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Operations ResearchProbabilityStatistics+1·Captain: mikedeng1

Estimating Variance From High, Low and Closing Prices I: S_t(S_t − X_t) + I_t(I_t − X_t) Has Mean σ²t for Brownian Motion With Any DriftResearch Paper

Motivation

The logarithm of a share price is commonly modelled as a Brownian motion with drift, Xt=σBt+ctX_t=\sigma B_t+ctXt​=σBt​+ct. The Black–Scholes option pricing formula needs the volatility σ\sigmaσ but not the drift ccc, so a practitioner must estimate σ2\sigma^2σ2 from data. Observing the whole path would give σ2\sigma^2σ2 exactly through its quadratic variation, but a real observer sees far less. The most readily available daily information is the opening and closing prices together with the day's high and low.

Parkinson (1980) proposed an estimator from the high–low range, and Garman and Klass (1980) found the minimum-variance estimator among a class of quadratic functions of high, low and close. Both were derived assuming zero drift, c=0c=0c=0, and the Garman–Klass estimator is biased when c≠0c\neq0c=0. Rogers and Satchell (Ann. Appl. Probab. 1 (1991) 504–512) proposed the estimator

σ^2≡S1(S1−X1)+I1(I1−X1),\hat\sigma^2\equiv S_1(S_1-X_1)+I_1(I_1-X_1),σ^2≡S1​(S1​−X1​)+I1​(I1​−X1​),

which is unbiased for every drift. Their estimator is now a standard tool in empirical finance for range-based volatility measurement.

Setting

Fix a probability space (Ω,F,P)(\Omega,\mathcal F,P)(Ω,F,P) carrying a standard Brownian motion B=(Bt)t≥0B=(B_t)_{t\ge0}B=(Bt​)t≥0​: B0=0B_0=0B0​=0, its increments over disjoint intervals are independent and Gaussian with variance equal to the length of the interval, and every sample path t↦Bt(ω)t\mapsto B_t(\omega)t↦Bt​(ω) is continuous. Fix a drift c∈Rc\in\mathbb Rc∈R and a volatility σ≥0\sigma\ge0σ≥0. The log-price is

Xt=σBt+ct,t≥0,X_t=\sigma B_t+ct,\qquad t\ge0,Xt​=σBt​+ct,t≥0,

and, for a trading period [0,t][0,t][0,t], the running maximum and running minimum are

St=sup⁡0≤u≤tXu,It=inf⁡0≤u≤tXu.S_t=\sup_{0\le u\le t}X_u,\qquad I_t=\inf_{0\le u\le t}X_u.St​=0≤u≤tsup​Xu​,It​=0≤u≤tinf​Xu​.

Thus StS_tSt​, ItI_tIt​ and XtX_tXt​ are the high, the low and the close of the log-price (with the open normalized to X0=0X_0=0X0​=0). In Lean these are logPrice σ c B t ω, runMax σ c B t ω and runMin σ c B t ω in the namespace RogersSatchell.Unbiased.

The proof in the paper passes through an exponential time: a random variable TTT with P(T>x)=e−λxP(T>x)=e^{-\lambda x}P(T>x)=e−λx (rate λ>0\lambda>0λ>0, mean λ−1\lambda^{-1}λ−1), independent of the whole path BBB. For σ>0\sigma>0σ>0 the rates

α=c2+2λσ2−cσ2,β=c2+2λσ2+cσ2\alpha=\frac{\sqrt{c^2+2\lambda\sigma^2}-c}{\sigma^2},\qquad \beta=\frac{\sqrt{c^2+2\lambda\sigma^2}+c}{\sigma^2}α=σ2c2+2λσ2​−c​,β=σ2c2+2λσ2​+c​

appear, in Lean alpha σ c lam and beta σ c lam.

Formalization targets

Goal: display (3)

For every c∈Rc\in\mathbb Rc∈R, every σ≥0\sigma\ge0σ≥0 and every t≥0t\ge0t≥0, St(St−Xt)+It(It−Xt)S_t(S_t-X_t)+I_t(I_t-X_t)St​(St​−Xt​)+It​(It​−Xt​) is integrable and

E[St(St−Xt)+It(It−Xt)]=σ2t.E\big[S_t(S_t-X_t)+I_t(I_t-X_t)\big]=\sigma^2t.E[St​(St​−Xt​)+It​(It​−Xt​)]=σ2t.

At t=1t=1t=1 this is the unbiasedness of σ^2\hat\sigma^2σ^2 of display (2). The statement quantifies over all drifts; the absence of ccc on the right-hand side is the content.

Milestones (Section 2, pp. 505–506)

  1. At an independent exponential time TTT of rate λ\lambdaλ: ST∼Exp⁡(α)S_T\sim\operatorname{Exp}(\alpha)ST​∼Exp(α) and −IT∼Exp⁡(β)-I_T\sim\operatorname{Exp}(\beta)−IT​∼Exp(β).
  2. The Wiener–Hopf splitting: STS_TST​ and ST−XTS_T-X_TST​−XT​ are independent, and ST−XTS_T-X_TST​−XT​ has the law of −IT-I_T−IT​.
  3. E[ST(ST−XT)]=1/(αβ)=σ2/2λE[S_T(S_T-X_T)]=1/(\alpha\beta)=\sigma^2/2\lambdaE[ST​(ST​−XT​)]=1/(αβ)=σ2/2λ.
  4. E[ST(ST−XT)]=∫0∞λe−λt E[St(St−Xt)] dtE[S_T(S_T-X_T)]=\int_0^\infty\lambda e^{-\lambda t}\,E[S_t(S_t-X_t)]\,dtE[ST​(ST​−XT​)]=∫0∞​λe−λtE[St​(St​−Xt​)]dt.
  5. E[St(St−Xt)]=σ2t/2E[S_t(S_t-X_t)]=\sigma^2t/2E[St​(St​−Xt​)]=σ2t/2 for every t≥0t\ge0t≥0.
  6. E[It(It−Xt)]=σ2t/2E[I_t(I_t-X_t)]=\sigma^2t/2E[It​(It​−Xt​)]=σ2t/2 for every t≥0t\ge0t≥0.
  7. (off the goal's path) With Y1=S1(S1−X1)Y_1=S_1(S_1-X_1)Y1​=S1​(S1​−X1​), Y2=I1(I1−X1)Y_2=I_1(I_1-X_1)Y2​=I1​(I1​−X1​): EY12=EY22=σ4/2E Y_1^2=EY_2^2=\sigma^4/2EY12​=EY22​=σ4/2, E(Y1+Y2)2≤2σ4E(Y_1+Y_2)^2\le2\sigma^4E(Y1​+Y2​)2≤2σ4 and var⁡(σ^2)≤σ4\operatorname{var}(\hat\sigma^2)\le\sigma^4var(σ^2)≤σ4, for every drift ccc.

Significance

The goal certifies a drift-free unbiased volatility estimator built from four numbers per trading day. Because only σ2\sigma^2σ2 enters the Black–Scholes formula, an estimator whose mean does not depend on the nuisance parameter ccc is exactly what is needed. Milestone 7 complements this with a drift-uniform bound on its variance, var⁡(σ^2)≤σ4\operatorname{var}(\hat\sigma^2)\le\sigma^4var(σ^2)≤σ4, while the exact value 0.331σ40.331\sigma^40.331σ4 quoted in the paper is only available at c=0c=0c=0.

On the formalization side, the results are classical and proved; none is machine-checked as far as the platform's catalog shows. A complete development would give the first formal treatment of the joint law of the running maximum of drifted Brownian motion at an exponential time, of the Wiener–Hopf splitting at the maximum, and of a Laplace-inversion argument for a moment function of the time horizon. All three are reusable well beyond volatility estimation: in ruin theory, queueing (reflected Brownian motion), and the pricing of lookback and barrier options.

Difficulty

The obvious approach, computing E[St(St−Xt)]E[S_t(S_t-X_t)]E[St​(St​−Xt​)] directly from the joint density of (St,Xt)(S_t,X_t)(St​,Xt​) for drifted Brownian motion, requires the reflection principle combined with a Girsanov change of measure, followed by a double integral involving Gaussian tails, done separately for each sign of ccc. The cancellation that makes the drift disappear is not visible in that computation, and a statement specialized to c=0c=0c=0 (where the reflection principle alone suffices) does not carry over. Every step of the milestone list rests on path properties of Brownian motion (the strong Markov property, the law of the running maximum, splitting at the maximum) that Mathlib does not yet provide for IsBrownianReal, and the passage from milestone 4 to milestone 5 needs uniqueness of the Laplace transform.

Formalization scope

  • Brownian motion is Mathlib's ProbabilityTheory.IsBrownianReal B P with B : ℝ≥0 → Ω → ℝ, plus the hypothesis that every sample path is continuous (the standard choice of a continuous version). Time is ℝ≥0.
  • StS_tSt​ and ItI_tIt​ are the real sSup/sInf of the path over the interval [0,t][0,t][0,t]; with continuous paths they are attained. The supremum is never taken over all times or in extended reals.
  • "EEE" is the Bochner integral, and every expectation identity also asserts integrability, so no identity can hold through Lean's convention that a non-integrable function integrates to 000.
  • "TTT exponential with mean λ−1\lambda^{-1}λ−1" is HasLaw T (expMeasure λ) P; "parameter α\alphaα" is read as rate α\alphaα. "Independent of BBB" is independence from the path-valued random variable with the product σ-algebra. STS_TST​ is evaluated at TTT truncated to [0,∞)[0,\infty)[0,∞).
  • "Has the same law as" is equality of image measures, together with the almost-everywhere measurability of both maps.
  • "Inversion of the Laplace transform gives" becomes the fixed-time identity for every t≥0t\ge0t≥0 (milestones 5 and 6), separate from the Laplace identity (milestone 4).
  • Milestones 1 and 3 assume σ>0\sigma>0σ>0 because α,β\alpha,\betaα,β divide by σ2\sigma^2σ2; the Wiener–Hopf splitting, the goal, and milestones 4–7 allow σ≥0\sigma\ge0σ≥0.

A formalization that specializes to c=0c=0c=0, takes the supremum over all of [0,∞)[0,\infty)[0,∞), or omits the integrability conjuncts is not the statement of this mission.

Infrastructure that a complete development needs: the reflection principle or the strong Markov property for Brownian motion, the exponential-time law of the running maximum of a Lévy process, and uniqueness of Laplace transforms for continuous functions. All of these are reusable; contributions of any of them are welcome. Related platform items cover other objects and are credited here: running maxima and exit problems for spectrally negative Lévy processes (Avram2004.Exit.reflected), a drifted Brownian motion in characteristic-function form in a queueing-network setting (Reiman84.QueueLength.Paths), and a GI/G/1 Wiener–Hopf transform identity (QueueingFundamentals.GG1.wiener_hopf_transform).

Selected references

  • L. C. G. Rogers and S. E. Satchell, Estimating variance from high, low and closing prices, The Annals of Applied Probability 1(4), 1991, 504–512. https://doi.org/10.1214/aoap/1177005835
  • M. B. Garman and M. J. Klass, On the estimation of security price volatilities from historical data, Journal of Business 53(1), 1980, 67–78. https://doi.org/10.1086/296072
  • M. Parkinson, The extreme value method for estimating the variance of the rate of return, Journal of Business 53(1), 1980, 61–65. https://doi.org/10.1086/296071
  • P. Greenwood and J. Pitman, Fluctuation identities for Lévy processes and splitting at the maximum, Advances in Applied Probability 12(4), 1980, 893–902. https://doi.org/10.2307/1426747
9 thms1 active userReviewed
CombinatoricsGraph Theory·Captain: mikedeng1

Graph Minors. X. Obstructions to Tree-Decomposition III: In the θ-Grid, the Separations of Order < θ With Small E(A) Form a Tangle of Order θResearch Paper

Why a grid has a tangle

Robertson and Seymour introduced tangles as a way to describe a region of a graph that cannot be isolated by a separation of low order. A separation divides the edges into two sides, and its order counts the vertices shared by those sides. A tangle makes a consistent choice of the side regarded as small at every order below a threshold. This turns an informal idea of a highly connected region into an object with explicit axioms. In Graph Minors. X, the authors connect tangles with branch-width, tree-width and grid minors; the grid construction is the direct example behind that connection. The paper states the existence of a tangle of order θ\thetaθ in every θ\thetaθ-grid as (7.3) on p. 173. Robertson and Seymour, 1991.

The result is already proved in the paper. The present target is its Lean statement and proof, together with the two numbered results from §7 on which the construction rests. This mission concerns the grid itself. The paper's further assertion that a grid minor induces a tangle in a larger graph uses the separate minor-transfer result (6.1), whose edge identities require additional definitions. Robertson and Seymour, 1991, pp. 170–173.

The grid, its edge boundary and its small sets

Fix an integer θ≥2\theta\ge2θ≥2. The θ\thetaθ-grid GGG has vertices (i,j)(i,j)(i,j) for 1≤i,j≤θ1\le i,j\le\theta1≤i,j≤θ. Two vertices are adjacent exactly when their coordinate differences have absolute values summing to one. For each iii, PiP_iPi​ is the horizontal row with vertices (i,1),…,(i,θ)(i,1),\ldots,(i,\theta)(i,1),…,(i,θ); for each jjj, QjQ_jQj​ is the vertical column. Write E(Pi)E(P_i)E(Pi​) and E(Qj)E(Q_j)E(Qj​) for their edge sets. The Lean development uses the already published definition of this same simple graph, with coordinates shifted to start at zero. The shift changes no adjacency or row and column relation. Robertson and Seymour, 1991, p. 171.

For an edge set X⊆E(G)X\subseteq E(G)X⊆E(G), the edge boundary ∂(X)\partial(X)∂(X) consists of vertices incident both with an edge in XXX and with an edge outside XXX. The source prints “vertices v∈Xv\in Xv∈X” when introducing this set. Since XXX is a set of edges, this is a type slip; the two incidence conditions give the intended reading. An edge set is small if ∣∂(X)∣<θ|\partial(X)|<\theta∣∂(X)∣<θ and it contains no complete row edge set E(Pi)E(P_i)E(Pi​). These are two separate requirements. An edge set can have a small boundary while still containing a whole row. Robertson and Seymour, 1991, pp. 171–172.

A subhypergraph AAA specifies subsets V(A)V(A)V(A) and E(A)E(A)E(A) of the grid's vertices and edges, retaining the incidences of the ambient grid. A separation (A,B)(A,B)(A,B) satisfies A∪B=GA\cup B=GA∪B=G and E(A∩B)=∅E(A\cap B)=\varnothingE(A∩B)=∅; its order is ∣V(A∩B)∣|V(A\cap B)|∣V(A∩B)∣. Although the grid is a simple graph, these are the paper's hypergraph definitions. A tangle T\mathcal TT of order θ\thetaθ contains only separations of order below θ\thetaθ and satisfies three axioms: it chooses an orientation of every such separation; the union of the first sides of any three chosen separations is not GGG; and no chosen first side contains every vertex of GGG. The chosen three may coincide. Robertson and Seymour, 1991, pp. 153–154.

Formalization targets

The first milestone, (7.1), identifies a symmetry between rows and columns under a low boundary:

∣∂(X)∣<θ⟹(∃i, E(Pi)⊆X)⟺(∃j, E(Qj)⊆X).|\partial(X)|<\theta\quad\Longrightarrow\quad \bigl(\exists i,\ E(P_i)\subseteq X\bigr) \Longleftrightarrow \bigl(\exists j,\ E(Q_j)\subseteq X\bigr).∣∂(X)∣<θ⟹(∃i, E(Pi​)⊆X)⟺(∃j, E(Qj​)⊆X).

The second milestone, (7.2), says that three small edge sets cannot cover all the grid's edges:

X1∪X2∪X3=E(G)⟹¬(X1,X2,X3 are all small).X_1\cup X_2\cup X_3=E(G) \quad\Longrightarrow\quad \neg\bigl(X_1,X_2,X_3\text{ are all small}\bigr).X1​∪X2​∪X3​=E(G)⟹¬(X1​,X2​,X3​ are all small).

The goal, (7.3), defines Tθ\mathcal T_\thetaTθ​ rather than taking it as an arbitrary set. It selects precisely the separations (A,B)(A,B)(A,B) of order less than θ\thetaθ for which E(A)E(A)E(A) is small, and asserts

Tθ is a tangle in G of order θ.\mathcal T_\theta\text{ is a tangle in }G\text{ of order }\theta.Tθ​ is a tangle in G of order θ.

These are the numbered §7 results on pp. 171–173, in the order used by the paper. Robertson and Seymour, 1991, pp. 171–173.

What the result supplies

The theorem gives an explicit tangle in a familiar graph for every order θ≥2\theta\ge2θ≥2. A tangle is more than a numerical connectivity bound: it records coherent choices across all separations below its order. In the paper, the grid tangle feeds the link between large grids and tangles of high order. The extension from a grid minor in another graph to a tangle of that graph invokes (6.1), beyond this mission's goal. The converse direction, that large tree-width forces a large grid minor, is (7.4), proved in Graph Minors V (Robertson and Seymour, 1986); the published definitions and statements of that paper on this platform are about grid minors and tree-width, not tangles. Robertson and Seymour, 1991, pp. 170, 173.

Formalizing (7.3) will make the grid tangle available as a checked object alongside the already published grid graph. It will also produce reusable definitions for an edge boundary, small edge sets and the paper's hypergraph separations. The Lean files here are draft statements with open proofs; the published 1986 grid definition is the existing checked ingredient. No machine-checked proof of (7.1), (7.2) or (7.3) is claimed by this proposal.

Where the difficulty lies

The obvious attempt at (7.2) counts boundary vertices column by column. If every column QjQ_jQj​ has all its edges in X1∪X2X_1\cup X_2X1​∪X2​ and meets both sets, each column contributes at least two vertices to ∣∂(X1)∣+∣∂(X2)∣|\partial(X_1)|+|\partial(X_2)|∣∂(X1​)∣+∣∂(X2​)∣, so the two boundaries together have at least 2θ2\theta2θ vertices. This only works when the third set misses the first and last rows; in general the third set can absorb edges of every column, and no single count over the whole grid bounds all three boundaries at once. The statement is a covering property of three sets, not a bound on any one of them, and the paper's argument for it is credited to D. Kleitman and M. Saks. The goal must then meet all three tangle axioms. The page's proof of (7.3) argues the first axiom and says only that the rest follows from (7.2); the third axiom, V(A)≠V(G)V(A)\ne V(G)V(A)=V(G), is part of the definition and must be established, not dropped. Robertson and Seymour, 1991, pp. 172–173.

Formalization scope

The source assumes finite hypergraphs throughout, and §7 fixes θ≥2\theta\ge2θ≥2. Lean uses a finite simple graph on Fin θ × Fin θ, reusing RobertsonSeymour1986.GM5.grid, and views its edge set as the edge type of a local hypergraph. Subhypergraphs hold vertex and edge subsets with inherited incidence. Set.ncard counts boundary vertices and separation order. Rows and columns use all grid edges whose two endpoints have the specified coordinate. This representation keeps every grid edge's identity, even though it is written as a SimpleGraph edge subtype.

IsSmall retains both ∣∂(X)∣<θ|\partial(X)|<\theta∣∂(X)∣<θ and the exclusion of full row edge sets. boundary requires an incident edge on each side of XXX. Both details are necessary for the claimed tangle: an IsSmall without the row clause would call every set with a small boundary small, including sets that contain whole rows, and the resulting set of separations is not a tangle; a boundary defined with "every edge outside XXX" instead of "some edge outside XXX" would be empty and make the size condition vacuous. The formalization keeps the third tangle axiom and does not replace it with an easier condition. The definitions of hypergraph, separation and tangle duplicate the shared encoding used by the other missions for this paper and can later be consolidated. The definitions also include the paper's tangle number and maximum edge size for that shared layer, though the grid goal does not invoke them; on finite inputs their maxima are bounded, and their empty-set value is zero.

The companion missions are Graph Minors. X. Obstructions to Tree-Decomposition I: Tangle Number Equals max(Branch-Width, Largest Edge Size), max(β(G), γ(G)) = θ(G); Graph Minors. X. Obstructions to Tree-Decomposition II: Branch-Width and Tree-Width Satisfy max(β, γ) ≤ ω + 1 ≤ max(⌊3β/2⌋, γ, 1); Graph Minors. X. Obstructions to Tree-Decomposition IV: Mutually Distinguishable Tangles Have a Tree-Decomposition Separating Them by Their Distinctions; and Graph Minors. X. Obstructions to Tree-Decomposition V: A θ-Pervasive Class of Designs Gives a Tree-Decomposition over 𝒮^{3θ−2} ∪ ℛ_{4θ−3}. Those missions address the paper's other main results; this one isolates the grid construction.

Selected references

  • N. Robertson and P. D. Seymour, Graph Minors. X. Obstructions to Tree-Decomposition, Journal of Combinatorial Theory, Series B 52 (1991), 153–190. DOI: 10.1016/0095-8956(91)90061-n.
  • N. Robertson and P. D. Seymour, Graph Minors. V. Excluding a Planar Graph, Journal of Combinatorial Theory, Series B 41 (1986), 92–114. DOI: 10.1016/0095-8956(86)90030-4.
9 thms1 active userReviewed
CombinatoricsGraph Theory·Captain: mikedeng1

Graph Minors. X. Obstructions to Tree-Decomposition V: A θ-Pervasive Class of Designs Gives a Tree-Decomposition over 𝒮^{3θ−2} ∪ ℛ_{4θ−3}Research Paper

Motivation

Tangles were introduced by Robertson and Seymour in Graph Minors. X (JCTB 1991) to make precise the idea of a "highly connected region" of a graph. A tangle orients every low-order separation of the graph towards one side, consistently. They are the organising notion of the later papers of the Graph Minors series, which culminate in the graph structure theorem and the proof of Wagner's conjecture.

Section 11 of Graph Minors X, Structure relative to a tangle, asks how local and global structure are related. In the paper's words: suppose that GGG has large tangle number, but relative to each high-order tangle the graph has a structure of a certain kind XXX. What can be inferred about the global structure of GGG? One might guess that GGG has a tree-decomposition into pieces each with structure XXX, but that is false. The theorem of §11 shows that GGG does have a tree-decomposition into pieces which almost have structure XXX. The authors state that they need this for an application in a later paper of the series, cited as [6], Graph minors. XVII. Excluding a non-planar graph (submitted); it appeared as Graph Minors XVI (2003), where the local structure relative to a tangle is a near-embedding in a surface.

Setting

A hypergraph GGG has a finite vertex set V(G)V(G)V(G), a finite edge set E(G)E(G)E(G) and an incidence relation. A subhypergraph G′⊆GG' \subseteq GG′⊆G has V(G′)⊆V(G)V(G') \subseteq V(G)V(G′)⊆V(G) and E(G′)⊆E(G)E(G') \subseteq E(G)E(G′)⊆E(G), with every end of an edge of G′G'G′ in V(G′)V(G')V(G′). A separation of GGG is a pair (A,B)(A, B)(A,B) of subhypergraphs with A∪B=GA \cup B = GA∪B=G and E(A∩B)=∅E(A \cap B) = \emptysetE(A∩B)=∅, and its order is ∣V(A∩B)∣|V(A \cap B)|∣V(A∩B)∣.

For θ≥1\theta \ge 1θ≥1, a tangle of order θ\thetaθ in GGG is a set T\mathcal TT of separations of order <θ< \theta<θ such that (i) for each separation (A,B)(A, B)(A,B) of order <θ< \theta<θ one of (A,B)(A,B)(A,B), (B,A)(B,A)(B,A) is in T\mathcal TT; (ii) no three members (Ai,Bi)(A_i, B_i)(Ai​,Bi​) of T\mathcal TT have A1∪A2∪A3=GA_1 \cup A_2 \cup A_3 = GA1​∪A2​∪A3​=G; (iii) V(A)≠V(G)V(A) \ne V(G)V(A)=V(G) for (A,B)∈T(A, B) \in \mathcal T(A,B)∈T.

A tree-decomposition (T,τ)(T, \tau)(T,τ) of GGG is a tree TTT and subhypergraphs τ(t)\tau(t)τ(t), t∈V(T)t \in V(T)t∈V(T), whose union is GGG, which are pairwise edge-disjoint, and with τ(t)∩τ(t′′)⊆τ(t′)\tau(t) \cap \tau(t'') \subseteq \tau(t')τ(t)∩τ(t′′)⊆τ(t′) whenever t′t't′ lies on the path of TTT between ttt and t′′t''t′′.

A design is a pair (H,M)(H, M)(H,M) of a hypergraph HHH and a set MMM of subsets of V(H)V(H)V(H).

  • The design of a node t0t_0t0​ of (T,τ)(T, \tau)(T,τ) with neighbours t1,…,tkt_1, \dots, t_kt1​,…,tk​ is (τ(t0),{V(τ(t0)∩τ(ti))})(\tau(t_0), \{V(\tau(t_0) \cap \tau(t_i))\})(τ(t0​),{V(τ(t0​)∩τ(ti​))}). A tree-decomposition is over a class S\mathcal SS of designs if the design of every node belongs to S\mathcal SS.
  • (H′,M′)(H', M')(H′,M′) is an nnn-enlargement of (H,M)(H, M)(H,M) if, for some Z⊆V(H′)Z \subseteq V(H')Z⊆V(H′) with ∣Z∣≤n|Z| \le n∣Z∣≤n, H⊆H′H \subseteq H'H⊆H′, V(H′)−V(H)⊆ZV(H') - V(H) \subseteq ZV(H′)−V(H)⊆Z, E(H′)⊆E(H)E(H') \subseteq E(H)E(H′)⊆E(H), and X∩V(H)∈MX \cap V(H) \in MX∩V(H)∈M for every X∈M′X \in M'X∈M′ other than ZZZ. Sn\mathcal S^nSn is the class of nnn-enlargements of members of S\mathcal SS, and Rn\mathcal R_nRn​ is the class of designs with at most nnn vertices.
  • A location in G′G'G′ is a set of separations (Ai,Bi)(A_i, B_i)(Ai​,Bi​) of G′G'G′ with Ai⊆BjA_i \subseteq B_jAi​⊆Bj​ for i≠ji \ne ji=j. Its design is (G′∩B1∩⋯∩Bk,{V(Ai∩Bi)})(G' \cap B_1 \cap \dots \cap B_k, \{V(A_i \cap B_i)\})(G′∩B1​∩⋯∩Bk​,{V(Ai​∩Bi​)}).
  • A class S\mathcal SS is θ\thetaθ-pervasive in GGG if for every subhypergraph G′⊆GG' \subseteq GG′⊆G and every tangle T\mathcal TT in G′G'G′ of order ≥θ\ge \theta≥θ, some location L⊆T\mathcal L \subseteq \mathcal TL⊆T in G′G'G′ has its design in S\mathcal SS.
  • The ZZZ-extension of (H,M)(H, M)(H,M) is (H,M∪{Z})(H, M \cup \{Z\})(H,M∪{Z}).

Formalization targets

Goal: (11.1), p. 185

For θ≥1\theta \ge 1θ≥1 and a class S\mathcal SS that is θ\thetaθ-pervasive in GGG,

G has a tree-decomposition over S3θ−2∪R4θ−3.G \text{ has a tree-decomposition over } \mathcal S^{3\theta-2} \cup \mathcal R_{4\theta-3}.G has a tree-decomposition over S3θ−2∪R4θ−3​.

Milestone: (11.2), pp. 185–186

If S\mathcal SS is θ\thetaθ-pervasive in GGG and ∣Z∣=3θ−2|Z| = 3\theta - 2∣Z∣=3θ−2, then either some separation (A,B)(A, B)(A,B) of order <θ< \theta<θ has

∣(Z∪V(A))∩V(B)∣, ∣(Z∪V(B))∩V(A)∣≤3θ−3,|(Z \cup V(A)) \cap V(B)|,\ |(Z \cup V(B)) \cap V(A)| \le 3\theta - 3,∣(Z∪V(A))∩V(B)∣, ∣(Z∪V(B))∩V(A)∣≤3θ−3,

or some location {(Ai,Bi)}\{(A_i, B_i)\}{(Ai​,Bi​)} in GGG with design in S\mathcal SS has ∣Z∩V(Ai)∣≤∣V(Ai∩Bi)∣<θ|Z \cap V(A_i)| \le |V(A_i \cap B_i)| < \theta∣Z∩V(Ai​)∣≤∣V(Ai​∩Bi​)∣<θ for all iii.

Milestone: (11.3), p. 186

If ∣Z∣≤3θ−2|Z| \le 3\theta - 2∣Z∣≤3θ−2, there is a tree-decomposition of GGG over S′=S3θ−2∪R4θ−3\mathcal S' = \mathcal S^{3\theta-2} \cup \mathcal R_{4\theta-3}S′=S3θ−2∪R4θ−3​ with a node t0t_0t0​ such that Z⊆V(τ(t0))Z \subseteq V(\tau(t_0))Z⊆V(τ(t0​)) and the ZZZ-extension of the design of t0t_0t0​ is in S′\mathcal S'S′. The goal is the case Z=∅Z = \emptysetZ=∅.

Companion: the remark on p. 188

For every θ≥1\theta \ge 1θ≥1, if GGG has no tangle of order θ\thetaθ, then

ω(G)≤4θ−4.\omega(G) \le 4\theta - 4.ω(G)≤4θ−4.

Consequently ω(G)≤4θ(G)\omega(G) \le 4\theta(G)ω(G)≤4θ(G), where θ(G)\theta(G)θ(G) is the tangle number. This is the p. 188 remark following (11.3).

Significance

(11.1) converts local information, stated tangle by tangle, into a global decomposition. Every piece of the decomposition is either small (at most 4θ−34\theta - 34θ−3 vertices) or differs from a structure in S\mathcal SS by at most 3θ−23\theta - 23θ−2 added vertices. This is the kind of local-to-global step the later Graph Minors papers need: there the local structure near each high-order tangle is a near-embedding in a surface, and a result of this shape glues such local structures along a tree. With S=∅\mathcal S = \emptysetS=∅ it gives a tree-width bound ω(G)≤4θ(G)\omega(G) \le 4\theta(G)ω(G)≤4θ(G), a weaker form of the tangle/tree-width duality.

The result has been proved since 1991. To our knowledge no proof assistant formalizes it, and none formalizes the hypergraph tangles or tree-decompositions of this paper. This mission produces machine-checked statements of the paper's notions of design, enlargement, location and pervasiveness, the structure theorem, and its inductive strengthening.

Difficulty

The first idea is to take the pieces in S\mathcal SS themselves as the pieces of the tree-decomposition. That fails, and the paper says so: the pieces can only almost have the structure. Locations for different tangles interact, and the decomposition must absorb up to 3θ−23\theta - 23θ−2 extra vertices into each piece. The induction also has to control a set ZZZ of attachment vertices of bounded size: a piece built at one node must still accept the vertices through which it is glued to the rest of the tree. Keeping ∣Z∣≤3θ−2|Z| \le 3\theta - 2∣Z∣≤3θ−2 throughout the recursion is the delicate point, and it is why the strengthened statement (11.3), not (11.1), is the one that admits induction.

Formalization scope

  • Hypergraphs. A hypergraph is a structure Hypergraph V E with an incidence relation. Finiteness is [Finite V] [Finite E] on every theorem. Subhypergraphs, separations, tangles and tree-decompositions are the series' shared encodings (namespace RobertsonSeymour1991.GM10.Structure). The tree of a tree-decomposition is a SimpleGraph on Fin n satisfying IsTree.
  • Designs. Every design the statements involve has as hypergraph a subhypergraph of the fixed GGG. So a design is a GGG-design G.Sub × Set (Set V), and a class of designs is a set of GGG-designs. Classes need not be closed under isomorphism; the paper never uses that.
  • Relative tangles. Separations, tangles and locations in a subhypergraph G′G'G′ are pairs of subhypergraphs of GGG whose union is G′G'G′. For G′=GG' = GG′=G they agree definitionally with the absolute notions.
  • Pervasiveness. It quantifies over every subhypergraph G′G'G′ and every order θ′≥θ\theta' \ge \thetaθ′≥θ. Restricting to G′=GG' = GG′=G would be a different, stronger theorem. The paper's opening remark in the proof of (11.3), that pervasiveness passes to subhypergraphs, is immediate in this encoding and is not a separate item.
  • Edge cases. The empty set is a location; its design is (G′,∅)(G', \emptyset)(G′,∅).
  • Integer arithmetic. Since θ≥1\theta \ge 1θ≥1, the bounds 3θ−23\theta-23θ−2, 3θ−33\theta-33θ−3 and 4θ−34\theta-34θ−3 are exact natural numbers. Tree-width is an integer, and it is −1-1−1 for an empty vertex set.
  • No trivial instances. IsPervasive is satisfiable: the class of all designs is θ\thetaθ-pervasive, through the empty location. The conclusion is satisfiable too: the one-node decomposition lies over R∣V(G)∣\mathcal R_{|V(G)|}R∣V(G)∣​. So neither the hypothesis nor the conclusion of (11.1) is vacuous.

