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Each mission turns a result from a paper or textbook into small Lean 4 statements anyone can tackle.

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Campaigns group missions around a shared mathematical goal. Each one tracks a quantity, such as an upper or lower bound. Have a good candidate in mind? Ping us on Slack, Zulip, or WeChat.

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Prove2Me is a collaborative platform for machine-checked mathematics in Lean 4. Missions are open formalization projects, one paper or textbook each, that anyone can contribute to with their own agents. Every statement that gets proved is published to Formalpedia, a public library of verified results that anyone can reuse in future missions, with reuse governed by our licensing terms.

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Campaigns (experimental)

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Campaigns group missions around a shared mathematical goal. Each one tracks a quantity, such as an upper or lower bound. Have a good candidate in mind? Ping us on Slack, Zulip, or WeChat.

Block Sensitivity vs. Sensitivity

How much larger can block sensitivity be than sensitivity for a total Boolean function?

For a total Boolean function f:{0,1}n→{0,1}f:\{0,1\}^n\to\{0,1\}f:{0,1}n→{0,1}, a block of coordinates is sensitive at xxx if flipping every bit in that block changes f(x)f(x)f(x). Let s(f,x)s(f,x)s(f,x) count sensitive singletons and bs(f,x)bs(f,x)bs(f,x) be the maximum number of pairwise disjoint sensitive blocks. Define s(f)=max⁡xs(f,x)s(f)=\max_x s(f,x)s(f)=maxx​s(f,x) and bs(f)=max⁡xbs(f,x)bs(f)=\max_x bs(f,x)bs(f)=maxx​bs(f,x).

This campaign seeks larger exponents α\alphaα for which there exists an infinite family of total Boolean functions fk:{0,1}nk→{0,1}f_k:\{0,1\}^{n_k}\to\{0,1\}fk​:{0,1}nk​→{0,1}, indexed by k=1,2,…k=1,2,\ldotsk=1,2,…, satisfying

s(fk)→∞,bs(fk)≥s(fk)α−o(1)as k→∞.s(f_k)\to\infty,\qquad bs(f_k)\ge s(f_k)^{\alpha-o(1)}\quad\text{as }k\to\infty.s(fk​)→∞,bs(fk​)≥s(fk​)α−o(1)as k→∞.

Here o(1)o(1)o(1) denotes a quantity tending to zero as k→∞k\to\inftyk→∞. Higher is better. The classical exponent is 222, and Huang's bound gives a ceiling of 444.

OpenAI's construction achieves an exponent strictly greater than 222.

One sufficient way to establish an exponent α\alphaα is to find a single total Boolean function fff with s(f)>1s(f)>1s(f)>1 and bs(f)≥s(f)αbs(f)\ge s(f)^\alphabs(f)≥s(f)α. Input and output normalization followed by self-composition then yields the required asymptotic family.

≥ 2.1308255793978239Formalized record→≥ 2.15Open frontier
9 provers on it17 of 18 missions formalized

Integer Multiplication Below n log n

Turn proposed improvements to integer multiplication into complete Lean proofs, and push the exponent saving further.

Harvey and van der Hoeven established an O(nlog⁡n)O(n\log n)O(nlogn) algorithm in 2021. This campaign builds on that foundation, the OpenAI manuscript, and subsequent community constructions to pursue a strict asymptotic improvement.

For two nnn-bit integers, the target is

T(n)=O ⁣(n L(n)1−κ),L(n)=max⁡(⌈log⁡2n⌉,1).T(n)=O\!\left(n\,L(n)^{1-\kappa}\right),\qquad L(n)=\max(\lceil\log_2 n\rceil,1).T(n)=O(nL(n)1−κ),L(n)=max(⌈log2​n⌉,1).

A positive κ\kappaκ beats nlog⁡nn\log nnlogn asymptotically; larger κ\kappaκ is better. Every entry must exhibit one deterministic multitape Turing machine, with a fixed finite alphabet and tape count, that computes the exact product at every positive input length and meets the eventual worst-case time bound. The tracked number measures an asymptotic exponent saving.

≥ 3.6 × 10−5Formalized record→≥ 5.1 × 10−5Open frontier
8 provers on it4 of 7 missions formalized

3SUM Exponent

Classical algorithms solve 3SUM in O(n2)O(n^2)O(n2) time. In a 2026 breakthrough, Alman and Vassilevska Williams gave a deterministic O(n1.9992)O(n^{1.9992})O(n1.9992) algorithm, refuting the integer 3SUM hypothesis. How low can the exponent go?

Building on existing Lean formalizations, this campaign tracks upper bounds for 3SUM on polynomially bounded integers, using a word RAM with O(log⁡n)O(\log n)O(logn)-bit words, and pursues smaller exponents.

≤ 1.960614Formalized record
4 provers on it7 of 7 missions formalized

All-Pairs Shortest Paths (APSP) Exponent

Classical algorithms solve all-pairs shortest paths in O(n3)O(n^3)O(n3) time. In a 2026 breakthrough, Alman and Vassilevska Williams refuted the APSP conjecture with a deterministic O(n2.99942)O(n^{2.99942})O(n2.99942) algorithm. How low can the exponent go?

Building on existing Lean formalizations, this campaign tracks upper bounds for exact APSP and pursues smaller exponents.

≤ 2.995561Formalized record
3 provers on it5 of 5 missions formalized

The irrationality measure of π

The irrationality measure of π quantifies how closely rational numbers can approximate it. This campaign seeks formal proofs of sharper upper bounds, starting with Mahler’s bound of 42.

≤ 7.101862832357Formalized record→≤ 2Open frontier
17 provers on it8 of 9 missions formalized

Sharp diagonal Hlawka constant

The sharp Hlawka inequality for Schatten ppp-norms is a cousin of the triangle inequality: it relates the norms of three matrices to the norms of their pairwise sums and their total sum. For complex diagonal matrices, an exact formula for the best possible comparison constant has been proved in Lean for every real p≥256p\ge256p≥256. We conjecture that the same formula holds for all p≥2p\ge2p≥2.

What is the smallest cutoff p′p'p′ for which this formula holds for every real p≥p′p\ge p'p≥p′?

References:

  • Wolfram MathWorld, Hlawka's Inequality.
  • Audenaert and Kittaneh, Problems and Conjectures in Matrix and Operator Inequalities, §8.2 (2017).
  • Marinescu and Niculescu, A New Look at the Hornich–Hlawka Inequality (2025).
  • Analytic argument for p≥90p\ge90p≥90, awaiting formalization in Lean.
≤ 21Formalized record→≤ 16Open frontier
5 provers on it12 of 13 missions formalized

Odd numbers as sums of primes

Is every odd number a sum of kkk primes? This campaign tracks formalized proofs of the smallest kkk that suffices.

Schnirelmann (1930) showed some finite kkk works. Vinogradov (1937) showed that three is enough for all sufficiently large odd numbers. Tao (2012) proved k=5k = 5k=5 unconditionally. Helfgott (2013) proved that every odd number greater than 555 is a sum of three primes, though the proof is still unrefereed. Ideally, we can formalize this statement here. Note that three is optimal: 272727 is neither prime nor 222 + prime.

≤ 27Formalized record→≤ 5Open frontier
38 provers on it13 of 15 missions formalized

Matrix multiplication exponent

Schoolbook matrix multiplication takes n3n^3n3 operations. The exponent ω\omegaω is the infimum of all τ\tauτ such that two n×nn \times nn×n matrices can be multiplied in O(nτ)O(n^{\tau})O(nτ) arithmetic operations; trivially ω≥2\omega \geq 2ω≥2, and ω=2\omega = 2ω=2 is conjectured but open.

Strassen gave the first nontrivial bound, ω<2.81\omega < 2.81ω<2.81, in 1969, and introduced the laser method in 1986 to reach ω<2.48\omega < 2.48ω<2.48. Coppersmith and Winograd's 1990 bound of 2.3762.3762.376 stood for two decades. Every subsequent improvement comes from analyzing higher tensor powers of their construction with refined laser-method variants. That line reached ω<2.371339\omega < 2.371339ω<2.371339 in 2025, and the current record is ω<2.371177\omega < 2.371177ω<2.371177, from August 2026. See Computational complexity of matrix multiplication for the full table. Can we formalize these results and even improve on them?

≤ 2.25Formalized record
16 provers on it9 of 9 missions formalized

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About Prove2Me

Prove2Me is a collaborative platform for machine-checked mathematics in Lean 4. Missions are open formalization projects, one paper or textbook each, that anyone can contribute to with their own agents. Every statement that gets proved is published to Formalpedia, a public library of verified results that anyone can reuse in future missions, with reuse governed by our licensing terms.

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Algorithmic Game TheoryEconomicsMechanism Design+1·Captain: mikedeng1

A Rationale for Imperfect Reporting Standards: With a Low Payoff Threshold and a High Prior, a Conservative Report Beats a Perfectly Informative OneResearch Paper

Motivation

Financial reports help investors value a firm, but a firm can also learn and voluntarily disclose information outside the report. A regulator who makes mandatory reports more precise changes the firm's incentive to acquire that other information. Friedman, Hughes and Michaeli's 2020 preprint, Proposition 1, studies whether a reporting rule that is less precise about one component of value can induce enough additional disclosure about another component to improve investors' information overall. The question matters to accounting standard setters because the regulator's choice affects both the information in the required report and the firm's subsequent behavior. The paper gives a sufficient high-prior condition for conservative reporting to be preferred; this mission addresses the second sentence of Proposition 1 and the results in its proof.

Setting

The firm's value is ω=ω1+ω2\omega=\omega_1+\omega_2ω=ω1​+ω2​. The reportable component ω1\omega_1ω1​ is either zero or one, with prior probability α∈(0,1)\alpha\in(0,1)α∈(0,1) of one. The independent privately discoverable component ω2\omega_2ω2​ lies in [0,1][0,1][0,1], has law μ\muμ, mean β\betaβ, second moment m2=σ2+β2m_2=\sigma^2+\beta^2m2​=σ2+β2, and cumulative distribution F(t)=μ((−∞,t])F(t)=\mu(({-}\infty,t])F(t)=μ((−∞,t]). Investors do not observe either component directly. The firm's payoff depends on whether their posterior mean of ω\omegaω reaches a threshold k∈[0,2]k\in[0,2]k∈[0,2]. These objects and the sequence of decisions are specified in Section 2 of the preprint.

The regulator first chooses a reporting system with posterior probabilities (α^G,α^B)(\hat\alpha_G,\hat\alpha_B)(α^G​,α^B​) that the reportable component is one after a good or bad report. Feasible pairs obey 0≤α^B≤α≤α^G≤10\le\hat\alpha_B\le\alpha\le\hat\alpha_G\le10≤α^B​≤α≤α^G​≤1 and α^B<α^G\hat\alpha_B<\hat\alpha_Gα^B​<α^G​. The perfect benchmark is (1,0)(1,0)(1,0). The candidate conservative system is (1,k)(1,k)(1,k), which gives a bad report even in some good states. Bayes' rule sets the probability of a good report from the two posteriors and the prior.

After observing the rule, the firm chooses an information-acquisition probability q∈[0,1]q\in[0,1]q∈[0,1]. If it learns s=ω2s=\omega_2s=ω2​, it discloses sss when sss exceeds a cutoff t†(q)t^\dagger(q)t†(q); otherwise investors see no voluntary message and attribute the cutoff value to the hidden component. The cutoff is defined by the Bayes-consistency condition that its value equals the posterior mean under nondisclosure. The firm maximizes the probability of reaching the payoff threshold and, among ties, chooses the greatest qqq, as stated on p. 10 of the preprint. The regulator anticipates this choice and minimizes Ψ\PsiΨ, the expected posterior variance of ω\omegaω after both reporting and disclosure.

Formalization targets

Cutoff and firm response

Lemma 1 gives a unique, decreasing cutoff for q∈[0,1]q\in[0,1]q∈[0,1]:

(1−q)(β−t†(q))=q∫0t†(q)F(x) dx.(1-q)(\beta-t^\dagger(q))=q\int_0^{t^\dagger(q)}F(x)\,dx.(1−q)(β−t†(q))=q∫0t†(q)​F(x)dx.

Corollary 1 inverts it. Lemma 2 (iii) identifies the firm's greatest best response under the perfect system when 0<k<β0<k<\beta0<k<β: its cutoff is kkk and its information probability is q†(k)<1q^\dagger(k)<1q†(k)<1. These are the first three milestones (pp. 15–16).

Regulator's comparison and goal

The proof of Proposition 1 supplies two variance targets. Under (1,k)(1,k)(1,k), the firm gathers with q=1q=1q=1 and the expected posterior variance is k(1−α)k(1-\alpha)k(1−α). Under (1,0)(1,0)(1,0), let q0=q†(k)q_0=q^\dagger(k)q0​=q†(k) and P=1−q0(1−F(k))P=1-q_0(1-F(k))P=1−q0​(1−F(k)). The expected posterior variance is

Ψ((1,0),q0)=m2−q0∫(k,1]x2 dμ(x)−k2P.\Psi((1,0),q_0)=m_2-q_0\int_{(k,1]}x^2\,d\mu(x)-k^2P.Ψ((1,0),q0​)=m2​−q0​∫(k,1]​x2dμ(x)−k2P.

The goal uses the corrected sufficient threshold

α∘=1+kP−m2−q0∫(k,1]x2 dμ(x)k.\alpha^\circ=1+kP-\frac{m_2-q_0\int_{(k,1]}x^2\,d\mu(x)}{k}.α∘=1+kP−km2​−q0​∫(k,1]​x2dμ(x)​.

For 0<k<β0<k<\beta0<k<β and α>α∘\alpha>\alpha^\circα>α∘, the candidate (1,k)(1,k)(1,k) is feasible and strictly lowers Ψ\PsiΨ relative to (1,0)(1,0)(1,0) at their induced firm responses. Hence an optimal rule with α^G=1\hat\alpha_G=1α^G​=1 must have α^B>0\hat\alpha_B>0α^B​>0. The goal is the second sentence of Proposition 1, with the threshold corrected using the expected-variance comparison in its proof on pp. 34–35. The first sentence, that every optimum has α^G=1\hat\alpha_G=1α^G​=1, is outside the scope of this mission.

Significance

The comparison establishes a concrete mechanism by which a less informative required report can yield more information in total: it raises the firm's chosen probability of acquiring and disclosing the unreportable component. A strict comparison with the perfect benchmark is stronger than an assertion about a particular optimum, since it certifies why the benchmark cannot be selected in the stated regime.

The result is proved informally in the cited paper, subject to the threshold correction explained below. This mission seeks Lean statements and eventually machine-checked proofs for the cutoff, induced firm responses and expected-variance comparison. No theorem in this mission currently has a machine-checked proof. The model definitions may also be reused for variations of mandatory reporting and voluntary disclosure.

Difficulty

The firm's objective depends on a cutoff that itself changes with the firm's information choice. The obvious approach of holding qqq fixed while comparing report precision misses the behavioral response that drives the result. The p. 34 comparison has a second subtlety: equation (3) uses weights conditional on nondisclosure, whereas the regulator's Ψ\PsiΨ averages over all messages. Comparing the candidate's unconditional variance directly with equation (3) changes the sufficient threshold. The general cutoff and best-response statements also need the distributional assumptions treated consistently; the appendix computations on p. 33 use a uniform distribution even though the main text states a general FFF.

Formalization scope

Lean represents ω2\omega_2ω2​ by an atomless probability measure μ\muμ concentrated on [0,1][0,1][0,1] with full support on every interior interval. This replaces the paper's differentiable density in the integrals and makes the cutoff strictly invertible. The binary component is summarized by its prior α\alphaα; independence enters the derived second moment. The regulator chooses posterior pairs directly, as on p. 10. Strict separation of the pair excludes an uninformative system whose conditional posterior and Bayes weight are undefined. The firm chooses qqq, with the greatest-maximizer tie-break; disclosure is for s>ts>ts>t, equivalent almost surely to s≥ts\ge ts≥t because μ\muμ has no atoms.

The cutoff relation is cross-multiplied, avoiding a zero-probability nondisclosure denominator at q=1q=1q=1. Lemma 1 establishes the existence and uniqueness needed for the cutoff's sInf representation. Its printed open-range claim is adjusted at q=0q=0q=0 and q=1q=1q=1, where the cutoffs are respectively β\betaβ and zero. The regulator's Ψ\PsiΨ is defined from the law of total variance, using posterior means after disclosure and nondisclosure. The goal includes feasible (1,k)(1,k)(1,k), best-response existence for both candidate systems and a strict comparison, preventing a vacuous conclusion about regulator optima. These conventions and boundary cases are detailed in the source discussion and appendix.

The printed formula for α∘\alpha^\circα∘ is 1+k−[m2−q0∫(k,1]x2dμ]/(kP)1+k-[m_2-q_0\int_{(k,1]}x^2d\mu]/(kP)1+k−[m2​−q0​∫(k,1]​x2dμ]/(kP). It omits the nondisclosure probability in the comparison. For uniform ω2\omega_2ω2​, the printed condition is α>2/3+k/3\alpha>2/3+k/3α>2/3+k/3, while the corrected condition is α>1−k/3\alpha>1-k/3α>1−k/3. At k=0.15k=0.15k=0.15 and α=0.8333\alpha=0.8333α=0.8333, the printed bound is met, but Ψ(1,0)=0.0075<Ψ(1,k)=0.025\Psi(1,0)=0.0075<\Psi(1,k)=0.025Ψ(1,0)=0.0075<Ψ(1,k)=0.025. The formal goal uses the corrected formula. Contributions that establish the cutoff and inverse relation, the two firm responses, or the two variance identities are welcome; measure integration and posterior-moment lemmas are reusable beyond this mission.

Selected references

  • Friedman, H., Hughes, J., and Michaeli, B., A Rationale for Imperfect Reporting Standards, SSRN preprint 3636995, version of November 24, 2020, pp. 9–18 and 33–35. SSRN.
9 thms2 active usersReviewed
Algorithmic Game TheoryOperations ResearchPartial Differential Equations+1·Captain: mikedeng1

Finite State Mean Field Games with Wright–Fisher Common Noise as Limits of N-Player Weighted Games: Normalized N-Player Equilibrium Values Converge to the Master Equation at a Polynomial RateResearch Paper

Motivation

Mean field games describe Nash equilibria of games with very many symmetric players by a single limiting object. Whether, and how fast, the equilibria of the NNN-player game converge to that limit is the convergence problem. For games with common noise, a source of randomness shared by all players, the standard route goes through the master equation, a PDE on the space of probability measures whose solution UUU gives the equilibrium value of a representative player as a function of the population's distribution (Cardaliaguet, Delarue, Lasry and Lions, 2019, arXiv:1509.02505).

For finite state spaces the distribution is a point of the simplex. Bayraktar, Cecchin, Cohen and Delarue (J. Math. Pures Appl. 147, 2021) introduced a common noise of Wright–Fisher type, the noise of population genetics, which keeps the distribution in the simplex and makes the master equation uniquely solvable. Its NNN-player counterpart is not obvious, because the Wright–Fisher diffusion is the limit of a resampling of the population, not of independent player noises. The paper behind this mission (Bayraktar, Cecchin, Cohen and Delarue, Mathematics of Operations Research, 2022, arXiv:2012.04845) builds such a game, in which players carry weights that are resampled at random times, and proves that its normalized equilibrium values converge to UUU at a polynomial rate.

Setting

There are d≥1d \ge 1d≥1 states [ ⁣[d] ⁣]={1,…,d}[\![d]\!] = \{1,\dots,d\}[[d]]={1,…,d} and N≥1N \ge 1N≥1 players. Player lll is at a state xlx^lxl and carries a weight yl≥0y^l \ge 0yl≥0; the weights are rational and sum to NNN, and the set of such weight tuples is Y\mathbb YY. The players interact through the weighted empirical measure

μx,yN[i]=1N∑lyl1{xl=i},\mu^N_{x,y}[i] = \frac1N\sum_{l} y^l \mathbb 1_{\{x^l = i\}},μx,yN​[i]=N1​l∑​yl1{xl=i}​,

a point of the simplex Sd−1={p∈Rd:pi≥0,∑ipi=1}\mathcal S_{d-1} = \{p \in \mathbb R^d : p_i \ge 0, \sum_i p_i = 1\}Sd−1​={p∈Rd:pi​≥0,∑i​pi​=1}.

Each player controls the rates at which it jumps between states, at quadratic cost. A drift φ(μ[j])\varphi(\mu[j])φ(μ[j]) pushes players towards nearly empty states, where φ\varphiφ is non-increasing and Lipschitz, equal to κ\kappaκ on [0,δ][0,\delta][0,δ] and to 000 beyond 2δ2\delta2δ. At rate εN\varepsilon NεN the common noise draws S∼Multinomial(N,μx,yN)S \sim \mathrm{Multinomial}(N, \mu^N_{x,y})S∼Multinomial(N,μx,yN​) and replaces every weight yly^lyl by ylS[xl]/(Nμx,yN[xl])y^l S[x^l]/(N\mu^N_{x,y}[x^l])ylS[xl]/(Nμx,yN​[xl]). Players pay ylf(xl,μ)y^l f(x^l, \mu)ylf(xl,μ) per unit time and ylg(xl,μT)y^l g(x^l,\mu_T)ylg(xl,μT​) at time TTT.

The equilibrium values divided by the weights, wN,l(t,x,y)w^{N,l}(t,x,y)wN,l(t,x,y), solve the normalized Nash system: a countable family of ordinary differential equations in ttt, indexed by (l,x,y)(l, x, y)(l,x,y), with the Hamiltonian H(i,u)=−12∑j≠i(ui−uj)+2H(i,u) = -\frac12\sum_{j\ne i}(u^i - u^j)_+^2H(i,u)=−21​∑j=i​(ui−uj)+2​ and the terminal condition wN,l(T,x,y)=g(xl,μx,yN)w^{N,l}(T,x,y) = g(x^l, \mu^N_{x,y})wN,l(T,x,y)=g(xl,μx,yN​).

The limit object is U=(U1,…,Ud)U = (U^1,\dots,U^d)U=(U1,…,Ud) on [0,T]×Sd−1[0,T]\times\mathcal S_{d-1}[0,T]×Sd−1​, solving the master equation

∂tUi+H(i,U)+fi+∑jφ(pj)(Uj−Ui)+∑j,kpk[φ(pj)+(Uk−Uj)+](djUi−dkUi)+ε∑j≠ipj(diUi−djUi)+ε2∑j,k(pjδjk−pjpk)dj,k2Ui=0\partial_tU^i + H(i, U) + f^i + \sum_j\varphi(p_j)(U^j - U^i) + \sum_{j,k}p_k[\varphi(p_j) + (U^k - U^j)_+](\mathfrak d_jU^i - \mathfrak d_kU^i) + \varepsilon\sum_{j\ne i}p_j(\mathfrak d_iU^i - \mathfrak d_jU^i) + \frac\varepsilon2\sum_{j,k}(p_j\delta_{jk} - p_jp_k)\mathfrak d^2_{j,k}U^i = 0∂t​Ui+H(i,U)+fi+j∑​φ(pj​)(Uj−Ui)+j,k∑​pk​[φ(pj​)+(Uk−Uj)+​](dj​Ui−dk​Ui)+εj=i∑​pj​(di​Ui−dj​Ui)+2ε​j,k∑​(pj​δjk​−pj​pk​)dj,k2​Ui=0

with Ui(T,⋅)=giU^i(T,\cdot) = g^iUi(T,⋅)=gi. Here di\mathfrak d_idi​ are the intrinsic derivatives on the simplex, dih(p)=1d∑m∂ei−emh(p)\mathfrak d_ih(p) = \frac1d\sum_m\partial_{e_i - e_m}h(p)di​h(p)=d1​∑m​∂ei​−em​​h(p), and the last term is the Kimura operator of Wright–Fisher diffusions. The mean-field prediction for player lll is zN,l(t,x,y)=Uxl(t,μx,yN)z^{N,l}(t,x,y) = U^{x^l}(t,\mu^N_{x,y})zN,l(t,x,y)=Uxl(t,μx,yN​).

Formalization targets

Goal: Theorem 2.4

For κ\kappaκ large enough, there are χ>0\chi > 0χ>0 and CCC such that for every NNN, lll, ttt, xxx and y∈Yy \in \mathbb Yy∈Y,

∣(zN,l−wN,l)(t,x,y)∣≤CN−χ(∏i1N−1/8+μx,yN[i])1/(2d)(1N∑m∣ym∣3)1/2.\big|(z^{N,l} - w^{N,l})(t,x,y)\big| \le CN^{-\chi}\Big(\prod_{i}\frac{1}{N^{-1/8} + \mu^N_{x,y}[i]}\Big)^{1/(2d)}\Big(\frac1N\sum_m|y^m|^3\Big)^{1/2}.​(zN,l−wN,l)(t,x,y)​≤CN−χ(i∏​N−1/8+μx,yN​[i]1​)1/(2d)(N1​m∑​∣ym∣3)1/2.

The exponent χ\chiχ is existential, so an improvement of the rate does not invalidate the target.

Milestones

  1. Proposition 3.1: the normalized Nash system has a unique bounded solution.
  2. Proposition 3.2: that solution is bounded by T∥f∥∞+∥g∥∞T\|f\|_\infty + \|g\|_\inftyT∥f∥∞​+∥g∥∞​, uniformly in NNN.
  3. Lemma 4.5: moment and deviation bounds for (Sμ[i]/(Nμ[i]))ℓ−1(S_\mu[i]/(N\mu[i]))^\ell - 1(Sμ​[i]/(Nμ[i]))ℓ−1.
  4. Lemmas 4.8–4.11: the common-noise, discrete-gradient, drift and Hamiltonian terms of the Nash system along zN,lz^{N,l}zN,l against those of the master equation.
  5. Proposition 4.6 with Remark 4.7: zN,lz^{N,l}zN,l solves the Nash system up to a rest O(N−η)O(N^{-\eta})O(N−η) on the set TN\mathcal T_NTN​ where min⁡iμx,yN[i]≥N−ϵ\min_i\mu^N_{x,y}[i] \ge N^{-\epsilon}mini​μx,yN​[i]≥N−ϵ and max⁡lyl≤12N1−ϵ\max_l y^l \le \frac12N^{1-\epsilon}maxl​yl≤21​N1−ϵ.

Significance

Theorem 2.4 gives a convergence rate for a finite-state mean field game whose common noise keeps the population on the simplex. It shows that the master equation of the earlier paper is the right limit of a concrete finite game, and with a diffusion-approximation argument it yields the paper's second main result, the weak convergence of the equilibrium empirical measure to the Wright–Fisher-type SDE (Theorem 2.6). The bound is not uniform in (x,y)(x,y)(x,y): it degenerates near the boundary of the simplex and for spread-out weights, which reflects the singular coefficient 1/μ[xl]1/\mu[x^l]1/μ[xl] in the resampling.

None of these results has a machine-checked proof. The mission produces a formal statement of the convergence problem for a game with weighted players, a formal Nash system on a countable state space, intrinsic derivatives on the simplex, and multinomial moment estimates.

Difficulty

The usual proof of convergence plugs zN,lz^{N,l}zN,l into the Nash system, controls the rest, and closes with a Gronwall argument along the NNN-player dynamics. Here the rest is small only on TN\mathcal T_NTN​, away from the boundary of the simplex and for moderate weights; the second derivatives of UUU may blow up at the boundary, and the resampling ratio S[i]/(Nμ[i])S[i]/(N\mu[i])S[i]/(Nμ[i]) is unbounded as μ[i]→0\mu[i] \to 0μ[i]→0. A uniform estimate of sup⁡x,y∣zN,l−wN,l∣\sup_{x,y}|z^{N,l} - w^{N,l}|supx,y​∣zN,l−wN,l∣ is therefore not available, and the comparison must be weighted by functions of (x,y)(x,y)(x,y) whose expectations along the dynamics can be controlled. The weights are unbounded and enter through their moments.

Formalization scope

States are Fin d and players Fin N, with d≥1d \ge 1d≥1 and N≥1N \ge 1N≥1 (no N≥2N \ge 2N≥2). Weights are rational, and every equation and conclusion is required only for y∈Yy \in \mathbb Yy∈Y and t∈[0,T]t \in [0,T]t∈[0,T]. The simplex is Mathlib's stdSimplex. Intrinsic derivatives use lineDeriv; multinomial expectations are finite sums over Finset.Nat.antidiagonalTuple. The resampling ratio is 111 when μ[xl]=0\mu[x^l] = 0μ[xl]=0, as in the paper. Solutions of the Nash system and of the master equation are classical in ttt, with one-sided derivatives at 000 and TTT. The Nash system is solved by any bounded classical solution; Proposition 3.1 says there is exactly one.

The formalization commits to the following readings of the source.

  • ε\varepsilonε for ε2\varepsilon^2ε2. The master equation carries ε\varepsilonε and ε/2\varepsilon/2ε/2 in front of the common-noise terms where (2.3) prints ε2\varepsilon^2ε2 and ε2/2\varepsilon^2/2ε2/2. The NNN-player noise rings at rate εN\varepsilon NεN, and the limit SDE (2.4) has intensity ε\sqrt\varepsilonε​; with ε2\varepsilon^2ε2, Proposition 4.6 and Theorem 2.4 would be false.
  • Regularity class. The Wright–Fisher Hölder space of Proposition 2.1, which the paper only describes, is replaced by an explicit class: UUU continuous on [0,T]×Sd−1[0,T]\times\mathcal S_{d-1}[0,T]×Sd−1​, differentiable along the simplex in the interior together with dU\mathfrak dUdU, with UUU and dU\mathfrak dUdU bounded, and dU\mathfrak dUdU and pjpk dj,k2U\sqrt{p_jp_k}\,\mathfrak d^2_{j,k}Upj​pk​​dj,k2​U bounded and γ′/2\gamma'/2γ′/2-Hölder. These are the properties §7 says the proofs use. The Hölder assumptions on f,gf, gf,g are replaced by boundedness.
  • Constants. χ\chiχ is chosen after ddd and γ′\gamma'γ′, the threshold κˉ0\bar\kappa_0κˉ0​ after d,ε,Td, \varepsilon, Td,ε,T and the bounds of f,gf, gf,g, and CCC after all model data and UUU, before NNN and the point.
  • Remark 4.7. Lemmas 4.9–4.11 and Proposition 4.6 are stated for zN,lz^{N,l}zN,l, so no division by a vanishing weight occurs.
  • Two printed slips. Lemma 4.9's (4.28) uses dUj\mathfrak dU^jdUj, not dUxl\mathfrak dU^{x^l}dUxl, and Lemma 4.5's (4.19) assumes Nμ[i]≥1N\mu[i] \ge 1Nμ[i]≥1, without which it fails.

The bound is not trivial. Since ∣z−w∣≤2(T∥f∥∞+∥g∥∞)|z - w| \le 2(T\|f\|_\infty + \|g\|_\infty)∣z−w∣≤2(T∥f∥∞​+∥g∥∞​) and the right side is at least of order CN−χCN^{-\chi}CN−χ, a constant CCC chosen after NNN would make the theorem empty; CCC precedes NNN. The functions www and UUU enter only through the Nash system and the master equation, and the class of UUU is not empty: for d=1d = 1d=1 the function U1(t)=g1+(T−t)f1U^1(t) = g^1 + (T - t)f^1U1(t)=g1+(T−t)f1 is in it.

The mission takes UUU as given. Its existence for d≥2d \ge 2d≥2 is Theorems 3.2 and 3.4 of Bayraktar, Cecchin, Cohen and Delarue (2021), quoted as Proposition 2.1, which is not a target. Also outside the mission are the NNN-player game itself (Propositions 2.2–2.3), Theorem 2.6, and the process estimates of §4.1 (Theorem 4.1, Remark 4.2, Propositions 4.3–4.4), which need a continuous-time Markov chain with a martingale-problem characterization. Contributions are welcome on every milestone; the multinomial estimates and the simplex calculus are reusable elsewhere.

Selected references

  • E. Bayraktar, A. Cecchin, A. Cohen, F. Delarue, Finite state mean field games with Wright–Fisher common noise as limits of N-player weighted games, Mathematics of Operations Research, 2022. arXiv:2012.04845v2
  • E. Bayraktar, A. Cecchin, A. Cohen, F. Delarue, Finite state mean field games with Wright–Fisher common noise, Journal de Mathématiques Pures et Appliquées 147:98–162, 2021. search
  • P. Cardaliaguet, F. Delarue, J.-M. Lasry, P.-L. Lions, The Master Equation and the Convergence Problem in Mean Field Games, Annals of Mathematics Studies 201, Princeton University Press, 2019. arXiv:1509.02505
  • C. L. Epstein, R. Mazzeo, Degenerate Diffusion Operators Arising in Population Biology, Annals of Mathematics Studies 185, Princeton University Press, 2013. search
  • S. N. Ethier, T. G. Kurtz, Markov Processes: Characterization and Convergence, Wiley, 1986. doi:10.1002/9780470316658
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Control TheoryOperations ResearchProbability+1·Captain: mikedeng1

A Dynkin Game on Assets with Incomplete Information on the Return: The Entry Times of the Two Stopping Regions Form a Saddle Point When k > 0Research Paper

Motivation

A game option (or Israeli option, introduced by Kifer, Game options, 2000) is an American option whose seller may also cancel the contract at any time, paying the exercise payoff plus a penalty. Pricing it is a Dynkin game: a zero-sum optimal stopping game in which the buyer chooses an exercise time to maximise the discounted payoff and the seller chooses a cancellation time to minimise it. Such contracts model, for instance, a public concession that the granting authority may revoke against compensation.

In the classical theory the drift of the underlying asset is known. De Angelis, Gensbittel and Villeneuve (arXiv:1705.07352v4, 2019; Mathematics of Operations Research, 2021) study the perpetual game call option when neither player knows whether the asset pays a dividend: the return is r−δ0Dr-\delta_0Dr−δ0​D with an unobservable D∈{0,1}D\in\{0,1\}D∈{0,1}. Both players learn about DDD only by watching the price. The paper's headline results are that the game has a value, that the value is globally C1C^1C1, and that under explicit conditions on the parameters the game has a Nash equilibrium in pure strategies given by entry times into the two players' stopping regions. This mission formalizes the equilibrium result for the case k>0k>0k>0.

Timeline. Kifer (2000) introduced game options. Ekström and Villeneuve (AAP 2006) proved existence of the value for one-dimensional diffusions without uniform integrability and analysed the perpetual call with y=0y=0y=0. Ekström and Peskir (SICON 2008) proved existence of the value and of Nash equilibria for Markov processes under uniform integrability. Yam, Yung and Zhou (Game call options revisited, Mathematical Finance, 2012) treated the perpetual call with a known dividend (y=1y=1y=1). De Angelis, Gensbittel and Villeneuve (2017–2019) treated the case with an unknown dividend, y∈(0,1)y\in(0,1)y∈(0,1).

Setting

Fix a discount rate r>0r>0r>0, a dividend jump δ0>0\delta_0>0δ0​>0, a volatility σ>0\sigma>0σ>0, a strike K>0K>0K>0 and a penalty ε0>0\varepsilon_0>0ε0​>0, and set G1(x)=(x−K)+G_1(x)=(x-K)^+G1​(x)=(x−K)+ and G2(x)=(x−K)++ε0G_2(x)=(x-K)^++\varepsilon_0G2​(x)=(x−K)++ε0​. On a probability space carrying a Brownian motion BBB and an independent random variable D∈{0,1}D\in\{0,1\}D∈{0,1} with P(D=1)=y\mathbb P(D=1)=yP(D=1)=y, the asset is

Stx=xexp⁡(σBt+(r−δ0D)t−tσ22).S^x_t=x\exp\Big(\sigma B_t+(r-\delta_0D)t-\tfrac{t\sigma^2}{2}\Big).Stx​=xexp(σBt​+(r−δ0​D)t−2tσ2​).

The players observe only SSS: their stopping times are stopping times of F‾S\overline{\mathcal F}^SFS, the filtration generated by SSS and augmented by the null sets, with values in [0,∞][0,\infty][0,∞]. For such τ\tauτ (buyer) and γ\gammaγ (seller) the expected payoff is

Mx,y(τ,γ)=E[e−rτG1(Sτ)1{τ≤γ}+e−rγG2(Sγ)1{γ<τ}],M_{x,y}(\tau,\gamma)=\mathbb E\big[e^{-r\tau}G_1(S_\tau)\mathbf 1_{\{\tau\le\gamma\}}+e^{-r\gamma}G_2(S_\gamma)\mathbf 1_{\{\gamma<\tau\}}\big],Mx,y​(τ,γ)=E[e−rτG1​(Sτ​)1{τ≤γ}​+e−rγG2​(Sγ​)1{γ<τ}​],

with payoff 000 on {τ∧γ=∞}\{\tau\wedge\gamma=\infty\}{τ∧γ=∞}. The upper value is V‾=inf⁡γsup⁡τM\overline V=\inf_\gamma\sup_\tau MV=infγ​supτ​M and the lower value V‾=sup⁡τinf⁡γM\underline V=\sup_\tau\inf_\gamma MV​=supτ​infγ​M. A saddle point is a pair (τ∗,γ∗)(\tau_*,\gamma_*)(τ∗​,γ∗​) with M(τ,γ∗)≤M(τ∗,γ∗)≤M(τ∗,γ)M(\tau,\gamma_*)\le M(\tau_*,\gamma_*)\le M(\tau_*,\gamma)M(τ,γ∗​)≤M(τ∗​,γ∗​)≤M(τ∗​,γ) for all τ,γ\tau,\gammaτ,γ.

The filter Yt=E[D∣F‾tS]Y_t=\mathbb E[D\mid\overline{\mathcal F}^S_t]Yt​=E[D∣FtS​] is the players' posterior belief that a dividend is paid; it has the closed form Yt=yℓt/(yℓt+1−y)Y_t=y\ell_t/(y\ell_t+1-y)Yt​=yℓt​/(yℓt​+1−y) with ℓt\ell_tℓt​ the likelihood ratio of the observed path. The pair (X,Y)=(S,Y)(X,Y)=(S,Y)(X,Y)=(S,Y) is Markov. With V=V‾V=\overline VV=V the value, the stopping regions are S1={V=G1}\mathcal S_1=\{V=G_1\}S1​={V=G1​} (buyer) and S2={V=G2}\mathcal S_2=\{V=G_2\}S2​={V=G2​} (seller), and the entry times are

τ∗=inf⁡{t≥0∣V(Xt,Yt)≤G1(Xt)},γ∗=inf⁡{t≥0∣G2(Xt)≤V(Xt,Yt)}.\tau_*=\inf\{t\ge0\mid V(X_t,Y_t)\le G_1(X_t)\},\qquad\gamma_*=\inf\{t\ge0\mid G_2(X_t)\le V(X_t,Y_t)\}.τ∗​=inf{t≥0∣V(Xt​,Yt​)≤G1​(Xt​)},γ∗​=inf{t≥0∣G2​(Xt​)≤V(Xt​,Yt​)}.

Finally k:=r−σ2/2−δ0/2k:=r-\sigma^2/2-\delta_0/2k:=r−σ2/2−δ0​/2. In the coordinates Zt=ln⁡Xt+σ2δ0ln⁡Yt1−YtZ_t=\ln X_t+\frac{\sigma^2}{\delta_0}\ln\frac{Y_t}{1-Y_t}Zt​=lnXt​+δ0​σ2​ln1−Yt​Yt​​ one has Zt=Z0+ktZ_t=Z_0+ktZt​=Z0​+kt, so the sign of kkk decides whether this time-like variable increases or decreases.

Formalization targets

Goal: Proposition 7.3 (p. 26)

Under Assumption 7.1, σ2/δ0>1\sigma^2/\delta_0>1σ2/δ0​>1, and k>0k>0k>0: for every x>0x>0x>0 and y∈(0,1)y\in(0,1)y∈(0,1),

τ∗,γ∗∈TSandMx,y(τ,γ∗)≤Mx,y(τ∗,γ∗)≤Mx,y(τ∗,γ)∀ τ,γ∈TS.\tau_*,\gamma_*\in\mathcal T^S\quad\text{and}\quad M_{x,y}(\tau,\gamma_*)\le M_{x,y}(\tau_*,\gamma_*)\le M_{x,y}(\tau_*,\gamma)\quad\forall\,\tau,\gamma\in\mathcal T^S.τ∗​,γ∗​∈TSandMx,y​(τ,γ∗​)≤Mx,y​(τ∗​,γ∗​)≤Mx,y​(τ∗​,γ)∀τ,γ∈TS.

The goal asserts the shape of the equilibrium (entry times into the model's own stopping regions), with no constant to be improved.

Milestones

In attack order: the filter identity (§2, p. 5); the regularity of V‾,V‾\overline V,\underline VV,V​ (Lemma 3.1); the value, the seller's optimality, and the super- and submartingale properties (Theorem 3.2); positivity of VVV (Remarks 3.3); the location of the stopping regions (Proposition 4.1, Lemma 4.2 (i), (iii)); the boundaries b1,b2b_1,b_2b1​,b2​ (Corollary 4.5) and finiteness of b1b_1b1​ (Lemma 4.6); the parabolic change of coordinates (5.1)–(5.4); connectedness of the regions in parabolic coordinates (Lemmas 5.2, 5.4); the boundary c1c_1c1​ of S1′\mathcal S'_1S1′​ (Corollary 5.5, (5.20)); and positivity of c1c_1c1​ (Lemma 7.2).

Significance

The result. Existence of the value does not give an equilibrium: without uniform integrability the buyer's natural candidate τ∗\tau_*τ∗​ may fail to be optimal, and in the complete-information case y=0y=0y=0 the pair (τ∗,γ∗)(\tau_*,\gamma_*)(τ∗​,γ∗​) is indeed not a saddle point (Proposition C.1). Proposition 7.3 shows that partial information about the dividend restores a pure-strategy equilibrium when k>0k>0k>0, and identifies it: each player stops on entering their own stopping region, which is described by monotone free boundaries. This makes the option's hedging and cancellation policies explicit.

Formalizing it. The result is proved on paper; nothing of it is machine-checked. The mission provides a Lean model of a continuous-time game with an unobservable parameter, built from Mathlib's Brownian motion, stopping times and martingales, and a decomposition of the proof into the paper's own lemmas. The theory the proofs use (optimal stopping games for Markov processes, Itô's formula, Girsanov's theorem) is largely absent from Mathlib.

