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Convex OptimizationOperations ResearchOptimization·Captain: Shuze Chen

Convex Optimization III: Conic Duality and the S-procedureTextbook

Two quadratic functions can be compared losslessly. The S-procedure says that, when the constraint is strictly feasible, the implication

q1(x)≤0  ⟹  q2(x)≤0,qk(x)=xTFkx+2gkTx+hk,q_1(x) \le 0 \;\Longrightarrow\; q_2(x) \le 0, \qquad q_k(x) = x^{T}F_k x + 2g_k^{T}x + h_k,q1​(x)≤0⟹q2​(x)≤0,qk​(x)=xTFk​x+2gkT​x+hk​,

holds if and only if a single nonnegative multiplier certifies it as a matrix inequality, λ[F1g1g1Th1]⪰[F2g2g2Th2]\lambda \begin{bmatrix} F_1 & g_1 \\ g_1^{T} & h_1\end{bmatrix} \succeq \begin{bmatrix} F_2 & g_2 \\ g_2^{T} & h_2\end{bmatrix}λ[F1​g1T​​g1​h1​​]⪰[F2​g2T​​g2​h2​​] for some λ≥0\lambda \ge 0λ≥0. It is a cornerstone of control theory, trust-region methods and robust optimization, and a rare case in which a nonconvex problem has zero duality gap. The route runs through the theory this mission builds from Boyd & Vandenberghe §5.8–5.9 and Appendix B: strong alternatives for convex inequality systems, cone-program strong duality under a generalized Slater condition, semidefinite programming duality, the LMI theorems of alternatives, and the hidden convexity of the joint range of two quadratic forms.

17 thms5 active usersReviewed
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Convex OptimizationOperations ResearchOptimization·Captain: Shuze Chen

Convex Optimization I: Prékopa's TheoremTextbook

Log-concave functions are the meeting point of convex analysis and probability: densities of Gaussian, exponential, uniform and Wishart distributions are all log-concave, and countless facts of applied probability flow from one structural theorem — integrating out variables preserves log-concavity. This mission builds the convex-analysis spine of Boyd & Vandenberghe's Convex Optimization (Chapters 2–3) — separation and supporting hyperplanes, dual cones, the first- and second-order differential characterizations of convexity, Fenchel conjugacy — and climbs to Prékopa's theorem via the Prékopa–Leindler inequality, a landmark of Brunn–Minkowski theory absent from Mathlib.

29 thms5 active usersReviewed
🏆Completed
Machine LearningOperations ResearchQuantum Information+1·Captain: tianyipeng

Markov Entanglement: Value Decomposition Error in Multi-agent MDPsResearch Paper

Value decomposition — approximating the value of a joint state by a sum of per-agent local values — is a staple of multi-agent dynamic programming and reinforcement learning, from index policies for restless bandits to modern MARL architectures, yet it is normally used without justification. Chen and Peng (arXiv:2506.02385) supply one. They show a multi-agent MDP admits an exact value decomposition precisely when its transition matrix is not entangled — a notion built in direct analogy with quantum entanglement — and then turn that qualitative characterisation into a quantitative one: a measure of Markov entanglement bounds the decomposition error in general. This mission formalizes that core theory. The goal is Theorem 6, the general N-agent bound in the occupancy-weighted norm; the milestones are the equivalence between separability and exact decomposition, the perturbation machinery that carries a one-step transition error into a value-function error, and the extensions to shared global state and shared rewards. The paper's restless-bandit application, which needs mean-field machinery of its own, is left to a second mission in the series.

25 thms5 active usersReviewed
🏆Completed
Optimal TransportPure Mathematics·Captain: ykanoria

Excursion Coupling for the Monge Problem on the Line (Juillet 2019)Research Paper

The Monge optimal transport problem on the real line with the classical distance cost ∣x−y∣|x-y|∣x−y∣ famously fails to have a unique solution. Juillet (2019) restored uniqueness by considering the strictly concave power costs ∣x−y∣p|x-y|^p∣x−y∣p with p<1p<1p<1 and letting p→1−p\to 1^-p→1−: the limit selects a distinguished optimal plan, the excursion coupling, built from the level sets of the difference Fσ=Fμ−FνF_\sigma=F_\mu-F_\nuFσ​=Fμ​−Fν​ of the cumulative distribution functions. This mission formalizes the completed-graph construction, the generalized Banach indicatrix identities of Bertoin-Yor, the alternating crossing structure of almost every level, and the marginal identities for the crossing counting measures. It culminates in Propositions 3.5-3.6: every monotone transport plan is concentrated on the paired routes, and the marginals uniquely determine the coupling carried by those routes, including in the presence of atoms.

This mission formalizes the key implication 3=>4 in Juillet's Main Theorem.

37 thms5 active usersReviewed
🏆Completed
Linear OptimizationOperations ResearchOptimization·Captain: Shuze Chen

Introduction to Linear Optimization X: Max-Flow Min-CutTextbook

How much flow can be sent from a source sss to a sink ttt through a network with arc capacities uij∈(0,∞]u_{ij}\in(0,\infty]uij​∈(0,∞] — and what certifies that no more is possible? This mission formalizes §7.4-7.5 of Bertsimas & Tsitsiklis. The circulation calculus of §7.4 supplies the two structural tools: the flow decomposition theorem (Lemma 7.1 — every nonzero nonnegative circulation is a positive combination f=∑iaifi\mathbf{f}=\sum_i a_i\mathbf{f}^if=∑i​ai​fi of simple circulations with only forward arcs, with integer aia_iai​ when f\mathbf{f}f is integer) and the optimality criterion for the minimum cost network flow problem (Theorem 7.6 — a feasible flow is optimal if and only if there is no unsaturated cycle with negative cost). Section 7.5 then formulates the maximum flow problem (max⁡bs\max b_smaxbs​ s.t. Af=b\mathbf{A}\mathbf{f}=\mathbf{b}Af=b, bt=−bsb_t=-b_sbt​=−bs​, bi=0b_i=0bi​=0 for i≠s,ti\ne s,ti=s,t, 0≤f≤u0\le\mathbf{f}\le\mathbf{u}0≤f≤u), defines augmenting paths (Definition 7.2: fij<uijf_{ij}<u_{ij}fij​<uij​ on forward arcs, fij>0f_{ij}>0fij​>0 on backward arcs) and the Ford–Fulkerson algorithm, and proves integer invariance and finite termination for integer capacities (Theorem 7.8). The goal is Theorem 7.10:

(a) if the Ford–Fulkerson algorithm terminates because no augmenting path can be found, the current flow is optimal;

(b) the value of the maximum flow equals the minimum cut capacity

C(S)=∑{(i,j)∈A∣i∈S, j∉S}uijC(S)=\sum_{\{(i,j)\in\mathcal{A}\mid i\in S,\,j\notin S\}}u_{ij}C(S)={(i,j)∈A∣i∈S,j∈/S}∑​uij​

— the archetypal combinatorial min-max theorem, which the book notes can also be read as LP duality (pp. 311-312).

14 thms5 active usersReviewed
🏆Completed
Bandit AlgorithmsMachine LearningOperations Research·Captain: Shuze Chen

Bandit Algorithms XIII: Pure Exploration and Best-Arm IdentificationTextbook

Sometimes reward during learning is irrelevant — a pharmaceutical company running phase-II trials only cares about identifying the best treatment, as quickly and as reliably as possible. Chapter 33 of Lattimore–Szepesvári formalizes fixed-confidence best-arm identification: a policy together with a stopping time τ\tauτ and a recommendation must be sound (wrong with probability at most δ\deltaδ) while minimizing E[τ]\mathbb{E}[\tau]E[τ]. The information-theoretic complexity is c∗(ν)−1=sup⁡α∈Pk−1inf⁡ν′∈Ealt(ν)∑iαiD(νi,νi′)c^*(\nu)^{-1} = \sup_{\alpha\in\mathcal{P}_{k-1}} \inf_{\nu'\in\mathcal{E}_{alt}(\nu)} \sum_i \alpha_i D(\nu_i, \nu_i')c∗(ν)−1=supα∈Pk−1​​infν′∈Ealt​(ν)​∑i​αi​D(νi​,νi′​): every sound strategy needs E[τ]≥c∗(ν)log⁡14δ\mathbb{E}[\tau] \ge c^*(\nu)\log\frac{1}{4\delta}E[τ]≥c∗(ν)log4δ1​, and the Track-and-Stop algorithm — the goal theorem — achieves lim⁡δ→0E[τ]/log⁡(1/δ)=c∗(ν)\lim_{\delta\to 0} \mathbb{E}[\tau]/\log(1/\delta) = c^*(\nu)limδ→0​E[τ]/log(1/δ)=c∗(ν) exactly. The mission also covers the fixed-budget counterpart, sequential halving.

50 thms5 active usersReviewed
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Bandit AlgorithmsMachine LearningOperations Research·Captain: Shuze Chen

Bandit Algorithms IV: Bernoulli Bandits and KL-UCBTextbook

When rewards are binary — a click or no click, a cure or no cure — the subgaussian machinery of Missions I–III is not tight: the variance of a Bernoulli arm degrades near the boundary of [0,1][0,1][0,1], and the correct exponential rate is governed by the binary relative entropy d(p,q)=plog⁡pq+(1−p)log⁡1−p1−qd(p,q) = p\log\frac{p}{q} + (1-p)\log\frac{1-p}{1-q}d(p,q)=plogqp​+(1−p)log1−q1−p​ rather than a squared distance. Chapter 10 of Lattimore–Szepesvári develops Chernoff's tail bound in its information-theoretic form and the KL-UCB algorithm, whose upper confidence bounds are level sets of ddd. The goal theorem shows KL-UCB attains

lim sup⁡n→∞Rn/log⁡n=∑i:Δi>0Δi/d(μi,μ∗)\limsup_{n\to\infty} R_n/\log n = \sum_{i:\Delta_i>0} \Delta_i/d(\mu_i, \mu^*)n→∞limsup​Rn​/logn=i:Δi​>0∑​Δi​/d(μi​,μ∗)

— asymptotic optimality with exactly the constant demanded by the lower bound of Mission VII, strictly improving subgaussian UCB on every Bernoulli instance.

25 thms5 active usersReviewed
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Bandit AlgorithmsMachine LearningOperations Research·Captain: Shuze Chen

Bandit Algorithms VI: Information-Theoretic FoundationsTextbook

Every lower bound in bandit theory rests on one question: how hard is it to tell two probability measures apart from a sample? The answer is quantified by the relative entropy D(P,Q)D(P,Q)D(P,Q), and the sharpest elementary tool is the Bretagnolle–Huber inequality: for any event AAA, P(A)+Q(Ac)≥12exp⁡(−D(P,Q))P(A) + Q(A^c) \ge \frac{1}{2}\exp(-D(P,Q))P(A)+Q(Ac)≥21​exp(−D(P,Q)) — no test can distinguish PPP from QQQ with total error probability below 12e−D(P,Q)\frac{1}{2}e^{-D(P,Q)}21​e−D(P,Q). This mission formalizes Chapter 14 of Lattimore–Szepesvári: the Bretagnolle–Huber inequality (the goal theorem, proved via Le Cam's inequality ∫p∧q≥12(∫pq)2\int p \wedge q \ge \frac{1}{2}(\int\sqrt{pq})^2∫p∧q≥21​(∫pq​)2), Pinsker's inequality δ(P,Q)≤D(P,Q)/2\delta(P,Q) \le \sqrt{D(P,Q)/2}δ(P,Q)≤D(P,Q)/2​, and the closed-form divergences between Gaussians and Bernoullis. These half-page inequalities power every impossibility result in Missions VII, XI and beyond.

5 thms5 active usersReviewed
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Operations ResearchProbabilityStatistics·Captain: mikedeng1

AI Agents for Inventory Control: Human-LLM-OR Complementarity: P[CE > δ] ≥ sup_t (F_a(t) − F_b(t + δ)) for Every Joint Law of (a, b), with Equality for Some CouplingResearch Paper

Motivation

Large language models are now deployed as decision aids next to human decision-makers, and a basic empirical question is whether the pair does better than either party alone. Baek, Fu, Ma and Peng (arXiv:2602.12631v2) study this question for inventory control: they build a benchmark of multi-period inventory problems, compare operations-research policies, LLM agents and their hybrids, and run a classroom experiment in which students manage inventory with and without an AI assistant.

The experiment raises a statistical issue that is independent of inventory control. Average gains at the population level do not show that any individual benefits: if weak decision-makers simply adopt the AI's recommendation and strong ones ignore it, the average collaborative performance can exceed both stand-alone averages while no single person improves on the better of their own and the AI's performance. The quantity of interest is therefore the fraction of individuals who benefit, and it is not identified: each person is observed in only one condition (alone or with the AI), so the joint law of the two outcomes is unknown and only their marginal laws can be estimated.

Section 6.1 of the paper answers this with a distribution-free lower bound on the fraction of individuals whose gain exceeds a threshold, computed from the two marginal distributions alone, and shows that the bound cannot be improved. The bound is an instance of the classical bounds on the distribution of a difference of two random variables with given marginals (Makarov, 1981; Rüschendorf, 1982; Frank, Nelsen and Schweizer, 1987), applied to the identification problem of a human–AI experiment.

Setting

A person iii is drawn from a population. Write yH(i)y_H^{(i)}yH(i)​ for their performance alone, yAIy_{AI}yAI​ for the AI's performance, and yH+AI(i)y_{H+AI}^{(i)}yH+AI(i)​ for their performance with the AI. The individual complementarity effect is

CEi=yH+AI(i)−max⁡(yH(i),yAI).\mathrm{CE}_i = y_{H+AI}^{(i)} - \max\bigl(y_H^{(i)}, y_{AI}\bigr).CEi​=yH+AI(i)​−max(yH(i)​,yAI​).

Set a(i)=max⁡(yH(i),yAI)a(i) = \max(y_H^{(i)}, y_{AI})a(i)=max(yH(i)​,yAI​) and b(i)=yH+AI(i)b(i) = y_{H+AI}^{(i)}b(i)=yH+AI(i)​, so that CEi=b(i)−a(i)\mathrm{CE}_i = b(i) - a(i)CEi​=b(i)−a(i). In the formal development the population is a probability space (Ω,P)(\Omega, P)(Ω,P) and a,b:Ω→Ra, b : \Omega \to \mathbb Ra,b:Ω→R are measurable functions.

The cumulative distribution function of a probability law μ\muμ on R\mathbb RR is the right-continuous function F(t)=μ((−∞,t])F(t) = \mu((-\infty, t])F(t)=μ((−∞,t]); FaF_aFa​ and FbF_bFb​ denote those of aaa and bbb. A joint law (coupling) of (a,b)(a, b)(a,b) with marginals μa,μb\mu_a, \mu_bμa​,μb​ is a probability measure π\piπ on R2\mathbb R^2R2 whose first and second marginals are μa\mu_aμa​ and μb\mu_bμb​. For a threshold δ≥0\delta \ge 0δ≥0 the bound is

ε(δ)=sup⁡t∈R(Fa(t)−Fb(t+δ)),\varepsilon(\delta) = \sup_{t \in \mathbb R} \bigl(F_a(t) - F_b(t + \delta)\bigr),ε(δ)=t∈Rsup​(Fa​(t)−Fb​(t+δ)),

called makarovBound δ μa μb in Lean.

Formalization targets

Goal: Theorem 1 (p. 17)

For every δ≥0\delta \ge 0δ≥0:

  1. for every population law of (a,b)(a, b)(a,b),
P[CEi>δ]  ≥  sup⁡t∈R(Fa(t)−Fb(t+δ));\mathbb P[\mathrm{CE}_i > \delta] \;\ge\; \sup_{t \in \mathbb R}\bigl(F_a(t) - F_b(t + \delta)\bigr);P[CEi​>δ]≥t∈Rsup​(Fa​(t)−Fb​(t+δ));
  1. for any two marginal laws μa,μb\mu_a, \mu_bμa​,μb​ on R\mathbb RR there is a joint law π\piπ with these marginals under which π[b−a>δ]=ε(δ)\pi[b - a > \delta] = \varepsilon(\delta)π[b−a>δ]=ε(δ).

Both clauses are part of the goal. The first says the bound is valid; the second says it is the best bound obtainable from the marginals.

Milestones (Appendix K, p. 46)

  • (5): P[CEi>δ]≥P[b>t+δ, a≤t]\mathbb P[\mathrm{CE}_i > \delta] \ge \mathbb P[b > t + \delta,\ a \le t]P[CEi​>δ]≥P[b>t+δ, a≤t] for every ttt.
  • (6): P[b>t+δ, a≤t]≥(1−Fb(t+δ))+Fa(t)−1=Fa(t)−Fb(t+δ)\mathbb P[b > t + \delta,\ a \le t] \ge (1 - F_b(t + \delta)) + F_a(t) - 1 = F_a(t) - F_b(t + \delta)P[b>t+δ, a≤t]≥(1−Fb​(t+δ))+Fa​(t)−1=Fa​(t)−Fb​(t+δ).
  • ε(δ)≥0\varepsilon(\delta) \ge 0ε(δ)≥0.
  • If ε=1\varepsilon = 1ε=1, then b−a>δb - a > \deltab−a>δ almost surely under every coupling.
  • For ε<1\varepsilon < 1ε<1: the retained sub-distributions Fa+=max⁡{Fa−ε,0}F_{a^+} = \max\{F_a - \varepsilon, 0\}Fa+​=max{Fa​−ε,0} and Fb−=min⁡{Fb,1−ε}F_{b^-} = \min\{F_b, 1 - \varepsilon\}Fb−​=min{Fb​,1−ε} are distribution functions of sub-measures of mass 1−ε1 - \varepsilon1−ε, and Fa+(t)≤Fb−(t+δ)F_{a^+}(t) \le F_{b^-}(t + \delta)Fa+​(t)≤Fb−​(t+δ).
  • Retained masses ordered in this way can be coupled with b−a≤δb - a \le \deltab−a≤δ almost surely.
  • Adding an arbitrary coupling of the remaining ε\varepsilonε-mass gives a joint law with Pr⁡(b−a>δ)≤ε\Pr(b - a > \delta) \le \varepsilonPr(b−a>δ)≤ε.

Significance

The result. The bound converts two marginal distributions, each estimable from a separate experimental arm, into a guaranteed lower bound on the share of individuals who gain more than δ\deltaδ from collaboration. Tightness shows that no other function of the marginals gives a better guarantee: any improvement needs information about the joint law. At δ=0\delta = 0δ=0 (Corollary 1, p. 18) the bound is a one-sided Kolmogorov–Smirnov distance between the two marginals, which the paper estimates from its classroom data in §6.2.

Formalizing it. The result is proved in the paper, with one gap: the degenerate case ε=1\varepsilon = 1ε=1 of the tightness proof asserts a threshold t∗t^*t∗ that need not exist (see below). The mission targets a machine-checked proof of both clauses for arbitrary laws on R\mathbb RR, atoms included. Along the way it needs two reusable pieces: the decomposition of a law on R\mathbb RR into its lower ε\varepsilonε-mass and the rest, and the monotone coupling of two finite measures ordered in the first-order stochastic sense. No machine-checked statement of the Makarov bound or of its sharpness was found on the platform or in Mathlib.

Difficulty

The lower bound is a two-line argument. The content is tightness, and three points are delicate. First, the supremum need not be attained, so the case ε=1\varepsilon = 1ε=1 cannot be handled by choosing a threshold as the printed proof does; for δ=1/2\delta = 1/2δ=1/2, a∼Uniform(−1,0)a \sim \mathrm{Uniform}(-1, 0)a∼Uniform(−1,0) and b≡1/2b \equiv 1/2b≡1/2, one has ε=1\varepsilon = 1ε=1 but no such threshold. Second, when ε<1\varepsilon < 1ε<1 the split of a law at its ε\varepsilonε-quantile must cut through atoms: a retained sub-measure is not, in general, the restriction of the law to a set. Third, the event {b−a>δ}\{b - a > \delta\}{b−a>δ} is strict and the CDFs are right-continuous, so atoms of aaa at ttt and of bbb at t+δt + \deltat+δ must be accounted for exactly; changing either convention changes the value of the bound.

Formalization scope

All objects live in the namespace HumanAIComp.Bound. Laws on R\mathbb RR are Measure ℝ with IsProbabilityMeasure; distribution functions are Mathlib's ProbabilityTheory.cdf; probabilities are Measure.real. The population is an arbitrary probability space and a,ba, ba,b are arbitrary measurable real functions: the theorem and its proof never use the form a=max⁡(yH,yAI)a = \max(y_H, y_{AI})a=max(yH​,yAI​), which is one instance. Couplings are the published MongeKantorovichYao.transferencePlans μa μb. The bound is a real supremum over t∈Rt \in \mathbb Rt∈R of a family bounded above by 111, so it is the true supremum. The hypothesis δ≥0\delta \ge 0δ≥0 of the paper is kept.

A formalization that fixed example marginals, or let the coupling's marginals vary, would make the tightness clause trivial; the goal quantifies over all pairs of probability laws on R\mathbb RR and requires a coupling with exactly those marginals. The milestones on the case ε=1\varepsilon = 1ε=1 state only the conclusion, not the printed threshold claim.

The monotone coupling theorem for probability measures is on the platform as StochasticOrders.Usual.usual_order_coupling_iff_v2 (Proved), and is included as a reference. Contributions of general lemmas about sub-measures with prescribed distribution functions, and about couplings of finite measures, are welcome.

Selected references

  • J. Baek, Y. Fu, W. Ma, T. Peng, AI Agents for Inventory Control: Human-LLM-OR Complementarity, arXiv:2602.12631v2, 2026. https://arxiv.org/abs/2602.12631
  • G. D. Makarov, Estimates for the distribution function of a sum of two random variables when the marginal distributions are fixed, Theory of Probability and its Applications 26 (1981) 803–806. https://doi.org/10.1137/1126086
  • L. Rüschendorf, Random variables with maximum sums, Advances in Applied Probability 14 (1982) 623–632. https://doi.org/10.2307/1426677
  • M. J. Frank, R. B. Nelsen, B. Schweizer, Best-possible bounds for the distribution of a sum — a problem of Kolmogorov, Probability Theory and Related Fields 74 (1987) 199–211. https://doi.org/10.1007/BF00569989
  • M. Shaked, J. G. Shanthikumar, Stochastic Orders, Springer, 2007. https://doi.org/10.1007/978-0-387-34675-5
12 thms4 active usersReviewed
🏆Completed
Convex OptimizationOperations ResearchOptimization·Captain: mikedeng1

Convexification of Permutation-Invariant Sets and an Application to Sparse Principal Component Analysis: Sparsity Theorem, the Closed-Form Minimizer of a Symmetric Gauge over Sparse Weak MajorantsResearch Paper

Motivation

Many problems in statistics and signal processing ask for a vector that is both small in some norm and sparse, with at most KKK nonzero entries. The best-known example is sparse principal component analysis (sparse PCA), whose feasible set is the set of unit vectors in the Euclidean norm with at most KKK nonzero entries (d'Aspremont et al. 2007). Cardinality constraints make such sets nonconvex, and convex relaxations of the problem need a description of their convex hull.

