Ex∥2L(x;y)=f(x)+\langle y,q-Ex\rangle+\frac\rho2\|q-Ex\|^2L(x;y)=f(x)+⟨y,q−Ex⟩+2ρ​∥q−Ex∥2, the augmented dual is d(y)=min⁡x∈XL(x;y)d(y)=\min_{x\in X}L(x;y)d(y)=minx∈X​L(x;y), and X(y)=arg⁡min⁡x∈XL(x;y)X(y)=\arg\min_{x\in X}L(x;y)X(y)=argminx∈X​L(x;y). For x∈Xx\in Xx∈X, xˉ\bar xxˉ denotes the point of X(y)X(y)X(y) nearest to xxx.

Assumption B concerns the approximation functions uk(vk;x)u_k(v_k;x)uk​(vk​;x): each upper-bounds G(x)=g(x)+ρ2∥Ex−q∥2G(x)=g(x)+\frac\rho2\|Ex-q\|^2G(x)=g(x)+2ρ​∥Ex−q∥2 along block kkk, is tight with matching gradient at vk=xkv_k=x_kvk​=xk​, is continuous, strongly convex in vkv_kvk​ with a uniform modulus γk>0\gamma_k>0γk​>0, and has an LkL_kLk​-Lipschitz gradient in vkv_kvk​.

BSUM-M (1.12). From x1∈Xx^1\in Xx1∈X and any y1y^1y1, for r≥1r\ge1r≥1:

yr+1=yr+αr(q−Exr),xkr+1=arg⁡min⁡xk∈Xkuk(xk;wkr+1)−⟨yr+1,Ekxk⟩+hk(xk),y^{r+1}=y^r+\alpha^r(q-Ex^r),\qquad x_k^{r+1}=\arg\min_{x_k\in X_k}u_k(x_k;w_k^{r+1})-\langle y^{r+1},E_kx_k\rangle+h_k(x_k),yr+1=yr+αr(q−Exr),xkr+1​=argxk​∈Xk​min​uk​(xk​;wkr+1​)−⟨yr+1,Ek​xk​⟩+hk​(xk​),

for k=1,…,Kk=1,\dots,Kk=1,…,K in order, with the Gauss–Seidel point wkr+1=(x1r+1,…,xk−1r+1,xkr,…,xKr)w_k^{r+1}=(x_1^{r+1},\dots,x_{k-1}^{r+1},x_k^r,\dots,x_K^r)wkr+1​=(x1r+1​,…,xk−1r+1​,xkr​,…,xKr​).

The proximal gradient is ∇~xL(x;y)=x−prox⁡(x−∇x(L(x;y)−h(x)))\tilde\nabla_xL(x;y)=x-\operatorname{prox}(x-\nabla_x(L(x;y)-h(x)))∇~x​L(x;y)=x−prox(x−∇x​(L(x;y)−h(x))) with prox⁡(z)=arg⁡min⁡u∈Xh(u)+12∥z−u∥2\operatorname{prox}(z)=\arg\min_{u\in X}h(u)+\frac12\|z-u\|^2prox(z)=argminu∈X​h(u)+21​∥z−u∥2. The error bound asks for τ>0\tau>0τ>0 with dist⁡(x,X(y))≤τ∥∇~xL(x;y)∥\operatorname{dist}(x,X(y))\le\tau\|\tilde\nabla_xL(x;y)\|dist(x,X(y))≤τ∥∇~x​L(x;y)∥ for all x∈Xx\in Xx∈X and all yyy.

Formalization targets

Goal: Theorem 2.1, part 1

Under Assumptions A and B and the error bound, there is αˉ>0\bar\alpha>0αˉ>0 such that for stepsizes αr>0\alpha^r>0αr>0 that are either constant with αr=α≤αˉ\alpha^r=\alpha\le\bar\alphaαr=α≤αˉ, or satisfy ∑rαr=∞\sum_r\alpha^r=\infty∑r​αr=∞ and αr→0\alpha^r\to0αr→0, every BSUM-M run satisfies

lim⁡r→∞∥Exr−q∥=0,lim⁡r→∞∥xr−xr+1∥=0,lim⁡r→∞∥xr−xˉr∥=0,\lim_{r\to\infty}\|Ex^r-q\|=0,\qquad\lim_{r\to\infty}\|x^r-x^{r+1}\|=0,\qquad\lim_{r\to\infty}\|x^r-\bar x^r\|=0,r→∞lim​∥Exr−q∥=0,r→∞lim​∥xr−xr+1∥=0,r→∞lim​∥xr−xˉr∥=0,

and every limit point of {(xr,yr)}\{(x^r,y^r)\}{(xr,yr)} is a primal and dual optimal solution. The threshold αˉ\bar\alphaαˉ is not specified; no rate is claimed.

Milestones

Lemma 2.3(1) (one sweep decreases L(⋅;yr+1)L(\cdot;y^{r+1})L(⋅;yr+1) by γ∥xr−xr+1∥2\gamma\|x^r-x^{r+1}\|^2γ∥xr−xr+1∥2), Lemma 2.5(1) (dual gap decrease), Lemma 2.6(1) (primal gap bound), Lemma 2.4(1) (the proximal gradient at xrx^rxr is O(∥xr+1−xr∥)O(\|x^{r+1}-x^r\|)O(∥xr+1−xr∥)) and Lemma 2.1 (differentiability of ddd, ∇d(y)=q−Ex(y)\nabla d(y)=q-Ex(y)∇d(y)=q−Ex(y), and Lipschitz continuity of ∇d\nabla d∇d on superlevel sets).

Significance

The theorem gives a convergent multi-block method of multipliers whose block subproblems may be replaced by any majorizer satisfying Assumption B, such as a linearized proximal step. It covers the cyclic Gauss–Seidel order, where the direct multi-block ADMM can fail, and it does not require strong convexity of fff (the matrix AAA need not have full column rank). The paper's randomized variant (part 2 of the same theorem) is a separate mission.

The result is proved in the paper (the proof of part 1 is described as following the steps written out for part 2). It has not been machine-checked. Formalization adds a verified account of the potential-function argument for a primal-dual method with inexact block updates, and checks three printed statements that need correction (see the scope section): a formal proof settles them.

Difficulty

The obvious approach is to treat BSUM-M as an inexact dual gradient ascent on ddd, but a single Gauss–Seidel sweep does not compute x(yr+1)∈X(yr+1)x(y^{r+1})\in X(y^{r+1})x(yr+1)∈X(yr+1), so the dual step uses a gradient at the wrong point. Controlling that error requires relating the primal step length to the distance from X(y)X(y)X(y), which fails without an error bound: L(⋅;y)L(\cdot;y)L(⋅;y) is not strongly convex, X(y)X(y)X(y) need not be a singleton, and the proximal gradient can be small far from X(y)X(y)X(y). The cyclic order adds a second gap: block kkk is linearized at wkr+1w_k^{r+1}wkr+1​, not at xrx^rxr. With a constant stepsize the dual ascent must not outrun the primal descent, which is where the smallness threshold enters.

Formalization scope

Citation basis: the arXiv preprint arXiv:1401.7079v1 (28 Jan 2014); every index refers to that version, not to the revised journal version (Mathematics of Operations Research, 2020).

Representation: blocks are indexed by Fin K with K≥1K\ge1K≥1; the block space is PiLp 2 of Euclidean spaces (the Euclidean norm, not the sup norm). ℓ\ellℓ is real valued and C1C^1C1 on all of Rp\mathbb R^pRp, which specializes the paper's extended-valued ℓ\ellℓ. ddd, d∗d^*d∗ and f∗f^*f∗ are real infima and suprema over nonempty compact sets, where they are attained. The algorithm is a predicate on sequences indexed from r=1r=1r=1; argmin steps are minimality conditions, the minimizer being unique. The initial point is required to lie in XXX. "Sufficiently small" is an existential threshold quantified before the stepsizes and the run. ∥xr−xˉr∥\|x^r-\bar x^r\|∥xr−xˉr∥ is the distance from xrx^rxr to X(yr)X(y^r)X(yr). Limit points are cluster points of the joint sequence; boundedness of {yr}\{y^r\}{yr} is neither assumed nor concluded.

Interpretations and corrections, each labelled in the item's statement:

  • the proximity operator in (2.3) includes the constraint set XXX, as the paper's optimality relation (2.14) requires;
  • d(y)d(y)d(y) is min⁡x∈XL(x;y)\min_{x\in X}L(x;y)minx∈X​L(x;y); (1.9) prints g(x)g(x)g(x) and an unconstrained minimum;
  • (2.17) has ExrEx^rExr where its proof (2.19) has Exr−1Ex^{r-1}Exr−1; the proved inequality is stated;
  • (2.12) evaluates the proximal gradient at yry^ryr and is false at r=1r=1r=1; it is stated at yr+1y^{r+1}yr+1;
  • Lemma 2.1's clause "AkxkA_kx_kAk​xk​ constant on X(y)X(y)X(y)" fails for non-separable ℓ\ellℓ; it is stated as "AxAxAx constant".

The error bound is a hypothesis of the goal, as in the paper, and is not derived from Assumption A: the paper's Lemma 2.2 does not hold under Assumption A alone. A formalization that makes the hypotheses unsatisfiable, drops the run's dependence on yr+1y^{r+1}yr+1, or lets αˉ\bar\alphaαˉ depend on the run is not this theorem. A sanity check that the hypotheses are satisfiable (a one-block instance with a constant run) is part of the drafting record.

Infrastructure needed: proximity operators of convex functions restricted to polyhedra and their nonexpansiveness; Danskin-type differentiability of a parametric minimum over a compact set; smoothness of the augmented dual; elementary convergence lemmas for nonnegative sequences with summable decrements. These pieces are reusable for other augmented Lagrangian and ADMM analyses. Proofs of the milestones are welcome independently of the goal.

Selected references

  • M. Hong, T.-H. Chang, X. Wang, M. Razaviyayn, S. Ma, Z.-Q. Luo, A Block Successive Upper Bound Minimization Method of Multipliers for Linearly Constrained Convex Optimization, arXiv:1401.7079v1, 2014; Mathematics of Operations Research 45(3), 2020. https://arxiv.org/abs/1401.7079 , https://doi.org/10.1287/moor.2019.1010
  • M. Hong, Z.-Q. Luo, On the linear convergence of the alternating direction method of multipliers, Mathematical Programming 162, 2017. https://doi.org/10.1007/s10107-016-1034-2
  • M. Razaviyayn, M. Hong, Z.-Q. Luo, A unified convergence analysis of block successive minimization methods for nonsmooth optimization, SIAM Journal on Optimization 23(2), 2013. https://doi.org/10.1137/120891009
  • C. Chen, B. He, Y. Ye, X. Yuan, The direct extension of ADMM for multi-block convex minimization problems is not necessarily convergent, Mathematical Programming 155, 2016. https://doi.org/10.1007/s10107-014-0826-5
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AnalysisFunctional AnalysisProbability·Captain: mikedeng1

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

Motivation

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

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

Setting

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

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

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

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

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

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

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

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

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

Formalization targets

Goal: Corollary 2.3

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

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

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

Milestones

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

Significance

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

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

Difficulty

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

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

Formalization scope

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

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

Selected references

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

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

Motivation

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

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

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

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

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

Setting

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

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

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

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

The SDE of the main theorem is

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

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

Formalization targets

Goal: Theorem 4.1

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

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

Milestones

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

Significance

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

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

Difficulty

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

Formalization scope

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

Deviations from the page, all disclosed in the statements:

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

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

Selected references

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

A Mean Field Game of Optimal Portfolio Liquidation 1: Under Weak Interaction the Liquidation Mean Field Game Has a Unique Equilibrium, Given by a Singular Conditional Mean-Field FBSDEResearch Paper

Motivation

Large traders who must unwind a position by a deadline face a trade-off between trading fast, which moves prices against them, and trading slowly, which exposes them to price risk. When many traders liquidate at once, each one's execution price also depends on the aggregate selling rate of the others. Fu, Graewe, Horst and Popier (arXiv:1804.04911) model this as a mean field game (MFG) with common noise and a hard liquidation constraint: every position must be zero at the terminal time TTT. Single-player liquidation with this constraint leads to backward equations with singular terminal values (Ankirchner, Jeanblanc and Kruse, SIAM J. Control Optim. 2014; Graewe, Horst and Séré, Stoch. Proc. Appl. 2018). Earlier MFG models of execution (Cardaliaguet and Lehalle, Math. Financ. Econ. 2018; Carmona and Lacker, Ann. Appl. Probab. 2015) allow no liquidation constraint. This mission formalizes the paper's first main result: the constrained game has a unique equilibrium under a weak-interaction condition.

Setting

Fix T>0T>0T>0 and a probability space carrying an mmm-dimensional Brownian motion W~=(W0,W)\widetilde W=(W^0,W)W=(W0,W), where W0W^0W0 is the one-dimensional common noise, and an initial portfolio X∈L2\mathcal X\in L^2X∈L2 independent of W~\widetilde WW. Let F0\mathbb F^0F0 be the filtration of W0W^0W0 and F\mathbb FF that of (X,W0,W)(\mathcal X,W^0,W)(X,W0,W), both augmented by null sets. The cost coefficients are bounded nonnegative F\mathbb FF-progressive processes κ\kappaκ (interaction), λ\lambdaλ (risk aversion) and η\etaη (temporary impact), with λ,η\lambda,\etaλ,η bounded away from zero.

A player's trading rate ξ\xiξ produces the position Xtξ=X−∫0tξsdsX^\xi_t=\mathcal X-\int_0^t\xi_sdsXtξ​=X−∫0t​ξs​ds. The admissible strategies are AF(X)={ξ∈LF2:∫0Tξsds=X}\mathcal A_{\mathbb F}(\mathcal X)=\{\xi\in L^2_{\mathbb F}:\int_0^T\xi_sds=\mathcal X\}AF​(X)={ξ∈LF2​:∫0T​ξs​ds=X}. Given an F0\mathbb F^0F0-progressive aggregate rate μ\muμ, the cost is

J(X,ξ;μ)=E[∫0T(κsXsξμs+ηsξs2+λs(Xsξ)2)ds ∣ X],J(\mathcal X,\xi;\mu)=\mathbb E\Big[\int_0^T\big(\kappa_sX^\xi_s\mu_s+\eta_s\xi_s^2+\lambda_s(X^\xi_s)^2\big)ds\ \Big|\ \mathcal X\Big],J(X,ξ;μ)=E[∫0T​(κs​Xsξ​μs​+ηs​ξs2​+λs​(Xsξ​)2)ds ​ X],

and V(X;μ)V(\mathcal X;\mu)V(X;μ) is its essential infimum over AF(X)\mathcal A_{\mathbb F}(\mathcal X)AF​(X). A process μ\muμ solves the MFG (1.7) if some optimal strategy ξ∗\xi^*ξ∗ given μ\muμ satisfies μt=E[ξt∗∣Ft0]\mu_t=\mathbb E[\xi^*_t\mid\mathcal F^0_t]μt​=E[ξt∗​∣Ft0​] for a.e. ttt.

The equilibrium is described by the conditional mean-field FBSDE (2.3):

Xt=X−∫0tYs2ηsds,XT=0,−dYt=(κt E[Yt2ηt∣Ft0]+2λtXt)dt−Zt dW~t  on [0,T).X_t=\mathcal X-\int_0^t\frac{Y_s}{2\eta_s}ds,\quad X_T=0,\quad -dY_t=\Big(\kappa_t\,\mathbb E\Big[\frac{Y_t}{2\eta_t}\Big|\mathcal F^0_t\Big]+2\lambda_tX_t\Big)dt-Z_t\,d\widetilde W_t\ \ \text{on }[0,T).Xt​=X−∫0t​2ηs​Ys​​ds,XT​=0,−dYt​=(κt​E[2ηt​Yt​​​Ft0​]+2λt​Xt​)dt−Zt​dWt​  on [0,T).

Solutions are sought in weighted spaces: Y∈HlY\in\mathcal H_lY∈Hl​ if Esup⁡t≤T∣Yt/(T−t)l∣2<∞\mathbb E\sup_{t\le T}|Y_t/(T-t)^l|^2<\inftyEsupt≤T​∣Yt​/(T−t)l∣2<∞, and Y∈MlY\in\mathcal M_lY∈Ml​ if (T−t)−l∣Yt∣(T-t)^{-l}|Y_t|(T−t)−l∣Yt​∣ is essentially bounded. The weak-interaction condition (Assumption 2.3) asks for θ>0\theta>0θ>0 with κmax⁡/(4η⋆)<θ<4λ⋆/κmax⁡\kappa_{\max}/(4\eta_\star)<\theta<4\lambda_\star/\kappa_{\max}κmax​/(4η⋆​)<θ<4λ⋆​/κmax​, and α:=η⋆/∥η∥∈(0,1]\alpha:=\eta_\star/\|\eta\|\in(0,1]α:=η⋆​/∥η∥∈(0,1]. The decoupling Y=AX+BY=AX+BY=AX+B uses the solution AAA of the singular Riccati BSDE −dAt=(2λt−At2/(2ηt))dt−ZtAdW~t-dA_t=(2\lambda_t-A_t^2/(2\eta_t))dt-Z^A_td\widetilde W_t−dAt​=(2λt​−At2​/(2ηt​))dt−ZtA​dWt​, AT=+∞A_T=+\inftyAT​=+∞.

Formalization targets

Goal: Theorem 2.4

Under Assumption 2.3 the FBSDE (2.3) has a unique solution

(X,Y,Z)∈Hα×LF2([0,T])×LF2([0,T−];Rm);(X,Y,Z)\in\mathcal H_\alpha\times L^2_{\mathbb F}([0,T])\times L^2_{\mathbb F}([0,T-];\mathbb R^m);(X,Y,Z)∈Hα​×LF2​([0,T])×LF2​([0,T−];Rm);

ξ∗=Y/(2η)\xi^*=Y/(2\eta)ξ∗=Y/(2η) is optimal, XXX is the optimal position, μt∗=E[Yt/(2ηt)∣Ft0]\mu^*_t=\mathbb E[Y_t/(2\eta_t)\mid\mathcal F^0_t]μt∗​=E[Yt​/(2ηt​)∣Ft0​] is the unique solution of the MFG (1.7), and

V(X;μ∗)=12A0X2+12B0X+12E[∫0TκsXs∗μs∗ds ∣ X].V(\mathcal X;\mu^*)=\tfrac12A_0\mathcal X^2+\tfrac12B_0\mathcal X+\tfrac12\mathbb E\Big[\int_0^T\kappa_sX^*_s\mu^*_sds\ \Big|\ \mathcal X\Big].V(X;μ∗)=21​A0​X2+21​B0​X+21​E[∫0T​κs​Xs∗​μs∗​ds ​ X].

Milestones

The milestones follow the paper's proof: Fact 2.2 on the weighted spaces; Lemma A.1, existence and uniqueness of AAA with the bounds (A.1), and A∈M−1A\in\mathcal M_{-1}A∈M−1​; the decay estimate (2.9), exp⁡(−∫rsAu/(2ηu)du)≤((T−s)/(T−r))α\exp(-\int_r^sA_u/(2\eta_u)du)\le((T-s)/(T-r))^\alphaexp(−∫rs​Au​/(2ηu​)du)≤((T−s)/(T−r))α; Lemma 2.5, an a priori estimate for the decoupled system (2.11) with homotopy parameter p∈[0,1]\mathfrak p\in[0,1]p∈[0,1]; Lemma 2.6, explicit unique solvability at p=0\mathfrak p=0p=0; Lemma 2.7, the continuation step p→p+d\mathfrak p\to\mathfrak p+\mathfrak dp→p+d; Proposition 2.8, unique solvability of (2.3) with (2.10) and a norm bound; the boundary limit (2.15); and Proposition 2.9, optimality, the equilibrium property and the value formula.

Significance

The theorem gives a complete equilibrium description for constrained liquidation with many players and stochastic, partially common market data: the equilibrium rate is the conditional expectation of the decoupled feedback rate given the common noise, and its value is explicit in terms of the Riccati solution. It is the basis of the paper's other two results, the O(N−1/2)O(N^{-1/2})O(N−1/2)-Nash property of the equilibrium in the NNN-player game (Theorem 3.3) and the approximation by penalized games (Theorem 4.6), which are separate missions in this series.

The result is proved in the paper; none of it is machine-checked. A formal development would contain the first formal treatment of BSDEs with singular terminal value and of a conditional (common-noise) mean-field FBSDE. Shorter proofs of individual steps, in particular of the a priori estimate and the continuation step, are welcome.

Difficulty

The obvious approach fails at the terminal time. Standard FBSDE theory requires a terminal condition for YYY; here only XT=0X_T=0XT​=0 is known, and YTY_TYT​ is undetermined. The decoupling coefficient AAA blows up like (T−t)−1(T-t)^{-1}(T−t)−1, so the driver of the equation for BBB is singular, and the classical monotonicity method of Hu–Peng and Peng–Wu, applied to (X,B)(X,B)(X,B) in unweighted spaces, does not close. The paper works instead with weighted norms that encode the rate at which XXX and BBB vanish at TTT, and runs the continuation on the triple (X,B,Y)(X,B,Y)(X,B,Y). The mean-field term is a conditional expectation given the common-noise filtration, not an expectation, so it remains random and has to be controlled pathwise in the weighted norms.

Formalization scope

Time is ℝ≥0; processes are real valued and W~\widetilde WW has m=k+1m=k+1m=k+1 coordinates, coordinate 000 being W0W^0W0. The Itô calculus is the published definition Peng1990.SMP.Stochastic (standard Brownian motion, LF2L^2_{\mathbb F}LF2​, Itô integrals, BSDEs in integrated form). The explicit choices:

  • Filtrations are augmented by the measurable null sets, and F\mathbb FF contains σ(X)\sigma(\mathcal X)σ(X).
  • κmax⁡,η⋆,λ⋆,∥η∥\kappa_{\max},\eta_\star,\lambda_\star,\|\eta\|κmax​,η⋆​,λ⋆​,∥η∥ are essential bounds over dt⊗dPdt\otimes d\mathbb Pdt⊗dP. Condition (2.4) is written without division, and "1/λ,1/η1/\lambda,1/\eta1/λ,1/η bounded" as positive essential lower bounds.
  • Assumption 2.3 is a hypothesis of every statement of §2, as the paper's standing assumption. Lemma A.1 (appendix) assumes only what §A assumes: λ,η\lambda,\etaλ,η progressive, nonnegative and bounded, and 1/η1/\eta1/η bounded.
  • Backward equations on [0,T)[0,T)[0,T) are imposed on every [0,τ][0,\tau][0,τ], τ<T\tau<Tτ<T. AT=∞A_T=\inftyAT​=∞ means At→+∞A_t\to+\inftyAt​→+∞ as t↑Tt\uparrow Tt↑T a.s.
  • Weighted norms are computed in [0,∞][0,\infty][0,∞], with the weight (T−t)−l(T-t)^{-l}(T−t)−l in ℝ≥0∞.
  • Every conditional expectation E[⋅∣Ft0]\mathbb E[\cdot\mid\mathcal F^0_t]E[⋅∣Ft0​] in an equation is evaluated through a progressive version, and its argument is required to be integrable.
  • The value is an essential infimum of conditional costs.
  • The relation Y=AX+BY=AX+BY=AX+B is part of the solution concept of (2.11): without it, YYY is determined only up to an additive F0\mathcal F_0F0​-measurable constant.
  • The constant of Proposition 2.8 is uniform over initial portfolios in an L2L^2L2 ball, for fixed coefficients.
  • Fact 2.2's product rule assumes paths of K1K_1K1​ continuous on [0,T)[0,T)[0,T), and its claim that KT=0K_T=0KT​=0 for K∈MlK\in\mathcal M_lK∈Ml​ is not stated. Both printed versions fail under the essential-supremum norm.

The interaction term must stay conditioned on Ft0\mathcal F^0_tFt0​: conditioning on Ft\mathcal F_tFt​ makes it Yt/(2ηt)Y_t/(2\eta_t)Yt​/(2ηt​) itself and collapses the game. The constraint XT=0X_T=0XT​=0 and the admissibility condition ∫0Tξ=X\int_0^T\xi=\mathcal X∫0T​ξ=X cannot be dropped either. The degenerate instance κ≡0\kappa\equiv0κ≡0 satisfies all hypotheses but decouples the game.

A complete development needs the following, all reusable beyond this mission: martingale representation for the augmented filtration F\mathbb FF; existence of progressive versions of conditional expectation processes; Doob's inequality on [0,τ][0,\tau][0,τ]; and linear BSDE solution formulas.

Selected references

  • G. Fu, P. Graewe, U. Horst, A. Popier, A Mean Field Game of Optimal Portfolio Liquidation, arXiv:1804.04911v3, 2021; Math. Oper. Res. 46(4), 2021. https://arxiv.org/abs/1804.04911
  • S. Ankirchner, M. Jeanblanc, T. Kruse, BSDEs with singular terminal condition and a control problem with constraints, SIAM J. Control Optim. 52(2), 2014. https://doi.org/10.1137/130913411
  • P. Graewe, U. Horst, E. Séré, Smooth solutions to portfolio liquidation problems under price-sensitive market impact, Stoch. Proc. Appl. 128(3), 2018. https://doi.org/10.1016/j.spa.2017.07.002
  • P. Cardaliaguet, C.-A. Lehalle, Mean field game of controls and an application to trade crowding, Math. Financ. Econ. 12, 2018. https://doi.org/10.1007/s11579-017-0206-z
  • R. Carmona, D. Lacker, A probabilistic weak formulation of mean field games and applications, Ann. Appl. Probab. 25(3), 2015. https://doi.org/10.1214/14-AAP1020
  • Y. Hu, S. Peng, Solution of forward-backward stochastic differential equations, Probab. Theory Related Fields 103, 1995. https://doi.org/10.1007/BF01204214
15 thms1 active userReviewed
AlgebraCombinatoricsComplexity Theory+1·Captain: mikedeng1

Promise Constraint Satisfaction: Algebraic Structure and a Symmetric Boolean Dichotomy 1: Folded Symmetric PCSPs Avoiding Parity, Majority and Alternating-Threshold Have Only C-Fixing PolymorphismsResearch Paper

Why promise constraint satisfaction

A constraint satisfaction problem (CSP) asks whether variables can be assigned values so that every constraint, drawn from a fixed finite set of relations, holds. The algebraic approach to CSPs explains their complexity through polymorphisms, the operations that preserve all constraint relations; this programme culminated in the CSP dichotomy theorem of Bulatov and Zhuk (2017). A promise CSP (PCSP) pairs each relation PPP with a weaker relation Q⊇PQ \supseteq PQ⊇P: given an instance that is promised to be satisfiable with the PPP-constraints, one must distinguish it from instances that are not even satisfiable with the QQQ-constraints. Approximate graph colouring (is a 3-colourable graph 100-colourable?) and (2+ε)(2+\varepsilon)(2+ε)-SAT are PCSPs, and their complexity is not captured by the classical theory.

Brakensiek and Guruswami (arXiv:1704.01937) developed the polymorphism theory of PCSPs and classified the Boolean, symmetric, folded case.

Timeline.

  • 1978: Schaefer classifies Boolean CSPs into polynomial-time and NP-complete.
  • 2014: Austrin, Guruswami and Håstad prove (2+ε)(2+\varepsilon)(2+ε)-SAT NP-hard with an argument based on polymorphisms (SIAM J. Comput. 46(5), 2017).
  • 2016–2018: Brakensiek and Guruswami introduce the general PCSP framework and prove a dichotomy for folded symmetric Boolean PCSPs (SODA 2018; arXiv:1704.01937v2, 2021; SIAM J. Comput. 50(6), 2021).
  • 2019–2021: Barto, Bulín, Krokhin and Opršal recast the theory in terms of minions (J. ACM 68(4), 2021). Ficak, Kozik, Olšák and Stankiewicz extend the Boolean symmetric dichotomy beyond the folded case (ICALP 2019).

Setting

Fix the Boolean domain {0,1}\{0,1\}{0,1}. A promise relation of arity kkk is a pair (P,Q)(P, Q)(P,Q) with P⊆Q⊆{0,1}kP \subseteq Q \subseteq \{0,1\}^kP⊆Q⊆{0,1}k, and a family Γ\GammaΓ is a finite set of promise relations, possibly of different arities. A function f:{0,1}L→{0,1}f : \{0,1\}^L \to \{0,1\}f:{0,1}L→{0,1} is a polymorphism of (P,Q)(P,Q)(P,Q) if, whenever x(1),…,x(L)∈Px^{(1)}, \dots, x^{(L)} \in Px(1),…,x(L)∈P, applying fff coordinate-wise gives a tuple in QQQ; Pol(Γ)\mathrm{Pol}(\Gamma)Pol(Γ) is the set of functions that are polymorphisms of every member of Γ\GammaΓ.

A relation is symmetric if it is closed under permuting coordinates. Every symmetric relation has the form Hamk(S)={x:∣x∣∈S}\mathrm{Ham}_k(S) = \{x : |x| \in S\}Hamk​(S)={x:∣x∣∈S}, where ∣x∣|x|∣x∣ is the Hamming weight. A function is folded if f(xˉ)=¬f(x)f(\bar x) = \neg f(x)f(xˉ)=¬f(x), and idempotent if f(0,…,0)=0f(0,\dots,0) = 0f(0,…,0)=0 and f(1,…,1)=1f(1,\dots,1) = 1f(1,…,1)=1; a family is folded (idempotent) if all its polymorphisms are. For odd LLL the paper singles out three function families:

ParL(x)=⨁i=1Lxi,MajL(x)=[∑ixi>L2],ATL(x)=[∑i=1L(−1)i−1xi>0],\mathrm{Par}_L(x) = \bigoplus_{i=1}^L x_i, \qquad \mathrm{Maj}_L(x) = \Big[\sum_{i} x_i > \tfrac L2\Big], \qquad \mathrm{AT}_L(x) = \Big[\sum_{i=1}^L (-1)^{i-1} x_i > 0\Big],ParL​(x)=i=1⨁L​xi​,MajL​(x)=[i∑​xi​>2L​],ATL​(x)=[i=1∑L​(−1)i−1xi​>0],

and their negations Par‾L,Maj‾L,AT‾L\overline{\mathrm{Par}}_L, \overline{\mathrm{Maj}}_L, \overline{\mathrm{AT}}_LParL​,Maj​L​,ATL​. Finally, fff is CCC-fixing if some set SSS of at most CCC coordinates satisfies f(x)=f(0,…,0)f(x) = f(0,\dots,0)f(x)=f(0,…,0) whenever xxx vanishes on SSS.

Formalization targets

Goal: Theorem 4.13

Let Γ\GammaΓ be a finite, folded, symmetric family. If there are odd L1,…,L6L_1, \dots, L_6L1​,…,L6​ with

ParL1, ATL2, MajL3, Par‾L4, AT‾L5, Maj‾L6∉Pol(Γ),\mathrm{Par}_{L_1},\ \mathrm{AT}_{L_2},\ \mathrm{Maj}_{L_3},\ \overline{\mathrm{Par}}_{L_4},\ \overline{\mathrm{AT}}_{L_5},\ \overline{\mathrm{Maj}}_{L_6} \notin \mathrm{Pol}(\Gamma),ParL1​​, ATL2​​, MajL3​​, ParL4​​, ATL5​​, Maj​L6​​∈/Pol(Γ),

then

∃ C(Γ)  ∀L  ∀f∈Pol(Γ)∩{0,1}{0,1}L: f is C(Γ)-fixing.\exists\, C(\Gamma)\ \ \forall L\ \ \forall f \in \mathrm{Pol}(\Gamma) \cap \{0,1\}^{\{0,1\}^L}:\ f \text{ is } C(\Gamma)\text{-fixing}.∃C(Γ)  ∀L  ∀f∈Pol(Γ)∩{0,1}{0,1}L: f is C(Γ)-fixing.

No value of CCC is fixed: the goal asserts only that one bound works for all arities.

Milestones

The milestones follow the paper's proof:

  • the tools of §2: Propositions 2.10, 2.12 and 2.15 and Lemma 2.13(1), which split polymorphisms into idempotent and negated idempotent ones;
  • the arity-reduction Claims 4.2, 4.3 and 4.4;
  • the closure computations Claim 4.6 (AT\mathrm{AT}AT) and Claim 4.8 (Maj\mathrm{Maj}Maj);
  • the relaxation Lemmas 4.5 and 4.7, which replace Γ\GammaΓ by a single canonical symmetric promise relation;
  • the additive-combinatorics Lemma 4.9 and its bounded Remark;
  • Lemma 4.10 and Corollary 4.11, which bound the coordinates iii with f(ei)=1f(e_i) = 1f(ei​)=1;
  • Lemma 4.12, the idempotent case of the goal.

Significance

Theorem 4.13 is the structural half of the paper's main dichotomy (Theorem 2.16): a folded symmetric Boolean PCSP is polynomial-time solvable if it has one of the six families as polymorphisms for every odd arity, and NP-hard otherwise. Hardness follows by feeding the CCC-fixing structure into a Label Cover reduction (Theorem 5.3). Bounded "fixing" or junta-like structure of all polymorphisms is the standard route from algebra to NP-hardness for PCSPs. This theorem is the cleanest Boolean instance of it, and it underlies later classifications of symmetric Boolean PCSPs.

The result has been proved and published since 2018. To our knowledge none of it has been formalized. A formalization supplies a checked Boolean polymorphism toolkit (Hamming-weight relations, folding, idempotence, relaxations), checked closure computations under alternating-threshold and majority operations, and a uniform-constant Frobenius-type lemma. All of these can be reused by other Boolean PCSP missions.

Difficulty

The obvious argument fixes a polymorphism fff and bounds its relevant coordinates directly from a constraint that Par\mathrm{Par}Par, AT\mathrm{AT}AT or Maj\mathrm{Maj}Maj violates. This gives a bound that depends on the arity LLL, and an LLL-dependent bound is trivial (C=LC = LC=L always works). The work is in making the constant uniform. The proof has to replace Γ\GammaΓ by a single canonical promise relation that does not depend on fff, classify exactly which symmetric relations exclude ATL\mathrm{AT}_LATL​ and MajL\mathrm{Maj}_LMajL​, and use an additive-combinatorics lemma whose constants depend only on that relation's arity. Its bounded version must hold with the same constants. The non-idempotent polymorphisms need a separate reduction through the negated family ¬Γ\neg\Gamma¬Γ.

Formalization scope

The domain {0,1}\{0,1\}{0,1} is Bool (false =0= 0=0). A family Γ\GammaΓ is a pair of relational structures 𝔸 𝔹 : RelStruct τ ar Bool from the published definition PCSPBLPAff_Symmetric_Setting, with [Fintype τ] (finitely many relations) and 𝔸.rel R ⊆ 𝔹.rel R (promise). IsPolymorphism 𝔸 𝔹 f from that file is Definition 2.4. Coordinates are Fin L, so the 1-based sign (−1)i−1(-1)^{i-1}(−1)i−1 of ATL\mathrm{AT}_LATL​ becomes (−1)i(-1)^{i}(−1)i. Anti-functions negate the output. Family properties (folded, idempotent, non-degenerate) quantify over polymorphisms of every arity L≥0L \ge 0L≥0. A folded or idempotent family has no nullary polymorphisms, so admitting L=0L = 0L=0 changes nothing. The constants C(Γ)C(\Gamma)C(Γ), c(Γ)c(\Gamma)c(Γ), A(n)A(n)A(n) and d(n)d(n)d(n) are quantified before the arity and the function (respectively before S0,S1S_0, S_1S0​,S1​). A statement that lets the constant depend on fff or LLL is trivially true and is not the goal.