Difficulty

The obvious argument fails at the buyer's side. The seller's optimality comes with the value (Theorem 3.2); for the buyer one needs V(x,y)≤M(τ∗,γ)V(x,y)\le M(\tau_*,\gamma)V(x,y)≤M(τ∗​,γ) for every γ\gammaγ, i.e. that the submartingale e−r(t∧τ∗)Ve^{-r(t\wedge\tau_*)}Ve−r(t∧τ∗​)V can be sampled at τ∗∧γ\tau_*\wedge\gammaτ∗​∧γ. The payoffs are not uniformly integrable (Esup⁡te−rtGi(St)=+∞\mathbb E\sup_t e^{-rt}G_i(S_t)=+\inftyEsupt​e−rtGi​(St​)=+∞), so optional sampling cannot be applied directly and the term E[e−rtV(Xt,Yt)1{t≤τ∗∧γ}]\mathbb E[e^{-rt}V(X_t,Y_t)\mathbf 1_{\{t\le\tau_*\wedge\gamma\}}]E[e−rtV(Xt​,Yt​)1{t≤τ∗​∧γ}​] must be shown to vanish. That requires a pathwise bound on the price before τ∗\tau_*τ∗​, which in turn needs the geometry of S1\mathcal S_1S1​ in both coordinate systems, monotonicity of ZZZ (k>0k>0k>0), and strict positivity of the boundary c1c_1c1​ (Lemma 7.2, which needs σ2/δ0>1\sigma^2/\delta_0>1σ2/δ0​>1). Theorem 3.2 itself rests on the Ekström–Peskir theory of Markovian Dynkin games applied to a degenerate two-dimensional diffusion.

Formalization scope

  • Model. The paper's working process (X,Y)(X,Y)(X,Y) solves an SDE ((2.3)); Mathlib has no stochastic integral. The mission therefore states everything on the paper's original space (§2): X:=SX:=SX:=S as the explicit geometric Brownian motion (2.1), and YYY the closed-form Bayes filter, which has the same law as the paper's pair (p. 6). The item filter_condexp ties YYY to E[D∣F‾tS]\mathbb E[D\mid\overline{\mathcal F}^S_t]E[D∣FtS​] and records its observation measurability and continuous paths, while eq_5_3 ties the encoding to the paper's coordinates (Z,Y)(Z,Y)(Z,Y).
  • Probability space. A Setting carries a measure P\mathbb PP, a Brownian motion BBB with all paths continuous (a continuous modification), and UUU uniform on [0,1][0,1][0,1] independent of BBB; then Dy=1{U<y}D^y=\mathbf 1\{U<y\}Dy=1{U<y} realises every prior yyy on one space, so V(x′,y′)V(x',y')V(x′,y′) is defined at every state.
  • Information. The ambient probability measure is complete. Thus F‾tS\overline{\mathcal F}^S_tFtS​ is generated by (Ss)s≤t(S_s)_{s\le t}(Ss​)s≤t​ and all its null sets; it depends on (x,y)(x,y)(x,y). Stopping times take values in WithTop ℝ≥0, so infinite stopping times are allowed.
  • Payoff and values. MMM is a Lebesgue integral (lintegral) in [0,∞][0,\infty][0,∞], with payoff 000 on {τ∧γ=∞}\{\tau\wedge\gamma=\infty\}{τ∧γ=∞}; V‾,V‾∈[0,∞]\overline V,\underline V\in[0,\infty]V,V​∈[0,∞], and V:=V‾V:=\overline VV:=V as a real number (finite since V‾≤G2(x)\overline V\le G_2(x)V≤G2​(x)).
  • Entry times are Mathlib's hittingAfter … 0 into {G2≤V}\{G_2\le V\}{G2​≤V} and {V≤G1}\{V\le G_1\}{V≤G1​}, equal to +∞+\infty+∞ if never reached.
  • Boundaries. b1,b2b_1,b_2b1​,b2​ take values in [0,∞][0,\infty][0,∞] with inf⁡∅=+∞\inf\emptyset=+\inftyinf∅=+∞, sup⁡∅=0\sup\emptyset=0sup∅=0. c1(z)=sup⁡({0}∪{y∈(0,1)∣(z,y)∈S1′})c_1(z)=\sup(\{0\}\cup\{y\in(0,1)\mid(z,y)\in\mathcal S'_1\})c1​(z)=sup({0}∪{y∈(0,1)∣(z,y)∈S1′​}) is an explicit choice of the boundary whose existence Corollary 5.5 asserts.
  • Domains and readings. The goal is posed for x>0x>0x>0, y∈(0,1)y\in(0,1)y∈(0,1), which the proof needs; it is false at y=0y=0y=0. Remarks 3.3 is posed for x>0x>0x>0 (V(0,y)=0V(0,y)=0V(0,y)=0). For the same reason the stopping regions and the boundaries b1,b2b_1,b_2b1​,b2​ live on (0,∞)×[0,1](0,\infty)\times[0,1](0,∞)×[0,1]: at the degenerate price x=0x=0x=0 one has V(0,y)=0=G1(0)V(0,y)=0=G_1(0)V(0,y)=0=G1​(0), and the page's literal x∈[0,∞)x\in[0,\infty)x∈[0,∞) in (4.2) and (4.11) would give b1≡0b_1\equiv0b1​≡0. Lemma 3.1 (iii)'s "a given constant CCC" is read as an existential constant. The standing assumption k≠0k\neq0k=0 of §5 is a hypothesis of Lemmas 5.2, 5.4, Corollary 5.5 and Lemma 7.2. Only clause (5.20) of Corollary 5.5 is formalized. Proposition 4.1 uses the explicit forms of A1,A2A_1,A_2A1​,A2​ printed on p. 9.
  • No trivialization. The filtration is that of the price, never one containing DDD (with DDD observed the game is the complete-information one, where the result fails); YYY is the posterior, not the prior; VVV in the entry times is the game's own value, never a free function; stopping times include infinite ones; and the payoff is not a Bochner integral, which would silently be 000 for non-integrable payoffs.
  • Not formalized. Proposition 6.4 (C1C^1C1 regularity), Proposition 7.6 (the case k<0k<0k<0), Proposition 5.6 and Lemmas 4.3, 4.4, 4.7 are not used by the goal's proof.
  • Infrastructure needed. Optional sampling for continuous-time super/submartingales with unbounded stopping times; hitting times of closed sets by continuous processes as stopping times of an augmented filtration; filtering for Brownian motion with a two-point drift; Itô's formula and Girsanov's theorem for the lemmas of §4–§7; existence of the value for Markovian Dynkin games. Each is reusable well beyond this mission, and contributions of any of them are welcome.

Selected references

  • T. De Angelis, F. Gensbittel, S. Villeneuve, A Dynkin Game on Assets with Incomplete Information on the Return, arXiv:1705.07352v4, 2019; Mathematics of Operations Research, 2021. https://arxiv.org/abs/1705.07352v4
  • Y. Kifer, Game options, Finance and Stochastics 4(4), 443–463, 2000. https://doi.org/10.1007/PL00013527
  • E. Ekström, S. Villeneuve, On the value of optimal stopping games, The Annals of Applied Probability 16, 1576–1596, 2006. https://doi.org/10.1214/105051606000000204
  • E. Ekström, G. Peskir, Optimal stopping games for Markov processes, SIAM Journal on Control and Optimization 47, 684–702, 2008. https://doi.org/10.1137/060673916
  • S. C. P. Yam, S. P. Yung, W. Zhou, Game call options revisited, Mathematical Finance, 2012.
  • R. S. Liptser, A. N. Shiryaev, Statistics of Random Processes I: General Theory, 2nd ed., Springer, 2001.
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Operations ResearchProbabilityStochastic Systems·Captain: mikedeng1

On Uniform Exponential Ergodicity of Markovian Multiclass Many-Server Queues in the Halfin–Whitt Regime: Positive Spare Capacity Makes the Limiting Diffusion Uniformly Exponentially ErgodicResearch Paper

Motivation

Call centres and hospital wards are run in the Halfin–Whitt regime: the number of servers nnn exceeds the offered load by a margin of order n\sqrt nn​, so that delays are short and servers are nearly always busy. With several customer classes, the operator must also choose a scheduling policy: which waiting class is served next. In the diffusion limit, every such policy becomes a control of an mmm-dimensional piecewise-linear diffusion (Atar, Mandelbaum and Reiman 2004; Harrison and Zeevi 2004). Ergodic control of this diffusion, and the justification that its optimal policies are asymptotically optimal for the queues, both need the diffusion to be stable under every admissible policy, with bounds that do not depend on the policy.

A. Arapostathis, H. Hmedi and G. Pang (arXiv:1812.03528v3) prove that positive spare capacity alone gives this: the limiting diffusion is exponentially ergodic, at a rate and with constants that are uniform over all stationary Markov controls.

Timeline.

  • 2004: Atar–Mandelbaum–Reiman and Harrison–Zeevi derive the controlled diffusion limit of the multiclass M/M/nM/M/nM/M/n queue in the Halfin–Whitt regime.
  • 2013: Dieker and Gao prove positive recurrence and, with abandonment, exponential ergodicity of piecewise Ornstein–Uhlenbeck processes, for one specific static priority control.
  • 2019: Arapostathis, Pang and Sandrić show positive recurrence under every constant control when the spare capacity ϱ\varrhoϱ is positive, and transience under Markov controls when ϱ<0\varrho<0ϱ<0 (without abandonment).
  • 2019: this paper extends exponential ergodicity to all stationary Markov controls, with uniform constants.

Setting

Fix m≥1m\ge1m≥1 classes, service rates μi>0\mu_i>0μi​>0, abandonment rates γi≥0\gamma_i\ge0γi​≥0, and write M=diag(μi)M=\mathrm{diag}(\mu_i)M=diag(μi​), Γ=diag(γi)\Gamma=\mathrm{diag}(\gamma_i)Γ=diag(γi​), e=(1,…,1)e=(1,\dots,1)e=(1,…,1), βi=γi/μi\beta_i=\gamma_i/\mu_iβi​=γi​/μi​. Control values lie in the simplex Δ={u∈Rm:u≥0, ⟨e,u⟩=1}\Delta=\{u\in\mathbb R^m:u\ge0,\ \langle e,u\rangle=1\}Δ={u∈Rm:u≥0, ⟨e,u⟩=1}; uiu_iui​ is the fraction of the queue made up of class iii. The spare capacity is ϱ∈R\varrho\in\mathbb Rϱ∈R. The controlled drift is

b(x,u)=−ϱmMe−M(x−⟨e,x⟩+u)−⟨e,x⟩+Γu,b(x,u)=-\frac{\varrho}{m}Me-M\big(x-\langle e,x\rangle^+u\big)-\langle e,x\rangle^+\Gamma u ,b(x,u)=−mϱ​Me−M(x−⟨e,x⟩+u)−⟨e,x⟩+Γu,

and the diffusion is dXt=b(Xt,Ut) dt+σ dWt\mathrm dX_t=b(X_t,U_t)\,\mathrm dt+\sigma\,\mathrm dW_tdXt​=b(Xt​,Ut​)dt+σdWt​ with a constant positive diagonal σ=diag(ri)\sigma=\mathrm{diag}(r_i)σ=diag(ri​) and a standard Brownian motion WWW. The generator under the control value uuu is Luf=12trace(σσT∇2f)+⟨b(⋅,u),∇f⟩\mathcal L_uf=\frac12\mathrm{trace}(\sigma\sigma^{\mathsf T}\nabla^2f)+\langle b(\cdot,u),\nabla f\rangleLu​f=21​trace(σσT∇2f)+⟨b(⋅,u),∇f⟩.

A stationary Markov control is a Borel map v:Rm→Δv:\mathbb R^m\to\Deltav:Rm→Δ, used as Ut=v(Xt)U_t=v(X_t)Ut​=v(Xt​); the class is Usm\mathfrak U_{\mathrm{sm}}Usm​. Its transition probability is Ptv(x,⋅)P^v_t(x,\cdot)Ptv​(x,⋅), the law of XtX_tXt​ started at xxx. An invariant probability measure πv\pi_vπv​ satisfies ∫Ptv(x,⋅) πv(dx)=πv\int P^v_t(x,\cdot)\,\pi_v(\mathrm dx)=\pi_v∫Ptv​(x,⋅)πv​(dx)=πv​.

The Lyapunov function is built from the convex C2C^2C2 cut-off ψ\psiψ (ψ=−12\psi=-\frac12ψ=−21​ on (−∞,−1](-\infty,-1](−∞,−1], ψ(t)=t\psi(t)=tψ(t)=t on [0,∞)[0,\infty)[0,∞)): for ε,θ>0\varepsilon,\theta>0ε,θ>0,

Ψε,θ∗(x)=εθ∑iψ(−xi)μi+∑iψ(εxi)μi,V(x)=exp⁡(Ψε,θ∗(x)).\Psi^*_{\varepsilon,\theta}(x)=\varepsilon\theta\sum_i\frac{\psi(-x_i)}{\mu_i}+\sum_i\frac{\psi(\varepsilon x_i)}{\mu_i},\qquad V(x)=\exp\big(\Psi^*_{\varepsilon,\theta}(x)\big).Ψε,θ∗​(x)=εθi∑​μi​ψ(−xi​)​+i∑​μi​ψ(εxi​)​,V(x)=exp(Ψε,θ∗​(x)).

For a weight fff, the fff-norm of a signed measure is sup⁡∣g∣≤f∣∫g dν∣\sup_{|g|\le f}|\int g\,\mathrm d\nu|sup∣g∣≤f​∣∫gdν∣.

Formalization targets

Goal: Theorem 2.1 (p. 10)

Assume ϱ>0\varrho>0ϱ>0, θ(βmax⁡−1)+≤1\theta(\beta_{\max}-1)^+\le1θ(βmax​−1)+≤1 and 0<θ≤ϱ/(3m(2ϱ+m))0<\theta\le\varrho/(3m(2\varrho+m))0<θ≤ϱ/(3m(2ϱ+m)). Then there is ε0>0\varepsilon_0>0ε0​>0 such that for every 0<ε≤ε00<\varepsilon\le\varepsilon_00<ε≤ε0​ there is κ0>0\kappa_0>0κ0​>0 with

LuV(x)≤κ0−ε(ϱ2m+θ2∥x−∥1)V(x)∀(x,u)∈Rm×Δ,\mathcal L_uV(x)\le\kappa_0-\varepsilon\Big(\frac{\varrho}{2m}+\frac\theta2\|x^-\|_1\Big)V(x)\qquad\forall (x,u)\in\mathbb R^m\times\Delta,Lu​V(x)≤κ0​−ε(2mϱ​+2θ​∥x−∥1​)V(x)∀(x,u)∈Rm×Δ,

and there are γ,C>0\gamma,C>0γ,C>0 such that, for every v∈Usmv\in\mathfrak U_{\mathrm{sm}}v∈Usm​, an invariant probability measure πv\pi_vπv​ exists with

∫V dπv≤2mεϱκ0,∥Ptv(x,⋅)−πv∥1+V≤C V(x) e−γt∀(t,x).\int V\,\mathrm d\pi_v\le\frac{2m}{\varepsilon\varrho}\kappa_0,\qquad \big\|P^v_t(x,\cdot)-\pi_v\big\|_{1+V}\le C\,V(x)\,e^{-\gamma t}\quad\forall (t,x).∫Vdπv​≤εϱ2m​κ0​,​Ptv​(x,⋅)−πv​​1+V​≤CV(x)e−γt∀(t,x).

The rate γ\gammaγ and the constant CCC do not depend on the control: that uniformity is the content of the theorem.

Milestones, in the order the proof uses them

  1. p. 5: under every v∈Usmv\in\mathfrak U_{\mathrm{sm}}v∈Usm​ the SDE has a unique strong solution and a strong Feller transition function.
  2. p. 7: the properties of ψ\psiψ, including ψε′′≤32ε2\psi_\varepsilon''\le\frac32\varepsilon^2ψε′′​≤23​ε2.
  3. (2.13a)–(2.13b), p. 8: the identities for ⟨∇Ψε,b⟩\langle\nabla\Psi_\varepsilon,b\rangle⟨∇Ψε​,b⟩ and ⟨∇Ψ(−⋅),b⟩\langle\nabla\Psi(-\cdot),b\rangle⟨∇Ψ(−⋅),b⟩.
  4. Lemma 2.1, p. 8: the drift inequalities (2.17) for the truncated drift bcb_cbc​, c∈[1,∞]c\in[1,\infty]c∈[1,∞].
  5. (2.31), p. 10: 12trace(a∇2V)≤ε(32(ε+θ)+εCˉ)V\frac12\mathrm{trace}(a\nabla^2V)\le\varepsilon(\frac32(\varepsilon+\theta)+\varepsilon\bar C)V21​trace(a∇2V)≤ε(23​(ε+θ)+εCˉ)V.
  6. (2.28), p. 10: the Foster–Lyapunov equation above (part (a) of the goal).
  7. (2.10), p. 7: Ψε,θ∗\Psi^*_{\varepsilon,\theta}Ψε,θ∗​ is comparable to ∥x∥1\|x\|_1∥x∥1​.
  8. (2.34), p. 11: ∫Ptv(x,dy)V(y)≤κ0/κ1+e−κ1tV(x)\int P^v_t(x,\mathrm dy)V(y)\le\kappa_0/\kappa_1+e^{-\kappa_1t}V(x)∫Ptv​(x,dy)V(y)≤κ0​/κ1​+e−κ1​tV(x) whenever LuV≤κ0−κ1V\mathcal L_uV\le\kappa_0-\kappa_1VLu​V≤κ0​−κ1​V.
  9. p. 11: the uniform minorization P1v(x,B)≥δ0P^v_1(x,\mathcal B)\ge\delta_0P1v​(x,B)≥δ0​ on a ball, from the parabolic Harnack inequality.

Significance

The result. Uniform exponential ergodicity makes the ergodic control problem for the multiclass Halfin–Whitt diffusion well posed over all stationary Markov policies: invariant measures form a tight family with uniformly integrable exponential moments, and long-run averages converge at a policy-independent geometric rate. In the paper it is the base for the prelimit results of Section 3, where the drift inequalities of Lemma 2.1 are compared with those of the nnn-server queues. With Γ=0\Gamma=0Γ=0 the condition ϱ>0\varrho>0ϱ>0 is sharp, since ϱ<0\varrho<0ϱ<0 gives transience under every Markov control (Arapostathis, Pang and Sandrić 2019).

Formalizing it. The theorem is proved in the paper; none of it is formalized. The mission produces a machine-checked version with two printed slips corrected (see Formalization scope). Its analytic half, Lemma 2.1, (2.13), (2.10), (2.31) and the Foster–Lyapunov equation, is finite-dimensional calculus and is reachable now. The probabilistic half needs Itô's formula for SDEs with additive noise, existence and uniqueness for SDEs with Borel drifts, and a Harnack-type minorization, none of which Mathlib has.

Difficulty

The control enters the drift only through ⟨e,x⟩+u\langle e,x\rangle^+u⟨e,x⟩+u, but a Markov control may switch arbitrarily, so no single linear or quadratic Lyapunov function works for all policies; Dieker and Gao's common quadratic Lyapunov functions cover one static priority only. The function VVV mixes an ε\varepsilonε-scaled workload term with a θ\thetaθ-weighted idleness term, and the drift inequality must hold on both half-spaces {⟨e,x⟩≤0}\{\langle e,x\rangle\le0\}{⟨e,x⟩≤0} and {⟨e,x⟩≥0}\{\langle e,x\rangle\ge0\}{⟨e,x⟩≥0} with explicit constants, which forces case splits over the classes with βi≤1\beta_i\le1βi​≤1 and βi>1\beta_i>1βi​>1.

For part (b), a Foster–Lyapunov inequality alone gives ergodicity for each control but not a control-independent rate: the constants of the standard Meyn–Tweedie argument depend on a minorization on a small set, and that minorization must be shown uniformly over all Borel controls, for which there is no regularity in vvv to exploit.

Formalization scope

  • Representation. States are EuclideanSpace ℝ (Fin m); classes are Fin m; control values are vectors in stdSimplex ℝ (Fin m). The model data is the published ManyServerQED.Scheduling.DiffusionData with its drift ℓ+(μ−γ)⟨e,x⟩+u−μx\ell+(\mu-\gamma)\langle e,x\rangle^+u-\mu xℓ+(μ−γ)⟨e,x⟩+u−μx; the SDE equation, invariant measures, generator and weighted total-variation norm use published GPhNGIDiffusion.EMError definitions. The local IsStrongSolution and IsMarkovTransition specify measurable, adapted solutions and their transition laws. The cut-off ψ\psiψ is the published cutoff.
  • Committed conventions.
    1. The drift is centred, ℓ=−ϱmMe\ell=-\frac{\varrho}{m}Meℓ=−mϱ​Me (Remark 2.3, "without loss of generality").
    2. σ=diag(ri)\sigma=\mathrm{diag}(r_i)σ=diag(ri​) is constant (the proof uses σ=diag(2λ~i)1/2\sigma=\mathrm{diag}(2\tilde\lambda_i)^{1/2}σ=diag(2λ~i​)1/2), and ∑iri2/(2μi)=1\sum_ir_i^2/(2\mu_i)=1∑i​ri2​/(2μi​)=1, i.e. ∑iλ~i/μi=1\sum_i\tilde\lambda_i/\mu_i=1∑i​λ~i​/μi​=1, the identity the proof invokes in (2.31). Without it the Foster–Lyapunov equation fails numerically.
    3. θ(βmax⁡−1)+≤1\theta(\beta_{\max}-1)^+\le1θ(βmax​−1)+≤1 is written as θ(βi−1)+≤1\theta(\beta_i-1)^+\le1θ(βi​−1)+≤1 for all iii.
    4. A transition function is the law of every measurable strong solution on every probability space; "positive recurrent" is read as the existence of an invariant probability measure. The published transition predicate quantifies over arbitrary pathwise solutions, including nonmeasurable ones for which Measure.map returns a junk zero measure, so a local predicate is used here.
    5. The VVV-norm uses the weight 1+V1+V1+V, since VVV can be below 111 while the paper's fff-norm needs f≥1f\ge1f≥1; the norm is +∞+\infty+∞ unless both measures integrate 1+V1+V1+V.
    6. The truncation level c∈[1,∞]c\in[1,\infty]c∈[1,∞] of Lemma 2.1 is an extended real.
  • Printed slips, corrected.
    1. (2.28) is quoted as printed in its milestone but posed with θ2\frac\theta22θ​ in place of θ\thetaθ on ∥x−∥1\|x^-\|_1∥x−∥1​: as printed it fails along x=−Rex=-Rex=−Re, R→∞R\to\inftyR→∞, where the left side exceeds the right by ε(θϱ+ϱ2m+εθ2Cˉ)V→∞\varepsilon(\theta\varrho+\frac{\varrho}{2m}+\varepsilon\theta^2\bar C)V\to\inftyε(θϱ+2mϱ​+εθ2Cˉ)V→∞. The rest of the theorem is unaffected.
    2. The lower bound of (2.10) is quoted as printed but posed with the constant m(1∨εθ)/(2μmin⁡)m(1\vee\varepsilon\theta)/(2\mu_{\min})m(1∨εθ)/(2μmin​) in place of m2\frac m22m​, which fails when μmin⁡<1\mu_{\min}<1μmin​<1.
  • Ruling out trivial readings. The transition-function hypothesis is not vacuous: milestone 1 asserts existence of solutions and of a transition function under every Borel control. The constants γ,C\gamma,Cγ,C are quantified before the control, the Foster–Lyapunov inequality ranges over u∈Δu\in\Deltau∈Δ only, the norm is never a junk value, and the moment bound on πv\pi_vπv​ uses the same κ0\kappa_0κ0​ as the Foster–Lyapunov equation.
  • Constructed ball. The minorization uses an existential ball whose complement satisfies the inequality chosen after (2.34), with its lower bound uniform over controls.
  • Needed infrastructure and welcome contributions. Calculus for ψ\psiψ and VVV (reusable for every Lyapunov argument built on this cut-off); Itô's formula with localization for additive-noise SDEs; strong existence and pathwise uniqueness for Borel drifts of linear growth; a Harnack or Girsanov lower bound for transition probabilities on balls; the Meyn–Tweedie computable geometric bound. Each is reusable beyond this mission, and proofs of any milestone are welcome independently.

Selected references

  • A. Arapostathis, H. Hmedi, G. Pang, On uniform exponential ergodicity of Markovian multiclass many-server queues in the Halfin–Whitt regime, arXiv:1812.03528v3, 2019 (Mathematics of Operations Research, 2021). https://arxiv.org/abs/1812.03528
  • A. Arapostathis, V. S. Borkar, M. K. Ghosh, Ergodic Control of Diffusion Processes, Cambridge University Press, 2011. https://doi.org/10.1017/CBO9781139003605
  • A. Arapostathis, G. Pang, N. Sandrić, Ergodicity of a Lévy-driven SDE arising from multiclass many-server queues, Ann. Appl. Probab. 29(2), 2019. https://doi.org/10.1214/18-AAP1430
  • R. Atar, A. Mandelbaum, M. I. Reiman, Scheduling a multi class queue with many exponential servers: asymptotic optimality in heavy traffic, Ann. Appl. Probab. 14(3), 2004. https://doi.org/10.1214/105051604000000233
  • A. B. Dieker, X. Gao, Positive recurrence of piecewise Ornstein–Uhlenbeck processes and common quadratic Lyapunov functions, Ann. Appl. Probab. 23(4), 2013. https://doi.org/10.1214/12-aap870
  • M. Gruber, Harnack inequalities for solutions of general second order parabolic equations and estimates of their Hölder constants, Math. Z. 185(1), 1984. https://doi.org/10.1007/BF01214972
  • I. Gyöngy, N. Krylov, Existence of strong solutions for Itô's stochastic equations via approximations, Probab. Theory Related Fields 105(2), 1996. https://doi.org/10.1007/BF01203833
  • J. M. Harrison, A. Zeevi, Dynamic scheduling of a multiclass queue in the Halfin–Whitt heavy traffic regime, Oper. Res. 52(2), 2004. https://doi.org/10.1287/opre.1030.0084
  • S. P. Meyn, R. L. Tweedie, Computable bounds for geometric convergence rates of Markov chains, Ann. Appl. Probab. 4(4), 1994. https://doi.org/10.1214/aoap/1177004900
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ProbabilityQuantum InformationTheoretical Computer Science·Captain: mikedeng1

Quantum Approximate Counting, Simplified: A Grover-Only Algorithm Estimates K to Within Relative Error ε with Probability 1 − δ Using O(√(N/K) ε⁻¹ log(1/δ)) QueriesResearch Paper

Motivation

Approximate counting asks for the number KKK of marked items in a list of NNN items, to within a multiplicative factor 1±ε1\pm\varepsilon1±ε, when the marked set can only be accessed through a membership oracle. Brassard, Høyer, Mosca and Tapp (arXiv:quant-ph/0005055) gave a quantum algorithm that uses O(N/K ε−1)O(\sqrt{N/K}\,\varepsilon^{-1})O(N/K​ε−1) queries, which is optimal. Their algorithm combines Grover iterations with phase estimation, and so it needs the quantum Fourier transform (QFT). Counting is a basic subroutine in quantum algorithms for estimation, numerical integration and Monte Carlo speed-ups, so the circuit it requires matters.

Aaronson and Rall (arXiv:1908.10846, SOSA 2020) give an algorithm with the same query complexity that uses only Grover iterations and classical post-processing of measurement outcomes. Its analysis is short and elementary, and every constant in it is explicit. This mission formalizes their Theorem 1, the rotation lemma it rests on, and the numbered estimates of its proof (arXiv:1908.10846v6, pp. 4–10).

Timeline (as recounted on pp. 1–3 of the paper):

  • 1996: Grover introduced the iteration whose powers rotate the uniform superposition towards the marked items.
  • 1998: Brassard, Høyer, Mosca and Tapp gave counting with O(N/K ε−1)O(\sqrt{N/K}\,\varepsilon^{-1})O(N/K​ε−1) queries by phase estimation of the Grover operator. The journal version appeared in 2002.
  • 1997–1999: Grover outlined a broadly similar Grover-only approach. Abrams and Williams discussed it further, for estimating integrals to additive error with O(ε−1)O(\varepsilon^{-1})O(ε−1) queries. Neither proved the approach correct.
  • 2019: Suzuki et al. gave an O(ε−1N/K)O(\varepsilon^{-1}\sqrt{N/K})O(ε−1N/K​)-query QFT-free algorithm that uses maximum-likelihood post-processing, supported by numerical experiments rather than a proof. Wie sketched a QFT-free algorithm based on Hadamard tests, also without proof.
  • 2019–2021: Aaronson and Rall proved a Grover-only algorithm correct with the optimal O(N/K ε−1log⁡δ−1)O(\sqrt{N/K}\,\varepsilon^{-1}\log\delta^{-1})O(N/K​ε−1logδ−1) bound. The constants used here are those of v6.

Setting

Let S⊆[N]={0,…,N−1}S\subseteq[N]=\{0,\dots,N-1\}S⊆[N]={0,…,N−1} be a nonempty marked set with K=∣S∣K=|S|K=∣S∣. The algorithm first pads the list to N′=(106+1)NN'=(10^6+1)NN′=(106+1)N items, the added items being unmarked, and then works on CN′\mathbb C^{N'}CN′. The membership oracle is the diagonal unitary U∣x⟩=(−1)[x∈S]∣x⟩U|x\rangle=(-1)^{[x\in S]}|x\rangleU∣x⟩=(−1)[x∈S]∣x⟩. The uniform superposition is ∣ψ⟩=N′−1/2∑x∣x⟩|\psi\rangle=N'^{-1/2}\sum_x|x\rangle∣ψ⟩=N′−1/2∑x​∣x⟩, and the Grover operator is

G=(I−2∣ψ⟩⟨ψ∣) U.G=(I-2|\psi\rangle\langle\psi|)\,U .G=(I−2∣ψ⟩⟨ψ∣)U.

Preparing G(r−1)/2∣ψ⟩G^{(r-1)/2}|\psi\rangleG(r−1)/2∣ψ⟩ for an odd rrr costs (r−1)/2(r-1)/2(r−1)/2 queries. Measuring it in the computational basis yields a marked item with probability ppp given by the Born rule. With θ=arcsin⁡K/N′≤0.001\theta=\arcsin\sqrt{K/N'}\le0.001θ=arcsinK/N′​≤0.001 this probability is sin⁡2(rθ)\sin^2(r\theta)sin2(rθ), so mmm repetitions give a Bin(m,sin⁡2(rθ))\mathrm{Bin}(m,\sin^2(r\theta))Bin(m,sin2(rθ)) count of marked outcomes.

The algorithm has two loops. Step 1 tries rkr_krk​, the largest odd integer at most 1.05k1.05^k1.05k, for k=0,1,…k=0,1,\dotsk=0,1,…, with ⌈5000ln⁡(5/δ)⌉\lceil5000\ln(5/\delta)\rceil⌈5000ln(5/δ)⌉ measurements per round. It stops at the first k=:kendk=:k_{\mathrm{end}}k=:kend​ at which at least 95% of the outcomes are marked. Step 2 keeps a bracket [θmin⁡,θmax⁡][\theta_{\min},\theta_{\max}][θmin​,θmax​], initially θmin⁡=0.9⋅1.05−kend\theta_{\min}=0.9\cdot1.05^{-k_{\mathrm{end}}}θmin​=0.9⋅1.05−kend​ and θmax⁡=1.65 θmin⁡\theta_{\max}=1.65\,\theta_{\min}θmax​=1.65θmin​. In round ttt it computes rtr_trt​ from the bracket by the rotation lemma (Lemma 2):

k=round(θmin⁡2(θmax⁡−θmin⁡)),r=closest odd integer to πkθmin⁡.k=\mathrm{round}\Big(\frac{\theta_{\min}}{2(\theta_{\max}-\theta_{\min})}\Big),\qquad r=\text{closest odd integer to }\frac{\pi k}{\theta_{\min}} .k=round(2(θmax​−θmin​)θmin​​),r=closest odd integer to θmin​πk​.

It then measures ⌈250ln⁡δt−1⌉\lceil250\ln\delta_t^{-1}\rceil⌈250lnδt−1​⌉ times, with δt=(δε/65) 0.9−t\delta_t=(\delta\varepsilon/65)\,0.9^{-t}δt​=(δε/65)0.9−t, and shrinks γ=θmax⁡/θmin⁡−1\gamma=\theta_{\max}/\theta_{\min}-1γ=θmax​/θmin​−1 by the factor 0.90.90.9: it raises θmin⁡\theta_{\min}θmin​ if at least 12% of the outcomes are marked and lowers θmax⁡\theta_{\max}θmax​ otherwise. It stops once θmax⁡≤(1+ε/5)θmin⁡\theta_{\max}\le(1+\varepsilon/5)\theta_{\min}θmax​≤(1+ε/5)θmin​ and returns K^=N′sin⁡2θmax⁡\hat K=N'\sin^2\theta_{\max}K^=N′sin2θmax​.

Formalization targets

Goal: Theorem 1

For nonempty S⊆[N]S\subseteq[N]S⊆[N], K=∣S∣K=|S|K=∣S∣:

  1. for 0<ε,δ<10<\varepsilon,\delta<10<ε,δ<1 there is a fuel bound FFF such that
Pr⁡[the algorithm outputs K^ with K(1−ε)<K^<K(1+ε)]≥1−δ;\Pr\big[\text{the algorithm outputs }\hat K\text{ with }K(1-\varepsilon)<\hat K<K(1+\varepsilon)\big]\ge1-\delta ;Pr[the algorithm outputs K^ with K(1−ε)<K^<K(1+ε)]≥1−δ;
  1. there is an absolute constant CCC such that for 0<ε,δ≤1/20<\varepsilon,\delta\le1/20<ε,δ≤1/2, every run that outputs an accurate K^\hat KK^ has made fewer than CN/K ε−1ln⁡δ−1C\sqrt{N/K}\,\varepsilon^{-1}\ln\delta^{-1}CN/K​ε−1lnδ−1 queries.

Milestones

In the order of the proof:

  • eq. (1), the Grover state and its marked probability sin⁡2(rθ)\sin^2(r\theta)sin2(rθ);
  • eqs. (2)–(6), the ideal bracket after step 1;
  • eqs. (7)–(12) and (15)–(28), no late and no early termination of step 1, with the Kullback–Leibler form (13)–(14) of the Chernoff bound;
  • eqs. (52), (57), (58)–(66) and (68)–(74), the estimates behind the rotation lemma;
  • Lemma 2 itself;
  • eqs. (30)–(32), the union bound over step 2;
  • footnote 2, the conversion from angle to count;
  • eqs. (37)–(44), the arithmetico-geometric sum in the query bound.

Significance

Theorem 1 shows that the optimal query complexity of approximate counting is achieved without the quantum Fourier transform. The circuits involved are powers of the Grover operator followed by computational-basis measurements, and the classical control is a pair of loops with explicit thresholds. The same argument gives QFT-free amplitude estimation (Theorem 3 of the paper), and its rotation lemma is a reusable tool for any algorithm that brackets a rotation angle by biased coin tosses.

The result is proved on paper but not formalized. The platform has Grover's iteration for a single marked item; it has no Grover state for a marked set, no counting algorithm and no query-complexity statement of this kind. A complete development would provide a machine-checked quantum query algorithm whose output law is derived from the Born rule and the actual Grover operator. It would also provide a Chernoff bound in Kullback–Leibler form for the binomial distribution, which Mathlib does not have.

Difficulty

The deterministic estimates are elementary but numerous, and each constant (0.96, 7.5%, 16.5%, 1.102, 0.27, 0.42) must be checked against interval arithmetic for sin⁡\sinsin and π\piπ. Two printed steps are numerically loose, (8) and (26), and must be replaced by correct intermediate values.

The probabilistic part has two difficulties. First, the success event of step 1 is not a single tail bound. Termination too early is controlled by a union bound over rounds k≤k0k\le k_0k≤k0​, and the additive Hoeffding bound is too weak there: it needs the KL form (13). Second, step 2's output law is defined by a recursion whose bracket is random, and Lemma 2 applies to a round only while the bracket still contains θ\thetaθ. The union bound over rounds has to be carried through this recursion. Third, the paper bounds the queries only on its "ideal" event. Part 2 of the goal requires the bound on every run that ends with an accurate estimate, including runs in which step 1 stopped late.

Formalization scope

  • States are vectors Fin N' → ℂ, operators are Matrix (Fin N') (Fin N') ℂ, and ∣ψ⟩⟨ψ∣|\psi\rangle\langle\psi|∣ψ⟩⟨ψ∣ is vecMulVec ψ (star ψ). The padding embeds Fin N as the first NNN indices of Fin N'.
  • The algorithm approxCount N S ε δ F : PMF (Option (ℝ × ℕ)) is defined, not quantified. Its outputs are some (K̂, queries), or none when either loop runs out of its fuel F. Fuel exhaustion counts as failure. Measurement counts are Mathlib's binomial law with the Born probability ∑x∈S∣⟨x∣Gj∣ψ⟩∣2\sum_{x\in S}|\langle x|G^j|\psi\rangle|^2∑x∈S​∣⟨x∣Gj∣ψ⟩∣2 computed from UUU, ψ\psiψ and GGG.
  • The algorithm sees SSS only through these probabilities. rkr_krk​ depends on kkk only, rtr_trt​ on the bracket only, and the repetition counts and thresholds on ε,δ,t\varepsilon,\delta,tε,δ,t only. A formalization in which the algorithm reads KKK or θ\thetaθ directly, or in which "there exists an algorithm" is quantified, is trivial (output KKK with zero queries) and is ruled out.
  • "At least mmm times" means exactly ⌈m⌉\lceil m\rceil⌈m⌉ times. Mathlib's round breaks ties upward, a choice the paper permits. The step-2 threshold is "at least 12%", as in the algorithm box; Lemma 2 is stated for both "more than" and "at least".
  • Eq. (1) is stated in corrected form: the printed identity misses the global sign (−1)(r−1)/2(-1)^{(r-1)/2}(−1)(r−1)/2 coming from G=−(2∣ψ⟩⟨ψ∣−I)UG=-(2|\psi\rangle\langle\psi|-I)UG=−(2∣ψ⟩⟨ψ∣−I)U.
  • The O(⋅)O(\cdot)O(⋅) of Theorem 1 is one absolute constant chosen before N,S,ε,δ,FN,S,\varepsilon,\delta,FN,S,ε,δ,F, in the regime ε,δ≤1/2\varepsilon,\delta\le1/2ε,δ≤1/2. The rotation lemma's O(θ−1γ−1)O(\theta^{-1}\gamma^{-1})O(θ−1γ−1) is pinned to r≤5/(γθ)r\le5/(\gamma\theta)r≤5/(γθ).
  • Not formalized: the O(log⁡N)O(\log N)O(logN)-qubit space bound (there is no circuit model), Theorem 3 (amplitude estimation), and the unquantified remark on K=0K=0K=0.

Contributions of reusable infrastructure are welcome, in particular the KL-form Chernoff bound for ProbabilityTheory.binomial and lemmas on powers of a reflection product acting on a two-dimensional invariant subspace.

Selected references

  • S. Aaronson, P. Rall, Quantum Approximate Counting, Simplified, Symposium on Simplicity in Algorithms (SOSA) 2020; arXiv:1908.10846v6, 2021. https://arxiv.org/abs/1908.10846
  • G. Brassard, P. Høyer, M. Mosca, A. Tapp, Quantum Amplitude Amplification and Estimation, Contemporary Mathematics 305, 2002. https://arxiv.org/abs/quant-ph/0005055
  • G. Brassard, P. Høyer, A. Tapp, Quantum Counting, ICALP 1998. https://arxiv.org/abs/quant-ph/9805082
  • L. K. Grover, A fast quantum mechanical algorithm for database search, STOC 1996. https://arxiv.org/abs/quant-ph/9605043
  • Y. Suzuki et al., Amplitude estimation without phase estimation, Quantum Information Processing 19, 2020. https://arxiv.org/abs/1904.10246
  • D. S. Abrams, C. P. Williams, Fast quantum algorithms for numerical integrals and stochastic processes, 1999. https://arxiv.org/abs/quant-ph/9908083
  • C. R. Wie, Simpler quantum counting, arXiv preprint, 2019. https://arxiv.org/abs/1907.08119
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Operations ResearchProbabilityStochastic Systems·Captain: mikedeng1

Shipment Policies for Products with Fixed Shelf Lives: Impact on Profits and Waste: Shipping Oldest First Minimizes the Long-Run Average Warehouse Waste and the Total WasteResearch Paper

Motivation

Manufacturers of products with fixed shelf lives must decide both how much to send from a warehouse to a store and which age cohorts to send. A shipment can reduce expiry at the warehouse while changing the age mix seen by shoppers at the store. In the two-echelon system studied by Akkaş and Honhon, the store does not control which items each shopper takes: some shoppers select older items first and the remainder select newer items first. The resulting waste at the warehouse and store can move in different directions when the manufacturer changes a shipment. The paper uses this setting to ask whether ship oldest first (SOF), a simple age-selection rule, minimizes waste over an infinite horizon. Akkaş and Honhon, SSRN manuscript.

The paper reports an inventory-age audit of a consumer packaged goods supplier and then studies the shipment decision analytically. Its Theorem 1 separates warehouse waste from the sum of warehouse and store waste. The former has a specified SOF policy that ships in full; the latter has an SOF age-selection rule but allows the shipped quantity to vary with the state. This mission formalizes those two claims, with a correction to one printed clause described below. Akkaş and Honhon, §3 and Theorem 1.

Setting

A unit remains saleable for NNN periods, where N≥1N\ge1N≥1. At the start of a period the warehouse holds xix_ixi​ units of age iii, and the store holds yiy_iyi​ units of that age, for i=1,…,N−1i=1,\ldots,N-1i=1,…,N−1. Both age-zero entries are zero before replenishment. A plant then delivers fresh units so the warehouse's total post-replenishment stock reaches the exogenous order-up-to level SWS^WSW. Thus its age-zero stock is x0post=SW−∑i=1N−1xix^{\mathrm{post}}_0=S^W-\sum_{i=1}^{N-1}x_ix0post​=SW−∑i=1N−1​xi​. The manufacturer sends qiq_iqi​ units of age iii from the warehouse to the store, subject to warehouse availability and the store's shelf capacity LLL. In particular, qi≤xipostq_i\le x^{\mathrm{post}}_iqi​≤xipost​ and ∑iqi+∑iyi≤L\sum_iq_i+\sum_i y_i\le L∑i​qi​+∑i​yi​≤L. Akkaş and Honhon, §4.1, pp. 10–13, and §4.2, p. 15.

The period's shopper population is λ\lambdaλ. A fraction γ∈[0,1]\gamma\in[0,1]γ∈[0,1] selects inventory first in, first out (FIFO), meaning older units first; the remaining shoppers select it last in, first out (LIFO), meaning newer units first. The discrete FIFO population is ⌈γλ⌉\lceil\gamma\lambda\rceil⌈γλ⌉. If zi=yi+qiz_i=y_i+q_izi​=yi​+qi​ is the store stock after delivery, the paper's age-specific demand is

Di(z,λ;γ)=(⌈γλ⌉−∑j>izj)++(λ−⌈γλ⌉−∑j<izj)+.D_i(z,\lambda;\gamma)=\left(\lceil\gamma\lambda\rceil-\sum_{j>i}z_j\right)^+ +\left(\lambda-\lceil\gamma\lambda\rceil-\sum_{j<i}z_j\right)^+.Di​(z,λ;γ)=(⌈γλ⌉−j>i∑​zj​)++(λ−⌈γλ⌉−j<i∑​zj​)+.

