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Dynamic ProgrammingProbabilityReinforcement Learning·Captain: mikedeng1

Global Optimality Guarantees for Policy Gradient Methods 5: The Effective Concentrability Coefficient Is at Most 1/min ρ(s), ‖dη_π*/dρ‖∞, or C/cResearch Paper

Motivation

Policy gradient methods optimize a parameterized policy for a Markov decision process by local search on its expected cost. The objective is nonconvex, so local search can in principle stall at a poor stationary point. Bhandari and Russo, Global Optimality Guarantees for Policy Gradient Methods show that for a broad family of control problems this does not happen, and, in quantitative form, that the objective is gradient dominated: its suboptimality is bounded by a multiple of the size of its gradient. The multiple involves a single problem-dependent quantity, the effective concentrability coefficient κρ\kappa_\rhoκρ​, which measures how well the initial state distribution ρ\rhoρ covers the states that matter for optimal behaviour. Theorem 2 and the convergence rates of Theorem 5 of the paper are only informative when κρ\kappa_\rhoκρ​ is finite, so sufficient conditions for a finite κρ\kappa_\rhoκρ​ are what make those results usable. This mission formalizes the paper's three such conditions (Theorem 4).

Distribution-mismatch coefficients of this kind go back to Kakade and Langford (2002), and appear in the analyses of approximate dynamic programming by Scherrer and Geist (2014) and of policy gradient methods in finite MDPs by Agarwal et al. (2021).

Setting

A discounted Markov decision process consists of a measurable state space S\mathcal SS, nonempty feasible action sets As\mathcal A_sAs​, a bounded measurable per-period cost g(s,a)g(s,a)g(s,a), a transition kernel P(⋅∣s,a)P(\cdot\mid s,a)P(⋅∣s,a), a discount factor γ∈(0,1)\gamma\in(0,1)γ∈(0,1) and an initial probability distribution ρ\rhoρ on S\mathcal SS. A feasible measurable stationary policy π\piπ (π∈Π\pi\in\Piπ∈Π) picks an action π(s)∈As\pi(s)\in\mathcal A_sπ(s)∈As​ in every state. Its cost-to-go Jπ(s)J_\pi(s)Jπ​(s) is the expected discounted cost from sss, its discounted state-occupancy measure is

ηπ(⋅)=(1−γ)∑t≥0γt Pr⁡ρπ(st∈⋅),\eta_\pi(\cdot)=(1-\gamma)\sum_{t\ge0}\gamma^t\,\Pr{}^\pi_\rho(s_t\in\cdot),ηπ​(⋅)=(1−γ)t≥0∑​γtPrρπ​(st​∈⋅),

and its average cost is ℓ(π)=(1−γ)∫Jπ dρ\ell(\pi)=(1-\gamma)\int J_\pi\,d\rhoℓ(π)=(1−γ)∫Jπ​dρ. The Bellman operator acts on bounded measurable functions by

(TJ)(s)=min⁡a∈As[g(s,a)+γ∫J(s′) P(ds′∣s,a)].(TJ)(s)=\min_{a\in\mathcal A_s}\Big[g(s,a)+\gamma\int J(s')\,P(ds'\mid s,a)\Big].(TJ)(s)=a∈As​min​[g(s,a)+γ∫J(s′)P(ds′∣s,a)].

An optimal policy π∗\pi^*π∗ minimizes JπJ_\piJπ​ at every state; J∗=Jπ∗J^*=J_{\pi^*}J∗=Jπ∗​. A policy class ΠΘ={πθ:θ∈Θ}\Pi_\Theta=\{\pi_\theta:\theta\in\Theta\}ΠΘ​={πθ​:θ∈Θ} is indexed by a convex set Θ⊆Rd\Theta\subseteq\mathbb R^dΘ⊆Rd, and JΘ={Jπθ:θ∈Θ}\mathcal J_\Theta=\{J_{\pi_\theta}:\theta\in\Theta\}JΘ​={Jπθ​​:θ∈Θ}.

The effective concentrability coefficient κρ\kappa_\rhoκρ​ (Definition 3) is the smallest scalar κ\kappaκ such that

∥J−J∗∥1,ρ≤κ1−γ ∥J−TJ∥1,ρ∀J∈JΘ,(13)\|J-J^*\|_{1,\rho}\le\frac{\kappa}{1-\gamma}\,\|J-TJ\|_{1,\rho}\qquad\forall J\in\mathcal J_\Theta,\tag{13}∥J−J∗∥1,ρ​≤1−γκ​∥J−TJ∥1,ρ​∀J∈JΘ​,(13)

with ∥J∥1,ρ=∫∣J∣ dρ\|J\|_{1,\rho}=\int|J|\,d\rho∥J∥1,ρ​=∫∣J∣dρ, and κρ=∞\kappa_\rho=\inftyκρ​=∞ if no scalar works. It converts a ρ\rhoρ-weighted Bellman error into a ρ\rhoρ-weighted optimality gap.

Formalization targets

Goal: Theorem 4(b)

If ηπ∗(B)≤Cρ(B)\eta_{\pi^*}(B)\le C\rho(B)ηπ∗​(B)≤Cρ(B) for every measurable set BBB, then CCC satisfies (13); equivalently

κρ≤∥dηπ∗dρ∥∞.\kappa_\rho\le\Big\|\frac{d\eta_{\pi^*}}{d\rho}\Big\|_\infty .κρ​≤​dρdηπ∗​​​∞​.

Companions: Theorem 4(a) and 4(c)

(a) If S\mathcal SS is finite and ρ(s)>0\rho(s)>0ρ(s)>0 for all sss, then κρ≤1/min⁡sρ(s)\kappa_\rho\le 1/\min_{s}\rho(s)κρ​≤1/mins​ρ(s). (c) If TTT is a contraction with modulus γ\gammaγ in a norm ∥⋅∥\|\cdot\|∥⋅∥ with c∥J∥≤∥J∥1,ρ≤C∥J∥c\|J\|\le\|J\|_{1,\rho}\le C\|J\|c∥J∥≤∥J∥1,ρ​≤C∥J∥, then κρ≤C/c\kappa_\rho\le C/cκρ​≤C/c.

Milestones

The element-wise inequalities TJ⪯TπJTJ\preceq T_\pi JTJ⪯Tπ​J, TJπ⪯JπTJ_\pi\preceq J_\piTJπ​⪯Jπ​ (5); the performance difference identity ℓ(π)−ℓ(πˉ)=∫[TπJπˉ−Jπˉ] dηπ\ell(\pi)-\ell(\bar\pi)=\int[T_\pi J_{\bar\pi}-J_{\bar\pi}]\,d\eta_\piℓ(π)−ℓ(πˉ)=∫[Tπ​Jπˉ​−Jπˉ​]dηπ​ (29); the sup-norm bound ∥Jπ−J∗∥∞≤(1−γ)−1∥Jπ−TJπ∥∞\|J_\pi-J^*\|_\infty\le(1-\gamma)^{-1}\|J_\pi-TJ_\pi\|_\infty∥Jπ​−J∗∥∞​≤(1−γ)−1∥Jπ​−TJπ​∥∞​ (26); the occupancy-weighted inequality (1−γ)∫(Jπ−J∗) dρ≤∫(Jπ−TJπ) dηπ∗(1-\gamma)\int(J_\pi-J^*)\,d\rho\le\int(J_\pi-TJ_\pi)\,d\eta_{\pi^*}(1−γ)∫(Jπ​−J∗)dρ≤∫(Jπ​−TJπ​)dηπ∗​ from the proof of part (b); and the contraction step ∥J−J∗∥≤(1−γ)−1∥J−TJ∥\|J-J^*\|\le(1-\gamma)^{-1}\|J-TJ\|∥J−J∗∥≤(1−γ)−1∥J−TJ∥ from the proof of part (c).

Significance

Theorem 4 is what turns the paper's gradient-dominance theorem into a usable statement: with part (b), the constant in Theorem 2 is bounded by the worst-case likelihood ratio between the optimal policy's state distribution and the initial distribution, a quantity that can be checked without knowing the policy class. Part (a) shows that in finite problems any fully supported initial distribution suffices, and part (c) gives a route through weighted norms, used in the paper for optimal stopping (Lemma 13).

The results are proved in the paper. None of them is machine-checked. The mission produces a general-state-space formalization of the discounted cost MDP (kernels, occupancy measures, Bellman operators, measurable selection) together with the performance difference identity on measurable state spaces; existing formal developments of policy gradient theory on the platform are for finite MDPs only. The occupancy-measure and Bellman-operator layer is shared with the other missions of this series.

Difficulty

The argument for part (b) is short on paper, but each step is a measure-theoretic statement about infinite-horizon objects. The performance difference identity (29) exchanges an infinite discounted sum with integration against the chain's laws and needs the occupancy measure to be built from the ttt-step kernels of the controlled chain. The change of measure from ηπ∗\eta_{\pi^*}ηπ∗​ to ρ\rhoρ needs the Bellman error Jπ−TJπJ_\pi-TJ_\piJπ​−TJπ​ to be nonnegative and integrable; its measurability is not automatic, because TJTJTJ is a pointwise minimum over uncountably many actions, and is supplied by the measurable selection assumption. Part (c) needs the fixed-point property TJ∗=J∗TJ^*=J^*TJ∗=J∗ of the optimal cost-to-go, which again rests on measurable selection.

Formalization scope

All statements use one Lean layer: MDP S A with measurable spaces S, A (a generalization of the paper's Borel subsets of Euclidean spaces), the cost and kernel given on all of S×A\mathcal S\times\mathcal AS×A, measurable stationary policies MPolicy S A, and costToGo, occupancy, loss, bellmanPi, bellmanOpt. The paper prints the Bellman operators (3)–(4) without the discount factor; every later use includes it, and so does the formalization. The optimal policy is a binder πstar with IsOptimal M πstar. Assumptions 1 and 2 of the paper are standing hypotheses of every main statement.

The coefficient κρ\kappa_\rhoκρ​ is never formed as a number: "κρ≤X\kappa_\rho\le Xκρ​≤X" is the predicate IsConcBound M Θ πθ πstar X, which says that XXX satisfies (13); because the right-hand side of (13) is nondecreasing in the scalar, the two are equivalent. Part (b) quantifies over every CCC with ηπ∗≤Cρ\eta_{\pi^*}\le C\rhoηπ∗​≤Cρ setwise, which is equivalent to ∥dηπ∗/dρ∥∞≤C\|d\eta_{\pi^*}/d\rho\|_\infty\le C∥dηπ∗​/dρ∥∞​≤C; a real-valued essential supremum is avoided because it reads 000 exactly when the paper's bound is infinite. Part (a) assumes ρ(s)>0\rho(s)>0ρ(s)>0 for every state, since otherwise 1/min⁡ρ1/\min\rho1/minρ is +∞+\infty+∞ on paper and 000 in Lean. Part (c) requires the norm comparison (21) on all bounded measurable functions, as its proof uses it on J−J∗J-J^*J−J∗ and J−TJJ-TJJ−TJ, and encodes "a norm" by subadditivity, the one property used.

A formalization in which (13) or the occupancy-weighted inequality is assumed, or in which κρ\kappa_\rhoκρ​ is a junk value of an empty infimum, would make the goal trivial; neither is used.

Contributions are welcome on every milestone, in particular on the performance difference identity and the measurability of the cost-to-go and of TJTJTJ, which are reusable for any discounted MDP on a measurable state space.

Selected references

  • J. Bhandari, D. Russo, Global Optimality Guarantees for Policy Gradient Methods, Operations Research, 2024; cited version arXiv:1906.01786v3, 2022. https://arxiv.org/abs/1906.01786v3 (DOI 10.1287/opre.2021.0014)
  • S. Kakade, J. Langford, Approximately Optimal Approximate Reinforcement Learning, ICML 2002. https://dl.acm.org/doi/10.5555/645531.656005
  • B. Scherrer, M. Geist, Local Policy Search in a Convex Space and Conservative Policy Iteration as Boosted Policy Search, ECML PKDD 2014. https://arxiv.org/abs/1306.1520
  • A. Agarwal, S. Kakade, J. Lee, G. Mahajan, On the Theory of Policy Gradient Methods: Optimality, Approximation, and Distribution Shift, JMLR 22, 2021. https://arxiv.org/abs/1908.00261
  • D. Bertsekas, Dynamic Programming and Optimal Control, Athena Scientific, 1995.
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Dynamic ProgrammingOptimizationReinforcement Learning·Captain: mikedeng1

Global Optimality Guarantees for Policy Gradient Methods 4: In Finite-Horizon Problems with a Non-Stationary Policy Class Containing an Optimal Policy, Every Stationary Point Is OptimalResearch Paper

Motivation

Policy gradient methods optimize a parameterized policy by gradient descent on its expected total cost. They are a staple of reinforcement learning and of simulation-based optimization in operations research, but the objective is nonconvex in the policy parameters, and the standard theory guarantees convergence only to a stationary point. J. Bhandari and D. Russo (arXiv:1906.01786v3, Operations Research, 2024, DOI 10.1287/opre.2021.0014) identify structural conditions under which every stationary point is globally optimal.

Their first result (Theorem 1) requires the policy class to be closed under policy improvement. That excludes many classes used in practice, where it is known only that some member of the class is optimal: base-stock policies in finite-horizon inventory control are the standard example (Bertsekas, Dynamic Programming and Optimal Control, 1995). For stationary policy classes, containing an optimal policy is not enough: the paper's Example 1 has a policy class that contains the optimal policy, and policy gradient still gets stuck in a bad local minimum. Theorem 3 shows that for finite-horizon problems with a non-stationary policy class (separate parameters for each period), containing an optimal policy suffices, together with a single-period regularity condition imposed only at the optimal cost-to-go. This mission formalizes Theorem 3.

Setting

A Markov decision process consists of a state space S\mathcal SS, nonempty feasible action sets As\mathcal A_sAs​, a bounded measurable cost g(s,a)g(s,a)g(s,a), a transition kernel P(⋅∣s,a)P(\cdot\mid s,a)P(⋅∣s,a), a discount factor γ∈(0,1)\gamma\in(0,1)γ∈(0,1) and an initial distribution ρ\rhoρ. A policy is a measurable map π\piπ with π(s)∈As\pi(s)\in\mathcal A_sπ(s)∈As​; Π\PiΠ is the set of all of them. The cost-to-go is Jπ(s)=Esπ[∑t≥0γtg(st,π(st))]J_\pi(s)=\mathbb E^\pi_s[\sum_{t\ge0}\gamma^t g(s_t,\pi(s_t))]Jπ​(s)=Esπ​[∑t≥0​γtg(st​,π(st​))], the loss is ℓ(π)=(1−γ)∫Jπ dρ\ell(\pi)=(1-\gamma)\int J_\pi\,d\rhoℓ(π)=(1−γ)∫Jπ​dρ, and the discounted state-occupancy measure is ηπ=(1−γ)∑t≥0γtPρπ(st∈⋅)\eta_\pi=(1-\gamma)\sum_{t\ge0}\gamma^tP^\pi_\rho(s_t\in\cdot)ηπ​=(1−γ)∑t≥0​γtPρπ​(st​∈⋅). An optimal policy π∗\pi^*π∗ has Jπ∗≤JπJ_{\pi^*}\le J_\piJπ∗​≤Jπ​ pointwise for all π∈Π\pi\in\Piπ∈Π; J∗=Jπ∗J^*=J_{\pi^*}J∗=Jπ∗​. With the Bellman operator (TπJ)(s)=g(s,π(s))+γ∫J(s′)P(ds′∣s,π(s))(T_\pi J)(s)=g(s,\pi(s))+\gamma\int J(s')P(ds'\mid s,\pi(s))(Tπ​J)(s)=g(s,π(s))+γ∫J(s′)P(ds′∣s,π(s)), the weighted policy-iteration objective is

B(πˉ∣η,J)=∫(TπˉJ)(s) η(ds).\mathcal B(\bar\pi\mid\eta,J)=\int (T_{\bar\pi}J)(s)\,\eta(ds).B(πˉ∣η,J)=∫(Tπˉ​J)(s)η(ds).

A parameterized policy class is ΠΘ={πθ:θ∈Θ}\Pi_\Theta=\{\pi_\theta:\theta\in\Theta\}ΠΘ​={πθ​:θ∈Θ} for a convex Θ⊆Rd\Theta\subseteq\mathbb R^dΘ⊆Rd, and ℓ(θ)=ℓ(πθ)\ell(\theta)=\ell(\pi_\theta)ℓ(θ)=ℓ(πθ​). A point θ∈Θ\theta\in\Thetaθ∈Θ is stationary for min⁡Θf\min_\Theta fminΘ​f if fff is differentiable at θ\thetaθ and ⟨∇f(θ),θ′−θ⟩≥0\langle\nabla f(\theta),\theta'-\theta\rangle\ge0⟨∇f(θ),θ′−θ⟩≥0 for all θ′∈Θ\theta'\in\Thetaθ′∈Θ.

The finite-horizon structure (Condition 3) embeds a time-inhomogeneous problem in this discounted formulation: the states split into stages S1,…,SH,SH+1\mathcal S_1,\dots,\mathcal S_H,\mathcal S_{H+1}S1​,…,SH​,SH+1​; from a state in Sh\mathcal S_hSh​, h≤Hh\le Hh≤H, every feasible action leads to Sh+1\mathcal S_{h+1}Sh+1​; and SH+1={τ}\mathcal S_{H+1}=\{\tau\}SH+1​={τ} is a costless absorbing state. The parameter is a concatenation θ=(θ1,…,θH)\theta=(\theta_1,\dots,\theta_H)θ=(θ1​,…,θH​), the parameter set is a product Θ=Θ1×⋯×ΘH\Theta=\Theta_1\times\cdots\times\Theta_HΘ=Θ1​×⋯×ΘH​, and on Sh\mathcal S_hSh​ the action πθ(s)\pi_\theta(s)πθ​(s) depends only on θh\theta_hθh​. The stage objectives are Bh(θˉh∣η,J)=∫Sh(TπθˉJ) dη\mathcal B_h(\bar\theta_h\mid\eta,J)=\int_{\mathcal S_h}(T_{\pi_{\bar\theta}}J)\,d\etaBh​(θˉh​∣η,J)=∫Sh​​(Tπθˉ​​J)dη.

Condition 4 asks that for every η∈{ηπ:π∈ΠΘ}\eta\in\{\eta_\pi:\pi\in\Pi_\Theta\}η∈{ηπ​:π∈ΠΘ​}, the problem min⁡θ∈ΘB(θ∣η,J∗)\min_{\theta\in\Theta}\mathcal B(\theta\mid\eta,J^*)minθ∈Θ​B(θ∣η,J∗) has no suboptimal stationary points. Assumption 3 asks that ηπ≪ρ\eta_\pi\ll\rhoηπ​≪ρ for every π∈ΠΘ\pi\in\Pi_\Thetaπ∈ΠΘ​. Condition 0 asks that the policy-iteration objective be continuously differentiable in the parameters.

Formalization targets

Goal: Theorem 3 (p. 17)

Under Conditions 0, 3 and 4 and Assumption 3, if πθ∗\pi_{\theta^*}πθ∗​ is an optimal policy for some θ∗∈Θ\theta^*\in\Thetaθ∗∈Θ, then every stationary point θ\thetaθ of ℓ\ellℓ on Θ\ThetaΘ satisfies

ℓ(πθ)=ℓ(π∗).\ell(\pi_\theta)=\ell(\pi^*).ℓ(πθ​)=ℓ(π∗).

Milestones

  1. Lemma 6 (policy gradient theorem): ∇ℓ(θ)=∇θˉB(θˉ∣ηπθ,Jπθ)∣θˉ=θ\nabla\ell(\theta)=\nabla_{\bar\theta}\mathcal B(\bar\theta\mid\eta_{\pi_\theta},J_{\pi_\theta})|_{\bar\theta=\theta}∇ℓ(θ)=∇θˉ​B(θˉ∣ηπθ​​,Jπθ​​)∣θˉ=θ​.
  2. Lemma 17 (balance equation): ηπ(M)=∫[(1−γ)ρ(M)+γP(M∣s,π(s))] ηπ(ds)\eta_\pi(\mathcal M)=\int[(1-\gamma)\rho(\mathcal M)+\gamma P(\mathcal M\mid s,\pi(s))]\,\eta_\pi(ds)ηπ​(M)=∫[(1−γ)ρ(M)+γP(M∣s,π(s))]ηπ​(ds).
  3. The stage-wise balance equation: for M⊆Sh+1\mathcal M\subseteq\mathcal S_{h+1}M⊆Sh+1​, ηπ(M)=(1−γ)ρ(M)+γ∫ShP(M∣s,π(s)) ηπ(ds)\eta_\pi(\mathcal M)=(1-\gamma)\rho(\mathcal M)+\gamma\int_{\mathcal S_h}P(\mathcal M\mid s,\pi(s))\,\eta_\pi(ds)ηπ​(M)=(1−γ)ρ(M)+γ∫Sh​​P(M∣s,π(s))ηπ​(ds).
  4. Separability (30): θ\thetaθ minimizes B(⋅∣η,J)\mathcal B(\cdot\mid\eta,J)B(⋅∣η,J) over Θ\ThetaΘ iff each θh\theta_hθh​ minimizes Bh(⋅∣η,J)\mathcal B_h(\cdot\mid\eta,J)Bh​(⋅∣η,J) over Θh\Theta_hΘh​.
  5. Stage-wise stationarity (31): θ\thetaθ is stationary for ℓ\ellℓ iff each θh\theta_hθh​ is stationary for Bh(⋅∣ηπθ,Jπθ)\mathcal B_h(\cdot\mid\eta_{\pi_\theta},J_{\pi_\theta})Bh​(⋅∣ηπθ​​,Jπθ​​) on Θh\Theta_hΘh​.
  6. Lemma 1: π∈arg⁡min⁡Πℓ\pi\in\arg\min_{\Pi}\ellπ∈argminΠ​ℓ iff Jπ=J∗J_\pi=J^*Jπ​=J∗ ρ\rhoρ-almost surely.

Significance

Theorem 3 covers finite-horizon dynamic programs in which a structured class of time-varying policies is known to contain an optimal policy, but is not closed under policy improvement: the paper's Example 8, multi-period inventory control with base-stock policies, is the motivating case. Policy gradient on such a class has no suboptimal stationary points, so any method that finds a stationary point finds a globally optimal policy, optimal among all policies and not only within the class. Condition 4 involves only the Bellman objective of the optimal cost-to-go J∗J^*J∗, which often has regularity (for instance convexity) that the cost-to-go of an arbitrary policy lacks.

The result is proved in the paper. To our knowledge no part of it, nor the policy gradient theorem for deterministic policies on general state spaces, has a machine-checked proof. Formalizing it requires a measure-theoretic treatment of occupancy measures, the stage-wise decomposition of the weighted policy-iteration objective, and the backward induction of App. D.2.

Difficulty

The obvious approach reasons stage by stage directly on ℓ\ellℓ, but ℓ\ellℓ couples the stages: changing θh\theta_hθh​ changes the distribution of states visited after stage hhh. The paper's argument instead passes through the policy gradient theorem, which turns stationarity of ℓ\ellℓ into stationarity of single-period problems weighted by the occupancy measure of the current policy. These single-period problems involve JπθJ_{\pi_\theta}Jπθ​​, while Condition 4 speaks about J∗J^*J∗; relating them requires a backward induction over stages in which almost-sure equality Jπθ=J∗J_{\pi_\theta}=J^*Jπθ​​=J∗ on stage h+1h+1h+1 is transported to stage hhh through the balance equation. This step needs the occupancy measures of all policies in the class, including policies other than πθ\pi_\thetaπθ​, to be equivalent to ρ\rhoρ, which is where Assumption 3 enters. The naive variant with a stationary policy class fails (Example 1).

Formalization scope

The state and action spaces are arbitrary measurable spaces (the paper takes Borel subsets of Euclidean spaces; no argument uses that structure). Cost and kernel are given on all state-action pairs; the cost is bounded. Policies are deterministic, stationary and measurable; parameters live in EuclideanSpace ℝ (Fin d), so gradients and norms are Euclidean. J∗J^*J∗ is never defined as an infimum: an optimal policy π∗\pi^*π∗ is a hypothesis, with J∗=Jπ∗J^*=J_{\pi^*}J∗=Jπ∗​. Stages and sub-vectors are numbered from 111 by a measurable stage index and a block index on coordinates; the product structure of Θ\ThetaΘ is encoded as closure under exchanging one block.

Hypotheses beyond the printed sentence of Theorem 3, all disclosed in the item statements: Assumption 3 (announced on p. 17 as required, used in the proof); Condition 0 (needed for Lemma 6, which the proof invokes), in a joint form that the proof of Lemma 6 uses and that implies the printed partial-map form; the standing Assumptions 1 and 2 of §2; and, inside Condition 4, differentiability of θ↦B(θ∣η,J∗)\theta\mapsto\mathcal B(\theta\mid\eta,J^*)θ↦B(θ∣η,J∗) on Θ\ThetaΘ, the premise of Definition 1. The Bellman operators carry the factor γ\gammaγ omitted in the printed (3)–(4). The stage-wise balance equation is stated for h<Hh<Hh<H; the printed range h≤Hh\le Hh≤H fails at the absorbing state.

A formalization in which the goal assumes the stage-wise characterization (31), the balance equation, or Jπθ=J∗J_{\pi_\theta}=J^*Jπθ​​=J∗ on any stage is not Theorem 3; neither is one where "contains an optimal policy" means optimal only within ΠΘ\Pi_\ThetaΠΘ​. Stationarity includes differentiability, so a junk zero gradient never makes a point stationary.

Needed infrastructure: occupancy measures as series of iterated kernels and their balance equation, the cost-to-go as a bounded measurable function, the performance difference identity, the policy gradient theorem, and the decomposition of integrals over the stage partition. The occupancy-measure and policy gradient results are reusable for every mission of this series; contributions of these general lemmas are welcome.

Selected references

  • J. Bhandari, D. Russo, Global Optimality Guarantees for Policy Gradient Methods, arXiv:1906.01786v3, 2022; Operations Research, 2024. https://arxiv.org/abs/1906.01786 , https://doi.org/10.1287/opre.2021.0014
  • S. Kakade, J. Langford, Approximately Optimal Approximate Reinforcement Learning, ICML, 2002. https://dl.acm.org/doi/10.5555/645531.656005
  • I. Osband, B. Van Roy, D. Russo, Z. Wen, Deep Exploration via Randomized Value Functions, JMLR 20, 2019. https://jmlr.org/papers/v20/18-339.html
  • D. Silver, G. Lever, N. Heess, T. Degris, D. Wierstra, M. Riedmiller, Deterministic Policy Gradient Algorithms, ICML, 2014. https://proceedings.mlr.press/v32/silver14.html
  • D. P. Bertsekas, Dynamic Programming and Optimal Control, Athena Scientific, 1995. https://www.athenasc.com/dpbook.html
10 thms2 active usersReviewed
Dynamic ProgrammingOptimizationReinforcement Learning·Captain: mikedeng1

Global Optimality Guarantees for Policy Gradient Methods 3: Under Closure up to Inherent Bellman Error ε, Every Stationary Point Is Within κε/(1−γ) of OptimalResearch Paper

Why approximate closure matters

Policy gradient methods search for a policy by changing a finite vector of parameters. The method can reach a stationary point of its objective without finding an optimal policy: a small change in the available parameters might not represent the policy improvement that the underlying control problem calls for. Bhandari and Russo identify a condition on the policy class that limits this obstruction. Their exact-closure result rules out suboptimal stationary points; their approximate-closure result measures the residual cost when the class can represent policy improvements only approximately. This mission formalizes the latter statement, Theorem 5 of Bhandari and Russo, Global Optimality Guarantees for Policy Gradient Methods, using the arXiv v3 text and numbering.

The result concerns the optimization landscape rather than a particular gradient algorithm or convergence rate. It applies to structured policy classes in discounted control problems, including settings with general state spaces. The paper also discusses state aggregation as a source of small approximation error in Lemma 15; that example motivates the error condition, while the target here is the general guarantee of Theorem 5. The error is measured in the states visited by each current policy, so the condition describes what the restricted class can do where improvement affects that policy's performance.

The discounted control setting

A Markov decision process has a measurable state space SSS, a measurable action space AAA, and a nonempty feasible action set AsA_sAs​ at each state sss. Choosing a∈Asa\in A_sa∈As​ incurs a bounded cost g(s,a)g(s,a)g(s,a) and changes the state according to a probability kernel P(⋅∣s,a)P(\cdot\mid s,a)P(⋅∣s,a). A discount factor γ∈(0,1)\gamma\in(0,1)γ∈(0,1) reduces future costs, and an initial probability measure ρ\rhoρ specifies where evaluation begins. A stationary policy is a measurable choice π(s)∈As\pi(s)\in A_sπ(s)∈As​.

The cost-to-go Jπ(s)J_\pi(s)Jπ​(s) is the expected sum of discounted costs when starting at sss and following π\piπ. The discounted occupancy measure ηπ\eta_\piηπ​ is the normalized, discounted distribution of visited states when the initial state has law ρ\rhoρ. The policy's objective is ℓ(π)=(1−γ)∫Jπ dρ\ell(\pi)=(1-\gamma)\int J_\pi\,d\rhoℓ(π)=(1−γ)∫Jπ​dρ. The factor 1−γ1-\gamma1−γ puts ℓ\ellℓ on the scale of a per-period cost. An optimal policy π∗\pi^*π∗ minimizes cost-to-go at every state. Section 2, pp. 5–8 supplies these objects and Assumptions 1 and 2: absolute continuity of ηπ∗\eta_{\pi^*}ηπ∗​ with respect to ρ\rhoρ, and measurable selection of a Bellman-minimizing action for bounded measurable value functions.

A parameter θ\thetaθ belongs to a convex set Θ⊆Rd\Theta\subseteq\mathbb R^dΘ⊆Rd and determines a feasible policy πθ\pi_\thetaπθ​. The policy gradient objective is ℓ(θ)=ℓ(πθ)\ell(\theta)=\ell(\pi_\theta)ℓ(θ)=ℓ(πθ​). A stationary point is a feasible parameter with ⟨θ′−θ,∇ℓ(θ)⟩≥0\langle\theta'-\theta,\nabla\ell(\theta)\rangle\ge0⟨θ′−θ,∇ℓ(θ)⟩≥0 for every θ′∈Θ\theta'\in\Thetaθ′∈Θ. The Bellman optimality operator TTT selects the smallest one-step cost plus discounted future value among feasible actions. The weighted policy improvement objective B(θˉ∣ηπθ,Jπθ)B(\bar\theta\mid\eta_{\pi_\theta},J_{\pi_\theta})B(θˉ∣ηπθ​​,Jπθ​​) evaluates the one-step Bellman update from a candidate policy πθˉ\pi_{\bar\theta}πθˉ​, averaged under the current policy's occupancy measure. Section 5.1, pp. 12–14 introduces its smoothness and stationary-point conditions.

Formalization targets

The target is Theorem 5, p. 26. Condition 5 says the restricted class has inherent Bellman error ε≥0\varepsilon\ge0ε≥0: for each current policy in the class, a class member gets within ε\varepsilonε of the best one-step weighted Bellman objective over all feasible policies. Condition 2.A says stationary points of that weighted one-step objective are global minima over Θ\ThetaΘ. Condition 0 supplies differentiability. For a nonnegative coefficient κ\kappaκ satisfying the effective concentrability inequality (13), the goal is continuous differentiability of ℓ\ellℓ and, at every stationary point,

ℓ(πθ)−ℓ(π∗)≤κ1−γ ε.\ell(\pi_\theta)-\ell(\pi^*)\le\frac{\kappa}{1-\gamma}\,\varepsilon.ℓ(πθ​)−ℓ(π∗)≤1−γκ​ε.

The paper defines κρ\kappa_\rhoκρ​ as the least coefficient satisfying (13). The Lean statement quantifies over an admissible κ\kappaκ; its conclusion therefore includes the bound at κρ\kappa_\rhoκρ​ when that coefficient is finite. The milestone list follows the paper's supporting statements: occupancy domination after (2), Bellman inequalities (5), the performance difference identity (29), the policy gradient formula in Lemma 6, the stationary policy-improvement identity in Lemma 7, and the Bellman-error bound displayed in the proof of Theorem 5.

What the result establishes

The bound turns a property of the policy class into a quantitative guarantee about every stationary parameter. If ε=0\varepsilon=0ε=0 and a finite concentrability bound applies, the stated cost gap is zero. For positive error, it separates the approximation error from the factor κ/(1−γ)\kappa/(1-\gamma)κ/(1−γ) that reflects evaluation under the exploratory start distribution and the effective planning horizon. Thus a small gradient alone is not the claim; the structural conditions on the one-step objective and the policy class determine what stationarity means for long-run cost. Theorem 5 and its discussion, §8 make this interpretation explicit.

The paper proves Theorem 5. The declarations in this mission currently compile as open theorem statements; they are not machine-checked proofs. A complete development would formalize the links among discounted kernels, occupancy integrals, Bellman operators, and gradients on the parameter space. The general measurable-state MDP definitions would be reusable for other discounted control results, while the stationary-point and approximate-closure predicates provide a vocabulary for further policy-gradient theorems.

Where the difficulty lies

A stationary point of ℓ\ellℓ need not be a minimum of the one-step Bellman objective by definition. Condition 0 and Lemma 6 connect their gradients, and Condition 2.A then links stationary points to minima of the restricted one-step objective. Approximate closure only compares that restricted minimum with the unrestricted one up to ε\varepsilonε. The final result also requires moving an error measured under ηπθ\eta_{\pi_\theta}ηπθ​​ to one under ρ\rhoρ and relating Bellman residual to the optimality gap. Each comparison has a distinct measure or operator, and losing a discount factor changes the constant in the theorem.

Formalization scope

The Lean model uses arbitrary measurable spaces for SSS and AAA and measurable stationary policies, extending the paper's Borel-subset setting. The cost and kernel are defined on all S×AS\times AS×A and are uniformly bounded there; feasibility still restricts every policy and Bellman minimization to AsA_sAs​. These extensions let Condition 0 evaluate nearby parameter values even when their policies need not be feasible. The representation uses Mathlib kernels, measures, Bochner integrals, and Euclidean parameter vectors. It fixes 0<γ<10<\gamma<10<γ<1, a probability initial distribution, nonempty feasible action sets, an optimal policy, and the paper's Assumptions 1 and 2. The goal carries a nonnegative concentrability coefficient and Conditions 0, 2.A, and 5; it does not assume exact closure or the Bellman-error conclusion it is meant to establish.

Two corrections to the printed assumptions are explicit. The Bellman operators contain γ\gammaγ, consistently with equations (6) and (7), although displays (3) and (4) omit it. Condition 0 asks for joint continuous differentiability near the current parameter pair, the form used by the proof of Lemma 6; the printed condition lists two partial maps. The theorem's κ\kappaκ is constrained to be nonnegative to represent the paper's effective concentrability coefficient. Definitions use pointwise optimality rather than a real-valued infimum over policies, and Bellman minimization uses the nonempty feasible-action subtype. These choices prevent default values of ill-bounded infima or non-integrable functions from turning the target into an empty claim. The needed contributions are proofs of the six milestones and the final bound, plus supporting measurable-kernel and gradient facts.

