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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.

≥ 2.131125302137Formalized record→≥ 2.15Open frontier
10 provers on it19 of 20 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→≤ 1.9202796Open frontier
4 provers on it7 of 8 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
18 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.
≤ 12Formalized record→≤ 2Open frontier
7 provers on it14 of 15 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.

≤ 23Formalized record→≤ 5Open frontier
40 provers on it15 of 17 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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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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Bandit AlgorithmsMachine LearningOperations Research+1·Captain: mikedeng1

Thompson Sampling with Information Relaxation Penalties III: As T → ∞ the Action Laws of IRS.FH and IRS.V-Zero Converge to That of Thompson SamplingResearch Paper

Motivation

Thompson sampling (TS) is the standard randomized heuristic for the Bayesian multi-armed bandit: at each decision it samples a parameter vector from the current posterior and pulls the arm that would be best if the sample were true. It ignores the remaining horizon. Min, Maglaras and Moallemi (arXiv:1902.04251, Management Science, 2025) obtain horizon-aware generalizations of TS from the information relaxation duality of Brown, Smith and Sun (Oper. Res. 2010). Each penalty function yields an upper bound on the Bayes-optimal value and an IRS policy. Such a policy samples a whole future outcome and plays the first action of the penalized clairvoyant optimum. With the zero-information penalty it is exactly TS.

Two of these policies, IRS.FH and IRS.V-Zero, are designed to interpolate between TS and the myopic rule. When one period remains they pull the arm with the highest predictive mean (Remark 5 of the paper). This mission formalizes the other end, Proposition 1: when many periods remain, they randomize exactly as Thompson sampling does. The paper presents this as the sense in which IRS policies "behave like TS during the initial decision epochs" and shift smoothly from exploration to exploitation without a tuning parameter.

Setting

There are K≥1K \ge 1K≥1 arms A={1,…,K}\mathcal A = \{1,\dots,K\}A={1,…,K}. Arm aaa has an unknown parameter θa\theta_aθa​. Given θa\theta_aθa​, its rewards Ra,1,Ra,2,…R_{a,1}, R_{a,2}, \dotsRa,1​,Ra,2​,… are i.i.d. with law Ra(θa)\mathcal R_a(\theta_a)Ra​(θa​). The prior of θa\theta_aθa​ is Pa(ya)\mathcal P_a(y_a)Pa​(ya​), a member of a conjugate family indexed by a belief yay_aya​. A Bayesian update Ua\mathcal U_aUa​ maps (ya,r)(y_a, r)(ya​,r) to the posterior belief after a reward rrr. The arms are independent. Throughout, rewards are integrable: Eya∣Ra,1∣<∞\mathbb E_{y_a}|R_{a,1}| < \inftyEya​​∣Ra,1​∣<∞ for every belief (display (3)).

  • The conditional mean reward is μa(θa)=E[Ra,n∣θa]\mu_a(\theta_a) = \mathbb E[R_{a,n} \mid \theta_a]μa​(θa​)=E[Ra,n​∣θa​], and the predictive mean is μˉa(ya)=Eya[μa(θa)]\bar\mu_a(y_a) = \mathbb E_{y_a}[\mu_a(\theta_a)]μˉ​a​(ya​)=Eya​​[μa​(θa​)].
  • The outcome ω=(θ,(Ra,n)a,n)\omega = (\theta, (R_{a,n})_{a,n})ω=(θ,(Ra,n​)a,n​) has law I(y)\mathcal I(y)I(y).
  • The posterior predictive mean after the first nnn rewards of arm aaa is μ^a,n(ω;ya)=Eya[μa(θa)∣Ra,1,…,Ra,n]\hat\mu_{a,n}(\omega; y_a) = \mathbb E_{y_a}[\mu_a(\theta_a) \mid R_{a,1},\dots,R_{a,n}]μ^​a,n​(ω;ya​)=Eya​​[μa​(θa​)∣Ra,1​,…,Ra,n​].

At remaining horizon TTT and belief yyy, the three policies act as follows:

  1. TS samples θ~∼P(y)\tilde\theta \sim \mathcal P(y)θ~∼P(y) and plays ATS(y)=argmax⁡aμa(θ~a)A^{TS}(y) = \operatorname{argmax}_a \mu_a(\tilde\theta_a)ATS(y)=argmaxa​μa​(θ~a​).
  2. IRS.FH samples ω~∼I(y)\tilde\omega \sim \mathcal I(y)ω~∼I(y) and plays AIRS.FH(T,y)=argmax⁡aμ^a,T−1(ω~)A^{IRS.FH}(T,y) = \operatorname{argmax}_a \hat\mu_{a,T-1}(\tilde\omega)AIRS.FH(T,y)=argmaxa​μ^​a,T−1​(ω~), the arm with the best posterior mean after T−1T-1T−1 sampled rewards of every arm.
  3. IRS.V-Zero samples ω~∼I(y)\tilde\omega \sim \mathcal I(y)ω~∼I(y) and solves the allocation problem
max⁡n∈NT∑a=1K∑i=1naμ^a,i−1(ω~),NT={n∈N0K:∑ana=T}.\max_{n \in \mathcal N_T} \sum_{a=1}^K \sum_{i=1}^{n_a} \hat\mu_{a,i-1}(\tilde\omega), \qquad \mathcal N_T = \Big\{n \in \mathbb N_0^K : \sum_a n_a = T\Big\}.n∈NT​max​a=1∑K​i=1∑na​​μ^​a,i−1​(ω~),NT​={n∈N0K​:a∑​na​=T}.

It then plays the arm AIRS.V-Zero(T,y)=argmax⁡an~a∗A^{IRS.V\text{-}Zero}(T,y) = \operatorname{argmax}_a \tilde n^*_aAIRS.V-Zero(T,y)=argmaxa​n~a∗​ to which the optimal allocation n~∗\tilde n^*n~∗ assigns the most pulls.

Each action is a random variable driven by the policy's own sample.

Formalization targets

Goal: Proposition 1 (p. 25)

Assume μi(θi)≠μj(θj)\mu_i(\theta_i) \ne \mu_j(\theta_j)μi​(θi​)=μj​(θj​) almost surely under P(y)\mathcal P(y)P(y), for all i≠ji \ne ji=j. Then for every arm aaa,

lim⁡T→∞P[AIRS.FH(T,y)=a]=P[ATS(y)=a],lim⁡T→∞P[AIRS.V-Zero(T,y)=a]=P[ATS(y)=a].\lim_{T\to\infty} \mathbb P[A^{IRS.FH}(T,y) = a] = \mathbb P[A^{TS}(y) = a], \qquad \lim_{T\to\infty} \mathbb P[A^{IRS.V\text{-}Zero}(T,y) = a] = \mathbb P[A^{TS}(y) = a].T→∞lim​P[AIRS.FH(T,y)=a]=P[ATS(y)=a],T→∞lim​P[AIRS.V-Zero(T,y)=a]=P[ATS(y)=a].

This holds for every choice of the tie-breaking rules in the argmaxes and in the allocation problem.

Milestones

  1. Proposition 4 (p. 53): μa(θa)\mu_a(\theta_a)μa​(θa​) and max⁡aμa(θa)\max_a \mu_a(\theta_a)maxa​μa​(θa​) are integrable under the prior.
  2. Proposition 5 (p. 54): μ^a,n\hat\mu_{a,n}μ^​a,n​ and the sample mean 1n∑i≤nRa,i\frac1n\sum_{i\le n} R_{a,i}n1​∑i≤n​Ra,i​ converge almost surely to μa(θa)\mu_a(\theta_a)μa​(θa​).
  3. Display (109) (p. 54): if a sequence of vectors converges to a vector with distinct entries, every argmax rule eventually selects the argmax of the limit.
  4. The allocation argument (113)–(123) (pp. 54–56): if the payoff rows converge to distinct limits, then for large TTT every optimal allocation gives its largest share only to the arm with the largest limit.
  5. Display (55) alone: the IRS.FH half of the goal.

Significance

Proposition 1 identifies the long-horizon behaviour of the two IRS policies with that of Thompson sampling. Together with Remark 5 it pins down both ends of the horizon. It explains why their simulated regret curves track TS early and the myopic policy late (§5 of the paper). It also shows that the design choice "play the arm with the largest allocation" in IRS.V-Zero is the one that recovers TS. Other selection rules, such as any arm with a positive allocation, need not.

The paper gives a complete proof in Appendix D.1–D.2. A machine-checked version adds three things. It fixes the probabilistic model of a conjugate Bayesian bandit with infinite reward sequences in Lean, which the companion missions on the same paper also need. It makes the role of tie-breaking explicit. And it repairs a step of the printed proof: the bound n∘(AT∘)≥⌊T/2⌋n^\circ(A^\circ_T) \ge \lfloor T/2 \rfloorn∘(AT∘​)≥⌊T/2⌋ in §D.2 holds only for two arms, and the general case needs ⌈T/K⌉\lceil T/K \rceil⌈T/K⌉ and a threshold growing with KKK. No formalization of this result is known on Prove2Me or in Mathlib.

Difficulty

The IRS.FH half reduces to almost-sure convergence of posterior means, which is a martingale argument (Lévy's upward theorem). That argument needs μa(θa)\mu_a(\theta_a)μa​(θa​) to be measurable with respect to the limit σ\sigmaσ-algebra of the reward sequence, a fact supplied by the strong law of large numbers. Building the outcome law, a mixture over θ\thetaθ of infinite product measures, and identifying the conjugate update with conditional expectation are where the measure theory lies.

The IRS.V-Zero half does not follow from convergence of the posterior means alone. The selected arm is a function of an optimal allocation of a combinatorial problem whose size grows with TTT. The naive expectation that the arm with the best limit receives "most" pulls has to be proved by an exchange argument that handles the finitely many early terms, where the posterior means can still be badly ordered. The printed version of this argument is correct only for K=2K = 2K=2.

Formalization scope

  • Arms are Fin K with NeZero K; the reward sequence of an arm is ℕ → ℝ, 0-based.
  • One parameter type and one belief type serve all arms; reward laws and priors are Markov kernels.
  • Conjugacy is stated as Bayes' rule on rectangles for every belief. The update is assumed jointly measurable, and the standing integrability (3) is assumed for every belief.
  • The outcome law I(y)\mathcal I(y)I(y) is a product over arms of mixtures ∫δθ⊗Ra(θ)⊗N Pa(ya)(dθ)\int \delta_\theta \otimes \mathcal R_a(\theta)^{\otimes \mathbb N}\, \mathcal P_a(y_a)(d\theta)∫δθ​⊗Ra​(θ)⊗NPa​(ya​)(dθ).
  • μ^a,n\hat\mu_{a,n}μ^​a,n​ is the pathwise conjugate version μˉa(ya,n)\bar\mu_a(y_{a,n})μˉ​a​(ya,n​) of the conditional expectation (10), defined at every outcome so that it can sit inside an argmax.
  • P[A=a]\mathbb P[A = a]P[A=a] is the mass of {a}\{a\}{a} under the pushforward of the policy's sampling law. All tie-breaking rules are required to be measurable; otherwise the pushforward would be the zero measure.
  • The assumption of the proposition is required almost surely under the prior, not as injectivity of μ\muμ.
  • A formalization in which the selectors were non-measurable, the outcome law degenerate, or the distinctness hypothesis unsatisfiable would make the goal vacuous. The definitions rule out the first two, and a deterministic two-arm instance shows the hypotheses are satisfiable.

The development needs Lévy's upward theorem (MeasureTheory.tendsto_ae_condExp in Mathlib) and the strong law of large numbers (ProbabilityTheory.strong_law_ae). It also needs a lemma identifying iterated conjugate updates with the posterior given finitely many rewards, and the measurability of θ↦Ra(θ)⊗N\theta \mapsto \mathcal R_a(\theta)^{\otimes\mathbb N}θ↦Ra​(θ)⊗N. These last two are reusable for any Bayesian bandit or sequential-estimation development. Contributions of the two deterministic milestones are self-contained and welcome first.

Selected references

  • S. Min, C. Maglaras, C. C. Moallemi, Thompson Sampling with Information Relaxation Penalties, Management Science, 2025; preprint arXiv:1902.04251v2, 2021. https://arxiv.org/abs/1902.04251
  • D. B. Brown, J. E. Smith, P. Sun, Information Relaxations and Duality in Stochastic Dynamic Programs, Operations Research 58(4), 2010. https://doi.org/10.1287/opre.1090.0796
  • W. R. Thompson, On the Likelihood that One Unknown Probability Exceeds Another in View of the Evidence of Two Samples, Biometrika 25(3/4), 1933. https://doi.org/10.2307/2332286
  • D. Russo, B. Van Roy, Learning to Optimize via Posterior Sampling, Mathematics of Operations Research 39(4), 2014. https://doi.org/10.1287/moor.2014.0650
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Algorithmic Game TheoryMechanism Design·Captain: mikedeng1

Round-Robin Beyond Additive Agents: Existence and Fairness of Approximate Equilibria 3: For Submodular Valuations Every α-Approximate Pure Nash Equilibrium of Round-Robin Is α/3-EF1Research Paper

Motivation

Round-Robin is the simplest allocation rule for indivisible goods: agents take turns, in a fixed order, picking their favourite remaining good. When agents have additive valuations and report them truthfully, the outcome is envy-free up to one good (EF1) — every agent values its own bundle at least as much as any other bundle with one good removed, a notion going back to Lipton et al., 2004 and Budish (2011) — which makes Round-Robin a standard baseline in fair division (Markakis, 2017). The mechanism, however, only sees reported rankings, and agents can gain by misreporting; without monetary transfers no truthful mechanism has a meaningful fairness guarantee even for two additive agents. Amanatidis, Birmpas, Lazos, Leonardi and Reiffenhäuser (arXiv:2301.13652, Mathematics of Operations Research, 2025) therefore study equilibrium fairness of Round-Robin when valuations go beyond additive. This mission concerns their fairness result for submodular valuations: strategic play does not destroy fairness, it only degrades it by a constant factor.

Timeline. Aziz, Goldberg and Walsh (ADT 2017) proved that Round-Robin always has a pure Nash equilibrium for additive valuations. Amanatidis et al. (WINE 2021) initiated the study of equilibrium fairness and showed that, for additive valuations, Round-Robin has equilibria and each of them yields an EF1 allocation with respect to the true valuations. The 2023 paper extends equilibrium existence to cancelable valuations (exact PNE) and submodular valuations (1/2-approximate PNE, with 1/2 tight), and proves that approximate equilibria are approximately EF1: factor α/3\alpha/3α/3 for submodular and α/2\alpha/2α/2 for subadditive cancelable valuations.

Setting

There are n≥1n\ge1n≥1 agents and a set MMM of mmm goods. Agent iii has a valuation vi:2M→Rv_i:2^M\to\mathbb Rvi​:2M→R that is normalized (vi(∅)=0v_i(\emptyset)=0vi​(∅)=0) and non-decreasing. The marginal value of a good ggg with respect to a set SSS is vi(g∣S)=vi(S∪{g})−vi(S)v_i(g\mid S)=v_i(S\cup\{g\})-v_i(S)vi​(g∣S)=vi​(S∪{g})−vi​(S), and viv_ivi​ is submodular if vi(g∣S)≥vi(g∣T)v_i(g\mid S)\ge v_i(g\mid T)vi​(g∣S)≥vi​(g∣T) whenever S⊆TS\subseteq TS⊆T and g∉Tg\notin Tg∈/T.

Each agent reports a ranking ≻i\succ_i≻i​, a total order on MMM. Round-Robin(≻)(\succ)(≻) runs mmm steps; in step ttt (counted from 000) agent t mod nt\bmod ntmodn receives its ≻\succ≻-top good among those still unallocated. The result is an allocation (A1,…,An)(A_1,\dots,A_n)(A1​,…,An​). An allocation is α\alphaα-EF1 if for all agents i,ji,ji,j with Aj≠∅A_j\ne\emptysetAj​=∅ some g∈Ajg\in A_jg∈Aj​ satisfies vi(Ai)≥α vi(Aj∖{g})v_i(A_i)\ge\alpha\, v_i(A_j\setminus\{g\})vi​(Ai​)≥αvi​(Aj​∖{g}). A profile ≻\succ≻ is an α\alphaα-approximate pure Nash equilibrium (PNE) if no agent iii can, by reporting any other ranking ≻i′\succ'_i≻i′​, obtain a bundle worth more than 1/α1/\alpha1/α times its current one:

α⋅vi(RR(≻i′,≻−i)i)≤vi(RR(≻)i).\alpha\cdot v_i\big(\text{RR}(\succ'_i,\succ_{-i})_i\big)\le v_i\big(\text{RR}(\succ)_i\big).α⋅vi​(RR(≻i′​,≻−i​)i​)≤vi​(RR(≻)i​).

In Lean the objects are marginal, IsValuation, IsSubmodular, IsRanking, roundRobin, IsApproxEF1 and IsApproxPNE in RoundRobinEq.SubmodularEF1.Setting; the step-to-agent map agentAt n t = t % n comes from the shared module RoundRobinEq.CancelableBluff.Setting.

Formalization targets

Goal: Theorem 4.4

For α∈(0,1]\alpha\in(0,1]α∈(0,1] and submodular valuations, every α\alphaα-approximate PNE ≻\succ≻ of Round-Robin yields an allocation that is α/3\alpha/3α/3-EF1 with respect to the true valuations:

∀i,j, Aj≠∅ ⇒ ∃g∈Aj:  vi(Ai) ≥ α3 vi(Aj∖{g}).\forall i,j,\ A_j\ne\emptyset\ \Rightarrow\ \exists g\in A_j:\ \ v_i(A_i)\ \ge\ \tfrac{\alpha}{3}\, v_i(A_j\setminus\{g\}).∀i,j, Aj​=∅ ⇒ ∃g∈Aj​:  vi​(Ai​) ≥ 3α​vi​(Aj​∖{g}).

Milestones

  1. Theorem 2.1 (Nemhauser–Wolsey–Fisher): vvv is non-decreasing submodular iff v(T)≤v(S)+∑g∈T∖Sv(g∣S)v(T)\le v(S)+\sum_{g\in T\setminus S}v(g\mid S)v(T)≤v(S)+∑g∈T∖S​v(g∣S) for all S,TS,TS,T.
  2. Lemma 4.6: if agent iii deviates, at most r−1r-1r−1 of the goods allocated before its rrr-th turn in the deviation run are still unallocated at that point of the original run.
  3. Lemma 4.7: in the original allocation, no agent holds more than 2(r−1)2(r-1)2(r−1) of the goods the deviation run allocates between iii's first and rrr-th turns.
  4. The parity split: splitting another agent's bundle (minus its first good) into odd- and even-indexed halves Y1,Y2Y_1,Y_2Y1​,Y2​, each half meets that set in at most r−1r-1r−1 goods.
  5. Inequality (2): agent iii's greedy deviation dominates, good by good and marginally, each half YℓY_\ellYℓ​ renamed by Algorithm 3.
  6. The closing bound vi(Aj∖{y1})≤3αvi(Ai)v_i(A_j\setminus\{y_1\})\le \tfrac3\alpha v_i(A_i)vi​(Aj​∖{y1​})≤α3​vi​(Ai​).

Companions (not milestones): Lemma 4.1 (the greedy response is 1/2-EF1 from the deviator's perspective) and Theorem 4.2 (two agents: α/2\alpha/2α/2).

Significance

The theorem says that fairness of Round-Robin is robust to strategic misreporting for a class far beyond additive valuations: whatever approximate equilibrium agents settle in, each agent's envy up to one good is bounded by 3/α3/\alpha3/α. Combined with the existence of a 1/2-approximate PNE (Theorem 3.7 of the same paper), it gives an equilibrium that is 1/6-EF1. Lemmas 4.6 and 4.7 are statements about two runs of Round-Robin that differ in one agent's report; they involve no valuations and are reused verbatim for subadditive cancelable valuations (Theorem 4.5).

The result is proved in the paper; nothing in it is formalized anywhere to our knowledge. The mission builds a finite fair-division layer (Round-Robin as a step-by-step process, rankings, α-EF1, approximate PNE) that does not exist in Mathlib, and checks the combinatorial coupling of two runs, which is where the paper's argument carries its weight.

Difficulty

The obvious argument compares agent iii's equilibrium bundle with its bundle after a good deviation (Algorithm 4's greedy response) and then compares that with agent jjj's bundle. With two agents everything not in AiA_iAi​ or Ai′A'_iAi′​ goes to jjj, and this closes the argument. With nnn agents the deviation reshuffles goods among all other agents, and there is no direct control on what jjj ends up holding relative to the deviation run. The proof needs a global statement (Lemma 4.6) about how much two Round-Robin runs that differ in one report can diverge before each of iii's turns, and then a careful indexing of AjA_jAj​ by allocation time in the other run, so that a counting bound turns into the good-by-good inequality (2). The bookkeeping of steps, rounds and two simultaneous runs is the main work.

Formalization scope

  • Agents are Fin n with n≥1n\ge1n≥1, 0-based; goods a finite type M. The paper's standing simplification m=knm=knm=kn (p. 7) is a hypothesis Fintype.card M = k * n of every theorem; the paper's reduction to this case (dummy goods) is not formalized.
  • Valuations are real-valued, normalized and non-decreasing (non-negativity follows); submodularity is the marginal form of p. 5.
  • Rankings are duplicate-free lists of all goods; deviations in the PNE hypothesis range over rankings only, and α∈(0,1]\alpha\in(0,1]α∈(0,1] is carried explicitly.
  • Steps and rounds are 0-based: the paper's SrS_rSr​ is allocBefore σ (r*n + i), and the paper's bounds r−1r-1r−1 for Sr−1′S'_{r-1}Sr−1′​, r∈[k]r\in[k]r∈[k], appear as rrr for r<kr<kr<k.
  • Algorithms 3 and 4 are encoded relationally (any tie-breaking); a statement for all relational solutions is at least as strong as the paper's.
  • Lemmas 4.6, 4.7 and the parity split are stated for an arbitrary deviating ranking, without valuations; inequality (2) is stated for an arbitrary set function and without the equilibrium hypothesis. These are disclosed strengthenings.

Trivializing formalizations are excluded: deviations over arbitrary lists (which would strengthen the hypothesis), α≤0\alpha\le0α≤0, EF1 computed on reported rankings instead of the true valuations, or the EF1 witness fixed in the goal statement would each change the theorem, and none is used.

Contributions welcome: proofs of Lemma 4.6 by induction on rounds (the reusable core), basic API for allocBefore/roundRobin (every good is allocated once, ∣Ai∣=k|A_i|=k∣Ai​∣=k), and Theorem 2.1.

Selected references

  • G. Amanatidis, G. Birmpas, P. Lazos, S. Leonardi, R. Reiffenhäuser, Round-Robin Beyond Additive Agents: Existence and Fairness of Approximate Equilibria, Mathematics of Operations Research, 2025; arXiv:2301.13652v1 (2023). https://arxiv.org/abs/2301.13652
  • G. L. Nemhauser, L. A. Wolsey, M. L. Fisher, An analysis of approximations for maximizing submodular set functions—I, Mathematical Programming 14, 1978. https://doi.org/10.1007/BF01588971
  • R. J. Lipton, E. Markakis, E. Mossel, A. Saberi, On approximately fair allocations of indivisible goods, EC 2004. https://doi.org/10.1145/988772.988792
  • H. Aziz, P. Goldberg, T. Walsh, Equilibria in sequential allocation, ADT 2017, LNCS 10576, pp. 270–283 (Springer).
  • G. Amanatidis, G. Birmpas, F. Fusco, P. Lazos, S. Leonardi, R. Reiffenhäuser, Allocating Indivisible Goods to Strategic Agents: Pure Nash Equilibria and Fairness, WINE 2021, LNCS 13112, pp. 149–166. https://arxiv.org/abs/2109.08644
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EconomicsMechanism DesignOperations Research+2·Captain: mikedeng1

Selling Data to Marketers 4: Under the Rotation Order, Data Appends with Costs Below the Prior Mean Serve High-Cost Marketers Efficiently and Under- (Over-) Supply Low-Cost Ones Below (Above) v⁺Research Paper

Motivation

Data brokers sell consumer data to firms that use it to decide whom to target, whom to lend to, or where to open a store. Two kinds of products are common: a marketing list, which supplies contact information without which the buyer cannot act at all, and a data append, which enriches information about consumers the buyer can already reach (Federal Trade Commission, Data Brokers, 2014). A seller who does not know a buyer's cost of acting must screen buyers with a menu of plans that differ in price and in how informative the data are.

Liang Guo's paper Selling Data to Marketers (Management Science, doi:10.1287/mnsc.2023.01350) characterizes the optimal menu, first for a binary-value model (§3) and then for a general information structure ordered by rotation (§4), following Johnson and Myatt (2006). This mission formalizes Proposition 7: data appends under the rotation order. It is the fourth mission of a series built from the same manuscript; the first three cover marketing lists and data appends in the binary model and marketing lists under the rotation order.