The other main results of the paper are separate missions of this series:

  • Graph Minors. X. Obstructions to Tree-Decomposition I (tangle number versus branch-width);
  • II (branch-width versus tree-width);
  • III (the grid tangle);
  • IV (the tree-decomposition separating mutually distinguishable tangles).

Contributions are welcome on any item: proofs of (11.2) and (11.3), and of the p. 188 companion. The companion needs two auxiliary facts: a tangle of order ≥θ\ge \theta≥θ in a subhypergraph yields one of order θ\thetaθ in GGG, and tree-width is bounded by bag size.

Selected references

  • N. Robertson, P. D. Seymour, Graph Minors. X. Obstructions to Tree-Decomposition, J. Combin. Theory Ser. B 52 (1991) 153–190. https://doi.org/10.1016/0095-8956(91)90061-n
  • N. Robertson, P. D. Seymour, Graph Minors. XVI. Excluding a non-planar graph, J. Combin. Theory Ser. B 89 (2003) 43–76. https://doi.org/10.1016/S0095-8956(03)00042-X
  • N. Robertson, P. D. Seymour, Graph Minors. V. Excluding a planar graph, J. Combin. Theory Ser. B 41 (1986) 92–114. https://doi.org/10.1016/0095-8956(86)90030-4
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CombinatoricsGraph Theory·Captain: mikedeng1

Graph Minors. X. Obstructions to Tree-Decomposition II: Branch-Width and Tree-Width Satisfy max(β, γ) ≤ ω + 1 ≤ max(⌊3β/2⌋, γ, 1)Research Paper

Motivation

Tree-width measures how closely a graph resembles a tree. It is the central width parameter of the Graph Minors series of N. Robertson and P. D. Seymour, which proves that finite graphs are well-quasi-ordered by the minor relation, and it governs the complexity of many algorithms: problems that are NP-hard in general become solvable in linear time on graphs of bounded tree-width (Courcelle's theorem). Branch-width, introduced in Graph Minors X (Robertson, Seymour 1991), is a second width parameter, defined from ternary trees whose leaves carry the edges of the graph. It is the natural parameter for the paper's main minimax theorem, which equates branch-width with the maximum order of a tangle, the obstruction to small decompositions.

Section 5 of Graph Minors X shows that the two parameters are equivalent, within a factor 3/2. This is what transfers the tangle duality from branch-width to tree-width, and it is why later work (for instance on matroid branch-width and on rank-width) treats branch-width as an interchangeable substitute for tree-width.

Setting

All objects are finite. A hypergraph GGG has a vertex set V(G)V(G)V(G), an edge set E(G)E(G)E(G), and an incidence relation; the ends of an edge are the vertices incident with it, and an edge may have any number of ends. γ(G)\gamma(G)γ(G) is the maximum number of ends of an edge, or 000 if E(G)=∅E(G)=\emptysetE(G)=∅. A subhypergraph consists of subsets of V(G)V(G)V(G) and E(G)E(G)E(G) such that every end of a chosen edge is a chosen vertex; unions, intersections and inclusion of subhypergraphs are taken setwise.

A tree is a connected non-null graph without circuits; its leaves are its vertices of valency at most 111, and it is ternary if every valency is 111 or 333.

A branch-decomposition of GGG is a pair (T,τ)(T,\tau)(T,τ) with TTT a ternary tree and τ\tauτ a bijection from the leaves of TTT onto E(G)E(G)E(G). The order of an edge fff of TTT is the number of vertices vvv of GGG such that vvv is an end both of an edge labelling a leaf in one component of T∖fT\setminus fT∖f and of an edge labelling a leaf in the other. The width of (T,τ)(T,\tau)(T,τ) is the maximum order of an edge of TTT, and the branch-width β(G)\beta(G)β(G) is the minimum width, or 000 if ∣E(G)∣≤1|E(G)|\le 1∣E(G)∣≤1.

A tree-decomposition of GGG is a pair (T,τ)(T,\tau)(T,τ) with TTT a tree and τ(t)\tau(t)τ(t) a subhypergraph of GGG for every t∈V(T)t\in V(T)t∈V(T), such that

  1. the union of all τ(t)\tau(t)τ(t) is GGG;
  2. for distinct t,t′t,t't,t′, the parts τ(t)\tau(t)τ(t) and τ(t′)\tau(t')τ(t′) share no edge;
  3. if t′t't′ lies on the path of TTT between ttt and t′′t''t′′, then τ(t)∩τ(t′′)⊆τ(t′)\tau(t)\cap\tau(t'')\subseteq\tau(t')τ(t)∩τ(t′′)⊆τ(t′).

Its width is max⁡t (∣V(τ(t))∣−1)\max_t\,(|V(\tau(t))|-1)maxt​(∣V(τ(t))∣−1), and the tree-width ω(G)\omega(G)ω(G) is the minimum width; ω(G)=−1\omega(G)=-1ω(G)=−1 exactly when V(G)=∅V(G)=\emptysetV(G)=∅. Each part is a subhypergraph and each edge lies in exactly one part, which differs from the familiar vertex-bag tree-decompositions of graphs, but gives the same tree-width on graphs.

The tangle number θ(G)\theta(G)θ(G) is the maximum order of a tangle in GGG (p. 154), or 000 if there are none.

Formalization targets

Goal: (5.1)

max⁡(β(G),γ(G))  ≤  ω(G)+1  ≤  max⁡(⌊32β(G)⌋, γ(G), 1)for every finite hypergraph G.\max\bigl(\beta(G),\gamma(G)\bigr)\;\le\;\omega(G)+1\;\le\;\max\bigl(\lfloor\tfrac32\beta(G)\rfloor,\ \gamma(G),\ 1\bigr)\qquad\text{for every finite hypergraph } G.max(β(G),γ(G))≤ω(G)+1≤max(⌊23​β(G)⌋, γ(G), 1)for every finite hypergraph G.

Milestones

  • Second inequality of (5.1): ω(G)+1≤max⁡(⌊32β(G)⌋,γ(G),1)\omega(G)+1\le\max(\lfloor\tfrac32\beta(G)\rfloor,\gamma(G),1)ω(G)+1≤max(⌊23​β(G)⌋,γ(G),1).
  • Claims (1), (2), (3) of the proof of (5.1), under the proof's standing assumptions γ(G)>0\gamma(G)>0γ(G)>0, ∣E(G)∣≥2|E(G)|\ge 2∣E(G)∣≥2 and no isolated vertices: there is a tree-decomposition of width ω(G)\omega(G)ω(G) in which (1) every edge eee is the only edge of a leaf part whose vertices are exactly the ends of eee, and parts at vertices of valency ≥2\ge2≥2 have no edges; (2) moreover every leaf part has exactly one edge; (3) moreover every vertex of TTT has valency at most 333. The claims are cumulative.
  • First inequality of (5.1): max⁡(β(G),γ(G))≤ω(G)+1\max(\beta(G),\gamma(G))\le\omega(G)+1max(β(G),γ(G))≤ω(G)+1.

Companion: (5.2)

θ(G)  ≤  ω(G)+1  ≤  32 θ(G).\theta(G)\;\le\;\omega(G)+1\;\le\;\tfrac32\,\theta(G).θ(G)≤ω(G)+1≤23​θ(G).

Significance

The result. (5.1) shows that branch-width and tree-width bound each other up to the factor 3/23/23/2 and the edge-size correction, and the page records that both bounds are attained (KnK_nKn​ with 3∣n3\mid n3∣n for the right-hand side, Kn,nK_{n,n}Kn,n​ minus a perfect matching for the left-hand side). Together with the minimax theorem (4.3) of the same paper, max⁡(β(G),γ(G))=θ(G)\max(\beta(G),\gamma(G))=\theta(G)max(β(G),γ(G))=θ(G) unless γ(G)=0\gamma(G)=0γ(G)=0 and V(G)≠∅V(G)\ne\emptysetV(G)=∅, it yields (5.2): tangles are, up to the factor 3/23/23/2, the exact obstruction to tree-decompositions of small width. That duality is the form in which tree-width enters the later papers of the Graph Minors series.

Formalizing it. The result is proved (1991); no machine-checked proof of it is known to exist. The platform holds tree-width statements for simple graphs with vertex bags (Graph Minors V, RobertsonSeymour1986.GM5.treewidth_le_theta9 and excluding_planar_graph), which are a different theorem about a different object. This mission formalizes the hypergraph tree-decomposition and branch-decomposition of Graph Minors X and the comparison between them. The companion missions of this series are Graph Minors. X. Obstructions to Tree-Decomposition I (the minimax theorem (4.3)), III (the grid tangle (7.3)), IV (the tree-decomposition separating distinguishable tangles (10.3)) and V (the structure theorem (11.1)).

Difficulty

The second inequality converts a branch-decomposition into a tree-decomposition; the difficulty is to obtain the bound with the floor ⌊32β⌋\lfloor\tfrac32\beta\rfloor⌊23​β⌋ and the separate γ(G)\gamma(G)γ(G) term exactly, not up to an additive error.

The first inequality is where the obvious approach stalls: a tree-decomposition of minimum width is not a branch-decomposition. Its tree may have vertices of any valency, its leaves may carry no edge or several, and an edge may sit at an internal vertex. The three claims of the proof normalize an optimal tree-decomposition step by step without increasing its width. Each step modifies a tree on a finite vertex type while preserving three structural conditions (covering, edge-disjointness, the path condition), and the final step, suppressing vertices of valency 222, must be shown to produce a ternary tree with the edge orders bounded by part sizes. Most of the formal work is this tree surgery.

Formalization scope

  • Every theorem quantifies over types V, E with [Finite V] [Finite E] (the paper's "all hypergraphs in this paper are finite", p. 154) and a hypergraph G : Hypergraph V E given by its incidence relation.
  • Trees are SimpleGraph (Fin n) with IsTree (connected, hence non-null, and acyclic). A leaf is a vertex of valency at most 111; valency is (T.neighborSet t).ncard.
  • A branch-decomposition stores τ\tauτ as its inverse, an injective map from edges onto the leaves. β(G)\beta(G)β(G) is set to 000 when ∣E(G)∣≤1|E(G)|\le1∣E(G)∣≤1 and is otherwise the sInf of the widths, which is a genuine minimum because a branch-decomposition exists when ∣E(G)∣≥2|E(G)|\ge2∣E(G)∣≥2.
  • Widths of tree-decompositions are integers, so that ω(G)=−1\omega(G)=-1ω(G)=−1 when V(G)=∅V(G)=\emptysetV(G)=∅. ω(G)\omega(G)ω(G) is the sInf in Z\mathbb ZZ of all www bounding every ∣V(τ(t))∣−1|V(\tau(t))|-1∣V(τ(t))∣−1; the set is nonempty (one-vertex tree with τ=G\tau=Gτ=G) and bounded below by −1-1−1, so the sInf is the minimum width and not a junk value.
  • ⌊32β(G)⌋\lfloor\tfrac32\beta(G)\rfloor⌊23​β(G)⌋ is the natural-number division 3 * β / 2; the ceiling would be a weaker statement. In (5.2), ω(G)+1≤32θ(G)\omega(G)+1\le\tfrac32\theta(G)ω(G)+1≤23​θ(G) is stated as 2(ω(G)+1)≤3θ(G)2(\omega(G)+1)\le3\theta(G)2(ω(G)+1)≤3θ(G), which is equivalent.
  • The claims read "we may assume X" as "some tree-decomposition of width ω(G)\omega(G)ω(G) satisfies X", under the proof's standing assumptions γ(G)>0\gamma(G)>0γ(G)>0, ∣E(G)∣≥2|E(G)|\ge2∣E(G)∣≥2 and no isolated vertices (p. 168).
  • Condition (ii) of a tree-decomposition, edge-disjointness of the parts, is kept as on the page. Replacing it by "every edge lies in some part", or allowing an empty tree, would change the tree-width and trivialize the comparison; both are ruled out.

Infrastructure needed and reusable beyond this mission: tree surgery on SimpleGraph (Fin n) (attaching a leaf, deleting a leaf, splitting a vertex, suppressing valency-2 vertices), the existence of branch-decompositions for ∣E∣≥2|E|\ge2∣E∣≥2, and the computation of sInf-defined widths. Contributions of such lemmas, of proofs of the individual claims, and of small examples (KnK_nKn​, grids) are welcome.

Selected references

  • N. Robertson, P. D. Seymour, Graph Minors. X. Obstructions to Tree-Decomposition, J. Combin. Theory Ser. B 52 (1991) 153–190. https://doi.org/10.1016/0095-8956(91)90061-n
  • N. Robertson, P. D. Seymour, Graph Minors. V. Excluding a Planar Graph, J. Combin. Theory Ser. B 41 (1986) 92–114. https://doi.org/10.1016/0095-8956(86)90030-4
  • B. Courcelle, The monadic second-order logic of graphs. I. Recognizable sets of finite graphs, Information and Computation 85 (1990) 12–75. https://doi.org/10.1016/0890-5401(90)90043-H
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🏆Completed
Number Theory·Captain: xuanji

Every Odd Number Greater Than 1 is the Sum of at Most 41 PrimesResearch Paper

Motivation

Schnirelmann showed around 1930, by elementary means, that some absolute constant kkk makes every integer n>1n > 1n>1 a sum of at most kkk primes. For odd nnn:

  • Schnirelmann (1930s): some finite kkk, by elementary methods.
  • Klimov, Pil'tai, Sheptitskaya (1972): 115115115; Riesel–Vaughan (1983): 191919 for all integers, using zero-based prime-counting estimates.
  • Ramaré (1995): every even integer is a sum of at most six primes, so every odd n>1n > 1n>1 is a sum of at most seven. (Ann. Sc. Norm. Super. Pisa, 1995)
  • Tao (2014): at most five primes. (arXiv:1201.6656)
  • Helfgott (2013): every odd n>5n > 5n>5 is a sum of three primes. (arXiv:1312.7748)

The campaign's earlier values (100 001100\,001100001 down to 858585) came from Schnirelmann's method with every constant written out, using Chebyshev-type lower bounds for π(y)\pi(y)π(y) and a Selberg sieve whose singular-series weight C(s)C(s)C(s) was crude. The 858585 entry hit the limit of that crude weight. This entry replaces it by the sharp weight K(s)=∏p∣s, p>2p−1p−2K(s) = \prod_{p \mid s,\, p > 2} \frac{p-1}{p-2}K(s)=∏p∣s,p>2​p−2p−1​, using the platform's proved prime-pair sieve (TaoFivePrimes.siebert_prime_pair_bound, Siebert's bound as used by Riesel–Vaughan) and its PrimePairSieve components. No zeta-zero input is used.

Setting

A representation of nnn as a sum of at most kkk primes is a finite multiset of primes summing to nnn with at most kkk elements counted with multiplicity. The Schnirelmann density of A⊆Z≥0A \subseteq \mathbb{Z}_{\ge 0}A⊆Z≥0​ is σ(A)=inf⁡N≥1∣A∩{1,…,N}∣/N\sigma(A) = \inf_{N \ge 1} |A \cap \{1, \dots, N\}|/Nσ(A)=infN≥1​∣A∩{1,…,N}∣/N (Mathlib: schnirelmannDensity).

Formalization target

Goal

∀n∈N,n odd, n>1  ⟹  ∃ s multiset of primes, ∣s∣≤41, ∑s=n.\forall n \in \mathbb{N},\quad n \text{ odd},\ n > 1 \implies \exists\, s \text{ multiset of primes},\ |s| \le 41,\ \textstyle\sum s = n.∀n∈N,n odd, n>1⟹∃s multiset of primes, ∣s∣≤41, ∑s=n.

This is the campaign template with the value 414141 filled in.

How the bound arises

Let B={(p−3)/2:p odd prime}B = \{(p-3)/2 : p \text{ odd prime}\}B={(p−3)/2:p odd prime} and A=B+BA = B + BA=B+B. We show σ(A)≥1/20\sigma(A) \ge 1/20σ(A)≥1/20, then conclude with Mann's theorem. Write L=log⁡yL = \log yL=logy for the scale and C=2∏p>2(1−(p−1)−2)≤1.3217C = 2\prod_{p>2}(1 - (p-1)^{-2}) \le 1.3217C=2∏p>2​(1−(p−1)−2)≤1.3217 for the twin-prime constant.

  1. Chebyshev's constant a≈0.9212a \approx 0.9212a≈0.9212. For x≥30x \ge 30x≥30, ψ(x)≥ax−5log⁡x+5\psi(x) \ge ax - 5\log x + 5ψ(x)≥ax−5logx+5 (as in the 858585 entry). Through B⊆AB \subseteq AB⊆A this covers L<30L < 30L<30.
  2. Small-shift range (Riesel–Vaughan 1983, Lemma 8), 30≤L≤200030 \le L \le 200030≤L≤2000. Fix the first 150150150 odd primes p1≤877p_1 \le 877p1​≤877 and let R(s)R(s)R(s) count s=p1+qs = p_1 + qs=p1​+q with qqq prime. The second moment ∑R(s)2\sum R(s)^2∑R(s)2 needs the number of prime pairs (q,q+d)(q, q+d)(q,q+d), which Siebert's bound gives as at most 8C K(d) x/log⁡2x8C\,K(d)\,x/\log^2 x8CK(d)x/log2x with no error term. The kernel sum ∑p2<p1K(p1−p2)≤19496\sum_{p_2 < p_1} K(p_1 - p_2) \le 19496∑p2​<p1​​K(p1​−p2​)≤19496 is a finite kernel computation. Cauchy–Schwarz gives #{s≤y:R(s)>0}≥y/39\#\{s \le y : R(s) > 0\} \ge y/39#{s≤y:R(s)>0}≥y/39 on this range.
  3. Large range L≥2000L \ge 2000L≥2000. A Goldbach analogue of Siebert's bound, r(s)≤8C K(s) (s+1)/log⁡2(s+1)+s+1/2+2r(s) \le 8C\,K(s)\,(s+1)/\log^2(s+1) + \sqrt{s+1}/2 + 2r(s)≤8CK(s)(s+1)/log2(s+1)+s+1​/2+2 for even sss, comes from the platform's weighted large-sieve bound for sifted sets applied to {p:s−p prime}\{p : s - p \text{ prime}\}{p:s−p prime} with the shift d=2sP−sd = 2sP - sd=2sP−s (PPP the primorial of the sieve level, so p∣d  ⟺  p∣sp \mid d \iff p \mid sp∣d⟺p∣s for sieving primes), the divisor-kernel comparison and the base-denominator threshold. Combined with the weighted first moment ∑r(s)log⁡2s/s≥0.8477 n\sum r(s)\log^2 s/s \ge 0.8477\,n∑r(s)log2s/s≥0.8477n, the twelfth moment ∑s≤x evenK(s)12≤19500 x\sum_{s \le x \text{ even}} K(s)^{12} \le 19500\,x∑s≤x even​K(s)12≤19500x and Hölder, this gives #{s≤n:r(s)>0}≥n/39\#\{s \le n : r(s) > 0\} \ge n/39#{s≤n:r(s)>0}≥n/39.
  4. Mann's theorem turns 20 σ(A)≥120\,\sigma(A) \ge 120σ(A)≥1 into 20A=Z≥020A = \mathbb{Z}_{\ge 0}20A=Z≥0​, so every odd n≥123n \ge 123n≥123 is a sum of 404040 odd primes plus one 333; odd 83≤n<12383 \le n < 12383≤n<123 use twos and threes to make exactly 414141, and smaller nnn use one 333 and twos: K=2⋅20+1=41K = 2 \cdot 20 + 1 = 41K=2⋅20+1=41.

Significance

The argument stays elementary: no prime number theorem and no zeros of ζ\zetaζ or LLL-functions. New reusable components:

  1. A Goldbach analogue of Siebert's prime-pair bound with the sharp singular-series weight K(s)K(s)K(s), built from the platform's PrimePairSieve nodes.
  2. The Riesel–Vaughan small-shift argument driven by Siebert's bound.
  3. An explicit twelfth-moment bound for K(s)K(s)K(s).

Formalization scope

The Lean statement is the campaign template verbatim with 414141 in place of the value. Already proved on the platform and imported: TaoFivePrimes.siebert_prime_pair_bound, PrimePairSieve_reciprocal_weighted_sifted_bound, PrimePairSieve.divisor_kernel_comparison, PrimePairSieve.reciprocal_base_denominator_dominates_threshold, PrimePairSieve.sieve_constants_certificate, Schnir.basis_of_density.

Selected references

  • H. Riesel, R. C. Vaughan, On sums of primes, Ark. Mat. 21 (1983), 45–74.
  • P. Pollack, Not Always Buried Deep, AMS, 2009, Chapter 6, §6. https://www.pollack-math.net/NABDofficial.pdf
  • K. S. Kedlaya, Notes on Analytic Number Theory, Chapter 13, "The Selberg sieve". https://kskedlaya.org/ant/chap-selberg.html
  • O. Ramaré, On Šnirel'man's constant, Ann. Sc. Norm. Super. Pisa (4) 22 (1995), 645–706.
  • T. Tao, Every odd number greater than 1 is the sum of at most five primes, Math. Comp. 83 (2014). https://arxiv.org/abs/1201.6656
  • Chebyshev's lower bound as formalized in PrimeNumberTheoremAnd (PrimeNumberTheoremAnd/IEANTN/Chebyshev.lean).
  • H.-E. Siebert, Montgomery's weighted sieve for dimension two, Monatsh. Math. 82 (1976), 327–336.
  • Explicit improvement of the 858585 constant (unpublished AI-assisted calculation, October 2026). Source of the constant 414141; not peer reviewed.
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🏆Completed
CombinatoricsTheoretical Computer Science·Captain: wurtle

APSP in O(n^2.9983) via All-Edges Exact TriangleResearch Paper

All-pairs shortest paths (APSP) computes the shortest distance between every pair of vertices in a weighted graph.

We strengthen the previously formalized O(n2.99942)O(n^{2.99942})O(n2.99942) bound to O(n2.9983)O(n^{2.9983})O(n2.9983) for deterministic APSP on directed graphs with polynomially bounded integer weights and no negative cycles, using the same word-RAM model. It formalizes the improvement outlined by Alman and Vassilevska Williams in their conclusion.

References:

  1. Josh Alman and Virginia Vassilevska Williams, Truly Subquadratic 3SUM and Truly Subcubic APSP via Triangles in Sparse Lopsided Graphs, 2026, Theorems 17 and 19 and conclusion footnote 10.
  2. Virginia Vassilevska Williams and Ryan Williams, Finding, Minimizing, and Counting Weighted Subgraphs, 2013, Theorem 3.3 and Proposition 3.4.
  3. Virginia Vassilevska Williams and Ryan Williams, Subcubic Equivalences Between Path, Matrix, and Triangle Problems, 2018, Theorem 4.2.
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ProbabilityStochastic Systems·Captain: mikedeng1

Weak Limit Theorems for Stochastic Integrals and Stochastic Differential Equations: Under C2.2(i), (Xₙ, Yₙ) ⇒ (X, Y) in the Skorohod Topology Implies (Xₙ, Yₙ, ∫Xₙ dYₙ) ⇒ (X, Y, ∫X dY)Research Paper

Motivation

Many approximation results in probability and operations research take the form of a sequence of discrete or jump-driven systems converging to a diffusion or another limit process. When the approximating systems are written as stochastic integral equations, Xn(t)=Xn(0)+∫0tσ(Xn(s−)) dYn(s)X_n(t) = X_n(0) + \int_0^t \sigma(X_n(s-))\,dY_n(s)Xn​(t)=Xn​(0)+∫0t​σ(Xn​(s−))dYn​(s), the key step is to show that the stochastic integrals converge whenever the integrands and the integrators converge. That this is not automatic was known from the work of Wong and Zakai (1965): smooth approximations of Brownian motion produce a Stratonovich, not an Itô, limit. Kurtz and Protter (1991) give a condition on the integrators under which convergence in distribution of the pair (integrand, integrator) in the Skorohod topology implies convergence in distribution of the triple (integrand, integrator, integral). The result is essentially the theorem of Jakubowski, Mémin and Pagès (1989), with a formulation and proof that avoid the general theory of semimartingale characteristics. It underlies diffusion approximations for queueing and storage networks, approximation schemes for stochastic differential equations, and limit theorems for statistics and filters that are written as stochastic integrals.

Setting

Time is [0,∞)[0,\infty)[0,∞). A path x:[0,∞)→Ex:[0,\infty)\to Ex:[0,∞)→E in a metric space EEE is cadlag if it is right-continuous and has a left limit x(t−)x(t-)x(t−) at every t>0t>0t>0; DE[0,∞)D_E[0,\infty)DE​[0,∞) is the set of cadlag paths, and x(0−)=x(0)x(0-)=x(0)x(0−)=x(0). Let Λ\LambdaΛ be the set of continuous, strictly increasing maps of [0,∞)[0,\infty)[0,∞) onto itself. Cadlag paths xnx_nxn​ converge to xxx in the Skorohod (J1) topology if there are λn∈Λ\lambda_n\in\Lambdaλn​∈Λ with xn∘λn(t)→x(t)x_n\circ\lambda_n(t)\to x(t)xn​∘λn​(t)→x(t) and λn(t)→t\lambda_n(t)\to tλn​(t)→t uniformly on bounded intervals. For a product space E1×E2E_1\times E_2E1​×E2​ the pair (xn,yn)(x_n,y_n)(xn​,yn​) converges if one sequence λn\lambda_nλn​ serves both components; this is strictly stronger than convergence of each component.

Let Mkm\mathbb M^{km}Mkm be the real k×mk\times mk×m matrices. For a Mkm\mathbb M^{km}Mkm-valued process XXX and an Rm\mathbb R^mRm-valued process YYY, the stochastic integral (1.7) is

∫0tX(s−) dY(s)=lim⁡∑iX(ti)(Y(ti+1)−Y(ti)),\int_0^t X(s-)\,dY(s)=\lim\sum_i X(t_i)\big(Y(t_{i+1})-Y(t_i)\big),∫0t​X(s−)dY(s)=limi∑​X(ti​)(Y(ti+1​)−Y(ti​)),

the limit in probability along partitions {ti}\{t_i\}{ti​} of [0,t][0,t][0,t] whose mesh tends to zero. Throughout, ∫X dY\int X\,dY∫XdY means ∫X(s−) dY(s)\int X(s-)\,dY(s)∫X(s−)dY(s). An {Ft}\{\mathcal F_t\}{Ft​}-adapted cadlag process YYY is a semimartingale if Y=M+AY=M+AY=M+A with MMM an {Ft}\{\mathcal F_t\}{Ft​}-local martingale and AAA of finite variation on bounded intervals, with total variation Tt(A)T_t(A)Tt​(A) on [0,t][0,t][0,t]. [M][M][M] denotes the quadratic variation.

For δ∈(0,∞]\delta\in(0,\infty]δ∈(0,∞] let hδ(r)=(1−δ/r)+h_\delta(r)=(1-\delta/r)^+hδ​(r)=(1−δ/r)+ and

Jδ(x)(t)=∑s≤thδ(∣x(s)−x(s−)∣)(x(s)−x(s−)),J_\delta(x)(t)=\sum_{s\le t}h_\delta\big(|x(s)-x(s-)|\big)\big(x(s)-x(s-)\big),Jδ​(x)(t)=s≤t∑​hδ​(∣x(s)−x(s−)∣)(x(s)−x(s−)),

which collects the part of the jumps larger than δ\deltaδ; Yδ=Y−Jδ(Y)Y^\delta=Y-J_\delta(Y)Yδ=Y−Jδ​(Y) then has jumps of size at most δ\deltaδ. Condition C2.2(i) on a sequence YnY_nYn​ asks for decompositions Ynδ=Mnδ+AnδY_n^\delta=M_n^\delta+A_n^\deltaYnδ​=Mnδ​+Anδ​ such that for each α>0\alpha>0α>0 there are stopping times τnα\tau_n^\alphaτnα​ with P{τnα≤α}≤1/αP\{\tau_n^\alpha\le\alpha\}\le1/\alphaP{τnα​≤α}≤1/α and sup⁡nE[[Mnδ]t∧τnα+Tt∧τnα(Anδ)]<∞\sup_nE\big[[M_n^\delta]_{t\wedge\tau_n^\alpha}+T_{t\wedge\tau_n^\alpha}(A_n^\delta)\big]<\inftysupn​E[[Mnδ​]t∧τnα​​+Tt∧τnα​​(Anδ​)]<∞. ⇒\Rightarrow⇒ denotes convergence in distribution.

Formalization targets

Goal: Theorem 2.2 (distributional part)

For each nnn, let (Xn,Yn)(X_n,Y_n)(Xn​,Yn​) be {Ftn}\{\mathcal F^n_t\}{Ftn​}-adapted with paths in DMkm×Rm[0,∞)D_{\mathbb M^{km}\times\mathbb R^m}[0,\infty)DMkm×Rm​[0,∞), YnY_nYn​ an {Ftn}\{\mathcal F^n_t\}{Ftn​}-semimartingale satisfying C2.2(i) for some δ∈(0,∞]\delta\in(0,\infty]δ∈(0,∞]. If (Xn,Yn)⇒(X,Y)(X_n,Y_n)\Rightarrow(X,Y)(Xn​,Yn​)⇒(X,Y) in the Skorohod topology on DMkm×Rm[0,∞)D_{\mathbb M^{km}\times\mathbb R^m}[0,\infty)DMkm×Rm​[0,∞), then YYY is a semimartingale with respect to a filtration to which XXX and YYY are adapted, and

(Xn, Yn, ∫Xn dYn)⇒(X, Y, ∫X dY)in DMkm×Rm×Rk[0,∞).\Big(X_n,\,Y_n,\,\int X_n\,dY_n\Big)\Rightarrow\Big(X,\,Y,\,\int X\,dY\Big)\quad\text{in }D_{\mathbb M^{km}\times\mathbb R^m\times\mathbb R^k}[0,\infty).(Xn​,Yn​,∫Xn​dYn​)⇒(X,Y,∫XdY)in DMkm×Rm×Rk​[0,∞).

Milestones, in the order the proof uses them

  • Lemma 2.1: time-change-equivariant maps that are continuous for local uniform convergence are Skorohod-continuous, jointly with their argument.
  • Continuity of JδJ_\deltaJδ​ (after (2.1)): (xn,Jδ(xn))→(x,Jδ(x))(x_n,J_\delta(x_n))\to(x,J_\delta(x))(xn​,Jδ​(xn​))→(x,Jδ​(x)) and (xn,xn−Jδ(xn))→(x,x−Jδ(x))(x_n,x_n-J_\delta(x_n))\to(x,x-J_\delta(x))(xn​,xn​−Jδ​(xn​))→(x,x−Jδ​(x)).
  • Lemma 6.2: a sequential characterization of Skorohod convergence.
  • The step approximation IεI_\varepsilonIε​ of §6, with r(z(t),Iε(z)(t))≤εr(z(t),I_\varepsilon(z)(t))\le\varepsilonr(z(t),Iε​(z)(t))≤ε.
  • Lemma 6.1: zn→zz_n\to zzn​→z implies (zn,Iε(zn))→(z,Iε(z))(z_n,I_\varepsilon(z_n))\to(z,I_\varepsilon(z))(zn​,Iε​(zn​))→(z,Iε​(z)) almost surely in the random thresholds.
  • (1.12)–(1.13): integrals against step functions with uniformly bounded jump counts converge, jointly with integrand and integrator.
  • (2.2): ∫xn(s−) dJδ(yn)(s)→∫x(s−) dJδ(y)(s)\int x_n(s-)\,dJ_\delta(y_n)(s)\to\int x(s-)\,dJ_\delta(y)(s)∫xn​(s−)dJδ​(yn​)(s)→∫x(s−)dJδ​(y)(s).
  • (2.7): E[sup⁡s≤t∧τ∣R(s)∣]≤ε(2E[[M]t∧τ]1/2+E[Tt∧τ(A)])E\big[\sup_{s\le t\wedge\tau}|R(s)|\big]\le\varepsilon\big(2E[[M]_{t\wedge\tau}]^{1/2}+E[T_{t\wedge\tau}(A)]\big)E[sups≤t∧τ​∣R(s)∣]≤ε(2E[[M]t∧τ​]1/2+E[Tt∧τ​(A)]) for R=∫H d(M+A)R=\int H\,d(M+A)R=∫Hd(M+A) with ∣H∣≤ε|H|\le\varepsilon∣H∣≤ε.
  • Remark 2.4: the limit YYY is a semimartingale.

Significance

The result. Theorem 2.2 reduces convergence of stochastic integrals to two checks: joint convergence of integrand and integrator, and the uniform control C2.2(i) on the integrators. Remarks 2.3 and 2.5 give simple sufficient conditions (stochastic boundedness of Tt(Anδ)T_t(A_n^\delta)Tt​(Anδ​) plus a second-moment bound; relative compactness for a fixed integrator), and Section 5 of the paper derives from it weak limit theorems for stochastic differential equations driven by semimartingales, including Wong–Zakai-type corrections. Without the theorem, each diffusion approximation that passes through an integral equation needs its own ad hoc argument.