Selected references

  • J. Bhandari and D. Russo, Global Optimality Guarantees for Policy Gradient Methods, Operations Research 72 (2024); preprint arXiv:1906.01786v3 (2022), arXiv, DOI.
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More Risk-Sensitive Markov Decision Processes 2: The Finite-Horizon Discounted Problem Is Solved by Value Iteration on the State Extended by Accumulated Cost and DiscountResearch Paper

Motivation

Sequential decisions often have costs whose timing matters. A controller may choose an action now, observe a random next state, and choose again. Ordinary expected-cost minimization averages the sum of the costs. A risk-sensitive criterion first applies an increasing function UUU to the total cost and then takes its expectation. The curvature of UUU changes how uncertain costs affect the ranking of policies: convex utility penalizes variability in a cost-minimization problem, while concave utility has the opposite tendency. Bäuerle and Rieder study this criterion for controlled Markov processes with general continuous increasing utility, rather than fixing an exponential function. Their finite-horizon discounted result is Theorem 3.6, pp. 10–12 of the authors' manuscript.

Discounting gives early and late costs different weights. For linear UUU, the remaining expected cost can be described using only the current physical state. For general UUU, the effect of a future cost also depends on what has already been paid and on the discount weight currently attached to the next cost. The mission targets the paper's finite-horizon treatment of these two additional quantities. The infinite-horizon problem is a separate part of the paper.

Setting

The state space EEE and action space AAA are Borel spaces. At state xxx, the nonempty set D(x)D(x)D(x) contains the actions that may be chosen. If action a∈D(x)a\in D(x)a∈D(x) is selected, the next state has distribution Q(⋅∣x,a)Q(\cdot\mid x,a)Q(⋅∣x,a) and the stage cost is c(x,a)c(x,a)c(x,a). The cost is measurable and bounded between positive constants c‾\underline cc​ and c‾\overline cc. The discount factor satisfies 0<β<10<\beta<10<β<1, and U:[0,∞)→RU:[0,\infty)\to\mathbb RU:[0,∞)→R is continuous and strictly increasing. The paper imposes its compactness and continuity conditions (CC) on UUU, DDD, ccc, and QQQ; these are stated in the model item and correspond to §2, pp. 3–4.

A history policy σ=(g0,g1,…)\sigma=(g_0,g_1,\ldots)σ=(g0​,g1​,…) chooses AnA_nAn​ measurably from the states and actions observed through time nnn. Starting from xxx, it induces a law for the state-action trajectory. The first nnn stages incur the discounted cost Cβn=∑k=0n−1βkc(Xk,Ak)C^n_\beta=\sum_{k=0}^{n-1}\beta^k c(X_k,A_k)Cβn​=∑k=0n−1​βkc(Xk​,Ak​), with Cβ0=0C^0_\beta=0Cβ0​=0. The paper minimizes Exσ[U(CβN)]E_x^\sigma[U(C^N_\beta)]Exσ​[U(CβN​)] over every admissible history policy. The inverse utility appearing in the paper's original certainty-equivalent criterion can be omitted when selecting a minimizer because UUU is strictly increasing §2, p. 3; §3.3, p. 10.

The extended state is E^=E×[0,∞)×(0,1]\hat E=E\times[0,\infty)\times(0,1]E^=E×[0,∞)×(0,1]. Its coordinates (x,y,z)(x,y,z)(x,y,z) record the current physical state, accumulated cost, and current discount weight. Define Vnσ(x,y,z)=Exσ[U(y+zCβn)]V_{n\sigma}(x,y,z)=E_x^\sigma[U(y+zC^n_\beta)]Vnσ​(x,y,z)=Exσ​[U(y+zCβn​)] and Vn=inf⁡σ∈ΠVnσV_n=\inf_{\sigma\in\Pi}V_{n\sigma}Vn​=infσ∈Π​Vnσ​. A measurable extended-state decision rule fff chooses an action in D(x)D(x)D(x). The paper's operator TfT_fTf​ integrates a continuation value at (x′,y+zc(x,f(x,y,z)),zβ)(x',y+zc(x,f(x,y,z)),z\beta)(x′,y+zc(x,f(x,y,z)),zβ); TTT takes the infimum of the same integral over D(x)D(x)D(x) equations (3.8)–(3.9), pp. 10–11.

Formalization targets

The first target identifies the cost iteration of any sequence of extended-state rules π=(f0,f1,…)\pi=(f_0,f_1,\ldots)π=(f0​,f1​,…):

Vnπ=Tf0⋯Tfn−1U,1≤n≤N.V_{n\pi}=T_{f_0}\cdots T_{f_{n-1}}U,\qquad 1\le n\le N.Vnπ​=Tf0​​⋯Tfn−1​​U,1≤n≤N.

The second target is the paper's value iteration for the infimum over all history policies, together with membership of every VnV_nVn​ in its regularity class C(E^)C(\hat E)C(E^):

V0(x,y,z)=U(y),Vn=TVn−1,Vn∈C(E^).V_0(x,y,z)=U(y),\qquad V_n=TV_{n-1},\qquad V_n\in C(\hat E).V0​(x,y,z)=U(y),Vn​=TVn−1​,Vn​∈C(E^).

The goal is Theorem 3.6(c): minimizers fk∗f_k^*fk∗​ of Vk−1V_{k-1}Vk−1​ exist, and their stage-dependent history rules attain the original objective JN(x)=VN(x,0,1)J_N(x)=V_N(x,0,1)JN​(x)=VN​(x,0,1) for every xxx. At stage n<Nn<Nn<N, the rule uses fN−n∗f_{N-n}^*fN−n∗​ at the current state, the observed sum ∑j<nβjc(Xj,Aj)\sum_{j<n}\beta^jc(X_j,A_j)∑j<n​βjc(Xj​,Aj​), and βn\beta^nβn. “Optimal” compares against all admissible history policies, including those that use more of the history than these three quantities.

Significance

Theorem 3.6 gives a finite sequence of minimum-operator evaluations for a problem whose utility of total cost is not additively separable in the physical state alone. Its policy statement also identifies which observable quantities an optimal controller needs to retain. Together, these results relate the original history-dependent problem to an extended-state Markov decision problem §3.3, pp. 10–12.

The paper proves these statements. This mission asks for machine-checked definitions and proofs of the finite-horizon discounted theorem, including the comparison with all admissible history policies. The model layer and the finite-dimensional expectation construction can support later formalizations of other risk-sensitive objectives. The mission itself has no completed proof at the drafting stage.

Difficulty

The extra discount coordinate is essential: after one action, the next cost enters utility with weight zβz\betazβ, not zzz. Keeping only accumulated cost would describe a different process. The other demanding point is the policy comparison. An iteration over extended-state decision rules has to establish the value of an infimum over arbitrary measurable history policies. Regularity and measurable selection must also be maintained at each step under (CC). The proof of Theorem 3.6 invokes the corresponding total-cost argument from Theorem 3.1, pp. 5–6; the formal development must supply the precise discounted version.

Formalization scope

Lean represents EEE and AAA as Borel subsets of Polish spaces, with standard Borel measurable structures. The controlled process is a separate reusable definition containing DDD, QQQ, and history policies; the risk-sensitive model adds ccc, β\betaβ, and UUU. The admissible graph is Borel and every section D(x)D(x)D(x) is nonempty. A history is a chronological finite list of earlier state-action pairs and a current state. Each rule is defined on all lists, but only admissible lists of the matching length are visited. The transition kernel is total as a Lean object, and its values outside DDD are irrelevant.

Policy values use nested kernel integrals representing the finite-dimensional marginals of the path law. They are defined from the cost and utility, so the Bellman recursion remains a theorem. The optimized value is an infimum over the subtype of measurable, admissible infinite history policies. The real infimum is meaningful here because this policy class is nonempty under (CC) and finite-horizon costs keep utility bounded on the relevant interval. The extended state uses real coordinates restricted to y≥0y\ge0y≥0 and 0<z≤10<z\le10<z≤1; its transition stays in that domain. “Increasing” in C(E^)C(\hat E)C(E^) means componentwise nondecreasing in (y,z)(y,z)(y,z). A minimizer is an admissible measurable rule satisfying Tfv=TvT_fv=TvTf​v=Tv on the entire extended domain.

The source's proof sentence that TTT preserves C(E^)C(\hat E)C(E^) is recorded with explicit integrability of each one-step continuation. For an arbitrary real-valued member of C(E^)C(\hat E)C(E^) on an unbounded state space, the source's conditions alone do not ensure a finite real expectation. This domain condition prevents Lean's zero value for a nonintegrable real integral from turning the assertion into a different one. It does not narrow the finite-horizon values appearing in the goal. Contributions toward finite-dimensional expectation identities, kernel integrability, the regularity of VnV_nVn​, and measurable minimizer selection are within scope.

Selected references

  • N. Bäuerle and U. Rieder, More Risk-Sensitive Markov Decision Processes, authors' manuscript, KIT repository 1000039663; published in Mathematics of Operations Research 39(1):105–120, 2014. Manuscript; DOI.
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Optimal Control of Markov Processes with Incomplete State Information 2: The Minimal Expected Cost Lies Between the Complete-Information and Open-Loop ValuesResearch Paper

Why observations matter in finite-horizon control

When a controller acts on a system whose state is hidden, measurements may help it choose later actions, but the value of those measurements depends on the transition law, the observation mechanism, and the available controls. Åström's 1965 paper gave a finite-state formulation of this problem and compared the best expected loss under incomplete measurements with two limiting cases: exact state observations and no useful observations. The comparison, stated in (5.12), quantifies the value of the information available to the controller without requiring a particular numerical example. Åström, 1965.

The bounds are useful when an exact partially observed policy is difficult to calculate. The complete-information problem provides an optimistic benchmark, because a controller that sees the hidden state can condition its decision on more information. The open-loop problem provides a conservative benchmark, because it commits to a control schedule without responding to later measurements. Both auxiliary problems have simpler backward equations than the partially observed problem, as Åström notes in §V of the paper. Åström, 1965, pp. 190–193.

Model and notation

The hidden state xtx_txt​ belongs to a finite nonempty set SSS, and the measured output yty_tyt​ belongs to a finite nonempty set YYY. There are N≥1N\ge1N≥1 decision stages. At stage ttt, a control u(t)u(t)u(t) is chosen from a nonempty compact set U⊆RdU\subseteq\mathbb R^dU⊆Rd. Given state iii and control u(t)u(t)u(t), the next state is jjj with probability pij(u(t),t+1)p_{ij}(u(t),t+1)pij​(u(t),t+1). At state iii, the observed output is jjj with probability qijq_{ij}qij​; observations are conditionally independent given the state path. The stage loss is g(u,i,t)g(u,i,t)g(u,i,t), with no fixed sign, terminal loss, or discount. The transition probabilities and loss are continuous in the control. Åström, 1965, §II.

An admissible control law may use the whole output history y1,…,yty_1,\ldots,y_ty1​,…,yt​ when choosing u(t)u(t)u(t). Write J(c)J(c)J(c) for its expected total loss, computed from the joint law of the state and output paths, and write OPT\mathrm{OPT}OPT for the infimum of J(c)J(c)J(c) over every such admissible law. The distribution of x1x_1x1​ is p1p_1p1​. After the first output η1\eta_1η1​, the belief w(1)w(1)w(1) is the conditional distribution of x1x_1x1​. More generally, w(t)w(t)w(t) is the conditional distribution of xtx_txt​ given outputs through time ttt, when that history has positive probability.

Three backward values describe the information regimes. The partial-observation value Vk(w)V_k(w)Vk​(w) obeys the Bayesian recursion (3.28). The complete-information value Vk′(w)V'_k(w)Vk′​(w) is the linear extension ∑iSk(i)wi\sum_i S_k(i)w_i∑i​Sk​(i)wi​ of the statewise recursion (5.4). The open-loop value Vk′′(w)V''_k(w)Vk′′​(w) obeys (5.7), in which the belief moves by prediction through P(u)P(u)P(u) without using an output. Each recursion has terminal value zero at N+1N+1N+1. Åström, 1965, pp. 184, 190–191.

Formalization targets

Theorem 2 identifies the partial-observation value with the original control problem: a selector attaining the minimum in (3.28) exists, and every such selector yields an admissible feedback law attaining OPT=Eη1V1(w(1))\mathrm{OPT}=\mathbb E_{\eta_1}V_1(w(1))OPT=Eη1​​V1​(w(1)). Theorem 4 gives the complete-information lower bound Vk′(w)≤Vk(w)V'_k(w)\le V_k(w)Vk′​(w)≤Vk​(w), and Theorem 5 gives the open-loop upper bound Vk(w)≤Vk′′(w)V_k(w)\le V''_k(w)Vk​(w)≤Vk′′​(w) for every probability belief and every stage 1≤k≤N1\le k\le N1≤k≤N. Both inequalities apply to a general observation matrix. Åström, 1965, Theorems 2, 4 and 5.

The goal is the paper's expected-cost comparison (5.12), with its middle term explicitly identified as the minimum of the original problem:

OPT=Eη1V1(w(1)),Eη1V1′(w(1))≤OPT≤Eη1V1′′(w(1)).\mathrm{OPT}=\mathbb E_{\eta_1}V_1(w(1)),\qquad \mathbb E_{\eta_1}V'_1(w(1))\le\mathrm{OPT}\le \mathbb E_{\eta_1}V''_1(w(1)).OPT=Eη1​​V1​(w(1)),Eη1​​V1′​(w(1))≤OPT≤Eη1​​V1′′​(w(1)).

Here the expectation is over the first measured output under p1p_1p1​ and QQQ. An output with probability zero contributes zero. The left and right members represent, respectively, the costs with perfect state information and with no useful measurements. Åström, 1965, (5.12), p. 193.

What the result provides

For any model satisfying the stated finite-state assumptions, the two easier dynamic programs bracket the best achievable expected loss with partial information. The differences between these values are the paper's measures of the value of perfect state information and the value of incomplete state information, described immediately after (5.12). Because the loss may have either sign, these are order comparisons of minimal costs rather than bounds that depend on a nonnegativity convention. Åström, 1965, (5.13)–(5.14).

The mathematical result was established in the paper. This mission asks for machine-checked proofs of its finite-path model, the three value recursions, the identification of P.1's minimum, and the information bounds. The value functions are linked by shared definitions, so later finite-state partially observed control developments can reuse the pathwise cost and Bayes update instead of rebuilding them for each theorem.

Where the proof is difficult

The tempting comparison between the three Bellman equations cannot simply replace the posterior belief by its average: the controller may choose different actions after different observations, and the continuation value is generally nonlinear in the belief. The exact-information case must also be read at beliefs concentrated at a single state. Its value formula is linear in an arbitrary input belief by definition, but the partial-observation value need not equal that linear function away from those state vertices. A second issue is connecting a feedback solution of (3.28) to the original expected loss over all output-history laws; using a belief-defined objective at the outset would assume the identification that Theorem 2 establishes.

Formalization scope

The Lean model uses finite state, output, and horizon types, a nonempty compact control set in Rd\mathbb R^dRd, stochastic transition and observation rows, and continuous dependence on controls where the paper requires it. All probabilities and expectations are finite sums and products. A Fin N index of zero represents paper time one. The model starts from the law of x1x_1x1​, since §II introduces the law of x0x_0x0​ but specifies neither a control at time zero nor the transition to x1x_1x1​. The transition controlled at time ttt is therefore written with the paper's transition index t+1t+1t+1. These conventions make the first-output expectation and (3.22) use the same timing.

The norm of zjz^jzj is its ℓ1\ell^1ℓ1 norm, the sum of absolute coordinates. At an impossible output, Lean's totalized posterior is zero; the associated continuation term has weight zero. Conditional-probability claims apply only to positive-probability histories. Each minimum over controls is represented by a real infimum over UUU. The compact control set is nonempty and the continuous costs are bounded on it, so this has the intended finite attained meaning on probability beliefs. The terminal values VN+1V_{N+1}VN+1​, SN+1S_{N+1}SN+1​ and VN+1′′V''_{N+1}VN+1′′​ are zero.

The original objective is a separate pathwise expected cost, minimized over all admissible output-history laws. The target includes its equality with Eη1V1(w(1))\mathbb E_{\eta_1}V_1(w(1))Eη1​​V1​(w(1)); stating only an inequality between three unrelated Bellman solutions would omit the subject of (5.12). Reusable contributions include finite-path probability identities, the Bayes recursion, attainment for continuous control minima, and the three value comparisons. No special observation matrix is assumed in Theorems 4, 5, or the goal.

Selected references

  • K. J. Åström, Optimal Control of Markov Processes with Incomplete State Information, Journal of Mathematical Analysis and Applications 10(1):174–205, 1965. DOI: 10.1016/0022-247X(65)90154-X.
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Universality in Polytope Phase Transitions and Message Passing Algorithms 2: State Evolution, Empirical Averages of Polynomial AMP Iterates Converge to Gaussian ExpectationsResearch Paper

Motivation

Approximate message passing (AMP) is an iterative method for large systems with random matrices. At each step, every coordinate receives a weighted combination of nonlinear messages from all other coordinates, together with a correction for dependence created by earlier steps. For symmetric random matrices, the correction makes a simple description of the high-dimensional iterates possible: a finite collection of covariance matrices predicts their limiting distributions. Bayati, Lelarge and Montanari prove this state evolution statement for polynomial AMP on a broad class of independent sub-Gaussian matrix entries, rather than only Gaussian entries (paper, §§1.2–1.3). It gives a precise distributional account of an algorithm whose coordinates are coupled at every iteration.

The paper has three distinct headline results. Its Theorem 3 compares AMP moments under two matrix laws with equal entry variances, and its Theorem 2 concerns projected cross-polytopes. This mission targets Theorem 4, which identifies the limit of empirical averages of AMP iterates with a Gaussian expectation. The companion missions address the other results; the statements here use their own copy of the paper's AMP model because draft definitions cannot yet be imported across proposals (paper, pp. 5, 8–9).

Setting

For each size NNN, let A(N)A(N)A(N) be a random symmetric N×NN\times NN×N matrix with zero diagonal. Its entries above the diagonal are independent, centered, and sub-Gaussian at scale C/NC/NC/N. Each coordinate iii carries a polynomial map fi(⋅;t):Rq→Rqf^i(\cdot;t):\mathbb R^q\to\mathbb R^qfi(⋅;t):Rq→Rq at iteration ttt and an initial vector xi0x_i^0xi0​. Their coefficients have degree at most ddd and a uniform bound CCC. The AMP orbit is

xit+1=∑jAijfj(xjt;t)−∑jAij2Jfj(xjt;t)fi(xit−1;t−1).x_i^{t+1}=\sum_j A_{ij}f^j(x_j^t;t) -\sum_j A_{ij}^{2}Jf^j(x_j^t;t)f^i(x_i^{t-1};t-1).xit+1​=j∑​Aij​fj(xjt​;t)−j∑​Aij2​Jfj(xjt​;t)fi(xit−1​;t−1).

The second sum is the Onsager memory term; it is absent at t=0t=0t=0. Here JfjJf^jJfj is the Jacobian, so its product with the preceding qqq-vector is another qqq-vector. The initial vectors obey an exponential bound on their squared Euclidean norms. These assumptions form the paper's (C,d)(C,d)(C,d)-regularity condition (Definitions 2–4, pp. 6–7).

A converging sequence has a fixed finite set of classes a∈[k]a\in[k]a∈[k]. Coordinate iii belongs to CaNC_a^NCaN​ for one class aaa, whose proportion approaches ca∈(0,1)c_a\in(0,1)ca​∈(0,1). A symmetric nonnegative matrix WWW specifies entry variances: if i∈CaNi\in C_a^Ni∈CaN​ and j∈CbNj\in C_b^Nj∈CbN​, then EAij2=Wab/N\mathbb E A_{ij}^2=W_{ab}/NEAij2​=Wab​/N. Independent labels Y(i)Y(i)Y(i) have class-dependent laws PaP_aPa​, each a finite mixture of Gaussian laws that may be degenerate. The polynomial maps have the common form fi(x;t)=g(x,Y(i),a,t)f^i(x;t)=g(x,Y(i),a,t)fi(x;t)=g(x,Y(i),a,t) for i∈CaNi\in C_a^Ni∈CaN​ (Definition 5, pp. 8–9).

The empirical second moments of g(xi0,Y(i),a,0)g(x_i^0,Y(i),a,0)g(xi0​,Y(i),a,0) converge in probability to a prescribed positive semidefinite matrix Σ^a0\widehat\Sigma_a^0Σa0​. For t≥1t\ge1t≥1, state evolution defines

Σat=∑bcbWabΣ^bt−1,Σ^at=E[g(Zat,Ya,a,t)g(Zat,Ya,a,t)T],\Sigma_a^t=\sum_b c_bW_{ab}\widehat\Sigma_b^{t-1},\qquad \widehat\Sigma_a^t=\mathbb E\big[g(Z_a^t,Y_a,a,t)g(Z_a^t,Y_a,a,t)^{\mathsf T}\big],Σat​=b∑​cb​Wab​Σbt−1​,Σat​=E[g(Zat​,Ya​,a,t)g(Zat​,Ya​,a,t)T],

where Zat∼N(0,Σat)Z_a^t\sim\mathcal N(0,\Sigma_a^t)Zat​∼N(0,Σat​) is independent of Ya∼PaY_a\sim P_aYa​∼Pa​. The index t−1t-1t−1 in the first formula and ttt in the second are essential (equations (1.9)–(1.11), p. 9).

Formalization targets

Coordinate moments and concentration

For a nonnegative multi-index mmm and a coordinate sequence eventually in class aaa, Proposition 4 identifies the Gaussian limit of each moment. Proposition 5 says the variance of the class-average monomial tends to zero:

E[(xi(N)t)m]⟶E[(Zat)m],Var⁡ ⁣(1∣CaN∣∑i∈CaN(xit)m)⟶0.\mathbb E[(x_{i(N)}^t)^m]\longrightarrow\mathbb E[(Z_a^t)^m],\qquad \operatorname{Var}\!\left(\frac1{|C_a^N|}\sum_{i\in C_a^N}(x_i^t)^m\right)\longrightarrow0.E[(xi(N)t​)m]⟶E[(Zat​)m],Var​∣CaN​∣1​i∈CaN​∑​(xit​)m​⟶0.

The diagonal two-time identity (4.4) is another milestone: Σat,t\Sigma_a^{t,t}Σat,t​ has four blocks, each equal to Σat\Sigma_a^tΣat​. These are the paper's stated intermediate targets (pp. 15, 30, 32).

Main goal: Theorem 4

For t≥1t\ge1t≥1, class aaa, and every locally Lipschitz function ψ\psiψ with ∣ψ(x,y)∣≤K(1+∥x∥22+∥y∥22)K|\psi(x,y)|\le K(1+\|x\|_2^2+\|y\|_2^2)^K∣ψ(x,y)∣≤K(1+∥x∥22​+∥y∥22​)K for some KKK, prove convergence in probability:

1∣CaN∣∑j∈CaNψ(xjt,Y(j))⟶E[ψ(Zat,Ya)].\frac1{|C_a^N|}\sum_{j\in C_a^N}\psi(x_j^t,Y(j)) \longrightarrow \mathbb E[\psi(Z_a^t,Y_a)].∣CaN​∣1​j∈CaN​∑​ψ(xjt​,Y(j))⟶E[ψ(Zat​,Ya​)].

The target covers polynomial-growth test functions, including functions beyond monomials. The expectation on the right is under the product law of the Gaussian state and the independent class label (Theorem 4, p. 9).

Significance

The theorem assigns a computable asymptotic distribution to each class of AMP coordinates at every fixed positive iteration time. It can be used to evaluate empirical observables without tracking the full coupled NNN-dimensional random trajectory. The class weights and variance profile permit heterogeneous coordinates, while the sub-Gaussian assumption covers more matrix laws than a Gaussian-only statement (paper, Introduction and Theorem 4).

The paper proves this result. The mission's Lean statements are compilation-checked targets, with proofs still to be formalized. A completed development would establish the measure-theoretic meaning of the covariance recursion and its Gaussian expectations, as well as the moment and concentration claims needed for the empirical limit. The polynomial representation, random-matrix regularity predicate, and Gaussian transport are reusable for other AMP results from the same paper.

Difficulty

The matrix A(N)A(N)A(N) is reused at every AMP iteration, so a new coordinate is correlated with earlier coordinates and with the matrix entries that produced them. A direct independent-summand argument for its Gaussian limit is unavailable. The memory term is tuned to this dependence, and any formal proof must account for its exact Jacobian and squared-entry form. Passing from individual moments to empirical averages also requires control of correlations between different coordinates. The target allows locally Lipschitz functions with polynomial growth, so convergence for a fixed monomial alone does not finish the job (paper, §4.7).

Formalization scope

Vectors in Rq\mathbb R^qRq are functions Fin q → ℝ; squared Euclidean norms are explicit sums of coordinate squares. Polynomials use bounded real coefficient arrays as in (4.10), with an explicit Jacobian. Fin N uses zero-based indices. The orbit stores the current and preceding iterates and omits the memory term at t=0t=0t=0. A single probability space carries all sizes; matrix entries, labels, coefficients, and initial vectors have explicit measurability and independence conditions.

The paper's displayed sub-Gaussian formula conflicts with its stated C/NC/NC/N scale, so the model uses the scale required by its moment estimates and imposes the moment-generating bound for all real arguments. Its initial exponential bound is read almost surely at every size, which ensures the expectations used by the paper are well-defined. Label-dependent polynomial coefficients are measurable. The full label vector is independent of the matrix and initial vectors; this makes explicit the independence needed for Theorem 4's Gaussian-label product law. Independence of the induced polynomial coefficients alone would not imply it when ggg ignores part of a label. The initial covariance limit is entrywise convergence in probability; finite-dimensional equivalence makes this the same matrix convergence. Class averages divide by the class cardinality, even though that expression has Lean's default value at an empty class for a small NNN. Positive limiting class fractions make those finite exceptions irrelevant.

Gaussian laws live on Mathlib's Euclidean space and are transported to coordinate vectors. Theorems explicitly assert positive semidefiniteness or integrability where a non-PSD covariance, non-integrable expectation, or non-square-integrable variance could otherwise give a default value. The source's Y(i)Y(i)Y(i) in (1.12) is read as Y(j)Y(j)Y(j), its summation index, and its final covariance as Σat\Sigma_a^tΣat​. The Gaussian covariance is computed by the recursion above; it is not defined from the proposed limit. Contributions establishing moment bounds, covariance positivity, Gaussian integrability, the three milestones, or the full Theorem 4 are within scope.

Selected references

  • M. Bayati, M. Lelarge and A. Montanari, Universality in polytope phase transitions and message passing algorithms, Annals of Applied Probability 25(2), 2015, 753–822. arXiv:1207.7321v2; DOI:10.1214/14-AAP1010.
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Dynamic ProgrammingOptimizationReinforcement Learning·Captain: mikedeng1

Global Optimality Guarantees for Policy Gradient Methods 1: If the Policy Class Is Closed Under Policy Improvement, Every Stationary Point of the Policy Gradient Objective Is Globally OptimalResearch Paper

Why the landscape of policy gradient matters

Policy gradient methods optimize a parameterized policy for a Markov decision process by running gradient descent on its expected cost. They underlie most large-scale reinforcement learning, from robotics to game playing, and are also natural in operations research, where structured policy classes (linear feedback, base-stock levels, thresholds) are standard. The objective, however, is almost never convex in the parameters, and classical theory only promises convergence to stationary points. Whether such methods find optimal policies therefore depends on the landscape: whether stationary points can be suboptimal.

J. Bhandari and D. Russo (arXiv:1906.01786v3, published in Operations Research, 2024, DOI 10.1287/opre.2021.0014) identify structural conditions under which the answer is no, connecting policy gradient to classical policy iteration. Fazel et al. (2018) established a landscape result for linear-quadratic control; Kakade and Langford (2002) developed a performance-difference identity for conservative policy iteration on finite MDPs. Bhandari and Russo's Theorem 1 gives a general sufficient condition on a general state space; Agarwal et al. (2021) developed the tabular case in detail.

Setting

A Markov decision process is a tuple (S,(As)s∈S,g,P,γ,ρ)(\mathcal S,(\mathcal A_s)_{s\in\mathcal S},g,P,\gamma,\rho)(S,(As​)s∈S​,g,P,γ,ρ): a measurable state space S\mathcal SS, nonempty feasible action sets As⊆A\mathcal A_s\subseteq\mathcal AAs​⊆A, a bounded measurable cost g(s,a)g(s,a)g(s,a), a transition kernel P(⋅∣s,a)P(\cdot\mid s,a)P(⋅∣s,a), a discount factor γ∈(0,1)\gamma\in(0,1)γ∈(0,1) and an initial probability distribution ρ\rhoρ. A policy is a measurable map π:S→A\pi:\mathcal S\to\mathcal Aπ:S→A; it is feasible, π∈Π\pi\in\Piπ∈Π, if π(s)∈As\pi(s)\in\mathcal A_sπ(s)∈As​ for every sss.

For a policy π\piπ, the cost-to-go Jπ(s)J_\pi(s)Jπ​(s) is the expected discounted sum of costs started from sss. The discounted average cost is ℓ(π)=(1−γ)∫Jπ dρ\ell(\pi) = (1-\gamma)\int J_\pi\,d\rhoℓ(π)=(1−γ)∫Jπ​dρ, and the discounted state-occupancy measure is ηπ=(1−γ)∑t≥0γtPρπ(st∈⋅)\eta_\pi = (1-\gamma)\sum_{t\ge0}\gamma^t P^\pi_\rho(s_t\in\cdot)ηπ​=(1−γ)∑t≥0​γtPρπ​(st​∈⋅). The Bellman operators are

(TπJ)(s)=g(s,π(s))+γ ⁣∫ ⁣J dP(⋅∣s,π(s)),(TJ)(s)=min⁡a∈As[g(s,a)+γ ⁣∫ ⁣J dP(⋅∣s,a)].(T_\pi J)(s) = g(s,\pi(s))+\gamma\!\int\! J\,dP(\cdot\mid s,\pi(s)),\qquad (TJ)(s) = \min_{a\in\mathcal A_s}\Big[g(s,a)+\gamma\!\int\! J\,dP(\cdot\mid s,a)\Big].(Tπ​J)(s)=g(s,π(s))+γ∫JdP(⋅∣s,π(s)),(TJ)(s)=a∈As​min​[g(s,a)+γ∫JdP(⋅∣s,a)].

An optimal policy π∗\pi^*π∗ satisfies Jπ∗≤JπJ_{\pi^*}\le J_\piJπ∗​≤Jπ​ pointwise for every π∈Π\pi\in\Piπ∈Π. Two standing assumptions hold throughout: Assumption 1, ηπ∗≪ρ\eta_{\pi^*}\ll\rhoηπ∗​≪ρ (the initial distribution is exploratory), and Assumption 2, measurable selection of a minimizing action in TTT.

A parameterized policy class is ΠΘ={πθ:θ∈Θ}⊆Π\Pi_\Theta = \{\pi_\theta:\theta\in\Theta\}\subseteq\PiΠΘ​={πθ​:θ∈Θ}⊆Π with Θ⊆Rd\Theta\subseteq\mathbb R^dΘ⊆Rd convex, and ℓ(θ)=ℓ(πθ)\ell(\theta) = \ell(\pi_\theta)ℓ(θ)=ℓ(πθ​) is the policy gradient objective. A point θ∈Θ\theta\in\Thetaθ∈Θ is stationary if ⟨θ′−θ,∇ℓ(θ)⟩≥0\langle\theta'-\theta,\nabla\ell(\theta)\rangle\ge0⟨θ′−θ,∇ℓ(θ)⟩≥0 for all θ′∈Θ\theta'\in\Thetaθ′∈Θ. The weighted policy-iteration objective is

B(θˉ∣η,J)=∫(TπθˉJ) dη,\mathcal B(\bar\theta\mid\eta,J) = \int (T_{\pi_{\bar\theta}}J)\,d\eta ,B(θˉ∣η,J)=∫(Tπθˉ​​J)dη,

the cost of following πθˉ\pi_{\bar\theta}πθˉ​ for one period and then incurring JJJ, averaged over η\etaη.

The three conditions of the main theorem are:

  • Condition 0 (differentiability): the policy parameter and the parameter that generates the occupancy measure vary jointly, with the resulting B\mathcal BB continuously differentiable near each (θ,θ)(\theta,\theta)(θ,θ);
  • Condition 1 (closure under policy improvement): for each π∈ΠΘ\pi\in\Pi_\Thetaπ∈ΠΘ​ some π+∈ΠΘ\pi^+\in\Pi_\Thetaπ+∈ΠΘ​ attains min⁡π′∈ΠB(π′∣ηπ,Jπ)\min_{\pi'\in\Pi}\mathcal B(\pi'\mid\eta_\pi,J_\pi)minπ′∈Π​B(π′∣ηπ​,Jπ​);
  • Condition 2.A: for each π∈ΠΘ\pi\in\Pi_\Thetaπ∈ΠΘ​, θˉ↦B(θˉ∣ηπ,Jπ)\bar\theta\mapsto\mathcal B(\bar\theta\mid\eta_\pi,J_\pi)θˉ↦B(θˉ∣ηπ​,Jπ​) has no suboptimal stationary points on Θ\ThetaΘ.

Formalization targets

Goal: Theorem 1 (p. 14)

Under Conditions 0, 1 and 2.A, ℓ\ellℓ is continuously differentiable, and for every θ∈Θ\theta\in\Thetaθ∈Θ

θ is a stationary point of ℓ⟺ℓ(πθ)=ℓ(π∗).\theta\ \text{is a stationary point of }\ell\quad\Longleftrightarrow\quad \ell(\pi_\theta) = \ell(\pi^*).θ is a stationary point of ℓ⟺ℓ(πθ​)=ℓ(π∗).

The right side compares with the optimum over all feasible policies, not only the class.

Milestones

  1. ηπ⪰(1−γ)ρ\eta_\pi\succeq(1-\gamma)\rhoηπ​⪰(1−γ)ρ (p. 7) and the element-wise inequalities (5), TJ⪯TπJTJ\preceq T_\pi JTJ⪯Tπ​J and TJπ⪯JπTJ_\pi\preceq J_\piTJπ​⪯Jπ​ (p. 7).
  2. The performance difference identity (29), ℓ(π)−ℓ(πˉ)=∫[TπJπˉ−Jπˉ] dηπ\ell(\pi)-\ell(\bar\pi) = \int[T_\pi J_{\bar\pi}-J_{\bar\pi}]\,d\eta_\piℓ(π)−ℓ(πˉ)=∫[Tπ​Jπˉ​−Jπˉ​]dηπ​ (p. 39).
  3. Lemma 6, the policy gradient theorem: ∇ℓ(θ)=∇θˉB(θˉ∣ηπθ,Jπθ)∣θˉ=θ\nabla\ell(\theta) = \nabla_{\bar\theta}\mathcal B(\bar\theta\mid\eta_{\pi_\theta},J_{\pi_\theta})|_{\bar\theta=\theta}∇ℓ(θ)=∇θˉ​B(θˉ∣ηπθ​​,Jπθ​​)∣θˉ=θ​ (p. 13).
  4. Lemma 7: at a stationary point, ∫Jπθ dηπθ=min⁡π∈ΠΘ∫(TπJπθ) dηπθ\int J_{\pi_\theta}\,d\eta_{\pi_\theta} = \min_{\pi\in\Pi_\Theta}\int(T_\pi J_{\pi_\theta})\,d\eta_{\pi_\theta}∫Jπθ​​dηπθ​​=minπ∈ΠΘ​​∫(Tπ​Jπθ​​)dηπθ​​ (p. 14).
  5. Lemma 8, the on-average Bellman equation: ℓ(π)=ℓ(π∗)  ⟺  ∫(Jπ−TJπ) dρ=0\ell(\pi) = \ell(\pi^*)\iff\int(J_\pi-TJ_\pi)\,d\rho = 0ℓ(π)=ℓ(π∗)⟺∫(Jπ​−TJπ​)dρ=0 (p. 15).