Setting

A marketer can take an action (target a consumer) at cost ccc; the action's value uuu is uncertain with prior mean u^\hat uu^. A data service of informativeness α∈[α‾,αˉ]⊂(0,1)\alpha\in[\underline\alpha,\bar\alpha]\subset(0,1)α∈[α​,αˉ]⊂(0,1) produces a signal, and its information is summarized by the posterior mean vvv. For each α\alphaα, vvv has cumulative distribution function H(v,α)H(v,\alpha)H(v,α) on a support [v‾,vˉ][\underline v,\bar v][v​,vˉ], with a strictly positive density h(v,α)h(v,\alpha)h(v,α) and mean u^\hat uu^ for every α\alphaα. The family is rotation ordered: there is a point v+∈(v‾,vˉ)v^+\in(\underline v,\bar v)v+∈(v​,vˉ) with

∂H(v,α)∂α>0 (v<v+),∂H(v,α)∂α<0 (v>v+).\frac{\partial H(v,\alpha)}{\partial\alpha}>0 \ (v<v^+),\qquad \frac{\partial H(v,\alpha)}{\partial\alpha}<0 \ (v>v^+).∂α∂H(v,α)​>0 (v<v+),∂α∂H(v,α)​<0 (v>v+).

A more informative service spreads the posterior mean away from u^\hat uu^.

A service plan (T,α)(T,\alpha)(T,α) charges a fixed fee T≥0T\ge0T≥0. Serving a marketer with informativeness α\alphaα costs the seller k(α)k(\alpha)k(α), with k(α‾)=0k(\underline\alpha)=0k(α​)=0 and kkk increasing. A marketer targets exactly when v>cv>cv>c, so a marketer with cost cic_ici​ who buys (Tj,αj)(T_j,\alpha_j)(Tj​,αj​) earns

Uij=−Tj+∫civˉ(v−ci) dH(v,αj).U_{ij}=-T_j+\int_{c_i}^{\bar v}(v-c_i)\,dH(v,\alpha_j).Uij​=−Tj​+∫ci​vˉ​(v−ci​)dH(v,αj​).

Costs are cHc_HcH​ with probability θ∈(0,1)\theta\in(0,1)θ∈(0,1) and cLc_LcL​ with probability 1−θ1-\theta1−θ, 0<cL<cH0<c_L<c_H0<cL​<cH​. A data-append buyer can act without the data, so its outside option is Ui0=max⁡{u^−ci,0}U_{i0}=\max\{\hat u-c_i,0\}Ui0​=max{u^−ci​,0}.

The seller offers a menu (TH,αH),(TL,αL)(T_H,\alpha_H),(T_L,\alpha_L)(TH​,αH​),(TL​,αL​) and maximizes Π=θ[TH−k(αH)]+(1−θ)[TL−k(αL)]\Pi=\theta[T_H-k(\alpha_H)]+(1-\theta)[T_L-k(\alpha_L)]Π=θ[TH​−k(αH​)]+(1−θ)[TL​−k(αL​)] subject to individual rationality Uii≥Ui0U_{ii}\ge U_{i0}Uii​≥Ui0​ and incentive compatibility Uii≥Uii′U_{ii}\ge U_{ii'}Uii​≥Uii′​ for both types. Call any maximizer an optimal menu, with levels αH∗,αL∗\alpha^*_H,\alpha^*_LαH∗​,αL∗​. The benchmark with observable costs is

max⁡α∈[α‾,αˉ] θi[∫civˉ(v−ci) dH(v,α)−k(α)],\max_{\alpha\in[\underline\alpha,\bar\alpha]}\ \theta_i\Big[\int_{c_i}^{\bar v}(v-c_i)\,dH(v,\alpha)-k(\alpha)\Big],α∈[α​,αˉ]max​ θi​[∫ci​vˉ​(v−ci​)dH(v,α)−k(α)],

and its maximizers are the efficient levels αie\alpha^e_iαie​.

Formalization targets

Goal: Proposition 7

Assume cL<cH<u^c_L<c_H<\hat ucL​<cH​<u^. If cL<cH<v+c_L<c_H<v^+cL​<cH​<v+, then

αH∗=αHe,αL∗<αLe,\alpha^*_H=\alpha^e_H,\qquad \alpha^*_L<\alpha^e_L ,αH∗​=αHe​,αL∗​<αLe​,

and if v+<cL<cHv^+<c_L<c_Hv+<cL​<cH​, then

αH∗=αHe,αL∗>αLe.\alpha^*_H=\alpha^e_H,\qquad \alpha^*_L>\alpha^e_L .αH∗​=αHe​,αL∗​>αLe​.

Here αH∗=αHe\alpha^*_H=\alpha^e_HαH∗​=αHe​ means that the set of αH\alpha_HαH​-levels of optimal menus equals the set of efficient levels, and each strict inequality holds for every optimal menu and every efficient level.

Milestones

  1. The willingness to pay for a data append (p. 20): for c≤u^c\le\hat uc≤u^, Uij−Ui0=−Tj+∫v‾ci(ci−v) dH(v,αj)U_{ij}-U_{i0}=-T_j+\int_{\underline v}^{c_i}(c_i-v)\,dH(v,\alpha_j)Uij​−Ui0​=−Tj​+∫v​ci​​(ci​−v)dH(v,αj​), which is increasing in cic_ici​.
  2. Its integrated form (proof of Proposition 8, p. 33): Uij−Ui0=−Tj+∫v‾ciH(v,αj) dvU_{ij}-U_{i0}=-T_j+\int_{\underline v}^{c_i}H(v,\alpha_j)\,dvUij​−Ui0​=−Tj​+∫v​ci​​H(v,αj​)dv.
  3. The reduction (15) (p. 20): substituting the binding IRLIR_LIRL​ and ICH,LIC_{H,L}ICH,L​ turns the screening problem into a maximization over (αH,αL)(\alpha_H,\alpha_L)(αH​,αL​).
  4. (15) integrated by parts, and αH∗=αHe\alpha^*_H=\alpha^e_HαH∗​=αHe​ for it (p. 33).
  5. The derivative ∂Π/∂αL\partial\Pi/\partial\alpha_L∂Π/∂αL​ of (15) compared with the benchmark's (p. 33).

Significance

Proposition 7 is the general-distribution form of a "double reversal". With marketing lists the low-cost marketers are the high type: they get efficient information, and the high-cost marketers' information is distorted (Proposition 5 of the paper). With data appends and costs below the prior mean, the outside option makes the high-cost marketers value data more. The roles of the types swap, and the direction of the distortion flips with the position of the costs relative to the rotation point. The result tells a data seller which customers to under- or over-supply, and shows that the answer depends on whether its data enable an action or only refine it.

The paper proves the result on a few pages, partly by phrases such as "it can be readily verified". No machine-checked version exists. A formalization makes explicit what the printed argument leaves implicit: that the dropped constraints hold at the reduced optimum, which regularity of kkk and HHH the strict inequalities need, and that statements about "the" optimum hold for every optimum when maximizers are not unique.

Difficulty

The obvious approach substitutes the binding constraints and compares first-order conditions. Two steps of it fail as stated. First, the reduction to (15) drops IRHIR_HIRH​ and ICL,HIC_{L,H}ICL,H​; ICL,HIC_{L,H}ICL,H​ holds at a maximizer of (15) only when the two informativeness levels are ordered as the rotation order dictates. That ordering is available only when both costs lie on the same side of v+v^+v+. Second, first-order conditions say nothing at a corner of [α‾,αˉ][\underline\alpha,\bar\alpha][α​,αˉ]. The strict comparison αL∗≠αLe\alpha^*_L\ne\alpha^e_LαL∗​=αLe​ needs the efficient level to be interior, where the derivative of kkk exists. That comes from the conditions of footnote 5 together with the mean-preserving property of the family. The selling cost need not be convex, so maximizers can be non-unique, and every comparison must hold for every pair of maximizers.

Formalization scope

  • Information structure. A structure RotationFamily with a bounded support v‾<vˉ\underline v<\bar vv​<vˉ (the paper allows an unbounded one). H(⋅,α)H(\cdot,\alpha)H(⋅,α) is continuous on [v‾,vˉ][\underline v,\bar v][v​,vˉ] with H(v‾,α)=0H(\underline v,\alpha)=0H(v​,α)=0, H(vˉ,α)=1H(\bar v,\alpha)=1H(vˉ,α)=1 and derivative h(⋅,α)>0h(\cdot,\alpha)>0h(⋅,α)>0, continuous on the closed support. ∂H/∂α\partial H/\partial\alpha∂H/∂α exists on the closed support. The rotation order (9) holds on the open support, and the mean is u^\hat uu^ for every α∈(0,1)\alpha\in(0,1)α∈(0,1). Condition (10) is not assumed; it follows.
  • Model. Model extends it with 0<α‾<αˉ<10<\underline\alpha<\bar\alpha<10<α​<αˉ<1, θ∈(0,1)\theta\in(0,1)θ∈(0,1), and 0<cL<cH0<c_L<c_H0<cL​<cH​ with both costs in (v‾,vˉ)(\underline v,\bar v)(v​,vˉ) (a pin: the integrals ∫civˉ\int_{c_i}^{\bar v}∫ci​vˉ​ presume it). It also fixes k(α‾)=0k(\underline\alpha)=0k(α​)=0 with kkk monotone on [α‾,αˉ][\underline\alpha,\bar\alpha][α​,αˉ]. dHdHdH is written as h dvh\,dvhdv.
  • Objects of the goal. Optimal menus are maximizers of the full problem: fees T≥0T\ge0T≥0, levels in [α‾,αˉ][\underline\alpha,\bar\alpha][α​,αˉ], IRiIR_iIRi​ with outside option max⁡{u^−ci,0}\max\{\hat u-c_i,0\}max{u^−ci​,0}, and both IC constraints. Efficient levels are maximizers of the benchmark (12). Neither is defined through (15) or a first-order condition. That would make the first half of the goal a restatement of milestone 4, and writing the outside option as u^−c\hat u-cu^−c instead of the maximum would change the model.
  • Pinned hypotheses. On the goal only: the part of footnote 5 the strict results use (kkk continuous on [α‾,αˉ][\underline\alpha,\bar\alpha][α​,αˉ], differentiable inside, k′(α‾)=0k'(\underline\alpha)=0k′(α​)=0 from the right, k′(α)→+∞k'(\alpha)\to+\inftyk′(α)→+∞ as α→αˉ−\alpha\to\bar\alpha^-α→αˉ−) and joint continuity of ∂H/∂α\partial H/\partial\alpha∂H/∂α on [v‾,vˉ]×(0,1)[\underline v,\bar v]\times(0,1)[v​,vˉ]×(0,1). The derivative milestone uses only the latter. Convexity of kkk is not assumed.
  • Range restriction. The first sentence of Proposition 7 (αH∗=αHe\alpha^*_H=\alpha^e_HαH∗​=αHe​) is posed on the full problem only within the two ranges cH<v+c_H<v^+cH​<v+ and v+<cLv^+<c_Lv+<cL​. For (15) it is posed without restriction in milestone 4. The branch v+<cL<cH<u^v^+<c_L<c_H<\hat uv+<cL​<cH​<u^ is empty when v+≥u^v^+\ge\hat uv+≥u^, for example for symmetric structures; non-symmetric rotation families with v+<u^v^+<\hat uv+<u^ inhabit it.
  • Reuse. Topkis's monotonicity theorem (Theorem 2.8.4) is on the platform and is the tool the paper invokes. The integration-by-parts facts for distribution functions on a bounded support, and differentiation of ∫cvˉH(v,α) dv\int_c^{\bar v}H(v,\alpha)\,dv∫cvˉ​H(v,α)dv in α\alphaα, are reusable beyond this mission. Proofs of the milestones in any order are welcome.

Selected references

  • Liang Guo, Selling Data to Marketers, Management Science, 2025 (author's manuscript used here). https://doi.org/10.1287/mnsc.2023.01350
  • Justin P. Johnson and David P. Myatt, On the Simple Economics of Advertising, Marketing, and Product Design, American Economic Review 96(3), 2006. https://doi.org/10.1257/000282806777211946
  • Donald M. Topkis, Supermodularity and Complementarity, Princeton University Press, 1998. https://doi.org/10.1515/9781400822539
  • Federal Trade Commission, Data Brokers: A Call for Transparency and Accountability, 2014. https://www.ftc.gov/reports/data-brokers-call-transparency-accountability-report-federal-trade-commission-may-2014
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CombinatoricsTheoretical Computer Science·Captain: Yuxuan Xu

Deterministic Integer 3SUM in O(n^1.999017): Sharp Binomial-Tail AnalysisResearch Paper

Why sharpen the integer 3SUM exponent?

3SUM asks whether an input sequence contains three entries at different positions whose sum is zero. The classical quadratic running time makes it a benchmark for fine-grained algorithm design: even a small fixed improvement in the exponent changes its asymptotic complexity. The setting here is polynomially bounded integers and a deterministic word RAM; the input-size exponent, rather than an experimental speedup, is the quantity being studied.

Alman and Vassilevska Williams (2026) give a deterministic truly subquadratic integer 3SUM algorithm through thin matrix products and reductions involving Exact Triangle. Xu's manuscript, Deterministic Integer 3SUM in O(n^1.999017) Time via a Sharper Binomial-Tail Analysis, dated 13 October 2026, refines the analysis of that framework. Its claimed bound is the formalization target here. The Hexagon link identifies the author's submission page, which may require authentication; it is not presented as a public article identifier or evidence of peer review.

Inputs, machine model, and analytic quantities

An input of size nnn is a function x:{0,…,n−1}→Zx:\{0,\ldots,n-1\}\to\mathbb Zx:{0,…,n−1}→Z. For a fixed natural number κ\kappaκ, every entry obeys ∣xi∣≤nκ|x_i|\le n^\kappa∣xi​∣≤nκ. Acceptance means that there are pairwise distinct indices i,j,ki,j,ki,j,k with xi+xj+xk=0x_i+x_j+x_k=0xi​+xj​+xk​=0. Repeated values at different positions are allowed. This is a decision problem, so the algorithm need not return a witness triple.

The word-RAM specification is the campaign's existing EndStatement definition, imported from its foundation mission. For each fixed κ\kappaκ, one finite deterministic program, one word-width threshold constant, and one time-bound function must work for all input sizes and all word widths above that threshold. Words have finite signed interpretations; arithmetic, indirect memory access, branching, acceptance, and rejection are defined operationally. The result concerns this exact model.

For the supporting analysis, let H(u)=−ulog⁡u−(1−u)log⁡(1−u)H(u)=-u\log u-(1-u)\log(1-u)H(u)=−ulogu−(1−u)log(1−u), with endpoint values H(0)=H(1)=0H(0)=H(1)=0H(0)=H(1)=0. All logarithms are natural. For an integer c>10c>10c>10, a positive integer mmm, and 0<θ<0.90<\theta<0.90<θ<0.9, set L=cmL=cmL=cm, D=4mD=4^mD=4m, t=⌈θm⌉t=\lceil\theta m\rceilt=⌈θm⌉, and

βd=(Lm−d)9L−m+d,M=β0.\beta_d=\binom L{m-d}9^{L-m+d},\qquad M=\beta_0.βd​=(m−dL​)9L−m+d,M=β0​.

The sharp preprocessing saving, query exponent, and encoding exponent are

γ∗(c,θ)=cH(1/c)−cH((1−θ)/c)−θlog⁡9log⁡4,\gamma_*(c,\theta)=\frac{cH(1/c)-cH((1-\theta)/c)-\theta\log9}{\log4},γ∗​(c,θ)=log4cH(1/c)−cH((1−θ)/c)−θlog9​, q(θ)=H(θ)+θlog⁡9log⁡4,A(c)=clog⁡10−cH(1/c)/2−(c−1)log⁡3log⁡4.q(\theta)=\frac{H(\theta)+\theta\log9}{\log4},\qquad A(c)=\frac{c\log10-cH(1/c)/2-(c-1)\log3}{\log4}.q(θ)=log4H(θ)+θlog9​,A(c)=log4clog10−cH(1/c)/2−(c−1)log3​.

These auxiliary definitions describe costs; they neither redefine 3SUM nor assume the existence of a fast algorithm.

Formalization targets

The campaign goal is the exact fixed bound

EndStatement.ThreeSum.SolvedInTime  1.999017.\texttt{EndStatement.ThreeSum.SolvedInTime}\;1.999017.EndStatement.ThreeSum.SolvedInTime1.999017.

The first supporting milestone is the two-sided binomial entropy estimate. The second is the manuscript's normalized tail bound

1M∑d=tmβd≤cm+11−9/(c−1)D−γ∗(c,θ).\frac1M\sum_{d=t}^m\beta_d\le\frac{cm+1}{1-9/(c-1)}D^{-\gamma_*(c,\theta)}.M1​d=t∑m​βd​≤1−9/(c−1)cm+1​D−γ∗​(c,θ).

A further milestone establishes strict improvement over the earlier preprocessing saving γ(c,θ)=θlog⁡((c−1)/9)/log⁡4\gamma(c,\theta)=\theta\log((c-1)/9)/\log4γ(c,θ)=θlog((c−1)/9)/log4 at fixed parameters. The algorithmic milestone combines the manuscript's Propositions 4.1 and 5.1: admissible sharp-tail parameters must yield a program satisfying the shared 3SUM specification, not merely a numerical inequality.

The final supporting milestone certifies the exact choice

c=21,θ=0.11202,a=0.05665,s=0.06945.c=21,\qquad\theta=0.11202,\qquad a=0.05665,\qquad s=0.06945.c=21,θ=0.11202,a=0.05665,s=0.06945.

It includes the preprocessing, query, encoding, prime-selection, and instance-construction inequalities, together with

2−as/4=1.999016414375,1.999017−(2−as/4)=0.000000585625>0.2-as/4=1.999016414375,\qquad1.999017-(2-as/4)=0.000000585625>0.2−as/4=1.999016414375,1.999017−(2−as/4)=0.000000585625>0.

Every terminating decimal denotes an exact rational number. The target is the fixed big-OOO exponent 1.999017; the smaller cutoff is accompanied by residual asymptotic losses in the manuscript and is not asserted as the same fixed bound.

What completing this mission would establish

A complete proof would certify the manuscript's improved integer 3SUM bound in the campaign's common machine model. The gain is an analysis refinement of the inherited algorithm and reductions. It does not claim a new algorithmic framework, optimal parameters, global optimality, or priority over all other work.

The manuscript also gives an auxiliary O(n1.999073)O(n^{1.999073})O(n1.999073) bound by retuning the previous estimate. That weaker result is background, not this mission's campaign value. The existing upstream formalization is prior work; it does not automatically certify either refinement. The supplied rational interval verifier checks the parameter inequalities, but those checks alone do not prove a word-RAM running-time theorem. The main goal and the newly drafted supporting statements remain open Lean proof obligations.

Where the difficulty lies

A better tail estimate is insufficient unless every other cost remains within the final budget. Shared encoding work, all queries, deterministic prime selection, witness scanning, and instance construction must be included. The word-size and address bounds must remain valid after changing parameters. Ceiling operations, restricting DDD to powers of four, and bounded-size exceptions must also be handled.

The central formalization burden is the connection between the analytic estimates and an actual deterministic program. Assuming an oracle with the desired running time would remove that burden and would not establish the stated target. Likewise, checking a finite range of sizes or a floating-point optimizer's output cannot establish the universal algorithmic statement.

Formalization scope and conventions

The environment is Lean 4.33.1 with Mathlib revision 0df444a360eaa60ab8c11dca51a86af692955474. The foundation reference and the campaign goal's import are retained. Supporting definitions use real logarithms, real powers, natural binomial coefficients, finite sums, and a natural ceiling. Domain hypotheses exclude invalid entropy-tail regimes; endpoint binomial cases are included explicitly.

For r=1999017/1000000r=1999017/1000000r=1999017/1000000, the shared time predicate means that there exists K∈NK\in\mathbb NK∈N such that T(n)1000000≤Kn1999017T(n)^{1000000}\le K n^{1999017}T(n)1000000≤Kn1999017 for every n≥2n\ge2n≥2. Correctness and termination still cover every input size, including n<3n<3n<3. The manuscript's κ≥1\kappa\ge1κ≥1 convention must be extended to the campaign's κ=0\kappa=0κ=0 case, and its word-size analysis must justify uniform correctness at every sufficiently large word width. Both are explicit interface obligations.

Reusable contributions include entropy and tail estimates, rigorous logarithm enclosures, and parameterized cost-to-program results. Existing compatible library results should be reused where available. The manuscript and metadata were prepared with AI assistance; this mission makes no claim of completed human review or completed formal verification of the improved bound.

Selected references

  • Yuxuan Xu, Deterministic Integer 3SUM in O(n^1.999017) Time via a Sharper Binomial-Tail Analysis, manuscript, 13 October 2026. Author-supplied Hexagon submission page. Target: Theorem 1.1; supporting analysis: Sections 3–6.
  • Josh Alman and Virginia Vassilevska Williams, Truly Subquadratic 3SUM and Truly Subcubic APSP via Triangles in Sparse Lopsided Graphs, arXiv preprint, 2026. arXiv:2610.06783v1. Inherited ingredients: Section 4, Lemma 29, Theorem 30, Corollary 31, and the deterministic reductions cited in Xu's Section 2.
  • Anthropic, Truly Subquadratic 3SUM and Truly Subcubic APSP: a Lean 4 formalization, source repository, 2026. Pinned source at commit e1a4e6508154ea59f030480661590a9fe3018011. Its EndStatement.lean supplies the shared specification, not a proof of this mission's new exponent.
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Linear OptimizationOperations ResearchOptimization·Captain: mikedeng1

On the Optimality of Affine Policies for Budgeted Uncertainty Sets 3: With a Network Recourse Matrix, the Optimal Affine Policy Costs m/2 − 1 While the Adjustable Optimum Is 0Research Paper

Why the sign of the recourse matrix matters

A two-stage adjustable robust linear program chooses a first-stage decision xxx before an uncertain right-hand side hhh is revealed, and a second-stage (recourse) decision y(h)y(h)y(h) afterwards, minimising the worst case over an uncertainty set U\mathcal UU of the total cost. Computing the optimal value zAR(U)z_{AR}(\mathcal U)zAR​(U) is hard in general (Feige et al., 2007), and the standard tractable restriction is to affine policies y(h)=Ph+qy(h)=Ph+qy(h)=Ph+q (Ben-Tal et al., 2004), whose optimal value zAff(U)z_{Aff}(\mathcal U)zAff​(U) is computed by a single linear program.

El Housni and Goyal (arXiv:1807.00163v2) show that, when the recourse matrix BBB is non-negative and U\mathcal UU is a budget of uncertainty set, zAffz_{Aff}zAff​ is within a factor O(log⁡n/log⁡log⁡n)O(\log n/\log\log n)O(logn/loglogn) of zARz_{AR}zAR​. Their Section 7 asks whether the non-negativity of BBB is needed, and answers with a family of two-stage lot-sizing instances whose recourse matrix is a network matrix with entries in {−1,0,1}\{-1,0,1\}{−1,0,1}. On this family the adjustable problem has value 000 while every affine policy costs at least m/2−1m/2-1m/2−1. Lot-sizing and transportation recourse are among the most common uses of two-stage robust optimisation (see Bertsimas and de Ruiter, 2016), so the instance is a natural one, not an artefact.

Lower bounds on the gap between affine and adjustable policies were known before (Bertsimas and Goyal, 2012); the point of the present family is that the adjustable value is exactly 000, so the ratio zAff/zARz_{Aff}/z_{AR}zAff​/zAR​ is infinite and the difference zAff−zARz_{Aff}-z_{AR}zAff​−zAR​ grows linearly in mmm.

Setting

The lot-sizing problem (7.1). There are mmm nodes. Node iii stores inventory xix_ixi​ at cost cic_ici​ per unit, up to a capacity KiK_iKi​, and faces an uncertain demand hih_ihi​. After hhh is revealed, inventory may be shipped from node iii to node jjj in amount yij(h)≥0y_{ij}(h)\ge0yij​(h)≥0 at cost dijd_{ij}dij​ per unit. A solution (x,y)(x,y)(x,y) is feasible when 0≤xi≤Ki0\le x_i\le K_i0≤xi​≤Ki​ and, for every h∈Uh\in\mathcal Uh∈U,

xi+∑jyji(h)−∑jyij(h) ≥ hi(i∈[m]).x_i+\sum_{j}y_{ji}(h)-\sum_j y_{ij}(h)\ \ge\ h_i\qquad(i\in[m]).xi​+j∑​yji​(h)−j∑​yij​(h) ≥ hi​(i∈[m]).

The objective is the first-stage cost ∑icixi\sum_ic_ix_i∑i​ci​xi​ plus the worst case over h∈Uh\in\mathcal Uh∈U of the transportation cost ∑ijdijyij(h)\sum_{ij}d_{ij}y_{ij}(h)∑ij​dij​yij​(h). The optimum over all rules h↦y(h)h\mapsto y(h)h↦y(h) is zAR(U)z_{AR}(\mathcal U)zAR​(U), and the optimum over affine rules y(h)=Ph+qy(h)=Ph+qy(h)=Ph+q (one row of PPP per arc, one column per node) is zAff(U)z_{Aff}(\mathcal U)zAff​(U).

The family (7.2). Let m=2km=2km=2k, and split the nodes into J1J_1J1​ and J2J_2J2​ with ∣J1∣=∣J2∣=k|J_1|=|J_2|=k∣J1​∣=∣J2​∣=k. Set ci=0c_i=0ci​=0 on J1J_1J1​ and ci=1c_i=1ci​=1 on J2J_2J2​, Ki=1K_i=1Ki​=1 everywhere, dij=0d_{ij}=0dij​=0 for i∈J1i\in J_1i∈J1​, j∈J2j\in J_2j∈J2​, and dij=∞d_{ij}=\inftydij​=∞ otherwise. The uncertainty set is

U={h∈[0,1]m ∣ ∑i=1mhi≤m/2}.\mathcal U=\Big\{h\in[0,1]^m\ \Big|\ \sum_{i=1}^m h_i\le m/2\Big\}.U={h∈[0,1]m ​ i=1∑m​hi​≤m/2}.

