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

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

Campaigns (experimental)

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

3SUM Exponent

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

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

≤ 1.999074Formalized record
3 provers on it4 of 4 missions formalized

All-Pairs Shortest Paths (APSP) Exponent

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

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

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

The irrationality measure of π

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

≤ 7.103205334138Formalized record→≤ 2Open frontier
8 provers on it7 of 8 missions formalized

Sharp diagonal Hlawka constant

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

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

References:

  • Wolfram MathWorld, Hlawka's Inequality.
  • Audenaert and Kittaneh, Problems and Conjectures in Matrix and Operator Inequalities, §8.2 (2017).
  • Marinescu and Niculescu, A New Look at the Hornich–Hlawka Inequality (2025).
  • Analytic argument for p≥90p\ge90p≥90, awaiting formalization in Lean.
≤ 80Formalized record
3 provers on it7 of 7 missions formalized

Odd numbers as sums of primes

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

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

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

Matrix multiplication exponent

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

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

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

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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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Number Theory·Captain: Lucas

Chebotarëv's Density Theorem (Stevenhagen–Lenstra 1996)Research Paper

Motivation

Given a monic polynomial fff with integer coefficients, one can reduce it modulo each prime ppp and factor it over the finite field Fp\mathbb F_pFp​. The way fff factors changes with ppp, and the question of how often each factorization pattern occurs has a precise answer: Chebotarëv's density theorem (1922). It is the common generalization of Dirichlet's theorem on primes in arithmetic progressions (1837) and a theorem of Frobenius (1880, published 1896), and it underlies a large part of algebraic number theory, for example the fact that a Galois extension of a number field is determined by the set of primes that split completely in it. This mission follows the elementary exposition of P. Stevenhagen and H. W. Lenstra, Jr. (Math. Intelligencer 18 (1996)), which states all three theorems over Q\mathbb QQ with a minimum of terminology.

Timeline.

  • 1837 — Dirichlet: primes are equidistributed (in analytic density) over the invertible residue classes modulo mmm.
  • 1880/1896 — Frobenius: the density of primes with a given decomposition type of fff modulo ppp equals the proportion of Galois group elements with that cycle pattern; he conjectures the sharper statement for conjugacy classes.
  • 1896 — de la Vallée-Poussin: Dirichlet's theorem for natural density.
  • 1922/1925 — Chebotarëv proves Frobenius's conjecture, without class field theory.
  • 1935 — Deuring's proof via Artin reciprocity, now the textbook route.

Setting

Let f∈Z[X]f\in\mathbb Z[X]f∈Z[X] be monic of degree nnn with nonzero discriminant Δ(f)\Delta(f)Δ(f), so that fff has nnn distinct complex zeros α1,…,αn\alpha_1,\dots,\alpha_nα1​,…,αn​. Let K=Q(α1,…,αn)K=\mathbb Q(\alpha_1,\dots,\alpha_n)K=Q(α1​,…,αn​) be its splitting field and G=Gal(K/Q)G=\mathrm{Gal}(K/\mathbb Q)G=Gal(K/Q) its Galois group. Every σ∈G\sigma\in Gσ∈G permutes the zeros; the lengths of the cycles (including cycles of length 1) form the cycle pattern of σ\sigmaσ, a partition of nnn.

For a prime p∤Δ(f)p\nmid\Delta(f)p∤Δ(f), the degrees of the irreducible factors of f mod pf \bmod pfmodp over Fp\mathbb F_pFp​ form the decomposition type of fff modulo ppp, again a partition of nnn.

A Frobenius substitution of ppp is an element σ∈G\sigma\in Gσ∈G such that, for some prime ideal Q\mathfrak QQ of the ring of integers OK\mathcal O_KOK​ lying over ppp,

σ(x)≡xp(modQ)for all x∈OK.\sigma(x)\equiv x^p \pmod{\mathfrak Q}\qquad\text{for all }x\in\mathcal O_K .σ(x)≡xp(modQ)for all x∈OK​.

For p∤Δ(f)p\nmid\Delta(f)p∤Δ(f) these elements form a single conjugacy class of GGG, written σp\sigma_pσp​.

A set SSS of primes has (analytic, or Dirichlet) density δ\deltaδ if

∑p∈Sp−slog⁡1s−1⟶δ(s↓1),\frac{\sum_{p\in S}p^{-s}}{\log\frac{1}{s-1}}\longrightarrow\delta\qquad(s\downarrow 1),logs−11​∑p∈S​p−s​⟶δ(s↓1),

and natural density δ\deltaδ if #{p≤x:p∈S}/#{p≤x}→δ\#\{p\le x:p\in S\}/\#\{p\le x\}\to\delta#{p≤x:p∈S}/#{p≤x}→δ as x→∞x\to\inftyx→∞.

Formalization targets

Goal: Chebotarëv's density theorem

For every conjugacy class CCC of GGG,

the set {p prime:p∤Δ(f), σp∈C} has analytic density #C#G.\text{the set }\{p \text{ prime}: p\nmid\Delta(f),\ \sigma_p\in C\}\text{ has analytic density }\frac{\#C}{\#G}.the set {p prime:p∤Δ(f), σp​∈C} has analytic density #G#C​.

Milestones

  1. Theorem of Dirichlet: for m≥1m\ge1m≥1 and gcd⁡(a,m)=1\gcd(a,m)=1gcd(a,m)=1, the primes p≡a(modm)p\equiv a \pmod mp≡a(modm) have density 1/φ(m)1/\varphi(m)1/φ(m).
  2. A set of primes with natural density δ\deltaδ has analytic density δ\deltaδ.
  3. Galois theory of finite fields: for a squarefree g∈Fp[X]g\in\mathbb F_p[X]g∈Fp​[X], the cycle pattern of x↦xpx\mapsto x^px↦xp on the zeros of ggg equals the decomposition type of ggg.
  4. For p∤Δ(f)p\nmid\Delta(f)p∤Δ(f), the Frobenius substitutions of ppp form exactly one conjugacy class of GGG.
  5. For p∤Δ(f)p\nmid\Delta(f)p∤Δ(f), the cycle pattern of σp\sigma_pσp​ equals the decomposition type of fff modulo ppp.
  6. For f=Xm−1f=X^m-1f=Xm−1 and p∤mp\nmid mp∤m, σp(ζ)=ζp\sigma_p(\zeta)=\zeta^pσp​(ζ)=ζp for every primitive mmm-th root of unity ζ\zetaζ; that is, σp\sigma_pσp​ corresponds to p mod mp \bmod mpmodm under G≅(Z/mZ)×G\cong(\mathbb Z/m\mathbb Z)^\timesG≅(Z/mZ)×.
  7. Theorem of Frobenius: the primes p∤Δ(f)p\nmid\Delta(f)p∤Δ(f) for which fff has a given decomposition type ttt have density #{σ∈G:cycle pattern t}/#G\#\{\sigma\in G:\text{cycle pattern }t\}/\#G#{σ∈G:cycle pattern t}/#G.

Significance

Chebotarëv's theorem shows that every conjugacy class of the Galois group occurs as a Frobenius class for infinitely many primes, with a predictable frequency. Its standard consequences include: the Frobenius elements are equidistributed; a Galois extension is determined by its completely split primes; if fff has a zero modulo almost every prime then fff is linear or reducible; prime ideals are equidistributed over ideal classes. The theorem is the first step in many arguments in arithmetic geometry (e.g. Serre's work on ℓ\ellℓ-adic representations).

The theorem is classical and proved; this mission is about formalizing it. Mathlib contains Frobenius elements in Galois extensions of Dedekind domains and Dirichlet's theorem in the form "infinitely many primes in each coprime residue class", but, to our knowledge, neither the density form of Dirichlet's theorem nor Frobenius's or Chebotarëv's density theorem.

Difficulty

The Galois-theoretic parts (milestones 3–6) are standard but require connecting Frobenius elements in OK\mathcal O_KOK​ with factorization of fff modulo ppp, including the fact that p∤Δ(f)p\nmid\Delta(f)p∤Δ(f) forces ppp to be unramified in KKK. The analytic core is harder: one needs Dedekind zeta functions and LLL-functions of number fields and their behaviour at s=1s=1s=1. The reduction of the general case to the cyclotomic case (Chebotarëv's "crossing" with cyclotomic extensions) needs the density statement over an arbitrary number field as base, not only over Q\mathbb QQ; in particular, the statement over Q\mathbb QQ alone cannot be proved by induction on itself.

Formalization scope

All declarations live in the namespace ChebotarevDensity and share one definition file.

  • KKK is Mathlib's SplittingField of fff viewed in Q[X]\mathbb Q[X]Q[X]; GGG is Polynomial.Gal; Δ(f)\Delta(f)Δ(f) is Mathlib's Polynomial.discr.
  • A Frobenius substitution is expressed with Mathlib's IsArithFrobAt at some prime ideal of OK\mathcal O_KOK​ containing ppp; "σp∈C\sigma_p\in Cσp​∈C" means that some Frobenius substitution of ppp lies in CCC (for p∤Δ(f)p\nmid\Delta(f)p∤Δ(f) this is equivalent to all of them lying in CCC, by milestone 4).
  • The cycle pattern is Equiv.Perm.partition of the permutation induced on the complex zeros of fff; it includes fixed points.
  • The decomposition type is the multiset of degrees of the normalized (monic) irreducible factors of f mod pf \bmod pfmodp.
  • Analytic density uses ∑′p−s\sum' p^{-s}∑′p−s over the primes of SSS and the limit s→1+s\to1^+s→1+ within (1,∞)(1,\infty)(1,∞); natural density compares prime counts up to x∈Nx\in\mathbb Nx∈N.
  • The hypotheses Δ(f)≠0\Delta(f)\neq0Δ(f)=0 and "fff monic" are those of the source; the theorems are not vacuous, since e.g. f=Xm−1f=X^m-1f=Xm−1 satisfies them.

Welcome contributions: Dedekind zeta functions and Hecke LLL-functions at s=1s=1s=1, the density form of Dirichlet's theorem, unramifiedness of primes not dividing the discriminant, and the general number-field version of the theorem.

Selected references

  • P. Stevenhagen, H. W. Lenstra, Jr., Chebotarëv and his density theorem, Math. Intelligencer 18 (1996), no. 2, 26–37. doi:10.1007/BF03027290
  • N. Tschebotareff, Die Bestimmung der Dichtigkeit einer Menge von Primzahlen, welche zu einer gegebenen Substitutionsklasse gehören, Math. Ann. 95 (1925), 191–228. doi:10.1007/BF01206606
  • S. Lang, Algebraic Number Theory, Addison-Wesley, 1970, Chap. VIII.
  • J. Neukirch, Class Field Theory, Springer, 1986, Chap. V.
  • Chebotarev density theorem, Wikipedia. link
16 thms2 active usersReviewed
Algebraic GeometryNumber Theory·Captain: Lucas

Lam–Litt conjecture: algebraicity and integrality of solutions to algebraic ODEsOpen Problem

Motivation

A classical way to recognize an algebraic function is through the arithmetic of its Taylor coefficients. Eisenstein's theorem (1852) says that if a power series f∈Q[[z]]f\in\mathbb{Q}[[z]]f∈Q[[z]] is algebraic over Q[z]\mathbb{Q}[z]Q[z], only finitely many primes occur in the denominators of its coefficients. The converse fails in general: many transcendental power series have integer coefficients. Lam and Litt (arXiv:2501.13175) conjecture that the converse does hold for power series that solve an algebraic differential equation at a non-singular point, and that even a weak control on denominators — primes ppp may appear, but only after roughly ω(p)≫p\omega(p)\gg pω(p)≫p coefficients — already forces algebraicity.

For linear differential equations, the conjecture is a strengthening of the Grothendieck–Katz ppp-curvature conjecture, one of the central open problems about algebraic solutions of linear differential equations (arXiv:2501.13175). The bounded-denominator form is Problem 1 on Litt's list of open problems (problemsilike.com/1).

Timeline.

  • 1852 — Eisenstein: algebraic power series over Q\mathbb{Q}Q have bounded denominators (implication (1)⇒(2) below).
  • 1970s — Grothendieck and Katz: the ppp-curvature conjecture for linear differential equations.
  • 2025 — Lam and Litt formulate the conjecture for (possibly non-linear) algebraic differential equations and prove it for many equations and initial conditions of algebro-geometric interest, including Picard–Fuchs equations at initial conditions corresponding to cycle classes, and isomonodromy equations such as Painlevé VI and the Schlesinger system at initial conditions corresponding to Picard–Fuchs equations (arXiv:2501.13175).

Setting

Let f=∑k≥0akzk∈Q[[z]]f=\sum_{k\ge0}a_kz^k\in\mathbb{Q}[[z]]f=∑k≥0​ak​zk∈Q[[z]] be a formal power series with rational coefficients and write f(i)f^{(i)}f(i) for its iii-th formal derivative. Let g∈Q(z,y0,…,yn−1)g\in\mathbb{Q}(z,y_0,\dots,y_{n-1})g∈Q(z,y0​,…,yn−1​) be a rational function in n+1n+1n+1 variables. The series fff solves the algebraic ODE defined by ggg if

f(n)(z)=g(z,f(z),f′(z),…,f(n−1)(z))f^{(n)}(z)=g\bigl(z,f(z),f'(z),\dots,f^{(n-1)}(z)\bigr)f(n)(z)=g(z,f(z),f′(z),…,f(n−1)(z))

and ggg is defined at (0,f(0),…,f(n−1)(0))\bigl(0,f(0),\dots,f^{(n-1)}(0)\bigr)(0,f(0),…,f(n−1)(0)). Concretely, g=p/qg=p/qg=p/q for polynomials p,qp,qp,q with q(0,f(0),…,f(n−1)(0))≠0q\bigl(0,f(0),\dots,f^{(n-1)}(0)\bigr)\neq0q(0,f(0),…,f(n−1)(0))=0 and f(n)⋅q(z,f,…,f(n−1))=p(z,f,…,f(n−1))f^{(n)}\cdot q(z,f,\dots,f^{(n-1)})=p(z,f,\dots,f^{(n-1)})f(n)⋅q(z,f,…,f(n−1))=p(z,f,…,f(n−1)).

For N∈NN\in\mathbb{N}N∈N, Z[1/N]⊆Q\mathbb{Z}[1/N]\subseteq\mathbb{Q}Z[1/N]⊆Q is the subring generated by 1/N1/N1/N. For a function ω\omegaω from the primes to Z\mathbb{Z}Z, the coefficients of fff are ω\omegaω-integral if for every prime ppp the numbers a0,…,aω(p)a_0,\dots,a_{\omega(p)}a0​,…,aω(p)​ lie in Z(p)\mathbb{Z}_{(p)}Z(p)​ (denominators prime to ppp); ω\omegaω is superlinear if ω(p)/p→∞\omega(p)/p\to\inftyω(p)/p→∞.

Formalization targets

Goal: the Lam–Litt conjecture

For fff solving an algebraic ODE as above, the following are equivalent:

(1) f is algebraic over Q[z];(2) ∃N, ∀k, ak∈Z[1/N];(3) ∃ ω superlinear with (ak) ω-integral.\text{(1) } f \text{ is algebraic over } \mathbb{Q}[z];\qquad \text{(2) } \exists N,\ \forall k,\ a_k\in\mathbb{Z}[1/N];\qquad \text{(3) } \exists\,\omega \text{ superlinear with } (a_k) \ \omega\text{-integral}.(1) f is algebraic over Q[z];(2) ∃N, ∀k, ak​∈Z[1/N];(3) ∃ω superlinear with (ak​) ω-integral.

Milestones

  • (1)⇒(2), Eisenstein's theorem (no ODE hypothesis needed).
  • (2)⇒(3), elementary (no ODE hypothesis needed).
  • (3)⇒(2), open.
  • (2)⇒(1), open; Litt's Problem 1.

Together the four milestones imply the goal; the last two are the open content of the conjecture.

Significance

A proof would give an arithmetic criterion for algebraicity of solutions of arbitrary algebraic differential equations, and, for linear equations, would imply the Grothendieck–Katz ppp-curvature conjecture (arXiv:2501.13175). Lam and Litt draw algebro-geometric consequences from the cases they prove.

For formalization: the conjecture is open, so the goal and the two open milestones are research targets. Eisenstein's theorem is a classical result; formalizing it is concrete, self-contained work. The implication (2)⇒(3) is elementary. The cases proved by Lam and Litt are candidates for further milestones.

Difficulty

Integrality of coefficients alone does not detect algebraicity: there are transcendental power series with integer coefficients that satisfy linear differential equations, such as ∑k(2kk)2zk\sum_k\binom{2k}{k}^2z^k∑k​(k2k​)2zk. Its equation is singular at z=0z=0z=0, which the non-singularity hypothesis on ggg excludes; the conjecture asserts that at non-singular points such examples cannot occur. Even for linear equations the statement contains the Grothendieck–Katz conjecture, which is open in general.

Formalization scope

  • Power series are PowerSeries ℚ with the formal derivative; rational functions are the fraction field of MvPolynomial (Fin (n + 1)) ℚ, where variable 0 is zzz and variable i + 1 is f(i)f^{(i)}f(i).
  • The ODE hypothesis is existential: some representation g=p/qg=p/qg=p/q with qqq nonzero at the initial point and f(n)q(… )=p(… )f^{(n)}q(\dots)=p(\dots)f(n)q(…)=p(…) as power series. This non-singularity requirement is essential and must not be dropped.
  • Algebraicity is IsAlgebraic (Polynomial ℚ) f, i.e. over Q[z]\mathbb{Q}[z]Q[z] (equivalently over Q(z)\mathbb{Q}(z)Q(z)).
  • Z[1/N]\mathbb{Z}[1/N]Z[1/N] is the subalgebra of Q\mathbb{Q}Q generated by 1/N1/N1/N; since 1/0=01/0=01/0=0 in Lean, N=0N=0N=0 gives Z\mathbb{Z}Z.
  • ω\omegaω takes values in Z\mathbb{Z}Z; negative values impose no condition at that prime. Superlinearity is the limit ω(p)/p→∞\omega(p)/p\to\inftyω(p)/p→∞ along the primes.
  • The goal is a List.TFAE of the three conditions.

Useful infrastructure: formal derivatives and substitution for power series, algebraic power series and their coefficient arithmetic (Eisenstein), and ppp-adic valuations of coefficients. Formalizations of Eisenstein's theorem and of the special cases proved by Lam and Litt are welcome.

Selected references

  • Y. H. J. Lam, D. Litt, Algebraicity and integrality of solutions to differential equations, arXiv preprint, 2025. https://arxiv.org/abs/2501.13175
  • D. Litt, Problem 1, problems list. https://www.problemsilike.com/1
  • G. Eisenstein, Über eine allgemeine Eigenschaft der Reihen-Entwicklungen aller algebraischen Funktionen, Bericht der Königl. Preuss. Akademie der Wissenschaften zu Berlin, 1852.
  • Formal Conjectures project, FormalConjectures/LittProblems/1.lean. https://github.com/google-deepmind/formal-conjectures
6 thms2 active usersReviewed
🏆Completed
Dynamic ProgrammingDynamical SystemsOptimization·Captain: Lucas

Lindgren 2022: Dynamic-Programming Price Adjustment and Lyapunov StabilityResearch Paper

Motivation

In a Walrasian pure exchange economy, agents trade a fixed stock of lll commodities, and a price vector p∈Rlp\in\mathbb R^lp∈Rl is a general equilibrium when aggregate excess demand vanishes. Existence of equilibrium (Arrow–Debreu, 1954) says nothing about how prices reach it. The classical tâtonnement model of Samuelson (1947), dpi/ds=ciZi(p)dp_i/ds = c_i Z_i(p)dpi​/ds=ci​Zi​(p), is not derived from any optimization principle, and Scarf (1960) gave economies in which it is not globally stable; see also Smale's survey Dynamics in General Equilibrium Theory (JSTOR 1817235) and the chaotic tâtonnement examples of Bala–Majumdar (JSTOR 25054664).

Lindgren (doi:10.3390/analytics1010003) proposes instead that the economy as a whole chooses a price path by dynamic programming: it minimizes a running cost combining a quadratic transaction cost for price changes and the agents' aggregate minimal expenditure. From the resulting Hamilton–Jacobi–Bellman (HJB) equation the paper derives an evolution equation for the price velocity and a condition under which the value function acts as a Lyapunov function: the equilibrium is approached when price adjustments are large enough. This mission formalizes those derivations.

Setting

There are lll commodities and nnn agents. Prices are vectors p=(p1,…,pl)∈Rlp=(p_1,\dots,p_l)\in\mathbb R^lp=(p1​,…,pl​)∈Rl, and the paper's implicit summation xiyi=∑i=1lxiyix^iy_i=\sum_{i=1}^l x_iy_ixiyi​=∑i=1l​xi​yi​ is written ⟨x,y⟩\langle x,y\rangle⟨x,y⟩. Agent jjj has an expenditure function ej(p)e_j(p)ej​(p) (minimal cost of reaching a fixed utility level), and the market weighs agents with constants λj>0\lambda_j>0λj​>0; the aggregate expenditure is

E(p)=λjej(p)=∑j=1nλjej(p).E(p)=\lambda^je_j(p)=\sum_{j=1}^n\lambda_je_j(p).E(p)=λjej​(p)=j=1∑n​λj​ej​(p).

The economy controls the price velocity v=dp/dsv=dp/dsv=dp/ds and minimizes the cost functional (eq. (7))

∫tT(12m⟨v,v⟩+E(p)) ds,m>0,\int_t^T\Big(\tfrac12 m\langle v,v\rangle+E(p)\Big)\,ds,\qquad m>0,∫tT​(21​m⟨v,v⟩+E(p))ds,m>0,

whose value function is J(t,p)J(t,p)J(t,p). The Hamiltonian (eq. (8)) is

H(v)=12m⟨v,v⟩+E(p)+⟨∇J,v⟩,H(v)=\tfrac12 m\langle v,v\rangle+E(p)+\langle\nabla J,v\rangle ,H(v)=21​m⟨v,v⟩+E(p)+⟨∇J,v⟩,

the optimal policy (eq. (9)) is v=−1m∇Jv=-\tfrac1m\nabla Jv=−m1​∇J, and the HJB equation (eq. (10)) reads

∂J∂t=12m⟨∇J,∇J⟩−E(p).\frac{\partial J}{\partial t}=\frac1{2m}\langle\nabla J,\nabla J\rangle-E(p).∂t∂J​=2m1​⟨∇J,∇J⟩−E(p).

Here ∇\nabla∇ always denotes the gradient with respect to prices. Shephard's lemma identifies the Hicksian demand of agent jjj with hj=∇ejh^j=\nabla e_jhj=∇ej​. For the stability analysis the paper runs time forward, which reverses the sign of the HJB equation: ∂J/∂s=−12m⟨∇J,∇J⟩+E(p)\partial J/\partial s=-\frac1{2m}\langle\nabla J,\nabla J\rangle+E(p)∂J/∂s=−2m1​⟨∇J,∇J⟩+E(p).

Formalization targets

Goal — Lyapunov stability condition (Section 3)

If JJJ is C1C^1C1 and solves the time-reversed HJB equation, and the price path follows the optimal policy p˙(s)=v(s)=−1m∇J(s,p(s))\dot p(s)=v(s)=-\frac1m\nabla J(s,p(s))p˙​(s)=v(s)=−m1​∇J(s,p(s)), then on any interval [t,T][t,T][t,T] on which

E(p(s))<32 m ⟨v(s),v(s)⟩,E(p(s))<\tfrac32\,m\,\langle v(s),v(s)\rangle,E(p(s))<23​m⟨v(s),v(s)⟩,

the function s↦J(s,p(s))s\mapsto J(s,p(s))s↦J(s,p(s)) is strictly decreasing; if moreover J(T,p(T))=0J(T,p(T))=0J(T,p(T))=0, it is strictly positive on [t,T)[t,T)[t,T).

Milestones

  1. Eq. (4): under the normalization ⟨p,p⟩=1\langle p,p\rangle=1⟨p,p⟩=1, ⟨p,p˙⟩=0\langle p,\dot p\rangle=0⟨p,p˙​⟩=0.
  2. Eq. (9): for m>0m>0m>0, vvv minimizes HHH if and only if mv=−∇Jmv=-\nabla Jmv=−∇J.
  3. Eq. (10): the HJB equation −∂tJ=min⁡vH-\partial_tJ=\min_vH−∂t​J=minv​H takes the explicit form above.
  4. Eq. (12): for a C2C^2C2 solution of (10), v=−1m∇Jv=-\frac1m\nabla Jv=−m1​∇J satisfies
m∂vi∂t+12m ∇i⟨v,v⟩=∇iE.m\frac{\partial v_i}{\partial t}+\tfrac12 m\,\nabla_i\langle v,v\rangle=\nabla_iE .m∂t∂vi​​+21​m∇i​⟨v,v⟩=∇i​E.
  1. Eq. (14): with Shephard's lemma, the right-hand side becomes ∑jλjhij\sum_j\lambda_jh^j_i∑j​λj​hij​.
  2. Eq. (19): along the optimal path, dJds=E(p)−32m⟨v,v⟩\dfrac{dJ}{ds}=E(p)-\tfrac32 m\langle v,v\rangledsdJ​=E(p)−23​m⟨v,v⟩.

Significance

The paper's contribution is the claim that price dynamics derived from an optimization principle are nonlinear and only conditionally stable, with stability requiring sufficiently fast price changes; the author connects this to volatility clustering in financial time series. The derivations in the paper are formal calculations with the regularity of JJJ left implicit. Formalizing them pins down exactly which smoothness assumptions each step needs (for instance, eq. (12) uses equality of mixed partial derivatives, hence a C2C^2C2 value function), and which facts are imported from outside (the HJB equation itself, Shephard's lemma). The resulting statements are reusable calculus facts about HJB equations with quadratic control cost.

Difficulty

Each step is a short computation on paper; the formal difficulty is in the calculus infrastructure: partial derivatives of functions on R×Rl\mathbb R\times\mathbb R^lR×Rl, symmetry of second derivatives, the chain rule along a curve, and turning a pointwise negative derivative into strict monotonicity on a closed interval. The HJB equation is taken as a hypothesis on JJJ rather than derived from the definition of the value function, because the paper asserts it without proof and a rigorous derivation would require viscosity-solution theory.

Formalization scope

All declarations live in the namespace LindgrenPriceDynamics. Prices are functions Fin l → ℝ; partial derivatives are Fréchet derivatives applied to standard basis vectors, and time derivatives are one-variable derivatives in the time argument. The value function is a function J : ℝ → (Fin l → ℝ) → ℝ whose joint regularity is stated for the uncurried map on ℝ × (Fin l → ℝ). The standing assumption m>0m>0m>0 is kept; positivity of λj\lambda_jλj​ and eje_jej​ is not needed by any stated conclusion and is not imposed. Prices are not restricted to the positive orthant. The goal's large-velocity hypothesis is satisfiable (e.g. l=1l=1l=1, J=ap2+csJ=ap^2+csJ=ap2+cs, E=2a2p2/m+cE=2a^2p^2/m+cE=2a2p2/m+c with small c>0c>0c>0 on a bounded interval), so the goal is not vacuous.

Selected references

  • J. Lindgren, General Equilibrium with Price Adjustments — A Dynamic Programming Approach, Analytics 1 (2022) 27–34. https://doi.org/10.3390/analytics1010003
  • S. Smale, Dynamics in General Equilibrium Theory, American Economic Review 66 (1976) 288–294. https://www.jstor.org/stable/1817235
  • H. Scarf, Some Examples of Global Instability of the Competitive Equilibrium, International Economic Review 1 (1960) 157–172.
  • A. Mas-Colell, M. Whinston, J. Green, Microeconomic Theory, Oxford University Press, 1995.
  • V. Bala, M. Majumdar, Chaotic Tatonnement, Economic Theory 2 (1992) 437–445. https://www.jstor.org/stable/25054664
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AlgebraAnalysis·Captain: Lucas

Smale's Mean Value ConjectureOpen Problem

Motivation

The mean value problem, also called Smale's mean value conjecture, was posed by Stephen Smale in 1981 in his study of the complexity of root-finding algorithms for polynomials (Smale 1981). For a real differentiable function the mean value theorem produces, between two points, a point where the derivative equals a difference quotient. For a complex polynomial no such point need exist on a segment, and Smale asked for a substitute in which the special point is a critical point of the polynomial (a zero of its derivative). Estimates of this kind control how far Newton-type iterations can move, which is where Smale's original interest came from. The problem appears in lists of unsolved problems in mathematics, including Smale's own list of problems for the next century.

Timeline

  • 1981 — Smale poses the problem and proves the inequality below with constant K=4K = 4K=4 (Smale 1981). The example P(z)=zd−dzP(z) = z^d - dzP(z)=zd−dz shows that the constant cannot be smaller than d−1d\frac{d-1}{d}dd−1​ in degree ddd, so no constant below 111 works in all degrees.
  • 1989 — Tischler proves the inequality with the optimal constant K=d−1dK = \frac{d-1}{d}K=dd−1​ when all roots of PPP are real, and when all roots of PPP have the same absolute value (Tischler 1989).
  • 2007 — Conte, Fujikawa and Lakic prove K≤4d−1d+1K \le 4\frac{d-1}{d+1}K≤4d+1d−1​ (Conte–Fujikawa–Lakic 2007). Crane proves K<4−2.263dK < 4 - \frac{2.263}{\sqrt d}K<4−d​2.263​ for d≥8d \ge 8d≥8 (Crane 2007).
  • 2009 — Dubinin and Sugawa prove the reverse (dual) inequality with constant 1d 4d\frac{1}{d\,4^d}d4d1​ (Dubinin–Sugawa 2009); optimizing this lower bound is the dual mean value problem (Ng–Zhang 2016).

No absolute constant K<4K < 4K<4 is known that works in every degree.

Setting

Let PPP be a polynomial with complex coefficients of degree d≥2d \ge 2d≥2, and write P′P'P′ for its derivative. A critical point of PPP is a complex number ccc with P′(c)=0P'(c) = 0P′(c)=0; since d≥2d \ge 2d≥2, P′P'P′ is a nonconstant polynomial of degree d−1d-1d−1, so PPP has at least one and at most d−1d-1d−1 distinct critical points. Fix a complex number zzz that is not a critical point, P′(z)≠0P'(z) \ne 0P′(z)=0. For every critical point ccc we then have c≠zc \ne zc=z, and the difference quotient

P(z)−P(c)z−c\frac{P(z) - P(c)}{z - c}z−cP(z)−P(c)​

is well defined. The question is how small this quotient can be made, relative to ∣P′(z)∣|P'(z)|∣P′(z)∣, by choosing the critical point ccc well.

Formalization targets

Goal: Smale's mean value conjecture (K=1K = 1K=1)

For every complex polynomial PPP of degree d≥2d \ge 2d≥2 and every z∈Cz \in \mathbb Cz∈C with P′(z)≠0P'(z) \ne 0P′(z)=0 there is a critical point ccc of PPP with

∣P(z)−P(c)z−c∣≤∣P′(z)∣.\left| \frac{P(z) - P(c)}{z - c} \right| \le |P'(z)|.​z−cP(z)−P(c)​​≤∣P′(z)∣.

Stronger: the optimal constant

The same with ∣P′(z)∣|P'(z)|∣P′(z)∣ replaced by d−1d ∣P′(z)∣\frac{d-1}{d}\,|P'(z)|dd−1​∣P′(z)∣; the example zd−dzz^d - dzzd−dz shows this constant cannot be lowered.

Known results (milestones)

  1. Smale's inequality with K=4K = 4K=4.
  2. The extremal example P(z)=zd−dzP(z) = z^d - dzP(z)=zd−dz at z=0z = 0z=0, where every critical point gives exactly d−1d∣P′(0)∣\frac{d-1}{d}|P'(0)|dd−1​∣P′(0)∣, and its consequence that no constant K<1K < 1K<1 works in all degrees.
  3. Tischler's optimal inequality for polynomials with only real roots, and for polynomials whose roots all have the same absolute value.
  4. The Conte–Fujikawa–Lakic bound K≤4d−1d+1K \le 4\frac{d-1}{d+1}K≤4d+1d−1​.
  5. Crane's bound K<4−2.263dK < 4 - \frac{2.263}{\sqrt d}K<4−d​2.263​ for d≥8d \ge 8d≥8.
  6. The Dubinin–Sugawa dual inequality ∣P(z)−P(c)z−c∣≥∣P′(z)∣d 4d\left|\frac{P(z)-P(c)}{z-c}\right| \ge \frac{|P'(z)|}{d\,4^d}​z−cP(z)−P(c)​​≥d4d∣P′(z)∣​ for some critical point ccc.

Significance

The result itself. A positive answer gives a sharp, degree-independent mean value inequality for complex polynomials: for every non-critical point, some critical value is reachable along a chord whose slope is at most the local derivative. Bounds of this type feed into the analysis of Newton's method and of path-following root finders, and into the study of how critical values of a polynomial are distributed relative to its values. The conjecture is part of a family of open extremal problems on the geometry of critical points, alongside Sendov's conjecture.

Formalizing it. The goal and the optimal-constant form are open. The milestones are published theorems, none of which is known to have a machine-checked proof. Formalizing Smale's K=4K = 4K=4 bound and Tischler's special cases would put the classical tools of the subject (critical points of polynomials, univalent function estimates, root location) on a formal footing that later attempts can reuse.

Difficulty

The obvious strategies control the quotient through one critical point at a time: for instance, bounding ∣P(z)−P(c)∣|P(z) - P(c)|∣P(z)−P(c)∣ by integrating P′P'P′ along the segment from ccc to zzz. Such estimates lose a constant factor that depends on how the critical points are spread out, and the known uniform arguments all pass through distortion theorems for univalent functions, whose constants lead to KKK close to 444. Reaching K=1K = 1K=1 requires using all critical points simultaneously, and no argument doing this in every degree is known. The equality case zd−dzz^d - dzzd−dz, in which every critical point is equally bad, shows that any successful argument must be sharp for polynomials with maximally symmetric critical configurations.

Formalization scope

Polynomials are elements of ℂ[X] (Mathlib's Polynomial ℂ); the degree is natDegree, the derivative is Polynomial.derivative, evaluation is Polynomial.eval, and the roots of PPP are the multiset P.roots (counted with multiplicity). A critical point is a c : ℂ with P.derivative.eval c = 0. The absolute value is the norm ‖·‖ on ℂ, and the constants d−1d\frac{d-1}{d}dd−1​ and 4d−1d+14\frac{d-1}{d+1}4d+1d−1​ are computed in ℝ from the cast of natDegree.

Every statement assumes P′(z)≠0P'(z) \ne 0P′(z)=0. This is the standard normalization and is essential in Lean: division by zero returns 000, so without it the choice c=zc = zc=z would make the inequality trivially true whenever zzz is itself a critical point. With the hypothesis, every critical point ccc differs from zzz and the quotient is a genuine difference quotient.

