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Operations ResearchOptimization·Captain: Shuze Chen

Scheduling Parallel Machines On-Line: Removing advance knowledge of release datesResearch Paper

Motivation

A scheduler in a computing system may know how to allocate a fixed collection of jobs efficiently while having no reliable forecast of future arrivals. A guarantee for jobs available at the outset does not immediately answer whether decisions remain effective when new work appears during execution. Unknown release dates capture this distinction: a job becomes available and visible only at its release time. Shmoys, Wein and Williamson separate this information restriction from uncertainty about processing requirements and give a general conversion between the two arrival models. The present target is their Theorem 2.1, rather than the independent unknown-size conversion later in the paper. Source, §2.

The question concerns both efficient computation and execution on physical resources. A short schedule selected with knowledge of future jobs is not an online algorithm. Conversely, an online rule can make legitimate decisions yet produce schedules much longer than the best off-line schedule. The target retains both requirements and asks how much a scheduler's makespan guarantee deteriorates when advance knowledge of arrivals is removed.

Setting

A job is a finite processing task using some of a fixed finite collection of exclusive resources. An instance has a finite set JJJ of job identities, job data djd_jdj​, and real release dates rj≥0r_j\ge0rj​≥0. Jobs cannot receive processing before release. Each execution specifies resource allocations over time and must satisfy the job's processing rules. Two jobs cannot occupy the same resource simultaneously. The completion time CjC_jCj​ is the time at which job jjj has finished, and the makespan is

Cmax⁡=max⁡({0}∪{Cj:j∈J}).C_{\max}=\max(\{0\}\cup\{C_j:j\in J\}).Cmax​=max({0}∪{Cj​:j∈J}).

The empty instance therefore has makespan zero. The off-line optimum Cmax⁡∗(I)C_{\max}^{*}(I)Cmax∗​(I) is the least makespan among feasible schedules for the original released instance III, with the same resources and processing rules as the online scheduler.

For parallel machines, a job of size pj>0p_j>0pj​>0 runs at speed sij>0s_{ij}>0sij​>0 on machine iii. Identical machines have all speeds equal to one; uniformly related machines have sij=sis_{ij}=s_isij​=si​; unrelated machines allow job-dependent speeds. Nonpreemptive execution completes a job in one uninterrupted interval. A restart discards a canceled attempt's work. Preemption permits work to accumulate across interruptions and migration. These are separate choices of the environment, not extra powers granted to the transformed scheduler. Source, §1, p. 1314.

The base scheduler A\mathcal AA receives a finite admitted batch whose local release dates are all zero. Its admission information may include job sizes, or sizes may remain hidden until processing reveals completion. The transformation preserves that choice. In particular, removing advance knowledge of release dates does not remove information about sizes that the base scheduler needs.

Formalization targets

The goal is the complete algorithm transformation of Theorem 2.1. Let ρ≥1\rho\ge1ρ≥1 and suppose one uniform polynomial-time scheduler A\mathcal AA always produces feasible zero-release schedules satisfying

Cmax⁡A(B)≤ρCmax⁡∗(B).C_{\max}^{\mathcal A}(B)\le\rho C_{\max}^{*}(B).CmaxA​(B)≤ρCmax∗​(B).

Then the paper's batching controller supplies one causal polynomial-time scheduler A′\mathcal A'A′ for unknown release dates such that, for every finite valid released instance,

Cmax⁡A′(I)≤2ρCmax⁡∗(I).C_{\max}^{\mathcal A'}(I)\le2\rho C_{\max}^{*}(I).CmaxA′​(I)≤2ρCmax∗​(I).

Both guarantees are pure multiplicative inequalities, without an unspecified additive constant. The constant 2ρ2\rho2ρ is fixed by the published theorem. Source, Theorem 2.1, pp. 1316–1317.

The formal target also requires an execution of the controller, feasibility of its assembled schedule, disjoint batches covering every job, and at most n=∣J∣n=|J|n=∣J∣ nonempty base invocations. If the base computation costs at most c(N+1)dc(N+1)^dc(N+1)d, the stated metered bound for the wrapper is

nc(N(I)+1)d+10(N(I)+1)2.n c\bigl(N(I)+1\bigr)^d+10\bigl(N(I)+1\bigr)^2.nc(N(I)+1)d+10(N(I)+1)2.

Here N(I)N(I)N(I) counts encoded data cells, including release-date cells for analysis, and the constants c,dc,dc,d and the base code are independent of both the instance and the resource configuration. The Lean statement indexes configurations explicitly, allowing their approximation factor ρ(v)\rho(v)ρ(v) while retaining exactly 2ρ(v)2\rho(v)2ρ(v) in each configuration. The coefficient 10 is a bookkeeping allowance, not an approximation factor. There are no numbered milestone dependencies in the source proof; the only theorem target is Theorem 2.1.

Significance

The result allows zero-release scheduling guarantees to be used in settings with unpredictable arrivals while controlling their loss. Its scope is broader than one machine class. The source explicitly includes shop scheduling and allocation of submeshes, reflecting the independence of the conversion from particular speed formulas or off-line optimization methods. Source, p. 1317.

The mathematical theorem was proved in 1995. The task here is to formalize its statement and eventually its known guarantee. The local draft provides resource-use schedules, processing observations, an interpreted base program, and a controller whose execution is tied to the resulting schedule. Its theorem remains an open Lean proof obligation. These definitions also expose precisely what future formal proofs may assume about release information, processing information, and computation.

Difficulty

A makespan inequality alone cannot certify the result. A construction may accidentally inspect future job data, use an unattainable off-line value as an action, or count physical processing time as computational effort. Each produces a different statement from a polynomial-time online transformation.

Boundary events require equally careful treatment. Arrivals at a completion time must belong to the next batch; an arrival after an idle interval must not be lost; simultaneous arrivals must be collected together in a fixed job-ID order. Empty input and a single batch must remain meaningful without referring to nonexistent preceding batches. The source's compact stage notation is not itself an implementation specification for these cases. None of these concerns permits dropping the computational or information clauses from the target.

Formalization scope

The development uses nonnegative real time, natural-number job identities, finite profiles of half-open resource-use intervals, and a static job-local legality relation. It includes concrete parallel, shop, and mesh environment definitions. Whole-job restriction, time translation, release relaxation, and joining disjoint schedules preserve the intended static semantics. Time-dependent resource availability, external deadlines, and cross-job setup requirements are outside that interface.

The optimum inequality is written against every feasible off-line comparator. Valid jobs each have a finite legal execution; sequential execution after all releases supplies a finite feasible comparator, and makespans are bounded below by zero. Universal comparison is consequently equivalent to comparison with their infimum, including empty input.

The computational convention is an explicit finite-cell real RAM, with a finite program, a costed interpreter, and a processing port restricted to requested allocations and completion feedback. It permits arbitrary real times and does not assert a bit-complexity bound for arbitrary reals. Known and hidden sizes have separate admission encodings. Waiting for completion is a physical operation, whereas arithmetic, queue copying and message handling contribute to computation. No future job count or terminal-arrival notification is given to the controller.

The goal expressly rules out scalar-trace and vacuous-algorithm formalizations: it requires actual feasible resource schedules generated by the fixed controller using the interpreted base program, together with the computational bound. No variant theorem is posed. The recorded two-unit-job example demonstrates sharpness of this batching construction's factor 2, without claiming optimality among all possible online schedulers.

Selected references

  • David B. Shmoys, Joel Wein and David P. Williamson, Scheduling Parallel Machines On-Line, SIAM Journal on Computing 24(6), 1313–1331, 1995. Published article. Theorem 2.1 and its proof occupy printed pp. 1316–1317, PDF pp. 4–5.
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Operations ResearchOptimizationProbability+1·Captain: Shuze Chen

Modeling, Measuring and Managing Risk XII: The Value-of-Information Process Is a SupermartingaleTextbook

Motivation

Multi-stage stochastic optimization models a decision maker who acts at times 0,1,…,T−10,1,\dots,T-10,1,…,T−1 while a random scenario unfolds, and who may use at each time only the information revealed so far. This nonanticipativity constraint is what separates a genuine multi-stage problem from a collection of deterministic ones. A standard way of measuring its cost, the expected value of perfect information of decision analysis and stochastic programming (Birge & Louveaux 2011, Ch. 4), is to compare the decision maker's optimal value with that of a clairvoyant who sees the whole scenario before deciding.

Pflug and Römisch (Modeling, Measuring and Managing Risk, World Scientific 2007, §5.2) carry out this comparison not only at the root of a scenario tree but at every node, with the expectation replaced by a general acceptability functional A\mathcal AA. This produces three stochastic processes on the tree: the optimality process, the clairvoyant process, and their difference, the value-of-information process. The book shows that, for functionals that behave linearly under mixing of distributions, the value of information is a supermartingale: the expected remaining value of perfect information decreases as the scenario is revealed, and vanishes at the horizon.

Setting

Let (Ω,F,P)(\Omega,\mathcal F,P)(Ω,F,P) be a probability space and T≥0T\ge0T≥0. A tree process is a process (νt)t=0,…,T(\nu_t)_{t=0,\dots,T}(νt​)t=0,…,T​, νt\nu_tνt​ taking values in a finite set NtN_tNt​ of nodes, with σ(νt)=σ(νs: s≤t)\sigma(\nu_t)=\sigma(\nu_s:\,s\le t)σ(νt​)=σ(νs​:s≤t) for every ttt: the current node determines the whole path that led to it. The root stage N0N_0N0​ consists of one node. The standard filtration is F=(F0,…,FT)\boldsymbol{\mathcal F}=(\mathcal F_0,\dots,\mathcal F_T)F=(F0​,…,FT​) with Ft=σ(νt)\mathcal F_t=\sigma(\nu_t)Ft​=σ(νt​), and the clairvoyant's filtration is FT=(FT,…,FT)\boldsymbol{\mathcal F}^T=(\mathcal F_T,\dots,\mathcal F_T)FT=(FT​,…,FT​).

Scenario variables are ξt=ft(νt)\xi_t=f_t(\nu_t)ξt​=ft​(νt​), t=1,…,Tt=1,\dots,Tt=1,…,T. A profit function H(x0,ξ1,x1,…,xT−1,ξT)H(x_0,\xi_1,x_1,\dots,x_{T-1},\xi_T)H(x0​,ξ1​,x1​,…,xT−1​,ξT​), written H(x,ξ)H(x,\xi)H(x,ξ), depends on a decision sequence x=(x0,…,xT−1)x=(x_0,\dots,x_{T-1})x=(x0​,…,xT−1​) lying in a decision space X\mathcal XX. A decision rule xxx is a random sequence; it is non-anticipative, x⊲Fx\lhd\boldsymbol{\mathcal F}x⊲F, if each xtx_txt​ is Ft\mathcal F_tFt​-measurable, and clairvoyant, x⊲FTx\lhd\boldsymbol{\mathcal F}^Tx⊲FT, if each xtx_txt​ is FT\mathcal F_TFT​-measurable.

A version-independent probability functional R\mathcal RR assigns a real number to each distribution in its domain D\mathcal DD of distributions on R\mathbb RR. For a Markov kernel K(⋅∣v)K(\cdot\mid v)K(⋅∣v) on R\mathbb RR and a distribution GGG on R\mathbb RR, the compound distribution is K∘G=∫K(⋅∣v) dG(v)K\circ G=\int K(\cdot\mid v)\,dG(v)K∘G=∫K(⋅∣v)dG(v). R\mathcal RR is compound linear, compound convex or compound concave if

R{K∘G}  =, ≤, ≥  ∫R{K(⋅∣v)} dG(v)\mathcal R\{K\circ G\}\ \ =,\ \le,\ \ge\ \ \int\mathcal R\{K(\cdot\mid v)\}\,dG(v)R{K∘G}  =, ≤, ≥  ∫R{K(⋅∣v)}dG(v)

respectively, for all KKK, GGG with K(⋅∣v)∈DK(\cdot\mid v)\in\mathcal DK(⋅∣v)∈D for GGG-almost every vvv and K∘G∈DK\circ G\in\mathcal DK∘G∈D, for which the right-hand integral exists ("compound linear on D\mathcal DD"; the book's Example 2.13 uses exactly this domain-relative form for expected utility).

Fix such a functional A\mathcal AA (an acceptability functional; larger is better), whose domain contains the law of every feasible profit H(x,ξ)H(x,\xi)H(x,ξ) under the conditional probabilities below. For a node vvv of νt\nu_tνt​ with P{νt=v}>0P\{\nu_t=v\}>0P{νt​=v}>0 let P{νt=v}=P(⋅∣νt=v)P^{\{\nu_t=v\}}=P(\cdot\mid\nu_t=v)P{νt​=v}=P(⋅∣νt​=v) and let AP{νt=v}[Y]\mathcal A_{P^{\{\nu_t=v\}}}[Y]AP{νt​=v}​[Y] be A\mathcal AA applied to the law of YYY under it. The conditional problems are

At(v)=max⁡{AP{νt=v}[H(x,ξ)]:x⊲F, x∈X},Ct(v)=max⁡{AP{νt=v}[H(x,ξ)]:x⊲FT, x∈X}.A_t(v)=\max\{\mathcal A_{P^{\{\nu_t=v\}}}[H(x,\xi)] : x\lhd\boldsymbol{\mathcal F},\ x\in\mathcal X\},\qquad C_t(v)=\max\{\mathcal A_{P^{\{\nu_t=v\}}}[H(x,\xi)] : x\lhd\boldsymbol{\mathcal F}^T,\ x\in\mathcal X\}.At​(v)=max{AP{νt​=v}​[H(x,ξ)]:x⊲F, x∈X},Ct​(v)=max{AP{νt​=v}​[H(x,ξ)]:x⊲FT, x∈X}.

At the root these are the multi-stage problem A0A_0A0​ and the clairvoyant's problem C0C_0C0​. The optimality process is At=At(νt)A_t=A_t(\nu_t)At​=At​(νt​), the clairvoyant process Ct=Ct(νt)C_t=C_t(\nu_t)Ct​=Ct​(νt​), and the value-of-information process Dt=Ct−AtD_t=C_t-A_tDt​=Ct​−At​.

Formalization targets

Goal: Corollary 5.3

If A\mathcal AA is compound linear on its domain, then

Dt=Ct(νt)−At(νt),t=0,…,T,D_t=C_t(\nu_t)-A_t(\nu_t),\qquad t=0,\dots,T,Dt​=Ct​(νt​)−At​(νt​),t=0,…,T,

is a supermartingale under PPP with respect to (Ft)(\mathcal F_t)(Ft​).

Milestones

  1. Proposition 2.12. For a sub-σ\sigmaσ-algebra F1\mathcal F_1F1​ and R(Y∣F1)\mathcal R(Y\mid\mathcal F_1)R(Y∣F1​) the functional applied to the conditional distribution of YYY given F1\mathcal F_1F1​: compound linearity gives R(Y)=E[R(Y∣F1)]\mathcal R(Y)=\mathbb E[\mathcal R(Y\mid\mathcal F_1)]R(Y)=E[R(Y∣F1​)], compound convexity ≤\le≤, compound concavity ≥\ge≥.
  2. Lemma 5.1. If A\mathcal AA is compound convex, (Ct)(C_t)(Ct​) is a submartingale; if compound linear, a martingale.
  3. Lemma 5.2. If A\mathcal AA is compound convex, (At)(A_t)(At​) is a submartingale.

The goal is the weakest statement of the chain: it fixes no constants and asserts only the direction of drift of DtD_tDt​.

Significance

D0=C0−A0D_0=C_0-A_0D0​=C0​−A0​ is the value of perfect information of the multi-stage problem, which the book interprets as a multi-period deviation-type risk functional (the multi-period average value-at-risk deviation of its Chapter 3 is an instance). The supermartingale property gives this risk a dynamic meaning: as the scenario is revealed, the remaining value of information decreases in conditional mean, and it is zero at the horizon. The two lemmas separate the effect of information into its two sources: the clairvoyant's value is a fair game for compound linear functionals, while the non-anticipative decision maker's value can only improve in conditional mean, because a decision fixed at time ttt remains feasible after more is revealed.

The results are proved in the book. No formal version is known: the platform has no item on value-of-information processes, clairvoyant problems or compounding properties of functionals; the closest related items are a complete-information bound in partially observed Markov decision processes and a submartingale property of stable multi-period risk processes, both in other settings. A formalization adds a precise setting (finite scenario trees, conditioning on nodes, attained maxima) in which the chain from Definition 2.11 to Corollary 5.3 is checked.

Difficulty

The supermartingale inequality is a statement about conditional expectations on a tree, while compound convexity is a statement about functionals of mixtures of distributions; the work is to identify the law of the profit under P{νt=v}P^{\{\nu_t=v\}}P{νt​=v} as a compound distribution of the laws under the children's conditional probabilities, with the children encoded as a real mixing parameter. The book's proof of Lemma 5.1 interchanges the maximum and the functional, a step it justifies elsewhere only for monotone functionals, which Lemma 5.1 does not assume; its proof of Lemma 5.2 applies an inequality stated for nonrandom decisions to random ones. A solver should not rely on either step as printed. The martingale half of Lemma 5.1 needs the reverse inequality, for which the optimizers of the child problems must be combined into one feasible clairvoyant decision; the same combination is not available for non-anticipative decisions, which is why the optimality process is only a submartingale. Proposition 2.12 additionally needs regular conditional distributions.

Formalization scope

Lean 4 with Mathlib. Time is Fin (T + 1), stage 000 being the single root node ([Unique (N 0)]), so F0\mathcal F_0F0​ is trivial. Node types are finite with measurable singletons; this is what makes P(⋅∣νt=v)P(\cdot\mid\nu_t=v)P(⋅∣νt​=v) meaningful at every node of positive probability (Mathlib's ProbabilityTheory.cond) and every process integrable. The filtration is a Mathlib Filtration assumed equal to σ(νt)\sigma(\nu_t)σ(νt​) at each stage, and sub-, super- and martingales are Mathlib's Submartingale, Supermartingale, Martingale. Decisions take values in a measurable space with measurable singletons, x∈Xx\in\mathcal Xx∈X holds for every ω\omegaω, and HHH is jointly measurable. The functional is 𝒜 : Measure ℝ → ℝ, version-independent by construction, evaluated only at probability measures; it is real-valued (the book allows R‾\overline{\mathbb R}R) with a domain 𝒟 : Set (Measure ℝ), and each compounding (in)equality is required only when the mixed and the mixing distributions lie in D\mathcal DD and v↦R{K(⋅∣v)}v\mapsto\mathcal R\{K(\cdot\mid v)\}v↦R{K(⋅∣v)} is integrable. The tree theorems assume that D\mathcal DD contains the law of every feasible profit under every conditional probability of a positive-probability node; Proposition 2.12 assumes Y∈dom⁡RY\in\operatorname{dom}\mathcal RY∈domR and that the conditional distributions are in D\mathcal DD almost surely. Mixing is over Markov kernels from R\mathbb RR to R\mathbb RR (K ∘ₘ G). Proposition 2.12 uses Mathlib's condExpKernel on a standard Borel space and assumes E[R(Y∣F1)]\mathbb E[\mathcal R(Y\mid\mathcal F_1)]E[R(Y∣F1​)] exists.

The maxima At(v)A_t(v)At​(v), Ct(v)C_t(v)Ct​(v) are not defined through sSup: the theorems take them as given numbers and assume each is the greatest element of its value set at every node of positive probability. This rules out the trivializing formalization in which a junk supremum of an empty or unbounded set makes the processes constant and the claim empty. The book's remark "in particular if A\mathcal AA is the expectation" is covered as an instance and not stated separately: the expectation is compound linear on the distributions with a finite mean, and on a finite tree every feasible profit has finitely many values. Taking D\mathcal DD to be all distributions instead would exclude the expectation, because Lean's Bochner integral of a non-integrable function is 000.

Needed infrastructure: finite partitions and conditional expectation on atoms, mixtures of conditional laws, measurable selection of child optimizers on a finite tree, and the disintegration property of condExpKernel. The definitions CompoundLinear/CompoundConvex/CompoundConcave, IsTreeProcess, and the decision-problem sets are reusable for other results of the book on conditional acceptability and multi-stage problems. Proofs of any milestone, and sorry-free instances showing the hypotheses are satisfiable (e.g. a bounded expected utility on a two-stage tree), are welcome.

Selected references

  • G. Ch. Pflug, W. Römisch, Modeling, Measuring and Managing Risk, World Scientific, 2007, §2.1.2 and §5.2. https://doi.org/10.1142/6478
  • J. R. Birge, F. Louveaux, Introduction to Stochastic Programming, 2nd ed., Springer, 2011 (value of perfect information and of the stochastic solution). https://doi.org/10.1007/978-1-4614-0237-4
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Operations ResearchOptimizationProbability+1·Captain: Shuze Chen

Modeling, Measuring and Managing Risk IX: Dual Representation of the Nested Average Value-at-RiskTextbook

Motivation

Risk that unfolds over several periods is measured in two common ways. One adds up one-period measurements of each payment, each made with the information available one step earlier. The other composes one-period conditional measurements backwards in time, the way dynamic programming evaluates a policy. The second way is the one used in multistage stochastic programming with risk-averse objectives, because it is time-consistent by construction: a plan that is optimal today stays optimal when re-evaluated tomorrow. Ruszczyński and Shapiro (Conditional risk mappings, Math. Oper. Res. 2006) built the general theory of such compositions. Artzner, Delbaen, Eber, Heath and Ku (Ann. Oper. Res. 2007) studied the matching dynamic-programming (Bellman) principle for coherent multiperiod risk-adjusted values.

The most widely used one-period building block is the average value-at-risk. When it is applied conditionally at every stage, the composition is the nested average value-at-risk. Section 3.3 of Pflug and Römisch, Modeling, Measuring and Managing Risk (World Scientific 2007), treats both constructions. It builds the nested functional, shows that it depends only on the total payoff, gives its dual representation as an infimum over bounded-growth martingale densities, and compares it with the additive (multi-period) average value-at-risk. This mission formalizes that section's statements.

Setting

Let (Ω,F,P)(\Omega,\mathcal F,\mathbb P)(Ω,F,P) be a probability space with a filtration F0={∅,Ω}⊆F1⊆⋯⊆FT=F\mathcal F_0=\{\emptyset,\Omega\}\subseteq\mathcal F_1\subseteq\dots\subseteq\mathcal F_T=\mathcal FF0​={∅,Ω}⊆F1​⊆⋯⊆FT​=F. Random variables that agree almost surely are identified, and all (in)equalities between them hold almost surely. The book uses profit variables, where larger is better. Fix p∈[1,∞)p\in[1,\infty)p∈[1,∞) and put Yt=Lp(Ω,Ft,P)\mathcal Y_t=L_p(\Omega,\mathcal F_t,\mathbb P)Yt​=Lp​(Ω,Ft​,P). An income process is Y=(Y1,…,YT)Y=(Y_1,\dots,Y_T)Y=(Y1​,…,YT​) with Yt∈YtY_t\in\mathcal Y_tYt​∈Yt​.

A conditional acceptability mapping At−1:YT→Yt−1\mathcal A_{t-1}:\mathcal Y_T\to\mathcal Y_{t-1}At−1​:YT​→Yt−1​ has three properties:

  • (CA1) At−1(YT+Yt−1)=At−1(YT)+Yt−1\mathcal A_{t-1}(Y_T+Y_{t-1})=\mathcal A_{t-1}(Y_T)+Y_{t-1}At−1​(YT​+Yt−1​)=At−1​(YT​)+Yt−1​ for Yt−1∈Yt−1Y_{t-1}\in\mathcal Y_{t-1}Yt−1​∈Yt−1​;
  • (CA2) it is concave;
  • (CA3) it is monotone.

A family A0,…,AT−1\mathcal A_0,\dots,\mathcal A_{T-1}A0​,…,AT−1​ defines the nested functional and the compositions

A(Y;F)=A0[Y1+⋯+AT−2[YT−1+AT−1(YT)]⋯],A(t)=A0∘⋯∘At−1.\mathcal A(Y;\boldsymbol{\mathcal F})=\mathcal A_0\big[Y_1+\dots+\mathcal A_{T-2}[Y_{T-1}+\mathcal A_{T-1}(Y_T)]\cdots\big],\qquad \mathcal A^{(t)}=\mathcal A_0\circ\dots\circ\mathcal A_{t-1}.A(Y;F)=A0​[Y1​+⋯+AT−2​[YT−1​+AT−1​(YT​)]⋯],A(t)=A0​∘⋯∘At−1​.

Since F0\mathcal F_0F0​ is trivial, both are constants.

For α∈(0,1]\alpha\in(0,1]α∈(0,1] and a sub-σ\sigmaσ-field G\mathcal GG, the conditional average value-at-risk AV@Rα(Y∣G)∈L1(G)\mathbb{AV@R}_\alpha(Y\mid\mathcal G)\in L_1(\mathcal G)AV@Rα​(Y∣G)∈L1​(G) of Y∈L1(F)Y\in L_1(\mathcal F)Y∈L1​(F) is defined implicitly by

E(AV@Rα(Y∣G) 1B)=inf⁡{E(YZ):0≤Z≤1α1B, E(Z∣G)=1B}(B∈G).\mathbb E\big(\mathbb{AV@R}_\alpha(Y\mid\mathcal G)\,\mathbb 1_B\big)=\inf\Big\{\mathbb E(YZ):0\le Z\le\tfrac1\alpha\mathbb 1_B,\ \mathbb E(Z\mid\mathcal G)=\mathbb 1_B\Big\}\qquad(B\in\mathcal G).E(AV@Rα​(Y∣G)1B​)=inf{E(YZ):0≤Z≤α1​1B​, E(Z∣G)=1B​}(B∈G).

With trivial G\mathcal GG this is the lower-tail average 1α∫0αG−1(u) du\frac1\alpha\int_0^\alpha G^{-1}(u)\,duα1​∫0α​G−1(u)du of the quantile function. The nested average value-at-risk is

nAV@Rα(Y;F)=AV@Rα(⋅∣F0)∘⋯∘AV@Rα(⋅∣FT−1)(∑t=1TYt).\mathrm{n}\mathbb{AV@R}_\alpha(Y;\boldsymbol{\mathcal F})=\mathbb{AV@R}_\alpha(\cdot\mid\mathcal F_0)\circ\dots\circ\mathbb{AV@R}_\alpha(\cdot\mid\mathcal F_{T-1})\Big(\sum_{t=1}^TY_t\Big).nAV@Rα​(Y;F)=AV@Rα​(⋅∣F0​)∘⋯∘AV@Rα​(⋅∣FT−1​)(t=1∑T​Yt​).

The multi-period average value-at-risk is AV@Rα,c(Y;F)=∑t=1Tct E[AV@Rαt(Yt∣Ft−1)]\mathbb{AV@R}_{\alpha,c}(Y;\boldsymbol{\mathcal F})=\sum_{t=1}^Tc_t\,\mathbb E[\mathbb{AV@R}_{\alpha_t}(Y_t\mid\mathcal F_{t-1})]AV@Rα,c​(Y;F)=∑t=1T​ct​E[AV@Rαt​​(Yt​∣Ft−1​)]. Below it is used with all αt=α\alpha_t=\alphaαt​=α and ct=1c_t=1ct​=1.

Formalization targets

Goal: dual representation of the nested average value-at-risk (Proposition 3.35, (3.49))

For Yt∈L1(Ft)Y_t\in L_1(\mathcal F_t)Yt​∈L1​(Ft​) and α∈(0,1]\alpha\in(0,1]α∈(0,1], the nested average value-at-risk is well defined, and

nAV@Rα(Y;F)=inf⁡{E[(Y1+⋯+YT)ZT]:0≤Zt≤1αZt−1, E(Zt∣Ft−1)=Zt−1, Z0=1, t=1,…,T}.\mathrm{n}\mathbb{AV@R}_\alpha(Y;\boldsymbol{\mathcal F})=\inf\Big\{\mathbb E\big[(Y_1+\dots+Y_T)Z_T\big]:0\le Z_t\le\tfrac1\alpha Z_{t-1},\ \mathbb E(Z_t\mid\mathcal F_{t-1})=Z_{t-1},\ Z_0=1,\ t=1,\dots,T\Big\}.nAV@Rα​(Y;F)=inf{E[(Y1​+⋯+YT​)ZT​]:0≤Zt​≤α1​Zt−1​, E(Zt​∣Ft−1​)=Zt−1​, Z0​=1, t=1,…,T}.

Here ZtZ_tZt​ is Ft\mathcal F_tFt​-measurable. The feasible (Zt)(Z_t)(Zt​) are nonnegative martingales whose one-step growth is at most 1/α1/\alpha1/α.

Milestones

  1. Proposition 3.33. The nested functional of any family of conditional acceptability mappings has these properties:
    • it is weakly translation-equivariant, concave and monotone;
    • every A(t)\mathcal A^{(t)}A(t) is an acceptability functional;
    • A(Y;F)=A(T)(Y1+⋯+YT)\mathcal A(Y;\boldsymbol{\mathcal F})=\mathcal A^{(T)}(Y_1+\dots+Y_T)A(Y;F)=A(T)(Y1​+⋯+YT​) (3.47);
    • positive homogeneity is inherited from the mappings.
  2. The step in the proof of Proposition 3.35 (via (2.59)). For bounded Z1≥0Z_1\ge0Z1​≥0 that is F1\mathcal F_1F1​-measurable, E(AV@Rα(Y∣F1)Z1)=inf⁡{E(YZ2):0≤Z2≤1αZ1, E(Z2∣F1)=Z1}\mathbb E(\mathbb{AV@R}_\alpha(Y\mid\mathcal F_1)Z_1)=\inf\{\mathbb E(YZ_2):0\le Z_2\le\frac1\alpha Z_1,\ \mathbb E(Z_2\mid\mathcal F_1)=Z_1\}E(AV@Rα​(Y∣F1​)Z1​)=inf{E(YZ2​):0≤Z2​≤α1​Z1​, E(Z2​∣F1​)=Z1​}.
  3. Proposition 3.36(ii). For a final process (Y1=⋯=YT−1=0Y_1=\dots=Y_{T-1}=0Y1​=⋯=YT−1​=0), nAV@Rα(Y;F)≤AV@Rα(Y;F)\mathrm{n}\mathbb{AV@R}_\alpha(Y;\boldsymbol{\mathcal F})\le\mathbb{AV@R}_\alpha(Y;\boldsymbol{\mathcal F})nAV@Rα​(Y;F)≤AV@Rα​(Y;F).

Further items

  • Proposition 3.36(i), nAV@Rα≤α−(T−1)AV@Rα\mathrm{n}\mathbb{AV@R}_\alpha\le\alpha^{-(T-1)}\mathbb{AV@R}_\alphanAV@Rα​≤α−(T−1)AV@Rα​, stated as printed.
  • The information-monotonicity clause of Proposition 3.35: if Ft⊆Ft′\mathcal F_t\subseteq\mathcal F'_tFt​⊆Ft′​ for all ttt, then nAV@Rα(Y;F)≤nAV@Rα(Y;F′)\mathrm{n}\mathbb{AV@R}_\alpha(Y;\boldsymbol{\mathcal F})\le\mathrm{n}\mathbb{AV@R}_\alpha(Y;\boldsymbol{\mathcal F}')nAV@Rα​(Y;F)≤nAV@Rα​(Y;F′). It is stated as its own item, as printed.

Significance

The representation (3.49) shows that the nested average value-at-risk is a coherent functional of the total payoff. Its dual set consists of martingale densities with a multiplicative growth bound. Proposition 3.36 builds on this description to compare the nested and additive constructions. The same description underlies cutting-plane methods for risk-averse multistage programs: there the nested value is evaluated stage by stage, and each stage contributes one factor Zt/Zt−1∈[0,1/α]Z_t/Z_{t-1}\in[0,1/\alpha]Zt​/Zt−1​∈[0,1/α]. Proposition 3.33 is the general mechanism behind this: predictable translation-equivariance collapses a nested definition into a cumulative one.

All of these results are proved in the book, some only in outline. None is machine-checked. The platform has loss-side, upper-tail conditional value-at-risk results in other conventions and a nested risk-adjusted cost in an SDDP setting. It has no statement of the nested average value-at-risk or of (3.49). Formalizing this section yields a reusable treatment of conditional average values-at-risk defined by duality, together with their compositions along a filtration.

Difficulty

The conditional average value-at-risk is not given by a formula. It is defined through a family of infima indexed by the sets B∈GB\in\mathcal GB∈G, so composing two of them requires knowing what the first one does when paired with a general bounded weight rather than an indicator. Merging the infima of successive stages into one infimum over processes needs measurable selection of near-optimal densities, conditional on the earlier stages, and the martingale constraint must be preserved. The printed proof treats T=2T=2T=2 in a few lines and asserts that the general case "follows by induction". Its last display also carries a misprint, E(Z1)=0\mathbb E(Z_1)=0E(Z1​)=0 for E(Z1)=1\mathbb E(Z_1)=1E(Z1​)=1 (FINDINGS F5).

Formalization scope

Random variables are functions Ω → ℝ. The filtration is Mathlib's Filtration ℕ, and only indices 0,…,T0,\dots,T0,…,T matter. IsStandardFiltration records that F0\mathcal F_0F0​ is trivial and FT=F\mathcal F_T=\mathcal FFT​=F. The conditional average value-at-risk is the predicate IsConditionalAVaR, a literal transcription of the defining relation, with the infimum computed in EReal. The nested and multi-period values are predicates that are existential over versions of the conditional average values-at-risk. The goal therefore asserts existence and the identity separately. A version of the goal that only assumed some value exists, or that took a bare real infimum, would be vacuous or junk-valued, and the formal statement rules out both. The expectation of the F0\mathcal F_0F0​-measurable output is the functional's real value. The dual set requires ZtZ_tZt​ to be Ft\mathcal F_tFt​-measurable, which the page leaves implicit.

Beyond the paper. Two corrected variants are posed beside the faithful statements:

  • Information monotonicity (F1). Refining F1\mathcal F_1F1​ in a two-period example lowers the nested value from −5-5−5 to −10-10−10. The variant asserts that a counterexample exists.
  • Proposition 3.36(i) for Yt≥0Y_t\ge0Yt​≥0 (F2). The printed inequality fails for Y2≡−1Y_2\equiv-1Y2​≡−1 with α=1/2\alpha=1/2α=1/2. The variant adds the nonnegativity that the proof uses.

The faithful statements stay as printed and are expected to be disproved.

Contributions that would be reused beyond this mission:

  • existence and uniqueness of the conditional average value-at-risk on L1L_1L1​;
  • its extension to bounded nonnegative weights;
  • a general composition lemma for dual representations of conditional acceptability mappings.