Kim, Tawarmalani and Richard (arXiv:1910.02573v2, Mathematics of Operations Research, 2022) describe convex hulls of sets that are invariant under permutations and sign changes of coordinates through majorization inequalities. Their §3 applies this to cardinality-constrained norm balls: for every symmetric gauge function ∥⋅∥s\|\cdot\|_s∥⋅∥s​ (a norm invariant under permutations and sign changes) it gives the convex hull of {x:∥x∥s≤1,card⁡(x)≤K}\{x : \|x\|_s \le 1, \operatorname{card}(x) \le K\}{x:∥x∥s​≤1,card(x)≤K} as the unit ball of an explicit norm, and the Sparsity Theorem gives a closed-form optimal solution of the associated majorization program. For the Euclidean norm, the norm obtained is the KKK-support norm of Argyriou, Foygel and Srebro (2012), used as a regularizer in sparse prediction.

Setting

Vectors live in Rn\mathbb R^nRn. For x∈Rnx \in \mathbb R^nx∈Rn, ∣x∣=(∣x1∣,…,∣xn∣)|x| = (|x_1|, \dots, |x_n|)∣x∣=(∣x1​∣,…,∣xn​∣), x[i]x_{[i]}x[i]​ is the iii-th largest entry of xxx, and ∣x∣[i]|x|_{[i]}∣x∣[i]​ is the iii-th largest entry of ∣x∣|x|∣x∣. card⁡(x)\operatorname{card}(x)card(x) is the number of nonzero entries.

Majorization. xxx majorizes yyy, written x≥myx \ge_m yx≥m​y, if ∑i≤jx[i]≥∑i≤jy[i]\sum_{i \le j} x_{[i]} \ge \sum_{i \le j} y_{[i]}∑i≤j​x[i]​≥∑i≤j​y[i]​ for j=1,…,n−1j = 1, \dots, n-1j=1,…,n−1, with equality of the full sums. yyy is weakly submajorized by xxx, written x≥wmyx \ge_{wm} yx≥wm​y, if the partial-sum inequalities hold for j=1,…,nj = 1, \dots, nj=1,…,n and no equality is required.

Fix a symmetric gauge function ∥⋅∥s\|\cdot\|_s∥⋅∥s​ and an integer KKK with 1<K<n1 < K < n1<K<n (for K=1K = 1K=1 the hull is an ℓ1\ell_1ℓ1​ ball, and for K=nK = nK=n the constraint is void). Set

N∥⋅∥sK={x∈Rn∣∥x∥s≤1, card⁡(x)≤K}.N^K_{\|\cdot\|_s} = \{x \in \mathbb R^n \mid \|x\|_s \le 1,\ \operatorname{card}(x) \le K\}.N∥⋅∥s​K​={x∈Rn∣∥x∥s​≤1, card(x)≤K}.

Its convex hull is a compact convex set, symmetric about 000, with 000 in its interior. Its gauge

∥x∥c=inf⁡{t>0∣x/t∈conv⁡(N∥⋅∥sK)}\|x\|_c = \inf\{t > 0 \mid x/t \in \operatorname{conv}(N^K_{\|\cdot\|_s})\}∥x∥c​=inf{t>0∣x/t∈conv(N∥⋅∥s​K​)}

is therefore a norm. For x∈Rnx \in \mathbb R^nx∈Rn and i=1,…,Ki = 1, \dots, Ki=1,…,K put

s(x)i=∑j=in∣x∣[j]K−i+1,s(x)_i = \frac{\sum_{j=i}^{n} |x|_{[j]}}{K - i + 1},s(x)i​=K−i+1∑j=in​∣x∣[j]​​,

let ixi_xix​ be the smallest index minimizing s(x)is(x)_is(x)i​ over 1≤i≤K1 \le i \le K1≤i≤K, and δ(x)=s(x)ix\delta(x) = s(x)_{i_x}δ(x)=s(x)ix​​. The vector u(x)u(x)u(x) of (15) has entries ∣x∣[i]|x|_{[i]}∣x∣[i]​ for i<ixi < i_xi<ix​, δ(x)\delta(x)δ(x) for ix≤i≤Ki_x \le i \le Kix​≤i≤K, and 000 beyond KKK.

Formalization targets

Goal: the Sparsity Theorem (Theorem 3.2, p. 9)

For every x∈Rnx \in \mathbb R^nx∈Rn, u(x)u(x)u(x) is an optimal solution of

min⁡ ∥u∥ss.t.u1≥⋯≥uK≥0,uK+1=⋯=un=0,u≥wm∣x∣,(11)\min\ \|u\|_s \quad\text{s.t.}\quad u_1 \ge \dots \ge u_K \ge 0,\quad u_{K+1} = \dots = u_n = 0,\quad u \ge_{wm} |x|, \tag{11}min ∥u∥s​s.t.u1​≥⋯≥uK​≥0,uK+1​=⋯=un​=0,u≥wm​∣x∣,(11)

and, as the paper reads the theorem on p. 6,

x∈conv⁡(N∥⋅∥sK)  ⟺  ∥u(x)∥s≤1.x \in \operatorname{conv}\big(N^K_{\|\cdot\|_s}\big) \iff \|u(x)\|_s \le 1.x∈conv(N∥⋅∥s​K​)⟺∥u(x)∥s​≤1.

Milestones

In attack order:

  • Lemma 2.1: a linear map that maps SSS into itself maps conv⁡(S)\operatorname{conv}(S)conv(S) into itself.
  • Lemma 2.2: x≥myx \ge_m yx≥m​y iff yyy is a convex combination of permutations of xxx. This is already proved on the platform.
  • Lemma 3.1: permutation-invariant norms are monotone under ≥m\ge_m≥m​.
  • Proposition 3.1: conv⁡(NK)\operatorname{conv}(N^K)conv(NK) is a convex body.
  • Proposition 3.2: conv⁡(NK)\operatorname{conv}(N^K)conv(NK) is the unit ball of the sign- and permutation-invariant norm ∥⋅∥c\|\cdot\|_c∥⋅∥c​.
  • Proposition 3.3: ∥x∥c=∥x∥s\|x\|_c = \|x\|_s∥x∥c​=∥x∥s​ when card⁡(x)≤K\operatorname{card}(x) \le Kcard(x)≤K.
  • Proposition 3.4: the recursion and unimodality of s(x)s(x)s(x), u(x)≥m∣x∣u(x) \ge_m |x|u(x)≥m​∣x∣, and u(x)1=max⁡{∣x∣[1],s(x)1}u(x)_1 = \max\{|x|_{[1]}, s(x)_1\}u(x)1​=max{∣x∣[1]​,s(x)1​}.
  • Theorem 3.1: ∥x∥c=∥u(x)∥s\|x\|_c = \|u(x)\|_s∥x∥c​=∥u(x)∥s​.
  • The weak-majorization fact 5.A.9 of Marshall–Olkin–Arnold, which the proof of Theorem 3.2 cites: u≥wmyu \ge_{wm} yu≥wm​y implies that some u′u'u′ satisfies u≥mu′u \ge_m u'u≥m​u′ and u′≥yu' \ge yu′≥y.

Significance

The result. The theorem reduces membership in the convex hull of a cardinality-constrained norm ball to one sort of ∣x∣|x|∣x∣, a scan over KKK averages and one evaluation of ∥⋅∥s\|\cdot\|_s∥⋅∥s​. It also gives an explicit extended formulation and a separating hyperplane (Corollary 3.1). The paper uses these to build relaxations for sparse PCA whose valid inequalities rest on this hull description. Specialized to ℓ2\ell_2ℓ2​ it recovers the closed form of the KKK-support norm, and specialized to ℓ∞\ell_\inftyℓ∞​ the norm of Proposition 3.5. The result holds for every symmetric gauge, so it covers all ℓp\ell_pℓp​ norms at once.

Formalizing it. The result is proved in the paper; none of it is machine-checked. The mission would supply a formal theory of majorization and weak majorization through sums of largest entries, Schur-convexity of symmetric norms, and the gauge of a convex hull of a symmetric nonconvex set. The platform already has Lemma 2.2 (the Hardy–Littlewood–Pólya/Birkhoff characterization) as a proved theorem, and the mission builds on it.

Difficulty

The inequality ∥x∥c≤∥u(x)∥s\|x\|_c \le \|u(x)\|_s∥x∥c​≤∥u(x)∥s​ follows from u(x)≥m∣x∣u(x) \ge_m |x|u(x)≥m​∣x∣ and the monotonicity of symmetric norms under majorization. The reverse inequality ∥x∥c≥∥u(x)∥s\|x\|_c \ge \|u(x)\|_s∥x∥c​≥∥u(x)∥s​ is the hard part. An upper bound on a gauge needs a single convex combination, but a lower bound needs a linear inequality that holds on the whole nonconvex set N∥⋅∥sKN^K_{\|\cdot\|_s}N∥⋅∥s​K​, for an arbitrary symmetric gauge whose dual norm is not known in closed form. Bounding by ∥x∥s\|x\|_s∥x∥s​ itself does not work: the two norms agree only on KKK-sparse vectors. The particular index ixi_xix​, the first minimizer of s(x)s(x)s(x), is what makes the closed form exact, and replacing it by any other index breaks the identity. The paper treats sorted order statistics as notation; a formal proof has to carry them explicitly.

Formalization scope

Vectors are Fin n → ℝ, and Lean index iii is the paper's i+1i+1i+1. A norm ∥⋅∥s\|\cdot\|_s∥⋅∥s​ is a plain function (Fin n → ℝ) → ℝ that satisfies the axioms in the structures IsPermInvNorm (definite, subadditive, absolutely homogeneous, permutation-invariant) and IsSymmetricGauge (also sign-invariant). Lean's built-in norm on Fin n → ℝ is the sup norm, so stating the theorems for it would prove only the ℓ∞\ell_\inftyℓ∞​ case; every statement here instead quantifies over all symmetric gauges. The standing assumption 1<K<n1 < K < n1<K<n (p. 6) is a hypothesis of every §3 item.

Sums of the jjj largest entries are the published ModernConvex.Spectral.sumLargest (from ModernConvex_Spectral_SDR), used only for 1≤j≤n1 \le j \le n1≤j≤n. With it, ≥m\ge_m≥m​ is the right-hand side of the published majorization_principle. Weak majorization runs over j=1,…,nj = 1, \dots, nj=1,…,n. ∣x∣[⋅]|x|_{[\cdot]}∣x∣[⋅]​ is built from Mathlib's Tuple.sort. s(x)s(x)s(x) and ixi_xix​ keep the paper's 1-based indices and are used only on 1,…,K1, \dots, K1,…,K. The convention s(x)0=s(x)K+1=∞s(x)_0 = s(x)_{K+1} = \inftys(x)0​=s(x)K+1​=∞ only excludes those indices from the minimization. The norm ∥⋅∥c\|\cdot\|_c∥⋅∥c​ is Mathlib's gauge of convexHull ℝ (NK ns K): (14) writes a minimum, which is an infimum at x=0x = 0x=0. A convex body is a compact convex set with nonempty interior.

In the goal, the minimizer is the specific closed-form u(x)u(x)u(x), and minimality is over every feasible point of (11). The equivalence in part 2 is with membership in the actual convex hull, not with a set chosen to make it true. Contributions are welcome at every milestone; Lemma 3.1, 5.A.9 and Propositions 3.1–3.2 are reusable beyond this mission.

Selected references

  • J. Kim, M. Tawarmalani, J.-P. P. Richard, Convexification of Permutation-Invariant Sets and an Application to Sparse Principal Component Analysis, Mathematics of Operations Research, 2022; arXiv:1910.02573v2. https://arxiv.org/abs/1910.02573v2
  • A. W. Marshall, I. Olkin, B. C. Arnold, Inequalities: Theory of Majorization and Its Applications, 2nd ed., Springer, 2011. https://doi.org/10.1007/978-0-387-68276-1
  • A. Argyriou, R. Foygel, N. Srebro, Sparse Prediction with the k-Support Norm, NeurIPS 2012. https://arxiv.org/abs/1204.5043
  • A. d'Aspremont, L. El Ghaoui, M. I. Jordan, G. R. G. Lanckriet, A Direct Formulation for Sparse PCA Using Semidefinite Programming, SIAM Review 49(3), 2007. https://doi.org/10.1137/050645506
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Bandit AlgorithmsInformation TheoryMachine Learning+1·Captain: mikedeng1

Phase Transitions in Bandits with Switching Constraints: every policy with at most S switches has regret at least the phase-dependent rate up to a logarithmic factorResearch Paper

Motivation

In many sequential decision problems, changing the action is costly or administratively limited: a retailer can revise a posted price only a few times per season, a clinical trial can change its treatment allocation only a few times, and a firm can reconfigure its production line only so often. The multi-armed bandit with switching constraints (BwSC) captures this tension between learning and limited adaptivity: the learner must explore to find a good action, but every change of action consumes a hard budget. Simchi-Levi and Xu (arXiv:1905.10825, Management Science 2023) determine the optimal regret of this problem up to logarithmic factors.

Timeline. Classical bandit theory gives the minimax regret Θ(KT)\Theta(\sqrt{KT})Θ(KT​) for KKK arms and horizon TTT with unlimited switching (Auer, Cesa-Bianchi, Freund and Schapire, 2002; Lattimore and Szepesvári, Bandit Algorithms, 2020). Cesa-Bianchi, Dekel and Shamir (2013) showed that in adversarial bandits with switching costs the regret is Θ~(T2/3)\widetilde\Theta(T^{2/3})Θ(T2/3). For stochastic bandits processed in a fixed number of batches, Perchet, Rigollet, Chassang and Snowberg (2016) and Gao, Han, Ren and Zhou (2019) obtained regret rates of the form T1/(2−21−M)T^{1/(2-2^{1-M})}T1/(2−21−M) for MMM batches. Simchi-Levi and Xu (2019, revised 2021) treat a hard budget SSS on the number of switches and prove matching upper and lower bounds; the lower bound, Theorem 2, is the subject of this mission.

Setting

There are K>1K>1K>1 arms and TTT rounds. In round ttt the learner picks at∈[K]a_t\in[K]at​∈[K] and observes a reward Xt∼N(μat,1)X_t\sim\mathcal N(\mu_{a_t},1)Xt​∼N(μat​​,1) from the unit-variance Gaussian environment with mean vector μ∈RK\mu\in\mathbb R^Kμ∈RK; admissible environments have mean spread ∣μi−μj∣≤1|\mu_i-\mu_j|\le1∣μi​−μj​∣≤1. A policy π\piπ chooses at+1a_{t+1}at+1​ by a Markov kernel from the past actions and rewards; Pμπ\mathbb P^\pi_\muPμπ​ is the law of the history. The regret is

Rμπ(T)=Tmax⁡iμi−Eμπ[∑t=1TXt].R^\pi_\mu(T)=T\max_i\mu_i-\mathbb E^\pi_\mu\Big[\sum_{t=1}^T X_t\Big].Rμπ​(T)=Timax​μi​−Eμπ​[t=1∑T​Xt​].

With unit switching costs, the number of switches is ∑t=1T−11{at≠at+1}\sum_{t=1}^{T-1}\mathbb 1\{a_t\neq a_{t+1}\}∑t=1T−1​1{at​=at+1​}. For a budget S∈NS\in\mathbb NS∈N, the class ΠS\Pi_SΠS​ of SSS-switch policies consists of the policies whose number of switches is at most SSS almost surely under every environment.

The budget enters through the phase index q(S,K)=⌊(S−1)/(K−1)⌋q(S,K)=\lfloor (S-1)/(K-1)\rfloorq(S,K)=⌊(S−1)/(K−1)⌋ (with q(0,K)=0q(0,K)=0q(0,K)=0) and the remainder r(S,K)=S−1−q(S,K)(K−1)r(S,K)=S-1-q(S,K)(K-1)r(S,K)=S−1−q(S,K)(K−1) (so r(0,K)=−1r(0,K)=-1r(0,K)=−1). Two rates appear, with a(q)=1/(2−2−q)a(q)=1/(2-2^{-q})a(q)=1/(2−2−q):

A=(K−r(S,K))2−a(q(S,K))K Ta(q(S,K)),B=K1−a(q(S,K)+1) Ta(q(S,K)+1).A=\frac{(K-r(S,K))^{2-a(q(S,K))}}{K}\,T^{a(q(S,K))},\qquad B=K^{1-a(q(S,K)+1)}\,T^{a(q(S,K)+1)}.A=K(K−r(S,K))2−a(q(S,K))​Ta(q(S,K)),B=K1−a(q(S,K)+1)Ta(q(S,K)+1).

In Lean these are IsSwitchPolicy S T π, qIdx S K, rIdx S K, rateA K S T, rateB K S T, on top of the published BanditPolicy, banditMeasure, banditRegret and gaussianBandit.

Formalization targets

Goal: Theorem 2 (p. 21)

There is an absolute constant C>0C>0C>0 such that for all K>1K>1K>1, S∈NS\in\mathbb NS∈N, T≥2KT\ge2KT≥2K and every π∈ΠS\pi\in\Pi_Sπ∈ΠS​, some admissible Gaussian environment μ\muμ satisfies

Rμπ(T) ≥ Clog⁡Tmax⁡{A, B}.R^\pi_\mu(T)\ \ge\ \frac{C}{\log T}\max\{A,\ B\}.Rμπ​(T) ≥ logTC​max{A, B}.

The constant is not fixed: the goal asserts the shape of the bound, which survives any improvement of constants.

Milestones

The proof in Appendix J (pp. 59–75) reduces to the regime q(S,K)+2≤log⁡2log⁡2(T/K)q(S,K)+2\le\log_2\log_2(T/K)q(S,K)+2≤log2​log2​(T/K) (p. 59, two bounds by O(KT)O(\sqrt{KT})O(KT​) outside it) and then runs a five-step program on two families of environments:

  1. the localized Pinsker inequality (Lemma 5) and the generalized reverse Fano inequality (Proposition 5, (35));
  2. counting bounds on risky events under a single environment (Lemmas 6–7, Corollary 4);
  3. bad-event regret bounds under alternative environments and the reduction to bad-event probabilities (Lemmas 8–11);
  4. divergence bounds for restricted measures (property 1 of p. 72, Lemmas 12–13);
  5. the final probability bounds (46)–(47).

Significance

The result. Theorem 2, together with the AdaLS upper bound (Theorem 1), shows that the optimal regret is Θ~(max⁡{A,B})\widetilde\Theta(\max\{A,B\})Θ(max{A,B}) for every KKK, SSS and TTT. In particular, for fixed KKK the regret as a function of TTT is Θ~(T1/(2−2−q(S,K)))\widetilde\Theta(T^{1/(2-2^{-q(S,K)})})Θ(T1/(2−2−q(S,K))): it changes only when SSS crosses a multiple of K−1K-1K−1, a phase transition in the switching budget, and Θ(log⁡log⁡T)\Theta(\log\log T)Θ(loglogT) switches suffice for the classical T\sqrt TT​ rate. The lower bound holds for all randomized adaptive policies, not only batched ones.

Formalizing it. The result is proved on paper but has no machine-checked proof. Formalizing the lower bound adds a reusable change-of-measure toolkit for adaptively collected data: a reverse Fano-type inequality over families of measure spaces, stopping-time-based counting arguments on switching patterns, and divergence bounds for censored histories. Three printed steps needed repair (see Formalization scope), so the formal development also certifies a corrected version of the argument.

Difficulty

The obvious argument fails at the counting step. A naive choice of risky events (arms unobserved in fixed time windows) only gives a sum of probabilities of at least K−1−⌊S/(q+1)⌋K-1-\lfloor S/(q+1)\rfloorK−1−⌊S/(q+1)⌋, which vanishes when SSS is at the end of a phase; this loses the floor ⌊(S−1)/(K−1)⌋\lfloor (S-1)/(K-1)\rfloor⌊(S−1)/(K−1)⌋ in the exponent. The paper's events in the last window are defined through the stopping time at which the switching budget is exhausted, and they interact with the measure-change step: the restricted measures must hide enough information about the tested arm to make divergences small, while still deciding the stopping-time event. A second difficulty is that the policy is adaptive and randomized, so all events and measures are path-dependent.

Formalization scope

  • Model. Histories are the published canonical bandit histories Fin T → Fin K × ℝ; rounds are 1-based in every statement (entry sss is round s+1s+1s+1). Environments are unit-variance Gaussian (gaussianBandit), which is all the proof uses (p. 59).
  • Admissible policies. IsSwitchPolicy S T π asks the budget to hold almost surely under every unit-variance Gaussian environment, a weaker requirement than the paper's "for all sub-Gaussian D\mathcal DD", so the goal covers at least the paper's policy class. The regret lower bound is witnessed by one Gaussian instance with mean spread at most 111, which implies the paper's bound on the supremum.
  • Conventions. S∈NS\in\mathbb NS∈N and unit costs (§3, p. 14); q(0,K)=0q(0,K)=0q(0,K)=0 and r(0,K)=−1r(0,K)=-1r(0,K)=−1 by the paper's convention ⌊x⌋=0\lfloor x\rfloor=0⌊x⌋=0 for x<0x<0x<0; τ=∞\tau=\inftyτ=∞ is encoded as T+1T+1T+1; divergences are Mathlib's klDiv in [0,∞][0,\infty][0,∞], and the reverse KL is Dre(P∥Q)=KL(Q∥P)D_{\rm re}(\mathbb P\|\mathbb Q)=\mathrm{KL}(\mathbb Q\|\mathbb P)Dre​(P∥Q)=KL(Q∥P); conditional expectations in Lemmas 8 and 10 are stated in product form.
  • Repairs. (i) Lemma 8's integrand is the regret Tμ∗−∑tμatT\mu^*-\sum_t\mu_{a_t}Tμ∗−∑t​μat​​; the printed integrand is non-positive for j=q+2j=q+2j=q+2. (ii) The artificial measures (45) are replaced by records stopped at the first pull of the tested arm in the window; the printed measures do not have the claimed divergence. (iii) The p. 59 bound 2KT\sqrt{2KT}2KT​ is corrected to 2KT2\sqrt{KT}2KT​, and the companion bound for the first term, which the page omits, is a separate milestone. The first-class lemmas assume q(S,K)≥1q(S,K)\ge1q(S,K)≥1, where the page's construction is defined; the goal does not.
  • Ruled out. A constant CCC depending on KKK, SSS or TTT; dropping the mean-spread condition; restricting to deterministic or batched policies; a switching constraint only in expectation; or stating the theorem for one fixed (K,S)(K,S)(K,S) — each makes the statement trivial or different, and none is used.
  • Infrastructure. Reused: the published canonical bandit model, the Bernoulli divergence ExploreFirst.FundIneq.klBer, the first half of Lemma 5 (ExploreFirst.Collective.lemma_6) and the classical bound BanditAlgorithm.bandit_minimax_lower_bound. Needed and reusable beyond this mission: the divergence decomposition for stopped histories, joint convexity and data processing for KL across different spaces, and the KL divergence of unit-variance Gaussians. Proofs of any milestone, and of the Gaussian-instance reduction, are welcome.

