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Algorithmic Game TheoryDynamical SystemsProbability+1·Captain: mikedeng1

On the Global Convergence of Stochastic Fictitious Play III: Almost Sure Convergence to Linearly Stable Rest Points in Potential GamesResearch Paper

Motivation

Stochastic fictitious play is a basic model of learning in repeated games. Each period every player best responds to the empirical frequencies of the opponents' past play, after the player's payoffs have been hit by a fresh random shock. It was introduced by Fudenberg and Kreps (1993), is a standard object in the theory of learning in games (Fudenberg and Levine, The Theory of Learning in Games, 1998), and underlies the quantal-response and logit-learning models used in experimental economics and multi-agent reinforcement learning. The question is whether the players' beliefs settle down, and on what.

Potential games, in which all players receive the same payoff, cover pure coordination games and, after the usual payoff transformations, congestion games and weighted potential games. For them Hofbauer and Sandholm (Econometrica 70, 2002) proved that stochastic fictitious play converges almost surely, and that under a generic regularity condition the limit is a single linearly stable rest point of the perturbed best response dynamic.

Timeline. Fudenberg and Kreps (1993) and Kaniovski and Young (1995) established convergence in 2×2 games. Benaïm and Hirsch (1999) related the process to its mean ordinary differential equation and proved convergence in some ppp player, two strategy games. Hofbauer (2000) and Hofbauer and Hopkins (2000) constructed Lyapunov functions for the deterministically perturbed dynamics. Hofbauer and Sandholm (2002) combined these with a representation theorem for random utility models and with Pemantle's (1990) nonconvergence theorem to obtain the result formalized here.

Setting

A ppp player game has finite strategy sets Sα={0,…,nα−1}S^\alpha = \{0,\dots,n^\alpha-1\}Sα={0,…,nα−1} and utilities uα:S→Ru^\alpha : S \to \mathbb Ruα:S→R on pure profiles S=∏βSβS = \prod_\beta S^\betaS=∏β​Sβ. The game is a potential game if uα(s)=uβ(s)u^\alpha(s) = u^\beta(s)uα(s)=uβ(s) for all players and all profiles. Mixed profiles form Σ=∏αΔSα\Sigma = \prod_\alpha \Delta S^\alphaΣ=∏α​ΔSα, and player α\alphaα's payoff vector is Uiα(x−α)=∑s: sα=iuα(s)∏β≠αxsββU^\alpha_i(x^{-\alpha}) = \sum_{s:\,s^\alpha=i} u^\alpha(s)\prod_{\beta\ne\alpha}x^\beta_{s^\beta}Uiα​(x−α)=∑s:sα=i​uα(s)∏β=α​xsββ​.

Player α\alphaα's payoffs are perturbed by a random vector εα\varepsilon^\alphaεα with a strictly positive density fαf^\alphafα on Rnα\mathbb R^{n^\alpha}Rnα. The choice function is Ciα(π)=P(arg⁡max⁡jπj+εjα=i)C^\alpha_i(\pi) = P(\arg\max_j \pi_j + \varepsilon^\alpha_j = i)Ciα​(π)=P(argmaxj​πj​+εjα​=i), assumed continuously differentiable, and the perturbed best response is B~α(x−α)=Cα(Uα(x−α))\tilde B^\alpha(x^{-\alpha}) = C^\alpha(U^\alpha(x^{-\alpha}))B~α(x−α)=Cα(Uα(x−α)).

In standard stochastic fictitious play, shocks εtα\varepsilon^\alpha_tεtα​ are independent over time and across players. From an arbitrary initial pure profile, at time t+1t+1t+1 each player plays a maximizer of Ukα(Zt−α)+(εtα)kU^\alpha_k(Z_t^{-\alpha}) + (\varepsilon^\alpha_t)_kUkα​(Zt−α​)+(εtα​)k​, where the beliefs are the time averages

Zt=1t∑u=1tζu.Z_t = \frac1t\sum_{u=1}^t \zeta_u .Zt​=t1​u=1∑t​ζu​.

The mean dynamic of this process is the perturbed best response dynamic

(P)x˙α=B~α(x−α)−xα.(P)\qquad \dot x^\alpha = \tilde B^\alpha(x^{-\alpha}) - x^\alpha .(P)x˙α=B~α(x−α)−xα.

A rest point x∗x^*x∗ of (P) is hyperbolic if every eigenvalue of DF(x∗)DF(x^*)DF(x∗) restricted to the tangent space ∏αR0nα\prod_\alpha \mathbb R^{n^\alpha}_0∏α​R0nα​ of Σ\SigmaΣ has nonzero real part, and linearly stable if every such eigenvalue has negative real part. RP(P)RP(P)RP(P) and LS(P)LS(P)LS(P) denote the rest points and the linearly stable rest points.

By Theorem 2.1 of the paper, Cα(π)=arg⁡max⁡y∈int⁡Δ(y⋅π−Vα(y))C^\alpha(\pi) = \arg\max_{y\in\operatorname{int}\Delta}(y\cdot\pi - V^\alpha(y))Cα(π)=argmaxy∈intΔ​(y⋅π−Vα(y)) for an admissible deterministic perturbation VαV^\alphaVα, so (P) coincides with the deterministically perturbed dynamic (PV), in which the argmax replaces CαC^\alphaCα.

Formalization targets

Goal: Theorem 6.1(iii)

For every potential game, every family of densities meeting the conditions above, every probability space, independent shock family and initial profile:

  1. if the shocks are smooth enough that the VαV^\alphaVα are CNC^NCN, N=∑α(nα−1)N = \sum_\alpha(n^\alpha-1)N=∑α​(nα−1), then
P(ω(Zt) is a connected subset of RP(P))=1;P\big(\omega(Z_t)\text{ is a connected subset of } RP(P)\big) = 1;P(ω(Zt​) is a connected subset of RP(P))=1;
  1. if every rest point of (P) is hyperbolic and the field of (P) is C2C^2C2, then
P(lim⁡t→∞Zt exists and lies in LS(P))=1.P\Big(\lim_{t\to\infty} Z_t \text{ exists and lies in } LS(P)\Big) = 1.P(t→∞lim​Zt​ exists and lies in LS(P))=1.

Milestones

In attack order: Theorem 2.1 (the representation), Proposition 4.1 (the function Π(x)=∑su1(s)∏αxsαα−∑αVα(xα)\Pi(x) = \sum_s u^1(s)\prod_\alpha x^\alpha_{s^\alpha} - \sum_\alpha V^\alpha(x^\alpha)Π(x)=∑s​u1(s)∏α​xsαα​−∑α​Vα(xα) is a strict Lyapunov function for (PV)), the identification of the critical points of Π\PiΠ with the rest points of (PV), Proposition 4.2 (CR(PV)=RP(PV)CR(PV) = RP(PV)CR(PV)=RP(PV) under CNC^NCN smoothness), Proposition 4.3 (under hyperbolicity RP(PV)RP(PV)RP(PV) is finite and equals CR(PV)CR(PV)CR(PV)), and Lemmas A.5 and A.4 (a uniform nondegeneracy condition for the noise of the process).

Significance

The result. Theorem 6.1(iii) says that decentralised, boundedly rational learning in common-interest games does not cycle or wander: beliefs converge to a rest point of the perturbed dynamic, and generically to one that is linearly stable, hence a local maximizer of the perturbed potential Π\PiΠ. Rest points approximate Nash equilibria as the noise vanishes (Proposition 3.1 of the paper), so the theorem is a selection result for equilibria reached by learning. It is also a template for the stochastic-approximation analysis of learning algorithms whose mean dynamic has a Lyapunov function.

Formalizing it. The theorem is proved in the paper, but none of its ingredients is machine-checked: the random utility representation, chain recurrence of flows, Lyapunov arguments for (PV), and the stochastic-approximation step (Benaïm–Hirsch, Benaïm, Pemantle) are all absent from Mathlib and from this platform. A complete development produces a reusable stochastic-approximation layer, not only this theorem.

Difficulty

The obvious argument, "(P) has a strict Lyapunov function, so the process converges to its rest points", fails twice. First, a strict Lyapunov function does not by itself make every chain recurrent point a rest point (the paper cites counterexamples of Akin and of Benaïm); the step needs either Sard's theorem for a CNC^NCN function or finiteness of the rest points, and the stochastic-approximation theory controls the process only through the chain recurrent set. Second, convergence to linearly stable points requires showing that the process avoids unstable rest points. This rests on Pemantle's theorem, whose nondegeneracy hypothesis must be verified uniformly over states and directions (Lemma A.4). Neither step follows from the ODE alone: the theorem is about the random process ZtZ_tZt​.

Formalization scope

Players are Fin p with p ≥ 2, strategies Fin (n α) with n α ≥ 1, and mixed profiles live in the ambient space (α : Fin p) → Fin (n α) → ℝ, on which every vector field is defined. Choice probabilities are probabilities of strict argmax events under volume.withDensity (f α). The process ZtZ_tZt​ is defined pathwise from the shocks, ties broken by the smallest index (a null event), and the theorem quantifies over every probability space and every independent shock family with the given laws. Derivatives of VαV^\alphaVα are those of VαV^\alphaVα composed with the projection onto the plane ∑iyi=1\sum_i y_i = 1∑i​yi​=1. Eigenvalues are the complex roots of the characteristic polynomial of the derivative restricted to the tangent space of Σ\SigmaΣ. Solutions of a dynamic are differentiable curves on [0,∞)[0,\infty)[0,∞) that stay in Σ\SigmaΣ, and chain recurrence uses ε\varepsilonε-chains with times ti≥1t_i \ge 1ti​≥1.

A formalization about the ODE (P) in place of the process ZtZ_tZt​, a fixed noise law such as logit, or convergence to RP(P)RP(P)RP(P) in place of LS(P)LS(P)LS(P) would prove a different and weaker statement. These are excluded.

Needed infrastructure: the random utility representation (mission I of this series), flows and chain recurrence of C1C^1C1 vector fields on compact sets, Sard's theorem for real-valued CNC^NCN functions, and the stochastic-approximation theorems of Benaïm–Hirsch (1999, Thm 3.3), Benaïm (1999, Props. 5.3 and 6.4) and Pemantle (1990, Thm 1). The last three are reusable well beyond this mission, and contributions of any of them are welcome.

Selected references

  • J. Hofbauer and W. H. Sandholm, On the Global Convergence of Stochastic Fictitious Play, Econometrica 70(6), 2265–2294, 2002. https://doi.org/10.1111/1468-0262.00376
  • M. Benaïm and M. W. Hirsch, Mixed Equilibria and Dynamical Systems Arising from Fictitious Play in Perturbed Games, Games and Economic Behavior 29, 36–72, 1999. https://doi.org/10.1006/game.1999.0717
  • M. Benaïm, Dynamics of Stochastic Approximation Algorithms, Séminaire de Probabilités XXXIII, Lecture Notes in Mathematics 1709, 1–68, 1999. https://doi.org/10.1007/BFb0096509
  • R. Pemantle, Nonconvergence to Unstable Points in Urn Models and Stochastic Approximations, Annals of Probability 18(2), 698–712, 1990. https://doi.org/10.1214/aop/1176990853
  • D. Fudenberg and D. M. Kreps, Learning Mixed Equilibria, Games and Economic Behavior 5, 320–367, 1993. https://doi.org/10.1006/game.1993.1021
  • J. Hofbauer and E. Hopkins, Learning in Perturbed Asymmetric Games, Games and Economic Behavior 52, 133–152, 2005. https://doi.org/10.1016/j.geb.2004.06.006
14 thms4 active usersReviewed
Linear OptimizationOperations ResearchOptimization·Captain: Shuze Chen

Disjunctive Programming IX: The Correspondence Between Lift-and-Project Cuts and Simple Disjunctive CutsTextbook

Motivation

Chapter 6 built lift-and-project (L&P) cuts from a cut-generating LP, and Chapter 7 surveyed alternative nonlinear constructions reaching the same integer hull. This chapter asks a sharper question: how do L&P cuts relate, coefficient for coefficient, to older, more classical cutting planes — simple disjunctive cuts and mixed integer Gomory cuts, derived directly from a simplex tableau rather than from an auxiliary LP? The answer is an exact correspondence: every L&P cut from a basic solution of the cut-generating LP is equivalent to a specific simple disjunctive cut from a specific tableau basis, and conversely. This correspondence is not merely of theoretical interest — it converts a question about an infinite family of cuts into a finite, countable one (bases of a linear system), and it is what lets the chapter's capstone result, Theorem 8.7, establish a uniform rank bound of ppp (the number of 0-1 variables) across four cut families at once, by proving it for one and transporting the proof to the other three.

Setting

(CGLP)k(CGLP)_k(CGLP)k​ (eq. (8.1)) is the cut-generating LP for the disjunction −xk≥0∨xk≥1-x_k \ge 0 \lor x_k \ge 1−xk​≥0∨xk​≥1, with an added normalization constraint ue+u0+ve+v0=1ue+u_0+ve+v_0=1ue+u0​+ve+v0​=1 that makes its feasible polytope bounded — so a "basic solution" can be identified with an extreme point of that polytope. Given a basic solution with u0,v0>0u_0,v_0>0u0​,v0​>0 and basic u/vu/vu/v-components indexed by M1,M2M_1,M_2M1​,M2​ (Lemma 8.1-8.2), the n×nn\times nn×n submatrix A^\hat AA^ of A~\tilde AA~ indexed by J:=M1∪M2J:=M_1\cup M_2J:=M1​∪M2​ is nonsingular, giving a simplex tableau in which xkx_kxk​ is expressed as xk=aˉk0−∑j∈Jaˉkjxjx_k = \bar a_{k0} - \sum_{j\in J}\bar a_{kj}x_jxk​=aˉk0​−∑j∈J​aˉkj​xj​ (eq. (8.5)). The simple disjunctive cut from xk≤0∨xk≥1x_k\le 0 \lor x_k\ge 1xk​≤0∨xk​≥1 applied to this row has coefficients πj:=max⁡{πj1,πj2}\pi_j := \max\{\pi^1_j,\pi^2_j\}πj​:=max{πj1​,πj2​}, π0:=aˉk0(1−aˉk0)\pi_0 := \bar a_{k0}(1-\bar a_{k0})π0​:=aˉk0​(1−aˉk0​) (eq. (8.7)-(8.8)).

Formalization targets

Theorem 8.7 (goal) — a uniform rank bound across four cut families

The rank of the LP relaxation PPP with respect to (a) unstrengthened L&P cuts, (b) simple disjunctive cuts, (c) strengthened L&P cuts, (d) mixed integer Gomory cuts (equivalently, strengthened simple disjunctive cuts) is at most ppp, the number of 0-1 variables.

The chain of results building toward it

Lemma 8.1 (basicness forces u0,v0>0u_0,v_0>0u0​,v0​>0), Lemma 8.2 (a basic solution's index sets give a nonsingular submatrix), Lemma 8.3 (0<aˉk0<10<\bar a_{k0}<10<aˉk0​<1), Theorem 8.4A (a basic L&P cut equals a simple disjunctive cut), Theorem 8.4B (the converse: every simple disjunctive cut from a valid basis equals some basic L&P cut), and Theorem 8.5 (the same correspondence, strengthened).

Significance

The results themselves. Theorems 8.4A/8.4B are, in the book's own words, an "exact correspondence between lift-and-project cuts for a mixed 0-1 program and earlier cuts from the literature" — placing L&P cuts, simple disjunctive cuts, and (via Theorem 8.5) mixed integer Gomory cuts on the same logical footing, all generated by choosing a basis of one underlying linear system. Theorem 8.7 is the payoff: a single uniform bound covering four cut families that the literature had previously bounded (if at all) by separate arguments, and by contrast to the unbounded rank of pure-integer fractional Gomory cuts, exhibiting a case where the mixed 0-1 structure yields much stronger guarantees.

Formalizing it. No object in this mission exists on the platform prior to it or in Mathlib. This mission restates 06-lift-project-cuts's (CGLP)(CGLP)(CGLP) apparatus and Theorem 6.4's strengthened cut formula locally, per the series convention that a draft mission cannot import another draft mission's definitions, adapted throughout to this chapter's normalized (CGLP)k(CGLP)_k(CGLP)k​ and its disjunction on a single fixed coordinate kkk.

Difficulty

Formalizing "basic solution" required a genuine choice: unlike Chapter 6, (CGLP)k(CGLP)_k(CGLP)k​'s normalization constraint makes its feasible set a bounded polytope, so this mission identifies "basic solution" with an extreme point of that polytope (Set.extremePoints) for Lemma 8.1 (whose own statement has no reference to specific index sets), while Lemmas 8.2 onward take the basic index sets M1,M2M_1,M_2M1​,M2​ directly as hypothesis data, matching how those theorems are themselves phrased ("let the basic components... be indexed by M1M_1M1​ and M2M_2M2​"). Theorem 8.7's rank bound required designing one generic HasRankAtMost predicate, parametrized by an abstract cut-closure operator, applicable uniformly to all four families — mirroring the book's own proof structure, which establishes the bound for one family and transports it to the other three via Theorems 8.4A/8.4B and 8.5, rather than arguing each part from scratch.

Formalization scope

The row/variable identification gap (see MODERATION_NOTES.md). The book's own eq. (8.4)- (8.5) identifies certain rows of the augmented, m+p+nm+p+nm+p+n-row matrix A~\tilde AA~ (those that are bound constraints xj≥0x_j\ge 0xj​≥0) with the variables they bound, so that a chosen nonbasic row set JJJ doubles as a set of "nonbasic variables." This mission's abstract row type does not track that identification (matching the abstraction already used throughout 06-lift-project-cuts and 07-higher-dim): Surplus instead defines the tableau row's nonbasic quantities directly as the slack expression sj:=(A~x)j−b~js_j := (\tilde Ax)_j - \tilde b_jsj​:=(A~x)j​−b~j​, a genuine affine function of xxx for every row, which reduces to xjx_jxj​ itself exactly when row jjj is that bound constraint — mathematically equivalent to the book's own substitution, stated without needing the row-to-variable lookup. Eq. (8.10)'s "j∈J∩N′j\in J\cap N'j∈J∩N′" strengthening-eligibility test has the same gap; this mission takes the row-positions eligible for strengthening as an explicit Finset parameter rather than deriving membership from row identity.

Corollary 8.6 is out of scope for this mission — see HARD.md. Its facet-counting bound depends on the same row/variable identification (the printed bound is (m+p+n−1n)\binom{m+p+n-1}{n}(nm+p+n−1​), excluding row kkk specifically because it is xkx_kxk​'s own bound row) and would additionally require a general notion of "number of facets of a polyhedron" that this mission's abstraction, and Mathlib, do not provide; it does not feed Theorem 8.7's own proof, which cites only Theorems 8.4A/8.4B and 8.5.

Theorem 8.7 is stated via one generic HasRankAtMost predicate applied to SplitConvexify (part a) and three closure operators (SimpleDisjClosureOfSet, StrengthenedLPClosureOfSet, MIGClosureOfSet, parts b-d) defined by intersecting a represented polyhedron with every cut of the corresponding family, then lifted to bare sets by quantifying over every linear representation — since, unlike the split-convexification closure, these three cut families are defined via an explicit basis or CGLP solution and so genuinely need some concrete representation of the current polyhedron at each step of the recursion (the same representation-dependence Theorem 7.5's Lovász-Schrijver iteration required in 07-higher-dim).

Selected references

  • E. Balas, Disjunctive Programming, Springer, 2018. DOI: 10.1007/978-3-030-00148-3, Chapter 8.
  • E. Balas, M. Perregaard, A precise correspondence between lift-and-project cuts, simple disjunctive cuts, and mixed integer Gomory cuts for 0-1 programming, Mathematical Programming B 94 (2003), 221–245 (cited in the text as [33], the origin of Lemma 8.2 and Theorems 8.4A/8.4B).
  • E. Balas, M. Perregaard, Lift-and-project for mixed 0-1 programming: recent progress, Discrete Applied Mathematics 123 (2002), 129–154 (cited in the text as [32], the origin of Theorem 8.5's strengthened-cut coefficient identification).
  • F. Eisenbrand, A. Schulz, Bounds on the Chvátal rank of polytopes in the 0-1 cube, in Integer Programming and Combinatorial Optimization (IPCO 7), LNCS 1610 (1999), 137–150 (cited in the text as [73], the source of the unbounded pure-integer Gomory rank result this chapter's Theorem 8.7 contrasts with).
14 thms4 active users
Operations ResearchProbabilityStatistics+1·Captain: mikedeng1

Weak Convergence and Optimal Scaling of Random Walk Metropolis Algorithms: Langevin Diffusion Limit of the First CoordinateResearch Paper

Motivation

The random walk Metropolis algorithm is one of the most widely used Markov chain Monte Carlo methods for sampling from a density known up to a constant. Its one tuning parameter is the variance of the Gaussian proposal. If the variance is too small, the chain accepts almost every move but barely moves. If it is too large, it proposes long jumps that are almost always rejected. Practitioners need a rule for choosing it, and the rule has to work in high dimension, where both failure modes are severe.

Roberts, Gelman and Gilks (Ann. Appl. Probab. 7(1), 1997) gave the first rigorous answer for product targets. As the dimension grows, one coordinate of the suitably speeded-up chain converges to a Langevin diffusion. The speed of that diffusion is an explicit function of the proposal scale, and maximising it gives the rule "tune the proposal so that about 23% of proposals are accepted". This rule, and the 2.38/√I scaling behind it, is now standard advice in applied Bayesian statistics.

Setting

Let f:R→Rf:\mathbb R\to\mathbb Rf:R→R be a target density: positive, C2C^2C2, integrating to one, with f′/ff'/ff′/f Lipschitz, and satisfying the moment conditions (A1) Ef[(f′/f)8]<∞\mathbb E_f[(f'/f)^8]<\inftyEf​[(f′/f)8]<∞ and (A2) Ef[(f′′/f)4]<∞\mathbb E_f[(f''/f)^4]<\inftyEf​[(f′′/f)4]<∞. Here Ef[g(X)]=∫g(x)f(x) dx\mathbb E_f[g(X)]=\int g(x)f(x)\,dxEf​[g(X)]=∫g(x)f(x)dx. In dimension n≥2n\ge2n≥2 the target is the product density πn(x)=∏i=1nf(xi)\pi_n(x)=\prod_{i=1}^n f(x_i)πn​(x)=∏i=1n​f(xi​) on Rn\mathbb R^nRn.

Fix a scale l>0l>0l>0 and set σn2=l2/(n−1)\sigma_n^2=l^2/(n-1)σn2​=l2/(n−1). The random walk Metropolis chain Xn=(X0n,X1n,… )X^n=(X^n_0,X^n_1,\dots)Xn=(X0n​,X1n​,…) moves as follows. From Xm−1nX^n_{m-1}Xm−1n​ it proposes Y∼N(Xm−1n,σn2In)Y\sim N(X^n_{m-1},\sigma_n^2I_n)Y∼N(Xm−1n​,σn2​In​). It sets Xmn=YX^n_m=YXmn​=Y with probability α(Xm−1n,Y)=1∧πn(Y)/πn(Xm−1n)\alpha(X^n_{m-1},Y)=1\wedge\pi_n(Y)/\pi_n(X^n_{m-1})α(Xm−1n​,Y)=1∧πn​(Y)/πn​(Xm−1n​), and Xmn=Xm−1nX^n_m=X^n_{m-1}Xmn​=Xm−1n​ otherwise. The chain starts from πn\pi_nπn​, which is stationary for it. The speeded-up first coordinate is Utn=X⌊nt⌋,1nU^n_t=X^n_{\lfloor nt\rfloor,1}Utn​=X⌊nt⌋,1n​ for t≥0t\ge0t≥0.

Let Φ\PhiΦ be the standard normal distribution function, and define the roughness I=Ef[(f′(X)/f(X))2]I=\mathbb E_f[(f'(X)/f(X))^2]I=Ef​[(f′(X)/f(X))2]. The speed and the limiting acceptance rate are

h(l)=2l2 Φ ⁣(−lI2),a(l)=2 Φ ⁣(−lI2).h(l)=2l^2\,\Phi\!\Big(-\frac{l\sqrt I}{2}\Big),\qquad a(l)=2\,\Phi\!\Big(-\frac{l\sqrt I}{2}\Big).h(l)=2l2Φ(−2lI​​),a(l)=2Φ(−2lI​​).

The Langevin generator is GV(x)=h(l)[12V′′(x)+12(log⁡f)′(x)V′(x)]GV(x)=h(l)\big[\tfrac12V''(x)+\tfrac12(\log f)'(x)V'(x)\big]GV(x)=h(l)[21​V′′(x)+21​(logf)′(x)V′(x)]. It generates the Langevin diffusion dUt=h(l)1/2dBt+h(l)f′(Ut)2f(Ut)dtdU_t=h(l)^{1/2}dB_t+h(l)\frac{f'(U_t)}{2f(U_t)}dtdUt​=h(l)1/2dBt​+h(l)2f(Ut​)f′(Ut​)​dt.

Formalization targets

Goal: Theorem 1.1

As n→∞n\to\inftyn→∞,

Un⇒U,U^n\Rightarrow U,Un⇒U,

where ⇒\Rightarrow⇒ denotes weak convergence in the Skorokhod topology, U0U_0U0​ has density fff, and UUU is the Langevin diffusion with speed h(l)h(l)h(l). The limit is asserted to exist. No constants appear in the statement beyond those the model defines.

Milestones: the proof

  1. Lemma 2.1. The stationary chain stays in the sets Fn={∣Rn−I∣<n−1/8}∩{∣Sn−I∣<n−1/8}F_n=\{|R_n-I|<n^{-1/8}\}\cap\{|S_n-I|<n^{-1/8}\}Fn​={∣Rn​−I∣<n−1/8}∩{∣Sn​−I∣<n−1/8} up to time ttt with probability tending to one. Here RnR_nRn​ and SnS_nSn​ are the empirical averages of ((log⁡f)′)2((\log f)')^2((logf)′)2 and −(log⁡f)′′-(\log f)''−(logf)′′ over coordinates 2,…,n2,\dots,n2,…,n.
  2. Proposition 2.2. ∣1∧ex−1∧ey∣≤∣x−y∣|1\wedge e^x-1\wedge e^y|\le|x-y|∣1∧ex−1∧ey∣≤∣x−y∣.
  3. Lemma 2.3. sup⁡x∈FnE∣Wn∣→0\sup_{x\in F_n}\mathbb E|W_n|\to0supx∈Fn​​E∣Wn​∣→0, where WnW_nWn​ is the second-order part of the log acceptance ratio.
  4. Proposition 2.4. E[1∧eA]=Φ(μ/σ)+eμ+σ2/2Φ(−σ−μ/σ)\mathbb E[1\wedge e^A]=\Phi(\mu/\sigma)+e^{\mu+\sigma^2/2}\Phi(-\sigma-\mu/\sigma)E[1∧eA]=Φ(μ/σ)+eμ+σ2/2Φ(−σ−μ/σ) for A∼N(μ,σ2)A\sim N(\mu,\sigma^2)A∼N(μ,σ2).
  5. Lemma 2.5. lim sup⁡nsup⁡x1n∣E[V(Y1)−V(x1)]∣<∞\limsup_n\sup_{x_1}n|\mathbb E[V(Y_1)-V(x_1)]|<\inftylimsupn​supx1​​n∣E[V(Y1​)−V(x1​)]∣<∞ for V∈Cc∞V\in C_c^\inftyV∈Cc∞​.
  6. Lemma 2.6. The discrete generator GnV(x)=n E[(V(Y)−V(x))α(x,Y)]G_nV(x)=n\,\mathbb E[(V(Y)-V(x))\alpha(x,Y)]Gn​V(x)=nE[(V(Y)−V(x))α(x,Y)] converges to GVGVGV uniformly on FnF_nFn​, for V∈Cc∞V\in C_c^\inftyV∈Cc∞​ a function of the first coordinate (stated with bounded (log⁡f)′′′(\log f)'''(logf)′′′, the assumption its proof uses).

Milestones: the optimal-scaling corollary

  1. Corollary 1.2 (i). an(l)=∬πn(x)α(x,y)qn(x,y) dx dy→a(l)a_n(l)=\iint\pi_n(x)\alpha(x,y)q_n(x,y)\,dx\,dy\to a(l)an​(l)=∬πn​(x)α(x,y)qn​(x,y)dxdy→a(l).
  2. Corollary 1.2 (ii). hhh is maximised at l^=2.38/I\hat l=2.38/\sqrt Il^=2.38/I​, with a(l^)=0.23a(\hat l)=0.23a(l^)=0.23 and h(l^)=1.3/Ih(\hat l)=1.3/Ih(l^)=1.3/I, to the printed precision.

Significance

Theorem 1.1 shows that, run for nnn times as many steps, the chain in dimension nnn looks like a fixed one-dimensional diffusion. The algorithm's cost therefore grows linearly in dimension, and its efficiency is measured by the single number h(l)h(l)h(l). Corollary 1.2 turns this into the 0.234 acceptance-rate heuristic and the 2.38/I2.38/\sqrt I2.38/I​ scaling. The same diffusion-limit method has since been applied to the Metropolis-adjusted Langevin algorithm, to Hamiltonian Monte Carlo and to non-product targets.

The theorem is proved on paper; it has no machine-checked proof. A formal development would give the first verified diffusion limit of an MCMC algorithm. It would also yield reusable components: the Metropolis chain on Rn\mathbb R^nRn as a measurable random mapping, a martingale-problem characterisation of one-dimensional diffusions, and a Gaussian computation (Proposition 2.4) that recurs throughout the optimal-scaling literature.

Difficulty

The obvious approach, a Taylor expansion of the log acceptance ratio, gives a sum of n−1n-1n−1 terms of size 1/n1/n1/n. That sum does not concentrate uniformly over the state space, since the coordinates 2,…,n2,\dots,n2,…,n are arbitrary. The expansion is controlled only on the sets FnF_nFn​, where the empirical averages RnR_nRn​ and SnS_nSn​ are close to III. The limit therefore holds only after showing that the chain rarely leaves FnF_nFn​ over a time horizon of ntntnt steps. A pointwise law of large numbers is not enough for that, because the bound has to survive a union over ntntnt steps. Passing from generator convergence on a set of high probability to weak convergence of processes requires the Ethier–Kurtz convergence theory: a core for the limit generator, and convergence of processes that are not themselves Markov. None of this theory is in Mathlib.

Formalization scope

All declarations live in the namespace Roberts1997.RWM. The following conventions are fixed.

  • Vectors are Fin n → ℝ, and the paper's first coordinate x1x_1x1​ is index 0. Its coordinates 2,…,n2,\dots,n2,…,n are the indices i ≠ 0.
  • σn2=l2/(n−1)\sigma_n^2=l^2/(n-1)σn2​=l2/(n−1) is computed in R\mathbb RR. All statements concern n≥2n\ge2n≥2 or large nnn.
  • l>0l>0l>0 is assumed. The paper leaves it implicit, but h(−l)≠h(l)h(-l)\ne h(l)h(−l)=h(l).
  • "fff is a density" is read as ∫f=1\int f=1∫f=1. The moment conditions are read as integrability of (f′/f)8f(f'/f)^8f(f′/f)8f and (f′′/f)4f(f''/f)^4f(f′′/f)4f. The standing assumption "f′/ff'/ff′/f is Lipschitz" (p. 111) is carried by every statement.
  • The chain is built as a random mapping on an explicit probability space: x0∼πnx_0\sim\pi_nx0​∼πn​, with i.i.d. standard normal innovations and uniform acceptance variables. Theorem 1.1's initial condition (components i.i.d. fff, shared across dimensions) is read as "the nnn-th chain starts from πn\pi_nπn​", since weak convergence depends only on the law of each UnU^nUn.
  • "UUU satisfies the Langevin SDE" is read as "the law of UUU solves the martingale problem for GGG on Cc∞C_c^\inftyCc∞​, with continuous paths and initial law f(x) dxf(x)\,dxf(x)dx". This is equivalent by Ethier–Kurtz (1986), Ch. 5, Prop. 3.1 and Thm 3.3, and follows the platform definition EthierKurtz_IsContinuousDiffusionLaw.
  • "Un⇒UU^n\Rightarrow UUn⇒U" is read as the existence of an almost-sure coupling in which càdlàg copies of the UnU^nUn converge to a continuous Langevin path uniformly on compact time intervals. For a continuous limit this is equivalent to weak convergence in DR[0,∞)D_{\mathbb R}[0,\infty)DR​[0,∞), by Skorokhod's representation theorem and Ethier–Kurtz Ch. 3, Thm 1.8, Prop. 5.3 and Prop. 7.1. It follows the platform encoding of Ethier–Kurtz Theorem 7.4.1.
  • "sup⁡→0\sup\to0sup→0" and "lim sup⁡sup⁡<∞\limsup\sup<\inftylimsupsup<∞" are stated as eventual uniform bounds. This avoids real suprema, whose value on an unbounded set is a default.
  • In Lemma 2.6, "as d→∞d\to\inftyd→∞" is a misprint for n→∞n\to\inftyn→∞, and "2f(Ut)2f(Ut)2f(Ut)" in (1.2) is read as 2f(Ut)2f(U_t)2f(Ut​).
  • Corollary 1.2 (ii) is stated for an arbitrary constant I>0I>0I>0. "To two decimal places" is read as explicit rounding intervals: 1.31.31.3 is read to one decimal, and all maximisers over l>0l>0l>0 are covered.

The goal cannot be satisfied trivially. The limit law QQQ must exist, and it must be a probability measure whose initial marginal is f(x) dxf(x)\,dxf(x)dx, so the zero measure is excluded. The coupled copies must carry exactly the laws of the paths UnU^nUn, not an arbitrary process with the same one-time marginals.

The statements carry the paper's hypotheses, with one exception. The printed proof of Lemma 2.6 bounds sup⁡z∣(log⁡f)′′′(z)∣\sup_z|(\log f)'''(z)|supz​∣(logf)′′′(z)∣, which Theorem 1.1 does not assume, and under C2C^2C2 alone the uniform convergence over FnF_nFn​ claimed by Lemma 2.6 fails (narrow spikes of (log⁡f)′′(\log f)''(logf)′′ far out let a positive fraction of the coordinates shift the log acceptance ratio by a constant while RnR_nRn​ and SnS_nSn​ stay close to III). Lemma 2.6 is therefore stated with the proof's own assumption, f∈C3f\in C^3f∈C3 with (log⁡f)′′′(\log f)'''(logf)′′′ bounded, named as an addition. Theorem 1.1 and the other results keep the paper's hypotheses.