Selected references

  • G. Ch. Pflug and W. Römisch, Modeling, Measuring and Managing Risk, World Scientific, 2007, §3.3. https://doi.org/10.1142/6478
  • A. Ruszczyński and A. Shapiro, Conditional risk mappings, Mathematics of Operations Research 31(3), 2006. https://doi.org/10.1287/moor.1060.0204
  • P. Artzner, F. Delbaen, J.-M. Eber, D. Heath and H. Ku, Coherent multiperiod risk adjusted values and Bellman's principle, Annals of Operations Research 152, 2007. https://doi.org/10.1007/s10479-006-0132-6
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Modeling, Measuring and Managing Risk XI: The Mean-Variance Efficient Portfolio in Closed FormTextbook

Why mean-variance portfolios

An investor who splits a budget across MMM risky assets faces a trade-off between expected return and risk. Markowitz proposed measuring risk by the variance of the portfolio return and selecting, for each required expected return, the portfolio of least variance (Markowitz 1952). Tobin added a risk-free asset (Tobin 1958), and Sharpe, Lintner and Mossin turned the resulting one-fund structure into the capital asset pricing model (CAPM), whose beta equation is still the standard first model of expected returns in finance (Sharpe 1964).

This mission formalizes the closed-form part of that theory as presented in §4.2.3 of Pflug and Römisch, Modeling, Measuring and Managing Risk (World Scientific 2007, doi:10.1142/6478), pp. 189–195: the explicit efficient portfolio without a risk-free asset (Proposition 4.8), the solution with a risk-free asset (Proposition 4.9), and the CAPM equation with its variance bound (Proposition 4.10).

Setting

Let (Ω,F,P)(\Omega,\mathcal F,\mathbb P)(Ω,F,P) be a probability space and ξ=(ξ(1),…,ξ(M))\xi=(\xi^{(1)},\dots,\xi^{(M)})ξ=(ξ(1),…,ξ(M)) a random vector of returns, each coordinate with a finite second moment. Returns are profits: larger is better. The vector of expected returns is r=Eξr=\mathbb E\xir=Eξ and the covariance matrix is the M×MM\times MM×M matrix CCC with Cij=Cov(ξ(i),ξ(j))C_{ij}=\mathbb{C}\mathrm{ov}(\xi^{(i)},\xi^{(j)})Cij​=Cov(ξ(i),ξ(j)); it is symmetric and positive semidefinite. A portfolio is a weight vector x∈RMx\in\mathbb R^Mx∈RM (negative weights, i.e. short positions, are allowed) with return Yx=∑mxmξ(m)Y_x=\sum_m x_m\xi^{(m)}Yx​=∑m​xm​ξ(m), so that E(Yx)=r⊤x\mathbb E(Y_x)=r^\top xE(Yx​)=r⊤x and Var(Yx)=x⊤Cx\mathbb{V}\mathrm{ar}(Y_x)=x^\top CxVar(Yx​)=x⊤Cx. Write 1\mathbb 11 for the all-ones vector.

The CAPM problem without a risk-free asset fixes a required return μ\muμ and asks for

minimize x⊤Cxsubject tor⊤x=μ,  1⊤x=1.(4.20)\text{minimize } x^\top Cx\quad\text{subject to}\quad r^\top x=\mu,\ \ \mathbb 1^\top x=1. \tag{4.20}minimize x⊤Cxsubject tor⊤x=μ,  1⊤x=1.(4.20)

With a risk-free asset of constant return r0r_0r0​, a portfolio is a pair (x0,x~)(x_0,\tilde x)(x0​,x~), where x0x_0x0​ is the holding of the risk-free asset and x~\tilde xx~ the holdings of the risky assets ξ~\tilde\xiξ~​, with mean r~\tilde rr~ and covariance C~\tilde CC~. Its return is Yx=x0r0+x~⊤ξ~Y_x=x_0r_0+\tilde x^\top\tilde\xiYx​=x0​r0​+x~⊤ξ~​, and the problem is

minimize 12x~⊤C~x~subject tor~⊤x~+r0x0=μ,  1M⊤x~+x0=1.(4.23)\text{minimize } \tfrac12\tilde x^\top\tilde C\tilde x\quad\text{subject to}\quad \tilde r^\top\tilde x+r_0x_0=\mu,\ \ \mathbb 1_M^\top\tilde x+x_0=1. \tag{4.23}minimize 21​x~⊤C~x~subject tor~⊤x~+r0​x0​=μ,  1M⊤​x~+x0​=1.(4.23)

A portfolio is efficient if it solves the respective problem for some μ\muμ. The market portfolio x+x_+x+​ holds nothing in the risk-free asset and C~−1(r~−r01)/1⊤C~−1(r~−r01)\tilde C^{-1}(\tilde r-r_0\mathbb 1)/\mathbb 1^\top\tilde C^{-1}(\tilde r-r_0\mathbb 1)C~−1(r~−r0​1)/1⊤C~−1(r~−r0​1) in the risky ones; Y+Y_+Y+​ is its return, μ+=E(Y+)\mu_+=\mathbb E(Y_+)μ+​=E(Y+​) and σ+2=Var(Y+)\sigma_+^2=\mathbb{V}\mathrm{ar}(Y_+)σ+2​=Var(Y+​).

Formalization targets

Goal: Proposition 4.8, the efficient portfolio in closed form

Assume CCC is invertible and rrr is not a multiple of 1\mathbb 11. With

a=r⊤C−1r,b=r⊤C−11,c=1⊤C−11,d=ac−b2,(4.22)a=r^\top C^{-1}r,\quad b=r^\top C^{-1}\mathbb 1,\quad c=\mathbb 1^\top C^{-1}\mathbb 1,\quad d=ac-b^2, \tag{4.22}a=r⊤C−1r,b=r⊤C−11,c=1⊤C−11,d=ac−b2,(4.22)

the unique solution of (4.20) is

x∗(μ)=μ[cdC−1r−bdC−11]+[adC−11−bdC−1r],(4.21)x^*(\mu)=\mu\Big[\frac cd C^{-1}r-\frac bd C^{-1}\mathbb 1\Big]+\Big[\frac ad C^{-1}\mathbb 1-\frac bd C^{-1}r\Big], \tag{4.21}x∗(μ)=μ[dc​C−1r−db​C−11]+[da​C−11−db​C−1r],(4.21)

any two efficient portfolios for different returns span all efficient portfolios by affine combinations (the Two Fund Theorem in this model), and

E(Yμ)=μ,Var(Yμ)=μ2c−2μb+ad.\mathbb E(Y_\mu)=\mu,\qquad \mathbb{V}\mathrm{ar}(Y_\mu)=\frac{\mu^2c-2\mu b+a}{d}.E(Yμ​)=μ,Var(Yμ​)=dμ2c−2μb+a​.

The efficient frontier is therefore a parabola in the (variance, mean) plane.

Milestones and further results

Propositions 4.10 (i) and (ii) are milestones; Proposition 4.9 is a further item of the mission on which they stand.

  1. Proposition 4.9. If C~\tilde CC~ is invertible and r~≠r01\tilde r\ne r_0\mathbb 1r~=r0​1, then with q=(r~−r01)⊤C~−1(r~−r01)q=(\tilde r-r_0\mathbb 1)^\top\tilde C^{-1}(\tilde r-r_0\mathbb 1)q=(r~−r0​1)⊤C~−1(r~−r0​1) the unique solution of (4.23) is
x∗(μ)=1q((r~−μ1)⊤C~−1(r~−r01)(μ−r0)C~−1(r~−r01)),x^*(\mu)=\frac1q\begin{pmatrix}(\tilde r-\mu\mathbb 1)^\top\tilde C^{-1}(\tilde r-r_0\mathbb 1)\\(\mu-r_0)\tilde C^{-1}(\tilde r-r_0\mathbb 1)\end{pmatrix},x∗(μ)=q1​((r~−μ1)⊤C~−1(r~−r0​1)(μ−r0​)C~−1(r~−r0​1)​),

and, when 1⊤C~−1(r~−r01)≠0\mathbb 1^\top\tilde C^{-1}(\tilde r-r_0\mathbb 1)\ne01⊤C~−1(r~−r0​1)=0, every efficient portfolio is an affine combination of (1,0,…,0)(1,0,\dots,0)(1,0,…,0) and x+x_+x+​. 2. Proposition 4.10 (i), the CAPM equation (4.25). For every portfolio with x0+1⊤x~=1x_0+\mathbb 1^\top\tilde x=1x0​+1⊤x~=1,

E(Yx)=r0+β(x)(μ+−r0),β(x)=Cov(Yx,Y+)Var(Y+).\mathbb E(Y_x)=r_0+\beta(x)(\mu_+-r_0),\qquad \beta(x)=\frac{\mathbb{C}\mathrm{ov}(Y_x,Y_+)}{\mathbb{V}\mathrm{ar}(Y_+)}.E(Yx​)=r0​+β(x)(μ+​−r0​),β(x)=Var(Y+​)Cov(Yx​,Y+​)​.
  1. Proposition 4.10 (ii). For every such portfolio
Var(Yx)≥(E(Yx)−r0μ+−r0)2σ+2,\mathbb{V}\mathrm{ar}(Y_x)\ge\Big(\frac{\mathbb E(Y_x)-r_0}{\mu_+-r_0}\Big)^2\sigma_+^2,Var(Yx​)≥(μ+​−r0​E(Yx​)−r0​​)2σ+2​,

with equality if and only if the portfolio is efficient, and, as printed, if and only if Corr(Yx,Y+)=1\mathbb{C}\mathrm{orr}(Y_x,Y_+)=1Corr(Yx​,Y+​)=1.

Significance

Proposition 4.8 is the explicit description of the mean-variance efficient set: the efficient portfolios form a line in weight space, and the minimal variance is a quadratic function of the required return. Proposition 4.9 shows that a risk-free asset turns this line into one through the risk-free portfolio (the one-fund, or separation, property), and Proposition 4.10 derives from it the CAPM relation between a portfolio's expected excess return and its beta, together with the capital-market-line bound. These are the statements on which the later sections of the chapter, and most textbook treatments of portfolio theory, build: risk-return diagrams, the market portfolio, beta as a risk measure.

The results are classical and their proofs are elementary, but they are not in Mathlib, and no Prove2Me item states them; the closest platform item is the multi-period mean-variance mutual fund theorem of Bäuerle and Rieder (MDPFinance.MeanVariance.mutual_fund_theorem), a different, dynamic statement. A formalization makes the hypotheses explicit that the printed proofs leave implicit (invertibility and nondegeneracy conditions, the budget constraint behind "any portfolio") and checks the printed equality conditions, one of which is false as stated.

Difficulty

The Lagrange conditions of the printed proof are necessary conditions only. Turning them into the statement requires showing that the stationary point is the global minimizer and the only one, which uses positive definiteness of CCC; the hypothesis gives only invertibility, and positive definiteness has to come from CCC being a covariance matrix. Dividing by ddd needs d>0d>0d>0, which is not among the hypotheses and must be derived from "rrr is not a multiple of 1\mathbb 11" together with the structure of CCC. The variance identities require computing variances and covariances of linear combinations of square-integrable random variables. In Proposition 4.10 (ii) the equality case is where the printed statement goes wrong: a portfolio short in the market portfolio attains equality with correlation −1-1−1.

Formalization scope

All statements live in the namespace RiskFunctionals.Frontier. Assets are indexed by Fin M; vectors are Fin M → ℝ, matrices Matrix (Fin M) (Fin M) ℝ, and C−1C^{-1}C−1 is Mathlib's matrix inverse. The mean vector and covariance matrix are computed from a random vector with MemLp 2 coordinates on a probability space using Mathlib's covariance and variance, so "CCC invertible" is the printed hypothesis and positive definiteness is a consequence, not an assumption. "The solution" is stated as existence and uniqueness of a global minimizer on the feasible set (IsSolution420, IsSolution423). The divisions by qqq, by 1⊤C~−1(r~−r01)\mathbb 1^\top\tilde C^{-1}(\tilde r-r_0\mathbb 1)1⊤C~−1(r~−r0​1) and by ddd are guarded by the printed or implicit nondegeneracy hypotheses; a statement in which d=0d=0d=0 or q=0q=0q=0 were allowed would make the closed forms the zero vector, so these guards are part of the statement rather than conveniences. The correlation is used only where the portfolio variance is positive, since it is undefined otherwise.

Beyond the paper. One variant item is posed beside the faithful statements: capm_variance_bound_corrected (corrected, finding F4) replaces the equality condition Corr(Yx,Y+)=1\mathbb{C}\mathrm{orr}(Y_x,Y_+)=1Corr(Yx​,Y+​)=1 of Proposition 4.10 (ii) by ∣Corr(Yx,Y+)∣=1|\mathbb{C}\mathrm{orr}(Y_x,Y_+)|=1∣Corr(Yx​,Y+​)∣=1; with one risky asset of mean 2 and variance 1, r0=1r_0=1r0​=1 and x=(2,−1)x=(2,-1)x=(2,−1), equality holds while the correlation is −1-1−1. The faithful Proposition 4.10 (ii) is therefore expected to be disproved.

A complete development needs the variance and covariance of finite linear combinations of L2L^2L2 random variables, positive semidefiniteness of covariance matrices, and the minimization of a positive definite quadratic form under linear equality constraints. These are reusable well beyond this mission; proofs of them as separate lemmas are welcome.

Selected references

  • G. Ch. Pflug and W. Römisch, Modeling, Measuring and Managing Risk, World Scientific, 2007, §4.2.3, pp. 189–195. https://doi.org/10.1142/6478
  • H. Markowitz, Portfolio Selection, Journal of Finance 7(1), 77–91, 1952. https://doi.org/10.2307/2975974
  • J. Tobin, Liquidity Preference as Behavior Towards Risk, Review of Economic Studies 25(2), 65–86, 1958. https://doi.org/10.2307/2296205
  • W. F. Sharpe, Capital Asset Prices: A Theory of Market Equilibrium under Conditions of Risk, Journal of Finance 19(3), 425–442, 1964. https://doi.org/10.1111/j.1540-6261.1964.tb02865.x
  • R. C. Merton, An Analytic Derivation of the Efficient Portfolio Frontier, Journal of Financial and Quantitative Analysis 7(4), 1851–1872, 1972. https://doi.org/10.2307/2329621
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Modeling, Measuring and Managing Risk VI: Choquet Representation of Distortion FunctionalsTextbook

Motivation

A distortion functional values an uncertain profit YYY by integrating its quantiles against a reweighting of the probability scale: small (bad) quantiles receive more weight, large ones less. The construction appears in actuarial pricing (the distortion premium principles of Denneberg and Wang), in decision theory (Yaari's dual theory of choice), and in finance as spectral risk measures (Acerbi) or weighted values-at-risk (Cherny). Its central structural fact is that every concave distortion is a mixture of average values-at-risk, the lower-tail averages AV@Rα\mathbb{AV@R}_\alphaAV@Rα​: this Choquet representation reduces properties of the whole class (concavity, monotonicity with respect to second-order dominance, comonotone additivity) to those of one family. The representation was proved by Acerbi (2002), Jones and Zitikis (2003) and Pflug (2006). This mission formalizes it as Proposition 2.64 of Pflug and Römisch, Modeling, Measuring and Managing Risk (World Scientific 2007, §2.4.2), together with the lemmas of that section.

Setting

All random variables are profit variables (larger is better) on a probability space (Ω,F,P)(\Omega,\mathcal F,\mathbb P)(Ω,F,P). For a random variable YYY with distribution function G(u)=P{Y≤u}G(u)=\mathbb P\{Y\le u\}G(u)=P{Y≤u} and left limit G(u−)=P{Y<u}G(u-)=\mathbb P\{Y<u\}G(u−)=P{Y<u}, the quantile function is the left-continuous inverse

G−1(p)=inf⁡{u:G(u)≥p},0<p≤1,G^{-1}(p)=\inf\{u: G(u)\ge p\},\qquad 0<p\le1,G−1(p)=inf{u:G(u)≥p},0<p≤1,

and the average value-at-risk at level 0<α≤10<\alpha\le10<α≤1 is

AV@Rα{G}=1α∫0αG−1(u) du.\mathbb{AV@R}_\alpha\{G\}=\frac1\alpha\int_0^\alpha G^{-1}(u)\,du .AV@Rα​{G}=α1​∫0α​G−1(u)du.

A distortion function HHH is a bounded, right continuous, increasing function on [0,1][0,1][0,1], the distribution function of a non-negative measure dHdHdH on [0,1][0,1][0,1] (not necessarily a probability measure). Writing GH\mathcal G_HGH​ for the distributions GGG for which G−1G^{-1}G−1 is dHdHdH integrable, the distortion acceptability functional is

AH{G}=∫01G−1(p) dH(p),G∈GH,\mathcal A_H\{G\}=\int_0^1 G^{-1}(p)\,dH(p),\qquad G\in\mathcal G_H,AH​{G}=∫01​G−1(p)dH(p),G∈GH​,

also written AH(Y)\mathcal A_H(Y)AH​(Y). H(p)=pH(p)=pH(p)=p gives the expectation, H=1[α,1]H=\mathbb 1_{[\alpha,1]}H=1[α,1]​ the value-at-risk G−1(α)G^{-1}(\alpha)G−1(α), and H(p)=min⁡(p/α,1)H(p)=\min(p/\alpha,1)H(p)=min(p/α,1) the average value-at-risk. HHH is concave when H(p)=∫0ph(α) dαH(p)=\int_0^p h(\alpha)\,d\alphaH(p)=∫0p​h(α)dα with a nonincreasing density hhh, which may be unbounded near 000.

Two orders on random variables enter: Z≺CXDZ∗Z\prec_{CXD}Z^*Z≺CXD​Z∗ (convex order) when E U(Z)≤E U(Z∗)\mathbb E\,U(Z)\le\mathbb E\,U(Z^*)EU(Z)≤EU(Z∗) for every convex UUU for which both expectations exist; and Y1,Y2Y_1,Y_2Y1​,Y2​ are comonotone when their joint distribution function is min⁡(G1(u),G2(v))\min(G_1(u),G_2(v))min(G1​(u),G2​(v)). A functional is comonotone additive when it is additive on comonotone pairs.

Formalization targets

Goal: the Choquet representation (Proposition 2.64)

If HHH is concave, there is an increasing function MMM on [0,1][0,1][0,1] with M(0)=0M(0)=0M(0)=0 and M(1)=H(1)M(1)=H(1)M(1)=H(1) such that, for every G∈GHG\in\mathcal G_HG∈GH​,

AH{G}=∫01AV@Rα{G} dM(α).\mathcal A_H\{G\}=\int_0^1\mathbb{AV@R}_\alpha\{G\}\,dM(\alpha).AH​{G}=∫01​AV@Rα​{G}dM(α).

Conversely, every comonotone additive functional having such a Choquet representation is a distortion functional. The goal leaves MMM otherwise unspecified; one MMM serves every GGG.

Milestones

  1. Examples 2.63: the three distortions H(p)=pH(p)=pH(p)=p, 1[α,1](p)\mathbb 1_{[\alpha,1]}(p)1[α,1]​(p) and min⁡(p/α,1)\min(p/\alpha,1)min(p/α,1) give E(Y)=−∫−∞0G+∫0∞(1−G)\mathbb E(Y)=-\int_{-\infty}^0G+\int_0^\infty(1-G)E(Y)=−∫−∞0​G+∫0∞​(1−G), G−1(α)G^{-1}(\alpha)G−1(α) and AV@Rα\mathbb{AV@R}_\alphaAV@Rα​.
  2. Lemma 2.62: for G∈GHG\in\mathcal G_HG∈GH​, with Hˉ(u)=H(1)−H(1−u)\bar H(u)=H(1)-H(1-u)Hˉ(u)=H(1)−H(1−u),
∫01G−1(p) dH(p)=−∫−∞0H(G(u)) du+∫0∞Hˉ(1−G(u)) du.\int_0^1 G^{-1}(p)\,dH(p)=-\int_{-\infty}^0H(G(u))\,du+\int_0^\infty\bar H(1-G(u))\,du .∫01​G−1(p)dH(p)=−∫−∞0​H(G(u))du+∫0∞​Hˉ(1−G(u))du.
  1. Eq. (2.68): for UUU uniform on [0,1][0,1][0,1] and independent of YYY, the generalized quantile transform (1−U)G(Y−)+UG(Y)(1-U)G(Y-)+UG(Y)(1−U)G(Y−)+UG(Y) is uniform on [0,1][0,1][0,1].
  2. Eq. (2.69): for differentiable HHH with H(p)=∫0phH(p)=\int_0^phH(p)=∫0p​h, AH(Y)=E[Y h((1−U)G(Y−)+UG(Y))]\mathcal A_H(Y)=\mathbb E\big[Y\,h\big((1-U)G(Y-)+UG(Y)\big)\big]AH​(Y)=E[Yh((1−U)G(Y−)+UG(Y))].
  3. Proposition 2.65, as printed: for differentiable HHH, AH(Y)=inf⁡{E(YZ):Z=h(U), U uniform}=inf⁡{E(YZ):Z≺CXDh(U)}\mathcal A_H(Y)=\inf\{\mathbb E(YZ): Z=h(U),\ U\text{ uniform}\}=\inf\{\mathbb E(YZ):Z\prec_{CXD}h(U)\}AH​(Y)=inf{E(YZ):Z=h(U), U uniform}=inf{E(YZ):Z≺CXD​h(U)}, attained at Z=h((1−U)G(Y−)+UG(Y))Z=h\big((1-U)G(Y-)+UG(Y)\big)Z=h((1−U)G(Y−)+UG(Y)).

Significance

The Choquet representation identifies the concave distortion functionals with the closed convex cone generated by the average values-at-risk. Downstream, this gives the coherence properties of spectral risk measures, their consistency with second-order stochastic dominance, and, through Proposition 2.65, a dual description by rearrangements of the distortion density that is used to optimize portfolios under such criteria. It also separates the class from the larger family of law-invariant coherent functionals, which are infima of such mixtures over a family of mixing measures (Kusuoka) rather than single mixtures.

The results are classical and proved in the literature; none is machine-checked in this form. A related loss-side layer exists on the platform (MultistageStochastic.distortion_avar_mixture, proved, for a spectrum σ\sigmaσ on L∞L_\inftyL∞​ with the upper-tail AV@R), but its sign, tail and integrability conventions differ, so it does not state this book's theorem. The formalization adds a quantile calculus with atoms (the left-continuous G−1G^{-1}G−1, G(u−)G(u-)G(u−), the generalized quantile transform) and Lebesgue–Stieltjes integration against distortion measures, both reusable for the rest of the series.

Difficulty

The forward direction is not a finite-dimensional extreme-point argument: hhh may be unbounded at 000, so the mixing measure dMdMdM must be obtained as a limit and the exchange of integrals justified for quantile functions that are only dHdHdH-integrable, with G−1G^{-1}G−1 unbounded at both ends. Distributions with atoms make G−1(G(u))<uG^{-1}(G(u))<uG−1(G(u))<u on flat stretches, which is exactly where Lemma 2.62 and (2.69) need care.

Proposition 2.65 is false as printed (finding F1): for the differentiable convex H(p)=p2H(p)=p^2H(p)=p2 and YYY uniform on [0,1][0,1][0,1], AH(Y)=2/3\mathcal A_H(Y)=2/3AH​(Y)=2/3, while Z=2(1−Y)=h(1−Y)Z=2(1-Y)=h(1-Y)Z=2(1−Y)=h(1−Y) gives E(YZ)=1/3\mathbb E(YZ)=1/3E(YZ)=1/3. Its printed proof uses that hhh is nonincreasing. The faithful milestone is therefore expected to be disproved; a corrected variant is posed beside it.

Formalization scope

Distributions are probability measures μ\muμ on R\mathbb RR; for a random variable, μ\muμ is the image measure of P\mathbb PP under YYY. G−1G^{-1}G−1 is computed by sInf; its junk value 000 (at p=1p=1p=1 when G<1G<1G<1 everywhere, and at p≤0p\le0p≤0) is never charged. HHH and MMM are Mathlib StieltjesFunctions; AH\mathcal A_HAH​ integrates over (0,1](0,1](0,1] against dHdHdH. Membership in GH\mathcal G_HGH​ contains dHdHdH-integrability of G−1G^{-1}G−1, H(0)=0H(0)=0H(0)=0 (the mass dHdHdH puts on p=0p=0p=0, where G−1=−∞G^{-1}=-\inftyG−1=−∞), and finiteness of G−1(1)G^{-1}(1)G−1(1) when dHdHdH charges p=1p=1p=1. MMM vanishes on (−∞,0](-\infty,0](−∞,0], so dMdMdM has no atom at 000, and the representation integrates over [0,1][0,1][0,1]; dMdMdM-integrability of α↦AV@Rα\alpha\mapsto\mathbb{AV@R}_\alphaα↦AV@Rα​ is part of the conclusion, and the converse is stated on integrable YYY for which that integrability holds. Infima in Proposition 2.65 are greatest lower bounds of value sets restricted to integrable products, with attainment stated separately. Uniform variables are measurable with law Lebesgue measure on [0,1][0,1][0,1], and UUU is independent of YYY in (2.68)–(2.69), as Proposition 1.3 requires. The book's VY=(1−U)[G(Y−)−G(Y)]V_Y=(1-U)[G(Y-)-G(Y)]VY​=(1−U)[G(Y−)−G(Y)] has a sign typo and is used as (1−U)[G(Y)−G(Y−)](1-U)[G(Y)-G(Y-)](1−U)[G(Y)−G(Y−)].

A trivializing formalization would integrate a quantile function that is not dHdHdH- or dMdMdM-integrable, where Lean's integral returns 000, or take an infimum of an empty set; every such integral is guarded by an integrability hypothesis or an asserted integrability, and every infimum is an IsGLB of a set shown nonempty by the attainment clause.

Beyond the paper. One variant: [Corrected] Proposition 2.65 adds the hypothesis "HHH concave" and changes nothing else (finding F1, the counterexample above). A further finding (F2) records that the converse half of Proposition 2.64 does not use comonotone additivity; no variant is posed for it.

Contributions welcome: proofs of the milestones, a disproof of the printed Proposition 2.65, and reusable lemmas on quantile functions with atoms and on Stieltjes integration on [0,1][0,1][0,1].

Selected references

  • G. Ch. Pflug, W. Römisch, Modeling, Measuring and Managing Risk, World Scientific, 2007. https://doi.org/10.1142/6478
  • C. Acerbi, Spectral measures of risk: a coherent representation of subjective risk aversion, Journal of Banking & Finance 26 (2002). https://doi.org/10.1016/S0378-4266(02)00281-9
  • B. L. Jones, R. Zitikis, Empirical estimation of risk measures and related quantities, North American Actuarial Journal 7 (2003). https://doi.org/10.1080/10920277.2003.10596118
  • G. Ch. Pflug, On distortion functionals, Statistics & Decisions 24 (2006). https://doi.org/10.1524/stnd.2006.24.1.45
  • M. E. Yaari, The dual theory of choice under risk, Econometrica 55 (1987). https://doi.org/10.2307/1911158
  • S. S. Wang, A class of distortion operators for pricing financial and insurance risks, Journal of Risk and Insurance 67 (2000). https://doi.org/10.2307/253675
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Modeling, Measuring and Managing Risk IV: Kusuoka Representations of Version-Independent Acceptability FunctionalsTextbook

Motivation

Risk measures used in portfolio optimization, insurance pricing and regulation are almost always law invariant: they assign a number to a random profit YYY that depends only on its distribution, not on the scenario in which each outcome occurs. Kusuoka (Kusuoka 2001) showed that on a non-atomic space every law-invariant coherent risk measure is the worst case, over a family of weightings, of mixtures of one elementary functional, the average value-at-risk (also called conditional value-at-risk or expected shortfall). This reduces the design and the computation of law-invariant risk measures to the choice of a set of probability measures on the interval of confidence levels, and it underlies the use of the average value-at-risk as the building block of spectral and distortion risk measures.

This mission formalizes the version of Kusuoka's theorem proved in G. Ch. Pflug and W. Römisch, Modeling, Measuring and Managing Risk (World Scientific 2007, §2.2.4, Theorem 2.45), stated for acceptability functionals of profit variables on LpL_pLp​, 1≤p<∞1\le p<\infty1≤p<∞, together with the coupling and realization results its proof uses and a worked example from the same section.

Setting

Let (Ω,F,P)(\Omega,\mathcal F,\mathbb P)(Ω,F,P) be a probability space. It is non-atomic if no measurable set AAA with P(A)>0\mathbb P(A)>0P(A)>0 has only subsets of probability 000 or P(A)\mathbb P(A)P(A). Fix 1≤p<∞1\le p<\infty1≤p<∞ and the conjugate exponent qqq, 1/p+1/q=11/p+1/q=11/p+1/q=1; LpL_pLp​ is the space of real random variables with finite ppp-th moment (identified when equal almost surely) and LqL_qLq​ its dual, paired by E(YZ)\mathbb E(YZ)E(YZ).

For YYY with distribution function G(u)=P{Y≤u}G(u)=\mathbb P\{Y\le u\}G(u)=P{Y≤u}, the quantile function is G−1(p)=inf⁡{u:G(u)≥p}G^{-1}(p)=\inf\{u: G(u)\ge p\}G−1(p)=inf{u:G(u)≥p}, 0<p≤10<p\le10<p≤1, and the average value-at-risk at level 0<α≤10<\alpha\le10<α≤1 is the lower-tail average

AV@Rα(Y)=1α∫0αG−1(u) du.\mathbb{AV@R}_\alpha(Y)=\frac1\alpha\int_0^\alpha G^{-1}(u)\,du .AV@Rα​(Y)=α1​∫0α​G−1(u)du.

The book uses profit variables, so larger values are better and AV@Rα\mathbb{AV@R}_\alphaAV@Rα​ averages the worst α\alphaα-fraction of outcomes; AV@R1(Y)=EY\mathbb{AV@R}_1(Y)=\mathbb EYAV@R1​(Y)=EY.

A real valued A:Lp→R\mathcal A:L_p\to\mathbb RA:Lp​→R is an acceptability functional if it is translation equivariant, A(Y+c)=A(Y)+c\mathcal A(Y+c)=\mathcal A(Y)+cA(Y+c)=A(Y)+c (A1), concave (A2), and monotone, Y(1)≤Y(2)Y^{(1)}\le Y^{(2)}Y(1)≤Y(2) a.s. ⇒A(Y(1))≤A(Y(2))\Rightarrow\mathcal A(Y^{(1)})\le\mathcal A(Y^{(2)})⇒A(Y(1))≤A(Y(2)) (A3). It is version-independent if A(Y(1))=A(Y(2))\mathcal A(Y^{(1)})=\mathcal A(Y^{(2)})A(Y(1))=A(Y(2)) whenever Y(1)Y^{(1)}Y(1) and Y(2)Y^{(2)}Y(2) have the same distribution. A dual representation is

A(Y)=inf⁡{E(YZ)−A(Z):Z∈ZA},ZA⊆Lq,\mathcal A(Y)=\inf\{\mathbb E(YZ)-A(Z): Z\in\mathcal Z_{\mathcal A}\},\qquad \mathcal Z_{\mathcal A}\subseteq L_q,A(Y)=inf{E(YZ)−A(Z):Z∈ZA​},ZA​⊆Lq​,

and (A,ZA)(A,\mathcal Z_{\mathcal A})(A,ZA​) is version-independent if equally distributed Z,Z~Z,\tilde ZZ,Z~ are both or neither in ZA\mathcal Z_{\mathcal A}ZA​, with A(Z)=A(Z~)A(Z)=A(\tilde Z)A(Z)=A(Z~). Theorem 2.45 adds the conditions (C1) A=0A=0A=0, (C2) every Z∈ZAZ\in\mathcal Z_{\mathcal A}Z∈ZA​ is non-negative, (C3) every Z∈ZAZ\in\mathcal Z_{\mathcal A}Z∈ZA​ has EZ=1\mathbb E Z=1EZ=1.

Formalization targets

Goal: Theorem 2.45(i)

Under (C1), (C2) and (C3) there is a family G\mathcal GG of probability measures on (0,1](0,1](0,1], fixed independently of YYY, such that for every Y∈LpY\in L_pY∈Lp​

A(Y)=inf⁡{∫(0,1]AV@Rα(Y) dm(α):m∈G}.(2.37)\mathcal A(Y)=\inf\Big\{\int_{(0,1]}\mathbb{AV@R}_\alpha(Y)\,dm(\alpha): m\in\mathcal G\Big\}. \tag{2.37}A(Y)=inf{∫(0,1]​AV@Rα​(Y)dm(α):m∈G}.(2.37)

Milestones

  • Theorem A.2 (p. 266): on a non-atomic probability space every probability law on a complete separable metric space is the law of some random variable.
  • Proposition 1.8 (p. 11): for given marginals, the covariance is maximal under the comonotone coupling and minimal under the antimonotone coupling.
  • Eq. (2.38) (p. 61): under (C1), A(Y)=inf⁡{∫01F−1(u)G−1(1−u) du:G∈G}\mathcal A(Y)=\inf\{\int_0^1F^{-1}(u)G^{-1}(1-u)\,du: G\in\mathcal G\}A(Y)=inf{∫01​F−1(u)G−1(1−u)du:G∈G}, with FFF the law of YYY and G\mathcal GG the laws of the Z∈ZAZ\in\mathcal Z_{\mathcal A}Z∈ZA​.
  • Theorem 2.45(ii)–(iv) (p. 60): the representations with non-negative measures under (C1)+(C2), with two families of measures under (C1),
A(Y)=inf⁡{∫AV@Rα(Y) dmG(1)(α)−∫AV@R1−α(−Y) dmG(2)(α)},\mathcal A(Y)=\inf\Big\{\int\mathbb{AV@R}_\alpha(Y)\,dm^{(1)}_G(\alpha)-\int\mathbb{AV@R}_{1-\alpha}(-Y)\,dm^{(2)}_G(\alpha)\Big\},A(Y)=inf{∫AV@Rα​(Y)dmG(1)​(α)−∫AV@R1−α​(−Y)dmG(2)​(α)},

and in general with an additional penalty −A~{G}-\tilde A\{G\}−A~{G} and AV@Rα(−Y)\mathbb{AV@R}_\alpha(-Y)AV@Rα​(−Y) in the second integral.

  • Example 2.46, Eq. (2.41) (p. 64): E(Y)−12E∣Y−EY∣=inf⁡{∫(0,1]AV@Rα(Y) dm(α):m∈P(0,1], ∫(0,1)v−1 dm(v)≤1}\mathbb E(Y)-\tfrac12\mathbb E|Y-\mathbb EY|=\inf\{\int_{(0,1]}\mathbb{AV@R}_\alpha(Y)\,dm(\alpha): m\in\mathcal P(0,1],\ \int_{(0,1)}v^{-1}\,dm(v)\le1\}E(Y)−21​E∣Y−EY∣=inf{∫(0,1]​AV@Rα​(Y)dm(α):m∈P(0,1], ∫(0,1)​v−1dm(v)≤1}.