Inventory can thus move only from J1J_1J1​ to J2J_2J2​, at no cost; stocking J1J_1J1​ is free and stocking J2J_2J2​ costs one per unit.

In the Lean development the general problem is the structure LotSizing N E (nodes N, usable arcs E with tail src, head tgt, distances d), with the predicate Feasible, the cost cost, and the sets adjustableValues, affineValues of objective values. The family is lotSizingFamily k, on nodes Fin k ⊕ Fin k and arcs Fin k × Fin k.

Formalization targets

Goal: Lemma 7.1

For every k≥1k\ge1k≥1,

zAR(U)=0andzAff(U)=m2−1=k−1,z_{AR}(\mathcal U)=0\qquad\text{and}\qquad z_{Aff}(\mathcal U)=\frac m2-1=k-1,zAR​(U)=0andzAff​(U)=2m​−1=k−1,

each stated as IsLeast of the corresponding set of objective values, which asserts that the value is attained and is the minimum. The unboundedness of the gap, zAff−zAR=k−1→∞z_{Aff}-z_{AR}=k-1\to\inftyzAff​−zAR​=k−1→∞, is immediate.

Milestones (Appendix D, in proof order)

  1. The first-stage decision x=1J1x=\mathbb 1_{J_1}x=1J1​​ admits a second-stage policy with cost 000 in every scenario (p. 35).
  2. (D.3), for k≥2k\ge2k≥2: every feasible affine solution has xi=1x_i=1xi​=1 on J1J_1J1​, and its flow on arc (i,j)(i,j)(i,j) depends on hih_ihi​ only, with P(i,j),i+qij=0P_{(i,j),i}+q_{ij}=0P(i,j),i​+qij​=0 (p. 36).
  3. For k≥2k\ge2k≥2, every feasible affine solution satisfies xj+qℓj≥1x_j+q_{\ell j}\ge1xj​+qℓj​≥1 for ℓ∈J1\ell\in J_1ℓ∈J1​, j∈J2j\in J_2j∈J2​ (pp. 36–37).
  4. Every feasible affine solution has ∑j∈J2xj≥m/2−1\sum_{j\in J_2}x_j\ge m/2-1∑j∈J2​​xj​≥m/2−1, hence zAff≥m/2−1z_{Aff}\ge m/2-1zAff​≥m/2−1 (p. 37).
  5. The explicit affine solution x=1−emx=\mathbb 1-e_mx=1−em​, yim(h)=1−hiy_{im}(h)=1-h_iyim​(h)=1−hi​, is feasible and costs m/2−1m/2-1m/2−1 (p. 37).

Significance

The result. The approximation guarantees of the paper (O(log⁡n/log⁡log⁡n)O(\log n/\log\log n)O(logn/loglogn) for budget sets, O(log⁡2n/log⁡log⁡n)O(\log^2 n/\log\log n)O(log2n/loglogn) for disjoint constrained budgets) assume B≥0B\ge0B≥0. Lemma 7.1 shows that this assumption is not a convenience of the proof: with a network recourse matrix no bound on zAff/zARz_{Aff}/z_{AR}zAff​/zAR​ of any form holds, even for a budget set and a bipartite network. Any extension of the guarantees to transportation or flow recourse must therefore change the policy class or add structure, which is the open direction the paper states after the lemma.

Formalizing it. The lemma is proved in the paper; it has not been machine-checked. The mission produces a reusable definition of the two-stage robust lot-sizing problem with arc-based recourse, the precise instance family, and checked versions of the five steps of Appendix D. Two of those steps hold only for m≥4m\ge4m≥4 and one is printed with its indices swapped (see the scope section); the formal statements make those boundaries explicit.

Difficulty

The adjustable half is a transportation argument, and the affine upper bound is a direct verification of one explicit solution. The substance is the affine lower bound, which must hold for every feasible affine solution, not for a particular one. Comparing an affine policy with the adjustable optimum on a few extreme scenarios gives nothing: on any single scenario an affine policy can match the adjustable cost. What fails for affine policies is simultaneous feasibility over the whole of U\mathcal UU, and the lower bound has to extract a cost from that requirement alone. It is also sensitive to the size of the instance: two of the intermediate steps of Appendix D are false for m=2m=2m=2, so a formal proof has to treat small mmm separately.

Formalization scope

  • Model. Vectors are functions on finite types with the componentwise order; indices are 0-based. The second stage is a rule y:RN→REy:\mathbb R^N\to\mathbb R^Ey:RN→RE, which gives the same values as choosing y(h)y(h)y(h) separately per scenario. The epigraph variable zzz of (7.1) appears through the sets of objective values ttt with ∑icixi+∑adaya(h)≤t\sum_ic_ix_i+\sum_a d_a y_a(h)\le t∑i​ci​xi​+∑a​da​ya​(h)≤t for all h∈Uh\in\mathcal Uh∈U.
  • Infinite distances. Arcs with dij=∞d_{ij}=\inftydij​=∞ are omitted rather than given an extended-real cost: a finite-cost solution never uses them, so no optimal value changes, and App. D itself works with the reduced constraints (D.1)–(D.2) and with a matrix PPP having "one row per edge". The kept arcs J1×J2J_1\times J_2J1​×J2​ have d=0d=0d=0, and the cost keeps the term ∑adaya(h)\sum_a d_a y_a(h)∑a​da​ya​(h) so that (7.1) is visible.
  • Values as IsLeast. No real infimum is used, so "z=0z=0z=0" cannot hold on an empty feasible set; feasibility includes 0≤x≤K0\le x\le K0≤x≤K, Ph+q≥0Ph+q\ge0Ph+q≥0 on all of U\mathcal UU, and the coverage constraint at every node, including the outflow constraint (D.2) at J1J_1J1​.
  • Sizes. The paper's "mmm even" is m=2km=2km=2k. The goal assumes k≥1k\ge1k≥1; at k=0k=0k=0 the affine value would be 0≠−10\ne-10=−1.
  • Corrections, disclosed in the items. (i) The paper builds the zero-cost adjustable policy only at extreme points of U\mathcal UU; the milestone quantifies over all of U\mathcal UU, as feasibility requires. (ii) (D.3) and the bound xj+qℓj≥1x_j+q_{\ell j}\ge1xj​+qℓj​≥1 are false for m=2m=2m=2 (explicit counterexamples are in the items' notes) and carry the hypothesis k≥2k\ge2k≥2. (iii) "for any j∈J1j\in J_1j∈J1​ and for any ℓ∈J2\ell\in J_2ℓ∈J2​" on p. 37 has the indices swapped and is stated with ℓ∈J1\ell\in J_1ℓ∈J1​, j∈J2j\in J_2j∈J2​.
  • Not formalized. That (7.1) has a network recourse matrix with entries in {−1,0,1}\{-1,0,1\}{−1,0,1} is descriptive and is not stated; total unimodularity is not needed.
  • Reusable parts. LotSizing (any node set, any arc set, any uncertainty set) can host other two-stage lot-sizing and transportation results. Proofs of any milestone, and alternative arguments for the affine lower bound, are welcome.

The source is arXiv:1807.00163v2; its printed page numbers equal the PDF's.

Selected references

  • O. El Housni, V. Goyal, On the Optimality of Affine Policies for Budgeted Uncertainty Sets, arXiv:1807.00163v2, 2019 (Mathematics of Operations Research 46(2), 2021). https://arxiv.org/abs/1807.00163v2
  • A. Ben-Tal, A. Goryashko, E. Guslitzer, A. Nemirovski, Adjustable robust solutions of uncertain linear programs, Mathematical Programming 99(2), 2004. https://doi.org/10.1007/s10107-003-0454-y
  • D. Bertsimas, V. Goyal, On the power and limitations of affine policies in two-stage adaptive optimization, Mathematical Programming 134(2), 2012. https://doi.org/10.1007/s10107-011-0444-4
  • D. Bertsimas, F. de Ruiter, Duality in two-stage adaptive linear optimization: Faster computation and stronger bounds, INFORMS Journal on Computing 28(3), 2016. https://doi.org/10.1287/ijoc.2016.0689
  • U. Feige, K. Jain, M. Mahdian, V. Mirrokni, Robust combinatorial optimization with exponential scenarios, IPCO 2007. https://doi.org/10.1007/978-3-540-72792-7_33
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Quantum Information·Captain: Lucas

Superconducting Quantum Computing: Universality of Single-Qubit Gates and iSWAPTextbook

Motivation

Superconducting circuits built from capacitors, inductors and Josephson junctions are the dominant platform for current quantum processors (Google, IBM, Rigetti, IQM and others). The source article — the Wikipedia entry Superconducting quantum computing — states two facts about the gate model on this hardware that this mission makes precise:

  1. two-qubit gates such as iSWAP "can be achieved through coherent exchange" between two coupled qubits, whose interaction is described by the coupling Hamiltonian H^=ℏJ2(σ1xσ2x+σ1yσ2y)\hat H=\frac{\hbar J}{2}(\sigma_1^x\sigma_2^x+\sigma_1^y\sigma_2^y)H^=2ℏJ​(σ1x​σ2x​+σ1y​σ2y​) (section Transmon);
  2. "single-qubit gates combined with two-qubit gates form a universal gate set" (section Criteria for a viable quantum processor), and, for instance, a three-qubit Toffoli gate "is implemented using a combination of single and two-qubit gates" (section Quantum gates).

Statement 2 is a mathematical theorem, not an engineering claim: it says that every unitary operation on nnn qubits can be written exactly as a finite product of the hardware's elementary gates. Its classical form with CNOT as the two-qubit gate is due to Barenco et al. (1995); the iSWAP version follows because CNOT can be built from two iSWAPs and single-qubit gates (Schuch–Siewert 2003).

Timeline.

  • 1995 — DiVincenzo shows two-qubit gates are universal; Barenco et al. prove that single-qubit gates and CNOT generate all nnn-qubit unitaries exactly.
  • 2003 — Schuch and Siewert analyse the XY (iSWAP-type) interaction and give a CNOT construction using two iSWAP gates.
  • 2007 — the transmon is introduced; capacitively coupled transmons realise the XY interaction.
  • 2012 — a Toffoli gate is demonstrated on three superconducting transmon qubits.

Setting

An nnn-qubit register has computational basis states ∣x⟩|x\rangle∣x⟩ labelled by bit strings x∈{0,1}nx\in\{0,1\}^nx∈{0,1}n; its operations form the unitary group U(2n)U(2^n)U(2n). For a 2×22\times22×2 unitary UUU and a qubit kkk, the single-qubit gate U(k)U^{(k)}U(k) applies UUU to qubit kkk and leaves the others unchanged. For a 4×44\times44×4 matrix GGG and an ordered pair of distinct qubits (i,j)(i,j)(i,j), G(i,j)G^{(i,j)}G(i,j) applies GGG to qubits i,ji,ji,j (qubit iii is the first tensor factor). Write

Sn={U(k):U∈U(2), k a qubit},Gn(G)={G(i,j):i≠j}.\mathcal S_n=\{U^{(k)} : U\in U(2),\ k\text{ a qubit}\},\qquad \mathcal G_n(G)=\{G^{(i,j)} : i\neq j\}.Sn​={U(k):U∈U(2), k a qubit},Gn​(G)={G(i,j):i=j}.

The gates used are

iSWAP=(100000i00i000001),CNOT=(1000010000010010)\mathrm{iSWAP}=\begin{pmatrix}1&0&0&0\\0&0&i&0\\0&i&0&0\\0&0&0&1\end{pmatrix},\qquad \mathrm{CNOT}=\begin{pmatrix}1&0&0&0\\0&1&0&0\\0&0&0&1\\0&0&1&0\end{pmatrix}iSWAP=​1000​00i0​0i00​0001​​,CNOT=​1000​0100​0001​0010​​

in the basis ∣00⟩,∣01⟩,∣10⟩,∣11⟩|00\rangle,|01\rangle,|10\rangle,|11\rangle∣00⟩,∣01⟩,∣10⟩,∣11⟩, and the Toffoli gate ∣a,b,c⟩↦∣a,b,c⊕ab⟩|a,b,c\rangle\mapsto|a,b,c\oplus ab\rangle∣a,b,c⟩↦∣a,b,c⊕ab⟩. Time evolution under a Hamiltonian HHH is U(t)=exp⁡(−itH/ℏ)U(t)=\exp(-itH/\hbar)U(t)=exp(−itH/ℏ), and the coupling Hamiltonian is H=ℏJ2(σx⊗σx+σy⊗σy)H=\frac{\hbar J}{2}(\sigma^x\otimes\sigma^x+\sigma^y\otimes\sigma^y)H=2ℏJ​(σx⊗σx+σy⊗σy). A two-level unitary acts as the identity outside the span of two basis vectors.

Formalization targets

Goal — universality of single-qubit gates and iSWAP

For every n≥1n\ge1n≥1,

⟨ Sn∪Gn(iSWAP) ⟩=U(2n).\big\langle\,\mathcal S_n\cup\mathcal G_n(\mathrm{iSWAP})\,\big\rangle=U(2^n).⟨Sn​∪Gn​(iSWAP)⟩=U(2n).

Milestones

  1. Coherent exchange: exp⁡ ⁣(−itℏH)=iSWAP†\exp\!\big(-\tfrac{it}{\hbar}H\big)=\mathrm{iSWAP}^\daggerexp(−ℏit​H)=iSWAP† at t=π/(2J)t=\pi/(2J)t=π/(2J), for ℏ,J≠0\hbar,J\ne0ℏ,J=0.
  2. CNOT=(A⊗B) iSWAP (C⊗D) iSWAP (E⊗F)\mathrm{CNOT}=(A\otimes B)\,\mathrm{iSWAP}\,(C\otimes D)\,\mathrm{iSWAP}\,(E\otimes F)CNOT=(A⊗B)iSWAP(C⊗D)iSWAP(E⊗F) for some A,…,F∈U(2)A,\dots,F\in U(2)A,…,F∈U(2).
  3. Two-level unitaries generate U(Cι)U(\mathbb C^\iota)U(Cι) for every finite ι\iotaι.
  4. ⟨ Sn∪Gn(CNOT) ⟩=U(2n)\big\langle\,\mathcal S_n\cup\mathcal G_n(\mathrm{CNOT})\,\big\rangle=U(2^n)⟨Sn​∪Gn​(CNOT)⟩=U(2n) for n≥1n\ge1n≥1.
  5. Toffoli∈⟨ S3∪G3(CNOT) ⟩\mathrm{Toffoli}\in\big\langle\,\mathcal S_3\cup\mathcal G_3(\mathrm{CNOT})\,\big\rangleToffoli∈⟨S3​∪G3​(CNOT)⟩.

Significance

The goal theorem is the formal justification for compiling arbitrary quantum algorithms to superconducting hardware whose native entangling interaction is of XY/iSWAP type: any target unitary, however large, has an exact decomposition into the hardware's elementary operations. Milestone 1 connects the abstract gate to the physical Hamiltonian; milestones 3–4 are the textbook universality theorem in the CNOT form, reusable for any other two-qubit gate that can synthesise CNOT; milestone 5 is the Toffoli construction mentioned in the source.

All results are classical and proved in the literature. To the best of the drafter's knowledge they are not yet available as machine-checked statements in Mathlib in this form; the mission's contribution is a complete formal development.

Difficulty

The naive route — "decompose into two-level unitaries, then implement each with gates" — hides real work: a two-level unitary on basis states ∣x⟩,∣y⟩|x\rangle,|y\rangle∣x⟩,∣y⟩ with x,yx,yx,y differing in many bits must be conjugated by a Gray-code sequence of controlled-NOT style gates into one acting on a single qubit, controlled on all others, and multiply-controlled single-qubit gates must then be reduced to single-qubit gates and CNOTs. Keeping indices, tensor embeddings and controls consistent over nnn qubits is the main formal burden. Milestone 1 requires computing a matrix exponential exactly, which in Lean means handling NormedSpace.exp on a non-diagonal matrix.

Formalization scope

  • Basis states of nnn qubits are functions Fin n → Fin 2; two-qubit operators are indexed by Fin 2 × Fin 2 with the Kronecker product ⊗ₖ, first factor = first qubit.
  • Universality is exact: the subgroup generated (Subgroup.closure) inside Matrix.unitaryGroup equals ⊤; no approximation or topological closure is involved, which is why the full continuous family U(2)U(2)U(2) of single-qubit gates is included.
  • n=0n=0n=0 is excluded: with no qubits there are no generators, while U(1)U(1)U(1) is nontrivial.
  • The gate sets contain only the stated gates; a formalization that adds arbitrary two-qubit unitaries to the generators would make the goal trivially true and is not acceptable.
  • Needed infrastructure: tensor embeddings of gates into nnn-qubit registers, controlled gates, Gray-code arguments, and exponentials of 2×22\times22×2 / 4×44\times44×4 matrices. Lemmas about embeddings (onQubit, onPair) and multiply-controlled gates are reusable for any quantum-circuit mission.

Selected references

  • Wikipedia, Superconducting quantum computing (sections Quantum gates, Criteria for a viable quantum processor, Transmon). https://en.wikipedia.org/wiki/Superconducting_quantum_computing
  • A. Barenco, C. H. Bennett, R. Cleve, D. P. DiVincenzo, N. Margolus, P. Shor, T. Sleator, J. Smolin, H. Weinfurter, Elementary gates for quantum computation, Phys. Rev. A 52, 3457 (1995). https://doi.org/10.1103/PhysRevA.52.3457
  • N. Schuch, J. Siewert, Natural two-qubit gate for quantum computation using the XY interaction, Phys. Rev. A 67, 032301 (2003). https://doi.org/10.1103/PhysRevA.67.032301
  • M. A. Nielsen, I. L. Chuang, Quantum Computation and Quantum Information, Cambridge University Press (2000), §4.5.
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Quantum Information·Captain: Lucas

Grover's Algorithm (Wikipedia): Quantum Search with Success Probability 1 − 1/N in ⌈π√N/4⌉ IterationsTextbook

Motivation

Grover's algorithm is a quantum algorithm for unstructured search: given black-box access to a function f ⁣:{0,1,…,N−1}→{0,1}f\colon\{0,1,\dots,N-1\}\to\{0,1\}f:{0,1,…,N−1}→{0,1} that takes the value 111 at exactly one input ω\omegaω, it finds ω\omegaω with high probability using O(N)O(\sqrt N)O(N​) evaluations of fff. It was devised by Lov Grover in 1996 (Grover, STOC 1996). Classically the same task needs Θ(N)\Theta(N)Θ(N) evaluations, since there is no better approach than trying the inputs one after the other. Bennett, Bernstein, Brassard and Vazirani showed that every quantum algorithm needs Ω(N)\Omega(\sqrt N)Ω(N​) evaluations (BBBV, SIAM J. Comput. 1997), so the quadratic speedup is optimal.

Because many problems contain exhaustive search as a subroutine, the algorithm and its generalization, amplitude amplification, speed up a broad class of algorithms: brute-force attacks on symmetric-key cryptography (a 128-bit key in roughly 2642^{64}264 iterations), algorithms for NP-complete problems such as 3SAT, and black-box problems such as element distinctness and the collision problem.

This mission follows the presentation of the algorithm and of its analysis in the Wikipedia article Grover's algorithm (revision 1373498442), which gives two analyses of the same algorithm, a geometric proof and an algebraic proof, following Nielsen–Chuang 2010, Chapter 6.

Setting

Fix N≥1N \ge 1N≥1. The state space is H=CN\mathcal H = \mathbb C^NH=CN with standard basis ∣0⟩,…,∣N−1⟩|0\rangle,\dots,|N-1\rangle∣0⟩,…,∣N−1⟩ and inner product ⟨u∣v⟩=∑xux‾vx\langle u|v\rangle = \sum_x \overline{u_x}v_x⟨u∣v⟩=∑x​ux​​vx​. Let f ⁣:{0,…,N−1}→{0,1}f\colon\{0,\dots,N-1\}\to\{0,1\}f:{0,…,N−1}→{0,1} have exactly one index ω\omegaω with f(ω)=1f(\omega) = 1f(ω)=1.

  • The oracle is the unitary Uω∣x⟩=(−1)f(x)∣x⟩U_\omega|x\rangle = (-1)^{f(x)}|x\rangleUω​∣x⟩=(−1)f(x)∣x⟩. The standard oracle acts on H⊗C2\mathcal H\otimes\mathbb C^2H⊗C2 (one extra ancillary qubit) by Uf∣x⟩∣y⟩=∣x⟩∣y⊕f(x)⟩U_f|x\rangle|y\rangle = |x\rangle|y\oplus f(x)\rangleUf​∣x⟩∣y⟩=∣x⟩∣y⊕f(x)⟩.
  • The uniform superposition is ∣s⟩=1N∑x=0N−1∣x⟩|s\rangle = \frac{1}{\sqrt N}\sum_{x=0}^{N-1}|x\rangle∣s⟩=N​1​∑x=0N−1​∣x⟩, and the Grover diffusion operator is Us=2∣s⟩⟨s∣−IU_s = 2|s\rangle\langle s| - IUs​=2∣s⟩⟨s∣−I.
  • A Grover iteration applies UωU_\omegaUω​ and then UsU_sUs​, i.e. the operator UsUωU_sU_\omegaUs​Uω​.

The algorithm. (1) Initialize the system to ∣s⟩|s\rangle∣s⟩. (2) Perform the Grover iteration rrr times. (3) Measure the resulting state (UsUω)r∣s⟩(U_sU_\omega)^r|s\rangle(Us​Uω​)r∣s⟩ in the computational basis; by the Born rule the outcome is ω\omegaω with probability ∣⟨ω∣(UsUω)r∣s⟩∣2|\langle\omega|(U_sU_\omega)^r|s\rangle|^2∣⟨ω∣(Us​Uω​)r∣s⟩∣2.

Two further objects appear in the analysis: the ket ∣s′⟩=1N−1∑x≠ω∣x⟩|s'\rangle = \frac{1}{\sqrt{N-1}}\sum_{x\ne\omega}|x\rangle∣s′⟩=N−1​1​∑x=ω​∣x⟩ perpendicular to ∣ω⟩|\omega\rangle∣ω⟩, and the angles θ=2arcsin⁡1N\theta = 2\arcsin\frac{1}{\sqrt N}θ=2arcsinN​1​ (geometric proof) and t=arcsin⁡1N=θ/2t = \arcsin\frac{1}{\sqrt N} = \theta/2t=arcsinN​1​=θ/2 (algebraic proof).

Formalization targets

Goal — success probability 1−1/N1 - 1/N1−1/N within ⌈π4N⌉\lceil\frac\pi4\sqrt N\rceil⌈4π​N​⌉ iterations

∃ r≤⌈π4N⌉:∣⟨ω∣(UsUω)r∣s⟩∣2≥1−1N.\exists\, r \le \left\lceil\frac{\pi}{4}\sqrt N\right\rceil:\qquad \bigl|\langle\omega|(U_sU_\omega)^r|s\rangle\bigr|^2 \ge 1 - \frac1N .∃r≤⌈4π​N​⌉:​⟨ω∣(Us​Uω​)r∣s⟩​2≥1−N1​.

This combines the article's headline claims: the algorithm outputs ω\omegaω with probability at least 1/21/21/2 (for N≥2N \ge 2N≥2) using O(N)O(\sqrt N)O(N​) applications of UωU_\omegaUω​, the success probability approaches 111 for N≫1N \gg 1N≫1, and the number of iterations satisfies r(N)≤⌈π4N⌉r(N) \le \lceil\frac\pi4\sqrt N\rceilr(N)≤⌈4π​N​⌉. The goal does not fix rrr.

Milestones

Listed in the article's order.

  1. Alternative oracle definition: Uf(∣x⟩⊗∣−⟩)=(Uω∣x⟩)⊗∣−⟩U_f\bigl(|x\rangle\otimes|-\rangle\bigr) = (U_\omega|x\rangle)\otimes|-\rangleUf​(∣x⟩⊗∣−⟩)=(Uω​∣x⟩)⊗∣−⟩ with ∣−⟩=12(∣0⟩−∣1⟩)|-\rangle = \frac{1}{\sqrt2}(|0\rangle - |1\rangle)∣−⟩=2​1​(∣0⟩−∣1⟩).
  2. Unitarity: UωU_\omegaUω​ and UsU_sUs​ are unitary.
  3. Iteration count: r(N)=⌊π/(4t)⌋≤⌈π4N⌉r(N) = \lfloor\pi/(4t)\rfloor \le \lceil\frac\pi4\sqrt N\rceilr(N)=⌊π/(4t)⌋≤⌈4π​N​⌉.
  4. Geometric proof: on span{∣s′⟩,∣ω⟩}\mathrm{span}\{|s'\rangle,|\omega\rangle\}span{∣s′⟩,∣ω⟩}, UωU_\omegaUω​ is the reflection across ∣s′⟩|s'\rangle∣s′⟩; Uω=I−2∣ω⟩⟨ω∣U_\omega = I - 2|\omega\rangle\langle\omega|Uω​=I−2∣ω⟩⟨ω∣ (Householder form); UsU_sUs​ is the reflection through ∣s⟩|s\rangle∣s⟩; UsUωU_sU_\omegaUs​Uω​ rotates the plane by θ\thetaθ; ⟨s′∣s⟩=(N−1)/N\langle s'|s\rangle = \sqrt{(N-1)/N}⟨s′∣s⟩=(N−1)/N​; and the exact success probability is
∣⟨ω∣(UsUω)r∣s⟩∣2=sin⁡2 ⁣((r+12)θ).\bigl|\langle\omega|(U_sU_\omega)^r|s\rangle\bigr|^2 = \sin^2\!\bigl((r+\tfrac12)\theta\bigr).​⟨ω∣(Us​Uω​)r∣s⟩​2=sin2((r+21​)θ).
  1. Algebraic proof: the action of UsU_sUs​ and UωU_\omegaUω​ on span{∣ω⟩,∣s⟩}\mathrm{span}\{|\omega\rangle,|s\rangle\}span{∣ω⟩,∣s⟩} by explicit 2×22\times 22×2 matrices; the Jordan form UsUω=M diag(e2it,e−2it) M−1U_sU_\omega = M\,\mathrm{diag}(e^{2it},e^{-2it})\,M^{-1}Us​Uω​=Mdiag(e2it,e−2it)M−1 and its rrr-th power; the success probability sin⁡2((2r+1)t)\sin^2((2r+1)t)sin2((2r+1)t) computed in coordinates; and, stopping at r=⌊π/4t⌋r = \lfloor\pi/4t\rfloorr=⌊π/4t⌋, error at most 1/N1/N1/N.