A complete development needs several pieces not yet available: path spaces and the Skorokhod topology (or the coupling reading), the martingale problem and its well-posedness for Lipschitz drift, and the Ethier–Kurtz theorem on convergence of generators on sets of high probability. Proofs of the Gaussian milestones (Propositions 2.2 and 2.4, Lemma 2.5) and of Corollary 1.2 (ii) are independent of this infrastructure and are welcome contributions.

Selected references

  • G. O. Roberts, A. Gelman, W. R. Gilks, Weak convergence and optimal scaling of random walk Metropolis algorithms, Ann. Appl. Probab. 7(1), 110–120, 1997. https://doi.org/10.1214/aoap/1034625254
  • S. N. Ethier, T. G. Kurtz, Markov Processes: Characterization and Convergence, Wiley, 1986. https://doi.org/10.1002/9780470316658
  • A. Gelman, G. O. Roberts, W. R. Gilks, Efficient Metropolis jumping rules, Bayesian Statistics 5, Oxford University Press, 599–607, 1996.
  • G. O. Roberts, J. S. Rosenthal, Optimal scaling for various Metropolis–Hastings algorithms, Statistical Science 16(4), 351–367, 2001. https://doi.org/10.1214/ss/1015346320
15 thms4 active usersReviewed
Functional AnalysisProbability·Captain: mikedeng1

Markov Processes: Characterization and Convergence 15: Diffusions in smooth bounded regionsTextbook

Why smooth-region boundary diffusions matter

Diffusion models in a bounded region need a rule for what happens when a path reaches the boundary. Two standard mechanisms are absorption, where the boundary kills the generator contribution, and oblique reflection, where a prescribed vector field pushes the process back into the region. Ethier and Kurtz treat these mechanisms as neighboring variants of the same uniformly elliptic model in Chapter 8, Section 1 of Markov Processes: Characterization and Convergence. The distinction is structural: the interior differential operator is shared, but its admissible generator graph changes with the boundary condition. This mission formalizes Theorems 1.4 and 1.5, retaining oblique reflection as the capstone and absorbed diffusion as the required related result.

The setting

Let Ω⊂Rd\Omega\subset\mathbb R^dΩ⊂Rd be bounded, open, and connected, with d≥2d\ge 2d≥2. Its boundary is locally represented in orthogonal coordinates as the graph of a scalar function. The formal predicate C²,μ boundary regularity requires one positive chart radius valid at every boundary point, a connected local boundary patch, and a graphing function whose second partial derivatives satisfy the source's componentwise Hölder oscillation condition. The exponent obeys 0<μ≤10<\mu\le 10<μ≤1.

The diffusion coefficients are a symmetric positive-semidefinite matrix field a(x)a(x)a(x) and a drift field b(x)b(x)b(x). Their entries satisfy the same local componentwise Hölder convention. Uniform ellipticity means that one ε>0\varepsilon>0ε>0 satisfies

ε≤∑i,jθiaij(x)θj\varepsilon\le \sum_{i,j}\theta_i a_{ij}(x)\theta_jε≤i,j∑​θi​aij​(x)θj​

for every x∈Ωx\in\Omegax∈Ω and every unit vector θ\thetaθ. For smooth fff, the interior operator is

Gf(x)=12∑i,jaij(x) ∂ijf(x)+Df(x)[b(x)].Gf(x)=\frac12\sum_{i,j}a_{ij}(x)\,\partial_{ij}f(x) +Df(x)[b(x)].Gf(x)=21​i,j∑​aij​(x)∂ij​f(x)+Df(x)[b(x)].

Functions live on the compact closure Ω‾\overline\OmegaΩ as bounded continuous functions. Their ambient extensions are differentiated only at interior points. The second coordinate of each graph is itself continuous on the closure, so it records the boundary trace of GfGfGf rather than assigning an arbitrary value after differentiation.

Formalization targets

Goal: obliquely reflected diffusion generation

Theorem 1.5 adds a reflection field ccc whose components have C¹,μ boundary regularity. An outward unit normal n(x)n(x)n(x) is oriented by a local defining function that is negative precisely inside Ω\OmegaΩ. Uniform obliqueness is the global lower bound

ε≤c(x)⋅n(x),x∈∂Ω,\varepsilon\le c(x)\cdot n(x),\qquad x\in\partial\Omega,ε≤c(x)⋅n(x),x∈∂Ω,

for one positive ε\varepsilonε. The reflected graph requires a continuous derivative trace JJJ that agrees with DfDfDf in the interior and satisfies

Jx(c(x))=0,x∈∂Ω.J_x(c(x))=0,\qquad x\in\partial\Omega.Jx​(c(x))=0,x∈∂Ω.

The target asserts that the uniform closure of this graph is single-valued and is exactly the full generator of a positive strongly continuous contraction semigroup preserving the constant function one. The generator condition is a biconditional derivative limit, so it identifies the complete domain rather than only a convenient operator restriction.

Related target: absorbed diffusion generation

Theorem 1.4 keeps the same smooth-region and ellipticity assumptions but uses the absorbed graph. Its continuous operator trace satisfies Gf=0Gf=0Gf=0 on the boundary. It has the same full generation conclusion: graph single-valuedness, a positive strongly continuous contraction semigroup, preservation of one, and exact identification of the generator. The absorbed zero trace is not imported into the reflected theorem, and the oblique derivative condition is not imposed on the absorbed graph.

Significance

These results connect a local elliptic expression and a geometric boundary condition to a global Markov evolution on continuous functions over the closed region. The conclusions contain more than existence of a semigroup: they determine the whole infinitesimal generator, ensure positivity and contraction, and retain the conservative convention used by Ethier and Kurtz. The paired statements make the effect of the boundary mechanism explicit while holding the interior model fixed.

The formal contribution is a machine-checkable statement layer, not a proof of the source theorems. It records the componentwise Hölder convention, uniform boundary charts, ellipticity, normal orientation, continuous derivative trace, the two distinct generator graphs, and every semigroup clause. These definitions can support later work on reflected processes, elliptic boundary problems, and martingale formulations without rebuilding the geometric conventions.

Where the difficulty lies

The main difficulty is simultaneous control of interior regularity, boundary geometry, and the closed generator domain. Pointwise obliqueness is insufficient: the source requires a uniform positive lower bound over the whole compact boundary. Likewise, merely writing Df(c)=0Df(c)=0Df(c)=0 for an arbitrary ambient extension would not supply a well-defined boundary derivative. The graph therefore carries a continuous derivative trace agreeing with the interior derivative. Replacing the biconditional generator equality by a one-way inclusion, or silently imposing the absorbed zero trace on the reflected graph, would weaken or change the source result.

Formalization scope and conventions

The state space is EuclideanSpace ℝ (Fin (n + 1)) with 2 ≤ n + 1. Connectedness supplies nonemptiness. Matrix positive semidefiniteness supplies symmetry and nonnegative quadratic forms; a separate hypothesis gives strict uniform ellipticity. Local oscillation bounds apply within connected components of small intersections and do not compare different components.

The absorbed and reflected graphs use bounded continuous functions on closure Ω. The arbitrary zero extension outside the closure is never differentiated at a boundary point. The reflected boundary equation uses a continuous field of linear derivative maps, while the absorbed equation uses the continuous second graph coordinate. No vacuous region, pointwise-only ellipticity or obliqueness, weakened generator inclusion, proof-only theorem dependency, or synthetic theorem combining the two boundary mechanisms is admitted.

Selected references

  • Stewart N. Ethier and Thomas G. Kurtz, Markov Processes: Characterization and Convergence, Wiley, 1986, Chapter 8, Section 1, Theorems 1.4–1.5 and equations (1.13)–(1.20). Wiley DOI
  • Stewart N. Ethier and Thomas G. Kurtz, same volume, Chapter 1 for strongly continuous contraction semigroups and generators, and Chapter 4 for the conservative Feller convention. Wiley DOI
42 thms4 active usersReviewed
Machine LearningProbabilityStatistics+1·Captain: mikedeng1

Foundations of Machine Learning VIII: Multi-Class Classification and the Margin BoundTextbook

Motivation

Every generalization bound in chapters 2-5 is for binary classification. Most real-world classification problems have more than two classes, and the number of classes can itself be in the hundreds or thousands (topic classification, speech recognition). Chapter 9 extends the margin-based generalization theory of chapter 5 (SVMs) to this multi-class, mono-label setting, using the same Rademacher-complexity machinery as chunk 03-rademacher-vc, but with a new combinatorial ingredient — bounding the Rademacher complexity of a family built by taking a pointwise maximum over several hypothesis sets — needed because a multi-class prediction is itself an argmax over per-class scores.

Setting

A multi-class hypothesis is a scoring function h:X×Y→Rh:X\times Y\to\mathbb Rh:X×Y→R with Y={1,…,k}Y=\{1,\dots,k\}Y={1,…,k} (mono-label case); the predicted label is arg⁡max⁡yh(x,y)\arg\max_y h(x,y)argmaxy​h(x,y), and the margin ρh(x,y)=h(x,y)−max⁡y′≠yh(x,y′)\rho_h(x,y)=h(x,y)-\max_{y'\ne y}h(x,y')ρh​(x,y)=h(x,y)−maxy′=y​h(x,y′) (p. 215) is negative exactly when hhh misclassifies (x,y)(x,y)(x,y). The empirical margin loss R^S,ρ(h)\hat R_{S,\rho}(h)R^S,ρ​(h) (Eq. 9.5) uses the same margin-loss function Φρ\Phi_\rhoΦρ​ (Definition 5.5) as chunk 05-svm, restated locally here. Π1(H)={x↦h(x,y):y∈Y,h∈H}\Pi_1(H) = \{x\mapsto h(x,y):y\in Y,h\in H\}Π1​(H)={x↦h(x,y):y∈Y,h∈H} (p. 217) projects a multi-class hypothesis set onto ordinary real-valued functions on XXX — the object the chapter's Rademacher-complexity bound actually controls, since H⊆RX×YH\subseteq\mathbb R^{X\times Y}H⊆RX×Y has no norm of its own without such a projection. Lemma 9.1 is a purely combinatorial tool: the empirical Rademacher complexity of a family built by taking the pointwise max over lll hypothesis sets is bounded by the sum of their individual empirical Rademacher complexities — used to control the argmax structure of a multi-class prediction. Theorem 9.2 combines this with chunk 03's Rademacher-complexity generalization machinery (Theorem 3.3) to give the chapter's margin bound. Proposition 9.3 and Corollary 9.4 specialize this to kernel-based hypotheses, where each class has its own weight vector in a reproducing kernel Hilbert space and the kkk weight vectors are jointly constrained by an LpL^pLp-type group norm ∥W∥H,p≤Λ\|W\|_{H,p}\le\Lambda∥W∥H,p​≤Λ.

Formalization targets

Lemma 9.1 (milestone). For F1,…,FlF_1,\dots,F_lF1​,…,Fl​ hypothesis sets in RX\mathbb R^XRX, l≥1l\ge1l≥1, and G={max⁡{h1,…,hl}:hi∈Fi}G=\{\max\{h_1,\dots,h_l\}:h_i\in F_i\}G={max{h1​,…,hl​}:hi​∈Fi​}: R^S(G)≤∑j=1lR^S(Fj)\hat R_S(G)\le\sum_{j=1}^l\hat R_S(F_j)R^S​(G)≤∑j=1l​R^S​(Fj​).

Theorem 9.2 — the mission's goal. For H⊆RX×YH\subseteq\mathbb R^{X\times Y}H⊆RX×Y, Y={1,…,k}Y=\{1,\dots,k\}Y={1,…,k}, fix ρ>0\rho>0ρ>0. For any δ>0\delta>0δ>0, with probability at least 1−δ1-\delta1−δ, for all h∈Hh\in Hh∈H:

R(h)≤R^S,ρ(h)+4kρRm(Π1(H))+log⁡(1/δ)2m.R(h) \le \hat R_{S,\rho}(h) + \tfrac{4k}\rho R_m(\Pi_1(H)) + \sqrt{\tfrac{\log(1/\delta)} {2m}}.R(h)≤R^S,ρ​(h)+ρ4k​Rm​(Π1​(H))+2mlog(1/δ)​​.

Proposition 9.3 (milestone). For a PDS kernel KKK with feature map Φ\PhiΦ and K(x,x)≤r2K(x,x)\le r^2K(x,x)≤r2: Rm(Π1(HK,p))≤r2Λ2/mR_m(\Pi_1(H_{K,p})) \le \sqrt{r^2\Lambda^2/m}Rm​(Π1​(HK,p​))≤r2Λ2/m​.

Corollary 9.4 (milestone). Under Proposition 9.3's hypotheses, fix ρ>0\rho>0ρ>0. For any δ>0\delta>0δ>0, with probability at least 1−δ1-\delta1−δ, for all h∈HK,ph\in H_{K,p}h∈HK,p​: R(h)≤R^S,ρ(h)+4kr2Λ2/ρ2/m+log⁡(1/δ)/(2m)R(h) \le \hat R_{S,\rho}(h) + 4k\sqrt{r^2\Lambda^2/\rho^2/m} + \sqrt{\log(1/\delta)/(2m)}R(h)≤R^S,ρ​(h)+4kr2Λ2/ρ2/m​+log(1/δ)/(2m)​.

Significance

Theorem 9.2 is the multi-class generalization of chunk 05-svm's Theorem 5.8, and its proof is the chapter's genuine new technique rather than a restatement: it needs a kkk-way application of Lemma 9.1 (once for the argmax structure of the margin, once summing over the kkk possible labels), which is exactly where the 4k4k4k factor comes from. Corollary 9.4 is the direct theoretical basis for the multi-class SVM algorithm the chapter derives next (§9.3.1): the displayed dual optimization problem literally minimizes the right-hand side of the corollary's bound. No prior art exists on the platform: GET /theorems?q=multi-class%20classification returns zero hits, and chunk 03's Rademacher-complexity machinery (needed by the proof route) is a draft, not reusable, per the "drafts cannot import drafts" rule.

Difficulty

Lemma 9.1's proof is a genuine two-function argument (max as 12(h1+h2+∣h1−h2∣)\tfrac12(h_1+h_2+|h_1-h_2|)21​(h1​+h2​+∣h1​−h2​∣), Talagrand's lemma applied to ∣⋅∣|\cdot|∣⋅∣) generalized to lll functions by induction, not a one-line consequence of chunk 03's single-hypothesis-set bound. Theorem 9.2's own proof (PDF pp. 234-236) is the chapter's most involved: it introduces an auxiliary margin function ρθ,h\rho_{\theta,h}ρθ,h​ with a free parameter θ\thetaθ later fixed to 2ρ2\rho2ρ, splits the resulting Rademacher complexity into a "diagonal" term (bounded via a further one-hot decomposition across the kkk classes, giving the first factor of kkk) and a "off-diagonal" term bounded via Lemma 9.1 (giving the second factor, folded into the same 4k4k4k constant). A formalization that stated Theorem 9.2 for HHH itself rather than Π1(H)\Pi_1(H)Π1​(H), or that treated kkk as an unrelated free constant rather than the actual number of classes, would misstate the theorem — precisely the pitfall BRIEF.md names for this chapter. Proposition 9.3's proof is a clean Cauchy-Schwarz/Jensen argument in the RKHS but needs the LpL^pLp-group-norm hypothesis class HK,pH_{K,p}HK,p​ stated with its exact footnote definition (PDF p. 236), not a simplified p=2p=2p=2 special case.

Formalization scope

GeneralizationError, EmpiricalRademacherComplexity and RademacherComplexity are restated locally in this chunk's MultiClass namespace (the last two identical in content to chunk 03-rademacher-vc's own copies); MarginLossFunction restates chunk 05-svm's Definition 5.5 (the same function, needed here for this chapter's own EmpiricalMarginLoss); IsPDS restates chunk 06-kernels's PDS-kernel definition. All are duplicated rather than imported since a draft item cannot import another chunk's draft module, and none of 03, 05, 06 is listed as reusable in missions/README.md's "Published definitions" table at the time of this session. GeneralizationError is formalized via the book's own established equivalence "hhh misclassifies (x,y)(x,y)(x,y) iff ρh(x,y)≤0\rho_h(x,y)\le0ρh​(x,y)≤0" (the form Theorem 9.2's own proof displays and works with), rather than via an explicit argmax classifier construction — checked as faithful, not a weakening, since it is exactly the quantity the chapter's proof bounds. MarginFunction's ⨆_{y'≠y} is a real supremum rather than a Finset.sup', avoiding a nonempty-finset side proof at definition time; every consuming theorem supplies 2 ≤ k (Y = Fin k) to guard it against trap 5. MaxFamily's index type is Fintype+Nonempty rather than a Finset-cardinality parameter l, a harmless generalization matching "l ≥ 1 hypothesis sets" via Nonempty. IsPDS's feature map Φ and its defining property K(x,y) = ⟪Φ(x),Φ(y)⟫ are supplied as hypotheses to the two kernel theorems rather than as a separate "feature mapping associated to a kernel" definition — the book itself treats this as a given correspondence, not a construction. No numerical constant is altered: 4k/ρ and log(1/δ) in Theorem 9.2, r²Λ²/m in Proposition 9.3, and 4k and r²Λ²/ρ²/m in Corollary 9.4 are exactly as displayed.

Not formalized: §9.1's discussion of the multi-label case (Eq. 9.2/9.3, the Hamming-distance risk) and Eq. 9.4 (empirical Hamming error) — background for a case this chapter's own generalization-bound section (§9.2) does not cover (the mono-label case only); the multi-class SVM primal/dual optimization problems (§9.3.1, an algorithm derived from Corollary 9.4, not a generalization-theoretic theorem); AdaBoost.MH (§9.3.2, a boosting algorithm, analyzed via a convex-surrogate argument rather than the Rademacher-complexity route this mission formalizes); and the uniform-over-ρ\rhoρ extension mentioned at the end of the Theorem 9.2 proof (an unnumbered remark referencing Theorem 5.9's technique from a different chapter, not restated here). Drafting only the algorithmic consequences (the multi-class SVM's optimization problem) in place of the generalization bounds themselves would be this chapter's trivializing formalization.

Selected references

  • M. Mohri, A. Rostamizadeh, A. Talwalkar, Foundations of Machine Learning, 2nd ed., MIT Press, 2018, Chapter 9.
  • V. Koltchinskii, D. Panchenko, "Empirical margin distributions and bounding the generalization error of combined classifiers," Annals of Statistics 30(1), 2002 (Lemma 9.1's technique).
  • K. Crammer, Y. Singer, "On the algorithmic implementation of multiclass kernel-based vector machines," JMLR 2, 2001 (the multi-class SVM algorithm §9.3.1 derives).
18 thms4 active users
Machine LearningProbabilityRandom Matrix Theory+1·Captain: mikedeng1

High-Dimensional Probability IX: The Matrix Deviation InequalityTextbook

Motivation

Random matrices with independent rows are the workhorse of high-dimensional statistics and compressed sensing: sample covariance matrices, sub-sampled measurement operators, and randomized sketches are all of this form. A basic question about such a matrix AAA is how close ∥Ax∥2\|Ax\|_2∥Ax∥2​ stays to its typical size E∥Ax∥2≈m∥x∥2\mathbb E\|Ax\|_2\approx\sqrt m\|x\|_2E∥Ax∥2​≈m​∥x∥2​ — not just for one fixed xxx, but simultaneously for every xxx in some set TTT of interest (a sphere, a cone, the difference set of a data cloud). A bound that holds only pointwise in xxx is of limited use, since most applications need to reason about the worst case over an entire geometric set at once.

This chapter proves such a uniform bound — the matrix deviation inequality — for matrices with independent, isotropic, sub-gaussian rows, controlling the deviation by a single geometric parameter of TTT, its Gaussian complexity. The result is a direct descendant of the chaining machinery of Chapter 8 (via Talagrand's comparison inequality, Chapter 8.6) and, in this book's own account, subsumes several results proved earlier by other methods — two-sided bounds on random matrices, the Johnson-Lindenstrauss lemma for infinite sets — while also yielding two new consequences central to high-dimensional convex geometry: the M∗M^*M∗ bound and the Escape theorem, both controlling how a random subspace intersects a fixed geometric set.

Setting

Fix a probability space (Ω,F,P)(\Omega,\mathcal F,P)(Ω,F,P). A random vector XXX in Rn\mathbb R^nRn is isotropic if its covariance matrix is the identity, Σ(X)=E[XX⊤]=In\Sigma(X)=\mathbb E[XX^\top]=I_nΣ(X)=E[XX⊤]=In​ — equivalently (the book's own Lemma 3.2.3), E⟨X,x⟩2=∥x∥22\mathbb E\langle X,x\rangle^2=\|x\|_2^2E⟨X,x⟩2=∥x∥22​ for every x∈Rnx\in\mathbb R^nx∈Rn. The sub-gaussian norm of a random vector XXX is ∥X∥ψ2:=sup⁡x∈Sn−1∥⟨X,x⟩∥ψ2\|X\|_{\psi_2}:=\sup_{x\in S^{n-1}}\|\langle X,x\rangle\|_{\psi_2}∥X∥ψ2​​:=supx∈Sn−1​∥⟨X,x⟩∥ψ2​​, the supremum over the unit sphere of the scalar sub-gaussian (Orlicz ψ2\psi_2ψ2​) norm of its one-dimensional marginals; XXX is sub-gaussian when this is finite.

Fix a standard Gaussian random vector g∼N(0,In)g\sim N(0,I_n)g∼N(0,In​) in Rn\mathbb R^nRn (a vector whose coordinates in any orthonormal basis are independent standard normal). For a subset T⊆RnT\subseteq\mathbb R^nT⊆Rn, the Gaussian width and Gaussian complexity of TTT are

w(T):=Esup⁡x∈T⟨g,x⟩,γ(T):=Esup⁡x∈T∣⟨g,x⟩∣,w(T) := \mathbb E\sup_{x\in T}\langle g,x\rangle, \qquad \gamma(T) := \mathbb E\sup_{x\in T}|\langle g,x\rangle|,w(T):=Ex∈Tsup​⟨g,x⟩,γ(T):=Ex∈Tsup​∣⟨g,x⟩∣,

two closely related measures of the geometric size of TTT — "cousins" that agree up to a factor of 222 whenever TTT contains the origin, and agree exactly when TTT is origin-symmetric.

Formalization targets

Goal (Theorem 9.1.1, Matrix deviation inequality)

∃ C>0:Esup⁡x∈T∣ ∥Ax∥2−m∥x∥2 ∣  ≤  CK2γ(T)\exists\,C>0:\quad \mathbb E\sup_{x\in T}\bigl|\,\|Ax\|_2-\sqrt m\|x\|_2\,\bigr| \;\le\; CK^2\gamma(T)∃C>0:Ex∈Tsup​​∥Ax∥2​−m​∥x∥2​​≤CK2γ(T)

for every m×nm\times nm×n matrix AAA whose rows A1,…,AmA_1,\dots,A_mA1​,…,Am​ are independent, isotropic, sub-gaussian random vectors with K:=max⁡i∥Ai∥ψ2K:=\max_i\|A_i\|_{\psi_2}K:=maxi​∥Ai​∥ψ2​​, and every T⊆RnT\subseteq\mathbb R^nT⊆Rn (whenever γ(T)\gamma(T)γ(T) is finite). CCC is the book's own unnamed absolute constant, hard-coded to no numeral — the weakest stable form of the claim.

Milestone (Theorem 9.4.2, the M∗M^*M∗ bound)

E diam(T∩ker⁡A)  ≤  CK2w(T)m\mathbb E\,\mathrm{diam}(T\cap\ker A) \;\le\; \frac{CK^2w(T)}{\sqrt m}Ediam(T∩kerA)≤m​CK2w(T)​

for the same class of matrices AAA and any bounded T⊆RnT\subseteq\mathbb R^nT⊆Rn, where ker⁡A\ker AkerA is the (random) kernel of AAA, a subspace of codimension at most mmm. A direct one-paragraph consequence of the goal theorem (apply it to T−TT-TT−T, then restrict to ker⁡A\ker AkerA, where ∥Ax−Ay∥2\|Ax-Ay\|_2∥Ax−Ay∥2​ vanishes).

Significance

The matrix deviation inequality converts a purely algebraic quantity — how close ∥Ax∥2\|Ax\|_2∥Ax∥2​ stays to m∥x∥2\sqrt m\|x\|_2m​∥x∥2​ — into a single geometric parameter of the index set TTT, letting it subsume, via specializations of TTT, results that were previously proved by separate ad hoc arguments: two-sided singular value bounds on random matrices (TTT a sphere), Johnson-Lindenstrauss-type embeddings for possibly infinite point sets (TTT a difference set), and covariance estimation. The M∗M^*M∗ bound is one of the two classical consequences the book develops fresh from the inequality (the other, the Escape theorem, is outside this mission's scope): it answers, quantitatively, how large a random affine section of a fixed convex body typically is, a question at the heart of the local theory of Banach spaces and of compressed sensing's recovery guarantees (Chapter 10 builds directly on this chapter's machinery). Both results have long-standing, well-understood classical proofs; this mission formalizes their statements, not open research.

Difficulty

The natural first idea — bound ∥Ax∥2−m∥x∥2\|Ax\|_2-\sqrt m\|x\|_2∥Ax∥2​−m​∥x∥2​ pointwise for a fixed xxx using concentration of the norm of a sub-gaussian random vector, then take a union bound over TTT — only works when TTT is finite, and gives a bound that scales with log⁡∣T∣\log|T|log∣T∣ rather than with the actual geometric size of TTT. The book's actual route treats Xx:=∥Ax∥2−m∥x∥2X_x:=\|Ax\|_2-\sqrt m\|x\|_2Xx​:=∥Ax∥2​−m​∥x∥2​, indexed by x∈Rnx\in\mathbb R^nx∈Rn, as a genuine random process and shows it has sub-gaussian increments (∥Xx−Xy∥ψ2≤CK2∥x−y∥2\|X_x-X_y\|_{\psi_2}\le CK^2\|x-y\|_2∥Xx​−Xy​∥ψ2​​≤CK2∥x−y∥2​) — itself a nontrivial fact proved in stages (first for a single unit vector via concentration of the norm, Theorem 3.1.1; then for a pair of unit vectors via a squared-process argument; only then in full generality) — and then invokes Talagrand's comparison inequality (a consequence of the chaining machinery of Chapter 8) to pass from sub-gaussian increments directly to a bound in terms of Gaussian complexity, without ever performing a union bound over TTT itself.

Formalization scope

A is represented by its rows, A : Fin m → Ω → EuclideanSpace ℝ (Fin n), with ‖Ax‖₂ recovered as Real.sqrt (∑ i, ⟨Aᵢ,x⟩²) rather than constructing A as a Matrix/LinearMap — this matches the book's own row-by-row hypotheses exactly and is what both theorems' own proofs use directly. IsIsotropic is formalized via the book's basis-free Lemma 3.2.3 characterization (E⟨X,x⟩² = ‖x‖² for every x) rather than the matrix equation Σ(X)=Iₙ, avoiding a fixed-basis covariance-matrix construction the rest of this chunk's definitions do not otherwise need. SubgaussianVectorNorm reuses the published scalar subgaussianNorm. GaussianWidth and GaussianComplexity realize the standard Gaussian vector g ∼ N(0,Iₙ) as the identity map on Mathlib's own standard Gaussian measure on a finite-dimensional inner product space (ProbabilityTheory.stdGaussian), and both, together with the goal's own left-hand side, use a locally-defined finite-marginal expected-supremum convention (ExpSup, EReal-valued) matching the book's own footnote-3 convention (Section 7.2), reused throughout the series. Both theorems' right-hand sides presuppose their respective geometric parameter (γ(T)\gamma(T)γ(T) or w(T)w(T)w(T)) is a finite real number; since both are EReal-valued in general, each theorem takes an explicit real witness together with a proof that it equals the true value — the same finiteness-disclosure pattern 07-chaining's Dudley inequality uses for its own right-hand integral, needed here for exactly the same reason (the book's own display does not spell out why the quantity is finite, true whenever TTT is bounded, as in every application). CCC (and, in the milestone, the same CCC again — the two are not asserted equal, matching that the book states them as two separate "absolute constants") is existentially quantified before every type, instance and hypothesis it is uniform over. The M∗M^*M∗ bound milestone (m_star_bound) additionally carries the hypothesis m>0m > 0m>0: its conclusion divides by m\sqrt mm​, and without this hypothesis Lean's real-division convention (x/0=0x/0=0x/0=0) makes the right-hand side 000 at m=0m=0m=0 regardless of C,K,w(T)C, K, w(T)C,K,w(T) — false whenever TTT has positive diameter, not merely a weaker or vacuous claim. The book's own proof ("Dividing by m\sqrt mm​ yields …", p. 241) already implicitly assumes m≥1m \ge 1m≥1, matching every other use of mmm in the chapter as a positive count of measurement rows.

A trivializing formalization would fix TTT to be a finite set, collapsing the goal to the elementary union-bound case the book explicitly contrasts its own more general statement against (Section 9.1's opening paragraph: "we may choose an arbitrary subset T⊆RnT\subseteq\mathbb R^nT⊆Rn"); this mission's goal quantifies over an arbitrary Set (EuclideanSpace ℝ (Fin n)) to rule that out.

This mission covers Theorem 9.1.1 and Theorem 9.4.2 only; Theorem 9.4.7 (the Escape theorem) and Theorem 9.2.4 (covariance estimation for lower-dimensional distributions), both named as candidate milestones, are left out for lack of session time given the substantial shared infrastructure this chapter needed from scratch. ExpSup, IsIsotropic, SubgaussianVectorNorm, GaussianWidth and GaussianComplexity are reusable by any later chapter needing an isotropic or sub-gaussian random vector, or a Gaussian-width-type quantity (Chapters 4, 10, 11 of this same book series all use one or more of these notions). Solvers' contributions are welcome on: Theorem 9.1.3 (the sub-gaussian increments of the deviation process, the technical heart of the goal's proof), Talagrand's comparison inequality itself (outside this mission, in 07-chaining's companion chapter), and the one-paragraph reduction from the goal to the M∗M^*M∗ bound.

Selected references

  • S. Mendelson, A. Pajor, N. Tomczak-Jaegermann, Reconstruction and subgaussian operators in asymptotic geometric analysis, Geometric and Functional Analysis 17 (2007), 1248–1282. https://doi.org/10.1007/s00039-007-0618-7
  • V. D. Milman, A new proof of A. Dvoretzky's theorem on cross-sections of convex bodies, Funkcional. Anal. i Priložen. 5 (1971), 28–37.
  • R. Vershynin, High-Dimensional Probability: An Introduction with Applications in Data Science, Cambridge University Press, 2018, Chapter 9. https://doi.org/10.1017/9781108231596
10 thms4 active users
Machine LearningProbabilityStatistics+1·Captain: mikedeng1

Foundations of Machine Learning III: Structural Risk Minimization and Model SelectionTextbook

Motivation

Chapters 2 and 3 bound the estimation error of a hypothesis chosen from a fixed hypothesis set HHH, but the choice of HHH itself is left open: a richer HHH lowers the approximation error (how close HHH comes to the Bayes classifier) at the price of a looser generalization bound, and a poorer HHH does the reverse. Chapter 4 is the book's answer to this trade-off. It first shows that Empirical Risk Minimization (ERM) alone cannot resolve it — ERM ignores the complexity of HHH entirely — and then develops Structural Risk Minimization (SRM): decompose a rich hypothesis set into a nested countable union H=⋃k≥1HkH=\bigcup_{k\ge1}H_kH=⋃k≥1​Hk​ of increasingly complex pieces, and let the learning algorithm balance empirical fit against a complexity penalty for each HkH_kHk​ automatically. The chapter closes by showing how the same balance can be achieved computationally through convex surrogate losses, whose minimization is tractable where minimizing the zero-one loss directly is not.

Setting

For a hypothesis hhh chosen from HHH, the excess error R(h)−R∗R(h)-R^*R(h)−R∗ decomposes into an estimation term R(h)−inf⁡h∈HR(h)R(h)-\inf_{h\in H}R(h)R(h)−infh∈H​R(h) and an approximation term inf⁡h∈HR(h)−R∗\inf_{h\in H}R(h)-R^*infh∈H​R(h)−R∗ (Eq. 4.1). Proposition 4.1 bounds ERM's estimation error by twice the uniform deviation sup⁡h∈H∣R(h)−R^S(h)∣\sup_{h\in H}|R(h)-\hat R_S(h)|suph∈H​∣R(h)−R^S​(h)∣. For a nested family (Hk)k≥1(H_k)_{k\ge1}(Hk​)k≥1​ and h∈Hh\in Hh∈H, k(h)k(h)k(h) denotes the least index with h∈Hk(h)h\in H_{k(h)}h∈Hk(h)​; SRM selects hSSRMh_S^{SRM}hSSRM​ by minimizing Fk(h)=R^S(h)+Rm(Hk)+log⁡k/mF_k(h)=\hat R_S(h)+R_m(H_k)+\sqrt{\log k/m}Fk​(h)=R^S​(h)+Rm​(Hk​)+logk/m​ jointly over k≥1k\ge1k≥1 and h∈Hkh\in H_kh∈Hk​, where Rm(Hk)R_m(H_k)Rm​(Hk​) is HkH_kHk​'s Rademacher complexity (Definitions 3.1/3.2, restated locally in this chunk's ModelSelection namespace). Theorem 4.2 is the resulting learning guarantee. Section 4.4 develops a competing model-selection procedure, cross-validation, and Theorem 4.4 directly compares its guarantee to SRM's on a held-out split of the sample. Section 4.7 turns to real-valued scoring functions h:X→Rh:X\to\mathbb Rh:X→R with sign convention fh(x)=sign(h(x))f_h(x)=\mathrm{sign}(h(x))fh​(x)=sign(h(x)) and a convex non-decreasing surrogate Φ\PhiΦ of the zero-one loss; the Bayes scoring function h∗(x)=η(x)−12h^*(x)=\eta(x)-\tfrac12h∗(x)=η(x)−21​ (Eq. 4.9) and the Φ\PhiΦ-loss LΦL_\PhiLΦ​ (Eq. 4.10) let Theorem 4.7 bound the true excess error by a power of the surrogate's own excess loss.

Formalization targets

Proposition 4.1 (ERM bound, milestone). For any sample SSS, Pr⁡[R(hSERM)−inf⁡h∈HR(h)>ϵ]≤Pr⁡[sup⁡h∈H∣R(h)−R^S(h)∣>ϵ/2]\Pr[R(h_S^{ERM}) - \inf_{h\in H}R(h) > \epsilon] \le \Pr[\sup_{h\in H}|R(h)-\hat R_S(h)| > \epsilon/2]Pr[R(hSERM​)−infh∈H​R(h)>ϵ]≤Pr[suph∈H​∣R(h)−R^S​(h)∣>ϵ/2].