Significance

The result. The Kusuoka representation says that the average values-at-risk are the extreme points of law-invariant acceptability: any such functional is determined by a set of mixing measures on the confidence levels. Consequences used in the rest of the book and in the literature include the identification of comonotone additive functionals with single mixtures (Choquet representations), explicit representations of mean–deviation functionals such as (2.41), and the reduction of optimization problems with law-invariant risk constraints to families of average value-at-risk constraints. The statement for LpL_pLp​, rather than for bounded variables, is what makes it applicable to models with unbounded returns.

Formalizing it. The theorem is proved in the book and in the literature; it has not been machine-checked. Formalizing it requires infrastructure that is reusable beyond this mission: the quantile function and the average value-at-risk on LpL_pLp​, the realization of a prescribed joint law on an arbitrary non-atomic probability space, and the Hardy–Littlewood-type rearrangement inequality behind the antimonotone coupling. Related platform results are in other conventions: a distortion functional of losses on L∞L_\inftyL∞​ as a single mixture of average values-at-risk (MultistageStochastic.distortion_avar_mixture, proved) and Schmeidler's comonotonic characterization on finite uniform spaces (RiskUncSets.Distortion.theorem_4_1, open). Neither covers the infimum over a family, profit variables, or LpL_pLp​.

Difficulty

The obvious argument is to write each Z∈ZAZ\in\mathcal Z_{\mathcal A}Z∈ZA​ as a mixing measure directly. This fails because E(YZ)\mathbb E(YZ)E(YZ) depends on the joint law of (Y,Z)(Y,Z)(Y,Z), not on the two marginals; the infimum must first be reduced to antimonotone couplings, which requires (a) that every coupling of the two marginals can be realized on the given space without leaving ZA\mathcal Z_{\mathcal A}ZA​, using version-independence of both A\mathcal AA and (A,ZA)(A,\mathcal Z_{\mathcal A})(A,ZA​) and non-atomicity, and (b) the extremal property of the antimonotone coupling for products of an LpL_pLp​ and an LqL_qLq​ variable, where quantile functions may be unbounded at both ends. The passage from G−1(1−u)G^{-1}(1-u)G−1(1−u) to a mixing measure is a Stieltjes integration by parts on (0,1)(0,1)(0,1) that must handle a point mass at 111, and the integrability of α↦AV@Rα(Y)\alpha\mapsto\mathbb{AV@R}_\alpha(Y)α↦AV@Rα​(Y), which tends to the essential infimum of YYY (possibly −∞-\infty−∞) as α→0\alpha\to0α→0. Non-atomicity cannot be dropped: the book's Counterexample on p. 63 is a version-independent functional on a two-point space without representation (2.37).

Formalization scope

Probability spaces are (Ω, ℱ, P) with IsProbabilityMeasure P; non-atomicity is the book's notion (no atoms), which is stronger than Mathlib's NoAtoms. Random variables are elements of Lp ℝ p P with 1 ≤ p, p ≠ ⊤, and dual variables elements of Lp ℝ q P with p.HolderConjugate q. The quantile function is the left-continuous inverse of the book's (1.3), evaluated only on (0,1)(0,1)(0,1) or inside integrals over (0,α](0,\alpha](0,α]; AV@Rα\mathbb{AV@R}_\alphaAV@Rα​ is the lower-tail average (2.15), not the upper-tail loss CVaR. Version-independence is "equal laws give equal values" (IdentDistrib). Every infimum is stated as a greatest lower bound in R\mathbb RR (IsGLB), which forces the indexing set to be nonempty and bounded below; measures on (0,1](0,1](0,1] are measures on R\mathbb RR with no mass outside (0,1](0,1](0,1]. The family G\mathcal GG is quantified before YYY: a family allowed to depend on YYY would reduce (2.37) to matching the single number A(Y)\mathcal A(Y)A(Y) by some mixture, a much weaker statement, and that reading is excluded. Each representation also asserts that every integrand is integrable against every measure of the family, so that no integral can take Lean's default value 000.

Beyond the paper. Two variant items accompany the goal. kusuoka_representation_strong ([Strengthened]) drops (C2) and (C3): for a real valued acceptability functional they follow from (A1), (A3) and the dual representation, since E(YZ)≥A(Y)\mathbb E(YZ)\ge\mathcal A(Y)E(YZ)≥A(Y) for every YYY forces EZ=1\mathbb EZ=1EZ=1 (constants) and Z≥0Z\ge0Z≥0 (scaled indicators). kusuoka_representation_probe ([Sharpness probe]) drops non-atomicity; it is expected to be false by the p. 63 Counterexample, and a disproof is the sought outcome. The printed proof of Theorem 2.45(iii) has a sign gap (it derives +∫AV@R1−α(−Y) dm(2)+\int\mathbb{AV@R}_{1-\alpha}(-Y)\,dm^{(2)}+∫AV@R1−α​(−Y)dm(2)); the statements (iii) and (iv) are kept as printed.

Contributions welcome: the quantile transform and realization of joint laws on non-atomic spaces, the rearrangement inequality on Lp×LqL_p\times L_qLp​×Lq​, and the integration-by-parts construction of the mixing measure, each of which can be submitted as a separate lemma.

Selected references

  • G. Ch. Pflug, W. Römisch, Modeling, Measuring and Managing Risk, World Scientific, 2007, §2.2.4 and Appendix A. https://doi.org/10.1142/6478
  • S. Kusuoka, On law invariant coherent risk measures, Advances in Mathematical Economics 3, 83–95, 2001. https://doi.org/10.1007/978-4-431-67891-5_4
  • W. Hoeffding, Masstabinvariante Korrelationstheorie, Schriften des Mathematischen Instituts der Universität Berlin 5, 179–233, 1940.
  • S. T. Rachev, Probability Metrics and the Stability of Stochastic Models, Wiley, 1991 (Lemma 2.5.1, cited for Theorem A.2).
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Stochastic Networks XV: Positive Recurrence under MaxWeight SchedulingTextbook

Scheduling shared service capacity

A switch or wireless network can have several queues ready for service while its hardware permits only certain combinations to be served together. A scheduler must choose a feasible combination repeatedly as new packets arrive. The question is whether this local sequence of decisions keeps the queue process stable whenever the arrival rates fit within the network's service capacity. Kelly and Yudovina formulate this question for finite service schedules and independent Poisson arrivals in §7.8 of Stochastic Networks.

MaxWeight scheduling gives larger queues greater influence over the choice of schedule. An exponent controls how strongly queue length affects priority. The chapter's target is a stability guarantee for every positive exponent, rather than a guarantee confined to the familiar linear weighting. The supplied Lecture Notes PDF states this as Theorem 7.13, printed page 180, and develops supporting analytic questions in Appendix D.

The queueing model

Let RRR be a finite nonempty set of queues. A schedule is a vector σ∈NR\sigma\in\mathbb N^Rσ∈NR describing how many packets each queue can serve in one time slot. The feasible schedule family SSS is finite and nonempty. It is downward closed: reducing any schedule coordinate leaves a feasible schedule. This includes the possibility of unused service when a selected queue has fewer packets than the schedule permits.

The admissible region is

Λ={v∈RR:v≥0, ∃(cσ)σ∈S, cσ≥0, ∑σ∈Scσ=1, v≤∑σ∈Scσσ}.\Lambda=\left\{v\in\mathbb R^R:v\ge0,\ \exists(c_\sigma)_{\sigma\in S},\ c_\sigma\ge0,\ \sum_{\sigma\in S}c_\sigma=1,\ v\le\sum_{\sigma\in S}c_\sigma\sigma\right\}.Λ={v∈RR:v≥0, ∃(cσ​)σ∈S​, cσ​≥0, σ∈S∑​cσ​=1, v≤σ∈S∑​cσ​σ}.

It describes arrival rates dominated by an average of feasible schedules. The interior used here is the ordinary interior in RR\mathbb R^RRR.

Fix α>0\alpha>0α>0. At queue vector qqq, a schedule is drawn from a fixed probability distribution supported on the maximizers of ∑rσrqrα\sum_r\sigma_rq_r^\alpha∑r​σr​qrα​. New arrivals ArA_rAr​ in the slot are independent Poisson variables of means λr\lambda_rλr​, independent of the scheduling randomization and the past. The next queue vector is

qr′=(qr−σr)++Ar.q'_r=(q_r-\sigma_r)^++A_r.qr′​=(qr​−σr​)++Ar​.

These laws specify a homogeneous Markov chain on the countable state space NR\mathbb N^RNR. They follow the general model in §7.8 and the explicit empty-queue convention in Example D.4, printed page 213.

Formalization targets

The goal is Theorem 7.13: for λ∈int⁡Λ\lambda\in\operatorname{int}\Lambdaλ∈intΛ, the MaxWeight-α\alphaα queue chain is positive recurrent. In return-time notation,

∀q∈NR,Eq[τq+]<∞,τq+=inf⁡{n≥1:q(n)=q}.\forall q\in\mathbb N^R,\qquad \mathbb E_q[\tau_q^+]<\infty,\qquad \tau_q^+=\inf\{n\ge1:q(n)=q\}.∀q∈NR,Eq​[τq+​]<∞,τq+​=inf{n≥1:q(n)=q}.

This retains every positive value of α\alphaα and the full queue process.

Three supporting targets are selected from the same supplied source. Proposition D.1 states the Foster–Lyapunov criterion for an irreducible countable chain and an arbitrary finite exception set. A nonnegative function with drift at most −ϵ-\epsilon−ϵ outside that set and at most b−ϵb-\epsilonb−ϵ inside it yields finite expected return to the set from every starting state and positive recurrence.

Exercise 7.18 concerns the weighted drift

D(q)=∑rqrαE[qr′−qr∣q].D(q)=\sum_rq_r^\alpha\mathbb E[q'_r-q_r\mid q].D(q)=r∑​qrα​E[qr′​−qr​∣q].

It asks for constants ϵ,K>0\epsilon,K>0ϵ,K>0 and finite bbb such that

∥q∥2>K  ⟹  D(q)<−ϵ∥q∥2α,∥q∥2≤K  ⟹  D(q)<b.\|q\|_2>K\implies D(q)<-\epsilon\|q\|_2^\alpha,\qquad \|q\|_2\le K\implies D(q)<b.∥q∥2​>K⟹D(q)<−ϵ∥q∥2α​,∥q∥2​≤K⟹D(q)<b.

Exercise D.1(3) asks for finite moments of Y=max⁡(A,B)Y=\max(A,B)Y=max(A,B), where BBB is a finite service bound and AAA is Poisson, and for the tail term

E ⁣[(∣(1+Y/K)α+1∣+1)1{Y>δK}]\mathbb E\!\left[\left(\left|(1+Y/K)^{\alpha+1}\right|+1\right)\mathbf1_{\{Y>\delta K\}}\right]E[(​(1+Y/K)α+1​+1)1{Y>δK}​]

to tend to zero as K→∞K\to\inftyK→∞ for fixed δ>0\delta>0δ>0. The source locations are printed pages 210–211, 182, and 214–215 respectively.

What the result establishes

The recurrence conclusion concerns repeated operation over an unlimited number of slots. It asserts a finite mean return time to each queue state under the specified policy. It does not require an explicit formula for the stationary distribution, nor does it prescribe a numerical delay guarantee. The result therefore identifies a capacity regime in which this queue-based scheduling rule is stable, while leaving performance within that regime as a separate question.

The formalization contribution is the connection between a concrete random scheduling transition law and recurrence on an infinite state space. Its reusable components include the capacity region of finite schedules, capped-service queue transitions, extended return expectations, and the Poisson envelope estimates. The textbook presents the theorem as an established result with a proof sketch. The theorem items here are statements awaiting proofs; compilation verifies their Lean syntax and types, not their mathematical proofs.

Where faithfulness requires care

Negative drift by itself is insufficient for the recurrence conclusion. The distinctions between negative drift, drift bounded away from zero, and control of upward increments matter in the chapter's discussion, printed pages 180–181. Arbitrary positive real exponents also require attention at empty queues and to unbounded Poisson arrivals.

The sketch's equality between actual departures and a chosen schedule fails when a positive queue is shorter than the proposed service. This is a proof gap, not a counterexample to the stability theorem. Appendix D additionally switches between conditioning on the full vector and conditioning on one coordinate in (D.5). Those conditional expectations need not agree for coupled schedules. The selected statements retain actual capped departures and avoid relying on that ambiguous display. Completing the analytic link to the goal remains part of the proof task.

Formalization scope

Queue and schedule coordinates are natural numbers, rates are nonnegative real numbers, and the exponent is an arbitrary positive real. The schedule family is a finite set of vectors. Random tie rules are stationary probability kernels supported on the maximizing schedules; the source specifies no particular distribution among ties. The norm in Exercise 7.18 is made Euclidean explicitly. Constants there are chosen before the queue vector is quantified, so they cannot depend on the current state or time.

Return times are represented by extended nonnegative sums of survival probabilities. Consequently, an event of never returning has infinite expected cost. Real drift sums have explicit absolute-integrability conditions. In the queue drift and Poisson moment items, integrability is a conclusion, not an assumed substitute for analysis. The Poisson tail term is an unconditional tail integral, including when its conditioning event would have probability zero.

No selected statement contains an unspecified O(⋅)O(\cdot)O(⋅) term or a high-probability claim; there are therefore no numerical asymptotic constants to instantiate. Exercise D.1 is included only through its explicitly numbered part (3). The remaining parts, (D.5), congestion-control optimization results, and the switch-specific matching example are outside this mission's theorem list. No variants are posed.

Stability is not defined as negative drift, and the goal is not restricted to α=1\alpha=1α=1 or a finite truncation of the queue space. Mathlib supplies probability mass functions, product measures, Poisson laws, real powers, and topology. The local definitions supply the scheduling and recurrence interfaces needed to state the targets.

Selected references

  • F. P. Kelly and E. Yudovina, Stochastic Networks, Cambridge University Press, 2014. DOI: 10.1017/CBO9781139565363. Exact indices and quotations refer to the supplied Lecture Notes on Stochastic Networks PDF, SHA-256 ec271d555059aee58613e5e9a98b8346214b16185c527314f5d94c1ac8b17b6a; correspondence with a particular published printing has not been verified.
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Stochastic Networks XIII: The Capacity Region of Distributed Random AccessTextbook

Motivation

Stations sharing a communication channel must decide when to transmit. If nearby stations transmit together, their signals may interfere; if they all wait, capacity is wasted. A central scheduler can coordinate activity, but distributed access assigns decisions to individual stations. The mathematical question is whether simple random local decisions can supply all the service combinations that the interference constraints permit. This mission concerns the idealized continuous-time model in Section 5.4 of Kelly and Yudovina, Stochastic Networks, using the supplied Lecture Notes PDF.

The model isolates a capacity question from implementation issues. Stations sense active neighbors immediately, so collisions do not occur. Transmission durations and attempt clocks are exponential. The question concerns the equilibrium activity of this process for fixed parameters. Delayed sensing, packet queues, and parameter adaptation require additional results and are outside the theorem's claim.

Setting

An interference graph is a finite simple undirected graph whose vertices are stations. An edge means that its two endpoints cannot transmit together. Write RRR for the station set and SSS for the set of binary activity vectors n=(nr)r∈Rn=(n_r)_{r\in R}n=(nr​)r∈R​ satisfying this restriction. The value nr=1n_r=1nr​=1 means that station rrr is transmitting. The all-zero vector is always feasible.

Each station has a finite real parameter θr\theta_rθr​. An active station stops transmitting at rate 111. An inactive station starts at rate exp⁡(θr)\exp(\theta_r)exp(θr​) when all its neighbors are inactive. These transitions define a continuous-time Markov chain on SSS. Its generator is QQQ, with negative total outgoing rates on the diagonal, and its transition matrices are P(t)=exp⁡(tQ)P(t)=\exp(tQ)P(t)=exp(tQ) for t≥0t\ge0t≥0.

A distribution ppp on feasible schedules offers mean activity ∑np(n)nr\sum_n p(n)n_r∑n​p(n)nr​ at station rrr. The capacity region includes every nonnegative arrival vector that some such distribution can dominate:

Λ={λ≥0:∃p≥0,∑n∈Sp(n)=1,∑n∈Sp(n)nr≥λr(r∈R)}.\Lambda=\left\{\lambda\ge0:\exists p\ge0,\quad\sum_{n\in S}p(n)=1,\quad \sum_{n\in S}p(n)n_r\ge\lambda_r\quad(r\in R)\right\}.Λ={λ≥0:∃p≥0,n∈S∑​p(n)=1,n∈S∑​p(n)nr​≥λr​(r∈R)}.

This definition permits arbitrary distributions on feasible schedules. The random-access process produces a much more specific family, indexed by one real number per station.

Formalization targets

Equation (5.8) identifies the stationary distribution of the specified chain:

πθ(n)=exp⁡(∑rnrθr)∑m∈Sexp⁡(∑rmrθr),πθP(t)=πθ(t≥0).\pi_\theta(n)=\frac{\exp(\sum_r n_r\theta_r)}{\sum_{m\in S}\exp(\sum_r m_r\theta_r)}, \qquad \pi_\theta P(t)=\pi_\theta\quad(t\ge0).πθ​(n)=∑m∈S​exp(∑r​mr​θr​)exp(∑r​nr​θr​)​,πθ​P(t)=πθ​(t≥0).

The goal is Theorem 5.17, printed page 126 of the supplied PDF. Every arrival vector in the ordinary interior of Λ\LambdaΛ has strictly smaller coordinates than the equilibrium service vector for some finite parameters:

λ∈int⁡Λ⟹∃θ∈RR,λr<∑n∈Snrπθ(n)(r∈R).\lambda\in\operatorname{int}\Lambda \quad\Longrightarrow\quad \exists\theta\in\mathbb R^R,\quad \lambda_r<\sum_{n\in S}n_r\pi_\theta(n)\quad(r\in R).λ∈intΛ⟹∃θ∈RR,λr​<n∈S∑​nr​πθ​(n)(r∈R).

Three Appendix C milestones supply the accompanying optimization statements. For a convex objective fff and componentwise convex constraint map hhh on a convex set XXX, Theorem C.7 asserts convexity of the extended value function ϕ(b)=inf⁡{f(x):x∈X,h(x)≤b}\phi(b)=\inf\{f(x):x\in X,h(x)\le b\}ϕ(b)=inf{f(x):x∈X,h(x)≤b}. Theorem C.3 supplies a nonvertical support at an interior point of its finite-value domain. Theorem C.4 states the equivalence between such support and the strong Lagrangian principle for equality constraints, with

Lb(x;y)=f(x)+yT(b−h(x)),ϕ(b)=inf⁡x∈XLb(x;y).L_b(x;y)=f(x)+y^T(b-h(x)),\qquad \phi(b)=\inf_{x\in X}L_b(x;y).Lb​(x;y)=f(x)+yT(b−h(x)),ϕ(b)=x∈Xinf​Lb​(x;y).

The faithful C.4 statement is retained without an unprinted finiteness hypothesis. Its infinite-value defect and the separately labelled correction are described below. The goal itself retains the source's strict service inequalities.

Significance

The capacity theorem says that the exponential random-access family does not leave a gap inside the region attainable by arbitrary mixtures of independent schedules. It provides a service margin in every coordinate at once. Its quantifiers allow the parameters to depend on the graph and arrival vector, but require every parameter to remain a finite real number. The theorem does not provide a uniform parameter bound as the arrival vector approaches the boundary.

The known mathematical result is attributed to Jiang and Walrand in the supplied source. The formalization target is a checked statement of that result and its supporting mathematical interfaces. The proposal's theorem declarations remain proof tasks. The finite exclusion process, its invariant law, and the distinction between feasible schedule mixtures and exponential-family marginals are reusable in later work on scheduling. The extended-value optimization layer can also support problems unrelated to communication networks.

Difficulty

Normalizing positive exponential weights only constructs a probability distribution. It does not establish that the distribution is invariant under the given dynamics, nor that its marginal vectors cover every strictly feasible demand. Changing one station's parameter changes the other stations' equilibrium opportunities through interference. Coordinatewise scalar tuning therefore does not settle simultaneous coverage.

The optimization statements require care at infeasible and unbounded problems. A real-valued infimum with a default value would conceal these cases. In particular, the literal C.4 equivalence fails for an empty domain: both primal and Lagrangian infima are +∞+\infty+∞, but no finite-height hyperplane touches that value. This is an issue with the unrestricted statement, not a new hypothesis for the capacity theorem.

Formalization scope

Stations are indexed by Fin d, and activity coordinates by Fin 2. Simple graphs enforce symmetry and exclude self-interference. A decidability instance is computational bookkeeping for a finite adjacency relation. The empty station set is permitted: it has one empty schedule, and the service conclusion has no coordinates. For one station the mean activity is exp⁡(θ)/(1+exp⁡(θ))\exp(\theta)/(1+\exp(\theta))exp(θ)/(1+exp(θ)). All normalizing sums are finite and strictly positive because the empty schedule contributes weight one.

Interior means ambient Euclidean interior. Arrival vectors in the closed region alone are insufficient: at the one-station boundary demand λ=1\lambda=1λ=1, no finite parameter supplies service greater than one. Finding F1 records this sharpness example; no extra sharpness item is posed.

The CTMC is represented by its finite generator and matrix-exponential transition semigroup. Its stationary-law theorem asserts invariance for every nonnegative time. Optimization infima use EReal, so infeasibility gives +∞+\infty+∞ and unboundedness below gives −∞-\infty−∞. Convexity is expressed through the real epigraph; supporting affine functions have real heights and slopes. Slack elimination in (C.2) preserves the inequality h(x)≤bh(x)\le bh(x)≤b. No asymptotic constants or failure probabilities require instantiation in these targets.

Beyond the paper. The single corrected variant of C.4 adds exactly that ϕ(b)\phi(b)ϕ(b) is finite. Finding F2 gives the empty-domain counterexample to the unrestricted equivalence and the supporting argument for the correction. The original remains the milestone anchor. Findings F3 and F4 separately record the slack-multiplier sign error on printed page 209 and the word “maximized” in the minimization argument on printed page 127; neither changes the goal or creates a variant.

The definitions have concrete mathematical bodies without proof placeholders. The theorem types expose their defining formulas for independent auditing, and use Mathlib's finite sums, graph types, topology, convexity, extended reals, and matrix exponential. A formulation that assumes the desired service vector or proves only normalization would not capture this mission.

Selected references

  • F. P. Kelly and E. Yudovina, Stochastic Networks, Cambridge University Press, 2014. DOI. All numbered claims and page citations refer to the supplied Lecture Notes on Stochastic Networks PDF: Section 5.4, printed pages 125–128 (PDF pages 133–136), and Appendix C, printed pages 207–209 (PDF pages 215–217). Equivalence of this supplied file to a particular published printing is unverified.
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Robust Optimization XIII: Exact Quadratic Decision Rules on EllipsoidsTextbook

Decisions made with partial information

An adjustable decision is a rule that responds to information revealed after an optimization problem is specified. In production planning, for example, a later quantity may depend on observed demand, while an earlier commitment must remain constant. A robust counterpart requires the resulting decisions to satisfy the constraints for every realization in a prescribed uncertainty set. The information available to each decision is part of the model: observing one linear combination of uncertain data does not permit a policy to use all the data coordinates.

Quadratic rules provide a finite family of responses with more flexibility than affine rules. The resulting robust constraints still quantify over infinitely many uncertain realizations. This mission concerns the case in which that infinite family has an exact finite semidefinite representation: fixed recourse and ellipsoidal uncertainty, as stated in Corollary 14.3.8 of Ben-Tal, El Ghaoui and Nemirovski. The result is about optimization over the selected quadratic rules; it makes no claim that these rules attain the best value among all possible responses.

The model and the information available to a policy

Let z∈RLz\in\mathbb R^Lz∈RL denote the uncertain data and let

Z={z:∥Qz∥2≤1},Q∈Rr×L,ker⁡Q={0}.Z=\{z:\|Qz\|_2\le1\},\qquad Q\in\mathbb R^{r\times L},\quad\ker Q=\{0\}.Z={z:∥Qz∥2​≤1},Q∈Rr×L,kerQ={0}.

The uncertain linear problem has nnn decision variables and mmm constraint rows:

min⁡x{c(z)Tx+d(z):A(z)x≥b(z)}.\min_x\{c(z)^Tx+d(z):A(z)x\ge b(z)\}.xmin​{c(z)Tx+d(z):A(z)x≥b(z)}.

All four data functions are affine in zzz. For variable jjj, a specified matrix Pj∈Rkj×LP_j\in\mathbb R^{k_j\times L}Pj​∈Rkj​×L determines its observations. A quadratic decision rule has the form

Xj(z)=pj+qjTPjz+(Pjz)TRj(Pjz).X_j(z)=p_j+q_j^TP_jz+(P_jz)^TR_j(P_jz).Xj​(z)=pj​+qjT​Pj​z+(Pj​z)TRj​(Pj​z).

The optimization variables are the coefficients pj,qj,Rjp_j,q_j,R_jpj​,qj​,Rj​ and an objective threshold ttt. The matrices PjP_jPj​ are fixed data. The coefficient matrices RjR_jRj​ are unrestricted: using full arrays retains every quadratic polynomial, with harmless redundancy in their skew-symmetric parts. If Pj=0P_j=0Pj​=0, the policy is constant.

Fixed recourse means that whenever Pj≠0P_j\ne0Pj​=0, both cj(z)c_j(z)cj​(z) and column Aj(z)A_j(z)Aj​(z) are independent of zzz. Coefficients of nonadjustable variables may still be uncertain. This is Definition 14.3.1, printed p. 371, including the condition on the objective. Robust epigraph feasibility means that A(z)X(z)≥b(z)A(z)X(z)\ge b(z)A(z)X(z)≥b(z) and c(z)TX(z)+d(z)≤tc(z)^TX(z)+d(z)\le tc(z)TX(z)+d(z)≤t hold for every z∈Zz\in Zz∈Z.

Formalization targets

The supporting geometric target is Lemma 14.3.7, printed p. 384. The quadratic lift of zzz is the symmetric matrix with top-left entry zero, first column [0;z][0;z][0;z], and lower-right block zzTzz^TzzT. Its ordinary convex hull is compact and satisfies

conv⁡{[0zTzzzT]:z∈Z}={[0vTvW]:[1vTvW]⪰0, Tr⁡(QWQT)≤1}.\operatorname{conv}\left\{\begin{bmatrix}0&z^T\\z&zz^T\end{bmatrix}:z\in Z\right\} =\left\{\begin{bmatrix}0&v^T\\v&W\end{bmatrix}:\begin{bmatrix}1&v^T\\v&W\end{bmatrix}\succeq0,\ \operatorname{Tr}(QWQ^T)\le1\right\}.conv{[0z​zTzzT​]:z∈Z}={[0v​vTW​]:[1v​vTW​]⪰0, Tr(QWQT)≤1}.

The goal is Corollary 14.3.8. For every policy coefficient vector and threshold, robust epigraph feasibility is equivalent to feasibility of the explicit SDP after adding one nonnegative multiplier for each constraint row and one for the objective row. If the signed slack in row iii is written αi+βiTz+zTΓiz\alpha_i+\beta_i^Tz+z^T\Gamma_i zαi​+βiT​z+zTΓi​z, its matrix constraint is

[αi−λiβiT/2βi/2Γi+λiQTQ]⪰0,λi≥0.\begin{bmatrix}\alpha_i-\lambda_i&\beta_i^T/2\\\beta_i/2&\Gamma_i+\lambda_iQ^TQ\end{bmatrix}\succeq0,\qquad\lambda_i\ge0.[αi​−λi​βi​/2​βiT​/2Γi​+λi​QTQ​]⪰0,λi​≥0.

The model defines these coefficients directly from the original data and the observation matrices. The theorem also asserts that the matrices depend affinely on the SDP decision vector. There are m+1m+1m+1 matrix constraints of order L+1L+1L+1, and

N=1+∑j(1+kj+kj2)+(m+1)N=1+\sum_j(1+k_j+k_j^2)+(m+1)N=1+j∑​(1+kj​+kj2​)+(m+1)

scalar decision variables. With K=∑jkjK=\sum_jk_jK=∑j​kj​, the bound N≤1+n(1+K+K2)+(m+1)N\le1+n(1+K+K^2)+(m+1)N≤1+n(1+K+K2)+(m+1) and the corresponding dense matrix coefficient bound make the polynomial-size conclusion explicit.

What the exact representation provides

The equivalence retains every original policy coefficient and objective threshold. It therefore preserves the entire robust feasible epigraph, including instances with no feasible policy and optimization problems whose values are unbounded. The goal also states equality of attainable thresholds and preservation of minimizers for the same linear objective ttt in the finite SDP. It does not assume that either problem has a minimizer. Equality of a pair of real-valued infima would express less information and could conceal degenerate cases.

The mathematical results are established in the textbook. This mission supplies open Lean theorem statements for their formal verification and concrete definitions for their objects. The homogeneous S-lemma and the inhomogeneous S-procedure are already Proved on Prove2Me and are retained as references. The moment-hull identity and the complete quadratic-policy representation are the new targets. Their definition layer can also support work on polynomial policies and other lifted uncertainty sets.

Difficulty

Checking a quadratic constraint on an ellipsoid is a global requirement. Evaluating it at a finite collection of sample points does not establish the required universal inequality. Likewise, the image of a convex uncertainty set under the quadratic lift is generally not convex. The target must identify its whole convex hull, including compactness and boundary points.

The formalization must also preserve information restrictions through every matrix coefficient. Full observation cannot replace PjzP_jzPj​z, even if the resulting semidefinite program is easier to describe. The objective has uncertain affine data and participates in the same robust requirement as the constraints. These issues distinguish the complete statement from a single quadratic inequality or a result that assumes all coefficient columns are certain.

Formalization scope

All spaces and matrices are finite dimensional over the reals. The code uses finite functions for coordinates, but defines the uncertainty set through a sum of squares, so the norm is Euclidean. Matrix indices have a distinguished first coordinate. The unshifted lift has zero there; the positive-semidefinite moment block has one. Positive semidefiniteness also enforces symmetry of the moment matrix.

The model, uncertainty set, policy evaluation, original robust epigraph, and proposed SDP constraints are separate concrete definitions. Neither feasibility equivalence nor the moment-hull identity is assumed in the definitions. The theorem quantifies over every finite dimension, including zero; an empty observation list produces a constant policy. No division by a dimension or a policy-dependent denominator occurs.

The polynomial-size statement concerns the explicit real SDP representation, as in the book. It does not add a machine model or a bit-complexity theorem for an SDP solver. The formalization uses full quadratic coefficient arrays, so its stated counts need not be minimal. The bound includes all these redundant coefficients. There are no optional variants in this mission. The recorded sharpness observation about QQQ explains why its injectivity is retained in the compactness theorem.

Selected references

  • A. Ben-Tal, L. El Ghaoui and A. Nemirovski, Robust Optimization, Princeton University Press, 2009. DOI: 10.1515/9781400831050. Definition 14.3.1, printed p. 371; equation (14.3.6), printed p. 375; Lemma 14.3.7 and Corollary 14.3.8, printed pp. 384–385. The pinned PDF pages are respectively 397, 401, and 410–411.
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Robust Optimization XIV: Extreme-Scenario Reduction in Multistage InventoryTextbook

Inventory decisions under uncertain demand

An inventory manager chooses replenishment orders before knowing all future demand. Orders made today affect both the stock available tomorrow and the cost of later decisions. A flexible commitment contract adds another consideration: deviations from previously announced orders can incur penalties. The uncertainty therefore concerns a sequence of observations, and the object being optimized is a sequence of decision rules. Chapter 15 of Ben-Tal, El Ghaoui and Nemirovski, Robust Optimization uses this setting to compare the cost of unrestricted adaptive policies with the cost of affine policies.

For such a comparison, an exact benchmark matters. Evaluating a policy against every trajectory in a continuous uncertainty set can require infinitely many constraints. The chapter's Lemma 15.2.1 identifies a class of problems whose optimal value is preserved by restricting uncertainty to finitely many extreme scenarios. This mission formalizes that general lemma, which the book applies to inventory management, rather than the numerical experiments or a particular contract data set.

A multistage convex model

A history at stage ttt is the tuple dt−1=(d0,…,dt−1)d^{t-1}=(d_0,\ldots,d_{t-1})dt−1=(d0​,…,dt−1​), where each observation djd_jdj​ is a real vector of dimension njn_jnj​. A policy specifies a real decision vector St(dt−1)S_t(d^{t-1})St​(dt−1) of dimension mtm_tmt​ for every possible history. Dependence only on observations already available is called nonanticipativity. Two full trajectories with identical observed prefixes necessarily produce the same decision at that stage.

There are T+1T+1T+1 decision stages and uncertainty sets F0,…,FTF_0,\ldots,F_TF0​,…,FT​. All data except the observations are fixed. Linear maps At,Bt+1,Ct+1A_t,B_{t+1},C_{t+1}At​,Bt+1​,Ct+1​ and vectors btb_tbt​ impose the initial and linking inequalities

A1S1(d0)≥b1,A_1S_1(d^0)\ge b_1,A1​S1​(d0)≥b1​, At+1St+1(dt)≥Bt+1dt+Ct+1St(dt−1)+bt+1,1≤t≤T.A_{t+1}S_{t+1}(d^t)\ge B_{t+1}d^t+C_{t+1}S_t(d^{t-1})+b_{t+1},\qquad 1\le t\le T.At+1​St+1​(dt)≥Bt+1​dt+Ct+1​St​(dt−1)+bt+1​,1≤t≤T.

Vector inequalities hold coordinatewise. The term Bt+1dtB_{t+1}d^tBt+1​dt uses the whole observed prefix. A fixed real bound RRR restricts the infinity norm of each decision at stages 1,…,T1,\ldots,T1,…,T. The terminal decision ST+1S_{T+1}ST+1​ still appears in the last linking constraint, but the printed norm restriction does not cover it.

Each decision incurs a stage cost ftf_tft​. The costs are lower semicontinuous convex functions with polyhedral effective domains. A cost may be +∞+\infty+∞ outside its domain; within the domain it is finite. Polyhedrality of the domain does not require the cost itself to be piecewise linear. The total cost includes all T+1T+1T+1 stages.

Formalization target

Write Opt⁡(F0,…,FT)\operatorname{Opt}(F_0,\ldots,F_T)Opt(F0​,…,FT​) for the infimum of all real bounds EEE for which some policy satisfies the preceding constraints and

∑t=1T+1ft(St(dt−1))≤Efor every dT∈F0×⋯×FT.\sum_{t=1}^{T+1}f_t(S_t(d^{t-1}))\le E \qquad\text{for every }d^T\in F_0\times\cdots\times F_T.t=1∑T+1​ft​(St​(dt−1))≤Efor every dT∈F0​×⋯×FT​.