Formalizing it. The theorem is proved and classical; nothing here is open. Lean's Mathlib has no Skorohod space, no stochastic integral against a semimartingale and no semimartingale, so the mission produces the first machine-checked definitions of J1 convergence on DE[0,∞)D_E[0,\infty)DE​[0,∞), of the left-point stochastic integral (1.7), and of convergence in distribution of cadlag processes, together with the deterministic facts about them that a proof of Theorem 2.2 needs. The definitions are meant to be reused by later missions on weak convergence of processes and on stochastic differential equations (the paper's Theorem 5.4 is planned as a follow-up that references them).

Difficulty

The obvious argument — the integral is a continuous function of the pair (integrand, integrator), so the continuous mapping theorem applies — fails in two ways. First, the map (x,y)↦∫x(s−) dy(s)(x,y)\mapsto\int x(s-)\,dy(s)(x,y)↦∫x(s−)dy(s) is not continuous in the Skorohod topology, and for a general semimartingale integrator it is not even defined path by path. Example 1.1 makes the failure concrete: with X=Y=Xn=χ[1,∞)X=Y=X_n=\chi_{[1,\infty)}X=Y=Xn​=χ[1,∞)​ and Yn=χ[1+1/n,∞)Y_n=\chi_{[1+1/n,\infty)}Yn​=χ[1+1/n,∞)​, each component converges, yet ∫0tXn dYn=1\int_0^tX_n\,dY_n=1∫0t​Xn​dYn​=1 for t>1+1/nt>1+1/nt>1+1/n while ∫0tX dY=0\int_0^tX\,dY=0∫0t​XdY=0, because the jumps of integrand and integrator coalesce in the wrong order; joint convergence of the pair excludes this. Second, Example 1.2 shows that joint convergence is still not enough: integrators whose variation grows without bound (piecewise linear interpolations of Brownian motion) produce an extra drift 12t\tfrac12t21​t in the limit. C2.2(i) is the condition that excludes this, and the identification of the limit integral also requires knowing that the limit YYY is a semimartingale, which is not given.

Formalization scope

Time is ℝ≥0; a process is a map ℝ≥0 → Ω → E. Rm\mathbb R^mRm is Fin m → ℝ and Mkm\mathbb M^{km}Mkm is Fin k → Fin m → ℝ, with the sup metric; products carry the max metric (J1 convergence does not depend on the product metric). The conventions the formal statements commit to:

  • "xn→xx_n\to xxn​→x in the Skorohod topology" is the sequential definition of pp. 1037–1038 with one time change sequence; "uniformly for ttt in bounded intervals" is uniformly on [0,T][0,T][0,T] for every TTT. For a pair or a triple the time change is shared by all components.
  • "⇒\Rightarrow⇒" is convergence in distribution in coupling form: a probability space carrying copies of the processes and of the limit, with almost sure Skorohod convergence. Laws are taken on the product σ-algebra of path space; for the finite-dimensional state spaces here this is equivalent to weak convergence of the laws on DE[0,∞)D_E[0,\infty)DE​[0,∞).
  • The coupling relation is defined for Polish state spaces with their Borel σ-algebras. Every state space in the probabilistic milestones is a finite-dimensional real product and satisfies this requirement.
  • ∫X dY\int X\,dY∫XdY is the in-probability limit of left-point Riemann sums (1.7) over all partition sequences with mesh tending to zero, with cadlag paths. The prelimit integrals are given processes with this property; the limit integral is produced in the conclusion.
  • The semimartingale conclusion of Theorem 2.2 is stated for a copy of (X,Y)(X,Y)(X,Y) on a space that may carry extra randomness, with a filtration making both adapted.
  • In C2.2(i) the free ttt is universally quantified ("for every t≥0t\ge0t≥0") and the stopping times are chosen before ttt; expectations of nonnegative quantities are taken in [0,∞][0,\infty][0,∞]; t∧τ=tt\wedge\tau=tt∧τ=t when τ=∞\tau=\inftyτ=∞.
  • [M]=∑j[Mj][M]=\sum_j[M_j][M]=∑j​[Mj​] with [M](0)=0[M](0)=0[M](0)=0; since C2.2(i) asks for some decomposition, this agrees with Protter's convention [M](0)=M(0)2[M](0)=M(0)^2[M](0)=M(0)2.
  • In (2.1), ∣x∣=∑i∣xi∣|x|=\sum_i|x_i|∣x∣=∑i​∣xi​∣ (the paper's convention for vectors, p. 1049); in (2.7), Euclidean norms for RRR and T(A)T(A)T(A) and the Frobenius norm for the integrand.
  • "a.s." in Lemma 6.1 refers to the law of the thresholds θk\theta_kθk​, i.i.d. uniform on [12,1][\frac12,1][21​,1], and the null set may depend on the convergent sequence.
  • δ\deltaδ ranges over (0,∞](0,\infty](0,∞], with J∞=0J_\infty=0J∞​=0.

The theorem has trivializing formalizations, all excluded here: componentwise convergence of (Xn,Yn)(X_n,Y_n)(Xn​,Yn​) in place of joint convergence; an integral not pinned to (1.7) (any process would do); and assuming the limit integral, or the semimartingale property of YYY, as a hypothesis.

Local martingales and cross variations reuse the published Ethier–Kurtz definitions EthierKurtz_IsSourceLocalMartingale and EthierKurtz_HasCrossVariation. A complete development needs the Skorohod space and its tightness theory, the stochastic integral against semimartingales (existence and the Burkholder–Davis–Gundy/Doob estimates), and the quasimartingale criterion of Meyer and Zheng. Contributions to any of these layers are welcome; the deterministic milestones (Lemma 2.1, Lemma 6.2, the continuity of JδJ_\deltaJδ​, (1.12)–(1.13), Lemma 6.1) are independent of the probabilistic ones and reusable for any work on the J1 topology.

Selected references

  • T. G. Kurtz and P. Protter, Weak limit theorems for stochastic integrals and stochastic differential equations, Ann. Probab. 19 (1991), 1035–1070. https://doi.org/10.1214/aop/1176990334
  • A. Jakubowski, J. Mémin and G. Pagès, Convergence en loi des suites d'intégrales stochastiques sur l'espace D¹ de Skorokhod, Probab. Theory Related Fields 81 (1989), 111–137. https://doi.org/10.1007/BF00343739
  • S. N. Ethier and T. G. Kurtz, Markov Processes: Characterization and Convergence, Wiley, 1986. https://doi.org/10.1002/9780470316658
  • P. Protter, Stochastic Integration and Differential Equations, Springer, 1990. https://doi.org/10.1007/978-3-662-02619-9
  • E. Wong and M. Zakai, On the convergence of ordinary integrals to stochastic integrals, Ann. Math. Statist. 36 (1965), 1560–1564. https://doi.org/10.1214/aoms/1177699916
  • P. A. Meyer and W. A. Zheng, Tightness criteria for laws of semimartingales, Ann. Inst. H. Poincaré Probab. Statist. 20 (1984), 353–372. http://www.numdam.org/item/AIHPB_1984__20_4_353_0/
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Control TheoryConvex OptimizationProbability·Captain: mikedeng1

Convex Duality in Constrained Portfolio Optimization I: Financibility, Minimality, Dual Optimality and Parsimony of an Auxiliary Market Are Equivalent and Yield the Optimal Constrained PolicyResearch Paper

Motivation

An investor in a continuous-time market chooses, at every instant, how to split wealth between a bond and ddd stocks and how fast to consume, so as to maximize expected utility of consumption and terminal wealth. Without constraints on the portfolio, this problem was solved by the martingale method: Pliska (1986), Karatzas, Lehoczky and Shreve (1987) and Cox and Huang (1989) showed that in a complete market the optimal terminal wealth and consumption are explicit functions of a single state-price density, and the portfolio that finances them comes from the martingale representation theorem.

Real investors face constraints: no short selling, no borrowing, a cap on the fraction of wealth in a sector, an incomplete market in which some stocks cannot be traded at all. Each makes the market effectively incomplete, and the single state-price density no longer exists. Karatzas, Lehoczky, Shreve and Xu (1991) treated incompleteness, Xu (1990, thesis) short-selling prohibition, and He and Pearson (1991) short-sale constraints in a general setting. Cvitanić and Karatzas (1992) unified these cases: the portfolio must take values in an arbitrary nonempty closed convex set K⊂RdK\subset\mathbb R^dK⊂Rd, and the problem is embedded in a family of auxiliary unconstrained markets indexed by a dual process ν\nuν. This mission formalizes the paper's central characterization, Theorem 10.1, and the results its proof rests on.

Setting

A standard Brownian motion WWW in Rd\mathbb R^dRd lives on a complete probability space with its augmented filtration {Ft}\{\mathcal F_t\}{Ft​}, on a finite horizon [0,T][0,T][0,T]. The market M\mathcal MM has progressively measurable interest rate rrr, appreciation rates bbb and volatility matrix σ\sigmaσ, with r≥−ηr\ge-\etar≥−η, ξ∗σσ∗ξ≥ε∥ξ∥2\xi^*\sigma\sigma^*\xi\ge\varepsilon\|\xi\|^2ξ∗σσ∗ξ≥ε∥ξ∥2, E∫0Tr dt<∞E\int_0^Tr\,dt<\inftyE∫0T​rdt<∞, and a relative risk θ=σ−1(b−r1)\theta=\sigma^{-1}(b-r\mathbf 1)θ=σ−1(b−r1) with E∫0T∥θ∥2dt<∞E\int_0^T\|\theta\|^2dt<\inftyE∫0T​∥θ∥2dt<∞. The state-price density is H0=γ0Z0H_0=\gamma_0Z_0H0​=γ0​Z0​, with γ0(t)=e−∫0tr\gamma_0(t)=e^{-\int_0^tr}γ0​(t)=e−∫0t​r and Z0(t)=exp⁡(−∫0tθ∗dW−12∫0t∥θ∥2)Z_0(t)=\exp(-\int_0^t\theta^*dW-\frac12\int_0^t\|\theta\|^2)Z0​(t)=exp(−∫0t​θ∗dW−21​∫0t​∥θ∥2).

A portfolio π\piπ gives the proportions of wealth in the stocks, a consumption rate is c≥0c\ge0c≥0, and the wealth solves

dX=(rX−c) dt+Xπ∗σ (dW+θ dt),X(0)=x>0.dX=(rX-c)\,dt+X\pi^*\sigma\,(dW+\theta\,dt),\qquad X(0)=x>0.dX=(rX−c)dt+Xπ∗σ(dW+θdt),X(0)=x>0.

The pair is admissible, (π,c)∈A0(x)(\pi,c)\in\mathcal A_0(x)(π,c)∈A0​(x), if X≥0X\ge0X≥0. With utility functions U1(t,⋅)U_1(t,\cdot)U1​(t,⋅), U2U_2U2​ (strictly increasing, strictly concave, C1C^1C1, U′(0+)=∞U'(0+)=\inftyU′(0+)=∞, U′(∞)=0U'(\infty)=0U′(∞)=0), inverse marginals I1,I2I_1,I_2I1​,I2​ and conjugates U~1,U~2\tilde U_1,\tilde U_2U~1​,U~2​, the investor maximizes

J(x;π,c)=E∫0TU1(t,c(t)) dt+EU2(X(T))J(x;\pi,c)=E\int_0^TU_1(t,c(t))\,dt+EU_2(X(T))J(x;π,c)=E∫0T​U1​(t,c(t))dt+EU2​(X(T))

over A′(x)\mathcal A'(x)A′(x), the admissible pairs with integrable utility losses and π∈K\pi\in Kπ∈K almost everywhere. The value is V(x)V(x)V(x).

The support function δ(ν)=sup⁡π∈K(−π∗ν)∈R∪{+∞}\delta(\nu)=\sup_{\pi\in K}(-\pi^*\nu)\in\mathbb R\cup\{+\infty\}δ(ν)=supπ∈K​(−π∗ν)∈R∪{+∞} drives the duality. For ν\nuν in the class D\mathcal DD of square-integrable processes with E∫0Tδ(ν) dt<∞E\int_0^T\delta(\nu)\,dt<\inftyE∫0T​δ(ν)dt<∞, the auxiliary market Mν\mathcal M_\nuMν​ has interest rate r+δ(ν)r+\delta(\nu)r+δ(ν) and appreciation rates b+ν+δ(ν)1b+\nu+\delta(\nu)\mathbf 1b+ν+δ(ν)1, state-price density HνH_\nuHν​ and unconstrained value Vν(x)V_\nu(x)Vν​(x). For λ\lambdaλ in the subclass D′\mathcal D'D′ (where Xλ(y)=E[∫0THλI1(t,yHλ) dt+Hλ(T)I2(yHλ(T))]\mathcal X_\lambda(y)=E[\int_0^TH_\lambda I_1(t,yH_\lambda)\,dt+H_\lambda(T)I_2(yH_\lambda(T))]Xλ​(y)=E[∫0T​Hλ​I1​(t,yHλ​)dt+Hλ​(T)I2​(yHλ​(T))] is finite for all y>0y>0y>0), let y=Yλ(x)y=\mathcal Y_\lambda(x)y=Yλ​(x) solve Xλ(y)=x\mathcal X_\lambda(y)=xXλ​(y)=x. The Mλ\mathcal M_\lambdaMλ​-optimal consumption, terminal wealth and wealth are cλ=I1(t,yHλ)c_\lambda=I_1(t,yH_\lambda)cλ​=I1​(t,yHλ​), ξλ=I2(yHλ(T))\xi_\lambda=I_2(yH_\lambda(T))ξλ​=I2​(yHλ​(T)) and XλX_\lambdaXλ​.

Formalization targets

Goal: Theorem 10.1

Five conditions are considered for a capital x>0x>0x>0: (A) optimality of a pair (π^,c^)∈A′(x)(\hat\pi,\hat c)\in\mathcal A'(x)(π^,c^)∈A′(x), together with E[∫0Tc^U1′(t,c^) dt+X^(T)U2′(X^(T))]<∞E[\int_0^T\hat cU_1'(t,\hat c)\,dt+\hat X(T)U_2'(\hat X(T))]<\inftyE[∫0T​c^U1′​(t,c^)dt+X^(T)U2′​(X^(T))]<∞; and, for λ∈D′\lambda\in\mathcal D'λ∈D′, (B) financibility: some π^λ∈K\hat\pi_\lambda\in Kπ^λ​∈K with δ(λ)+π^λ∗λ=0\delta(\lambda)+\hat\pi_\lambda^*\lambda=0δ(λ)+π^λ∗​λ=0 finances (cλ,ξλ)(c_\lambda,\xi_\lambda)(cλ​,ξλ​) in M\mathcal MM; (C) minimality: Vλ(x)≤Vν(x)V_\lambda(x)\le V_\nu(x)Vλ​(x)≤Vν​(x) for all ν∈D\nu\in\mathcal Dν∈D, with Vλ(x)V_\lambda(x)Vλ​(x) attained by (cλ,ξλ)(c_\lambda,\xi_\lambda)(cλ​,ξλ​); (D) dual optimality: λ\lambdaλ minimizes ν↦E[∫0TU~1(t,yHν) dt+U~2(yHν(T))]\nu\mapsto E[\int_0^T\tilde U_1(t,yH_\nu)\,dt+\tilde U_2(yH_\nu(T))]ν↦E[∫0T​U~1​(t,yHν​)dt+U~2​(yHν​(T))] over D\mathcal DD; (E) parsimony: E[∫0THνcλ dt+Hν(T)ξλ]≤xE[\int_0^TH_\nu c_\lambda\,dt+H_\nu(T)\xi_\lambda]\le xE[∫0T​Hν​cλ​dt+Hν​(T)ξλ​]≤x for all ν∈D\nu\in\mathcal Dν∈D. The theorem asserts

(B)  ⟺  (C)  ⟺  (D)  ⟺  (E)  ⟹  (A) for (π^λ,cλ),(\mathrm B)\iff(\mathrm C)\iff(\mathrm D)\iff(\mathrm E)\implies(\mathrm A)\text{ for }(\hat\pi_\lambda,c_\lambda),(B)⟺(C)⟺(D)⟺(E)⟹(A) for (π^λ​,cλ​),

and, under the conditions (5.8) (c↦cU′(c)c\mapsto cU'(c)c↦cU′(c) nondecreasing), (8.25) (a uniform growth bound αU′(x)≥U′(γx)\alpha U'(x)\ge U'(\gamma x)αU′(x)≥U′(γx)) and (12.2) (finiteness of the dual functional for some ν\nuν), that (A) implies (B)–(E) for some λ∈D′\lambda\in\mathcal D'λ∈D′ with π^λ=π^\hat\pi_\lambda=\hat\piπ^λ​=π^.

Milestones

In proof order: the conjugate inequalities (5.5)–(5.6); the budget constraint (3.6); the unconstrained solution (Lemma 7.2, Proposition 7.3, Theorem 7.4); the embedding (8.14), V(x)≤Vν(x)V(x)\le V_\nu(x)V(x)≤Vν​(x); Proposition 8.3, (B) ⇒\Rightarrow⇒ optimality; the constrained budget constraint (9.4) and the hedging Theorem 9.1, (E) ⇒\Rightarrow⇒ (B); and Appendix A's Lemma A.1, Lemma A.2 and Proposition A.4, the steps of (A) ⇒\Rightarrow⇒ (B).

Significance

Theorem 10.1 turns a constrained stochastic control problem into a family of unconstrained ones plus a minimization over the dual process λ\lambdaλ. Condition (D) is a convex minimization over ν\nuν that does not involve portfolios. It leads to the dual problem of Section 12, whose solvability gives existence of optimal constrained policies (Theorem 13.1, the companion mission). Section 9's hedging theorem is the superreplication principle under convex constraints, the basis of later work on constrained hedging and pricing. With logarithmic utility the theorem gives explicit optimal policies, and for deterministic coefficients the dual problem reduces to a deterministic one.

These results are proved in the paper, which is the standard reference for the convex-duality approach. To our knowledge they have no machine-checked proof. The mission's statements also produce a reusable Lean model of a continuous-time Itô market with stochastic coefficients, admissible portfolios, consumption, utility functions and their conjugates.

Difficulty

The obvious argument, Lagrange duality for max⁡J\max JmaxJ subject to π∈K\pi\in Kπ∈K, fails at the first step: the constraint is on the control process, not on terminal wealth, so there is no static budget constraint to dualize. The paper's dual variable is a process, and for each candidate it changes both the interest rate and the drift. The direction (B) ⇒\Rightarrow⇒ (A) is relatively direct. The direction (E) ⇒\Rightarrow⇒ (B) is a hedging theorem under convex constraints (Theorem 9.1), where financing a claim requires the portfolio to land in KKK and to satisfy the complementary-slackness identity δ(λ)+π∗λ=0\delta(\lambda)+\pi^*\lambda=0δ(λ)+π∗λ=0, which no unconstrained construction delivers. The converse (A) ⇒\Rightarrow⇒ (B) must produce the dual process λ\lambdaλ from an optimal pair that is only assumed to exist, and the paper needs the extra growth conditions (5.8), (8.25), (12.2) for it. In Lean, stochastic integrals for integrands that are square integrable only almost surely, the martingale representation theorem for the Brownian filtration, and the product rule for Itô processes are not available in Mathlib.

Formalization scope

Processes are functions R≥0×Ω→E\mathbb R_{\ge0}\times\Omega\to ER≥0​×Ω→E constrained on [0,T][0,T][0,T]; vectors are EuclideanSpace ℝ (Fin d), matrices Matrix (Fin d) (Fin d) ℝ. The Brownian motion is the published EthierKurtz.IsStandardBrownian. The stochastic integral is a binder I, constrained only by the standing hypothesis that it is an Itô integral for every locally square-integrable integrand. This almost-sure variant of EthierKurtz.HasBrownianItoIntegral uses the published dyadic step helpers itoStepValue and itoStepSum. The hypothesis is satisfiable, by the classical construction.

The following readings are explicit in the Lean.

  • Triples. Classes are sets of triples (π,c,X)(\pi,c,X)(π,c,X) with XXX a wealth process: an adapted, a.s. continuous solution of the integral form of (3.1) or (8.10) whose integrals exist.
  • Extended reals. Utility expectations are extended reals, computed as positive minus negative parts. A utility at 000 is U(0+)U(0+)U(0+). Suprema are taken in the extended reals.
  • The support function. δ\deltaδ takes values in the extended reals. In drifts and discounts it enters as a real number, which is finite almost everywhere for ν∈D\nu\in\mathcal Dν∈D. The page's "E∫δ(ν)≤∞E\int\delta(\nu)\le\inftyE∫δ(ν)≤∞" in (8.1) is read as "<∞<\infty<∞".
  • Inverse marginals and conjugates. I(y)=inf⁡{x>0:U′(x)≤y}I(y)=\inf\{x>0: U'(x)\le y\}I(y)=inf{x>0:U′(x)≤y} and U~(y)=sup⁡x>0(U(x)−xy)\tilde U(y)=\sup_{x>0}(U(x)-xy)U~(y)=supx>0​(U(x)−xy).
  • The inverse Yλ\mathcal Y_\lambdaYλ​. Yλ(x)\mathcal Y_\lambda(x)Yλ​(x) and Y0(x)\mathcal Y_0(x)Y0​(x) are represented by a number y>0y>0y>0 with X(y)=x\mathcal X(y)=xX(y)=x.
  • The wealth XλX_\lambdaXλ​. It is a conditional expectation for each ttt. "X=XλX=X_\lambdaX=Xλ​" means X(t)=Xλ(t)X(t)=X_\lambda(t)X(t)=Xλ​(t) a.s. for every t≤Tt\le Tt≤T.
  • Almost everywhere. "ℓ⊗P\ell\otimes Pℓ⊗P-a.e." is almost everywhere for the product of Lebesgue measure on [0,T][0,T][0,T] and PPP. "a.s." is almost everywhere for PPP.
  • Theorem 9.1. Its conclusion "(π,c)∈A′(x)(\pi,c)\in\mathcal A'(x)(π,c)∈A′(x)" is formalized as A0(x)\mathcal A_0(x)A0​(x) plus π∈K\pi\in Kπ∈K a.e., since the theorem involves no utility.
  • (4.4). By Remark 4.2 it is not used in Theorem 10.1. It is kept, because the paper assumes it throughout.

A formalization in which the stochastic integral is an unconstrained function, a wealth process need not solve its equation, or δ\deltaδ is real-valued (so that sup⁡\supsup over an unbounded set returns 000) would make the statements vacuous or false; each is ruled out above. The proof will need almost-surely-square-integrable Itô integrals, Itô's product rule, nonnegative local martingales as supermartingales, and martingale representation in the Brownian filtration. All of these are reusable well beyond this mission, and contributions of any of them are welcome.

Selected references

  • J. Cvitanić and I. Karatzas, Convex duality in constrained portfolio optimization, Ann. Appl. Probab. 2(4) (1992) 767–818. https://doi.org/10.1214/aoap/1177005576
  • I. Karatzas, J. P. Lehoczky and S. E. Shreve, Optimal portfolio and consumption decisions for a "small investor" on a finite horizon, SIAM J. Control Optim. 25 (1987) 1557–1586. https://doi.org/10.1137/0325086
  • J. C. Cox and C. F. Huang, Optimal consumption and portfolio policies when asset prices follow a diffusion process, J. Econom. Theory 49 (1989) 33–83. https://doi.org/10.1016/0022-0531(89)90067-7
  • S. R. Pliska, A stochastic calculus model of continuous trading: optimal portfolios, Math. Oper. Res. 11 (1986) 371–382. https://doi.org/10.1287/moor.11.2.371
  • I. Karatzas, J. P. Lehoczky, S. E. Shreve and G. L. Xu, Martingale and duality methods for utility maximization in an incomplete market, SIAM J. Control Optim. 29 (1991) 702–730. https://doi.org/10.1137/0329039
  • H. He and N. D. Pearson, Consumption and portfolio policies with incomplete markets and short-sale constraints: the infinite-dimensional case, J. Econom. Theory 54 (1991) 259–304. https://doi.org/10.1016/0022-0531(91)90123-L
  • I. Karatzas and S. E. Shreve, Brownian Motion and Stochastic Calculus, Springer, 1988. https://doi.org/10.1007/978-1-4684-0302-2
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Numerical AnalysisOptimization·Captain: mikedeng1

Truncated-Newton Algorithms for Large-Scale Unconstrained Optimization 1: Truncated-Newton CG Iterates Have ‖g(x_k)‖ → 0 and Converge to Any Limit Point with Positive Definite HessianResearch Paper

Motivation

Large scale unconstrained optimization often makes an exact Newton step expensive. At each iterate, Newton's method asks for a solution of a linear system involving the Hessian, and the cost of solving that system can dominate the cost of evaluating the objective. Dembo and Steihaug's 1983 truncated Newton method uses conjugate gradients to stop the linear solve early, either when the residual is small enough or when the current direction has insufficient positive curvature. The resulting direction is paired with a line search. The question for this mission is whether those early exits still give a globally reliable optimization method under the paper's assumptions. The answer, in Theorem 2.1, is that every resulting run has gradient norm tending to zero, and a positive definite Hessian at one limit point makes the whole sequence converge to that point.

Setting

The objective is a twice continuously differentiable function f:Rn→Rf:\mathbb R^n\to\mathbb Rf:Rn→R. Write g(x)=∇f(x)g(x)=\nabla f(x)g(x)=∇f(x) for its gradient and H(x)=Dg(x)H(x)=Dg(x)H(x)=Dg(x) for its Hessian. For every initial point x0x_0x0​, the paper assumes that the sublevel set L(x0)={x:f(x)≤f(x0)}L(x_0)=\{x:f(x)\le f(x_0)\}L(x0​)={x:f(x)≤f(x0​)} is bounded. The formalization uses the Euclidean norm and its inner product, so the operator norm of HHH is also Euclidean.

At a major iterate xkx_kxk​, the minor conjugate-gradient iteration starts at p0=0p_0=0p0​=0 with residual and direction r0=d0=−g(xk)r_0=d_0=-g(x_k)r0​=d0​=−g(xk​). It maintains a scalar δi\delta_iδi​, initialized to ∥r0∥2\|r_0\|^2∥r0​∥2, alongside the usual conjugate-gradient state. Before taking its next conjugate-gradient step, it checks whether ⟨di,H(xk)di⟩≤εδi\langle d_i,H(x_k)d_i\rangle\le\varepsilon\delta_i⟨di​,H(xk​)di​⟩≤εδi​. If so, it returns d0=−g(xk)d_0=-g(x_k)d0​=−g(xk​) when i=0i=0i=0 and the current approximation pip_ipi​ otherwise. If this first test fails, it takes a conjugate-gradient step and checks whether ∥ri+1∥≤ηk∥g(xk)∥\|r_{i+1}\|\le\eta_k\|g(x_k)\|∥ri+1​∥≤ηk​∥g(xk​)∥. If so, it returns pi+1p_{i+1}pi+1​. A TNCG direction is the direction returned by the first exit that occurs. The forcing value ηk\eta_kηk​ sets the residual tolerance.

The major iteration chooses a positive step length λk\lambda_kλk​. With pkp_kpk​ the minor iteration's output and 0<α<1/20<\alpha<1/20<α<1/2, α<β<1\alpha<\beta<1α<β<1, the line search requires both sufficient decrease and a curvature condition:

f(xk+λkpk)≤f(xk)+αλk⟨g(xk),pk⟩,⟨g(xk+λkpk),pk⟩≥β⟨g(xk),pk⟩.f(x_k+\lambda_k p_k)\le f(x_k)+\alpha\lambda_k\langle g(x_k),p_k\rangle, \qquad \langle g(x_k+\lambda_kp_k),p_k\rangle\ge\beta\langle g(x_k),p_k\rangle.f(xk​+λk​pk​)≤f(xk​)+αλk​⟨g(xk​),pk​⟩,⟨g(xk​+λk​pk​),pk​⟩≥β⟨g(xk​),pk​⟩.

The update is xk+1=xk+λkpkx_{k+1}=x_k+\lambda_kp_kxk+1​=xk​+λk​pk​. A run is a sequence satisfying this rule from its specified starting point. The paper also states an alternative function-value curvature condition; this mission defines it because the local unit-step theorem discusses both choices, although the main run uses the displayed gradient condition.

Formalization targets

Global convergence

For every starting point there is a TNCG run, and every run satisfies

∥g(xk)∥⟶0.\|g(x_k)\|\longrightarrow0.∥g(xk​)∥⟶0.

If x∗x^*x∗ is a limit point of that run and H(x∗)H(x^*)H(x∗) is positive definite, then

xk⟶x∗.x_k\longrightarrow x^*.xk​⟶x∗.

The existence clause is the formal meaning of the paper's assertion that the iterates are well defined. The six milestones follow the paper's appendix: the conjugate-gradient relations of Theorem A.1; the uniform descent and direction bounds of Lemma A.2; the line-search existence and directional-derivative limit used in the proof of Theorem A.3; Theorem A.3 itself; and eventual unit-step admissibility in Theorem A.4. The companion Theorem 2.2 addresses the eventual residual exit and unit-step behavior when a run converges to a point with positive definite Hessian. These results are all stated in the original paper.

Significance

The target shows that the computational shortcut in the inner linear solve preserves a global first-order guarantee: no TNCG run can maintain a gradient norm bounded away from zero. It also identifies when the sequence has one limit, rather than merely having stationary accumulation points. The local companion result describes the regime where the truncated method can take full steps and the residual stopping test governs the minor iteration.

The mathematical results are proved in the 1983 paper, while this mission's Lean statements are open proof targets. A complete formalization would connect the finite-dimensional conjugate-gradient recurrence, the line-search argument on bounded sublevel sets, and the convergence statement in one machine-checked development. The conjugate-gradient identities and line-search facts could be reused in other optimization algorithms; the exact first-exit model and the global conclusion are specific to this method.

Difficulty

The minor iteration is not an ordinary positive definite conjugate-gradient solve. The Hessian may be indefinite away from a solution, and the iteration must stop at insufficient curvature before using a later residual state. A convergence argument that assumes positive definiteness at every iterate would therefore miss the case the algorithm was designed to handle. The line search must work for the returned direction, including the first iteration's steepest-descent fallback. The limit-point conclusion adds a separate issue: a vanishing gradient norm alone does not force an entire sequence to converge to a chosen limit point.

Formalization scope

Lean represents Rn\mathbb R^nRn as EuclideanSpace ℝ (Fin n), uses its Euclidean norm and inner product, and defines H(x)H(x)H(x) as the derivative of the gradient. The objective is C2C^2C2 and every sublevel set is bounded, as specified at the start of the paper. The TNCG recurrence is total, but an admissible direction must come from its first actual exit, with the curvature test preceding the residual test. At i=0i=0i=0, the curvature exit returns −g-g−g, not the zero initial approximation. This prevents a false stationary run. The residual test is written as a product inequality, equivalent to the paper's quotient when the residual test is reached.

Step lengths are positive. A run is extended through stationary points by zero directions, giving an infinite sequence on which a limit can be stated. Theorem 2.1 imposes no extra restriction on the forcing sequence and no upper bound on step lengths. Theorem A.1 corrects the printed Krylov-space index from Hk−1gH^{k-1}gHk−1g to HkgH^kgHkg. Theorem A.4 adds g(x∗)=0g(x^*)=0g(x∗)=0, needed for the conclusion and true in the paper's applications. Theorem 2.2 requires nonnegative forcing values and guards its residual-exit conclusion at stationary iterates. These corrections are recorded item by item in the moderation notes. Contributions to the conjugate-gradient identities, bounded-level-set line search, and isolated-limit-point argument are all within scope.

Selected references

  • R. S. Dembo and T. Steihaug, Truncated-Newton algorithms for large-scale unconstrained optimization, Mathematical Programming 26 (1983), 190–212. DOI: 10.1007/BF02592055.
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Dynamical SystemsGeometry & TopologySymplectic Geometry·Captain: Mazecto

Hryniewicz's Criterion: Disk-like Global Sections of Dynamically Convex Reeb Flows on S³Research Paper

Motivation

A global surface of section reduces a flow on a closed 3-manifold to an area-preserving map of a surface. It is a compact embedded surface whose boundary consists of periodic orbits, whose interior is transverse to the flow, and which every other trajectory hits infinitely often in forward and backward time. Poincaré introduced the idea for the restricted three-body problem. Once a section is a disk, results on area-preserving disk maps (Brouwer, Franks) give periodic orbits and other structure for the whole flow.

For Hamiltonian flows on star-shaped energy surfaces in R4\mathbb{R}^4R4, equivalently Reeb flows on the tight 3-sphere, it is natural to ask which periodic orbits bound such a disk. Hryniewicz's criterion answers this for dynamically convex flows, with no genericity assumption. The answer is purely topological: a periodic orbit bounds a disk-like global section exactly when it is unknotted with self-linking number −1-1−1. The criterion is used in celestial mechanics: Joung and van Koert apply it to validated periodic orbits of the restricted three-body problem (arXiv:2407.19159).

Timeline.

