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Actuarial ScienceProbability·Captain: WillR

Actuarial Mathematics XIII: Annual Loss Allocation and Finite Hattendorff IdentityTextbook

Motivation and actuarial context

A prospective life insurance reserve describes the expected remaining loss on a policy at a valuation date. An alternative way to understand the insurer's total future loss is to allocate it between individual policy years. Each year produces an insurance cashflow and a change in the reserve needed to support future benefits. When properly centred by the reserve balance, the resulting annual gains have expectation zero. Hattendorff's theorem connects this allocation to the striking result that losses for distinct years are uncorrelated and the variance of total discounted loss is the sum of their individual discounted variances.

The classical finite annual result is covered by Gerber, Life Insurance Mathematics, third edition, §6.7, particularly equations (6.7.3) and (6.7.6)–(6.7.10) [1]. A modern actuarial derivation is developed in the European Actuarial Journal article An elementary derivation of Hattendorff's theorem [2]. The connection to martingale increments is emphasised by Norberg [3] and by Gerber, Leung and Shiu [4].

This mission formalises a finite-scenario annual-loss allocation and Hattendorff-style variance identity. It makes the distinction between a proved algebraic decomposition and the deeper stochastic theorem explicit: annual orthogonality is a hypothesis of the capstone, with its derivation from conditional mortality and reserve dynamics reserved for a subsequent extension. Thus the mission does not claim that an arbitrary pair of yearly cashflows is uncorrelated.

Finite mortality scenarios and expected values

Let Ω\OmegaΩ be a finite sample space, and let wωw_\omegawω​ denote the probability assigned to scenario ω\omegaω. A valid scenario probability law has nonnegative weights summing to one. The mission defines the finite weighted expectation

Ew[X]=∑ω∈ΩwωX(ω).\mathbb E_w[X]=\sum_{\omega\in\Omega}w_\omega X(\omega).Ew​[X]=ω∈Ω∑​wω​X(ω).

Its supporting results establish expected values of constants and linear combinations. For scenario cashflows XXX and YYY, weighted variance and covariance are defined by

Var⁡w(X)=∑ωwω(X(ω)−Ew[X])2,Cov⁡w(X,Y)=∑ωwω(X(ω)−Ew[X])(Y(ω)−Ew[Y]).\begin{aligned} \operatorname{Var}_w(X) &=\sum_\omega w_\omega \left(X(\omega)-\mathbb E_w[X]\right)^2,\\ \operatorname{Cov}_w(X,Y) &=\sum_\omega w_\omega \left(X(\omega)-\mathbb E_w[X]\right) \left(Y(\omega)-\mathbb E_w[Y]\right). \end{aligned}Varw​(X)Covw​(X,Y)​=ω∑​wω​(X(ω)−Ew​[X])2,=ω∑​wω​(X(ω)−Ew​[X])(Y(ω)−Ew​[Y]).​

The definitions work for arbitrary real arrays of weights, while the actuarial probability interpretation assumes valid scenario probabilities. Finite sums avoid moment-integrability issues without imposing an artificial condition such as independence between years.

Annual insurer gains and reserve changes

Let Ck(ω)C_k(\omega)Ck​(ω) be the net insurer cash outgo during policy year kkk, measured at that year's start, and let RkR_kRk​ be the deterministic opening prospective reserve under a given in-force valuation basis. With per-year discount factor vvv, define the annual gain or loss component

Gk(ω)=Ck(ω)+vRk+1−Rk.G_k(\omega)=C_k(\omega)+vR_{k+1}-R_k.Gk​(ω)=Ck​(ω)+vRk+1​−Rk​.

The term vRk+1vR_{k+1}vRk+1​ represents the discounted liability carried into the next year, while RkR_kRk​ is the reserve released from the opening position. The sign convention is insurer loss, so positive values represent net outgo or an adverse change.

If the annual reserve balance is

Ew[Ck]+vRk+1=Rk,\mathbb E_w[C_k]+vR_{k+1}=R_k,Ew​[Ck​]+vRk+1​=Rk​,

then linearity gives

Ew[Gk]=0.\mathbb E_w[G_k]=0.Ew​[Gk​]=0.

This is the first actuarial component of Hattendorff's framework: properly reserved annual losses are centred under the valuation basis. The finite scenario weights need to sum to one, and the reserve balance must be assumed or established. Merely defining GkG_kGk​ does not give it zero mean.

Discounted loss allocation and telescoping

The total discounted annual gain through nnn years is

Ln(ω)=∑0≤k<nvkGk(ω).L_n(\omega)=\sum_{0\le k<n}v^kG_k(\omega).Ln​(ω)=0≤k<n∑​vkGk​(ω).

Expanding the annual gain definition and telescoping the reserve terms gives the pathwise identity

Ln(ω)=∑0≤k<nvkCk(ω)+vnRn−R0.\boxed{ L_n(\omega)= \sum_{0\le k<n}v^k C_k(\omega) +v^n R_n-R_0. }Ln​(ω)=0≤k<n∑​vkCk​(ω)+vnRn​−R0​.​

The terminal reserve is retained explicitly. It must not be assumed zero for an arbitrary incomplete policy horizon. This exact finite-period formula corresponds to the annual allocation of loss and reserve changes discussed in [1, §6.7, equation (6.7.3)], with the horizon and terminal liability clearly stated.

The empty-term case has L0=0L_0=0L0​=0. Increasing the horizon from nnn to n+1n+1n+1 adds precisely vnGnv^nG_nvnGn​. These boundary and recursion lemmas form a useful independent verification layer for the finite sum.

Orthogonality and the variance decomposition

When distinct annual gains have zero covariance,

Cov⁡w(Gi,Gj)=0(i≠j,  i,j<n),\operatorname{Cov}_w(G_i,G_j)=0 \qquad (i\ne j,\;i,j<n),Covw​(Gi​,Gj​)=0(i=j,i,j<n),

their discounted aggregate variance has no cross-year terms:

Var⁡w(Ln)=∑0≤k<nv2kVar⁡w(Gk).\boxed{ \operatorname{Var}_w(L_n) =\sum_{0\le k<n}v^{2k}\operatorname{Var}_w(G_k). }Varw​(Ln​)=0≤k<n∑​v2kVarw​(Gk​).​

Importantly, uncorrelated does not mean independent. Annual losses are linked by the same insured life, survival history and reserve process. Hattendorff's theorem establishes the required uncorrelatedness from the correct conditional insurance model; the zero-covariance condition is an explicit hypothesis in this mission's finite-scenario algebraic capstone. This distinction is important for the formalisation and is consistent with [1, equations (6.7.6)–(6.7.8)] and the martingale explanation in [3–4].

The supporting theorem on variance of a sum, variance scaling and covariance symmetry makes the algebra behind the annual allocation explicit. Zero-mean gain and zero-covariance assumptions must be separately justified when moving from this finite abstract setting to a particular mortality model.

Capstone and subsequent formal development

The capstone assumes a finite scenario law whose weights sum to one, a sequence of yearly cashflows CkC_kCk​, deterministic reserves RkR_kRk​, a reserve balance for each year k<nk<nk<n, and pairwise zero covariance of the resulting annual gains. It then proves three statements together: each year's gain is centred, the discounted variance splits additively by year, and the discounted sum telescopes to net cashflows plus the terminal reserve less opening reserve.

Five definitions establish weighted expectation, annual reserve gain, discounted aggregate gain, variance and covariance. Thirteen supporting theorem targets handle elementary expectation algebra, finite-year telescoping, zero-mean reserve gains, covariance symmetry and orthogonal variance decomposition. A capstone combines these results.

This is explicitly the finite algebraic and reserve-accounting stage, not a complete proof of Hattendorff's theorem for arbitrary life insurance contracts. A later mission should construct the curtate-lifetime annual innovations using the published reserve recursions of Mission XI, establish the conditional mean-zero property from survival information and derive cross-year orthogonality without assuming it. Only that later bridge will discharge the substantive stochastic obligation. No independence claim is made.

Every item is a proposed Lean statement. The isolated-module imports appear before other Lean commands, and no unpublished definition is treated as already available to the live compiler.

References

[1] Gerber, Hans U. (1997), Life Insurance Mathematics, third edition, Springer, Chapter 6, §6.7, Allocation of the Overall Loss to Policy Years, equations (6.7.3)–(6.7.10). Publisher book record.

[2] An elementary derivation of Hattendorff's theorem, European Actuarial Journal (2021), DOI: 10.1007/s13385-020-00256-9. Develops the annual insurer-loss formula using the prospective reserve recurrence.

[3] Norberg, Ragnar (1992), “Hattendorff's theorem and Thiele's differential equation generalized”, Scandinavian Actuarial Journal, pp. 2–14. Places the annual uncorrelated-loss principle in a broader stochastic and martingale setting.

[4] Gerber, Hans U., Leung, Bartholomew P. K. and Shiu, Elias S. W. (2003), “Indicator Function and Hattendorff Theorem”, North American Actuarial Journal, 7(1), pp. 38–47. Relates the actuarial theorem to uncorrelated martingale increments.

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Actuarial ScienceProbability·Captain: WillR

Actuarial Mathematics XIV: Multiple-Decrement Annual Reserve PremiumsTextbook

Motivation and actuarial context

A traditional life-insurance model may have one way of exiting the insured state, namely death. Many actuarial contracts instead allow multiple mutually exclusive decrements. A policyholder might exit through death, disability, withdrawal or retirement, and different causes may trigger different benefits. A net premium reserve must therefore allow one-year payments that vary by the cause of exit, as well as the liability continuing for policies that do not exit.

Gerber, Life Insurance Mathematics, third edition, Chapter 7 §7.5 [1], derives the multiple-decrement reserve and its one-year recursion, followed by a decomposition of premium into reserve accumulation and the expected cost of the net amounts at risk. The same models are related to the broader multiple-state framework developed in Dickson, Hardy and Waters (2009), Chapter 8, including §8.8 on multiple decrements [2].

This mission formalises the one-year multiple-decrement reserve balance and premium decomposition for a finite set of causes. It is a deliberately local actuarial model: it handles one policy year and deterministic opening and closing reserves, without assuming that the complete lifetime-dependent reserve functions from Missions XI or XII have already been published.

One-year decrement law

Let JJJ be a finite set of mutually exclusive causes of exit. Fix a policy in force at the start of the year. Let ppp denote the conditional probability of surviving in force to the following year, and qjq_jqj​ the conditional probability of decrement cause j∈Jj\in Jj∈J during the year.

The one-year decrement law is valid when

p≥0,qj≥0,p+∑j∈Jqj=1.p\ge0,\qquad q_j\ge0,\qquad p+\sum_{j\in J}q_j=1.p≥0,qj​≥0,p+j∈J∑​qj​=1.

The possible decrement causes are alternative outcomes of the same year. Their probabilities are added because the causes are mutually exclusive; they are not independent risks. The survival probability refers to remaining in force, rather than necessarily being alive in every possible post-decrement state.

The formal model treats JJJ as any finite type. No nonempty-type hypothesis is required: if JJJ is empty, the unit-probability law forces p=1p=1p=1 and reduces to certain survival, without exit benefits.

Benefit payments and the annual reserve balance

Let bjb_jbj​ be the benefit payable at the end of the year following exit for cause jjj. The conditional expected exit benefit before discounting is

B=∑j∈Jqjbj.B=\sum_{j\in J}q_jb_j.B=j∈J∑​qj​bj​.

Let RRR be the reserve immediately before the current premium, let R+R_+R+​ denote the reserve required at the next annual valuation for surviving policies, and let vvv be the annual discount factor. Assume the year-end reserve for policies which exit is zero after payment of the cause-specific benefit. Under this timing, the expected present value of the following-year liability is

v(pR++∑j∈Jqjbj).v\left(pR_+ +\sum_{j\in J}q_jb_j\right).v​pR+​+j∈J∑​qj​bj​​.

The required premium Π\PiΠ is defined by the annual reserve balance

R+Π=v(pR++∑j∈Jqjbj).\boxed{R+\Pi=v\left(pR_+ +\sum_{j\in J}q_jb_j\right).}R+Π=v​pR+​+j∈J∑​qj​bj​​.​

Equivalently, the formula defines

Π=v(pR++B)−R.\Pi=v\left(pR_++B\right)-R.Π=v(pR+​+B)−R.

This is the discrete conditional one-year multiple-decrement generalisation of the annual life-reserve recursion in [1, equation (7.5.2)]. It does not assert that the reserves RRR and R+R_+R+​ were derived from a complete prospective valuation, nor that an arbitrary premium chosen externally automatically satisfies the balance. Those tasks require a separate multi-year model.

Savings and risk premium components

The one-year required premium can be separated into two economically interpretable parts. The savings premium grows the opening reserve towards the next reserve:

Πsav=vR+−R.\Pi^{\mathrm{sav}}=vR_+-R.Πsav=vR+​−R.

The risk premium finances benefits above or below the amount of reserve that would otherwise remain at the next annual valuation:

Πrisk=v∑j∈Jqj(bj−R+).\Pi^{\mathrm{risk}}= v\sum_{j\in J}q_j(b_j-R_+).Πrisk=vj∈J∑​qj​(bj​−R+​).

Since the decrement law satisfies ∑jqj=1−p\sum_jq_j=1-p∑j​qj​=1−p,

Πsav+Πrisk=vR+−R+v∑jqj(bj−R+)=v(pR++∑jqjbj)−R=Π.\begin{aligned} \Pi^{\mathrm{sav}}+\Pi^{\mathrm{risk}} &=vR_+-R+ v\sum_jq_j(b_j-R_+)\\ &=v\left(pR_++\sum_jq_jb_j\right)-R\\ &=\Pi. \end{aligned}Πsav+Πrisk​=vR+​−R+vj∑​qj​(bj​−R+​)=v(pR+​+j∑​qj​bj​)−R=Π.​

Thus the principal premium decomposition is

Π=Πsav+Πrisk.\boxed{\Pi=\Pi^{\mathrm{sav}}+\Pi^{\mathrm{risk}}.}Π=Πsav+Πrisk.​

This follows the savings and risk-premium interpretation of [1, equations (7.5.3)–(7.5.5)]. A negative risk premium is possible algebraically when cause benefits are lower than the continuing reserve. The formal theorem does not assume all monetary amounts are nonnegative.

Boundary cases and formal theorem graph

If p=0p=0p=0, every in-force policy exits during the year, and the continuing reserve term vanishes:

Π=vB−R.\Pi=vB-R.Π=vB−R.

If no decrement can occur, p=1p=1p=1 and qj=0q_j=0qj​=0 for every cause, the required premium reduces to the savings component alone,

Π=Πsav=vR+−R.\Pi=\Pi^{\mathrm{sav}}=vR_+-R.Π=Πsav=vR+​−R.

If every cause of exit pays exactly the same amount as the following-year reserve, bj=R+b_j=R_+bj​=R+​, the risk component is zero. Scaling all monetary benefits and reserve amounts by a common factor scales the premium by that factor.

The draft introduces five definitions: a valid annual decrement law, expected cause benefit, required annual premium, savings premium and risk premium. Eleven supporting theorems establish probability conditions, zero and scaled benefits, reserve balance, zero-survival and no-decrement limits, risk-free exits and the premium decomposition. The capstone combines the one-year reserve balance with the savings/risk identity.

The definitions and theorem types are independent of unconfirmed Prove2Me actuarial declarations from earlier missions. Imports of local definitions are explicitly placed at the beginning of each Lean file, and the proposed statements do not treat a Draft declaration as a published theorem. The proofs of the individual statements remain to be supplied after captain and moderator review.

References

[1] Gerber, Hans U. (1997), Life Insurance Mathematics, third edition, Springer, Chapter 7, Multiple Decrements, §7.5, The Net Premium Reserve, equations (7.5.1)–(7.5.5). In particular (7.5.2) is the annual multiple-decrement recursion and (7.5.3)–(7.5.5) separate the savings and risk portions.

[2] Dickson, David C. M., Hardy, Mary R. and Waters, Howard R. (2009), Actuarial Mathematics for Life Contingent Risks, first edition, Chapter 8, Cambridge University Press, §8.8, Multiple Decrement Models.

[3] Dickson, Hardy and Waters (2009), Chapter 7, Policy Values, annual policy-value recursions. The one-cause formula provides the earlier special case from which the multiple-cause generalisation develops.

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Machine LearningOptimizationProbability+1·Captain: mikedeng1

Global Convergence of Policy Gradient Methods to (Almost) Locally Optimal Policies: Random-Horizon Policy Gradient with Robbins–Monro Stepsizes Drives the Policy Gradient to Zero Almost SurelyResearch Paper

Motivation

Policy gradient methods are the main family of reinforcement learning algorithms that search directly over a parameterized class of stochastic policies πθ\pi_\thetaπθ​, θ∈Rd\theta\in\mathbb R^dθ∈Rd, by stochastic gradient ascent on the expected discounted return. They underlie REINFORCE, actor-critic methods and their deep-learning descendants. The return is a nonconvex function of θ\thetaθ, and the gradient is available only through Monte Carlo samples of trajectories, so the basic question is what the iterates of such a method converge to.

Classical analyses of actor-critic algorithms (Konda and Tsitsiklis, 2003) use the ODE method of stochastic approximation and assume that the gradient estimate is unbiased. In the infinite-horizon discounted setting, a trajectory of finite length cannot by itself produce an unbiased sample of the gradient. Zhang, Koppel, Zhu and Başar (arXiv:1906.08383, SIAM J. Control Optim. 58(6), 2020) resolve this with random horizons: drawing the trajectory lengths from geometric distributions makes the resulting estimate exactly unbiased and almost surely bounded. They then prove convergence of the resulting random-horizon policy gradient (RPG) algorithm with the supermartingale convergence theorem, an optimization argument that also yields rates. This mission formalizes that first part of the paper (§2–§4 and App. A.1–A.4). The paper's later results on escaping saddle points are not part of it.

Setting

A finite Markov decision process is a tuple (S,A,P,R,γ)(\mathcal S,\mathcal A,P,R,\gamma)(S,A,P,R,γ): finite state and action sets, transition probabilities P(s′∣s,a)P(s'\mid s,a)P(s′∣s,a), rewards R(s,a)R(s,a)R(s,a) and a discount factor γ∈(0,1)\gamma\in(0,1)γ∈(0,1). A stochastic policy π\piπ gives a probability vector π(⋅∣s)\pi(\cdot\mid s)π(⋅∣s) on A\mathcal AA at each state. Its value Vπ(s)=E(∑t≥0γtR(st,at)∣s0=s)V_\pi(s)=\mathbb E\big(\sum_{t\ge0}\gamma^tR(s_t,a_t)\mid s_0=s\big)Vπ​(s)=E(∑t≥0​γtR(st​,at​)∣s0​=s) and Q-function Qπ(s,a)Q_\pi(s,a)Qπ​(s,a) are the expected discounted returns from a state, respectively a state-action pair.

A parameterized policy assigns to each θ∈Rd\theta\in\mathbb R^dθ∈Rd a policy πθ\pi_\thetaπθ​. Fix an initial state s0s_0s0​. The objective is

J(θ)=Vπθ(s0),max⁡θ∈RdJ(θ).J(\theta)=V_{\pi_\theta}(s_0),\qquad \max_{\theta\in\mathbb R^d}J(\theta).J(θ)=Vπθ​​(s0​),θ∈Rdmax​J(θ).

The score function is ∇θlog⁡πθ(a∣s)\nabla_\theta\log\pi_\theta(a\mid s)∇θ​logπθ​(a∣s). The discounted state-occupancy measure is ρπθ(s)=(1−γ)∑t≥0γtp(st=s∣s0,πθ)\rho_{\pi_\theta}(s)=(1-\gamma)\sum_{t\ge0}\gamma^tp(s_t=s\mid s_0,\pi_\theta)ρπθ​​(s)=(1−γ)∑t≥0​γtp(st​=s∣s0​,πθ​), and ρθ(s,a)=ρπθ(s)πθ(a∣s)\rho_\theta(s,a)=\rho_{\pi_\theta}(s)\pi_\theta(a\mid s)ρθ​(s,a)=ρπθ​​(s)πθ​(a∣s).

Assumption 3.1 asks for ∣R(s,a)∣≤UR|R(s,a)|\le U_R∣R(s,a)∣≤UR​ and for a differentiable policy whose score exists, is LΘL_\ThetaLΘ​-Lipschitz in θ\thetaθ and is bounded in norm by BΘ>0B_\Theta>0BΘ​>0. Two constants recur below:

L=URLΘ(1−γ)2+(1+γ)URBΘ2(1−γ)3,ℓ^=BΘUR(1−γ)(1−γ1/2).L=\frac{U_RL_\Theta}{(1-\gamma)^2}+\frac{(1+\gamma)U_RB_\Theta^2}{(1-\gamma)^3},\qquad \hat\ell=\frac{B_\Theta U_R}{(1-\gamma)(1-\gamma^{1/2})}.L=(1−γ)2UR​LΘ​​+(1−γ)3(1+γ)UR​BΘ2​​,ℓ^=(1−γ)(1−γ1/2)BΘ​UR​​.

The RPG algorithm (Algorithm 3) works as follows at the current iterate θk\theta_kθk​:

  1. Draw a horizon T∼Geom(1−γ)T\sim\mathrm{Geom}(1-\gamma)T∼Geom(1−γ) and simulate s0,a0,…,sT,aTs_0,a_0,\dots,s_T,a_Ts0​,a0​,…,sT​,aT​ under πθk\pi_{\theta_k}πθk​​.
  2. From the last pair (sT,aT)(s_T,a_T)(sT​,aT​), the subroutine EstQ draws an independent T′∼Geom(1−γ1/2)T'\sim\mathrm{Geom}(1-\gamma^{1/2})T′∼Geom(1−γ1/2), rolls out T′T'T′ further steps and returns Q^=∑t=0T′γt/2R(st,at)\hat Q=\sum_{t=0}^{T'}\gamma^{t/2}R(s_t,a_t)Q^​=∑t=0T′​γt/2R(st​,at​).
  3. Update
θk+1=θk+αk∇^J(θk),∇^J(θ)=11−γQ^ ∇log⁡πθ(aT∣sT).\theta_{k+1}=\theta_k+\alpha_k\hat\nabla J(\theta_k),\qquad \hat\nabla J(\theta)=\frac{1}{1-\gamma}\hat Q\,\nabla\log\pi_\theta(a_T\mid s_T).θk+1​=θk​+αk​∇^J(θk​),∇^J(θ)=1−γ1​Q^​∇logπθ​(aT​∣sT​).

Assumption 4.1 is the Robbins–Monro condition ∑kαk=∞\sum_k\alpha_k=\infty∑k​αk​=∞, ∑kαk2<∞\sum_k\alpha_k^2<\infty∑k​αk2​<∞.

Formalization targets

Goal: Theorem 4.2, in the form its proof establishes

Under Assumptions 3.1 and 4.1, almost surely

lim⁡k→∞∥∇J(θk)∥=0,\lim_{k\to\infty}\|\nabla J(\theta_k)\|=0,k→∞lim​∥∇J(θk​)∥=0,

and almost surely every cluster point θˉ\bar\thetaθˉ of (θk)(\theta_k)(θk​) satisfies ∇J(θˉ)=0\nabla J(\bar\theta)=0∇J(θˉ)=0. The page states the conclusion as "lim⁡kθk∈Θ∗\lim_k\theta_k\in\Theta^*limk​θk​∈Θ∗", where Θ∗\Theta^*Θ∗ is the set of stationary points. Read literally, that asserts convergence of θk\theta_kθk​, which fails when JJJ has no stationary point at all (one state, two actions, a softmax policy). The goal states what the proof on p. 30 concludes.

Milestones

  1. ∣Qπ(s,a)∣,∣Vπ(s)∣≤UR/(1−γ)|Q_\pi(s,a)|,|V_\pi(s)|\le U_R/(1-\gamma)∣Qπ​(s,a)∣,∣Vπ​(s)∣≤UR​/(1−γ) (p. 6).
  2. The policy gradient theorem (3.4): ∇J(θ)=11−γE(s,a)∼ρθ[∇log⁡πθ(a∣s)Qπθ(s,a)]\nabla J(\theta)=\frac1{1-\gamma}\mathbb E_{(s,a)\sim\rho_\theta}[\nabla\log\pi_\theta(a\mid s)Q_{\pi_\theta}(s,a)]∇J(θ)=1−γ1​E(s,a)∼ρθ​​[∇logπθ​(a∣s)Qπθ​​(s,a)].
  3. Lemma 3.2: ∇J\nabla J∇J is LLL-Lipschitz.
  4. Theorem 3.4, ∇^J\hat\nabla J∇^J clauses: E∇^J(θ)=∇J(θ)\mathbb E\hat\nabla J(\theta)=\nabla J(\theta)E∇^J(θ)=∇J(θ), ∥∇J(θ)∥≤BΘUR/(1−γ)2\|\nabla J(\theta)\|\le B_\Theta U_R/(1-\gamma)^2∥∇J(θ)∥≤BΘ​UR​/(1−γ)2, ∥∇^J(θ)∥≤ℓ^\|\hat\nabla J(\theta)\|\le\hat\ell∥∇^J(θ)∥≤ℓ^ a.s.
  5. Lemma A.1: the ascent inequality (A.23), and Wk=J(θk)−Lℓ^2∑j≥kαj2W_k=J(\theta_k)-L\hat\ell^2\sum_{j\ge k}\alpha_j^2Wk​=J(θk​)−Lℓ^2∑j≥k​αj2​ is a bounded submartingale with E[Wk+1∣Fk]≥Wk+αk∥∇J(θk)∥2\mathbb E[W_{k+1}\mid\mathcal F_k]\ge W_k+\alpha_k\|\nabla J(\theta_k)\|^2E[Wk+1​∣Fk​]≥Wk​+αk​∥∇J(θk​)∥2.
  6. (A.26): ∑kαk∥∇J(θk)∥2<∞\sum_k\alpha_k\|\nabla J(\theta_k)\|^2<\infty∑k​αk​∥∇J(θk​)∥2<∞ a.s.
  7. (A.27): lim inf⁡k∥∇J(θk)∥=0\liminf_k\|\nabla J(\theta_k)\|=0liminfk​∥∇J(θk​)∥=0 a.s.

Companion: Corollary 4.4 in its explicit form (A.37)

With constant stepsize α>0\alpha>0α>0 and Assumption 3.1 only, for every k≥1k\ge1k≥1,

1k∑m=1kE∥∇J(θm)∥2≤1kα⋅2UR1−γ+Lαℓ^2.\frac1k\sum_{m=1}^k\mathbb E\|\nabla J(\theta_m)\|^2\le\frac{1}{k\alpha}\cdot\frac{2U_R}{1-\gamma}+L\alpha\hat\ell^2.k1​m=1∑k​E∥∇J(θm​)∥2≤kα1​⋅1−γ2UR​​+Lαℓ^2.

Significance

The theorem shows that Monte Carlo policy gradient, with a sampling scheme that can be implemented from simulated trajectories alone, behaves like an exact stochastic gradient method on a smooth nonconvex objective. It needs no ODE approximation, no two-timescale critic and no assumption that the estimate is unbiased: unbiasedness is proved (Theorem 3.4). The same estimates give the finite-time bound of Corollary 4.4 and are the starting point of the paper's second part, which adds perturbations to escape saddle points.

To our knowledge none of these results has been machine-checked. The mission's work is to formalize the known proof: the infinite-horizon policy gradient theorem with a vector parameter, the smoothness bound with its explicit constant, the exact law of the random-horizon estimator and its moments, and the supermartingale argument. The formal statements also repair three misprints of the source: the conclusion of Theorem 4.2, the tail ∑j=k∞αk2\sum_{j=k}^\infty\alpha_k^2∑j=k∞​αk2​ of (A.22), which is read as ∑j≥kαj2\sum_{j\ge k}\alpha_j^2∑j≥k​αj2​, and the O(⋅)O(\cdot)O(⋅) of Corollary 4.4, which is replaced by its explicit form (A.37).

Difficulty

Each step of the argument is standard on paper. The work is in the parts that the paper treats in one line:

  • Unbiasedness. It rests on two separate identities. The law of the last state of a Geom(1−γ)\mathrm{Geom}(1-\gamma)Geom(1−γ)-length trajectory is ρπθ\rho_{\pi_\theta}ρπθ​​. A γ1/2\gamma^{1/2}γ1/2-discounted sum over a Geom(1−γ1/2)\mathrm{Geom}(1-\gamma^{1/2})Geom(1−γ1/2) horizon has the mean of a γ\gammaγ-discounted infinite sum. Both are exchanges of infinite sums over trajectories of unbounded length.
  • Smoothness. Lemma 3.2 requires differentiating JJJ twice through an infinite series of policy-dependent transition matrices, with bounds uniform in θ\thetaθ.
  • The final step. (A.26) and the non-summability of the stepsizes give only lim inf⁡∥∇J(θk)∥=0\liminf\|\nabla J(\theta_k)\|=0liminf∥∇J(θk​)∥=0. Upgrading this to a limit needs a separate pathwise argument, which uses the Lipschitz continuity of ∇J\nabla J∇J and the almost sure convergence of the martingale part of the iterates. The tempting first idea, that a summable series with non-summable weights forces its terms to zero, is false.

Formalization scope

  • Finite case. The state and action spaces are finite types. The paper also allows compact real vector spaces; this mission does not cover them. Values, Q-functions and occupation probabilities are the published FoundationsML layer (PolicyValue, QFunction, OccupationDist, IsPolicy, IsTransitionKernel). Rd\mathbb R^dRd is EuclideanSpace ℝ (Fin d), and ∇\nabla∇ is Mathlib's gradient.
  • Assumption 3.1 includes πθ(a∣s)>0\pi_\theta(a\mid s)>0πθ​(a∣s)>0: this is the reading of "the score function exists", since log⁡0\log 0log0 is a junk value in Lean. It also states LΘ≥0L_\Theta\ge0LΘ​≥0, which is implicit in "LΘL_\ThetaLΘ​-Lipschitz".
  • The algorithm is encoded by its exact sampling law. rpgLaw θ is the law of ∇^J(θ)\hat\nabla J(\theta)∇^J(θ), built from the geometric horizons, the trajectory probabilities and EstQ. A run is a filtered probability space carrying θk\theta_kθk​ and gkg_kgk​ with θk+1=θk+αkgk\theta_{k+1}=\theta_k+\alpha_kg_kθk+1​=θk​+αk​gk​ on every path, θk\theta_kθk​ adapted, and the conditional law of gkg_kgk​ given Fk\mathcal F_kFk​ equal to rpgLaw θ_k.
  • Ruled out. Postulating an abstract "unbiased bounded oracle" in place of rpgLaw would assume Theorem 3.4 and turn the goal into generic SGD; that encoding is ruled out. A sorry-free example shows that the run hypothesis is satisfiable and that rpgLaw is a probability measure.
  • Stepsizes and limits. The stepsizes are positive; the page says only "stepsize", and its proofs divide by αk\alpha_kαk​. Divergence of ∑αk\sum\alpha_k∑αk​ is Tendsto of the partial sums to +∞+\infty+∞. "Cluster point" is MapClusterPt.
  • Contributions welcome: proofs of any milestone, in particular the infinite-horizon policy gradient theorem with vector parameters and the unbiasedness of rpgLaw. These are reusable for every Monte Carlo policy gradient analysis.

Selected references

  • K. Zhang, A. Koppel, H. Zhu, T. Başar, Global Convergence of Policy Gradient Methods to (Almost) Locally Optimal Policies, SIAM J. Control Optim. 58(6), 2020. https://arxiv.org/abs/1906.08383 (v3 is the source of this mission)
  • R. S. Sutton, D. McAllester, S. Singh, Y. Mansour, Policy Gradient Methods for Reinforcement Learning with Function Approximation, NeurIPS 1999. https://papers.nips.cc/paper/1713-policy-gradient-methods-for-reinforcement-learning-with-function-approximation
  • V. R. Konda, J. N. Tsitsiklis, On Actor-Critic Algorithms, SIAM J. Control Optim. 42(4), 2003. https://doi.org/10.1137/S0363012901385691
  • D. P. Bertsekas, J. N. Tsitsiklis, Gradient Convergence in Gradient Methods with Errors, SIAM J. Optim. 10(3), 2000. https://doi.org/10.1137/S1052623497331063
  • H. Robbins, D. Siegmund, A Convergence Theorem for Non Negative Almost Supermartingales and Some Applications, in Optimizing Methods in Statistics, 1971. https://doi.org/10.1016/B978-0-12-604550-5.50015-8
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🏆Completed
Functional AnalysisNumerical AnalysisOptimization·Captain: mikedeng1

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

Motivation

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

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

Setting

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

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

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

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

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

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

Formalization targets

Goal: Theorem 3.4

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

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

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

Milestones

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

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

Significance

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

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

Difficulty

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

Formalization scope

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

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

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

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

Selected references

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

Stability Results on the Circumference of a Graph 2: A 2-Connected G with δ ≥ k, Circumference 10 ≤ c < n and e(G) > max{f(n,k+1,c), f(n,⌊c/2⌋−1,c)} Lies in W_{n,k,c}, W_{n,⌊c/2⌋,c}, X∪Y or Z_{n,k,c}Research Paper

Motivation

How many edges can a graph have if it contains no long cycle? This Turán-type question for the circumference goes back to Erdős and Gallai (1959), who showed that an nnn-vertex graph with circumference ccc has at most c(n−1)/2c(n-1)/2c(n−1)/2 edges. For 2-connected graphs the answer is exact and the extremal graphs are known, so the natural next question is stability: what does a graph look like when its edge count is just below the extremal value? Such statements are the standard input for exact results via the stability method, and for counting and spectral variants of the original problem.

Timeline.

  • 1959. Erdős and Gallai prove e(G)≤c(G)(n−1)/2e(G)\le c(G)(n-1)/2e(G)≤c(G)(n−1)/2.
  • 1976. Woodall asks for a bound for 2-connected graphs that also takes the minimum degree kkk into account: e(G)≤max⁡{f(n,k,c),f(n,⌊c/2⌋,c)}e(G)\le\max\{f(n,k,c),f(n,\lfloor c/2\rfloor,c)\}e(G)≤max{f(n,k,c),f(n,⌊c/2⌋,c)} when c(G)=c≤n−1c(G)=c\le n-1c(G)=c≤n−1 and δ(G)≥k\delta(G)\ge kδ(G)≥k.
  • 1977. Kopylov proves the case without minimum degree, the bound max⁡{f(n,2,c),f(n,⌊c/2⌋,c)}\max\{f(n,2,c),f(n,\lfloor c/2\rfloor,c)\}max{f(n,2,c),f(n,⌊c/2⌋,c)} for 2-connected graphs. His proof can be modified to settle Woodall's question.
  • 2016–2018. Füredi, Kostochka, Verstraëte and Luo prove the stability version of Kopylov's theorem for 10≤c≤n−110\le c\le n-110≤c≤n−1. Above max⁡{f(n,3,c),f(n,⌊c/2⌋−1,c)}\max\{f(n,3,c),f(n,\lfloor c/2\rfloor-1,c)\}max{f(n,3,c),f(n,⌊c/2⌋−1,c)} edges, GGG lies in Wn,2,cW_{n,2,c}Wn,2,c​ or Wn,⌊c/2⌋,cW_{n,\lfloor c/2\rfloor,c}Wn,⌊c/2⌋,c​, or, for odd ccc, in a member of two families Xn,c\mathcal X_{n,c}Xn,c​, Yn,c\mathcal Y_{n,c}Yn,c​.
  • 2016–2017. Li and Ning, and independently Füredi, Kostochka and Luo, prove the stability version of Erdős's minimum-degree theorem for non-Hamiltonian graphs.
  • 2017–2020. Ma and Ning prove a stability version of Woodall's bound for every minimum degree kkk (arXiv:1708.00704; Combinatorica 2020). It unifies both previous stability results.