For nonempty polytopes Dt⊂RntD_t\subset\mathbb R^{n_t}Dt​⊂Rnt​, the target is the complete value equality in Lemma 15.2.1, printed p. 430:

Opt⁡(D0,…,DT)=Opt⁡(Ext⁡D0,…,Ext⁡DT).\operatorname{Opt}(D_0,\ldots,D_T) =\operatorname{Opt}(\operatorname{Ext}D_0,\ldots,\operatorname{Ext}D_T).Opt(D0​,…,DT​)=Opt(ExtD0​,…,ExtDT​).

Here Ext⁡D\operatorname{Ext}DExtD denotes the set of extreme points of DDD. Both sides optimize over unrestricted nonanticipative policies. The target does not restrict those policies to affine rules, assert that every fixed policy has its worst cost at an extreme trajectory, or assert attainment of the optimum. The source states this lemma without a local numbered proof sequence, so the mission has one goal and its concrete model definitions, with no additional milestone chain.

What the result makes possible

For interval uncertainty, the extreme observations are interval endpoints. The book uses this consequence to replace a box of demand trajectories by a finite scenario set. It then describes a finite optimization problem whose decisions must agree whenever their available information agrees. These are exact comparisons of optimal values for the specified models, not estimates of sampling error. The number of scenarios can still grow exponentially with the horizon, as the chapter discusses on printed pp. 430–432 of the source.

The formalization makes the policy information pattern, terminal-stage treatment, and extended-value convention explicit. These details are useful beyond the inventory application because the lemma permits arbitrary compatible linear constraints and convex stage costs. The current artifacts state the known textbook result in Lean; a successful statement build is not a proof of the lemma. The reusable definitions are concrete and contain no unproved mathematical assertions.

Why the statement requires care

The uncertainty set is a product, but decisions at different stages are connected by constraints. A decision chosen for one trajectory cannot be chosen independently of another trajectory sharing the same history. Consequently, a statement about a single convex function on a polytope does not by itself express the multistage result. The target must retain the order of policy choice and universal quantification over trajectories, the complete cost sum, and the information available at each decision.

The final stage introduces a separate boundary issue: its cost and feasibility constraints remain present even though the printed bound stops one stage earlier. Omitting the final cost or extending the bound would change the problem. Degenerate and infeasible instances also require a value convention that does not assign them an arbitrary real number.

Formalization scope

Lean represents observations and decisions by finite real coordinate spaces, with dimensions allowed to vary by stage. Histories are finite dependent tuples; a policy's argument type contains exactly the observed prefix. Linear maps represent the book's matrices, including maps from stacked histories. Nonempty polytopes are convex hulls of nonempty finite sets, allowing singletons and lower-dimensional polytopes. The cost-domain predicate uses finitely many nonstrict matrix inequalities.

The extended optimal value is an EReal infimum of achievable real objective bounds. An empty set of bounds gives +∞+\infty+∞, while bounds unbounded below give −∞-\infty−∞. No subtraction of infinities occurs. Regular costs exclude −∞-\infty−∞, so the finite sum in the objective has no mixed-infinity ambiguity. The definition does not assume feasibility, boundedness below, or attainment. Zero horizon and zero-dimensional coordinate spaces follow the same displayed formulas.

Formalization Note No singleton assumption is placed on D0D_0D0​, and no measurability, continuity, or affine restriction is imposed on policies. The theorem expands its concrete model for independent auditing. A Lean type check verifies agreement with the separately named reusable definitions. The required mathematical infrastructure includes convex hulls, extreme points, lower semicontinuity, finite linear algebra, and extended-real order. Completion requires a proof of the stated value equality with precisely these hypotheses.

Selected references

  • A. Ben-Tal, L. El Ghaoui and A. Nemirovski, Robust Optimization, Princeton University Press, 2009, Chapter 15, §15.2.4.1, Lemma 15.2.1, printed p. 430 (PDF p. 456). DOI: 10.1515/9781400831050.
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Robust Optimization XI: Finite Reformulations of Worst-Case Convex LossTextbook

Robust fitting with uncertain measurements

Regression and classification fit a parameter vector to observed data. When measurements can vary within a prescribed set, a fit judged only at the nominal observations need not control its loss on the possible data. A worst-case loss constraint requires the loss bound to hold for every admissible matrix of measurements. Such a requirement can contain infinitely many inequalities even when the parameter vector has finitely many coordinates. Chapter 12 of Ben-Tal, El Ghaoui and Nemirovski, Robust Optimization (2009) identifies structural assumptions under which this requirement has an exact finite convex representation.

This mission concerns the representation in Theorem 12.2.5. Its application is to robust fitting problems whose uncertainty support function separates into a feature-dependent factor and the infinity norm of a residual-space vector. The result applies to both symmetric losses, such as norms of regression residuals, and asymmetric losses formed from positive residual parts.

Data, residuals, and loss

Let n,ℓ,mn,\ell,mn,ℓ,m be positive integers. The nominal data matrix Zn∈Rn×mZ^n\in\mathbb R^{n\times m}Zn∈Rn×m has one column per measurement and one row per feature. For a parameter vector θ∈Rn\theta\in\mathbb R^nθ∈Rn, its residual vector is r=(Zn)Tθ∈Rmr=(Z^n)^T\theta\in\mathbb R^mr=(Zn)Tθ∈Rm. A fixed matrix U∈Rn×ℓU\in\mathbb R^{n\times\ell}U∈Rn×ℓ describes the structure of permitted perturbations, and a nonnegative scalar ρ\rhoρ controls their size. The uncertain data matrices are

Z={Zn+ρUΔ:Δ∈D},\mathcal Z=\{Z^n+\rho U\Delta:\Delta\in D\},Z={Zn+ρUΔ:Δ∈D},

where D⊂Rℓ×mD\subset\mathbb R^{\ell\times m}D⊂Rℓ×m is convex, compact, and contains zero. No independence of its columns is imposed.

The loss function L:Rm→RL:\mathbb R^m\to\mathbb RL:Rm→R is finite and convex. Assumption L requires one of two forms: L(r)=π(∣r∣)L(r)=\pi(|r|)L(r)=π(∣r∣) for every rrr, or L(r)=π(r+)L(r)=\pi(r_+)L(r)=π(r+​) for every rrr. Absolute value and positive part act coordinatewise. The function π\piπ is convex and nondecreasing in every coordinate on the nonnegative orthant. The choice of form is global, rather than chosen separately at each residual.

Assumption A specifies the support of DDD in every rank-one direction:

max⁡Δ∈DuTΔv=ϕ(u)ψ(v).\max_{\Delta\in D}u^T\Delta v=\phi(u)\psi(v).Δ∈Dmax​uTΔv=ϕ(u)ψ(v).

Here ϕ\phiϕ is finite, nonnegative, convex, and positively homogeneous, and ψ\psiψ is a norm. The goal uses ψ(v)=∥v∥∞\psi(v)=\|v\|_\inftyψ(v)=∥v∥∞​. These are the standing objects and assumptions of Section 12.2, printed pages 311–319 of the source.

Formalization targets

For any real threshold τ\tauτ, the goal is the exact equivalence

∀Z∈Z: L(ZTθ)≤τ\forall Z\in\mathcal Z:\ L(Z^T\theta)\le\tau∀Z∈Z: L(ZTθ)≤τ

if and only if there exists a real κ\kappaκ satisfying

ρϕ(UTθ)≤κ,L((Zn)Tθ+κei)≤τ,L((Zn)Tθ−κei)≤τ(1≤i≤m).\rho\phi(U^T\theta)\le\kappa,\qquad L((Z^n)^T\theta+\kappa e_i)\le\tau,\qquad L((Z^n)^T\theta-\kappa e_i)\le\tau\quad(1\le i\le m).ρϕ(UTθ)≤κ,L((Zn)Tθ+κei​)≤τ,L((Zn)Tθ−κei​)≤τ(1≤i≤m).

The goal also states convexity in (θ,κ)(\theta,\kappa)(θ,κ) of the scalar functions on the left of these constraints. There are 2m2m2m shifted-loss inequalities and one amplitude inequality.

The numbered supporting targets preserve the source's identities. Equation 12.2.11 gives the Fenchel biconjugate representation of a finite convex loss. Equation 12.2.12 equates the worst-case realized loss with its conjugate expression involving the support of DDD. Equation 12.2.15 replaces that support by its factorization under Assumption A. Equation 12.2.18 equates the resulting worst-case loss with a maximum over the dual unit ball:

Lwc(r,κ)=max⁡ψ∗(ξ)≤1L(r+κξ),κ≥0.L_{\rm wc}(r,\kappa)=\max_{\psi^*(\xi)\le1}L(r+\kappa\xi),\qquad \kappa\ge0.Lwc​(r,κ)=ψ∗(ξ)≤1max​L(r+κξ),κ≥0.

The maxima in these identities are required to be attained. The Fenchel representation itself uses the source's supremum notation.

What the representation provides

Theorem 12.2.5 replaces a constraint over a continuum of data matrices with finitely many evaluations of the original loss and the uncertainty gauge. It retains the dependence of uncertainty on the fitted parameter through ϕ(UTθ)\phi(U^T\theta)ϕ(UTθ). Consequently, the representation describes exactly the robust feasible parameters, including zero uncertainty, rather than merely giving a sufficient condition. Evaluation efficiency remains relative to the supplied loss and gauge, as in the book's tractability discussion.

The mathematical result is established in the textbook. The contribution sought here is a machine-checked formalization of its statement and supporting identities. The general finite-dimensional Fenchel biconjugacy theorem already has a proved platform item and is reused as the first milestone; the other three identities and the capstone are open theorem statements in this draft.

Mathematical difficulty

The central issue is relating uncertainty in a matrix to uncertainty in the residual vector while preserving exactness. A uniform bound on individual matrix entries does not by itself express Assumption A. Conjugate functions also need extended values: replacing an infinite conjugate by a real default would change the optimization problem. Establishing equality of optimal values alone is insufficient for identities written with maxima; their attainment is part of the targets. The zero-amplitude case must agree with the nominal loss throughout.

Formalization scope

Vectors use finite-dimensional real Euclidean spaces and matrices have explicitly ordered feature and measurement indices. Coordinates use Fin m, so the first coordinate is indexed by zero. The infinity norm in the goal is taken on the plain coordinate function; it is not the Euclidean norm of the residual vector. The statements include both signs for every coordinate.

The published fenchelConjugate and fenchelBiconjugate definitions are reused. Conjugate objectives take values in EReal. Every claimed maximum is expressed using IsGreatest at a common finite real value, so existence, boundedness, equality, and attainment remain visible. The inner support supremum in Equation 12.2.12 is real-valued and ranges over a nonempty compact image. The dual unit ball in Equation 12.2.18 is represented directly by ξTv≤ψ(v)\xi^Tv\le\psi(v)ξTv≤ψ(v) for all vvv.

All hypotheses about the loss, gauge, norm, and uncertainty set are explicit in each new theorem. None assumes the desired finite reformulation. Assumption L is retained despite the recorded observation that a weaker loss hypothesis suffices for the mathematical equivalence. There are no variant targets. A computational cost model and an optimization algorithm are outside this formalization; the explicit finite formulas and their convexity are the representation being formalized. Reusable work includes finite-dimensional conjugacy, compact support maximization, and dual-norm geometry.

Selected references

  • A. Ben-Tal, L. El Ghaoui and A. Nemirovski, Robust Optimization, Princeton University Press, 2009. DOI: 10.1515/9781400831050. Section 12.2, printed pp. 311–319; Equations 12.2.11, 12.2.12, 12.2.15, 12.2.18 and Theorem 12.2.5.
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Robust Optimization II: Safe Robust Counterparts for Bounded Random PerturbationsTextbook

Motivation: reliability under random data

A linear constraint can fail when its coefficients vary. In an engineering or planning model, requiring it to hold for every imaginable realization may exclude useful decisions, while checking it only at an average realization may give little control over failure. A chance constraint specifies an acceptable probability of violation. Chapter 2 of Ben-Tal, El Ghaoui and Nemirovski, Robust Optimization studies deterministic convex conditions that guarantee this probabilistic requirement for a single uncertain linear inequality.

The chapter distinguishes a guarantee from an exact description of chance feasibility. Its robust constraints are safe approximations: satisfying them guarantees reliability, but a reliable decision need not satisfy them. The goal here concerns how known bounds on the perturbations can be incorporated into such an approximation without losing an explicit convex representation.

Setting: an uncertain scalar inequality

A decision is a vector x∈Rnx\in\mathbb R^nx∈Rn. The deterministic data are vectors a0,a1,…,aLa^0,a^1,\ldots,a^La0,a1,…,aL and scalars b0,b1,…,bLb^0,b^1,\ldots,b^Lb0,b1,…,bL. Define the residual coordinates by zi(x)=(ai)Tx−biz_i(x)=(a^i)^Tx-b^izi​(x)=(ai)Tx−bi, including the nominal coordinate i=0i=0i=0. A realized perturbation ζ∈RL\zeta\in\mathbb R^Lζ∈RL satisfies the constraint exactly when

z0(x)+∑i=1Lζizi(x)≤0.z_0(x)+\sum_{i=1}^L\zeta_i z_i(x)\le0.z0​(x)+i=1∑L​ζi​zi​(x)≤0.

For a probability law PPP and a tolerance 0<ε<10<\varepsilon<10<ε<1, chance feasibility means that the strict reverse inequality has probability at most ε\varepsilonε. Robust feasibility over a deterministic set ZZZ means that the displayed inequality holds for every η∈Z\eta\in Zη∈Z.

The perturbation coordinates are independent measurable real random variables. Their moment-generating functions obey the two-sided bound

EPetζi≤exp⁡(max⁡{μi−t,μi+t}+12σi2t2)(t∈R),\mathbb E_P e^{t\zeta_i}\le\exp\left(\max\{\mu_i^-t,\mu_i^+t\}+\frac12\sigma_i^2t^2\right)\qquad(t\in\mathbb R),EP​etζi​≤exp(max{μi−​t,μi+​t}+21​σi2​t2)(t∈R),

where μi−≤μi+\mu_i^-\le\mu_i^+μi−​≤μi+​ and σi≥0\sigma_i\ge0σi​≥0. These are the book's assumptions P.1–2. The goal additionally assumes almost-sure support bounds ai−≤ζi≤ai+a_i^-\le\zeta_i\le a_i^+ai−​≤ζi​≤ai+​, with finite endpoints satisfying ai−≤μi−≤μi+≤ai+a_i^-\le\mu_i^-\le\mu_i^+\le a_i^+ai−​≤μi−​≤μi+​≤ai+​. No positive lower bound on σi\sigma_iσi​ is imposed.

Formalization targets

Write B(y)=∑imax⁡{μi−yi,μi+yi}B(y)=\sum_i\max\{\mu_i^-y_i,\mu_i^+y_i\}B(y)=∑i​max{μi−​yi​,μi+​yi​}, D(y)=∑iσi2yi2D(y)=\sqrt{\sum_i\sigma_i^2y_i^2}D(y)=∑i​σi2​yi2​​, and rε=2log⁡(1/ε)r_\varepsilon=\sqrt{2\log(1/\varepsilon)}rε​=2log(1/ε)​. The general safety statement, Proposition 2.4.1, asserts that

z0+B(z)+rεD(z)≤0⟹P{z0+∑iziζi>0}≤ε.z_0+B(z)+r_\varepsilon D(z)\le0\quad\Longrightarrow\quad P\{z_0+\sum_i z_i\zeta_i>0\}\le\varepsilon.z0​+B(z)+rε​D(z)≤0⟹P{z0​+i∑​zi​ζi​>0}≤ε.

Its feasible set is convex. Proposition 2.4.2 states the tail bound at every nonnegative safety level rrr:

P{∑iziζi>B(z)+rD(z)}≤e−r2/2.P\{\sum_i z_i\zeta_i>B(z)+rD(z)\}\le e^{-r^2/2}.P{i∑​zi​ζi​>B(z)+rD(z)}≤e−r2/2.

Theorem 2.4.3 identifies the first deterministic inequality with robust feasibility over the moment uncertainty set

Zmom={η:∃w, μi−≤ηi−σiwi≤μi+ (1≤i≤L), ∑iwi2≤rε}.Z_{\rm mom}=\{\eta:\exists w,\ \mu_i^-\le\eta_i-\sigma_iw_i\le\mu_i^+\ (1\le i\le L),\ \sqrt{\sum_iw_i^2}\le r_\varepsilon\}.Zmom​={η:∃w, μi−​≤ηi​−σi​wi​≤μi+​ (1≤i≤L), i∑​wi2​​≤rε​}.

The capstone is Theorem 2.4.4. Let ZZZ be the intersection of ZmomZ_{\rm mom}Zmom​ with the support box [a−,a+][a^-,a^+][a−,a+]. Then xxx is robust feasible over ZZZ if and only if there exist extended residual vectors u,v∈RL+1u,v\in\mathbb R^{L+1}u,v∈RL+1 satisfying

zi(x)=ui+vi(0≤i≤L),z_i(x)=u_i+v_i\quad(0\le i\le L),zi​(x)=ui​+vi​(0≤i≤L), u0+∑imax⁡{ai−ui,ai+ui}≤0,v0+B(v)+rεD(v)≤0.u_0+\sum_i\max\{a_i^-u_i,a_i^+u_i\}\le0,\qquad v_0+B(v)+r_\varepsilon D(v)\le0.u0​+i∑​max{ai−​ui​,ai+​ui​}≤0,v0​+B(v)+rε​D(v)≤0.

This system is convex in its decision and auxiliary variables. Every feasible triple has violation probability at most ε\varepsilonε. The theorem includes both the deterministic equivalence and the probabilistic guarantee, as on printed page 48.

Two supporting targets retain the chapter's bounded mean-zero specialization. Proposition 2.3.1 gives the tail estimate P{∑iziζi>r∑izi2}≤e−r2/2P\{\sum_i z_i\zeta_i>r\sqrt{\sum_i z_i^2}\}\le e^{-r^2/2}P{∑i​zi​ζi​>r∑i​zi2​​}≤e−r2/2 for independent mean-zero perturbations in [−1,1][-1,1][−1,1]. Proposition 2.3.3 identifies robustness over the intersection of the unit box and a Euclidean ball with its lifted conic system and establishes the corresponding chance guarantee. These are supporting statements from the source, not replacements for the general capstone.

Significance: explicit conditions with a probability guarantee

The capstone connects a deterministic set of allowed perturbations with a stochastic model specified through moment bounds and support information. It gives a finite convex system whose feasible decisions satisfy the requested reliability level for every law meeting those assumptions. The statement does not require choosing a particular parametric distribution or estimating a probability separately for every decision.

These are known textbook results. The formalization targets are their Lean statements and eventual machine-checked proofs, including zero scales and boundary feasibility. The reusable content comprises finite-dimensional uncertainty sets, explicit exponential-moment hypotheses, and the relationship between lifted convex constraints and strict-event probabilities. The present authoring pass leaves the six theorem proofs open; compilation checks their types, not their truth.

Difficulty: boundary cases carry mathematical content

The exact robust representation includes equality cases in the endpoint order and permits degenerate ellipsoids. A formulation restricted to positive scales or strict interior intersections would omit cases of the stated theorem. The chance guarantee must also include the boundary of the explicit safe set; it cannot be replaced by a condition requiring an additional strict margin.

The printed proofs have local discrepancies recorded in the mission findings: the proof of Proposition 2.4.2 omits a sum and invokes an open-interval risk bound at its excluded endpoint when the safety level is zero, the first line of the goal's proof uses a different radius, and the limiting argument on page 50 asserts a zero limit that fails for strictly feasible residuals. These findings concern the proofs, not counterexamples to the theorem statements. The goal retains the printed constants and hypotheses.

Formalization scope

The namespace is RobustOpt2009.ScalarChance. Vectors use real-valued functions on Fin L; the nominal coordinate is a separate real component. All Euclidean lengths are explicit square roots of sums of squares, avoiding the default function-space sup norm. Probability is evaluated under a probability measure, and all random coordinates are measurable. The exponential-moment definition includes integrability, preventing nonintegrable Bochner integrals from supplying default zero values.

Scaled coordinates σiwi\sigma_iw_iσi​wi​ implement the book's zero-denominator convention: a zero scale forces zero displacement. Robust feasibility is a universal inequality, so no empty or unbounded real supremum is used. The exponential-certificate set, its topological closure, and the perturbation uncertainty set remain separate concrete objects. No definition assumes the desired equivalence or tail bound. Finite sums include the zero-dimensional case, where the statements reduce to their deterministic or empty-event versions.

Further work consists of proving the stated concentration, convexity, and exact representation claims using these definitions and Mathlib's probability and finite-dimensional analysis. No variants are posed in this chapter.

Selected references

  • Aharon Ben-Tal, Laurent El Ghaoui and Arkadi Nemirovski, Robust Optimization, Princeton University Press, 2009, Chapter 2, especially printed pp. 29–33 and 45–50. DOI: 10.1515/9781400831050. Published citation basis; PDF pages are printed pages plus 26.
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Robust Optimization IV: The Bernstein Uncertainty SetTextbook

Chance constraints and robust feasibility

An optimization model can require a linear inequality to hold with high probability when its coefficients are random. Such a chance constraint controls the probability of violation, but its feasible set need not be convex or easy to describe. A conservative convex approximation can make the requirement usable within a larger optimization model. Chapter 4 of Ben-Tal, El Ghaoui and Nemirovski, Robust Optimization studies when such approximations also have a robust interpretation: the inequality must hold for every perturbation in a deterministic uncertainty set.

The target here is the chapter's Bernstein construction. It starts from information about the joint exponential moments of a random vector, rather than a fixed list of scenarios. Its conclusion identifies exactly the uncertainty set associated with the conservative approximation. Exactness concerns the relationship between that approximation and robust feasibility; the approximation is still only a sufficient condition for the original chance constraint.

Probability model and conjugate data

Let ζ\zetaζ have probability distribution PPP on RL\mathbb R^LRL. A coefficient vector is a pair z=(z0,w)z=(z_0,w)z=(z0​,w), where z0∈Rz_0\in\mathbb Rz0​∈R and w∈RLw\in\mathbb R^Lw∈RL. The requirement is

P{z0+⟨w,ζ⟩>0}≤ϵ,0<ϵ<1.P\{z_0+\langle w,\zeta\rangle>0\}\le\epsilon,\qquad 0<\epsilon<1.P{z0​+⟨w,ζ⟩>0}≤ϵ,0<ϵ<1.

The violation event is strict. Equality in the underlying linear inequality therefore counts as feasible. The parameter ϵ\epsilonϵ controls the permitted probability of failure.

A logarithmic moment-generating majorant is a finite convex function Φ:RL→R\Phi:\mathbb R^L\to\mathbb RΦ:RL→R satisfying Φ(0)=0\Phi(0)=0Φ(0)=0 and

log⁡EPexp⁡⟨w,ζ⟩≤Φ(w)for all w.\log\mathbb E_P\exp\langle w,\zeta\rangle\le\Phi(w)\quad\text{for all }w.logEP​exp⟨w,ζ⟩≤Φ(w)for all w.

These are Assumption Q.1. They concern the joint distribution; independence of the coordinates is not required. Assumption Q.2 provides an affine conjugate representation

Φ(w)=sup⁡u∈RM{⟨w,Au+a⟩−ϕ(u)},\Phi(w)=\sup_{u\in\mathbb R^M}\{\langle w,Au+a\rangle-\phi(u)\},Φ(w)=u∈RMsup​{⟨w,Au+a⟩−ϕ(u)},

where AAA is linear, a∈RLa\in\mathbb R^La∈RL, and ϕ:RM→R∪{+∞}\phi:\mathbb R^M\to\mathbb R\cup\{+\infty\}ϕ:RM→R∪{+∞} is convex and lower semicontinuous. Every real sublevel set of ϕ\phiϕ is bounded. Allowing +∞+\infty+∞ permits restrictions on the effective domain without changing the ambient space.

Formalization targets

The goal is Theorem 4.2.5, printed pp. 85–86 of the book. Define the coefficient sets independently by

Zϵo={(z0,w):∃α>0, αz0+Φ(αw)≤log⁡ϵ},Zϵ=cl⁡Zϵo.Z^o_\epsilon=\{(z_0,w):\exists\alpha>0,\ \alpha z_0+\Phi(\alpha w)\le\log\epsilon\},\qquad Z_\epsilon=\operatorname{cl}Z^o_\epsilon.Zϵo​={(z0​,w):∃α>0, αz0​+Φ(αw)≤logϵ},Zϵ​=clZϵo​.

Define the auxiliary sublevel set and its affine image by

Uϵ={u:ϕ(u)≤log⁡(1/ϵ)},Zϵ=AUϵ+a.U_\epsilon=\{u:\phi(u)\le\log(1/\epsilon)\},\qquad \mathcal Z_\epsilon=AU_\epsilon+a.Uϵ​={u:ϕ(u)≤log(1/ϵ)},Zϵ​=AUϵ​+a.

The theorem says that UϵU_\epsilonUϵ​ is nonempty, convex, and compact and that

(z0,w)∈Zϵ  ⟺  z0+⟨ζ,w⟩≤0for every ζ∈Zϵ.(z_0,w)\in Z_\epsilon\iff z_0+\langle\zeta,w\rangle\le0\quad\text{for every }\zeta\in\mathcal Z_\epsilon.(z0​,w)∈Zϵ​⟺z0​+⟨ζ,w⟩≤0for every ζ∈Zϵ​.

It also retains the displayed perspective characterization and its probabilistic consequence:

(z0,w)∈Zϵ  ⟺  inf⁡β>0[z0+βΦ(β−1w)+βlog⁡(1/ϵ)]≤0,(z_0,w)\in Z_\epsilon\iff\inf_{\beta>0}\left[z_0+\beta\Phi(\beta^{-1}w)+\beta\log(1/\epsilon)\right]\le0,(z0​,w)∈Zϵ​⟺β>0inf​[z0​+βΦ(β−1w)+βlog(1/ϵ)]≤0,

and this condition implies the original chance constraint.

Four source-numbered milestones accompany the goal. Lemma B.1.1 identifies the closure of a homogenized convex sublevel set with the zero sublevel set of its perspective infimum, including finiteness and convexity of that function. Proposition 4.2.2 characterizes the Bernstein approximation and asserts its normal safety. Proposition 4.2.3 gives bounded sublevel sets for an affine conjugate representation whose linear map has trivial kernel. Theorem B.1.2 gives the general robust representation under its directional-limit assumption. Each statement retains its source hypotheses and all conclusion clauses.

Mathematical and formal significance

The chapter's result gives a deterministic meaning to a probabilistic sufficient condition. An uncertainty set chosen through the conjugate data describes precisely the same coefficient constraints as the Bernstein approximation. This connects the probability model to robust linear feasibility while preserving the distinction between a guarantee and an exact description of the original chance-feasible set.

The formalization supplies separate, concrete definitions for the probability condition, the coefficient cone, and the perturbation set. That separation makes the equality in the main result a substantive theorem. The appendix statements also expose reusable finite-dimensional convex analysis, including perspective values, closed cones, and affine images of extended-real sublevel sets. These are known mathematical results from the book; the current draft consists of type-checked statements awaiting Lean proofs. A successful statement build is not a proof of any of these assertions.

Difficulty

Closure and optimization at a boundary are central issues. The perspective infimum ranges over strictly positive scales, but its value may be approached only as the scale tends to zero. Replacing the infimum condition by the existence of one feasible scale would change the target. Similarly, an extended-real function can impose a proper effective domain, so a formalization restricted to everywhere-finite penalties would omit cases covered by the theorem.

The general appendix theorem includes a directional limit below a specified level. That limit can be negative infinity, including in the application to the chapter's coefficient variable. Requiring a finite real limit would exclude the intended application. Probability expressions also require attention to the strict violation event and to the meaning of an expectation when exponential moments diverge.

Formalization scope

Finite-dimensional real spaces are represented by functions on Fin n, with the standard topology. Coefficients are pairs (z0,w)(z_0,w)(z0​,w), so coefficient feasibility and perturbation membership have different types. The linear map is explicit and its affine translation is applied before taking the pairing. No independence, Gaussian distribution, bounded support, or injectivity assumption is added to the goal. Injectivity belongs only to Proposition 4.2.3 and its variant.

Formalization Note Infima and suprema are computed in the complete extended-real lattice. The penalty's negative-infinity value is explicitly excluded where the source uses R∪{+∞}\mathbb R\cup\{+\infty\}R∪{+∞}. Convexity is expressed by the real epigraph and lower semicontinuity by closed real sublevels. Q.1 uses the equivalent bound on the nonnegative integral of the exponential, avoiding a default real-integral value on nonintegrable inputs. The uncertainty set is the actual affine image of the specified sublevel set, not an assumed certificate for robust feasibility.

Beyond the paper. One additional target strengthens Proposition 4.2.3 by removing only lower semicontinuity. Finding F1 records that finite bounds in the positive and negative coordinate directions, together with injectivity, already bound each sublevel set. The faithful proposition retains lower semicontinuity and remains the milestone. This strengthening does not change the goal or remove the topological assumptions needed for compactness elsewhere.

Selected references

  • A. Ben-Tal, L. El Ghaoui and A. Nemirovski, Robust Optimization, Princeton University Press, 2009. DOI: 10.1515/9781400831050. Chapter 4, §§4.1–4.2.3, printed pp. 81–86 (PDF pp. 107–112); Appendix B, §§B.1.1–B.1.3, printed pp. 471–475 (PDF pp. 497–501). Citation basis: published.
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Robust Optimization III: Global Sensitivity for Linear ConstraintsTextbook

Motivation: controlling violations beyond normal uncertainty

A resource constraint can remain useful even when an exceptional disturbance makes exact satisfaction impractical. In such cases the model needs to distinguish the disturbances against which feasibility is mandatory from those for which a controlled violation is acceptable. Ordinary robust optimization specifies a set of perturbations and requires the constraint to hold everywhere in that set. It does not itself describe what happens outside that set. Chapter 3 of Ben-Tal, El Ghaoui and Nemirovski, Robust Optimization introduces a quantitative way to make this distinction for uncertain linear inequalities.

The object of this mission is the globalized robust counterpart of a single scalar inequality. Its tolerance is proportional to distance from a normal uncertainty range, with a prescribed restriction on admissible displacement directions. The goal is Proposition 3.2.1, which characterizes this global requirement by two ordinary robust inequalities. The result is a known theorem of the book; the target here is its faithful Lean formalization.

Setting: a perturbation structure and a scalar constraint

Let x∈Rnx\in\mathbb R^nx∈Rn be a decision vector. The data consist of vectors a0,a1,…,aL∈Rna^0,a^1,\ldots,a^L\in\mathbb R^na0,a1,…,aL∈Rn and scalars b0,b1,…,bL∈Rb^0,b^1,\ldots,b^L\in\mathbb Rb0,b1,…,bL∈R. A perturbation vector ζ∈RL\zeta\in\mathbb R^Lζ∈RL determines the inequality

[a0+∑ℓ=1Lζℓaℓ]Tx≤b0+∑ℓ=1Lζℓbℓ.\left[a^0+\sum_{\ell=1}^L\zeta_\ell a^\ell\right]^Tx \le b^0+\sum_{\ell=1}^L\zeta_\ell b^\ell.[a0+ℓ=1∑L​ζℓ​aℓ]Tx≤b0+ℓ=1∑L​ζℓ​bℓ.

The normal range ZZZ is a nonempty closed convex subset of RL\mathbb R^LRL. A closed convex cone KKK containing zero describes the possible directions of departure. The physically possible range is the sum

Z+K={z+d:z∈Z, d∈K}.Z+K=\{z+d:z\in Z,\ d\in K\}.Z+K={z+d:z∈Z, d∈K}.

Here KKK denotes the book's L\mathcal LL; LLL remains the number of perturbation coordinates. A fixed norm NNN measures displacement. These are the perturbation-structure assumptions (G.a–c) on printed page 68 of the source.

For a physically possible perturbation, its constrained distance from the normal range is

d(ζ,Z∣K)=inf⁡{N(ζ−z):z∈Z, ζ−z∈K}.d(\zeta,Z\mid K)=\inf\{N(\zeta-z):z\in Z,\ \zeta-z\in K\}.d(ζ,Z∣K)=inf{N(ζ−z):z∈Z, ζ−z∈K}.

The displacement restriction is part of the definition. The admissible set of displacement lengths is nonempty when ζ∈Z+K\zeta\in Z+Kζ∈Z+K and is bounded below by zero. Thus the distance has a finite real value on precisely the domain where the counterpart uses it.

A nonnegative real parameter α\alphaα is the global sensitivity. Global robustness requires the residual of the uncertain inequality to be at most αd(ζ,Z∣K)\alpha d(\zeta,Z\mid K)αd(ζ,Z∣K) for every physically possible perturbation. This is Definition 3.1.1 and equation (3.1.4) of the book.

Formalization targets

Write the residual and its directional part as

rx(ζ)=[a0+∑ℓζℓaℓ]Tx−b0−∑ℓζℓbℓ,qx(d)=[∑ℓdℓaℓ]Tx−∑ℓdℓbℓ.r_x(\zeta)=\left[a^0+\sum_\ell\zeta_\ell a^\ell\right]^Tx-b^0-\sum_\ell\zeta_\ell b^\ell, \qquad q_x(d)=\left[\sum_\ell d_\ell a^\ell\right]^Tx-\sum_\ell d_\ell b^\ell.rx​(ζ)=[a0+ℓ∑​ζℓ​aℓ]Tx−b0−ℓ∑​ζℓ​bℓ,qx​(d)=[ℓ∑​dℓ​aℓ]Tx−ℓ∑​dℓ​bℓ.

The goal is the complete equivalence of Proposition 3.2.1, printed page 69:

[∀ζ∈Z+K, rx(ζ)≤αd(ζ,Z∣K)]⟺{rx(ζ)≤0∀ζ∈Z,qx(d)≤α∀d∈K with N(d)≤1.\bigl[\forall\zeta\in Z+K,\ r_x(\zeta)\le\alpha d(\zeta,Z\mid K)\bigr] \quad\Longleftrightarrow\quad \begin{cases} r_x(\zeta)\le0&\forall\zeta\in Z,\\ q_x(d)\le\alpha&\forall d\in K\text{ with }N(d)\le1. \end{cases}[∀ζ∈Z+K, rx​(ζ)≤αd(ζ,Z∣K)]⟺{rx​(ζ)≤0qx​(d)≤α​∀ζ∈Z,∀d∈K with N(d)≤1.​

Both right-hand requirements are universal inequalities. The nominal coefficients occur in the first and do not occur in the second. The directional condition includes the zero direction and every direction on the boundary of the unit ball.

There are no separate supporting theorem milestones in this mission. The numbered Chapter 1 representation results discussed after the proposition describe applications of its conclusion. They are not intermediate targets needed to state this capstone.