  • 1998. Hofer, Wysocki and Zehnder prove that every dynamically convex contact form on S3S^3S3 has some periodic orbit P0P_0P0​, with Conley–Zehnder index 333, that bounds a disk-like global section. That disk is a page of an open book adapted to the flow. Strictly convex energy surfaces in R4\mathbb{R}^4R4 are dynamically convex (Ann. of Math. 148).
  • 2008/2012. Hryniewicz proves the "unknotted, self-linking −1-1−1" characterization in the non-degenerate case (arXiv:0812.4076).
  • 2010/2011. Hryniewicz and Salomão treat non-degenerate tight contact forms on S3S^3S3. Two extra conditions appear there: μCZ≥3\mu_{CZ}\ge 3μCZ​≥3, and linking with every orbit of index 222 (arXiv:1006.0049).
  • 2011/2014. Hryniewicz removes non-degeneracy for dynamically convex forms (arXiv:1105.2077, Theorem 1.7). In the same paper, Theorem 1.8 shows that any orbit coming from a fixed point of the first-return map of a disk-like section is again such a binding.
  • 2012. Albers, Fish, Frauenfelder, Hofer and van Koert use this circle of ideas to get disk-like sections in the planar circular restricted three-body problem (arXiv:1103.3881).

Setting

Use coordinates x=(q1,p1,q2,p2)x=(q_1,p_1,q_2,p_2)x=(q1​,p1​,q2​,p2​) on R4\mathbb{R}^4R4, the Liouville form λ0=12∑j(qj dpj−pj dqj)\lambda_0=\tfrac12\sum_j (q_j\,dp_j-p_j\,dq_j)λ0​=21​∑j​(qj​dpj​−pj​dqj​) and the symplectic form ω0=dλ0=∑jdqj∧dpj\omega_0=d\lambda_0=\sum_j dq_j\wedge dp_jω0​=dλ0​=∑j​dqj​∧dpj​.

Let H:R4→RH:\mathbb{R}^4\to\mathbb{R}H:R4→R be smooth and set S=H−1(1)S=H^{-1}(1)S=H−1(1). Assume that every ray from the origin meets SSS exactly once, and that it crosses SSS transversally:

dH(x) x>0(x∈S).dH(x)\,x>0\qquad(x\in S).dH(x)x>0(x∈S).

Then SSS is a strictly star-shaped hypersurface diffeomorphic to S3S^3S3. Every contact form on S3S^3S3 that matters below arises this way, up to diffeomorphism (see Formalization scope).

The Hamiltonian vector field XHX_HXH​ is defined by ιXHω0=−dH\iota_{X_H}\omega_0=-dHιXH​​ω0​=−dH. With this sign, λ0(XH)=12 dH(x) x>0\lambda_0(X_H)=\tfrac12\,dH(x)\,x>0λ0​(XH​)=21​dH(x)x>0 on SSS. So XH∣SX_H|_SXH​∣S​ is a positive multiple of the Reeb vector field of the contact form λ0∣S\lambda_0|_Sλ0​∣S​, and its orbits are the Reeb orbits reparametrized. A periodic orbit P=(x,T)P=(x,T)P=(x,T) is a solution with x(T)=x(0)x(T)=x(0)x(T)=x(0) and T>0T>0T>0. It is prime when TTT is its least positive period. The contact structure is ξ=ker⁡λ0∣S\xi=\ker\lambda_0|_Sξ=kerλ0​∣S​.

  • Conley–Zehnder index. Fix the global frame of ξ\xiξ given by the quaternionic rotations of ∇H\nabla H∇H. Along PPP, the linearized flow restricted to ξ\xiξ is a path φ:[0,1]→Sp(1)\varphi:[0,1]\to Sp(1)φ:[0,1]→Sp(1) with φ(0)=I\varphi(0)=Iφ(0)=I. The winding interval I(φ)I(\varphi)I(φ) collects the total rotations of all nonzero vectors, measured in turns. Then μCZ(P)\mu_{CZ}(P)μCZ​(P) is the lower semicontinuous index of Hryniewicz's §2.1.1. In particular,
μCZ(P)≥3  ⟺  min⁡I(φ)>1,\mu_{CZ}(P)\ge 3 \iff \min I(\varphi)>1,μCZ​(P)≥3⟺minI(φ)>1,

that is, every nonzero transverse vector turns by more than one full turn.

  • Dynamical convexity. The flow is dynamically convex if μCZ(P)≥3\mu_{CZ}(P)\ge 3μCZ​(P)≥3 for every periodic orbit PPP in SSS, prime or multiply covered.
  • Disk-like global surface of section. A smoothly embedded closed disk D⊂SD\subset SD⊂S such that ∂D=x(R)\partial D=x(\mathbb{R})∂D=x(R) for a periodic orbit PPP, XHX_HXH​ is transverse to D∖∂DD\setminus\partial DD∖∂D, and every trajectory not contained in ∂D\partial D∂D meets DDD at arbitrarily large positive and negative times. Then PPP bounds DDD.
  • Unknotted. PPP is unknotted if x(R)x(\mathbb{R})x(R) is the boundary of some smoothly embedded closed disk in SSS.
  • Self-linking number. Push xxx off itself along the global frame of ξ\xiξ to a disjoint loop x′x'x′. Then
sl⁡(P)=lk⁡(x,x′)∈Z,\operatorname{sl}(P)=\operatorname{lk}(x,x')\in\mathbb{Z},sl(P)=lk(x,x′)∈Z,

the linking number in S≅S3S\cong S^3S≅S3, with SSS oriented as the boundary of the star-shaped domain it bounds. This agrees with Hryniewicz's Definition 1.5, which uses a section of ξ\xiξ over a spanning disk.

Formalization targets

Goal: Hryniewicz's criterion (Theorem 1.7, first sentence)

For every dynamically convex strictly star-shaped SSS and every prime periodic orbit Pˉ\bar PPˉ:

Pˉ bounds a disk-like global surface of section  ⟺  Pˉ is unknotted and sl⁡(Pˉ)=−1.\bar P \text{ bounds a disk-like global surface of section} \iff \bar P \text{ is unknotted and } \operatorname{sl}(\bar P)=-1.Pˉ bounds a disk-like global surface of section⟺Pˉ is unknotted and sl(Pˉ)=−1.

The statement fixes no constants and no non-degeneracy, and it covers every dynamically convex star-shaped surface.

Stronger: adapted open book (Theorem 1.7, second sentence)

If Pˉ\bar PPˉ is unknotted with sl⁡(Pˉ)=−1\operatorname{sl}(\bar P)=-1sl(Pˉ)=−1, then S∖xˉ(R)S\setminus \bar x(\mathbb{R})S∖xˉ(R) fibres smoothly over R/Z\mathbb{R}/\mathbb{Z}R/Z. Every fibre is the interior of a disk-like global surface of section whose oriented boundary is Pˉ\bar PPˉ.

Further: new bindings from fixed points (Theorem 1.8)

Let D0D_0D0​ be any disk-like global section. Every periodic orbit through a fixed point of the first-return map of D0∖∂D0D_0\setminus\partial D_0D0​∖∂D0​ is unknotted, has self-linking number −1-1−1, and so bounds the page of an adapted open book.

Significance

The result. The criterion turns a dynamical question into a topological check. It does not depend on whether the orbit is degenerate, and degenerate orbits are what one meets at bifurcations and on symmetric levels. Every periodic orbit in a strictly convex energy surface that is unknotted with sl⁡=−1\operatorname{sl}=-1sl=−1 is a binding, so the flow is organised by many open books at once. Theorem 1.8 makes this concrete: the Hamiltonian flow twists around two different bindings, ∂D0\partial D_0∂D0​ and ∂D1\partial D_1∂D1​. In applications, numerically validated orbits become analytic global sections without a separate non-degeneracy check (Joung–van Koert, Theorems 1.2 and 1.5).

Formalizing it. The theorem is proved, in a 50-page paper that relies on Hofer–Wysocki–Zehnder's theory of pseudo-holomorphic curves in symplectizations. It has no machine-checked proof. Mathlib has no Conley–Zehnder index, no self-linking number, no linking number of curves in S3S^3S3, and no global surfaces of section. A Lean statement fixes every sign and orientation convention involved: the sign of XHX_HXH​, the orientation of SSS, which push-off defines sl⁡\operatorname{sl}sl, and the index of degenerate orbits. Each of these is easy to get wrong in prose. Formal proofs of the parts that use no holomorphic curves are valuable on their own: the necessity direction, the description of the index by winding intervals, and the explicit ellipsoid examples.

Difficulty

The obvious route is to approximate the contact form by non-degenerate forms λk→λ\lambda_k\to\lambdaλk​→λ that keep Pˉ\bar PPˉ as an orbit, and then apply the non-degenerate theorems. This fails. The λk\lambda_kλk​ need not be dynamically convex. They can have orbits of very high action with μCZ=2\mu_{CZ}=2μCZ​=2 that are not linked with Pˉ\bar PPˉ, so the Hryniewicz–Salomão criterion does not apply to λk\lambda_kλk​ (Hryniewicz, p. 4). The families of planes that would give the pages for λk\lambda_kλk​ have to be controlled directly as k→∞k\to\inftyk→∞, and this is not a formal limit argument.

A second obstruction is genuinely global. A disk spanning Pˉ\bar PPˉ and transverse to the flow in its interior is easy to produce when sl⁡(Pˉ)=−1\operatorname{sl}(\bar P)=-1sl(Pˉ)=−1. Showing that every trajectory returns to it is the whole content of the theorem, and no local or perturbative argument gives it.

For the formalization, nothing in the proof of sufficiency avoids finite-energy pseudo-holomorphic planes: Fredholm theory, asymptotic analysis, bubbling-off and compactness all enter. None of this exists in Lean.

Formalization scope

  • Ambient space. R4\mathbb{R}^4R4 is Fin 4 → ℝ with coordinates ordered (q1,p1,q2,p2)(q_1,p_1,q_2,p_2)(q1​,p1​,q2​,p2​). λ0\lambda_0λ0​, ω0\omega_0ω0​ and XHX_HXH​ are defined explicitly, with the sign conventions above.
  • Energy surfaces. Star-shaped surfaces are smooth (ContDiff ℝ ⊤) functions HHH with the ray condition and dH(x)x>0dH(x)x>0dH(x)x>0 on H−1(1)H^{-1}(1)H−1(1). The Reeb flow of a general dynamically convex form on S3S^3S3 reduces to this case, up to diffeomorphism and positive time change: such a form is tight (Hofer–Wysocki–Zehnder), and every tight form on S3S^3S3 comes from a star-shaped hypersurface (Eliashberg 1992). That reduction is not part of the targets. Hryniewicz makes the same reduction (§3, first paragraph).
  • Flow. The flow is the flow of XHX_HXH​, not of the Reeb field. All notions in the targets are invariant under positive time change. Periodic orbits are solutions of x˙=XH(x)\dot x=X_H(x)x˙=XH​(x) on all of R\mathbb{R}R. "Prime" means the recorded period is least.
  • Index. μCZ≥3\mu_{CZ}\ge 3μCZ​≥3 is encoded by the winding-interval condition in the global quaternionic frame, with degenerate orbits included. Multiply covered orbits are included in dynamical convexity.
  • Disks. Disks are smooth embeddings of the closed unit disk (injective, with injective differential up to the boundary). The return condition demands hits at arbitrarily large positive and negative times.
  • Ruling out vacuous encodings. A version without the two-sided return condition, with a dynamical-convexity predicate that no surface satisfies, or with sl⁡\operatorname{sl}sl that is not a linking number of the push-off, proves a different theorem. The ellipsoid milestone below is a non-vacuity check on the definitions.
  • Infrastructure. A complete development needs the following.
    • Reusable beyond this mission: the Conley–Zehnder index of paths in Sp(1)Sp(1)Sp(1), the linking number of disjoint loops in S3S^3S3 (or in R3\mathbb{R}^3R3 after stereographic projection), and global flows of vector fields on compact level sets.
    • Specific to this proof: contact topology of spanning disks (characteristic foliations, elimination of singularities), and finite-energy planes in R×S3\mathbb{R}\times S^3R×S3 with their Fredholm, asymptotic and compactness theory.
  • Contributions welcome. The definition layer, the index and linking-number libraries, the ellipsoid examples, Lemma 2.1, the necessity direction, Lemma 3.12, and any sub-step of the holomorphic-curve argument stated as an independent lemma.

Selected references

  • H. Hofer, K. Wysocki, E. Zehnder, The dynamics on three-dimensional strictly convex energy surfaces, Ann. of Math. 148 (1998), 197–289. https://doi.org/10.2307/120994
  • U. L. Hryniewicz, Fast finite-energy planes in symplectizations and applications, Trans. Amer. Math. Soc. 364 (2012), 1859–1931. https://arxiv.org/abs/0812.4076
  • U. L. Hryniewicz, P. A. S. Salomão, On the existence of disk-like global sections for Reeb flows on the tight 3-sphere, Duke Math. J. 160 (2011), 415–465. https://arxiv.org/abs/1006.0049
  • U. L. Hryniewicz, Systems of global surfaces of section for dynamically convex Reeb flows on the 3-sphere, J. Symplectic Geom. 12 (2014), 791–862. https://arxiv.org/abs/1105.2077
  • U. L. Hryniewicz, P. A. S. Salomão, Global surfaces of section for Reeb flows in dimension three and beyond, Proc. ICM 2018 (extended version). https://arxiv.org/abs/1712.01925
  • P. Albers, J. W. Fish, U. Frauenfelder, H. Hofer, O. van Koert, Global surfaces of section in the planar restricted 3-body problem, Arch. Ration. Mech. Anal. 204 (2012), 273–284. https://arxiv.org/abs/1103.3881
  • C. Joung, O. van Koert, Computational symplectic topology and symmetric orbits in the restricted three-body problem, Nonlinearity 38 (2025), 025015. https://arxiv.org/abs/2407.19159
  • Y. Eliashberg, Contact 3-manifolds twenty years since J. Martinet's work, Ann. Inst. Fourier 42 (1992), 165–192. https://doi.org/10.5802/aif.1288
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🏆Completed
Differential GeometryGeometry & TopologySymplectic Geometry·Captain: Mazecto

Gray's Stability Theorem for Contact StructuresResearch Paper

Motivation

A contact structure on a manifold of odd dimension 2k+12k+12k+1 is a field of hyperplanes ξ=ker⁡α\xi=\ker\alphaξ=kerα that is as far from integrable as possible. Contact structures are the odd-dimensional counterpart of symplectic forms. They arise on every star-shaped energy level of a Hamiltonian system, on unit cotangent bundles (geodesic flows), and on links of singularities. They are the setting of Reeb dynamics and of the Weinstein conjecture.

Gray's stability theorem says that on a closed manifold contact structures have no local moduli. If ξt\xi_tξt​, t∈[0,1]t\in[0,1]t∈[0,1], is a smooth family of contact structures, there is an isotopy ψt\psi_tψt​ with Tψt(ξ0)=ξtT\psi_t(\xi_0)=\xi_tTψt​(ξ0​)=ξt​. A contact structure can therefore be deformed only within its isotopy class, and every classification of contact structures (tight versus overtwisted, Eliashberg's classification on S3S^3S3) is a classification up to isotopy because of it.

Timeline.

  • 1959. Gray proves stability with deformation theory in the style of Kodaira–Spencer (Ann. of Math. 69).
  • 1965. Moser proves the analogous stability for volume forms by integrating a time-dependent vector field, now called the Moser trick (Trans. AMS 120).
  • Later. The Moser trick becomes the standard proof of Gray's theorem. Geiges' survey gives a short complete proof (arXiv:math/0307242, Theorem 2.20), which is the source of this mission. Its remarks record the limits of the statement: contact forms are not stable (Remark 2.21(1)), and on the open manifold S1×R2S^1\times\mathbb{R}^2S1×R2 stability fails (Remark 2.21(2), after Eliashberg).

Setting

The closed manifold is a compact submanifold of Euclidean space. Let F:Rn→RcF:\mathbb{R}^n\to\mathbb{R}^cF:Rn→Rc be smooth, let M=F−1(0)M=F^{-1}(0)M=F−1(0) be compact, and assume DF(y)DF(y)DF(y) is surjective for every y∈My\in My∈M. Then MMM is a closed smooth manifold of dimension n−cn-cn−c with tangent spaces

TyM=ker⁡DF(y).T_yM=\ker DF(y).Ty​M=kerDF(y).

A one-form is a smooth map α:Rn→(Rn)∗\alpha:\mathbb{R}^n\to(\mathbb{R}^n)^*α:Rn→(Rn)∗, restricted to TMTMTM. Its exterior derivative is

dαy(u,v)=Dαy(u)(v)−Dαy(v)(u).d\alpha_y(u,v)=D\alpha_y(u)(v)-D\alpha_y(v)(u).dαy​(u,v)=Dαy​(u)(v)−Dαy​(v)(u).
  • Contact form. α\alphaα is a contact form on MMM if at every y∈My\in My∈M the covector αy\alpha_yαy​ is nonzero on TyMT_yMTy​M and dαyd\alpha_ydαy​ is non-degenerate on the hyperplane
ξy=TyM∩ker⁡αy.\xi_y=T_yM\cap\ker\alpha_y.ξy​=Ty​M∩kerαy​.

This is the condition α∧(dα)k≠0\alpha\wedge(d\alpha)^k\neq0α∧(dα)k=0 in the form of Geiges' Remark 2.3. It forces dim⁡M\dim MdimM to be odd. The contact structure is ξ=ker⁡α\xi=\ker\alphaξ=kerα. Contact structures are cooriented throughout, as in Geiges' standing assumption (§2).

  • Smooth family. A family αt\alpha_tαt​ is smooth if (t,y)↦αt(y)(t,y)\mapsto\alpha_t(y)(t,y)↦αt​(y) is smooth. It is a family of contact forms if each αt\alpha_tαt​, t∈[0,1]t\in[0,1]t∈[0,1], is a contact form on MMM.
  • Isotopy. An isotopy of MMM is a smooth map (t,y)↦ψt(y)(t,y)\mapsto\psi_t(y)(t,y)↦ψt​(y) with ψ0=id\psi_0=\mathrm{id}ψ0​=id on MMM, such that each ψt\psi_tψt​, t∈[0,1]t\in[0,1]t∈[0,1], maps MMM bijectively onto MMM with injective differential on TMTMTM, i.e. is a diffeomorphism of MMM.
  • Pull-back. (ψt∗α)y(v)=αψt(y)(Dψt(y) v)(\psi_t^*\alpha)_y(v)=\alpha_{\psi_t(y)}(D\psi_t(y)\,v)(ψt∗​α)y​(v)=αψt​(y)​(Dψt​(y)v).

Formalization targets

Goal: Gray stability (Theorem 2.20)

For every smooth family of contact forms αt\alpha_tαt​, t∈[0,1]t\in[0,1]t∈[0,1], on MMM there is an isotopy ψt\psi_tψt​ of MMM with

Tψt(ξ0)=ξt(t∈[0,1]),ξt=ker⁡αt,T\psi_t(\xi_0)=\xi_t\qquad(t\in[0,1]),\qquad\xi_t=\ker\alpha_t,Tψt​(ξ0​)=ξt​(t∈[0,1]),ξt​=kerαt​,

stated pointwise: for v∈TyMv\in T_yMv∈Ty​M, α0(v)=0\alpha_0(v)=0α0​(v)=0 iff αt(Dψt(y)v)=0\alpha_t(D\psi_t(y)v)=0αt​(Dψt​(y)v)=0.

The goal concerns the contact structures. It fixes no normalization of the forms and no dimension.

Stronger: conformal form

The same isotopy can be chosen with smooth functions λt>0\lambda_t>0λt​>0 such that

ψt∗αt=λt α0on TM.\psi_t^*\alpha_t=\lambda_t\,\alpha_0\quad\text{on }TM.ψt∗​αt​=λt​α0​on TM.

Stronger: stationary points (Remark 2.21(3))

Moreover, every point p∈Mp\in Mp∈M at which α˙t\dot\alpha_tα˙t​ vanishes on TpMT_pMTp​M for all ttt stays fixed: ψt(p)=p\psi_t(p)=pψt​(p)=p.

Significance

The result. Gray stability is the basic rigidity statement of contact topology.

  • It reduces the classification of contact structures to isotopy classes, so invariants of a contact manifold are constant along deformations.
  • It is the first step of many local normal forms: Darboux's theorem and the neighbourhood theorems for Legendrian and transverse submanifolds are proved by applying it, or its proof, near a submanifold (Geiges §2.4–2.5).
  • In Hamiltonian dynamics it identifies the contact structures of a continuous family of star-shaped energy levels. Topological invariants of transverse periodic orbits, such as the self-linking number, are then constant along the family.

Formalizing it. The theorem is classical and has a short proof on paper. Mathlib, at the revision used here, has no differential forms on manifolds, no Lie derivative, no global flows of time-dependent vector fields on compact submanifolds, and no contact structures. The mission builds these concretely on submanifolds of Rn\mathbb{R}^nRn:

  • one-forms, their exterior derivative and pull-back;
  • the derivative of a pulled-back family along a flow (Lemma 2.19);
  • the pointwise linear algebra of a contact form: the Reeb vector, and the unique solution of the Moser equation;
  • global flows of smooth time-dependent vector fields tangent to a compact submanifold.

All of these are reusable for Moser's theorem on volume and symplectic forms and for the Darboux and neighbourhood theorems.

Difficulty

The proof is soft, but two steps are not formal.

  1. Solving for the vector field. Writing ψt\psi_tψt​ as the flow of XtX_tXt​, the equation ψt∗αt=λtα0\psi_t^*\alpha_t=\lambda_t\alpha_0ψt∗​αt​=λt​α0​ becomes
α˙t+iXtdαt=μtαt,Xt∈ξt.\dot\alpha_t+i_{X_t}d\alpha_t=\mu_t\alpha_t,\qquad X_t\in\xi_t.α˙t​+iXt​​dαt​=μt​αt​,Xt​∈ξt​.

It has a unique solution at each point, but only because dαtd\alpha_tdαt​ is non-degenerate on ξt\xi_tξt​ and the Reeb vector spans the kernel of dαt∣TMd\alpha_t|_{TM}dαt​∣TM​. The solution must also depend smoothly on (t,y)(t,y)(t,y) and be tangent to MMM; the ambient form αt\alpha_tαt​ is in general not contact off MMM. 2. Integrating it. The isotopy is the flow of XtX_tXt​, which must exist for all t∈[0,1]t\in[0,1]t∈[0,1] and stay on MMM. Compactness of MMM enters exactly here. On open manifolds the statement is false (Remark 2.21(2)).

The tempting shortcut of asking for ψt∗αt=α0\psi_t^*\alpha_t=\alpha_0ψt∗​αt​=α0​ does not work. Contact forms themselves are not stable, as the Hopf family on S3S^3S3 shows (Remark 2.21(1)), and the conformal factor λt\lambda_tλt​ cannot be dropped.

Formalization scope

  • Representation.
    • Rn\mathbb{R}^nRn is Fin n → ℝ; MMM is a compact regular level set F−1(0)F^{-1}(0)F−1(0) of a smooth F:Rn→RcF:\mathbb{R}^n\to\mathbb{R}^cF:Rn→Rc.
    • One-forms are maps Rn→(Rn→LR)\mathbb{R}^n\to(\mathbb{R}^n\to_L\mathbb{R})Rn→(Rn→L​R), smooth families are jointly smooth in (t,y)(t,y)(t,y) on R×Rn\mathbb{R}\times\mathbb{R}^nR×Rn, and dαd\alphadα is the antisymmetrized derivative.
    • An isotopy is a jointly smooth ψ:R×Rn→Rn\psi:\mathbb{R}\times\mathbb{R}^n\to\mathbb{R}^nψ:R×Rn→Rn that restricts, for t∈[0,1]t\in[0,1]t∈[0,1], to diffeomorphisms of MMM.
  • Committed conventions.
    • Contact structures are cooriented, i.e. given by global contact forms.
    • The contact condition is the non-degeneracy of dαd\alphadα on ξ\xiξ (Remark 2.3), not a wedge power.
    • Only the restrictions to TMTMTM and the values for t∈[0,1]t\in[0,1]t∈[0,1] matter.
  • Scope relative to the source. Every closed manifold embeds in some Rn\mathbb{R}^nRn, but not every closed manifold is a regular level set, since that requires a trivial normal bundle. The targets cover regular level sets, including all spheres and all star-shaped energy levels. The abstract version on any closed manifold is outside the targets until Mathlib has differential forms on manifolds.
  • Ruling out vacuous encodings. The isotopy must start at the identity on MMM, map MMM onto MMM for every t∈[0,1]t\in[0,1]t∈[0,1], and be a diffeomorphism there. Dropping any of these makes the goal trivial; for instance, the constant isotopy satisfies the goal whenever all ξt\xi_tξt​ agree. The Hopf family milestone checks that the contact condition is satisfiable and that the conformal factor is necessary.
  • Contributions welcome. The linear-algebra milestones (Reeb vector, Moser equation), Lemma 2.19, global flows on compact level sets, and the Hopf-family example. Moser's theorem for volume forms would be a natural sibling result built on the same infrastructure.

Selected references

  • J. W. Gray, Some global properties of contact structures, Ann. of Math. 69 (1959), 421–450. https://doi.org/10.2307/1970192
  • H. Geiges, Contact geometry, in Handbook of Differential Geometry, Vol. II, Elsevier (2006), 315–382; §2.2, Lemma 2.19, Theorem 2.20, Remark 2.21. https://arxiv.org/abs/math/0307242
  • H. Geiges, An Introduction to Contact Topology, Cambridge Stud. Adv. Math. 109, Cambridge Univ. Press (2008), §2.2. https://doi.org/10.1017/CBO9780511611438
  • J. Moser, On the volume elements on a manifold, Trans. Amer. Math. Soc. 120 (1965), 286–294. https://doi.org/10.1090/S0002-9947-1965-0182927-5
  • Y. Eliashberg, Contact 3-manifolds twenty years since J. Martinet's work, Ann. Inst. Fourier 42 (1992), 165–192. https://doi.org/10.5802/aif.1288
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CombinatoricsDiscrete GeometryGraph Theory·Captain: mikedeng1

Diameter of Polyhedra: Limits of Abstraction 1: The Base Abstraction in Dimension n/4 with n Facets Has Diameter Ω(n²/log n)Research Paper

Motivation

Whether the diameter of a polyhedron is bounded by a polynomial in its number of facets is one of the central open questions of convex geometry, and it bears directly on linear programming: the diameter of the graph of a polyhedron is a lower bound on the number of pivots of any simplex method that moves along edges. Write △u(d,n)\triangle_u(d,n)△u​(d,n) for the largest diameter of a ddd-dimensional polyhedron with nnn facets. The best known bounds are

n−d+⌊d/5⌋  ≤  △u(d,n)  ≤  n1+log⁡d,n - d + \lfloor d/5 \rfloor \;\le\; \triangle_u(d,n) \;\le\; n^{1+\log d},n−d+⌊d/5⌋≤△u​(d,n)≤n1+logd,

due to Klee and Walkup (1967) and Kalai and Kleitman (1992), and the gap between them has stood for decades.

A recurring approach is to isolate a few purely combinatorial properties of polyhedra and to prove bounds for every object having them. Eisenbrand, Hähnle, Razborov and Rothvoß (2010) proposed a base abstraction defined by a single property, shared by all abstractions from which earlier bounds were derived. They showed that the known upper bounds survive in it, and, as their main result, that it admits almost-quadratic diameter. This mission formalizes that lower bound.

Timeline.

  • 1967: Klee and Walkup, lower bound n−d+⌊d/5⌋n-d+\lfloor d/5\rfloorn−d+⌊d/5⌋ for unbounded polyhedra.
  • 1970: Larman, △u(d,n)≤2d−1n\triangle_u(d,n) \le 2^{d-1} n△u​(d,n)≤2d−1n (linear in fixed dimension).
  • 1974: Adler, Dantzig and Murty study abstract polytopes and their diameters.
  • 1992: Kalai and Kleitman, the quasi-polynomial bound n1+log⁡dn^{1+\log d}n1+logd.
  • 2010: Eisenbrand, Hähnle, Razborov and Rothvoß, the base abstraction; both upper bounds hold in it, and its diameter is Ω(n2/log⁡n)\Omega(n^2/\log n)Ω(n2/logn) in dimension n/4n/4n/4.
  • 2012: Santos disproves the Hirsch conjecture for polytopes; the polynomial question remains open.

Setting

Let [n]={1,…,n}[n] = \{1,\dots,n\}[n]={1,…,n} and let ([n]d)\binom{[n]}{d}(d[n]​) be the family of its ddd-element subsets. Consider a graph GGG whose vertex set VVV is a nonempty subfamily of ([n]d)\binom{[n]}{d}(d[n]​). The graph satisfies condition i) if

for each u,v∈Vu, v \in Vu,v∈V there exists a path connecting uuu and vvv whose intermediate vertices all contain u∩vu \cap vu∩v.

The base abstraction Bd,n\mathcal B_{d,n}Bd,n​ is the class of all such graphs; ddd is called the dimension and nnn the number of facets. Write distG(u,v)\mathrm{dist}_G(u,v)distG​(u,v) for the length of a shortest uuu–vvv path, and

D(d,n)=max⁡{distG(u,v):G∈Bd,n, u,v∈V(G)}.D(d,n) = \max\{\mathrm{dist}_G(u,v) : G \in \mathcal B_{d,n},\ u, v \in V(G)\}.D(d,n)=max{distG​(u,v):G∈Bd,n​, u,v∈V(G)}.

The geometry behind the definition: in a non-degenerate polyhedron every vertex lies on exactly ddd facets, so labelling vertices by their facets gives distinct ddd-subsets of [n][n][n]; and two vertices can be joined without leaving the smallest face containing both, i.e. through vertices lying on every facet common to uuu and vvv. Hence △u(d,n)≤D(d,n)\triangle_u(d,n) \le D(d,n)△u​(d,n)≤D(d,n) (the subject of a separate mission of this series).

In the Lean development, EHRR10.LowerBound.CondI V G is condition i), and EHRR10.LowerBound.InB d n V G says that VVV is nonempty, all its members have ddd elements, and condition i) holds.

Formalization targets

Goal: almost-quadratic diameter in dimension n/4n/4n/4

D(n/4, n)=Ω ⁣(n2log⁡n).D(n/4,\, n) = \Omega\!\left(\frac{n^2}{\log n}\right).D(n/4,n)=Ω(lognn2​).

Explicitly, there are c>0c > 0c>0 and NNN such that for every n≥Nn \ge Nn≥N with 4∣n4 \mid n4∣n there is a graph G∈Bn/4, nG \in \mathcal B_{n/4,\,n}G∈Bn/4,n​ and two vertices u,vu, vu,v of GGG with distG(u,v)≥c n2/log⁡n\mathrm{dist}_G(u,v) \ge c\, n^2/\log ndistG​(u,v)≥cn2/logn. The constants ccc and NNN are left unfixed, so the goal survives any improvement in the constant.

There are no milestones: the source is an extended abstract that states the result without a proof and names no intermediate lemma.

Significance

The result. Since △u(d,n)≤D(d,n)\triangle_u(d,n) \le D(d,n)△u​(d,n)≤D(d,n), any proof of a bound on DDD bounds the diameter of all non-degenerate polyhedra. The paper shows that the Kalai–Kleitman and Larman bounds are of this kind. The lower bound shows the limits of the approach: an argument that uses only condition i) cannot prove a linear (Hirsch-type) bound, because D(n/4,n)D(n/4,n)D(n/4,n) grows almost quadratically in nnn. Any proof of a linear bound must use further geometric properties of polyhedra. A polynomial, even quadratic, upper bound for DDD is not excluded by the result.

Formalizing it. The result is proved in the literature (Math. Oper. Res. 35 (2010) 786–794); it has no machine-checked proof. A formal proof requires an explicit combinatorial construction of graphs in the base abstraction with large diameter and a probabilistic existence argument, neither of which is currently on the platform. The platform's Hirsch campaign has the same abstraction in its layer-family form (Hirsch_clf, whose description mentions the Ω(n2/log⁡n)\Omega(n^2/\log n)Ω(n2/logn) families in prose) and the proved upper bound Hirsch.clf_saturated_quadratic_bound, L≤d(n−d)L \le d(n-d)L≤d(n−d), on a subclass that contains the constructions of this paper; neither states the lower bound.

Difficulty

A long path through all of ([n]d)\binom{[n]}{d}(d[n]​) has exponential length but violates condition i): two vertices of the path generally share elements that some intermediate vertex lacks. Condition i) must hold for every pair of vertices simultaneously, which forces the vertices containing any fixed set to induce a connected subgraph. Building a long graph means arranging many ddd-sets so that each of these exponentially many connectivity constraints holds at once while the graph distance between two vertices stays large. The authors announce that their construction relies on disjoint covering designs, and that the existence of such designs with the required parameters is obtained from the Lovász Local Lemma.