Crane's bound is stated as the existence, for each degree d≥8d \ge 8d≥8, of a constant strictly below 4−2.263d4 - \frac{2.263}{\sqrt d}4−d​2.263​ that works for all polynomials of degree exactly ddd; this is equivalent to the best constant in degree ddd being strictly below that value.

A complete development needs basic facts on critical points of complex polynomials (existence, the Gauss–Lucas theorem), and, for the classical bounds, results from the theory of univalent functions such as the Koebe quarter theorem and coefficient estimates. These are reusable well beyond this mission. Contributions of any milestone, of supporting lemmas, and of partial results in fixed small degree are welcome.

Selected references

  • S. Smale, The fundamental theorem of algebra and complexity theory, Bull. Amer. Math. Soc. (N.S.) 4 (1981), 1–36. https://doi.org/10.1090/S0273-0979-1981-14858-8
  • D. Tischler, Critical points and values of complex polynomials, J. Complexity 5 (1989), 438–456. https://doi.org/10.1016/0885-064X(89)90019-8
  • A. Conte, E. Fujikawa, N. Lakic, Smale's mean value conjecture and the coefficients of univalent functions, Proc. Amer. Math. Soc. 135 (2007), 3295–3300. https://doi.org/10.1090/S0002-9939-07-08861-2
  • E. Crane, A bound for Smale's mean value conjecture for complex polynomials, Bull. London Math. Soc. 39 (2007), 781–791. https://doi.org/10.1112/blms/bdm063
  • V. Dubinin, T. Sugawa, Dual mean value problem for complex polynomials, Proc. Japan Acad. Ser. A 85 (2009), 135–137. https://arxiv.org/abs/0906.4605
  • T.-W. Ng, Y. Zhang, Smale's mean value conjecture for finite Blaschke products, J. Anal. 24 (2016), 331–345. https://arxiv.org/abs/1609.00170
  • Wikipedia, Mean value problem. https://en.wikipedia.org/w/index.php?title=Mean_value_problem&oldid=1374678764
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Linear OptimizationNumerical AnalysisTheoretical Computer Science·Captain: Lucas

Extended Smale's 9th Problem I: no algorithm computes K digits of LP minimisersResearch Paper

Motivation

Linear programming is usually described as "solvable in polynomial time", but that statement is about rational inputs given exactly. In Smale's list of problems for the 21st century (Smale 1998), Problem 9 asks for a polynomial-time algorithm over the reals deciding the feasibility of Ax≥yAx \ge yAx≥y, and Smale explicitly calls for "models which process approximate inputs and which permit round-off computations". Real data such as 2\sqrt 22​, entries of a discrete cosine transform, or even 1/31/31/3 in floating point can only be accessed approximately.

Bastounis, Hansen and Vlačić pose the extended Smale's 9th problem: in a model where the algorithm can only query approximations of the input to any requested accuracy, can one compute minimisers of linear programming, basis pursuit and Lasso to KKK correct digits? Their Main Theorem I (Theorem 3.4) shows that the answer depends on KKK in a sharp way: for a suitable class of well-conditioned, bounded inputs, no algorithm at all (not only no efficient one) produces KKK correct digits, while K−1K-1K−1 digits are computable (but not in bounded time) and K−2K-2K−2 digits are computable in polynomial time.

This mission targets the first, impossibility, half of Theorem 3.4(i) for linear programming.

Setting

Linear program. For A∈Rm×NA \in \mathbb R^{m\times N}A∈Rm×N, y∈Rmy\in\mathbb R^my∈Rm and c=1N=(1,…,1)c = \mathbf 1_N=(1,\dots,1)c=1N​=(1,…,1), the solution set is

Ξ(y,A)=argmin⁡x∈RN ⟨x,c⟩subject toAx=y, x≥0.\Xi(y,A) = \operatorname*{argmin}_{x\in\mathbb R^N}\ \langle x, c\rangle \quad\text{subject to}\quad Ax = y,\ x\ge 0 .Ξ(y,A)=x∈RNargmin​ ⟨x,c⟩subject toAx=y, x≥0.

It is a subset of MN=RNM_N = \mathbb R^NMN​=RN with the ℓp\ell^pℓp norm, p∈[1,∞]p\in[1,\infty]p∈[1,∞]. An input is a pair ι=(y,A)\iota = (y,A)ι=(y,A), and the evaluations of ι\iotaι are its coordinates yiy_iyi​ and entries AijA_{ij}Aij​.

Extended model (Δ1\Delta_1Δ1​-information). Let Dn={k2−n:k∈Z}D_n = \{k2^{-n} : k\in\mathbb Z\}Dn​={k2−n:k∈Z}. An oracle representation of ι\iotaι is a family ι~=(ι~j,n)\tilde\iota = (\tilde\iota_{j,n})ι~=(ι~j,n​), indexed by evaluations jjj and accuracies n=1,2,…n = 1,2,\dotsn=1,2,…, with ι~j,n∈Dn+iDn\tilde\iota_{j,n}\in D_n + iD_nι~j,n​∈Dn​+iDn​ and ∣ι~j,n−fj(ι)∣≤2−n|\tilde\iota_{j,n} - f_j(\iota)|\le 2^{-n}∣ι~j,n​−fj​(ι)∣≤2−n. An algorithm must succeed on every oracle representation of every input.

General algorithm. To make impossibility results independent of the machine model, the paper uses general algorithms (Definition 9.3): a map Γ\GammaΓ from inputs to M∪{NH}M\cup\{\mathrm{NH}\}M∪{NH} (NH\mathrm{NH}NH = no output) together with a nonempty set ΛΓ(ι)\Lambda_\Gamma(\iota)ΛΓ​(ι) of evaluations read on ι\iotaι. This set is finite whenever Γ\GammaΓ halts. The output is determined by the values read, and any input that agrees on those values reads the same set. Turing machines and BSS machines with an oracle are special cases; general algorithms can even solve the halting problem.

Error and breakdown epsilon. The error is dist⁡(Γ(ι),Ξ(ι))=inf⁡ξ∈Ξ(ι)d(Γ(ι),ξ)\operatorname{dist}(\Gamma(\iota),\Xi(\iota)) = \inf_{\xi\in\Xi(\iota)} d(\Gamma(\iota),\xi)dist(Γ(ι),Ξ(ι))=infξ∈Ξ(ι)​d(Γ(ι),ξ), with distance ∞\infty∞ from NH\mathrm{NH}NH. The strong breakdown epsilon εBs\varepsilon_B^sεBs​ is the supremum of all ε≥0\varepsilon\ge 0ε≥0 such that every general algorithm has error >ε>\varepsilon>ε on some input (Definition 9.17).

Formalization targets

Goal: Theorem 3.4(i), deterministic part, for LP

For every integer K≥1K\ge1K≥1, all dimensions 4≤m<N4\le m<N4≤m<N and every p∈[1,∞]p\in[1,\infty]p∈[1,∞] there is a nonempty class Ωm,N\Omega_{m,N}Ωm,N​ of inputs (y,A)(y,A)(y,A) with nonempty solution sets, ∥y∥∞≤2\|y\|_\infty\le 2∥y∥∞​≤2 and ∥A∥max⁡=1\|A\|_{\max}=1∥A∥max​=1, such that

¬ ∃ Γ general algorithm on oracle representations:∀ ι~,  dist⁡ℓp(Γ(ι~), Ξ(ι))≤10−K.\neg\,\exists\,\Gamma\ \text{general algorithm on oracle representations}:\quad \forall\,\tilde\iota,\ \ \operatorname{dist}_{\ell^p}\big(\Gamma(\tilde\iota),\,\Xi(\iota)\big)\le 10^{-K}.¬∃Γ general algorithm on oracle representations:∀ι~,  distℓp​(Γ(ι~),Ξ(ι))≤10−K.

Milestones

  1. Lemma 11.1: the explicit solution sets of the LP inputs (y1e1,A(α,β,m,N))(y_1e_1, A(\alpha,\beta,m,N))(y1​e1​,A(α,β,m,N)).
  2. Proposition 10.5 (ii), deterministic part: two input sequences that converge in evaluation to a common input and whose solutions stay κ\kappaκ apart force εBs≥κ/2\varepsilon_B^s\ge\kappa/2εBs​≥κ/2 for a suitable choice of Δ1\Delta_1Δ1​-information.
  3. §9.6, (i) ⇒ (ii): a lower bound on εBs\varepsilon_B^sεBs​ for one specific Δ1\Delta_1Δ1​-information transfers to the problem with all oracle representations.
  4. Proposition 9.32 (i) (deterministic consequence via Proposition 10.1): εBs>10−K\varepsilon_B^s>10^{-K}εBs​>10−K for LP on a suitable Ωm,N\Omega_{m,N}Ωm,N​.

Significance

The theorem shows that for LP with inexact input, being non-computable in Turing's sense does not rule out a finer complexity theory. The paper builds a "KKK / K−1K-1K−1 / K−2K-2K−2 digits" classification on this. It also explains why established solvers can return wrong answers with a success flag on small, well-conditioned LPs (§4 of the paper), and it bears on computer-assisted proofs that rely on inexact LP, such as the Flyspeck proof of the Kepler conjecture.

The result is proved on paper. As far as the proposer knows, it has not been machine-checked. This mission formalizes the deterministic impossibility part for LP and puts in place reusable infrastructure: general algorithms, breakdown epsilons and Δ1\Delta_1Δ1​-information. That infrastructure is the base for later missions on the randomised parts of Theorem 3.4(i)–(ii), the weak breakdown epsilon (iii), the exit-flag theorem (Theorem 5.1), and basis pursuit and Lasso.

Difficulty

The obvious objection is that LP is in P for rational inputs, so some rounding scheme ought to work. It fails because an algorithm must halt after reading finitely many approximations. Two inputs that agree to that accuracy but have minimisers far apart then receive the same output. Setting this up needs a notion of algorithm strong enough to cover every computational model, a precise Δ1\Delta_1Δ1​-information model in which the adversary controls the approximations, and explicit LP geometry in which an arbitrarily small perturbation of AAA moves the minimiser by a fixed amount.

Formalization scope

  • Inputs are (y,A)∈(Fin m→R)×Matrix(Fin m)(Fin N) R(y,A)\in(\mathrm{Fin}\,m\to\mathbb R)\times\mathrm{Matrix}(\mathrm{Fin}\,m)(\mathrm{Fin}\,N)\,\mathbb R(y,A)∈(Finm→R)×Matrix(Finm)(FinN)R. Evaluations are complex-valued, as in Definition 9.2. Outputs lie in PiLp p (Fin N → ℝ).
  • A general algorithm is a structure with an output run : Ω → Option M (none = NH) and a read set queried, satisfying the axioms (i)–(iii) of Definition 9.3.
  • Errors take values in [0,∞][0,\infty][0,∞] (ℝ≥0∞), and the error of NH is ∞\infty∞. The infimum over an empty solution set is ∞\infty∞. The goal also requires nonempty solution sets, so no junk value enters.
  • Oracle accuracies are indexed by n∈{1,2,… }n\in\{1,2,\dots\}n∈{1,2,…} (ℕ+). An oracle input is stored as a pair (input, oracle family), and algorithms can read only the oracle family.
  • Out of scope: randomised algorithms, the positive statements (iii)–(iv), runtime, and the condition-number bounds Cond(AA∗)≤3.2\mathrm{Cond}(AA^*)\le3.2Cond(AA∗)≤3.2, CFP≤4C_{FP}\le4CFP​≤4, Cond(Ξ)≤179\mathrm{Cond}(\Xi)\le179Cond(Ξ)≤179.

Selected references

  • A. Bastounis, A. C. Hansen, V. Vlačić, The extended Smale's 9th problem — On computational barriers and paradoxes in estimation, regularisation, computer-assisted proofs, and learning, preprint (2021).
  • S. Smale, Mathematical problems for the next century, Math. Intelligencer 20 (1998). https://doi.org/10.1007/BF03025291
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🏆Completed
Group Theory·Captain: dbenbenn

Monod: groups of piecewise projective homeomorphisms are non-amenable without free subgroupsResearch Paper

This mission formalizes N. Monod, Groups of piecewise projective homeomorphisms, Proceedings of the National Academy of Sciences 110 (2013) 4524–4527, doi:10.1073/pnas.1218426110: the groups H(A)H(A)H(A) of piecewise projective homeomorphisms of the line are non-amenable and have no free subgroups whenever A≠ZA \neq \mathbf{Z}A=Z.

Motivation

The paper opens with the Banach–Tarski paradox and von Neumann's notion of amenability: "Tarski readily proved that amenability is the only obstruction to paradoxical decompositions. However, the known paradoxes relied more prosaically on the existence of non-abelian free subgroups. Therefore, the main open problem in the subject remained for half a century to find non-amenable groups without free subgroups" (p. 1). That problem, the so-called von Neumann conjecture, was answered by Ol'shanskii around 1980, with Tarski monsters. Monod's groups give "straightforward torsion-free counter-examples", "so simple that many additional properties can be established" (p. 1).

Monod's groups are close relatives of Thompson's groups: Thurston's model identifies Thompson's group FFF with piecewise PSL2(Z)\mathrm{PSL}_2(\mathbf{Z})PSL2​(Z) maps of the line with rational breakpoints (p. 2). Whether FFF is amenable is a notorious open problem, and whether H(Z)H(\mathbf{Z})H(Z) is amenable is Monod's Problem 12 (p. 2).

Timeline

  • 1914–1929. Hausdorff's paradox (1914); Banach–Tarski (1924); von Neumann introduces amenable groups (1929); Tarski characterizes amenability by the absence of paradoxical decompositions.
  • 1950s. Day's classes; the question whether every non-amenable group contains a free subgroup of rank two becomes attached to von Neumann's name.
  • c. 1965–1975. Thompson's groups FFF, TTT, VVV; Thurston's piecewise projective models of FFF and TTT.
  • 1979–1982. Ol'shanskii proves Tarski monsters non-amenable; Adyan does the same for free Burnside groups.
  • 1985. Brin–Squier: groups of piecewise linear homeomorphisms of the line have no free subgroups.
  • 2003. Ol'shanskii–Sapir: finitely presented non-amenable groups without free subgroups.
  • 2013. Monod: the piecewise projective groups H(A)H(A)H(A) (this paper).
  • 2016. Lodha–Moore: a finitely presented subgroup of Monod's group, non-amenable and without free subgroups.

Setting

The projective line P1\mathbf{P}^1P1 is OnePoint ℝ, on which SL2(A)\mathrm{SL}_2(A)SL2​(A) acts through GL2(R)\mathrm{GL}_2(\mathbf{R})GL2​(R) by Möbius transformations (mob, using Mathlib's action on OnePoint). For a subring AAA of R\mathbf{R}R (A : Subring ℝ; Z\mathbf{Z}Z is ⊥, R\mathbf{R}R is ⊤), P A is PAP_APA​, the set of fixed points of hyperbolic elements (trace of absolute value greater than 222).

A homeomorphism of P1\mathbf{P}^1P1 is piecewise in PSL2(A)\mathrm{PSL}_2(A)PSL2​(A) with breakpoints in EEE (IsPiecewiseProjOn A E f) when, off some finite subset of EEE, it agrees near every point with a Möbius transformation from SL2(A)\mathrm{SL}_2(A)SL2​(A). Monod's GGG (Gpp) is the group generated by the homeomorphisms piecewise in PSL2(R)\mathrm{PSL}_2(\mathbf{R})PSL2​(R), with breakpoints anywhere, and HHH (Hpp) is its stabilizer of ∞\infty∞ (fixInf). For a subring AAA, G(A)G(A)G(A) (G A) is the subgroup of GGG generated by its elements that are piecewise in PSL2(A)\mathrm{PSL}_2(A)PSL2​(A) with breakpoints in PAP_APA​ (IsPiecewiseProj A), and H(A)H(A)H(A) (H A) is its stabilizer of ∞\infty∞; H(Z)H(\mathbf{Z})H(Z) is H ⊥. GRat is the subgroup of GGG generated by its elements piecewise in PSL2(Z)\mathrm{PSL}_2(\mathbf{Z})PSL2​(Z) with breakpoints in Q∪{∞}\mathbf{Q} \cup \{\infty\}Q∪{∞}, and HRat its stabilizer of ∞\infty∞: the rational-breakpoint variants of G(Z)G(\mathbf{Z})G(Z) and H(Z)H(\mathbf{Z})H(Z) (p. 2).

Amenability is Garrido.IsAmenable (a finitely additive left-invariant probability measure on all subsets), and "no non-abelian free subgroup" is Chou.NoFreeSubgroupOfRankTwo; both are published definitions, in the bundles Garrido_Amenability and Chou_Classes. Co-amenable subgroups (IsCoamenable), inner amenability (IsInnerAmenable) and pointwise stabilizers (fixSubgroup), all on p. 3, are defined in the bundle in the same style.

A relation R⊆X×XR \subseteq X \times XR⊆X×X is amenable for a measure μ\muμ (IsAmenableRel μ R, p. 2) when it has a left invariant mean in the sense of Connes–Feldman–Weiss: a positive, unital map from bounded measurable functions on RRR to functions on XXX, linear up to μ\muμ-null sets and invariant under the partial transformations of RRR. volP1 is the Lebesgue measure class on P1\mathbf{P}^1P1.

Target

The goal is Theorem 1, "The group H(A)H(A)H(A) is non-amenable if A≠ZA \neq \mathbf{Z}A=Z" (p. 1), introduced as "the main result of this article". The proof (p. 2) passes to a countable dense subring A′A'A′ of AAA, compares the orbits of H(A′)H(A')H(A′) and PSL2(A′)\mathrm{PSL}_2(A')PSL2​(A′) on P1∖{∞}\mathbf{P}^1 \setminus \{\infty\}P1∖{∞} (Proposition 9), and concludes from two facts about measured equivalence relations: the orbit relation of an amenable group's action is amenable, and, by a theorem of Carrière and Ghys, the orbit relation of PSL2(A′)\mathrm{PSL}_2(A')PSL2​(A′) on P1\mathbf{P}^1P1 is not.

The milestones are, in the paper's order: G(A)G(A)G(A) consists exactly of the elements of GGG piecewise in PSL2(A)\mathrm{PSL}_2(A)PSL2​(A) with breakpoints in PAP_APA​; H=H(R)H = H(\mathbf{R})H=H(R); HHH preserves orientation, is left-orderable and torsion-free; Proposition 9; the countable dense subring; the orbit relation of a measurable action of an amenable group is amenable; the orbit relation of PSL2(A)\mathrm{PSL}_2(A)PSL2​(A) on P1\mathbf{P}^1P1 is not amenable (Carrière–Ghys, external); Lemma 13 and Theorem 14 leading to Theorem 2 (HHH has no free subgroups); Corollary 3; Proposition 6 (bi-orderability); Lemma 16, Proposition 7 (co-amenability of pointwise stabilizers), Proposition 15 and Proposition 5 (inner amenability); and Thurston's identification of the rational-breakpoint variants of H(Z)H(\mathbf{Z})H(Z) and G(Z)G(\mathbf{Z})G(Z) with FFF and TTT.

Significance

The result. Theorem 1 and Theorem 2 together make H(A)H(A)H(A), for instance A=Z[2]A = \mathbf{Z}[\sqrt 2]A=Z[2​], a torsion-free counterexample to the von Neumann conjecture, with finitely generated examples (Corollary 3). The groups are concrete enough to carry many further properties (Propositions 5–7).

Formalizing it. Nothing on amenability of groups of homeomorphisms of the line, or on measured equivalence relations, is in Mathlib. Amenability and Følner's theorem are on this platform from Garrido I, the Banach–Tarski paradox from Garrido II, Brin–Squier's theorem from its own mission, and Thompson's FFF and TTT (CannonFloydParry, CannonFloydParry_T) from the Cannon–Floyd–Parry missions.

Difficulty

The algebraic half, Theorem 2 and Propositions 5–9, follows Brin–Squier and elementary dynamics on the circle. The analytic half is the passage through measured equivalence relations in the proof of Theorem 1. The mission defines amenability of a relation as Connes–Feldman–Weiss do, by an invariant mean valued in L∞L^\inftyL∞, which is the form under which an amenable group's orbit relation is amenable without extra set-theoretic hypotheses. The step taken from the literature, that the orbit relation of PSL2(A)\mathrm{PSL}_2(A)PSL2​(A) on P1\mathbf{P}^1P1 is not amenable for AAA countable and dense, rests on Carrière–Ghys's theorem and on Zimmer's theory of amenable actions (Adams–Elliott–Giordano). The milestone is proved (Monod.not_isAmenableRel_mob) by an elementary route that needs neither: a ping-pong argument in SL2(A)\mathrm{SL}_2(A)SL2​(A) that contradicts an invariant mean directly.

What is left out

  • The second sentence of Proposition 6 (no non-trivial homomorphism from a Kazhdan group) and Proposition 8 (actions on CAT(0) spaces): property (T) and CAT(0) spaces are not in Mathlib.
  • Proposition 4 (L2L^2L2-Betti numbers), the remarks on group laws, on the Dixmier problem and on bounded cohomology.
  • Remarks 10 and 11, which discuss alternative proofs of the step taken from Carrière–Ghys.

Formalization scope

  • P1\mathbf{P}^1P1 is OnePoint ℝ and PSL2(A)\mathrm{PSL}_2(A)PSL2​(A) acts through Matrix.SpecialLinearGroup (Fin 2) A; since −1-1−1 acts trivially the orbits are those of PSL2(A)\mathrm{PSL}_2(A)PSL2​(A).
  • "Piecewise with finitely many pieces, each an interval" is stated locally: off a finite set of breakpoints, fff agrees near each point with one Möbius transformation. Pieces then extend over arcs because two Möbius maps agreeing near a point agree everywhere.
  • The groups are subgroups of the homeomorphism group of OnePoint ℝ, each defined as the subgroup generated by the maps the paper describes; the milestones state that G(A)G(A)G(A) is exactly its set of such maps and that G=G(R)G = G(\mathbf{R})G=G(R).
  • An amenable measured equivalence relation (p. 2) is one with a left invariant mean in the sense of Connes–Feldman–Weiss (an operator from L∞L^\inftyL∞ of the relation to L∞(X,μ)L^\infty(X, \mu)L∞(X,μ), their Definition 6), as in Schmidt, whom the paper cites. The paper describes it as a measurable assignment of means on the orbits, the motivating form in Connes–Feldman–Weiss; for that form, "an amenable group's action produces an amenable relation" is known only assuming CH. P1\mathbf{P}^1P1 carries its Borel σ-algebra and the Lebesgue measure class (volP1).
  • "Metabelian" is the vanishing of the second derived subgroup, and "contains a free abelian group of rank two" is an injective homomorphism from Z2\mathbf{Z}^2Z2.
  • Reused platform items, which solutions may import: the amenability and free-subgroup definitions (Garrido, Chou), Brin–Squier's Theorem 3.1, and Thompson's FFF and TTT (Cannon–Floyd–Parry).

Selected references

  • N. Monod, Groups of piecewise projective homeomorphisms, Proc. Natl. Acad. Sci. USA 110 (2013) 4524–4527. doi:10.1073/pnas.1218426110
  • Y. Carrière, É. Ghys, Relations d'équivalence moyennables sur les groupes de Lie, C. R. Acad. Sci. Paris Sér. I Math. 300 (1985) 677–680 (no DOI).
  • 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
  • K. Schmidt, Algebraic ideas in ergodic theory, CBMS Regional Conference Series in Mathematics 76, AMS (1990) (a book; no DOI).
  • M. G. Brin, C. C. Squier, Groups of piecewise linear homeomorphisms of the real line, Invent. Math. 79 (1985) 485–498. doi:10.1007/BF01388519
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Group Theory·Captain: dbenbenn

Is Thompson's group F amenable? (Geoghegan's conjecture)Open Problem

This mission formalizes Geoghegan's conjecture that Thompson's group FFF is not amenable, in the form stated by Cannon, Floyd and Parry, Introductory notes on Richard Thompson's groups, L'Enseignement Math. (2) 42 (1996), §4, p. 227 (doi:10.5169/seals-87877), together with the landmark results of the literature on the question.

Motivation

A discrete group is amenable when it carries a finitely additive, translation-invariant probability measure on all of its subsets. Groups containing a non-abelian free subgroup are not amenable, and the question whether every non-amenable group contains one (the von Neumann problem) made Thompson's group FFF the first natural candidate for a counterexample: it contains no non-abelian free subgroup, and it is not elementary amenable. Geoghegan conjectured in 1979 that FFF is not amenable; several announced solutions in each direction did not survive. In 2026 OpenAI released a proof that FFF is not amenable, with a Lean formalization; adapted to this mission's definitions, it is the solution of the goal.

Timeline.

  • 1965: Richard Thompson defines the groups FFF, TTT and VVV (Cannon–Floyd–Parry, p. 215).
  • 1979: Geoghegan conjectures that FFF contains no non-abelian free subgroup and is not amenable (Cannon–Floyd–Parry, p. 227).
  • 1985: Brin and Squier prove that FFF contains no non-abelian free subgroup (doi:10.1007/BF01388519).
  • 1996: Cannon, Floyd and Parry prove, using Chou's work on elementary amenable groups, that FFF is not elementary amenable (Theorem 4.10).
  • 2009–2014: announced proofs of amenability (Shavgulidze, 2009; Moore, 2012) and of non-amenability (Akhmedov, 2009; Beklaryan, 2011; Wajnryb–Witowicz, 2014) are withdrawn by their authors or found to contain serious errors.
  • 2013: Moore proves that if FFF is amenable, its Følner sets grow at least like a tower of exponentials (doi:10.4171/GGD/201).
  • 2013: Monod introduces the groups H(A)H(A)H(A) of piecewise-projective homeomorphisms of the line, proves that they have no non-abelian free subgroup and are not amenable for every subring A≠ZA \ne \mathbf ZA=Z of R\mathbf RR, and asks whether H(Z)H(\mathbf Z)H(Z) is amenable (Problem 12) (doi:10.1073/pnas.1218426110).
  • 2015: Juschenko, Matte Bon, Monod and de la Salle introduce extensive amenability of group actions, and prove that a subgroup of Monod's group of piecewise-projective homeomorphisms of the line is amenable if and only if its action on the line is extensively amenable (Theorem 6.4; arXiv 2015; published 2018, doi:10.1017/etds.2016.32).
  • 2017: Kaimanovich proves that random walks on FFF with finitely supported, strictly non-degenerate step distributions have non-trivial Poisson boundary (doi:10.1017/9781316576571.013).
  • 2019: Chornyi shows that FFF is amenable if and only if its action on the dyadic rationals in (0,1)(0,1)(0,1) is extensively amenable (arXiv:1907.01440).
  • 2019: Kim, Koberda and Lodha show that large powers of two homeomorphisms of the line with overlapping supports generate a copy of FFF (doi:10.24033/asens.2397).
  • 2021: Stankov records, from Kim–Koberda–Lodha, that H(Z)H(\mathbf Z)H(Z) contains a copy of FFF, so that amenability of H(Z)H(\mathbf Z)H(Z) would imply amenability of FFF (doi:10.1017/etds.2019.76).
  • 2023: Monod shows that the Thompson group HQ(Z)≅FH_{\mathbf Q}(\mathbf Z) \cong FHQ​(Z)≅F is not co-amenable in the group HQ(Q)H_{\mathbf Q}(\mathbf Q)HQ​(Q) (doi:10.4171/ggd/883).
  • 2023: Guba's survey records that "the famous problem about amenability of FFF remains open" (doi:10.46298/jgcc.2023.15.1.11315).
  • 2026: OpenAI proves that FFF is not amenable: a Lipschitz self-map of the Hilbert ball with no approximate fixed point (Benyamini–Sternfeld), composed with a recursive colouring of dyadic partitions that FFF transports exactly, gives a uniform lower bound on the Følner ratios of FFF. The proof comes with a Lean formalization (Thompson's group F is nonamenable, September 23, 2026, github.com/openai/math).

Setting

Let UI be the unit interval [0,1][0,1][0,1]. Thompson's group FFF (CannonFloydParry.F) is the group, under composition, of the order-preserving homeomorphisms of [0,1][0,1][0,1] that are piecewise linear with finitely many breakpoints, every breakpoint a dyadic rational k/2nk/2^nk/2n and every slope a power of 222. It is generated by two elements and finitely presented (Cannon–Floyd–Parry, Corollary 2.6 and Theorem 3.4).

A mean on a set SSS is a function mmm from the subsets of SSS to [0,∞][0,\infty][0,∞] with m(∅)=0m(\emptyset) = 0m(∅)=0, m(A∪B)=m(A)+m(B)m(A \cup B) = m(A) + m(B)m(A∪B)=m(A)+m(B) for disjoint A,BA, BA,B, and m(S)=1m(S) = 1m(S)=1. A group GGG is amenable (Garrido.IsAmenable G) when it carries a mean with m(gA)=m(A)m(gA) = m(A)m(gA)=m(A) for all g∈Gg \in Gg∈G and A⊆GA \subseteq GA⊆G, where gA={ga:a∈A}gA = \{ga : a \in A\}gA={ga:a∈A}. This is equivalent to the definition Cannon, Floyd and Parry give on p. 227, whose means take values in [0,1][0,1][0,1].

The milestones use four further notions, defined precisely in the definitions item and in their own statements:

  • A finite set A⊆GA \subseteq GA⊆G is ε\varepsilonε-Følner for a finite Γ⊆G\Gamma \subseteq GΓ⊆G when ∑γ∈Γ∣γA△A∣<ε∣A∣\sum_{\gamma\in\Gamma}|\gamma A \mathbin{\triangle} A| < \varepsilon|A|∑γ∈Γ​∣γA△A∣<ε∣A∣; by Følner's criterion, GGG is amenable exactly when it has such sets for every ε>0\varepsilon > 0ε>0.
  • A finitely supported probability measure μ\muμ on GGG drives a random walk; μ\muμ is strictly non-degenerate when its support generates GGG as a semigroup, and the walk is Liouville when every bounded μ\muμ-harmonic function, f(g)=∑hμ(h)f(gh)f(g) = \sum_h \mu(h) f(gh)f(g)=∑h​μ(h)f(gh), is constant.
  • An action of GGG on a set XXX is extensively amenable when the finite subsets of XXX carry a GGG-invariant mean that, for each finite E0⊆XE_0 \subseteq XE0​⊆X, gives full weight to the finite sets containing E0E_0E0​.
  • For a subring AAA of R\mathbf RR, Monod's group H(A)H(A)H(A) consists of the homeomorphisms of the real line that are piecewise projective, x↦(ax+b)/(cx+d)x \mapsto (ax+b)/(cx+d)x↦(ax+b)/(cx+d) with (abcd)∈SL2(A)\left(\begin{smallmatrix} a & b \\ c & d \end{smallmatrix}\right) \in \mathrm{SL}_2(A)(ac​bd​)∈SL2​(A), with finitely many breakpoints, each a fixed point of a hyperbolic element of SL2(A)\mathrm{SL}_2(A)SL2​(A). HB(A)H_B(A)HB​(A) allows breakpoints in a set BBB instead; HQ(Z)H_{\mathbf Q}(\mathbf Z)HQ​(Z) is isomorphic to FFF (Thurston). A subgroup KKK of JJJ is co-amenable when J/KJ/KJ/K carries a JJJ-invariant mean.

Formalization targets

Goal: Geoghegan's conjecture

¬ IsAmenable(F).\neg\,\mathrm{IsAmenable}(F).¬IsAmenable(F).

The question was open until 2026. OpenAI's proof of the conjecture (see the timeline), transferred to CannonFloydParry.F and Garrido.IsAmenable, proves this statement.

Landmarks

The milestones are results from the literature, stated as their sources state them: FFF has no non-abelian free subgroup (Cannon–Floyd–Parry, Corollary 4.9) and is not elementary amenable (Theorem 4.10), and Følner's criterion, all three already proved and linked as references; Moore's tower lower bound on Følner sets of FFF; Kaimanovich's theorem that random walks on FFF with finitely supported strictly non-degenerate steps are not Liouville; Chornyi's reformulation of amenability of FFF as extensive amenability of its action on the dyadic rationals; Stankov's embedding of FFF into Monod's H(Z)H(\mathbf Z)H(Z); Monod's theorem that HQ(Z)≅FH_{\mathbf Q}(\mathbf Z) \cong FHQ​(Z)≅F is not co-amenable in HQ(Q)H_{\mathbf Q}(\mathbf Q)HQ​(Q); and the theorem of Juschenko, Matte Bon, Monod and de la Salle that a subgroup of Monod's group of piecewise-projective homeomorphisms of the line is amenable if and only if its action on the line is extensively amenable.

A second open statement

Monod's Problem 12 asks whether H(Z)H(\mathbf Z)H(Z) is amenable; it is stated as ¬ Garrido.IsAmenable (Monod.H ⊥), where ⊥ is the smallest subring of R\mathbf RR, namely Z\mathbf ZZ; this is parallel to the goal. Through Stankov's embedding, the proof of the goal proves it. By the theorem of Juschenko, Matte Bon, Monod and de la Salle, it is equivalent to the statement that the action of H(Z)H(\mathbf Z)H(Z) on the line is not extensively amenable; that theorem is proved on this platform, through the germ-groupoid theorem of Juschenko, Nekrashevych and de la Salle (GermGroupoid.isAmenable_of_isExtensivelyAmenableOn), and for the subgroups of H(Z)H(\mathbf Z)H(Z) also in a sharper form, with extensive amenability on the set of possible breakpoints only (the breakpoint criterion).

Significance

The result. A proof of the conjecture would make FFF a finitely presented, torsion-free, non-amenable group with no non-abelian free subgroup, with a concrete description as a group of homeomorphisms of the interval. A disproof would make FFF an amenable group that is not elementary amenable, and by Moore's theorem one whose Følner sets are at least tower-sized.

Formalizing it. Corollary 4.9 and Theorem 4.10 of Cannon–Floyd–Parry are formalized and proved on this platform and enter as references. Chornyi's corollary is proved here; its "if" direction is proved directly, by establishing the case that Chornyi applies of the Juschenko–Matte Bon–Monod–de la Salle criterion. Moore's theorem is formalized and published together with the lemmas of its proof, and the milestone here has a solution that reduces it to that statement. Kaimanovich's theorem, Stankov's embedding, Monod's 2023 theorem and the theorem of Juschenko, Matte Bon, Monod and de la Salle are proved here as well, the last through the germ-groupoid theorem of Juschenko, Nekrashevych and de la Salle (GermGroupoid.isAmenable_of_isExtensivelyAmenableOn). The definitions of Følner sets, harmonic functions on groups and extensive amenability are reusable beyond this mission.

Difficulty

The obstructions to amenability that settle the question for most groups are absent here: FFF has no non-abelian free subgroup, and its elementary structure is well understood. In the other direction, the usual constructions of invariant means fail: by Moore's theorem any Følner set of FFF is at least tower-sized, so no explicit search can exhibit one, and by Kaimanovich's theorem the finitely supported random walks on FFF are not Liouville, so the random-walk route to amenability through a trivial Poisson boundary is closed.

Formalization scope

Lean representation and conventions.