Setting

All graphs are finite and simple, with vertex set {0,…,n−1}\{0,\dots,n-1\}{0,…,n−1}. The circumference c(G)c(G)c(G) is the length (number of edges) of a longest cycle. GGG is 2-connected if it has at least three vertices and stays connected after deleting any one vertex. δ(G)\delta(G)δ(G) is the minimum degree and e(G)e(G)e(G) the number of edges.

For k≤⌊c/2⌋k\le\lfloor c/2\rfloork≤⌊c/2⌋, the graph Wn,k,cW_{n,k,c}Wn,k,c​ is a clique Kc−k+1K_{c-k+1}Kc−k+1​ together with n−(c−k+1)n-(c-k+1)n−(c−k+1) further vertices, each joined to the same kkk vertices of the clique. It has nnn vertices, minimum degree kkk, circumference ccc, and

f(n,k,c)=(c−k+12)+k (n−c+k−1)f(n,k,c)=\binom{c-k+1}{2}+k\,(n-c+k-1)f(n,k,c)=(2c−k+1​)+k(n−c+k−1)

edges. The graph Zn,k,cZ_{n,k,c}Zn,k,c​ is the union of a clique Kc−k+1K_{c-k+1}Kc−k+1​ and n−(c−k+1)k−1\frac{n-(c-k+1)}{k-1}k−1n−(c−k+1)​ cliques Kk+1K_{k+1}Kk+1​, any two of the cliques sharing the same two vertices. The families Xn,c\mathcal X_{n,c}Xn,c​ and Yn,c\mathcal Y_{n,c}Yn,c​ consist of graphs on A∪B∪XA\cup B\cup XA∪B∪X (resp. A∪B∪YA\cup B\cup YA∪B∪Y) with AAA a clique of size ⌊c/2⌋\lfloor c/2\rfloor⌊c/2⌋, BBB stable and AAA complete to BBB. In Xn,c\mathcal X_{n,c}Xn,c​ every vertex of XXX has exactly two neighbours, the same a∈Aa\in Aa∈A and b∈Bb\in Bb∈B. In Yn,c\mathcal Y_{n,c}Yn,c​, YYY carries a star forest whose stars all attach to the same two vertices a,b∈Aa,b\in Aa,b∈A in a prescribed way.

The proof works with the CCC-closure G‾\overline GG of a cycle CCC. It is obtained by replacing G[C]G[C]G[C] by its (c+1)(c+1)(c+1)-closure, which repeatedly joins non-adjacent pairs of G[C]G[C]G[C] whose degree sum is at least c+1c+1c+1. A cycle is locally maximal if every longer cycle uses at least three edges between V(C)V(C)V(C) and the rest of the graph.

Formalization targets

Goal: Theorem 1.7

Let k≥2k\ge2k≥2 and let GGG be 2-connected on nnn vertices with δ(G)≥k\delta(G)\ge kδ(G)≥k and circumference ccc, 10≤c≤n−110\le c\le n-110≤c≤n−1. If

e(G)>max⁡{f(n,k+1,c), f(n,⌊c/2⌋−1,c)},e(G)>\max\{f(n,k+1,c),\ f(n,\lfloor c/2\rfloor-1,c)\},e(G)>max{f(n,k+1,c), f(n,⌊c/2⌋−1,c)},

then G⊆Wn,k,cG\subseteq W_{n,k,c}G⊆Wn,k,c​, or G⊆Wn,⌊c/2⌋,cG\subseteq W_{n,\lfloor c/2\rfloor,c}G⊆Wn,⌊c/2⌋,c​, or (k=2k=2k=2, ccc odd, and GGG is a subgraph of a member of Xn,c∪Yn,c\mathcal X_{n,c}\cup\mathcal Y_{n,c}Xn,c​∪Yn,c​), or (k≥3k\ge3k≥3 and G⊆Zn,k,cG\subseteq Z_{n,k,c}G⊆Zn,k,c​).

Stronger: Theorem 1.9

For a longest cycle CCC, the same hypotheses give one of four alternatives. Either G‾≅Wn,k,c\overline G\cong W_{n,k,c}G≅Wn,k,c​; or G⊆Wn,⌊c/2⌋,cG\subseteq W_{n,\lfloor c/2\rfloor,c}G⊆Wn,⌊c/2⌋,c​; or the X∪Y\mathcal X\cup\mathcal YX∪Y alternative holds; or k≥3k\ge3k≥3 and G‾≅Zn,k,c\overline G\cong Z_{n,k,c}G≅Zn,k,c​.

Milestones

The milestones follow the paper's proof.

  • Theorem 1.9 splits into Theorem 1.12, for many edges off CCC, and Theorem 4.1, for many edges on CCC.
  • Theorem 4.1 combines Lemmas 2.7, 2.8 and 2.11 on closures with the structural Lemmas 4.2, 4.3 and 4.4.
  • Two arithmetic facts about fff and h(n,k)=(n−k2)+k(k−1)h(n,k)=\binom{n-k}{2}+k(k-1)h(n,k)=(2n−k​)+k(k−1), and Lemmas 2.5, 2.6 and 2.10, support these.

Significance

The theorem describes every 2-connected graph whose edge count comes within one step of Woodall's extremal bound in either parameter. At k=2k=2k=2 it recovers the theorem of Füredi, Kostochka, Luo and Verstraëte exactly. At c=n−1c=n-1c=n−1 it refines the Li–Ning / Füredi–Kostochka–Luo stability theorem for non-Hamiltonian 2-connected graphs. It also gives Corollary 1.8 for 3-connected graphs, where only the two WWW graphs remain. Theorem 1.9 goes further and identifies the extremal configurations exactly, up to the closure.

On the formal side, Mathlib has walks, cycles, Hamiltonian paths and cycles, clique numbers and graph embeddings. It has no circumference theory, no Bondy–Chvátal closure, no Hamiltonian-connectedness and none of the classical extremal results the proof cites (Dirac, Bondy, Chvátal, Erdős–Gallai, Fan). No result of this mission is known to have a machine-checked proof. The mission asks for the paper's proof, or any other proof, of the goal; for its refinement, Theorem 1.9; and for the closure and attachment lemmas on the way.

Difficulty

The obvious approach is to delete a low-degree vertex and induct, as in the classical proofs of Erdős–Gallai type bounds. It does not reach stability. Deleting a vertex can destroy 2-connectivity, and the extremal family changes with kkk: the threshold f(n,k+1,c)f(n,k+1,c)f(n,k+1,c) moves with the minimum degree, and the new graph Zn,k,cZ_{n,k,c}Zn,k,c​ appears only for k≥3k\ge3k≥3.

The edges inside V(C)V(C)V(C) are the hard part. A longest cycle gives no direct control over G[C]G[C]G[C]. The paper's route needs two non-trivial reductions:

  • a closure that keeps longest path lengths (Lemma 2.6), applied to a locally maximal cycle so that G‾[C]\overline G[C]G[C] becomes highly structured;
  • a degree-sequence dichotomy derived from Chvátal's Hamiltonicity theorem (Lemmas 2.10, 2.11).

After that, Lemma 4.2 is four pages of degree-sequence casework, and Lemma 4.4 is a ten-claim structural argument.

Formalization scope

Vertices are Fin n and graphs are Mathlib SimpleGraphs. Further conventions:

  • "G⊆HG\subseteq HG⊆H" is an embedding (⊑, a subgraph up to relabelling), and "G‾=W\overline G=WG=W" or "G∈{W,Z}G\in\{W,Z\}G∈{W,Z}" is a graph isomorphism.
  • "Circumference ccc" means a cycle of length ccc exists and no cycle is longer; "longest cycle" is defined by comparison with all cycles. Neither is a supremum, which would be 000 on acyclic graphs.
  • ⌊c/2⌋\lfloor c/2\rfloor⌊c/2⌋ is natural-number division. fff and hhh are natural-number expressions that are exact in every range used.
  • The kkk-closure is the least kkk-closed supergraph, which equals the page's recursive closure. A companion sanity file proves that it contains GGG, is kkk-closed, and lies below every kkk-closed supergraph.
  • Hamiltonian-connected quantifies over distinct pairs.
  • Lemma 2.5's bounds are stated in Z\mathbb ZZ.

Added hypothesis: k≥2k\ge2k≥2 in Theorems 1.7, 1.9, 4.1 and Lemma 4.4. As printed, the theorems claim every kkk, but they fail at k=1k=1k=1: a member of X18,11\mathcal X_{18,11}X18,11​ with ∣X∣=2|X|=2∣X∣=2 is 2-connected, has circumference 111111 and 69>6869>6869>68 edges, yet lies in neither W18,1,11W_{18,1,11}W18,1,11​ nor W18,5,11W_{18,5,11}W18,5,11​. Zn,k,cZ_{n,k,c}Zn,k,c​ also divides by k−1k-1k−1. Lemma 4.3 has no minimum-degree hypothesis and is stated for every kkk.

Trivializations ruled out.

  • The page's alternatives "if k=2k=2k=2 and ccc is odd, then …" and "if k≥3k\ge3k≥3, then …" are encoded as conjunctions. As implications they would hold vacuously.
  • The Zn,k,cZ_{n,k,c}Zn,k,c​ alternatives carry the divisibility (k−1)∣n−(c−k+1)(k-1)\mid n-(c-k+1)(k−1)∣n−(c−k+1), so no truncated last block is admitted.
  • Equalities of graphs are isomorphisms, never containments.
  • The closure cannot be replaced by an arbitrary closed supergraph such as the complete graph.

Infrastructure. A complete development needs:

  • closure and Pósa-rotation arguments;
  • Chvátal's degree-sequence theorem;
  • Dirac's and Bondy's circumference bounds;
  • Fan's long-path theorem;
  • the Fan–Lv–Wang edge-switching lemma;
  • Erdős–Gallai for paths.

All of these are reusable well beyond this mission, and contributions of any of them are welcome. Theorem 1.12 is also the goal of the companion mission on the stability of Bondy's theorem.

Selected references

  • J. Ma, B. Ning, Stability results on the circumference of a graph, Combinatorica 40 (2020); arXiv:1708.00704v2. https://arxiv.org/abs/1708.00704, https://doi.org/10.1007/s00493-019-3843-4
  • G. N. Kopylov, Maximal paths and cycles in a graph, Dokl. Akad. Nauk SSSR 234 (1977), 19–21.
  • D. R. Woodall, Maximal circuits of graphs I, Acta Math. Acad. Sci. Hungar. 28 (1976), 77–80.
  • Z. Füredi, A. Kostochka, R. Luo, J. Verstraëte, Stability in the Erdős–Gallai theorem on cycles and paths, II, Discrete Math. 341 (2018), 1253–1263.
  • Z. Füredi, A. Kostochka, J. Verstraëte, Stability in the Erdős–Gallai theorems on cycles and paths, J. Combin. Theory Ser. B 121 (2016), 197–228.
  • J. A. Bondy, V. Chvátal, A method in graph theory, Discrete Math. 15 (1976), 111–135. https://doi.org/10.1016/0012-365X(76)90078-9
  • G. Fan, X. Lv, P. Wang, Cycles in 2-connected graphs, J. Combin. Theory Ser. B 92 (2004), 379–394.
  • P. Erdős, T. Gallai, On maximal paths and circuits of graphs, Acta Math. Acad. Sci. Hungar. 10 (1959), 337–356. https://doi.org/10.1007/BF02024498
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Linear OptimizationOperations ResearchOptimization·Captain: mikedeng1

Production Scheduling for Strategic Open Pit Mine Planning: A Mixed-Integer Programming Approach 3: Variable-Right-Hand-Side Production Cuts along a Precedence Chain Are ValidResearch Paper

Motivation

Strategic open pit mine planning decides which parts of an ore body are excavated, in which period, and where each block of material is sent: to a processing plant, a stockpile or a waste dump. Rivera Letelier, Espinoza, Goycoolea, Moreno and Muñoz (Operations Research 68(5), 2020) state the problem as a mixed-integer program, the precedence-constrained production scheduling problem with clusters (PCPSP-C), which extends the formulation of Bienstock and Zuckerberg (IPCO 2010) to clusters of blocks that are extracted together. The integer versions of this program have large integrality gaps on production scheduling instances (§5, p. 1432), so the authors derive problem-specific cutting planes. This mission concerns the variable-right-hand-side (VRHS) production cuts of §5.2. They combine the precedence order of the clusters with the capacity of a single destination: if a solution sends many blocks to a capacitated destination, the predecessors of those blocks must be fully extracted.

The VRHS cuts are introduced first on a one-period, two-destination set, the mode-knapsack set MK (§5.2.1), and then generalised to the full multi-period clustered model (§5.2.2). Disaggregated formulations with destination choices go back to Boland et al. (Comput. Oper. Res. 2009); cutting planes for the precedence-constrained knapsack structure of open pit scheduling were studied by Bley et al. (Comput. Oper. Res. 2010).

All page references are journal pages of the published Operations Research article.

Setting

An instance has finite sets B\mathcal BB of blocks, D\mathcal DD of destinations and C\mathcal CC of clusters, the latter a partition of B\mathcal BB, and periods T={1,…,T}\mathcal T=\{1,\dots,T\}T={1,…,T}. Block bbb lies in cluster c(b)c(b)c(b) and has weight qb≥0q_b\ge 0qb​≥0. A precedence relation b1≺b2b_1\prec b_2b1​≺b2​ on blocks induces one on clusters (c1≺c2c_1\prec c_2c1​≺c2​ if some block of c1c_1c1​ precedes some block of c2c_2c2​), assumed to be a strict partial order. The arc set A\mathcal AA is its transitive reduction: (c,c′)∈A(c,c')\in\mathcal A(c,c′)∈A when c′c'c′ is an immediate predecessor of ccc. The reverse closure of a cluster is rcl(c)={c}∪{c′:c≺c′}rcl(c)=\{c\}\cup\{c':c\prec c'\}rcl(c)={c}∪{c′:c≺c′}, the cluster and everything that requires it; for a set SSS of clusters, q(S)=∑c∈S∑b∈cqbq(S)=\sum_{c\in S}\sum_{b\in c}q_bq(S)=∑c∈S​∑b∈c​qb​.

Variables xc,tx_{c,t}xc,t​ give the fraction of cluster ccc extracted in period ttt, and yb,d,ty_{b,d,t}yb,d,t​ the fraction of block bbb sent to destination ddd in period ttt. The constraints (2)–(7) of p. 1427 are

xc(b),t=∑dyb,d,t,∑txc,t≤1,∑t′≤txc,t′≤∑t′≤txc′,t′  ((c,c′)∈A),Gy≤g,y≥0,x_{c(b),t}=\sum_{d}y_{b,d,t},\qquad \sum_{t}x_{c,t}\le 1,\qquad \sum_{t'\le t}x_{c,t'}\le\sum_{t'\le t}x_{c',t'}\ \ ((c,c')\in\mathcal A),\qquad Gy\le g,\qquad y\ge 0,xc(b),t​=d∑​yb,d,t​,t∑​xc,t​≤1,t′≤t∑​xc,t′​≤t′≤t∑​xc′,t′​  ((c,c′)∈A),Gy≤g,y≥0,

together with an integrality condition: full integrality (10), xc,t∈{0,1}x_{c,t}\in\{0,1\}xc,t​∈{0,1}, defines the PCPSP-F, and partial integrality (11), "∑t′≤txc,t′>0\sum_{t'\le t}x_{c,t'}>0∑t′≤t​xc,t′​>0 implies ∑t′≤txc′,t′=1\sum_{t'\le t}x_{c',t'}=1∑t′≤t​xc′,t′​=1 for (c,c′)∈A(c,c')\in\mathcal A(c,c′)∈A", defines the PCPSP-P. The general rows Gy≤gGy\le gGy≤g include the destination capacity rows (9), ∑bqb yb,d,t≤Utd\sum_b q_b\,y_{b,d,t}\le U^d_t∑b​qb​yb,d,t​≤Utd​. The cuts use the cumulative variables wc,t=∑t′=1txc,t′w_{c,t}=\sum_{t'=1}^{t}x_{c,t'}wc,t​=∑t′=1t​xc,t′​ (17).

The mode-knapsack set MK (p. 1433) fixes a DAG G=(B,A)G=(\mathcal B,\mathcal A)G=(B,A), weights qb>0q_b>0qb​>0 and a capacity U>0U>0U>0, and consists of the vectors (x,yP,yW)(x,y^P,y^W)(x,yP,yW) with

∑bqbybP≤U,ybP+ybW=xb,xb≤1,xb>0⇒xb′=1 ((b,b′)∈A),yP,yW≥0.\sum_b q_b y^P_b\le U,\qquad y^P_b+y^W_b=x_b,\qquad x_b\le 1,\qquad x_b>0\Rightarrow x_{b'}=1\ ((b,b')\in\mathcal A),\qquad y^P,y^W\ge 0.b∑​qb​ybP​≤U,ybP​+ybW​=xb​,xb​≤1,xb​>0⇒xb′​=1 ((b,b′)∈A),yP,yW≥0.

Formalization targets

Goal: Theorem 7 (VRHS cuts), p. 1434

Fix d∈Dd\in\mathcal Dd∈D, t∈Tt\in\mathcal Tt∈T and clusters c1≺c2≺⋯≺cnc_1\prec c_2\prec\dots\prec c_nc1​≺c2​≺⋯≺cn​ with q(rcl(c1)∖rcl(cn))<Utd<q(rcl(c1))q(rcl(c_1)\setminus rcl(c_n))<U^d_t<q(rcl(c_1))q(rcl(c1​)∖rcl(cn​))<Utd​<q(rcl(c1​)). Let Δk=rcl(ck)∖rcl(ck+1)\Delta_k=rcl(c_k)\setminus rcl(c_{k+1})Δk​=rcl(ck​)∖rcl(ck+1​), δk=q(Δk)\delta_k=q(\Delta_k)δk​=q(Δk​) for k<nk<nk<n, and Δn=rcl(cn)\Delta_n=rcl(c_n)Δn​=rcl(cn​), δn=Utd−q(rcl(c1)∖rcl(cn))\delta_n=U^d_t-q(rcl(c_1)\setminus rcl(c_n))δn​=Utd​−q(rcl(c1​)∖rcl(cn​)). For constants 0≤αb≤10\le\alpha_b\le 10≤αb​≤1 (b∈cnb\in c_nb∈cn​), the inequality

∑k=1n−1∑c∈Δk∑b∈cqbyb,d,t+∑b∈cnαbqbyb,d,t+∑c∈rcl(cn)∖{cn}∑b∈cqbyb,d,t≤∑k=1nδkwck,t(32)\sum_{k=1}^{n-1}\sum_{c\in\Delta_k}\sum_{b\in c}q_b y_{b,d,t}+\sum_{b\in c_n}\alpha_b q_b y_{b,d,t}+\sum_{c\in rcl(c_n)\setminus\{c_n\}}\sum_{b\in c}q_b y_{b,d,t}\le\sum_{k=1}^{n}\delta_k w_{c_k,t}\tag{32}k=1∑n−1​c∈Δk​∑​b∈c∑​qb​yb,d,t​+b∈cn​∑​αb​qb​yb,d,t​+c∈rcl(cn​)∖{cn​}∑​b∈c∑​qb​yb,d,t​≤k=1∑n​δk​wck​,t​(32)

is valid for the PCPSP-F, and, when ∑b∈cnαbqb≤Utd−q(rcl(c1)∖rcl(cn))\sum_{b\in c_n}\alpha_b q_b\le U^d_t-q(rcl(c_1)\setminus rcl(c_n))∑b∈cn​​αb​qb​≤Utd​−q(rcl(c1​)∖rcl(cn​)) (33), for the PCPSP-P. The goal is the conjunction of the two validity claims.

Milestones

  • (29)–(30), p. 1434: under either integrality condition, wc,t<1w_{c,t}<1wc,t​<1 implies yb,d,t=0y_{b,d,t}=0yb,d,t​=0 for every block of a cluster in rcl(c)∖{c}rcl(c)\setminus\{c\}rcl(c)∖{c}, and yb,d,t≤wc(b),ty_{b,d,t}\le w_{c(b),t}yb,d,t​≤wc(b),t​. The third condition (31) of the page is the capacity row (9) itself.
  • (35), p. 1435: ∑c∈Δk∑b∈cqbyb,d,t≤δkwck,t\sum_{c\in\Delta_k}\sum_{b\in c}q_b y_{b,d,t}\le\delta_k w_{c_k,t}∑c∈Δk​​∑b∈c​qb​yb,d,t​≤δk​wck​,t​ for k=1,…,n−1k=1,\dots,n-1k=1,…,n−1.
  • (36), p. 1435: under (33), ∑b∈cnαbqbyb,d,t≤δnwcn,t\sum_{b\in c_n}\alpha_b q_b y_{b,d,t}\le\delta_n w_{c_n,t}∑b∈cn​​αb​qb​yb,d,t​≤δn​wcn​,t​.
  • Theorem 5, p. 1434: in MK, every block bbb with qb≤Uq_b\le Uqb​≤U gives the valid inequality ∑b′∈rcl(b)qb′yb′P≤Uxb\sum_{b'\in rcl(b)}q_{b'}y^P_{b'}\le U x_b∑b′∈rcl(b)​qb′​yb′P​≤Uxb​.

Significance

A valid inequality removes fractional points of the linear relaxation while keeping every feasible schedule. The VRHS cuts are among the production cuts that the paper evaluates in its computational study (§8), alongside the extraction cuts and the hourglass cuts. Their right-hand side is not a constant but a combination of extraction variables along a chain, which is what lets them couple the destination capacity with the precedence order; the paper's Theorem 5 shows the mechanism on MK, Theorem 7 in the full model. The partial integrality regime, under which the second half of Theorem 7 holds, is the one used by commercial mine planning software (p. 1427).

The results are proved in the paper by case analysis on the first index kkk with wck,t<1w_{c_k,t}<1wck​,t​<1. None of them has a machine-checked proof. Formalizing them makes explicit which rows of the formulation each cut uses (the destination capacity (9) and the integrality condition), and what role the coefficient condition (33) plays in the partially integral case.

Difficulty

The proof uses that Δ1,…,Δn−1\Delta_1,\dots,\Delta_{n-1}Δ1​,…,Δn−1​ partition rcl(c1)∖rcl(cn)rcl(c_1)\setminus rcl(c_n)rcl(c1​)∖rcl(cn​) and are disjoint from rcl(cn)rcl(c_n)rcl(cn​), which requires rcl(ck+1)⊆rcl(ck)rcl(c_{k+1})\subseteq rcl(c_k)rcl(ck+1​)⊆rcl(ck​) along the chain. It uses that wc,t≤wck,tw_{c,t}\le w_{c_k,t}wc,t​≤wck​,t​ for every c∈rcl(ck)c\in rcl(c_k)c∈rcl(ck​), and that wc,t<1w_{c,t}<1wc,t​<1 forces all strict successors of ccc to be unextracted; both chain the constraints (4) and (11) along covering arcs of a finite strict order, since the formulation constrains only the arcs of A\mathcal AA, not all of ≺\prec≺. A natural first attempt, arguing directly from ≺\prec≺, therefore does not apply. The counting step needs x≥0x\ge 0x≥0, which is not a constraint of the formulation but follows from xc(b),t=∑dyb,d,tx_{c(b),t}=\sum_d y_{b,d,t}xc(b),t​=∑d​yb,d,t​, y≥0y\ge 0y≥0 and the nonemptiness of clusters. In the partial integrality case a fractional wcn,tw_{c_n,t}wcn​,t​ is possible, and the bound on the cnc_ncn​ term must come from (33) rather than from integrality.

Formalization scope

Blocks, destinations and clusters are finite types; periods are Fin T, index ttt standing for period t+1t+1t+1. An instance carries the block-to-cluster map, the block precedence, values, discount rate, weights, capacities and mmm side rows Gy≤gGy\le gGy≤g. Cluster precedence is derived from block precedence; A\mathcal AA is its covering relation, and constraints (4) and (11) range over A\mathcal AA only. The chain c1,…,cnc_1,\dots,c_nc1​,…,cn​ is a function on N\mathbb NN read at 1,…,n1,\dots,n1,…,n with n≥1n\ge 1n≥1, and condition 1 of Theorem 7 is stated for consecutive pairs. In (32), yyy is taken at the single period ttt and www is cumulative.

The standing assumptions of §2.1 are hypotheses of every PCPSP-C statement: clusters cover B\mathcal BB (so each is nonempty), ≺\prec≺ is a strict partial order on clusters, r>0r>0r>0, and qb≥0q_b\ge 0qb​≥0. A cut "valid for the PCPSP-F (PCPSP-P)" is stated as: at every point feasible for the formulation with full (partial) integrality whose destination capacity rows (9) hold, the inequality holds. The capacity rows enter as an explicit hypothesis because the paper assumes they are among the rows of Gy≤gGy\le gGy≤g; without them the cut is false. Validity is never asserted for the LP relaxation, where (29) and (32) fail, so the integrality condition cannot be dropped. Conditions 2 and 3 of Theorem 7 are kept as on the page, although the proof does not use condition 3. In MK, the DAG property, q>0q>0q>0 and U>0U>0U>0 are hypotheses; an arc (b,b′)(b,b')(b,b′) means that extracting bbb forces b′b'b′, and rcl(b)rcl(b)rcl(b) collects bbb and the blocks from which bbb is reachable.

The development needs only finite sums, finite sets and orders from Mathlib. Contributions are welcome on the chaining lemma for covering relations of finite strict orders, on the nonnegativity and monotonicity of www, and on the partition {Δk}\{\Delta_k\}{Δk​} of rcl(c1)∖rcl(cn)rcl(c_1)\setminus rcl(c_n)rcl(c1​)∖rcl(cn​), which the goal and the milestones share.

Selected references

  • O. Rivera Letelier, D. Espinoza, M. Goycoolea, E. Moreno, G. Muñoz, Production Scheduling for Strategic Open Pit Mine Planning: A Mixed-Integer Programming Approach, Operations Research 68(5):1425–1444, 2020. https://doi.org/10.1287/opre.2019.1965
  • D. Bienstock, M. Zuckerberg, Solving LP Relaxations of Large-Scale Precedence Constrained Problems, Proc. 14th IPCO, LNCS 6080, 1–14, 2010. https://doi.org/10.1007/978-3-642-13036-6_1
  • N. Boland, I. Dumitrescu, G. Froyland, A. M. Gleixner, LP-based disaggregation approaches to solving the open pit mining production scheduling problem with block processing selectivity, Computers & Operations Research 36(4):1064–1089, 2009. https://doi.org/10.1016/j.cor.2007.12.006
  • A. Bley, N. Boland, C. Fricke, G. Froyland, A strengthened formulation and cutting planes for the open pit mine production scheduling problem, Computers & Operations Research 37(9):1641–1647, 2010. https://doi.org/10.1016/j.cor.2009.12.008
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Convex OptimizationMachine LearningOptimization+1·Captain: mikedeng1

Distributed Stochastic Gradient Tracking Methods I: With a Constant Stepsize, DSGT's Limiting Mean-Square Error Is at Most (Γ+1)ασ²/(Γμn) Plus a Network TermResearch Paper

Distributed learning with noisy gradients

Many learning and estimation problems are solved by a network of agents: each agent holds part of the data, can talk only to its neighbours, and wants to compute the minimizer of the average of all agents' objectives. Examples are sensor networks, multi-robot systems, and data-parallel training without a central server (Nedić and Ozdaglar 2009; Lian et al. 2017). In these settings the agents rarely know their exact gradients; they sample them, one data point or one mini-batch at a time.

Gradient tracking methods let each agent keep, next to its estimate of the minimizer, a running estimate of the network-average gradient. With exact gradients they converge linearly with a constant stepsize (Qu and Li 2018; Nedić, Olshevsky and Shi 2017), which plain distributed gradient descent does not. S. Pu and A. Nedić (Math. Program. 187 (2021) 409–457) analysed the same scheme when every gradient is replaced by an unbiased noisy sample, and called it DSGT (distributed stochastic gradient tracking). This mission formalizes their constant-stepsize result, Theorem 1.

Setting

There are nnn agents. Agent iii holds a cost fi:Rp→Rf_i:\mathbb R^p\to\mathbb Rfi​:Rp→R, and the agents seek

x∗∈arg⁡min⁡x∈Rpf(x),f(x)=1n∑i=1nfi(x).x^*\in\arg\min_{x\in\mathbb R^p} f(x),\qquad f(x)=\frac1n\sum_{i=1}^n f_i(x).x∗∈argx∈Rpmin​f(x),f(x)=n1​i=1∑n​fi​(x).

Each fif_ifi​ is μ\muμ-strongly convex with LLL-Lipschitz gradient: ⟨∇fi(x)−∇fi(x′),x−x′⟩≥μ∥x−x′∥2\langle\nabla f_i(x)-\nabla f_i(x'),x-x'\rangle\ge\mu\|x-x'\|^2⟨∇fi​(x)−∇fi​(x′),x−x′⟩≥μ∥x−x′∥2 and ∥∇fi(x)−∇fi(x′)∥≤L∥x−x′∥\|\nabla f_i(x)-\nabla f_i(x')\|\le L\|x-x'\|∥∇fi​(x)−∇fi​(x′)∥≤L∥x−x′∥.

Noisy gradients. At time kkk agent iii draws a random sample ξi,k\xi_{i,k}ξi,k​ and observes gi(x,ξi,k)g_i(x,\xi_{i,k})gi​(x,ξi,k​), with E[gi(x,ξi,k)]=∇fi(x)\mathbb E[g_i(x,\xi_{i,k})]=\nabla f_i(x)E[gi​(x,ξi,k​)]=∇fi​(x) and E∥gi(x,ξi,k)−∇fi(x)∥2≤σ2\mathbb E\|g_i(x,\xi_{i,k})-\nabla f_i(x)\|^2\le\sigma^2E∥gi​(x,ξi,k​)−∇fi​(x)∥2≤σ2; the samples are independent.

The network. Agents are coupled by a nonnegative doubly stochastic matrix W=[wij]\mathbf W=[w_{ij}]W=[wij​] (rows and columns sum to 111), with wij>0w_{ij}>0wij​>0 exactly when iii and jjj communicate, some wii>0w_{ii}>0wii​>0, and a connected undirected communication graph. The number

ρw=∥W−1n11⊤∥2<1,\rho_w=\Big\|\mathbf W-\tfrac1n\mathbf 1\mathbf 1^\top\Big\|_2<1,ρw​=​W−n1​11⊤​2​<1,

the spectral norm, measures how fast one round of averaging brings the agents together.

DSGT. Each agent keeps xi,kx_{i,k}xi,k​ and a tracker yi,ky_{i,k}yi,k​. Stacking them as rows of xk,yk∈Rn×p\mathbf x_k,\mathbf y_k\in\mathbb R^{n\times p}xk​,yk​∈Rn×p and writing G(x,ξ)G(\mathbf x,\boldsymbol\xi)G(x,ξ) for the matrix with rows gi(xi,ξi)g_i(x_i,\xi_i)gi​(xi​,ξi​), the method with constant stepsize α>0\alpha>0α>0 is

xk+1=W(xk−αyk),yk+1=Wyk+G(xk+1,ξk+1)−G(xk,ξk),\mathbf x_{k+1}=\mathbf W(\mathbf x_k-\alpha\mathbf y_k),\qquad \mathbf y_{k+1}=\mathbf W\mathbf y_k+G(\mathbf x_{k+1},\boldsymbol\xi_{k+1})-G(\mathbf x_k,\boldsymbol\xi_k),xk+1​=W(xk​−αyk​),yk+1​=Wyk​+G(xk+1​,ξk+1​)−G(xk​,ξk​),

started from a deterministic x0\mathbf x_0x0​ and y0=G(x0,ξ0)\mathbf y_0=G(\mathbf x_0,\boldsymbol\xi_0)y0​=G(x0​,ξ0​). The two error measures are the distance of the average xˉk=1n∑ixi,k\bar x_k=\frac1n\sum_ix_{i,k}xˉk​=n1​∑i​xi,k​ to x∗x^*x∗ and the consensus error ∥xk−1xˉk∥2=∑i∥xi,k−xˉk∥2\|\mathbf x_k-\mathbf 1\bar x_k\|^2=\sum_i\|x_{i,k}-\bar x_k\|^2∥xk​−1xˉk​∥2=∑i​∥xi,k​−xˉk​∥2.

Formalization targets

Goal: Theorem 1

Fix Γ>1\Gamma>1Γ>1 and a stepsize α\alphaα below the explicit threshold (7) of the paper (a minimum of three expressions in ρw\rho_wρw​, ∥W−I∥\|\mathbf W-\mathbf I\|∥W−I∥, μ\muμ, LLL, Γ\GammaΓ). Then a certain explicit 3×33\times33×3 matrix A\mathbf AA has spectral radius ρ(A)<1\rho(\mathbf A)<1ρ(A)<1, and with Mσ=[3α2L2+2(αL+1)(n+1)]σ2M_\sigma=[3\alpha^2L^2+2(\alpha L+1)(n+1)]\sigma^2Mσ​=[3α2L2+2(αL+1)(n+1)]σ2,

lim sup⁡k→∞E∥xˉk−x∗∥2≤Γ+1Γασ2μn+Γ+1Γ−1 4α2L2(1+αμ)(1+ρw2)ρw2μ2n(1−ρw2)3 Mσ,\limsup_{k\to\infty}\mathbb E\|\bar x_k-x^*\|^2\le\frac{\Gamma+1}{\Gamma}\frac{\alpha\sigma^2}{\mu n}+\frac{\Gamma+1}{\Gamma-1}\,\frac{4\alpha^2L^2(1+\alpha\mu)(1+\rho_w^2)\rho_w^2}{\mu^2n(1-\rho_w^2)^3}\,M_\sigma,k→∞limsup​E∥xˉk​−x∗∥2≤ΓΓ+1​μnασ2​+Γ−1Γ+1​μ2n(1−ρw2​)34α2L2(1+αμ)(1+ρw2​)ρw2​​Mσ​, lim sup⁡k→∞E∥xk−1xˉk∥2≤Γ+1Γ−1 4α2(1+ρw2)ρw2(2α2L3σ2+μMσ)μ(1−ρw2)3.\limsup_{k\to\infty}\mathbb E\|\mathbf x_k-\mathbf 1\bar x_k\|^2\le\frac{\Gamma+1}{\Gamma-1}\,\frac{4\alpha^2(1+\rho_w^2)\rho_w^2(2\alpha^2L^3\sigma^2+\mu M_\sigma)}{\mu(1-\rho_w^2)^3}.k→∞limsup​E∥xk​−1xˉk​∥2≤Γ−1Γ+1​μ(1−ρw2​)34α2(1+ρw2​)ρw2​(2α2L3σ2+μMσ​)​.

The constants are the paper's, so the goal is stated with them.

Companion: Corollary 1

Under a further stepsize condition (13), ρ(A)≤1−Γ−1Γ+1αμ\rho(\mathbf A)\le1-\frac{\Gamma-1}{\Gamma+1}\alpha\muρ(A)≤1−Γ+1Γ−1​αμ.

Milestones

The milestones follow the paper's proof: the tracking identity (6); Lemma 1 on ρw\rho_wρw​; the one-step conditional estimates of Lemmas 2–4 and the auxiliary Lemmas 8–9; the linear system of inequalities (21) and its iterate (22); the determinant criterion Lemma 5; the bound det⁡(I−A)>0\det(\mathbf I-\mathbf A)>0det(I−A)>0 under the relations (23)–(25); and the lower bound (27) on the auxiliary parameter β\betaβ.