Formalization scope

  • [n][n][n] is Fin n; vertices are the ddd-sets themselves, V : Finset (Finset (Fin n)) and G : SimpleGraph V. Distinct vertices carry distinct labels.
  • Condition i) is stated with walks, and requires every vertex of the walk (endpoints included, which is automatic) to contain u∩vu \cap vu∩v. A walk contains a path on a subset of its vertices, so this is the page's condition.
  • "Connected" is encoded as V≠∅V \ne \emptysetV=∅; connectivity follows from condition i).
  • The page writes D(n/4,n)D(n/4,n)D(n/4,n) without rounding; the goal is read literally: 4∣n4 \mid n4∣n and dimension exactly n/4n/4n/4.
  • Ω(⋅)\Omega(\cdot)Ω(⋅) is made explicit as ∃c>0,∃N,∀n≥N\exists c > 0, \exists N, \forall n \ge N∃c>0,∃N,∀n≥N. The logarithm is natural (Real.log); the base only rescales ccc.
  • "D(n/4,n)≥BD(n/4,n) \ge BD(n/4,n)≥B" is stated as the existence of one graph in the class with two vertices at SimpleGraph.dist at least BBB; DDD is not defined as a supremum, so no junk value enters. SimpleGraph.dist returns 000 for unreachable pairs, which could only make the statement harder.
  • Only the lower half of Ω\OmegaΩ is claimed, as on the page.

The goal cannot be trivialized by a non-injective labelling (vertices are the sets), by checking condition i) only on adjacent pairs (it is required for all pairs, with u∩vu\cap vu∩v kept along the whole walk), or by a zero constant (c>0c > 0c>0 is required).

Infrastructure that a solution needs and that is reusable beyond this mission: covering designs and disjoint covering designs over Finset (Fin n), the Lovász Local Lemma (posed on the platform as AppliedComb.ManyFaces.local_lemma_symmetric), and a toolkit for proving condition i) for graphs assembled from blocks. Contributions of any of these as separate theorems are welcome.

Selected references

  • F. Eisenbrand, N. Hähnle, A. Razborov, T. Rothvoß, Diameter of Polyhedra: Limits of Abstraction, Dagstuhl Seminar Proceedings 10211 (Flexible Network Design), 2010 (the extended abstract this mission cites). http://drops.dagstuhl.de/opus/volltexte/2010/2724
  • F. Eisenbrand, N. Hähnle, A. Razborov, T. Rothvoß, Diameter of Polyhedra: Limits of Abstraction, Mathematics of Operations Research 35(4), 786–794, 2010 (full proofs). https://doi.org/10.1287/moor.1100.0470
  • G. Kalai, D. J. Kleitman, A quasi-polynomial bound for the diameter of graphs of polyhedra, Bull. Amer. Math. Soc. 26(2), 315–316, 1992. https://doi.org/10.1090/S0273-0979-1992-00285-9
  • D. G. Larman, Paths on polytopes, Proc. London Math. Soc. 20(3), 161–178, 1970. https://doi.org/10.1112/plms/s3-20.1.161
  • V. Klee, D. W. Walkup, The d-step conjecture for polyhedra of dimension d < 6, Acta Math. 117, 53–78, 1967. https://doi.org/10.1007/BF02395040
  • F. Santos, A counterexample to the Hirsch conjecture, Annals of Mathematics 176(1), 383–412, 2012. https://doi.org/10.4007/annals.2012.176.1.7
  • N. Alon, J. Spencer, The Probabilistic Method, 3rd ed., Wiley, 2008 (Lovász Local Lemma).
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Machine LearningProbabilityStatistics·Captain: mikedeng1

Optimal Rates for the Regularized Least-Squares Algorithm III: Against Every Algorithm, a Single Distribution in P(b, c) Keeps the Expected Excess Risk above ℓ^(−cB/(cB+1)) for B > b (Theorem 3)Research Paper

Why individual lower rates

Regularized least squares (RLS) in a reproducing kernel Hilbert space is a basic estimator of nonparametric regression and of kernel-based learning. Its learning rate is the speed at which the expected excess risk goes to zero as the sample size ℓ\ellℓ grows. A rate is useful only if it is known to be optimal, and optimality is a lower-bound statement about all learning algorithms.

Caponnetto and De Vito (Found. Comput. Math. 7 (2007)) prove two kinds of lower bound. The first is a minimax lower rate (their Theorem 2): for every algorithm and every ℓ\ellℓ, some distribution in the prior is hard. Their Section 2 (p. 6) points out a weakness of this notion: the bad distribution may change with ℓ\ellℓ. A practitioner, however, faces one fixed unknown distribution and asks how the error decreases as data accumulate. The individual lower rate answers that question. It asks for a single distribution, chosen against the algorithm but not depending on ℓ\ellℓ, on which the expected excess risk stays above aℓa_\ellaℓ​ along infinitely many ℓ\ellℓ.

The notion comes from nonparametric regression. Györfi, Kohler, Krzyżak and Walk (A Distribution-Free Theory of Nonparametric Regression, Springer 2002, §3, Theorem 3.3) proved individual lower rates for classes of smooth regression functions. Theorem 3 of Caponnetto–De Vito carries the result to vector-valued RKHS with the spectral priors P(b,c)\mathcal P(b, c)P(b,c). Theorem 1 of the same paper shows that these priors are learned by RLS at rate ℓ−bc/(bc+1)\ell^{-bc/(bc+1)}ℓ−bc/(bc+1).

Setting

The input space XXX is Polish. The output space YYY is a real Hilbert space of finite dimension ddd. The hypothesis space H\mathcal HH is a separable real Hilbert space of functions f:X→Yf : X \to Yf:X→Y in which evaluation is continuous, so that f(x)=Kx∗ff(x) = K_x^* ff(x)=Kx∗​f for bounded operators Kx:Y→HK_x : Y \to \mathcal HKx​:Y→H. Hypothesis 1 asks that (x,t)↦⟨Ktv,Kxw⟩H(x, t) \mapsto \langle K_t v, K_x w\rangle_{\mathcal H}(x,t)↦⟨Kt​v,Kx​w⟩H​ be measurable and that Tr⁡(Kx∗Kx)≤κ\operatorname{Tr}(K_x^*K_x) \le \kappaTr(Kx∗​Kx​)≤κ for every xxx.

A distribution ρ\rhoρ on Z=X×YZ = X \times YZ=X×Y has marginal ρX\rho_XρX​ and conditional distributions ρ(⋅∣x)\rho(\cdot \mid x)ρ(⋅∣x). The risk of f∈Hf \in \mathcal Hf∈H is

E[f]=∫Z∥f(x)−y∥Y2 dρ(x,y).\mathcal E[f] = \int_Z \|f(x) - y\|_Y^2 \, d\rho(x, y).E[f]=∫Z​∥f(x)−y∥Y2​dρ(x,y).

Hypothesis 2 asks for square-integrable outputs, a minimizer fHf_{\mathcal H}fH​ of E\mathcal EE over H\mathcal HH, and a Bernstein-type moment bound on the noise y−fH(x)y - f_{\mathcal H}(x)y−fH​(x) with constants M,ΣM, \SigmaM,Σ.

The operator T=∫XKxKx∗ dρX(x)T = \int_X K_x K_x^*\, d\rho_X(x)T=∫X​Kx​Kx∗​dρX​(x) on H\mathcal HH satisfies ⟨Tf,g⟩=∫X⟨f(x),g(x)⟩Y dρX\langle Tf, g\rangle = \int_X \langle f(x), g(x)\rangle_Y \, d\rho_X⟨Tf,g⟩=∫X​⟨f(x),g(x)⟩Y​dρX​. Its nonzero eigenvalues are t1≥t2≥…t_1 \ge t_2 \ge \dotst1​≥t2​≥…, with orthonormal eigenvectors ene_nen​.

For positive constants M,Σ,R,α,βM, \Sigma, R, \alpha, \betaM,Σ,R,α,β and parameters 1<b<∞1 < b < \infty1<b<∞, 1≤c≤21 \le c \le 21≤c≤2, the prior P(b,c)\mathcal P(b, c)P(b,c) (Definition 1) is the set of probability measures ρ\rhoρ satisfying three conditions:

  • Hypothesis 2 holds for the minimal-norm minimizer fHf_{\mathcal H}fH​;
  • fH=T(c−1)/2gf_{\mathcal H} = T^{(c-1)/2} gfH​=T(c−1)/2g with ∥g∥H2≤R\|g\|_{\mathcal H}^2 \le R∥g∥H2​≤R (a source condition);
  • the eigenvalues satisfy α≤nbtn≤β\alpha \le n^b t_n \le \betaα≤nbtn​≤β for all n≥1n \ge 1n≥1.

A learning algorithm is a sequence of maps fℓ:Zℓ→Hf_\ell : Z^\ell \to \mathcal Hfℓ​:Zℓ→H, and fzℓf^\ell_{\mathbf z}fzℓ​ is its output on a sample z\mathbf zz of size ℓ\ellℓ drawn from ρℓ\rho^\ellρℓ.

Formalization targets

Goal: Theorem 3 (p. 11)

For every B>bB > bB>b,

inf⁡{fℓ} sup⁡ρ∈P(b,c) lim sup⁡ℓ→∞Ez∼ρℓ(E[fzℓ]−E[fH])ℓ−cB/(cB+1)>0.\inf_{\{f_\ell\}}\ \sup_{\rho \in \mathcal P(b, c)}\ \limsup_{\ell \to \infty} \frac{\mathbb E_{\mathbf z \sim \rho^\ell}\big(\mathcal E[f^\ell_{\mathbf z}] - \mathcal E[f_{\mathcal H}]\big)}{\ell^{-cB/(cB+1)}} > 0 .{fℓ​}inf​ ρ∈P(b,c)sup​ ℓ→∞limsup​ℓ−cB/(cB+1)Ez∼ρℓ​(E[fzℓ​]−E[fH​])​>0.

Equivalently, there is C>0C > 0C>0 such that every algorithm admits one ρ∈P(b,c)\rho \in \mathcal P(b, c)ρ∈P(b,c) with expected excess risk at least Cℓ−cB/(cB+1)C\ell^{-cB/(cB+1)}Cℓ−cB/(cB+1) for infinitely many ℓ\ellℓ. The constant may depend on the prior and on BBB, but not on the algorithm.

Milestones

  1. Proposition 7 (pp. 25–26). A fair sign sss observed as y=sg+ny = sg + ny=sg+n with i.i.d. N(0,σ2)\mathcal N(0, \sigma^2)N(0,σ2) noise has Bayes error Φ(−∥g∥/σ)\Phi(-\|g\|/\sigma)Φ(−∥g∥/σ).
  2. P′⊂P(b,c)\mathcal P' \subset \mathcal P(b, c)P′⊂P(b,c) (pp. 26–27). This concerns distributions with marginal ν\nuν and conditional distribution N(m(s)(x),σ2Id)\mathcal N(m^{(s)}(x), \sigma^2\mathrm{Id})N(m(s)(x),σ2Id), where
m(s)=∑nsnγn/tn en,γn=n−(Bc+1)ϵϵ+1αcR,m^{(s)} = \sum_n s_n\sqrt{\gamma_n/t_n}\,e_n, \qquad \gamma_n = n^{-(Bc+1)}\tfrac{\epsilon}{\epsilon+1}\alpha^c R,m(s)=n∑​sn​γn​/tn​​en​,γn​=n−(Bc+1)ϵ+1ϵ​αcR,

with ϵ=(B−b)c\epsilon = (B - b)cϵ=(B−b)c and s∈{±1}∞s \in \{\pm1\}^\inftys∈{±1}∞. Every such distribution belongs to the prior. 3. (63) (p. 27). Under these distributions, E[f]−E[m(s)]=∑n(cn−sn)2γn\mathcal E[f] - \mathcal E[m^{(s)}] = \sum_n (c_n - s_n)^2\gamma_nE[f]−E[m(s)]=∑n​(cn​−sn​)2γn​ with cn=tn/γn⟨f,en⟩c_n = \sqrt{t_n/\gamma_n}\langle f, e_n\ranglecn​=tn​/γn​​⟨f,en​⟩. 4. (68) (p. 28, corrected). ∑ℓγn≤1γn≥u1/(Bc+1)2Bc ℓ−Bc/(Bc+1)\sum_{\ell\gamma_n \le 1} \gamma_n \ge \tfrac{u^{1/(Bc+1)}}{2Bc}\,\ell^{-Bc/(Bc+1)}∑ℓγn​≤1​γn​≥2Bcu1/(Bc+1)​ℓ−Bc/(Bc+1) for ℓ≥(2Bc)Bc+1/u\ell \ge (2Bc)^{Bc+1}/uℓ≥(2Bc)Bc+1/u, where u=ϵϵ+1αcRu = \tfrac{\epsilon}{\epsilon+1}\alpha^c Ru=ϵ+1ϵ​αcR. 5. (67) (pp. 28–30). Averaged over independent fair signs SSS, the expected number of sign errors over {n:ℓγn≤1}\{n : \ell\gamma_n \le 1\}{n:ℓγn​≤1}, weighted by γn\gamma_nγn​, is at least Φ(−1/σ)∑ℓγn≤1γn\Phi(-1/\sigma)\sum_{\ell\gamma_n \le 1}\gamma_nΦ(−1/σ)∑ℓγn​≤1​γn​.

Significance

Theorem 3 shows that no algorithm, RLS included, converges on every fixed distribution of P(b,c)\mathcal P(b, c)P(b,c) faster than ℓ−cB/(cB+1)\ell^{-cB/(cB+1)}ℓ−cB/(cB+1), for any B>bB > bB>b. For c>1c > 1c>1 this exponent is arbitrarily close to the exponent bc/(bc+1)bc/(bc+1)bc/(bc+1) of the upper rate of Theorem 1, so RLS with the regularization parameter of Theorem 1 is near-optimal even in the individual sense. The paper notes (p. 6) that full individual optimality would still need an upper rate in expectation or an individual lower rate in probability; that question is outside this mission.

The theorem is proved on paper and has been cited widely. To our knowledge no part of it has been machine-checked. A formalization would produce:

  • a checked reduction from a learning lower bound to Gaussian sign testing;
  • a Lean model of Gaussian-noise regression with vector outputs;
  • an explicit, checked version of the corrected computation (68).

Difficulty

A minimax argument picks a hard distribution for each ℓ\ellℓ, and that is not allowed here: the distribution must be fixed before ℓ\ellℓ varies. The obvious repair, taking the worst distribution for one ℓ\ellℓ and keeping it, fails, because a distribution that is hard at sample size ℓ\ellℓ can be easy at sample size 10ℓ10\ell10ℓ.

What has to be shown is a lower bound that holds for one distribution simultaneously along infinitely many sample sizes. Bounds that hold separately at each ℓ\ellℓ, with a distribution that may depend on ℓ\ellℓ, do not combine into such a bound.

A second difficulty arises in any reduction to a coordinatewise testing problem: each observation yiy_iyi​ depends on all spectral coordinates of the regression function at once, so testing one coordinate is not literally the problem of Proposition 7.

Formalization scope

H\mathcal HH is Mathlib's RKHS ℝ H X Y, with KxK_xKx​ = RKHS.kerFun H x and YYY finite-dimensional. The paper's Σ\SigmaΣ is written Sig.

  • The operator TTT. It is never formed as an operator-valued integral. It enters through its quadratic form and through an eigen-system (en,tn)(e_n, t_n)(en​,tn​) with summable weights.
  • Indexing. Indices start at 000, so the paper's tnt_ntn​ is t (n-1).
  • The prior. InPrior encodes ρ∈P(b,c)\rho \in \mathcal P(b, c)ρ∈P(b,c), including "probability measure".
  • Expectations. Expectations are lintegrals of nonnegative quantities, and samples are Fin ℓ → X × Y under the product measure.
  • Algorithms. A learning algorithm is a family of maps from samples to H\mathcal HH, and it must be measurable.
  • Added hypothesis. P(b,c)\mathcal P(b, c)P(b,c) is assumed nonempty. The proof starts from "an arbitrary ρ0∈P(b,c)\rho_0 \in \mathcal P(b, c)ρ0​∈P(b,c)", and with an empty prior the supremum is over the empty set and the statement fails.
  • The noise. Gaussian noise with covariance σ2Id\sigma^2\mathrm{Id}σ2Id is σξ\sigma\xiσξ with ξ∼\xi \simξ∼ stdGaussian Y.
  • SdS^dSd. It is read as the surface area of the unit sphere of Rd\mathbb R^dRd.

Two parts of the print are corrected, and both corrections are stated in the items.

  • (68). The printed constant v=u−Bc/(Bc+1)/(2Bc)v = u^{-Bc/(Bc+1)}/(2Bc)v=u−Bc/(Bc+1)/(2Bc) and threshold 2Bc(2Bcu)Bc2Bc(2Bcu)^{Bc}2Bc(2Bcu)Bc come from dropping the factor uuu in an integral, and the printed inequality fails for u<1/2u < 1/2u<1/2. The corrected constant is u1/(Bc+1)/(2Bc)u^{1/(Bc+1)}/(2Bc)u1/(Bc+1)/(2Bc), with threshold (2Bc)Bc+1/u(2Bc)^{Bc+1}/u(2Bc)Bc+1/u.
  • (67). It is stated with the explicit constant C=Φ(−1/σ)C = \Phi(-1/\sigma)C=Φ(−1/σ) that the proof obtains.

The goal mentions none of P′\mathcal P'P′, m(s)m^{(s)}m(s), γn\gamma_nγn​ or Φ\PhiΦ. It is the lower rate (3) for the full prior P(b,c)\mathcal P(b, c)P(b,c) with aℓ=ℓ−cB/(cB+1)a_\ell = \ell^{-cB/(cB+1)}aℓ​=ℓ−cB/(cB+1). A formalization that fixed the algorithm, let the distribution depend on ℓ\ellℓ, or let the constant depend on the algorithm would prove a different, weaker statement.

A complete development needs:

  • Gaussian measures on finite-dimensional inner product spaces, and the distribution function of the standard normal;
  • conditional distributions on Polish products;
  • infinite products of fair coins;
  • series in Hilbert spaces with orthogonal terms.

Reusable pieces include Proposition 7, the Bayes-error monotonicity argument on p. 29, and the identification of the risk minimizer of a Gaussian-noise model. Contributions on any milestone are welcome, as are proofs of the measurability facts (elements of H\mathcal HH are measurable under Hypothesis 1).

Selected references

  • A. Caponnetto and E. De Vito, Optimal rates for the regularized least-squares algorithm, Found. Comput. Math. 7 (2007) 331–368. https://doi.org/10.1007/s10208-006-0196-8
  • L. Györfi, M. Kohler, A. Krzyżak and H. Walk, A Distribution-Free Theory of Nonparametric Regression, Springer Series in Statistics, 2002 (§3, Theorem 3.3; Lemma 3.2).
  • R. DeVore, G. Kerkyacharian, D. Picard and V. Temlyakov, Approximation methods for supervised learning, Found. Comput. Math. 6 (2006) 3–58.
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Machine LearningProbabilityStatistics·Captain: mikedeng1

Optimal Rates for the Regularized Least-Squares Algorithm II: No Learning Algorithm Converges Faster than ℓ^(−bc/(bc+1)) Uniformly over P(b, c) — the Minimax Lower Rate (Theorem 2)Research Paper

Why lower bounds for kernel regression matter

Regularized least squares (RLS), also called kernel ridge regression, is one of the standard estimators of statistical learning: given a sample of input–output pairs, it fits a function from a reproducing kernel Hilbert space by minimizing the empirical squared error plus a multiple of the squared norm. Caponnetto and De Vito (FoCM 2007) proved that, over a class of distributions described by two parameters — the decay of the eigenvalues of the kernel's covariance operator and the smoothness of the regression function relative to it — RLS with a well-chosen regularization parameter converges at the rate ℓ−bc/(bc+1)\ell^{-bc/(bc+1)}ℓ−bc/(bc+1) in the sample size ℓ\ellℓ (their Theorem 1). An upper rate on its own does not say whether another method could do better. This mission formalizes the matching minimax lower rate (their Theorem 2): when the output space is finite dimensional, no learning algorithm whatsoever converges faster than ℓ−bc/(bc+1)\ell^{-bc/(bc+1)}ℓ−bc/(bc+1) uniformly over the class. Together the two theorems say that RLS is rate-optimal, and they are the reference point for later work on spectral regularization, early stopping and distributed kernel methods.

The paper's lower bound adapts the minimax analysis of DeVore, Kerkyacharian, Picard and Temlyakov (FoCM 2006) to the vector-valued RKHS setting.

Setting

Inputs xxx lie in a Polish space XXX and outputs yyy in a real Hilbert space YYY of finite dimension ddd. The hypothesis space H\mathcal HH is a separable Hilbert space of functions f:X→Yf : X \to Yf:X→Y in which evaluation is continuous; Kx:Y→HK_x : Y \to \mathcal HKx​:Y→H is the adjoint of evaluation at xxx, so f(x)=Kx∗ff(x) = K_x^* ff(x)=Kx∗​f. Hypothesis 1 asks that (x,t)↦⟨Ktv,Kxw⟩H(x,t) \mapsto \langle K_t v, K_x w\rangle_{\mathcal H}(x,t)↦⟨Kt​v,Kx​w⟩H​ be measurable and that Tr⁡(Kx∗Kx)≤κ\operatorname{Tr}(K_x^*K_x) \le \kappaTr(Kx∗​Kx​)≤κ for every xxx.

A distribution ρ\rhoρ on Z=X×YZ = X \times YZ=X×Y has risk E[f]=∫∥f(x)−y∥2 dρ\mathcal E[f] = \int \|f(x) - y\|^2\, d\rhoE[f]=∫∥f(x)−y∥2dρ. Hypothesis 2 asks that ∫∥y∥2dρ<∞\int\|y\|^2 d\rho < \infty∫∥y∥2dρ<∞, that the risk has a minimizer fH∈Hf_{\mathcal H} \in \mathcal HfH​∈H (taken of minimal norm), and that the noise y−fH(x)y - f_{\mathcal H}(x)y−fH​(x) satisfies a Bernstein moment condition with constants M,ΣM, \SigmaM,Σ. With ρX\rho_XρX​ the marginal of ρ\rhoρ, the operator T=∫KxKx∗ dρX(x)T = \int K_x K_x^*\, d\rho_X(x)T=∫Kx​Kx∗​dρX​(x) on H\mathcal HH has the quadratic form ⟨Tf,g⟩=∫⟨f(x),g(x)⟩ dρX\langle Tf, g\rangle = \int \langle f(x), g(x)\rangle\, d\rho_X⟨Tf,g⟩=∫⟨f(x),g(x)⟩dρX​ and a spectral decomposition T=∑ntn⟨⋅,en⟩enT = \sum_n t_n \langle\cdot, e_n\rangle e_nT=∑n​tn​⟨⋅,en​⟩en​.

The prior P(b,c)\mathcal P(b,c)P(b,c) (Definition 1, with fixed positive M,Σ,R,α,βM, \Sigma, R, \alpha, \betaM,Σ,R,α,β, 1<b<∞1 < b < \infty1<b<∞ and 1≤c≤21 \le c \le 21≤c≤2) is the set of probability measures ρ\rhoρ satisfying Hypothesis 2 with M,ΣM, \SigmaM,Σ such that

  • TTT has infinitely many positive eigenvalues t1≥t2≥…t_1 \ge t_2 \ge \dotst1​≥t2​≥… with α≤nbtn≤β\alpha \le n^b t_n \le \betaα≤nbtn​≤β (a capacity condition);
  • fH=T(c−1)/2gf_{\mathcal H} = T^{(c-1)/2} gfH​=T(c−1)/2g for some ggg with ∥g∥2≤R\|g\|^2 \le R∥g∥2≤R (a source condition).

Formalization targets

Goal: Theorem 2 (p. 11)

lim⁡τ→0 lim inf⁡ℓ→∞ inf⁡fℓ sup⁡ρ∈P(b,c) Pz∼ρℓ[E[fzℓ]−E[fH]>τ ℓ−bcbc+1]=1,\lim_{\tau \to 0}\ \liminf_{\ell \to \infty}\ \inf_{f_\ell}\ \sup_{\rho \in \mathcal P(b,c)}\ \mathbb P_{\mathbf z \sim \rho^\ell}\Big[\mathcal E[f^\ell_{\mathbf z}] - \mathcal E[f_{\mathcal H}] > \tau\, \ell^{-\frac{bc}{bc+1}}\Big] = 1,τ→0lim​ ℓ→∞liminf​ fℓ​inf​ ρ∈P(b,c)sup​ Pz∼ρℓ​[E[fzℓ​]−E[fH​]>τℓ−bc+1bc​]=1,

the infimum over all learning algorithms fℓ:Zℓ→Hf_\ell : Z^\ell \to \mathcal Hfℓ​:Zℓ→H. The constant in front of the rate is left free, so the goal asserts only the exponent.

Milestones

  1. Proposition 4 (p. 21): for f=T(c−1)/2gf = T^{(c-1)/2}gf=T(c−1)/2g, ∥g∥2≤R\|g\|^2 \le R∥g∥2≤R, the explicit distribution ρf\rho_fρf​ with marginal ν\nuν (the marginal of some ρ0∈P(b,c)\rho_0 \in \mathcal P(b,c)ρ0​∈P(b,c)) and 2d2d2d-point conditional law is a probability measure with regression function fff, and lies in P(b,c)\mathcal P(b,c)P(b,c) when min⁡(M,Σ)≥2(4d+1)κcR\min(M,\Sigma) \ge 2(4d+1)\sqrt{\kappa^c R}min(M,Σ)≥2(4d+1)κcR​.
  2. Proposition 4, (54): K(ρf,ρf′)≤1615dL2∥T(f−f′)∥2\mathcal K(\rho_f, \rho_{f'}) \le \frac{16}{15 d L^2}\|\sqrt T(f - f')\|^2K(ρf​,ρf′​)≤15dL216​∥T​(f−f′)∥2 with L=4κcRL = 4\sqrt{\kappa^c R}L=4κcR​.
  3. Proposition 6 (p. 24): for m>16m > 16m>16 there are N≥em/24N \ge e^{m/24}N≥em/24 sign vectors in {−1,+1}m\{-1,+1\}^m{−1,+1}m with pairwise ∑n(σin−σjn)2≥m\sum_n(\sigma_i^n - \sigma_j^n)^2 \ge m∑n​(σin​−σjn​)2≥m.
  4. Proposition 5 (pp. 22–23): for small ϵ\epsilonϵ there are Nϵ≥eγϵ−1/(bc)N_\epsilon \ge e^{\gamma\epsilon^{-1/(bc)}}Nϵ​≥eγϵ−1/(bc) functions in the source class with ϵ≤∥T(fi−fj)∥2≤4ϵ\epsilon \le \|\sqrt T(f_i - f_j)\|^2 \le 4\epsilonϵ≤∥T​(fi​−fj​)∥2≤4ϵ.
  5. Theorem 5 (p. 24): for every algorithm some ρ∗∈P(b,c)\rho_* \in \mathcal P(b,c)ρ∗​∈P(b,c) has P[excess risk>ϵ/4]≥min⁡{N∗/(N∗+1), e−3/eN∗ e−4ℓϵ/(15dκcR)}\mathbb P[\text{excess risk} > \epsilon/4] \ge \min\{N^*/(N^*+1),\ e^{-3/e}\sqrt{N^*}\, e^{-4\ell\epsilon/(15 d\kappa^c R)}\}P[excess risk>ϵ/4]≥min{N∗/(N∗+1), e−3/eN∗​e−4ℓϵ/(15dκcR)}, N∗=eγϵ−1/(bc)N^* = e^{\gamma\epsilon^{-1/(bc)}}N∗=eγϵ−1/(bc).

Significance

The result. Theorem 2 shows that the exponent bc/(bc+1)bc/(bc+1)bc/(bc+1) attained by RLS cannot be improved by any estimator over P(b,c)\mathcal P(b,c)P(b,c) when dim⁡Y<∞\dim Y < \inftydimY<∞; for c=1c = 1c=1 RLS is optimal up to a logarithmic factor. It separates what is a property of the problem class from what is a property of the algorithm: improvements to kernel methods must change the class (stronger assumptions) rather than the rate. The construction — a packing of the source class measured in the T\sqrt TT​-norm, combined with a KL bound for an explicit noise model — is the template reused in many later lower bounds for kernel and inverse-problem estimators.

Formalizing it. The result has been proved since 2007; no machine-checked version exists. A formal proof needs the information-theoretic lower-bound machinery (a Fano-type inequality for many hypotheses), a Varshamov–Gilbert-type packing of the Hamming cube, KL divergence between explicit mixtures, and the spectral description of the covariance operator of a vector-valued RKHS. Each of these is reusable well beyond this paper. The mission also makes precise the paper's implicit conventions (see below), which a pen-and-paper reader fills in silently.

Difficulty

The upper half of the argument is not the hard part; the hard part is that the lower bound is uniform over all measurable algorithms, which no direct computation reaches. The step that does not follow from the paper alone is Theorem 5: its proof invokes Lemma 3.3 and Eq. 3.12 of DeVore et al., a Fano-type inequality bounding the probability of correct identification among NNN hypotheses with pairwise KL divergence at most a given level. That lemma is not stated in the paper and is not in Mathlib; it must be formalized. A second obstacle is the packing (Proposition 6), whose proof is a probabilistic union bound with Hoeffding's inequality. A naive attempt to prove Theorem 2 by exhibiting a single bad distribution fails: for any fixed ρ\rhoρ some algorithm (the constant one returning fρf_{\rho}fρ​) has zero excess risk, so the bad distribution must depend on the algorithm, and the order of quantifiers is essential.

Formalization scope

Mathlib's RKHS ℝ H X Y provides the function space with continuous evaluation, RKHS.kerFun is KxK_xKx​, and InformationTheory.klDiv is the Kullback–Leibler information. The operator TTT is never built as an operator-valued Bochner integral: it is recorded through its quadratic form ∫⟨f(x),g(x)⟩dρX\int\langle f(x), g(x)\rangle d\rho_X∫⟨f(x),g(x)⟩dρX​ and an eigen-system indexed by N\mathbb NN from 000 (the paper's tnt_ntn​ is t (n-1)). The trace in Hypothesis 1 is a series over a Hilbert basis of YYY; the conditional law in Hypothesis 2 is Measure.condKernel, and the moment integral there is a lintegral. E[fH]\mathcal E[f_{\mathcal H}]E[fH​] in the goal is inf⁡f∈HE[f]\inf_{f \in \mathcal H}\mathcal E[f]inff∈H​E[f].

Conventions and added hypotheses, each implicit on the page:

  • P(b,c)\mathcal P(b,c)P(b,c) is assumed nonempty; the proof fixes ρ0∈P(b,c)\rho_0 \in \mathcal P(b,c)ρ0​∈P(b,c), and over an empty prior the supremum is over the empty set and the statement is false.
  • Algorithms are measurable maps Zℓ→HZ^\ell \to \mathcal HZℓ→H; this is the reading under which the probability in the goal is defined, and it restricts the infimum relative to "all mappings".
  • The constants M,Σ,R,α,β,κM, \Sigma, R, \alpha, \beta, \kappaM,Σ,R,α,β,κ are positive; the basis (vj)(v_j)(vj​) of YYY in Proposition 4 is orthonormal.
  • Proposition 4's "∥g∥2≤R\|g\|^2 \le R∥g∥2≤R" for f′f'f′ is read as ∥g′∥2≤R\|g'\|^2 \le R∥g′∥2≤R; Proposition 6's "i≠,ji \ne, ji=,j" as i≠ji \ne ji=j; (56) is required for i≠ji \ne ji=j. The proof's variance display on p. 22 is wrong for d≥2d \ge 2d≥2, but the conclusion of Proposition 4 holds.

The goal is the ε\varepsilonε–τ\tauτ–LLL unfolding of the limit and mentions neither ρf\rho_fρf​, the KL bound nor the packing, so it cannot be discharged by any of the milestones' constructions in isolation; the distribution ρ\rhoρ is chosen after the algorithm, never before it.

Contributions welcome: a general Fano/DeVore-type lemma for finitely many hypotheses, the Varshamov–Gilbert bound, KL ≤ χ² for finite mixtures, and lemmas relating covForm to the excess risk.

Selected references

  • A. Caponnetto, E. De Vito, Optimal rates for the regularized least-squares algorithm, Found. Comput. Math. 7 (2007) 331–368. https://doi.org/10.1007/s10208-006-0196-8
  • R. DeVore, G. Kerkyacharian, D. Picard, V. Temlyakov, Approximation methods for supervised learning, Found. Comput. Math. 6 (2006) 3–58. https://doi.org/10.1007/s10208-004-0158-6
  • L. Györfi, M. Kohler, A. Krzyżak, H. Walk, A Distribution-Free Theory of Nonparametric Regression, Springer, 2002. https://doi.org/10.1007/b97848
  • A. B. Tsybakov, Introduction to Nonparametric Estimation, Springer, 2009. https://doi.org/10.1007/b13794
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Optimal Rates for the Regularized Least-Squares Algorithm I: With λ Tuned to the Effective Dimension, Regularized Least Squares Attains the Rate ℓ^(−bc/(bc+1)) Uniformly over P(b, c) (Theorem 1)Research Paper

Motivation

Regularized least squares (RLS, also called kernel ridge regression or Tikhonov regularization) is the simplest learning algorithm built on a reproducing kernel Hilbert space. Given ℓ\ellℓ examples (xi,yi)(x_i,y_i)(xi​,yi​) drawn independently from an unknown distribution ρ\rhoρ, it returns the function in a hypothesis space H\mathcal HH that minimizes the empirical squared error plus λ\lambdaλ times the squared norm. It is used in regression, in multi-task learning with vector-valued outputs, and as the reference case for spectral regularization methods.