  • FFF is a subgroup of the order isomorphisms of UI; H(A)H(A)H(A) and HB(A)H_B(A)HB​(A) are subgroups of the homeomorphisms of OnePoint ℝ. Groups of maps multiply by composition, (fg)(x)=f(g(x))(fg)(x) = f(g(x))(fg)(x)=f(g(x)); statements from sources that write the product in the other order are restated for this convention, with the equivalence explained in their natural-language statements.
  • Means take values in [0,∞][0,\infty][0,∞]; total mass 111 and finite additivity keep every value in [0,1][0,1][0,1].
  • Extensive amenability is stated for an action on [0,1][0,1][0,1] relative to the set of dyadic rationals in (0,1)(0,1)(0,1); the statement of Chornyi's corollary includes that FFF maps this set to itself.
  • The goal cannot be satisfied vacuously: amenability is a single existential statement about means on FFF, and FFF is a fixed, nontrivial, finitely generated group.

What is left out.

  • The Poisson boundary is not formalized: "Liouville" is Kaimanovich's equivalent reformulation through bounded harmonic functions on sgr⁡μ\operatorname{sgr}\musgrμ (p. 8).
  • The "in particular" clause of Moore's Theorem 1.1, on the Følner function, is not stated separately; with Følner's criterion it follows from the stated bound.
  • The withdrawn and disputed proofs in the timeline are not formalized.

What a development needs. Thompson's group FFF and its dyadic action (Cannon–Floyd–Parry §4), its tree diagrams and presentations, and amenability, Følner's criterion and the closure properties of amenable groups (Garrido I) are published and proved on this platform, as are Monod's groups and the isomorphism HQ(Z)≅FH_{\mathbf Q}(\mathbf Z) \cong FHQ​(Z)≅F (Monod.contDiff_and_exists_mulEquiv_HRat_F). Mathlib has Følner filters for measurable groups and Schreier graphs of quivers, but no random walks on groups; the proofs of the landmarks here supply what they need, and the germ-groupoid theorem of Juschenko, Nekrashevych and de la Salle (GermGroupoid.isAmenable_of_isExtensivelyAmenableOn) is reusable beyond this mission. Reductions of the goal or of Problem 12 to new, sharper statements are welcome, as is a disproof of either.

Selected references

  • J. W. Cannon, W. J. Floyd, W. R. Parry, Introductory notes on Richard Thompson's groups, L'Enseignement Math. (2) 42 (1996) 215–256. doi:10.5169/seals-87877
  • M. G. Brin, C. C. Squier, Groups of piecewise linear homeomorphisms of the real line, Invent. Math. 79 (1985) 485–498. doi:10.1007/BF01388519
  • J. T. Moore, Fast growth in the Følner function for Thompson's group F, Groups Geom. Dyn. 7 (2013) 633–651. doi:10.4171/GGD/201
  • V. A. Kaimanovich, Thompson's group F is not Liouville, in Groups, Graphs and Random Walks, LMS Lecture Note Ser. 436 (2017) 300–342. doi:10.1017/9781316576571.013
  • N. Monod, Groups of piecewise projective homeomorphisms, Proc. Natl. Acad. Sci. USA 110 (2013) 4524–4527. doi:10.1073/pnas.1218426110
  • K. Juschenko, N. Matte Bon, N. Monod, M. de la Salle, Extensive amenability and an application to interval exchanges, Ergodic Theory Dynam. Systems 38 (2018) 195–219. doi:10.1017/etds.2016.32
  • M. Chornyi, Superharmonic functions on the Lamplighter graph of Thompson's group F, preprint (2019). arXiv:1907.01440
  • V. Guba, Amenability problem for Thompson's group F: state of the art, J. Groups Complex. Cryptol. 15 (2023), no. 1. doi:10.46298/jgcc.2023.15.1.11315
  • S.-h. Kim, T. Koberda, Y. Lodha, Chain groups of homeomorphisms of the interval, Ann. Sci. Éc. Norm. Supér. (4) 52 (2019) 797–820. doi:10.24033/asens.2397
  • B. Stankov, Non-triviality of the Poisson boundary of random walks on the group H(ℤ) of Monod, Ergodic Theory Dynam. Systems 41 (2021) 1160–1189. doi:10.1017/etds.2019.76
  • OpenAI, Thompson's group F is nonamenable, OpenAI Math Release preprint (September 23, 2026). github.com/openai/math
  • N. Monod, Some comments on piecewise-projective groups of the line, Groups Geom. Dyn. 19 (2025) 459–476. doi:10.4171/ggd/883
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Differential GeometryDynamical Systems·Captain: Lucas

Pugh's Closing LemmaResearch Paper

Motivation

A periodic point of a map f ⁣:M→Mf\colon M\to Mf:M→M is a point xxx with fn(x)=xf^n(x)=xfn(x)=x for some n≥1n\ge 1n≥1. A nonwandering point is a much weaker form of recurrence: every neighbourhood UUU of xxx eventually returns to meet itself, fn(U)∩U≠∅f^n(U)\cap U\ne\emptysetfn(U)∩U=∅ for some n≥1n\ge 1n≥1. Every periodic point is nonwandering, but a nonwandering point need not be periodic, and the orbit of such a point may never come back to xxx exactly.

Pugh's closing lemma asserts that this gap can be closed by an arbitrarily small change of the system: if xxx is nonwandering for a C1C^1C1 diffeomorphism fff of a compact manifold, then some diffeomorphism ggg, as close to fff as desired in the C1C^1C1 topology, has xxx as a periodic point (Wikipedia, "Pugh's closing lemma"). The result was proved by C. C. Pugh in 1967 (Pugh 1967), in the same paper as the General Density Theorem: for a C1C^1C1-generic diffeomorphism the periodic points are dense in the nonwandering set. The source article describes the lemma as establishing a close relationship between chaotic and periodic behaviour and notes that it underlies some autonomous convergence theorems. The article also points to Smale's problems as related material.

Setting

Let MMM be a compact smooth manifold of dimension ddd, Hausdorff and without boundary. Write Diff1(M)\mathrm{Diff}^1(M)Diff1(M) for the set of C1C^1C1 diffeomorphisms g ⁣:M→Mg\colon M\to Mg:M→M: bijections such that ggg and g−1g^{-1}g−1 are continuously differentiable. For g∈Diff1(M)g\in\mathrm{Diff}^1(M)g∈Diff1(M), Tg ⁣:TM→TMTg\colon TM\to TMTg:TM→TM denotes its tangent map on the tangent bundle.

The C1C^1C1 topology on Diff1(M)\mathrm{Diff}^1(M)Diff1(M) is the coarsest topology for which g↦Tgg\mapsto Tgg↦Tg is continuous, where the space C(TM,TM)C(TM,TM)C(TM,TM) of continuous self-maps of TMTMTM carries the compact-open topology. Two diffeomorphisms are C1C^1C1-close when they, and their derivatives, are uniformly close.

For a map h ⁣:X→Xh\colon X\to Xh:X→X of a topological space:

  • xxx is nonwandering if for every neighbourhood UUU of xxx there is n≥1n\ge 1n≥1 with hn(U)∩U≠∅h^n(U)\cap U\ne\emptysethn(U)∩U=∅; the nonwandering set is Ω(h)\Omega(h)Ω(h);
  • Per(h)={x:∃ n≥1, hn(x)=x}\mathrm{Per}(h)=\{x : \exists\, n\ge 1,\ h^n(x)=x\}Per(h)={x:∃n≥1, hn(x)=x} is the set of periodic points.

Formalization targets

Goal: Pugh's closing lemma

For every f∈Diff1(M)f\in\mathrm{Diff}^1(M)f∈Diff1(M) and every x∈Ω(f)x\in\Omega(f)x∈Ω(f),

∀ U a C1-neighbourhood of f,∃ g∈U,  x∈Per(g).\forall\ \mathcal U \text{ a } C^1\text{-neighbourhood of } f,\quad \exists\, g\in\mathcal U,\ \ x\in\mathrm{Per}(g).∀ U a C1-neighbourhood of f,∃g∈U,  x∈Per(g).

Milestones

  1. Per(f)⊆Ω(f)\mathrm{Per}(f)\subseteq\Omega(f)Per(f)⊆Ω(f) for any map fff.
  2. Ω(f)\Omega(f)Ω(f) is closed for any map fff.
  3. f(Ω(f))=Ω(f)f(\Omega(f))=\Omega(f)f(Ω(f))=Ω(f) for a homeomorphism fff.
  4. Ω(f)≠∅\Omega(f)\ne\emptysetΩ(f)=∅ for any map of a nonempty compact space.
  5. General Density Theorem (Pugh 1967): there is a residual set G⊆Diff1(M)\mathcal G\subseteq\mathrm{Diff}^1(M)G⊆Diff1(M) with
Per(g)‾=Ω(g)(g∈G).\overline{\mathrm{Per}(g)}=\Omega(g)\qquad (g\in\mathcal G).Per(g)​=Ω(g)(g∈G).

Milestones 1–4 are elementary background facts that are not stated in the source article; milestone 5 is the second theorem named in the title of the source's reference.

Significance

The result. The closing lemma turns a topological recurrence property into periodicity after a C1C^1C1-small perturbation. Combined with genericity arguments it gives the General Density Theorem, so that for generic C1C^1C1 diffeomorphisms the whole nonwandering set is the closure of the periodic orbits. It is one of the basic perturbation tools of C1C^1C1 generic dynamics.

Formalizing it. The theorem is classical and proved in the literature. The drafter is not aware of a machine-checked proof. A formalization needs the C1C^1C1 topology on diffeomorphism groups, local perturbation lemmas in charts and the combinatorics of the closing argument. None of these is currently available in Mathlib as far as the drafter knows.

Difficulty

The first idea is to take the returning piece of orbit near xxx and push it back to xxx with a small local perturbation. This fails in the C1C^1C1 topology. Moving a point by distance δ\deltaδ with a bump supported in a ball of radius rrr costs C1C^1C1 size about δ/r\delta/rδ/r, and the return may happen at a distance comparable to the size of the only available ball. The perturbation then fails to be C1C^1C1-small. The derivative DfnDf^nDfn along the return can also distort any fixed neighbourhood shape without bound. Controlling this distortion is the central difficulty.

Formalization scope

  • Diff1(M)\mathrm{Diff}^1(M)Diff1(M) and its C1C^1C1 topology come from the published definition file BCWCentralizer_Basic. Diff1(M)\mathrm{Diff}^1(M)Diff1(M) is M ≃ₘ^1⟮𝓡 d, 𝓡 d⟯ M, and the topology is induced by g↦Tgg\mapsto Tgg↦Tg into C(TangentBundle, TangentBundle) with the compact-open topology. On a compact manifold this is the usual C1C^1C1 topology.
  • "Compact smooth manifold": a Hausdorff compact space with a C∞C^\inftyC∞ atlas modelled on Rd\mathbb R^dRd, so without boundary. ddd is arbitrary.
  • "Arbitrarily close" means that every neighbourhood of fff in the C1C^1C1 topology contains a suitable ggg. "Periodic" requires a period n≥1n\ge 1n≥1. Allowing n=0n=0n=0 would make every point periodic and the statement trivial.
  • The perturbation ggg is only required to be a C1C^1C1 diffeomorphism, matching Diff1(M)\mathrm{Diff}^1(M)Diff1(M) in the source.
  • The nonwandering notion is the definition item PughClosingLemma_nonwandering, shared by all statements. It is reusable for any topological dynamics mission.

Welcome contributions: a general theory of the C1C^1C1 topology on Diff1(M)\mathrm{Diff}^1(M)Diff1(M) (for example, that it is Baire), local perturbation lemmas, and proofs of the milestones.

Selected references

  • C. C. Pugh, An Improved Closing Lemma and a General Density Theorem, American Journal of Mathematics 89 (4), 1967, 1010–1021. https://doi.org/10.2307/2373414
  • Wikipedia, Pugh's closing lemma, revision 1304222873. https://en.wikipedia.org/w/index.php?title=Pugh%27s_closing_lemma&oldid=1304222873
  • V. Araújo, M. J. Pacifico, Three-Dimensional Flows, Springer, 2010, ISBN 978-3-642-11414-4.
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Dynamical Systems·Captain: Lucas

The C¹-generic diffeomorphism has trivial centralizer (Bonatti–Crovisier–Wilkinson)Research Paper

Motivation

Two commuting diffeomorphisms f,gf,gf,g of a manifold MMM share all of their dynamics: ggg permutes the orbits of fff and preserves every smooth and topological invariant of fff. The centralizer of f∈Diffr(M)f\in\mathrm{Diff}^r(M)f∈Diffr(M),

Zr(f)={g∈Diffr(M):fg=gf},Z^r(f)=\{g\in\mathrm{Diff}^r(M): fg=gf\},Zr(f)={g∈Diffr(M):fg=gf},

always contains the cyclic group ⟨f⟩={fn:n∈Z}\langle f\rangle=\{f^n:n\in\mathbb Z\}⟨f⟩={fn:n∈Z}, and fff has trivial centralizer when Zr(f)=⟨f⟩Z^r(f)=\langle f\rangleZr(f)=⟨f⟩. S. Smale asked whether diffeomorphisms with trivial centralizer are dense, residual, or even open and dense in Diffr(M)\mathrm{Diff}^r(M)Diffr(M) (one of Smale's problems for the 21st century).

Timeline: Kopell (1970) answered the question for r≥2r\ge2r≥2 on the circle; Palis–Yoccoz, Fisher and Burslem obtained results under hyperbolicity or partial hyperbolicity assumptions; Togawa treated generic Axiom A diffeomorphisms in the C1C^1C1 topology; Bonatti–Crovisier–Vago–Wilkinson showed that trivial-centralizer diffeomorphisms do not contain an open dense set in Diff1(M)\mathrm{Diff}^1(M)Diff1(M); and Bonatti–Crovisier–Wilkinson (this paper, arXiv:0804.1416) proved residuality in Diff1(M)\mathrm{Diff}^1(M)Diff1(M) for every compact manifold.

Setting

MMM is a closed (compact, boundaryless), connected smooth manifold of dimension ddd. Diff1(M)\mathrm{Diff}^1(M)Diff1(M) is the space of C1C^1C1 diffeomorphisms of MMM with the C1C^1C1 topology; a subset is residual if it contains a countable intersection of open dense sets.

Formalization targets

Goal (Main Theorem, p. 3)

There is a residual subset R⊂Diff1(M)\mathcal R\subset\mathrm{Diff}^1(M)R⊂Diff1(M) such that for every f∈Rf\in\mathcal Rf∈R and every g∈Diff1(M)g\in\mathrm{Diff}^1(M)g∈Diff1(M) with fg=gffg=gffg=gf, one has g=fng=f^ng=fn for some n∈Zn\in\mathbb Zn∈Z.

Milestones

Following Section 2 of the paper: the classical upper-semicontinuity lemma used for Proposition 2.5, the wandering part of Theorem A (unbounded distortion is C1C^1C1-generic), Proposition 2.5 (density of trivial Lipschitz centralizers implies residuality) and Theorem 2.3 (residuality of trivial Lipschitz centralizers when dim⁡M≥2\dim M\ge2dimM≥2).

Significance

The theorem answers the second (and hence the first) part of Smale's question in the C1C^1C1 topology, and exhibits a precise link between dynamical properties of fff (large derivative and unbounded distortion) and the algebraic structure of fff inside the group Diff1(M)\mathrm{Diff}^1(M)Diff1(M). The result is proved in the literature; it has not been formalized.

Difficulty

The density of trivial centralizers comes from perturbation results (Theorems A and B) that change the derivative without changing the topological dynamics (tidy perturbations in topological towers). Density alone does not give residuality, since the set of diffeomorphisms with the large derivative property is not residual (Appendix); the passage from dense to residual needs the Lipschitz centralizer and a semicontinuity argument.

Formalization scope

MMM is a charted space over Rd\mathbb R^dRd with a C∞C^\inftyC∞ atlas, Hausdorff, compact and connected; Diff1(M)\mathrm{Diff}^1(M)Diff1(M) is Mathlib's type of C1C^1C1 diffeomorphisms. The C1C^1C1 topology is encoded as the topology induced by f↦Tff\mapsto Tff↦Tf into the compact-open topology on continuous self-maps of the tangent bundle TMTMTM. Powers fnf^nfn, n∈Zn\in\mathbb Zn∈Z, are taken in the permutation group of MMM. Bi-Lipschitz homeomorphisms are defined chart-locally (equivalent on a compact manifold to bi-Lipschitz for a Riemannian distance). Jacobians ∣det⁡Dfn∣|\det Df^n|∣detDfn∣ are computed with respect to an arbitrary continuous Riemannian metric; the unbounded-distortion property does not depend on this choice.

Contributions welcome: the C1C^1C1 topology API (Baire property, continuity of composition), the Kupka–Smale and closing-lemma genericity results, and the perturbation machinery of Sections 3–7.

Selected references

  • C. Bonatti, S. Crovisier, A. Wilkinson, The C1C^1C1 generic diffeomorphism has trivial centralizer, Publ. Math. IHÉS 109 (2009); arXiv:0804.1416. https://arxiv.org/abs/0804.1416
  • S. Smale, Mathematical problems for the next century, Math. Intelligencer 20 (1998).
  • N. Kopell, Commuting diffeomorphisms, Proc. Sympos. Pure Math. 14 (1970).
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Discrete GeometryMathematical Physics·Captain: Lucas

Thomson Problem: Seven Electrons and the Known Exact SolutionsOpen Problem

Motivation

The Thomson problem asks for the configuration of NNN electrons, constrained to the surface of the unit sphere and repelling each other according to Coulomb's law, that minimises the total electrostatic potential energy. J. J. Thomson posed it in 1904 in connection with his "plum pudding" atomic model. The same energy-minimisation question reappears in the arrangement of protein subunits in spherical virus shells, in colloidosomes, in fullerene patterns and in multi-electron bubbles, and it is a special case (s=1s=1s=1) of the Riesz sss-energy problem on the sphere; the logarithmic variant is Smale's 7th problem.

Despite its elementary statement, the minimum is rigorously known only for a handful of values of NNN.

Timeline of exact solutions (as reported in the source).

  • N=1,2N=1,2N=1,2: trivial; for N=2N=2N=2 the optimum is an antipodal pair with U=1/2U=1/2U=1/2.
  • N=3N=3N=3: equilateral triangle on a great circle — L. Föppl (1912).
  • N=4N=4N=4: regular tetrahedron (listed in the source without a citation).
  • N=6N=6N=6: regular octahedron — V. A. Yudin (1992).
  • N=12N=12N=12: regular icosahedron — N. N. Andreev (1996).
  • N=5N=5N=5: triangular bipyramid — R. Schwartz (2013), computer-assisted.
  • N=7N=7N=7: pentagonal bipyramid — long observed numerically; in September 2026 an exact, Lean-kernel-checked proof was claimed (H. Tran, Vals AI).
  • N=8N=8N=8 and N=20N=20N=20: numerically, the optimum is not the cube, resp. the dodecahedron.

Setting

A configuration of NNN points is a map x:{0,…,N−1}→R3x:\{0,\dots,N-1\}\to\mathbb R^3x:{0,…,N−1}→R3. It is admissible if every point lies on the unit sphere, ∥xi∥=1\|x_i\|=1∥xi​∥=1, and the points are pairwise distinct. In units with e=1e=1e=1 and ke=1k_e=1ke​=1 its Coulomb energy is

U(x)=∑0≤i<j≤N−11∥xi−xj∥.U(x)=\sum_{0\le i<j\le N-1}\frac{1}{\|x_i-x_j\|}.U(x)=0≤i<j≤N−1∑​∥xi​−xj​∥1​.

An admissible xxx is an energy minimiser (solves the Thomson problem for NNN) if U(x)≤U(y)U(x)\le U(y)U(x)≤U(y) for every admissible NNN-point configuration yyy.

Explicit candidate configurations are fixed in the definitions file: the antipodal pair (N=2N=2N=2), an equatorial equilateral triangle (N=3N=3N=3), the regular tetrahedron (N=4N=4N=4), the triangular bipyramid (N=5N=5N=5), the regular octahedron (N=6N=6N=6), the pentagonal bipyramid (N=7N=7N=7: the two poles plus a regular pentagon (cos⁡2πk5,sin⁡2πk5,0)(\cos\tfrac{2\pi k}5,\sin\tfrac{2\pi k}5,0)(cos52πk​,sin52πk​,0) on the equator) and the regular icosahedron (N=12N=12N=12).

Formalization targets

Goal: N=7N=7N=7

the pentagonal bipyramid is an energy minimiser for N=7.\text{the pentagonal bipyramid is an energy minimiser for } N=7 .the pentagonal bipyramid is an energy minimiser for N=7.

This asserts admissibility of the seven points and the inequality U(P7)≤U(y)U(P_7)\le U(y)U(P7​)≤U(y) against every admissible seven-point configuration yyy. It fixes no numerical value of the minimum and does not assert uniqueness.

Milestones: the other known exact solutions

N=1: U≡0;N=2: antipodal pair optimal, U=12;N=1:\ U\equiv 0;\qquad N=2:\ \text{antipodal pair optimal},\ U=\tfrac12;N=1: U≡0;N=2: antipodal pair optimal, U=21​; N=3,4,5,6,12: triangle, tetrahedron, triangular bipyramid, octahedron, icosahedron are energy minimisers.N=3,4,5,6,12:\ \text{triangle, tetrahedron, triangular bipyramid, octahedron, icosahedron are energy minimisers.}N=3,4,5,6,12: triangle, tetrahedron, triangular bipyramid, octahedron, icosahedron are energy minimisers.

Significance

The result. Among the values of NNN listed in the source, N=7N=7N=7 is the smallest one whose optimum was, until the 2026 claim, supported only by numerical computation; the cases N≤6N\le 6N≤6 and N=12N=12N=12 were settled earlier. Settling N=7N=7N=7 extends the short list of rigorously known Thomson minimisers.

Formalizing it. The N=7N=7N=7 result reported in the source is recent and described there as a claimed Lean-kernel-checked proof; a formalization on this platform against a public, reviewed statement would corroborate it independently. For the milestones, the source attributes the N=3,5,6,12N=3,5,6,12N=3,5,6,12 cases to published proofs (Föppl 1912, Schwartz 2013, Yudin 1992, Andreev 1996); the source does not describe machine-checked proofs of these, and each is a self-contained formalization target.

Difficulty

The energy is a non-convex function on the configuration space (S2)N(S^2)^N(S2)N with many critical points, so numerical minimisation — which is how most entries of the source's table of smallest known energies were obtained — does not certify global optimality. The N=5N=5N=5 case, the most recent classical entry before N=7N=7N=7, was resolved only with a computer-assisted proof (Schwartz 2013).

Formalization scope

Points live in EuclideanSpace ℝ (Fin 3); configurations are functions Fin N → EuclideanSpace ℝ (Fin 3). Admissibility requires unit norm and injectivity (distinct points), matching the source's "NNN distinct points". The energy sums 1/dist(xi,xj)1/\mathrm{dist}(x_i,x_j)1/dist(xi​,xj​) over i<ji<ji<j; Lean's 1/0=01/0=01/0=0 convention is harmless because coincident points are excluded by admissibility. The candidate configurations are fixed in one particular orientation; since the energy is invariant under orthogonal maps and relabelling, this is no loss of generality. The statement "xxx is an energy minimiser" includes admissibility of xxx itself, so the goal cannot be satisfied by a degenerate candidate.

Reusable infrastructure welcome: energy invariance under isometries and permutations, existence of minimisers by compactness, linear-programming (Delsarte–Yudin) bounds on the sphere, and interval-arithmetic tooling for certified numerical bounds.

Selected references

  • Wikipedia, Thomson problem (source of this mission). https://en.wikipedia.org/wiki/Thomson_problem
  • J. J. Thomson, On the Structure of the Atom…, Philosophical Magazine 7 (1904), 237–265.
  • L. Föppl, Stabile Anordnungen von Elektronen im Atom, J. Reine Angew. Math. 141 (1912), 251–301. https://doi.org/10.1515/crll.1912.141.251
  • V. A. Yudin, The minimum of potential energy of a system of point charges, Discrete Math. Appl. 3 (1993), 75–81. https://doi.org/10.1515/dma.1993.3.1.75
  • N. N. Andreev, An extremal property of the icosahedron, East J. Approx. 2 (1996), 459–462.
  • R. Schwartz, The five-electron case of Thomson's problem, Experimental Mathematics 22 (2013), 157–186. https://arxiv.org/abs/1001.3702
  • S. Smale, Mathematical Problems for the Next Century, Math. Intelligencer 20 (1998), 7–15. https://doi.org/10.1007/bf03025291
  • Vals AI, A Lean Proof of the Thomson Problem for Seven Electrons (2026). https://www.vals.ai/blogs/thomson-n7-lean-proof
9 thms2 active usersReviewed
Dynamical Systems·Captain: Lucas

Hilbert's 16th Problem for Algebraic Limit Cycles (Llibre's Conjecture)Open Problem

Motivation

The second part of Hilbert's 16th problem (Paris, 1900) asks for the maximal number and the relative position of the limit cycles of a planar polynomial differential system

x˙=P(x,y),y˙=Q(x,y),\dot x = P(x,y),\qquad \dot y = Q(x,y),x˙=P(x,y),y˙​=Q(x,y),

where P,QP,QP,Q are real polynomials of degree at most ddd. Smale listed it in 1998 among the mathematical problems for the next century and remarked that, apart from the Riemann hypothesis, it seems the hardest of Hilbert's problems (Smale 1998). Even for d=2d = 2d=2 it is not known whether the number of limit cycles is uniformly bounded.

J. Llibre's survey Sobre el problema 16 de Hilbert (La Gaceta de la RSME 18 (2015), 543–554) organises the question into seven problems and concentrates on a more tractable restriction: algebraic limit cycles, i.e. limit cycles contained in a real algebraic curve. For this restriction there is an explicit conjecture for the maximal number (Conjecture 1 of the survey, first stated in Llibre–Ramírez–Sadovskaia 2010). This mission formalizes that conjecture as its goal, together with the results of the survey on which it rests.

Timeline (as reported in the survey):

  • 1891–1897 — Poincaré introduces limit cycles and proves finiteness for systems without saddle connections.
  • 1900 — Hilbert poses the 16th problem.
  • 1923 — Dulac claims every polynomial system has finitely many limit cycles; in 1985 Ilyashenko finds a gap.
  • 1957/1959 — Petrovskii and Landis claim H(2)=3H(2)=3H(2)=3 and later find an error; 1979 (Chen–Wang) and 1982 (Shi) give quadratic systems with 4 limit cycles.
  • 1986 — Bamon proves finiteness for quadratic systems; 1991/1992 — Ilyashenko and Écalle independently prove finiteness for all polynomial systems.
  • 2001 — Christopher realises any non-singular algebraic curve's bounded components as hyperbolic limit cycles of a system of the same degree (Christopher 2001).
  • 2004 — Llibre and Rodríguez show every configuration of limit cycles is realisable by algebraic limit cycles (Llibre–Rodríguez 2004).
  • 2007 — Llibre and Zhao give a cubic system with two algebraic limit cycles (Llibre–Zhao 2007).
  • 2010 — Llibre, Ramírez and Sadovskaia bound the number of algebraic limit cycles when all invariant algebraic curves are generic, and state the conjecture.

Setting

A polynomial vector field is a pair V=(P,Q)V = (P, Q)V=(P,Q) of real polynomials in x,yx,yx,y; its degree is max⁡(deg⁡P,deg⁡Q)\max(\deg P, \deg Q)max(degP,degQ). A solution is a differentiable curve γ:R→R2\gamma:\mathbb R\to\mathbb R^2γ:R→R2 with γ′(t)=(P,Q)(γ(t))\gamma'(t) = (P,Q)(\gamma(t))γ′(t)=(P,Q)(γ(t)) for all ttt. A periodic orbit is the image of a non-constant periodic solution. A limit cycle is a periodic orbit OOO that is isolated among periodic orbits: some open set U⊇OU \supseteq OU⊇O contains no periodic orbit other than OOO.

A limit cycle is algebraic if it is contained in the zero set {f=0}\{f = 0\}{f=0} of a non-zero real polynomial fff. The algebraic Hilbert number Ha(d)H_a(d)Ha​(d) is the supremum, over all polynomial vector fields of degree at most ddd, of the number of algebraic limit cycles (a value in N∪{∞}\mathbb N \cup \{\infty\}N∪{∞}).

A curve f=0f = 0f=0 is invariant with cofactor KKK if P fx+Q fy=KfP\,f_x + Q\,f_y = K fPfx​+Qfy​=Kf. A family of irreducible curves is generic if (i) no curve is singular, (ii) the top-degree homogeneous part of each curve is square-free, (iii) distinct curves meet transversally, (iv) no three distinct curves share a point, and (v) the top-degree homogeneous parts of distinct curves are coprime.

Formalization targets

Goal — Conjecture 1 (Llibre–Ramírez–Sadovskaia)

Ha(d)=1+(d−1)(d−2)2(d≥2).H_a(d) = 1 + \frac{(d-1)(d-2)}{2}\qquad (d \ge 2).Ha​(d)=1+2(d−1)(d−2)​(d≥2).

The equality asserts both that the number of algebraic limit cycles is bounded by the right-hand side for every field of degree at most ddd, and that the bound is attained.

Milestones (in the order of the survey)

  1. §2, Problem 1 — every polynomial vector field has finitely many limit cycles (Écalle, Ilyashenko).
  2. §3 — H(1)=0H(1) = 0H(1)=0: vector fields of degree at most 111 have no limit cycles.
  3. Theorem 1(a),(b) — every configuration of limit cycles is realised, and realised by algebraic limit cycles in degree ≤2(n+r)−1\le 2(n+r)-1≤2(n+r)−1.
  4. Theorem 2 (Christopher) — the bounded components of a non-singular curve f=0f = 0f=0 are exactly the limit cycles, all hyperbolic, of x˙=αf−Dfy\dot x = \alpha f - D f_yx˙=αf−Dfy​, y˙=βf+Dfx\dot y = \beta f + D f_xy˙​=βf+Dfx​.
  5. Proposition 3 — invariance of fff is equivalent to invariance of its irreducible factors, with Kf=∑niKfiK_f = \sum n_i K_{f_i}Kf​=∑ni​Kfi​​.
  6. Theorem 4(a),(b) — for degree d≥2d \ge 2d≥2 and generic invariant curves, at most 1+(d−1)(d−2)21 + \frac{(d-1)(d-2)}{2}1+2(d−1)(d−2)​ (even ddd) or (d−1)(d−2)2\frac{(d-1)(d-2)}{2}2(d−1)(d−2)​ (odd ddd) algebraic limit cycles, and the bounds are attained.
  7. §7 example — the cubic system x˙=2y(10+xy)\dot x = 2y(10+xy)x˙=2y(10+xy), y˙=20x+y−20x3−2x2y+4y3\dot y = 20x + y - 20x^3 - 2x^2 y + 4y^3y˙​=20x+y−20x3−2x2y+4y3 has two algebraic limit cycles in 2x4−4x2+4y2+1=02x^4 - 4x^2 + 4y^2 + 1 = 02x4−4x2+4y2+1=0.
  8. Conjecture 2 — Ha(2)=1H_a(2) = 1Ha​(2)=1.
  9. Theorem 5 (Giacomini–Llibre–Viano) — an inverse integrating factor vanishes on every limit cycle.

Significance

A proof of the goal would settle Problems 6 and 7 of the survey: it would give a uniform bound, depending only on the degree, for the number of algebraic limit cycles, and identify the sharp value. The conjecture is consistent with every example known to the survey: the generic bound of Theorem 4 is sharp for even ddd, and the known non-generic examples exceed the generic bound only in odd degree and by one. Conjecture 2 (d=2d = 2d=2) is its first open case.

On the formal side, the milestones require a reusable library of planar dynamics that is currently absent from Mathlib: periodic orbits and limit cycles of planar vector fields, hyperbolicity via the divergence integral, inverse integrating factors, invariant algebraic curves and Darboux-type arguments, and topological configurations of Jordan curves. Theorems 1, 2, 4 and 5, Proposition 3 and the cubic example are proved in the literature but, as far as the proposal author knows, not formalized; the goal and Conjecture 2 are open.

Difficulty

The obvious route bounds the number of ovals of the invariant curve (Harnack's theorem) and relates the degree of the curve to the degree of the field. This fails because a field of degree ddd can have invariant curves of arbitrarily high degree, so no a-priori degree bound on the curve is available; Theorem 4 obtains one only under the genericity conditions (i)–(v), and the degree-3 example shows that non-generic curves behave differently. On the formal side, the dynamical milestones (Theorems 2 and 5, the cubic example) need Poincaré–Bendixson-type planar topology and uniqueness of solutions, which Mathlib does not yet provide.

Formalization scope

  • Polynomials are MvPolynomial (Fin 2) ℝ with variable 0 as xxx and 1 as yyy; points are ℝ × ℝ. The degree of a field is the maximum of the total degrees of PPP and QQQ, and Ha(d)H_a(d)Ha​(d) ranges over fields of degree at most ddd, matching equation (1) of the survey.
  • Counts of limit cycles are Set.encard values in ℕ∞, so an infinite family is ∞\infty∞, never silently 000; Ha(d)H_a(d)Ha​(d) is an iSup in ℕ∞, so the goal also asserts finiteness.
  • Solutions are global (HasDerivAt at every real time). A limit cycle is isolated among periodic orbits contained in a neighbourhood. An algebraic limit cycle lies in the zero set of some non-zero polynomial, with no degree restriction on the curve.
  • Genericity conditions (i), (iii), (iv) are imposed at complex points of C2\mathbb C^2C2; (ii), (v) use square-freeness and coprimality in R[x,y]\mathbb R[x,y]R[x,y]; "distinct curves" means non-associated polynomials.
  • Hyperbolicity of a limit cycle is encoded by a non-zero divergence integral over one period.
  • Theorem 1(b) is formalized without its final sentence (existence of a Darboux first integral).
  • Trivializing encodings are ruled out: algebraic limit cycles require a non-zero polynomial, and the conjecture is an equality in ℕ∞, not an inequality over a possibly empty family.

Contributions welcome: a planar ODE library (uniqueness, flows, Poincaré–Bendixson), Darboux theory of integrability, and proofs of the classical milestones.

