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Control TheoryOperations ResearchProbability+1·Captain: iris

Joint Inventory and Scheduling Control in a Repair Facility: The Barrier Policy Is Optimal for the Equivalent Workload Formulation When Emergency Repairs Pay OffResearch Paper

Repair facilities and the value of emergency repairs

A firm that maintains capital goods (aircraft, medical scanners, lithography machines) keeps spare parts and runs a repair shop. When a part fails, it is replaced from stock if possible. Otherwise a machine waits, and the firm pays a backorder cost. The firm must choose how many spares of each part type to hold, which failed part to repair next, and when to pay for an outside emergency repair. Özkan and van Houtum study this joint control problem in the heavy-traffic regime of a closed repairable-parts network (SSRN 3784144; published later in Operations Research). This mission works from the SSRN copy.

The limiting problem is solved exactly, and the answer is a decision rule: emergency repairs are worth using exactly when the least backorder saving per unit of repair time exceeds the least emergency cost per unit of repair time.

Setting

There are n≥1n\ge1n≥1 part types (SKUs), with repair rates μi>0\mu_i>0μi​>0, limiting breakdown rates λi>0\lambda_i>0λi​>0, costs bi,ci,hi>0b_i,c_i,h_i>0bi​,ci​,hi​>0, a drift θ≤0\theta\le0θ≤0 and a variance Σ>0\Sigma>0Σ>0. Let XXX be a Brownian motion with drift 000 and variance Σ\SigmaΣ, started at 000. An inventory vector S∈R+nS\in\mathbb R^n_+S∈R+n​ is fixed.

The equivalent workload formulation (EWF) chooses a workload W≥0W\ge0W≥0, an idleness process III, an emergency repair process EEE, and an allocation a(t)∈A(W(t))a(t)\in\mathcal A(W(t))a(t)∈A(W(t)), where

A(w)={q∈R+n:∑iqi/μi=w},\mathcal A(w)=\Big\{q\in\mathbb R^n_+:\sum_i q_i/\mu_i=w\Big\},A(w)={q∈R+n​:i∑​qi​/μi​=w},

subject to

W(t)=X(t)+θt−∑iλiμi∫0t(ai(s)−Si)+ ds+I(t)−E(t).W(t)=X(t)+\theta t-\sum_i\frac{\lambda_i}{\mu_i}\int_0^t(a_i(s)-S_i)^+\,ds+I(t)-E(t).W(t)=X(t)+θt−i∑​μi​λi​​∫0t​(ai​(s)−Si​)+ds+I(t)−E(t).

The processes III and EEE start at 000, are nondecreasing, càdlàg and adapted. Write bjμj/λj=min⁡ibiμi/λib_j\mu_j/\lambda_j=\min_i b_i\mu_i/\lambda_ibj​μj​/λj​=mini​bi​μi​/λi​ and ckμk=min⁡iciμic_k\mu_k=\min_i c_i\mu_ick​μk​=mini​ci​μi​. The objective is

lim sup⁡t→∞ ∑ihiSi+1t E[∑ibi∫0t(ai(s)−Si)+ ds+ckμkE(t)].\limsup_{t\to\infty}\ \sum_i h_iS_i+\frac1t\,\mathbf E\Big[\sum_i b_i\int_0^t(a_i(s)-S_i)^+\,ds+c_k\mu_kE(t)\Big].t→∞limsup​ i∑​hi​Si​+t1​E[i∑​bi​∫0t​(ai​(s)−Si​)+ds+ck​μk​E(t)].

The candidate solution comes from the Bellman system (13): find (f,B,γ)(f,B,\gamma)(f,B,γ) with f∈C2f\in C^2f∈C2, B>0B>0B>0, γ≥0\gamma\ge0γ≥0 such that

12Σf′′(w)+θf′(w)+min⁡q∈A(w)∑i(bi−λiμif′(w))(qi−Si)+=γon [0,B],\tfrac12\Sigma f''(w)+\theta f'(w)+\min_{q\in\mathcal A(w)}\sum_i\Big(b_i-\frac{\lambda_i}{\mu_i}f'(w)\Big)(q_i-S_i)^+=\gamma\quad\text{on }[0,B],21​Σf′′(w)+θf′(w)+q∈A(w)min​i∑​(bi​−μi​λi​​f′(w))(qi​−Si​)+=γon [0,B],

with ≥γ\ge\gamma≥γ for w>Bw>Bw>B, 0≤f′≤ckμk0\le f'\le c_k\mu_k0≤f′≤ck​μk​ on R+\mathbb R_+R+​, f′(0)=0f'(0)=0f′(0)=0 and f′(B)=ckμkf'(B)=c_k\mu_kf′(B)=ck​μk​.

The barrier policy reflects the workload at 000 and at BBB and allocates by q∗q^*q∗, which backorders only one SKU, κ(w)∈arg⁡min⁡i{biμi−λif′(w)}\kappa(w)\in\arg\min_i\{b_i\mu_i-\lambda_if'(w)\}κ(w)∈argmini​{bi​μi​−λi​f′(w)}, above total inventory.

Formalization targets

Goal: Theorem 2

Suppose bjμj/λj>ckμkb_j\mu_j/\lambda_j>c_k\mu_kbj​μj​/λj​>ck​μk​. Then (13) has a solution, and for each solution a barrier policy with upper barrier BBB exists, and

lim⁡t→∞1t E[∑ibi∫0t(ai(s)−Si)+ ds+ckμkE(t)]=γ\lim_{t\to\infty}\frac1t\,\mathbf E\Big[\sum_i b_i\int_0^t(a_i(s)-S_i)^+\,ds+c_k\mu_kE(t)\Big]=\gammat→∞lim​t1​E[i∑​bi​∫0t​(ai​(s)−Si​)+ds+ck​μk​E(t)]=γ

under it, while every EWF-feasible solution with the same SSS has objective at least ∑ihiSi+γ\sum_ih_iS_i+\gamma∑i​hi​Si​+γ.

Milestones

  • The allocation problem: Lemma 1.
  • The initial value problem for f′f'f′: Lemmas A.3.1, A.3.2, A.3.3, A.3.6, A.3.8, A.3.9.
  • The Bellman system: Lemma 2 Part ii.
  • The regulators: Lemmas A.4.3 and 4.
  • The verification argument: (A.58), (A.45)–(A.47), (A.62), (A.63).

Significance

Theorem 2 identifies an explicit optimal policy and its cost for a singular ergodic control problem with a state-dependent drift. The cost is computed by a one-dimensional free-boundary problem, which is what makes the inventory optimization of the paper's §5 tractable.

The result is proved in the paper; no machine-checked proof of it is known to this mission. Formalizing it adds a verification theorem for ergodic singular control with jump controls, a reflected equation with discontinuous monotone drift, and a global analysis of a piecewise linear ODE. These are the recurring pieces of Brownian control problems in operations research. The only other instance on the platform is AtaBarjesteh23.Workload, for a different workload formulation, and its goals are still open.

The formalization also corrects the source. Printed Lemma 4 claims a regulator solution for every càdlàg input, and that is false when q∗q^*q∗ makes the drift jump (see Difficulty). The mission states the corrected lemma and the barrier policy almost surely.

Difficulty

The obvious existence argument for the barrier policy fails. The drift β(w)=∑i(λi/μi)(qi∗(w)−Si)+\beta(w)=\sum_i(\lambda_i/\mu_i)(q_i^*(w)-S_i)^+β(w)=∑i​(λi​/μi​)(qi∗​(w)−Si​)+ jumps upward wherever κ\kappaκ changes. The paper patches the regulator over the intervals between jumps. On a path that approaches a jump point w0w_0w0​ from below with slope strictly between the two one-sided values of β\betaβ, the workload can neither cross w0w_0w0​ nor stay there. So no solution exists for that path, and existence holds only for almost every Brownian path, where the noise prevents this. Pathwise uniqueness is still true because β\betaβ is nondecreasing on [0,B][0,B][0,B].

The second difficulty is the competitor class. Feasible solutions need not be Markov, work-conserving or continuous, and EEE may jump. Expected workload may even grow linearly. Itô's formula alone therefore does not give the lower bound: the jumps of EEE and III and the growth of E[W(t)]\mathbf E[W(t)]E[W(t)] need separate treatment.

Formalization scope

Time is indexed by R\mathbb RR, and only t≥0t\ge0t≥0 is constrained. The SKU set is Fin n with n≥1n\ge1n≥1. Costs are computed in R≥0∪{∞}\mathbb R_{\ge0}\cup\{\infty\}R≥0​∪{∞} with lower integrals, so an infinite expectation is ∞\infty∞. The measures dℓd\elldℓ and dududu are Lebesgue–Stieltjes measures of the path extended by 000 to negative times. Feasibility requires progressive measurability of the allocation and integrable paths, and it holds for every ω\omegaω. The filtration satisfies the usual conditions, as in the paper. The published definition AtaBarjesteh23.Workload.IsDriftBM is the Brownian motion.

The allocation q∗q^*q∗ is fixed: the fill of OA A.2 when no SKU is backordered, and the largest-λ\lambdaλ tie-break otherwise. That is the right-continuous choice named on OA p.26. Regulators are stated for b≤Bb\le Bb≤B, where f′f'f′ is strictly increasing.

A trivial reading is excluded in three ways. The goal asserts existence of the Bellman solution and of the barrier policy, so it is not conditional on either. The lower bound ranges over all feasible solutions. A path with non-integrable allocation is not feasible, so it cannot gain a junk drift of 000.

The development needs an Itô formula for processes with finite-variation jump parts, a reflection map on D\mathbb DD, and global ODE comparison arguments. Each is reusable beyond this mission. Contributions to any of them are welcome, and so is a pathwise treatment of the regulator with monotone discontinuous drift.

Selected references

  • E. Özkan, G.-J. van Houtum, Joint Inventory and Scheduling Control in a Repair Facility, SSRN 3784144 (2023). https://ssrn.com/abstract=3784144
  • E. Özkan, G.-J. van Houtum, Joint Inventory and Scheduling Control in a Repair Facility, Operations Research (2023). https://doi.org/10.1287/opre.2023.2459
  • J. M. Harrison, Brownian Models of Performance and Control, Cambridge University Press, 2013. https://doi.org/10.1017/CBO9781139087698
  • W. Whitt, Stochastic-Process Limits, Springer, 2002. https://doi.org/10.1007/b97479
  • A. Ju. Veretennikov, On strong solutions and explicit formulas for solutions of stochastic integral equations, Math. USSR-Sb. 39 (1981). https://doi.org/10.1070/SM1981v039n03ABEH001518
42 thms2 active usersReviewed
Numerical AnalysisOperations ResearchOptimization·Captain: iris

A 0/1 Constrained Optimization Solving Sample Average Approximation for Chance Constrained Programming: SNSCO Takes Full Newton Steps and Converges Locally Superlinearly or QuadraticallyResearch Paper

Motivation

A chance constrained program minimizes a cost while requiring a random constraint to hold with high probability. It models decisions under uncertainty in energy systems, finance, and process and water-quality engineering. Replacing the probability by an empirical frequency over NNN samples gives the sample average approximation, whose constraint counts the violated samples. This counting function is a 0/1 loss: it is discontinuous, and the resulting problem is NP-hard. The usual remedies are mixed-integer reformulations, or smooth and convex surrogates that change the problem.

Zhou, Pan, Xiu and Li (arXiv:2210.11889v5) work on the 0/1 constraint directly. They compute the projection onto the constraint set, define a stationarity condition from it, and rewrite that condition as a system of equations. A semismooth Newton method, SNSCO, then solves the system. This mission formalizes the local analysis of SNSCO.

Setting

Let f:RK→Rf:\mathbb R^K\to\mathbb Rf:RK→R and G:RK→RM×NG:\mathbb R^K\to\mathbb R^{M\times N}G:RK→RM×N be continuously differentiable, let Ω⊆RK\Omega\subseteq\mathbb R^KΩ⊆RK be nonempty, closed and convex, and let s≥1s\ge 1s≥1 be an integer. For a matrix ZZZ, the quantity ∥Z∥0+\|Z\|_0^+∥Z∥0+​ counts the columns of ZZZ with a positive entry. The problem (SCO) is

min⁡x∈Ωf(x)subject to∥G(x)∥0+≤s.\min_{x\in\Omega} f(x)\quad\text{subject to}\quad \|G(x)\|_0^+\le s.x∈Ωmin​f(x)subject to∥G(x)∥0+​≤s.

With G(x)=(g(x,ξ1),…,g(x,ξN))G(x)=(g(x,\xi_1),\dots,g(x,\xi_N))G(x)=(g(x,ξ1​),…,g(x,ξN​)) and s=⌈αN⌉s=\lceil\alpha N\rceils=⌈αN⌉ this is the sample average approximation.

Write S:={Z:∥Z∥0+≤s}\mathcal S:=\{Z:\|Z\|_0^+\le s\}S:={Z:∥Z∥0+​≤s}. The set ΠS(Z)\Pi_{\mathcal S}(Z)ΠS​(Z) of nearest points of S\mathcal SS has a closed form. It is described by a family T(Z;s)\mathbb T(Z;s)T(Z;s) of column sets, which records the choices of sss columns of largest positive part. A point x∗x^*x∗ with multiplier W∗W^*W∗ is τ\tauτ-stationary if

x∗=ΠΩ(x∗−τ[∇f(x∗)+∑Wmn∗∇Gmn(x∗)]),Z∗∈ΠS(Z∗+τW∗),x^*=\Pi_\Omega\bigl(x^*-\tau[\nabla f(x^*)+\textstyle\sum W^*_{mn}\nabla G_{mn}(x^*)]\bigr),\qquad Z^*\in\Pi_{\mathcal S}(Z^*+\tau W^*),x∗=ΠΩ​(x∗−τ[∇f(x∗)+∑Wmn∗​∇Gmn​(x∗)]),Z∗∈ΠS​(Z∗+τW∗),

where Z∗=G(x∗)Z^*=G(x^*)Z∗=G(x∗). Put w=(x;vec(W))w=(x;\mathrm{vec}(W))w=(x;vec(W)) and Λ=G(x)+τW\Lambda=G(x)+\tau WΛ=G(x)+τW. For an index set V\mathcal VV, the map F(w;V)F(w;\mathcal V)F(w;V) collects a projected-gradient residual φ(w;V)\varphi(w;\mathcal V)φ(w;V), the entries of G(x)G(x)G(x) on V\mathcal VV, and the entries of WWW off V\mathcal VV. Stationarity becomes F(w∗;V∗)=0F(w^*;\mathcal V_*)=0F(w∗;V∗​)=0, where V∗\mathcal V_*V∗​ is the set of zero entries of Z∗Z^*Z∗ in columns of zero maximum.

SNSCO does not know V∗\mathcal V_*V∗​. At wℓw^\ellwℓ it selects Tℓ∈T(Λℓ;s)T_\ell\in\mathbb T(\Lambda^\ell;s)Tℓ​∈T(Λℓ;s) and Vℓ:=UTℓ={(m,n):n∈Tℓ, Λmnℓ≥0}\mathcal V_\ell:=U_{T_\ell}=\{(m,n):n\in T_\ell,\ \Lambda^\ell_{mn}\ge0\}Vℓ​:=UTℓ​​={(m,n):n∈Tℓ​, Λmnℓ​≥0}, takes an element HℓH^\ellHℓ of the Clarke generalized Jacobian of φ(⋅;Vℓ)\varphi(\cdot;\mathcal V_\ell)φ(⋅;Vℓ​), and solves a Newton system with a regularization block −μℓI-\mu_\ell I−μℓ​I. A backtracking test on ∥G∥0+≤(γ+1)s\|G\|_0^+\le(\gamma+1)s∥G∥0+​≤(γ+1)s fixes the step size.

Formalization targets

Goal: Theorem 5

Let x∗x^*x∗ be τ\tauτ-stationary with 0<τ<τ∗0<\tau<\tau_*0<τ<τ∗​, let Assumption 2 hold, and let γ≥∣Γ0∗∣/s\gamma\ge|\Gamma_0^*|/sγ≥∣Γ0∗​∣/s. Then there is η>0\eta>0η>0 such that every run of SNSCO with ∥w0−w∗∥<η\|w^0-w^*\|<\eta∥w0−w∗∥<η takes full Newton steps and satisfies

wℓ→w∗,∥wℓ+1−w∗∥=o(∥wℓ−w∗∥).w^\ell\to w^*,\qquad \|w^{\ell+1}-w^*\|=o(\|w^\ell-w^*\|).wℓ→w∗,∥wℓ+1−w∗∥=o(∥wℓ−w∗∥).

Under strong semismoothness of φ(⋅;V∗)\varphi(\cdot;\mathcal V_*)φ(⋅;V∗​) and of GmnG_{mn}Gmn​, (m,n)∈V∗(m,n)\in\mathcal V_*(m,n)∈V∗​, the bound improves to

∥wℓ+1−w∗∥≤C∥wℓ−w∗∥2.\|w^{\ell+1}-w^*\|\le C\|w^\ell-w^*\|^2 .∥wℓ+1−w∗∥≤C∥wℓ−w∗∥2.

Both clauses hold for every selection of TℓT_\ellTℓ​ and HℓH^\ellHℓ, with η\etaη and CCC chosen before the run.

Milestones

In proof order: the sign of Zs↓Z^\downarrow_sZs↓​ (9); the closed form of ΠS\Pi_{\mathcal S}ΠS​ (Proposition 1); column-wise complementarity (24); the fixed-point inclusion (Proposition 2); the stationary equations (Theorem 4); identification of the active set (Lemma 2); semismoothness of F(⋅;V)F(\cdot;\mathcal V)F(⋅;V) (Lemma 3); uniform regularity of the Newton matrix (Lemma 4); and the superlinear and quadratic one-step estimates, (85) and the last display of p.22.

Significance

The theorem gives a local rate for an algorithm that attacks the 0/1 constraint itself, with no surrogate and no integer variables. The projection and the stationary equations are reusable for any problem with a column-counting constraint, including support vector machines and one-bit compressed sensing, which the paper notes as special cases.

The paper proves the result, and this mission adds the machine-checked proof. Two corrections are also recorded in the statements. The sentence of Theorem 5 omits τ<τ∗\tau<\tau_*τ<τ∗​, without which it is false at τ=τ∗\tau=\tau_*τ=τ∗​. Lemmas 3 and 4 hold only for those V⊆V∗\mathcal V\subseteq\mathcal V_*V⊆V∗​ with WV‾∗=0W^*_{\overline{\mathcal V}}=0WV∗​=0. As far as known, no result with a varying index set is formalized: the proved nonsmooth Newton theorems on the platform (Qi and Sun 1993 and Qi 1993) fix one system.

Difficulty

The standard Newton argument bounds F(wℓ)−F(w∗)−Hℓ(wℓ−w∗)F(w^\ell)-F(w^*)-H^\ell(w^\ell-w^*)F(wℓ)−F(w∗)−Hℓ(wℓ−w∗) for one fixed map FFF. Here the map F(⋅;UTℓ)F(\cdot;U_{T_\ell})F(⋅;UTℓ​​) changes with the iterate, so that argument does not apply directly. It needs F(w∗;UTℓ)=0F(w^*;U_{T_\ell})=0F(w∗;UTℓ​​)=0 for whichever set the iterate selects, although UTℓU_{T_\ell}UTℓ​​ need not equal V∗\mathcal V_*V∗​. This identification is where τ<τ∗\tau<\tau_*τ<τ∗​ enters. Semismoothness is assumed only for φ(⋅;V∗)\varphi(\cdot;\mathcal V_*)φ(⋅;V∗​) and must transfer to each φ(⋅;V)\varphi(\cdot;\mathcal V)φ(⋅;V), which involves a Clarke Jacobian of a composition with a non-surjective linear map. The chain rule available there is weaker than the usual inclusion.

Formalization scope

Points live in EuclideanSpace ℝ (Fin K) and matrices in Matrix (Fin M) (Fin N) ℝ, with [NeZero M] so that columns have a maximum. The variable www lives in the Euclidean space on Fin K ⊕ (Fin M × Fin N), and FFF and ∇Fμ\nabla F_\mu∇Fμ​ are written on that index type, so no block permutation appears. The Clarke Jacobian is the platform's NonsmoothNewton.Shared.clarkeJac. Semismoothness is the paper's (10)–(11), not Qi and Sun's limit form. ΠΩ\Pi_\OmegaΠΩ​ is a function chosen by Classical.epsilon, and ΠS\Pi_{\mathcal S}ΠS​ is a set. The hypothesis τ<τ∗\tau<\tau_*τ<τ∗​ is BelowTauStar, with no division and with τ∗=+∞\tau_*=+\inftyτ∗​=+∞ when ∥Z∗∥0+<s\|Z^*\|_0^+<s∥Z∗∥0+​<s or W:Γ0∗∗=0W^*_{:\Gamma_0^*}=0W:Γ0∗​∗​=0. A run has no stopping test, and it is a predicate on sequences, so every selection is covered.