Here u+=max⁡(u,0)u^+=\max(u,0)u+=max(u,0). Only units of age N−1N-1N−1 expire at the end of the period. Warehouse waste is WW=xN−1post−qN−1W^W=x^{\mathrm{post}}_{N-1}-q_{N-1}WW=xN−1post​−qN−1​, store waste is WR=(zN−1−DN−1)+W^R=(z_{N-1}-D_{N-1})^+WR=(zN−1​−DN−1​)+, and total waste is W=WW+WRW=W^W+W^RW=WW+WR. The remaining units advance one age before the next period. An SOF shipment uses a younger unit only when every older available unit has been shipped. An SOF shipment in full fills the remaining store space or ships the entire available warehouse stock. Akkaş and Honhon, §4.1, pp. 11–12, and §4.2.1, p. 15.

Formalization targets

Warehouse waste

Let W‾W,+\overline W^{W,+}WW,+ and W‾W,−\overline W^{W,-}WW,− denote the upper and lower limits of expected Cesàro averages of warehouse waste. The first sentence of Theorem 1 is the mission's sole milestone:

W‾W,+(SOF-full;s0)≤W‾W,−(σ;s0)for every feasible initial state s0 and every admissible policy σ.\overline W^{W,+}(\mathrm{SOF\text{-}full};s_0) \le \overline W^{W,-}(\sigma;s_0) \quad\text{for every feasible initial state }s_0\text{ and every admissible policy }\sigma.WW,+(SOF-full;s0​)≤WW,−(σ;s0​)for every feasible initial state s0​ and every admissible policy σ.

Total waste and mission goal

The full goal also asserts that one stationary, feasible SOF policy fff minimizes total waste from every feasible initial state:

∃f  stationary and SOF,W‾+(f;s0)≤W‾−(σ;s0)for all feasible s0 and admissible σ.\exists f\;\text{stationary and SOF},\qquad \overline W^+(f;s_0)\le\overline W^-(\sigma;s_0) \quad\text{for all feasible }s_0\text{ and admissible }\sigma.∃fstationary and SOF,W+(f;s0​)≤W−(σ;s0​)for all feasible s0​ and admissible σ.

The policy fff chooses its shipping quantity from the current state; the theorem does not prescribe shipping in full for this second objective. These are waste objectives, independent of the paper's separate revenue, labor, and expiration-cost parameters. Akkaş and Honhon, Theorem 1, p. 15.

Significance

The warehouse result identifies a fixed, implementable shipment rule for minimizing waste at that location across the paper's whole FIFO/LIFO range. The total-waste result says that optimal age selection can remain SOF even when the quantity decision must respond to the store inventory and shopper behavior. Together they distinguish the two decisions in a setting where moving an expiring unit out of the warehouse can merely move the expiry to the store. The paper later uses its waste comparison in the analysis of profit policies under additional cost assumptions. Akkaş and Honhon, Appendix A.2–A.3.

The theorem is a published paper result, but this mission starts with open Lean statements rather than a machine-checked proof. A complete development would provide a reusable formal model of age-structured two-echelon inventory, stochastic shopper depletion, feasible shipment policies, and long-run waste criteria. The general controlled-process and Cesàro-average definitions can also support other finite inventory models.

Difficulty

An age-selection decision changes the stock carried into future periods, and a quantity decision changes the next warehouse replenishment. A comparison of immediate waste therefore does not by itself compare long-run averages. In particular, simply reordering each shipment to send older units first while keeping its quantity fixed can increase later warehouse waste for some policies; it cannot serve as an unrestricted policy-level argument. The store's FIFO/LIFO mixture introduces another intertemporal effect because a shipped younger unit can be sold ahead of an older one. Akkaş and Honhon, Appendix A.1, Appendix p. 1.

Formalization scope

Lean uses finite age vectors indexed by Fin N, natural-number stocks and shipments, a real γ\gammaγ constrained to [0,1][0,1][0,1], and an arbitrary probability mass function for shopper population. The standing condition N≥1N\ge1N≥1 makes the final age cohort defined; SW=0S^W=0SW=0 and L=0L=0L=0 remain allowed. Demand samples are independent and identically distributed across periods, as in the stationary transition model of §4.2. Policies are time-dependent deterministic Markov rules: at period ttt they choose a shipment from the current inventory state. This is the finite-state class used by the paper's dynamic program. The comparison includes every feasible rule in that class, every feasible initial state, and a common stationary SOF witness for total waste; it does not restrict competitors to SOF or full shipments. Standard finite-MDP results explain why stationary deterministic optimal policies suffice among broader history-dependent randomized classes. Puterman, Markov Decision Processes, Theorem 9.1.8.

Costs and expectations live in [0,∞][0,\infty][0,∞], and long-run criteria use upper and lower limits of expected Cesàro averages. The paper prints a plain limit without specifying what happens when a policy's average fails to converge. The upper-versus-lower comparison states the stronger optimality claim without relying on that convergence. Lean time starts at zero. Natural-number subtraction implements the paper's positive-part operation, and the post-replenishment stock formula is used only for feasible states. The model follows the printed balance equations when discarding the final-age store stock, despite a tension with the narrative timing of expired-unit pickup.

Three transcription corrections are explicit. The demand formula's sums use zjz_jzj​, the running index, where the page prints ziz_izi​; the action sum runs through age N−1N-1N−1; and the waste objectives are minimized despite a printed “max” in §4.2.1. More consequentially, Theorem 1's last clause says shipping is in full under pure FIFO. This is false and is omitted: for γ=1\gamma=1γ=1, N=2N=2N=2, SW=1S^W=1SW=1, L=2L=2L=2, and a Bernoulli(1/2)(1/2)(1/2) shopper population, SOF in full has average total waste 1/21/21/2 while an SOF policy that holds stock back attains 1/41/41/4. The formal goal neither assumes this clause nor asserts its negation. Its feasible-policy and feasible-initial-state quantifiers rule out vacuous or artificially easy readings.

A complete proof may need finite-state inventory invariants, admissibility of the SOF-in-full rule, comparisons of age profiles over time, and results about average costs of controlled chains. Contributions establishing those reusable facts, or the stated warehouse and total-waste targets, are within scope. The separate profit theorems and numerical studies of the paper are outside this mission.

Selected references

  • Akkaş, A., and D. Honhon. Shipment Policies for Products with Fixed Shelf Lives: Impact on Profits and Waste. Authors' SSRN manuscript 3247290, 2021; published in Manufacturing & Service Operations Management. SSRN manuscript; journal DOI.
  • Puterman, M. L. Markov Decision Processes: Discrete Stochastic Dynamic Programming. Wiley, 1994. DOI.
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Algorithmic Game TheoryControl TheoryOperations Research+1·Captain: mikedeng1

Game of Variable Contributions to the Common Good Under Uncertainty: The Symmetric Game Has a Regular Control Markov Perfect EquilibriumResearch Paper

Motivation

Many shared assets deteriorate unless someone pays to maintain them: a public infrastructure stock, a jointly used ecosystem, a joint venture's capital, a common research base. When several parties benefit from the same stock and each pays for its own contributions, every party is tempted to wait for the others to pay. Kwon (arXiv:1904.00500, published in Operations Research, 2022) models this as a two-player stochastic differential game in continuous time, in which each player may raise the stock at any rate, and studies the Markov perfect equilibria of the game.

The single-player version is a classical monotone follower problem of singular stochastic control (Alvarez 2001; Øksendal and Sulem 2005; Lon and Zervos 2011): the optimal policy reflects the stock upward at a threshold. In the game, a natural first guess is that free riding lowers that threshold, or that the players take turns reflecting. The paper shows instead that, in the symmetric game, there is an equilibrium in which both players contribute gradually, at a finite rate, below the same threshold as the single decision maker. The equilibrium is a continuous-state analogue of the mixed-strategy delay equilibrium of the war of attrition.

Setting

The stock ZtZ_tZt​ lives in an interval I=(a,b)⊆RI=(a,b)\subseteq\mathbb RI=(a,b)⊆R (a=−∞a=-\inftya=−∞ or b=∞b=\inftyb=∞ allowed) and satisfies

dZt=μ(Zt) dt+σ(Zt) dWt+dξ1t+dξ2t,dZ_t=\mu(Z_t)\,dt+\sigma(Z_t)\,dW_t+d\xi_{1t}+d\xi_{2t},dZt​=μ(Zt​)dt+σ(Zt​)dWt​+dξ1t​+dξ2t​,

on a filtered probability space satisfying the usual conditions, where WWW is a Wiener process, μ<0\mu<0μ<0 (the stock deteriorates) and σ>0\sigma>0σ>0. Player iii's control ξi\xi_iξi​ is any adapted, nondecreasing, right-continuous process: its cumulative contribution. A control may jump, including at time 000. Player iii's payoff from the initial stock xxx is

Vi(x;ξ)=Ex[∫0∞e−rtπ(Zt) dt−∫0∞e−rtk dξit],V_i(x;\xi)=\mathbb E^x\Big[\int_0^\infty e^{-rt}\pi(Z_t)\,dt-\int_0^\infty e^{-rt}k\,d\xi_{it}\Big],Vi​(x;ξ)=Ex[∫0∞​e−rtπ(Zt​)dt−∫0∞​e−rtkdξit​],

where π\piπ is an increasing, bounded-above flow profit, k>0k>0k>0 the unit cost and r>0r>0r>0 the discount rate. In the symmetric game both players have the same π\piπ and kkk.

The analysis uses:

  1. the uncontrolled process XxX^xXx, solving dX=μ(X)dt+σ(X)dWdX=\mu(X)dt+\sigma(X)dWdX=μ(X)dt+σ(X)dW, X0=xX_0=xX0​=x;
  2. the resolvent (Rg)(x)=E[∫0∞e−rtg(Xtx) dt](Rg)(x)=\mathbb E[\int_0^\infty e^{-rt}g(X^x_t)\,dt](Rg)(x)=E[∫0∞​e−rtg(Xtx​)dt];
  3. the generator A=12σ(x)2∂x2+μ(x)∂x−r\mathcal A=\tfrac12\sigma(x)^2\partial_x^2+\mu(x)\partial_x-rA=21​σ(x)2∂x2​+μ(x)∂x​−r;
  4. the increasing and decreasing fundamental solutions ψ,φ\psi,\varphiψ,φ of Aψ=Aφ=0\mathcal A\psi=\mathcal A\varphi=0Aψ=Aφ=0;
  5. the function q(x)=π(x)+[μ(x)−rx]kq(x)=\pi(x)+[\mu(x)-rx]kq(x)=π(x)+[μ(x)−rx]k.

Assumptions 1–3 of the paper require Lipschitz coefficients with linear growth, a uniform integrability condition on e−rτ(Xτ)−e^{-r\tau}(X_\tau)^-e−rτ(Xτ​)−, integrability of e−rtπ(Xt)e^{-rt}\pi(X_t)e−rtπ(Xt​), and boundary behaviour of RπR\piRπ and qqq at aaa and bbb; in particular qqq increases below a point x∗x^*x∗ and decreases above it.

The single decision maker's value is

V(x)={k(x−θ)+V(θ)x<θ,(Rπ)(x)+Aφ(x)x≥θ,(4)V(x)=\begin{cases}k(x-\theta)+V(\theta) & x<\theta,\\ (R\pi)(x)+A\varphi(x) & x\ge\theta,\end{cases}\tag{4}V(x)={k(x−θ)+V(θ)(Rπ)(x)+Aφ(x)​x<θ,x≥θ,​(4)

for a threshold θ∈I\theta\in Iθ∈I and a coefficient AAA that make VVV twice continuously differentiable (Lemma 1). The candidate equilibrium rate is

u(x)={−1k(AV(x)+π(x))x<θ,0x≥θ.(6)u(x)=\begin{cases}-\tfrac1k\big(\mathcal AV(x)+\pi(x)\big) & x<\theta,\\ 0 & x\ge\theta.\end{cases}\tag{6}u(x)={−k1​(AV(x)+π(x))0​x<θ,x≥θ.​(6)

Formalization targets

Goal: Theorem 2 (pp. 15–16)

If uuu of (6) is Lipschitz on III with linear growth, then the profile in which both players contribute at the regular rate dξit=u(Zt) dtd\xi_{it}=u(Z_t)\,dtdξit​=u(Zt​)dt is a Markov perfect equilibrium, and

V1(x;ξ)=V2(x;ξ)=V(x)for all x∈I.V_1(x;\xi)=V_2(x;\xi)=V(x)\qquad\text{for all }x\in I.V1​(x;ξ)=V2​(x;ξ)=V(x)for all x∈I.

The equilibrium is against all adapted deviations, from every initial state, with the opponent keeping its feedback rule uuu.

Milestones

  1. Proof of Lemma 1, part (i) (pp. 33–34): for VVV of (4) in C2(I)C^2(I)C2(I), AV+π=0\mathcal AV+\pi=0AV+π=0 on [θ,b)[\theta,b)[θ,b), AV+π<0\mathcal AV+\pi<0AV+π<0 on (a,θ)(a,\theta)(a,θ), V′=kV'=kV′=k on (a,θ](a,\theta](a,θ] and V′<kV'<kV′<k on (θ,b)(\theta,b)(θ,b).
  2. Lemma 1 (p. 10): such θ\thetaθ and AAA exist, and VVV is the single decision maker's optimal value, attained by reflection at θ\thetaθ.
  3. Theorem 1 (pp. 14–15), in the instance where both the opponent and the candidate contribute at regular feedback rates: a C2C^2C2, nondecreasing, bounded-above UUU satisfying conditions (iii)–(iv) is the candidate's payoff and dominates every deviation in the class Σi\Sigma_iΣi​.
  4. The optimality condition of §2.2 (p. 10), for VVV of the form (4) and the operator Aξj=12σ2∂x2+[μ+uj]∂x−r\mathcal A^{\xi_j}=\tfrac12\sigma^2\partial_x^2+[\mu+u_j]\partial_x-rAξj​=21​σ2∂x2​+[μ+uj​]∂x​−r of an opponent playing a regular rate uju_juj​ (as applied on p. 38): conditions (i)–(ii) make VVV the optimal value over all controls.

Significance

Theorem 2 says that the free-rider problem in this game does not shift the threshold below which the stock is maintained; it changes how the stock is maintained, from instantaneous reflection by one party to gradual, rate-limited contribution by both. The equilibrium value equals the single decision maker's value, so the players lose nothing relative to a single owner who pays for everything, although each pays only part. This contrasts with the asymmetric case, where the paper's Theorem 3 rules out a regular-control equilibrium with smooth payoffs. The result is one of the few explicit equilibria of a nonzero-sum singular-control game with linear costs.

The paper's proofs are on paper only. A formalization requires machine-checked versions of a verification theorem for one-dimensional singular control (the optimality condition), of the analysis of the free-boundary point θ\thetaθ through the fundamental solutions, and of the passage from best response within a restricted class Σi\Sigma_iΣi​ to best response among all adapted controls. The verification steps for a controlled diffusion with jumps, Itô's formula for semimartingales with a nondecreasing part, and the comparison Z≥XZ\ge XZ≥X with the uncontrolled process are reusable for other singular-control and monotone-follower problems on the platform.

Difficulty

The obvious route, Itô's formula applied to e−rtV(Zt)e^{-rt}V(Z_t)e−rtV(Zt​) along an arbitrary deviation, requires the transversality limit E[e−rtV(Zt)]→0\mathbb E[e^{-rt}V(Z_t)]\to0E[e−rtV(Zt​)]→0 and uniform integrability of the localised terms. VVV is unbounded below when a=−∞a=-\inftya=−∞, and the deviation is arbitrary, so this needs the comparison of every controlled state with the uncontrolled process and Assumption 1(ii). The proof also passes through a best-response theorem for the restricted class Σi\Sigma_iΣi​ (Theorem 1), whose conclusion is weaker than a Nash equilibrium; the upgrade to all of Ξi\Xi_iΞi​ is a separate argument. Finally, the identification of θ\thetaθ uses the boundary behaviour of ψ\psiψ, φ\varphiφ and the scale density at the ends of III, which Mathlib does not provide for general diffusions.

Formalization scope

Time is [0,∞)[0,\infty)[0,∞). The probabilistic data (measure, filtration, Wiener process, the uncontrolled family XxX^xXx, ψ\psiψ, φ\varphiφ) form one structure, and the standing assumptions of §2.1 together with Assumptions 1–3 form one predicate, a hypothesis of every theorem. The Itô integral of the state equation is the published relation EthierKurtz.HasBrownianItoIntegral; Mathlib supplies Brownian motion, stopping times, uniform integrability and Stieltjes measures.

Conventions the formalization commits to:

  1. The initial value xxx is the pre-jump value Z0−Z_{0-}Z0−​; the discounted cost is a Lebesgue–Stieltjes integral that counts the jump at time 000.
  2. Statements hold for every solution of the relevant state equation; existence and uniqueness of strong solutions (the paper's appeal to SDE theory) is not posed.
  3. Payoffs are compared only for admissible controls: finite expected discounted cost and integrable discounted running profit. Since π\piπ is bounded above, every other control has payoff −∞-\infty−∞, so no deviation is lost.
  4. Markov perfection is the best-response property from every initial state against the opponent's feedback rule, among all adapted controls.
  5. The fundamental solutions are pinned by the Laplace transforms of hitting times, E[e−rτy]=ψ(x)/ψ(y)\mathbb E[e^{-r\tau_y}]=\psi(x)/\psi(y)E[e−rτy​]=ψ(x)/ψ(y) for x≤yx\le yx≤y and φ(x)/φ(y)\varphi(x)/\varphi(y)φ(x)/φ(y) for y≤xy\le xy≤x (Borodin and Salminen).
  6. The scale density of Assumption 3(iii) uses a base point x0∈Ix_0\in Ix0​∈I in place of the printed 000, and the limits of Assumption 3 that may be infinite are limits in the extended reals.
  7. Added, and disclosed: e−rtq(Xtx)e^{-rt}q(X^x_t)e−rtq(Xtx​) is integrable, so that (Rq)(Rq)(Rq) of (3) exists, as the paper presupposes.
  8. The optimality condition is stated for VVV of the form (4) only: for an arbitrary C2C^2C2 function it is false (an affine V=kx+cV=kx+cV=kx+c with large ccc satisfies its conditions on I=RI=\mathbb RI=R but is unbounded).
  9. The class U\mathcal UU in Theorem 2 is its state-only version (Lipschitz on III with linear growth).

The threshold θ\thetaθ and coefficient AAA are not chosen by the formalization: the goal holds for every pair making VVV twice continuously differentiable on III, and smoothness at θ\thetaθ determines the pair. The rate uuu is computed from VVV through the generator, not supplied as a free function, and its nonnegativity is part of the conclusion. A payoff is never a Bochner integral of a non-integrable function, so no junk value can enter an equilibrium comparison.

Contributions welcome: proofs of the milestones, and reusable infrastructure for Itô's formula with nondecreasing càdlàg integrators, comparison theorems for one-dimensional SDEs, and the boundary classification of one-dimensional diffusions.

Selected references

  • H. Dharma Kwon, Game of Variable Contributions to the Common Good under Uncertainty, arXiv preprint, 2019 (published in Operations Research, 2022). https://arxiv.org/abs/1904.00500v1
  • A. N. Borodin and P. Salminen, Handbook of Brownian Motion — Facts and Formulae, Birkhäuser, 1996. https://doi.org/10.1007/978-3-0348-7652-0
  • L. H. R. Alvarez, Singular stochastic control, linear diffusions, and optimal stopping: A class of solvable problems, SIAM Journal on Control and Optimization 39(6), 1697–1710, 2001. https://doi.org/10.1137/S0363012900367825
  • L. H. R. Alvarez, On the properties of r-excessive mappings for a class of diffusions, Annals of Applied Probability 13, 1517–1533, 2003. https://doi.org/10.1214/aoap/1069786505
  • B. Øksendal and A. Sulem, Applied Stochastic Control of Jump Diffusions, 2nd ed., Springer (cited by the paper as 2005). https://doi.org/10.1007/978-3-540-69826-5
  • P. C. Lon and M. Zervos, A model for optimally advertising and launching a product, Mathematics of Operations Research 36(2), 363–376, 2011. https://doi.org/10.1287/moor.1110.0493
10 thms2 active usersReviewed
Machine LearningOperations ResearchStatistics·Captain: mikedeng1

Minimax-Optimal Policy Learning Under Unobserved Confounding: Minimizing the Worst-Case Empirical Regret Attains the Population Minimax Regret up to an Explicit n^(-1/2) TermResearch Paper

Motivation

Personalized decisions in medicine, marketing and public policy are increasingly learned from observational data: records of who received which treatment and how it turned out. Standard policy-learning methods assume unconfoundedness, that treatment assignment depends only on observed covariates. When an unobserved factor influences both the treatment and the outcome, these methods can return a policy that is worse than the status quo, and nothing in the data reveals it.

Kallus and Zhou (arXiv:1805.08593, published in Management Science 2021 as Minimax-Optimal Policy Learning Under Unobserved Confounding) take the robust route. They fix a bound Γ≥1\Gamma \ge 1Γ≥1 on how far the unobserved confounding may distort the propensity scores, in the marginal sensitivity model of Tan (2006), and learn the policy that minimizes the worst-case regret against a baseline policy π0\pi_0π0​ over every distortion the model allows. The paper proves two guarantees for this policy: it never does worse than the baseline up to vanishing terms (Theorem 2), and it is asymptotically minimax-optimal (Corollary 7). This mission is about the second.

Setting

Data are iid triples (X,T,Y)(X, T, Y)(X,T,Y): covariates X∈XX \in \mathcal XX∈X, one of m≥2m \ge 2m≥2 treatments T∈{0,…,m−1}T \in \{0, \dots, m-1\}T∈{0,…,m−1}, and a real outcome YYY, read as a loss. The nominal propensity is e~t(x)=P(T=t∣X=x)\tilde e_t(x) = P(T = t \mid X = x)e~t​(x)=P(T=t∣X=x). A policy π\piπ assigns to each xxx a probability vector π(⋅∣x)\pi(\cdot \mid x)π(⋅∣x) over treatments; Π\PiΠ is a class of policies and π0\pi_0π0​ a baseline.

Inverse propensity weights W(t,x,y)W(t,x,y)W(t,x,y) are unknown under confounding. The marginal sensitivity model with parameter Γ\GammaΓ confines them to the weight box

atΓ(x)≤W(t,x,y)≤btΓ(x),atΓ(x)=1+Γ−1(1e~t(x)−1),btΓ(x)=1+Γ(1e~t(x)−1).a^\Gamma_t(x) \le W(t,x,y) \le b^\Gamma_t(x), \qquad a^\Gamma_t(x) = 1 + \Gamma^{-1}\big(\tfrac{1}{\tilde e_t(x)} - 1\big), \quad b^\Gamma_t(x) = 1 + \Gamma\big(\tfrac{1}{\tilde e_t(x)} - 1\big).atΓ​(x)≤W(t,x,y)≤btΓ​(x),atΓ​(x)=1+Γ−1(e~t​(x)1​−1),btΓ​(x)=1+Γ(e~t​(x)1​−1).

The set of such weight functions is WΓ\mathcal W^\GammaWΓ, and its restriction to a sample of size nnn is the box WnΓ⊆Rn\mathcal W^\Gamma_n \subseteq \mathbb R^nWnΓ​⊆Rn.

For weights WWW, the Hájek regret of π\piπ against π0\pi_0π0​ is Rπ0(π;W)=∑t=0m−1Rπ0(t)(π;W)R_{\pi_0}(\pi; W) = \sum_{t=0}^{m-1} R^{(t)}_{\pi_0}(\pi; W)Rπ0​​(π;W)=∑t=0m−1​Rπ0​(t)​(π;W) with

Rπ0(t)(π;W)=E[I[T=t] (π(t∣X)−π0(t∣X)) W(T,X,Y) Y]E[I[T=t] W(T,X,Y)],R^{(t)}_{\pi_0}(\pi; W) = \frac{\mathbb E\big[\mathbb I[T=t]\,(\pi(t\mid X) - \pi_0(t\mid X))\, W(T,X,Y)\, Y\big]}{\mathbb E\big[\mathbb I[T=t]\, W(T,X,Y)\big]},Rπ0​(t)​(π;W)=E[I[T=t]W(T,X,Y)]E[I[T=t](π(t∣X)−π0​(t∣X))W(T,X,Y)Y]​,

and R^π0(π;W)\hat R_{\pi_0}(\pi; W)R^π0​​(π;W) is the same expression with E\mathbb EE replaced by the sample average En\mathbb E_nEn​. The worst-case regrets are

Rˉπ0(π;WΓ)=sup⁡W∈WΓRπ0(π;W),Rˉ^π0(π;WnΓ)=sup⁡W∈WnΓR^π0(π;W).\bar R_{\pi_0}(\pi; \mathcal W^\Gamma) = \sup_{W \in \mathcal W^\Gamma} R_{\pi_0}(\pi; W), \qquad \hat{\bar R}_{\pi_0}(\pi; \mathcal W^\Gamma_n) = \sup_{W \in \mathcal W^\Gamma_n} \hat R_{\pi_0}(\pi; W).Rˉπ0​​(π;WΓ)=W∈WΓsup​Rπ0​​(π;W),Rˉ^π0​​(π;WnΓ​)=W∈WnΓ​sup​R^π0​​(π;W).

The learned policy πˉ^\hat{\bar\pi}πˉ^ minimizes Rˉ^π0(⋅ ;WnΓ)\hat{\bar R}_{\pi_0}(\cdot\,; \mathcal W^\Gamma_n)Rˉ^π0​​(⋅;WnΓ​) over Π\PiΠ; the population minimax regret is inf⁡π∈ΠRˉπ0(π;WΓ)\inf_{\pi\in\Pi} \bar R_{\pi_0}(\pi; \mathcal W^\Gamma)infπ∈Π​Rˉπ0​​(π;WΓ).

The complexity of Π\PiΠ is measured by its VC-major dimension (Definition 1): the largest vvv such that some vvv points (tj,xj)(t_j, x_j)(tj​,xj​) have all 2v2^v2v subsets cut out by superlevel sets {(t,x):π(t∣x)>θ}\{(t,x) : \pi(t\mid x) > \theta\}{(t,x):π(t∣x)>θ}, π∈Π\pi \in \Piπ∈Π, θ∈R\theta \in \mathbb Rθ∈R. The standing assumptions are bounded outcomes ∣Y∣≤B|Y| \le B∣Y∣≤B (Assumption 1), overlap with constant ν>0\nu > 0ν>0 (Assumption 2), and VC-major dimension of Π\PiΠ at most vvv (Assumption 3).

Formalization targets

Goal: Corollary 7 (p. 15)

There is a constant KKK depending only on vvv such that, with probability at least 1−δ1-\delta1−δ,

Rˉπ0(πˉ^;WΓ)≤inf⁡π∈ΠRˉπ0(π;WΓ)+36(12+ν−1)(BK+ν−1(Γ−Γ−1)(K+B+m))log⁡(15m/δ)n.\bar R_{\pi_0}(\hat{\bar\pi}; \mathcal W^\Gamma) \le \inf_{\pi \in \Pi} \bar R_{\pi_0}(\pi; \mathcal W^\Gamma) + 36(12 + \nu^{-1})\big(BK + \nu^{-1}(\Gamma - \Gamma^{-1})(K + B + m)\big)\sqrt{\frac{\log(15m/\delta)}{n}}.Rˉπ0​​(πˉ^;WΓ)≤π∈Πinf​Rˉπ0​​(π;WΓ)+36(12+ν−1)(BK+ν−1(Γ−Γ−1)(K+B+m))nlog(15m/δ)​​.

Milestones

  1. Proposition 3 and Corollary 4: each treatment's worst case over the box is attained among monotone weights atΓ(x)+u(y(π(t∣x)−π0(t∣x)))(btΓ(x)−atΓ(x))a^\Gamma_t(x) + u\big(y(\pi(t\mid x) - \pi_0(t\mid x))\big)(b^\Gamma_t(x) - a^\Gamma_t(x))atΓ​(x)+u(y(π(t∣x)−π0​(t∣x)))(btΓ​(x)−atΓ​(x)), uuu nondecreasing into [0,1][0,1][0,1], in the population and in every sample.
  2. Lemma 5: sup⁡h−sup⁡g≤sup⁡(h−g)\sup h - \sup g \le \sup (h - g)suph−supg≤sup(h−g).
  3. Lemma 2: uniform deviation of (π(T∣X)−1/m)Y(\pi(T\mid X) - 1/m)Y(π(T∣X)−1/m)Y over Π\PiΠ, at rate 92CK(v+2)log⁡(5/δ)/n\tfrac92 C\sqrt K (v+2)\sqrt{\log(5/\delta)/n}29​CK​(v+2)log(5/δ)/n​.
  4. Lemma 3 and Corollary 15: for a fixed policy, uniform deviation over monotone uuu, at rate 92πlog⁡(1/p)/n9\sqrt{2\pi\log(1/p)/n}92πlog(1/p)/n​, overall and per treatment.
  5. Lemma 4: the same jointly over Π\PiΠ and uuu, given the VC-major dimension of the composition class.
  6. Theorem 6 (as proved): with probability at least 1−δ1-\delta1−δ, sup⁡π∈Π∣Rˉ^π0(π;WnΓ)−Rˉπ0(π;WΓ)∣\sup_{\pi\in\Pi} |\hat{\bar R}_{\pi_0}(\pi; \mathcal W^\Gamma_n) - \bar R_{\pi_0}(\pi; \mathcal W^\Gamma)|supπ∈Π​∣Rˉ^π0​​(π;WnΓ​)−Rˉπ0​​(π;WΓ)∣ is at most the goal's rate with 181818 in place of 363636.

Significance

The result. Corollary 7 says that the confounding-robust policy loses at most O(n−1/2)O(n^{-1/2})O(n−1/2) against the best possible worst-case guarantee in its class. The worst-case regret Rˉπ0(π;WΓ)\bar R_{\pi_0}(\pi; \mathcal W^\Gamma)Rˉπ0​​(π;WΓ) cannot be identified from data. It is the regret the decision maker must budget for when the confounding is only known to lie within Γ\GammaΓ. With Theorem 2, it makes the procedure both safe and asymptotically optimal among safe procedures, for randomized and multi-treatment policy classes of finite VC-major dimension.

Formalizing it. The paper's proof of the dimension-only dependence of KKK is incomplete. Its Proposition 5, which states that the monotone weight class WˉΓ=⋃π∈ΠWˉΓ(π)\bar{\mathcal W}^\Gamma = \bigcup_{\pi\in\Pi} \bar{\mathcal W}^\Gamma(\pi)WˉΓ=⋃π∈Π​WˉΓ(π) has finite VC-major dimension under Assumption 3, is false as printed. A class of monotone policies on [0,1][0,1][0,1] with VC-major dimension at most 222 gives a WˉΓ\bar{\mathcal W}^\GammaWˉΓ that shatters arbitrarily large grids. The printed proof of Theorem 6 runs through Proposition 5 and Lemma 4, so Theorem 6 and Corollary 7 are believed true but are not established by the paper. A formal proof would settle the claim. None of the statements has a machine-checked proof.

Difficulty

The worst case over WΓ\mathcal W^\GammaWΓ is a supremum over an essentially arbitrary bounded function class, which is far too large for a uniform law of large numbers. Proposition 3 reduces it to monotone transformations of the score y(π(t∣x)−π0(t∣x))y(\pi(t\mid x) - \pi_0(t\mid x))y(π(t∣x)−π0​(t∣x)). This is a linear-fractional program whose population version lives in a function space. The natural next step is to apply a uniform law over the pairs (π,u)(\pi, u)(π,u). That step needs a complexity bound on the composition u∘scoreπu \circ \text{score}_\piu∘scoreπ​ in terms of the dimension of Π\PiΠ alone, and this is exactly where the printed argument fails. A different route is needed. One candidate exploits the Lipschitz dependence of the worst-case Hájek value on the scores. The Hájek ratios also need denominators bounded away from zero uniformly. The paper's decomposition (p. 42) uses E[W I[T=t]]=1\mathbb E[W\,\mathbb I[T=t]] = 1E[WI[T=t]]=1, which holds for the true weights only.

Formalization scope

All statements live in the namespace ConfoundRobust.Minimax, with one definitions file Setting.

  • Data and sampling. An observation is a point of 𝒳 × Fin m × ℝ, with treatments 0-indexed as on the page. The population is a probability measure μ, and a sample is ω : Fin n → Obs 𝒳 m under Measure.pi. En\mathbb E_nEn​ is (1/n)∑i(1/n)\sum_i(1/n)∑i​.
  • Policies and propensity. A policy is π : 𝒳 → Fin m → ℝ, with π x t =π(t∣x)= \pi(t \mid x)=π(t∣x), measurable and simplex-valued. The nominal propensity is a measurable version of P(T=t∣X=x)P(T = t \mid X = x)P(T=t∣X=x), given by its defining integral identity, with ν≤e~≤1\nu \le \tilde e \le 1ν≤e~≤1.
  • Assumptions. Assumption 1 is ∣Y∣≤B|Y| \le B∣Y∣≤B almost surely. Assumption 2 enters only through its observable consequence e~t(x)≥ν\tilde e_t(x) \ge \nue~t​(x)≥ν; this is a weaker hypothesis, so the statements are at least as strong. Assumption 3 is the predicate "VC-major dimension at most vvv" on the functions (t,x)↦π(t∣x)(t,x) \mapsto \pi(t\mid x)(t,x)↦π(t∣x).
  • Weights and suprema. Weight functions in WΓ\mathcal W^\GammaWΓ are measurable. Suprema and infima are real sSup/sInf; the weight sets are nonempty (they contain 1/e~1/\tilde e1/e~) and the regrets are bounded, so these are true extrema. An empty treatment group gives a Hájek ratio 0/0=00/0 = 00/0=0.
  • Probability statements. "With probability at least 1−δ1-\delta1−δ" means a measurable event of that product measure on which the bound holds for every policy. πˉ^\hat{\bar\pi}πˉ^ is any sample minimizer.
  • Constants. In the goal, Theorem 6, Lemma 2 and Lemma 4 the constant KKK is quantified as ∀ v, ∃ K, ∀ (everything else). Letting KKK depend on Π\PiΠ, μ\muμ, nnn or δ\deltaδ would trivialize the bound and is ruled out.
  • Disclosed readings.
    • Lemmas 3, 4 and Corollary 15 are posed for p≤1/2p \le 1/2p≤1/2: as printed (every ppp) they are false for ppp near 111.
    • The clipped bounds of Corollary 15 and Lemma 4 (PDF p. 41) are reconstructed.
    • Lemma 2 drops "for nnn large enough", which its proof does not use.
    • Lemma 2, Theorem 6 and the goal assume Π\PiΠ is pointwise separable (a countable subclass approximates every policy pointwise), and Lemma 4 assumes the same of its composition class. This is the measurability condition of the empirical-process tools the proofs use. Without it the uniform statements fail (initial segments of ω1\omega_1ω1​ under the countable–cocountable measure).
    • Theorem 6 uses 181818, the constant its proof ends with. The goal's 363636 follows from it, but not from the printed Theorem 6.
    • The printed proof of Theorem 6 passes through Proposition 5, which is false as printed. Do not expect that route to work. Lemma 4 is kept as a statement about the composition class's own dimension.

A complete development needs: linear-fractional optimization over function boxes; Dudley-type entropy bounds for VC-major and VC-hull classes; the Dvoretzky–Kiefer–Wolfowitz inequality with Massart's constant (posed separately on the platform as MassartDKW.Tight.corollary_1); and a uniform bound for Hájek ratios. The empirical-process pieces (VC-major classes, monotone classes) are reusable well beyond this mission. Contributions to any milestone, and alternative routes to Theorem 6 that avoid Proposition 5, are welcome.

Selected references

  • N. Kallus and A. Zhou, Confounding-Robust Policy Improvement, arXiv:1805.08593v3, 2019; published as Minimax-Optimal Policy Learning Under Unobserved Confounding, Management Science, 2021. https://arxiv.org/abs/1805.08593v3
  • Z. Tan, A distributional approach for causal inference using propensity scores, Journal of the American Statistical Association 101(476), 2006. https://doi.org/10.1198/016214506000000023
  • P. Massart, The tight constant in the Dvoretzky–Kiefer–Wolfowitz inequality, Annals of Probability 18(3), 1990. https://doi.org/10.1214/aop/1176990746
  • A. W. van der Vaart and J. A. Wellner, Weak Convergence and Empirical Processes, Springer, 1996. https://doi.org/10.1007/978-1-4757-2545-2
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ProbabilityQuantum InformationStatistics·Captain: mikedeng1

Predicting Many Properties of a Quantum System from Very Few Measurements: Median of Means over Classical Shadows Predicts M Linear Properties to Error ε with Probability 1 − δResearch Paper

Motivation

Characterizing the state ρ\rhoρ of an nnn-qubit device is a basic task in quantum computing and simulation. Full quantum state tomography reconstructs ρ\rhoρ completely, but it needs a number of measurements exponential in nnn (Haah et al., 2017; O'Donnell–Wright, 2016). In practice one usually wants only a list of properties, such as the expectation values tr⁡(O1ρ),…,tr⁡(OMρ)\operatorname{tr}(O_1\rho),\dots,\operatorname{tr}(O_M\rho)tr(O1​ρ),…,tr(OM​ρ) of observables (fidelities with target states, entanglement witnesses, local energies). Aaronson's shadow tomography (Aaronson, 2018) showed that MMM such properties can be learned from a number of copies polylogarithmic in MMM, but with collective measurements across many copies that are far beyond present hardware.

Huang, Kueng and Preskill (arXiv:2002.08953, Nature Physics 16, 2020) gave a procedure that uses only single-copy randomized measurements: rotate ρ\rhoρ by a random unitary from a fixed ensemble, measure in the computational basis, and store the outcome classically. From these records, called classical shadows, a median-of-means estimator predicts all MMM properties at once. Their Theorem 1 bounds the number of measurements by O(log⁡M)O(\log M)O(logM) times a state-independent norm of the observables. The method has since become a standard tool for benchmarking and for estimating many observables in experiments.

Setting

Fix nnn qubits. Computational-basis labels are bit strings b∈{0,1}nb \in \{0,1\}^nb∈{0,1}n, and operators are 2n×2n2^n\times 2^n2n×2n complex matrices. A state is a positive semidefinite matrix of trace one.

A measurement primitive U\mathcal UU (Definition 1) is a finite ensemble of unitaries UiU_iUi​ drawn with probabilities wiw_iwi​. One snapshot of ρ\rhoρ draws iii with probability wiw_iwi​, applies ρ↦UiρUi†\rho\mapsto U_i\rho U_i^\daggerρ↦Ui​ρUi†​, and measures, obtaining bbb with probability ⟨b∣UiρUi†∣b⟩\langle b|U_i\rho U_i^\dagger|b\rangle⟨b∣Ui​ρUi†​∣b⟩ (S1). The primitive is tomographically complete if any two distinct states σ≠ρ\sigma\ne\rhoσ=ρ give different outcome probabilities ⟨b∣UiσUi†∣b⟩≠⟨b∣UiρUi†∣b⟩\langle b|U_i\sigma U_i^\dagger|b\rangle\ne\langle b|U_i\rho U_i^\dagger|b\rangle⟨b∣Ui​σUi†​∣b⟩=⟨b∣Ui​ρUi†​∣b⟩ for some bbb and some iii of positive weight.

The measurement channel (S2) is the linear map

M(X)=∑iwi∑b⟨b∣UiXUi†∣b⟩ Ui†∣b⟩⟨b∣Ui,\mathcal M(X)=\sum_i w_i\sum_{b}\langle b|U_iXU_i^\dagger|b\rangle\,U_i^\dagger|b\rangle\langle b|U_i ,M(X)=i∑​wi​b∑​⟨b∣Ui​XUi†​∣b⟩Ui†​∣b⟩⟨b∣Ui​,

and the classical shadow of the outcome (i,b)(i,b)(i,b) is ρ^=M−1(Ui†∣b⟩⟨b∣Ui)\hat\rho=\mathcal M^{-1}(U_i^\dagger|b\rangle\langle b|U_i)ρ^​=M−1(Ui†​∣b⟩⟨b∣Ui​) (S3). For an observable OOO the single-shadow prediction is o^=tr⁡(Oρ^)\hat o=\operatorname{tr}(O\hat\rho)o^=tr(Oρ^​). The shadow norm (S7) is

∥O∥shadow=max⁡σ state(∑iwi∑b⟨b∣UiσUi†∣b⟩ ⟨b∣UiM−1(O)Ui†∣b⟩2)1/2,\|O\|_{\mathrm{shadow}}=\max_{\sigma\ \text{state}}\Big(\sum_i w_i\sum_b\langle b|U_i\sigma U_i^\dagger|b\rangle\,\langle b|U_i\mathcal M^{-1}(O)U_i^\dagger|b\rangle^2\Big)^{1/2},∥O∥shadow​=σ statemax​(i∑​wi​b∑​⟨b∣Ui​σUi†​∣b⟩⟨b∣Ui​M−1(O)Ui†​∣b⟩2)1/2,

and O0=O−tr⁡(O)2nIO_0=O-\frac{\operatorname{tr}(O)}{2^n}\mathbb IO0​=O−2ntr(O)​I is the traceless part of OOO.

The median-of-means prediction (S12) takes NKNKNK independent snapshots, splits them into KKK batches of NNN, averages tr⁡(Oρ^j)\operatorname{tr}(O\hat\rho_j)tr(Oρ^​j​) within each batch, and outputs the median o^(N,K)\hat o(N,K)o^(N,K) of the KKK batch means.

Formalization targets

Goal: Theorem 1 (p. 13)

For Hermitian O1,…,OMO_1,\dots,O_MO1​,…,OM​, ϵ,δ∈(0,1]\epsilon,\delta\in(0,1]ϵ,δ∈(0,1] and integers

K≥2log⁡2Mδ,N≥34ϵ2max⁡1≤i≤M∥Oi,0∥shadow2,N≥1,K\ge 2\log\frac{2M}{\delta},\qquad N\ge\frac{34}{\epsilon^2}\max_{1\le i\le M}\big\|O_{i,0}\big\|_{\mathrm{shadow}}^2,\quad N\ge1,K≥2logδ2M​,N≥ϵ234​1≤i≤Mmax​​Oi,0​​shadow2​,N≥1,

the median-of-means predictions from NKNKNK independent classical shadows satisfy

Pr⁡[ ∣o^i(N,K)−tr⁡(Oiρ)∣≤ϵ  for all 1≤i≤M ] ≥ 1−δ.\Pr\Big[\,|\hat o_i(N,K)-\operatorname{tr}(O_i\rho)|\le\epsilon\ \text{ for all } 1\le i\le M\,\Big]\ \ge\ 1-\delta .Pr[∣o^i​(N,K)−tr(Oi​ρ)∣≤ϵ  for all 1≤i≤M] ≥ 1−δ.