Selected references

  • D. Simchi-Levi and Y. Xu, Phase Transitions in Bandits with Switching Constraints, Management Science, 2023; arXiv:1905.10825v4. https://arxiv.org/abs/1905.10825
  • T. Lattimore and C. Szepesvári, Bandit Algorithms, Cambridge University Press, 2020. https://doi.org/10.1017/9781108571401
  • N. Cesa-Bianchi, O. Dekel and O. Shamir, Online Learning with Switching Costs and Other Adaptive Adversaries, NeurIPS 2013. https://arxiv.org/abs/1302.4387
  • V. Perchet, P. Rigollet, S. Chassang and E. Snowberg, Batched Bandit Problems, Annals of Statistics, 2016. https://arxiv.org/abs/1505.00369
  • Z. Gao, Y. Han, Z. Ren and Z. Zhou, Batched Multi-armed Bandits Problem, NeurIPS 2019. https://arxiv.org/abs/1904.01763
  • S. Gerchinovitz, P. Ménard and G. Stoltz, Fano's Inequality for Random Variables, Statistical Science, 2020. https://arxiv.org/abs/1702.05985
26 thms4 active usersReviewed
🏆Completed
Quantum Information·Captain: Goku

Coding Theorems of Quantum Information TheoryResearch Paper

Motivation

Coding theorems and (strong) converses for memoryless quantum communication channels and quantum sources are proved: for the quantum source the coding theorem is reviewed, and the strong converse proven. For classical information transmission via quantum channels we give a new proof of the coding theorem, and prove the strong converse, even under the extended model of nonstationary channels. As a by-product we obtain a new proof of the famous Holevo bound. Then multi-user systems are investigated, and the capacity region for the quantum multiple access channel is determined. The last chapter contains a preliminary discussion of some models of compression of correlated quantum sources, and a proposal for a program to obtain operational meaning for quantum conditional entropy. An appendix features the introduction of a notation and calculus of entropy in quantum systems.

This mission is the statement-level formalization of Coding Theorems of Quantum Information Theory (arXiv:quant-ph/9907077v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

76 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Theorem I.1: Dbar²≤1−Fbar≤Dbar; for quantum encoders also 1−Fbar≤1−Fe. (Theorem I.1, PDF p. 8). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

9 results of the paper are not stated yet, because the library lacks an interface they need:

  • I.3-subnormalized: A valid complete statement of I.3-subnormalized under its printed hypotheses (source-ambiguity)
  • Lemma II.8: A valid complete statement of Lemma II.8 under its printed hypotheses (source-ambiguity)
  • Lemma II.12: A valid complete statement of Lemma II.12 under its printed hypotheses (source-ambiguity)
  • Lemma II.15: A valid complete statement of Lemma II.15 under its printed hypotheses (source-ambiguity)
  • Remark II.22: A valid complete statement of Remark II.22 under its printed hypotheses (source-ambiguity)
  • Lemma II.24: A valid complete statement of Lemma II.24 under its printed hypotheses (source-ambiguity)
  • Theorem IV.14: A valid complete statement of Theorem IV.14 under its printed hypotheses (source-ambiguity)
  • Theorem A.3: A valid complete statement of Theorem A.3 under its printed hypotheses (source-ambiguity)
  • Corollary A.25: A valid complete statement of Corollary A.25 under its printed hypotheses (source-ambiguity)

Selected references

  • Coding Theorems of Quantum Information Theory, arXiv:quant-ph/9907077v1, https://arxiv.org/abs/quant-ph/9907077v1
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🏆Completed
Machine LearningOperations ResearchOptimization·Captain: mikedeng1

Efficient Online Linear Optimization with Approximation Algorithms: Online Gradient Descent with Infeasible Projections onto CH(αK) Has Expected α-Regret at Most α²R²/(Tη) + ηF²/2 + 3FεResearch Paper

Online learning with an approximation algorithm

Many sequential decision problems have a combinatorial action set: each round a decision maker picks a route, a schedule or a cut, and only afterwards learns its cost. When the offline problem — minimize a known linear cost over the action set — is NP-hard, the best available tool is an approximation algorithm, which returns a feasible action whose cost is within a factor α\alphaα of optimal. The natural benchmark online is then the α\alphaα-regret: the learner's average cost minus α\alphaα times the average cost of the best fixed action in hindsight.

Kakade, Kalai and Ligett (SIAM J. Comput. 2009) showed that any α\alphaα-approximation oracle can be converted into an online algorithm with vanishing α\alphaα-regret, but their conversion may call the oracle O(T)O(T)O(T) times per round. Garber (arXiv:1709.03093, Mathematics of Operations Research 2021) gave the first conversion whose expected α\alphaα-regret is O(T−1/3)O(T^{-1/3})O(T−1/3) while the number of oracle calls per round is polylogarithmic in TTT, in both the full-information and the bandit settings. This mission formalizes the full-information regret bound, Theorem 1 of that paper.

Setting

Vectors live in Rd\mathbb R^dRd with the Euclidean norm ∥⋅∥\|\cdot\|∥⋅∥ and dot product x⋅fx\cdot fx⋅f; R+d\mathbb R^d_+R+d​ is the non-negative orthant. An instance consists of compact sets K,F⊂R+d\mathcal K,\mathcal F\subset\mathbb R^d_+K,F⊂R+d​, with K\mathcal KK nonempty, and constants R,F,C>0R,F,C>0R,F,C>0 such that ∥x∥≤R\|x\|\le R∥x∥≤R on K\mathcal KK, ∥f∥≤F\|f\|\le F∥f∥≤F on F\mathcal FF, and 0≤x⋅f≤C0\le x\cdot f\le C0≤x⋅f≤C for x∈Kx\in\mathcal Kx∈K, f∈Ff\in\mathcal Ff∈F. Here K\mathcal KK is the set of actions and F\mathcal FF the set of loss (or payoff) vectors.

An α\alphaα-approximation oracle (α>0\alpha>0α>0) is a map OK\mathcal O_{\mathcal K}OK​ that, for every c∈R+dc\in\mathbb R^d_+c∈R+d​, returns OK(c)∈K\mathcal O_{\mathcal K}(c)\in\mathcal KOK​(c)∈K with OK(c)⋅c≤αmin⁡x∈Kx⋅c\mathcal O_{\mathcal K}(c)\cdot c\le\alpha\min_{x\in\mathcal K}x\cdot cOK​(c)⋅c≤αminx∈K​x⋅c when α≥1\alpha\ge1α≥1 (loss minimization), or OK(c)⋅c≥αmax⁡x∈Kx⋅c\mathcal O_{\mathcal K}(c)\cdot c\ge\alpha\max_{x\in\mathcal K}x\cdot cOK​(c)⋅c≥αmaxx∈K​x⋅c when α<1\alpha<1α<1 (payoff maximization).

Over TTT rounds an oblivious adversary fixes f1,…,fT∈Ff_1,\dots,f_T\in\mathcal Ff1​,…,fT​∈F in advance, and the learner plays x1,…,xT∈Kx_1,\dots,x_T\in\mathcal Kx1​,…,xT​∈K. The α\alphaα-regret is

1T∑t=1Txt⋅ft−αmin⁡x∈K1T∑t=1Tx⋅ft(α≥1),αmax⁡x∈K1T∑t=1Tx⋅ft−1T∑t=1Txt⋅ft(α<1).\frac1T\sum_{t=1}^Tx_t\cdot f_t-\alpha\min_{x\in\mathcal K}\frac1T\sum_{t=1}^Tx\cdot f_t\quad(\alpha\ge1),\qquad \alpha\max_{x\in\mathcal K}\frac1T\sum_{t=1}^Tx\cdot f_t-\frac1T\sum_{t=1}^Tx_t\cdot f_t\quad(\alpha<1).T1​t=1∑T​xt​⋅ft​−αx∈Kmin​T1​t=1∑T​x⋅ft​(α≥1),αx∈Kmax​T1​t=1∑T​x⋅ft​−T1​t=1∑T​xt​⋅ft​(α<1).

The algorithm (Algorithm 3) is online gradient descent over CH(αK)\mathrm{CH}(\alpha\mathcal K)CH(αK), the convex hull of αK={αx:x∈K}\alpha\mathcal K=\{\alpha x:x\in\mathcal K\}αK={αx:x∈K}, with exact projections replaced by infeasible projections: a point y~\tilde yy~​ with ∥y~−z∥2≤∥y−z∥2\|\tilde y-z\|^2\le\|y-z\|^2∥y~​−z∥2≤∥y−z∥2 for all z∈CH(αK)z\in\mathrm{CH}(\alpha\mathcal K)z∈CH(αK). They are computed by Algorithm 2, which repeatedly runs an Ellipsoid-method separation-or-decomposition procedure (Lemma 5) driven by an extended oracle O^K\hat{\mathcal O}_{\mathcal K}O^K​ (Lemma 1) that accepts every direction in Rd\mathbb R^dRd. When no separating direction is found, the procedure returns a probability vector (a1,…,aN)(a_1,\dots,a_N)(a1​,…,aN​) over feasible points s1,…,sN∈Ks_1,\dots,s_N\in\mathcal Ks1​,…,sN​∈K, and the learner samples its next action from it.

Formalization targets

Goal: Theorem 1 (regret bound)

For η>0\eta>0η>0, ε∈(0,(α+2)R]\varepsilon\in(0,(\alpha+2)R]ε∈(0,(α+2)R] and T≥1T\ge1T≥1, the points s1,…,sTs_1,\dots,s_Ts1​,…,sT​ played by Algorithm 3 satisfy

E[α-regret({(st,ft)}t∈[T])]≤α2R2Tη+ηF22+3Fε.\mathbb E\big[\alpha\text{-regret}(\{(s_t,f_t)\}_{t\in[T]})\big]\le\frac{\alpha^2R^2}{T\eta}+\frac{\eta F^2}{2}+3F\varepsilon .E[α-regret({(st​,ft​)}t∈[T]​)]≤Tηα2R2​+2ηF2​+3Fε.

The statement covers both α≥1\alpha\ge1α≥1 and α<1\alpha<1α<1 and every dimension d≥2d\ge2d≥2.

Milestones

  1. Lemma 1 (p. 6): the extended oracle O^K(c)=(v,s)\hat{\mathcal O}_{\mathcal K}(c)=(v,s)O^K​(c)=(v,s) satisfies v⋅c≤min⁡x∈αKx⋅cv\cdot c\le\min_{x\in\alpha\mathcal K}x\cdot cv⋅c≤minx∈αK​x⋅c, sss dominates vvv on F\mathcal FF, and ∥v∥≤(α+2)R\|v\|\le(\alpha+2)R∥v∥≤(α+2)R.
  2. Lemma 2 (p. 7): online gradient descent with infeasible projections keeps the regret bound 12Tη∥x1−x∥2+η2T∑t∥ft∥2\frac1{2T\eta}\|x_1-x\|^2+\frac\eta{2T}\sum_t\|f_t\|^22Tη1​∥x1​−x∥2+2Tη​∑t​∥ft​∥2 against every xxx in the feasible set.
  3. Lemma 6 (p. 11): if min⁡i(x−vi)⋅w≤ε\min_i(x-v_i)\cdot w\le\varepsilonmini​(x−vi​)⋅w≤ε for every unit vector www, the minimum-norm convex combination ppp of the viv_ivi​ satisfies ∥p−x∥≤ε\|p-x\|\le\varepsilon∥p−x∥≤ε.
  4. Lemma 5 (pp. 9–10): with N≥c d2ln⁡(α+1)R+∥x∥εN\ge c\,d^2\ln\frac{(\alpha+1)R+\|x\|}{\varepsilon}N≥cd2lnε(α+1)R+∥x∥​ Ellipsoid iterations, the procedure either finds www with (x−z)⋅w≥ε(x-z)\cdot w\ge\varepsilon(x−z)⋅w≥ε on αK\alpha\mathcal KαK and ∥w∥≤1\|w\|\le1∥w∥≤1, or a convex combination ppp of oracle outputs with ∥x−p∥≤3ε\|x-p\|\le3\varepsilon∥x−p∥≤3ε.
  5. Lemma 7 (p. 12): Algorithm 2 terminates and returns an infeasible projection y~\tilde yy~​ of its input onto CH(αK)\mathrm{CH}(\alpha\mathcal K)CH(αK) with ∥p−y~∥≤3ε\|p-\tilde y\|\le3\varepsilon∥p−y~​∥≤3ε.

Significance

Theorem 1 shows that low α\alphaα-regret needs nothing beyond black-box access to an offline approximation algorithm, with an oracle cost per round that grows only logarithmically in the accuracy. It applies to any combinatorial problem with a linear objective and a known approximation algorithm, and it is the base of the paper's bandit result (Theorem 2), whose analysis reuses the same infeasible-projection argument.

The result is proved in the paper; none of it has been machine-checked. The mission adds a formal account of the model and the algorithms, including the conventions the paper leaves implicit (which Ellipsoid method, what the expectation ranges over). It also records two printed claims that are not stated here because they are incorrect as written: Lemma 7's iteration count ⌈α2R2/ε2⌉\lceil\alpha^2R^2/\varepsilon^2\rceil⌈α2R2/ε2⌉, replaced by termination, and the bound 2α2R22\alpha^2R^22α2R2 in Lemma 7's "Moreover" clause. A formal proof would confirm the regret bound independently of these slips.

Difficulty

The obvious approach, online gradient descent over CH(αK)\mathrm{CH}(\alpha\mathcal K)CH(αK), needs Euclidean projections onto a set that can only be accessed by approximate linear optimization over K\mathcal KK, and only for directions in R+d\mathbb R^d_+R+d​. Such an oracle cannot certify membership in CH(αK)\mathrm{CH}(\alpha\mathcal K)CH(αK) and cannot optimize over it exactly, so exact projection is out of reach. Simulating the projection by an Ellipsoid run on CH(αK)\mathrm{CH}(\alpha\mathcal K)CH(αK) itself also fails: the oracle answers only non-negative directions, and its answers are off by the factor α\alphaα. The regret analysis must therefore survive projections that are infeasible, decompositions that are only approximately correct, and points that are not even in K\mathcal KK.

For a formal proof the hardest part is Lemma 5. It is an Ellipsoid-method volume argument whose cut rule queries the oracle at every iterate, whose iteration constant is universal, and whose logarithm can be negative.

Formalization scope

All work is in the namespace ApproxOLO.FullInfo, in one definitions module. Vectors are Fin d → ℝ, and every norm is the Euclidean euclNorm x = √(x·x); Mathlib's ‖·‖ on this type (the sup norm) is not used anywhere. The two regimes α≥1\alpha\ge1α≥1 and α<1\alpha<1α<1 are kept everywhere, in the oracle, the regret, the extended oracle and the update yt+1=y~t∓ηfty_{t+1}=\tilde y_t\mp\eta f_tyt+1​=y~​t​∓ηft​. The oracle guarantee is stated for every x∈Kx\in\mathcal Kx∈K, which is equivalent to the min/max form. In the regret, the min and max are sInf/sSup of the image of the compact nonempty K\mathcal KK.

The Ellipsoid method, which the paper does not specify, is fixed as follows: it starts at the unit ball, and its update is the standard central cut from the published LinearOptimization_EllipsoidMethod module, with cut vectors x−vx-vx−v and −w-w−w in that module's sign convention. That update has the factor d2/(d2−1)d^2/(d^2-1)d2/(d2−1), so Lemma 5, Lemma 7 and Theorem 1 assume d≥2d\ge2d≥2. T≥1T\ge1T≥1 is assumed wherever the factor 1/T1/T1/T appears. The universal constant ccc of Lemma 5 is quantified once, before the dimension and the instance. Each call of the procedure uses a positive integer number of iterations NNN satisfying that lower bound, and the number may differ from call to call.

Algorithms 2 and 3 are run predicates. The choices the paper leaves open (s1s_1s1​, the iteration budgets, the optimal solution of Problem (5)) are quantified universally. The expected α\alphaα-regret is Eq. (1) evaluated at the per-round expected losses ∑iai si⋅ft\sum_ia_i\,s_i\cdot f_t∑i​ai​si​⋅ft​. This equals the expectation by linearity, because the iterates never depend on the samples and the adversary is oblivious.

A statement with N=0N=0N=0 allowed, an infeasible oracle hypothesis, a fixed α≥1\alpha\ge1α≥1, or a sup-norm in place of the Euclidean norm would be a different and partly trivial theorem; the statements exclude each of these. The sanity file exhibits an instance, an oracle and a one-round run satisfying all hypotheses.

Not formalized: the oracle-complexity bound K(η,ε)K(\eta,\varepsilon)K(η,ε) and the "In particular" rates of Theorem 1 (big-OOO statements with hidden constants), Lemma 7's iteration count and "Moreover" clause, the bandit setting (Definition 1, Algorithm 4, Theorem 2), and the comparison scheme of Lemmas 3–4. Reusable beyond this mission: the extended oracle, infeasible projections and Lemma 2, Lemma 6 on minimum-norm points of convex hulls, and the separation-or-decomposition procedure. Proofs of any milestone are welcome, as is a formal version of the oracle-complexity bound with explicit constants.

Selected references

  • D. Garber, Efficient Online Linear Optimization with Approximation Algorithms, Mathematics of Operations Research 46(1), 2021; preprint arXiv:1709.03093v1, 2017. https://arxiv.org/abs/1709.03093
  • S. M. Kakade, A. T. Kalai, K. Ligett, Playing Games with Approximation Algorithms, SIAM Journal on Computing 39(3), 2009. https://doi.org/10.1137/070701704
  • M. Zinkevich, Online Convex Programming and Generalized Infinitesimal Gradient Ascent, Proceedings of ICML, 2003 (the origin of online gradient descent, reference [17] of the paper).
  • D. Bertsimas, J. N. Tsitsiklis, Introduction to Linear Optimization, Athena Scientific, 1997, Chapter 8 (the Ellipsoid method).
  • M. Grötschel, L. Lovász, A. Schrijver, Geometric Algorithms and Combinatorial Optimization, Springer, 1988. https://doi.org/10.1007/978-3-642-97881-4
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Information TheoryQuantum Information·Captain: mikedeng1

An Intuitive Proof of the Data Processing Inequality: Conditional von Neumann Entropy Cannot Increase Under Partial Trace, via the Smooth Min-Entropy DPI and the Quantum AEPResearch Paper

Motivation

The data processing inequality (DPI) for the conditional von Neumann entropy says that discarding part of the side information cannot make a quantum system less uncertain: for every tripartite state ρABC\rho_{ABC}ρABC​,

H(A∣BC)ρ≤H(A∣B)ρ.H(A|BC)_\rho \le H(A|B)_\rho .H(A∣BC)ρ​≤H(A∣B)ρ​.

It is equivalent to strong subadditivity of the von Neumann entropy, proved by Lieb and Ruskai in 1973 (Lieb–Ruskai), and it underlies most of quantum Shannon theory: the converse bounds of channel coding, the monotonicity of mutual information under local operations, and the security analysis of quantum key distribution all reduce to it. The known proofs rest on operator convexity (Lieb's concavity theorem) or on other non-elementary matrix analysis.

Beaudry and Renner (arXiv:1107.0740v2, Quantum Inf. Comput. 12 (2012) 432) give a proof that avoids operator convexity entirely. It first proves the DPI for a one-shot quantity, the smooth min-entropy, where it follows almost directly from the definition, and then recovers the von Neumann statement through the quantum asymptotic equipartition property (QAEP) of Tomamichel, Colbeck and Renner (arXiv:0811.1221), for which the paper supplies a short self-contained proof.

Timeline. 1973: Lieb–Ruskai prove strong subadditivity. 2009: Tomamichel–Colbeck–Renner prove the QAEP with explicit convergence rates. 2010: Tomamichel–Colbeck–Renner establish the duality and data processing of smooth entropies (arXiv:0907.5238). 2011–2012: Beaudry–Renner assemble these into the route formalized here.

Setting

All Hilbert spaces are finite-dimensional, and all logarithms are base 2. A density matrix is a positive semidefinite matrix of trace one; S=(H)S_=(\mathcal H)S=​(H) is their set and S≤(H)S_\le(\mathcal H)S≤​(H) is the set of subnormalized states (positive semidefinite, trace at most one). A state on HA⊗HB\mathcal H_A\otimes\mathcal H_BHA​⊗HB​ is written ρAB\rho_{AB}ρAB​, and its marginal ρB=Tr⁡AρAB\rho_B=\operatorname{Tr}_A\rho_{AB}ρB​=TrA​ρAB​. The von Neumann entropy is H(A)ρ=−Tr⁡ρAlog⁡ρAH(A)_\rho=-\operatorname{Tr}\rho_A\log\rho_AH(A)ρ​=−TrρA​logρA​ and the conditional entropy H(A∣B)ρ=H(AB)ρ−H(B)ρH(A|B)_\rho=H(AB)_\rho-H(B)_\rhoH(A∣B)ρ​=H(AB)ρ​−H(B)ρ​.

The min-entropy of AAA conditioned on BBB is

Hmin⁡(A∣B)ρ=max⁡{λ∈R:∃ σB∈S=(HB), ρAB≤2−λ 1A⊗σB}.H_{\min}(A|B)_\rho=\max\{\lambda\in\mathbb R : \exists\,\sigma_B\in S_=(\mathcal H_B),\ \rho_{AB}\le 2^{-\lambda}\,\mathbb 1_A\otimes\sigma_B\}.Hmin​(A∣B)ρ​=max{λ∈R:∃σB​∈S=​(HB​), ρAB​≤2−λ1A​⊗σB​}.

The purified distance between subnormalized states is P(ρ,σ)=1−Fˉ(ρ,σ)2P(\rho,\sigma)=\sqrt{1-\bar F(\rho,\sigma)^2}P(ρ,σ)=1−Fˉ(ρ,σ)2​, where Fˉ(ρ,σ)=∥ρσ∥1+(1−Tr⁡ρ)(1−Tr⁡σ)\bar F(\rho,\sigma)=\|\sqrt\rho\sqrt\sigma\|_1+\sqrt{(1-\operatorname{Tr}\rho)(1-\operatorname{Tr}\sigma)}Fˉ(ρ,σ)=∥ρ​σ​∥1​+(1−Trρ)(1−Trσ)​ is the generalized fidelity. The smooth min-entropy maximizes the min-entropy over the ball Bε(ρ)={ρ′∈S≤:P(ρ,ρ′)≤ε}\mathcal B^\varepsilon(\rho)=\{\rho'\in S_\le : P(\rho,\rho')\le\varepsilon\}Bε(ρ)={ρ′∈S≤​:P(ρ,ρ′)≤ε}:

Hmin⁡ε(A∣B)ρ=max⁡ρ′∈Bε(ρAB)Hmin⁡(A∣B)ρ′.H^\varepsilon_{\min}(A|B)_\rho=\max_{\rho'\in\mathcal B^\varepsilon(\rho_{AB})}H_{\min}(A|B)_{\rho'} .Hminε​(A∣B)ρ​=ρ′∈Bε(ρAB​)max​Hmin​(A∣B)ρ′​.

For nnn independent copies, ρ⊗n\rho^{\otimes n}ρ⊗n is a state on An⊗BnA^n\otimes B^nAn⊗Bn. The non-conditional entropies Hmin⁡(A)ρ=−log⁡∥ρ∥∞H_{\min}(A)_\rho=-\log\|\rho\|_\inftyHmin​(A)ρ​=−log∥ρ∥∞​, H0(A)ρ=log⁡rank⁡ρH_0(A)_\rho=\log\operatorname{rank}\rhoH0​(A)ρ​=logrankρ and Hα(A)ρ=11−αlog⁡Tr⁡ραH_\alpha(A)_\rho=\frac{1}{1-\alpha}\log\operatorname{Tr}\rho^\alphaHα​(A)ρ​=1−α1​logTrρα, and their smoothings over the same ball, appear in the intermediate lemmas.