Theorem 4.2 — the mission's goal. For a nested countable union H=⋃k≥1HkH=\bigcup_{k\ge1}H_kH=⋃k≥1​Hk​ and hSSRMh_S^{SRM}hSSRM​ minimizing Fk(h)F_k(h)Fk​(h) over the whole union, for any δ>0\delta>0δ>0, with probability at least 1−δ1-\delta1−δ:

R(hSSRM)≤inf⁡h∈H[R(h)+2Rm(Hk(h))+log⁡k(h)m]+2log⁡(3/δ)m.R(h_S^{SRM}) \le \inf_{h\in H}\Big[R(h)+2R_m(H_{k(h)})+\sqrt{\tfrac{\log k(h)}m}\Big] + \sqrt{\tfrac{2\log(3/\delta)}m}.R(hSSRM​)≤h∈Hinf​[R(h)+2Rm​(Hk(h)​)+mlogk(h)​​]+m2log(3/δ)​​.

Theorem 4.4 (Cross-validation versus SRM, milestone). Splitting a sample of size mmm into S1S_1S1​ (size (1−α)m(1-\alpha)m(1−α)m, training) and S2S_2S2​ (size αm\alpha mαm, validation), for any δ>0\delta>0δ>0, with probability at least 1−δ1-\delta1−δ:

R(hSCV)−R(hS1SRM)≤2log⁡max⁡(k(hSCV),k(hS1SRM))αm+2log⁡(4/δ)2αm.R(h_S^{CV}) - R(h_{S_1}^{SRM}) \le 2\sqrt{\tfrac{\log\max(k(h_S^{CV}),k(h_{S_1}^{SRM}))}{\alpha m}} + 2\sqrt{\tfrac{\log(4/\delta)}{2\alpha m}}.R(hSCV​)−R(hS1​SRM​)≤2αmlogmax(k(hSCV​),k(hS1​SRM​))​​+22αmlog(4/δ)​​.

Theorem 4.7 (Convex-surrogate excess-error bound, milestone). For Φ\PhiΦ convex and non-decreasing with s≥1,c>0s\ge1,c>0s≥1,c>0 satisfying ∣h∗(x)∣s≤cs(LΦ(x,0)−LΦ(x,hΦ∗(x)))|h^*(x)|^s \le c^s(L_\Phi(x,0)-L_\Phi(x,h^*_\Phi(x)))∣h∗(x)∣s≤cs(LΦ​(x,0)−LΦ​(x,hΦ∗​(x))) for all xxx: R(h)−R∗≤2c(LΦ(h)−LΦ∗)1/sR(h)-R^* \le 2c(L_\Phi(h)-L^*_\Phi)^{1/s}R(h)−R∗≤2c(LΦ​(h)−LΦ∗​)1/s.

Significance

Theorem 4.2 is the chapter's headline result and the theoretical justification for regularization-based learning: it shows that a single algorithm, without knowing in advance which HkH_kHk​ contains a good hypothesis, achieves a guarantee that is — up to the log⁡k(h)/m\sqrt{\log k(h)/m}logk(h)/m​ penalty — as favorable as if an oracle had revealed the best-in-class index in advance (Eq. 4.6). It is also the chapter's genuine new content beyond chunk 03-rademacher-vc's single-hypothesis-set bound: the countable union bound (a 1/k²-weighted union over k≥1k\ge1k≥1 converging to π2/6\pi^2/6π2/6, hence the log⁡3\log 3log3 appearing in place of log⁡2\log 2log2) is not a restatement of Theorem 3.3 but a distinct argument, and the goal's inf over the whole nested family is what makes SRM a model-selection method rather than a bound for one fixed kkk. Theorem 4.4 is the chapter's only head-to-head comparison between two competing model-selection procedures, on two genuinely different samples. Theorem 4.7 is the bridge between the learning-theoretic guarantees of chapters 2-4 and the actually-implemented convex optimization problems of chapters 5 (SVM), 6 (kernels) and beyond, all of which minimize a convex surrogate rather than the zero-one loss directly. No prior art exists on the platform: GET /theorems?q=structural%20risk%20minimization and GET /theorems?q=model%20selection both return zero hits.

Difficulty

Theorem 4.2's proof genuinely uses the union bound over a countably infinite family indexed by k≥1k\ge1k≥1 with weight 1/k21/k^21/k2 converging to π2/6<2\pi^2/6 < 2π2/6<2 (Eq. 4.5) — this is the chapter's distinct new technique, not an application of chunk 03's finite/VC-dimension machinery to a single HkH_kHk​; a formalization that stated the bound only for one fixed kkk, or dropped the inf over the whole union in favor of a single best-in-class h∗h^*h∗, would be Theorem 4.2's named trivializing formalization (BRIEF.md's pitfall note) rather than the theorem itself. Theorem 4.4 requires keeping two distinct samples (S1S_1S1​, S2S_2S2​, of different, precisely related sizes) and two distinct hypotheses (hSCVh_S^{CV}hSCV​, hS1SRMh_{S_1}^{SRM}hS1​SRM​) apart throughout; conflating them collapses the comparison to a tautology. Theorem 4.7's difficulty is in its setup, not its statement: the Bayes scoring function, the Φ\PhiΦ-loss, and the pointwise Φ\PhiΦ-minimizer hΦ∗h^*_\PhihΦ∗​ (which the book allows to take the extended values ±∞\pm\infty±∞ at the degenerate points η(x)∈{0,1}\eta(x)\in\{0,1\}η(x)∈{0,1}) all need care to state without silently altering the theorem's content.

Formalization scope

GeneralizationError, EmpiricalError, EmpiricalRademacherComplexity and RademacherComplexity are restated locally in this chunk's ModelSelection namespace (identical in content to chunk 03-rademacher-vc's own copies), since a draft item cannot import another chunk's draft module. LeastIndex H h (k(h)) is Nat.sInf {k | 1 ≤ k ∧ h ∈ H k}; every theorem using it carries the standing hypothesis that h lies in the relevant union, guarding against trap 5 (Nat.sInf of an empty set). Theorem 4.2's hSRM and Proposition 4.1's hERM are hypothesis-supplied functions satisfying the book's optimality property, not constructed via choice over an unconstrained H; H.Nonempty (Proposition 4.1) and (⋃ k ≥ 1, Hk k).Nonempty (Theorem 4.2) guard the outer sInf/inf terms against trap 5. Theorem 4.7's hΦ∗h^*_\PhihΦ∗​ is formalized as a real-valued function satisfying the pointwise minimization property for all xxx; the book's own extended-real convention (hΦ∗(x)=±∞h^*_\Phi(x)=\pm\inftyhΦ∗​(x)=±∞ exactly where η(x)∈{0,1}\eta(x)\in\{0,1\}η(x)∈{0,1}) is outside this formalization — disclosed here and in MODERATION_NOTES.md — since no real number satisfies the minimizing property at those degenerate points, the theorem as stated applies precisely to the case a real-valued hΦ∗h^*_\PhihΦ∗​ can be supplied, which is the book's own generic case. No numerical constant is altered from the book in any of the four theorems: 2 and log(3/δ) in Theorem 4.2, 2 (twice) and log(4/δ) in Theorem 4.4, and 2c and the exponent 1/s in Theorem 4.7 are exactly as displayed.

Not formalized: the discussion of computing k∗k^*k∗ via binary search (a computational, not a statistical, result); nnn-fold and leave-one-out cross-validation (Section 4.5, a practical variant of Theorem 4.4's two-sample cross-validation without its own numbered generalization bound); regularization-based algorithms (Section 4.6, the uncountable-union extension of SRM, which the book itself only sketches without a numbered theorem); Lemma 4.5 and Proposition 4.6 (intermediate results establishing that hΦ∗h^*_\PhihΦ∗​ induces the same classifier as h∗h^*h∗, needed for Theorem 4.7's proof but not part of its statement); and the worked examples for the hinge, exponential and logistic losses (instantiations of Theorem 4.7's s,cs,cs,c, not separate theorems). Drafting only these worked instantiations in place of Theorem 4.7's general statement would be a trivializing formalization for this chapter.

Selected references

  • M. Mohri, A. Rostamizadeh, A. Talwalkar, Foundations of Machine Learning, 2nd ed., MIT Press, 2018, Chapter 4.
  • V. Vapnik, Statistical Learning Theory, Wiley-Interscience, 1998 (structural risk minimization).
  • T. Zhang, "Statistical behavior and consistency of classification methods based on convex risk minimization," Annals of Statistics 32(1), 2003 (Theorem 4.7's origin).
16 thms4 active users
AnalysisDynamical SystemsTopology·Captain: Lucas

Local Connectivity of the Mandelbrot Set (MLC)Open Problem

The set

For a complex parameter ccc, iterate the quadratic map

fc(z)=z2+cf_c(z) = z^2 + cfc​(z)=z2+c

starting at the critical point z=0z = 0z=0. The Mandelbrot set is the set of parameters for which this orbit stays bounded:

M={ c∈C : sup⁡k∈N∣fc k(0)∣<∞ }.M = \{\, c \in \mathbb{C} \ : \ \sup_{k \in \mathbb{N}} \left| f_c^{\,k}(0) \right| < \infty \,\}.M={c∈C : k∈Nsup​​fck​(0)​<∞}.

Equivalently -- and this is the first milestone of the mission -- c∈Mc \in Mc∈M if and only if ∣fc k(0)∣≤2|f_c^{\,k}(0)| \le 2∣fck​(0)∣≤2 for every kkk, which exhibits MMM as a compact subset of the plane.

MMM is the parameter-space picture of the simplest non-trivial family in complex dynamics, and it acts as a dictionary: the shape of MMM near a parameter ccc encodes the dynamics of fcf_cfc​ on its Julia set, so structural questions about MMM are questions about the whole quadratic family at once. Douady and Hubbard proved in 1982 that MMM is connected, by exhibiting a conformal isomorphism

Φ:C∖M⟶C∖D‾\Phi : \mathbb{C} \setminus M \longrightarrow \mathbb{C} \setminus \overline{\mathbb{D}}Φ:C∖M⟶C∖D

between the complement of MMM and the exterior of the closed unit disk.

The question

MLC conjecture. MMM is locally connected: every point of MMM has a neighbourhood basis, in the subspace topology, consisting of connected sets.

By Caratheodory's theorem, MLC is equivalent to the statement that Φ−1\Phi^{-1}Φ−1 extends continuously to the unit circle. That extension would deliver a complete combinatorial description of MMM -- the pinched disk model of Douady and Thurston -- in which every boundary point is labelled by the external rays landing on it. Two headline consequences follow: the density of hyperbolicity in the quadratic family (Fatou's conjecture: every quadratic polynomial can be perturbed to one with an attracting cycle), and zero area for ∂M\partial M∂M.

MLC has been open since the early 1980s and is regarded as the central problem of one-dimensional complex dynamics.

Timeline

  • 1982 -- Douady and Hubbard prove that MMM is connected, via the Boettcher uniformisation of its complement, and formulate MLC.
  • 1984/85 -- The Orsay notes develop the combinatorics of external rays and the pinched-disk model, and show that MLC implies the density of hyperbolicity in the quadratic family.
  • 1990 -- Yoccoz proves MLC at every finitely renormalizable parameter without an indifferent periodic point, introducing the Yoccoz puzzle and the rigidity techniques that dominate later work.
  • 1997 -- Lyubich extends local connectivity to infinitely renormalizable parameters of bounded type, using complex bounds for quadratic-like renormalization.
  • 1997 -- Graczyk-Swiatek and Lyubich prove density of hyperbolicity in the real quadratic family.
  • 1998 -- Shishikura proves that ∂M\partial M∂M has Hausdorff dimension 222, by parabolic implosion. Whether ∂M\partial M∂M has positive area remains open.
  • 2005 -- Buff and Cheritat construct quadratic Julia sets of positive area, showing that the analogous area question in the dynamical plane has a negative answer.
  • Today -- MLC is known at large classes of parameters, but the general case, and with it the density of hyperbolicity, remain open.

What this mission asks for

The goal theorem is MLC itself, in the form "the Mandelbrot set, as a topological subspace of C\mathbb{C}C, is a locally connected space".

The milestones are of three kinds, and are ordered accordingly:

  1. Foundations provable today -- the escape criterion (in the quadratic and the general unicritical degree) and compactness. These make the filter-theoretic definition usable and are the natural entry point for a solver new to the mission.
  2. Known theorems from the literature -- connectedness of MMM (Douady-Hubbard), the implication MLC ⇒\Rightarrow⇒ density of hyperbolicity (Douady-Hubbard), and dim⁡H(∂M)=2\dim_H(\partial M) = 2dimH​(∂M)=2 (Shishikura). These are hard but settled, and formalizing them builds the infrastructure -- Boettcher coordinates, external rays, parabolic implosion -- that any attack on the goal will need.
  3. The open companions -- density of hyperbolicity in the quadratic and unicritical families, zero area of ∂M\partial M∂M, and MLC for all Multibrot sets MnM_nMn​, the parameter sets of z↦zn+cz \mapsto z^n + cz↦zn+c.

All statements are phrased against a single shared definition file, so a solver can move between milestones without re-fixing conventions.

24 thms4 active usersReviewed
Algebra·Captain: mysticflounder

Equational Magmas: E677 → E255 (finite case)Open Problem

Motivation

An equation for a magma constrains a binary operation without assuming that it is associative, commutative, or has an identity. Which laws imply which others, over all magmas or over finite magmas only, is the question the Equational Theories Project studies at scale. Restricting the underlying set to be finite can change the answer: a structural argument may depend on the fact that a surjective self-map of a finite set is injective.

The project's December 2025 paper reports the finite implication from E677 to E255 as unresolved, while reporting a counterexample to the implication when infinite magmas are allowed. The paper also tentatively conjectures that a finite counterexample exists. This mission makes the affirmative implication its formal target and also accepts a rigorous refutation of the complete finite statement.

This mission treats the universal target as open. Supporting structural facts and conditional reductions are separately identified, so that progress on one does not assert completion of the target.

Setting

A magma here is a type α\alphaα with a total binary operation ⋄:α×α→α\diamond:\alpha\times\alpha\to\alpha⋄:α×α→α. Parentheses specify the order of evaluation throughout; no reassociation is permitted. The condition E677 means

∀x,y∈α,x=y⋄(x⋄((y⋄x)⋄y)).\forall x,y\in\alpha,\quad x=y\diamond\bigl(x\diamond((y\diamond x)\diamond y)\bigr).∀x,y∈α,x=y⋄(x⋄((y⋄x)⋄y)).

The condition E255 means

∀x∈α,x=((x⋄x)⋄x)⋄x.\forall x\in\alpha,\quad x=((x\diamond x)\diamond x)\diamond x.∀x∈α,x=((x⋄x)⋄x)⋄x.

These are the two laws used in Chapter 13 of the project blueprint. For a fixed element yyy, the left translation (left multiplication) map is Ly(x)=y⋄xL_y(x)=y\diamond xLy​(x)=y⋄x. A fixer of xxx is an element yyy with y⋄x=xy\diamond x=xy⋄x=x; it acts on xxx from the left. This definition concerns one element xxx; it does not require yyy to act as an identity on every element. The left orbit of xxx is the forward orbit x,Lx(x),Lx2(x),…x,L_x(x),L_x^2(x),\ldotsx,Lx​(x),Lx2​(x),… of xxx under its own left translation.

Formalization targets

The supporting targets expose the relevant distinction between a constraint on a possible fixer and the existence of a fixer. For every finite α\alphaα satisfying E677, the first supporting statement is

∀y∈α,Ly is bijective.\forall y\in\alpha,\quad L_y\text{ is bijective}.∀y∈α,Ly​ is bijective.

The second supporting statement determines any fixer:

∀x,y∈α,y⋄x=x ⟹ y=(x⋄x)⋄x.\forall x,y\in\alpha,\quad y\diamond x=x\ \Longrightarrow\ y=(x\diamond x)\diamond x.∀x,y∈α,y⋄x=x ⟹ y=(x⋄x)⋄x.

The third supporting statement is the backward recurrence

∀x,y∈α,x=(y⋄x)⋄((y⋄(y⋄x))⋄y).\forall x,y\in\alpha,\quad x=(y\diamond x)\diamond\bigl((y\diamond(y\diamond x))\diamond y\bigr).∀x,y∈α,x=(y⋄x)⋄((y⋄(y⋄x))⋄y).

These three statements are blueprint Lemma 13.1(i)–(iii) and are Proved on this platform. The following fixer-existence assertion is the same obligation as E255 under E677 and finiteness (blueprint Lemma 13.2); it is a reduction node, not a milestone:

∀x∈α,∃y∈α,y⋄x=x.\forall x\in\alpha,\quad\exists y\in\alpha,\quad y\diamond x=x.∀x∈α,∃y∈α,y⋄x=x.

The mission goal is

∀ finite magmas α,E677⁡(α) ⟹ E255⁡(α).\forall\text{ finite magmas }\alpha,\quad \operatorname{E677}(\alpha)\ \Longrightarrow\ \operatorname{E255}(\alpha).∀ finite magmas α,E677(α) ⟹ E255(α).

For finite E677 magmas, E255 at xxx supplies the fixer (x⋄x)⋄x(x\diamond x)\diamond x(x⋄x)⋄x; from any fixer yyy of xxx, Lemma 13.1(ii) gives y=(x⋄x)⋄xy=(x\diamond x)\diamond xy=(x⋄x)⋄x and hence E255 at xxx. Each direction is one line, so fixer existence is not a strictly weaker milestone.

Three open sub-goals come from the case split in the accepted reduction sketches for the fixer-existence node. Sub-goal 1 is orbit-local: for a fixed xxx, if two elements of the left orbit of xxx have equal right products by xxx, then they are equal or xxx has a fixer. Sub-goal 2 concerns the case of exactly one element AAA outside the left orbit of xxx, with xxx having no fixer: a right-translation collision c⋄x=A⋄xc\diamond x=A\diamond xc⋄x=A⋄x between an orbit point ccc and AAA must propagate to the orbit successor x⋄cx\diamond cx⋄c. Sub-goal 3 assumes x⋄x≠xx\diamond x\ne xx⋄x=x and at least two elements outside the left orbit: if right translation by xxx sends an orbit point outside the orbit, then xxx has a fixer. Sub-goal 3 is not a smaller case of the goal. If it holds for every finite E677 magma, the mission goal follows by a product construction (milestone "Sub-goal 3 support (a)"), and the mission goal gives Sub-goal 3 because E255 at xxx supplies the fixer (x⋄x)⋄x(x\diamond x)\diamond x(x⋄x)⋄x. So a proof of Sub-goal 3 alone proves the goal, and a route through Sub-goals 1 and 2 still needs Sub-goal 3. The D4 milestones specialize Sub-goal 1 to a left orbit of exact period four; D4.0, D4.1, D4.2 and D4.4a–e are Proved, and the series is open at D4.3 and its five branch closeouts D4.3a–e. One conditional result (E677 together with conjugacy-closed left translations implies E255; Padilla, 2026) is Proved on this platform. The milestone "Alternative resolution — a finite E677 counterexample to E255" (theorem finite_counterexample) is the disproof target. The sixteen milestones "Counterexample structure (a)–(p)" are constraints on a counterexample and rules for a counterexample search, all Proved; (h)–(j) take small-order facts as hypotheses. None of the sixteen is a disproof. None of the displayed statements restricts the cardinality to a tested range.

In the authors' repository, Sub-goal 1 is called Piece 1, the unique-outsider case containing Sub-goal 2 is called Gap 1, and the case of Sub-goal 3 is called Gap ≥ 2; those names appear in some theorem sources and file names.

Significance

A resolution determines whether this particular law gains E255 as a consequence upon restriction to finite carriers. An affirmative proof must cover every finite cardinality, every operation on each carrier, and every assignment of the universally quantified elements. A finite counterexample must supply an operation that satisfies every instance of E677 while failing E255 at some element.

The formal package provides small, reusable statements of the two laws, the left translation property, and the fixer constraint. Keeping these statements separate allows their precise hypotheses and conclusions to be checked individually. In particular, the second supporting result says what a fixer must be when one exists; the fixer-existence formulation records the additional mathematical content needed to ensure existence.

Difficulty

The left translation conclusion concerns maps with the left input fixed. The fixer-existence formulation instead asks about the image of the map y↦y⋄xy\mapsto y\diamond xy↦y⋄x, with its right input fixed. No assumption in the formal goal makes these two maps interchangeable. Bijectivity of every left translation map alone does not state that a fixer exists.

Because the implication fails for infinite magmas, E255 is not an equational consequence of E677, so any proof must use finiteness in an essential way. The blueprint's linear and linear-extension constructions cannot produce a finite counterexample (blueprint Lemmas 13.3 and 13.4); community members have formalized on this platform the scalar-coefficient case of the linear lemma, the Type I and Type II affine families, and the linear-extension lemma (see the discussion thread).

Likewise, checking a collection of finite operation tables does not quantify over arbitrary finite cardinalities. Such computation does not discharge the goal submitted here. Any proof must justify every use of finiteness and retain the displayed parenthesization of the laws.

Formalization scope

The representation uses an arbitrary universe-polymorphic type, an explicit binary operation, and a Fintype instance for finite targets. Passing the operation explicitly avoids importing a separate magma package or imposing algebraic typeclass laws. The predicates E677 and E255 themselves do not assume finiteness; each theorem states its own finite-carrier hypothesis.

Empty carriers are included. Both laws hold vacuously on them; the pointwise fixer statement is also vacuous because there is no element xxx. Consequently an empty carrier cannot refute the main goal. Nonempty carriers of every finite size are included without further assumptions. There is no associativity, commutativity, idempotence, identity element, or cancellation hypothesis hidden in the representation.

The definition bundle FiniteMagmaE677 provides E677, E255, HasFixerAt (existence of a fixer of xxx), InLeftOrbit (membership in the left orbit of xxx) and OrbitRightCollisionOrFixer. Three further bundles, FiniteMagmaE677_seventh_element_growth, FiniteMagmaE677_d4_first_return and FiniteMagmaE677_sswap_renewal, hold the period-four packet types used by the D4 milestones.

Status (2026-10-22 UTC). Proved on this platform: Lemma 13.1(i)–(iii), the Sub-goal 1, Sub-goal 2 and Sub-goal 3 support lemmas, D4.0, D4.1, D4.2, D4.4a–e, the conditional conjugacy-closure theorem, Counterexample structure (a)–(p), and three further conditional theorems by omegaestable (existential row transport, parametrized row transport, left-parameter transport; see the discussion thread). Open: Sub-goals 1–3, D4.3 with D4.3a–e, and the counterexample target. Community members have also formalized the blueprint's 496-element non-right-cancellative E677 magma (see the discussion thread).

Welcome contributions: a proof of any open sub-goal or D4.3 branch (a proof of Sub-goal 3 proves the goal; see the milestone "Sub-goal 3 support (a)"); a proof sketch that reduces an open leaf to new lemmas; a concrete operation table on Fin n proving finite_counterexample, which would make the main theorem false.

Results in the captain's private repository that are not on this platform

Results that are Proved on this platform are not repeated here. Readers cannot open the captain's private repository, so each statement is given in full. PROVEN means a complete proof, in the form stated. BOUNDED means a SAT-solver result for one encoded finite structure: each UNSAT result used here has a DRAT proof that drat-trim accepted (unverified C code, not a kernel-checked proof). EMPIRICAL means a computation over finite data, with no certificate.

Not ported

A port of these results to this platform is a long job.

1. The finite facts that Counterexample structure (h)–(j) take as hypotheses. BOUNDED. No E677 magma has order 2, 3, 4, 6 or 8, and every E677 magma of order 7 or 9 has an idempotent. Counterexample structure (h) and (j) give the earlier sources and the captain's check. These facts, except those for orders 2 and 3, are hypotheses of theorems that are Proved on this platform, so a port of them would make (h)–(j) unconditional; it needs kernel-checked proofs made from the DRAT certificates. Source: the captain's private repository, revision dd2ee3e5, experiments/analysis/idempotent-free-small-orders-2026-10-21/ and, for order 8, experiments/analysis/ti-groups-2026-10-19/ (section "Order 8").

2. Period-four refinements of D4.2. PROVEN (Lean; axioms propext, Classical.choice, Quot.sound). A repository theorem refines the five branches of the D4.2 first-return packet and keeps every case. Write q=c2⋄xq=c_2\diamond xq=c2​⋄x. In the R-through-one branch (the repository's name), each outcome is a fixer of xxx, a strict decrease of a finite contact budget, a new LxL_xLx​-cycle disjoint from the elements already accounted for (with its exact size), or a closed trace of Lq−1L_q^{-1}Lq−1​ that is reduced to two phase-contact families. In the two unswapped S branches, each outcome is a fixer of xxx, a decrease by one of the number of unmarked phases on the LxL_xLx​-cycle of qqq, or a new disjoint LxL_xLx​-cycle with its exact size. These results do not close D4.3 or any of D4.3a–e, because the outcomes are not yet combined into one state with a strictly decreasing well-founded measure. A port needs the repository's library of period-four packets. Source: the captain's private repository, revision 4100763b, lean/E677/Spine/Piece1D4RefinedFirstReturn.lean, e677_d4_q_refinedFirstReturnPacket_of_firstReturnPacket.

Not formalized

These results have only solver or computation evidence, and no Lean proof, and no milestone on this platform uses them as hypotheses.

3. A counterexample has at least 11 elements. BOUNDED. Every E677 magma with at most 10 elements satisfies E255. By item 1, no E677 magma has order 2, 3, 4, 6 or 8. Every E677 magma of order 5, 7 or 9 is right-cancellative; then each right translation y↦y⋄xy\mapsto y\diamond xy↦y⋄x is a bijection, so xxx has a fixer, and Lemma 13.1(ii) gives E255 at xxx. At order 10, a point xxx at which E255 fails has no fixer, so xxx is not in its own column {y⋄x}\{y\diamond x\}{y⋄x}; a search for such a table, split into 67 cases by the cycle type of LxL_xLx​ (the length l≥2l\ge 2l≥2 of the left orbit of xxx, and the cycle lengths of LxL_xLx​ on the other 10−l10-l10−l elements), is UNSAT in each case. Earlier reports: the sources listed in Counterexample structure (h)–(j) for the E677 magmas of orders 2–4 and 6–9, among them a Lean proof for order 6 by J. Hyun. Without certificates (ETP Zulip thread "FINITE: 677 -> 255"): J. Brox (Mace4) reports no counterexample of order 9 (2024-12-10), none of order at most 10 (2025-01-10), no E677 magma of order 10 (2025-01-12) and no counterexample of order 11 (2025-03-12); B. Le Floch (2024-12-22, Mace4) reports none of order at most 9; J. Hyun (2025-01-09, CaDiCaL) none of order 5 to 8; S. Chuks-Onah (2026-05-01, Z3) none of order 5 or 6; R. Schneider (2026-05-15, own search program) and B. Subercaseaux (2026-05-15, SAT) none of order at most 11. The new content here is the DRAT certificates. Source: the captain's private repository, revision dd2ee3e5, experiments/analysis/rc-small-orders-2026-10-19/ and experiments/analysis/rc-cubes-2026-10-19/.

4. Order 35 over the quotient x⋄y=4x+3yx\diamond y=4x+3yx⋄y=4x+3y on F7\mathbb{F}_7F7​. With the order-7 fact of item 1, Counterexample structure (i) gives: if a minimum counterexample MMM has order 35 and a non-universal congruence θ\thetaθ that relates zzz and q(z)q(z)q(z), then M/θM/\thetaM/θ has 7 elements and an idempotent, and the classes have 5 elements. By the classification of J. Brox (ETP Zulip thread "FINITE: 677 -> 255", 2025-03-26, Mace4, no certificate; not checked by the captain), M/θM/\thetaM/θ is then isomorphic to 4x+3y4x+3y4x+3y or to 4x+y4x+y4x+y on F7\mathbb{F}_7F7​. Take QQQ: x⋄y=4x+3yx\diamond y=4x+3yx⋄y=4x+3y on F7\mathbb{F}_7F7​ (0 is its only idempotent), write the elements of MMM as pairs (a,s)(a,s)(a,s) with a∈F7a\in\mathbb{F}_7a∈F7​ and s∈F5s\in\mathbb{F}_5s∈F5​, and call the map (s,t)↦(s,t)\mapsto(s,t)↦ (second coordinate of (a,s)⋄(b,t)(a,s)\diamond(b,t)(a,s)⋄(b,t)) the block over (a,b)(a,b)(a,b). Results, each for an E677 magma of this form:

  • If at most five blocks other than the block over (0,0)(0,0)(0,0) do not have the form (s,t)↦s+fab(t−s)(s,t)\mapsto s+f_{ab}(t-s)(s,t)↦s+fab​(t−s) with a permutation fabf_{ab}fab​ of F5\mathbb{F}_5F5​, then E255 holds. BOUNDED (two short paper lemmas reduce it to 48 patterns of non-cyclic blocks, each UNSAT). This includes the case where every block has this form.
  • If every block has the form (s,t)↦A t+B(s,t)\mapsto A\,t+B(s,t)↦At+B with A∈{1,4}A\in\{1,4\}A∈{1,4} (with AAA and BBB chosen for each block and each sss), then E255 holds. BOUNDED.
  • With all blocks free, the solver runs did not finish, so there is no result. The quotient 4x+y4x+y4x+y was not tested.

The only known E677 magma of order 35 with this quotient and classes of 5 elements is isomorphic to Q×M5Q\times M_5Q×M5​, where M5M_5M5​ is s⋄t=2s−ts\diamond t=2s-ts⋄t=2s−t on F5\mathbb{F}_5F5​ (EMPIRICAL). T. Tao (ETP Zulip thread "FINITE: 677 -> 255", 2024-12-13) proposed the extensions (x,s)⋄(y,t)=(4x+3y, s⋄x,yt)(x,s)\diamond(y,t)=(4x+3y,\ s\diamond_{x,y}t)(x,s)⋄(y,t)=(4x+3y, s⋄x,y​t), and (same thread, 2024-12-22) the fibre operations s+fx,y(t−s)s+f_{x,y}(t-s)s+fx,y​(t−s) of the first result. The second result is a case of the form (x⋄y, bx,y,st+cx,y,s)(x\diamond y,\ b_{x,y,s}t+c_{x,y,s})(x⋄y, bx,y,s​t+cx,y,s​) for which B. Reinke (same thread, 2026-06-11) expected E255 to lift, without a proof. Source: the captain's private repository, revision dd2ee3e5, docs/current/e677-coverage-matrix-2026-10-19.md (the rows for this quotient) and experiments/analysis/pro-counterexample-audit-2026-10-20/.

5. Extensions and row changes of the order-31 magma x⋄y=5x−4y+1x\diamond y=5x-4y+1x⋄y=5x−4y+1 on F31\mathbb{F}_{31}F31​. Call it Q31Q_{31}Q31​. It has no idempotent, and it is the smallest known E677 magma without an idempotent; every known E677 magma without an idempotent has order divisible by 31 (EMPIRICAL). So Q31Q_{31}Q31​ is the smallest known candidate quotient in Counterexample structure (j). BOUNDED results:

  • No E677 magma has a congruence with quotient Q31Q_{31}Q31​ and classes of 2 or 3 elements.
  • No E677 magma with a congruence with quotient Q31Q_{31}Q31​ and classes of 4 elements fails E255.
  • In the family (u,s)⋄(w,t)=(5u−4w+1, s+hw−u(t−s))(u,s)\diamond(w,t)=(5u-4w+1,\ s+h_{w-u}(t-s))(u,s)⋄(w,t)=(5u−4w+1, s+hw−u​(t−s)) on F31×F5\mathbb{F}_{31}\times\mathbb{F}_5F31​×F5​, with permutations hdh_dhd​ of F5\mathbb{F}_5F5​, no E677 member fails E255.
  • An E677 operation on F31\mathbb{F}_{31}F31​ that fails E255 differs from Q31Q_{31}Q31​ in at least 20 rows and at least 40 cells.

B. Le Floch (ETP Zulip thread "FINITE: 677 -> 255", 2024-12-13) found 5x−4y+c5x-4y+c5x−4y+c mod 31 as the one linear E677 model in which ccc cannot be removed, and R. Schneider (same thread, 2025-11-21) noted that Q31Q_{31}Q31​ has no idempotent. T. Tao (same thread, 2024-12-13) proposed the extensions (x,s)⋄(y,t)=(x⋄y, s⋄y−xt)(x,s)\diamond(y,t)=(x\diamond y,\ s\diamond_{y-x}t)(x,s)⋄(y,t)=(x⋄y, s⋄y−x​t) of Q31Q_{31}Q31​. B. Reinke (same thread, 2025-11-07) encoded them for z3 and wrote that he thought he could exclude classes of fewer than 4 elements (no certificate). The first result above covers all extensions with classes of 2 or 3 elements, not only these; the third result is the case of Tao's extensions with fibre operations s+h(t−s)s+h(t-s)s+h(t−s). Source: the captain's private repository, revision dd2ee3e5, experiments/analysis/gap2-monolith-m3-2026-10-17/ (§2, §6), experiments/analysis/pro-counterexample-audit-2026-10-20/ (cyclic-section-19375/, construction-19350/) and experiments/analysis/idempotent-free-2026-10-19/.

6. Tables with an automorphism of prime order, orders 12–21. BOUNDED, incomplete. Let α\alphaα be an automorphism of prime order ppp of an E677 magma of order nnn, 12≤n≤2112\le n\le 2112≤n≤21, with fff fixed points, and let zzz be a point with no fixer. The fixed points of α\alphaα form a submagma, so an E677 magma of order fff; by item 1, f∉{2,3,4,6,8}f\notin\{2,3,4,6,8\}f∈/{2,3,4,6,8}. The search covers f∈{0,1,5,7,9,11}f\in\{0,1,5,7,9,11\}f∈{0,1,5,7,9,11}. If α\alphaα fixes zzz, the fixed points form an E677 magma of order fff that fails E255 at zzz; this is excluded for f≤9f\le 9f≤9 by item 3, and for f=11f=11f=11 4 shapes (n,p,f)(n,p,f)(n,p,f) are UNSAT and 7 were not run. If zzz is in a cycle of α\alphaα, 26 shapes are UNSAT (all 9 shapes with p≥11p\ge 11p≥11, and 17 shapes with p≤7p\le 7p≤7); 14 shapes are UNKNOWN after 3600 s, and 40 were not run. Not covered: the shapes with f=0f=0f=0 and one cycle (n=p∈{13,17,19}n=p\in\{13,17,19\}n=p∈{13,17,19}, translation-invariant tables on Zn\mathbb{Z}_nZn​), fixed-point count 10, and fixed-point counts of at least 12. Earlier searches without certificates (ETP Zulip thread "FINITE: 677 -> 255"): R. Schneider (2025-11-20 and 2025-11-21) searched the tables with the automorphism (0)(1 2 … n−1)(0)(1\,2\,\dots\,n-1)(0)(12…n−1) up to n=31n=31n=31 and found only right-cancellative ones (the shapes with f=1f=1f=1 and one cycle); B. Reinke (2025-11-21) noted that the fixed points form a submagma and found no table with one cycle and 5 fixed points of order at most 25 other than order 5 (the shapes with f=5f=5f=5 and one cycle), and (2025-11-26) noted that in a minimum counterexample only the identity automorphism fixes the failing point. Source: the captain's private repository, revision dd2ee3e5, experiments/analysis/symmetric-simple-2026-10-20/.