The goal must not be restated for the one-step map, with Lemma 2's conclusion assumed, or for fixed V=V∗\mathcal V=\mathcal V_*V=V∗​. A verification file shows that the run predicate and Assumption 2 are satisfiable on a concrete instance.

Needed infrastructure: the Clarke Jacobian of a Lipschitz map on Euclidean space (nonemptiness, local boundedness and closedness, partly available on the platform) and its behaviour under composition with a linear map. The results on ΠS\Pi_{\mathcal S}ΠS​ are elementary and self-contained. Contributions of general lemmas on Clarke Jacobians are welcome.

Selected references

  • S. Zhou, L. Pan, N. Xiu, G. Y. Li, A 0/1 Constrained Optimization Solving Sample Average Approximation for Chance Constrained Programming, arXiv:2210.11889v5, 2026. https://arxiv.org/abs/2210.11889v5
  • L. Qi, J. Sun, A nonsmooth version of Newton's method, Mathematical Programming 58, 1993. https://doi.org/10.1007/BF01581275
  • L. Qi, Convergence analysis of some algorithms for solving nonsmooth equations, Mathematics of Operations Research 18, 1993. https://doi.org/10.1287/moor.18.1.227
  • F. H. Clarke, Optimization and Nonsmooth Analysis, SIAM Classics in Applied Mathematics 5, 1990. https://doi.org/10.1137/1.9781611971309
16 thms2 active usersReviewed
🏆Completed
Number Theory·Captain: Yuxuan Xu

Every odd integer greater than 1 is a sum of at most 19 primesResearch Paper

Motivation

Writing an integer as a sum of primes is a basic question in additive number theory. A uniform bound asks for one number of summands that works for every integer in a stated class. The bound must cover the smallest eligible integers as well as arbitrarily large ones. The odd-prime-sum campaign records machine-checked values of this uniform bound for odd integers greater than one.

This entry records the value 191919. Its mathematical source is the odd-integer corollary of the result of Riesel and Vaughan, On sums of primes (1983). Their paper proves that every even natural number is a sum of at most eighteen primes, and obtains the nineteen-prime statement for integers greater than one. The present entry isolates the odd-integer conclusion required by the campaign. Stronger mathematical bounds are known, including Helfgott's ternary Goldbach theorem; the campaign concerns the availability of checked formal proofs.

Setting

A multiset is a finite collection that permits repetitions and does not distinguish order. If sss is a multiset of natural numbers, ∣s∣|s|∣s∣ counts its elements with multiplicity and ∑s\sum s∑s is their sum. A prime is a natural number greater than one with precisely its usual positive divisors. The prime 222 is permitted in the final representation. The auxiliary estimates also use odd primes, meaning primes different from 222.

The shared additive sets are

B={(p−3)/2:p is an odd prime},A=B+B.B=\{(p-3)/2:p\text{ is an odd prime}\},\qquad A=B+B.B={(p−3)/2:p is an odd prime},A=B+B.

The quotients in this definition are nonnegative integers. For a positive integer NNN, write A(N)A(N)A(N) for the number of elements of AAA in the interval [1,N][1,N][1,N]. A Schnirelmann density is the infimum of the ratios A(N)/NA(N)/NA(N)/N over positive NNN. The shared definitions fix this convention, including the treatment of zero separately from the counting interval.

Another auxiliary quantity, R(n)R(n)R(n), counts natural numbers s≤ns\le ns≤n that can be written as a sum of two odd primes. Logarithms in the estimates are natural logarithms. A fixed family Q\mathcal QQ consists of 800080008000 distinct odd primes, from 333 through 818178181781817. Its finite certificate uses an integer lookup function W^\widehat WW for rounded singular weights, with scale 100001000010000. The definition of that lookup function and its comparison with the original prime-factor weights are separate checked components.

Target

The main goal is the following uniform representation statement:

∀n∈N,n>1 and n odd⟹∃s,∣s∣≤19,∑s=n,every element of s is prime.\forall n\in\mathbb N,\quad n>1\ \text{and}\ n\text{ odd}\quad\Longrightarrow\quad \exists s,\quad |s|\le19,\quad \sum s=n,\quad\text{every element of }s\text{ is prime}.∀n∈N,n>1 and n odd⟹∃s,∣s∣≤19,∑s=n,every element of s is prime.

The number of summands is an upper bound. Repeated primes are allowed, and the statement includes n=3n=3n=3 and n=5n=5n=5.

The linked supporting statements include the explicit intermediate estimate

R(n)≥1001799n(26≤log⁡n≤260),R(n)\ge\frac{100}{1799}n\qquad(26\le\log n\le260),R(n)≥1799100​n(26≤logn≤260),

the same estimate for n≥exp⁡(260)n\ge\exp(260)n≥exp(260), and the small-range estimate

A(N)≥N/9(N≥1, log⁡(2N+6)≤26).A(N)\ge N/9\qquad(N\ge1,\ \log(2N+6)\le26).A(N)≥N/9(N≥1, log(2N+6)≤26).

The finite arithmetic milestone states

∑a∈Q∑b∈Qb<aW^ ⁣(a−b2)≤557349373474.\sum_{a\in\mathcal Q}\sum_{\substack{b\in\mathcal Q\\b<a}} \widehat W\!\left(\frac{a-b}{2}\right)\le557349373474.a∈Q∑​b∈Qb<a​∑​W(2a−b​)≤557349373474.

Each supporting node states its exact hypotheses and numerical range.

Significance

The mathematical nineteen-prime bound is due to Riesel and Vaughan. This entry supplies a checked formal derivation of its odd-integer corollary using the campaign's exact multiset statement. Its auxiliary thresholds and numerical constants are those displayed in the linked formal estimates; they are not presented as verbatim quotations of the paper's intermediate lemmas.

The formal development makes the analytic estimates, finite counting statements, lookup-table comparisons, and integer computations independently reusable. The certificate identifies the stored numerical data with the original finite sums. The final theorem therefore covers the entire stated domain, with the finite calculations and the uniform estimates in the same dependency chain. These components provide a verified baseline for subsequent entries with smaller values.

Difficulty

The main formalization difficulty is obtaining uniform coverage. An estimate valid only for sufficiently large integers leaves a separate obligation for every smaller eligible integer. Explicit cutoffs require compatible counting conventions and correctly included endpoints. Shifts between natural-number sets and real logarithmic estimates also introduce finite corrections that must be retained.

The numerical part has a different requirement: a stored table or a computed total must refer to precisely the same primes and weights as the mathematical statements. The fixed prime family, weight comparison, and finite-sum certificate address these identification obligations. Large arithmetic is represented by exact natural numbers and included in checked proof terms, so the result is independent of floating-point approximations or an asserted external computation.

Formalization scope

The goal uses natural numbers, ordinary primality, and finite multisets. It quantifies over every odd natural number greater than one, with no size cutoff in the conclusion. Auxiliary sets and counting functions use the shared Schnirelmann definitions. The prime-family and packed-integer definitions are referenced as existing declarations rather than replaced by alternative models.

The development targets Lean 4.33.14.33.14.33.1 and the campaign's Mathlib environment, commit 0df444a360eaa60ab8c11dca51a86af692955474. The goal and the supporting theorem references have accepted proofs, with their dependency paths and closed proof frontiers checked. Exact finite arithmetic uses kernel-checked natural-number operations. The stored integers, their identification with the original data, and the resulting sum bound are distinct theorem-level steps.

This proposal references the established goal and support nodes. The campaign-wide objective of reaching smaller values continues separately from the verification of the value recorded here. Contributions that strengthen the explicit estimates or provide independently checked later bounds can reuse the definitions and supporting results under their stated hypotheses.

Selected references

  • H. Riesel and R. C. Vaughan, On sums of primes, Arkiv för Matematik 21 (1983), 45–74. DOI.
  • H. A. Helfgott, The ternary Goldbach conjecture is true (2013). arXiv:1312.7748.
  • Lean community, Mathlib, campaign-pinned revision. Source.
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Control TheoryOperations ResearchPartial Differential Equations+2·Captain: iris

Robustness of Stochastic Optimal Control to Approximate Diffusion Models Under Several Cost Evaluation Criteria: Discounted-Optimal Policies of Approximate Models Are Asymptotically OptimalResearch Paper

Why the mismatch between model and system matters

Optimal controllers are computed from a model, and the model is at best an approximation of the system that the controller will drive. The coefficients may be estimated from data, regularized for computation, or replaced by simpler functions. The question of robustness is whether the loss caused by this mismatch vanishes as the model improves. Kara and Yüksel answered it for discrete-time Markov decision processes under a condition they call continuous convergence in the control (SIAM J. Control Optim. 2020; average cost: arXiv:2003.05769). Pradhan and Yüksel treat the continuous-time counterpart for non-degenerate controlled diffusions, under several cost criteria (arXiv:2205.05894v2). This mission formalizes the discounted case, which the later sections of that paper use as their template.

Controlled diffusions and discounted optimality

Let U\mathbb UU be a compact metric space of control actions and V=P(U)\mathrm V=\mathcal P(\mathbb U)V=P(U) the space of probability measures on it. Given a drift b:Rd×U→Rdb:\mathbb R^d\times\mathbb U\to\mathbb R^db:Rd×U→Rd and a diffusion matrix σ:Rd→Rd×d\sigma:\mathbb R^d\to\mathbb R^{d\times d}σ:Rd→Rd×d, the state solves

dXt=b(Xt,Ut) dt+σ(Xt) dWt,X0=x,\mathrm dX_t=b(X_t,U_t)\,\mathrm dt+\sigma(X_t)\,\mathrm dW_t,\qquad X_0=x,dXt​=b(Xt​,Ut​)dt+σ(Xt​)dWt​,X0​=x,

where WWW is a ddd-dimensional standard Wiener process, UUU is a V\mathrm VV-valued process, and b(x,v)=∫Ub(x,ζ) v(dζ)b(x,\mathrm v)=\int_{\mathbb U}b(x,\zeta)\,\mathrm v(\mathrm d\zeta)b(x,v)=∫U​b(x,ζ)v(dζ). The process UUU is an admissible control if the increments of WWW after time sss are independent of the completion of σ(X0,Ur,Wr:r≤s)\sigma(X_0,U_r,W_r:r\le s)σ(X0​,Ur​,Wr​:r≤s). A stationary Markov control is a Borel map v:Rd→Vv:\mathbb R^d\to\mathrm Vv:Rd→V, used as Ut=v(Xt)U_t=v(X_t)Ut​=v(Xt​); these form the set Usm\mathfrak U_{\mathsf{sm}}Usm​.

For a bounded running cost c≥0c\ge0c≥0 and α>0\alpha>0α>0, the discounted cost and the optimal value are

JαU(x,c)=ExU[∫0∞e−αsc(Xs,Us) ds],Vα(x)=inf⁡UJαU(x,c).\mathcal J^U_\alpha(x,c)=\mathbb E^U_x\left[\int_0^\infty e^{-\alpha s}c(X_s,U_s)\,\mathrm ds\right],\qquad V_\alpha(x)=\inf_{U}\mathcal J^U_\alpha(x,c).JαU​(x,c)=ExU​[∫0∞​e−αsc(Xs​,Us​)ds],Vα​(x)=Uinf​JαU​(x,c).

An approximating model (bn,σn,cn)(b_n,\sigma_n,c_n)(bn​,σn​,cn​) has its own optimal value VαnV^n_\alphaVαn​. It converges to (b,σ,c)(b,\sigma,c)(b,σ,c) if σn→σ\sigma_n\to\sigmaσn​→σ almost everywhere and if, for almost every xxx, ζn→ζ\zeta_n\to\zetaζn​→ζ implies cn(x,ζn)→c(x,ζ)c_n(x,\zeta_n)\to c(x,\zeta)cn​(x,ζn​)→c(x,ζ) and bn(x,ζn)→b(x,ζ)b_n(x,\zeta_n)\to b(x,\zeta)bn​(x,ζn​)→b(x,ζ). This last condition is continuous convergence in controls.

Formalization targets

Goal: robustness of optimal policies

Under assumptions (A1)–(A5), if vn∗∈Usmv^*_n\in\mathfrak U_{\mathsf{sm}}vn∗​∈Usm​ is optimal for the model (bn,σn,cn)(b_n,\sigma_n,c_n)(bn​,σn​,cn​) and v∗v^*v∗ for the true model, then for all x∈Rdx\in\mathbb R^dx∈Rd

lim⁡n→∞Jαvn∗(x,c)=Jαv∗(x,c).\lim_{n\to\infty}\mathcal J^{v^*_n}_\alpha(x,c)=\mathcal J^{v^*}_\alpha(x,c).n→∞lim​Jαvn∗​​(x,c)=Jαv∗​(x,c).

The left side runs vn∗v^*_nvn∗​ on the true dynamics with the true cost. The statement quantifies over every choice of optimal controls and every initial state, and the value is an infimum over all admissible controls.

Milestones

Vαn(x)→Vα(x)for all x(Theorem 3.3)V^n_\alpha(x)\to V_\alpha(x)\quad\text{for all }x\qquad\text{(Theorem 3.3)}Vαn​(x)→Vα​(x)for all x(Theorem 3.3)

The milestones also include: well-posedness of (2.1) under every admissible control, and well-posedness and the strong Feller property under Usm\mathfrak U_{\mathsf{sm}}Usm​; compact metrizability of Usm\mathfrak U_{\mathsf{sm}}Usm​; the characterization of VαV_\alphaVα​ and of optimal controls by the HJB equation (Theorems 3.1 and 3.2); continuity of the cost in the policy (Remark 3.2); and optimality of limits of optimal controls.

What the result gives

The result. Theorem 3.3 alone says the optimal value is continuous in the model. Theorem 3.4 is stronger in content: it concerns the policy, which is what is actually deployed. A controller who solves an approximate problem suffers no asymptotic loss on the true system, without any quantitative knowledge of the error. The assumptions allow functional perturbations of the coefficients and uncountable action spaces.

The formalization. The theorems are proved in the paper, partly by citing Arapostathis, Borkar and Ghosh. A search of the platform found no formalization of them. A complete development would add the discounted HJB characterization for non-degenerate diffusions, the compact space of stationary Markov controls, and its topology. The published EthierKurtz SDE definitions supply the Brownian motion, the Itô integral and the strong solution predicate.

Where the difficulty lies

The obvious argument couples the two state processes through the same Wiener process and compares paths. It fails here: a stationary Markov control is merely measurable, so the closed-loop drift has no regularity in xxx, and neither it nor the convergence of σn\sigma_nσn​ gives a stable pathwise estimate. Moreover, the optimal policies vn∗v^*_nvn∗​ need not converge in any pointwise sense; they have limits only in a weak topology, in which products with gradients are delicate. The limit of vn∗v^*_nvn∗​ must be identified as optimal for a model that none of the vn∗v^*_nvn∗​ was designed for. Each of these steps also needs elliptic regularity that uniform ellipticity and uniform moduli of continuity have to supply.

Formalization scope

Rd\mathbb R^dRd is EthierKurtz.SDEState d; a d×dd\times dd×d matrix is an element of EthierKurtz.SDEDiffusion d, so its norm is Tr(σσT)\sqrt{\mathrm{Tr}(\sigma\sigma^{\mathsf T})}Tr(σσT)​. V\mathrm VV is ProbabilityMeasure U. All models live on one probability space with one Brownian motion, whose completeness is not assumed; the filtrations join the null sets explicitly. An admissible control is jointly measurable. The value is a real sInf over admissible pairs, a nonempty set bounded below. The optimality predicate requires a solution from every xxx, so a policy with no solutions is not optimal.

Two hypotheses are corrected, and each correction is declared on the items that use it. Read literally, (A5)(iii) makes Theorem 3.3 false, and (A5)(ii) makes Theorems 3.3 and 3.4 false:

  1. (A5)(iii) has constants uniform in nnn. The constants CRC_RCR​ and C0C_0C0​ of (A1)–(A3) are common to all models. Otherwise a vanishing σn\sigma_nσn​ near a point yields a sticky limit diffusion.
  2. (A5)(ii) has one null set. The exceptional set does not depend on the sequence ζn\zeta_nζn​. Otherwise bump functions in ζ\zetaζ moving with xxx defeat both theorems.

Also, cnc_ncn​ is real valued, not Rd\mathbb R^dRd-valued as printed, and it need not be nonnegative.

Mathlib has no Itô integral, no Sobolev spaces and no LpL^pLp elliptic theory. A proof needs Itô–Krylov-type calculus, interior W2,pW^{2,p}W2,p estimates and compact Sobolev embeddings, and these are reusable well beyond this mission. No statement of the mission mentions a Sobolev space. Contributions are welcome at every milestone, and also on those substrate results.

Selected references

  • S. Pradhan and S. Yüksel, Robustness of Stochastic Optimal Control to Approximate Diffusion Models Under Several Cost Evaluation Criteria, arXiv:2205.05894v2, 2023. https://arxiv.org/abs/2205.05894
  • A. Arapostathis, V. S. Borkar and M. K. Ghosh, Ergodic Control of Diffusion Processes, Cambridge University Press, 2012. https://mathscinet.ams.org/mathscinet-getitem?mr=2884272
  • A. D. Kara and S. Yüksel, Robustness to Incorrect System Models in Stochastic Control, SIAM J. Control Optim. 58 (2020), 1144–1182. https://doi.org/10.1137/18m1208058
  • A. D. Kara, M. Raginsky and S. Yüksel, Robustness to Incorrect Models and Data-Driven Learning in Average-Cost Optimal Stochastic Control, arXiv:2003.05769, 2020. https://arxiv.org/abs/2003.05769
  • S. Pradhan and S. Yüksel, Continuity of Cost in Borkar Control Topology and Implications on Discrete Space and Time Approximations for Controlled Diffusions Under Several Criteria, arXiv:2209.14982, 2022. https://arxiv.org/abs/2209.14982
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Markov ChainProbabilityStochastic Systems·Captain: iris

Polynomial Voting Rules: Under Poly(α), Shares Form a Martingale Converging to Dirichlet at Wasserstein Rate t^(−1/(1+α)); Voting Powers Form a Supermartingale Decaying Like t^(−α/(1+α))Research Paper

Why polynomial voting rules

In a proof-of-stake blockchain, the participants who validate transactions are selected in proportion to the stakes they hold, and each round of validation pays a reward in new stakes. Roşu and Saleh (Manag. Sci. 2021) and Tang (arXiv:2206.02227) analysed this mechanism as a Pólya urn: the reward is issued in every round, so the total stake grows linearly in time. In the protocols of Bitcoin and Ethereum the volume of stakes grows sublinearly, and security arguments ask that no bidder keep a large probability of being selected.

Tang and Yao (arXiv:2206.10105) propose a family of rules that slows the issuance. A rule with parameter α≥0\alpha\ge0α≥0 scales each bidder's selection probability by Nt−αN_t^{-\alpha}Nt−α​, where NtN_tNt​ is the current total stake, and α=0\alpha=0α=0 is the Pólya urn. The question is what this does to the distribution of wealth among bidders and to the voting power of each bidder as time grows.

The Poly(α\alphaα) model

There are KKK bidders with initial stakes n1,0,…,nK,0n_{1,0},\dots,n_{K,0}n1,0​,…,nK,0​, and N=∑knk,0≥1N=\sum_k n_{k,0}\ge1N=∑k​nk,0​≥1. Time is discrete. Write nk,tn_{k,t}nk,t​ for the stakes of bidder kkk at time ttt, Nt=∑knk,tN_t=\sum_k n_{k,t}Nt​=∑k​nk,t​ for the volume, πk,t=nk,t/Nt\pi_{k,t}=n_{k,t}/N_tπk,t​=nk,t​/Nt​ for the bidder share, and

θk,t=nk,tNt1+α=πk,tNtα\theta_{k,t}=\frac{n_{k,t}}{N_t^{1+\alpha}}=\frac{\pi_{k,t}}{N_t^\alpha}θk,t​=Nt1+α​nk,t​​=Ntα​πk,t​​

for the voting power. In each period a single stake is offered: given the past Ft\mathcal F_tFt​, bidder kkk receives it with probability θk,t\theta_{k,t}θk,t​, and nobody receives it with probability 1−Nt−α1-N_t^{-\alpha}1−Nt−α​. The Dirichlet distribution Dir(a1,…,aK)\mathrm{Dir}(a_1,\dots,a_K)Dir(a1​,…,aK​) is the law on the simplex with density proportional to ∏kxkak−1\prod_k x_k^{a_k-1}∏k​xkak​−1​, and dWd_WdW​ is the 1-Wasserstein distance.