Significance: separating two kinds of robustness

The equivalence distinguishes feasibility throughout the normal range from control of how the residual varies along admissible directions. As explained in Remark 3.2.2 of the book, it brings the globalized counterpart into contact with representation results for ordinary robust constraints. The proposition itself remains valid without a boundedness assumption on the normal range and without choosing a special shape such as a box or ellipsoid.

The formalization fixes the exact relationship between the domain of the distance and the quantifiers in the counterpart. It also makes the treatment of the cone and the norm explicit. These conventions are useful when subsequent developments specialize the model. The mission asks for a proof of the displayed equivalence; finite reformulations for particular uncertainty geometries and the chapter's antenna-array application are outside this target.

Difficulty: distance domains and boundary cases

The constrained distance cannot generally be replaced by ordinary distance to ZZZ. That substitution changes which normal points are eligible when evaluating a disturbance. The normal range can also be unbounded, so compactness of ZZZ is not available as a standing assumption. A formal proof must handle the domain of the infimum and the full directional quantification with these features intact.

The parameter α\alphaα may be zero. In that case the globalized condition requires exact feasibility throughout Z+KZ+KZ+K, as noted after Definition 3.1.1 in the source. The cone may consist only of zero, and the relevant displacement can have zero norm. None of these cases is excluded by a positivity assumption added for convenience.

Formalization scope

All coefficients and sensitivities are real. Decision and perturbation vectors use the finite coordinate types Fin n and Fin L; their zero-based indexing is a relabeling of the source sums. The nominal coefficients are separate parameters. The goal writes the coordinate sums and constrained infimum explicitly, using only Mathlib objects, so its meaning does not depend on an unpublished definition from another chapter.

An arbitrary norm is represented by Mathlib's real seminorm type together with definiteness: N(v)=0N(v)=0N(v)=0 implies v=0v=0v=0. Closedness uses the usual topology on finite-dimensional real coordinate space. Convexity of both sets, nonemptiness of ZZZ, membership of zero in KKK, and closure of KKK under nonnegative scaling are explicit hypotheses. The global robustness condition is the distance inequality itself, not a definition chosen to assume its desired characterization.

The real infimum is used only over a nonempty set of nonnegative lengths. Its value on an empty set is not used by the theorem. Zero coordinate dimensions are permitted with empty sums interpreted as zero. The faithful goal retains convexity of ZZZ; the separately recorded observation that it is unnecessary does not alter this statement. The remaining formal work concerns this exact equivalence, using finite sums, convex sets, seminorms, topology and real infima from Mathlib.

Selected references

  • Aharon Ben-Tal, Laurent El Ghaoui and Arkadi Nemirovski, Robust Optimization, Princeton University Press, 2009. DOI: 10.1515/9781400831050. Chapter 3, Definition 3.1.1 and equations (3.1.2)–(3.1.4), printed page 68 (PDF page 94); Proposition 3.2.1 and Remark 3.2.2, printed page 69 (PDF page 95); proof continuation, printed page 70 (PDF page 96).
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EconomicsOperations ResearchProbability·Captain: mikedeng1

An Axiomatic Foundation for the Expected Shortfall: Monotonicity, Law Invariance, Prudence and No Reward for Concentration Characterize ES on L¹Research Paper

Motivation

Banks hold capital against the risk of their trading books, and the amount is computed by a risk measure: a functional ρ\rhoρ that assigns a real number to each random loss XXX. For two decades the regulatory standard was the Value-at-Risk VaRp\mathrm{VaR}_pVaRp​, a quantile of the loss. The Fundamental Review of the Trading Book of the Basel Committee (BCBS, 2019) replaced it by the Expected Shortfall ESp\mathrm{ES}_pESp​, the average of the quantiles beyond level ppp. The academic case for ES rested mostly on coherence (Artzner, Delbaen, Eber and Heath, 1999), that is, on subadditivity, a property that the regulator's documents do not take as their starting point.

Wang and Zitikis (SSRN 3423042; Management Science, 2021, doi:10.1287/mnsc.2020.3617) give an axiomatic answer in the regulator's own terms. Besides three basic requirements (monotonicity, law invariance, prudence), they ask that a portfolio whose components all suffer their largest losses in the same stress scenario receive no diversification benefit. They prove that these four axioms characterize exactly the family {ESp:p∈(0,1)}\{\mathrm{ES}_p : p\in(0,1)\}{ESp​:p∈(0,1)}. Earlier characterizations of ES (Kusuoka, 2001; Acerbi and Tasche, 2002) start from coherence or comonotonic additivity; this one does not assume convexity, subadditivity or translation invariance.

Setting

Fix an atomless probability space (Ω,F,P)(\Omega,\mathcal F,\mathbb P)(Ω,F,P): every event of positive probability contains an event of strictly smaller positive probability. A random variable is a measurable X:Ω→RX:\Omega\to\mathbb RX:Ω→R; a positive value is a loss. L1L^1L1 is the set of integrable random variables, L+1L^1_+L+1​ its non-negative part, and LqL^qLq, q∈[0,∞]q\in[0,\infty]q∈[0,∞], the random variables with finite qqq-th moment. X=dYX\overset{d}{=}YX=dY means that XXX and YYY have the same distribution function.

For p∈(0,1)p\in(0,1)p∈(0,1),

VaRp(X)=inf⁡{x∈R:P(X≤x)≥p},ESp(X)=11−p∫p1VaRq(X) dq.\mathrm{VaR}_p(X)=\inf\{x\in\mathbb R:\mathbb P(X\le x)\ge p\},\qquad \mathrm{ES}_p(X)=\frac{1}{1-p}\int_p^1 \mathrm{VaR}_q(X)\,\mathrm dq .VaRp​(X)=inf{x∈R:P(X≤x)≥p},ESp​(X)=1−p1​∫p1​VaRq​(X)dq.

A tail event of XXX is an event AAA with 0<P(A)<10<\mathbb P(A)<10<P(A)<1 such that X(ω)≥X(ω′)X(\omega)\ge X(\omega')X(ω)≥X(ω′) for almost all ω∈A\omega\in Aω∈A and ω′∈Ac\omega'\in A^cω′∈Ac; a ppp-tail event is a tail event of probability 1−p1-p1−p. A vector (X1,…,Xn)(X_1,\dots,X_n)(X1​,…,Xn​) is ppp-concentrated if its components share a ppp-tail event. A functional ρ\rhoρ on a domain X\mathcal XX may satisfy:

  • M (monotonicity): ρ(X)≤ρ(Y)\rho(X)\le\rho(Y)ρ(X)≤ρ(Y) whenever X≤YX\le YX≤Y at every scenario;
  • LI (law invariance): ρ(X)=ρ(Y)\rho(X)=\rho(Y)ρ(X)=ρ(Y) whenever X=dYX\overset{d}{=}YX=dY;
  • P (prudence): lim⁡kρ(ξk)≥ρ(X)\lim_k\rho(\xi_k)\ge\rho(X)limk​ρ(ξk​)≥ρ(X) whenever ξk→X\xi_k\to Xξk​→X pointwise and the limit exists;
  • NRC (no reward for concentration): there is a stress event AAA such that ρ(X+Y)=ρ(X)+ρ(Y)\rho(X+Y)=\rho(X)+\rho(Y)ρ(X+Y)=ρ(X)+ρ(Y) for all X,YX,YX,Y sharing the tail event AAA.

ρ\rhoρ is ppp-additive if ρ(X+Y)=ρ(X)+ρ(Y)\rho(X+Y)=\rho(X)+\rho(Y)ρ(X+Y)=ρ(X)+ρ(Y) whenever XXX and YYY share a ppp-tail event.

Formalization targets

Goal: Theorem 1 (p. 9)

For ρ:L1→R\rho:L^1\to\mathbb Rρ:L1→R with ρ(1)=1\rho(1)=1ρ(1)=1,

ρ satisfies M, LI, P, NRC  ⟺  ρ=ESp on L1 for some p∈(0,1),\rho \text{ satisfies M, LI, P, NRC} \iff \rho=\mathrm{ES}_p \text{ on } L^1 \text{ for some } p\in(0,1),ρ satisfies M, LI, P, NRC⟺ρ=ESp​ on L1 for some p∈(0,1),

and in the forward direction p=1−P(A)p=1-\mathbb P(A)p=1−P(A) for every stress event AAA, uniquely.

Milestones, in attack order

  1. Lemma A.3 (p. 26): AAA is a ppp-tail event of XXX iff P(A)=1−p\mathbb P(A)=1-pP(A)=1−p and {X>VaRp(X)}⊂A⊂{X≥VaRp(X)}\{X>\mathrm{VaR}_p(X)\}\subset A\subset\{X\ge \mathrm{VaR}_p(X)\}{X>VaRp​(X)}⊂A⊂{X≥VaRp​(X)} a.s.; such an AAA exists.
  2. Lemma A.5 (p. 28): for a ppp-concentrated pair, the ppp-tail events of X+YX+YX+Y are the common ppp-tail events of XXX and YYY.
  3. Lemma A.7 (p. 32): for P(A)=1−p\mathbb P(A)=1-pP(A)=1−p, ESp(X)=E[X∣A]\mathrm{ES}_p(X)=\mathbb E[X\mid A]ESp​(X)=E[X∣A] iff AAA is a ppp-tail event of XXX.
  4. Theorem 5 (p. 15): ppp-concentration   ⟺  \iff⟺ maximizing the ESp\mathrm{ES}_pESp​ aggregation   ⟺  \iff⟺ ESp(∑iXi)=∑iESp(Xi)\mathrm{ES}_p(\sum_i X_i)=\sum_i\mathrm{ES}_p(X_i)ESp​(∑i​Xi​)=∑i​ESp​(Xi​).
  5. Example 1 (p. 16): VaRp\mathrm{VaR}_pVaRp​ is not ppp-additive.
  6. Proposition 1 (p. 10): ESp\mathrm{ES}_pESp​ and VaRp\mathrm{VaR}_pVaRp​ satisfy M, LI and P on L1L^1L1.
  7. Lemma A.1 (p. 19): monotone, additive, law-invariant functionals on L+1L^1_+L+1​ are λE\lambda\mathbb EλE, λ≥0\lambda\ge0λ≥0.
  8. Lemma A.2 (p. 20): a monotone ρ\rhoρ on L1L^1L1 is law invariant and ppp-additive iff ρ=aE+b ESp\rho=a\mathbb E+b\,\mathrm{ES}_pρ=aE+bESp​.
  9. Proposition 4 (p. 11): under LI on LqL^qLq, NRC   ⟺  \iff⟺ ppp-additivity for some ppp, with p=1−P(A)p=1-\mathbb P(A)p=1−P(A).

Significance

The theorem identifies ES as the only normalized risk measure on L1L^1L1 meeting four requirements that can be checked one by one, three of which every risk measure in practice satisfies. It shows that the passage from VaR to ES in the Basel framework follows from a no-diversification-benefit principle for concentrated portfolios, independently of the coherence argument. Theorem 5 describes the dependence structures for which ES is additive, which is a statement about worst-case aggregation of ES with fixed marginals. Example 1 shows that VaR fails the same requirement.

The results are proved in the paper. None of them is machine-checked. The Lean library has no quantile-based Expected Shortfall on a general probability space, no notion of tail event, and no characterization of law-invariant linear functionals. A completed mission would supply all three, together with the first formal axiomatic characterization of a regulatory risk measure.

Difficulty

Each axiom is weak on its own. Additivity is required only for pairs sharing one fixed stress event, and nothing is assumed about other pairs. The obvious approach, extending additivity from the stress event to all comonotonic pairs and then invoking Kusuoka's representation, fails because pairs sharing a single tail event are far from comonotonic. The real work is in Lemma A.2: building from a ppp-additive, law-invariant, monotone functional a linear functional on L+1L^1_+L+1​, which needs re-couplings on the atomless conditional spaces of AAA and AcA^cAc. Then come the identification of law-invariant linear functionals (Lemma A.1) and a monotonicity argument that excludes the mixtures aE+b ESpa\mathbb E+b\,\mathrm{ES}_paE+bESp​ with a≠0a\neq0a=0. On the ES side, Lemma A.7 and Theorem 5 need the dual representation of ES and a careful treatment of quantile ties, where {X>xp}\{X>x_p\}{X>xp​} and {X≥xp}\{X\ge x_p\}{X≥xp​} differ.

Formalization scope

  • Space. One probability space with the published atomlessness predicate TailRiskSharing.VaRConv.IsAtomless (every measurable set of positive mass splits), the published cdf distFn and left quantile VaRL, all from the definition module TailRiskSharing_VaRConv_Setting. The paper's VaRp\mathrm{VaR}_pVaRp​ is VaRL P (1 - p). Atomlessness is stated on every theorem that uses it; Proposition 1 and Example 1 do not.
  • Random variables are functions Ω → ℝ, not a.e. classes. A risk measure is any ρ : (Ω → ℝ) → ℝ constrained only on its domain. Axiom M is the sure order and Axiom P pointwise convergence at every scenario, the weakest forms in the paper's Remark 1. Law invariance makes ρ\rhoρ constant on a.s.-equal functions.
  • Tail events are read under P×P\mathbb P\times\mathbb PP×P: X(ω′)≤X(ω)X(\omega')\le X(\omega)X(ω′)≤X(ω) for P×P\mathbb P\times\mathbb PP×P-almost all (ω,ω′)∈A×Ac(\omega,\omega')\in A\times A^c(ω,ω′)∈A×Ac.
  • ESp\mathrm{ES}_pESp​ is the quantile integral over the open interval (p,1)(p,1)(p,1). E[X∣A]\mathbb E[X\mid A]E[X∣A] is E[X1A]/P(A)\mathbb E[X\mathbf 1_A]/\mathbb P(A)E[X1A​]/P(A).
  • The stress event satisfies 0<P(A)<10<\mathbb P(A)<10<P(A)<1. This is the one hypothesis added to the page. Read literally, NRC is satisfied by A=∅A=\emptysetA=∅, which is a tail event of no random variable, so every functional, VaRp\mathrm{VaR}_pVaRp​ included, would satisfy it and Theorem 1 would be false. The paper's own p=1−P(A)∈(0,1)p=1-\mathbb P(A)\in(0,1)p=1−P(A)∈(0,1) shows the intended reading.
  • Ruled out: a ρ\rhoρ on a quotient type with the a.s. order, a stress event that may be null, an ESp\mathrm{ES}_pESp​ defined through tail events or by a dual formula, a statement without atomlessness (Lemma A.1 fails with atoms), or a Theorem 1 that chooses ppp before ρ\rhoρ.
  • Not formalized: Theorem 2 (only ρ=0\rho=0ρ=0 on LqL^qLq, q<1q<1q<1), Propositions 2 and 3, Theorems 3, 4 and 6, the remaining appendix lemmas, and §5.
  • Infrastructure needed and reusable: quantile calculus for VaRL (monotonicity, quantile transforms of a uniform variable), the dual representation of ES, existence of couplings with prescribed joint law on atomless spaces, and the representation of law-invariant linear functionals on L1L^1L1. Each is useful beyond this mission, and contributions of any of them as separate lemmas are welcome.

Selected references

  • R. Wang and R. Zitikis, An Axiomatic Foundation for the Expected Shortfall, SSRN 3423042, version of 12 March 2020; Management Science 67(3), 2021. https://ssrn.com/abstract=3423042, https://doi.org/10.1287/mnsc.2020.3617
  • P. Artzner, F. Delbaen, J.-M. Eber and D. Heath, Coherent Measures of Risk, Mathematical Finance 9(3), 1999. https://doi.org/10.1111/1467-9965.00068
  • S. Kusuoka, On Law Invariant Coherent Risk Measures, Advances in Mathematical Economics 3, 2001. https://doi.org/10.1007/978-4-431-67891-5_4
  • C. Acerbi and D. Tasche, On the Coherence of Expected Shortfall, Journal of Banking & Finance 26(7), 2002. https://doi.org/10.1016/S0378-4266(02)00283-2
  • Basel Committee on Banking Supervision, Minimum Capital Requirements for Market Risk, 2019. https://www.bis.org/bcbs/publ/d457.htm
  • H. Föllmer and A. Schied, Stochastic Finance: An Introduction in Discrete Time, 4th ed., De Gruyter, 2016. https://doi.org/10.1515/9783110463453
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Functional AnalysisMathematical PhysicsRepresentation Theory·Captain: mikedeng1

C*-Algebras and Direct Integral Decomposition for Lie Supergroups: Unitary Representations of a Lie Supergroup and Nondegenerate -Representations of Its C-Algebra Form Isomorphic CategoriesResearch Paper

Motivation

Unitary representations turn symmetries into operators on Hilbert spaces. For ordinary locally compact groups, the associated group C∗C^*C∗-algebra lets one study these operators through a single algebraic object. A Lie supergroup adds odd infinitesimal symmetries to an ordinary Lie group. Its unitary representations must respect both the group action and those odd operators. Neeb and Salmasian construct a C∗C^*C∗-algebra A(G,g)\mathcal A(G,\mathfrak g)A(G,g) that captures this combined structure Neeb–Salmasian 2015. The representation correspondence is the point at which their construction becomes useful: a representation of A\mathcal AA retains precisely the data of a unitary supergroup representation.

The paper subsequently uses this bridge to discuss direct integral decompositions through the C∗C^*C∗-algebra. This mission concerns the bridge itself, Theorem 6.4. Its input is not a special connected or nilpotent group: the paper works with an arbitrary finite-dimensional Lie supergroup. The later CCR results in §7 add hypotheses and are outside this mission.

Setting

A finite-dimensional Lie supergroup is a pair (G,g)(G,\mathfrak g)(G,g). Here GGG is a real Lie group and g=g0ˉ⊕g1ˉ\mathfrak g=\mathfrak g_{\bar 0}\oplus\mathfrak g_{\bar 1}g=g0ˉ​⊕g1ˉ​ is a real Lie superalgebra. Its even part g0ˉ\mathfrak g_{\bar 0}g0ˉ​ is the Lie algebra of GGG. The group acts smoothly on the superalgebra by an adjoint action whose even restriction is the derivative of conjugation; differentiation of the action recovers the superbracket. These are the conditions of Definition 2.1, including the finite-dimensional convention stated just after it.

A unitary representation consists of a graded complex Hilbert space H=H0ˉ⊕H1ˉ\mathcal H=\mathcal H_{\bar 0}\oplus\mathcal H_{\bar 1}H=H0ˉ​⊕H1ˉ​, a strongly continuous unitary action π\piπ of GGG preserving that grading, and a real-linear superalgebra action ρπ\rho^\piρπ on the space H∞\mathcal H^\inftyH∞ of smooth orbit vectors. On even elements, ρπ\rho^\piρπ equals the derived group action. On odd elements, e−πi/4ρπ(x)e^{-\pi i/4}\rho^\pi(x)e−πi/4ρπ(x) is symmetric, and the odd action transforms under GGG through the adjoint action. This is Definition 2.3, including its parity and bracket requirements.

The paper adjoins a parity element ε\varepsilonε and writes Gε=G×{1,ε}G_\varepsilon=G\times\{1,\varepsilon\}Gε​=G×{1,ε}. A test function on this group is a pair of smooth, compactly supported complex functions on GGG. Using the complex universal enveloping algebra, the authors form an algebraic crossed product A∘\mathcal A^\circA∘. A word D=x1⋯xkD=x_1\cdots x_kD=x1​⋯xk​ and a test function fff act in each unitary representation by the bounded operator ρπ(D)π(f)\rho^\pi(D)\pi(f)ρπ(D)π(f). The norm of an algebraic element is the supremum of the norms of these represented operators; completion after quotienting its zero seminorm gives the non-unital C∗C^*C∗-algebra A=A(G,g)\mathcal A=\mathcal A(G,\mathfrak g)A=A(G,g) §§3–4.

A star representation of A\mathcal AA on H\mathcal HH is nondegenerate when the span of its image applied to H\mathcal HH is dense. A morphism between two unitary supergroup representations is a bounded, even, complex-linear operator intertwining both their GGG-actions and their g\mathfrak gg-actions on smooth vectors. A morphism between C∗C^*C∗-algebra representations intertwines every element of A\mathcal AA.

Formalization targets

Uniform control and smooth multiplier action

The first targets are the uniform bound of Proposition 3.2 and the smoothness statement of Proposition 5.1. For each word DDD and test pair fff, the same constant works for every unitary representation:

∃MD,f>0∀(π,ρπ,H),∥ρπ(D)π(f)∥≤MD,f.\exists M_{D,f}>0\quad\forall(\pi,\rho^\pi,\mathcal H),\qquad \|\rho^\pi(D)\pi(f)\|\le M_{D,f}.∃MD,f​>0∀(π,ρπ,H),∥ρπ(D)π(f)∥≤MD,f​.

The left multiplier orbit g↦ηG(g)ag\mapsto\eta_G(g)ag↦ηG​(g)a is smooth for every a∈A∘a\in\mathcal A^\circa∈A∘. The construction from a nondegenerate representation also identifies its smooth vectors with the represented algebraic core, as in Lemma 6.2. These are the analytic steps named in the milestone list.

Isomorphism of representation categories

The goal is Theorem 6.4. Propositions 6.1 and 6.3 give mutually inverse assignments on objects, and Theorem 6.4 retains the same intertwiners:

URep⁡(G,g)  ≅  Rep⁡nd(A(G,g)).\operatorname{URep}(G,\mathfrak g) \;\cong\; \operatorname{Rep}_{\mathrm{nd}}\bigl(\mathcal A(G,\mathfrak g)\bigr).URep(G,g)≅Repnd​(A(G,g)).

Thus each unitary representation yields exactly one nondegenerate representation agreeing on every generator, each nondegenerate representation comes from exactly one unitary supergroup representation, and a bounded operator intertwines one pair exactly when it intertwines the other. The goal includes all three clauses.

Significance

The result lets questions about unitary Lie supergroup representations be transferred to a C∗C^*C∗-algebra without losing the odd infinitesimal action or the morphisms. In the paper, this is the foundation for the later direct integral discussion and CCR criteria. Without the equivalence, properties of A\mathcal AA would have no stated connection to decomposition of unitary supergroup representations §7.

The mathematical result is proved in the cited paper; the local Lean declarations are open statements. A complete formal development would add machine-checked proofs for the uniform operator bounds, the algebra and multiplier facts, reconstruction of the odd action, and the categorical equivalence. The reusable parts include smooth-vector actions, integrated test-function operators, and a universal bounded family of representations.

Difficulty

The odd infinitesimal operators are defined on H∞\mathcal H^\inftyH∞, not automatically as bounded operators on all of H\mathcal HH. Integrating π\piπ against a test function supplies smooth vectors, but it does not by itself give a bound for an arbitrary word in the odd and even operators that is uniform over every representation. That uniformity is needed to construct one C∗C^*C∗-norm. In the reverse direction, a nondegenerate representation of A\mathcal AA first gives bounded operators; recovering the derived action on precisely the smooth core requires the multiplier and smoothness statements. An object-level bijection alone would still miss the paper's assertion about intertwiners.

Formalization scope

Lean models GGG as a finite-dimensional smooth real Lie group, with g0ˉ\mathfrak g_{\bar 0}g0ˉ​ its Mathlib group Lie algebra and g1ˉ\mathfrak g_{\bar 1}g1ˉ​ a finite-dimensional real normed space. The superbracket and odd adjoint action are fields of a Harish–Chandra pair. Smoothness uses C∞C^\inftyC∞, not analyticity. The group is neither assumed connected nor second countable. A left Haar measure is fixed. The Hilbert spaces quantified in the mission belong to Type; the index of all such unitary representations belongs to Type 1.

The test space D(Gε)\mathcal D(G_\varepsilon)D(Gε​) is encoded as pairs of functions, and the enveloping-algebra elements needed here as finite words. A\mathcal AA is the closed non-unital star subalgebra of the bounded product of operator algebras generated by their representation families. This uses all Type-small unitary representations; the paper takes unitary-equivalence classes of cyclic ones, which yield the same norm through its Remark 2.5. The algebra depends only on (G,g)(G,\mathfrak g)(G,g) and Haar measure, and ρπ\rho^\piρπ acts on H∞\mathcal H^\inftyH∞ itself. This rules out a choice of algebra or an off-domain operator value that would make the correspondence automatic.

The published smooth-orbit and vector-integral definitions from van Dijk–Neeb–Salmasian–Zellner are reused. Completing this mission calls for the Dixmier–Malliavin factorization, Gårding smoothing, bounded operator estimates, non-unital C∗C^*C∗-algebra representations and multiplier actions. Contributions proving those general tools or the source-labelled milestones are within scope. The generator family is represented through vectors rather than an operator-norm Bochner integral, whose measurability is unavailable for a merely strongly continuous representation.

Selected references

  • K.-H. Neeb and H. Salmasian, “C*-algebras and direct integral decomposition for Lie supergroups,” arXiv:1506.01558v1, 2015. Preprint.
  • G. van Dijk, K.-H. Neeb, H. Salmasian and C. Zellner, On the characterization of trace class representations and Schwartz operators, arXiv:1512.02451v1, 2015. Preprint.
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Functional AnalysisQuantum Information·Captain: mikedeng1

Approximation of Multipartite Quantum States and the Relative Entropy of Entanglement: Lower Semicontinuity of the Relative Entropy of Entanglement at States with n−1 FA-Property MarginalsResearch Paper

Motivation

The relative entropy of entanglement measures how distinguishable a multipartite quantum state is from all fully separable states. In finite dimensions it is a standard entanglement measure, but infinite-dimensional systems raise a basic analytical problem: the measure may take the value +∞+\infty+∞, and finite-rank approximations do not automatically control its behavior at a limit state. Shirokov's analysis identifies a broad class of states at which the direct relative entropy of entanglement is finite and lower semicontinuous. The result applies when all but possibly one marginal state satisfy the FA-property, a spectral condition that includes useful finite-entropy states without requiring finite-dimensional Hilbert spaces.

The paper relates the direct measure to a universal extension formed from local finite-rank compressions. This mission isolates the ERE_RER​ part of Theorem 2 A) and the source results needed to reach it. A later paper by Lami and Shirokov addresses more general global lower semicontinuity questions using a different operator model and hypotheses; its statements are related work, not imports into this mission. Shirokov, §4.3; Lami–Shirokov.

Setting

There are nnn parties A1,…,AnA_1,\ldots,A_nA1​,…,An​, with separable Hilbert spaces HAs\mathcal H_{A_s}HAs​​. A state ρ\rhoρ is a positive trace-class operator with trace one on their joint system. Its marginal ρAs\rho_{A_s}ρAs​​ is obtained by tracing out every party except AsA_sAs​. A product state is a tensor product of one state per party. The set Ss\mathfrak S_sSs​ of fully separable states is the trace-norm closed convex hull of product states. Closure matters in infinite dimension: restricting to finite convex combinations would change the infimum below. Shirokov, pp. 10–11, (26).

Write H(ρ∥σ)H(\rho\|\sigma)H(ρ∥σ) for Lindblad's quantum relative entropy, including the trace correction for unnormalized positive operators and the value +∞+\infty+∞ on support failure. The direct relative entropy of entanglement is

ER(ρ)=inf⁡σ∈SsH(ρ∥σ).E_R(\rho)=\inf_{\sigma\in\mathfrak S_s}H(\rho\|\sigma).ER​(ρ)=σ∈Ss​inf​H(ρ∥σ).

The von Neumann entropy H(ρ)H(\rho)H(ρ) and ER(ρ)E_R(\rho)ER​(ρ) are extended nonnegative real quantities in natural-logarithm units. A state has the FA-property when its eigenvalues λj\lambda_jλj​ admit nonnegative numbers gjg_jgj​ with ∑jλjgj<+∞\sum_j\lambda_jg_j<+\infty∑j​λj​gj​<+∞ and lim⁡β↓0(∑je−βgj)β=1\lim_{\beta\downarrow0}(\sum_je^{-\beta g_j})^\beta=1limβ↓0​(∑j​e−βgj​)β=1. In particular, the FA-property implies finite entropy. The set S∗\mathfrak S_*S∗​ consists of joint states with the FA-property on at least n−1n-1n−1 marginals. Shirokov, pp. 2, 4, 14, (1), (34).

For each party, a finite-rank orthogonal projector compresses the joint state. The universal extension E^R\widehat E_RER​ takes the supremum of the homogeneous ERE_RER​ values of all such local compressions. A compressed positive operator XXX with trace c>0c>0c>0 is valued as cER(X/c)cE_R(X/c)cER​(X/c); the zero operator has value zero. Local spectral projectors built from the marginals define the approximation ΛrL(ρ)\Lambda_r^L(\rho)ΛrL​(ρ) used in Theorem 1. Shirokov, pp. 7, 12–13, (17), (31).

Formalization targets

Goal: Theorem 2 A), the ERE_RER​ case

For ρ0∈S∗\rho_0\in\mathfrak S_*ρ0​∈S∗​, ER(ρ0)<+∞E_R(\rho_0)<+\inftyER​(ρ0​)<+∞. For every sequence of states ρk→ρ0\rho_k\to\rho_0ρk​→ρ0​ in trace norm,

ER(ρ0)≤lim inf⁡k→∞ER(ρk).E_R(\rho_0)\le\liminf_{k\to\infty}E_R(\rho_k).ER​(ρ0​)≤k→∞liminf​ER​(ρk​).

The sequence itself may lie anywhere in the full state space. This is the sequential lower semicontinuity assertion (35), together with finiteness, in Theorem 2 A).

Supporting targets

The milestones, in attack order, are: the FA entropy consequence (p. 4); the pure-state separable comparison of Lemma 3; the σ\sigmaσ-convexity of ERE_RER​ (first sentence of Theorem 2 E)); the upper bound (28) by any n−1n-1n−1 marginal entropies,

ER(ρ)≤∑s≠tH(ρAs);E_R(\rho)\le\sum_{s\ne t}H(\rho_{A_s});ER​(ρ)≤s=t∑​H(ρAs​​);

the concavity-defect bound (27), pER(ρ)+(1−p)ER(σ)≤ER(pρ+(1−p)σ)+h2(p)pE_R(\rho)+(1-p)E_R(\sigma)\le E_R(p\rho+(1-p)\sigma)+h_2(p)pER​(ρ)+(1−p)ER​(σ)≤ER​(pρ+(1−p)σ)+h2​(p); membership of ERE_RER​ in Lnn−1(1,1)L_n^{n-1}(1,1)Lnn−1​(1,1); the LLL-class assertion of Theorem 1; the relative-entropy inequality of Lemma 1 for positive maps with trace-preserving sum; the comparison E^R≤ER\widehat E_R\le E_RER​≤ER​; lower semicontinuity of E^R\widehat E_RER​; and the equality ER=E^RE_R=\widehat E_RER​=ER​ on S∗\mathfrak S_*S∗​ (Theorem 2 B)). These are claims made in the paper, with the portions outside the ERE_RER​ route explicitly scoped in the item descriptions. Shirokov, pp. 4, 8, 11, 13–15, 20, 25.

Significance

The theorem gives a stable finite value of ERE_RER​ at every state in S∗\mathfrak S_*S∗​: approximating sequences cannot converge there while hiding a smaller limiting value. This matters when infinite-dimensional states are approximated by finite-rank or energy-constrained states, because pointwise convergence of operators alone does not control an extended-valued entanglement measure. The equality with E^R\widehat E_RER​ also identifies the direct measure with a globally lower semicontinuous construction on the stated domain. Shirokov, Theorem 2 and discussion in §4.3.

The mathematical result is proved in the source paper. The formalization work is to express its spectral FA condition, multipartite partial traces, trace-norm separability, finite-rank compression, homogeneous extension, and extended-real inequalities in Lean, then prove the milestones and goal. The published P01 definition already supplies von Neumann entropy and Lindblad relative entropy; the propositions in this mission are open Lean statements, not machine-checked proofs. This shared infrastructure can support other infinite-dimensional quantum information results involving separability and marginal entropies.

Difficulty

A direct argument from the infimum defining ERE_RER​ cannot simply exchange that infimum with a state limit: the separable comparison state that nearly minimizes at one point need not remain useful along a convergent sequence. Infinite values also make real-valued continuity bounds insufficient. The paper's theorem therefore has to coordinate a finite-entropy estimate on n−1n-1n−1 marginals with control of local finite-rank approximations and a lower semicontinuous extension. The approximation estimate is uniform over a class of functions, with the rank threshold and error sequence chosen before the function. Shirokov, Theorem 1 and proof of Theorem 2 A).

Formalization scope

Each HAs\mathcal H_{A_s}HAs​​ is represented as ℓ2(Is)\ell^2(I_s)ℓ2(Is​) for a countable basis index type. Parties are indexed by Fin⁡(n)\operatorname{Fin}(n)Fin(n), and the joint basis uses their dependent Cartesian product. The state topology is the trace-norm topology of the published P33 state structure. Entropy, relative entropy, and ERE_RER​ take values in [0,+∞][0,+\infty][0,+∞]; no real-valued surrogate replaces an infinite value. The FA-property requires an actual orthonormal eigenbasis tied to the state's coefficients. Its partition sum is computed in [0,+∞][0,+\infty][0,+∞], so divergence cannot default to zero. The definition of S∗\mathfrak S_*S∗​ says at least n−1n-1n−1 FA marginals and does not impose FA on the sequence in the goal.

The Lnm(C,D)L_n^m(C,D)Lnm​(C,D) class is represented with a finite set of FA parties in place of the first mmm parties, reflecting the paper's relabeling symmetry. Within that class, ERE_RER​ is converted to a real number only on the finite-entropy domain. The universal extension uses all finite orthonormal local families and the homogeneous convention for compressed positive operators. The setting also defines countable separable decompositions, finite-rank projectors, the spectral approximation relation, binary entropy in nats, and positive linear maps on the trace class. The proviso of (27) that "all the involved quantities are finite" (p. 11) is stated as finiteness of ERE_RER​ at the two mixed states. These definitions and the cited P01/P33 libraries are the reusable work. A definition of FA that every state satisfies, a separable set without trace closure, or a real ERE_RER​ that discards +∞+\infty+∞ would trivialize or alter the target.

The paper also states a regularized ER∞E_R^\inftyER∞​ case. It is outside this mission: its proof in version 2 invokes propositions by broken “??” references that are absent from the source. The hatted-class and NNN-class portions of Theorem 1, the regularized equality in Theorem 2 B), and the entanglement-monotone part of the universal-extension bullet are likewise outside these ERE_RER​ milestones. Contributions proving the stated Lean milestones, improving the common operator definitions, and then proving the goal are welcome.