Significance

Theorem 1 converts a question about a nonconvex, multi-period objective into checks on single-period problems. Any algorithm that provably reaches stationary points (projected gradient descent, for instance) then reaches globally optimal policies whenever the policy class is closed under improvement and the one-step problems are benign. The paper verifies the conditions for LQ control, finite MDPs with softmax policies, optimal stopping with threshold policies and inventory control with base-stock policies; the quantitative refinements (gradient dominance, approximate closure, finite horizons) are the subject of the later missions of this series.

The result is proved in the paper; nothing in it has been machine-checked. A formalization would produce a measure-theoretic library for discounted MDPs on general spaces (cost-to-go via kernels, occupancy measures, Bellman operators, the performance difference identity) that is reusable well beyond this paper, and would pin down the exact differentiability hypothesis the argument needs.

Difficulty

The obvious route, differentiating ℓ(θ)=(1−γ)∫Jπθ dρ\ell(\theta) = (1-\gamma)\int J_{\pi_\theta}\,d\rhoℓ(θ)=(1−γ)∫Jπθ​​dρ directly, requires differentiating an infinite discounted sum of ttt-step kernels in the parameter, and on a general state space that derivative is not available without regularity of the transition law. The performance difference identity demands an exchange of an infinite series with integrals against composed kernels, and measurability of every object involved, including TJπTJ_\piTJπ​, which is measurable only through the selection assumption. The stationary-implies-optimal direction must pass from an inequality weighted by ηπθ\eta_{\pi_\theta}ηπθ​​ to one weighted by ρ\rhoρ, and then to ηπ∗\eta_{\pi^*}ηπ∗​, where Assumption 1 enters.

Formalization scope

S\mathcal SS and A\mathcal AA are arbitrary measurable spaces; the paper takes Borel subsets of Euclidean spaces, a structure no argument uses. The cost ggg is bounded and, with the kernel PPP, defined on all of S×A\mathcal S\times\mathcal AS×A: Condition 0 differentiates at parameters near Θ\ThetaΘ, where πθ\pi_\thetaπθ​ need not be feasible. Policies are deterministic, stationary and measurable; randomized policies are covered by taking actions to be probability vectors. Θ⊆Rd\Theta\subseteq\mathbb R^dΘ⊆Rd is the Euclidean space, gradients are Euclidean, and Θ\ThetaΘ is convex (not assumed closed).

Conventions committed to in Lean:

  • a stationary point includes differentiability of the function at that point;
  • J∗J^*J∗ is never an infimum over policies: an optimal policy π∗\pi^*π∗ is a hypothesis, and J∗=Jπ∗J^* = J_{\pi^*}J∗=Jπ∗​;
  • TTT is an infimum over As\mathcal A_sAs​, equal to the minimum on bounded functions;
  • the Bellman operators carry the factor γ\gammaγ, which the printed (3)–(4) omit but every other display and proof uses;
  • Condition 0 is the joint form: (θˉ,θ′)↦B(θˉ∣ηπθ′,Jπθ)(\bar\theta,\theta')\mapsto\mathcal B(\bar\theta\mid\eta_{\pi_{\theta'}},J_{\pi_\theta})(θˉ,θ′)↦B(θˉ∣ηπθ′​​,Jπθ​​) is C1C^1C1 near (θ,θ)(\theta,\theta)(θ,θ). The printed condition asks only for its two partial maps; the paper's proof of Lemma 6 expands a total derivative into partials, which needs the joint form, and the joint form implies the printed one;
  • Assumptions 1 and 2 are hypotheses of the goal (standing assumptions of §2);
  • Lemma 7 also carries Condition 0, which its proof uses through Lemma 6.

The goal does not assume that ΠΘ\Pi_\ThetaΠΘ​ contains π∗\pi^*π∗, the equation of Lemma 7 or the conclusion of Lemma 8; a formalization that takes any of these as a hypothesis trivializes the theorem.

A complete development needs the composition of kernels, interchange of series and integrals for bounded functions, the fixed-point identity TπJπ=JπT_\pi J_\pi = J_\piTπ​Jπ​=Jπ​, the performance difference identity, the first-order optimality condition on a convex set, and the chain rule for a jointly C1C^1C1 function along the diagonal. The MDP layer, the identity (29) and the element-wise inequalities are reused by the other missions of the series. Proofs of the milestones, and proofs of the identity (29) in isolation, are welcome.

Selected references

  • J. Bhandari, D. Russo, Global Optimality Guarantees for Policy Gradient Methods, Operations Research, 2024 (arXiv:1906.01786v3, 2022). https://arxiv.org/abs/1906.01786, https://doi.org/10.1287/opre.2021.0014
  • S. Kakade, J. Langford, Approximately Optimal Approximate Reinforcement Learning, ICML, 2002. https://dl.acm.org/doi/10.5555/645531.656005
  • M. Fazel, R. Ge, S. Kakade, M. Mesbahi, Global Convergence of Policy Gradient Methods for the Linear Quadratic Regulator, ICML, 2018. https://arxiv.org/abs/1801.05039
  • A. Agarwal, S. Kakade, J. Lee, G. Mahajan, On the Theory of Policy Gradient Methods: Optimality, Approximation, and Distribution Shift, JMLR, 2021. https://arxiv.org/abs/1908.00261
  • O. Hernández-Lerma, J. B. Lasserre, Discrete-Time Markov Control Processes, Springer, 1996. https://doi.org/10.1007/978-1-4612-0729-0
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Bandit AlgorithmsMachine LearningProbability·Captain: mikedeng1

A Tutorial on Thompson Sampling II: Under Thompson Sampling, Per-Period Expected Regret Splits into a Pessimism Term and a Width Term for Any History-Determined U_tResearch Paper

Motivation

An online decision maker repeatedly chooses an action, observes an outcome, and receives a reward. In a Bayesian model, an unknown parameter controls the outcomes, and the decision maker begins with a prior distribution for that parameter. Thompson sampling acts by drawing a parameter from its current posterior distribution and choosing an action that would be best if that draw were correct. This makes it applicable when an agent can simulate a plausible model and optimize an action for that model. Russo, Van Roy, Kazerouni, Osband, and Wen explain this rule for general online decision problems in Section 4 of their tutorial.

The tutorial's Section 8.1.2 asks how to analyze the rule's expected regret. An upper confidence bound method chooses an action using an optimistic score and can analyze regret through the score's optimism and its uncertainty width. Thompson sampling does not choose its actions by maximizing such a score. Yet the tutorial shows that any score computed from the observed past can be used to split Thompson sampling's expected regret into the same two types of terms. The result is stated on pp. 72–73, equation (8.4) and the display that follows.

Setting

Let X\mathcal XX be a finite, nonempty set of actions, YYY a finite set of outcomes, and Θ\ThetaΘ a measurable parameter space. A prior probability measure PPP is placed on the unknown parameter θ∈Θ\theta\in\Thetaθ∈Θ. If action x∈Xx\in\mathcal Xx∈X is selected, the outcome is sampled from a probability kernel qθ(⋅∣x)q_\theta(\cdot\mid x)qθ​(⋅∣x) on YYY. A known function r:Y→Rr:Y\to\mathbb Rr:Y→R turns an outcome into a reward. The mean reward of action xxx under parameter θ\thetaθ is

μ(x,θ)=∑y∈Yqθ(y∣x)r(y).\mu(x,\theta)=\sum_{y\in Y}q_\theta(y\mid x)r(y).μ(x,θ)=y∈Y∑​qθ​(y∣x)r(y).

For each θ\thetaθ, choose an action x∗(θ)x^*(\theta)x∗(θ) maximizing μ(⋅,θ)\mu(\cdot,\theta)μ(⋅,θ). This choice uses a fixed tie-break and is measurable. The same selector is used throughout the mission. A length-ttt history HtH_tHt​ records the first ttt action–outcome pairs. A policy π\piπ assigns an action distribution to every such history. The prior, the policy, and the outcome kernel together determine the law of all histories: first draw θ\thetaθ from PPP, then choose each action from π\piπ using the past history, and finally generate its outcome using qθq_\thetaqθ​.

After history hhh, the posterior law of x∗x^*x∗ is obtained by reweighting the prior by the likelihood of the observed outcomes. Thompson sampling draws a parameter from this posterior and plays the selected optimum for that parameter. Thus the law of its next action, given hhh, is the posterior law of x∗x^*x∗ given hhh. The policy remains defined even for a history with zero likelihood; choices there do not affect expectations.

For a period ttt, let Ut(x)U_t(x)Ut​(x) be any real score that uses the action xxx and the observed history Ht−1H_{t-1}Ht−1​. The score is fixed before the period's outcome or the unknown parameter can be inspected. The period regret is μ(x∗,θ)−μ(xt,θ)\mu(x^*,\theta)-\mu(x_t,\theta)μ(x∗,θ)−μ(xt​,θ), with expectation taken over the prior, the policy's randomization, and the outcome process.

Formalization targets

Probability matching and equation (8.4)

The first target makes posterior sampling precise. For every feasible history hhh and action aaa, the probability that Thompson sampling next plays aaa, together with observing hhh, equals the joint probability that the selected optimum is aaa and the history is hhh. Consequently, for every history-determined UtU_tUt​,

Eπ[Ut(xt)]=Eπ[Ut(x∗)].\mathbb E_\pi[U_t(x_t)] =\mathbb E_\pi[U_t(x^*)].Eπ​[Ut​(xt​)]=Eπ​[Ut​(x∗)].

This is equation (8.4) on p. 72. It asserts equality of unconditional expectations while preserving the fact that UtU_tUt​ may depend on the past. It does not assert that xtx_txt​ and x∗x^*x∗ have the same joint law with θ\thetaθ.

Per-period regret decomposition

The goal is the full chain of equalities displayed on p. 73:

Eπ[μ(x∗,θ)−μ(xt,θ)]=Eπ[μ(x∗,θ)−Ut(xt)]+Eπ[Ut(xt)−μ(xt,θ)]=Eπ[μ(x∗,θ)−Ut(x∗)]⏟pessimism+Eπ[Ut(xt)−μ(xt,θ)]⏟width.\begin{aligned} \mathbb E_\pi[\mu(x^*,\theta)-\mu(x_t,\theta)] &=\mathbb E_\pi[\mu(x^*,\theta)-U_t(x_t)] +\mathbb E_\pi[U_t(x_t)-\mu(x_t,\theta)]\\ &=\underbrace{\mathbb E_\pi[\mu(x^*,\theta)-U_t(x^*)]}_{\text{pessimism}} +\underbrace{\mathbb E_\pi[U_t(x_t)-\mu(x_t,\theta)]}_{\text{width}}. \end{aligned}Eπ​[μ(x∗,θ)−μ(xt​,θ)]​=Eπ​[μ(x∗,θ)−Ut​(xt​)]+Eπ​[Ut​(xt​)−μ(xt​,θ)]=pessimismEπ​[μ(x∗,θ)−Ut​(x∗)]​​+widthEπ​[Ut​(xt​)−μ(xt​,θ)]​​.​

The theorem holds for every score UtU_tUt​ determined by the past history. In particular, UtU_tUt​ need not be a confidence bound for the identity to hold. Being a useful upper confidence bound matters when one later estimates the two terms.

Significance

The equality permits analyses built around optimistic scores to be transferred to Thompson sampling. It separates expected regret into a term measuring whether the score falls below the true optimal mean and another measuring the gap between the score and the true mean at the sampled action. The tutorial cites Russo and Van Roy for the surrounding regret bounds; the identity here is the precise bridge used in that discussion.

The result is already proved in the tutorial. This mission seeks a machine-checked proof of its finite-action, finite-outcome form, including the posterior-sampling law, the policy-dependent history distribution, and the conditioning behind equation (8.4). The goal and milestones are open Lean statements, not completed machine-checked proofs. Their definitions can be reused in later finite Bayesian decision models with a general measurable parameter.

Difficulty

The central issue is that xtx_txt​ and x∗x^*x∗ are not interchangeable inside an expression that depends on θ\thetaθ. The sampled action and the selected optimum have the same distribution after conditioning on the observed past, but generally have different dependence on the true parameter. For example, replacing UtU_tUt​ by μ(⋅,θ)\mu(\cdot,\theta)μ(⋅,θ) would make the claimed equality false. A formal proof therefore has to respect the boundary between history-derived scores and parameter-dependent quantities, and it must use the same history law to interpret every expectation. Histories of zero probability also require a consistent posterior convention.

Formalization scope

The Lean model uses finite action and outcome types and a general measurable parameter type. This is a disclosed specialization of the tutorial, which also allows infinite actions and more general outcome spaces. The kernel qθq_\thetaqθ​ is nonnegative, sums to one over outcomes, and is measurable in θ\thetaθ. The prior is a probability measure. The reward function is real valued and bounded because its domain is finite. The optimal-action selector has measurable fibers and maximizes the mean reward for every parameter. These conditions make the integrands measurable and bounded, avoiding default values of nonintegrable Lean integrals.

Histories are functions from a finite period index to action–outcome pairs. Policies are normalized, nonnegative behavioural action probabilities. The likelihood of a history multiplies both its policy action factors and its kernel outcome factors. The posterior uses only outcome likelihood factors, which give the Bayes update on every positive-evidence history. The Thompson-sampling predicate enforces the posterior action probabilities on those histories and permits any normalized policy on impossible ones. Lean period sss denotes the tutorial's period t=s+1t=s+1t=s+1.

The shared tie-break is essential: Thompson sampling and x∗x^*x∗ use the same selected maximizer. The score has type Ht−1→X→RH_{t-1}\to\mathcal X\to\mathbb RHt−1​→X→R, so it cannot inspect θ\thetaθ or the current outcome. No definition is allowed to supply regret or the decomposition as a predetermined constant; the expectation is built from the prior, policy and outcome kernel. The development needs reusable definitions for the Bayesian model, finite histories, behavioural policies, likelihoods, posterior masses, and the two regret terms. Contributions proving probability matching, equation (8.4), and the final identity are welcome.

Selected references

  • Daniel J. Russo, Benjamin Van Roy, Abbas Kazerouni, Ian Osband, and Zheng Wen, A Tutorial on Thompson Sampling, Foundations and Trends in Machine Learning 11(1), 2018. DOI: 10.1561/2200000070.
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Dynamic ProgrammingOptimizationReinforcement Learning·Captain: mikedeng1

Global Optimality Guarantees for Policy Gradient Methods 6: In the KL-Regularized Finite MDP, a Regularized-Optimal Policy Is Within λ(1 + log(1 + c/λ)) of OptimalResearch Paper

Motivation

Policy gradient methods for Markov decision processes are frequently run on a regularized objective rather than on the cost of interest: a convex penalty on the action distribution is added to every single-period cost. Regularization smooths the problem, makes optimal policies strictly stochastic, and keeps iterates away from the boundary of the probability simplex, where gradients of common parameterizations vanish. Entropy and relative-entropy penalties are standard in this role; a unified treatment of regularized MDPs is given by Geist, Scherrer and Pietquin (2019), and Agarwal, Kakade, Lee and Mahajan (2021) analyse policy gradient with a log-barrier penalty added to the softmax objective.

Regularization changes the problem being solved. Anyone who uses it needs a quantitative answer to one question: how suboptimal, for the original costs, is a policy that is exactly optimal for the regularized costs? Bhandari and Russo (arXiv:1906.01786v3), whose main results establish that policy gradient objectives have no suboptimal stationary points under a closure condition, answer this question for a relative-entropy regularizer in finite MDPs (their Lemma 10). Bounds of this type for the negative-entropy regularizer are in Geist et al.; as Bhandari and Russo note (p. 20), those bounds do not apply to the unbounded log-barrier regularizer used here.

Setting

The state space S={1,…,n}\mathcal S=\{1,\dots,n\}S={1,…,n} is finite. There are kkk deterministic actions e1,…,eke_1,\dots,e_ke1​,…,ek​, and an action is a probability vector a∈Δk−1a\in\Delta_{k-1}a∈Δk−1​. A policy π\piπ chooses π(s)=(π(1∣s),…,π(k∣s))∈Δk−1\pi(s)=(\pi(1|s),\dots,\pi(k|s))\in\Delta_{k-1}π(s)=(π(1∣s),…,π(k∣s))∈Δk−1​ at each state; Π\PiΠ is the set of all such policies. Transitions are linear in the action,

P(s′∣s,a)=∑i=1kP(s′∣s,ei) ai,P(s'|s,a)=\sum_{i=1}^kP(s'|s,e_i)\,a_i ,P(s′∣s,a)=i=1∑k​P(s′∣s,ei​)ai​,

where each P(⋅∣s,ei)P(\cdot|s,e_i)P(⋅∣s,ei​) is a probability vector. Each state has a nonnegative cost vector gs∈R+kg_s\in\mathbb R^k_+gs​∈R+k​. For λ≥0\lambda\ge0λ≥0, the regularized cost is

gλ(s,a)=gs⊤a+λ DKL(U∥a),DKL(U∥a)=∑i=1k1klog⁡1/kai,g_\lambda(s,a)=g_s^\top a+\lambda\,D_{\mathrm{KL}}(U\|a),\qquad D_{\mathrm{KL}}(U\|a)=\sum_{i=1}^k\frac1k\log\frac{1/k}{a_i},gλ​(s,a)=gs⊤​a+λDKL​(U∥a),DKL​(U∥a)=i=1∑k​k1​logai​1/k​,

where UUU is the uniform distribution. The divergence is +∞+\infty+∞ unless every ai>0a_i>0ai​>0, so gλg_\lambdagλ​ takes values in [0,∞][0,\infty][0,∞].

Given a discount factor γ∈(0,1)\gamma\in(0,1)γ∈(0,1) and an initial distribution ρ\rhoρ, the discounted average cost of a policy is

ℓλ(π)=(1−γ)∑sρ(s) Jλ,π(s),Jλ,π(s)=Esπ[∑t≥0γtgλ(st,π(st))].\ell_\lambda(\pi)=(1-\gamma)\sum_{s}\rho(s)\,J_{\lambda,\pi}(s),\qquad J_{\lambda,\pi}(s)=\mathbb E^\pi_s\Big[\sum_{t\ge0}\gamma^tg_\lambda(s_t,\pi(s_t))\Big].ℓλ​(π)=(1−γ)s∑​ρ(s)Jλ,π​(s),Jλ,π​(s)=Esπ​[t≥0∑​γtgλ​(st​,π(st​))].

ℓ0\ell_0ℓ0​ is the unregularized cost. The discounted occupancy of π\piπ is ηπ(s′)=(1−γ)∑sρ(s)∑t≥0γtPr⁡π(st=s′∣s0=s)\eta_\pi(s')=(1-\gamma)\sum_s\rho(s)\sum_{t\ge0}\gamma^t\Pr^\pi(s_t=s'\mid s_0=s)ηπ​(s′)=(1−γ)∑s​ρ(s)∑t≥0​γtPrπ(st​=s′∣s0​=s). J0∗J^*_0J0∗​ and Q0∗Q^*_0Q0∗​ denote the optimal cost-to-go and state-action cost-to-go of the unregularized problem. The constant of the result is

c=2max⁡s,i∣gs,i∣1−γ.c=\frac{2\max_{s,i}|g_{s,i}|}{1-\gamma}.c=1−γ2maxs,i​∣gs,i​∣​.

Formalization targets

Goal: Lemma 10 (impact of regularization)

If πλ∗∈arg⁡min⁡π∈Πℓλ(π)\pi^*_\lambda\in\arg\min_{\pi\in\Pi}\ell_\lambda(\pi)πλ∗​∈argminπ∈Π​ℓλ​(π) with λ≥0\lambda\ge0λ≥0, then

ℓ0(πλ∗)≤min⁡π∈Πℓ0(π)+λ(1+log⁡(1+cλ)).\ell_0(\pi^*_\lambda)\le\min_{\pi\in\Pi}\ell_0(\pi)+\lambda\Big(1+\log\Big(1+\frac c\lambda\Big)\Big).ℓ0​(πλ∗​)≤π∈Πmin​ℓ0​(π)+λ(1+log(1+λc​)).

Milestones (the steps of the proof in Appendix E.2)

  1. Cost decomposition (34): ℓλ(π)=∑sηπ(s)gλ(s,π(s))=ℓ0(π)+λ∑sηπ(s)D(U∥π(s))\ell_\lambda(\pi)=\sum_s\eta_\pi(s)g_\lambda(s,\pi(s))=\ell_0(\pi)+\lambda\sum_s\eta_\pi(s)D(U\|\pi(s))ℓλ​(π)=∑s​ηπ​(s)gλ​(s,π(s))=ℓ0​(π)+λ∑s​ηπ​(s)D(U∥π(s)) for every π∈Π\pi\in\Piπ∈Π.
  2. One-step bound (37): for a policy πλ\pi_\lambdaπλ​ that, at every state, minimizes a↦∑iQ0∗(s,ei)ai+λD(U∥a)a\mapsto\sum_iQ^*_0(s,e_i)a_i+\lambda D(U\|a)a↦∑i​Q0∗​(s,ei​)ai​+λD(U∥a) over the simplex (construction (36)),
∑iQ0∗(s,ei)πλ(i∣s)≤min⁡a∈Δk−1∑iQ0∗(s,ei)ai+λ,T0πλJ0∗≤J0∗+λe.\sum_iQ^*_0(s,e_i)\pi_\lambda(i|s)\le\min_{a\in\Delta_{k-1}}\sum_iQ^*_0(s,e_i)a_i+\lambda,\qquad T^{\pi_\lambda}_0J^*_0\le J^*_0+\lambda e.i∑​Q0∗​(s,ei​)πλ​(i∣s)≤a∈Δk−1​min​i∑​Q0∗​(s,ei​)ai​+λ,T0πλ​​J0∗​≤J0∗​+λe.
  1. Suboptimality of πλ\pi_\lambdaπλ​ (35): ℓ0(πλ)≤min⁡π∈Πℓ0(π)+λ\ell_0(\pi_\lambda)\le\min_{\pi\in\Pi}\ell_0(\pi)+\lambdaℓ0​(πλ​)≤minπ∈Π​ℓ0​(π)+λ.
  2. Divergence bound (Step 3): λ D(U∥πλ(s))≤λlog⁡(1+c/λ)\lambda\,D(U\|\pi_\lambda(s))\le\lambda\log(1+c/\lambda)λD(U∥πλ​(s))≤λlog(1+c/λ) for every state sss.

Significance

The result. Lemma 10 says that the price of regularization is of order λlog⁡(1/λ)\lambda\log(1/\lambda)λlog(1/λ) as λ↓0\lambda\downarrow0λ↓0, with an explicit constant depending only on the cost scale and the effective horizon 1/(1−γ)1/(1-\gamma)1/(1−γ). Together with the paper's landscape results (Example 4 shows the regularized policy-iteration objective is strongly convex and the policy class is closed under policy improvement, so the regularized objective is gradient dominated), it turns convergence of first-order methods on the regularized problem into near-optimality for the original problem, and it gives a principled rule for choosing λ\lambdaλ as a function of the target accuracy. The bound holds for the log-barrier (relative entropy from the uniform distribution) regularizer, which is unbounded on the simplex, a case the negative-entropy analyses do not cover.

Formalizing it. The result and its proof are published (arXiv:1906.01786v3; Operations Research, 2024). No machine-checked proof of Lemma 10 or of its steps is known. The mission produces Lean statements of the lemma and of the four steps of its proof, built on a published finite-MDP layer, and invites proofs. Step 2 relies on the duality-gap bound for log-barrier problems from interior-point theory, which the paper cites from Boyd and Vandenberghe; a formal proof of that bound (in the simplex case) is reusable for any log-barrier analysis.

Difficulty

The first idea, comparing πλ∗\pi^*_\lambdaπλ∗​ with an unregularized optimal policy π0∗\pi^*_0π0∗​, fails: π0∗\pi^*_0π0∗​ is typically deterministic, so D(U∥π0∗(s))=∞D(U\|\pi^*_0(s))=\inftyD(U∥π0∗​(s))=∞ and ℓλ(π0∗)=∞\ell_\lambda(\pi^*_0)=\inftyℓλ​(π0∗​)=∞, giving no information. The comparison policy has to be built by hand: it must be strictly stochastic, nearly optimal for the unregularized problem, and have bounded divergence from the uniform distribution at every state. Each of these three properties is a separate argument: a duality-gap bound for a barrier problem on the simplex, a propagation of a one-step Bellman inequality to the whole horizon, and a quantitative lower bound on the smallest action probability of the barrier minimizer.

A second pitfall is the printed form of the lemma, whose right-hand side is min⁡πℓλ(π)+λ(1+log⁡(1+c/λ))\min_\pi\ell_\lambda(\pi)+\lambda(1+\log(1+c/\lambda))minπ​ℓλ​(π)+λ(1+log(1+c/λ)); since DKL≥0D_{\mathrm{KL}}\ge0DKL​≥0 gives ℓ0(πλ∗)≤ℓλ(πλ∗)=min⁡πℓλ(π)\ell_0(\pi^*_\lambda)\le\ell_\lambda(\pi^*_\lambda)=\min_\pi\ell_\lambda(\pi)ℓ0​(πλ∗​)≤ℓλ​(πλ∗​)=minπ​ℓλ​(π), that inequality is trivially true. The proof establishes, and the text on p. 20 announces, the bound against min⁡πℓ0(π)\min_\pi\ell_0(\pi)minπ​ℓ0​(π), which is the goal here.

Formalization scope

States and deterministic actions are finite types S and I (nonempty, as on the page, so that ccc is defined); k=∣I∣k=|I|k=∣I∣. Policies, transition kernels, the occupation distributions, the cost-to-go J0,πJ_{0,\pi}J0,π​ and Q0,πQ_{0,\pi}Q0,π​ come from the published FoundationsML.ReinforcementLearning layer (IsPolicy, IsTransitionKernel, OccupationDist, PolicyValue, QFunction), with the cost vector passed in the reward slot: PolicyValue is a plain discounted sum, so this is the cost-to-go. Optimality is the cost-minimizing notion, defined locally.

DKL(U∥⋅)D_{\mathrm{KL}}(U\|\cdot)DKL​(U∥⋅), gλg_\lambdagλ​ and ℓλ\ell_\lambdaℓλ​ take values in [0,∞][0,\infty][0,∞], with DKL=+∞D_{\mathrm{KL}}=+\inftyDKL​=+∞ off the open simplex; real-valued junk such as log⁡0=0\log0=0log0=0 never stands in for +∞+\infty+∞, and ℓλ\ell_\lambdaℓλ​ is never coerced to R\mathbb RR (that would make boundary policies look optimal). At λ=0\lambda=0λ=0 the convention 0⋅∞=00\cdot\infty=00⋅∞=0 gives g0(s,a)=gs⊤ag_0(s,a)=g_s^\top ag0​(s,a)=gs⊤​a, and Lean's c/0=0c/0=0c/0=0 makes the goal's bound 000, the limit of the page's bound. min⁡πℓ0(π)\min_\pi\ell_0(\pi)minπ​ℓ0​(π) is written as "≤ℓ0(π)+…\le\ell_0(\pi)+\dots≤ℓ0​(π)+… for every policy π\piπ". The minimizer πλ∗\pi^*_\lambdaπλ∗​ is a hypothesis (any minimizer); the barrier-greedy policy πλ\pi_\lambdaπλ​ of (36) appears only in the milestones, never in the goal. A statement of the goal with the printed right-hand side min⁡πℓλ(π)+…\min_\pi\ell_\lambda(\pi)+\dotsminπ​ℓλ​(π)+…, or one that assumes (35) or the divergence bound, would be a trivializing formalization and is ruled out.

Welcome contributions: proofs of the four milestones and the goal; a general Lean lemma that the discounted cost of a stationary policy in a finite MDP equals the occupancy-weighted single-period cost (milestone 1), which is reusable across policy gradient formalizations; and the log-barrier duality-gap bound on the simplex.

Selected references

  • J. Bhandari and D. Russo, Global Optimality Guarantees for Policy Gradient Methods, arXiv:1906.01786v3, 2022; Operations Research, 2024. https://arxiv.org/abs/1906.01786 (DOI 10.1287/opre.2021.0014)
  • M. Geist, B. Scherrer and O. Pietquin, A Theory of Regularized Markov Decision Processes, ICML, 2019. https://arxiv.org/abs/1901.11275
  • A. Agarwal, S. M. Kakade, J. D. Lee and G. Mahajan, On the Theory of Policy Gradient Methods: Optimality, Approximation, and Distribution Shift, Journal of Machine Learning Research 22(98), 2021. https://arxiv.org/abs/1908.00261
  • S. Boyd and L. Vandenberghe, Convex Optimization, Cambridge University Press, 2004, Chapter 11. https://web.stanford.edu/~boyd/cvxbook/
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Algorithmic Game TheoryOperations ResearchOptimization·Captain: mikedeng1

Disruption and Rerouting in Supply Chain Networks I: Every Supply Chain Network Has a Unique General Equilibrium of Rerouting Prices, Switching Costs and Default CascadesResearch Paper

Motivation

A failed buyer can leave a supplier with goods it can no longer sell through an existing order. A failed supplier can leave a buyer without inputs for future production. In a network, either loss can weaken another firm and start a sequence of defaults. Birge, Capponi and Chen model these effects together with two responses: suppliers reroute unsold goods to other buyers, and buyers seek replacement suppliers. Their accepted manuscript asks whether the resulting market decisions and the default cascade determine a single outcome. The issue matters when a network's resilience or fragility is measured from that outcome: a measure based on an unspecified equilibrium would not be well defined.

Setting

A supply chain order network has finitely many firms i,ji,ji,j and goods mmm. An order oijmo^m_{ij}oijm​ is the nonnegative quantity of good mmm that firm iii promises to deliver to firm jjj. The network also records each good's original price pmp^mpm, each firm's initial equity wiw_iwi​, its safety stock θim\theta_i^mθim​ and holding cost λim\lambda_i^mλim​, and a realized net production cost cic_ici​. The realization is fixed throughout this mission; the source treats it as random when comparing network performance later in the paper. Rerouting one unit costs firm iii an amount ιim\iota_i^mιim​; an unfilled unit of demand incurs back-order cost bimb_i^mbim​. These costs and the orders and stocks are nonnegative. The basic model is on pp. 8–17 of the manuscript.

If firm jjj defaults, a promised delivery to it is not made. Write γijm\gamma^m_{ij}γijm​ for this undelivered order, and rˉim=∑jγijm\bar r_i^m=\sum_j\gamma^m_{ij}rˉim​=∑j​γijm​ for firm iii's total amount of good mmm available to reroute. If a supplier jjj defaults, write δjim\delta^m_{ji}δjim​ for the buyer iii's lost input. After using safety stock, that buyer's unserved demand is σˉim=(∑jδjim−θim)+\bar\sigma_i^m=(\sum_j\delta^m_{ji}-\theta_i^m)^+σˉim​=(∑j​δjim​−θim​)+, where x+=max⁡(0,x)x^+=\max(0,x)x+=max(0,x). These are the quantities in equations (1)–(5).

The rerouted market for good mmm contains firms with rˉim>0\bar r_i^m>0rˉim​>0. At price πim\pi_i^mπim​, firm iii can sell up to rˉim\bar r_i^mrˉim​. Aggregate demand at price π\piπ is dm(π)d_m(\pi)dm​(π), with inverse demand dm−1d_m^{-1}dm−1​. The sourcing market contains firms with σˉim>0\bar\sigma_i^m>0σˉim​>0. At switching cost κim\kappa_i^mκim​, firm iii can replace up to σˉim\bar\sigma_i^mσˉim​ units. Aggregate supply is sm(κ)s_m(\kappa)sm​(κ), with inverse supply sm−1s_m^{-1}sm−1​. In either market, an efficient allocation maximizes the stated integral objective over the capacity box, and allocates proportionally to capacity among firms quoting the same price or cost. A partial equilibrium additionally makes every active firm's quoted price or cost a best response to all nonnegative unilateral deviations. These are Definitions 2.1–2.2 and 3.1–3.2.

A firm's ex-post net worth ei∗e_i^*ei∗​ combines original-order revenue, production and stock costs, rerouting revenue and cost, and back-order and replacement-supplier costs exactly as in equation (10). A firm defaults when its net worth is strictly negative. Starting with no undelivered orders or unserved demand, the update maps Φ∗\Phi^*Φ∗ and Ψ∗\Psi^*Ψ∗ mark all orders affected by firms that default after each market has reached its partial equilibrium. A market stable state is both the limit of that sequence and a fixed point of the update. A general equilibrium combines such a state with a partial equilibrium in every market (Definitions 3.3–3.4 and equation (18)).

Formalization targets

The goal is Proposition 4.3, stated on p. 24:

∃! (Π,K,Γ,Δ)  GeneralEquilibrium⁡(Π,K,Γ,Δ).\exists!\,(\Pi,K,\Gamma,\Delta)\;\operatorname{GeneralEquilibrium}(\Pi,K,\Gamma,\Delta).∃!(Π,K,Γ,Δ)GeneralEquilibrium(Π,K,Γ,Δ).

The quadruple consists of rerouting prices Π\PiΠ, switching costs KKK, undelivered orders Γ\GammaΓ, and unserved demand Δ\DeltaΔ. The claim includes existence and uniqueness of the full outcome, not merely of its default set. The milestone list follows the paper's dependency path: Propositions A.3 and A.6 identify the unique efficient allocations in the two markets; Propositions 4.1 and 4.2 identify their partial equilibria; Lemma A.7 states that greater disruption cannot increase any firm's partial-equilibrium net worth; and Lemma A.8 states that the default updates are bounded and increasing. The numbered results and their equations are in the E-Companion, EC pp. 4–12, and the main text, p. 22.

Significance

Proposition 4.3 makes the network's outcome a function of its order commitments, stocks, prices, market functions, and realized production costs. Later comparisons of network structures can therefore refer to the equilibrium without choosing among several price or default profiles. The result also separates local market choice from the way losses spread through the network: a firm can reroute or switch optimally and still fail once the effects of other failures are accounted for.

The paper proves the result in its E-Companion, EC pp. 12–13. This mission concerns a Lean statement of that known result and the reusable definitions needed to check a proof. The draft propositions are open proof obligations; this proposal does not claim machine-checked proofs of them. The two market allocation predicates, the default update, and the cascade limit can also support later formal work on the paper's resilience results.