Formalization targets

Goal: Theorem 6 (long-time behavior)

For every KKK, every initial stake vector and every real α≥0\alpha\ge0α≥0, the share process (πk,t)(\pi_{k,t})(πk,t​) is an Ft\mathcal F_tFt​-martingale, and almost surely

(π1,t,…,πK,t)→(π1,∞,…,πK,∞)=dDir(n1,0,…,nK,0),(\pi_{1,t},\dots,\pi_{K,t})\to(\pi_{1,\infty},\dots,\pi_{K,\infty})\overset d=\mathrm{Dir}(n_{1,0},\dots,n_{K,0}),(π1,t​,…,πK,t​)→(π1,∞​,…,πK,∞​)=dDir(n1,0​,…,nK,0​), dW(πk,t,Beta(nk,0,N−nk,0))=O(t−11+α).d_W\big(\pi_{k,t},\mathrm{Beta}(n_{k,0},N-n_{k,0})\big)=O\big(t^{-\frac1{1+\alpha}}\big).dW​(πk,t​,Beta(nk,0​,N−nk,0​))=O(t−1+α1​).

The voting power (θk,t)(\theta_{k,t})(θk,t​) is an Ft\mathcal F_tFt​-supermartingale, for α>0\alpha>0α>0 it tends to 000 almost surely, and

(1+α)α1+α tα1+α θk,t⟶dBeta(nk,0,N−nk,0).(1+\alpha)^{\frac\alpha{1+\alpha}}\,t^{\frac\alpha{1+\alpha}}\,\theta_{k,t}\overset d\longrightarrow\mathrm{Beta}(n_{k,0},N-n_{k,0}).(1+α)1+αα​t1+αα​θk,t​⟶d​Beta(nk,0​,N−nk,0​).

Milestones

The milestones follow the paper's argument, from the weakest ingredient to the goal: the time-changed urn representation (Proposition 1); divergence of NtN_tNt​; the law of large numbers Nt1+α/t→1+αN_t^{1+\alpha}/t\to1+\alphaNt1+α​/t→1+α in probability (Proposition 2 (ii)); the lower-tail large deviation bound (Theorem 3 (i)); the Beta marginals of a Dirichlet law; the one-step identity (2.18); the Dirichlet limit of the Pólya urn; the Goldstein–Reinert rate (2.19); the conditional law of the stakes given Nt=sN_t=sNt​=s; and the one-step identity for θk,t\theta_{k,t}θk,t​.

Significance

Theorem 6 separates what the rule changes from what it preserves. The limit of the shares, and hence the level of decentralization, does not depend on α\alphaα; the speed of convergence and the decay of voting power do. The bound t−1/(1+α)t^{-1/(1+\alpha)}t−1/(1+α) is stated in the paper to be sharp. The decay of θk,t\theta_{k,t}θk,t​ is the security gain of the rule, since no bidder retains a non-vanishing chance of being selected.

The theorem is proved in the paper. No machine-checked proof of it is known. A formalization delivers more than this statement: the Pólya urn with its Dirichlet limit, in full generality of initial composition, is not on the platform or in Mathlib, and the Goldstein–Reinert bound is a nontrivial Stein's-method result. The published mission on the Roşu–Saleh model treats a different chain, with one tracked investor and deterministic rewards.

Difficulty

The first clause is a one-line computation, and the martingale convergence theorem gives the existence of the limit. The substance lies elsewhere.

Identifying the limit requires the embedding of the urn: the colour of each award is independent of the award times. A direct calculation with the one-step law does not give this, because the time change LtL_tLt​ is random and the statement is one about laws of whole paths.

The rate (2.16) cannot be obtained from the martingale structure. It needs the conditional law given Nt=sN_t=sNt​=s, the urn rate (2.19), and a tail bound for NtN_tNt​ at the scale t1/(1+α)t^{1/(1+\alpha)}t1/(1+α), where the exponential tail must beat the polynomial rate.

Divergence of NtN_tNt​ is not a Borel–Cantelli consequence of a deterministic lower bound on the award probability: for α>1\alpha>1α>1 the sum ∑t(N+t)−α\sum_t(N+t)^{-\alpha}∑t​(N+t)−α converges. The argument has to use that each holding time is finite. Convergence (2.7) requires moment asymptotics for a Markov chain whose increments depend on its state.

Formalization scope

The chain is PolyVoting.Model μ K α n₀, a structure on a probability space. It carries a stake process n : ℕ → Ω → Fin K → ℕ, adapted to a filtration ℱ, with n 0 = n₀, and the joint conditional one-step law: Model holds for any filtration satisfying the law, the natural filtration among them. α is real and 0 ≤ α, with Real.rpow throughout, and 1 ≤ ∑ k, n₀ k. The Pólya urn is Model μ K 0 n₀, with no second definition. Derived quantities are M.total, M.share and M.power.

d_W is the published WassersteinDRO.Duality.wassersteinDistance 1 on ℝ, valued in ℝ≥0∞, and rates are compared in ℝ≥0∞, so an infinite distance cannot satisfy the bound. dirichletMeasure is the pushforward of a density on the first K - 1 coordinates. betaMeasure is Mathlib's.

Clauses naming a limit law are guarded exactly where the law would be undefined: every n₀ j ≥ 1 for Dir, and 1 ≤ n₀ k < N for Beta. The martingale, supermartingale and almost sure clauses are unguarded. A guard placed on them would narrow the theorem, and dropping a guard on a Beta clause would make it false rather than trivial, since Mathlib's betaMeasure a 0 is the zero measure.

A complete development needs a reusable theory of the Pólya urn (exchangeability or moments, the Dirichlet limit, the Stein bound), discrete-time random time change for Markov chains, and moment asymptotics. Those parts are useful beyond this mission, and contributions to any of them are welcome.

Selected references

  • W. Tang and D. D. Yao, Polynomial Voting Rules, arXiv:2206.10105v5, 2024. https://arxiv.org/abs/2206.10105
  • I. Roşu and F. Saleh, Evolution of shares in a proof-of-stake cryptocurrency, Manag. Sci. 67(2):661–672, 2021. https://doi.org/10.1287/mnsc.2020.3791
  • W. Tang, Stability of shares in the Proof of Stake protocol – concentration and phase transitions, 2022. https://arxiv.org/abs/2206.02227
  • L. Goldstein and G. Reinert, Stein's method for the beta distribution and the Pólya-Eggenberger urn, J. Appl. Probab. 50(4):1187–1205, 2013. https://doi.org/10.1239/jap/1389370107
  • C. Villani, Optimal transport: old and new, Springer, 2009. https://doi.org/10.1007/978-3-540-71050-9
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CombinatoricsOperations ResearchOptimization·Captain: iris

A Test Score-Based Approach to Stochastic Submodular Optimization: Selecting the Top k Items by Replication Test Score Gives a (1 − 1/e)/(5 − 1/e)-Approximation Under Extended Diminishing ReturnsResearch Paper

Motivation

Many selection problems ask for a team of kkk items out of nnn candidates whose individual performances are random and whose joint value is not additive: a team of contributors where only the best submission counts, a slate of content topics where a user clicks if at least one topic appeals, a portfolio of research projects where the strongest result dominates. The natural model is stochastic submodular maximization: choose SSS with ∣S∣=k|S|=k∣S∣=k to maximize u(S)=E[g(MS(X))]u(S)=\mathbb E[g(M_S(X))]u(S)=E[g(MS​(X))], where XiX_iXi​ is the random performance of item iii and ggg is a monotone submodular value function of the performance vector (Asadpour and Nazerzadeh, Maximizing stochastic monotone submodular functions, Management Science 2016). The problem is NP-hard even for g=min⁡g=\ming=min (Goel, Guha and Munagala, PODS 2006, as cited on p.12 of arXiv:1605.07172v4).

Greedy and continuous-relaxation methods need to evaluate uuu on many candidate sets, each evaluation being an expectation over a joint distribution. In practice a platform often wants something simpler: a test score aia_iai​ per item, computed from that item's own distribution only, followed by picking the kkk items with the highest scores. Sekar, Vojnovic and Yun (arXiv:1605.07172, Management Science 2021) ask which scores make this trivial algorithm a constant-factor approximation. Mean scores and quantile scores can fail badly (the paper's Example 1 and Propositions 1–2). The paper's answer is the replication test score: the expected value of a virtual team made of kkk independent copies of item iii.

Setting

Items are N={1,…,n}N=\{1,\dots,n\}N={1,…,n}, the cardinality is 0<k≤n0<k\le n0<k≤n, and item iii has a nonnegative random performance Xi∼PiX_i\sim P_iXi​∼Pi​; the XiX_iXi​ are independent and not necessarily identically distributed. A value function g:R+n→R+g:\mathbb R_+^n\to\mathbb R_+g:R+n​→R+​ is

  • monotone if x≤yx\le yx≤y componentwise implies g(x)≤g(y)g(x)\le g(y)g(x)≤g(y);
  • submodular if g(x∨y)+g(x∧y)≤g(x)+g(y)g(x\vee y)+g(x\wedge y)\le g(x)+g(y)g(x∨y)+g(x∧y)≤g(x)+g(y) (eq. (3));
  • symmetric if g(x∘σ)=g(x)g(x\circ\sigma)=g(x)g(x∘σ)=g(x) for every permutation σ\sigmaσ of the coordinates.

For S⊆NS\subseteq NS⊆N, MS(x)M_S(x)MS​(x) keeps the coordinates in SSS and sets the others to 000; the utility is u(S)=E[g(MS(X))]u(S)=\mathbb E[g(M_S(X))]u(S)=E[g(MS​(X))] (eq. (4)). The replication test score of item iii is

ai=E[g(Xi(1),…,Xi(k),0,…,0)],a_i=\mathbb E\bigl[g(X_i^{(1)},\dots,X_i^{(k)},0,\dots,0)\bigr],ai​=E[g(Xi(1)​,…,Xi(k)​,0,…,0)],

with Xi(1),…,Xi(k)X_i^{(1)},\dots,X_i^{(k)}Xi(1)​,…,Xi(k)​ independent copies of XiX_iXi​ (Definition 2).

Writing g(z,x)g(z,x)g(z,x) for ggg at z∈R+n−1z\in\mathbb R_+^{n-1}z∈R+n−1​ extended by one coordinate xxx, and g(z)=g(z,0)g(z)=g(z,0)g(z)=g(z,0), the function ggg has extended diminishing returns (Definition 1) if every value vvv of ggg is taken at some zzz such that g(z,x)−g(z)≤g(y,x)−g(y)g(z,x)-g(z)\le g(y,x)-g(y)g(z,x)−g(z)≤g(y,x)−g(y) for all x≥0x\ge0x≥0 and all yyy with g(y)≤vg(y)\le vg(y)≤v: a new item helps a group worth vvv no more than it helps any group worth less. Sums of concave functions of the total, the maximum, CES functions, success probabilities and top-rrr sums all have it (Appendix A).

A pair of set functions (v‾,vˉ)(\underline v,\bar v)(v​,vˉ) is a (p,q)(p,q)(p,q)-sketch of uuu if p v‾≤u≤q vˉp\,\underline v\le u\le q\,\bar vpv​≤u≤qvˉ; scores are (p,q)(p,q)(p,q)-good if (min⁡i∈Sai,max⁡i∈Sai)(\min_{i\in S}a_i,\max_{i\in S}a_i)(mini∈S​ai​,maxi∈S​ai​) is a (p,q)(p,q)(p,q)-sketch.

Formalization targets

Goal: Theorem 1

For every top-kkk set SSS of the replication scores (any tie-breaking) and every TTT with ∣T∣=k|T|=k∣T∣=k,

u(S)≥1−1/e5−1/e u(T).u(S)\ge\frac{1-1/e}{5-1/e}\,u(T).u(S)≥5−1/e1−1/e​u(T).

The constant is the paper's; no family of ggg on growing dimension, no continuity and no relation between nnn and kkk beyond k≤nk\le nk≤n is assumed.

Milestones

  1. Lemma 1: uuu is monotone submodular.
  2. Lemma 2 and Corollary 1: (p,q)(p,q)(p,q)-good scores make top-kkk selection a p/(p+q)p/(p+q)p/(p+q)-approximation,
u(S)≥pp+q u(T).u(S)\ge\frac{p}{p+q}\,u(T).u(S)≥p+qp​u(T).
  1. Lemma 4, lower half: inequality (18), u(A∪{i})≥(1−1k)u(A)+1kaiu(A\cup\{i\})\ge(1-\tfrac1k)u(A)+\tfrac1k a_iu(A∪{i})≥(1−k1​)u(A)+k1​ai​, and its cascade u(S)≥(1−1/e)min⁡i∈Saiu(S)\ge(1-1/e)\min_{i\in S}a_iu(S)≥(1−1/e)mini∈S​ai​ for ∣S∣=k|S|=k∣S∣=k.
  2. Lemma 4, upper half: the overlay bound (22)–(23), the chain (25)–(29), inequality (c) and the Markov step, giving u(S)≤4max⁡i∈Saiu(S)\le4\max_{i\in S}a_iu(S)≤4maxi∈S​ai​ for 0<∣S∣≤k0<|S|\le k0<∣S∣≤k.
  3. Lemma 4 itself: replication scores are (1−1/e,4)(1-1/e,4)(1−1/e,4)-good. Theorem 1 is Corollary 1 with p=1−1/ep=1-1/ep=1−1/e, q=4q=4q=4.

Significance

The theorem shows that for a broad class of symmetric value functions a score computed from one item's distribution in isolation, without any joint evaluation, gives a constant-factor guarantee. Replication scores can be estimated by showing kkk copies of an item to users and averaging, so the guarantee covers algorithms that a platform can run without knowing ggg or the PiP_iPi​. The sketch framework of Lemma 2 and Corollary 1 is independent of the stochastic setting and applies to any submodular set function with a minorant and majorant of this form. The paper's welfare-maximization result (Theorem 2) extends the same approach and is not part of this mission.

The result is proved in the paper; no machine-checked proof of it or of the sketch lemma exists on the platform. Formalizing it also repairs the printed argument. The printed proof evaluates ggg on up to n−1+kn-1+kn−1+k coordinates (footnote 6 concedes the abuse) and assumes ggg continuous with an attained maximum, which neither the theorem nor the examples of §2.3 (step success probabilities) provide. Lemma 2 is false as printed when n<2kn<2kn<2k or when uuu is not monotone, and Definition 3's "for all S⊆NS\subseteq NS⊆N" makes Lemma 4 false at sizes other than kkk. The mission states the corrected lemmas, with counterexamples recorded in the items.

Difficulty

The obvious proof of the upper bound adds the n−1n-1n−1 "fictitious" items of a vector zzz with g(z)≈c akg(z)\approx c\,a_kg(z)≈cak​ to SSS and bounds each marginal by a replica marginal. With ggg defined on exactly nnn coordinates, S∗∪SS^*\cup SS∗∪S does not fit, so (22)–(23) must be replaced by an inequality that stays inside nnn coordinates; symmetry of ggg is what makes this possible. The choice of zzz uses extended diminishing returns at a value v≤2akv\le 2a_kv≤2ak​ that must be attained on k−1k-1k−1 coordinates; without continuity such a vvv need not equal min⁡{2ak,gk−1max⁡}\min\{2a_k,g^{\max}_{k-1}\}min{2ak​,gk−1max​}, and gk−1max⁡g^{\max}_{k-1}gk−1max​ need not be attained (for g(x)=1−e−∑xig(x)=1-e^{-\sum x_i}g(x)=1−e−∑xi​ it is not). The lower bound (18) at j>1j>1j>1 likewise compares j−1j-1j−1 items plus kkk replicas, up to 2k−12k-12k−1 coordinates. The measure-theoretic side (product measures, conditioning on g(Yi)≤g(z)g(Y_i)\le g(z)g(Yi​)≤g(z), Fubini over replicas) is routine but must be carried out with the integrability that the replication scores alone provide.

Formalization scope

Items are Fin (m + 1) with n=m+1n=m+1n=m+1; performances are ℝ≥0; the laws PiP_iPi​ are probability measures on ℝ≥0 and independence is Measure.pi P. The padding element φ\varphiφ is 000. Expectations are Bochner integrals, so ggg is assumed measurable and the kkk-fold replica g(Xi(1),…,Xi(k),0,…,0)g(X_i^{(1)},\dots,X_i^{(k)},0,\dots,0)g(Xi(1)​,…,Xi(k)​,0,…,0) integrable for each iii; the integrability of every u(S)u(S)u(S) is derived, not assumed. Extended diminishing returns is stated with the value vvv attained on R+n−1\mathbb R_+^{n-1}R+n−1​, which the printed definition implies. A top-kkk set is any SSS with ∣S∣=k|S|=k∣S∣=k and aj≤aia_j\le a_iaj​≤ai​ for i∈Si\in Si∈S, j∉Sj\notin Sj∈/S, so no tie-breaking rule is fixed. (p,q)(p,q)(p,q)-good scores require the lower sketch bound at ∣S∣=k|S|=k∣S∣=k and the upper one at 0<∣S∣≤k0<|S|\le k0<∣S∣≤k.

The statement is not trivialized by an empty instance: the hypotheses hold for g=∑ixig=\sum_i x_ig=∑i​xi​ and g=max⁡ixig=\max_i x_ig=maxi​xi​ at every nnn, and at n=3n=3n=3, k=2k=2k=2, g=max⁡g=\maxg=max with P1=P2=δ1P_1=P_2=\delta_1P1​=P2​=δ1​, P3=0.8 δ0+0.2 δ2P_3=0.8\,\delta_0+0.2\,\delta_2P3​=0.8δ0​+0.2δ2​ the top-2 set has utility 111 while another pair has 1.21.21.2.

The development needs product measures over replicas, conditioning by independence, and a monotone-submodular calculus for set functions; the sketch lemma and the overlay inequality are reusable for other test-score results. Proofs of any milestone, alternative arguments for the upper bound, and better constants are welcome.

Selected references

  • S. Sekar, M. Vojnovic, S.-Y. Yun, A Test Score Based Approach to Stochastic Submodular Optimization, Management Science, 2021; arXiv:1605.07172v4 (2019). https://arxiv.org/abs/1605.07172
  • A. Asadpour, H. Nazerzadeh, Maximizing Stochastic Monotone Submodular Functions, Management Science 62(8), 2016. https://doi.org/10.1287/mnsc.2015.2254
  • A. Goel, S. Guha, K. Munagala, Asking the Right Questions: Model-Driven Optimization Using Probes, PODS 2006, pp. 203–212.
  • G. L. Nemhauser, L. A. Wolsey, M. L. Fisher, An Analysis of Approximations for Maximizing Submodular Set Functions—I, Mathematical Programming 14, 1978. https://doi.org/10.1007/BF01588971
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Scalable Reinforcement Learning for Multi-Agent Networked Systems: High-Probability Stationarity Bound for Scalable Actor Critic with κ\kappaκ-Hop Truncated Q-FunctionsResearch Paper

Motivation

Many control problems are posed on networks of agents that each see only a local state and take a local action: traffic signals at intersections, wireless transmitters sharing a channel, nodes of an epidemic or a power grid. Treated as one Markov decision process, such a system has a state space whose size is exponential in the number of agents nnn, so tabular reinforcement learning, and even storing a single Q-function, is out of reach. Qu, Wierman and Li (arXiv:1912.02906; Operations Research, 2022) exploit the network structure: if the next local state depends only on the neighbours' states, then the influence of far-away agents on an agent's Q-function decays with graph distance, and each agent can learn with tables indexed only by its κ-hop neighbourhood. Their algorithm, Scalable Actor Critic (SAC), comes with a non-asymptotic guarantee: it finds an approximate stationary point of the global objective with an error that decays exponentially in κ\kappaκ.

Setting

There are nnn agents N={1,…,n}\mathcal N=\{1,\dots,n\}N={1,…,n} on an undirected graph GGG. For κ≥0\kappa\ge0κ≥0 the κ-hop neighbourhood NiκN_i^\kappaNiκ​ is the set of agents at graph distance at most κ\kappaκ from iii, Ni=Ni1N_i=N_i^1Ni​=Ni1​, and f(κ)=max⁡i∣Niκ∣f(\kappa)=\max_i|N_i^\kappa|f(κ)=maxi​∣Niκ​∣. Agent iii has finite local state and action sets Si\mathcal S_iSi​, Ai\mathcal A_iAi​; global states and actions are tuples s∈S=∏iSis\in\mathcal S=\prod_i\mathcal S_is∈S=∏i​Si​, a∈A=∏iAia\in\mathcal A=\prod_i\mathcal A_ia∈A=∏i​Ai​. Transitions factorize,

P(s(t+1)∣s(t),a(t))=∏i=1nP(si(t+1)∣sNi(t),ai(t)),P(s(t+1)\mid s(t),a(t))=\prod_{i=1}^nP\big(s_i(t+1)\mid s_{N_i}(t),a_i(t)\big),P(s(t+1)∣s(t),a(t))=i=1∏n​P(si​(t+1)∣sNi​​(t),ai​(t)),

agent iii earns ri(si,ai)r_i(s_i,a_i)ri​(si​,ai​), the global reward is r=1n∑irir=\frac1n\sum_ir_ir=n1​∑i​ri​, s(0)∼π0s(0)\sim\pi_0s(0)∼π0​ and γ∈(0,1)\gamma\in(0,1)γ∈(0,1) is the discount factor.