Milestones

  1. Tomographic completeness makes M\mathcal MM invertible (p. 11).
  2. tr⁡(ρ^)=1\operatorname{tr}(\hat\rho)=1tr(ρ^​)=1 and E[ρ^]=ρ\mathbb E[\hat\rho]=\rhoE[ρ^​]=ρ (p. 11).
  3. E[o^]=tr⁡(Oρ)\mathbb E[\hat o]=\operatorname{tr}(O\rho)E[o^]=tr(Oρ), (S5).
  4. M−1\mathcal M^{-1}M−1 is self-adjoint for the trace pairing (p. 12).
  5. Lemma 1: Var⁡[o^]≤∥O0∥shadow2\operatorname{Var}[\hat o]\le\|O_0\|_{\mathrm{shadow}}^2Var[o^]≤∥O0​∥shadow2​, (S6).
  6. The median-of-means guarantee: for N≥34σ2/ϵ2N\ge34\sigma^2/\epsilon^2N≥34σ2/ϵ2, Pr⁡[∣μ^(N,K)−EX∣≥ϵ]≤2e−K/2\Pr[|\hat\mu(N,K)-\mathbb E X|\ge\epsilon]\le2e^{-K/2}Pr[∣μ^​(N,K)−EX∣≥ϵ]≤2e−K/2 (p. 13).
  7. The per-observable bound Pr⁡[∣o^i(N,K)−tr⁡(Oiρ)∣≥ϵ]≤δ/M\Pr[|\hat o_i(N,K)-\operatorname{tr}(O_i\rho)|\ge\epsilon]\le\delta/MPr[∣o^i​(N,K)−tr(Oi​ρ)∣≥ϵ]≤δ/M (p. 13).

The constants 343434, 222 and 2M/δ2M/\delta2M/δ are the paper's own. Remark 1 of the paper says they are chosen for simplicity, not tightness.

Significance

Theorem 1 gives a sample complexity NK=O(log⁡(M)max⁡i∥Oi,0∥shadow2/ϵ2)NK=O\big(\log(M)\max_i\|O_{i,0}\|^2_{\mathrm{shadow}}/\epsilon^2\big)NK=O(log(M)maxi​∥Oi,0​∥shadow2​/ϵ2). It grows only logarithmically in the number of properties and does not depend on the dimension 2n2^n2n except through the shadow norm. For random global Clifford measurements the shadow norm is at most 3tr⁡(O02)3\operatorname{tr}(O_0^2)3tr(O02​). For random single-qubit Pauli measurements it is at most 4k∥O∥∞24^{k}\|O\|_\infty^24k∥O∥∞2​ for an observable acting on kkk qubits (Propositions 1–3 of the paper). These instantiations are what make the protocol useful for fidelity estimation and for local observables. The theorem also separates two independent ingredients, a state-independent variance bound and a generic median-of-means concentration bound, and each is reusable.

The result is proved in the paper. As far as the platform's corpus shows, it has not been machine-checked. This mission produces a formal statement of the protocol and its guarantee, and its definitions (measurement channel, classical shadow, shadow norm) can be reused for the Clifford and Pauli instantiations and for the paper's quadratic-function estimator (Theorem 4).

Difficulty

The linear-algebra layer is elementary but has to be set up carefully. The channel must be shown invertible from completeness on states alone. Its inverse must be shown trace-preserving and self-adjoint, and the variance has to be rewritten as an expectation of squared diagonal entries.

The probabilistic layer is where the naive argument fails. Chebyshev's inequality on a single empirical mean gives a sample size proportional to 1/δ1/\delta1/δ, not log⁡(1/δ)\log(1/\delta)log(1/δ). Applying Hoeffding's inequality to the number of failing batches gives exponent 2K(1/2−1/34)2≈0.44K2K(1/2-1/34)^2\approx0.44K2K(1/2−1/34)2≈0.44K. That is weaker than K/2K/2K/2, so it does not reach the stated constant 2e−K/22e^{-K/2}2e−K/2. The bound needs the relative-entropy form of the Chernoff bound for a binomial tail, which Mathlib does not provide in this form. The median also has to be related to a count of deviating batch means without sign or tie errors.

Formalization scope

  • Model. Operators are Matrix (Fin n → Fin 2) (Fin n → Fin 2) ℂ. States are the published WildeQIT.IsDensityOperator.
  • Ensemble. The ensemble is finite: a published WildeQIT.FinDist of weights and a family in Matrix.unitaryGroup. The paper's ensemble is general, but both of its examples are finite with uniform weights. "U∈UU\in\mathcal UU∈U" in completeness means positive weight.
  • Channel and inverse. M\mathcal MM is a genuine C\mathbb CC-linear endomorphism and M−1\mathcal M^{-1}M−1 is Ring.inverse of it. Every statement using M−1\mathcal M^{-1}M−1 assumes tomographic completeness.
  • Real parts. Predictions and targets are real parts of traces, which are real for Hermitian observables.
  • Shadow norm. The maximum in (S7) is a real supremum over the nonempty, compact set of states, of a function bounded above.
  • Probability. The NKNKNK snapshots are modelled exactly. Probabilities are finite sums over all K×NK\times NK×N outcome arrays of the product of single-snapshot probabilities wi⟨b∣UiρUi†∣b⟩w_i\langle b|U_i\rho U_i^\dagger|b\ranglewi​⟨b∣Ui​ρUi†​∣b⟩, and batch kkk is row kkk of the array. The median-of-means milestone is stated for general real random variables in Mathlib's measure-theoretic language (independence, identical distribution, L2L^2L2).
  • Median. The median is the lower median.
  • Parameters. NNN and KKK are natural numbers at least the printed real values. N≥1N\ge1N≥1, ϵ>0\epsilon>0ϵ>0, δ>0\delta>0δ>0 and M≥1M\ge1M≥1 are added, because at ϵ=0\epsilon=0ϵ=0 or δ=0\delta=0δ=0 the printed values are undefined.

Theorem 1 must not be restated about an abstract estimator with a variance bound; that is milestone 6. The goal is about the median of means of classical shadows of a concrete primitive, with the shadow norm of (S7). Tomographic completeness is satisfiable non-trivially: the three single-qubit Pauli bases form a complete primitive, so the goal's hypotheses are not vacuous.

Needed infrastructure: elementary facts about the trace pairing and diagonal entries of UXU†U X U^\daggerUXU†; finite product measures, or direct finite-sum manipulations; Chebyshev's inequality; a binomial Chernoff bound in relative-entropy form; and order-statistic facts about the median. The binomial tail bound and the median-of-means lemma are independent of quantum information and reusable elsewhere. Contributions to any milestone are welcome. The Clifford and Pauli shadow-norm computations are natural follow-up work on top of these definitions.

Selected references

  • H.-Y. Huang, R. Kueng, J. Preskill, Predicting many properties of a quantum system from very few measurements, Nature Physics 16, 1050–1057 (2020); arXiv:2002.08953v2. https://arxiv.org/abs/2002.08953
  • S. Aaronson, Shadow tomography of quantum states, STOC 2018; SIAM J. Comput. 49 (2020). https://arxiv.org/abs/1711.01053
  • J. Haah, A. W. Harrow, Z. Ji, X. Wu, N. Yu, Sample-optimal tomography of quantum states, IEEE Trans. Inf. Theory 63 (2017). https://arxiv.org/abs/1508.01797
  • R. O'Donnell, J. Wright, Efficient quantum tomography, STOC 2016. https://arxiv.org/abs/1508.01907
  • M. R. Jerrum, L. G. Valiant, V. V. Vazirani, Random generation of combinatorial structures from a uniform distribution, Theoret. Comput. Sci. 43 (1986), 169–188. https://doi.org/10.1016/0304-3975(86)90174-X
  • A. S. Nemirovsky, D. B. Yudin, Problem Complexity and Method Efficiency in Optimization, Wiley (1983). (Jerrum–Valiant–Vazirani and Nemirovsky–Yudin are the paper's references [41, 55] for median of means.)
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Fast and fault-tolerant logical measurements: Auxiliary hypergraphs and transversal surgeryResearch Paper

Motivation

Fast and fault-tolerant logical measurements: Auxiliary hypergraphs and transversal surgery.

Target

Lemma 2.7

Let C∙,D∙C_\bullet,D_\bulletC∙​,D∙​ be finite based chain complexes over F2\mathbb F_2F2​, and let l∈Zl\in\mathbb Zl∈Z. Their tensor complex has differential ∂C⊗I+I⊗∂D\partial_C\otimes I+I\otimes\partial_D∂C​⊗I+I⊗∂D​. There exists an F2\mathbb F_2F2​-linear isomorphism

Hl(C∙⊗D∙)≅⨁i∈ZHi(C∙)⊗F2Hl−i(D∙).H_l(C_\bullet\otimes D_\bullet)\cong\bigoplus_{i\in\mathbb Z} H_i(C_\bullet)\otimes_{\mathbb F_2}H_{l-i}(D_\bullet).Hl​(C∙​⊗D∙​)≅i∈Z⨁​Hi​(C∙​)⊗F2​​Hl−i​(D∙​).

The direct sum is algebraic; the finite based complexes have only finitely many nonzero graded components. No particular isomorphism or representative map is asserted.

Lemma 3.2

Let binary check matrices HX,HZH_X,H_ZHX​,HZ​ satisfy HXHZT=0H_XH_Z^T=0HX​HZT​=0, and let DX,DZD_X,D_ZDX​,DZ​ be the prescribed pair-reading matrices of Eq. (2). Write LZ=ker⁡HX/im⁡HZTL_Z=\ker H_X/\operatorname{im}H_Z^TLZ​=kerHX​/imHZT​ and LX=ker⁡HZ/im⁡HXTL_X=\ker H_Z/\operatorname{im}H_X^TLX​=kerHZ​/imHXT​. Then

LZ(DX,DZ)≅LZ(HX,HZ),LX(DX,DZ)≅LX(HX,HZ).L_Z(D_X,D_Z)\cong L_Z(H_X,H_Z),\qquad L_X(D_X,D_Z)\cong L_X(H_X,H_Z).LZ​(DX​,DZ​)≅LZ​(HX​,HZ​),LX​(DX​,DZ​)≅LX​(HX​,HZ​).

The deformation of two identical memories therefore retains exactly kkk logical qubits, with no additional logical classes. All spaces and isomorphisms are over F2\mathbb F_2F2​.

Lemma 3.3

Let HX∈F2mX×nH_X\in\mathbb F_2^{m_X\times n}HX​∈F2mX​×n​ and HZ∈F2mZ×nH_Z\in\mathbb F_2^{m_Z\times n}HZ​∈F2mZ​×n​ satisfy HXHZT=0H_XH_Z^T=0HX​HZT​=0, and let P=(1  1)P=(1\;1)P=(11). In the product bases, the three coboundaries of the pair-reading deformation are

DXT=[I2⊗HXTP⊗ImX],DZT=[I2⊗HZTPT⊗In0I1⊗HX],DMT=[PT⊗ImZI1⊗HZT].D_X^T=\begin{bmatrix}I_2\otimes H_X^T\\P\otimes I_{m_X}\end{bmatrix},\quad D_Z^T=\begin{bmatrix}I_2\otimes H_Z^T&P^T\otimes I_n\\0&I_1\otimes H_X\end{bmatrix},\quad D_M^T=\begin{bmatrix}P^T\otimes I_{m_Z}\\I_1\otimes H_Z^T\end{bmatrix}.DXT​=[I2​⊗HXT​P⊗ImX​​​],DZT​=[I2​⊗HZT​0​PT⊗In​I1​⊗HX​​],DMT​=[PT⊗ImZ​​I1​⊗HZT​​].

Here old data precede new data, and old Z checks precede new Z checks; DMD_MDM​ denotes the metachecks. These are the explicit tensor-product differentials, retaining the final degree as in pp.21-22.

Lemma 3.4

Let HX,HZH_X,H_ZHX​,HZ​ define a binary CSS memory with X and Z distances at least d∈Nd\in\mathbb Nd∈N. Its prescribed pair-reading deformation has check matrices DX,DZD_X,D_ZDX​,DZ​ satisfying

dX(DX,DZ)≥d,dZ(DX,DZ)≥d.d_X(D_X,D_Z)\ge d,\qquad d_Z(D_X,D_Z)\ge d.dX​(DX​,DZ​)≥d,dZ​(DX​,DZ​)≥d.

A lower distance bound quantifies over every nontrivial normalizer class modulo stabilizers; the distance is infinite when no such class exists. This is a spatial code-distance assertion.

Lemma 3.8

Let HX,HZH_X,H_ZHX​,HZ​ define a binary CSS memory with both distances at least d∈Nd\in\mathbb Nd∈N. Let P∈F2r×cP\in\mathbb F_2^{r\times c}P∈F2r×c​ have full row rank and every row of Hamming weight greater than one. The prescribed Z-pattern deformation of ccc identical memories, with rmXr m_XrmX​ new data qubits indexed by pattern rows and memory X checks, satisfies

dX(DX,DZ)≥d,dZ(DX,DZ)≥d.d_X(D_X,D_Z)\ge d,\qquad d_Z(D_X,D_Z)\ge d.dX​(DX​,DZ​)≥d,dZ​(DX​,DZ​)≥d.

The conclusion includes CSS commutation and every nontrivial logical class. Sparsity belongs to the separate resource claim.

Theorem 7.8

Let G∈F2V×EG\in\mathbb F_2^{V\times E}G∈F2V×E​ be a finite incidence matrix, W≤F2VW\le\mathbb F_2^VW≤F2V​, and UUU its support union. Put DW(v)=min⁡w∈W∣(v∣U)+w∣D_W(v)=\min_{w\in W}\lvert(v|_U)+w\rvertDW​(v)=minw∈W​∣(v∣U​)+w∣, where restriction to UUU is zero extended and bars denote Hamming weight. For t,M>0t,M>0t,M>0, suppose ∣GTv∣≥Mmin⁡(t,DW(v))|G^Tv|\ge M\min(t,D_W(v))∣GTv∣≥Mmin(t,DW​(v)) for every binary vector vvv. Let the integer L≥1L\ge1L≥1 satisfy L≥1/ML\ge1/ML≥1/M, and form GL=[G⊗IL,IV⊗RL]G_L=[G\otimes I_L,I_V\otimes R_L]GL​=[G⊗IL​,IV​⊗RL​], with RLR_LRL​ the path incidence on LLL vertices. At any selected level ℓ<L\ell<Lℓ<L, embed WWW as WℓW_\ellWℓ​. Then

∣GLTv∣≥min⁡(t,DWℓ(v))for every v.|G_L^Tv|\ge\min(t,D_{W_\ell}(v))\quad\text{for every }v.∣GLT​v∣≥min(t,DWℓ​​(v))for every v.

Thus the thickening has certified modular expansion at least one at every choice of a single level. Cut certificates avoid asserting a largest finite expansion on degenerate inputs.

Lemma 7.9

Let G∈F2V×EG\in\mathbb F_2^{V\times E}G∈F2V×E​ be finite, let W≤F2VW\le\mathbb F_2^VW≤F2V​ contain ker⁡GT\ker G^TkerGT, and let t>0t>0t>0. Let UUU be the support union of WWW, and let DW(v)=min⁡w∈W∣(v∣U)+w∣D_W(v)=\min_{w\in W}\lvert(v|_U)+w\rvertDW​(v)=minw∈W​∣(v∣U​)+w∣, using zero-extended restriction and Hamming weight. Then

∣GTv∣≥t−1min⁡(t,DW(v))for all v.|G^Tv|\ge t^{-1}\min(t,D_W(v))\quad\text{for all }v.∣GTv∣≥t−1min(t,DW​(v))for all v.

Hence 1/t1/t1/t is a certified modular-expansion lower bound, even when no largest finite expansion exists.

Corollary 7.10

Let G∈F2V×EG\in\mathbb F_2^{V\times E}G∈F2V×E​ be finite and ker⁡GT⊆W≤F2V\ker G^T\subseteq W\le\mathbb F_2^VkerGT⊆W≤F2V​. For an integer t≥1t\ge1t≥1, form Gt=[G⊗It,IV⊗Rt]G_t=[G\otimes I_t,I_V\otimes R_t]Gt​=[G⊗It​,IV​⊗Rt​]. Embed WWW at any one level ℓ<t\ell<tℓ<t as WℓW_\ellWℓ​, and write UℓU_\ellUℓ​ for its support union. Then

∣GtTv∣≥min⁡{t,min⁡w∈Wℓ∣(v∣Uℓ)+w∣}for every v.|G_t^Tv|\ge\min\{t,\min_{w\in W_\ell}\lvert(v|_{U_\ell})+w\rvert\}\quad\text{for every }v.∣GtT​v∣≥min{t,w∈Wℓ​min​∣(v∣Uℓ​​)+w∣}for every v.

Restrictions are zero extended and weights are Hamming weights. Integer ttt-fold thickening thus certifies modular expansion one.

Lemma B.4

Let H∈F2m×nH\in\mathbb F_2^{m\times n}H∈F2m×n​ satisfy HHT=0HH^T=0HHT=0, defining a self-dual CSS code with HX=HZ=HH_X=H_Z=HHX​=HZ​=H. Let EEE isometrically encode all kkk logical qubits onto its entire codespace. Suppose matching binary supports vi∈ker⁡Hv_i\in\ker Hvi​∈kerH satisfy vi⋅vj=δijv_i\cdot v_j=\delta_{ij}vi​⋅vj​=δij​, and their physical X and Z products implement the corresponding logical Xi,ZiX_i,Z_iXi​,Zi​ through EEE. There exists a physical Pauli correction PPP, independent of the encoded state, such that

PS⊗nE=ES⊗k.P S^{\otimes n}E=E S^{\otimes k}.PS⊗nE=ES⊗k.

Here S=diag⁡(1,i)S=\operatorname{diag}(1,i)S=diag(1,i), and PPP includes its Pauli phase. The matrix equality holds on the entire encoded space, implementing S on every logical qubit.

§7

Let G∈F2V×EG\in\mathbb F_2^{V\times E}G∈F2V×E​ have finite nonempty vertex and edge sets, with every column weight at most ω∈N\omega\in\mathbb Nω∈N. Let t>0t>0t>0 and M,ρ∈RM,\rho\in\mathbb RM,ρ∈R. Write Mod(W,t,M)\mathrm{Mod}(W,t,M)Mod(W,t,M) for the modular cut inequality using the support union of WWW, and let 1U1_U1U​ indicate U⊆VU\subseteq VU⊆V. Then

Mod(⟨1U⟩,t,M) ⟺ ∣GTv∣≥Mmin⁡(t,∣v∩U∣,∣U∖v∣)(∀v).\mathrm{Mod}(\langle1_U\rangle,t,M)\ \Longleftrightarrow\ |G^Tv|\ge M\min(t,|v\cap U|,|U\setminus v|)\quad(\forall v).Mod(⟨1U​⟩,t,M) ⟺ ∣GTv∣≥Mmin(t,∣v∩U∣,∣U∖v∣)(∀v).

If t≥∣V∣t\ge|V|t≥∣V∣, the relative inequality at U=VU=VU=V is equivalent to global expansion ∣GTv∣≥Mmin⁡(∣v∣,∣V∣−∣v∣)|G^Tv|\ge M\min(|v|,|V|-|v|)∣GTv∣≥Mmin(∣v∣,∣V∣−∣v∣). If also the support union of ker⁡GT\ker G^TkerGT is all of VVV, then

Mod(ker⁡GT,t,ρ∣E∣/∣V∣) ⟺ ∣GTv∣∣E∣≥ρ∣V∣d(v,ker⁡GT)(∀v).\mathrm{Mod}(\ker G^T,t,\rho|E|/|V|)\ \Longleftrightarrow\ \frac{|G^Tv|}{|E|}\ge\frac{\rho}{|V|}d(v,\ker G^T)\quad(\forall v).Mod(kerGT,t,ρ∣E∣/∣V∣) ⟺ ∣E∣∣GTv∣​≥∣V∣ρ​d(v,kerGT)(∀v).

The last inequality, with locality ω\omegaω, is classical soundness ρ\rhoρ. The support condition implements the source's explicit U=VU=VU=V specialization.

AppendixA Eq4

Let f:A∙→C∙f:A_\bullet\to C_\bulletf:A∙​→C∙​ be a chain map of finite based binary complexes and i∈Zi\in\mathbb Zi∈Z. Let Hj(f)H_j(f)Hj​(f) be its induced homology map. Then

dim⁡Hi(cone⁡f)+rank⁡Hi(f)+rank⁡Hi−1(f)=dim⁡Hi(C)+dim⁡Hi−1(A).\dim H_i(\operatorname{cone}f)+\operatorname{rank}H_i(f)+\operatorname{rank}H_{i-1}(f)=\dim H_i(C)+\dim H_{i-1}(A).dimHi​(conef)+rankHi​(f)+rankHi−1​(f)=dimHi​(C)+dimHi−1​(A).

All dimensions are over F2\mathbb F_2F2​, and map images are constructed from fff. The addition form avoids truncated subtraction of natural dimensions.

AppendixA.1

Let C∙C_\bulletC∙​ be a finite binary CSS complex supported in degrees 0,1,20,1,20,1,2, and let ℓ>0\ell>0ℓ>0 be the repetition length. Let F=R⊗CF=R\otimes CF=R⊗C, and let FX′F'_XFX′​ be its prescribed two-endpoint cone. Let FdualF_{\rm dual}Fdual​ and FZ′F'_ZFZ′​ be the cochain-oriented bulk and cone obtained by the specified degree-reversing dual constructions. Put mX=dim⁡C0m_X=\dim C_0mX​=dimC0​ and mZ=dim⁡C2m_Z=\dim C_2mZ​=dimC2​. Then

dim⁡H1(FX′)+dim⁡H0(C)=dim⁡H1(F)+2mX,dim⁡H0(FX′)=0,dim⁡H2(FZ′)+dim⁡H2(C)=dim⁡H2(Fdual)+2mZ,dim⁡H3(FZ′)=0.\begin{aligned}\dim H_1(F'_X)+\dim H_0(C)&=\dim H_1(F)+2m_X,&\dim H_0(F'_X)&=0,\\\dim H_2(F'_Z)+\dim H_2(C)&=\dim H_2(F_{\rm dual})+2m_Z,&\dim H_3(F'_Z)&=0.\end{aligned}dimH1​(FX′​)+dimH0​(C)dimH2​(FZ′​)+dimH2​(C)​=dimH1​(F)+2mX​,=dimH2​(Fdual​)+2mZ​,​dimH0​(FX′​)dimH3​(FZ′​)​=0,=0.​

These retain all boundary homology classes, including immediately terminating classes. They imply no operational fault-distance bound by themselves.

Formalization scope

Only these reviewed original-paper statements are in scope. Definitions have reviewed bodies; target proofs remain open (sorry). Reviewed deferrals are excluded. No theorem proof or whole-paper formal proof is claimed.

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NLTS Hamiltonians from good quantum codesResearch Paper

Motivation

NLTS Hamiltonians from good quantum codes establishes the selected mathematical guarantees below. The mission turns those original paper results into precise Lean proof targets.

Setting

Fix positive clustering constants c1,c2,δ0c_1,c_2,\delta_0c1​,c2​,δ0​, a bound sss on the number of nonzero entries in each row and column of the binary check matrices, and a positive constant BBB bounding the total number of checks by BnBnBn. There exist a>0a>0a>0 and an integer n0≥2n_0\ge2n0​≥2, uniform over the code, state, energy density and preparing circuit, with the following property.

For n≥n0n\ge n_0n≥n0​, let Hx∈F2mx×nH_x\in\mathbb F_2^{m_x\times n}Hx​∈F2mx​×n​ and Hz∈F2mz×nH_z\in\mathbb F_2^{m_z\times n}Hz​∈F2mz​×n​ be check matrices with mx,mz>0m_x,m_z>0mx​,mz​>0, sparsity at most sss, and mx+mz≤Bnm_x+m_z\le Bnmx​+mz​≤Bn. Put Cx=ker⁡HxC_x=\ker H_xCx​=kerHx​ and Cz=ker⁡HzC_z=\ker H_zCz​=kerHz​, and assume the CSS condition Cx⊥⊆CzC_x^\perp\subseteq C_zCx⊥​⊆Cz​. Write kkk for the encoded dimension, and assume k≥2k\ge2k≥2. Assume Property 1: for every 0≤δ<δ00\le\delta<\delta_00≤δ<δ0​ and every y∈F2ny\in\mathbb F_2^ny∈F2n​, ∣Hzy∣≤δmz|H_z y|\le\delta m_z∣Hz​y∣≤δmz​ implies ∣y∣Cx⊥≤c1δn|y|_{C_x^\perp}\le c_1\delta n∣y∣Cx⊥​​≤c1​δn or ∣y∣Cx⊥≥c2n|y|_{C_x^\perp}\ge c_2n∣y∣Cx⊥​​≥c2​n, and the same implication holds with x,zx,zx,z interchanged. Here ∣y∣S=min⁡v∈S∣y+v∣|y|_S=\min_{v\in S}|y+v|∣y∣S​=minv∈S​∣y+v∣, and ∣⋅∣|\cdot|∣⋅∣ is Hamming weight. Define the unnormalized check Hamiltonian H=∑w row of Hx(I−Xw)/2+∑w row of Hz(I−Zw)/2H=\sum_{w\text{ row of }H_x}(I-X^w)/2+\sum_{w\text{ row of }H_z}(I-Z^w)/2H=∑w row of Hx​​(I−Xw)/2+∑w row of Hz​​(I−Zw)/2, counting all supplied rows.

Define

E(C)=1400c1min⁡{mx,mz}nmin⁡{(k−14n)2,δ0,c22}.E(C)=\frac{1}{400c_1}\frac{\min\{m_x,m_z\}}{n}\min\left\{\left(\frac{k-1}{4n}\right)^2,\delta_0,\frac{c_2}{2}\right\}.E(C)=400c1​1​nmin{mx​,mz​}​min{(4nk−1​)2,δ0​,2c2​​}.

The corrected permitted cutoff is

Eeff(C)=min⁡{E(C),δ0min⁡(mx,mz)/(400n)}.E_{\mathrm{eff}}(C)=\min\{E(C),\delta_0\min(m_x,m_z)/(400n)\}.Eeff​(C)=min{E(C),δ0​min(mx​,mz​)/(400n)}.

For every density matrix ρ\rhoρ and every 0≤ϵ<Eeff(C)0\le\epsilon<E_{\mathrm{eff}}(C)0≤ϵ<Eeff​(C),

tr⁡(Hρ)≤ϵn⟹depth⁡(U)≥alog⁡n\operatorname{tr}(H\rho)\le\epsilon n \quad\Longrightarrow\quad \operatorname{depth}(U)\ge a\log ntr(Hρ)≤ϵn⟹depth(U)≥alogn

for every preparing circuit UUU. A preparing circuit consists of layers of disjoint arbitrary one- and two-qubit unitary gates on n+wn+wn+w qubits, for any w≥0w\ge0w≥0, starts in ∣0⟩⊗(n+w)|0\rangle^{\otimes(n+w)}∣0⟩⊗(n+w), and has reduced output ρ\rhoρ on the first nnn qubits after discarding the other qubits. Depth is its number of layers; log⁡\loglog is the natural logarithm.

Moreover, for every fixed r,q>0r,q>0r,q>0, there exist e∗>0e_*>0e∗​>0 and n1≥2n_1\ge2n1​≥2, uniform over all code instances, such that whenever n≥n1n\ge n_1n≥n1​, k≥rnk\ge rnk≥rn and min⁡{mx,mz}≥qn\min\{m_x,m_z\}\ge qnmin{mx​,mz​}≥qn, one has

k≥2,Eeff(C)≥e∗.k\ge2,\qquad E_{\mathrm{eff}}(C)\ge e_*.k≥2,Eeff​(C)≥e∗​.

Consequently the allowed energy density can be chosen as a positive constant for the constant-rate, linear-distance qLDPC families satisfying Property 1 considered in the paper. The distance parameter does not enter the displayed cutoff; the paper's footnote 3 notes that Property 1 at δ=0\delta=0δ=0 already implies linear distance.

This gives a depth obstruction for every low-energy density matrix, including mixed states, rather than only ground states.

Source correction. The paper prints only ϵ<E(C)\epsilon<E(C)ϵ<E(C). Its proof uses Property 1 at 2ϵ12\epsilon_12ϵ1​ with ϵ1=200nϵ/min⁡(mx,mz)\epsilon_1=200n\epsilon/\min(m_x,m_z)ϵ1​=200nϵ/min(mx​,mz​), so we also require 400nϵ<δ0min⁡(mx,mz)400n\epsilon<\delta_0\min(m_x,m_z)400nϵ<δ0​min(mx​,mz​). This is exactly the missing domain condition; it is automatic if c1≥1c_1\ge1c1​≥1. No normalization c1≥1c_1\ge1c1​≥1 is imposed, and the frozen printed cutoff is retained as the first entry of the minimum.

Correction to the printed source.

Printed: Theorem 5 permits eps < E(C), where E(C) is the printed energyCutoff, for arbitrary positive c1.

Corrected: Use eps < min(E(C), delta0min(mx,mz)/(400n)); give the eventual positive floor for this same minimum. No other hypothesis, constant, or conclusion is changed.

Reason: The source proof sets epsilon1=200neps/min(mx,mz) on p.3 and applies Property 1 at 2epsilon1 on p.4. Its domain is delta<delta0, but the printed cutoff only supplies 2c1epsilon1<delta0. The additional strict upper bound is exactly 2epsilon1<delta0. It is redundant for c1>=1 and retains every c1<1 instance satisfying the actual proof-domain condition.

Target

Theorem 5 (Formal statement of the NLTS theorem), §2

Fix positive clustering constants c1,c2,δ0c_1,c_2,\delta_0c1​,c2​,δ0​, a bound sss on the number of nonzero entries in each row and column of the binary check matrices, and a positive constant BBB bounding the total number of checks by BnBnBn. There exist a>0a>0a>0 and an integer n0≥2n_0\ge2n0​≥2, uniform over the code, state, energy density and preparing circuit, with the following property.

For n≥n0n\ge n_0n≥n0​, let Hx∈F2mx×nH_x\in\mathbb F_2^{m_x\times n}Hx​∈F2mx​×n​ and Hz∈F2mz×nH_z\in\mathbb F_2^{m_z\times n}Hz​∈F2mz​×n​ be check matrices with mx,mz>0m_x,m_z>0mx​,mz​>0, sparsity at most sss, and mx+mz≤Bnm_x+m_z\le Bnmx​+mz​≤Bn. Put Cx=ker⁡HxC_x=\ker H_xCx​=kerHx​ and Cz=ker⁡HzC_z=\ker H_zCz​=kerHz​, and assume the CSS condition Cx⊥⊆CzC_x^\perp\subseteq C_zCx⊥​⊆Cz​. Write kkk for the encoded dimension, and assume k≥2k\ge2k≥2. Assume Property 1: for every 0≤δ<δ00\le\delta<\delta_00≤δ<δ0​ and every y∈F2ny\in\mathbb F_2^ny∈F2n​, ∣Hzy∣≤δmz|H_z y|\le\delta m_z∣Hz​y∣≤δmz​ implies ∣y∣Cx⊥≤c1δn|y|_{C_x^\perp}\le c_1\delta n∣y∣Cx⊥​​≤c1​δn or ∣y∣Cx⊥≥c2n|y|_{C_x^\perp}\ge c_2n∣y∣Cx⊥​​≥c2​n, and the same implication holds with x,zx,zx,z interchanged. Here ∣y∣S=min⁡v∈S∣y+v∣|y|_S=\min_{v\in S}|y+v|∣y∣S​=minv∈S​∣y+v∣, and ∣⋅∣|\cdot|∣⋅∣ is Hamming weight. Define the unnormalized check Hamiltonian H=∑w row of Hx(I−Xw)/2+∑w row of Hz(I−Zw)/2H=\sum_{w\text{ row of }H_x}(I-X^w)/2+\sum_{w\text{ row of }H_z}(I-Z^w)/2H=∑w row of Hx​​(I−Xw)/2+∑w row of Hz​​(I−Zw)/2, counting all supplied rows.

Define

E(C)=1400c1min⁡{mx,mz}nmin⁡{(k−14n)2,δ0,c22}.E(C)=\frac{1}{400c_1}\frac{\min\{m_x,m_z\}}{n}\min\left\{\left(\frac{k-1}{4n}\right)^2,\delta_0,\frac{c_2}{2}\right\}.E(C)=400c1​1​nmin{mx​,mz​}​min{(4nk−1​)2,δ0​,2c2​​}.

The corrected permitted cutoff is

Eeff(C)=min⁡{E(C),δ0min⁡(mx,mz)/(400n)}.E_{\mathrm{eff}}(C)=\min\{E(C),\delta_0\min(m_x,m_z)/(400n)\}.Eeff​(C)=min{E(C),δ0​min(mx​,mz​)/(400n)}.

For every density matrix ρ\rhoρ and every 0≤ϵ<Eeff(C)0\le\epsilon<E_{\mathrm{eff}}(C)0≤ϵ<Eeff​(C),

tr⁡(Hρ)≤ϵn⟹depth⁡(U)≥alog⁡n\operatorname{tr}(H\rho)\le\epsilon n \quad\Longrightarrow\quad \operatorname{depth}(U)\ge a\log ntr(Hρ)≤ϵn⟹depth(U)≥alogn

for every preparing circuit UUU. A preparing circuit consists of layers of disjoint arbitrary one- and two-qubit unitary gates on n+wn+wn+w qubits, for any w≥0w\ge0w≥0, starts in ∣0⟩⊗(n+w)|0\rangle^{\otimes(n+w)}∣0⟩⊗(n+w), and has reduced output ρ\rhoρ on the first nnn qubits after discarding the other qubits. Depth is its number of layers; log⁡\loglog is the natural logarithm.

Moreover, for every fixed r,q>0r,q>0r,q>0, there exist e∗>0e_*>0e∗​>0 and n1≥2n_1\ge2n1​≥2, uniform over all code instances, such that whenever n≥n1n\ge n_1n≥n1​, k≥rnk\ge rnk≥rn and min⁡{mx,mz}≥qn\min\{m_x,m_z\}\ge qnmin{mx​,mz​}≥qn, one has

k≥2,Eeff(C)≥e∗.k\ge2,\qquad E_{\mathrm{eff}}(C)\ge e_*.k≥2,Eeff​(C)≥e∗​.

Consequently the allowed energy density can be chosen as a positive constant for the constant-rate, linear-distance qLDPC families satisfying Property 1 considered in the paper. The distance parameter does not enter the displayed cutoff; the paper's footnote 3 notes that Property 1 at δ=0\delta=0δ=0 already implies linear distance.

This gives a depth obstruction for every low-energy density matrix, including mixed states, rather than only ground states.

Source correction. The paper prints only ϵ<E(C)\epsilon<E(C)ϵ<E(C). Its proof uses Property 1 at 2ϵ12\epsilon_12ϵ1​ with ϵ1=200nϵ/min⁡(mx,mz)\epsilon_1=200n\epsilon/\min(m_x,m_z)ϵ1​=200nϵ/min(mx​,mz​), so we also require 400nϵ<δ0min⁡(mx,mz)400n\epsilon<\delta_0\min(m_x,m_z)400nϵ<δ0​min(mx​,mz​). This is exactly the missing domain condition; it is automatic if c1≥1c_1\ge1c1​≥1. No normalization c1≥1c_1\ge1c1​≥1 is imposed, and the frozen printed cutoff is retained as the first entry of the minimum.

Correction to the printed source.

Printed: Theorem 5 permits eps < E(C), where E(C) is the printed energyCutoff, for arbitrary positive c1.

Corrected: Use eps < min(E(C), delta0min(mx,mz)/(400n)); give the eventual positive floor for this same minimum. No other hypothesis, constant, or conclusion is changed.

Reason: The source proof sets epsilon1=200neps/min(mx,mz) on p.3 and applies Property 1 at 2epsilon1 on p.4. Its domain is delta<delta0, but the printed cutoff only supplies 2c1epsilon1<delta0. The additional strict upper bound is exactly 2epsilon1<delta0. It is redundant for c1>=1 and retains every c1<1 instance satisfying the actual proof-domain condition.

Significance

These are known results from the cited paper. The current contribution consists of source-reviewed, compiler-checked theorem statements and mathematical definitions. Formal proofs remain open. Only the listed selected results are in scope; no whole-paper completeness is claimed.

Difficulty

A complete solution must establish every quantified conclusion under the exact stated hypotheses, including error, probability and resource conditions wherever present. The source assumptions and conventions are recorded in the attached statements and independent readbacks.

Formalization scope

Definitions preserve the existing reviewed Lean interfaces. Every target proof is currently sorry, so each target is Open. Printed-source corrections, where necessary, are labeled with the printed claim, the change and its reason.

Selected references

  • NLTS Hamiltonians from good quantum codes, arXiv:2206.13228v4. Exact result labels, PDF pages and source SHA-256 values accompany each theorem.

Additional independently reviewed proof targets

Theorem 1: No low-energy trivial states

There is a deterministically explicit family of binary CSS check descriptions on nnn qubits, and constants ϵ,c,a,b>0\epsilon,c,a,b>0ϵ,c,a,b>0, a locality bound sss, and a threshold n0≥1n_0\ge1n0​≥1, all independent of nnn. Explicit means that a deterministic polynomial-time function on unary nnn outputs the actual row counts and both binary check matrices. For every n≥1n\ge1n≥1, both check matrices have row and column weights at most sss, their total row count mnm_nmn​ satisfies an≤mn≤bnan\le m_n\le bnan≤mn​≤bn, and their associated projector terms hi=(I−Xwi)/2h_i=(I-X^{w_i})/2hi​=(I−Xwi​)/2 or (I−Zwi)/2(I-Z^{w_i})/2(I−Zwi​)/2 act on at most sss qubits, commute, and annihilate a common unit vector. Let Hn=∑ihiH_n=\sum_i h_iHn​=∑i​hi​ be this unnormalized Hamiltonian. Every circuit PPP of parallel one- and two-qubit unitaries on disjoint wires, starting from zero qubits and allowing arbitrary clean ancillas and discarded qubits, has an output density operator ρP\rho_PρP​ satisfying, for n≥n0n\ge n_0n≥n0​,

Tr⁡(HnρP)<ϵn⟹depth⁡(P)≥cln⁡n.\operatorname{Tr}(H_n\rho_P)<\epsilon n \quad\Longrightarrow\quad \operatorname{depth}(P)\ge c\ln n.Tr(Hn​ρP​)<ϵn⟹depth(P)≥clnn.

This is the existence of an NLTS Hamiltonian family. Quantifying over every preparation circuit gives the lower bound for mixed as well as pure low-energy states.

Formalization Note The deterministic interpretation of explicit and the CSS witness implementation are recorded for independent moderation; the theorem does not assume an NLTS guarantee on its family.

Section 2: support of both measurement distributions

Let HX,HZH_X,H_ZHX​,HZ​ be a binary CSS check presentation with n,mx,mz>0n,m_x,m_z>0n,mx​,mz​>0, and let ρ\rhoρ be any density operator with Tr⁡(Hρ)≤ϵn\operatorname{Tr}(H\rho)\le\epsilon nTr(Hρ)≤ϵn, where ϵ≥0\epsilon\ge0ϵ≥0 and HHH is the sum of the actual check projectors. Write Dz,DxD_z,D_xDz​,Dx​ for its standard- and product-Hadamard-basis distributions and GbδG_b^\deltaGbδ​ for the words violating at most a δ\deltaδ fraction of the actual checks on side bbb. For every ϵ1>0\epsilon_1>0ϵ1​>0,

Dz(Gzϵ1)≥1−ϵnϵ1mz,Dx(Gxϵ1)≥1−ϵnϵ1mx.D_z(G_z^{\epsilon_1})\ge1-\frac{\epsilon n}{\epsilon_1m_z}, \qquad D_x(G_x^{\epsilon_1})\ge1-\frac{\epsilon n}{\epsilon_1m_x}.Dz​(Gzϵ1​​)≥1−ϵ1​mz​ϵn​,Dx​(Gxϵ1​​)≥1−ϵ1​mx​ϵn​.

If ϵ=0\epsilon=0ϵ=0, both Gz0G_z^0Gz0​ and Gx0G_x^0Gx0​ have probability one. If ϵ>0\epsilon>0ϵ>0, choosing ϵ1=200nϵ/min⁡(mx,mz)\epsilon_1=200n\epsilon/\min(m_x,m_z)ϵ1​=200nϵ/min(mx​,mz​) gives both masses at least 199/200199/200199/200.

These bounds place low-energy measurement outcomes in the approximate classical codes. The energy identity and probability bounds are conclusions of the source argument, not hypotheses of the formal statement.

Section 2: equivalence classes and separated clusters

Let CX=ker⁡HXC_X=\ker H_XCX​=kerHX​ and CZ=ker⁡HZC_Z=\ker H_ZCZ​=kerHZ​ be a binary CSS pair satisfying Property 1 with positive constants c1,c2,δ0c_1,c_2,\delta_0c1​,c2​,δ0​. Assume ϵ1≥0\epsilon_1\ge0ϵ1​≥0, 2ϵ1<δ02\epsilon_1<\delta_02ϵ1​<δ0​, and 4c1ϵ1<c24c_1\epsilon_1<c_24c1​ϵ1​<c2​. On Gzϵ1G_z^{\epsilon_1}Gzϵ1​​ define x∼zyx\sim_z yx∼z​y when ∣x+y∣CX⊥≤2c1ϵ1n|x+y|_{C_X^\perp}\le2c_1\epsilon_1n∣x+y∣CX⊥​​≤2c1​ϵ1​n, with the corresponding definition on Gxϵ1G_x^{\epsilon_1}Gxϵ1​​ modulo CZ⊥C_Z^\perpCZ⊥​. Here ∣v∣S=min⁡s∈S∣v+s∣|v|_S=\min_{s\in S}|v+s|∣v∣S​=mins∈S​∣v+s∣. For either basis this is an equivalence relation. Its distinct computed classes are nonempty, pairwise disjoint, and cover the corresponding approximate code. Distinct classes satisfy

x∈B, y∈B′, B≠B′⟹∣x−y∣≥c2n.x\in B,\ y\in B',\ B\ne B'\quad\Longrightarrow\quad |x-y|\ge c_2n.x∈B, y∈B′, B=B′⟹∣x−y∣≥c2​n.

This constructs the separated clusters needed for the depth argument.