Significance

The result. The goal says that unstructured search over NNN items costs O(N)O(\sqrt N)O(N​) oracle queries on a quantum computer, with failure probability at most 1/N1/N1/N for a single run, and hence that the expected number of queries until ω\omegaω is found is still O(N)O(\sqrt N)O(N​). It is the quantitative content behind the use of Grover's algorithm as a subroutine and behind its role in post-quantum key-length recommendations.

Formalizing it. The result is classical and fully proved on paper. The work here is to formalize the article's two proofs: the reflection/rotation picture and the algebraic diagonalization, together with the equivalence of the two oracle models and the explicit bound ⌈π4N⌉\lceil\frac\pi4\sqrt N\rceil⌈4π​N​⌉ stated in the article. A separate platform mission, Grover's Algorithm, already contains machine-checked proofs of the amplitude formula sin⁡((2k+1)θ)\sin((2k+1)\theta)sin((2k+1)θ) and of a success guarantee with iteration bound ⌈π/(4arcsin⁡(1/N))⌉\lceil\pi/(4\arcsin(1/\sqrt N))\rceil⌈π/(4arcsin(1/N​))⌉, in a model where the oracle is given by the marked index. This mission differs in that it derives the oracle from the function fff, includes the ancilla-based standard oracle, the Householder and reflection statements, the algebraic Jordan-form analysis, and the bound ⌈π4N⌉\lceil\frac\pi4\sqrt N\rceil⌈4π​N​⌉ in terms of N\sqrt NN​. The lower bound of Bennett–Bernstein–Brassard–Vazirani (optimality) is out of scope.

Difficulty

None of the steps is deep; the difficulty lies in the bookkeeping. The plane span{∣ω⟩,∣s⟩}\mathrm{span}\{|\omega\rangle, |s\rangle\}span{∣ω⟩,∣s⟩} is not spanned by an orthonormal pair, so the matrices of the algebraic proof are in a non-orthogonal spanning set, and the probability formula must be transported from that 2×22\times22×2 picture back to the NNN-dimensional state. Passing from the exact formula sin⁡2((r+12)θ)\sin^2((r+\frac12)\theta)sin2((r+21​)θ) to the bound 1−1/N1 - 1/N1−1/N requires choosing an integer rrr, controlling (2r+1)t(2r+1)t(2r+1)t to within ttt of π/2\pi/2π/2, and comparing arcsin⁡(1/N)\arcsin(1/\sqrt N)arcsin(1/N​) with 1/N1/\sqrt N1/N​ to reach ⌈π4N⌉\lceil\frac\pi4\sqrt N\rceil⌈4π​N​⌉. Edge cases matter: N=1N = 1N=1 (where t=π/2t = \pi/2t=π/2, ∣s′⟩|s'\rangle∣s′⟩ is undefined and MMM is singular) and the integer rounding of r=π/4tr = \pi/4tr=π/4t.

Formalization scope

All statements import one definitions file, GroverWiki_Defs, and live in the namespace GroverWiki.

  • States are vectors Fin N → ℂ; operators are matrices Matrix (Fin N) (Fin N) ℂ acting by mulVec; the two-register space is indexed by Fin N × Fin 2. Bit values are Fin 2, so ⊕ is addition in Fin 2.
  • The oracle is built from f : Fin N → Fin 2; uniqueness of the marked item is the hypothesis ∀ x, f x = 1 ↔ x = ω.
  • The measurement probability of outcome x is ‖ψ x‖ ^ 2, applied to the state (U_s U_ω)^r |s⟩.
  • Scalars such as 1/N1/\sqrt N1/N​ are real numbers cast to C\mathbb CC. For N=1N = 1N=1, Lean's conventions give ∣s′⟩=0|s'\rangle = 0∣s′⟩=0; statements about ∣s′⟩|s'\rangle∣s′⟩ or M−1M^{-1}M−1 assume N≥2N \ge 2N≥2, as the article implicitly does.
  • The article's non-integer r=π/4tr = \pi/4tr=π/4t is formalized as ⌊π/4t⌋\lfloor \pi/4t\rfloor⌊π/4t⌋, and "error O(1/N)O(1/N)O(1/N)" as the explicit bound 1/N1/N1/N.

The goal is not trivialized by the model: the state is the actual output of the algorithm, the iteration count is bounded explicitly, and the probability bound is the Born-rule probability of the marked index. Contributions of reusable lemmas on reflections and rotations in two-dimensional subspaces of CN\mathbb C^NCN are welcome.

Selected references

  • L. K. Grover, A fast quantum mechanical algorithm for database search, Proc. 28th ACM STOC, 1996. https://doi.org/10.1145/237814.237866 (arXiv: https://arxiv.org/abs/quant-ph/9605043)
  • C. H. Bennett, E. Bernstein, G. Brassard, U. Vazirani, Strengths and weaknesses of quantum computing, SIAM J. Comput. 26(5), 1997. https://doi.org/10.1137/s0097539796300933
  • M. A. Nielsen, I. L. Chuang, Quantum Computation and Quantum Information, Cambridge University Press, 2010, pp. 276–305. https://doi.org/10.1017/CBO9780511976667
  • Wikipedia, Grover's algorithm, revision 1373498442. https://en.wikipedia.org/w/index.php?title=Grover%27s_algorithm&oldid=1373498442
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AnalysisFunctional AnalysisProbability·Captain: Lucas

Hamburger Moment Problem (Wikipedia) I: Characterization and Uniqueness of SolutionsTextbook

Motivation

A sequence of real numbers (m0,m1,m2,… )(m_0, m_1, m_2, \dots)(m0​,m1​,m2​,…) often arrives as a list of moments: averages E[Xn]\mathbb E[X^n]E[Xn] of powers of a random variable, traces ⟨Tne,e⟩\langle T^n e, e\rangle⟨Tne,e⟩ of powers of a self-adjoint operator, or coefficients of a continued fraction. The Hamburger moment problem, named after Hans Ludwig Hamburger (1920–21), asks when such a list really comes from a measure on the whole real line, and, when it does, whether the measure is determined by its moments. The question sits at the junction of probability (the method of moments, identification of limit laws), spectral theory of symmetric operators and Jacobi matrices, and the theory of orthogonal polynomials; standard monographs include Shohat–Tamarkin (1943) and Schmüdgen (2017).

Timeline (as summarized in the source article and its references):

  1. 1894 — Stieltjes treats the analogous problem on [0,+∞)[0,+\infty)[0,+∞) (the Stieltjes moment problem).
  2. 1920–21 — Hamburger extends the theory to the whole real line: solvability is equivalent to positivity of the Hankel kernel (mj+k)(m_{j+k})(mj+k​).
  3. 1920s — Carleman gives a growth condition on the moments guaranteeing uniqueness (Carleman's condition); the factorial growth bound ∣mn∣≤CDnn!|m_n| \le C D^n n!∣mn​∣≤CDnn! is a special case (Reed–Simon 1975, p. 205).
  4. Later — the operator-theoretic treatment through self-adjoint extensions of the shift operator and its spectral measure becomes standard (Reed–Simon 1975, p. 145).

Setting

Let m=(mn)n≥0m = (m_n)_{n \ge 0}m=(mn​)n≥0​ be a sequence of real numbers. A solution of the Hamburger moment problem for mmm is a positive Borel measure μ\muμ on R\mathbb RR such that every power xnx^nxn is μ\muμ-integrable and

mn=∫−∞∞xn dμ(x)(n=0,1,2,… ).m_n = \int_{-\infty}^{\infty} x^n \, d\mu(x) \qquad (n = 0, 1, 2, \dots).mn​=∫−∞∞​xndμ(x)(n=0,1,2,…).

The sequence mmm is a moment sequence if at least one solution exists.

The Hankel kernel of mmm is the infinite matrix A=(mj+k)j,k≥0A = (m_{j+k})_{j,k \ge 0}A=(mj+k​)j,k≥0​. It is positive definite (in the sense of the source) if

∑j,k≥0mj+k cjck‾  ≥  0\sum_{j,k \ge 0} m_{j+k}\, c_j \overline{c_k} \;\ge\; 0j,k≥0∑​mj+k​cj​ck​​≥0

for every finitary complex sequence (cj)j≥0(c_j)_{j \ge 0}(cj​)j≥0​, i.e. cj=0c_j = 0cj​=0 for all but finitely many jjj. Its finite sections are the (n+1)×(n+1)(n+1)\times(n+1)(n+1)×(n+1) Hankel matrices

Δn=(mi+j)0≤i,j≤n.\Delta_n = (m_{i+j})_{0 \le i,j \le n}.Δn​=(mi+j​)0≤i,j≤n​.

In the Lean development these objects are IsMomentMeasure m μ, IsMomentSequence m, hankelForm m c, HankelPosDef m and hankelMatrix m n, all in the namespace HamburgerMoment.

Formalization targets

Goal — Hamburger's characterization

m is a moment sequence  ⟺  ∑j,k≥0mj+kcjck‾≥0 for every finitary (cj)⊂C.m \text{ is a moment sequence} \iff \sum_{j,k \ge 0} m_{j+k} c_j \overline{c_k} \ge 0 \text{ for every finitary } (c_j) \subset \mathbb C.m is a moment sequence⟺j,k≥0∑​mj+k​cj​ck​​≥0 for every finitary (cj​)⊂C.

Milestones

  1. The identity ∑j,kmj+kcjck‾=∫∣∑jcjxj∣2 dμ(x)\sum_{j,k} m_{j+k} c_j \overline{c_k} = \int |\sum_j c_j x^j|^2 \, d\mu(x)∑j,k​mj+k​cj​ck​​=∫∣∑j​cj​xj∣2dμ(x) for any solution μ\muμ, and the resulting "only if" direction.
  2. The "if" direction: a positive definite Hankel kernel is the kernel of a moment sequence.
  3. The solution set is convex; hence a solvable problem has either a unique solution or infinitely many.
  4. Positivity of AAA gives det⁡Δn≥0\det \Delta_n \ge 0detΔn​≥0 for all nnn; if det⁡Δn=0\det \Delta_n = 0detΔn​=0 for some nnn, the solution is unique and finitely supported.
  5. Uniqueness under the growth bound ∣mn∣≤CDnn!|m_n| \le C D^n n!∣mn​∣≤CDnn!.
  6. Existence of moment sequences with more than one solution.
  7. The real-polynomial identity ∫p2 dμ=∑j,kajakmj+k≥0\int p^2 \, d\mu = \sum_{j,k} a_j a_k m_{j+k} \ge 0∫p2dμ=∑j,k​aj​ak​mj+k​≥0, and the characterization of moment sequences by positive semidefiniteness of all real Hankel matrices Δn\Delta_nΔn​.

Significance

The result. Hamburger's theorem turns an existence question about measures into a family of finite-dimensional positivity conditions that can be checked on the data. It is the basic tool behind the method of moments in probability (identifying a distribution from its moments, when the problem is determinate), behind the spectral theory of Jacobi matrices, and behind Gauss quadrature and orthogonal polynomials on the line. The uniqueness criteria decide when moments determine a law; the non-uniqueness examples (for instance the log-normal distribution) show that they do not always do so.

Formalizing it. All results here are classical and proved in the literature; to the best of the captain's knowledge none of them is currently available as a formal statement in Mathlib, which has neither moment problems nor Hankel kernels. The mission produces a reusable vocabulary (moment measures, Hankel forms and matrices) and machine-checked versions of the existence theorem, the uniqueness criteria and the non-uniqueness phenomenon.

Difficulty

The "only if" direction is a direct computation. The converse is the substance: from positivity of countably many finite quadratic forms one must produce a countably additive measure on a non-compact space with all moments matching. Compactness arguments on finite sections give measures whose low-order moments match, but mass can escape to infinity and higher moments need not converge; the source's route instead goes through the Hilbert space completion of finitary sequences, self-adjoint extensions of the (generally unbounded) shift operator and the spectral theorem for unbounded self-adjoint operators — machinery that is only partly present in Mathlib. An alternative route via positive linear functionals on polynomials (M. Riesz extension, Riesz–Markov–Kakutani) has to control the same escape of mass. The uniqueness criterion requires quasi-analyticity or Carleman-type estimates.

Formalization scope

  1. Sequences are m : ℕ → ℝ; measures are Measure ℝ on the Borel σ-algebra of R\mathbb RR. A solution must have every power xnx^nxn integrable, so in particular μ\muμ is finite with total mass m0m_0m0​.
  2. Finitary complex sequences are finitely supported functions ℕ →₀ ℂ, and the Hankel form is the finite double sum over the support. "≥0\ge 0≥0" is the order on C\mathbb CC (the value is a nonnegative real number), matching the source.
  3. Δn\Delta_nΔn​ is the real matrix indexed by Fin (n + 1); positive semidefiniteness is Mathlib's Matrix.PosSemidef.
  4. Uniqueness statements quantify over all solutions; finite support means the solution vanishes outside a finite set.

Needed infrastructure and welcome contributions: polynomial integrability under finite moments, positive linear functionals on R[x]\mathbb R[x]R[x], a Riesz–Markov or spectral-measure construction on R\mathbb RR, Vandermonde arguments for finitely supported measures, and Carleman / quasi-analyticity estimates. The definitions of moment measures and Hankel kernels are reusable for the Stieltjes and Hausdorff moment problems.

Selected references

  • Wikipedia, Hamburger moment problem, revision oldid=1356180072, https://en.wikipedia.org/w/index.php?title=Hamburger_moment_problem&oldid=1356180072
  • H. Hamburger, Über eine Erweiterung des Stieltjesschen Momentenproblems, Math. Ann. 81 (1920), 235–319; 82 (1921), 120–164, 168–187.
  • M. Reed, B. Simon, Methods of Modern Mathematical Physics II: Fourier Analysis, Self-Adjointness, Academic Press, 1975, pp. 145, 205.
  • T. S. Chihara, An Introduction to Orthogonal Polynomials, Gordon and Breach, 1978, pp. 56, 73.
  • K. Schmüdgen, The Moment Problem, Graduate Texts in Mathematics 277, Springer, 2017. https://doi.org/10.1007/978-3-319-64546-9
  • J. A. Shohat, J. D. Tamarkin, The Problem of Moments, AMS, 1943.
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Number TheoryQuantum Information·Captain: Lucas

Shor's Algorithm (Wikipedia): Quantum Order Finding and the Reduction of FactoringTextbook

Motivation

Shor's algorithm is a quantum algorithm that finds a nontrivial factor of an integer NNN in time polynomial in log⁡N\log NlogN, and its variants compute discrete logarithms in finite cyclic groups. It was developed by Peter Shor in 1994 (Shor, FOCS 1994; Shor, SIAM J. Comput. 1997). No classical polynomial-time factoring algorithm is known; the best classical method, the general number field sieve, runs in sub-exponential time. Because the security of RSA and of finite-field and elliptic-curve Diffie–Hellman rests on the hardness of factoring and of discrete logarithms, Shor's algorithm is the main reason these schemes are considered breakable by a large fault-tolerant quantum computer, and the main motivation for post-quantum cryptography.

This mission follows the presentation of the algorithm in the Wikipedia article Shor's algorithm (revision 1378862216), which describes the quantum part through quantum phase estimation, an approach due to Kitaev (Kitaev 1995) and standard in textbooks (Nielsen–Chuang 2010).

Setting

Let 1<a<N1 < a < N1<a<N be integers with gcd⁡(a,N)=1\gcd(a, N) = 1gcd(a,N)=1. The order r=ord⁡N(a)r = \operatorname{ord}_N(a)r=ordN​(a) is the smallest positive integer with ar≡1(modN)a^r \equiv 1 \pmod Nar≡1(modN).

Classical reduction. If rrr is even and N∤ar/2+1N \nmid a^{r/2}+1N∤ar/2+1, then gcd⁡(N,ar/2−1)\gcd(N, a^{r/2}-1)gcd(N,ar/2−1) is a nontrivial factor of NNN. Factoring therefore reduces to computing orders.

Quantum order finding. Let n=⌈log⁡2N⌉n = \lceil\log_2 N\rceiln=⌈log2​N⌉ and Q=22nQ = 2^{2n}Q=22n. A state of an mmm-qubit register is a vector in C2m\mathbb C^{2^m}C2m with standard basis ∣0⟩,…,∣2m−1⟩|0\rangle, \dots, |2^m-1\rangle∣0⟩,…,∣2m−1⟩. The modular-multiplication gate is the nnn-qubit gate

U∣k⟩=∣ak mod N⟩ (0≤k<N),U∣k⟩=∣k⟩ (N≤k<2n).U|k\rangle = |ak \bmod N\rangle \ (0 \le k < N), \qquad U|k\rangle = |k\rangle \ (N \le k < 2^n).U∣k⟩=∣akmodN⟩ (0≤k<N),U∣k⟩=∣k⟩ (N≤k<2n).

With ωr=e2πi/r\omega_r = e^{2\pi i/r}ωr​=e2πi/r, the states ∣ψj⟩=r−1/2∑k=0r−1ωr−kj∣ak mod N⟩|\psi_j\rangle = r^{-1/2}\sum_{k=0}^{r-1}\omega_r^{-kj}|a^k \bmod N\rangle∣ψj​⟩=r−1/2∑k=0r−1​ωr−kj​∣akmodN⟩ are eigenvectors of UUU with eigenvalues ωrj\omega_r^jωrj​. The order-finding circuit acts on a 2n2n2n-qubit first register and the nnn-qubit second register: Hadamard gates H⊗2nH^{\otimes 2n}H⊗2n on the first register, controlled gates C-U2iC\text{-}U^{2^i}C-U2i for i=0,…,2n−1i = 0, \dots, 2n-1i=0,…,2n−1 (qubit iii of the first register controls U2iU^{2^i}U2i on the second), and the inverse quantum Fourier transform QFT22n−1\mathrm{QFT}^{-1}_{2^{2n}}QFT22n−1​ on the first register. It is applied to ∣0⟩⊗2n∣1⟩|0\rangle^{\otimes 2n}|1\rangle∣0⟩⊗2n∣1⟩ and the first register is measured, producing an outcome k∈{0,…,Q−1}k \in \{0, \dots, Q-1\}k∈{0,…,Q−1} with probability P(k)P(k)P(k). Finally the continued fractions algorithm is run on k/Qk/Qk/Q.

Formalization targets

Goal: one run of the order-finding subroutine

For every j∈{0,…,r−1}j \in \{0, \dots, r-1\}j∈{0,…,r−1},

∑k : ∣k/22n−j/r∣≤2−(2n+1)P(k)  ≥  4π2r,\sum_{k\,:\,|k/2^{2n} - j/r| \le 2^{-(2n+1)}} P(k) \;\ge\; \frac{4}{\pi^2 r},k:∣k/22n−j/r∣≤2−(2n+1)∑​P(k)≥π2r4​,

and for every such kkk some continued fraction convergent of k/22nk/2^{2n}k/22n equals j/rj/rj/r in lowest terms, i.e. has numerator j/gcd⁡(j,r)j/\gcd(j,r)j/gcd(j,r) and denominator r/gcd⁡(j,r)r/\gcd(j,r)r/gcd(j,r). Summed over jjj, a single run yields with probability at least 4/π24/\pi^24/π2 an outcome from which the continued fractions algorithm recovers some j/rj/rj/r in lowest terms.

Milestones

  1. Classical reduction (article section "Classical reduction"): gcd⁡(a,N)≠1\gcd(a,N) \ne 1gcd(a,N)=1 is a nontrivial factor; N∣(ar/2−1)(ar/2+1)N \mid (a^{r/2}-1)(a^{r/2}+1)N∣(ar/2−1)(ar/2+1) for even rrr; N∤ar/2−1N \nmid a^{r/2}-1N∤ar/2−1; and gcd⁡(N,ar/2∓1)\gcd(N, a^{r/2} \mp 1)gcd(N,ar/2∓1) are nontrivial factors when N∤ar/2+1N \nmid a^{r/2}+1N∤ar/2+1.
  2. Spectrum of UUU (section "Quantum phase estimation"): Ur=IU^r = IUr=I; every eigenvalue is some ωrk\omega_r^kωrk​; U∣ψj⟩=ωrj∣ψj⟩U|\psi_j\rangle = \omega_r^j|\psi_j\rangleU∣ψj​⟩=ωrj​∣ψj​⟩; ∑jωrjk=0\sum_{j}\omega_r^{jk} = 0∑j​ωrjk​=0 for 1≤k≤r−11 \le k \le r-11≤k≤r−1; r−1/2∑j∣ψj⟩=∣1⟩r^{-1/2}\sum_j|\psi_j\rangle = |1\rangler−1/2∑j​∣ψj​⟩=∣1⟩.
  3. Phase estimation: on ∣0⟩⊗2n∣ψj⟩|0\rangle^{\otimes 2n}|\psi_j\rangle∣0⟩⊗2n∣ψj​⟩ the circuit outputs ∣ϕj⟩∣ψj⟩|\phi_j\rangle|\psi_j\rangle∣ϕj​⟩∣ψj​⟩ with ∣⟨k∣ϕj⟩∣2≥4/π2|\langle k|\phi_j\rangle|^2 \ge 4/\pi^2∣⟨k∣ϕj​⟩∣2≥4/π2 at every nearest integer kkk to 22nj/r2^{2n}j/r22nj/r; on ∣0⟩⊗2n∣1⟩|0\rangle^{\otimes 2n}|1\rangle∣0⟩⊗2n∣1⟩ each ∣ϕj⟩|\phi_j\rangle∣ϕj​⟩ is found with probability 1/r1/r1/r.
  4. Continued fractions and register size (section "Choosing the size of the first register"): ∣j/r−φ∣<1/(2r2)|j/r - \varphi| < 1/(2r^2)∣j/r−φ∣<1/(2r2) implies φ\varphiφ has j/rj/rj/r in lowest terms as a convergent, and 2−(2n+1)≤1/(2N2)≤1/(2r2)2^{-(2n+1)} \le 1/(2N^2) \le 1/(2r^2)2−(2n+1)≤1/(2N2)≤1/(2r2).
  5. Discrete logarithms (section "Shor's algorithm for discrete logarithms"): f(a,b)=gax−bf(a,b) = g^a x^{-b}f(a,b)=gax−b on Zp×Zp\mathbb Z_p \times \mathbb Z_pZp​×Zp​ is a homomorphism with kernel the multiples of (r,1)(r,1)(r,1).

Significance

The goal is the quantitative statement behind the article's claim that phase estimation "gives as output a random integer of the form jr22n\frac{j}{r}2^{2n}rj​22n" and that a 2n2n2n-qubit first register suffices to recover j/rj/rj/r. Combined with the classical milestones, it is the correctness argument of Shor's factoring algorithm, minus the separate number-theoretic estimate of how often a random aaa has even order with ar/2≢−1a^{r/2} \not\equiv -1ar/2≡−1, which the article does not state.

The results are classical and their proofs are published. The work this mission asks for is a machine-checked proof against an explicit gate-level model of the circuit — Hadamard tensor power, controlled modular-multiplication gates, inverse QFT — rather than against a closed-form output distribution assumed up front. Related missions on the platform formalize Shor's 1997 paper, which analyses the circuit by a direct Fourier-sum computation with q≥N2q \ge N^2q≥N2; this mission follows the phase-estimation route with the article's constants.

Difficulty

The spectral facts about UUU and the classical reduction are short arguments. The main obstacle is the circuit: showing that the product of the 2n2n2n controlled gates C-U2iC\text{-}U^{2^i}C-U2i acts on ∣x⟩∣ψj⟩|x\rangle|\psi_j\rangle∣x⟩∣ψj​⟩ as multiplication by ωrjx\omega_r^{jx}ωrjx​ requires the binary expansion of xxx and the commutation of the controlled gates, and the subsequent inverse QFT must be computed explicitly. The bound 4/π24/\pi^24/π2 requires an estimate of ∣∑x<Qe2πixδ∣\left|\sum_{x<Q} e^{2\pi i x\delta}\right|​∑x<Q​e2πixδ​ for ∣δ∣≤1/(2Q)|\delta| \le 1/(2Q)∣δ∣≤1/(2Q) which is uniform in QQQ; a crude estimate gives a weaker constant. The measurement identity P(k)=1r∑jPj(k)P(k) = \frac1r\sum_j P_j(k)P(k)=r1​∑j​Pj​(k) requires the orthonormality of the ∣ψj⟩|\psi_j\rangle∣ψj​⟩, which uses that a0,…,ar−1a^0, \dots, a^{r-1}a0,…,ar−1 are distinct modulo NNN.