Difficulty

The market and network conditions interact. An arbitrary fixed point of the default update need not be the state reached from zero; using only the fixed-point equation loses the uniqueness asserted by the paper. Conversely, knowing a cascade limit does not by itself show that the limit is fixed, because the update changes discontinuously when a firm's net worth crosses zero. At the market level, the price and switching-cost equilibria must be established from optimization and best-response conditions. Writing the formulas for the claimed equilibrium prices into those definitions would leave the central market claims unproved.

Formalization scope

Firms are Fin N and goods are Fin M, with N,M>0N,M>0N,M>0; the source numbers both from one, while Lean numbers them from zero. Orders and all default matrices are real valued and coordinatewise ordered. Active markets may be empty, as at the start of the cascade. Market objectives are ordinary real interval integrals over finite capacity boxes. The standing conditions include the paper's smoothness, concavity, and monotonicity assumptions on demand wherever it is positive and on the supply function, plus inverse identities and continuity on the quantity ranges used by the model. The inverse functions remain general data tied to dmd_mdm​ and sms_msm​; no linear demand or supply curve is imposed.

Several domain conventions make the displayed formulas meaningful. Assumption 2.1's minimum order is read over positive-order suppliers of a good; over all firms it would force zero safety stock whenever a nonsupplier exists. The inverse supply is nonnegative on feasible quantities, with sm(0)≤0s_m(0)\le0sm​(0)≤0, so the claimed switching cost belongs to the nonnegative strategy space. Demand inverse at zero is fixed to the reservation price. Assumptions 4.1–4.2 apply at each positive active-market total; for the general-equilibrium goal they are required for every binary 0/oijm0/o^m_{ij}0/oijm​ profile the cascade can visit. Differentiability at those totals is explicit. Initial equity and the order, stock, holding, rerouting, and back-order data are nonnegative; the realized net production cost can have either sign. The model uses the p. 23 convention for prices and costs outside active markets.

An efficient allocation remains an optimizer of equations (7) or (9), with proportional tie handling; a partial equilibrium remains a best response to every admissible deviation. The general equilibrium includes both the limit from zero and the fixed-point condition. These clauses exclude an equilibrium that is true by definition or a fixed point unrelated to the default cascade. The source's informal statement that every firm “supplies, consumes, or purchases” a good has no separate activity flag in this model; a firm with no internal order can still have outside production or consumption represented in cic_ici​. Milestone statements involving arbitrary disruption profiles restrict them to the feasible order box [0,O][0,O][0,O], where the market inverses are defined.

Selected references

  • John R. Birge, Agostino Capponi, and Peng-Chu Chen, Disruption and Rerouting in Supply Chain Networks, accepted manuscript dated October 31, 2022, SSRN 3669363; published in Operations Research, 2023, DOI 10.1287/opre.2022.2409.
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Information TheoryProbabilityRandom Matrix Theory·Captain: mikedeng1

Universality in Polytope Phase Transitions and Message Passing Algorithms 1: Polynomial AMP Iterates Have the Same Asymptotic Moments for All Sub-Gaussian Matrices with Equal Entry VariancesResearch Paper

Motivation

Approximate message passing (AMP) is a family of iterative algorithms driven by a large random matrix. It was introduced for compressed sensing by Donoho, Maleki and Montanari (PNAS 2009), and it is also used for low-rank matrix estimation, regression and spin-glass optimization. Its main appeal is that, for Gaussian random matrices, the empirical distribution of its iterates is tracked exactly in the large-dimensional limit by a scalar or low-dimensional recursion called state evolution. Bolthausen (CMP 2014) and Bayati and Montanari (IEEE Trans. Inf. Theory 2011) proved this for Gaussian matrices. Those proofs condition on the matrix through linear observations, and that conditioning argument works only for Gaussian entries.

In practice, and in the compressed-sensing phase transition that motivates the paper, the matrices are not Gaussian: Bernoulli, Rademacher and other sub-Gaussian ensembles are used. Bayati, Lelarge and Montanari (arXiv:1207.7321, Ann. Appl. Probab. 25(2), 2015) prove that the asymptotic behaviour of AMP with polynomial nonlinearities is universal: it depends on the law of the matrix entries only through their variances. This mission formalizes that universality theorem, Theorem 3 of the paper, together with the main steps of its proof.

Setting

Fix a dimension q≥1q \ge 1q≥1 and a degree bound d≥0d \ge 0d≥0. For each NNN, an AMP instance consists of three objects:

  • a symmetric matrix A∈RN×NA \in \mathbb R^{N\times N}A∈RN×N with Aii=0A_{ii} = 0Aii​=0;
  • polynomial maps fj(⋅ ;t):Rq→Rqf^j(\cdot\,; t):\mathbb R^q\to\mathbb R^qfj(⋅;t):Rq→Rq of degree at most ddd, one for each j∈[N]j\in[N]j∈[N] and each time t≥0t\ge 0t≥0;
  • an initial condition x0=(x10,…,xN0)x^0 = (x^0_1,\dots,x^0_N)x0=(x10​,…,xN0​) with xi0∈Rqx^0_i \in \mathbb R^qxi0​∈Rq.

The AMP orbit is

xit+1  =  ∑jAij fj(xjt;t)  −  ∑jAij2 ∂fj∂x(xjt;t) fi(xit−1;t−1),x^{t+1}_i \;=\; \sum_{j} A_{ij}\, f^j(x^t_j; t) \;-\; \sum_{j} A_{ij}^2\, \frac{\partial f^j}{\partial x}(x^t_j; t)\, f^i(x^{t-1}_i; t-1),xit+1​=j∑​Aij​fj(xjt​;t)−j∑​Aij2​∂x∂fj​(xjt​;t)fi(xit−1​;t−1),

where ∂fj/∂x\partial f^j/\partial x∂fj/∂x is the q×qq\times qq×q Jacobian. The second term, the memory or Onsager term, is absent at t=0t=0t=0. A sequence of random instances indexed by NNN is (C,d)(C,d)(C,d)-regular if it satisfies the following conditions:

  1. the entries AijA_{ij}Aij​, i<ji<ji<j, are independent and centered, and each is sub-Gaussian with scale factor C/NC/NC/N, that is, EeλAij≤eCλ2/(2N)\mathbb E e^{\lambda A_{ij}}\le e^{C\lambda^2/(2N)}EeλAij​≤eCλ2/(2N) for all real λ\lambdaλ;
  2. all coefficients of the polynomials are bounded by CCC;
  3. the matrix, the polynomials and the initial condition are mutually independent;
  4. ∑iexp⁡(∥xi0∥22/C)≤NC\sum_i \exp(\|x^0_i\|_2^2/C)\le NC∑i​exp(∥xi0​∥22​/C)≤NC.

The proof also uses an auxiliary message-passing iteration. It consists of messages zi→jt∈Rqz^t_{i\to j}\in\mathbb R^qzi→jt​∈Rq with zi→j0=xi0z^0_{i\to j}=x^0_izi→j0​=xi0​ and

zi→jt+1(r)=∑ℓ≠jAℓi frℓ(zℓ→it;t),zit+1(r)=∑ℓAℓi frℓ(zℓ→it;t).z^{t+1}_{i\to j}(r)=\sum_{\ell\neq j} A_{\ell i}\, f^\ell_r(z^t_{\ell\to i};t),\qquad z^{t+1}_{i}(r)=\sum_{\ell} A_{\ell i}\, f^\ell_r(z^t_{\ell\to i};t).zi→jt+1​(r)=ℓ=j∑​Aℓi​frℓ​(zℓ→it​;t),zit+1​(r)=ℓ∑​Aℓi​frℓ​(zℓ→it​;t).

Monomials are written xm=∏rx(r)m(r)x^m=\prod_r x(r)^{m(r)}xm=∏r​x(r)m(r) for m∈Nqm\in\mathbb N^qm∈Nq.

Formalization targets

Goal: Theorem 3 (p. 8)

Let (A(N),FN,x0,N)(A(N),\mathcal F_N,x^{0,N})(A(N),FN​,x0,N) and (A~(N),FN,x0,N)(\tilde A(N),\mathcal F_N,x^{0,N})(A~(N),FN​,x0,N) be two (C,d)(C,d)(C,d)-regular sequences. They share the polynomials and the initial condition, and EAij2=EA~ij2\mathbb E A_{ij}^2=\mathbb E\tilde A_{ij}^2EAij2​=EA~ij2​ for all i<ji<ji<j. Then for every ttt and every family of polynomials pN,i:Rq→Rp_{N,i}:\mathbb R^q\to\mathbb RpN,i​:Rq→R of degree at most ddd with coefficients bounded by BBB,

lim⁡N→∞1N∑i=1N{E pN,i(xit)−E pN,i(x~it)}=0.\lim_{N\to\infty}\frac1N\sum_{i=1}^N\Big\{\mathbb E\,p_{N,i}(x^t_i)-\mathbb E\,p_{N,i}(\tilde x^t_i)\Big\}=0 .N→∞lim​N1​i=1∑N​{EpN,i​(xit​)−EpN,i​(x~it​)}=0.

Milestones

  • Lemma 12 (p. 70): xs≤(s/e)sexx^s\le (s/e)^s e^xxs≤(s/e)sex for s,x>0s,x>0s,x>0.
  • (4.15) (p. 20): a sub-Gaussian variable with scale factor C/NC/NC/N satisfies E∣X∣s≤2Cs/2(s/e)s/2N−s/2\mathbb E|X|^s\le 2C^{s/2}(s/e)^{s/2}N^{-s/2}E∣X∣s≤2Cs/2(s/e)s/2N−s/2.
  • Proposition 1 (p. 16): ∣E(zit)m−E(z~it)m∣≤KN−1/2|\mathbb E(z^t_i)^m-\mathbb E(\tilde z^t_i)^m|\le KN^{-1/2}∣E(zit​)m−E(z~it​)m∣≤KN−1/2 for t≥1t\ge1t≥1.
  • Lemma 2, uniform bounds (pp. 22–23): ∣Ezit(r)m∣≤K|\mathbb E z^t_i(r)^m|\le K∣Ezit​(r)m∣≤K and ∣Ezi→jt(r)m∣≤K|\mathbb E z^t_{i\to j}(r)^m|\le K∣Ezi→jt​(r)m∣≤K.
  • Proposition 3 (p. 17), averaged over coordinates: 1N∑i∣E(xit)m−E(zit)m∣≤KN−1/2\frac1N\sum_i|\mathbb E(x^t_i)^m-\mathbb E(z^t_i)^m|\le KN^{-1/2}N1​∑i​∣E(xit​)m−E(zit​)m∣≤KN−1/2 for t≥1t\ge1t≥1. The page states the bound for each iii; that form fails when one coordinate of x0,Nx^{0,N}x0,N grows like log⁡N\sqrt{\log N}logN​, which Definition 4(3) permits, and the averaged form is what Theorem 3 needs.

In each milestone KKK depends only on C,d,q,t,mC,d,q,t,mC,d,q,t,m, as Note 2 of the paper specifies.

Significance

Theorem 3 lets results proved for Gaussian matrices be transferred to every sub-Gaussian ensemble with the same variance profile. In the paper, it is the first link of a chain:

  • Theorem 3 gives state evolution for general matrices (Theorem 4, the second mission of this series);
  • state evolution, together with an analysis of AMP as a solver of ℓ1\ell_1ℓ1​ minimization, gives the universality of the Donoho–Tanner phase transition for random projections of the cross-polytope (Theorem 2, the third mission).

The universality of the weak-neighborliness threshold for non-Gaussian matrices, observed numerically by Donoho and Tanner (Phil. Trans. R. Soc. A 2009), is a consequence of this chain.

The result has been proved since 2012. No machine-checked proof of it, or of any AMP state-evolution statement, is known to exist. The mission asks for a formalization of the published proof, or of any other argument. Two pieces of the proof are useful elsewhere: the absolute-moment bound for sub-Gaussian variables and the moment comparison of the message-passing iteration.

Difficulty

The first idea is a Lindeberg-type swap: replace the entries of AAA by those of A~\tilde AA~ one at a time and bound each change. This does not work directly. Every iterate xitx^t_ixit​ depends on all N(N−1)/2N(N-1)/2N(N−1)/2 entries through ttt nested polynomial layers. The memory term also couples consecutive iterates through the squares Aij2A_{ij}^2Aij2​. A single swap therefore changes every coordinate of every later iterate, and the per-swap errors have to be summed over Θ(N2)\Theta(N^2)Θ(N2) swaps with a total error of o(1)o(1)o(1).

Two features of the statement make it delicate. Only second moments of the entries are matched, so every contribution of higher moments of the entries must be shown to vanish in the limit. In addition, the AMP orbit is not itself a message-passing iteration: its moments match those of ztz^tzt (Proposition 3) only because of the memory term, and without that term they do not. A formal proof also has to establish finiteness of all the moments involved, which the paper takes for granted.

Formalization scope

Vectors in Rq\mathbb R^qRq are Fin q → ℝ, and indices are 0-based. A polynomial is given by its coefficient vector over the exponent vectors of total degree at most ddd, as in (4.10) of the paper. This keeps random polynomials in a measurable space. The Jacobian is the explicit sum of formal partial derivatives. A sorry-free sanity file checks it against the analytic derivative on an example and checks the memory term on a small instance.

The orbit is computed by recursion on (xt,xt−1)(x^t,x^{t-1})(xt,xt−1), with no memory term at t=0t=0t=0. The memory term uses Aij2A_{ij}^2Aij2​ itself, not its expectation 1/N1/N1/N. All random objects live on one probability space. The two sequences of Theorem 3 share one coefficient process and one initial condition.

Three readings of the printed Definition 4 are disclosed:

  • sub-Gaussianity is required for all real λ\lambdaλ (Mathlib's HasSubgaussianMGF), not only for λ>0\lambda > 0λ>0;
  • the scale factor is C/NC/NC/N, as the proof uses. The printed bracket (Cλ)2/(2N2)(C\lambda)^2/(2N^2)(Cλ)2/(2N2) would rule out every ensemble with variance 1/N1/N1/N once N>C2N > C^2N>C2, which would make the theorem vacuous;
  • the initial-condition bound holds almost surely for every NNN, not "with probability converging to one".

Every expectation appearing in a target is also asserted to be finite. Without that, a bound or a limit could hold only because Lean assigns the value 000 to the integral of a non-integrable function. Squared Euclidean norms are written as sums of squares, never as the sup norm that Mathlib puts on Fin q → ℝ. The deterministic identities of the tree expansion (Lemma 1, Lemma 3) and the first claim of Lemma 2 are not posed, because they need the labelled-tree families of Definition 6. Contributions of that tree machinery are welcome. Moment bounds for sub-Gaussian variables and polynomial moment estimates for sums of independent variables are reusable well beyond this mission.

Selected references

  • M. Bayati, M. Lelarge, A. Montanari, Universality in polytope phase transitions and message passing algorithms, Ann. Appl. Probab. 25(2):753–822, 2015. arXiv:1207.7321v2, DOI
  • D. L. Donoho, A. Maleki, A. Montanari, Message-passing algorithms for compressed sensing, PNAS 106(45):18914–18919, 2009. DOI
  • M. Bayati, A. Montanari, The dynamics of message passing on dense graphs, with applications to compressed sensing, IEEE Trans. Inf. Theory 57(2):764–785, 2011. DOI
  • E. Bolthausen, An iterative construction of solutions of the TAP equations for the Sherrington–Kirkpatrick model, Comm. Math. Phys. 325:333–366, 2014. DOI
  • D. L. Donoho, J. Tanner, Observed universality of phase transitions in high-dimensional geometry, Phil. Trans. R. Soc. A 367:4273–4293, 2009. DOI
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Operations ResearchOptimization·Captain: mikedeng1

Disruption and Rerouting in Supply Chain Networks II: A More Diversified Tiered Supply Chain Network Is More ResilientResearch Paper

Why order diversification matters

A firm can lose a planned input when one of its suppliers defaults. Safety stock can absorb some of that loss, while the rest becomes demand for replacement supply. A network with more buyer and supplier links spreads orders across more firms, but the resulting benefit depends on which firms default, how much each link carries, and the price of replacement supply. Birge, Capponi, and Chen study this interaction in a supply chain model with firm defaults, switched demand, and market prices. Their Theorem 5.1 asserts that a particular order-preserving form of diversification improves the network's resilience. This mission formalizes that comparison in the notation and conventions of the accepted manuscript, including its E-Companion proof.

The question is relevant to supply chain design because adding a link alone does not specify how much business moves to it. The theorem compares two networks that retain each firm's total incoming and outgoing order quantities. It therefore isolates the effect of redistributing those orders among more partners. The result concerns a precise resilience metric: the fraction of a network's baseline out-of-stock cost reduced by holding safety stock. It does not claim that diversification prevents all defaults or reduces every component of systemic loss.

Networks, defaults, and resilience

There are NNN firms and MMM goods. The order quantity oijmo^m_{ij}oijm​ is the amount of good mmm that firm iii promises to deliver to firm jjj. Good mmm has price pmp^mpm. Firm iii has initial equity wiw_iwi​ and a unit holding cost λim\lambda_i^mλim​ for safety stock of good mmm. Its realized net production cost is cic_ici​. Two networks AAA and BBB share prices, equity, holding costs, firms, and goods; their order quantities may differ. The source calls this five-part data a supply chain network, with a stock profile that is specialized here to a common scalar θ\thetaθ for the resilience comparison (§2, pp. 8–9; §5.1, p. 25).

A tiered network places each firm in a tier mi∈{1,…,M+1}m_i\in\{1,\ldots,M+1\}mi​∈{1,…,M+1}. A positive order of good mmm runs from tier mmm to tier m+1m+1m+1. Tier 1 firms supply good 1, tier M+1M+1M+1 firms buy good MMM, and every intermediate firm both buys and supplies its designated goods. The undirected graph underlying positive orders is connected. The model's supplier set UiU_iUi​ contains firms delivering good mi−1m_i-1mi​−1 to iii, and its buyer set LiL_iLi​ contains firms receiving good mim_imi​ from iii (§5.2–5.3, pp. 26–27).

For a common realization ccc and safety stock θ\thetaθ, the fundamental-default set D0(θ)D_0(\theta)D0​(θ) contains firms whose initial net worth is strictly negative:

D0(θ)={i:wi+∑m=1M(pm∑joijm−θλim)−ci<0}.D_0(\theta)=\left\{i: w_i+\sum_{m=1}^{M}\left(p^m\sum_j o^m_{ij}-\theta\lambda_i^m\right)-c_i<0\right\}.D0​(θ)={i:wi​+m=1∑M​(pmj∑​oijm​−θλim​)−ci​<0}.

The switched demand of firm iii for good mmm is σim(D0(θ),θ)=(∑k∈D0(θ)okim−θ)+\sigma_i^m(D_0(\theta),\theta)=\left(\sum_{k\in D_0(\theta)}o^m_{ki}-\theta\right)^+σim​(D0​(θ),θ)=(∑k∈D0​(θ)​okim​−θ)+. The inverse supply function sm−1s_m^{-1}sm−1​ prices the aggregate replacement demand for good mmm. Firm iii's cost ζi(θ)\zeta_i(\theta)ζi​(θ) sums holding cost and switched-demand cost over every good. The network's resilience ratio ζ(θ)\zeta(\theta)ζ(θ) is its aggregate reduction in this cost divided by aggregate cost at zero safety stock (§5.1, p. 25).

Formalization targets

For each firm, BBB is more diversified than AAA when total incoming and outgoing orders are unchanged, UiA⊆UiBU_i^A\subseteq U_i^BUiA​⊆UiB​ and LiA⊆LiBL_i^A\subseteq L_i^BLiA​⊆LiB​, and an expanded neighbor set divides orders into quantities no larger than the old quantities. Where a neighbor set is unchanged, its individual order quantities are unchanged. This is the complete condition of Definition 5.3, with the supplier good indexed as mi−1m_i-1mi​−1 as required by §5.2.

The goal is Theorem 5.1: for two tiered networks sharing their non-order data and tier assignment,

B more diversified than A⟹ζA(θ)≤ζB(θ)B\text{ more diversified than }A\quad\Longrightarrow\quad \zeta^A(\theta)\le\zeta^B(\theta)B more diversified than A⟹ζA(θ)≤ζB(θ)

for every admissible common safety stock θ\thetaθ and common realized production-cost vector ccc. The three milestones are the tier-grouped expression for total cost, its order comparison between AAA and BBB, and equality of their zero-stock baseline costs. They are the steps of the displayed chain in the E-Companion, EC p. 18, rather than separate numbered lemmas.

What the result establishes

The theorem gives an order-sensitive comparison of the paper's out-of-stock metric. It says that, under the stated redistribution constraints, the same amount of uniform safety stock offsets at least as large a fraction of baseline cost in the more diversified network. It supports comparisons of network designs with equal firm-level order totals. It does not rank networks with different equity, prices, or holding costs, and it does not address the paper's distinct contagion-based fragility metric (§5.1–5.3).

The result is proved in the paper; the open work here is its machine-checked formalization. The definitions of tiered order networks, fundamental defaults, switched demand, and the resilience ratio give reusable interfaces for later results about the same model. The draft Lean theorems state the full result and the three intermediate targets, with proofs left for solvers. The comparison also makes the paper's indexing and cost conventions explicit so those interfaces can be audited independently.

Where the difficulty lies

The default set depends on the order network, even though the two networks use the same realized costs. Thus a cost comparison cannot begin by treating defaulted firms as an unrelated common parameter. Moreover, switched demand takes a positive part after subtracting safety stock, and the inverse supply curve is evaluated at an aggregate across firms. Merely comparing individual orders or counting more links does not determine the resulting total cost. The final resilience ratio has a baseline-cost denominator that can be zero. The formalization has to cover that boundary case as well as positive baseline cost.

Formalization scope

Firms use Fin N; goods and tiers use the paper's one-based natural-number indices. Both NNN and MMM are positive. Orders and holding costs are nonnegative, prices are nonnegative, and initial equity is nonnegative (the source assumes every firm is initially solvent, p. 9). A tiered network has only consecutive-tier positive orders, has activity appropriate to every firm's tier, and has a connected underlying undirected graph. The two networks share ppp, www, λ\lambdaλ, the inverse supply curves, and the tier map. The source's tier-constant rerouting cost does not occur in the resilience metric and is not represented in these statements.

The paper prints Assumption 2.1 as a minimum over all firms. Since non-suppliers have zero orders, that literal reading would force θ=0\theta=0θ=0 and empty the theorem of its intended positive-stock content. The formalization reads the bound over actual suppliers, with θ≥0\theta\ge0θ≥0. It uses monotone inverse supply curves, as implied by Assumption 2.3, and explicitly requires their values to be nonnegative for nonnegative demand; the latter is an additional convention corresponding to nonnegative inverse supply prices. These choices appear in the definitions and in the statement audit notes.

The printed supplier-order superscript in Definition 5.3 uses mim_imi​, while §5.2 says firm iii buys good mi−1m_i-1mi​−1; the Lean definition uses the latter. The E-Companion's cost chain drops holding costs for goods a firm does not buy, although §5.1 sums them for all goods. The formalized cost and tier-grouped milestone retain the full sum. The paper states an almost-sure comparison under a random cost vector; its proof is pointwise, and the goal quantifies over every common realization. Each network computes its own default set. Lean sets 0/0=00/0=00/0=0, so a zero baseline cost requires no extra positive-denominator assumption. These conventions rule out a vacuous zero-stock reading or a cost formula weakened by omitting terms.

Selected references

  • J. R. Birge, A. Capponi, and P.-C. Chen, Disruption and Rerouting in Supply Chain Networks, accepted manuscript dated October 31, 2022, SSRN 3669363; Operations Research, 2023, DOI 10.1287/opre.2022.2409. The mission follows the manuscript's pagination and its E-Companion.
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Algorithmic Game TheoryEconomics·Captain: mikedeng1

Competitive Equilibrium with Indivisible Goods and Generic Budgets 2: Every Competitive Equilibrium Gives Each Agent Her ℓ-out-of-d Maximin Share for Every Rational ℓ/d at Most Her BudgetResearch Paper

Motivation

Competitive equilibrium is a way to divide goods when each participant has a budget reflecting her entitlement. With divisible goods, proportional value is a natural fairness target. Indivisible goods make that target unavailable in some markets: a single item cannot give two agents positive fractions of its value. The question becomes what fairness a market outcome can guarantee without dividing an item or assuming that agents value items additively. Babaioff, Nisan and Talgam-Cohen, §2.3 and §3 place this question in a discrete Fisher market, where budgets determine purchasing power but leftover money has no value to agents.

The paper introduces an ℓ\ellℓ-out-of-ddd maximin share to express the entitlement of an agent whose budget is at least ℓ/d\ell/dℓ/d. Its Proposition 3.2 says that every competitive equilibrium provides this share. The result applies to any number of agents and to arbitrary cardinal preferences; it does not require the additive assumptions used for the paper's equilibrium existence results. The same paper compares the conclusion with the earlier one-out-of-(n+1)(n+1)(n+1) guarantee for nearly equal budgets and explains that other rational shares can give a stronger benchmark in a given market. Babaioff, Nisan and Talgam-Cohen, §3.3

Setting

Let MMM be a finite set of indivisible items and NNN a finite set of agents. Agent iii has a valuation vi(S)v_i(S)vi​(S) for each bundle S⊆MS\subseteq MS⊆M and a positive budget bib_ibi​. The budgets are normalized by ∑i∈Nbi=1\sum_{i\in N}b_i=1∑i∈N​bi​=1. An allocation S=(Si)i∈NS=(S_i)_{i\in N}S=(Si​)i∈N​ partitions all items: each item belongs to exactly one agent's bundle. A price vector gives each item jjj a nonnegative real price pjp_jpj​, and the price of a bundle is p(S)=∑j∈Spjp(S)=\sum_{j\in S}p_jp(S)=∑j∈S​pj​. Babaioff, Nisan and Talgam-Cohen, §2.1–2.2

An allocated bundle SiS_iSi​ is demanded when it costs at most bib_ibi​ and every bundle that iii strictly prefers costs more than bib_ibi​. A competitive equilibrium (CE) is an allocation and price vector for which each agent demands her allocated bundle. Demand compares SiS_iSi​ with every subset of MMM, including bundles assigned to other agents and unions of several such bundles. Money is an allocation device in this model; an agent's valuation concerns her bundle alone. Babaioff, Nisan and Talgam-Cohen, Definition 2.1

For d>0d>0d>0 and 0≤ℓ≤d0\le\ell\le d0≤ℓ≤d, consider every partition (T1,…,Td)(T_1,\ldots,T_d)(T1​,…,Td​) of MMM into ddd labeled parts. Empty parts are permitted. For each partition, an adversary can leave the agent any ℓ\ellℓ parts, so the smallest value of a union of exactly ℓ\ellℓ parts is her guarantee for that partition. The agent chooses the partition that maximizes this worst-case value. This is her ℓ\ellℓ-out-of-ddd maximin share. The allocation SSS guarantees the share when vi(Si)v_i(S_i)vi​(Si​) is at least the resulting maximin value. Babaioff, Nisan and Talgam-Cohen, Theorem 1.2 and Definition 3.1

Formalization targets

Equilibrium fairness

For every agent iii, every competitive equilibrium, and every pair of natural numbers ℓ,d\ell,dℓ,d with d>0d>0d>0 and ℓ/d≤bi\ell/d\le b_iℓ/d≤bi​, the goal is Proposition 3.2:

vi(Si)≥max⁡(T1,…,Td)min⁡L⊆[d], ∣L∣=ℓvi ⁣(⋃t∈LTt).v_i(S_i)\ge \max_{(T_1,\ldots,T_d)} \min_{L\subseteq[d],\,|L|=\ell} v_i\!\left(\bigcup_{t\in L}T_t\right).vi​(Si​)≥(T1​,…,Td​)max​L⊆[d],∣L∣=ℓmin​vi​(t∈L⋃​Tt​).

The three milestones record the paper's intermediate claims in order: the total price of all items is at most the total budget; among ddd parts, some ℓ\ellℓ have price at most ℓ/d\ell/dℓ/d of the total; and a bundle an agent can afford is no better for her than the bundle she demands. The goal quantifies over every eligible rational share rather than selecting a single fixed denominator. Babaioff, Nisan and Talgam-Cohen, proof of Proposition 3.2

Related equilibrium properties

Two companions record the first welfare theorem, which makes a CE allocation Pareto optimal under strict preferences, and the appendix's coalition form of justified envy. The latter excludes the single case in which the comparing agent's bundle and the coalition's union are both empty, because the printed strict comparison is false there. These companions provide context for the equilibrium notion; neither changes the valuation generality of Proposition 3.2. Babaioff, Nisan and Talgam-Cohen, Theorem 2.4 and Claim A.8

Significance

The proposition gives a fairness conclusion conditional on equilibrium existence. It covers agents with different entitlements and nonadditive valuations, using a share that the agent herself evaluates through a partition of the items. The result does not assert that an equilibrium exists for every market. It says that any equilibrium already present meets all the stated rational-share benchmarks simultaneously. The paper uses this to relate competitive outcomes to maximin guarantees previously studied for nearly equal budgets. Babaioff, Nisan and Talgam-Cohen, §3

A machine-checked development would add a reusable account of finite allocations, bundle prices, demand, and maximin shares, plus a certified bridge between equilibrium and fairness. The draft Lean items in this mission are open statements with sorry; the local build checks their types and imports, not their mathematical proofs. The equivalence of the chosen maximin encoding with the finite max–min formula is checked separately in a sorry-free sanity file. Formal proofs of the goal and its milestones remain solver work.

Difficulty

The main formal issue is to keep the quantifiers and boundary cases aligned with the fairness definition. The guarantee concerns every partition into ddd parts, including empty parts, and the worst choice among subsets of exactly ℓ\ellℓ parts. A benchmark formed from one convenient partition, from at most ℓ\ellℓ parts, or from a restricted family of affordable bundles would have a different meaning. The total price comparison also depends on every item being allocated exactly once. The appendix companion has a separate edge case: strict envy cannot follow from demand when the two compared bundles coincide as the empty set.

Formalization scope

Items are Fin m, agents are Fin n, and valuations are real-valued functions on finite item sets. An allocation is a function from items to agents, so feasibility and market clearing are part of its type. A partition into ddd parts is a function from items to Fin d; it allows empty parts. Prices and budgets are real. The goal assumes positive budgets with sum one, nonnegative prices through the CE predicate, and d>0d>0d>0. The case ℓ=0\ell=0ℓ=0 is allowed; the budget condition implies ℓ≤d\ell\le dℓ≤d. The Lean maximin guarantee is written as a quantified comparison rather than using a real supremum or infimum, avoiding default values on empty extrema. A sanity theorem relates it to the finite max–min expression under its proper domain conditions.

The paper's normalization and arbitrary-preference scope are retained in the goal. Strict preferences are used only for the first-welfare and appendix companions. There, injective valuations exclude the paper's exception for identical items, and the appendix claim additionally excludes the case in which the comparing agent's bundle and the coalition's union are both empty. The mission's setting is repeated locally because no published platform definition has the same bundle market and budget conventions; the related housing, divisible-goods, and convex-economy models use different objects.

Contributions should preserve full market clearing, demand over every item bundle, nonnegative prices, all ddd-part partitions, and exactly ℓ\ellℓ selected parts. The definitions and finite averaging milestone can be reused in other fair-division developments. Proving the three source milestones and the goal, or improving the formal treatment of the appendix edge case, are within scope.

Selected references

  • M. Babaioff, N. Nisan, and I. Talgam-Cohen, Competitive Equilibrium with Indivisible Goods and Generic Budgets, Mathematics of Operations Research, 2021; arXiv:1703.08150v2, DOI:10.1287/moor.2020.1062. The mission cites the pinned preprint's pages and numbering.
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Mathematical Physics·Captain: Lucas

Weinberg 1967: A Model of Leptons — tree-level electroweak boson spectrumResearch Paper

Motivation

In A Model of Leptons (Weinberg, Phys. Rev. Lett. 19, 1264 (1967)) Steven Weinberg proposed that the photon and the intermediate bosons of the weak interaction are gauge fields of a single symmetry group, SU(2)×U(1)SU(2)\times U(1)SU(2)×U(1), and that the visible differences between them — the photon is massless, the weak bosons are heavy, and their couplings differ — come from a spontaneously broken symmetry of the vacuum rather than of the Lagrangian. The Goldstone bosons that such a breaking would normally produce are removed by the gauge fields (the Higgs–Englert–Brout–Guralnik–Hagen–Kibble mechanism). This model became the leptonic sector of the Standard Model of particle physics.

The paper is three pages long and its quantitative content is a short chain of finite-dimensional algebra: after the scalar field is replaced by its vacuum value, the gauge-boson mass terms form a quadratic form whose diagonalization gives the charged boson WWW, the neutral boson ZZZ and the massless photon, together with formulas for their masses, for the electric charge and for the weak coupling constant. This mission formalizes that chain.

Setting

The model has two gauge couplings ggg (for the isospin fields A⃗μ=(Aμ1,Aμ2,Aμ3)\vec A_\mu=(A^1_\mu,A^2_\mu,A^3_\mu)Aμ​=(Aμ1​,Aμ2​,Aμ3​)) and g′g'g′ (for the hypercharge field BμB_\muBμ​), and a complex scalar doublet φ\varphiφ whose vacuum expectation value is ⟨φ⟩=λ(10)\langle\varphi\rangle=\lambda\binom10⟨φ⟩=λ(01​) with λ\lambdaλ real. Replacing φ\varphiφ by ⟨φ⟩\langle\varphi\rangle⟨φ⟩ in the Lagrangian (eq. (4) of the paper) leaves the spin-one mass terms (eq. (7))

−18λ2g2[(Aμ1)2+(Aμ2)2]−18λ2(gAμ3+g′Bμ)2.-\tfrac18\lambda^2g^2\big[(A^1_\mu)^2+(A^2_\mu)^2\big]-\tfrac18\lambda^2\big(gA^3_\mu+g'B_\mu\big)^2 .−81​λ2g2[(Aμ1​)2+(Aμ2​)2]−81​λ2(gAμ3​+g′Bμ​)2.

At a fixed spacetime point we write the gauge fields as a vector V=(A1,A2,A3,B)∈R4V=(A^1,A^2,A^3,B)\in\mathbb R^4V=(A1,A2,A3,B)∈R4. The mass terms are then −12VTMV-\tfrac12V^{\mathsf T}\mathcal MV−21​VTMV for the symmetric mass-squared matrix

M=λ24(g20000g20000g2gg′00gg′g′2).\mathcal M=\frac{\lambda^2}{4}\begin{pmatrix}g^2&0&0&0\\0&g^2&0&0\\0&0&g^2&gg'\\0&0&gg'&g'^2\end{pmatrix}.M=4λ2​​g2000​0g200​00g2gg′​00gg′g′2​​.