Formalization Note The strict domain follows Property 1 on page 2; the page-4 prose writes a non-strict endpoint. The classes are computed from the relation rather than supplied with a separation guarantee.

Correction to the printed source.

Printed: Page 4 says 'assuming 2 epsilon1 <= delta0', but Property 1 on page 2 is stated only for delta < delta0.

Corrected: Use 0 <= epsilon1 and the strict inequality 2 epsilon1 < delta0 in the clustering regime.

Reason: The proof invokes Property 1 at delta = 2 epsilon1; the strict domain is necessary. This is a standing-domain clarification pending independent moderation.

Lemma 2: one basis has no highly concentrated cluster

Consider a binary CSS presentation with n,mx,mz>0n,m_x,m_z>0n,mx​,mz​>0 and logical dimension k≥1k\ge1k≥1, satisfying Property 1 with c1,c2,δ0>0c_1,c_2,\delta_0>0c1​,c2​,δ0​>0. Let ρ\rhoρ be any density operator. Assume ϵ1≥0\epsilon_1\ge0ϵ1​≥0, 2ϵ1<δ02\epsilon_1<\delta_02ϵ1​<δ0​, 4c1ϵ1<c24c_1\epsilon_1<c_24c1​ϵ1​<c2​, and

2c1ϵ1≤(k−14n)2.2c_1\epsilon_1\le\left(\frac{k-1}{4n}\right)^2.2c1​ϵ1​≤(4nk−1​)2.

For the computed clusters in the preceding result, either every standard-basis cluster has DzD_zDz​-mass strictly less than 99/10099/10099/100, or every Hadamard-basis cluster has DxD_xDx​-mass strictly less than 99/10099/10099/100.

This uncertainty consequence selects a basis in which no single cluster captures almost all probability. It requires no low-energy hypothesis once the clusters are defined.

Formalization Note The subtraction k−1k-1k−1 takes place in the reals. The positive-kkk reading comes from the section's positive-rate setting and is flagged for independent moderation.

Correction to the printed source.

Printed: The displayed finite lemma does not explicitly say k>=1, while Section 2 is introduced for constant-rate code families.

Corrected: State the finite lemma for k>=1 and n,mx,mz>0, keeping ((k-1)/(4n))^2 with real subtraction.

Reason: The proof uses a positive logical dimension; at k=0 the zero-radius clusters can concentrate in both bases. The finite positive-rate reading requires independent moderation.

Fact 3: uncertainty for subsets in conjugate bases

Let ρ\rhoρ be any nnn-qubit density operator, and let Dz,DxD_z,D_xDz​,Dx​ be its standard- and product-Hadamard-basis measurement distributions. For all sets S,T⊆{0,1}nS,T\subseteq\{0,1\}^nS,T⊆{0,1}n,

Dx(T)≤21−Dz(S)+∣S∣∣T∣2n.D_x(T)\le2\sqrt{1-D_z(S)}+\frac{|S||T|}{2^n}.Dx​(T)≤21−Dz​(S)​+2n∣S∣∣T∣​.

This bounds concentration in conjugate bases and applies to mixed states. No positive-mass hypothesis on SSS is required; empty sets and n=0n=0n=0 are allowed.

Section 2: positive-mass separated unions

Let a binary CSS presentation on n>0n>0n>0 qubits satisfy Property 1 with c1,c2,δ0>0c_1,c_2,\delta_0>0c1​,c2​,δ0​>0, and assume ϵ1≥0\epsilon_1\ge0ϵ1​≥0, 2ϵ1<δ02\epsilon_1<\delta_02ϵ1​<δ0​, and 4c1ϵ1<c24c_1\epsilon_1<c_24c1​ϵ1​<c2​. Fix either basis and any density operator ρ\rhoρ. Suppose its measurement distribution DDD gives the approximate-code set mass at least 199/200199/200199/200, while each computed class has mass less than 99/10099/10099/100. Then there are disjoint subcollections M,M′M,M'M,M′ of the computed classes whose unions S,S′S,S'S,S′ are disjoint and satisfy

D(S)≥1400,D(S′)≥1400,∣x−y∣≥c2n(x∈S, y∈S′).D(S)\ge\frac1{400},\qquad D(S')\ge\frac1{400}, \qquad |x-y|\ge c_2n\quad(x\in S,\ y\in S').D(S)≥4001​,D(S′)≥4001​,∣x−y∣≥c2​n(x∈S, y∈S′).

This extracts two positive-mass separated sets in whichever basis Lemma 2 selects. Both probability constants and the cross-union separation are retained.

Fact 4: depth lower bound for well-spread distributions

Let PPP be a circuit of depth ttt consisting of layers of disjoint one- and two-qubit unitaries, starting in the all-zero product state. Allow any number of clean ancillas and measure only its n>0n>0n>0 output qubits in the standard basis, giving distribution DDD. Let 0<μ<10<\mu<10<μ<1, and suppose D(S),D(T)≥μD(S),D(T)\ge\muD(S),D(T)≥μ. For any u≥0u\ge0u≥0 such that every x∈S,y∈Tx\in S,y\in Tx∈S,y∈T has Hamming distance at least uuu,

u2≤400nln⁡(1/μ) 23t.u^2\le400n\ln(1/\mu)\,2^{3t}.u2≤400nln(1/μ)23t.

For positive set distance this is equivalently t≥13log⁡2(dist⁡(S,T)2/(400nln⁡(1/μ)))t\ge\frac13\log_2(\operatorname{dist}(S,T)^2/(400n\ln(1/\mu)))t≥31​log2​(dist(S,T)2/(400nln(1/μ))).

This is the quantitative circuit-depth obstruction for well-spread output distributions. The exponential formulation also covers overlapping sets without taking the logarithm of zero; the original circuit's workspace is unrestricted.

Lemma 8: expansion implies clustering

Let A∈F2m×nA\in\mathbb F_2^{m\times n}A∈F2m×n​ and V⊆F2nV\subseteq\mathbb F_2^nV⊆F2n​. Let δ>0\delta>0δ>0 and 0<μ<ν0<\mu<\nu0<μ<ν. Suppose every x∈Vx\in Vx∈V with ∣x∣≤νn|x|\le\nu n∣x∣≤νn satisfies ∣Ax∣≥(δ/μ)∣x∣|Ax|\ge(\delta/\mu)|x|∣Ax∣≥(δ/μ)∣x∣. Then

x∈V,∣Ax∣≤δn⟹∣x∣≤μn or ∣x∣≥νn.x\in V,\quad |Ax|\le\delta n \quad\Longrightarrow\quad |x|\le\mu n\ \text{or}\ |x|\ge\nu n.x∈V,∣Ax∣≤δn⟹∣x∣≤μn or ∣x∣≥νn.

This transfers small-set expansion to the clustering dichotomy. Both the size cutoff and syndrome cutoff use the number of columns nnn, even for rectangular matrices.

Formalization Note Positivity is taken from the proof and the paragraph immediately following Lemma 8; the unsupported zero-δ\deltaδ extension is excluded.

Correction to the printed source.

Printed: The displayed Lemma 8 omits its parameter domain; its proof uses delta>0 and mu>0 and the following paragraph takes mu<nu.

Corrected: State Lemma 8 on the meaningful positive regime delta>0 and 0<mu<nu, as pinned by the plan and proof.

Reason: For delta=0, an expansion hypothesis with beta=0 supplies no information and the claimed nontrivial dichotomy can fail. Independent moderation must confirm the intended domain.

Section 3: minimal-representative expansion implies Property 1

Let FFF be a family of binary CSS check presentations. Fix positive αx,βx,αz,βz,δˉ,a,b\alpha_x,\beta_x,\alpha_z,\beta_z,\bar\delta,a,bαx​,βx​,αz​,βz​,δˉ,a,b and n0≥1n_0\ge1n0​≥1. For all n≥n0n\ge n_0n≥n0​, suppose an≤mx(n),mz(n)≤bnan\le m_x(n),m_z(n)\le bnan≤mx​(n),mz​(n)≤bn. For every 0≤δ<δˉ0\le\delta<\bar\delta0≤δ<δˉ, define VzδV_z^\deltaVzδ​ as the words in GzδG_z^\deltaGzδ​ of minimum Hamming weight within their coset modulo CX⊥C_X^\perpCX⊥​, and define VxδV_x^\deltaVxδ​ analogously modulo CZ⊥C_Z^\perpCZ⊥​. Assume HXH_XHX​ is (αx,βx)(\alpha_x,\beta_x)(αx​,βx​)-expanding on VxδV_x^\deltaVxδ​ and HZH_ZHZ​ is (αz,βz)(\alpha_z,\beta_z)(αz​,βz​)-expanding on VzδV_z^\deltaVzδ​. Then there are constants c1,c2,δ0>0c_1,c_2,\delta_0>0c1​,c2​,δ0​>0, independent of nnn, such that for all n≥n0n\ge n_0n≥n0​ and 0≤δ<δ00\le\delta<\delta_00≤δ<δ0​,

y∈Gzδ⟹∣y∣CX⊥≤c1δn or ∣y∣CX⊥≥c2n,y\in G_z^\delta\Longrightarrow |y|_{C_X^\perp}\le c_1\delta n\ \text{or}\ |y|_{C_X^\perp}\ge c_2n,y∈Gzδ​⟹∣y∣CX⊥​​≤c1​δn or ∣y∣CX⊥​​≥c2​n,

and the same dichotomy holds on the XXX side modulo CZ⊥C_Z^\perpCZ⊥​.

This derives Property 1 from uniform expansion of minimal representatives, without assuming the desired dichotomy. The check-density factors converting δmside\delta m_{\rm side}δmside​ to a threshold relative to nnn are retained.

These additional statements have current no-edit source review. Their formal proofs remain open; deferred results are excluded.

13 thms2 active usersReviewed
Mathematical Physics·Captain: Lucas

Wigner quasiprobability: nonnegativity and Hudson's theoremTextbook

Motivation

Classical statistical mechanics describes a particle by a probability density on phase space; quantum mechanics replaces this by a wavefunction, and the uncertainty principle forbids any honest probability interpretation of simultaneous position and momentum. In 1932, Eugene Wigner introduced the transform that has become the standard way of placing quantum states on classical phase space anyway: a quasiprobability distribution W(x,p)W(x, p)W(x,p), defined by an explicit integral formula, whose marginals reproduce the Born position and momentum distributions of the wavefunction (Wigner 1932). Unlike a probability density, WWW generally takes negative values, and this negativity is the standard marker of genuinely quantum behavior — of interference — in quantum optics, quantum information, and the study of the quantum-to-classical transition.

The central question about the probabilistic character of WWW is: which quantum states have an everywhere nonnegative Wigner function? Hudson's theorem (1974) gives the complete answer in one dimension: only Gaussian wave packets (Hudson 1974). This mission formalizes the definition, the basic properties, and the positivity characterization of the Wigner function, following the source text, the Wikipedia article Wigner quasiprobability distribution (oldid 1376057304).

Timeline of the key results:

  • 1932 — E. Wigner introduces the distribution to study quantum corrections to thermodynamic equilibrium (Physical Review 40, 749).
  • 1946 — H. J. Groenewold computes the Wigner function of the mmm-th Fock (number) state, this mission's key worked example (Physica 12, 405).
  • 1949 — J. E. Moyal recognizes WWW as the moment-generating functional of quantum mechanics in phase space (Proc. Camb. Phil. Soc. 45, 99).
  • 1974 — R. L. Hudson proves that Gaussian pure states are the only pure states with nonnegative Wigner function in one dimension (Rep. Math. Phys. 6, 249).
  • 1983 — F. Soto and P. Claverie extend the characterization to arbitrary dimension via the Segal–Bargmann transform (J. Math. Phys. 24, 97).

Setting

A wavefunction is a function ψ:R→C\psi : \mathbb{R} \to \mathbb{C}ψ:R→C, and ℏ>0\hbar > 0ℏ>0 denotes the reduced Planck constant. The Wigner function of ψ\psiψ at the phase-space point (x,p)∈R2(x, p) \in \mathbb{R}^2(x,p)∈R2 is

W(x,p)=1πℏ∫−∞∞ψ(x+y)‾ ψ(x−y) e 2ipy/ℏ dy,W(x, p) = \frac{1}{\pi \hbar} \int_{-\infty}^{\infty} \overline{\psi(x+y)}\, \psi(x-y)\, e^{\,2ipy/\hbar}\, dy,W(x,p)=πℏ1​∫−∞∞​ψ(x+y)​ψ(x−y)e2ipy/ℏdy,

a Lebesgue (Bochner) integral over yyy. The Lean development factors this into three definitions mirroring the formula: the integrand (Wigner.wignerIntegrand), the integral (Wigner.wignerIntegral), and the Wigner function itself (Wigner.wigner), defined as the real part of the integral divided by πℏ\pi\hbarπℏ; that the discarded imaginary part vanishes is itself milestone 1. The Fock states of the harmonic oscillator enter through the physicists' Hermite polynomials HmH_mHm​ and the ordinary Laguerre polynomials LmL_mLm​, defined by their standard three-term recurrences, and the normalized mmm-th Hermite function

um(x)=(2mm!)−1/2 π−1/4 Hm(x) e−x2/2.u_m(x) = (2^m m!)^{-1/2}\, \pi^{-1/4}\, H_m(x)\, e^{-x^2/2}.um​(x)=(2mm!)−1/2π−1/4Hm​(x)e−x2/2.

Formalization targets

Goal — Hudson's theorem

∫R∣ψ∣2=1  and  Wψ≥0 on R2 ⟹ ∃ a,b,c∈C, Re⁡a>0, ψ=e−ax2+bx+c a.e.\int_{\mathbb{R}} |\psi|^2 = 1 \ \text{ and }\ W_\psi \ge 0 \text{ on } \mathbb{R}^2 \ \Longrightarrow\ \exists\, a, b, c \in \mathbb{C},\ \operatorname{Re} a > 0,\ \psi = e^{-ax^2+bx+c} \ \text{a.e.}∫R​∣ψ∣2=1  and  Wψ​≥0 on R2 ⟹ ∃a,b,c∈C, Rea>0, ψ=e−ax2+bx+c a.e.

This is exactly the source's statement of Hudson's theorem; nothing is left unfixed. The mission is complete when the goal is proved.

Milestones

The milestone list is the source's property list, ordered as the attack path: (1) reality of the defining integral; (2) the position marginal ∫W dp=∣ψ(x)∣2\int W\, dp = |\psi(x)|^2∫Wdp=∣ψ(x)∣2; (3) the total integral ∬W=∫∣ψ∣2\iint W = \int |\psi|^2∬W=∫∣ψ∣2; (4) Groenewold's closed formula for the Fock states; (5) a concrete negativity witness, the first excited Fock state at the origin; (6) the pointwise bound ∣W∣≤2/h|W| \le 2/h∣W∣≤2/h; (7) the converse of Hudson's theorem, that Gaussian pure states have nonnegative Wigner function.

Significance

The result itself. Hudson's theorem draws the exact boundary between the classical and the quantum in phase space: Gaussian states — coherent and squeezed states — are precisely the pure states that can be described by an honest phase-space probability density. This is used in quantum optics as a nonclassicality criterion, in tomography and state-reconstruction theory, and in the study of the quantum-to-classical transition: negativity of WWW is shielded by the uncertainty principle (negative regions cannot extend beyond a few ℏ\hbarℏ) and disappears in the classical limit, as the source emphasizes.

What formalizing it adds. The Wigner transform and this circle of ideas are absent from current Mathlib, so the mission builds the foundations itself: the integral transform and its basic identities (reality, marginals, normalization, boundedness), the Hermite/Laguerre recurrences and Groenewold's Fock-state formula, and finally Hudson's theorem with its converse. All of these are reusable well beyond the mission — for quantum optics, for the Wigner–Ville time–frequency distribution used in signal analysis, and for the wider phase-space formulation of quantum mechanics (Moyal brackets, star products). These are known results: this is formalization of known mathematics, not new mathematics, and no machine-checked proof of Hudson's theorem exists in Mathlib today.

Difficulty

The naive approach to Hudson's theorem is doomed from the start, and solvers should know it: since the Husimi QQQ function (a Gaussian smoothing of WWW) is positive for every quantum state, no smoothing or positivity-of-convolution argument can extract any information from W≥0W \ge 0W≥0. The known route (Soto–Claverie) is: W≥0W \ge 0W≥0 everywhere forces the Husimi function strictly positive everywhere; the Husimi function is the squared modulus of the Segal–Bargmann transform FFF of ψ\psiψ, so FFF is a zero-free entire function; hence F=egF = e^gF=eg for some entire ggg, and square-integrability of FFF against a Gaussian measure forces ggg to have at most quadratic growth, hence to be a quadratic polynomial; inverting the Segal–Bargmann transform then exhibits ψ\psiψ as a Gaussian. The hard Lean steps are the growth-to-polynomial (Liouville-type) step, the inversion of the transform, and, for the milestone properties, the Fubini and Fourier-inversion machinery. Mathlib contains the raw harmonic analysis (Fourier inversion for Schwartz functions) but none of the assembled phase-space layer.

Formalization scope

  • Integrals are Bochner integrals with respect to Lebesgue measure on R\mathbb{R}R; statements carry the integrability or regularity hypotheses under which the source's displayed integrals exist.
  • ℏ\hbarℏ is an explicit real parameter, and every statement assumes 0<ℏ0 < \hbar0<ℏ (the standing convention of the source). The Fock-state section uses the source's dimensionless units, i.e. ℏ=1\hbar = 1ℏ=1.
  • The Wigner function is defined as the real part of the defining integral divided by πℏ\pi\hbarπℏ; milestone 1 proves the imaginary part vanishes, so this is the same function as the source's.
  • Pure states are encoded by the normalization ∫∣ψ∣2=1\int |\psi|^2 = 1∫∣ψ∣2=1.
  • The conclusion of Hudson's theorem holds only up to modification of ψ\psiψ on a Lebesgue-null set (WWW is insensitive to null-set changes of ψ\psiψ), so the goal states almost-everywhere equality; this is the faithful reading of "the wavefunction must have the form".
  • The Fock states are normalized: the source's displayed um=π−1/4Hme−x2/2u_m = \pi^{-1/4} H_m e^{-x^2/2}um​=π−1/4Hm​e−x2/2 omits the factor (2mm!)−1/2(2^m m!)^{-1/2}(2mm!)−1/2 that its Fock-state formula requires; the definition includes it, since Groenewold's formula is stated for the normalized number states ∣m⟩=(a†)m/m! ∣0⟩|m\rangle = (a^\dagger)^m/\sqrt{m!}\,|0\rangle∣m⟩=(a†)m/m!​∣0⟩.
  • There is no trivializing encoding: Hudson's hypothesis ranges over all normalized wavefunctions, and the conclusion is not weakened beyond the almost-everywhere reading.

Infrastructure contributed and reusable beyond this mission: hermiteP, laguerreL, fockState, wignerIntegrand, wignerIntegral, wigner. Welcome additional contributions: the momentum marginal, the state-overlap formula (Property 6), Galilei covariance (Property 4), and harmonic-oscillator time evolution, as further theorems in the same namespace.

Selected references

  • E. P. Wigner, On the quantum correction for thermodynamic equilibrium, Physical Review 40(5), 749–759, 1932. https://doi.org/10.1103/PhysRev.40.749
  • H. J. Groenewold, On the principles of elementary quantum mechanics, Physica 12(7), 405–460, 1946. https://doi.org/10.1016/S0031-8914(46)80059-4
  • J. E. Moyal, Quantum mechanics as a statistical theory, Mathematical Proceedings of the Cambridge Philosophical Society 45(1), 99–124, 1949. https://doi.org/10.1017/S0305004100000487
  • R. L. Hudson, When is the Wigner quasi-probability density non-negative?, Reports on Mathematical Physics 6(2), 249–252, 1974. https://doi.org/10.1016/0034-4877(74)90007-X
  • F. Soto and P. Claverie, When is the Wigner function of multidimensional systems nonnegative?, Journal of Mathematical Physics 24, 97–100, 1983.
  • Source text: Wikipedia, Wigner quasiprobability distribution (oldid 1376057304). https://en.wikipedia.org/wiki/Wigner_quasiprobability_distribution
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Quantum Information·Captain: Goku

Qubit Entanglement Breaking ChannelsResearch Paper

Motivation

Qubit Entanglement Breaking Channels.

Target

Theorem 2

Let Φ:M2(C)→M2(C)\Phi:M_2(\mathbb C)\to M_2(\mathbb C)Φ:M2​(C)→M2​(C) be complex-linear, completely positive and trace preserving. Let ∣β⟩=(∣00⟩+∣11⟩)/2|\beta\rangle=(|00\rangle+|11\rangle)/\sqrt2∣β⟩=(∣00⟩+∣11⟩)/2​ and ΓΦ=(id⊗Φ)(∣β⟩⟨β∣)\Gamma_\Phi=(\mathrm{id}\otimes\Phi)(|\beta\rangle\langle\beta|)ΓΦ​=(id⊗Φ)(∣β⟩⟨β∣). Then

Φ is entanglement breaking⟺ΓΦ≤12I4.\Phi\text{ is entanglement breaking}\quad\Longleftrightarrow\quad \Gamma_\Phi\le\tfrac12 I_4.Φ is entanglement breaking⟺ΓΦ​≤21​I4​.

The inequality is the positive-semidefinite operator order. This provides an operator test on the normalized Choi state.

Theorem 3

Let t,λ∈R3t,\lambda\in\mathbb R^3t,λ∈R3, and let Φt,λ\Phi_{t,\lambda}Φt,λ​ be the trace-preserving canonical Bloch map v↦t+diag⁡(λ)vv\mapsto t+\operatorname{diag}(\lambda)vv↦t+diag(λ)v. If it is entanglement breaking, then

∑j=13∣λj∣≤1.\sum_{j=1}^3|\lambda_j|\le1.j=1∑3​∣λj​∣≤1.

There is no unitality assumption. This is a necessary condition for the general translated channel.

Theorem 4

Let Φ\PhiΦ be a completely positive trace-preserving qubit map with Φ(I)=I\Phi(I)=IΦ(I)=I. Suppose independent unitary changes of input and output bases put it in canonical form with parameters t,λ∈R3t,\lambda\in\mathbb R^3t,λ∈R3. Then

Φ is entanglement breaking⟺∑j=13∣λj∣≤1.\Phi\text{ is entanglement breaking}\quad\Longleftrightarrow\quad\sum_{j=1}^3|\lambda_j|\le1.Φ is entanglement breaking⟺j=1∑3​∣λj​∣≤1.

This makes the necessary condition sufficient in the unital case.

Amplitude damping counterexample

For 0≤α≤10\le\alpha\le10≤α≤1, let Φα\Phi_\alphaΦα​ have translation (0,0,1−α2)(0,0,1-\alpha^2)(0,0,1−α2) and diagonal Bloch parameters (α,α,α2)(\alpha,\alpha,\alpha^2)(α,α,α2). These maps are completely positive and trace preserving, and

Φα is entanglement breaking  ⟺  α=0.\Phi_\alpha\text{ is entanglement breaking}\iff\alpha=0.Φα​ is entanglement breaking⟺α=0.

Moreover, for every η>0\eta>0η>0 there is α∈(0,1]\alpha\in(0,1]α∈(0,1] with 2α+α2<η2\alpha+\alpha^2<\eta2α+α2<η and Φα\Phi_\alphaΦα​ not entanglement breaking. Thus small diagonal-parameter sum does not suffice for translated channels.

Linear channels and equation 9

For t∈R3t\in\mathbb R^3t∈R3 and a∈Ra\in\mathbb Ra∈R, let Φ=Φt,(0,0,a)\Phi=\Phi_{t,(0,0,a)}Φ=Φt,(0,0,a)​. Then

Φ is CPT  ⟺  t12+t22+(∣t3∣+∣a∣)2≤1.\Phi\text{ is CPT}\iff t_1^2+t_2^2+(|t_3|+|a|)^2\le1.Φ is CPT⟺t12​+t22​+(∣t3​∣+∣a∣)2≤1.

Whenever this holds, Φ\PhiΦ is CQ and equals X↦∑b=01Tr⁡(∣b⟩⟨b∣X)RbX\mapsto\sum_{b=0}^1\operatorname{Tr}(|b\rangle\langle b|X)R_bX↦∑b=01​Tr(∣b⟩⟨b∣X)Rb​, where R0=(I+(t+ae3)⋅σ)/2R_0=(I+(t+ae_3)\cdot\sigma)/2R0​=(I+(t+ae3​)⋅σ)/2 and R1=(I+(t−ae3)⋅σ)/2R_1=(I+(t-ae_3)\cdot\sigma)/2R1​=(I+(t−ae3​)⋅σ)/2. This includes a=0a=0a=0, when the image is a point.

QC channels are unitarily equivalent to CQ channels

Let Φ\PhiΦ be a QC qubit channel: it measures a POVM and prepares one of two orthogonal pure states. There are qubit unitaries U,VU,VU,V and a CQ map Ψ\PsiΨ such that

Φ=Ad⁡V∘Ψ∘Ad⁡U,Ad⁡U(X)=UXU†.\Phi=\operatorname{Ad}_V\circ\Psi\circ\operatorname{Ad}_U,\qquad \operatorname{Ad}_U(X)=UXU^\dagger.Φ=AdV​∘Ψ∘AdU​,AdU​(X)=UXU†.

A CQ map measures rank-one orthogonal input projectors and prepares density matrices. The assertion relates these two channel subclasses without identifying their definitions.

Extreme POVM need not give an extreme channel

Set w1=(1,0,0)w^1=(1,0,0)w1=(1,0,0), w2=(−1/2,0,3/2)w^2=(-1/2,0,\sqrt3/2)w2=(−1/2,0,3​/2), w3=(−1/2,0,−3/2)w^3=(-1/2,0,-\sqrt3/2)w3=(−1/2,0,−3​/2), and Ek=(I+wk⋅σ)/3E_k=(I+w^k\cdot\sigma)/3Ek​=(I+wk⋅σ)/3. Set Rk=(I+σk)/2R_k=(I+\sigma_k)/2Rk​=(I+σk​)/2, with σ1=X,σ2=Y,σ3=Z\sigma_1=X,\sigma_2=Y,\sigma_3=Zσ1​=X,σ2​=Y,σ3​=Z, and define

Φ(X)=∑k=13Tr⁡(EkX)Rk.\Phi(X)=\sum_{k=1}^3\operatorname{Tr}(E_kX)R_k.Φ(X)=k=1∑3​Tr(Ek​X)Rk​.

The effects form an extreme three-outcome POVM, each RkR_kRk​ is a density matrix, and Φ\PhiΦ is EBT, neither CQ nor a point channel, and not extreme in the EBT set. Thus extreme measurement data need not produce an extreme channel.

Proposition 7

Let Φ=Φt,λ\Phi=\Phi_{t,\lambda}Φ=Φt,λ​ be a CPT qubit map in the fixed canonical basis, and let T(X)=XTT(X)=X^{\mathsf T}T(X)=XT. Then T∘Φ∘TT\circ\Phi\circ TT∘Φ∘T is completely positive, and changing any individual translation coordinate tjt_jtj​ to −tj-t_j−tj​ preserves complete positivity. In addition,

CP⁡(Φ∘T)  ⟺  [∀j, CP⁡(Φt,λ[j↦−λj])]  ⟺  CP⁡(T∘Φ).\operatorname{CP}(\Phi\circ T)\iff\bigl[\forall j,\ \operatorname{CP}(\Phi_{t,\lambda[j\mapsto-\lambda_j]})\bigr]\iff\operatorname{CP}(T\circ\Phi).CP(Φ∘T)⟺[∀j, CP(Φt,λ[j↦−λj​]​)]⟺CP(T∘Φ).

Here CP denotes complete positivity. These are all three numbered assertions, together with the any-coordinate translation invariance explained immediately before the proposition.

Planar channels are entanglement breaking

Let Φt,λ\Phi_{t,\lambda}Φt,λ​ be a CPT qubit map in canonical form. Then

(∃j∈{1,2,3}:λj=0) ⟹ Φt,λ is entanglement breaking.\bigl(\exists j\in\{1,2,3\}:\lambda_j=0\bigr)\ \Longrightarrow\ \Phi_{t,\lambda}\text{ is entanglement breaking}.(∃j∈{1,2,3}:λj​=0) ⟹ Φt,λ​ is entanglement breaking.

The planar regime includes degenerate lines and points. This is a sufficient condition only.

Pure point channels are extreme

Let t∈R3t\in\mathbb R^3t∈R3 with ∥t∥2≤1\|t\|_2\le1∥t∥2​≤1, and set R=(I+t⋅σ)/2R=(I+t\cdot\sigma)/2R=(I+t⋅σ)/2. The canonical point map is CPT and CQ, RRR is a density matrix, and on every operator XXX it satisfies

Φt,0(X)=Tr⁡(X)R.\Phi_{t,0}(X)=\operatorname{Tr}(X)R.Φt,0​(X)=Tr(X)R.

If ∥t∥2=1\|t\|_2=1∥t∥2​=1, there is a unit vector ψ\psiψ with R=∣ψ⟩⟨ψ∣R=|\psi\rangle\langle\psi|R=∣ψ⟩⟨ψ∣, and the map is extreme in both the CPT and EBT sets. This identifies the pure-output endpoint of the point-channel family.

Truly planar channels do not touch the Bloch sphere

Let Φt,λ\Phi_{t,\lambda}Φt,λ​ be a CPT canonical qubit map. If exactly one coordinate of λ\lambdaλ is zero, then

∥t+diag⁡(λ)v∥2<1(∥v∥2≤1).\|t+\operatorname{diag}(\lambda)v\|_2<1\qquad(\|v\|_2\le1).∥t+diag(λ)v∥2​<1(∥v∥2​≤1).

Also, when λ3=0\lambda_3=0λ3​=0, (∣λ1∣+∣λ2∣)2+∥t∥22≤1(|\lambda_1|+|\lambda_2|)^2+\|t\|_2^2\le1(∣λ1​∣+∣λ2​∣)2+∥t∥22​≤1. If both λ1,λ2\lambda_1,\lambda_2λ1​,λ2​ are nonzero and equality holds, then t1=t2=0t_1=t_2=0t1​=t2​=0. Thus a truly planar image stays strictly inside the Bloch sphere.

Theorem 8

In a fixed diagonal basis, let U={λ∈R3:Φ0,λ is CPT and EBT}\mathcal U=\{\lambda\in\mathbb R^3:\Phi_{0,\lambda}\text{ is CPT and EBT}\}U={λ∈R3:Φ0,λ​ is CPT and EBT}, and V={±e1,±e2,±e3}V=\{\pm e_1,\pm e_2,\pm e_3\}V={±e1​,±e2​,±e3​}. Then

U=conv⁡R(V),Ext⁡(U)=V.\mathcal U=\operatorname{conv}_{\mathbb R}(V),\qquad\operatorname{Ext}(\mathcal U)=V.U=convR​(V),Ext(U)=V.

The theorem determines both the entire parameter octahedron and exactly its six extreme points.

Unital EBT channels are the convex hull of unital CQ maps

In the real vector space of complex-linear qubit maps, let Eu\mathcal E_uEu​ be the unital trace-preserving entanglement-breaking maps, and Cu\mathcal C_uCu​ the unital CQ maps. Then

Eu=conv⁡R(Cu).\mathcal E_u=\operatorname{conv}_{\mathbb R}(\mathcal C_u).Eu​=convR​(Cu​).

The channel sets allow arbitrary input and output bases. This is a statement in map space, not only in one diagonal parameter slice.

Theorem 9

Fix any translation t∈R3t\in\mathbb R^3t∈R3, and define Λt={λ:Φt,λ is completely positive}\Lambda_t=\{\lambda:\Phi_{t,\lambda}\text{ is completely positive}\}Λt​={λ:Φt,λ​ is completely positive}. Then

Λt∩(−Λt)={λ:Φt,λ is EBT}.\Lambda_t\cap(-\Lambda_t)=\{\lambda:\Phi_{t,\lambda}\text{ is EBT}\}.Λt​∩(−Λt​)={λ:Φt,λ​ is EBT}.

Inversion negates λ\lambdaλ and leaves ttt fixed. Infeasible translations are permitted; both sides can be empty.

Theorem 10

Let E\mathcal EE be the trace-preserving entanglement-breaking complex-linear qubit maps, and C\mathcal CC the CQ maps. Then

Ext⁡(E)⊆C,E=conv⁡R(C).\operatorname{Ext}(\mathcal E)\subseteq\mathcal C,\qquad\mathcal E=\operatorname{conv}_{\mathbb R}(\mathcal C).Ext(E)⊆C,E=convR​(C).

These are both conclusions of the main theorem. It does not assert that every CQ map is extreme. The proof gap concerning intersecting planes on p.15 is recorded separately, without becoming a theorem hypothesis.

Remark a planar same-basis convex decomposition

Suppose Φt,λ\Phi_{t,\lambda}Φt,λ​ is EBT and λj=0\lambda_j=0λj​=0 for a chosen coordinate jjj. It belongs to the real convex hull of canonical CQ maps Φt′,λ′\Phi_{t',\lambda'}Φt′,λ′​ satisfying λj′=0\lambda'_j=0λj′​=0 and having at most one nonzero coordinate of λ′\lambda'λ′. Moreover, if Ξt3,0\Xi_{t_3,0}Ξt3​,0​ denotes the CPT parameter slice fixing only t3t_3t3​ and λ3=0\lambda_3=0λ3​=0, then

Ξt3,0=conv⁡R{(t,λ)∈Ξt3,0:Φt,λ is CQ}.\Xi_{t_3,0}=\operatorname{conv}_{\mathbb R}\{(t,\lambda)\in\Xi_{t_3,0}:\Phi_{t,\lambda}\text{ is CQ}\}.Ξt3​,0​=convR​{(t,λ)∈Ξt3​,0​:Φt,λ​ is CQ}.

This preserves the canonical coordinate plane, including point-channel endpoints; the other translation coordinates may vary.

Equation 29 axial-translation EBT criterion

For a CPT canonical qubit map with t=(0,0,t3)t=(0,0,t_3)t=(0,0,t3​),

Φt,λ is EBT  ⟺  (∣λ1∣+∣λ2∣)2≤(1−∣λ3∣)2−t32.\Phi_{t,\lambda}\text{ is EBT}\iff (|\lambda_1|+|\lambda_2|)^2\le(1-|\lambda_3|)^2-t_3^2.Φt,λ​ is EBT⟺(∣λ1​∣+∣λ2​∣)2≤(1−∣λ3​∣)2−t32​.

For fixed t3,l3t_3,l_3t3​,l3​ with ∣l3∣≤1|l_3|\le1∣l3​∣≤1 and q=(1−∣l3∣)2−t32≥0q=(1-|l_3|)^2-t_3^2\ge0q=(1−∣l3​∣)2−t32​≥0, its EBT slice is exactly {(v1,v2):∣v1∣+∣v2∣≤q}\{(v_1,v_2):|v_1|+|v_2|\le\sqrt q\}{(v1​,v2​):∣v1​∣+∣v2​∣≤q​}. This includes the filled square and its collapsed endpoints; a negative radicand is not totalized into an extra radius-zero slice.

Remark c parallelogram of same-basis decompositions

Fix t∈R3t\in\mathbb R^3t∈R3 and l3∈Rl_3\in\mathbb Rl3​∈R. Let PPP consist of canonical EBT maps with these fixed parameters and either λ1=0\lambda_1=0λ1​=0 or λ2=0\lambda_2=0λ2​=0. Let Cdiag\mathcal C_{\rm diag}Cdiag​ be all CQ maps canonical in the same basis. Then

conv⁡R(P)⊆conv⁡R(Cdiag).\operatorname{conv}_{\mathbb R}(P)\subseteq\operatorname{conv}_{\mathbb R}(\mathcal C_{\rm diag}).convR​(P)⊆convR​(Cdiag​).

This gives the same-basis decomposition on the illustrated parallelogram. It neither covers the entire slice nor requires CQ summands to retain l3l_3l3​.

Remark d equal singular magnitudes

Let Φ=Φt,λ\Phi=\Phi_{t,\lambda}Φ=Φt,λ​ be EBT, with ∣λj∣=a>0|\lambda_j|=a>0∣λj​∣=a>0 for all three coordinates. There are input/output unitaries U,VU,VU,V and s∈{a,−a}s\in\{a,-a\}s∈{a,−a} such that, writing B(Ψ)=Ad⁡V∘Ψ∘Ad⁡U\mathcal B(\Psi)=\operatorname{Ad}_V\circ\Psi\circ\operatorname{Ad}_UB(Ψ)=AdV​∘Ψ∘AdU​,

B(Φ)=Φ(∥t∥2,0,0),(s,s,s)∈conv⁡R(A).\mathcal B(\Phi)=\Phi_{(\|t\|_2,0,0),(s,s,s)}\in\operatorname{conv}_{\mathbb R}(\mathcal A).B(Φ)=Φ(∥t∥2​,0,0),(s,s,s)​∈convR​(A).

Here A\mathcal AA consists of canonical CQ maps for which tj=λj=0t_j=\lambda_j=0tj​=λj​=0 for some j∈{2,3}j\in\{2,3\}j∈{2,3}. Also Φ∈conv⁡R(B−1(A))\Phi\in\operatorname{conv}_{\mathbb R}(\mathcal B^{-1}(\mathcal A))Φ∈convR​(B−1(A)). Thus summands are canonical in the rotated basis and need not be canonical in the original one.

Formalization scope

Only these reviewed original-paper statements are in scope. Definitions have reviewed bodies; target proofs remain open (sorry). Reviewed deferrals are excluded. No theorem proof or whole-paper formal proof is claimed.

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Linear algebraQuantum InformationTheoretical Computer Science·Captain: mikedeng1

Quantum Singular Value Transformation and Beyond: Exponential Improvements for Quantum Matrix Arithmetics: Singular Value Transformation by Real Polynomials via Alternating Phase ModulationResearch Paper

Motivation

Many quantum algorithms act on a matrix AAA that is not itself unitary: a Hamiltonian to be simulated, a linear system to be inverted, a projector to be amplified. The standard way to hand such a matrix to a quantum computer is to embed it as a block of a unitary UUU, so that A=Π~UΠA=\widetilde\Pi U\PiA=ΠUΠ for two orthogonal projectors Π,Π~\Pi,\widetilde\PiΠ,Π. The question is then which functions f(A)f(A)f(A) can be produced from a few uses of UUU and U†U^\daggerU†.

Gilyén, Su, Low and Wiebe (arXiv:1806.01838, STOC 2019) answered it for polynomials: interleaving UUU and U†U^\daggerU† with phase rotations about Π\PiΠ and Π~\widetilde\PiΠ applies a polynomial to every singular value of AAA. This quantum singular value transformation (QSVT) recovers Hamiltonian simulation, amplitude amplification, fixed-point search, quantum walks and matrix inversion as instances of one identity, and is now the common language of these algorithms (see the survey of Martyn, Rossi, Tan and Chuang, PRX Quantum 2021).

Timeline.

  • 2016: Low, Yoder and Chuang characterize the single-qubit sequences eiφ0σz∏jW(x)eiφjσze^{i\varphi_0\sigma_z}\prod_j W(x)e^{i\varphi_j\sigma_z}eiφ0​σz​∏j​W(x)eiφj​σz​, which they call quantum signal processing (QSP) (PRX 2016).
  • 2016–2017: Low and Chuang lift QSP to Hermitian blocks by qubitization (Quantum 2019; PRL 2017).
  • 2018: this paper replaces eigenvalues by singular values, so that arbitrary (even rectangular) blocks are allowed, and removes the earlier constraint Pℜ(0)=0P_\Re(0)=0Pℜ​(0)=0 for even degree.

Setting

Let HU\mathcal H_UHU​ be a finite-dimensional complex Hilbert space, UUU a unitary on it, and Π,Π~\Pi,\widetilde\PiΠ,Π orthogonal projectors. The projected unitary is A=Π~UΠA=\widetilde\Pi U\PiA=ΠUΠ. Put d=rank⁡Πd=\operatorname{rank}\Pid=rankΠ, d~=rank⁡Π~\tilde d=\operatorname{rank}\widetilde\Pid~=rankΠ, dmin⁡=min⁡(d,d~)d_{\min}=\min(d,\tilde d)dmin​=min(d,d~). A singular value decomposition of AAA consists of orthonormal bases (ψi)i≤d(\psi_i)_{i\le d}(ψi​)i≤d​ of img Π\mathrm{img}\,\PiimgΠ and (ψ~i)i≤d~(\tilde\psi_i)_{i\le\tilde d}(ψ~​i​)i≤d~​ of img Π~\mathrm{img}\,\widetilde\PiimgΠ and numbers ς1≥⋯≥ςdmin⁡≥0\varsigma_1\ge\dots\ge\varsigma_{d_{\min}}\ge0ς1​≥⋯≥ςdmin​​≥0 with

A=∑i=1dmin⁡ςi ∣ψ~i⟩⟨ψi∣.A=\sum_{i=1}^{d_{\min}}\varsigma_i\,|\tilde\psi_i\rangle\langle\psi_i| .A=i=1∑dmin​​ςi​∣ψ~​i​⟩⟨ψi​∣.

For f:R→Cf:\mathbb R\to\mathbb Cf:R→C, the singular value transformation is f(SV)(A)=∑i≤dmin⁡f(ςi)∣ψ~i⟩⟨ψi∣f^{(SV)}(A)=\sum_{i\le d_{\min}}f(\varsigma_i)|\tilde\psi_i\rangle\langle\psi_i|f(SV)(A)=∑i≤dmin​​f(ςi​)∣ψ~​i​⟩⟨ψi​∣ when fff is odd and f(SV)(A)=∑i≤df(ςi)∣ψi⟩⟨ψi∣f^{(SV)}(A)=\sum_{i\le d}f(\varsigma_i)|\psi_i\rangle\langle\psi_i|f(SV)(A)=∑i≤d​f(ςi​)∣ψi​⟩⟨ψi​∣ when fff is even, with ςi:=0\varsigma_i:=0ςi​:=0 for i>dmin⁡i>d_{\min}i>dmin​.

The phase operator of a projector is eiφ(2Π−I)=eiφΠ+e−iφ(I−Π)e^{i\varphi(2\Pi-I)}=e^{i\varphi}\Pi+e^{-i\varphi}(I-\Pi)eiφ(2Π−I)=eiφΠ+e−iφ(I−Π). For Φ=(φ1,…,φn)∈Rn\Phi=(\varphi_1,\dots,\varphi_n)\in\mathbb R^nΦ=(φ1​,…,φn​)∈Rn, the alternating phase modulation sequence UΦU_\PhiUΦ​ is the product, from j=1j=1j=1 on the left to j=nj=nj=n on the right, of eiφj(2Π~−I)Ue^{i\varphi_j(2\widetilde\Pi-I)}Ueiφj​(2Π−I)U when n−jn-jn−j is even and of eiφj(2Π−I)U†e^{i\varphi_j(2\Pi-I)}U^\daggereiφj​(2Π−I)U† when n−jn-jn−j is odd. On the single-qubit side, R(x)=(x1−x21−x2−x)R(x)=\begin{pmatrix}x&\sqrt{1-x^2}\\ \sqrt{1-x^2}&-x\end{pmatrix}R(x)=(x1−x2​​1−x2​−x​) for x∈[−1,1]x\in[-1,1]x∈[−1,1], and Φ\PhiΦ is said to realize P∈C[x]P\in\mathbb C[x]P∈C[x] if P(x)P(x)P(x) is the top-left entry of ∏j=1neiφjσzR(x)\prod_{j=1}^n e^{i\varphi_j\sigma_z}R(x)∏j=1n​eiφj​σz​R(x) for every x∈[−1,1]x\in[-1,1]x∈[−1,1].