Formalization scope

States are coordinate vectors Fin d → ℂ, gates are complex matrices acting by Matrix.mulVec, two-register operators are Kronecker products on Fin d₁ × Fin d₂, and measurement probabilities are sums of squared moduli. The order is orderOf (a : ZMod N) and nnn is Nat.clog 2 N. Convergents are Mathlib's Real.convergent, the standard continued fraction expansion. The goal is a statement about the specific circuit defined in the mission's definition file, so it cannot be satisfied by choosing a convenient output distribution, and the recovery statement is quantified over a fixed jjj, so the trivial convergent ⌊k/Q⌋=0\lfloor k/Q\rfloor = 0⌊k/Q⌋=0 (which equals 0/r0/r0/r) does not discharge it for j≠0j \ne 0j=0.

Reusable infrastructure welcome from this mission: the action of the Kronecker-product phase estimation circuit on eigenstates, the explicit inverse QFT computation, and the 4/π24/\pi^24/π2 estimate for the Fejér-type kernel.

Selected references

  • P. W. Shor, Algorithms for quantum computation: discrete logarithms and factoring, Proc. 35th FOCS, 1994. https://doi.org/10.1109/sfcs.1994.365700
  • P. W. Shor, Polynomial-time algorithms for prime factorization and discrete logarithms on a quantum computer, SIAM J. Comput. 26(5), 1997. https://arxiv.org/abs/quant-ph/9508027
  • A. Yu. Kitaev, Quantum measurements and the Abelian stabilizer problem, 1995. https://arxiv.org/abs/quant-ph/9511026
  • M. A. Nielsen, I. L. Chuang, Quantum Computation and Quantum Information, Cambridge University Press, 2010. https://doi.org/10.1017/CBO9780511976667
  • Wikipedia, Shor's algorithm, revision 1378862216. https://en.wikipedia.org/w/index.php?title=Shor%27s_algorithm&oldid=1378862216
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Differential Geometry·Captain: Lucas

Generalized Complex Structures I: Linear Algebra of Generalized Almost Complex StructuresTextbook

Motivation

Generalized complex geometry, introduced by N. Hitchin (Generalized Calabi–Yau manifolds, 2003) and developed by M. Gualtieri (thesis, 2004; Annals 2011), treats complex and symplectic structures as two special cases of one notion. It replaces the tangent bundle TTT of a manifold by the generalized tangent bundle T⊕T∗T\oplus T^*T⊕T∗ and an almost complex structure on TTT by an orthogonal almost complex structure on T⊕T∗T\oplus T^*T⊕T∗. The framework is used in string theory: supersymmetric flux compactifications require (possibly twisted) generalized complex structures (Graña 2006).

The pointwise theory is pure linear algebra, and the global statements of the subject rest on it: the equivalence between a generalized almost complex structure and its −1\sqrt{-1}−1​-eigenbundle, Gualtieri's classification of maximal isotropic subspaces by pairs (E,ε)(E,\varepsilon)(E,ε), the type invariant and its behaviour under B-field shifts, and the two model examples (complex and symplectic). This mission formalizes that linear-algebraic layer as presented in the Wikipedia article Generalized complex structure.

Setting

Fix N≥0N\ge 0N≥0. A fiber of the tangent bundle is T=RNT=\mathbb R^NT=RN; its dual T∗T^*T∗ is identified with RN\mathbb R^NRN through the standard dual basis, so a one-form ξ\xiξ acts by ξ(Y)=∑iξiYi\xi(Y)=\sum_i\xi_iY_iξ(Y)=∑i​ξi​Yi​. The generalized tangent space is T⊕T∗T\oplus T^*T⊕T∗, whose elements are formal sums X+ξX+\xiX+ξ, with the natural inner product of signature (N,N)(N,N)(N,N)

⟨X+ξ,  Y+η⟩=12(ξ(Y)+η(X)).\langle X+\xi,\;Y+\eta\rangle=\tfrac12\bigl(\xi(Y)+\eta(X)\bigr).⟨X+ξ,Y+η⟩=21​(ξ(Y)+η(X)).

The same formula defines a complex bilinear form on the complexification (T⊕T∗)⊗C=CN⊕CN(T\oplus T^*)\otimes\mathbb C=\mathbb C^N\oplus\mathbb C^N(T⊕T∗)⊗C=CN⊕CN, which carries the complex conjugation v↦vˉv\mapsto\bar vv↦vˉ.

  1. A generalized almost complex structure is a real linear map J:T⊕T∗→T⊕T∗\mathcal J:T\oplus T^*\to T\oplus T^*J:T⊕T∗→T⊕T∗ with J2=−Id\mathcal J^2=-\mathrm{Id}J2=−Id and ⟨Ju,Jv⟩=⟨u,v⟩\langle\mathcal J u,\mathcal J v\rangle=\langle u,v\rangle⟨Ju,Jv⟩=⟨u,v⟩.
  2. Its −1\sqrt{-1}−1​-eigenbundle is L={v∈(T⊕T∗)⊗C: Jv=−1 v}L=\{v\in(T\oplus T^*)\otimes\mathbb C:\ \mathcal J v=\sqrt{-1}\,v\}L={v∈(T⊕T∗)⊗C: Jv=−1​v}; Lˉ\bar LLˉ denotes the conjugate subspace.
  3. A subspace LLL is isotropic if ⟨ℓ,ℓ′⟩=0\langle\ell,\ell'\rangle=0⟨ℓ,ℓ′⟩=0 for all ℓ,ℓ′∈L\ell,\ell'\in Lℓ,ℓ′∈L, and maximal isotropic if moreover dim⁡L=N\dim L=NdimL=N.
  4. For a subspace E⊆TE\subseteq TE⊆T and a bilinear form ε\varepsilonε on EEE, L(E,ε)={X+ξ: X∈E, ξ∣E=ε(X,⋅)}L(E,\varepsilon)=\{X+\xi:\ X\in E,\ \xi|_E=\varepsilon(X,\cdot)\}L(E,ε)={X+ξ: X∈E, ξ∣E​=ε(X,⋅)}.
  5. The type of a complex subspace LLL is 2N2N2N minus the real dimension of its projection πT(L)\pi_T(L)πT​(L) to T⊗CT\otimes\mathbb CT⊗C, i.e. 2 (N−dim⁡CπT(L))2\,(N-\dim_{\mathbb C}\pi_T(L))2(N−dimC​πT​(L)); the real index is r=dim⁡C(L∩Lˉ)r=\dim_{\mathbb C}(L\cap\bar L)r=dimC​(L∩Lˉ).
  6. The B-field shift by a 2-form BBB is eB(X+ξ)=X+ξ+iXBe^B(X+\xi)=X+\xi+i_XBeB(X+ξ)=X+ξ+iX​B.
  7. An almost complex structure J0J_0J0​ on TTT gives JJ0(X+ξ)=−J0X+ξ∘J0\mathcal J_{J_0}(X+\xi)=-J_0X+\xi\circ J_0JJ0​​(X+ξ)=−J0​X+ξ∘J0​; a nondegenerate 2-form ω\omegaω gives Jω(X+ξ)=−(ω♭)−1ξ+ω♭X\mathcal J_\omega(X+\xi)=-(\omega^\flat)^{-1}\xi+\omega^\flat XJω​(X+ξ)=−(ω♭)−1ξ+ω♭X with ω♭X=iXω\omega^\flat X=i_X\omegaω♭X=iX​ω.

Formalization targets

Goal: the eigenbundle correspondence

For every generalized almost complex structure J\mathcal JJ, its eigenbundle LLL satisfies

(i) L∩Lˉ=0,(ii) L is maximal isotropic,\text{(i)}\ L\cap\bar L=0,\qquad\text{(ii)}\ L\ \text{is maximal isotropic},(i) L∩Lˉ=0,(ii) L is maximal isotropic,

and conversely every complex subspace LLL satisfying (i) and (ii) is the −1\sqrt{-1}−1​-eigenbundle of a unique generalized almost complex structure. Hence (i), (ii) form an alternative definition of generalized almost complex structure.

Milestones

  1. The eigenbundle of J\mathcal JJ satisfies (i) and (ii).
  2. J\mathcal JJ is uniquely determined by its eigenbundle.
  3. Every LLL satisfying (i), (ii) is the eigenbundle of some J\mathcal JJ.
  4. L(E,ε)L(E,\varepsilon)L(E,ε) is maximal isotropic whenever ε\varepsilonε is a 2-form (real or complex case).
  5. Every maximal isotropic subspace has the form L(E,ε)L(E,\varepsilon)L(E,ε) (Gualtieri).
  6. The pair (E,ε)(E,\varepsilon)(E,ε) is determined by L(E,ε)L(E,\varepsilon)L(E,ε).
  7. A generalized almost complex structure has type at most NNN.
  8. B-field shifts are isometries of T⊕T∗T\oplus T^*T⊕T∗.
  9. The type is invariant under B-field shifts.
  10. A maximal isotropic LLL is the eigenbundle of a generalized almost complex structure iff r=0r=0r=0.
  11. Complex structures give generalized almost complex structures of type NNN.
  12. Nondegenerate 2-forms give generalized almost complex structures of type 000.
  13. Up to a B-field shift, the symplectic ones are the only structures of type 000.

Significance

The goal makes the two descriptions of a generalized almost complex structure interchangeable: integrability (closure of LLL under the Courant bracket), the canonical pure-spinor line and the type are all phrased in terms of LLL, while the definition is phrased in terms of J\mathcal JJ. The classification by (E,ε)(E,\varepsilon)(E,ε) is the normal form behind the type, the local classification near regular points, and the identification of the complex and symplectic extremes. All of these results are classical and proved in the cited literature; the remaining work is their machine-checked formalization. A formal library of this linear algebra is a prerequisite for later missions on the manifold-level theory (Courant bracket, generalized Darboux theorem).

Difficulty

The goal mixes real and complex linear algebra. Recovering a real map J\mathcal JJ from a complex subspace LLL requires knowing that L⊕LˉL\oplus\bar LL⊕Lˉ is the whole complexification and that the map which is −1\sqrt{-1}−1​ on LLL and −−1-\sqrt{-1}−−1​ on Lˉ\bar LLˉ commutes with conjugation and is orthogonal; each of these uses hypotheses (i) and (ii), and the dimension condition dim⁡L=N\dim L=NdimL=N cannot be dropped. The classification needs a dimension count for L(E,ε)L(E,\varepsilon)L(E,ε) (functionals on EEE versus the annihilator of EEE) and, in the converse direction, the extraction of ε\varepsilonε from an arbitrary maximal isotropic subspace. For the complex example, the type computation requires the dimension of the −−1-\sqrt{-1}−−1​-eigenspace of a real complex structure, which is exactly N/2N/2N/2.

Formalization scope

Everything is fiberwise and in coordinates: T=RNT=\mathbb R^NT=RN is Fin N → ℝ, T⊕T∗T\oplus T^*T⊕T∗ is GIdx N → ℝ with GIdx N = Fin N ⊕ Fin N (vector part on Sum.inl, one-form part on Sum.inr), endomorphisms are matrices over GIdx N, and the complexification is GIdx N → ℂ with the real matrix acting through R→C\mathbb R\to\mathbb CR→C. 2-forms on TTT are skew matrices BBB with B(X,Y)=XTBYB(X,Y)=X^{\mathsf T}BYB(X,Y)=XTBY; 2-forms on a subspace EEE are skew bilinear forms on EEE. Nondegeneracy of ω\omegaω is det⁡ω≠0\det\omega\neq0detω=0 (the inverse used in Jω\mathcal J_\omegaJω​ is the matrix inverse). The type uses the article's real-dimension convention, so it is twice Gualtieri's complex type. The classification milestones are stated over RCLike fields, i.e. for both R\mathbb RR and C\mathbb CC, as in the article.

Out of scope for this mission: the Courant bracket and integrability, the canonical (pure spinor) bundle, upper semicontinuity of the type, the generalized Darboux theorem, local holomorphicity, and the GGG-structure description. These need manifold-level infrastructure (Lie derivatives and exterior derivatives of forms on manifolds) and are left for later missions.

Selected references

  • N. Hitchin, Generalized Calabi–Yau manifolds, Q. J. Math. 54 (2003) 281–308. https://doi.org/10.1093/qmath/hag025
  • M. Gualtieri, Generalized complex geometry, PhD thesis, Oxford, 2004. https://arxiv.org/abs/math.DG/0401221
  • M. Gualtieri, Generalized complex geometry, Ann. of Math. 174 (2011) 75–123. https://arxiv.org/abs/0911.0993
  • M. Graña, Flux compactifications in string theory: a comprehensive review, Phys. Rep. 423 (2006) 91–158. https://arxiv.org/abs/hep-th/0509003
  • Wikipedia, Generalized complex structure (revision 1288019306). https://en.wikipedia.org/w/index.php?title=Generalized_complex_structure&oldid=1288019306
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Mathematical Physics·Captain: Lucas

Giddings 1999: Boundary S matrix and the AdS/CFT dictionary — free-field spectrum on global AdSResearch Paper

Motivation

The AdS/CFT correspondence (Maldacena 1997) relates quantum gravity on anti-de Sitter (AdS) space to a conformal field theory (CFT) living on its timelike boundary. Gubser–Klebanov–Polyakov and Witten gave the CFT-from-AdS direction of the dictionary: CFT correlators are computed from bulk Green functions. Giddings (PRL 83, 2707, 1999) supplies an entry in the reverse direction. Because AdS confines particles and has no ordinary asymptotic states, a flat-space S matrix does not exist; the paper defines a boundary S matrix from in/out states built out of wave packets incident from the boundary, derives an LSZ-type reduction formula (eq. 42), and concludes that the boundary S matrix equals the boundary CFT correlator (eqs. 44–45).

Every step of that argument rests on the classical theory of the free Klein–Gordon field on global AdS: the parameters h±,νh_\pm,\nuh±​,ν (eq. 4), the discrete normalizable spectrum ωnl=2h++2n+l\omega_{nl}=2h_++2n+lωnl​=2h+​+2n+l with modes behaving like (cos⁡r)2h+(\cos r)^{2h_+}(cosr)2h+​ at the boundary (eqs. 5–7), the non-normalizable modes behaving like (cos⁡r)2h−(\cos r)^{2h_-}(cosr)2h−​ (eqs. 8–9), and the boundary limit (eqs. 19–20) that fixes the normalization 2ν2\nu2ν of the bulk–boundary propagator.

Setting

Fix an integer d≥2d\ge 2d≥2, an AdS radius R>0R>0R>0 and a scalar mass m∈Rm\in\mathbb Rm∈R. Global AdSd+1\mathrm{AdS}_{d+1}AdSd+1​ has metric (eq. 2)

ds2=R2sec⁡2r (−dt2+dr2+sin⁡2r dΩd−12),0≤r<π2.ds^2=R^2\sec^2 r\,\bigl(-dt^2+dr^2+\sin^2 r\,d\Omega_{d-1}^2\bigr),\qquad 0\le r<\tfrac\pi2 .ds2=R2sec2r(−dt2+dr2+sin2rdΩd−12​),0≤r<2π​.

Define (eq. 4)

ν=12d2+4m2R2,2h±=d2±ν.\nu=\tfrac12\sqrt{d^2+4m^2R^2},\qquad 2h_\pm=\tfrac d2\pm\nu .ν=21​d2+4m2R2​,2h±​=2d​±ν.

A mode ϕ=e−iωtYlm⃗(Ω)χ(r)\phi=e^{-i\omega t}Y_{l\vec m}(\Omega)\chi(r)ϕ=e−iωtYlm​(Ω)χ(r), with Ylm⃗Y_{l\vec m}Ylm​ a spherical harmonic on Sd−1S^{d-1}Sd−1, solves the free equation (□−m2)ϕ=0(\Box-m^2)\phi=0(□−m2)ϕ=0 (eq. 3) exactly when the radial profile χ\chiχ satisfies, on 0<r<π/20<r<\pi/20<r<π/2,

χ′′+d−1sin⁡rcos⁡rχ′+ω2χ−l(l+d−2)sin⁡2rχ−m2R2cos⁡2rχ=0.\chi''+\frac{d-1}{\sin r\cos r}\chi'+\omega^2\chi-\frac{l(l+d-2)}{\sin^2 r}\chi-\frac{m^2R^2}{\cos^2 r}\chi=0 .χ′′+sinrcosrd−1​χ′+ω2χ−sin2rl(l+d−2)​χ−cos2rm2R2​χ=0.

A normalizable mode is a nonzero C2C^2C2 solution that is bounded as r→0r\to0r→0 (regular at the centre of AdS) and has finite Klein–Gordon norm, i.e. ∫0π/2tan⁡d−1r χ(r)2 dr<∞\int_0^{\pi/2}\tan^{d-1}r\,\chi(r)^2\,dr<\infty∫0π/2​tand−1rχ(r)2dr<∞. The explicit modes of eq. (5) are

χnl(r)=sin⁡lr (cos⁡r)2h+ Pn(l+d/2−1,  ν)(cos⁡2r),\chi_{nl}(r)=\sin^l r\,(\cos r)^{2h_+}\,P_n^{(l+d/2-1,\;\nu)}(\cos 2r),χnl​(r)=sinlr(cosr)2h+​Pn(l+d/2−1,ν)​(cos2r),

with Pn(α,β)P_n^{(\alpha,\beta)}Pn(α,β)​ the Jacobi polynomial, and the eigenfrequencies of eq. (7) are ωnl=2h++2n+l\omega_{nl}=2h_++2n+lωnl​=2h+​+2n+l.

Formalization targets

Goal: the normalizable spectrum (eqs. 3–7)

For every ω∈R\omega\in\mathbb Rω∈R, l∈Nl\in\mathbb Nl∈N and radial profile χ\chiχ,

χ is a normalizable mode at (ω,l)  ⟺  ∃n∈N: ∣ω∣=ωnl and χ=c χnl on (0,π2) for some c≠0.\chi \text{ is a normalizable mode at }(\omega,l)\iff \exists n\in\mathbb N:\ |\omega|=\omega_{nl}\ \text{and}\ \chi=c\,\chi_{nl}\text{ on }(0,\tfrac\pi2)\text{ for some }c\neq0 .χ is a normalizable mode at (ω,l)⟺∃n∈N: ∣ω∣=ωnl​ and χ=cχnl​ on (0,2π​) for some c=0.

Milestones

  1. Eq. (4): 2h±2h_\pm2h±​ are the two roots of Δ(Δ−d)=m2R2\Delta(\Delta-d)=m^2R^2Δ(Δ−d)=m2R2, and 2h+−2h−=2ν2h_+-2h_-=2\nu2h+​−2h−​=2ν.
  2. Eqs. (5), (7): χnl\chi_{nl}χnl​ solves the radial equation at ω=ωnl\omega=\omega_{nl}ω=ωnl​.
  3. Eq. (6): χnl(r)/(cos⁡r)2h+→knl≠0\chi_{nl}(r)/(\cos r)^{2h_+}\to k_{nl}\neq0χnl​(r)/(cosr)2h+​→knl​=0 as r→π/2r\to\pi/2r→π/2.
  4. Eq. (5): χnl\chi_{nl}χnl​ is a normalizable mode at (ωnl,l)(\omega_{nl},l)(ωnl​,l).
  5. Eqs. (8)–(9): for ∣ω∣|\omega|∣ω∣ outside the spectrum there is a solution regular at r=0r=0r=0 with χ(r)/(cos⁡r)2h−→1\chi(r)/(\cos r)^{2h_-}\to1χ(r)/(cosr)2h−​→1.
  6. Eqs. (19)–(20): lim⁡r→π/2(tan⁡r)d−1[(cos⁡r)2h−∂r↔(cos⁡r)2h+]=−2ν\displaystyle\lim_{r\to\pi/2}(\tan r)^{d-1}\bigl[(\cos r)^{2h_-}\overleftrightarrow{\partial_r}(\cos r)^{2h_+}\bigr]=-2\nur→π/2lim​(tanr)d−1[(cosr)2h−​∂r​​(cosr)2h+​]=−2ν.
  7. Eqs. (12), (33): Δb>Δ⇒(cos⁡r)Δb−Δ→0\Delta_b>\Delta\Rightarrow(\cos r)^{\Delta_b-\Delta}\to0Δb​>Δ⇒(cosr)Δb​−Δ→0.
  8. Eqs. (23), (42)–(44): given Witten's formula (43), the LSZ expression (42) built from the wave packets (23) equals ∫∏a[dba fa(ba)/Za] ⟨T∏aO(ba)⟩\int\prod_a[db_a\,f_a(b_a)/Z_a]\,\langle T\prod_a\mathcal O(b_a)\rangle∫∏a​[dba​fa​(ba​)/Za​]⟨T∏a​O(ba​)⟩.

Significance

The goal is the precise mathematical content behind the paper's statement that free solutions "exist at arbitrary frequency but are only normalizable for a discrete set of frequencies". This spectrum is what makes the boundary operators aωlm⃗a_{\omega l\vec m}aωlm​ of eq. (25) act as creation and annihilation operators (eqs. 27–29), and the boundary exponents 2h±2h_\pm2h±​ and the constant 2ν2\nu2ν determine the normalizations in eqs. (20), (21), (28) and (29). The physics derivation of eqs. (28)–(42) is not rigorous mathematics; milestone 8 isolates the final step from (42)–(43) to (44), which is an exact identity about integral kernels.

The radial results are classical (the paper attributes the explicit solutions to Balasubramanian–Kraus–Lawrence). This mission asks for machine-checked proofs of these results, together with the reusable Jacobi-polynomial and boundary-asymptotics infrastructure they require.

Difficulty

Verifying that χnl\chi_{nl}χnl​ solves the equation is a computation. The goal's converse direction is the hard part: one must show that a solution regular at r=0r=0r=0 can have finite Klein–Gordon norm only when ∣ω∣|\omega|∣ω∣ equals some ωnl\omega_{nl}ωnl​, and that it is then unique up to a scalar. This requires controlling both regular singular points r=0r=0r=0 and r=π/2r=\pi/2r=π/2 of the radial equation, including the resonant cases where 2ν2\nu2ν or l+d/2−1l+d/2-1l+d/2−1 is an integer and logarithms appear. Since d≥2d\ge2d≥2 forces ν≥1\nu\ge1ν≥1, the (cos⁡r)2h−(\cos r)^{2h_-}(cosr)2h−​ branch is never square-integrable, so the second quantization available for 0<ν<10<\nu<10<ν<1 does not arise.

Formalization scope

  • ddd is a natural number with d≥2d\ge2d≥2; m,Rm,Rm,R are real with R>0R>0R>0; l,nl,nl,n are natural numbers; ω\omegaω is real and only ∣ω∣|\omega|∣ω∣ matters.
  • Radial profiles are real-valued functions R→R\mathbb R\to\mathbb RR→R; only their values on (0,π/2)(0,\pi/2)(0,π/2) enter any definition. Complex modes reduce to their real and imaginary parts.
  • Regularity at the origin is encoded as boundedness of ∣χ∣|\chi|∣χ∣ on (0,π/4](0,\pi/4](0,π/4]. Finite Klein–Gordon norm is integrability of tan⁡d−1r χ(r)2\tan^{d-1}r\,\chi(r)^2tand−1rχ(r)2 on (0,π/2)(0,\pi/2)(0,π/2).
  • The Jacobi polynomial is defined by the explicit finite sum with generalized binomial coefficients. Powers of cos⁡r\cos rcosr with real exponents use Real.rpow; cos⁡r>0\cos r>0cosr>0 on the relevant range.
  • Nontriviality (χ≠0\chi\neq0χ=0 somewhere) is part of the definition of a normalizable mode, so the zero function never counts.
  • Milestone 8 takes the LSZ right-hand side (42) as the definition of the boundary S matrix and Witten's relation (43) as a hypothesis, with joint integrability of the integrand. In- and out-packets are listed together, and the plane-wave limit (45) is not formalized.

Selected references

  • S. B. Giddings, Boundary S matrix and the anti–de Sitter space to conformal field theory dictionary, Phys. Rev. Lett. 83, 2707 (1999). https://doi.org/10.1103/PhysRevLett.83.2707
  • V. Balasubramanian, P. Kraus, A. Lawrence, Bulk vs. boundary dynamics in anti-de Sitter spacetime, Phys. Rev. D 59, 046003 (1999). https://arxiv.org/abs/hep-th/9805171
  • E. Witten, Anti de Sitter space and holography, Adv. Theor. Math. Phys. 2, 253 (1998). https://arxiv.org/abs/hep-th/9802150
  • J. Maldacena, The large N limit of superconformal field theories and supergravity, Adv. Theor. Math. Phys. 2, 231 (1998). https://arxiv.org/abs/hep-th/9711200
  • S. S. Gubser, I. Klebanov, A. Polyakov, Gauge theory correlators from non-critical string theory, Phys. Lett. B 428, 105 (1998). https://arxiv.org/abs/hep-th/9802109
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Mathematical Physics·Captain: Lucas

Hu–Wang 2023: Hubble Tension — Distance Relations Behind the H₀ ProbesResearch Paper

Motivation

The Hubble constant H0H_0H0​, the present expansion rate of the Universe, is inferred in two largely independent ways: from the cosmic microwave background (CMB) assuming the flat ΛCDM model, giving H0=67.40±0.50H_0 = 67.40 \pm 0.50H0​=67.40±0.50 km/s/Mpc (Planck 2018), and from the local distance ladder of Cepheids and Type Ia supernovae, giving H0=73.04±1.04H_0 = 73.04 \pm 1.04H0​=73.04±1.04 km/s/Mpc (Riess et al. 2022). The 4σ–6σ gap between such estimates is the Hubble tension. The review of Hu and Wang (2023) surveys the independent probes used to arbitrate it (strongly lensed quasars, megamasers, gravitational waves, fast radio bursts, the tip of the red giant branch) and the evidence, from a possible redshift dependence of the inferred H0H_0H0​, that the late-time Universe may need modification.