Significance

The first term of the bound on E∥xˉk−x∗∥2\mathbb E\|\bar x_k-x^*\|^2E∥xˉk​−x∗∥2, ασ2/(μn)\alpha\sigma^2/(\mu n)ασ2/(μn) up to the factor (Γ+1)/Γ(\Gamma+1)/\Gamma(Γ+1)/Γ, is the error of centralized stochastic gradient descent that averages nnn samples per step; it does not depend on the network. The network enters only through terms of order α2\alpha^2α2. So for small stepsizes a decentralized method with gradient tracking pays nothing in the limiting error for having no central server. Theorem 1 is one of the standard references for this statement in decentralized stochastic optimization.

The result is proved in the paper, with constants. It has no machine-checked proof that we know of. Formalizing it produces a checked development of the linear-system method for distributed algorithms: conditional moment bounds for coupled stochastic recursions, a 3×33\times33×3 linear system of inequalities between expectations, and a Perron–Frobenius criterion for its stability. The same pattern recurs in the analysis of many gradient-tracking and variance-reduced decentralized methods.

Difficulty

The obvious argument would bound each error by itself, but the three quantities E∥xˉk−x∗∥2\mathbb E\|\bar x_k-x^*\|^2E∥xˉk​−x∗∥2, E∥xk−1xˉk∥2\mathbb E\|\mathbf x_k-\mathbf 1\bar x_k\|^2E∥xk​−1xˉk​∥2 and E∥yk−1yˉk∥2\mathbb E\|\mathbf y_k-\mathbf 1\bar y_k\|^2E∥yk​−1yˉ​k​∥2 feed into one another, and none of them contracts on its own. The tracker error in particular depends on the next iterate, which itself depends on the current noise, so the cross terms do not vanish in conditional expectation and must be estimated separately (Lemmas 8 and 9).

Once the coupled system is set up, its stability needs the spectral radius of a nonnegative 3×33\times33×3 matrix whose entries depend on all constants at once, and the explicit limiting bounds need its inverse. The determinant criterion of Lemma 5 rests on Perron–Frobenius theory, which Mathlib provides only in part.

Formalization scope

Stacked variables are Fin n → EuclideanSpace ℝ (Fin p). Every matrix norm is written out: ∥x−1xˉ∥2=∑i∥xi−xˉ∥2\|\mathbf x-\mathbf 1\bar x\|^2=\sum_i\|x_i-\bar x\|^2∥x−1xˉ∥2=∑i​∥xi​−xˉ∥2 (Frobenius), ∥W−I∥\|\mathbf W-\mathbf I\|∥W−I∥ is the Frobenius norm of the n×nn\times nn×n matrix, and ρw\rho_wρw​ is the operator norm of W−1n11⊤\mathbf W-\frac1n\mathbf 1\mathbf 1^\topW−n1​11⊤ on Euclidean Rn\mathbb R^nRn. Spectral radii are taken over C\mathbb CC, so complex eigenvalues count. Expectations are Bochner integrals, and every bounded expectation comes with an integrability conclusion. "lim sup⁡kak≤B\limsup_k a_k\le Blimsupk​ak​≤B" is stated as "for every ε>0\varepsilon>0ε>0, eventually ak≤B+εa_k\le B+\varepsilonak​≤B+ε". Fk\mathcal F_kFk​ is the σ-algebra generated by ξ0,…,ξk−1\boldsymbol\xi_0,\dots,\boldsymbol\xi_{k-1}ξ0​,…,ξk−1​, and conditional statements hold almost surely.

Standing assumptions and additions, all stated in the items:

  1. Assumptions 3–4 on W\mathbf WW are hypotheses of every statement about the iterates, although Theorem 1 cites only Assumptions 1–2.
  2. Independence of the noise is mutual independence of all ξi,k\xi_{i,k}ξi,k​; gig_igi​ is jointly measurable; p≥1p\ge1p≥1.
  3. ρw>0\rho_w>0ρw​>0, because β\betaβ, A\mathbf AA and (7) divide by ρw\rho_wρw​.
  4. 3αL≤13\alpha L\le13αL≤1 in (20), (21), (22) and Theorem 1: the last step of the paper's proof of (20) needs it, and (7) does not imply it in general (for ρw=0.01\rho_w=0.01ρw​=0.01, Γ=1.1\Gamma=1.1Γ=1.1, μ=L\mu=Lμ=L it allows α≈0.48/L\alpha\approx0.48/Lα≈0.48/L).

The goal speaks only about the DSGT iterates, x∗x^*x∗ and the matrix A\mathbf AA; it does not assume the linear system (21), ρ(A)<1\rho(\mathbf A)<1ρ(A)<1 or any estimate of the proof. The clause of Theorem 1 that sup⁡l≥kE[⋅]\sup_{l\ge k}\mathbb E[\cdot]supl≥k​E[⋅] approaches the limsup at the rate O(ρ(A)k)\mathcal O(\rho(\mathbf A)^k)O(ρ(A)k) carries an unquantified constant and is not formalized: the paper's proof yields only the envelope (22) and the limit of its right-hand side, not a rate at which sup⁡l≥kE[⋅]\sup_{l\ge k}\mathbb E[\cdot]supl≥k​E[⋅] reaches the limsup; the envelope (22) is a milestone. Theorem 2 (diminishing stepsizes) is the subject of the second mission of the series.

A complete development needs conditional expectations of functions of independent samples, a Frobenius-norm calculus for stacked vectors, the consensus contraction of Lemma 1, and the Perron–Frobenius facts behind Lemma 5. The last two are reusable beyond this mission. Proofs of any milestone, and of the deterministic matrix lemmas in particular, are welcome independently.

Selected references

  • S. Pu, A. Nedić, Distributed stochastic gradient tracking methods, Mathematical Programming 187 (2021) 409–457. https://doi.org/10.1007/s10107-020-01487-0
  • A. Nedić, A. Olshevsky, W. Shi, Achieving geometric convergence for distributed optimization over time-varying graphs, SIAM J. Optim. 27 (2017) 2597–2633. https://arxiv.org/abs/1607.03218
  • G. Qu, N. Li, Harnessing smoothness to accelerate distributed optimization, IEEE Trans. Control Netw. Syst. 5 (2018) 1245–1260. https://arxiv.org/abs/1605.07112
  • A. Nedić, A. Ozdaglar, Distributed subgradient methods for multi-agent optimization, IEEE Trans. Automat. Control 54 (2009) 48–61. https://doi.org/10.1109/TAC.2008.2009515
  • X. Lian, C. Zhang, H. Zhang, C.-J. Hsieh, W. Zhang, J. Liu, Can decentralized algorithms outperform centralized algorithms? A case study for decentralized parallel stochastic gradient descent, NeurIPS 2017. https://arxiv.org/abs/1705.09056
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Functional AnalysisNumerical AnalysisOptimization·Captain: mikedeng1

A Forward-Backward Splitting Method for Monotone Inclusions Without Cocoercivity 1: The Forward-Reflected-Backward Method Converges Weakly to a Zero of A + BResearch Paper

Monotone inclusions and the cost of splitting

Many problems in convex optimization, variational inequalities and saddle-point computation can be written as a monotone inclusion: find xxx in a real Hilbert space HHH with

0∈(A+B)(x),0 \in (A+B)(x),0∈(A+B)(x),

where AAA is a set-valued maximally monotone operator (a subdifferential, a normal cone, a constraint) and BBB is a single-valued monotone operator (a gradient, or the skew operator of a saddle-point problem). Splitting methods solve such problems using AAA and BBB separately: a backward step evaluates the resolvent JλA=(I+λA)−1J_{\lambda A}=(I+\lambda A)^{-1}JλA​=(I+λA)−1, and a forward step evaluates BBB.

The classical forward-backward method xk+1=JλA(xk−λB(xk))x_{k+1}=J_{\lambda A}(x_k-\lambda B(x_k))xk+1​=JλA​(xk​−λB(xk​)) converges when BBB is cocoercive, but can fail when BBB is merely monotone and Lipschitz, which is the case for saddle-point operators such as B(z1,z2)=(z2,−z1)B(z_1,z_2)=(z_2,-z_1)B(z1​,z2​)=(z2​,−z1​). Tseng's forward-backward-forward method (Tseng 2000) removes the cocoercivity assumption at the price of two evaluations of BBB per iteration. Malitsky and Tam (arXiv:1808.04162; SIAM J. Optim. 30(2), 2020) propose the forward-reflected-backward method, which needs one evaluation of BBB and one resolvent of AAA per iteration, reusing the previous value of BBB.

Timeline of the relevant results:

  • 1967: Opial's lemma on weak convergence of sequences in Hilbert space (Opial 1967).
  • 1979: Lions and Mercier analyse forward-backward splitting with cocoercive BBB (Lions–Mercier 1979).
  • 1980: Popov's modified Arrow–Hurwicz method for saddle points, with one operator evaluation per step (Popov 1980).
  • 2000: Tseng's forward-backward-forward method for monotone and Lipschitz BBB.
  • 2015: Malitsky's projected reflected gradient method for variational inequalities (Malitsky 2015), the special case A=NCA=N_CA=NC​, BBB affine.
  • 2018–2020: Malitsky and Tam, the forward-reflected-backward method, Theorem 2.5.

Setting

HHH is a real Hilbert space with inner product ⟨⋅,⋅⟩\langle\cdot,\cdot\rangle⟨⋅,⋅⟩. A set-valued operator A:H⇉HA:H\rightrightarrows HA:H⇉H is monotone if ⟨x−y,u−v⟩≥0\langle x-y,u-v\rangle\ge 0⟨x−y,u−v⟩≥0 whenever u∈A(x)u\in A(x)u∈A(x), v∈A(y)v\in A(y)v∈A(y), and maximally monotone if its graph is not properly contained in the graph of another monotone operator. Its resolvent JλA=(I+λA)−1J_{\lambda A}=(I+\lambda A)^{-1}JλA​=(I+λA)−1 is, for λ>0\lambda>0λ>0 and AAA maximally monotone, an everywhere defined single-valued map, characterised by λ−1(w−JλAw)∈A(JλAw)\lambda^{-1}(w-J_{\lambda A}w)\in A(J_{\lambda A}w)λ−1(w−JλA​w)∈A(JλA​w). A map B:H→HB:H\to HB:H→H is LLL-Lipschitz if ∥B(x)−B(y)∥≤L∥x−y∥\|B(x)-B(y)\|\le L\|x-y\|∥B(x)−B(y)∥≤L∥x−y∥, and monotone if ⟨x−y,B(x)−B(y)⟩≥0\langle x-y,B(x)-B(y)\rangle\ge0⟨x−y,B(x)−B(y)⟩≥0.

The zero set is (A+B)−1(0)={x:−B(x)∈A(x)}(A+B)^{-1}(0)=\{x : -B(x)\in A(x)\}(A+B)−1(0)={x:−B(x)∈A(x)}. Given initial points x0,x−1∈Hx_0,x_{-1}\in Hx0​,x−1​∈H and step sizes (λk)k≥−1(\lambda_k)_{k\ge-1}(λk​)k≥−1​, the forward-reflected-backward method is

xk+1=JλkA(xk−λkB(xk)−λk−1(B(xk)−B(xk−1)))∀k∈N.(13)x_{k+1}=J_{\lambda_k A}\big(x_k-\lambda_k B(x_k)-\lambda_{k-1}(B(x_k)-B(x_{k-1}))\big)\qquad\forall k\in\mathbb N. \tag{13}xk+1​=Jλk​A​(xk​−λk​B(xk​)−λk−1​(B(xk​)−B(xk−1​)))∀k∈N.(13)

A sequence (xk)(x_k)(xk​) converges weakly to xˉ\bar xxˉ if ⟨xk,v⟩→⟨xˉ,v⟩\langle x_k,v\rangle\to\langle\bar x,v\rangle⟨xk​,v⟩→⟨xˉ,v⟩ for every v∈Hv\in Hv∈H; a sequential weak cluster point is the weak limit of a subsequence.

Formalization targets

Goal: Theorem 2.5 (p. 6)

If AAA is maximally monotone, BBB is monotone and LLL-Lipschitz, (A+B)−1(0)≠∅(A+B)^{-1}(0)\ne\varnothing(A+B)−1(0)=∅, and (λk)⊆[ε,1−2ε2L](\lambda_k)\subseteq[\varepsilon,\tfrac{1-2\varepsilon}{2L}](λk​)⊆[ε,2L1−2ε​] for some ε>0\varepsilon>0ε>0, then every sequence generated by (13) satisfies

xk⇀xˉfor some xˉ∈(A+B)−1(0).x_k\rightharpoonup\bar x\quad\text{for some }\bar x\in(A+B)^{-1}(0).xk​⇀xˉfor some xˉ∈(A+B)−1(0).

Milestones

In attack order:

  1. Proposition 2.3, the basic inequality (19) for one resolvent step.
  2. Lemma 2.4, the energy inequality (20).
  3. The telescoped bound after (24).
  4. Boundedness of (xk)(x_k)(xk​) and ∥xk−xk+1∥→0\|x_k-x_{k+1}\|\to0∥xk​−xk+1​∥→0.
  5. Weak cluster points lie in the zero set.
  6. Convergence of the energy (26).
  7. Its limit equals lim⁡∥xk−xˉ∥2\lim\|x_k-\bar x\|^2lim∥xk​−xˉ∥2.
  8. Lemma 2.2, an Opial-type criterion for weak convergence.

Corollary 2.6, the constant-step case λ∈(0,12L)\lambda\in(0,\tfrac1{2L})λ∈(0,2L1​), is included as a companion theorem.

Significance

Theorem 2.5 shows that monotone inclusions with a Lipschitz, non-cocoercive single-valued part can be solved by a splitting method with the per-iteration cost of forward-backward splitting: one forward and one backward evaluation. For saddle-point problems, where each evaluation of BBB is a pair of matrix–vector products, this halves the operator cost of Tseng's method. The method contains the projected reflected gradient method and, for A=0A=0A=0, Popov's method and the optimistic gradient method used in training generative adversarial networks (Remark 2.1). The analysis of this section is reused for the linear rate, the linesearch, the inertial variant and the three-operator variant of later sections (missions 2–5 of this series).

The theorem is proved in the paper. Formalizing it requires a machine-checked Opial-type lemma and a machine-checked demiclosedness argument for maximally monotone operators perturbed by a continuous monotone map, both reusable well beyond this mission. To our knowledge no machine-checked proof of convergence of the forward-reflected-backward method exists.

Difficulty

The energy inequality of Lemma 2.4 is algebra plus monotonicity and the Lipschitz estimate, and it yields boundedness and ∥xk+1−xk∥→0\|x_{k+1}-x_k\|\to0∥xk+1​−xk​∥→0. The difficulty lies in passing from these facts to weak convergence of the whole sequence. Norm convergence is false in general, so a Cauchy-sequence argument is unavailable. The energy is not Fejér monotone in ∥xk−x∥\|x_k-x\|∥xk​−x∥ alone, because of the cross term 2λk−1⟨B(xk)−B(xk−1),x−xk⟩2\lambda_{k-1}\langle B(x_k)-B(x_{k-1}),x-x_k\rangle2λk−1​⟨B(xk​)−B(xk−1​),x−xk​⟩, so the standard Fejér/Opial lemma does not apply directly. Identifying weak cluster points as zeros requires the weak-strong closedness of the graph of A+BA+BA+B, which in turn rests on maximal monotonicity of the sum: this is not a consequence of monotonicity of the two parts, and the inclusion (25) can be passed to the limit only because the step sizes stay above ε\varepsilonε.

Formalization scope

The Lean development uses a real inner product space H (InnerProductSpace ℝ H), complete wherever the page needs it, and the published operator vocabulary ThreeOpSplitting.Accel.MonotoneOperators (monotone and maximally monotone set-valued operators, monotone and Lipschitz single-valued maps, resolvents). Conventions:

  • Resolvents are hypotheses. The iteration is driven by a family J:R→H→HJ:\mathbb R\to H\to HJ:R→H→H with γ−1(w−J(γ)w)∈A(J(γ)w)\gamma^{-1}(w-J(\gamma)w)\in A(J(\gamma)w)γ−1(w−J(γ)w)∈A(J(γ)w) for all γ>0\gamma>0γ>0, w∈Hw\in Hw∈H; for maximally monotone AAA such a family exists and is unique. The goal keeps maximal monotonicity of AAA as a hypothesis as well.
  • Index shift. Lean's x j is xj−1x_{j-1}xj−1​ and lam j is λj−1\lambda_{j-1}λj−1​; the initial points are arbitrary.
  • Step range. Every λj\lambda_jλj​, j≥−1j\ge-1j≥−1, lies in [ε,(1−2ε)/(2L)][\varepsilon,(1-2\varepsilon)/(2L)][ε,(1−2ε)/(2L)], including λ−1\lambda_{-1}λ−1​ as on p. 4. L>0L>0L>0 is assumed, since the range divides by LLL.
  • Weak convergence is convergence of ⟨xk,v⟩\langle x_k,v\rangle⟨xk​,v⟩ for every vvv; cluster points are sequential weak cluster points (subsequences along strictly increasing index maps).
  • Several milestones are stated in a stronger form than the page, with AAA only monotone, HHH not complete, or a conclusion for every zero rather than the cluster point. Each item's note says which.

Three formalizations would trivialize the goal and are excluded:

  • an unconstrained resolvent map;
  • norm convergence or convergence of a subsequence in place of weak convergence of the whole sequence;
  • a step range shrunk or pinned to a constant.

A complete development needs the Opial-type Lemma 2.2, which in turn needs weak sequential compactness of bounded sets in Hilbert space, and maximal monotonicity of A+BA+BA+B for continuous monotone BBB (Bauschke–Combettes, Corollaries 20.25 and 24.4(i)) with its demiclosedness (Proposition 20.33). These are general results of monotone operator theory, and contributions of them as separate theorems are welcome.

Selected references

  • Y. Malitsky and M. K. Tam, A Forward-Backward Splitting Method for Monotone Inclusions Without Cocoercivity, SIAM J. Optim. 30(2), 2020; arXiv:1808.04162v4. https://arxiv.org/abs/1808.04162v4 (DOI https://doi.org/10.1137/18M1207260)
  • H. H. Bauschke and P. L. Combettes, Convex Analysis and Monotone Operator Theory in Hilbert Spaces, 2nd ed., Springer, 2017. https://doi.org/10.1007/978-3-319-48311-5
  • P. Tseng, A modified forward-backward splitting method for maximal monotone mappings, SIAM J. Control Optim. 38(2), 2000. https://doi.org/10.1137/S0363012998338806
  • Y. Malitsky, Projected reflected gradient methods for monotone variational inequalities, SIAM J. Optim. 25(1), 2015. https://doi.org/10.1137/14097238X
  • L. D. Popov, A modification of the Arrow–Hurwicz method for search of saddle points, Math. Notes 28, 1980. https://doi.org/10.1007/BF01141092
  • P.-L. Lions and B. Mercier, Splitting algorithms for the sum of two nonlinear operators, SIAM J. Numer. Anal. 16(6), 1979. https://doi.org/10.1137/0716071
  • Z. Opial, Weak convergence of the sequence of successive approximations for nonexpansive mappings, Bull. Amer. Math. Soc. 73, 1967. https://doi.org/10.1090/S0002-9904-1967-11761-0
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Algorithmic Game TheoryGraph TheoryProbability+1·Captain: mikedeng1

A Case Study on Stochastic Games on Large Graphs in Mean Field and Sparse Regimes I: An Explicit Markovian Nash Equilibrium on Every Finite Transitive GraphResearch Paper

Motivation

Mean field games describe Nash equilibria of large populations in which every player interacts with every other player symmetrically, through the empirical distribution of all states. Many systems of interest are not of this kind: agents in a network interact only with their neighbours, and the interaction structure is a graph rather than a complete graph. Understanding when equilibria on large graphs behave like mean field equilibria, and when they do not, requires models in which the equilibrium on a finite graph can be computed exactly.

Lacker and Soret (arXiv:2005.14102v2, Math. Oper. Res. 2022) introduced such a model: a linear–quadratic flocking game on an arbitrary finite graph, in which each player steers a Brownian particle and pays a terminal penalty for being far from the average of her neighbours. For vertex-transitive graphs they solved the game in closed form, up to a scalar ODE, with an equilibrium that depends on the graph only through the spectrum of its Laplacian. This mission formalizes that finite-graph result, Theorem 2.5 of the paper. Its large-graph consequences are the subject of missions II and III of this series.

Setting

Let GGG be a finite simple graph on vertices V={1,…,n}V=\{1,\dots,n\}V={1,…,n}, with adjacency matrix AGA_GAG​ and degree matrix DGD_GDG​. When GGG has no isolated vertices its random-walk Laplacian is

LG:=DG−1AG−I.L_G := D_G^{-1}A_G - I .LG​:=DG−1​AG​−I.

GGG is transitive if for every two vertices u,vu,vu,v there is a graph automorphism mapping uuu to vvv. A transitive graph is regular, so its Laplacian LG=AG/δ(G)−IL_G = A_G/\delta(G) - ILG​=AG​/δ(G)−I is symmetric, with eigenvalues in [−2,0][-2,0][−2,0].

Fix a horizon T>0T>0T>0, a noise level σ>0\sigma>0σ>0 and a cost constant c>0c>0c>0. Each vertex vvv is a player with state

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

driven by independent Brownian motions WvW_vWv​, from a non-random initial state X(0)=x0∈RVX(0)=x_0\in\mathbb R^VX(0)=x0​∈RV. A Markovian control αv\alpha_vαv​ is a Borel function of time and the full state vector with at most linear growth. Player vvv minimises

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

A profile (αv)v(\alpha_v)_v(αv​)v​ is a Markovian Nash equilibrium if no player can lower her cost by switching unilaterally to another Markovian control.

The equilibrium is built from

QG(x):=det⁡(I−xLG)1/n,fG′(t)=c QG′(fG(t)), fG(0)=0,Q_G(x) := \det(I-xL_G)^{1/n},\qquad f_G'(t) = c\,Q_G'(f_G(t)),\ f_G(0)=0,QG​(x):=det(I−xLG​)1/n,fG′​(t)=cQG′​(fG​(t)), fG​(0)=0, PG(t):=−fG′(T−t) LG(I−fG(T−t)LG)−1,αiG(t,x):=−ei⊤PG(t)x.P_G(t) := -f_G'(T-t)\,L_G\big(I-f_G(T-t)L_G\big)^{-1},\qquad \alpha^G_i(t,x) := -e_i^\top P_G(t)x .PG​(t):=−fG′​(T−t)LG​(I−fG​(T−t)LG​)−1,αiG​(t,x):=−ei⊤​PG​(t)x.

Formalization targets

Goal: Theorem 2.5

For a finite transitive graph GGG without isolated vertices:

  1. QGQ_GQG​ is well defined and continuously differentiable on R+\mathbb R_+R+​, and the ODE has a unique solution fG:[0,T]→R+f_G:[0,T]\to\mathbb R_+fG​:[0,T]→R+​.
  2. (αiG)i(\alpha^G_i)_i(αiG​)i​ is a Markovian Nash equilibrium for every initial state.
  3. For every t∈(0,T]t\in(0,T]t∈(0,T], the equilibrium state X(t)X(t)X(t) is Gaussian with
EX(t)=(I−fG(T−t)LG)(I−fG(T)LG)−1x0,Cov X(t)=σ2(I−fG(T−t)LG)2∫0t(I−fG(T−s)LG)−2 ds.\mathbb E X(t) = (I-f_G(T-t)L_G)(I-f_G(T)L_G)^{-1}x_0,\qquad \mathrm{Cov}\,X(t) = \sigma^2(I-f_G(T-t)L_G)^2\int_0^t(I-f_G(T-s)L_G)^{-2}\,ds .EX(t)=(I−fG​(T−t)LG​)(I−fG​(T)LG​)−1x0​,CovX(t)=σ2(I−fG​(T−t)LG​)2∫0t​(I−fG​(T−s)LG​)−2ds.
  1. The average equilibrium cost satisfies
1n∑vJv=∣PG(0)x0∣22 Tr PG(0)−σ22log⁡Tr PG(0)n fG′(T).\frac1n\sum_{v}J_v = \frac{|P_G(0)x_0|^2}{2\,\mathrm{Tr}\,P_G(0)} - \frac{\sigma^2}{2}\log\frac{\mathrm{Tr}\,P_G(0)}{n\,f_G'(T)} .n1​v∑​Jv​=2TrPG​(0)∣PG​(0)x0​∣2​−2σ2​lognfG′​(T)TrPG​(0)​.

All four parts are in the goal statement.

Milestones

The milestones follow the paper's proof in §2.2, §3 and §4.

  • Graph-spectral facts. Transitive graphs are regular with symmetric LGL_GLG​ (§2.2). The spectrum of LGL_GLG​ lies in [−2,0][-2,0][−2,0] (Remark 2.4). The eigenvalue distribution μG\mu_GμG​ has mean −1-1−1 ((3.2)), and QG=QμGQ_G = Q_{\mu_G}QG​=QμG​​ (§2.3).
  • The ODE. Bounds on QμQ_\muQμ​ and its first two derivatives (Proposition 3.1), and well-posedness of fμ′=cQμ′(fμ)f_\mu' = cQ_\mu'(f_\mu)fμ′​=cQμ′​(fμ​) with explicit bounds (Proposition 3.2).
  • Symmetry. Commutation of LGL_GLG​ with automorphism matrices, and constancy of the diagonal of equivariant matrices (Lemma 4.1).
  • The Riccati system. The properties of PG(t)P_G(t)PG​(t) (§4.4 (i)–(iii)), the reduction of the Nash PDE system to matrix Riccati equations (Lemma 4.2), and the verification that the explicit Fi=(Tr P/n)−1Peiei⊤PF^i = (\mathrm{Tr}\,P/n)^{-1}Pe_ie_i^\top PFi=(TrP/n)−1Pei​ei⊤​P solve them (§4.4).
  • Law and value. The fundamental matrix exp⁡(−∫stP)=(I−f(T−t)L)(I−f(T−s)L)−1\exp(-\int_s^tP) = (I-f(T-t)L)(I-f(T-s)L)^{-1}exp(−∫st​P)=(I−f(T−t)L)(I−f(T−s)L)−1 (§4.5) and the averaged value identity (§4.6).

Significance

The result. Theorem 2.5 is one of the few explicit Nash equilibria of a stochastic differential game on a non-complete graph. Two features of it are not visible in mean field theory. The equilibrium controls are nonlocal: each player reacts to the whole state vector, not only to her neighbours. The whole equilibrium (law, value, controls) depends on the graph only through the spectrum of LGL_GLG​. The second feature drives the paper's later results. Weak convergence of the eigenvalue distributions μGn\mu_{G_n}μGn​​ yields limits of the equilibrium, and these separate the dense regime, where the mean field approximation is valid, from the sparse regime, where it is not.

Formalizing it. The result is proved in the paper; nothing here is open. No machine-checked version of it or of its ingredients exists: the random-walk Laplacian of a graph, linear–quadratic stochastic differential games, verification theorems for Nash systems, and Gaussian laws of linear SDEs with time-dependent coefficients. The mission produces a checked statement of the equilibrium together with reusable layers: spectral facts about D−1A−ID^{-1}A - ID−1A−I, an ODE analysis for QμQ_\muQμ​, and a Riccati reduction for quadratic Nash systems.

Difficulty

Three steps resist a direct approach.

  • The verification theorem. The paper passes from a classical solution of the Nash system (4.1) to a Nash equilibrium by appeal to a standard verification argument. Over the full class of Borel controls with linear growth, this requires Itô's formula for the quadratic value functions, together with integrability of the deviated state processes.
  • The Riccati system. The nnn coupled matrix equations (4.6) have no general closed-form solution. The explicit solution exists only because transitivity forces ei⊤P(t)ei=Tr(P(t))/ne_i^\top P(t)e_i = \mathrm{Tr}(P(t))/nei⊤​P(t)ei​=Tr(P(t))/n for every iii. That identity has to be derived from the action of the automorphism group (Lemma 4.1), not from regularity alone.
  • The law of the state. It requires solving a linear SDE with a time-dependent matrix and identifying its Gaussian law, a step for which the library has little support.

Formalization scope

Lean conventions:

  • Vertices. The vertex set is Fin n, so the paper's 1,…,n1,\dots,n1,…,n become 0,…,n−10,\dots,n-10,…,n−1. The state space is the platform's EthierKurtz.SDEState n (Euclidean Rn\mathbb R^nRn).
  • The Laplacian. LGL_GLG​ is the random-walk Laplacian D−1A−ID^{-1}A-ID−1A−I, not Mathlib's D−AD-AD−A.
  • Time and controls. Time is real. Controls are Borel on R×Rn\mathbb R\times\mathbb R^nR×Rn with linear growth on [0,T][0,T][0,T]; their values off [0,T][0,T][0,T] are never used.
  • Solutions of (2.1). A solution is a pathwise strong solution on a probability space that the solution itself carries, adapted to the completed Brownian filtration. Costs are compared across solutions; this is faithful because (2.1) has a unique strong solution.
  • Costs are [0,∞][0,\infty][0,∞]-valued lower Lebesgue integrals. They are converted to reals only after their finiteness is asserted.
  • Existence of the equilibrium state. The goal also asserts that the equilibrium state equation has a solution, so that the Nash property cannot hold vacuously.
  • Derivatives. fG′(T−t)f_G'(T-t)fG′​(T−t) is written as its ODE value cQG′(fG(T−t))cQ_G'(f_G(T-t))cQG′​(fG​(T−t)). The ODE is solved on [0,T][0,T][0,T] with one-sided derivatives at the endpoints, and uniqueness is agreement on [0,T][0,T][0,T].
  • Matrix conventions. Covariance integrals are entrywise. Gaussian laws are Mathlib's multivariateGaussian.
  • Added hypotheses. 0<n0<n0<n is added to three milestones that are false on the empty graph.

A formalization that fixes x0=0x_0=0x0​=0, restricts deviations to linear controls, drops the existence of the equilibrium state process, or replaces LGL_GLG​ by D−AD-AD−A is not this theorem.

Infrastructure that a complete development needs:

  • symmetric-matrix spectral calculus for LGL_GLG​ and for the matrix functions (I−xL)−1(I-xL)^{-1}(I−xL)−1 and log⁡(I−xL)\log(I-xL)log(I−xL);
  • differentiation under the integral for QμQ_\muQμ​;
  • Picard–Lindelöf and Grönwall on R+\mathbb R_+R+​;
  • Itô's formula for quadratic functions of a diffusion with additive noise;
  • the Gaussian law of ∫0tM(t,s) dWs\int_0^t M(t,s)\,dW_s∫0t​M(t,s)dWs​ for deterministic MMM.

The spectral, ODE and Riccati layers are reusable beyond this mission. Proofs of individual milestones are welcome; so are general verification theorems for linear–quadratic games.

Selected references

  • D. Lacker, A. Soret, A case study on stochastic games on large graphs in mean field and sparse regimes, arXiv:2005.14102v2, 2021; Math. Oper. Res. 47(2), 2022. https://arxiv.org/abs/2005.14102
  • F. Chung, Spectral Graph Theory, CBMS Regional Conference Series in Mathematics 92, AMS, 1997. https://doi.org/10.1090/cbms/092
  • R. Carmona, F. Delarue, Probabilistic Theory of Mean Field Games with Applications I, Springer, 2018. https://doi.org/10.1007/978-3-319-58920-6
  • A. Veretennikov, On strong solutions and explicit formulas for solutions of stochastic integral equations, Math. USSR-Sb. 39(3), 1981. https://doi.org/10.1070/SM1981v039n03ABEH001522
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Three Conjectures in Extremal Spectral Graph Theory 2: For Large n, K₂ + Pₙ₋₂ Is the Unique Planar Graph on n Vertices of Maximum Spectral Radius (Boots–Royle / Cao–Vince Conjecture)Research Paper

Motivation

The spectral radius of a graph, the largest eigenvalue of its adjacency matrix, measures how densely and how unevenly the edges of the graph are distributed. Asking which graph in a class maximizes it is a spectral analogue of the extremal question "which graph in the class has the most edges". For planar graphs the question has a long history in spectral graph theory, going back at least to Schwenk and Wilson. It also arose in geography, where the spectral radius serves as a measure of the connectivity of planar networks. To compare real networks with a theoretical upper bound, geographers wanted the planar graph of maximum spectral radius (arXiv:1606.01916v2, p. 3).

Timeline, as recorded by Tait and Tobin (pp. 1–3):

  • 1978, Schwenk and Wilson: early study of the eigenvalues of planar graphs.
  • 1991, Boots and Royle, and independently 1993, Cao and Vince: conjecture that the planar graph on n≥9n \ge 9n≥9 vertices of maximum spectral radius is P2+Pn−2P_2 + P_{n-2}P2​+Pn−2​ (Conjecture 1 of the paper). The conjecture is false for n∈{7,8}n \in \{7, 8\}n∈{7,8}, so some lower bound on nnn is necessary (p. 2).
  • 1988–2000: successive improvements of the upper bound on the spectral radius of planar graphs, by Hong (1988, 1995, 1998), Cao and Vince (1993), Guiduli (1996) and Ellingham and Zha (2000). These bounds do not identify the extremal graph.
  • 2010, Dvořák and Mohar: an upper bound on the spectral radius of planar graphs of given maximum degree.
  • Guiduli and Hayes were reported by Ellingham and Zha to have proved the conjecture for large nnn. The preprint never appeared (p. 3).
  • 2017, Tait and Tobin: proof of the conjecture for all sufficiently large nnn (Theorem 15).

Setting

All graphs are finite and simple. A graph on nnn vertices has vertex set {0,1,…,n−1}\{0, 1, \dots, n-1\}{0,1,…,n−1}. Its adjacency matrix A(G)A(G)A(G) is the n×nn \times nn×n real matrix with entry 111 in position (u,w)(u, w)(u,w) when u∼wu \sim wu∼w and 000 otherwise. Its eigenvalues are real, and the largest is the spectral radius λ1(G)\lambda_1(G)λ1​(G).

A graph is planar if it can be drawn in the plane with vertices as distinct points and edges as simple arcs joining their ends, such that an arc meets no vertex other than its ends and two arcs meet only at common ends.

For graphs GGG and HHH on disjoint vertex sets, the join G+HG + HG+H is the graph on the union of the two vertex sets that keeps every edge of GGG and of HHH and adds every edge between a vertex of GGG and a vertex of HHH. Write K2K_2K2​ for a single edge, PmP_mPm​ for the path on mmm vertices, and K2+Pn−2K_2 + P_{n-2}K2​+Pn−2​ for their join: two adjacent vertices, both joined to every vertex of a path on the remaining n−2n - 2n−2 vertices. The paper also writes it P2+Pn−2P_2 + P_{n-2}P2​+Pn−2​.

A planar graph GGG on nnn vertices is a planar spectral maximizer if λ1(G′)≤λ1(G)\lambda_1(G') \le \lambda_1(G)λ1​(G′)≤λ1​(G) for every planar graph G′G'G′ on the same nnn vertices.

The milestones refer to a leading eigenvector v\mathbf vv of a maximizer, scaled so that every entry is positive and the largest entry is 111, and to a vertex xxx with vx=1\mathbf v_x = 1vx​=1. For a parameter ε>0\varepsilon > 0ε>0 they use the sets L={z:vz>ε}L = \{z : \mathbf v_z > \varepsilon\}L={z:vz​>ε} and S=V(G)∖LS = V(G) \setminus LS=V(G)∖L, the edge counts e(X)e(X)e(X) (edges inside XXX) and e(X,Y)e(X, Y)e(X,Y) (edges between XXX and YYY), and a second vertex www with vw>1−24ε\mathbf v_w > 1 - 24\varepsilonvw​>1−24ε that is adjacent to all but 94εn94\varepsilon n94εn vertices of SSS.