Selected references

  • J. Llibre, Sobre el problema 16 de Hilbert, La Gaceta de la RSME 18 (2015), no. 3, 543–554 (source of this mission).
  • J. Llibre, R. Ramírez, N. Sadovskaia, On the 16th Hilbert problem for algebraic limit cycles, J. Differential Equations 248 (2010), 1401–1409. https://doi.org/10.1016/j.jde.2009.11.023
  • J. Llibre, G. Rodríguez, Configurations of limit cycles and planar polynomial vector fields, J. Differential Equations 198 (2004), 374–380. https://doi.org/10.1016/j.jde.2003.10.008
  • C. Christopher, Polynomial vector fields with prescribed algebraic limit cycles, Geom. Dedicata 88 (2001), 255–258. https://doi.org/10.1023/a:1013171019668
  • H. Giacomini, J. Llibre, M. Viano, On the nonexistence, existence and uniqueness of limit cycles, Nonlinearity 9 (1996), 501–516. https://doi.org/10.1088/0951-7715/9/2/013
  • J. Llibre, Y. Zhao, Algebraic limit cycles in polynomial systems of differential equations, J. Phys. A 40 (2007), 14207–14222. https://doi.org/10.1088/1751-8113/40/47/012
  • Yu. Ilyashenko, Centennial history of Hilbert's 16th problem, Bull. Amer. Math. Soc. 39 (2002), 301–354. https://doi.org/10.1090/s0273-0979-02-00946-1
  • S. Smale, Mathematical problems for the next century, Math. Intelligencer 20 (1998), no. 2, 7–15. https://doi.org/10.1007/bf03025291
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Dynamic ProgrammingMarkov ChainOperations Research·Captain: mikedeng1

Analysis and Algorithms for Service Parts Supply Chains II: The Single-Unit Single-Customer DecompositionTextbook

Motivation

A base-stock (order-up-to) policy orders, in every period, exactly enough to bring the inventory position (stock on hand plus stock on order minus backorders) up to a target level. It is the policy used in practice for repairable and consumable service parts, and the analysis of every later chapter of Muckstadt's book assumes it. Its optimality is therefore a foundational question, and there are three classical ways to prove it.

  • 1960, Clark and Scarf proved optimality of echelon base-stock policies for finite-horizon serial systems by dynamic programming, decomposing the cost into one term per echelon (Management Science 6(4)).
  • 1984, Federgruen and Zipkin gave a lower-bound argument for the infinite-horizon average-cost case (Operations Research 32(4)); Chen and Song (2001) used it for Markov-modulated demand (Operations Research 49(2)).
  • 2008, Muharremoglu and Tsitsiklis introduced the single-unit single-customer approach: every unit of stock is paired with one future customer, and the inventory problem splits into countably many independent two-action problems (Operations Research 56(5)).

This mission formalizes the third approach, in the finite-horizon single-location form presented in Section 2.2.1 of Muckstadt (2005).

Setting

A single item is reviewed in periods n=1,…,Nn = 1, \dots, Nn=1,…,N. An exogenous, time-homogeneous Markov chain sns_nsn​ on a finite set Σ\SigmaΣ is observed at the start of period nnn; given sn=ss_n = ssn​=s, the demand Dn∈{0,1,2,… }D_n \in \{0,1,2,\dots\}Dn​∈{0,1,2,…} has law κ(s,⋅)\kappa(s,\cdot)κ(s,⋅) and is independent of sn+1s_{n+1}sn+1​. Excess demand is backordered.

Every unit of demand is a customer, and customers are indexed in arrival order, the v0v_0v0​ initially waiting customers first. A customer's distance is 000 once served, 111 while waiting, and 2,3,…2, 3, \dots2,3,… for future customers in the order they will arrive. Units are indexed by location: 000 (used), 111 (on hand), 2,…,m2, \dots, m2,…,m (in transit) and m+1m+1m+1 (at the supplier, which holds countably many units). The state is

xn=(sn,(z1n,y1n),(z2n,y2n),…),x_n = \big(s_n, (z_{1n}, y_{1n}), (z_{2n}, y_{2n}), \dots\big),xn​=(sn​,(z1n​,y1n​),(z2n​,y2n​),…),

with zjnz_{jn}zjn​ the location of unit jjj and yjny_{jn}yjn​ the distance of customer jjj. In period nnn: units in transit move one location closer and the released units move from m+1m+1m+1 to mmm (so an order is on hand m−1m-1m−1 periods later); the demand DnD_nDn​ brings the customers at distances 2,…,Dn+12, \dots, D_n+12,…,Dn​+1 to distance 111 and moves the others DnD_nDn​ steps closer; units on hand serve waiting customers, lowest indices first; then hhh is charged per unit on hand and bbb per waiting customer, with 0<h<b0 < h < b0<h<b. The criterion is the expected cost over the NNN periods, discounted by α∈(0,1]\alpha \in (0,1]α∈(0,1].

A policy for the whole system S\mathcal SS chooses a finite set of units at the supplier to release. It is monotone if it releases lower-indexed units first, and committed if unit jjj only ever serves customer jjj. The subsystem Sw\mathcal S_wSw​ is unit www with customer www under commitment, with state xnw=(sn,zwn,ywn)x^w_n = (s_n, z_{wn}, y_{wn})xnw​=(sn​,zwn​,ywn​) and actions Release and Hold. The set Rn∗(s,y)R^*_n(s,y)Rn∗​(s,y) contains the optimal actions of a subsystem whose unit is at the supplier and whose customer is at distance yyy, and the critical distance is

y∗(n,s)=max⁡{ y:Rn∗(s,y)∋Release }.y^*(n,s) = \max\{\, y : R^*_n(s,y) \ni \mathit{Release} \,\}.y∗(n,s)=max{y:Rn∗​(s,y)∋Release}.

Formalization targets

Goal: Theorem 5 (p. 29)

Every policy that, in each period nnn and Markov state sns_nsn​, releases the lowest-indexed units at the supplier to raise the inventory position to

y∗(n,sn)−1y^*(n, s_n) - 1y∗(n,sn​)−1

is optimal for S\mathcal SS among all policies, from every starting state. Such a policy exists. The levels are not fixed numbers but the critical distances of the single-unit problem, so the goal asserts the structure of an optimal policy and identifies its levels, without committing to any constant.

Milestones

  1. Lemma 1 (p. 26): some monotone policy is optimal, every monotone policy is committed, and so some committed policy is optimal.
  2. Theorem 4 (p. 27): the optimal cost of S\mathcal SS is the sum over www of the optimal costs of Sw\mathcal S_wSw​,
V1S(s,x1)=∑wV1(s,(zw1,yw1)),V^{\mathcal S}_1(s, x_1) = \sum_{w} V_1\big(s, (z_{w1}, y_{w1})\big),V1S​(s,x1​)=w∑​V1​(s,(zw1​,yw1​)),

and managing every subsystem independently and optimally is optimal for S\mathcal SS. 3. Lemma 2 (p. 28): Rn∗(s,y+1)={Release}R^*_n(s, y+1) = \{\mathit{Release}\}Rn∗​(s,y+1)={Release} implies Release∈Rn∗(s,y)\mathit{Release} \in R^*_n(s, y)Release∈Rn∗​(s,y). 4. Section 2.2.1.2.2 (p. 29): the critical distance policy, release if and only if y≤y∗(n,s)y \le y^*(n,s)y≤y∗(n,s), is optimal for every subsystem.

Significance

The result shows that under Markov-modulated demand a single-location system is optimally run by a state-dependent base-stock policy. The same unit–customer argument gives echelon base-stock optimality in serial systems with noncrossing stochastic lead times (Sections 2.2.2–2.2.3). The decomposition also yields the levels themselves: they are the critical distances of a two-action problem, which can be solved one customer at a time.

The theorems are proved in the literature (Muharremoglu and Tsitsiklis 2008) and in the book. To our knowledge no machine-checked proof of any base-stock optimality theorem exists, by dynamic programming or by decomposition. The book's proof is informal in three places a formalization has to settle:

  • Lemma 1 is asserted as "clearly" true;
  • Lemma 2's proof by contradiction covers only uniquely optimal releases, while the critical distance policy also needs the case of ties;
  • the passage from the subsystem policy to the inventory position (Theorem 5) is an "intuitive argument".

A formal development makes each of these precise.

Difficulty

The obvious argument says that costs are linear, so the cost of S\mathcal SS is the sum of unit–customer costs and everything decouples. That is only half of Theorem 4. The pairing of unit jjj with customer jjj holds only under monotone policies, and a general policy for S\mathcal SS observes the whole infinite state xnx_nxn​, not just xnwx^w_nxnw​. The lower bound therefore needs Lemma 1 together with the fact that extra information about the demand history does not help a Markov decision problem. The upper bound needs the lowest-index matching to cost no more than committed matching.

The second difficulty is that the threshold structure is not the obvious consequence of Lemma 2. The set of distances at which releasing is optimal must be shown to be an initial segment {1,…,y∗}\{1, \dots, y^*\}{1,…,y∗} when ties are allowed. Unbounded demand makes that set possibly unbounded (it is, in the last m−1m-1m−1 periods). Finally, the release decisions of the subsystems must be counted to recover an inventory position, which uses the invariant that future customers occupy consecutive distances.

Formalization scope

Everything is in the namespace ServiceParts.UnitDecomp, with three definition files.

Model. Model bundles the chain, the demand law, mmm, hhh, bbb and α\alphaα with the standing assumptions 1≤m1 \le m1≤m, 0<h<b0 < h < b0<h<b, 0<α≤10 < \alpha \le 10<α≤1, together with the per-unit and per-customer motions and a generic finite-horizon expected-cost recursion. Costs are in [0,∞][0,\infty][0,∞].

Subsystem. Subsystem defines a subsystem, its optimal cost, Rn∗R^*_nRn∗​, y∗(n,s)y^*(n,s)y∗(n,s) and the critical distance policy.

System. System defines S\mathcal SS with lowest-index matching, its policies (finite release sets), monotone and committed policies, starting states, the inventory position and the order-up-to release.

Conventions and pinnings:

  • Indexing. Units and customers are indexed from 000; Lean index jjj is the book's j+1j+1j+1.
  • Policy class. Policies are Markov: functions of the period, the Markov state and the configuration, as on p. 25.
  • Optimality. Optimal means attaining the infimum over all policies for S\mathcal SS. Restricting the class to monotone or base-stock policies would make Theorem 5 circular and is ruled out.
  • Starting states. The book's "any starting state x1x_1x1​" is the configuration built on pp. 23–24 from v0v_0v0​ and the stock at locations 1,…,m1, \dots, m1,…,m. For arbitrarily labelled states Theorem 4 is false.
  • Critical distance. y∗(n,s)y^*(n,s)y∗(n,s) is a supremum in N∪{∞}\mathbb N \cup \{\infty\}N∪{∞}. Where it is ∞\infty∞ (a released unit cannot arrive before the horizon), Theorem 5 leaves the policy free.
  • Distance 0. Lemma 2 and the optimality of RnR_nRn​ are stated for customers at distance at least 1. At distance 0 with the unit at the supplier (a configuration committed policies never reach), both are false as printed.

Corrections to the book:

  • h>0h > 0h>0 is added. With h=0h = 0h=0 an optimal policy with finite orders need not exist, so Theorem 5 fails.
  • Chain structure is pinned. The chain's ergodicity is unused on a finite horizon and omitted. The conditional independence of DnD_nDn​ and sn+1s_{n+1}sn+1​ given sns_nsn​ is added as a reading of "given sns_nsn​, the distribution of DnD_nDn​ is known".
  • Vacuous corner. If some state's demand has infinite mean, every policy may cost ∞\infty∞ and the optimality statements hold vacuously.

Out of scope: stochastic noncrossing lead times (Section 2.2.2), serial systems (Section 2.2.3; compare the disproved platform statement SupplyChainTheory.clark_scarf_sequential), and continuous review (Section 2.2.4, which the book calls intuitive).

Proofs of any milestone are welcome. A reusable by-product would be a general lemma that Markov policies are optimal among history-dependent ones for finite-horizon problems with countable randomness and costs in [0,∞][0,\infty][0,∞].

Selected references

  • J. A. Muckstadt, Analysis and Algorithms for Service Parts Supply Chains, Springer, 2005, Section 2.2, pp. 22–31. https://doi.org/10.1007/b138879
  • A. Muharremoglu and J. N. Tsitsiklis, A single-unit decomposition approach to multiechelon inventory systems, Operations Research 56(5), 2008. https://doi.org/10.1287/opre.1080.0620
  • A. J. Clark and H. Scarf, Optimal policies for a multi-echelon inventory problem, Management Science 6(4), 1960. https://doi.org/10.1287/mnsc.6.4.475
  • A. Federgruen and P. Zipkin, Computational issues in an infinite-horizon, multiechelon inventory model, Operations Research 32(4), 1984. https://doi.org/10.1287/opre.32.4.818
  • F. Chen and J.-S. Song, Optimal policies for multiechelon inventory problems with Markov-modulated demand, Operations Research 49(2), 2001. https://doi.org/10.1287/opre.49.2.226.13528
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Functional Analysis·Captain: savarin

Sharp diagonal Hlawka constants: formalize the supplied proof at cutoff 90Research Paper

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

This mission extends the best possible constant for complex diagonal matrices from p≥256p\ge256p≥256 to every real p≥90p\ge90p≥90. The result is proved in Lean. The constant and its formula are unchanged from the foundation mission: the largest comparison constant required by the cyclic family of three 3×33\times33×3 diagonal matrices. For each exponent, it works for every triple of diagonal matrices, whatever their size, and no smaller constant does.

The mission started from a supplied pen-and-paper proof. Lowering the cutoff took more than replacing 256 with 90: several estimates in the original argument had to be strengthened. The research note proves the bound for real entries first, then transfers it to complex entries and shows that the constant cannot be improved. The goal theorem below gives the exact formula and statement.

This is the second step of the sharp diagonal Hlawka campaign, and it reuses the foundation's definitions and supporting results. The campaign invites further improvements below 90, keeping the same formula.

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

References

  • K. M. R. Audenaert and F. Kittaneh, Problems and Conjectures in Matrix and Operator Inequalities, arXiv preprint, 2012, §8.2, Problem 7. arXiv:1201.5232
  • Ezzeri Esa, Hlawka–Schatten inequalities: sharp diagonal construction, Lean source repository, 2026, revision 79aa498bfcf7b22bd91d771fb32ec278e2d4704b. Source library
  • Ezzeri Esa and project contributors, The cyclic bound for every real p ≥ 90, research note with appendices and exact certificates, 2026. Research note

Established results on Prove2Me

  • The accepted sharp diagonal bound for every real p ≥ 256.
  • The accepted diagonal Schatten norm identity.
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Markov ChainProbabilityStatistics·Captain: mikedeng1

A Note on Metropolis–Hastings Kernels for General State Spaces III: The Maximal Kernel of a Mixture Proposal Dominates the Mixture of Maximal Kernels Off the DiagonalResearch Paper

Motivation

A Markov chain Monte Carlo sampler is often assembled from simpler parts. A practitioner who has several proposal mechanisms Q1,Q2,…Q_1, Q_2, \dotsQ1​,Q2​,… for a Metropolis–Hastings sampler can combine them in two ways. Either each QiQ_iQi​ drives its own Metropolis–Hastings kernel PiP_iPi​ and the sampler picks kernel PiP_iPi​ with probability βi\beta_iβi​ at each step, or the mixture Q=∑iβiQiQ = \sum_i \beta_i Q_iQ=∑i​βi​Qi​ is used as a single proposal inside one Metropolis–Hastings kernel. Both samplers leave the target π\piπ invariant, so the choice is about efficiency.

Section 4 of Tierney (1998) settles the comparison: when both samplers use the maximal acceptance probability, the second never does worse in terms of asymptotic variances of sample-path averages. The statement that carries this is Proposition 5, an ordering of kernels in Peskun's off-diagonal order; the variance comparison then follows from Theorem 4 of the same paper, the general-state-space extension of Peskun (1973).

Timeline. Peskun (1973) introduced off-diagonal domination for finite state spaces and showed that the Metropolis–Hastings acceptance probability is maximal in that order. A version of Proposition 5 for discrete chains appears in the appendix of Tierney (1991) and in the rejoinder of Besag, Green, Higdon and Mengersen (1995). Tierney (1998) states and proves it for general state spaces, using the measure-theoretic description of Metropolis–Hastings kernels from §2 of the same paper.

Setting

Let (E,E)(E, \mathcal E)(E,E) be a measurable space and π\piπ a probability measure on it, the target. A proposal kernel Q(x,dy)Q(x, dy)Q(x,dy) is a Markov kernel on EEE. Given a measurable acceptance probability α:E×E→[0,1]\alpha : E \times E \to [0,1]α:E×E→[0,1], the Metropolis–Hastings kernel is

P(x,dy)=Q(x,dy) α(x,y)+δx(dy)∫(1−α(x,u)) Q(x,du),P(x, dy) = Q(x, dy)\,\alpha(x, y) + \delta_x(dy) \int \bigl(1 - \alpha(x, u)\bigr)\, Q(x, du),P(x,dy)=Q(x,dy)α(x,y)+δx​(dy)∫(1−α(x,u))Q(x,du),

where δx\delta_xδx​ is the point mass at xxx (mhKernel Q α).

Put μ(dx,dy)=π(dx)Q(x,dy)\mu(dx, dy) = \pi(dx) Q(x, dy)μ(dx,dy)=π(dx)Q(x,dy) and μT(dx,dy)=μ(dy,dx)\mu^T(dx, dy) = \mu(dy, dx)μT(dx,dy)=μ(dy,dx). With ν=μ+μT\nu = \mu + \mu^Tν=μ+μT and h=dμ/dνh = d\mu/d\nuh=dμ/dν (canonDensity), let

R={(x,y):h(x,y)>0, h(y,x)>0},r(x,y)=h(x,y)/h(y,x) on R,r=1 on RcR = \{(x, y) : h(x, y) > 0,\ h(y, x) > 0\},\qquad r(x, y) = h(x, y)/h(y, x) \text{ on } R,\quad r = 1 \text{ on } R^cR={(x,y):h(x,y)>0, h(y,x)>0},r(x,y)=h(x,y)/h(y,x) on R,r=1 on Rc

(canonR, canonRatio). The set RRR is symmetric, μ\muμ and μT\mu^TμT are mutually absolutely continuous on RRR and mutually singular off it (Proposition 1 of the paper). The Metropolis–Hastings acceptance probability is

αMH(x,y)=min⁡{1,r(y,x)} if (x,y)∈R,αMH(x,y)=0 otherwise\alpha_{MH}(x, y) = \min\{1, r(y, x)\} \text{ if } (x, y) \in R, \qquad \alpha_{MH}(x, y) = 0 \text{ otherwise}αMH​(x,y)=min{1,r(y,x)} if (x,y)∈R,αMH​(x,y)=0 otherwise

(alphaMH π Q), and the kernel with α=αMH\alpha = \alpha_{MH}α=αMH​ is the maximal Metropolis–Hastings kernel for QQQ (maxMHKernel π Q).

For kernels P1,P2P_1, P_2P1​,P2​ on EEE, P1P_1P1​ dominates P2P_2P2​ off the diagonal, P1⪰P2P_1 \succeq P_2P1​⪰P2​ (OffDiagDominates π P₁ P₂), if for π\piπ-almost every xxx, P1(x,A∖{x})≥P2(x,A∖{x})P_1(x, A \setminus \{x\}) \ge P_2(x, A \setminus \{x\})P1​(x,A∖{x})≥P2​(x,A∖{x}) for all A∈EA \in \mathcal EA∈E. For a countable family of kernels KiK_iKi​ and weights βi≥0\beta_i \ge 0βi​≥0, the mixture ∑iβiKi\sum_i \beta_i K_i∑i​βi​Ki​ is the kernel x↦∑iβiKi(x,⋅)x \mapsto \sum_i \beta_i K_i(x, \cdot)x↦∑i​βi​Ki​(x,⋅) (mixKernel β K).

Formalization targets

Goal: Proposition 5

Let QiQ_iQi​ be a finite or countable family of proposal kernels and βi≥0\beta_i \ge 0βi​≥0 with ∑iβi=1\sum_i \beta_i = 1∑i​βi​=1. Let PiP_iPi​ be the maximal Metropolis–Hastings kernel for QiQ_iQi​ and PPP the maximal Metropolis–Hastings kernel for Q=∑iβiQiQ = \sum_i \beta_i Q_iQ=∑i​βi​Qi​. Then

P⪰∑iβiPi.P \succeq \sum_i \beta_i P_i .P⪰i∑​βi​Pi​.

Both sides use maximal kernels: PPP uses αMH\alpha_{MH}αMH​ of the mixture proposal, each PiP_iPi​ its own αMH(i)\alpha^{(i)}_{MH}αMH(i)​, and the same weights βi\beta_iβi​ form both mixtures.

Milestones

  1. The construction in the proof of Proposition 1 (p. 2) yields a set RRR and ratio rrr with the properties of Proposition 1 for μ=π⊗Q\mu = \pi \otimes Qμ=π⊗Q.
  2. αMH\alpha_{MH}αMH​ satisfies conditions (i) and (ii) of Theorem 2 (p. 3): αMH=0\alpha_{MH} = 0αMH​=0 μ\muμ-a.e. on RcR^cRc, and αMH(x,y)r(x,y)=αMH(y,x)\alpha_{MH}(x, y) r(x, y) = \alpha_{MH}(y, x)αMH​(x,y)r(x,y)=αMH​(y,x) μ\muμ-a.e. on RRR.
  3. The maximal kernel satisfies detailed balance, π(dx)P(x,dy)=π(dy)P(y,dx)\pi(dx) P(x, dy) = \pi(dy) P(y, dx)π(dx)P(x,dy)=π(dy)P(y,dx).
  4. For any symmetric σ\sigmaσ-finite ν\nuν dominating μ\muμ, with h=dμ/dνh = d\mu/d\nuh=dμ/dν:
π(dx)Q(x,dy) αMH(x,y)=min⁡{h(y,x),h(x,y)} ν(dx,dy).\pi(dx) Q(x, dy)\, \alpha_{MH}(x, y) = \min\{h(y, x), h(x, y)\}\, \nu(dx, dy).π(dx)Q(x,dy)αMH​(x,y)=min{h(y,x),h(x,y)}ν(dx,dy).
  1. As measures on E×EE \times EE×E:
π(dx)Q(x,dy) αMH(x,y)≥∑iβi π(dx)Qi(x,dy) αMH(i)(x,y).\pi(dx) Q(x, dy)\, \alpha_{MH}(x, y) \ge \sum_i \beta_i\, \pi(dx) Q_i(x, dy)\, \alpha^{(i)}_{MH}(x, y).π(dx)Q(x,dy)αMH​(x,y)≥i∑​βi​π(dx)Qi​(x,dy)αMH(i)​(x,y).

A companion item states the maximality of αMH\alpha_{MH}αMH​ (§3, p. 7): every measurable acceptance probability α\alphaα whose kernel is reversible satisfies α≤αMH\alpha \le \alpha_{MH}α≤αMH​ μ\muμ-a.e., so the maximal kernel dominates every reversible Metropolis–Hastings kernel with the same proposal.

Significance

The result. Proposition 5, combined with Theorem 4 of the paper (off-diagonal domination orders asymptotic variances of reversible kernels), shows that for every function fff with finite variance the asymptotic variance of 1n∑kf(Xk)\frac1n \sum_{k} f(X_k)n1​∑k​f(Xk​) under the mixture-proposal sampler is at most that under the mixture of samplers. Per-iteration cost can be higher for the mixture proposal, since αMH\alpha_{MH}αMH​ then needs the densities of all components; Proposition 5 isolates the statistical side of that trade-off. The maximality companion states the fact behind the name "maximal kernel": αMH\alpha_{MH}αMH​ is the largest acceptance probability that keeps a Metropolis–Hastings kernel reversible.

Formalizing it. The paper's proof is a computation of about six lines with Radon–Nikodym densities. A formal version must make explicit what the computation leaves implicit: that αMH\alpha_{MH}αMH​, defined from one dominating measure, has the same density form for every symmetric dominating measure; that the measure inequality on E×EE \times EE×E passes to the kernel-level statement with one null set for all AAA; and that the mixture proposal and the mixture of kernels are handled as countable sums of kernels. As of September 2026 neither Mathlib nor this platform has a machine-checked version of Proposition 5, of the maximality of αMH\alpha_{MH}αMH​, or of reversibility of the Metropolis–Hastings kernel on a general state space; only finite-state Metropolis chains have been formalized on the platform.

Difficulty

The obvious argument works pointwise with densities: write every kernel as a density against a common reference measure and compare min⁡{⋅,⋅}\min\{\cdot, \cdot\}min{⋅,⋅} of sums with sums of minima. On a general state space there is no common reference measure given in advance, and αMH\alpha_{MH}αMH​ is only defined up to μ\muμ-null sets, through a Radon–Nikodym derivative with respect to μ+μT\mu + \mu^Tμ+μT, a measure that differs for QQQ and for each QiQ_iQi​. The step that needs care is relating these different versions: the densities hih_ihi​ of the μi\mu_iμi​ against a common symmetric ν\nuν, the density of μ=∑iβiμi\mu = \sum_i \beta_i \mu_iμ=∑i​βi​μi​, and the transpose densities h(y,x)h(y, x)h(y,x), which are densities of μT\mu^TμT only because ν\nuν is symmetric.

The second difficulty is the passage from measures to kernels. The inequality between measures on E×EE \times EE×E gives, for each fixed AAA, the kernel inequality for π\piπ-almost every xxx, with a null set that depends on AAA. The order ⪰\succeq⪰ requires one null set for all AAA, and the diagonal must be removed, which needs the diagonal to be measurable.

Formalization scope

The formalization is in Lean 4 with Mathlib, in the namespace TierneyMH.Mixture. The state space is a type E with a σ-algebra; π is a probability measure; proposal kernels are Markov kernels Kernel E E. Acceptance probabilities and densities take values in [0,∞][0, \infty][0,∞] (ℝ≥0∞); a general α\alphaα is assumed measurable with α≤1\alpha \le 1α≤1. μ\muμ is π ⊗ₘ Q, μT\mu^TμT its image under Prod.swap, detailed balance is Kernel.IsReversible. Mixtures are indexed by a countable type ("a sequence", which includes finite families), with weights in ℝ≥0 and HasSum β 1.

Added hypotheses, both labelled in the statements: singletons are measurable (implicit in the paper's A∖{x}A \setminus \{x\}A∖{x} and δx\delta_xδx​), on the goal and the maximality companion; and, on the goal only, the σ-algebra of EEE is countably generated. The second is an addition to the paper: it is what makes the exceptional null set in ⪰\succeq⪰ uniform over AAA in the passage from the measure inequality to the kernels. It is not assumed in the measure-level milestones.

αMH\alpha_{MH}αMH​ is one fixed version, built from Mathlib's rnDeriv exactly as in the proof of Proposition 1 (with ν=μ+μT\nu = \mu + \mu^Tν=μ+μT, not an arbitrary dominating measure), and all statements are insensitive to the version. The ratio rrr is set to 1 on the null subset of RRR where hhh is infinite, so that 0<r<∞0 < r < \infty0<r<∞ and r(x,y)=1/r(y,x)r(x, y) = 1/r(y, x)r(x,y)=1/r(y,x) hold everywhere, as Proposition 1 asks.

Trivializations ruled out: αMH\alpha_{MH}αMH​ is the indicator of RRR times min⁡{1,r(y,x)}\min\{1, r(y, x)\}min{1,r(y,x)}, never an arbitrary acceptance function or a single α\alphaα shared by all components; ⪰\succeq⪰ compares A∖{x}A \setminus \{x\}A∖{x}, not AAA (on AAA the rejection masses differ and the comparison is false); and the conclusion is about the Metropolis–Hastings kernels themselves, not about the measure identity alone. All hypotheses are satisfiable, for instance on EEE = Bool with π\piπ uniform, two proposals Q1=πQ_1 = \piQ1​=π and Q2=δxQ_2 = \delta_xQ2​=δx​ and weights (1/2,1/2)(1/2, 1/2)(1/2,1/2).

Needed infrastructure, reusable for other Metropolis–Hastings results: Radon–Nikodym calculus for product measures and their transposes, countable sums of kernels, and a monotone-class argument over a countable generating family. The Metropolis–Hastings kernel, RRR, rrr and off-diagonal domination are defined identically in the companion missions I (detailed balance, Theorem 2) and II (Peskun ordering, Theorem 4) of this series. Proofs of milestones in any order, and proofs of the goal from the milestones, are welcome.

Selected references

  • L. Tierney, A Note on Metropolis–Hastings Kernels for General State Spaces, The Annals of Applied Probability 8(1), 1998, 1–9. https://doi.org/10.1214/aoap/1027961031
  • P. H. Peskun, Optimum Monte Carlo sampling using Markov chains, Biometrika 60(3), 1973, 607–612. https://doi.org/10.1093/biomet/60.3.607
  • J. Besag, P. Green, D. Higdon, K. Mengersen, Bayesian computation and stochastic systems (with discussion), Statistical Science 10(1), 1995, 3–66. https://doi.org/10.1214/ss/1177010123
  • W. K. Hastings, Monte Carlo sampling methods using Markov chains and their applications, Biometrika 57(1), 1970, 97–109. https://doi.org/10.1093/biomet/57.1.97
  • N. Metropolis, A. W. Rosenbluth, M. N. Rosenbluth, A. H. Teller, E. Teller, Equations of state calculations by fast computing machines, J. Chemical Physics 21, 1953, 1087–1091. https://doi.org/10.1063/1.1699114
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🏆Completed
Number TheoryProbabilityQuantum Information+1·Captain: mikedeng1

Polynomial-Time Algorithms for Prime Factorization and Discrete Logarithms on a Quantum Computer 4: The Discrete Logarithm Circuit Gives a Good Output with Probability at Least 1/480Research Paper

Motivation

The discrete logarithm problem modulo a prime asks, given a prime ppp, a generator ggg of the multiplicative group modulo ppp, and a nonzero residue xxx, for the exponent rrr with gr≡x(modp)g^r\equiv x \pmod pgr≡x(modp). Its presumed classical hardness underlies Diffie–Hellman key exchange, ElGamal encryption and the Digital Signature Algorithm. The best classical algorithm known when Shor wrote, Gordon's adaptation of the number field sieve, runs in time exp⁡(O((log⁡p)1/3(log⁡log⁡p)2/3))\exp(O((\log p)^{1/3}(\log\log p)^{2/3}))exp(O((logp)1/3(loglogp)2/3)).

In §6 of Polynomial-Time Algorithms for Prime Factorization and Discrete Logarithms on a Quantum Computer (SIAM J. Comput. 26(5), 1997; doi:10.1137/S0097539795293172, arXiv:quant-ph/9508027), Shor gave a quantum algorithm that uses two modular exponentiations and two quantum Fourier transforms and outputs, with constant probability, a pair from which rrr can be computed. The quantitative core of that analysis is a single number: the circuit produces a "good" output with probability at least 1/4801/4801/480. This mission formalizes that bound and the three estimates it is assembled from.

Setting

Let ppp be a prime and ggg a generator of (Z/pZ)×(\mathbb Z/p\mathbb Z)^\times(Z/pZ)×, so that 1,g,…,gp−21,g,\dots,g^{p-2}1,g,…,gp−2 are all the nonzero residues. Fix the unknown rrr with 0≤r<p−10\le r<p-10≤r<p−1 and put x=grx=g^rx=gr. Let q=2lq=2^lq=2l be the power of 222 with p<q<2pp<q<2pp<q<2p.

The Fourier matrix AqA_qAq​ is the q×qq\times qq×q matrix with entries (Aq)a,c=q−1/2exp⁡(2πi ac/q)(A_q)_{a,c}=q^{-1/2}\exp(2\pi i\,ac/q)(Aq​)a,c​=q−1/2exp(2πiac/q) for 0≤a,c<q0\le a,c<q0≤a,c<q (§4, eq. (4.1)). Rows index input basis vectors and columns output basis vectors.

The algorithm uses three registers: two holding numbers 0≤a,b<q0\le a,b<q0≤a,b<q and one holding a nonzero residue modulo ppp. It starts from the state

1p−1∑a=0p−2∑b=0p−2∣a,b,gax−b (mod p)⟩(6.1)\frac{1}{p-1}\sum_{a=0}^{p-2}\sum_{b=0}^{p-2}|a,b,g^ax^{-b}\ (\mathrm{mod}\ p)\rangle \qquad (6.1)p−11​a=0∑p−2​b=0∑p−2​∣a,b,gax−b (mod p)⟩(6.1)

(preFourierState), applies AqA_qAq​ to each of the first two registers (finalState), and measures all three registers. The probability of observing ∣c,d,y⟩|c,d,y\rangle∣c,d,y⟩ is the squared modulus of its amplitude (outcomeProb).

For integers zzz and q>0q>0q>0, the symmetric residue {z}q\{z\}_q{z}q​ is the residue of zzz modulo qqq in (−q/2,q/2](-q/2,q/2](−q/2,q/2] (symmRes). Put

T=rc+d−rp−1{c(p−1)}q.T=rc+d-\frac{r}{p-1}\{c(p-1)\}_q .T=rc+d−p−1r​{c(p−1)}q​.

An observed state ∣c,d,y⟩|c,d,y\rangle∣c,d,y⟩ is good (IsGood) when

∣{T}q∣≤12(6.10)and∣{c(p−1)}q∣≤q/12(6.11).|\{T\}_q|\le\tfrac12 \quad (6.10) \qquad\text{and}\qquad |\{c(p-1)\}_q|\le q/12 \quad (6.11).∣{T}q​∣≤21​(6.10)and∣{c(p−1)}q​∣≤q/12(6.11).

Goodness depends only on (c,d)(c,d)(c,d).

Formalization targets

Goal: a good output with probability at least 1/4801/4801/480 (§6, p. 1504)

∑0≤c,d<q(c,d) good ∑y∈(Z/p)×Pr⁡[c,d,y] ≥ 1480.\sum_{\substack{0\le c,d<q\\ (c,d)\ \text{good}}}\ \sum_{y\in(\mathbb Z/p)^\times}\Pr[c,d,y]\ \ge\ \frac1{480}.0≤c,d<q(c,d) good​∑​ y∈(Z/p)×∑​Pr[c,d,y] ≥ 4801​.

The constant is the one the page carries forward. The goal fixes no threshold on ppp: it is stated for every prime ppp that admits a power of two strictly between ppp and 2p2p2p.

Milestones

  1. The output distribution, eq. (6.4). For 0≤k<p−10\le k<p-10≤k<p−1,
Pr⁡[c,d,gk]=∣1(p−1)q∑0≤a,b≤p−2a−rb≡k (p−1)exp⁡(2πiq(ac+bd))∣2.\Pr[c,d,g^k]=\left|\frac{1}{(p-1)q}\sum_{\substack{0\le a,b\le p-2\\ a-rb\equiv k\ (p-1)}}\exp\Bigl(\frac{2\pi i}{q}(ac+bd)\Bigr)\right|^2 .Pr[c,d,gk]=​(p−1)q1​0≤a,b≤p−2a−rb≡k (p−1)​∑​exp(q2πi​(ac+bd))​2.
  1. Each good state is likely, eq. (6.17). If (c,d)(c,d)(c,d) is good, then Pr⁡[c,d,y]≥1/(20q2)\Pr[c,d,y]\ge 1/(20q^2)Pr[c,d,y]≥1/(20q2) for every yyy.
  2. Many good pairs (p. 1504). At least q/12q/12q/12 pairs (c,d)(c,d)(c,d) are good.
  3. Each good ccc is likely (p. 1504). If (c,d)(c,d)(c,d) is good for some ddd, then ∑d′,yPr⁡[c,d′,y]≥(p−1)/(20q2)≥1/(40q)\sum_{d',y}\Pr[c,d',y]\ge(p-1)/(20q^2)\ge1/(40q)∑d′,y​Pr[c,d′,y]≥(p−1)/(20q2)≥1/(40q).