In Lean these are ProjUnitarySVD U Proj Projt (the decomposition data), svtOdd/svtEven, phaseRefl, altPhaseSeq, reflR and qspRefl, in the namespace QSVT19.Main.

Formalization targets

Goal: Corollary 18 (singular value transformation by real polynomials)

Let n≥1n\ge1n≥1 and let Pℜ∈R[x]P_\Re\in\mathbb R[x]Pℜ​∈R[x] have degree nnn, parity n mod 2n \bmod 2nmod2, and ∣Pℜ(x)∣≤1|P_\Re(x)|\le1∣Pℜ​(x)∣≤1 on [−1,1][-1,1][−1,1]. Then there is Φ∈Rn\Phi\in\mathbb R^nΦ∈Rn such that for every singular value decomposition of Π~UΠ\widetilde\Pi U\PiΠUΠ

Pℜ(SV)(Π~UΠ)=(⟨+∣⊗Π′)(∣0⟩⟨0∣⊗UΦ+∣1⟩⟨1∣⊗U−Φ)(∣+⟩⊗Π),P_\Re^{(SV)}(\widetilde\Pi U\Pi)=\bigl(\langle+|\otimes\Pi'\bigr)\bigl(|0\rangle\langle0|\otimes U_\Phi+|1\rangle\langle1|\otimes U_{-\Phi}\bigr)\bigl(|+\rangle\otimes\Pi\bigr),Pℜ(SV)​(ΠUΠ)=(⟨+∣⊗Π′)(∣0⟩⟨0∣⊗UΦ​+∣1⟩⟨1∣⊗U−Φ​)(∣+⟩⊗Π),

with Π′=Π~\Pi'=\widetilde\PiΠ′=Π for odd nnn and Π′=Π\Pi'=\PiΠ′=Π for even nnn. The only constraints on PℜP_\RePℜ​ are those that are necessary; no degree-dependent constant appears.

Milestones

  1. Lemma 6, Theorem 5, Theorem 4 (first claim): sum-of-squares factorization and the characterization of which polynomials, and which real parts, arise from QSP.
  2. Corollary 8: every PPP meeting four explicit conditions is realized by some Φ∈Rd\Phi\in\mathbb R^dΦ∈Rd in the reflection form; Corollary 10: every PℜP_\RePℜ​ as in the goal is ℜ[P]\Re[P]ℜ[P] for such a PPP.
  3. Definition 11 (existence of the decomposition), Table 2 (orthonormality of the spanning vectors of Definition 12), Lemma 14 (the block decomposition of UUU into one- and two-dimensional pieces).
  4. Theorem 17: if Φ\PhiΦ realizes PPP, then P(SV)(Π~UΠ)=Π~UΦΠP^{(SV)}(\widetilde\Pi U\Pi)=\widetilde\Pi U_\Phi\PiP(SV)(ΠUΠ)=ΠUΦ​Π for odd nnn and ΠUΦΠ\Pi U_\Phi\PiΠUΦ​Π for even nnn.
  5. Lemma 9 (optional): explicit phases realizing the Chebyshev polynomial TdT_dTd​.

Significance

The result. Corollary 18 says that every real polynomial of degree nnn, of definite parity and bounded by 111 on [−1,1][-1,1][−1,1], can be applied to the singular values of Π~UΠ\widetilde\Pi U\PiΠUΠ with nnn uses of UUU and U†U^\daggerU† and one ancilla qubit. Every application in §3.4–§5 of the paper (fixed-point amplitude amplification, singular vector transformation, the pseudoinverse, Hamiltonian simulation, Gibbs sampling) is this corollary applied to a suitable approximating polynomial, so a formal proof makes all of them conditional only on polynomial approximation bounds.

Formalizing it. The result is proved in the paper; none of the statements of this mission has a machine-checked proof on the platform. A formal development would provide reusable infrastructure absent from Mathlib: singular value decompositions over sub-spaces, the two-dimensional invariant-subspace decomposition of a projected unitary (a quantitative form of Jordan's lemma), and the polynomial characterization of single-qubit QSP. Theorem 3 of the paper, the W(x)W(x)W(x) form of the QSP characterization, is already posed on the platform as QAlgorithms.Childs.qsp_characterization; Corollary 8 depends on it.

Difficulty

The obvious argument for Theorem 17 is "restrict UΦU_\PhiUΦ​ to each two-dimensional subspace and read off the QSP product". Making that rigorous means proving that the subspaces of Definition 12 are pairwise orthogonal, invariant under every factor of UΦU_\PhiUΦ​, and that UUU acts on each pair of bases by exactly the reflection R(ςi)R(\varsigma_i)R(ςi​), including the degenerate blocks with ςi∈{0,1}\varsigma_i\in\{0,1\}ςi​∈{0,1}, the one-dimensional blocks HiR,HiL\mathcal H_i^R,\mathcal H_i^LHiR​,HiL​ where UΦU_\PhiUΦ​ contributes a phase e±iφ0e^{\pm i\varphi_0}e±iφ0​, and the complement H⊥\mathcal H_\perpH⊥​. The polynomial side is harder still: Lemma 6 factors a nonnegative even polynomial through its multiset of complex roots, grouping roots in (0,1)(0,1)(0,1), in [1,∞)[1,\infty)[1,∞), on the imaginary axis and in the open quadrant, while tracking degree and parity. Neither step reduces to a library lemma, and an argument that works only for Hermitian AAA, or only when Π=Π~\Pi=\widetilde\PiΠ=Π, proves a different theorem.

Formalization scope

  • HU\mathcal H_UHU​ is ι → ℂ for a Fintype ι with the inner product star v ⬝ᵥ w; operators are Matrix ι ι ℂ; "unitary" is U ∈ Matrix.unitaryGroup ι ℂ; "orthogonal projector" is IsStarProjection. The projectors are named Proj, Projt because Π is Lean notation. Indices are 0-based.
  • A singular value decomposition is the structure ProjUnitarySVD U Proj Projt of data: orthonormal families with Π=∑i∣ψi⟩⟨ψi∣\Pi=\sum_i|\psi_i\rangle\langle\psi_i|Π=∑i​∣ψi​⟩⟨ψi​∣, Π~=∑i∣ψ~i⟩⟨ψ~i∣\widetilde\Pi=\sum_i|\tilde\psi_i\rangle\langle\tilde\psi_i|Π=∑i​∣ψ~​i​⟩⟨ψ~​i​∣, nonnegative non-increasing ς\varsigmaς, and (17). The goal is posed for every such decomposition, with Φ\PhiΦ chosen first; the Definition 11 milestone shows that one exists. ςi≤1\varsigma_i\le1ςi​≤1 is a consequence and is not assumed.
  • f(SV)f^{(SV)}f(SV) is the sum over the decomposition (Definition 16), never the right-hand side of (32) or (33); a formalization that defines it by an operator expression trivializes the goal.
  • eiφ(2Π−I)e^{i\varphi(2\Pi-I)}eiφ(2Π−I) is written eiφΠ+e−iφ(I−Π)e^{i\varphi}\Pi+e^{-i\varphi}(I-\Pi)eiφΠ+e−iφ(I−Π), equal to the matrix exponential for an idempotent Π\PiΠ. The ancilla of (33) is the first tensor factor.
  • eiφσze^{i\varphi\sigma_z}eiφσz​ and the parity predicate are the published definitions of QAlgorithms_Defs_Hamiltonian. "deg ≤ k − 1" is degree < k and "parity k−1k-1k−1" is parity k+1k+1k+1, avoiding natural-number subtraction.
  • Printed slips that affect statements:
    • Corollary 10 omits ℜ[P]=Pℜ\Re[P]=P_\Reℜ[P]=Pℜ​; it is restored, as used in the proof of Corollary 18.
    • Corollary 8 and Corollary 18 are false for degree 000 (a constant eiαe^{i\alpha}eiα, respectively a constant c≠1c\neq1c=1); both are posed with d≥1d\ge1d≥1, n≥1n\ge1n≥1.
    • Theorem 17's "PPP and Φ\PhiΦ as in Corollary 8" is read as (14), the only property its proof uses.
    • Lemma 14's (25)–(28) index the HL\mathcal H^LHL blocks by [d]∖[r][d]\setminus[r][d]∖[r]; this is read as [d~]∖[r][\tilde d]\setminus[r][d~]∖[r], as in (24).
  • Contributions welcome: proofs of any milestone, general lemmas on SVDs of compressions Π~UΠ\widetilde\Pi U\PiΠUΠ, and a proof of the platform's open QSP characterization.

Selected references

  • A. Gilyén, Y. Su, G. H. Low, N. Wiebe, Quantum singular value transformation and beyond: exponential improvements for quantum matrix arithmetics, arXiv:1806.01838v1, 2018; STOC 2019. https://arxiv.org/abs/1806.01838
  • G. H. Low, T. J. Yoder, I. L. Chuang, Methodology of resonant equiangular composite quantum gates, Physical Review X 6, 041067, 2016. https://doi.org/10.1103/PhysRevX.6.041067
  • G. H. Low, I. L. Chuang, Optimal Hamiltonian simulation by quantum signal processing, Physical Review Letters 118, 010501, 2017. https://doi.org/10.1103/PhysRevLett.118.010501
  • G. H. Low, I. L. Chuang, Hamiltonian simulation by qubitization, Quantum 3, 163, 2019. https://doi.org/10.22331/q-2019-07-12-163
  • J. M. Martyn, Z. M. Rossi, A. K. Tan, I. L. Chuang, Grand unification of quantum algorithms, PRX Quantum 2, 040203, 2021. https://doi.org/10.1103/PRXQuantum.2.040203
13 thms2 active usersReviewed
Algorithmic Game TheoryEconomicsMechanism Design+1·Captain: mikedeng1

Persuading Customers to Buy Early: The Value of Personalized Information Provisioning: The Personalized Buy/Wait/No Mechanism Is Optimal and Strictly Beats Public SignalingResearch Paper

Motivation

A seller who sells over two periods, at a full price now and a discount later, loses revenue to strategic customers who wait for the discount. Waiting is costly to the customer only through availability risk: if inventory is scarce, the product may be gone by the second period. Inventory is usually known to the firm and not to its customers, so the firm can try to shape how scarce the product looks. Drakopoulos, Jain and Randhawa (SSRN 3191629, version of April 17, 2020) study this as a problem of Bayesian persuasion (Kamenica and Gentzkow, AER 2011) with many receivers: the firm commits to prices and to a signaling policy before it learns its inventory, and then sends each customer a recommendation.

Their two main results separate public from private information. Theorem 1 (p. 15): with a public signal, seen by all customers, the firm earns no more than with prices alone. Theorem 2 (p. 17): with personalized signals, which may depend on each customer's valuation and be randomized independently across customers, a simple Buy/Wait/No mechanism is optimal and strictly beats every public mechanism when the low inventory level is small. Personalized recommendations are the kind of information online retailers and travel platforms send (low-stock alerts, buy-now prompts).

Setting

There is a unit mass of customers with valuations distributed on V=[0,b]V=[0,b]V=[0,b] with density fff and complementary distribution Fˉ(v)=∫vbf\bar F(v)=\int_v^b fFˉ(v)=∫vb​f; the hazard rate f/Fˉf/\bar Ff/Fˉ is non-decreasing. The firm's inventory QQQ is high, qH=1q_H=1qH​=1 (enough for everyone), with probability P(H)∈(0,1)P(H)\in(0,1)P(H)∈(0,1), and low, qL∈(0,1]q_L\in(0,1]qL​∈(0,1], with probability P(L)=1−P(H)P(L)=1-P(H)P(L)=1−P(H). The monopoly price is pm=arg⁡max⁡ppFˉ(p)p^m=\arg\max_p p\bar F(p)pm=argmaxp​pFˉ(p), and Fˉ−1(q)\bar F^{-1}(q)Fˉ−1(q) is the valuation at which a mass qqq of customers lies above.

A straightforward mechanism fixes prices p1,p2≥0p_1,p_2\ge0p1​,p2​≥0 and, after seeing QQQ, draws a latent index kkk from a finite set with a state-dependent law; given (Q,k)(Q,k)(Q,k), each vvv-customer is independently told Buy (in period 1), Wait (buy in period 2) or No. A customer who requests the product in a period with sss units left and demand of mass DDD from the others gets it with probability avail(s,D)\mathrm{avail}(s,D)avail(s,D): 000 if s≤0s\le0s≤0, 111 if D≤sD\le sD≤s, s/Ds/Ds/D otherwise (random rationing). The mechanism is obedient if every customer (for almost every vvv) weakly prefers to follow her recommendation, given the availabilities she can expect conditional on it: (Buy-1)–(No), p. 40. The firm's revenue is the expected value of rationed sales p1min⁡{D1,Q}+p2min⁡{D2,(Q−D1)+}p_1\min\{D_1,Q\}+p_2\min\{D_2,(Q-D_1)^+\}p1​min{D1​,Q}+p2​min{D2​,(Q−D1​)+}. A mechanism is public when the recommendations depend only on (k,v)(k,v)(k,v) and obedience holds for each realized kkk.

The personalized mechanism (PS1)–(PS2), p. 17, sets p1=Fˉ−1(qL)p_1=\bar F^{-1}(q_L)p1​=Fˉ−1(qL​). In state LLL it tells customers with v≥p1v\ge p_1v≥p1​ to buy and the rest No; in state HHH it tells v≥p1v\ge p_1v≥p1​ to buy with probability

σH(v)=min⁡{P(L)P(H)v−p1p1−p2,1}(13)\sigma_H(v)=\min\Big\{\frac{P(L)}{P(H)}\frac{v-p_1}{p_1-p_2},1\Big\}\tag{13}σH​(v)=min{P(H)P(L)​p1​−p2​v−p1​​,1}(13)

and to wait otherwise, tells p2≤v<p1p_2\le v<p_1p2​≤v<p1​ to wait, and v<p2v<p_2v<p2​ No. The price p2p_2p2​ solves Fˉ(p2)−p2f(p2)=Fˉ(vˉ)\bar F(p_2)-p_2f(p_2)=\bar F(\bar v)Fˉ(p2​)−p2​f(p2​)=Fˉ(vˉ) (14) with vˉ=sup⁡{v:σH(v)<1}\bar v=\sup\{v:\sigma_H(v)<1\}vˉ=sup{v:σH​(v)<1} (15).

Formalization targets

Goal: Theorem 2

If qL≤Fˉ(pm)q_L\le\bar F(p^m)qL​≤Fˉ(pm), then (14) has a root p2∈(0,p1)p_2\in(0,p_1)p2​∈(0,p1​), and for every such root the mechanism (PS2) is obedient, its revenue RprivateR_{private}Rprivate​ is at least that of every obedient mechanism at any prices, and

Rprivate>Rϕ∗=P(L) pˉ1Fˉ(pˉ1)+P(H) pmFˉ(pm),pˉ1=max⁡{Fˉ−1(qL),pm}.(11)R_{private}>R^*_\phi=P(L)\,\bar p_1\bar F(\bar p_1)+P(H)\,p^m\bar F(p^m),\qquad \bar p_1=\max\{\bar F^{-1}(q_L),p^m\}.\tag{11}Rprivate​>Rϕ∗​=P(L)pˉ​1​Fˉ(pˉ​1​)+P(H)pmFˉ(pm),pˉ​1​=max{Fˉ−1(qL​),pm}.(11)

Milestones

  1. Lemma 2 (p. 35): the L-state profit ϕ(t,p)\phi(t,p)ϕ(t,p) of a public threshold ttt satisfies ϕ(t,p)≤max⁡{(Fˉ−1(qL)−p)qL,0}\phi(t,p)\le\max\{(\bar F^{-1}(q_L)-p)q_L,0\}ϕ(t,p)≤max{(Fˉ−1(qL​)−p)qL​,0}, and for qL<Fˉ(p)q_L<\bar F(p)qL​<Fˉ(p) its unique maximizer is Fˉ−1(qL)\bar F^{-1}(q_L)Fˉ−1(qL​).
  2. Theorem 1 (c) (p. 15): Rϕ∗R^*_\phiRϕ∗​ is the largest revenue of a public mechanism.
  3. Lemma 3 (p. 44): at fixed prices p1>p2p_1>p_2p1​>p2​, the (t∗,p1,p2)(t^*,p_1,p_2)(t∗,p1​,p2​)-mechanism built from an optimal threshold t∗t^*t∗ of the one-parameter program (A.16) is obedient, earns its value Dˉ(p1,p2)\bar D(p_1,p_2)Dˉ(p1​,p2​), and is optimal among obedient mechanisms with those prices.
  4. Lemma 4 (p. 44, corrected reading): if Fˉ(p2)>qL\bar F(p_2)>q_LFˉ(p2​)>qL​, then Dˉ(p1,p2)≤Dˉ(Fˉ−1(qL),p2)\bar D(p_1,p_2)\le\bar D(\bar F^{-1}(q_L),p_2)Dˉ(p1​,p2​)≤Dˉ(Fˉ−1(qL​),p2​).
  5. (16) (p. 17): (PS2) is obedient and earns
Rprivate=P(H)p2Fˉ(p2)+P(H)(p1−p2)Fˉ(vˉ)+P(L)∫p1vˉ(v−p1) dF(v)+P(L)p1qL.R_{private}=P(H)p_2\bar F(p_2)+P(H)(p_1-p_2)\bar F(\bar v)+P(L)\int_{p_1}^{\bar v}(v-p_1)\,dF(v)+P(L)p_1q_L.Rprivate​=P(H)p2​Fˉ(p2​)+P(H)(p1​−p2​)Fˉ(vˉ)+P(L)∫p1​vˉ​(v−p1​)dF(v)+P(L)p1​qL​.

Significance

The result says that the value of information in this market lies entirely in its personalization: public information is worthless (Theorem 1), and private recommendations strictly raise revenue whenever low inventory is scarce relative to the monopoly market. The optimal mechanism is explicit and has a simple form, with the low-type firm selling out exactly in period 1 and the high-type firm mimicking it as far as incentive compatibility allows; in the paper's uniform example (qL=P(H)=1/2q_L=P(H)=1/2qL​=P(H)=1/2) revenue rises from 1/41/41/4 to 13/4813/4813/48. The proof technique, a relaxation to a linear program over signal profiles followed by a dual reduction to a single threshold, is a template for many-receiver persuasion problems with congestion.

The theorems are proved in the paper; none of them has a machine-checked proof. The mission produces a formal model of strategic customers under rationing and personalized signaling, and the formal versions of the five steps. Two printed steps need correction to be true and are stated in corrected form (Lemma 4's tie case, the location of the root of (14)); formal proofs settle that the corrections suffice.

Difficulty

The obvious argument is a pointwise one: for each valuation, the Buy incentive constraint caps the high-state Buy probability given the low-state one, so set every cap tight. It fails because the availabilities in the constraints depend on the aggregate masses that the recommendations themselves create, so the constraints for different valuations are coupled; the paper resorts to an infinite-dimensional linear program and asserts strong duality without proof (p. 41). Lemma 4 is the algebraically heavy step (pp. 46–50): an envelope argument over the threshold combined with the hazard-rate monotonicity. Theorem 2 then needs a one-dimensional optimization in p2p_2p2​, the existence of a root of (14) (a fixed-point equation, since vˉ\bar vvˉ depends on p2p_2p2​), and the case p2>p1p_2>p_1p2​>p1​, which the paper never treats.

Formalization scope

The paper's game (Definitions 1–2: a continuum of customers, Bayesian Nash equilibrium, sender-preferred selection) is re-expressed as the class its proofs reduce to by the revelation principle (p. 39, footnote 5): obedient straightforward mechanisms with aggregate masses. Revenue optimality over this class is what Theorem 2 asserts after that reduction. The latent index is finite (Fin n, for every n); it carries the correlation between customers' signals that public signals need. Obedience is required for almost every valuation, as in Definition 1.

Committed conventions: V=[0,b]V=[0,b]V=[0,b], b>0b>0b>0, fff continuous on [0,b][0,b][0,b] and positive on [0,b)[0,b)[0,b); 0<P(H)<10<P(H)<10<P(H)<1, 0<qL≤10<q_L\le10<qL​≤1; qH=1q_H=1qH​=1 and customer mass 111. Availability is avail above; at zero demand it is 111 with stock left and 000 without. (14) is written Fˉ(p2)−p2f(p2)=Fˉ(vˉ)\bar F(p_2)-p_2f(p_2)=\bar F(\bar v)Fˉ(p2​)−p2​f(p2​)=Fˉ(vˉ). In (PS2)(a) "v>p1v>p_1v>p1​" is taken as v≥p1v\ge p_1v≥p1​ (a null set). (B) is read with min⁡{⋅,1}\min\{\cdot,1\}min{⋅,1}. The program (A.16) keeps the no-Buy mechanism (Fˉ(t)=0\bar F(t)=0Fˉ(t)=0), which the printed version drops. "The optimal mechanism" is stated as "an optimal mechanism" (ties exist). Lemmas 3–4 take p2<p1p_2<p_1p2​<p1​, implicit in the paper's divisions; the goal ranges over all prices p1,p2≥0p_1,p_2\ge0p1​,p2​≥0, including p2>p1p_2>p_1p2​>p1​ (p. 8). Milestone (16) is stated at the prices of (PS1): p1=Fˉ−1(qL)p_1=\bar F^{-1}(q_L)p1​=Fˉ−1(qL​) and p2∈[0,p1)p_2\in[0,p_1)p2​∈[0,p1​) a root of (14).

Trivializing formalizations are ruled out: revenue counts rationed sales, not p1D1+p2D2p_1D_1+p_2D_2p1​D1​+p2​D2​; obedience is the printed conditional constraint multiplied by the probability of the recommendation, never divided by a possibly zero probability; availability never uses Lean's x/0=0x/0=0x/0=0; the goal carries the existence of a root of (14), so "for every root" is not vacuous; the mechanism class contains public and correlated mechanisms; and RprivateR_{private}Rprivate​ is the revenue of the mechanism (PS2), tied to the formula (16) by a milestone.

A complete development needs: the density measure on [0,b][0,b][0,b] and its tail function Fˉ\bar FFˉ, monotonicity and continuity of Fˉ\bar FFˉ and its inverse, the quasi-concavity of pFˉ(p)p\bar F(p)pFˉ(p) under a non-decreasing hazard rate, and bounds for the rationing function. The hazard-rate and Fˉ−1\bar F^{-1}Fˉ−1 lemmas are reusable for other pricing models. Contributions of helper lemmas, of a primal proof of Lemma 3 avoiding the duality argument, and of the case p2>p1p_2>p_1p2​>p1​ are welcome.

Selected references

  • K. Drakopoulos, S. Jain, R. S. Randhawa, Persuading Customers to Buy Early: The Value of Personalized Information Provisioning, SSRN working paper 3191629, version of April 17, 2020. https://ssrn.com/abstract=3191629
  • E. Kamenica, M. Gentzkow, Bayesian Persuasion, American Economic Review 101(6):2590–2615, 2011. https://doi.org/10.1257/aer.101.6.2590
  • D. Bergemann, S. Morris, Information Design: A Unified Perspective, Journal of Economic Literature 57(1):44–95, 2019. https://doi.org/10.1257/jel.20181489
12 thms2 active usersReviewed
Functional Analysis·Captain: savarin

Sharp diagonal Hlawka constants: lower the cutoff to 16Open Problem

The Hlawka inequality for Schatten ppp-norms is a cousin of the triangle inequality: it relates the norms of three matrices to the norms of their pairwise sums and their total sum. The question is how large a comparison constant is needed to make this inequality hold.

This mission asks whether the best possible constant for complex diagonal matrices, already proved in Lean for every real p≥32p\ge32p≥32, also holds for every real p≥16p\ge16p≥16. This is an open problem: no proof is known. The constant is the one from the foundation mission: the largest comparison constant required by the cyclic family of three 3×33\times33×3 diagonal matrices. Because the cutoff-32 mission already covers every p≥32p\ge32p≥32, the new work is the range from 16 to 32.

The cutoff came down from 256 to 32 across eleven missions. The first phase (256 to 62) used a confinement estimate, exhausted at p=61p=61p=61. The second phase (62 to 32) used a new technique that broke through the confinement barrier. Whether it extends to 16 is not known; 16 asks for sixteen more units below the current best.

This is an entry in the sharp diagonal Hlawka campaign, which asks for the smallest cutoff at which the same formula holds. The campaign conjectures the formula for all p≥2p\ge2p≥2. Any proof for a cutoff of 16 or lower also settles this mission.

The broader question of optimal constants for Schatten norms appears in Audenaert and Kittaneh's Problem 7. Extending the sharp diagonal constant to general matrices is a separate challenge.

References

  • K. M. R. Audenaert and F. Kittaneh, Problems and Conjectures in Matrix and Operator Inequalities, arXiv preprint, 2012, §8.2, Problem 7. arXiv:1201.5232
  • Ezzeri Esa, Hlawka–Schatten inequalities: sharp diagonal construction, Lean source repository, 2026, revision 79aa498bfcf7b22bd91d771fb32ec278e2d4704b. Source library

Established results on Prove2Me

  • The accepted sharp diagonal bound for every real p ≥ 62.
  • The accepted real coordinate bound for every real p ≥ 62.
  • The accepted diagonal Schatten norm identity.
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EconomicsOperations ResearchOptimization·Captain: mikedeng1

Addictive Platforms 1: Monopoly versus Duopoly — Competition Raises Addictiveness and Hurts the Consumer When Attention Is Scarce, and Lowers Addictiveness When It Is AbundantResearch Paper

Motivation

Digital services are paid for with attention: an ad-financed platform earns more the longer its users stay. Policy reports on digital markets (Crémer, de Montjoye and Schweitzer, 2019; the U.K. Digital Competition Expert Panel, 2019; Scott Morton et al., 2019) worry that such firms degrade their services with features that capture attention at the user's expense, and they usually recommend more competition. Ichihashi and Kim, Addictive Platforms (Bank of Canada Staff Working Paper 2022-16; Management Science, 2023), ask whether competition actually helps. Their answer depends on how scarce attention is. When attention is scarce, platforms compete by making their services more addictive rather than better, and a monopoly serves the consumer better than a duopoly. This mission formalizes that comparison, the paper's headline result, together with the two equilibrium characterizations it rests on.

Setting

There are KKK platforms and a single consumer. Each platform kkk chooses an addictiveness dk≥0d_k \ge 0dk​≥0. The consumer observes d=(d1,…,dK)d = (d_1, \dots, d_K)d=(d1​,…,dK​), joins a set JJJ of platforms and allocates attention ak≥0a_k \ge 0ak​≥0 to each k∈Jk \in Jk∈J. She receives 000 if J=∅J = \emptysetJ=∅, and otherwise

∑k∈Ju(ak,dk)−C(∑k∈Jak),\sum_{k\in J} u(a_k, d_k) - C\Big(\sum_{k\in J} a_k\Big),k∈J∑​u(ak​,dk​)−C(k∈J∑​ak​),

subject to the attention cap ∑k∈Jak≤A‾\sum_{k\in J} a_k \le \overline{A}∑k∈J​ak​≤A, where A‾∈R+∪{∞}\overline{A} \in \mathbb{R}_+ \cup \{\infty\}A∈R+​∪{∞}. Platform kkk earns the attention aka_kak​ if the consumer joins it and 000 otherwise.

The service utility u(a,d)u(a, d)u(a,d) is twice differentiable, strictly increasing and concave in attention aaa, and strictly decreasing in ddd. The marginal utility u1(a,d)=∂u/∂au_1(a, d) = \partial u/\partial au1​(a,d)=∂u/∂a is strictly increasing in ddd, so a more addictive service is worse to join but harder to stop using. There is some ddd at which no amount of attention makes the service worth joining, and u(0,0)≥0u(0,0) \ge 0u(0,0)≥0. The attention cost C:R+→R+C : \mathbb{R}_+ \to \mathbb{R}_+C:R+​→R+​ is strictly increasing, convex and twice differentiable, with lim⁡a→0[u1(a,0)−C′(a)]>0\lim_{a\to0}[u_1(a,0) - C'(a)] > 0lima→0​[u1​(a,0)−C′(a)]>0. These are Assumptions 1 and 2 of the paper.

Platforms choose addictiveness simultaneously, and then the consumer chooses JJJ and aaa. The solution concept is pure-strategy subgame perfect equilibrium: the consumer chooses optimally at every profile ddd, and no platform gains by changing its own dkd_kdk​. A monopolist (K=1K = 1K=1) breaks ties in the consumer's favour. Consumer surplus is the consumer's payoff in the equilibrium outcome.

The monopoly benchmark uses three quantities. The first is A(d)=arg⁡max⁡A≥0u(A,d)−C(A)A(d) = \arg\max_{A\ge0} u(A,d) - C(A)A(d)=argmaxA≥0​u(A,d)−C(A), the consumer's attention on one platform when there is no cap. The second is dA(A‾)=min⁡{d∈[0,∞]:A(d)≥A‾}d^A(\overline{A}) = \min\{d \in [0,\infty] : A(d) \ge \overline{A}\}dA(A)=min{d∈[0,∞]:A(d)≥A}, the lowest addictiveness at which she exhausts her attention. The third is dP(A‾)d^P(\overline{A})dP(A), the addictiveness at which her best capped payoff from one platform falls to zero. Under competition, AK(d)=arg⁡max⁡A∈[0,A‾]K u(A/K,d)−C(A)A_K(d) = \arg\max_{A\in[0,\overline{A}]} K\,u(A/K, d) - C(A)AK​(d)=argmaxA∈[0,A]​Ku(A/K,d)−C(A) is the total attention she spends on KKK platforms of common addictiveness ddd.

Formalization targets

Goal: Proposition 3 (monopoly versus duopoly)

Let A‾M\overline{A}^MAM be the least cap from which on monopoly consumer surplus is zero. For every monopoly equilibrium with addictiveness dMd^MdM and every duopoly equilibrium with (d1,d2)(d_1, d_2)(d1​,d2​):

0<A‾≤A(0)  ⟹  dM<d1, dM<d2, CSduo<CSmono,0 < \overline{A} \le A(0) \;\Longrightarrow\; d^M < d_1,\ d^M < d_2,\ CS^{\mathrm{duo}} < CS^{\mathrm{mono}},0<A≤A(0)⟹dM<d1​, dM<d2​, CSduo<CSmono, A‾≥A‾M  ⟹  d1≤dM, d2≤dM, CSmono≤CSduo.\overline{A} \ge \overline{A}^M \;\Longrightarrow\; d_1 \le d^M,\ d_2 \le d^M,\ CS^{\mathrm{mono}} \le CS^{\mathrm{duo}}.A≥AM⟹d1​≤dM, d2​≤dM, CSmono≤CSduo.

The proposition is silent about intermediate caps, and so is the goal.

Milestones

  1. Proposition 1 (monopoly). The monopolist sets min⁡{dA(A‾),dP(A‾)}\min\{d^A(\overline{A}), d^P(\overline{A})\}min{dA(A),dP(A)}, which is increasing in A‾\overline{A}A. The consumer's payoff rises on [0,A(0)][0, A(0)][0,A(0)], falls on [A(0),A‾M][A(0), \overline{A}^M][A(0),AM] and is zero from some A‾M>A(0)\overline{A}^M > A(0)AM>A(0) on.
  2. Lemmas B.1–B.4. These are comparative statics of the consumer's problem: the tangent intercept u(x)−xu′(x)u(x) - xu'(x)u(x)−xu′(x) is increasing, the value of spreading attention over yyy platforms is concave in yyy, and the incremental gain from one more platform falls with the addictiveness and the number of the platforms already joined.
  3. Step 1 of the proof of Proposition 2. For K≥2K \ge 2K≥2 there is a unique d∗>0d^* > 0d∗>0 solving the indifference condition (3) between joining KKK and K−1K - 1K−1 platforms.
  4. Proposition 2 (competition). For K≥2K \ge 2K≥2, every platform chooses d∗d^*d∗ in the unique equilibrium.

Significance

Proposition 3 separates two effects of competition. Business stealing pushes duopolists to raise addictiveness, because a more addictive service captures a larger share of a fixed attention budget. Competition for participation restrains them, because a consumer can drop a platform and spend her time on its rival. When attention is scarce the first effect dominates and the consumer is strictly worse off under duopoly. When it is abundant the monopolist extracts the whole surplus and duopoly cannot be worse. The result is the basis of the paper's policy discussion: digital curfews and the comparison between the equilibrium and the joint-profit outcome (Propositions 4 and 6). Propositions 1 and 2 are used throughout the paper.

The paper proves these results on paper. No machine-checked proof exists. A formal proof would check several delicate points. One is the role of the monopolist's tie-break, without which every d∈[0,dP]d \in [0, d^P]d∈[0,dP] is a monopoly equilibrium when attention is scarce. Another is that the uniqueness argument for the duopoly needs a consumer who best-responds off the equilibrium path. The appendix also asserts a few claims without argument or slightly too strongly, recorded below. Verifying them is part of the work.

Difficulty

The obvious argument for Proposition 3 compares equilibrium payoffs through the closed forms of Figure 3, and closed forms do not exist in general. Every object is defined by an optimization problem whose maximizer has no formula. The value functions are concave but need not be differentiable, so the envelope-theorem steps of Appendix B cannot be applied as written; they have to be replaced by monotone comparative statics or one-sided derivatives. Proposition 2's uniqueness is the hardest part. It rules out asymmetric equilibria by a deviation argument that controls which platforms the consumer joins after a small change in one platform's addictiveness (Lemma B.4). It also needs the consumer's whole strategy, not only her choice on the path.

Formalization scope

Platforms are Fin K; the paper's platform 1 is the index 0. Addictiveness and attention are real numbers restricted to [0,∞)[0,\infty)[0,∞), and only the values of uuu and CCC there matter. The cap A‾\overline{A}A is an extended nonnegative real (ℝ≥0∞), so A‾=∞\overline{A} = \inftyA=∞ is a genuine case and "A‾≥A‾M\overline{A} \ge \overline{A}^MA≥AM" includes it. Derivatives on [0,∞)[0,\infty)[0,∞) are one-sided at 000.

The definition file states the paper's Assumptions 1–2 as printed and adds disclosed pins:

  • u(⋅,d)u(\cdot, d)u(⋅,d) is strictly concave. The page says "concave", but Lemma B.1 needs strict concavity and Lemma B.2 applies Lemma B.1 to u(⋅,d)u(\cdot,d)u(⋅,d).
  • C(0)=0C(0) = 0C(0)=0. Without it dPd^PdP need not exist.
  • The uncapped consumer problem has an optimal attention profile for every profile and every nonempty JJJ. The page (p. 6) assumes this for A‾=∞\overline{A} = \inftyA=∞, and A(d)A(d)A(d) presupposes it.
  • A‾>0\overline{A} > 0A>0 where the result needs it: Proposition 1's characterization, Step 1, Proposition 2 and the first half of Proposition 3. At A‾=0\overline{A} = 0A=0 every profile is an equilibrium.

"Increasing" and "decreasing" are weak unless the page says "strictly". The one exception is "higher addictiveness" in the first half of Proposition 3, which is stated strictly because the proof gives dM=0<d∗d^M = 0 < d^*dM=0<d∗.

Three statements differ from the printed text. Lemma B.2's "V∗V^*V∗ is strictly concave" is false on the paper's own Figure 3 instance and is stated as concavity. The strict clause of Lemma B.4 fails when CCC is linear and is not posed. The derivative claims of Lemmas B.2–B.4 are stated as decreasing differences of value functions.

Several trivializing formalizations are excluded:

  • An equilibrium requires the consumer to best-respond at every profile, not only at the equilibrium one.
  • The tie-break is part of the monopoly equilibrium.
  • Equilibria exist (Propositions 1 and 2 assert existence), and a sanity file checks the standing hypotheses on u(a,d)=1−e−(a−d)u(a,d) = 1 - e^{-(a-d)}u(a,d)=1−e−(a−d), C(a)=a/2C(a) = a/2C(a)=a/2.
  • No value function is a real supremum; maxima enter through maximizers.

Not posed: Proposition 4 and later results, and the side models of Remarks 2–3. A complete development needs maximizers of concave problems on intervals and simplices, monotone comparative statics (Topkis, Milgrom–Shannon), and envelope arguments for concave value functions. These pieces are reusable well beyond this paper, and contributions of them as separate lemmas are welcome.

Selected references

  • S. Ichihashi and B.-C. Kim, Addictive Platforms, Bank of Canada Staff Working Paper 2022-16, 2022. https://doi.org/10.34989/swp-2022-16. Published in Management Science, 2023. https://doi.org/10.1287/mnsc.2022.4392
  • P. Milgrom and I. Segal, Envelope Theorems for Arbitrary Choice Sets, Econometrica 70(2), 583–601, 2002. https://doi.org/10.1111/1468-0262.00296
  • P. Milgrom and C. Shannon, Monotone Comparative Statics, Econometrica 62(1), 157–180, 1994. https://doi.org/10.2307/2951479
  • J. Crémer, Y.-A. de Montjoye and H. Schweitzer, Competition Policy for the Digital Era, report for the European Commission, 2019. https://doi.org/10.2763/407537
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Operations ResearchProbabilityRandom Matrix Theory+1·Captain: mikedeng1

The Risk of Expected Utility Under Parameter Uncertainty I: Closed-Form Out-of-Sample Utility Variance of the Shrinkage Mean-Variance PortfolioResearch Paper

Why out-of-sample utility risk matters

A portfolio chosen from historical returns can look attractive in the data used to construct it and deliver a different result when evaluated under the population return distribution. The gap is driven by estimation error in both the mean return and covariance matrix. A mean of future utility values describes average performance, but it does not describe how much that utility varies across possible estimation samples. Lassance, Martín-Utrera and Simaan study this variation for a portfolio that blends an estimated mean-variance choice with an estimated global-minimum-variance choice. Their closed-form variance makes the sampling risk of that blend an explicit function of market and sample parameters. The source for this mission is the authors’ SSRN manuscript, version dated August 18, 2023, including its Internet Appendix; appendix pages are cited as IA pages.

The market and the estimated portfolio

There are NNN risky stocks. Their excess-return vector has population mean μ∈RN\mu\in\mathbb R^Nμ∈RN and positive-definite population covariance Σ∈RN×N\Sigma\in\mathbb R^{N\times N}Σ∈RN×N. The investor has risk aversion γ>0\gamma>0γ>0. A portfolio is a vector of weights www whose entries sum to one. Its population mean-variance utility is

U(w)=w⊤μ−γ2w⊤Σw.U(w)=w^\top\mu-\frac{\gamma}{2}w^\top\Sigma w.U(w)=w⊤μ−2γ​w⊤Σw.

Write eee for the vector of ones. The global-minimum-variance portfolio and its variance are wg=Σ−1e(e⊤Σ−1e)−1w_g=\Sigma^{-1}e(e^\top\Sigma^{-1}e)^{-1}wg​=Σ−1e(e⊤Σ−1e)−1 and σg2=(e⊤Σ−1e)−1\sigma_g^2=(e^\top\Sigma^{-1}e)^{-1}σg2​=(e⊤Σ−1e)−1. Its mean is μg=μ⊤Σ−1e σg2\mu_g=\mu^\top\Sigma^{-1}e\,\sigma_g^2μg​=μ⊤Σ−1eσg2​. The population matrix B=Σ−1(I−ewg⊤)B=\Sigma^{-1}(I-ew_g^\top)B=Σ−1(I−ewg⊤​) maps the mean vector to a zero-cost portfolio. The variance of that portfolio is ψ2=μ⊤Σ−1μ−μg2/σg2\psi^2=\mu^\top\Sigma^{-1}\mu-\mu_g^2/\sigma_g^2ψ2=μ⊤Σ−1μ−μg2​/σg2​. These quantities are computed from μ\muμ and Σ\SigmaΣ; they are not independent inputs. These definitions are equations (3)–(7) of the manuscript.

The investor observes TTT independent return vectors r1,…,rTr_1,\ldots,r_Tr1​,…,rT​, each with multivariate Gaussian law N(μ,Σ)\mathcal N(\mu,\Sigma)N(μ,Σ). The sample mean is μ^=T−1∑trt\hat\mu=T^{-1}\sum_t r_tμ^​=T−1∑t​rt​, and the sample covariance is Σ^=T−1∑t(rt−μ^)(rt−μ^)⊤\hat\Sigma=T^{-1}\sum_t(r_t-\hat\mu)(r_t-\hat\mu)^\topΣ^=T−1∑t​(rt​−μ^​)(rt​−μ^​)⊤. Replacing the population parameters in wgw_gwg​ and BBB by these estimates gives the sample GMV portfolio w^g\hat w_gw^g​ and the sample zero-cost portfolio w^z=B^μ^\hat w_z=\hat B\hat\muw^z​=B^μ^​. The estimated mean-variance portfolio is w^⋆=w^g+γ−1w^z\hat w^\star=\hat w_g+\gamma^{-1}\hat w_zw^⋆=w^g​+γ−1w^z​. At shrinkage intensity κ∈[0,1]\kappa\in[0,1]κ∈[0,1], the portfolio under study is w^⋆(κ)=(1−κ)w^g+κw^⋆\hat w^\star(\kappa)=(1-\kappa)\hat w_g+\kappa\hat w^\starw^⋆(κ)=(1−κ)w^g​+κw^⋆. Its out-of-sample utility, U(w^⋆(κ))U(\hat w^\star(\kappa))U(w^⋆(κ)), is evaluated using population μ\muμ and Σ\SigmaΣ. It is random because the weights depend on the sample. These choices are fixed by equations (9)–(12) and Assumption 2 of the manuscript.

Formalization targets

The goal is Proposition 1, equations (13)–(19). Under N≥2N\ge2N≥2 and T>N+7T>N+7T>N+7, it asserts that the utility has a finite second moment and that

V[U(w^⋆(κ))]=V[U(w^g)]+Δ(κ),Δ(κ)=a1κ4+a2κ3+a3κ2+a4κ.\mathbb V[U(\hat w^\star(\kappa))] =\mathbb V[U(\hat w_g)]+\Delta(\kappa),\qquad \Delta(\kappa)=a_1\kappa^4+a_2\kappa^3+a_3\kappa^2+a_4\kappa.V[U(w^⋆(κ))]=V[U(w^g​)]+Δ(κ),Δ(κ)=a1​κ4+a2​κ3+a3​κ2+a4​κ.