Formalization targets

Goal: Theorem 15

∃N0 ∀n≥N0 ∀G on n vertices:G is a planar spectral maximizer  ⟺  G≅K2+Pn−2.\exists N_0\ \forall n \ge N_0\ \forall G \text{ on } n \text{ vertices}: \quad G \text{ is a planar spectral maximizer} \iff G \cong K_2 + P_{n-2}.∃N0​ ∀n≥N0​ ∀G on n vertices:G is a planar spectral maximizer⟺G≅K2​+Pn−2​.

The threshold N0N_0N0​ is not fixed. The paper proves the statement only for nnn beyond an unspecified bound, and the conjecture's bound n≥9n \ge 9n≥9 remains open. The equivalence encodes "the unique maximizer is K2+Pn−2K_2 + P_{n-2}K2​+Pn−2​": every maximizer is isomorphic to it, and it is itself a maximizer.

Milestones, in the order of the proof

  1. If HHH is a proper spanning subgraph of a connected graph GGG, then λ1(H)<λ1(G)\lambda_1(H) < \lambda_1(G)λ1​(H)<λ1​(G) (§1.2, already proved on the platform).
  2. A planar graph on n≥3n \ge 3n≥3 vertices has no K3,3K_{3,3}K3,3​ subgraph and at most 3n−63n - 63n−6 edges, and each of its bipartite subgraphs has at most 2n−42n - 42n−4 edges (p. 8).
  3. Lemma 8: 2n−4<λ1<6n\sqrt{2n-4} < \lambda_1 < \sqrt{6n}2n−4​<λ1​<6n​.
  4. The counts ∣L∣≤32n−4/ε|L| \le 3\sqrt{2n-4}/\varepsilon∣L∣≤32n−4​/ε, e(S,L)≤2n−4e(S, L) \le 2n - 4e(S,L)≤2n−4, e(S)≤3n−6e(S) \le 3n - 6e(S)≤3n−6, e(L)≤92n−4/εe(L) \le 9\sqrt{2n-4}/\varepsilone(L)≤92n−4​/ε (p. 8).
  5. Lemma 9: ∑z∈Lvz≤ε2n−4+18/ε\sum_{z \in L} \mathbf v_z \le \varepsilon\sqrt{2n-4} + 18/\varepsilon∑z∈L​vz​≤ε2n−4​+18/ε and ∑z∈Svz≤(1+3ε)2n−4\sum_{z \in S} \mathbf v_z \le (1 + 3\varepsilon)\sqrt{2n-4}∑z∈S​vz​≤(1+3ε)2n−4​.
  6. Eq. (7): ∑y∼u, y∈Svy≥(vu−ε)2n−4−18/ε\sum_{y \sim u,\, y \in S} \mathbf v_y \ge (\mathbf v_u - \varepsilon)\sqrt{2n-4} - 18/\varepsilon∑y∼u,y∈S​vy​≥(vu​−ε)2n−4​−18/ε for u∈Lu \in Lu∈L.
  7. Lemma 10: vz>1/6n\mathbf v_z > 1/\sqrt{6n}vz​>1/6n​ for every vertex zzz.
  8. ∣{y∈S:y≁x}∣≤14εn|\{y \in S : y \not\sim x\}| \le 14\varepsilon n∣{y∈S:y∼x}∣≤14εn (p. 10).
  9. Lemma 11: a vertex w∈Lw \in Lw∈L, w≠xw \ne xw=x, with vw>1−24ε\mathbf v_w > 1 - 24\varepsilonvw​>1−24ε and ∣{y∈S:y≁w}∣≤94εn|\{y \in S : y \not\sim w\}| \le 94\varepsilon n∣{y∈S:y∼w}∣≤94εn.
  10. Lemma 12: vu<1/10\mathbf v_u < 1/10vu​<1/10 for every u∉{x,w}u \notin \{x, w\}u∈/{x,w}.
  11. Lemma 13: x∼wx \sim wx∼w.
  12. Lemma 14: every vertex other than xxx and www is adjacent to both.
  13. A planar graph with two distinct vertices adjacent to all other vertices is a spanning subgraph of K2+Pn−2K_2 + P_{n-2}K2​+Pn−2​ (proof of Theorem 15, p. 13).

Significance

The result. Theorem 15 settles the Boots–Royle / Cao–Vince conjecture for all large nnn. It identifies the planar graph of maximum spectral radius exactly, so the theoretical upper bound that the geographic application asks for is λ1(K2+Pn−2)\lambda_1(K_2 + P_{n-2})λ1​(K2​+Pn−2​). Along the way, Lemmas 8–14 describe the eigenvector of the extremal graph: two vertices carry almost all of the eigenvector weight, and every other entry is below 1/101/101/10. The same method proves the outerplanar analogue (Theorem 7, the companion mission of this series).

Formalizing it. The theorem is proved on paper and has no machine-checked proof. Formalizing it needs several pieces that are absent from Mathlib or the platform and are reusable: the edge bound 3n−63n - 63n−6 and the bipartite bound 2n−42n - 42n−4 for topologically planar graphs, the non-planarity of K3,3K_{3,3}K3,3​ and K5K_5K5​ and of their subdivisions, Rayleigh-quotient comparison of spectral radii, and the face structure of maximal planar graphs. Each milestone is a self-contained target.

Difficulty

Counting edges does not separate the candidates. A maximizer can be taken to be a maximal planar graph, so it has exactly 3n−63n - 63n−6 edges. Every maximal planar graph on nnn vertices has the same number of edges, and the standard lower bound λ1≥2∣E∣/n\lambda_1 \ge 2|E|/nλ1​≥2∣E∣/n is the same for all of them. The extremal graph is pinned down only through its eigenvector. One has to show that the weight concentrates on two vertices, which are then forced to be adjacent to each other (Lemma 13) and to every other vertex (Lemma 14). Lemma 13 is the step specific to planarity. It uses the triangular faces of a maximal planar graph to find an edge switch that keeps the graph planar. In the formal setting, planarity is topological, so every planarity fact of the argument (the edge counts, the K3,3K_{3,3}K3,3​ and K5K_5K5​ obstructions, the faces of a triangulation) has to be derived from the drawing.

Formalization scope

  • Graphs are SimpleGraph (Fin n). "GGG is K2+Pn−2K_2 + P_{n-2}K2​+Pn−2​" is a graph isomorphism G ≃g bookPath n, where bookPath n lives on Fin 2 ⊕ Fin (n - 2). It is not an equality on a fixed labelling.
  • λ1\lambda_1λ1​ is the published WangKangXue.SpectralTuran.specRad, the largest eigenvalue of the real adjacency matrix.
  • Planarity is the published topological RobertsonSeymour1986.GM5.IsPlanar: a drawing by simple arcs. It is not replaced by K5K_5K5​/K3,3K_{3,3}K3,3​-minor-freeness or by an edge count, either of which would change the class the maximum ranges over.
  • Extremality is IsSpecMax IsPlanar G: GGG is planar and λ1(G′)≤λ1(G)\lambda_1(G') \le \lambda_1(G)λ1​(G′)≤λ1​(G) for every planar G′G'G′ on Fin n. Every milestone from Lemma 8 to Lemma 14 assumes it. These lemmas are false for an arbitrary planar graph, so a statement that drops the hypothesis, or replaces it by a property implying the conclusion, is not acceptable.
  • The eigenvector is universally quantified: every v\mathbf vv with Av=λ1vA\mathbf v = \lambda_1 \mathbf vAv=λ1​v, all entries positive, all entries at most 111, and every xxx with vx=1\mathbf v_x = 1vx​=1. Such a vector exists because the maximizer is connected (Perron–Frobenius). A statement that only asserts the existence of some eigenvector is weaker and is ruled out.
  • Quantifiers. "For nnn sufficiently large" is ∃N ∀n≥N\exists N\ \forall n \ge N∃N ∀n≥N, and NNN may depend on ε\varepsilonε. Milestones 4–8 hold for every ε>0\varepsilon > 0ε>0. Lemmas 11–14 hold for 0<ε<ε00 < \varepsilon < \varepsilon_00<ε<ε0​ with an unspecified ε0\varepsilon_0ε0​, because the paper chooses ε\varepsilonε small. The quantifier on ε\varepsilonε is always outermost, so ε\varepsilonε never depends on nnn or GGG. Lemmas 12–14 hold for every vertex www satisfying the conclusion of Lemma 11 (the predicate IsSecondHub), with the constants 242424 and 949494.
  • Added hypotheses. n≥3n \ge 3n≥3 in the planar facts and in Lemma 8, where the paper's standing "nnn large enough" is needed only to that extent. The page names the vertex of Lemma 12 vvv, the same letter as the eigenvector; it is renamed uuu. Lemma 14's set AAA is stated in unfolded form.
  • Infrastructure that a complete development needs: Euler's formula for topologically planar graphs, the non-planarity of K3,3K_{3,3}K3,3​ and K5K_5K5​, Perron–Frobenius for connected graphs, and the Rayleigh quotient. Proofs of the planar facts (milestone 2) are reusable well beyond this mission. Contributions toward any of them are welcome.

Selected references

  • M. Tait and J. Tobin, Three conjectures in extremal spectral graph theory, J. Combin. Theory Ser. B (2017). Preprint arXiv:1606.01916v2. https://arxiv.org/abs/1606.01916, DOI https://doi.org/10.1016/j.jctb.2017.04.006
  • B. N. Boots and G. F. Royle, A conjecture on the maximum value of the principal eigenvalue of a planar graph, Geographical Analysis 23(3) (1991), 276–282.
  • D. Cao and A. Vince, The spectral radius of a planar graph, Linear Algebra Appl. 187 (1993), 251–257.
  • A. J. Schwenk and R. J. Wilson, On the eigenvalues of a graph, in: Selected Topics in Graph Theory, Academic Press, 1978, 307–336.
  • Hong Yuan, A bound on the spectral radius of graphs, Linear Algebra Appl. 108 (1988), 135–139.
  • M. N. Ellingham and X. Zha, The spectral radius of graphs on surfaces, J. Combin. Theory Ser. B 78(1) (2000), 45–56.
  • Z. Dvořák and B. Mohar, Spectral radius of finite and infinite planar graphs and of graphs of bounded genus, J. Combin. Theory Ser. B 100(6) (2010), 729–739.

Bibliographic data as given in the bibliography of Tait and Tobin (pp. 21–23).

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

Motivation

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

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

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

Setting

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

The Wasserstein distance of order ppp is given by

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

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

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

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

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

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

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

Formalization targets

Goal: Theorem 1 (p. 17)

If κ<∞\kappa<\inftyκ<∞, then

vP=vD<∞.v_P=v_D<\infty.vP​=vD​<∞.

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

Milestones

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

Significance

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

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

Difficulty

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

Formalization scope

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

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

Selected references

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

Three Conjectures in Extremal Spectral Graph Theory 1: For Large n, K₁ + Pₙ₋₁ Is the Unique Outerplanar Graph on n Vertices of Maximum Spectral Radius (Cvetković–Rowlinson Conjecture)Research Paper

Motivation

The spectral radius λ1(G)\lambda_1(G)λ1​(G) of a graph GGG, the largest eigenvalue of its adjacency matrix, is a standard measure of how densely and how centrally a graph is connected. A classical theme of spectral graph theory asks, for a natural family of graphs, which member of the family on nnn vertices maximizes λ1\lambda_1λ1​. For planar graphs this question was raised by geographers comparing road and transport networks, and for outerplanar graphs it was posed by Cvetković and Rowlinson in their 1990 survey of the largest eigenvalue of a graph, where they relate it to the study of subfamilies of Hamiltonian graphs.

Conjecture (Cvetković–Rowlinson, 1990). The outerplanar graph on nnn vertices of maximum spectral radius is K1+Pn−1K_1 + P_{n-1}K1​+Pn−1​.

Timeline:

  • 1990. Cvetković and Rowlinson state the conjecture (Linear and Multilinear Algebra 28).
  • 1990. Rowlinson makes partial progress, on the index of certain outerplanar graphs (Ars Combinatoria 29).
  • 1993. Cao and Vince work on the spectral radius of planar graphs and the related conjecture (Linear Algebra Appl. 187).
  • 2001. Zhou, Lin and Hu study the spectral radius of Hamiltonian planar and outerplanar graphs (Tsinghua Science and Technology 6).
  • 2017. Tait and Tobin prove the conjecture for all sufficiently large nnn (arXiv:1606.01916, J. Combin. Theory Ser. B, doi:10.1016/j.jctb.2017.04.006), Theorem 7.

This mission formalizes Section 2 of Tait and Tobin.

Setting

All graphs are finite and simple. An nnn-vertex graph GGG has vertex set V(G)={0,…,n−1}V(G) = \{0, \dots, n-1\}V(G)={0,…,n−1}, adjacency matrix A(G)A(G)A(G), and spectral radius λ1(G)\lambda_1(G)λ1​(G), the largest eigenvalue of the real symmetric matrix A(G)A(G)A(G). Write dud_udu​ for the degree of a vertex uuu and N(u)N(u)N(u) for its neighbourhood.

A plane drawing of GGG places the vertices at distinct points of R2\mathbb R^2R2 and each edge as a simple arc between its ends; an arc passes through no other vertex, and two arcs meet only at a common end. The union of the vertex points and arcs is a compact set, so its complement has exactly one unbounded connected component, the outer face. A graph is outerplanar if it has a plane drawing in which every vertex lies on the boundary of the outer face.

The join G+HG + HG+H of two graphs is their disjoint union together with all edges between them. The fan K1+Pn−1K_1 + P_{n-1}K1​+Pn−1​ is a single vertex joined to every vertex of a path on n−1n-1n−1 vertices; it is outerplanar and has 2n−32n-32n−3 edges.

An outerplanar graph GGG on nnn vertices is a spectral maximizer if λ1(G′)≤λ1(G)\lambda_1(G') \le \lambda_1(G)λ1​(G′)≤λ1​(G) for every outerplanar graph G′G'G′ on the same nnn vertices.

Several milestones refer to a Perron vector: an eigenvector v\mathbf vv of A(G)A(G)A(G) for λ1\lambda_1λ1​ with all entries positive, normalized so that its maximum entry is 111, together with a vertex xxx with vx=1\mathbf v_x = 1vx​=1. For a connected graph such a vector exists by the Perron–Frobenius theorem.

Formalization targets

Goal: Theorem 7

There is NNN such that for every n≥Nn \ge Nn≥N and every graph GGG on nnn vertices,

G is an outerplanar spectral maximizer  ⟺  G≅K1+Pn−1.G \text{ is an outerplanar spectral maximizer} \iff G \cong K_1 + P_{n-1}.G is an outerplanar spectral maximizer⟺G≅K1​+Pn−1​.

The forward direction is the paper's Theorem 7; the converse says that the fan is the maximizer, as the conjecture reads. The threshold NNN is left unspecified, as in the paper.

Milestones

The milestones follow the proof in Section 2, in order:

  1. a strict subgraph of a connected graph has strictly smaller λ1\lambda_1λ1​ (already proved on the platform);
  2. an outerplanar graph on n≥2n \ge 2n≥2 vertices has at most 2n−32n-32n−3 edges and no K2,3K_{2,3}K2,3​ subgraph;
  3. Lemma 3: for n≥3n \ge 3n≥3 a spectral maximizer has λ1>n−1\lambda_1 > \sqrt{n-1}λ1​>n−1​;
  4. Lemma 4: du>vun−11nd_u > \mathbf v_u n - 11\sqrt ndu​>vu​n−11n​ for every vertex uuu;
  5. Lemma 5: for nnn large, dx>n−11nd_x > n - 11\sqrt ndx​>n−11n​ and vu<C1/n\mathbf v_u < C_1/\sqrt nvu​<C1​/n​ for every u≠xu \ne xu=x, with an absolute constant C1C_1C1​;
  6. Lemma 6: for nnn large, ∑z∈Bvz<C2/n\sum_{z\in B}\mathbf v_z < C_2/\sqrt n∑z∈B​vz​<C2​/n​, where B=V(G)∖(N(x)∪{x})B = V(G)\setminus(N(x)\cup\{x\})B=V(G)∖(N(x)∪{x});
  7. for nnn large, B=∅B = \emptysetB=∅: xxx is adjacent to every other vertex;
  8. an outerplanar graph with a vertex adjacent to all others is a spanning subgraph of K1+Pn−1K_1 + P_{n-1}K1​+Pn−1​.

Significance

The theorem settles, for all large nnn, a conjecture that had been open since 1990 and had resisted several partial attacks. The same paper settles, in the same framework, the planar analogue (the Boots–Royle and Cao–Vince conjecture, K2+Pn−2K_2 + P_{n-2}K2​+Pn−2​) and a conjecture on spectral irregularity. The outerplanar case is the shortest of the three.

On the formal side, the result is proved on paper but has no machine-checked proof. Completing the mission produces a formal theory of outerplanar plane drawings (edge bound, K2,3K_{2,3}K2,3​-freeness, outerplanarity of the fan), eigenvector estimates for extremal graphs, and the full extremal theorem. The edge bound and the K2,3K_{2,3}K2,3​ exclusion are reusable for any later work on outerplanar or series–parallel graphs. Determining the exact threshold NNN, or proving the statement for every n≥2n \ge 2n≥2, would be a strengthening beyond the paper.

Difficulty

There are two separate difficulties. The first is topological: the facts about outerplanar graphs that the spectral argument uses (at most 2n−32n-32n−3 edges, no K2,3K_{2,3}K2,3​ subgraph, no cycle in G−xG - xG−x when xxx dominates, outerplanarity of the fan) are folklore on paper but require a Jordan-curve-type argument about plane drawings, of which Mathlib currently contains very little. The second is spectral: the edge-switching step that proves B=∅B = \emptysetB=∅ compares λ1\lambda_1λ1​ of two graphs through the Rayleigh quotient, and needs a positive Perron vector and the variational characterization of the largest eigenvalue for symmetric matrices. A purely combinatorial edge-maximization argument does not work: the fan is not the only outerplanar graph with 2n−32n-32n−3 edges, so maximizing the number of edges does not identify the spectral maximizer.

Formalization scope

  • Graphs are SimpleGraph (Fin n); λ1\lambda_1λ1​ is the published WangKangXue.SpectralTuran.specRad, the largest eigenvalue of G.adjMatrix ℝ.
  • Outerplanarity is topological: a published RobertsonSeymour1986.GM5.PlaneDrawing with every vertex point in the closure of the unbounded component of the complement of the drawing. It is not replaced by a forbidden-minor characterization; such characterizations are theorems about outerplanarity, and would change which graphs compete in the maximization.
  • Extremality is IsSpecMax IsOuterplanar G: GGG is outerplanar and no outerplanar graph on the same vertex set has larger λ1\lambda_1λ1​. It is never weakened to a comparison with the fan.
  • "GGG is K1+Pn−1K_1 + P_{n-1}K1​+Pn−1​" is a graph isomorphism G ≃g fan n, with the fan on Fin 1 ⊕ Fin (n - 1).
  • Perron-vector statements quantify over every positive eigenvector for λ1\lambda_1λ1​ with maximum entry 111 and every vertex xxx with vx=1\mathbf v_x = 1vx​=1; existential quantification over v\mathbf vv would be weaker.
  • "For some absolute constant" is an existential quantifier placed before the threshold, the graph and the vector; "for nnn sufficiently large" is ∃ N, ∀ n ≥ N.
  • Added hypotheses, each forced by a degenerate case: n≥2n \ge 2n≥2 for the edge bound (the bound 2n−32n-32n−3 is negative below), n≥3n \ge 3n≥3 for Lemma 3 (it fails for n=2n = 2n=2, where the maximizer K2K_2K2​ has λ1=1=n−1\lambda_1 = 1 = \sqrt{n-1}λ1​=1=n−1​).

A complete development needs the Perron–Frobenius theorem for symmetric nonnegative matrices and the Rayleigh quotient characterization of λ1\lambda_1λ1​, both of general use; the theory of outerplanar drawings; and the counting arguments of the lemmas. Contributions to any of these layers are welcome, as are independent proofs of the outerplanar facts from the drawing definition.

Selected references

  • M. Tait and J. Tobin, Three conjectures in extremal spectral graph theory, J. Combin. Theory Ser. B (2017), https://doi.org/10.1016/j.jctb.2017.04.006; preprint arXiv:1606.01916v2, https://arxiv.org/abs/1606.01916
  • D. Cvetković and P. Rowlinson, The largest eigenvalue of a graph: a survey, Linear and Multilinear Algebra 28 (1990), 3–33.
  • P. Rowlinson, On the index of certain outerplanar graphs, Ars Combinatoria 29 (1990), 221–225.
  • D. Cao and A. Vince, The spectral radius of a planar graph, Linear Algebra Appl. 187 (1993), 251–257.
  • J. Zhou, C. Lin and G. Hu, Spectral radius of Hamiltonian planar graphs and outerplanar graphs, Tsinghua Science and Technology 6 (2001), 350–354.
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Control TheoryConvex OptimizationGraph Theory+1·Captain: mikedeng1

Achieving Geometric Convergence for Distributed Optimization Over Time-Varying Graphs 2: Push-DIGing Converges R-Linearly over Time-Varying Directed Graphs for Every Step Size Below 1.5(1−δ)²/(μ̄J₂)Research Paper

Distributed optimization over directed, changing networks

In distributed optimization, nnn agents cooperatively minimize the average f(x)=1n∑i=1nfi(x)f(x)=\frac1n\sum_{i=1}^n f_i(x)f(x)=n1​∑i=1n​fi​(x) of private cost functions fi:Rp→Rf_i:\mathbb R^p\to\mathbb Rfi​:Rp→R, exchanging information only with their current neighbours in a communication network. The model covers sensor networks, multi-robot coordination and machine learning with data split across machines, where no node can see the whole objective. In many of these systems communication is one-directional (broadcast radios with unequal ranges, asymmetric links) and the network changes over time.

Directed links raise a specific obstacle: a node cannot in general choose weights that are both row and column stochastic, because it knows its out-degree but not how its messages are combined by others. The push-sum (ratio consensus) protocol of Kempe, Dobra and Gehrke (2003) circumvents this with column stochastic weights and a scalar correction. Nedić and Olshevsky (2015) combined it with diminishing-step subgradient methods over time-varying directed graphs, obtaining sublinear rates. Gradient tracking methods (Xu, Zhu, Soh and Xie, 2015; Qu and Li, 2016) and EXTRA (Shi, Ling, Wu and Yin, 2015) reached linear rates with constant steps on undirected or static graphs. Nedić, Olshevsky and Shi (arXiv 2016, SIAM J. Optim. 2017) proved geometric convergence of gradient tracking over graphs that are both time-varying and directed; this mission formalizes that result.

Setting

The agents are {1,…,n}\{1,\dots,n\}{1,…,n}. At each time kkk there is a set A(k)\mathcal A(k)A(k) of arcs; an arc j→ij\to ij→i means agent jjj can send to agent iii. The out-degree djout(k)d^{\rm out}_j(k)djout​(k) counts the agents i≠ji\ne ji=j with j→ij\to ij→i in A(k)\mathcal A(k)A(k).

Assumption 6. There is B~⊖>0\tilde B_\ominus>0B~⊖​>0 such that for every t≥0t\ge0t≥0 the union of the arc sets over the window tB~⊖,…,(t+1)B~⊖−1t\tilde B_\ominus,\dots,(t+1)\tilde B_\ominus-1tB~⊖​,…,(t+1)B~⊖​−1 is strongly connected. Put B⊖=2B~⊖−1B_\ominus=2\tilde B_\ominus-1B⊖​=2B~⊖​−1.

Assumption 7. The mixing matrix C(k)C(k)C(k) has Cij(k)=1/(djout(k)+1)C_{ij}(k)=1/(d^{\rm out}_j(k)+1)Cij​(k)=1/(djout​(k)+1) if i=ji=ji=j or j→i∈A(k)j\to i\in\mathcal A(k)j→i∈A(k), and 000 otherwise; each C(k)C(k)C(k) is column stochastic.

Each fif_ifi​ is differentiable with LiL_iLi​-Lipschitz gradient (Assumption 4) and μi\mu_iμi​-strongly convex with μi≥0\mu_i\ge0μi​≥0, some μi>0\mu_i>0μi​>0 (Assumption 5). Write L=max⁡iLiL=\max_iL_iL=maxi​Li​, μˉ=1n∑iμi\bar\mu=\frac1n\sum_i\mu_iμˉ​=n1​∑i​μi​, κˉ=L/μˉ\bar\kappa=L/\bar\muκˉ=L/μˉ​, and x∗x^*x∗ for the minimizer of fff.

Iterates are n×pn\times pn×p matrices whose row iii belongs to agent iii; ∇f(x)\nabla\mathbf f(\mathbf x)∇f(x) has rows ∇fi(xi)\nabla f_i(x_i)∇fi​(xi​), and ∥⋅∥F\|\cdot\|_F∥⋅∥F​ is the Frobenius norm. Push-DIGing starts from x(0)=u(0)\mathbf x(0)=\mathbf u(0)x(0)=u(0), y(0)=∇f(x(0))\mathbf y(0)=\nabla\mathbf f(\mathbf x(0))y(0)=∇f(x(0)), v(0)=1\mathbf v(0)=\mathbf 1v(0)=1 and iterates, with step size α>0\alpha>0α>0 and V(k)=diag⁡{v(k)}V(k)=\operatorname{diag}\{\mathbf v(k)\}V(k)=diag{v(k)},

u(k+1)=C(k)(u(k)−αy(k)),v(k+1)=C(k)v(k),x(k+1)=V(k+1)−1u(k+1),\mathbf u(k+1)=C(k)(\mathbf u(k)-\alpha\mathbf y(k)),\quad \mathbf v(k+1)=C(k)\mathbf v(k),\quad \mathbf x(k+1)=V(k+1)^{-1}\mathbf u(k+1),u(k+1)=C(k)(u(k)−αy(k)),v(k+1)=C(k)v(k),x(k+1)=V(k+1)−1u(k+1), y(k+1)=C(k)y(k)+∇f(x(k+1))−∇f(x(k)).\mathbf y(k+1)=C(k)\mathbf y(k)+\nabla\mathbf f(\mathbf x(k+1))-\nabla\mathbf f(\mathbf x(k)).y(k+1)=C(k)y(k)+∇f(x(k+1))−∇f(x(k)).

The constants of the rate are τ~=n−(2+nB⊖)\tilde\tau=n^{-(2+nB_\ominus)}τ~=n−(2+nB⊖​), Q1=2n(1+τ~−nB⊖)/(1−τ~nB⊖)Q_1=2n(1+\tilde\tau^{-nB_\ominus})/(1-\tilde\tau^{nB_\ominus})Q1​=2n(1+τ~−nB⊖​)/(1−τ~nB⊖​), ∥V−1∥max⁡1=sup⁡k,i1/vi(k)\|V^{-1}\|^1_{\max}=\sup_{k,i}1/v_i(k)∥V−1∥max1​=supk,i​1/vi​(k) and, for an integer BBB,

δ=Q1(1−τ~nB⊖)B−1nB⊖,J2=3Q1∥V−1∥max⁡1κˉB(δ+Q1(B−1))(1+n)(1+4nκˉ).\delta=Q_1\big(1-\tilde\tau^{nB_\ominus}\big)^{\frac{B-1}{nB_\ominus}},\qquad J_2=3Q_1\|V^{-1}\|^1_{\max}\bar\kappa B\big(\delta+Q_1(B-1)\big)(1+\sqrt n)\big(1+4\sqrt n\sqrt{\bar\kappa}\big).δ=Q1​(1−τ~nB⊖​)nB⊖​B−1​,J2​=3Q1​∥V−1∥max1​κˉB(δ+Q1​(B−1))(1+n​)(1+4n​κˉ​).

Formalization targets

Goal: Theorem 18

For n≥2n\ge2n≥2, B≥B⊖B\ge B_\ominusB≥B⊖​ with δ<1\delta<1δ<1, and every step size

0<α<1.5(1−δ)2μˉJ2,0<\alpha<\frac{1.5(1-\delta)^2}{\bar\mu J_2},0<α<μˉ​J2​1.5(1−δ)2​,

there is C>0C>0C>0 with ∥x(k)−1(x∗)⊤∥F≤Cλk\|\mathbf x(k)-\mathbf 1(x^*)^\top\|_F\le C\lambda^k∥x(k)−1(x∗)⊤∥F​≤Cλk for all kkk, where 0<λ<10<\lambda<10<λ<1 is

λ=1−αμˉ/1.52B  if  α≤1.5(J22+(1−δ2)J2−δJ2)2μˉJ2(J2+1)2,λ=αμˉJ2/1.5+δB  otherwise.\lambda=\sqrt[2B]{1-\alpha\bar\mu/1.5}\ \text{ if }\ \alpha\le\frac{1.5\big(\sqrt{J_2^2+(1-\delta^2)J_2}-\delta J_2\big)^2}{\bar\mu J_2(J_2+1)^2},\qquad \lambda=\sqrt[B]{\sqrt{\alpha\bar\mu J_2/1.5}+\delta}\ \text{ otherwise}.λ=2B1−αμˉ​/1.5​  if  α≤μˉ​J2​(J2​+1)21.5(J22​+(1−δ2)J2​​−δJ2​)2​,λ=Bαμˉ​J2​/1.5​+δ​  otherwise.

Milestones

The paper's proof runs a small gain argument around the cycle q→z→hˇ→xˇ→q\mathbf q\to\mathbf z\to\check{\mathbf h}\to\check{\mathbf x}\to\mathbf qq→z→hˇ→xˇ→q, where q(k)=x(k)−1(x∗)⊤\mathbf q(k)=\mathbf x(k)-\mathbf 1(x^*)^\topq(k)=x(k)−1(x∗)⊤, z\mathbf zz are gradient increments, h(k)=V(k)−1y(k)\mathbf h(k)=V(k)^{-1}\mathbf y(k)h(k)=V(k)−1y(k) and  ˇ\check{\ } ˇ is the deviation from the row average. The milestones are the paper's own statements: the equivalent recursion (48) in terms of the row stochastic R~(k)=V(k+1)−1C(k)V(k)\tilde R(k)=V(k+1)^{-1}C(k)V(k)R~(k)=V(k+1)−1C(k)V(k); the bound (49) ∥V−1∥max⁡1≤nnB⊖\|V^{-1}\|^1_{\max}\le n^{nB_\ominus}∥V−1∥max1​≤nnB⊖​ and row stochasticity of R~(k)\tilde R(k)R~(k); Lemma 13 (BBB-step contraction by δ\deltaδ); Lemmas 14–17 (the four arrows); Lemma 8 (an error bound for inexact gradient descent); Theorem 3 (the small gain theorem) and Lemma 4.

Significance

The theorem gives a geometric rate, with explicit constants, for a first-order method that uses only out-degree information, constant step sizes, one gradient per agent per round, and networks that are directed and need only be strongly connected jointly over windows. Before it, linear rates for distributed gradient methods required undirected or static graphs. The explicit λ\lambdaλ quantifies how the rate degrades with nnn, B⊖B_\ominusB⊖​ and the condition number κˉ\bar\kappaκˉ. The result is proved in the paper; to the extent known, no machine-checked proof exists. A formalization yields a checked statement of the rate together with reusable components: the ergodic-norm small gain theorem, the push-sum weight bound, and the inexact gradient lemma, which also serve the companion DIGing mission on undirected graphs.

Difficulty

The natural Lyapunov approach fails: with asymmetric, time-varying weights there is in general no quadratic function that decreases at every step, and the consensus error contracts only over windows of BBB iterations. The analysis therefore works with ergodic norms max⁡k≤Kλ−k∥s(k)∥F\max_{k\le K}\lambda^{-k}\|\mathbf s(k)\|_Fmaxk≤K​λ−k∥s(k)∥F​ and chains four inequalities. Two further inputs come from outside the paper: the lower bound vi(k)≥n−nB⊖v_i(k)\ge n^{-nB_\ominus}vi​(k)≥n−nB⊖​ (Corollary 2(b) of Nedić–Olshevsky 2015) and the contraction of products of row stochastic matrices with entries bounded below on arcs (Lemma 5 of Nedić–Ozdaglar 2010), both of which a complete development has to prove.

Formalization scope

Stacked iterates are functions Fin n → EuclideanSpace ℝ (Fin p); agents are indexed from 0 and time from 0. An arc j→ij\to ij→i is a pair (j, i) in a finite set A k. The weights v(k)\mathbf v(k)v(k) are defined from CCC alone, so ∥V−1∥max⁡1\|V^{-1}\|^1_{\max}∥V−1∥max1​ is a constant of the graph sequence; it enters statements as a number with the hypothesis that it is the least upper bound of {1/vi(k)}\{1/v_i(k)\}{1/vi​(k)}, never as a real supremum. Real powers are Real.rpow. The ergodic norm is the truncated maximum; the untruncated supremum is replaced by its pointwise meaning.

Four hypotheses are added to the page, each disclosed in the statements:

  1. Assumption 7 includes the self-weight Cjj(k)=1/(djout(k)+1)C_{jj}(k)=1/(d^{\rm out}_j(k)+1)Cjj​(k)=1/(djout​(k)+1). The printed rule assigns weights on arcs only, which makes column sums d/(d+1)d/(d+1)d/(d+1); the paper's agent updates (p. 21) and analysis use the push-sum convention.
  2. The step-size interval is open on the right: at α=1.5(1−δ)2/(μˉJ2)\alpha=1.5(1-\delta)^2/(\bar\mu J_2)α=1.5(1−δ)2/(μˉ​J2​) the printed formula gives λ=1\lambda=1λ=1.
  3. B≥B⊖B\ge B_\ominusB≥B⊖​, required by Lemma 13, makes "large enough" precise.
  4. n≥2n\ge2n≥2: at n=1n=1n=1 the constant Q1Q_1Q1​ has a zero denominator.

The goal states only the hypotheses of Theorem 18 and the rate; it does not assume any of the arrows, gains, auxiliary parameters β,η\beta,\etaβ,η or ergodic-norm bounds, so it cannot be discharged by assembling hypotheses.

A complete development needs matrix-product contraction bounds for push-sum, Frobenius-norm calculus on stacked matrices, and strong convexity estimates for inexact gradient steps. The small gain theorem, Lemma 8 and the push-sum lemmas are reusable beyond this mission. Proofs of individual milestones are welcome independently.