Out of scope are the complexity conclusions: "PCSP(Γ\GammaΓ) is NP-hard" (Theorems 2.16 and 5.3) and item 2 of Lemma 2.13 (transfer of tractability). The cited inputs for those conclusions are also out of scope: the PCP theorem with parallel repetition (Proposition 5.2) and Schaefer's theorem. No complexity predicate appears in any statement.

A complete development needs the following, with Mathlib's Nat.frobeniusNumber as a starting point for Lemma 4.9:

  • explicit matrix constructions for Claims 4.6 and 4.8;
  • closure of polymorphisms under projections (minors), used in Lemma 4.10 and Corollary 4.11;
  • a Frobenius-coin argument with constants uniform in the sets S0,S1S_0, S_1S0​,S1​.

Contributions are welcome at any milestone, including separate proofs of the closure computations and of Lemma 4.9.

Selected references

  • J. Brakensiek, V. Guruswami, Promise Constraint Satisfaction: Algebraic Structure and a Symmetric Boolean Dichotomy, arXiv:1704.01937v2, 2021; SIAM J. Comput. 50(6), 2021. https://arxiv.org/abs/1704.01937
  • P. Austrin, V. Guruswami, J. Håstad, (2+ε)-SAT is NP-hard, SIAM J. Comput. 46(5), 2017. https://doi.org/10.1137/15M1006507
  • L. Barto, J. Bulín, A. Krokhin, J. Opršal, Algebraic approach to promise constraint satisfaction, J. ACM 68(4), 2021. https://doi.org/10.1145/3457606
  • M. Ficak, M. Kozik, M. Olšák, S. Stankiewicz, Dichotomy for symmetric Boolean PCSPs, ICALP 2019. https://doi.org/10.4230/LIPIcs.ICALP.2019.57
  • T. J. Schaefer, The complexity of satisfiability problems, STOC 1978. https://doi.org/10.1145/800133.804350
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Algorithmic Game TheoryControl TheoryOperations Research+2·Captain: mikedeng1

A Mean Field Game of Optimal Portfolio Liquidation 3: The Mean-Field Equilibrium Strategies Form an O(1/√N)-Nash Equilibrium of the N-Player Liquidation GameResearch Paper

Motivation

A trader who must sell a large position within a fixed horizon faces a trade-off: selling fast moves the price against her (temporary price impact), selling slowly exposes her to price risk. Since Almgren and Chriss, this optimal liquidation problem has been studied as a stochastic control problem with a terminal state constraint: the remaining position must be zero at the horizon TTT. When many traders liquidate at the same time, each trader's sales also depress the price that the others receive (permanent price impact), and the problem becomes a game.

Fu, Graewe, Horst and Popier (arXiv:1804.04911v3) study this game in the mean-field limit. Their §2 constructs a mean-field equilibrium through a singular conditional mean-field FBSDE. Their §3, the subject of this mission, justifies the limit: the strategies computed from the mean field game are an approximate Nash equilibrium of the finite game with NNN traders, with an error of order 1/N1/\sqrt N1/N​. Without such a result, the mean-field equilibrium describes a model nobody plays; with it, the equilibrium is a usable approximation for large but finite markets.

The approximation of NNN-player games by mean field games goes back to Huang, Malhamé and Caines (2006) and Lasry and Lions (2007); Carmona and Delarue (SIAM J. Control Optim. 51, 2013) proved an εN\varepsilon_NεN​-Nash property for a McKean–Vlasov class with state interaction and a rate N−1/(d+4)N^{-1/(d+4)}N−1/(d+4). The present game differs in three respects: players interact through their controls (the average trading rate), there is a common noise observed by all, and each player's state must reach zero at time TTT.

Setting

A single probability space carries a one-dimensional Brownian motion W0W^0W0 (the common noise, which drives the benchmark price and is observed by every player), for each player iii a kkk-dimensional Brownian motion WiW^iWi (the private noise), and i.i.d. initial portfolios Xi\mathcal X^iXi with law ν\nuν; all of these are mutually independent. Player iii observes Fi\mathbb F^iFi, Fti=σ(Xi,Ws0,Wsi, s≤t)\mathcal F^i_t=\sigma(\mathcal X^i,W^0_s,W^i_s,\ s\le t)Fti​=σ(Xi,Ws0​,Wsi​, s≤t), and chooses a trading rate ξi\xi^iξi; her position is Xti=Xi−∫0tξsi dsX^i_t=\mathcal X^i-\int_0^t\xi^i_s\,dsXti​=Xi−∫0t​ξsi​ds and must satisfy XTi=0X^i_T=0XTi​=0. Given the profile ξ⃗=(ξ1,…,ξN)\vec\xi=(\xi^1,\dots,\xi^N)ξ​=(ξ1,…,ξN), her conditional cost is

JN,i(ξ⃗)=E[∫0T(κtiN∑j=1NξtjXti+ηti(ξti)2+λti(Xti)2)dt ∣ Xi],J^{N,i}(\vec\xi)=\mathbb E\Big[\int_0^T\Big(\frac{\kappa^i_t}{N}\sum_{j=1}^N\xi^j_tX^i_t+\eta^i_t(\xi^i_t)^2+\lambda^i_t(X^i_t)^2\Big)dt\ \Big|\ \mathcal X^i\Big],JN,i(ξ​)=E[∫0T​(Nκti​​j=1∑N​ξtj​Xti​+ηti​(ξti​)2+λti​(Xti​)2)dt ​ Xi],

where κi\kappa^iκi (permanent impact), ηi\eta^iηi (temporary impact) and λi\lambda^iλi (risk aversion) are nonnegative bounded processes. Under Assumption 3.1 they are the same deterministic measurable functionals κ,η,λ\kappa,\eta,\lambdaκ,η,λ of (t,Xi,W⋅∧ti,W⋅∧t0)(t,\mathcal X^i,W^i_{\cdot\wedge t},W^0_{\cdot\wedge t})(t,Xi,W⋅∧ti​,W⋅∧t0​) for every player, so the players are statistically identical.

In the mean field game, the average 1N∑jξj\frac1N\sum_j\xi^jN1​∑j​ξj is replaced by a process μ\muμ adapted to the common-noise filtration F0\mathbb F^0F0, and an equilibrium is a μ∗\mu^*μ∗ with μt∗=E[ξt∗∣Ft0]\mu^*_t=\mathbb E[\xi^*_t\mid\mathcal F^0_t]μt∗​=E[ξt∗​∣Ft0​] for the representative player's best response ξ∗\xi^*ξ∗. The paper characterizes it through the FBSDE (2.3),

dXt=−Yt2ηtdt,−dYt=(κt E[Yt2ηt∣Ft0]+2λtXt)dt−Zt dW~t,X0=X, XT=0,dX_t=-\frac{Y_t}{2\eta_t}dt,\qquad -dY_t=\Big(\kappa_t\,\mathbb E\Big[\frac{Y_t}{2\eta_t}\Big|\mathcal F^0_t\Big]+2\lambda_tX_t\Big)dt-Z_t\,d\widetilde W_t,\qquad X_0=\mathcal X,\ X_T=0,dXt​=−2ηt​Yt​​dt,−dYt​=(κt​E[2ηt​Yt​​​Ft0​]+2λt​Xt​)dt−Zt​dWt​,X0​=X, XT​=0,

with W~=(W0,W)\widetilde W=(W^0,W)W=(W0,W); the optimal rate is ξ∗=Y/(2η)\xi^*=Y/(2\eta)ξ∗=Y/(2η). Player iii's mean-field strategy ξ∗,i=Yi/(2ηi)\xi^{*,i}=Y^i/(2\eta^i)ξ∗,i=Yi/(2ηi) comes from the same FBSDE with her own data.

Formalization targets

Goal: Theorem 3.3

For a positive function MMM with ψ≤M\psi\le Mψ≤M, where ψ(Xi)=E[∫0T∣ξt∗,i∣2dt∣Xi]\psi(\mathcal X^i)=\mathbb E[\int_0^T|\xi^{*,i}_t|^2dt\mid\mathcal X^i]ψ(Xi)=E[∫0T​∣ξt∗,i​∣2dt∣Xi], and admissible sets Ai={ξ∈AFi(Xi):E[∫0T∣ξt∣2dt∣Xi]≤M(Xi)}\mathcal A^i=\{\xi\in\mathcal A_{\mathbb F^i}(\mathcal X^i):\mathbb E[\int_0^T|\xi_t|^2dt\mid\mathcal X^i]\le M(\mathcal X^i)\}Ai={ξ∈AFi​(Xi):E[∫0T​∣ξt​∣2dt∣Xi]≤M(Xi)}, there is a function ggg, independent of iii and NNN, with

JN,i(ξ⃗∗)≤JN,i(ξi,ξ∗,−i)+g(Xi)Nfor all N≥1, 1≤i≤N, ξi∈Ai.J^{N,i}(\vec\xi^*)\le J^{N,i}(\xi^i,\xi^{*,-i})+\frac{g(\mathcal X^i)}{\sqrt N}\qquad\text{for all }N\ge1,\ 1\le i\le N,\ \xi^i\in\mathcal A^i .JN,i(ξ​∗)≤JN,i(ξi,ξ∗,−i)+N​g(Xi)​for all N≥1, 1≤i≤N, ξi∈Ai.

The goal asserts only the shape of the bound, not its constant.

Milestones

  1. Lemma 3.2: one measurable map Φ\PhiΦ gives (Xi,Yi,∫0⋅Zi)=Φ(Xi,Wi,W0)(X^i,Y^i,\int_0^\cdot Z^i)=\Phi(\mathcal X^i,W^i,W^0)(Xi,Yi,∫0⋅​Zi)=Φ(Xi,Wi,W0) for every player, and ξ∗,i=ϕ(Xi,W0,Wi)\xi^{*,i}=\phi(\mathcal X^i,W^0,W^i)ξ∗,i=ϕ(Xi,W0,Wi) (3.1).
  2. (3.2): a single μ∗\mu^*μ∗ with μt∗=E[ξt∗,i∣Ft0]\mu^*_t=\mathbb E[\xi^{*,i}_t\mid\mathcal F^0_t]μt∗​=E[ξt∗,i​∣Ft0​] for every iii.
  3. (3.3): E∫0T∣ξt∗,i∣2dt≤C\mathbb E\int_0^T|\xi^{*,i}_t|^2dt\le CE∫0T​∣ξt∗,i​∣2dt≤C uniformly in iii.
  4. (3.5): E[∫0T(μt∗−1N∑jξt∗,j)2dt∣Xi]≤2(M(Xi)+(2N−1)C)/N2\mathbb E[\int_0^T(\mu^*_t-\frac1N\sum_j\xi^{*,j}_t)^2dt\mid\mathcal X^i]\le 2(M(\mathcal X^i)+(2N-1)C)/N^2E[∫0T​(μt∗​−N1​∑j​ξt∗,j​)2dt∣Xi]≤2(M(Xi)+(2N−1)C)/N2.
  5. The bounds on I1I_1I1​ and I2I_2I2​ (p. 24): the two differences of conditional costs into which the proof splits JN,i(ξ,ξ∗,−i)−JN,i(ξ⃗∗)J^{N,i}(\xi,\xi^{*,-i})-J^{N,i}(\vec\xi^*)JN,i(ξ,ξ∗,−i)−JN,i(ξ​∗) are O(1/N)O(1/\sqrt N)O(1/N​).

Significance

The result turns the mean-field equilibrium of §2 into a statement about the finite market: when all NNN traders use their mean-field strategies, a trader who deviates can save at most g(Xi)/Ng(\mathcal X^i)/\sqrt Ng(Xi)/N​ in conditional expected cost. The error bound depends on the trader's own initial position only through M(Xi)M(\mathcal X^i)M(Xi), and the rate 1/N1/\sqrt N1/N​ is dimension-free, in contrast with the N−1/(d+4)N^{-1/(d+4)}N−1/(d+4) rates of state-interaction games, because the interaction runs through the empirical mean of the controls rather than through an empirical measure.

The paper's proof of Theorem 3.3 is short but rests on several facts it states without proof: the Yamada–Watanabe-type Lemma 3.2 (whose proof is referred to other papers), the identification (3.2) of a common conditional mean, and the moment bound (3.3) attributed to Proposition 2.8. This mission makes each of these a separate machine-checkable statement. As far as we know, none of these results, nor any optimal-liquidation mean field game, has a machine-checked proof.

Difficulty

The estimate (3.5) is a law-of-large-numbers bound for the average of NNN processes that are not independent: all of them depend on the common noise W0W^0W0. The obvious argument, expanding the square and using independence, fails as stated; the cross terms vanish only conditionally on W0W^0W0, and only once one knows that every ξ∗,j\xi^{*,j}ξ∗,j is the same measurable functional of (Xj,W0,Wj)(\mathcal X^j,W^0,W^j)(Xj,W0,Wj). That is Lemma 3.2, a Yamada–Watanabe-type statement for a singular FBSDE with a conditional mean-field term, which needs strong uniqueness of the FBSDE in the class Hα×L2×L2([0,T−])\mathcal H_\alpha\times L^2\times L^2([0,T-])Hα​×L2×L2([0,T−]) and is the main technical step. The terminal constraint XT=0X_T=0XT​=0 makes the backward component singular at TTT (YYY blows up like X/(T−t)X/(T-t)X/(T−t)), so standard Lipschitz FBSDE theory does not apply. Finally, the deviation ξ\xiξ is constrained only through a conditional second-moment bound MMM, and the comparison with the mean-field cost uses the optimality of ξ∗,i\xi^{*,i}ξ∗,i (Proposition 2.9) against μ∗\mu^*μ∗.

Formalization scope

Everything is stated on one probability space carrying all players, with players indexed by N\mathbb NN; the NNN-player game uses players i<Ni<Ni<N (the paper's 1,…,N1,\dots,N1,…,N, shifted by one). Time is R≥0\mathbb R_{\ge0}R≥0​ and the processes are real valued. Choices made explicit:

  • Assumption 2.3 for every player is a hypothesis of every theorem: the paper states it "throughout" (p. 8), and the proof of Theorem 3.3 uses Propositions 2.8 and 2.9, which need it. Its constants κmax⁡,η⋆,λ⋆,∥η∥\kappa_{\max},\eta_\star,\lambda_\star,\|\eta\|κmax​,η⋆​,λ⋆​,∥η∥ are essential bounds over [0,T]×Ω[0,T]\times\Omega[0,T]×Ω; "1/λ,1/η∈L∞1/\lambda,1/\eta\in L^\infty1/λ,1/η∈L∞" is a positive essential lower bound.
  • The equilibrium processes (Xi,Yi,Zi)(X^i,Y^i,Z^i)(Xi,Yi,Zi) are hypotheses: solutions of (2.3) for player iii's data in the class of Theorem 2.4. ξ∗,i\xi^{*,i}ξ∗,i is defined as Yi/(2ηi)Y^i/(2\eta^i)Yi/(2ηi), never through ϕ\phiϕ.
  • Conditioning on Xi=xi\mathcal X^i=x^iXi=xi is conditioning on σ(Xi)\sigma(\mathcal X^i)σ(Xi); every conclusion holds almost surely, i.e. for ν\nuν-a.e. xix^ixi. "ψ≤M\psi\le Mψ≤M" is the a.s. inequality of conditional second moments, and MMM is assumed measurable.
  • ggg is quantified before NNN and iii. A statement in which ggg may depend on NNN is trivially true and is ruled out.
  • Filtrations are augmented by null sets. Each conditional expectation E[ ⋅∣Ft0]\mathbb E[\,\cdot\mid\mathcal F^0_t]E[⋅∣Ft0​] is evaluated through a progressive version of an integrable argument. BSDEs on [0,T)[0,T)[0,T) are imposed on every [0,τ][0,\tau][0,τ], τ<T\tau<Tτ<T.
  • Lemma 3.2's path spaces carry the product σ-algebra; its identities hold for each ttt almost surely.
  • The paper's bound on I2I_2I2​ is stated for ∣I2∣|I_2|∣I2​∣, which is what its Cauchy–Schwarz step gives and what the proof needs.

The development reuses the Itô-calculus definitions of Peng1990.SMP.Stochastic (standard Brownian motion, LF2L^2_{\mathbb F}LF2​, Itô integrals, BSDEs). Contributions useful beyond this mission: conditional independence given a common noise for functionals of independent inputs, a Yamada–Watanabe argument for FBSDEs, and conditional Cauchy–Schwarz bounds for time integrals. Proofs of any milestone, and of the facts from §2 they rely on, are welcome.

Selected references

  • G. Fu, P. Graewe, U. Horst, A. Popier, A Mean Field Game of Optimal Portfolio Liquidation, arXiv:1804.04911v3, 2021; Math. Oper. Res. 46(4), 2021. https://arxiv.org/abs/1804.04911
  • R. Almgren, N. Chriss, Optimal execution of portfolio transactions, J. Risk 3(2), 2001. https://doi.org/10.21314/JOR.2001.041
  • M. Huang, R. P. Malhamé, P. E. Caines, Large population stochastic dynamic games: closed-loop McKean–Vlasov systems and the Nash certainty equivalence principle, Commun. Inf. Syst. 6(3), 2006. https://doi.org/10.4310/CIS.2006.v6.n3.a5
  • J.-M. Lasry, P.-L. Lions, Mean field games, Jpn. J. Math. 2, 2007. https://doi.org/10.1007/s11537-007-0657-8
  • R. Carmona, F. Delarue, Probabilistic analysis of mean-field games, SIAM J. Control Optim. 51(4), 2013. https://doi.org/10.1137/120883499
  • S. Peng, A general stochastic maximum principle for optimal control problems, SIAM J. Control Optim. 28(4), 1990. https://doi.org/10.1137/0328054
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Algorithmic Game TheoryOperations ResearchOptimization·Captain: mikedeng1

Supplier Centrality and Auditing Priority in Socially Responsible Supply Chains I: Under Downstream Competition No Buyer Audits the Common Supplier in Any EquilibriumResearch Paper

Motivation

Brands are routinely held responsible for the labour and environmental practices of their suppliers. A brand that is linked in public to a non-compliant supplier loses consumer willingness to pay, and firms answer this risk by auditing their suppliers. Supply networks are not trees, however: one supplier often serves several competing brands. Chen, Qi and Dawande (SSRN 2889889, Manufacturing & Service Operations Management, 2020) ask how the position of a supplier in such a network, and in particular its centrality (the number of buyers it serves), affects which suppliers get audited when buyers decide on their own, and when they audit jointly.

This mission formalizes the paper's answer for unilateral auditing by competing buyers (Sec. 4.2, Proposition 2). A companion mission treats joint auditing (Proposition 3).

Setting

Two buyers B1,B2B_1, B_2B1​,B2​ source from three suppliers: an independent supplier SiS_iSi​ for each buyer BiB_iBi​, and a common supplier ScS_cSc​ that serves both. Each supplier complies with social-responsibility standards with probability e∈(0,1)e \in (0,1)e∈(0,1). In stage 1, buyer BiB_iBi​ chooses an auditing effort eii∈[0,1]e_{ii} \in [0,1]eii​∈[0,1] on SiS_iSi​ and eic∈[0,1]e_{ic} \in [0,1]eic​∈[0,1] on ScS_cSc​, and audits at most one of them: eii eic=0e_{ii}\,e_{ic} = 0eii​eic​=0. Auditing a supplier with effort x>0x > 0x>0 costs K+a2x2K + \tfrac a2 x^2K+2a​x2, with a fixed cost K≥0K \ge 0K≥0 and a>0a > 0a>0; effort 000 means no audit and costs nothing.

A non-compliant supplier that passes the audits is discovered in public with probability r∈(0,1]r \in (0,1]r∈(0,1]. Hence SiS_iSi​ causes damage to BiB_iBi​ with probability λI(eii)=r(1−e)(1−eii)\lambda_I(e_{ii}) = r(1-e)(1-e_{ii})λI​(eii​)=r(1−e)(1−eii​), and ScS_cSc​ causes damage to both buyers with probability λC(e1c,e2c)=r(1−e)(1−e1c)(1−e2c)\lambda_C(e_{1c},e_{2c}) = r(1-e)(1-e_{1c})(1-e_{2c})λC​(e1c​,e2c​)=r(1−e)(1−e1c​)(1−e2c​), independently. A buyer with at least one exposed supplier suffers the MWTP damage dM>0d_M > 0dM​>0: his demand intercept drops from α\alphaα to α−dM\alpha - d_Mα−dM​. Each exposed supplier is then paid w^≥w\hat w \ge ww^≥w per unit instead of www, so a buyer with n∈{0,1,2}n \in \{0,1,2\}n∈{0,1,2} exposed suppliers has unit cost (2−n)w+nw^(2-n)w + n\hat w(2−n)w+nw^.

In stage 2 the buyers compete in quantities with inverse demands pi=Ai−qi−βqi′p_i = A_i - q_i - \beta q_{i'}pi​=Ai​−qi​−βqi′​, β∈(0,1]\beta \in (0,1]β∈(0,1] (Dixit 1979; Singh and Vives 1984). Its equilibrium profit for B1B_1B1​ is π1b(n1,n2)=q1∗(n1,n2)2\pi^b_1(n_1,n_2) = q^*_1(n_1,n_2)^2π1b​(n1​,n2​)=q1∗​(n1​,n2​)2, in closed form (Lemma 1). Buyer B1B_1B1​'s ex ante expected profit Π1b(e11,e1c;e22,e2c)\Pi^b_1(e_{11},e_{1c};e_{22},e_{2c})Π1b​(e11​,e1c​;e22​,e2c​) is the expectation of π1b\pi^b_1π1b​ over the eight damage outcomes, minus his audit costs; Π2b\Pi^b_2Π2b​ is symmetric. Three conditions on (α,β,w,w^,dM)(\alpha,\beta,w,\hat w,d_M)(α,β,w,w^,dM​) (p. 8) make all stage-2 quantities positive.

An equilibrium is a profile (s1,s2)(s_1,s_2)(s1​,s2​), si=(eii,eic)s_i = (e_{ii},e_{ic})si​=(eii​,eic​), in which each buyer's strategy is a best response to the other's, with the tie-breaking rule of p. 10: a buyer who is indifferent between auditing and not auditing does not audit. Two explicit efforts, eI∗e^*_IeI∗​ (eq. (1)) and e^I\hat e_Ie^I​ (eq. (2)), are rational functions of the parameters; e^I\hat e_Ie^I​ is a buyer's optimal effort on his independent supplier when the rival audits nobody, and eI∗e^*_IeI∗​ is the symmetric solution when both audit their independent suppliers.

Formalization targets

Goal: Proposition 2

Assume β∈(0,1]\beta \in (0,1]β∈(0,1] and e^I<1\hat e_I < 1e^I​<1. There exist KuL<KuM<KuHK^L_u < K^M_u < K^H_uKuL​<KuM​<KuH​ such that for every K≥0K \ge 0K≥0, writing A=((eI∗,0),(eI∗,0))A = ((e^*_I,0),(e^*_I,0))A=((eI∗​,0),(eI∗​,0)), B1=((e^I,0),(0,0))B_1 = ((\hat e_I,0),(0,0))B1​=((e^I​,0),(0,0)), B2=((0,0),(e^I,0))B_2 = ((0,0),(\hat e_I,0))B2​=((0,0),(e^I​,0)), N=((0,0),(0,0))N = ((0,0),(0,0))N=((0,0),(0,0)),

EqSet(K)={{A}K<KuL,{A,B1,B2}KuL≤K<KuM,{B1,B2}KuM≤K<KuH,{N}K≥KuH.\mathrm{EqSet}(K) = \begin{cases} \{A\} & K < K^L_u,\\ \{A, B_1, B_2\} & K^L_u \le K < K^M_u,\\ \{B_1, B_2\} & K^M_u \le K < K^H_u,\\ \{N\} & K \ge K^H_u. \end{cases}EqSet(K)=⎩⎨⎧​{A}{A,B1​,B2​}{B1​,B2​}{N}​K<KuL​,KuL​≤K<KuM​,KuM​≤K<KuH​,K≥KuH​.​

In every equilibrium the common supplier receives zero effort.

Milestones

Lemma 1 (stage-2 equilibrium), the OA.2 expected-profit display, the best-response function (OA-9) with eI∗e^*_IeI∗​ and e^I\hat e_Ie^I​ as its values, the dominance inequality (OA-11), Lemmas OA5 and OA6 (the two kinds of auditing equilibria and their threshold ranges), the monotonicity facts (OA-14)–(OA-15), Lemma OA7 (the order of the thresholds) and Lemma OA8 (no equilibrium audits ScS_cSc​). The thresholds of the milestones are the explicit ones the proof defines in (OA-10), (OA-12), (OA-13).

Significance

The result separates network position from competition. Without downstream competition (β=0\beta = 0β=0, Proposition 1) there is a Pareto-dominant equilibrium in which one buyer audits the common supplier. With competition, Proposition 2 shows that the common supplier, the most central and therefore the most consequential source of risk, is never audited: auditing it would also protect the rival, who free-rides. This inefficiency is what motivates the paper's analysis of joint auditing (Proposition 3) and of social welfare (Proposition 4).

The result is proved in the paper, partly by omission: the e-companion leaves the proof of Lemma OA8 and the case K≥KuHK \ge K^H_uK≥KuH​ to the reader. No machine-checked version exists. A formal proof would give a complete case analysis of a two-stage game with a discontinuous fixed cost, a constrained strategy set and a tie-breaking rule, and would check the paper's closed forms, several of which are printed with small slips.

Difficulty

The first-order conditions alone do not determine the equilibria. The fixed cost makes each buyer's payoff discontinuous at zero effort, so every candidate must be compared with no audit, and the best response is a choice among three regimes (audit SiS_iSi​, audit ScS_cSc​, audit nobody). Uniqueness claims therefore require excluding every profile in the constrained strategy set, including those where a buyer audits the common supplier, for which the paper gives no proof. The threshold comparisons KuL<KuM<KuHK^L_u < K^M_u < K^H_uKuL​<KuM​<KuH​ rest on monotonicity in the rival's effort, and the expected profit is multilinear in the four efforts (plus the quadratic audit costs), with coefficients that are differences of squared Cournot quantities whose signs depend on the p. 8 conditions.

Formalization scope

All objects live in the namespace SupplierAudit.Competition. The source is the authors' accepted manuscript on SSRN (2889889); main-text printed pages equal PDF pages, and e-companion page ec kkk is PDF page 28+k28 + k28+k.

  • Parameters. A structure Params carries α,β,w,w^,dM,e,r,a\alpha, \beta, w, \hat w, d_M, e, r, aα,β,w,w^,dM​,e,r,a and the standing assumptions β∈[0,1]\beta \in [0,1]β∈[0,1], w≤w^w \le \hat ww≤w^, dM>0d_M > 0dM​>0, e∈(0,1)e \in (0,1)e∈(0,1), r∈(0,1]r \in (0,1]r∈(0,1], a>0a > 0a>0 and the three conditions of p. 8. The theorems add β>0\beta > 0β>0 (competition, Sec. 4.2). KKK is a separate real argument and the goal quantifies over K≥0K \ge 0K≥0.
  • Stage 2. The general linear differentiated Cournot duopoly is its own definition (CournotDuopoly). The model's stage-2 profit is the closed form q1∗(n1,n2)2q^*_1(n_1,n_2)^2q1∗​(n1​,n2​)2 for all (n1,n2)(n_1,n_2)(n1​,n2​); Lemma 1 states that it is the game's unique equilibrium.
  • Expected profit. Π1b\Pi^b_1Π1b​ is the eight-outcome expectation; Π2b\Pi^b_2Π2b​ is Π1b\Pi^b_1Π1b​ with the roles exchanged. The grouped display of OA.2 is a milestone.
  • Strategies and equilibrium. Strategies are pairs in [0,1]2[0,1]^2[0,1]2 with product zero. Equilibria include the strict-improvement tie-breaking rule of p. 10; without it the goal is false at K=KuMK = K^M_uK=KuM​ and K=KuHK = K^H_uK=KuH​.
  • Interior efforts. The paper assumes equilibrium efforts lie in (0,1)(0,1)(0,1) (p. 10; sufficient conditions in OA.1 are not given in closed form). This is encoded as the single hypothesis e^I<1\hat e_I < 1e^I​<1 on the explicit formula (2), never as a hypothesis on an unknown equilibrium variable.
  • Thresholds. The goal states the thresholds existentially, as printed, with their order as part of the conclusion; the milestones use the explicit (OA-10), (OA-12), (OA-13). eI∗e^*_IeI∗​, e^I\hat e_Ie^I​ and e11∗(⋅)e^*_{11}(\cdot)e11∗​(⋅) are the printed formulas, not argmaxes.
  • Printed slips, corrected. In (OA-11) the second prefactor should be β(w^−w)\beta(\hat w - w)β(w^−w); only the strict inequality is stated. The printed derivative of e11∗e^*_{11}e11∗​ in the proof of Lemma OA7 lacks a factor 1/a1/a1/a; only monotonicity is stated.

A formalization in which equilibrium is plain Nash, efforts range over all of R\mathbb RR, a buyer may audit both suppliers, or "interior" is a hypothesis on the equilibrium efforts themselves would state a different (and in places false or vacuous) theorem; these are ruled out by the definitions above. Proofs of any milestone are welcome, as is reusable infrastructure for linear Cournot duopolies and for finite expectations over independent Bernoulli events.

Selected references

  • F. Chen, A. Qi, M. Dawande, Supplier Centrality and Auditing Priority in Socially-Responsible Supply Chains, Manufacturing & Service Operations Management, 2020 (accepted manuscript). https://ssrn.com/abstract=2889889
  • A. Dixit, A Model of Duopoly Suggesting a Theory of Entry Barriers, Bell Journal of Economics 10(1), 1979. https://doi.org/10.2307/3003317
  • N. Singh, X. Vives, Price and Quantity Competition in a Differentiated Duopoly, RAND Journal of Economics 15(4), 1984. https://doi.org/10.2307/2555525
  • E. L. Plambeck, T. A. Taylor, Supplier Evasion of a Buyer's Audit: Implications for Motivating Supplier Social and Environmental Responsibility, Manufacturing & Service Operations Management 18(2), 2016. https://doi.org/10.1287/msom.2015.0550
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Partial Differential EquationsProbabilityStochastic Systems·Captain: mikedeng1

On Viscosity Solutions of Path Dependent PDEs: Comparison Principle for Viscosity Sub- and Supersolutions of Semilinear PPDEs, and u^0 from the BSDE Is the Unique Viscosity SolutionResearch Paper

Motivation

Many quantities in stochastic control, mathematical finance and stochastic differential games depend on the whole past of a Brownian path rather than on its current position: the price of an Asian or lookback option, the value of a control problem with delay, the solution of a non-Markovian backward stochastic differential equation (BSDE). For Markovian problems the value is a function v(t,x)v(t,x)v(t,x) and solves a parabolic PDE, and the theory of viscosity solutions (Crandall, Ishii and Lions) gives existence, uniqueness and stability without any smoothness. For path-dependent problems the value is a functional u(t,ω)u(t,\omega)u(t,ω) of the path, and the corresponding equation is a path-dependent PDE (PPDE), written with the horizontal and vertical derivatives introduced by Dupire (SSRN 1435551) and developed into a functional Itô calculus by Cont and Fournié (arXiv:1002.2446). Classical solutions of PPDEs rarely exist, so a weak notion is needed.

Timeline:

  • 1990. Pardoux and Peng prove well-posedness of BSDEs with Lipschitz generator (doi:10.1016/0167-6911(90)90082-6); the BSDE value is the natural candidate solution of a semilinear PPDE.
  • 2009–2013. Dupire, and Cont and Fournié, define pathwise derivatives and prove a functional Itô formula; Peng asks for a viscosity theory of PPDEs (ICM 2010).
  • 2011–2014. Ekren, Keller, Touzi and Zhang (arXiv:1109.5971, Ann. Probab. 42 (2014) 204–236) define viscosity solutions of semilinear PPDEs through an optimal stopping problem under a nonlinear expectation and prove existence, stability, comparison and uniqueness. Fully nonlinear PPDEs follow in Ekren, Touzi and Zhang (arXiv:1210.0006).

Setting

Fix d≥1d \ge 1d≥1 and T>0T>0T>0. Let Ω\OmegaΩ be the space of continuous paths ω:[0,T]→Rd\omega:[0,T]\to\mathbb R^dω:[0,T]→Rd with ω0=0\omega_0 = 0ω0​=0, BBB the canonical process, F\mathbb FF the filtration it generates, P0P_0P0​ the Wiener measure and Λ=[0,T]×Ω\Lambda = [0,T]\times\OmegaΛ=[0,T]×Ω. On Λ\LambdaΛ the pseudometric is d∞((t,ω),(t′,ω′))=∣t−t′∣+sup⁡s≤T∣ωt∧s−ωt′∧s′∣d_\infty((t,\omega),(t',\omega')) = |t-t'| + \sup_{s\le T}|\omega_{t\wedge s}-\omega'_{t'\wedge s}|d∞​((t,ω),(t′,ω′))=∣t−t′∣+sups≤T​∣ωt∧s​−ωt′∧s′​∣. For t≤Tt\le Tt≤T, Ωt\Omega^tΩt is the space of continuous paths on [t,T][t,T][t,T] vanishing at ttt, with Wiener measure P0tP^t_0P0t​, and Ω^t\hat\Omega^tΩ^t the space of càdlàg paths on [t,T][t,T][t,T]. The concatenation ω⊗tω′\omega\otimes_t\omega'ω⊗t​ω′ follows ω\omegaω up to ttt and then ωt+ω′\omega_t + \omega'ωt​+ω′, and ut,ω(s,ω′)=u(s,ω⊗tω′)u^{t,\omega}(s,\omega') = u(s,\omega\otimes_t\omega')ut,ω(s,ω′)=u(s,ω⊗t​ω′).

A functional u^\hat uu^ on [t,T]×Ω^t[t,T]\times\hat\Omega^t[t,T]×Ω^t has the Dupire derivatives ∂ωu^\partial_\omega\hat u∂ω​u^, the derivative under a bump h1[s,T]eih\mathbf 1_{[s,T]}e_ih1[s,T]​ei​ of the path, and ∂tu^\partial_t\hat u∂t​u^, the right derivative in time along the stopped path. Cb1,2(Λt)C^{1,2}_b(\Lambda^t)Cb1,2​(Λt) is the class of functionals that agree on continuous paths with some u^\hat uu^ whose derivatives ∂tu^\partial_t\hat u∂t​u^, ∂ωu^\partial_\omega\hat u∂ω​u^, ∂ωω2u^\partial^2_{\omega\omega}\hat u∂ωω2​u^ exist and are bounded and d∞d_\inftyd∞​-continuous.