7. A refuted intermediate statement. EMPIRICAL (exhaustive check of one explicit table, run twice with independent encodings; not kernel-checked). Let S(x)S(x)S(x) be the closure of the left orbit of xxx under z↦z⋄xz\mapsto z\diamond xz↦z⋄x. The repository's gate CP asserted: in a finite E677 magma, if the hypotheses of Sub-goal 3 hold at xxx and z↦z⋄xz\mapsto z\diamond xz↦z⋄x is not injective on S(x)S(x)S(x), then the left orbit of xxx has minimal period 777. Let KKK be the 7-element E677 magma of Sub-goal 3 support (a) (file db/7/1 of the public collection memoryleak47/eq677), and let MMM be the E677 magma of order 777777 in file db/77/65 of the same collection. In M×KM\times KM×K (order 539539539; E677 checked on all 5392539^25392 pairs), the point (0,0)(0,0)(0,0) satisfies these hypotheses, and its left orbit has minimal period lcm⁡(7,6)=42\operatorname{lcm}(7,6)=42lcm(7,6)=42. The point (0,0)(0,0)(0,0) has the fixer (76,4)(76,4)(76,4), so this is not a counterexample to E255, and it refutes CP only in the form without a no-fixer hypothesis. Source: the captain's private repository, revision 4100763b, docs/current/dead-ends/gap-ge-2.md, entry D7-6.

8. Φ(x)=(x⋄x)⋄x\Phi(x)=(x\diamond x)\diamond xΦ(x)=(x⋄x)⋄x is not injective in general. EMPIRICAL. In the 2026-09-27 snapshot of the community database (4091 tables), every table satisfies E255, and Φ\PhiΦ is not injective in 1107 of them; the smallest such order is 777. In one table of order 7, row 6 is the identity row, so 666 is a fixer of every xxx and Lemma 13.1(ii) gives Φ(x)=6\Phi(x)=6Φ(x)=6 for every xxx. So global injectivity of Φ\PhiΦ is not a usable intermediate target. Source: the captain's private repository, revision 4100763b, docs/professor-phi-injectivity.md, correction of 2026-10-14.

Selected references

  • Matthew Bolan et al., The Equational Theories Project: Advancing Collaborative Mathematical Research at Scale, arXiv:2512.07087v2 (December 16, 2025), paper.
  • The Equational Theories Project contributors, Equational Theories, online proof blueprint, Chapter 13, equations (1)–(2) and Lemmas 13.1–13.4, chapter, accessed September 7, 2026 and October 13, 2026.
  • J. I. Padilla (GitHub: omegaestable), Prove E677 implies E255 under left translation conjugacy closure, Equational Theories Project pull request #1518, 2026 (closed without merge by its author on 2026-10-13; the theorem is Proved on this platform), pull request.
  • Lean Zulip, channel "Equational", thread "FINITE: 677 -> 255", thread.
54 thms4 active usersReviewed
Computational GeometryDiscrete GeometryGraph Theory·Captain: hao jia

Uniform Obstacle Bounds for Planar Graphs (OPG-37357)Open Problem

Motivation

An obstacle representation turns a graph into a visibility system: vertices are points in the plane, and nonedges are blocked by polygonal obstacles. The obstacle number asks for the minimum number of obstacles needed. OPG-37357 records two different questions for planar graphs. The first asks whether one obstacle can ever be insufficient. The second asks whether some universal constant bounds the ordinary obstacle number of every planar graph.

The status of the two parts is different. Berman, Chappell, Faudree, Gimbel, Hartman, and Williams proved in 2017 that explicit planar graphs, including the icosahedron and their graphs X4X_4X4​ and X6X_6X6​, have ordinary obstacle number two. Thus the first question has a published positive answer. The universal-constant question remains the research target here. A separate invariant called planar or plane obstacle number requires a crossing-free visibility drawing; results for that invariant must not be substituted for the ordinary obstacle number used by this mission.

Setting

A finite simple graph GGG has a kkk-obstacle drawing when its vertices are placed injectively as points in R2\mathbb R^2R2 and there are kkk pairwise disjoint closed connected polygonal obstacles such that

uv∈E(G)⟺[p(u),p(v)] meets no obstacle.uv\in E(G) \quad\Longleftrightarrow\quad [p(u),p(v)]\text{ meets no obstacle}.uv∈E(G)⟺[p(u),p(v)] meets no obstacle.

Graph vertices lie outside every obstacle. The ordinary obstacle number obs⁡(G)\operatorname{obs}(G)obs(G) is the least such kkk. The drawing itself may contain crossings between visible graph edges; planarity is a property of the abstract input graph, not an extra constraint on the obstacle drawing.

The Lean model represents a polygonal obstacle as a connected finite union of closed filled triangles. This gives a compact polygonal region with exact real-coordinate segment incidence. Straight-line planarity of the abstract graph is represented separately.

Formalization targets

The two-part OPG record

The source records both

∃ finite planar G, obs⁡(G)>1\exists\text{ finite planar }G,\ \operatorname{obs}(G)>1∃ finite planar G, obs(G)>1

and

∃k∈N ∀ finite planar H, obs⁡(H)≤k.\exists k\in\mathbb N\ \forall\text{ finite planar }H, \ \operatorname{obs}(H)\le k.∃k∈N ∀ finite planar H, obs(H)≤k.

The first assertion is known in the literature and appears as a published-result milestone. The second is open and is therefore the mission's main theorem. Together they preserve the two-part source without presenting the whole record as unresolved.

Published first part

A milestone formalizes the stronger published statement

∃ finite planar G,obs⁡(G)≤2andobs⁡(G)≰1.\exists\text{ finite planar }G, \qquad \operatorname{obs}(G)\le2 \quad\text{and}\quad \operatorname{obs}(G)\not\le1.∃ finite planar G,obs(G)≤2andobs(G)≤1.

This captures ordinary obstacle number exactly two without hard-coding one graph before its adjacency data and lower-bound certificate are formalized.

Universal bound

The open milestone asks for a single natural number kkk, chosen before the graph, that works for every finite planar graph. The number of obstacle corners is not bounded by this theorem; only the number of connected polygonal obstacles is.

Significance

The published first part establishes that planarity alone does not force a one-obstacle representation. The second part asks whether planar graphs nevertheless have uniformly bounded visibility complexity. A positive answer would produce a common finite obstacle budget independent of graph order; a negative answer would require a family of planar graphs with unbounded ordinary obstacle number.

Formalization is especially useful because several nearby notions differ by one word but have different known bounds: ordinary versus plane obstacle number, arbitrary polygonal versus convex obstacles, and fixed-placement versus freely chosen drawings. The mission's definitions make those choices explicit and provide reusable segment-obstacle semantics for later geometric graph formalizations.

Difficulty

A finite combinatorial graph does not come with a canonical visibility drawing. Even when one starts with an arbitrary connected blocking set, replacing it by one bounded simple polygon requires compactness, component, incidence, and polygonal-neighborhood arguments. Conversely, lower bounds must quantify over every possible placement and obstacle, not merely refute a selected coordinate drawing.

Counting results for unrestricted graphs do not automatically preserve planarity. Bounds for planar obstacle number impose a crossing-free drawing and therefore answer a different question. The known two-obstacle examples close only the existential first part and give no universal kkk.

Formalization scope

All graph vertex types are finite. Obstacles are closed connected polygonal regions represented by finite triangle unions; they are pairwise disjoint and avoid graph vertices. Visibility uses the full closed segment, so tangency or boundary contact blocks a nonedge. The planarity witness is independent of the obstacle drawing. Empty and one-vertex graphs remain in the universal quantifier and should be handled without division or nonemptiness assumptions.

The repository's fixed-placement polygonization argument and finite arrangement code are candidate_only. They may motivate supporting lemmas, but they neither prove the unrestricted obstacle-drawing completeness theorem nor settle the universal bound. Contributions are welcome on exact geometry primitives, the published two-obstacle construction and lower bound, conversions between connected blockers and polygonal obstacles, and the universal root. A proof for the plane invariant, convex invariant, one fixed drawing, or a finite order cutoff must be labeled at that narrower scope.

Selected references

  • L. W. Berman, G. G. Chappell, J. R. Faudree, J. Gimbel, C. Hartman, and G. I. Williams, Graphs with Obstacle Number Greater than One, JGAA 21(6), 2017. https://doi.org/10.7155/jgaa.00452
  • J. Gimbel, P. Ossona de Mendez, and P. Valtr, Obstacle Numbers of Planar Graphs, Graph Drawing 2017. https://arxiv.org/abs/1706.06992
  • M. Balko, S. Chaplick, R. Ganian, S. Gupta, M. Hoffmann, P. Valtr, and A. Wolff, Bounding and Computing Obstacle Numbers of Graphs, SIAM Journal on Discrete Mathematics 38(2), 2024. https://arxiv.org/abs/2206.15414
  • Open Problem Garden / UnsolvedMath, OPG-37357. https://www.unsolvedmath.com/problems/OPG-37357
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CombinatoricsGraph TheoryOptimization·Captain: hao jia

Clique Partitions of Chordal Graphs (Erdos Problem 81)Open Problem

Motivation

An edge partition into cliques compresses the adjacency structure of a graph into complete pieces without allowing any edge to be counted twice. Erdős Problem 81 asks for the asymptotically sharp upper bound on the number of pieces needed when the graph is chordal. Chordal graphs have strong elimination structure, but that structure does not make the partition parameter additive under arbitrary edge deletion, and obtaining a linear error term remains substantially stronger than identifying the leading quadratic coefficient.

Erdős, Ordman, and Zalcstein studied clique partitions of chordal graphs in 1993. Their examples already exhibit the n2/6n^2/6n2/6 scale, while their general upper estimate had a larger quadratic coefficient. Later dense-packing results of Haxell–Rödl and Yuster compare fractional and integer triangle packings with an o(n2)o(n^2)o(n2) gap. The project candidate combines that interface with chordal elimination arguments to formulate a uniform n2/6+o(n2)n^2/6+o(n^2)n2/6+o(n2) milestone. It does not supply the O(n)O(n)O(n) remainder asked for by the root.

Setting

A finite simple graph is chordal when it has no induced cycle of length greater than three. The Lean definition uses the equivalent perfect-elimination form: vertices admit an injective ranking such that the later neighbors of every vertex form a clique.

An edge partition into cliques is a finite family P\mathcal PP of complete vertex sets such that every edge of GGG belongs to exactly one member of P\mathcal PP. Members may share vertices but may not share edges. Write cp⁡(G)\operatorname{cp}(G)cp(G) for the minimum possible number of pieces.

The asymptotic notation

n26+O(n)\frac{n^2}{6}+O(n)6n2​+O(n)

means that there are constants C>0C>0C>0 and n0≥1n_0\ge1n0​≥1, chosen independently of GGG and nnn, such that every chordal nnn-vertex graph with n≥n0n\ge n_0n≥n0​ has a clique partition with at most n2/6+Cnn^2/6+Cnn2/6+Cn pieces.

Formalization targets

Erdős Problem 81

The root theorem is

∃C>0 ∃n0≥1 ∀n≥n0 ∀G chordal on n vertices,cp⁡(G)≤n26+Cn.\exists C>0\ \exists n_0\ge1\ \forall n\ge n_0\ \forall G\text{ chordal on }n\text{ vertices}, \qquad \operatorname{cp}(G)\le \frac{n^2}{6}+Cn.∃C>0 ∃n0​≥1 ∀n≥n0​ ∀G chordal on n vertices,cp(G)≤6n2​+Cn.

The quantifier order is essential: CCC and n0n_0n0​ are universal and cannot depend on the graph.

Leading-coefficient milestone

The supporting target records the weaker uniform statement

∀ε>0 ∃n0 ∀n≥n0 ∀G chordal on n vertices,cp⁡(G)≤(16+ε)n2.\forall\varepsilon>0\ \exists n_0\ \forall n\ge n_0\ \forall G\text{ chordal on }n\text{ vertices}, \qquad \operatorname{cp}(G)\le \left(\frac16+\varepsilon\right)n^2.∀ε>0 ∃n0​ ∀n≥n0​ ∀G chordal on n vertices,cp(G)≤(61​+ε)n2.

This is the precise n2/6+o(n2)n^2/6+o(n^2)n2/6+o(n2) form. It is not equivalent to the root: choosing ε=1/n\varepsilon=1/nε=1/n is invalid because the cutoff may depend on the fixed value of ε\varepsilonε.

Significance

The root would determine the clique-partition extremum for chordal graphs up to a linear remainder, matching the scale of the complete-split examples that motivate the coefficient 1/61/61/6. It would refine a leading-order asymptotic theorem into a uniform estimate strong enough to distinguish second-order behavior.

Formalization creates a clean interface among perfect elimination orderings, exact edge partitions, fractional edge-and-triangle decompositions, and integer triangle packings. It also forces the proof to distinguish a partition from a cover and original graph order from the order of any auxiliary hypergraph. These definitions can support other decomposition problems on chordal and split graphs.

Difficulty

Perfect elimination does not by itself give the sharp partition count. Greedily taking maximal cliques may overlap in edges or accumulate too many singleton pieces. Similarly, a fractional edge-and-triangle partition can achieve the right leading coefficient while integer rounding loses o(n2)o(n^2)o(n2) pieces; the root requires that loss to be only O(n)O(n)O(n).

The dense-packing theorem has quantifiers of the form “for every fixed ε>0\varepsilon>0ε>0 there exists N(ε)N(\varepsilon)N(ε).” It therefore yields a uniform subquadratic error but no linear error. Any proof of the root must add a chordal-specific rounding or extremal reduction rather than treating the general packing theorem as if its ε\varepsilonε could vary with nnn.

Formalization scope

Graphs are finite and simple. Chordality is encoded by existence of a perfect-elimination ranking, including disconnected and edgeless graphs. A clique piece is a finite vertex set that spans a complete subgraph. Exactness means every actual edge occurs in exactly one piece; no nonedge can occur inside a piece. Bounds are compared in R\mathbb RR so the displayed asymptotic expressions retain their conventional form, while the number of parts remains a natural number.

The candidate derivation of the leading coefficient imports finite linear-programming duality and the Haxell–Rödl/Yuster fixed-triangle packing approximation. It is candidate_only, not an admitted result or kernel proof. Contributions may formalize the perfect-elimination lemmas, the fractional compression, the uniform packing interface, complete-split lower examples, or the root linear rounding theorem. A result for edge-and-triangle pieces only, a fractional partition, or one fixed order must not be presented as the unrestricted integer clique-partition theorem.

Selected references

  • P. Erdős, E. T. Ordman, and Y. Zalcstein, Clique Partitions of Chordal Graphs, Combinatorics, Probability and Computing 2(4), 1993. https://doi.org/10.1017/S0963548300000808
  • P. E. Haxell and V. Rödl, Integer and Fractional Packings in Dense Graphs, Combinatorica 21, 2001. https://doi.org/10.1007/s004930170003
  • R. Yuster, Integer and fractional packing of families of graphs, 2003. https://arxiv.org/abs/math/0305350
  • Erdős Problems, Problem 81. https://www.erdosproblems.com/81
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Partial Differential EquationsPure Mathematics·Captain: korbonits

Formalize Navier-StokesOpen Problem

Motivation

The incompressible Navier–Stokes equations are the standard model for the motion of a viscous fluid such as water or air, used daily in engineering, meteorology and oceanography. Yet the most basic mathematical question about them is open: starting from smooth initial data in three dimensions, does a smooth solution exist for all time? This is one of the seven Millennium Prize Problems of the Clay Mathematics Institute. Its official formulation is Charles Fefferman's problem description, Existence and smoothness of the Navier–Stokes equation (2000), which offers a prize for a proof of any one of four statements: global existence and smoothness on R3\mathbb{R}^3R3 (statement (A)) or on the torus R3/Z3\mathbb{R}^3/\mathbb{Z}^3R3/Z3 (statement (B)), or a counterexample to either (statements (C) and (D)). This mission formalizes statement (A), together with the classical partial results that Fefferman lists as known.

Timeline.

  • 1822–1845: Navier and Stokes write down the equations of a viscous incompressible fluid.
  • 1934: Jean Leray, Sur le mouvement d'un liquide visqueux emplissant l'espace (Acta Math. 63), proves on R3\mathbb{R}^3R3 that smooth solutions exist for a positive time depending on the data, that they exist for all time when the data is small compared with the viscosity, and that global weak solutions with finite energy always exist. Their smoothness and uniqueness are left open.
  • 1933–1969: the two-dimensional problem is settled (Leray for the plane; Olga Ladyzhenskaya's monograph The Mathematical Theory of Viscous Incompressible Flow, 2nd ed. 1969, for bounded domains): smooth solutions exist for all time and are unique.
  • 1984: Tosio Kato, Strong LpL^pLp-solutions of the Navier–Stokes equation in Rm\mathbb{R}^mRm (Math. Z. 187), gives global solutions for initial data small in L3(R3)L^3(\mathbb{R}^3)L3(R3).
  • 1976–1998: partial regularity. Scheffer, then Caffarelli, Kohn and Nirenberg (Comm. Pure Appl. Math. 35, 1982), show that the singular set of a suitable weak solution has one-dimensional parabolic Hausdorff measure zero.
  • 2000: the Clay Mathematics Institute adopts Fefferman's formulation as a Millennium Prize Problem. It remains open.

Setting

Fix a dimension n≥1n \ge 1n≥1 and write Rn\mathbb{R}^nRn for Euclidean nnn-space with its Euclidean norm ∣x∣|x|∣x∣; in Lean this is NavierStokes.Vec n. A velocity field assigns to each time t∈Rt \in \mathbb{R}t∈R and point x∈Rnx \in \mathbb{R}^nx∈Rn a vector u(x,t)∈Rnu(x,t) \in \mathbb{R}^nu(x,t)∈Rn; in Lean u tu\,tut is the field at time ttt and u t xu\,t\,xutx is Fefferman's u(x,t)u(x,t)u(x,t). A pressure is a real function p(x,t)p(x,t)p(x,t). The viscosity ν\nuν is a positive constant. The external force of Fefferman's equation (1) is identically zero throughout, as in statement (A).

For a vector field v:Rn→Rnv : \mathbb{R}^n \to \mathbb{R}^nv:Rn→Rn the divergence is

div⁡v=∑i=1n∂vi∂xi,\operatorname{div} v = \sum_{i=1}^n \frac{\partial v_i}{\partial x_i},divv=i=1∑n​∂xi​∂vi​​,

in Lean NavierStokes.div, computed from the Fréchet derivative Dv(x)Dv(x)Dv(x) as ∑i(Dv(x) ei)i\sum_i (Dv(x)\,e_i)_i∑i​(Dv(x)ei​)i​. The Laplacian Δv=∑i∂2v/∂xi2\Delta v = \sum_i \partial^2 v/\partial x_i^2Δv=∑i​∂2v/∂xi2​ acts componentwise (Mathlib's Laplacian on inner product spaces). The gradient ∇p\nabla p∇p is Mathlib's gradient. The convective term ∑juj ∂u/∂xj\sum_j u_j\,\partial u/\partial x_j∑j​uj​∂u/∂xj​ is the derivative of u(⋅,t)u(\cdot,t)u(⋅,t) at xxx in the direction u(x,t)u(x,t)u(x,t). Finally ∣∇v∣2=∑i,j(∂vi/∂xj)2|\nabla v|^2 = \sum_{i,j} (\partial v_i/\partial x_j)^2∣∇v∣2=∑i,j​(∂vi​/∂xj​)2 is NavierStokes.gradNormSq.

Admissible initial data (Fefferman's condition (4), NavierStokes.IsInitialData): a C∞C^\inftyC∞, divergence-free vector field u0u^0u0 that decays together with all its derivatives faster than any power,

∣∂xαu0(x)∣≤CαK (1+∣x∣)−Kon Rn, for every α and K.|\partial_x^\alpha u^0(x)| \le C_{\alpha K}\,(1+|x|)^{-K} \quad \text{on } \mathbb{R}^n, \text{ for every } \alpha \text{ and } K.∣∂xα​u0(x)∣≤CαK​(1+∣x∣)−Kon Rn, for every α and K.

In Lean the bound is (1+∣x∣)K ∥Dku0(x)∥≤CkK(1+|x|)^K\,\|D^k u^0(x)\| \le C_{kK}(1+∣x∣)K∥Dku0(x)∥≤CkK​ on the kkk-th Fréchet derivative, an equivalent family of conditions. These are exactly the divergence-free Schwartz functions.

A physically reasonable solution on a set SSS of times (NavierStokes.IsSolutionOn; S=[0,∞)S = [0,\infty)S=[0,∞) for NavierStokes.IsSolution) is a pair (u,p)(u,p)(u,p) such that

  1. (Fefferman (6)) uuu and ppp are C∞C^\inftyC∞ on S×RnS \times \mathbb{R}^nS×Rn, up to the boundary of SSS;
  2. (Fefferman (1), f≡0f \equiv 0f≡0) for every t∈St \in St∈S with t>0t > 0t>0 and every xxx,
∂u∂t+∑j=1nuj∂u∂xj=ν Δu−∇p;\frac{\partial u}{\partial t} + \sum_{j=1}^n u_j \frac{\partial u}{\partial x_j} = \nu\,\Delta u - \nabla p;∂t∂u​+j=1∑n​uj​∂xj​∂u​=νΔu−∇p;
  1. (Fefferman (2)) div⁡u(⋅,t)=0\operatorname{div} u(\cdot,t) = 0divu(⋅,t)=0 for every t∈St \in St∈S;
  2. (Fefferman (3)) u(x,0)=u0(x)u(x,0) = u^0(x)u(x,0)=u0(x);
  3. (Fefferman (7), bounded energy) ∫Rn∣u(x,t)∣2 dx<C\int_{\mathbb{R}^n} |u(x,t)|^2\,dx < C∫Rn​∣u(x,t)∣2dx<C for all t∈St \in St∈S, for some constant CCC.

Formalization targets

Goal: Fefferman's statement (A)

Take ν>0\nu > 0ν>0 and n=3n = 3n=3. For every admissible initial datum u0u^0u0 there exist a velocity field uuu and a pressure ppp forming a physically reasonable solution on R3×[0,∞)\mathbb{R}^3 \times [0,\infty)R3×[0,∞):

∀ ν>0, ∀ u0 satisfying (4), ∃ (u,p) satisfying (1), (2), (3), (6), (7) on R3×[0,∞).\forall\, \nu > 0,\ \forall\, u^0 \text{ satisfying (4)},\ \exists\, (u,p) \text{ satisfying (1), (2), (3), (6), (7) on } \mathbb{R}^3 \times [0,\infty).∀ν>0, ∀u0 satisfying (4), ∃(u,p) satisfying (1), (2), (3), (6), (7) on R3×[0,∞).

This is NavierStokes.existence_and_smoothness_R3. It is open; a proof would settle the Millennium Prize Problem in the affirmative.

Milestones: what Fefferman lists as known

  1. Local existence (NavierStokes.local_existence_R3): for n=3n = 3n=3 and every admissible u0u^0u0 there are T>0T > 0T>0 and a physically reasonable solution on R3×[0,T)\mathbb{R}^3 \times [0,T)R3×[0,T). Fefferman: "(A) and (B) hold ... if the time interval [0,∞)[0,\infty)[0,∞) is replaced by a small time interval [0,T)[0,T)[0,T), with TTT depending on the initial data."
  2. Global existence for small data (NavierStokes.small_data_global_existence_R3): there is an absolute constant c>0c > 0c>0 such that, for n=3n = 3n=3, (A) holds for every admissible u0u^0u0 with
∥u0∥L22 ∥∇u0∥L22≤c ν4.\|u^0\|_{L^2}^2\,\|\nabla u^0\|_{L^2}^2 \le c\,\nu^4.∥u0∥L22​∥∇u0∥L22​≤cν4.

Fefferman: "(A) and (B) hold provided the initial velocity u0u^0u0 satisfies a smallness condition." The scale-invariant product is Leray's form of the condition; it implies smallness of ∥u0∥L3/ν\|u^0\|_{L^3}/\nu∥u0∥L3​/ν, so Kato's theorem also applies. 3. The two-dimensional case (NavierStokes.existence_and_smoothness_R2): statement (A) with n=2n = 2n=2. Fefferman: "In two dimensions, the analogues of assertions (A) and (B) have been known for a long time (Ladyzhenskaya)."

A bridging lemma, NavierStokes.isInitialData_iff_schwartz, identifies the admissible data with the divergence-free elements of Mathlib's Schwartz space.

Significance

The result itself. Statement (A) asks whether the basic model of viscous flow is well posed in the classical sense, i.e. whether smooth finite-energy flows can develop singularities in finite time. A positive answer shows the equations never leave the classical regime; a negative one shows the model predicts its own breakdown. Fefferman: "since we don't even know whether these solutions exist, our understanding is at a very primitive level."

Formalizing it. None of the results in this mission has a machine-checked proof, and Mathlib contains no theory of the Navier–Stokes or Euler equations. The milestones are all proved in the literature; formalizing them requires building, on Mathlib's calculus, measure theory and Schwartz space, the heat semigroup on Rn\mathbb{R}^nRn, the pressure equation Δp=−∑i,j∂i∂j(uiuj)\Delta p = -\sum_{i,j} \partial_i\partial_j(u_i u_j)Δp=−∑i,j​∂i​∂j​(ui​uj​) or the Leray projection, energy estimates, and a fixed-point construction of solutions, most of which is reusable for other evolution equations. The goal is open and expected to remain so; its role is to fix in Lean the exact statement the prize asks for, so partial results are formalized against it.

Difficulty

The energy identity ddt∫∣u∣2=−2ν∫∣∇u∣2\frac{d}{dt}\int|u|^2 = -2\nu\int|\nabla u|^2dtd​∫∣u∣2=−2ν∫∣∇u∣2 controls uuu in L2L^2L2 and ∇u\nabla u∇u in Lt,x2L^2_{t,x}Lt,x2​, but in three dimensions this control is supercritical: under the scaling uλ(x,t)=λu(λx,λ2t)u_\lambda(x,t) = \lambda u(\lambda x, \lambda^2 t)uλ​(x,t)=λu(λx,λ2t) that preserves the equations, the energy of uλu_\lambdauλ​ shrinks as λ→∞\lambda \to \inftyλ→∞, so bounded energy does not prevent concentration at small scales. Every known continuation criterion (Leray, Prodi–Serrin, Beale–Kato–Majda, Escauriaza–Seregin–Šverák) needs a quantity at or above critical scaling, none of which the energy controls. The obvious first idea, an ordinary differential inequality for ∥∇u(t)∥L2\|\nabla u(t)\|_{L^2}∥∇u(t)∥L2​, gives ddt∥∇u∥L22≤Cν−3∥∇u∥L26\frac{d}{dt}\|\nabla u\|_{L^2}^2 \le C\nu^{-3}\|\nabla u\|_{L^2}^6dtd​∥∇u∥L22​≤Cν−3∥∇u∥L26​, which closes only for small data or short time. That is exactly why milestones 1 and 2 are theorems and the goal is not.

The formalization adds a second difficulty: the solutions of the literature live in Sobolev or Besov spaces, with pointwise smoothness of uuu and ppp recovered afterwards by regularity theory, and Mathlib has neither Sobolev spaces on Rn\mathbb{R}^nRn nor the heat semigroup in usable form.

Formalization scope

  • Rn\mathbb{R}^nRn is EuclideanSpace ℝ (Fin n) with Lebesgue measure; the dimension is a parameter, the goal fixes n=3n = 3n=3 and the 2D milestone n=2n = 2n=2.
  • A velocity field is a function of all real times, but every condition is imposed only on the time set SSS; values at negative times are unconstrained.
  • Smoothness on Rn×[0,∞)\mathbb{R}^n \times [0,\infty)Rn×[0,∞) is Mathlib's ContDiffOn of the uncurried map on the closed half-space, i.e. all derivatives extend continuously to t=0t = 0t=0. The momentum equation is imposed at interior times t>0t > 0t>0 with two-sided derivatives; by continuity of the derivatives this is equivalent to Fefferman's "t≥0t \ge 0t≥0".
  • Derivatives are Mathlib's total functions (fderiv, deriv, iteratedFDeriv, gradient, Laplacian) with junk value 000 at non-differentiable points; the smoothness hypotheses make every derivative in the statements honest.
  • The energy is a Lebesgue integral in [0,∞][0,\infty][0,∞], equal to ∞\infty∞ when u(⋅,t)∉L2u(\cdot,t) \notin L^2u(⋅,t)∈/L2, so bounded energy cannot hold vacuously. The L2L^2L2 norms in the small-data hypothesis are Bochner integrals, genuine for Schwartz data.
  • No normalization is imposed on the pressure, as in Fefferman's text.

No trivializing formalization. The zero field solves the equations only for u0=0u^0 = 0u0=0; for any other admissible u0u^0u0 the initial condition, smoothness, the equation on t>0t > 0t>0 and bounded energy must all hold.

Infrastructure needed and welcome contributions. The heat kernel on Rn\mathbb{R}^nRn with Schwartz bounds; the Riesz-transform representation of the pressure or the Leray projection; energy identities for smooth decaying solutions; local existence by Picard iteration; the two-dimensional vorticity equation and its maximum principle. Theorems in the NavierStokes namespace, decompositions of the milestones, and Mathlib lemmas about ContDiffOn on half-spaces are all welcome. Statements (B), (C), (D) and the Euler equations (ν=0\nu = 0ν=0) are out of scope.

Selected references

  • C. L. Fefferman, Existence and smoothness of the Navier–Stokes equation, Clay Mathematics Institute Millennium Prize Problem description, 2000. https://www.claymath.org/wp-content/uploads/2022/06/navierstokes.pdf
  • J. Leray, Sur le mouvement d'un liquide visqueux emplissant l'espace, Acta Mathematica 63 (1934), 193–248. https://doi.org/10.1007/BF02547354
  • O. A. Ladyzhenskaya, The Mathematical Theory of Viscous Incompressible Flow, 2nd ed., Gordon and Breach, 1969. https://archive.org/details/mathematicaltheo0000lady
  • T. Kato, Strong LpL^pLp-solutions of the Navier–Stokes equation in Rm\mathbb{R}^mRm, with applications to weak solutions, Mathematische Zeitschrift 187 (1984), 471–480. https://doi.org/10.1007/BF01174182
  • L. Caffarelli, R. Kohn, L. Nirenberg, Partial regularity of suitable weak solutions of the Navier–Stokes equations, Communications on Pure and Applied Mathematics 35 (1982), 771–831. https://doi.org/10.1002/cpa.3160350604
  • A. J. Majda, A. L. Bertozzi, Vorticity and Incompressible Flow, Cambridge University Press, 2002. https://doi.org/10.1017/CBO9780511613203
  • J. C. Robinson, J. L. Rodrigo, W. Sadowski, The Three-Dimensional Navier–Stokes Equations: Classical Theory, Cambridge University Press, 2016. https://doi.org/10.1017/CBO9781139095143
20 thms4 active usersReviewed
Quantum InformationTheoretical Computer Science·Captain: Goku

Stabilizer Rank of Magic StatesOpen Problem

Motivation

Quantum circuits built from Clifford gates alone are classically simulable in polynomial time. Universality is recovered by adding copies of a magic state, and the fastest known classical simulators of such circuits work by writing the magic-state input as a short linear combination of stabilizer states. The length of the shortest such combination -- the stabilizer rank -- is therefore the exponent governing classical simulation of quantum computation in this model, and lower bounds on it are among the very few unconditional obstructions to classical simulation available at all.

A timeline of what is established for the standard magic state ∣H⟩|H\rangle∣H⟩:

  • 2016. Bravyi, Smith and Smolin exhibit a decomposition giving χ(∣H⊗6⟩)≤7\chi(|H^{\otimes 6}\rangle)\le 7χ(∣H⊗6⟩)≤7, hence χ(∣H⊗n⟩)≤7 n/6≤2 0.468n\chi(|H^{\otimes n}\rangle)\le 7^{\,n/6}\le 2^{\,0.468n}χ(∣H⊗n⟩)≤7n/6≤20.468n, and prove a lower bound of order n\sqrt{n}n​.
  • 2020. Huang, Newman and Szegedy show that hardness assumptions stronger than P≠NP\mathrm{P}\neq\mathrm{NP}P=NP, such as the exponential time hypothesis, imply χ(∣H⊗n⟩)=2Ω(n)\chi(|H^{\otimes n}\rangle)=2^{\Omega(n)}χ(∣H⊗n⟩)=2Ω(n) (arXiv link).
  • 2022. Peleg, Shpilka and Volk improve the unconditional lower bound to Ω(n)\Omega(n)Ω(n) and give the first non-trivial bound for the approximate rank (arXiv:2106.03214).
  • 2024. A quadratic lower bound is obtained for the approximate stabilizer rank (arXiv:2305.10277).

Between the linear unconditional lower bound and the 20.468n2^{0.468n}20.468n upper bound lies the open problem this mission targets.

Setting

Index the computational basis of an nnn-qubit system by bit strings x∈{0,1}nx\in\{0,1\}^nx∈{0,1}n, so a state is a vector ψ∈C2n\psi\in\mathbb{C}^{2^n}ψ∈C2n with coordinates ψ(x)\psi(x)ψ(x).

The Pauli operators are XaZbX^aZ^bXaZb for a,b∈{0,1}na,b\in\{0,1\}^na,b∈{0,1}n, acting by XaZb∣x⟩=(−1) b⋅x∣x⊕a⟩X^aZ^b|x\rangle=(-1)^{\,b\cdot x}|x\oplus a\rangleXaZb∣x⟩=(−1)b⋅x∣x⊕a⟩, where b⋅xb\cdot xb⋅x counts the coordinates on which both are 111 and ⊕\oplus⊕ is bitwise addition; the Pauli group is the set of 4⋅4n4\cdot 4^n4⋅4n operators icXaZbi^cX^aZ^bicXaZb. A unitary UUU is a Clifford unitary when UPU†UPU^\daggerUPU† lies in the Pauli group for every Pauli group element PPP, and a stabilizer state is a vector U∣0⋯0⟩U|0\cdots0\rangleU∣0⋯0⟩ for some Clifford UUU. There are 2n∏k=1n(2k+1)2^n\prod_{k=1}^{n}(2^k+1)2n∏k=1n​(2k+1) of them up to phase -- six for a single qubit.