Formalization targets

Goal: the von Neumann entropy DPI (Theorem 3)

H(A∣BC)ρ≤H(A∣B)ρ(ρ∈S=(HABC)).H(A|BC)_\rho\le H(A|B)_\rho\qquad(\rho\in S_=(\mathcal H_{ABC})).H(A∣BC)ρ​≤H(A∣B)ρ​(ρ∈S=​(HABC​)).

The goal is the existing Open platform theorem QAlgorithms.Papers.Independent.Gap48.P20.strongSubadditivity, which states 0≤H(CB)+H(RB)−H(B)−H(CRB)0\le H(CB)+H(RB)-H(B)-H(CRB)0≤H(CB)+H(RB)−H(B)−H(CRB) for every density matrix on C⊗R⊗BC\otimes R\otimes BC⊗R⊗B; with A↦CA\mapsto CA↦C, C↦RC\mapsto RC↦R this is exactly H(ABC)+H(B)≤H(AB)+H(BC)H(ABC)+H(B)\le H(AB)+H(BC)H(ABC)+H(B)≤H(AB)+H(BC), the expanded form of the inequality above. It is referenced, not restated.

The smooth min-entropy DPI (Theorem 1)

Hmin⁡ε(A∣BC)ρ≤Hmin⁡ε(A∣B)ρ.H^\varepsilon_{\min}(A|BC)_\rho\le H^\varepsilon_{\min}(A|B)_\rho .Hminε​(A∣BC)ρ​≤Hminε​(A∣B)ρ​.

The QAEP (Theorem 2)

lim⁡ε→0lim⁡n→∞1nHmin⁡ε(An∣Bn)ρ⊗n=H(A∣B)ρ,\lim_{\varepsilon\to0}\lim_{n\to\infty}\frac1n H^\varepsilon_{\min}(A^n|B^n)_{\rho^{\otimes n}}=H(A|B)_\rho ,ε→0lim​n→∞lim​n1​Hminε​(An∣Bn)ρ⊗n​=H(A∣B)ρ​,

split into the lower bound (Lemma 4.1) and the upper bound (Lemma 4.2). The milestones below them are the paper's own lemmas: monotonicity of the purified distance (Lemma A.1), Uhlmann's theorem (Theorem A.1, an existing Open platform theorem), the chain rule (Lemma 5.1), the Rényi lower bound (Lemma 5.2), the limit α→1\alpha\to1α→1 of Rényi entropies (Lemma B.2), the non-conditional QAEP for Hmin⁡εH^\varepsilon_{\min}Hminε​ and H0εH^\varepsilon_0H0ε​ (Lemmas 5.4, 5.5), the bound by a nearby conditional entropy (Lemma 5.6), the eigenvalue-alignment bound (Lemma A.2) and the almost-i.i.d. limit (Lemma B.1).

Significance

The DPI for the von Neumann entropy is the single most used inequality in quantum information theory, and strong subadditivity is the structural fact behind it. A machine-checked proof of it is a prerequisite for formalizing essentially any converse theorem of quantum Shannon theory. The QAEP, a milestone here, is independently the bridge between one-shot and asymptotic information theory: it is what makes smooth entropies the right finite-blocklength replacements for the von Neumann entropy.

Both strong subadditivity and the QAEP are proved results; nothing in this mission is open mathematics. What the mission adds is a machine-checked route through one-shot entropies. The goal theorem is Open on the platform: it is posed but has no accepted proof. The milestones of this route, from the smooth min-entropy DPI to the QAEP, are not formalized anywhere on the platform. A completed development would also leave reusable pieces: monotonicity of the purified distance, the chain rule for smooth entropies, and the i.i.d. limits of smooth entropies.

Difficulty

Theorem 1 is short once the purified distance is known to be monotone under trace non-increasing completely positive maps, and that monotonicity (Lemma A.1) is itself the first real obstacle, since it is a statement about the generalized fidelity of subnormalized states. The bulk of the work is the QAEP. Its lower half needs a chain rule that trades conditional for non-conditional entropies at the cost of tripling the smoothing parameter, then precise i.i.d. limits of the non-conditional smooth entropies. The upper half needs a continuity statement for the conditional entropy of states that are only close to ρ⊗n\rho^{\otimes n}ρ⊗n, uniform in nnn after division by nnn. The tempting reading of the double limit as a single limit in nnn at fixed ε\varepsilonε is stronger than what the paper proves; the inner limit's existence is not established there.

Formalization scope

States are complex matrices indexed by finite types; a bipartite state is a matrix on A × B, a tripartite one on A × (B × C) with B × C the conditioning system of H(A∣BC)H(A|BC)H(A∣BC). The smooth conditional min-entropy, the purified distance, the generalized fidelity, the conditional entropy H(A∣B)H(A|B)H(A∣B) and the grouped tensor power ρ⊗n\rho^{\otimes n}ρ⊗n on AnBnA^nB^nAnBn are the published definitions QAlgorithms_Papers_Independent_Information100_P67; the Rényi entropy and Tr⁡C\operatorname{Tr}_CTrC​ come from QAlgorithms_Papers_Independent_Dependency50_P35. Smooth entropies take values in the extended reals, so an empty ball gives −∞-\infty−∞ and a ball containing 000 gives +∞+\infty+∞.

A local definitions module adds the non-conditional entropies Hmin⁡H_{\min}Hmin​, Hmin⁡εH^\varepsilon_{\min}Hminε​, H0H_0H0​, H0εH^\varepsilon_0H0ε​, trace non-increasing Kraus families, and the conditional entropy (36) of a subnormalized state ρ~\tilde\rhoρ~​, 1Tr⁡ρ~max⁡σBTr⁡ρ~(log⁡(1⊗σB)−log⁡ρ~)\frac{1}{\operatorname{Tr}\tilde\rho}\max_{\sigma_B}\operatorname{Tr}\tilde\rho(\log(\mathbb 1\otimes\sigma_B)-\log\tilde\rho)Trρ~​1​maxσB​​Trρ~​(log(1⊗σB​)−logρ~​), with the maximum taken over positive definite σB\sigma_BσB​ so that Lean's convention log⁡0=0\log0=0log0=0 cannot enter. The double limit lim⁡ε→0lim⁡n→∞\lim_{\varepsilon\to0}\lim_{n\to\infty}limε→0​limn→∞​ is read through two predicates: "L≤lim⁡lim⁡fL\le\lim\lim fL≤limlimf" means that for every δ>0\delta>0δ>0 there is ε0>0\varepsilon_0>0ε0​>0 with L−δ≤f(ε,n)L-\delta\le f(\varepsilon,n)L−δ≤f(ε,n) for all ε∈(0,ε0)\varepsilon\in(0,\varepsilon_0)ε∈(0,ε0​) and all large nnn, and "lim⁡lim⁡f≤L\lim\lim f\le Llimlimf≤L" is the mirror statement.

Trivializing encodings are ruled out: the smooth entropies are the published sup over the full subnormalized purified-distance ball, not free reals and not the ball {ρ}\{\rho\}{ρ}; ε\varepsilonε is quantified universally below ε0\varepsilon_0ε0​ and is never allowed to depend on nnn; and the entropy of the nearby state in Lemma 5.6 is (36), not H(AB)−H(B)H(AB)-H(B)H(AB)−H(B).

The paper's Lemma 5.3, (30), is false as printed and is not posed: at ε=0\varepsilon=0ε=0 it states H0≤HαH_0\le H_\alphaH0​≤Hα​ for α<1\alpha<1α<1, the reverse of Rényi monotonicity, and ρ=diag⁡(0.9,0.1)\rho=\operatorname{diag}(0.9,0.1)ρ=diag(0.9,0.1), α=3/4\alpha=3/4α=3/4, ε=0.1\varepsilon=0.1ε=0.1 gives 1>0.86371>0.86371>0.8637. Lemma 5.5, which its proof serves, is true and is a milestone. Uhlmann's theorem (Theorem A.1) is the existing Open platform theorem Claimed50.P12.lemmaB_3.

Contributions of any milestone are welcome. The purified-distance monotonicity and the Rényi-limit lemmas are reusable well beyond this paper.

Selected references

  • N. J. Beaudry and R. Renner, An intuitive proof of the data processing inequality, Quantum Inf. Comput. 12 (2012) 432–441. https://arxiv.org/abs/1107.0740v2
  • E. H. Lieb and M. B. Ruskai, Proof of the strong subadditivity of quantum-mechanical entropy, J. Math. Phys. 14 (1973) 1938–1941. https://doi.org/10.1063/1.1666274
  • M. Tomamichel, R. Colbeck and R. Renner, A fully quantum asymptotic equipartition property, IEEE Trans. Inf. Theory 55 (2009) 5840–5847. https://arxiv.org/abs/0811.1221
  • M. Tomamichel, R. Colbeck and R. Renner, Duality between smooth min- and max-entropies, IEEE Trans. Inf. Theory 56 (2010) 4674–4681. https://arxiv.org/abs/0907.5238
  • B. Schumacher, Quantum coding, Phys. Rev. A 51 (1995) 2738–2747. https://doi.org/10.1103/PhysRevA.51.2738
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Convex OptimizationOperations ResearchProbability+1·Captain: Shuze Chen

Stochastic Networks XVI: The Stability Region of Alpha-Fair Flow AllocationsTextbook

Stability of networks carrying files

Bandwidth allocation determines how quickly a network transfers each file, but files also arrive and depart while the network operates. An allocation can be feasible at every instant and still allow the number of unfinished files to grow without an equilibrium. The relevant question is therefore about the interaction of the allocation rule with the changing population of flows. Chapter 8 of Kelly and Yudovina's Stochastic Networks studies this question under a separation between rapid packet-level control and slower file-level changes. The target here is its characterization of stability for weighted alpha-fair allocations.

The distinction matters even in small networks. Capacity assigned to one route can prevent another route from using several resources together. Consequently, unused capacity at individual resources does not by itself identify a stable allocation policy. A stability theorem must address both the network constraints and the stochastic evolution of the population. The chapter contrasts alpha-fair sharing with priority rules that can have a smaller stability region.

Flow counts and bandwidth allocation

A route is a nonempty collection of resources used by a file transfer. There are finitely many routes and resources. The incidence matrix AAA has entry Ajr=1A_{jr}=1Ajr​=1 when route rrr uses resource jjj, and zero otherwise. Resource jjj has positive capacity CjC_jCj​. A state n∈NRn\in\mathbb N^Rn∈NR records the number nrn_rnr​ of unfinished files on each route; there is no upper bound on this count.

Files arrive on route rrr as independent Poisson processes of positive intensity νr\nu_rνr​. Their sizes are independent exponential random variables with positive parameter μr\mu_rμr​, so their mean size is 1/μr1/\mu_r1/μr​. The offered load is ρr=νr/μr\rho_r=\nu_r/\mu_rρr​=νr​/μr​. If each file on route rrr receives rate xr(n)x_r(n)xr​(n), its aggregate service allocation is Xr(n)=nrxr(n)X_r(n)=n_rx_r(n)Xr​(n)=nr​xr​(n). Births have intensity νr\nu_rνr​, and departures have intensity μrXr(n)\mu_rX_r(n)μr​Xr​(n) when nr>0n_r>0nr​>0.

For positive weights wrw_rwr​ and α>0\alpha>0α>0, the weighted alpha-fair allocation maximizes the aggregate objective

Gn(X)={∑rwrnrαXr1−α/(1−α),α≠1,∑rwrnrlog⁡Xr,α=1,G_n(X)=\begin{cases} \sum_r w_r n_r^\alpha X_r^{1-\alpha}/(1-\alpha),&\alpha\ne1,\\ \sum_r w_r n_r\log X_r,&\alpha=1, \end{cases}Gn​(X)={∑r​wr​nrα​Xr1−α​/(1−α),∑r​wr​nr​logXr​,​α=1,α=1,​

subject to X≥0X\ge0X≥0 and AX≤CAX\le CAX≤C. Active routes receive positive rates; inactive routes have zero aggregate allocation and zero utility contribution. These are the model and optimization rule in Sections 8.1–8.3 of the supplied source.

Formalization targets

The first milestone is Exercise 8.3. The per-flow objective FnF_nFn​ is concave on its finite-utility domain, and its coordinate derivative has the common form

∂Fn∂xr=wrnrxr−α.\frac{\partial F_n}{\partial x_r}=w_rn_rx_r^{-\alpha}.∂xr​∂Fn​​=wr​nr​xr−α​.

The second milestone is Equation (8.5). For a feasible comparison vector UUU positive on active coordinates, the full supporting-utility chain is

Gn′(U)⋅(U−X(n))≤Gn(U)−Gn(X(n))≤0.G_n'(U)\cdot(U-X(n))\le G_n(U)-G_n(X(n))\le0.Gn′​(U)⋅(U−X(n))≤Gn​(U)−Gn​(X(n))≤0.

The third milestone is Exercise D.2. With the chapter's Lyapunov function LLL and first-order expression HHH, the actual generator satisfies a remainder bound uniform over the entire state space:

QL(n)≤H(n)+η∑rnrα+b(η>0).QL(n)\le H(n)+\eta\sum_r n_r^\alpha+b\qquad(\eta>0).QL(n)≤H(n)+ηr∑​nrα​+b(η>0).

The constant bbb is independent of nnn. Under strict subcriticality, this exercise also asks for a strictly negative drift outside a finite exception set and a finite bound inside it.

The goal remains the complete Theorem 8.2:

the flow-count process has an equilibrium distribution⟺∑r:j∈rρr<Cjfor every j.\text{the flow-count process has an equilibrium distribution} \quad\Longleftrightarrow\quad \sum_{r:j\in r}\rho_r<C_j\quad\text{for every }j.the flow-count process has an equilibrium distribution⟺r:j∈r∑​ρr​<Cj​for every j.

The source identifies this equilibrium property with positive recurrence. Equality at a resource capacity belongs to the nonpositive-recurrent side of the equivalence. None of the milestones substitutes for that stochastic conclusion.

What the characterization provides

Theorem 8.2 identifies the stability region using only the offered loads and capacities, for every fixed positive choice of weights and alpha. Those choices affect allocation but do not change the region asserted by the theorem. The result also distinguishes stability from instantaneous feasibility: the conclusion concerns a probability law for an unbounded population over continuous time. This is the result stated in Chapter 8, rather than a new research conjecture.

The formalization reuses published feasibility, utility, concavity, derivative, tangent, and deterministic drift results. Its remaining targets include inactive routes and the stochastic equivalence. The new definition layer supplies a countable transition function and an invariant-distribution predicate usable in subsequent flow-level results. The proposed theorems are proof targets, not completed machine-checked proofs.

Analytic and stochastic obligations

The chapter presents a sketch of the stability proof. A finite-time conditional increment is not automatically its first-order approximation, especially when some coordinates are empty. Reallocation also changes service rates while every route remains nonempty; finding F6 records a two-route counterexample to the sketch's explanation of finite-time equality. A negative expression obtained from the optimization problem is therefore insufficient to establish positive recurrence. Exercise D.2 addresses the actual drift and the uniformity needed over unbounded counts.

The necessity sketch also identifies a single-resource reduction with the equal-sharing exercise. For unequal weights, that identification requires additional justification: the reduced allocation need not share capacity equally. This proof gap is recorded with a two-route instance. It does not change the printed theorem or introduce a variant. The separate printed mistakes in Exercises 8.1, 8.2, and 8.10 remain documented findings; those exercises are outside the selected milestones.

Formalization scope

Finite index types represent resources and routes, while states are functions into the natural numbers. Parameters are real and positive, and every route uses at least one resource. Zero-count departures are explicitly absent. The utility retains the logarithmic case and both ranges on either side of one. Concavity includes active zero rates when alpha is below one; otherwise that boundary has extended utility minus infinity. Coordinate derivatives are asserted where the active-coordinate derivative exists.

The process is represented through its continuous-time transition function, constructed as a Poisson mixture of powers of a bounded-rate transition matrix. Equilibrium requires invariance for every nonnegative real time and a probability measure on canonical trajectories whose coordinate process realizes all the stationary Markov finite-dimensional distributions. Probability sums use extended nonnegative reals, so divergent mass is not replaced by zero. The rate bound is the explicit quantity

B=1+∑rνr+(∑rμr)(∑jCj).B=1+\sum_r\nu_r+\left(\sum_r\mu_r\right)\left(\sum_jC_j\right).B=1+r∑​νr​+(r∑​μr​)(j∑​Cj​).

It is a construction parameter, not an approximation constant or a new capacity restriction. No big-O or high-probability assertion is used. In Exercise D.2, the remainder constant may depend on the fixed network and on the chosen positive tolerance, but not on the state; the finite exception set uses total occupancy.

Positive recurrence is not defined as negative drift or rate balance, and neither a stationary distribution nor a drift inequality is assumed in the goal. Further contributions can establish the process properties, the generator estimates, and the recurrence equivalence. The existing published definitions are retained under their original names; other chapters' unpublished modules are not imported.

Selected references

  • F. P. Kelly and E. Yudovina, Stochastic Networks, Cambridge University Press, 2014. DOI. Source indices refer to the supplied Lecture Notes on Stochastic Networks PDF: Chapter 8, printed pp. 186–199, and Appendix D, printed pp. 212–215. Equivalence to a particular published printing has not been established.
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Convex OptimizationOperations ResearchOptimization+1·Captain: Shuze Chen

Stochastic Networks XII: Implied Costs and Sensitivity in Loss NetworksTextbook

Motivation

An accepted call earns revenue but occupies circuits that could serve later calls. In a network, those consequences extend beyond the links used by the original call: a change in blocking on one link changes the traffic reaching other links. Network planning therefore needs a marginal value that accounts for these indirect effects. Chapter 4 of Kelly and Yudovina's Stochastic Networks develops such values for the Erlang fixed-point approximation. The relevant question is how revenue changes when offered traffic or installed capacity changes, with the network allowed to settle to its new fixed point.

The mission concerns this sensitivity calculation. It complements the scalar Erlang formula and fixed-point uniqueness results, which already have published formalizations. It does not claim that the approximation equals the exact stationary performance of the underlying stochastic loss network.

Setting

A loss network has finitely many links and routes. Link jjj has a positive integer number CjC_jCj​ of circuits. A call of route rrr requires AjrA_{jr}Ajr​ circuits at link jjj, where the matrix entries are nonnegative integers. Its offered traffic is νr>0\nu_r>0νr​>0, and carrying it earns a real value wrw_rwr​. Every link in the stated system is used by at least one route.

The Erlang fixed point assigns a blocking probability BjB_jBj​ to each link. In the independent-link approximation, the acceptance probability and carried traffic of route rrr are

ar=1−Lr=∏j(1−Bj)Ajr,λr=νrar.a_r=1-L_r=\prod_j(1-B_j)^{A_{jr}},\qquad \lambda_r=\nu_ra_r.ar​=1−Lr​=j∏​(1−Bj​)Ajr​,λr​=νr​ar​.

Write qj=∑rAjrλrq_j=\sum_rA_{jr}\lambda_rqj​=∑r​Ajr​λr​ for carried circuit load and ρj=qj/(1−Bj)\rho_j=q_j/(1-B_j)ρj​=qj​/(1−Bj​) for reduced offered load. The defining equations are Bj=E(ρj,Cj)B_j=E(\rho_j,C_j)Bj​=E(ρj​,Cj​), where EEE is Erlang's scalar blocking formula. Revenue is W(ν;C)=∑rwrλrW(\nu;C)=\sum_rw_r\lambda_rW(ν;C)=∑r​wr​λr​.

The capacity derivative requires an additional convention. The scalar Erlang formula is extended by linear interpolation between successive integer capacities, and the network fixed point is then recomputed using that extension. At the original integer capacities, capacity sensitivity means the derivative from the left. Interpolating the final network revenue would define a different function. These conventions are specified on printed page 102 of the supplied source.

Formalization targets

The goal is Theorem 4.6, printed page 103. Define the improvement quantity

δj=ρj(E(ρj,Cj−1)−E(ρj,Cj)).\delta_j=\rho_j\bigl(E(\rho_j,C_j-1)-E(\rho_j,C_j)\bigr).δj​=ρj​(E(ρj​,Cj​−1)−E(ρj​,Cj​)).

There is a unique route-surplus vector sss and link-cost vector ccc satisfying

sr=wr−∑jcjAjr,cj=δj∑rAjrλr(sr+cj)qj.s_r=w_r-\sum_jc_jA_{jr},\qquad c_j=\delta_j\frac{\sum_rA_{jr}\lambda_r(s_r+c_j)}{q_j}.sr​=wr​−j∑​cj​Ajr​,cj​=δj​qj​∑r​Ajr​λr​(sr​+cj​)​.

The goal asserts existence of the derivatives and their values:

∂W∂νr=arsr,∂−W∂Cj=cj.\frac{\partial W}{\partial\nu_r}=a_rs_r,\qquad \frac{\partial^-W}{\partial C_j}=c_j.∂νr​∂W​=ar​sr​,∂Cj​∂−W​=cj​.

Uniqueness concerns all solutions of the local cost equations, independently of whether they also satisfy a derivative identity.

Three source milestones support this target. Exercise 1.8 gives the scalar Erlang traffic derivative. Theorem 3.20 supplies existence and uniqueness of the integer-capacity fixed point. Both are reused as published references. Exercise 4.9 supplies the matrix characterization. With Λ=diag⁡(λr)\Lambda=\operatorname{diag}(\lambda_r)Λ=diag(λr​) and Γ=diag⁡(δj/[(1−δj)qj])\Gamma=\operatorname{diag}(\delta_j/[(1-\delta_j)q_j])Γ=diag(δj​/[(1−δj​)qj​]), it states

c(I+AΛATΓ)=wΛATΓ.c(I+A\Lambda A^T\Gamma)=w\Lambda A^T\Gamma.c(I+AΛATΓ)=wΛATΓ.

The symmetric matrix Q=I+Γ1/2AΛATΓ1/2Q=I+\Gamma^{1/2}A\Lambda A^T\Gamma^{1/2}Q=I+Γ1/2AΛATΓ1/2 is positive definite and invertible, and the unique costs are

c=wΛATΓ1/2Q−1Γ1/2.c=w\Lambda A^T\Gamma^{1/2}Q^{-1}\Gamma^{1/2}.c=wΛATΓ1/2Q−1Γ1/2.

These are the claims of Exercise 4.9, printed pages 106–107, including both the equivalence and the explicit solution.

Significance

An implied cost assigns the marginal revenue effect of capacity to an individual link. A route's surplus compares its direct value with the total implied cost of the circuits it uses. The theorem thus relates local quantities to derivatives of a network-wide objective. As explained in Remark 4.7, the link costs are also shadow prices for capacity. Their interpretation includes the effect on later traffic, rather than just the revenue of the currently admitted call.

The formal contribution is the precise connection between the actual fixed-point revenue function, one-sided capacity sensitivity, and the unique local linear system. The published scalar derivative and fixed-point theorem remain references, not duplicate problems. The new definition layer and matrix characterization provide reusable objects for later formal work on routing and capacity sensitivity. The submitted theorem statements are proof obligations; successful compilation does not supply their proofs.