Selected references

  • A. Nedić, A. Olshevsky, W. Shi, Achieving geometric convergence for distributed optimization over time-varying graphs, SIAM J. Optim. 27 (2017) 2597–2633; arXiv:1607.03218v3. https://arxiv.org/abs/1607.03218 — https://doi.org/10.1137/16M1084316
  • A. Nedić, A. Olshevsky, Distributed optimization over time-varying directed graphs, IEEE Trans. Automat. Control 60 (2015) 601–615. https://arxiv.org/abs/1303.2289
  • A. Nedić, A. Olshevsky, Stochastic gradient-push for strongly convex functions on time-varying directed graphs, arXiv:1406.2075, 2014. https://arxiv.org/abs/1406.2075
  • D. Kempe, A. Dobra, J. Gehrke, Gossip-based computation of aggregate information, Proc. 44th IEEE FOCS, 2003, 482–491. https://doi.org/10.1109/SFCS.2003.1238221
  • W. Shi, Q. Ling, G. Wu, W. Yin, EXTRA: an exact first-order algorithm for decentralized consensus optimization, SIAM J. Optim. 25 (2015) 944–966. https://arxiv.org/abs/1404.6264
  • G. Qu, N. Li, Harnessing smoothness to accelerate distributed optimization, arXiv:1605.07112, 2016. https://arxiv.org/abs/1605.07112
  • J. Xu, S. Zhu, Y. C. Soh, L. Xie, Augmented distributed gradient methods for multi-agent optimization under uncoordinated constant stepsizes, Proc. 54th IEEE CDC, 2015, 2055–2060.
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Operations ResearchOptimizationProbability·Captain: mikedeng1

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

Why trade credit terms matter

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

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

The model

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

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

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

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

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

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

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

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

Formalization targets

Goal: Proposition 3 (p. 15)

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

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

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

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

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

Milestones

They are listed in the order the proof uses them:

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

Significance

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

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

Difficulty

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

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

Formalization scope

All objects live in TradeCredit.Terms.Model.

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

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

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

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

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

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

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

Selected references

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

Three Conjectures in Extremal Spectral Graph Theory 3: For Large n, a Connected n-Vertex Graph Maximizing Spectral Radius Minus Average Degree Is a Pineapple GraphResearch Paper

Motivation

How far is a graph from being regular? Several numerical irregularity measures answer this question, and spectral graph theory supplies a natural one. For a graph GGG with nnn vertices and e(G)e(G)e(G) edges, the largest eigenvalue λ1(G)\lambda_1(G)λ1​(G) of the adjacency matrix is always at least the average degree d(G)=2e(G)/nd(G) = 2e(G)/nd(G)=2e(G)/n, with equality exactly when GGG is regular. The difference λ1−d\lambda_1 - dλ1​−d is therefore a measure of irregularity; it was studied by Bell (1992) alongside the variance of the degrees, and it is one of several such measures, with Albertson's ∑uv∈E∣du−dv∣\sum_{uv \in E} |d_u - d_v|∑uv∈E​∣du​−dv​∣ and Nikiforov's degree deviation among the others. The measures are incomparable in general, and one way to understand what each gauges is to determine its extremal graphs.

A basic extremal question asks which graphs are the most irregular. Among all graphs the question is uninteresting, because isolated vertices lower ddd without lowering λ1\lambda_1λ1​. Among connected graphs it is a genuine optimization problem. Using the variable neighbourhood search system AutoGraphiX, Aouchiche, Bell, Cvetković, Hansen, Rowlinson, Simić and Stevanović (2008) found that the maximizers of λ1−d\lambda_1 - dλ1​−d over connected graphs on nnn vertices are always pineapple graphs, a clique with pendant vertices hanging from one clique vertex, and they conjectured that this holds for every nnn (Aouchiche et al., European J. Oper. Res. 2008).

Timeline:

  • 1992: Bell compares λ1−d\lambda_1 - dλ1​−d with the degree variance as irregularity measures.
  • 1988: Hong proves λ12≤2e(G)−(n−1)\lambda_1^2 \le 2e(G) - (n-1)λ12​≤2e(G)−(n−1) for graphs without isolated vertices.
  • 2008: Aouchiche et al. state the pineapple conjecture from computer experiments, and determine which pineapple is best (clique size ⌈n/2⌉+1\lceil n/2\rceil + 1⌈n/2⌉+1).
  • 2017: Tait and Tobin prove the conjecture for all sufficiently large nnn (arXiv:1606.01916, J. Combin. Theory Ser. B), in the same paper that settles the spectral extremal problems for outerplanar and planar graphs.

This mission formalizes Section 4 of Tait and Tobin.

Setting

All graphs are finite and simple; an nnn-vertex graph has vertex set {0,…,n−1}\{0, \dots, n-1\}{0,…,n−1}. The spectral radius λ1(G)\lambda_1(G)λ1​(G) is the largest eigenvalue of the adjacency matrix AAA of GGG, the published platform definition specRad. The average degree is d(G)=2e(G)/nd(G) = 2e(G)/nd(G)=2e(G)/n, a real number.

A connected graph GGG on nnn vertices is a maximizer of λ1−d\lambda_1 - dλ1​−d (Lean: IsIrregMax G) if

λ1(G′)−d(G′)≤λ1(G)−d(G)for every connected graph G′ on the same n vertices.\lambda_1(G') - d(G') \le \lambda_1(G) - d(G) \quad \text{for every connected graph } G' \text{ on the same } n \text{ vertices.}λ1​(G′)−d(G′)≤λ1​(G)−d(G)for every connected graph G′ on the same n vertices.

The pineapple PA(p,q)PA(p,q)PA(p,q) (Lean: pineapple p q) has p+qp+qp+q vertices: the first ppp form a complete graph KpK_pKp​, and each of the other qqq vertices is a pendant vertex, adjacent only to the clique vertex 000. Stars (p≤2p \le 2p≤2) and complete graphs (q=0q = 0q=0) are degenerate pineapples.

The lemmas of the mission speak about the leading eigenvector v\mathbf vv of a maximizer GGG: a vector with Av=λ1vA\mathbf v = \lambda_1 \mathbf vAv=λ1​v, all entries positive, normalized so that its largest entry is 111. Such a vector exists by the Perron–Frobenius theorem because GGG is connected. xxx denotes a vertex with vx=1\mathbf v_x = 1vx​=1, dud_udu​ the degree of uuu, and N(x)N(x)N(x) the neighbourhood of xxx. Some statements carry a small parameter ε>0\varepsilon > 0ε>0, fixed before nnn.

Formalization targets

Goal: Theorem 21

∃N ∀n≥N ∀G on n vertices:G maximizes λ1−d  ⟹  ∃ p,q, p+q=n, G≅PA(p,q).\exists N\ \forall n \ge N\ \forall G \text{ on } n \text{ vertices}:\quad G \text{ maximizes } \lambda_1 - d \;\Longrightarrow\; \exists\, p, q,\ p + q = n,\ G \cong PA(p,q).∃N ∀n≥N ∀G on n vertices:G maximizes λ1​−d⟹∃p,q, p+q=n, G≅PA(p,q).

The clique size ppp is left free. The optimal value p=⌈n/2⌉+1p = \lceil n/2\rceil + 1p=⌈n/2⌉+1 is determined by Aouchiche et al. by optimizing a cubic polynomial over pineapples; Tait and Tobin cite it and do not prove it, so it is not part of the goal.

Milestones, in the order of the proof

  1. Hong's inequality λ12≤2e(G)−(n−1)\lambda_1^2 \le 2e(G) - (n-1)λ12​≤2e(G)−(n−1) for connected GGG (cited, p. 14).
  2. The pineapple H=PA(⌈n/2⌉+1,⌊n/2⌋−1)H = PA(\lceil n/2\rceil+1, \lfloor n/2\rfloor-1)H=PA(⌈n/2⌉+1,⌊n/2⌋−1) has λ1(H)−2e(H)/n≥n/4−3/2\lambda_1(H) - 2e(H)/n \ge n/4 - 3/2λ1​(H)−2e(H)/n≥n/4−3/2 (p. 14).
  3. Lemma 16: λ1=n/2+c1n\lambda_1 = n/2 + c_1\sqrt nλ1​=n/2+c1​n​ and d=n/4+c2nd = n/4 + c_2\sqrt nd=n/4+c2​n​ with ∣c1∣,∣c2∣<1|c_1|, |c_2| < 1∣c1​∣,∣c2​∣<1.
  4. Lemma 17: 0≤1∣N(x)∣∑y∼x(dy−λ1vy)≤c3n0 \le \frac{1}{|N(x)|}\sum_{y\sim x}(d_y - \lambda_1\mathbf v_y) \le c_3\sqrt n0≤∣N(x)∣1​∑y∼x​(dy​−λ1​vy​)≤c3​n​.
  5. Lemma 18: a vertex u≠xu \ne xu=x with vu>1−2ε\mathbf v_u > 1 - 2\varepsilonvu​>1−2ε, du−λ1vu=O(n)d_u - \lambda_1\mathbf v_u = O(\sqrt n)du​−λ1​vu​=O(n​) and du≥(1/2−2ε)nd_u \ge (1/2 - 2\varepsilon)ndu​≥(1/2−2ε)n.
  6. Inequality (11): n/2+n+5≥vtv>n/2−2εn−O(n)n/2 + \sqrt n + 5 \ge \mathbf v^t\mathbf v > n/2 - 2\varepsilon n - O(\sqrt n)n/2+n​+5≥vtv>n/2−2εn−O(n​).
  7. Lemma 19 (corrected): vavb>1/2+n−1/2+5n−1\mathbf v_a\mathbf v_b > 1/2 + n^{-1/2} + 5n^{-1}va​vb​>1/2+n−1/2+5n−1 forces a∼ba \sim ba∼b; vavb<1/2−3ε\mathbf v_a\mathbf v_b < 1/2 - 3\varepsilonva​vb​<1/2−3ε forbids a∼ba \sim ba∼b when G−abG - abG−ab is connected.
  8. Every vertex other than a lone vertex of entry 111 is adjacent to a vertex of entry 111 (p. 18, corrected).
  9. Proposition 20: a partition U,V,WU, V, WU,V,W with UUU a clique of size about n/2n/2n/2 and entries near 111, VVV pendant vertices of entry below (2+ε)/n(2+\varepsilon)/n(2+ε)/n, and WWW vertices of entry near 1/21/21/2 adjacent only to UUU.
  10. W=∅W = \emptysetW=∅: GGG is a clique together with pendant vertices (pp. 20–21).

Significance

The result. Theorem 21 identifies the most spectrally irregular connected graphs for large nnn, confirming a conjecture that came from computer search and that had resisted the usual graph-transformation arguments. Combined with the cited optimization over pineapples, it gives the exact maximum of λ1−d\lambda_1 - dλ1​−d over connected nnn-vertex graphs for large nnn, which in turn bounds λ1\lambda_1λ1​ by ddd plus an explicit term for every connected graph. The intermediate statements, notably Lemma 19 which converts products of Perron entries into adjacency, are reusable in other spectral extremal problems over connected graphs.

Formalizing it. The theorem is proved on paper for large nnn; no machine-checked proof of it, or of Hong's inequality, is known. The formalization must make every "for nnn sufficiently large" and every O(n)O(\sqrt n)O(n​) explicit, and it repairs two statements that are false as printed (see Formalization scope). A small-nnn verification, or a proof for all nnn, would be further contributions.

Difficulty

The obvious approach is local improvement: given a non-pineapple, move an edge and show that λ1−d\lambda_1 - dλ1​−d increases. Each move changes both terms, by amounts of order vavb/vtv\mathbf v_a\mathbf v_b/\mathbf v^t\mathbf vva​vb​/vtv and 2/n2/n2/n respectively, and these are comparable; neither the sign of the change nor connectivity of the modified graph is under control without first knowing the global structure. The proof therefore needs the whole chain of asymptotic estimates: the size of λ1\lambda_1λ1​ and ddd, a second vertex of nearly maximal entry, the norm of the Perron vector, and only then the adjacency rules of Lemma 19. Every edge deletion must also keep the graph connected, since the maximum ranges over connected graphs.

Formalization scope

  • Vertices are Fin n; graphs are SimpleGraph (Fin n) with classical decidability. λ1\lambda_1λ1​ is the published WangKangXue.SpectralTuran.specRad, the largest eigenvalue of G.adjMatrix ℝ. ddd is avgDeg G = 2 · #edges / n in R\mathbb RR.
  • The maximum is over connected graphs on the same vertex set (IsIrregMax); dropping connectivity changes the problem.
  • The Perron vector enters as universally quantified hypotheses: any v with (G.adjMatrix ℝ).mulVec v = specRad G • v, all entries positive, all entries at most 111, and a vertex x with v x = 1. It is never quantified existentially.
  • "For nnn sufficiently large" is ∃ N, ∀ n ≥ N. Constants from O(n)O(\sqrt n)O(n​) and "a constant c3c_3c3​ not depending on nnn" are existentially quantified before NNN, nnn and GGG. In Lemma 18, inequality (11) and Lemma 19 the proof works for every ε>0\varepsilon > 0ε>0, which is universally quantified; Proposition 20 needs ε\varepsilonε small and is stated for 0<ε<ε00 < \varepsilon < \varepsilon_00<ε<ε0​.
  • ⌈n/2⌉\lceil n/2\rceil⌈n/2⌉ and ⌊n/2⌋\lfloor n/2\rfloor⌊n/2⌋ are the natural-number quotients (n+1)/2(n+1)/2(n+1)/2 and n/2n/2n/2; the pineapple lower bound assumes n≥2n \ge 2n≥2.
  • "GGG is a pineapple" is a graph isomorphism G ≃g pineapple p q with p+q=np + q = np+q=n. The pineapple is defined by its edges, clique plus pendants at one vertex; it is not defined by any property that the proof establishes, and the clique size is not pinned.
  • Two printed statements are corrected and the corrections are disclosed. Lemma 19's second half requires G−abG - abG−ab to be connected (without it, a pendant edge of the extremal pineapple is a counterexample), and both halves are for distinct vertices. The claim on p. 18 that every vertex has a neighbour of entry 111 excludes only a vertex that is the unique vertex of entry 111 (the hub of a pineapple is the exception). Lemma 17's summand is (dy−λ1vy)(d_y - \lambda_1\mathbf v_y)(dy​−λ1​vy​), as in its proof.
  • A trivializing formalization is ruled out: the class is connected graphs, extremality is the hypothesis rather than a consequence, the eigenvector is universally quantified, constants do not depend on nnn, and the clique size is free. A maximizer exists for every n≥1n \ge 1n≥1, so the goal is not vacuous.
  • Needed infrastructure: Perron–Frobenius for connected graphs, the Rayleigh-quotient characterization of λ1\lambda_1λ1​, Cauchy interlacing (or monotonicity of λ1\lambda_1λ1​ under subgraphs), and Hong's inequality. These are reusable well beyond this mission, and contributions of any of them are welcome.

Selected references

  • M. Tait and J. Tobin, Three conjectures in extremal spectral graph theory, J. Combin. Theory Ser. B (2017); arXiv:1606.01916v2. https://arxiv.org/abs/1606.01916
  • M. Aouchiche, F. K. Bell, D. Cvetković, P. Hansen, P. Rowlinson, S. K. Simić and D. Stevanović, Variable neighborhood search for extremal graphs. 16. Some conjectures related to the largest eigenvalue of a graph, European J. Oper. Res. 191(3) (2008) 661–676. (Reference [3] of Tait–Tobin.)
  • Y. Hong, A bound on the spectral radius of graphs, Linear Algebra Appl. 108 (1988) 135–139. (Reference [37].)
  • F. K. Bell, A note on the irregularity of graphs, Linear Algebra Appl. 161 (1992) 45–54. (Reference [5].)
  • M. O. Albertson, The irregularity of a graph, Ars Combin. 46 (1997) 219–225. (Reference [1].)
  • V. Nikiforov, Eigenvalues and degree deviation in graphs, Linear Algebra Appl. 414(1) (2006) 347–360. (Reference [26].)
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Optimal TransportProbabilityStatistics·Captain: mikedeng1

Finite-Sample Guarantees for Wasserstein Distributionally Robust Optimization: Breaking the Curse of Dimensionality 1: Under T_p(τ), True Loss ≤ Empirical Loss + R(√(τt/n); −f) w.p. ≥ 1 − e^(−t)Research Paper

Motivation

Wasserstein distributionally robust optimization (Wasserstein DRO) replaces the expected loss under an empirical distribution by the worst-case expected loss over all distributions within a Wasserstein distance ρ\rhoρ of it. It is used in operations research, statistics and machine learning to guard decisions and predictors against the gap between the sample and the population. The statistical question it raises is how large ρ\rhoρ must be for the robust loss to bound the true loss with high probability. Classical answers go through the concentration of the empirical measure in Wasserstein distance, which forces ρ≍n−1/d\rho\asymp n^{-1/d}ρ≍n−1/d in dimension ddd: the curse of dimensionality.

Gao (arXiv:2009.04382; Operations Research, 2023) shows that a radius of order n−1/2n^{-1/2}n−1/2 suffices, independently of the dimension. The first ingredient, and the subject of this mission, is a new concentration inequality for the empirical mean of a single loss function, whose rate is governed by the Wasserstein regularizer itself.

Setting

Let Z\mathcal ZZ be a separable Banach space with norm ∥⋅∥\|\cdot\|∥⋅∥ and let p∈[1,2]p\in[1,2]p∈[1,2]. Pp(Z)\mathcal P_p(\mathcal Z)Pp​(Z) is the set of Borel probability measures with E[∥z∥p]<∞\mathbb E[\|z\|^p]<\inftyE[∥z∥p]<∞, and the Wasserstein distance of order ppp is

Wp(P,Q)p=inf⁡π E(z~,z)∼π[∥z~−z∥p],\mathcal W_p(\mathbb P,\mathbb Q)^p=\inf_\pi\ \mathbb E_{(\tilde z,z)\sim\pi}\big[\|\tilde z-z\|^p\big],Wp​(P,Q)p=πinf​ E(z~,z)∼π​[∥z~−z∥p],

the infimum over couplings π\piπ of P\mathbb PP and Q\mathbb QQ. For a loss f:Z→Rf:\mathcal Z\to\mathbb Rf:Z→R, a nominal distribution Q\mathbb QQ and a radius ρ≥0\rho\ge0ρ≥0, the Wasserstein regularizer is the excess of the robust loss over the nominal loss,

RQ,p(ρ;f)=sup⁡P∈Pp(Z){EP[f]:Wp(P,Q)≤ρ}−EQ[f].\mathcal R_{\mathbb Q,p}(\rho;f)=\sup_{\mathbb P\in\mathcal P_p(\mathcal Z)}\big\{\mathbb E_{\mathbb P}[f]:\mathcal W_p(\mathbb P,\mathbb Q)\le\rho\big\}-\mathbb E_{\mathbb Q}[f].RQ,p​(ρ;f)=P∈Pp​(Z)sup​{EP​[f]:Wp​(P,Q)≤ρ}−EQ​[f].

The data are nnn i.i.d. samples z1,…,znz_1,\dots,z_nz1​,…,zn​ from an unknown Ptrue\mathbb P_{\rm true}Ptrue​; P⊗\mathbb P_\otimesP⊗​ is their joint law and EPn[f]=1n∑if(zi)\mathbb E_{\mathbb P_n}[f]=\frac1n\sum_i f(z_i)EPn​​[f]=n1​∑i​f(zi​) is the empirical loss. A distribution P\mathbb PP satisfies the transportation-information inequality Tp(τ)T_p(\tau)Tp​(τ) if

Wp(Q,P)≤τ H(Q∥P)∀ Q∈Pp(Z),\mathcal W_p(\mathbb Q,\mathbb P)\le\sqrt{\tau\,H(\mathbb Q\|\mathbb P)}\qquad\forall\,\mathbb Q\in\mathcal P_p(\mathcal Z),Wp​(Q,P)≤τH(Q∥P)​∀Q∈Pp​(Z),

with HHH the relative entropy. T1T_1T1​ holds for every distribution with a Gaussian moment E[ea∥z∥2]<∞\mathbb E[e^{a\|z\|^2}]<\inftyE[ea∥z∥2]<∞, and T2T_2T2​ (Talagrand's inequality) is implied by a log-Sobolev inequality.

The rate function is built from

Φg(t)=Ez∼Ptrue[sup⁡z~∈Z{t(g(z~)−g(z))−∥z~−z∥p}],Ip(ε;g)p=sup⁡t>0{εt−Φg(t)}.\Phi_g(t)=\mathbb E_{z\sim\mathbb P_{\rm true}}\Big[\sup_{\tilde z\in\mathcal Z}\big\{t(g(\tilde z)-g(z))-\|\tilde z-z\|^p\big\}\Big],\qquad \mathcal I_p(\varepsilon;g)^p=\sup_{t>0}\{\varepsilon t-\Phi_g(t)\}.Φg​(t)=Ez∼Ptrue​​[z~∈Zsup​{t(g(z~)−g(z))−∥z~−z∥p}],Ip​(ε;g)p=t>0sup​{εt−Φg​(t)}.

Formalization targets

Goal: Theorem 1 (variation-based concentration, p. 7)

If f≤M+L∥z∥pf\le M+L\|z\|^pf≤M+L∥z∥p with M,L>0M,L>0M,L>0 and Ptrue\mathbb P_{\rm true}Ptrue​ satisfies Tp(τ)T_p(\tau)Tp​(τ), then for every ε>0\varepsilon>0ε>0

P⊗{EPn[f]−EPtrue[f]<−ε}≤exp⁡(−n Ip(ε;−f)2/τ),\mathbb P_\otimes\big\{\mathbb E_{\mathbb P_n}[f]-\mathbb E_{\mathbb P_{\rm true}}[f]<-\varepsilon\big\}\le\exp\big(-n\,\mathcal I_p(\varepsilon;-f)^2/\tau\big),P⊗​{EPn​​[f]−EPtrue​​[f]<−ε}≤exp(−nIp​(ε;−f)2/τ),

and for every t>0t>0t>0, with probability at least 1−e−t1-e^{-t}1−e−t,

EPtrue[f]≤EPn[f]+RPtrue,p(τtn;−f).\mathbb E_{\mathbb P_{\rm true}}[f]\le\mathbb E_{\mathbb P_n}[f]+\mathcal R_{\mathbb P_{\rm true},p}\Big(\sqrt{\tfrac{\tau t}{n}};-f\Big).EPtrue​​[f]≤EPn​​[f]+RPtrue​,p​(nτt​​;−f).

Milestones

  1. Lemma 4 (p. 21): if P\mathbb PP satisfies Tp(τ)T_p(\tau)Tp​(τ), the product P⊗n\mathbb P^{\otimes n}P⊗n satisfies Tp(τn2/p−1)T_p(\tau n^{2/p-1})Tp​(τn2/p−1) for the ℓp\ell_pℓp​ product distance dp(z,z~)p=∑i∥zi−z~i∥p\mathsf d_p(z,\tilde z)^p=\sum_i\|z_i-\tilde z_i\|^pdp​(z,z~)p=∑i​∥zi​−z~i​∥p.
  2. Identity (5) (p. 21): the relative entropy of an exponential tilt, H(ν(g)∥ν)=Eν(g)[g]−ln⁡Eν[eg]H(\nu^{(g)}\|\nu)=\mathbb E_{\nu^{(g)}}[g]-\ln\mathbb E_\nu[e^g]H(ν(g)∥ν)=Eν(g)​[g]−lnEν​[eg]. Already proved on the platform and referenced.
  3. Proposition 1 (p. 6): Ip(⋅;f)\mathcal I_p(\cdot;f)Ip​(⋅;f) inverts the regularizer, Ip(RPtrue,p(ρ;f);f)=ρ\mathcal I_p(\mathcal R_{\mathbb P_{\rm true},p}(\rho;f);f)=\rhoIp​(RPtrue​,p​(ρ;f);f)=ρ when the dual minimizer λo\lambda_oλo​ of the strong-duality problem (1) exceeds the growth rate λ‾\underline\lambdaλ​ of fff, and ≥ρ\ge\rho≥ρ when they coincide.
  4. Lemma 5 (p. 21): the same two bounds for a general F:Zn→RF:\mathcal Z^n\to\mathbb RF:Zn→R with E⊗[F]=0\mathbb E_\otimes[F]=0E⊗​[F]=0 and ppp-growth, with rate J(ε;F)\mathcal J(\varepsilon;F)J(ε;F) and bound R(τt/n;F)\mathcal R(\sqrt{\tau t/n};F)R(τt/n​;F).
  5. Corollary 1 (p. 7), two items: for p=1p=1p=1 under a uniform Lipschitz bound, EPtrue[f]≤EPn[f]+τt/n ∥f∥Lip\mathbb E_{\mathbb P_{\rm true}}[f]\le\mathbb E_{\mathbb P_n}[f]+\sqrt{\tau t/n}\,\|f\|_{\rm Lip}EPtrue​​[f]≤EPn​​[f]+τt/n​∥f∥Lip​; for p=2p=2p=2 under a Lipschitz gradient, the bound τt/n ∥∥∇f∥∗∥Ptrue,2+ℏτt/n\sqrt{\tau t/n}\,\|\|\nabla f\|_*\|_{\mathbb P_{\rm true},2}+\hbar\tau t/nτt/n​∥∥∇f∥∗​∥Ptrue​,2​+ℏτt/n.

Significance

Theorem 1 says that the large-deviation rate of the empirical loss is the inverse of the Wasserstein regularizer, and that the regularizer at radius τt/n\sqrt{\tau t/n}τt/n​ is a valid high-probability correction of the empirical loss. Neither involves the dimension of Z\mathcal ZZ or the complexity of a covering of it. The paper builds its covering-number and local-Rademacher guarantees for Wasserstein DRO (Sections 4.1–4.2, the subject of two companion missions) on this single-function result, and Corollary 1 recovers, for p=1p=1p=1, the Lipschitz-norm bound known from transportation inequalities while sharpening it for p=2p=2p=2.

The results are proved in the paper; none is formalized. A complete development would give a machine-checked tensorization of transportation-information inequalities on Banach spaces and a Marton–Herbst-type concentration argument, both of which are used well beyond DRO.

Difficulty

The proof combines three ingredients that Mathlib does not yet connect. Tensorization (Lemma 4) needs disintegration of a measure on Zn\mathcal Z^nZn and the chain rule for relative entropy, together with a gluing of couplings and Hölder's inequality for the dimension constant. Lemma 5 combines TpT_pTp​ with Kantorovich duality for the cost 1ndpp\frac1n\mathsf d_p^pn1​dpp​ and the entropy of an exponential tilt, then optimizes a Young-inequality split over two parameters for p<2p<2p<2, and extends from bounded FFF to ppp-growth by monotone truncation. Proposition 1 rests on the strong duality (1) of Gao and Kleywegt, an external result, and on the first-order optimality condition of a convex perspective function. A naive approach that bounds the deviation by Wp(Pn,Ptrue)\mathcal W_p(\mathbb P_n,\mathbb P_{\rm true})Wp​(Pn​,Ptrue​) fails: that distance decays like n−1/dn^{-1/d}n−1/d, which is exactly the curse the theorem avoids.

Formalization scope

The source is arXiv:2009.04382; its printed page numbers equal the PDF's. The Lean development lives in the namespace WassFSG.Conc and uses these conventions:

  • Z\mathcal ZZ is a real Banach space with its Borel σ\sigmaσ-algebra and is second countable (separable), as the cited duality results require; Wpp\mathcal W_p^pWpp​ is the published optimal transport cost with cost ∥u−w∥p\|u-w\|^p∥u−w∥p, and HHH is Mathlib's klDiv.
  • Expectations of a loss inside the robust supremum are extended integrals ∫f+−∫f−\int f^+-\int f^-∫f+−∫f− in [−∞,∞][-\infty,\infty][−∞,∞]; the regularizer is valued in [−∞,∞][-\infty,\infty][−∞,∞].
  • Ipp\mathcal I_p^pIpp​ and Jp\mathcal J^pJp are read as max⁡(0,sup⁡t>0{⋯ })∈[0,∞]\max(0,\sup_{t>0}\{\cdots\})\in[0,\infty]max(0,supt>0​{⋯})∈[0,∞], since the paper's declared codomain R+∪{+∞}\mathbb R_+\cup\{+\infty\}R+​∪{+∞} fails without it; an infinite rate gives the bound 000, never 111.
  • Lemma 5's printed "min" is an infimum, and Proposition 1's printed limit λ‾\underline\lambdaλ​ is a lim sup⁡\limsuplimsup.
  • The product space carries the ℓp\ell_pℓp​-sum cost, not the sup metric.
  • "With probability at least 1−δ1-\delta1−δ" bounds the outer measure of the bad set by δ\deltaδ; the sample size satisfies n≥1n\ge1n≥1.
  • Added hypotheses: measurability and Ptrue\mathbb P_{\rm true}Ptrue​-integrability of fff in Theorem 1 and Proposition 1, measurability of FFF in Lemma 5, and a nontrivial Z\mathcal ZZ and Ptrue∈Pp(Z)\mathbb P_{\rm true}\in\mathcal P_p(\mathcal Z)Ptrue​∈Pp​(Z) (presupposed by the dual problem (1)) in Proposition 1.
  • Theorem 1's growth hypothesis is kept as printed, an upper bound on fff. When −f-f−f has no ppp-growth bound, both conclusions hold trivially (the rate is 000 and the regularizer is +∞+\infty+∞).

A formalization that reads an infinite Ip\mathcal I_pIp​ through a real coercion would turn the tail bound into the trivial bound 111; the conventions above rule this out. Likewise a regularizer whose supremum ranged only over measures supported on the sample, or a TpT_pTp​ condition over a restricted class of Q\mathbb QQ, would be a different statement.

Contributions welcome: Lemma 4 and Corollary 1 are independent entry points; a proof of the duality (1) under the paper's growth condition would be reusable by every Wasserstein DRO mission.

Selected references

  • R. Gao, Finite-Sample Guarantees for Wasserstein Distributionally Robust Optimization: Breaking the Curse of Dimensionality, Operations Research, 2023; preprint arXiv:2009.04382.
  • R. Gao and A. Kleywegt, Distributionally Robust Stochastic Optimization with Wasserstein Distance, Mathematics of Operations Research, 2023; arXiv:1604.02199.
  • C. Villani, Optimal Transport: Old and New, Springer, 2009; doi:10.1007/978-3-540-71050-9.
  • N. Gozlan and C. Léonard, Transport Inequalities. A Survey, Markov Processes and Related Fields, 2010; arXiv:1003.3852.
  • F. Bolley and C. Villani, Weighted Csiszár–Kullback–Pinsker inequalities and applications to transportation inequalities, Annales de la Faculté des Sciences de Toulouse, 2005; doi:10.5802/afst.1095.
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Control TheoryOptimizationProbability+1·Captain: mikedeng1

Open-Loop and Closed-Loop Solvabilities for Stochastic Linear Quadratic Optimal Control Problems 4: A Problem Open-Loop Solvable at Every (t, x) but Closed-Loop Solvable on No [t, 1]Research Paper

Why open-loop and closed-loop solvability must be told apart

In a stochastic linear–quadratic (LQ) optimal control problem a controller steers a linear stochastic differential equation and pays a quadratic cost. When the cost weights are allowed to be indefinite — as in mean–variance portfolio selection, where the control weight is zero — the problem can still be well posed, and two different notions of solution appear. An open-loop optimal control is a process chosen for one given initial pair (t,x)(t,x)(t,x). A closed-loop optimal strategy is a feedback law u=ΘX+vu=\Theta X+vu=ΘX+v that is optimal for every initial state at once. A closed-loop optimal strategy yields an open-loop optimal control for each initial state; the converse is the question.

Timeline. Chen, Li and Zhou (1998, doi:10.1137/S0363012996310478) started the theory of indefinite stochastic LQ control. Ait Rami, Moore and Zhou (2002, doi:10.1137/S0363012900371083) introduced the generalized Riccati equation with a Moore–Penrose pseudoinverse and stated that, for Problem (SLQ)0^00 with continuous coefficients and S=0S=0S=0, a continuous open-loop optimal control exists at every initial pair if and only if the Riccati equation has a solution satisfying a range condition and a sign condition. Sun and Yong (2014, doi:10.1137/140953642) characterized closed-loop solvability by regular solutions of that Riccati equation. Sun, Li and Yong (2016, doi:10.1137/15M103532X) showed by two explicit examples that the 2002 equivalence fails in both directions, and that open-loop solvability is strictly weaker than closed-loop solvability. This mission formalizes those examples.

Setting

Let WWW be a standard one-dimensional Brownian motion on a probability space (Ω,F,P)(\Omega,\mathcal F,\mathbb P)(Ω,F,P) and F\mathbb FF its augmented natural filtration. For (t,x)∈[0,T)×Rn(t,x)\in[0,T)\times\mathbb R^n(t,x)∈[0,T)×Rn and a control uuu in the space U[t,T]\mathcal U[t,T]U[t,T] of F\mathbb FF-progressively measurable Rm\mathbb R^mRm-valued processes with E∫tT∣u∣2ds<∞\mathbb E\int_t^T|u|^2ds<\inftyE∫tT​∣u∣2ds<∞, the state equation is

dX=(AX+Bu+b) ds+(CX+Du+σ) dW,X(t)=x,dX=(AX+Bu+b)\,ds+(CX+Du+\sigma)\,dW,\qquad X(t)=x,dX=(AX+Bu+b)ds+(CX+Du+σ)dW,X(t)=x,

and the cost J(t,x;u)J(t,x;u)J(t,x;u) is the expectation of ⟨GX(T),X(T)⟩+2⟨g,X(T)⟩\langle GX(T),X(T)\rangle+2\langle g,X(T)\rangle⟨GX(T),X(T)⟩+2⟨g,X(T)⟩ plus the time integral of a quadratic form in (X,u)(X,u)(X,u) with weights Q,S,RQ,S,RQ,S,R and linear terms q,ρq,\rhoq,ρ. Problem (SLQ)0^00 is the case b=σ=g=q=ρ=0b=\sigma=g=q=\rho=0b=σ=g=q=ρ=0, with cost J0J^0J0 and value function V0(t,x)=inf⁡u∈U[t,T]J0(t,x;u)V^0(t,x)=\inf_{u\in\mathcal U[t,T]}J^0(t,x;u)V0(t,x)=infu∈U[t,T]​J0(t,x;u).

The Riccati equation (4.6) is

P˙+PA+A⊤P+C⊤PC+Q−(PB+C⊤PD+S⊤)(R+D⊤PD)†(B⊤P+D⊤PC+S)=0,P(T)=G,\dot P+PA+A^\top P+C^\top PC+Q-(PB+C^\top PD+S^\top)(R+D^\top PD)^\dagger(B^\top P+D^\top PC+S)=0,\qquad P(T)=G,P˙+PA+A⊤P+C⊤PC+Q−(PB+C⊤PD+S⊤)(R+D⊤PD)†(B⊤P+D⊤PC+S)=0,P(T)=G,

where M†M^\daggerM† is the Moore–Penrose pseudoinverse. A solution is regular if (4.7) R(B⊤P+D⊤PC+S)⊆R(R+D⊤PD)\mathcal R(B^\top P+D^\top PC+S)\subseteq\mathcal R(R+D^\top PD)R(B⊤P+D⊤PC+S)⊆R(R+D⊤PD) a.e., (4.8) (R+D⊤PD)†(B⊤P+D⊤PC+S)∈L2(R+D^\top PD)^\dagger(B^\top P+D^\top PC+S)\in L^2(R+D⊤PD)†(B⊤P+D⊤PC+S)∈L2, and (4.9) R+D⊤PD≥0R+D^\top PD\ge 0R+D⊤PD≥0 a.e.

Example 7.1 is Problem (SLQ)0^00 with n=1n=1n=1, m=2m=2m=2, T=1T=1T=1:

dX=[u1+u2] ds+[u1−u2] dW,J0(t,x;u)=E X(1)2,dX=[u_1+u_2]\,ds+[u_1-u_2]\,dW,\qquad J^0(t,x;u)=\mathbb E\,X(1)^2,dX=[u1​+u2​]ds+[u1​−u2​]dW,J0(t,x;u)=EX(1)2,

that is, A=C=Q=0A=C=Q=0A=C=Q=0, B=(1,1)B=(1,1)B=(1,1), D=(1,−1)D=(1,-1)D=(1,−1), G=1G=1G=1, S=0S=0S=0, R=0R=0R=0.