The stabilizer rank χ(ψ)\chi(\psi)χ(ψ) is the least rrr admitting coefficients c1,…,cr∈Cc_1,\dots,c_r\in\mathbb{C}c1​,…,cr​∈C and stabilizer states φ1,…,φr\varphi_1,\dots,\varphi_rφ1​,…,φr​ with ψ=∑j≤rcjφj\psi=\sum_{j\le r}c_j\varphi_jψ=∑j≤r​cj​φj​.

The magic state is ∣H⟩=cos⁡(π/8)∣0⟩+sin⁡(π/8)∣1⟩|H\rangle=\cos(\pi/8)|0\rangle+\sin(\pi/8)|1\rangle∣H⟩=cos(π/8)∣0⟩+sin(π/8)∣1⟩, and ∣H⊗n⟩|H^{\otimes n}\rangle∣H⊗n⟩ its nnn-fold tensor power, with coordinates cos⁡(π/8) n−∣x∣sin⁡(π/8) ∣x∣\cos(\pi/8)^{\,n-|x|}\sin(\pi/8)^{\,|x|}cos(π/8)n−∣x∣sin(π/8)∣x∣ where ∣x∣|x|∣x∣ is the Hamming weight of xxx.

Target

The goal is a super-polynomial lower bound: for every exponent ddd and constant CCC there exists nnn with

χ(∣H⊗n⟩)  >  C nd,\chi\bigl(|H^{\otimes n}\rangle\bigr)\;>\;C\,n^{d},χ(∣H⊗n⟩)>Cnd,

equivalently, χ(∣H⊗n⟩)\chi(|H^{\otimes n}\rangle)χ(∣H⊗n⟩) is not O(nd)O(n^d)O(nd) for any fixed ddd.

Stronger statements are expected but are deliberately not the goal. An exponential bound χ=2Ω(n)\chi=2^{\Omega(n)}χ=2Ω(n) is believed and follows from hardness assumptions, but a goal naming a specific growth rate would be superseded by the next improvement; super-polynomiality is the weakest statement that settles the question of principle.

Significance

The result itself. A super-polynomial lower bound would unconditionally rule out efficient classical simulation of Clifford-plus-magic-state circuits by stabilizer decomposition, currently the leading such technique. The converse direction shows how much is at stake: a polynomial upper bound on χ(∣H⊗n⟩)\chi(|H^{\otimes n}\rangle)χ(∣H⊗n⟩) would imply BPP=BQP\mathrm{BPP}=\mathrm{BQP}BPP=BQP, and via postselection P=NP\mathrm{P}=\mathrm{NP}P=NP. There is also a purely classical payoff -- improving the known bound even to super-linear would produce a Boolean function computable in polynomial time requiring a super-linear number of summands in any decomposition into exponentials of quadratic forms over F2\mathbb{F}_2F2​, resolving a separate open question.

Formalizing it. The goal is open, so no known proof is being transcribed. What the mission produces is a machine-checked statement of the problem together with formalizations of the established bounds, none of which has a machine-checked proof anywhere. It also produces the first Pauli/Clifford/stabilizer layer in Lean: no existing Lean library contains the nnn-qubit Pauli group, the Clifford group, or stabilizer states, and that layer is reusable for stabilizer error correction, magic monotones, and Clifford simulation generally.

Difficulty

Counting settles the problem for random states: the stabilizer states are too few for short combinations to cover a generic state, so almost every state has exponential stabilizer rank. This says nothing about ∣H⊗n⟩|H^{\otimes n}\rangle∣H⊗n⟩, which is a single explicit, highly structured vector, and the entire difficulty is that lower bounds must be proved for that specific state rather than for a typical one. Every newcomer proposes the counting argument; it does not apply.

The known techniques reduce the question to statements about decompositions of explicit Boolean functions into quadratic-form exponentials, and the barrier is quantitative: the available arguments lose a factor that caps them at linear bounds. The source of the current record documents explicitly why its method cannot pass super-linear, and the fact that going beyond linear would resolve an independent open problem in Boolean function complexity indicates the obstruction is not merely technical.

Formalization scope

State vectors are functions {0,1}n→C\{0,1\}^n\to\mathbb{C}{0,1}n→C and are not required to be normalised; normalisation does not affect the rank, and stabilizer states are unit vectors automatically as Clifford images of ∣0⋯0⟩|0\cdots0\rangle∣0⋯0⟩. The Pauli group is given by the explicit parametrisation icXaZbi^cX^aZ^bicXaZb rather than an abstract presentation, and the Clifford group is characterised as its unitary normaliser, equivalent to the usual generated-by-H,S,CNOTH,S,\mathrm{CNOT}H,S,CNOT description. Because eiθUe^{i\theta}UeiθU normalises the Pauli group whenever UUU does, the stabilizer states are closed under global phase; this is harmless, as the coefficients are arbitrary complex numbers.

One trivialising reading must be excluded. The rank is defined as an infimum over a set of natural numbers, and Lean gives the empty infimum the value 000; if no decomposition existed the rank would be 000 for every state and the goal would be false rather than merely unproved. The milestone χ(ψ)≤2n\chi(\psi)\le 2^nχ(ψ)≤2n is what certifies the set is nonempty, making the rank a genuine minimum, and it should be proved first. Separately, the goal quantifies CCC over all reals including negative values, for which the inequality is trivially satisfiable; the content lies in large positive CCC.

A complete development needs, beyond the published definitions, the correspondence between stabilizer states and affine subspaces carrying quadratic phase functions, on which all known lower-bound arguments rest. Contributions of any milestone are welcome, as are function-level reformulations of the rank and the equivalent characterisation of stabilizer states via maximal abelian Pauli subgroups.

Selected references

  • S. Peleg, A. Shpilka, B. L. Volk, Lower Bounds on Stabilizer Rank, Quantum 6 (2022) 652; arXiv:2106.03214.
  • S. Bravyi, G. Smith, J. Smolin, Trading Classical and Quantum Computational Resources, Phys. Rev. X 6 (2016) 021043; arXiv:1506.01396.
  • C. Huang, M. Newman, M. Szegedy, Explicit Lower Bounds on Strong Quantum Simulation, IEEE Trans. Inf. Theory 66(9) (2020) 5585--5600.
  • Quadratic Lower Bounds on the Approximate Stabilizer Rank: A Probabilistic Approach, STOC 2024; arXiv:2305.10277.
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Differential GeometryGeometry & Topology·Captain: xuanji

Strong Whitney embedding in dimension 2nResearch Paper

Motivation: an intrinsic manifold in a fixed Euclidean space

A smooth manifold is a space that can be described locally by real coordinates, even when no single coordinate chart describes the whole space. Differential geometry works with these local descriptions, whereas an embedding realizes the entire space inside one Euclidean space without losing either its topology or its infinitesimal geometry. The strong Whitney embedding theorem supplies a dimension bound depending only on the dimension of the manifold. This mission targets the precise version selected by LeanEval v1, rather than a substitute formulation.

The benchmark attributes the strong result to Hassler Whitney's 1944 paper and distinguishes it from the earlier bound of 2n+12n+12n+1. The result is a known mathematical theorem; the remaining task here is its formal proof in Lean. The exact benchmark declaration is authoritative for the target and its hypotheses, not a reconstruction from the historical literature (source and attribution).

Setting: topology, smoothness, and the differential

Let nnn be a natural number satisfying 1≤n1\le n1≤n. Let MMM carry a topology and a smooth atlas modeled on Rn\mathbb R^nRn, with the usual model having no boundary. The topology is Hausdorff: distinct points admit disjoint neighborhoods. It is second countable: there is a countable collection of open sets from which every open set can be assembled as a union. These are explicit hypotheses, alongside the chosen charted-space and smooth-manifold structures, in the Lean statement.

A topological embedding is a map that is a homeomorphism onto its image, where the image has the subspace topology inherited from the codomain. An immersion has an injective differential at every point. For a smooth map eee, write dexd e_xdex​ for the induced linear map on tangent spaces at xxx. These are separate requirements: the target asks for global topological embedding and pointwise injectivity of the differential together, as well as infinite differentiability. Their precise Lean meanings are the existing Mathlib predicates used directly by the benchmark, not new mission-specific definitions.

Formalization target: the single root theorem

For every n≥1n\ge1n≥1 and every MMM with the structures and hypotheses just stated, establish

∃e:M⟶R2n,e∈C∞(M,R2n) ∧ e is a topological embedding ∧ ∀x∈M, dex is injective.\exists e:M\longrightarrow\mathbb R^{2n},\qquad e\in C^\infty(M,\mathbb R^{2n}) \ \land\ e\text{ is a topological embedding} \ \land\ \forall x\in M,\ d e_x\text{ is injective}.∃e:M⟶R2n,e∈C∞(M,R2n) ∧ e is a topological embedding ∧ ∀x∈M, dex​ is injective.

The codomain has dimension exactly 2n2n2n. The quantifier ranges over all such manifolds, including noncompact ones. There is exactly one goal theorem and no auxiliary theorem items, definition items, or milestones. The declaration is LeanEval.Geometry.WhitneyEmbeddingProblem.whitney_embedding, with the binders and conclusion preserved from the benchmark source.

Significance: the full theorem rather than an easier restriction

The result realizes the given manifold in a Euclidean space with a uniform dimension bound. Its value in this formulation is the simultaneous control of topology, smoothness, and the differential, without a compactness assumption. Replacing the image-topology condition with mere injectivity would omit part of the requested conclusion; replacing 2n2n2n with an unspecified dimension would omit the quantitative constraint. Both distinctions are explicit in the benchmark's explanation.

A completed formalization would supply a reusable strong embedding theorem on top of Mathlib's manifold language. This is a long-term infrastructure task, not a claim that a short proof is available. The September 5, 2026 LeanEval v1 snapshot supplied for this task records no accepted benchmark credit for this target. That dated benchmark status is not a claim about all formalization projects, and preparing an open theorem statement does not establish the theorem or earn benchmark credit.

Difficulty: the dimension bound and the noncompact scope

The existing compact embedding result discussed by the benchmark provides an embedding into some finite-dimensional Euclidean space. That does not settle the present goal: it assumes compactness and does not supply the 2n2n2n bound. Consequently, simply invoking that result cannot discharge the unrestricted benchmark statement. The source identifies substantial differential-topological infrastructure behind the strong theorem; this proposal does not advertise an easy proof or prescribe a decomposition (benchmark discussion).

All positive dimensions remain in scope, including n=1n=1n=1 and n=2n=2n=2. Noncompactness is not a later extension or optional strengthening. The absence of an assumption must not be replaced by an implicit restriction in a new definition or an easier surrogate theorem.

Formalization scope: unchanged Mathlib predicates

The source model is EuclideanSpace ℝ (Fin n), and the target is EuclideanSpace ℝ (Fin (2 * n)). Smoothness is expressed by ContMDiff (𝓡 n) (𝓡 (2 * n)) ∞ e; the other two conjuncts are IsEmbedding e and pointwise Function.Injective of mfderiv. The type MMM remains universe-polymorphic. No compactness, connectedness, orientability, or nonemptiness hypothesis is added. The empty manifold is included; dimension zero is excluded. Neither properness nor closedness of the image is demanded by the conclusion (exact declaration).

Mathlib already provides the vocabulary needed to state the goal: Euclidean spaces, charts, manifold smoothness, topological embeddings, and manifold derivatives. No custom definition item is necessary. Future proof work may develop reusable infrastructure, but this draft contains only the root theorem and intentionally imposes no supporting targets. A proof must establish that exact statement, not the compact-only, immersion-only, or weak 2n+12n+12n+1 alternative.

Selected references

  • LeanEval contributors, Whitney embedding theorem (strong form, sharp dimension 2n), LeanEval v1 source declaration and manifest, statement revision 1, pinned source and manifest. These specify the exact formal target.
  • H. Whitney, The self-intersections of a smooth n-manifold in 2n-space, Annals of Mathematics (2) 45 (1944), 220–246, DOI. Historical attribution as recorded in the LeanEval manifest; no alternate statement from this reference replaces the benchmark goal.
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Number Theory·Captain: Community (Bot)

The Goldbach ConjectureOpen Problem

Every even integer greater than 222 is the sum of two primes. Christian Goldbach posed it in a 1742 letter to Euler, and it has resisted proof for nearly three centuries while being verified computationally up to 4×10184\times10^{18}4×1018 — making it one of the oldest and most famous open problems in all of mathematics. Its ternary sibling, the weak Goldbach conjecture, was settled by Helfgott in 2013, but the strong form stated here remains wide open: the circle method controls three-prime sums yet loses control at two. This headline mission hosts the conjecture as a machine-checked target for partial results, reductions between its variants, and any future attack.

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Complexity Theory·Captain: marwahaha

Integer multiplication implies finite-precision Fourier boundsTextbook

From a multiplication algorithm to a Fourier algorithm

A faster algorithm for multiplying binary integers is useful beyond integer arithmetic when another problem can be reduced to it without losing the improvement in representation changes or numerical preparation. This mission asks for that connection for the discrete Fourier transform. Its goal is a theorem about actual machines: any correct binary multiplication machine with a runtime bound supplies a Fourier machine with a derived runtime bound and a specified numerical accuracy.

The mathematical route is classical. Bluestein's identity relates Fourier sums to polynomial convolution; Kronecker substitution relates bounded integer convolution to integer multiplication. A finite-precision version joins them. Harvey and van der Hoeven give an explicit multitape formulation, including numerical error, in Sections 2–3.4 of Integer multiplication is at least as hard as matrix transposition. This mission isolates that general transfer and its implementation obligations. It does not concern the paper's subsequent matrix-transposition reduction.

Binary inputs, approximate complex outputs, and machine time

A multitape Turing machine has finitely many states, finitely many tape symbols, and a fixed finite number of tapes. Each transition reads the symbols under its heads, writes symbols, and moves each head by at most one cell. Time is the number of transitions until halting. The shared IntMul.MultitapeTM model fixes a read-only input tape and a separate output tape. An output is required to occupy the complete specified output tape, followed by blanks. The model is already used by integer-multiplication results in the library.

At working precision ppp, a pair of integers (a,c)(a,c)(a,c) represents the complex number 2−p(a+ic)2^{-p}(a+ic)2−p(a+ic). The input coordinates lie in the closed complex unit disc. A numerical output remains a finite list of such pairs; arbitrary exact complex numbers appear only in its mathematical specification. Integers use fixed-width sign-magnitude binary encoding. Natural parameters have self-delimiting binary headers, and array entries occur in their ordinary index order. Reading headers, writing outputs, handling carries, and moving data are all part of the machine's execution.

For n≥1n\ge1n≥1, the ordinary, unnormalised transform is

Dn(X)k=∑j=0n−1e−2πijk/nXj.D_n(X)_k=\sum_{j=0}^{n-1}e^{-2\pi i jk/n}X_j.Dn​(X)k​=j=0∑n−1​e−2πijk/nXj​.

The supporting numerical theorem uses the normalised transform Dn(X)/nD_n(X)/nDn​(X)/n, which maps the unit polydisc into itself. Error is measured in absolute complex norm, or equivalently in units of 2−p2^{-p}2−p when working with fixed-point coordinates.

The complete transfer target

Let MMM be any machine that correctly multiplies two sss-bit integers within T(s)T(s)T(s) transitions for every s≥1s\ge1s≥1. No monotonicity, smoothness, or computability assumption is imposed on the bound TTT. Write ℓ(n)=max⁡(⌈log⁡2n⌉,1)\ell(n)=\max(\lceil\log_2 n\rceil,1)ℓ(n)=max(⌈log2​n⌉,1). For requested accuracy b≥1b\ge1b≥1, use

q=b+3ℓ(n)+5.q=b+3\ell(n)+5.q=b+3ℓ(n)+5.

The main theorem asserts the existence of one Fourier machine and one positive constant CCC, uniform over all lengths, requested accuracies, and admissible input vectors. For a vector encoded at precision qqq, it produces an approximation to the ordinary DFT with coordinatewise error strictly below 2−b2^{-b}2−b, and takes at most

C[T(nq)+nT(q)+qℓ(q)2+nq]C\left[T(nq)+nT(q)+q\ell(q)^2+nq\right]C[T(nq)+nT(q)+qℓ(q)2+nq]

transitions. The root-computation term remains explicit, including when the requested precision is extremely large compared with the transform length. The output magnitude is bounded by nnn, and the output encoding has enough magnitude bits for this growth.

A companion theorem allows the encoded vector itself to approximate an arbitrary complex vector with coordinate error at most δ\deltaδ. Its final error is below nδ+2−bn\delta+2^{-b}nδ+2−b. A substitution theorem replaces TTT by any pointwise upper bound. An asymptotic corollary accepts the library's existing IntMul.MulTimeBound g predicate directly and gives the analogous bound in terms of ggg, once working precision exceeds a fixed threshold.

The source-sized supporting theorem retains two multiplication machines, an auxiliary size parameter m≥npm\ge npm≥np, and the source's precision conditions. Its time is O(T(m)+nT′(p))O(T(m)+nT'(p))O(T(m)+nT′(p)) and its additional normalised error is less than 12n212n^212n2 units of 2−p2^{-p}2−p. The source's arbitrary positive regime constants are represented by positive integer constants; this cofinal family covers every positive real choice. The unrestricted-overhead theorem is an explicitly stated extension obtained by retaining preparation terms instead of absorbing them into the restricted regime.

What completing this mission establishes

The result makes transfer depend on the multiplier's correctness and runtime guarantee, not its internal arithmetic method. A new multiplication theorem can then feed the Fourier theorem through a reusable interface. Input size expansion and lower-order costs remain visible, so an improvement is never claimed by silently identifying a vector length with an integer bit length.

The previous arithmetic-transfer development already has accepted proofs for the chirp identity, explicit arithmetic operation counts, signed packing correctness, and packed operand lengths. Accepted fixed-point rounding and product-error results are also available. Those are supporting results; none alone proves this mission's final machine theorem. The new machine-existence and runtime statements are open formal proof obligations until the verification system accepts their proofs. Compilation of their statements is a separate check.

Why the implementation and numerical obligations matter

Counting an exact complex multiplication as one step cannot establish a bit-runtime bound. Likewise, an abstract function returning a convolution together with a chosen charge does not exhibit a machine that computes it in that time. The final goal therefore has no Fourier-oracle hypothesis, no supplied fast encoder or decoder, and no supplied root table.

The milestone list includes finite-width encoding correctness, fixed-point multiplication as a machine, root approximation, constant-factor operand-size adaptation, and linear-time packing and balanced-digit extraction. It also includes the full convolution and normalised Fourier machine theorems, the explicit-overhead variant, the guard-bit inequality, and the end-to-end consequences. Existing numerical lemmas and Kronecker correctness are referenced rather than duplicated.

Formalization conventions and boundaries

The Lean definitions reuse the published IntMul.MultitapeTM transition semantics and IntMul.HvdH rounding and Kronecker definitions. The new namespace is BitDFT. Transform length, requested accuracy, and arithmetic precision are positive in the machine theorems. Auxiliary encoding functions are total; every theorem using them for numerical data supplies the range conditions that prevent magnitude truncation. The decoding primitive returns a prescribed number of balanced digits; reconstruction is supplied separately by signed Kronecker correctness under its spacing conditions.

The theorem concerns approximate Fourier computation in the binary machine model. It does not claim a matching bound for exact complex arithmetic circuits, nor that preparation is negligible for every multiplier and precision regime. Bounds use actual transition counts with constants chosen before the input parameters. Formalization requires complete implementation proofs, including root construction, and cannot be completed by assuming the desired Fourier machine or its running time.

Selected references

  • David Harvey and Joris van der Hoeven, Integer multiplication is at least as hard as matrix transposition, 2025, Sections 2–3.4, Lemmas 2.1, 2.2 and 3.2, Propositions 3.1 and 3.3. Paper.
  • David Harvey and Joris van der Hoeven, Integer multiplication in time O(n log n), Annals of Mathematics 193 (2021), 563–617. Publication.
  • L. I. Bluestein, A linear filtering approach to the computation of discrete Fourier transform, IEEE Transactions on Audio and Electroacoustics 18 (1970), 451–455. DOI.
  • BitDFT transfer specification, companion Lean development, 24 October 2026. The explicit-overhead and requested-accuracy statements specify the complete transfer assembled from the cited reductions.
35 thms3 active usersReviewed
AlgebraCategory TheoryGroup Theory·Captain: mikedeng1

Strict 2-Groups are Crossed Modules: The 2-Categories of Strict 2-Groups and of Crossed Modules Are 2-EquivalentResearch Paper

Two models of a 2-group

A 2-group is a categorified group: a monoidal category in which every object and every morphism is invertible. When the associativity and unit laws hold as equalities rather than up to isomorphism, the 2-group is called strict. Strict 2-groups appear as the fundamental 2-groups of homotopy 2-types, as symmetry objects of gauge theories with higher form fields, and as automorphism 2-groups of groups and of algebras (Baez–Lauda 2004).

A second, older model is the crossed module, introduced by Whitehead in homotopy theory (Whitehead 1949): a group morphism τ:H→G\tau:H\to Gτ:H→G with an action of GGG on HHH satisfying two compatibility laws. Crossed modules are concrete and easy to compute with, and they classify the same objects. That the two notions agree is folklore; it appears in Mac Lane, Categories for the Working Mathematician, §XII.8 and in Forrester-Barker 2002 at the level of objects. Porst's note (arXiv:0812.1464) writes out the full statement: the two 2-categories, with their morphisms and 2-morphisms, are 2-equivalent. This mission formalizes that statement and its proof structure.

Setting

Strict 2-groups. A strict 2-group G=(G0,G1,s,t,i,∘)\mathcal G=(G_0,G_1,s,t,i,\circ)G=(G0​,G1​,s,t,i,∘) is an internal category in the category of groups: groups G0G_0G0​ (objects) and G1G_1G1​ (morphisms), group morphisms s,t:G1→G0s,t:G_1\to G_0s,t:G1​→G0​ and i:G0→G1i:G_0\to G_1i:G0​→G1​ with s i=t i=ids\,i=t\,i=\mathrm{id}si=ti=id, and a composition a∘ba\circ ba∘b ("aaa after bbb") defined when sa=tbs a=t bsa=tb, which is associative, unital, has s(a∘b)=sbs(a\circ b)=s bs(a∘b)=sb, t(a∘b)=tat(a\circ b)=t at(a∘b)=ta, and is a group morphism on composable pairs (the interchange law (aa′)∘(bb′)=(a∘b)(a′∘b′)(aa')\circ(bb')=(a\circ b)(a'\circ b')(aa′)∘(bb′)=(a∘b)(a′∘b′)).

A morphism (F0,F1)(F_0,F_1)(F0​,F1​) of strict 2-groups is an internal functor: two group morphisms commuting with s,t,i,∘s,t,i,\circs,t,i,∘. A 2-morphism ϑ:F⇒E\vartheta:F\Rightarrow Eϑ:F⇒E is an internal natural transformation: a group morphism ϑ:G0→G1′\vartheta:G_0\to G_1'ϑ:G0​→G1′​ with s′ϑ=F0s'\vartheta=F_0s′ϑ=F0​, t′ϑ=E0t'\vartheta=E_0t′ϑ=E0​ and ϑ(ta)∘′F1a=E1a∘′ϑ(sa)\vartheta(ta)\circ'F_1a=E_1a\circ'\vartheta(sa)ϑ(ta)∘′F1​a=E1​a∘′ϑ(sa). These form the 2-category 2-Grp2\text{-}\mathit{Grp}2-Grp.

Crossed modules. A crossed module χ=(G,H,τ,α)\chi=(G,H,\tau,\alpha)χ=(G,H,τ,α) consists of groups G,HG,HG,H, a group morphism τ:H→G\tau:H\to Gτ:H→G and an action α\alphaα of GGG on HHH by automorphisms, with

τ(α(g,h))=g τ(h) g−1,α(τh,h′)=h h′ h−1(Peiffer identity).\tau(\alpha(g,h))=g\,\tau(h)\,g^{-1},\qquad \alpha(\tau h,h')=h\,h'\,h^{-1}\quad(\text{Peiffer identity}).τ(α(g,h))=gτ(h)g−1,α(τh,h′)=hh′h−1(Peiffer identity).

A morphism (γ,δ)(\gamma,\delta)(γ,δ) is a pair of group morphisms commuting with τ\tauτ and α\alphaα. A 2-morphism η:(γ,δ)⇒(Γ,Δ)\eta:(\gamma,\delta)\Rightarrow(\Gamma,\Delta)η:(γ,δ)⇒(Γ,Δ) is a map η:G→H′\eta:G\to H'η:G→H′ with η(gg~)=ηg α′(γg,ηg~)\eta(g\tilde g)=\eta g\,\alpha'(\gamma g,\eta\tilde g)η(gg~​)=ηgα′(γg,ηg~​), τ′η(g)=Γg (γg)−1\tau'\eta(g)=\Gamma g\,(\gamma g)^{-1}τ′η(g)=Γg(γg)−1 and ητ(h)=Δh (δh)−1\eta\tau(h)=\Delta h\,(\delta h)^{-1}ητ(h)=Δh(δh)−1. These form the 2-category X-ModX\text{-}\mathit{Mod}X-Mod.

The 2-functors. T:2-Grp→X-ModT:2\text{-}\mathit{Grp}\to X\text{-}\mathit{Mod}T:2-Grp→X-Mod sends G\mathcal GG to (G0,ker⁡s,t∣ker⁡s,Ad∘i)(G_0,\ker s,t|_{\ker s},\mathrm{Ad}\circ i)(G0​,kers,t∣kers​,Ad∘i). S:X-Mod→2-GrpS:X\text{-}\mathit{Mod}\to2\text{-}\mathit{Grp}S:X-Mod→2-Grp sends χ\chiχ to (G,H⋊G,s,t,i)(G,H\rtimes G,s,t,i)(G,H⋊G,s,t,i) with s(h,g)=gs(h,g)=gs(h,g)=g, t(h,g)=τh gt(h,g)=\tau h\,gt(h,g)=τhg, i(g)=(e,g)i(g)=(e,g)i(g)=(e,g) and (j,τh g)∘(h,g)=(jh,g)(j,\tau h\,g)\circ(h,g)=(jh,g)(j,τhg)∘(h,g)=(jh,g). The round-trip components are ξG=(id,φ−1)\xi_{\mathcal G}=(\mathrm{id},\varphi^{-1})ξG​=(id,φ−1) with φ−1(h,g)=h ig\varphi^{-1}(h,g)=h\,igφ−1(h,g)=hig, and ζχ=(id,π1∣ker⁡π2)\zeta_\chi=(\mathrm{id},\pi_1|_{\ker\pi_2})ζχ​=(id,π1​∣kerπ2​​).

Formalization targets

Goal: Theorem, §6, p. 16

2-Grp ≃ X-Mod2\text{-}\mathit{Grp}\ \simeq\ X\text{-}\mathit{Mod}2-Grp ≃ X-Mod

Both are 2-categories, and there are 2-functors in both directions with 2-natural isomorphisms from both composites to the identities. The goal is existential in the 2-functors and isomorphisms, as the paper's theorem is; the explicit witnesses are the milestones.

Milestones

  1. §2, Proposition (9): in a strict 2-group, a∘b=a i(sa)−1 ba\circ b=a\,i(sa)^{-1}\,ba∘b=ai(sa)−1b for composable a,ba,ba,b.
  2. §2, Corollary (10): for a∈ker⁡sa\in\ker sa∈kers, a∘b=aba\circ b=aba∘b=ab.
  3. §2, (11): φ:G1→ker⁡s⋊G0\varphi:G_1\to\ker s\rtimes G_0φ:G1​→kers⋊G0​, a↦(a i(sa)−1,sa)a\mapsto(a\,i(sa)^{-1},sa)a↦(ai(sa)−1,sa), is a group isomorphism with inverse (h,g)↦h ig(h,g)\mapsto h\,ig(h,g)↦hig.
  4. §2, p. 7: 2-Grp2\text{-}\mathit{Grp}2-Grp is a 2-category.
  5. §3, p. 10: X-ModX\text{-}\mathit{Mod}X-Mod is a 2-category.
  6. §4: T0GT_0\mathcal GT0​G is a crossed module.
  7. §4: TTT is a 2-functor.
  8. §5: S0χS_0\chiS0​χ is a strict 2-group.
  9. §5: SSS is a 2-functor.
  10. §6: ξ:ST⇒id2-Grp\xi:ST\Rightarrow\mathrm{id}_{2\text{-}\mathit{Grp}}ξ:ST⇒id2-Grp​ is a 2-natural isomorphism.
  11. §6: ζ:TS⇒idX-Mod\zeta:TS\Rightarrow\mathrm{id}_{X\text{-}\mathit{Mod}}ζ:TS⇒idX-Mod​ is a 2-natural isomorphism.

Significance

The 2-equivalence is what makes crossed modules a faithful computational model for strict 2-groups. Morphisms, 2-morphisms, and the classification of strict 2-groups by the invariants π1=coker⁡τ\pi_1=\operatorname{coker}\tauπ1​=cokerτ, π2=ker⁡τ\pi_2=\ker\tauπ2​=kerτ and a class in H3(π1,π2)H^3(\pi_1,\pi_2)H3(π1​,π2​) can all be computed on the crossed-module side, and constructions such as the automorphism 2-group of a group, normal subgroups and central extensions (§7 of the paper) transfer to strict 2-groups through SSS. The 2-categorical statement, rather than the object-level correspondence, is what is needed when 2-morphisms matter, for example for homotopies between maps of 2-types.

The result is classical and is proved in the source; the work here is to formalize it. Mathlib has semidirect products, conjugation actions on normal subgroups and an abstract bicategory library, but no strict 2-groups, no crossed modules and no 2-equivalence between them. One related item is on the platform: a proved theorem that a crossed module yields a strict 2-group on H⋊GH\rtimes GH⋊G, stated for a different definition of strict 2-group that carries an extra arrow-inverse datum. It is referenced; milestone 8 restates it for this mission's definitions.

Difficulty

No single step is deep; the difficulty is the volume of exact bookkeeping. Each 2-category requires closure of lawful cells under three compositions, two unit laws on both levels, two associativity laws and the interchange law. In X-ModX\text{-}\mathit{Mod}X-Mod the interchange law needs the identity Δ′η⋅η′γ=η′Γ⋅δ′η\Delta'\eta\cdot\eta'\gamma=\eta'\Gamma\cdot\delta'\etaΔ′η⋅η′γ=η′Γ⋅δ′η, which uses the Peiffer identity and both chain homotopy conditions. Each 2-functor must preserve vertical and horizontal composition of 2-cells, and the paper leaves some of these checks (horizontal composition for TTT, the interchange law in X-ModX\text{-}\mathit{Mod}X-Mod) to the reader. The groups HHH and G1G_1G1​ are non-abelian, so every factor order must be respected. The 2-cell part of 2-naturality for ξ\xiξ and ζ\zetaζ rests on Proposition (9), which converts compositions into products.

A natural first idea is to instantiate Mathlib's Bicategory for both sides. That places every 2-category law inside a definition, where the platform requires definitions to be free of proofs, and the strict laws would have to be proved before any statement can be written. The mission therefore states the laws as theorems over raw data.

Formalization scope

  • A 2-category is a Raw2Cat: raw data (object, 1-cell and 2-cell types, identities, vertical and horizontal compositions) plus predicates IsOb, Is1, Is2 selecting the lawful cells. IsStrict2Category, IsTwoFunctor and IsTwoNatIso quantify over lawful cells only. 2-cells are typed by their objects, so boundary 1-cells are explicit arguments.
  • All compositions in Raw2Cat are diagrammatic (comp1 f g is "fff, then ggg"). The composition inside a strict 2-group keeps the paper's order (a∘ba\circ ba∘b is "aaa after bbb"). T.comp S is the paper's STSTST.
  • Groups live in one universe. 1-cells of both 2-categories, and 2-cells of 2-Grp2\text{-}\mathit{Grp}2-Grp, are pairs of plain functions or plain functions, with multiplicativity a clause of the lawfulness predicate. The action of a crossed module is a group morphism G →* MulAut H.
  • The composition of a strict 2-group is a total function whose axioms hold on composable pairs; s i=t i=ids\,i=t\,i=\mathrm{id}si=ti=id are structure fields, the rest of the axioms the predicate IsStrictTwoGroup. Equivariance is a field of CrossedModule, the Peiffer identity the predicate IsCrossedModule.
  • T1T_1T1​'s second component is written π1φ′∘f1\pi_1\varphi'\circ f_1π1​φ′∘f1​, which equals f1∣ker⁡sf_1|_{\ker s}f1​∣kers​ on every morphism of strict 2-groups.
  • The paper writes the domain of ξG\xi_{\mathcal G}ξG​ as TSGTS\mathcal GTSG; it is STGST\mathcal GSTG.
  • TwoEquivalent includes the 2-category axioms of both sides, preservation of vertical and horizontal composition of 2-cells by both 2-functors, and the 2-cell part of diagram (7). An equivalence of the underlying 1-categories, or a statement about arbitrary 2-categories with TTT and SSS as hypotheses, does not prove the goal.

Everything is stated over Mathlib alone. The Raw2Cat interface and the definitions of strict 2-groups and crossed modules are reusable for further work on 2-groups, for example the classification by H3H^3H3 or Lie 2-groups. Proofs of any milestone, and of the goal directly, are welcome.

Selected references

  • Sven-S. Porst, Strict 2-Groups are Crossed Modules, preprint, 2008. https://arxiv.org/abs/0812.1464
  • John C. Baez and Aaron D. Lauda, Higher-Dimensional Algebra V: 2-Groups, Theory and Applications of Categories 12 (2004). https://arxiv.org/abs/math/0307200
  • Magnus Forrester-Barker, Group Objects and Internal Categories, preprint, 2002. https://arxiv.org/abs/math/0212065
  • Saunders Mac Lane, Categories for the Working Mathematician, 2nd ed., Springer, 1998, §XII.8. https://doi.org/10.1007/978-1-4757-4721-8
  • J. H. C. Whitehead, Combinatorial homotopy II, Bull. Amer. Math. Soc. 55 (1949). https://doi.org/10.1090/S0002-9904-1949-09213-3
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CombinatoricsGraph TheoryOperations Research+1·Captain: mikedeng1

Edge Dominating Sets in Graphs: The Edge Dominating Set Problem Is NP-Complete for Bipartite Graphs of Maximum Degree 3Research Paper

Motivation

A set FFF of edges of a graph dominates the graph if every other edge shares an endpoint with an edge of FFF. Every maximal matching is an edge dominating set, and conversely a minimum edge dominating set can be turned into a minimal maximal matching of the same size, so the edge dominating set problem is the problem of finding a minimum maximal matching. Yannakakis and Gavril (SIAM J. Appl. Math. 38(3), 1980) list several places where it appears: covering problems for 0-1 matrices, the design of telephone switching networks, and approximation of minimum node covers (§1, p. 364). The paper settles its complexity on restricted graph classes.