The equation is the semilinear PPDE

(Lu)(t,ω):=−∂tu−12tr⁡(∂ωω2u)−f(t,ω,u,∂ωu)=0,0≤t<T.(\mathcal L u)(t,\omega) := -\partial_t u - \tfrac12\operatorname{tr}\big(\partial^2_{\omega\omega}u\big) - f\big(t,\omega,u,\partial_\omega u\big) = 0,\qquad 0\le t<T.(Lu)(t,ω):=−∂t​u−21​tr(∂ωω2​u)−f(t,ω,u,∂ω​u)=0,0≤t<T.

For L≥0L\ge0L≥0, E‾tL\underline{\mathcal E}^L_tE​tL​ and E‾tL\overline{\mathcal E}^L_tEtL​ are the infimum and supremum of expectations under the Girsanov measures Pt,βP^{t,\beta}Pt,β, ∣βi∣≤L|\beta^i|\le L∣βi∣≤L. A bounded d∞d_\inftyd∞​-continuous uuu is a viscosity LLL-subsolution if (Lt,ωφ)(t,0)≤0(\mathcal L^{t,\omega}\varphi)(t,\mathbf 0)\le0(Lt,ωφ)(t,0)≤0 at every (t,ω)(t,\omega)(t,ω) with t<Tt<Tt<T for every test function φ∈Cb1,2(Λt)\varphi\in C^{1,2}_b(\Lambda^t)φ∈Cb1,2​(Λt) that touches ut,ωu^{t,\omega}ut,ω from above in the sense

0=φ(t,0)−u(t,ω)=min⁡τ~∈TtE‾tL[(φ−ut,ω)τ~∧τ]for some τ∈T+t,0 = \varphi(t,\mathbf 0)-u(t,\omega) = \min_{\tilde\tau\in\mathcal T^t}\underline{\mathcal E}^L_t\big[(\varphi-u^{t,\omega})_{\tilde\tau\wedge\tau}\big]\quad\text{for some }\tau\in\mathcal T^t_+ ,0=φ(t,0)−u(t,ω)=τ~∈Ttmin​E​tL​[(φ−ut,ω)τ~∧τ​]for some τ∈T+t​,

where Tt\mathcal T^tTt is a class of stopping times with open level sets. Supersolutions use max⁡\maxmax and E‾tL\overline{\mathcal E}^L_tEtL​. A viscosity subsolution is an LLL-subsolution for some LLL, the same LLL at every point. The candidate solution is u0(t,ω)=Yt0,t,ωu^0(t,\omega) = Y^{0,t,\omega}_tu0(t,ω)=Yt0,t,ω​, where Y0,t,ωY^{0,t,\omega}Y0,t,ω solves the BSDE with terminal value gt,ωg^{t,\omega}gt,ω and generator ft,ωf^{t,\omega}ft,ω under P0tP^t_0P0t​.

Formalization targets

Goal: Theorem 4.6

Under Assumption 4.2 (fff bounded, progressively measurable, continuous in ttt, uniformly continuous in ω\omegaω, Lipschitz in (y,z)(y,z)(y,z); ggg bounded and uniformly continuous) and Assumption 4.4 (an extension f^\hat ff^​ of fff to càdlàg paths, continuous and Lipschitz), for every viscosity subsolution u1u^1u1 and supersolution u2u^2u2,

u1(T,⋅)≤g≤u2(T,⋅) ⟹ u1≤u2  on Λ,u^1(T,\cdot)\le g\le u^2(T,\cdot)\ \Longrightarrow\ u^1\le u^2\ \text{ on }\Lambda,u1(T,⋅)≤g≤u2(T,⋅) ⟹ u1≤u2  on Λ,

and consequently u0u^0u0 is the unique viscosity solution with terminal condition ggg.

Milestones

In the order the proof uses them: Example 2.5 (hitting times lie in T\mathcal TT); Proposition 5.4 (u0u^0u0 is uniformly continuous); Theorem 4.3 (u0u^0u0 is a viscosity solution); Lemma 5.7 (partial comparison when one of u1,u2u^1,u^2u1,u2 is smooth) and its form under the weaker condition (5.11); the bound u‾≤u0≤uˉ\underline u\le u^0\le\bar uu​≤u0≤uˉ of (6.3) between the Perron envelopes

uˉ(t,ω)=inf⁡{φ(t,0):φ∈D‾(t,ω)},u‾(t,ω)=sup⁡{φ(t,0):φ∈D‾(t,ω)};\bar u(t,\omega) = \inf\{\varphi(t,\mathbf 0):\varphi\in\overline{\mathcal D}(t,\omega)\},\qquad \underline u(t,\omega) = \sup\{\varphi(t,\mathbf 0):\varphi\in\underline{\mathcal D}(t,\omega)\};uˉ(t,ω)=inf{φ(t,0):φ∈D(t,ω)},u​(t,ω)=sup{φ(t,0):φ∈D​(t,ω)};

Lemma 6.3 (classical solutions built from an ODE with random coefficients); and Theorem 6.1, u‾=uˉ\underline u = \bar uu​=uˉ.

Significance

Theorem 4.6 makes the definition of the paper a well-posed one: existence (Theorem 4.3) without uniqueness would allow any number of solutions, and the comparison principle is what identifies the BSDE value as the solution. It gives a path-dependent nonlinear Feynman–Kac formula, characterising non-Markovian BSDEs analytically, and it is the template on which the fully nonlinear theory, path-dependent games and non-Markovian control were later built.

The result is proved, in this paper, and the proof is not known to have been machine-checked. The formalization contributes a precise Lean account of the definitions (Dupire derivatives through extensions to càdlàg paths, the stopping-time class Tt\mathcal T^tTt, Girsanov measures, the piecewise class Cˉ1,2\bar C^{1,2}Cˉ1,2) and a checked proof of comparison. Pieces of independent value are a functional Itô formula for Cb1,2C^{1,2}_bCb1,2​ functionals, Girsanov's theorem on the canonical space, comparison for BSDEs, and optimal stopping under the nonlinear expectation E‾L\underline{\mathcal E}^LE​L.

Difficulty

The classical proof of comparison doubles variables and uses the Crandall–Ishii lemma, which rests on local compactness of the state space; Ω\OmegaΩ is infinite-dimensional and not locally compact, so that route fails. The paper instead proves comparison when one side is smooth (Lemma 5.7), and then shows that the Perron envelopes u‾\underline uu​ and uˉ\bar uuˉ, built from piecewise-smooth super- and subsolutions, coincide. That equality needs an approximation of an arbitrary square-integrable BSDE integrand ZZZ by processes that are piecewise differentiable in time with uniformly continuous derivative, so that the resulting functionals lie in Cˉ1,2\bar C^{1,2}Cˉ1,2 (Lemmas 6.3–6.5). The partial comparison relies on optimal stopping under E‾L\underline{\mathcal E}^LE​L, which the paper treats with heuristic arguments in Remark 3.11 and references to later work, so that step will need its own development.

Formalization scope

Time is [0,∞)[0,\infty)[0,∞) with a fixed horizon TTT; paths take values in Euclidean Rd\mathbb R^dRd and are constant after TTT. Ωt\Omega^tΩt is encoded as continuous paths vanishing on [0,t][0,t][0,t] and Ω^t\hat\Omega^tΩ^t as càdlàg paths constant on [0,t][0,t][0,t], so Ω=Ω0\Omega = \Omega^0Ω=Ω0. Filtrations are the raw ones generated by the canonical process. The Wiener measure is a hypothesis on finite-dimensional laws, and P0tP^t_0P0t​ is its image under the shift. The stochastic integral and BSDE solutions are those of the platform definition Peng1990.SMP.Stochastic.

Conventions and readings, all disclosed in the items:

  • the standing assumptions are Assumptions 4.2 and 4.4 as printed; "continuous in ttt" is for each fixed (ω,y,z)(\omega,y,z)(ω,y,z), "uniformly continuous in ω\omegaω" is one modulus uniform in (t,y,z)(t,y,z)(t,y,z), and the Lipschitz bound uses ∣y−y′∣+∣z−z′∣|y-y'|+|z-z'|∣y−y′∣+∣z−z′∣;
  • Cb1,2C^{1,2}_bCb1,2​ membership is witnessed by an extension to càdlàg paths together with its derivatives, and every statement involving derivatives quantifies over all such extensions; by Theorem 2.4(i) of the paper they agree on Λ\LambdaΛ;
  • the min⁡\minmin/max⁡\maxmax in the test sets is attained at τ~≡t\tilde\tau\equiv tτ~≡t, so the test condition is written as "every Girsanov expectation is ≥0\ge0≥0" (resp. ≤0\le0≤0), with integrability required; no real infimum or supremum is formed, and Theorem 6.1 is stated with greatest lower and least upper bounds;
  • u0u^0u0 is characterised by the BSDE, not constructed: the statements quantify over every uuu satisfying the characterisation, which by Pardoux–Peng holds for exactly one uuu;
  • in (6.2) and (5.11) the sign of the operator is required P0tP^t_0P0t​-a.s. for s∈[t,T)s\in[t,T)s∈[t,T);
  • Lemma 6.3 adds Assumption 4.4, which the page omits although (6.8) uses f^\hat ff^​, and reads "θ=θ^\theta=\hat\thetaθ=θ^ in Λ\LambdaΛ" as Λt\Lambda^tΛt.

No trivializing reading is available: the test functions are exactly the Cb1,2(Λt)C^{1,2}_b(\Lambda^t)Cb1,2​(Λt) functionals satisfying (3.6), the measures exactly the Girsanov measures with ∣βi∣≤L|\beta^i|\le L∣βi∣≤L, and the stopping times exactly Tt\mathcal T^tTt. A test set that is too large makes sub- and supersolutions scarce and the comparison principle weaker, a test set that is too small makes them abundant and the principle false, and neither is the case here.

The source is arXiv:1109.5971v2, the IMS electronic reprint of the Annals of Probability article; its printed page numbers equal the PDF's. Lemmas 6.4 and 6.5 (the approximation of ZZZ) are part of the proof but not stated as items. Contributions welcome: the functional Itô formula, Girsanov on Ωt\Omega^tΩt, BSDE comparison and stability, and the optimal stopping theory under E‾L\underline{\mathcal E}^LE​L.

Selected references

  • I. Ekren, C. Keller, N. Touzi, J. Zhang, On viscosity solutions of path dependent PDEs, Ann. Probab. 42(1) (2014) 204–236. arXiv:1109.5971, doi:10.1214/12-AOP788
  • B. Dupire, Functional Itô calculus, Bloomberg Portfolio Research Paper 2009-04 (2009). SSRN 1435551
  • R. Cont, D.-A. Fournié, Functional Itô calculus and stochastic integral representation of martingales, Ann. Probab. 41(1) (2013) 109–133. arXiv:1002.2446
  • É. Pardoux, S. Peng, Adapted solution of a backward stochastic differential equation, Systems Control Lett. 14 (1990) 55–61. doi:10.1016/0167-6911(90)90082-6
  • I. Ekren, N. Touzi, J. Zhang, Viscosity solutions of fully nonlinear parabolic path dependent PDEs: Part I, Ann. Probab. 44(2) (2016) 1212–1253. arXiv:1210.0006
16 thms1 active userReviewed
Convex OptimizationOperations ResearchOptimization+1·Captain: mikedeng1

Sparse Regression at Scale: Branch-and-Bound rooted in First-Order Optimization 5: Dual Bounds from Active-Set Primal Solutions Lose Only O(kε), Independent of pResearch Paper

Motivation

Best-subset selection with ridge shrinkage, min⁡β12∥y−Xβ∥22+λ0∥β∥0+λ2∥β∥22\min_\beta \tfrac12\|y-X\beta\|_2^2+\lambda_0\|\beta\|_0+\lambda_2\|\beta\|_2^2minβ​21​∥y−Xβ∥22​+λ0​∥β∥0​+λ2​∥β∥22​, is a mixed-integer program that statisticians want to solve to certified optimality at the scale of modern data (ppp up to 10710^7107 features). Hazimeh, Mazumder and Saab (arXiv:2004.06152, Mathematical Programming 2022) built a branch-and-bound solver, L0BnB, whose node relaxations are solved in the primal space by active-set coordinate descent instead of by an interior-point method. Branch-and-bound prunes a node only with a valid dual bound, a certified lower bound on the node's relaxation value. A primal method returns an approximate minimizer, not such a bound, so the solver must turn an inexact primal point into a dual feasible point and needs to know how much is lost in doing so. This mission formalizes the paper's answer, its main theorem (Theorem 3).

Setting

Data are X∈Rn×pX\in\mathbb R^{n\times p}X∈Rn×p with columns X1,…,XpX_1,\dots,X_pX1​,…,Xp​, y∈Rny\in\mathbb R^ny∈Rn, and parameters λ0,λ2,M>0\lambda_0,\lambda_2,M>0λ0​,λ2​,M>0. The reverse Huber penalty is B(t)=∣t∣\mathcal B(t)=|t|B(t)=∣t∣ for ∣t∣≤1|t|\le1∣t∣≤1 and (t2+1)/2(t^2+1)/2(t2+1)/2 for ∣t∣≥1|t|\ge1∣t∣≥1. The penalty ψ(b)\psi(b)ψ(b) equals ψ1(b)=2λ0B(bλ2/λ0)\psi_1(b)=2\lambda_0\mathcal B(b\sqrt{\lambda_2/\lambda_0})ψ1​(b)=2λ0​B(bλ2​/λ0​​) if λ0/λ2≤M\sqrt{\lambda_0/\lambda_2}\le Mλ0​/λ2​​≤M and ψ2(b)=(λ0/M+λ2M)∣b∣\psi_2(b)=(\lambda_0/M+\lambda_2M)|b|ψ2​(b)=(λ0​/M+λ2​M)∣b∣ otherwise. The reduced relaxation (5) is

min⁡β∈Rp F(β)=12∥y−Xβ∥22+∑iψ(βi)s.t.∥β∥∞≤M.\min_{\beta\in\mathbb R^p}\ F(\beta)=\tfrac12\|y-X\beta\|_2^2+\sum_{i}\psi(\beta_i)\quad\text{s.t.}\quad \|\beta\|_\infty\le M .β∈Rpmin​ F(β)=21​∥y−Xβ∥22​+i∑​ψ(βi​)s.t.∥β∥∞​≤M.

Throughout, the columns of XXX and yyy have unit ℓ2\ell_2ℓ2​ norm (the standing assumption of Section 3 of the paper).

Algorithm 2 (active-set coordinate descent) returns a point β^\hat\betaβ^​ in the box such that the set

V={i∉Supp⁡(β^): 0≠arg min⁡∣t∣≤MF(β^1,…,t,…,β^p)}V=\{i\notin\operatorname{Supp}(\hat\beta):\ 0\ne\operatorname*{arg\,min}_{|t|\le M}F(\hat\beta_1,\dots,t,\dots,\hat\beta_p)\}V={i∈/Supp(β^​): 0=∣t∣≤Margmin​F(β^​1​,…,t,…,β^​p​)}

is empty: no coordinate outside the support wants to move. Write r^=y−Xβ^\hat r=y-X\hat\betar^=y−Xβ^​, k=∥β^∥0k=\|\hat\beta\|_0k=∥β^​∥0​, and let β∗\beta^*β∗ be an optimal solution of (5) with r∗=y−Xβ∗r^*=y-X\beta^*r∗=y−Xβ∗. The primal gap is ϵ=∥X(β∗−β^)∥2\epsilon=\|X(\beta^*-\hat\beta)\|_2ϵ=∥X(β∗−β^​)∥2​.

The two duals of (5) (Theorem 2 of the paper) are, with v(α,γi)=[(α⊤Xi−γi)2/(4λ2)−λ0]++M∣γi∣v(\alpha,\gamma_i)=[(\alpha^\top X_i-\gamma_i)^2/(4\lambda_2)-\lambda_0]_++M|\gamma_i|v(α,γi​)=[(α⊤Xi​−γi​)2/(4λ2​)−λ0​]+​+M∣γi​∣,

h1(α,γ)=−12∥α∥22−α⊤y−∑iv(α,γi),h2(ρ,μ)=−12∥ρ∥22−ρ⊤y−M∥μ∥1,h_1(\alpha,\gamma)=-\tfrac12\|\alpha\|_2^2-\alpha^\top y-\textstyle\sum_i v(\alpha,\gamma_i),\qquad h_2(\rho,\mu)=-\tfrac12\|\rho\|_2^2-\rho^\top y-M\|\mu\|_1,h1​(α,γ)=−21​∥α∥22​−α⊤y−∑i​v(α,γi​),h2​(ρ,μ)=−21​∥ρ∥22​−ρ⊤y−M∥μ∥1​,

the latter under ∣ρ⊤Xi∣−μi≤λ0/M+λ2M|\rho^\top X_i|-\mu_i\le\lambda_0/M+\lambda_2M∣ρ⊤Xi​∣−μi​≤λ0​/M+λ2​M. The dual variables built from β∗\beta^*β∗ are α∗=ρ∗=−r∗\alpha^*=\rho^*=-r^*α∗=ρ∗=−r∗, γi∗=1[∣βi∗∣=M](α∗⊤Xi−2Mλ2sign⁡(α∗⊤Xi))\gamma^*_i=\mathbb 1_{[|\beta^*_i|=M]}(\alpha^{*\top}X_i-2M\lambda_2\operatorname{sign}(\alpha^{*\top}X_i))γi∗​=1[∣βi∗​∣=M]​(α∗⊤Xi​−2Mλ2​sign(α∗⊤Xi​)) and μi∗=1[∣βi∗∣=M](∣ρ∗⊤Xi∣−λ0/M−λ2M)\mu^*_i=\mathbb 1_{[|\beta^*_i|=M]}(|\rho^{*\top}X_i|-\lambda_0/M-\lambda_2M)μi∗​=1[∣βi∗​∣=M]​(∣ρ∗⊤Xi​∣−λ0​/M−λ2​M). The dual points built from β^\hat\betaβ^​ are α^=ρ^=−r^\hat\alpha=\hat\rho=-\hat rα^=ρ^​=−r^, with γ^\hat\gammaγ^​ a maximizer of h1(α^,⋅)h_1(\hat\alpha,\cdot)h1​(α^,⋅) (25) and μ^\hat\muμ^​ a maximizer of h2(ρ^,⋅)h_2(\hat\rho,\cdot)h2​(ρ^​,⋅) under the constraints (27).

Formalization targets

Goal: Theorem 3 with the proof's constants

If λ0/λ2≤M\sqrt{\lambda_0/\lambda_2}\le Mλ0​/λ2​​≤M, with ci=(2λ2)−1c_i=(2\lambda_2)^{-1}ci​=(2λ2​)−1 when ∣βi∗∣<M|\beta^*_i|<M∣βi∗​∣<M and ci=Mc_i=Mci​=M when ∣βi∗∣=M|\beta^*_i|=M∣βi∗​∣=M,

h1(α^,γ^) ≥ h1(α∗,γ∗)−2ϵ−12ϵ2−∑i∈Supp⁡(β^)(ciϵ+(4λ2)−1ϵ2).(55)h_1(\hat\alpha,\hat\gamma)\ \ge\ h_1(\alpha^*,\gamma^*)-2\epsilon-\tfrac12\epsilon^2-\sum_{i\in\operatorname{Supp}(\hat\beta)}\big(c_i\epsilon+(4\lambda_2)^{-1}\epsilon^2\big).\qquad(55)h1​(α^,γ^​) ≥ h1​(α∗,γ∗)−2ϵ−21​ϵ2−i∈Supp(β^​)∑​(ci​ϵ+(4λ2​)−1ϵ2).(55)

If λ0/λ2>M\sqrt{\lambda_0/\lambda_2}>Mλ0​/λ2​​>M,

h2(ρ^,μ^) ≥ h2(ρ∗,μ∗)−ϵ(2+Mk)−12ϵ2.(59)h_2(\hat\rho,\hat\mu)\ \ge\ h_2(\rho^*,\mu^*)-\epsilon(2+Mk)-\tfrac12\epsilon^2.\qquad(59)h2​(ρ^​,μ^​) ≥ h2​(ρ∗,μ∗)−ϵ(2+Mk)−21​ϵ2.(59)

The paper states these as −kO(ϵ)−kO(ϵ2)-kO(\epsilon)-kO(\epsilon^2)−kO(ϵ)−kO(ϵ2) (29) and −kO(ϵ)−O(ϵ2)-kO(\epsilon)-O(\epsilon^2)−kO(ϵ)−O(ϵ2) (30); the goal states the expressions its proof establishes.

Milestones

In the order the proof uses them: the closed-form coordinate updates (14) and (15); Proposition 3, V={i∉Supp⁡(β^):∣⟨r^,Xi⟩∣>c(λ0,λ2,M)}V=\{i\notin\operatorname{Supp}(\hat\beta): |\langle\hat r,X_i\rangle|>c(\lambda_0,\lambda_2,M)\}V={i∈/Supp(β^​):∣⟨r^,Xi​⟩∣>c(λ0​,λ2​,M)}; the bound ∥α∗∥2≤1\|\alpha^*\|_2\le1∥α∗∥2​≤1; Lemma 2, which bounds v(α^,γ^i)v(\hat\alpha,\hat\gamma_i)v(α^,γ^​i​) coordinate by coordinate and makes it vanish off the support; inequality (53); the closed form (28) of μ^\hat\muμ^​; the optimality conditions (58); the bound (57) ∣μ^i∣≤ϵ+∣μi∗∣|\hat\mu_i|\le\epsilon+|\mu^*_i|∣μ^​i​∣≤ϵ+∣μi∗​∣ on the support; and inequality (56).

Significance

The result. In both regimes the loss of the dual bound is controlled by the primal gap times the sparsity kkk of the iterate, with constants depending only on MMM and λ2\lambda_2λ2​; the number of features ppp does not enter. Since L0BnB seeks solutions with k≪pk\ll pk≪p, the cheap dual bound obtained from an inexact primal solution is nearly as good as the exact one, which is what allows pruning without an interior-point solve at every node. The paper notes that with plain coordinate descent in place of Algorithm 2 the same argument gives ppp in place of kkk.

Formalizing it. The result is proved in the paper; it has no machine-checked proof. The mission produces a checked version of the main theorem with explicit constants, a formal model of what "output of an active-set method" means for the analysis, and reusable closed forms for the boxed soft-thresholding updates of an ℓ1\ell_1ℓ1​- or reverse-Huber-penalized box-constrained least squares problem.

Difficulty

The bound is not a consequence of weak duality alone: weak duality says only that each dual value is below the primal optimum, and says nothing about how far the constructed dual point is from the dual optimum. The obvious estimate, a Lipschitz bound on h1h_1h1​ or h2h_2h2​ summed over all coordinates, gives a loss proportional to ppp. Getting kkk instead requires showing that the dual contribution of every coordinate outside Supp⁡(β^)\operatorname{Supp}(\hat\beta)Supp(β^​) vanishes exactly, which uses the emptiness of VVV through Proposition 3 and the closed forms (14)–(15) of one-dimensional nonsmooth box-constrained problems. On the support, the loss must be bounded using the structure of γ∗\gamma^*γ∗ and μ∗\mu^*μ∗ at coordinates where β∗\beta^*β∗ hits the box, which is where ci=Mc_i=Mci​=M and (58) enter.

Formalization scope

Indices are Fin p; norms are explicit sums; sign⁡\operatorname{sign}sign is Real.sign with sign⁡(0)=0\operatorname{sign}(0)=0sign(0)=0; [a]+[a]_+[a]+​ is max a 0. The unit norms of the columns of XXX and of yyy are hypotheses, never built into the definitions, and each theorem assumes only the ones it uses. β∗\beta^*β∗ is any point of the box minimizing FFF over the box. The output of Algorithm 2 is modelled by its two properties used in the paper: ∥β^∥∞≤M\|\hat\beta\|_\infty\le M∥β^​∥∞​≤M and V=∅V=\emptysetV=∅ ("0≠arg⁡min⁡0\ne\arg\min0=argmin" encoded as "000 is not a minimizer"); the iterations are not formalized. γ^\hat\gammaγ^​ and μ^\hat\muμ^​ are arbitrary maximizers satisfying (25) and (27). The dual variables (23)–(24) are defined by their formulas; their optimality (Theorem 2, a separate mission) is neither assumed nor needed, and the goal is an inequality between explicit numbers.

Instantiations of O(⋅)O(\cdot)O(⋅). (29) is stated as (55): kO(ϵ)+kO(ϵ2)kO(\epsilon)+kO(\epsilon^2)kO(ϵ)+kO(ϵ2) becomes 2ϵ+12ϵ2+∑i∈Supp⁡(β^)(ciϵ+(4λ2)−1ϵ2)2\epsilon+\tfrac12\epsilon^2+\sum_{i\in\operatorname{Supp}(\hat\beta)}(c_i\epsilon+(4\lambda_2)^{-1}\epsilon^2)2ϵ+21​ϵ2+∑i∈Supp(β^​)​(ci​ϵ+(4λ2​)−1ϵ2) with ci∈{(2λ2)−1,M}c_i\in\{(2\lambda_2)^{-1},M\}ci​∈{(2λ2​)−1,M} decided by β∗\beta^*β∗. (30) is stated as (59): kO(ϵ)+O(ϵ2)kO(\epsilon)+O(\epsilon^2)kO(ϵ)+O(ϵ2) becomes ϵ(2+Mk)+12ϵ2\epsilon(2+Mk)+\tfrac12\epsilon^2ϵ(2+Mk)+21​ϵ2. The proof's final rearrangement of (29), which counts ∣β^i∣|\hat\beta_i|∣β^​i​∣ instead of ∣βi∗∣|\beta^*_i|∣βi∗​∣, is not used.

A formalization that takes β^=β∗\hat\beta=\beta^*β^​=β∗, γ^=γ∗\hat\gamma=\gamma^*γ^​=γ∗ or μ^=μ∗\hat\mu=\mu^*μ^​=μ∗, that drops the hypothesis V=∅V=\emptysetV=∅, or that replaces the constants by an existential "∃C\exists C∃C" would be trivial or a different statement; the goal quantifies over every optimal β∗\beta^*β∗, every box-feasible β^\hat\betaβ^​ with V=∅V=\emptysetV=∅ and every maximizer γ^\hat\gammaγ^​, μ^\hat\muμ^​, with the explicit constants above.

Needed infrastructure: one-dimensional convex minimization on an interval with piecewise penalties, Cauchy–Schwarz for finite sums, and first-order optimality conditions for box-constrained composite problems. Proofs of any milestone are welcome independently.

Selected references

  • H. Hazimeh, R. Mazumder, A. Saab, Sparse Regression at Scale: Branch-and-Bound rooted in First-Order Optimization, arXiv:2004.06152v2, 2021; Mathematical Programming 196 (2022). https://arxiv.org/abs/2004.06152
  • P. Tseng, Convergence of a block coordinate descent method for nondifferentiable minimization, J. Optim. Theory Appl. 109 (2001). https://doi.org/10.1023/A:1017501703105
  • J. Friedman, T. Hastie, R. Tibshirani, Regularization paths for generalized linear models via coordinate descent, J. Stat. Softw. 33 (2010). https://doi.org/10.18637/jss.v033.i01
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Algorithmic Game TheoryControl TheoryProbability·Captain: mikedeng1

A Probabilistic Weak Formulation of Mean Field Games and Applications 3: Distributed Controls from a Mean Field Game Solution Form an ε_n-Nash Equilibrium of the n-Player Game, ε_n → 0Research Paper

Why approximate Nash equilibria of finite games

Mean field games (MFGs) were introduced by Lasry and Lions (Jpn. J. Math. 2007) and by Huang, Malhamé and Caines (Commun. Inf. Syst. 2006) as limits of stochastic differential games with many symmetric players whose interaction runs through the empirical distribution of their states. An MFG is a fixed point problem for one representative player facing a flow of measures, and it is much easier to analyse than an nnn-player game. The justification for studying it is a converse statement: a solution of the MFG should yield strategies that are nearly optimal for every player of the finite game when nnn is large. Results of this type were proved by Huang, Malhamé and Caines for linear-quadratic models and by Carmona and Delarue (SIAM J. Control Optim. 2013) in the strong formulation with Lipschitz data.

Carmona and Lacker (arXiv:1307.1152v2; Ann. Appl. Probab. 25(3), 2015) set up MFGs in a weak formulation: controls change the law of the state through a Girsanov density instead of entering the state equation. This allows measurable, path-dependent data and controls that need only be progressively measurable. Their Theorem 4.2 is the finite-player approximation in this generality. This mission formalizes it.

Setting

Let C=C([0,T];Rd)\mathcal C=C([0,T];\mathbb R^d)C=C([0,T];Rd) with the sup norm, and fix a measurable weight ψ:C→[1,∞)\psi:\mathcal C\to[1,\infty)ψ:C→[1,∞). Pψ(C)\mathcal P_\psi(\mathcal C)Pψ​(C) is the set of probability measures μ\muμ on C\mathcal CC with ∫ψ dμ<∞\int\psi\,d\mu<\infty∫ψdμ<∞, carrying the topology τψ\tau_\psiτψ​: the weakest topology making μ↦∫f dμ\mu\mapsto\int f\,d\muμ↦∫fdμ continuous for every measurable fff with ∣f∣≤c ψ|f|\le c\,\psi∣f∣≤cψ. The control set AAA is a compact convex subset of a normed space, and P(A)\mathcal P(A)P(A) carries the weak topology.

The data are a volatility σ(t,x)\sigma(t,x)σ(t,x), a drift b(t,x,μ,a)b(t,x,\mu,a)b(t,x,μ,a), a running reward f(t,x,μ,q,a)f(t,x,\mu,q,a)f(t,x,μ,q,a) and a terminal reward g(x,μ)g(x,\mu)g(x,μ), where x∈Cx\in\mathcal Cx∈C is a whole path, μ∈Pψ(C)\mu\in\mathcal P_\psi(\mathcal C)μ∈Pψ​(C) and q∈P(A)q\in\mathcal P(A)q∈P(A). On a probability space with an initial value ξ∼λ0\xi\sim\lambda_0ξ∼λ0​ and an independent Wiener process WWW, let XXX solve dXt=σ(t,X) dWtdX_t=\sigma(t,X)\,dW_tdXt​=σ(t,X)dWt​, X0=ξX_0=\xiX0​=ξ. A control α\alphaα (an AAA-valued progressive process) and a measure μ\muμ define a new probability Pμ,αP^{\mu,\alpha}Pμ,α with density

dPμ,αdP=E(∫0⋅σ−1b(t,X,μ,αt) dWt)T,\frac{dP^{\mu,\alpha}}{dP}=\mathcal E\Big(\int_0^\cdot\sigma^{-1}b(t,X,\mu,\alpha_t)\,dW_t\Big)_T,dPdPμ,α​=E(∫0⋅​σ−1b(t,X,μ,αt​)dWt​)T​,

under which XXX has drift b(t,X,μ,αt)b(t,X,\mu,\alpha_t)b(t,X,μ,αt​). The reward is Jμ,q(α)=Eμ,α[∫0Tf(t,X,μ,qt,αt) dt+g(X,μ)]J^{\mu,q}(\alpha)=\mathbb E^{\mu,\alpha}[\int_0^Tf(t,X,\mu,q_t,\alpha_t)\,dt+g(X,\mu)]Jμ,q(α)=Eμ,α[∫0T​f(t,X,μ,qt​,αt​)dt+g(X,μ)]. A pair (μ^,q^)(\hat\mu,\hat q)(μ^​,q^​) is a solution of the MFG (Definition 3.4) if some α^\hat\alphaα^ maximizes Jμ^,q^J^{\hat\mu,\hat q}Jμ^​,q^​ and reproduces the input: Pμ^,α^∘X−1=μ^P^{\hat\mu,\hat\alpha}\circ X^{-1}=\hat\muPμ^​,α^∘X−1=μ^​ and Pμ^,α^∘α^t−1=q^tP^{\hat\mu,\hat\alpha}\circ\hat\alpha_t^{-1}=\hat q_tPμ^​,α^∘α^t−1​=q^​t​ for a.e. ttt. Under the standing assumptions the optimal control is a function α^(t,X)\hat\alpha(t,X)α^(t,X) of the path, the closed-loop control.

The nnn-player game. On a probability space with independent Wiener processes WiW^iWi and i.i.d. initial values ξi∼λ0\xi^i\sim\lambda_0ξi∼λ0​, let XiX^iXi solve dXti=b(t,Xi,α^(t,Xi)) dt+σ(t,Xi) dWtidX^i_t=b(t,X^i,\hat\alpha(t,X^i))\,dt+\sigma(t,X^i)\,dW^i_tdXti​=b(t,Xi,α^(t,Xi))dt+σ(t,Xi)dWti​ (the drift has no mean field term under (F.1)). The distributed controls are αti=α^(t,Xi)\alpha^i_t=\hat\alpha(t,X^i)αti​=α^(t,Xi): each player uses only their own state. A deviation β∈An\beta\in\mathbb A_nβ∈An​ is any process that is progressively measurable for the filtration Fn\mathbb F^nFn of all nnn states (full information). A profile β=(β1,…,βn)\beta=(\beta^1,\dots,\beta^n)β=(β1,…,βn) changes the probability to Pn(β)P_n(\beta)Pn​(β), with density the Doléans exponential of ∑i∫(σ−1b(t,Xi,βti)−σ−1b(t,Xi,αti)) dWti\sum_i\int(\sigma^{-1}b(t,X^i,\beta^i_t)-\sigma^{-1}b(t,X^i,\alpha^i_t))\,dW^i_t∑i​∫(σ−1b(t,Xi,βti​)−σ−1b(t,Xi,αti​))dWti​. Player iii then receives

Jn,i(β)=EPn(β)[∫0Tf(t,Xi,μn,qn(βt),βti) dt+g(Xi,μn)],J_{n,i}(\beta)=\mathbb E^{P_n(\beta)}\Big[\int_0^Tf\big(t,X^i,\mu^n,q^n(\beta_t),\beta^i_t\big)\,dt+g(X^i,\mu^n)\Big],Jn,i​(β)=EPn​(β)[∫0T​f(t,Xi,μn,qn(βt​),βti​)dt+g(Xi,μn)],

with μn=1n∑jδXj\mu^n=\frac1n\sum_j\delta_{X^j}μn=n1​∑j​δXj​ and qn(βt)=1n∑jδβtjq^n(\beta_t)=\frac1n\sum_j\delta_{\beta^j_t}qn(βt​)=n1​∑j​δβtj​​.

Formalization targets

Goal: Theorem 4.2 (p. 13)

Under (S), (C) and (F), there is a sequence ϵn≥0\epsilon_n\ge0ϵn​≥0, ϵn→0\epsilon_n\to0ϵn​→0, such that for all n≥1n\ge1n≥1, 1≤i≤n1\le i\le n1≤i≤n and β∈An\beta\in\mathbb A_nβ∈An​,

Jn,i(α1,…,αi−1,β,αi+1,…,αn)≤Jn,i(α1,…,αn)+ϵn.J_{n,i}(\alpha^1,\dots,\alpha^{i-1},\beta,\alpha^{i+1},\dots,\alpha^n)\le J_{n,i}(\alpha^1,\dots,\alpha^n)+\epsilon_n.Jn,i​(α1,…,αi−1,β,αi+1,…,αn)≤Jn,i​(α1,…,αn)+ϵn​.