Difficulty

Differentiating revenue while holding the blocking vector fixed misses the indirect effects that the theorem measures. Blocking is itself an implicit function of all offered traffics and capacities. Moreover, the scalar interpolation has corners at integer capacities, so ordinary two-sided capacity differentiability is not the required statement. The formal obligations include existence of the appropriate derivatives; merely evaluating a total derivative operator would not establish that existence.

The printed proof explicitly treats a 000–111 incidence matrix, whereas the surrounding fixed-point model allows arbitrary nonnegative integer circuit requirements. Finding F2 records this proof-scope gap. The goal retains the general integer statement. Exercise 4.9 also requires legitimate denominators and an invertible matrix; these properties must be established from the network data rather than supplied as assumed conclusions.

Formalization scope

Links and routes use finite, zero-based index types. Values, traffic, and blocking coordinates are real. The base capacities are positive integers, offered traffic is positive, and each link is used. The last condition states the domain of the printed weighted-average quotient: an isolated link would make its denominator zero. No injectivity or rank condition on the incidence matrix is imposed. Empty link sets are allowed; in that case every route has acceptance one and revenue is linear in offered traffic.

The scalar Erlang formula and integer fixed-point relation reuse the series' published definitions. The new physical fixed-point selector is constructed from the interpolated equations, with a total fallback outside the existence domain. Its definition assumes no differentiability or cost identity. The goal additionally verifies the selected integer-capacity vector against the published fixed-point relation. A formalization that assumes the sensitivity identities, or replaces revenue by an arbitrary function constrained to satisfy them, would trivialize the target and is excluded here.

No asymptotic notation or unspecified constants occur in these targets. Exercise 4.8's marker-route reduction is left as a proof resource rather than a separate milestone. The queueing-cost strict-convexity assertion in Exercise 4.7 is outside this loss-network mission; its counterexample remains recorded as F1. Finding F3 records why the displayed improvement formula cannot simply be extended to noninteger base capacities: at unit load and capacity 3/23/23/2, a single-link example gives actual capacity derivative 3/103/103/10 but cost formula 2/52/52/5. No variant item is posed.

Selected references

  • F. P. Kelly and E. Yudovina, Stochastic Networks, Cambridge University Press, 2014. DOI. This mission cites the supplied PDF titled Lecture Notes on Stochastic Networks: Exercise 1.8, printed page 20; Theorem 3.20, printed page 67; and Section 4.3.2, printed pages 102–107. PDF pages are eight greater than printed pages. Equivalence with a particular published printing has not been established.
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Operations ResearchOptimizationReinforcement Learning·Captain: Shuze Chen

Fast Global Convergence of Natural Policy Gradient Methods with Entropy Regularization: Global linear convergence of exact natural policy gradientResearch Paper

Motivation: quantitative convergence of policy optimization

A decision maker repeatedly chooses an action, receives a reward, and moves to another state. A policy specifies how to randomize the next action in each state. Optimizing these choices directly is a central approach to reinforcement learning, but the resulting objective need not be concave in its policy parameters. A useful convergence guarantee must therefore describe behavior from an arbitrary admissible starting policy, rather than only near a favorable solution.

Entropy regularization rewards policies for maintaining randomness. This changes both the optimization problem and the behavior of policy updates. Cen, Cheng, Chen, Wei and Chi establish explicit global linear convergence for an entropy-regularized natural policy gradient update with exact evaluation. This mission targets that result, retaining its two error measures, initialization constant, and complete range of fixed learning rates.

Setting: finite discounted decisions with entropy rewards

Let the state set SSS and action set AAA be finite and nonempty. A transition kernel P(x∣s,a)P(x\mid s,a)P(x∣s,a) specifies a probability distribution over the next state xxx. Rewards satisfy r(s,a)∈[0,1]r(s,a)\in[0,1]r(s,a)∈[0,1], and the discount factor satisfies 0<γ<10<\gamma<10<γ<1. A stationary randomized policy π(a∣s)\pi(a\mid s)π(a∣s) is a probability vector over actions at every state. Starting at sss, successive actions follow the policy and successive states follow the transition kernel.

For a positive temperature τ\tauτ, the regularized value is

Vτπ(s)=Esπ∑k≥0γk[r(sk,ak)−τlog⁡π(ak∣sk)].V_\tau^\pi(s)=\mathbb E_s^\pi\sum_{k\ge0}\gamma^k\bigl[r(s_k,a_k)-\tau\log\pi(a_k\mid s_k)\bigr].Vτπ​(s)=Esπ​k≥0∑​γk[r(sk​,ak​)−τlogπ(ak​∣sk​)].

Zero-probability actions contribute zero to the expected entropy term. The soft action value is

Qτπ(s,a)=r(s,a)+γ∑xP(x∣s,a)Vτπ(x).Q_\tau^\pi(s,a)=r(s,a)+\gamma\sum_xP(x\mid s,a)V_\tau^\pi(x).Qτπ​(s,a)=r(s,a)+γx∑​P(x∣s,a)Vτπ​(x).

Its immediate reward has no entropy penalty. The optimal value Vτ∗(s)V_\tau^*(s)Vτ∗​(s) is the supremum of regularized returns over the entire closed simplex of stationary policies; Qτ∗=r+γPVτ∗Q_\tau^*=r+\gamma PV_\tau^*Qτ∗​=r+γPVτ∗​. The canonical optimal policy is πτ∗=softmax⁡(Qτ∗/τ)\pi_\tau^*=\operatorname{softmax}(Q_\tau^*/\tau)πτ∗​=softmax(Qτ∗​/τ), with its optimality stated as a separate supporting target. These conventions follow §2.1 and Appendix C.2.

Initialize at any strictly positive policy, equivalently any policy obtained from finite real logits by softmax. Fix 0<η≤(1−γ)/τ0<\eta\le(1-\gamma)/\tau0<η≤(1−γ)/τ and write α=1−ητ/(1−γ)\alpha=1-\eta\tau/(1-\gamma)α=1−ητ/(1−γ). The exact algorithm evaluates Qτ(t)=Qτπ(t)Q_\tau^{(t)}=Q_\tau^{\pi^{(t)}}Qτ(t)​=Qτπ(t)​ and then updates

π(t+1)(a∣s)=π(t)(a∣s)αexp⁡(ηQτ(t)(s,a)/(1−γ))∑bπ(t)(b∣s)αexp⁡(ηQτ(t)(s,b)/(1−γ)).\pi^{(t+1)}(a\mid s)=\frac{\pi^{(t)}(a\mid s)^\alpha\exp(\eta Q_\tau^{(t)}(s,a)/(1-\gamma))}{\sum_b\pi^{(t)}(b\mid s)^\alpha\exp(\eta Q_\tau^{(t)}(s,b)/(1-\gamma))}.π(t+1)(a∣s)=∑b​π(t)(b∣s)αexp(ηQτ(t)​(s,b)/(1−γ))π(t)(a∣s)αexp(ηQτ(t)​(s,a)/(1−γ))​.

This is Algorithm 1, equation (18). The faithful MDP statements also retain the paper's p. 13 assumption that the optimal policy has a stationary state distribution with strictly positive mass at every state. No uniqueness or irreducibility is required.

Formalization targets

The goal is Theorem 1, p. 10. Define

C1=∥Qτ∗−Qτ(0)∥∞+2τα∥log⁡πτ∗−log⁡π(0)∥∞.C_1=\|Q_\tau^*-Q_\tau^{(0)}\|_\infty+2\tau\alpha\|\log\pi_\tau^*-\log\pi^{(0)}\|_\infty.C1​=∥Qτ∗​−Qτ(0)​∥∞​+2τα∥logπτ∗​−logπ(0)∥∞​.

For every t≥0t\ge0t≥0, the two required bounds are

∥Qτ∗−Qτ(t+1)∥∞≤C1γ(1−ητ)t,\|Q_\tau^*-Q_\tau^{(t+1)}\|_\infty\le C_1\gamma(1-\eta\tau)^t,∥Qτ∗​−Qτ(t+1)​∥∞​≤C1​γ(1−ητ)t, ∥log⁡πτ∗−log⁡π(t+1)∥∞≤2C1τ−1(1−ητ)t.\|\log\pi_\tau^*-\log\pi^{(t+1)}\|_\infty\le2C_1\tau^{-1}(1-\eta\tau)^t.∥logπτ∗​−logπ(t+1)∥∞​≤2C1​τ−1(1−ητ)t.

The supporting milestones retain the source's order of use and exact strength. Lemma 1 expresses the one-step value improvement as an expectation, under the new policy's normalized discounted visitation law, of two directed KL divergences:

ΔVτ(ρ)=Es∼dρ(t+1)[(η−1−τ1−γ)KL(πs(t+1)∥πs(t))+η−1KL(πs(t)∥πs(t+1))].\Delta V_\tau(\rho)=\mathbb E_{s\sim d_\rho^{(t+1)}}\left[\left(\eta^{-1}-\frac\tau{1-\gamma}\right)\mathrm{KL}(\pi^{(t+1)}_s\|\pi^{(t)}_s)+\eta^{-1}\mathrm{KL}(\pi^{(t)}_s\|\pi^{(t+1)}_s)\right].ΔVτ​(ρ)=Es∼dρ(t+1)​​[(η−1−1−γτ​)KL(πs(t+1)​∥πs(t)​)+η−1KL(πs(t)​∥πs(t+1)​)].

Lemma 2 concerns the variational soft Bellman operator Tτ\mathcal T_\tauTτ​. Its three targets are the log-sum-exp formula, the fixed point Tτ(Qτ∗)=Qτ∗\mathcal T_\tau(Q_\tau^*)=Q_\tau^*Tτ​(Qτ∗​)=Qτ∗​, and

∥Tτ(Q1)−Tτ(Q2)∥∞≤γ∥Q1−Q2∥∞.\|\mathcal T_\tau(Q_1)-\mathcal T_\tau(Q_2)\|_\infty\le\gamma\|Q_1-Q_2\|_\infty.∥Tτ​(Q1​)−Tτ​(Q2​)∥∞​≤γ∥Q1​−Q2​∥∞​.

Appendix A.2, equation (66), supplies the general vector bound

∥log⁡softmax⁡(θ1)−log⁡softmax⁡(θ2)∥∞≤2∥θ1−θ2∥∞.\|\log\operatorname{softmax}(\theta_1)-\log\operatorname{softmax}(\theta_2)\|_\infty\le2\|\theta_1-\theta_2\|_\infty.∥logsoftmax(θ1​)−logsoftmax(θ2​)∥∞​≤2∥θ1​−θ2​∥∞​.

Lemma 3 uses the unnormalized auxiliary sequence from (42), defined by ξ(0)(s,a)=(∑beQτ∗(s,b)/τ)π(0)(a∣s)\xi^{(0)}(s,a)=(\sum_b e^{Q_\tau^*(s,b)/\tau})\pi^{(0)}(a\mid s)ξ(0)(s,a)=(∑b​eQτ∗​(s,b)/τ)π(0)(a∣s) and ξ(t+1)=(ξ(t))αe(1−α)Qτ(t)/τ\xi^{(t+1)}=(\xi^{(t)})^\alpha e^{(1-\alpha)Q_\tau^{(t)}/\tau}ξ(t+1)=(ξ(t))αe(1−α)Qτ(t)​/τ. Its target is

∥Qτ∗−Qτ(t+1)∥∞≤γ∥Qτ∗−τlog⁡ξ(t+1)∥∞+γαt+1∥Qτ(0)−τlog⁡ξ(0)∥∞.\|Q_\tau^*-Q_\tau^{(t+1)}\|_\infty\le\gamma\|Q_\tau^*-\tau\log\xi^{(t+1)}\|_\infty+\gamma\alpha^{t+1}\|Q_\tau^{(0)}-\tau\log\xi^{(0)}\|_\infty.∥Qτ∗​−Qτ(t+1)​∥∞​≤γ∥Qτ∗​−τlogξ(t+1)∥∞​+γαt+1∥Qτ(0)​−τlogξ(0)∥∞​.

All four milestone statements are from pp. 14–17 and 25. A further ordinary supporting target states that the canonical optimal policy attains Vτ∗V_\tau^*Vτ∗​ and establishes the value characterization in (74).

Significance: simultaneous control of values and probabilities

The goal gives finite-time quantitative control of every soft action value and every log action probability. Its constants expose the influence of initialization, discount, temperature, and learning rate. At the endpoint η=(1−γ)/τ\eta=(1-\gamma)/\tauη=(1−γ)/τ, the update becomes soft policy iteration; the same theorem covers smaller positive steps. These are claims of the source theorem, rather than asymptotic conclusions substituted for its explicit bounds.

The mathematical result is already established in the cited paper. The remaining work is a machine-checked proof connecting actual discounted returns, optimization over policies, and the specified recurrence. The local theorem files are open statements. Published policy, occupation, discounted-return, and softmax definitions provide reusable infrastructure, while this mission adds the entropy-specific objects needed for that connection.

Difficulty: the update retains its policy history

A contraction theorem for soft value iteration does not by itself establish the stated bounds for general learning rates. The policy update depends on both its evaluated action values and its current probabilities. The target controls these coupled quantities with the paper's exact constants. It must also handle the endpoint where the retention exponent is zero. Convergence of an arbitrary error recurrence, or convergence only from uniform initialization, would leave the target unresolved.

Finding F6 records a minor error in the printed proof of Lemma 2 on p. 27: moving an absolute value inside an expectation requires an inequality. The triangle inequality repairs that step without changing the theorem statement.

Formalization scope

State and action spaces are arbitrary nonempty finite types. Probabilities and rewards are real arrays; stochasticity and reward bounds are explicit predicates. Values use the published infinite occupation series. Optimal values use real suprema over valid policies, including policies with zero entries. Finite entropy bounds and geometric discounting make these suprema finite and the series summable on the theorem domain. The variational Bellman objective is continuous on a compact simplex, so its supremum is attained.

Norms are the supremum norms on ordinary finite function spaces. Time is indexed by natural numbers starting at zero. Policy powers use real exponents, and natural logarithms are entrywise. The constructed sequence is the algorithm itself; no convergence, monotonicity, or contraction assumption is inserted into its definition. Supporting proofs for well-definedness and optimality are welcome alongside proofs of the numbered targets.

The scope excludes approximate evaluation, sampling guarantees, local quadratic convergence, Fisher-pseudoinverse equivalence, and the separate value bound (24). Recorded source findings explain these distinctions. No variant is posed in this draft; the possible removal of the stationary-support assumption remains a separate finding.

Selected references

  • Shicong Cen, Chen Cheng, Yuxin Chen, Yuting Wei and Yuejie Chi, Fast Global Convergence of Natural Policy Gradient Methods with Entropy Regularization, arXiv preprint, version 5, 2021. Pinned source: arXiv:2007.06558v5. All theorem numbers and pages in this mission refer exclusively to this version.
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Convex OptimizationOperations ResearchOptimization·Captain: Shuze Chen

Robust Optimization VI: The Matrix Cube Bound for Robust Least SquaresTextbook

Reliable least-squares constraints under uncertain data

A least-squares constraint limits the Euclidean length of a residual. When the coefficients of that residual are uncertain, checking the constraint at nominal data does not ensure that it holds for the data that actually occur. A robust constraint requires the same decision to satisfy the bound for every allowed perturbation. Such constraints arise naturally when fitting or designing a system whose coefficients are known only within specified bounds. Chapter 7 of Ben-Tal, El Ghaoui and Nemirovski, Robust Optimization studies explicit semidefinite approximations to these robust constraints.

The focus here is structured norm-bounded uncertainty: several perturbation blocks vary independently, each subject to a Euclidean operator-norm bound. This includes independent scalar perturbations as well as full matrix perturbations. The goal is to express a safe constraint using finitely many matrix inequalities and to quantify the conservatism of that replacement.

Residuals, perturbations, and matrix envelopes

Let y∈Rdy\in\mathbb R^dy∈Rd be a decision and let τ∈R\tau\in\mathbb Rτ∈R be a proposed bound on a residual in Rk\mathbb R^kRk. The nominal residual c(y)c(y)c(y) is affine. Its uncertain value is

c(y)+∑ν=1NLν(y)TηνRν(y).c(y)+\sum_{\nu=1}^N L_\nu(y)^T\eta_\nu R_\nu(y).c(y)+ν=1∑N​Lν​(y)Tην​Rν​(y).

Here each ην\eta_\nuην​ is a real rectangular matrix satisfying ∥ην∥2,2≤ρ\|\eta_\nu\|_{2,2}\le\rho∥ην​∥2,2​≤ρ, where ρ>0\rho>0ρ>0. The Euclidean operator norm measures the largest ratio ∥ηνv∥2/∥v∥2\|\eta_\nu v\|_2/\|v\|_2∥ην​v∥2​/∥v∥2​ over nonzero vectors. Both factors are affine functions of the decision, neither is identically zero, and at least one factor in each block is constant. Selected scalar blocks have the form θνI\theta_\nu Iθν​I; the source normalizes these blocks to size 1×11\times11×1.

Write Rρ(y,τ)R_\rho(y,\tau)Rρ​(y,τ) for robust feasibility: the residual length is at most τ\tauτ for every admissible collection of perturbations. Introduce the arrow matrix

Arrow⁡(u,τ)=[τuTuτIk].\operatorname{Arrow}(u,\tau)= \begin{bmatrix}\tau&u^T\\u&\tau I_k\end{bmatrix}.Arrow(u,τ)=[τu​uTτIk​​].

The oriented factors L^ν\widehat L_\nuLν​ and R^ν(y)\widehat R_\nu(y)Rν​(y) are the factors in the arrow representation of the vector perturbation; the former is fixed and the latter is affine. These objects and the following system are specified in equations (7.1.1)–(7.1.11).

Let Sρ(y,τ)S_\rho(y,\tau)Sρ​(y,τ) mean that symmetric matrices YνY_\nuYν​ and real multipliers λν\lambda_\nuλν​ exist satisfying

Yν⪰±(L^νTR^ν(y)+R^ν(y)TL^ν),ν∈Is,Y_\nu\succeq\pm(\widehat L_\nu^T\widehat R_\nu(y)+ \widehat R_\nu(y)^T\widehat L_\nu),\qquad\nu\in I_s,Yν​⪰±(LνT​Rν​(y)+Rν​(y)TLν​),ν∈Is​, [Yν−λνL^νTL^νR^ν(y)TR^ν(y)λνIqν]⪰0,ν∉Is,\begin{bmatrix} Y_\nu-\lambda_\nu\widehat L_\nu^T\widehat L_\nu&\widehat R_\nu(y)^T\\ \widehat R_\nu(y)&\lambda_\nu I_{q_\nu} \end{bmatrix}\succeq0,\qquad\nu\notin I_s,[Yν​−λν​LνT​Lν​Rν​(y)​Rν​(y)Tλν​Iqν​​​]⪰0,ν∈/Is​, Arrow⁡(c(y),τ)−ρ∑νYν⪰0.\operatorname{Arrow}(c(y),\tau)-\rho\sum_\nu Y_\nu\succeq0.Arrow(c(y),τ)−ρν∑​Yν​⪰0.

The notation X⪰0X\succeq0X⪰0 means that XXX is positive semidefinite. The relation X⪰±BX\succeq\pm BX⪰±B denotes both inequalities X−B⪰0X-B\succeq0X−B⪰0 and X+B⪰0X+B\succeq0X+B⪰0.

Formalization targets

The goal is Theorem 7.1.2, including all three conclusions:

Sρ(y,τ)⟹Rρ(y,τ),S_\rho(y,\tau)\Longrightarrow R_\rho(y,\tau),Sρ​(y,τ)⟹Rρ​(y,τ), ¬Sρ(y,τ)⟹¬R(π/2)ρ(y,τ),\neg S_\rho(y,\tau)\Longrightarrow\neg R_{(\pi/2)\rho}(y,\tau),¬Sρ​(y,τ)⟹¬R(π/2)ρ​(y,τ), N=1⟹(Sρ(y,τ)⟺Rρ(y,τ)).N=1\Longrightarrow\bigl(S_\rho(y,\tau)\Longleftrightarrow R_\rho(y,\tau)\bigr).N=1⟹(Sρ​(y,τ)⟺Rρ​(y,τ)).

The second conclusion compares uncertainty radii for the same decision and threshold. It is not a comparison of objective values.

The supporting targets are the arrow-matrix equivalence of Lemma 6.3.3, the two versions of the S-lemma in Lemma 6.3.5, and the mixed matrix-cube theorem, Theorem 7.1.3. The S-lemma statements are referenced as existing proved results. For the mixed cube, A(ρ)\mathcal A(\rho)A(ρ) denotes positivity for all allowed scalar and full-matrix perturbations; B(ρ)\mathcal B(\rho)B(ρ) denotes the existence of separate symmetric envelopes whose radius-scaled sum is dominated by the nominal matrix. The theorem asserts safety, exactness for one block, and

¬B(ρ)⟹¬A(ϑ(μ)ρ)\neg\mathcal B(\rho)\Longrightarrow\neg\mathcal A(\vartheta(\mu)\rho)¬B(ρ)⟹¬A(ϑ(μ)ρ)

when the scalar coefficient matrices have ranks at most μ≥2\mu\ge2μ≥2. The universal nondecreasing function satisfies ϑ(2)=π/2\vartheta(2)=\pi/2ϑ(2)=π/2, ϑ(4)=2\vartheta(4)=2ϑ(4)=2, and ϑ(μ)≤πμ/2\vartheta(\mu)\le\pi\sqrt{\mu/2}ϑ(μ)≤πμ/2​.

What the bound provides

Safety makes every feasible lifted certificate a valid robust decision. The tightness bound also limits how much a rejected decision can gain from replacing the approximation by the exact robust constraint: inflating the uncertainty radius by π/2\pi/2π/2 must expose a violation. Single-block exactness identifies an uncertainty model where the approximation loses nothing. These are the precise guarantees established in Chapter 7.

The formalization records the relation between an explicit finite matrix system and a universally quantified residual inequality. It also supplies a mixed scalar/full-block formulation that is broader than the existing scalar-only matrix-cube statement. The mathematical results are established in the textbook; the new theorem declarations here are proof targets, not completed machine-checked proofs.

Difficulty

A bound valid separately for each perturbation block does not by itself quantify the conservatism of combining those bounds. The mixed theorem must control this loss uniformly over matrix dimensions and the number of blocks while retaining its exact single-block clause. The least-squares target additionally depends on the specific arrow structure of vector residuals. Treating its coefficients as arbitrary symmetric matrices would lose the stated constant. Boundary cases with singular positive semidefinite matrices and factors vanishing at a particular decision also remain part of the problem.

Formalization scope

The development uses finite real matrices, genuine affine maps, and Mathlib's Euclidean vector spaces. Residual dimension and block sizes are positive; a decision space of dimension zero is allowed. The matrix-cube model permits either block family to be empty. Robust feasibility is defined directly by universal quantification, avoiding any supremum convention for empty or unbounded sets.

Formalization Note The two block constructors retain both original choices of the constant factor. When the original right factor is fixed, the perturbation is transposed and its dimensions are exchanged, as on printed p. 181. Scalar blocks use the source's 1×11\times11×1 normalization. Arrow factors are constructed from these data; neither a rank bound nor a certificate equivalence is a hypothesis. The explicit affine LMIs represent tractability; no separate computational-complexity model is introduced.