A localized policy gives agent iii a parameter θi∈Rdi\theta_i\in\mathbb R^{d_i}θi​∈Rdi​ and a law ζiθi(⋅∣si)\zeta_i^{\theta_i}(\cdot\mid s_i)ζiθi​​(⋅∣si​) on Ai\mathcal A_iAi​; agents act independently, ζθ(a∣s)=∏iζiθi(ai∣si)\zeta^\theta(a\mid s)=\prod_i\zeta_i^{\theta_i}(a_i\mid s_i)ζθ(a∣s)=∏i​ζiθi​​(ai​∣si​). The objective is J(θ)=Es∼π0E[∑t≥0γtr(s(t),a(t))∣s(0)=s]J(\theta)=\mathbb E_{s\sim\pi_0}\mathbb E[\sum_{t\ge0}\gamma^tr(s(t),a(t))\mid s(0)=s]J(θ)=Es∼π0​​E[∑t≥0​γtr(s(t),a(t))∣s(0)=s], and Qiθ(s,a)Q_i^\theta(s,a)Qiθ​(s,a) is the discounted sum of agent iii's rewards started from (s,a)(s,a)(s,a).

The (c,ρ)(c,\rho)(c,ρ)-exponential decay property holds when, for every policy θ\thetaθ and agent iii, ∣Qiθ(z)−Qiθ(z′)∣≤cρκ+1|Q_i^\theta(z)-Q_i^\theta(z')|\le c\rho^{\kappa+1}∣Qiθ​(z)−Qiθ​(z′)∣≤cρκ+1 whenever z=(s,a)z=(s,a)z=(s,a) and z′z'z′ agree on NiκN_i^\kappaNiκ​. Then a truncated Q-function, a weighted average of QiθQ_i^\thetaQiθ​ over the coordinates outside NiκN_i^\kappaNiκ​, is a table on ZNiκ=SNiκ×ANiκ\mathcal Z_{N_i^\kappa}=\mathcal S_{N_i^\kappa}\times\mathcal A_{N_i^\kappa}ZNiκ​​=SNiκ​​×ANiκ​​ within cρκ+1c\rho^{\kappa+1}cρκ+1 of QiθQ_i^\thetaQiθ​.

SAC (Algorithm 1) repeats, for m=0,1,…m=0,1,\dotsm=0,1,…: draw an episode z(0),…,z(T)z(0),\dots,z(T)z(0),…,z(T) under θ(m)\theta(m)θ(m); each agent runs temporal-difference learning with step αt=h/(t+t0)\alpha_t=h/(t+t_0)αt​=h/(t+t0​) on its local pairs zNiκ(t)z_{N_i^\kappa}(t)zNiκ​​(t), producing a table Q^iT\hat Q^T_iQ^​iT​; then each agent forms g^i(m)=∑t=0Tγt1n∑j∈NiκQ^jT(zNjκ(t))∇θilog⁡ζiθi(m)(ai(t)∣si(t))\hat g_i(m)=\sum_{t=0}^T\gamma^t\frac1n\sum_{j\in N_i^\kappa}\hat Q^T_j(z_{N_j^\kappa}(t))\nabla_{\theta_i}\log\zeta_i^{\theta_i(m)}(a_i(t)\mid s_i(t))g^​i​(m)=∑t=0T​γtn1​∑j∈Niκ​​Q^​jT​(zNjκ​​(t))∇θi​​logζiθi​(m)​(ai​(t)∣si​(t)) and steps θi(m+1)=θi(m)+ηmg^i(m)\theta_i(m+1)=\theta_i(m)+\eta_m\hat g_i(m)θi​(m+1)=θi​(m)+ηm​g^​i​(m) with ηm=η/m+1\eta_m=\eta/\sqrt{m+1}ηm​=η/m+1​.

Formalization targets

Goal: Theorem 4

Under bounded rewards 0≤ri≤rˉ0\le r_i\le\bar r0≤ri​≤rˉ and ∣Si∣≤S|\mathcal S_i|\le S∣Si​∣≤S, ∣Ai∣≤A|\mathcal A_i|\le A∣Ai​∣≤A (Assumption 1), exponential decay with ρ≤γ\rho\le\gammaρ≤γ (Assumption 2), sufficient local exploration with parameters τ,σ\tau,\sigmaτ,σ (Assumption 3), and ∥∇θilog⁡ζi∥≤Li\|\nabla_{\theta_i}\log\zeta_i\|\le L_i∥∇θi​​logζi​∥≤Li​, L=∑iLi2L=\sqrt{\sum_iL_i^2}L=∑i​Li2​​, with ∇J\nabla J∇J L′L'L′-Lipschitz (Assumption 4), and for step sizes and an episode length TTT satisfying explicit conditions, with probability at least 1−δ1-\delta1−δ,

∑m=0M−1ηm∥∇J(θ(m))∥2∑m=0M−1ηm≤2rˉη(1−γ)+8rˉ2L2(1−γ)4log⁡Mlog⁡4δ+96rˉ2L′L2(1−γ)4ηlog⁡MM+1+12L2crˉ(1−γ)5ρκ+1.\frac{\sum_{m=0}^{M-1}\eta_m\|\nabla J(\theta(m))\|^2}{\sum_{m=0}^{M-1}\eta_m}\le\frac{\frac{2\bar r}{\eta(1-\gamma)}+\frac{8\bar r^2L^2}{(1-\gamma)^4}\sqrt{\log M\log\frac4\delta}+\frac{96\bar r^2L'L^2}{(1-\gamma)^4}\eta\log M}{\sqrt{M+1}}+\frac{12L^2c\bar r}{(1-\gamma)^5}\rho^{\kappa+1}.∑m=0M−1​ηm​∑m=0M−1​ηm​∥∇J(θ(m))∥2​≤M+1​η(1−γ)2rˉ​+(1−γ)48rˉ2L2​logMlogδ4​​+(1−γ)496rˉ2L′L2​ηlogM​+(1−γ)512L2crˉ​ρκ+1.

The constants are those of the paper; the statement is the paper's Theorem 4 at full strength.

Milestones

The milestones follow the paper's proof, from foundations to the components of the main bound:

  1. Lemma 1, the policy gradient theorem ∇J(θ)=11−γEs∼πθ,a∼ζθ[Qθ(s,a)∇log⁡ζθ(a∣s)]\nabla J(\theta)=\frac{1}{1-\gamma}\mathbb E_{s\sim\pi^\theta,a\sim\zeta^\theta}[Q^\theta(s,a)\nabla\log\zeta^\theta(a\mid s)]∇J(θ)=1−γ1​Es∼πθ,a∼ζθ​[Qθ(s,a)∇logζθ(a∣s)].
  2. Lemma 3, accuracy of truncated Q-functions (cρκ+1c\rho^{\kappa+1}cρκ+1) and of the truncated policy gradient (cLi1−γρκ+1\frac{cL_i}{1-\gamma}\rho^{\kappa+1}1−γcLi​​ρκ+1).
  3. Lemma 17, the projected Bellman operator gd=ΠdTDΦg_d=\Pi_dT_D\Phigd​=Πd​TD​Φ: a γ\gammaγ-contraction in ∥⋅∥∞\|\cdot\|_\infty∥⋅∥∞​ whose fixed point is within cρκ+11−γ\frac{c\rho^{\kappa+1}}{1-\gamma}1−γcρκ+1​ of QiθQ_i^\thetaQiθ​.
  4. Lemma 9 and Lemma 12, real-analysis bounds on the step-size products of the critic recursion.
  5. Lemma 18, an Azuma–Hoeffding bound for martingale differences whose conditional mean vanishes τ\tauτ steps back: ∣∑k=0tXk∣≤2τ∑kXˉk2log⁡(2τ/δ)|\sum_{k=0}^tX_k|\le\sqrt{2\tau\sum_k\bar X_k^2\log(2\tau/\delta)}∣∑k=0t​Xk​∣≤2τ∑k​Xˉk2​log(2τ/δ)​.
  6. Theorem 5, the critic bound sup⁡(s,a)∣Qiθ(s,a)−Q^iT(sNiκ,aNiκ)∣≤CaT+t0+Ca′T+t0+2cρκ+1(1−γ)2\sup_{(s,a)}|Q_i^\theta(s,a)-\hat Q^T_i(s_{N_i^\kappa},a_{N_i^\kappa})|\le\frac{C_a}{\sqrt{T+t_0}}+\frac{C_a'}{T+t_0}+\frac{2c\rho^{\kappa+1}}{(1-\gamma)^2}sup(s,a)​∣Qiθ​(s,a)−Q^​iT​(sNiκ​​,aNiκ​​)∣≤T+t0​​Ca​​+T+t0​Ca′​​+(1−γ)22cρκ+1​ with probability 1−δ1-\delta1−δ.
  7. Lemmas 13–16, the bounds on the three error terms e1=g^−ge^1=\hat g-ge1=g^​−g (critic error), e2=g−he^2=g-he2=g−h (sampling noise, a martingale difference) and e3=h−∇Je^3=h-\nabla Je3=h−∇J (truncation), and the almost-sure norm bounds rˉL/(1−γ)2\bar rL/(1-\gamma)^2rˉL/(1−γ)2.

Significance

Theorem 4 is a finite-sample guarantee for a model-free multi-agent algorithm whose memory per agent depends on the size of the largest κ-hop neighbourhood, not on nnn. The bias term O(ρκ+1)O(\rho^{\kappa+1})O(ρκ+1) quantifies how much communication radius buys: each additional hop shrinks the guaranteed gap to stationarity by a factor ρ≤γ\rho\le\gammaρ≤γ. The truncation idea (Lemma 3) and the exponential decay property have since been used in a line of work on networked and mean-field reinforcement learning.

The result is proved in the paper; none of it is formalized. A complete formalization would give machine-checked versions of the policy gradient theorem for product policies, of a shifted Azuma–Hoeffding inequality, and of a finite-time analysis of tabular TD learning with state aggregation, each of which is reusable. Related platform items exist in other conventions: the discounted policy gradient theorem from a start state, SampleComplexityRL.PolicyGrad.discounted_policy_gradient, and the open RandomHorizonPG.Asymp.policy_gradient_theorem; the Hoeffding–Azuma inequality ModernOnlineLearning.OnlineToBatch.theorem_3_9 (the case τ=1\tau=1τ=1 of Lemma 18).

Difficulty

The critic is the hard part. The TD iterate on local pairs is not a stochastic approximation of a fixed operator: the sampling distribution of zNiκ(t)z_{N_i^\kappa}(t)zNiκ​​(t) changes with ttt, consecutive samples are dependent, and the truncated table has no exact fixed point equal to QiθQ_i^\thetaQiθ​. The usual argument for TD learning, a fixed contraction plus martingale-difference noise, fails at both ends: the operator moves with the sampling distribution, and the noise has zero conditional mean only given the information τ\tauτ steps back. On the actor side, the critic error must be controlled simultaneously for all agents and all outer iterations, while the policy of each iteration depends on all earlier episodes.

Formalization scope

The setting is finite: agents are Fin n, local state and action sets are finite types, and parameters are θi∈Rdi\theta_i\in\mathbb R^{d_i}θi​∈Rdi​, with θ\thetaθ in PiLp 2 so that ∥θ∥\|\theta\|∥θ∥ is the Euclidean norm of the whole tuple and ∇J\nabla J∇J is Mathlib's gradient. The local kernel of agent iii is typed on the restricted tuple sNis_{N_i}sNi​​, so locality is part of the model. QiθQ_i^\thetaQiθ​, QθQ^\thetaQθ and JJJ are built from the published finite-MDP layer FoundationsML.ReinforcementLearning (QFunction, PolicyValue, OccupationDist) applied to the global MDP. Policies are assumed positive and differentiable in their parameters, which Assumption 4 presupposes. Assumption 3's "probability at time τ\tauτ given z(1)z(1)z(1)" is the (τ−1)(\tau-1)(τ−1)-step law of the state-action chain.

Probabilities are explicit finite sums: the law of a run of SAC over MMM outer iterations is the product of the episode probabilities, episode mmm drawn under the policy θ(m)\theta(m)θ(m) that the algorithm computed from the earlier episodes. The critic tables are functions on the local pairs ZNiκ\mathcal Z_{N_i^\kappa}ZNiκ​​, updated exactly as in (14), and the actor uses each neighbour's own table at its own local pair.

No hypothesis is vacuous: the assumptions hold together, for instance, for one agent with one state, two actions, a constant policy with zero-dimensional parameter, τ=2\tau=2τ=2, σ=12\sigma=\frac12σ=21​, and c,ρ>0c,\rho>0c,ρ>0 with ρ≤γ\rho\le\gammaρ≤γ. Contributions of any milestone are welcome; Lemmas 9, 12 and 18 are self-contained and need none of the model.

Selected references

  • G. Qu, A. Wierman, N. Li, Scalable Reinforcement Learning for Multi-Agent Networked Systems, arXiv:1912.02906v3; Operations Research 70(6), 2022. https://arxiv.org/abs/1912.02906 · https://doi.org/10.1287/opre.2021.2226
  • R. S. Sutton, D. McAllester, S. Singh, Y. Mansour, Policy gradient methods for reinforcement learning with function approximation, NeurIPS 2000. https://proceedings.neurips.cc/paper/1999/hash/464d828b85b0bed98e80ade0a5c43b0f-Abstract.html
  • R. Srikant, L. Ying, Finite-time error bounds for linear stochastic approximation and TD learning, COLT 2019. https://arxiv.org/abs/1902.00923
  • G. Qu, Y. Lin, A. Wierman, N. Li, Scalable multi-agent reinforcement learning for networked systems with average reward, NeurIPS 2020. https://arxiv.org/abs/2006.06626
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Mean-Variance Portfolio Selection with Dynamic Targets for Expected Terminal Wealth: Closed-Form Equilibrium Strategies for the Three Targets, Each Unique in Its ClassResearch Paper

Why mean-variance with a moving target

Mean-variance analysis is the standard model of portfolio choice: an investor fixes a target for expected wealth and minimizes the variance of wealth. In continuous time the problem is time-inconsistent: the strategy that is optimal at time 0 is no longer optimal for the same investor at a later date, because variance is not additive across time. Dynamic programming therefore does not apply directly. A large literature treats the agent's selves at different times as players in a game and looks for equilibrium strategies.

The earlier equilibrium literature mainly studies the penalty formulation, in which variance is traded against mean through a risk-aversion parameter. He and Jiang (Math. Oper. Res. 47(1):587–615, 2022) study the constraint formulation: at each time the agent minimizes the variance of terminal wealth subject to a target for its expectation. Their motivation is practical, since an expected-return target is easier to elicit than a risk-aversion degree. The target may depend on time and on current wealth, which gives the title's dynamic targets. Their definition of equilibrium under such a constraint is new: no constraint of this kind had been considered for time-inconsistent problems in continuous time.

Setting

A market has a risk-free asset with rate r(t)r(t)r(t) and mmm stocks with excess return vector b(t)b(t)b(t) and volatility matrix σ(t)∈Rm×d\sigma(t)\in\mathbb R^{m\times d}σ(t)∈Rm×d, all deterministic, right-continuous and bounded, with b(t)≠0b(t)\neq0b(t)=0 and σ(t)σ(t)⊤⪰δI\sigma(t)\sigma(t)^\top\succeq\delta Iσ(t)σ(t)⊤⪰δI. A feedback strategy π(t,x)\pi(t,x)π(t,x) gives the dollars held in the stocks at time t∈[0,T)t\in[0,T)t∈[0,T) with wealth xxx. The wealth follows

dX(t)=(r(t)X(t)+π(t)⊤b(t))dt+π(t)⊤σ(t) dW(t),X(0)=x0>0.dX(t)=\bigl(r(t)X(t)+\pi(t)^\top b(t)\bigr)dt+\pi(t)^\top\sigma(t)\,dW(t),\quad X(0)=x_0>0 .dX(t)=(r(t)X(t)+π(t)⊤b(t))dt+π(t)⊤σ(t)dW(t),X(0)=x0​>0.

The portfolio must satisfy Qπ≥0Q\pi\ge0Qπ≥0 for an nnn-by-mmm matrix QQQ, and the target is Et[X(T)]≥L(t,X(t))E_t[X(T)]\ge L(t,X(t))Et​[X(T)]≥L(t,X(t)).

For a deviation π∈Rm\pi\in\mathbb R^mπ∈Rm at time ttt, the strategy πt,ε,π\pi_{t,\varepsilon,\pi}πt,ε,π​ uses π\piπ on [t,t+ε)[t,t+\varepsilon)[t,t+ε) and π^\hat\piπ^ afterwards. A feasible π^\hat\piπ^ is an equilibrium strategy if, for every ttt, every reachable wealth xxx and every admissible deviation π≠π^(t,x)\pi\neq\hat\pi(t,x)π=π^(t,x), for all small ε\varepsilonε,

var⁡t(Xπt,ε,π(T))−var⁡t(Xπ^(T))≥0.\operatorname{var}_t\bigl(X^{\pi_{t,\varepsilon,\pi}}(T)\bigr)-\operatorname{var}_t\bigl(X^{\hat\pi}(T)\bigr)\ge0 .vart​(Xπt,ε,π​(T))−vart​(Xπ^(T))≥0.

Three targets are studied, for a function ψ≥0\psi\ge0ψ≥0 integrable on [0,T)[0,T)[0,T): the gross-return target L(t,x)=xe∫tT(r+ψ)L(t,x)=xe^{\int_t^T(r+\psi)}L(t,x)=xe∫tT​(r+ψ), the premium target L(t,x)=1γ(e∫tTψ−1)+xe∫tTrL(t,x)=\frac1\gamma(e^{\int_t^T\psi}-1)+xe^{\int_t^Tr}L(t,x)=γ1​(e∫tT​ψ−1)+xe∫tT​r, and the aspiration target L(t,x)=e−∫tTψxe∫tTr+(1−e−∫tTψ)ξL(t,x)=e^{-\int_t^T\psi}xe^{\int_t^Tr}+(1-e^{-\int_t^T\psi})\xiL(t,x)=e−∫tT​ψxe∫tT​r+(1−e−∫tT​ψ)ξ. For each, v∗(t)v^*(t)v∗(t) denotes the unique solution of the static quadratic program

min⁡v 12v⊤σ(t)σ(t)⊤vsubject tob(t)⊤v≥ψ(t), Qv≥0.\min_v\ \tfrac12v^\top\sigma(t)\sigma(t)^\top v\quad\text{subject to}\quad b(t)^\top v\ge\psi(t),\ Qv\ge0 .vmin​ 21​v⊤σ(t)σ(t)⊤vsubject tob(t)⊤v≥ψ(t), Qv≥0.

Formalization targets

Goal: Theorem 1

Under the paper's Assumptions 1–4, the following strategies are equilibrium strategies:

π^(t,x)=xv∗(t),π^(t,x)=1γe∫tT(ψ−r)v∗(t),π^(t,x)=v∗(t)(x∗(t)−x),\hat\pi(t,x)=xv^*(t),\qquad \hat\pi(t,x)=\tfrac1\gamma e^{\int_t^T(\psi-r)}v^*(t),\qquad \hat\pi(t,x)=v^*(t)\bigl(x^*(t)-x\bigr),π^(t,x)=xv∗(t),π^(t,x)=γ1​e∫tT​(ψ−r)v∗(t),π^(t,x)=v∗(t)(x∗(t)−x),

for the three targets respectively, with x∗(t)=ξe−∫tTrx^*(t)=\xi e^{-\int_t^Tr}x∗(t)=ξe−∫tT​r and ξ≥x0e∫0Tr\xi\ge x_0e^{\int_0^Tr}ξ≥x0​e∫0T​r, the last under a condition (2.13) comparing ψ/ρ\psi/\rhoψ/ρ with ∫∥σ⊤v∗∥2\int\|\sigma^\top v^*\|^2∫∥σ⊤v∗∥2. Each is the only equilibrium in its natural class: strategies proportional to xxx, independent of xxx, or proportional to x∗(t)−xx^*(t)-xx∗(t)−x, with right-continuous and square-integrable coefficient. For the third class this needs (2.15), a uniform version of (2.13).

Milestones

The milestones follow the proof. They are the existence and right-continuity of v∗v^*v∗; Lemma 2, on parametric quadratic programs; Lemma 3, which compares spikes that are Lipschitz in wealth with constant ones; and, for each target, the closed-form moments, the first-order limits, the characterization of equilibrium by a static problem, and the corresponding part of Theorem 1.

Significance

Theorem 1 reduces a game among a continuum of selves to one static quadratic program per date. The equilibrium can therefore be computed by standard solvers, and in closed form when there are no portfolio constraints. The closed forms carry the economic conclusions of the paper: the first target gives a deterministic proportion of wealth, the second a deterministic dollar amount, and the third a contrarian rule that invests less as wealth nears the aspiration path. Section 3 of the paper uses them to compare equilibrium with the pre-committed strategy and with the penalty formulation.