No rate is claimed; the theorem asserts only that the gain from deviating vanishes uniformly over players and deviations.

Milestones

  1. Lemma 5.6 (p. 16): for compact KKK, joint continuity of G:E×K→RG:E\times K\to\mathbb RG:E×K→R at {x0}×K\{x_0\}\times K{x0​}×K is equivalent to continuity of G(x0,⋅)G(x_0,\cdot)G(x0​,⋅) together with continuity at x0x_0x0​ of x↦sup⁡y∈K∣G(x,y)−G(x0,y)∣x\mapsto\sup_{y\in K}|G(x,y)-G(x_0,y)|x↦supy∈K​∣G(x,y)−G(x0​,y)∣.
  2. Lemma 8.1 (p. 32): for empirically measurable FFF with ∣F(x,μ)∣≤c(ψ(x)+∫ψ dμ)|F(x,\mu)|\le c(\psi(x)+\int\psi\,d\mu)∣F(x,μ)∣≤c(ψ(x)+∫ψdμ) and F(x,⋅)F(x,\cdot)F(x,⋅) continuous at μ^\hat\muμ^​, E∣F(Xi,μn)−F(Xi,μ^)∣p→0\mathbb E|F(X^i,\mu^n)-F(X^i,\hat\mu)|^p\to0E∣F(Xi,μn)−F(Xi,μ^​)∣p→0 for p∈[1,2)p\in[1,2)p∈[1,2).
  3. The LpL^pLp bound (p. 33): {dPn(βα)/dP:β∈An, n≥1}\{dP_n(\beta^\alpha)/dP:\beta\in\mathbb A_n,\ n\ge1\}{dPn​(βα)/dP:β∈An​, n≥1} is bounded in LpL^pLp for each p≥1p\ge1p≥1, where βα=(β,α2,…,αn)\beta^\alpha=(\beta,\alpha^2,\dots,\alpha^n)βα=(β,α2,…,αn).
  4. Lemma 8.2 (p. 32): sup⁡β∈An∣Jn,1(βα)−Jn′(β)∣→0\sup_{\beta\in\mathbb A_n}|J_{n,1}(\beta^\alpha)-J'_n(\beta)|\to0supβ∈An​​∣Jn,1​(βα)−Jn′​(β)∣→0, where Jn′(β)=EPn(βα)[∫0Tf(t,X1,μ^,q^t,βt) dt+g(X1,μ^)]J'_n(\beta)=\mathbb E^{P_n(\beta^\alpha)}[\int_0^Tf(t,X^1,\hat\mu,\hat q_t,\beta_t)\,dt+g(X^1,\hat\mu)]Jn′​(β)=EPn​(βα)[∫0T​f(t,X1,μ^​,q^​t​,βt​)dt+g(X1,μ^​)].
  5. Lemma 8.3 (p. 33): Jn′(α1)≥Jn′(β)J'_n(\alpha^1)\ge J'_n(\beta)Jn′​(α1)≥Jn′​(β) for every β∈An\beta\in\mathbb A_nβ∈An​.

Significance

Theorem 4.2 states the sense in which an MFG solution solves the finite game. It covers path-dependent and merely measurable coefficients, interaction through the law of the controls, and full-information deviations against distributed strategies. In the paper it underlies the applications of §6: the price impact model, where Proposition 6.1 adds the rate C/nC/\sqrt nC/n​, and the flocking model. The result is qualitative: it gives no rate in general.

The result is proved in the paper. No machine-checked proof of it or of its lemmas exists on the platform. The mission produces a formal statement layer for weak-formulation MFGs: path space, Pψ\mathcal P_\psiPψ​ with τψ\tau_\psiτψ​, Girsanov densities over Itô versions, Definition 3.4, and the nnn-player game. It then asks for the formal proof of the theorem. Missions 1 and 2 of this series (existence and uniqueness of MFG solutions) use the same model encoding. The strong-formulation result of Carmona and Delarue is a separate statement with a separate model and is not part of this mission.

Difficulty

The obvious route replaces μn\mu^nμn by μ^\hat\muμ^​ and qn(βt)q^n(\beta_t)qn(βt​) by q^t\hat q_tq^​t​ in Jn,iJ_{n,i}Jn,i​ and appeals to the law of large numbers. This fails for two reasons. First, the expectation is taken under Pn(β)P_n(\beta)Pn​(β), which depends on the deviation β\betaβ, and β\betaβ may depend on all players' states. The convergence therefore has to be uniform over a class of measures and requires uniform integrability of the densities. Second, τψ\tau_\psiτψ​ is neither metrizable nor separable. Continuity in μ\muμ does not reduce to sequences, and dominated convergence does not hold for nets, so the almost sure convergence of empirical measures does not by itself transfer to the rewards. The remaining step asks whether full information helps the deviating player against the limiting environment. It is not a direct consequence of the optimality of α^\hat\alphaα^ in the mean field problem, which is posed over a smaller filtration.

Formalization scope

  • Paths and time. States are Fin d → ℝ. C\mathcal CC is C(Set.Icc 0 T, Fin d → ℝ) with its Borel σ-field. Time is ℝ≥0; only [0,T][0,T][0,T] matters.
  • Measures and topologies. Pψ(C)\mathcal P_\psi(\mathcal C)Pψ​(C) is a structure carrying τψ\tau_\psiτψ​ as its only topology. P(A)\mathcal P(A)P(A) is Mathlib's ProbabilityMeasure A with the weak topology and its Borel σ-field. Progressive measurability uses the canonical filtration on C\mathcal CC.
  • Base space. It is abstract: any probability space with ξ\xiξ and an independent Brownian motion WWW. The canonical space is an instance. Filtrations are augmented by the measurable null sets.
  • Stochastic integrals. All stochastic integrals come from the published Peng1990.SMP.Stochastic L2L^2L2 Itô layer. "Strong solution" therefore includes square integrability, E∫0T∥σ(t,X)∥2dt<∞\mathbb E\int_0^T\|\sigma(t,X)\|^2dt<\inftyE∫0T​∥σ(t,X)∥2dt<∞ and sup⁡tE∣Xt−ξ∣2<∞\sup_t\mathbb E|X_t-\xi|^2<\inftysupt​E∣Xt​−ξ∣2<∞.
  • Assumptions (S). Nonsingularity of σ\sigmaσ is encoded as invertibility of det⁡σ\det\sigmadetσ. The "increasing" ρ\rhoρ of (S.4) is encoded as monotone.
  • Densities and values. A density is a relation over versions of the Itô integrals. Every statement asserts that a version exists and holds for every version, so no statement holds because the set of versions is empty. Jn,iJ_{n,i}Jn,i​ and Jn′J'_nJn′​ are computed as EP[D(⋯ )]\mathbb E^P[D(\cdots)]EP[D(⋯)] for a version DDD. Suprema over An\mathbb A_nAn​ are unfolded into ∀ε ∃N\forall\varepsilon\,\exists N∀ε∃N form, never written as real ⨆.
  • Players. Players are indexed from 000, so player 1 is index 000.
  • Hypotheses. (S), (C), (F), the fixed solution with its closed-loop control and the game space are bundled into one structure.

Two readings of the goal would make it trivial, and the statement excludes both. If ϵ\epsilonϵ were allowed to depend on iii or β\betaβ, the bound would carry no content. If the deviation were evaluated under the undeviated measure PPP instead of Pn(β)P_n(\beta)Pn​(β), the game would be a different one. (F.4) is genuine continuity, not the sequential continuity of (E).

A complete development needs:

  • the strong law of large numbers for i.i.d. path-valued variables tested against BψB_\psiBψ​ functions;
  • LpL^pLp bounds for Doléans exponentials of bounded integrands;
  • Girsanov's theorem for the L2L^2L2 Itô layer;
  • comparison for BSDEs (Pardoux–Peng).

The Girsanov and BSDE comparison results are reusable well beyond this mission and are welcome as separate contributions, as are proofs of Lemma 5.6 and of the LpL^pLp bound.

Selected references

  • R. Carmona, D. Lacker, A probabilistic weak formulation of mean field games and applications, arXiv:1307.1152v2, 2014; Ann. Appl. Probab. 25(3), 2015. https://arxiv.org/abs/1307.1152v2, https://doi.org/10.1214/14-AAP1020
  • J.-M. Lasry, P.-L. Lions, Mean field games, Jpn. J. Math. 2, 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, Commun. Inf. Syst. 6(3), 2006. https://doi.org/10.4310/CIS.2006.v6.n3.a5
  • R. Carmona, F. Delarue, Probabilistic analysis of mean-field games, SIAM J. Control Optim. 51(4), 2013. https://doi.org/10.1137/120883499
  • É. Pardoux, S. Peng, Adapted solution of a backward stochastic differential equation, Systems Control Lett. 14, 1990. https://doi.org/10.1016/0167-6911(90)90082-6
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Information TheoryMachine LearningProbability+1·Captain: mikedeng1

Information-Theoretic Analysis of Generalization Capability of Learning Algorithms II: n ≥ (8σ²/α²)(ε/β + log(2/β)) Samples Give |L_μ(W) − L_S(W)| ≤ α with Probability at Least 1 − β (Theorem 3)Research Paper

Motivation

A learning algorithm picks a hypothesis WWW from a dataset SSS; its generalization error Lμ(W)−LS(W)L_\mu(W) - L_S(W)Lμ​(W)−LS​(W) measures how far the empirical risk the algorithm sees is from the population risk it is judged by. Classical bounds control this error through the complexity of the hypothesis space (VC dimension, Rademacher complexity) or through the algorithm's stability. An information-theoretic approach instead controls it through how much the output reveals about the data. Russo and Zou (arXiv:1511.05219) introduced this view for adaptive data analysis, and Xu and Raginsky (arXiv:1705.07809) turned it into a general framework for learning algorithms; the framework underlies a large later literature on mutual-information and conditional-mutual-information generalization bounds.

Expected-value bounds of the form ∣E[Lμ(W)−LS(W)]∣≤2σ2I/n|\mathbb E[L_\mu(W) - L_S(W)]| \le \sqrt{2\sigma^2 I/n}∣E[Lμ​(W)−LS​(W)]∣≤2σ2I/n​ say nothing about a single run of the algorithm. A learner usually needs the error to be small with high probability. This mission formalizes Xu and Raginsky's high-probability result, Theorem 3, which gives a sample size sufficient for ∣Lμ(W)−LS(W)∣≤α|L_\mu(W) - L_S(W)| \le \alpha∣Lμ​(W)−LS​(W)∣≤α with probability at least 1−β1-\beta1−β under an information budget.

Timeline. 2016: Russo and Zou bound the expected bias of adaptively selected statistics by mutual information, for finite hypothesis classes. 2016: Bassily, Nissim, Smith, Steinke, Stemmer and Ullman (arXiv:1511.02513) introduce the "monitor technique" to convert expected bounds into high-probability bounds for differentially private and stable algorithms. 2017: Xu and Raginsky adapt the monitor technique to mutual information, obtaining Theorem 3 and its byproduct Theorem 4.

Setting

There is an instance space Z\mathsf ZZ with an unknown probability measure μ\muμ, a hypothesis space W\mathsf WW, and a nonnegative loss ℓ:W×Z→R+\ell:\mathsf W\times\mathsf Z\to\mathbb R_+ℓ:W×Z→R+​. A learning algorithm is a Markov kernel PW∣SP_{W|S}PW∣S​: it receives a dataset S=(Z1,…,Zn)S = (Z_1,\dots,Z_n)S=(Z1​,…,Zn​) of nnn i.i.d. draws from μ\muμ and outputs a random W∈WW\in\mathsf WW∈W. The joint law of data and output is PS,W=μ⊗n⊗PW∣SP_{S,W} = \mu^{\otimes n}\otimes P_{W|S}PS,W​=μ⊗n⊗PW∣S​.

The population risk and empirical risk of www are

Lμ(w)=∫Zℓ(w,z) μ(dz),LS(w)=1n∑i=1nℓ(w,Zi).L_\mu(w) = \int_{\mathsf Z}\ell(w,z)\,\mu(dz),\qquad L_S(w) = \frac1n\sum_{i=1}^n \ell(w,Z_i).Lμ​(w)=∫Z​ℓ(w,z)μ(dz),LS​(w)=n1​i=1∑n​ℓ(w,Zi​).

The empirical-risk vector is ΛW(S)=(LS(w))w∈W\Lambda_{\mathsf W}(S) = (L_S(w))_{w\in\mathsf W}ΛW​(S)=(LS​(w))w∈W​. For random variables X,YX, YX,Y with joint law PX,YP_{X,Y}PX,Y​, the mutual information is I(X;Y)=D(PX,Y ∥ PX⊗PY)∈[0,∞]I(X;Y) = D(P_{X,Y}\,\|\,P_X\otimes P_Y)\in[0,\infty]I(X;Y)=D(PX,Y​∥PX​⊗PY​)∈[0,∞], the Kullback–Leibler divergence from the joint law to the product of the marginals. The algorithm's information budget is I(ΛW(S);W)≤εI(\Lambda_{\mathsf W}(S);W)\le\varepsilonI(ΛW​(S);W)≤ε.

A real random variable UUU is σ\sigmaσ-subgaussian if log⁡E[eλ(U−EU)]≤λ2σ2/2\log\mathbb E[e^{\lambda(U - \mathbb EU)}]\le\lambda^2\sigma^2/2logE[eλ(U−EU)]≤λ2σ2/2 for all λ∈R\lambda\in\mathbb Rλ∈R. The standing assumption is that ℓ(w,Z)\ell(w,Z)ℓ(w,Z), Z∼μZ\sim\muZ∼μ, is σ\sigmaσ-subgaussian for every www; a loss with values in [a,b][a,b][a,b] qualifies with σ=(b−a)/2\sigma = (b-a)/2σ=(b−a)/2.

Formalization targets

Goal: Theorem 3

If I(ΛW(S);W)≤εI(\Lambda_{\mathsf W}(S);W)\le\varepsilonI(ΛW​(S);W)≤ε, then for any α>0\alpha>0α>0 and 0<β≤10<\beta\le10<β≤1, every sample size

n ≥ 8σ2α2(εβ+log⁡2β)guaranteesP[∣Lμ(W)−LS(W)∣>α]≤β,n\ \ge\ \frac{8\sigma^2}{\alpha^2}\Big(\frac{\varepsilon}{\beta}+\log\frac2\beta\Big)\quad\text{guarantees}\quad \mathbb P\big[|L_\mu(W)-L_S(W)|>\alpha\big]\le\beta,n ≥ α28σ2​(βε​+logβ2​)guaranteesP[∣Lμ​(W)−LS​(W)∣>α]≤β,

the probability being under PS,WP_{S,W}PS,W​.

Milestones

  1. Lemma B.1 — mmm independent parallel runs: I(ΛW(S1),…,ΛW(Sm);Wm)≤mεI(\Lambda_{\mathsf W}(S_1),\dots,\Lambda_{\mathsf W}(S_m);W^m)\le m\varepsilonI(ΛW​(S1​),…,ΛW​(Sm​);Wm)≤mε.
  2. Lemma B.2 — for any algorithm outputting (W,T,R)∈W×[m]×{±1}(W,T,R)\in\mathsf W\times[m]\times\{\pm1\}(W,T,R)∈W×[m]×{±1} from mmm datasets with information at most ε\varepsilonε: E[R(LST(W)−Lμ(W))]≤2σ2ε/n\mathbb E[R(L_{S_T}(W)-L_\mu(W))]\le\sqrt{2\sigma^2\varepsilon/n}E[R(LST​​(W)−Lμ​(W))]≤2σ2ε/n​.
  3. The monitor's information (p. 12): the arg max selector (W∗,T∗,R∗)(W^*,T^*,R^*)(W∗,T∗,R∗) of one of the mmm runs satisfies I(ΛW(S1),…,ΛW(Sm);W∗,T∗,R∗)≤mε+log⁡(2m)I(\Lambda_{\mathsf W}(S_1),\dots,\Lambda_{\mathsf W}(S_m);W^*,T^*,R^*)\le m\varepsilon+\log(2m)I(ΛW​(S1​),…,ΛW​(Sm​);W∗,T∗,R∗)≤mε+log(2m).
  4. (B.7) — E[max⁡t∈[m]∣LSt(Wt)−Lμ(Wt)∣]≤2σ2n(mε+log⁡(2m))\mathbb E\big[\max_{t\in[m]}|L_{S_t}(W_t)-L_\mu(W_t)|\big]\le\sqrt{\tfrac{2\sigma^2}{n}(m\varepsilon+\log(2m))}E[maxt∈[m]​∣LSt​​(Wt​)−Lμ​(Wt​)∣]≤n2σ2​(mε+log(2m))​.
  5. Theorem 4 — the case m=1m=1m=1: E∣Lμ(W)−LS(W)∣≤2σ2n(ε+log⁡2)\mathbb E|L_\mu(W)-L_S(W)|\le\sqrt{\tfrac{2\sigma^2}{n}(\varepsilon+\log 2)}E∣Lμ​(W)−LS​(W)∣≤n2σ2​(ε+log2)​.

Significance

The result. Theorem 3 shows that a sample complexity polynomial in 1/α1/\alpha1/α and logarithmic in 1/β1/\beta1/β, the same order as for a data-independent hypothesis (where Chernoff–Hoeffding gives 2σ2α2log⁡2β\frac{2\sigma^2}{\alpha^2}\log\frac2\betaα22σ2​logβ2​), still suffices for a data-dependent one, provided the information budget ε\varepsilonε is small relative to β\betaβ. It requires only subgaussian losses, whereas the earlier high-probability bounds of differential privacy apply to bounded losses or bounded-difference functions. Since I(ΛW(S);W)≤I(S;W)I(\Lambda_{\mathsf W}(S);W)\le I(S;W)I(ΛW​(S);W)≤I(S;W), any algorithm with small input-output mutual information (the Gibbs algorithm, noisy empirical risk minimization, adaptive compositions of such) inherits the guarantee. Theorem 4 improves Russo and Zou's bound on the expected absolute error.

Formalizing it. The result is proved in the paper; to the best of current knowledge no machine-checked version exists. The mission produces a Lean statement of the theorem with the correct domain of validity (see the scope section), and its proof will require a reusable layer of measure-theoretic information theory: mutual information of joint laws, its additivity over independent pairs, the data-processing inequality, a bound by the logarithm of the number of values of a discrete variable, and the Donsker–Varadhan route from mutual information to expectations of subgaussian functions.

Difficulty

The obvious argument fails at the step from an expectation to a probability. Markov's inequality applied to Theorem 4 gives a sample size of order σ2(ε+log⁡2)/(α2β2)\sigma^2(\varepsilon+\log 2)/(\alpha^2\beta^2)σ2(ε+log2)/(α2β2), quadratic in 1/β1/\beta1/β. A union-bound or Chernoff argument per hypothesis does not apply, because WWW depends on SSS and the deviation at the selected hypothesis is not a sum of independent terms. The paper's route runs m≈1/βm\approx 1/\betam≈1/β independent copies and selects the worst one; the delicate part is bounding the information the selection itself adds, which needs the chain rule and data processing for mutual information on general (non-discrete) spaces, and an expectation bound that holds uniformly over every selection rule.

Formalization scope

Lean conventions:

  • Z\mathsf ZZ, W\mathsf WW are measurable spaces; datasets are Fin n → Z with law Measure.pi, taken from the published LearnStability.Characterization.Setting (sampleLaw, risk, empRisk); the algorithm is a Markov kernel; the joint law is sampleLaw μ n ⊗ₘ κ.
  • W\mathsf WW is countable with measurable singletons in the deviation bounds (Lemma B.2, (B.7), Theorems 3 and 4). The paper claims its results hold "even when W\mathsf WW is uncountably infinite" (p. 4). Under the product σ-algebra on RW\mathbb R^{\mathsf W}RW this fails: with Z=[0,1]\mathsf Z=[0,1]Z=[0,1], μ\muμ uniform, W=[0,1]n\mathsf W=[0,1]^nW=[0,1]n, ℓ(w,z)=1{z∈{w1,…,wn}}\ell(w,z)=\mathbf 1\{z\in\{w_1,\dots,w_n\}\}ℓ(w,z)=1{z∈{w1​,…,wn​}} and the algorithm W=SW=SW=S, one has I(ΛW(S);W)=0I(\Lambda_{\mathsf W}(S);W)=0I(ΛW​(S);W)=0 but ∣Lμ(W)−LS(W)∣=1|L_\mu(W)-L_S(W)|=1∣Lμ​(W)−LS​(W)∣=1 always. Lemma B.1 and the monitor's information bound hold for arbitrary measurable W\mathsf WW.
  • The loss is jointly measurable; n≥1n\ge1n≥1; ε≥0\varepsilon\ge0ε≥0; σ\sigmaσ-subgaussianity is Mathlib's HasSubgaussianMGF of the centred loss with variance proxy σ2\sigma^2σ2.
  • Mutual information is valued in [0,∞][0,\infty][0,∞]; the budget is I ≤ ENNReal.ofReal ε. Expectations of nonnegative quantities (∣⋅∣|\cdot|∣⋅∣, max⁡t\max_tmaxt​) are lower Lebesgue integrals; Lemma B.2's signed expectation is a Bochner integral whose integrand is integrable under the hypotheses.
  • [m][m][m] is Fin m; the sign r∈{±1}r\in\{\pm1\}r∈{±1} is a Bool read through sgn.
  • "A sample complexity of n=…n = \dotsn=…" is read as n≥…n\ge\dotsn≥…, as the proof requires.
  • The monitor of milestone 3 is a Markov kernel selecting (T∗,R∗)(T^*,R^*)(T∗,R∗) from all runs and choosing an arg max as in (B.3) almost surely; ties may be resolved randomly.

Two printed slips are corrected in the Lean and disclosed in the item notes: the proof of Lemma B.2 claims rLst(w)rL_{s_t}(w)rLst​​(w) is σ/n\sigma/\sqrt nσ/n​-subgaussian under the product of marginals (false; the centred version is), and (B.6) bounds the negative of the quantity in (B.4) ((B.7) is still correct).

The hypothesis is I(ΛW(S);W)≤εI(\Lambda_{\mathsf W}(S);W)\le\varepsilonI(ΛW​(S);W)≤ε, not the stronger I(S;W)≤εI(S;W)\le\varepsilonI(S;W)≤ε, and the goal mentions neither the parallel copies nor the monitor; a formalization that strengthened the hypothesis, dropped the measurability of the loss (so that the law of (ΛW(S),W)(\Lambda_{\mathsf W}(S),W)(ΛW​(S),W) collapses to the zero measure and every mutual information is 000), or allowed ε<0\varepsilon<0ε<0 would be a weaker, vacuous or false statement.

Welcome contributions: chain rule and data processing for klDiv-based mutual information, additivity over independent products, the log⁡k\log klogk bound for finitely-valued outputs, and the Donsker–Varadhan decoupling lemma; these are reusable across the series and beyond.

Selected references

  • A. Xu and M. Raginsky, Information-theoretic analysis of generalization capability of learning algorithms, NIPS 2017. arXiv:1705.07809v2
  • D. Russo and J. Zou, Controlling bias in adaptive data analysis using information theory, AISTATS 2016. arXiv:1511.05219
  • R. Bassily, K. Nissim, A. Smith, T. Steinke, U. Stemmer and J. Ullman, Algorithmic stability for adaptive data analysis, STOC 2016. arXiv:1511.02513
  • S. Shalev-Shwartz, O. Shamir, N. Srebro and K. Sridharan, Learnability, stability and uniform convergence, JMLR 11, 2010. jmlr.org
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Algorithmic Game TheoryProbabilityStochastic Systems·Captain: mikedeng1

From the Master Equation to Mean Field Game Limit Theory: Large Deviations and Concentration of Measure 2: Nash Equilibrium Empirical Measure Flows Satisfy a Weak LDP Under Common NoiseResearch Paper

Motivation

A mean field game describes the Nash equilibria of nnn symmetric players whose states interact only through their empirical distribution, in the limit n→∞n\to\inftyn→∞. The law of large numbers for the equilibria — convergence of the empirical measure of the nnn-player equilibrium to the mean field equilibrium — was proved in the diffusion setting by Cardaliaguet, Delarue, Lasry and Lions through the master equation (arXiv:1509.02505), and refined by Delarue, Lacker and Ramanan into fluctuation estimates and a central limit theorem in a companion paper (Electron. J. Probab. 2019). The next question is the size of rare deviations: the probability that the nnn-player equilibrium empirical measure flow stays near a flow different from the mean field limit decays exponentially in nnn, and the exponent is a rate function. Delarue, Lacker and Ramanan (arXiv:1804.08550) prove such a large deviation principle (LDP), including the case of a common noise affecting all players, for which no LDP was previously known even for McKean–Vlasov particle systems.

Timeline. Dawson and Gärtner (1987) proved the LDP for the empirical measure flows of weakly interacting diffusions without common noise, with time-independent coefficients and deterministic initial states, using the action functional adopted here. Budhiraja, Dupuis and Fischer (Ann. Probab. 2012) gave a weak-convergence proof for the empirical measure of paths. For mean field games, master-equation methods gave limit theorems, including LDPs, for finite state spaces without common noise (Cecchin–Fischer, arXiv:1704.00984; Cecchin–Pelino, arXiv:1707.01819; Bayraktar–Cohen, arXiv:1707.02648), and Lacker and Ramanan proved an LDP for static games (arXiv:1702.02113). The present paper (arXiv v1, 2018; Ann. Probab. 2020) treats diffusion-based games, with common noise.

Setting

On a filtered probability space (Ω,F,F,P)(\Omega,\mathcal F,\mathbb F,\mathbb P)(Ω,F,F,P) live a d0d_0d0​-dimensional Brownian motion WWW (the common noise), independent ddd-dimensional Brownian motions B1,B2,…B^1,B^2,\dotsB1,B2,…, and i.i.d. initial states X01,X02,…X^1_0,X^2_0,\dotsX01​,X02​,… with law μ0\mu_0μ0​. The whole initial-state family is independent of the joint noise family, as specified for (6.1). Player iii of nnn controls

dXti=b(Xti,mXtn,αti) dt+σ dBti+σ0 dWt,mxn=1n∑i=1nδxi,dX^i_t=b(X^i_t,m^n_{\boldsymbol X_t},\alpha^i_t)\,dt+\sigma\,dB^i_t+\sigma_0\,dW_t,\qquad m^n_{\boldsymbol x}=\frac1n\sum_{i=1}^n\delta_{x_i},dXti​=b(Xti​,mXt​n​,αti​)dt+σdBti​+σ0​dWt​,mxn​=n1​i=1∑n​δxi​​,

with running cost fff and terminal cost ggg. With the Hamiltonian H(x,m,y)=inf⁡a[b(x,m,a)⋅y+f(x,m,a)]H(x,m,y)=\inf_a[b(x,m,a)\cdot y+f(x,m,a)]H(x,m,y)=infa​[b(x,m,a)⋅y+f(x,m,a)], its minimizer α^\hat\alphaα^ and b^(x,m,y)=b(x,m,α^(x,m,y))\hat b(x,m,y)=b(x,m,\hat\alpha(x,m,y))b^(x,m,y)=b(x,m,α^(x,m,y)), a classical solution (vn,i)i(v^{n,i})_i(vn,i)i​ of the Nash system (2.6) gives the equilibrium states

dXti=b^(Xti,mXtn,Dxivn,i(t,Xt))dt+σ dBti+σ0 dWt.(2.7)dX^i_t=\hat b\big(X^i_t,m^n_{\boldsymbol X_t},D_{x_i}v^{n,i}(t,\boldsymbol X_t)\big)dt+\sigma\,dB^i_t+\sigma_0\,dW_t. \qquad (2.7)dXti​=b^(Xti​,mXt​n​,Dxi​​vn,i(t,Xt​))dt+σdBti​+σ0​dWt​.(2.7)

The master equation (2.8) is a PDE for U(t,x,m)U(t,x,m)U(t,x,m) on [0,T]×Rd×P2(Rd)[0,T]\times\mathbb R^d\times\mathcal P^2(\mathbb R^d)[0,T]×Rd×P2(Rd) involving derivatives in the measure argument. Assumption A asks for Lipschitz b^\hat bb^ (with exponent p∗∈[1,2]p^*\in[1,2]p∗∈[1,2] for the Wasserstein metric), non-degenerate σ\sigmaσ, p′>4p'>4p′>4 moments of μ0\mu_0μ0​, classical solutions of the Nash systems, and a classical solution UUU of the master equation with bounded derivatives; B or B′ controls f^\hat ff^​.

The state space is C([0,T];P1(Rd))C([0,T];\mathcal P^1(\mathbb R^d))C([0,T];P1(Rd)): flows ν=(νt)\nu=(\nu_t)ν=(νt​) of probability measures with finite first moment, continuous for the 1-Wasserstein distance W1\mathcal W_1W1​, with the uniform metric sup⁡tW1(νt,νt′)\sup_t\mathcal W_1(\nu_t,\nu'_t)supt​W1​(νt​,νt′​). The rate function uses the drift b~(t,x,m)=b^(x,m,DxU(t,x,m))\tilde b(t,x,m)=\hat b(x,m,D_xU(t,x,m))b~(t,x,m)=b^(x,m,Dx​U(t,x,m)) and the Dawson–Gärtner action functional

I(ν)=12∫0T∥ν˙t−Lt,νt∗νt∥νt2 dt,Lt,mφ=12Tr[σσ⊤D2φ]+Dφ⋅b~(t,⋅,m),I(\nu)=\frac12\int_0^T\big\|\dot\nu_t-\mathcal L^*_{t,\nu_t}\nu_t\big\|^2_{\nu_t}\,dt,\qquad \mathcal L_{t,m}\varphi=\tfrac12\mathrm{Tr}[\sigma\sigma^\top D^2\varphi]+D\varphi\cdot\tilde b(t,\cdot,m),I(ν)=21​∫0T​​ν˙t​−Lt,νt​∗​νt​​νt​2​dt,Lt,m​φ=21​Tr[σσ⊤D2φ]+Dφ⋅b~(t,⋅,m),

with ∥γ∥m2=sup⁡φ⟨γ,φ⟩2/⟨m,∣Dφ∣2⟩\|\gamma\|^2_m=\sup_\varphi\langle\gamma,\varphi\rangle^2/\langle m,|D\varphi|^2\rangle∥γ∥m2​=supφ​⟨γ,φ⟩2/⟨m,∣Dφ∣2⟩ over test functions, and I=∞I=\inftyI=∞ off absolutely continuous paths. With common noise, the drift is shifted along the mean path: I~ϕ\tilde I^\phiI~ϕ is III for the drift b~(t,x+ϕt,m∘τ−ϕt−1)\tilde b(t,x+\phi_t,m\circ\tau^{-1}_{-\phi_t})b~(t,x+ϕt​,m∘τ−ϕt​−1​), τx(z)=z−x\tau_x(z)=z-xτx​(z)=z−x, and

Jσ0(ν)=I~Mb~,ν((νt∘τMtb~,ν−1)t),Mtb~,ν=σΠσ−1σ0σ−1(∫x d(νt−ν0)−∫0t⟨νs,b~(s,⋅,νs)⟩ds),J^{\sigma_0}(\nu)=\tilde I^{\mathbb M^{\tilde b,\nu}}\big((\nu_t\circ\tau^{-1}_{\mathbb M^{\tilde b,\nu}_t})_t\big),\quad \mathbb M^{\tilde b,\nu}_t=\sigma\Pi_{\sigma^{-1}\sigma_0}\sigma^{-1}\Big(\int x\,d(\nu_t-\nu_0)-\int_0^t\langle\nu_s,\tilde b(s,\cdot,\nu_s)\rangle ds\Big),Jσ0​(ν)=I~Mb~,ν((νt​∘τMtb~,ν​−1​)t​),Mtb~,ν​=σΠσ−1σ0​​σ−1(∫xd(νt​−ν0​)−∫0t​⟨νs​,b~(s,⋅,νs​)⟩ds),

where Πσ−1σ0\Pi_{\sigma^{-1}\sigma_0}Πσ−1σ0​​ is the orthogonal projection onto the image of σ−1σ0\sigma^{-1}\sigma_0σ−1σ0​. R\mathcal RR is relative entropy.

Formalization targets

Goal: Theorem 3.10 (weak LDP, common noise allowed)

If p∗=1p^*=1p∗=1, A and B or B′ hold, and ∫eλ∣x∣μ0(dx)<∞\int e^{\lambda|x|}\mu_0(dx)<\infty∫eλ∣x∣μ0​(dx)<∞ for every λ>0\lambda>0λ>0, then for open OOO, compact KKK and closed FFF,

lim inf⁡n1nlog⁡P(mXn∈O)≥−inf⁡O(Jσ0+R(⋅0∣μ0)),lim sup⁡n1nlog⁡P(mXn∈K)≤−inf⁡K(Jσ0+R(⋅0∣μ0)),\liminf_n\tfrac1n\log\mathbb P(m^n_{\boldsymbol X}\in O)\ge-\inf_O\big(J^{\sigma_0}+\mathcal R(\cdot_0|\mu_0)\big),\qquad \limsup_n\tfrac1n\log\mathbb P(m^n_{\boldsymbol X}\in K)\le-\inf_K\big(J^{\sigma_0}+\mathcal R(\cdot_0|\mu_0)\big),nliminf​n1​logP(mXn​∈O)≥−Oinf​(Jσ0​+R(⋅0​∣μ0​)),nlimsup​n1​logP(mXn​∈K)≤−Kinf​(Jσ0​+R(⋅0​∣μ0​)), lim sup⁡n1nlog⁡P(mXn∈F)≤−lim⁡δ↘0inf⁡Fδ(Jσ0+R(⋅0∣μ0)).\limsup_n\tfrac1n\log\mathbb P(m^n_{\boldsymbol X}\in F)\le-\lim_{\delta\searrow0}\inf_{F_\delta}\big(J^{\sigma_0}+\mathcal R(\cdot_0|\mu_0)\big).nlimsup​n1​logP(mXn​∈F)≤−δ↘0lim​Fδ​inf​(Jσ0​+R(⋅0​∣μ0​)).

Milestones

Exponential equivalence of the Nash flows and the McKean–Vlasov particle flows (Corollary 6.1); a weak LDP for the noises and initial states (Proposition 6.15); uniform continuity of the McKean–Vlasov solution map (Lemma 6.16); the shifted action (Lemma 6.4); identification of the contracted entropy (Lemma 6.17); the weak LDP for general weakly interacting systems with common noise (Theorem 6.8) and its transfer to the Nash flows (Theorem 6.13); compactness after centering (Proposition 6.11); removal of the δ\deltaδ-relaxation on compacts, and the full LDP without common noise (Proposition 6.10); explicit forms of Jσ0J^{\sigma_0}Jσ0​ (Proposition 6.5, Theorem 6.6). A companion item states Theorem 3.9: without common noise, a full LDP with the good rate function I(ν)+R(ν0∣μ0)I(\nu)+\mathcal R(\nu_0|\mu_0)I(ν)+R(ν0​∣μ0​).