Significance

The result. The bound 1/4801/4801/480 is what turns the circuit into an algorithm. Repeating the circuit O(1)O(1)O(1) times in expectation yields a good output, and from a good pair (c,d)(c,d)(c,d) one reads off an equation that determines rrr modulo divisors of p−1p-1p−1 (§6, eqs. (6.18)–(6.20)). Together with the quantum Fourier transform circuit and reversible modular exponentiation, this places the discrete logarithm modulo a prime in quantum polynomial time. Every later analysis of quantum attacks on discrete-logarithm cryptography starts from this success probability or a sharpened version of it.

Formalizing it. The result has been proved since 1994–1997 and is textbook material; it is not open. As far as is known, no machine-checked proof of Shor's discrete-logarithm analysis exists. The paper's proof of eq. (6.17) replaces a sum by an integral with an error term O(W/(pq))O(W/(pq))O(W/(pq)) whose constant is not given, yet states 1/(20q2)1/(20q^2)1/(20q2) for every prime. A formal proof must therefore either control that error explicitly or find another argument, and so settles a point the paper leaves informal. Numerically, the smallest value of q2Pr⁡[c,d,y]q^2\Pr[c,d,y]q2Pr[c,d,y] over good states is about 0.490.490.49 for all primes p<90p<90p<90, so the unconditional claim is not in doubt for small ppp. The page also contains two small slips, recorded under Formalization scope; a complete development pins down exactly what is true.

Difficulty

The exponential sum (6.4) runs over pairs (a,b)(a,b)(a,b) satisfying a congruence modulo p−1p-1p−1, while the phases are taken modulo qqq. The two moduli are unrelated: qqq is a power of two and p−1p-1p−1 is arbitrary. Eliminating aaa through the congruence introduces a floor function ⌊(br+k)/(p−1)⌋\lfloor(br+k)/(p-1)\rfloor⌊(br+k)/(p−1)⌋, and the resulting phase is not linear in bbb. The obvious estimate treats the sum as a geometric series in bbb and bounds it by its first-order phase; this fails because the floor term perturbs every phase by an amount of size up to ∣{c(p−1)}q∣|\{c(p-1)\}_q|∣{c(p−1)}q​∣. Condition (6.11) only keeps this perturbation within π/6\pi/6π/6 of the main phase; it does not remove it. The per-state bound must survive this perturbation uniformly in ppp, rrr and kkk, including small primes where the paper's integral approximation gives no explicit control.

The count of good pairs needs a separate argument about how often a multiple c(p−1)c(p-1)c(p−1) lies within q/12q/12q/12 of a multiple of qqq when gcd⁡(p−1,q)\gcd(p-1,q)gcd(p−1,q) is large.

Formalization scope

  • States are functions Fin q × Fin q × (ZMod p)ˣ → ℂ. The first two registers range over {0,…,q−1}\{0,\dots,q-1\}{0,…,q−1}; the third over the units modulo ppp.
  • Matrix convention. Following §2, rows are inputs, so the amplitude of ∣c,d,y⟩|c,d,y\rangle∣c,d,y⟩ after the transforms is ∑a,bψ(a,b,y)(Aq)a,c(Aq)b,d\sum_{a,b}\psi(a,b,y)(A_q)_{a,c}(A_q)_{b,d}∑a,b​ψ(a,b,y)(Aq​)a,c​(Aq​)b,d​. finalState is defined this way from (6.1) and AqA_qAq​. It is not typed in as the closed form (6.3) or (6.4). A formalization that defined the final state by (6.4) directly would make milestone 1 trivial, and is ruled out.
  • Probability of a basis state is the squared norm of its amplitude, with no normalization hypothesis.
  • Parameters. ppp is prime (Fact p.Prime). The generator is encoded as orderOf g = p - 1. r<p−1r<p-1r<p−1 is a parameter, with x=grx=g^rx=gr. qqq is given by q = 2 ^ l together with p<q<2pp<q<2pp<q<2p. No large-ppp threshold is added anywhere.
  • Arithmetic. x−bx^{-b}x−b is x⁻¹ ^ b in the unit group. p−1p-1p−1 is computed in Z\mathbb ZZ and R\mathbb RR inside TTT and the congruences, and as natural-number subtraction only where p≥2p\ge2p≥2 makes it exact. TTT is real.
  • Condition (6.10) is stated as "some integer jjj has ∣T−jq∣≤12|T-jq|\le\frac12∣T−jq∣≤21​". Because q≥4q\ge4q≥4, this is equivalent to the page's form with jjj the closest integer to T/qT/qT/q.
  • Not formalized. The preparation of (6.1) by testing and restarting is not formalized; the state (6.1) is taken as displayed. The printed test "whether the number is less than ppp" should read p−1p-1p−1, as the sums in (6.1) show. Also out of scope: the recovery of rrr (eqs. (6.18)–(6.20)), the repetition count "480t480t480t", and all running-time claims.
  • Printed slips.
    • The page asserts that for each ccc there is exactly one ddd satisfying (6.10). At a tie {T}q=±12\{T\}_q=\pm\frac12{T}q​=±21​ there can be two such ddd. Milestone 3 states only the count, which needs at least one.
    • The page's intermediate bound "at least p/(240q)p/(240q)p/(240q)" should be (p−1)/(240q)(p-1)/(240q)(p−1)/(240q). The conclusion 1/4801/4801/480 is unaffected, since qqq and 2p2p2p are both even and so q≤2(p−1)q\le 2(p-1)q≤2(p−1). Only 1/4801/4801/480 is stated.

Needed infrastructure: finite exponential sums and their modulus, the symmetric residue and its basic properties, and counting multiples in residue classes of Z/q\mathbb Z/qZ/q. The exponential-sum estimates of milestones 1 and 2 are reusable in the order-finding analysis of §5 of the same paper. Proofs of any milestone, of the normalization ∑Pr⁡=1\sum\Pr=1∑Pr=1, and of auxiliary lemmas about symmRes are welcome.

Selected references

  • P. W. Shor, Polynomial-Time Algorithms for Prime Factorization and Discrete Logarithms on a Quantum Computer, SIAM J. Comput. 26(5):1484–1509, 1997. https://doi.org/10.1137/S0097539795293172 (preprint: https://arxiv.org/abs/quant-ph/9508027)
  • D. M. Gordon, Discrete logarithms in GF(p) using the number field sieve, SIAM J. Discrete Math. 6(1):124–138, 1993. https://doi.org/10.1137/0406010
  • W. Diffie and M. E. Hellman, New directions in cryptography, IEEE Trans. Inform. Theory 22(6):644–654, 1976. https://doi.org/10.1109/TIT.1976.1055638
  • M. A. Nielsen and I. L. Chuang, Quantum Computation and Quantum Information, Cambridge University Press, 2000. https://doi.org/10.1017/CBO9780511976667
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AnalysisControl TheoryPartial Differential Equations·Captain: mikedeng1

Stability and Instability Results of the Wave Equation with a Delay Term in the Boundary or Internal Feedbacks IV: Arbitrarily Small Destabilizing Delays for Internal DampingResearch Paper

Motivation

Feedback laws in engineering are applied with a lag: sensors, actuators and communication channels introduce a time delay τ\tauτ between the measurement of a state and the control that reacts to it. For finite-dimensional systems small delays are usually harmless. For distributed systems such as the wave equation they need not be: Datko, Lagnese and Polis (SIAM J. Control Optim. 24, 1986) and Datko (SIAM J. Control Optim. 26, 1988) showed, for one-dimensional examples, that an arbitrarily small delay in a stabilizing feedback can destroy stability. The question matters to anyone who designs boundary or internal controllers for vibrating structures and wants to know whether a stabilizing law is robust to delay.

Nicaise and Pignotti (SIAM J. Control Optim. 45 (2006)) study the wave equation on a bounded domain of Rn\mathbb R^nRn with a damping term that combines an instantaneous and a delayed velocity feedback, with coefficients μ1\mu_1μ1​ and μ2\mu_2μ2​. They show that the system is exponentially stable when μ2<μ1\mu_2 < \mu_1μ2​<μ1​ (Theorems 1.1 and 1.3), and that when μ2≥μ1\mu_2 \ge \mu_1μ2​≥μ1​ stability can fail (Theorems 1.2 and 1.4). This mission is Theorem 1.4, the internal-damping instability result, in the case the paper proves.

  • 1986–1988: Datko, Lagnese and Polis; Datko — destabilization by small delays in one-dimensional boundary-damped wave equations.
  • 2006: Nicaise and Pignotti — the multi-dimensional dichotomy μ2<μ1\mu_2 < \mu_1μ2​<μ1​ (stability) versus μ2≥μ1\mu_2 \ge \mu_1μ2​≥μ1​ (instability for some delays), for boundary and internal feedback.

Setting

Let n≥1n \ge 1n≥1 and let Ω⊂Rn\Omega \subset \mathbb R^nΩ⊂Rn be a bounded open set with boundary Γ\GammaΓ of class C2C^2C2, split as Γ=ΓD∪ΓN\Gamma = \Gamma_D \cup \Gamma_NΓ=ΓD​∪ΓN​ with ΓD‾∩ΓN‾=∅\overline{\Gamma_D} \cap \overline{\Gamma_N} = \emptysetΓD​​∩ΓN​​=∅ and ΓD≠∅\Gamma_D \neq \emptysetΓD​=∅. Write ν\nuν for the outer unit normal and ∂u/∂ν\partial u/\partial\nu∂u/∂ν for the normal derivative. Let μ1>0\mu_1 > 0μ1​>0, μ2>0\mu_2 > 0μ2​>0 and let τ>0\tau > 0τ>0 be the delay. With damping coefficient a≡1a \equiv 1a≡1 the problem is

utt(x,t)−Δu(x,t)+μ1ut(x,t)+μ2ut(x,t−τ)=0in Ω×(0,∞),u_{tt}(x,t) - \Delta u(x,t) + \mu_1 u_t(x,t) + \mu_2 u_t(x,t-\tau) = 0 \quad \text{in } \Omega \times (0,\infty),utt​(x,t)−Δu(x,t)+μ1​ut​(x,t)+μ2​ut​(x,t−τ)=0in Ω×(0,∞), u=0  on ΓD×(0,∞),∂u∂ν=0  on ΓN×(0,∞),u = 0 \ \text{ on } \Gamma_D \times (0,\infty), \qquad \frac{\partial u}{\partial\nu} = 0 \ \text{ on } \Gamma_N \times (0,\infty),u=0  on ΓD​×(0,∞),∂ν∂u​=0  on ΓN​×(0,∞),

with initial data u(⋅,0)=u0u(\cdot,0) = u_0u(⋅,0)=u0​, ut(⋅,0)=u1u_t(\cdot,0) = u_1ut​(⋅,0)=u1​ and a history ut=g0u_t = g_0ut​=g0​ on Ω×(−τ,0)\Omega \times (-\tau, 0)Ω×(−τ,0). The standard energy of a solution is

E(t)=12∫Ω{∣ut(x,t)∣2+∣∇u(x,t)∣2} dx.\mathcal E(t) = \frac12 \int_\Omega \big\{ |u_t(x,t)|^2 + |\nabla u(x,t)|^2 \big\}\,dx .E(t)=21​∫Ω​{∣ut​(x,t)∣2+∣∇u(x,t)∣2}dx.

The condition μ2<μ1\mu_2 < \mu_1μ2​<μ1​ is the paper's assumption (1.8). The paper's problem (1.12)–(1.16) carries a general coefficient a∈L∞(Ω)a \in L^\infty(\Omega)a∈L∞(Ω) with a≥0a \ge 0a≥0 and a>a0>0a > a_0 > 0a>a0​>0 near ΓN\Gamma_NΓN​; a≡1a \equiv 1a≡1 is one such coefficient.

Formalization targets

Goal: Theorem 1.4 for a≡1a \equiv 1a≡1

If (1.8) fails, i.e. 0<μ1≤μ20 < \mu_1 \le \mu_20<μ1​≤μ2​, then

∀ε>0 ∃τ∈(0,ε) ∃u solving the problem with delay τ:  E(t)↛0 (t→∞),\forall \varepsilon > 0\ \exists \tau \in (0,\varepsilon)\ \exists u \text{ solving the problem with delay } \tau:\ \ \mathcal E(t) \not\to 0 \ (t \to \infty),∀ε>0 ∃τ∈(0,ε) ∃u solving the problem with delay τ:  E(t)→0 (t→∞),

and the same holds with "τ∈(0,ε)\tau \in (0,\varepsilon)τ∈(0,ε)" replaced by "τ>M\tau > Mτ>M", for every MMM. The goal asserts only non-decay, not a rate of growth or the value of the energy, so it survives any sharpening of the examples.

Milestones

  1. (5.21)–(5.23): if φ\varphiφ is an eigenfunction of the mixed Dirichlet–Neumann Laplacian, Δφ=−Λ2φ\Delta\varphi = -\Lambda^2\varphiΔφ=−Λ2φ, and λ∈C\lambda \in \mathbb Cλ∈C solves λ2+(μ1+μ2e−λτ)λ=−Λ2\lambda^2 + (\mu_1 + \mu_2 e^{-\lambda\tau})\lambda = -\Lambda^2λ2+(μ1​+μ2​e−λτ)λ=−Λ2, then eλtφ(x)e^{\lambda t}\varphi(x)eλtφ(x) is a solution.
  2. (5.24)–(5.25): with λ=α+iβ\lambda = \alpha + i\betaλ=α+iβ and βτ=(2l+1)π\beta\tau = (2l+1)\piβτ=(2l+1)π, that equation is equivalent to α2+β2=Λ2\alpha^2 + \beta^2 = \Lambda^2α2+β2=Λ2, μ2e−ατ=2α+μ1\mu_2 e^{-\alpha\tau} = 2\alpha + \mu_1μ2​e−ατ=2α+μ1​.
  3. Case (a), μ1=μ2\mu_1 = \mu_2μ1​=μ2​: the system forces α=0\alpha = 0α=0 and β2=Λ2\beta^2 = \Lambda^2β2=Λ2.
  4. Case (b), μ2>μ1\mu_2 > \mu_1μ2​>μ1​, (5.26)–(5.27): for every Λ>0\Lambda > 0Λ>0 and lll there is α∈(0,(μ2−μ1)/2)\alpha \in (0, (\mu_2-\mu_1)/2)α∈(0,(μ2​−μ1​)/2) with τ(α)=α−1ln⁡(μ2/(μ1+2α))>0\tau(\alpha) = \alpha^{-1}\ln(\mu_2/(\mu_1+2\alpha)) > 0τ(α)=α−1ln(μ2​/(μ1​+2α))>0 solving the system.
  5. Energy of separated solutions (p. 1584): E(t)=e2 Re(λ)t E(0)\mathcal E(t) = e^{2\,\mathrm{Re}(\lambda)t}\,\mathcal E(0)E(t)=e2Re(λ)tE(0) with E(0)>0\mathcal E(0) > 0E(0)>0.
  6. Delay bounds (p. 1585, corrected): (2l+1)π/Λ<τ<(2l+1)π/Λ2−(μ2−μ1)2/4(2l+1)\pi/\Lambda < \tau < (2l+1)\pi/\sqrt{\Lambda^2 - (\mu_2-\mu_1)^2/4}(2l+1)π/Λ<τ<(2l+1)π/Λ2−(μ2​−μ1​)2/4​, the second when Λ2>(μ2−μ1)2/4\Lambda^2 > (\mu_2-\mu_1)^2/4Λ2>(μ2​−μ1​)2/4.

Significance

The result shows that the stability threshold μ2<μ1\mu_2 < \mu_1μ2​<μ1​ of Theorem 1.3 is sharp in the sense that matters for design: at or beyond the threshold there is no delay margin, since delays as small as desired already produce solutions whose energy does not decay. Together with Theorem 1.3 it gives a complete dichotomy in the coefficients (μ1,μ2)(\mu_1,\mu_2)(μ1​,μ2​) for the internally damped wave equation with delay, in any dimension, and it identifies the mechanism (roots of the characteristic equation on or to the right of the imaginary axis) that later work on delayed stabilization has had to avoid.

The result is proved in the paper; to the best of current knowledge it has not been machine-checked. The mission's product is a formal proof of the a≡1a \equiv 1a≡1 case together with its algebraic core: the reduction of the transcendental characteristic equation, the analysis of both cases, and the two-sided bounds on the delays. The spectral input it needs, an unbounded sequence of eigenvalues of the mixed Dirichlet–Neumann Laplacian with regular eigenfunctions, is reusable well beyond this paper.

Difficulty

The scalar part is elementary. The difficulty is the spectral input. The small delays come from τn,l≈(2l+1)π/Λn\tau_{n,l} \approx (2l+1)\pi/\Lambda_nτn,l​≈(2l+1)π/Λn​ with Λn→∞\Lambda_n \to \inftyΛn​→∞, so the proof needs infinitely many eigenvalues Λn2→∞\Lambda_n^2 \to \inftyΛn2​→∞ of the Laplacian with mixed Dirichlet–Neumann conditions on a C2C^2C2 domain, with eigenfunctions that are C2C^2C2 inside and C1C^1C1 up to the boundary. This requires compactness of the embedding HΓD1(Ω)↪L2(Ω)H^1_{\Gamma_D}(\Omega) \hookrightarrow L^2(\Omega)HΓD​1​(Ω)↪L2(Ω), the spectral theorem for compact self-adjoint operators, and elliptic regularity for a mixed problem, none of which is available in Mathlib for domains in Rn\mathbb R^nRn. A single eigenpair gives only the large delays (letting l→∞l \to \inftyl→∞); it does not give the small ones.

A second point: the paper's own bound (2l+1)2π2/τn,l2≤Λn2(2l+1)^2\pi^2/\tau_{n,l}^2 \le \Lambda_n^2(2l+1)2π2/τn,l2​≤Λn2​ bounds τn,l\tau_{n,l}τn,l​ only from below, so it does not by itself give τn,l→0\tau_{n,l} \to 0τn,l​→0; the upper bound of milestone 6 is needed.

Formalization scope

  • Space: Rn\mathbb R^nRn is EuclideanSpace ℝ (Fin n) with n≥1n \ge 1n≥1. The C2C^2C2 boundary is given by a global C2C^2C2 defining function ψ\psiψ (Ω={ψ<0}\Omega = \{\psi < 0\}Ω={ψ<0}, ∂Ω={ψ=0}\partial\Omega = \{\psi = 0\}∂Ω={ψ=0}, ∇ψ≠0\nabla\psi \ne 0∇ψ=0 on ∂Ω\partial\Omega∂Ω); ν=∇ψ/∣∇ψ∣\nu = \nabla\psi/|\nabla\psi|ν=∇ψ/∣∇ψ∣; the surface measure is pinned by the Gauss–Green formula for all C1C^1C1 fields.
  • Solutions are complex valued functions u(x,t)u(x,t)u(x,t) defined for all t∈Rt \in \mathbb Rt∈R, C2C^2C2 on Ω×R\Omega \times \mathbb RΩ×R and C1C^1C1 on Ω‾×R\overline\Omega \times \mathbb RΩ×R; the equation and boundary conditions hold for t>0t > 0t>0; initial data and history are the traces of uuu. The Neumann condition uses the derivative within Ω‾\overline\OmegaΩ. ∣∇u∣2|\nabla u|^2∣∇u∣2 is the sum of the squared moduli of the partial derivatives.
  • Corrected scope: Theorem 1.4 is printed for a general aaa satisfying (1.17)–(1.18); §5.2 proves it only for a≡1a \equiv 1a≡1, which is what is stated.
  • Corrected slips: (5.22) prints Δφ=−μ2φ\Delta\varphi = -\mu^2\varphiΔφ=−μ2φ for −Λ2φ-\Lambda^2\varphi−Λ2φ; p. 1584 prints eα+iβφ(x)e^{\alpha+i\beta}\varphi(x)eα+iβφ(x) for e(α+iβ)tφ(x)e^{(\alpha+i\beta)t}\varphi(x)e(α+iβ)tφ(x); the p. 1585 bound is supplemented by the upper bound of milestone 6. Milestone texts are quoted verbatim, including the slips.
  • The standing hypotheses (1.6)–(1.7) and the constant ξ\xiξ of (1.10) are not used by §5.2 and are omitted, which strengthens the statements.
  • A trivializing formalization is ruled out: the goal's conclusion E↛0\mathcal E \not\to 0E→0 excludes u≡0u \equiv 0u≡0, the energy integrand is continuous on the compact Ω‾\overline\OmegaΩ so the integral is genuine, and the normal derivative is taken within Ω‾\overline\OmegaΩ so the Neumann condition is not satisfied by a junk value.
  • No statement assumes the existence of eigenvalues; supplying the spectral theory of the mixed Laplacian is part of the goal. Contributions welcome: the spectral theorem for the mixed Dirichlet–Neumann Laplacian on a bounded C2C^2C2 domain, boundary regularity of its eigenfunctions, and the energy identity for separated solutions.

Selected references

  • S. Nicaise, C. Pignotti, Stability and instability results of the wave equation with a delay term in the boundary or internal feedbacks, SIAM J. Control Optim. 45(5):1561–1585, 2006. https://doi.org/10.1137/060648891
  • R. Datko, Not all feedback stabilized hyperbolic systems are robust with respect to small time delays in their feedbacks, SIAM J. Control Optim. 26:697–713, 1988.
  • R. Datko, J. Lagnese, M. P. Polis, An example on the effect of time delays in boundary feedback stabilization of wave equations, SIAM J. Control Optim. 24:152–156, 1986.
  • P. Grisvard, Elliptic Problems in Nonsmooth Domains, Pitman, 1985 (regularity of mixed boundary value problems).
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AnalysisControl TheoryPartial Differential Equations·Captain: mikedeng1

Stability and Instability Results of the Wave Equation with a Delay Term in the Boundary or Internal Feedbacks III: Destabilizing Delays for Boundary FeedbackResearch Paper

Motivation

Boundary feedback stabilization of the wave equation asks whether a damping term placed on part of the boundary drives the energy of every solution to zero. Without delay the answer is classical: the feedback ∂u/∂ν=−μ1ut\partial u/\partial\nu = -\mu_1 u_t∂u/∂ν=−μ1​ut​ on a part ΓN\Gamma_NΓN​ of the boundary gives exponential energy decay under geometric conditions (Chen, Lagnese, Lasiecka–Triggiani, Komornik–Zuazua). In practice a feedback is applied with a lag, and a small lag can destroy stability. Datko, Lagnese and Polis (doi:10.1137/0324007) and Datko (doi:10.1137/0326040) showed, in one space dimension, that a purely delayed boundary feedback destabilizes the system for arbitrarily small delays.

Nicaise and Pignotti (doi:10.1137/060648891) study a feedback made of an instantaneous part and a delayed part, with weights μ1\mu_1μ1​ and μ2\mu_2μ2​, in any space dimension. Their Theorem 1.1 gives exponential decay when μ2<μ1\mu_2 < \mu_1μ2​<μ1​. This mission formalizes the converse, Theorem 1.2: when μ2≥μ1\mu_2 \ge \mu_1μ2​≥μ1​, some delays admit solutions whose energy does not decay at all.

Timeline.

  • 1986: Datko, Lagnese and Polis, a one-dimensional wave equation whose delayed boundary feedback is unstable.
  • 1988: Datko, instability under arbitrarily small delays for a class of hyperbolic systems.
  • 2006: Xu, Yung and Li (doi:10.1051/cocv:2006021), one space dimension, by spectral analysis: stability for μ2<μ1\mu_2 < \mu_1μ2​<μ1​, instability for μ2>μ1\mu_2 > \mu_1μ2​>μ1​, possible instabilities for μ1=μ2\mu_1 = \mu_2μ1​=μ2​.
  • 2006: Nicaise and Pignotti, the same dichotomy in any dimension nnn, with explicit destabilizing delays built from eigenfunctions (§5.1).

Setting

Let n≥1n \ge 1n≥1 and let Ω⊂Rn\Omega \subset \mathbb R^nΩ⊂Rn be a bounded open set with boundary Γ\GammaΓ of class C2C^2C2. The boundary is split as Γ=ΓD∪ΓN\Gamma = \Gamma_D \cup \Gamma_NΓ=ΓD​∪ΓN​, with ΓD‾∩ΓN‾=∅\overline{\Gamma_D} \cap \overline{\Gamma_N} = \emptysetΓD​​∩ΓN​​=∅ and ΓD≠∅\Gamma_D \neq \emptysetΓD​=∅. Write ν\nuν for the outer unit normal and dΓd\GammadΓ for the surface measure. Together these data form a mixed domain (MixedDomain n in Lean).

Fix μ1,μ2>0\mu_1, \mu_2 > 0μ1​,μ2​>0 and a delay τ>0\tau > 0τ>0. The problem (1.1)–(1.3) is

{utt(x,t)−Δu(x,t)=0in Ω×(0,+∞),u(x,t)=0on ΓD×(0,+∞),∂u∂ν(x,t)=−μ1ut(x,t)−μ2ut(x,t−τ)on ΓN×(0,+∞),\begin{cases} u_{tt}(x,t) - \Delta u(x,t) = 0 & \text{in } \Omega \times (0,+\infty),\\ u(x,t) = 0 & \text{on } \Gamma_D \times (0,+\infty),\\ \dfrac{\partial u}{\partial\nu}(x,t) = -\mu_1 u_t(x,t) - \mu_2 u_t(x,t-\tau) & \text{on } \Gamma_N \times (0,+\infty), \end{cases}⎩⎨⎧​utt​(x,t)−Δu(x,t)=0u(x,t)=0∂ν∂u​(x,t)=−μ1​ut​(x,t)−μ2​ut​(x,t−τ)​in Ω×(0,+∞),on ΓD​×(0,+∞),on ΓN​×(0,+∞),​

with initial data u(⋅,0)u(\cdot,0)u(⋅,0), ut(⋅,0)u_t(\cdot,0)ut​(⋅,0) and a history utu_tut​ on ΓN×(−τ,0)\Gamma_N \times (-\tau,0)ΓN​×(−τ,0) (1.4)–(1.5). The standard energy of a solution is (3.7)

E(t)=12∫Ω(∣ut(x,t)∣2+∣∇u(x,t)∣2) dx.\mathcal E(t) = \frac12\int_\Omega \big(|u_t(x,t)|^2 + |\nabla u(x,t)|^2\big)\,dx .E(t)=21​∫Ω​(∣ut​(x,t)∣2+∣∇u(x,t)∣2)dx.

Condition (1.8) of the paper is μ2<μ1\mu_2 < \mu_1μ2​<μ1​. This mission concerns the complementary case μ2≥μ1\mu_2 \ge \mu_1μ2​≥μ1​.

For real functions www on Ω\OmegaΩ, (5.11) defines q0(w)=∫ΓN∣w∣2 dΓq_0(w) = \int_{\Gamma_N} |w|^2\,d\Gammaq0​(w)=∫ΓN​​∣w∣2dΓ and q1(w)=∫Ω∣∇w∣2 dxq_1(w) = \int_\Omega |\nabla w|^2\,dxq1​(w)=∫Ω​∣∇w∣2dx.

Formalization targets

Goal: Theorem 1.2 (p. 1563)

If μ2≥μ1\mu_2 \ge \mu_1μ2​≥μ1​, there exist delays 0<τ0<τ1<⋯0 < \tau_0 < \tau_1 < \cdots0<τ0​<τ1​<⋯ and, for each kkk, a classical solution uku_kuk​ of (1.1)–(1.3) with delay τk\tau_kτk​ and a constant ck>0c_k > 0ck​>0 such that

Ek(t)=ckfor all t≥0.\mathcal E_k(t) = c_k \qquad \text{for all } t \ge 0 .Ek​(t)=ck​for all t≥0.

The statement fixes no formula for the delays and no value of the energy. It asserts only the existence of infinitely many delays for which the energy does not decay.

Milestones

  1. (5.1)–(5.2), pp. 1579–1580. If λ∈C\lambda \in \mathbb Cλ∈C and φ\varphiφ solves −Δφ+λ2φ=0-\Delta\varphi + \lambda^2\varphi = 0−Δφ+λ2φ=0 in Ω\OmegaΩ, φ=0\varphi = 0φ=0 on ΓD\Gamma_DΓD​ and ∂φ/∂ν=−(μ1+μ2e−λτ)λφ\partial\varphi/\partial\nu = -(\mu_1 + \mu_2 e^{-\lambda\tau})\lambda\varphi∂φ/∂ν=−(μ1​+μ2​e−λτ)λφ on ΓN\Gamma_NΓN​, then u=eλtφu = e^{\lambda t}\varphiu=eλtφ solves (1.1)–(1.3).
  2. (5.5)–(5.7), pp. 1580 and 1582. For b>0b > 0b>0, l∈Nl \in \mathbb Nl∈N and bτ=arccos⁡(−μ1/μ2)+2lπb\tau = \arccos(-\mu_1/\mu_2) + 2l\pibτ=arccos(−μ1​/μ2​)+2lπ:
cos⁡(bτ)=−μ1/μ2,μ2sin⁡(bτ)=μ22−μ12,(μ1+μ2e−ibτ) ib=bμ22−μ12.\cos(b\tau) = -\mu_1/\mu_2,\qquad \mu_2\sin(b\tau) = \sqrt{\mu_2^2-\mu_1^2},\qquad (\mu_1 + \mu_2e^{-ib\tau})\,ib = b\sqrt{\mu_2^2-\mu_1^2}.cos(bτ)=−μ1​/μ2​,μ2​sin(bτ)=μ22​−μ12​​,(μ1​+μ2​e−ibτ)ib=bμ22​−μ12​​.
  1. Case (a), μ1=μ2\mu_1 = \mu_2μ1​=μ2​, p. 1581. For a normalized mixed Dirichlet–Neumann eigenfunction φ\varphiφ with −Δφ=b2φ-\Delta\varphi = b^2\varphi−Δφ=b2φ and τ=(2l+1)π/b\tau = (2l+1)\pi/bτ=(2l+1)π/b, the function u=eibtφu = e^{ibt}\varphiu=eibtφ is a solution and
∫Ω(∣∇u∣2+∣ut∣2) dx=2b2(t≥0).\int_\Omega(|\nabla u|^2 + |u_t|^2)\,dx = 2b^2 \quad (t \ge 0).∫Ω​(∣∇u∣2+∣ut​∣2)dx=2b2(t≥0).
  1. Case (b), μ2>μ1\mu_2 > \mu_1μ2​>μ1​, pp. 1581–1582. A normalized minimizer φ\varphiφ of s q0(w)+s2q0(w)2+4q1(w)s\,q_0(w) + \sqrt{s^2q_0(w)^2 + 4q_1(w)}sq0​(w)+s2q0​(w)2+4q1​(w)​, where s=μ22−μ12s = \sqrt{\mu_2^2-\mu_1^2}s=μ22​−μ12​​, solves the variational problem (5.7) with 2b2b2b equal to the minimum value.

Significance

The result. Theorem 1.2 shows that the threshold μ2<μ1\mu_2 < \mu_1μ2​<μ1​ of Theorem 1.1 is sharp in the following sense: once the delayed weight reaches the instantaneous one, no geometric assumption restores asymptotic stability for every delay. Together, Theorems 1.1 and 1.2 separate robust from non-robust boundary feedbacks by a single inequality between the two gains. The explicit delays of case (a), τn,l=(2l+1)π/bn\tau_{n,l} = (2l+1)\pi/b_nτn,l​=(2l+1)π/bn​, become arbitrarily small or large. So even an arbitrarily short lag in an equally weighted feedback can remove decay.

The formalization. The paper proves the result. It has not been formalized, and Mathlib has no wave equation on domains, no mixed eigenvalue problems and no Sobolev spaces on domains. This mission produces:

  • a machine-checked statement of the instability half of the paper's dichotomy;
  • the reduction to a spectral problem as separate, checkable steps;
  • a precise record of what the paper leaves implicit. In case (b) the existence of the minimizer is assumed ("if the minimum … is attained"), and in case (a) the existence of Dirichlet–Neumann eigenfunctions is quoted.

Difficulty

Milestones 1 and 2 are calculus and trigonometry. The difficulty sits in producing φ\varphiφ. The goal needs a nonzero function φ\varphiφ that is C2C^2C2 in Ω\OmegaΩ and C1C^1C1 up to the boundary and solves an eigenvalue problem with mixed Dirichlet and Neumann (case (a)) or Dirichlet and Robin-type (case (b)) boundary conditions. Existence requires compactness of HΓD1(Ω)↪L2(Ω)H^1_{\Gamma_D}(\Omega) \hookrightarrow L^2(\Omega)HΓD​1​(Ω)↪L2(Ω) and of the trace into L2(ΓN)L^2(\Gamma_N)L2(ΓN​), followed by elliptic regularity up to a C2C^2C2 boundary. None of these is in Mathlib.

A shortcut does not work: in case (b) the frequency bbb enters the boundary condition, so φ\varphiφ is not an eigenfunction of a fixed self-adjoint operator. The page instead minimizes a non-quadratic functional, and its first-variation computation (5.18)–(5.19) needs care: the functional is not 2-homogeneous, so the normalization by 1+ε2∥v∥21 + \varepsilon^2\|v\|^21+ε2∥v∥2 does not literally give g(ε)≥g(0)g(\varepsilon) \ge g(0)g(ε)≥g(0), although the first-order condition is right.

Taking real parts does not give a real-valued solution with constant energy: in case (b) the energy of cos⁡(bt)φ\cos(bt)\varphicos(bt)φ oscillates.

Formalization scope

  • Solutions are complex-valued, u:Rn×R→Cu : \mathbb R^n \times \mathbb R \to \mathbb Cu:Rn×R→C, as the page's eλtφe^{\lambda t}\varphieλtφ with λ∈C\lambda \in \mathbb Cλ∈C are. ∣ut∣2|u_t|^2∣ut​∣2 and ∣∇u∣2=∑i∣∂iu∣2|\nabla u|^2 = \sum_i |\partial_i u|^2∣∇u∣2=∑i​∣∂i​u∣2 are squared moduli.
  • Classical solutions. A solution is C2C^2C2 on Ω×R\Omega \times \mathbb RΩ×R and C1C^1C1 on Ω‾×R\overline\Omega \times \mathbb RΩ×R. It solves the equations for t>0t > 0t>0, and its values at t≤0t \le 0t≤0 are the initial data and history. The normal derivative is the derivative within Ω‾\overline\OmegaΩ applied to ν\nuν. C2C^2C2 regularity up to the boundary is not required, because eigenfunctions of mixed problems generally lack it.
  • The domain. The C2C^2C2 boundary is given by a global defining function ψ\psiψ with Ω={ψ<0}\Omega = \{\psi < 0\}Ω={ψ<0}. The surface measure is pinned down by the Gauss–Green formula for all C1C^1C1 vector fields, which determines it uniquely.
  • Dropped hypotheses. The geometric hypotheses (1.6)–(1.7) and the parameter ξ\xiξ of (1.10) are not used in §5.1 and are omitted. This strengthens the statements.
  • Sobolev spaces. HΓD1(Ω)H^1_{\Gamma_D}(\Omega)HΓD​1​(Ω) is replaced in milestone 4 by the class of real functions that are C2C^2C2 in Ω\OmegaΩ, C1C^1C1 on Ω‾\overline\OmegaΩ and zero on ΓD\Gamma_DΓD​, both as the minimization class and as the test class.
  • Non-triviality. The goal requires the constant energy to be positive and the delays to be strictly increasing. Without positivity, the zero solution would satisfy "constant energy". Without strict monotonicity, one delay repeated would count as a sequence.