The reusable setup comprises Euclidean operator bounds, arrow matrices, structured least-squares data, and mixed matrix-envelope predicates. The Schur-complement result is referenced for its positive-definite branch; Mathlib supplies the corresponding positive-semidefinite equivalence under a positive-definite diagonal block. The alternative intersection-of-ellipsoids model and the nearby statement with the recorded scaling error are outside this mission. No variant is posed.

Selected references

  • Aharon Ben-Tal, Laurent El Ghaoui and Arkadi Nemirovski, Robust Optimization, Princeton University Press, 2009. DOI. Lemmas 6.3.3–6.3.5, printed pp. 163–164 (PDF pp. 189–190); Section 7.1.1 and Theorems 7.1.2–7.1.3, printed pp. 179–183 (PDF pp. 205–209). Citation basis: published.
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Robust Optimization VIII: Rank-Sensitive Approximation of Robust LMIsTextbook

Certifying matrix inequalities under uncertainty

A linear matrix inequality requires a symmetric matrix, whose entries depend affinely on design variables, to be positive semidefinite. Such constraints express many optimization and control requirements. When coefficients are uncertain, a design must satisfy a whole family of matrix inequalities. Checking each possible perturbation separately is generally impractical: even independent scalar intervals can generate exponentially many extreme cases. Chapter 9 of Ben-Tal, El Ghaoui and Nemirovski, Robust Optimization studies a finite semidefinite approximation and quantifies its conservatism.

The motivating question is concrete. A finite certificate may guarantee that a design survives all perturbations of size at most a specified radius. If this certificate fails, how much larger must the uncertainty radius become before the original robust requirement also fails? The chapter's answer depends on the ranks of scalar perturbation matrices, rather than solely on the number of uncertain coefficients or on the ambient matrix dimension.

Scalar and full matrix perturbations

Let y∈Rny\in\mathbb R^ny∈Rn be a design vector and m>0m>0m>0 the size of the symmetric matrix inequality. There are sss scalar blocks and fff full matrix blocks, with s+f≥1s+f\ge1s+f≥1. The nominal matrix An(y)A^n(y)An(y) and scalar coefficient matrices Ai(y)A_i(y)Ai​(y) are symmetric and affine in yyy. A full block has an affine factor Lj(y)∈Rpj×mL_j(y)\in\mathbb R^{p_j\times m}Lj​(y)∈Rpj​×m and a fixed nonzero factor Rj∈Rqj×mR_j\in\mathbb R^{q_j\times m}Rj​∈Rqj​×m, where pj,qj>0p_j,q_j>0pj​,qj​>0.

The uncertain matrix is

An(y)+∑i=1sziAi(y)+∑j=1f[Lj(y)TZjRj+RjTZjTLj(y)].A^n(y)+\sum_{i=1}^s z_iA_i(y) +\sum_{j=1}^f\bigl[L_j(y)^TZ_jR_j+R_j^TZ_j^TL_j(y)\bigr].An(y)+i=1∑s​zi​Ai​(y)+j=1∑f​[Lj​(y)TZj​Rj​+RjT​ZjT​Lj​(y)].

At radius ρ>0\rho>0ρ>0, the scalar perturbations satisfy ∣zi∣≤ρ|z_i|\le\rho∣zi​∣≤ρ and full matrix perturbations satisfy ∥Zj∥2,2≤ρ\|Z_j\|_{2,2}\le\rho∥Zj​∥2,2​≤ρ. Here the operator norm is induced by Euclidean vector norms. The robust counterpart Ay(ρ)\mathcal A_y(\rho)Ay​(ρ) requires positive semidefiniteness for every allowed collection of perturbations, independently across blocks.

Define Cy(ρ)\mathcal C_y(\rho)Cy​(ρ) by existence of symmetric matrices Ui,VjU_i,V_jUi​,Vj​ and real scalars λj\lambda_jλj​ satisfying

Ui⪰±Ai(y),[λjIpjLj(y)Lj(y)TVj−λjRjTRj]⪰0,U_i\succeq\pm A_i(y),\qquad \begin{bmatrix} \lambda_jI_{p_j}&L_j(y)\\ L_j(y)^T&V_j-\lambda_jR_j^TR_j \end{bmatrix}\succeq0,Ui​⪰±Ai​(y),[λj​Ipj​​Lj​(y)T​Lj​(y)Vj​−λj​RjT​Rj​​]⪰0, An(y)−ρ(∑iUi+∑jVj)⪰0.A^n(y)-\rho\left(\sum_iU_i+\sum_jV_j\right)\succeq0.An(y)−ρ(i∑​Ui​+j∑​Vj​)⪰0.

For a fixed radius this is a finite system of affine matrix inequalities, including when one of the two block classes is empty.

Formalization targets

The goal is Theorem 9.1.2, including all three conclusions. The approximation is safe:

Cy(ρ)⟹Ay(ρ).\mathcal C_y(\rho)\Longrightarrow\mathcal A_y(\rho).Cy​(ρ)⟹Ay​(ρ).

Let μ\muμ be the smallest integer at least two bounding every rank⁡Ai(y′)\operatorname{rank}A_i(y')rankAi​(y′), for every scalar index and every design vector y′y'y′. One universal function ϑ\varthetaϑ, independent of the instance, satisfies

ϑ(2)=π2,ϑ(4)=2,ϑ(μ)≤πμ/2(μ>2),\vartheta(2)=\frac\pi2,\qquad\vartheta(4)=2,\qquad \vartheta(\mu)\le\pi\sqrt{\mu/2}\quad(\mu>2),ϑ(2)=2π​,ϑ(4)=2,ϑ(μ)≤πμ/2​(μ>2),

and gives the tightness guarantee

¬Cy(ρ)⟹¬Ay(ϑ(μ)ρ).\neg\mathcal C_y(\rho)\Longrightarrow \neg\mathcal A_y(\vartheta(\mu)\rho).¬Cy​(ρ)⟹¬Ay​(ϑ(μ)ρ).

Finally, Cy(ρ)\mathcal C_y(\rho)Cy​(ρ) and Ay(ρ)\mathcal A_y(\rho)Ay​(ρ) are equivalent when there is a single block, or when all blocks are scalar and their coefficient matrices have rank at most one throughout the design space.

The supporting targets retain the book's numbering. Lemma 6.3.5(i) supplies the homogeneous S-Lemma. Theorem 8.2.3 supplies exact full-block reformulation. Both have compatible Proved references. Proposition B.4.12 concerns Gaussian products of Euclidean norms: its constants are π/4\pi/4π/4 in the complex case and 2/π2/\pi2/π in the real case, multiplying the Frobenius norms of the two matrices. Theorem 7.1.3 states the mixed scalar/full-block Matrix Cube Theorem, including safety, single-block exactness and a universal nondecreasing tightness function. These are source-numbered mathematical results, rather than a newly invented decomposition.

What the rank bound provides

The rank-sensitive estimate measures how far a feasible finite certificate can lag behind robust feasibility. Low-rank scalar coefficients give a dimension-independent factor, and the exactness clauses identify situations with no approximation loss. The guarantee concerns the specified uncertainty model: it does not assert that every robust semidefinite problem has a comparably tight finite reformulation.

The textbook already proves these mathematical results. This mission asks for their Lean formalization. Existing machine-checked homogeneous S-Lemma and full-perturbation results provide reusable references. The existing Open scalar-only Matrix Cube Theorem remains a separate published item; the present mixed-block target includes matrix perturbations and additional conclusions. No proof of a newly drafted theorem is claimed by the statement compilation checks.

Difficulty

Positive semidefiniteness must hold simultaneously in all vector directions and for every collection of uncertain blocks. Separate bounds on individual matrix entries do not express that requirement. The factor must also be uniform across all matrix dimensions and all affine families: proving a bound for one fixed design does not establish the theorem's global rank convention.

The two norm conventions are another source of error. Operator norms describe allowed perturbations, while Frobenius norms occur in the Gaussian estimate. Similarly, a standard complex Gaussian has independent real and imaginary parts of variance one half, so replacing it by unscaled real and imaginary standard normals would change the constants.

Formalization scope

All matrix dimensions are finite. The theorem statements make positive matrix and block sizes explicit, while scalar and full block counts can individually be zero. Designs are arbitrary real vectors and coefficient dependence is affine. The nominal matrix is assumed symmetric, not positive semidefinite in advance. Feasibility and certificate predicates are defined independently; no certificate equivalence or desired approximation bound is assumed as part of the data.

The definition modules provide reusable models for structured uncertainty, block domination, finite certificates and Gaussian norm products. The theorem declarations expand the same formulas within their statements so each blind read-back has the complete mathematical context. Positive semidefiniteness includes symmetry. The least uniform rank is specified by a least-element predicate, avoiding a real-valued supremum over an unbounded design space. Gaussian integrability is asserted alongside the expectation inequalities, rather than imposed as an additional assumption.

The chapter's control example, numerical trajectories and exercises are outside this capstone mission. The mixed-block supporting theorem is taken from Theorem 7.1.3; the appendix's differently oriented displayed certificate contains a rectangular dimension mismatch recorded in the local findings. The main theorem retains its printed constant, even though the appendix states a stronger upper bound. No corrected or strengthened variant is posed.

Selected references

  • A. Ben-Tal, L. El Ghaoui and A. Nemirovski, Robust Optimization, Princeton University Press, 2009. DOI. Goal: Theorem 9.1.2, printed pp. 225–226; supporting results: Lemma 6.3.5, Theorems 7.1.3 and 8.2.3, Proposition B.4.12.
  • L. El Ghaoui, F. Oustry and H. Lebret, “Robust Solutions to Uncertain Semidefinite Programs,” SIAM Journal on Optimization 9(1), 1998, pp. 33–52. DOI. The published full-perturbation lemma supplies the compatible exact certificate reference.
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Robust Optimization VII: Exact Robust LMIs with Norm-Bounded UncertaintyTextbook

Robust matrix constraints in design

A design constraint may require a symmetric matrix to remain positive semidefinite even when some of its coefficients are uncertain. Such constraints arise in the structural design problems discussed in Chapter 8 of Ben-Tal, El Ghaoui and Nemirovski, Robust Optimization. A design that satisfies a constraint at the nominal data can fail after a perturbation. The mathematical question is therefore whether the same design satisfies the matrix inequality throughout a specified uncertainty set.

A robust counterpart imposes the original constraint for every admissible perturbation. Even when each individual constraint is simple, the resulting family is generally infinite. This mission concerns one specific family for which the book gives an exact finite representation: a full rectangular matrix perturbation bounded in its Euclidean operator norm. The goal is Theorem 8.2.3, including its nonzero fixed-factor hypothesis and its semidefinite boundary cases.

Affine data and full matrix uncertainty

A real symmetric matrix MMM is positive semidefinite, written M⪰0M\succeq0M⪰0, when vTMv≥0v^TMv\ge0vTMv≥0 for every real vector vvv. A linear matrix inequality requires a symmetric matrix whose entries depend affinely on the decision variables to be positive semidefinite. Affine dependence permits both a constant term and a linear term.

Let y∈Rdy\in\mathbb R^dy∈Rd denote the design variables. The nominal matrix An(y)A^n(y)An(y) is a symmetric n×nn\times nn×n matrix, and L(y)L(y)L(y) is a p×np\times np×n matrix. Both depend affinely on yyy. The matrix R∈Rq×nR\in\mathbb R^{q\times n}R∈Rq×n is fixed and nonzero. A perturbation is any real p×qp\times qp×q matrix ζ\zetaζ satisfying ∥ζ∥2,2≤ρ\|\zeta\|_{2,2}\le\rho∥ζ∥2,2​≤ρ, where ρ>0\rho>0ρ>0 and the Euclidean operator norm measures the greatest expansion of a Euclidean unit vector. Full uncertainty means that no sparsity, diagonal, or block structure is imposed on ζ\zetaζ.

The perturbed matrix is

An(y)+L(y)TζR+RTζTL(y).A^n(y)+L(y)^T\zeta R+R^T\zeta^T L(y).An(y)+L(y)TζR+RTζTL(y).

The two perturbation terms are transposes of one another. Thus this expression is symmetric. This is the fixed-RRR orientation of Definition 8.2.1; the source permits interchanging the two factors when the other factor is constant. All these conventions come from §8.2.1, printed pp. 205–206.

Formalization targets

The supporting milestone is the homogeneous S-lemma, Lemma 6.3.5(i). For real symmetric matrices H,KH,KH,K of equal size, assuming xˉTHxˉ>0\bar x^TH\bar x>0xˉTHxˉ>0 for some xˉ\bar xxˉ, it states

[∀x, xTHx≥0⟹xTKx≥0]⟺[∃λ≥0, K−λH⪰0].\bigl[\forall x,\ x^THx\ge0\Longrightarrow x^TKx\ge0\bigr] \quad\Longleftrightarrow\quad \bigl[\exists\lambda\ge0,\ K-\lambda H\succeq0\bigr].[∀x, xTHx≥0⟹xTKx≥0]⟺[∃λ≥0, K−λH⪰0].

The published proved item ModernConvex.SLemma.s_lemma supplies this result. Only part (i) is a milestone: the source's proof of the selected capstone uses the homogeneous version.

The goal is the following equivalence for each design yyy:

∀ζ∈Rp×q,∥ζ∥2,2≤ρ⟹An(y)+L(y)TζR+RTζTL(y)⪰0⟺∃λ∈R,[λIpρL(y)ρL(y)TAn(y)−λRTR]⪰0.\begin{aligned} &\forall\zeta\in\mathbb R^{p\times q},\quad \|\zeta\|_{2,2}\le\rho\Longrightarrow A^n(y)+L(y)^T\zeta R+R^T\zeta^T L(y)\succeq0\\ &\quad\Longleftrightarrow\quad \exists\lambda\in\mathbb R,\quad \begin{bmatrix} \lambda I_p&\rho L(y)\\ \rho L(y)^T&A^n(y)-\lambda R^TR \end{bmatrix}\succeq0. \end{aligned}​∀ζ∈Rp×q,∥ζ∥2,2​≤ρ⟹An(y)+L(y)TζR+RTζTL(y)⪰0⟺∃λ∈R,[λIp​ρL(y)T​ρL(y)An(y)−λRTR​]⪰0.​

This is Theorem 8.2.3, equations (8.2.6)–(8.2.7), printed pp. 206–207. The existential multiplier is chosen for the design, independently of the perturbation. Equivalently, projecting the feasible set in (y,λ)(y,\lambda)(y,λ) onto yyy gives exactly the robust feasible set.

What exactness provides

The block inequality is affine in the joint variables (y,λ)(y,\lambda)(y,λ) because RRR is fixed. The theorem therefore replaces an infinite family of matrix constraints by one finite matrix inequality with one additional scalar variable. Both directions matter: a feasible certificate guarantees robustness, and every robustly feasible design admits a certificate. The result is stronger than a sufficient relaxation because it loses no feasible designs.

The mathematical theorem is already established in the textbook. The local draft states its exact affine form for a Lean proof. The S-lemma is already proved on Prove2Me, as is the related full linear-fractional perturbation lemma RobustSDP.FullPert.lemma_3_1. That reference includes feedback data and a unit-radius formulation; its relationship to the present statement requires a change of orientation and block coordinates. It is included as prior art rather than labeled as another numbered result from this chapter.

Difficulty at the semidefinite boundary

The constraint allows singular matrices. Replacing semidefiniteness by positive definiteness would discard designs permitted by the theorem. Likewise, a reformulation requiring a strictly positive multiplier would change the allowed boundary behavior. The difficult content is the existence of a single scalar certificate for all perturbations, with exactly the displayed block matrix, while retaining those boundaries. A check on a finite sample of perturbations does not establish this universal statement.

Formalization scope

All data are real and finite dimensional. Mathlib supplies matrices, transposes, multiplication, affine maps, identity matrices, block matrices, positive semidefiniteness, and the Euclidean operator norm. These existing definitions are used directly; no new definition layer is needed. Matrix indices use Fin, and the block matrix uses the disjoint sum of its two index sets. The row dimension ppp is positive. The nonzero condition on RRR already forces nnn and qqq to be positive. A zero design dimension represents constant affine data.

The nominal matrix is symmetric at every design. It need not be invertible, and L(y)L(y)L(y) may vanish. The multiplier is a real existential variable, with its sign constrained by the block inequality itself. Robust feasibility is an explicit universal statement over the norm ball; no certificate equivalence is assumed in a definition. Theorems 6.3.2 and Proposition 6.4.1 are precursor results, not additional targets of this capstone mission.

Beyond the paper. One sharpness probe removes only R≠0R\ne0R=0 from the faithful goal. Constant scalar data An=0A^n=0An=0, L=1L=1L=1, R=0R=0R=0, ρ=1\rho=1ρ=1 satisfy every perturbed original inequality, but the certificate is [λ110]\left[\begin{smallmatrix}\lambda&1\\1&0\end{smallmatrix}\right][λ1​10​], whose determinant is −1-1−1. Finding F1 records this evidence. The probe seeks a disproof and is neither the goal nor a milestone.

Selected references

  • A. Ben-Tal, L. El Ghaoui and A. Nemirovski, Robust Optimization, Princeton University Press, 2009. DOI 10.1515/9781400831050. Definition 8.2.1 and Theorem 8.2.3, printed pp. 205–207; Lemma 6.3.5(i), printed p. 164. The canonical PDF uses a 26-page offset.
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Robust Optimization V: Exact Robust Conic Quadratic ReformulationsTextbook

Robust constraints with finite certificates

An engineering decision often has to satisfy a bound even when some coefficients are known only within an uncertainty set. A robust counterpart requires the bound to hold for every allowed realization. For a norm constraint, this replaces a single inequality by an infinite family. The practical question is when that family has an exact finite representation that preserves the feasible decisions. Chapter 6 of Ben-Tal, El Ghaoui and Nemirovski, Robust Optimization identifies such representations for several uncertainty models. This mission concerns its unstructured norm-bounded model and Theorem 6.3.2.

The result is relevant when an uncertain matrix acts on a residual vector and the model specifies a bound on its largest singular value. It allows the robust constraint to be expressed through positive-semidefinite matrices and a conic certificate. The uncertainty model is consequential: independent uncertainty on the two sides is an explicit assumption, and the theorem does not claim the same formula for coupled perturbations.

Independent uncertainty on the two sides

The decision is a vector y∈Rny\in\mathbb R^ny∈Rn. The nominal residual is by=Any+bn∈Rkb_y=A^ny+b^n\in\mathbb R^kby​=Any+bn∈Rk, where AnA^nAn and bnb^nbn are fixed. The uncertain left side has one of two forms:

by+L(y)TηR,by+LTηR(y).b_y+L(y)^T\eta R,\qquad b_y+L^T\eta R(y).by​+L(y)TηR,by​+LTηR(y).

The dimensions ppp and qqq are positive. The matrix η\etaη ranges over all real p×qp\times qp×q matrices whose induced Euclidean operator norm is at most one. Equivalently, ∥ηu∥2≤∥u∥2\|\eta u\|_2\le\|u\|_2∥ηu∥2​≤∥u∥2​ for every vector uuu. In the first form L(y)L(y)L(y) is affine and RRR is fixed and nonzero. In the second, LLL is fixed and nonzero and R(y)R(y)R(y) is affine. The dimensions of LLL and RRR are p×kp\times kp×k and qqq, respectively.

The right side is σ(y)Tχ+δ(y)\sigma(y)^T\chi+\delta(y)σ(y)Tχ+δ(y), with affine functions σ\sigmaσ and δ\deltaδ. Its perturbation set is

Z={χ∈Rr:∃u∈Rs, Pχ+Qu+c∈K}.Z=\{\chi\in\mathbb R^r:\exists u\in\mathbb R^s,\ P\chi+Qu+c\in K\}.Z={χ∈Rr:∃u∈Rs, Pχ+Qu+c∈K}.

Here P,Q,cP,Q,cP,Q,c are fixed data. The set is closed under the standing convention in Section 5.1.2 (printed p. 151). The literal polyhedral branch does not explicitly require it to be nonempty; this omission is retained in the faithful goal and corrected in a separate companion. Either KKK is a closed convex pointed cone and this representation is strictly feasible, or KKK has an explicit finite homogeneous inequality representation. The source denotes the vector ccc by ppp; the new letter avoids confusing it with the row dimension of η\etaη. The perturbations η\etaη and χ\chiχ are chosen independently.

Formalization targets

The goal is the full equivalence in both parts of Theorem 6.3.2, at every decision yyy. Write

D(y,τ,v):τ+cTv≤δ(y),PTv=σ(y),QTv=0,v∈K∗,D(y,\tau,v):\quad \tau+c^Tv\le\delta(y),\quad P^Tv=\sigma(y),\quad Q^Tv=0,\quad v\in K^*,D(y,τ,v):τ+cTv≤δ(y),PTv=σ(y),QTv=0,v∈K∗,

where the dual cone is K∗={v:vTz≥0 for every z∈K}K^*=\{v:v^Tz\ge0\text{ for every }z\in K\}K∗={v:vTz≥0 for every z∈K}. In the first case, the target is

[∀η,χ admissible, ∥by+L(y)TηR∥2≤σ(y)Tχ+δ(y)]  ⟺  ∃τ,v,λ: D(y,τ,v) and M1⪰0,\bigl[\forall\eta,\chi\text{ admissible},\ \|b_y+L(y)^T\eta R\|_2\le\sigma(y)^T\chi+\delta(y)\bigr] \iff \exists\tau,v,\lambda:\ D(y,\tau,v)\ \text{and}\ M_1\succeq0,[∀η,χ admissible, ∥by​+L(y)TηR∥2​≤σ(y)Tχ+δ(y)]⟺∃τ,v,λ: D(y,τ,v) and M1​⪰0,

with

M1=(τIkL(y)TbyL(y)λIp0byT0τ−λRTR).M_1=\begin{pmatrix}\tau I_k&L(y)^T&b_y\\L(y)&\lambda I_p&0\\b_y^T&0&\tau-\lambda R^TR\end{pmatrix}.M1​=​τIk​L(y)byT​​L(y)TλIp​0​by​0τ−λRTR​​.

In the second case the analogous equivalence uses

M2=(τIk−λLTL0by0λIqR(y)byTR(y)Tτ).M_2=\begin{pmatrix}\tau I_k-\lambda L^TL&0&b_y\\0&\lambda I_q&R(y)\\b_y^T&R(y)^T&\tau\end{pmatrix}.M2​=​τIk​−λLTL0byT​​0λIq​R(y)T​by​R(y)τ​​.

These are the matrices on printed page 162, equations (6.3.4) and (6.3.5). Positive semidefiniteness, written M⪰0M\succeq0M⪰0, means that the symmetric matrix has nonnegative quadratic form on every vector.

The supporting targets retain the book's numbering: the conic representation in Theorem 1.3.4, the Lorentz-cone arrow representation in Lemma 6.3.3, and the Schur-complement and S-lemma results in Lemmas 6.3.4–6.3.5. The Schur-complement reference covers the positive-definite branch; Mathlib supplies the semidefinite branch. Both forms of the S-lemma have published proved references. The homogeneous S-lemma and inhomogeneous S-procedure are reused rather than posed again.

What the equivalence establishes

The result identifies exactly the original decisions that satisfy every uncertain inequality. The auxiliary variables describe a projection: their existence is equivalent to robust feasibility at that decision. It is therefore stronger than a sufficient conservative certificate. The nominal residual, the affine factor and the right-side coefficients remain arbitrary within the stated dimensions and assumptions.