Significance

The result quantifies how unlikely atypical equilibrium behaviour is in large games: rare macroscopic deviations of the equilibrium empirical measure flow cost exp⁡(−n rate)\exp(-n\,\mathrm{rate})exp(−nrate), and the rate function makes explicit that the common noise moves the mean of the population for free in the directions of the image of σ0\sigma_0σ0​. When σ0≠0\sigma_0\ne0σ0​=0 the rate function has non-compact level sets, which is why the principle is weak and why the closed-set bound carries the δ\deltaδ-relaxation.

The proof transfers the LDP from the McKean–Vlasov particle system to the Nash system through the master equation, a method that applies beyond this model. Nothing in this paper is formalized: there is no large deviation principle, no Wasserstein space of measure flows, no derivative on Wasserstein space and no mean field game on the platform. A formal development produces reusable definitions (weak and full LDPs, the Dawson–Gärtner action functional, C([0,T];P1)C([0,T];\mathcal P^1)C([0,T];P1)) and checked proofs of the contraction and exponential-equivalence steps. The exponential estimate behind Corollary 6.1 (Theorem 4.3) is the companion mission's milestone and rests on estimates quoted from the companion central-limit-theorem paper.

Difficulty

The obvious route — exponential equivalence plus the Dawson–Gärtner LDP for the particle system — fails twice. The particle drift b~\tilde bb~ is time-dependent and the initial states are random, which the classical results do not cover; and with common noise there is no LDP to transfer. The proof instead freezes the noise: it proves a weak LDP for the pair (empirical measure of initial states and idiosyncratic paths, common noise path), which needs Sanov's theorem in the W1\mathcal W_1W1​ topology and the Brownian support theorem, and contracts it through the McKean–Vlasov solution map. The contraction principle requires the rate function to be good, and it is not when σ0≠0\sigma_0\ne0σ0​=0; uniform continuity of the solution map and the δ\deltaδ-enlargements replace goodness.

Formalization scope

Time is [0,T]⊂R≥0[0,T]\subset\mathbb R_{\ge0}[0,T]⊂R≥0​ with T>0T>0T>0; paths are continuous maps on [0,T][0,T][0,T], and solutions of the SDEs are path-valued, adapted, and satisfy the integral equations almost surely. Players are indexed from 000. Probability measures with finite ppp-th moment are guarded by an explicit predicate, and Wp\mathcal W_pWp​ is the published WassersteinDRO.Duality.wassersteinDistance, kept in [0,∞][0,\infty][0,∞]. Derivatives in xxx, vvv, ttt are genuine derivatives; derivatives in the measure are normalized flat-derivative witnesses. Relative entropy is Mathlib's klDiv. Logarithms of probabilities are in [−∞,∞][-\infty,\infty][−∞,∞]; open, closed and compact sets are those of the uniform W1\mathcal W_1W1​ metric, and lim⁡δ↘0\lim_{\delta\searrow0}limδ↘0​ is a supremum over δ>0\delta>0δ>0. The action functional is an infimum over all distributional time derivatives, with test functions and distributions from Mathlib. The common-noise paths are d0d_0d0​-dimensional.

Standing assumptions are carried explicitly: the filtered space and noises of §2.3, joint independence of initial states and noises from §6.1, Assumption A (with the Borel measurability of b,f,gb,f,gb,f,g), B or B′, p∗=1p^*=1p∗=1 where the paper assumes it, and, for §6, Condition 6.3 and non-degenerate σ\sigmaσ. Two disclosed additions: Theorems 3.9, 3.10 and 6.13 assume b~\tilde bb~ bounded (Condition 6.3(2) requires it; Assumption A does not imply it), and Theorem 6.13 assumes p∗=1p^*=1p∗=1. The solutions of the Nash systems, the master equation and the SDEs are hypotheses; existence is not posed.

A rate function identically 000 or ∞\infty∞, or bounds over a restricted family of sets, would trivialize the statements: the seminorm is a supremum over all test functions, I=∞I=\inftyI=∞ exactly off absolutely continuous flows, and the bounds quantify over every open, compact or closed set. A complete development needs Sanov's theorem in W1\mathcal W_1W1​, the Brownian support theorem, the contraction principle, Dawson–Gärtner's analysis of distribution-valued paths, and stochastic calculus for the particle systems; each of these is reusable, and contributions to any of them are welcome.

Selected references

  • F. Delarue, D. Lacker, K. Ramanan, From the master equation to mean field game limit theory: large deviations and concentration of measure, Ann. Probab. 48(1), 2020; arXiv v1, 2018. https://arxiv.org/abs/1804.08550
  • F. Delarue, D. Lacker, K. Ramanan, From the master equation to mean field game limit theory: a central limit theorem, Electron. J. Probab. 24, 2019 (reference [19] of the paper).
  • P. Cardaliaguet, F. Delarue, J.-M. Lasry, P.-L. Lions, The master equation and the convergence problem in mean field games, Ann. Math. Studies 201, 2019. https://arxiv.org/abs/1509.02505
  • D. Dawson, J. Gärtner, Large deviations from the McKean–Vlasov limit for weakly interacting diffusions, Stochastics 20(4), 1987, 247–308.
  • A. Budhiraja, P. Dupuis, M. Fischer, Large deviation properties of weakly interacting processes via weak convergence methods, Ann. Probab. 40(1), 2012, 74–102.
  • R. Wang, X. Wang, L. Wu, Sanov's theorem in the Wasserstein distance: a necessary and sufficient condition, Statist. Probab. Lett. 80(5), 2010, 505–512.
  • A. Cecchin, G. Pelino, Convergence, fluctuations and large deviations for finite state mean field games via the master equation, 2017. https://arxiv.org/abs/1707.01819
  • D. Lacker, K. Ramanan, Rare Nash equilibria and the price of anarchy in large static games, 2017. https://arxiv.org/abs/1702.02113
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Convex OptimizationDynamical SystemsFunctional Analysis+2·Captain: mikedeng1

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

Motivation

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

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

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

Setting

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

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

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

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

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

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

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

Formalization targets

Goal: Theorem 4.2 (p. 18)

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

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

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

Milestones

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

Significance

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

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

Difficulty

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

Formalization scope

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

Selected references

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

Quality in Supply Chain Encroachment III: With a Fixed Cost of Quality, the Encroaching Manufacturer Does Not Differentiate Quality Across ChannelsResearch Paper

Why channel quality matters

A manufacturer that sells through a retailer can also open a direct sales channel. The direct channel lets the manufacturer reach consumers, but it competes with the retailer, whose orders generate wholesale revenue. The manufacturer can further choose whether the two channels carry products of the same quality. These decisions interact because quality changes both consumer demand and the retailer's response. Ha, Long and Nasiry study this interaction in a sequential supply-chain game. Their fixed-quality-cost extension asks what happens when a high-quality design can be converted into a lower-quality variant without paying a separate production cost for each unit (Ha, Long and Nasiry, §6.2).

The main result is specific to this cost regime. With a cost per unit that rises with quality, different products can be attractive across the channels; with the paper's one-time cost of creating quality, Proposition 6(i) asserts equal qualities when the direct channel makes positive sales. This mission targets that fixed-cost proposition in the authors' manuscript, including its game and the reduced-profit claims used in the e-Companion (Ha, Long and Nasiry, pp. 20, 36–37).

The sequential market

The market has mass one of consumers, indexed by a taste for quality θ\thetaθ uniformly distributed on [0,1][0,1][0,1]. A consumer buying a product of quality v>0v>0v>0 at price ppp receives surplus θv−p\theta v-pθv−p. The manufacturer offers quality u>0u>0u>0 through her own direct channel and quality tu>0tu>0tu>0 through the retailer. The ratio ttt therefore records which channel has higher quality. The manufacturer pays a fixed cost of quality max⁡{ku2,k(tu)2}\max\{ku^2,k(tu)^2\}max{ku2,k(tu)2}, with k>0k>0k>0, and a direct selling cost c≥0c\ge0c≥0 per unit. The retailer has zero selling cost. Unlike a unit production cost, this fixed cost is paid once and does not scale with either channel's quantity (Ha, Long and Nasiry, pp. 7–8, 20).

The manufacturer first chooses wholesale price www and qualities u,tuu,tuu,tu. After observing them, the retailer chooses its order qR≥0q_R\ge0qR​≥0. The manufacturer observes that order and chooses her direct quantity qM≥0q_M\ge0qM​≥0. When 0<t≤10<t\le10<t≤1, market-clearing prices are

pM=u(1−qM−tqR),pR=tu(1−qM−qR).p_M=u(1-q_M-tq_R),\qquad p_R=tu(1-q_M-q_R).pM​=u(1−qM​−tqR​),pR​=tu(1−qM​−qR​).

When t≥1t\ge1t≥1, the retailer's product has higher quality, and the corresponding prices are

pM=u(1−qM−qR),pR=tu(1−qR)−uqM.p_M=u(1-q_M-q_R),\qquad p_R=tu(1-q_R)-uq_M.pM​=u(1−qM​−qR​),pR​=tu(1−qR​)−uqM​.

The manufacturer receives wholesale revenue plus direct-channel revenue, less the direct selling cost and fixed quality cost. The retailer receives its retail margin times qRq_RqR​. Encroachment means qM>0q_M>0qM​>0 on the equilibrium path, rather than the mere existence of a direct channel (Ha, Long and Nasiry, pp. 8, 11, 15, 36).

Formalization targets

Equal quality under encroachment

For a subgame-perfect equilibrium σ\sigmaσ of the fixed-cost game, the goal is Proposition 6(i):

qM(σ)>0⟹t(σ)=1.q_M(\sigma)>0\quad\Longrightarrow\quad t(\sigma)=1.qM​(σ)>0⟹t(σ)=1.

The formal statement assumes c>0c>0c>0. At c=0c=0c=0, the high-direct-quality reduced profit is independent of ttt, so the printed claim fails to force t=1t=1t=1; this is a substantive qualification of the manuscript's standing c≥0c\ge0c≥0 convention. The goal concerns the complete game, with contingent actions at every decision node, rather than only the closed-form optimization problem (Ha, Long and Nasiry, pp. 20, 36).

Subgame and optimization claims

The milestone list follows the authors' two quality regimes. The e-Companion gives best responses, wholesale prices, and reduced profits in each regime. In the high-direct-quality regime, Claim 3 concludes that an optimum with positive direct sales has t=1t=1t=1. In the low-direct-quality regime, Lemma 2 concludes that an optimum either has t=1t=1t=1 or lies at no encroachment. The latter alternative is outside the strict encroachment-feasible set used by the Lean milestone. Footnote 2 supplies a one-variable sign inequality used in the analysis of that regime (Ha, Long and Nasiry, pp. 36–37).

What the result gives

Proposition 6(i) determines the manufacturer's quality choice conditional on active direct sales: both channels carry quality uuu. It narrows the set of equilibrium outcomes that the fixed-cost model can support and distinguishes the role of a one-time design cost from the paper's earlier variable-cost model. The paper states a separate profit comparison in Proposition 6(ii); this mission does not formalize it because the e-Companion omits its proof and the fixed-cost no-encroachment benchmark for that comparison is not stated (Ha, Long and Nasiry, pp. 20, 37).

A complete Lean development would connect the reduced-profit calculations on page 36 to subgame-perfect play in the three-stage game, and establish the optimization claims over their stated feasible sets. The definitions of two-quality inverse demand, contingent strategies, and nodewise optimality are reusable for related channel games. The goal and milestones here are draft statements, without machine-checked proofs of their economic conclusions.

Central difficulty

The manufacturer chooses quality and wholesale price before the retailer's order, yet the direct quantity is chosen only after that order. Consequently, the retailer's payoff depends on the manufacturer's continuation response, and the first-stage choice must account for both later decisions. The reduced profit also changes at t=1t=1t=1, where the higher-quality channel switches. A calculation for one regime alone does not establish the full-game claim. The strict qM>0q_M>0qM​>0 region matters: its boundary represents no encroachment and supports a different alternative in Lemma 2 (Ha, Long and Nasiry, p. 36).

Formalization scope

Lean uses real wholesale prices and qualities, positive uuu and ttt, and nonnegative quantities. Wholesale price has no sign restriction in the manuscript. The market has unit size and the retailer's selling cost is zero. The two inverse-demand expressions are applied to all nonnegative quantities, following the paper's algebraic game model. A profile contains a stage-one action, a retailer order rule for every observed (w,u,t)(w,u,t)(w,u,t), and a direct-quantity rule for every observed (w,u,t,qR)(w,u,t,q_R)(w,u,t,qR​). Subgame perfection requires feasible best replies at every such history, including histories off the equilibrium path. Fixed cost is max⁡{ku2,k(tu)2}\max\{ku^2,k(tu)^2\}max{ku2,k(tu)2}, paid once, while cqMcq_McqM​ is a per-unit selling cost.

The reduced profits ΠHi\Pi_{\mathrm{Hi}}ΠHi​ and ΠLo\Pi_{\mathrm{Lo}}ΠLo​ are used only on their respective open encroachment-feasible domains, where the displayed denominators are positive. Claim 3 is stated for a joint maximizer in (t,u)(t,u)(t,u); keeping uuu fixed while moving to t=1t=1t=1 can leave that feasible set. Lemma 2 excludes the no-encroachment boundary in its Lean statement. Neither reduced profit replaces the full-game payoff in the goal. Contributions that connect the subgame formulas to arbitrary equilibrium profiles, prove the sign inequality, or establish the two optimization results are within scope (Ha, Long and Nasiry, pp. 36–37).

Selected references

  • A. Ha, X. Long and J. Nasiry, Quality in Supply Chain Encroachment, authors' manuscript, SSRN 3970373, published in Manufacturing & Service Operations Management 18(2), 2016. Manuscript. Journal DOI.
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Numerical AnalysisOptimization·Captain: mikedeng1

Error Bounds, Quadratic Growth, and Linear Convergence of Proximal Methods IV: For Prox-Regular Compositions h∘c, Subregularity of the Subdifferential and of the Prox-Gradient Map CoincideResearch Paper

Motivation

Linear convergence of first-order methods is usually proved through an error bound: near a solution, the distance to the solution set is controlled by the size of a computable residual, such as the length of a proximal-gradient step. For the prox-linear method, which minimizes a composition h(c(x))h(c(x))h(c(x)) of a nonsmooth outer function hhh with a smooth map ccc by repeatedly solving the subproblem obtained from linearizing ccc, Drusvyatskiy and Lewis showed in §5 of their paper (arXiv:1602.06661, Theorem 5.10) that the error bound is equivalent to subregularity of the subdifferential ∂φ\partial\varphi∂φ, a property of the objective alone and closely tied to quadratic growth. That result needs hhh convex and finite-valued.

Many composite models violate both assumptions: constraints enter as indicator functions (h=+∞h=+\inftyh=+∞ off a set), and outer functions such as truncated or concave-composite penalties are nonconvex. §8 of the paper extends the equivalence to closed, extended-real-valued, prox-regular hhh. This mission formalizes that extension (Theorem 8.11) together with the results of §8 its proof rests on.

Setting

Fix a C1C^1C1-smooth map c:Rn→Rmc:\mathbb R^n\to\mathbb R^mc:Rn→Rm and a closed (lower semicontinuous) function h:Rm→R‾=R∪{±∞}h:\mathbb R^m\to\overline{\mathbb R}=\mathbb R\cup\{\pm\infty\}h:Rm→R=R∪{±∞}, and consider

min⁡x φ(x)=h(c(x)).(8.2)\min_x\ \varphi(x)=h(c(x)).\qquad(8.2)xmin​ φ(x)=h(c(x)).(8.2)

The linearized function is φ(x;y)=h(c(x)+∇c(x)(y−x))\varphi(x;y)=h\big(c(x)+\nabla c(x)(y-x)\big)φ(x;y)=h(c(x)+∇c(x)(y−x)) and, for t>0t>0t>0, φt(x;y)=φ(x;y)+12t∥x−y∥2\varphi_t(x;y)=\varphi(x;y)+\frac1{2t}\|x-y\|^2φt​(x;y)=φ(x;y)+2t1​∥x−y∥2.

Subgradients are built in three layers (Definition 8.1). A vector vvv is a proximal subgradient of fff at xˉ\bar xxˉ (f(xˉ)f(\bar x)f(xˉ) finite) if f(x)≥f(xˉ)+⟨v,x−xˉ⟩−r2∥x−xˉ∥2f(x)\ge f(\bar x)+\langle v,x-\bar x\rangle-\frac r2\|x-\bar x\|^2f(x)≥f(xˉ)+⟨v,x−xˉ⟩−2r​∥x−xˉ∥2 for some r>0r>0r>0 and all xxx near xˉ\bar xxˉ. The limiting subdifferential ∂f(xˉ)\partial f(\bar x)∂f(xˉ) collects limits of proximal subgradients vi∈∂pf(xi)v_i\in\partial_pf(x_i)vi​∈∂p​f(xi​) with (xi,f(xi),vi)→(xˉ,f(xˉ),v)(x_i,f(x_i),v_i)\to(\bar x,f(\bar x),v)(xi​,f(xi​),vi​)→(xˉ,f(xˉ),v); xˉ\bar xxˉ is stationary if 0∈∂f(xˉ)0\in\partial f(\bar x)0∈∂f(xˉ). The horizon subdifferential ∂∞f(xˉ)\partial^\infty f(\bar x)∂∞f(xˉ) collects limits of tivit_iv_iti​vi​ with vi∈∂f(xi)v_i\in\partial f(x_i)vi​∈∂f(xi​), ti↘0t_i\searrow0ti​↘0, (xi,f(xi))→(xˉ,f(xˉ))(x_i,f(x_i))\to(\bar x,f(\bar x))(xi​,f(xi​))→(xˉ,f(xˉ)).

The map ccc is transverse to hhh at xˉ\bar xxˉ, written c⋔xˉhc\pitchfork_{\bar x}hc⋔xˉ​h, if ∂∞h(c(xˉ))∩Null⁡(∇c(xˉ)∗)={0}\partial^\infty h(c(\bar x))\cap\operatorname{Null}(\nabla c(\bar x)^*)=\{0\}∂∞h(c(xˉ))∩Null(∇c(xˉ)∗)={0} (8.3). The stationary point map St(x)\mathcal S_t(x)St​(x) is the set of stationary points of φt(x;⋅)\varphi_t(x;\cdot)φt​(x;⋅), and the prox-gradient mapping is Gt(x)=t−1(x−St(x))\mathcal G_t(x)=t^{-1}(x-\mathcal S_t(x))Gt​(x)=t−1(x−St​(x)); both are set-valued.

A set-valued map FFF is subregular at (xˉ,yˉ)∈gph⁡F(\bar x,\bar y)\in\operatorname{gph}F(xˉ,yˉ​)∈gphF with constant l>0l>0l>0 if dist⁡(x;F−1(yˉ))≤ldist⁡(yˉ;F(x))\operatorname{dist}(x;F^{-1}(\bar y))\le l\operatorname{dist}(\bar y;F(x))dist(x;F−1(yˉ​))≤ldist(yˉ​;F(x)) for xxx near xˉ\bar xxˉ (Definition 5.7), and metrically regular around (xˉ,yˉ)(\bar x,\bar y)(xˉ,yˉ​) if the same holds with yˉ\bar yyˉ​ replaced by every yyy near yˉ\bar yyˉ​ (Definition 8.3). A closed fff is prox-regular at xˉ\bar xxˉ for vˉ∈∂f(xˉ)\bar v\in\partial f(\bar x)vˉ∈∂f(xˉ) if the quadratic minorant f(y)≥f(x)+⟨v,y−x⟩−r2∥y−x∥2f(y)\ge f(x)+\langle v,y-x\rangle-\frac r2\|y-x\|^2f(y)≥f(x)+⟨v,y−x⟩−2r​∥y−x∥2 holds uniformly for x,yx,yx,y near xˉ\bar xxˉ with f(x)f(x)f(x) near f(xˉ)f(\bar x)f(xˉ) and v∈∂f(x)v\in\partial f(x)v∈∂f(x) near vˉ\bar vvˉ (Definition 8.7). Finally, a φ\varphiφ-attentive localization of ∂φ\partial\varphi∂φ around (xˉ,0)(\bar x,0)(xˉ,0) is a map WWW agreeing with ∂φ(x)\partial\varphi(x)∂φ(x) near 000 whenever xxx is near xˉ\bar xxˉ and φ(x)\varphi(x)φ(x) is near φ(xˉ)\varphi(\bar x)φ(xˉ); a φ(⋅,⋅)\varphi(\cdot,\cdot)φ(⋅,⋅)-attentive localization of St\mathcal S_tSt​ agrees with St(x)\mathcal S_t(x)St​(x) at points yyy near xˉ\bar xxˉ with φ(x;y)\varphi(x;y)φ(x;y) near φ(xˉ)\varphi(\bar x)φ(xˉ), and one of Gt\mathcal G_tGt​ has the form t−1(I−W^)t^{-1}(I-\widehat W)t−1(I−W) with W^\widehat WW such a localization of St\mathcal S_tSt​ (Definition 8.10).

Formalization targets

Goal: Theorem 8.11 (p. 31)

Assume c⋔xˉhc\pitchfork_{\bar x}hc⋔xˉ​h, 0∈∂φ(xˉ)0\in\partial\varphi(\bar x)0∈∂φ(xˉ), ∇c\nabla c∇c Lipschitz around xˉ\bar xxˉ, and hhh prox-regular at c(xˉ)c(\bar x)c(xˉ) for every w∈∂h(c(xˉ))w\in\partial h(c(\bar x))w∈∂h(c(xˉ)) with ∇c(xˉ)∗w=0\nabla c(\bar x)^*w=0∇c(xˉ)∗w=0. Let (i) be "some φ\varphiφ-attentive localization of ∂φ\partial\varphi∂φ is subregular at (xˉ,0)(\bar x,0)(xˉ,0)" and (ii) "some φ(⋅,⋅)\varphi(\cdot,\cdot)φ(⋅,⋅)-attentive localization of Gt\mathcal G_tGt​ is subregular at (xˉ,0)(\bar x,0)(xˉ,0)". Then

(i)⇒(ii) for all t>0,∃ tˉ>0: (ii)⇒(i) for all t∈(0,tˉ),\text{(i)}\Rightarrow\text{(ii) for all }t>0,\qquad \exists\,\bar t>0:\ \text{(ii)}\Rightarrow\text{(i) for all }t\in(0,\bar t),(i)⇒(ii) for all t>0,∃tˉ>0: (ii)⇒(i) for all t∈(0,tˉ),

and, when hhh is convex, ∂φ\partial\varphi∂φ is subregular at (xˉ,0)(\bar x,0)(xˉ,0) if and only if Gt\mathcal G_tGt​ is, for every t>0t>0t>0. The constants of subregularity are left existential: the goal asserts the shape of the equivalence, not a particular constant.

Milestones

  1. Theorem 8.4 (p. 26): metric regularity of a closed set-valued map is preserved, with uniform constants, under affine perturbations HHH with small ∥∇H∥\|\nabla H\|∥∇H∥.
  2. Corollary 8.5 (p. 26): a constraint system F(x)∈QF(x)\in QF(x)∈Q transverse at xˉ\bar xxˉ is uniformly metrically regular under small affine perturbations.
  3. Theorem 8.6 (p. 27): the comparison inequalities between φ(y)\varphi(y)φ(y) and φ(x;⋅)\varphi(x;\cdot)φ(x;⋅) after moving yyy by O(∥y−x∥2)O(\|y-x\|^2)O(∥y−x∥2).
  4. Proposition 8.8 (p. 28): the linearized maps inherit transversality, and φ(x;⋅)\varphi(x;\cdot)φ(x;⋅) is prox-regular at xˉ\bar xxˉ uniformly in xxx (8.4).
  5. Theorem 8.9 (p. 29): every stationary point xtx^txt of the subproblem lies near a point x^\hat xx^ that is nearly stationary for φ\varphiφ, with dist⁡(0;∂φ(x^))≤(a+b/t)∥xt−x∥\operatorname{dist}(0;\partial\varphi(\hat x))\le(a+b/t)\|x^t-x\|dist(0;∂φ(x^))≤(a+b/t)∥xt−x∥.

Significance

Subregularity of Gt\mathcal G_tGt​ at (xˉ,0)(\bar x,0)(xˉ,0) is exactly the error bound property of the prox-linear step, the hypothesis under which linear convergence arguments run. Theorem 8.11 says that, for the attentive parts of the graphs, this property is equivalent to subregularity of ∂φ\partial\varphi∂φ, which does not refer to any algorithm or step size. It therefore covers constrained composite problems (indicator functions hhh), nonconvex prox-regular penalties, and, in the convex case, removes the finite-valuedness assumption of Theorem 5.10.

The results are proved in the paper, partly by citation to Dontchev, Lewis and Rockafellar and to Lewis and Wright's analysis of prox-linear subproblems (arXiv:0812.0423). None of them is formalized: Mathlib has no proximal, limiting or horizon subdifferential, no metric regularity, and no prox-regularity. A formalization supplies these notions, checks the constant-chasing in Theorems 8.9 and 8.11, and fixes the precise quantifier order the prose leaves implicit.

Difficulty

The obvious route, copying the §5 argument, fails at its first step: §5 starts from the inequalities ∣φ(y)−φ(x;y)∣≤Lβ2∥x−y∥2|\varphi(y)-\varphi(x;y)|\le\frac{L\beta}2\|x-y\|^2∣φ(y)−φ(x;y)∣≤2Lβ​∥x−y∥2, and when hhh takes the value +∞+\infty+∞ one of φ(y)\varphi(y)φ(y), φ(x;y)\varphi(x;y)φ(x;y) can be finite while the other is infinite, so no such inequality holds. Theorem 8.6 replaces it by a comparison after perturbing yyy, which needs the stability of metric regularity (Theorem 8.4) and the epigraphical description of subgradients. A second obstacle is that St\mathcal S_tSt​ collects stationary points of nonconvex subproblems, so it is set-valued and possibly empty; the proofs need prox-regularity that is uniform over the family φ(x;⋅)\varphi(x;\cdot)φ(x;⋅) (Proposition 8.8) and a local existence result for St\mathcal S_tSt​ to obtain the threshold tˉ\bar ttˉ. The limiting-subdifferential calculus (the chain rule ∂φ(xˉ)⊆∇c(xˉ)∗∂h(c(xˉ))\partial\varphi(\bar x)\subseteq\nabla c(\bar x)^*\partial h(c(\bar x))∂φ(xˉ)⊆∇c(xˉ)∗∂h(c(xˉ)) under transversality) is itself a substantial piece of variational analysis.

Formalization scope

Points are in EuclideanSpace ℝ (Fin n); hhh, φ\varphiφ, φ(x;⋅)\varphi(x;\cdot)φ(x;⋅) and φt(x;⋅)\varphi_t(x;\cdot)φt​(x;⋅) are EReal-valued. Standing assumptions on every statement: ccc is C1C^1C1 (ContDiff ℝ 1 c), hhh is lower semicontinuous and never −∞-\infty−∞ (the page's closed functions are only ever evaluated where finite or +∞+\infty+∞; this is a disclosed addition). ∇c(x)\nabla c(x)∇c(x) is fderiv ℝ c x and ∇c(x)∗\nabla c(x)^*∇c(x)∗ its adjoint. "∣a−φ(xˉ)∣<ϵ|a-\varphi(\bar x)|<\epsilon∣a−φ(xˉ)∣<ϵ" requires aaa finite. dist⁡(yˉ;∅)=+∞\operatorname{dist}(\bar y;\varnothing)=+\inftydist(yˉ​;∅)=+∞, so (sub)regularity inequalities are stated for every element of F(x)F(x)F(x), and metric regularity carries nonemptiness of F−1(y)F^{-1}(y)F−1(y); dist⁡(0;∂φ(x^))≤r\operatorname{dist}(0;\partial\varphi(\hat x))\le rdist(0;∂φ(x^))≤r is the existence of a subgradient of norm at most rrr. St\mathcal S_tSt​ and Gt\mathcal G_tGt​ are sets defined by stationarity, never a chosen minimizer. Two printed slips are corrected and disclosed: in Definition 8.10 (2) the neighbourhood Y\mathcal YY is a neighbourhood of xˉ\bar xxˉ, and in Theorem 8.11 the threshold satisfies tˉ>0\bar t>0tˉ>0 (with tˉ=0\bar t=0tˉ=0 the converse would be vacuous). "When hhh is convex" is the convexity inequality in R‾\overline{\mathbb R}R, with the theorem's other hypotheses kept.

A trivializing formalization is ruled out: subregularity always includes 0∈F(xˉ)0\in F(\bar x)0∈F(xˉ), a constant l>0l>0l>0 and a neighbourhood, so the content of (i) and (ii) cannot collapse into the trivial existence of a localization (any map is a localization of itself); and distances to empty sets are never junk zeros.

A complete development needs the three subdifferentials and their basic calculus (sum rule with a smooth function, chain rule under transversality, closedness of the limiting subdifferential), metric regularity and its perturbation stability, Ekeland's variational principle (on the platform as EkelandVP.General.ekeland_variational_principle), and a local existence result for stationary points of the subproblems. The subdifferential and regularity layer is reusable well beyond this mission. Proofs of any milestone, and of supporting lemmas on the variational-analysis substrate, are welcome.

Selected references

  • D. Drusvyatskiy and A. S. Lewis, Error bounds, quadratic growth, and linear convergence of proximal methods, Math. Oper. Res. 43(3), 2018; arXiv:1602.06661v2. https://arxiv.org/abs/1602.06661
  • A. L. Dontchev, A. S. Lewis and R. T. Rockafellar, The radius of metric regularity, Trans. Amer. Math. Soc. 355(2), 2003. https://doi.org/10.1090/S0002-9947-02-03088-X
  • A. S. Lewis and S. J. Wright, A proximal method for composite minimization, Math. Program. 158, 2016. https://arxiv.org/abs/0812.0423
  • R. A. Poliquin and R. T. Rockafellar, Prox-regular functions in variational analysis, Trans. Amer. Math. Soc. 348(5), 1996. https://doi.org/10.1090/S0002-9947-96-01544-9
  • R. T. Rockafellar and R. J.-B. Wets, Variational Analysis, Grundlehren 317, Springer, 1998. https://doi.org/10.1007/978-3-642-02431-3
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Optimal TransportProbabilityStatistics·Captain: mikedeng1

On the Rate of Convergence in Wasserstein Distance of the Empirical Measure II: Concentration Inequalities for T_p(μ_N, μ) under Exponential or Polynomial Moments (Theorem 2)Research Paper

Motivation

Approximating an unknown probability measure μ\muμ by the empirical measure μN=1N∑k=1NδXk\mu_N=\frac1N\sum_{k=1}^N\delta_{X_k}μN​=N1​∑k=1N​δXk​​ of an i.i.d. sample is the basic operation of statistics, Monte Carlo integration, quantization and particle approximations of nonlinear PDEs. The natural way to compare μN\mu_NμN​ with μ\muμ on Rd\mathbb R^dRd is an optimal-transport cost, because it metrizes weak convergence together with convergence of moments. For many applications the mean of this cost is not enough: one needs to know how unlikely a large deviation is, for a fixed sample size NNN.

The main consumer in operations research is data-driven distributionally robust optimization. Mohajerin Esfahani and Kuhn (Math. Program. 171, 2018) build Wasserstein balls around μN\mu_NμN​ whose radius is calibrated so that the true distribution lies inside with probability 1−β1-\beta1−β; their finite-sample guarantee (their inequality (7), quoted from this paper for p=1p=1p=1) is exactly a concentration inequality of the kind proved here. On Prove2Me that inequality appears as the hypothesis Concentration7 of WassDDRO.Consistency.Setting; Theorem 2 of this mission is the statement that discharges it.

Timeline. Bolley, Guillin and Villani (PTRF 137, 2007) proved concentration inequalities for Tp(μN,μ)\mathcal T_p(\mu_N,\mu)Tp​(μN​,μ) on non-compact spaces, under assumptions that often included functional inequalities for μ\muμ, and for rather large deviations. Boissard (Electron. J. Probab. 16, 2011) gave bounds in T1\mathcal T_1T1​ for empirical and occupation measures. Boissard and Le Gouic (arXiv:1105.5263) and Dereich, Scheutzow and Schottstedt (Ann. IHP 49, 2013) studied the mean speed of convergence; the latter introduced the multiscale bound used here and obtained sharp moment estimates for a limited range of parameters. Fournier and Guillin (arXiv:1312.2128, 2013; PTRF 162, 2015) gave moment bounds for all p>0p>0p>0 and d≥1d\ge1d≥1 under a qqq-th moment (their Theorem 1, mission I of this series) and the concentration inequalities of their Theorem 2, the subject of this mission, under integrability conditions only.

Setting

Fix d≥1d\ge1d≥1 and give Rd\mathbb R^dRd the Euclidean norm ∣x∣|x|∣x∣. Let μ\muμ be a Borel probability measure on Rd\mathbb R^dRd and X1,…,XNX_1,\dots,X_NX1​,…,XN​ i.i.d. with law μ\muμ. For p>0p>0p>0 the transport cost between probability measures μ,ν\mu,\nuμ,ν is

Tp(μ,ν)=inf⁡{∫∣x−y∣p ξ(dx,dy): ξ∈H(μ,ν)},\mathcal T_p(\mu,\nu)=\inf\Big\{\int|x-y|^p\,\xi(dx,dy):\ \xi\in\mathcal H(\mu,\nu)\Big\},Tp​(μ,ν)=inf{∫∣x−y∣pξ(dx,dy): ξ∈H(μ,ν)},

where H(μ,ν)\mathcal H(\mu,\nu)H(μ,ν) is the set of couplings, measures on Rd×Rd\mathbb R^d\times\mathbb R^dRd×Rd with marginals μ\muμ and ν\nuν (no 1/p1/p1/p root is taken). The moment conditions use

Mq(μ)=∫∣x∣q μ(dx),Eα,γ(μ)=∫eγ∣x∣α μ(dx).M_q(\mu)=\int|x|^q\,\mu(dx),\qquad \mathcal E_{\alpha,\gamma}(\mu)=\int e^{\gamma|x|^\alpha}\,\mu(dx).Mq​(μ)=∫∣x∣qμ(dx),Eα,γ​(μ)=∫eγ∣x∣αμ(dx).

The proof works with a multiscale distance Dp\mathcal D_pDp​. For ℓ≥0\ell\ge0ℓ≥0 let Pℓ\mathcal P_\ellPℓ​ be the partition of (−1,1]d(-1,1]^d(−1,1]d into 2dℓ2^{d\ell}2dℓ dyadic cubes of side 21−ℓ2^{1-\ell}21−ℓ. For measures on (−1,1]d(-1,1]^d(−1,1]d,

Dp(μ,ν)=2p−12∑ℓ≥12−pℓ∑F∈Pℓ∣μ(F)−ν(F)∣.\mathcal D_p(\mu,\nu)=\frac{2^p-1}{2}\sum_{\ell\ge1}2^{-p\ell}\sum_{F\in\mathcal P_\ell}|\mu(F)-\nu(F)|.Dp​(μ,ν)=22p−1​ℓ≥1∑​2−pℓF∈Pℓ​∑​∣μ(F)−ν(F)∣.