A complete development needs the following:

  • Green's first identity on C2C^2C2 domains for functions that are C1C^1C1 up to the boundary;
  • existence and regularity of eigenfunctions of the Laplacian with mixed boundary conditions;
  • in case (b), existence of the minimizer (Rellich compactness and the trace theorem).

These pieces are reusable well beyond this mission. Contributions of any of them, or of an alternative route to a φ\varphiφ with the required properties, are welcome.

Selected references

  • S. Nicaise, C. Pignotti, Stability and instability results of the wave equation with a delay term in the boundary or internal feedbacks, SIAM J. Control Optim. 45(5):1561–1585, 2006. https://doi.org/10.1137/060648891
  • R. Datko, J. Lagnese, M. P. Polis, An example on the effect of time delays in boundary feedback stabilization of wave equations, SIAM J. Control Optim. 24:152–156, 1986. https://doi.org/10.1137/0324007
  • R. Datko, Not all feedback stabilized hyperbolic systems are robust with respect to small time delays in their feedbacks, SIAM J. Control Optim. 26:697–713, 1988. https://doi.org/10.1137/0326040
  • G. Q. Xu, S. P. Yung, L. K. Li, Stabilization of wave systems with input delay in the boundary control, ESAIM Control Optim. Calc. Var. 12:770–785, 2006. https://doi.org/10.1051/cocv:2006021
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Operations ResearchOptimization·Captain: mikedeng1

Global Convergence of Splitting Methods for Nonconvex Composite Optimization IV: Descent and Stationary Cluster Points of the Proximal Gradient MethodResearch Paper

Motivation

Many problems in statistics, signal processing and machine learning minimize a sum of a smooth loss and a nonsmooth regularizer: least squares with an ℓ0\ell_0ℓ0​ or ℓ1/2\ell_{1/2}ℓ1/2​ penalty, and constrained problems in which the regularizer is the indicator of a nonconvex set. The proximal gradient method (also called forward–backward splitting) is the standard first-order algorithm for such problems. Each step takes a gradient step on the smooth part and then applies the proximal mapping of the nonsmooth part, which for many nonconvex regularizers (hard thresholding, projection onto sparse vectors) has a closed form.

For a smooth part hhh whose gradient is LLL-Lipschitz, the classical analysis allows any constant step size β∈(0,1/L)\beta \in (0, 1/L)β∈(0,1/L), and every cluster point of the iterates is stationary; Li and Pong cite Bredies and Lorenz (Minimization of non-convex, non-smooth functionals by iterative thresholding, preprint, 2009) for this. Attouch, Bolte and Svaiter (Math. Program., 2013) added convergence of the whole sequence when h+Ph + Ph+P has the Kurdyka–Łojasiewicz property. When hhh is nonconvex, however, LLL is governed by the most negative curvature of hhh as much as by the most positive one, and the admissible step sizes can be much smaller than the convex part of hhh alone would require.

Li and Pong (SIAM J. Optim., 2015; preprint arXiv:1407.0753v6) show that the concave part of hhh imposes no restriction on the step size: it suffices to bound the curvature of hhh after it has been offset by a convex function. This mission formalizes that result, Theorem 4 of their paper. It is the fourth mission of a series on the paper; the first three treat its results on the alternating direction method of multipliers.

Setting

Work in Rn\mathbb{R}^nRn with the Euclidean inner product ⟨⋅,⋅⟩\langle\cdot,\cdot\rangle⟨⋅,⋅⟩ and norm ∥⋅∥\|\cdot\|∥⋅∥. The problem is

min⁡x∈Rn  h(x)+P(x),\min_{x \in \mathbb{R}^n}\; h(x) + P(x),x∈Rnmin​h(x)+P(x),

under the paper's standing assumptions: h:Rn→Rh : \mathbb{R}^n \to \mathbb{R}h:Rn→R is twice continuously differentiable with a bounded Hessian ∇2h\nabla^2 h∇2h; P:Rn→(−∞,+∞]P : \mathbb{R}^n \to (-\infty, +\infty]P:Rn→(−∞,+∞] is proper (never −∞-\infty−∞, finite somewhere) and closed (lower semicontinuous); and for every τ>0\tau > 0τ>0 and uuu the proximal problem min⁡yτP(y)+12∥y−u∥2\min_y \tau P(y) + \frac12\|y - u\|^2miny​τP(y)+21​∥y−u∥2 has a minimizer. Neither hhh nor PPP is assumed convex.

A vector vvv is a regular subgradient of PPP at xxx (with P(x)<∞P(x) < \inftyP(x)<∞) if P(z)≥P(x)+⟨v,z−x⟩−ε∥z−x∥P(z) \ge P(x) + \langle v, z - x\rangle - \varepsilon\|z - x\|P(z)≥P(x)+⟨v,z−x⟩−ε∥z−x∥ for all zzz near xxx, for every ε>0\varepsilon > 0ε>0. The limiting subdifferential ∂P(x)\partial P(x)∂P(x) collects the limits v=lim⁡vtv = \lim v^tv=limvt of regular subgradients vtv^tvt at points xt→xx^t \to xxt→x with P(xt)→P(x)P(x^t) \to P(x)P(xt)→P(x). A point xxx is stationary if

0∈∇h(x)+∂P(x).0 \in \nabla h(x) + \partial P(x).0∈∇h(x)+∂P(x).

Given a step size β>0\beta > 0β>0 and an arbitrary starting point x0x^0x0, the proximal gradient method generates (xt)t≥0(x^t)_{t \ge 0}(xt)t≥0​ by

xt+1∈Arg min⁡x{⟨∇h(xt),x−xt⟩+12β∥x−xt∥2+P(x)}.(43)x^{t+1} \in \operatorname*{Arg\,min}_x \Bigl\{ \langle \nabla h(x^t), x - x^t\rangle + \frac{1}{2\beta}\|x - x^t\|^2 + P(x) \Bigr\}. \tag{43}xt+1∈xArgmin​{⟨∇h(xt),x−xt⟩+2β1​∥x−xt∥2+P(x)}.(43)

Any minimizer may be selected. A cluster point of (xt)(x^t)(xt) is the limit of a subsequence xtix^{t_i}xti​.

The step-size condition involves a convex function qqq and a constant ℓ>0\ell > 0ℓ>0 with

−ℓI⪯∇2h(x)+∇2q(x)⪯ℓIfor all x,(44)-\ell I \preceq \nabla^2 h(x) + \nabla^2 q(x) \preceq \ell I \quad \text{for all } x, \tag{44}−ℓI⪯∇2h(x)+∇2q(x)⪯ℓIfor all x,(44)

where ⪯\preceq⪯ is the Loewner order on symmetric linear maps.

Formalization targets

Goal: Theorem 4

Suppose qqq is twice continuously differentiable and convex, ℓ>0\ell > 0ℓ>0, (44) holds, and (xt)(x^t)(xt) is generated by (43) with β∈(0,1/ℓ)\beta \in (0, 1/\ell)β∈(0,1/ℓ). Then

h(xt+1)+P(xt+1)≤h(xt)+P(xt)for all t,h(x^{t+1}) + P(x^{t+1}) \le h(x^t) + P(x^t) \quad \text{for all } t,h(xt+1)+P(xt+1)≤h(xt)+P(xt)for all t,

and every cluster point x∗x^*x∗ of (xt)(x^t)(xt), if one exists, satisfies 0∈∇h(x∗)+∂P(x∗)0 \in \nabla h(x^*) + \partial P(x^*)0∈∇h(x∗)+∂P(x∗).

The goal does not assert that a cluster point exists, nor that the whole sequence converges; both are false without further assumptions.

Milestones

In the order of the paper's proof:

  1. Eq. (3): robustness of ∂\partial∂ under xt→xx^t \to xxt→x, f(xt)→f(x)f(x^t) \to f(x)f(xt)→f(x), vt→vv^t \to vvt→v.
  2. Eq. (45): under (44), (h+q)(v)≤(h+q)(u)+⟨∇h(u)+∇q(u),v−u⟩+ℓ2∥v−u∥2(h+q)(v) \le (h+q)(u) + \langle \nabla h(u) + \nabla q(u), v - u\rangle + \frac{\ell}{2}\|v - u\|^2(h+q)(v)≤(h+q)(u)+⟨∇h(u)+∇q(u),v−u⟩+2ℓ​∥v−u∥2.
  3. Eq. (46): h(xt+1)+P(xt+1)≤h(xt)+P(xt)+(ℓ2−12β)∥xt+1−xt∥2h(x^{t+1}) + P(x^{t+1}) \le h(x^t) + P(x^t) + \bigl(\frac{\ell}{2} - \frac{1}{2\beta}\bigr)\|x^{t+1} - x^t\|^2h(xt+1)+P(xt+1)≤h(xt)+P(xt)+(2ℓ​−2β1​)∥xt+1−xt∥2.
  4. The summed bound after (46): (12β−ℓ2)∑t=0N−1∥xt+1−xt∥2+h(xN)+P(xN)≤h(x0)+P(x0)\bigl(\frac{1}{2\beta} - \frac{\ell}{2}\bigr)\sum_{t=0}^{N-1}\|x^{t+1} - x^t\|^2 + h(x^N) + P(x^N) \le h(x^0) + P(x^0)(2β1​−2ℓ​)∑t=0N−1​∥xt+1−xt∥2+h(xN)+P(xN)≤h(x0)+P(x0).
  5. Vanishing steps: if a cluster point exists, ∥xt+1−xt∥→0\|x^{t+1} - x^t\| \to 0∥xt+1−xt∥→0.
  6. Function-value convergence: if xti→x∗x^{t_i} \to x^*xti​→x∗, then P(xti+1)→P(x∗)P(x^{t_i+1}) \to P(x^*)P(xti​+1)→P(x∗).
  7. Eq. (47): 0∈∇h(xt)+1β(xt+1−xt)+∂P(xt+1)0 \in \nabla h(x^t) + \frac{1}{\beta}(x^{t+1} - x^t) + \partial P(x^{t+1})0∈∇h(xt)+β1​(xt+1−xt)+∂P(xt+1) for every ttt.

Significance

The result. For h=h1−h2h = h_1 - h_2h=h1​−h2​ a difference of convex C2C^2C2 functions with ∇h1\nabla h_1∇h1​ being L1L_1L1​-Lipschitz, (44) holds with q=h2q = h_2q=h2​ and ℓ=L1\ell = L_1ℓ=L1​, so the step size may be taken in (0,1/L1)(0, 1/L_1)(0,1/L1​) whatever the curvature of h2h_2h2​. For an indefinite quadratic h(x)=12⟨x,Qx⟩h(x) = \frac12\langle x, Qx\rangleh(x)=21​⟨x,Qx⟩ the admissible range becomes (0,1/λmax⁡(Q))(0, 1/\lambda_{\max}(Q))(0,1/λmax​(Q)) instead of (0,1/max⁡i∣λi(Q)∣)(0, 1/\max_i|\lambda_i(Q)|)(0,1/maxi​∣λi​(Q)∣), and for a concave quadratic every positive step size is admissible. Because the method is a descent method under this rule, its iterates stay in a sublevel set of h+Ph + Ph+P, so the sequence is bounded whenever h+Ph + Ph+P is coercive. The same estimates feed the whole-sequence convergence argument for Kurdyka–Łojasiewicz functions.

Formalizing it. The theorem is proved in the paper; to the best of current knowledge it has no machine-checked proof. Formalizing it requires the limiting subdifferential of an extended-real-valued function, its closedness property (3), and a Fermat rule for a smooth-plus-nonsmooth sum, none of which is in Mathlib. These are reusable for any nonconvex first-order method analysed through cluster points.

Difficulty

The descent part rests on (45), a descent inequality for h+qh + qh+q whose Lipschitz constant is read off from a two-sided Hessian bound; the familiar descent lemma is stated for hhh alone and does not apply, since ∇h\nabla h∇h may have a much larger Lipschitz constant than ℓ\ellℓ.

The stationarity part is where the naive argument fails. Passing to the limit in (47) needs not only xti+1→x∗x^{t_i+1} \to x^*xti​+1→x∗ but also P(xti+1)→P(x∗)P(x^{t_i+1}) \to P(x^*)P(xti​+1)→P(x∗), because the limiting subdifferential is closed only under PPP-attentive convergence. Lower semicontinuity gives one inequality; the other must come from the minimizing property (43) compared against x∗x^*x∗. The objective may be +∞+\infty+∞ at x0x^0x0, so summability of the steps has to be extracted without assuming a finite starting value.

Formalization scope

The space is EuclideanSpace ℝ (Fin n). hhh and qqq are real-valued; PPP takes values in EReal, and every objective value h(x)+P(x)h(x) + P(x)h(x)+P(x) is compared in EReal, never through EReal.toReal. The Hessian is the derivative of the gradient map, a continuous linear self-map; the Loewner order is Mathlib's partial order A ≤ B ↔ (B - A).IsPositive, and both sides of (44) are kept. The regular subgradient is encoded in its ε\varepsilonε-neighbourhood form, and the limiting subdifferential requires all three convergences xt→xx^t \to xxt→x, P(xt)→P(x)P(x^t) \to P(x)P(xt)→P(x), vt→vv^t \to vvt→v. Stationarity is ∃w∈∂P(x), ∇h(x)+w=0\exists w \in \partial P(x),\ \nabla h(x) + w = 0∃w∈∂P(x), ∇h(x)+w=0. The update (43) is a relation on sequences: xt+1x^{t+1}xt+1 minimizes the bracket over all of Rn\mathbb{R}^nRn, with no uniqueness and a free starting point. A cluster point is the limit of xφ(i)x^{\varphi(i)}xφ(i) for a strictly increasing φ\varphiφ.

Trivializing formalizations are ruled out: (44) is not replaced by "∇h\nabla h∇h is ℓ\ellℓ-Lipschitz", which is the classical special case q=0q = 0q=0; P(x0)<∞P(x^0) < \inftyP(x0)<∞, boundedness of the sequence and existence of a cluster point are not assumed; and a limiting subdifferential without P(xt)→P(x)P(x^t) \to P(x)P(xt)→P(x) is not used, since that would make stationarity a weaker statement.

Contributions welcome: the closedness (3) and the Fermat rule behind (47) for the limiting subdifferential, a descent lemma from a two-sided Hessian bound, and the telescoping and limit arguments of the proof.

Selected references

  • G. Li and T. K. Pong, Global convergence of splitting methods for nonconvex composite optimization, SIAM J. Optim. 25(4), 2015. Preprint arXiv:1407.0753v6. https://arxiv.org/abs/1407.0753 · https://doi.org/10.1137/140998135
  • H. Attouch, J. Bolte and B. F. Svaiter, Convergence of descent methods for semi-algebraic and tame problems: proximal algorithms, forward–backward splitting, and regularized Gauss–Seidel methods, Math. Program. 137, 2013. https://doi.org/10.1007/s10107-011-0484-9
  • K. Bredies and D. A. Lorenz, Minimization of non-convex, non-smooth functionals by iterative thresholding, preprint, 2009 (reference [9] of Li–Pong; no stable link recorded there).
  • R. T. Rockafellar and R. J.-B. Wets, Variational Analysis, Springer, 1998. https://doi.org/10.1007/978-3-642-02431-3
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Operations ResearchOptimization·Captain: mikedeng1

Global Convergence of Splitting Methods for Nonconvex Composite Optimization III: For Semi-Algebraic Problems the ADMM Sequence Converges and Has Finite LengthResearch Paper

Motivation

The alternating direction method of multipliers (ADMM) is a standard method for problems of the form min⁡xh(x)+P(Mx)\min_x h(x)+P(\mathcal Mx)minx​h(x)+P(Mx), in which a smooth loss hhh is composed with a structured, possibly nonsmooth regularizer PPP through a linear map M\mathcal MM. Its convergence theory was developed for convex problems, yet it is routinely run on nonconvex ones: sparse recovery with the ℓ0\ell_0ℓ0​ constraint, low-rank matrix problems, and total-variation-type models with nonconvex penalties. For such problems a practitioner wants a guarantee about the iterates actually produced, not only about the existence of good subsequences.

Li and Pong (arXiv:1407.0753v6, SIAM J. Optim. 25(4), 2015) gave the first such guarantee for the classical ADMM on nonconvex composite problems with a surjective M\mathcal MM. Their Theorem 1 shows that cluster points of the (proximal) ADMM are stationary; their Theorem 3, the subject of this mission, shows that for semi-algebraic data the whole sequence converges. The argument adapts the Kurdyka–Łojasiewicz (KL) framework of Attouch, Bolte and Svaiter (Math. Program. 137, 2013) to a setting where the ADMM only decreases its merit function in the xxx-block.

Setting

Fix M:Rn→Rm\mathcal M:\mathbb R^n\to\mathbb R^mM:Rn→Rm linear, h:Rn→Rh:\mathbb R^n\to\mathbb Rh:Rn→R twice continuously differentiable with bounded Hessian, and P:Rm→(−∞,+∞]P:\mathbb R^m\to(-\infty,+\infty]P:Rm→(−∞,+∞] proper (finite somewhere) and closed (lower semicontinuous). For β>0\beta>0β>0 the augmented Lagrangian is

Lβ(x,y,z)=h(x)+P(y)−⟨z,Mx−y⟩+β2∥Mx−y∥2.L_\beta(x,y,z)=h(x)+P(y)-\langle z,\mathcal Mx-y\rangle+\tfrac\beta2\|\mathcal Mx-y\|^2 .Lβ​(x,y,z)=h(x)+P(y)−⟨z,Mx−y⟩+2β​∥Mx−y∥2.

The ADMM produces (xt,yt,zt)t≥0(x^t,y^t,z^t)_{t\ge0}(xt,yt,zt)t≥0​ from arbitrary (x0,z0)(x^0,z^0)(x0,z0) by

yt+1∈Arg min⁡yLβ(xt,y,zt),xt+1∈Arg min⁡xLβ(x,yt+1,zt),zt+1=zt−β(Mxt+1−yt+1).y^{t+1}\in\operatorname*{Arg\,min}_y L_\beta(x^t,y,z^t),\quad x^{t+1}\in\operatorname*{Arg\,min}_x L_\beta(x,y^{t+1},z^t),\quad z^{t+1}=z^t-\beta(\mathcal Mx^{t+1}-y^{t+1}).yt+1∈yArgmin​Lβ​(xt,y,zt),xt+1∈xArgmin​Lβ​(x,yt+1,zt),zt+1=zt−β(Mxt+1−yt+1).

Assumption 1 with T1=0\mathcal T_1=0T1​=0 asks for σ,δ>0\sigma,\delta>0σ,δ>0, γ∈(0,1)\gamma\in(0,1)γ∈(0,1) and symmetric maps Q1,Q2,Q3\mathcal Q_1,\mathcal Q_2,\mathcal Q_3Q1​,Q2​,Q3​ with MM∗⪰σI\mathcal M\mathcal M^*\succeq\sigma\mathcal IMM∗⪰σI, Q1⪰∇2h(x)⪰Q2\mathcal Q_1\succeq\nabla^2h(x)\succeq\mathcal Q_2Q1​⪰∇2h(x)⪰Q2​ and Q3⪰[∇2h(x)]2\mathcal Q_3\succeq[\nabla^2h(x)]^2Q3​⪰[∇2h(x)]2 for all xxx, Q2+βM∗M⪰δI\mathcal Q_2+\beta\mathcal M^*\mathcal M\succeq\delta\mathcal IQ2​+βM∗M⪰δI, and δI≻2σβγQ3\delta\mathcal I\succ\frac{2}{\sigma\beta\gamma}\mathcal Q_3δI≻σβγ2​Q3​.

The limiting subdifferential ∂f(x)\partial f(x)∂f(x) of fff consists of limits vvv of regular subgradients vtv^tvt at points xt→xx^t\to xxt→x with f(xt)→f(x)f(x^t)\to f(x)f(xt)→f(x). A point xxx is stationary if 0∈∇h(x)+M∗∂P(Mx)0\in\nabla h(x)+\mathcal M^*\partial P(\mathcal Mx)0∈∇h(x)+M∗∂P(Mx).

A set in RN\mathbb R^NRN is semi-algebraic if it is a finite union of sets cut out by finitely many polynomial equations pi=0p_i=0pi​=0 and strict inequalities gj<0g_j<0gj​<0; a function is semi-algebraic if its graph is. A proper fff has the KL property at x^∈dom⁡∂f\hat x\in\operatorname{dom}\partial fx^∈dom∂f if there are η>0\eta>0η>0, a neighbourhood VVV of x^\hat xx^ and a continuous concave φ:[0,η)→R+\varphi:[0,\eta)\to\mathbb R_+φ:[0,η)→R+​ with φ(0)=0\varphi(0)=0φ(0)=0, φ∈C1(0,η)\varphi\in C^1(0,\eta)φ∈C1(0,η), φ′>0\varphi'>0φ′>0, such that φ′(f(x)−f(x^)) dist⁡(0,∂f(x))≥1\varphi'(f(x)-f(\hat x))\,\operatorname{dist}(0,\partial f(x))\ge1φ′(f(x)−f(x^))dist(0,∂f(x))≥1 whenever x∈Vx\in Vx∈V and f(x^)<f(x)<f(x^)+ηf(\hat x)<f(x)<f(\hat x)+\etaf(x^)<f(x)<f(x^)+η. A KL function is proper, closed, and KL at every point of dom⁡∂f\operatorname{dom}\partial fdom∂f.

In the Lean development LβL_\betaLβ​ is augLag h P M β x y z, and also augLagX h P M β as a single function on the triple space Rn×Rm×Rm\mathbb R^n\times\mathbb R^m\times\mathbb R^mRn×Rm×Rm with the Euclidean inner product.

Formalization targets

Goal: Theorem 3 (p. 13)

Under the standing assumptions and Assumption 1 with T1=0\mathcal T_1=0T1​=0, if hhh and PPP are semi-algebraic and the ADMM sequence has a cluster point (x∗,y∗,z∗)(x^*,y^*,z^*)(x∗,y∗,z∗), then

(xt,yt,zt)→(x∗,y∗,z∗),0∈∇h(x∗)+M∗∂P(Mx∗),∑t∥xt+1−xt∥<∞.(x^t,y^t,z^t)\to(x^*,y^*,z^*),\qquad 0\in\nabla h(x^*)+\mathcal M^*\partial P(\mathcal Mx^*),\qquad \sum_{t}\|x^{t+1}-x^t\|<\infty .(xt,yt,zt)→(x∗,y∗,z∗),0∈∇h(x∗)+M∗∂P(Mx∗),t∑​∥xt+1−xt∥<∞.

No constants are fixed: every parameter is quantified exactly as in the paper.

Milestones

  1. (35): some w∈∂Lβ(xt+1,yt+1,zt+1)w\in\partial L_\beta(x^{t+1},y^{t+1},z^{t+1})w∈∂Lβ​(xt+1,yt+1,zt+1) has ∥w∥≤C∥xt+1−xt∥\|w\|\le C\|x^{t+1}-x^t\|∥w∥≤C∥xt+1−xt∥ for t≥1t\ge1t≥1.
  2. (36): Lβ(xt,yt,zt)−Lβ(xt+1,yt+1,zt+1)≥D∥xt+1−xt∥2L_\beta(x^t,y^t,z^t)-L_\beta(x^{t+1},y^{t+1},z^{t+1})\ge D\|x^{t+1}-x^t\|^2Lβ​(xt,yt,zt)−Lβ​(xt+1,yt+1,zt+1)≥D∥xt+1−xt∥2 for t≥1t\ge1t≥1.
  3. (39): Lβ(xt,yt,zt)→Lβ(x∗,y∗,z∗)L_\beta(x^t,y^t,z^t)\to L_\beta(x^*,y^*,z^*)Lβ​(xt,yt,zt)→Lβ​(x∗,y∗,z∗).
  4. Finite termination when LβL_\betaLβ​ reaches its limit value.
  5. (41): the one-step KL estimate.
  6. Remark 4(1): the goal with "LβL_\betaLβ​ is a KL function" in place of semi-algebraicity.
  7. LβL_\betaLβ​ is semi-algebraic when hhh and PPP are.
  8. Proper closed semi-algebraic functions are KL functions, with φ(s)=cs1−θ\varphi(s)=cs^{1-\theta}φ(s)=cs1−θ.

Milestones 6, 7 and 8 together imply the goal.

Significance

The result. Theorem 3 upgrades subsequential convergence to convergence of the whole iterate sequence, with finite length of the xxx-trajectory, for a nonconvex ADMM without any convexity of hhh or PPP. Semi-algebraicity covers the paper's applications: polynomial losses, the ℓ0\ell_0ℓ0​ constraint, and indicators of polyhedral or algebraic sets. Remark 4(1) isolates the only property actually used, the KL property of LβL_\betaLβ​, so the result extends to any class of functions for which that property is known (for instance, globally subanalytic or o-minimal definable data).

Formalizing it. The result is proved in the paper and, as far as is known, formalized nowhere. The mission produces a machine-checked version of the paper's convergence argument, a Lean definition of the KL property with the correct convention for empty subdifferentials, and a semi-algebraic set predicate over MvPolynomial. Milestone 8 is a published theorem of real algebraic geometry and nonsmooth analysis (Bolte–Daniilidis–Lewis 2007) that the paper quotes without proof; it is part of what a complete development of the goal requires.

Difficulty

The obvious route is to invoke the abstract convergence theorem of Attouch–Bolte–Svaiter for descent methods. It does not apply: its sufficient-decrease hypothesis requires LβL_\betaLβ​ to drop by a multiple of ∥xt+1−xt∥2+∥yt+1−yt∥2+∥zt+1−zt∥2\|x^{t+1}-x^t\|^2+\|y^{t+1}-y^t\|^2+\|z^{t+1}-z^t\|^2∥xt+1−xt∥2+∥yt+1−yt∥2+∥zt+1−zt∥2, while the ADMM only guarantees a drop proportional to ∥xt+1−xt∥2\|x^{t+1}-x^t\|^2∥xt+1−xt∥2 (Remark 4(2)). The relative-error bound (35) is likewise in terms of the xxx-step alone, and relating the yyy- and zzz-blocks back to the xxx-block uses the surjectivity of M\mathcal MM and the specific structure of the multiplier update. The neighbourhood on which the KL inequality holds is a neighbourhood of the full triple, whereas the trajectory is controlled only in xxx.

The semi-algebraic part has a separate difficulty: showing that LβL_\betaLβ​ is semi-algebraic needs closure of semi-algebraic sets under projection (the Tarski–Seidenberg theorem), and the KL property of semi-algebraic functions needs the Łojasiewicz inequality for subanalytic or semi-algebraic functions. Mathlib has neither.

Formalization scope

Spaces are EuclideanSpace ℝ (Fin n); M\mathcal MM is a continuous linear map and M∗\mathcal M^*M∗ its adjoint. PPP and LβL_\betaLβ​ take values in EReal, never passed through toReal except where the value is provably finite. ⪰\succeq⪰ is Mathlib's Loewner order on self-maps; the Hessian is fderiv ℝ (gradient h). The ADMM is the proximal-ADMM relation with ϕ=0\phi=0ϕ=0; argmin steps are "value at most the value anywhere", with no uniqueness; y0y^0y0 is unconstrained. The triple space is the nested L2L^2L2 product, so its inner product is the sum of the block inner products.

The KL inequality is stated for every v∈∂f(x)v\in\partial f(x)v∈∂f(x), which encodes dist⁡(0,∅)=+∞\operatorname{dist}(0,\emptyset)=+\inftydist(0,∅)=+∞. Writing it with Metric.infDist 0 (∂f x) would give dist⁡(0,∅)=0\operatorname{dist}(0,\emptyset)=0dist(0,∅)=0 and make the KL property fail at every point with empty subdifferential, so that "semi-algebraic implies KL" becomes false and the goal becomes a statement about a different notion. The KL property is required only at points of dom⁡∂f\operatorname{dom}\partial fdom∂f, only on a neighbourhood and only for values in (f(x^),f(x^)+η)(f(\hat x),f(\hat x)+\eta)(f(x^),f(x^)+η); φ\varphiφ is differentiable only on the open interval. Semi-algebraicity of an extended-valued function is that of its graph over its real values. η\etaη is a positive real, which is equivalent to the paper's η∈(0,∞]\eta\in(0,\infty]η∈(0,∞].

The hypotheses ϕ=0\phi=0ϕ=0 and T1=0\mathcal T_1=0T1​=0 are part of the theorem, not a simplification: the analogous statement for the proximal ADMM is open (Remark 4(3)). The cluster point is assumed, not derived.

Needed infrastructure: calculus of the limiting subdifferential (a smooth-plus-separable sum rule), the Tarski–Seidenberg theorem, and the Łojasiewicz/KL inequality for semi-algebraic functions. The last two are reusable far beyond this mission; contributions toward them, and toward the analytic core (milestones 1–6), are welcome.

Selected references

  • G. Li, T. K. Pong, Global convergence of splitting methods for nonconvex composite optimization, SIAM J. Optim. 25(4), 2015. https://arxiv.org/abs/1407.0753 (v6 is the cited version)
  • H. Attouch, J. Bolte, P. Redont, A. Soubeyran, Proximal alternating minimization and projection methods for nonconvex problems: an approach based on the Kurdyka–Łojasiewicz inequality, Math. Oper. Res. 35(2), 2010. https://doi.org/10.1287/moor.1100.0449
  • H. Attouch, J. Bolte, B. F. Svaiter, Convergence of descent methods for semi-algebraic and tame problems, Math. Program. 137, 2013. https://doi.org/10.1007/s10107-011-0484-9
  • J. Bolte, A. Daniilidis, A. Lewis, The Łojasiewicz inequality for nonsmooth subanalytic functions with applications to subgradient dynamical systems, SIAM J. Optim. 17(4), 2007. https://doi.org/10.1137/050644641
  • R. T. Rockafellar, R. J.-B. Wets, Variational Analysis, Springer, 1998. https://doi.org/10.1007/978-3-642-02431-3
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Operations ResearchOptimization·Captain: mikedeng1

Global Convergence of Splitting Methods for Nonconvex Composite Optimization II: The Proximal ADMM Sequence Is Bounded Under CoercivityResearch Paper

Motivation

The alternating direction method of multipliers (ADMM) splits a problem of the form min⁡xh(x)+P(Mx)\min_x h(x) + P(\mathcal M x)minx​h(x)+P(Mx) into a sequence of simpler subproblems, one in which the nonsmooth term PPP enters only through its proximal map and one in which only the smooth term hhh appears. For convex problems its convergence theory is classical. In signal processing and statistics, however, the method is routinely run on nonconvex models, such as ℓ0\ell_0ℓ0​- or ℓ1/2\ell_{1/2}ℓ1/2​-regularized least squares, where PPP is nonconvex and possibly discontinuous and convex theory does not apply.

Li and Pong (arXiv:1407.0753, SIAM J. Optim. 25(4), 2015) gave a convergence analysis of a proximal variant of the ADMM for this nonconvex setting. Their Theorem 1 shows that every cluster point of the iterates is a stationary point. That statement is only informative if cluster points exist. Theorem 2, the subject of this mission, gives conditions on hhh, PPP and M\mathcal MM under which the whole sequence of iterates is bounded, so that cluster points exist and Theorem 1 applies.

Setting

Let n,m≥0n, m \ge 0n,m≥0. The data are:

  • h:Rn→Rh : \mathbb{R}^n \to \mathbb{R}h:Rn→R, twice continuously differentiable with bounded Hessian ∇2h\nabla^2 h∇2h;
  • P:Rm→(−∞,+∞]P : \mathbb{R}^m \to (-\infty, +\infty]P:Rm→(−∞,+∞], proper (never −∞-\infty−∞, finite somewhere) and closed (lower semicontinuous);
  • M:Rn→Rm\mathcal M : \mathbb{R}^n \to \mathbb{R}^mM:Rn→Rm linear, with adjoint M∗\mathcal M^*M∗;
  • a penalty β>0\beta > 0β>0 and a convex, twice continuously differentiable ϕ:Rn→R\phi : \mathbb{R}^n \to \mathbb{R}ϕ:Rn→R.

The augmented Lagrangian is

Lβ(x,y,z)=h(x)+P(y)−⟨z,Mx−y⟩+β2∥Mx−y∥2,L_\beta(x, y, z) = h(x) + P(y) - \langle z, \mathcal M x - y\rangle + \frac{\beta}{2}\|\mathcal M x - y\|^2 ,Lβ​(x,y,z)=h(x)+P(y)−⟨z,Mx−y⟩+2β​∥Mx−y∥2,

and the Bregman distance of ϕ\phiϕ is Dϕ(x1,x2)=ϕ(x1)−ϕ(x2)−⟨∇ϕ(x2),x1−x2⟩D_\phi(x_1, x_2) = \phi(x_1) - \phi(x_2) - \langle\nabla\phi(x_2), x_1 - x_2\rangleDϕ​(x1​,x2​)=ϕ(x1​)−ϕ(x2​)−⟨∇ϕ(x2​),x1​−x2​⟩. A sequence (xt,yt,zt)t≥0(x^t, y^t, z^t)_{t\ge 0}(xt,yt,zt)t≥0​ is generated by the proximal ADMM if, from arbitrary x0,z0x^0, z^0x0,z0,

yt+1∈Arg min⁡yLβ(xt,y,zt),xt+1∈Arg min⁡x{Lβ(x,yt+1,zt)+Dϕ(x,xt)},zt+1=zt−β(Mxt+1−yt+1).y^{t+1} \in \operatorname*{Arg\,min}_y L_\beta(x^t, y, z^t), \quad x^{t+1} \in \operatorname*{Arg\,min}_x \{L_\beta(x, y^{t+1}, z^t) + D_\phi(x, x^t)\}, \quad z^{t+1} = z^t - \beta(\mathcal M x^{t+1} - y^{t+1}).yt+1∈yArgmin​Lβ​(xt,y,zt),xt+1∈xArgmin​{Lβ​(x,yt+1,zt)+Dϕ​(x,xt)},zt+1=zt−β(Mxt+1−yt+1).