Selected references

  • M. E. Shirokov, Approximation of multipartite quantum states and the relative entropy of entanglement, arXiv preprint, version 2, 2024. arXiv:2103.12111v2.
  • L. Lami and M. E. Shirokov, Attainability and lower semi-continuity of the relative entropy of entanglement, and variations on the theme, arXiv preprint, 2021. arXiv:2105.08091.
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Information TheoryQuantum Information·Captain: mikedeng1

General Benchmarks for Quantum Repeaters: For the Qudit Dephasing Channel the Entanglement-Flux Upper Bound Meets the Coherent Information, log₂ d − H(P)Research Paper

Motivation

A quantum repeater is judged by how much it beats direct transmission over a point-to-point link. The natural yardsticks are the two-way assisted capacities of the link's channel E\mathcal EE: the quantum capacity Q2(E)Q_2(\mathcal E)Q2​(E) and the secret-key capacity K(E)K(\mathcal E)K(E), the best rates of entanglement and key that two parties can obtain over many uses of E\mathcal EE when unlimited two-way classical communication and local operations are free. Computing them exactly for a given channel is rare, because it requires a lower and an upper bound that meet.

Pirandola and Laurenza (arXiv:1512.04945v2, 2016) obtain such matching bounds for a family of channels. The lower bound is the coherent information of the channel (with its reverse version), which is achievable by the hashing protocol. The upper bound is the entanglement flux Φ(E)\Phi(\mathcal E)Φ(E), the relative entropy of entanglement of the channel's Choi matrix, which bounds KKK for channels that can be simulated by teleportation. For the qudit dephasing channel the two bounds coincide, which gives Q2=K=log⁡2d−H(P)Q_2=K=\log_2 d-H(\mathbf P)Q2​=K=log2​d−H(P) (Eqs. (20) and (95)). This mission formalizes that coincidence.

Setting

Fix a dimension d≥2d\ge2d≥2 and the computational basis {∣j⟩}j=0d−1\{|j\rangle\}_{j=0}^{d-1}{∣j⟩}j=0d−1​ of a qudit. Let ω=e2πi/d\omega=e^{2\pi i/d}ω=e2πi/d and let ZZZ be the generalized phase operator, Z∣j⟩=ωj∣j⟩Z|j\rangle=\omega^j|j\rangleZ∣j⟩=ωj∣j⟩. For a dephasing probability p∈[0,1]p\in[0,1]p∈[0,1] define the binomial weights

Pm(p,d)=(d−1m)pm(1−p)d−1−m,m=0,…,d−1,P_m(p,d)=\binom{d-1}{m}p^m(1-p)^{d-1-m},\qquad m=0,\dots,d-1,Pm​(p,d)=(md−1​)pm(1−p)d−1−m,m=0,…,d−1,

and the qudit dephasing channel, given by its Kraus operators,

Pd(ρ)=∑m=0d−1EmρEm†,Em=Pm(p,d) Zm.\mathcal P_d(\rho)=\sum_{m=0}^{d-1}E_m\rho E_m^\dagger,\qquad E_m=\sqrt{P_m(p,d)}\,Z^m .Pd​(ρ)=m=0∑d−1​Em​ρEm†​,Em​=Pm​(p,d)​Zm.

Write P={Pm(p,d)}m\mathbf P=\{P_m(p,d)\}_mP={Pm​(p,d)}m​ and H(P)=−∑mPmlog⁡2PmH(\mathbf P)=-\sum_mP_m\log_2P_mH(P)=−∑m​Pm​log2​Pm​ (with 0log⁡0=00\log0=00log0=0) for its Shannon entropy.

The Choi matrix of a map E\mathcal EE on d×dd\times dd×d matrices is ρE=(I⊗E)(Ψd)\rho_{\mathcal E}=(\mathcal I\otimes\mathcal E)(\Psi_d)ρE​=(I⊗E)(Ψd​), where ∣Ψd⟩=d−1/2∑i∣ii⟩|\Psi_d\rangle=d^{-1/2}\sum_i|ii\rangle∣Ψd​⟩=d−1/2∑i​∣ii⟩. The first tensor factor is the reference RRR, the second the channel output BBB. With the von Neumann entropy S(ρ)=−Tr ρlog⁡2ρS(\rho)=-\mathrm{Tr}\,\rho\log_2\rhoS(ρ)=−Trρlog2​ρ:

  • the coherent information of the channel is IC(E)=S(TrRρE)−S(ρE)I_C(\mathcal E)=S(\mathrm{Tr}_R\rho_{\mathcal E})-S(\rho_{\mathcal E})IC​(E)=S(TrR​ρE​)−S(ρE​);
  • the reverse coherent information is IRC(E)=S(TrBρE)−S(ρE)I_{RC}(\mathcal E)=S(\mathrm{Tr}_B\rho_{\mathcal E})-S(\rho_{\mathcal E})IRC​(E)=S(TrB​ρE​)−S(ρE​);
  • the relative entropy is S(ρ∥σ)=Tr[ρ(log⁡2ρ−log⁡2σ)]S(\rho\|\sigma)=\mathrm{Tr}[\rho(\log_2\rho-\log_2\sigma)]S(ρ∥σ)=Tr[ρ(log2​ρ−log2​σ)], and +∞+\infty+∞ when the support of ρ\rhoρ is not inside that of σ\sigmaσ;
  • the relative entropy of entanglement of a bipartite state is ER(ρ)=inf⁡σ∈SEPS(ρ∥σ)E_R(\rho)=\inf_{\sigma\in\mathrm{SEP}}S(\rho\|\sigma)ER​(ρ)=infσ∈SEP​S(ρ∥σ), the infimum over all separable states for the cut R:BR:BR:B;
  • the entanglement flux of the channel is Φ(E)=ER(ρE)\Phi(\mathcal E)=E_R(\rho_{\mathcal E})Φ(E)=ER​(ρE​).

The paper's candidate separable state is σ~=∑i1d∣i⟩⟨i∣⊗Pd(∣i⟩⟨i∣)\tilde\sigma=\sum_i\frac1d|i\rangle\langle i|\otimes\mathcal P_d(|i\rangle\langle i|)σ~=∑i​d1​∣i⟩⟨i∣⊗Pd​(∣i⟩⟨i∣).

Formalization targets

Goal (Eqs. (94)–(95), p. 11)

For every d≥2d\ge2d≥2 and p∈[0,1]p\in[0,1]p∈[0,1]:

IC(Pd)=IRC(Pd)=log⁡2d−H(P),Φ(Pd)≤log⁡2d−H(P).I_C(\mathcal P_d)=I_{RC}(\mathcal P_d)=\log_2d-H(\mathbf P),\qquad \Phi(\mathcal P_d)\le\log_2d-H(\mathbf P).IC​(Pd​)=IRC​(Pd​)=log2​d−H(P),Φ(Pd​)≤log2​d−H(P).

The lower and the upper bound on the two-way capacities therefore meet. The statement keeps ddd and ppp free and asserts exact values, not numerical constants.

Milestones (in attack order)

  1. The Choi matrix of Pd\mathcal P_dPd​ in closed form (p. 11, display between Eqs. (90) and (91)).
  2. Eq. (91): S(ρPd)=H(P)S(\rho_{\mathcal P_d})=H(\mathbf P)S(ρPd​​)=H(P).
  3. Eq. (68): S(ρ∥σ)=−S(ρ)−∑i⟨i∣ρ∣i⟩log⁡siS(\rho\|\sigma)=-S(\rho)-\sum_i\langle i|\rho|i\rangle\log s_iS(ρ∥σ)=−S(ρ)−∑i​⟨i∣ρ∣i⟩logsi​ in the eigenbasis of σ\sigmaσ, under support inclusion.
  4. Eq. (92): σ~=∑i1d∣ii⟩⟨ii∣\tilde\sigma=\sum_i\frac1d|ii\rangle\langle ii|σ~=∑i​d1​∣ii⟩⟨ii∣ and σ~\tilde\sigmaσ~ is separable.
  5. Eq. (93): Tr(ρPdlog⁡2σ~)=−log⁡2d\mathrm{Tr}(\rho_{\mathcal P_d}\log_2\tilde\sigma)=-\log_2dTr(ρPd​​log2​σ~)=−log2​d, with the support of ρPd\rho_{\mathcal P_d}ρPd​​ inside that of σ~\tilde\sigmaσ~.
  6. Eq. (94): Φ(Pd)≤S(ρPd∥σ~)=log⁡2d−H(P)\Phi(\mathcal P_d)\le S(\rho_{\mathcal P_d}\|\tilde\sigma)=\log_2d-H(\mathbf P)Φ(Pd​)≤S(ρPd​​∥σ~)=log2​d−H(P).
  7. Eq. (45): for a unital, trace-preserving map E\mathcal EE, IC(E)=IRC(E)=log⁡2d−S(ρE)I_C(\mathcal E)=I_{RC}(\mathcal E)=\log_2d-S(\rho_{\mathcal E})IC​(E)=IRC​(E)=log2​d−S(ρE​).

Significance

The result. The coincidence of the two bounds pins down Q2Q_2Q2​ and KKK of the qudit dephasing channel for every ddd and ppp, which gives the repeaterless benchmark for any qudit link dominated by dephasing. At d=2d=2d=2 it recovers the qubit dephasing benchmark 1−H2(p)1-H_2(p)1−H2​(p) of the same paper (Eq. (75), with p↔1−pp\leftrightarrow1-pp↔1−p, which the binary entropy does not see). Combined with the operational facts the paper imports (the hashing inequality and the bound of KKK by the flux for teleportation-covariant channels), it yields the capacity formula (95).

Formalizing it. The paper's computation is complete but terse. The formalization makes three implicit points explicit: the support of the Choi matrix lies inside the support of the rank-ddd state σ~\tilde\sigmaσ~ (so log⁡σ~\log\tilde\sigmalogσ~ is taken on its support); the claim of "ddd non-zero eigenvalues" in (91) fails at p∈{0,1}p\in\{0,1\}p∈{0,1}, while the entropy identity does not; and (45) needs trace preservation as well as unitality. The results are proved in the paper and, as far as the platform's catalogue shows, formalized nowhere. Eq. (68) and Eq. (45) are reusable lemmas about arbitrary states and unital channels.

Difficulty

The calculation on the page is short; the difficulty lies in what it leaves to the reader. The entropy identity (91) asks for the spectrum of a d2×d2d^2\times d^2d2×d2 matrix that is not diagonal in the computational basis, while the von Neumann entropy is defined through the matrix functional calculus, so "diagonalizing" has to be made precise. The state σ~\tilde\sigmaσ~ has rank ddd in dimension d2d^2d2: the relative entropy against it is finite only because of a support inclusion the paper does not mention, and a computation that ignores the kernel of σ~\tilde\sigmaσ~ does not establish the value. The upper bound needs σ~\tilde\sigmaσ~ to be separable in the sense of the infimum, a finite convex combination of product density matrices, not merely diagonal. Finally, the coherent information is a difference of entropies of a partial trace and of the full Choi matrix; equating it to log⁡2d−H(P)\log_2 d-H(\mathbf P)log2​d−H(P) requires both that the output marginal is maximally mixed and the entropy identity (91).

Formalization scope

Qudit indices are Fin d, with d≥2d\ge2d≥2 (and [NeZero d] where an instance needs it); ppp is real with 0≤p≤10\le p\le10≤p≤1. ZmZ^mZm is a matrix power, ω=exp⁡(2πi/d)\omega=\exp(2\pi i/d)ω=exp(2πi/d), and the channel is the published QAlgorithms.krausApply of the Kraus family Pm Zm\sqrt{P_m}\,Z^mPm​​Zm. The Choi matrix is the published QAlgorithms.idTensorSuperop applied to maximallyEntangledProjector d (entries 1/d1/d1/d on ∣ii⟩⟨jj∣|ii\rangle\langle jj|∣ii⟩⟨jj∣), the reference being the first factor of Fin d × Fin d. Entropies are in bits with 0log⁡0=00\log0=00log0=0: QAlgorithms.vnEntropy for states and a local Shannon entropy for the weights. The partial traces are QAlgorithms.traceLeft (over the reference) and QAlgorithms.traceRight (over the output). The relative entropy and ERE_RER​ are the published relativeEntropyBits and relativeEntanglement (Umegaki entropy divided by ln⁡2\ln2ln2, +∞+\infty+∞ off support, infimum over IsSeparableDensity, values in [0,∞][0,\infty][0,∞]). The real bound is embedded with ENNReal.ofReal; since H(P)≤log⁡2dH(\mathbf P)\le\log_2dH(P)≤log2​d, nothing is lost.

None of the defined quantities is given by its closed form: the Choi matrix is computed from the channel, ERE_RER​ is the infimum over all separable states (not S(ρ∥σ~)S(\rho\|\tilde\sigma)S(ρ∥σ~) or an infimum over diagonal states), and ICI_CIC​ is defined from partial traces, not as log⁡2d−S(ρE)\log_2d-S(\rho_{\mathcal E})log2​d−S(ρE​). This rules out the trivializing formalization in which a milestone or the goal holds by definition. The bound log⁡2d\log_2dlog2​d alone holds for every state; the goal's bound is log⁡2d−H(P)\log_2d-H(\mathbf P)log2​d−H(P).

The operational capacities Q2Q_2Q2​ and KKK of Eq. (95) are not formalized. They are defined over adaptive LOCC protocols with private-state targets, which have no substrate on the platform. The paper also does not prove the two bridges from them to the bounds: it imports K≤ΦK\le\PhiK≤Φ (Eq. (2), from Pirandola et al.) and the hashing inequality (from Devetak and Winter). For the same reason, the reverse inequality Φ(Pd)≥log⁡2d−H(P)\Phi(\mathcal P_d)\ge\log_2d-H(\mathbf P)Φ(Pd​)≥log2​d−H(P) is not stated, since the paper obtains it only through the hashing bound. Teleportation stretching, convexity of the flux, the bosonic Gaussian channels and the erasure channel are outside this mission.

Contributions are welcome at every level: the spectrum of circulant blocks, the support calculus of the Umegaki entropy, and the separable decomposition of diagonal states are all reusable beyond this mission.

Selected references

  • S. Pirandola, R. Laurenza, General Benchmarks for Quantum Repeaters, arXiv preprint, v2, 2016. https://arxiv.org/abs/1512.04945v2
  • S. Pirandola, R. Laurenza, C. Ottaviani, L. Banchi, Fundamental limits of repeaterless quantum communications, Nature Communications 8, 15043, 2017. https://doi.org/10.1038/ncomms15043
  • I. Devetak, A. Winter, Distillation of secret key and entanglement from quantum states, Proc. R. Soc. A 461, 207–235, 2005. https://doi.org/10.1098/rspa.2004.1372
  • V. Vedral, M. B. Plenio, Entanglement measures and purification procedures, Phys. Rev. A 57, 1619, 1998. https://doi.org/10.1103/PhysRevA.57.1619
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Mathematical PhysicsProbabilityQuantum Information·Captain: mikedeng1

Large Deviations in Quantum Spin Chain: Full Large Deviation Principle with a Good Rate Function for C*-Finitely Correlated StatesResearch Paper

Motivation

Measurements of long quantum spin chains can have outcomes far from their typical values. A large-deviation principle quantifies how quickly the probability of such outcomes decreases with the number of sites. In a classical lattice system this is a standard way to describe rare macroscopic fluctuations; in a quantum chain, observables on overlapping sets of sites generally fail to commute, which makes the corresponding probability laws harder to analyze. Ogata's 2008 paper establishes a full principle for the energy density of any translation-invariant finite-range interaction in a C∗C^*C∗-finitely correlated state. Its introduction explains that earlier spin-chain results covered upper bounds or more restricted observables and states, while the lower bound for general observables remained the substantial issue. Ogata, pp. 2–4

The finitely correlated class includes local states generated from finite auxiliary memory. It is large enough to include mixtures and periodic behavior, so a theorem restricted to a primitive transfer map would miss part of Ogata's statement. This mission targets the printed Theorem 1.2 in its full scope. Ogata, p. 4

Setting

At each site let Md(C)M_d(\mathbb C)Md​(C) be the algebra of complex d×dd\times dd×d matrices. On sites 1,…,n1,\ldots,n1,…,n, the local algebra is the nnn-fold tensor product, represented as matrices whose rows and columns are spin configurations. A finite-range translation-invariant interaction Φ\PhiΦ assigns a Hermitian operator Φ(X)\Phi(X)Φ(X) to each finite set of sites X⊂ZX\subset\mathbb ZX⊂Z, with the same term on translated sets and with Φ(X)=0\Phi(X)=0Φ(X)=0 when the diameter of XXX exceeds a fixed range. Its finite-volume Hamiltonian is

HΦ([1,n])=∑X⊆[1,n]Φ(X).H_\Phi([1,n])=\sum_{X\subseteq[1,n]}\Phi(X).HΦ​([1,n])=X⊆[1,n]∑​Φ(X).

The sum includes the scalar term associated with the empty set. The interaction need not be nearest-neighbor and may have a term on any finite pattern within its range. Ogata, pp. 2–3

A C∗C^*C∗-finitely correlated state is specified by a finite-dimensional auxiliary algebra B\mathcal BB, a unital completely positive map E:Md(C)⊗B→B\mathcal E:M_d(\mathbb C)\otimes\mathcal B\to\mathcal BE:Md​(C)⊗B→B, and a faithful stationary state ρ\rhoρ on B\mathcal BB. Iterating E\mathcal EE gives a compatible local state ωn\omega_nωn​ on nnn sites. The probability measure μn,Φ\mu_{n,\Phi}μn,Φ​ is the spectral distribution of HΦ([1,n])/nH_\Phi([1,n])/nHΦ​([1,n])/n in ωn\omega_nωn​: for a Borel set B⊆RB\subseteq\mathbb RB⊆R, it assigns the state weight of the spectral projection corresponding to BBB. These local restrictions determine the distributions used in the theorem. Ogata, pp. 3–4

Formalization targets

Full large-deviation principle

The goal is a good rate function I:R→[0,∞]I:\mathbb R\to[0,\infty]I:R→[0,∞]: III is lower semicontinuous and each set {x:I(x)≤a}\{x:I(x)\le a\}{x:I(x)≤a} is compact for finite a≥0a\ge0a≥0. For every closed CCC and open OOO in R\mathbb RR, Theorem 1.2 asserts

lim sup⁡n→∞1nlog⁡μn,Φ(C)≤−inf⁡x∈CI(x),\limsup_{n\to\infty}\frac1n\log\mu_{n,\Phi}(C)\le-\inf_{x\in C}I(x),n→∞limsup​n1​logμn,Φ​(C)≤−x∈Cinf​I(x), lim inf⁡n→∞1nlog⁡μn,Φ(O)≥−inf⁡x∈OI(x).\liminf_{n\to\infty}\frac1n\log\mu_{n,\Phi}(O)\ge-\inf_{x\in O}I(x).n→∞liminf​n1​logμn,Φ​(O)≥−x∈Oinf​I(x).

One rate function serves both inequalities and every eligible set. The statement asserts existence, without imposing a formula for III or a primitivity condition on the auxiliary map. Ogata, pp. 3–4

Supporting targets

The milestone list includes the paper's Gärtner–Ellis theorem, the spectral-law exponential-moment identity behind equation (1), the two-sided order estimate (15) for a gapped auxiliary map, the regrouping of lll consecutive sites into one site, under which the same state is generated by the lll-th iterate E(l)\mathcal E^{(l)}E(l) of the transfer map and E(l)^1=(E^1)l\widehat{\mathcal E^{(l)}}_1=(\widehat{\mathcal E}_1)^lE(l)1​=(E1​)l, and the differentiable limiting pressure under condition (14). In the last target, the pressure is the limit of n−1log⁡ωn(eαHΦ([1,n]))n^{-1}\log\omega_n(e^{\alpha H_\Phi([1,n])})n−1logωn​(eαHΦ​([1,n])) for every real α\alphaα. These are narrower claims with separate hypotheses; none replaces the full goal. Ogata, pp. 4–5, 12–15

Significance

The theorem gives an exponential-scale description of the energy-density distribution for all translation-invariant finite-range interactions in this state class. The upper bound controls probability on closed sets; the lower bound supplies the matching guarantee for open sets. Compact sublevel sets prevent low-rate mass from escaping to infinity. The result is already proved in Ogata's paper; the remaining work here is a machine-checked development of the statement and its supporting mathematics. Ogata, Theorem 1.2

Formalizing the finite-dimensional transfer construction, its spectral measures, and an extended-valued LDP vocabulary would also make these objects available for later spin-chain results. The goal itself is not currently accompanied by a machine-checked proof in this mission. The Gärtner–Ellis and auxiliary-map statements are likewise proof targets, not asserted as solved Lean facts.

Difficulty

The exponential of a sum of overlapping local interaction terms cannot generally be factored into independent one-site contributions. Even when an auxiliary transfer map has a spectral gap and yields a differentiable limiting pressure, that argument does not directly cover every finitely correlated state. A mixture can have a limiting log moment generating function with a corner; the resulting rate function can be nonconvex. Ogata's printed Lemma 4.1 reduces to special components but omits the separate mixture step needed to recover the unrestricted theorem. The goal retains the theorem's printed hypotheses, while the condition-(14) milestone records precisely the restricted pressure claim. Ogata, pp. 12–15

Formalization scope

The Lean model uses finite matrices for local algebras. A nonempty finite site basis represents Md(C)M_d(\mathbb C)Md​(C), with site 1 indexed by 0. An interaction stores one Hermitian term for each support anchored at its least site; all translates that fit in [1,n][1,n][1,n] appear in the Hamiltonian. The scalar empty-set term is retained. The auxiliary algebra is represented by a full matrix algebra Mk(C)M_k(\mathbb C)Mk​(C); finite-dimensional C∗C^*C∗-algebra data have an equivalent full-matrix representation for the generated local states. Stationarity is written in the primal trace form. The recursive local state places the first site's matrix in the outermost application of E\mathcal EE.

The spectral law is formed from the eigenvalues and spectral weights of the actual Hamiltonian. It is not supplied as an arbitrary sequence of measures. The theorem uses no ergodicity, spectral-gap, or condition-(14) binder, and both LDP bounds range over every closed or open subset of R\mathbb RR. Logarithms of probabilities take values in the extended reals, with log⁡0=−∞\log0=-\inftylog0=−∞; sequence limits are at n→∞n\to\inftyn→∞, so the placeholder value at n=0n=0n=0 is immaterial. Nonnegative lower integrals represent exponential moments. In the restricted pressure milestone, the real logarithm applies to a positive state expectation. These choices also rule out a vacuous proof based on a zero measure, a moment represented by a non-integrable Bochner integral, or a rate function unrelated to the spectral law.

Reusable contributions include finite-dimensional spectral-law lemmas, positivity and stationarity facts for completely positive maps, good-rate-function and LDP lemmas on R\mathbb RR, and the Gärtner–Ellis result. The full theorem additionally needs a treatment of non-ergodic finite mixtures and periodic components that preserves both large-deviation bounds.

Selected references

  • Yoshiko Ogata, Large Deviations in Quantum Spin Chain, arXiv preprint, 2008. arXiv:0803.0113v1.
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Mathematical PhysicsQuantum InformationQuantum Mechanics·Captain: mikedeng1

A No-Go Theorem for Gaussian Quantum Error Correction: Gaussian Encoding and Decoding Cannot Lower the Entanglement Degradation of a Single-Mode Gaussian ChannelResearch Paper

Motivation

Optical quantum communication commonly encodes information in continuous variables such as the position and momentum quadratures of a light mode. Gaussian states and Gaussian operations are attractive in this setting because phase shifters, squeezers, beam splitters, and homodyne measurements are standard optical tools. Transmission through a lossy or noisy line can also be modeled by a Gaussian channel. The practical question is whether adding vacuum modes and Gaussian encoding and decoding can protect a signal against such a channel. Niset, Fiurášek, and Cerf (2008) give a negative answer for the code class defined in their Fig. 1.

The result sits after the early impossibility results for distilling Gaussian entanglement with Gaussian operations, including Giedke and Cirac (2002). Those results concern shared states and allowed local operations. The 2008 paper asks the channel-coding question directly: whether a finite Gaussian code can make a fixed single-mode Gaussian channel less damaging to entanglement. It introduces a scalar, entanglement degradation, to state the answer for every single-mode Gaussian channel in one inequality.

Setting

A single optical mode has two real quadratures, xxx and ppp. For nnn modes, the order is (x1,p1,…,xn,pn)(x_1,p_1,\ldots,x_n,p_n)(x1​,p1​,…,xn​,pn​). A state has a real covariance matrix γ\gammaγ recording its second moments in this order. The vacuum covariance matrix is the identity III. A Gaussian channel TTT on one mode is described at the covariance level by two real 2×22\times22×2 matrices MMM and NNN:

γ⟼MγMT+N.\gamma\longmapsto M\gamma M^{\mathsf T}+N.γ⟼MγMT+N.

Here NNN is the added noise. Complete positivity imposes symmetry and a matrix positivity condition on NNN; in particular, it gives det⁡N≥(det⁡M−1)2\det N\ge(\det M-1)^2detN≥(detM−1)2. A Gaussian unitary changes covariances by a symplectic matrix SSS, satisfying SJST=JSJS^{\mathsf T}=JSJST=J for the canonical symplectic form JJJ. Displacements affect first moments only and therefore play no role in these covariance formulas.

The code G(n,E,D)G(n,E,D)G(n,E,D) uses a positive integer nnn. The input occupies mode zero in the formalization; the other n−1n-1n−1 modes are vacuum ancillas. A Gaussian encoding unitary EEE acts on all modes, then the same channel TTT acts independently once on each mode, and a Gaussian decoding unitary DDD acts on all modes. Only the first output mode is retained. This defines an effective single-mode channel TGCT_{GC}TGC​ with matrices MGC,NGCM_{GC},N_{GC}MGC​,NGC​. The ancillas contribute noise to NGCN_{GC}NGC​ even before the nnn channel uses are counted.

For a channel T=(M,N)T=(M,N)T=(M,N), the paper defines its degradation by

D[T]=min⁡{det⁡N(1+det⁡M)2,1}.D[T]=\min\left\{\frac{\det N}{(1+\det M)^2},1\right\}.D[T]=min{(1+detM)2detN​,1}.

The intended value is 111 when the denominator vanishes: the quotient is then interpreted as infinite and is saturated by the minimum. This quantity is related to the entanglement remaining when TTT acts on one half of a two-mode squeezed vacuum as the squeezing grows. The paper measures that entanglement through the smallest symplectic eigenvalue ν−\nu_-ν−​ after partial transpose and the logarithmic negativity EN=max⁡{0,−log⁡ν−}E_N=\max\{0,-\log\nu_-\}EN​=max{0,−logν−​}.

Formalization targets

Main no-go theorem

The mission goal is the theorem on page 3, equation (11): for every completely positive single-mode Gaussian channel and every finite code of the stated form,

D[T]≤D[TGC].D[T]\le D[T_{GC}].D[T]≤D[TGC​].

This is the assertion that the code cannot lower the channel's entanglement degradation. It includes n=1n=1n=1, singular channels, and channels with negative determinant MMM. No numerical performance constant or bound on the number of modes is fixed.

Supporting results

The milestones record the paper's channel-noise constraint (2), the fact that the code produces a Gaussian channel, the local matrix normal forms used in Lemma 2, the asymptotic calculations (8) and (10), the entanglement-breaking case, and Lemma 2 itself. Lemma 2 characterizes the degradation through the limiting squared eigenvalue and, when finite, gives EN=−12log⁡D[T]E_N=-\tfrac12\log D[T]EN​=−21​logD[T]. The milestones retain the paper's distinction between positive, negative, and zero determinant regimes.

Significance

The theorem rules out a specific and broad way of improving Gaussian transmission: adding any finite number of vacuum ancillas and using Gaussian unitaries before and after independent uses of a fixed channel cannot improve this intrinsic entanglement measure. The paper applies this conclusion to attenuation, amplification, and classical-noise channels, showing how an apparent reduction in one channel parameter can be offset by increased noise. It also relates degradation to an upper bound on quantum capacity, though that further bound is outside this mission. Niset, Fiurášek, and Cerf (2008)

The paper's theorem is proved in the mathematical literature; the goal here is a machine-checked statement and, eventually, a proof in the covariance-matrix representation. The published covariance layer already supplies symplectic forms, two-mode squeezed covariances, partial transpose, and an intrinsic ν−\nu_-ν−​; this mission adds the channel and code definitions required to state the no-go theorem. Those definitions can be reused for other single-mode Gaussian-channel questions. A complete proof still needs substantial results connecting codes, Gaussian operations, and entanglement behavior; a compiled sorry statement alone does not establish the theorem.

Difficulty

One might try to compare det⁡N\det NdetN before and after the code. That scalar does not track the code: encoding mixes signal and vacuum modes, each copy of the channel adds noise, decoding mixes the modes again, and discarding modes changes both MGCM_{GC}MGC​ and NGCN_{GC}NGC​. Neither determinant separately gives the desired inequality. The boundary det⁡M=−1\det M=-1detM=−1 also defeats a direct real-valued transcription of the printed quotient. The asymptotic entanglement formulas cross several determinant regimes, with different normal forms and a separate entanglement-breaking case. The central challenge is to retain the physical meaning of all these cases in one theorem over arbitrary finite codes.

Formalization scope

Lean uses real matrices indexed by interleaved mode and quadrature coordinates. The published QAlgorithms_Papers_Independent_Frontier30_P13 layer provides ModeQuadrature, phaseJ, squeezedCM, partial transpose, and the intrinsic smallest symplectic eigenvalue lambdaMin; QAlgorithms_Papers_Independent_Dependency50_P10 provides entrywise complexification. A channel is required to satisfy the Gaussian complete-positivity matrix inequality. Encoders and decoders satisfy SJST=JSJS^{\mathsf T}=JSJST=J. The code uses the same (M,N)(M,N)(M,N) on every one of its nnn modes, with n≥1n\ge1n≥1, and includes the vacuum covariance on every ancillary mode. Gaussian unitaries enter through their symplectic matrices; their displacement parts do not affect covariances.

The definition of DDD explicitly saturates at 111 when 1+det⁡M=01+\det M=01+detM=0, avoiding Lean's zero value for division by zero. The squeezed input uses cosh⁡(2r)\cosh(2r)cosh(2r) and sinh⁡(2r)\sinh(2r)sinh(2r). The eigenvalue ν−\nu_-ν−​ is the intrinsic lambdaMin, not an unguarded square-root expression. Logarithmic negativity uses the natural logarithm; its finite limit statement assumes det⁡N>0\det N>0detN>0, while the degradation statement still covers det⁡N=0\det N=0detN=0. The infinite-squeezing output is represented by limits of finite-rrr covariances and entanglement quantities.

The code's vacuum term, all nnn noise blocks, the symplectic equation, and the guarded degradation are essential to the target; dropping any of them would change the question. Lemma 1's teleportation equivalence and the external Gaussian no-distillation theorem are not formalized here. Their faithful treatment would require operational Gaussian states, measurements, and protocols beyond the covariance model. Contributions establishing those interfaces, proving the stated matrix milestones, or connecting the two layers are welcome.

Selected references

  • J. Niset, J. Fiurášek, and N. J. Cerf, A No-Go Theorem for Gaussian Quantum Error Correction, Physical Review Letters 102, 120501, 2009; arXiv:0811.3128v1 (2008). The preprint is the citation basis for page and equation numbers here.
  • G. Giedke and J. I. Cirac, Characterization of Gaussian operations and distillation of Gaussian states, Physical Review A 66, 032316, 2002; arXiv:quant-ph/0204085.
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Mathematical PhysicsQuantum InformationRepresentation Theory·Captain: mikedeng1

Qudit circuits with SU(d) symmetry: Locality imposes additional conservation laws: Tr(Ω[ρ]^l) is conserved by every unitary generated by 2-local SU(d)-invariant gatesResearch Paper

Motivation

Quantum circuits whose gates respect a global symmetry are a standard model for quantum simulation, for symmetry-protected quantum computing, and for the study of conserved quantities in quantum dynamics. For SU(d) symmetry on nnn qudits, the unitaries that commute with every U⊗nU^{\otimes n}U⊗n are, by Schur–Weyl duality, exactly the unitaries in the linear span of the qudit permutations. A natural question is whether every such unitary can be built from local symmetric gates, as happens without symmetry, where 2-qudit gates are universal.

Marvian, Liu and Hulse (arXiv:2105.12877) show that for d≥3d \ge 3d≥3 the answer is no, and that the obstruction appears as conservation laws. Unitaries generated by 2-local SU(d)-invariant gates conserve quantities that general SU(d)-invariant unitaries change. The paper gives two families of such laws. The first, Theorem 1 (the fsgnf_{\mathrm{sgn}}fsgn​ law, from a Z2\mathbb Z_2Z2​ symmetry of the swap Hamiltonians), is a separate result of the paper and is not part of this mission. The second, Theorem 2, is the target here. It comes from a correspondence between a subspace of the qudits and a system of free fermions.

Timeline: Marvian (Nature Physics 18, 283, 2022) showed that symmetry together with locality restricts the realizable unitaries in general, with examples for U(1) and SU(2) symmetry. For qubits with SU(2) symmetry, the constraints restrict only relative phases between sectors of inequivalent irreducible representations (p. 3 of the present paper). The present paper (arXiv:2105.12877, v2 January 2022) treats SU(d) with d≥3d\ge 3d≥3, where constraints beyond relative phases appear. The connection to Marin's 2007 description of the Lie algebra generated by transpositions (J. Algebra 310, 742) is discussed on p. 9.

Setting

Consider nnn qudits with Hilbert space (Cd)⊗n(\mathbb C^d)^{\otimes n}(Cd)⊗n and computational basis ∣x1⟩⋯∣xn⟩|x_1\rangle\cdots|x_n\rangle∣x1​⟩⋯∣xn​⟩, xi∈{0,…,d−1}x_i\in\{0,\dots,d-1\}xi​∈{0,…,d−1}.

  • A unitary VVV is SU(d)-invariant if [V,U⊗n]=0[V,U^{\otimes n}]=0[V,U⊗n]=0 for every U∈SU(d)U\in\mathrm{SU}(d)U∈SU(d) (Eq. (1)).
  • VVV is 2-local on qudits a,ba,ba,b if V=Wab⊗IrestV=W_{ab}\otimes\mathbb I_{\text{rest}}V=Wab​⊗Irest​.
  • V2\mathcal V_2V2​ is the group generated by finite products of 2-local SU(d)-invariant unitaries.
  • P(σ)\mathbf P(\sigma)P(σ) is the permutation operator of σ∈Sn\sigma\in S_nσ∈Sn​, and Pab\mathbf P_{ab}Pab​ is the swap of qudits a,ba,ba,b.

For L≤min⁡{n,d−1}L\le\min\{n,d-1\}L≤min{n,d−1}, the vector (⋀m=1L∣m⟩)⊗∣0⟩⊗(n−L)\big(\bigwedge_{m=1}^L|m\rangle\big)\otimes|0\rangle^{\otimes(n-L)}(⋀m=1L​∣m⟩)⊗∣0⟩⊗(n−L) antisymmetrizes the levels 1,…,L1,\dots,L1,…,L over the first LLL qudits with weight 1/L!1/\sqrt{L!}1/L!​ (Eq. (40)). The subspace Hcomp\mathcal H_{\mathrm{comp}}Hcomp​ is the span of all permutations of these vectors (Eq. (42)), and Πcomp\Pi_{\mathrm{comp}}Πcomp​ is the orthogonal projector onto it.