For measures on Rd\mathbb R^dRd one cuts space into the shells B0=(−1,1]dB_0=(-1,1]^dB0​=(−1,1]d, Bn=(−2n,2n]d∖(−2n−1,2n−1]dB_n=(-2^n,2^n]^d\setminus(-2^{n-1},2^{n-1}]^dBn​=(−2n,2n]d∖(−2n−1,2n−1]d, rescales each to (−1,1]d(-1,1]^d(−1,1]d (the measure RBnμ\mathcal R_{B_n}\muRBn​​μ), and sums the compact distances with weights 2pn2^{pn}2pn. Lemma 5 bounds Tp\mathcal T_pTp​ by κp,dDp\kappa_{p,d}\mathcal D_pκp,d​Dp​. The splitting Dp(μN,μ)≤ZNp+VNp\mathcal D_p(\mu_N,\mu)\le Z^p_N+V^p_NDp​(μN​,μ)≤ZNp​+VNp​ separates the fluctuation of the shell masses, ZNp=∑n2pn∣μN(Bn)−μ(Bn)∣Z^p_N=\sum_n2^{pn}|\mu_N(B_n)-\mu(B_n)|ZNp​=∑n​2pn∣μN​(Bn​)−μ(Bn​)∣, from the fluctuation inside the shells, VNp=∑n2pnμ(Bn)Dp(RBnμN,RBnμ)V^p_N=\sum_n2^{pn}\mu(B_n)\mathcal D_p(\mathcal R_{B_n}\mu_N,\mathcal R_{B_n}\mu)VNp​=∑n​2pnμ(Bn​)Dp​(RBn​​μN​,RBn​​μ). A Poisson measure ΠN\Pi_NΠN​ with intensity NμN\muNμ (a Poisson(NNN) number of i.i.d. μ\muμ points) and f(x)=(1+x)log⁡(1+x)−xf(x)=(1+x)\log(1+x)-xf(x)=(1+x)log(1+x)−x enter the compact case.

Formalization targets

Goal: Theorem 2 (p. 3)

Assume p≥d/2p\ge d/2p≥d/2 or p≥1p\ge1p≥1, and one of (1) Eα,γ(μ)<∞\mathcal E_{\alpha,\gamma}(\mu)<\inftyEα,γ​(μ)<∞ with α>p\alpha>pα>p; (2) Eα,γ(μ)<∞\mathcal E_{\alpha,\gamma}(\mu)<\inftyEα,γ​(μ)<∞ with α∈(0,p)\alpha\in(0,p)α∈(0,p); (3) Mq(μ)<∞M_q(\mu)<\inftyMq​(μ)<∞ with q>2pq>2pq>2p. Then for all N≥1N\ge1N≥1, x>0x>0x>0,

P(Tp(μN,μ)≥x)≤a(N,x)1{x≤1}+b(N,x),\mathbb P\big(\mathcal T_p(\mu_N,\mu)\ge x\big)\le a(N,x)\mathbf 1_{\{x\le1\}}+b(N,x),P(Tp​(μN​,μ)≥x)≤a(N,x)1{x≤1}​+b(N,x),

with a(N,x)=Ce−cNx2a(N,x)=Ce^{-cNx^2}a(N,x)=Ce−cNx2, Ce−cN(x/log⁡(2+1/x))2Ce^{-cN(x/\log(2+1/x))^2}Ce−cN(x/log(2+1/x))2 or Ce−cNxd/pCe^{-cNx^{d/p}}Ce−cNxd/p according as p>d/2p>d/2p>d/2, p=d/2p=d/2p=d/2, p∈[1,d/2)p\in[1,d/2)p∈[1,d/2), and b(N,x)=Ce−cNxα/p1{x>1}b(N,x)=Ce^{-cNx^{\alpha/p}}\mathbf 1_{\{x>1\}}b(N,x)=Ce−cNxα/p1{x>1}​ under (1), Ce−c(Nx)(α−ε)/p1{x≤1}+Ce−c(Nx)α/p1{x>1}C e^{-c(Nx)^{(\alpha-\varepsilon)/p}}\mathbf 1_{\{x\le1\}}+Ce^{-c(Nx)^{\alpha/p}}\mathbf 1_{\{x>1\}}Ce−c(Nx)(α−ε)/p1{x≤1}​+Ce−c(Nx)α/p1{x>1}​ under (2), CN(Nx)−(q−ε)/pCN(Nx)^{-(q-\varepsilon)/p}CN(Nx)−(q−ε)/p under (3). The constants C,c>0C,c>0C,c>0 depend only on p,dp,dp,d, the parameters of the condition, the value of the moment and ε\varepsilonε.

Milestones

In attack order: Lemma 5 (the coupling bound Tp≤κp,dDp\mathcal T_p\le\kappa_{p,d}\mathcal D_pTp​≤κp,d​Dp​); Lemma 9 (Poisson moment generating function and tails); Proposition 8 (concentration for ΠN(Rd)Dp(ΨN,μ)\Pi_N(\mathbb R^d)\mathcal D_p(\Psi_N,\mu)ΠN​(Rd)Dp​(ΨN​,μ) in the Poissonized compact case); Lemma 11 (P[Poisson(N)=N+k]≥e−2N−1/2/2\mathbb P[\mathrm{Poisson}(N)=N+k]\ge e^{-2}N^{-1/2}/\sqrt2P[Poisson(N)=N+k]≥e−2N−1/2/2​ for k≤⌊N⌋k\le\lfloor\sqrt N\rfloork≤⌊N​⌋); Proposition 10 (the compact case of Theorem 2, P[Dp(μN,μ)≥x]≤1{x≤1}a(N,x)\mathbb P[\mathcal D_p(\mu_N,\mu)\ge x]\le\mathbf 1_{\{x\le1\}}a(N,x)P[Dp​(μN​,μ)≥x]≤1{x≤1}​a(N,x)); Lemma 12 (binomial deviations); Lemma 13 (the tail of ZNpZ^p_NZNp​); display (6) (P[VNp≥x/(2κp,d)]≤a(N,x)1{x≤A}\mathbb P[V^p_N\ge x/(2\kappa_{p,d})]\le a(N,x)\mathbf 1_{\{x\le A\}}P[VNp​≥x/(2κp,d​)]≤a(N,x)1{x≤A}​).

Significance

The result. Theorem 2 gives, for every dimension and every ppp in its range, a deviation inequality whose small-xxx part a(N,x)a(N,x)a(N,x) has the same dimension-dependent exponent as the mean rate of Theorem 1, and whose large-xxx part b(N,x)b(N,x)b(N,x) is governed only by the tail of μ\muμ. Under exponential moments the tail is again exponential; under a polynomial moment it is polynomial, which is the correct order. It is the input for finite-sample confidence radii in Wasserstein DRO, for non-asymptotic guarantees in quantization and for propagation-of-chaos estimates.

Formalizing it. The theorem is proved (2013, published 2015) and widely cited; no machine-checked proof of it, or of any rate for the empirical measure in transport cost, exists in Mathlib or on Prove2Me. The work is formalizing the known proof: Poisson and binomial concentration (Lemmas 9, 12), the local Poisson bound (Lemma 11), Poissonization and depoissonization (Propositions 8, 10), and the shell decomposition (Lemma 13, display (6)). Lemmas 9, 11 and 12 are general probability facts useful well beyond this paper.

Difficulty

The obvious route is a bounded-differences (McDiarmid) inequality for ω↦Tp(μN,μ)\omega\mapsto\mathcal T_p(\mu_N,\mu)ω↦Tp​(μN​,μ). On Rd\mathbb R^dRd it is not available: moving a single sample point changes the cost by an amount that is unbounded, and the measures allowed here have only exponential or polynomial moments. Even on a compact set it bounds the deviation from the mean rather than from 000, so it gives nothing below the mean rate, and it does not see the dimension-dependent exponent xd/px^{d/p}xd/p of a(N,x)a(N,x)a(N,x). The bound must hold at all scales of the dyadic decomposition simultaneously, while the cell counts of a multinomial sample are dependent, and in the non-compact case the masses of far-away shells, which are rare events, must be controlled with a tail that degrades exactly as the moment condition allows.

Formalization scope

Rd\mathbb R^dRd is EuclideanSpace ℝ (Fin d) with d≥1d\ge1d≥1; the Euclidean norm matters, since κp,d\kappa_{p,d}κp,d​ involves the diameter of (−1,1]d(-1,1]^d(−1,1]d. The sample is ω:Fin N→Rd\omega:\mathrm{Fin}\,N\to\mathbb R^dω:FinN→Rd under the product measure μ⊗N\mu^{\otimes N}μ⊗N, and μN\mu_NμN​ is the published WassersteinDRO.Duality.empiricalDistribution; couplings are the published WassersteinLinOpt.Ball.couplings. Costs, moments, Dp\mathcal D_pDp​, ZNpZ^p_NZNp​, VNpV^p_NVNp​ and expectations are valued in [0,∞][0,\infty][0,∞] (lower Lebesgue integrals and [0,∞][0,\infty][0,∞]-valued series), so no bound can hold through a junk value of a divergent integral. Probabilities are the product measure applied to the event. ΠN\Pi_NΠN​ is represented by its law, a Poisson(NNN) mixture of i.i.d. samples, as on p. 13. Poisson and binomial laws are Mathlib's poissonMeasure and binomial.

Constants: in each of the three parts, the condition's parameters, the moment value Eα,γ(μ)=E0\mathcal E_{\alpha,\gamma}(\mu)=E_0Eα,γ​(μ)=E0​ (resp. Mq(μ)=M0M_q(\mu)=M_0Mq​(μ)=M0​) and ε\varepsilonε are fixed before ∃ C,c\exists\,C,c∃C,c, and μ,N,x\mu,N,xμ,N,x come after. A formalization with μ\muμ fixed before the constants would be trivial (the constants could absorb μ\muμ), and one stating the goal as the sum of the bounds for ZNpZ^p_NZNp​ and VNpV^p_NVNp​ would assume the proof; the goal mentions neither Dp\mathcal D_pDp​, ΠN\Pi_NΠN​, ZNpZ^p_NZNp​ nor VNpV^p_NVNp​.

Departures from the print, each disclosed in the statements: the page writes Tp(μN,μ)\mathcal T_p(\mu^N,\mu)Tp​(μN,μ) for Tp(μN,μ)\mathcal T_p(\mu_N,\mu)Tp​(μN​,μ); Theorem 2 opens with "p>0p>0p>0" but prints a(N,x)a(N,x)a(N,x) only for p>d/2p>d/2p>d/2, p=d/2p=d/2p=d/2, p∈[1,d/2)p\in[1,d/2)p∈[1,d/2), so it is posed for p≥d/2p\ge d/2p≥d/2 or p≥1p\ge1p≥1; Proposition 8's "p≥1p\ge1p≥1" is relaxed to that range (its proof does not use p≥1p\ge1p≥1, and Theorem 2 needs it for every p>d/2p>d/2p>d/2) (Proposition 10 is posed, as printed, for every p>0p>0p>0); Lemma 12 assumes N≥1N\ge1N≥1 and a positive success probability, without which (a) and (b) are false. "Supported in (−1,1]d(-1,1]^d(−1,1]d" is μ\muμ-null complement of B0B_0B0​.

The definitions of Tp\mathcal T_pTp​, MqM_qMq​, Notation 4 and Lemma 5 duplicate those of mission I of the series and are to be merged later. Contributions on Poisson and binomial concentration, and on transport costs between discrete measures, are reusable and welcome.

Selected references

  • N. Fournier, A. Guillin, On the rate of convergence in Wasserstein distance of the empirical measure, arXiv:1312.2128v1, 2013; Probab. Theory Relat. Fields 162 (2015) 707–738. https://arxiv.org/abs/1312.2128
  • S. Dereich, M. Scheutzow, R. Schottstedt, Constructive quantization: approximation by empirical measures, Ann. Inst. H. Poincaré Probab. Statist. 49 (2013) 1183–1203. https://doi.org/10.1214/12-AIHP489
  • F. Bolley, A. Guillin, C. Villani, Quantitative concentration inequalities for empirical measures on non-compact spaces, Probab. Theory Relat. Fields 137 (2007) 541–593. https://doi.org/10.1007/s00440-006-0004-7
  • E. Boissard, T. Le Gouic, On the mean speed of convergence of empirical and occupation measures in Wasserstein distance, preprint, 2011. https://arxiv.org/abs/1105.5263
  • P. Mohajerin Esfahani, D. Kuhn, Data-driven distributionally robust optimization using the Wasserstein metric, Math. Program. 171 (2018) 115–166. https://doi.org/10.1007/s10107-017-1172-1
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Quality in Supply Chain Encroachment II: Under Quality Differentiation the Direct Channel Carries the High-Quality Product, the Manufacturer Gains and the Retailer LosesResearch Paper

Motivation

Manufacturers increasingly sell directly to consumers while continuing to supply independent retailers, a practice known as supply chain encroachment. The direct channel competes with the retailer for the same consumers, and the conventional advice for easing that conflict is to sell different products in the two channels. Ha, Long and Nasiry (MSOM 18(2), 2016; authors' manuscript SSRN 3970373) study this advice in a model where the manufacturer chooses product quality herself. This mission formalizes their Section 5: when the manufacturer may offer one quality directly and another through the retailer, which channel gets the better product, when is differentiation worth it, and who gains from encroachment.

The model builds on two lines of work. With exogenous quality, Arya, Mittendorf and Sappington (Marketing Science, 2007) showed that encroachment can benefit both firms, through a lower wholesale price. Vertical differentiation with a convex cost of quality goes back to Mussa and Rosen (JET, 1978), Moorthy (1988) and Motta (1993), where differentiation lets firms segment the market. The paper combines the two and finds that, once quality is endogenous, the retailer never gains.

Setting

A market of size 111 consists of consumers with types θ\thetaθ uniformly distributed on [0,1][0,1][0,1]; a consumer of type θ\thetaθ obtains surplus θv−p\theta v-pθv−p from a product of quality vvv at price ppp. A manufacturer sells a product of quality u>0u>0u>0 through her direct channel and a product of quality tututu, with quality ratio t>0t>0t>0, through a retailer. Producing one unit of quality vvv costs kv2kv^2kv2 (k>0k>0k>0); every unit sold directly costs a further direct selling cost c≥0c\ge 0c≥0; the retailer's selling cost is 000.

With quantities qMq_MqM​ (direct) and qRq_RqR​ (retailer), the market-clearing prices are, for t≤1t\le 1t≤1 (direct channel carries the higher quality),

pM=u(1−qM−t qR),pR=tu(1−qM−qR),p_M=u(1-q_M-t\,q_R),\qquad p_R=tu(1-q_M-q_R),pM​=u(1−qM​−tqR​),pR​=tu(1−qM​−qR​),

and for t>1t>1t>1 (retailer carries the higher quality)

pM=u(1−qM−qR),pR=tu(1−qR)−u qM.p_M=u(1-q_M-q_R),\qquad p_R=tu(1-q_R)-u\,q_M .pM​=u(1−qM​−qR​),pR​=tu(1−qR​)−uqM​.

The profits are ΠR=(pR−w)qR\Pi_R=(p_R-w)q_RΠR​=(pR​−w)qR​ and ΠM=(w−k(tu)2)qR+(pM−c−ku2)qM\Pi_M=(w-k(tu)^2)q_R+(p_M-c-ku^2)q_MΠM​=(w−k(tu)2)qR​+(pM​−c−ku2)qM​.

The game has three stages: (i) the manufacturer chooses a wholesale price www, the quality uuu and the ratio ttt; (ii) the retailer orders qR≥0q_R\ge0qR​≥0; (iii) the manufacturer chooses qM≥0q_M\ge0qM​≥0. Solutions are subgame-perfect equilibria. The manufacturer encroaches when qM∗>0q^*_M>0qM∗​>0 on the equilibrium path. Fixing t=1t=1t=1 gives the uniform-quality game of §4.1. The benchmark of §3.2 has no direct channel; its equilibrium profits are ΠMN=154k\Pi^N_M=\frac1{54k}ΠMN​=54k1​ and ΠRN=1108k\Pi^N_R=\frac1{108k}ΠRN​=108k1​.

Formalization targets

Goal: Proposition 4(ii)

In every subgame-perfect equilibrium with qM∗>0q^*_M>0qM∗​>0,

ΠM∗>154k=ΠMNandΠR∗<1108k=ΠRN.\Pi^*_M>\frac{1}{54k}=\Pi^N_M\qquad\text{and}\qquad \Pi^*_R<\frac{1}{108k}=\Pi^N_R .ΠM∗​>54k1​=ΠMN​andΠR∗​<108k1​=ΠRN​.

The statement makes no assumption on which quality the manufacturer chooses, on the size of ccc or on the form of the equilibrium; the constants are the benchmark's.

Milestones

  1. The benchmark equilibrium (uN=13ku^N=\frac1{3k}uN=3k1​, wN=29kw^N=\frac2{9k}wN=9k2​, qRN=16q^N_R=\frac16qRN​=61​ and the two profits), p. 9.
  2. The quantity subgame (7) for t<1t<1t<1, p. 16, and the reduced profit ΠM(t,u)\Pi_M(t,u)ΠM​(t,u) obtained by optimizing www, p. 29.
  3. Lemma 1(i)–(ii): the manufacturer's optimal ratio t(u)t(u)t(u) for given uuu, when the retailer's product is lower (t≤1t\le1t≤1) or higher (t≥1t\ge1t≥1) quality.
  4. Claim 1 and Lemma 1(iii): for c<112kc<\frac1{12k}c<12k1​ the profits of the two kinds of differentiation cross exactly once in uuu.
  5. Proposition 3: under encroachment, t∗≤1t^*\le1t∗≤1.
  6. Proposition 1(iii) in the uniform-quality game.
  7. Claim 2 and Proposition 4(i): thresholds 0<c1<c20<c_1<c_20<c1​<c2​ such that the manufacturer differentiates (t∗<1t^*<1t∗<1) for c<c1c<c_1c<c1​, uses uniform quality for c1<c<c2c_1<c<c_2c1​<c<c2​, and does not encroach for c>c2c>c_2c>c2​.

Companions

The §6.1 benchmark in which both qualities go through the retailer (ΠMN2=150k\Pi^{N2}_M=\frac1{50k}ΠMN2​=50k1​, ΠRN2=1100k\Pi^{N2}_R=\frac1{100k}ΠRN2​=100k1​), Proposition 5 (the win–lose outcome against that benchmark), and the existence of an equilibrium. The threshold milestones assert existence for each cost, so their conclusions have an equilibrium to describe.

Significance

Proposition 4(ii) says that letting the manufacturer differentiate quality across channels does not change who wins: the manufacturer still gains from encroachment and the retailer still loses, although one might expect the retailer to benefit from not facing an identical product. Proposition 3 adds that differentiation, when used, puts the higher quality in the direct channel, and Proposition 4(i) shows that for intermediate selling costs the manufacturer prefers no differentiation at all, contrary to the monopoly intuition that segmentation always pays. Proposition 5 shows the conclusion persists against a benchmark in which the retailer already carries a two-product line.

The results are proved in the paper, in part with numerical verification (e.g. the bounds on u^\hat uu^ in the proof of Proposition 3, and the location of c1c_1c1​ and c2c_2c2​). None of them has been machine-checked. A formal development would turn these numerical steps into proofs and would leave a reusable, explicit model of a three-stage Stackelberg game with a vertically differentiated linear demand.

Difficulty

The equilibrium analysis is not a single concave program. Backward induction produces closed forms only on regions (the retailer's order must leave the manufacturer a positive direct quantity, and the retailer's quantity must stay positive), and the manufacturer's stage-1 problem is a comparison across these regions and across t<1t<1t<1, t=1t=1t=1 and t>1t>1t>1. The profit of low-quality encroachment, ΠML(u)\Pi^L_M(u)ΠML​(u), involves a square root in uuu, and the paper controls its critical points by a case analysis on polynomial derivatives with numerically located crossing points (pp. 39–40). The thresholds c1≈0.0973/kc_1\approx0.0973/kc1​≈0.0973/k and c2≈0.1019/kc_2\approx0.1019/kc2​≈0.1019/k are defined implicitly by the equality of maximized profits. Comparing the equilibrium profit with 154k\frac1{54k}54k1​ therefore requires bounding a maximum taken over a piecewise-defined family, not evaluating one formula.

Formalization scope

The game is defined in QualityEncroach.Differ.Game. Quantities are restricted to be nonnegative; the wholesale price is unrestricted, as in the paper; qualities satisfy u>0u>0u>0, t>0t>0t>0. The price formulas are used for all nonnegative quantities, as in the paper; the t>1t>1t>1 case, which the paper says "can be derived similarly", is that derivation. The equilibrium notion is subgame perfection written in one-shot-deviation form at every history, on and off the path. Benchmark profits appear as the constants 154k\frac1{54k}54k1​, 1108k\frac1{108k}108k1​ (and 150k\frac1{50k}50k1​, 1100k\frac1{100k}100k1​); separate items derive them from the benchmark games. Threshold statements give c2>0c_2>0c2​>0 and 0<c1<c20<c_1<c_20<c1​<c2​ depending only on kkk, assert equilibrium existence at every c≥0c\ge0c≥0, and say nothing at c=c2c=c_2c=c2​, where the paper's statements disagree. Lemma 1 and Claim 1 are stated about the paper's reduced-form profits, defined by the displayed formulas in QualityEncroach.Differ.Reduced; the item reduced_profit_high links ΠM(t,u)\Pi_M(t,u)ΠM​(t,u) for t≤1t\le1t≤1 to the game. Claim 1 retains c=0c=0c=0 and quantifies only over positive qualities, so no reduced form is evaluated at u=0u=0u=0.

The goal is about subgame-perfect equilibria of the game, not about the reduced forms: a proof that only compares closed-form profits does not prove it without the milestones linking those forms to equilibrium play. The goal is not vacuous only if an equilibrium with qM∗>0q^*_M>0qM∗​>0 exists; the companion spe_exists asserts existence.

Contributions are welcome at every level: the benchmark and the quantity subgame are routine calculus on quadratics; Lemma 1(i)–(ii) are one-variable sign analyses; Claim 1, Lemma 1(iii), Proposition 3 and the thresholds require the case analyses of the appendix.

Selected references

  • A. Ha, X. Long, J. Nasiry, Quality in Supply Chain Encroachment, Manufacturing & Service Operations Management 18(2), 2016. https://doi.org/10.1287/msom.2015.0562 (authors' manuscript: https://ssrn.com/abstract=3970373)
  • A. Arya, B. Mittendorf, D. Sappington, The Bright Side of Supplier Encroachment, Marketing Science 26(5), 2007. https://doi.org/10.1287/mksc.1060.0228
  • M. Mussa, S. Rosen, Monopoly and Product Quality, Journal of Economic Theory 18(2), 1978. https://doi.org/10.1016/0022-0531(78)90085-6
  • K. S. Moorthy, Product and Price Competition in a Duopoly, Marketing Science 7(2), 1988. https://doi.org/10.1287/mksc.7.2.141
  • M. Motta, Endogenous Quality Choice: Price vs. Quantity Competition, Journal of Industrial Economics 41(2), 1993. https://doi.org/10.2307/2950430
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A Probabilistic Weak Formulation of Mean Field Games and Applications 2: Under Unique Hamiltonian Maximizers and Lasry–Lions Monotonicity, the Mean Field Game Has at Most One SolutionResearch Paper

Motivation

Mean field games, introduced independently by Lasry and Lions (Mean field games, Jpn. J. Math. 2007) and by Huang, Malhamé and Caines (2006), describe the Nash equilibria of games with a very large number of symmetric players, each of whom reacts only to the empirical distribution of the others. In the limit, an equilibrium is a fixed point: a flow of population laws such that the optimal response of a single representative player to that flow reproduces it.

Existence of such fixed points is typically obtained by compactness, and says nothing about whether the equilibrium is determined by the data. Uniqueness matters for the use of the model: a unique equilibrium can be computed, approximated, and compared across parameters, while multiple equilibria raise a selection problem. Lasry and Lions showed by counterexamples that uniqueness fails in general, and identified a monotonicity condition on the population-dependent part of the reward under which it holds; outside that condition, uniqueness is typically available only for short horizons and Lipschitz coefficients.

Carmona and Lacker (arXiv:1307.1152v2, 2014; Ann. Appl. Probab. 25(3), 2015) set up a weak formulation of mean field games in which the controlled state is obtained from a fixed driftless diffusion by a Girsanov change of measure, so that the coefficients may be merely measurable in the state and path dependent. This mission formalizes their uniqueness theorem (Theorem 3.8): the Lasry–Lions argument carried out in the weak formulation, through backward stochastic differential equations.

Setting

Fix a horizon TTT, a dimension ddd, the path space C=C([0,T];Rd)\mathcal C = C([0,T];\mathbb R^d)C=C([0,T];Rd) with the sup norm, and a measurable ψ:C→[1,∞)\psi:\mathcal C\to[1,\infty)ψ:C→[1,∞). Write Pψ(C)\mathcal P_\psi(\mathcal C)Pψ​(C) for the probability measures μ\muμ on C\mathcal CC with ∫ψ dμ<∞\int\psi\,d\mu<\infty∫ψdμ<∞. A control set AAA is a compact convex subset of a normed space, and P(A)\mathcal P(A)P(A) is the set of probability measures on AAA with the weak topology.

On a probability space (Ω,P)(\Omega,P)(Ω,P) carrying an initial state ξ\xiξ and an independent ddd-dimensional Brownian motion WWW, filtered by the augmented filtration of (ξ,W)(\xi,W)(ξ,W), let XXX solve the driftless state equation dXt=σ(t,X) dWtdX_t=\sigma(t,X)\,dW_tdXt​=σ(t,X)dWt​, X0=ξX_0=\xiX0​=ξ. The admissible controls A\mathbb AA are the progressively measurable AAA-valued processes. For μ∈Pψ(C)\mu\in\mathcal P_\psi(\mathcal C)μ∈Pψ​(C) and α∈A\alpha\in\mathbb Aα∈A the measure Pμ,αP^{\mu,\alpha}Pμ,α has density

dPμ,αdP=E(∫0⋅σ−1b(t,X,μ,αt) dWt)T,\frac{dP^{\mu,\alpha}}{dP}=\mathcal E\Big(\int_0^\cdot\sigma^{-1}b(t,X,\mu,\alpha_t)\,dW_t\Big)_T,dPdPμ,α​=E(∫0⋅​σ−1b(t,X,μ,αt​)dWt​)T​,

under which XXX has drift b(t,X,μ,αt)b(t,X,\mu,\alpha_t)b(t,X,μ,αt​). For a flow q:[0,T]→P(A)q:[0,T]\to\mathcal P(A)q:[0,T]→P(A) the reward is

Jμ,q(α)=Eμ,α[∫0Tf(t,X,μ,qt,αt) dt+g(X,μ)].J^{\mu,q}(\alpha)=E^{\mu,\alpha}\Big[\int_0^T f(t,X,\mu,q_t,\alpha_t)\,dt+g(X,\mu)\Big].Jμ,q(α)=Eμ,α[∫0T​f(t,X,μ,qt​,αt​)dt+g(X,μ)].

A pair (μ,q)(\mu,q)(μ,q) is a solution of the MFG (Definition 3.4) if some α∈A\alpha\in\mathbb Aα∈A maximizes Jμ,qJ^{\mu,q}Jμ,q over A\mathbb AA, Pμ,α∘X−1=μP^{\mu,\alpha}\circ X^{-1}=\muPμ,α∘X−1=μ, and Pμ,α∘αt−1=qtP^{\mu,\alpha}\circ\alpha_t^{-1}=q_tPμ,α∘αt−1​=qt​ for almost every ttt.

The Hamiltonian is h(t,x,μ,q,z,a)=f(t,x,μ,q,a)+z⋅σ−1b(t,x,μ,a)h(t,x,\mu,q,z,a)=f(t,x,\mu,q,a)+z\cdot\sigma^{-1}b(t,x,\mu,a)h(t,x,μ,q,z,a)=f(t,x,μ,q,a)+z⋅σ−1b(t,x,μ,a), with maximum HHH over a∈Aa\in Aa∈A and maximizer set A(t,x,μ,q,z)A(t,x,\mu,q,z)A(t,x,μ,q,z). Assumption (U) asks that (U.1) the maximizer is unique; (U.2) b=b(t,x,a)b=b(t,x,a)b=b(t,x,a) does not depend on μ\muμ; (U.3) f=f1(t,x,μ)+f2(t,μ,q)+f3(t,x,a)f=f_1(t,x,\mu)+f_2(t,\mu,q)+f_3(t,x,a)f=f1​(t,x,μ)+f2​(t,μ,q)+f3​(t,x,a); and (U.4) the Lasry–Lions monotonicity condition

∫C[g(x,μ)−g(x,μ′)+∫0T(f1(t,x,μ)−f1(t,x,μ′))dt](μ−μ′)(dx)≤0for all μ,μ′.\int_{\mathcal C}\Big[g(x,\mu)-g(x,\mu')+\int_0^T\big(f_1(t,x,\mu)-f_1(t,x,\mu')\big)dt\Big](\mu-\mu')(dx)\le0\qquad\text{for all }\mu,\mu'.∫C​[g(x,μ)−g(x,μ′)+∫0T​(f1​(t,x,μ)−f1​(t,x,μ′))dt](μ−μ′)(dx)≤0for all μ,μ′.

The standing assumptions (S) of the paper (measurability, continuity in aaa, nonsingular σ\sigmaσ, bounded σ−1b\sigma^{-1}bσ−1b, a ψ\psiψ-growth bound on f,gf,gf,g, and a separation of fff) are in force throughout.

Formalization targets

Goal: Theorem 3.8

Under (S) and (U), if (μ1,q1)(\mu^1,q^1)(μ1,q1) and (μ2,q2)(\mu^2,q^2)(μ2,q2) are solutions of the MFG, then

μ1=μ2andqt1=qt2 for almost every t∈[0,T].\mu^1=\mu^2\qquad\text{and}\qquad q^1_t=q^2_t\ \text{for almost every }t\in[0,T].μ1=μ2andqt1​=qt2​ for almost every t∈[0,T].

Definition 3.4 constrains qtq_tqt​ only for almost every ttt, so this is the strongest identification possible.

Milestones

  1. §7.3, p. 30. For a solution (μ,q)(\mu,q)(μ,q) with optimal control α\alphaα and a solution (Y,Z)(Y,Z)(Y,Z) of the BSDE Yt=g(X,μ)+∫tTH(s,X,μ,qs,Zs)ds−∫tTZsdWsY_t=g(X,\mu)+\int_t^TH(s,X,\mu,q_s,Z_s)ds-\int_t^TZ_sdW_sYt​=g(X,μ)+∫tT​H(s,X,μ,qs​,Zs​)ds−∫tT​Zs​dWs​ (7.1), αt\alpha_tαt​ maximizes the Hamiltonian at ZtZ_tZt​, dt×dPdt\times dPdt×dP-a.e.; under (U.1) every such maximizing control agrees with α\alphaα a.e.
  2. (7.9)–(7.10). E[Y01−Y02]E[Y^1_0-Y^2_0]E[Y01​−Y02​] written as an expectation under Pμ1,α1P^{\mu^1,\alpha^1}Pμ1,α1 and under Pμ2,α2P^{\mu^2,\alpha^2}Pμ2,α2.
  3. (7.11)–(7.12). Pointwise bounds from maximization of the Hamiltonian, strict when the controls differ.
  4. (7.13). [Eμ1,α1−Eμ2,α2][Δg(X)+∫0TΔf1(t,X)dt]=0\big[E^{\mu^1,\alpha^1}-E^{\mu^2,\alpha^2}\big]\big[\Delta g(X)+\int_0^T\Delta f_1(t,X)dt\big]=0[Eμ1,α1−Eμ2,α2][Δg(X)+∫0T​Δf1​(t,X)dt]=0.
  5. §7.3, p. 31. α1=α2\alpha^1=\alpha^2α1=α2, L×P\mathcal L\times PL×P-a.e.

Significance

Theorem 3.8, combined with the existence theorem of the same paper (Theorem 3.5, the first mission of this series), gives existence and uniqueness of the equilibrium (Corollary 3.9) for coefficients that are only measurable and path dependent in the state, under a monotonicity condition and no Lipschitz or small-horizon requirement. Uniqueness is also what makes the approximation result of the paper (Theorem 4.2, the third mission) refer to the equilibrium.

The result is proved in the paper. It has not been machine-checked; no mean field game uniqueness theorem in a weak or Girsanov formulation is formalized in Lean or Mathlib. The formal development would contain, as reusable parts, the Doléans exponential of a bounded Itô integrand as a probability density, the change of Brownian motion under it, the comparison principle for BSDEs with Lipschitz drivers, and the Lasry–Lions monotonicity argument.

Difficulty

The argument compares two equilibria through two different measures Pμ1,α1P^{\mu^1,\alpha^1}Pμ1,α1 and Pμ2,α2P^{\mu^2,\alpha^2}Pμ2,α2. The direct Lasry–Lions computation, which differentiates a pairing of a Hamilton–Jacobi–Bellman solution with a Fokker–Planck solution, is not available: there is no PDE, and the value functions are only known through BSDEs. The proof needs (a) that an optimal control maximizes the Hamiltonian along the adjoint process ZZZ — the necessity half of the BSDE optimality criterion, which the paper uses without a displayed proof; (b) the representation of E[Y01−Y02]E[Y^1_0-Y^2_0]E[Y01​−Y02​] under each of the two measures, which requires that the stochastic integrals ∫(Z1−Z2) dWμi,αi\int(Z^1-Z^2)\,dW^{\mu^i,\alpha^i}∫(Z1−Z2)dWμi,αi be true martingales under the changed measures; and (c) turning a strict pointwise inequality on a set of positive dt×dPdt\times dPdt×dP-measure into a strict inequality of expectations, which uses the equivalence P∼Pμi,αiP\sim P^{\mu^i,\alpha^i}P∼Pμi,αi.

Formalization scope

The Lean development lives in the namespace WeakMFG.Uniqueness and builds on the published definition Peng1990.SMP.Stochastic (Brownian motion, L2L^2L2 Itô integrals, Itô processes, BSDEs). Conventions:

  • Base space. Any probability space carrying ξ\xiξ and an independent standard Brownian motion WWW, with the filtration σ(ξ)∨σ(Ws:s≤t)\sigma(\xi)\vee\sigma(W_s:s\le t)σ(ξ)∨σ(Ws​:s≤t) completed by the measurable null sets; the canonical space of the paper is an instance.
  • State. "Strong solution" of dX=σ(t,X)dWdX=\sigma(t,X)dWdX=σ(t,X)dW is read in the L2L^2L2 Itô theory (square-integrable solutions); σ(t,X)>0\sigma(t,X)>0σ(t,X)>0 is matrix invertibility; states are vectors of Rd\mathbb R^dRd with the sup norm, Euclidean squares written as sums of squares.
  • Measures. Pψ(C)\mathcal P_\psi(\mathcal C)Pψ​(C) is a structure carrying the topology τψ\tau_\psiτψ​; P(A)\mathcal P(A)P(A) has the weak topology and its Borel σ\sigmaσ-field; time is R≥0\mathbb R_{\ge0}R≥0​, of which only [0,T][0,T][0,T] enters.
  • Densities. Itô integrals are determined up to versions, so dPμ,α/dPdP^{\mu,\alpha}/dPdPμ,α/dP is a predicate on a random variable; statements assert that a version exists and hold for every version. Optimality is stated against every admissible competitor, never through a real supremum.
  • Added hypotheses, disclosed. Joint measurability of (t,x,q,a)↦f(t,x,μ,q,a)(t,x,q,a)\mapsto f(t,x,\mu,q,a)(t,x,q,a)↦f(t,x,μ,q,a), which the reward presupposes; in (U.4), integrability of the integrals the page writes; the slip in (U.3), which omits qqq from the arguments of fff, is corrected.