For a linear self-map T\mathcal TT, write ∥x∥T2=⟨x,Tx⟩\|x\|^2_{\mathcal T} = \langle x, \mathcal T x\rangle∥x∥T2​=⟨x,Tx⟩, and write ⪰\succeq⪰, ≻\succ≻ for the semidefinite and definite order of symmetric maps. Assumption 1 asks for σ>0\sigma > 0σ>0 with MM∗⪰σI\mathcal M\mathcal M^* \succeq \sigma\mathcal IMM∗⪰σI (so M\mathcal MM is surjective), bounds Q1⪰∇2h⪰Q2\mathcal Q_1 \succeq \nabla^2 h \succeq \mathcal Q_2Q1​⪰∇2h⪰Q2​, maps T1⪰T2⪰0\mathcal T_1 \succeq \mathcal T_2 \succeq 0T1​⪰T2​⪰0 with T12⪰[∇2ϕ]2⪰T22\mathcal T_1^2 \succeq [\nabla^2\phi]^2 \succeq \mathcal T_2^2T12​⪰[∇2ϕ]2⪰T22​, δ>0\delta > 0δ>0 with Q2+βM∗M+T2⪰δI\mathcal Q_2 + \beta\mathcal M^*\mathcal M + \mathcal T_2 \succeq \delta\mathcal IQ2​+βM∗M+T2​⪰δI, a bound Q3⪰[∇2h+∇2ϕ]2\mathcal Q_3 \succeq [\nabla^2 h + \nabla^2\phi]^2Q3​⪰[∇2h+∇2ϕ]2, and γ∈(0,1)\gamma \in (0,1)γ∈(0,1) with

δI+T2≻2σβ(1γQ3+11−γT12).\delta\mathcal I + \mathcal T_2 \succ \frac{2}{\sigma\beta}\Bigl(\frac1\gamma\mathcal Q_3 + \frac1{1-\gamma}\mathcal T_1^2\Bigr).δI+T2​≻σβ2​(γ1​Q3​+1−γ1​T12​).

Formalization targets

Goal: Theorem 2 (p. 11)

Suppose Assumption 1 holds and, with the same σ\sigmaσ and γ\gammaγ, there is 0<ζ<2βγ0 < \zeta < 2\beta\gamma0<ζ<2βγ with

h0:=inf⁡x{h(x)−1σζ∥∇h(x)∥2}>−∞.(29)h_0 := \inf_x\Bigl\{h(x) - \frac{1}{\sigma\zeta}\|\nabla h(x)\|^2\Bigr\} > -\infty. \tag{29}h0​:=xinf​{h(x)−σζ1​∥∇h(x)∥2}>−∞.(29)

Suppose that either (i) M\mathcal MM is invertible and lim inf⁡∥y∥→∞P(y)=∞\liminf_{\|y\|\to\infty} P(y) = \inftyliminf∥y∥→∞​P(y)=∞, or (ii) lim inf⁡∥x∥→∞h(x)=∞\liminf_{\|x\|\to\infty} h(x) = \inftyliminf∥x∥→∞​h(x)=∞ and inf⁡yP(y)>−∞\inf_y P(y) > -\inftyinfy​P(y)>−∞. Then

sup⁡t≥0 (∥xt∥+∥yt∥+∥zt∥)<∞.\sup_{t \ge 0}\ \bigl(\|x^t\| + \|y^t\| + \|z^t\|\bigr) < \infty .t≥0sup​ (∥xt∥+∥yt∥+∥zt∥)<∞.

Milestones

The milestones are the numbered displays of the paper's proof:

  • Eq. (13): M∗zt+1=∇h(xt+1)+∇ϕ(xt+1)−∇ϕ(xt)\mathcal M^* z^{t+1} = \nabla h(x^{t+1}) + \nabla\phi(x^{t+1}) - \nabla\phi(x^t)M∗zt+1=∇h(xt+1)+∇ϕ(xt+1)−∇ϕ(xt).
  • Eq. (20): the one-step estimate Lβ(wt+1)≤Lβ(wt)+12∥xt+1−xt∥2σβγQ3−δI−T22+12∥xt−xt−1∥2σβ(1−γ)T122L_\beta(w^{t+1}) \le L_\beta(w^t) + \tfrac12\|x^{t+1}-x^t\|^2_{\frac{2}{\sigma\beta\gamma}\mathcal Q_3 - \delta\mathcal I - \mathcal T_2} + \tfrac12\|x^t - x^{t-1}\|^2_{\frac{2}{\sigma\beta(1-\gamma)}\mathcal T_1^2}Lβ​(wt+1)≤Lβ​(wt)+21​∥xt+1−xt∥σβγ2​Q3​−δI−T2​2​+21​∥xt−xt−1∥σβ(1−γ)2​T12​2​ for t≥1t \ge 1t≥1.
  • Eq. (30): the merit quantity Lβ(wt)+12∥xt−xt−1∥2σβ(1−γ)T122L_\beta(w^t) + \tfrac12\|x^t - x^{t-1}\|^2_{\frac{2}{\sigma\beta(1-\gamma)}\mathcal T_1^2}Lβ​(wt)+21​∥xt−xt−1∥σβ(1−γ)2​T12​2​ stays below its value at t=1t = 1t=1.
  • Eq. (31): σ∥zt∥2≤1γ∥∇h(xt)∥2+11−γ∥xt−xt−1∥T122\sigma\|z^t\|^2 \le \frac1\gamma\|\nabla h(x^t)\|^2 + \frac1{1-\gamma}\|x^t - x^{t-1}\|^2_{\mathcal T_1^2}σ∥zt∥2≤γ1​∥∇h(xt)∥2+1−γ1​∥xt−xt−1∥T12​2​ for t≥1t \ge 1t≥1.
  • Eq. (32): a lower estimate of that value at t=1t = 1t=1 by μh(xt)+(1−μ)h0+cσ∥∇h(xt)∥2+P(yt)+β2∥Mxt−yt−zt/β∥2+…\mu h(x^t) + (1-\mu)h_0 + \frac{c}{\sigma}\|\nabla h(x^t)\|^2 + P(y^t) + \frac\beta2\|\mathcal M x^t - y^t - z^t/\beta\|^2 + \ldotsμh(xt)+(1−μ)h0​+σc​∥∇h(xt)∥2+P(yt)+2β​∥Mxt−yt−zt/β∥2+…, where c=1−μζ−12βγ>0c = \frac{1-\mu}{\zeta} - \frac{1}{2\beta\gamma} > 0c=ζ1−μ​−2βγ1​>0.

Significance

The result. Theorem 2 supplies the existence of cluster points that Theorem 1 assumes. The two together give an unconditional statement: under Assumption 1, (29) and either coercivity condition, the proximal ADMM has a cluster point and every one of them is stationary. The hypotheses cover the models that motivate the paper. Least squares with a coercive nonconvex regularizer falls under case (i) with M=I\mathcal M = \mathcal IM=I, and a strongly convex quadratic hhh with a regularizer that is bounded below and a general surjective M\mathcal MM falls under case (ii) (Examples 4–6 of the paper). Boundedness is also a standing hypothesis of the paper's Theorem 3, the Kurdyka–Łojasiewicz argument for convergence of the whole sequence.

Formalizing it. The result has been proved since 2015. As far as a search of the platform shows, neither it nor the underlying Lyapunov-type estimates for the ADMM has been machine-checked. This mission formalizes the known proof. The estimates (20), (30) and (31) are shared with the stationarity analysis of the same algorithm, so they serve any later formal work on nonconvex ADMM variants.

Difficulty

The obvious approach is to bound the iterates by the monotone quantity of Eq. (30). That quantity involves LβL_\betaLβ​, which contains −⟨z,Mx−y⟩-\langle z, \mathcal M x - y\rangle−⟨z,Mx−y⟩ and is not bounded below a priori, so its decrease alone does not bound anything. The dual term has to be absorbed. It is controlled through ∇h(xt)\nabla h(x^t)∇h(xt) and the last primal step, and the part involving ∥∇h(xt)∥2\|\nabla h(x^t)\|^2∥∇h(xt)∥2 is then paid for out of hhh itself. Condition (29) exists to make exactly this trade possible, which is why it couples ζ\zetaζ to the γ\gammaγ of Assumption 1. The two cases then extract boundedness in opposite orders: (i) goes from yty^tyt through ztz^tzt to xtx^txt using invertibility of M\mathcal MM, and (ii) goes from xtx^txt through ztz^tzt to yty^tyt. In case (i) the lower bound on PPP that the argument needs is not assumed and must itself be derived from coercivity and lower semicontinuity.

Formalization scope

  • Spaces and values. Spaces are EuclideanSpace ℝ (Fin n) and EuclideanSpace ℝ (Fin m), and M\mathcal MM is a continuous linear map with Mathlib's adjoint. PPP, LβL_\betaLβ​ and every inequality containing them live in EReal, stated additively so that no extended-real subtraction occurs.
  • Assumption 1 is one definition with its witnesses σ,δ,γ,Q1,Q2,T1,T2,Q3\sigma, \delta, \gamma, \mathcal Q_1, \mathcal Q_2, \mathcal T_1, \mathcal T_2, \mathcal Q_3σ,δ,γ,Q1​,Q2​,T1​,T2​,Q3​ as explicit parameters, and ⪰\succeq⪰ is Mathlib's Loewner order on self-maps. ∥x∥T2\|x\|^2_{\mathcal T}∥x∥T2​ is ⟨x,Tx⟩\langle x, \mathcal T x\rangle⟨x,Tx⟩ for every T\mathcal TT, including indefinite ones.
  • Condition (29) takes ζ\zetaζ and a real lower bound h0h_0h0​ as parameters, with the same σ\sigmaσ and γ\gammaγ as Assumption 1.
  • The algorithm is a relation on sequences. An argmin is a global minimizer, not necessarily unique. x0x^0x0 and z0z^0z0 are free, and y0y^0y0 is unconstrained. No existence of minimizers is asserted.
  • Coercivity is stated in its ∀r ∃R\forall r\,\exists R∀r∃R form, and "invertible" is bijectivity of M\mathcal MM.
  • Boundedness means one radius for all three blocks and all t≥0t \ge 0t≥0.

Ruling out trivial versions. A formalization that bounds only xtx^txt, fixes γ\gammaγ or ζ\zetaζ to an example's values, lets (29) use a fresh γ\gammaγ, adds a lower bound on PPP in case (i), or assumes minimizers that make the sequence constant proves a different, weaker theorem, and is not the target.

Definitions needed. Proper and closed extended-valued functions, the Hessian as fderiv of gradient, the augmented Lagrangian, the Bregman distance, the proximal-ADMM relation and Assumption 1 are all provided. They mirror the definitions of the companion mission on cluster points of the same algorithm. A solver will need standard facts beyond them: first-order optimality for a differentiable function, the mean-value bound ∥∇ϕ(a)−∇ϕ(b)∥2≤∥a−b∥T122\|\nabla\phi(a) - \nabla\phi(b)\|^2 \le \|a-b\|^2_{\mathcal T_1^2}∥∇ϕ(a)−∇ϕ(b)∥2≤∥a−b∥T12​2​ from the Hessian sandwich, and strong convexity of the xxx-subproblem. Proofs of individual milestones are welcome independently.

Selected references

  • G. Li and T. K. Pong, Global Convergence of Splitting Methods for Nonconvex Composite Optimization, SIAM J. Optim. 25(4), 2015; preprint arXiv:1407.0753v6. https://arxiv.org/abs/1407.0753 (DOI 10.1137/140998135)
  • S. Boyd, N. Parikh, E. Chu, B. Peleato and J. Eckstein, Distributed Optimization and Statistical Learning via the Alternating Direction Method of Multipliers, Found. Trends Mach. Learn. 3(1), 2011. https://doi.org/10.1561/2200000016
  • H. Attouch, J. Bolte and B. F. Svaiter, Convergence of descent methods for semi-algebraic and tame problems, Math. Program. 137, 2013. https://doi.org/10.1007/s10107-011-0484-9
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Approximately Optimal Approximate Reinforcement Learning II: Near-Optimality of a Policy with Small Policy AdvantageResearch Paper

Motivation

Approximate policy iteration and policy-gradient methods stop when they can no longer find a direction of improvement. Kakade and Langford (ICML 2002) asked what such a stopping point guarantees. Their algorithm, conservative policy iteration, halts at a policy π\piπ for which no policy can improve much on π\piπ as measured under a restart distribution μ\muμ; the quantity that is small is the optimal policy advantage OPT(Aπ,μ)\mathrm{OPT}(\mathbb A_{\pi,\mu})OPT(Aπ,μ​). Theorem 6.2 of the paper translates this local condition into a global statement: the performance of π\piπ is close to optimal, with a loss controlled by how well μ\muμ covers the states an optimal policy visits.

The bound is the origin of the distribution mismatch coefficient ∥dπ∗,μ~/μ∥∞\|d_{\pi^*,\tilde\mu}/\mu\|_\infty∥dπ∗,μ~​​/μ∥∞​, which reappears in the analysis of approximate dynamic programming (concentrability coefficients, Munos 2003), of conservative and trust-region methods, and of the convergence of policy gradient methods (Agarwal, Kakade, Lee, Mahajan 2021), where it governs the rate. The performance difference lemma (Lemma 6.1) used in its proof has become a standard tool of reinforcement learning theory.

Setting

A finite Markov decision process has a finite nonempty state set SSS, a finite nonempty action set AAA, transition probabilities P(s′;s,a)P(s';s,a)P(s′;s,a) (for each s,as,as,a a probability distribution over s′s's′), a reward function R:S×A→[0,R]\mathcal R:S\times A\to[0,R]R:S×A→[0,R] with R>0R>0R>0, and a discount factor 0≤γ<10\le\gamma<10≤γ<1. A stochastic policy π(a;s)\pi(a;s)π(a;s) is, for each state sss, a probability distribution over actions. A state distribution is a probability vector μ\muμ on SSS.

The normalized value function is Vπ(s)=(1−γ)E[∑t≥0γtR(st,at)∣π,s]V_\pi(s)=(1-\gamma)E[\sum_{t\ge0}\gamma^t\mathcal R(s_t,a_t)\mid\pi,s]Vπ​(s)=(1−γ)E[∑t≥0​γtR(st​,at​)∣π,s], where s0=ss_0=ss0​=s, at∼π(⋅;st)a_t\sim\pi(\cdot;s_t)at​∼π(⋅;st​) and st+1∼P(⋅;st,at)s_{t+1}\sim P(\cdot;s_t,a_t)st+1​∼P(⋅;st​,at​). The state–action value is Qπ(s,a)=(1−γ)R(s,a)+γ∑s′P(s′;s,a)Vπ(s′)Q_\pi(s,a)=(1-\gamma)\mathcal R(s,a)+\gamma\sum_{s'}P(s';s,a)V_\pi(s')Qπ​(s,a)=(1−γ)R(s,a)+γ∑s′​P(s′;s,a)Vπ​(s′) and the advantage is Aπ(s,a)=Qπ(s,a)−Vπ(s)A_\pi(s,a)=Q_\pi(s,a)-V_\pi(s)Aπ​(s,a)=Qπ​(s,a)−Vπ​(s). The discounted future state distribution from μ\muμ is

dπ,μ(s)=(1−γ)∑t≥0γtPr⁡(st=s;π,μ),s0∼μ,d_{\pi,\mu}(s)=(1-\gamma)\sum_{t\ge0}\gamma^t\Pr(s_t=s;\pi,\mu),\qquad s_0\sim\mu,dπ,μ​(s)=(1−γ)t≥0∑​γtPr(st​=s;π,μ),s0​∼μ,

and the performance of π\piπ from μ\muμ is ημ(π)=∑sμ(s)Vπ(s)\eta_\mu(\pi)=\sum_s\mu(s)V_\pi(s)ημ​(π)=∑s​μ(s)Vπ​(s).

The policy advantage of π′\pi'π′ with respect to π\piπ and μ\muμ is Aπ,μ(π′)=∑sdπ,μ(s)∑aπ′(a;s)Aπ(s,a)\mathbb A_{\pi,\mu}(\pi')=\sum_sd_{\pi,\mu}(s)\sum_a\pi'(a;s)A_\pi(s,a)Aπ,μ​(π′)=∑s​dπ,μ​(s)∑a​π′(a;s)Aπ​(s,a): the expected advantage of π′\pi'π′ over π\piπ on the states π\piπ itself visits. Its maximum over all stochastic policies is OPT(Aπ,μ)=max⁡π′Aπ,μ(π′)\mathrm{OPT}(\mathbb A_{\pi,\mu})=\max_{\pi'}\mathbb A_{\pi,\mu}(\pi')OPT(Aπ,μ​)=maxπ′​Aπ,μ​(π′) (Definition 4.3). An optimal policy π∗\pi^*π∗ satisfies Vπ(s)≤Vπ∗(s)V_\pi(s)\le V_{\pi^*}(s)Vπ​(s)≤Vπ∗​(s) for every policy π\piπ and every state sss. For nonnegative f,gf,gf,g on SSS, ∥f/g∥∞=max⁡sf(s)/g(s)\|f/g\|_\infty=\max_sf(s)/g(s)∥f/g∥∞​=maxs​f(s)/g(s) (p. 5).

Formalization targets

Goal: Theorem 6.2 (p. 6)

If OPT(Aπ,μ)<ε\mathrm{OPT}(\mathbb A_{\pi,\mu})<\varepsilonOPT(Aπ,μ​)<ε and π∗\pi^*π∗ is optimal, then for every state distribution μ~\tilde\muμ~​

ημ~(π∗)−ημ~(π)≤ε1−γ∥dπ∗,μ~dπ,μ∥∞≤ε(1−γ)2∥dπ∗,μ~μ∥∞.\eta_{\tilde\mu}(\pi^*)-\eta_{\tilde\mu}(\pi)\le\frac{\varepsilon}{1-\gamma}\left\|\frac{d_{\pi^*,\tilde\mu}}{d_{\pi,\mu}}\right\|_\infty\le\frac{\varepsilon}{(1-\gamma)^2}\left\|\frac{d_{\pi^*,\tilde\mu}}{\mu}\right\|_\infty.ημ~​​(π∗)−ημ~​​(π)≤1−γε​​dπ,μ​dπ∗,μ~​​​​∞​≤(1−γ)2ε​​μdπ∗,μ~​​​​∞​.

The goal states both inequalities and the outer bound. The evaluation distribution μ~\tilde\muμ~​ is arbitrary and unrelated to the restart distribution μ\muμ; taking μ~=D\tilde\mu=Dμ~​=D, the start distribution, gives Corollary 4.5 (p. 5).

Milestone: Lemma 6.1 (p. 6)

For any policies π~\tilde\piπ~, π\piπ and any starting distribution μ\muμ,

ημ(π~)−ημ(π)=11−γE(a,s)∼π~dπ~,μ[Aπ(s,a)].\eta_\mu(\tilde\pi)-\eta_\mu(\pi)=\frac{1}{1-\gamma}E_{(a,s)\sim\tilde\pi d_{\tilde\pi,\mu}}\big[A_\pi(s,a)\big].ημ​(π~)−ημ​(π)=1−γ1​E(a,s)∼π~dπ~,μ​​[Aπ​(s,a)].

The states are weighted by the future state distribution of the new policy π~\tilde\piπ~, the advantage is that of the old policy π\piπ.

Significance

Theorem 6.2 is the quality guarantee for conservative policy iteration: combined with the paper's Theorem 4.4 (the algorithm stops with OPT(Aπ,μ)<2ε\mathrm{OPT}(\mathbb A_{\pi,\mu})<2\varepsilonOPT(Aπ,μ​)<2ε after polynomially many calls), it bounds the suboptimality of the returned policy for any target distribution, independently of the size of the state space except through the mismatch coefficient. It also explains the role of the restart distribution: a more uniform μ\muμ makes ∥dπ∗,μ~/μ∥∞\|d_{\pi^*,\tilde\mu}/\mu\|_\infty∥dπ∗,μ~​​/μ∥∞​ small. Lemma 6.1 is used throughout later theory, from trust-region policy optimization to the global convergence of policy gradient methods.

Both results are proved in the paper, with short arguments. The contribution of this mission is a machine-checked version of the infinite-horizon discounted statement in the paper's normalization, with the ∥⋅∥∞\|\cdot\|_\infty∥⋅∥∞​ ratios handled exactly, including states where a denominator vanishes. Neither the discounted performance difference lemma for stochastic policies nor the distribution mismatch bound is known to be formalized in Mathlib; a finite-horizon performance difference identity has been formalized separately and is a different statement.

Difficulty

The mathematics is short; the difficulty is in the infinite-horizon bookkeeping. The value function and dπ,μd_{\pi,\mu}dπ,μ​ are infinite series, and Lemma 6.1 relates the series of two different policies: its natural one-line argument uses the Bellman equation for VπV_\piVπ​, which is not the definition here, together with interchanges of infinite sums over time with finite sums over states and actions, each of which needs summability. Theorem 6.2 then needs two facts that are not stated as results in the paper: that OPT(Aπ,μ)\mathrm{OPT}(\mathbb A_{\pi,\mu})OPT(Aπ,μ​) equals ∑sdπ,μ(s)max⁡aAπ(s,a)\sum_sd_{\pi,\mu}(s)\max_aA_\pi(s,a)∑s​dπ,μ​(s)maxa​Aπ​(s,a) (the supremum over policies is attained by a greedy policy, and max⁡aAπ(s,a)≥0\max_aA_\pi(s,a)\ge0maxa​Aπ​(s,a)≥0), and that dπ,μ(s)≥(1−γ)μ(s)d_{\pi,\mu}(s)\ge(1-\gamma)\mu(s)dπ,μ​(s)≥(1−γ)μ(s). Reading the ℓ∞\ell_\inftyℓ∞​ ratio with real division would give a false statement when a denominator is zero; the statement avoids this.

Formalization scope

States and actions are finite nonempty types; policies and kernels are real-valued functions π s a (the paper's π(a;s)\pi(a;s)π(a;s)) and P s a s' (the paper's P(s′;s,a)P(s';s,a)P(s′;s,a)), with their distribution properties as explicit hypotheses. The published definitions IsTransitionKernel, IsPolicy, InducedTransition, OccupationDist, InducedReward and PolicyValue from the Foundations of Machine Learning series are reused; VπV_\piVπ​ is (1−γ)(1-\gamma)(1−γ) times PolicyValue, the defining series. OPT\mathrm{OPT}OPT is the supremum of the policy advantages over stochastic policies, which is the paper's maximum. Optimality of π∗\pi^*π∗ is relative to stationary stochastic policies, the paper's policy class; the existence of an optimal policy (the paper's "well known result", p. 2) is not part of this mission.

Every hypothesis is explicit: rewards in [0,R][0,R][0,R] with R>0R>0R>0, 0≤γ<10\le\gamma<10≤γ<1, PPP a kernel, π\piπ and π∗\pi^*π∗ stochastic policies, μ\muμ and μ~\tilde\muμ~​ state distributions. Each ∥f/g∥∞\|f/g\|_\infty∥f/g∥∞​ bound is stated multiplicatively: "X≤K∥f/g∥∞X\le K\|f/g\|_\inftyX≤K∥f/g∥∞​" is "X≤KCX\le KCX≤KC for every CCC with f(s)≤Cg(s)f(s)\le Cg(s)f(s)≤Cg(s) for all sss". When some g(s)=0<f(s)g(s)=0<f(s)g(s)=0<f(s) no such CCC exists and the bound is empty, which matches ∥f/g∥∞=+∞\|f/g\|_\infty=+\infty∥f/g∥∞​=+∞; no full-support assumption is made on μ\muμ or μ~\tilde\muμ~​. The hypothesis OPT(Aπ,μ)<ε\mathrm{OPT}(\mathbb A_{\pi,\mu})<\varepsilonOPT(Aπ,μ​)<ε is on the supremum itself, not on the closed form ∑sdπ,μ(s)max⁡aAπ(s,a)\sum_sd_{\pi,\mu}(s)\max_aA_\pi(s,a)∑s​dπ,μ​(s)maxa​Aπ​(s,a), which is a step of the proof; a formalization that assumed the closed form, or that divided by dπ,μd_{\pi,\mu}dπ,μ​ in real arithmetic, would not be this theorem. The proof of the theorem uses only that π∗\pi^*π∗ is a policy; optimality is kept as a hypothesis because the paper states it.

The proof on p. 7 twice writes dπ,μ(s)≤(1−γ)μ(s)d_{\pi,\mu}(s)\le(1-\gamma)\mu(s)dπ,μ​(s)≤(1−γ)μ(s); the inequality it uses, and the one stated on p. 5, is dπ,μ(s)≥(1−γ)μ(s)d_{\pi,\mu}(s)\ge(1-\gamma)\mu(s)dπ,μ​(s)≥(1−γ)μ(s). This slip is in the proof, not in the statement. Pages are PDF pages; the paper has no printed page numbers.

Useful reusable infrastructure: summability and Bellman equations for the normalized discounted value, dπ,μd_{\pi,\mu}dπ,μ​ as a probability distribution with dπ,μ≥(1−γ)μd_{\pi,\mu}\ge(1-\gamma)\mudπ,μ​≥(1−γ)μ, and attainment of OPT\mathrm{OPT}OPT by a greedy policy. Contributions of any of these as separate lemmas are welcome.

Selected references

  • S. Kakade, J. Langford, Approximately Optimal Approximate Reinforcement Learning, Proceedings of the 19th International Conference on Machine Learning (ICML), 2002. https://dl.acm.org/doi/10.5555/645531.656005
  • R. Munos, Error Bounds for Approximate Policy Iteration, ICML 2003. https://dl.acm.org/doi/10.5555/3041838.3041903
  • A. Agarwal, S. Kakade, J. Lee, G. Mahajan, On the Theory of Policy Gradient Methods: Optimality, Approximation, and Distribution Shift, Journal of Machine Learning Research 22(98), 2021. https://jmlr.org/papers/v22/19-736.html
  • J. Schulman, S. Levine, P. Abbeel, M. Jordan, P. Moritz, Trust Region Policy Optimization, ICML 2015. https://arxiv.org/abs/1502.05477
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Optimal Two- and Three-Stage Production Schedules with Setup Times Included 2: Johnson's Rule for Three MachinesResearch Paper

Motivation

Johnson's 1954 paper in Naval Research Logistics Quarterly is the starting point of machine scheduling theory. Its first section solves the two-machine flow shop: nnn items must pass through machine 1 and then machine 2, and an explicit ordering rule minimizes the total elapsed time. Its second section treats three machines. There the problem "loses some of the nice structure of the two-stage case" (p. 65), and the general three-machine problem was later shown to be strongly NP-hard (Garey, Johnson and Sethi, 1976). Johnson nevertheless identifies a restricted case, in which the middle machine is dominated by the first (or the last), where the two-machine rule still gives an optimal schedule. That case, and the structural facts behind it, are the content of this mission.

The three-machine results are still the reference point for polynomially solvable flow shops and for lower bounds in branch-and-bound methods for the general problem.

Timeline.

  • 1954: Johnson proves the two-machine rule (Theorem 1) and, for three machines, the reduction to a common ordering (Lemma 3), a closed form for the elapsed time, and optimality of the rule on Ai+BiA_i + B_iAi​+Bi​, Bi+CiB_i + C_iBi​+Ci​ when min⁡Ai≥max⁡Bj\min A_i \ge \max B_jminAi​≥maxBj​ (Theorem 2), with the mirror case min⁡Ci≥max⁡Bj\min C_i \ge \max B_jminCi​≥maxBj​ asserted.
  • 1976: Garey, Johnson and Sethi show that minimizing makespan in a three-machine flow shop is strongly NP-hard in general, so some restriction of Theorem 2's kind is unavoidable for an exact ordering rule.

Setting

There are nnn items and three machines. Item iii needs processing time Ai>0A_i > 0Ai​>0 on machine 1, Bi>0B_i > 0Bi​>0 on machine 2 and Ci>0C_i > 0Ci​>0 on machine 3, in that order. Each machine handles at most one item at a time, and processing is not interrupted.

A schedule assigns each item start times si1,si2,si3s^1_i, s^2_i, s^3_isi1​,si2​,si3​. It is feasible when all start times are at least 000 on machine 1, the processing intervals of distinct items on the same machine do not overlap, and si1+Ai≤si2s^1_i + A_i \le s^2_isi1​+Ai​≤si2​, si2+Bi≤si3s^2_i + B_i \le s^3_isi2​+Bi​≤si3​. The three machines may process the items in different orders. The total elapsed time (makespan) is max⁡i(si3+Ci)\max_i (s^3_i + C_i)maxi​(si3​+Ci​).

An ordering σ\sigmaσ lists the items, σ(k)\sigma(k)σ(k) being the item in position kkk. Its as-soon-as-possible schedule processes the items in the order σ\sigmaσ on every machine and starts each item on each machine as early as the rules allow. For an ordering, with positions 1,…,n1, \dots, n1,…,n, Johnson defines

Ku=∑i=1uAi−∑i=1u−1Bi,Hv=∑i=1vBi−∑i=1v−1Ci,K_u = \sum_{i=1}^{u} A_i - \sum_{i=1}^{u-1} B_i, \qquad H_v = \sum_{i=1}^{v} B_i - \sum_{i=1}^{v-1} C_i,Ku​=i=1∑u​Ai​−i=1∑u−1​Bi​,Hv​=i=1∑v​Bi​−i=1∑v−1​Ci​,

the sums running over the items in the first uuu (resp. vvv) positions.

Johnson's three-stage rule says that item iii definitely precedes item jjj when

min⁡(Ai+Bi, Cj+Bj)<min⁡(Aj+Bj, Ci+Bi)(IV)\min(A_i + B_i,\ C_j + B_j) < \min(A_j + B_j,\ C_i + B_i) \tag{IV}min(Ai​+Bi​, Cj​+Bj​)<min(Aj​+Bj​, Ci​+Bi​)(IV)

and calls them indifferent under equality. An ordering is consistent with (IV) when no item placed later is definitely preferred to an item placed earlier.

Formalization targets

Goal: Theorem 2 (p. 67)

If every AiA_iAi​ is at least every BjB_jBj​, then an ordering consistent with (IV) exists, and for every such ordering σ\sigmaσ the as-soon-as-possible schedule of σ\sigmaσ is feasible and satisfies

makespan⁡(as-soon-as-possible schedule of σ)≤makespan⁡(s)for every feasible schedule s.\operatorname{makespan}(\text{as-soon-as-possible schedule of } \sigma) \le \operatorname{makespan}(s) \quad \text{for every feasible schedule } s .makespan(as-soon-as-possible schedule of σ)≤makespan(s)for every feasible schedule s.

Milestones

  1. Lemma 3 (p. 65). Every feasible schedule is matched or beaten by the as-soon-as-possible schedule of some single ordering.
  2. Closed form (p. 66). For every ordering, the total idle time of machine 3 is ∑iYi=max⁡1≤u≤v≤n(Hv+Ku)\sum_i Y_i = \max_{1 \le u \le v \le n}(H_v + K_u)∑i​Yi​=max1≤u≤v≤n​(Hv​+Ku​), so that
makespan⁡=∑i=1nCi+max⁡1≤u≤v≤n(Ku+Hv),\operatorname{makespan} = \sum_{i=1}^{n} C_i + \max_{1 \le u \le v \le n} (K_u + H_v),makespan=i=1∑n​Ci​+1≤u≤v≤nmax​(Ku​+Hv​),

the "maximum walk" of p. 68. 3. Special case (p. 67). If min⁡Ai≥max⁡Bj\min A_i \ge \max B_jminAi​≥maxBj​ then max⁡u≤vKu=Kv\max_{u \le v} K_u = K_vmaxu≤v​Ku​=Kv​, so the makespan is ∑iCi+max⁡v(Hv+Kv)\sum_i C_i + \max_v (H_v + K_v)∑i​Ci​+maxv​(Hv​+Kv​). 4. (III) ⇔\Leftrightarrow⇔ (IV) (p. 67). Interchanging the items in positions j,j+1j, j+1j,j+1 changes HHH and KKK only at j,j+1j, j+1j,j+1, and the interchange is strictly worse for the diagonal terms exactly when (IV) holds. 5. Lemma 4 (p. 67). Relation (IV) is transitive, except when the middle item is indifferent to both others. 6. Mirror case (p. 68). The conclusion of Theorem 2 also holds when every CiC_iCi​ is at least every BjB_jBj​.

Significance

The result. Theorem 2 gives an O(nlog⁡n)O(n \log n)O(nlogn) exact method for a class of three-machine flow shops, in a problem that is strongly NP-hard in general. Lemma 3 says that, for three machines, permutation schedules are dominant; Johnson's example on p. 65 shows this fails for four machines. The closed form of milestone 2 expresses the makespan of any ordering as a longest path in a grid, the device behind most later flow-shop lower bounds.

Formalizing it. All results are proved on paper, some tersely: Lemma 3's proof is two lines and cites the wrong lemma, Lemma 4 is proved by reference to Lemma 2, and the mirror case is asserted without proof. A search of Mathlib and of the platform catalog found no machine-checked proof of any of them. The mission produces a checked account of the three-machine flow shop, including the comparison against all feasible schedules rather than only permutation schedules, and pins down the exact form of the hypotheses (see below).

Difficulty

The interchange argument of the two-machine case does not transfer directly. For a general ordering the makespan involves max⁡u≤v(Hv+Ku)\max_{u \le v}(H_v + K_u)maxu≤v​(Hv​+Ku​), and interchanging adjacent items changes terms that depend on everything placed earlier; the page notes that "the decision is not independent of what precedes the interchanged elements". The hypothesis min⁡A≥max⁡B\min A \ge \max BminA≥maxB is what makes KKK nondecreasing along the ordering, collapsing the double maximum to the diagonal. A second obstacle is that (IV) is not a total preorder: ties break transitivity, so passing from "no adjacent pair can be improved" to "optimal" needs the all-pairs consistency and the tie exception of Lemma 4. Finally, Lemma 3 is a statement about arbitrary start-time schedules, so the reduction to orderings must handle machines whose orders differ.

Formalization scope

Items are Fin n; processing times are real-valued functions A B C : Fin n → ℝ, assumed positive in each theorem that is about schedules (the paper's standing assumption, p. 61). A schedule is three start-time functions; feasibility is spelled out as above with non-overlap written as a disjunction of inequalities. The makespan is the maximum of the machine-3 completion times together with 000, so the empty instance has makespan 000. An ordering is an Equiv.Perm (Fin n) with σ k the item in position k; positions are 0-based, so the Lean K u, H v are the paper's Ku+1K_{u+1}Ku+1​, Hv+1H_{v+1}Hv+1​. Statements with maxima over positions assume n≥1n \ge 1n≥1.

Hypotheses made explicit or corrected:

  • min⁡Ai≥max⁡Bi\min A_i \ge \max B_iminAi​≥maxBi​ is read globally, Bj≤AiB_j \le A_iBj​≤Ai​ for all i,ji, ji,j, as in the section heading. The pointwise reading Bi≤AiB_i \le A_iBi​≤Ai​ makes Theorem 2 false (an instance with five items is recorded in the Formalization Note of the goal).
  • Consistency with (IV) is required for all pairs of positions, not only adjacent ones.
  • Lemma 4 carries Lemma 2's exception for an item indifferent to both others; without it the statement is false.
  • Lemma 3's proof cites "Lemma 2" where Lemma 1 is meant.
  • The interchange equivalence (milestone 4) is stated for arbitrary reals, which is stronger than the page needs.