For an operator AAA on one qudit, AiA_iAi​ is AAA acting on qudit iii. Let Qij=(Ii−∣0⟩⟨0∣i)∣0⟩⟨0∣jQ_{ij}=(\mathbb I_i-|0\rangle\langle0|_i)|0\rangle\langle0|_jQij​=(Ii​−∣0⟩⟨0∣i​)∣0⟩⟨0∣j​. The map Ω\OmegaΩ sends an operator ρ\rhoρ on the qudits to the n×nn\times nn×n matrix

Ω[ρ]=∑i,j=1nΩij[ρ] ∣i⟩⟨j∣,Ωij[ρ]={Tr(ΠcompρΠcomp PijQij)i≠j,Tr(ΠcompρΠcomp (Ii−∣0⟩⟨0∣i))i=j\Omega[\rho]=\sum_{i,j=1}^n\Omega_{ij}[\rho]\,|i\rangle\langle j|,\qquad \Omega_{ij}[\rho]=\begin{cases}\mathrm{Tr}\big(\Pi_{\mathrm{comp}}\rho\Pi_{\mathrm{comp}}\,\mathbf P_{ij}Q_{ij}\big)& i\neq j,\\ \mathrm{Tr}\big(\Pi_{\mathrm{comp}}\rho\Pi_{\mathrm{comp}}\,(\mathbb I_i-|0\rangle\langle0|_i)\big)& i=j\end{cases}Ω[ρ]=i,j=1∑n​Ωij​[ρ]∣i⟩⟨j∣,Ωij​[ρ]={Tr(Πcomp​ρΠcomp​Pij​Qij​)Tr(Πcomp​ρΠcomp​(Ii​−∣0⟩⟨0∣i​))​i=j,i=j​

(Eqs. (49), (51)). On the fermionic side there are nnn sites, creation operators cj†c_j^\daggercj†​, the vacuum ∣vac⟩|\mathrm{vac}\rangle∣vac⟩, and the fermionic swap Pabf=If−(ca†−cb†)(ca−cb)\mathbf P^f_{ab}=\mathbb I^f-(c_a^\dagger-c_b^\dagger)(c_a-c_b)Pabf​=If−(ca†​−cb†​)(ca​−cb​) (Eq. (28)). Its single-particle counterpart is Eab=I−(∣a⟩−∣b⟩)(⟨a∣−⟨b∣)E_{ab}=\mathbb I-(|a\rangle-|b\rangle)(\langle a|-\langle b|)Eab​=I−(∣a⟩−∣b⟩)(⟨a∣−⟨b∣) on Cn\mathbb C^nCn (Eq. (33)). The map UfU^fUf sends P(σ)[(⋀m∣m⟩)⊗∣0⟩⊗(n−L)]\mathbf P(\sigma)\big[\big(\bigwedge_{m}|m\rangle\big)\otimes|0\rangle^{\otimes(n-L)}\big]P(σ)[(⋀m​∣m⟩)⊗∣0⟩⊗(n−L)] to ∏i=1Lcσ(i)†∣vac⟩\prod_{i=1}^L c^\dagger_{\sigma(i)}|\mathrm{vac}\rangle∏i=1L​cσ(i)†​∣vac⟩ (Eq. (41)).

Formalization targets

Goal: Theorem 2 (p. 11)

For every V∈V2V\in\mathcal V_2V∈V2​, every density operator ρ\rhoρ on nnn qudits and every positive integer lll,

Tr(Ω[VρV†]l)=Tr(Ω[ρ]l).\mathrm{Tr}\big(\Omega[V\rho V^\dagger]^l\big)=\mathrm{Tr}\big(\Omega[\rho]^l\big).Tr(Ω[VρV†]l)=Tr(Ω[ρ]l).

The statement holds for all nnn and ddd. Its content is the case l≥2l\ge 2l≥2: the case l=1l=1l=1 holds for every SU(d)-invariant unitary (Eq. (55)).

Milestones (in attack order)

  1. Eq. (5): up to a global phase, a 2-local SU(d)-invariant unitary on qudits a,ba,ba,b equals eiθPab=cos⁡θ I+isin⁡θ Pabe^{i\theta\mathbf P_{ab}}=\cos\theta\,\mathbb I+i\sin\theta\,\mathbf P_{ab}eiθPab​=cosθI+isinθPab​.
  2. Eqs. (27)–(29): Pabfcj†Pabf†=cσab(j)†\mathbf P^f_{ab}c_j^\dagger\mathbf P^{f\dagger}_{ab}=c^\dagger_{\sigma_{ab}(j)}Pabf​cj†​Pabf†​=cσab​(j)†​, Pabf∣vac⟩=∣vac⟩\mathbf P^f_{ab}|\mathrm{vac}\rangle=|\mathrm{vac}\ranglePabf​∣vac⟩=∣vac⟩, and Pabf\mathbf P^f_{ab}Pabf​ is Hermitian and unitary.
  3. Eq. (31): eiθPabfcj†e−iθPabf=e−iθ(cos⁡θ cj†+isin⁡θ cσab(j)†)e^{i\theta\mathbf P^f_{ab}}c_j^\dagger e^{-i\theta\mathbf P^f_{ab}}=e^{-i\theta}(\cos\theta\,c_j^\dagger+i\sin\theta\,c^\dagger_{\sigma_{ab}(j)})eiθPabf​cj†​e−iθPabf​=e−iθ(cosθcj†​+isinθcσab​(j)†​).
  4. Eq. (34): the same dynamics written through the single-particle unitary eiθ(Eab−I)e^{i\theta(E_{ab}-\mathbb I)}eiθ(Eab​−I).
  5. p. 9: P(σ)Πcomp=ΠcompP(σ)\mathbf P(\sigma)\Pi_{\mathrm{comp}}=\Pi_{\mathrm{comp}}\mathbf P(\sigma)P(σ)Πcomp​=Πcomp​P(σ).
  6. Eq. (41) and App. C5: UfU^fUf satisfies (41) and is an isometry on Hcomp\mathcal H_{\mathrm{comp}}Hcomp​.
  7. Eq. (44): UfeiθPabΠcomp=eiθPabfUfΠcompU^fe^{i\theta\mathbf P_{ab}}\Pi_{\mathrm{comp}}=e^{i\theta\mathbf P^f_{ab}}U^f\Pi_{\mathrm{comp}}UfeiθPab​Πcomp​=eiθPabf​UfΠcomp​.
  8. App. C7, (C42)–(C43): the qudit form (51) and the fermionic form (50) of Ω\OmegaΩ agree.
  9. Lemma 3: Ω[eiθPabρe−iθPab]=eiθEabΩ[ρ]e−iθEab\Omega[e^{i\theta\mathbf P_{ab}}\rho e^{-i\theta\mathbf P_{ab}}]=e^{i\theta E_{ab}}\Omega[\rho]e^{-i\theta E_{ab}}Ω[eiθPab​ρe−iθPab​]=eiθEab​Ω[ρ]e−iθEab​, and Ω\OmegaΩ is completely positive.

Significance

Theorem 2 gives an infinite family of polynomial invariants of the state, Tr(Ω[ρ]l)\mathrm{Tr}(\Omega[\rho]^l)Tr(Ω[ρ]l) for l=1,2,…l=1,2,\dotsl=1,2,…. Together these fix the spectrum of Ω[ρ]\Omega[\rho]Ω[ρ], so every Rényi entropy of the single-particle density operator Ω[ρ]/Tr Ω[ρ]\Omega[\rho]/\mathrm{Tr}\,\Omega[\rho]Ω[ρ]/TrΩ[ρ] is conserved. Already for l=2l=2l=2 the law is violated by SU(d)-invariant Hamiltonians with 3-local terms (p. 11 and §IV D). This shows that, for d≥3d\ge3d≥3, 2-local SU(d)-invariant gates are not universal among SU(d)-invariant unitaries, even up to relative phases, and that 3-local interactions can be detected from the dynamics of Ω\OmegaΩ. For d=2d=2d=2 the laws hold for all SU(2)-invariant unitaries.

The result is proved in the paper. As far as a search of the platform shows, it has not been formalized. A formalization adds machine-checked versions of the qudit–fermion correspondence of §IV B, including the isometry UfU^fUf and the intertwining relation (44), and of the free-fermion form of the swap dynamics. These are statements about finite-dimensional matrices, so the whole development stays inside Mathlib's linear algebra.

Difficulty

The obvious route is to show that each generator acts on Ω[ρ]\Omega[\rho]Ω[ρ] by conjugation with an n×nn\times nn×n unitary, and then to induct over products. The difficulty is the generator step. The definition (51) of Ω\OmegaΩ involves the projector Πcomp\Pi_{\mathrm{comp}}Πcomp​ onto a span of antisymmetrized vectors, and nothing in (51) shows directly why conjugating ρ\rhoρ by eiθPabe^{i\theta\mathbf P_{ab}}eiθPab​ should conjugate Ω[ρ]\Omega[\rho]Ω[ρ] by eiθEabe^{i\theta E_{ab}}eiθEab​. The covariance becomes visible only after Hcomp\mathcal H_{\mathrm{comp}}Hcomp​ is identified with fermionic Fock sectors, where the swap becomes a quadratic, particle-number-preserving Hamiltonian. That identification needs care with the signs of the fermionic creation operators and with the ordering of products. A second obstacle is the characterization of the generators (Eq. (5)). It rests on the commutant of {U⊗U:U∈SU(d)}\{U\otimes U : U\in\mathrm{SU}(d)\}{U⊗U:U∈SU(d)} being spanned by I\mathbb II and the swap, a Schur–Weyl statement for two qudits that Mathlib does not provide.

Formalization scope

Operators on the qudits are matrices indexed by Fin n → Fin d, with sites and levels 0-based and [NeZero d] assumed so that ∣0⟩|0\rangle∣0⟩ exists. Fock-space operators are matrices indexed by Finset (Fin n), the set of occupied sites. The creation operator uses the Jordan–Wigner sign (−1)∣{k∈T:k<j}∣(-1)^{|\{k\in T:k<j\}|}(−1)∣{k∈T:k<j}∣, the encoding of the public definition QAlgorithms_Papers_Independent_Next46_P23, copied rather than imported.

The following conventions are fixed:

  • P(σ)∣y⟩=∣y∘σ−1⟩\mathbf P(\sigma)|y\rangle=|y\circ\sigma^{-1}\rangleP(σ)∣y⟩=∣y∘σ−1⟩, the representation convention the paper uses in Eq. (30) and App. C5. Eq. (9) as printed describes P(σ−1)\mathbf P(\sigma^{-1})P(σ−1), and under it the map of Eq. (41) is not well defined. All other objects coincide under the two conventions.
  • Exponentials of involutions are written in the closed form cos⁡θ I+isin⁡θX\cos\theta\,\mathbb I+i\sin\theta XcosθI+isinθX of Eq. (5), and θ\thetaθ ranges over [0,2π)[0,2\pi)[0,2π) as in the paper.
  • Πcomp\Pi_{\mathrm{comp}}Πcomp​ is the matrix of Mathlib's orthogonal projection onto Hcomp⊆\mathcal H_{\mathrm{comp}}\subseteqHcomp​⊆ EuclideanSpace ℂ (Fin n → Fin d).
  • UfU^fUf is an explicit linear map defined on the whole space. It sends the basis state with ∣m⟩|m\rangle∣m⟩ on site p(m)p(m)p(m), m=1,…,Lm=1,\dots,Lm=1,…,L, to 1L!cp(1)†⋯cp(L)†∣vac⟩\frac1{\sqrt{L!}}c^\dagger_{p(1)}\cdots c^\dagger_{p(L)}|\mathrm{vac}\rangleL!​1​cp(1)†​⋯cp(L)†​∣vac⟩, and all other basis states to 000.
  • Complete positivity is the published QAlgorithms.Entanglement.IsCompletelyPositive.

The following trivializing formalizations are ruled out:

  • Ω\OmegaΩ is not identically zero: the normalization 1/L!1/\sqrt{L!}1/L!​ and the range L≤min⁡{n,d−1}L\le\min\{n,d-1\}L≤min{n,d−1} are as printed, and Hcomp≠0\mathcal H_{\mathrm{comp}}\neq 0Hcomp​=0 is checked.
  • V2\mathcal V_2V2​ is the group generated by all 2-local SU(d)-invariant unitaries, defined literally on p. 3. It is neither the generating set of Eq. (6) nor the group of all SU(d)-invariant unitaries, for which the statement is false when d≥3d\ge3d≥3.
  • The goal uses the qudit form (51) of Ω\OmegaΩ, not the fermionic form (50).

A complete development needs:

  • the two-qudit commutant of U⊗UU\otimes UU⊗U;
  • the CAR algebra on Finset Fock space;
  • the orthonormality of the antisymmetrized vectors;
  • the trace identity Tr((WXW†)l)=Tr(Xl)\mathrm{Tr}((WXW^\dagger)^l)=\mathrm{Tr}(X^l)Tr((WXW†)l)=Tr(Xl).

The Fock-space and permutation-operator lemmas can be reused for other qudit–fermion and Schur–Weyl statements. Contributions welcome: proofs of any milestone, and lemma-level infrastructure on the Fock space.

Selected references

  • I. Marvian, H. Liu, A. Hulse, Qudit circuits with SU(d) symmetry: Locality imposes additional conservation laws, arXiv:2105.12877v2, 2022. https://arxiv.org/abs/2105.12877
  • I. Marvian, Restrictions on realizable unitary operations imposed by symmetry and locality, Nature Physics 18, 283–289, 2022. https://doi.org/10.1038/s41567-021-01464-0
  • I. Marin, L'algèbre de Lie des transpositions, Journal of Algebra 310, 742–774, 2007. https://doi.org/10.1016/j.jalgebra.2006.08.018
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AlgebraCombinatoricsRepresentation Theory·Captain: mikedeng1

Supersymmetric Polynomials and the Center of the Walled Brauer Algebra: When B_{r,s}(δ) Is Semisimple, Supersymmetric Polynomials in the Jucys–Murphy Elements Generate Its CenterResearch Paper

Motivation

The walled Brauer algebra Br,s(δ)B_{r,s}(\delta)Br,s​(δ) is the centralizer algebra of mixed Schur–Weyl duality: for δ=n\delta=nδ=n it acts on the mixed tensor space V⊗r⊗(V∗)⊗sV^{\otimes r}\otimes (V^*)^{\otimes s}V⊗r⊗(V∗)⊗s of V=CnV=\mathbb C^nV=Cn and commutes with gln\mathfrak{gl}_ngln​, and for δ=m−n\delta=m-nδ=m−n it plays the same role for the general linear supergroup GL(m∣n)GL(m|n)GL(m∣n). Its representation theory has been studied through cellular structures and blocks (Cox–De Visscher–Doty–Martin 2008), Khovanov arc algebras (Brundan–Stroppel 2012) and cyclotomic quotients (Sartori–Stroppel 2015).

For the group algebra CSn\mathbb C\mathfrak S_nCSn​ of the symmetric group there is a classical description of the center: it consists of the symmetric polynomials in the Jucys–Murphy elements Lk=∑j<k(j,k)L_k=\sum_{j<k}(j,k)Lk​=∑j<k​(j,k) (Jucys 1974, Murphy 1983). Jung and Kim (arXiv:1508.06469v2) prove the walled analogue: when Br,s(δ)B_{r,s}(\delta)Br,s​(δ) is semisimple, its center is generated by the supersymmetric polynomials in its Jucys–Murphy elements. This mission formalizes that theorem and the chain of results leading to it.

Timeline. Jucys (1974) and Murphy (1981, 1983) describe the center of CSn\mathbb C\mathfrak S_nCSn​ through Jucys–Murphy elements. Stembridge (1985) characterizes supersymmetric polynomials and shows that the power sums generate them. Cox, De Visscher, Doty and Martin (2008) give the cellular structure of Br,s(δ)B_{r,s}(\delta)Br,s​(δ), its blocks in characteristic zero and a semisimplicity criterion. Brundan and Stroppel (2012) prove that the central element zr,sz_{r,s}zr,s​ (essentially L1+⋯+Lr+sL_1+\dots+L_{r+s}L1​+⋯+Lr+s​) acts on cell modules by a content sum. Jung and Kim (2015, revised 2017) prove the generation theorem for all supersymmetric polynomials.

Setting

Fix integers r,s≥0r,s\ge0r,s≥0 and δ∈C\delta\in\mathbb Cδ∈C. An (r,s)(r,s)(r,s)-walled Brauer diagram is a pairing of 2(r+s)2(r+s)2(r+s) vertices, r+sr+sr+s on top and r+sr+sr+s on the bottom, with a wall between positions rrr and r+1r+1r+1, such that vertical edges do not cross the wall and horizontal edges do. Br,s(δ)B_{r,s}(\delta)Br,s​(δ) is the complex vector space with these diagrams as basis; two diagrams are multiplied by stacking them and replacing each closed loop by a factor δ\deltaδ.

For vertices a≠ba\ne ba=b on the same side of the wall, (a,b)(a,b)(a,b) is the diagram of the transposition of aaa and bbb. For 1≤j≤r<k≤r+s1\le j\le r<k\le r+s1≤j≤r<k≤r+s, ej,ke_{j,k}ej,k​ is the diagram with a top arc and a bottom arc joining jjj and kkk and all other vertices joined straight down. The Jucys–Murphy elements (Definition 2.1) are

Lk=∑j=1k−1(j,k)(1≤k≤r),Lk=−∑j=1rej,k+∑j=r+1k−1(j,k)+δ(r<k≤r+s).L_k=\sum_{j=1}^{k-1}(j,k)\quad(1\le k\le r),\qquad L_k=-\sum_{j=1}^{r}e_{j,k}+\sum_{j=r+1}^{k-1}(j,k)+\delta\quad(r<k\le r+s).Lk​=j=1∑k−1​(j,k)(1≤k≤r),Lk​=−j=1∑r​ej,k​+j=r+1∑k−1​(j,k)+δ(r<k≤r+s).

A polynomial p∈C[x1,…,xr,y1,…,ys]p\in\mathbb C[x_1,\dots,x_r,y_1,\dots,y_s]p∈C[x1​,…,xr​,y1​,…,ys​] is supersymmetric (Definition 2.8) if it is symmetric in the xix_ixi​ and in the yjy_jyj​ separately, and the substitution xr=−y1=tx_r=-y_1=txr​=−y1​=t produces a polynomial independent of ttt. Examples are the power sums pk=∑ixik+(−1)k+1∑jyjkp_k=\sum_i x_i^k+(-1)^{k+1}\sum_j y_j^kpk​=∑i​xik​+(−1)k+1∑j​yjk​. Write Sr,s[x;y]S_{r,s}[x;y]Sr,s​[x;y] for the supersymmetric polynomials and p(L1,…,Lr+s)p(L_1,\dots,L_{r+s})p(L1​,…,Lr+s​) for the substitution xi↦Lix_i\mapsto L_ixi​↦Li​, yj↦Lr+jy_j\mapsto L_{r+j}yj​↦Lr+j​.

The cell modules Cr,s(λ)C_{r,s}(\lambda)Cr,s​(λ) are indexed by bipartitions λ=(λL,λR)\lambda=(\lambda^L,\lambda^R)λ=(λL,λR) with ∣λL∣=r−t|\lambda^L|=r-t∣λL∣=r−t, ∣λR∣=s−t|\lambda^R|=s-t∣λR∣=s−t, 0≤t≤min⁡(r,s)0\le t\le\min(r,s)0≤t≤min(r,s); this set is Λr,s\Lambda_{r,s}Λr,s​. The set Λ˙r,s\dot\Lambda_{r,s}Λ˙r,s​ equals Λr,s\Lambda_{r,s}Λr,s​ except when δ=0\delta=0δ=0 and r=s≠0r=s\ne0r=s=0, where (∅,∅)(\varnothing,\varnothing)(∅,∅) is removed; it indexes the simple modules. The content vector c(λ,⋅)∈Cr+sc(\lambda,\cdot)\in\mathbb C^{r+s}c(λ,⋅)∈Cr+s lists the contents of λL\lambda^LλL, then 2t2t2t zeros, then the contents of λR\lambda^RλR shifted by δ\deltaδ.

Formalization targets

Goal: Theorem 3.5

Br,s(δ) semisimple ⟹ C[p(L1,…,Lr+s):p∈Sr,s[x;y]]=Z(Br,s(δ)).B_{r,s}(\delta)\ \text{semisimple}\ \Longrightarrow\ \mathbb C\bigl[p(L_1,\dots,L_{r+s}) : p\in S_{r,s}[x;y]\bigr]=Z\bigl(B_{r,s}(\delta)\bigr).Br,s​(δ) semisimple ⟹ C[p(L1​,…,Lr+s​):p∈Sr,s​[x;y]]=Z(Br,s​(δ)).

Both inclusions are asserted. The goal fixes no constants; the hypothesis holds for all but finitely many δ\deltaδ (Proposition 1.1).

Milestones

  1. Relations among generators: Lemma 2.3 and Proposition 2.4.
  2. The LkL_kLk​ commute (Proposition 2.6); the power sums pk(L1,…,Lr+s)p_k(L_1,\dots,L_{r+s})pk​(L1​,…,Lr+s​) are central (Proposition 2.7).
  3. Stembridge's theorem, Sr,s[x;y]=C[p0,p1,… ]S_{r,s}[x;y]=\mathbb C[p_0,p_1,\dots]Sr,s​[x;y]=C[p0​,p1​,…], and its consequence, Corollary 2.9: every p(L1,…,Lr+s)p(L_1,\dots,L_{r+s})p(L1​,…,Lr+s​) with ppp supersymmetric is central, for every δ\deltaδ.
  4. Separation: Lemma 2.11 (generating functions), the semisimplicity criterion Proposition 1.1, and Lemma 2.12 (supersymmetric polynomials separate the content vectors).
  5. Central characters: Lemma 3.2, Proposition 3.1 and Corollary 3.3, by which f(L1,…,Lr+s)f(L_1,\dots,L_{r+s})f(L1​,…,Lr+s​) acts on Cr,s(λ)C_{r,s}(\lambda)Cr,s​(λ) as f(c(λ,1),…,c(λ,r+s))f(c(\lambda,1),\dots,c(\lambda,r+s))f(c(λ,1),…,c(λ,r+s)).
  6. Counting: Lemma 3.4 (a nonsingular evaluation matrix) and dim⁡Z(Br,s(δ))=∣Λ˙r,s∣\dim Z(B_{r,s}(\delta))=|\dot\Lambda_{r,s}|dimZ(Br,s​(δ))=∣Λ˙r,s​∣ in the semisimple case.

Significance

The theorem gives an explicit generating set for the center of a semisimple walled Brauer algebra, parallel to the symmetric-group case. Its consequences in the paper include a description of the Gelfand–Zetlin subalgebra and formulas for primitive idempotents (§4), an alternative proof of the block classification of Cox et al. (§5), and, via the same method, the center of the quantized walled Brauer algebra (§6). Corollary 2.9 alone, valid for every δ\deltaδ, provides a supply of central elements whose action on each cell module is computed by Corollary 3.3.

The theorem is proved in the paper; no part of it is formalized. A formalization would supply machine-checked Jucys–Murphy relations for a diagram algebra built on a published, generic encoding of walled Brauer diagrams, a Lean development of supersymmetric polynomials (including Stembridge's theorem, absent from Mathlib), and a reusable dimension count for centers of semisimple algebras in terms of simple modules.

Difficulty

The inclusion of the supersymmetric polynomials in the center (Corollary 2.9) reduces to diagram relations plus Stembridge's theorem; the latter is a nontrivial statement about polynomial rings, with no counterpart in Mathlib. The reverse inclusion is the harder half. A central element is not visibly a polynomial in the LkL_kLk​: the argument must show that enough linearly independent central elements of the form p(L1,…,Lr+s)p(L_1,\dots,L_{r+s})p(L1​,…,Lr+s​) exist, which requires computing their scalars on every cell module (an explicit cellular computation involving the arc elements τt\tau_tτt​), separating all content vectors (where semisimplicity enters through the criterion of Cox et al.), and comparing with dim⁡Z\dim ZdimZ, which needs Wedderburn–Artin together with the classification of simple modules. Separation genuinely fails outside the semisimple range, so no argument independent of δ\deltaδ can work.

Formalization scope

The algebra, diagrams, cell modules Cr,s(λ)C_{r,s}(\lambda)Cr,s​(λ), the index sets Λr,s\Lambda_{r,s}Λr,s​ (CellIndex) and Λ˙r,s\dot\Lambda_{r,s}Λ˙r,s​ (Label) and contents are the published definitions WalledBrauer_Blocks_{Diagram, Algebra, ModuleTheory, Partitions, CellModules}, used as references. New definitions are in WalledBrauer.Center.Setting. Conventions:

  • The base field is C\mathbb CC; r,sr,sr,s are arbitrary natural numbers, including 000; δ∈C\delta\in\mathbb Cδ∈C is arbitrary.
  • Vertices are 0-based (Fin (r + s)); the paper's LkL_kLk​ is jm δ ⟨k-1, _⟩.
  • The published algebra multiplies diagrams with the left factor on top, the opposite of the paper's convention. One-sided relations are transcribed literally with the platform's product; each is the image of the paper's relation under the up–down flip, an anti-automorphism fixing every (a,b)(a,b)(a,b), ej,ke_{j,k}ej,k​, LkL_kLk​ and τt\tau_tτt​. The center, generated subalgebras, semisimplicity and central characters do not depend on the convention.
  • Polynomials are MvPolynomial (Fin r ⊕ Fin s) ℂ. The evaluation p(L1,…,Lr+s)p(L_1,\dots,L_{r+s})p(L1​,…,Lr+s​) is defined monomial by monomial in increasing vertex order, without assuming that the LkL_kLk​ commute; it is never routed through a commutative subalgebra.
  • The cancellation property is vacuous when r=0r=0r=0 or s=0s=0s=0. Semisimplicity is IsSemisimpleRing, the center is Subalgebra.center ℂ, "generate" is Algebra.adjoin ℂ. In Proposition 1.1, r+s−2r+s-2r+s−2 is real.
  • Lemma 2.11's equality of rational functions is stated cross-multiplied in C[z]\mathbb C[z]C[z].

Supersymmetry is defined intrinsically on polynomials, never through the algebra, so neither inclusion of the goal holds by definition; stating only ⊆\subseteq⊆ or only ⊇\supseteq⊇ as the goal is excluded.

Proofs of any milestone are welcome, as are reusable developments of supersymmetric polynomials (Stembridge's theorem, elementary supersymmetric polynomials) and of the center of a split semisimple algebra.

Selected references

  • J. H. Jung and M. Kim, Supersymmetric polynomials and the center of the walled Brauer algebra, arXiv:1508.06469v2, 2017. https://arxiv.org/abs/1508.06469
  • A. Cox, M. De Visscher, S. Doty and P. Martin, On the blocks of the walled Brauer algebra, J. Algebra 320 (2008), 169–212. https://arxiv.org/abs/0709.0851
  • J. Brundan and C. Stroppel, Gradings on walled Brauer algebras and Khovanov's arc algebra, Adv. Math. 231 (2012), 709–773. https://arxiv.org/abs/1107.0999
  • A. Sartori and C. Stroppel, Walled Brauer algebras as idempotent truncations of level 2 cyclotomic quotients, J. Algebra 440 (2015), 602–638. https://arxiv.org/abs/1411.2771
  • J. R. Stembridge, A characterization of supersymmetric polynomials, J. Algebra 95 (1985), 439–444. https://mathscinet.ams.org/mathscinet-getitem?mr=801279
  • Y. Li, Jucys–Murphy elements and centres of cellular algebras, Bull. Aust. Math. Soc. 85 (2012), 261–270. https://mathscinet.ams.org/mathscinet-getitem?mr=2891540
  • G. E. Murphy, The idempotents of the symmetric group and Nakayama's conjecture, J. Algebra 81 (1983), 258–265. https://mathscinet.ams.org/mathscinet-getitem?mr=696137
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Functional AnalysisQuantum InformationStatistics·Captain: mikedeng1

Randomization Theorems for Quantum Channels: Equivalent Characterizations of ε-Post-Processing Deficiency of Channels via the Diamond Norm and Its DualResearch Paper

Comparison of experiments and its quantum versions

Statistical decision theory compares two experiments by asking which one is more useful: one experiment is deficient with respect to another if, in every decision problem, it achieves nearly the same payoff. The randomization criterion turns this operational comparison into a structural one: an experiment is ϵ\epsilonϵ-deficient exactly when a Markov kernel (a randomization) maps the better experiment to within ϵ\epsilonϵ of the worse one in L1L^1L1-distance. Its exact case, the Blackwell–Sherman–Stein theorem, is a standard tool in statistics and economics, and the approximate version is the basis of Le Cam's theory of comparison of experiments (Strasser 1985; Torgersen 1991).

Quantum information asks the same question for quantum devices: when can one channel be simulated from another by further processing, and how is that detected by tasks? A short timeline of the results this mission builds on:

  • 1951. Blackwell, Sherman and Stein: the exact classical criterion for finite experiments.
  • 2005. Shmaya proves a quantum version for quantum information structures (bipartite states), with completely positive maps as randomizations.
  • 2009. Chefles reformulates Shmaya's result for comparison of quantum channels.
  • 2010. Matsumoto introduces quantum decision problems (payoff operators, channels as decision rules) and proves a quantum randomization criterion by a minimax argument.
  • 2012. Buscemi obtains a quantum Blackwell–Sherman–Stein theorem for quantum statistical models; Jenčová treats quantum binary experiments.
  • 2013–2014. Jenčová develops base-section norms, a family containing the diamond norm and its dual, and proves randomization theorems for channels in which positivity is given by an arbitrary admissible family of cones (arXiv:1404.3900v1).

This mission formalizes the central result of the last paper: the randomization theorem for post-processings of channels (Theorem 3, p. 15).

Setting

All spaces are finite-dimensional. A Hilbert space is Ch\mathbb C^hCh with its standard basis and B(H)B(H)B(H) is the algebra of h×hh\times hh×h complex matrices. A C-algebra* A⊆B(H)\mathcal A\subseteq B(H)A⊆B(H) is a block-diagonal algebra ⨁kB(Hk)\bigoplus_k B(H_k)⨁k​B(Hk​) with H=⨁kHkH=\bigoplus_k H_kH=⨁k​Hk​; full matrix algebras and the diagonal (classical) algebras Dn\mathbb D_nDn​ are the extreme cases. S(A)\mathfrak S(\mathcal A)S(A) is the set of density matrices in A\mathcal AA.

L(A,B)\mathcal L(\mathcal A,\mathcal B)L(A,B) is the real space of Hermitian linear maps from A\mathcal AA to B\mathcal BB, paired with L(B,A)\mathcal L(\mathcal B,\mathcal A)L(B,A) by ⟨ϕ,ψ⟩=s(ϕ∘ψ)\langle\phi,\psi\rangle=s(\phi\circ\psi)⟨ϕ,ψ⟩=s(ϕ∘ψ), where s(χ)=∑i,j⟨i,χ(∣i⟩⟨j∣)j⟩s(\chi)=\sum_{i,j}\langle i,\chi(|i\rangle\langle j|)j\rangles(χ)=∑i,j​⟨i,χ(∣i⟩⟨j∣)j⟩ is the trace of a map on matrices.

An admissible family of positive cones P\mathcal PP (Definition 1) assigns a closed convex cone P(H,K)\mathcal P(H,K)P(H,K) of Hermitian maps to every pair of spaces, with EB⊆P⊆PosEB\subseteq\mathcal P\subseteq PosEB⊆P⊆Pos, P∘P⊆P\mathcal P\circ\mathcal P\subseteq\mathcal PP∘P⊆P and CP∘P∘CP⊆PCP\circ\mathcal P\circ CP\subseteq\mathcal PCP∘P∘CP⊆P. Here PosPosPos, CPCPCP and EBEBEB are the positive, completely positive and entanglement-breaking maps. Examples are PosPosPos, CPCPCP, EBEBEB and the kkk-positive maps. Restricted to algebras, P(A,B)\mathcal P(\mathcal A,\mathcal B)P(A,B) is a cone in L(A,B)\mathcal L(\mathcal A,\mathcal B)L(A,B), and P∗(A,B)\mathcal P^*(\mathcal A,\mathcal B)P∗(A,B) is the dual of P(B,A)\mathcal P(\mathcal B,\mathcal A)P(B,A) under the pairing. A P\mathcal PP-channel is a trace-preserving element of P\mathcal PP; they form C(A,B)\mathcal C(\mathcal A,\mathcal B)C(A,B). ΦI,σ\Phi_{I,\sigma}ΦI,σ​ is the replacement map a↦(Tr a)σa\mapsto(\mathrm{Tr}\,a)\sigmaa↦(Tra)σ.

The two norms on L(A,B)\mathcal L(\mathcal A,\mathcal B)L(A,B) are

∥ϕ∥⋄=inf⁡α∈C(A,B)inf⁡{λ>0:−λα≤ϕ≤λα},∥ϕ∥⋄=inf⁡σ∈S(B)inf⁡{λ>0:−λΦI,σ≤∗ϕ≤∗λΦI,σ},\|\phi\|_\diamond=\inf_{\alpha\in\mathcal C(\mathcal A,\mathcal B)}\inf\{\lambda>0:-\lambda\alpha\le\phi\le\lambda\alpha\},\qquad \|\phi\|^\diamond=\inf_{\sigma\in\mathfrak S(\mathcal B)}\inf\{\lambda>0:-\lambda\Phi_{I,\sigma}\le^*\phi\le^*\lambda\Phi_{I,\sigma}\},∥ϕ∥⋄​=α∈C(A,B)inf​inf{λ>0:−λα≤ϕ≤λα},∥ϕ∥⋄=σ∈S(B)inf​inf{λ>0:−λΦI,σ​≤∗ϕ≤∗λΦI,σ​},

where ≤\le≤ and ≤∗\le^*≤∗ are the orders of P\mathcal PP and P∗\mathcal P^*P∗. For P=CP\mathcal P=CPP=CP, ∥⋅∥⋄\|\cdot\|_\diamond∥⋅∥⋄​ is the usual diamond norm.