A formalization whose hypotheses contain the conclusion is ruled out: the goal assumes only that the two pairs are solutions in the sense of Definition 3.4 — no BSDE solution, no Hamiltonian maximization, no equality of densities is assumed. Uniqueness of qqq is stated almost everywhere in time, and nowhere is equality of the two optimal controls as functions asked for.

Contributions welcome: the Doléans exponential and Girsanov's theorem for bounded drifts in the L2L^2L2 Itô layer, existence and comparison for Lipschitz BSDEs on a filtration enlarged by an independent initial condition, and the measurable maximum theorem for the Hamiltonian. These are reusable beyond this mission, in particular by the other two missions of the series.

Selected references

  • R. Carmona, D. Lacker, A probabilistic weak formulation of mean field games and applications, arXiv:1307.1152v2, 2014; Ann. Appl. Probab. 25(3), 2015. https://arxiv.org/abs/1307.1152
  • 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. P. Malhamé, P. E. 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
  • E. Pardoux, S. Peng, Adapted solution of a backward stochastic differential equation, Systems & Control Letters 14(1), 1990. https://doi.org/10.1016/0167-6911(90)90082-6
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Optimal TransportProbabilityStatistics·Captain: mikedeng1

On the Rate of Convergence in Wasserstein Distance of the Empirical Measure I: Non-Asymptotic Moment Bounds on E T_p(μ_N, μ) under a q-th Moment Condition (Theorem 1)Research Paper

Motivation

How fast does the empirical measure of an i.i.d. sample approach the law it is drawn from? When distance is measured by optimal transport, the answer enters the analysis of statistical estimators built from empirical distributions, quantization of probability measures, Monte Carlo and particle approximations of nonlinear PDEs (McKean–Vlasov systems), and the radius calibration of Wasserstein ambiguity sets in data-driven distributionally robust optimization.

The question has a long history. Ajtai, Komlós and Tusnády (1984) found the (log⁡N/N)1/2(\log N/N)^{1/2}(logN/N)1/2 rate for uniform samples in the unit square. Horowitz–Karandikar (1994), Rachev–Rüschendorf and Mischler–Mouhot gave bounds that were far from optimal outside the compactly supported case. Boissard and Le Gouic (2014) and Dereich, Scheutzow and Schottstedt (2013) introduced multiscale couplings; the latter obtained sharp moment bounds for p∈[1,d/2)p\in[1,d/2)p∈[1,d/2), d≥3d\ge3d≥3, under a moment condition q>dp/(d−p)q>dp/(d-p)q>dp/(d−p). Fournier and Guillin (arXiv:1312.2128, Probab. Theory Relat. Fields 162, 2015) extended these bounds to every p>0p>0p>0, every dimension d≥1d\ge1d≥1 and every moment order q>pq>pq>p, with explicit dependence on the moment.

Setting

Fix d≥1d\ge1d≥1 and write ∣⋅∣|\cdot|∣⋅∣ for the Euclidean norm on Rd\mathbb R^dRd. For probability measures μ,ν\mu,\nuμ,ν on Rd\mathbb R^dRd and p>0p>0p>0, the transport cost is

Tp(μ,ν)=inf⁡{∫∣x−y∣p ξ(dx,dy): ξ∈H(μ,ν)}∈[0,∞],\mathcal T_p(\mu,\nu)=\inf\Big\{\int|x-y|^p\,\xi(dx,dy):\ \xi\in\mathcal H(\mu,\nu)\Big\}\in[0,\infty],Tp​(μ,ν)=inf{∫∣x−y∣pξ(dx,dy): ξ∈H(μ,ν)}∈[0,∞],

where H(μ,ν)\mathcal H(\mu,\nu)H(μ,ν) is the set of couplings, measures on Rd×Rd\mathbb R^d\times\mathbb R^dRd×Rd with marginals μ\muμ and ν\nuν. The Wasserstein distance is Tp1/p\mathcal T_p^{1/p}Tp1/p​ for p>1p>1p>1 and Tp\mathcal T_pTp​ for p≤1p\le1p≤1; the statements here are about Tp\mathcal T_pTp​ itself. The moment of order q>0q>0q>0 is Mq(μ)=∫∣x∣q μ(dx)M_q(\mu)=\int|x|^q\,\mu(dx)Mq​(μ)=∫∣x∣qμ(dx).

Let X1,X2,…X_1,X_2,\dotsX1​,X2​,… be i.i.d. with law μ\muμ and let μN=1N∑k=1NδXk\mu_N=\frac1N\sum_{k=1}^N\delta_{X_k}μN​=N1​∑k=1N​δXk​​. The quantity of interest is E Tp(μN,μ)\mathbb E\,\mathcal T_p(\mu_N,\mu)ETp​(μN​,μ).

The proof works through a multiscale distance. For ℓ≥0\ell\ge0ℓ≥0, Pℓ\mathcal P_\ellPℓ​ is the partition of (−1,1]d(-1,1]^d(−1,1]d into 2dℓ2^{d\ell}2dℓ dyadic cubes of side 21−ℓ2^{1-\ell}21−ℓ. The dyadic shells are B0=(−1,1]dB_0=(-1,1]^dB0​=(−1,1]d and Bn=(−2n,2n]d∖(−2n−1,2n−1]dB_n=(-2^n,2^n]^d\setminus(-2^{n-1},2^{n-1}]^dBn​=(−2n,2n]d∖(−2n−1,2n−1]d. For measures on (−1,1]d(-1,1]^d(−1,1]d, Dp(μ,ν)=2p−12∑ℓ≥12−pℓ∑F∈Pℓ∣μ(F)−ν(F)∣\mathcal D_p(\mu,\nu)=\frac{2^p-1}{2}\sum_{\ell\ge1}2^{-p\ell}\sum_{F\in\mathcal P_\ell}|\mu(F)-\nu(F)|Dp​(μ,ν)=22p−1​∑ℓ≥1​2−pℓ∑F∈Pℓ​​∣μ(F)−ν(F)∣, and for measures on Rd\mathbb R^dRd,

Dp(μ,ν)=∑n≥02pn(∣μ(Bn)−ν(Bn)∣+(μ(Bn)∧ν(Bn))Dp(RBnμ,RBnν)),\mathcal D_p(\mu,\nu)=\sum_{n\ge0}2^{pn}\Big(|\mu(B_n)-\nu(B_n)|+\big(\mu(B_n)\wedge\nu(B_n)\big)\mathcal D_p(\mathcal R_{B_n}\mu,\mathcal R_{B_n}\nu)\Big),Dp​(μ,ν)=n≥0∑​2pn(∣μ(Bn​)−ν(Bn​)∣+(μ(Bn​)∧ν(Bn​))Dp​(RBn​​μ,RBn​​ν)),

where RBnμ\mathcal R_{B_n}\muRBn​​μ is μ\muμ conditioned on BnB_nBn​ and rescaled by 2−n2^{-n}2−n.

In Lean, Rd\mathbb R^dRd is EuclideanSpace ℝ (Fin d); Tp\mathcal T_pTp​, MqM_qMq​, Dp\mathcal D_pDp​ are transportCost, moment, Dp (compact case Dcube) in FournierGuillin.Moment, valued in ℝ≥0∞. μN\mu_NμN​ is the published WassersteinDRO.Duality.empiricalDistribution, and H(μ,ν)\mathcal H(\mu,\nu)H(μ,ν) the published WassersteinLinOpt.Ball.couplings.

Formalization targets

Goal: Theorem 1 (p. 2)

For p>0p>0p>0 and q>pq>pq>p there is C=C(p,d,q)C=C(p,d,q)C=C(p,d,q) such that for every μ\muμ with Mq(μ)<∞M_q(\mu)<\inftyMq​(μ)<∞ and every N≥1N\ge1N≥1,

E Tp(μN,μ)≤C Mqp/q(μ)×{N−1/2+N−(q−p)/qp>d/2, q≠2p,N−1/2log⁡(1+N)+N−(q−p)/qp=d/2, q≠2p,N−p/d+N−(q−p)/qp∈(0,d/2), q≠dp/(d−p).\mathbb E\,\mathcal T_p(\mu_N,\mu)\le C\,M_q^{p/q}(\mu)\times\begin{cases}N^{-1/2}+N^{-(q-p)/q}&p>d/2,\ q\ne2p,\\ N^{-1/2}\log(1+N)+N^{-(q-p)/q}&p=d/2,\ q\ne2p,\\ N^{-p/d}+N^{-(q-p)/q}&p\in(0,d/2),\ q\ne dp/(d-p).\end{cases}ETp​(μN​,μ)≤CMqp/q​(μ)×⎩⎨⎧​N−1/2+N−(q−p)/qN−1/2log(1+N)+N−(q−p)/qN−p/d+N−(q−p)/q​p>d/2, q=2p,p=d/2, q=2p,p∈(0,d/2), q=dp/(d−p).​

The constant is left unspecified, as in the paper.

Milestones

  1. Lemma 5 (p. 6): Tp(μ,ν)≤κp,d Dp(μ,ν)\mathcal T_p(\mu,\nu)\le\kappa_{p,d}\,\mathcal D_p(\mu,\nu)Tp​(μ,ν)≤κp,d​Dp​(μ,ν) with κp,d=2p(1+d/2)(2p+1)/(2p−1)\kappa_{p,d}=2^{p(1+d/2)}(2^p+1)/(2^p-1)κp,d​=2p(1+d/2)(2p+1)/(2p−1), for all probability measures.
  2. Lemma 6 (p. 7): Dp(μ,ν)≤C∑n≥02pn∑ℓ≥02−pℓ∑F∈Pℓ∣μ(2nF∩Bn)−ν(2nF∩Bn)∣\mathcal D_p(\mu,\nu)\le C\sum_{n\ge0}2^{pn}\sum_{\ell\ge0}2^{-p\ell}\sum_{F\in\mathcal P_\ell}|\mu(2^nF\cap B_n)-\nu(2^nF\cap B_n)|Dp​(μ,ν)≤C∑n≥0​2pn∑ℓ≥0​2−pℓ∑F∈Pℓ​​∣μ(2nF∩Bn​)−ν(2nF∩Bn​)∣.
  3. Shell tails (p. 8): Mq(μ)=1M_q(\mu)=1Mq​(μ)=1 implies μ(Bn)≤2−q(n−1)\mu(B_n)\le2^{-q(n-1)}μ(Bn​)≤2−q(n−1).
  4. Binomial mean deviation (p. 8): E∣μN(A)−μ(A)∣≤min⁡{2μ(A),μ(A)/N}\mathbb E|\mu_N(A)-\mu(A)|\le\min\{2\mu(A),\sqrt{\mu(A)/N}\}E∣μN​(A)−μ(A)∣≤min{2μ(A),μ(A)/N​}.
  5. Level bound (p. 8): ∑F∈PℓE∣μN(2nF∩Bn)−μ(2nF∩Bn)∣≤min⁡{2μ(Bn),2dℓ/2(μ(Bn)/N)1/2}\sum_{F\in\mathcal P_\ell}\mathbb E|\mu_N(2^nF\cap B_n)-\mu(2^nF\cap B_n)|\le\min\{2\mu(B_n),2^{d\ell/2}(\mu(B_n)/N)^{1/2}\}∑F∈Pℓ​​E∣μN​(2nF∩Bn​)−μ(2nF∩Bn​)∣≤min{2μ(Bn​),2dℓ/2(μ(Bn​)/N)1/2}.
  6. Display (4) (p. 8): E Dp(μN,μ)≤C∑n2pn∑ℓ2−pℓmin⁡{2−qn,2dℓ/2(2−qn/N)1/2}\mathbb E\,\mathcal D_p(\mu_N,\mu)\le C\sum_{n}2^{pn}\sum_{\ell}2^{-p\ell}\min\{2^{-qn},2^{d\ell/2}(2^{-qn}/N)^{1/2}\}EDp​(μN​,μ)≤C∑n​2pn∑ℓ​2−pℓmin{2−qn,2dℓ/2(2−qn/N)1/2} when Mq(μ)=1M_q(\mu)=1Mq​(μ)=1.
  7. Step 1 (p. 8): the scale series ∑ℓ≥02−pℓmin⁡{ε,2dℓ/2(ε/N)1/2}\sum_{\ell\ge0}2^{-p\ell}\min\{\varepsilon,2^{d\ell/2}(\varepsilon/N)^{1/2}\}∑ℓ≥0​2−pℓmin{ε,2dℓ/2(ε/N)1/2} in the three regimes.

Significance

Theorem 1 is the standard non-asymptotic rate for empirical measures in Wasserstein distance under moment assumptions alone. The three regimes are sharp for general laws: N−1/2N^{-1/2}N−1/2 is attained by two-point laws, N−p/dN^{-p/d}N−p/d by the uniform law on a cube, and the term N−(q−p)/qN^{-(q-p)/q}N−(q−p)/q by heavy-tailed laws (examples on pp. 2–3 of the paper). It is the input to finite-sample guarantees for Wasserstein distributionally robust optimization, to propagation-of-chaos rates for particle systems, and to quantization error bounds.

The paper result is proved; it has, to our knowledge, no machine-checked proof. A formalization adds the multiscale coupling bound (Lemma 5), a reusable comparison between transport costs and dyadic mass differences, and binomial mean-deviation estimates for empirical measures, all of which serve other rates of convergence (the concentration bounds of Theorem 2 of the same paper rest on Lemma 5).

Difficulty

The obvious route bounds Tp\mathcal T_pTp​ by a coupling on a single partition of fixed mesh and optimizes the mesh. This loses a logarithm or a power in every regime and cannot reach N−p/dN^{-p/d}N−p/d for p<d/2p<d/2p<d/2 or N−1/2N^{-1/2}N−1/2 for p>d/2p>d/2p>d/2: the error at all scales must be controlled simultaneously, which is what Dp\mathcal D_pDp​ does. The step that requires work in Lean is Lemma 5: it builds an explicit coupling scale by scale inside (−1,1]d(-1,1]^d(−1,1]d and glues the shells BnB_nBn​ together, and it must hold for arbitrary probability measures with possibly infinite cost. The remaining steps are careful summations of geometric series in nnn and ℓ\ellℓ whose regimes depend on ppp versus d/2d/2d/2 and on qqq versus 2p2p2p or dp/(d−p)dp/(d-p)dp/(d−p).

Formalization scope

Conventions: Rd\mathbb R^dRd with the Euclidean norm (the paper's constant κp,d\kappa_{p,d}κp,d​ uses the diameter bound 21+d/22^{1+d/2}21+d/2 of (−1,1]d(-1,1]^d(−1,1]d, which holds for that norm); d≥1d\ge1d≥1, N≥1N\ge1N≥1, p>0p>0p>0, μ\muμ a probability measure. The sample X1,…,XNX_1,\dots,X_NX1​,…,XN​ is a point of (Rd)N(\mathbb R^d)^N(Rd)N under the product measure μ⊗N\mu^{\otimes N}μ⊗N, i.e. the first NNN terms of the i.i.d. sequence. Expectations are lower Lebesgue integrals of [0,∞][0,\infty][0,∞]-valued functions and all series of nonnegative terms are summed in [0,∞][0,\infty][0,∞], so no bound holds by a junk value of a non-integrable integrand or a non-summable series. Constants "depending only on p,d,qp,d,qp,d,q" are quantified after p,d,qp,d,qp,d,q and before μ\muμ and NNN; a statement with the constant chosen after μ\muμ would only assert finiteness and is ruled out.

Corrections of the print, disclosed in the items: the third case of Theorem 1 is printed with q≠d/(d−p)q\ne d/(d-p)q=d/(d−p); the remark below the theorem and Step 4 of the proof show the excluded value is q=dp/(d−p)q=dp/(d-p)q=dp/(d−p) (the two agree only for p=1p=1p=1), and the goal excludes q=dp/(d−p)q=dp/(d-p)q=dp/(d−p). Step 1 is printed for ε∈(0,1)\varepsilon\in(0,1)ε∈(0,1) but applied at ε=1\varepsilon=1ε=1; it is stated for ε∈(0,1]\varepsilon\in(0,1]ε∈(0,1]. The display defining Tp\mathcal T_pTp​ says p≥1p\ge1p≥1, but the paper uses it for all p>0p>0p>0, and so does the definition.

Needed infrastructure: couplings and gluing of measures on products, dyadic partitions of boxes and their counting, binomial variance, and summation of geometric series with case analysis. Lemma 5 and the binomial estimates are reusable beyond this mission. Proofs of any milestone are welcome, as are alternative proofs of the goal.

Selected references

  • N. Fournier, A. Guillin, On the rate of convergence in Wasserstein distance of the empirical measure, Probab. Theory Relat. Fields 162 (2015) 707–738; arXiv:1312.2128v1. https://arxiv.org/abs/1312.2128 · https://doi.org/10.1007/s00440-014-0583-7
  • S. Dereich, M. Scheutzow, R. Schottstedt, Constructive quantization: approximation by empirical measures, Ann. Inst. Henri Poincaré Probab. Stat. 49 (2013) 1183–1203. https://arxiv.org/abs/1108.5346
  • M. Ajtai, J. Komlós, G. Tusnády, On optimal matchings, Combinatorica 4 (1984) 259–264. https://doi.org/10.1007/BF02579135
  • E. Boissard, T. Le Gouic, On the mean speed of convergence of empirical and occupation measures in Wasserstein distance, Ann. Inst. Henri Poincaré Probab. Stat. 50 (2014) 539–563. https://arxiv.org/abs/1105.5263
  • J. Horowitz, R. L. Karandikar, Mean rates of convergence of empirical measures in the Wasserstein metric, J. Comput. Appl. Math. 55 (1994) 261–273. https://doi.org/10.1016/0377-0427(94)90033-7
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Control TheoryOptimal TransportPartial Differential Equations+1·Captain: mikedeng1

Mean Field Games Master Equations with Nonseparable Hamiltonians and Displacement Monotonicity: Under Displacement Monotone H and G, the Master Equation Has a Unique Global Classical SolutionResearch Paper

Motivation

Mean field games (Lasry–Lions 2006–2007; Huang–Malhamé–Caines 2006) describe Nash equilibria of games with a very large number of symmetric players, each interacting with the others only through the empirical distribution of their states. When all players are also exposed to a common noise, the equilibrium is no longer described by a forward–backward pair of PDEs but by a single equation on the space of probability measures, the master equation. The master equation is the object that lets one prove convergence of NNN-player equilibria to the mean field limit (Cardaliaguet–Delarue–Lasry–Lions 2019), so a global classical solution is the starting point of that theory.

Global well-posedness requires a monotonicity condition; without one, uniqueness of equilibria fails. Before this paper, global results were known under the Lasry–Lions monotonicity condition and for separable Hamiltonians H(x,μ,p)=H0(x,p)−F(x,μ)H(x,\mu,p)=H_0(x,p)-F(x,\mu)H(x,μ,p)=H0​(x,p)−F(x,μ), and under displacement convexity in deterministic potential games (Gangbo–Mészáros 2022). Gangbo, Mészáros, Mou and Zhang (Ann. Probab. 50 (2022)) prove global well-posedness for nonseparable Hamiltonians under displacement monotonicity, a condition that is different from Lasry–Lions monotonicity and that has a natural extension to Hamiltonians depending jointly on (x,μ,p)(x,\mu,p)(x,μ,p).

Setting

Let P2=P2(Rd)\mathcal P_2=\mathcal P_2(\mathbb R^d)P2​=P2​(Rd) be the Borel probability measures on Rd\mathbb R^dRd with finite second moment, with the 2-Wasserstein distance W2W_2W2​. For U:P2→RU:\mathcal P_2\to\mathbb RU:P2​→R, the Lions derivative ∂μU(μ,x~)∈Rd\partial_\mu U(\mu,\tilde x)\in\mathbb R^d∂μ​U(μ,x~)∈Rd is characterized by

U(Lξ+η)−U(μ)=E[⟨∂μU(μ,ξ),η⟩]+o(∥η∥2),Lξ=μ.U(\mathcal L_{\xi+\eta})-U(\mu)=\mathbb E[\langle\partial_\mu U(\mu,\xi),\eta\rangle]+o(\|\eta\|_2),\qquad \mathcal L_\xi=\mu .U(Lξ+η​)−U(μ)=E[⟨∂μ​U(μ,ξ),η⟩]+o(∥η∥2​),Lξ​=μ.

The class C2(Rd×P2)\mathcal C^2(\mathbb R^d\times\mathcal P_2)C2(Rd×P2​) consists of continuous U(x,μ)U(x,\mu)U(x,μ) for which ∂xU\partial_xU∂x​U, ∂xxU\partial_{xx}U∂xx​U, ∂μU(x,μ,x~)\partial_\mu U(x,\mu,\tilde x)∂μ​U(x,μ,x~), ∂x∂μU\partial_x\partial_\mu U∂x​∂μ​U, ∂x~∂μU\partial_{\tilde x}\partial_\mu U∂x~​∂μ​U and ∂μμU(x,μ,x~,xˉ)\partial_{\mu\mu}U(x,\mu,\tilde x,\bar x)∂μμ​U(x,μ,x~,xˉ) exist and extend to jointly continuous functions of all their arguments.

The data are a horizon T>0T>0T>0, a common-noise intensity β≥0\beta\ge0β≥0 with β^2=1+β2\hat\beta^2=1+\beta^2β^​2=1+β2, a Hamiltonian H(x,μ,p)H(x,\mu,p)H(x,μ,p) and a terminal cost G(x,μ)G(x,\mu)G(x,μ). The master equation on Θ=[0,T]×Rd×P2\Theta=[0,T]\times\mathbb R^d\times\mathcal P_2Θ=[0,T]×Rd×P2​ is

−∂tV−β^22tr⁡(∂xxV)+H(x,μ,∂xV)−NV=0,V(T,x,μ)=G(x,μ),-\partial_tV-\tfrac{\hat\beta^2}{2}\operatorname{tr}(\partial_{xx}V)+H(x,\mu,\partial_xV)-\mathcal NV=0,\qquad V(T,x,\mu)=G(x,\mu),−∂t​V−2β^​2​tr(∂xx​V)+H(x,μ,∂x​V)−NV=0,V(T,x,μ)=G(x,μ),

with the nonlocal operator

NV=tr⁡ E~ˉ[β^22∂x~∂μV(t,x,μ,ξ~)+β22∂μμV(t,x,μ,ξˉ,ξ~)+β2∂x∂μV(t,x,μ,ξ~)−∂μV(t,x,μ,ξ~)(∂pH)⊤(ξ~,μ,∂xV(t,ξ~,μ))],\mathcal NV=\operatorname{tr}\,\bar{\tilde{\mathbb E}}\Big[\tfrac{\hat\beta^2}{2}\partial_{\tilde x}\partial_\mu V(t,x,\mu,\tilde\xi)+\tfrac{\beta^2}{2}\partial_{\mu\mu}V(t,x,\mu,\bar\xi,\tilde\xi)+\beta^2\partial_x\partial_\mu V(t,x,\mu,\tilde\xi)-\partial_\mu V(t,x,\mu,\tilde\xi)(\partial_pH)^\top(\tilde\xi,\mu,\partial_xV(t,\tilde\xi,\mu))\Big],NV=trE~ˉ[2β^​2​∂x~​∂μ​V(t,x,μ,ξ~​)+2β2​∂μμ​V(t,x,μ,ξˉ​,ξ~​)+β2∂x​∂μ​V(t,x,μ,ξ~​)−∂μ​V(t,x,μ,ξ~​)(∂p​H)⊤(ξ~​,μ,∂x​V(t,ξ~​,μ))],

where ξ~,ξˉ\tilde\xi,\bar\xiξ~​,ξˉ​ are independent with law μ\muμ. A classical solution is a V∈C1,2,2(Θ)V\in\mathcal C^{1,2,2}(\Theta)V∈C1,2,2(Θ) satisfying the equation on (0,T)(0,T)(0,T) and the terminal condition.

U(x,μ)U(x,\mu)U(x,μ) is displacement monotone (2.16) if for all square-integrable ξ,η\xi,\etaξ,η with Lξ=μ\mathcal L_\xi=\muLξ​=μ and an independent copy (ξ~,η~)(\tilde\xi,\tilde\eta)(ξ~​,η~​),

E~[⟨∂xμU(ξ,μ,ξ~)η~,η⟩+⟨∂xxU(ξ,μ)η,η⟩]≥0.\tilde{\mathbb E}\big[\langle\partial_{x\mu}U(\xi,\mu,\tilde\xi)\tilde\eta,\eta\rangle+\langle\partial_{xx}U(\xi,\mu)\eta,\eta\rangle\big]\ge0 .E~[⟨∂xμ​U(ξ,μ,ξ~​)η~​,η⟩+⟨∂xx​U(ξ,μ)η,η⟩]≥0.

The Hamiltonian is displacement monotone (Definition 3.4) if a bilinear form built from ∂xμH\partial_{x\mu}H∂xμ​H, ∂xxH\partial_{xx}H∂xx​H and a correction 14E∣(∂ppH)−1/2E~[∂pμH η~]∣2\tfrac14\mathbb E\big|(\partial_{pp}H)^{-1/2}\tilde{\mathbb E}[\partial_{p\mu}H\,\tilde\eta]\big|^241​E​(∂pp​H)−1/2E~[∂pμ​Hη~​]​2 is nonpositive, with p=φ(ξ)p=\varphi(\xi)p=φ(ξ) for every bounded Lipschitz C1C^1C1 map φ\varphiφ. Assumptions 3.1 and 3.2 impose regularity and bounds on GGG and HHH; Assumption 3.5 imposes the two monotonicity conditions.

Formalization targets

Goal: Theorem 6.3, first sentence

Under Assumptions 3.1, 3.2 and 3.5, the master equation on [0,T][0,T][0,T] has a classical solution VVV with bounded ∂xV\partial_xV∂x​V, ∂xxV\partial_{xx}V∂xx​V, ∂μV\partial_\mu V∂μ​V, ∂xμV\partial_{x\mu}V∂xμ​V, and it is the only classical solution in that class:

∃! V∈C1,2,2(Θ) solving (1.1) with ∂xV,∂xxV,∂μV,∂xμV bounded.\exists!\,V\in\mathcal C^{1,2,2}(\Theta)\ \text{solving (1.1) with}\ \partial_xV,\partial_{xx}V,\partial_\mu V,\partial_{x\mu}V\ \text{bounded}.∃!V∈C1,2,2(Θ) solving (1.1) with ∂x​V,∂xx​V,∂μ​V,∂xμ​V bounded.

Milestones

  1. Lemma 2.1: ∂x~μU(μ,x~)\partial_{\tilde x\mu}U(\mu,\tilde x)∂x~μ​U(μ,x~) is symmetric for U∈C2(P2)U\in\mathcal C^2(\mathcal P_2)U∈C2(P2​).
  2. Theorem 4.1: along a sufficiently regular classical solution, V(t,⋅,⋅)V(t,\cdot,\cdot)V(t,⋅,⋅) is displacement monotone for every t∈[0,T]t\in[0,T]t∈[0,T].
  3. Theorem 5.1: if V(t,⋅,⋅)V(t,\cdot,\cdot)V(t,⋅,⋅) is displacement semimonotone with constant λ\lambdaλ, then VVV and ∂xV\partial_xV∂x​V are W2W_2W2​-Lipschitz in μ\muμ with a constant depending only on ddd, TTT, ∥∂xV∥∞\|\partial_xV\|_\infty∥∂x​V∥∞​, ∥∂xxV∥∞\|\partial_{xx}V\|_\infty∥∂xx​V∥∞​, L2GL_2^GL2G​, LH(∥∂xV∥∞)L^H(\|\partial_xV\|_\infty)LH(∥∂x​V∥∞​) and λ\lambdaλ.
  4. Proposition 6.2(iii) with (6.7): on a short interval [t0,T][t_0,T][t0​,T], of length δ\deltaδ independent of L1GL_1^GL1G​, the master equation has a unique classical solution with full C2\mathcal C^2C2 regularity and ∣∂μV(t0)∣,∣∂xμV(t0)∣≤C1μ|\partial_\mu V(t_0)|,|\partial_{x\mu}V(t_0)|\le C_1^\mu∣∂μ​V(t0​)∣,∣∂xμ​V(t0​)∣≤C1μ​.

Significance

The theorem gives global classical well-posedness of the master equation with common noise for a class of Hamiltonians that need not be separable and data that need not be Lasry–Lions monotone. A classical solution is what the convergence analysis of NNN-player games and the construction of approximate equilibria take as input. Theorem 4.1, displacement monotonicity propagating backward along the equation, is the central structural fact; Theorem 5.1 converts it into an a priori Lipschitz bound in μ\muμ that is uniform in time, which is what allows local solutions to be continued.

The result is proved in the paper; nothing in this mission is open mathematically. No part of it is formalized anywhere. The mission produces a formal statement of the master equation, its classical solutions and the displacement monotonicity conditions, plus targets for a machine-checked proof. Calculus on Wasserstein space with Lions derivatives is absent from Mathlib, so even Lemma 2.1 requires new infrastructure.

Difficulty

Local well-posedness holds for any regular data; the obstacle is continuing the solution to the whole interval. The length of the local interval depends on the Lipschitz constant of the terminal data in μ\muμ, and without a uniform-in-time bound on that constant the local intervals can shrink to zero. Lasry–Lions monotonicity is not available here, and for nonseparable HHH it has no obvious analogue. Any argument that controls this constant has to work with second-order Lions derivatives, which needs full C2\mathcal C^2C2 regularity in the measure variable. That regularity is itself only known on short intervals.

Formalization scope

  • States are EuclideanSpace ℝ (Fin d). P2\mathcal P_2P2​ is a subtype of measures, so functions of μ\muμ are defined only on P2\mathcal P_2P2​. W2W_2W2​ is the published WassersteinDRO.Duality.wassersteinDistance with p=2p=2p=2, converted to a real number.
  • There is no probability space. Every expectation over ξ,η\xi,\etaξ,η and independent copies is an integral against an L2\mathbb L^2L2-coupling π\piπ (the joint law of (ξ,η)(\xi,\eta)(ξ,η)), against π⊗π\pi\otimes\piπ⊗π, or against μ⊗μ\mu\otimes\muμ⊗μ. Quantifying over all couplings is the reading of "for all ξ,η∈L2\xi,\eta\in\mathbb L^2ξ,η∈L2".
  • The Lions derivative is stated in coupling form, uniformly over all ξ\xiξ of law μ\muμ. Derivatives are explicit witnesses, i.e. global versions, and joint continuity is required as on the page.
  • Derivatives are (bi)linear maps. ⟨∂xμU η~,η⟩\langle\partial_{x\mu}U\,\tilde\eta,\eta\rangle⟨∂xμ​Uη~​,η⟩ takes the xxx-direction η\etaη first. Matrix norms are operator norms; this choice changes no statement, since all constants are existential.
  • C2(Rd×P2×Rk)\mathcal C^2(\mathbb R^d\times\mathcal P_2\times\mathbb R^k)C2(Rd×P2​×Rk), which the page uses without defining, lumps the Euclidean variables into one. "H∈C3H\in\mathcal C^3H∈C3" is read as existence and joint continuity of the (x,p)(x,p)(x,p)-derivatives up to order three. Vector-valued memberships are stated coordinatewise.
  • ∂ppH\partial_{pp}H∂pp​H is assumed positive definite, which the page's (∂ppH)−1/2(\partial_{pp}H)^{-1/2}(∂pp​H)−1/2 presupposes. ∣A−1/2w∣2|A^{-1/2}w|^2∣A−1/2w∣2 is written ⟨A−1w,w⟩\langle A^{-1}w,w\rangle⟨A−1w,w⟩.
  • The expectations in NV\mathcal NVNV are required to exist, so a non-integrable integrand cannot make the equation hold through a Bochner integral defaulting to 000. L2GL_2^GL2G​ (Remark 3.3) is used in its Lipschitz form.
  • "Depending only on" clauses are quantifier orders. In Proposition 6.2, δ\deltaδ depends on d,T,C0,L0G,LH,L2Gd,T,C_0,L_0^G,L^H,L_2^Gd,T,C0​,L0G​,LH,L2G​; this expands LH(C1x)L^H(C_1^x)LH(C1x​), whose constant C1xC_1^xC1x​ comes from a BSDE. Uniqueness is within the bounded-derivative class of Theorem 6.3.
  • Out of scope: the second sentence of Theorem 6.3 (well-posedness of the McKean–Vlasov FBSDEs and the representation (6.6)), Proposition 6.1, and Proposition 6.2(i), (ii) and (2.27). They need Brownian motions with common noise and BSDEs.
  • A statement in which the regularity hypotheses cannot all hold at once, or in which existence of the solution is assumed, would be a trivializing formalization and is not acceptable. The hypotheses here are taken from the page, which shows they are satisfiable (Remark 3.6(i), Lemma 3.8).
  • Wanted contributions: first- and second-order calculus on P2\mathcal P_2P2​ (Lions derivatives, the chain rule along μ↦Lξ+εη\mu\mapsto\mathcal L_{\xi+\varepsilon\eta}μ↦Lξ+εη​, symmetry of ∂x~μ\partial_{\tilde x\mu}∂x~μ​). These are reusable for any mean field problem.

Selected references

  • W. Gangbo, A. R. Mészáros, C. Mou, J. Zhang, Mean field games master equations with nonseparable Hamiltonians and displacement monotonicity, Ann. Probab. 50(6), 2178–2217, 2022. https://doi.org/10.1214/22-AOP1580
  • J.-M. Lasry, P.-L. Lions, Mean field games, Jpn. J. Math. 2, 229–260, 2007. https://doi.org/10.1007/s11537-007-0657-8
  • P. Cardaliaguet, F. Delarue, J.-M. Lasry, P.-L. Lions, The Master Equation and the Convergence Problem in Mean Field Games, Annals of Mathematics Studies 201, Princeton University Press, 2019. https://doi.org/10.2307/j.ctvckq7qf
  • R. Carmona, F. Delarue, Probabilistic Theory of Mean Field Games with Applications I–II, Springer, 2018. https://doi.org/10.1007/978-3-319-58920-6
  • W. Gangbo, A. R. Mészáros, Global well-posedness of master equations for deterministic displacement convex potential mean field games, Comm. Pure Appl. Math. 75, 2685–2801, 2022. https://doi.org/10.1002/cpa.22069
11 thms1 active userReviewed
Algorithmic Game TheoryOptimal TransportProbability+1·Captain: mikedeng1

From the Master Equation to Mean Field Game Limit Theory: Large Deviations and Concentration of Measure 1: Without Common Noise, n-Player Nash Equilibria Concentrate Dimension-FreeResearch Paper

Motivation

A large stochastic game has one state process per player. Each player's feedback changes with the empirical distribution of all states, so a finite population remains coupled even when the idiosyncratic Brownian motions are independent. A useful quantitative question is whether a statistic of the entire collection of equilibrium trajectories can deviate substantially from its mean as the population grows. Delarue, Lacker, and Ramanan answer this for smooth closed-loop mean-field games in their large-deviations and concentration paper. Their result concerns the equilibrium state paths themselves, rather than only a fixed-time empirical measure.