Formalization adds the following. The result is proved on paper, and no machine-checked proof of it is on the platform. The platform contains equilibrium notions for log returns under a penalty and for open-loop controls, but no equilibrium under an expected-value constraint. A complete formalization also makes the definition itself exact: the printed set of admissible deviations does not match the one the proof uses, and the formal statements fix this explicitly.

Difficulty

The obvious argument differentiates ε↦var⁡t(Xπt,ε,π(T))\varepsilon\mapsto\operatorname{var}_t(X^{\pi_{t,\varepsilon,\pi}}(T))ε↦vart​(Xπt,ε,π​(T)) at 0 by a Hamilton–Jacobi equilibrium system. That route gives only the weak condition lim inf⁡≥0\liminf\ge0liminf≥0, and the first-order condition does not imply the regular equilibrium inequality, which must hold for every small ε\varepsilonε. It is also not enough to compute the derivative at a binding target: when the target binds, the set of admissible deviations is itself described only to first order, so necessity needs a perturbation of the boundary, which is where Assumption 2 is used. For uniqueness in the third class the linear coefficient of the static problem has the opposite sign to the first two, so a minimizer need not meet the target, and the conclusion needs a separate backward-in-time argument. A constant spike π\piπ is not of the form that admits the closed-form moments, so its moments must be compared with those of a wealth-proportional spike, to order ε\varepsilonε. Nothing in the setting allows the coefficients to be assumed constant, and the portfolio constraint rules out any closed-form v∗v^*v∗ in general.

Formalization scope

Vectors are Fin m → ℝ, and σ(t)\sigma(t)σ(t) is a Matrix (Fin m) (Fin d) ℝ. All squared norms are Euclidean (sqNorm). Strategies are total functions of which only [0,T)×R[0,T)\times\mathbb R[0,T)×R matters. The Brownian motion lives on a filtered space with the usual conditions, and the goal is quantified over all such spaces. The Itô integral is a sum over coordinates of the published EntropyMFG.Enhanced.HasItoIntegral. EtE_tEt​ and var⁡t\operatorname{var}_tvart​ at (t,x)(t,x)(t,x) are the mean and variance of the solution started at (t,x)(t,x)(t,x); along the agent's own path, EtE_tEt​ is conditional expectation given Ft\mathcal F_tFt​.

Two corrections to the printed text are in force. The set Πt,xπ^\Pi^{\hat\pi}_{t,x}Πt,xπ^​ is the time-ttt self's set, with only Qπ≥0Q\pi\ge0Qπ≥0 and the target at (t,x)(t,x)(t,x), which is the set the proof uses; the printed feasibility would make uniqueness false and can make the set empty. The uniqueness clause for the third target assumes ξ>x0e∫0Tr\xi>x_0e^{\int_0^Tr}ξ>x0​e∫0T​r. The counterexamples are in the Differences list of each item.

Trivialization is ruled out as follows: reachable sets contain atoms and interiors of supports, the goal uses the regular inequality for each small ε\varepsilonε rather than the first-order condition, and v∗v^*v∗ is tied to (2.10) at every date.

A complete development needs existence, uniqueness and moments for linear SDEs with square-integrable coefficients, Doléans exponentials, a Burkholder–Davis–Gundy inequality with Gronwall estimates, a Feynman–Kac identity, the support of lognormal laws, and KKT analysis of convex quadratic programs. The SDE and finite-dimensional QP layers are reusable beyond this mission. The finite-dimensional milestones are self-contained entry points, and contributions on the stochastic-calculus layer are welcome.

Selected references

  • X. D. He, Z. Jiang, Mean-Variance Portfolio Selection with Dynamic Targets for Expected Terminal Wealth, Mathematics of Operations Research 47(1):587–615, 2022. https://doi.org/10.1287/moor.2021.1142
  • X. D. He, Z. Jiang, On the equilibrium strategies for time-inconsistent problems in continuous time, working paper, 2019. https://ssrn.com/abstract=3308274
  • T. Björk, A. Murgoci, A general theory of Markovian time inconsistent stochastic control problems, working paper, 2010. https://ssrn.com/abstract=1694759
  • Y.-J. Huang, Z. Zhou, Strong and weak equilibria for time-inconsistent stochastic control in continuous time, Mathematics of Operations Research, 2019 (forthcoming when cited). https://arxiv.org/abs/1809.09243
  • I. Ekeland, A. Lazrak, Equilibrium policies when preferences are time inconsistent, 2008. https://arxiv.org/abs/0808.3790
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CombinatoricsGraph TheoryProbability·Captain: iris

Uniqueness and Universality of the Brownian Map: uniform random q-angulations with n faces (q = 3 or q even), graph distances scaled by c_q n^(-1/4), converge in distribution to the Brownian mapResearch Paper

Random planar maps and the question of a universal limit

A planar map is a finite connected graph embedded in the sphere, viewed up to orientation-preserving homeomorphisms; loops and multiple edges are allowed. Planar maps were enumerated by Tutte in the 1960s, appear in algebraic geometry and in the theory of matrix integrals, and serve in theoretical physics as discrete models of two-dimensional random geometry (quantum gravity). A natural question is what a large random planar map looks like as a metric space, once its graph distance is rescaled so that the diameter stays bounded.

Schramm asked in 2006 (ICM proceedings) whether uniform random triangulations, rescaled by n−1/4n^{-1/4}n−1/4, converge to a limiting random metric space. The history of the question:

  • Chassaing–Schaeffer (2004) showed that distances in uniform quadrangulations with nnn faces are of order n1/4n^{1/4}n1/4, using the Cori–Vauquelin–Schaeffer bijection with labeled trees.
  • Marckert–Mokkadem (2006) introduced the name Brownian map for a limit object built from the Brownian snake, in a weak form of convergence.
  • Le Gall (2007) proved that uniform 2p2p2p-angulations have Gromov–Hausdorff limits along subsequences, all of the form ([0,1]/ ⁣≈,D)([0,1]/\!\approx, D)([0,1]/≈,D) with DDD only bounded above and below; the uniqueness of the limit remained open.
  • Le Gall (2010) described the geodesics to the distinguished point of any such limit.
  • Le Gall (2013, this paper) and, independently for quadrangulations, Miermont (2013) identified the distance DDD, which proves convergence of the whole sequence and the universality of the limit.

Setting

Fix q≥3q\ge3q≥3 with q=3q=3q=3 or qqq even. A rooted planar qqq-angulation is a planar map whose faces all have degree qqq (an edge with the same face on both sides counts twice), with a distinguished oriented edge. Let AnqA^q_nAnq​ be the finite set of rooted qqq-angulations with nnn faces (An3=∅A^3_n=\varnothingAn3​=∅ for odd nnn) and MnM_nMn​ a uniform element of AnqA^q_nAnq​, with vertex set mnm_nmn​ and graph distance dgrd_{gr}dgr​. The space (K,dGH)(\mathbb K, d_{GH})(K,dGH​) of isometry classes of compact metric spaces with the Gromov–Hausdorff distance is Polish, and (mn,c dgr)(m_n, c\,d_{gr})(mn​,cdgr​) is a random element of it.

The Brownian map is built from two random paths on [0,1][0,1][0,1]. Let eee be a normalized Brownian excursion and de(s,t)=es+et−2min⁡[s∧t,s∨t]ed_e(s,t)=e_s+e_t-2\min_{[s\wedge t,s\vee t]}ede​(s,t)=es​+et​−2min[s∧t,s∨t]​e; the CRT is Te=[0,1]/{de=0}\mathcal T_e=[0,1]/\{d_e=0\}Te​=[0,1]/{de​=0} with projection pep_epe​. Conditionally on eee, let ZZZ be a centred Gaussian process with E[ZsZt∣e]=min⁡[s∧t,s∨t]e\mathbb E[Z_sZ_t\mid e]=\min_{[s\wedge t,s\vee t]}eE[Zs​Zt​∣e]=min[s∧t,s∨t]​e (Brownian labels). For s≤ts\le ts≤t set

D∘(s,t)=Zs+Zt−2max⁡(min⁡[s,t]Z, min⁡[t,1]∪[0,s]Z),D^\circ(s,t)=Z_s+Z_t-2\max\Big(\min_{[s,t]}Z,\ \min_{[t,1]\cup[0,s]}Z\Big),D∘(s,t)=Zs​+Zt​−2max([s,t]min​Z, [t,1]∪[0,s]min​Z),

extend it to Te\mathcal T_eTe​ by minimizing over representatives, and let D∗D^*D∗ be the largest chain distance below D∘D^\circD∘: D∗(a,b)=inf⁡∑i=1kD∘(ai−1,ai)D^*(a,b)=\inf\sum_{i=1}^kD^\circ(a_{i-1},a_i)D∗(a,b)=inf∑i=1k​D∘(ai−1​,ai​) over a0=a,…,ak=ba_0=a,\dots,a_k=ba0​=a,…,ak​=b. The quotient m∞=Te/{D∘=0}m_\infty=\mathcal T_e/\{D^\circ=0\}m∞​=Te​/{D∘=0} with the distance D∗D^*D∗ is the Brownian map (m∞,D∗)(m_\infty,D^*)(m∞​,D∗). In Lean these are dCirc, dStar and brownianMap.

Formalization targets

Goal: Theorem 1.1

With cq=(9/(q(q−2)))1/4c_q=(9/(q(q-2)))^{1/4}cq​=(9/(q(q−2)))1/4 for even qqq and c3=61/4c_3=6^{1/4}c3​=61/4,

(mn, cqn−1/4dgr)→n→∞(d)(m∞,D∗)in K.(m_n,\ c_q n^{-1/4}d_{gr})\xrightarrow[n\to\infty]{(d)}(m_\infty,D^*)\quad\text{in }\mathbb K .(mn​, cq​n−1/4dgr​)(d)n→∞​(m∞​,D∗)in K.

The limit law does not depend on qqq. Both branches (q=3q=3q=3 and every even q≥4q\ge4q≥4) are part of one statement.

Milestones

The bipartite case q=2pq=2pq=2p goes through the Bouttier–Di Francesco–Guitter (BDG) coding of rooted pointed 2p2p2p-angulations by labeled ppp-trees θ∈Tnp\theta\in\mathbb T^p_nθ∈Tnp​:

  1. Eqs. (3), (4): in the BDG map, dgr(∂,v)=ℓv−min⁡ℓ+1d_{gr}(\partial,v)=\ell_v-\min\ell+1dgr​(∂,v)=ℓv​−minℓ+1, and dgr(vi,vj)d_{gr}(v_i,v_j)dgr​(vi​,vj​) is bounded by the discrete analogue of D∘D^\circD∘.
  2. Lemmas 2.1, 2.2: increase times of eee and ZZZ are disjoint; labels just before the hitting time SrS_rSr​ stay below −r+ε-r+\sqrt\varepsilon−r+ε​ except with probability O(εβ0)O(\varepsilon^{\beta_0})O(εβ0​).
  3. Theorem 2.3: along subsequences, rescaled contour, labels and distances converge jointly to (e,Z,D)(e,Z,D)(e,Z,D) with D≤D∗≤D∘D\le D^*\le D^\circD≤D∗≤D∘, D(s,s∗)=Zs+ΔD(s,s_*)=Z_s+\DeltaD(s,s∗​)=Zs​+Δ, and (mn,κpn−1/4dgr)→([0,1]/{D=0},D)(m_n,\kappa_pn^{-1/4}d_{gr})\to([0,1]/\{D=0\},D)(mn​,κp​n−1/4dgr​)→([0,1]/{D=0},D).
  4. Theorem 2.4: geodesics to x∗x_*x∗​ are simple geodesics.
  5. Proposition 6.1: D∗≤CδD1−δD^*\le C_\delta D^{1-\delta}D∗≤Cδ​D1−δ.
  6. Theorem 7.2: D=D∗D=D^*D=D∗ almost surely; with Theorem 2.3 this is the goal for q=2pq=2pq=2p.
  7. Corollary 7.3: D∗(U,V)=(d)D∗(s∗,U)=ZU+Δ=(d)ΔD^*(U,V)\overset{(d)}{=}D^*(s_*,U)=Z_U+\Delta\overset{(d)}{=}\DeltaD∗(U,V)=(d)D∗(s∗​,U)=ZU​+Δ=(d)Δ for independent uniform U,VU,VU,V, the input of the triangulation case.

Significance

The theorem identifies one random metric space as the scaling limit of uniform triangulations and of uniform 2p2p2p-angulations, with explicit constants. It answers Schramm's question, shows that the subsequential limits of Le Gall (2007) are all the same, and gives the explicit formula (1) for the distance conjectured there. The Brownian map has since been shown to be the limit of many further classes (general maps, simple triangulations, maps with prescribed degrees) and to coincide with Liouville quantum gravity with parameter 8/3\sqrt{8/3}8/3​ (Miller–Sheffield), so this convergence is the base of a large part of random geometry.

The result is proved in the literature (Le Gall, Ann. Probab. 2013; Miermont, Acta Math. 2013, for q=4q=4q=4). It has no machine-checked proof. Formalizing it requires the BDG and triangulation bijections, Gromov–Hausdorff convergence in distribution, the CRT, the Brownian snake and fine path properties of Brownian labels; each milestone is a self-contained target, and Theorems 2.3–2.4 are themselves results imported from earlier papers whose proofs are only sketched here.

Difficulty

The obvious route, prove tightness, extract a subsequential limit (m∞,D)(m_\infty,D)(m∞​,D), and then identify DDD, stalls at the identification. The bounds D≤D∗≤D∘D\le D^*\le D^\circD≤D∗≤D∘ and the exact distances to x∗x_*x∗​ come cheaply from labels, but they do not determine DDD between two typical points: there is no labeling formula for dgr(v,v′)d_{gr}(v,v')dgr​(v,v′) in the discrete map, only the upper bound (4). Any identification must rule out that a limiting geodesic between typical points is substantially shorter than the chain distance D∗D^*D∗, a statement about the fine geometry of geodesics in the limit that no compactness argument provides.

Formalization scope

Rooted planar maps are rotation systems with root dart 000 up to root-preserving relabelling (the published definition OAI.FKCRT.RootedMap, referenced); faces are cycles of the face permutation and a qqq-angulation with nnn faces has qn/2qn/2qn/2 edges. The normalized excursion is the 3-dimensional Bessel bridge OAI.FKCRT.standardExcursion; labels are specified by conditional characteristic functions. Probability statements quantify over every probability space carrying these objects. K\mathbb KK is Mathlib's GHSpace with its Borel σ\sigmaσ-algebra, and convergence in distribution is convergence of expectations of bounded continuous test functions. The Brownian map is [0,1]/{D∗=0}[0,1]/\{D^*=0\}[0,1]/{D∗=0} with D∗D^*D∗ unfolded on [0,1][0,1][0,1], which equals Te/{D∘=0}\mathcal T_e/\{D^\circ=0\}Te​/{D∘=0} almost surely. "The setting of Theorem 2.3" is a predicate on the joint law of a subsequential limit (e,Z,D)(e,Z,D)(e,Z,D), not an arbitrary DDD with properties (a)–(b).

The goal asserts measurability of the Brownian map as a random element of K\mathbb KK; without it the expectation of a non-measurable function would be a junk value. Mathlib has no existence theorem for Brownian motion, so the realization quantifier is non-vacuous only through the classical existence theorem.

A complete development needs: labeled trees and contour coding; the BDG bijection and its triangulation analogue (§8, not yet among the milestones); the CRT and Brownian snake; Gromov–Hausdorff convergence of random spaces; geodesics in quotient metric spaces. The tree and map infrastructure and the Gromov–Hausdorff tools are reusable for other random-map missions. Formalizations of the remaining steps (Proposition 3.1 on maps with geodesic boundaries, Lemmas 3.4, 4.3, 5.1–5.3, 7.1, and the triangulation results of §8) are welcome as additional milestones.

Selected references

  • J.-F. Le Gall, Uniqueness and universality of the Brownian map, Ann. Probab. 41 (2013) 2880–2960; arXiv:1105.4842v2. https://arxiv.org/abs/1105.4842 , https://doi.org/10.1214/12-AOP792
  • G. Miermont, The Brownian map is the scaling limit of uniform random plane quadrangulations, Acta Math. 210 (2013) 319–401. https://arxiv.org/abs/1104.1606
  • J.-F. Le Gall, The topological structure of scaling limits of large planar maps, Invent. Math. 169 (2007) 621–670. https://arxiv.org/abs/math/0607567
  • J.-F. Le Gall, Geodesics in large planar maps and in the Brownian map, Acta Math. 205 (2010) 287–360. https://arxiv.org/abs/0804.3012
  • J. Bouttier, P. Di Francesco, E. Guitter, Planar maps as labeled mobiles, Electron. J. Combin. 11 (2004) R69. https://arxiv.org/abs/math/0405099
  • P. Chassaing, G. Schaeffer, Random planar lattices and integrated superBrownian excursion, Probab. Theory Related Fields 128 (2004) 161–212. https://arxiv.org/abs/math/0205226
  • J.-F. Marckert, A. Mokkadem, Limit of normalized quadrangulations: the Brownian map, Ann. Probab. 34 (2006) 2144–2202. https://arxiv.org/abs/math/0403398
  • O. Schramm, Conformally invariant scaling limits: an overview and a collection of problems, Proc. ICM 2006. https://arxiv.org/abs/math/0602151
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Graph TheoryOperations ResearchOptimization·Captain: iris

Convexification of Bilinear Terms over Network Polytopes: For m=1m = 1m=1, Every Tree Meeting Exactly One Endpoint of Arc lll Gives an EC&R Assignment of Class l±l^\pml± for Every Partition of Its NodesResearch Paper

Bilinear terms over network flows

Products yjxiy_jx_iyj​xi​ of a flow variable xix_ixi​ and a second decision variable yjy_jyj​ appear whenever a flow decision interacts with a pricing, design or selection decision: pooling and blending problems, network interdiction, transportation with fixed charges, and bilevel network models. Global solvers handle such terms by convexification: they replace the nonconvex set defined by z=yjxiz=y_jx_iz=yj​xi​ with a description of its convex hull and branch on the remainder. The classical tool is the McCormick envelope (McCormick 1976), which is exact when xix_ixi​ and yjy_jyj​ each range over an interval but weak when xxx is constrained jointly, for example by flow balance.

Davarnia, Richard and Tawarmalani (SIAM J. Optim. 2017) introduced the extended cancel-and-relax (EC&R) procedure, which describes the convex hull of bilinear terms over a polytope by aggregating constraints so that bilinear terms cancel. Khademnia and Davarnia (arXiv:2302.14151, published in Mathematics of Operations Research, 2025) specialize EC&R to the case where the polytope is a network-flow polytope and show that the aggregations needed are described by trees and forests of the network.

Setting

Let G=(V,A)G=(V,A)G=(V,A) be a finite network: a node set VVV, an arc set AAA, and for every arc kkk a tail t(k)t(k)t(k) and a head h(k)≠t(k)h(k)\neq t(k)h(k)=t(k). Parallel arcs are allowed. The flow-balance constraint at a node iii is split into two inequalities:

  • the positive row i+i^+i+: ∑k: t(k)=ixk−∑k: h(k)=ixk≥fi\sum_{k:\,t(k)=i}x_k-\sum_{k:\,h(k)=i}x_k\ge f_i∑k:t(k)=i​xk​−∑k:h(k)=i​xk​≥fi​;
  • the negative row i−i^-i−: −∑k: t(k)=ixk+∑k: h(k)=ixk≥−fi-\sum_{k:\,t(k)=i}x_k+\sum_{k:\,h(k)=i}x_k\ge -f_i−∑k:t(k)=i​xk​+∑k:h(k)=i​xk​≥−fi​.

Together with the bounds 0≤x≤u0\le x\le u0≤x≤u they form the network polytope Ξ\XiΞ. With one extra variable y1∈[0,1]y_1\in[0,1]y1​∈[0,1], the paper's set is

S1={(x,y1,z)∈Ξ×[0,1]×RA: y1xk=zk for all k∈A}.\mathcal S^1=\{(x,y_1,z)\in\Xi\times[0,1]\times\mathbb R^A:\ y_1x_k=z_k\ \text{for all } k\in A\}.S1={(x,y1​,z)∈Ξ×[0,1]×RA: y1​xk​=zk​ for all k∈A}.