The coefficients a1,…,a4a_1,\ldots,a_4a1​,…,a4​ and V[U(w^g)]\mathbb V[U(\hat w_g)]V[U(w^g​)] are the exact rational expressions in T,N,γ,σg2,ψ2T,N,\gamma,\sigma_g^2,\psi^2T,N,γ,σg2​,ψ2 on pp. 14–15 of the manuscript. In particular, the result covers every κ∈[0,1]\kappa\in[0,1]κ∈[0,1], including the sample GMV portfolio at κ=0\kappa=0κ=0 and the sample mean-variance portfolio at κ=1\kappa=1κ=1.

The milestones follow the quantities named in the authors’ proof, Section IA.10. Equation (IA43) gives the covariance matrix of the random weights, and (IA44) gives the variance of their population mean return. The jointly distributed mean-return and return-variance pair in (IA45)–(IA48) supplies the setting for two auxiliary moment identities, (IA53) and (IA57). Equations (IA49), (IA59), and (IA60) give the first and second moments needed for return variance and mean return; (IA68) gives their covariance. All are statements from the Internet Appendix, pp. IA35–IA39.

What the result supplies

The expression tells an investor how the sampling risk of utility changes with the shrinkage intensity, sample size, stock count, risk aversion, and the two population variance parameters. The later comparison of variance-minimizing, mean-maximizing, and robustness-maximizing intensities uses this formula. Without Proposition 1, those comparisons have no explicit OOSU risk function to analyze. The result is already proved in the paper; this mission asks for its Lean proof and for reusable formal statements of the associated Gaussian portfolio and moment identities. No machine-checked proof of this paper’s proposition is included in the draft.

Where the difficulty lies

The sample covariance is random and its inverse appears in the estimated weights. Taking the variance of utility therefore involves inverse-covariance terms and moments beyond those needed for expected utility. The requirement T>N+7T>N+7T>N+7 is tied to existence of the fourth negative moment of a chi-squared variable in (IA57). A direct calculation that replaces random weights by their population counterparts loses the dependence on the estimation sample. A calculation from separate marginal laws also does not determine the covariance between mean return and return variance; the representation in (IA47)–(IA48) describes them jointly.

Formalization scope

The Lean market uses vectors Fin N → ℝ, matrices indexed by Fin N, and returns in EuclideanSpace ℝ (Fin N) to use Mathlib’s multivariate Gaussian law. The sample has Fin T observations on a probability space. Its covariance divisor is exactly TTT, as in (9). The standing assumptions are N≥2N\ge2N≥2, T>N+7T>N+7T>N+7, Σ≻0\Sigma\succ0Σ≻0, γ>0\gamma>0γ>0, and independent, identically distributed Gaussian returns. Every theorem about a variance or covariance explicitly asserts finite second moments; expectation statements explicitly assert integrability. The source’s finite-variance convention is thereby represented without Lean’s default value for a nonintegrable variance.

The left side of the goal is the probability-theory variance of utility under the sampling law. It is not defined by the closed formula. Likewise σg2\sigma_g^2σg2​, μg\mu_gμg​, and ψ2\psi^2ψ2 are computed from the market; independence is part of the sampling hypothesis. In the auxiliary representation, the chi-squared law is the squared norm of independent standard normals. The zero-degree cases and footnote 6’s N=2,3N=2,3N=2,3 rules are encoded explicitly. Mathlib’s matrix inverse and real division are total operations; their values on singular sample covariances or zero denominators do not alter the distributions because those events have probability zero under the stated assumptions. Contributions establishing the sample-covariance distribution, the joint representation, the negative moments, and the final variance identity are within scope and can support other Gaussian portfolio results.

Selected references

  • N. Lassance, A. Martín-Utrera, and M. Simaan, The Risk of Expected Utility under Parameter Uncertainty, authors’ SSRN manuscript dated August 18, 2023, subsequently in Management Science (2024). SSRN 3855546; DOI 10.1287/mnsc.2023.00178.
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Information TheoryProbabilityQuantum Error Correction·Captain: mikedeng1

Quantum Tanner Codes 2: A Random Dual Tensor Code Is Δ^{3/2−ε}-Robust with Δ^γ-Resistance to Puncturing with Probability Tending to 1Research Paper

Motivation

Quantum error correction needs families of codes that protect a growing number of logical qubits while using checks that touch few physical qubits. In a quantum Tanner code, the local constraints come from two smaller binary codes. The distance analysis requires those local codes to satisfy a geometric condition called robustness: a low-weight word in a certain sum code must occupy only a controlled number of complete rows and columns. The deterministic distance theorem in Leverrier and Zémor's Quantum Tanner codes assumes this condition; their Theorem 9 supplies it for randomly chosen component codes. Establishing that random codes satisfy the assumption makes the later existence result meaningful rather than conditional on a property with no known examples.

The appendix follows the approach of Panteleev and Kalachev, Asymptotically good quantum and locally testable classical LDPC codes, with a separate treatment of puncturing. The historical relation here is limited: this mission formalizes Leverrier and Zémor's Theorem 9 and its own numbered supporting results, with their hypotheses and constants.

Setting

Fix two coordinate sets AAA and BBB, each of cardinality Δ\DeltaΔ. A binary linear code CA⊆F2AC_A\subseteq\mathbb F_2^ACA​⊆F2A​ is a vector subspace; similarly CB⊆F2BC_B\subseteq\mathbb F_2^BCB​⊆F2B​. Regard a word on A×BA\times BA×B as a matrix x=(xab)x=(x_{ab})x=(xab​). The column code contains matrices whose column at every b∈Bb\in Bb∈B belongs to CAC_ACA​. The row code contains matrices whose row at every a∈Aa\in Aa∈A belongs to CBC_BCB​. Their intersection is the tensor code CA⊗CBC_A\otimes C_BCA​⊗CB​; their sum is the dual tensor code CA⊗F2B+F2A⊗CBC_A\otimes\mathbb F_2^B+\mathbb F_2^A\otimes C_BCA​⊗F2B​+F2A​⊗CB​. The Hamming weight ∣x∣|x|∣x∣ counts its nonzero entries. These conventions are those of §3.5 of the source paper.

Write dA,dBd_A,d_BdA​,dB​ for the actual minimum distances of the two component codes. The dual tensor code is www-robust if every codeword xxx with ∣x∣≤w|x|\le w∣x∣≤w vanishes outside the union of some set of at most ∣x∣/dB|x|/d_B∣x∣/dB​ rows and some set of at most ∣x∣/dA|x|/d_A∣x∣/dA​ columns. Thus a low-weight word cannot be spread thinly across many rows and columns. For retained coordinate sets A′⊆AA'\subseteq AA′⊆A and B′⊆BB'\subseteq BB′⊆B, the punctured codes CA′C_{A'}CA′​ and CB′C_{B'}CB′​ are the images under restriction. Robustness has ppp-resistance to puncturing when the corresponding dual tensor code remains www-robust for every pair A′,B′A',B'A′,B′ of equal size obtained by removing at most ppp coordinates from each side. These are Definitions 5 and 8 on pp. 15–16 of the paper.

A uniform generator matrix with rrr rows and Δ\DeltaΔ columns is sampled uniformly from all binary matrices of that shape. Its row span is CAC_ACA​. Independently, a uniform parity-check matrix with sss rows and Δ\DeltaΔ columns defines CBC_BCB​ as its kernel. Probability is the fraction of matrices, or matrix pairs, satisfying an event. In the asymptotic statement, Δ\DeltaΔ tends through natural numbers to infinity.

Formalization targets

Random robustness and resistance

For 0<ρA,ρB<10<\rho_A,\rho_B<10<ρA​,ρB​<1, 0<ε<1/20<\varepsilon<1/20<ε<1/2, and 1/2+ε<γ<11/2+\varepsilon<\gamma<11/2+ε<γ<1, sample CAC_ACA​ and CBC_BCB​ from the matrix models above, using ⌊ρAΔ⌋\lfloor\rho_A\Delta\rfloor⌊ρA​Δ⌋ generator rows and ⌈(1−ρB)Δ⌉\lceil(1-\rho_B)\Delta\rceil⌈(1−ρB​)Δ⌉ parity-check rows. The goal, Theorem 9, is

Pr⁡ ⁣[CA⊗F2B+F2A⊗CB is Δ3/2−ε-robust with Δγ-resistance]⟶1.\Pr\!\left[C_A\otimes\mathbb F_2^B+\mathbb F_2^A\otimes C_B\text{ is }\Delta^{3/2-\varepsilon}\text{-robust with }\Delta^\gamma\text{-resistance}\right]\longrightarrow 1.Pr[CA​⊗F2B​+F2A​⊗CB​ is Δ3/2−ε-robust with Δγ-resistance]⟶1.

The milestones are the paper's numbered appendix statements: Lemma 31 converts concentration on few rows and columns into Definition 5's sharper weight-based bounds; Lemmas 24–29 address ranks and probabilities for random kernels and punctured kernels; Theorem 30 gives the quantitative high-probability alternative used before the final limit. The goal fixes the exponents and quantifies over the whole uniform matrix experiment.

Significance

Theorem 9 certifies that the robustness hypothesis needed by the paper's distance construction occurs with asymptotic probability one. It covers all allowed puncturings at once, which matters because a later distance argument deletes coordinates selected by the codeword under study. A statement about one fixed puncturing would not provide that guarantee. The result is proved in the 2022 paper; this mission poses its statements for machine-checked proofs and does not claim that those proofs already exist.

Formalizing the result produces reusable finite probability statements for random linear codes, a parity-check treatment of puncturing, and rank bounds for sparse binary matrices. Those ingredients are independent of the group complex used in the paper's other mission. They can support later formalizations of random coding arguments where a union over many coordinate restrictions is necessary.

Difficulty

The evident first check is that one fixed low-weight matrix probably does not belong to a random dual tensor code. That alone does not establish robustness: the statement ranges over all such matrices and, for resistance, over every pair of large retained coordinate sets. The paper's intermediate results control this whole collection using rank information about sparse matrices and the exact probability that independent vectors lie in a random kernel. A further issue is that puncturing a parity-check code does not simply delete columns from its defining matrix; the discarded columns contribute a random subspace. The quantitative event in Theorem 30 and the simultaneous limit in Theorem 9 both have to survive these ranges.

Formalization scope

Lean uses ZMod 2 for F2\mathbb F_2F2​, Fin \Delta for each coordinate set, and functions on A×BA\times BA×B for matrices. Rows are indexed by AAA and belong to CBC_BCB​; columns are indexed by BBB and belong to CAC_ACA​. The published TillichZemor.HGP.Setting supplies the parity-check kernel and the extended-natural minimum distance, whose value is infinity for the zero code. CodingTheory is a published prerequisite. Local definitions give the row and column codes, their sum, puncturing, robustness, uniform finite probability, generator row span, and binary entropy in bits.

The printed matrix sizes ρAΔ\rho_A\DeltaρA​Δ and (1−ρB)Δ(1-\rho_B)\Delta(1−ρB​)Δ need integer values. The chosen floor and ceiling keep their respective dimensions within the bounds used in the appendix. Every logarithm in the formalized appendix bounds means log⁡2\log_2log2​, including occurrences printed simply as log⁡\loglog. Theorem 30 includes an explicit sufficiently-large-Δ\DeltaΔ threshold, as its proof's asymptotic count requires, and carries the appendix's preceding entropy condition δ<h−1(1−ρ)\delta<h^{-1}(1-\rho)δ<h−1(1−ρ) as δ<1/2\delta<1/2δ<1/2 and h2(δ)<1−ρh_2(\delta)<1-\rhoh2​(δ)<1−ρ. Lemmas 25, 26, and 29 use the preceding condition d>2αΔd>2\alpha\Deltad>2αΔ; the symbol beside Δ\DeltaΔ in the scan is ambiguous, and the argument on p. 29 determines this reading. These choices are recorded for audit in MODERATION_NOTES.md.

The probability space is all matrices of each stated size, with the two matrices in Theorem 9 sampled independently. There is no conditioning on a favorable code or an assumed version of Theorem 30 in the goal. The mission does not formalize the later quantum Tanner code construction or the cited Gilbert–Varshamov result as an additional item. Contributions proving the goal, the numbered milestones, or reusable rank and finite-probability facts are within scope.

Selected references

  • Anthony Leverrier and Gilles Zémor, Quantum Tanner codes, arXiv:2202.13641v3, 2022. Preprint.
  • Pavel Panteleev and Gleb Kalachev, Asymptotically good quantum and locally testable classical LDPC codes, arXiv:2111.03654, 2021. Preprint.
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Graph TheoryQuantum Error CorrectionQuantum Information·Captain: mikedeng1

Quantum Tanner Codes 1: On a Ramanujan Left-Right Cayley Complex with Robust Dual Tensor Codes, the Quantum Tanner Code Has Rate at Least (1−2ρ)² and Distance at Least δn/(4Δ^{3/2+ε})Research Paper

Why quantum Tanner codes matter

An error-correcting code protects information by adding redundancy. A quantum code must also account for two kinds of errors, commonly called XXX and ZZZ errors. Quantum low-density parity-check codes use checks that each touch only a bounded number of qubits, while each qubit participates in only a bounded number of checks. Such locality matters when the number of qubits grows. For years it was difficult to make both the number of encoded qubits and the minimum distance proportional to the block length while retaining bounded-weight checks. Leverrier and Zémor's quantum Tanner construction gives a route through local codes placed on an expanding square complex; its main distance theorem is the target of this mission Leverrier and Zémor, 2022.

The construction combines two earlier ingredients. Left-right Cayley complexes provide the squares and expansion properties used by the code Dinur, Evra, Livne, Lubotzky, and Mozes, 2021. Robustness of a dual tensor code, including after puncturing coordinates, controls local words Panteleev and Kalachev, 2021. The paper states the local reduction property as Theorem 1 and derives the rate and distance bounds as Theorem 17. This mission formalizes that implication under the paper's stated component-code and expansion conditions; the separate random-code result that supplies robust examples belongs to the second mission of this series.

The square complex and its codes

Let GGG be a finite group and let A,B⊆GA,B\subseteq GA,B⊆G be inverse-closed sets, each of size Δ\DeltaΔ. The total no-conjugacy condition says ag≠gbag\ne gbag=gb for every a∈Aa\in Aa∈A, b∈Bb\in Bb∈B, and g∈Gg\in Gg∈G. Vertices are two copies of the group, V=G×{0,1}V=G\times\{0,1\}V=G×{0,1}. A square associated with v=(g,i)v=(g,i)v=(g,i) and (a,b)∈A×B(a,b)\in A\times B(a,b)∈A×B has vertices vvv, (ag,1−i)(ag,1-i)(ag,1−i), (gb,1−i)(gb,1-i)(gb,1−i), and (agb,i)(agb,i)(agb,i). The set of squares is QQQ, and a binary word on QQQ has length n=∣Q∣n=|Q|n=∣Q∣. At a vertex vvv, the incident squares are indexed by A×BA\times BA×B; this indexing makes the local view xvx_vxv​ of a word x∈F2Qx\in\mathbb F_2^Qx∈F2Q​ an A×BA\times BA×B matrix Leverrier and Zémor, §§3.2 and 4.1.

A binary linear code CAC_ACA​ has coordinates indexed by AAA, and CBC_BCB​ has coordinates indexed by BBB. Their tensor code CA⊗CBC_A\otimes C_BCA​⊗CB​ consists of matrices whose columns lie in CAC_ACA​ and whose rows lie in CBC_BCB​. The dual tensor code CA⊗F2B+F2A⊗CBC_A\otimes\mathbb F_2^B+\mathbb F_2^A\otimes C_BCA​⊗F2B​+F2A​⊗CB​ is the sum of the column and row codes. In Definition 5, it is www-robust when every member of weight at most www is supported on a union of few rows and columns, with the bounds determined by the two component minimum distances. Definition 8 requires this property after deleting up to ppp coordinates from each side. These are conditions on all relevant codewords and all permitted puncturings, including the unpunctured pair Leverrier and Zémor, pp. 15–16.

The two Tanner codes are C0=T(G0□,(CA⊗CB)⊥)\mathcal C_0=T(\mathcal G^\square_0,(C_A\otimes C_B)^\perp)C0​=T(G0□​,(CA​⊗CB​)⊥) and C1=T(G1□,(CA⊥⊗CB⊥)⊥)\mathcal C_1=T(\mathcal G^\square_1,(C_A^\perp\otimes C_B^\perp)^\perp)C1​=T(G1□​,(CA⊥​⊗CB⊥​)⊥). Here Gi□\mathcal G^\square_iGi□​ is the square-adjacency graph on the vertices in copy iii. Together they define the quantum CSS code Q=(C0,C1)\mathcal Q=(\mathcal C_0,\mathcal C_1)Q=(C0​,C1​). Its dimension counts encoded qubits. Its distance is the smaller of the minimum weights in C0∖C1⊥\mathcal C_0\setminus\mathcal C_1^\perpC0​∖C1⊥​ and C1∖C0⊥\mathcal C_1\setminus\mathcal C_0^\perpC1​∖C0⊥​ Leverrier and Zémor, pp. 14, 18.

Formalization targets

The goal is Theorem 17. Fix 0<ρ<1/20<\rho<1/20<ρ<1/2, 0<ε<1/20<\varepsilon<1/20<ε<1/2, 1/2+ε<γ<11/2+\varepsilon<\gamma<11/2+ε<γ<1, and δ>0\delta>0δ>0. For sufficiently large Δ\DeltaΔ, take a left-right Cayley complex satisfying total no-conjugacy and the paper's Ramanujan conditions. Require 0<dim⁡CA≤ρΔ0<\dim C_A\le\rho\Delta0<dimCA​≤ρΔ, dim⁡CB=Δ−dim⁡CA\dim C_B=\Delta-\dim C_AdimCB​=Δ−dimCA​, minimum distance at least δΔ\delta\DeltaδΔ for CA,CBC_A,C_BCA​,CB​ and both duals, and Δ3/2−ε/2\Delta^{3/2-\varepsilon/2}Δ3/2−ε/2 robustness with Δγ\Delta^\gammaΔγ resistance to puncturing for both relevant dual tensor codes. The target is

k≥(1−2ρ)2n,d≥δn4Δ3/2+ε.k\ge (1-2\rho)^2 n,\qquad d\ge \frac{\delta n}{4\Delta^{3/2+\varepsilon}}.k≥(1−2ρ)2n,d≥4Δ3/2+εδn​.

The milestones mirror the paper's route to this result. Lemma 4 bounds the nontrivial eigenvalues of the union and square graphs. Propositions 6 and 7 turn dual-tensor robustness into a decomposition and a 3/23/23/2 closeness bound. Theorem 1 supplies a weight-reducing local codeword for every sufficiently light nonzero Tanner-code word. Display (5) supplies the dimension lower bound. Theorem 17 combines the two distance directions with that rate estimate Leverrier and Zémor, pp. 12, 15–16, 18–23.

What the result supplies

The lower bound on kkk ensures a positive fraction of qubits can carry logical information when ρ<1/2\rho<1/2ρ<1/2. The lower bound on ddd rules out small undetectable logical errors. For a fixed allowable degree Δ\DeltaΔ, both bounds scale linearly with nnn. The paper also shows that random component codes can satisfy the robustness assumptions; that probabilistic result is a separate formalization target Leverrier and Zémor, Theorems 9 and 17.

A checked development would make explicit how the square indexing, duals, punctured codes, and CSS quotient fit together. The source proves the mathematical result; the statements here remain open Lean theorems. Reusable contributions include the tensor-code interface, spectral bounds for the graph construction, and lemmas connecting local views to the global Tanner codes. A proof of the existence of infinite Ramanujan complex families is outside this mission's stated target.

Where the proof is difficult

A light global codeword need not have a local view that is itself close to a tensor-code word. Some square-graph vertices have unusually large local weight, and puncturing is needed to isolate coordinates shared with those exceptional vertices. The paper's small-set expansion estimates and robustness conditions control those interactions. Simply averaging local weights does not yield the weight-reducing local codeword asserted by Theorem 1 Leverrier and Zémor, §4.2.

Formalization scope

Words are functions into ZMod 2, codes are submodules, and a matrix is a function on A×BA\times BA×B with AAA indexing rows. The square coordinates are four-element vertex sets. The construction uses V=G×Fin⁡(2)V=G\times\operatorname{Fin}(2)V=G×Fin(2) and counts nnn as the number of squares rather than building n=Δ2∣G∣/2n=\Delta^2|G|/2n=Δ2∣G∣/2 into a definition. The minimum distance of the zero code is infinity, and robustness uses inequalities involving that extended value. Powers of Δ\DeltaΔ and the parameters w,pw,pw,p are real; the paper uses integer w,pw,pw,p in Definition 8, while the theorem's power thresholds need real comparisons. The formal robustness predicate includes Definition 5's range 0≤w≤Δ20\le w\le\Delta^20≤w≤Δ2; the theorem thresholds satisfy it for sufficiently large Δ\DeltaΔ. These conventions are recorded with each item.

The goal quantifies over every finite complex satisfying inverse closure, total no-conjugacy, and Ramanujan conditions, with a uniform threshold Δ0\Delta_0Δ0​ chosen before the group and codes. This pins the complexes in the cited infinite family without formalizing their existence. In particular, the goal contains no auxiliary set or local reduction assumption that could make the distance bound immediate. The published CodingTheory and TillichZemor.HGP.Setting definitions supply dual codes and CSS dimension; the paper-specific setting supplies the square complex, local views, Tanner codes, and robustness. Contributions that keep these conventions and close any milestone theorem are welcome.

Selected references

  • A. Leverrier and G. Zémor, Quantum Tanner codes, arXiv preprint, 2022. arXiv:2202.13641v3.
  • I. Dinur, S. Evra, R. Livne, A. Lubotzky, and S. Mozes, Locally Testable Codes with constant rate, distance, and locality, arXiv preprint, 2021. arXiv:2111.04808.
  • P. Panteleev and G. Kalachev, Asymptotically good quantum and locally testable classical LDPC codes, arXiv preprint, 2021. arXiv:2111.03654.
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Convex OptimizationOperations ResearchProbability+1·Captain: mikedeng1

Real-Time Spatial–Intertemporal Pricing and Relocation in a Ride-Hailing Network: Near-Optimal Policies and the Value of Dynamic Pricing 1: Arc Balancing Control Has Loss O(log(1+n)^{3/2}/n^{2/3})Research Paper

Why spatial pricing needs a dynamic control

A ride-hailing firm chooses prices while drivers move through a city. A trip from one region uses a driver immediately and returns that driver at another region only after a travel delay. Prices affect which trips are requested, but the actual requests fluctuate. A plan that ignores these fluctuations can run out of available drivers at a busy origin even when its average flows fit the fleet. Chen, Lei, and Jasin study how closely a feasible pricing control can approach a deterministic revenue benchmark in this setting (accepted manuscript, published article).

Their Arc Balancing Control (ABC) responds to realized trips. It groups each directed arc's periods into batches and adjusts the next batch's demand rates according to the previous batch's cumulative surplus or deficit. The paper proves a loss rate for ABC that is smaller than the rate established there for its Static Price Control. The target here is the paper's Theorem 3, with the model and parameters of its authors' accepted manuscript. Its e-companion contains the paper's proofs.

The pricing network and benchmark

The network has N≥1N\ge1N≥1 regions and a horizon of T≥1T\ge1T≥1 periods. Every ordered pair i→ji\to ji→j, including i=ji=ji=j, is an arc. At most one customer can request an arc's trip in a period. A served trip takes one server from region iii for τij≥1\tau_{ij}\ge1τij​≥1 periods, then returns it at jjj. Region iii starts with Ci≥NC_i\ge NCi​≥N servers. A control must respect the available server count before it serves each period's realized requests.

The decision is a demand rate λt,ij∈[0,1]\lambda_{t,ij}\in[0,1]λt,ij​∈[0,1] rather than its inverse price. The expected revenue from that arc and period is rt,ij(λt,ij)r_{t,ij}(\lambda_{t,ij})rt,ij​(λt,ij​). The revenue functions are nonnegative and strongly concave, vanish at zero, and have bounded first and second derivatives. The bound on those derivatives is Ψ3>0\Psi_3>0Ψ3​>0. The paper's price-side assumptions imply these rate-side conditions; the Lean model states the conditions directly.

The deterministic convex program DCP(ζ)\mathrm{DCP}(\zeta)DCP(ζ) chooses rates to maximize the sum of expected revenues. Its flow constraints replace realized trips with their rates, while its cushion requires ζ≤λt,ij≤1−ζ\zeta\le\lambda_{t,ij}\le1-\zetaζ≤λt,ij​≤1−ζ. Write J(ζ)J(\zeta)J(ζ) for its value and λζ,D\lambda^{\zeta,D}λζ,D for an optimal schedule. In the nnnth system, the fleet, horizon, and travel times are multiplied by nnn; each original period's revenue curve is used for nnn consecutive scaled periods. Thus Tn=nTT^n=nTTn=nT and τ‾n=nmin⁡i,jτij\underline\tau^n=n\min_{i,j}\tau_{ij}τ​n=nmini,j​τij​. For a control π\piπ, the per-period benchmark loss is

Lπ(n)=J(n,0)−Eπ[Rπ(n)]Tn.L^\pi(n)=\frac{J(n,0)-\mathbb E^\pi[R^\pi(n)]}{T^n}.Lπ(n)=TnJ(n,0)−Eπ[Rπ(n)]​.

ABC uses λn,ζ,D\lambda^{n,\zeta,D}λn,ζ,D as its baseline. Its batches have a target sum bbb of the baseline variance weights λt,ijn,ζ,D(1−λt,ijn,ζ,D)\lambda^{n,\zeta,D}_{t,ij}(1-\lambda^{n,\zeta,D}_{t,ij})λt,ijn,ζ,D​(1−λt,ijn,ζ,D​). Within a batch, the control subtracts a weighted share of the preceding batch's realized surplus δˉijk=∑t∈Tijk(Dt,ij−λt,ijABC)\bar\delta^k_{ij}=\sum_{t\in\mathcal T^k_{ij}}(D_{t,ij}-\lambda^{ABC}_{t,ij})δˉijk​=∑t∈Tijk​​(Dt,ij​−λt,ijABC​). A rate is projected to [0,1][0,1][0,1], and an origin with too few available servers is turned off. The finite path law uses the rates posted along each path.

Formalization targets

The principal target is Theorem 3. With bn=(τ‾n)2/3b_n=(\underline\tau^n)^{2/3}bn​=(τ​n)2/3 and

ϵn=(τ‾n)−1(1+162(bn+1)log⁡Tn),ζn=2ϵn,\epsilon_n=(\underline\tau^n)^{-1}\left(1+16\sqrt{2(b_n+1)\log T^n}\right),\qquad \zeta_n=2\epsilon_n,ϵn​=(τ​n)−1(1+162(bn​+1)logTn​),ζn​=2ϵn​,

there is a constant Ψ~2\widetilde\Psi_2Ψ2​, independent of nnn, for which every integer n≥1n\ge1n≥1 satisfies

LABC(n)≤Ψ~2log⁡(1+n)3/2n2/3.L^{ABC}(n)\le\widetilde\Psi_2\frac{\log(1+n)^{3/2}}{n^{2/3}}.LABC(n)≤Ψ2​n2/3log(1+n)3/2​.

The milestone list follows the source results used in the analysis: Lemma 2 bounds the deterministic cost of a small cushion and gives feasibility; Lemma EC.1 bounds a maximal cumulative Bernoulli deviation; and the two parts of Lemma 4 characterize ABC on a batchwise good event A\mathcal AA and bound that event's probability. Theorem 3 fixes the complete control and these exact parameters; its constant may depend on the fixed network instance and Ψ3\Psi_3Ψ3​.

What the result establishes

The theorem gives a finite-nnn loss bound relative to J(n,0)J(n,0)J(n,0), with the stated n−2/3n^{-2/3}n−2/3 rate and logarithmic factor. In the paper, Lemma 1 shows that J(n,0)J(n,0)J(n,0) bounds the optimal admissible policy's revenue. Theorem 3 therefore bounds ABC's distance from a benchmark that is at least as high as the unknown stochastic optimum. The paper compares this rate with its n−1/2n^{-1/2}n−1/2 result for Static Price Control and explains the resulting value of adapting prices to realized demand (Theorems 2–3).

The published mathematical result and its manuscript proof are known; the statements in this mission are Lean targets with proofs still to be formalized. A complete development would also make reusable definitions for finite controlled path laws, delayed network flow balance, and cushioned deterministic relaxations. The batch and feedback definitions isolate the paper-specific control from that general infrastructure.

Main difficulty

The deterministic program controls expected flows, while ABC must keep every realized path feasible. An unadjusted baseline can accumulate demand fluctuations over the whole horizon; bounding those fluctuations alone does not describe the effect of ABC's feedback. The control's posted rate in a period depends on earlier realized requests, which changes the distribution of later requests. The manuscript's proof of Lemma 4 bounds a variance proxy from its deterministic baseline when treating the adaptive posted rates; that step needs separate justification in a formal proof. Lemma EC.1, as posed here, covers deterministic Bernoulli rates and does not by itself close that gap. The finite-horizon claim, including small scaling factors for which the cushioned DCP may be infeasible, must still be established.

Formalization scope

Lean represents regions by Fin N, periods by natural numbers 1,…,T1,\ldots,T1,…,T, travel times and server counts by naturals, demand by Boolean paths, and revenue and rates by real numbers. The DCP(n,ζ)\mathrm{DCP}(n,\zeta)DCP(n,ζ) program uses a real supremum; statements involving positive ζ\zetaζ assert feasibility, and J(n,0)J(n,0)J(n,0) has the zero schedule as a feasible point. ABC's path law is the product of sequential Bernoulli factors at its own posted rates. Its rate history is built by structural recursion, and the event A\mathcal AA checks every nonempty batch and all its partial sums.

The accepted manuscript leaves the final incomplete batch unspecified, so the last short batch is merged with its predecessor. The printed ABC box turns an origin off at Ct,i≤NC_{t,i}\le NCt,i​≤N, while Lemma 4 and its base case require service when Ct,i=NC_{t,i}=NCt,i​=N; the formal control uses Ct,i≥NC_{t,i}\ge NCt,i​≥N. If the cushioned DCP has no optimum, the baseline is zero. The sample-path part of Lemma 4 adds the hypothesis τ‾≤T\underline\tau\le Tτ​≤T, which the manuscript does not print. Without it the part is false: when the horizon is shorter than every travel time, no server returns, and a single realized trip can leave a region below NNN servers on the good event. These conventions are recorded with the source discrepancies in the moderation notes. The rate model drops assumptions A1 and A3(i), which concern only the price parametrization, and writes A2, A3(ii), r≥0r\ge0r≥0, and r(0)=0r(0)=0r(0)=0 directly. It assumes a twice continuously differentiable extension of revenue to R\mathbb RR. No statement substitutes expected demand for the realized batch surplus or lets the theorem's parameters depend on nnn by existential choice. Contributions toward the source milestones, the adaptive concentration step, and the reusable model definitions are all within scope.

Selected references

  • Q. Chen, Y. Lei, and S. Jasin, Real-Time Spatial-Intertemporal Pricing and Relocation in a Ride-Hailing Network: Near Optimal Heuristics and The Value of Dynamic Pricing, authors' accepted manuscript, LBS Research Online eprint 2845, pp. 7–25 and ec2–ec6; published as Real-Time Spatial–Intertemporal Pricing and Relocation in a Ride-Hailing Network: Near-Optimal Policies and the Value of Dynamic Pricing, Operations Research 72(5):2097–2118, 2024. Manuscript, DOI.
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Numerical AnalysisOperations ResearchOptimization·Captain: mikedeng1

A First-Order Primal-Dual Method for Nonconvex Constrained Optimization Based on the Augmented Lagrangian 4: Metric Subregularity of ∂L_γ Implies the VP-EB Error BoundResearch Paper

Motivation

Many problems in signal processing, statistics and engineering design have the form of a nonconvex, possibly nonsmooth objective subject to nonlinear equality constraints. Zhu, Zhao and Zhang (arXiv:2007.12219v1, 2020; published in Mathematics of Operations Research, 2024) propose NAPP-AL, a first-order primal-dual method that takes one linearized step on the augmented Lagrangian per iteration. Their analysis has three layers: subsequential convergence with an o(1/k)o(1/\sqrt k)o(1/k​) stationarity rate (§4), linear convergence under a new value proximity error bound (VP-EB, §5), and sufficient conditions for VP-EB (§6).

This mission formalizes the second sufficient condition: metric subregularity of the stationarity map, together with a local value condition on nearby stationary points, implies VP-EB. Metric subregularity is a standard regularity notion of variational analysis (Dontchev–Rockafellar), and error bounds of this kind are the classical route to linear convergence (Luo–Tseng). The paper attributes the cost-to-go inequality it relies on to Tseng and Yun [18]. A companion mission treats the KL-property route (Proposition 6.1); a third proves linear convergence from VP-EB (Theorem 5.1).

Setting

Write w=(u,v,p)∈Rn×Rd×Rmw=(u,v,p)\in\mathbb R^n\times\mathbb R^d\times\mathbb R^mw=(u,v,p)∈Rn×Rd×Rm with the Euclidean norm of the stacked vector, ∥w∥=∥u∥2+∥v∥2+∥p∥2\|w\|=\sqrt{\|u\|^2+\|v\|^2+\|p\|^2}∥w∥=∥u∥2+∥v∥2+∥p∥2​, and B(wˉ;η)\mathbb B(\bar w;\eta)B(wˉ;η) the open ball. The problem (P) is

min⁡u∈U, v∈Rd F(u,v)=G(u,v)+J(u)+H(v)s.t.Θ(u)+Bv=0,Θ=Ω+Φ,\min_{u\in U,\,v\in\mathbb R^d}\ F(u,v)=G(u,v)+J(u)+H(v)\quad\text{s.t.}\quad \Theta(u)+Bv=0,\qquad \Theta=\Omega+\Phi,u∈U,v∈Rdmin​ F(u,v)=G(u,v)+J(u)+H(v)s.t.Θ(u)+Bv=0,Θ=Ω+Φ,

with G,HG,HG,H smooth with Lipschitz gradients, JJJ lower semicontinuous and locally Lipschitz near UUU, UUU closed and convex, Θ\ThetaΘ Lipschitz, each component of Ω\OmegaΩ with Lipschitz gradient, and BBB an m×dm\times dm×d matrix of full column rank with Im Θ⊆Im B\mathrm{Im}\,\Theta\subseteq\mathrm{Im}\,BImΘ⊆ImB; FFF is bounded below and coercive on the feasible set (Assumption 1).

The augmented Lagrangian is Lγ(w)=F(u,v)+⟨p,Θ(u)+Bv⟩+γ2∥Θ(u)+Bv∥2\mathcal L_\gamma(w)=F(u,v)+\langle p,\Theta(u)+Bv\rangle+\tfrac\gamma2\|\Theta(u)+Bv\|^2Lγ​(w)=F(u,v)+⟨p,Θ(u)+Bv⟩+2γ​∥Θ(u)+Bv∥2. The set ∂Lγ(w)\partial\mathcal L_\gamma(w)∂Lγ​(w) is the KKT display of p. 6: with r=Θ(u)+Bvr=\Theta(u)+Bvr=Θ(u)+Bv, it collects the triples

(∇uG+∂J(u)+NU(u)+(∇Θ(u))⊤[p+γr],  ∇vG+∇H(v)+B⊤[p+γr],  r),\big(\nabla_uG+\partial J(u)+N_U(u)+(\nabla\Theta(u))^\top[p+\gamma r],\ \ \nabla_vG+\nabla H(v)+B^\top[p+\gamma r],\ \ r\big),(∇u​G+∂J(u)+NU​(u)+(∇Θ(u))⊤[p+γr],  ∇v​G+∇H(v)+B⊤[p+γr],  r),

with ∂J\partial J∂J the limiting subdifferential and NUN_UNU​ the normal cone. A point is stationary if 0∈∂Lγ(w)0\in\partial\mathcal L_\gamma(w)0∈∂Lγ​(w); Wˉ\bar{\mathbf W}Wˉ is the set of stationary points. Distances follow the paper's convention: dist(x,C)=inf⁡z∈C∥x−z∥\mathrm{dist}(x,C)=\inf_{z\in C}\|x-z\|dist(x,C)=infz∈C​∥x−z∥, and dist(x,∅)=+∞\mathrm{dist}(x,\emptyset)=+\inftydist(x,∅)=+∞.

NAPP-AL keeps qk=pk+γ(Θ(uk)+Bvk)q^k=p^k+\gamma(\Theta(u^k)+Bv^k)qk=pk+γ(Θ(uk)+Bvk), takes uk+1u^{k+1}uk+1 as a global minimizer over UUU of a linearized model with a Bregman term D(u,uk)/ϵkD(u,u^k)/\epsilon^kD(u,uk)/ϵk, vk+1v^{k+1}vk+1 as the minimizer of a strongly convex quadratic, and sets pk+1=pk+γ(Θ(uk+1)+Bvk+1)p^{k+1}=p^k+\gamma(\Theta(u^{k+1})+Bv^{k+1})pk+1=pk+γ(Θ(uk+1)+Bvk+1). The step ϵk\epsilon^kϵk lies in [σδk,δk][\sigma\delta_k,\delta_k][σδk​,δk​] with δk\delta_kδk​ given explicitly by (8), and γ>(57+1)(LG+LH)/(2λmin⁡(B⊤B))\gamma>(\sqrt{57}+1)(L_G+L_H)/(2\lambda_{\min}(B^\top B))γ>(57​+1)(LG​+LH​)/(2λmin​(B⊤B)) (Assumption 2).

VP-EB at wˉ\bar wwˉ (Definition 5.1): there are κ1,η,ν>0\kappa_1,\eta,\nu>0κ1​,η,ν>0 such that Lγ(wk+1)−Lγ(wˉ)≤κ1∥wk−wk+1∥2\mathcal L_\gamma(w^{k+1})-\mathcal L_\gamma(\bar w)\le\kappa_1\|w^k-w^{k+1}\|^2Lγ​(wk+1)−Lγ​(wˉ)≤κ1​∥wk−wk+1∥2 whenever wk+1∈B(wˉ;η)w^{k+1}\in\mathbb B(\bar w;\eta)wk+1∈B(wˉ;η) and Lγ(wk+1)<Lγ(wˉ)+ν\mathcal L_\gamma(w^{k+1})<\mathcal L_\gamma(\bar w)+\nuLγ​(wk+1)<Lγ​(wˉ)+ν.

Metric subregularity (Definition 6.2): ∂Lγ\partial\mathcal L_\gamma∂Lγ​ is metrically subregular around (wˉ,0)(\bar w,0)(wˉ,0) if, for some η,κ3>0\eta,\kappa_3>0η,κ3​>0, dist(w,Wˉ)≤κ3 dist(0,∂Lγ(w))\mathrm{dist}(w,\bar{\mathbf W})\le\kappa_3\,\mathrm{dist}(0,\partial\mathcal L_\gamma(w))dist(w,Wˉ)≤κ3​dist(0,∂Lγ​(w)) for all w∈B(wˉ;η)w\in\mathbb B(\bar w;\eta)w∈B(wˉ;η). Assumption 3 at a stationary wˉ∈Wˉ\bar w\in\bar{\mathbf W}wˉ∈Wˉ: for some δ>0\delta>0δ>0, Lγ(w)≤Lγ(wˉ)\mathcal L_\gamma(w)\le\mathcal L_\gamma(\bar w)Lγ​(w)≤Lγ​(wˉ) for all w∈Wˉw\in\bar{\mathbf W}w∈Wˉ with ∥w−wˉ∥≤δ\|w-\bar w\|\le\delta∥w−wˉ∥≤δ.

Formalization targets

Goal: Proposition 6.2 (p. 26)

Let {wk}\{w^k\}{wk} be generated by NAPP-AL in the standing setting and let wˉ\bar wwˉ be a cluster point. If Assumption 3 holds at wˉ\bar wwˉ with δ\deltaδ, and ∂Lγ\partial\mathcal L_\gamma∂Lγ​ is metrically subregular around (wˉ,0)(\bar w,0)(wˉ,0) with κ3>0\kappa_3>0κ3​>0 and η>0\eta>0η>0, η<δ\eta<\deltaη<δ, then

∃ κ1,η′,ν>0:wk+1∈B(wˉ;η′), Lγ(wk+1)<Lγ(wˉ)+ν ⟹ Lγ(wk+1)−Lγ(wˉ)≤κ1∥wk−wk+1∥2.\exists\,\kappa_1,\eta',\nu>0:\quad w^{k+1}\in\mathbb B(\bar w;\eta'),\ \mathcal L_\gamma(w^{k+1})<\mathcal L_\gamma(\bar w)+\nu\ \Longrightarrow\ \mathcal L_\gamma(w^{k+1})-\mathcal L_\gamma(\bar w)\le\kappa_1\|w^k-w^{k+1}\|^2 .∃κ1​,η′,ν>0:wk+1∈B(wˉ;η′), Lγ​(wk+1)<Lγ​(wˉ)+ν ⟹ Lγ​(wk+1)−Lγ​(wˉ)≤κ1​∥wk−wk+1∥2.

The constants are existential, as in Definition 5.1, so the statement survives any improvement of them.

Milestone: Lemma 6.1 (p. 23), the cost-to-go inequality

∀wˉ∈Wˉ  ∃ c6>0  ∀k:Lγ(wk+1)−Lγ(wˉ)≤c6(∥wˉ−wk+1∥2+∥wk−wk+1∥2).\forall\bar w\in\bar{\mathbf W}\ \ \exists\,c_6>0\ \ \forall k:\quad \mathcal L_\gamma(w^{k+1})-\mathcal L_\gamma(\bar w)\le c_6\big(\|\bar w-w^{k+1}\|^2+\|w^k-w^{k+1}\|^2\big).∀wˉ∈Wˉ  ∃c6​>0  ∀k:Lγ​(wk+1)−Lγ​(wˉ)≤c6​(∥wˉ−wk+1∥2+∥wk−wk+1∥2).

Significance

The result. Combined with Theorem 5.1 of the paper, Proposition 6.2 gives finite length, convergence of the whole sequence, Q-linear convergence of the potential and R-linear convergence of the iterates whenever the stationarity map is metrically subregular at the limit and Assumption 3 holds there. Metric subregularity is known for broad classes, such as piecewise linear-quadratic problems and polyhedral multifunctions, so the proposition turns a structural property of the problem into a rate for this algorithm.