Several probes in that survey turn an observable into a value of H0H_0H0​ through an explicit formula in a flat ΛCDM background. This mission formalizes those formulas, Eqs. (1)–(8) of the review, and the mathematical properties that the inference relies on: that a measured time-delay distance determines H0H_0H0​ uniquely, that the dispersion measure–redshift relation of fast radio bursts is invertible, and that a "running" H0H_0H0​ diagnostic is a genuine test of flat ΛCDM.

Setting

Fix a matter density parameter Ωm≥0\Omega_m \ge 0Ωm​≥0 and impose spatial flatness, so that the dark-energy density parameter is ΩΛ=1−Ωm\Omega_\Lambda = 1 - \Omega_mΩΛ​=1−Ωm​. The dimensionless expansion rate is

E(z)=Ωm(1+z)3+1−Ωm,E(z) = \sqrt{\Omega_m(1+z)^3 + 1 - \Omega_m},E(z)=Ωm​(1+z)3+1−Ωm​​,

and the Hubble rate at redshift zzz is H(z)=H0E(z)H(z) = H_0 E(z)H(z)=H0​E(z).

Distances. For redshifts z1≤z2z_1 \le z_2z1​≤z2​ and speed of light ccc, the angular diameter distance between them is (Eq. (2))

D12=cH0(1+z2)∫z1z2dz′E(z′),D_{12} = \frac{c}{H_0(1+z_2)} \int_{z_1}^{z_2} \frac{dz'}{E(z')},D12​=H0​(1+z2​)c​∫z1​z2​​E(z′)dz′​,

and the distance from the observer to redshift zzz is the case z1=0z_1 = 0z1​=0 (Eq. (3)). A lens at redshift zlensz_{\rm lens}zlens​ in front of a quasar at zsz_szs​ has distances DdD_dDd​ (to the lens), DsD_sDs​ (to the source) and DdsD_{ds}Dds​ (lens to source), and the time-delay distance (Eq. (1))

DΔt=(1+zlens)DdDsDdsD_{\Delta t} = (1+z_{\rm lens}) \frac{D_d D_s}{D_{ds}}DΔt​=(1+zlens​)Dds​Dd​Ds​​

is the quantity inferred from the time delay between lensed images.

Fast radio bursts. The mean intergalactic dispersion measure at redshift zzz is (Eq. (5))

⟨DMIGM(z)⟩=AΩbH02H0∫0zfIGM(z′) fe(z′) (1+z′)Ωm(1+z′)3+1−Ωm dz′,A=3c8πGmp,\langle {\rm DM_{IGM}}(z)\rangle = \frac{A\Omega_b H_0^2}{H_0}\int_0^{z}\frac{f_{\rm IGM}(z')\,f_e(z')\,(1+z')}{\sqrt{\Omega_m(1+z')^3+1-\Omega_m}}\,dz', \qquad A = \frac{3c}{8\pi G m_p},⟨DMIGM​(z)⟩=H0​AΩb​H02​​∫0z​Ωm​(1+z′)3+1−Ωm​​fIGM​(z′)fe​(z′)(1+z′)​dz′,A=8πGmp​3c​,

where Ωb\Omega_bΩb​ is the baryon density parameter, fIGMf_{\rm IGM}fIGM​ the fraction of baryons in the intergalactic medium, and fe=YHXe,H+12YHeXe,Hef_e = Y_H X_{e,H} + \frac12 Y_{He} X_{e,He}fe​=YH​Xe,H​+21​YHe​Xe,He​ the electron fraction. The observed dispersion measure adds Milky Way and host contributions (Eq. (4)).

Redshift-dependent H0H_0H0​. Data binned in redshift are placed at the weighted redshift zˉ=∑nznσn−2/∑nσn−2\bar z = \sum_n z_n \sigma_n^{-2} / \sum_n \sigma_n^{-2}zˉ=∑n​zn​σn−2​/∑n​σn−2​ (Eq. (6)); the trend of H0H_0H0​ across bins is fitted by the evolution function g(z)=H~0/(1+z)αg(z) = \tilde H_0/(1+z)^\alphag(z)=H~0​/(1+z)α (Eq. (7)); and for an arbitrary expansion history HHH the H0H_0H0​ diagnostic is (Eq. (8))

H0(z)=H(z)1−Ωm0+Ωm0(1+z)3.H_0(z) = \frac{H(z)}{\sqrt{1-\Omega_{m0}+\Omega_{m0}(1+z)^3}}.H0​(z)=1−Ωm0​+Ωm0​(1+z)3​H(z)​.

Formalization targets

Goal: the time-delay distance determines H0H_0H0​

For c>0c > 0c>0, Ωm≥0\Omega_m \ge 0Ωm​≥0 and 0<zlens<zs0 < z_{\rm lens} < z_s0<zlens​<zs​ there is K>0K > 0K>0 such that for every H0>0H_0 > 0H0​>0,

DΔt(H0)=KH0.D_{\Delta t}(H_0) = \frac{K}{H_0}.DΔt​(H0​)=H0​K​.

The constant KKK is left unspecified: the goal asserts only the shape of the dependence, which is what makes the quasar-lensing inference of H0H_0H0​ well posed.

Milestones

  1. Eqs. (2)–(3): in flat ΛCDM, Dds=Ds−1+zlens1+zsDdD_{ds} = D_s - \frac{1+z_{\rm lens}}{1+z_s} D_dDds​=Ds​−1+zs​1+zlens​​Dd​ for 0≤zlens≤zs0 \le z_{\rm lens} \le z_s0≤zlens​≤zs​.
  2. 1/H01/H_01/H0​ scaling: H0DΔt(H0)H_0 D_{\Delta t}(H_0)H0​DΔt​(H0​) is independent of H0≠0H_0 \neq 0H0​=0.
  3. Positivity: DΔt>0D_{\Delta t} > 0DΔt​>0 for c,H0>0c, H_0 > 0c,H0​>0 and 0<zlens<zs0 < z_{\rm lens} < z_s0<zlens​<zs​.
  4. Eq. (5): ⟨DMIGM(z)⟩\langle {\rm DM_{IGM}}(z)\rangle⟨DMIGM​(z)⟩ is strictly increasing on z≥0z \ge 0z≥0 for positive continuous fIGMf_{\rm IGM}fIGM​, fef_efe​.
  5. Electron fraction: fe=7/8f_e = 7/8fe​=7/8 for YH=0.75Y_H = 0.75YH​=0.75, YHe=0.25Y_{He} = 0.25YHe​=0.25, full ionization.
  6. Eq. (6): zˉ\bar zzˉ lies in any interval containing all the znz_nzn​.
  7. Eq. (7): ggg is strictly decreasing for H~0>0\tilde H_0 > 0H~0​>0, α>0\alpha > 0α>0.
  8. Eq. (8): H0(z)≡H0H_0(z) \equiv H_0H0​(z)≡H0​ on z≥0z \ge 0z≥0 if and only if H(z)=H0E(z)H(z) = H_0 E(z)H(z)=H0​E(z) on z≥0z \ge 0z≥0.

Significance

The results. The review's quantitative arguments use these formulas as black boxes. The goal and milestones 1–3 make precise the statement that the time-delay distance is "primarily sensitive to H0H_0H0​": it is exactly inversely proportional to H0H_0H0​, with all other cosmological dependence in a positive constant. Milestone 4 is the invertibility of the dispersion measure–redshift relation on which FRB cosmology rests. Milestones 6–8 underpin the "descending H0H_0H0​" evidence of Section 5: the effective redshift of a bin is a redshift of that bin, a positive exponent in ggg means a decreasing trend, and a non-constant diagnostic H0(z)H_0(z)H0​(z) is equivalent to a departure from flat ΛCDM.

Formalizing them. These facts are standard and their proofs are short on paper. The mission also records a transcription issue in the source: Eq. (3) prints the integrand as Ωm(1+z′)3+ΩΛ\sqrt{\Omega_m(1+z')^3+\Omega_\Lambda}Ωm​(1+z′)3+ΩΛ​​, which is inconsistent with Eq. (2); the formalization uses the reciprocal square root, as in Eq. (2).

Difficulty

The algebraic statements (milestones 2, 5, 7, 8) require care only with Lean's total division and real powers. The analytic statements involve interval integrals: milestone 1 needs integrability of 1/E1/E1/E on [0,zs][0, z_s][0,zs​] and additivity of the integral, and milestones 3 and 4 need strict positivity of the integral of a positive continuous function over a nondegenerate interval. Unfolding the definitions and clearing denominators fails as soon as a denominator such as DdsD_{ds}Dds​ or E(z)E(z)E(z) might vanish; each such case has to be ruled out from the hypotheses.

Formalization scope

All quantities are real-valued. Flatness is built in by writing 1−Ωm1 - \Omega_m1−Ωm​ for ΩΛ\Omega_\LambdaΩΛ​; Ωm≥0\Omega_m \ge 0Ωm​≥0 is assumed where needed, while Ωm≤1\Omega_m \le 1Ωm​≤1 is never needed and is not assumed. The angular diameter distances are interval integrals of 1/E1/E1/E; division by zero evaluates to 000, so positivity of the relevant denominators is either assumed or proved. The power (1+z)α(1+z)^\alpha(1+z)α in Eq. (7) is the real power and the weights σn−2\sigma_n^{-2}σn−2​ in Eq. (6) are integer powers. Physical constants (ccc, GGG, mpm_pmp​) and the functions fIGMf_{\rm IGM}fIGM​, fef_efe​ are free parameters, not numerical values. The statistical analyses of the review (likelihood fits, Gaussian-process reconstructions, quoted σ-levels) are out of scope.

All definitions live in one shared definition file in the HuWang2023 namespace; the distance functions and the H0H_0H0​ diagnostic are reusable for other flat-ΛCDM missions.

Selected references

  • J.-P. Hu and F.-Y. Wang, Hubble Tension: The Evidence of New Physics, Universe 9 (2023) 94. https://doi.org/10.3390/universe9020094
  • Planck Collaboration, Planck 2018 results. VI. Cosmological parameters, A&A 641 (2020) A6. https://arxiv.org/abs/1807.06209
  • A. G. Riess et al., A Comprehensive Measurement of the Local Value of the Hubble Constant with 1 km/s/Mpc Uncertainty from the Hubble Space Telescope and the SH0ES Team, ApJL 934 (2022) L7. https://arxiv.org/abs/2112.04510
  • K. C. Wong et al., H0LiCOW XIII. A 2.4% measurement of H0H_0H0​ from lensed quasars, MNRAS 498 (2020) 1420. https://arxiv.org/abs/1907.04869
  • J.-P. Macquart et al., A census of baryons in the Universe from localized fast radio bursts, Nature 581 (2020) 391. https://arxiv.org/abs/2005.13161
  • C. Krishnan, E. Ó Colgáin, M. M. Sheikh-Jabbari, T. Yang, Running Hubble tension and a H0H_0H0​ diagnostic, Phys. Rev. D 103 (2021) 103509. https://arxiv.org/abs/2011.02858
  • M. G. Dainotti et al., On the Hubble constant tension in the SNe Ia Pantheon sample, ApJ 912 (2021) 150. https://arxiv.org/abs/2103.02117
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Number TheoryTheoretical Computer Science·Captain: Lucas

General Number Field Sieve: Congruence of SquaresTextbook

Motivation

The general number field sieve (GNFS) is the most efficient classical algorithm known for factoring integers larger than about 1010010^{100}10100. Its heuristic running time for an integer nnn is

exp⁡ ⁣(((64/9)1/3+o(1))(log⁡n)1/3(log⁡log⁡n)2/3)=Ln[1/3, (64/9)1/3],\exp\!\Big(\big((64/9)^{1/3}+o(1)\big)(\log n)^{1/3}(\log\log n)^{2/3}\Big) = L_n\big[1/3,\,(64/9)^{1/3}\big],exp(((64/9)1/3+o(1))(logn)1/3(loglogn)2/3)=Ln​[1/3,(64/9)1/3],

super-polynomial but sub-exponential in the bit length of nnn. Every record factorization of a general RSA modulus of recent decades (RSA-768, RSA-240, RSA-250) was obtained with it, so the security margins of RSA key sizes are calibrated against it (Pomerance, A Tale of Two Sieves, 1996; Boudot et al., 2020).

Like the rational and quadratic sieves, GNFS works by producing a congruence of squares x2≡y2(modn)x^2 \equiv y^2 \pmod nx2≡y2(modn) and then taking gcd⁡(x−y,n)\gcd(x-y,n)gcd(x−y,n). Its gain comes from searching for smooth values that are sub-exponential in the size of nnn, which forces the algorithm to compute in algebraic number fields.

Setting

Let f∈Z[x]f \in \mathbb{Z}[x]f∈Z[x] be a polynomial of degree ddd and θ∈C\theta \in \mathbb{C}θ∈C a root of fff. The number field Q(θ)\mathbb{Q}(\theta)Q(θ) is the set of complex numbers ∑i<daiθi\sum_{i<d} a_i\theta^i∑i<d​ai​θi with ai∈Qa_i \in \mathbb{Q}ai​∈Q; it is ddd-dimensional over Q\mathbb{Q}Q when fff is irreducible over Q\mathbb{Q}Q. The ring Z[θ]\mathbb{Z}[\theta]Z[θ] is the subring of C\mathbb{C}C generated by θ\thetaθ; the ring of integers OQ(θ)\mathcal{O}_{\mathbb{Q}(\theta)}OQ(θ)​ consists of the elements of Q(θ)\mathbb{Q}(\theta)Q(θ) that are roots of monic integer polynomials. It contains Z[θ]\mathbb{Z}[\theta]Z[θ] when fff is monic, and the two can differ.

GNFS chooses two irreducible integer polynomials f1,f2f_1, f_2f1​,f2​ with a common root mmm modulo nnn, i.e. n∣f1(m)n \mid f_1(m)n∣f1​(m) and n∣f2(m)n \mid f_2(m)n∣f2​(m). A simple choice is the base-mmm polynomial: write n=admd+⋯+a1m+a0n = a_d m^d + \dots + a_1 m + a_0n=ad​md+⋯+a1​m+a0​ with digits 0≤ai<m0 \le a_i < m0≤ai​<m, put f1(x)=∑aixif_1(x) = \sum a_i x^if1​(x)=∑ai​xi and f2(x)=x−mf_2(x) = x - mf2​(x)=x−m. Pairs of integers (a,b)(a,b)(a,b) (relations) are sieved so that both homogenized values Fj(a,b)=bdeg⁡fjfj(a/b)F_j(a,b) = b^{\deg f_j} f_j(a/b)Fj​(a,b)=bdegfj​fj​(a/b) are smooth; up to the leading coefficient these are the norms N(a−bθj)N(a - b\theta_j)N(a−bθj​). Linear algebra over F2\mathbb{F}_2F2​ then selects a set SSS of relations for which

∏(a,b)∈S(a−bθ1)=γ12,γ1∈Z[θ1],∏(a,b)∈S(a−bθ2)=γ22,γ2∈Z[θ2].\prod_{(a,b)\in S}(a-b\theta_1) = \gamma_1^2,\quad \gamma_1 \in \mathbb{Z}[\theta_1], \qquad \prod_{(a,b)\in S}(a-b\theta_2) = \gamma_2^2,\quad \gamma_2 \in \mathbb{Z}[\theta_2].(a,b)∈S∏​(a−bθ1​)=γ12​,γ1​∈Z[θ1​],(a,b)∈S∏​(a−bθ2​)=γ22​,γ2​∈Z[θ2​].

Because mmm is a root of both polynomials mod nnn, there are ring homomorphisms φj:Z[θj]→Z/nZ\varphi_j : \mathbb{Z}[\theta_j] \to \mathbb{Z}/n\mathbb{Z}φj​:Z[θj​]→Z/nZ with φj(θj)=m\varphi_j(\theta_j) = mφj​(θj​)=m. Both send ∏S(a−bθj)\prod_S(a - b\theta_j)∏S​(a−bθj​) to ∏S(a−bm)\prod_S(a - bm)∏S​(a−bm).

Formalization targets

Goal: the congruence of squares

For f1,f2f_1, f_2f1​,f2​ irreducible in Z[x]\mathbb{Z}[x]Z[x] with complex roots θ1,θ2\theta_1,\theta_2θ1​,θ2​, a common root mmm mod nnn, and SSS, γ1\gamma_1γ1​, γ2\gamma_2γ2​ as above:

∃ φj:Z[θj]→Z/nZ, φj(θj)=m,and every such pair satisfiesφ1(γ1)2=φ2(γ2)2.\exists\,\varphi_j:\mathbb{Z}[\theta_j]\to\mathbb{Z}/n\mathbb{Z},\ \varphi_j(\theta_j)=m, \qquad\text{and every such pair satisfies}\qquad \varphi_1(\gamma_1)^2 = \varphi_2(\gamma_2)^2 .∃φj​:Z[θj​]→Z/nZ, φj​(θj​)=m,and every such pair satisfiesφ1​(γ1​)2=φ2​(γ2​)2.

This is the correctness statement of the algebraic part of GNFS: whatever relations the sieve and linear algebra produce, the square-root step yields x=φ1(γ1)x = \varphi_1(\gamma_1)x=φ1​(γ1​), y=φ2(γ2)y = \varphi_2(\gamma_2)y=φ2​(γ2​) with n∣x2−y2n \mid x^2 - y^2n∣x2−y2.

Supporting statements (milestones)

  1. [Q(θ):Q]=d[\mathbb{Q}(\theta):\mathbb{Q}] = d[Q(θ):Q]=d for fff irreducible over Q\mathbb{Q}Q.
  2. Z[θ]\mathbb{Z}[\theta]Z[θ] can be strictly smaller than the ring of integers.
  3. The base-mmm polynomial has digits 0≤ai<m0\le a_i<m0≤ai​<m as coefficients and f(m)=nf(m)=nf(m)=n, so mmm is a root mod nnn.
  4. Existence of the homomorphism Z[θ]→Z/nZ\mathbb{Z}[\theta]\to\mathbb{Z}/n\mathbb{Z}Z[θ]→Z/nZ, θ↦m\theta\mapsto mθ↦m.
  5. cd NQ(θ)/Q(a−bθ)=bdf(a/b)c_d\,N_{\mathbb{Q}(\theta)/\mathbb{Q}}(a-b\theta) = b^d f(a/b)cd​NQ(θ)/Q​(a−bθ)=bdf(a/b), where cdc_dcd​ is the leading coefficient.
  6. If n∣x2−y2n\mid x^2-y^2n∣x2−y2, n∤x−yn\nmid x-yn∤x−y, n∤x+yn\nmid x+yn∤x+y, then 1<gcd⁡(x−y,n)<n1<\gcd(x-y,n)<n1<gcd(x−y,n)<n.
  7. For odd nnn with at least two prime factors and a unit xxx, at least half of the square roots of x2x^2x2 mod nnn differ from ±x\pm x±x (the "probability at least 1/21/21/2" of the final step).

Significance

The goal and milestones together certify that every output of the GNFS pipeline that passes the square-root step is a genuine congruence of squares, and that such a congruence splits nnn with probability at least 1/21/21/2 over the choice of square root. This is the part of the algorithm whose correctness is unconditional; the running-time bound is heuristic and is not a target here.

These results are classical and appear in standard references (Lenstra–Lenstra 1993; Crandall–Pomerance 2005, §6.2). The mission's contribution is a machine-checked formal version connecting number fields in C\mathbb{C}C, integer polynomials, and residue rings, which current libraries do not package for this purpose.

Difficulty

The ring homomorphism Z[θ]→Z/nZ\mathbb{Z}[\theta] \to \mathbb{Z}/n\mathbb{Z}Z[θ]→Z/nZ is the delicate point. Z[θ]\mathbb{Z}[\theta]Z[θ] is a subring of C\mathbb{C}C, not a quotient ring, so a map defined by θ↦m\theta \mapsto mθ↦m is well defined only if every integer polynomial vanishing at θ\thetaθ is a multiple of fff in Z[x]\mathbb{Z}[x]Z[x]. This needs fff irreducible over Z\mathbb{Z}Z (in particular primitive), via Gauss's lemma; for f(x)=2xf(x) = 2xf(x)=2x and n=2n = 2n=2, every mmm is a root mod nnn, but θ=0\theta = 0θ=0 only admits θ↦0\theta \mapsto 0θ↦0. The norm identity requires identifying f/cdf/c_df/cd​ as the minimal polynomial of θ\thetaθ and expressing the norm as a product over conjugates. The probability milestone needs the Chinese remainder theorem and counting square roots of units modulo odd prime powers.

Formalization scope

All statements live in the namespace GNFS. Number fields are realized inside C\mathbb{C}C: Q(θ)\mathbb{Q}(\theta)Q(θ) is ℚ⟮θ⟯ and Z[θ]\mathbb{Z}[\theta]Z[θ] is Algebra.adjoin ℤ {θ}. Residues mod nnn are ZMod n with n∈Nn \in \mathbb{N}n∈N (n=0n = 0n=0 gives Z\mathbb{Z}Z, consistent with every statement). Two definitions are shared: GNFS.baseMPolynomial n m, the polynomial whose coefficients are the base-mmm digits of nnn (via Nat.digits), and GNFS.homogenize f a b =∑i≤dciaibd−i= \sum_{i\le d} c_i a^i b^{d-i}=∑i≤d​ci​aibd−i.

Irreducibility "over the rationals" with integer coefficients is encoded as irreducibility in Z[x]\mathbb{Z}[x]Z[x] (primitive and irreducible over Q\mathbb{Q}Q) where a homomorphism to Z/nZ\mathbb{Z}/n\mathbb{Z}Z/nZ is needed. Without primitivity the claimed homomorphism can fail to exist. The goal asserts both the existence of the homomorphisms and the equality for every such pair, so it cannot be satisfied by the trivial choice x=yx = yx=y. The sieving, smoothness, linear-algebra and complexity aspects of the article are out of scope.

Reusable by-products: norms of linear elements in simple extensions, homomorphisms out of Z[θ]\mathbb{Z}[\theta]Z[θ], and square-root counting in Z/nZ\mathbb{Z}/n\mathbb{Z}Z/nZ.

Selected references

  • Wikipedia, General number field sieve, revision 1377718368. https://en.wikipedia.org/w/index.php?title=General_number_field_sieve&oldid=1377718368
  • C. Pomerance, A Tale of Two Sieves, Notices of the AMS 43(12), 1996. https://www.ams.org/notices/199612/pomerance.pdf
  • A. K. Lenstra, H. W. Lenstra Jr. (eds.), The development of the number field sieve, Lecture Notes in Math. 1554, Springer, 1993. https://doi.org/10.1007/BFb0091534
  • R. Crandall, C. Pomerance, Prime Numbers: A Computational Perspective, 2nd ed., Springer, 2005, §6.2. https://doi.org/10.1007/0-387-28979-8
  • F. Boudot et al., Comparing the difficulty of factorization and discrete logarithm: a 240-digit experiment, CRYPTO 2020. https://eprint.iacr.org/2020/697
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Functional AnalysisHarmonic Analysis·Captain: Lucas

Schwartz Space (Wikipedia): the Fourier Transform is an Automorphism of 𝒮(ℝⁿ)Textbook

Motivation

The Schwartz space S(Rn)\mathcal{S}(\mathbb{R}^n)S(Rn) of smooth, rapidly decreasing functions is the standard domain on which Fourier analysis on Rn\mathbb{R}^nRn works without integrability caveats. Its defining property, singled out in the lead of the source article, is that the Fourier transform maps S(Rn)\mathcal{S}(\mathbb{R}^n)S(Rn) isomorphically onto itself. By duality this allows the Fourier transform to be defined on the dual space S′(Rn)\mathcal{S}'(\mathbb{R}^n)S′(Rn) of tempered distributions, which is the setting of the modern theory of linear partial differential equations (Hörmander, Vol. I) and of much of mathematical physics (Reed–Simon, Vol. I). The space is named after Laurent Schwartz.

This mission formalizes the definition and the elementary analytic properties of S(Rn)\mathcal{S}(\mathbb{R}^n)S(Rn) exactly as stated in the Wikipedia article Schwartz space (revision 1360762580), with the Fourier-automorphism property as the goal.

Setting

Write Rn\mathbb{R}^nRn for the coordinate space with the Euclidean norm ∣x∣=(x12+⋯+xn2)1/2|x| = (x_1^2 + \dots + x_n^2)^{1/2}∣x∣=(x12​+⋯+xn2​)1/2 and Lebesgue measure. A multi-index is a tuple α=(α1,…,αn)∈Nn\alpha = (\alpha_1, \dots, \alpha_n) \in \mathbb{N}^nα=(α1​,…,αn​)∈Nn, and xα=x1α1⋯xnαnx^\alpha = x_1^{\alpha_1} \cdots x_n^{\alpha_n}xα=x1α1​​⋯xnαn​​. For a function f:Rn→Cf : \mathbb{R}^n \to \mathbb{C}f:Rn→C, ∂if\partial_i f∂i​f denotes the partial derivative in the iii-th coordinate direction and

Dβf=∂1β1⋯∂nβnf.D^\beta f = \partial_1^{\beta_1} \cdots \partial_n^{\beta_n} f .Dβf=∂1β1​​⋯∂nβn​​f.