An EC&R aggregation of class lσl^\sigmalσ (l∈Al\in Al∈A, σ∈{+,−}\sigma\in\{+,-\}σ∈{+,−}) adds the base equality y1xl−zl=0y_1x_l-z_l=0y1​xl​−zl​=0 with weight σ1\sigma 1σ1, each row ttt of a set I1\mathcal I_1I1​ multiplied by γty1\gamma_t y_1γt​y1​, and each row ttt of a set Iˉ\bar{\mathcal I}Iˉ multiplied by θt(1−y1)\theta_t(1-y_1)θt​(1−y1​), with γ,θ≥0\gamma,\theta\ge0γ,θ≥0 and I1∩Iˉ=∅\mathcal I_1\cap\bar{\mathcal I}=\emptysetI1​∩Iˉ=∅. A bilinear term y1xky_1x_ky1​xk​ is created by a constraint if that constraint contributes a nonzero coefficient to it, and canceled if it is created and its aggregated coefficient is zero. The pair [I1,Iˉ][\mathcal I_1,\bar{\mathcal I}][I1​,Iˉ] is an EC&R assignment if some weights satisfy

  • (C1) at least ∣I1∣+∣Iˉ∣|\mathcal I_1|+|\bar{\mathcal I}|∣I1​∣+∣Iˉ∣ bilinear terms are canceled, and
  • (C2) if I1∪Iˉ≠∅\mathcal I_1\cup\bar{\mathcal I}\ne\emptysetI1​∪Iˉ=∅, every used constraint, the base included, creates at least one canceled term.

Gˉ\bar GGˉ is the undirected graph underlying GGG. In Lean these are NetBilinear.Network, Network.underlying, Network.incRow (the row Eis,k=s([t(k)=i]−[h(k)=i])E_{i^s,k}=s([t(k)=i]-[h(k)=i])Eis,k​=s([t(k)=i]−[h(k)=i])), rowsWith s X (the rows {is}i∈X\{i^s\}_{i\in X}{is}i∈X​), IsECRAssignmentOne and Network.IsECRAssignment.

Formalization targets

Goal: Theorem 2 (p.7)

Let Tˉ\bar TTˉ be a tree in Gˉ\bar GGˉ with node set I~\tilde II~, let lll be an arc with exactly one endpoint in I~\tilde II~, and let I~=I~1⊔I~2\tilde I=\tilde I_1\sqcup\tilde I_2I~=I~1​⊔I~2​ be any partition. Then

h(l)∈I~  ⟹  [{i+}I~1,{i−}I~2] is EC&R of class l+ and [{i−}I~1,{i+}I~2] of class l−,t(l)∈I~  ⟹  [{i−}I~1,{i+}I~2] is EC&R of class l+ and [{i+}I~1,{i−}I~2] of class l−.\begin{aligned} h(l)\in\tilde I&\implies [\{i^+\}_{\tilde I_1},\{i^-\}_{\tilde I_2}]\ \text{is EC\&R of class } l^+ \ \text{and}\ [\{i^-\}_{\tilde I_1},\{i^+\}_{\tilde I_2}]\ \text{of class } l^-,\\ t(l)\in\tilde I&\implies [\{i^-\}_{\tilde I_1},\{i^+\}_{\tilde I_2}]\ \text{is EC\&R of class } l^+ \ \text{and}\ [\{i^+\}_{\tilde I_1},\{i^-\}_{\tilde I_2}]\ \text{of class } l^-. \end{aligned}h(l)∈I~t(l)∈I~​⟹[{i+}I~1​​,{i−}I~2​​] is EC&R of class l+ and [{i−}I~1​​,{i+}I~2​​] of class l−,⟹[{i−}I~1​​,{i+}I~2​​] is EC&R of class l+ and [{i+}I~1​​,{i−}I~2​​] of class l−.​

All four parts are stated, for every finite loopless network, every tree of Gˉ\bar GGˉ (including a single node) and every partition (including I~1=∅\tilde I_1=\emptysetI~1​=∅ or I~2=∅\tilde I_2=\emptysetI~2​=∅).

Milestones (steps of the proof, with all weights equal to 111)

  1. A tree on I~\tilde II~ has ∣I~∣−1|\tilde I|-1∣I~∣−1 edges (already proved on the platform, FamousTheorems.tree_card_edges_6b).
  2. Every arc with both endpoints in I~\tilde II~ has its term y1xry_1x_ry1​xr​ canceled.
  3. The base term y1xly_1x_ly1​xl​ is canceled.
  4. Condition (C1) holds.
  5. Condition (C2) holds.

Milestones 4 and 5 together give the goal.

Significance

Proposition 2 of the paper shows the converse direction: every non-trivial facet-defining EC&R inequality of conv(S1)\mathrm{conv}(\mathcal S^1)conv(S1) comes from such a tree. Together the two results replace a search over all constraint subsets and weights with an enumeration of subtrees of the network, which is how the paper generates cutting planes in its computational section. A tree consisting of no nodes recovers the McCormick bounds, so every nonempty tree is a candidate strengthening.

The result is proved in the paper; no machine-checked version exists. This mission produces a formal statement and proof of the tree-to-assignment direction, a reusable formal definition of the EC&R conditions for one yyy variable over an arbitrary constraint matrix, and a network layer (augmented incidence rows, undirected variant) that allows parallel arcs.

Difficulty

Each single cancellation is a two-term identity, so the obstacle is not algebra. (C1) counts distinct canceled terms, and the count must reach the number of tree nodes even though an edge of Gˉ\bar GGˉ may stand for several parallel arcs and the tree is only given as a subgraph of Gˉ\bar GGˉ. (C2) asks for a canceled term at every node of the tree; the paper's argument uses a tree arc incident to the node, which does not exist when the tree is a single node, so that case is not covered by the printed argument. The paper proves part (i) only and leaves (ii)–(iv) to "similar arguments", so the sign conventions of all four parts must be checked separately.

Formalization scope

  • Nodes and arcs are finite types; arcs carry tail, head and the condition tail k ≠ head k. A self-loop is excluded because Theorem 2 is false for one: a loop at a tree node is incident to exactly one node, but its term occurs only in the base equality and never cancels.
  • Gˉ\bar GGˉ is a Mathlib SimpleGraph; "a tree with node set I~\tilde II~" is a subgraph T with T.verts = Ĩ and T.coe.IsTree. Mathlib trees are nonempty.
  • "Exactly one endpoint" is Xor (tail l ∈ Ĩ) (head l ∈ Ĩ).
  • The EC&R predicate is the reduced form [I1,Iˉ][\mathcal I_1,\bar{\mathcal I}][I1​,Iˉ] of Remark 1 (p.5): weights are existential and nonnegative, a canceled term must be created by some used constraint (otherwise (C1) would hold for free), and (C2) keeps its guard. The supplies, capacities and the variables zzz do not enter (C1) and (C2) and are not modelled.
  • The network layer and the general m=1m=1m=1 EC&R predicate (IsECRAssignmentOne, any constraint matrix) are reusable beyond this mission. Proofs of the milestones and the goal are welcome, as are formal statements of the converse (Proposition 2) and of the m>1m>1m>1 forest results.

Selected references

  • E. Khademnia and D. Davarnia, Convexification of Bilinear Terms over Network Polytopes, arXiv:2302.14151v2, 2024; Mathematics of Operations Research, 2025. https://arxiv.org/abs/2302.14151v2
  • D. Davarnia, J.-P. P. Richard and M. Tawarmalani, Simultaneous Convexification of Bilinear Functions over Polytopes with Application to Network Interdiction, SIAM Journal on Optimization 27(3), 2017. https://doi.org/10.1137/16M1066166
  • G. P. McCormick, Computability of global solutions to factorable nonconvex programs: Part I — Convex underestimating problems, Mathematical Programming 10, 1976. https://doi.org/10.1007/BF01580665
9 thms2 active usersReviewed
Quantum Information·Captain: Gohan

Correlation measures of a quantum state and information characteristics of a quantum channelResearch Paper

Motivation

We discuss the interconnections between basic correlation measures of a bipartite quantum state and basic information characteristics of a quantum channel, focusing on the benefits of these interconnections for solving specific problems concerning the characteristics of both types. We describe properties of the (unoptimized and optimized) quantum discord in infinite-dimensional bipartite systems. In particular, using the generalized Koashi-Winter relation, a simple condition is obtained that guarantees that a state with zero quantum discord is quantum-classical. Two possible definitions of the quantum discord for states with infinite one-way classical correlation are proposed and analysed. The generalized versions of Koashi-Winter and Xi-Lu-Wang-Li relations are used to obtain advanced continuity bounds for the Holevo information at the outputs of a channel and its complementary channel (as functions of a channel for a given ensemble of input states), for the Holevo capacity and the unregularized private capacity of a quantum channel depending either on the input dimension or on the input energy bound. We also discuss the properties of quantum channels which are "doppelgangers" of the monotonicity of the quantum discord and the entropy reduction of a local measurement under quantum channels acting on an unmeasured subsystem.

This mission is the statement-level formalization of Correlation measures of a quantum state and information characteristics of a quantum channel (arXiv:2304.05388v3). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

55 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Proposition 3: zero discord is quantum-classical under either finite-entropy condition (abstract seed) (Proposition 3: zero discord is quantum-classical under either finite-entropy condition (abstract seed), PDF p. 19). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Deferred results

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

  • Corollary 4: refined energy-constrained entropy-reduction continuity: Specified domain/convention for G inverse at ln d0 in the refined energy bound (source-ambiguity)
  • Conjecture 1: general zero-discord characterization: A proved resolution of the explicitly stated open conjecture (hard)
  • Proposition 4C): Correct simultaneous B-unitary transport of the fixed measurement (source-ambiguity)
  • Conjecture 2: equality of the two optimized extensions: A proved resolution of the explicitly stated open conjecture (hard)
  • Proposition 7A–B: energy-constrained output Holevo continuity: Specified domain/convention for G inverse at ln d0 in the refined energy bound (source-ambiguity)
  • Proposition 7C: oscillator asymptotic tightness: The quantifiers of asymptotically tight in external [11, Definition 1, Section 3.2.1] (source-ambiguity)
  • Corollary 8A–B: energy-constrained privacy continuity: Specified domain/convention for G inverse at ln d0 in the refined energy bound (source-ambiguity)
  • Corollary 8C: oscillator privacy asymptotic tightness: The quantifiers of asymptotically tight in external [11, Definition 1, Section 3.2.1] (source-ambiguity)
  • Proposition 9A–B: energy-constrained Holevo-capacity continuity: Specified domain/convention for G inverse at ln d0 in the refined energy bound (source-ambiguity)
  • Proposition 9C: oscillator Holevo-capacity tightness: The quantifiers of asymptotically tight in external [11, Definition 1, Section 3.2.1] (source-ambiguity)
  • Proposition 10: printed private-capacity sharpness claim: A corrected private-capacity witness domain and a precise external sharpness definition (source-ambiguity)
  • Proposition 11A–B: energy-constrained private-capacity continuity: Specified domain/convention for G inverse at ln d0 in the refined energy bound (source-ambiguity)
  • Proposition 11C: oscillator private-capacity sharpness: The quantifiers of asymptotically tight in external [11, Definition 1, Section 3.2.1] (source-ambiguity)

Selected references

  • Correlation measures of a quantum state and information characteristics of a quantum channel, arXiv:2304.05388v3, https://arxiv.org/abs/2304.05388v3
65 thms2 active usersReviewed
Quantum Information·Captain: Gohan

Secure Identification and QKD in the Bounded-Quantum-Storage ModelResearch Paper

Motivation

We consider the problem of secure identification: user U proves to server S that he knows an agreed (possibly low-entropy) password w, while giving away as little information on w as possible, namely the adversary can exclude at most one possible password for each execution of the scheme. We propose a solution in the bounded-quantum-storage model, where U and S may exchange qubits, and a dishonest party is assumed to have limited quantum memory. No other restriction is posed upon the adversary. An improved version of the proposed identification scheme is also secure against a man-in-the-middle attack, but requires U and S to additionally share a high-entropy key k. However, security is still guaranteed if one party loses k to the attacker but notices the loss. In both versions of the scheme, the honest participants need no quantum memory, and noise and imperfect quantum sources can be tolerated. The schemes compose sequentially, and w and k can securely be re-used. A small modification to the identification scheme results in a quantum-key-distribution (QKD) scheme, secure in the bounded-quantum-storage model, with the same re-usability properties of the keys, and without assuming authenticated channels. This is in sharp contrast to known QKD schemes (with unbounded adversary) without authenticated channels, where authentication keys must be updated, and unsuccessful executions can cause the parties to run out of keys.

This mission is the statement-level formalization of Secure Identification and QKD in the Bounded-Quantum-Storage Model (arXiv:0708.2557v3). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

7 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Passive secure AND from password identification (§1, unnumbered: passive-secure AND reduction, PDF p. 3). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Deferred results

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

  • Paper seed pinned to the complete Theorem3.6 (basic identification): Finite code-distance and integer tag-length selection, with a uniform asymptotic error envelope in n−8q (source-ambiguity)
  • §1, cited Lo97 impossibility: unrestricted adversary; password identification; user learns no outcome (hard)
  • §1, cited NPS07 AND round lower bound: statistical semi-honest quantum AND; unrestricted adversary; round-complexity family (hard)
  • §1, unnumbered identification round lower bound: passive AND reduction; statistical identification security; superpolynomial round bound (hard)
  • §1, cited BCS09 entire-password leakage: FS09 security model; unrestricted dishonest party; entire password leakage (hard)
  • §1, unnumbered classical memory O(n²) separation: honest classical memory n; classical key-distribution reduction; one-bit average entropy1/2; adversarial memory O(n²) (source-ambiguity)
  • §1, cited DM04 key-distribution memory attack: honest memory n; adversary Ω(n²) memory; arbitrarily small remaining entropy (hard)
  • §1, cited noisy-storage subsequent result: noisy storage channel; simple storage strategy; Q-ID security (hard)
  • §1, cited DFL+09 commitment preamble: concrete commitment preamble; computational security assumption; joint memory/computational attack requirement (hard)
  • §2.1, cited operational meaning of trace distance: half trace norm; arbitrary evolution and observer discrimination (hard)
  • Lemma2.1: event decomposition of Markov reconstruction: normalized ccq law; event conditioning; computed Markov reconstruction; PSD remainder (source-ambiguity)
  • Theorem2.3: cited BB84 uncertainty relation: normalized mixed n-qubit state; independent BB84 basis measurement; average event entropy; σ(λ) (hard)
  • Theorem2.4: cited quantum privacy amplification: q-qubit ccq side information; independent universal-2 seed; average event entropy; uniform ℓ-bit output with seed/side information retained (hard)
  • §§3.1/4.2, unnumbered sequential composition and reusable keys: sequential executions; password guess history; posterior password law; joint W,K secrecy; security-error accumulation (source-ambiguity)
  • §3.1, cited FS08a/FS09 real/ideal bridge: actual Q-ID execution; Definitions3.2/3.3; external ideal identification functionality; simulator/extractor experiment; classical outer environment (hard)
  • §3.2, cited randomized 1–2 OT security: DFR+07 randomized OT; unrestricted dishonest sender; memory-bounded dishonest receiver (hard)
  • §3.3, cited Tho83 asymptotic coding ingredient: binary code family; asymptotic GV rate; binary entropy inverse; finite block length/distance (hard)
  • §3.4, unnumbered noisy-tag mutual identification: independent tag-bit flips; closeness threshold; server reveals flip positions; mutual-identification acceptance/security (source-ambiguity)
  • §3.5, cited DS05 Lemma5: δ-biased binary linear code families; infinitely many lengths n′; efficient constant-fraction decoding (hard)
  • §3.5, cited FS08b Theorem3.2 and smooth extension: Match the explicit FS08b syndrome extractor to this paper’s average event-deletion entropy, q-qubit penalty, smoothing loss and distance normalization (hard)
  • §3.5, unnumbered imperfect-source distance substitution: independent multi-pulse positions η; full bit/basis leakage at those positions; random residual code distance; smoothing/tail error (source-ambiguity)
  • §3.5, unnumbered constant-noise Q-ID robustness: error-tolerant Q-ID; syndrome encoder/decoder; channel error process; independent multi-pulse sources; correctness/security error (source-ambiguity)
  • §4.1, unnumbered active-relay attack on Q-ID: measure-and-forward attack; observed server rejection; password code coordinate; tag detects disturbance (source-ambiguity)
  • Proposition4.2: Q-ID+ man-in-the-middle security: concrete Q-ID+; Definition4.1 including final decision; uniform independent K; authenticated full tuple; syndrome/decoder with variable length; uniform negligible error envelopes (source-ambiguity)
  • Theorem4.3: Q-ID+ active and leaked-key impersonation security: Q-ID+; Definition4.1 with secret K; Definitions3.2/3.3 with K leaked; binary entropy inverse; integer output/test size; uniform negligible security error (source-ambiguity)
  • §4.4, unnumbered Q-ID+ noisy-channel/source robustness: noise law; correction radius δ; test acceptance threshold; multi-pulse concentration; honest correctness (source-ambiguity)
  • §5, unnumbered reusable-key QKD without authenticated channels: Q-ID+ plus extra independent strong-universal-2 extraction; authenticated extractor seed; extra entropy budget; OTP password confirmation; remaining output key; joint W,K secrecy; accept/abort agreement (source-ambiguity)

Selected references

  • Secure Identification and QKD in the Bounded-Quantum-Storage Model, arXiv:0708.2557v3, https://arxiv.org/abs/0708.2557v3
16 thms2 active usersReviewed
Quantum Information·Captain: Gohan

Encoding a qubit in an oscillatorResearch Paper

Motivation

Quantum error-correcting codes are constructed that embed a finite-dimensional code space in the infinite-dimensional Hilbert space of a system described by continuous quantum variables. These codes exploit the noncommutative geometry of phase space to protect against errors that shift the values of the canonical variables q and p. In the setting of quantum optics, fault-tolerant universal quantum computation can be executed on the protected code subspace using linear optical operations, squeezing, homodyne detection, and photon counting; however, nonlinear mode coupling is required for the preparation of the encoded states. Finite-dimensional versions of these codes can be constructed that protect encoded quantum information against shifts in the amplitude or phase of a d-state system. Continuous-variable codes can be invoked to establish lower bounds on the quantum capacity of Gaussian quantum channels.

This mission is the statement-level formalization of Encoding a qubit in an oscillator (arXiv:quant-ph/0008040v3). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

21 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Abstract / §IV (21)–(27): ideal single-oscillator qunit code and exact small-shift correction (Abstract / §IV (21)–(27): ideal single-oscillator qunit code and exact small-shift correction, PDF p. 1). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Deferred results

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

  • §III: realization on a magnetic torus: Magnetic-torus line-bundle Hamiltonian and actual fixed-Landau-level spectral subspace (hard)
  • §V (30)–(39): finite-squeezing error and photon estimates: Precise source theorem for §V (30)–(39): finite-squeezing error and photon estimates (source-ambiguity)
  • §VI (64): dimension and logical quotient of a lattice code: Multimode generalized stabilizer eigenspace with generator-product phases and logical quotient action (hard)
  • §VI: concatenation with a finite block code: Paper-local oscillator channel realization and logical/syndrome recovery, using available generic trace-class channel predicates (hard)
  • §VII (70)–(73): displacement mixture and recovery criterion: Actual L2 Weyl representation, random-displacement channel integral, and logical recovery bound (hard)
  • §VII (74)–(78): isotropic diffusion generator and moments: Brownian Weyl channel realization with unbounded-generator domain and second-moment pairing (hard)
  • §VII (79)–(81): error-correction efficacy for amplitude damping: Precise source theorem for §VII (79)–(81): error-correction efficacy for amplitude damping (source-ambiguity)
  • §VII (82)–(89): displacement expansion of a phase rotation: Fock/Schroedinger Weyl correspondence and Abel-regularized distributional trace of phase rotation (hard)
  • §VII: correction of small overrotation: Precise source theorem for §VII: correction of small overrotation (source-ambiguity)
  • §VIII (90), (93)–(95): positive Gaussian quantum capacity: Precise source theorem for §VIII (90), (93)–(95): positive Gaussian quantum capacity (source-ambiguity)
  • §VIII: numerical square/hexagonal threshold comparison: Precise source theorem for §VIII: numerical square/hexagonal threshold comparison (source-ambiguity)
  • §VIII: reduction of general Gaussian displacement noise: Metaplectic conjugation of full Gaussian displacement channels, including removal of the mean (hard)
  • §IX (100)–(104): oscillator implementation of logical Clifford gates: Character-compatible generalized-code intertwiners for all finite logical Clifford gates (hard)
  • §IX: lifting every finite encoded Clifford to the qudit: Precise source theorem for §IX: lifting every finite encoded Clifford to the qudit (source-ambiguity)
  • §X (105), Fig.4: ideal homodyne syndrome recovery: Actual ideal SUM/homodyne ancilla instrument with no logical information leakage (hard)
  • Abstract / §§X–XI: fault-tolerant universal computation: Precise source theorem for Abstract / §§X–XI: fault-tolerant universal computation (source-ambiguity)
  • §XI.A (106)–(108): photon number modulo four and logical H: Fock spectral photon-number operator linked to Fourier transform on the ideal square comb encoder (hard)
  • §XI.A (117)–(119): gate action on embedded shift errors: Actual Fourier/SUM displacement covariance on generalized code and physical errors, with modular logical carries (hard)
  • §XI.B (128)–(137): photon preparation of cubic phase states: Precise source theorem for §XI.B (128)–(137): photon preparation of cubic phase states (source-ambiguity)
  • §XI.B (140)–(149): cubic-gate error budget and photon precision: Precise source theorem for §XI.B (140)–(149): cubic-gate error budget and photon precision (source-ambiguity)
  • §XI.C: purification of nonsymplectic resource states: Precise source theorem for §XI.C: purification of nonsymplectic resource states (source-ambiguity)
  • §XII: no finite-dimensional Clifford encoder: Precise source theorem for §XII: no finite-dimensional Clifford encoder (source-ambiguity)
  • §XII: physical Gaussian-acceptance preparation and improvement: Precise source theorem for §XII: physical Gaussian-acceptance preparation and improvement (source-ambiguity)
  • §XII (158)–(162): symplectic equivalence and many-mode encoding: Character-aligned metaplectic transport between generalized self-dual lattice-state rays (hard)
  • §XIII (163): generalized ground space of the cosine Hamiltonian: Precise source theorem for §XIII (163): generalized ground space of the cosine Hamiltonian (source-ambiguity)
  • §XIII: periodic-potential cooling and Landau bands: Precise source theorem for §XIII: periodic-potential cooling and Landau bands (source-ambiguity)
  • §XII (155)–(157), Fig.8: modular-position preparation: Ideal modular-position measurement with conditional action on generalized input, linked to the number-coupled meter (hard)

Selected references

  • Encoding a qubit in an oscillator, arXiv:quant-ph/0008040v3, https://arxiv.org/abs/quant-ph/0008040v3
28 thms2 active usersReviewed
Quantum Information·Captain: Gohan

Quantum Feedback ChannelsResearch Paper

Motivation

In Shannon information theory the capacity of a memoryless communication channel cannot be increased by the use of feedback. In quantum information theory the no-cloning theorem means that noiseless copying and feedback of quantum information cannot be achieved. In this paper, quantum feedback is defined as the unlimited use of a noiseless quantum channel from receiver to sender. Given such quantum feedback, it is shown to provide no increase in the entanglement--assisted capacities of a memoryless quantum channel, in direct analogy to the classical case. It is also shown that in various cases of non-assisted capacities, feedback may increase the capacity of memoryless quantum channels.