A field of definite mass mmm is a linear combination c⋅Vc\cdot Vc⋅V whose coefficient vector ccc satisfies Mc=m2c\mathcal Mc=m^2cMc=m2c. The paper's candidates are

W=2−1/2(A1+iA2),Z=gA3+g′B(g2+g′2)1/2,A=−g′A3+gB(g2+g′2)1/2,W=2^{-1/2}(A^1+iA^2),\quad Z=\frac{gA^3+g'B}{(g^2+g'^2)^{1/2}},\quad A=\frac{-g'A^3+gB}{(g^2+g'^2)^{1/2}},W=2−1/2(A1+iA2),Z=(g2+g′2)1/2gA3+g′B​,A=(g2+g′2)1/2−g′A3+gB​,

with masses MW=12λgM_W=\tfrac12\lambda gMW​=21​λg, MZ=12λ(g2+g′2)1/2M_Z=\tfrac12\lambda(g^2+g'^2)^{1/2}MZ​=21​λ(g2+g′2)1/2, MA=0M_A=0MA​=0. The rationalized electric charge is e=gg′/(g2+g′2)1/2e=gg'/(g^2+g'^2)^{1/2}e=gg′/(g2+g′2)1/2, and the weak coupling constant GWG_WGW​ is defined by GW/2=g2/8MW2G_W/\sqrt2=g^2/8M_W^2GW​/2​=g2/8MW2​. The electron gets the mass Me=λGeM_e=\lambda G_eMe​=λGe​ from its Yukawa coupling GeG_eGe​. The electric charge in the paper's conventions is Q=T3−YQ=T_3-YQ=T3​−Y, where T3T_3T3​ is the third isospin component and Y=NR+12NLY=N_R+\tfrac12N_LY=NR​+21​NL​ the hypercharge.

Target

The goal theorem states, for g2+g′2>0g^2+g'^2>0g2+g′2>0:

Mw=MW2w,Mz=MZ2z,Ma=0,z⋅z=a⋅a=1, z⋅a=0,\mathcal Mw=M_W^2w,\qquad \mathcal Mz=M_Z^2z,\qquad \mathcal Ma=0,\qquad z\cdot z=a\cdot a=1,\ z\cdot a=0,Mw=MW2​w,Mz=MZ2​z,Ma=0,z⋅z=a⋅a=1, z⋅a=0,

where w,z,aw,z,aw,z,a are the coefficient vectors of W,Z,AW,Z,AW,Z,A, and, for all T3,YT_3,YT3​,Y and all field values,

gT3A3+g′YB=−e (T3−Y) A+g2T3+g′2Y(g2+g′2)1/2 Z,gT_3A^3+g'YB=-e\,(T_3-Y)\,A+\frac{g^2T_3+g'^2Y}{(g^2+g'^2)^{1/2}}\,Z,gT3​A3+g′YB=−e(T3​−Y)A+(g2+g′2)1/2g2T3​+g′2Y​Z,

so the massless field is the photon and it couples to Q=T3−YQ=T_3-YQ=T3​−Y with strength eee.

The milestones follow the paper's numbered equations: eq. (7) as a quadratic form; eqs. (8)–(9) (WWW and MWM_WMW​); eqs. (10), (12) (ZZZ and MZM_ZMZ​); eqs. (11), (13) (photon massless); the orthonormality of (10)–(11); eq. (15) (the charge); eq. (16) (GW/2=g2/8MW2=1/2λ2G_W/\sqrt2=g^2/8M_W^2=1/2\lambda^2GW​/2​=g2/8MW2​=1/2λ2); Ge=Me/λ=21/4MeGW1/2G_e=M_e/\lambda=2^{1/4}M_eG_W^{1/2}Ge​=Me​/λ=21/4Me​GW1/2​; g,g′>eg,g'>eg,g′>e; the parameter-free forms of the bounds MW>40M_W>40MW​>40 BeV, MZ>MWM_Z>M_WMZ​>MW​, MZ>80M_Z>80MZ​>80 BeV; and the tree-level vacuum condition λ2=M12/2h\lambda^2=M_1^2/2hλ2=M12​/2h.

Significance

The result itself. These formulas are the tree-level predictions that made the model testable: a massless photon, a charged WWW and a neutral ZZZ with MZ>MWM_Z>M_WMZ​>MW​, and the relations tying eee, GWG_WGW​, MWM_WMW​ and MZM_ZMZ​ to g,g′,λg,g',\lambdag,g′,λ. The existence of the neutral boson ZZZ (and its neutral currents) was the model's new prediction, later confirmed experimentally.

Formalizing it. The results are classical and fully proved on paper. The mission produces a machine-checked record of the paper's algebra, with every hypothesis stated (for example, that ggg and g′g'g′ are not both zero), and a reusable encoding of the electroweak boson mass matrix.

Difficulty

The mathematics is elementary; the difficulty lies in faithfulness. The paper's sign conventions are not fully consistent (substituting the vacuum value into eq. (4) as printed gives gA3−g′BgA^3-g'BgA3−g′B in the second mass term, while eq. (7) prints gA3+g′BgA^3+g'BgA3+g′B, which is the combination consistent with eq. (10)). The numerical claims (40 BeV, 80 BeV, 2.07×10−62.07\times10^{-6}2.07×10−6) depend on experimental inputs and on rounding. The formalization therefore takes eq. (7) as printed as its starting point and states the bounds in parameter-free form.

Formalization scope

  • Gauge-field configurations are vectors in R4\mathbb R^4R4 in the order (A1,A2,A3,B)(A^1,A^2,A^3,B)(A1,A2,A3,B); WWW uses C4\mathbb C^4C4. The mass matrix is given entrywise, and milestone eq. (7) connects it to the printed mass term.
  • The hypothesis g2+g′2>0g^2+g'^2>0g2+g′2>0 is imposed wherever ZZZ, AAA or eee must be nondegenerate: in Lean, division by zero returns 000, so for g=g′=0g=g'=0g=g′=0 these objects would silently be 000. Similarly GW=0G_W=0GW​=0 when λg=0\lambda g=0λg=0, so eq. (16) assumes g,λ≠0g,\lambda\neq0g,λ=0.
  • MWM_WMW​ and MZM_ZMZ​ are signed (12λg\tfrac12\lambda g21​λg without absolute value); mass statements are about squares.
  • Only stationarity is formalized for the vacuum condition, not the scalar masses. The Fierz-transformed eee–ν\nuν interaction and the fermion couplings of eq. (14) beyond the charge are not formalized.
  • All objects live in a single definition file, WeinbergLeptons_Model, in namespace WeinbergLeptons.

Selected references

  • S. Weinberg, A Model of Leptons, Phys. Rev. Lett. 19, 1264–1266 (1967). doi:10.1103/PhysRevLett.19.1264
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Bandit AlgorithmsMachine Learning·Captain: mikedeng1

An Optimal Algorithm for Stochastic and Adversarial Bandits III: α-Tsallis-INF With Gap-Tuned Asymmetric Regularization Has Logarithmic Pseudo-Regret When the Best Arm Is UniqueResearch Paper

Motivation

In the multi-armed bandit problem a learner repeatedly chooses one of KKK actions and observes only the loss of the action it chose. Two models of the environment dominate the literature. In the stochastic model the losses of each arm are drawn i.i.d. from a fixed distribution, and the optimal pseudo-regret grows like ∑i≠i∗log⁡(T)/Δi\sum_{i\ne i^*}\log(T)/\Delta_i∑i=i∗​log(T)/Δi​, where Δi\Delta_iΔi​ is the gap between the mean loss of arm iii and that of the best arm i∗i^*i∗ (Lai and Robbins, 1985). In the adversarial model the losses are arbitrary and the optimal rate is Θ(KT)\Theta(\sqrt{KT})Θ(KT​) (Audibert and Bubeck, 2010). Algorithms that are near-optimal in both models without knowing which one they face are called best of both worlds.

Timeline:

  • Bubeck and Slivkins (2012) gave the first best-of-both-worlds algorithm and asked whether one algorithm could be optimal in both regimes.
  • Seldin and Slivkins (2014) and Auer and Chiang (2016) obtained log⁡2T\log^2 Tlog2T or log⁡3T\log^3 Tlog3T stochastic rates with KT\sqrt{KT}KT​-type adversarial guarantees.
  • Wei and Luo (2018) introduced the stochastically constrained adversarial regime and the log-barrier algorithm BROAD.
  • Zimmert and Seldin (2021) showed that online mirror descent with the 12\tfrac1221​-Tsallis entropy (Tsallis-INF) is optimal in both regimes up to constants. Their Theorem 4, the subject of this mission, studies the whole family of α\alphaα-Tsallis regularizers with gap-dependent tuning in the stochastically constrained regime.

Setting

There are K≥2K\ge2K≥2 arms and rounds t=1,2,…t=1,2,\dotst=1,2,…. In round ttt the learner draws an arm ItI_tIt​ from a probability vector wtw_twt​ in the simplex ΔK−1\Delta^{K-1}ΔK−1, the environment fixes losses ℓt∈[0,1]K\ell_t\in[0,1]^Kℓt​∈[0,1]K, and only ℓt,It\ell_{t,I_t}ℓt,It​​ is observed. The environment may adapt to the past actions I1,…,It−1I_1,\dots,I_{t-1}I1​,…,It−1​ and use its own randomization, modelled by a seed ω\omegaω drawn once from a probability measure μ\muμ. The pseudo-regret is

Reg‾T=E[∑t=1Tℓt,It]−min⁡iE[∑t=1Tℓt,i],\overline{Reg}_T=\mathbb E\Big[\sum_{t=1}^T\ell_{t,I_t}\Big]-\min_i\mathbb E\Big[\sum_{t=1}^T\ell_{t,i}\Big],Reg​T​=E[t=1∑T​ℓt,It​​]−imin​E[t=1∑T​ℓt,i​],

with the expectation over the seed and the learner's draws; a minimizing arm is a best arm in hindsight iT∗i^*_TiT∗​.

α-Tsallis-INF is online mirror descent on the simplex. With α∈(0,1)\alpha\in(0,1)α∈(0,1), regularization parameters ξi>0\xi_i>0ξi​>0 and learning rates ηt>0\eta_t>0ηt​>0, set

Ψ(w)=−∑iwiα−αwiα(1−α)ξi,Ψt=Ψ/ηt.\Psi(w)=-\sum_i\frac{w_i^\alpha-\alpha w_i}{\alpha(1-\alpha)\xi_i},\qquad\Psi_t=\Psi/\eta_t .Ψ(w)=−i∑​α(1−α)ξi​wiα​−αwi​​,Ψt​=Ψ/ηt​.

The learner keeps importance-weighted loss estimates ℓ^t,i=1(It=i)ℓt,i/wt,i\hat\ell_{t,i}=\mathbb 1(I_t=i)\ell_{t,i}/w_{t,i}ℓ^t,i​=1(It​=i)ℓt,i​/wt,i​, their sums L^t\hat L_tL^t​, and plays wt=arg⁡max⁡w∈ΔK−1⟨w,−L^t−1⟩−Ψt(w)w_t=\arg\max_{w\in\Delta^{K-1}}\langle w,-\hat L_{t-1}\rangle-\Psi_t(w)wt​=argmaxw∈ΔK−1​⟨w,−L^t−1​⟩−Ψt​(w). The potential Φt(Y)=max⁡w∈ΔK−1⟨w,Y⟩−Ψt(w)\Phi_t(Y)=\max_{w\in\Delta^{K-1}}\langle w,Y\rangle-\Psi_t(w)Φt​(Y)=maxw∈ΔK−1​⟨w,Y⟩−Ψt​(w) splits the regret into a stability term E[∑tℓt,It+Φt(−L^t)−Φt(−L^t−1)]\mathbb E[\sum_t\ell_{t,I_t}+\Phi_t(-\hat L_t)-\Phi_t(-\hat L_{t-1})]E[∑t​ℓt,It​​+Φt​(−L^t​)−Φt​(−L^t−1​)] and a penalty term E[∑tΦt(−L^t−1)−Φt(−L^t)−ℓt,iT∗]\mathbb E[\sum_t\Phi_t(-\hat L_{t-1})-\Phi_t(-\hat L_t)-\ell_{t,i^*_T}]E[∑t​Φt​(−L^t−1​)−Φt​(−L^t​)−ℓt,iT∗​​].

In the stochastically constrained regime the loss differences have fixed means, E[ℓt,i−ℓt,i∗]=Δi\mathbb E[\ell_{t,i}-\ell_{t,i^*}]=\Delta_iE[ℓt,i​−ℓt,i∗​]=Δi​, with a unique best arm i∗i^*i∗ (Δi>0\Delta_i>0Δi​>0 for i≠i∗i\ne i^*i=i∗). Then Reg‾T=E[∑t∑i≠i∗wt,iΔi]\overline{Reg}_T=\mathbb E[\sum_t\sum_{i\ne i^*}w_{t,i}\Delta_i]Reg​T​=E[∑t​∑i=i∗​wt,i​Δi​] and iT∗=i∗i^*_T=i^*iT∗​=i∗. Write Δmin⁡=min⁡i≠i∗Δi\Delta_{\min}=\min_{i\ne i^*}\Delta_iΔmin​=mini=i∗​Δi​. Theorem 4 uses

ηt=16α4 1−tˉ−1+α(1−α)tα,tˉ=max⁡{e,t},ξi=Δi1−2α (i≠i∗),ξi∗=Δmin⁡1−2α.\eta_t=\frac{16^\alpha}{4}\,\frac{1-\bar t^{-1+\alpha}}{(1-\alpha)t^\alpha},\quad\bar t=\max\{e,t\},\qquad\xi_i=\Delta_i^{1-2\alpha}\ (i\ne i^*),\quad\xi_{i^*}=\Delta_{\min}^{1-2\alpha}.ηt​=416α​(1−α)tα1−tˉ−1+α​,tˉ=max{e,t},ξi​=Δi1−2α​ (i=i∗),ξi∗​=Δmin1−2α​.

Formalization targets

Goal: Theorem 4 (p. 12)

With T0=16Δmin⁡2log⁡216Δmin⁡2T_0=\frac{16}{\Delta_{\min}^2}\log^2\frac{16}{\Delta_{\min}^2}T0​=Δmin2​16​log2Δmin2​16​, for every T≥1T\ge1T≥1,

Reg‾T≤∑i≠i∗(8min⁡{11−α,log⁡T}+64)(log⁡T+1)Δi+16log⁡4(T0)Δmin⁡+4.\overline{Reg}_T\le\sum_{i\ne i^*}\frac{\big(8\min\{\frac1{1-\alpha},\log T\}+64\big)(\log T+1)}{\Delta_i}+\frac{16\log^4(T_0)}{\Delta_{\min}}+4 .Reg​T​≤i=i∗∑​Δi​(8min{1−α1​,logT}+64)(logT+1)​+Δmin​16log4(T0​)​+4.

Milestones

Lemma 17 (Hessian control along a mirror step); Lemma 11, cases 1 and 4 (instantaneous stability); Lemma 20 and Lemma 12, part 2 (penalty); Lemmas 14 and 16 (scalar inequalities for the learning-rate factors); displays (26) and (30) of Appendix D, the stability and penalty bounds under the parameters of Theorem 4.

Lemmas 20 and 12 cover any causal unbiased loss estimator satisfying the bandit feedback assumptions; the other bandit bounds use the importance-weighted estimator.

Significance

The theorem shows that the logarithmic stochastic rate is not special to the 12\tfrac1221​-Tsallis entropy: for every α∈(0,1)\alpha\in(0,1)α∈(0,1), tuning the regularizer to the gaps gives pseudo-regret of order ∑i≠i∗min⁡{11−α,log⁡T}log⁡T/Δi\sum_{i\ne i^*}\min\{\frac1{1-\alpha},\log T\}\log T/\Delta_i∑i=i∗​min{1−α1​,logT}logT/Δi​ in stochastically constrained environments. This places the log-barrier (α→0\alpha\to0α→0) and entropic (α→1\alpha\to1α→1) regularizers of earlier algorithms in one family, and isolates the role of asymmetric regularization. Unlike Theorem 1, it needs the gaps to tune ξ\xiξ, so it is a statement about the reach of the method rather than a practical algorithm.

The result is proved in the paper; no part of it has a machine-checked proof. Formalizing it produces a complete verified analysis of an online-mirror-descent bandit algorithm with time-varying, non-monotone learning rates, including the stability–penalty decomposition, the Hessian control of Lemma 17 and the explicit constant chase of Appendix D. The analysis also checks two points the paper leaves open: the printed bound has log⁡T\log TlogT where its proof gives log⁡T+1\log T+1logT+1, and Appendix D applies Lemma 12, which assumes non-increasing learning rates, to a rate that increases for a few early rounds when α\alphaα is small.

Difficulty

The obvious argument bounds each round's stability by ∑iηtξi2E[wt,i]1−α\sum_i\frac{\eta_t\xi_i}2\mathbb E[w_{t,i}]^{1-\alpha}∑i​2ηt​ξi​​E[wt,i​]1−α (Lemma 11, case 1) and sums. That bound contains the best arm, whose weight tends to one, so it grows polynomially in TTT and cannot give a logarithmic rate. The arm i∗i^*i∗ has to be removed from the stability, which needs a shifted second-order expansion where losses become slightly negative, and that is only controlled once ηtξi≤14\eta_t\xi_i\le\frac14ηt​ξi​≤41​ (Lemma 17). The early rounds before T0T_0T0​ must be paid for separately, and the asymmetric ξ\xiξ and the learning rate interact through constants that must be tracked exactly for the self-bounding step to close.

Formalization scope

Arms are Fin K with K≥2K\ge2K≥2 and the paper's arm iii is i - 1. Rounds start at 1; an action sequence is h : ℕ → Fin K with h 0 unused. The adversary is the published RegretBandits.Adversarial.Adversary (losses in [0,1][0,1][0,1] depending on past actions only) composed with a seed drawn from a probability measure, with losses measurable in the seed. Expectations are explicit: an integral over the seed of a finite sum over action paths weighted by ∏twt,It\prod_t w_{t,I_t}∏t​wt,It​​. The algorithm is an argmax predicate on the weight function, never a choice function. Φt\Phi_tΦt​ is a real supremum over the simplex. Logarithms are natural, and real powers are Real.rpow with nonnegative bases.

The goal takes α∈(0,1)\alpha\in(0,1)α∈(0,1); the endpoints α∈{0,1}\alpha\in\{0,1\}α∈{0,1}, where the paper's learning rate and regularizer are limits, are not stated. The regime "stochastically constrained with a unique best arm" is replaced by the two consequences the proof uses: the self-bounding inequality Reg‾T≥E[∑t∑i≠i∗wt,iΔi]\overline{Reg}_T\ge\mathbb E[\sum_t\sum_{i\ne i^*}w_{t,i}\Delta_i]Reg​T​≥E[∑t​∑i=i∗​wt,i​Δi​] and iT∗=i∗i^*_T=i^*iT∗​=i∗. Every such regime satisfies both, so the formal statement is at least as strong as the printed one. The constant log⁡T+1\log T+1logT+1 in the first term is the one the proof reaches. A trivial formalization is ruled out: the expectation is a genuine probability law, the gaps are tied to the losses through the self-bounding hypothesis, and the weights are determined by the algorithm, so the bound cannot hold vacuously.

A complete development needs the explicit law of a bandit run with an adaptive randomized adversary, unbiasedness of the IW estimator, convex conjugates and Bregman divergences on the simplex, and elementary real analysis for Lemmas 14 and 16. The run-law and the stability–penalty decomposition are reusable for any mirror-descent bandit algorithm. Proofs of any milestone, and of the scalar Lemmas 14 and 16 in particular, are welcome independently.

Selected references

  • J. Zimmert and Y. Seldin, Tsallis-INF: An Optimal Algorithm for Stochastic and Adversarial Bandits, Journal of Machine Learning Research 22(28), 2021. https://arxiv.org/abs/1807.07623 (v6)
  • S. Bubeck and A. Slivkins, The best of both worlds: stochastic and adversarial bandits, COLT 2012. https://arxiv.org/abs/1202.4473
  • C.-Y. Wei and H. Luo, More adaptive algorithms for adversarial bandits, COLT 2018. https://arxiv.org/abs/1801.03265
  • J. Abernethy, C. Lee and A. Tewari, Fighting bandits with a new kind of smoothness, NeurIPS 2015. https://arxiv.org/abs/1512.04152
  • T. L. Lai and H. Robbins, Asymptotically efficient adaptive allocation rules, Advances in Applied Mathematics 6(1), 1985. https://doi.org/10.1016/0196-8858(85)90002-8
  • J.-Y. Audibert and S. Bubeck, Regret bounds and minimax policies under partial monitoring, Journal of Machine Learning Research 11, 2010. https://jmlr.org/papers/v11/audibert10a.html
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Formal VerificationMathematical LogicTheory of Computation·Captain: mikedeng1

Monitoring Metric First-Order Temporal Properties: The Monitor M_Φ Outputs Exactly the Violations (¬Φ)^(D̄,τ̄,i) of a Bounded MFOTL Formula Φ, as Regular Sets, at Every Time Point iResearch Paper

Motivation

Runtime monitoring checks a running system against a specification by inspecting its trace of events as it is produced. Policies on data, such as "every published report was approved within the last 10 days" or "each value stored in in reaches out within 5 time units", quantify over data values and constrain the time between events. Metric first-order temporal logic (MFOTL) expresses such policies: it extends first-order logic with past and future temporal operators that carry intervals of allowed time differences.

Basin, Klaedtke, Müller and Zălinescu (J. ACM 62(2), Article 15, 2015) give a monitor for MFOTL properties □Φ\square\Phi□Φ with Φ\PhiΦ bounded. It allows negation and quantification over the infinite domain N\mathbb NN without restriction, because every relation it manipulates is represented by a finite automaton: the input structures are automatic structures. The paper implements it in the prototype tool MonPoly-Reg (§6). Its correctness rests on Theorem 3.9: the monitor reports exactly the violations of Φ\PhiΦ, at every time point.

Setting

A signature S=(C,R,ι)S=(C,R,\iota)S=(C,R,ι) has finitely many constants and predicates with arities. Formulas are built from t≈t′t\approx t't≈t′ and r(t1,…,tι(r))r(t_1,\dots,t_{\iota(r)})r(t1​,…,tι(r)​) by ¬\neg¬, ∨\vee∨, ∃x\exists x∃x and the temporal operators ∙I\bullet_I∙I​ (previous), ∘I\circ_I∘I​ (next), SI\mathsf S_ISI​ (since) and UI\mathsf U_IUI​ (until), where I=[b,b′)I=[b,b')I=[b,b′) is a nonempty interval of N\mathbb NN with b′∈N∪{∞}b'\in\mathbb N\cup\{\infty\}b′∈N∪{∞}. A formula is bounded if every UI\mathsf U_IUI​ in it has b′<∞b'<\inftyb′<∞.

A temporal structure (Dˉ,τˉ)(\bar{\mathcal D},\bar\tau)(Dˉ,τˉ) assigns to each time point i∈Ni\in\mathbb Ni∈N relations rDi⊆Nι(r)r^{\mathcal D_i}\subseteq\mathbb N^{\iota(r)}rDi​⊆Nι(r) and a time stamp τi∈N\tau_i\in\mathbb Nτi​∈N; constants are rigid, τ0≤τ1≤⋯\tau_0\le\tau_1\le\cdotsτ0​≤τ1​≤⋯, and τˉ\bar\tauτˉ exceeds every bound. Satisfaction (Dˉ,τˉ,v,i)⊨φ(\bar{\mathcal D},\bar\tau,v,i)\models\varphi(Dˉ,τˉ,v,i)⊨φ is Definition 2.2; for example ψ UI ψ′\psi\,\mathsf U_I\,\psi'ψUI​ψ′ holds at iii if ψ′\psi'ψ′ holds at some j≥ij\ge ij≥i with τj−τi∈I\tau_j-\tau_i\in Iτj​−τi​∈I and ψ\psiψ holds at all k∈[i,j)k\in[i,j)k∈[i,j). For φ\varphiφ with free variables x1<⋯<xnx_1<\dots<x_nx1​<⋯<xn​, the satisfying set is

φ(Dˉ,τˉ,i)={dˉ∈Nn∣(Dˉ,τˉ,v[xˉ↦dˉ],i)⊨φ for some v}.\varphi^{(\bar{\mathcal D},\bar\tau,i)}=\{\bar d\in\mathbb N^n\mid(\bar{\mathcal D},\bar\tau,v[\bar x\mapsto\bar d],i)\models\varphi\ \text{for some }v\}.φ(Dˉ,τˉ,i)={dˉ∈Nn∣(Dˉ,τˉ,v[xˉ↦dˉ],i)⊨φ for some v}.

A domain representation is a regular language L\mathcal LL over a finite alphabet with a surjection ν:L→N\nu:\mathcal L\to\mathbb Nν:L→N whose equality relation is regular. A relation A⊆NkA\subseteq\mathbb N^kA⊆Nk is regular if the words u1⊗⋯⊗uku_1\otimes\cdots\otimes u_ku1​⊗⋯⊗uk​ (the letter-by-letter convolution, padded with #\##) with (ν(u1),…,ν(uk))∈A(\nu(u_1),\dots,\nu(u_k))\in A(ν(u1​),…,ν(uk​))∈A form a regular language.

The monitor MΦ\mathsf M_\PhiMΦ​ (Fig. 2) reads (D0,τ0),(D1,τ1),…(\mathcal D_0,\tau_0),(\mathcal D_1,\tau_1),\dots(D0​,τ0​),(D1​,τ1​),… one element per loop iteration. It extends each Dj\mathcal D_jDj​ to D^j\hat{\mathcal D}_jD^j​ with auxiliary relations pαp_\alphapα​ (and rαr_\alpharα​, sαs_\alphasα​ for since and until) for every temporal subformula α\alphaα, built incrementally by the constructions of §3.4 once a list QQQ of pending triples (α,j,S)(\alpha,j,S)(α,j,S) says that enough of the future has been read. When D^i\hat{\mathcal D}_iD^i​ is complete it outputs the set (¬Φ^)D^i(\neg\hat\Phi)^{\hat{\mathcal D}_i}(¬Φ^)D^i​ with τi\tau_iτi​, where Φ^\hat\PhiΦ^ is Φ\PhiΦ with each top-level temporal subformula α\alphaα replaced by the atom pα(xˉ)p_\alpha(\bar x)pα​(xˉ).

Formalization targets

Goal: Theorem 3.9

For every input satisfying the restrictions of §3.1 and every bounded Φ\PhiΦ:

(i)(n,O,t) output by line 9 ⟹ O=(¬Φ)(Dˉ,τˉ,n), O regular, t=τn;\text{(i)}\quad (n,O,t)\ \text{output by line 9}\ \Longrightarrow\ O=(\neg\Phi)^{(\bar{\mathcal D},\bar\tau,n)},\ O\ \text{regular},\ t=\tau_n;(i)(n,O,t) output by line 9 ⟹ O=(¬Φ)(Dˉ,τˉ,n), O regular, t=τn​; (ii)∀n∈N,n=0 or some output at index n−1 occurs,\text{(ii)}\quad \forall n\in\mathbb N,\quad n=0\ \text{or some output at index }n-1\text{ occurs},(ii)∀n∈N,n=0 or some output at index n−1 occurs,

where each output is followed by line 11 setting iii to the next index. This records counter values reached inside the while loop, including values that may never appear at a loop entry. Part (ii) excludes the vacuous reading of (i).

Milestones

  1. Lemma 3.4: φ^D^i=φ(Dˉ,τˉ,i)\hat\varphi^{\hat{\mathcal D}_i}=\varphi^{(\bar{\mathcal D},\bar\tau,i)}φ^​D^i​=φ(Dˉ,τˉ,i) once the auxiliary relations of tsub(φ)\mathit{tsub}(\varphi)tsub(φ) are correct, and regularity is preserved.
  2. Lemmas 3.5–3.8: the constructions for ∙I\bullet_I∙I​, ∘I\circ_I∘I​, SI\mathsf S_ISI​ and bounded UI\mathsf U_IUI​ produce regular relations equal to the satisfying sets, with the stated characterizations of rαr_\alpharα​ and sαs_\alphasα​.
  3. Observations (1)–(3) of the proof of Theorem 3.9 on the list QQQ and the counter iii.
  4. The claim that line 7 can always be executed, in the form: if (α,j,∅)∈Qk(\alpha,j,\emptyset)\in Q_k(α,j,∅)∈Qk​ then the build stores pαD^j=α(Dˉ,τˉ,j)p_\alpha^{\hat{\mathcal D}_j}=\alpha^{(\bar{\mathcal D},\bar\tau,j)}pαD^j​​=α(Dˉ,τˉ,j), which is regular.

Significance

Theorem 3.9 makes MΦ\mathsf M_\PhiMΦ​ a sound and complete monitor for the safety fragment □Φ\square\Phi□Φ, Φ\PhiΦ bounded: every violation at every time point is reported, nothing else is, and every output is a finitely represented (regular) set even though it may be infinite. It covers unrestricted negation and quantification, which finite-relation monitors (§4 of the paper) cannot handle. The incremental constructions of §3.4 are the template reused by later MFOTL monitors.

The paper gives a mathematical proof of its monitor's correctness. This mission asks for a Lean proof that checks the MFOTL semantics, automatic relations over N\mathbb NN, and the correctness of this particular monitor, including the until construction whose printed version is defective (see Formalization scope).

Difficulty

Two parts are hard. The regularity claims need the fundamental property of automatic structures: first-order definable relations are regular, which requires closure of padded convolution languages under Boolean operations, cylindrification, permutation of tracks and projection, the last with removal of trailing padding. The arithmetic constraints of the since and until constructions additionally need successor and offset relations definable from ≺\prec≺.

The scheduling argument is the other part. Correctness of a build at (α,j)(\alpha,j)(α,j) requires that every input relation, at time points up to j+ℓjj+\ell_jj+ℓj​ for until, was built before and not discarded since. Following only the syntax of α\alphaα does not settle this: a needed relation for a subformula at a later time point may be built in the same iteration as α\alphaα's.

Formalization scope

The domain is N\mathbb NN, as §3.1 assumes. Relations are sets of lists of natural numbers, ordered by the sorted free variables. Interval upper bounds are in N∞\mathbb N_\inftyN∞​; intervals carry the proof that they are nonempty. The representation (L,ν)(\mathcal L,\nu)(L,ν) is a single parameter shared by the hypothesis "every rDir^{\mathcal D_i}rDi​ is regular" and the regularity claims of the conclusions; it is never chosen existentially. The binary predicate ≺\prec≺ interpreted as <<< is a hypothesis.

Two hypotheses on Φ\PhiΦ besides boundedness are the paper's own "without loss of generality" assumptions: each temporal subformula occurs once in Φ\PhiΦ (§3.6), and the direct subformulas of each SI\mathsf S_ISI​, UI\mathsf U_IUI​ subformula have the same free variables (§3.4; achieved by padding with x≈xx\approx xx≈x, as in §3.5). No other restriction is placed on Φ\PhiΦ.

The printed until construction (§3.4.4) is repaired: the guard of UrU_rUr​ is "aˉ∈β^D^i+k\bar a\in\hat\beta^{\hat{\mathcal D}_{i+k}}aˉ∈β^​D^i+k​ for all ℓi−1≤k≤ℓi\ell_{i-1}\le k\le\ell_iℓi−1​≤k≤ℓi​", since the printed guard empties rαr_\alpharα​ in the paper's own example of §3.5; UsU_sUs​ keeps only tuples with j′≥1j'\ge1j′≥1, since otherwise a γ\gammaγ-witness at time point i−1i-1i−1 survives to time point iii when τi=τi−1\tau_i=\tau_{i-1}τi​=τi−1​; and time-stamp equations are encoded additively. Lemma 3.8(i) reads aˉ∈Nn\bar a\in\mathbb N^naˉ∈Nn and adds j≤ℓij\le\ell_ij≤ℓi​. "Effectively computable" in Theorem 3.9(i) is not formalized. Part (ii) uses the output at index n−1n-1n−1 as the record of the line-11 increment to nnn; for n=0n=0n=0, the counter is initialized by line 2. Loop-entry states alone can skip counter values reached within one iteration.

The monitor is a state machine whose builds and outputs are computed only from its store of relations; it never consults the satisfaction relation or satisfying sets. A formalization in which line 7 reads the semantics would turn Theorem 3.9(i) into a restatement of Lemma 3.4, and is ruled out. A build whose input is missing stores nothing, so a monitor that silently fails would violate (ii).

Contributions welcome: the theory of automatic relations (reusable beyond this mission), the semantic halves of Lemmas 3.4–3.8, and the scheduling invariants.

Selected references

  • D. Basin, F. Klaedtke, S. Müller, E. Zălinescu, Monitoring metric first-order temporal properties, J. ACM 62(2), Article 15, 2015. https://doi.org/10.1145/2699444
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The Endpoint Distribution of Directed Polymers 1: In the Low-Temperature Phase the Endpoint Distribution Is Asymptotically Purely Atomic, and at High Temperature It Is NotResearch Paper

Motivation

A directed polymer in a random environment is a random walk whose paths are weighted by the disorder they encounter. The walk favors paths with large accumulated weight, and its endpoint distribution can concentrate on a small number of sites even though the number of possible paths grows exponentially. Understanding how much probability remains spread across many small endpoint masses is a basic question about localization. The distinction matters especially beyond exactly solvable polymer models, where explicit formulas for the endpoint law are rarely available. Bates and Chatterjee study this question for independent disorder in every spatial dimension d≥1d\geq1d≥1 under a finite exponential-moment condition Bates and Chatterjee, 2021.

The paper separates two temperature regimes using the limiting free energy. Earlier localization statements detected persistent large atoms. The target here asks whether those atoms account for all endpoint probability in a time-averaged sense. It also specifies the complementary high-temperature behavior, where a suitable vanishing mass threshold captures asymptotically none of the probability. The result is Theorem 1.1 of the preprint, restated as Theorem 6.3 Bates and Chatterjee, 2021, pp. 16, 43.

Setting

Fix d≥1d\geq1d≥1. A path starts at the origin in Zd\mathbb Z^dZd and makes one of its 2d2d2d nearest-neighbor moves at each integer time. The environment (Xi,x)(X_{i,x})(Xi,x​) consists of independent, identically distributed real random variables with common law L\mathfrak LL. The disorder law is nondegenerate: it is not concentrated at one number. An inverse temperature β≥0\beta\geq0β≥0 determines the weight of a path γ\gammaγ of length nnn:

wβ(γ)=exp⁡ ⁣(β∑i=1nXi,γ(i)),Zn=(2d)−n∑γwβ(γ).w_\beta(\gamma)=\exp\!\left(\beta\sum_{i=1}^{n}X_{i,\gamma(i)}\right),\qquad Z_n=(2d)^{-n}\sum_{\gamma}w_\beta(\gamma).wβ​(γ)=exp(βi=1∑n​Xi,γ(i)​),Zn​=(2d)−nγ∑​wβ​(γ).

The endpoint mass function fn(x)f_n(x)fn​(x) is the sum of weights of paths ending at xxx, divided by the sum of all path weights. Thus fnf_nfn​ is a probability mass function on Zd\mathbb Z^dZd. For ε>0\varepsilon>0ε>0, the ε\varepsilonε-atoms are the sites Anε={x:fn(x)>ε}\mathcal A_n^\varepsilon=\{x:f_n(x)>\varepsilon\}Anε​={x:fn​(x)>ε}, and ρn(ωn∈Anε)\rho_n(\omega_n\in\mathcal A_n^\varepsilon)ρn​(ωn​∈Anε​) is their total mass. The strict inequality matters at a threshold equal to an atom mass.