For α,β∈Nn\alpha, \beta \in \mathbb{N}^nα,β∈Nn put

∥f∥α,β=sup⁡x∈Rn∣xα(Dβf)(x)∣∈[0,∞].\|f\|_{\alpha,\beta} = \sup_{x \in \mathbb{R}^n} \bigl| x^\alpha (D^\beta f)(x) \bigr| \in [0, \infty].∥f∥α,β​=x∈Rnsup​​xα(Dβf)(x)​∈[0,∞].

The Schwartz space is

S(Rn,C)={f∈C∞(Rn,C):∥f∥α,β<∞ for all α,β∈Nn}.\mathcal{S}(\mathbb{R}^n, \mathbb{C}) = \bigl\{ f \in C^\infty(\mathbb{R}^n, \mathbb{C}) : \|f\|_{\alpha,\beta} < \infty \text{ for all } \alpha, \beta \in \mathbb{N}^n \bigr\}.S(Rn,C)={f∈C∞(Rn,C):∥f∥α,β​<∞ for all α,β∈Nn}.

Informally, fff and all its derivatives decay at infinity faster than any reciprocal power of ∣x∣|x|∣x∣.

The Fourier transform of f:Rn→Cf : \mathbb{R}^n \to \mathbb{C}f:Rn→C is

(Ff)(ξ)=∫Rne−2πi⟨x,ξ⟩f(x) dx.(\mathcal{F} f)(\xi) = \int_{\mathbb{R}^n} e^{-2\pi i \langle x, \xi \rangle} f(x) \, dx .(Ff)(ξ)=∫Rn​e−2πi⟨x,ξ⟩f(x)dx.

In the Lean development these objects are SchwartzSpaceWiki.monomial, partialDeriv, iteratedPartialDeriv, schwartzSeminorm, schwartzSpace n and fourierTransform.

Formalization targets

Goal: the Fourier transform is an automorphism of S(Rn)\mathcal{S}(\mathbb{R}^n)S(Rn)

F:S(Rn)→S(Rn) is a linear bijection.\mathcal{F} : \mathcal{S}(\mathbb{R}^n) \to \mathcal{S}(\mathbb{R}^n) \text{ is a linear bijection.}F:S(Rn)→S(Rn) is a linear bijection.

Formally: Set.BijOn fourierTransform (schwartzSpace n) (schwartzSpace n) together with F(f+cg)=Ff+c Fg\mathcal{F}(f + c g) = \mathcal{F} f + c\,\mathcal{F} gF(f+cg)=Ff+cFg for f,g∈S(Rn)f, g \in \mathcal{S}(\mathbb{R}^n)f,g∈S(Rn) and c∈Cc \in \mathbb{C}c∈C.

Milestones (in the order of the source)

  1. S(Rn)\mathcal{S}(\mathbb{R}^n)S(Rn) is a complex linear subspace of C∞(Rn,C)C^\infty(\mathbb{R}^n, \mathbb{C})C∞(Rn,C).
  2. xαe−a∣x∣2∈S(Rn)x^\alpha e^{-a|x|^2} \in \mathcal{S}(\mathbb{R}^n)xαe−a∣x∣2∈S(Rn) for every multi-index α\alphaα and every a>0a > 0a>0.
  3. Cc∞(Rn)⊆S(Rn)C_c^\infty(\mathbb{R}^n) \subseteq \mathcal{S}(\mathbb{R}^n)Cc∞​(Rn)⊆S(Rn): smooth compactly supported functions are Schwartz functions.
  4. P(x)e−a∣x∣2∈S(Rn)P(x) e^{-a|x|^2} \in \mathcal{S}(\mathbb{R}^n)P(x)e−a∣x∣2∈S(Rn) for every polynomial PPP and a>0a > 0a>0, and P↦Pe−a∣x∣2P \mapsto P e^{-a|x|^2}P↦Pe−a∣x∣2 is injective.
  5. f,g∈S(Rn)⇒fg∈S(Rn)f, g \in \mathcal{S}(\mathbb{R}^n) \Rightarrow fg \in \mathcal{S}(\mathbb{R}^n)f,g∈S(Rn)⇒fg∈S(Rn).
  6. If f∈S(Rn)f \in \mathcal{S}(\mathbb{R}^n)f∈S(Rn) and ggg is smooth and bounded with all its derivatives, then fg∈S(Rn)fg \in \mathcal{S}(\mathbb{R}^n)fg∈S(Rn).
  7. Every f∈S(Rn)f \in \mathcal{S}(\mathbb{R}^n)f∈S(Rn) is Lipschitz, hence uniformly continuous.
  8. For 1≤p<∞1 \le p < \infty1≤p<∞, S(Rn)⊆Lp(Rn)\mathcal{S}(\mathbb{R}^n) \subseteq L^p(\mathbb{R}^n)S(Rn)⊆Lp(Rn) and it is dense there.

Significance

The result itself. The automorphism property is what makes S(Rn)\mathcal{S}(\mathbb{R}^n)S(Rn) the natural test-function space for tempered distributions: the Fourier transform of a tempered distribution TTT is defined by ⟨FT,φ⟩=⟨T,Fφ⟩\langle \mathcal{F} T, \varphi \rangle = \langle T, \mathcal{F} \varphi \rangle⟨FT,φ⟩=⟨T,Fφ⟩, which only makes sense because Fφ\mathcal{F}\varphiFφ is again a Schwartz function. Density in LpL^pLp (milestone 8) is what lets identities proved on Schwartz functions, such as Plancherel's theorem, extend to L2L^2L2 and other LpL^pLp spaces. The closure properties (milestones 1, 5, 6) say that S(Rn)\mathcal{S}(\mathbb{R}^n)S(Rn) is an algebra and a module over smooth functions with bounded derivatives.

Formalizing it. All results here are classical. Mathlib contains a Schwartz-space type SchwartzMap built on iterated Fréchet derivatives and the norm ∥x∥k\|x\|^k∥x∥k, together with a Fourier transform on it. This mission instead states everything for the concrete, coordinate-wise multi-index definition used in the source. A complete development therefore includes a proof that the two definitions agree, which is reusable on its own.

Difficulty

The multi-index seminorms sup⁡∣xαDβf∣\sup |x^\alpha D^\beta f|sup∣xαDβf∣ are coordinate-wise, while the standard library works with the total derivative and the full norm ∣x∣k|x|^k∣x∣k. The comparison needs inequalities in both directions between ∣xα∣|x^\alpha|∣xα∣ and powers of ∣x∣|x|∣x∣, and between the iterated partial derivatives DβfD^\beta fDβf and the norm of the kkk-th Fréchet derivative. For the goal, surjectivity is the hard part: it needs the Fourier inversion formula on S(Rn)\mathcal{S}(\mathbb{R}^n)S(Rn), not only the fact that F\mathcal{F}F preserves decay and smoothness. For milestone 8, density requires approximating arbitrary LpL^pLp functions, e.g. by compactly supported smooth functions, and this does not follow from the definition of S\mathcal{S}S alone.

Formalization scope

  • Rn\mathbb{R}^nRn is EuclideanSpace ℝ (Fin n) (Euclidean norm, Lebesgue volume). Functions take values in C\mathbb{C}C. n=0n = 0n=0 is allowed.
  • Smoothness is ContDiff ℝ (⊤ : ℕ∞), i.e. C∞C^\inftyC∞ (not analyticity).
  • ∂if(x)\partial_i f(x)∂i​f(x) is fderiv ℝ f x (EuclideanSpace.single i 1), and DβD^\betaDβ applies ∂1β1,…,∂nβn\partial_1^{\beta_1}, \dots, \partial_n^{\beta_n}∂1β1​​,…,∂nβn​​ in a fixed order. For smooth fff the order does not matter.
  • The seminorm ∥f∥α,β\|f\|_{\alpha,\beta}∥f∥α,β​ is a supremum in [0,∞][0, \infty][0,∞] (ℝ≥0∞), so "<∞< \infty<∞" really means bounded. A real-valued supremum would return 000 on unbounded sets and trivialize the definition.
  • The source does not fix a Fourier normalisation. The convention e−2πi⟨x,ξ⟩e^{-2\pi i\langle x,\xi\rangle}e−2πi⟨x,ξ⟩ is used. fourierTransform is a Bochner integral, which is 000 for non-integrable integrands. Every target only applies it to Schwartz functions, which are integrable.
  • The goal is stated as a bijection of the set schwartzSpace n onto itself plus linearity on it. It does not presuppose that schwartzSpace n has been given a module structure.
  • Not included: the topological statements of the source (that S(Rn)\mathcal{S}(\mathbb{R}^n)S(Rn) is a nuclear Montel Fréchet space, ultrabornological, reflexive, etc., and the corresponding facts for its strong dual). They require equipping the set with its seminorm topology, which this mission does not define. They are natural follow-up missions.

Contributions welcome: the equivalence with Mathlib's SchwartzMap, coordinate–norm comparison lemmas for xαx^\alphaxα, and the Leibniz rule for iteratedPartialDeriv.

Selected references

  • Wikipedia contributors, Schwartz space, revision 1360762580. https://en.wikipedia.org/w/index.php?title=Schwartz_space&oldid=1360762580
  • L. Hörmander, The Analysis of Linear Partial Differential Operators I, 2nd ed., Springer, 1990. ISBN 3-540-52343-X.
  • M. Reed, B. Simon, Methods of Modern Mathematical Physics I: Functional Analysis, revised ed., Academic Press, 1980. ISBN 0-12-585050-6.
  • E. M. Stein, R. Shakarchi, Fourier Analysis: An Introduction, Princeton University Press, 2003. ISBN 0-691-11384-X.
  • F. Trèves, Topological Vector Spaces, Distributions and Kernels, Dover, 2006 [1967]. ISBN 978-0-486-45352-1.
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Quantum Information·Captain: Goku

Lecture Notes on Quantum Algorithms 23: Trace inequality |tr(XYZ)| ≤ ‖X‖_F ‖Y‖ ‖Z‖_FTextbook

Motivation

This mission develops Chapter 23 of Lecture Notes on Quantum Algorithms by Andrew Childs. The chapter's selected results describe the mathematical guarantees below.

Setting and conventions

The linked theorem statements and shared definitions specify the register types, oracle access, normalization, and resource conventions. Their source locators and independent readbacks accompany each target.

Chapter goal

Let m,n≥0m,n\ge 0m,n≥0 be integers and let X∈Cm×nX\in\mathbb C^{m\times n}X∈Cm×n, Y∈Cn×nY\in\mathbb C^{n\times n}Y∈Cn×n and Z∈Cn×mZ\in\mathbb C^{n\times m}Z∈Cn×m be complex matrices. Write ∥A∥F\|A\|_F∥A∥F​ for the Frobenius norm, ∥A∥F2=∑a,b∣Aab∣2\|A\|_F^2=\sum_{a,b}|A_{ab}|^2∥A∥F2​=∑a,b​∣Aab​∣2, and ∥Y∥\|Y\|∥Y∥ for the spectral (operator) norm of YYY, i.e. its largest singular value. Then

∣tr⁡(XYZ)∣≤∥X∥F ∥Y∥ ∥Z∥F.|\operatorname{tr}(XYZ)| \le \|X\|_F\,\|Y\|\,\|Z\|_F .∣tr(XYZ)∣≤∥X∥F​∥Y∥∥Z∥F​.

In the generalized adversary method this inequality bounds both the final value of the weight function for Boolean functions and how much one query can change it.

Formalization Note The index sets are {0,…,m−1}\{0,\dots,m-1\}{0,…,m−1} and {0,…,n−1}\{0,\dots,n-1\}{0,…,n−1}; the Frobenius norm is frobNorm and the spectral norm is specNorm (Mathlib's ℓ2\ell^2ℓ2 operator norm on matrices). When m=0m=0m=0 or n=0n=0n=0 both sides are 000.

Significance

These are known mathematical results. Their Lean statements have been checked and reviewed against the cited source; formal proofs remain open for contributors.

Supporting targets

  • Proposition 23.2: Trace inequality |tr(XYZ)| ≤ ‖X‖_F ‖Y‖ ‖Z‖_F.

Formalization scope

Prove the existing statements under their stated hypotheses and definitions. Any correction to a printed source claim remains explicit in its target description. All listed target proofs are currently sorry; no proof is claimed. The mission goal is the designated chapter capstone; the remaining targets are separate milestones. Parts a, b, c and d are merged into their original chapter.

Selected references

  • Andrew Childs, Lecture Notes on Quantum Algorithms, 17 April 2025. https://www.cs.umd.edu/~amchilds/qa/qa.pdf.
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Machine LearningQuantum Information·Captain: Goku

A Survey of Quantum Learning Theory 5: Atıcı–Servedio: time-efficient quantum learning of k-juntas (corrected)Textbook

Motivation

This mission develops Chapter 5 of A Survey of Quantum Learning Theory by Srinivasan Arunachalam and Ronald de Wolf. The chapter's selected results describe the mathematical guarantees below.

Setting and conventions

The linked theorem statements and shared definitions specify the register types, oracle access, normalization, and resource conventions. Their source locators and independent readbacks accompany each target.

Chapter goal

This is a corrected form of the Atıcı–Servedio theorem on learning juntas from uniform quantum examples.

A function f:{0,1}n→{0,1}f:\{0,1\}^n\to\{0,1\}f:{0,1}n→{0,1} is a kkk-junta if it depends on at most kkk of its nnn input bits. A uniform quantum example of fff is the (n+1)(n+1)(n+1)-qubit state ∑x∈{0,1}n2−n/2∣x,f(x)⟩\sum_{x\in\{0,1\}^n}2^{-n/2}|x,f(x)\rangle∑x∈{0,1}n​2−n/2∣x,f(x)⟩; a uniform classical example is a pair (x,f(x))(x,f(x))(x,f(x)) with xxx uniform on {0,1}n\{0,1\}^n{0,1}n. The error of a hypothesis hhh is Pr⁡x[h(x)≠f(x)]\Pr_{x}[h(x)\neq f(x)]Prx​[h(x)=f(x)] for uniform xxx.

Time is measured in the following hybrid cost model, which is the one the source's proof sketch counts in. A learner (1) applies a circuit over the gate set {H,T,CNOT}\{H,T,\mathrm{CNOT}\}{H,T,CNOT} to TQT_QTQ​ uniform quantum examples and some ancillas in ∣0⟩|0\rangle∣0⟩ and measures every qubit in the computational basis; (2) maps the outcome by a Boolean circuit of AND/OR/NOT gates to a set V⊆[n]V\subseteq[n]V⊆[n] of variables; (3) reads TCT_CTC​ uniform classical examples and outputs the truth-table hypothesis h(x)=f(xj)h(x)=f(x_j)h(x)=f(xj​) for the first example xjx_jxj​ that agrees with xxx on VVV (h(x)=0h(x)=0h(x)=0 if there is none). Its time is the number of quantum gates, plus the number of measured qubits, plus the number of Boolean gates, plus TCT_CTC​ (one unit per classical example, which is read and written into the table cell indexed by its VVV-bits), plus 2∣V∣2^{|V|}2∣V∣ table cells (worst case over the outcomes).

For every δ∈(0,1)\delta\in(0,1)δ∈(0,1) there is a constant C>0C>0C>0 such that for all n,kn,kn,k with 2≤k≤n2\le k\le n2≤k≤n and all ε∈(0,1/2]\varepsilon\in(0,1/2]ε∈(0,1/2] there is such a learner with

TQ≤C klog⁡kε,TC≤C 2klog⁡1ε,time≤C(nklog⁡kε+2klog⁡1ε),T_Q\le C\,\frac{k\log k}{\varepsilon},\qquad T_C\le C\,2^k\log\frac1\varepsilon,\qquad \mathrm{time}\le C\Big(\frac{nk\log k}{\varepsilon}+2^k\log\frac1\varepsilon\Big),TQ​≤Cεklogk​,TC​≤C2klogε1​,time≤C(εnklogk​+2klogε1​),

which, for every kkk-junta fff, outputs with probability at least 1−δ1-\delta1−δ (over the measurement outcomes and the classical examples) a hypothesis of error at most ε\varepsilonε.

The theorem shows that quantum examples remove the nΘ(k)n^{\Theta(k)}nΘ(k) search over candidate variable sets that the best known classical learners need, which is why juntas are a notorious bottleneck classically.

Formalization Note The source states no cost model, no confidence parameter, and O(2k)O(2^k)O(2k) classical examples. The cost model above, the fixed-confidence reading (constants depend on δ\deltaδ only), and the O(2klog⁡(1/ε))O(2^k\log(1/\varepsilon))O(2klog(1/ε)) classical examples of the source's own proof sketch are the corrections. The thresholds k≥2k\ge2k≥2 and ε≤1/2\varepsilon\le1/2ε≤1/2 make log⁡k\log klogk and log⁡(1/ε)\log(1/\varepsilon)log(1/ε) positive.

Significance

These are known mathematical results. Their Lean statements have been checked and reviewed against the cited source; formal proofs remain open for contributors.

Supporting targets

  • Theorem 5.4: Atıcı–Servedio: time-efficient quantum learning of k-juntas (corrected).

Formalization scope

Prove the existing statements under their stated hypotheses and definitions. Any correction to a printed source claim remains explicit in its target description. All listed target proofs are currently sorry; no proof is claimed. The mission goal is the designated chapter capstone; the remaining targets are separate milestones. Parts a, b, c and d are merged into their original chapter.

Selected references

  • Srinivasan Arunachalam and Ronald de Wolf, A Survey of Quantum Learning Theory, 2017, v3. https://arxiv.org/pdf/1701.06806v3.
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Quantum Error CorrectionQuantum Information·Captain: Goku

An Introduction to Quantum Error Correction and Fault-Tolerant Quantum Computation 3: Every error syndrome of a stabilizer is realized by a Pauli errorTextbook

Motivation

This mission develops Chapter 3 of An Introduction to Quantum Error Correction and Fault-Tolerant Quantum Computation by Daniel Gottesman. The chapter's selected results describe the mathematical guarantees below.

Setting and conventions

The linked theorem statements and shared definitions specify the register types, oracle access, normalization, and resource conventions. Their source locators and independent readbacks accompany each target.

Chapter goal

Let Pn\mathcal P_nPn​ be the nnn-qubit Pauli group and let g1,…,ga∈Png_1,\dots,g_a\in\mathcal P_ng1​,…,ga​∈Pn​ generate a stabilizer S=⟨g1,…,ga⟩S=\langle g_1,\dots,g_a\rangleS=⟨g1​,…,ga​⟩, that is, an Abelian subgroup of Pn\mathcal P_nPn​ with −I∉S-I\notin S−I∈/S, and suppose the generators are independent, i.e. ∣S∣=2a|S|=2^a∣S∣=2a. The error syndrome of a Pauli operator EEE is the vector in F2a\mathbb F_2^aF2a​ whose iii-th bit is 000 if gig_igi​ commutes with EEE and 111 if it anticommutes.

Then for every v∈F2av\in\mathbb F_2^av∈F2a​ there is E∈PnE\in\mathcal P_nE∈Pn​ with syndrome vvv:

giE=Egi  if vi=0,giE=−Egi  if vi=1(i=1,…,a).g_iE=Eg_i\ \text{ if } v_i=0,\qquad g_iE=-Eg_i\ \text{ if } v_i=1\qquad(i=1,\dots,a).gi​E=Egi​  if vi​=0,gi​E=−Egi​  if vi​=1(i=1,…,a).

This lemma is the step in the proof of the dimension count of stabilizer codes (Theorem 5) that shows all 2a2^a2a syndrome subspaces are nonempty.

Formalization Note The syndrome is relative to the generator list, as in the source's proof; the independence of the generators (used in the proof as linear independence of their binary vectors) is the hypothesis ∣S∣=2a|S|=2^a∣S∣=2a. The anticommutation clause is stated explicitly.

Significance

These are known mathematical results. Their Lean statements have been checked and reviewed against the cited source; formal proofs remain open for contributors.

Supporting targets

  • Theorem 5: Stabilizer codes: an Abelian S of order 2^a without -1 gives an [[n, n-a, d]] code.
  • Lemma 1: Every error syndrome of a stabilizer is realized by a Pauli error.

Formalization scope

Prove the existing statements under their stated hypotheses and definitions. Any correction to a printed source claim remains explicit in its target description. All listed target proofs are currently sorry; no proof is claimed. The mission goal is the designated chapter capstone; the remaining targets are separate milestones. Parts a, b, c and d are merged into their original chapter.

Selected references

  • Daniel Gottesman, An Introduction to Quantum Error Correction and Fault-Tolerant Quantum Computation, 2009, v1. https://arxiv.org/pdf/0904.2557v1.
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OptimizationQuantum Information·Captain: Goku

Quantum algorithms for optimizers 3: Correctness of the digits computed by iterative phase estimation (corrected)Textbook

Motivation

This mission develops Chapter 3 of Quantum algorithms for optimizers by Giacomo Nannicini. The chapter's selected results describe the mathematical guarantees below.

Setting and conventions

The linked theorem statements and shared definitions specify the register types, oracle access, normalization, and resource conventions. Their source locators and independent readbacks accompany each target.

Chapter goal

Let φ∈[0,1)\varphi\in[0,1)φ∈[0,1) be a phase (in full turns), h∈Nh\in\mathbb Nh∈N (h=q−2h=q-2h=q−2), and let ω1,…,ωh\omega_1,\dots,\omega_hω1​,…,ωh​ be the angle estimates used by the iterative phase estimation algorithm of §3.3.2, ωi\omega_iωi​ being the estimate of 2i−1φ2^{i-1}\varphi2i−1φ. The algorithm computes binary digits p1,…,ph+2p_1,\dots,p_{h+2}p1​,…,ph+2​ as follows: phph+1ph+2p_hp_{h+1}p_{h+2}ph​ph+1​ph+2​ are the digits of ωh\omega_hωh​ rounded to the closest multiple of 1/81/81/8 (modulo 111); then for j=h−1,…,1j=h-1,\dots,1j=h−1,…,1, pj=0p_j=0pj​=0 if d(0.0pj+1pj+2,ωj)<1/4d(0.0p_{j+1}p_{j+2},\omega_j)<1/4d(0.0pj+1​pj+2​,ωj​)<1/4 and pj=1p_j=1pj​=1 otherwise. Here d(x,y)d(x,y)d(x,y) is the distance between xxx and yyy modulo 111.

Fix 1≤j≤h1\le j\le h1≤j≤h. If d(ωi,2i−1φ)≤1/16d(\omega_i,2^{i-1}\varphi)\le 1/16d(ωi​,2i−1φ)≤1/16 for every step i=h,h−1,…,ji=h,h-1,\dots,ji=h,h−1,…,j, then

d(0.pjpj+1…ph+2, 2j−1φ) ≤ 2−(h+3−j).d\big(0.p_jp_{j+1}\dots p_{h+2},\ 2^{j-1}\varphi\big)\ \le\ 2^{-(h+3-j)} .d(0.pj​pj+1​…ph+2​, 2j−1φ) ≤ 2−(h+3−j).

In particular, for j=1j=1j=1 the algorithm outputs q=h+2q=h+2q=h+2 binary digits of φ\varphiφ with error at most 2−q2^{-q}2−q on the circle, which together with a union bound over the hhh estimation steps gives the success guarantee of iterative phase estimation.

Formalization Note The page states the bound with plain absolute values and strict inequality. Both are corrected: angles are only known modulo 111 (so all distances are on the circle), and the strict bound already fails at the base case (ωh=1/16\omega_h=1/16ωh​=1/16 is equidistant from 000 and 1/81/81/8, and rounding gives error exactly 1/81/81/8); the induction proves ≤\le≤, matching the goal Pr⁡(min⁡{… }≤2−q)\Pr(\min\{\dots\}\le 2^{-q})Pr(min{…}≤2−q) on p.66. The digits are the shared definition ipeDigits h ω and 0.pj…ph+20.p_j\dots p_{h+2}0.pj​…ph+2​ is binFracFrom.

Significance

These are known mathematical results. Their Lean statements have been checked and reviewed against the cited source; formal proofs remain open for contributors.

Supporting targets

  • Proposition 3.14: Phase estimation on an inexact eigenstate succeeds with probability at least (1 − δ)|⟨ξ|ψ⟩|²*.
  • Proposition 3.16: Combining cosine and sine estimates into an angle estimate (corrected).
  • Proposition 3.17: Correctness of the digits computed by iterative phase estimation (corrected).

Formalization scope

Prove the existing statements under their stated hypotheses and definitions. Any correction to a printed source claim remains explicit in its target description. All listed target proofs are currently sorry; no proof is claimed. The mission goal is the designated chapter capstone; the remaining targets are separate milestones. Parts a, b, c and d are merged into their original chapter.

Selected references

  • Giacomo Nannicini, Quantum algorithms for optimizers, 2025, v5; notes dated 9 July 2025. https://arxiv.org/pdf/2408.07086v5.
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Quantum Information·Captain: Goku

Lecture Notes on Quantum Algorithms 18: Spectral gap and marked fraction bound the norm of the unmarked blockTextbook

Motivation

This mission develops Chapter 18 of Lecture Notes on Quantum Algorithms by Andrew Childs. The chapter's selected results describe the mathematical guarantees below.

Setting and conventions

The linked theorem statements and shared definitions specify the register types, oracle access, normalization, and resource conventions. Their source locators and independent readbacks accompany each target.