This mission is the statement-level formalization of Quantum Feedback Channels (arXiv:quant-ph/0209076v4). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

7 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Classical entanglement-assisted capacity is unchanged by feedback (§I, Eq. (1), PDF p. 1). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Deferred results

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

  • §IV, Eq. (28): Integer-budget EPR generation, consuming entanglement-assisted quantum code families, and their actual CPTP two-phase execution. (hard)
  • §IV, Eq. (29): Specialization of the executed two-phase resource interface to the qubit erasure channel. The zero-cutoff source correction has been independently approved at the formula level; no corrected theorem is submitted. (hard)

Selected references

  • Quantum Feedback Channels, arXiv:quant-ph/0209076v4, https://arxiv.org/abs/quant-ph/0209076v4
10 thms2 active usersReviewed
Quantum Information·Captain: Gohan

An introduction to measurement based quantum computationResearch Paper

Motivation

In the formalism of measurement based quantum computation we start with a given fixed entangled state of many qubits and perform computation by applying a sequence of measurements to designated qubits in designated bases. The choice of basis for later measurements may depend on earlier measurement outcomes and the final result of the computation is determined from the classical data of all the measurement outcomes. This is in contrast to the more familiar gate array model in which computational steps are unitary operations, developing a large entangled state prior to some final measurements for the output. Two principal schemes of measurement based computation are teleportation quantum computation (TQC) and the so-called cluster model or one-way quantum computer (1WQC). We will describe these schemes and show how they are able to perform universal quantum computation. We will outline various possible relationships between the models which serve to clarify their workings. We will also discuss possible novel computational benefits of the measurement based models compared to the gate array model, especially issues of parallelisability of algorithms.

This mission is the statement-level formalization of An introduction to measurement based quantum computation (arXiv:quant-ph/0508124v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

22 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Lemma 1: maximally entangled contraction (Lemma 1: maximally entangled contraction, PDF p. 3). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Deferred results

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

  • Abstract and §§2–5: universality of TQC and 1WQC: destructive TQC/rectangular-cluster compiler with input/output embeddings (hard)
  • §2: cited/background Euler decompositions and universal gate sets: audited phase-aware Euler/W decompositions and exact universal-set theorem (hard)
  • §3: adaptive gate sequences and Pauli frame: recursive causal TQC circuit translation and accumulated Pauli frame (hard)
  • §3 and §5.1: Pauli-corrected Z readout and early outputs: joint corrected readout and output-bit-independent scheduling for constructed patterns (hard)
  • §4 Theorem [9]: Clifford generators: projective Clifford generation or an explicit scalar-phase generator convention (source-ambiguity)
  • §4 and §5.1: Clifford arrays need one measurement layer: source-restricted parallel TQC and 1WQC pattern schedules (hard)
  • §4: parity postprocessing of Clifford byproducts: computed Clifford frame and fan-in-two XOR program (hard)
  • §4: recalled logarithmic-depth Clifford gate array: ancilla, gate-arity and wire-count conventions for the stated depth bound (source-ambiguity)
  • §4 Remark: Knill–Gottesman theorem [10]: finite circuit description and runtime bound including its unrestricted gate count (source-ambiguity)
  • §4 Remark: logarithmic-depth classical simulation [11]: parallel classical sampling model, fan-in, size parameter and uniformity (source-ambiguity)
  • §5: assertion that outcomes are always uniform: a valid restriction under which the claimed uniformity is true (source-ambiguity)
  • §6.1 Theorem [6,12]: two measurement layers: two-layer 1WQC composition for each separate CX/rotation family (hard)
  • §6.1 Remark [13]: CX and y rotations: real-orthogonal universality or an explicit complex-state encoding (source-ambiguity)
  • §6.2: efficient classical simulation of one-dimensional patterns: computable entries, precision/error and charged controller runtime (source-ambiguity)
  • §7.1: remaining projected teleportation interpretations [18]: virtual Z/CZ patterns and their complete physical outcome map (hard)
  • §8: polynomial resource equivalence of models: effective model descriptions and charged coherent classical controllers (hard)
  • §8: asserted linear gate/qubit overhead: charged coherent control and rectangular routing cost (source-ambiguity)
  • §8 Conjecture: logarithmically many quantum layers: proof of the explicitly unproved conjecture (hard)
  • §8: Shor special case [19]: formal uniform factoring algorithm with its approximation and success parameters (hard)

Selected references

  • An introduction to measurement based quantum computation, arXiv:quant-ph/0508124v2, https://arxiv.org/abs/quant-ph/0508124v2
28 thms2 active usersReviewed
Quantum Information·Captain: Gohan

Non-integral central extensions of loop groupsResearch Paper

Motivation

It is well-known that the central extensions of the loop group of a compact, simple and 1-connected Lie group are parametrised by their level k∈Zk \in Zk∈Z. This article concerns the question how much can be said for arbitrary k∈Rk \in Rk∈R and we show that for each kkk there exists a Lie groupoid which has the level kkk central extension as its quotient if k∈Zk \in Zk∈Z. By considering categorified principal bundles we show, moreover, that the corresponding Lie groupoid has the expected bundle structure.

This mission is the statement-level formalization of Non-integral central extensions of loop groups (arXiv:0910.1937v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

2 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is The locally smooth cocycle defines a Lie extension and principal bundle (Section 2, unnumbered: the cocycle twisted Lie extension, PDF p. 4). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Deferred results

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

  • Abstract and Introduction: arbitrary real levels and principal 2-bundles: Period-defined level 2-group, smooth Morita equivalence and principal 2-bundle construction (hard)
  • Section 1: Neeb classification of central extensions: Local/global smooth cohomology quotients and equivalence classes of central Lie extensions (hard)
  • Section 1: Neeb integration exact sequences and period criterion: Differentiation, period and flux maps on quotient cohomology (hard)
  • Theorem 2.1: extending a generating local Lie structure: Extension of a generating local manifold atlas to the full abstract group (hard)
  • Proposition 2.3: classification of the underlying bundle: Underlying principal-bundle isomorphism classes and their Cech class map (hard)
  • Corollary 2.4: globally smooth representatives and triviality: Underlying topological bundle triviality and global smooth representative equivalence (hard)
  • Section 2, unnumbered: characteristic-map exact sequence: Additive local/global H2 quotients, additive Cech H1 and induced inclusion/tau homomorphisms (hard)
  • Section 2 closing observation: discrete-coefficient principal bundles: Actual discrete-abelian principal covering and compatible lifted Lie group operations (hard)
  • Section 3: normalized loop cocycle and real period lattice: Normalized loop Killing cocycle and its actual real period lattice (hard)
  • Section 3: integrability exactly at integral levels: Differentiation-based integration criterion for k*omega with circle coefficients (hard)
  • Section 3: universality at levels plus/minus one: Universal central loop extension with both kernel and total-group morphisms (hard)
  • Section 3, unnumbered: global integration on the based path group: Actual based path Lie group, endpoint differential and integrating global cocycle (hard)
  • Sections 3–4: classical normal subgroup and integral quotient: Filling-independent graph subgroup N_k inside the matching level path extension (source-ambiguity)
  • Remark 4.1: smooth action groupoid and smooth quotient: Freeness/principal-action condition for a smooth quotient Morita equivalence (source-ambiguity)
  • Section 4: smooth versus continuous mapping homotopies: Relative smooth/continuous homotopy comparison for disk and sphere maps (hard)
  • Section 4: smooth mapping-group Lie structure: Compact-source C-infinity mapping-group topology and locally convex Lie atlas (hard)
  • Lemma 4.2: the disk-filling quotient Lie group: Concrete disk mapping quotient by the identity component of boundary-trivial smooth maps (hard)
  • Section 4, unnumbered: the boundary central extension: Boundary homomorphism on the filling quotient and its pi2 kernel identification (hard)
  • Section 4, unnumbered: general boundary crossed module and four-term sequence: Geometric boundary crossed-module action and four actual exact-sequence maps (hard)
  • Section 4: characteristic third cohomology class: Choice-independent characteristic H3 class of the actual geometric crossed module (hard)
  • Section 4, unnumbered: smooth disk integral on the quotient: Actual surface integration of the normalized left-invariant two-form on relative disk classes (hard)
  • Section 4: explicit path cocycle formula and Murray identity: Missing loop evaluation and logarithmic partial-derivative convention in the kappa_k double integral (source-ambiguity)
  • Proposition 4.3: the explicit real-level smooth right action: Specified real-level right action through the unresolved kappa_k formula (source-ambiguity)
  • Sections 1 and 4: integral-level orbit quotients and endpoint interpolation: Matching-level orbit quotient and endpoint interpolation for the specified action (source-ambiguity)
  • Section 5, unnumbered: the section-cover groupoid and Morita functor: Inconsistent P1 coordinates and source/target direction in the claimed inclusion functor (source-ambiguity)
  • Proposition 5.1: the specified principal 2-bundle structure: Inconsistent specified 2-action and inverse local trivialization (source-ambiguity)
  • Corollary 5.2: rational-level quotient principal bundle: Rational band construction on the particular inconsistent groupoid P_k (source-ambiguity)
  • Section 5, unnumbered closing result: rational-level Lie central extension: Actual rational quotient object and conflicting non-inheritance assertion (source-ambiguity)
  • Section 5 proof observation: no global section of the filling cover: Topology of the filling-group covering proving absence of a global smooth section (hard)

Selected references

  • Non-integral central extensions of loop groups, arXiv:0910.1937v1, https://arxiv.org/abs/0910.1937v1
6 thms2 active usersReviewed
Quantum Information·Captain: Gohan

Entanglement entropy of two disjoint intervals in conformal field theoryResearch Paper

Motivation

We study the entanglement of two disjoint intervals in the conformal field theory of the Luttinger liquid (free compactified boson). Trρ_A^n for any integer n is calculated as the four-point function of a particular type of twist fields and the final result is expressed in a compact form in terms of the Riemann-Siegel theta functions. In the decompactification limit we provide the analytic continuation valid for all model parameters and from this we extract the entanglement entropy. These predictions are checked against existing numerical data.

This mission is the statement-level formalization of Entanglement entropy of two disjoint intervals in conformal field theory (arXiv:0905.2069v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

15 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Replica theta-quotient symmetries and self-dual value (Eqs. (8)–(11), symmetries, PDF p. 4). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Deferred results

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

  • Main result, Eqs. (4),(8)–(11): Constructed real compactified-scalar vacuum, regulated spatial marginal, and replica-sewn partition functions with common normalization. (hard)
  • Section 4.3.3: The six explicit order-four terms, coefficients, moduli, and their allowed argument dependence. (source-ambiguity)
  • Section 4.6, Eq. (75): Two independently constructed real compactified vacua and the actual different-radii complex-scalar replica factor. (hard)
  • Section 5, Eqs. (76)–(79): A deformation, subtraction and growth prescription fixing the intended nonintegral replica continuation of D_n. (source-ambiguity)
  • Section 5.1, Eqs. (80),(82): Actual interval von Neumann entropies and mutual information with a radius-compatible decompactification limit. (hard)
  • Eq. (81): Actual single-interval and two-interval Renyi entropies from compatible vacuum marginals. (hard)
  • Section 5.2, Eq. (84): Corrected physical entropy coefficient and a justified all-alpha replica limit. (source-ambiguity)
  • Conclusion, Eq. (86): Constructed general vacuum CFT and its multi-interval twist-field covariance and independent conformal moduli. (hard)
  • Appendix D.3, Eqs. (D.16)–(D.19): A consistent general-alpha resummation transform and its inverse, with a summability prescription. (source-ambiguity)

Selected references

  • Entanglement entropy of two disjoint intervals in conformal field theory, arXiv:0905.2069v2, https://arxiv.org/abs/0905.2069v2
17 thms2 active usersReviewed
Quantum Information·Captain: Gohan

On completion of the cone of CP linear maps with respect to the energy-constrained diamond normResearch Paper

Motivation

For a given positive operator GGG we consider the cones of linear maps between Banach spaces of trace class operators characterized by the Stinespring-like representation with G\sqrt{G}G​-bounded and G\sqrt{G}G​-infinitesimal operators correspondingly. We prove the completeness of both cones w.r.t. the energy-constrained diamond norm induced by GGG (as an energy observable) and the coincidence of the second cone with the completion of the cone of CP linear maps w.r.t. this norm. We show that the sets of quantum channels and quantum operations are complete w.r.t. the energy-constrained diamond norm for any energy observable GGG. Some properties of the maps belonging to the introduced cones are described. In particular, the corresponding generalization of the Kretschmann-Schlingemann-Werner theorem is obtained. We also give a nonconstructive description of the completion of the set of all Hermitian-preserving completely bounded linear maps w.r.t. the ECD norm.

This mission is the statement-level formalization of On completion of the cone of CP linear maps with respect to the energy-constrained diamond norm (arXiv:1810.10922v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

2 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Remark 2: component bounds and the finite-family converse (Remark 2, PDF p. 17). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Deferred results

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

  • Theorem 1 A–C (the completion result announced in the abstract): ECD metric on representation-equivalence classes and spectral cutoff maps (hard)
  • Corollary 1: Infinite-dimensional channels/operations with the full ECD metric (hard)
  • Corollary 2: Equality of partial-trace maps for all finite-energy states (hard)
  • Lemma 4: Representation-defined amplified maps and their trace-norm supremum (hard)
  • Lemma 5: Energy-dependent common-environment representatives and Bures distance (hard)
  • Lemma 6: Amplified intrinsic Bures metric and the contraction defect dilation (hard)
  • Remark 1 and equation (34): Positive trace-class Bures distance and pure-state ECD supremum (hard)
  • Proposition 1 A–B: Continuous positive extensions to T_(G tensor I) and trace-norm energy slices (hard)
  • Proposition 2: Complex-linear partial-trace cross maps for nonclosable operators (hard)
  • Proposition 3 A–B: Trace-class Kraus summation and generalized Stinespring map relation (hard)
  • Theorem 2: generalized KSW inequalities: Fixed-environment representing fibers and intrinsic ECD/Bures quantities (hard)
  • Theorem 3 A–B: Independently defined Y_G from energy-slice continuous amplifications (hard)
  • Lemma 8: Y_G amplification and simultaneous marginal energy constraints (hard)
  • Proposition 4: Trace-class block maps and independent Y_G-positive cone (hard)
  • Proposition 5: Actual ECD closure of full trace-class HP completely bounded maps (hard)
  • Unnumbered main result: incompleteness before completion: Two actual normed map spaces and the unbounded-energy ECD metric (hard)
  • Unnumbered construction: representative-independent amplification: Nonclosable representative amplification on the full energy domain (hard)
  • Unnumbered result: Y_G norm and concavity: Energy-slice-continuity-defined Y_G and ECD finiteness (hard)
  • Conjecture (explicitly unproved; deferred): A proof of the explicitly open CP-difference conjecture (source-ambiguity)

Selected references

  • On completion of the cone of CP linear maps with respect to the energy-constrained diamond norm, arXiv:1810.10922v2, https://arxiv.org/abs/1810.10922v2
4 thms2 active usersReviewed
Quantum Information·Captain: Gohan

Locking classical correlation in quantum statesResearch Paper

Motivation

We show that there exist bipartite quantum states which contain large hidden classical correlation that can be unlocked by a disproportionately small amount of classical communication. In particular, there are (2n+1)(2n+1)(2n+1)-qubit states for which a one bit message doubles the optimal classical mutual information between measurement results on the subsystems, from n/2n/2n/2 bits to nnn bits. States exhibiting this behavior need not be entangled. We study the range of states exhibiting this phenomenon and bound its magnitude.

This mission is the statement-level formalization of Locking classical correlation in quantum states (arXiv:quant-ph/0303088v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

12 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Separable two-basis one-bit locking (Eq. (5), conclusion on PDF p. 3, PDF p. 2). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Deferred results

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

  • Eq. (8) and following paragraph: Meaning of the asymptotic family, proportionality and approximation in Eq. (8) (source-ambiguity)
  • Closing discussion, two-key paragraph: Fully specified two-key density matrix and quantitative one-way/two-way comparison (source-ambiguity)

Selected references

  • Locking classical correlation in quantum states, arXiv:quant-ph/0303088v1, https://arxiv.org/abs/quant-ph/0303088v1
17 thms2 active usersReviewed
Quantum Information·Captain: Gohan

Quantum channels with polytopic images and image additivityResearch Paper

Motivation

We study quantum channels with respect to their image, i.e., the image of the set of density operators under the action of the channel. We first characterize the set of quantum channels having polytopic images and show that additivity of the minimal output entropy can be violated in this class. We then provide a complete characterization of quantum channels TTT that are universally image additive in the sense that for any quantum channel SSS, the image of T⊗ST \otimes ST⊗S is the convex hull of the tensor product of the images of TTT and SSS. These channels turn out to form a strict subset of entanglement breaking channels with polytopic images and a strict superset of classical-quantum channels.

This mission is the statement-level formalization of Quantum channels with polytopic images and image additivity (arXiv:1408.2340v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

21 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Channels with polytopic images (Theorem 3.5, Channels with polytopic images; seed and first informal theorem on p.2, PDF p. 6). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Deferred results

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

  • Proposition 5.2, equation (17): An explicit correction of equation (17) with separate tensor-factor dimensions, noise-factor density states, a global block embedding and zero transient block. (source-ambiguity)
  • Appendix A, equations (23)-(24), continuation p.16: An audited corrected signed Fujiwara-Algoet criterion, including boundary cases or explicit canonical sign-order assumptions. (source-ambiguity)

Selected references

  • Quantum channels with polytopic images and image additivity, arXiv:1408.2340v1, https://arxiv.org/abs/1408.2340v1
30 thms2 active usersReviewed
Quantum Information·Captain: Gohan

The representations of cyclotomic BMW algebrasResearch Paper

Motivation

In this paper, we prove that the cyclotomic BMW algebras B2p+1,n are cellular in the sense of [16]. We also classify the irreducible B2p+1,nmodules over a field.