The paper proves the problem NP-complete for planar graphs of maximum degree 3 (THEOREM 1) and for bipartite graphs of maximum degree 3 (THEOREM 2). This mission formalizes THEOREM 2, the one the rest of the paper builds on: §3 combines it with a correspondence between edge dominating sets and independent sets of total graphs to obtain COROLLARY 1 (independent set on total graphs of bipartite graphs) and COROLLARY 2 (achromatic number on complements of bipartite graphs).

Setting

Graphs are finite, undirected, without parallel edges or self-loops (p. 364). A graph GGG is bipartite if its vertices can be coloured with two colours so that every edge joins different colours; it has maximum degree 3 if every vertex has at most 3 neighbours.

The edge dominating set problem (pp. 365–366). Input: a graph G=(V,E)G=(V,E)G=(V,E) and a positive integer kkk. Property: GGG has a set F⊆EF\subseteq EF⊆E with ∣F∣≤k|F|\le k∣F∣≤k such that every edge of E∖FE\setminus FE∖F shares a vertex with an edge of FFF. The language EDSbip,3\mathrm{EDS}_{\mathrm{bip},3}EDSbip,3​ is the set of binary codes of pairs (G,k)(G,k)(G,k) with GGG bipartite of maximum degree 3, k≥1k\ge1k≥1, and the property holding.

The SAT-3-restricted problem (p. 365, from Yannakakis [13]). Input: clauses C1,…,CpC_1,\dots,C_pC1​,…,Cp​, each with at most three literals, in which every variable occurs exactly twice positively and exactly once negated. Property: some truth assignment satisfies all clauses. Its language is SAT3R\mathrm{SAT3R}SAT3R.

NP-completeness is Cook's and Karp's notion (p. 365): a language LLL is NP-complete if L∈NPL\in\mathrm{NP}L∈NP and every language in NP reduces to LLL by a polynomial-time many-one reduction.

The construction (pp. 367–368). For a formula with nnn variables, the proof builds a graph GGG with three literal vertices per variable (each with a pendant vertex), three variable-side vertices ai,bi,cia_i,b_i,c_iai​,bi​,ci​, and two vertices dj,dj′d_j,d'_jdj​,dj′​ per clause; it then replaces the clause vertices of degree 4 by copies of a 14-vertex gadget HHH (Fig. 3), obtaining G∗G^*G∗.

Formalization targets

Goal: THEOREM 2

SAT3R is NP-complete ⟹ EDSbip,3 is NP-complete.\mathrm{SAT3R}\ \text{is NP-complete}\ \Longrightarrow\ \mathrm{EDS}_{\mathrm{bip},3}\ \text{is NP-complete}.SAT3R is NP-complete ⟹ EDSbip,3​ is NP-complete.

The hypothesis is the one fact the proof takes from outside the paper (its reference [13]). The conclusion is the full claim: membership in NP and NP-hardness.

Milestones

In the order the proof uses them:

  1. the printed bipartition (S,T)(S,T)(S,T) of GGG;
  2. part (i): a satisfying assignment gives an edge dominating set FFF of GGG with ∣F∣=3n|F|=3n∣F∣=3n;
  3. part (ii), first step: every edge dominating set of GGG has an edge at each of the 3n3n3n literal vertices, so ∣F∣≥3n|F|\ge3n∣F∣≥3n;
  4. part (ii): from an edge dominating set with ∣F∣=3n|F|=3n∣F∣=3n the assignment τ\tauτ read off FFF satisfies all clauses;
  5. GGG has maximum degree 4, attained exactly at djd_jdj​ of all-positive and dj′d'_jdj′​ of all-negated 3-literal clauses;
  6. H−{x,y,z}H-\{x,y,z\}H−{x,y,z} is three uuu–vvv paths of length 4, so HHH needs four of its own edges even when all three attachment edges are in FFF;
  7. four edges of HHH suffice if at least one attachment edge is in FFF;
  8. five edges of HHH are needed if none is;
  9. G∗G^*G∗ is bipartite, has maximum degree 3, and has an edge dominating set with at most 3n+4q3n+4q3n+4q edges iff the formula is satisfiable (qqq the number of replaced clauses);
  10. SAT3R≤pEDSbip,3\mathrm{SAT3R}\le_p\mathrm{EDS}_{\mathrm{bip},3}SAT3R≤p​EDSbip,3​;
  11. EDSbip,3∈NP\mathrm{EDS}_{\mathrm{bip},3}\in\mathrm{NP}EDSbip,3​∈NP.

Significance

The result. THEOREM 2 places minimum maximal matching among the NP-hard problems even for sparse bipartite graphs, where the related maximum matching problem is solvable in polynomial time. It is the starting point of the paper's §3, which transfers hardness to independent sets in total graphs and to the achromatic number of complements of bipartite graphs, and it is the standard citation for the hardness of edge domination in bounded-degree bipartite graphs.

Formalizing it. The result has been known since 1980; no machine-checked proof of it is known to exist. The mission produces a checked reduction on an explicit Turing-machine model, a verified finite gadget, and the correspondence between edge dominating sets of the constructed graph and satisfying assignments. Formalization also brought out two slips in the printed proof (see below), which the milestones state in corrected form.

Difficulty

The combinatorial core, parts (i) and (ii), is a counting argument on GGG. The difficulties lie elsewhere:

  • The gadget substitution is not as printed. The text replaces dj,dj′d_j,d'_jdj​,dj′​ by HHH for every 3-literal clause. A clause with literals of both signs then produces an odd cycle through HHH, so G∗G^*G∗ is not bipartite. Only the clauses with a degree-4 node, those whose three literals have one sign, need replacing, and the threshold of G∗G^*G∗ (3n+4q3n+4q3n+4q) is not printed and must be derived from the gadget's properties.
  • The gadget facts are finite but not small: they quantify over subsets of 18 edges.
  • The machine model. The polynomial-time reduction must decode binary formula codes, build G∗G^*G∗, relabel it onto {0,…,N−1}\{0,\dots,N-1\}{0,…,N−1}, and output an adjacency matrix, all on multi-tape Turing machines with an explicit step bound, and it must send every non-code to a fixed no-instance.

Formalization scope

Formulas, assignments, the formula code and the complexity classes are those of the published CookLevin framework (in which 3-SAT and CLIQUE are already proved NP-complete); graph instances use the published NPGraph code (vertex count and threshold in unary, then the row-major adjacency matrix). Conventions:

  • SAT-3-restricted is read with multiplicity: every clause has at most three literal occurrences, every variable occurring in the formula occurs exactly twice positively and once negated, counted over all clauses. Repeated literals and empty clauses are allowed.
  • "Maximum degree 3" means every degree is at most 3; kkk is at least 1; graphs are simple (symmetric, loop-free adjacency matrix).
  • The NP-completeness of SAT-3-restricted is the goal's hypothesis, not an item. The paper takes it from [13], and it is not on the platform.
  • The vertices of GGG are indexed by literal occurrences, with 0-based clause and position indices. The vertex type of G∗G^*G∗ keeps the deleted clause vertices and an unused copy of HHH per unreplaced clause as isolated vertices.
  • Corrections: the degree-4 nodes are djd_jdj​ of all-positive and dj′d'_jdj′​ of all-negated 3-literal clauses, and HHH replaces only those clauses. The printed text is kept verbatim in the milestones.

Dropping the bipartite or the degree restriction from the target language, assuming NP-hardness of the target, or restricting edge dominating sets to matchings would each give a different and weaker theorem, and none of them is the goal.

THEOREM 1 (planar graphs of maximum degree 3) is not part of this mission: it needs planarity, which has no published substrate. §3 and §4 of the paper (total graphs, trees) are not included either.

Useful contributions: proofs of the gadget facts (finite, possibly by verified enumeration), of parts (i) and (ii), of the G∗G^*G∗ equivalence, and Turing-machine implementations of the reduction and the NP verifier; general lemmas about edge dominating sets and the NPGraph encoding are reusable beyond this mission.

Selected references

  • M. Yannakakis, F. Gavril, Edge dominating sets in graphs, SIAM J. Appl. Math. 38(3) (1980) 364–372. https://doi.org/10.1137/0138030
  • M. Yannakakis, Edge-deletion problems, Tech. Rep. 249, Computer Science Laboratory, Princeton Univ., 1978 (the paper's reference [13], source of the SAT-3-restricted problem; no online copy known).
  • S. A. Cook, The complexity of theorem-proving procedures, Proc. 3rd ACM STOC (1971) 151–158. https://doi.org/10.1145/800157.805047
  • R. M. Karp, Reducibility among combinatorial problems, in Complexity of Computer Computations (1972) 85–104. https://doi.org/10.1007/978-1-4684-2001-2_9
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CombinatoricsComplexity TheoryComputational Complexity·Captain: mikedeng1

Kurodoko is NP-Complete: Deciding the Solvability of Kurodoko Puzzles Is NP-CompleteResearch Paper

Motivation

Kurodoko ("where are the black squares?") is a pen-and-paper logic puzzle published by Nikoli. Its rules are short: colour some squares of a grid black so that the numbered squares stay white, no two black squares touch, the white squares stay connected, and every number counts the white squares it can see along its row and column. The computational complexity of pen-and-paper puzzles is an established topic: surveys such as Demaine and Hearn, Playing Games with Algorithms (2009), list dozens of puzzles whose solvability is NP-complete, and Yato's thesis studies the related problem of finding a second solution. Before Kölker's paper the complexity of Kurodoko was open (§1, p. 694).

J. Kölker, Kurodoko is NP-Complete, J. Inf. Process. 20(3), 694–706 (2012), settles it: deciding whether a Kurodoko instance has a solution is NP-complete. Membership in NP is short (Theorem 2, p. 695). Hardness (Theorem 3, p. 695) is a gadget reduction from one-in-three SAT, the satisfiability variant in which every clause must have exactly one true literal, shown NP-complete by Schaefer, The complexity of satisfiability problems, STOC 1978. The reduction is given twice, in prose (§4) and as a Python program (Appendix A.1), "in order to ensure there is no ambiguity".

Setting

An instance consists of a width www, a height hhh and a list of clues. The board has the squares (r,c)(r,c)(r,c) with row 0≤r<h0\le r<h0≤r<h and column 0≤c<w0\le c<w0≤c<w; two squares are adjacent when ∣r−r′∣+∣c−c′∣=1|r-r'|+|c-c'|=1∣r−r′∣+∣c−c′∣=1. A clue (r,c,n)(r,c,n)(r,c,n) puts the number nnn on the square (r,c)(r,c)(r,c); the clue squares form the set CCC, and the values form a function N:C→{1,…,w+h−1}N:C\to\{1,\dots,w+h-1\}N:C→{1,…,w+h−1}.

A solution is a set BBB of board squares (the black squares; the rest, WWW, are white) such that

  1. every clue square is white, B∩C=∅B\cap C=\emptysetB∩C=∅;
  2. no two black squares are adjacent;
  3. any two white squares are joined by a path of adjacent white squares;
  4. every clue square vvv touches exactly N(v)N(v)N(v) squares, where vvv touches the squares uuu in its own row or column such that all squares from vvv to uuu inclusive are white. For a white vvv this count is hz+vt−1\mathrm{hz}+\mathrm{vt}-1hz+vt−1, the lengths of its maximal horizontal and vertical white runs, minus one for vvv itself.

The Kurodoko Decision Problem asks whether a given instance has a solution. The input writes www and hhh in binary and lists the clue squares and their values, so the board can have exponentially many squares in the input length. In the Lean development, kurodokoLang is the set of binary codes of well-formed solvable instances.

A one-in-three SAT instance is a formula FFF: a list of clauses, each of three literals xxx or ¬x\neg x¬x. A one-in-three assignment makes exactly one literal occurrence of every clause true. oneInThreeLang is the set of codes of formulas that have one.

Formalization targets

Goal: NP-completeness

1in3SAT NP-complete ⟹ Kurodoko NP-complete.\mathsf{1in3SAT}\ \text{NP-complete}\ \Longrightarrow\ \mathsf{Kurodoko}\ \text{NP-complete}.1in3SAT NP-complete ⟹ Kurodoko NP-complete.

NP-completeness is the platform's CookPvsNP.NPComplete: membership in NP\mathbf{NP}NP, and a polynomial-time many-one reduction from every NP\mathbf{NP}NP language. The NP-completeness of one-in-three SAT is the only fact the paper imports, and it is the hypothesis.

The two halves

Kurodoko∈NP(Theorem 2),L′∈NP ⟹ L′≤pKurodoko(Theorem 3).\mathsf{Kurodoko}\in\mathbf{NP}\qquad\text{(Theorem 2)},\qquad\qquad L'\in\mathbf{NP}\ \Longrightarrow\ L'\le_p\mathsf{Kurodoko}\qquad\text{(Theorem 3)}.Kurodoko∈NP(Theorem 2),L′∈NP ⟹ L′≤p​Kurodoko(Theorem 3).

The reduction

For the board K(F)K(F)K(F) that the reduction assembles from a formula FFF:

K(F) solvable ⟹ F has a one-in-three assignment(Theorem 4),K(F)\ \text{solvable}\ \Longrightarrow\ F\ \text{has a one-in-three assignment}\qquad\text{(Theorem 4)},K(F) solvable ⟹ F has a one-in-three assignment(Theorem 4), F has a one-in-three assignment ⟹ K(F) solvable(Theorem 5),F\ \text{has a one-in-three assignment}\ \Longrightarrow\ K(F)\ \text{solvable}\qquad\text{(Theorem 5)},F has a one-in-three assignment ⟹ K(F) solvable(Theorem 5),

and the word map is polynomial-time computable with s∈1in3SAT  ⟺  f(s)∈Kurodokos\in\mathsf{1in3SAT}\iff f(s)\in\mathsf{Kurodoko}s∈1in3SAT⟺f(s)∈Kurodoko.

Supporting milestones

  • the compression step of Theorem 2: merging two adjacent black-free rows (or columns) preserves rule 3, and afterwards w,h≤2∣B∣+1w,h\le 2|B|+1w,h≤2∣B∣+1;
  • Lemma 1: every ? square of the assembled board lies on a ray;
  • the gadget claim of §4.1: in every solution of K(F)K(F)K(F) each placed gadget obeys its relation on its port squares (for example no=sin_o=s_ino​=si​ for a Wire, wi+si+ei=1w_i+s_i+e_i=1wi​+si​+ei​=1 for a Choice).

Significance

The result. Kurodoko joins the family of Nikoli puzzles known to be NP-complete. It follows that no polynomial-time solver exists unless P=NP\mathbf P=\mathbf{NP}P=NP, and that the puzzle can encode any problem in NP\mathbf{NP}NP. Every number in the produced instance is linear in the size of the formula, so the problem is strongly NP-complete (§6, p. 700).

Formalizing it. The paper's result is proved on paper but not machine-checked. Its correctness rests on nine hand-designed 17×1717\times1717×17 gadgets and on deductions "by inspection" (Appendix A.2), which are exactly the steps a formal proof makes checkable. The formalization has already found two slips in the printed program: occurrences keyed by the signed literal (which crashes on any negated literal), and a mirrored Sidesplit, under which the unsatisfiable clause (x,x,x)(x,x,x)(x,x,x) produces a solvable board. The mission states the corrected reduction. The platform has the complexity layer CookPvsNP_defs, binary codes and several NP-completeness results, but no puzzle, no grid-colouring problem and no one-in-three SAT.

Difficulty

Membership in NP is not immediate, because www and hhh are binary: a witness BBB is short, but checking rule 3 by searching the board takes exponential time. The checker must first compress runs of black-free rows and columns, and the compressed board must be shown to have the same connectivity.

Hardness is a concrete construction of tens of thousands of squares. Theorem 4 needs every gadget to behave as specified in every solution of the whole board, not only in isolation. The ? clues take values that depend on the global layout through rays crossing several gadgets (Lemma 1), and their correctness depends on the overlap structure of neighbouring gadgets. Theorem 5 needs an explicit global solution and a proof that its white squares are connected across the whole board. A per-gadget check on a computer does not settle either direction, because the board grows with the formula. Polynomial-time computability on one-tape Turing machines is a separate, bookkeeping-heavy obligation.

Formalization scope

  • Model. Squares are pairs (r, c) : ℕ × ℕ, row first; B : Finset (ℕ × ℕ) lies on the board. Rule 3 is read as preconnectedness: any two white squares are joined by a chain of adjacent white squares, which holds vacuously when there is no white square. Rule 4 is touchCount, which counts the clue square once. Well-formedness (clues on the board, pairwise distinct, values in {1,…,w+h−1}\{1,\dots,w+h-1\}{1,…,w+h−1}) is part of the language.
  • Codes. Instances are written over the published BSym alphabet with encNats as w,h,r1,c1,n1,…w,h,r_1,c_1,n_1,\dotsw,h,r1​,c1​,n1​,…, all in binary. Formulas use the published CNF and encodeCNF.
  • One-in-three SAT. Every clause has exactly three literals; negations and repeated variables are allowed, and "exactly one" counts literal occurrences, matching the one wire per occurrence of the reduction. Its NP-completeness is a hypothesis of the goal and of Theorem 3.
  • The reduction transcribes Appendix A.1 string by string and function by function, with two corrections: occurrences are keyed by the variable, and tee_l = rotate ltee. The empty formula goes to the solvable instance (1,1,[])(1,1,[])(1,1,[]), and a word that is not the code of a three-literal formula goes to the code of a fixed unsolvable instance. The Lean reduction's clue lists coincide with the corrected Python program's on the tested formulas.
  • Ruled out. The goal is not "Theorem 4 ∧ Theorem 5": that drops NP membership and polynomial time. The reduction milestone names the paper's map rather than a bare PolyReducible.
  • Not formalized. Theorem 1 (an observation about the clue 1) and the remarks of §6.
  • Reusable. The Kurodoko language and one-in-three SAT over the CookPvsNP layer. A proof of one-in-three SAT's NP-completeness in that framework, or of Cook's theorem (CookPvsNP.SAT_npComplete, open), would discharge the hypothesis. Contributions to the polynomial-time bookkeeping and to the gadget deductions are welcome.

Selected references

  • J. Kölker, Kurodoko is NP-Complete, Journal of Information Processing 20(3), 694–706, 2012. https://doi.org/10.2197/ipsjjip.20.694
  • T. J. Schaefer, The complexity of satisfiability problems, Proc. 10th Annual ACM Symposium on Theory of Computing, 216–226, 1978. https://doi.org/10.1145/800133.804350
  • E. D. Demaine and R. A. Hearn, Playing Games with Algorithms: Algorithmic Combinatorial Game Theory, in Games of No Chance 3, MSRI Publications 56, Cambridge University Press, 3–56, 2009. https://arxiv.org/abs/cs/0106019
  • S. A. Cook, The P versus NP problem, Clay Mathematics Institute Millennium Problems, 2000. https://www.claymath.org/wp-content/uploads/2022/06/pvsnp.pdf
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Mathematical PhysicsQuantum Information·Captain: mikedeng1

Asymmetric Quantum Cloning Machines in Any Dimension: The Tight No-Cloning Inequality for Isotropic ClonersResearch Paper

Motivation

The no-cloning theorem says that no physical process turns an unknown quantum state ∣ψ⟩|\psi\rangle∣ψ⟩ into two copies ∣ψ⟩∣ψ⟩|\psi\rangle|\psi\rangle∣ψ⟩∣ψ⟩. Once perfect copies are excluded, the quantitative question is how good two imperfect copies can be, and how the quality of one copy trades off against the quality of the other. The answer bounds what an eavesdropper on a quantum key distribution channel can learn while disturbing the legitimate signal, and it quantifies how much quantum information can be spread over two systems.

N. J. Cerf, in Asymmetric quantum cloning machines in any dimension (arXiv:quant-ph/9805024, J. Mod. Opt. 47, 187 (2000)), answers this for cloners of an NNN-level system whose two copies are degraded uniformly in every direction. The answer is a single inequality between the two noise levels, Eq. (1.1) on p. 2, restated as Eq. (3.21) on p. 15.

Timeline.

  • 1982: Wootters–Zurek and Dieks prove the no-cloning theorem.
  • 1996: Bužek and Hillery construct the symmetric universal qubit cloner (PRA 54, 1844).
  • 1998: Werner proves optimality of the symmetric NNN-level cloner for many copies (PRA 58, 1827).
  • 1998: Cerf introduces the asymmetric Pauli cloners for qubits and, in the paper of this mission, the asymmetric Heisenberg cloners for NNN-level systems, together with the no-cloning inequality.
  • 2005: Iblisdir, Acín, Cerf, Filip, Fiurášek and Gisin treat multipartite asymmetric cloning (PRA 72, 042328).
  • 2017: Hashagen revisits the optimality of asymmetric universal cloning (QIC 17, 747).

Setting

Fix an integer N≥2N \ge 2N≥2 and an NNN-level system with basis ∣0⟩,…,∣N−1⟩|0\rangle, \dots, |N-1\rangle∣0⟩,…,∣N−1⟩; labels are taken modulo NNN. A quantum channel is a completely positive trace-preserving linear map between operator spaces. In finite dimension it is the same as a map ρ↦∑iKiρKi†\rho \mapsto \sum_i K_i \rho K_i^\daggerρ↦∑i​Ki​ρKi†​ given by finitely many matrices KiK_iKi​ with ∑iKi†Ki=1\sum_i K_i^\dagger K_i = \mathbb 1∑i​Ki†​Ki​=1.

The depolarizing channel with fraction π\piπ is

Dπ(ρ)=πN(Tr⁡ρ) 1+(1−π) ρ:\mathcal D_\pi(\rho) = \frac{\pi}{N}(\operatorname{Tr}\rho)\,\mathbb 1 + (1-\pi)\,\rho :Dπ​(ρ)=Nπ​(Trρ)1+(1−π)ρ:

the input is replaced by the maximally mixed state with probability π\piπ and left unchanged otherwise.

A 1→21 \to 21→2 cloner is a channel TTT from an NNN-level input to two NNN-level outputs AAA and BBB. Its copies are the output channels ρ↦Tr⁡BT(ρ)\rho \mapsto \operatorname{Tr}_B T(\rho)ρ↦TrB​T(ρ) and ρ↦Tr⁡AT(ρ)\rho \mapsto \operatorname{Tr}_A T(\rho)ρ↦TrA​T(ρ). The cloner is isotropic with depolarizing fractions πa,πb\pi_a, \pi_bπa​,πb​ if

Tr⁡BT(ρ)=Dπa(ρ),Tr⁡AT(ρ)=Dπb(ρ)for every ρ.\operatorname{Tr}_B T(\rho) = \mathcal D_{\pi_a}(\rho), \qquad \operatorname{Tr}_A T(\rho) = \mathcal D_{\pi_b}(\rho) \quad \text{for every } \rho .TrB​T(ρ)=Dπa​​(ρ),TrA​T(ρ)=Dπb​​(ρ)for every ρ.

The paper writes πa=a2\pi_a = a^2πa​=a2 and πb=b2\pi_b = b^2πb​=b2 with a,b≥0a, b \ge 0a,b≥0.

The paper's construction uses the following objects, defined in the mission's definition file:

  • the N2N^2N2 maximally entangled states ∣ψm,n⟩=N−1/2∑je2πi jn/N∣j⟩∣j+m⟩|\psi_{m,n}\rangle = N^{-1/2}\sum_j e^{2\pi i\, jn/N}|j\rangle|j+m\rangle∣ψm,n​⟩=N−1/2∑j​e2πijn/N∣j⟩∣j+m⟩ (Eq. (3.1));
  • the error operators Um,n=∑ke2πi kn/N∣k+m⟩⟨k∣U_{m,n} = \sum_k e^{2\pi i\, kn/N}|k+m\rangle\langle k|Um,n​=∑k​e2πikn/N∣k+m⟩⟨k∣ (Eq. (3.5));
  • the Heisenberg channels ρ↦∑m,npm,nUm,nρUm,n†\rho \mapsto \sum_{m,n} p_{m,n} U_{m,n}\rho U_{m,n}^\daggerρ↦∑m,n​pm,n​Um,n​ρUm,n†​;
  • the four-system double-ME states ∣Ψ⟩=∑m,nαm,n∣ψm,n⟩RA∣ψm,N−n⟩BC|\Psi\rangle = \sum_{m,n}\alpha_{m,n}|\psi_{m,n}\rangle_{RA}|\psi_{m,N-n}\rangle_{BC}∣Ψ⟩=∑m,n​αm,n​∣ψm,n​⟩RA​∣ψm,N−n​⟩BC​ (Eq. (3.8)), which describe the Heisenberg cloning machines (HCMs);
  • the dual amplitudes βm,n=1N∑x,ye2πi(nx−my)/Nαx,y\beta_{m,n} = \frac1N\sum_{x,y}e^{2\pi i(nx-my)/N}\alpha_{x,y}βm,n​=N1​∑x,y​e2πi(nx−my)/Nαx,y​ (Eq. (3.11));
  • the isotropic ansatz αm,n=a^ δm,0δn,0+a/N\alpha_{m,n} = \hat a\,\delta_{m,0}\delta_{n,0} + a/Nαm,n​=a^δm,0​δn,0​+a/N (Eq. (3.16)).

Formalization targets

Goal: the tight no-cloning inequality (Eq. (1.1) = (3.21))

For N≥2N \ge 2N≥2:

(i)T isotropic with fractions πa,πb  ⟹  πa+2Nπaπb+πb≥1,\text{(i)}\quad T \text{ isotropic with fractions } \pi_a, \pi_b \;\Longrightarrow\; \pi_a + \frac{2}{N}\sqrt{\pi_a}\sqrt{\pi_b} + \pi_b \ge 1 ,(i)T isotropic with fractions πa​,πb​⟹πa​+N2​πa​​πb​​+πb​≥1, (ii)πa,πb≥0,  πa+2Nπaπb+πb=1  ⟹  ∃ T isotropic with fractions πa,πb.\text{(ii)}\quad \pi_a, \pi_b \ge 0,\ \ \pi_a + \frac{2}{N}\sqrt{\pi_a}\sqrt{\pi_b} + \pi_b = 1 \;\Longrightarrow\; \exists\, T \text{ isotropic with fractions } \pi_a, \pi_b .(ii)πa​,πb​≥0,  πa​+N2​πa​​πb​​+πb​=1⟹∃T isotropic with fractions πa​,πb​.

Clause (i) says that the region inside the ellipse a2+2Nab+b2=1a^2 + \frac2N ab + b^2 = 1a2+N2​ab+b2=1 is forbidden. Clause (ii) is the paper's statement that the inequality is tight and saturated by HCMs.

Milestones (Eqs. (3.3)–(3.19))

The milestones are the identities of §III A–C that the paper's argument rests on:

  • the orthonormal basis of maximally entangled states (3.3) and its relation to the error operators (3.7);
  • the joint state of a Heisenberg channel with a maximally entangled reference (3.6);
  • the two reduced states of a double-ME state, (3.9) and (3.12), and the Fourier relation between them, (3.10)–(3.11);
  • for the isotropic ansatz: the normalization (3.17), the reduced state (3.18), its reading as a depolarizing channel, and the self-duality (3.19).

Significance

The inequality is a complementarity relation between two copies: if one copy is nearly perfect (πa→0\pi_a \to 0πa​→0), the other is nearly fully depolarized (πb→1\pi_b \to 1πb​→1). Its symmetric point πa=πb=N/(2(N+1))\pi_a = \pi_b = N/(2(N+1))πa​=πb​=N/(2(N+1)) is the optimal universal symmetric cloner. As N→∞N \to \inftyN→∞ the ellipse tends to the line πa+πb=1\pi_a + \pi_b = 1πa​+πb​=1, the classical trade-off of sending the input to one output or the other. For N=2N = 2N=2 it is the qubit no-cloning inequality of the paper's §II, Eq. (2.31).

The paper derives the inequality inside the family of Heisenberg cloners, under the conjecture (p. 13) that an NNN-dimensional ancilla suffices, but states it for all isotropic cloners. Later work, for example Hashagen (2017), studies optimality over general cloners by other methods. To our knowledge none of these results has been machine-checked. The mission states the claim for every channel with depolarizing outputs, and a complete development yields a verified Bell-basis and Weyl-operator layer for qudits.

Difficulty

Clause (ii) is a construction: an explicit HCM, checked through the milestones. Clause (i) is harder. The paper's derivation only shows that HCMs with isotropic amplitudes lie on the ellipse (3.20) and then minimizes over phases. That argument does not bound cloners outside the Heisenberg family: a general channel to A⊗BA \otimes BA⊗B need not have a Heisenberg-covariant dilation, and its ancilla can be larger than NNN. So clause (i) cannot be obtained by reading the inequality off the HCM parametrization. It requires an argument valid for every completely positive map with the prescribed marginals.

Formalization scope

  • A cloner is T : QAlgorithms.Superop (Fin N) (Fin N × Fin N) with QAlgorithms.IsChannel T, a finite normalized Kraus family. The first factor of the output is AAA.
  • Copies are WildeQIT.partialTraceRight (output AAA) and partialTraceLeft (output BBB). The depolarizing channel is the published QAlgorithms.QuditFidelity.depolarizingMap.
  • The marginal conditions are imposed on every matrix, which for a linear map is equivalent to imposing them on density matrices.
  • Labels modulo NNN are Fin N arithmetic. In two-register objects the reference RRR is the first factor, matching QAlgorithms.idTensorSuperop. Four-register vectors are functions on ((R,A),(B,C))((R,A),(B,C))((R,A),(B,C)).
  • The goal assumes 2≤N2 \le N2≤N. At N=1N = 1N=1 every fraction gives the identity map, and clause (i) fails.
  • No sign condition is placed on πa,πb\pi_a, \pi_bπa​,πb​ in clause (i), because complete positivity forces them to be nonnegative.
  • The milestones hold for every N≥1N \ge 1N≥1 and every amplitude array. Normalization is not assumed.

Clause (i) quantifies over all channels with depolarizing outputs. A version quantified only over HCMs built from (3.8) and (3.16) reduces to Re(ab∗)≤∣a∣∣b∣\mathrm{Re}(ab^*) \le |a||b|Re(ab∗)≤∣a∣∣b∣ and is not the paper's claim.

The reusable parts are the Bell-basis identities (3.3), (3.7) and (3.6), the partial-trace computations (3.9) and (3.12), and the Fourier identity (3.10). Contributions are welcome in three places: proofs of the milestones; a lemma that a four-partite pure state with maximally mixed reference marginal defines a channel whose joint states are ρRA\rho_{RA}ρRA​ and ρRB\rho_{RB}ρRB​, used for clause (ii); and a proof of clause (i) over arbitrary channels, for example through Choi matrices and a positivity argument.

Selected references

  • N. J. Cerf, Asymmetric quantum cloning machines in any dimension, arXiv:quant-ph/9805024v2 (1998); J. Mod. Opt. 47, 187 (2000). https://arxiv.org/abs/quant-ph/9805024
  • N. J. Cerf, Pauli cloning of a quantum bit, Phys. Rev. Lett. 84, 4497 (2000). https://doi.org/10.1103/PhysRevLett.84.4497
  • V. Bužek, M. Hillery, Quantum copying: beyond the no-cloning theorem, Phys. Rev. A 54, 1844 (1996). https://doi.org/10.1103/PhysRevA.54.1844
  • R. F. Werner, Optimal cloning of pure states, Phys. Rev. A 58, 1827 (1998). https://doi.org/10.1103/PhysRevA.58.1827
  • S. Iblisdir, A. Acín, N. J. Cerf, R. Filip, J. Fiurášek, N. Gisin, Multipartite asymmetric quantum cloning, Phys. Rev. A 72, 042328 (2005). https://doi.org/10.1103/PhysRevA.72.042328
  • A. K. Hashagen, Universal asymmetric quantum cloning revisited, Quantum Inf. Comput. 17, 747 (2017). https://arxiv.org/abs/1609.01974
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Mathematical PhysicsQuantum Information·Captain: mikedeng1

Entangling operations and their implementation using a small amount of entanglement: The Gate exp(−i(π/2^N)σx⊗σx) Is Implemented with Unit Probability Using α_N f_N < 5.97932·α_N Ebits on AverageResearch Paper

Motivation

A two-qubit gate whose qubits sit in different laboratories cannot be applied by local operations and classical communication (LOCC) alone: it can create entanglement, so it must consume some. The basic question of distributed quantum computation is how much. The textbook answer, teleporting one qubit to the other side, applying the gate and teleporting back, costs two ebits (maximally entangled pairs) whatever the gate. For gates close to the identity this is wasteful: a gate that can only create a small amount of entanglement should not need two ebits to implement.

J. I. Cirac, W. Dür, B. Kraus and M. Lewenstein (arXiv:quant-ph/0007057v1, published as Phys. Rev. Lett. 86, 544 (2001)) answered this for the family of phase gates U(α)=e−iα σx⊗σxU(\alpha)=e^{-i\alpha\,\sigma_x\otimes\sigma_x}U(α)=e−iασx​⊗σx​ with binary phases αN=π/2N\alpha_N=\pi/2^NαN​=π/2N, the gates of the quantum Fourier transform. Their protocol implements U(αN)U(\alpha_N)U(αN​) exactly, with probability one, using on average an amount of entanglement proportional to αN\alpha_NαN​ and about two classical bits in each direction. Shortly before, Eisert, Jacobs, Papadopoulos and Plenio had shown that one ebit and two classical bits suffice for a controlled-NOT (arXiv:quant-ph/0005101); Cirac et al. showed that the cost can go to zero with the gate's phase.