Chapter goal

Let N≥2N \ge 2N≥2 and let PPP be a symmetric N×NN \times NN×N stochastic matrix (Pkj≥0P_{kj} \ge 0Pkj​≥0, ∑kPkj=1\sum_k P_{kj} = 1∑k​Pkj​=1 for all jjj, P=PTP = P^{\mathsf T}P=PT) describing a random walk on the vertex set V={1,…,N}V = \{1,\dots,N\}V={1,…,N}. Let M⊆VM \subseteq VM⊆V be a set of marked vertices and let PMP_MPM​ be the matrix obtained from PPP by deleting the rows and columns indexed by MMM. Let δ>0\delta > 0δ>0 and ϵ>0\epsilon > 0ϵ>0.

Lemma. If the second largest eigenvalue of PPP in absolute value is at most 1−δ1-\delta1−δ (that is, listing the eigenvalues of PPP with multiplicity, at most one has absolute value greater than 1−δ1-\delta1−δ) and ∣M∣≥ϵN|M| \ge \epsilon N∣M∣≥ϵN, then

∥PM∥≤1−δϵ,\|P_M\| \le 1 - \delta\epsilon,∥PM​∥≤1−δϵ,

where ∥⋅∥\|\cdot\|∥⋅∥ is the spectral (operator) norm.

Together with Pr⁡[no marked vertex after t steps]≤∥PM∥t\Pr[\text{no marked vertex after } t \text{ steps}] \le \|P_M\|^tPr[no marked vertex after t steps]≤∥PM​∥t, this gives the classical hitting time O(1/(δϵ))O(1/(\delta\epsilon))O(1/(δϵ)), and it is the input to the quantum walk search bound O(1/δϵ)O(1/\sqrt{\delta\epsilon})O(1/δϵ​).

Formalization Note N≥2N \ge 2N≥2 because the source speaks of a second eigenvalue, and δ,ϵ>0\delta, \epsilon > 0δ,ϵ>0 because they are a spectral gap and a fraction; without these the statement fails (e.g. N=1N = 1N=1, P=(1)P = (1)P=(1), M=VM = VM=V, δ=3\delta = 3δ=3, ϵ=1\epsilon = 1ϵ=1). Symmetry is stated as Hermitian, which for a real matrix is the same thing; the eigenvalues are the Mathlib eigenvalue list of the Hermitian matrix. If M=VM = VM=V, PMP_MPM​ is the empty matrix, of norm 000.

Significance

These are known mathematical results. Their Lean statements have been checked and reviewed against the cited source; formal proofs remain open for contributors.

Supporting targets

  • Theorem 18.1: Spectrum of the Szegedy quantum walk.
  • Lemma 18.2: Spectral gap and marked fraction bound the norm of the unmarked block.

Formalization scope

Prove the existing statements under their stated hypotheses and definitions. Any correction to a printed source claim remains explicit in its target description. All listed target proofs are currently sorry; no proof is claimed. The mission goal is the designated chapter capstone; the remaining targets are separate milestones. Parts a, b, c and d are merged into their original chapter.

Selected references

  • Andrew Childs, Lecture Notes on Quantum Algorithms, 17 April 2025. https://www.cs.umd.edu/~amchilds/qa/qa.pdf.
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🏆Completed
Quantum Information·Captain: Goku

Lecture Notes on Quantum Algorithms 2: Group commutators of an ϵ²-net of S_ϵ form an O(ϵ³)-net of S_{ϵ²}Textbook

Motivation

This mission develops Chapter 2 of Lecture Notes on Quantum Algorithms by Andrew Childs. The chapter's selected results describe the mathematical guarantees below.

Setting and conventions

The linked theorem statements and shared definitions specify the register types, oracle access, normalization, and resource conventions. Their source locators and independent readbacks accompany each target.

Chapter goal

For U,V∈SU(2)U,V\in SU(2)U,V∈SU(2) write [ ⁣[U,V] ⁣]=UVU−1V−1[\![U,V]\!]=UVU^{-1}V^{-1}[[U,V]]=UVU−1V−1 for the group commutator. For ϵ≥0\epsilon\ge0ϵ≥0 let

Sϵ={U∈SU(2):∥I−U∥≤ϵ}S_\epsilon=\{U\in SU(2):\|I-U\|\le\epsilon\}Sϵ​={U∈SU(2):∥I−U∥≤ϵ}

be the ϵ\epsilonϵ-ball around the identity, with ∥⋅∥\|\cdot\|∥⋅∥ the spectral norm. For Γ,S⊆SU(2)\Gamma,S\subseteq SU(2)Γ,S⊆SU(2), Γ\GammaΓ is a δ\deltaδ-net for SSS if every A∈SA\in SA∈S has some U∈ΓU\in\GammaU∈Γ with ∥A−U∥≤δ\|A-U\|\le\delta∥A−U∥≤δ.

The lemma says there are constants C>0C>0C>0 and ϵ0>0\epsilon_0>0ϵ0​>0 such that, for every 0<ϵ≤ϵ00<\epsilon\le\epsilon_00<ϵ≤ϵ0​ and every Γ⊆SU(2)\Gamma\subseteq SU(2)Γ⊆SU(2), the following holds. If Γ\GammaΓ is an ϵ2\epsilon^2ϵ2-net for SϵS_\epsilonSϵ​, then

[ ⁣[Γ,Γ] ⁣]={[ ⁣[U,V] ⁣]:U,V∈Γ} is a Cϵ3-net for Sϵ2.[\![\Gamma,\Gamma]\!]=\{[\![U,V]\!]:U,V\in\Gamma\}\ \text{is a } C\epsilon^3\text{-net for } S_{\epsilon^2}.[[Γ,Γ]]={[[U,V]]:U,V∈Γ} is a Cϵ3-net for Sϵ2​.

This is the key step of the Solovay–Kitaev construction. Applied recursively, it turns a coarse net near the identity into nets of doubly-exponentially improving precision.

Formalization Note The source writes O(ϵ3)O(\epsilon^3)O(ϵ3) as ϵ→0\epsilon\to0ϵ→0. Here it is written as explicit constants CCC and ϵ0\epsilon_0ϵ0​, chosen before Γ\GammaΓ, because the source's recursion uses one constant at every level.

Significance

These are known mathematical results. Their Lean statements have been checked and reviewed against the cited source; formal proofs remain open for contributors.

Supporting targets

  • Theorem 2.1: Solovay–Kitaev: gate-set independence with polylogarithmic overhead.
  • Lemma 2.2: Subadditivity of errors in products of unitaries.
  • Lemma 2.3: Group commutators of an ϵ²-net of S_ϵ form an O(ϵ³)-net of S_{ϵ²}.

Formalization scope

Prove the existing statements under their stated hypotheses and definitions. Any correction to a printed source claim remains explicit in its target description. All listed target proofs are currently sorry; no proof is claimed. The mission goal is the designated chapter capstone; the remaining targets are separate milestones. Parts a, b, c and d are merged into their original chapter.

Selected references

  • Andrew Childs, Lecture Notes on Quantum Algorithms, 17 April 2025. https://www.cs.umd.edu/~amchilds/qa/qa.pdf.
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🏆Completed
OptimizationQuantum Information·Captain: Goku

Quantum algorithms for optimizers 6: Unitary conjugation commutes with the matrix exponential: e^{iUHU†t} = U e^{iHt} U†Textbook

Motivation

This mission develops Chapter 6 of Quantum algorithms for optimizers by Giacomo Nannicini. The chapter's selected results describe the mathematical guarantees below.

Setting and conventions

The linked theorem statements and shared definitions specify the register types, oracle access, normalization, and resource conventions. Their source locators and independent readbacks accompany each target.

Chapter goal

Let n≥0n \ge 0n≥0, let UUU be a unitary 2n×2n2^n \times 2^n2n×2n matrix, let H\mathcal{H}H be a Hamiltonian on nnn qubits, that is, a Hermitian 2n×2n2^n \times 2^n2n×2n complex matrix, and let t∈Rt \in \mathbb{R}t∈R. With the matrix exponential eA=∑k=0∞Ak/k!e^A = \sum_{k=0}^\infty A^k / k!eA=∑k=0∞​Ak/k!,

eiUHU†t=U eiHt U†.e^{iU\mathcal{H}U^\dagger t} = U\, e^{i\mathcal{H}t}\, U^\dagger.eiUHU†t=UeiHtU†.

This is what makes diagonalizable Hamiltonians easy to simulate: if UUU diagonalizes H\mathcal{H}H, simulating H\mathcal{H}H reduces to applying U†U^\daggerU†, a diagonal phase, and UUU.

Formalization Note The matrix exponential is Mathlib's power series NormedSpace.exp; U†U^\daggerU† is the conjugate transpose (star U). Hermiticity of H\mathcal{H}H is kept because the source says Hamiltonian (Def. 6.1), although the identity holds for every square matrix.

Significance

These are known mathematical results. Their Lean statements have been checked and reviewed against the cited source; formal proofs remain open for contributors.

Supporting targets

  • Proposition 6.9: Phase condition under which the clock Hamiltonian transports |u^(1)⟩ to e^{iϕ}|u^(N)⟩.
  • Proposition 6.12: Unitary conjugation commutes with the matrix exponential: e^{iUHU†t} = U e^{iHt} U†.

Formalization scope

Prove the existing statements under their stated hypotheses and definitions. Any correction to a printed source claim remains explicit in its target description. All listed target proofs are currently sorry; no proof is claimed. The mission goal is the designated chapter capstone; the remaining targets are separate milestones. Parts a, b, c and d are merged into their original chapter.

Selected references

  • Giacomo Nannicini, Quantum algorithms for optimizers, 2025, v5; notes dated 9 July 2025. https://arxiv.org/pdf/2408.07086v5.
3 thms2 active usersReviewed
🏆Completed
Quantum Information·Captain: Goku

Quantum Computing: Lecture Notes 7: Amplitude amplification: Q^k A|0^m⟩ = sin((2k+1)θ)|ψ1⟩ + cos((2k+1)θ)|ψ0⟩, and O(1/√p) rounds sufficeTextbook

Motivation

This mission develops Chapter 7 of Quantum Computing: Lecture Notes by Ronald de Wolf. The chapter's selected results describe the mathematical guarantees below.

Setting and conventions

The linked theorem statements and shared definitions specify the register types, oracle access, normalization, and resource conventions. Their source locators and independent readbacks accompany each target.

Chapter goal

Let AAA be a unitary on mmm qubits (a circuit without measurements) and p∈(0,1]p\in(0,1]p∈(0,1], and suppose

A∣0m⟩=p ∣ψ1⟩+1−p ∣ψ0⟩,A|0^m\rangle=\sqrt p\,|\psi_1\rangle+\sqrt{1-p}\,|\psi_0\rangle,A∣0m⟩=p​∣ψ1​⟩+1−p​∣ψ0​⟩,

where ∣ψ1⟩,∣ψ0⟩|\psi_1\rangle,|\psi_0\rangle∣ψ1​⟩,∣ψ0​⟩ are orthogonal unit vectors (the good and the bad state). Let RGR_GRG​ be a unitary with RG∣ψ1⟩=−∣ψ1⟩R_G|\psi_1\rangle=-|\psi_1\rangleRG​∣ψ1​⟩=−∣ψ1​⟩ and RG∣ψ0⟩=∣ψ0⟩R_G|\psi_0\rangle=|\psi_0\rangleRG​∣ψ0​⟩=∣ψ0​⟩, let R0R_0R0​ fix ∣0m⟩|0^m\rangle∣0m⟩ and negate every other basis state, and let Q=AR0A−1RGQ=AR_0A^{-1}R_GQ=AR0​A−1RG​ be one round (reflect through ∣ψ0⟩|\psi_0\rangle∣ψ0​⟩, then through ∣U⟩=A∣0m⟩|U\rangle=A|0^m\rangle∣U⟩=A∣0m⟩). Put θ=arcsin⁡p\theta=\arcsin\sqrt pθ=arcsinp​.

  1. For every k∈Nk\in\mathbb Nk∈N,
QkA∣0m⟩=sin⁡((2k+1)θ) ∣ψ1⟩+cos⁡((2k+1)θ) ∣ψ0⟩.Q^kA|0^m\rangle=\sin((2k+1)\theta)\,|\psi_1\rangle+\cos((2k+1)\theta)\,|\psi_0\rangle.QkA∣0m⟩=sin((2k+1)θ)∣ψ1​⟩+cos((2k+1)θ)∣ψ0​⟩.
  1. If k∈Nk\in\mathbb Nk∈N is an integer closest to π4θ−12\frac{\pi}{4\theta}-\frac124θπ​−21​, then k≤π4θ≤π4pk\le\frac{\pi}{4\theta}\le\frac{\pi}{4\sqrt p}k≤4θπ​≤4p​π​, and the good state has probability ∣⟨ψ1∣QkA∣0m⟩∣2≥1−p|\langle\psi_1|Q^kA|0^m\rangle|^2\ge 1-p∣⟨ψ1​∣QkA∣0m⟩∣2≥1−p.

So O(1/p)O(1/\sqrt p)O(1/p​) applications of AAA, A−1A^{-1}A−1 and RGR_GRG​ raise the success probability from ppp to nearly 111, a quadratic improvement over the O(1/p)O(1/p)O(1/p) classical repetitions. Grover's algorithm is the special case A=H⊗nA=H^{\otimes n}A=H⊗n, RG=Ox,±R_G=O_{x,\pm}RG​=Ox,±​.

Formalization Note A−1A^{-1}A−1 is the conjugate transpose A∗A^*A∗ (as AAA is unitary). RGR_GRG​ is constrained only on ψ1\psi_1ψ1​ and ψ0\psi_0ψ0​, as in the source. The hypotheses require m≥1m\ge1m≥1, since two orthonormal vectors need dimension at least 2.

Significance

These are known mathematical results. Their Lean statements have been checked and reviewed against the cited source; formal proofs remain open for contributors.

Supporting targets

  • §7.2: Grover's algorithm with known t: P_k = sin²((2k+1)θ), and k ≈ π/(4θ) − 1/2 ≤ (π/4)√(N/t) iterations succeed with probability ≥ 1 − t/N.
  • §7.3: Amplitude amplification: Q^k A|0^m⟩ = sin((2k+1)θ)|ψ1⟩ + cos((2k+1)θ)|ψ0⟩, and O(1/√p) rounds suffice.

Formalization scope

Prove the existing statements under their stated hypotheses and definitions. Any correction to a printed source claim remains explicit in its target description. All listed target proofs are currently sorry; no proof is claimed. The mission goal is the designated chapter capstone; the remaining targets are separate milestones. Parts a, b, c and d are merged into their original chapter.

Selected references

  • Ronald de Wolf, Quantum Computing: Lecture Notes, 27 August 2026. https://homepages.cwi.nl/~rdewolf/qcnotes.pdf.
3 thms2 active usersReviewed
🏆Completed
Quantum Information·Captain: Goku

Quantum Computing: Lecture Notes 2: Bernstein–Vazirani: one phase query recovers the hidden stringTextbook

Motivation

This mission develops Chapter 2 of Quantum Computing: Lecture Notes by Ronald de Wolf. The chapter's selected results describe the mathematical guarantees below.

Setting and conventions

The linked theorem statements and shared definitions specify the register types, oracle access, normalization, and resource conventions. Their source locators and independent readbacks accompany each target.

Chapter goal

This is the correctness of the Bernstein–Vazirani algorithm.

Let n≥0n \ge 0n≥0 and N=2nN = 2^nN=2n, and fix a hidden string a∈{0,1}na \in \{0,1\}^na∈{0,1}n. The input x∈{0,1}Nx \in \{0,1\}^Nx∈{0,1}N is given by xi=(i⋅a) mod 2x_i = (i \cdot a) \bmod 2xi​=(i⋅a)mod2 for every i∈{0,1}ni \in \{0,1\}^ni∈{0,1}n, where i⋅a=∑k=1nikaki \cdot a = \sum_{k=1}^n i_k a_ki⋅a=∑k=1n​ik​ak​. With the phase query Ox,±:∣i⟩↦(−1)xi∣i⟩O_{x,\pm} : |i\rangle \mapsto (-1)^{x_i}|i\rangleOx,±​:∣i⟩↦(−1)xi​∣i⟩ and the nnn-qubit Hadamard transform H⊗nH^{\otimes n}H⊗n, the Deutsch–Jozsa circuit gives

H⊗n Ox,± H⊗n ∣0n⟩=∣a⟩.H^{\otimes n} \, O_{x,\pm} \, H^{\otimes n} \, |0^n\rangle = |a\rangle .H⊗nOx,±​H⊗n∣0n⟩=∣a⟩.

In particular, measuring the final state in the computational basis yields aaa with probability 111.

So one query and 2n2n2n Hadamard gates (the O(n)O(n)O(n) other operations) recover aaa exactly. Only the query depends on the input. Classically, nnn queries are needed.

Formalization Note The input xxx is bvInput a, i.e. i↦i⋅a mod 2i \mapsto i\cdot a \bmod 2i↦i⋅amod2. The circuit is the same fixed definition deutschJozsaState as in the Deutsch–Jozsa statement. The state equality is exact, with no global phase: the source says the result is the classical state ∣a⟩|a\rangle∣a⟩, and that is what the computation gives.

Significance

These are known mathematical results. Their Lean statements have been checked and reviewed against the cited source; formal proofs remain open for contributors.

Supporting targets

  • §2.4.1: Deutsch–Jozsa: one phase query decides constant vs balanced with certainty.
  • §2.4.2: Bernstein–Vazirani: one phase query recovers the hidden string.

Formalization scope

Prove the existing statements under their stated hypotheses and definitions. Any correction to a printed source claim remains explicit in its target description. All listed target proofs are currently sorry; no proof is claimed. The mission goal is the designated chapter capstone; the remaining targets are separate milestones. Parts a, b, c and d are merged into their original chapter.

Selected references

  • Ronald de Wolf, Quantum Computing: Lecture Notes, 27 August 2026. https://homepages.cwi.nl/~rdewolf/qcnotes.pdf.
2 thms2 active usersReviewed
🏆Completed
OptimizationQuantum Information·Captain: Goku

Quantum algorithms for optimizers 2: Simon's algorithm: n+t uniform samples orthogonal to a contain n−1 independent vectors with probability ≥ 1 − 2^{−(t+1)}Textbook

Motivation

This mission develops Chapter 2 of Quantum algorithms for optimizers by Giacomo Nannicini. The chapter's selected results describe the mathematical guarantees below.

Setting and conventions

The linked theorem statements and shared definitions specify the register types, oracle access, normalization, and resource conventions. Their source locators and independent readbacks accompany each target.

Chapter goal

This is the sampling bound behind the classical post-processing of Simon's algorithm.

Let n≥1n \ge 1n≥1 and t≥0t \ge 0t≥0 be integers, and let F2={0,1}\mathbb F_2 = \{0,1\}F2​={0,1} be the field with two elements. Fix a nonzero vector a∈F2na \in \mathbb F_2^na∈F2n​ and let

Va={k∈F2n:k⋅a=∑i=1nkiai≡0(mod2)}V_a = \{k \in \mathbb F_2^n : k \cdot a = \textstyle\sum_{i=1}^n k_i a_i \equiv 0 \pmod 2\}Va​={k∈F2n​:k⋅a=∑i=1n​ki​ai​≡0(mod2)}

be the (n−1)(n-1)(n−1)-dimensional subspace of vectors orthogonal to aaa. Draw k(1),…,k(n+t)k^{(1)}, \dots, k^{(n+t)}k(1),…,k(n+t) independently and uniformly at random from VaV_aVa​. Then

Pr⁡[some n−1 of k(1),…,k(n+t) are linearly independent over F2]≥1−12t+1.\Pr\big[\text{some } n-1 \text{ of } k^{(1)}, \dots, k^{(n+t)} \text{ are linearly independent over } \mathbb F_2\big] \ge 1 - \frac{1}{2^{t+1}}.Pr[some n−1 of k(1),…,k(n+t) are linearly independent over F2​]≥1−2t+11​.

The bound does not depend on nnn, so n+O(1)n + O(1)n+O(1) runs of Simon's circuit suffice to determine the hidden string aaa with high probability.

Formalization Note The probability is the fraction of all ∣Va∣n+t|V_a|^{n+t}∣Va​∣n+t tuples (k(1),…,k(n+t))∈Van+t(k^{(1)},\dots,k^{(n+t)}) \in V_a^{n+t}(k(1),…,k(n+t))∈Van+t​ for which there are n−1n-1n−1 distinct indices whose vectors are linearly independent; vectors of F2n\mathbb F_2^nF2n​ are functions Fin n→Z/2Z\mathrm{Fin}\,n \to \mathbb Z/2\mathbb ZFinn→Z/2Z.

Significance

These are known mathematical results. Their Lean statements have been checked and reviewed against the cited source; formal proofs remain open for contributors.

Supporting targets

  • Proposition 2.8: Simon's algorithm: n+t uniform samples orthogonal to a contain n−1 independent vectors with probability ≥ 1 − 2^{−(t+1)}.

Formalization scope

Prove the existing statements under their stated hypotheses and definitions. Any correction to a printed source claim remains explicit in its target description. All listed target proofs are currently sorry; no proof is claimed. The mission goal is the designated chapter capstone; the remaining targets are separate milestones. Parts a, b, c and d are merged into their original chapter.

Selected references

  • Giacomo Nannicini, Quantum algorithms for optimizers, 2025, v5; notes dated 9 July 2025. https://arxiv.org/pdf/2408.07086v5.
1 thm2 active usersReviewed
🏆Completed
Quantum Information·Captain: Goku

Lecture Notes on Quantum Algorithms 5: Ω(√N) deterministic classical queries for the HSP with N trivially intersecting subgroupsTextbook

Motivation

This mission develops Chapter 5 of Lecture Notes on Quantum Algorithms by Andrew Childs. The chapter's selected results describe the mathematical guarantees below.

Setting and conventions

The linked theorem statements and shared definitions specify the register types, oracle access, normalization, and resource conventions. Their source locators and independent readbacks accompany each target.

Chapter goal

In the hidden subgroup problem (HSP) on a finite group GGG, an algorithm has black-box access to a function f:G→Sf : G \to Sf:G→S, where SSS is a finite set, promised to hide some unknown subgroup H≤GH \le GH≤G:

f(x)=f(y)  ⟺  x−1y∈H(x,y∈G).f(x) = f(y) \iff x^{-1}y \in H \qquad (x, y \in G).f(x)=f(y)⟺x−1y∈H(x,y∈G).

The goal is to determine HHH. A deterministic classical algorithm is a decision tree: it queries group elements g1,g2,…g_1, g_2, \dotsg1​,g2​,… adaptively, each query returning f(gℓ)∈Sf(g_\ell) \in Sf(gℓ​)∈S, and finally outputs a subgroup of GGG. It solves the HSP if, for every subgroup H≤GH \le GH≤G and every fff hiding HHH, its output is HHH. Its query count on input fff is the number of queries it makes on fff.

Theorem. There are an absolute constant c>0c > 0c>0 and a threshold N0N_0N0​ such that the following holds for every N≥N0N \ge N_0N≥N0​. Let GGG be a finite group and SSS a finite set with ∣S∣≥∣G∣|S| \ge |G|∣S∣≥∣G∣, and suppose GGG has a family H\mathcal HH of NNN distinct subgroups any two of which have only the identity in common, i.e. H∩K={1}H \cap K = \{1\}H∩K={1} for all distinct H,K∈HH, K \in \mathcal HH,K∈H. Then every deterministic classical algorithm that solves the HSP on GGG (with values in SSS) makes, on some input fff hiding some subgroup of GGG,

#queries(f)≥cN.\#\text{queries}(f) \ge c\sqrt{N}.#queries(f)≥cN​.

The theorem shows that the HSP is classically hard whenever the group has many trivially intersecting subgroups (for example Simon's problem), in contrast with efficient quantum algorithms for abelian groups.

Formalization Note The algorithm outputs the subgroup itself rather than a generating set, which changes nothing for a query lower bound. The condition ∣S∣≥∣G∣|S| \ge |G|∣S∣≥∣G∣ makes every subgroup of GGG hideable; the proof's adversary labels each new query with a fresh value, and with a very small SSS (say ∣S∣=1|S| = 1∣S∣=1) only H=GH = GH=G can be hidden, so the bound would fail. The constants ccc and N0N_0N0​ are chosen before the group, the set SSS, the family and the algorithm. The threshold N0N_0N0​ is needed because for the trivial group N=1N = 1N=1 and no queries are needed. The phrase "whose only common element is the identity" is read pairwise, as in the section's "trivially intersecting subgroups" and as the proof needs when it counts at most t(t−1)t(t-1)t(t−1) non-identity values gj−1gkg_j^{-1}g_kgj−1​gk​ against NNN subgroups. Read as ⋂H={1}\bigcap \mathcal H = \{1\}⋂H={1}, the theorem is false: in the cyclic group of squarefree order p1⋯pkp_1\cdots p_kp1​⋯pk​, all 2k2^k2k subgroups intersect trivially, yet k+1k+1k+1 queries determine HHH.

Significance

These are known mathematical results. Their Lean statements have been checked and reviewed against the cited source; formal proofs remain open for contributors.

Supporting targets

  • Theorem 5.1: Ω(√N) deterministic classical queries for the HSP with N trivially intersecting subgroups.

Formalization scope

Prove the existing statements under their stated hypotheses and definitions. Any correction to a printed source claim remains explicit in its target description. All listed target proofs are currently sorry; no proof is claimed. The mission goal is the designated chapter capstone; the remaining targets are separate milestones. Parts a, b, c and d are merged into their original chapter.

Selected references

  • Andrew Childs, Lecture Notes on Quantum Algorithms, 17 April 2025. https://www.cs.umd.edu/~amchilds/qa/qa.pdf.
1 thm2 active usersReviewed
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