Given channels Φ∈C(A,B)\Phi\in\mathcal C(\mathcal A,\mathcal B)Φ∈C(A,B) and Ψ∈C(A,B′)\Psi\in\mathcal C(\mathcal A,\mathcal B')Ψ∈C(A,B′), a decision algebra D\mathcal DD, decision rules α∈C(B,D)\alpha\in\mathcal C(\mathcal B,\mathcal D)α∈C(B,D) and payoff maps Γ∈P∗(D,A)\Gamma\in\mathcal P^*(\mathcal D,\mathcal A)Γ∈P∗(D,A), Ψ\PsiΨ is (ϵ,D)(\epsilon,\mathcal D)(ϵ,D)-post-processing deficient with respect to Φ\PhiΦ, written Ψ⪰ϵ,DΦ\Psi\succeq_{\epsilon,\mathcal D}\PhiΨ⪰ϵ,D​Φ, if every payoff ⟨α∘Φ,Γ⟩\langle\alpha\circ\Phi,\Gamma\rangle⟨α∘Φ,Γ⟩ achievable from Φ\PhiΦ is achievable from Ψ\PsiΨ up to ϵ∥Γ∥⋄\epsilon\|\Gamma\|^\diamondϵ∥Γ∥⋄ (Definition 3).

Formalization targets

Goal: Theorem 3 (Post-processings)

For ϵ≥0\epsilon\ge0ϵ≥0 the following are equivalent:

(i) Ψ⪰ϵ,DΦ;(ii) ∥Φ∘Γ∥⋄≤∥Ψ∘Γ∥⋄+ϵ∥Γ∥⋄  ∀ Γ∈P∗(D,A);\text{(i) } \Psi\succeq_{\epsilon,\mathcal D}\Phi;\qquad \text{(ii) } \|\Phi\circ\Gamma\|^\diamond\le\|\Psi\circ\Gamma\|^\diamond+\epsilon\|\Gamma\|^\diamond\ \ \forall\,\Gamma\in\mathcal P^*(\mathcal D,\mathcal A);(i) Ψ⪰ϵ,D​Φ;(ii) ∥Φ∘Γ∥⋄≤∥Ψ∘Γ∥⋄+ϵ∥Γ∥⋄  ∀Γ∈P∗(D,A); (iii) ∀ Γ∈L(D,A), ∀ α ∃ α′: ⟨α∘Φ,Γ⟩≤⟨α′∘Ψ,Γ⟩+2ϵ∥Γ∥⋄;(iv) ∀ α ∃ α′: ∥α∘Φ−α′∘Ψ∥⋄≤2ϵ.\text{(iii) } \forall\,\Gamma\in\mathcal L(\mathcal D,\mathcal A),\ \forall\,\alpha\ \exists\,\alpha':\ \langle\alpha\circ\Phi,\Gamma\rangle\le\langle\alpha'\circ\Psi,\Gamma\rangle+2\epsilon\|\Gamma\|^\diamond;\qquad \text{(iv) } \forall\,\alpha\ \exists\,\alpha':\ \|\alpha\circ\Phi-\alpha'\circ\Psi\|_\diamond\le2\epsilon .(iii) ∀Γ∈L(D,A), ∀α ∃α′: ⟨α∘Φ,Γ⟩≤⟨α′∘Ψ,Γ⟩+2ϵ∥Γ∥⋄;(iv) ∀α ∃α′: ∥α∘Φ−α′∘Ψ∥⋄​≤2ϵ.

Moreover, if id∈P\mathrm{id}\in\mathcal Pid∈P, then Ψ⪰ϵΦ\Psi\succeq_\epsilon\PhiΨ⪰ϵ​Φ (all decision algebras) iff Ψ⪰ϵ,BΦ\Psi\succeq_{\epsilon,\mathcal B}\PhiΨ⪰ϵ,B​Φ.

Milestones

Lemma 1 (trace property of sss); identity (1); ⟨ϕ,ΦI,σ⟩=Tr ϕ(σ)\langle\phi,\Phi_{I,\sigma}\rangle=\mathrm{Tr}\,\phi(\sigma)⟨ϕ,ΦI,σ​⟩=Trϕ(σ) (proof of Lemma 2); P∗∘P, P∘P∗⊆P∗∩CP\mathcal P^*\circ\mathcal P,\ \mathcal P\circ\mathcal P^*\subseteq\mathcal P^*\cap CPP∗∘P, P∘P∗⊆P∗∩CP (p. 8); Corollary 8 (ii) for ∥⋅∥⋄\|\cdot\|^\diamond∥⋅∥⋄; the dual formula (4) for ∥⋅∥⋄\|\cdot\|_\diamond∥⋅∥⋄​; Corollary 8 (iii) for channels; and Lemma 4, monotonicity of both norms under channels.

Significance

Theorem 3 says that a channel is approximately worse than another in every post-processing decision task exactly when every post-processing of the better channel can be approximated, in the (P\mathcal PP-)diamond norm, by a post-processing of the worse one. It contains the classical randomization criterion (classical algebras, P=Pos\mathcal P=PosP=Pos) and Matsumoto's quantum criterion (cq-channels, P=CP\mathcal P=CPP=CP) as special cases. Through the Moreover clause, it reduces deficiency over all decision algebras to a single one, the output algebra. Because P\mathcal PP is arbitrary, the same statement covers positive, kkk-positive and completely positive simulation.

The paper gives complete proofs, and the result is not open. No machine-checked version of it, of the base-section norms, or of admissible cone families exists on the platform or in Mathlib. A complete development gives a reusable, Mathlib-only layer for Hermitian maps between block algebras, their trace pairing, cone families, and the diamond norm defined relative to a cone; and a formal proof of a quantum decision-theoretic equivalence that relies on a minimax theorem.

Difficulty

The equivalence (i)⇔(ii) and the implication (iv)⇒(i) are short once the norm duality is available: Corollary 8 (ii) and (iii), which identify norms of positive elements and differences of channels with suprema of payoffs. Formalizing those duality statements is the first obstacle. They rest on the appendix theory of base sections, including the fact (Theorem 8) that ∥⋅∥⋄\|\cdot\|_\diamond∥⋅∥⋄​ and ∥⋅∥⋄\|\cdot\|^\diamond∥⋅∥⋄ are dual norms, which uses an extension theorem for positive functionals and closedness of the cones.

The step (iii)⇒(iv) is where the argument cannot be done pointwise. Condition (iii) gives, for each payoff Γ\GammaΓ separately, a decision rule α′\alpha'α′ depending on Γ\GammaΓ; condition (iv) needs one α′\alpha'α′ that works for all Γ\GammaΓ at once. Exchanging the two quantifiers requires a minimax theorem on the compact convex sets O⋄\mathcal O^\diamondO⋄ (the unit ball of ∥⋅∥⋄\|\cdot\|^\diamond∥⋅∥⋄) and C(B′,D)\mathcal C(\mathcal B',\mathcal D)C(B′,D), followed by formula (4). Compactness of C(B′,D)\mathcal C(\mathcal B',\mathcal D)C(B′,D) needs closedness of P\mathcal PP.

Formalization scope

All definitions are in one module, ChannelRandomization.PostProc.Setting, and depend only on Mathlib.

  • Dimensions are natural numbers and spaces are Cn\mathbb C^nCn. Maps are C\mathbb CC-linear maps of matrices, and Hermiticity ϕ(x∗)=ϕ(x)∗\phi(x^*)=\phi(x)^*ϕ(x∗)=ϕ(x)∗ is a separate predicate. sss is the page's sum (its real part, equal to it for Hermitian maps).
  • A C*-algebra is a block label c:{1,…,n}→Nc:\{1,\dots,n\}\to\mathbb Nc:{1,…,n}→N, standing for the matrices with xij=0x_{ij}=0xij​=0 whenever c(i)≠c(j)c(i)\ne c(j)c(i)=c(j). This is the paper's representation ⨁kB(Hk)⊆B(⨁kHk)\bigoplus_k B(H_k)\subseteq B(\bigoplus_k H_k)⨁k​B(Hk​)⊆B(⨁k​Hk​). L(A,B)\mathcal L(\mathcal A,\mathcal B)L(A,B) consists of the Hermitian maps with range in B\mathcal BB that vanish on the Hilbert–Schmidt complement of A\mathcal AA.
  • An admissible family is a structure with one cone for every pair of dimensions. "Proper" is encoded as closedness (in the pointwise topology). Pointedness and solidity follow from EB⊆P⊆PosEB\subseteq\mathcal P\subseteq PosEB⊆P⊆Pos.
  • ∥⋅∥⋄\|\cdot\|_\diamond∥⋅∥⋄​ and ∥⋅∥⋄\|\cdot\|^\diamond∥⋅∥⋄ are defined by the infima (5) and (7). The supremum forms (4) and Corollary 8 are theorems. All infima and suprema are real sInf/sSup. Their sets are nonempty and bounded when the dimensions are positive, and in dimension 0 both sides of every statement are 0.
  • Theorem 3 is stated for every admissible family, every pair of channels with a common input, every ϵ≥0\epsilon\ge0ϵ≥0 and every decision algebra, as a four-way equivalence (List.TFAE) together with the Moreover clause. "id∈P\mathrm{id}\in\mathcal Pid∈P" means that the identity of B(Cn)B(\mathbb C^n)B(Cn) lies in P\mathcal PP for every nnn.

The structure of admissible families is not vacuous: the positive maps form an instance, constructed sorry-free in a separate verification file. A formalization that defines the norms by the supremum formulas, fixes P=CP\mathcal P=CPP=CP, drops the closedness of the cones, or restricts the decision algebra D\mathcal DD to one kind proves a different statement and does not count.

Out of scope are the pre-processing theorem (Theorem 5, whose proof the paper omits as "practically the same as the proof of Theorem 3"), the cq- and qc-channel specializations of §3.2.1–3.2.3, the pointwise deficiency results, and the Choi-matrix formula of Theorem 1.

Contributions are welcome at every level: proofs of the milestones, a general Lean theory of base sections and their norms (Theorem 8, Corollary 8 in abstract form) that would serve other ordered-vector-space arguments, and alternative proofs of (iii)⇒(iv) using Mathlib's minimax theorem.

Selected references

  • A. Jenčová, Randomization theorems for quantum channels, arXiv preprint, 2014. https://arxiv.org/abs/1404.3900v1
  • A. Jenčová, Base norms and discrimination of generalized quantum channels, arXiv preprint, 2013. https://arxiv.org/abs/1308.4030
  • K. Matsumoto, A quantum version of randomization criterion, arXiv preprint, 2010. https://arxiv.org/abs/1012.2650
  • A. Chefles, The quantum Blackwell theorem and minimum error state discrimination, arXiv preprint, 2009. https://arxiv.org/abs/0907.0866
  • F. Buscemi, Comparison of quantum statistical models: equivalent conditions for sufficiency, Commun. Math. Phys. 310, 625–647, 2012. https://arxiv.org/abs/1004.3794
  • E. Shmaya, Comparison of information structures and completely positive maps, J. Phys. A 38, 9717–9727, 2005. https://arxiv.org/abs/quant-ph/0412001
  • D. Blackwell, Comparison of experiments, Proc. 2nd Berkeley Symp. Math. Stat. Probab., 93–102, 1951.
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AnalysisFunctional Analysis·Captain: mikedeng1

A reduction method for noncommutative Lp-spaces and applications: The Dyadic Crossed Product of a σ-Finite von Neumann Algebra Is the w*-Closure of Increasing Finite Subalgebras with ExpectationsResearch Paper

Motivation

Noncommutative LpL_pLp​-spaces built from a von Neumann algebra MMM come in two kinds. When MMM carries a normal faithful trace, Lp(M)L_p(M)Lp​(M) is a space of (unbounded) operators affiliated with MMM, and much of classical analysis — martingale inequalities, square functions, maximal inequalities, interpolation — has been carried over to this tracial setting. Algebras of type III, which occur naturally in quantum field theory and quantum statistical mechanics, have no such trace; their LpL_pLp​-spaces are Haagerup's, defined through a crossed product and the dual weight.

Haagerup, Junge and Xu (arXiv:0806.3635, Trans. AMS 362 (2010)) give a general method for transferring tracial results to type III algebras. Its engine is a reduction theorem, due to Haagerup and circulated as an unpublished manuscript since the late 1970s: after enlarging MMM to a crossed product, the algebra is approximated by an increasing sequence of finite von Neumann algebras, in a way that respects the state and its modular group. This mission formalizes that theorem, §2 of the paper.

Timeline. Haagerup constructs his LpL_pLp​-spaces in 1979 (Colloq. Internat. CNRS 274) and proves the reduction in the manuscript [H3]. Junge and Xu use it for noncommutative Burkholder–Rosenthal inequalities (Ann. Probab. 2003) and maximal ergodic theorems (J. AMS 2007). The 2008 preprint, revised in 2009, gives the first published proof together with its applications to LpL_pLp​ approximation, extension of maps to crossed products, and martingale and maximal inequalities.

Setting

MMM is a von Neumann algebra on a Hilbert space HHH with a normal faithful state φ\varphiφ. Up to spatial isomorphism MMM is in standard form: there is a unit vector ξ\xiξ, cyclic and separating for MMM, with φ(x)=⟨xξ,ξ⟩\varphi(x) = \langle x\xi,\xi\rangleφ(x)=⟨xξ,ξ⟩. Tomita–Takesaki theory supplies the modular operator Δ\DeltaΔ and the modular automorphism group σtφ(x)=ΔitxΔ−it\sigma^\varphi_t(x) = \Delta^{it}x\Delta^{-it}σtφ​(x)=ΔitxΔ−it.

G=⋃n≥12−nZG = \bigcup_{n\ge1}2^{-n}\mathbb ZG=⋃n≥1​2−nZ is the group of dyadic rationals with the discrete topology. On ℓ2(G,H)\ell^2(G,H)ℓ2(G,H) define

(π(x)η)(h)=σ−hφ(x) η(h),(λ(g)η)(h)=η(h−g),(\pi(x)\eta)(h) = \sigma^\varphi_{-h}(x)\,\eta(h),\qquad (\lambda(g)\eta)(h) = \eta(h-g),(π(x)η)(h)=σ−hφ​(x)η(h),(λ(g)η)(h)=η(h−g),

for x∈Mx\in Mx∈M, g,h∈Gg,h\in Gg,h∈G. The crossed product R=M⋊σφG\mathcal R = M\rtimes_{\sigma^\varphi}GR=M⋊σφ​G is the von Neumann algebra generated by π(M)\pi(M)π(M) and λ(G)\lambda(G)λ(G). With ξ^=δ0⊗ξ\hat\xi = \delta_0\otimes\xiξ^​=δ0​⊗ξ, the dual state is φ^(y)=⟨yξ^,ξ^⟩\hat\varphi(y) = \langle y\hat\xi,\hat\xi\rangleφ^​(y)=⟨yξ^​,ξ^​⟩; on generators φ^(λ(g)π(x))\hat\varphi(\lambda(g)\pi(x))φ^​(λ(g)π(x)) equals φ(x)\varphi(x)φ(x) for g=0g = 0g=0 and 000 otherwise. Its modular group is σφ^\sigma^{\hat\varphi}σφ^​, and ∥y∥φ^=φ^(y∗y)1/2\|y\|_{\hat\varphi} = \hat\varphi(y^*y)^{1/2}∥y∥φ^​​=φ^​(y∗y)1/2.

For a bounded functional ψ\psiψ on an algebra AAA, the centralizer is Aψ={x∈A:ψ(xy)=ψ(yx) ∀y∈A}A_\psi = \{x\in A:\psi(xy) = \psi(yx)\ \forall y\in A\}Aψ​={x∈A:ψ(xy)=ψ(yx) ∀y∈A}. With bn=−i Log λ(2−n)b_n = -i\,\mathrm{Log}\,\lambda(2^{-n})bn​=−iLogλ(2−n) (branch 0≤Im⁡Log<2π0\le\operatorname{Im}\mathrm{Log}<2\pi0≤ImLog<2π), an=2nbna_n = 2^nb_nan​=2nbn​ and φn(x)=φ^(e−anx)\varphi_n(x) = \hat\varphi(e^{-a_n}x)φn​(x)=φ^​(e−an​x), the subalgebras are Rn=Rφn\mathcal R_n = \mathcal R_{\varphi_n}Rn​=Rφn​​. A von Neumann algebra is finite if every isometry in it is unitary. A conditional expectation from R\mathcal RR onto a subalgebra AAA is a positive linear AAA-bimodular map onto AAA fixing AAA.

Formalization targets

Goal: Theorem 2.1 (p. 6)

There is an increasing sequence (Rn)(\mathcal R_n)(Rn​) of von Neumann subalgebras of R\mathcal RR such that each Rn\mathcal R_nRn​ is finite, ⋃nRn\bigcup_n\mathcal R_n⋃n​Rn​ is w*-dense in R\mathcal RR, and for each nnn there is a normal faithful conditional expectation Φn:R→Rn\Phi_n:\mathcal R\to\mathcal R_nΦn​:R→Rn​ with

φ^∘Φn=φ^,σtφ^∘Φn=Φn∘σtφ^(t∈R).\hat\varphi\circ\Phi_n = \hat\varphi,\qquad \sigma^{\hat\varphi}_t\circ\Phi_n = \Phi_n\circ\sigma^{\hat\varphi}_t\quad(t\in\mathbb R).φ^​∘Φn​=φ^​,σtφ^​​∘Φn​=Φn​∘σtφ^​​(t∈R).

The goal asserts existence only, as printed; the construction Rn=Rφn\mathcal R_n = \mathcal R_{\varphi_n}Rn​=Rφn​​ is the content of the milestones.

Milestones

  1. Dual modular data (p. 6, (1.7) p. 4): ξ^\hat\xiξ^​ is cyclic and separating for R\mathcal RR, so φ^\hat\varphiφ^​ has modular data; σtφ^(π(x))=π(σtφ(x))\sigma^{\hat\varphi}_t(\pi(x)) = \pi(\sigma^\varphi_t(x))σtφ^​​(π(x))=π(σtφ​(x)) and σtφ^(λ(g))=λ(g)\sigma^{\hat\varphi}_t(\lambda(g)) = \lambda(g)σtφ^​​(λ(g))=λ(g).
  2. Lemma 2.2: φ^(f(λ(t)))=∫Tf dm\hat\varphi(f(\lambda(t))) = \int_{\mathbb T}f\,dmφ^​(f(λ(t)))=∫T​fdm for t∈G∖{0}t\in G\setminus\{0\}t∈G∖{0}.
  3. Lemma 2.3: λ(t)∈Z(Rφ^)\lambda(t)\in Z(\mathcal R_{\hat\varphi})λ(t)∈Z(Rφ^​​); bnb_nbn​ is the unique element of Z(Rφ^)Z(\mathcal R_{\hat\varphi})Z(Rφ^​​) with 0≤bn≤2π0\le b_n\le2\pi0≤bn​≤2π and eibn=λ(2−n)e^{ib_n} = \lambda(2^{-n})eibn​=λ(2−n).
  4. Lemma 2.4: σφn\sigma^{\varphi_n}σφn​ is 2−n2^{-n}2−n-periodic; there is a unique φ^\hat\varphiφ^​-preserving, σφ^\sigma^{\hat\varphi}σφ^​-commuting normal faithful conditional expectation onto Rn\mathcal R_nRn​; Rn⊆Rn+1\mathcal R_n\subseteq\mathcal R_{n+1}Rn​⊆Rn+1​.
  5. Lemma 2.5: for a normal faithful state ψ\psiψ, analytic xxx gives xψx∗≤cψx\psi x^*\le c\psixψx∗≤cψ, and xxx in the centralizer gives xψx∗≤∥x∥2ψx\psi x^*\le\|x\|^2\psixψx∗≤∥x∥2ψ.
  6. Lemma 2.6: ∥[bn,x]∥φ^→0\|[b_n,x]\|_{\hat\varphi}\to0∥[bn​,x]∥φ^​​→0, sup⁡∣t∣≤1∥[eitbn,x]∥φ^→0\sup_{|t|\le1}\|[e^{itb_n},x]\|_{\hat\varphi}\to0sup∣t∣≤1​∥[eitbn​,x]∥φ^​​→0, and sup⁡t∥σtφ^(x)−eiantxe−iant∥φ^→0\sup_t\|\sigma^{\hat\varphi}_t(x)-e^{ia_nt}xe^{-ia_nt}\|_{\hat\varphi}\to0supt​∥σtφ^​​(x)−eian​txe−ian​t∥φ^​​→0.
  7. Lemma 2.7: Φn(x)→x\Phi_n(x)\to xΦn​(x)→x σ-strongly, so ⋃nRn\bigcup_n\mathcal R_n⋃n​Rn​ is σ-strongly dense.

Significance

The reduction theorem lets a statement about Haagerup Lp(M)L_p(M)Lp​(M) be proved by checking it on the finite algebras Rn\mathcal R_nRn​, where traces exist, and passing to the limit: the expectations Φn\Phi_nΦn​ extend to contractive projections on LpL_pLp​ and their ranges exhaust Lp(R)L_p(\mathcal R)Lp​(R), which contains Lp(M)L_p(M)Lp​(M) complementably. The paper uses this to obtain noncommutative Burkholder–Gundy, Stein, Burkholder–Rosenthal and Doob inequalities, and maximal ergodic inequalities, for type III algebras; for some of these no other proof is known. The theorem has since become a standard tool in noncommutative probability and harmonic analysis.

The theorem is proved (in the cited paper, with details on pp. 7–11). It has not been formalized: Mathlib has von Neumann algebras as double commutants but no crossed products, conditional expectations, modular theory or Haagerup LpL_pLp​-spaces. This mission produces a formal statement of the reduction theorem and of each lemma of its proof, built on the published standard-form encoding of Tomita–Takesaki data, and invites solvers to formalize the known proof.

Difficulty

The modular group of a type III algebra is outer and aperiodic, so no centralizer is large enough to be finite and dense at once. The proof works around this by perturbing φ^\hat\varphiφ^​ to states φn\varphi_nφn​ whose modular groups are periodic, and the delicate step is density: showing that the centralizers Rφn\mathcal R_{\varphi_n}Rφn​​ eventually see every element of R\mathcal RR. This rests on uniform estimates in the φ^\hat\varphiφ^​-norm (Lemma 2.6) that need the distribution of λ(t)\lambda(t)λ(t) under φ^\hat\varphiφ^​ (Lemma 2.2), analytic elements (Lemma 2.5), and an L2L_2L2​ approximation of the logarithm by trigonometric polynomials. Norm density of ⋃nRn\bigcup_n\mathcal R_n⋃n​Rn​ is false in general; only weak*-type density holds. For finite MMM the statement is easy (R\mathcal RR is already finite); the content is the type III case.

Formalization scope

(M,φ)(M,\varphi)(M,φ) is given by the published OAI.BoundedRecovery.StandardModularData H: a von Neumann algebra on HHH, a unit cyclic separating vector ξ\xiξ, log⁡Δ\log\DeltalogΔ as a nondegenerate functional calculus, and JJJ, tied together by the closed Tomita relation; σtφ\sigma^\varphi_tσtφ​ is its sigma. Every σ-finite von Neumann algebra with a normal faithful state is spatially isomorphic to such data, and every statement is invariant under spatial isomorphism.

The crossed product is built on lp (fun _ : dyadic => H) 2, as the double commutant of π(M)∪λ(G)\pi(M)\cup\lambda(G)π(M)∪λ(G) and their adjoints. π(x)\pi(x)π(x), λ(g)\lambda(g)λ(g) and bnb_nbn​ are the bounded operators characterized by their pointwise formulas; bnb_nbn​ is the Laurent operator of θ↦θ\theta\mapsto\thetaθ↦θ on [0,2π)[0,2\pi)[0,2π) in the shift λ(2−n)\lambda(2^{-n})λ(2−n), which is −i Log λ(2−n)-i\,\mathrm{Log}\,\lambda(2^{-n})−iLogλ(2−n) (Mathlib has no Borel functional calculus). Centralizers use the commutation form for bounded functionals. Finiteness is the published OAI.FiniteFactor.IsFiniteAlgebra (every isometry is unitary). W*-density is equality of the double commutant with R\mathcal RR; σ-strong convergence of bounded sequences is strong convergence. Order on operators is the Loewner order. Lemma 2.2 is stated for continuous fff, which already determines the distribution.

Hypothesized modular data. The platform has no Tomita–Takesaki existence theorem, so the modular data of φ^\hat\varphiφ^​ (and of φn\varphi_nφn​ in Lemma 2.4 (i)) enter as hypotheses S^\hat SS^ with S^.M=R\hat S.M = \mathcal RS^.M=R and S^.ξ=ξ^\hat S.\xi = \hat\xiS^.ξ=ξ^​; the first milestone proves such S^\hat SS^ exists, so the goal is not vacuous. The formalization does not restrict to finite, finite-dimensional or tracial MMM (where the goal is empty); σφ^\sigma^{\hat\varphi}σφ^​ is never defined by a formula; finite means "every isometry is unitary", not finite-dimensional; and density is never norm density.

Reusable beyond this mission: the dyadic crossed product and dual state, conditional expectations, the commutation-form centralizer, and Lemma 2.5 for arbitrary standard-form data. Welcome contributions include the existence of modular data for crossed products, the shift and Laurent operators on ℓ2\ell^2ℓ2 of a discrete group, and the averaging construction of conditional expectations from periodic modular groups.

Selected references

  • U. Haagerup, M. Junge, Q. Xu, A reduction method for noncommutative LpL_pLp​-spaces and applications, Trans. Amer. Math. Soc. 362 (2010), 2125–2165; arXiv:0806.3635v2. https://arxiv.org/abs/0806.3635
  • U. Haagerup, LpL^pLp-spaces associated with an arbitrary von Neumann algebra, Algèbres d'opérateurs et leurs applications en physique mathématique, Colloq. Internat. CNRS 274 (1979), 175–184.
  • Ş. Strătilă, Modular Theory in Operator Algebras, Editura Academiei / Abacus Press, 1981 (dual weights, §19).
  • M. Takesaki, Theory of Operator Algebras II, Encyclopaedia Math. Sci. 125, Springer, 2003. https://doi.org/10.1007/978-3-662-10451-4
  • M. Junge, Q. Xu, Noncommutative maximal ergodic theorems, J. Amer. Math. Soc. 20 (2007), 385–439. https://doi.org/10.1090/S0894-0347-06-00533-9
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ProbabilityQuantum InformationRandom Matrix Theory·Captain: mikedeng1

Matrix concentration inequalities and efficiency of random universal sets of quantum gates: P(δ(ν_S,t) ≥ δ) ≤ 2e^{−δS artanh δ}(1−δ²)^{−S/2}Σ_{λ∈Λ_t} d_λ for S Gates Drawn from an Exact t-DesignResearch Paper

Why random gate sets matter

Quantum information protocols often require a finite collection of unitary gates whose averages reproduce those of the full unitary group. A unitary design gives a precise finite-moment version of that requirement. When gates are sampled from an exact design, a practitioner needs to know how many independent draws make the empirical collection a reliable approximation. Dulian and Sawicki give an explicit probability bound for that question in Theorem 1 of their paper. The bound depends on the sample count, the desired accuracy, and the dimensions of the irreducible representations visible at the chosen moment order.

The result joins two subjects. Matrix concentration controls the norm of a sum of random operators. Representation theory identifies which operator blocks occur in the moment being estimated and supplies their dimensions. Neither ingredient alone gives the numerical bound stated by the paper. This mission formalizes their combination for independent gates drawn from any exact ttt-design, including Haar-distributed gates.

Unitary moments and sampled gates

Fix integers d,t≥0d,t\ge0d,t≥0. Write U(d)U(d)U(d) for the group of complex d×dd\times dd×d unitary matrices and μ\muμ for its Haar probability measure. For a gate U∈U(d)U\in U(d)U∈U(d), its mixed tensor representation is

Ut,t=U⊗t⊗U‾⊗t,U^{t,t}=U^{\otimes t}\otimes\overline U^{\otimes t},Ut,t=U⊗t⊗U⊗t,

where the bar conjugates every matrix entry. For a probability measure ν\nuν on U(d)U(d)U(d), the moment operator is Tν,t=∫Ut,t dν(U)T_{\nu,t}=\int U^{t,t}\,d\nu(U)Tν,t​=∫Ut,tdν(U). An exact ttt-design is a probability measure ν\nuν satisfying Tν,t=Tμ,tT_{\nu,t}=T_{\mu,t}Tν,t​=Tμ,t​. The design distance is δ(ν,t)=∥Tν,t−Tμ,t∥\delta(\nu,t)=\|T_{\nu,t}-T_{\mu,t}\|δ(ν,t)=∥Tν,t​−Tμ,t​∥, using the spectral operator norm.

Draw SSS independent gates U1,…,USU_1,\ldots,U_SU1​,…,US​ from an exact ttt-design ν\nuν, with S≥1S\ge1S≥1. Their empirical measure νS\nu_SνS​ counts every draw, including repetitions, with weight 1/S1/S1/S. Thus TνS,t=S−1∑k=1SUkt,tT_{\nu_S,t}=S^{-1}\sum_{k=1}^S U_k^{t,t}TνS​,t​=S−1∑k=1S​Ukt,t​. This convention implements the sum used in the paper's concentration argument and remains meaningful when the sampling distribution has atoms.

The moment representation splits into a trivial part and nontrivial irreducible blocks indexed by Λt\Lambda_tΛt​. An index λ=(λ1,…,λd)\lambda=(\lambda_1,\ldots,\lambda_d)λ=(λ1​,…,λd​) is a nonzero weakly decreasing integer tuple with ∑iλi=0\sum_i\lambda_i=0∑i​λi​=0 and ∑imax⁡(λi,0)≤t\sum_i\max(\lambda_i,0)\le t∑i​max(λi​,0)≤t. Its block dimension is the Weyl dimension

dλ=∏1≤i<j≤dλi−λj+j−ij−i.d_\lambda=\prod_{1\le i<j\le d}\frac{\lambda_i-\lambda_j+j-i}{j-i}.dλ​=1≤i<j≤d∏​j−iλi​−λj​+j−i​.

This explicit index set and dimension formula come from equations (20), (22), and (23) of the source. The zero- and one-dimensional cases are included in the formal statement; their nontrivial index set can be empty.

Formalization targets

The goal is the corrected positive-threshold form of Theorem 1, for S≥1S\ge1S≥1 and 0<δ<10<\delta<10<δ<1:

Pr⁡(δ(νS,t)≥δ)≤2e−δSartanh⁡(δ)(1−δ2)S/2∑λ∈Λtdλ.\Pr\bigl(\delta(\nu_S,t)\ge\delta\bigr)\le \frac{2e^{-\delta S\operatorname{artanh}(\delta)}}{(1-\delta^2)^{S/2}} \sum_{\lambda\in\Lambda_t}d_\lambda.Pr(δ(νS​,t)≥δ)≤(1−δ2)S/22e−δSartanh(δ)​λ∈Λt​∑​dλ​.

The paper prints “any δ<1\delta<1δ<1.” Its formula fails for some nonpositive δ\deltaδ: a negative threshold makes the event certain while the displayed expression can decrease below one as SSS grows. At δ=0\delta=0δ=0, an empty Λt\Lambda_tΛt​ also gives a zero right-hand side for a certain event. The positive-threshold range is the meaningful form of its result.

The milestone list follows the paper's numbered claims. Fact 2 provides a master concentration bound for independent complex matrices through Hermitian dilation. Theorem 18 specializes it to one irreducible block, with its two equivalent closed forms of the tail factor. Lemma 16 and equation (24) connect the full design distance to the norms of those blocks and state the resulting union bound. Fact 9 supplies the decomposition indexed by Λt\Lambda_tΛt​ and the Weyl dimensions needed to turn the block sum into Theorem 1's explicit sum.

What the result provides

The bound gives a finite-sample guarantee for the mixed tensor moment of random gates. It exposes how an accuracy threshold and a representation-theoretic dimension sum determine the chance that the empirical moment differs from Haar averaging. A reader can evaluate the right-hand side once ddd, ttt, SSS, and δ\deltaδ are fixed. The bound also covers Haar random gates because Haar measure itself is an exact design at every order, as the paper observes in Section 6.

The mathematical result was proved by Dulian and Sawicki; the machine-checked development requested here remains to be built. Existing published Prove2Me modules already provide a spectral matrix norm, a Hermitian dilation, and a general matrix master bound. The new formalization must establish the paper's mixed tensor representation model, its irreducible decomposition and weight dimensions, the one-block estimate, and their assembly into the displayed inequality. These components can serve later results on random unitary designs and matrix concentration.

Main difficulty

The operator Ut,tU^{t,t}Ut,t acts on a space of dimension d2td^{2t}d2t, so applying a single matrix tail bound directly to it leaves a prefactor governed by that large ambient dimension. The paper's sharper expression depends on separating the nontrivial irreducible blocks, removing the Haar-invariant part, and identifying the dimensions of exactly the blocks that occur. The critical representation-theoretic step is the complete, multiplicity-aware decomposition in Fact 9. A bound for an arbitrary collection of block matrices would not identify the paper's Λt\Lambda_tΛt​ or its Weyl dimension sum.

Formalization scope

Lean represents U(d)U(d)U(d) as Matrix.unitaryGroup (Fin d) ℂ with the measurable space induced from the published Borel structure on complex matrices. The mixed tensor basis is indexed by a pair of functions from Fin t to Fin d; ordinary factors come first, conjugate factors second. The measure μ\muμ is required to be a left- and right-invariant probability measure. An exact design is a probability measure with equality of the full mixed tttth moment, not merely a first moment or a one-sided tensor power. Independent samples use the product measure, and the empirical moment is their average with multiplicity.

The norm is the published L2L^2L2 operator norm on matrices. The set Λt\Lambda_tΛt​ is a finite set of integer tuples; bounds −t≤λi≤t-t\le\lambda_i\le t−t≤λi​≤t follow from its defining constraints. The Weyl product uses zero-based Fin d indices, which preserve every difference j−ij-ij−i. All real exponents are real powers, with positive bases in the stated threshold range. The supremum over zero nontrivial blocks is defined to be zero, matching the zero design distance in that case.

The representation structure requires positive dimensions and multiplicities, irreducibility, pairwise inequivalence, orthogonal isometric embeddings, completeness, and intertwining with the concrete mixed tensor action. Those requirements prevent a vacuous or incomplete block family from making the goal automatic. Contributions are welcome on the representation decomposition, the Haar projection onto the trivial part, the non-Hermitian matrix bound, and the probability-to-block reduction. The source's highest-weight labels are kept: the block indexed by λ∈Λt\lambda\in\Lambda_tλ∈Λt​ has λ\lambdaλ as its highest weight, expressed through weights of the diagonal torus and the dominance order of the simple roots Li−Li+1L_i-L_{i+1}Li​−Li+1​, and its dimension is the Weyl product dλd_\lambdadλ​.

Selected references

  • C. Dulian and A. Sawicki, Matrix concentration inequalities and efficiency of random universal sets of quantum gates, arXiv preprint (2023), arXiv:2202.05371v3.
  • J. A. Tropp, An Introduction to Matrix Concentration Inequalities, Foundations and Trends in Machine Learning, 2015, doi:10.1561/2200000048.
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