Write Fn=log⁡Zn/nF_n=\log Z_n/nFn​=logZn​/n for n≥1n\geq1n≥1, with F0=0F_0=0F0​=0, and λ(α)=log⁡ELeαX\lambda(\alpha)=\log\mathbb E_{\mathfrak L}e^{\alpha X}λ(α)=logEL​eαX. The standing condition is that this exponential moment is finite for every α∈[−2β,2β]\alpha\in[-2\beta,2\beta]α∈[−2β,2β]. The paper's Theorem A characterizes the high-temperature phase by lim⁡nEFn=λ(β)\lim_n\mathbb E F_n=\lambda(\beta)limn​EFn​=λ(β) and the low-temperature phase by lim⁡nEFn<λ(β)\lim_n\mathbb E F_n<\lambda(\beta)limn​EFn​<λ(β) Bates and Chatterjee, 2021, pp. 4–5.

Formalization targets

Asymptotic pure atomicity

The goal is both clauses of Theorem 1.1. For every positive deterministic sequence εi→0\varepsilon_i\to0εi​→0, low temperature gives

1n∑i=0n−1ρi(ωi∈Aiεi)⟶1almost surely.\frac1n\sum_{i=0}^{n-1}\rho_i(\omega_i\in\mathcal A_i^{\varepsilon_i})\longrightarrow1 \quad\text{almost surely}.n1​i=0∑n−1​ρi​(ωi​∈Aiεi​​)⟶1almost surely.

At high temperature there exists a positive deterministic sequence εi→0\varepsilon_i\to0εi​→0 for which the same average converges almost surely to 000. The sequence in this second clause is selected independently of the realized environment. Together the clauses characterize the paper's stronger, almost-sure form of asymptotic pure atomicity Bates and Chatterjee, 2021, Theorems 1.1 and 6.3.

The milestones are fifteen statements of the paper, in the order the proof of the goal uses them:

  • the triangle inequality for the distance ddd on partitioned subprobability measures (Lemma 2.3) and sequential compactness of (S,d)(\mathcal S,d)(S,d) (Theorem 2.8);
  • continuity of the update law f↦Tff\mapsto\mathcal Tff↦Tf into (P(S),W)(\mathcal P(\mathcal S),\mathcal W)(P(S),W) and of the log moments f↦Elog⁡qF~f\mapsto\mathbb E\log^q\widetilde Ff↦ElogqF (Proposition 3.2);
  • convergence of the empirical endpoint measures μn=1n∑i<nδfi\mu_n=\frac1n\sum_{i<n}\delta_{f_i}μn​=n1​∑i<n​δfi​​ to the fixed-point set K\mathcal KK (Corollary 4.3); invariant laws charge only states of mass 000 or 111 (Proposition 4.4);
  • the variational formula for the free energy: ∣Fn−R(μn)∣→0|F_n-\mathcal R(\mu_n)|\to0∣Fn​−R(μn​)∣→0 (Proposition 4.5), the lower bound (Proposition 4.6), the key inequality ∑i<nR(Tiδf0)≥Elog⁡Zn\sum_{i<n}\mathcal R(\mathcal T^i\delta_{f_0})\ge\mathbb E\log Z_n∑i<n​R(Tiδf0​​)≥ElogZn​ (Lemma 4.8), and lim⁡Fn=inf⁡ν∈KR(ν)\lim F_n=\inf_{\nu\in\mathcal K}\mathcal R(\nu)limFn​=infν∈K​R(ν) (Theorem 4.7);
  • convergence of μn\mu_nμn​ to the minimizing set M\mathcal MM (Theorem 4.9), the extrema of RRR (Lemma 5.1) and the fixed-point characterization of the two phases (Theorem 5.2);
  • semicontinuity of the atom functionals (Lemma 6.1), a fixed-threshold criterion for pure atomicity (Lemma 6.2), and a Dini theorem for semicontinuous functions (Lemma 6.4).

Significance

The low-temperature conclusion rules out a residual diffuse component in the time-averaged endpoint law. A vanishing threshold may still be used to collect almost all of the polymer's probability. The high-temperature clause shows that this property distinguishes the phases under the stated moment assumption. The result strengthens a statement that only asks for a positive amount of mass on large atoms, and gives an almost-sure conclusion for the Cesàro averages Bates and Chatterjee, 2021, §§1.2.3, 6.

A formal development would supply a reusable compactification of endpoint probability measures and a checked route from its invariant laws to localization observables. The milestones expose the pieces that need separate verification, and the compactification and variational formula are reusable for the companion mission on geometric localization. The paper proves the mathematical theorem; this mission asks for its Lean proof and the supporting definitions. A compiled statement with sorry is a proof obligation, not a completed machine-checked result.

Difficulty

The endpoint distribution may move through space as time grows, so ordinary pointwise convergence of mass functions does not capture concentration. The compact state space used by the paper permits separated clusters to live on different copies of Zd\mathbb Z^dZd. Its distance identifies translated representatives and loses information about remote mass. A direct application of weak convergence to the event f(x)>εf(x)>\varepsilonf(x)>ε also fails at a threshold, because the mass-above-threshold functional is not continuous. The proof must handle its one-sided semicontinuity and the limiting behavior of the update law Bates and Chatterjee, 2021, §§2–3, 6.

Formalization scope

Lean represents sites as Fin d → ℤ and paths as finite step sequences, so the starting point, the 2d2d2d choices per step, and the normalization of ZnZ_nZn​ are explicit. An environment is a measurable independent family on a probability space with common law L\mathfrak LL. The unused time-zero row comes from indexing cells by N\mathbb NN; only rows with index at least one enter the polymer. The moment condition includes the full interval [−2β,2β][-2\beta,2\beta][−2β,2β], and the disorder law must be nondegenerate. Both phase predicates refer to the canonical product environment, making the classification depend on L\mathfrak LL, ddd, and β\betaβ rather than on an arbitrary realization.

Partitioned subprobability measures are structures of nonnegative summable functions with mass at most one. Their topology is generated by the paper's distance balls. The Borel representation identifies states at distance zero, corresponding to the paper's separation quotient S\mathcal SS. Finite partial isometries carry the degree penalty 2−deg⁡φ2^{-\deg\varphi}2−degφ through an infimum over admissible degrees. The update uses an extended nonnegative sum before conversion to a real denominator. The intended probability law requires the almost-sure finiteness of that denominator and measurability of the update. The real-valued energy integrals require the stated moment condition; a default value for a nonintegrable integral cannot serve as the paper's expectation, and a non-measurable update would make the pushforward Tf\mathcal TfTf the zero measure, which is not the paper's object either. The infimum inf⁡ν∈KR(ν)\inf_{\nu\in\mathcal K}\mathcal R(\nu)infν∈K​R(ν) is taken over the set K\mathcal KK itself, never as a real infimum whose empty inner range defaults to 000. The intermediate results in §§3–4 and Lemma 5.1 use the standing β>0\beta>0β>0 range. Theorems 1.1 and 5.2 explicitly include β=0\beta=0β=0. Wasserstein cost imports the published RWPI.SqrtLasso.transportCost definition.

Solvers can contribute proofs of the compactness, continuity, variational-formula, invariant-law, and atom-functional milestones, or of reusable supporting results such as Lemma 2.11 (measurability of the update) and Corollary 2.5 (when d(f,g)=0d(f,g)=0d(f,g)=0). The strict positivity of thresholds, nondegenerate disorder, genuine probability laws, and full phase hypotheses are essential: removing any of them could make a formally easy statement unrelated to Theorem 1.1.

Selected references

  • Erik Bates and Sourav Chatterjee, The endpoint distribution of directed polymers, Annals of Probability 48 (2020); preprint arXiv:1612.03443v5 (2021). Preprint.
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Machine LearningProbabilityStatistics·Captain: mikedeng1

Distribution-Free, Risk-Controlling Prediction Sets III: Thresholding the Conditional Expected Loss Gives the Smallest Sets Among Predictors of No Larger Risk (Theorem 8)Research Paper

Motivation

A set-valued predictor returns, for each input xxx, a set of plausible responses rather than a single guess. Such sets are used wherever a model's output feeds a decision with asymmetric costs: a medical classifier that lists every diagnosis it cannot rule out, a segmentation model that marks every pixel that may belong to a tumour, a protein-structure predictor that reports a range of distances. Bates, Angelopoulos, Lei, Malik and Jordan, Distribution-Free, Risk-Controlling Prediction Sets (J. ACM 68(6), 2021), calibrate a nested family of such predictors {Tλ}\{\mathcal T_\lambda\}{Tλ​} so that a chosen loss is controlled with high probability, without distributional assumptions.

Calibration says nothing about which family to calibrate. Any nested family can be made risk-controlling; families differ in how large their sets are, and large sets are uninformative. §4 of the paper asks which family is best in the population: which predictor achieves a given risk with the smallest expected set size. For a weighted miscoverage loss (Theorem 7, §4.2) the answer thresholds a weighted conditional density, in the spirit of the optimality results of Sadinle, Lei and Wasserman (2019) for classification. Theorem 8 (§4.3) extends the answer to every loss of integral form. This mission formalizes Theorem 8.

Setting

Let (X,Y)(X, Y)(X,Y) take values in X×Y\mathcal X \times \mathcal YX×Y with law PPP, marginal PXP_XPX​, and conditional law κ(x)\kappa(x)κ(x) of YYY given X=xX = xX=x. Prediction sets are subsets of a measurable space Z\mathcal ZZ (in the paper's examples Z=Y\mathcal Z = \mathcal YZ=Y). A set-valued predictor is a map T:X→2Z\mathcal T : \mathcal X \to 2^{\mathcal Z}T:X→2Z.

Fix a finite measure μ\muμ on Z\mathcal ZZ and a nonnegative cost ℓ:Y×Z→[0,∞)\ell : \mathcal Y \times \mathcal Z \to [0, \infty)ℓ:Y×Z→[0,∞); ℓ(y,z)\ell(y, z)ℓ(y,z) is the cost of leaving zzz out of the prediction set when the true response is yyy. The loss of a set S\mathcal SS is the total cost of what it leaves out,

L(y;S)=∫z∈Scℓ(y,z) dμ(z),L(y; \mathcal S) = \int_{z \in \mathcal S^c} \ell(y, z)\, d\mu(z),L(y;S)=∫z∈Sc​ℓ(y,z)dμ(z),

and the risk of a predictor is R(T)=E[L(Y;T(X))]R(\mathcal T) = \mathbb E[L(Y; \mathcal T(X))]R(T)=E[L(Y;T(X))] (§2.1). Larger sets have smaller loss. The conditional expected cost of omitting zzz at xxx is

E[ℓ(Y;z)∣X=x]=∫ℓ(y,z) dκ(x)(y),\mathbb E[\ell(Y; z) \mid X = x] = \int \ell(y, z)\, d\kappa(x)(y),E[ℓ(Y;z)∣X=x]=∫ℓ(y,z)dκ(x)(y),

and for λ<0\lambda < 0λ<0 the threshold predictor of display (11) is

Tλ(x)={z∈Z:E[ℓ(Y;z)∣X=x]≥−λ}.\mathcal T_\lambda(x) = \{z \in \mathcal Z : \mathbb E[\ell(Y; z) \mid X = x] \ge -\lambda\}.Tλ​(x)={z∈Z:E[ℓ(Y;z)∣X=x]≥−λ}.

It includes exactly the points whose omission is expected to cost at least −λ-\lambda−λ. The size of a set is its μ\muμ-measure, ∣S∣=μ(S)|\mathcal S| = \mu(\mathcal S)∣S∣=μ(S), and the expected size of a predictor is E[∣T(X)∣]=∫μ(T(x)) dPX(x)\mathbb E[|\mathcal T(X)|] = \int \mu(\mathcal T(x))\, dP_X(x)E[∣T(X)∣]=∫μ(T(x))dPX​(x).

In Lean: setLoss μ ℓ y S, risk P μ ℓ T, condLoss κ ℓ x z, thresholdSet κ ℓ lam x and expSize P μ T in the namespace RiskControl.Optimal.

Formalization targets

Goal: Theorem 8

For every λ<0\lambda < 0λ<0 and every set-valued predictor T′\mathcal T'T′ (with measurable graph),

R(T′)≤R(Tλ)  ⟹  E[∣Tλ(X)∣]≤E[∣T′(X)∣].R(\mathcal T') \le R(\mathcal T_\lambda) \implies \mathbb E\big[|\mathcal T_\lambda(X)|\big] \le \mathbb E\big[|\mathcal T'(X)|\big].R(T′)≤R(Tλ​)⟹E[∣Tλ​(X)∣]≤E[∣T′(X)∣].

No constant is involved; the statement is uniform over ℓ\ellℓ, μ\muμ, PPP and T′\mathcal T'T′.

Milestones: the steps of the proof (p. 27)

  1. Moving the conditional expectation inside the μ\muμ-integral: for a predictor A\mathcal AA with measurable graph, E[∫A(X)ℓ(Y;z) dμ(z)]=E[∫A(X)E[ℓ(Y;z)∣X] dμ(z)]\mathbb E[\int_{\mathcal A(X)} \ell(Y; z)\, d\mu(z)] = \mathbb E[\int_{\mathcal A(X)} \mathbb E[\ell(Y; z) \mid X]\, d\mu(z)]E[∫A(X)​ℓ(Y;z)dμ(z)]=E[∫A(X)​E[ℓ(Y;z)∣X]dμ(z)].
  2. From the risk comparison to the set differences:
E[∫T′(X)∖Tλ(X)E[ℓ(Y;z)∣X] dμ]≥E[∫Tλ(X)∖T′(X)E[ℓ(Y;z)∣X] dμ].\mathbb E\Big[\int_{\mathcal T'(X) \setminus \mathcal T_\lambda(X)} \mathbb E[\ell(Y; z) \mid X]\, d\mu\Big] \ge \mathbb E\Big[\int_{\mathcal T_\lambda(X) \setminus \mathcal T'(X)} \mathbb E[\ell(Y; z) \mid X]\, d\mu\Big].E[∫T′(X)∖Tλ​(X)​E[ℓ(Y;z)∣X]dμ]≥E[∫Tλ​(X)∖T′(X)​E[ℓ(Y;z)∣X]dμ].
  1. From costs to sizes: E∣T′(X)∖Tλ(X)∣≥E∣Tλ(X)∖T′(X)∣\mathbb E|\mathcal T'(X) \setminus \mathcal T_\lambda(X)| \ge \mathbb E|\mathcal T_\lambda(X) \setminus \mathcal T'(X)|E∣T′(X)∖Tλ​(X)∣≥E∣Tλ​(X)∖T′(X)∣.
  2. From set differences to sets: E∣A(X)∖B(X)∣≤E∣B(X)∖A(X)∣\mathbb E|\mathcal A(X) \setminus \mathcal B(X)| \le \mathbb E|\mathcal B(X) \setminus \mathcal A(X)|E∣A(X)∖B(X)∣≤E∣B(X)∖A(X)∣ implies E∣A(X)∣≤E∣B(X)∣\mathbb E|\mathcal A(X)| \le \mathbb E|\mathcal B(X)|E∣A(X)∣≤E∣B(X)∣.

Significance

The result. Theorem 8 identifies the population-optimal shape of a set-valued predictor for every loss that charges for omitted points through a nonnegative cost and a finite measure. It justifies building nested families by thresholding an estimate of the conditional expected cost: if the estimate were exact, no other predictor with the same or smaller risk could have smaller sets on average. It contains the weighted-miscoverage case (Theorem 7) when Y\mathcal YY is discrete and μ\muμ is counting measure, and it covers losses for which no such special case exists, such as costs that depend on the distance between zzz and yyy.

Formalizing it. The proof on p. 27 is a chain of eight displays. A machine-checked version settles the measure-theoretic points the chain passes over: the conditional expectation inside an integral over a random set, the cancellation of possibly infinite terms, and the range of λ\lambdaλ. To our knowledge no formal proof of Theorem 8 or of the Neyman–Pearson-type optimality results it generalizes for set predictors exists in Lean or Mathlib.

Difficulty

The natural reading of the proof subtracts the quantity E∫ZE[ℓ(Y;z)∣X] dμ(z)\mathbb E\int_{\mathcal Z} \mathbb E[\ell(Y; z) \mid X]\, d\mu(z)E∫Z​E[ℓ(Y;z)∣X]dμ(z) from both sides of the risk comparison to pass from complements to sets. Nothing in the setting makes this quantity finite, so that step is not valid as written, and a proof that follows the displays literally breaks there. The theorem itself does not need finiteness of ℓ\ellℓ, and no such hypothesis is in scope.

The other obstacle is measure-theoretic bookkeeping. The conditional expectation E[ℓ(Y;z)∣X]\mathbb E[\ell(Y; z) \mid X]E[ℓ(Y;z)∣X] is indexed by a point zzz of a second space, and must be a jointly measurable function of (x,z)(x, z)(x,z) before it can be integrated over the random set T(X)\mathcal T(X)T(X); here it is given by a regular conditional distribution, and every integral over T(x)\mathcal T(x)T(x) needs the measurability of the graph of T\mathcal TT.

Formalization scope

  • Spaces and measures. X,Y,Z\mathcal X, \mathcal Y, \mathcal ZX,Y,Z are arbitrary measurable spaces; PPP is a probability measure on X×Y\mathcal X \times \mathcal YX×Y; μ\muμ is a finite measure on Z\mathcal ZZ; ℓ\ellℓ takes values in [0,∞)[0, \infty)[0,∞) and is jointly measurable.
  • Conditional law. E[ℓ(Y;z)∣X=x]\mathbb E[\ell(Y; z) \mid X = x]E[ℓ(Y;z)∣X=x] is ∫ℓ(y,z) dκ(x)(y)\int \ell(y, z)\, d\kappa(x)(y)∫ℓ(y,z)dκ(x)(y) for a Markov kernel κ\kappaκ with P=PX⊗κP = P_X \otimes \kappaP=PX​⊗κ, which is exactly the statement that κ\kappaκ is a regular conditional distribution of YYY given XXX. Such a kernel exists, for instance, when Y\mathcal YY is standard Borel; the formalization does not assume this. The threshold predictor is built from the same κ\kappaκ and the same ℓ\ellℓ as the risk; neither is a free object.
  • Integrals. Every integral is a lower Lebesgue integral with values in [0,∞][0, \infty][0,∞]; no integrability hypothesis is made, and an infinite risk is +∞+\infty+∞.
  • Range of λ\lambdaλ (correction of the print). The paper states Theorem 8 for λ∈Λ⊂(−∞,0]\lambda \in \Lambda \subset (-\infty, 0]λ∈Λ⊂(−∞,0]. At λ=0\lambda = 0λ=0 it is false: with ℓ≡0\ell \equiv 0ℓ≡0 and μ(Z)>0\mu(\mathcal Z) > 0μ(Z)>0, T0(x)=Z\mathcal T_0(x) = \mathcal ZT0​(x)=Z and T′≡∅\mathcal T' \equiv \emptysetT′≡∅ both have risk 000, but E∣T′(X)∣=0<μ(Z)\mathbb E|\mathcal T'(X)| = 0 < \mu(\mathcal Z)E∣T′(X)∣=0<μ(Z). The proof divides by −λ-\lambda−λ. Theorem 8 and its milestones are posed for λ<0\lambda < 0λ<0.
  • Set size (correction of the print). p. 13 describes ∣⋅∣|\cdot|∣⋅∣ as Lebesgue or counting measure, a sentence written for Theorem 7. In Theorem 8 the proof measures sets with the measure μ\muμ of the loss, and ∣⋅∣=μ|\cdot| = \mu∣⋅∣=μ throughout.
  • Measurable graphs. The competing predictor T′\mathcal T'T′ is required to have a measurable graph {(x,z):z∈T′(x)}\{(x, z) : z \in \mathcal T'(x)\}{(x,z):z∈T′(x)}; otherwise its risk and expected size are not integrals of measurable functions. The page leaves this implicit. The graph of Tλ\mathcal T_\lambdaTλ​ is measurable by construction.
  • Not a trivialization. The goal is stated about the threshold sets (11) built from the given ℓ\ellℓ, μ\muμ and κ\kappaκ, for every competing predictor; it does not assume any of the intermediate inequalities, and its hypotheses are satisfiable (for instance ℓ≡1\ell \equiv 1ℓ≡1, λ=−1/2\lambda = -1/2λ=−1/2, where Tλ(x)=Z\mathcal T_\lambda(x) = \mathcal ZTλ​(x)=Z).

The development needs Mathlib's composition of a measure with a kernel, Tonelli's theorem for kernels and lower integrals over sections of a measurable set. Lemmas about expected μ\muμ-sizes of random sets (milestone 4) and about moving a kernel integral inside a set integral (milestone 1) are reusable beyond this mission. Proofs of the milestones, and of the goal by other routes, are welcome.

Selected references

  • S. Bates, A. Angelopoulos, L. Lei, J. Malik, M. I. Jordan, Distribution-Free, Risk-Controlling Prediction Sets, Journal of the ACM 68(6), 2021. arXiv:2101.02703v3. https://arxiv.org/abs/2101.02703 — Theorem 8, p. 13; proof p. 27.
  • M. Sadinle, J. Lei, L. Wasserman, Least Ambiguous Set-Valued Classifiers With Bounded Error Levels, Journal of the American Statistical Association 114(525), 2019. https://doi.org/10.1080/01621459.2017.1395341
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Machine LearningProbabilityStatistics·Captain: mikedeng1

Distribution-Free, Risk-Controlling Prediction Sets I: Upper Confidence Bound Calibration Selects a λ̂ Whose Risk Is at Most α with Probability at Least 1 − δ (Theorem 1)Research Paper

Motivation

A trained classifier or regressor returns a point prediction, but many uses of machine learning need a prediction set: a set of plausible labels together with a guarantee about how often, or how badly, it misses the truth. Medical imaging, protein structure prediction and multi-label classification are examples where a user wants a set whose expected loss is bounded, not just a best guess. Bates, Angelopoulos, Lei, Malik and Jordan (arXiv:2101.02703, J. ACM 68(6), 2021) give a procedure that wraps any black-box predictor and returns sets whose risk is controlled, with no assumption on the data distribution beyond i.i.d. calibration data.

The procedure generalizes split conformal prediction (Vovk, Gammerman and Shafer, 2005) and the tolerance regions of Wilks (1941), which control only the probability of missing the label, to an arbitrary monotone loss on sets (false-negative rate, coverage of a segmentation mask, a hierarchical loss). This mission formalizes its central guarantee, Theorem 1 (p. 5), together with the abstract form Theorem A.1 (p. 26) from which the paper derives it.

Setting

Let (X,Y)(X, Y)(X,Y) be a random pair in X×Y\mathcal X \times \mathcal YX×Y with law PPP, and let Z\mathcal ZZ be a set of labels. A set-valued predictor is a map T:X→2Z\mathcal T : \mathcal X \to 2^{\mathcal Z}T:X→2Z. The paper considers a family {Tλ}λ∈Λ\{\mathcal T_\lambda\}_{\lambda \in \Lambda}{Tλ​}λ∈Λ​ indexed by a closed set Λ⊆R∪{±∞}\Lambda \subseteq \mathbb R \cup \{\pm\infty\}Λ⊆R∪{±∞} that is nested:

λ1<λ2  ⟹  Tλ1(x)⊆Tλ2(x).(1)\lambda_1 < \lambda_2 \implies \mathcal T_{\lambda_1}(x) \subseteq \mathcal T_{\lambda_2}(x). \tag{1}λ1​<λ2​⟹Tλ1​​(x)⊆Tλ2​​(x).(1)

A loss on sets L(y,S)≥0L(y, S) \ge 0L(y,S)≥0 is required to decrease as the set grows:

S⊆S′  ⟹  L(y,S)≥L(y,S′).(2)S \subseteq S' \implies L(y, S) \ge L(y, S'). \tag{2}S⊆S′⟹L(y,S)≥L(y,S′).(2)

The risk of Tλ\mathcal T_\lambdaTλ​ is R(λ)=E[L(Y,Tλ(X))]R(\lambda) = \mathbb E[L(Y, \mathcal T_\lambda(X))]R(λ)=E[L(Y,Tλ​(X))], and the section assumes some λmax⁡∈Λ\lambda_{\max} \in \Lambdaλmax​∈Λ with R(λmax⁡)=0R(\lambda_{\max}) = 0R(λmax​)=0.

A risk-controlling prediction set at levels (α,δ)(\alpha, \delta)(α,δ) (Definition 1, p. 2) is a data-dependent predictor T\mathcal TT with R(T)≤αR(\mathcal T) \le \alphaR(T)≤α with probability at least 1−δ1 - \delta1−δ.

Given an i.i.d. calibration sample D=((X1,Y1),…,(Xn,Yn))D = ((X_1, Y_1), \dots, (X_n, Y_n))D=((X1​,Y1​),…,(Xn​,Yn​)), a pointwise upper confidence bound is a function R^+(λ)=R^+(D,λ)\widehat R^+(\lambda) = \widehat R^+(D, \lambda)R+(λ)=R+(D,λ) with

P(R(λ)≤R^+(λ))≥1−δfor each fixed λ.(3)P\big(R(\lambda) \le \widehat R^+(\lambda)\big) \ge 1 - \delta \quad \text{for each fixed } \lambda. \tag{3}P(R(λ)≤R+(λ))≥1−δfor each fixed λ.(3)

UCB calibration selects

λ^=inf⁡{λ∈Λ:R^+(λ′)<α  ∀λ′∈Λ, λ′≥λ}.(4)\hat\lambda = \inf\big\{\lambda \in \Lambda : \widehat R^+(\lambda') < \alpha \ \ \forall \lambda' \in \Lambda,\ \lambda' \ge \lambda\big\}. \tag{4}λ^=inf{λ∈Λ:R+(λ′)<α  ∀λ′∈Λ, λ′≥λ}.(4)

In Lean, the risk is RiskControl.UCB.risk P L T lam, the calibration set of (4) for one realization r of R^+\widehat R^+R+ is calSet Λ r α, and λ^\hat\lambdaλ^ is lambdaHat Λ r α.

Formalization targets

Goal: Theorem 1 (p. 5)

In the setting above, if (3) holds for every λ∈Λ\lambda \in \Lambdaλ∈Λ and RRR is continuous on Λ\LambdaΛ, then

Pn(R(Tλ^)≤α)≥1−δ.P^n\big(R(\mathcal T_{\hat\lambda}) \le \alpha\big) \ge 1 - \delta .Pn(R(Tλ^​)≤α)≥1−δ.

Nothing is assumed of R^+\widehat R^+R+ beyond (3); α\alphaα and δ\deltaδ are arbitrary reals.

Milestones

  1. Monotone risk (§2.1, pp. 4–5): (1) and (2) make RRR nonincreasing on Λ\LambdaΛ.
  2. The failure point (proof of Theorem A.1, p. 26, corrected): λ†=sup⁡{λ∈Λ:R(λ)>α}\lambda^\dagger = \sup\{\lambda \in \Lambda : R(\lambda) > \alpha\}λ†=sup{λ∈Λ:R(λ)>α} lies in Λ\LambdaΛ and R(λ†)≥αR(\lambda^\dagger) \ge \alphaR(λ†)≥α.
  3. Failure implies a low bound at λ†\lambda^\daggerλ† (p. 26, corrected): deterministically, R(λ^)>αR(\hat\lambda) > \alphaR(λ^)>α implies R^+(λ†)<α\widehat R^+(\lambda^\dagger) < \alphaR+(λ†)<α.
  4. Theorem A.1 (p. 26): for any continuous nonincreasing R:Λ→RR : \Lambda \to \mathbb RR:Λ→R and any R^+\widehat R^+R+ satisfying (3) on an abstract probability space, P(R(λ^)≤α)≥1−δP(R(\hat\lambda) \le \alpha) \ge 1 - \deltaP(R(λ^)≤α)≥1−δ.

Significance

Theorem 1 turns a confidence bound for one fixed parameter into a guarantee for a parameter chosen from the data. No uniform convergence over Λ\LambdaΛ is needed, so any concentration inequality for a mean (Hoeffding, Bentkus, the betting bound of Waudby-Smith and Ramdas) yields a calibration procedure immediately; the paper's Theorems 2–5 and 9–10 are of exactly this form, and the later Learn-then-Test and conformal risk control frameworks build on the same template.

The result is proved in the paper; nothing here is open. What the mission adds is a machine-checked version of an argument whose printed form has a gap. The printed proof of Theorem A.1 introduces λ∗=inf⁡{λ∈Λ:R(λ)≤α}\lambda^* = \inf\{\lambda \in \Lambda : R(\lambda) \le \alpha\}λ∗=inf{λ∈Λ:R(λ)≤α} and asserts R(λ∗)=αR(\lambda^*) = \alphaR(λ∗)=α "by continuity", which is false when Λ\LambdaΛ is not an interval. Finite grids, the usual choice of Λ\LambdaΛ in practice, are not intervals. The theorem remains true, and milestones 2 and 3 state the corrected steps. No formalization of risk-controlling prediction sets or of conformal prediction is known to exist in Lean or on this platform.

Difficulty

The obvious argument applies the confidence bound at λ^\hat\lambdaλ^; that fails because λ^\hat\lambdaλ^ depends on the data, so (3) says nothing at λ=λ^\lambda = \hat\lambdaλ=λ^. The proof must find one deterministic point at which a failure of calibration forces a failure of (3). The paper's choice λ∗\lambda^*λ∗ works only when RRR attains the value α\alphaα on Λ\LambdaΛ; on Λ={0,1}\Lambda = \{0, 1\}Λ={0,1} with R(0)=1R(0) = 1R(0)=1, R(1)=0R(1) = 0R(1)=0, α=1/2\alpha = 1/2α=1/2 and the exact bound R^+=R\widehat R^+ = RR+=R, the event {R^+(λ∗)<α}\{\widehat R^+(\lambda^*) < \alpha\}{R+(λ∗)<α} has probability one, so the printed last step does not bound anything. The second difficulty is boundary behaviour: Λ\LambdaΛ may contain ±∞\pm\infty±∞, the infimum in (4) may be over an empty set, and the calibration set need not contain its own infimum.

Formalization scope

  • Λ\LambdaΛ is a closed subset of EReal (the extended reals with the order topology); λ\lambdaλ is only compared, never added. Continuity of RRR is in the subspace topology of Λ\LambdaΛ.
  • Set-valued predictions are Set 𝒵, i.e. Y′=2Z\mathcal Y' = 2^{\mathcal Z}Y′=2Z (the paper uses 2Y2^{\mathcal Y}2Y for most of its examples).
  • The risk is the published definition WassersteinDRO.Duality.nominalRisk, a Bochner integral. Because a non-integrable integrand integrates to 000 in Lean, Theorem 1 assumes (x,y)↦L(y,Tλ(x))(x, y) \mapsto L(y, \mathcal T_\lambda(x))(x,y)↦L(y,Tλ​(x)) is PPP-integrable for every λ∈Λ\lambda \in \Lambdaλ∈Λ.
  • The standing assumptions of §2.1 are hypotheses of Theorem 1: Λ\LambdaΛ closed, (1) on Λ\LambdaΛ, (2), L≥0L \ge 0L≥0, and R(λmax⁡)=0R(\lambda_{\max}) = 0R(λmax​)=0 for some λmax⁡∈Λ\lambda_{\max} \in \Lambdaλmax​∈Λ. The monotonicity of RRR is not assumed in Theorem 1; it is milestone 1. Theorem A.1 assumes it, as printed.
  • The i.i.d. sample is Fin n → 𝒳 × 𝒴 under the product measure PnP^nPn. R^+\widehat R^+R+ is an arbitrary real function of the sample and of λ\lambdaλ; an infinite bound is represented by any value ≥α\ge \alpha≥α.
  • "With probability at least 1−δ1 - \delta1−δ" is written as a failure probability at most δ\deltaδ, measured as an outer measure; no measurability of R^+\widehat R^+R+ or λ^\hat\lambdaλ^ is assumed. For a measurable event this is the page's statement.
  • λ^\hat\lambdaλ^ is an infimum in EReal, so inf⁡∅=+∞\inf \emptyset = +\inftyinf∅=+∞ as on the page. Since +∞+\infty+∞ need not belong to Λ\LambdaΛ, the failure event is "the set in (4) is nonempty and R(λ^)>αR(\hat\lambda) > \alphaR(λ^)>α"; when the set is nonempty, λ^∈Λ\hat\lambda \in \Lambdaλ^∈Λ. When it is empty the procedure certifies nothing, and the natural output is Tλmax⁡\mathcal T_{\lambda_{\max}}Tλmax​​, of risk 000.
  • Corrections of the print: Theorem A.1's conclusion reads P(R(λ)≤α)P(R(\lambda) \le \alpha)P(R(λ)≤α), stated here with λ^\hat\lambdaλ^; the proof's point λ∗\lambda^*λ∗ and the claim R(λ∗)=αR(\lambda^*) = \alphaR(λ∗)=α are replaced by λ†=sup⁡{λ∈Λ:R(λ)>α}\lambda^\dagger = \sup\{\lambda \in \Lambda : R(\lambda) > \alpha\}λ†=sup{λ∈Λ:R(λ)>α} and R(λ†)≥αR(\lambda^\dagger) \ge \alphaR(λ†)≥α, which coincide with the page for an interval Λ\LambdaΛ.
  • A formalization that assumes RRR monotone in Theorem 1, quantifies over R^+\widehat R^+R+ inside the event, takes a real-valued infimum (which is 000 on unbounded sets) or drops the integrability guard would state a different theorem; the statement here does none of these.

Needed infrastructure is small: closed subsets of EReal and their infima and suprema (IsClosed.sInf_mem, IsClosed.sSup_mem), continuity within a set, monotonicity of the Bochner integral, and monotonicity of outer measure. Proofs of the milestones are welcome individually; the deterministic milestones 2 and 3 are reusable for every UCB-calibration theorem of the paper.

Selected references

  • S. Bates, A. Angelopoulos, L. Lei, J. Malik, M. I. Jordan, Distribution-Free, Risk-Controlling Prediction Sets, J. ACM 68(6), 2021; arXiv:2101.02703v3. https://arxiv.org/abs/2101.02703
  • V. Vovk, A. Gammerman, G. Shafer, Algorithmic Learning in a Random World, Springer, 2005. https://doi.org/10.1007/b106715
  • S. S. Wilks, Determination of sample sizes for setting tolerance limits, Ann. Math. Statist. 12(1), 1941. https://doi.org/10.1214/aoms/1177731788
  • I. Waudby-Smith, A. Ramdas, Estimating means of bounded random variables by betting, arXiv:2010.09686, 2020. https://arxiv.org/abs/2010.09686
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CombinatoricsGraph Theory·Captain: mikedeng1

Turán Graphs with Bounded Matching Number 2: For Color-Critical H of Chromatic Number k+1 > 2, Large s and n ≫ s, H-Free Graphs with Matching Number at Most s Have at Most g(n,k,s) EdgesResearch Paper

Motivation

Two classical extremal results bound the number of edges of an nnn-vertex graph under a single restriction. Turán's theorem (1941) says that a graph with no clique on k+1k+1k+1 vertices has at most t(n,k)t(n,k)t(n,k) edges, the edge count of the balanced complete kkk-partite graph. The Erdős–Gallai theorem (1959) gives the maximum number of edges of an nnn-vertex graph whose largest matching has at most sss edges. N. Alon and P. Frankl, Turán graphs with bounded matching number (arXiv:2210.15076v1; J. Combin. Theory Ser. B, 2024, DOI 10.1016/j.jctb.2023.12.002), combine the two restrictions. Their Theorem 1.1 determines the maximum for the clique constraint and every n≥2s+1n\ge 2s+1n≥2s+1 (mission 1 of this series). Their Proposition 3.1, the goal here, treats a whole class of forbidden graphs, the color-critical ones, when sss is large in terms of the forbidden graph and nnn is large in terms of sss.