Formalization targets

Goal: Example 7.1

For every (t,x)∈[0,1)×R(t,x)\in[0,1)\times\mathbb R(t,x)∈[0,1)×R,

u(t,x)∗(s)=−(x2−2t,x2−2t)⊤ is open-loop optimal,V0(t,x)=0,u^*_{(t,x)}(s)=-\Big(\frac{x}{2-2t},\frac{x}{2-2t}\Big)^\top\ \text{is open-loop optimal},\qquad V^0(t,x)=0,u(t,x)∗​(s)=−(2−2tx​,2−2tx​)⊤ is open-loop optimal,V0(t,x)=0,

while V0(1,x)=x2V^0(1,x)=x^2V0(1,x)=x2, and for every t∈[0,1)t\in[0,1)t∈[0,1) the problem is not closed-loop solvable on [t,1][t,1][t,1].

Milestones

  1. (7.3): the Riccati equation has the unique solution P≡1P\equiv1P≡1, and it violates (4.7).
  2. Theorem 4.3 for (SLQ)0^00: closed-loop solvability on [t,T][t,T][t,T] is equivalent to the existence of a regular solution on [t,T][t,T][t,T].
  3. (7.5)–(7.6): with RRR replaced by R+εIR+\varepsilon IR+εI the Riccati equation has the strongly regular solution Pε(t)=ε/(ε+2−2t)P_\varepsilon(t)=\varepsilon/(\varepsilon+2-2t)Pε​(t)=ε/(ε+2−2t).
  4. (7.7): Pε(t)→0P_\varepsilon(t)\to 0Pε​(t)→0 for t<1t<1t<1 and Pε(1)=1P_\varepsilon(1)=1Pε​(1)=1.
  5. (7.9)–(7.10): the closed-loop state and control of the regularized problem, uε=−(xε+2−2t,xε+2−2t)⊤u_\varepsilon=-\big(\frac{x}{\varepsilon+2-2t},\frac{x}{\varepsilon+2-2t}\big)^\topuε​=−(ε+2−2tx​,ε+2−2tx​)⊤.
  6. uε→u(t,x)∗u_\varepsilon\to u^*_{(t,x)}uε​→u(t,x)∗​ in L2L^2L2 as ε→0\varepsilon\to0ε→0.

Companion: Example 7.2

For dX=u dsdX=u\,dsdX=uds and J=X(1)2+∫t1s2u2dsJ=X(1)^2+\int_t^1s^2u^2dsJ=X(1)2+∫t1​s2u2ds, the Riccati equation (7.12) has the unique solution P(t)=tP(t)=tP(t)=t, which satisfies (4.7) and (4.9), yet no open-loop optimal control exists at (0,x)(0,x)(0,x), x≠0x\neq0x=0.

Significance

The result. Example 7.1 refutes the necessity half of the Ait Rami–Moore–Zhou criterion: a continuous open-loop optimal control exists at every initial pair, but the Riccati equation has no regular solution. Example 7.2 refutes the sufficiency half. Together they show that the Riccati equation with conditions (4.7) and (4.9) characterizes neither notion, and that open-loop solvability is strictly weaker than closed-loop solvability; Example 7.1 also exhibits a finite value function that is discontinuous in time. These facts are why the paper develops separate characterizations of open-loop solvability (through the regularized Riccati solutions PεP_\varepsilonPε​) instead of the Riccati equation itself.

Formalizing it. The examples are proved in the paper by appeal to its Theorems 5.3 and 6.2 and to Theorem 4.3 from Sun–Yong (2014). Nothing in this chain is machine-checked anywhere. A formal proof of the goal must verify the explicit optimal control against the canonical stochastic state equation, compute the value function, and rule out every closed-loop strategy; it can use Theorem 4.3 (posed here as a milestone) or a direct argument. The definitions built here (the stochastic LQ problem, the pseudoinverse Riccati equation, regularity) are shared with the other missions of this series.

Difficulty

Open-loop optimality looks immediate because J0=EX(1)2≥0J^0=\mathbb EX(1)^2\ge0J0=EX(1)2≥0, but it requires showing that the state driven by u∗u^*u∗ hits 000 at time 111, which means identifying the solution of the stochastic state equation for this control. The value at t=1t=1t=1 requires the degenerate interval [1,1][1,1][1,1] to be handled inside the same SDE framework. The hard part is the negative claim: it quantifies over all feedback pairs (Θ,v)(\Theta,v)(Θ,v) with Θ∈L2\Theta\in L^2Θ∈L2, and must show that no such pair drives every initial state to 000 at time 111. The paper reduces this to Theorem 4.3, whose proof (in Sun–Yong 2014) is a substantial piece of stochastic LQ theory; checking that P≡1P\equiv 1P≡1 fails the range condition is the easy end of that chain.

Formalization scope

Time is R≥0\mathbb R_{\ge0}R≥0​, vectors are Fin k → ℝ, inner products are dot products, and ∣u∣2=u⋅u|u|^2=u\cdot u∣u∣2=u⋅u. The Brownian motion is the published Peng1990.SMP.IsStdBrownian, the filtration the published augmented filtration, the SDE solution concept the published Peng1990.SMP.SolvesSDE, and the pseudoinverse the published HarmonicGames.Decomposition.pinv.

  • The state from (t,x)(t,x)(t,x) is an SDE from time 000 with coefficients switched on at ttt, with a.s. continuous paths and Esup⁡∣X∣2<∞\mathbb E\sup|X|^2<\inftyEsup∣X∣2<∞; the cost uses a chosen solution, unique by [23, Proposition 2.1].
  • Value functions are infima in the extended reals over admissible controls.
  • The Riccati equation is in integral form on [t0,T][t_0,T][t0​,T]; regularity is (4.7)–(4.9) on [t0,T][t_0,T][t0​,T].
  • A closed-loop optimal strategy on [t,T][t,T][t,T] requires Θ∈L2(t,T)\Theta\in L^2(t,T)Θ∈L2(t,T), v∈U[t,T]v\in\mathcal U[t,T]v∈U[t,T], and, for every initial state, a solution of the closed-loop system that is no worse than any admissible control.
  • Theorem 4.3 is stated on [t,T][t,T][t,T] (the paper states it on [0,T][0,T][0,T] and applies it on [t,1][t,1][t,1]).
  • The goal places no hypotheses on the probability space beyond the Brownian motion.

Proving only that P≡1P\equiv1P≡1 violates (4.7) does not settle the goal: the goal is about solvability of the control problem itself, and "not closed-loop solvable on any [t,1][t,1][t,1]" is stated for every t<1t<1t<1, not as the failure on some interval.

Contributions are welcome on any milestone, on the well-posedness of linear SDEs in this framework, and on the pseudoinverse identities (Penrose equations, the pseudoinverse of a scaled symmetric matrix) that the Riccati computations need.

Selected references

  • J. Sun, X. Li, J. Yong, Open-loop and closed-loop solvabilities for stochastic linear quadratic optimal control problems, SIAM J. Control Optim. 54(5) (2016) 2274–2308. doi:10.1137/15M103532X
  • M. Ait Rami, J. B. Moore, X. Y. Zhou, Indefinite stochastic linear quadratic control and generalized differential Riccati equation, SIAM J. Control Optim. 40 (2002) 1296–1311. doi:10.1137/S0363012900371083
  • J. Sun, J. Yong, Linear quadratic stochastic differential games: open-loop and closed-loop saddle points, SIAM J. Control Optim. 52 (2014) 4082–4121. doi:10.1137/140953642
  • S. Chen, X. Li, X. Y. Zhou, Stochastic linear quadratic regulators with indefinite control weight costs, SIAM J. Control Optim. 36 (1998) 1685–1702. doi:10.1137/S0363012996310478
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Open-Loop and Closed-Loop Solvabilities for Stochastic Linear Quadratic Optimal Control Problems 3: Open-Loop Solvability Is Equivalent to Convergence of the Riccati Minimizing SequenceResearch Paper

Motivation

Linear–quadratic (LQ) optimal control is the basic test case of stochastic control: a linear stochastic differential equation, a quadratic cost, and an optimal control that one expects to be a linear feedback of the state computed from a Riccati equation. In the indefinite stochastic case the weighting matrices GGG, QQQ, RRR carry no sign condition. The cost can then be convex without being uniformly convex, an optimal control may fail to exist although the value is finite, and the Riccati equation may have no solution of the kind the classical theory needs.

Sun, Li and Yong (SIAM J. Control Optim. 54 (2016) 2274–2308) separate finiteness, convexity, open-loop solvability and closed-loop solvability for this problem. This mission covers their Section 6. Under uniform convexity the optimal control is the Riccati feedback of Corollary 4.7. Section 6 removes uniform convexity: it regularizes the control weight RRR to R+εIR+\varepsilon IR+εI, takes the Riccati feedback control uεu_\varepsilonuε​ of each regularized problem, and shows that open-loop solvability of the original problem is exactly the convergence of uεu_\varepsilonuε​ along some sequence εk→0\varepsilon_k\to0εk​→0.

Timeline. Chen, Li and Zhou (SIAM J. Control Optim. 36 (1998)) introduced indefinite stochastic LQ problems. Ait Rami, Moore and Zhou (SIAM J. Control Optim. 40 (2002)) introduced the generalized Riccati equation with a pseudoinverse. Sun and Yong (SIAM J. Control Optim. 52 (2014)) characterized closed-loop solvability by regular solutions of that equation. In 2016 Sun, Li and Yong characterized uniform convexity by strongly regular solutions and open-loop solvability by the regularized feedback sequence treated here.

Setting

Fix a horizon T>0T>0T>0 and a probability space carrying a one-dimensional standard Brownian motion WWW, with F\mathbb FF the augmented natural filtration of WWW. For an initial pair (t,x)∈[0,T)×Rn(t,x)\in[0,T)\times\mathbb R^n(t,x)∈[0,T)×Rn and an admissible control u∈U[t,T]u\in\mathcal U[t,T]u∈U[t,T], an F\mathbb FF-progressively measurable Rm\mathbb R^mRm-valued process with E∫tT∣u∣2ds<∞\mathbb E\int_t^T|u|^2ds<\inftyE∫tT​∣u∣2ds<∞, the state solves

dX=(AX+Bu+b) ds+(CX+Du+σ) dW,X(t)=x.dX=(AX+Bu+b)\,ds+(CX+Du+\sigma)\,dW,\qquad X(t)=x .dX=(AX+Bu+b)ds+(CX+Du+σ)dW,X(t)=x.

The cost is

J(t,x;u)=E[⟨GX(T),X(T)⟩+2⟨g,X(T)⟩+∫tT(⟨QX,X⟩+2⟨SX,u⟩+⟨Ru,u⟩+2⟨q,X⟩+2⟨ρ,u⟩)ds].J(t,x;u)=\mathbb E\Big[\langle GX(T),X(T)\rangle+2\langle g,X(T)\rangle+\int_t^T\big(\langle QX,X\rangle+2\langle SX,u\rangle+\langle Ru,u\rangle+2\langle q,X\rangle+2\langle\rho,u\rangle\big)ds\Big].J(t,x;u)=E[⟨GX(T),X(T)⟩+2⟨g,X(T)⟩+∫tT​(⟨QX,X⟩+2⟨SX,u⟩+⟨Ru,u⟩+2⟨q,X⟩+2⟨ρ,u⟩)ds].

The coefficients A,B,C,D,Q,S,RA,B,C,D,Q,S,RA,B,C,D,Q,S,R and GGG are deterministic, b,σ,q,ρ,gb,\sigma,q,\rho,gb,σ,q,ρ,g are random, and the integrability conditions are (H1)–(H2). The value function is V(t,x)=inf⁡uJ(t,x;u)∈[−∞,∞)V(t,x)=\inf_uJ(t,x;u)\in[-\infty,\infty)V(t,x)=infu​J(t,x;u)∈[−∞,∞). A control u∗u^*u∗ is open-loop optimal at (t,x)(t,x)(t,x) if J(t,x;u∗)≤J(t,x;u)J(t,x;u^*)\le J(t,x;u)J(t,x;u∗)≤J(t,x;u) for every u∈U[t,T]u\in\mathcal U[t,T]u∈U[t,T]. Problem (SLQ)0^00 is the case b,σ,g,q,ρ=0b,\sigma,g,q,\rho=0b,σ,g,q,ρ=0, with cost J0J^0J0.

For ε>0\varepsilon>0ε>0 let PεP_\varepsilonPε​ be the strongly regular solution of the Riccati equation (5.7),

P˙ε+PεA+A⊤Pε+C⊤PεC+Q−Kε⊤Σε−1Kε=0,Pε(T)=G,\dot P_\varepsilon+P_\varepsilon A+A^\top P_\varepsilon+C^\top P_\varepsilon C+Q-K_\varepsilon^\top\Sigma_\varepsilon^{-1}K_\varepsilon=0,\qquad P_\varepsilon(T)=G,P˙ε​+Pε​A+A⊤Pε​+C⊤Pε​C+Q−Kε⊤​Σε−1​Kε​=0,Pε​(T)=G,

where Σε=R+εI+D⊤PεD≥λI\Sigma_\varepsilon=R+\varepsilon I+D^\top P_\varepsilon D\ge\lambda IΣε​=R+εI+D⊤Pε​D≥λI for some λ>0\lambda>0λ>0 and Kε=B⊤Pε+D⊤PεC+SK_\varepsilon=B^\top P_\varepsilon+D^\top P_\varepsilon C+SKε​=B⊤Pε​+D⊤Pε​C+S. Let (ηε,ζε)(\eta_\varepsilon,\zeta_\varepsilon)(ηε​,ζε​) be the adapted solution of the linear backward equation (4.11) for these data, and put

Θε=−Σε−1Kε,vε=−Σε−1(B⊤ηε+D⊤ζε+D⊤Pεσ+ρ).\Theta_\varepsilon=-\Sigma_\varepsilon^{-1}K_\varepsilon,\qquad v_\varepsilon=-\Sigma_\varepsilon^{-1}\big(B^\top\eta_\varepsilon+D^\top\zeta_\varepsilon+D^\top P_\varepsilon\sigma+\rho\big).Θε​=−Σε−1​Kε​,vε​=−Σε−1​(B⊤ηε​+D⊤ζε​+D⊤Pε​σ+ρ).

With XεX_\varepsilonXε​ the solution of the closed-loop system dXε=[(A+BΘε)Xε+Bvε+b]ds+[(C+DΘε)Xε+Dvε+σ]dWdX_\varepsilon=[(A+B\Theta_\varepsilon)X_\varepsilon+Bv_\varepsilon+b]ds+[(C+D\Theta_\varepsilon)X_\varepsilon+Dv_\varepsilon+\sigma]dWdXε​=[(A+BΘε​)Xε​+Bvε​+b]ds+[(C+DΘε​)Xε​+Dvε​+σ]dW, Xε(t)=xX_\varepsilon(t)=xXε​(t)=x, the regularized feedback sequence is

uε=ΘεXε+vε,ε>0.u_\varepsilon=\Theta_\varepsilon X_\varepsilon+v_\varepsilon,\qquad\varepsilon>0 .uε​=Θε​Xε​+vε​,ε>0.

U[t,T]=LF2(t,T;Rm)\mathcal U[t,T]=L^2_{\mathbb F}(t,T;\mathbb R^m)U[t,T]=LF2​(t,T;Rm) is a Hilbert space with inner product E∫tT⟨u,v⟩ds\mathbb E\int_t^T\langle u,v\rangle dsE∫tT​⟨u,v⟩ds; weak and strong convergence of controls refer to it.

Formalization targets

Goal: Theorem 6.2

Assume (H1)–(H2) and that u↦J0(0,0;u)u\mapsto J^0(0,0;u)u↦J0(0,0;u) is convex. For (t,x)∈[0,T)×Rn(t,x)\in[0,T)\times\mathbb R^n(t,x)∈[0,T)×Rn the following are equivalent:

(SLQ) is open-loop solvable at (t,x)  ⟺  ∃ εk↓0: uεk⇀u∗  ⟺  ∃ εk↓0: uεk→u∗ in U[t,T],\text{(SLQ) is open-loop solvable at }(t,x)\iff\exists\,\varepsilon_k\downarrow0:\ u_{\varepsilon_k}\rightharpoonup u^*\iff\exists\,\varepsilon_k\downarrow0:\ u_{\varepsilon_k}\to u^*\text{ in }\mathcal U[t,T],(SLQ) is open-loop solvable at (t,x)⟺∃εk​↓0: uεk​​⇀u∗⟺∃εk​↓0: uεk​​→u∗ in U[t,T],

and every weak or strong limit of such a subsequence is an open-loop optimal control at (t,x)(t,x)(t,x). The goal assumes convexity, not uniform convexity, and no finiteness.

Milestones

  1. Corollary 3.4: convexity of J(t,x;⋅)J(t,x;\cdot)J(t,x;⋅) or J0(t,x;⋅)J^0(t,x;\cdot)J0(t,x;⋅) at one xxx, at every xxx, and J0(t,0;u)≥0J^0(t,0;u)\ge0J0(t,0;u)≥0 on U[t,T]\mathcal U[t,T]U[t,T] are equivalent.
  2. The zero extension (4.3): J0(t,0;u)=J0(0,0;0I[0,t)⊕u)J^0(t,0;u)=J^0(0,0;0I_{[0,t)}\oplus u)J0(t,0;u)=J0(0,0;0I[0,t)​⊕u).
  3. Corollary 4.7: under uniform convexity, the Riccati feedback control (4.28) is the unique open-loop optimal control.
  4. Theorem 6.1: if the problem is finite, lim⁡ε→0+J(t,x;uε)=V(t,x)\lim_{\varepsilon\to0^+}J(t,x;u_\varepsilon)=V(t,x)limε→0+​J(t,x;uε​)=V(t,x).
  5. Lemma 6.3: in a Hilbert space the norm is weakly lower semicontinuous, and strong convergence is weak convergence plus convergence of norms.
  6. (6.7): E∫tT∣uε∣2ds≤(Vε−V)/ε≤E∫tT∣v∗∣2ds\mathbb E\int_t^T|u_\varepsilon|^2ds\le(V_\varepsilon-V)/\varepsilon\le\mathbb E\int_t^T|v^*|^2dsE∫tT​∣uε​∣2ds≤(Vε​−V)/ε≤E∫tT​∣v∗∣2ds for any optimal v∗v^*v∗.
  7. Weak lower semicontinuity of u↦J(t,x;u)u\mapsto J(t,x;u)u↦J(t,x;u).

Two further statements follow the goal: open-loop solvability is equivalent to sup⁡ε>0E∫tT∣uε∣2ds<∞\sup_{\varepsilon>0}\mathbb E\int_t^T|u_\varepsilon|^2ds<\inftysupε>0​E∫tT​∣uε​∣2ds<∞ (p. 2303), and Proposition 6.4: if sup⁡ε>0∫0T∣Θε∣2ds<∞\sup_{\varepsilon>0}\int_0^T|\Theta_\varepsilon|^2ds<\inftysupε>0​∫0T​∣Θε​∣2ds<∞, the Riccati equation (4.6) has a regular solution and Problem (SLQ)0^00 is closed-loop solvable.

Significance

Theorem 6.1 gives a minimizing sequence computed from Riccati and backward equations whenever the problem is finite. Theorem 6.2 turns it into a test for open-loop solvability that needs no uniform convexity and no regular solution of the original Riccati equation. When an optimal control exists, it is recovered as the limit of feedback controls. Proposition 6.4 converts a bound on the gains Θε\Theta_\varepsilonΘε​ into closed-loop solvability of the homogeneous problem. Section 7 of the paper shows that open-loop solvability does not imply closed-loop solvability, so a criterion phrased directly in open-loop terms is needed.

All of these results are proved in the paper. None of them, nor the solution theory of stochastic LQ problems they rest on, had a machine-checked proof on Prove2Me or in Mathlib as of October 2026. A formal development needs the well-posedness of linear SDEs and BSDEs with integrable coefficients, the Riccati theory of Section 4, and the Hilbert-space structure of the space of admissible controls. Those parts are reusable for any stochastic LQ problem.

Difficulty

The obvious approach takes any minimizing sequence and extracts a weakly convergent subsequence. That fails without uniform convexity: a minimizing sequence need not be bounded, and boundedness is exactly what open-loop solvability provides in (6.7). The converse direction needs the limit of the regularized costs to identify the value, which requires both the minimizing property of uεu_\varepsilonuε​ (Theorem 6.1) and weak lower semicontinuity of JJJ. That in turn rests on convexity being transported from J0(0,0;⋅)J^0(0,0;\cdot)J0(0,0;⋅) to J(t,x;⋅)J(t,x;\cdot)J(t,x;⋅) through Corollary 3.4 and the zero extension. Upgrading weak to strong convergence uses the norm bound (6.7) with the limit itself as the optimal control. Every step depends on Corollary 4.7, the Riccati representation of the optimal control of the regularized problem, whose proof requires the theory of Section 4.

Formalization scope

The probability basis is a probability space with a one-dimensional standard Brownian motion and its augmented natural filtration. Vectors are Fin k → ℝ and matrices Matrix (Fin k) (Fin l) ℝ. Time is ℝ≥0, and ∣u∣2|u|^2∣u∣2 is the Euclidean dot product u ⬝ᵥ u. (H1)–(H2) are standing assumptions, with entrywise LpL^pLp conditions on the matrix coefficients. The state from (t,x)(t,x)(t,x) is a strong solution of the published SDE notion Peng1990.SMP.SolvesSDE whose coefficients are switched on at ttt; it has a.s. continuous paths and Esup⁡∣X∣2<∞\mathbb E\sup|X|^2<\inftyEsup∣X∣2<∞. The cost is evaluated along a chosen solution, which is unique. VVV is an infimum in the extended reals. Limits in ε\varepsilonε are taken as ε→0+\varepsilon\to0^+ε→0+. "A subsequence" is a sequence εk>0\varepsilon_k>0εk​>0 with εk→0\varepsilon_k\to0εk​→0, and the limit control is required to be admissible. The backward equations use the published Peng1990.SMP.SolvesBSDE, and the pseudoinverse in (4.6) and (4.11) is the published HarmonicGames.Decomposition.pinv.

Theorem 6.1 prints the term −Θε⊤ρ-\Theta_\varepsilon^\top\rho−Θε⊤​ρ in its backward equation. The equation (4.11) that its proof uses through Corollary 4.7 has +Θε⊤ρ+\Theta_\varepsilon^\top\rho+Θε⊤​ρ, and the formalization uses (4.11). Corollary 3.4 is stated without its item (vi), which involves an operator M2(t)M_2(t)M2​(t) that the paper quotes from another source.

The families PεP_\varepsilonPε​, (ηε,ζε)(\eta_\varepsilon,\zeta_\varepsilon)(ηε​,ζε​) and XεX_\varepsilonXε​ are hypotheses pinned by their equations for every ε>0\varepsilon>0ε>0. The sequence uεu_\varepsilonuε​ is therefore the Riccati feedback sequence (6.2), never an arbitrary minimizing sequence or an arbitrary family of ε\varepsilonε-optimal controls; with such a family the implication (ii) ⇒ (i) would be a different theorem.

Contributions are welcome at every level: the solution theory of linear SDEs and BSDEs, Itô's formula for quadratic forms, Riccati and Lyapunov equations in integral form, weak compactness in LF2L^2_{\mathbb F}LF2​, and the milestones themselves.

Selected references

  • J. Sun, X. Li, J. Yong, Open-loop and closed-loop solvabilities for stochastic linear quadratic optimal control problems, SIAM J. Control Optim. 54(5) (2016) 2274–2308. https://doi.org/10.1137/15M103532X
  • J. Sun, J. Yong, Linear quadratic stochastic differential games: open-loop and closed-loop saddle points, SIAM J. Control Optim. 52(6) (2014) 4082–4121. https://doi.org/10.1137/140953642
  • S. Chen, X. Li, X. Y. Zhou, Stochastic linear quadratic regulators with indefinite control weight costs, SIAM J. Control Optim. 36(5) (1998) 1685–1702. https://doi.org/10.1137/S0363012996310478
  • M. Ait Rami, J. B. Moore, X. Y. Zhou, Indefinite stochastic linear quadratic control and generalized differential Riccati equation, SIAM J. Control Optim. 40(4) (2002) 1296–1311. https://doi.org/10.1137/S0363012900371083
  • S. Peng, A general stochastic maximum principle for optimal control problems, SIAM J. Control Optim. 28(4) (1990) 966–979. https://doi.org/10.1137/0328054
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Convex OptimizationOptimization·Captain: mikedeng1

On the Convergence of Decentralized Gradient Descent II: For Convex Smooth fᵢ the Mean Iterate Has Objective Error r̄(k) ≤ 4C²/(αk) Until r̄ Falls to C√2·αL_hD/(1 − β)Research Paper

Motivation

In decentralized optimization, nnn agents connected by a communication network jointly minimize a sum of private functions without a central coordinator: each agent sees only its own fif_ifi​ and talks only to its neighbours. Applications include sensor networks, distributed estimation, multi-agent control and learning over data spread across machines. The simplest method in this setting is decentralized gradient descent (DGD), in which every agent averages its neighbours' iterates and then takes a local gradient step. DGD and its relatives were analysed by Nedić and Ozdaglar (IEEE TAC 2009) and many later papers, almost always under the assumption that the (sub)gradients are bounded.

K. Yuan, Q. Ling and W. Yin (arXiv:1310.7063v3; SIAM J. Optim. 26(3), 2016) removed that assumption for DGD with a fixed stepsize. They showed that a stepsize bound depending on the spectrum of the mixing matrix keeps the gradients bounded, that the agents stay within O(α/(1−β))O(\alpha/(1-\beta))O(α/(1−β)) of their mean, and that for convex smooth fif_ifi​ the objective error of the mean decreases at rate O(1/(αk))O(1/(\alpha k))O(1/(αk)) until it reaches a neighbourhood of size O(α/(1−β))O(\alpha/(1-\beta))O(α/(1−β)). This mission formalizes that last result, Theorem 2 of the paper, together with the lemmas its proof rests on.

Setting

Consider n≥2n \ge 2n≥2 agents on a connected undirected graph GGG. Agent iii holds a function fi:Rp→Rf_i : \mathbb R^p \to \mathbb Rfi​:Rp→R, and the agents solve

min⁡x∈Rpf(x)=∑i=1nfi(x),(2)\min_{x \in \mathbb R^p} f(x) = \sum_{i=1}^n f_i(x), \qquad (2)x∈Rpmin​f(x)=i=1∑n​fi​(x),(2)

with solution set X∗\mathcal X^*X∗, assumed nonempty.

A mixing matrix W=[wij]W = [w_{ij}]W=[wij​] is symmetric and doubly stochastic, and wij≠0w_{ij} \ne 0wij​=0 only if i=ji = ji=j or iii and jjj are neighbours. Its eigenvalues are 1=λ1(W)≥λ2(W)≥⋯≥λn(W)≥−11 = \lambda_1(W) \ge \lambda_2(W) \ge \dots \ge \lambda_n(W) \ge -11=λ1​(W)≥λ2​(W)≥⋯≥λn​(W)≥−1, and

β=max⁡{∣λ2(W)∣,∣λn(W)∣}.(5)\beta = \max\{|\lambda_2(W)|, |\lambda_n(W)|\}. \qquad (5)β=max{∣λ2​(W)∣,∣λn​(W)∣}.(5)

Assumption 1 (p. 4): (a) each fif_ifi​ is convex, bounded below, and differentiable with an LfiL_{f_i}Lfi​​-Lipschitz gradient, Lfi>0L_{f_i} > 0Lfi​​>0; (b) the network is connected and WWW is symmetric, doubly stochastic, with β<1\beta < 1β<1.

DGD with stepsize α\alphaα, started from x(i)(0)=0x_{(i)}(0) = 0x(i)​(0)=0, is

x(i)(k+1)=∑j=1nwij x(j)(k)−α∇fi(x(i)(k)),i=1,…,n.(4)x_{(i)}(k+1) = \sum_{j=1}^n w_{ij}\, x_{(j)}(k) - \alpha \nabla f_i(x_{(i)}(k)), \qquad i = 1, \dots, n. \qquad (4)x(i)​(k+1)=j=1∑n​wij​x(j)​(k)−α∇fi​(x(i)​(k)),i=1,…,n.(4)

Stacked vectors [x(i)]=[x(1);… ;x(n)]∈Rnp[x_{(i)}] = [x_{(1)}; \dots; x_{(n)}] \in \mathbb R^{np}[x(i)​]=[x(1)​;…;x(n)​]∈Rnp carry the Euclidean norm. Write h(k)=[∇f1(x(1)(k));… ;∇fn(x(n)(k))]h(k) = [\nabla f_1(x_{(1)}(k)); \dots; \nabla f_n(x_{(n)}(k))]h(k)=[∇f1​(x(1)​(k));…;∇fn​(x(n)​(k))], xˉ(k)=1n∑ix(i)(k)\bar x(k) = \frac1n\sum_i x_{(i)}(k)xˉ(k)=n1​∑i​x(i)​(k), g(k)=1n∑i∇fi(x(i)(k))g(k) = \frac1n\sum_i\nabla f_i(x_{(i)}(k))g(k)=n1​∑i​∇fi​(x(i)​(k)), gˉ(k)=1n∑i∇fi(xˉ(k))\bar g(k) = \frac1n\sum_i \nabla f_i(\bar x(k))gˉ​(k)=n1​∑i​∇fi​(xˉ(k)), fˉ=1nf\bar f = \frac1n ffˉ​=n1​f, Lh=max⁡iLfiL_h = \max_i L_{f_i}Lh​=maxi​Lfi​​, Lfˉ=1n∑iLfiL_{\bar f} = \frac1n\sum_i L_{f_i}Lfˉ​​=n1​∑i​Lfi​​, fio=inf⁡fif_i^o = \inf f_ifio​=inffi​ and

D=2Lh∑i=1n(fi(0)−fio).(10)D = \sqrt{2L_h\textstyle\sum_{i=1}^n\big(f_i(0) - f_i^o\big)}. \qquad (10)D=2Lh​∑i=1n​(fi​(0)−fio​)​.(10)

The paper reads DGD as unit-step gradient descent on the Lyapunov function

ξα([x(i)])=−12∑i,jwij x(i)⊤x(j)+∑i(12∥x(i)∥2+αfi(x(i))).(8)\xi_\alpha([x_{(i)}]) = -\tfrac12\textstyle\sum_{i,j} w_{ij}\, x_{(i)}^\top x_{(j)} + \sum_i\big(\tfrac12\|x_{(i)}\|^2 + \alpha f_i(x_{(i)})\big). \qquad (8)ξα​([x(i)​])=−21​∑i,j​wij​x(i)⊤​x(j)​+∑i​(21​∥x(i)​∥2+αfi​(x(i)​)).(8)

For a minimizer [x~(i)][\tilde x_{(i)}][x~(i)​] of ξα\xi_\alphaξα​ and a solution x∗∈X∗x^* \in \mathcal X^*x∗∈X∗, set

C=1n(∥[x(i)(0)−x~(i)]∥+∥[x~(i)−x∗]∥),rˉ(k)=fˉ(xˉ(k))−fˉ(x∗).(17)C = \frac{1}{\sqrt n}\Big(\|[x_{(i)}(0) - \tilde x_{(i)}]\| + \|[\tilde x_{(i)} - x^*]\|\Big), \qquad \bar r(k) = \bar f(\bar x(k)) - \bar f(x^*). \qquad (17)C=n​1​(∥[x(i)​(0)−x~(i)​]∥+∥[x~(i)​−x∗]∥),rˉ(k)=fˉ​(xˉ(k))−fˉ​(x∗).(17)

Formalization targets

Goal: Theorem 2 with the constants of its proof

Let 0<α≤min⁡{(1+λn(W))/Lh, 1/Lfˉ}0 < \alpha \le \min\{(1+\lambda_n(W))/L_h,\ 1/L_{\bar f}\}0<α≤min{(1+λn​(W))/Lh​, 1/Lfˉ​​} and T=C2⋅αLhD/(1−β)T = C\sqrt2\cdot\alpha L_h D/(1-\beta)T=C2​⋅αLh​D/(1−β). Then

rˉ(k)>T ⟹ rˉ(k+1)≤rˉ(k)−α4C2 rˉ(k)2,\bar r(k) > T \ \Longrightarrow\ \bar r(k+1) \le \bar r(k) - \frac{\alpha}{4C^2}\,\bar r(k)^2,rˉ(k)>T ⟹ rˉ(k+1)≤rˉ(k)−4C2α​rˉ(k)2,

and, for k≥1k \ge 1k≥1, if rˉ(j)>T\bar r(j) > Trˉ(j)>T for every j<kj < kj<k, then

rˉ(k)≤4C2αk.\bar r(k) \le \frac{4C^2}{\alpha k}.rˉ(k)≤αk4C2​.

The paper prints these as rˉ(k+1)≤rˉ(k)−O(αrˉ2(k))\bar r(k+1) \le \bar r(k) - O(\alpha\bar r^2(k))rˉ(k+1)≤rˉ(k)−O(αrˉ2(k)) and rˉ(k)≤O(1/(αk))\bar r(k) \le O(1/(\alpha k))rˉ(k)≤O(1/(αk)). The constants are the ones its proof fixes: the recursion with α/(2C2)\alpha/(2C^2)α/(2C2) (milestone below) and the threshold condition "(α/(2C2))rˉ2(k)>2⋅α3D2Lh2/(2(1−β)2)(\alpha/(2C^2))\bar r^2(k) > 2\cdot\alpha^3D^2L_h^2/(2(1-\beta)^2)(α/(2C2))rˉ2(k)>2⋅α3D2Lh2​/(2(1−β)2)", under which the error term absorbs half of the quadratic decrease. That gives α/(4C2)\alpha/(4C^2)α/(4C2), and "1/rˉ(k)1/\bar r(k)1/rˉ(k) increases at Ω(αk)\Omega(\alpha k)Ω(αk)" with this constant gives 4C2/(αk)4C^2/(\alpha k)4C2/(αk).

Milestones

  1. Theorem 1, (10): for 0<α≤(1+λn(W))/Lh0 < \alpha \le (1+\lambda_n(W))/L_h0<α≤(1+λn​(W))/Lh​, ∥h(k)∥≤D\|h(k)\| \le D∥h(k)∥≤D for every kkk.
  2. Lemma 1: if ∥h(s)∥≤B\|h(s)\| \le B∥h(s)∥≤B for all sss, then ∥x(i)(k)−xˉ(k)∥≤αB/(1−β)\|x_{(i)}(k) - \bar x(k)\| \le \alpha B/(1-\beta)∥x(i)​(k)−xˉ(k)∥≤αB/(1−β).
  3. Lemma 2: ∥∇fi(x(i)(k))−∇fi(xˉ(k))∥≤αBLfi/(1−β)\|\nabla f_i(x_{(i)}(k)) - \nabla f_i(\bar x(k))\| \le \alpha B L_{f_i}/(1-\beta)∥∇fi​(x(i)​(k))−∇fi​(xˉ(k))∥≤αBLfi​​/(1−β) and ∥g(k)−gˉ(k)∥≤αBLh/(1−β)\|g(k) - \bar g(k)\| \le \alpha B L_h/(1-\beta)∥g(k)−gˉ​(k)∥≤αBLh​/(1−β).
  4. (15): xˉ(k+1)=xˉ(k)−αg(k)\bar x(k+1) = \bar x(k) - \alpha g(k)xˉ(k+1)=xˉ(k)−αg(k).
  5. (17): ∥[x(i)(k)−x~(i)]∥≤∥[x(i)(0)−x~(i)]∥\|[x_{(i)}(k) - \tilde x_{(i)}]\| \le \|[x_{(i)}(0) - \tilde x_{(i)}]\|∥[x(i)​(k)−x~(i)​]∥≤∥[x(i)​(0)−x~(i)​]∥ and ∥xˉ(k)−x∗∥≤C\|\bar x(k) - x^*\| \le C∥xˉ(k)−x∗∥≤C.
  6. rˉ(k+1)≤rˉ(k)−α2∥gˉ(k)∥2+α3D2Lh22(1−β)2\bar r(k+1) \le \bar r(k) - \frac{\alpha}{2}\|\bar g(k)\|^2 + \frac{\alpha^3D^2L_h^2}{2(1-\beta)^2}rˉ(k+1)≤rˉ(k)−2α​∥gˉ​(k)∥2+2(1−β)2α3D2Lh2​​.
  7. rˉ(k+1)≤rˉ(k)−α2C2rˉ(k)2+α3D2Lh22(1−β)2\bar r(k+1) \le \bar r(k) - \frac{\alpha}{2C^2}\bar r(k)^2 + \frac{\alpha^3D^2L_h^2}{2(1-\beta)^2}rˉ(k+1)≤rˉ(k)−2C2α​rˉ(k)2+2(1−β)2α3D2Lh2​​.