The book states the equivalence. This mission preserves its literal hypotheses, including the empty-uncertainty omission recorded in finding F6. Consequently the faithful goal admits a disproof; a corrected companion adds nonempty right uncertainty and retains both equivalences. A successful statement build establishes type correctness; it is not a proof. The remaining theorem items are open formalization tasks, while the referenced S-lemma and positive-definite Schur-complement results already have machine-checked proofs. The finite block constructions can also serve later work on robust quadratic constraints with other uncertainty models.

Boundary cases and certificate attainment

Exactness must include feasible points on the boundary of the semidefinite cone. In particular, τ=0\tau=0τ=0 cannot be discarded or treated by assuming an inverse of τI\tau IτI. An argument restricted to positive τ\tauτ would leave part of the theorem unproved. The nonzero fixed factors and the right-side regularity assumptions also have distinct roles and must survive every reformulation.

The source proof contains two local typographical discrepancies recorded in the mission's findings: the sign of a displayed Schur-complement minimizer and a missing additive δ(y)\delta(y)δ(y) in equation (6.3.6.a). Neither discrepancy changes the theorem statements. A third proof gap is the use of a right-side minimum where only an infimum is guaranteed: the closed, strictly feasible set {(a,b):a,b≥0,ab≥1}\{(a,b):a,b\ge0,ab\ge1\}{(a,b):a,b≥0,ab≥1} has infimum zero for the objective bbb, without a minimizer (F7). Certificate attainment also matters: replacing an existential certificate with a limiting family would change the target.

Formalization scope

Coordinates use real function spaces indexed by finite sets, with explicit Euclidean norms ∑ixi2\sqrt{\sum_i x_i^2}∑i​xi2​​. Matrix uncertainty is defined by the contraction property, so the default supremum norm on function spaces never substitutes for the intended operator norm. The two LMI matrices are concrete block matrices, and robust feasibility is independently defined by universal quantification over the two adversaries. Certificate existence is not part of the definition of robustness. Affine maps encode dependence on the decision; there is no full-column-rank restriction on the conic data.

The perturbation dimensions p,qp,qp,q are positive, so the multiplier identity blocks retain their sign implications. Other coordinate spaces can have dimension zero. The nonzero hypotheses exclude impossible fixed-factor cases automatically. All scalar bounds and multipliers are real. There are no real infima, suprema, divisions or integrals whose default values could conceal infeasibility. The cone and dual-cone definitions are reused from the published ModernConvex conic-problem module. The new setup supplies the lifted set, regularity predicate, operator ball and the explicit matrices. Its regularity predicate includes closedness from Section 5.1.2; convexity follows from the lifted cone representation. Nonemptiness is an additional premise only of the corrected companions.

Beyond the paper. A corrected companion to Theorem 1.3.4 adds nonemptiness of the perturbation set. The literal polyhedral statement allows P=Q=0P=Q=0P=Q=0, c=−1c=-1c=−1, K=R+K=\mathbb R_+K=R+​, giving an empty set, while a nonzero uncertain right coefficient makes its certificate impossible. The faithful theorem remains the milestone; the correction is a separate item and is not the goal. This finding concerns the literal absence of a nonemptiness clause, rather than the common convention that an uncertainty set has realizations. The same issue affects Theorem 6.3.2 (F6): with the same empty right set and σ(y)=1\sigma(y)=1σ(y)=1, both robust conditions are vacuous, but PTv=σ(y)P^Tv=\sigma(y)PTv=σ(y) requires 0=10=10=1. A second corrected companion adds exactly nonempty right uncertainty to both cases. The literal theorem remains the goal, and neither companion is a milestone.

Selected references

  • A. Ben-Tal, L. El Ghaoui and A. Nemirovski, Robust Optimization, Princeton University Press, 2009. DOI. Theorem 1.3.4, printed p. 20; Theorem 6.3.2 and Lemmas 6.3.3–6.3.5, printed pp. 162–164.
  • A. Ben-Tal and A. Nemirovski, Lectures on Modern Convex Optimization, SIAM, 2001. DOI. Published formalizations supply the cone conventions and homogeneous S-lemma.
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Information TheoryQuantum InformationTheoretical Computer Science·Captain: mikedeng1

Improving the Security of Quantum Protocols via Commit-and-Open: After the Commit-and-Open Test, Any Dishonest Bob Is β-Benign Up to a Negligible Trace DistanceResearch Paper

Motivation

Many two-party quantum protocols, such as oblivious transfer and password-based identification, start the same way: Alice sends Bob nnn qubits ∣x⟩θ|x\rangle_\theta∣x⟩θ​ encoding random bits xxx in random BB84 bases θ∈{+,×}n\theta\in\{+,\times\}^nθ∈{+,×}n. Their security proofs work only against a restricted Bob, for example one with bounded quantum memory (Damgård, Fehr, Salvail, Schaffner 2005). Unrestricted security is impossible for such tasks in the plain model.

Damgård, Fehr, Lunemann, Salvail and Schaffner (arXiv:0902.3918, CRYPTO 2009) proposed a generic commit-and-open compiler. Bob commits to his measurement bases θ^\hat\thetaθ^ and outcomes x^\hat xx^ position by position. Alice opens a random fraction α\alphaα of the commitments and checks that xi=x^ix_i=\hat x_ixi​=x^i​ wherever her basis agreed with Bob's. Their headline result, Theorem 4.2, says that the compiled protocol is computationally secure against any polynomial-time Bob. Its proof reduces everything computational to one information-theoretic statement: after the test, a dishonest Bob is β-benign (Definition 4.1), up to a negligible error. The paper's introduction presents this statement as the new tool. This mission formalizes it.

Setting

Alice holds mmm qubits, one half of each of mmm EPR pairs, in a register A=C{0,1}mA=\mathbb C^{\{0,1\}^m}A=C{0,1}m. Bob holds an arbitrary finite-dimensional register EEE. The joint state right before the test is an arbitrary unit vector ∣φAE⟩∈HA⊗HE|\varphi_{AE}\rangle\in\mathcal H_A\otimes\mathcal H_E∣φAE​⟩∈HA​⊗HE​. This is the state after a dishonest Bob has received his halves and committed to x^∈{0,1}m\hat x\in\{0,1\}^mx^∈{0,1}m and θ^∈{+,×}m\hat\theta\in\{+,\times\}^mθ^∈{+,×}m.

The test is a pair (T,T′)(T,T')(T,T′). TTT is a uniformly random set of k=⌊αm⌋k=\lfloor\alpha m\rfloork=⌊αm⌋ positions; T′={i∈T:θi=θ^i}T'=\{i\in T:\theta_i=\hat\theta_i\}T′={i∈T:θi​=θ^i​} for Alice's uniform bases θ\thetaθ is a uniform subset of TTT. So PTest(T,T′)=1/((mk)2k)P_{Test}(T,T')=1/(\binom mk 2^k)PTest​(T,T′)=1/((km​)2k). In the analysed version of the protocol (Fig. 4), Alice measures the positions in TTT in Bob's bases θ^∣T\hat\theta|_Tθ^∣T​ and accepts iff xi=x^ix_i=\hat x_ixi​=x^i​ for all i∈T′i\in T'i∈T′. She then measures the remaining n=m−kn=m-kn=m−k positions in her bases θ∣Tˉ\theta|_{\bar T}θ∣Tˉ​, producing XXX.

The quantities of interest are:

  • the min-entropy H∞(X)=−log⁡2max⁡xPX(x)H_\infty(X)=-\log_2\max_xP_X(x)H∞​(X)=−log2​maxx​PX​(x) and its conditional version H∞(X∣I∣X∣Iˉ=x∣Iˉ)H_\infty(X|_I\mid X|_{\bar I}=x|_{\bar I})H∞​(X∣I​∣X∣Iˉ​=x∣Iˉ​);
  • the max-entropy H0(ρ)=log⁡2rank⁡ρH_0(\rho)=\log_2\operatorname{rank}\rhoH0​(ρ)=log2​rankρ;
  • the Hamming distance dHd_HdH​ and the relative distance rH=dH/lengthr_H=d_H/\text{length}rH​=dH​/length;
  • the trace distance δ(ρ,σ)=12tr⁡∣ρ−σ∣\delta(\rho,\sigma)=\tfrac12\operatorname{tr}|\rho-\sigma|δ(ρ,σ)=21​tr∣ρ−σ∣;
  • the binary entropy h(μ)=−(μlog⁡2μ+(1−μ)log⁡2(1−μ))h(\mu)=-(\mu\log_2\mu+(1-\mu)\log_2(1-\mu))h(μ)=−(μlog2​μ+(1−μ)log2​(1−μ)).

A function ν(m)\nu(m)ν(m) is negligible if ∣ν(m)∣≤m−c|\nu(m)|\le m^{-c}∣ν(m)∣≤m−c for every ccc and all large mmm.

The real cq state is ρTestAE=∑testPTest(test)∣test⟩⟨test∣⊗∣φAE⟩⟨φAE∣\rho_{TestAE}=\sum_{test}P_{Test}(test)|test\rangle\langle test|\otimes|\varphi_{AE}\rangle\langle\varphi_{AE}|ρTestAE​=∑test​PTest​(test)∣test⟩⟨test∣⊗∣φAE​⟩⟨φAE​∣. The set

Btest={x:rH(x∣Tˉ,x^∣Tˉ)≤rH(x∣T′,x^∣T′)+ε}B_{test}=\{x: r_H(x|_{\bar T},\hat x|_{\bar T})\le r_H(x|_{T'},\hat x|_{T'})+\varepsilon\}Btest​={x:rH​(x∣Tˉ​,x^∣Tˉ​)≤rH​(x∣T′​,x^∣T′​)+ε}

collects the outcomes whose error rate on the unopened positions is predicted by the error rate on T′T'T′.

Formalization targets

Goal: commit-and-open forces benign behaviour (§4.3, p. 12)

For every 0<α<10<\alpha<10<α<1 and β>0\beta>0β>0 there is a negligible ν\nuν such that, for every mmm, x^\hat xx^, θ^\hat\thetaθ^, finite EEE and unit ∣φAE⟩|\varphi_{AE}\rangle∣φAE​⟩, there are unit vectors ∣φ~AEtest⟩|\tilde\varphi^{test}_{AE}\rangle∣φ~​AEtest​⟩ with

δ(ρTestAE, ∑testPTest(test)∣test⟩⟨test∣⊗∣φ~AEtest⟩⟨φ~AEtest∣)≤ν(m),\delta\Big(\rho_{TestAE},\ \sum_{test}P_{Test}(test)|test\rangle\langle test|\otimes|\tilde\varphi^{test}_{AE}\rangle\langle\tilde\varphi^{test}_{AE}|\Big)\le\nu(m),δ(ρTestAE​, test∑​PTest​(test)∣test⟩⟨test∣⊗∣φ~​AEtest​⟩⟨φ~​AEtest​∣)≤ν(m),

and such that, in the ideal state, every branch Alice accepts satisfies the bounds (1) of Definition 4.1:

H∞(X∣I∣X∣Iˉ=x∣Iˉ)≥dH(θ∣I,θ^∣I)−βn,H0(ρER)≤βn.H_\infty\big(X|_I\mid X|_{\bar I}=x|_{\bar I}\big)\ge d_H(\theta|_I,\hat\theta|_I)-\beta n,\qquad H_0(\rho_{ER})\le\beta n.H∞​(X∣I​∣X∣Iˉ​=x∣Iˉ​)≥dH​(θ∣I​,θ^∣I​)−βn,H0​(ρER​)≤βn.

No constant is hard-coded; β\betaβ is arbitrary.

Milestones

  • Lemma 2.3: measuring a superposition of ∣J∣|J|∣J∣ product vectors loses at most log⁡∣J∣\log|J|log∣J∣ bits of min-entropy, and leaves Bob's register with rank at most ∣J∣|J|∣J∣.
  • The trace distance of pure states, 1−∣⟨ψ∣φ⟩∣2\sqrt{1-|\langle\psi|\varphi\rangle|^2}1−∣⟨ψ∣φ⟩∣2​.
  • The trace distance of two cq states over TestTestTest is the PTestP_{Test}PTest​-average of the branch distances.
  • The classical sampling bound: Pr⁡test[x∉Btest]\Pr_{test}[x\notin B_{test}]Prtest​[x∈/Btest​] is negligible, uniformly in xxx.
  • Lemma 4.3: ρTestAE\rho_{TestAE}ρTestAE​ is negligibly close to a state each of whose branches is supported on BtestB_{test}Btest​ in Bob's basis.
  • The Hamming-ball bound ∣{y:dH(y,y^)≤μn}∣≤2h(μ)n|\{y:d_H(y,\hat y)\le\mu n\}|\le2^{h(\mu)n}∣{y:dH​(y,y^​)≤μn}∣≤2h(μ)n for 0≤μ≤120\le\mu\le\tfrac120≤μ≤21​.
  • Corollary 4.4: on such a branch, H∞≥dH−h(err+ε)nH_\infty\ge d_H-h(err+\varepsilon)nH∞​≥dH​−h(err+ε)n and H0≤h(err+ε)nH_0\le h(err+\varepsilon)nH0​≤h(err+ε)n, where errerrerr is the error rate on T′T'T′.

Significance

The goal is what makes the compiler work. Combined with the security of the original protocol against benign Bob, it turns any BB84-type protocol that is secure in a restricted model into one secure against arbitrary dishonest Bob in the computational setting. The paper derives oblivious transfer and password-based identification this way (§6). The same statement also preserves bounded-quantum-storage security (§5.2). Its quantitative form, β=h(err+ε)\beta=h(err+\varepsilon)β=h(err+ε), shows how noise tolerance enters (§5.1).

The paper's headline Theorem 4.2 is computational: it quantifies over polynomial-time quantum adversaries and simulators in the common-reference-string model, with a dual-mode commitment scheme specified in prose. That wrapper is out of scope. The unconditional core claim, closing §4.3, is a statement about finite-dimensional states, entropies and a sampling distribution. To our knowledge no machine-checked proof of it, of Lemma 4.3, or of Corollary 4.4 exists. Formalizing it also produces reusable pieces: min- and max-entropy of superpositions, trace distance of pure and cq states, and a sampling bound for random subsets.

Difficulty

The statement mixes a quantum and a classical argument, and neither carries the whole weight. The obvious attempt, applying an entropic uncertainty relation directly to Bob's state, fails: Bob's register may be entangled with all of Alice's qubits, so nothing bounds its rank a priori. The bound appears only after the real state is replaced by a nearby one, and that replacement must be uniform over Bob's register and strategy. Uniformity is the delicate point: the negligible function must not depend on mmm, x^\hat xx^, θ^\hat\thetaθ^ or the state.

The sampling step concerns sampling without replacement (TTT of fixed size), followed by an independent subsample T′T'T′ that can be empty. The entropy bounds then need the Hamming-ball estimate at the real radius (err+ε)n(err+\varepsilon)n(err+ε)n, valid only up to 12\tfrac1221​.

Formalization scope

  • Registers are C{0,1}m\mathbb C^{\{0,1\}^m}C{0,1}m (EuclideanSpace ℂ (Fin m → Bool)) and CE\mathbb C^ECE for a finite type E. Joint states are unit vectors of the product. The joint state is pure, which the paper argues is without loss of generality: a mixed state is purified and the purifier joins EEE.
  • Bits are Bool; bases are Bool with false = +++, true = ×\times×. Positions are 0-based Fin m.
  • ∣T∣=⌊αm⌋|T|=\lfloor\alpha m\rfloor∣T∣=⌊αm⌋ and n=m−⌊αm⌋n=m-\lfloor\alpha m\rfloorn=m−⌊αm⌋; these match the paper's αm\alpha mαm and (1−α)m(1-\alpha)m(1−α)m whenever αm\alpha mαm is an integer.
  • log⁡=log⁡2\log=\log_2log=log2​. hhh is Mathlib's Real.binEntropy divided by ln⁡2\ln2ln2. The trace norm is the published WildeQIT.traceNorm, and the trace distance carries the factor 12\tfrac1221​.
  • Alice's two measurements (in θ^\hat\thetaθ^ on TTT, in θ\thetaθ on Tˉ\bar TTˉ) are encoded as one measurement in the mixed basis. Conditional min-entropies condition on x∣Tx|_Tx∣T​ as well.
  • Bob's post-measurement state is kept unnormalized, which leaves its rank unchanged. Statements that condition on an outcome assume it has positive probability.
  • rHr_HrH​ on the empty set is 000.
  • Corollary 4.4 assumes err+ε≤12err+\varepsilon\le\tfrac12err+ε≤21​. The printed err≤12err\le\tfrac12err≤21​ is not sufficient: at err=ε=12err=\varepsilon=\tfrac12err=ε=21​ the conclusion fails. The goal is unaffected.
  • The ideal vectors in the goal depend on the test only, and one ν\nuν serves all mmm, x^\hat xx^, θ^\hat\thetaθ^, EEE and states. Neither conclusion is trivial on its own: taking the ideal state equal to the real one gives distance 000, and taking it to be the honest state ∣x^⟩θ^⊗∣e⟩|\hat x\rangle_{\hat\theta}\otimes|e\rangle∣x^⟩θ^​⊗∣e⟩ satisfies (1). The goal demands both at once.

Contributions are welcome on any milestone. The sampling bound and the pure-state and block-diagonal trace-distance identities are independent of the rest. The trace-norm lemmas and the Hamming-ball bound are useful beyond this mission.

Selected references

  • I. Damgård, S. Fehr, C. Lunemann, L. Salvail, C. Schaffner, Improving the Security of Quantum Protocols via Commit-and-Open, CRYPTO 2009; arXiv:0902.3918v4. https://arxiv.org/abs/0902.3918
  • I. Damgård, S. Fehr, L. Salvail, C. Schaffner, Cryptography in the Bounded Quantum-Storage Model, FOCS 2005. https://arxiv.org/abs/quant-ph/0508222
  • W. Hoeffding, Probability Inequalities for Sums of Bounded Random Variables, J. Amer. Statist. Assoc. 58 (1963). https://doi.org/10.1080/01621459.1963.10500830
  • S. Fehr, C. Schaffner, Composing Quantum Protocols in a Classical Environment, TCC 2009. https://arxiv.org/abs/0804.1059
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Differential GeometryMathematical Physics·Captain: mikedeng1

Optics of Nonuniformly Moving Media: Light Rays in a Moving Dielectric Are Null Geodesics of Gordon's Optical MetricResearch Paper

Motivation

The path of a light beam changes when the transparent material through which it travels moves. This matters when interpreting light bending and phase shifts around a flowing liquid, and when asking whether a dielectric can imitate some effects of curved spacetime. Leonhardt and Piwnicki gave a geometrical-optics treatment of a moving, nondispersive dielectric and related its ray dynamics to a spacetime metric in their 1999 paper. This mission isolates their statement that light rays are null geodesics of that metric. Their treatment also connects this geometric picture to a Hamiltonian, a Lagrangian with an artificial mass, and a raised wave vector tangent to the ray. The physical model assumes that the refractive index and flow change gradually over an optical wavelength and cycle; the mission starts with the resulting local optical data rather than claiming an error estimate for that approximation.

Setting

A nondispersive dielectric has a refractive index nnn that is independent of optical frequency. Let c>0c>0c>0 denote the vacuum speed of light, and let u∈R3u\in\mathbb R^3u∈R3 be the velocity of the material at an event, with ∣u∣<c|u|<c∣u∣<c. The paper uses n≥1n\geq1n≥1. The four-flow is U=γ(1,u/c)U=\gamma(1,u/c)U=γ(1,u/c), where γ=(1−∣u∣2/c2)−1/2\gamma=(1-|u|^2/c^2)^{-1/2}γ=(1−∣u∣2/c2)−1/2; spacetime coordinates are (x0,x1,x2,x3)(x^0,x^1,x^2,x^3)(x0,x1,x2,x3) with x0=ctx^0=ctx0=ct. The flat metric is η=diag⁡(1,−1,−1,−1)\eta=\operatorname{diag}(1,-1,-1,-1)η=diag(1,−1,−1,−1).

Gordon's optical metric has contravariant and covariant matrices

gμν=ημν+(n2−1)UμUν,gμν=ημν+(n−2−1)UμUν.g^{\mu\nu}=\eta^{\mu\nu}+(n^2-1)U^\mu U^\nu,\qquad g_{\mu\nu}=\eta_{\mu\nu}+(n^{-2}-1)U_\mu U_\nu.gμν=ημν+(n2−1)UμUν,gμν​=ημν​+(n−2−1)Uμ​Uν​.

The second matrix is the inverse of the first in the physical regime §III.B–C, equations (31), (42)–(43). A wave has laboratory frequency ω\omegaω and spatial wave vector kkk; its covariant wave vector is kν=(ω/c,−k)k_\nu=(\omega/c,-k)kν​=(ω/c,−k). The eikonal null equation gμνkμkν=0g^{\mu\nu}k_\mu k_\nu=0gμνkμ​kν​=0 becomes the dispersion relation ω2−c2∣k∣2+(n2−1)γ2(ω−u⋅k)2=0\omega^2-c^2|k|^2+(n^2-1)\gamma^2(\omega-u\cdot k)^2=0ω2−c2∣k∣2+(n2−1)γ2(ω−u⋅k)2=0. The paper solves it for its positive comoving-frequency branch ω=H(k)\omega=H(k)ω=H(k) and defines the laboratory ray velocity v=∇kH(k)v=\nabla_kH(k)v=∇k​H(k). A ray parametrized by laboratory time has tangent (c,v)(c,v)(c,v), since x0=ctx^0=ctx0=ct §III.B, equations (28)–(36).

Formalization targets

The goal is the existing Open platform theorem QAlgorithms.Papers.Independent.Renew46.P42.rays_nullGeodesic, posed from §III.D, equations (50)–(51). For a twice continuously differentiable optical patch with n≥1n\geq1n≥1 and subluminal flow, and a ray satisfying both Hamilton equations with k≠0k\ne0k=0, it asserts at every point of the ray

gμνq˙μq˙ν=0,∇q˙q˙=aq˙for some scalar a.g_{\mu\nu}\dot q^\mu\dot q^\nu=0,\qquad \nabla_{\dot q}\dot q=a\dot q\quad\text{for some scalar }a.gμν​q˙​μq˙​ν=0,∇q˙​​q˙​=aq˙​for some scalar a.

The scalar aaa allows laboratory time to be a nonaffine parameter. The goal also includes the local-rest-frame identity

gμν(Λv)μ(Λv)ν=v02n2−(v12+v22+v32),g_{\mu\nu}(\Lambda v)^\mu(\Lambda v)^\nu=\frac{v_0^2}{n^2}-(v_1^2+v_2^2+v_3^2),gμν​(Λv)μ(Λv)ν=n2v02​​−(v12​+v22​+v32​),

where Λ\LambdaΛ takes a displacement vvv from the medium's rest frame to the laboratory frame. The milestones follow the paper's path: the polarization-independent wave symbol, the dispersion polynomial, the Hamiltonian and its comoving light speed, the inverse metric, the massive action, the rest-frame line element, the zero proper time of the ray tangent, and the tangent relation for the raised wave vector. Three of these are new draft statements; the remaining five are published platform references. The rest-frame milestone is the pointwise form of the goal's second conjunct.