Color-critical graphs are the natural class for exact Turán results: by a theorem of M. Simonovits (1968), for a color-critical HHH of chromatic number k+1k+1k+1 the Turán graph T(N,k)T(N,k)T(N,k) is extremal for HHH-freeness once NNN is large. Proposition 3.1 is the analogue of Simonovits' theorem under a matching constraint.

Setting

All graphs are finite and simple. For a graph GGG, a matching is a set of pairwise disjoint edges, and the matching number ν(G)\nu(G)ν(G) is the largest size of a matching. For a graph HHH, GGG is HHH-free if it contains no subgraph (not necessarily induced) isomorphic to HHH. The chromatic number χ(H)\chi(H)χ(H) is the least number of colors in a proper vertex coloring. HHH is color-critical if it has an edge eee with χ(H−e)<χ(H)\chi(H-e)<\chi(H)χ(H−e)<χ(H); examples are complete graphs and odd cycles.

The Turán graph T(n,k)T(n,k)T(n,k) is the complete kkk-partite graph on nnn vertices with classes of sizes as equal as possible; t(n,k)t(n,k)t(n,k) is its number of edges. For k≥2k\ge 2k≥2 and 2s≤n2s\le n2s≤n, the graph G(n,k,s)G(n,k,s)G(n,k,s) is the complete kkk-partite graph on nnn vertices consisting of k−1k-1k−1 classes of sizes as equal as possible whose total size is sss, and one further class of size n−sn-sn−s. Its number of edges is g(n,k,s)g(n,k,s)g(n,k,s).

In the Lean development, vertices of GGG are Fin n; the shared objects of this series live in TuranMatching.Clique.Setting: ν\nuν is matchingNumber, t(n,k)t(n,k)t(n,k) is turanNum n k (Mathlib's turanGraph), G(n,k,s)G(n,k,s)G(n,k,s) is bigGraph n k s, g(n,k,s)g(n,k,s)g(n,k,s) is gNum n k s, color-criticality is IsColorCritical, and the set XXX of vertices of degree exceeding 2s2s2s is highDeg G s.

Formalization targets

Goal: Proposition 3.1 (p. 5)

There is n0:N→Nn_0:\mathbb N\to\mathbb Nn0​:N→N such that for every color-critical HHH with χ(H)=k+1>2\chi(H)=k+1>2χ(H)=k+1>2 there is s0(H)s_0(H)s0​(H) with: for all s>s0(H)s>s_0(H)s>s0​(H) and n>n0(s)n>n_0(s)n>n0​(s),

max⁡{∣E(G)∣:∣V(G)∣=n, G H-free, ν(G)≤s}=g(n,k,s).\max\{|E(G)| : |V(G)|=n,\ G\ H\text{-free},\ \nu(G)\le s\}=g(n,k,s).max{∣E(G)∣:∣V(G)∣=n, G H-free, ν(G)≤s}=g(n,k,s).

The maximum is stated as an upper bound for every admissible GGG together with an admissible graph attaining g(n,k,s)g(n,k,s)g(n,k,s). The thresholds s0s_0s0​ and n0n_0n0​ are left existential, as on the page.

Milestones (pp. 5–6)

  1. G(n,k,s)G(n,k,s)G(n,k,s) is kkk-colorable, HHH-free for every HHH with χ(H)=k+1\chi(H)=k+1χ(H)=k+1, and ν(G(n,k,s))=s\nu(G(n,k,s))=sν(G(n,k,s))=s (for 2s≤n2s\le n2s≤n).
  2. If ν(G)≤s\nu(G)\le sν(G)≤s then at most sss vertices have degree exceeding 2s2s2s: ∣X∣≤s|X|\le s∣X∣≤s.
  3. If every degree is at most 2s2s2s and ν(G)≤s\nu(G)\le sν(G)≤s, then ∣E(G)∣≤(2s+1)s|E(G)|\le(2s+1)s∣E(G)∣≤(2s+1)s.
  4. If ν(G)≤s\nu(G)\le sν(G)≤s and ∣X∣<s|X|<s∣X∣<s, then ∣E(G)∣<(s−1)n+2(s+1)s|E(G)|<(s-1)n+2(s+1)s∣E(G)∣<(s−1)n+2(s+1)s.
  5. (s−1)n+2(s+1)s<g(n,k,s)(s-1)n+2(s+1)s<g(n,k,s)(s−1)n+2(s+1)s<g(n,k,s) for n>3s2+2sn>3s^2+2sn>3s2+2s.
  6. If ν(G)≤s\nu(G)\le sν(G)≤s and ∣X∣=s|X|=s∣X∣=s, then V−XV-XV−X is independent.
  7. Simonovits' theorem: an HHH-free graph on N≥N0(H)N\ge N_0(H)N≥N0​(H) vertices has at most t(N,k)t(N,k)t(N,k) edges.
  8. If ∣X∣=s|X|=s∣X∣=s, V−XV-XV−X is independent, ZZZ is disjoint from XXX with ∣Z∣=⌊s/(k−1)⌋|Z|=\lfloor s/(k-1)\rfloor∣Z∣=⌊s/(k−1)⌋ and G[X∪Z]G[X\cup Z]G[X∪Z] has at most t(s+⌊s/(k−1)⌋,k)t(s+\lfloor s/(k-1)\rfloor,k)t(s+⌊s/(k−1)⌋,k) edges, then ∣E(G)∣≤g(n,k,s)|E(G)|\le g(n,k,s)∣E(G)∣≤g(n,k,s).

Significance

The proposition settles, for every color-critical HHH and large parameters, the Turán problem with a bounded matching number, and identifies the extremal graph G(n,k,s)G(n,k,s)G(n,k,s), which does not depend on HHH beyond its chromatic number. For H=Kk+1H=K_{k+1}H=Kk+1​ it agrees with the large-nnn case of Theorem 1.1 of the same paper. The structural steps (few high-degree vertices, the independence of the low-degree side) are reusable in other degree-based arguments under matching constraints.

The result is proved in the paper; none of it is formalized. The mission produces, besides the goal, two classical theorems absent from Mathlib in the forms needed here: the matching-number consequence of Vizing's theorem (milestone 3) and Simonovits' exact Turán theorem for color-critical graphs (milestone 7). Milestone 7 is a cited classical theorem, not a result of Alon and Frankl; it is posed because the proof rests on it. Mathlib currently has Turán's theorem for cliques and the Erdős–Stone–Simonovits density theorem, but not the exact result for color-critical graphs.

Difficulty

Milestones 1, 2, 4, 5, 6 and 8 are elementary counting arguments, though each requires building matchings or explicit counts in Lean. Milestone 8 contains the paper's "easy to see" isomorphism, which in Lean is an identity between two edge counts, t(s+m,k)+(n−s−m)s=g(n,k,s)t(s+m,k)+(n-s-m)s=g(n,k,s)t(s+m,k)+(n−s−m)s=g(n,k,s) with m=⌊s/(k−1)⌋m=\lfloor s/(k-1)\rfloorm=⌊s/(k−1)⌋.

Milestone 3 needs Vizing's edge-coloring theorem (a graph of maximum degree Δ\DeltaΔ is properly (Δ+1)(\Delta+1)(Δ+1)-edge-colorable). A naive greedy edge coloring gives only 2Δ−12\Delta-12Δ−1 colors, which bounds the edge count by about (4s−1)s(4s-1)s(4s−1)s and is too weak for the comparison in milestones 4 and 5.

Milestone 7 is the hardest item. The density version (Erdős–Stone–Simonovits) gives t(N,k)+o(N2)t(N,k)+o(N^2)t(N,k)+o(N2) edges only; the exact bound for color-critical HHH requires Simonovits' stability method, an argument that an almost-extremal HHH-free graph is close to T(N,k)T(N,k)T(N,k) followed by a cleaning step that uses the critical edge.

Formalization scope

Graphs are SimpleGraph (Fin n) with decidable adjacency; edges are counted by #G.edgeFinset. The matching number is the supremum, in N\mathbb NN, of the edge counts of matching subgraphs; the set is nonempty and bounded, so this is the true maximum and not a junk value. g(n,k,s)g(n,k,s)g(n,k,s) is defined as the edge count of the graph G(n,k,s)G(n,k,s)G(n,k,s), not by a closed formula. Chromatic numbers live in N∪{∞}\mathbb N\cup\{\infty\}N∪{∞} (Mathlib's chromaticNumber), both in the definition of color-critical and in the hypothesis χ(H)=k+1\chi(H)=k+1χ(H)=k+1. HHH-freeness is Mathlib's SimpleGraph.Free (no subgraph copy). The vertex type of HHH is any finite type in the lowest universe.

Conventions committed to:

  • k≥2k\ge 2k≥2 is the page's k+1>2k+1>2k+1>2; it is needed because G(n,k,s)G(n,k,s)G(n,k,s) has k−1k-1k−1 classes and the proof divides by k−1k-1k−1.
  • Quantifier order is the page's: n0n_0n0​ is a function of sss alone and is chosen before HHH; s0s_0s0​ depends on HHH only.
  • Milestone 1 states kkk-colorability for the page's "kkk chromatic", and carries 2s≤n2s\le n2s≤n, which the page leaves implicit.
  • Milestone 3 bounds edges where the page writes "the number of vertices"; the vertex count is not bounded.
  • Milestone 5 uses the threshold n>3s2+2sn>3s^2+2sn>3s2+2s. The page's "nnn exceeding, say, 3s23s^23s2" is too small: for k=2k=2k=2, s=2s=2s=2, n=13n=13n=13 one has (s−1)n+2(s+1)s=25>22=g(13,2,2)(s-1)n+2(s+1)s=25>22=g(13,2,2)(s−1)n+2(s+1)s=25>22=g(13,2,2). The goal is unaffected, since n0(s)n_0(s)n0​(s) is unspecified.
  • Milestone 4 carries s≥1s\ge 1s≥1 so that s−1s-1s−1 is honest natural-number subtraction.

A formalization that states only the upper bound, without an attaining graph, or that places the existential n0n_0n0​ after sss is fixed as a constant independent of sss, or that defines ν\nuν or ggg so that they take junk values, is a different and weaker statement and is ruled out.

Infrastructure that would be reusable beyond this mission: a matching-number API on Mathlib's Subgraph.IsMatching (in particular ν(G)≤ν(G′)\nu(G)\le\nu(G')ν(G)≤ν(G′) for G≤G′G\le G'G≤G′ and the behaviour under induced subgraphs); Vizing's theorem; and Simonovits' theorem. Contributions of any of these, and of partial results toward milestone 7 (for example the case H=C2ℓ+1H=C_{2\ell+1}H=C2ℓ+1​), are welcome.

Selected references

  • N. Alon and P. Frankl, Turán graphs with bounded matching number, arXiv:2210.15076v1, 2022; J. Combin. Theory Ser. B, 2024. https://arxiv.org/abs/2210.15076, https://doi.org/10.1016/j.jctb.2023.12.002
  • M. Simonovits, A method for solving extremal problems in graph theory, stability problems, in: Theory of Graphs (Proc. Colloq., Tihany, 1966), Academic Press, 1968, pp. 279–319.
  • P. Erdős and T. Gallai, On maximal paths and circuits of graphs, Acta Math. Acad. Sci. Hungar. 10 (1959), 337–356. https://doi.org/10.1007/BF02024498
  • P. Turán, On an extremal problem in graph theory (in Hungarian), Mat. Fiz. Lapok 48 (1941), 436–452.
  • V. G. Vizing, On an estimate of the chromatic class of a p-graph, Diskret. Analiz 3 (1964), 25–30.
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Algorithmic Game TheoryEconomics·Captain: mikedeng1

Competitive Equilibrium with Indivisible Goods and Generic Budgets 1: Two Additive Agents with Almost Equal but Unequal Budgets Have a Competitive Equilibrium Giving Each Agent Her Truncated ShareResearch Paper

Motivation

Many allocation problems divide indivisible goods among agents who are entitled to different shares but cannot pay with real money: course seats among students, shifts among workers, inherited items among heirs. A standard mechanism gives each agent a budget of artificial currency and lets a market run. When budgets are equal this is the competitive equilibrium from equal incomes (CEEI) of Varian (1974), the basis of the course-allocation mechanism of Budish (2011). With indivisible items, however, an equilibrium can fail to exist: one item and two agents with equal budgets already admit none, because whoever does not get the item could afford it at any price the owner can pay.

Babaioff, Nisan and Talgam-Cohen (arXiv 2017; Math. Oper. Res. 2021, doi:10.1287/moor.2020.1062) ask whether this failure is robust or a knife edge, and answer for two agents with additive preferences: an arbitrarily small, strict inequality between the budgets restores existence. Budish's approximate CEEI perturbs budgets randomly for the same reason; this mission formalizes the exact two-agent result.

Setting

A discrete Fisher market has a set MMM of mmm indivisible items and two agents. Agent iii has a valuation viv_ivi​ assigning a real value to every bundle S⊆MS\subseteq MS⊆M, and a budget bi>0b_i>0bi​>0. Valuations are additive (vi(S)=∑j∈Svi({j})v_i(S)=\sum_{j\in S}v_i(\{j\})vi​(S)=∑j∈S​vi​({j})), normalized (vi(M)=1v_i(M)=1vi​(M)=1), non-negative, monotone (vi(S)<vi(T)v_i(S)<v_i(T)vi​(S)<vi​(T) when S⊊TS\subsetneq TS⊊T) and strict (different bundles have different values). Budgets are normalized, b1+b2=1b_1+b_2=1b1​+b2​=1; money has no value to the agents.

An allocation S=(S1,S2)\mathcal S=(\mathcal S_1,\mathcal S_2)S=(S1​,S2​) is a partition of all items between the agents. Item prices pj≥0p_j\ge 0pj​≥0 give bundle prices p(S)=∑j∈Spjp(S)=\sum_{j\in S}p_jp(S)=∑j∈S​pj​. Agent iii demands SSS if p(S)≤bip(S)\le b_ip(S)≤bi​ and p(T)>bip(T)>b_ip(T)>bi​ for every bundle TTT with vi(T)>vi(S)v_i(T)>v_i(S)vi​(T)>vi​(S). A competitive equilibrium (CE) is a pair (S,p)(\mathcal S,p)(S,p) in which each agent demands her own bundle. An allocation is Pareto optimal (PO) if every other allocation is strictly worse for some agent.

Agent iii's budget-proportional share is bib_ibi​ (her budget times vi(M)=1v_i(M)=1vi​(M)=1). Her truncated share is the best value she gets in a PO allocation that gives her at most that share:

bi−=max⁡{vi(Si): S PO, vi(Si)≤bi}.b_i^-=\max\{v_i(\mathcal S_i):\ \mathcal S\ \text{PO},\ v_i(\mathcal S_i)\le b_i\}.bi−​=max{vi​(Si​): S PO, vi​(Si​)≤bi​}.

The Lean development uses the same names: bundle σ i for Si\mathcal S_iSi​, price, IsCE, IsPO, IsStandardValuation, GetsTruncatedShare.

Formalization targets

Goal: Theorem 7.1 (p. 17)

For every two-agent additive market there is ϵ>0\epsilon>0ϵ>0 such that every budget pair with

b2<b1≤b2+ϵb_2<b_1\le b_2+\epsilonb2​<b1​≤b2​+ϵ

admits a CE (S,p)(\mathcal S,p)(S,p) in which vj(Sj)≥bj−v_j(\mathcal S_j)\ge b_j^-vj​(Sj​)≥bj−​ for both agents. The goal fixes no value of ϵ\epsilonϵ; it asserts only that one exists for each market.

Milestones

  1. Proposition 4.1 (p. 10): for a PO allocation with non-empty bundles and budget-exhausting prices, CE is equivalent to a pairwise swap condition, Condition (1).
  2. Lemma 4.3 (p. 11): a budget-exhausting combination pricing pj=αv1({j})+βv2({j})p_j=\alpha v_1(\{j\})+\beta v_2(\{j\})pj​=αv1​({j})+βv2​({j}) (α,β≥0\alpha,\beta\ge0α,β≥0, max⁡{α,β}>0\max\{\alpha,\beta\}>0max{α,β}>0) at a PO allocation is a CE.
  3. Proposition 5.1 (p. 12): budget-proportional and anti-proportional PO allocations are supported in a CE.
  4. Lemma 5.5 (p. 14): without budget-proportional or PO anti-proportional allocations, agent iii's augmented-share minimizer is agent kkk's truncated-share maximizer.
  5. Lemma 6.3 (p. 15): if the budgets avoid the finite exceptional set RiR_iRi​ and the rectangle of allocations TiT_iTi​ is empty, a CE with truncated shares exists.
  6. Case 1 of the proof (p. 18): a CE at budgets (12,12)(\tfrac12,\tfrac12)(21​,21​) remains a CE, after rescaling prices, when agent 1's budget is raised slightly.
  7. RiR_iRi​ avoidance (p. 19): almost equal but unequal budgets lie outside RiR_iRi​.

Two companion statements are drafted without being milestones: Theorem 4.4 (second welfare theorem) and Theorem 5.2 (a budget-proportional allocation implies a CE).

Significance

The result. Theorem 7.1 shows that the non-existence of CEEI with indivisible goods is a measure-zero phenomenon for two additive agents: equal budgets are the only bad point near equality, and the equilibrium obtained is also fair in the truncated-share sense. It justifies tie-breaking by tiny budget differences in practice. It is the two-agent base case of the paper's main open question (§9.1, p. 20), whether generic almost-equal budgets guarantee a CE for more than two agents; the paper also leaves open two agents with arbitrary generic budgets and non-identical preferences (p. 21). For arbitrary, not almost-equal, budgets, Segal-Halevi (AAMAS 2018) shows that genericity does not guarantee existence for four additive agents.

Formalizing it. No machine-checked proof of any result of this paper is known. The paper's own argument for one case of the goal is incomplete: in Case 2(b) of the proof of Theorem 7.1 (p. 19) it asserts that the two candidate allocations are mirror images of each other and that the rectangles T1,T2T_1,T_2T1​,T2​ are empty. Both claims fail on an explicit three-item market. Theorem 7.1 itself held in every one of 6000 markets checked numerically during planning, including that one, where a CE with truncated shares exists at prices proportional to one agent's valuation. A formal proof therefore has to supply an argument the paper does not contain; the two false steps are not posed as milestones.

Difficulty

The milestones 1–5 are finite combinatorics on the Pareto frontier with sign bookkeeping. The difficulty sits in Case 2(b) of the goal: every allocation gives one agent more than 12\tfrac1221​ and the other less. The natural route, invoking Lemma 6.3, needs some TiT_iTi​ to be empty, and in that case both can be non-empty. Lemma 6.3 does not cover it, and the paper's symmetry argument cannot be repaired by choosing ϵ\epsilonϵ smaller, since in the counterexample the two candidate allocations stay the same for every small ϵ\epsilonϵ. A complete proof must show directly that one of the two "as fair as possible" allocations is supported by suitable prices.

Formalization scope

Items are Fin m and agents Fin 2; the paper's agents 1, 2 are indices 0, 1, so "b1>b2b_1>b_2b1​>b2​" reads b 1 < b 0. An allocation is a map σ : Fin m → Fin 2, which builds in that every item is allocated exactly once. All quantities are real numbers. Demand quantifies over every bundle, with strict inequality p(T)>bip(T)>b_ip(T)>bi​. Prices are non-negative by definition of a CE. The truncated share is a maximum over PO allocations only.

Two conventions are disclosed restrictions or additions:

  1. Strictness without identical items. The paper allows identical items as the single exception to strict preferences (p. 6). Here each valuation is injective on bundles, so markets with identical items are excluded.
  2. Rescaled prices in Case 1. The page says the perturbed CE uses unchanged prices; at normalized budgets the prices must be divided by 1+ϵ1+\epsilon1+ϵ, and the milestone says so.

In the goal ϵ\epsilonϵ is chosen after the valuations and before the budgets. A formalization in which ϵ\epsilonϵ depends on the budgets, demand ranges over a restricted family of bundles, allocations need not allocate every item, prices may be negative, or the truncated share is a maximum over all allocations, would be a different and in several cases trivial statement; all of these are ruled out.

The definitions file GenericBudgets.AlmostEqual.Setting holds the market, CE, PO, the fairness notions, combination pricing, Condition (1), TiT_iTi​ and RiR_iRi​, and is reusable for any two-agent indivisible-goods market with budgets. Proofs of the milestones, a repaired argument for Case 2(b), and general nnn-agent versions of the CE and PO infrastructure are welcome.

Selected references

  • M. Babaioff, N. Nisan, I. Talgam-Cohen, Competitive Equilibrium with Indivisible Goods and Generic Budgets, arXiv:1703.08150v2, 2018; Mathematics of Operations Research 46(1), 2021. https://arxiv.org/abs/1703.08150v2, https://doi.org/10.1287/moor.2020.1062
  • H. R. Varian, Equity, envy, and efficiency, Journal of Economic Theory 9(1), 1974. https://doi.org/10.1016/0022-0531(74)90075-1
  • E. Budish, The combinatorial assignment problem: approximate competitive equilibrium from equal incomes, Journal of Political Economy 119(6), 2011. https://doi.org/10.1086/664613
  • E. Segal-Halevi, Competitive equilibrium for almost all incomes, Proceedings of AAMAS 2018, pp. 1267–1275. https://arxiv.org/abs/1705.04212
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Linear OptimizationMachine LearningOperations Research+1·Captain: mikedeng1

Strong Mixed-Integer Programming Formulations for Trained Neural Networks 2: Under Strict Activity Every Inequality of the Exponential Family (6b) Is Facet-DefiningResearch Paper

Motivation

Trained neural networks are increasingly embedded inside optimization models: to verify that a classifier is robust to small input perturbations, to optimize over a learned surrogate of an expensive system, or to choose decisions whose outcome is predicted by a network. When the network uses rectified linear units (ReLU), each neuron y=max⁡{0, w⋅x+b}y=\max\{0,\,w\cdot x+b\}y=max{0,w⋅x+b} is piecewise linear, and the whole network can be written exactly as a mixed-integer program (MIP) with one binary variable per neuron. How fast a branch-and-bound solver closes such a model depends on how tight the linear-programming relaxation of each neuron's formulation is.

Anderson, Huchette, Tjandraatmadja and Vielma (arXiv:1811.08359v2, the IPCO 2019 extended abstract) gave a formulation (6) of a single ReLU neuron over a box that uses only the original variables and one binary variable, and is ideal: its LP relaxation has integral extreme points (Proposition 1, p. 6). The price is an exponential family of inequalities (6b), one for every subset III of the support of www. The present mission formalizes their Proposition 2: each of these inequalities is facet-defining, so no member of the family can be dropped without weakening the relaxation. A longer journal version of the work, with different numbering, appeared later (arXiv:1811.01988); this mission follows the extended abstract.

Setting

Fix η∈N\eta\in\mathbb Nη∈N, a weight vector w∈Rηw\in\mathbb R^\etaw∈Rη, a bias b∈Rb\in\mathbb Rb∈R, and bounds L,U∈RηL,U\in\mathbb R^\etaL,U∈Rη with Li<UiL_i<U_iLi​<Ui​ for every iii (§1.3, p. 4). Write f(x)=w⋅x+bf(x)=w\cdot x+bf(x)=w⋅x+b and [L,U]={x:L≤x≤U}[L,U]=\{x : L\le x\le U\}[L,U]={x:L≤x≤U}. The sign-adjusted bounds are

L˘i={Liwi≥0Uiwi<0,U˘i={Uiwi≥0Liwi<0,\breve L_i=\begin{cases}L_i & w_i\ge 0\\ U_i & w_i<0\end{cases},\qquad \breve U_i=\begin{cases}U_i & w_i\ge 0\\ L_i & w_i<0\end{cases},L˘i​={Li​Ui​​wi​≥0wi​<0​,U˘i​={Ui​Li​​wi​≥0wi​<0​,

so that M+(f)=w⋅U˘+bM^+(f)=w\cdot\breve U+bM+(f)=w⋅U˘+b and M−(f)=w⋅L˘+bM^-(f)=w\cdot\breve L+bM−(f)=w⋅L˘+b are the maximum and minimum of fff over [L,U][L,U][L,U]. The support is supp⁡(w)={i:wi≠0}\operatorname{supp}(w)=\{i : w_i\neq 0\}supp(w)={i:wi​=0}. Strict activity means M−(f)<0<M+(f)M^-(f)<0<M^+(f)M−(f)<0<M+(f): the neuron is neither always off nor always on over the box. The paper assumes it throughout (§1.3).

Formulation (6) (p. 6) consists of the points (x,y,z)(x,y,z)(x,y,z) with

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

In Lean, form6 w b L U is this set, and relax6 w b L U is its LP relaxation (0≤z≤10\le z\le10≤z≤1 in place of z∈{0,1}z\in\{0,1\}z∈{0,1}). The right-hand side of (6b) for the subset III is rhs6b w b L U I x z.

An inequality g≤0g\le0g≤0 is facet-defining for a set PPP when it holds on PPP, its face F=P∩{g=0}F=P\cap\{g=0\}F=P∩{g=0} is nonempty, and dim⁡F=dim⁡P−1\dim F=\dim P-1dimF=dimP−1, the dimension of a set being that of its affine hull. The paper uses this standard notion without defining it.

Formalization targets

Goal: Proposition 2 (p. 6)

Under L<UL<UL<U and strict activity, for every I⊆supp⁡(w)I\subseteq\operatorname{supp}(w)I⊆supp(w), the inequality (6b) for III is facet-defining for

P=conv⁡{(x,y,z):(x,y,z) satisfies (6a)–(6c)}.P=\operatorname{conv}\{(x,y,z) : (x,y,z)\text{ satisfies (6a)–(6c)}\}.P=conv{(x,y,z):(x,y,z) satisfies (6a)–(6c)}.

The page states the result as "Each inequality in (6b) is facet-defining", and adds right after the proof line: "We require the assumption of strict activity above, as introduced in Section 1.3."

Milestones (App. A.2, p. 15)

  1. For some ε>0\varepsilon>0ε>0, the η+2\eta+2η+2 points p0=(L˘,0,0)p^0=(\breve L,0,0)p0=(L˘,0,0), p1=(U˘,f(U˘),1)p^1=(\breve U,f(\breve U),1)p1=(U˘,f(U˘),1), p~i=(L˘+εσiei,0,0)\tilde p^i=(\breve L+\varepsilon\sigma_ie^i,0,0)p~​i=(L˘+εσi​ei,0,0) for i∉Ii\notin Ii∈/I, and p~i=(U˘−εσiei,f(U˘−εσiei),1)\tilde p^i=(\breve U-\varepsilon\sigma_ie^i,f(\breve U-\varepsilon\sigma_ie^i),1)p~​i=(U˘−εσi​ei,f(U˘−εσi​ei),1) for i∈Ii\in Ii∈I are feasible with respect to (6) and satisfy (6b) for III at equality; here σi=±1\sigma_i=\pm1σi​=±1 is the sign of wiw_iwi​ (with σi=1\sigma_i=1σi​=1 when wi=0w_i=0wi​=0).
  2. For every ε>0\varepsilon>0ε>0 these η+2\eta+2η+2 points are affinely independent.

Significance

The result. Proposition 1 shows that (6) is ideal; Proposition 2 shows it cannot be made smaller: removing any single inequality (6b) produces a strictly weaker relaxation. Since the family has 2∣supp⁡(w)∣2^{|\operatorname{supp}(w)|}2∣supp(w)∣ members, this is what justifies the paper's practical recommendation to start from the big-MMM formulation and separate inequalities of (6b) on demand (Proposition 3, p. 7) rather than to search for a smaller ideal description in the same variables. The facet structure also gives the geometric picture the paper describes after Proposition 2: each facet is the convex combination of an (η−∣I∣)(\eta-|I|)(η−∣I∣)-dimensional face at z=0z=0z=0 and an ∣I∣|I|∣I∣-dimensional face at z=1z=1z=1.

Formalizing it. The result is proved in the paper, in a half-page appendix; it has not been machine-checked. The formalization adds two things. First, the proof is written for w≥0w\ge0w≥0 "without loss of generality by appropriately interchanging +++ and −-−"; the Lean statements are for every sign pattern, including zero weights. Second, the appendix exhibits η+2\eta+2η+2 affinely independent points on the face, which bounds the face dimension from below; the statement that the face has dimension exactly one less than the polyhedron also needs the polyhedron to be full-dimensional and the face to lie in a proper hyperplane, steps the extended abstract leaves implicit and a complete proof must supply.

Difficulty

The arithmetic in each step is elementary. The work lies in the bookkeeping: choosing a single ε\varepsilonε that keeps every perturbed point inside the box and on the correct side of f=0f=0f=0 (this is exactly where strict activity enters), checking the perturbed points against all 2∣supp⁡(w)∣2^{|\operatorname{supp}(w)|}2∣supp(w)∣ inequalities of (6b) and not only the one for III, and turning a row-reduction argument on an (η+1)×(η+2)(\eta+1)\times(\eta+2)(η+1)×(η+2) matrix into a statement about AffineIndependent and finrank of a vectorSpan in Lean. The natural shortcut, proving only that η+2\eta+2η+2 affinely independent tight points exist, is not Proposition 2: it says nothing about the dimension of the polyhedron itself.

Formalization scope

Inputs are Fin η → ℝ (indices 0,…,η−10,\dots,\eta-10,…,η−1 for the paper's 1,…,η1,\dots,\eta1,…,η); a point (x,y,z)(x,y,z)(x,y,z) is p : (Fin η → ℝ) × ℝ × ℝ with p.1 = x, p.2.1 = y, p.2.2 = z. M±(f)M^\pm(f)M±(f) are given by their closed forms w⋅U˘+bw\cdot\breve U+bw⋅U˘+b and w⋅L˘+bw\cdot\breve L+bw⋅L˘+b. In (6b), "i∉Ii\notin Ii∈/I" ranges over all indices outside III, zero weights included; III ranges over subsets of supp⁡(w)\operatorname{supp}(w)supp(w), as on the page.

Every goal and milestone keeps the standing assumptions of §1.3, Li<UiL_i<U_iLi​<Ui​ for all iii and strict activity, except the affine-independence milestone, which holds without them and is stated without them (a stronger statement). No other hypothesis is added. Strict activity excludes η=0\eta=0η=0, so no nonemptiness assumption on the index set is needed.

IsFacetDefining P g is the standard notion: validity, a nonempty face, and dim⁡F+1=dim⁡P\dim F+1=\dim PdimF+1=dimP with dimensions the finrank of the vectorSpan. The equation is written with +1+1+1 on the left so that no natural-number subtraction can make the empty set or a point a facet. The polyhedron is the convex hull of the points of (6), not the set form6 itself (which is not convex, since z∈{0,1}z\in\{0,1\}z∈{0,1}); by Proposition 1 it equals the LP relaxation relax6, but the statement does not depend on that.

The shared objects of this paper (the ReLU graph, L˘\breve LL˘, U˘\breve UU˘, M±M^\pmM±, support, strict activity, formulation (6), ideality) come from the shared definitions module ReluMIP.Ideal.Setting, common to the companion mission on Proposition 1; this mission's own definitions module adds form6, IsFacetDefining, the sign inward, and the indexed family facetPts of the η+2\eta+2η+2 points. The facet notion and the affine-independence argument are reusable for other facet proofs of polyhedra in product spaces. Proofs of the milestones, of the goal, and of the full-dimensionality step are all welcome.

Selected references

  • R. Anderson, J. Huchette, C. Tjandraatmadja, J. P. Vielma, Strong mixed-integer programming formulations for trained neural networks, IPCO 2019, LNCS 11480, pp. 27–42; preprint arXiv:1811.08359v2, 2019. https://arxiv.org/abs/1811.08359v2
  • R. Anderson, J. Huchette, W. Ma, C. Tjandraatmadja, J. P. Vielma, Strong mixed-integer programming formulations for trained neural networks, Mathematical Programming 183 (2020), 3–39. https://doi.org/10.1007/s10107-020-01474-5
  • G. L. Nemhauser, L. A. Wolsey, Integer and Combinatorial Optimization, Wiley, 1988. https://doi.org/10.1002/9781118627372
  • M. Conforti, G. Cornuéjols, G. Zambelli, Integer Programming, Springer, 2014. https://doi.org/10.1007/978-3-319-11008-0
  • J. P. Vielma, Mixed integer linear programming formulation techniques, SIAM Review 57 (2015), 3–57. https://doi.org/10.1137/130915303
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Differential GeometryFunctional AnalysisProbability·Captain: mikedeng1

Bakry–Émery Curvature-Dimension Condition and Riemannian Ricci Curvature Bounds 5: A Product of Riemannian Energy Measure Spaces with BE(K,N_X) and BE(K,N_Y) Satisfies BE(K,N_X+N_Y)Research Paper

Motivation

A lower bound KKK on the Ricci curvature of a Riemannian manifold and an upper bound NNN on its dimension can be expressed without coordinates in two ways. The Bakry–Émery condition BE(K,N)\mathrm{BE}(K,N)BE(K,N) is a property of the heat semigroup and its generator: the iterated carré du champ Γ2\Gamma_2Γ2​ dominates KΓ+1N(Δf)2K\Gamma+\frac1N(\Delta f)^2KΓ+N1​(Δf)2 (Bakry–Émery 1985). The Riemannian curvature-dimension conditions RCD(K,∞)\mathrm{RCD}(K,\infty)RCD(K,∞) and RCD∗(K,N)\mathrm{RCD}^*(K,N)RCD∗(K,N) are properties of a metric measure space, defined through optimal transport (Ambrosio–Gigli–Savaré 2014). A basic test for any notion of "Ricci curvature at least KKK, dimension at most NNN" is its behaviour under products: on a product of manifolds, Ricci curvature bounds combine and dimensions add.

The paper of Ambrosio, Gigli and Savaré (arXiv:1209.5786) proves that BE(K,∞)\mathrm{BE}(K,\infty)BE(K,∞) and RCD(K,∞)\mathrm{RCD}(K,\infty)RCD(K,∞) coincide on a natural class of Dirichlet-form spaces, and draws from it, in its §5.1, two tensorization results. The first (Theorem 5.1) is the stability of RCD(K,∞)\mathrm{RCD}(K,\infty)RCD(K,∞) under products. This had been proved in Ambrosio–Gigli–Savaré 2014 only under a nonbranching assumption on the factors; the equivalence removes that assumption. The second (Theorem 5.2) is the dimensional statement: the product of two Riemannian Energy measure spaces satisfying BE(K,NX)\mathrm{BE}(K,N_X)BE(K,NX​) and BE(K,NY)\mathrm{BE}(K,N_Y)BE(K,NY​) satisfies BE(K,NX+NY)\mathrm{BE}(K,N_X+N_Y)BE(K,NX​+NY​), the bound on the dimension of the product that the smooth case predicts.