The basic statistical question is how fast the excess risk of the RLS estimator goes to zero as ℓ\ellℓ grows, and how to choose λ=λℓ\lambda=\lambda_\ellλ=λℓ​ to get that speed. Caponnetto and De Vito (FoCM 2007) answered it for a family of priors P(b,c)\mathcal P(b,c)P(b,c) described by two numbers: the decay rate bbb of the eigenvalues of the covariance operator of the input distribution and the regularity ccc of the target function. Their Theorem 1 gives the upper rate ℓ−bc/(bc+1)\ell^{-bc/(bc+1)}ℓ−bc/(bc+1); Theorems 2 and 3 show that no algorithm does better when the output space is finite dimensional. This mission formalizes the upper rate.

Timeline. Cucker and Smale (2002) and De Vito, Caponnetto and Rosasco (2005) gave rates for RLS that did not depend on the eigenvalue decay of ρX\rho_XρX​. Zhang (2005) introduced the effective dimension N(λ)\mathcal N(\lambda)N(λ) as the complexity measure. Caponnetto and De Vito (authors' copy dated 2006, published 2007) combined it with a source condition to obtain rates that are optimal over P(b,c)\mathcal P(b,c)P(b,c), for vector-valued outputs. Steinwart, Hush and Scovel (2009) and Fischer and Steinwart (2020) later extended the analysis to other norms and to c<1c<1c<1.

Setting

The input space XXX is a Polish space and the output space YYY is a real separable Hilbert space. The hypothesis space H\mathcal HH is a real separable Hilbert space of functions f:X→Yf:X\to Yf:X→Y in which evaluation at each point is continuous. For x∈Xx\in Xx∈X, Kx:Y→HK_x:Y\to\mathcal HKx​:Y→H is the adjoint of evaluation at xxx, so f(x)=Kx∗ff(x)=K_x^*ff(x)=Kx∗​f. Hypothesis 1 adds a measurability condition and a uniform trace bound Tr⁡(Kx∗Kx)≤κ\operatorname{Tr}(K_x^*K_x)\le\kappaTr(Kx∗​Kx​)≤κ.

A distribution ρ\rhoρ on Z=X×YZ=X\times YZ=X×Y has marginal ρX\rho_XρX​ and conditional laws ρ(⋅∣x)\rho(\cdot\mid x)ρ(⋅∣x). The expected risk of f∈Hf\in\mathcal Hf∈H is E[f]=∫∥f(x)−y∥Y2 dρ\mathcal E[f]=\int\|f(x)-y\|_Y^2\,d\rhoE[f]=∫∥f(x)−y∥Y2​dρ. Hypothesis 2 asks that E∥y∥2<∞\mathbb E\|y\|^2<\inftyE∥y∥2<∞, that E\mathcal EE attains its infimum over H\mathcal HH at some fHf_{\mathcal H}fH​ (the minimizer of minimal norm is used), and that the noise y−fH(x)y-f_{\mathcal H}(x)y−fH​(x) satisfies a Bernstein moment condition with constants M,ΣM,\SigmaM,Σ.

The covariance operator T=∫XKxKx∗ dρXT=\int_XK_xK_x^*\,d\rho_XT=∫X​Kx​Kx∗​dρX​ is positive and trace class, with ⟨Tf,f⟩H=∫X∥f(x)∥Y2 dρX\langle Tf,f\rangle_{\mathcal H}=\int_X\|f(x)\|_Y^2\,d\rho_X⟨Tf,f⟩H​=∫X​∥f(x)∥Y2​dρX​ and eigen-decomposition T=∑ntn⟨⋅,en⟩enT=\sum_nt_n\langle\cdot,e_n\rangle e_nT=∑n​tn​⟨⋅,en​⟩en​, t1≥t2≥⋯>0t_1\ge t_2\ge\dots>0t1​≥t2​≥⋯>0. The prior P(b,c)\mathcal P(b,c)P(b,c), for 1<b<∞1<b<\infty1<b<∞ and 1≤c≤21\le c\le21≤c≤2, consists of the ρ\rhoρ satisfying Hypothesis 2, with fH=T(c−1)/2gf_{\mathcal H}=T^{(c-1)/2}gfH​=T(c−1)/2g for some ∥g∥2≤R\|g\|^2\le R∥g∥2≤R (source condition), and with α≤nbtn≤β\alpha\le n^bt_n\le\betaα≤nbtn​≤β for all nnn (eigenvalue decay).

The RLS estimator fzλf_{\mathbf z}^\lambdafzλ​ minimizes 1ℓ∑i∥f(xi)−yi∥Y2+λ∥f∥H2\frac1\ell\sum_i\|f(x_i)-y_i\|_Y^2+\lambda\|f\|_{\mathcal H}^2ℓ1​∑i​∥f(xi​)−yi​∥Y2​+λ∥f∥H2​ over H\mathcal HH.

Formalization targets

Goal: Theorem 1, 1<b<+∞1<b<+\infty1<b<+∞

With λℓ=ℓ−b/(bc+1)\lambda_\ell=\ell^{-b/(bc+1)}λℓ​=ℓ−b/(bc+1) and aℓ=ℓ−bc/(bc+1)a_\ell=\ell^{-bc/(bc+1)}aℓ​=ℓ−bc/(bc+1) for c>1c>1c>1, and λℓ=aℓ=(log⁡ℓ/ℓ)b/(b+1)\lambda_\ell=a_\ell=(\log\ell/\ell)^{b/(b+1)}λℓ​=aℓ​=(logℓ/ℓ)b/(b+1) for c=1c=1c=1,

lim⁡τ→∞lim sup⁡ℓ→∞sup⁡ρ∈P(b,c)Pz∼ρℓ[E[fzλℓ]−E[fH]>τaℓ]=0.\lim_{\tau\to\infty}\limsup_{\ell\to\infty}\sup_{\rho\in\mathcal P(b,c)}\mathbb P_{\mathbf z\sim\rho^\ell}\Big[\mathcal E[f_{\mathbf z}^{\lambda_\ell}]-\mathcal E[f_{\mathcal H}]>\tau a_\ell\Big]=0.τ→∞lim​ℓ→∞limsup​ρ∈P(b,c)sup​Pz∼ρℓ​[E[fzλℓ​​]−E[fH​]>τaℓ​]=0.

The statement fixes the rate, not the constants: the threshold τ\tauτ absorbs every constant of the prior.

Milestones

  1. Proposition 1 iii)–v): the excess risk is ∥T(f−fH)∥2\|\sqrt T(f-f_{\mathcal H})\|^2∥T​(f−fH​)∥2; the regularized expected and empirical risks have unique minimizers fλ=(T+λ)−1TfHf^\lambda=(T+\lambda)^{-1}Tf_{\mathcal H}fλ=(T+λ)−1TfH​ and fzλ=(Tx+λ)−1gzf_{\mathbf z}^\lambda=(T_{\mathbf x}+\lambda)^{-1}g_{\mathbf z}fzλ​=(Tx​+λ)−1gz​.
  2. Proposition 2: a Bernstein inequality for means of i.i.d. Hilbert-space-valued variables.
  3. Theorem 4: with probability ≥1−η\ge1-\eta≥1−η,
E[fzλ]−E[fH]≤3Cη(A(λ)+κ2B(λ)ℓ2λ+κA(λ)ℓλ+κM2ℓ2λ+Σ2N(λ)ℓ),\mathcal E[f_{\mathbf z}^\lambda]-\mathcal E[f_{\mathcal H}]\le3C_\eta\Big(\mathcal A(\lambda)+\frac{\kappa^2\mathcal B(\lambda)}{\ell^2\lambda}+\frac{\kappa\mathcal A(\lambda)}{\ell\lambda}+\frac{\kappa M^2}{\ell^2\lambda}+\frac{\Sigma^2\mathcal N(\lambda)}{\ell}\Big),E[fzλ​]−E[fH​]≤3Cη​(A(λ)+ℓ2λκ2B(λ)​+ℓλκA(λ)​+ℓ2λκM2​+ℓΣ2N(λ)​),

provided ℓ≥2CηκN(λ)/λ\ell\ge2C_\eta\kappa\mathcal N(\lambda)/\lambdaℓ≥2Cη​κN(λ)/λ and λ≤∥T∥\lambda\le\|T\|λ≤∥T∥, where Cη=32log⁡2(6/η)C_\eta=32\log^2(6/\eta)Cη​=32log2(6/η), A(λ)=E[fλ]−E[fH]\mathcal A(\lambda)=\mathcal E[f^\lambda]-\mathcal E[f_{\mathcal H}]A(λ)=E[fλ]−E[fH​], B(λ)=∥fλ−fH∥2\mathcal B(\lambda)=\|f^\lambda-f_{\mathcal H}\|^2B(λ)=∥fλ−fH​∥2 and N(λ)=Tr⁡[(T+λ)−1T]\mathcal N(\lambda)=\operatorname{Tr}[(T+\lambda)^{-1}T]N(λ)=Tr[(T+λ)−1T]. 4. Proposition 3: on P(b,c)\mathcal P(b,c)P(b,c), A(λ)≤λc∥T(1−c)/2fH∥2\mathcal A(\lambda)\le\lambda^c\|T^{(1-c)/2}f_{\mathcal H}\|^2A(λ)≤λc∥T(1−c)/2fH​∥2, B(λ)≤λc−1∥T(1−c)/2fH∥2\mathcal B(\lambda)\le\lambda^{c-1}\|T^{(1-c)/2}f_{\mathcal H}\|^2B(λ)≤λc−1∥T(1−c)/2fH​∥2 and N(λ)≤bb−1β1/bλ−1/b\mathcal N(\lambda)\le\frac b{b-1}\beta^{1/b}\lambda^{-1/b}N(λ)≤b−1b​β1/bλ−1/b.

Significance

The result. Theorem 1 says that RLS with λℓ\lambda_\ellλℓ​ chosen from (b,c)(b,c)(b,c) achieves the rate ℓ−bc/(bc+1)\ell^{-bc/(bc+1)}ℓ−bc/(bc+1) uniformly over the prior, and the companion lower bounds show this is the minimax rate for 1<c≤21<c\le21<c≤2 and finite-dimensional YYY. The rate interpolates between the parametric rate 1/ℓ1/\ell1/ℓ (fast eigenvalue decay, smooth target) and slower nonparametric rates, and it identifies the effective dimension, rather than the dimension of H\mathcal HH, as the quantity that governs complexity. Theorem 4 is a non-asymptotic bound of independent use; it is the template for later analyses of spectral regularization, gradient descent with early stopping, and random-feature approximations of kernel methods.

The formalization. The result is proved on paper; no machine-checked proof of a kernel ridge regression rate is known to exist. A formal development requires a Bernstein inequality in Hilbert spaces, spectral calculus for a trace-class operator defined from a measure, and the operator-perturbation argument of Theorem 4. Two printed constants are corrected here: Theorem 4's proof yields 3Cη3C_\eta3Cη​, not CηC_\etaCη​, and Proposition 3's bound on N(λ)\mathcal N(\lambda)N(λ) has β1/b\beta^{1/b}β1/b in place of β\betaβ. The paper also states Theorem 1 for b=+∞b=+\inftyb=+∞; that branch fails for 1≤c<21\le c<21≤c<2 and is not posed.

Difficulty

The obvious argument bounds ∥fzλ−fλ∥H\|f_{\mathbf z}^\lambda-f^\lambda\|_{\mathcal H}∥fzλ​−fλ∥H​ by uniform concentration of TxT_{\mathbf x}Tx​ around TTT and multiplies by ∥T∥\|\sqrt T\|∥T​∥. That gives a variance term that ignores the eigenvalue decay of TTT, and hence a rate that does not improve with bbb. The optimal rate needs the variance measured through N(λ)\mathcal N(\lambda)N(λ), which requires controlling T(Tx+λ)−1\sqrt T(T_{\mathbf x}+\lambda)^{-1}T​(Tx​+λ)−1 in operator norm with high probability. This in turn needs concentration of (T+λ)−1/2(T−Tx)(T+\lambda)^{-1/2}(T-T_{\mathbf x})(T+λ)−1/2(T−Tx​) in Hilbert–Schmidt norm, and the condition ℓ≳N(λ)/λ\ell\gtrsim\mathcal N(\lambda)/\lambdaℓ≳N(λ)/λ under which the empirical operator is close enough to TTT. The noise is unbounded, so only the moment condition (9) is available, and the concentration step must use moment bounds rather than boundedness.

Formalization scope

H\mathcal HH is Mathlib's RKHS ℝ H X Y, and KxK_xKx​ is RKHS.kerFun H x. The trace in Hypothesis 1 is computed in a fixed Hilbert basis of YYY. ρX\rho_XρX​ is the first marginal and ρ(⋅∣x)\rho(\cdot\mid x)ρ(⋅∣x) is condKernel. The operator TTT is not built as an operator-valued integral. It enters through its quadratic form ∫⟨f(x),g(x)⟩ dρX\int\langle f(x),g(x)\rangle\,d\rho_X∫⟨f(x),g(x)⟩dρX​ and through an eigen-system (en,tn)(e_n,t_n)(en​,tn​), indexed from 000, so (17) reads α≤(n+1)btn≤β\alpha\le(n+1)^bt_n\le\betaα≤(n+1)btn​≤β. The effective dimension is ∑ntn/(tn+λ)\sum_nt_n/(t_n+\lambda)∑n​tn​/(tn​+λ). Samples are Fin ℓ → X × Y under the product measure, and probabilities of events are outer measures. "With probability at least 1−η1-\eta1−η" is stated as "the bad event has measure at most η\etaη". The noise condition and the moments of Proposition 2 are integrals of nonnegative functions with values in [0,∞][0,\infty][0,∞].

The hypotheses the paper uses but does not display are added: positivity of M,Σ,R,α,β,κM,\Sigma,R,\alpha,\beta,\kappaM,Σ,R,α,β,κ, and integrability of the random variable in Proposition 2. The RLS estimator of the goal is any family of minimizers of (18) for ℓ≥2\ell\ge2ℓ≥2; at ℓ=1\ell=1ℓ=1 and c=1c=1c=1 the parameter λ1=0\lambda_1=0λ1​=0 is degenerate. The goal quantifies uniformly: LLL is chosen before ρ\rhoρ, and the estimator is fixed before ρ\rhoρ. The goal must not be replaced by a statement about A,B,N\mathcal A,\mathcal B,\mathcal NA,B,N or by Theorem 4's event: it is the uniform rate for the estimator itself.

Reusable infrastructure: Hilbert-space Bernstein inequalities (Proposition 2 alone is a valuable target), spectral calculus for compact positive operators given by a quadratic form, and the representer/normal equation for vector-valued RLS. Contributions of proofs for any milestone, and of supporting lemmas about trace-class operators and effective dimension, are welcome.

Selected references

  • A. Caponnetto, E. De Vito, Optimal rates for the regularized least-squares algorithm, Found. Comput. Math. 7 (2007) 331–368. https://doi.org/10.1007/s10208-006-0196-8
  • F. Cucker, S. Smale, On the mathematical foundations of learning, Bull. Amer. Math. Soc. 39 (2002) 1–49. https://doi.org/10.1090/S0273-0979-01-00923-5
  • E. De Vito, A. Caponnetto, L. Rosasco, Model selection for regularized least-squares algorithm in learning theory, Found. Comput. Math. 5 (2005) 59–85. https://doi.org/10.1007/s10208-004-0134-1
  • T. Zhang, Learning bounds for kernel regression using effective data dimensionality, Neural Comput. 17 (2005) 2077–2098. https://doi.org/10.1162/0899766054323008
  • I. Pinelis, Optimum bounds for the distributions of martingales in Banach spaces, Ann. Probab. 22 (1994) 1679–1706. https://doi.org/10.1214/aop/1176988477
  • I. Steinwart, D. Hush, C. Scovel, Optimal rates for regularized least squares regression, COLT 2009. https://www.cs.mcgill.ca/~colt2009/papers/038.pdf
  • S. Fischer, I. Steinwart, Sobolev norm learning rates for regularized least-squares algorithms, J. Mach. Learn. Res. 21 (2020) 1–38. https://jmlr.org/papers/v21/19-734.html
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Machine LearningOptimal TransportProbability+1·Captain: mikedeng1

Robust Wasserstein Profile Inference and Applications to Machine Learning 3: The Scaled Robust Wasserstein Profile n^(ρ/2)·R_n(θ*) Is Asymptotically Stochastically Bounded by R̄(ρ)Research Paper

Motivation

Many statistical parameters are defined implicitly, as the root θ∗\theta_*θ∗​ of an estimating equation E[h(W,θ∗)]=0\mathbb E[h(W, \theta_*)] = \mathbf 0E[h(W,θ∗​)]=0: a mean, a quantile, a regression coefficient, the minimizer of an expected loss. Owen's empirical likelihood builds confidence regions for such parameters by asking how far the empirical distribution of the data must be reweighted before the equation holds, and the profile of that distance has a chi-squared limit (Owen, Empirical Likelihood, 2001).

Blanchet, Kang and Murthy replace reweighting by transport: they measure how much the data must be moved, in the sense of optimal transport, before the equation holds. The resulting Robust Wasserstein Profile (RWP) function plays the role of the empirical-likelihood profile, and its value at the true parameter is exactly the smallest radius of a Wasserstein ball around the data that contains a distribution satisfying the estimating equation. Its asymptotic law is therefore what is needed to choose the radius of Wasserstein distributionally robust estimators, such as the square-root LASSO and regularized logistic regression, in a data-driven way (arXiv:1610.05627, §§1, 3, 4). This mission formalizes the paper's main limit theorem, Theorem 3.

Setting

Let c:Rm×Rm→[0,∞]c : \mathbb R^m \times \mathbb R^m \to [0, \infty]c:Rm×Rm→[0,∞] be a cost. The optimal transport cost between probability laws PPP and QQQ on Rm\mathbb R^mRm is

Dc(P,Q)=inf⁡{Eπ[c(U,W)]:πU=P, πW=Q},D_c(P, Q) = \inf\{ \mathbb E_\pi[c(U, W)] : \pi_U = P,\ \pi_W = Q \},Dc​(P,Q)=inf{Eπ​[c(U,W)]:πU​=P, πW​=Q},

the infimum over all joint laws π\piπ of a pair (U,W)(U, W)(U,W) with the given marginals (Eq. (7)). In this mission c(u,w)=∥w−u∥qρc(u, w) = \|w - u\|_q^\rhoc(u,w)=∥w−u∥qρ​ with ρ≥1\rho \ge 1ρ≥1 and q∈(1,∞]q \in (1, \infty]q∈(1,∞], and ppp denotes the conjugate exponent, 1/p+1/q=11/p + 1/q = 11/p+1/q=1.

Let h:Rm×Rl→Rrh : \mathbb R^m \times \mathbb R^l \to \mathbb R^rh:Rm×Rl→Rr be an estimating function, and let W,W1,W2,…W, W_1, W_2, \dotsW,W1​,W2​,… be i.i.d. random vectors in Rm\mathbb R^mRm with E[h(W,θ∗)]=0\mathbb E[h(W, \theta_*)] = \mathbf 0E[h(W,θ∗​)]=0. With Pn\mathbb P_nPn​ the empirical distribution of W1,…,WnW_1, \dots, W_nW1​,…,Wn​, the RWP function is

Rn(θ)=inf⁡{Dc(P,Pn):EP[h(W,θ)]=0}.(16)R_n(\theta) = \inf\{ D_c(P, \mathbb P_n) : \mathbb E_P[h(W, \theta)] = \mathbf 0 \}. \qquad (16)Rn​(θ)=inf{Dc​(P,Pn​):EP​[h(W,θ)]=0}.(16)

Write Dwh(w,θ∗)D_w h(w, \theta_*)Dw​h(w,θ∗​) for the r×mr \times mr×m Jacobian of w↦h(w,θ∗)w \mapsto h(w, \theta_*)w↦h(w,θ∗​), and ∥ζTDwh(w,θ∗)∥p\|\zeta^T D_w h(w, \theta_*)\|_p∥ζTDw​h(w,θ∗​)∥p​ for the ℓp\ell_pℓp​ norm of the row vector ζTDwh(w,θ∗)∈Rm\zeta^T D_w h(w, \theta_*) \in \mathbb R^mζTDw​h(w,θ∗​)∈Rm, ζ∈Rr\zeta \in \mathbb R^rζ∈Rr. The assumptions are:

  • A1) c(u,w)=∥u−w∥qρc(u, w) = \|u - w\|_q^\rhoc(u,w)=∥u−w∥qρ​, ρ≥1\rho \ge 1ρ≥1;
  • A2) E[h(W,θ∗)]=0\mathbb E[h(W, \theta_*)] = \mathbf 0E[h(W,θ∗​)]=0 and E∥h(W,θ∗)∥22<∞\mathbb E\|h(W, \theta_*)\|_2^2 < \inftyE∥h(W,θ∗​)∥22​<∞;
  • A3) h(⋅,θ∗)h(\cdot, \theta_*)h(⋅,θ∗​) is continuously differentiable;
  • A4) for every ζ≠0\zeta \ne 0ζ=0, P(∥ζTDwh(W,θ∗)∥p>0)>0\mathbb P(\|\zeta^T D_w h(W, \theta_*)\|_p > 0) > 0P(∥ζTDw​h(W,θ∗​)∥p​>0)>0.

A sequence XnX_nXn​ is asymptotically stochastically bounded by XXX, written Xn≲DXX_n \lesssim_D XXn​≲D​X, if lim sup⁡nE[f(Xn)]≤E[f(X)]\limsup_n \mathbb E[f(X_n)] \le \mathbb E[f(X)]limsupn​E[f(Xn​)]≤E[f(X)] for every continuous, bounded, non-decreasing fff.

Formalization targets

Goal: Theorem 3 (p. 15)

Let H∼N(0,E[h(W,θ∗)h(W,θ∗)T])H \sim \mathcal N(\mathbf 0, \mathbb E[h(W, \theta_*) h(W, \theta_*)^T])H∼N(0,E[h(W,θ∗​)h(W,θ∗​)T]). Under A1)–A4),

nρ/2Rn(θ∗;ρ)≲DRˉ(ρ),n^{\rho/2} R_n(\theta_*; \rho) \lesssim_D \bar R(\rho),nρ/2Rn​(θ∗​;ρ)≲D​Rˉ(ρ),

where for ρ>1\rho > 1ρ>1

Rˉ(ρ)=max⁡ζ∈Rr{ρζTH−(ρ−1) E∥ζTDwh(W,θ∗)∥pρ/(ρ−1)},\bar R(\rho) = \max_{\zeta \in \mathbb R^r} \Big\{ \rho \zeta^T H - (\rho - 1)\, \mathbb E\|\zeta^T D_w h(W, \theta_*)\|_p^{\rho/(\rho - 1)} \Big\},Rˉ(ρ)=ζ∈Rrmax​{ρζTH−(ρ−1)E∥ζTDw​h(W,θ∗​)∥pρ/(ρ−1)​},

and for ρ=1\rho = 1ρ=1

Rˉ(1)=max⁡ζ: P(∥ζTDwh(W,θ∗)∥p>1)=0ζTH.\bar R(1) = \max_{\zeta :\ \mathbb P(\|\zeta^T D_w h(W, \theta_*)\|_p > 1) = 0} \zeta^T H.Rˉ(1)=ζ: P(∥ζTDw​h(W,θ∗​)∥p​>1)=0max​ζTH.

The formal goal also asserts that Rn(θ∗)R_n(\theta_*)Rn​(θ∗​) is finite and measurable and that both maxima are attained; these are facts the paper's statement presupposes.

Milestones (proof of Theorem 3, App. A.3)

  1. Proposition 3 (p. 13): strong duality, Rn(θ)=sup⁡λ{−1n∑isup⁡u{λTh(u,θ)−c(u,Wi)}}R_n(\theta) = \sup_\lambda \{ -\frac1n \sum_i \sup_u \{\lambda^T h(u, \theta) - c(u, W_i)\} \}Rn​(θ)=supλ​{−n1​∑i​supu​{λTh(u,θ)−c(u,Wi​)}} when 0∈int⁡conv⁡h(Rm,θ)\mathbf 0 \in \operatorname{int} \operatorname{conv} h(\mathbb R^m, \theta)0∈intconvh(Rm,θ).
  2. (31)–(32) (p. 32): nρ/2Rn(θ∗)=sup⁡ζ{−ζTHn−Mn(ζ)}n^{\rho/2} R_n(\theta_*) = \sup_\zeta \{ -\zeta^T H_n - M_n(\zeta) \}nρ/2Rn​(θ∗​)=supζ​{−ζTHn​−Mn​(ζ)}, with Hn=n−1/2∑ih(Wi,θ∗)H_n = n^{-1/2} \sum_i h(W_i, \theta_*)Hn​=n−1/2∑i​h(Wi​,θ∗​) and the random penalty MnM_nMn​.
  3. Lemma 2 (p. 32): the supremum in (31) localizes to a compact set of ζ\zetaζ with high probability.
  4. (42) (p. 36): max⁡Δ{vTΔ−∥Δ∥qρ}=∥v∥pρ/(ρ−1)(1/ρ)1/(ρ−1)(1−1/ρ)\max_\Delta \{ v^T \Delta - \|\Delta\|_q^\rho \} = \|v\|_p^{\rho/(\rho-1)} (1/\rho)^{1/(\rho-1)} (1 - 1/\rho)maxΔ​{vTΔ−∥Δ∥qρ​}=∥v∥pρ/(ρ−1)​(1/ρ)1/(ρ−1)(1−1/ρ).
  5. Lemma 3 (p. 34): a uniform law of large numbers for the localized penalty.

Significance

Theorem 3 gives the rate n−ρ/2n^{-\rho/2}n−ρ/2 at which the RWP function at the true parameter vanishes and an explicit random variable bounding its rescaled limit. The (1−α)(1-\alpha)(1−α)-quantile ηα\eta_\alphaηα​ of Rˉ(ρ)\bar R(\rho)Rˉ(ρ) yields a radius δ=n−ρ/2ηα\delta = n^{-\rho/2}\eta_\alphaδ=n−ρ/2ηα​ for which the Wasserstein ball around Pn\mathbb P_nPn​ contains, with asymptotic probability at least 1−α1 - \alpha1−α, a law satisfying the estimating equation at θ∗\theta_*θ∗​ (§3.1, (19)); this is the paper's prescription for the regularization parameter of square-root LASSO and of regularized logistic regression (§4). Example 3 (p. 14) shows the bound is sharp for the mean: nρ/2Rn(θ∗)⇒σWρ∣N(0,1)∣ρn^{\rho/2} R_n(\theta_*) \Rightarrow \sigma_W^\rho |N(0, 1)|^\rhonρ/2Rn​(θ∗​)⇒σWρ​∣N(0,1)∣ρ. Matching lower bounds (Propositions 4 and 5) need further assumptions and are not part of this mission.

The result is proved in the paper; no machine-checked version of it, or of any RWP or empirical-likelihood limit theorem, is known to exist. A formalization would check the duality argument for the problem of moments, the passage from the dual representation to a localized maximization, and the continuous-mapping step, and would produce reusable statements: strong duality for transport-cost moment problems, the closed form of the conjugate of ∥⋅∥qρ\|\cdot\|_q^\rho∥⋅∥qρ​, and a uniform law of large numbers over a compact parameter set.

Difficulty

The obvious route is to apply the central limit theorem to HnH_nHn​ and pass to the limit inside the dual representation (31). This fails as stated, for two reasons. First, the supremum in (31) is over all of Rr\mathbb R^rRr, and convergence of the objective on compact sets does not control the supremum; Lemma 2 is needed, and it uses A4) through a lower bound on E∥ζˉTDh(W)∥pp\mathbb E\|\bar\zeta^T Dh(W)\|_p^pE∥ζˉ​TDh(W)∥pp​ that is uniform over the unit sphere. Second, the penalty MnM_nMn​ involves the derivative of hhh at points Wi+n−1/2ΔuW_i + n^{-1/2}\Delta uWi​+n−1/2Δu that are not localized, with no moment assumption on DhDhDh; the proof must truncate to ∥Wi∥p≤c0\|W_i\|_p \le c_0∥Wi​∥p​≤c0​ and to a specific near-optimal Δ\DeltaΔ, and then remove the truncation. The case ρ=1\rho = 1ρ=1 differs: the inner supremum is 000 or +∞+\infty+∞, and the limit becomes a maximization over a constraint set.

Formalization scope

Vectors are Fin k → ℝ; ℓq\ell_qℓq​ and ℓp\ell_pℓp​ norms are Mathlib's PiLp norms, so q=∞q = \inftyq=∞ is allowed, with q∈(1,∞]q \in (1, \infty]q∈(1,∞] and p.HolderConjugate q. The samples are a sequence W : ℕ → Ω → (Fin m → ℝ), mutually independent (iIndepFun) and identically distributed with W 0, which plays the role of WWW; RnR_nRn​ uses W0,…,Wn−1W_0, \dots, W_{n-1}W0​,…,Wn−1​ through the published empiricalDistribution. Distinct samples are not assumed in Theorem 3; Proposition 3 and (31) keep the §3.1 assumption of distinct samples. Transport costs and RnR_nRn​ are [0,∞][0, \infty][0,∞]-valued lower Lebesgue integrals and infima; Rˉ(ρ)\bar R(\rho)Rˉ(ρ) is computed in the extended reals with the moment E∥⋅∥pρ/(ρ−1)\mathbb E\|\cdot\|_p^{\rho/(\rho-1)}E∥⋅∥pρ/(ρ−1)​ in [0,∞][0, \infty][0,∞]. HHH's law is multivariateGaussian 0 Cov on EuclideanSpace ℝ (Fin r).

The goal is a conjunction: finiteness of Rn(θ∗)R_n(\theta_*)Rn​(θ∗​) for n≥1n \ge 1n≥1, its a.e.-measurability, attainment of the maxima in Rˉ(ρ)\bar R(\rho)Rˉ(ρ), and the limsup bound. Without the first three, a real-valued formalization could hold for the wrong reason (an infinite RnR_nRn​ converted to 000, a non-measurable integrand integrated to 000, or an unbounded supremum replaced by 000); the conjunction rules this out.

Readings of the page recorded in the items: A1) says q≥1q \ge 1q≥1 while (17) and the proof of Lemma 2 use q>1q > 1q>1, and q∈(1,∞]q \in (1,\infty]q∈(1,∞] is used; Proposition 3 is stated for a cost that is finite everywhere, the setting of §3, because for a cost that is infinite on part of the space the interior condition on h(Rm,θ)h(\mathbb R^m, \theta)h(Rm,θ) does not imply the Slater condition used in App. B; Lemmas 2 and 3 state the standing assumptions A1), A3) and i.i.d. sampling that their statements leave implicit. The localized weak limit (45) is not a milestone: its penalty Mn′M'_nMn′​ depends on a ζ\zetaζ-dependent near-optimal direction that is not stated precisely enough on the page.

Needed infrastructure: the multivariate central limit theorem (Mathlib has the real-valued one), Hölder duality for PiLp norms, a strong-duality theorem for moment problems (Proposition 7, quoted from Isii and Karlin–Studden), and a uniform law of large numbers. The duality results and the conjugate formula (42) are reusable beyond this mission. Proofs of any milestone, and lemmas that serve them, are welcome.

Selected references

  • J. Blanchet, Y. Kang, K. Murthy, Robust Wasserstein Profile Inference and Applications to Machine Learning, J. Appl. Probab. 56(3), 2019; arXiv:1610.05627v4. https://arxiv.org/abs/1610.05627
  • A. B. Owen, Empirical Likelihood, Chapman & Hall/CRC, 2001. https://doi.org/10.1201/9781420036152
  • J. Blanchet, K. Murthy, Quantifying Distributional Model Risk via Optimal Transport, Math. Oper. Res. 44(2), 2019. https://arxiv.org/abs/1604.01446
  • K. Isii, On sharpness of Tchebycheff-type inequalities, Ann. Inst. Statist. Math. 14, 1962. https://doi.org/10.1007/BF02868641
  • C. Villani, Optimal Transport: Old and New, Springer, 2009. https://doi.org/10.1007/978-3-540-71050-9
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Number Theory·Captain: xuanji

Every Odd Number Greater Than 1 is the Sum of at Most 85 PrimesResearch Paper

Motivation

Schnirelmann showed around 1930, by elementary means, that some absolute constant kkk makes every integer n>1n > 1n>1 a sum of at most kkk primes. For odd nnn:

  • Schnirelmann (1930s): some finite kkk, by elementary methods.
  • Klimov, Pil'tai, Sheptitskaya (1972): 115115115; Riesel–Vaughan (1983): 191919 for all integers, using zero-based prime-counting estimates.
  • Ramaré (1995): every even integer is a sum of at most six primes, so every odd n>1n > 1n>1 is a sum of at most seven. (Ann. Sc. Norm. Super. Pisa, 1995)
  • Tao (2014): at most five primes. (arXiv:1201.6656)
  • Helfgott (2013): every odd n>5n > 5n>5 is a sum of three primes. (arXiv:1312.7748)

The campaign's earlier values (100 001100\,001100001 down to 151151151) came from Schnirelmann's method with every constant written out, using only weak Chebyshev lower bounds for π(y)\pi(y)π(y). This entry keeps the same machinery as the 151151151 entry but feeds it Chebyshev's sharper lower bound ψ(x)≥ax−5log⁡x+5\psi(x) \ge ax - 5\log x + 5ψ(x)≥ax−5logx+5 with a≈0.9212a \approx 0.9212a≈0.9212, obtained from the weights 1,−1,−1,−1,+11, -1, -1, -1, +11,−1,−1,−1,+1 at 1,2,3,5,301, 2, 3, 5, 301,2,3,5,30. No zeta-zero input is used.