Significance

The result identifies the same rays through two descriptions: Hamiltonian trajectories in a moving dielectric and null curves of a Lorentzian optical metric. It fixes which metric acts on covectors and which acts on tangent vectors, and it makes the rest-frame speed c/nc/nc/n visible in the line element. These identifications support the paper's later discussion of phase shifts and vortex flows §IV. Without the null-geodesic link, those later geometric analogies have no stated connection to the ray Hamiltonian.

The formalization work is still open even though the paper's result is known. The platform already has the shared definitions and six relevant theorem statements: three milestones are Proved, while the Hamiltonian characterization, the massive-action result, and the null-geodesic goal are Open. This proposal adds three local statements around equations (33) and (51) and the vanishing proper time. It does not duplicate the existing Open goal. A complete checked development would connect the local identities to the differential-geometric conclusion for rays in varying media.

Difficulty

The pointwise null identity is shorter than the geodesic conclusion. A ray velocity is a gradient of a Hamiltonian containing square roots, and its coordinates are defined only on the nonzero wave-vector branch used here. The full goal then has to relate Hamilton's time-parametrized equations to the Levi-Civita acceleration of a metric whose coefficients vary with position and time. A pointwise null calculation alone does not establish that the covariant acceleration is parallel to the tangent. The distinction between a covector kνk_\nukν​ and its raised vector kμk^\mukμ, together with the spatial minus sign in kν=(ω/c,−k)k_\nu=(\omega/c,-k)kν​=(ω/c,−k), is essential: using the wrong variance changes the dispersion relation and the tangent statement.

Formalization scope

The Lean model uses real coordinate vectors indexed by Fin 3 and Fin 4, real 4×44\times44×4 matrices, and the published module QAlgorithms_Papers_Independent_Renew46_P42. Its functions gUp, gDown, fourFlow, waveCovector, lorentzBoost, rayDispersion, rayHamiltonian, and rayVelocity are shared by the goal and every new draft. quadratic comes from the module's published dependency. The boost is the identity at zero flow. The ray tangent is (c,v1,v2,v3)(c,v_1,v_2,v_3)(c,v1​,v2​,v3​) in coordinates x0=ctx^0=ctx0=ct. Positive comoving frequency selects the Hamiltonian branch; laboratory frequency itself need not be positive.

The conditions c>0c>0c>0, n≥1n\geq1n≥1, and ∣u∣<c|u|<c∣u∣<c make the physical regime explicit. The zero-proper-time milestone also requires k≠0k\ne0k=0, where the Hamiltonian gradient represents a ray direction. The optical patch in the goal has an open domain and twice continuously differentiable index and flow. The ray has the stated regularity and satisfies both Hamilton equations on an open time set. The local null milestone has nonempty physical instances, rather than relying on a junk square-root value or zero wave vector. The curve-level goal is a universal implication and is vacuous when its open time set is empty. The paper's phrase about minimizing proper time is treated as a local null and pregeodesic claim, without a global minimizing assertion for Lorentzian length.

Reusable contributions include coordinate lemmas for the two Gordon metrics, Lorentz boosts, differentiation of the ray Hamiltonian, and the relation between Hamiltonian motion and covariant acceleration. The wave equation's slow-variation approximation, polarization transport, curvature formula, and vortex applications lie outside this mission's target.

Selected references

  • U. Leonhardt and P. Piwnicki, Optics of Nonuniformly Moving Media, Physical Review A 60, 4301–4312 (1999), pinned preprint arXiv:physics/9906038v3.
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Information TheoryMathematical PhysicsQuantum Information·Captain: mikedeng1

Capacities of Quantum Channels for Massive Bosons and Fermions: Under Average Energy and Particle-Number Constraints the Capacity Is the Grand-Canonical Entropy, Attained by Fock StatesResearch Paper

Motivation

Classical information can be sent by choosing a quantum state, transmitting it, and asking a receiver to measure it. An ideal noiseless channel seems to have no finite information limit if its carrier can occupy arbitrarily many quantum states. A physical carrier, however, has a limited average energy, and a channel carrying massive particles also has a limited average particle number. Sen(De), Sen, Gromek, Bruß, and Lewenstein ask for the greatest information transfer compatible with both constraints. Their answer connects the channel's information capacity to the entropy of the grand-canonical ensemble familiar from statistical mechanics. Sen(De) et al., pp. 1–2.

The paper also studies how capacities of Bose and Fermi systems respond to condensation and pairing. This mission concerns the result that supports those comparisons: the capacity formula for an ideal, noiseless channel under fixed average energy and particle number. Its finite-dimensional form gives a precise setting in which the optimization and its attaining ensemble can both be stated. Sen(De) et al., pp. 2–4.

Setting

The carrier has a finite-dimensional complex state space. Its Hamiltonian H\mathcal HH assigns energy, and its number operator N^\hat NN^ counts particles. The two Hermitian operators commute, so the system has an orthonormal basis of states with definite energy and particle number. These are the Fock states used as signals. For inverse temperature β\betaβ and chemical potential μ\muμ, the grand-canonical state is

ρGCE=exp⁡[−β(H−μN^)]Z,Z=tr⁡exp⁡[−β(H−μN^)].\rho_{\mathrm{GCE}}=\frac{\exp[-\beta(\mathcal H-\mu\hat N)]}{Z}, \qquad Z=\operatorname{tr}\exp[-\beta(\mathcal H-\mu\hat N)].ρGCE​=Zexp[−β(H−μN^)]​,Z=trexp[−β(H−μN^)].

A sender chooses one state ρi\rho_iρi​ from a finite ensemble E={(pi,ρi)}\mathcal E=\{(p_i,\rho_i)\}E={(pi​,ρi​)} with probability pip_ipi​. Each state may be mixed. The mean state is ρˉ=∑ipiρi\bar\rho=\sum_i p_i\rho_iρˉ​=∑i​pi​ρi​. A receiver chooses a finite quantum measurement and observes its outcome. The accessible information Iacc(E)I_{\mathrm{acc}}(\mathcal E)Iacc​(E) is the largest mutual information between the sender's label and the receiver's outcome among these measurements. The Holevo quantity is χ(E)=S(ρˉ)−∑ipiS(ρi)\chi(\mathcal E)=S(\bar\rho)-\sum_i p_iS(\rho_i)χ(E)=S(ρˉ​)−∑i​pi​S(ρi​), where SSS is von Neumann entropy. All information and entropy values use base-two logarithms, so their units are bits. Sen(De) et al., p. 1.

Fix EEE and NNN. An ensemble is admissible when its mean state obeys the two exact constraints tr⁡(ρˉH)=E\operatorname{tr}(\bar\rho\mathcal H)=Etr(ρˉ​H)=E and tr⁡(ρˉN^)=N\operatorname{tr}(\bar\rho\hat N)=Ntr(ρˉ​N^)=N. The paper defines CE,NC_{E,N}CE,N​ as the maximum accessible information among admissible ensembles. For the theorem here, EEE and NNN are the expectations of H\mathcal HH and N^\hat NN^ in ρGCE\rho_{\mathrm{GCE}}ρGCE​; no claim of a global inverse from (E,N)(E,N)(E,N) to (β,μ)(\beta,\mu)(β,μ) is needed. Sen(De) et al., p. 2.

Formalization targets

The first targets are the paper's entropy bounds: the Holevo bound Iacc(E)≤χ(E)I_{\mathrm{acc}}(\mathcal E)\leq\chi(\mathcal E)Iacc​(E)≤χ(E) and χ(E)≤S(ρˉ)\chi(\mathcal E)\leq S(\bar\rho)χ(E)≤S(ρˉ​). The grand-canonical variational principle says that, under the two fixed expectations, no state has greater entropy than ρGCE\rho_{\mathrm{GCE}}ρGCE​. The first and third targets correspond to existing Open platform statements; the second is drafted here. Sen(De) et al., pp. 1–2.

The goal combines the value of the capacity with its attainment:

CE,N=S(ρGCE),Iacc(EFock)=CE,N,C_{E,N}=S(\rho_{\mathrm{GCE}}), \qquad I_{\mathrm{acc}}(\mathcal E_{\mathrm{Fock}})=C_{E,N},CE,N​=S(ρGCE​),Iacc​(EFock​)=CE,N​,

where EFock\mathcal E_{\mathrm{Fock}}EFock​ consists of joint energy and number eigenstates with probabilities supplied by ρGCE\rho_{\mathrm{GCE}}ρGCE​. Two further milestones record that this ensemble has mean ρGCE\rho_{\mathrm{GCE}}ρGCE​ and that orthogonal pure signals make their classical label information accessible to a measurement. The goal includes an actual maximizing ensemble; an equality involving a supremum alone would leave the paper's attainment claim unstated. Sen(De) et al., p. 2 and abstract.

Significance

The result turns a channel optimization over encodings and measurements into a thermodynamic quantity, while specifying signals that reach the bound. The second constraint matters: energy by itself selects a canonical ensemble, whereas fixed average energy together with fixed average particle number selects a grand-canonical ensemble in the paper's setting. This is the connection the authors use when comparing massive Bose and Fermi carriers. Sen(De) et al., pp. 1–2.

A formalization would add a reusable statement linking three kinds of objects: operational accessible information, entropy maximization with conserved quantities, and a concrete optimal ensemble. The shared quantum definitions already exist on the platform; the Holevo and grand-canonical variational statements are Open goals, rather than machine-checked results claimed by this mission. The present draft has compile-checked statements, not proofs of the capacity theorem or those Open goals.

Difficulty

The accessible information is itself an optimization over measurements, while capacity optimizes it again over every admissible ensemble. Merely diagonalizing the grand-canonical state does not establish that no other ensemble, including an ensemble of mixed or noncommuting states, carries more accessible information. The matching attainment assertion also needs an ensemble of the paper's Fock states that obeys both average constraints. The comparison must use the same bit-valued entropy convention throughout, even though one existing grand-canonical platform theorem states its variational principle using natural logarithms.

Formalization scope

Lean represents states and observables by complex matrices indexed by a finite nonempty type, with H\mathcal HH and N^\hat NN^ Hermitian and commuting. The grand-canonical state uses the published Gibbs-state definition. Expected values are real parts of traces, and both constraints are equalities. The finite-dimensional model is exact for finitely many fermionic levels; it is a truncation of the unbounded bosonic Fock space, so this mission does not claim the paper's infinite-dimensional bosonic formula. The theorem permits every real β\betaβ and μ\muμ, with EEE and NNN defined from the resulting state.

The capacity domain includes all finite ensemble sizes and arbitrary mixed density matrices, and accessible information optimizes over all finite POVMs. Restricting the ensemble to Fock-diagonal or pure states, fixing its label type to the Fock basis, or fixing the measurement would turn the capacity claim into a different problem. The maximum is expressed as a greatest element of the value set, which records membership and hence attainment. The reusable work includes the ensemble entropy bound, the joint-eigenbasis interface, and the link between orthogonal signals and accessible information. Contributions that establish these links for the stated definitions or connect the existing Open reference theorems to this interface fit the mission. The paper's separately labelled comparison theorem for bosons and fermions, its asymptotic expansions, and its numerical figures are outside this mission.

Selected references

  • A. Sen(De), U. Sen, B. Gromek, D. Bruß, and M. Lewenstein, Capacities of Quantum Channels for Massive Bosons and Fermions, Physical Review Letters 2005; pinned preprint arXiv:quant-ph/0505028v2, 2006. arXiv
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AlgebraLinear algebraOptimization·Captain: mikedeng1

Invariant Semidefinite Programs: Every Matrix ∗-Algebra Is ∗-Isomorphic to a Direct Sum of Full Matrix AlgebrasResearch Paper

Motivation

Semidefinite programs that arise in coding theory, extremal geometry, crossing-number bounds and polynomial optimization are often too large to solve directly, but they are invariant under a large symmetry group. Restricting the matrix variable to the invariant matrices loses nothing, and the invariant matrices form a matrix ∗-algebra. The survey of Bachoc, Gijswijt, Schrijver and Vallentin (arXiv:1007.2905, published in the Handbook on Semidefinite, Conic and Polynomial Optimization, Springer, 2012) organizes this symmetry reduction into steps. Its Step 2 (§1.2, pp. 5–7) replaces an SDP over such an algebra by an SDP over a few small blocks, and the justification of that step is a single structure theorem: every matrix ∗-algebra is ∗-isomorphic to a direct sum of full matrix algebras (Theorem 1.2, restated as Theorem 2.7 on p. 13).

The theorem is classical. It is the finite-dimensional case of the structure theory of C∗-algebras (Davidson, C∗-Algebras by Example, Chapter I.10), and in the unital, non-star form it is the Wedderburn–Artin theorem for semisimple algebras over ℂ. Its use in SDP symmetry reduction goes back to Gatermann and Parrilo (2004) and de Klerk, Pasechnik and Schrijver (2007). Section 2.5 of the survey gives a short, elementary, self-contained proof using only linear algebra; this mission follows that proof.

Setting

A matrix ∗-algebra (Definition 2.1, p. 10) is a complex linear subspace A⊆Cn×n\mathcal A \subseteq \mathbb C^{n\times n}A⊆Cn×n that is closed under matrix multiplication and under the conjugate transpose X↦X∗X \mapsto X^*X↦X∗. It need not contain the identity matrix, and it may be {0}\{0\}{0}.

A map φ:A→B\varphi : \mathcal A \to \mathcal Bφ:A→B between matrix ∗-algebras is a ∗-homomorphism (Definition 2.6, p. 13) if it is linear, satisfies φ(XY)=φ(X)φ(Y)\varphi(XY) = \varphi(X)\varphi(Y)φ(XY)=φ(X)φ(Y) and φ(X∗)=φ(X)∗\varphi(X^*) = \varphi(X)^*φ(X∗)=φ(X)∗; a bijective ∗-homomorphism is a ∗-isomorphism. The direct sum ⨁k=1dCmk×mk\bigoplus_{k=1}^d \mathbb C^{m_k\times m_k}⨁k=1d​Cmk​×mk​ is the algebra of block-diagonal matrices with diagonal blocks of sizes m1,…,mdm_1, \dots, m_dm1​,…,md​ (p. 10).

The proof uses the following vocabulary (p. 13). The center of A\mathcal AA is CA={Z∈A:ZX=XZ for all X∈A}\mathcal C_{\mathcal A} = \{Z \in \mathcal A : ZX = XZ \text{ for all } X \in \mathcal A\}CA​={Z∈A:ZX=XZ for all X∈A}. The unit of A\mathcal AA is the unique E∈AE \in \mathcal AE∈A with EX=XE=XEX = XE = XEX=XE=X for all X∈AX \in \mathcal AX∈A. A\mathcal AA is simple if it is non-zero and CA=CE\mathcal C_{\mathcal A} = \mathbb C ECA​=CE. For a partition [n]=S0∪S1∪⋯∪Sk[n] = S_0 \cup S_1 \cup \dots \cup S_k[n]=S0​∪S1​∪⋯∪Sk​, IiI_iIi​ is the zero-one diagonal matrix with ones in the positions of SiS_iSi​.

Formalization targets

Goal: Theorem 2.7 (= Theorem 1.2), p. 13

For every matrix ∗-algebra A⊆Cn×n\mathcal A \subseteq \mathbb C^{n\times n}A⊆Cn×n there are ddd and m1,…,mdm_1, \dots, m_dm1​,…,md​ and a ∗-isomorphism

φ:A⟶⨁k=1dCmk×mk.\varphi : \mathcal A \longrightarrow \bigoplus_{k=1}^d \mathbb C^{m_k\times m_k}.φ:A⟶k=1⨁d​Cmk​×mk​.

The goal fixes no sizes: it asserts only the existence of the block structure, which is the form Step 2 uses.

Milestones, in the order of the paper's proof

  1. Theorem 2.2 (p. 11): a commutative matrix ∗-algebra is unitarily similar to {λ1I1+⋯+λkIk:λi∈C}\{\lambda_1 I_1 + \dots + \lambda_k I_k : \lambda_i \in \mathbb C\}{λ1​I1​+⋯+λk​Ik​:λi​∈C} for a partition with S1,…,SkS_1, \dots, S_kS1​,…,Sk​ nonempty and S0S_0S0​ possibly empty.
  2. A maximal commutative ∗-subalgebra B\mathcal BB of A\mathcal AA contains every element of A\mathcal AA that commutes with B\mathcal BB (p. 14).
  3. Observations (i)–(ii) (p. 14): with B\mathcal BB in diagonal form, for X∈AX \in \mathcal AX∈A each IiXIiI_iXI_iIi​XIi​ is a multiple of IiI_iIi​, and I0X=XI0=0I_0X = XI_0 = 0I0​X=XI0​=0.
  4. Observation (iii) (p. 14): each block IiXIjI_iXI_jIi​XIj​ is zero or a nonzero multiple of a square unitary matrix.
  5. The unit of A\mathcal AA exists and is unique (p. 13).
  6. The relation i∼j  ⟺  IiAIj≠{0}i \sim j \iff I_i\mathcal A I_j \neq \{0\}i∼j⟺Ii​AIj​={0} is an equivalence relation (p. 14).
  7. A=⨁i=1dEiA\mathcal A = \bigoplus_{i=1}^d E_i\mathcal AA=⨁i=1d​Ei​A, where E1,…,EdE_1, \dots, E_dE1​,…,Ed​ are the minimal idempotents of CA\mathcal C_{\mathcal A}CA​ and each EiAE_i\mathcal AEi​A is simple (p. 14).
  8. Every simple matrix ∗-algebra is ∗-isomorphic to a full matrix algebra Ck×k\mathbb C^{k\times k}Ck×k (p. 14, proved pp. 14–15).

Milestones 7 and 8 together give the goal.

Significance

The result. A ∗-isomorphism preserves positive semidefiniteness, so Theorem 2.7 turns the constraint "X∈AX \in \mathcal AX∈A, X⪰0X \succeq 0X⪰0" into ddd independent constraints on blocks of sizes m1,…,mdm_1, \dots, m_dm1​,…,md​, with ∑kmk2=dim⁡A\sum_k m_k^2 = \dim \mathcal A∑k​mk2​=dimA. This is what makes the Lovász ϑ-number of symmetric graphs, the Delsarte and Schrijver bounds for codes, and the crossing-number bound of de Klerk et al. computable at scale (§§4–6 of the survey). Without it, an invariant SDP still has a variable of the original size nnn.

Formalizing it. The theorem is proved and textbook material; it is not open. As far as a search of the platform shows, it is not formalized in this form: Mathlib has Wedderburn–Artin for semisimple unital algebras over an algebraically closed field, which yields an algebra isomorphism but neither the star structure nor the non-unital case, and the platform holds a proved matrix-units statement for unital ∗-subalgebras (HarlowTASI.fdStarAlgebra_exists_matrixUnits, attached to this mission as a reference). The mission adds the non-unital ∗-isomorphism, the simultaneous unitary diagonalization of a commutative matrix ∗-algebra, and the intermediate facts of the elementary proof, each stated in a reusable form.

Difficulty

Two points make the obvious routes insufficient. First, a matrix ∗-algebra need not contain the identity: its unit is a projection onto a subspace, and the coordinates in S0S_0S0​ carry no part of the algebra. Statements and arguments that start from a unital subalgebra do not apply without first cutting the algebra down to the range of its unit. Second, an algebra isomorphism onto a product of matrix algebras is not enough: the isomorphism must commute with the conjugate transpose, since positive semidefiniteness is defined through it. Abstract Wedderburn–Artin provides the first kind of isomorphism, and turning it into a ∗-isomorphism requires choosing the matrix units compatibly with the adjoint, which is where the content of the theorem lies. The elementary proof avoids ring theory entirely but has to control every off-diagonal block IiXIjI_iXI_jIi​XIj​, which is the role of observations (i)–(iii).

Formalization scope

  • A matrix ∗-algebra is NonUnitalStarSubalgebra ℂ (Matrix (Fin n) (Fin n) ℂ); Mathlib's star on matrices is the conjugate transpose. The index set [n][n][n] is Fin n (0-based).
  • A ∗-isomorphism is StarAlgEquiv ℂ (≃⋆ₐ[ℂ]) on the subtype of A\mathcal AA: additive, multiplicative, ℂ-linear, star-preserving and bijective, exactly Definition 2.6.
  • ⨁k=1dCmk×mk\bigoplus_{k=1}^d \mathbb C^{m_k\times m_k}⨁k=1d​Cmk​×mk​ is the product type (k : Fin d) → Matrix (Fin (m k)) (Fin (m k)) ℂ with pointwise operations and star; it is ∗-isomorphic to the block-diagonal algebra (Matrix.blockDiagonal'). d=0d = 0d=0 is allowed and is needed for A={0}\mathcal A = \{0\}A={0}.
  • A partition [n]=S0∪S1∪⋯∪Sk[n] = S_0 \cup S_1 \cup \dots \cup S_k[n]=S0​∪S1​∪⋯∪Sk​ is a map S : Fin n → Option (Fin k), with none for S0S_0S0​ and some i for Si+1S_{i+1}Si+1​; the paper's block AijA_{ij}Aij​ is represented by the full-size product IiXIjI_iXI_jIi​XIj​.
  • The center is the set of elements of A\mathcal AA commuting with A\mathcal AA, not the commutant in Cn×n\mathbb C^{n\times n}Cn×n. "Simple" is the paper's definition: non-zero, with center CE\mathbb C ECE for the unit EEE.
  • Milestones 3, 4 and 6 are stated in the proof's normalized setting: B\mathcal BB is a maximal commutative ∗-subalgebra of A\mathcal AA that is already in diagonal form; the unitary change of basis is milestone 1.

The goal is not to be read with a unital StarSubalgebra (that adds the hypothesis I∈AI \in \mathcal AI∈A and is the case already covered by the reference item), with an AlgEquiv that ignores the star, or with a mere linear equivalence (which exists for dimensional reasons and has no content). Each of these would trivialize or weaken the statement.

Useful infrastructure, reusable beyond this mission: simultaneous unitary diagonalization of commuting normal matrices, the unit and the central decomposition of a non-unital finite-dimensional ∗-algebra, and an explicit ∗-isomorphism from a corner algebra onto Ck×k\mathbb C^{k\times k}Ck×k. Proofs of any milestone, and alternative routes to the goal (for example through Mathlib's Wedderburn–Artin plus a star-compatibility argument), are welcome.

Selected references

  • C. Bachoc, D. C. Gijswijt, A. Schrijver, F. Vallentin, Invariant semidefinite programs, in: Handbook on Semidefinite, Conic and Polynomial Optimization, Springer, 2012. arXiv:1007.2905v2. https://arxiv.org/abs/1007.2905
  • K. R. Davidson, C∗-Algebras by Example, Fields Institute Monographs 6, American Mathematical Society, 1996. https://doi.org/10.1090/fim/006
  • K. Gatermann, P. A. Parrilo, Symmetry groups, semidefinite programs, and sums of squares, Journal of Pure and Applied Algebra 192 (2004) 95–128. https://doi.org/10.1016/j.jpaa.2003.12.011
  • E. de Klerk, D. V. Pasechnik, A. Schrijver, Reduction of symmetric semidefinite programs using the regular ∗-representation, Mathematical Programming 109 (2007) 613–624. https://doi.org/10.1007/s10107-006-0039-7
  • R. A. Horn, C. R. Johnson, Matrix Analysis, Cambridge University Press, 1985. https://doi.org/10.1017/CBO9780511810817
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