Setting

Six quantum systems are involved: A1,A2,A3A_1,A_2,A_3A1​,A2​,A3​ on Alice's side and B1,B2,B3B_1,B_2,B_3B1​,B2​,B3​ on Bob's, each of dimension ddd with computational basis {∣i⟩}\{|i\rangle\}{∣i⟩}. Let ∣Φ⟩=d−1/2∑i∣i⟩∣i⟩|\Phi\rangle=d^{-1/2}\sum_i|i\rangle|i\rangle∣Φ⟩=d−1/2∑i​∣i⟩∣i⟩ and P=∣Φ⟩⟨Φ∣P=|\Phi\rangle\langle\Phi|P=∣Φ⟩⟨Φ∣. A completely positive map E(ρ)=∑kOkρOk†\mathcal E(\rho)=\sum_kO_k\rho O_k^\daggerE(ρ)=∑k​Ok​ρOk†​ on A1B1A_1B_1A1​B1​ has the operator

EA1A2,B1B2=E(PA1A2⊗PB1B2),E_{A_1A_2,B_1B_2}=\mathcal E(P_{A_1A_2}\otimes P_{B_1B_2}),EA1​A2​,B1​B2​​=E(PA1​A2​​⊗PB1​B2​​),

E\mathcal EE acting as the identity on A2B2A_2B_2A2​B2​. The map is recovered from EEE by a joint projection of A2A3A_2A_3A2​A3​ and B2B3B_2B_3B2​B3​ onto ∣Φ⟩|\Phi\rangle∣Φ⟩: E(ρ)=d4tr⁡A2A3B2B3(E ρA3B3PA2A3PB2B3)\mathcal E(\rho)=d^4\operatorname{tr}_{A_2A_3B_2B_3}(E\,\rho_{A_3B_3}P_{A_2A_3}P_{B_2B_3})E(ρ)=d4trA2​A3​B2​B3​​(EρA3​B3​​PA2​A3​​PB2​B3​​).

From now on d=2d=2d=2. Let σx,σy,σz\sigma_x,\sigma_y,\sigma_zσx​,σy​,σz​ be the Pauli matrices, αN=π/2N\alpha_N=\pi/2^NαN​=π/2N and U(α)=e−iα σxA1⊗σxB1U(\alpha)=e^{-i\alpha\,\sigma_x^{A_1}\otimes\sigma_x^{B_1}}U(α)=e−iασxA1​​⊗σxB1​​. The resource state is

∣ψβ⟩=cos⁡β ∣Φ+⟩A1A2∣Φ+⟩B1B2−isin⁡β ∣Ψ+⟩A1A2∣Ψ+⟩B1B2,|\psi_\beta\rangle=\cos\beta\,|\Phi^+\rangle_{A_1A_2}|\Phi^+\rangle_{B_1B_2}-i\sin\beta\,|\Psi^+\rangle_{A_1A_2}|\Psi^+\rangle_{B_1B_2},∣ψβ​⟩=cosβ∣Φ+⟩A1​A2​​∣Φ+⟩B1​B2​​−isinβ∣Ψ+⟩A1​A2​​∣Ψ+⟩B1​B2​​,

with ∣Φ+⟩=(∣00⟩+∣11⟩)/2|\Phi^+\rangle=(|00\rangle+|11\rangle)/\sqrt2∣Φ+⟩=(∣00⟩+∣11⟩)/2​, ∣Ψ+⟩=(∣01⟩+∣10⟩)/2|\Psi^+\rangle=(|01\rangle+|10\rangle)/\sqrt2∣Ψ+⟩=(∣01⟩+∣10⟩)/2​; it is the operator of U(β)U(\beta)U(β) written as a state. Its entropy of entanglement E(ψβ)E(\psi_\beta)E(ψβ​) is the von Neumann entropy, in bits, of its marginal on A1A2A_1A_2A1​A2​.

One step with resource ∣ψβ⟩|\psi_\beta\rangle∣ψβ​⟩: Alice measures A2A3A_2A_3A2​A3​ and Bob measures B2B3B_2B_3B2​B3​ in the Bell basis ∣Ψi1,i2⟩=(1⊗σi1,i2)∣Φ⟩|\Psi_{i_1,i_2}\rangle=(\mathbb 1\otimes\sigma_{i_1,i_2})|\Phi\rangle∣Ψi1​,i2​​⟩=(1⊗σi1​,i2​​)∣Φ⟩, with σ1,1=1\sigma_{1,1}=\mathbb 1σ1,1​=1, σ1,2=σx\sigma_{1,2}=\sigma_xσ1,2​=σx​, σ2,1=σy\sigma_{2,1}=\sigma_yσ2,1​=σy​, σ2,2=σz\sigma_{2,2}=\sigma_zσ2,2​=σz​, and each applies the Pauli operator of the outcome to A1A_1A1​ or B1B_1B1​. The step succeeds when i1=j1i_1=j_1i1​=j1​. The protocol for U(αN)U(\alpha_N)U(αN​) acts on an input on A3B3A_3B_3A3​B3​ and leaves the output on A1B1A_1B_1A1​B1​: step kkk uses ∣ψ2k−1αN⟩|\psi_{2^{k-1}\alpha_N}\rangle∣ψ2k−1αN​​⟩, and the protocol stops at the first success or after step NNN. With pkp_kpk​ the probability that step kkk is performed, the average entanglement consumed is Eˉ[U(αN)]=∑kpk E(ψ2k−1αN)\bar E[U(\alpha_N)]=\sum_kp_k\,E(\psi_{2^{k-1}\alpha_N})Eˉ[U(αN​)]=∑k​pk​E(ψ2k−1αN​​).

Formalization targets

Goal: unit probability at cost αNfN\alpha_Nf_NαN​fN​

For every N≥1N\ge1N≥1:

  1. every terminal branch of the protocol applies U(αN)U(\alpha_N)U(αN​) up to a scalar, and the branch operators KlK_lKl​ satisfy ∑lKl†Kl=1\sum_lK_l^\dagger K_l=\mathbb 1∑l​Kl†​Kl​=1;
  2. on every input state, step kkk is performed with probability (1/2)k−1(1/2)^{k-1}(1/2)k−1, and
Eˉ[U(αN)]=αNfN,fN=1π∑k=1N2kE(ψαk);\bar E[U(\alpha_N)]=\alpha_Nf_N,\qquad f_N=\frac1\pi\sum_{k=1}^N2^kE(\psi_{\alpha_k});Eˉ[U(αN​)]=αN​fN​,fN​=π1​k=1∑N​2kE(ψαk​​);
  1. the average classical communication in each direction is 2−(1/2)N−22-(1/2)^{N-2}2−(1/2)N−2 bits;
  2. fN<f∞=1π∑k≥12kE(ψαk)f_N<f_\infty=\frac1\pi\sum_{k\ge1}2^kE(\psi_{\alpha_k})fN​<f∞​=π1​∑k≥1​2kE(ψαk​​), the series converges, and
5.97931<f∞<5.97932.5.97931<f_\infty<5.97932.5.97931<f∞​<5.97932.

Milestones

In the order of the paper: the transpose identity (7) and the reconstruction (6)/(8) for general ddd; the operator of U(α)U(\alpha)U(α) (10); the step-outcome rule (each outcome has probability 1/161/161/16; the step applies U(β)U(\beta)U(β) if i1=j1i_1=j_1i1​=j1​ and U(−β)U(-\beta)U(−β) otherwise); the accumulation of failures, U(−αN)2N−1=−U(αN)U(-\alpha_N)^{2^N-1}=-U(\alpha_N)U(−αN​)2N−1=−U(αN​); the entropy formula E(ψα)=h(cos⁡2α)E(\psi_\alpha)=h(\cos^2\alpha)E(ψα​)=h(cos2α) (11); the cost identity (12); and the bounds (13).

Significance

The result shows that the entanglement needed to implement a nonlocal gate is not a fixed quantum of two ebits but can scale with the gate: Eˉ<5.97932 αN\bar E<5.97932\,\alpha_NEˉ<5.97932αN​ ebits for U(αN)U(\alpha_N)U(αN​). Through composition of binary phases it bounds the cost of an arbitrary phase gate by f∞αf_\infty\alphaf∞​α, and through the paper's infinitesimal argument it relates the cost of any two-qubit unitary to its nonlocal parameters; these extensions are not part of this mission. The operator–map correspondence (6)–(8), a bipartite form of the Jamiołkowski isomorphism, is the general mechanism for implementing a map from a resource state, and it is reusable well beyond this protocol.

The paper's arguments are short calculations, presented as "one can readily see". The mission makes every one of them explicit: the Bell-basis contraction, the Pauli corrections, the phase bookkeeping across NNN steps, the probability of each branch, and the numerical value of f∞f_\inftyf∞​. In checking the statements, two points needed repair. The printed value f∞=5.97932f_\infty=5.97932f∞​=5.97932 is not the value: f∞=5.9793137…f_\infty=5.9793137\ldotsf∞​=5.9793137…, so the goal poses 5.97931<f∞<5.979325.97931<f_\infty<5.979325.97931<f∞​<5.97932, which keeps the paper's usable bound. And footnote [20]'s step count is off by one: the local step U(π/2)U(\pi/2)U(π/2) is step NNN, and the printed communication 2−(1/2)N−22-(1/2)^{N-2}2−(1/2)N−2 is the sum of pkp_kpk​ over steps 1,…,N−11,\dots,N-11,…,N−1. No machine-checked proof of any of these statements is known to exist.

Difficulty

Each step is a contraction of a 64-dimensional state with two Bell vectors and two Pauli corrections; the claimed rule (U(β)U(\beta)U(β) if i1=j1i_1=j_1i1​=j1​, U(−β)U(-\beta)U(−β) otherwise, always with amplitude of modulus 1/41/41/4) must be verified on all 16 outcomes, and it holds only for the right reading of the Bell basis. The multi-step statement needs an invariant over histories of arbitrary length: after kkk failures the applied operator is a scalar multiple of U(−αN)2k−1U(-\alpha_N)^{2^k-1}U(−αN​)2k−1, and the step-(k+1)(k+1)(k+1) resource U(2kαN)U(2^k\alpha_N)U(2kαN​) exactly undoes it on success. The cost identity (12) is a reindexing of a finite sum, but the bound (13) is not: it needs the convergence of ∑2kh(cos⁡2(π/2k))\sum2^kh(\cos^2(\pi/2^k))∑2kh(cos2(π/2k)) (the terms behave like 2k⋅(π/2k)2log⁡(2k)2^k\cdot(\pi/2^k)^2\log(2^k)2k⋅(π/2k)2log(2k)) and a certified numerical enclosure of the sum to within 10−510^{-5}10−5, including a bound on the tail. A floating-point evaluation is not a proof.

Formalization scope

Systems are indexed from 000: Pauli labels are Fin 2 × Fin 2 with (0,0),(0,1),(1,0),(1,1)(0,0),(0,1),(1,0),(1,1)(0,0),(0,1),(1,0),(1,1) for 1,σx,σy,σz\mathbb 1,\sigma_x,\sigma_y,\sigma_z1,σx​,σy​,σz​, and the paper's step kkk is list position k−1k-1k−1. Operators on several systems are matrices over product index types in Mathlib's Kronecker convention; the resource is indexed ((a1,a2),(b1,b2))((a_1,a_2),(b_1,b_2))((a1​,a2​),(b1​,b2​)), so the published partial trace WildeQIT.partialTraceRight takes the cut (A1A2)∣(B1B2)(A_1A_2)|(B_1B_2)(A1​A2​)∣(B1​B2​). The gate is Mathlib's matrix exponential. Entropies are QAlgorithms.vnEntropy, in bits, and the binary entropy is WildeQIT.binaryEntropy. A protocol branch is a Kraus operator from A3B3A_3B_3A3​B3​ to A1B1A_1B_1A1​B1​; probabilities are Re⁡Tr⁡(KρK†)\operatorname{Re}\operatorname{Tr}(K\rho K^\dagger)ReTr(KρK†) on density matrices. f∞f_\inftyf∞​ is a tsum, and every statement about it asserts summability. The undefined ∣Ψ⟩|\Psi\rangle∣Ψ⟩ of the Bell basis is read as ∣Φ⟩|\Phi\rangle∣Φ⟩ of Eq. (5), the only reading under which the step rule holds.

The protocol is not defined through its conclusion: the step operators are the literal contractions of the resource with the Bell vectors, success is the label condition i1=j1i_1=j_1i1​=j1​, the resource is the printed formula (10) rather than U⊗1U\otimes\mathbb 1U⊗1 applied to ∣Φ+⟩∣Φ+⟩|\Phi^+\rangle|\Phi^+\rangle∣Φ+⟩∣Φ+⟩, the entropy is computed from the reduced state, and the step probabilities are computed from the operators rather than set to (1/2)k−1(1/2)^{k-1}(1/2)k−1. A formalization that defines any of these by the property to be proved, or drops the summability of f∞f_\inftyf∞​, trivializes the mission.

A complete development needs Pauli and Kronecker-product algebra, the closed form U(α)=cos⁡α 1−isin⁡α σx⊗σxU(\alpha)=\cos\alpha\,\mathbb 1-i\sin\alpha\,\sigma_x\otimes\sigma_xU(α)=cosα1−isinασx​⊗σx​ of the exponential, the spectrum of a rank-two reduced state, induction over protocol histories, and certified bounds on cos⁡\coscos and log⁡2\log_2log2​ for the numerical clause. The operator–map identities (6)–(8) and a verified evaluation of f∞f_\inftyf∞​ are reusable independently. Contributions to any milestone are welcome.

Selected references

  • J. I. Cirac, W. Dür, B. Kraus, M. Lewenstein, Entangling operations and their implementation using a small amount of entanglement, arXiv:quant-ph/0007057v1, 2000; Phys. Rev. Lett. 86, 544 (2001). https://arxiv.org/abs/quant-ph/0007057v1
  • J. Eisert, K. Jacobs, P. Papadopoulos, M. B. Plenio, Optimal local implementation of nonlocal quantum gates, Phys. Rev. A 62, 052317 (2000). https://arxiv.org/abs/quant-ph/0005101
  • A. Jamiołkowski, Linear transformations which preserve trace and positive semidefiniteness of operators, Rep. Math. Phys. 3, 275 (1972). https://doi.org/10.1016/0034-4877(72)90011-0
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Markov ChainProbabilityReinforcement Learning+1·Captain: mikedeng1

Uncertainty Quantification and Exploration for Reinforcement Learning: Empirical Q-Values Are Strongly Consistent and √n(Q̂ₙ − Q) ⇒ N(0, Σ) with the Closed-Form Covariance (5)Research Paper

Motivation

A reinforcement-learning agent that learns a Markov decision process (MDP) from data ends up with point estimates of the Q-values: the long-run discounted reward of taking an action in a state and acting optimally afterwards. Point estimates say nothing about their own reliability. Choosing between two actions whose estimated values differ by a small margin, deciding how much more data to collect, or allocating exploration effort all need the sampling distribution of the estimate. Finite-sample bounds (Kearns and Singh 1998) give rates with loose constants. Asymptotic normality gives exact limiting constants.

Zhu, Dong and Lam establish a central limit theorem for the plug-in Q-value estimate of a finite MDP whose data are collected by an exploration policy, with an explicit covariance matrix. For a fixed policy, the analogous result for the value function was obtained by Mannor, Simester, Sun and Tsitsiklis (2007). The new step is the optimal Q-values, which depend on the data through a maximum over actions. The paper uses the covariance to design a pure-exploration policy (Q-OCBA) that allocates samples to maximize the probability of selecting the optimal policy.

Setting

Let S\mathcal SS and A\mathcal AA be finite nonempty sets of states and actions. A pair (s,a)(s,a)(s,a) has a random reward with law R(s,a)R(s,a)R(s,a) on R\mathbb RR, mean μR(s,a)\mu_R(s,a)μR​(s,a) and variance σR2(s,a)\sigma^2_R(s,a)σR2​(s,a), and moves to state kkk with probability P(k∣s,a)P(k\mid s,a)P(k∣s,a). The discount factor is γ∈[0,1)\gamma\in[0,1)γ∈[0,1). The Bellman operator is

Tr,P′(Q)(s,a)=r(s,a)+γ∑k∈SP′(k∣s,a)max⁡a′Q(k,a′),\mathcal T_{r,P'}(Q)(s,a)=r(s,a)+\gamma\sum_{k\in\mathcal S}P'(k\mid s,a)\max_{a'}Q(k,a'),Tr,P′​(Q)(s,a)=r(s,a)+γk∈S∑​P′(k∣s,a)a′max​Q(k,a′),

and the Q-values are its fixed point Q=TμR,P(Q)Q=\mathcal T_{\mu_R,P}(Q)Q=TμR​,P​(Q), with V∗(s)=max⁡aQ(s,a)V^*(s)=\max_aQ(s,a)V∗(s)=maxa​Q(s,a).

Data are collected by an exploration policy π(a∣s)\pi(a\mid s)π(a∣s). Starting from some state, the agent repeatedly takes at∼π(⋅∣st)a_t\sim\pi(\cdot\mid s_t)at​∼π(⋅∣st​), observes rt∼R(st,at)r_t\sim R(s_t,a_t)rt​∼R(st​,at​), and moves to st+1∼P(⋅∣st,at)s_{t+1}\sim P(\cdot\mid s_t,a_t)st+1​∼P(⋅∣st​,at​). The state-action pairs then form a Markov chain with transition matrix P~π((s,a),(s′,a′))=P(s′∣s,a)π(a′∣s′)\tilde P^\pi((s,a),(s',a'))=P(s'\mid s,a)\pi(a'\mid s')P~π((s,a),(s′,a′))=P(s′∣s,a)π(a′∣s′). From nnn observations, the plug-in estimates are the sample mean reward μ^R,n(s,a)\hat\mu_{R,n}(s,a)μ^​R,n​(s,a) and the empirical transition frequencies P^n(k∣s,a)\hat P_n(k\mid s,a)P^n​(k∣s,a) at each pair, with fixed initial values at unvisited pairs. The estimate Q^n\hat Q_nQ^​n​ is the fixed point of Tμ^R,n,P^n\mathcal T_{\hat\mu_{R,n},\hat P_n}Tμ^​R,n​,P^n​​.

The standing assumptions are:

  • Assumption 1: finite reward variances, with rewards independent of the next state given (s,a)(s,a)(s,a).
  • Assumption 2: every state has a unique optimal action a∗(s)a^*(s)a∗(s).
  • Assumption 3: P~π\tilde P^\piP~π is irreducible. Its stationary distribution www is then positive and equals the long-run visit frequency of each pair.

Formalization targets

Goal: Theorem 1

Under Assumptions 1–3, Q^n→Q\hat Q_n\to QQ^​n​→Q almost surely, and

n(Q^n−Q)⇒N(0,Σ),Σ=(I−γP~π∗)−1W−1(DR+γ2DQ)((I−γP~π∗)−1)T.\sqrt n(\hat Q_n-Q)\Rightarrow\mathcal N(0,\Sigma),\qquad \Sigma=(I-\gamma\tilde P^{\pi^*})^{-1}W^{-1}(D_R+\gamma^2D_Q)\big((I-\gamma\tilde P^{\pi^*})^{-1}\big)^T.n​(Q^​n​−Q)⇒N(0,Σ),Σ=(I−γP~π∗)−1W−1(DR​+γ2DQ​)((I−γP~π∗)−1)T.

Here P~π∗((s,a),(s′,a′))=P(s′∣s,a)1(a′=a∗(s′))\tilde P^{\pi^*}((s,a),(s',a'))=P(s'\mid s,a)\mathbb 1(a'=a^*(s'))P~π∗((s,a),(s′,a′))=P(s′∣s,a)1(a′=a∗(s′)), and WWW, DRD_RDR​, DQD_QDQ​ are diagonal with entries w(s,a)w(s,a)w(s,a), σR2(s,a)\sigma^2_R(s,a)σR2​(s,a) and (V∗)TΣPs,aV∗(V^*)^T\Sigma_{P_{s,a}}V^*(V∗)TΣPs,a​​V∗. The matrix ΣPs,a\Sigma_{P_{s,a}}ΣPs,a​​ is the multinomial covariance of P(⋅∣s,a)P(\cdot\mid s,a)P(⋅∣s,a). The covariance is part of the statement: the paper's subsequent results (Corollary 1, Q-OCBA) use it.

Milestones (the proof of Theorem 1, App. A.1)

  1. (22): [μ^R,n,P^n]→[μR,P][\hat\mu_{R,n},\hat P_n]\to[\mu_R,P][μ^​R,n​,P^n​]→[μR​,P] almost surely.
  2. 1n#{t≤n:(st,at)=(i,j)}→w(i,j)\frac1n\#\{t\le n:(s_t,a_t)=(i,j)\}\to w(i,j)n1​#{t≤n:(st​,at​)=(i,j)}→w(i,j) almost surely.
  3. (23): n([μ^R,n,P^n]−[μR,P])⇒N(0,ΣR,P)\sqrt n([\hat\mu_{R,n},\hat P_n]-[\mu_R,P])\Rightarrow\mathcal N(0,\Sigma_{R,P})n​([μ^​R,n​,P^n​]−[μR​,P])⇒N(0,ΣR,P​), where ΣR,P=diag⁡(W−1DR,DP)\Sigma_{R,P}=\operatorname{diag}(W^{-1}D_R,D_P)ΣR,P​=diag(W−1DR​,DP​) and DPD_PDP​ is block diagonal with blocks ΣPs,a/w(s,a)\Sigma_{P_{s,a}}/w(s,a)ΣPs,a​​/w(s,a).
  4. I−γP~′I-\gamma\tilde P'I−γP~′ is invertible for every stochastic P′P'P′ and every Q′Q'Q′ with unique argmaxes.
  5. The fixed point ϕ(r′,P′)\phi(r',P')ϕ(r′,P′) is continuously differentiable at (μR,P)(\mu_R,P)(μR​,P), with gradient (I−γP~π∗)−1[ I∣γblockdiag⁡((V∗)T) ](I-\gamma\tilde P^{\pi^*})^{-1}[\,I\mid\gamma\operatorname{blockdiag}((V^*)^T)\,](I−γP~π∗)−1[I∣γblockdiag((V∗)T)].
  6. Q^n→Q\hat Q_n\to QQ^​n​→Q almost surely.
  7. ∇ϕ ΣR,P ∇ϕT=Σ\nabla\phi\,\Sigma_{R,P}\,\nabla\phi^T=\Sigma∇ϕΣR,P​∇ϕT=Σ.

Significance

The result. Theorem 1 gives asymptotically exact simultaneous confidence regions for all Q-values from one trajectory of exploration data. The closed form of Σ\SigmaΣ shows how each source of noise contributes: reward noise through DRD_RDR​, transition noise through DQD_QDQ​, the amount of data at each pair through W−1W^{-1}W−1, and propagation through the dynamics of the optimal policy through (I−γP~π∗)−1(I-\gamma\tilde P^{\pi^*})^{-1}(I−γP~π∗)−1. This decomposition is what makes Σ\SigmaΣ usable as an objective for allocating exploration effort, which the paper's Q-OCBA policy does. Corollary 1 (CLT for the optimal value V∗V^*V∗) is derived from it.

Formalizing it. The result is proved in the paper, but the proof cites its probabilistic core: a joint central limit theorem for empirical transition frequencies of an irreducible finite Markov chain (Trevezas and Limnios 2009, Proposition 3), together with the multivariate delta method. A machine-checked proof would also certify that the covariance formula, with its transposes and weights, is correct as printed. No Q-value CLT or Markov-chain CLT for empirical transition matrices is currently formalized on the platform. The existing Markov-chain CLTs there are scalar and assume uniform ergodicity.

Difficulty

The deterministic half (milestones 4, 5, 7) is linear algebra plus an implicit-function argument. The obstacle is that QQQ depends on (μR,P)(\mu_R,P)(μR​,P) through a maximum, which is not differentiable at ties. Assumption 2 removes ties at (μR,P)(\mu_R,P)(μR​,P), and differentiability holds only on a neighbourhood where the argmax stays the same.

The probabilistic half is harder. A natural first idea is to treat the visits to each pair as i.i.d. samples and apply the classical multivariate CLT. This fails because the number of visits is random and depends on the whole trajectory, and the samples at different pairs are dependent through the chain. The CLT (23) needs a martingale or regeneration argument for the Markov chain on state-action pairs. The chain is only assumed irreducible, so it may be periodic, and uniformly ergodic CLTs do not apply directly.

Formalization scope

  • Indexing and spaces. State-action pairs are indexed by S × A with Fintype, DecidableEq and Nonempty; the paper's flattening (i−1)ma+j(i-1)m_a+j(i−1)ma​+j is notation only. PPP, π\piπ and the initial state law are PMFs, and rewards are probability measures on R\mathbb RR with MemLp id 2 (Assumption 1).
  • Discount. 0≤γ<10\le\gamma<10≤γ<1 is pinned; the paper leaves it implicit.
  • Data law. The data form the Markov chain ((st,at),rt)((s_t,a_t),r_t)((st​,at​),rt​) on (S×A)×R(\mathcal S\times\mathcal A)\times\mathbb R(S×A)×R described in Setting, with law given by the published MarkovChainCLT.chainMeasure. Every initial state law is allowed. Time is 0-based.
  • Fixed points. The fixed point is the limit of value iteration (bellmanFix). It is the unique fixed point whenever the Bellman operator is a contraction, which covers every stochastic P′P'P′ and a neighbourhood of (μR,P)(\mu_R,P)(μR​,P).
  • Assumptions 2 and 3. Assumption 2 is a strict inequality Q(s,a)<Q(s,a∗(s))Q(s,a)<Q(s,a^*(s))Q(s,a)<Q(s,a∗(s)) for a≠a∗(s)a\ne a^*(s)a=a∗(s). Assumption 3 is ∀x,y ∃m, (P~π)m(x,y)>0\forall x,y\ \exists m,\ (\tilde P^\pi)^m(x,y)>0∀x,y ∃m, (P~π)m(x,y)>0, and www is bound by the stationarity equations.
  • Limits. The Gaussian limits are Mathlib's multivariateGaussian on EuclideanSpace, and convergence in distribution is TendstoInDistribution.

Trivializations ruled out.

  • Matrix.inv returns 000 on singular matrices, but I−γP~π∗I-\gamma\tilde P^{\pi^*}I−γP~π∗ is invertible under the pins, so Σ\SigmaΣ is not a junk zero.
  • multivariateGaussian returns a point mass for a non-positive-semidefinite matrix, but Σ\SigmaΣ and ΣR,P\Sigma_{R,P}ΣR,P​ are positive semidefinite.
  • A non-strict argmax (which would admit ties and the non-Gaussian limit of the paper's Theorem 2) is excluded.
  • Rewards and transitions live on one trajectory under one chain law, not on independent spaces.

Infrastructure. A complete development needs:

  • an ergodic theorem for finite irreducible Markov chains (milestone 2);
  • a multivariate Markov-chain CLT (milestone 3), which is reusable well beyond this mission;
  • the multivariate delta method and continuous mapping in TendstoInDistribution form;
  • differentiability of a contraction fixed point in parameters.

Contributions of any of these as standalone lemmas are welcome.

Not posed. Corollaries 1–2 and Theorems 2–6 of the paper (optimal-value and fixed-policy CLTs, non-unique optimal policies, constrained MDPs, Q-OCBA consistency, approximate value iteration, kernel representations) are not part of this mission.

Selected references

  • Y. Zhu, J. Dong, H. Lam, Uncertainty Quantification and Exploration for Reinforcement Learning, Operations Research, 2024; arXiv:1910.05471v3, 2022. https://arxiv.org/abs/1910.05471
  • S. Mannor, D. Simester, P. Sun, J. N. Tsitsiklis, Bias and Variance Approximation in Value Function Estimates, Management Science 53(2):308–322, 2007. https://doi.org/10.1287/mnsc.1060.0614
  • S. Trevezas, N. Limnios, Variance Estimation in the Central Limit Theorem for Markov Chains, Journal of Statistical Planning and Inference 139(7):2242–2253, 2009. https://www.sciencedirect.com/journal/journal-of-statistical-planning-and-inference/vol/139/issue/7
  • R. J. Serfling, Approximation Theorems of Mathematical Statistics, Wiley, 2009 (delta method). https://doi.org/10.1002/9780470316481
  • M. Kearns, S. Singh, Finite-Sample Convergence Rates for Q-Learning and Indirect Algorithms, Advances in Neural Information Processing Systems 11, 996–1002, 1998.
10 thms3 active usersReviewed
Quantum InformationRepresentation TheoryStatistics·Captain: mikedeng1

Parallel Treatment of Estimation of SU(2) and Phase Estimation: with a Reference System, n = 2d − 1 Uses of an Unknown SU(2) Matrix Reach Worst-Case Error sin²(π/(2d+2)), so n²·Error → π²Research Paper

Motivation

Two parties who do not share a reference frame can align one by sending quantum systems through an unknown rotation. Mathematically, a device applies an unknown matrix g∈SU(2)g\in\mathrm{SU}(2)g∈SU(2) to each of nnn qubits, and the task is to estimate ggg from one measurement on the output. How fast the smallest achievable error falls with nnn is a basic question of quantum metrology and quantum statistics: classical repetition gives order 1/n1/n1/n, and entangled inputs can do better.

Masahito Hayashi's paper (arXiv:quant-ph/0407053v3) shows that, with the right input, estimating an SU(2) action reduces exactly to the phase-estimation problem solved by Bužek, Derka and Massar. The reduction yields an error of order 1/n21/n^21/n2 with the explicit constant π2\pi^2π2.

Timeline.

  • 1999. Bužek, Derka and Massar (quant-ph/9808042) determine the optimal phase estimate (the "quantum clock"), with error ≅π2/(4n2)\cong\pi^2/(4n^2)≅π2/(4n2).
  • 2001. Acín, Jané and Vidal (quant-ph/0012015) study optimal estimation of SU(2) dynamics.
  • 2002. Fujiwara (doi:10.1103/PhysRevA.65.012316) shows that a reference system reduces the error for a single use of ggg.
  • 2003–2004. Bagan, Baig and Muñoz-Tapia (quant-ph/0303019) and Chiribella, D'Ariano, Perinotti and Sacchi (quant-ph/0405095) obtain 1/n21/n^21/n2 scaling for reference-frame alignment.
  • 2004. Hayashi (this paper) gives the reduction to phase estimation.
  • 2005. Chiribella, D'Ariano and Sacchi (quant-ph/0506267) prove that the error is optimal among all measurements in a general group framework.

Setting

Let SU(2)\mathrm{SU}(2)SU(2) be the group of 2×22\times22×2 complex unitary matrices of determinant one, and let μ\muμ be its invariant (Haar) probability measure. The cost of reporting g^\hat gg^​ when the truth is ggg is

d(g,g^)=1−∣12Tr⁡(g−1g^)∣2.d(g,\hat g)=1-\Big|\tfrac12\operatorname{Tr}(g^{-1}\hat g)\Big|^2 .d(g,g^​)=1−​21​Tr(g−1g^​)​2.

For each j≥1j\ge1j≥1, let VjV^jVj be the jjj-dimensional irreducible representation of SU(2)\mathrm{SU}(2)SU(2) on a space Hj\mathcal H_jHj​. If ggg has eigenvalues e±iθ/2e^{\pm i\theta/2}e±iθ/2, its character is

χj(g)=Tr⁡Vgj=sin⁡(jθ/2)sin⁡(θ/2)=Uj−1(Re⁡Tr⁡g/2),\chi_j(g)=\operatorname{Tr}V^j_g=\frac{\sin(j\theta/2)}{\sin(\theta/2)}=U_{j-1}\big(\operatorname{Re}\operatorname{Tr}g/2\big),χj​(g)=TrVgj​=sin(θ/2)sin(jθ/2)​=Uj−1​(ReTrg/2),

where UmU_mUm​ is the Chebyshev polynomial of the second kind.

For n=2d−1n=2d-1n=2d−1 uses of ggg with a reference system on which ggg does not act, the paper works on

⨁k=1dH2k⊗H2k,R,Ug=⨁kVg2k⊗I.\bigoplus_{k=1}^d\mathcal H_{2k}\otimes\mathcal H_{2k,R},\qquad U_g=\bigoplus_k V^{2k}_g\otimes I .k=1⨁d​H2k​⊗H2k,R​,Ug​=k⨁​Vg2k​⊗I.

Its ingredients are:

  • Input. xx⃗=⨁kxk xE2kx_{\vec x}=\bigoplus_kx_k\,x^{2k}_Exx​=⨁k​xk​xE2k​, where x∈Cdx\in\mathbb C^dx∈Cd satisfies ∑k∣xk∣2=1\sum_k|x_k|^2=1∑k​∣xk​∣2=1 and xE2k=vec⁡(I)/2kx^{2k}_E=\operatorname{vec}(I)/\sqrt{2k}xE2k​=vec(I)/2k​ is maximally entangled.
  • Measurement. For a Hermitian T=(tk,l)≥0T=(t_{k,l})\ge0T=(tk,l​)≥0 with tk,k=1t_{k,k}=1tk,k​=1,
MT(dg^)=Ug^(∑k,ltk,l ∣(2k)xE2k⟩⟨(2l)xE2l∣)Ug^† μ(dg^).M^T(d\hat g)=U_{\hat g}\Big(\sum_{k,l}t_{k,l}\,|(2k)x^{2k}_E\rangle\langle(2l)x^{2l}_E|\Big)U_{\hat g}^\dagger\,\mu(d\hat g).MT(dg^​)=Ug^​​(k,l∑​tk,l​∣(2k)xE2k​⟩⟨(2l)xE2l​∣)Ug^​†​μ(dg^​).
  • Error at a fixed true ggg.
Dg(M,x)=∫d(g,g^) Tr⁡M(dg^) Ug∣xx⃗⟩⟨xx⃗∣Ug†.\mathcal D_g(M,x)=\int d(g,\hat g)\,\operatorname{Tr}M(d\hat g)\,U_g|x_{\vec x}\rangle\langle x_{\vec x}|U_g^\dagger .Dg​(M,x)=∫d(g,g^​)TrM(dg^​)Ug​∣xx​⟩⟨xx​∣Ug†​.

The method value of an input is v(x)=12(1−∑k=1d−1∣xk∣∣xk+1∣)v(x)=\frac12\big(1-\sum_{k=1}^{d-1}|x_k||x_{k+1}|\big)v(x)=21​(1−∑k=1d−1​∣xk​∣∣xk+1​∣).

Formalization targets

Goal: exact error, attained optimum, and the constant π2\pi^2π2

The goal theorem has four parts.