Setting

A representation of nnn as a sum of at most kkk primes is a finite multiset of primes summing to nnn with at most kkk elements counted with multiplicity. The Schnirelmann density of A⊆Z≥0A \subseteq \mathbb{Z}_{\ge 0}A⊆Z≥0​ is σ(A)=inf⁡N≥1∣A∩{1,…,N}∣/N\sigma(A) = \inf_{N \ge 1} |A \cap \{1, \dots, N\}|/Nσ(A)=infN≥1​∣A∩{1,…,N}∣/N (Mathlib: schnirelmannDensity).

Formalization target

Goal

∀n∈N,n odd, n>1  ⟹  ∃ s multiset of primes, ∣s∣≤85, ∑s=n.\forall n \in \mathbb{N},\quad n \text{ odd},\ n > 1 \implies \exists\, s \text{ multiset of primes},\ |s| \le 85,\ \textstyle\sum s = n.∀n∈N,n odd, n>1⟹∃s multiset of primes, ∣s∣≤85, ∑s=n.

This is the campaign template with the value 858585 filled in.

How the bound arises

Let B={(p−3)/2:p odd prime}B = \{(p-3)/2 : p \text{ odd prime}\}B={(p−3)/2:p odd prime} and A=B+BA = B + BA=B+B. We show σ(A)≥1/42\sigma(A) \ge 1/42σ(A)≥1/42, then conclude with Mann's theorem as in the 241241241 entry. Write L=log⁡yL = \log yL=logy for the scale.

  1. Chebyshev's constant a≈0.9212a \approx 0.9212a≈0.9212. For x≥30x \ge 30x≥30, ψ(x)≥ax−5log⁡x+5\psi(x) \ge ax - 5\log x + 5ψ(x)≥ax−5logx+5 with a=715log⁡2+310log⁡3+16log⁡5a = \tfrac{7}{15}\log 2 + \tfrac{3}{10}\log 3 + \tfrac16 \log 5a=157​log2+103​log3+61​log5 (Chebyshev's argument with log⁡⌊x⌋!\log \lfloor x \rfloor!log⌊x⌋! and Stirling-type bounds; ported from the PrimeNumberTheoremAnd library with explicit bounds for log⁡3\log 3log3 and log⁡5\log 5log5). Since ψ(x)≤π(x)log⁡x\psi(x) \le \pi(x)\log xψ(x)≤π(x)logx, this gives π(x)≥(ax−O(log⁡x))/log⁡x\pi(x) \ge (ax - O(\log x))/\log xπ(x)≥(ax−O(logx))/logx. On its own it covers L≲76L \lesssim 76L≲76 through B⊆AB \subseteq AB⊆A.
  2. Small-shift range (Riesel–Vaughan 1983, Lemma 8), 76≤L≤700076 \le L \le 700076≤L≤7000. Fix the first 300300300 odd primes p1≤1993p_1 \le 1993p1​≤1993 and let R(s)R(s)R(s) count s=p1+qs = p_1 + qs=p1​+q with qqq prime. Then ∑sR(s)\sum_s R(s)∑s​R(s) needs only the lower bound for π\piπ, and ∑sR(s)2\sum_s R(s)^2∑s​R(s)2 needs an upper bound for prime pairs q,q+dq, q + dq,q+d with a fixed even shift ddd. That bound is the Selberg sieve for a(a+d)a(a+d)a(a+d) on an interval, whose local data are those of the existing Goldbach sieve with s:=ds := ds:=d. The weight sum ∑p1≠p2C(p1−p2)\sum_{p_1 \ne p_2} C(p_1 - p_2)∑p1​=p2​​C(p1​−p2​) over these primes is a finite kernel computation. Cauchy–Schwarz then gives #{s≤y:R(s)>0}≥y/83\#\{s \le y : R(s) > 0\} \ge y/83#{s≤y:R(s)>0}≥y/83 on this range.
  3. Large range L≥7000L \ge 7000L≥7000: the Selberg pointwise bound r(s)≤b C(s) s/log⁡2sr(s) \le b\,C(s)\,s/\log^2 sr(s)≤bC(s)s/log2s with b=8.13b = 8.13b=8.13, the weighted first moment (now with constant a2a^2a2), the sixteenth moment of C(s)C(s)C(s), and Hölder, as in the 241241241 entry, at a much higher threshold.
  4. Mann's theorem turns 42 σ(A)≥142\,\sigma(A) \ge 142σ(A)≥1 into 42A=Z≥042A = \mathbb{Z}_{\ge 0}42A=Z≥0​, so every odd n≥171n \ge 171n≥171 is a sum of exactly 858585 primes (848484 odd primes plus one 333, padded with twos and threes for small nnn), and small nnn are handled with twos and threes: K=2⋅42+1=85K = 2 \cdot 42 + 1 = 85K=2⋅42+1=85.

Significance

The argument stays elementary: no prime number theorem and no zeros of ζ\zetaζ or LLL-functions. New reusable components:

  1. Explicit Selberg upper bound for prime pairs (q,q+d)(q, q+d)(q,q+d) with a fixed shift, uniform in ddd.
  2. The Riesel–Vaughan small-shift second-moment argument.
  3. A self-contained Lean proof of Chebyshev's lower bound ψ(x)≥ax−5log⁡x+5\psi(x) \ge ax - 5\log x + 5ψ(x)≥ax−5logx+5 (a≈0.9212a \approx 0.9212a≈0.9212), carried into the sieve moments.

Formalization scope

The Lean statement is the campaign template verbatim with 858585 in place of the value. Already proved on the platform: Schnir.sieve_ineq, Schnir.G_lower, Schnir.basis_of_density. Mathlib supplies the Chebyshev function ψ\psiψ with ψ(x)≤π(x)log⁡x\psi(x) \le \pi(x)\log xψ(x)≤π(x)logx and the Λ² sieve framework.

Selected references

  • H. Riesel, R. C. Vaughan, On sums of primes, Ark. Mat. 21 (1983), 45–74.
  • P. Pollack, Not Always Buried Deep, AMS, 2009, Chapter 6, §6. https://www.pollack-math.net/NABDofficial.pdf
  • K. S. Kedlaya, Notes on Analytic Number Theory, Chapter 13, "The Selberg sieve". https://kskedlaya.org/ant/chap-selberg.html
  • O. Ramaré, On Šnirel'man's constant, Ann. Sc. Norm. Super. Pisa (4) 22 (1995), 645–706.
  • T. Tao, Every odd number greater than 1 is the sum of at most five primes, Math. Comp. 83 (2014). https://arxiv.org/abs/1201.6656
  • Chebyshev's lower bound as formalized in PrimeNumberTheoremAnd (PrimeNumberTheoremAnd/IEANTN/Chebyshev.lean).
  • Explicit improvement of the 151151151 constant (unpublished AI-assisted calculation, October 2026). Source of the constant 858585; not peer reviewed.
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Control TheoryDynamic ProgrammingProbability·Captain: mikedeng1

Discrete-Time Controlled Markov Processes with Average Cost Criterion: A Survey 5: Canonical Triplets Are Exactly the Solutions of the Coupled Optimality EquationsResearch Paper

Motivation

A controlled Markov process run under the long-run average cost criterion asks for a policy minimizing the asymptotic cost per stage. When every stationary policy induces a single recurrent class, the optimal average cost is a constant and is characterized by one equation, the average cost optimality equation (ACOE). In general it is not: under some policies the state process splits into several ergodic classes, different classes have different optimal costs, and the optimal average cost is a function ρ(x)\rho(x)ρ(x) of the initial state. This is the multichain case.

For finite models, Howard ([Dynamic Programming and Markov Processes, 1960, pp. 61–62]) introduced a pair of coupled equations for this situation: one for the gain function ρ\rhoρ alone, and one, the ACOE, for ρ\rhoρ together with a relative value function hhh. Denardo and Fox (1968) developed the approach for finite multichain Markov renewal programs. For general Borel models, Yushkevich (1973) and Dynkin and Yushkevich (1979) introduced canonical triplets: a gain ρ\rhoρ, a terminal cost hhh and a policy π∗\pi^*π∗ such that π∗\pi^*π∗ is optimal for every finite horizon NNN with terminal cost hhh, and the optimal NNN-stage cost is exactly h+Nρh + N\rhoh+Nρ. The survey of Arapostathis, Borkar, Fernández-Gaucherand, Ghosh and Marcus (SIAM J. Control Optim. 31 (1993), §6.1) states the link between the two notions as Theorem 6.2 and proves it on p. 317.

Setting

A controlled Markov process is a five-tuple (S,A,U,P,c)(\mathbf S, \mathbf A, U, P, c)(S,A,U,P,c):

  1. S\mathbf SS, the state space, and A\mathbf AA, the action space, are Borel spaces;
  2. U(x)⊆AU(x) \subseteq \mathbf AU(x)⊆A is the nonempty compact set of admissible actions at xxx, and K={(x,a):a∈U(x)}\mathbf K = \{(x,a) : a \in U(x)\}K={(x,a):a∈U(x)} is measurable;
  3. P(dy∣x,a)P(dy \mid x, a)P(dy∣x,a) is a transition kernel on S\mathbf SS given K\mathbf KK;
  4. c:K→Rc : \mathbf K \to \mathbb Rc:K→R is a measurable one-stage cost with c≥0c \ge 0c≥0 (the paper's standing Assumption 2.1).

A history is ht=(x0,a0,…,xt−1,at−1,xt)h_t = (x_0, a_0, \dots, x_{t-1}, a_{t-1}, x_t)ht​=(x0​,a0​,…,xt−1​,at−1​,xt​). An admissible policy π=(πt)\pi = (\pi_t)π=(πt​) is a sequence of stochastic kernels πt(⋅∣ht)\pi_t(\cdot \mid h_t)πt​(⋅∣ht​) on A\mathbf AA with πt(U(xt)∣ht)=1\pi_t(U(x_t) \mid h_t) = 1πt​(U(xt​)∣ht​)=1; the class of all of them is Π\PiΠ. A stationary deterministic policy f∈ΠSDf \in \Pi_{SD}f∈ΠSD​ is a measurable map f:S→Af : \mathbf S \to \mathbf Af:S→A with f(x)∈U(x)f(x) \in U(x)f(x)∈U(x). An initial state xxx and a policy π\piπ determine a probability measure Pxπ\mathcal P^\pi_xPxπ​ on trajectories, with expectation ExπE^\pi_xExπ​. For a terminal cost hhh and N∈N0N \in \mathbb N_0N∈N0​,

JN(x,π,h)=Exπ[∑t=0N−1c(Xt,At)+h(XN)],JN∗(x,h)=inf⁡π∈ΠJN(x,π,h).J_N(x, \pi, h) = E^\pi_x\Big[\sum_{t=0}^{N-1} c(X_t, A_t) + h(X_N)\Big], \qquad J^*_N(x, h) = \inf_{\pi \in \Pi} J_N(x, \pi, h).JN​(x,π,h)=Exπ​[t=0∑N−1​c(Xt​,At​)+h(XN​)],JN∗​(x,h)=π∈Πinf​JN​(x,π,h).

Mb(S)\mathcal M_b(\mathbf S)Mb​(S) denotes the bounded measurable real functions on S\mathbf SS. For R,H∈Mb(S)R, H \in \mathcal M_b(\mathbf S)R,H∈Mb​(S) and π∗∈Π\pi^* \in \Piπ∗∈Π, the triplet (R,H,π∗)(R, H, \pi^*)(R,H,π∗) is canonical if

JN(x,π∗,H)=JN∗(x,H)=H(x)+NR(x)∀N∈N0, x∈S.(6.4)J_N(x, \pi^*, H) = J^*_N(x, H) = H(x) + N R(x) \qquad \forall N \in \mathbb N_0,\ x \in \mathbf S. \tag{6.4}JN​(x,π∗,H)=JN∗​(x,H)=H(x)+NR(x)∀N∈N0​, x∈S.(6.4)

Formalization targets

Goal: Theorem 6.2

Let π∗∈ΠSD\pi^* \in \Pi_{SD}π∗∈ΠSD​, ρ,h∈Mb(S)\rho, h \in \mathcal M_b(\mathbf S)ρ,h∈Mb​(S), and ccc bounded on K\mathbf KK. Then (ρ,h,π∗)(\rho, h, \pi^*)(ρ,h,π∗) is a canonical triplet if and only if, for all x∈Sx \in \mathbf Sx∈S,

ρ(x)=inf⁡a∈U(x){∫Sρ(y)P(dy∣x,a)},(6.6)\rho(x) = \inf_{a \in U(x)} \Big\{ \int_{\mathbf S} \rho(y) P(dy \mid x, a) \Big\}, \tag{6.6}ρ(x)=a∈U(x)inf​{∫S​ρ(y)P(dy∣x,a)},(6.6) ρ(x)+h(x)=inf⁡a∈U(x){c(x,a)+∫Sh(y)P(dy∣x,a)},(6.7)\rho(x) + h(x) = \inf_{a \in U(x)} \Big\{ c(x,a) + \int_{\mathbf S} h(y) P(dy \mid x, a) \Big\}, \tag{6.7}ρ(x)+h(x)=a∈U(x)inf​{c(x,a)+∫S​h(y)P(dy∣x,a)},(6.7)

and π∗(x)\pi^*(x)π∗(x) attains the infimum in both (6.6) and (6.7).

Milestones (the steps of the proof on p. 317)

  1. One-step decomposition (last line of (6.8)): for f∈ΠSDf \in \Pi_{SD}f∈ΠSD​, JN+1(x,f,h)=c(x,f(x))+∫JN(y,f,h)P(dy∣x,f(x))J_{N+1}(x, f, h) = c(x, f(x)) + \int J_N(y, f, h) P(dy \mid x, f(x))JN+1​(x,f,h)=c(x,f(x))+∫JN​(y,f,h)P(dy∣x,f(x)).
  2. Dynamic programming step (second line of (6.8)): if JN∗(⋅,h)J^*_N(\cdot, h)JN∗​(⋅,h) is bounded and measurable, then JN+1(x,π,h)≥T(JN∗)(x)J_{N+1}(x, \pi, h) \ge T(J^*_N)(x)JN+1​(x,π,h)≥T(JN∗​)(x) for every admissible π\piπ, where T(v)(x)=inf⁡a∈U(x){c(x,a)+∫v dP(⋅∣x,a)}T(v)(x) = \inf_{a \in U(x)}\{c(x,a) + \int v\, dP(\cdot \mid x, a)\}T(v)(x)=infa∈U(x)​{c(x,a)+∫vdP(⋅∣x,a)} is the map (2.5).
  3. Sufficiency, lower bound: under (6.6)–(6.7) and JN∗=h+NρJ^*_N = h + N\rhoJN∗​=h+Nρ, JN+1∗≥h+(N+1)ρJ^*_{N+1} \ge h + (N+1)\rhoJN+1∗​≥h+(N+1)ρ.
  4. Sufficiency, upper bound: under (6.6)–(6.7) and JN(⋅,π∗,h)=h+NρJ_N(\cdot, \pi^*, h) = h + N\rhoJN​(⋅,π∗,h)=h+Nρ, JN+1(⋅,π∗,h)=h+(N+1)ρ≥JN+1∗J_{N+1}(\cdot, \pi^*, h) = h + (N+1)\rho \ge J^*_{N+1}JN+1​(⋅,π∗,h)=h+(N+1)ρ≥JN+1∗​.

Significance

The result. Theorem 6.2 turns a statement about every finite horizon and every history-dependent randomized policy into two pointwise equations in (ρ,h)(\rho, h)(ρ,h) and a pointwise selection condition on π∗\pi^*π∗. A canonical policy is NNN-stage optimal for every NNN with terminal cost hhh; dividing (6.4) by NNN shows that its average cost is ρ\rhoρ. In the paper this is the entry point of Theorem 6.3, which shows that a canonical policy is strong average optimal and that ρ\rhoρ is the optimal average cost, without any recurrence assumption. Equation (6.6) is the condition that makes ρ\rhoρ behave as a constant in the optimization; when ρ\rhoρ is constant it holds trivially, and Theorem 6.2 specializes to the bounded ACOE with a minimizing selector.

Formalizing it. The theorem is proved in the paper (and earlier by Yushkevich). This mission formalizes that proof on a general Borel model with history-dependent randomized policies and path measures built by the Ionescu-Tulcea theorem. Prove2Me has no formalization of the multichain coupled equations or of canonical triplets beyond finite models. The finite-horizon dynamic programming inequality of milestone 2, for policies that may use the whole history, is reusable in any finite-horizon or average-cost development on Borel spaces.

Difficulty

The algebra in the proof takes a few lines. The work is in two probabilistic facts that the paper uses without comment.

The first is the Markov decomposition of the (N+1)(N+1)(N+1)-stage cost: conditioning on the first state–action pair turns the remaining NNN stages into an NNN-stage problem started from the next state. For a stationary policy the continuation is the same policy. For a history-dependent policy, the continuation is a policy that depends measurably on (x0,a0)(x_0, a_0)(x0​,a0​). Expressing this on the Ionescu-Tulcea measure is where the effort goes.

The second is the identity JN+1∗=T(JN∗)J^*_{N+1} = T(J^*_N)JN+1∗​=T(JN∗​). On a Borel model, JN∗J^*_NJN∗​ need not be measurable and the infimum need not be attained by a measurable selector. That is why the paper usually works with semicontinuous models (p. 288). Theorem 6.2 avoids the issue: only the inequality JN+1∗≥T(JN∗)J^*_{N+1} \ge T(J^*_N)JN+1∗​≥T(JN∗​) is needed, under the measurability that JN∗=h+NρJ^*_N = h + N\rhoJN∗​=h+Nρ supplies, and the reverse direction is supplied by the given π∗\pi^*π∗. A first attempt that proves the full identity JN+1∗=T(JN∗)J^*_{N+1} = T(J^*_N)JN+1∗​=T(JN∗​) for general Borel models runs into measurable selection problems that the theorem never needs.

Formalization scope

  • Model. BorelCMP S A has standard Borel S and Borel A, compact nonempty U x with measurable graph, a measurable cost c : S × A → ℝ with c ≥ 0 on K, and a Markov kernel P. c and P are total on S × A; only values on K enter. No continuity of c or P is assumed: Theorem 6.2 does not use Assumptions 2.2, 2.3 or 6.1.
  • Policies. Policy M is the paper's Π\PiΠ: history-dependent, randomized, with admissibility πt(U(xt)c∣ht)=0\pi_t(U(x_t)^c \mid h_t) = 0πt​(U(xt​)c∣ht​)=0. StationaryPolicy M is ΠSD\Pi_{SD}ΠSD​ (measurable fff with f(x)∈U(x)f(x) \in U(x)f(x)∈U(x)). The infimum JN∗J^*_NJN∗​ ranges over all of Policy M. Restricting it to stationary policies would make sufficiency trivial and necessity false, and is not what the paper states.
  • Costs. JN(x,π,h)J_N(x, \pi, h)JN​(x,π,h) is a Bochner integral against the path measure. Every statement assumes ccc bounded on K\mathbf KK and hhh bounded measurable, so the integral is a genuine expectation. JN∗J^*_NJN∗​ is a real infimum, which is the true infimum because the family is bounded below by −sup⁡∣h∣-\sup|h|−sup∣h∣ and nonempty whenever a stationary policy is given.
  • Coupled equations. (6.6) and (6.7) with "π∗(x)\pi^*(x)π∗(x) attains the infimum" are encoded in attained form: equality at a=π∗(x)a = \pi^*(x)a=π∗(x) and the inequality for every a∈U(x)a \in U(x)a∈U(x). This is equivalent to the printed condition and never forms a real infimum.
  • The gain is a function. ρ\rhoρ is a function of the state, not a constant. Specializing to a constant ρ\rhoρ (the unichain case) would trivialize (6.6) and is not the theorem.
  • Explicit choices. The paper's induction from N−1N-1N−1 to NNN is stated from NNN to N+1N+1N+1, so that no natural-number subtraction appears. Milestone 2 takes the measurability and boundedness of JN∗(⋅,h)J^*_N(\cdot, h)JN∗​(⋅,h) as a hypothesis, and takes any pointwise lower bound www of T(JN∗)T(J^*_N)T(JN∗​) in place of the infimum. In the second display of the sufficiency part, the paper prints JN−1∗(y,π∗,h)J^*_{N-1}(y, \pi^*, h)JN−1∗​(y,π∗,h); the quantity meant is JN−1(y,π∗,h)J_{N-1}(y, \pi^*, h)JN−1​(y,π∗,h), which milestone 4 uses.
  • Infrastructure. A complete development needs the Markov property of Kernel.trajMeasure at the first step, the shifted (continuation) policy and its measurability in the first state–action pair, and bounded-convergence bookkeeping for the Bochner integrals. These are reusable for every finite-horizon statement on this model. Proofs of the milestones are welcome independently. So are alternative proofs of the goal that bypass milestone 2 and argue directly with the canonical policy.

Selected references

  • A. Arapostathis, V. S. Borkar, E. Fernández-Gaucherand, M. K. Ghosh, S. I. Marcus, Discrete-time controlled Markov processes with average cost criterion: a survey, SIAM J. Control Optim. 31(2) (1993), 282–344, §6.1, Theorem 6.2. https://doi.org/10.1137/0331018
  • A. A. Yushkevich, On a class of strategies in general Markov decision models, Theory Probab. Appl. 18 (1973), 777–779.
  • E. B. Dynkin, A. A. Yushkevich, Controlled Markov Processes, Springer-Verlag, New York, 1979.
  • R. A. Howard, Dynamic Programming and Markov Processes, MIT Press, Cambridge, MA, 1960, pp. 61–62.
  • E. V. Denardo, B. L. Fox, Multichain Markov renewal programs, SIAM J. Appl. Math. 16 (1968), 468–487.
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Number Theory·Captain: xuanji

Every Odd Number Greater Than 1 is the Sum of at Most 159 PrimesResearch Paper

Motivation

Schnirelmann showed around 1930, by elementary means, that some absolute constant kkk makes every integer n>1n > 1n>1 a sum of at most kkk primes. For odd nnn:

  • Schnirelmann (1930s): some finite kkk, by elementary methods.
  • Klimov, Pil'tai, Sheptitskaya (1972): 115115115; Riesel–Vaughan (1983): 191919 for all integers, using zero-based prime-counting estimates.
  • Ramaré (1995): every even integer is a sum of at most six primes, so every odd n>1n > 1n>1 is a sum of at most seven. (Ann. Sc. Norm. Super. Pisa, 1995)
  • Tao (2014): at most five primes. (arXiv:1201.6656)
  • Helfgott (2013): every odd n>5n > 5n>5 is a sum of three primes. (arXiv:1312.7748)

The campaign's earlier values (100 001100\,001100001 down to 241241241) came from Schnirelmann's method with every constant written out. Those arguments stall near 241241241 because the medium range relies only on a Chebyshev lower bound for π(y)\pi(y)π(y). This entry adds the small-shift idea of Riesel and Vaughan, which removes that bottleneck without any zeta-zero input.

Setting

A representation of nnn as a sum of at most kkk primes is a finite multiset of primes summing to nnn with at most kkk elements counted with multiplicity. The Schnirelmann density of A⊆Z≥0A \subseteq \mathbb{Z}_{\ge 0}A⊆Z≥0​ is σ(A)=inf⁡N≥1∣A∩{1,…,N}∣/N\sigma(A) = \inf_{N \ge 1} |A \cap \{1, \dots, N\}|/Nσ(A)=infN≥1​∣A∩{1,…,N}∣/N (Mathlib: schnirelmannDensity).

Formalization target

Goal

∀n∈N,n odd, n>1  ⟹  ∃ s multiset of primes, ∣s∣≤159, ∑s=n.\forall n \in \mathbb{N},\quad n \text{ odd},\ n > 1 \implies \exists\, s \text{ multiset of primes},\ |s| \le 159,\ \textstyle\sum s = n.∀n∈N,n odd, n>1⟹∃s multiset of primes, ∣s∣≤159, ∑s=n.

This is the campaign template with the value 159159159 filled in.

How the bound arises

Let B={(p−3)/2:p odd prime}B = \{(p-3)/2 : p \text{ odd prime}\}B={(p−3)/2:p odd prime} and A=B+BA = B + BA=B+B. We show σ(A)≥1/79\sigma(A) \ge 1/79σ(A)≥1/79, then conclude with Mann's theorem as in the 241241241 entry. Write L=log⁡yL = \log yL=logy for the scale.

  1. Chebyshev constant log⁡2\log 2log2. Mathlib's ψ(x)≥(x−1)log⁡2−log⁡(x+2)\psi(x) \ge (x-1)\log 2 - \log(x+2)ψ(x)≥(x−1)log2−log(x+2) gives π(x)≥(xlog⁡2−O(log⁡x))/log⁡x\pi(x) \ge (x \log 2 - O(\log x))/\log xπ(x)≥(xlog2−O(logx))/logx, better than the constant 2/32/32/3 used in earlier entries. On its own it covers L≲90L \lesssim 90L≲90 through B⊆AB \subseteq AB⊆A.
  2. Small-shift range (Riesel–Vaughan 1983, Lemma 8). Fix the first 150150150 odd primes p1p_1p1​ (up to 877877877) and let R(s)R(s)R(s) count s=p1+qs = p_1 + qs=p1​+q with qqq prime. Then ∑sR(s)\sum_s R(s)∑s​R(s) needs only π\piπ, and ∑sR(s)2\sum_s R(s)^2∑s​R(s)2 needs an upper bound for prime pairs q,q+dq, q + dq,q+d with a fixed even shift ddd. That bound is the Selberg sieve for a(a+d)a(a+d)a(a+d) on an interval, whose local data are those of the existing Goldbach sieve with s:=ds := ds:=d. The weight sum ∑p1≠p2C(p1−p2)\sum_{p_1 \ne p_2} C(p_1 - p_2)∑p1​=p2​​C(p1​−p2​) over these primes is a finite computation. Cauchy–Schwarz then gives #{s≤y:R(s)>0}≥y/158\#\{s \le y : R(s) > 0\} \ge y/158#{s≤y:R(s)>0}≥y/158 for 90≲L≤300090 \lesssim L \le 300090≲L≤3000.
  3. Large range L≥3000L \ge 3000L≥3000: the Selberg pointwise bound r(s)≤b C(s) s/log⁡2sr(s) \le b\,C(s)\,s/\log^2 sr(s)≤bC(s)s/log2s, the weighted first moment (now with constant (log⁡2)2(\log 2)^2(log2)2), a high moment of C(s)C(s)C(s), and Hölder, as in the 241241241 entry, at a much higher threshold.
  4. Mann's theorem turns 79 σ(A)≥179\,\sigma(A) \ge 179σ(A)≥1 into 79A=Z≥079A = \mathbb{Z}_{\ge 0}79A=Z≥0​, so every odd nnn beyond a small bound is a sum of 158158158 odd primes plus one 333, and small nnn are handled with twos and threes: K=2⋅79+1=159K = 2 \cdot 79 + 1 = 159K=2⋅79+1=159.

Significance

The argument stays elementary: no prime number theorem and no zeros of ζ\zetaζ or LLL-functions. New reusable components:

  1. Explicit Selberg upper bound for prime pairs (q,q+d)(q, q+d)(q,q+d) with a fixed shift, uniform in ddd.
  2. The Riesel–Vaughan small-shift second-moment argument.
  3. Chebyshev's log⁡2\log 2log2 constant from Mathlib carried into the sieve moments.

Formalization scope

The Lean statement is the campaign template verbatim with 159159159 in place of the value. Already proved on the platform: Schnir.sieve_ineq, Schnir.G_lower, Schnir.pi_lower, Schnir.basis_of_density. Mathlib supplies the Chebyshev bounds (Chebyshev.psi_ge', Chebyshev.theta_le_log4_mul_x) and the Λ² sieve framework (Mathlib.NumberTheory.SelbergSieve).

Selected references

  • H. Riesel, R. C. Vaughan, On sums of primes, Ark. Mat. 21 (1983), 45–74.
  • P. Pollack, Not Always Buried Deep, AMS, 2009, Chapter 6, §6. https://www.pollack-math.net/NABDofficial.pdf
  • K. S. Kedlaya, Notes on Analytic Number Theory, Chapter 13, "The Selberg sieve". https://kskedlaya.org/ant/chap-selberg.html
  • O. Ramaré, On Šnirel'man's constant, Ann. Sc. Norm. Super. Pisa (4) 22 (1995), 645–706.
  • T. Tao, Every odd number greater than 1 is the sum of at most five primes, Math. Comp. 83 (2014). https://arxiv.org/abs/1201.6656
  • Explicit improvement of the 241241241 constant (unpublished AI-assisted calculation, October 2026). Source of the constant 159159159; not peer reviewed.
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Number Theory·Captain: xuanji

Every Odd Number Greater Than 1 is the Sum of at Most 151 PrimesResearch Paper

Motivation

Schnirelmann showed around 1930, by elementary means, that some absolute constant kkk makes every integer n>1n > 1n>1 a sum of at most kkk primes. For odd nnn:

  • Schnirelmann (1930s): some finite kkk, by elementary methods.
  • Klimov, Pil'tai, Sheptitskaya (1972): 115115115; Riesel–Vaughan (1983): 191919 for all integers, using zero-based prime-counting estimates.
  • Ramaré (1995): every even integer is a sum of at most six primes, so every odd n>1n > 1n>1 is a sum of at most seven. (Ann. Sc. Norm. Super. Pisa, 1995)
  • Tao (2014): at most five primes. (arXiv:1201.6656)
  • Helfgott (2013): every odd n>5n > 5n>5 is a sum of three primes. (arXiv:1312.7748)

The campaign's earlier values (100 001100\,001100001 down to 241241241) came from Schnirelmann's method with every constant written out. Those arguments stall near 241241241 because the medium range relies only on a Chebyshev lower bound for π(y)\pi(y)π(y). This entry adds the small-shift idea of Riesel and Vaughan, which removes that bottleneck without any zeta-zero input.

Setting

A representation of nnn as a sum of at most kkk primes is a finite multiset of primes summing to nnn with at most kkk elements counted with multiplicity. The Schnirelmann density of A⊆Z≥0A \subseteq \mathbb{Z}_{\ge 0}A⊆Z≥0​ is σ(A)=inf⁡N≥1∣A∩{1,…,N}∣/N\sigma(A) = \inf_{N \ge 1} |A \cap \{1, \dots, N\}|/Nσ(A)=infN≥1​∣A∩{1,…,N}∣/N (Mathlib: schnirelmannDensity).

Formalization target

Goal

∀n∈N,n odd, n>1  ⟹  ∃ s multiset of primes, ∣s∣≤151, ∑s=n.\forall n \in \mathbb{N},\quad n \text{ odd},\ n > 1 \implies \exists\, s \text{ multiset of primes},\ |s| \le 151,\ \textstyle\sum s = n.∀n∈N,n odd, n>1⟹∃s multiset of primes, ∣s∣≤151, ∑s=n.

This is the campaign template with the value 151151151 filled in.

How the bound arises

Let B={(p−3)/2:p odd prime}B = \{(p-3)/2 : p \text{ odd prime}\}B={(p−3)/2:p odd prime} and A=B+BA = B + BA=B+B. We show σ(A)≥1/75\sigma(A) \ge 1/75σ(A)≥1/75, then conclude with Mann's theorem as in the 241241241 entry. Write L=log⁡yL = \log yL=logy for the scale.