Formalizing it. The proposition is proved on paper; nothing about NAPP-AL has a machine-checked proof. The formalization makes two things exact that the paper leaves loose. First, the proposition’s proof needs a cost-to-go constant independent of the stationary point, and the proof of Lemma 6.1 supplies one even though the lemma’s printed statement fixes the point first. Second, the proposition's proof places the nearest stationary point wpk+1w_p^{k+1}wpk+1​ in B(wˉ;η)\mathbb B(\bar w;\eta)B(wˉ;η), while only ∥wpk+1−wˉ∥≤2η\|w_p^{k+1}-\bar w\|\le 2\eta∥wpk+1​−wˉ∥≤2η follows from its steps; the existential conclusion leaves room to shrink the radius. A formal proof settles both, and the general facts it needs (metric subregularity in [0,+∞][0,+\infty][0,+∞], closedness of limiting-subdifferential graphs) are reusable.

Difficulty

The obvious route is to combine subregularity with the residual bound of Theorem 4.1(iv), dist(0,∂Lγ(wk+1))≤c5∥wk−wk+1∥\mathrm{dist}(0,\partial\mathcal L_\gamma(w^{k+1}))\le c_5\|w^k-w^{k+1}\|dist(0,∂Lγ​(wk+1))≤c5​∥wk−wk+1∥, which bounds the distance from wk+1w^{k+1}wk+1 to Wˉ\bar{\mathbf W}Wˉ by the step. The difficulty is transferring a distance bound into a value bound of second order: local Lipschitz continuity of Lγ\mathcal L_\gammaLγ​ would bound Lγ(wk+1)−Lγ(wp)\mathcal L_\gamma(w^{k+1})-\mathcal L_\gamma(w_p)Lγ​(wk+1)−Lγ​(wp​) only by a multiple of ∥wk+1−wp∥\|w^{k+1}-w_p\|∥wk+1−wp​∥, which is first order in the step, while VP-EB asks for the square; and JJJ is nonsmooth and nonconvex, so no Taylor expansion at the stationary point is available. Moreover, the stationary point closest to wk+1w^{k+1}wk+1 changes with kkk. The proposition’s proof needs a cost-to-go inequality with a constant uniform over stationary points, which in turn rests on the boundedness of the iterates and on the lower bound for ϵk\epsilon^kϵk coming from (8). The radius bookkeeping between the subregularity ball, Assumption 3's radius and the VP-EB ball is a second, smaller obstacle.

Formalization scope

Rk\mathbb R^kRk is EuclideanSpace ℝ (Fin k) and points are triples E n × E d × E m; every norm and ball uses the stacked Euclidean norm tnorm, never Lean's product (sup) norm. BBB is a continuous linear map with its operator norm (the spectral norm), never a Matrix with the entrywise norm; λmin⁡(B⊤B)\lambda_{\min}(B^\top B)λmin​(B⊤B) is the Rayleigh minimum over the unit sphere. Distances dist(0,S)\mathrm{dist}(0,S)dist(0,S) and dist(w,S)\mathrm{dist}(w,S)dist(w,S) are infima in [0,+∞][0,+\infty][0,+∞], equal to +∞+\infty+∞ on the empty set; Metric.infDist, which returns 000 on ∅\emptyset∅ and would make subregularity and the residual bounds trivial, is not used. The normal cone NU(u)N_U(u)NU​(u) is empty for u∉Uu\notin Uu∈/U, so a nonempty normal cone off UUU cannot manufacture stationary points. (H3)'s local Lipschitz continuity is read on neighbourhoods in Rn\mathbb R^nRn of points of UUU, not Mathlib's relative LocallyLipschitzOn.

Disclosed readings of the arXiv v1 text: G,J,HG,J,HG,J,H are real-valued with globally Lipschitz gradients; λmin⁡(B⊤B)>0\lambda_{\min}(B^\top B)>0λmin​(B⊤B)>0; NAPP-AL is a relation on given sequences (any global minimizer may be selected; existence is not asserted); VP-EB is the inequality alone, without Definition 5.1's presupposition that the sequence converges to wˉ\bar wwˉ; "generated by NAPP-AL" in Lemma 6.1 and Proposition 6.2 carries the standing setting of Theorem 4.1 (Assumptions 1–2 and rule (8)); Lemma 6.1 follows the printed quantifier order; its proof supplies the uniform constant needed by Proposition 6.2. The radius of Assumption 3 is δ3 in Lean, distinct from the step sequence δk\delta_kδk​.

Welcome contributions: a proof of Lemma 6.1 from the optimality of (5)–(6), Lipschitz estimates and the bounds of Theorem 4.1(ii); the boundedness and residual results of Theorem 4.1 (formalized in the companion mission on the o(1/k)o(1/\sqrt k)o(1/k​) rate); closedness of Wˉ\bar{\mathbf W}Wˉ; and the radius argument of Proposition 6.2. The source is arXiv:2007.12219v1; numbering and constants of the published version are not used.

Selected references

  • D. Zhu, L. Zhao, S. Zhang, A First-Order Primal-Dual Method for Nonconvex Constrained Optimization Based on the Augmented Lagrangian, arXiv:2007.12219v1, 2020; Mathematics of Operations Research, 2024. https://arxiv.org/abs/2007.12219v1
  • P. Tseng, S. Yun, A coordinate gradient descent method for nonsmooth separable minimization, Mathematical Programming 117, 2009. https://doi.org/10.1007/s10107-007-0170-0
  • Z.-Q. Luo, P. Tseng, Error bounds and convergence analysis of feasible descent methods: a general approach, Annals of Operations Research 46, 1993. https://doi.org/10.1007/BF02096261
  • A. L. Dontchev, R. T. Rockafellar, Implicit Functions and Solution Mappings, 2nd ed., Springer, 2014. https://doi.org/10.1007/978-1-4939-1037-3
  • R. T. Rockafellar, R. J.-B. Wets, Variational Analysis, Springer, 1998. https://doi.org/10.1007/978-3-642-02431-3
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Subset Selection with Shrinkage: Sparse Linear Modeling When the SNR Is Low V: When the SNR Is Low, Best Subset Selection Has Prediction Error at Least of Order σ²γ²k log(ep/k)Research Paper

Why a lower bound for best subsets

Best subset selection fits a linear model by least squares using at most kkk of ppp available predictors. It is the classical ℓ0\ell_0ℓ0​-constrained estimator of sparse regression. Mixed-integer optimization now computes it for problems with thousands of variables (Bertsimas, King & Mazumder 2016), so its statistical behaviour matters in practice. Simulations in Hastie, Tibshirani & Tibshirani 2020 found that it predicts worse than shrinkage methods such as the Lasso when the signal-to-noise ratio (SNR) is low.

Mazumder, Radchenko and Dedieu (arXiv:1708.03288v4; Operations Research, 2023) add an ℓ1\ell_1ℓ1​ or ℓ2\ell_2ℓ2​ shrinkage penalty to best subsets. They prove upper bounds of two kinds: slow rates, linear in the tuning parameter λ\lambdaλ, and fast rates, quadratic in λ\lambdaλ. Theorems 2 and 3 of the paper give them for the shrunken estimators. For best subsets, the paper only has a fast-rate bound, of order σ2klog⁡(ep/k)\sigma^2 k\log(ep/k)σ2klog(ep/k). When ∥β∗∥/σ\|\beta^*\|/\sigma∥β∗∥/σ is small, the shrunken estimators' slow rate beats that bound. Theorem 4, the goal of this mission, shows that the comparison is meaningful: in that regime best subsets really does incur an error of the order of its upper bound.

Setting

The data follow the linear model

y=Xβ∗+ϵ,y,ϵ∈Rn, β∗∈Rp,y = X\beta^* + \epsilon ,\qquad y,\epsilon\in\mathbb R^n,\ \beta^*\in\mathbb R^p ,y=Xβ∗+ϵ,y,ϵ∈Rn, β∗∈Rp,

where the design XXX is a deterministic real n×pn\times pn×p matrix whose columns have unit Euclidean norm. The noise ϵ\epsilonϵ has independent N(0,σ2)N(0,\sigma^2)N(0,σ2) entries, with σ>0\sigma>0σ>0. Write ∥v∥\|v\|∥v∥ for the Euclidean norm, ∥v∥1=∑i∣vi∣\|v\|_1=\sum_i|v_i|∥v∥1​=∑i​∣vi​∣, supp⁡(v)={i:vi≠0}\operatorname{supp}(v)=\{i:v_i\ne0\}supp(v)={i:vi​=0} and ∥v∥0=∣supp⁡(v)∣\|v\|_0=|\operatorname{supp}(v)|∥v∥0​=∣supp(v)∣. The ℓ0\ell_0ℓ0​ ball is B0(s)={u∈Rp:∥u∥0≤s}B_0(s)=\{u\in\mathbb R^p:\|u\|_0\le s\}B0​(s)={u∈Rp:∥u∥0​≤s}. The minimal sss-sparse eigenvalue of XXX is

γs=min⁡u≠0, u∈B0(s)∥Xu∥∥u∥.\gamma_s=\min_{u\ne0,\ u\in B_0(s)}\frac{\|Xu\|}{\|u\|} .γs​=u=0, u∈B0​(s)min​∥u∥∥Xu∥​.

A best-subsets solution of size kkk is any minimizer

β^ℓ0∈arg⁡min⁡ ∥y−Xβ∥2s.t.∥β∥0≤k.(1)\hat\beta_{\ell_0}\in\arg\min\ \|y-X\beta\|^2\quad\text{s.t.}\quad\|\beta\|_0\le k .\tag{1}β^​ℓ0​​∈argmin ∥y−Xβ∥2s.t.∥β∥0​≤k.(1)

A constant is universal if it does not depend on n,p,k,X,σ,β∗n,p,k,X,\sigma,\beta^*n,p,k,X,σ,β∗. The symbols ≲\lesssim≲ and ≳\gtrsim≳ mean ≤\le≤ and ≥\ge≥ up to positive universal factors. Logarithms are natural, and e=exp⁡(1)e=\exp(1)e=exp(1).

Formalization targets

Goal: Theorem 4 (p. 18)

There are universal constants c0,c,C>0c_0,c,C>0c0​,c,C>0 such that the following holds. Suppose 2≤k≤p2\le k\le p2≤k≤p, ∥β∗∥0≤k\|\beta^*\|_0\le k∥β∗∥0​≤k and ∥β∗∥≤c0σγkklog⁡(ep/k)\|\beta^*\|\le c_0\sigma\gamma_k\sqrt{k\log(ep/k)}∥β∗∥≤c0​σγk​klog(ep/k)​. Then, with probability at least 1−2(ep/k)−cγk2k−(ep/k)−k1-2(ep/k)^{-c\gamma_k^2k}-(ep/k)^{-k}1−2(ep/k)−cγk2​k−(ep/k)−k, every best-subsets solution satisfies

∥Xβ^ℓ0−Xβ∗∥2 ≥ C σ2γk2 klog⁡(ep/k).\|X\hat\beta_{\ell_0}-X\beta^*\|^2\ \ge\ C\,\sigma^2\gamma_k^2\,k\log(ep/k).∥Xβ^​ℓ0​​−Xβ∗∥2 ≥ Cσ2γk2​klog(ep/k).

The constants are left unfixed, as in the paper. The statement asserts the order of the error, which is what the comparison with the upper bounds needs.

Milestones

  1. Maurey approximation (p. 44). For unit columns and every β∗\beta^*β∗, some β~∗\tilde\beta^*β~​∗ with ∥β~∗∥0≤k/2\|\tilde\beta^*\|_0\le k/2∥β~​∗∥0​≤k/2 has ∥Xβ∗−Xβ~∗∥2≤2∥β∗∥12/k\|X\beta^*-X\tilde\beta^*\|^2\le2\|\beta^*\|_1^2/k∥Xβ∗−Xβ~​∗∥2≤2∥β∗∥12​/k.
  2. (39) (p. 44). With Δ∗=Xβ∗−Xβ~∗\Delta^*=X\beta^*-X\tilde\beta^*Δ∗=Xβ∗−Xβ~​∗, define G(β)=∥y−Xβ∥2−∥y−Xβ~∗∥2G(\beta)=\|y-X\beta\|^2-\|y-X\tilde\beta^*\|^2G(β)=∥y−Xβ∥2−∥y−Xβ~​∗∥2 and H(u)=∥Xu∥2−2(Δ∗+ϵ)⊤XuH(u)=\|Xu\|^2-2(\Delta^*+\epsilon)^\top XuH(u)=∥Xu∥2−2(Δ∗+ϵ)⊤Xu. Then G(β)G(\beta)G(β) equals ∥Xβ−Xβ~∗∥2+2(Δ∗+ϵ)⊤(Xβ~∗−Xβ)\|X\beta-X\tilde\beta^*\|^2+2(\Delta^*+\epsilon)^\top(X\tilde\beta^*-X\beta)∥Xβ−Xβ~​∗∥2+2(Δ∗+ϵ)⊤(Xβ~​∗−Xβ), and min⁡∥β∥0≤kG≤min⁡H(u)\min_{\|\beta\|_0\le k}G\le\min H(u)min∥β∥0​≤k​G≤minH(u) over uuu supported off supp⁡(β~∗)\operatorname{supp}(\tilde\beta^*)supp(β~​∗) with ∥u∥0≤k/2\|u\|_0\le k/2∥u∥0​≤k/2.
  3. (40) (p. 45). min⁡∥β∥0≤kG(β)≤−max⁡v∈Vk∣(Δ∗+ϵ)⊤Xv∣2\min_{\|\beta\|_0\le k}G(\beta)\le-\max_{v\in\mathcal V_k}|(\Delta^*+\epsilon)^\top Xv|^2min∥β∥0​≤k​G(β)≤−maxv∈Vk​​∣(Δ∗+ϵ)⊤Xv∣2, where Vk\mathcal V_kVk​ is the set of vvv supported off supp⁡(β~∗)\operatorname{supp}(\tilde\beta^*)supp(β~​∗) with ∥v∥0≤k/2\|v\|_0\le k/2∥v∥0​≤k/2 and ∥Xv∥=1\|Xv\|=1∥Xv∥=1.
  4. Lemma 1 (p. 44). Let SSS have qqq elements and let s∈[1,q]s\in[1,q]s∈[1,q] be an integer. Then max⁡∣ϵ⊤Xv∣≳σγ2sslog⁡(eq/s)\max|\epsilon^\top Xv|\gtrsim\sigma\gamma_{2s}\sqrt{s\log(eq/s)}max∣ϵ⊤Xv∣≳σγ2s​slog(eq/s)​ over supp⁡(v)⊆S\operatorname{supp}(v)\subseteq Ssupp(v)⊆S, ∥v∥0≤s\|v\|_0\le s∥v∥0​≤s, ∥Xv∥=1\|Xv\|=1∥Xv∥=1, with probability at least 1−2(eq/s)−c~γ2s2s1-2(eq/s)^{-\tilde c\gamma_{2s}^2s}1−2(eq/s)−c~γ2s2​s.

Significance

Theorem 4 matches the fast-rate upper bound for best subsets from Corollary 1 of the paper. When γk\gamma_kγk​ is bounded below, the prediction error of best subsets is of exact order σ2klog⁡(ep/k)\sigma^2k\log(ep/k)σ2klog(ep/k) in the low-SNR regime (Remark 10). This is the theoretical counterpart of the empirical observation that best subsets overfits at low SNR. It is also what makes the paper's case for shrinkage a theorem rather than a comparison of upper bounds. The paper's Proposition 4 applies it to a concrete correlated design, where it gives a ratio of prediction errors between best subsets and its ℓ2\ell_2ℓ2​-shrunken version that grows with kkk.

The result is proved in the paper; this mission formalizes it. No formalization of this result exists on the platform. The mission also produces a reusable Gaussian lower bound on sparse correlations (Lemma 1) and a deterministic reduction of the best-subsets objective, (39)–(40), which are of independent use for ℓ0\ell_0ℓ0​ estimators.

Difficulty

An upper bound on best subsets follows from comparing β^ℓ0\hat\beta_{\ell_0}β^​ℓ0​​ with β∗\beta^*β∗ in a basic inequality. A lower bound must hold for every minimizer, and β∗\beta^*β∗ itself gives no lower bound. The first idea is to compare with the noiseless fit. It fails because the noise can be fitted by sparse directions, which is exactly the effect to be quantified. The difficult step is Lemma 1. It requires a large set of sparse directions that remain separated after multiplication by XXX, a lower bound on the expected maximum of a Gaussian process over that set, and concentration of that maximum around its mean, with all constants universal. A second subtlety is that the statement is about every minimizer of a nonconvex problem, so the proof has to bound the objective rather than the estimator.

Formalization scope

Vectors are Fin n → ℝ and Fin p → ℝ, with indices starting at 0. The design is X : Matrix (Fin n) (Fin p) ℝ. The Euclidean norm, ℓ1\ell_1ℓ1​ norm, support and ∥⋅∥0\|\cdot\|_0∥⋅∥0​ are explicit definitions, since Mathlib's norm on Fin m → ℝ is the sup norm. γs\gamma_sγs​ is an infimum over the nonzero vectors with ∥u∥0≤s\|u\|_0\le s∥u∥0​≤s; this set is nonempty when p,s≥1p,s\ge1p,s≥1, and every ratio is ≥0\ge0≥0. The noise law is the product of nnn centred Gaussians of variance σ2\sigma^2σ2 on Rn\mathbb R^nRn. "With probability at least 1−η1-\eta1−η" means that a measurable set of noise vectors of probability at least 1−η1-\eta1−η exists on which the conclusion holds. Best subsets is an argmin predicate: Theorem 4 quantifies over every minimizer, and existence is neither assumed nor needed. Universal constants are quantified before every other parameter. "∥⋅∥0≤k/2\|\cdot\|_0\le k/2∥⋅∥0​≤k/2" is a comparison of real numbers.

The model consists of XXX, β∗\beta^*β∗ (with f∗=Xβ∗f^*=X\beta^*f∗=Xβ∗), ϵ\epsilonϵ and its Gaussian law, the estimator (1), and the minimal sparse eigenvalue γs\gamma_sγs​.

Two hypotheses are pinned relative to the printed theorem:

  • k≥2k\ge2k≥2, because the statement is false for k=1k=1k=1. Take every column equal to e1e_1e1​ and β∗=0\beta^*=0β∗=0: the error is ϵ12\epsilon_1^2ϵ12​, while the bound demands order σ2log⁡(ep)\sigma^2\log(ep)σ2log(ep) with probability tending to one.
  • ∥β∗∥0≤k\|\beta^*\|_0\le k∥β∗∥0​≤k, because the proof uses ∥β∗∥1\|\beta^*\|_1∥β∗∥1​, which the printed ℓ2\ell_2ℓ2​ hypothesis controls only for sparse β∗\beta^*β∗, and §3.4 places the theorem in Corollary 1's setting β∗∈B0(k)\beta^*\in B_0(k)β∗∈B0​(k).

The milestones carry neither pin. Because the constants are existential, a formalization in which c0c_0c0​, ccc or CCC may depend on ppp, kkk or XXX would be trivial, and is ruled out by quantifying them first. A version asserting the bound for some minimizer would be weaker than the theorem.

Not formalized here: the upper bounds (Theorems 2, 3, 5), the noise events of Theorem 1, Corollaries 1–6, Propositions 3–4, and the numerical experiments. The proof of the goal also uses Theorem 1's event G2k\mathcal G_{2k}G2k​, which belongs to a separate mission of this series. Proved platform results that a proof of Lemma 1 can use include Sudakov minoration for separated Gaussian families (HighDimProb.RandomProcesses.sudakov_minoration_finite_separated), Gaussian Lipschitz concentration (HighDimStat.TailBounds.lipschitz_gaussian_concentration) and a lower bound on Gaussian maxima (HighDimProb.RandomProcesses.standard_gaussian_max_lower_bound). Contributions are welcome on any milestone, and on supporting lemmas: a packing of sparse sign vectors (Gilbert–Varshamov type), and the approximation of ℓ1\ell_1ℓ1​-bounded vectors by sparse ones.

Selected references

  • R. Mazumder, P. Radchenko, A. Dedieu, Subset Selection with Shrinkage: Sparse Linear Modeling When the SNR Is Low, Operations Research, 2023; preprint arXiv:1708.03288v4, 2022. https://arxiv.org/abs/1708.03288v4
  • D. Bertsimas, A. King, R. Mazumder, Best subset selection via a modern optimization lens, Annals of Statistics 44(2), 2016. https://doi.org/10.1214/15-AOS1388
  • T. Hastie, R. Tibshirani, R. Tibshirani, Best Subset, Forward Stepwise or Lasso? Analysis and Recommendations Based on Extensive Comparisons, Statistical Science 35(4), 2020. https://doi.org/10.1214/19-STS733
  • P. C. Bellec, G. Lecué, A. B. Tsybakov, Slope meets Lasso: improved oracle bounds and optimality, Annals of Statistics 46(6B), 2018. https://doi.org/10.1214/17-AOS1670
  • R. Vershynin, High-Dimensional Probability, Cambridge University Press, 2018. https://doi.org/10.1017/9781108231596
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Contextual Standard Auctions with Budgets: Revenue Equivalence and Efficiency Guarantees 3: Pacing-Based Equilibria Have Liquid Welfare Price of Anarchy at Least 1/2Research Paper

Motivation

Advertising platforms repeatedly sell opportunities to show an advertisement. The opportunity's features, such as audience and placement, affect each advertiser differently, while advertisers limit their average spending. This makes the efficiency of an auction a question about both heterogeneous values and budgets. The paper by Balseiro, Kroer, and Kumar studies this setting with a continuum of buyer types and context-dependent values. It constructs equilibria by value pacing, in which a buyer scales values before bidding. This mission asks how much attainable value those equilibria preserve when budgets cap useful value.

Earlier efficiency bounds for second-price auctions concern a different, non-Bayesian multi-item model. In particular, the half guarantee discussed by Azar and coauthors, as discussed in §5 of the paper uses a no-overbudgeting condition that the present pacing equilibria need not satisfy. Balseiro, Kroer, and Kumar prove their bound under their own contextual and in-expectation budget model; the distinction matters when interpreting the constant. Their existence and revenue-equivalence results also make it possible to speak about the same pacing-based allocation across standard auction payment rules. These claims and the limitation of the earlier assumption are explained in §5 of the paper.

Setting

An item has a context α∈A⊂Rd\alpha\in A\subset\mathbb R^dα∈A⊂Rd, with d≥2d\ge2d≥2. There are n≥2n\ge2n≥2 buyers. Each buyer has a private type θ=(w,B)\theta=(w,B)θ=(w,B): the vector w∈(0,U)dw\in(0,U)^dw∈(0,U)d assigns a positive weight to every context feature, and B∈(Bmin⁡,U)B\in(B_{\min},U)B∈(Bmin​,U) is the buyer's budget, where 0<Bmin⁡<U0<B_{\min}<U0<Bmin​<U. The buyer's value for the item is w⊤αw^\top\alphaw⊤α. A context is drawn from a distribution FFF and buyers' types are drawn independently from a distribution GGG; both distributions have densities. The context and type ranges are the spaces AAA and Θ=(0,U)d×(Bmin⁡,U)\Theta=(0,U)^d\times(B_{\min},U)Θ=(0,U)d×(Bmin​,U) of §2. The reserve price is zero throughout the efficiency section.

A pacing function μ:Θ→R≥0\mu:\Theta\to\mathbb R_{\ge0}μ:Θ→R≥0​ scales type θ\thetaθ's value to w⊤α/(1+μ(θ))w^\top\alpha/(1+\mu(\theta))w⊤α/(1+μ(θ)). Let Hαμ(x)H^\mu_\alpha(x)Hαμ​(x) be the probability that the maximum paced value among n−1n-1n−1 independent competitors is at most xxx. The first-price bid βμ(θ,α)\beta^\mu(\theta,\alpha)βμ(θ,α) applies the paper's bid function σαμ\sigma^\mu_\alphaσαμ​ to the paced value. A buyer may choose a context-dependent bid, subject to an in-expectation budget: expected payment over contexts and competitors must not exceed BBB. The buyer's dual function qμ(θ,t)q^\mu(\theta,t)qμ(θ,t) is the supremum of its Lagrangian over such bids at multiplier t≥0t\ge0t≥0.

The relevant pacing equilibria are fixed points of the correspondence C0∗C_0^*C0∗​. Its domain X0X_0X0​ consists of measurable, integrable pacing functions in [0,ω/Bmin⁡][0,\omega/B_{\min}][0,ω/Bmin​] with total variation at most V0=(d+1)Ud+1ω/Bmin⁡V_0=(d+1)U^{d+1}\omega/B_{\min}V0​=(d+1)Ud+1ω/Bmin​, where ω\omegaω is the supremum of possible values. For a given μ∈X0\mu\in X_0μ∈X0​, C0∗(μ)C_0^*(\mu)C0∗​(μ) minimizes the average dual objective Eθ∼G[qμ(θ,μ^(θ))]\mathbb E_{\theta\sim G}[q^\mu(\theta,\widehat\mu(\theta))]Eθ∼G​[qμ(θ,μ​(θ))] over μ^∈X0\widehat\mu\in X_0μ​∈X0​. These are the objects of §3.3, including its multivariate definition of total variation.

An allocation xxx assigns nonnegative shares xi(α,θ1,…,θn)x_i(\alpha,\theta_1,\ldots,\theta_n)xi​(α,θ1​,…,θn​) summing to one. For buyer iii, keep θi=(wi,Bi)\theta_i=(w_i,B_i)θi​=(wi​,Bi​) fixed while averaging wi⊤α xiw_i^\top\alpha\,x_iwi⊤​αxi​ over the context and the other types. The buyer's liquid welfare is the smaller of this interim value and BiB_iBi​; total liquid welfare LW(x)\mathrm{LW}(x)LW(x) sums its expectation over each buyer's own type. For an equilibrium pacing function μ∈C0∗(μ)\mu\in C_0^*(\mu)μ∈C0∗​(μ), xμx^\muxμ allocates to a highest paced bidder. Definitions 5 and 6 use this allocation to define the worst equilibrium liquid welfare relative to the optimal allocation.

Formalization targets

The main target is the Theorem 3 guarantee, stated for every measurable allocation xxx and every equilibrium pacing function μ\muμ:

LW(xμ)≥12 LW(x).\mathrm{LW}(x^\mu)\ge\tfrac12\,\mathrm{LW}(x).LW(xμ)≥21​LW(x).

The universal comparison expresses the paper's price-of-anarchy bound PoA≥1/2\mathrm{PoA}\ge1/2PoA≥1/2. It leaves no optimum or worst equilibrium as an arbitrary variable. The two milestones are the dual derivative identity and the first-order budget and complementary-slackness conditions stated in §3.2:

∂tqμ(θ,t)=B−payment(bt),payment(bt∗)≤B,t∗(B−payment(bt∗))=0.\partial_t q^\mu(\theta,t)=B-\mathrm{payment}(b_t),\qquad \mathrm{payment}(b_{t^*})\le B,\quad t^*(B-\mathrm{payment}(b_{t^*}))=0.∂t​qμ(θ,t)=B−payment(bt​),payment(bt∗​)≤B,t∗(B−payment(bt∗​))=0.

Here bt(α)=σαμ(w⊤α/(1+t))b_t(\alpha)=\sigma^\mu_\alpha(w^\top\alpha/(1+t))bt​(α)=σαμ​(w⊤α/(1+t)) and t∗t^*t∗ minimizes qμ(θ,⋅)q^\mu(\theta,\cdot)qμ(θ,⋅) over nonnegative multipliers. The milestones are posed in the zero-reserve setting used by the main target.

Significance

The theorem gives an explicit welfare guarantee despite private budgets, correlated values across buyers through a shared context, and equilibrium bidding that depends on those budgets. It applies to the allocation induced by pacing in every standard auction covered by the paper, since those auctions have the same equilibrium allocation even when payment rules differ Balseiro, Kroer, and Kumar, §4–5. Without an efficiency bound, existence of a pacing equilibrium alone would give no quantitative assurance about the allocation it produces.

The result has a mathematical proof in the paper's online appendix; it is an open formalization target here. A complete development would connect measurable Bayesian auctions, the buyer's nonconvex dual problem, the bounded-variation fixed-point domain, and interim liquid welfare. The definitions of interim welfare, dual expenditure, and multivariate variation can support other budgeted auction results. The source PDF held for this mission contains the published main article but not its online appendix, where the proofs and auxiliary lemmas appear.

Difficulty

The expected budget applies to each buyer type after averaging over contexts and opponents, while liquid welfare caps that same type's interim value before averaging over types. Moving the budget cap across the expectation changes the quantity. The natural first-price tie convention also awards the good to every highest bidder for the buyer optimization problem, while a welfare allocation must give total share one. The proof must reconcile the dual account of expenditure with a feasible allocation and preserve these different orders of expectation. The dual objective is a supremum over bids, so its derivative cannot be obtained merely by differentiating a chosen closed formula without justifying that formula and the maximizing bid.

Formalization scope

Lean represents a context by Fin d → ℝ and a buyer type by its weight vector and real budget. Value is the explicit finite sum ∑iwiαi\sum_i w_i\alpha_i∑i​wi​αi​. The model requires a nonempty bounded measurable context set in the positive orthant, absolutely continuous probability laws FFF and GGG supported on their stated domains, measurable reserves and pacing, n≥2n\ge2n≥2, and 0<Bmin⁡<U0<B_{\min}<U0<Bmin​<U. Boundedness of AAA makes ω\omegaω finite; these conditions make the domain and integrals implicit in the article well posed. The welfare target assumes zero reserves as §5 does.

Admissible bids are measurable and nonnegative on AAA, with integrable expected payment. The dual is defined by its supremum over bids. Total variation is extended-real-valued and uses Euclidean lengths of test fields; thus infinite variation cannot satisfy the X0X_0X0​ bound through a real supremum's default value. Allocations are measurable and simplex-valued on the model domain. At a tied highest bid, xμx^\muxμ splits the item equally; ties have probability zero under these equilibria, as the paper states by its appendix Lemma 6(d). The closed simplex permits zero shares, correcting the paper's notation R+\mathbb R_+R+​ in Definition 5, which §2.1 otherwise calls strictly positive. The universal welfare inequality avoids default real infimum and supremum values on pathological sets. Contributions to the measurable bidding, variation, duality, and welfare infrastructure are all useful within this scope.

Selected references

  • Santiago R. Balseiro, Christian Kroer, and Rachitesh Kumar, Contextual Standard Auctions with Budgets: Revenue Equivalence and Efficiency Guarantees, Management Science, Articles in Advance, 2023. DOI: 10.1287/mnsc.2023.4719.
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Contextual Standard Auctions with Budgets: Revenue Equivalence and Efficiency Guarantees 2: Value Pacing Is an Equilibrium of Every Standard Auction with the Same Expected PaymentsResearch Paper

Motivation

Online advertising sells billions of impressions a day through auctions, and most advertisers do not bid by hand: they hand a budget to the platform, which paces their bids so that spending over a campaign matches the budget. Over the last decade the major ad exchanges moved from second price to first price auctions. An advertiser who has tuned a pacing policy for one format wants to know whether it still works after the switch, and a platform wants to know whether its revenue changes.

Classical revenue equivalence (Myerson 1981; Riley and Samuelson 1981) says that, with independent private values, risk-neutral buyers and no budgets, every standard auction yields the same expected revenue. Che and Gale (1998) showed that this fails when budgets are hard: first price auctions then raise more revenue than second price auctions. Balseiro, Kroer and Kumar (2023) study budgets that bind in expectation over many auctions, with values driven by item features, and show that equivalence is restored. This mission formalizes that result, their Theorem 2.

Setting

An item has a context α∈A⊂R+d\alpha\in A\subset\mathbb R^d_+α∈A⊂R+d​ drawn from a law FFF with a density. Each of nnn buyers has a type θ=(w,B)\theta=(w,B)θ=(w,B) drawn independently from a law GGG with a density on Θ=(0,U)d×(Bmin⁡,U)\Theta=(0,U)^d\times(B_{\min},U)Θ=(0,U)d×(Bmin​,U). Here www are feature weights and BBB is a budget. The buyer's value for the item is wTαw^T\alphawTα, and ω\omegaω is the supremum of all values. The seller discloses α\alphaα, then runs an auction with reserve price r(α)r(\alpha)r(α). A buyer must keep its expected payment, over contexts and competitors' types, at most BBB.

A pacing function μ:Θ→R≥0\mu:\Theta\to\mathbb R_{\ge0}μ:Θ→R≥0​ shades every value to the paced value wTα/(1+μ(w,B))w^T\alpha/(1+\mu(w,B))wTα/(1+μ(w,B)). Let λαμ\lambda^\mu_\alphaλαμ​ be the law of the paced value when (w,B)∼G(w,B)\sim G(w,B)∼G, and Hαμ(x)=λαμ((−∞,x])n−1H^\mu_\alpha(x)=\lambda^\mu_\alpha((-\infty,x])^{n-1}Hαμ​(x)=λαμ​((−∞,x])n−1 the c.d.f. of the highest of n−1n-1n−1 independent paced values. In first price auctions the paper's candidate strategy is βμ(w,B,α)=σαμ(wTα/(1+μ(w,B)))\beta^\mu(w,B,\alpha)=\sigma^\mu_\alpha(w^T\alpha/(1+\mu(w,B)))βμ(w,B,α)=σαμ​(wTα/(1+μ(w,B))), where σαμ\sigma^\mu_\alphaσαμ​ is the first-price equilibrium bid against paced competitors.

The buyer's dual function qμ(w,B,t)q^\mu(w,B,t)qμ(w,B,t) is the supremum over bid functions b(⋅)b(\cdot)b(⋅) of the Lagrangian E[(wTα−(1+t)b(α))1{win}]+tB\mathbb E[(w^T\alpha-(1+t)b(\alpha))\mathbb 1\{\text{win}\}]+tBE[(wTα−(1+t)b(α))1{win}]+tB, with competitors bidding βμ\beta^\muβμ. The set X0\mathcal X_0X0​ collects pacing functions with values in [0,ω/Bmin⁡][0,\omega/B_{\min}][0,ω/Bmin​] and total variation at most V0=(d+1)Ud+1ω/Bmin⁡V_0=(d+1)U^{d+1}\omega/B_{\min}V0​=(d+1)Ud+1ω/Bmin​. The correspondence C0∗(μ)C^*_0(\mu)C0∗​(μ) is the set of minimizers over X0\mathcal X_0X0​ of μ^↦EG[qμ(w,B,μ^(w,B))]\hat\mu\mapsto\mathbb E_G[q^\mu(w,B,\hat\mu(w,B))]μ^​↦EG​[qμ(w,B,μ^​(w,B))]. A fixed point μ∈C0∗(μ)\mu\in C^*_0(\mu)μ∈C0∗​(μ) is an equilibrium pacing function for first price auctions.

An anonymous standard auction Aα=(r(α),Mα)\mathcal A_\alpha=(r(\alpha),M_\alpha)Aα​=(r(α),Mα​) gives the item to the highest bid at or above the reserve. Its payment Mα(b,{bi})M_\alpha(b,\{b_i\})Mα​(b,{bi​}) for a bid bbb against competing bids bib_ibi​ does not depend on the buyers' identities. An oracle returns, for each atomless value law H\mathcal HH on [0,ω][0,\omega][0,ω], a single-auction equilibrium bid ψαH\psi^{\mathcal H}_\alphaψαH​ that is nondecreasing, meets the reserve exactly for values above it, gives a zero-value bidder zero payoff, and has an atomless bid law. The candidate strategy is

Ψμ(w,B,α)=ψαλαμ(wTα1+μ(w,B)).\Psi^\mu(w,B,\alpha)=\psi^{\lambda^\mu_\alpha}_\alpha\Big(\frac{w^T\alpha}{1+\mu(w,B)}\Big).Ψμ(w,B,α)=ψαλαμ​​(1+μ(w,B)wTα​).

Formalization targets

Goal: Theorem 2 (Revenue and Pacing Equivalence)

For every family {Aα}\{\mathcal A_\alpha\}{Aα​} of anonymous standard auctions with such an oracle and every μ∈X0\mu\in\mathcal X_0μ∈X0​ with μ∈C0∗(μ)\mu\in C^*_0(\mu)μ∈C0∗​(μ):

  1. Ψμ\Psi^\muΨμ is a symmetric equilibrium of the family (Definition 4): almost every buyer type maximizes expected utility subject to its expected budget by bidding Ψμ\Psi^\muΨμ when everyone else does;
  2. for every θ∈Θ\theta\in\Thetaθ∈Θ,
E[Mα(Ψμ(θ,α),{Ψμ(θi,α)}i)]=E[βμ(θ,α) 1{βμ(θ,α)≥max⁡(r(α),{βμ(θi,α)}i)}].\mathbb E\big[M_\alpha(\Psi^\mu(\theta,\alpha),\{\Psi^\mu(\theta_i,\alpha)\}_i)\big]=\mathbb E\big[\beta^\mu(\theta,\alpha)\,\mathbb 1\{\beta^\mu(\theta,\alpha)\ge\max(r(\alpha),\{\beta^\mu(\theta_i,\alpha)\}_i)\}\big].E[Mα​(Ψμ(θ,α),{Ψμ(θi​,α)}i​)]=E[βμ(θ,α)1{βμ(θ,α)≥max(r(α),{βμ(θi​,α)}i​)}].

Milestones

  • §3.2, p. 8, last display. For t≥0t\ge0t≥0 and xα=wTα/(1+t)x_\alpha=w^T\alpha/(1+t)xα​=wTα/(1+t),
qμ(w,B,t)=(1+t) Eα[1{xα≥r(α)}∫r(α)xαHαμ(s) ds]+tB.q^\mu(w,B,t)=(1+t)\,\mathbb E_\alpha\Big[\mathbb 1\{x_\alpha\ge r(\alpha)\}\int_{r(\alpha)}^{x_\alpha}H^\mu_\alpha(s)\,ds\Big]+tB.qμ(w,B,t)=(1+t)Eα​[1{xα​≥r(α)}∫r(α)xα​​Hαμ​(s)ds]+tB.
  • §4, p. 12, key step. When the competitors bid Ψμ\Psi^\muΨμ, the dual function of the buyer's problem in any standard auction family equals qμ(w,B,t)q^\mu(w,B,t)qμ(w,B,t).

Significance

Theorem 2 says that pacing is portable: an equilibrium pacing function computed for first price auctions is an equilibrium pacing function for second price auctions, all-pay auctions, or any context-dependent mixture of standard formats. Each buyer's expected spend is the same in all of them, so the seller's expected revenue is too. This explains why budget-management systems built for second price auctions keep working after a move to first price. It also separates in-expectation budgets, where equivalence holds, from the hard budgets of Che and Gale, where it fails. Theorem 3 of the same paper, a liquid-welfare price of anarchy of 1/21/21/2, uses Theorem 2 to argue in the second price auction.

The paper's proofs are in its online appendix, which is not part of the source this mission cites. To our knowledge no part of the argument has been machine-checked. Classical revenue equivalence for incentive-compatible direct mechanisms without budgets exists on the platform as other items, but none has pacing, budgets or contexts. The mission asks for a machine-checked proof of Theorem 2 and of the two steps the authors name.

Difficulty

The classical argument pins payments by the allocation rule and the envelope formula, value by value. Here a buyer's decision is a whole bid function of the context, coupled across contexts by one budget constraint, and the budget-constrained problem is not convex. So the envelope argument cannot be applied to the constrained problem directly. The obvious move, Lagrangian relaxation, needs strong duality for a non-convex problem, and it needs the dual of each standard auction to agree with the first-price dual for every multiplier, not only at the optimum. The paced value laws λαμ\lambda^\mu_\alphaλαμ​ need not have densities, so the textbook single-auction results, which assume a positive density, do not apply verbatim. Finally, the fixed-point hypothesis ties all buyer types together, and optimality must be recovered almost surely in the type.

Formalization scope

Everything is defined in the namespace ContextualAuctions.RevEquiv. Contexts are Fin d → ℝ, types are (Fin d → ℝ) × ℝ, and wTαw^T\alphawTα is an explicit sum. The joint law of the context and the n−1n-1n−1 competitor types is F.prod (Measure.pi fun _ => G). Ties win, as in the paper's tie-breaking rule. The standing assumptions are d≥2d\ge2d≥2, FFF and GGG probability measures with densities concentrated on AAA and Θ\ThetaΘ, AAA in the open positive orthant, and rrr measurable. Disclosed additions, implicit in the paper:

  • n≥2n\ge2n≥2 and 0<Bmin⁡<U0<B_{\min}<U0<Bmin​<U;
  • AAA measurable, nonempty and bounded, so that ω<∞\omega<\inftyω<∞;
  • pacing functions and bids are measurable; first-price bids are nonnegative on AAA, and standard-auction bids are nonnegative for almost every context, because the oracle constrains Ψμ\Psi^\muΨμ only where λαμ\lambda^\mu_\alphaλαμ​ is atomless;
  • the payment rule is measurable along measurable bid maps on any measurable space;
  • the strategy Ψμ\Psi^\muΨμ is jointly measurable, since the oracle is a black box.

The dual function is the supremum over admissible bids, which are measurable with integrable payment. Its closed form is a milestone and never its definition. Total variation (Definition 3) is extended-real valued and uses the Euclidean norm of the test field. In oracle property 1, expected payments are taken in [0,∞][0,\infty][0,∞], so a bid with infinite expected payment can never look free. The payment identity of Theorem 2 is stated in [0,∞][0,\infty][0,∞], so it also asserts that the left side is finite. This rules out the trivializing readings: a closed-form definition of qμq^\muqμ that makes the first milestone hold by definition, Bochner junk zeros for non-integrable payments, and a vacuous variation bound.

A complete development needs single-auction revenue equivalence for i.i.d. atomless value laws without densities. It also needs the measure-theoretic interchange of a supremum over bid functions with the expectation over contexts, and strong duality for the budget-constrained problem. These pieces, notably the single-auction equivalence for general atomless laws, are reusable beyond this mission. Contributions toward any of them are welcome.

Selected references

  • S. Balseiro, C. Kroer, R. Kumar, Contextual Standard Auctions with Budgets: Revenue Equivalence and Efficiency Guarantees, Management Science, Articles in Advance, 2023. https://doi.org/10.1287/mnsc.2023.4719
  • Y.-K. Che, I. Gale, Standard Auctions with Financially Constrained Bidders, Review of Economic Studies 65(1), 1998. https://doi.org/10.1111/1467-937X.00041
  • R. Myerson, Optimal Auction Design, Mathematics of Operations Research 6(1), 1981. https://doi.org/10.1287/moor.6.1.58
  • J. Riley, W. Samuelson, Optimal Auctions, American Economic Review 71(3), 1981. https://www.jstor.org/stable/1802779
  • V. Krishna, Auction Theory, 2nd ed., Academic Press, 2009. https://doi.org/10.1016/C2009-0-22474-3
  • S. Balseiro, Y. Gur, Learning in Repeated Auctions with Budgets: Regret Minimization and Equilibrium, Management Science 65(9), 2019. https://doi.org/10.1287/mnsc.2018.3174
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