Significance

Theorem 2 is the convex, non-strongly-convex case of the paper's analysis. It says that DGD with a constant stepsize behaves like centralized gradient descent, with rate O(1/k)O(1/k)O(1/k), until it reaches a floor of size O(α/(1−β))O(\alpha/(1-\beta))O(α/(1−β)). The floor shrinks with the stepsize and grows as the spectral gap 1−β1-\beta1−β of the network closes, which makes the trade-off between speed, accuracy and network connectivity explicit. The result is proved without bounded gradients; the boundedness comes out of the stepsize condition through the Lyapunov function. It is the baseline that exact methods such as EXTRA (Shi et al. 2015) were designed to improve on.

The paper's proof is complete in its main lines but informal in places: the rate is stated with O(⋅)O(\cdot)O(⋅), the constant CCC is written with a kkk-dependent x∗(k)x^*(k)x∗(k), and the minimizer of ξα\xi_\alphaξα​ is asserted to exist on grounds that do not suffice. To our knowledge no part of this analysis (DGD, mixing matrices with spectral bounds, the Lyapunov reformulation) has been machine-checked. A formal proof fixes the constants, records the needed hypotheses, and supplies decentralized-optimization infrastructure that Mathlib lacks.

Difficulty

The obvious approach treats the mean xˉ(k)\bar x(k)xˉ(k) as gradient descent on fˉ\bar ffˉ​ with the exact gradient gˉ(k)\bar g(k)gˉ​(k), which fails: by (15) the mean moves along g(k)g(k)g(k), the average of gradients taken at different points. Controlling g(k)−gˉ(k)g(k) - \bar g(k)g(k)−gˉ​(k) needs the consensus bound of Lemma 1, which in turn needs the gradients to be bounded, and no assumption bounds them. They are bounded only because DGD is unit-step gradient descent on ξα\xi_\alphaξα​ and the stepsize condition makes that descent monotone (Theorem 1). Lemma 1 also needs the operator-norm identity ∥Wm−1n11⊤∥=βm\|W^m - \frac1n\mathbf 1\mathbf 1^\top\| = \beta^m∥Wm−n1​11⊤∥=βm for a symmetric doubly stochastic WWW, a spectral fact about sorted eigenvalues. Finally, the recursion in rˉ\bar rrˉ needs a bound on ∥xˉ(k)−x∗∥\|\bar x(k) - x^*\|∥xˉ(k)−x∗∥ that is uniform in kkk, which comes from Fejér monotonicity of the iterates with respect to a minimizer of ξα\xi_\alphaξα​, not from anything about fˉ\bar ffˉ​.

Formalization scope

Rp\mathbb R^pRp is EuclideanSpace ℝ (Fin p) and stacked vectors are PiLp 2 (fun _ : Fin n => ℝᵖ), so every stacked norm (∥h(k)∥\|h(k)\|∥h(k)∥, DDD, CCC) is Euclidean on Rnp\mathbb R^{np}Rnp, not the sup norm. Gradients are Mathlib's gradient. DGD is a recursively defined sequence started at 000, not an arbitrary sequence with a property. λn(W)\lambda_n(W)λn​(W) and β\betaβ come from the eigenvalues of the symmetric WWW sorted with multiplicity (eigenvalues₀). fiof_i^ofio​ is inf⁡fi\inf f_iinffi​, and LhL_hLh​ is a supremum over the finite index set, i.e. a maximum.

Conventions and additions, each disclosed in the item statements:

  • n≥2n \ge 2n≥2 is part of Assumption 1 (so that λ2(W)\lambda_2(W)λ2​(W) exists); α>0\alpha > 0α>0 (a stepsize).
  • A minimizer [x~(i)][\tilde x_{(i)}][x~(i)​] of ξα\xi_\alphaξα​ is a hypothesis. The paper derives its existence from minimizers of the fif_ifi​, which Assumption 1 does not provide.
  • CCC uses one fixed x∗∈X∗x^* \in \mathcal X^*x∗∈X∗, chosen before kkk; that x∗x^*x∗ also defines fˉ∗=fˉ(x∗)\bar f^* = \bar f(x^*)fˉ​∗=fˉ​(x∗). On the page x∗x^*x∗ in (17) is x∗(k)x^*(k)x∗(k), which would make CCC depend on kkk.
  • Theorem 1's convergence sentence is not posed; it fails at the boundary stepsize α=(1+λn(W))/Lh\alpha = (1+\lambda_n(W))/L_hα=(1+λn​(W))/Lh​. Only the bound (10) is posed, for every k≥0k \ge 0k≥0.
  • Lemmas 1 and 2 take a generic gradient bound BBB in place of DDD.

Trivializing formalizations are ruled out. The iterates are the DGD recursion itself. The threshold in the rate is required at every earlier step, not only at step kkk. CCC does not depend on kkk. The constants α/(4C2)\alpha/(4C^2)α/(4C2) and 4C2/(αk)4C^2/(\alpha k)4C2/(αk) are explicit, not an existential placed before the data. A sorry-free instance (n=2n = 2n=2, W=1211⊤W = \frac12\mathbf 1\mathbf 1^\topW=21​11⊤, constant fif_ifi​) shows that the goal's hypotheses can all hold together.

A complete development needs: the operator norm of Wm−1n11⊤W^m - \frac1n\mathbf 1\mathbf 1^\topWm−n1​11⊤ via the spectral theorem, the descent lemma and co-coercivity for LLL-smooth convex functions on Euclidean space, ∥∇g∥2≤2L(g−inf⁡g)\|\nabla g\|^2 \le 2L(g - \inf g)∥∇g∥2≤2L(g−infg) for LLL-smooth functions bounded below, and Fejér monotonicity of gradient descent. These are reusable well beyond this mission. Contributions to any milestone are welcome; Lemmas 1–2 and (15) do not use convexity.

Selected references

  • K. Yuan, Q. Ling, W. Yin, On the Convergence of Decentralized Gradient Descent, SIAM J. Optim. 26(3), 2016, https://doi.org/10.1137/130943170; preprint arXiv:1310.7063v3 (the version cited throughout). https://arxiv.org/abs/1310.7063
  • A. Nedić, A. Ozdaglar, Distributed Subgradient Methods for Multi-Agent Optimization, IEEE Trans. Automat. Control 54(1):48–61, 2009. https://doi.org/10.1109/TAC.2008.2009515
  • Y. Nesterov, Gradient Methods for Minimizing Composite Objective Function, CORE report, 2007 (reference [21] of the paper, cited for the gradient-descent facts); journal version Math. Program. 140:125–161, 2013. https://doi.org/10.1007/s10107-012-0629-5
  • W. Shi, Q. Ling, G. Wu, W. Yin, EXTRA: An Exact First-Order Algorithm for Decentralized Consensus Optimization, SIAM J. Optim. 25(2):944–966, 2015. https://doi.org/10.1137/14096668X
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Algorithmic Game TheoryEconomicsOperations Research+1·Captain: mikedeng1

Dynamic Pricing in the Presence of Social Learning and Strategic Consumers 1: Under Pre-Announced Pricing, Social Learning Raises Optimal Expected Profit When Consumers Are Impatient or PatientResearch Paper

Motivation

Online reviews let consumers learn about a new product from the experience of earlier buyers. For a firm selling to strategic consumers, who time their purchases, this social learning (SL) cuts two ways. Reviews reveal quality, which can raise second-period demand; but a consumer who expects reviews also has a new reason to wait, and every consumer who waits writes no review. Papanastasiou and Savva (Management Science 63(4), 2017) build a two-period model in which both forces are endogenous and ask whether a monopolist that commits to its prices in advance is better or worse off when consumers learn from one another.

The benchmark without learning is the classical intertemporal pricing problem with strategic consumers (Landsberger and Meilijson, 1985), whose optimal pre-announced plan is a decreasing price path. This mission formalizes the paper's answer for pre-announced pricing: its Proposition 3.

Setting

A unit mass of consumers has preference types xxx uniform on [0,1][0,1][0,1]. A product of unknown mean quality q^\hat qq^​ is sold over two periods. Buying in period ttt gives type xxx the utility δct−1(x+q−pt)\delta_c^{t-1}(x+q-p_t)δct−1​(x+q−pt​), where δc∈[0,1]\delta_c\in[0,1]δc​∈[0,1] is the consumers' discount factor and qqq the perceived quality. The firm has unit cost c∈[0,1)c\in[0,1)c∈[0,1) and does not discount.

Everyone shares the prior q^∼N(0,σp2)\hat q\sim N(0,\sigma_p^2)q^​∼N(0,σp2​). Individual quality perceptions are N(q^,σq2)N(\hat q,\sigma_q^2)N(q^​,σq2​), and γ=σp2/σq2\gamma=\sigma_p^2/\sigma_q^2γ=σp2​/σq2​ is the SL influence parameter. If a mass n1n_1n1​ buys in period 1 and posts reviews, the posterior mean is qu=n1γn1γ+1Rq_u=\tfrac{n_1\gamma}{n_1\gamma+1}Rqu​=n1​γ+1n1​γ​R, where RRR is the average rating. Seen from period 1, quq_uqu​ is random, with the pre-posterior law

qu∼N ⁣(0, σp2 n1γn1γ+1).q_u\sim N\!\left(0,\ \sigma_p^2\,\frac{n_1\gamma}{n_1\gamma+1}\right).qu​∼N(0, σp2​n1​γ+1n1​γ​).

Under pre-announced pricing the firm commits to a plan {p1,p2}\{p_1,p_2\}{p1​,p2​}. Consumers then play a purchasing game. A set B⊆[0,1]B\subseteq[0,1]B⊆[0,1] of early buyers is an equilibrium if every type in BBB weakly prefers buying now, x−p1≥0x-p_1\ge 0x−p1​≥0 and x−p1≥δc E[(x+qu−p2)+]x-p_1\ge\delta_c\,\mathbb E[(x+q_u-p_2)^+]x−p1​≥δc​E[(x+qu​−p2​)+], and every other type weakly prefers to wait. Here quq_uqu​ has the pre-posterior law for n1=∣B∣n_1=|B|n1​=∣B∣. In period 2 the remaining types buy iff x+qu≥p2x+q_u\ge p_2x+qu​≥p2​. The firm's expected profit is

πp(p1,p2;B)=(p1−c) ∣B∣+(p2−c) E[ ∣{x∈[0,1]∖B: x+qu≥p2}∣ ],\pi_p(p_1,p_2;B)=(p_1-c)\,|B|+(p_2-c)\,\mathbb E\big[\,|\{x\in[0,1]\setminus B:\ x+q_u\ge p_2\}|\,\big],πp​(p1​,p2​;B)=(p1​−c)∣B∣+(p2​−c)E[∣{x∈[0,1]∖B: x+qu​≥p2​}∣],

and the optimal pre-announced profit πp∗\pi_p^*πp∗​ is its supremum over all plans and all their equilibria. Absence of SL is the same model at γ=0\gamma=0γ=0, where qu≡0q_u\equiv 0qu​≡0.

Formalization targets

Goal: Proposition 3

For γ>0\gamma>0γ>0 there are thresholds Δlp(γ)∈(0,1]\Delta_{lp}(\gamma)\in(0,1]Δlp​(γ)∈(0,1] and Δhp(γ)∈[0,1)\Delta_{hp}(\gamma)\in[0,1)Δhp​(γ)∈[0,1) such that

δc≤Δlp(γ)  or  δc≥Δhp(γ)⟹πp∗∣γ>πp∗∣γ=0.\delta_c\le\Delta_{lp}(\gamma)\ \text{ or }\ \delta_c\ge\Delta_{hp}(\gamma)\quad\Longrightarrow\quad \pi_p^*\big|_{\gamma}>\pi_p^*\big|_{\gamma=0}.δc​≤Δlp​(γ)  or  δc​≥Δhp​(γ)⟹πp∗​​γ​>πp∗​​γ=0​.

Milestones

  1. Lemma 1: the pre-posterior law above.
  2. Display (2): without SL, the buyer set is [τ(p1,p2),1][\tau(p_1,p_2),1][τ(p1​,p2​),1] for an explicit threshold τ\tauτ.
  3. Proposition 1: without SL, π∗=(1−c)2/(δc+3)\pi^*=(1-c)^2/(\delta_c+3)π∗=(1−c)2/(δc​+3), attained at p1∗=c(1+δc)+2δc+3p_1^*=\tfrac{c(1+\delta_c)+2}{\delta_c+3}p1∗​=δc​+3c(1+δc​)+2​ and p2∗=2c+δc+1δc+3p_2^*=\tfrac{2c+\delta_c+1}{\delta_c+3}p2∗​=δc​+32c+δc​+1​.
  4. Lemma 2: with SL, the buyer set is [θ,1][\theta,1][θ,1], where θ\thetaθ solves the implicit equation (3), or θ=1\theta=1θ=1 under adoption inertia. A companion item states that θ\thetaθ is monotone in γ,p1,δc,p2\gamma,p_1,\delta_c,p_2γ,p1​,δc​,p2​.
  5. Lemma 5: waiting is worth strictly more when more consumers buy early.
  6. Proposition 2: adoption inertia is never optimal, and patient consumers face an increasing optimal price path.
  7. Examples 1 and 2: with myopic consumers, SL raises the optimal second-period price and the optimal profit.
  8. πp∗\pi_p^*πp∗​ is continuous in δc∈[0,1]\delta_c\in[0,1]δc​∈[0,1].

Significance

Proposition 3 says that social learning helps the firm at both ends of the patience range. For myopic consumers this is the informational effect alone. For patient consumers it holds even though learning makes them strictly more inclined to wait (Lemma 2) and the committed price cannot react to the reviews. The paper's numerical experiments found no intermediate δc\delta_cδc​ at which learning hurts, but the theorem asserts only the two ends. The result underlies the managerial conclusions of the paper: firms gain from encouraging reviews even when consumers are strategic.

The result is proved in the paper; nothing in the model has been machine-checked before. A formal proof would check the equilibrium analysis of a continuum purchasing game with an endogenous information externality. Its intermediate results also serve the paper's two other missions: responsive pricing, and the comparison of responsive with pre-announced pricing. These are the Normal convex-order monotonicity (Lemma 5), the implicit threshold equation (Lemma 2), the no-SL benchmark (Proposition 1) and a Maximum-Theorem continuity statement.

Difficulty

The equilibrium threshold θ\thetaθ solves an equation whose Normal kernel has a variance that depends on θ\thetaθ itself. Existence, uniqueness and monotonicity are not closed-form computations.

The endpoint δc=1\delta_c=1δc​=1 is the delicate one. There learning makes waiting most attractive, and the strict gain over the no-SL optimum (1−c)2/4(1-c)^2/4(1−c)2/4 must come from a plan that still induces a positive mass of early buyers.

Continuity of πp∗\pi_p^*πp∗​ in δc\delta_cδc​ is a Maximum-Theorem argument for a supremum over an unbounded set of prices whose objective passes through an implicit equilibrium. Compactness of the relevant price set has to be established, not assumed.

Formalization scope

Every statement is taken over the standing assumptions σp>0\sigma_p>0σp​>0, γ≥0\gamma\ge 0γ≥0, δc∈[0,1]\delta_c\in[0,1]δc​∈[0,1], c∈[0,1)c\in[0,1)c∈[0,1), with firm discount factor 111 and pure strategies. Further conventions:

  • Absence of SL is the same model at γ=0\gamma=0γ=0. There the pre-posterior law is the point mass at 000, which is the paper's limit γ→0\gamma\to 0γ→0.
  • Best responses are weak. Equilibrium buyer sets are therefore unique only up to Lebesgue-null sets. The degenerate plan p1=p2p_1=p_2p1​=p2​ at δc=1\delta_c=1δc​=1 without SL, where every type is indifferent, is excluded from the uniqueness claim of (2).
  • Optimal values are suprema in the extended reals over all real plans and all purchasing equilibria. They are never real suprema with junk values, never the profit at a closed-form price, and never restricted to threshold equilibria. "Optimal plan" means a plan one of whose equilibria attains the supremum.
  • Proposition 3's thresholds are stated with the strict bounds Δlp>0\Delta_{lp}>0Δlp​>0 and Δhp<1\Delta_{hp}<1Δhp​<1. With closed bounds the claim would follow from the cases δc=0\delta_c=0δc​=0 and δc=1\delta_c=1δc​=1 alone.
  • Added hypotheses, each disclosed in its item:
    • p1∈[0,1]p_1\in[0,1]p1​∈[0,1] in Lemma 2 and its monotonicity item, and p1≥0p_1\ge 0p1​≥0 in (2);
    • δc>0\delta_c>0δc​>0 in Lemma 5;
    • p1<1p_1<1p1​<1 in Example 1 (at p1=1p_1=1p1​=1 nobody buys early, so the example's strict inequality fails there), and c<p1c<p_1c<p1​ for its no-SL uniqueness part;
    • δc<1\delta_c<1δc​<1 for uniqueness in Proposition 1;
    • n1>0n_1>0n1​>0 in Lemma 1;
    • existence of an optimal plan, asserted together with Proposition 2(ii);
    • monotonicity of θ\thetaθ is weak.
  • Not posed:
    • Lemma 2(ii) is built into the second-period demand.
    • The "unique equilibrium" clauses of Propositions 1 and 2 are the items for (2) and Lemma 2.
    • The fixed-price variant of Proposition 3 (pp. 17–18) is false at δc=1\delta_c=1δc​=1.

The witness used in the printed proof of Proposition 2(i) does not settle the case δc=1\delta_c=1δc​=1.

A complete development needs Gaussian expectations of hinge functions and their monotonicity in the variance (strict convex order), an implicit-equation argument for the threshold, and a version of Berge's Maximum Theorem. The Gaussian lemmas and the no-SL benchmark are reusable across the series. Contributions to any milestone are welcome.

Selected references

  • Y. Papanastasiou, N. Savva, Dynamic Pricing in the Presence of Social Learning and Strategic Consumers, Management Science 63(4):919–939, 2017. https://doi.org/10.1287/mnsc.2015.2378 (cited from the accepted manuscript MS-14-00028.R2, 2016)
  • M. Landsberger, I. Meilijson, Intertemporal price discrimination and sales strategy under incomplete information, RAND Journal of Economics 16(3):424–430, 1985. https://doi.org/10.2307/2555568
  • G. P. Cachon, R. Swinney, Purchasing, Pricing, and Quick Response in the Presence of Strategic Consumers, Management Science 55(3):497–511, 2009. https://doi.org/10.1287/mnsc.1080.0948
  • A. Müller, D. Stoyan, Comparison Methods for Stochastic Models and Risks, Wiley, 2002. https://doi.org/10.1002/9780470317167
  • R. K. Sundaram, A First Course in Optimization Theory, Cambridge University Press, 1996. https://doi.org/10.1017/CBO9780511804526
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AnalysisMathematical PhysicsProbability·Captain: mikedeng1

Conformal Weldings of Random Surfaces: SLE and the Quantum Gravity Zipper 2: For κ < 4, Reverse SLE_κ Zipping Welds Boundary Arcs of Equal Quantum Length, ν_h[z₋,0] = ν_h[0,z₊]Research Paper

Why conformal welding by quantum length

Liouville quantum gravity (LQG) equips a planar domain with a random area measure μh\mu_hμh​ and a random boundary length measure νh\nu_hνh​. Both are built from an instance hhh of the Gaussian free field (GFF). The Schramm–Loewner evolution SLEκ\mathrm{SLE}_\kappaSLEκ​ is the conformally invariant random curve that describes interfaces in critical planar models. Sheffield's paper (arXiv:1012.4797, Ann. Probab. 44 (2016)) shows that the two are linked by a conformal welding. Zipping up a free boundary GFF by a reverse Loewner flow glues two boundary arcs of equal quantum length, and the glued seam is an SLEκ\mathrm{SLE}_\kappaSLEκ​ curve.

This "quantum zipper" is the starting point of the mating-of-trees programme (Duplantier–Miller–Sheffield, arXiv:1409.7055). It is also the mechanism behind the conjectured, and partly proved, scaling limits of random planar maps decorated by statistical-physics models.

Timeline:

  • 2005 — reverse Loewner flows are studied by Rohde and Schramm (RS05). They show that for κ<4\kappa<4κ<4 the SLE trace is simple and its complement is a Hölder domain.
  • 2000 — Jones and Smirnov show that boundaries of Hölder domains are conformally removable (JS00).
  • 2011 — Duplantier and Sheffield construct μh\mu_hμh​ and νh\nu_hνh​ as almost sure limits along dyadic scales and prove the KPZ relation (DS11a).
  • 2010–2016 — this paper (arXiv v1 2010, v2 2015, journal 2016) proves the welding theorem (Theorem 1.3) and the quantum-length zipper (Theorem 1.8).

Setting

H={z:Im⁡z>0}\mathbb H=\{z:\operatorname{Im}z>0\}H={z:Imz>0}, and the free boundary Green's function is G(y,z)=−log⁡∣y−z∣−log⁡∣y−zˉ∣G(y,z)=-\log|y-z|-\log|y-\bar z|G(y,z)=−log∣y−z∣−log∣y−zˉ∣. Fix κ∈(0,4)\kappa\in(0,4)κ∈(0,4) and put γ=κ\gamma=\sqrt\kappaγ=κ​ and Q=2/γ+γ/2Q=2/\gamma+\gamma/2Q=2/γ+γ/2.

  • Reverse Loewner flow. For a standard Brownian motion BBB, ft=gt−κBtf_t=g_t-\sqrt\kappa B_tft​=gt​−κ​Bt​, where ∂tgt(z)=−2/(gt(z)−κBt)\partial_tg_t(z)=-2/(g_t(z)-\sqrt\kappa B_t)∂t​gt​(z)=−2/(gt​(z)−κ​Bt​) and g0(z)=zg_0(z)=zg0​(z)=z. Then fTf_TfT​ maps H\mathbb HH onto H∖ηT\mathbb H\setminus\eta_TH∖ηT​, and ηT\eta_TηT​ is a simple curve.
  • The coupled field. Let ht(z)=2κlog⁡∣ft(z)∣+Qlog⁡∣ft′(z)∣\mathfrak h_t(z)=\frac2{\sqrt\kappa}\log|f_t(z)|+Q\log|f_t'(z)|ht​(z)=κ​2​log∣ft​(z)∣+Qlog∣ft′​(z)∣. With h~\tilde hh~ a free boundary GFF independent of BBB,
h=hT+h~∘fT,h=\mathfrak h_T+\tilde h\circ f_T ,h=hT​+h~∘fT​,

which by Theorem 1.2 has the law of 2κlog⁡∣⋅∣+h~\frac2{\sqrt\kappa}\log|\cdot|+\tilde hκ​2​log∣⋅∣+h~ modulo additive constants.

  • Quantum length. hε(x)h_\varepsilon(x)hε​(x) is the mean of hhh on the upper semicircle of radius ε\varepsilonε around x∈Rx\in\mathbb Rx∈R. Then
νh=lim⁡n→∞εnγ2/4eγhεn(x)/2 dx,εn=2−n,\nu_h=\lim_{n\to\infty}\varepsilon_n^{\gamma^2/4}e^{\gamma h_{\varepsilon_n}(x)/2}\,dx,\qquad \varepsilon_n=2^{-n},νh​=n→∞lim​εnγ2/4​eγhεn​​(x)/2dx,εn​=2−n,

as a vague limit. The area measure μh\mu_hμh​ is the analogous limit with circle averages and exponent γ2/2\gamma^2/2γ2/2.

  • Quantum wedges. An α\alphaα-quantum wedge is the doubly marked surface (H,h)(\mathbb H,h)(H,h) with h=h†+Q(−log⁡∣⋅∣)+A−log⁡∣⋅∣h=h^\dagger+Q(-\log|\cdot|)+A_{-\log|\cdot|}h=h†+Q(−log∣⋅∣)+A−log∣⋅∣​ (1.10). Here h†h^\daggerh† is the lateral part of the GFF and AAA is a two-sided drifted Brownian motion. A surface is identified with its canonical description, normalized by μh(B1(0))=1\mu_h(B_1(0))=1μh​(B1​(0))=1.

Formalization targets

Goal: Theorem 1.3

Almost surely, for every zzz on ηT\eta_TηT​ and the two real points z−<0<z+z_-<0<z_+z−​<0<z+​ that fTf_TfT​ maps to zzz,

νh([z−,0])=νh([0,z+]).\nu_h\big([z_-,0]\big)=\nu_h\big([0,z_+]\big).νh​([z−​,0])=νh​([0,z+​]).

The statement is scale free: it does not depend on the additive constant of hhh.

Milestones

  1. Theorem 4.5. Reverse SLEκ,ρ\mathrm{SLE}_{\kappa,\rho}SLEκ,ρ​ zipping preserves the law of h^0+h~\hat{\mathfrak h}_0+\tilde hh^​0​+h~, with h^t=ht+12κ∫Gt(y,⋅)ρ(dy)\hat{\mathfrak h}_t=\mathfrak h_t+\frac1{2\sqrt\kappa}\int G_t(y,\cdot)\rho(dy)h^​t​=ht​+2κ​1​∫Gt​(y,⋅)ρ(dy).
  2. Proposition 5.4. Under e(h0,ρ)Γe^{(h^0,\rho)}\Gammae(h0,ρ)Γ, the zipper is the modified SLE of Theorem 4.5.
  3. Proposition 1.6. Zooming in at a νh\nu_hνh​-typical boundary point gives a γ\gammaγ-quantum wedge.
  4. Proposition 1.7. The γ\gammaγ-wedge is stationary under shifting the origin by a fixed quantum length.
  5. Lemma 5.6. Sampling xxx from νh[−δ,0]\nu_h[-\delta,0]νh​[−δ,0] under Γ\GammaΓ turns the zipper into SLEκ,ρ\mathrm{SLE}_{\kappa,\rho}SLEκ,ρ​ with ρ=γ2δx−γ2σ0,1\rho=\gamma^2\delta_x-\gamma^2\sigma_{0,1}ρ=γ2δx​−γ2σ0,1​.
  6. Theorem 1.8, length clause. On a (γ−2/γ)(\gamma-2/\gamma)(γ−2/γ)-quantum wedge with an independent SLEγ2\mathrm{SLE}_{\gamma^2}SLEγ2​, the quantum lengths of the two sides of the curve agree.

Significance

Theorem 1.3 says that reverse SLE zipping is a welding by quantum length. Combined with the removability of SLEκ\mathrm{SLE}_\kappaSLEκ​ for κ<4\kappa<4κ<4, it gives Theorem 1.4: the field hhh determines the curve ηT\eta_TηT​. The same equality of boundary lengths on the two sides of an SLE is the defining property of the quantum-zipper and mating-of-trees constructions, which build random surfaces by welding wedges together.

All results here are proved in the paper, and none has a machine-checked proof. The proofs are partly sketches: Proposition 5.5 ends with a limiting estimate, and the zero–one step of Theorem 1.8 is delegated to [DMS14a, Lemma 8.2]. A formal development would therefore check the most cited welding argument in random conformal geometry. The definitions it needs (arc averages of a GFF, νh\nu_hνh​, quantum wedges, conditionally Gaussian fields) are reusable for any LQG statement.

Difficulty

The obvious argument tries to compare the left and right boundary measures directly, ball by ball along the curve. It fails because the two measures depend on the field near the curve in the same way (5.1): nothing local distinguishes them, and nothing local forces them to agree. The paper instead builds a stationary picture (Lemma 5.6, Proposition 5.5, Figure 1.7). It shows that the curve splits a (γ−2/γ)(\gamma-2/\gamma)(γ−2/γ)-wedge into two independent γ\gammaγ-wedges, and it uses the ergodic theorem with scale invariance to force the ratio of the two lengths to be a constant ccc, which symmetry makes equal to 111. The last step transfers the result from the wedge to the field of Theorem 1.3 by absolute continuity. Every step uses Gaussian conditioning on random conformal images of the field, which current libraries lack.

Formalization scope

Conventions committed to in Lean:

  • Time is R≥0\mathbb R_{\ge0}R≥0​, and Brownian motion is Mathlib's IsBrownianReal. Flows are pathwise ODE solutions, with no stochastic integrals.
  • A field is a random map Ψ(ω,μ)=(h,μ)\Psi(\omega,\mu)=(h,\mu)Ψ(ω,μ)=(h,μ) on admissible measures: finite, bounded support in H\mathbb HH, finite logarithmic energy. Its law is given in characteristic-function form, as "conditionally Gaussian given G\mathcal GG with mean mmm and covariance CCC". The arc averages hε(z)=(h,σz,ε)h_\varepsilon(z)=(h,\sigma_{z,\varepsilon})hε​(z)=(h,σz,ε​) are continuous in (z,ε)(z,\varepsilon)(z,ε).
  • Additive constants are fixed by h1(0)=0h_1(0)=0h1​(0)=0 (semicircle of radius 111), the paper's normalization (5.9).
  • νh\nu_hνh​ and μh\mu_hμh​ are predicates: the a.s. vague limits along 2−n2^{-n}2−n with locally integrable densities. The measure ν≡0\nu\equiv0ν≡0 cannot satisfy them vacuously, and the sanity file proves that adding CCC to the field multiplies ν\nuν by eγC/2e^{\gamma C/2}eγC/2.
  • The points z±z_\pmz±​ are encoded by radial boundary limits of fTf_TfT​. "Agree in law" means equality of the laws of all pairings, and convergence of random surfaces means convergence of the finite-dimensional laws of ∫f dμcan\int f\,d\mu^{\mathrm{can}}∫fdμcan.
  • Γ\GammaΓ is encoded by its restriction to (h0,(ft)t≥0)(h^0,(f_t)_{t\ge0})(h0,(ft​)t≥0​). The forward SLE of Theorem 1.8 is the platform definition OAI.SLEExactGauge.IsOrdinaryChordalSLE.

Disclosed readings of the text:

  • "α<0\alpha<0α<0" in (1.10) is read as α<Q\alpha<Qα<Q.
  • The force set C\mathcal CC of Theorem 4.5 lies in H‾\overline{\mathbb H}H.
  • Proposition 5.4 uses the measure 2κ ρ2\sqrt\kappa\,\rho2κ​ρ in (4.4)–(4.6).
  • The "unit circle" of Lemma 5.6 is the upper unit semicircle.
  • γ=0\gamma=0γ=0 is excluded in Proposition 1.6.

Contributions are welcome on any of the following:

  • existence of the predicates (νh\nu_hνh​, wedges, Γ\GammaΓ);
  • Gaussian conditioning on conformal images;
  • the Itô computations behind Theorem 4.5;
  • the milestones themselves.

Selected references

  • S. Sheffield, Conformal weldings of random surfaces: SLE and the quantum gravity zipper, Ann. Probab. 44(5), 2016. https://arxiv.org/abs/1012.4797 (v2), https://doi.org/10.1214/15-AOP1055
  • B. Duplantier, S. Sheffield, Liouville quantum gravity and KPZ, Invent. Math. 185, 2011. https://arxiv.org/abs/0808.1560
  • S. Rohde, O. Schramm, Basic properties of SLE, Ann. of Math. 161, 2005. https://arxiv.org/abs/math/0106036
  • P. Jones, S. Smirnov, Removability theorems for Sobolev functions and quasiconformal maps, Ark. Mat. 38, 2000. https://doi.org/10.1007/BF02384490
  • B. Duplantier, J. Miller, S. Sheffield, Liouville quantum gravity as a mating of trees, Astérisque 427, 2021. https://arxiv.org/abs/1409.7055
  • S. Sheffield, Gaussian free fields for mathematicians, Probab. Theory Related Fields 139, 2007. https://arxiv.org/abs/math/0312099
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AnalysisDynamical SystemsStochastic Systems·Captain: mikedeng1

On Well-Posedness of Forward–Backward SDEs—A Unified Approach 3: With Constant Coefficients, σ₃ ≠ 0, σ₃h ≠ 1 the Dominating ODE Keeps y and (1 − σ₃y)⁻¹ Bounded for Every T Iff One of Four Cases HoldsResearch Paper

Motivation

A forward–backward stochastic differential equation (FBSDE) couples a forward diffusion XXX with a backward equation for a pair (Y,Z)(Y,Z)(Y,Z) whose terminal value depends on XTX_TXT​. Such systems arise from the stochastic maximum principle, from option pricing with large investors, and from stochastic differential games. Whether an FBSDE with Lipschitz coefficients has a unique solution on an arbitrary horizon [0,T][0,T][0,T] is a classical question: small-time solvability is easy, but global solvability can fail even for linear equations.

J. Ma, Z. Wu, D. Zhang and J. Zhang, On well-posedness of forward–backward SDEs—a unified approach (arXiv:1110.4658v2, Ann. Appl. Probab. 25 (2015)), reduce well-posedness to the existence of bounded solutions of two deterministic dominating ordinary differential equations, obtained from the difference quotients of the coefficients. For linear FBSDEs with constant coefficients the two dominating ODEs coincide, and the authors give sharp criteria for global solvability. This mission formalizes the criterion in the case σ3≠0\sigma_3\neq0σ3​=0, where the dominating ODE has a rational right-hand side with a pole.

Earlier global results for coupled FBSDEs rested on the four-step scheme (Ma–Protter–Yong 1994) or on monotonicity conditions (Hu–Peng 1995); §7.4 of the paper compares the dominating-ODE approach with these methods.

Setting

The linear FBSDE (4.1) with constant coefficients is determined by nine reals b1,b2,b3,σ1,σ2,σ3,f1,f2,f3b_1,b_2,b_3,\sigma_1,\sigma_2,\sigma_3,f_1,f_2,f_3b1​,b2​,b3​,σ1​,σ2​,σ3​,f1​,f2​,f3​ and a terminal slope hhh. Its dominating function is (3.9),

F(y)=f1+f2y+y(b1+b2y)+(f3+b3y) y (σ1+σ2y)1−σ3y,F(y)=f_1+f_2y+y(b_1+b_2y)+\frac{(f_3+b_3y)\,y\,(\sigma_1+\sigma_2y)}{1-\sigma_3y},F(y)=f1​+f2​y+y(b1​+b2​y)+1−σ3​y(f3​+b3​y)y(σ1​+σ2​y)​,

defined for y≠1/σ3y\neq1/\sigma_3y=1/σ3​. When σ3≠0\sigma_3\neq0σ3​=0 it can be rewritten as (5.8),

F(y)=α01/σ3−y+α1+α2y+α3y2,α3=b2−b3σ2σ3,F(y)=\frac{\alpha_0}{1/\sigma_3-y}+\alpha_1+\alpha_2y+\alpha_3y^2,\qquad \alpha_3=b_2-\frac{b_3\sigma_2}{\sigma_3},F(y)=1/σ3​−yα0​​+α1​+α2​y+α3​y2,α3​=b2​−σ3​b3​σ2​​,

for constants α0,α1,α2\alpha_0,\alpha_1,\alpha_2α0​,α1​,α2​. The dominating ODE (5.3) is the backward integral equation

yt=h+∫tTF(ys) ds,t∈[0,T].y_t=h+\int_t^TF(y_s)\,ds,\qquad t\in[0,T].yt​=h+∫tT​F(ys​)ds,t∈[0,T].