Setting

Let XXX be a complete separable metric space with a Borel measure m\mathfrak mm. A Dirichlet form is a quadratic, L2L^2L2-lower semicontinuous, Markovian functional E:L2(X,m)→[0,∞]\mathcal E:L^2(X,\mathfrak m)\to[0,\infty]E:L2(X,m)→[0,∞] with dense domain V\mathbb VV. Its generator ΔE\Delta_{\mathcal E}ΔE​ is defined by E(f,g)=−∫g ΔEf dm\mathcal E(f,g)=-\int g\,\Delta_{\mathcal E}f\,d\mathfrak mE(f,g)=−∫gΔE​fdm for all g∈Vg\in\mathbb Vg∈V, and its heat flow Pt\mathsf P_tPt​ solves ddtPtf=ΔEPtf\frac{d}{dt}\mathsf P_tf=\Delta_{\mathcal E}\mathsf P_tfdtd​Pt​f=ΔE​Pt​f. The carré du champ Γ(f)\Gamma(f)Γ(f) is the density of φ↦E(f,fφ)−12E(f2,φ)\varphi\mapsto\mathcal E(f,f\varphi)-\frac12\mathcal E(f^2,\varphi)φ↦E(f,fφ)−21​E(f2,φ). For ν=1/N≥0\nu=1/N\ge0ν=1/N≥0, BE(K,N)\mathrm{BE}(K,N)BE(K,N) is the weak form (2.33) of Γ2≥KΓ+ν(Δf)2\Gamma_2\ge K\Gamma+\nu(\Delta f)^2Γ2​≥KΓ+ν(Δf)2, written through the functional At[f;φ](s)=12∫(Pt−sf)2Psφ dm\mathsf A_t[f;\varphi](s)=\frac12\int(\mathsf P_{t-s}f)^2\mathsf P_s\varphi\,d\mathfrak mAt​[f;φ](s)=21​∫(Pt−s​f)2Ps​φdm.

The intrinsic distance is dE(x,y)=sup⁡{∣ψ(y)−ψ(x)∣:ψ continuous, Γ(ψ)≤1}\mathsf d_{\mathcal E}(x,y)=\sup\{|\psi(y)-\psi(x)|:\psi\text{ continuous},\ \Gamma(\psi)\le1\}dE​(x,y)=sup{∣ψ(y)−ψ(x)∣:ψ continuous, Γ(ψ)≤1}. An Energy measure space (Definition 3.6) is a strongly local Dirichlet form on a space whose metric is dE\mathsf d_{\mathcal E}dE​, with full-support measure and an exhausting function; a Riemannian Energy measure space (Definition 3.16) is in addition upper regular, and every ψ\psiψ with Γ(ψ)≤1\Gamma(\psi)\le1Γ(ψ)≤1 has a continuous version. An RCD(K,∞)\mathrm{RCD}(K,\infty)RCD(K,∞) space (Definition 3.1) is a length metric measure space with the growth bounds (MD.b) and (MD.exp) on which the relative entropy has an EVIK\mathrm{EVI}_KEVIK​ gradient flow in (P2(X),W2)(\mathscr P_2(X),W_2)(P2​(X),W2​).

The product (5.1) of (X,dX,mX)(X,\mathsf d_X,\mathfrak m_X)(X,dX​,mX​) and (Y,dY,mY)(Y,\mathsf d_Y,\mathfrak m_Y)(Y,dY​,mY​) is Z=X×YZ=X\times YZ=X×Y with

d((x,y),(x′,y′))=dX2(x,x′)+dY2(y,y′),m=mX×mY,\mathsf d((x,y),(x',y'))=\sqrt{\mathsf d_X^2(x,x')+\mathsf d_Y^2(y,y')},\qquad\mathfrak m=\mathfrak m_X\times\mathfrak m_Y,d((x,y),(x′,y′))=dX2​(x,x′)+dY2​(y,y′)​,m=mX​×mY​,

and the Cartesian Dirichlet form (5.2) is

E(f)=∫YEX(fy) dmY(y)+∫XEY(fx) dmX(x),\mathcal E(f)=\int_Y\mathcal E^X(f^y)\,d\mathfrak m_Y(y)+\int_X\mathcal E^Y(f^x)\,d\mathfrak m_X(x),E(f)=∫Y​EX(fy)dmY​(y)+∫X​EY(fx)dmX​(x),

where fy=f(⋅,y)f^y=f(\cdot,y)fy=f(⋅,y) and fx=f(x,⋅)f^x=f(x,\cdot)fx=f(x,⋅).

Formalization targets

Goal: Theorem 5.2

If (X,EX,mX)(X,\mathcal E^X,\mathfrak m_X)(X,EX,mX​) and (Y,EY,mY)(Y,\mathcal E^Y,\mathfrak m_Y)(Y,EY,mY​) are Riemannian Energy measure spaces satisfying (MD.exp), BE(K,NX)\mathrm{BE}(K,N_X)BE(K,NX​) and BE(K,NY)\mathrm{BE}(K,N_Y)BE(K,NY​), then

(Z,E,m) is a Riemannian Energy measure space with dE=d and BE(K,NX+NY).(Z,\mathcal E,\mathfrak m)\ \text{is a Riemannian Energy measure space with}\ \mathsf d_{\mathcal E}=\mathsf d\ \text{and}\ \mathrm{BE}(K,N_X+N_Y).(Z,E,m) is a Riemannian Energy measure space with dE​=d and BE(K,NX​+NY​).

In the parametrization ν=1/N\nu=1/Nν=1/N the product satisfies BE\mathrm{BE}BE with νZ=νXνY/(νX+νY)\nu_Z=\nu_X\nu_Y/(\nu_X+\nu_Y)νZ​=νX​νY​/(νX​+νY​).

Milestones

  1. Corollary 4.18 (i), p. 58: under (MD+exp) and a quadratic Cheeger energy, the length property together with the gradient bound
∣DPtf∣2≤e−2KtPt(∣Df∣w2)(4.30)|\mathrm D\mathsf P_tf|^2\le e^{-2Kt}\mathsf P_t(|\mathrm Df|_w^2)\tag{4.30}∣DPt​f∣2≤e−2KtPt​(∣Df∣w2​)(4.30)

implies RCD(K,∞)\mathrm{RCD}(K,\infty)RCD(K,∞). 2. Theorem 5.1, p. 60: the product of two RCD(K,∞)\mathrm{RCD}(K,\infty)RCD(K,∞) spaces is RCD(K,∞)\mathrm{RCD}(K,\infty)RCD(K,∞). 3. The elementary inequality of p. 62: νXa2+νYb2≥νXνYνX+νY(a+b)2\nu_Xa^2+\nu_Yb^2\ge\frac{\nu_X\nu_Y}{\nu_X+\nu_Y}(a+b)^2νX​a2+νY​b2≥νX​+νY​νX​νY​​(a+b)2 for positive νX,νY\nu_X,\nu_YνX​,νY​ and nonnegative a,ba,ba,b. 4. Lemma 5.3, p. 62: ΔZf(x,y)=ΔXfy(x)+ΔYfx(y)\Delta_Zf(x,y)=\Delta_Xf^y(x)+\Delta_Yf^x(y)ΔZ​f(x,y)=ΔX​fy(x)+ΔY​fx(y) under the fibrewise regularity (5.9), for the RCD factors and their Cheeger forms fixed in §5.1.

Significance

Theorem 5.1 shows that RCD(K,∞)\mathrm{RCD}(K,\infty)RCD(K,∞) is closed under products with no nonbranching condition on the factors, the hypothesis under which Ambrosio–Gigli–Savaré 2014 had obtained it. Theorem 5.2 gives the dimensional version for Dirichlet-form spaces, BE(K,NX)×BE(K,NY)⇒BE(K,NX+NY)\mathrm{BE}(K,N_X)\times\mathrm{BE}(K,N_Y)\Rightarrow\mathrm{BE}(K,N_X+N_Y)BE(K,NX​)×BE(K,NY​)⇒BE(K,NX​+NY​): a product of spaces of finite dimension has finite dimension, with the bound NX+NYN_X+N_YNX​+NY​ of the smooth case, while the condition BE(K,∞)\mathrm{BE}(K,\infty)BE(K,∞) alone loses all dimensional information.

Both results are proved in the paper; none of them, nor the objects they are stated for, has a machine-checked proof. The mission produces a Lean statement of the Cartesian Dirichlet form and of the product structure, the statements of the two tensorization theorems, and the characterization of RCD(K,∞)\mathrm{RCD}(K,\infty)RCD(K,∞) that drives Theorem 5.1. A formal proof would also check the measure-theoretic steps that the paper takes for granted: the measurability of y↦EX(fy)y\mapsto\mathcal E^X(f^y)y↦EX(fy), the Fubini arguments of Lemma 5.3, and the identification of the domain of the Cartesian form (cited from [Ambrosio–Gigli–Savaré 2014], Theorem 6.18).

Difficulty

The obvious argument works fibre by fibre: apply BE(K,NX)\mathrm{BE}(K,N_X)BE(K,NX​) to each section fyf^yfy and BE(K,NY)\mathrm{BE}(K,N_Y)BE(K,NY​) to each fxf^xfx, and add. This fails as stated, because Pt\mathsf P_tPt​ on ZZZ does not act on the sections separately: (Ptf)y(\mathsf P_tf)^y(Pt​f)y is an average over y′y'y′ of the semigroup of XXX applied to fy′f^{y'}fy′, weighted by the heat kernel of YYY, so fibrewise gradient and Laplacian bounds have to be transported through this average. For Theorem 5.2 a second step is not fibrewise at all: before any dimensional estimate, the product has to be shown to be a Riemannian Energy measure space whose intrinsic distance is the product distance, which in the paper goes through Theorem 5.1 and hence through the equivalence BE(K,∞)⇔RCD(K,∞)\mathrm{BE}(K,\infty)\Leftrightarrow\mathrm{RCD}(K,\infty)BE(K,∞)⇔RCD(K,∞) of Theorem 4.17.

Formalization scope

Functions on XXX are X → ℝ, and L2L^2L2 membership is MemLp f 2 m; every object is invariant under m\mathfrak mm-a.e. equality. Dirichlet forms take values in [0,∞][0,\infty][0,∞] and are +∞+\infty+∞ off L2L^2L2. Heat flows are passed as functions pinned by the predicate IsHeatSemigroup. Γ(f)\Gamma(f)Γ(f) is a predicate on a density. BE(K,N)\mathrm{BE}(K,N)BE(K,N) is parametrized by ν=1/N≥0\nu=1/N\ge0ν=1/N≥0; νZ=νXνY/(νX+νY)\nu_Z=\nu_X\nu_Y/(\nu_X+\nu_Y)νZ​=νX​νY​/(νX​+νY​) is 000 when either factor has N=∞N=\inftyN=∞. The product ZZZ is WithLp 2 (X × Y), whose metric is the ℓ2\ell^2ℓ2 distance (5.1); the plain type X × Y would carry the max-metric. The second term of (5.2) uses EY\mathcal E^YEY, correcting the printed EX(fx)\mathcal E^X(f^x)EX(fx). Factors are σ-finite.

Theorem 5.2 assumes (MD.exp) for both factors: its proof invokes Theorem 5.1, whose factors must be RCD(K,∞)\mathrm{RCD}(K,\infty)RCD(K,∞), which a Riemannian Energy measure space with BE(K,∞)\mathrm{BE}(K,\infty)BE(K,∞) is only under (MD.exp). In Corollary 4.18, the minimal weak gradient is written as ∣Df∣w2=Γ(f)|\mathrm Df|_w^2=\Gamma(f)∣Df∣w2​=Γ(f), the identity that (QCh) asserts. Lemma 5.3 carries the RCD and Cheeger-form assumptions established at the opening of §5.1. The elementary inequality retains the printed a,b≥0a,b\ge0a,b≥0; applying it to signed Laplacians requires its all-real extension.

The goal is not met by stating BE\mathrm{BE}BE on the product with νZ=0\nu_Z=0νZ​=0: that is BE(K,∞)\mathrm{BE}(K,\infty)BE(K,∞), a strictly weaker claim; nor by defining the product form through the Cheeger energy of ZZZ instead of (5.2).

A complete development needs the Cartesian form's domain theorem, a pointwise version of the heat semigroups, Theorem 4.17 of the paper and the converse RCD(K,∞)⇒BE(K,∞)\mathrm{RCD}(K,\infty)\Rightarrow\mathrm{BE}(K,\infty)RCD(K,∞)⇒BE(K,∞) from [Ambrosio–Gigli–Savaré 2014]. The product layer (sections, Cartesian form, Lemma 5.3) is reusable for any tensorization argument on Dirichlet forms. Proofs of the elementary inequality and of Lemma 5.3 are the natural first contributions.

Selected references

  • L. Ambrosio, N. Gigli, G. Savaré, Bakry–Émery curvature-dimension condition and Riemannian Ricci curvature bounds, Ann. Probab. 43(1), 339–404, 2015. arXiv:1209.5786v4
  • L. Ambrosio, N. Gigli, G. Savaré, Metric measure spaces with Riemannian Ricci curvature bounded from below, Duke Math. J. 163(7), 1405–1490, 2014. arXiv:1109.0222
  • D. Bakry, M. Émery, Diffusions hypercontractives, Séminaire de Probabilités XIX, Lecture Notes in Math. 1123, 177–206, 1985. doi:10.1007/BFb0075847
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Giunti–Studenikin 2015: Neutrino Oscillations, Majorana Form Factors and Spin PrecessionResearch Paper

Motivation

Neutrinos are the only Standard Model fermions whose masses, mixing and electromagnetic properties are still largely unknown. The review of Giunti and Studenikin (Rev. Mod. Phys. 87, 531 (2015)) collects the theory of neutrino masses and mixing, the general structure of neutrino electromagnetic form factors for Dirac and Majorana neutrinos, and the dynamics of neutrino spin and flavor in electromagnetic fields and matter. Most of the review is phenomenology (experimental bounds, astrophysical estimates), but a core of it consists of exact mathematical statements about finite-dimensional unitary matrices, Hermitian matrices and two-level linear Schrödinger equations. Those exact statements are what this mission targets.

Timeline of the results formalized here:

  • 1957–1968: Pontecorvo; Maki, Nakagawa and Sakata introduce neutrino mixing and oscillations.
  • 1957: Case; Radicati and Touschek observe that Majorana neutrinos cannot have diagonal magnetic or electric dipole moments.
  • 1971: Cisneros proposes spin precession νeL→νeR\nu_{eL}\to\nu_{eR}νeL​→νeR​ of solar neutrinos in a magnetic field.
  • 1978: Wolfenstein writes the evolution equation of neutrino flavor in matter; 1985: Mikheev and Smirnov identify its resonance (MSW effect).
  • 1986: Okun, Voloshin and Vysotsky; Voloshin and Vysotsky show that matter suppresses spin precession.

Setting

A mixing matrix is a unitary n×nn\times nn×n complex matrix UUU whose rows are labelled by flavors ℓ\ellℓ and whose columns are labelled by massive states kkk with masses mkm_kmk​. For a neutrino of energy E>0E>0E>0 that has travelled a distance LLL, the plane-wave transition probability (Eqs. (2.35)–(2.36)) is

Pνℓ→νℓ′(L,E)=∣∑kUℓk∗ e−imk2L/(2E) Uℓ′k∣2.P_{\nu_\ell\to\nu_{\ell'}}(L,E)=\Bigl|\sum_k U^*_{\ell k}\,e^{-i m_k^2 L/(2E)}\,U_{\ell' k}\Bigr|^2 .Pνℓ​→νℓ′​​(L,E)=​k∑​Uℓk∗​e−imk2​L/(2E)Uℓ′k​​2.

In the Lean development this is oscProb U m L E l l'. The standard parametrization UD(ϑ12,ϑ13,ϑ23,δ13)U^{\mathrm D}(\vartheta_{12},\vartheta_{13},\vartheta_{23},\delta_{13})UD(ϑ12​,ϑ13​,ϑ23​,δ13​) of Eq. (2.27) and the Majorana phase matrix DM=diag⁡(1,eiλ21,eiλ31)D^{\mathrm M}=\operatorname{diag}(1,e^{i\lambda_{21}},e^{i\lambda_{31}})DM=diag(1,eiλ21​,eiλ31​) of Eq. (2.28) are diracMixing and majoranaPhases; the two-neutrino rotation matrix of Eq. (2.38) is twoFlavorMixing.

In matter of constant electron density, the νe\nu_eνe​–νa\nu_aνa​ amplitudes (φe,φa)(\varphi_e,\varphi_a)(φe​,φa​) obey i ddxφ=Hφi\,\tfrac{d}{dx}\varphi=\mathrm H\varphiidxd​φ=Hφ with the effective Hamiltonian of Eq. (2.46) (mswHamiltonian), built from the vacuum squared-mass difference Δm2\Delta m^2Δm2, the mixing angle ϑ\varthetaϑ and the charged-current potential VCCV_{\rm CC}VCC​ with ACC=2EVCCA_{\rm CC}=2EV_{\rm CC}ACC​=2EVCC​. The effective squared-mass difference ΔmM2\Delta m^2_{\rm M}ΔmM2​ of Eq. (2.53) and effective angle ϑM\vartheta_{\rm M}ϑM​ of Eq. (2.54) are mswDeltaM2 and mswMixingAngle.

Electromagnetic form-factor matrices fΩ\mathbb f_\OmegafΩ​ (Ω=Q,M,E,A\Omega=Q,M,E,AΩ=Q,M,E,A: charge, magnetic, electric, anapole) are Hermitian N×NN\times NN×N complex matrices in the space of massive neutrinos; for Majorana neutrinos they are in addition antisymmetric (Ω=Q,M,E\Omega=Q,M,EΩ=Q,M,E) or symmetric (Ω=A\Omega=AΩ=A), Eqs. (3.66)–(3.68).

Finally, the helicity amplitudes (ψL,ψR)(\psi_L,\psi_R)(ψL​,ψR​) of an ultrarelativistic Dirac neutrino with magnetic moment μ\muμ in a transverse field B⊥B_\perpB⊥​ and matter potential VVV obey i ddxψ=(VμB⊥μB⊥0)ψi\,\tfrac{d}{dx}\psi=\begin{pmatrix}V&\mu B_\perp\\ \mu B_\perp&0\end{pmatrix}\psiidxd​ψ=(VμB⊥​​μB⊥​0​)ψ (Eqs. (6.23), (6.28); spinFlavorHamiltonian), with energy splitting ΔEM=V2+(2μB⊥)2\Delta E_{\rm M}=\sqrt{V^2+(2\mu B_\perp)^2}ΔEM​=V2+(2μB⊥​)2​ (Eq. (6.31); spinFlavorEnergySplitting).

Formalization targets

Goal: the general vacuum oscillation probability, Eq. (2.37)

For every unitary UUU, all masses mkm_kmk​, every LLL and every E>0E>0E>0,

Pνℓ→νℓ′=δℓℓ′−4∑k>jRe⁡(Uℓk∗Uℓ′kUℓjUℓ′j∗)sin⁡2 ⁣(Δmkj2L4E)−2∑k>jIm⁡(UℓkUℓj∗Uℓ′k∗Uℓ′j)sin⁡ ⁣(Δmkj2L2E),P_{\nu_\ell\to\nu_{\ell'}}=\delta_{\ell\ell'}-4\sum_{k>j}\operatorname{Re}\bigl(U^*_{\ell k}U_{\ell' k}U_{\ell j}U^*_{\ell' j}\bigr)\sin^2\!\Bigl(\frac{\Delta m^2_{kj}L}{4E}\Bigr)-2\sum_{k>j}\operatorname{Im}\bigl(U_{\ell k}U^*_{\ell j}U^*_{\ell' k}U_{\ell' j}\bigr)\sin\!\Bigl(\frac{\Delta m^2_{kj}L}{2E}\Bigr),Pνℓ​→νℓ′​​=δℓℓ′​−4k>j∑​Re(Uℓk∗​Uℓ′k​Uℓj​Uℓ′j∗​)sin2(4EΔmkj2​L​)−2k>j∑​Im(Uℓk​Uℓj∗​Uℓ′k∗​Uℓ′j​)sin(2EΔmkj2​L​),

with Δmkj2=mk2−mj2\Delta m^2_{kj}=m_k^2-m_j^2Δmkj2​=mk2​−mj2​. The number nnn of massive states is left free (the paper uses n=3n=3n=3, and n>3n>3n>3 with sterile neutrinos, Sec. II.F).

Milestones

  1. Eqs. (2.26)–(2.28): UDU^{\mathrm D}UD and UDDMU^{\mathrm D}D^{\mathrm M}UDDM are unitary.
  2. Eq. (2.39): two-neutrino transition probability sin⁡22ϑ sin⁡2(Δm2L/4E)\sin^2 2\vartheta\,\sin^2(\Delta m^2L/4E)sin22ϑsin2(Δm2L/4E).
  3. Eq. (2.40): two-neutrino survival probability 1−sin⁡22ϑ sin⁡2(Δm2L/4E)1-\sin^2 2\vartheta\,\sin^2(\Delta m^2L/4E)1−sin22ϑsin2(Δm2L/4E).
  4. Eqs. (2.50)–(2.54): UMTHUM=diag⁡(−ΔmM2,ΔmM2)/4EU_{\rm M}^T\mathrm H U_{\rm M}=\operatorname{diag}(-\Delta m^2_{\rm M},\Delta m^2_{\rm M})/4EUMT​HUM​=diag(−ΔmM2​,ΔmM2​)/4E.
  5. Eq. (2.57): MSW transition probability at constant density sin⁡22ϑMsin⁡2(ΔmM2x/4E)\sin^2 2\vartheta_{\rm M}\sin^2(\Delta m^2_{\rm M}x/4E)sin22ϑM​sin2(ΔmM2​x/4E).
  6. Eqs. (3.66)–(3.70): Majorana form-factor matrices — antisymmetric Hermitian matrices are purely imaginary with vanishing diagonal; symmetric Hermitian matrices are real.
  7. Eqs. (3.71)–(3.72): three-flavor antisymmetric Hermitian form factors are i∑jϵfijf~ji\sum_j\epsilon^{fij}\tilde{\mathbb f}^ji∑j​ϵfijf~​j with a real vector f~\tilde{\mathbb f}f~​.
  8. Eq. (6.27): spin precession in a transverse field, PνL→νR(x)=sin⁡2(∫0xμB⊥)P_{\nu_L\to\nu_R}(x)=\sin^2\bigl(\int_0^x\mu B_\perp\bigr)PνL​→νR​​(x)=sin2(∫0x​μB⊥​).
  9. Eq. (6.34): spin precession in matter, PνL→νR(x)=sin⁡22ξ sin⁡2(12ΔEMx)P_{\nu_L\to\nu_R}(x)=\sin^2 2\xi\,\sin^2(\tfrac12\Delta E_{\rm M}x)PνL​→νR​​(x)=sin22ξsin2(21​ΔEM​x) with sin⁡2ξ=2μB⊥/ΔEM\sin 2\xi=2\mu B_\perp/\Delta E_{\rm M}sin2ξ=2μB⊥​/ΔEM​.

Significance

Eq. (2.37) is the formula used in essentially every analysis of oscillation data; its two-neutrino specializations (2.39)–(2.40) and the matter formula (2.57) are the standard fitting functions for reactor, accelerator and solar experiments. The Majorana constraints (3.67)–(3.70) are the precise statement behind the claim that a measured diagonal magnetic moment would rule out Majorana neutrinos (under CPT). The spin-precession formulas (6.27) and (6.34) underlie the astrophysical bounds on neutrino magnetic moments.

All targets are established results with textbook derivations; none is open. What the mission adds is machine-checked versions with every convention (sign of the phase, ordering k>jk>jk>j, ranges of angles, boundary conditions of the Schrödinger equation) fixed explicitly. Related vacuum-oscillation statements from a different source already exist on the platform under the LipariNeutrino namespace; the present drafts are self-contained and follow this paper's notation and equation numbering.

Difficulty

The algebraic targets require careful bookkeeping of complex conjugation and of the unitarity relations UU†=U†U=1UU^\dagger=U^\dagger U=1UU†=U†U=1 inside double sums over k>jk>jk>j. The dynamical targets (2.57), (6.27), (6.34) are statements about every solution of a linear ODE with a given initial value, so a solution in closed form is not enough: uniqueness of solutions of the (for (6.27), non-autonomous) linear system must also be established in Lean.

Formalization scope

  • Flavor and mass indices are Fin n; two-neutrino indices 0,1 stand for (νe,νa)(\nu_e,\nu_a)(νe​,νa​), (νL,νR)(\nu_L,\nu_R)(νL​,νR​) or (ν1,ν2)(\nu_1,\nu_2)(ν1​,ν2​).
  • Masses mkm_kmk​ are arbitrary reals and enter only through mk2m_k^2mk2​.
  • Unitarity is membership in Matrix.unitaryGroup.
  • The evolution equations are encoded as HasDerivAt φ (-(I • H.mulVec (φ x))) x for all real xxx, i.e. φ′=−iHφ\varphi'=-i\mathrm H\varphiφ′=−iHφ, with initial value (1,0)(1,0)(1,0).
  • ϑM\vartheta_{\rm M}ϑM​ is defined as half the argument of (Δm2cos⁡2ϑ−2EVCC)+i Δm2sin⁡2ϑ(\Delta m^2\cos2\vartheta-2EV_{\rm CC})+i\,\Delta m^2\sin2\vartheta(Δm2cos2ϑ−2EVCC​)+iΔm2sin2ϑ, which realizes Eq. (2.54) without the division-by-zero at resonance; sin⁡2ξ=2μB⊥/ΔEM\sin 2\xi=2\mu B_\perp/\Delta E_{\rm M}sin2ξ=2μB⊥​/ΔEM​ is inlined, with Lean's convention 0/0=00/0=00/0=0 in the degenerate case V=μB⊥=0V=\mu B_\perp=0V=μB⊥​=0.
  • The source's angle ranges (0≤ϑ≤π/20\le\vartheta\le\pi/20≤ϑ≤π/2, 0≤δ13<2π0\le\delta_{13}<2\pi0≤δ13​<2π) and E>0E>0E>0 are kept as hypotheses.

Useful reusable infrastructure: uniqueness for linear ODEs in C2\mathbb C^2C2, closed-form exponentials of 2×22\times22×2 real symmetric matrices, and algebraic lemmas for unitary matrices.

Selected references

  • C. Giunti and A. Studenikin, Neutrino electromagnetic interactions: A window to new physics, Rev. Mod. Phys. 87, 531 (2015). https://doi.org/10.1103/RevModPhys.87.531
  • C. Giunti and C. W. Kim, Fundamentals of Neutrino Physics and Astrophysics, Oxford University Press (2007).
  • L. Wolfenstein, Neutrino oscillations in matter, Phys. Rev. D 17, 2369 (1978). https://doi.org/10.1103/PhysRevD.17.2369
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Linear algebraMathematical Physics·Captain: Lucas

Baumgarten 2018: How to (Un-) Quantum Mechanics — Phase-Space AlgebraResearch Paper

Motivation

C. Baumgarten's essay How to (Un-) Quantum Mechanics (arXiv:1810.06981, v2 2025) argues that much of the mathematical formalism usually presented as specifically "quantum" — Heisenberg's equation of motion, commutators, eigenvalue problems, the real Pauli and Dirac algebras — already follows from classical linear Hamiltonian mechanics on an abstract phase space. The physical and philosophical claims of the paper are outside the scope of a formalization, but its argument rests on a compact chain of linear-algebra facts stated in Sections IV–VI (pp. 13–20). This mission formalizes exactly that chain, so that the mathematical part of the argument can be checked independently of its interpretation.

Setting

Fix a number n≥0n \ge 0n≥0 of degrees of freedom. A phase-space vector is ψ=(q1,p1,…,qn,pn)T∈R2n\psi = (q_1,p_1,\dots,q_n,p_n)^T \in \mathbb R^{2n}ψ=(q1​,p1​,…,qn​,pn​)T∈R2n. The symplectic unit matrix is the Kronecker product

γ0=1n⊗η0,η0=(01−10).\gamma_0 = \mathbf 1_n \otimes \eta_0, \qquad \eta_0 = \begin{pmatrix}0 & 1\\ -1 & 0\end{pmatrix}.γ0​=1n​⊗η0​,η0​=(0−1​10​).

A real 2n×2n2n\times 2n2n×2n matrix is Hamiltonian if it equals γ0A\gamma_0 Aγ0​A with AAA symmetric, skew-Hamiltonian if it equals γ0B\gamma_0 Bγ0​B with BBB skew-symmetric, and symplectic if Mγ0MT=γ0M\gamma_0M^T = \gamma_0Mγ0​MT=γ0​.

Linear Hamiltonian motion is ψ˙=Hψ\dot\psi = H\psiψ˙​=Hψ with HHH Hamiltonian (the paper's Eq. 35, coming from the quadratic Hamiltonian 12ψTAψ\tfrac12\psi^TA\psi21​ψTAψ). A matrix of second moments Σ(τ)\Sigma(\tau)Σ(τ) (in the paper an average ⟨ψψT⟩\langle\psi\psi^T\rangle⟨ψψT⟩) then evolves by

Σ˙=HΣ+ΣHT(Eq. 40),\dot\Sigma = H\Sigma + \Sigma H^T \qquad\text{(Eq. 40)},Σ˙=HΣ+ΣHT(Eq. 40),

and the autocorrelation matrix is S=Σγ0TS = \Sigma\gamma_0^TS=Σγ0T​.

Target

The goal theorem combines the conclusions drawn on pp. 16–17: for HHH Hamiltonian and Σ\SigmaΣ a symmetric solution of Eq. (40), the autocorrelation matrix satisfies, for every time τ\tauτ,

χS(τ)=χS(0)andTr⁡(S(τ)2k+1)=0  (k∈N),\chi_{S(\tau)} = \chi_{S(0)} \qquad\text{and}\qquad \operatorname{Tr}\big(S(\tau)^{2k+1}\big) = 0 \ \ (k \in \mathbb N),χS(τ)​=χS(0)​andTr(S(τ)2k+1)=0  (k∈N),

where χ\chiχ is the characteristic polynomial: "the eigenvalues are constants of motion" (after Eq. 51) together with Eq. (48).

The milestones follow the paper's own steps, in order:

  1. pairing ±λ\pm\lambda±λ of eigenvalues of skew-symmetric matrices, and a vanishing eigenvalue in odd size (p. 13);
  2. conservation of HHH under ψ˙=J∇H\dot\psi = J\nabla Hψ˙​=J∇H with JJJ skew (Eqs. 26–28);
  3. identities of γ0\gamma_0γ0​ and the transpose rules for (skew-)Hamiltonian matrices (Eqs. 33, 36, 54);
  4. exp⁡(Hτ)ψ0\exp(H\tau)\psi_0exp(Hτ)ψ0​ solves ψ˙=Hψ\dot\psi = H\psiψ˙​=Hψ (Eq. 49);
  5. Heisenberg's equation S˙=[H,S]\dot S = [H,S]S˙=[H,S] for second moments (Eq. 42);
  6. the Lax invariants Tr⁡(Sk)\operatorname{Tr}(S^k)Tr(Sk) (Eq. 47) and tracelessness of odd powers (Eq. 48);
  7. symplecticity of exp⁡(Hτ)\exp(H\tau)exp(Hτ) and S(τ)=M(τ)S(0)M(−τ)S(\tau) = M(\tau)S(0)M(-\tau)S(τ)=M(τ)S(0)M(−τ) (Eqs. 50–51);
  8. the dimension counts n(2n+1)n(2n+1)n(2n+1) and n(2n−1)n(2n-1)n(2n−1) (Eqs. 55–56) and the (anti-)commutator table (Eq. 57);
  9. the matrix Euler formulas for the real Pauli matrices (Eq. 66).

Significance

The result itself. Each statement is classical linear algebra or linear ODE theory; the paper uses them to argue that Heisenberg's equation and the spectral description of observables arise from second moments of a classical Hamiltonian ensemble. A checked version separates what is a theorem from what is interpretation, and pins down the hypotheses (for example, that only symmetry of AAA is needed for Eq. 48, not positive definiteness).

Formalizing it. None of these statements is new mathematics; the work is to formalize them in the paper's notation (γ0=1n⊗η0\gamma_0 = \mathbf 1_n\otimes\eta_0γ0​=1n​⊗η0​, entrywise matrix derivatives, the matrix exponential) so that they can be reused for later parts of the paper, such as the real Dirac algebra of Sec. VII–VIII.

Difficulty

Most milestones are short calculations. The two steps needing real infrastructure are (i) the uniqueness of solutions of the linear matrix ODE S˙=[H,S]\dot S = [H,S]S˙=[H,S], needed to identify S(τ)S(\tau)S(τ) with exp⁡(Hτ)S(0)exp⁡(−Hτ)\exp(H\tau)S(0)\exp(-H\tau)exp(Hτ)S(0)exp(−Hτ), and (ii) the dimension counts, which require an explicit basis or an isomorphism with symmetric/skew-symmetric matrices. Going through the Lax invariants alone gives only the traces of powers of SSS, and recovering the characteristic polynomial from them needs Newton's identities; the similarity form of Eq. (51) gives the conservation of the characteristic polynomial directly.

Formalization scope

Everything is over R\mathbb RR. Matrices are indexed by pairs (i,b)(i,b)(i,b), i<ni<ni<n, b∈{0,1}b\in\{0,1\}b∈{0,1}, so that γ0\gamma_0γ0​ is literally a Kronecker product; n=0n = 0n=0 is allowed. Time derivatives of matrix-valued functions are entrywise HasDerivAt; exp⁡\expexp is Mathlib's power-series NormedSpace.exp. A Hamiltonian matrix is γ0A\gamma_0Aγ0​A with AAA symmetric (no definiteness); Σ\SigmaΣ is any symmetric solution of Eq. (40) — positivity is not assumed because it is not used. Eigenvalues of real skew-symmetric matrices are taken over C\mathbb CC. "Number of linearly independent elements" is the dimension of the real span. No statement is vacuous: all hypotheses are satisfied, for example, by H=γ0H = \gamma_0H=γ0​ and Σ≡1\Sigma \equiv \mathbf 1Σ≡1.

All statements share the definition file UnQM_phase_space and the namespace UnQuantumMechanics.

Selected references

  • C. Baumgarten, How to (Un-) Quantum Mechanics, arXiv:1810.06981v2 [physics.gen-ph], 2025. https://arxiv.org/abs/1810.06981
  • P. D. Lax, Integrals of nonlinear equations of evolution and solitary waves, Comm. Pure Appl. Math. 21 (1968), 467–490. https://doi.org/10.1002/cpa.3160210503
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