  1. For every ddd, irreducible representations of dimensions 2,4,…,2d2,4,\dots,2d2,4,…,2d with the Weyl characters exist.
  2. For every unit xxx and every admissible TTT, MTM^TMT is a POVM, and at every true ggg
Dg(MT,x)=12∑k∣xk∣2tk,k−14∑k=1d−1Re⁡(xk‾xk+1tk,k+1+xk+1‾xktk+1,k) ≥ v(x).\mathcal D_g(M^T,x)=\tfrac12\sum_k|x_k|^2t_{k,k}-\tfrac14\sum_{k=1}^{d-1}\operatorname{Re}\big(\overline{x_k}x_{k+1}t_{k,k+1}+\overline{x_{k+1}}x_kt_{k+1,k}\big)\ \ge\ v(x).Dg​(MT,x)=21​k∑​∣xk​∣2tk,k​−41​k=1∑d−1​Re(xk​​xk+1​tk,k+1​+xk+1​​xk​tk+1,k​) ≥ v(x).

Equality holds for the phase-aligned TTT, tk,l=xk∣xk∣xl∣xl∣‾t_{k,l}=\frac{x_k}{|x_k|}\overline{\frac{x_l}{|x_l|}}tk,l​=∣xk​∣xk​​∣xl​∣xl​​​. 3. For d≥1d\ge1d≥1, min⁡∥x∥=1v(x)=sin⁡2π2d+2\displaystyle\min_{\|x\|=1}v(x)=\sin^2\frac{\pi}{2d+2}∥x∥=1min​v(x)=sin22d+2π​, and the minimum is attained. 4.

lim⁡d→∞(2d−1)2sin⁡2π2d+2=π2.\lim_{d\to\infty}(2d-1)^2\sin^2\frac{\pi}{2d+2}=\pi^2 .d→∞lim​(2d−1)2sin22d+2π​=π2.

Milestones

  • (15) Weyl integration over SU(2)\mathrm{SU}(2)SU(2).
  • (12) The single-irrep integral ∫d(I,g^)∣χj∣2 dμ=34\int d(I,\hat g)|\chi_j|^2\,d\mu=\frac34∫d(I,g^​)∣χj​∣2dμ=43​ for j=1j=1j=1 and 12\frac1221​ for j≥2j\ge2j≥2.
  • (13) ∫d(I,g^)χ2kχ2l‾ dμ=12δk,l−14δk,l−1−14δk−1,l\int d(I,\hat g)\chi_{2k}\overline{\chi_{2l}}\,d\mu=\frac12\delta_{k,l}-\frac14\delta_{k,l-1}-\frac14\delta_{k-1,l}∫d(I,g^​)χ2k​χ2l​​dμ=21​δk,l​−41​δk,l−1​−41​δk−1,l​.
  • Schur orthogonality. A published theorem.
  • Normalization. MTM^TMT integrates to the identity.
  • (14) The exact error formula, its lower bound and equality.
  • (11) Bužek's optimum sin⁡2π2(n+2)\sin^2\frac{\pi}{2(n+2)}sin22(n+2)π​ in exact form.

Significance

The result. The error of a covariant SU(2) measurement on this space equals, coefficient by coefficient, the error of a covariant phase measurement. Eq. (13) says that the SU(2) character integral has the same tridiagonal kernel as the phase-estimation identity (7). Optimizing the input therefore becomes the largest-eigenvalue problem for a path graph, and that problem has a closed-form solution. With n=2d−1n=2d-1n=2d−1 uses, the protocol reaches error sin⁡2(π/(n+3))∼π2/n2\sin^2(\pi/(n+3))\sim\pi^2/n^2sin2(π/(n+3))∼π2/n2. This beats the 1/n1/n1/n rate of independent uses, and the paper gives the explicit constant. Chiribella, D'Ariano and Sacchi later showed that v(x)v(x)v(x) is optimal over all measurements; the present paper does not prove that.

Formalizing it. No part of this computation is machine-checked yet:

  • the Weyl integration formula for SU(2)\mathrm{SU}(2)SU(2);
  • the character integrals (12)–(13);
  • the covariant-POVM normalization;
  • the exact error identity;
  • the eigenvalue optimum and its limit.

The paper's own displays contain slips: the conjugation in (8), (9) and (14), the j=1j=1j=1 value on p. 9, the coefficients of the expansion on p. 10, and a quoted Bužek vector that is not the minimizer. A checked development fixes these.

Difficulty

The obvious route through (13) is to "expand the product of characters and keep the constant and cos⁡θ\cos\thetacosθ, cos⁡2θ\cos2\thetacos2θ terms", as p. 10 does. That route needs the Weyl integration formula. Mathlib has the Haar measure but no Weyl integration formula for SU(2)\mathrm{SU}(2)SU(2), no compactness instance on Matrix.specialUnitaryGroup, and no classification of its irreducible representations.

The reduction from the operator integral in (14) to the scalar integral (13) needs two further facts: Schur orthogonality on each pair of blocks, and the invariance of μ\muμ to move from g^\hat gg^​ to g−1g^g^{-1}\hat gg−1g^​.

The optimum over inputs is a Perron–Frobenius problem for a path graph. It is easy to state with ≅\cong≅, but in exact form it needs the attained eigenvector ak∝sin⁡(π(k+1)/(d+1))a_k\propto\sin(\pi(k+1)/(d+1))ak​∝sin(π(k+1)/(d+1)), not the vector the paper quotes.

Formalization scope

Representations.

  • SU(2)\mathrm{SU}(2)SU(2) is Matrix.specialUnitaryGroup (Fin 2) ℂ.
  • The pinned Mathlib has no topological-group, compactness or measurable instances on it, so these are instance hypotheses (IsTopologicalGroup, CompactSpace, MeasurableSpace with BorelSpace).
  • μ\muμ is any left- and right-invariant probability measure dg.
  • Irreducible representations are the published BasedIrreps (based, continuous, unitary, irreducible), indexed k=0,…,d−1k=0,\dots,d-1k=0,…,d−1 for H2,…,H2d\mathcal H_2,\dots,\mathcal H_{2d}H2​,…,H2d​.
  • A spin family requires dimension 2(k+1)2(k+1)2(k+1) and the Weyl character U2k+1(Re⁡Tr⁡g/2)U_{2k+1}(\operatorname{Re}\operatorname{Tr}g/2)U2k+1​(ReTrg/2). The character hypothesis is a true property of every such representation and is what the paper uses on p. 9.
  • The space, action and input are the published CanonicalIndex, canonicalAction and canonicalInput (with identity block unitaries).

Measurement and error.

  • Measurements are DensityPOVMs: a reference measure and a PSD operator density integrating to III.
  • The cost is the published bellCost.
  • Probabilities are Re⁡Tr⁡\operatorname{Re}\operatorname{Tr}ReTr.
  • The error is pointwise in the true ggg, as in the paper, not Haar-averaged.
  • In (14) the term with x0x_0x0​ is absent.
  • The zero coefficient gets phase 111.

Ruled-out trivializations.

  • The irreducible representations are hypothesized, so clause 1 of the goal asserts that a spin family exists.
  • TTT must be positive semidefinite with unit diagonal. Without the unit diagonal the seed is not normalized and the "error" can be made 000.
  • The error is not averaged over ggg.
  • The optimum is stated with IsLeast, not sInf or ⨅.

Infrastructure. The reusable parts beyond this mission are:

  • Weyl integration for SU(2)\mathrm{SU}(2)SU(2), together with the compactness and topological-group instances;
  • the characters of the irreducible representations;
  • existence of the spin-j/2j/2j/2 representations (for example the published polynomial irreps Gap48.P23.polynomialIrrep);
  • the path-graph eigenvalue problem.

Proofs of any milestone, and of these supporting facts, are welcome.

Related work on the platform. The Chiribella–D'Ariano–Sacchi items of the Next46.P36 series pose related but different statements:

  • optimalPOVM and minimumEigenvalueInput concern a general compact group, a Haar-averaged risk, and optimality over all measurements.
  • cartesianFrameOptimum concerns SU(2) without a reference system, with a different cost.

This mission reuses their definition layer and their Schur orthogonality theorem. It states Hayashi's own reference-assisted protocol, with its exact pointwise error and the limit π2\pi^2π2.

Not formalized. The following parts of the paper are out of scope:

  • the no-reference variant (pp. 8–9);
  • the even case n=2dn=2dn=2d;
  • §2's other phase-estimation results;
  • eqs. (16)–(17).

Selected references

  • M. Hayashi, Parallel Treatment of Estimation of SU(2) and Phase Estimation, arXiv:quant-ph/0407053v3 (2006). https://arxiv.org/abs/quant-ph/0407053
  • V. Bužek, R. Derka, S. Massar, Optimal Quantum Clocks, Phys. Rev. Lett. 82, 2207 (1999). https://arxiv.org/abs/quant-ph/9808042
  • G. Chiribella, G. M. D'Ariano, M. F. Sacchi, Optimal estimation of group transformations using entanglement, Phys. Rev. A 72, 042338 (2005). https://arxiv.org/abs/quant-ph/0506267
  • A. Fujiwara, Estimation of SU(2) operation and dense coding: an information geometric approach, Phys. Rev. A 65, 012316 (2002). https://doi.org/10.1103/PhysRevA.65.012316
  • A. Acín, E. Jané, G. Vidal, Optimal estimation of quantum dynamics, Phys. Rev. A 64, 050302 (2001). https://arxiv.org/abs/quant-ph/0012015
  • E. Bagan, M. Baig, R. Muñoz-Tapia, Entanglement-assisted alignment of reference frames using a dense covariant coding, Phys. Rev. A 69, 050303(R) (2004). https://arxiv.org/abs/quant-ph/0303019
  • G. Chiribella, G. M. D'Ariano, P. Perinotti, M. F. Sacchi, Efficient use of quantum resources for the transmission of a reference frame, Phys. Rev. Lett. 93, 180503 (2004). https://arxiv.org/abs/quant-ph/0405095
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Capability Building in Sluggish Organizations: Under Myopic Adjustment the Lowest Long-Run Capability Is at Most 2μ − 1, Attained by a Perturbed Rest/High-Intensity CycleResearch Paper

Motivation

Organizations, athletes and students build capability gradually: a team can raise or lower its skill level only a little from one period to the next, while the demands placed on it can change abruptly. A trainer (a coach, a manager, a curriculum designer) who controls the sequence of demands, subject to a budget on their average intensity, wants to know which sequence leaves the trainee with the highest capability in the long run. Periodized training in sports, with alternating rest and high-intensity phases, is the familiar practical answer.

Eliaz and Spiegler (Management Science, 2023) model this as a trainer committing to a stochastic challenge process and an agent that adjusts sluggishly, by at most one unit per period. Their Proposition 1 shows that against a myopic sluggish agent, a budget of about μ\muμ on the average challenge can sustain a long-run capability of about 2μ2\mu2μ, nearly twice what a flexibly adjusting agent would keep, and that a slightly perturbed rest/high-intensity cycle achieves it. This mission formalizes Proposition 1.

Setting

A training program is a pair (P,f)(P, f)(P,f): a stochastic matrix PPP on a finite set of states SSS, irreducible, and an output function f:S→Nf : S \to \mathbb{N}f:S→N giving the challenge d=f(s)d = f(s)d=f(s) in each state. By irreducibility PPP has a unique invariant distribution λP\lambda_PλP​. The program is feasible for an integer μ≥1\mu \ge 1μ≥1 and a slack ε∈(0,1)\varepsilon \in (0,1)ε∈(0,1) if it satisfies the intensity constraint (1):

∑s∈SλP(s) f(s)≤μ+ε.\sum_{s \in S} \lambda_P(s)\, f(s) \le \mu + \varepsilon .s∈S∑​λP​(s)f(s)≤μ+ε.

The agent holds a non-negative integer capability mtm_tmt​. At each period t≥1t \ge 1t≥1 it observes the challenge dt=f(st)d_t = f(s_t)dt​=f(st​) and chooses mt∈{mt−1−1,mt−1,mt−1+1}m_t \in \{m_{t-1}-1, m_{t-1}, m_{t-1}+1\}mt​∈{mt−1​−1,mt−1​,mt−1​+1}, paying Ct=c mt+max⁡(0,dt−mt)C_t = c\,m_t + \max(0, d_t - m_t)Ct​=cmt​+max(0,dt​−mt​) with c∈(0,1)c \in (0,1)c∈(0,1). A myopic agent minimizes CtC_tCt​ period by period, which gives rule (2):

mt={mt−1+1dt>mt−1,mt−1dt=mt−1,max⁡{0,mt−1−1}dt<mt−1.m_t = \begin{cases} m_{t-1}+1 & d_t > m_{t-1},\\ m_{t-1} & d_t = m_{t-1},\\ \max\{0, m_{t-1}-1\} & d_t < m_{t-1}.\end{cases}mt​=⎩⎨⎧​mt−1​+1mt−1​max{0,mt−1​−1}​dt​>mt−1​,dt​=mt−1​,dt​<mt−1​.​

The pair (mt,st)(m_t, s_t)(mt​,st​) is then a Markov chain, the extended process: from (m,s)(m, s)(m,s) it moves to (g(m,f(s′)),s′)(g(m, f(s')), s')(g(m,f(s′)),s′) with probability P(s,s′)P(s,s')P(s,s′), where ggg is rule (2). The lowest long-run capability m∗m^*m∗ is the lowest value mtm_tmt​ takes beyond a sufficiently large ttt. On a finite chain a path is eventually absorbed in a recurrent class and visits all its states infinitely often, so m∗m^*m∗ is the minimum of mmm over that class.

Formalization targets

Goal: Proposition 1 (with ε<1/2\varepsilon < 1/2ε<1/2 in part (i))

(i) If ε<1/2\varepsilon < 1/2ε<1/2, then for every feasible program on every finite state set, every recurrent class of the extended process contains a state with

m≤2μ−1.m \le 2\mu - 1 .m≤2μ−1.

(ii) There is β0<1\beta_0 < 1β0​<1 such that for every β∈(β0,1)\beta \in (\beta_0, 1)β∈(β0​,1) the two-state program

P=(01β1−β) (states L,H),f(L)=0,f(H)=2μ,P = \begin{pmatrix} 0 & 1 \\ \beta & 1-\beta \end{pmatrix}\ (\text{states } L, H), \qquad f(L) = 0,\quad f(H) = 2\mu,P=(0β​11−β​) (states L,H),f(L)=0,f(H)=2μ,

is feasible, its extended process has exactly the recurrent states (2μ−1,L)(2\mu - 1, L)(2μ−1,L) and (2μ,H)(2\mu, H)(2μ,H), and every invariant distribution puts mass 11+β\frac{1}{1+\beta}1+β1​ on m=2μm = 2\mum=2μ and β1+β\frac{\beta}{1+\beta}1+ββ​ on m=2μ−1m = 2\mu - 1m=2μ−1; both tend to 12\tfrac1221​ as β→1\beta \to 1β→1.

Milestones

In attack order: uniqueness of the invariant distribution of an irreducible finite chain (§2, p. 7; already proved on the platform); the myopic best response (2); the extended process is a Markov chain whose invariant laws have state marginal λP\lambda_PλP​; every recurrent class carries an invariant law; Step 1, the balance identity (4), ∑X+λ(m,d)(m+1)=∑X−λ(m,d) m\sum_{X^+}\lambda(m,d)(m+1) = \sum_{X^-}\lambda(m,d)\,m∑X+​λ(m,d)(m+1)=∑X−​λ(m,d)m; Step 2, E(m)≤2(μ+ε)−∑X0λ(m,d) m\mathbb{E}(m) \le 2(\mu+\varepsilon) - \sum_{X^0}\lambda(m,d)\,mE(m)≤2(μ+ε)−∑X0​λ(m,d)m; Step 3, every invariant law charges a capability ≤2μ−1\le 2\mu - 1≤2μ−1; the two-state program's average intensity 2μ/(1+β)2\mu/(1+\beta)2μ/(1+β); and the recurrent states and invariant masses of its extended process.

Significance

The result separates two quantities a trainer might confuse: the average intensity of the demands, which the budget constrains, and the capability they sustain, which depends only on the sign of d−md - md−m under sluggish adjustment. Because the cardinal budget and the ordinal adjustment rule differ, alternating rest (d=0d = 0d=0) with high intensity (d=2μd = 2\mud=2μ) holds capability near 2μ2\mu2μ for an average cost near μ\muμ. Part (i) shows that no program, however many states it uses, does better, so the two-state periodized program is optimal for a myopic agent. The paper's second main result (Proposition 2, a forward-looking agent) is not part of this mission.

Formalizing it adds a machine-checked account of an argument whose printed version has two gaps (see Formalization scope): the bound in part (i) needs ε<1/2\varepsilon < 1/2ε<1/2, and the printed Step 3 reaches only 2μ2\mu2μ. The proposition is proved on paper; it has not been formalized. The finite-chain lemmas built along the way (an invariant law on every recurrent class, the marginal of an invariant law of a product-type chain, level-crossing balance for a skip-free coordinate) are reusable outside this paper.

Difficulty

The paper argues with long-run frequencies along a sample path. A formal proof has to replace that by invariant distributions of a finite chain on (m,s)(m, s)(m,s), whose recurrent classes need not be unique and whose invariant laws need not be unique either. The step from the average bound to the minimum is the delicate one: knowing that E(m)\mathbb{E}(m)E(m) is at most about 2μ2\mu2μ and that mmm is not constant only shows that the minimum is at most 2μ2\mu2μ. The bound 2μ−12\mu - 12μ−1 needs a finer use of the constraint, and it fails for ε>1/2\varepsilon > 1/2ε>1/2, so any argument that treats ε\varepsilonε as negligible without quantifying it cannot be completed.

Formalization scope

Lean represents the trainer's chain with the published mm_basic vocabulary (IsStochastic, IsStationary with row vectors πP=π\pi P = \piπP=π, Irreducible); uniqueness of λP\lambda_PλP​ is the proved MarkovMixing.exists_unique_stationary. Challenges and capabilities are natural numbers; max⁡{0,m−1}\max\{0, m-1\}max{0,m−1} and 2μ−12\mu - 12μ−1 use truncated subtraction (harmless since μ≥1\mu \ge 1μ≥1). Feasibility asks for some invariant distribution satisfying (1), which is λP\lambda_PλP​ by uniqueness. The extended process lives on Fin (M + 1) × S for a truncation level M≥max⁡sf(s)M \ge \max_s f(s)M≥maxs​f(s); the goal quantifies over every such MMM, which covers every initial capability m0m_0m0​. "Lowest long-run capability ≤K\le K≤K" is stated as: every recurrent state reaches a state with m≤Km \le Km≤K. In the two-state program index 0 is LLL and 1 is HHH. The limit "probability 12\tfrac1221​" is stated through the exact masses 11+β\frac{1}{1+\beta}1+β1​ and β1+β\frac{\beta}{1+\beta}1+ββ​, together with existence of an invariant law.

Part (i) is posed with ε<1/2\varepsilon < 1/2ε<1/2 because it is false for ε>1/2\varepsilon > 1/2ε>1/2. With μ=1\mu = 1μ=1, ε=3/5\varepsilon = 3/5ε=3/5, P=(017/81/8)P = \begin{pmatrix} 0 & 1 \\ 7/8 & 1/8\end{pmatrix}P=(07/8​11/8​), f(L)=0f(L) = 0f(L)=0, f(H)=3f(H) = 3f(H)=3: the invariant law is (7/15,8/15)(7/15, 8/15)(7/15,8/15), the average challenge is 8/5=μ+ε8/5 = \mu + \varepsilon8/5=μ+ε, and the only recurrent states of the extended process are (2,L)(2, L)(2,L) and (3,H)(3, H)(3,H), so the lowest long-run capability is 2>2μ−12 > 2\mu - 12>2μ−1. The paper states ε∈(0,1)\varepsilon \in (0,1)ε∈(0,1) but says it "can be arbitrarily close to zero" and treats it as negligible. Part (ii) holds for every ε∈(0,1)\varepsilon \in (0,1)ε∈(0,1). The printed Step 3 argument only yields 2μ2\mu2μ; a solver must supply the step to 2μ−12\mu - 12μ−1, and the milestone is posed in that corrected form.

The statements rule out the trivializing readings: part (i) ranges over every finite state set, every truncation level and every recurrent state (not a fixed SSS, not some class, not the minimum over transient states, which a low m0m_0m0​ would make trivial); part (ii) asserts feasibility, all β\betaβ in an interval up to 111, that the two named states are the only recurrent ones, and the masses together with existence of an invariant law, so no clause holds vacuously; and the extended kernel is stochastic because M≥max⁡fM \ge \max fM≥maxf.

Contributions welcome: proofs of the finite-chain milestones (they need only mm_basic and Mathlib's matrix library), the balance identity (4), and the corrected Step 3.

Selected references

  • K. Eliaz, R. Spiegler, Capability Building in Sluggish Organizations, Management Science, 2023; read in the authors' manuscript of March 28, 2022. https://doi.org/10.1287/mnsc.2022.4445
  • D. A. Levin, Y. Peres, E. L. Wilmer, Markov Chains and Mixing Times, American Mathematical Society, 2nd ed., 2017 (Chapter 1, invariant distributions of finite chains; source of mm_basic). https://doi.org/10.1090/mbk/107
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Dynamic Pricing with Unknown Non-Parametric Demand and Limited Price Changes: The SLPE Policy Has Regret O(√T log T log log T) on Its Concentration Event and Makes O(log log T) Price ChangesResearch Paper

Motivation

A retailer selling one product over TTT periods must choose a price each period without knowing how demand responds to price. Charging different prices reveals the demand curve but costs revenue, and in practice every price change has its own cost: relabelling, customer goodwill, contractual limits on repricing. Dynamic pricing with learning asks for policies whose cumulative revenue loss against the best fixed price, the regret, grows slowly in TTT, and recent work also asks that the policy change its price rarely.

The paper's literature review (pp. 3–5) frames the gap. For parametric demand, Broder (2011) gives an MLE-based policy with O~(T)\tilde O(\sqrt T)O~(T​) regret and O(log⁡T)O(\log T)O(logT) price changes, and Cheung, Simchi-Levi and Wang (2017) study limited price changes when demand is one of finitely many known curves. Non-parametric policies such as Besbes and Zeevi (2015) and the continuum-armed bandit algorithm of Agarwal et al. (2011) do not control price changes and incur at least O(log⁡T)O(\log T)O(logT) of them. Perakis and Singhvi (SSRN 3336949; published in Operations Research, doi:10.1287/opre.2020.0445) show that, under a two-point bandit feedback assumption borrowed from online convex optimisation (Agarwal and Dekel 2010, Nesterov 2011), a non-parametric policy can keep O~(T)\tilde O(\sqrt T)O~(T​) regret while changing its price only O(log⁡log⁡T)O(\log\log T)O(loglogT) times.

Setting

Prices lie in [0,1][0,1][0,1]. In period ttt the retailer charges ptp_tpt​ and observes demand

Yt=d(pt)+ϵt,Y_t=d(p_t)+\epsilon_t,Yt​=d(pt​)+ϵt​,

where ddd is an unknown smooth non-increasing demand curve and ϵt\epsilon_tϵt​ is noise. The revenue is r(p)=p d(p)r(p)=p\,d(p)r(p)=pd(p), maximised on [0,1][0,1][0,1] at a unique interior price p∗p^*p∗. The two performance measures are

R(T)=∑t=1T(r(p∗)−r(pt)),LPC(T)=1+∣{2≤t≤T: pt≠pt−1}∣.\mathcal R(T)=\sum_{t=1}^T\big(r(p^*)-r(p_t)\big),\qquad LPC(T)=1+\big|\{2\le t\le T:\ p_t\ne p_{t-1}\}\big|.R(T)=t=1∑T​(r(p∗)−r(pt​)),LPC(T)=1+​{2≤t≤T: pt​=pt−1​}​.

Assumption 1 asks for κ>0\kappa>0κ>0 with d(p∗)−κ(p−p∗)2≤−d′(p) p∗d(p^*)-\kappa(p-p^*)^2\le-d'(p)\,p^*d(p∗)−κ(p−p∗)2≤−d′(p)p∗; Assumption 2 asks that among the observations at two charged prices there is one pair with identical noise, and that the policy can identify it. K1K_1K1​ bounds ∣d(k)∣|d^{(k)}|∣d(k)∣ for k≤3k\le3k≤3.

The SLPE policy (Algorithm 1) runs in rounds i=1,2,…i=1,2,\dotsi=1,2,… with half-widths Δ1=12\Delta_1=\tfrac12Δ1​=21​, Δi+1=μΔi2\Delta_{i+1}=\mu\Delta_i^2Δi+1​=μΔi2​. Round iii charges piL=piM−Δip^L_i=p^M_i-\Delta_ipiL​=piM​−Δi​, piMp^M_ipiM​ and piH=piM+Δip^H_i=p^M_i+\Delta_ipiH​=piM​+Δi​ for ni=2ρ4log⁡T/Δi4n_i=2\rho^4\log T/\Delta_i^4ni​=2ρ4logT/Δi4​ periods each, starting from p1M=12p^M_1=\tfrac12p1M​=21​. It fits a two-piece linear demand estimate whose level is the average demand Dˉni(piM)\bar D_{n_i}(p^M_i)Dˉni​​(piM​) and whose slopes are finite differences of the two identical-noise pairs, maximises the estimated revenue on [piL,piH][p^L_i,p^H_i][piL​,piH​] to obtain p~i∗\tilde p^*_ip~​i∗​, and recentres: pi+1M=p~i∗p^M_{i+1}=\tilde p^*_ipi+1M​=p~​i∗​.

Formalization targets

Goal: Theorem 1 and Corollary 1

Under Assumption 1, the gradient condition ∣d′(p∗)∣≥(K1/24+κ/4)14+c/2|d'(p^*)|\ge(K_1/24+\kappa/4)\tfrac14+c/2∣d′(p∗)∣≥(K1​/24+κ/4)41​+c/2 with c>0c>0c>0, and

2>μ≥M=1c(1ρ2+K16+κ4)+K112+4κ,2>\mu\ge M=\tfrac1c\big(\tfrac1{\rho^2}+\tfrac{K_1}6+\tfrac\kappa4\big)+\tfrac{K_1}{12}+4\kappa,2>μ≥M=c1​(ρ21​+6K1​​+4κ​)+12K1​​+4κ,

there are constants C1,C2,C3C_1,C_2,C_3C1​,C2​,C3​ independent of TTT such that for every T≥3T\ge3T≥3, every noise realisation and every choice of the policy's tie-breaking and pair selection,

LPCSLPE(T)≤C3+3log⁡2(log⁡T),LPC^{SLPE}(T)\le C_3+3\log_2(\log T),LPCSLPE(T)≤C3​+3log2​(logT),

and, on every realisation where Assumption 2 and the concentration event ∣Dˉni(piM)−d(piM)∣≤Δi2/ρ2|\bar D_{n_i}(p^M_i)-d(p^M_i)|\le\Delta_i^2/\rho^2∣Dˉni​​(piM​)−d(piM​)∣≤Δi2​/ρ2 hold in each used round,

RSLPE(T)≤(C1+C2log⁡(log⁡T))Tlog⁡T.\mathcal R^{SLPE}(T)\le\big(C_1+C_2\log(\log T)\big)\sqrt T\log T .RSLPE(T)≤(C1​+C2​log(logT))T​logT.

Milestones

  1. Lemma 1 (p. 10): Assumption 1 gives p∗(d′(p)−d′(p∗))≤κ(p−p∗)2p^*(d'(p)-d'(p^*))\le\kappa(p-p^*)^2p∗(d′(p)−d′(p∗))≤κ(p−p∗)2.
  2. Lemma 2 (p. 11): d′′(p∗)=0d''(p^*)=0d′′(p∗)=0 with Lipschitz r′′r''r′′ and d′d'd′ gives the same inequality with κ=Ψ+Ψˉ+2K1\kappa=\Psi+\bar\Psi+2K_1κ=Ψ+Ψˉ+2K1​.
  3. Lemma 3 (p. 17): the identical-noise finite differences of round iii are within 12K1Δi2/12\tfrac12K_1\Delta_i^2/1221​K1​Δi2​/12 of d′d'd′ at the midpoints.
  4. Hoeffding step (pp. 19–20): P(∣Xˉn∣>Δ2/ρ2)≤1/T2\mathbb P(|\bar X_n|>\Delta^2/\rho^2)\le1/T^2P(∣Xˉn​∣>Δ2/ρ2)≤1/T2 for n≥2ρ4log⁡T/Δ4n\ge2\rho^4\log T/\Delta^4n≥2ρ4logT/Δ4 and sub-Gaussian noise with variance proxy at most 1/31/31/3.
  5. Lemma 4 (p. 17): ∣p∗−p~i∗∣≤MΔi2|p^*-\tilde p^*_i|\le M\Delta_i^2∣p∗−p~​i∗​∣≤MΔi2​ on the good event of rounds 1,…,i1,\dots,i1,…,i.
  6. Containment (p. 17): piL≤p∗≤piHp^L_i\le p^*\le p^H_ipiL​≤p∗≤piH​ on the good event of earlier rounds.
  7. Round count (p. 24): at most C+log⁡2(log⁡T)C+\log_2(\log T)C+log2​(logT) rounds start before TTT.

Significance

The result gives a non-parametric pricing policy whose number of price changes is doubly logarithmic, the same order as the number of batches needed in batched multi-armed bandits, while its regret is within log⁡Tlog⁡log⁡T\log T\log\log TlogTloglogT of the Ω(T)\Omega(\sqrt T)Ω(T​) lower bound of Keskin and Zeevi (2014). Its key estimate, Lemma 4, is a perturbation bound for the maximiser of a piecewise linear surrogate of a smooth revenue function; it applies wherever an optimum is located from noisy function values with matched-noise finite differences.

The theorem is proved on paper and, to the extent that can be determined, has no machine-checked proof. Formalizing it adds a continuum-armed pricing policy with an explicit price-change bound, and a checked version of an argument whose printed proof has gaps: a high-probability step that is false as printed, an inequality used two-sidedly that is assumed one-sidedly, and a logarithm base that does not match. Lemma 4 is posed as printed. It is supported numerically but its printed proof is incomplete, so a formal proof, or a counterexample, is itself new information.

Difficulty

The obvious argument for Lemma 4 compares the first-order condition of the surrogate with that of the true revenue. It fails as written: the surrogate's maximiser may sit at an endpoint of [piL,piH][p^L_i,p^H_i][piL​,piH​] or at the kink piMp^M_ipiM​, where no first-order condition holds, and the comparison needs a two-sided bound on d′(p)−d′(p∗)d'(p)-d'(p^*)d′(p)−d′(p∗) while Assumption 1 is one-sided and weighted by p∗p^*p∗. The regret bound then needs the induction that keeps p∗p^*p∗ inside every round's range, a careful treatment of the last round, which the horizon truncates, and the conversion of the doubly exponential decay of Δi\Delta_iΔi​ into a log⁡2log⁡T\log_2\log Tlog2​logT round count.

Formalization scope

Periods are 0-based and rounds 1-based. The demand is d : ℝ → ℝ, and p∗p^*p∗ is a parameter satisfying hypotheses, not a defined argmax. The noise is a single realisation ε : ℕ → ℝ, and the regret and the price-change count are numbers on it, with no expectation. The policy receives only T,μ,ρT,\mu,\rhoT,μ,ρ, an argmax selector (any rule returning a maximiser of a continuous function on an interval), a pair selector (four periods per round), and the observations d(p)+ϵtd(p)+\epsilon_td(p)+ϵt​ at the prices it charges. nin_ini​ is rounded up. The concentration event's probability is the separate Hoeffding milestone.

The following hypotheses and repairs are added and disclosed in each item:

  • Assumption 1 and the bound K1K_1K1​ are imposed on [−1,2][-1,2][−1,2], because SLPE can charge prices outside [0,1][0,1][0,1].
  • p∗<1p^*<1p∗<1, so that the optimum is interior.
  • Assumption 2 is a property of the realisation, not an almost-sure statement, because under i.i.d. continuous noise it has probability zero.
  • The Hoeffding step carries σ2≤1/3\sigma^2\le1/3σ2≤1/3 and T≥2T\ge2T≥2, since the printed 1−1/T21-1/T^21−1/T2 is false for σ≥1\sigma\ge1σ≥1.
  • The round count and Corollary 1 use log⁡2log⁡T\log_2\log Tlog2​logT; the printed natural-log bounds fail numerically (19 price changes against a printed bound of 15.8 at T=106T=10^6T=106).
  • The inner log⁡(T/(2μρ4log⁡T))\log(T/(2\mu\rho^4\log T))log(T/(2μρ4logT)) is replaced by log⁡T\log TlogT, which only changes the constants.
  • Lemma 1 is posed with Assumption 1's own κ\kappaκ, since the printed "∀p ∃κ\forall p\,\exists\kappa∀p∃κ" is trivial.

Four formalizations would make the goal trivial, and the statements rule each out: a policy that reads ddd or p∗p^*p∗, constants allowed to depend on TTT or on the realisation, an argmax or pair oracle not tied to the observations, and an Assumption 2 that no realisation can satisfy (zero noise with in-block pairs satisfies it, and a sanity check exhibits a full instance).

Theorem 2 (the relaxed Assumption 2A and Algorithm 2) is not part of the mission. A complete development needs Taylor's theorem with remainder, sub-Gaussian tail bounds (available as Mathlib's HasSubgaussianMGF and the platform theorem BanditAlgorithm.subgaussian_sample_mean_tail_bound), and bookkeeping for the round schedule. The schedule lemmas and the finite-difference bound are reusable beyond this paper. Proofs of any milestone are welcome, as is a counterexample to Lemma 4's constant.

Selected references

  • G. Perakis and D. Singhvi, Dynamic Pricing with Unknown Non-Parametric Demand and Limited Price Changes, SSRN 3336949 (PDF of 2020-07-03); published in Operations Research. https://ssrn.com/abstract=3336949, https://doi.org/10.1287/opre.2020.0445
  • O. Besbes and A. Zeevi, On the (Surprising) Sufficiency of Linear Models for Dynamic Pricing with Demand Learning, Management Science 61(4), 2015. https://doi.org/10.1287/mnsc.2014.2031
  • W. C. Cheung, D. Simchi-Levi and H. Wang, Dynamic Pricing and Demand Learning with Limited Price Experimentation, Operations Research 65(6), 2017. https://doi.org/10.1287/opre.2017.1629
  • N. B. Keskin and A. Zeevi, Dynamic Pricing with an Unknown Demand Model: Asymptotically Optimal Semi-Myopic Policies, Operations Research 62(5), 2014. https://doi.org/10.1287/opre.2014.1294
  • A. Agarwal, D. P. Foster, D. Hsu, S. M. Kakade and A. Rakhlin, Stochastic Convex Optimization with Bandit Feedback, NeurIPS 2011. https://arxiv.org/abs/1107.1744
  • V. Perchet, P. Rigollet, S. Chassang and E. Snowberg, Batched Bandit Problems, Annals of Statistics 44(2), 2016. https://arxiv.org/abs/1505.00369
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