This mission is the statement-level formalization of The representations of cyclotomic BMW algebras (arXiv:0801.0465v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

21 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Unique generator-fixing reversal anti-isomorphism (Lemma 2.2, PDF p. 3). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Deferred results

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

  • Proposition 3.2: Unrestricted existence with arbitrary moments (source-ambiguity)
  • Lemma 4.2: Ordered multipartitions, actual updown paths, finite addable/removable boundary nodes, and the canonical replacement at step k (hard)
  • Lemma 4.6: Actual path content sequence, Definition 4.5 genericity, order of q squared, and return-equivalence classes (hard)
  • Lemma 4.8: Finite addable/removable boundary of an arbitrary ordered multipartition with multiplicative/inverse removable contents (hard)
  • Lemma 4.10: The specified boundary-product rational function W_k/y and its scalar simple-pole coefficients (hard)
  • Lemma 4.17: Canonical partial adjacent path swap, its actual domain, a_s(k), and compatible b roots (hard)
  • Theorem 4.19: Free vector space on actual updown tableaux and every explicitly constructed T,E,X and inverse-X operator with six root compatibilities (hard)
  • Proposition 4.29: Evaluation of canonically constructed lower central Laurent coefficients on the actual tableau content sequence (hard)
  • Corollary 4.30: Constructed E,X operators and action of the canonical lower central moments on E_k v_s (hard)
  • Lemma 4.31: Two canonically computed diagonal residue scalars at consecutive return steps (hard)
  • Lemma 4.32: Compatible actual partial swaps and the two b-radicands and diagonal residue scalars in their correct positions (hard)
  • Proposition 4.33: All three equivalence-class residue sums, with nonzero scalar denominators and reciprocal E_ss in clause b (hard)
  • Lemma 4.35: The pre-module seminormal operators and all twelve operator identities, including arbitrary negative moments (hard)
  • Lemma 4.36: The constructed pre-module T and E operators on actual path basis vectors (hard)
  • Proposition 4.37: The constructed operators and both ordered tangle identities on actual path vectors (hard)
  • Lemma 4.38: Constructed adjacent operators at paths with both no-return hypotheses (hard)
  • Lemma 4.40: Constructed adjacent operators with either of the two mixed return hypotheses (hard)
  • Proposition 4.41: Constructed adjacent operators at every tableau, including two consecutive returns (hard)
  • Lemma 4.42: Real logarithmic separation and sign regimes plus canonical positive/nonnegative roots satisfying all six global compatibilities (hard)
  • Lemma 5.8: Normalized actual Murphy m_st and M_st, canonical sigma_f on the lower Hecke quotient, and all four identities (hard)
  • Theorem 5.10: Normalized Murphy vectors, actual strict higher-cell ideal including B^(f+1), and the specified quotient-row span (hard)
  • Proposition 5.37: The full normalized double-triple cellular family, canonical reversal, and the complete strict higher-cell quotient (hard)
  • Theorem 5.41: explicit cellular basis (original abstract seed): The normalized explicit Murphy/BMW family with its actual finite label poset, indexed basis, and exact star index swap (hard)
  • Lemma 6.1: All-case maximal-f corner equality when moments can vanish (source-ambiguity)
  • Lemma 6.2: BMW and Hecke cell forms computed from the same corrected explicit cellular families (hard)
  • Theorem 6.3: Good-node Kleshchev labels and their ordered parameter-orbit Morita transport to the same right Hecke/BMW cell quotients (hard)

Selected references

  • The representations of cyclotomic BMW algebras, arXiv:0801.0465v2, https://arxiv.org/abs/0801.0465v2
23 thms2 active usersReviewed
Quantum Information·Captain: Gohan

Decomposition of Normal Operators and Its Application to Spectral TheoremResearch Paper

Motivation

A decomposition theorem for self-adjoint operators proved by Riesz and Lorch is extended to normal operators. This extension gives a new proof of the spectral theorem for unbounded normal operators.

This mission is the statement-level formalization of Decomposition of Normal Operators and Its Application to Spectral Theorem (arXiv:2006.04644v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

4 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Normal-operator decomposition with explicit closedness correction (Theorem 1.1, PDF p. 1). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Selected references

  • Decomposition of Normal Operators and Its Application to Spectral Theorem, arXiv:2006.04644v2, https://arxiv.org/abs/2006.04644v2
6 thms2 active usersReviewed
CombinatoricsOperations ResearchOptimization·Captain: iris

Semidefinite Programming Relaxations of the Traveling Salesman Problem and Their Integrality Gaps: The de Klerk–Sotirov SDP Has Integrality Gap at Least z for Every z ∈ ℕResearch Paper

Motivation

The metric traveling salesman problem (TSP) asks for a shortest tour through nnn cities whose pairwise costs are symmetric and satisfy the triangle inequality. The best-known guarantees for it come from relaxations: Christofides' 3/23/23/2-approximation is analysed against the subtour-elimination linear program (Held–Karp), and the integrality gap of that LP is conjectured to be 4/34/34/3. A relaxation with a provably smaller integrality gap would be a route to better approximation algorithms, so semidefinite programming (SDP) relaxations of the TSP have been proposed and studied as candidates.

One of them is the SDP of de Klerk and Sotirov (Math. Program. 2012), obtained by applying symmetry reduction to the SDP relaxation of the quadratic assignment problem of Povh and Rendl (Discrete Optim. 2009), specialized to the TSP. De Klerk and Sotirov showed it is incomparable with the subtour LP, and on the 24 classes of facet-defining instances of the TSP on 8 vertices it performed at least as well as the subtour LP on all but one. Gutekunst and Williamson (arXiv:1907.09054, Mathematics of Operations Research 2022) show that its integrality gap is unbounded.

Timeline. 1976: Christofides, 3/23/23/2 via the Held–Karp bound. 2008: de Klerk, Pasechnik and Sotirov, an SDP relaxation of the TSP based on the association scheme of the cycle. 2009: Povh and Rendl, the copositive and SDP relaxations of the QAP. 2012: de Klerk and Sotirov, the symmetry-reduced QAP SDP (SDP (2) here). 2017: Gutekunst and Williamson show the de Klerk–Pasechnik–Sotirov SDP has unbounded integrality gap. 2019: Gutekunst and Williamson show the same for SDP (2), and for the Povh–Rendl SDP (1) through earlier results.

Setting

An instance is a cost matrix D∈R(n+1)×(n+1)D\in\mathbb R^{(n+1)\times(n+1)}D∈R(n+1)×(n+1) that is metric: symmetric, zero on the diagonal, and satisfying Duw≤Duv+DvwD_{uw}\le D_{uv}+D_{vw}Duw​≤Duv​+Dvw​. OPTTSP(D)\mathrm{OPT}_{\mathrm{TSP}}(D)OPTTSP​(D) is the minimum cost of a Hamiltonian cycle.

Write JmJ_mJm​ for the all-ones matrix, Ejj=ejejTE_{jj}=e_je_j^{\mathsf T}Ejj​=ej​ejT​, ⊗\otimes⊗ for the Kronecker product, and vec⁡\operatorname{vec}vec for column stacking. The symmetric circulant basis Ci(m)C^{(m)}_iCi(m)​ has entries 1{t−s≡i}+1{s−t≡i}(modm)\mathbb 1\{t-s\equiv i\}+\mathbb 1\{s-t\equiv i\}\pmod m1{t−s≡i}+1{s−t≡i}(modm); C1(m)C^{(m)}_1C1(m)​ is the adjacency matrix of the mmm-cycle.

SDP (2) on n+1n+1n+1 vertices fixes indices r,s∈[n+1]r,s\in[n+1]r,s∈[n+1], sets α=[n+1]∖{r}\alpha=[n+1]\setminus\{r\}α=[n+1]∖{r}, β=[n+1]∖{s}\beta=[n+1]\setminus\{s\}β=[n+1]∖{s}, cˉ=vec⁡(C1[α,{r}]D[{s},β])\bar c=\operatorname{vec}(C_1[\alpha,\{r\}]D[\{s\},\beta])cˉ=vec(C1​[α,{r}]D[{s},β]), and minimizes

trace⁡((D[β]⊗12C1(n+1)[α]+Diag⁡(cˉ))Y)\operatorname{trace}\Bigl(\bigl(D[\beta]\otimes\tfrac12C^{(n+1)}_1[\alpha]+\operatorname{Diag}(\bar c)\bigr)Y\Bigr)trace((D[β]⊗21​C1(n+1)​[α]+Diag(cˉ))Y)

over symmetric Y∈Rn2×n2Y\in\mathbb R^{n^2\times n^2}Y∈Rn2×n2 with Y≥0Y\ge0Y≥0 entrywise, Y⪰0Y\succeq0Y⪰0, trace⁡((In⊗Ejj)Y)=trace⁡((Ejj⊗In)Y)=1\operatorname{trace}((I_n\otimes E_{jj})Y)=\operatorname{trace}((E_{jj}\otimes I_n)Y)=1trace((In​⊗Ejj​)Y)=trace((Ejj​⊗In​)Y)=1 for all jjj, trace⁡((In⊗(Jn−In)+(Jn−In)⊗In)Y)=0\operatorname{trace}((I_n\otimes(J_n-I_n)+(J_n-I_n)\otimes I_n)Y)=0trace((In​⊗(Jn​−In​)+(Jn​−In​)⊗In​)Y)=0 and trace⁡(Jn2Y)=n2\operatorname{trace}(J_{n^2}Y)=n^2trace(Jn2​Y)=n2. These are also the constraints of the Povh–Rendl SDP (1) on nnn vertices, whose objective is 12trace⁡((D⊗C1(n))Y)\tfrac12\operatorname{trace}((D\otimes C^{(n)}_1)Y)21​trace((D⊗C1(n)​)Y). Its optimal value is OPTSDP(D)\mathrm{OPT}_{\mathrm{SDP}}(D)OPTSDP​(D), and the integrality gap is sup⁡DOPTTSP(D)/OPTSDP(D)\sup_D \mathrm{OPT}_{\mathrm{TSP}}(D)/\mathrm{OPT}_{\mathrm{SDP}}(D)supD​OPTTSP​(D)/OPTSDP​(D) over metric instances.

The witnesses are simplicial instances: ggg groups of n/gn/gn/g cities, cost 000 inside a group and 111 between groups, i.e. D=(Jg−Ig)⊗Jn/gD=(J_g-I_g)\otimes J_{n/g}D=(Jg​−Ig​)⊗Jn/g​; the (n+1)(n+1)(n+1)-city version gives the first group one extra vertex. The feasible solution is

Y=12n[(Jg−Ig)⊗Jn/g⊗B+Ig⊗Jn/g⊗A+Ig⊗In/g⊗(2In−A)],(3)Y=\tfrac1{2n}\bigl[(J_g-I_g)\otimes J_{n/g}\otimes B+I_g\otimes J_{n/g}\otimes A+I_g\otimes I_{n/g}\otimes(2I_n-A)\bigr],\tag{3}Y=2n1​[(Jg​−Ig​)⊗Jn/g​⊗B+Ig​⊗Jn/g​⊗A+Ig​⊗In/g​⊗(2In​−A)],(3)

with A=∑i=1n/2aiCiA=\sum_{i=1}^{n/2}a_iC_iA=∑i=1n/2​ai​Ci​ and B=∑i=1n/2biCiB=\sum_{i=1}^{n/2}b_iC_iB=∑i=1n/2​bi​Ci​ for explicit trigonometric coefficients ai,bia_i,b_iai​,bi​ (coeffA, coeffB).

Formalization targets

Goal: Theorem 4.1

For every z∈Nz\in\mathbb Nz∈N and every choice of the indices r(n),s(n)r(n),s(n)r(n),s(n),

sup⁡n≥2, D metric on n+1 cities OPTTSP(D)OPTSDP(D) ≥ z.\sup_{n\ge2,\ D\ \text{metric on } n+1 \text{ cities}}\ \frac{\mathrm{OPT}_{\mathrm{TSP}}(D)}{\mathrm{OPT}_{\mathrm{SDP}}(D)}\ \ge\ z .n≥2, D metric on n+1 citiessup​ OPTSDP​(D)OPTTSP​(D)​ ≥ z.

It asserts only that the gap exceeds every integer, which is the paper's headline (Corollary 4.2: the gap is unbounded).

Milestones

  1. Feasibility of (3): Claims 4.5, 4.6, 4.7 and 4.12, Proposition 4.14, combined in Proposition 4.4, with the trigonometric Lemmas 4.8, 4.9, 4.10, 4.11, 4.13, 4.19, 4.20.
  2. The spectrum: Gray's Lemma 3.3 for circulant matrices, Claims 4.15, 4.17, 4.18.
  3. The objective: Theorem 4.21, 12trace⁡((D⊗C1)Y)≤c~g/n\tfrac12\operatorname{trace}((D\otimes C_1)Y)\le\tilde c_g/n21​trace((D⊗C1​)Y)≤c~g​/n for a constant chosen before nnn.
  4. The two halves of the final ratio: OPTTSP=g\mathrm{OPT}_{\mathrm{TSP}}=gOPTTSP​=g on the (n+1)(n+1)(n+1)-vertex instance, and the SDP (2) objective of YYY is at most c~g/n+2\tilde c_g/n+2c~g​/n+2 (equations (5)–(7)).

Significance

The theorem rules out the de Klerk–Sotirov SDP as a tool for proving any constant approximation ratio for the metric TSP in the way the subtour LP is used: there are metric instances whose optimal tour costs 2z2z2z while the SDP value stays below 2+ε2+\varepsilon2+ε. With the authors' earlier results, it completes the picture for every SDP relaxation of the TSP in Sotirov's survey: all have unbounded integrality gap, while the subtour LP, whose gap is at most 3/23/23/2, is exact on the simplicial instances. The construction also shows that SDP (2) is non-monotonic: adding vertices can lower its value.

All results are proved in the paper. None of them, nor any SDP relaxation of the TSP, the quadratic assignment problem or circulant spectra, is formalized on Prove2Me; the metric-TSP model (MetricTSP_model) is the only reused definition. The mission produces a machine-checked proof of the unbounded gap and, along the way, reusable facts about symmetric circulant matrices and Kronecker spectra.

Difficulty

Exhibiting a bad instance is not enough: one must certify that the SDP value is small, which needs an explicit feasible YYY and a proof that it is positive semidefinite. The natural first attempt, the two-group instances that already give an unbounded gap for SDP (1), yields only a gap of 222 for SDP (2) (§3 of the paper): the symmetry reduction adds the term trace⁡(Diag⁡(cˉ)Y)\operatorname{trace}(\operatorname{Diag}(\bar c)Y)trace(Diag(cˉ)Y), which the paper can only bound by a constant, not by o(1)o(1)o(1), so the tour cost must grow with the number of groups. With ggg groups the solution has three nested Kronecker levels and circulant blocks with trigonometric coefficients, and positive semidefiniteness reduces to sign conditions on cosine sums that must hold for every kkk, including the boundary indices.

Formalization scope

Cities and indices are 0-based Fin n; n2×n2n^2\times n^2n2×n2 matrices are indexed by Fin n × Fin n with the Kronecker block index first, and vec is Mathlib's column stacking. α,β\alpha,\betaα,β are Fin.succAbove r, Fin.succAbove s. Optimal values and the gap are in ℝ≥0∞: an infimum over an empty feasible set is ∞\infty∞, not a junk 000, and the SDP objective is nonnegative on metric instances. The indices r,sr,sr,s are arbitrary functions of the number of cities, so the goal cannot be met by choosing favourable indices. The section's standing assumptions (even g≥2g\ge2g≥2, g∣ng\mid ng∣n, g<ng<ng<n) are explicit hypotheses. The solution (3) is defined entrywise and proved equal to the Kronecker formula in the verification files; a sanity check evaluates the SDP (2) objective at a tour lift and recovers the tour cost, and the lift of a permutation is proved feasible, so the feasible set is nonempty.

Needed infrastructure: spectra of circulant matrices (discrete Fourier eigenvectors), eigenvalues of Kronecker products, positive semidefiniteness from an eigenbasis, finite cosine sums, and the optimal tour of a grouped 0/1 metric. The circulant and Kronecker results are reusable well beyond this mission. Contributions are welcome on any milestone; the trigonometric lemmas and Lemma 3.3 are independent entry points.

Selected references

  • S. C. Gutekunst and D. P. Williamson, Semidefinite programming relaxations of the traveling salesman problem and their integrality gaps, arXiv:1907.09054v1, 2019; Mathematics of Operations Research 47(1), 2022. https://arxiv.org/abs/1907.09054
  • E. de Klerk and R. Sotirov, Improved semidefinite programming bounds for quadratic assignment problems with suitable symmetry, Mathematical Programming 133, 2012. https://doi.org/10.1007/s10107-010-0437-5
  • J. Povh and F. Rendl, Copositive and semidefinite relaxations of the quadratic assignment problem, Discrete Optimization 6(3), 2009. https://doi.org/10.1016/j.disopt.2009.01.002
  • E. de Klerk, D. V. Pasechnik and R. Sotirov, On semidefinite programming relaxations of the traveling salesman problem, SIAM Journal on Optimization 19(4), 2008. https://doi.org/10.1137/070711141
  • S. C. Gutekunst and D. P. Williamson, The unbounded integrality gap of a semidefinite relaxation of the traveling salesman problem, SIAM Journal on Optimization 28(3), 2018. https://doi.org/10.1137/17M1154722
  • R. M. Gray, Toeplitz and circulant matrices: a review, Foundations and Trends in Communications and Information Theory 2(3), 2006. https://doi.org/10.1561/0100000006
37 thms2 active usersReviewed
Quantum Information·Captain: Gohan

Separability and entanglement of composite quantum systemsResearch Paper

Motivation

We provide a constructive algorithm to find the best separable approximation to an arbitrary density matrix of a composite quantum system of finite dimensions. The method leads to a condition of separability and to a measure of entanglement.

This mission is the statement-level formalization of Separability and entanglement of composite quantum systems (arXiv:quant-ph/9707043v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

11 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Unrestricted best separable approximation exists (Abstract and pp.2-3, unnumbered: unrestricted best separable approximation exists, PDF p. 2). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Deferred results

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

  • Theorem 1: BSA for any prescribed product-vector set V: An additional finiteness/closedness hypothesis on the allowed projectors ensuring attainment, or an explicit change from a maximum to a supremum; neither preserves the printed arbitrary-set result. (source-ambiguity)
  • Lemma 2, Eqs. (8a)-(8b): maximal pair formulas: A corrected complete pair-subtraction characterization with reciprocal in the orthogonal inverse-Gram case, boundary optima, and the singular-Gram/coincident-ray cases. These additions change the printed formulas. (source-ambiguity)
  • Theorem 2: pairwise maximality iff globally best separable approximation: A genuine global optimality certificate controlling simultaneous changes in all coefficients, or additional hypotheses making pairwise maximality sufficient. Pairwise maximality in the printed model is false as a certificate. (source-ambiguity)
  • Unnumbered geometric assertion before Eq. (11): A specified genericity notion and a corrected dimension threshold for a nonzero product-vector intersection; equality at (N-1)(M-1) cannot be retained. (source-ambiguity)
  • Eq. (11): literal uniqueness of every normalized component for every density matrix: Uniqueness of weighted operators, or uniqueness of normalized components restricted to strictly positive weights. The former is separately drafted; literal full-tuple uniqueness at endpoints is false. (source-ambiguity)
  • Abstract and conclusion: constructive pairwise algorithm for arbitrary dimensions: A specified iteration/stopping procedure with a valid proof that it attains the unrestricted optimum; finite sampling and the printed pairwise test do not provide this. (source-ambiguity)

Selected references

  • Separability and entanglement of composite quantum systems, arXiv:quant-ph/9707043v1, https://arxiv.org/abs/quant-ph/9707043v1
17 thms2 active usersReviewed
Quantum Information·Captain: Gohan

Entropic fluctuations of quantum dynamical semigroupsResearch Paper

Motivation

We study a class of finite dimensional quantum dynamical semigroups exp(tL) whose generators L are sums of Lindbladians satisfying the detailed balance condition. Such semigroup arise in the weak coupling (van Hove) limit of Hamiltonian dynamical systems describing open quantum systems out of equilibrium. We prove a general entropic fluctuation theorem for this class of semigroups by relating the cumulant generating function of entropy transport to the spectrum of a family of deformations of the generator L. We show that, besides the celebrated Evans-Searles symmetry, this cumulant generating function also satisfies the translation symmetry recently discovered by Andrieux et al., and that in the linear regime near equilibrium these two symmetries yield Kubo's and Onsager's linear response relations.

This mission is the statement-level formalization of Entropic fluctuations of quantum dynamical semigroups (arXiv:1305.4409v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

25 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Theorem 3.1 — full entropic fluctuation theorem (seed from abstract) (Theorem 3.1, PDF p. 7). The milestones are the other numbered results, in the paper's order, each quoting the paper.

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

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

Deferred results

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

  • §4(a)–(c) — microscopic time reversal implies generator time reversal: Microscopic antiunitary reservoir dynamics, GNS reference vectors, Fourier correlation spectra and Cauchy-principal-value transforms. (hard)
  • §5, (36) — two-measurement statistics and tilted dynamics: Countably discrete self-adjoint reservoir Hamiltonians with trace-class Gibbs operators and their analytically deformed full dynamics. (hard)
  • §5 — deformed weak-coupling dynamics limit: Explicit microscopic multi-time correlation decay hypotheses sufficient for the deformed Davies operator-norm limit. (source-ambiguity)
  • §5, (38) — microscopic counting-statistics scaling limit: Actual microscopic limiting FCS family and the deformed weak-coupling theorem under fully pinned hypotheses. (source-ambiguity)

Selected references

  • Entropic fluctuations of quantum dynamical semigroups, arXiv:1305.4409v2, https://arxiv.org/abs/1305.4409v2
36 thms2 active usersReviewed
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