The paper needs a solution satisfying (5.9): both yyy and (1−σ3y)−1(1-\sigma_3y)^{-1}(1−σ3​y)−1 are bounded on [0,T][0,T][0,T]. Since yT=hy_T=hyT​=h, this forces σ3h≠1\sigma_3h\neq1σ3​h=1 (Remark 5.5).

The comparison tool is Lemma 5.1. For measurable F0,F1,F2F^0,F^1,F^2F0,F1,F2 it gives a unique solution of yt0=h0+∫tTF0(s,ys0) dsy^0_t=h^0+\int_t^TF^0(s,y^0_s)\,dsyt0​=h0+∫tT​F0(s,ys0​)ds lying between a sub-solution y1y^1y1 and a super-solution y2y^2y2 of perturbed equations (5.2).

Formalization targets

Goal: Theorem 5.6 (corrected)

For σ3≠0\sigma_3\neq0σ3​=0 and hσ3≠1h\sigma_3\neq1hσ3​=1, the ODE (5.3) has a solution satisfying (5.9) for every T>0T>0T>0 if and only if one of the following holds:

  1. h<1/σ3h<1/\sigma_3h<1/σ3​, F(h)≤0F(h)\le0F(h)≤0, and FFF has a zero in (−∞,h](-\infty,h](−∞,h] or α3=0\alpha_3=0α3​=0;
  2. h>1/σ3h>1/\sigma_3h>1/σ3​, F(h)≥0F(h)\ge0F(h)≥0, and FFF has a zero in [h,∞)[h,\infty)[h,∞) or α3=0\alpha_3=0α3​=0;
  3. h<1/σ3h<1/\sigma_3h<1/σ3​, F(h)≥0F(h)\ge0F(h)≥0, and FFF has a zero in [h,1/σ3)[h,1/\sigma_3)[h,1/σ3​) or F(y)→0F(y)\to0F(y)→0 as y↑1/σ3y\uparrow1/\sigma_3y↑1/σ3​;
  4. h>1/σ3h>1/\sigma_3h>1/σ3​, F(h)≤0F(h)\le0F(h)≤0, and FFF has a zero in (1/σ3,h](1/\sigma_3,h](1/σ3​,h] or F(y)→0F(y)\to0F(y)→0 as y↓1/σ3y\downarrow1/\sigma_3y↓1/σ3​.

The limit alternatives in cases 3 and 4 are not printed in the paper. Without them the equivalence is false. Take σ3=1\sigma_3=1σ3​=1, f1=1f_1=1f1​=1, f2=−1f_2=-1f2​=−1, all other coefficients 000, and h=0h=0h=0. Then F(y)=1−yF(y)=1-yF(y)=1−y, and yt=1−et−Ty_t=1-e^{t-T}yt​=1−et−T satisfies (5.9) on every horizon, yet none of the printed cases holds. The gap is in the Appendix (p. 48): it asserts that FFF is positive on the closed interval [h,σ3−1][h,\sigma_3^{-1}][h,σ3−1​] when α0=0\alpha_0=0α0​=0, which fails when the polynomial part vanishes at the pole. A companion item records the counterexample.

Milestones

The milestones follow the paper's proof:

  • the decomposition (5.8);
  • the comparison Lemma 5.1;
  • the three sufficiency arguments of p. 23 (case (i) with a zero, case (i) with α3=0\alpha_3=0α3​=0, case (iii));
  • the necessity bounds of the Appendix:
    • in case (i): a zero exists when α3>0\alpha_3>0α3​>0, and F(y)≤−ε(h+1−y)2F(y)\le-\varepsilon(h+1-y)^2F(y)≤−ε(h+1−y)2 when α3<0\alpha_3<0α3​<0 and there is no zero;
    • in case (iii): a zero exists when α0<0\alpha_0<0α0​<0, and F(y)≥ε(σ3−1−y)−1F(y)\ge\varepsilon(\sigma_3^{-1}-y)^{-1}F(y)≥ε(σ3−1​−y)−1 when α0>0\alpha_0>0α0​>0 and there is no zero;
  • the comparison with the explicit solution (σ3−1−y~t)2=(σ3−1−h)2−2ε(T−t)(\sigma_3^{-1}-\tilde y_t)^2=(\sigma_3^{-1}-h)^2-2\varepsilon(T-t)(σ3−1​−y~​t​)2=(σ3−1​−h)2−2ε(T−t);
  • the case α0=0\alpha_0=0α0​=0, with the endpoint positivity made a hypothesis.

Significance

In the paper, Theorem 5.6 is the sharp solvability criterion for linear FBSDEs with constant coefficients and σ3≠0\sigma_3\neq0σ3​=0. The paper describes these sharp conditions as setting the "limits" for the solvability of general FBSDEs, and the nonlinear Theorems 5.9–5.11 and the main well-posedness Theorem 7.4 are modelled on them. Because the criterion is an equivalence, it also says when no regular decoupling field can be built from the dominating ODE, whatever the horizon.

The result is proved in the paper, but the printed statement is not correct as an equivalence (see above). The mission states and asks for a corrected version, a machine-checked counterexample to the printed one, and formal versions of each step of the proof. The deterministic parts (comparison for backward integral equations, finite-time blow-up of scalar autonomous ODEs, pole-reaching for rational vector fields) are basic real analysis with no current Lean library. They are reusable well beyond FBSDEs. No part of this paper has a machine-checked proof.

Difficulty

Each sufficiency case is an a priori bound: a comparison with a constant or explicitly solvable equation keeps the solution in a fixed interval away from the pole. The difficulty is on the necessity side, where three kinds of failure must be excluded:

  • blow-up to ±∞\pm\infty±∞ when α3≠0\alpha_3\neq0α3​=0 has the wrong sign;
  • reaching the pole in finite time when α0>0\alpha_0>0α0​>0;
  • reaching the pole when α0=0\alpha_0=0α0​=0.

The obvious argument for the last case, "FFF is bounded below by a positive constant up to the pole", is exactly what fails when FFF tends to 000 at the pole. There the solution approaches the pole only asymptotically, and the right criterion is the corrected one above. A second subtlety is that FFF is only locally Lipschitz off the pole, so comparison must be carried out on a band in which the solution provably stays.

Formalization scope

Time is real, with 0≤t≤T0\le t\le T0≤t≤T and T>0T>0T>0. The coefficients form a record Coeffs of nine reals, and Coeffs.F is (3.9) verbatim. A solution on [0,T][0,T][0,T] is a function y:R→Ry:\mathbb R\to\mathbb Ry:R→R such that, for every t∈[0,T]t\in[0,T]t∈[0,T], the integrand s↦F(ys)s\mapsto F(y_s)s↦F(ys​) is integrable on [t,T][t,T][t,T] and yt=h+∫tTF(ys) dsy_t=h+\int_t^TF(y_s)\,dsyt​=h+∫tT​F(ys​)ds; values outside [0,T][0,T][0,T] are irrelevant. Condition (5.9) is a uniform bound on ∣y∣|y|∣y∣ together with ∣1−σ3yt∣≥κ|1-\sigma_3y_t|\ge\kappa∣1−σ3​yt​∣≥κ for some κ>0\kappa>0κ>0. "For arbitrary TTT" is a universal quantifier over T>0T>0T>0 outside the existential.

Lean's conventions are total, so several trivializing formalizations are ruled out explicitly:

  • Lean's integral of a non-integrable function is 000, so integrability is part of the solution predicate.
  • Lean's x/0=0x/0=0x/0=0 gives Coeffs.F a junk value at the pole. No statement evaluates FFF there: every zero point, bound and limit in the statements lives strictly on one side of 1/σ31/\sigma_31/σ3​.
  • (5.9) is never encoded as a bound on the Lean inverse (1−σ3y)−1(1-\sigma_3y)^{-1}(1−σ3​y)−1, which is 000 at the pole.
  • σ3≠0\sigma_3\neq0σ3​=0 is assumed wherever α3\alpha_3α3​ or 1/σ31/\sigma_31/σ3​ appears.
  • Lemma 5.1 adds the hypothesis y1≤y2y^1\le y^2y1≤y2, without which it is false, and asks the cic^ici to be integrable.

The constants α0,α1,α2\alpha_0,\alpha_1,\alpha_2α0​,α1​,α2​ of (5.8) enter the necessity milestones only through the decomposition hypothesis, never through a formula.

The development needs a Picard–Lindelöf or comparison argument for backward scalar integral equations with locally Lipschitz right-hand sides, monotonicity of autonomous scalar solutions, and the intermediate value theorem. Contributions of a general comparison lemma for scalar integral equations would serve this mission and both other missions of the series.

Selected references

  • J. Ma, Z. Wu, D. Zhang, J. Zhang, On well-posedness of forward–backward SDEs—a unified approach, Ann. Appl. Probab. 25(4):2168–2214, 2015. arXiv:1110.4658v2, doi:10.1214/14-AAP1046
  • J. Ma, P. Protter, J. Yong, Solving forward–backward stochastic differential equations explicitly—a four step scheme, Probab. Theory Related Fields 98:339–359, 1994. doi:10.1007/BF01192258
  • Y. Hu, S. Peng, Solution of forward–backward stochastic differential equations, Probab. Theory Related Fields 103:273–283, 1995. doi:10.1007/BF01204218
  • J. Ma, J. Yong, Forward–Backward Stochastic Differential Equations and Their Applications, Lecture Notes in Math. 1702, Springer, 1999. doi:10.1007/978-3-540-48831-6
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Functional AnalysisNumerical AnalysisOptimization·Captain: mikedeng1

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

Motivation

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

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

Setting

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

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

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

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

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

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

Formalization targets

Goal: Theorem 4.4 (p. 12)

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

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

where ⇀\rightharpoonup⇀ is weak convergence in HHH.

Milestones

In the order the proof uses them:

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

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

Significance

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

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

Difficulty

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

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

Formalization scope

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

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

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

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

Selected references

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

Synchronization via Pinning Control on General Complex Networks II: Componentwise LMIs on the Strongly Connected Components Globally Synchronize a Pinned Network with a Directed Spanning TreeResearch Paper

Motivation

Networks of identical dynamical systems coupled along a directed graph model power grids, sensor and robot swarms, neural populations and coupled oscillators. A basic control question is how to steer every node of such a network onto a prescribed reference trajectory by acting directly on only a few nodes. This is pinning control: feedback is injected at a small set of pinned vertices, and the coupling has to carry the reference signal to the rest of the network.

For undirected or strongly connected networks, criteria for pinning synchronization go back to Wang and Chen (2002) and Chen, Liu and Lu (2007), and the first mission of this series treats the strongly connected case of Yu, Chen, Lü and Kurths (2013). Many networks of interest are not strongly connected: information flows down a hierarchy of groups, and the minimal requirement for the reference to reach every node is that the network, with the reference added as a virtual leader, contains a directed spanning tree rooted at the leader. Section 4 of that paper gives a criterion for this general case that splits into one condition per strongly connected component. This mission formalizes that criterion, Theorem 4.5, with the lemmas its proof uses and three corollaries.

Setting

There are NNN vertices with states xi(t)∈Rnx_i(t)\in\mathbb R^nxi​(t)∈Rn. The coupling configuration matrix G∈RN×NG\in\mathbb R^{N\times N}G∈RN×N has Gij≥0G_{ij}\ge0Gij​≥0 for i≠ji\ne ji=j, where Gij>0G_{ij}>0Gij​>0 records a connection from vertex jjj to vertex iii, and zero row sums, Gii=−∑j≠iGijG_{ii}=-\sum_{j\ne i}G_{ij}Gii​=−∑j=i​Gij​. Given a function f:Rn×R+→Rnf:\mathbb R^n\times\mathbb R_+\to\mathbb R^nf:Rn×R+​→Rn, a coupling strength ccc, an inner coupling matrix Γ∈Rn×n\Gamma\in\mathbb R^{n\times n}Γ∈Rn×n and pinning gains di≥0d_i\ge0di​≥0 (vertex iii is pinned when di>0d_i>0di​>0), the controlled network is

x˙i=f(xi,t)+c∑j=1NGijΓxj−c di Γ(xi−s),i=1,…,N,\dot x_i=f(x_i,t)+c\sum_{j=1}^N G_{ij}\Gamma x_j-c\,d_i\,\Gamma(x_i-s),\qquad i=1,\dots,N,x˙i​=f(xi​,t)+cj=1∑N​Gij​Γxj​−cdi​Γ(xi​−s),i=1,…,N,

where the reference sss solves s˙=f(s,t)\dot s=f(s,t)s˙=f(s,t). The network is globally synchronized when xi(t)−s(t)→0x_i(t)-s(t)\to0xi​(t)−s(t)→0 for every vertex and every pair of solutions.

The nonlinearity is controlled by Assumption 1: there is a matrix KKK with (x−y)T(f(x,t)−f(y,t))≤(x−y)TKΓ(x−y)(x-y)^{\mathsf T}(f(x,t)-f(y,t))\le(x-y)^{\mathsf T}K\Gamma(x-y)(x−y)T(f(x,t)−f(y,t))≤(x−y)TKΓ(x−y) for all x,yx,yx,y and t≥0t\ge0t≥0. Throughout §4 the paper also assumes that KKK and Γ\GammaΓ commute, that Γ\GammaΓ is positive definite, and puts θ=λmax⁡((K+KT)/2)≥0\theta=\lambda_{\max}((K+K^{\mathsf T})/2)\ge0θ=λmax​((K+KT)/2)≥0.

The vertices split into strongly connected components V1,…,VMV_1,\dots,V_MV1​,…,VM​. In the Frobenius normal form the components are ordered so that no edge goes from a later component to an earlier one, which makes GGG block lower triangular. For each component jjj the mission uses three matrices:

  • G~j\widetilde G_jGj​, the diagonal block of G−diag(d)G-\mathrm{diag}(d)G−diag(d) on VjV_jVj​;
  • AjA_jAj​, the within-component part of GGG with zero row sums;
  • Π~j=diag(Πj)\widetilde\Pi_j=\mathrm{diag}(\Pi_j)Πj​=diag(Πj​), where Πj\Pi_jΠj​ is a positive vector with ΠjTAj=0\Pi_j^{\mathsf T}A_j=0ΠjT​Aj​=0.

In Lean, component membership is a map blk : Fin N → Fin M, and Fin M carries the Frobenius order.

Formalization targets

Goal: Theorem 4.5

If, for every component jjj,

2θΠ~j+c(Π~jG~j+G~jTΠ~j)<0,(4.8)2\theta\widetilde\Pi_j+c\bigl(\widetilde\Pi_j\widetilde G_j+\widetilde G_j^{\mathsf T}\widetilde\Pi_j\bigr)<0, \tag{4.8}2θΠj​+c(Πj​Gj​+GjT​Πj​)<0,(4.8)

then the controlled network with a directed spanning tree is globally synchronized.

Milestones

  1. The θ bound (p. 1402). Commutation and Γ>0\Gamma>0Γ>0 turn Assumption 1 into (x−y)T(f(x,t)−f(y,t))≤θ(x−y)TΓ(x−y)(x-y)^{\mathsf T}(f(x,t)-f(y,t))\le\theta(x-y)^{\mathsf T}\Gamma(x-y)(x−y)T(f(x,t)−f(y,t))≤θ(x−y)TΓ(x−y).
  2. Lemma 2.13. The strict Schur complement test for a symmetric block matrix.
  3. Lemma 4.4. If Π~jG~j+G~jTΠ~j<0\widetilde\Pi_j\widetilde G_j+\widetilde G_j^{\mathsf T}\widetilde\Pi_j<0Πj​Gj​+GjT​Πj​<0 on every diagonal block of a block lower-triangular G‾\overline GG, then positive block weights Δj\Delta_jΔj​ exist with ΔΠ~G‾+G‾TΠ~Δ<0\Delta\widetilde\Pi\overline G+\overline G^{\mathsf T}\widetilde\Pi\Delta<0ΔΠG+GTΠΔ<0.
  4. (4.10). Along solutions, V=∑jΔje~jTΠ~je~jV=\sum_j\Delta_j\widetilde e_j^{\mathsf T}\widetilde\Pi_j\widetilde e_jV=∑j​Δj​ejT​Πj​ej​ satisfies V˙≤eT{[ΔΠ~(cG‾+θIN)+(cG‾+θIN)TΠ~Δ]⊗Γ}e\dot V\le e^{\mathsf T}\{[\Delta\widetilde\Pi(c\overline G+\theta I_N)+(c\overline G+\theta I_N)^{\mathsf T}\widetilde\Pi\Delta]\otimes\Gamma\}eV˙≤eT{[ΔΠ(cG+θIN​)+(cG+θIN​)TΠΔ]⊗Γ}e.

Companions

  • Corollary 4.7: the same conclusion under θΠ~j+c(A‾j−Π~jCj−Π~jD‾j)<0\theta\widetilde\Pi_j+c(\overline A_j-\widetilde\Pi_jC_j-\widetilde\Pi_j\overline D_j)<0θΠj​+c(Aj​−Πj​Cj​−Πj​Dj​)<0, which separates the outer in-degrees CjC_jCj​ from the pinning gains D‾j\overline D_jDj​.
  • Corollary 4.8 (i): an explicit coupling-strength threshold under Assumption 2.
  • Corollary 4.9: partial synchronization of the first components.

Significance

Theorem 4.5 replaces a single Nn×NnNn\times NnNn×Nn matrix inequality for the whole network with MMM inequalities, one of the size of each component. In practice the test runs component by component down the Frobenius order: decide which components need pinning, choose gains for each one separately, and get synchronization of the whole network. Corollary 4.7 makes this explicit in terms of the outer in-degrees: a component with no incoming edges from earlier components has to be pinned (Remark 4), while a component that receives enough weight from upstream needs no control. These conditions underlie the pinning scheme algorithm of §5 of the paper.

On the formal side, as far as a search of the platform and of Mathlib shows, none of these results is machine-checked. Mathlib has the positive semidefinite Schur complement and irreducible nonnegative matrices, but not the strict Schur complement, block-diagonal Lyapunov scaling, or Lyapunov arguments for networked ODEs with Kronecker-structured couplings. The mission produces, beyond the paper's theorem:

  • a reusable strict Schur complement lemma;
  • a block-triangular diagonal-stability lemma;
  • a template for Lyapunov estimates on coupled networks in Lean.

Difficulty

The obvious argument is to take one Lyapunov function weighted by a positive left null vector of the whole coupling matrix, as in the strongly connected case. Here it fails: the coupling matrix of a network that is not strongly connected has no positive left null vector, and condition (4.8) is local to each component. The central step is the passage from blockwise to global negative definiteness (Lemma 4.4). Condition (4.8) says nothing about the off-diagonal blocks that couple a component to earlier ones, and a block lower-triangular matrix whose symmetrized diagonal blocks are negative definite need not have a negative definite symmetric part; the component weights Δj\Delta_jΔj​ have to be found so that those couplings are dominated, which is a quantitative statement about Schur complements. Turning the resulting matrix inequality into convergence of the trajectories then needs a differential inequality on [0,∞)[0,\infty)[0,∞), a Kronecker-product definiteness argument with Γ\GammaΓ, and the commutation of KKK and Γ\GammaΓ to reach the θ bound.

Formalization scope

States are Fin n → ℝ and matrices are indexed by Fin N, Fin n, or the subtype of one component's vertices. Solutions are functions on ℝ that satisfy their ODE on [0,∞)[0,\infty)[0,∞) through HasDerivWithinAt … (Set.Ici 0). "For any initial conditions" means for every pair of solutions (s,x)(s,x)(s,x); existence of solutions is not claimed. Convergence is componentwise, which agrees with every norm on Rn\mathbb R^nRn. "Positive definite" is Mathlib's Matrix.PosDef, which includes symmetry, and X<0X<0X<0 is (-X).PosDef. λmax⁡\lambda_{\max}λmax​ is the least Rayleigh bound, IsLamMax, never a supremum of a possibly empty set.

The vertices are not permuted into Frobenius form. The hypotheses say instead that:

  • every component is nonempty;
  • every component is strongly connected inside itself;
  • every edge between components points forward in the order;
  • every vertex is reachable from a pinned vertex.

The weights Πj\Pi_jΠj​ are tied to the paper's object by ΠjTAj=0\Pi_j^{\mathsf T}A_j=0ΠjT​Aj​=0. The standing assumptions of p. 1402 (Assumption 1, KΓ=ΓKK\Gamma=\Gamma KKΓ=ΓK, θ=λmax⁡((K+KT)/2)≥0\theta=\lambda_{\max}((K+K^{\mathsf T})/2)\ge0θ=λmax​((K+KT)/2)≥0, Γ>0\Gamma>0Γ>0) are hypotheses of every goal-level statement. The goal does not assume the weights Δj\Delta_jΔj​, the bound (4.10), or definiteness of a whole-network matrix; it assumes only (4.8) on each component, so it cannot be trivialized by assuming its own conclusion. For n=0n=0n=0 the λmax⁡\lambda_{\max}λmax​ hypothesis cannot be met, so that degenerate dimension is excluded.

The pages contain three misprints. (4.10) has "−c-c−c" in its third line and "++++++" in its last; the last line, with a single +++, is formalized. Corollary 4.9 ranges "i=1,…,Ni=1,\dots,Ni=1,…,N" where the component range is meant.

A complete development needs a Gronwall-type decay lemma on [0,∞)[0,\infty)[0,∞), the strict Schur complement, definiteness of Kronecker products, and the square root of a positive definite matrix commuting with matrices that commute with it. Each of these is reusable well beyond this mission, and contributions to any of them are welcome, as are proofs of the milestones in any order.

Selected references

  • W. Yu, G. Chen, J. Lü, J. Kurths, Synchronization via pinning control on general complex networks, SIAM J. Control Optim. 51(2) (2013), 1395–1416. https://doi.org/10.1137/100781699
  • X. F. Wang, G. Chen, Pinning control of scale-free dynamical networks, Physica A 310 (2002), 521–531. https://doi.org/10.1016/S0378-4371(02)00772-0
  • T. Chen, X. Liu, W. Lu, Pinning complex networks by a single controller, IEEE Trans. Circuits Syst. I 54(6) (2007), 1317–1326. https://doi.org/10.1109/TCSI.2007.895383
  • S. Boyd, L. El Ghaoui, E. Feron, V. Balakrishnan, Linear Matrix Inequalities in System and Control Theory, SIAM, 1994. https://doi.org/10.1137/1.9781611970777
  • R. A. Brualdi, H. J. Ryser, Combinatorial Matrix Theory, Cambridge University Press, 1991. https://doi.org/10.1017/CBO9781107325708
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CombinatoricsGraph TheoryProbability+1·Captain: mikedeng1

A Proof of the Block Model Threshold Conjecture: If s² > d, a Labelling of G(n, a/n, b/n) Correlated with the Planted Partition Can Be Found Asymptotically Almost SurelyResearch Paper

Motivation

The stochastic block model is the basic random-graph model of a network with communities. It serves as a test bed for clustering algorithms in statistics, machine learning and theoretical computer science. In its sparse two-community form, each vertex has a constant expected degree, and the question is how much of the hidden partition a graph reveals. Using the cavity method of statistical physics, Decelle, Krzakala, Moore and Zdeborová (arXiv:1109.3041, 2011) conjectured a sharp threshold: one can label the vertices better than chance when the signal-to-noise ratio s2/ds^2/ds2/d exceeds one, and not otherwise.

Timeline:

  • 2011. Decelle, Krzakala, Moore and Zdeborová state the threshold conjecture, from belief propagation and the stability of its fixed point.
  • 2012. Mossel, Neeman and Sly prove the impossibility half: for s2≤ds^2\le ds2≤d no estimator is correlated with the planted partition. They also show that s2=ds^2=ds2=d is the threshold for distinguishing the model from an Erdős–Rényi graph (arXiv:1202.1499).
  • 2013. Krzakala, Moore, Mossel, Neeman, Sly, Zdeborová and Zhang propose spectral algorithms based on the non-backtracking matrix (arXiv:1306.5550).
  • 2013–2015. Mossel, Neeman and Sly prove the achievability half (arXiv:1311.4115, the source of this mission), with an algorithm built from counts of non-backtracking paths. Massoulié independently gives a different proof via self-avoiding path counts (arXiv:1311.3085).

Setting

Fix a,b>0a,b>0a,b>0 and let nnn be the number of vertices. In G(n,a/n,b/n)\mathcal G(n,a/n,b/n)G(n,a/n,b/n) every vertex uuu receives, independently and uniformly, a label σu∈{+1,−1}\sigma_u\in\{+1,-1\}σu​∈{+1,−1}. Then each unordered pair {u,v}\{u,v\}{u,v} is an edge independently, with probability a/na/na/n if σu=σv\sigma_u=\sigma_vσu​=σv​ and b/nb/nb/n otherwise. Write

d=a+b2,s=a−b2,d=\frac{a+b}{2},\qquad s=\frac{a-b}{2},d=2a+b​,s=2a−b​,

for the average degree and the signal strength; sss may be negative.

An estimator τ^\hat\tauτ^ receives only the graph GGG and outputs a labelling, possibly at random. Its overlap with the planted labelling is ∣1n∑vσvτ^v∣\bigl|\frac1n\sum_v\sigma_v\hat\tau_v\bigr|​n1​∑v​σv​τ^v​​, with an absolute value because the two communities carry no names. A uniformly random guess has overlap of order n−1/2n^{-1/2}n−1/2.

The proof works with paths γ=(u0,…,uk)\gamma=(u_0,\dots,u_k)γ=(u0​,…,uk​) in the complete graph: consecutive vertices distinct. A path is non-backtracking if ui≠ui+2u_i\ne u_{i+2}ui​=ui+2​ and self-avoiding if all its vertices are distinct. With We=1e∈E(G)−d/nW_e=\mathbf 1_{e\in E(G)}-d/nWe​=1e∈E(G)​−d/n and Xγ=∏iW{ui−1,ui}X_\gamma=\prod_iW_{\{u_{i-1},u_i\}}Xγ​=∏i​W{ui−1​,ui​}​, the path sums Nu,v(k)N^{(k)}_{u,v}Nu,v(k)​ and Yu,vY_{u,v}Yu,v​ add XγX_\gammaXγ​ over the non-backtracking, respectively self-avoiding, paths of length kkk from uuu to vvv. An ℓ\ellℓ-tangle is a connected subgraph of diameter at most 2ℓ2\ell2ℓ that contains two cycles.

Formalization targets

Goal: Theorem 2.1

For fixed a,b>0a,b>0a,b>0 with s2>ds^2>ds2>d there are an estimator τ^\hat\tauτ^ and an ε>0\varepsilon>0ε>0 with

lim⁡n→∞P[∣1n∑vσvτ^v∣≥ε]=1.\lim_{n\to\infty}\mathbb P\Bigl[\Bigl|\frac1n\sum_v\sigma_v\hat\tau_v\Bigr|\ge\varepsilon\Bigr]=1 .n→∞lim​P[​n1​v∑​σv​τ^v​​≥ε]=1.

The goal fixes neither ε\varepsilonε nor the algorithm, so it is the weakest form of the conjecture.

Companions

  • Theorem 2.2: the same conclusion for slowly growing an,bn=no(1/log⁡log⁡n)a_n,b_n=n^{o(1/\log\log n)}an​,bn​=no(1/loglogn) with sn2/dn≥λ>1s_n^2/d_n\ge\lambda>1sn2​/dn​≥λ>1.
  • Theorem 2.3: recovery of all but o(n)o(n)o(n) vertices when sn2/dn→∞s_n^2/d_n\to\inftysn2​/dn​→∞.

Milestones

  • Claim 4.3 and Lemma 4.7: counting paths by their new, old and returning steps and by their tangles.
  • Lemma 5.1 for m=1m=1m=1: the expected weight of a self-avoiding path or simple cycle is exactly σuσvsz/nz\sigma_u\sigma_vs^z/n^zσu​σv​sz/nz.
  • Lemma 6.2: the graph is ℓ\ellℓ-tangle-free with probability 1−n−1+o(1)1-n^{-1+o(1)}1−n−1+o(1).
  • Theorem 2.8 (1)–(4): the first and second moments of Yu,vY_{u,v}Yu,v​, the decorrelation of path sums for disjoint pairs, and the closeness of Nu,v(k)N^{(k)}_{u,v}Nu,v(k)​ to Yu,vY_{u,v}Yu,v​.
  • Lemma 3.5: the aggregate path sum between two small vertex sets.
  • Lemma 3.7: on the Poisson(ddd) Galton–Watson tree whose labels are copied along each edge with probability a/(a+b)a/(a+b)a/(a+b) and flipped otherwise, the depth-RRR label sum ΨR+\Psi^+_RΨR+​ of a tree with root label +1+1+1 satisfies P[ΨR+≥ξκsR]≥12+2ε\mathbb P[\Psi^+_R\ge\xi\kappa s^R]\ge\tfrac12+2\varepsilonP[ΨR+​≥ξκsR]≥21​+2ε for an independent uniform ξ\xiξ on [−1,1][-1,1][−1,1] and all large RRR.

Significance

Together with the impossibility result for s2≤ds^2\le ds2≤d, Theorem 2.1 establishes s2=ds^2=ds2=d as the detection threshold of the sparse two-community block model, a threshold first predicted by statistical physics. It equals the Kesten–Stigum bound for reconstruction on the Poisson Galton–Watson tree with the Ising channel, which locally describes the model. The non-backtracking and self-avoiding path statistics behind it led to the later spectral analyses of the non-backtracking matrix and to the multi-community theory.

The theorem is proved on paper. As far as is known, none of its ingredients is machine-checked: no formal statement of the block model, of path-count moments in sparse random graphs, or of tangle-freeness exists in Mathlib. The mission produces a faithful statement of the threshold theorem together with the first-moment, second-moment and combinatorial estimates the proof rests on. These can be attacked independently.

Difficulty

The obvious approach estimates σuσv\sigma_u\sigma_vσu​σv​ by the sign of the number of length-kkk paths between uuu and vvv, with k≈αlog⁡nk\approx\alpha\log nk≈αlogn. Its mean is right: it is of order sk/ns^k/nsk/n. Its variance is not under control. With probability about n−m2n^{-m^2}n−m2 a clique of size mmm appears near uuu and vvv, and on that event the number of paths is so large that the expectation is dominated by a rare configuration. A plain second-moment argument therefore fails. The rare dense structures (tangles) must be excluded by conditioning, and the non-backtracking count must be compared with the self-avoiding one, whose moments can be computed. Even then, the second moment determines σuσv\sigma_u\sigma_vσu​σv​ only with probability bounded away from 1/21/21/2. Turning many weakly correlated pairwise estimates into a globally correlated labelling is a separate step close to the threshold, where s2/ds^2/ds2/d is barely above one.

Formalization scope

Everything is a finite sum. Vertices are Fin n, graphs SimpleGraph (Fin n), labellings Fin n → Bool. The joint law of (σ,G)(\sigma,G)(σ,G) is written as an explicit weight. Conditioning on the labels of a vertex set UUU is a weighted average with positive denominator 2−∣U∣2^{-|U|}2−∣U∣. An estimator is a map from graphs to PMFs on labellings, so it never sees σ\sigmaσ and may be randomized. Its success probability is the probability that the overlap, with absolute value, is at least ε\varepsilonε, for an ε\varepsilonε fixed before nnn.

Asymptotic notation follows §1.3 of the paper. n−1+o(1)n^{-1+o(1)}n−1+o(1) is n−1+cnn^{-1+c_n}n−1+cn​ for an explicit cn→0c_n\to0cn​→0 chosen before the vertices, sets and labellings it is uniform over. "Sets of size no(1)n^{o(1)}no(1)" in a hypothesis means: for every en→0e_n\to0en​→0, all sets of size at most nenn^{e_n}nen​. Assumption 2.7 (s,d=no(1/log⁡log⁡n)s,d=n^{o(1/\log\log n)}s,d=no(1/loglogn) and log⁡log⁡n≪ℓ≪log⁡n\log\log n\ll\ell\ll\sqrt{\log n}loglogn≪ℓ≪logn​) and the preamble of Theorem 2.8 (s2/d≥λ>1s^2/d\ge\lambda>1s2/d≥λ>1, the choice of α\alphaα, k=⌈αlog⁡n⌉k=\lceil\alpha\log n\rceilk=⌈αlogn⌉) are shared definitions, so the four displays of Theorem 2.8 cannot drift apart. Non-asymptotic statements assume 0<a,b<n0<a,b<n0<a,b<n, which is Definition 1.1's q,q′∈(0,1)q,q'\in(0,1)q,q′∈(0,1).

Three printed slips are corrected and disclosed. Theorem 2.8 (2) carries the square (s2/(s2−d))2(s^2/(s^2-d))^2(s2/(s2−d))2 that the proof's display (17) gives. Theorem 2.8 (4) uses ∣s∣k|s|^k∣s∣k, since sss may be negative. Lemma 4.7 assumes distinct endpoints, as all its uses do.

The labelled branching tree of Lemma 3.7 is encoded by its generation counts: the numbers of +1+1+1 and −1-1−1 labelled vertices at depth rrr form a two-type Poisson chain on N2\mathbb N^2N2, which has the same law by Poisson thinning and superposition. Lemma 3.7 assumes s>0s>0s>0, the standing assumption of its section, and is stated for all sufficiently large RRR, the range its proof covers.

The statements rule out the trivial readings: the estimator cannot see σ\sigmaσ, the overlap carries its absolute value, ε\varepsilonε does not depend on nnn, antecedent o(1)o(1)o(1) bounds are universally quantified, and the model's weights are genuine probabilities for all large nnn.

Reusable infrastructure includes the finite-sum stochastic block model, path edge-type counts, and tangle-freeness. The weights of independent-edge random graphs and the Poisson Galton–Watson tree with the Ising broadcast are also of independent use. Contributions are welcome on any milestone, on infrastructure lemmas such as normalisation of the model's weights and independence of distinct edges given the labels, and on the steps of §3 that connect Theorem 2.8 to the goal.

Selected references

  • E. Mossel, J. Neeman, A. Sly, A Proof of the Block Model Threshold Conjecture, arXiv:1311.4115v4, 2015. https://arxiv.org/abs/1311.4115
  • E. Mossel, J. Neeman, A. Sly, Reconstruction and Estimation in the Planted Partition Model, Probab. Theory Related Fields 162 (2015). https://arxiv.org/abs/1202.1499
  • A. Decelle, F. Krzakala, C. Moore, L. Zdeborová, Asymptotic analysis of the stochastic block model for modular networks and its algorithmic applications, Phys. Rev. E 84 (2011). https://arxiv.org/abs/1109.3041
  • F. Krzakala, C. Moore, E. Mossel, J. Neeman, A. Sly, L. Zdeborová, P. Zhang, Spectral redemption in clustering sparse networks, PNAS 110 (2013). https://arxiv.org/abs/1306.5550
  • L. Massoulié, Community detection thresholds and the weak Ramanujan property, STOC 2014. https://arxiv.org/abs/1311.3085
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