The paper is part of a two-paper limit theory. Its companion central-limit paper supplies the Nash-to-McKean–Vlasov estimates quoted here as Theorems 4.1 and 4.2. The concentration argument also uses transport inequalities: Gozlan's dimension-free characterization explains the quadratic transport assumption on the initial law, while Djellout, Guillin, and Wu provide a transport principle for diffusion path laws. The present mission records the paper's main concentration theorem and four of its explicit intermediate targets.

Setting

Fix a horizon T>0T>0T>0 and a positive state dimension ddd. Player iii has a continuous state path Xi∈Cd=C([0,T];Rd)X^i\in C^d=C([0,T];\mathbb R^d)Xi∈Cd=C([0,T];Rd). The empirical measure of a vector x=(x1,…,xn)x=(x^1,\ldots,x^n)x=(x1,…,xn) is mxn=n−1∑iδxim_x^n=n^{-1}\sum_i\delta_{x^i}mxn​=n−1∑i​δxi​; the same formula applies to paths. The norm on CdC^dCd is ∥x∥∞=sup⁡t≤T∣xt∣\|x\|_\infty=\sup_{t\le T}|x_t|∥x∥∞​=supt≤T​∣xt​∣, and the product norm relevant to this mission is ∥x∥n,2=(∑i∥xi∥∞2)1/2\|x\|_{n,2}=(\sum_i\|x^i\|_\infty^2)^{1/2}∥x∥n,2​=(∑i​∥xi∥∞2​)1/2.

The game is posed on a filtered probability space with a common Wiener process WWW, independent idiosyncratic Wiener processes BiB^iBi, and i.i.d. initial states X0iX^i_0X0i​ of law μ0\mu_0μ0​. The action space is Polish. A drift b(x,m,a)b(x,m,a)b(x,m,a), running cost f(x,m,a)f(x,m,a)f(x,m,a), and terminal cost g(x,m)g(x,m)g(x,m) specify the control problem. The Hamiltonian H(x,m,y)H(x,m,y)H(x,m,y) minimizes b(x,m,a)⋅y+f(x,m,a)b(x,m,a)\cdot y+f(x,m,a)b(x,m,a)⋅y+f(x,m,a) over actions; a selected minimizer α^\hat\alphaα^ defines b^=b(⋅,α^)\hat b=b(\cdot,\hat\alpha)b^=b(⋅,α^) and f^=f(⋅,α^)\hat f=f(\cdot,\hat\alpha)f^​=f(⋅,α^).

Classical solutions vn,iv^{n,i}vn,i of the nnn-player Nash system (2.6) determine the feedback in the equilibrium state equation (2.7). A classical solution UUU of the master equation (2.8) determines the comparison particle equation (4.1). Both equations retain common-noise terms in their definitions. The goal sets the common-noise coefficient σ0\sigma_0σ0​ to zero. Assumption A imposes Hamiltonian attainment, Lipschitz b^\hat bb^, nondegenerate idiosyncratic diffusion, an initial moment above order four, and the stated classical solutions. Either B or B′ controls the selected running cost; B′ also bounds UUU and vn,iv^{n,i}vn,i as specified on pp. 8–9.

Formalization targets

The goal is Theorem 3.4. If μ0\mu_0μ0​ satisfies the quadratic transport inequality W2(μ0,ν)≤2κR(ν∣μ0)W_2(\mu_0,\nu)\le\sqrt{2\kappa R(\nu\mid\mu_0)}W2​(μ0​,ν)≤2κR(ν∣μ0​)​ for every ν≪μ0\nu\ll\mu_0ν≪μ0​ with finite second moment, then constants C,δ1,δ2>0C,\delta_1,\delta_2>0C,δ1​,δ2​>0 exist such that, for a>0a>0a>0, n≥C/a2n\ge C/a^2n≥C/a2, and every 1-Lipschitz Φ\PhiΦ on the product path space,

P ⁣(Φ(X)−EΦ(X)>a)≤2nexp⁡(−δ1a2n)+2exp⁡(−δ2a2).P\!\left(\Phi(X)-E\Phi(X)>a\right) \le 2n\exp(-\delta_1a^2n)+2\exp(-\delta_2a^2).P(Φ(X)−EΦ(X)>a)≤2nexp(−δ1​a2n)+2exp(−δ2​a2).

The four milestones retain the paper's two main comparison layers. Theorem 4.3 controls both the path-space Wasserstein distance between the Nash and comparison empirical measures and their synchronous squared path distance by 2nexp⁡(−ε2n2/κ2)2n\exp(-\varepsilon^2n^2/\kappa_2)2nexp(−ε2n2/κ2​) for n≥κ1/εn\ge\kappa_1/\varepsilonn≥κ1​/ε. Theorem 5.3 gives a dimension-uniform transport inequality and concentration bound for the law of a Lipschitz SDE in the coordinatewise product-supremum norm. Equation (5.7) bounds the change in a 1-Lipschitz path expectation when the deterministic initial vector changes. Theorem 5.4 gives P(Φ(X~)−EΦ(X~)>a)≤2e−δa2P(\Phi(\tilde X)-E\Phi(\tilde X)>a)\le2e^{-\delta a^2}P(Φ(X~)−EΦ(X~)>a)≤2e−δa2 for the interacting comparison system. The labels, constants, and domains follow the pinned preprint, pp. 12 and 16–20.

Significance

Theorem 3.4 supplies a finite-population tail estimate for every 1-Lipschitz observable of the entire equilibrium path vector. The first term becomes small at a population-dependent scale, while the second term has a rate independent of the number of players. This is stronger information than convergence of the empirical measure alone: it applies to path-dependent statistics and includes explicit deviation probabilities Theorem 3.4.

The mathematical statements are proved in the source paper, subject to its assumptions; Theorems 4.1 and 4.2 that support its comparison result are proved in the companion paper. The work here is to give these claims faithful machine-checkable statements and ultimately machine-checked proofs. The present draft is a set of open Lean theorem statements with sorry, so it asserts no completed formal proof. A completed development would also make its definitions of empirical path laws, Wasserstein continuity, flat derivatives, and interacting SDE solutions reusable for other mean-field models.

Difficulty

Independent-noise concentration cannot simply be applied to the Nash state paths. A player's drift depends on the empirical state measure and on a derivative of the nnn-player Nash solution, so changing one input can change every trajectory. The master equation describes a comparison system, but using it requires matching the Nash and master feedbacks on the same filtered probability space. The regularity in Assumptions A, B, and B′ is substantial: the master field has first and second derivatives in both space and measure, with uniform bounds. A formal proof must also preserve the exact path norm and the population-independent placement of constants. The SDE transport theorem's uniformity over dimensions is particularly consequential for Theorem 5.4 §§4–5.

Formalization scope

State vectors use finite-dimensional Euclidean spaces; time uses nonnegative reals and only [0,T][0,T][0,T] is evaluated. A continuous path is a ContinuousMap on that interval with its supremum norm. Finite products use PiLp 2; the scalar-coordinate version of the norm is used for Theorem 5.3. Players are indexed from zero, corresponding to the paper's indices 1,…,n1,\ldots,n1,…,n, and every theorem requires n≥1n\ge1n≥1. Probabilities and entropy are extended nonnegative values. Transport distances stay extended until a finite-moment hypothesis justifies their real value.

The filtered Wiener processes, i.i.d. initial states, Borel coefficients, Polish action space, Nash and master PDEs, and either B or B′ are represented explicitly. The master equation is imposed on P2\mathcal P_2P2​; its spatial gradient is also required on Pp∗\mathcal P_{p_*}Pp∗​​, as Assumption A(5) specifies. A flat measure derivative is a normalized witness satisfying (2.2), while spatial derivatives are actual Fréchet derivatives. SDE solutions are path-valued processes satisfying coordinate Itô integral relations; solution families are supplied as hypotheses, since their existence is asserted by the source. Expectations appearing in the conclusions are stated integrable, so a default zero integral cannot satisfy a tail bound accidentally. The model cannot be replaced by arbitrary paths or a vacuous solution predicate: the Nash and comparison paths must satisfy their respective equations with the same noises and initial states.

The mission includes Theorem 4.3, Theorem 5.3, (5.7), and Theorem 5.4. The quoted Theorems 4.1 and 4.2, the general transport equivalence of Theorem 5.1, and tensorization in Theorem 5.2 remain useful later contributions, with their original hypotheses and conclusions intact. The printed constant in the “moreover” clause of Theorem 5.1 is omitted because it is dimensionally incorrect; no substitute assertion is placed in this mission.

Selected references

  • F. Delarue, D. Lacker, and K. Ramanan, From the master equation to mean field game limit theory: Large deviations and concentration of measure, Annals of Probability 48 (2020), 211–263; formalization follows arXiv:1804.08550v1.
  • F. Delarue, D. Lacker, and K. Ramanan, From the master equation to mean field game limit theory: A central limit theorem, preprint (2018), arXiv:1804.08542.
  • N. Gozlan, A characterization of dimension free concentration in terms of transportation inequalities, Annals of Probability 37 (2009), 2480–2498, doi:10.1214/09-AOP470.
  • H. Djellout, A. Guillin, and L. Wu, Transportation cost-information inequalities and applications to random dynamical systems and diffusions, Annals of Probability 32 (2004), 2702–2732, doi:10.1214/009117904000000531.
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Differential GeometryNumerical AnalysisOptimization·Captain: mikedeng1

Riemannian Proximal Gradient Methods II: The Riemannian Proximal Gradient Method Converges at Rate O(1/k) under Retraction ConvexityResearch Paper

Motivation

Many problems in statistics, signal processing and machine learning minimize a smooth loss plus a nonsmooth regularizer over a set with manifold structure: sparse principal component analysis over the Stiefel manifold, sparse blind deconvolution over the sphere, and clustering and dictionary-learning models with orthogonality constraints. In Euclidean space the standard method for such composite problems is the proximal gradient method, whose O(1/k)O(1/k)O(1/k) rate for convex problems is classical (Beck–Teboulle 2009). Huang and Wei (arXiv:1909.06065v4, Mathematical Programming 2021) propose a Riemannian proximal gradient method (RPG) that solves its proximal subproblem on the tangent space and returns to the manifold through a retraction. They prove three things about it: global convergence, an O(1/k)O(1/k)O(1/k) rate under a convexity notion adapted to retractions, and local rates under a Riemannian Kurdyka–Łojasiewicz property. This mission covers the second result, Theorem 3.2.

Earlier Riemannian proximal methods either required the exponential map and parallel transport, or solved a Euclidean proximal problem in the ambient space (Chen, Ma, So, Zhang 2020, ManPG). Theorem 3.2 is stated for a general retraction, with an explicit constant.

Setting

Let M\mathcal MM be a finite-dimensional Riemannian manifold, with inner product ⟨⋅,⋅⟩x\langle\cdot,\cdot\rangle_x⟨⋅,⋅⟩x​ and norm ∥⋅∥x\|\cdot\|_x∥⋅∥x​ on each tangent space TxMT_x\mathcal MTx​M. A retraction is a family of smooth maps Rx:TxM→MR_x:T_x\mathcal M\to\mathcal MRx​:Tx​M→M with Rx(0x)=xR_x(0_x)=xRx​(0x​)=x and DRx(0x)=id\mathrm DR_x(0_x)=\mathrm{id}DRx​(0x​)=id. The problem is

min⁡x∈MF(x)=f(x)+g(x),\min_{x\in\mathcal M} F(x)=f(x)+g(x),x∈Mmin​F(x)=f(x)+g(x),

where fff is differentiable with Riemannian gradient grad⁡f\operatorname{grad} fgradf, and ggg is continuous and possibly nonsmooth.

For a function hhh on a real inner-product space VVV, the Clarke generalized directional derivative is h∘(η;v)=lim sup⁡ξ→η, t↓0(h(ξ+tv)−h(ξ))/th^\circ(\eta;v)=\limsup_{\xi\to\eta,\,t\downarrow0}(h(\xi+tv)-h(\xi))/th∘(η;v)=limsupξ→η,t↓0​(h(ξ+tv)−h(ξ))/t. The generalized subdifferential is ∂h(η)={ζ∣⟨ζ,v⟩≤h∘(η;v) ∀v}\partial h(\eta)=\{\zeta\mid\langle\zeta,v\rangle\le h^\circ(\eta;v)\ \forall v\}∂h(η)={ζ∣⟨ζ,v⟩≤h∘(η;v) ∀v}. A point η\etaη is stationary for hhh if 0∈∂h(η)0\in\partial h(\eta)0∈∂h(η).

Given a constant L~\tilde LL~, the RPG method (Algorithm 1) produces iterates xkx_kxk​ and steps ηxk∗∈TxkM\eta^*_{x_k}\in T_{x_k}\mathcal Mηxk​∗​∈Txk​​M as follows. Set

ℓxk(η)=⟨grad⁡f(xk),η⟩xk+L~2∥η∥xk2+g(Rxk(η)).\ell_{x_k}(\eta)=\langle\operatorname{grad} f(x_k),\eta\rangle_{x_k}+\frac{\tilde L}{2}\|\eta\|_{x_k}^2+g(R_{x_k}(\eta)).ℓxk​​(η)=⟨gradf(xk​),η⟩xk​​+2L~​∥η∥xk​2​+g(Rxk​​(η)).

Choose a stationary point ηxk∗\eta^*_{x_k}ηxk​∗​ of ℓxk\ell_{x_k}ℓxk​​ on TxkMT_{x_k}\mathcal MTxk​​M with ℓxk(0)≥ℓxk(ηxk∗)\ell_{x_k}(0)\ge\ell_{x_k}(\eta^*_{x_k})ℓxk​​(0)≥ℓxk​​(ηxk​∗​), and set xk+1=Rxk(ηxk∗)x_{k+1}=R_{x_k}(\eta^*_{x_k})xk+1​=Rxk​​(ηxk​∗​).

The assumptions involve the sublevel set Ωx0={x∣F(x)≤F(x0)}\Omega_{x_0}=\{x\mid F(x)\le F(x_0)\}Ωx0​​={x∣F(x)≤F(x0​)} and two notions defined with respect to RRR on a set N\mathcal NN:

  • LLL-retraction-smoothness: h(Rx(η))≤h(x)+⟨grad⁡h(x),η⟩x+L2∥η∥x2h(R_x(\eta))\le h(x)+\langle\operatorname{grad} h(x),\eta\rangle_x+\frac L2\|\eta\|_x^2h(Rx​(η))≤h(x)+⟨gradh(x),η⟩x​+2L​∥η∥x2​;
  • retraction-convexity: qx=h∘Rxq_x=h\circ R_xqx​=h∘Rx​ satisfies qx(η)≥qx(ξ)+⟨ζ,η−ξ⟩xq_x(\eta)\ge q_x(\xi)+\langle\zeta,\eta-\xi\rangle_xqx​(η)≥qx​(ξ)+⟨ζ,η−ξ⟩x​, where ζ\zetaζ is the gradient of qxq_xqx​ at ξ\xiξ, or any Riemannian subgradient of qxq_xqx​ at ξ\xiξ when hhh is nonsmooth.

Assumption 3.1 asks that FFF be bounded below and Ωx0\Omega_{x_0}Ωx0​​ compact. Assumption 3.3 provides an open Ω⊇Ωx0\Omega\supseteq\Omega_{x_0}Ω⊇Ωx0​​ on which fff is LLL-retraction-smooth and retraction-convex and ggg is retraction-convex. Assumption 3.4 bounds how far the retraction is from Euclidean: for all x,y,z∈Ωx,y,z\in\Omegax,y,z∈Ω,

∣∥Rx−1(z)−Rx−1(y)∥x2−∥Ry−1(z)∥y2∣≤κΩ∥Rx−1(y)∥x2.\bigl|\|R_x^{-1}(z)-R_x^{-1}(y)\|_x^2-\|R_y^{-1}(z)\|_y^2\bigr|\le\kappa_\Omega\|R_x^{-1}(y)\|_x^2 .​∥Rx−1​(z)−Rx−1​(y)∥x2​−∥Ry−1​(z)∥y2​​≤κΩ​∥Rx−1​(y)∥x2​.

Finally, β=(L~−L)/2\beta=(\tilde L-L)/2β=(L~−L)/2.

Formalization targets

Goal: Theorem 3.2

Let L~>max⁡(L,0)\tilde L>\max(L,0)L~>max(L,0), suppose Assumptions 3.1, 3.3 and 3.4 hold, and let x∗x_*x∗​ be any accumulation point of {xk}\{x_k\}{xk​}. Then for every k≥1k\ge1k≥1

F(xk)−F(x∗)≤1k(L~2∥Rx0−1(x∗)∥x02+L~κΩ2β(F(x0)−F(x∗))).(3.16)F(x_k)-F(x_*)\le\frac1k\left(\frac{\tilde L}{2}\|R_{x_0}^{-1}(x_*)\|_{x_0}^2+\frac{\tilde L\kappa_\Omega}{2\beta}\bigl(F(x_0)-F(x_*)\bigr)\right).\tag{3.16}F(xk​)−F(x∗​)≤k1​(2L~​∥Rx0​−1​(x∗​)∥x0​2​+2βL~κΩ​​(F(x0​)−F(x∗​))).(3.16)

The constants are those of the paper.

Milestones

  1. Lemma 3.1 (descent): F(xk)−F(xk+1)≥β∥ηxk∗∥xk2F(x_k)-F(x_{k+1})\ge\beta\|\eta^*_{x_k}\|_{x_k}^2F(xk​)−F(xk+1​)≥β∥ηxk​∗​∥xk​2​.
  2. Lemma 3.4 (Riemannian three-point inequality): for one step z=Rx(ηx∗)z=R_x(\eta^*_x)z=Rx​(ηx∗​) and any y=Rx(ξx)∈Ωy=R_x(\xi_x)\in\Omegay=Rx​(ξx​)∈Ω, F(z)≤F(y)+L~2(∥ξx∥x2−∥ξx−ηx∗∥x2)F(z)\le F(y)+\frac{\tilde L}{2}(\|\xi_x\|_x^2-\|\xi_x-\eta^*_x\|_x^2)F(z)≤F(y)+2L~​(∥ξx​∥x2​−∥ξx​−ηx∗​∥x2​).
  3. (3.17): the one-step estimate obtained from Lemma 3.4 with y=x∗y=x_*y=x∗​ and from Assumption 3.4.
  4. (3.18): the one-step estimate with ∥ηxk∗∥2\|\eta^*_{x_k}\|^2∥ηxk​∗​∥2 replaced by the decrease of FFF.
  5. (3.19): the averaged estimate over the first kkk steps.

Significance

Theorem 3.2 extends the O(1/k)O(1/k)O(1/k) function-value rate of the proximal gradient method to manifolds and general retractions. The constant is explicit: it combines the initial distance ∥Rx0−1(x∗)∥\|R_{x_0}^{-1}(x_*)\|∥Rx0​−1​(x∗​)∥ with a correction proportional to κΩ\kappa_\OmegaκΩ​, which measures how far the retraction is from Euclidean. In the Euclidean case Rx(η)=x+ηR_x(\eta)=x+\etaRx​(η)=x+η one can take κΩ=0\kappa_\Omega=0κΩ​=0, and the bound reduces to the classical one. The rate concerns F(xk)−F(x∗)F(x_k)-F(x_*)F(xk​)−F(x∗​), which the iteration bound of Theorem 3.1 (the norm of ηxk∗\eta^*_{x_k}ηxk​∗​) does not control.

The result is proved in the paper. None of it is formalized, and no machine-checked version of the Euclidean proximal-gradient rate is on the platform either. A formalization would supply the first checked version of Clarke stationarity on tangent spaces, of the retraction-based convexity and smoothness notions, and of a rate proof for a nonsmooth Riemannian algorithm. These pieces carry over to other retraction-based methods, such as the accelerated variants of §4 of the paper.

Difficulty

The arithmetic of the rate proof is a telescoping sum, so the work lies elsewhere. First, Lemma 3.4 needs a usable form of the stationarity condition 0∈∂ℓx(ηx∗)0\in\partial\ell_x(\eta^*_x)0∈∂ℓx​(ηx∗​): a subgradient of g∘Rxg\circ R_xg∘Rx​ at ηx∗\eta^*_xηx∗​ equal to −(grad⁡f(x)+L~ηx∗)-(\operatorname{grad} f(x)+\tilde L\eta^*_x)−(gradf(x)+L~ηx∗​). This requires a sum rule for the Clarke subdifferential of a C1C^1C1 function plus a locally Lipschitz one, on a tangent space whose norm comes from the Riemannian metric rather than from the model space. Second, the gradient of f∘Rxf\circ R_xf∘Rx​ at 0x0_x0x​ has to be identified with grad⁡f(x)\operatorname{grad} f(x)gradf(x) through DRx(0x)=id\mathrm DR_x(0_x)=\mathrm{id}DRx​(0x​)=id. In Mathlib this mixes manifold derivatives (mfderiv) with Fréchet derivatives on a space carrying two equivalent norms. Third, it has to be shown that the iterates and the accumulation point remain in Ω\OmegaΩ, so that Assumptions 3.3 and 3.4 apply at every step.

Formalization scope

Theorem numbers and pages are those of arXiv:1909.06065v4. M\mathcal MM is a smooth manifold modelled on a finite-dimensional real inner-product space EEE, with Mathlib's RiemannianBundle on the tangent bundle. All norms and inner products on TxMT_x\mathcal MTx​M are the Riemannian ones. Retractions and gradients are the published RiemOpt.BFGS.IsRetraction and RiemOpt.FR.IsGradient. The Clarke derivative is an EReal-valued limit superior along N(η)×N>0(0)\mathcal N(\eta)\times\mathcal N_{>0}(0)N(η)×N>0​(0). Algorithm 1 is modelled as a run (sequences xkx_kxk​, ηxk∗\eta^*_{x_k}ηxk​∗​ with the three defining properties), and every statement holds for every run. Indices start at 000, accumulation points are cluster points of the sequence, and the bounds divided by kkk are stated for k≥1k\ge1k≥1.

The formalization commits to the following readings:

  1. LLL-retraction-smoothness is required for every tangent vector at the points of the set. This is a strengthening of Definition 3.1, which only covers η\etaη with Rx(η)R_x(\eta)Rx​(η) in the set, and it is needed because Lemma 3.1 fails under the literal reading.
  2. In retraction-convexity the vector ζ\zetaζ depends on ξ\xiξ. It is the gradient of f∘Rxf\circ R_xf∘Rx​, respectively any Clarke subgradient of g∘Rxg\circ R_xg∘Rx​, as the sentence after (3.10) states.
  3. κΩ\kappa_\OmegaκΩ​ is a single constant.
  4. R−1R^{-1}R−1 is data with Rx(Rx−1(y))=yR_x(R_x^{-1}(y))=yRx​(Rx−1​(y))=y on Ω\OmegaΩ, together with the identification Rxk−1(xk+1)=ηxk∗R_{x_k}^{-1}(x_{k+1})=\eta^*_{x_k}Rxk​−1​(xk+1​)=ηxk​∗​ that the proof uses.
  5. Local Lipschitz continuity of g∘Rxg\circ R_xg∘Rx​ is assumed, as p. 5 presupposes when it defines the subdifferential.

A single ζ\zetaζ for all η,ξ\eta,\xiη,ξ in (3.10) would make retraction-convexity force qxq_xqx​ to be affine, and the theorem would only cover affine problems. That reading is excluded. Statements with the case k=0k=0k=0, where Lean's 1/0=01/0=01/0=0 makes (3.16) false, are excluded as well.

Contributions welcome: a Clarke sum rule for C1C^1C1 plus locally Lipschitz functions, the identification of the Fréchet derivative of f∘Rxf\circ R_xf∘Rx​ at 000 with the Riemannian gradient, and the five milestones in order. The Clarke layer and the derivative identification are reusable beyond this mission.

Selected references

  • W. Huang, K. Wei, Riemannian proximal gradient methods, Mathematical Programming, 2021; extended version arXiv:1909.06065v4. https://arxiv.org/abs/1909.06065v4, https://doi.org/10.1007/s10107-021-01632-3
  • A. Beck, M. Teboulle, A fast iterative shrinkage-thresholding algorithm for linear inverse problems, SIAM J. Imaging Sciences, 2009. https://doi.org/10.1137/080716542
  • S. Chen, S. Ma, A. M.-C. So, T. Zhang, Proximal gradient method for nonsmooth optimization over the Stiefel manifold, SIAM J. Optimization, 2020. https://doi.org/10.1137/18M122457X
  • F. H. Clarke, Optimization and Nonsmooth Analysis, Wiley, 1983. https://doi.org/10.1137/1.9781611971309
  • P.-A. Absil, R. Mahony, R. Sepulchre, Optimization Algorithms on Matrix Manifolds, Princeton University Press, 2008. https://doi.org/10.1515/9781400830244
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Convex OptimizationOptimization·Captain: mikedeng1

Faster Convergence Rates of Relaxed Peaceman-Rachford and ADMM Under Regularity Assumptions III: With Lipschitz ∇g and Small Stepsize, the DRS Objective Error Is O(1/(k+1)) and o(1/(k+1))Research Paper

Why this rate matters

Douglas–Rachford splitting is a method for minimizing a sum of two convex functions when each function has an accessible proximal operator. Its iterates are easy to state, but the speed of convergence of the objective at an individual proximal point is less immediate than convergence of an averaged point or of a residual. For optimization models in which one summand has a Lipschitz continuous gradient, Davis and Yin give explicit objective-error bounds that depend on the proximal stepsize. Their paper compares these bounds with forward–backward splitting and shows that DRS has an objective rate at least as fast when the stepsize is sufficiently small.

The present mission formalizes the rate in Theorem 3.2 and the Appendix B estimates that state the relevant contraction, monotonicity and summability properties. The companion Theorem 3.3 concerns the squared fixed-point residual. Both results are proved in the 2015 arXiv version of the paper, which fixes the numbering and constants used here; the journal article appeared in Mathematics of Operations Research in 2017.

The DRS setting

Let HHH be a real Hilbert space. Let f:H→(−∞,+∞]f:H\to(-\infty,+\infty]f:H→(−∞,+∞] be proper, lower semicontinuous and convex, and let g:H→Rg:H\to\mathbb Rg:H→R be convex and differentiable with a (1/β)(1/\beta)(1/β)-Lipschitz gradient for some β>0\beta>0β>0. The proximal map of a function hhh at stepsize γ>0\gamma>0γ>0 sends zzz to the minimizer of h(x)+∥x−z∥2/(2γ)h(x)+\|x-z\|^2/(2\gamma)h(x)+∥x−z∥2/(2γ). Write Pf=prox⁡γfP_f=\operatorname{prox}_{\gamma f}Pf​=proxγf​ and Pg=prox⁡γgP_g=\operatorname{prox}_{\gamma g}Pg​=proxγg​, and let RP=2P−IR_P=2P-IRP​=2P−I be the reflection associated with a proximal map PPP.

The Peaceman–Rachford map is TPRS=RPf∘RPgT_{\mathrm{PRS}}=R_{P_f}\circ R_{P_g}TPRS​=RPf​​∘RPg​​. The DRS run is the relaxed PRS run with relaxation parameter 1/21/21/2 at every step:

zk+1=12zk+12TPRS(zk),xgk=Pg(zk),xfk=Pf(RPg(zk)).z^{k+1}=\tfrac12z^k+\tfrac12T_{\mathrm{PRS}}(z^k),\qquad x_g^k=P_g(z^k),\qquad x_f^k=P_f(R_{P_g}(z^k)).zk+1=21​zk+21​TPRS​(zk),xgk​=Pg​(zk),xfk​=Pf​(RPg​​(zk)).

Equivalently, zk+1=zk+xfk−xgkz^{k+1}=z^k+x_f^k-x_g^kzk+1=zk+xfk​−xgk​. The initial z0∈Hz^0\in Hz0∈H is arbitrary. Let z∗z^*z∗ be a fixed point of TPRST_{\mathrm{PRS}}TPRS​, and put x∗=Pg(z∗)x^*=P_g(z^*)x∗=Pg​(z∗). The objective value compared in this mission is at xfkx_f^kxfk​ for both summands: ek=f(xfk)+g(xfk)−f(x∗)−g(x∗)e_k=f(x_f^k)+g(x_f^k)-f(x^*)-g(x^*)ek​=f(xfk​)+g(xfk​)−f(x∗)−g(x∗). These values are finite under the standing assumptions. The section's Assumption 5 requires the smoothness of ggg and constant relaxation 1/21/21/2; it applies to Theorems 3.2 and 3.3 even though their own sentences do not repeat it.

Formalization targets

Objective error: Theorem 3.2

Let ρ=(1+5)/2\rho=(1+\sqrt5)/2ρ=(1+5​)/2 be the positive root of r3−2r−1=0r^3-2r-1=0r3−2r−1=0, and κ≈1.24698\kappa\approx1.24698κ≈1.24698 the positive root of r3+r2−2r−1=0r^3+r^2-2r-1=0r3+r2−2r−1=0. The first target bounds the best objective error at every k≥0k\ge0k≥0:

min⁡0≤i≤kei≤12γ(k+1){∥xg0−x∗∥2,γ<ρβ,∥xg0−x∗∥2+γ3/β−2γβ−β2β2+γ2∥z0−z∗∥2,γ≥ρβ.\min_{0\le i\le k}e_i\le\frac{1}{2\gamma(k+1)}\begin{cases}\|x_g^0-x^*\|^2,&\gamma<\rho\beta,\\\|x_g^0-x^*\|^2+\dfrac{\gamma^3/\beta-2\gamma\beta-\beta^2}{\beta^2+\gamma^2}\|z^0-z^*\|^2,&\gamma\ge\rho\beta.\end{cases}0≤i≤kmin​ei​≤2γ(k+1)1​⎩⎨⎧​∥xg0​−x∗∥2,∥xg0​−x∗∥2+β2+γ2γ3/β−2γβ−β2​∥z0−z∗∥2,​γ<ρβ,γ≥ρβ.​

For every γ>0\gamma>0γ>0, this best error is o(1/(k+1))o(1/(k+1))o(1/(k+1)). When γ<κβ\gamma<\kappa\betaγ<κβ, the same first-case upper bound holds for each eke_kek​, and ek=o(1/(k+1))e_k=o(1/(k+1))ek​=o(1/(k+1)). The goal states all four clauses together. The paper prints ρ≈2.2056\rho\approx2.2056ρ≈2.2056, the positive root of r3−2r2−1r^3-2r^2-1r3−2r2−1. That threshold does not match the coefficient γ3/β−2γβ−β2\gamma^3/\beta-2\gamma\beta-\beta^2γ3/β−2γβ−β2 the proof needs to be nonpositive, and with it the first case fails: for f=0f=0f=0, g(x)=x2/(2β)g(x)=x^2/(2\beta)g(x)=x2/(2β) on R\mathbb RR, γ=2β\gamma=2\betaγ=2β and k=0k=0k=0 the error is twice the bound. The mission states the theorem with the threshold the proof supports, the positive root of r3−2r−1r^3-2r-1r3−2r−1.

Fixed-point residual: Theorem 3.3

For γ<κβ\gamma<\kappa\betaγ<κβ and k≥1k\ge1k≥1, the companion target is

∥zk−zk+1∥2≤β2∥xg0−x∗∥2k2(1+γ/β)2(β2−γ2/κ2),∥zk−zk+1∥2=o(1/k2).\|z^k-z^{k+1}\|^2\le\frac{\beta^2\|x_g^0-x^*\|^2}{k^2(1+\gamma/\beta)^2(\beta^2-\gamma^2/\kappa^2)},\qquad \|z^k-z^{k+1}\|^2=o(1/k^2).∥zk−zk+1∥2≤k2(1+γ/β)2(β2−γ2/κ2)β2∥xg0​−x∗∥2​,∥zk−zk+1∥2=o(1/k2).

The Appendix B milestones give the contraction of the smooth gradient at proximal points, a fundamental one-step inequality, monotonicity, the extremal admissible stepsize ratio, and two summability bounds. Their constants and indices match the printed displays (B.1), (B.4), (B.7), (B.8), (B.10) and (B.12).

What the result supplies

The objective theorem gives a rate directly at the proximal point xfkx_f^kxfk​ when the stepsize is below the smaller threshold. Outside that regime, it still gives a best-iterate rate for every positive stepsize, including the explicit correction term for larger γ\gammaγ. The residual theorem controls the change in the DRS state at the faster squared rate. These statements let later work compare DRS against other splitting methods using the same objective and residual quantities, rather than changing the point at which the objective is measured.

The paper proves these results (Theorem 3.2 with the corrected threshold ρ\rhoρ); their statements are not new conjectures. The formalization work is to connect extended-real convex functions, actual proximal minimizers, smooth gradients, infinite sums, finite minima, and little-o assertions in a single Lean development. The seven Appendix B milestones are also useful as separately importable facts about proximal splitting. A machine-checked proof is still needed for the draft theorems of this mission.

Where the analysis is delicate

The familiar convergence of the DRS fixed-point residual does not by itself give the objective error at xfkx_f^kxfk​. An objective comparison involves the two different proximal points and the smooth gradient evaluated at successive xgkx_g^kxgk​. The large-stepsize regime changes the coefficient of the gradient increment and therefore changes the explicit bound. For the per-iterate conclusion, one must establish a monotone, summable quantity that dominates the objective error; a best-iterate estimate alone does not yield the stated nonergodic little-o claim. This explains why the mission retains the Appendix B estimates rather than replacing the goal with a generic O(1/k)O(1/k)O(1/k) statement.

Formalization scope

The Lean carrier is a complete real inner-product space. The proper, closed, convex predicate for fff and the proximal-map predicate are imported from the published ThreeOpSplitting.ConvexRates.Problem definition; the published MoreauProx.Characterization.GammaZero supplies the subgradient notion used by the paper's surrounding analysis. The smooth ggg is a real-valued function, with its actual gradient supplied by Mathlib's gradient and constrained by the imported smoothness predicate. Each proximal map is a function with the defining minimization property; the theorems do not assume an arbitrary map can stand in for a prox.

The fixed point z∗z^*z∗ is an explicit hypothesis, as in the paper. The two root constants are positive real numbers satisfying their defining cubics, never decimal approximations. A finite minimum ranges over i=0,…,ki=0,\ldots,ki=0,…,k; infinite sums come with summability; asymptotic claims use genuine little-o. The k≥1k\ge1k≥1 condition protects the k2k^2k2 denominator in Theorem 3.3. The objective error is taken at xfkx_f^kxfk​, never at xgkx_g^kxgk​, and the goal contains no auxiliary monotonicity or summability assumption that would assert part of its proof. Further contributions that establish proximal finiteness, the Appendix B inequalities, and the rates themselves fit within this scope.

Selected references

  • Damek Davis and Wotao Yin, Faster convergence rates of relaxed Peaceman-Rachford and ADMM under regularity assumptions, Mathematics of Operations Research 42(3), 2017. arXiv:1407.5210v3; DOI:10.1287/moor.2016.0827.
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