  1. Chebyshev constant log⁡2\log 2log2. Mathlib's ψ(x)≥(x−1)log⁡2−log⁡(x+2)\psi(x) \ge (x-1)\log 2 - \log(x+2)ψ(x)≥(x−1)log2−log(x+2) gives π(x)≥(xlog⁡2−O(log⁡x))/log⁡x\pi(x) \ge (x \log 2 - O(\log x))/\log xπ(x)≥(xlog2−O(logx))/logx, better than the constant 2/32/32/3 used in earlier entries. On its own it covers L≲90L \lesssim 90L≲90 through B⊆AB \subseteq AB⊆A.
  2. Small-shift range (Riesel–Vaughan 1983, Lemma 8). Fix the first 500500500 odd primes p1p_1p1​ (up to 358135813581) and let R(s)R(s)R(s) count s=p1+qs = p_1 + qs=p1​+q with qqq prime. Then ∑sR(s)\sum_s R(s)∑s​R(s) needs only π\piπ, and ∑sR(s)2\sum_s R(s)^2∑s​R(s)2 needs an upper bound for prime pairs q,q+dq, q + dq,q+d with a fixed even shift ddd. That bound is the Selberg sieve for a(a+d)a(a+d)a(a+d) on an interval, whose local data are those of the existing Goldbach sieve with s:=ds := ds:=d. The weight sum ∑p1≠p2C(p1−p2)\sum_{p_1 \ne p_2} C(p_1 - p_2)∑p1​=p2​​C(p1​−p2​) over these primes is a finite computation. Cauchy–Schwarz then gives #{s≤y:R(s)>0}≥y/150\#\{s \le y : R(s) > 0\} \ge y/150#{s≤y:R(s)>0}≥y/150 for 90≲L≤10490 \lesssim L \le 10^490≲L≤104.
  3. Large range L≥104L \ge 10^4L≥104: the Selberg pointwise bound r(s)≤b C(s) s/log⁡2sr(s) \le b\,C(s)\,s/\log^2 sr(s)≤bC(s)s/log2s, the weighted first moment (now with constant (log⁡2)2(\log 2)^2(log2)2), a high moment of C(s)C(s)C(s), and Hölder, as in the 241241241 entry, at a much higher threshold.
  4. Mann's theorem turns 75 σ(A)≥175\,\sigma(A) \ge 175σ(A)≥1 into 75A=Z≥075A = \mathbb{Z}_{\ge 0}75A=Z≥0​, so every odd nnn beyond a small bound is a sum of 150150150 odd primes plus one 333, and small nnn are handled with twos and threes: K=2⋅75+1=151K = 2 \cdot 75 + 1 = 151K=2⋅75+1=151.

Significance

The argument stays elementary: no prime number theorem and no zeros of ζ\zetaζ or LLL-functions. New reusable components:

  1. Explicit Selberg upper bound for prime pairs (q,q+d)(q, q+d)(q,q+d) with a fixed shift, uniform in ddd.
  2. The Riesel–Vaughan small-shift second-moment argument.
  3. Chebyshev's log⁡2\log 2log2 constant from Mathlib carried into the sieve moments.

Formalization scope

The Lean statement is the campaign template verbatim with 151151151 in place of the value. Already proved on the platform: Schnir.sieve_ineq, Schnir.G_lower, Schnir.pi_lower, Schnir.basis_of_density. Mathlib supplies the Chebyshev bounds (Chebyshev.psi_ge', Chebyshev.theta_le_log4_mul_x) and the Λ² sieve framework (Mathlib.NumberTheory.SelbergSieve).

Selected references

  • H. Riesel, R. C. Vaughan, On sums of primes, Ark. Mat. 21 (1983), 45–74.
  • P. Pollack, Not Always Buried Deep, AMS, 2009, Chapter 6, §6. https://www.pollack-math.net/NABDofficial.pdf
  • K. S. Kedlaya, Notes on Analytic Number Theory, Chapter 13, "The Selberg sieve". https://kskedlaya.org/ant/chap-selberg.html
  • O. Ramaré, On Šnirel'man's constant, Ann. Sc. Norm. Super. Pisa (4) 22 (1995), 645–706.
  • T. Tao, Every odd number greater than 1 is the sum of at most five primes, Math. Comp. 83 (2014). https://arxiv.org/abs/1201.6656
  • Explicit improvement of the 241241241 constant (unpublished AI-assisted calculation, October 2026). Source of the constant 151151151; not peer reviewed.
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Every Odd Number Greater Than 1 is the Sum of at Most 241 PrimesResearch Paper

Motivation

Schnirelmann showed around 1930, by elementary means, that some absolute constant kkk makes every integer n>1n > 1n>1 a sum of at most kkk primes. For odd nnn:

  • Schnirelmann (1930s): some finite kkk, by elementary methods.
  • Vinogradov (1937): every sufficiently large odd integer is a sum of three primes.
  • Ramaré (1995): every even integer is a sum of at most six primes, so every odd n>1n > 1n>1 is a sum of at most seven. (Ann. Sc. Norm. Super. Pisa, 1995)
  • Tao (2014): at most five primes. (arXiv:1201.6656)
  • Helfgott (2013): every odd n>5n > 5n>5 is a sum of three primes. (arXiv:1312.7748)

The campaign's first proved value, 100 001100\,001100001, came from Schnirelmann's method with every constant written out. This entry records a sharper value, 241241241, from the same elementary circle of ideas.

Setting

A representation of nnn as a sum of at most kkk primes is a finite multiset of primes summing to nnn with at most kkk elements counted with multiplicity. The Schnirelmann density of A⊆Z≥0A \subseteq \mathbb{Z}_{\ge 0}A⊆Z≥0​ is σ(A)=inf⁡N≥1∣A∩{1,…,N}∣/N\sigma(A) = \inf_{N \ge 1} |A \cap \{1, \dots, N\}|/Nσ(A)=infN≥1​∣A∩{1,…,N}∣/N (Mathlib: schnirelmannDensity).

Formalization target

Goal

∀n∈N,n odd, n>1  ⟹  ∃ s multiset of primes, ∣s∣≤241, ∑s=n.\forall n \in \mathbb{N},\quad n \text{ odd},\ n > 1 \implies \exists\, s \text{ multiset of primes},\ |s| \le 241,\ \textstyle\sum s = n.∀n∈N,n odd, n>1⟹∃s multiset of primes, ∣s∣≤241, ∑s=n.

This is the campaign template with the value 241241241 filled in. The argument proves the stronger statement that every odd n≥483n \ge 483n≥483 is a sum of exactly 241241241 primes; the at-most form for all odd n>1n > 1n>1 follows.

How the bound arises

It follows the companion 351351351 entry, with every parameter pushed to the limit of the same tools. Let B={(p−3)/2:p odd prime}B = \{(p-3)/2 : p \text{ odd prime}\}B={(p−3)/2:p odd prime} and A=B+BA = B + BA=B+B. We show σ(A)≥1/120\sigma(A) \ge 1/120σ(A)≥1/120:

  1. Sieve at a low threshold. The explicit Selberg inequality with z=s/(log⁡s)2z = \sqrt{s}/(\log s)^2z=s​/(logs)2 gives r(s)≤454 C(s) s/(log⁡s)2r(s) \le \tfrac{45}{4}\,C(s)\,s/(\log s)^2r(s)≤445​C(s)s/(logs)2 for even s≥e130s \ge e^{130}s≥e130, where r(s)r(s)r(s) counts representations s=p+qs = p + qs=p+q by odd primes and C(s)=∏p∣s(1+p/(p−1)2)C(s) = \prod_{p \mid s}\bigl(1 + p/(p-1)^2\bigr)C(s)=∏p∣s​(1+p/(p−1)2).
  2. Weighted first moment. ∑e130<s≤xr(s) (log⁡s)2/s≥0.439 x\sum_{e^{130} < s \le x} r(s)\,(\log s)^2/s \ge 0.439\,x∑e130<s≤x​r(s)(logs)2/s≥0.439x for x≥e159x \ge e^{159}x≥e159.
  3. Sixteenth moment of CCC. Expanding C(s)16C(s)^{16}C(s)16 over squarefree divisors, treating the primes up to 313131 exactly and bounding the tail in one step, gives ∑s≤x, 2∣sC(s)16≤9.44⋅1012 x\sum_{s \le x,\, 2 \mid s} C(s)^{16} \le 9.44 \cdot 10^{12}\, x∑s≤x,2∣s​C(s)16≤9.44⋅1012x.
  4. Hölder with exponent 161616 then gives #{s≤x:r(s)>0}≥x/238\#\{s \le x : r(s) > 0\} \ge x/238#{s≤x:r(s)>0}≥x/238 for x≥e159x \ge e^{159}x≥e159. Below that scale, Chebyshev's bound π(y)−1≥2y/(3log⁡y)\pi(y) - 1 \ge 2y/(3 \log y)π(y)−1≥2y/(3logy) and B⊆AB \subseteq AB⊆A suffice, so σ(A)≥1/120\sigma(A) \ge 1/120σ(A)≥1/120 at every scale.
  5. Mann's theorem, σ(D+E)≥min⁡{1,σ(D)+σ(E)}\sigma(D + E) \ge \min\{1, \sigma(D) + \sigma(E)\}σ(D+E)≥min{1,σ(D)+σ(E)} for sets containing 000, gives 120A=Z≥0120A = \mathbb{Z}_{\ge 0}120A=Z≥0​, so 240B=Z≥0240B = \mathbb{Z}_{\ge 0}240B=Z≥0​. For odd n≥3K=723n \ge 3K = 723n≥3K=723, write (n−3K)/2(n - 3K)/2(n−3K)/2 as a sum of 240240240 elements of BBB and add one more 333. For 483≤n<723483 \le n < 723483≤n<723, use n−2Kn - 2Kn−2K threes and 3K−n3K - n3K−n twos. This gives K=241K = 241K=241.

About 241241241 is the floor of this method: the medium range relies on the Chebyshev constant 2/32/32/3, which forces the sieve threshold below e4k/3e^{4k/3}e4k/3 and so inflates the sieve coefficient.

Significance

The bound is far weaker than Tao's 555 or Helfgott's 333, but it rests on an elementary argument with no "sufficiently large" threshold and no prime number theorem, so it is a realistic target for a complete formalization. Reusable components:

  1. Explicit Chebyshev-type lower bound for π(y)\pi(y)π(y).
  2. Explicit Selberg upper-bound sieve for r(s)r(s)r(s) at an arbitrary threshold.
  3. High moments ∑s≤xC(s)q\sum_{s \le x} C(s)^{q}∑s≤x​C(s)q of the singular-series factor.
  4. Mann's theorem (αβ\alpha\betaαβ theorem) on Schnirelmann density.

Formalization scope

The Lean statement is the campaign template verbatim with 241241241 in place of the value. All the ingredients above except the moment bound and the final assembly are already proved on the platform (Schnir.sieve_ineq, Schnir.G_lower, Schnir.pi_lower, Schnir.basis_of_density).

Selected references

  • P. Pollack, Not Always Buried Deep, AMS, 2009, Chapter 6, §6. https://www.pollack-math.net/NABDofficial.pdf
  • K. S. Kedlaya, Notes on Analytic Number Theory, Chapter 13, "The Selberg sieve". https://kskedlaya.org/ant/chap-selberg.html
  • O. Ramaré, On Šnirel'man's constant, Ann. Sc. Norm. Super. Pisa (4) 22 (1995), 645–706.
  • T. Tao, Every odd number greater than 1 is the sum of at most five primes, Math. Comp. 83 (2014). https://arxiv.org/abs/1201.6656
  • H. A. Helfgott, The ternary Goldbach conjecture is true, 2013. https://arxiv.org/abs/1312.7748
  • Explicit improvement of the 100 001100\,001100001 constant (unpublished AI-assisted calculation, October 2026), extending the 351351351 entry. Source of the constant 241241241; not peer reviewed.
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Dynamical SystemsFunctional Analysis·Captain: dbenbenn

Connes–Feldman–Weiss: an amenable equivalence relation is generated by a single transformationResearch Paper

This mission formalizes A. Connes, J. Feldman and B. Weiss, An amenable equivalence relation is generated by a single transformation, Ergodic Theory Dynam. Systems 1 (1981) 431–450 (doi:10.1017/S014338570000136X).

Motivation

A countable group acting on a measure space partitions it into countable orbits, and much of ergodic theory studies actions only through this orbit equivalence relation. The simplest relations are those of a single transformation, the orbits of an action of Z\mathbb ZZ. Connes, Feldman and Weiss characterize exactly which relations are of this kind, up to null sets: the amenable ones, those carrying an invariant mean. Since the orbit relation of any action of a countable amenable group is amenable, every such action is orbit equivalent to an action of Z\mathbb ZZ. The same theorem gives the uniqueness of Cartan subalgebras in hyperfinite von Neumann algebras.

On this platform it is the missing link in the Lodha–Moore mission, which passes between Lodha and Moore's definition of a μ\muμ-amenable relation (an orbit relation of Z\mathbb ZZ off a null set) and the invariant-mean definition of the Monod bundle: one direction is proved, the other (LodhaMoore.isMuAmenable_of_isAmenableRel) is this mission's goal in Lodha and Moore's language.

Timeline.

  • 1959, 1963: Dye proves orbit equivalence for measure-preserving actions of abelian groups and groups of polynomial growth (doi:10.2307/2372852, doi:10.2307/2373108).
  • 1976: Krieger classifies non-singular transformations up to orbit equivalence (doi:10.1007/BF01360278).
  • 1977: Feldman and Moore set up countable Borel equivalence relations and their von Neumann algebras (doi:10.1090/S0002-9947-1977-0578656-4).
  • 1978: Zimmer introduces amenable actions and shows that discrete subgroups act amenably on G/PG/PG/P for PPP amenable (doi:10.1016/0022-1236(78)90013-7).
  • 1980: Ornstein and Weiss prove that every measure-preserving action of a countable amenable group is orbit equivalent to an action of Z\mathbb ZZ (doi:10.1090/S0273-0979-1980-14702-3).
  • 1981: Connes, Feldman and Weiss prove it for every amenable non-singular countable equivalence relation, without a group.
  • 2004: Kechris and Miller give a detailed modern account in Topics in orbit equivalence (doi:10.1007/b99421).

Setting

XXX is a standard Borel space with a σ\sigmaσ-finite measure μ\muμ. A discrete measured equivalence relation (IsDiscreteMeasured μ R) is a Borel equivalence relation R⊆X×XR \subseteq X \times XR⊆X×X whose classes are countable and for which μ\muμ is quasi-invariant: the saturation R(A)={x∣∃y∈A,(x,y)∈R}R(A) = \{x \mid \exists y \in A, (x, y) \in R\}R(A)={x∣∃y∈A,(x,y)∈R} of a null Borel set AAA is null.

RRR carries the measure m=∫νx dμ(x)m = \int \nu^x\, d\mu(x)m=∫νxdμ(x), νx\nu^xνx the counting measure on the class of xxx (relMeasure), and the module δ\deltaδ, the density of mmm against its image under (x,y)↦(y,x)(x, y) \mapsto (y, x)(x,y)↦(y,x) (module). A partial transformation of RRR is a Borel bijection between Borel subsets of XXX whose graph lies in RRR (Monod.PartialTransformation).

RRR is amenable (Monod.IsAmenableRel) when it has a left invariant mean: a positive normalized map PPP from bounded functions on RRR to bounded functions on XXX with P(fϕ)=(Pf)ϕP(f^\phi) = (Pf)^\phiP(fϕ)=(Pf)ϕ for every partial transformation ϕ\phiϕ (Definitions 5–6). RRR is of type I (IsTypeI) when, off a null saturated set, its quotient is a standard Borel space, and hyperfinite (IsHyperfinite) when, off a null set, it is a countable increasing union of type I equivalence relations (Definition 1). A finite subequivalence relation (IsFiniteSubrelation) is a Borel T⊆RT \subseteq RT⊆R that is an equivalence relation with finite classes on T(0)={x∣(x,x)∈T}T^{(0)} = \{x \mid (x, x) \in T\}T(0)={x∣(x,x)∈T}.

Formalization targets

Goal (p. 431)

For RRR amenable there are a non-singular Borel automorphism TTT of XXX and a null set NNN with

(x,y)∈R  ⟺  ∃n∈Z, y=Tnx(x,y∉N).(x, y) \in R \iff \exists n \in \mathbb Z,\ y = T^n x \qquad (x, y \notin N).(x,y)∈R⟺∃n∈Z, y=Tnx(x,y∈/N).

Milestones

  • §1 (p. 434): the type I criterion; hyperfinite relations are those generated by one automorphism (Dye, external); subrelations of hyperfinite relations are hyperfinite.
  • §§2–3: Lemma 2 (disintegration over a finite subrelation), Feldman and Moore's Theorem 1 (external, as the proof of Lemma 3 applies it), Lemma 3 (bounded sets), Lemma 4 (local triviality).
  • §§5–6: Lemma 8 (the Følner condition), Lemma 9 (approximation by finite subrelations), Theorem 10 (hyperfinite if and only if amenable).
  • §7: Corollary 12, Corollary 13 (Vershik), and Corollary 14 with the amenability of the action it rests on (Zimmer, external).

Significance

The result. Theorem 10 turns amenability, which is usually easy to check, into hyperfiniteness, which is the structure one wants: for instance, the action of SL2(Z)\mathrm{SL}_2(\mathbb Z)SL2​(Z) on the projective line, or of any discrete group on G/PG/PG/P with PPP amenable, is generated by a single transformation. On this platform it closes the open direction, LodhaMoore.isMuAmenable_of_isAmenableRel, and with it Lodha and Moore's Theorem 2.1.

Formalizing it. No machine-checked proof of the theorem exists, in Mathlib or elsewhere as far as a search finds; Mathlib has no theory of countable Borel equivalence relations. A complete development builds that theory from the descriptive set theory Mathlib has.

Difficulty

The theorem is about relations without a group. The obvious route, through a countable group generating RRR and an amenability of that group, is unavailable: the orbit relation of a nonamenable group, such as SL2(Z)\mathrm{SL}_2(\mathbb Z)SL2​(Z) acting on the projective line, can be amenable, and there is no group whose Følner sets one could use. The Følner sets of Lemma 8 have to be produced from the invariant mean on the relation itself, which needs duality between L1L^1L1 and L∞L^\inftyL∞ and convexity arguments. Underneath, even the basic facts used in §§1–3 (that RRR is a countable union of graphs of Borel automorphisms, that mmm is a measure, that saturations of Borel sets are Borel) rest on the Lusin–Novikov uniformization theorem, which is not in Mathlib. It is published here as standalone theorems: a Borel set with countable sections is a countable union of Borel graphs, and a countable-to-one Borel map is injective on countably many Borel pieces covering its domain.

Formalization scope

All statements carry the hypotheses of §1: XXX standard Borel (StandardBorelSpace), μ\muμ σ\sigmaσ-finite, RRR a Borel equivalence relation with countable classes and μ\muμ quasi-invariant. Lemmas 8 and 9 take μ\muμ a probability measure, as the paper's proof of Lemma 9 does. “Up to a null set” is read as “off a μ\muμ-null Borel set of points”, which by quasi-invariance agrees with the paper's mmm-null sets. Amenability is the published Monod definition, an invariant mean on bounded measurable functions modulo null sets; it is not trivial (the relation of PSL2(A)\mathrm{PSL}_2(A)PSL2​(A) for a countable dense subring AAA of R\mathbb RR is not amenable, Monod.not_isAmenableRel_mob).

The definitions are in the definition bundle ConnesFeldmanWeiss. Reusable beyond this mission: the Feldman–Moore theorem and the basic theory of countable Borel equivalence relations, both welcome as standalone theorems.

What is left out. Proposition 7 and Corollary 11 need the von Neumann algebra of a relation and its Cartan subalgebras, which Mathlib does not have. The final part of the paper (Lemma 15 to Corollary 21) treats relations with uncountable classes through transverse functions, including foliations; it is a different setting with its own definitions.

Selected references

  • A. Connes, J. Feldman, B. Weiss, An amenable equivalence relation is generated by a single transformation, Ergodic Theory Dynam. Systems 1 (1981) 431–450. doi:10.1017/S014338570000136X
  • H. A. Dye, On groups of measure preserving transformations. I, Amer. J. Math. 81 (1959) 119–159. doi:10.2307/2372852
  • J. Feldman, C. C. Moore, Ergodic equivalence relations, cohomology, and von Neumann algebras. I, Trans. Amer. Math. Soc. 234 (1977) 289–324. doi:10.1090/S0002-9947-1977-0578656-4
  • R. J. Zimmer, Amenable ergodic group actions and an application to Poisson boundaries of random walks, J. Funct. Anal. 27 (1978) 350–372. doi:10.1016/0022-1236(78)90013-7
  • D. Ornstein, B. Weiss, Ergodic theory of amenable group actions. I: The Rohlin lemma, Bull. Amer. Math. Soc. 2 (1980) 161–164. doi:10.1090/S0273-0979-1980-14702-3
  • A. S. Kechris, B. D. Miller, Topics in orbit equivalence, Lecture Notes in Math. 1852, Springer, 2004. doi:10.1007/b99421
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Dynamical SystemsPartial Differential Equations·Captain: shivm

Catalytic Reaction–Diffusion: Global Attraction of the Positive Equilibrium (AIM 416)Open Problem

Motivation

Nguyen and Tang study the irreversible catalytic network A+B→B+C\mathcal A+\mathcal B\to\mathcal B+\mathcal CA+B→B+C, B+C→A+B\mathcal B+\mathcal C\to\mathcal A+\mathcal BB+C→A+B, a simple reaction–diffusion system with both a positive and a boundary equilibrium (catalyst used up). They settle every mass regime but one and leave it as a conjecture (AIM problem 416).

Timeline. 2021: Fellner–Morgan–Tang give global classical solutions with uniform bounds. 2026: Nguyen–Tang prove convergence for M1<M2M_1<M_2M1​<M2​ and M1≥2M2M_1\ge2M_2M1​≥2M2​ and local results in between, conjecturing global attraction there.

Setting

On a bounded connected smooth domain Ω⊂Rn\Omega\subset\mathbb R^nΩ⊂Rn with ∣Ω∣=1|\Omega|=1∣Ω∣=1 and d1,d2,d3>0d_1,d_2,d_3>0d1​,d2​,d3​>0:

at−d1Δa=b(c−a),bt−d2Δb=b(c−a),ct−d3Δc=−b(c−a),a_t-d_1\Delta a=b(c-a),\quad b_t-d_2\Delta b=b(c-a),\quad c_t-d_3\Delta c=-b(c-a),at​−d1​Δa=b(c−a),bt​−d2​Δb=b(c−a),ct​−d3​Δc=−b(c−a),

with homogeneous Neumann conditions and strictly positive C2C^2C2 compatible initial data. The masses M1=∫Ω(a0+c0)M_1=\int_\Omega(a_0+c_0)M1​=∫Ω​(a0​+c0​), M2=∫Ω(b0+c0)M_2=\int_\Omega(b_0+c_0)M2​=∫Ω​(b0​+c0​) are conserved. The equilibria are the positive one (M12, M2−M12, M12)(\frac{M_1}2,\,M_2-\frac{M_1}2,\,\frac{M_1}2)(2M1​​,M2​−2M1​​,2M1​​) and the boundary one (M1−M2, 0, M2)(M_1-M_2,\,0,\,M_2)(M1​−M2​,0,M2​).

Formalization target

If M2≤M1<2M2M_2\le M_1<2M_2M2​≤M1​<2M2​, every classical solution converges uniformly on Ω\OmegaΩ to the positive equilibrium (no rate required).

Significance

This is the last open regime of Nguyen–Tang's stability analysis. Strict positivity is essential: with b0≡0b_0\equiv0b0​≡0 the solution stays away from the positive equilibrium.

Difficulty

For M1≥M2M_1\ge M_2M1​≥M2​ there is no positive lower bound on ∫Ωb\int_\Omega b∫Ω​b, so entropy dissipation can degenerate near the boundary equilibrium (b=0b=0b=0), and the local results do not exclude trajectories approaching it.

Formalization scope

Rn\mathbb R^nRn is EuclideanSpace ℝ (Fin n) and Δ\DeltaΔ is Mathlib's Laplacian. The domain is Ω={φ<0}\Omega=\{\varphi<0\}Ω={φ<0} for a C∞C^\inftyC∞ function φ\varphiφ with ∇φ≠0\nabla\varphi\ne0∇φ=0 on {φ=0}\{\varphi=0\}{φ=0}; the Neumann condition is the derivative within Ω‾\overline\OmegaΩ in the direction ∇φ\nabla\varphi∇φ. Solutions are continuous on [0,∞)×Ω‾[0,\infty)\times\overline\Omega[0,∞)×Ω and C1,2C^{1,2}C1,2 for t>0t>0t>0, and L∞L^\inftyL∞ convergence is TendstoUniformlyOn. The goal quantifies over classical solutions; their existence is proved in the literature (Fellner–Morgan–Tang; Nguyen–Tang, Theorem 2.1) but is not part of this statement.

Selected references

  • T. L. Nguyen, B. Q. Tang, Stability analysis of irreversible chemical reaction-diffusion systems with boundary equilibria, Z. Angew. Math. Phys. 77, 2026, 199. DOI
  • K. Fellner, J. Morgan, B. Q. Tang, Uniform-in-time bounds for quadratic reaction-diffusion systems with mass dissipation in higher dimensions, DCDS-S 14, 2021, 635–651. DOI
  • AIM open problems list, problem 416. github.com/MColbrook/AIM
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Calculus of VariationsMathematical PhysicsPartial Differential Equations·Captain: shivm

Uniqueness of the Hemispheric Saddle Profile on a Magnetic Sphere (AIM 241)Open Problem

Motivation

Gustafson, Meinert and Melcher construct axisymmetric saddle points of the micromagnetic energy of a spherical shell in two ways (a heat flow, and continuation from an explicit solution at κ=4\kappa=4κ=4). Their Remark 3.18 conjectures that a single uniqueness statement identifies the two; it is problem 241 of the AIM open problem list.

Timeline. 2016: Kravchuk et al. propose the model. 2025: Gustafson–Meinert–Melcher construct the saddle points and state the conjecture.

Setting

For anisotropy κ>0\kappa>0κ>0 the energy of m:S2→S2m:S^2\to S^2m:S2→S2 is Eκ(m)=12∫S2∣∇m∣2+κ (1−(m⋅x)2)\mathcal E_\kappa(m)=\frac12\int_{S^2}|\nabla m|^2+\kappa\,(1-(m\cdot x)^2)Eκ​(m)=21​∫S2​∣∇m∣2+κ(1−(m⋅x)2). An axisymmetric field m=(sin⁡hcos⁡φ, sin⁡hsin⁡φ, cos⁡h)m=(\sin h\cos\varphi,\ \sin h\sin\varphi,\ \cos h)m=(sinhcosφ, sinhsinφ, cosh) with profile h(θ)h(\theta)h(θ) is critical exactly when

h′′+cot⁡θ h′−sin⁡2h2sin⁡2θ−κ2sin⁡(2h−2θ)=0(0<θ<π).(2.6)h''+\cot\theta\,h'-\frac{\sin 2h}{2\sin^2\theta}-\frac{\kappa}{2}\sin(2h-2\theta)=0\qquad(0<\theta<\pi).\tag{2.6}h′′+cotθh′−2sin2θsin2h​−2κ​sin(2h−2θ)=0(0<θ<π).(2.6)

The hemispheric class H0,2H_{0,2}H0,2​ adds h(0)=0h(0)=0h(0)=0, h(π)=2πh(\pi)=2\pih(π)=2π, h(π−θ)=2π−h(θ)h(\pi-\theta)=2\pi-h(\theta)h(π−θ)=2π−h(θ).

Formalization target

For every κ≥4\kappa\ge4κ≥4 there is exactly one smooth profile in H0,2H_{0,2}H0,2​ that solves (2.6) and induces a smooth map S2→S2S^2\to S^2S2→S2. The statement may be proved or disproved.

Significance

Uniqueness would identify the two constructions as one saddle branch; a counterexample would give further degree-zero critical points of Eκ\mathcal E_\kappaEκ​.

Difficulty

(2.6) is singular at both poles and H0,2H_{0,2}H0,2​ is a two-point boundary condition, so standard ODE uniqueness does not apply, and the paper's comparison arguments only control solutions in the wedge θ≤h≤2θ\theta\le h\le 2\thetaθ≤h≤2θ. Numerical evidence (shooting) finds at κ=4\kappa=4κ=4, besides h=2θh=2\thetah=2θ, a second solution in the class with h′(0)≈3.899h'(0)\approx3.899h′(0)≈3.899 (similarly at κ=5,8\kappa=5,8κ=5,8), which leaves the wedge.

Formalization scope

Profiles are functions h:R→Rh:\mathbb R\to\mathbb Rh:R→R; all conditions, and the uniqueness, are imposed on [0,π][0,\pi][0,π] only (values outside are unconstrained, so uniqueness on R\mathbb RR would be trivially false). Smoothness is ContDiffOn ℝ ∞ on [0,π][0,\pi][0,π]. "Induces a smooth map" means the field extended to R3∖{0}\mathbb R^3\setminus\{0\}R3∖{0} as a function of x/∣x∣x/|x|x/∣x∣ is C∞C^\inftyC∞ there; this excludes profiles with a cone singularity at a pole. The paper's H0,2H_{0,2}H0,2​ uses piecewise C1C^1C1 profiles; by its Corollary 2.7 it has the same solutions.

Selected references

  • S. Gustafson, D. Meinert, C. Melcher, Saddle Point Configurations for Spherical Ferromagnets, preprint, 2025. arXiv:2509.05159
  • V. P. Kravchuk et al., Topologically stable magnetization states on a spherical shell: Curvature-stabilized skyrmions, Phys. Rev. B 94, 144402, 2016. DOI
  • AIM open problems list, problem 241. github.com/MColbrook/AIM
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CombinatoricsInformation Theory·Captain: shivm

Periodic Multidimensional Costas Arrays (Rubio–Torres Conjecture 1)Open Problem

Motivation

A Costas array is a permutation matrix in which the difference vectors between distinct dots are pairwise distinct; such arrays are frequency-hopping patterns for sonar and radar (Costas, 1984). Rubio and Torres ask whether their mmm-dimensional version can stay Costas in every window of its periodic extension, and conjecture that this happens only in the smallest order.

Timeline. 1984: Taylor proves that 2D periodic Costas arrays have order ≤2\le 2≤2. 2023: Rubio–Torres prove the odd-order and 3D cases, give 2×2×42\times2\times42×2×4 examples, and state Conjecture 1.

Setting

Let [n]={1,…,n}[n]=\{1,\dots,n\}[n]={1,…,n}, X=[a1]×⋯×[ak]X=[a_1]\times\cdots\times[a_k]X=[a1​]×⋯×[ak​], Y=[b1]×⋯×[bl]Y=[b_1]\times\cdots\times[b_l]Y=[b1​]×⋯×[bl​] with all sides ≥2\ge2≥2, and φ:X→Y\varphi:X\to Yφ:X→Y a bijection; the dots are (x,φ(x))∈Zk+l(x,\varphi(x))\in\mathbb Z^{k+l}(x,φ(x))∈Zk+l. The array is Costas if the difference vectors between distinct dots are distinct, and periodic Costas if moreover, after repeating the dots periodically over Zk+l\mathbb Z^{k+l}Zk+l, the dots inside every translate t+X×Yt+X\times Yt+X×Y have distinct difference vectors.

Formalization target

Conjecture 1: if k≥l≥1k\ge l\ge1k≥l≥1 and φ\varphiφ defines a periodic Costas array, then

∏i=1kai=2k,\prod_{i=1}^k a_i=2^k,i=1∏k​ai​=2k,

equivalently every ai=2a_i=2ai​=2. The condition k≥lk\ge lk≥l is a normalization (φ−1\varphi^{-1}φ−1 swaps the boxes).

Significance

A proof would give the multidimensional analogue of Taylor's theorem; a counterexample would give periodic distinct-difference patterns of non-power-of-two order.

Difficulty

The Rubio–Torres counting argument needs a bound that is available only when YYY is one-dimensional, which is why it stops at m=3m=3m=3. Computational evidence: an exhaustive window check reports that the 2×3×2×32\times3\times2\times32×3×2×3 array with dots (1,1,1,1),(1,2,1,2),(1,3,2,1),(2,1,1,3),(2,2,2,3),(2,3,2,2)(1,1,1,1),(1,2,1,2),(1,3,2,1),(2,1,1,3),(2,2,2,3),(2,3,2,2)(1,1,1,1),(1,2,1,2),(1,3,2,1),(2,1,1,3),(2,2,2,3),(2,3,2,2) is periodic Costas, which would disprove the conjecture.

Formalization scope

A point of Zk+l\mathbb Z^{k+l}Zk+l is a pair (x,y)(x,y)(x,y); boxes are 1-based; φ\varphiφ is a total function Zk→Zl\mathbb Z^k\to\mathbb Z^lZk→Zl whose values off XXX are unused. Differences are plain integer vectors (not reduced modulo the sides), windows range over all t∈Zk+lt\in\mathbb Z^{k+l}t∈Zk+l, and k,l≥1k,l\ge1k,l≥1 and sides ≥2\ge2≥2 are part of the definition, so no degenerate case holds vacuously.

Selected references

  • I. Rubio, J. Torres, Multidimensional Costas Arrays and Their Periodicity, IEEE Trans. Inf. Theory 69(8), 2023, 5032–5040. arXiv:2208.02378, DOI
  • J. P. Costas, A study of a class of detection waveforms having nearly ideal range-Doppler ambiguity properties, Proc. IEEE 72(8), 1984, 996–1009.
  • S. W. Golomb, H. Taylor, Constructions and properties of Costas arrays, Proc. IEEE 72(9), 1984, 1143–1163.
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About Prove2Me

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

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