Optimality in the goal is against every feasible schedule. A formalization that compares only orderings with each other, or that defines the objective as the closed form ∑C+max⁡(Ku+Hv)\sum C + \max(K_u + H_v)∑C+max(Ku​+Hv​), would drop Lemma 3's content and is ruled out: the makespan is the latest completion time of a start-time schedule. The existence clause keeps the optimality clause from being vacuous.

A complete development needs finite sums over initial segments of Fin n, Finset.sup', and permutation manipulations (adjacent transpositions, bubble-sort arguments). The feasibility model and the closed form are reusable for other flow-shop results; contributions of general lemmas on adjacent interchanges of permutations are welcome.

Selected references

  • S. M. Johnson, Optimal two- and three-stage production schedules with setup times included, Naval Research Logistics Quarterly 1(1):61–68, 1954. https://doi.org/10.1002/nav.3800010110
  • M. R. Garey, D. S. Johnson, R. Sethi, The complexity of flowshop and jobshop scheduling, Mathematics of Operations Research 1(2):117–129, 1976. https://doi.org/10.1287/moor.1.2.117
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Machine Learning·Captain: Minghui

Certified Federated Unlearning for Linearized ModelsResearch Paper

Removing a client's contribution

Federated learning combines information from several clients without pooling their raw training records. A client may later request removal of its contribution. Retraining on the retained records supplies a natural comparison model, but repeating the training process can be costly. Jin, Chen, Zhang, and Li introduce a linearized learning pipeline and a server-side removal procedure in Forgettable Federated Linear Learning with Certified Data Unlearning, arXiv:2306.02216v3. Their linearization makes the training objective quadratic, so the distinction between an exact Newton correction and an approximate correction can be studied explicitly.

This mission formalizes a corrected finite-run error bound motivated by that analysis. It is not a transcription or validation of the printed Theorem 2. The source audit found that the supplementary argument drops a finite-training term when passing to a limit, uses an invalid general inverse-perturbation inequality, and does not justify its three-term squared-norm constant. The draft preserves the removal problem while stating its error factors explicitly. The source anchors are Section III-C, Theorem 2, PDF pp. 5–6, and supplementary Section C5, PDF p. 16. The preprint first appeared in 2023; this mission fixes the revised May 2026 version so later source changes cannot silently alter its meaning.

Affine features and retained data

A parameter is a vector w∈Rdw\in\mathbb R^dw∈Rd. Record iii has a fixed linear feature map Ai:Rd→RkA_i:\mathbb R^d\to\mathbb R^kAi​:Rd→Rk, an offset aia_iai​, and a target yiy_iyi​. Its prediction is Aiw+aiA_iw+a_iAi​w+ai​. This represents the fixed linearization in the paper's equation (3); arbitrary real targets are permitted, and one-hot classification targets are a special case. Neither approximation accuracy for a nonlinear neural network nor an infinite-width limit is asserted.

Let DDD be the full finite dataset and SSS a nonempty subset of retained indices. Client removal is represented by retaining precisely the indices whose owner differs from the removed client. More general record removals are also allowed. For a fixed regularization parameter μ>0\mu>0μ>0, define

LS(w)=12∣S∣∑i∈S∥Aiw+ai−yi∥2+μ2∥w∥2.L_S(w)=\frac1{2|S|}\sum_{i\in S}\|A_iw+a_i-y_i\|^2+\frac\mu2\|w\|^2.LS​(w)=2∣S∣1​i∈S∑​∥Ai​w+ai​−yi​∥2+2μ​∥w∥2.

Write GS=∣S∣−1∑i∈SAi∗AiG_S=|S|^{-1}\sum_{i\in S}A_i^*A_iGS​=∣S∣−1∑i∈S​Ai∗​Ai​, HS=GS+μIH_S=G_S+\mu IHS​=GS​+μI, and bS=∣S∣−1∑i∈SAi∗(yi−ai)b_S=|S|^{-1}\sum_{i\in S}A_i^*(y_i-a_i)bS​=∣S∣−1∑i∈S​Ai∗​(yi​−ai​). Define uS=HS−1bSu_S=H_S^{-1}b_SuS​=HS−1​bS​ and let uDu_DuD​ use the full dataset. These reference parameters are computed from the data. The accepted child proofs establish the Hessian positivity and invertibility needed for the error bound; the broader unique-minimizer theorem is a separate supporting statement. The construction comes from Section III-A, PDF pp. 3–4, equations (3)–(5).

A separate nonempty server dataset PPP has Gram operator GPG_PGP​ and regularized Hessian HP=GP+μIH_P=G_P+\mu IHP​=GP​+μI. All operator norms below are Euclidean operator norms. The datasets and feature maps are fixed throughout the probability calculation.

Formalization targets

Let WWW be the trained parameter, RRR the parameter returned by retraining on SSS, and VVV an approximate removal correction. The removed parameter is W−VW-VW−V. Their joint probability model has finite outcome space Ω\OmegaΩ, with masses pω≥0p_\omega\ge0pω​≥0 summing to one. They may be dependent. This covers the outputs of finite randomized runs on finite data with fixed initialization; no independence assumption is used.

For each trained parameter www, define the server removal objective and its exact minimizer by

Fw(v)=12⟨v,HPv⟩−⟨HSw−bS,v⟩,vP(w)=HP−1(HSw−bS).F_w(v)=\tfrac12\langle v,H_Pv\rangle-\langle H_Sw-b_S,v\rangle, \qquad v_P(w)=H_P^{-1}(H_Sw-b_S).Fw​(v)=21​⟨v,HP​v⟩−⟨HS​w−bS​,v⟩,vP​(w)=HP−1​(HS​w−bS​).

This is the quadratic surrogate in Section III-B, PDF p. 5, equation (6). Define

Q=E[FW(V)−FW(vP(W))],κ=∥HP−1∥ ∥GP−GS∥,Q=\mathbb E[F_W(V)-F_W(v_P(W))],\quad \kappa=\|H_P^{-1}\|\,\|G_P-G_S\|,Q=E[FW​(V)−FW​(vP​(W))],κ=∥HP−1​∥∥GP​−GS​∥, Etrain=E∥W−uD∥2,Eretrain=E∥R−uS∥2.E_{\rm train}=\mathbb E\|W-u_D\|^2,\qquad E_{\rm retrain}=\mathbb E\|R-u_S\|^2.Etrain​=E∥W−uD​∥2,Eretrain​=E∥R−uS​∥2.

The corrected goal is

E∥W−V−R∥2≤6μQ+6κ2(Etrain+∥uD−uS∥2)+3Eretrain.\boxed{\mathbb E\|W-V-R\|^2\le \frac6\mu Q+6\kappa^2\bigl(E_{\rm train}+\|u_D-u_S\|^2\bigr) +3E_{\rm retrain}.}E∥W−V−R∥2≤μ6​Q+6κ2(Etrain​+∥uD​−uS​∥2)+3Eretrain​.​

The two completed milestones used by the accepted proof are the surrogate gap bound and the corrected signed removal-error identity:

μ2∥v−vP(w)∥2≤Fw(v)−Fw(vP(w)),\frac\mu2\|v-v_P(w)\|^2\le F_w(v)-F_w(v_P(w)),2μ​∥v−vP​(w)∥2≤Fw​(v)−Fw​(vP​(w)), w−v−r=HP−1(GP−GS)(w−uS)+(vP(w)−v)+(uS−r).w-v-r=H_P^{-1}(G_P-G_S)(w-u_S)+(v_P(w)-v)+(u_S-r).w−v−r=HP−1​(GP​−GS​)(w−uS​)+(vP​(w)−v)+(uS​−r).

The broader ridge-structure, exact-Newton-removal and inverse-perturbation statements remain available as separate open theorems. Their milestone entries were removed because the accepted proof does not depend on their full statements.

Formalization note: the completed root is a corrected, paper-derived error bound. Its formal bridge uses the two source-backed child theorems above, anchored to Section III-B (Section 3), PDF p. 5, equation (6), and Section III-C (Section 3), PDF p. 5 and PDF p. 6, Theorem 2; supplementary C5, PDF p. 16, unnumbered displays. The coefficients in the boxed goal are conservative; no optimality claim is made.

What the result supplies

The result connects the removal solver's objective gap, the difference between the server and retained Hessians, and the actual optimization errors to an observable parameter discrepancy. Exact Hessian matching sets κ=0\kappa=0κ=0. Exact removal optimization sets Q=0Q=0Q=0, but finite retraining error still remains. This distinguishes exact optimization of the retained objective from reproducing an unfinished retraining run.

The original paper motivates the comparison; the displayed corrected bound is a new formulation derived from its quadratic setting. The root Lean theorem and its two dependency milestones are now Proved. Their accepted proofs match the original formal statements exactly; the three separate supporting statements remain open. The requested OpenProblem classification describes the formalization task and does not assert that the elementary corrected inequality is an unresolved research conjecture.

The mathematical difficulty

An approximate server Hessian cannot be substituted for the retained Hessian without a sensitivity term. A bound on the difference of the Gram operators alone does not bound its action on every parameter vector. Likewise, a small training error relative to the full-data optimum does not imply that the full and retained optima coincide. The displacement ∥uD−uS∥\|u_D-u_S\|∥uD​−uS​∥ therefore remains visible. Formalization must respect the normalization of each empirical objective, the sign of the correction, and the operator norm used in the perturbation estimate.

Formalization scope

The model uses finite-dimensional real Euclidean spaces, continuous linear maps and adjoints, finite index sets, a total ring inverse, and finite weighted expectations. Positive regularization must justify every use of the inverse; it is not an invertibility assumption hidden inside the dataset. Nonempty retained and server data exclude division by an empty sample count. Zero-dimensional feature or parameter spaces are permitted and harmless. A finite law on an empty outcome type has no inhabitant because its masses cannot sum to one.

The root theorem quantifies over arbitrary output maps W,V,RW,V,RW,V,R. It is an error-propagation theorem in terms of their actual errors and surrogate gap, not a convergence theorem for a particular implementation. Obtaining algorithm-specific bounds on those quantities is separate future work. In particular, the draft does not import the source's unsupported all-smaller-learning-rates FedAvg contraction claim. It also makes no differential-privacy, distributional indistinguishability, nonlinear-network, or empirical accuracy assertion.

Selected references

  • Ruinan Jin, Minghui Chen, Qiong Zhang, Xiaoxiao Li, Forgettable Federated Linear Learning with Certified Data Unlearning, IEEE Transactions on Neural Networks and Learning Systems, early access (2026). arXiv:2306.02216v3, DOI. Main anchors: Section II-B, PDF p. 3, equation (1); Sections III-A–III-C, PDF pp. 3–6, equations (3)–(6), Theorem 2; supplementary Section C5, PDF p. 16, unnumbered displays.
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Machine LearningOptimizationStatistics·Captain: mikedeng1

Robustness and Generalization IV: Robustness of the Lasso on a Compact Sample SpaceResearch Paper

Motivation

The Lasso (Tibshirani 1996, doi:10.1111/j.2517-6161.1996.tb02080.x) is ℓ1\ell_1ℓ1​-penalized least squares regression, one of the standard estimators of statistics and machine learning because it selects sparse coefficient vectors. Explaining why a learned Lasso predictor generalizes is less routine than it looks. The two classical routes are uniform convergence over the hypothesis class and algorithmic stability (Bousquet and Elisseeff 2002, JMLR 2:499–526). The stability route is closed for the Lasso: Xu, Caramanis and Mannor (IEEE Trans. Inf. Theory 56(7), 2010, doi:10.1109/TIT.2010.2048503) showed that its uniform stability bound does not decrease with the sample size, a fact reproduced as Theorem 7 of Xu and Mannor (2012).

Xu and Mannor, Robustness and Generalization (Mach Learn 86 (2012) 391–423, doi:10.1007/s10994-011-5268-1), propose a third route, algorithmic robustness: if the sample space can be split into KKK cells such that a test point in the same cell as a training point has nearly the same loss, then the algorithm generalizes (their Theorem 1). Their Example 6 shows that the Lasso is robust in this sense, with a number of cells given by a covering number and a robustness level depending on the training responses. This mission formalizes Example 6 together with the general criterion it rests on (Theorem 6) and the Lipschitz estimate for the Lasso loss (Lemma 3).

Setting

A sample is a point z=(z(y),z(x))z = (z^{(y)}, z^{(x)})z=(z(y),z(x)) with a response z(y)∈Rz^{(y)} \in \mathbb Rz(y)∈R and a feature vector z(x)∈Rmz^{(x)} \in \mathbb R^mz(x)∈Rm, so the samples live in Rm+1\mathbb R^{m+1}Rm+1. The sample space Z⊆Rm+1\mathcal Z \subseteq \mathbb R^{m+1}Z⊆Rm+1 is a compact set, and Rm+1\mathbb R^{m+1}Rm+1 carries the norm ∥z∥∞=max⁡(∣z(y)∣,max⁡j∣zj(x)∣)\|z\|_\infty = \max(|z^{(y)}|, \max_j |z^{(x)}_j|)∥z∥∞​=max(∣z(y)∣,maxj​∣zj(x)​∣). A training set is s=(s1,…,sn)∈Zn\mathbf s = (s_1, \dots, s_n) \in \mathcal Z^ns=(s1​,…,sn​)∈Zn.

A learning algorithm maps each training set s\mathbf ss to a hypothesis As\mathcal A_{\mathbf s}As​; with a loss l(h,z)l(h, z)l(h,z), it is (K,ϵ(⋅))(K, \epsilon(\cdot))(K,ϵ(⋅))-robust (Definition 2, p. 396) if Z\mathcal ZZ can be partitioned into KKK disjoint sets C1,…,CKC_1, \dots, C_KC1​,…,CK​, fixed independently of the data, such that for every s∈Zn\mathbf s \in \mathcal Z^ns∈Zn, every training point s∈ss \in \mathbf ss∈s, every z∈Zz \in \mathcal Zz∈Z and every iii,

s,z∈Ci  ⟹  ∣l(As,s)−l(As,z)∣≤ϵ(s).s, z \in C_i \implies |l(\mathcal A_{\mathbf s}, s) - l(\mathcal A_{\mathbf s}, z)| \le \epsilon(\mathbf s).s,z∈Ci​⟹∣l(As​,s)−l(As​,z)∣≤ϵ(s).

For a metric ρ\rhoρ on Z\mathcal ZZ and ϵ>0\epsilon > 0ϵ>0, a set T^⊆Z\hat T \subseteq \mathcal ZT^⊆Z is an ϵ\epsilonϵ-cover of Z\mathcal ZZ if every point of Z\mathcal ZZ is within distance ≤ϵ\le \epsilon≤ϵ of a point of T^\hat TT^; the covering number N(ϵ,Z,ρ)\mathcal N(\epsilon, \mathcal Z, \rho)N(ϵ,Z,ρ) is the least cardinality of such a cover (Definition 1, p. 394).

For a coefficient vector w∈Rmw \in \mathbb R^mw∈Rm let ∥w∥1=∑j∣wj∣\|w\|_1 = \sum_j |w_j|∥w∥1​=∑j​∣wj​∣. Given c>0c > 0c>0, the Lasso is

min⁡w 1n∑i=1n(si(y)−w⊤si(x))2+c∥w∥1,(5)\min_{w} \ \frac1n \sum_{i=1}^n \big(s_i^{(y)} - w^\top s_i^{(x)}\big)^2 + c\|w\|_1, \tag{5}wmin​ n1​i=1∑n​(si(y)​−w⊤si(x)​)2+c∥w∥1​,(5)

a Lasso algorithm returns a minimizer As=w\mathcal A_{\mathbf s} = wAs​=w of (5) for each s\mathbf ss, and the loss is the absolute prediction error l(w,z)=∣z(y)−w⊤z(x)∣l(w, z) = |z^{(y)} - w^\top z^{(x)}|l(w,z)=∣z(y)−w⊤z(x)∣. Finally Y(s)=1n∑i=1n[si(y)]2Y(\mathbf s) = \frac1n \sum_{i=1}^n [s_i^{(y)}]^2Y(s)=n1​∑i=1n​[si(y)​]2.

Formalization targets

Goal: Example 6 (p. 404)

For every compact Z⊆Rm+1\mathcal Z \subseteq \mathbb R^{m+1}Z⊆Rm+1, every c>0c > 0c>0, every Lasso algorithm A\mathcal AA and every γ>0\gamma > 0γ>0,

A is (N(γ/2,Z,∥⋅∥∞), (Y(s)/c+1)γ)-robust.\mathcal A \text{ is } \Big(\mathcal N(\gamma/2, \mathcal Z, \|\cdot\|_\infty),\ \big(Y(\mathbf s)/c + 1\big)\gamma\Big)\text{-robust}.A is (N(γ/2,Z,∥⋅∥∞​), (Y(s)/c+1)γ)-robust.

The statement holds for every selection of a minimizer, since (5) need not have a unique solution.

Milestones

  1. Optimality bound (proof of Lemma 3, p. 419): every Lasso solution satisfies ∥w∗∥1≤1nc∑i=1n[si(y)]2\|w^*\|_1 \le \frac{1}{nc} \sum_{i=1}^n [s_i^{(y)}]^2∥w∗∥1​≤nc1​∑i=1n​[si(y)​]2.
  2. Lemma 3 (p. 419): for all za,zb∈Rm+1z_a, z_b \in \mathbb R^{m+1}za​,zb​∈Rm+1,
∣l(w∗(s),za)−l(w∗(s),zb)∣≤[1nc∑i=1n[si(y)]2+1]∥za−zb∥∞.|l(w^*(\mathbf s), z_a) - l(w^*(\mathbf s), z_b)| \le \Big[\frac{1}{nc} \sum_{i=1}^n [s_i^{(y)}]^2 + 1\Big] \|z_a - z_b\|_\infty.∣l(w∗(s),za​)−l(w∗(s),zb​)∣≤[nc1​i=1∑n​[si(y)​]2+1]∥za​−zb​∥∞​.
  1. Theorem 6 (p. 402): for a metric ρ\rhoρ on Z\mathcal ZZ and γ>0\gamma > 0γ>0, if ∣l(As,z1)−l(As,z2)∣≤ϵ(s)|l(\mathcal A_{\mathbf s}, z_1) - l(\mathcal A_{\mathbf s}, z_2)| \le \epsilon(\mathbf s)∣l(As​,z1​)−l(As​,z2​)∣≤ϵ(s) whenever z1∈sz_1 \in \mathbf sz1​∈s and ρ(z1,z2)≤γ\rho(z_1, z_2) \le \gammaρ(z1​,z2​)≤γ, and N(γ/2,Z,ρ)<∞\mathcal N(\gamma/2, \mathcal Z, \rho) < \inftyN(γ/2,Z,ρ)<∞, then A\mathcal AA is (N(γ/2,Z,ρ),ϵ(⋅))(\mathcal N(\gamma/2, \mathcal Z, \rho), \epsilon(\cdot))(N(γ/2,Z,ρ),ϵ(⋅))-robust.

Significance

Combined with Theorem 1 of the same paper, Example 6 yields a generalization bound for the Lasso of the form ϵ(s)+M(2Kln⁡2+2ln⁡(1/δ))/n\epsilon(\mathbf s) + M\sqrt{(2K\ln 2 + 2\ln(1/\delta))/n}ϵ(s)+M(2Kln2+2ln(1/δ))/n​ with KKK a covering number of the sample space, a bound that uses no stability of the algorithm and no uniqueness of the minimizer. Theorem 6 is the reusable part: it converts any data-dependent local Lipschitz or continuity estimate of the loss into robustness, and the paper derives its examples for the SVM, the Lasso, neural networks and PCA from it. The authors note (p. 404) that the resulting bound is weaker than VC-dimension bounds for linear predictors, since it depends exponentially on the dimension; the value of the example is the method, not the rate.

The results are proved in the paper, with short arguments. No machine-checked version of Theorem 6, Lemma 3 or Example 6 is known to exist. The formal work is to connect Mathlib's covering numbers to partitions of a set, to handle the ℓ1\ell_1ℓ1​/ℓ∞\ell_\inftyℓ∞​ pairing on R×Rm\mathbb R \times \mathbb R^mR×Rm, and to state robustness so that later missions of this series (the generalization bound of Theorem 1, mission I) can consume it.

Difficulty

The constant in the robustness level depends on the training set through Y(s)Y(\mathbf s)Y(s), while the partition in Definition 2 must be chosen before the training set is seen. A formalization that lets the cells depend on s\mathbf ss proves a much weaker, nearly empty statement, so the data dependence has to be carried entirely by ϵ(s)\epsilon(\mathbf s)ϵ(s) and the cells must depend only on Z\mathcal ZZ and γ\gammaγ. A cover by balls is not a partition, and the radius of the cover (γ/2\gamma/2γ/2) and the closeness threshold in Theorem 6 (γ\gammaγ) differ by the factor that the diameter of a cell requires. The Lipschitz estimate must bound a Lasso solution without any information beyond optimality, and the pairing between ∥w∥1\|w\|_1∥w∥1​ and ∥⋅∥∞\|\cdot\|_\infty∥⋅∥∞​ is the one that makes the constant come out as printed; a Euclidean norm on either side gives a different constant.

Formalization scope

  • Rm+1\mathbb R^{m+1}Rm+1 is ℝ × (Fin m → ℝ), a point being (z^{(y)}, z^{(x)}). Lean's norm on this product is the maximum of the absolute values of all coordinates, which is exactly ∥⋅∥∞\|\cdot\|_\infty∥⋅∥∞​. ∥w∥1\|w\|_1∥w∥1​ is written out as ∑j∣wj∣\sum_j |w_j|∑j​∣wj​∣, since the default norm on Fin m → ℝ is the sup norm; w⊤xw^\top xw⊤x is dotProduct w x.
  • The sample space is a set Z with IsCompact Z. Robustness (IsRobustOn) asks for cells C : Fin K → Set α that lie in Z, cover Z and are pairwise disjoint (empty cells allowed), chosen before the universally quantified training set; training sets are maps Fin n → α with all points in Z. No measurability is involved anywhere in this mission.
  • The covering number is Mathlib's Metric.coveringNumber at radius Real.toNNReal (γ / 2): closed balls, centres in Z (the metric space of Definition 1 is Z\mathcal ZZ itself), value in ℕ∞, converted with toNat. Theorem 6 assumes its finiteness, as the paper does; without that hypothesis toNat would return 000 and the statement would be false for nonempty Z. Example 6 does not assume it: it follows from compactness.
  • A Lasso algorithm is any function A with ∀ s, IsLassoSolution c s (A s); it is not defined by a choice of minimizer. The regularization parameter satisfies c>0c > 0c>0, which the paper leaves implicit. The factor 1/n1/n1/n is a real division; for n=0n = 0n=0 it is 000 in Lean, the objective reduces to c∥w∥1c\|w\|_1c∥w∥1​, and all statements remain true.
  • The robustness level is (Y(s)/c+1)γ(Y(\mathbf s)/c + 1)\gamma(Y(s)/c+1)γ in Example 6 and 1nc∑i[si(y)]2+1\frac{1}{nc}\sum_i [s_i^{(y)}]^2 + 1nc1​∑i​[si(y)​]2+1 in Lemma 3, each in its printed form.

Useful infrastructure beyond this mission: a lemma turning a finite cover of a set into a partition of it with cells of diameter at most twice the radius, and finiteness of Mathlib's internal covering number for compact sets. Contributions of either as separate theorems are welcome.

Selected references

  • H. Xu and S. Mannor, Robustness and Generalization, Machine Learning 86 (2012) 391–423. doi:10.1007/s10994-011-5268-1
  • R. Tibshirani, Regression Shrinkage and Selection via the Lasso, Journal of the Royal Statistical Society, Series B 58(1) (1996) 267–288. doi:10.1111/j.2517-6161.1996.tb02080.x
  • H. Xu, C. Caramanis and S. Mannor, Robust Regression and Lasso, IEEE Transactions on Information Theory 56(7) (2010) 3561–3574. doi:10.1109/TIT.2010.2048503
  • O. Bousquet and A. Elisseeff, Stability and Generalization, Journal of Machine Learning Research 2 (2002) 499–526. jmlr.org/papers/v2/bousquet02a
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Machine LearningProbabilityStatistics·Captain: mikedeng1

Robustness and Generalization III: Quantile-Value and Truncated-Mean Generalization Bounds for Pseudo-Robust AlgorithmsResearch Paper

Motivation

Classical generalization bounds control the gap between the expected loss of a learned hypothesis and its average loss on the training sample. The average is sensitive to outliers: when a non-negligible fraction of the sample is corrupted, the mean loss stops describing the quality of a solution, and quantile-type summaries such as the median become the natural measurement. Quantile losses have long been used for this reason in statistics and econometrics (Koenker and Bassett 1978; Huber 1981). The standard tools for proving generalization bounds — symmetrization, Rademacher and VC arguments — are built around the expected loss and do not extend to quantiles in any direct way.

Xu and Mannor (Mach Learn 86 (2012) 391–423) introduced algorithmic robustness: an algorithm is robust if the sample space can be partitioned into finitely many cells such that a test point falling in the same cell as a training point incurs a similar loss. Because the argument works cell by cell and needs no symmetrization, it transfers to loss functionals other than the mean. Sect. 4.1 of the paper uses this to bound the quantile value and the truncated mean of the testing error, and Sect. 5 relaxes robustness to pseudo robustness, which only asks the cell condition for a subset of the training samples. This mission formalizes the resulting Theorem 5 (p. 402), whose proof is Appendix C (pp. 415–418).

Setting

Let Z\mathcal ZZ be a measurable sample space, H\mathcal HH a set of hypotheses and l:H×Z→[0,M]l : \mathcal H \times \mathcal Z \to [0, M]l:H×Z→[0,M] a loss, with each l(h,⋅)l(h, \cdot)l(h,⋅) measurable. A training set s=(s1,…,sn)\mathbf s = (s_1, \dots, s_n)s=(s1​,…,sn​) consists of nnn i.i.d. draws from a probability measure μ\muμ on Z\mathcal ZZ; its empirical distribution is μemp=1n∑iδsi\mu_{\mathrm{emp}} = \frac1n \sum_i \delta_{s_i}μemp​=n1​∑i​δsi​​. A learning algorithm is a map A:Zn→H\mathcal A : \mathcal Z^n \to \mathcal HA:Zn→H, and As\mathcal A_{\mathbf s}As​ is the hypothesis learned from s\mathbf ss.

For a real random variable XXX and a level β\betaβ, the β\betaβ-quantile value is

Qβ(X)=inf⁡{c∈R:Pr⁡(X≤c)≥β},\mathbb Q^\beta(X) = \inf\{ c \in \mathbb R : \Pr(X \le c) \ge \beta \},Qβ(X)=inf{c∈R:Pr(X≤c)≥β},

and, writing Q=Qβ(X)Q = \mathbb Q^\beta(X)Q=Qβ(X), the β\betaβ-truncated mean is

Tβ(X)=E[X⋅1(X<Q)]+(β−Pr⁡[X<Q]) Q,\mathbb T^\beta(X) = \mathbb E[X \cdot \mathbf 1(X < Q)] + \big(\beta - \Pr[X < Q]\big)\, Q,Tβ(X)=E[X⋅1(X<Q)]+(β−Pr[X<Q])Q,

where the second term vanishes when Pr⁡[X=Q]=0\Pr[X = Q] = 0Pr[X=Q]=0. It is the contribution to EX\mathbb E XEX of the leftmost β\betaβ fraction of the distribution. For a hypothesis hhh and a measure ν\nuν on Z\mathcal ZZ put Q(h,β,ν)=Qβ(l(h,z))\mathcal Q(h, \beta, \nu) = \mathbb Q^\beta(l(h, z))Q(h,β,ν)=Qβ(l(h,z)) and T(h,β,ν)=Tβ(l(h,z))\mathcal T(h, \beta, \nu) = \mathbb T^\beta(l(h, z))T(h,β,ν)=Tβ(l(h,z)) with z∼νz \sim \nuz∼ν.

The algorithm is (K,ϵ(⋅),n^(⋅))(K, \epsilon(\cdot), \hat n(\cdot))(K,ϵ(⋅),n^(⋅)) pseudo robust, with ϵ:Zn→R\epsilon : \mathcal Z^n \to \mathbb Rϵ:Zn→R and n^:Zn→{1,…,n}\hat n : \mathcal Z^n \to \{1, \dots, n\}n^:Zn→{1,…,n}, if Z\mathcal ZZ can be partitioned into KKK disjoint sets C1,…,CKC_1, \dots, C_KC1​,…,CK​, fixed in advance, such that every training set s\mathbf ss has a subset s^\hat{\mathbf s}s^ of n^(s)\hat n(\mathbf s)n^(s) samples with: whenever s∈s^s \in \hat{\mathbf s}s∈s^ and z∈Zz \in \mathcal Zz∈Z lie in a common cell, ∣l(As,s)−l(As,z)∣≤ϵ(s)|l(\mathcal A_{\mathbf s}, s) - l(\mathcal A_{\mathbf s}, z)| \le \epsilon(\mathbf s)∣l(As​,s)−l(As​,z)∣≤ϵ(s). With n^≡n\hat n \equiv nn^≡n this is (K,ϵ(⋅))(K, \epsilon(\cdot))(K,ϵ(⋅))-robustness.

Formalization targets

Goal: Theorem 5 (p. 402)

Let λ0=(2Kln⁡2+2ln⁡(1/δ))/n\lambda_0 = \sqrt{(2K \ln 2 + 2 \ln(1/\delta))/n}λ0​=(2Kln2+2ln(1/δ))/n​ and r(s)=(n−n^(s))/nr(\mathbf s) = (n - \hat n(\mathbf s))/nr(s)=(n−n^(s))/n. If A\mathcal AA is (K,ϵ(⋅),n^(⋅))(K, \epsilon(\cdot), \hat n(\cdot))(K,ϵ(⋅),n^(⋅)) pseudo robust, β∈(0,1)\beta \in (0,1)β∈(0,1) and δ>0\delta > 0δ>0, then with probability at least 1−δ1 - \delta1−δ: whenever 0≤β−λ0−r(s)0 \le \beta - \lambda_0 - r(\mathbf s)0≤β−λ0​−r(s) and β+λ0+r(s)≤1\beta + \lambda_0 + r(\mathbf s) \le 1β+λ0​+r(s)≤1,

Q(As,β−λ0−r(s),μemp)−ϵ(s)≤Q(As,β,μ)≤Q(As,β+λ0+r(s),μemp)+ϵ(s),\mathcal Q(\mathcal A_{\mathbf s}, \beta - \lambda_0 - r(\mathbf s), \mu_{\mathrm{emp}}) - \epsilon(\mathbf s) \le \mathcal Q(\mathcal A_{\mathbf s}, \beta, \mu) \le \mathcal Q(\mathcal A_{\mathbf s}, \beta + \lambda_0 + r(\mathbf s), \mu_{\mathrm{emp}}) + \epsilon(\mathbf s),Q(As​,β−λ0​−r(s),μemp​)−ϵ(s)≤Q(As​,β,μ)≤Q(As​,β+λ0​+r(s),μemp​)+ϵ(s), T(As,β−λ0−r(s),μemp)−ϵ(s)≤T(As,β,μ)≤T(As,β+λ0+r(s),μemp)+ϵ(s).\mathcal T(\mathcal A_{\mathbf s}, \beta - \lambda_0 - r(\mathbf s), \mu_{\mathrm{emp}}) - \epsilon(\mathbf s) \le \mathcal T(\mathcal A_{\mathbf s}, \beta, \mu) \le \mathcal T(\mathcal A_{\mathbf s}, \beta + \lambda_0 + r(\mathbf s), \mu_{\mathrm{emp}}) + \epsilon(\mathbf s).T(As​,β−λ0​−r(s),μemp​)−ϵ(s)≤T(As​,β,μ)≤T(As​,β+λ0​+r(s),μemp​)+ϵ(s).

The constants are the paper's, and KKK, ϵ\epsilonϵ, n^\hat nn^, MMM, μ\muμ, δ\deltaδ and the algorithm are arbitrary.

Milestones (Appendix C)

  1. Property 1 (p. 415): for a nonnegative XXX and levels 0≤β2≤β1≤10 \le \beta_2 \le \beta_1 \le 10≤β2​≤β1​≤1 (with β1=1\beta_1 = 1β1​=1 only for XXX bounded above), Qβ1(X)≥Qβ2(X)\mathbb Q^{\beta_1}(X) \ge \mathbb Q^{\beta_2}(X)Qβ1​(X)≥Qβ2​(X) and Tβ1(X)≥Tβ2(X)\mathbb T^{\beta_1}(X) \ge \mathbb T^{\beta_2}(X)Tβ1​(X)≥Tβ2​(X).
  2. Property 2 (p. 415): if Pr⁡(Y≥a)≥Pr⁡(X≥a)\Pr(Y \ge a) \ge \Pr(X \ge a)Pr(Y≥a)≥Pr(X≥a) for all aaa, then Qβ(Y)≥Qβ(X)\mathbb Q^\beta(Y) \ge \mathbb Q^\beta(X)Qβ(Y)≥Qβ(X) and Tβ(Y)≥Tβ(X)\mathbb T^\beta(Y) \ge \mathbb T^\beta(X)Tβ(Y)≥Tβ(X) for β∈[0,1]\beta \in [0,1]β∈[0,1].
  3. The event E\mathcal EE (pp. 415–416): with NiN_iNi​ the indices of samples in CiC_iCi​, ∑i∣∣Ni∣/n−μ(Ci)∣≤λ0\sum_i \big| |N_i|/n - \mu(C_i) \big| \le \lambda_0∑i​​∣Ni​∣/n−μ(Ci​)​≤λ0​ with probability at least 1−δ1 - \delta1−δ.

Significance

The result. Theorem 5 shows that any pseudo-robust algorithm has a testing-error quantile and truncated mean that are bracketed by the empirical ones at levels shifted by λ0+(n−n^(s))/n\lambda_0 + (n - \hat n(\mathbf s))/nλ0​+(n−n^(s))/n, up to the robustness tolerance ϵ(s)\epsilon(\mathbf s)ϵ(s). The quantile of the testing error can therefore be estimated from training data for every algorithm to which the robustness framework applies — among them majority voting, SVMs, Lasso and principal component analysis (Sect. 6 of the paper) — without a separate complexity analysis of the loss class. The pseudo-robust form covers algorithms that are robust only away from a small set of training samples, which is the typical situation in the presence of outliers. The robust case n^≡n\hat n \equiv nn^≡n is the paper's Theorem 2 (p. 400).

Formalizing it. The paper states Theorem 5 and proves it in Appendix C; no machine-checked proof exists. The appendix contains misprints (see Formalization scope) and the argument uses minimizers of the loss over each cell, which need not exist; a formal proof settles which steps are sound as written. The definitions of quantile value and truncated mean of a law on R\mathbb RR developed here are reusable beyond this mission.

Difficulty

The concentration step is the same as for the expected loss: on the event E\mathcal EE the empirical cell frequencies are close to the cell probabilities. The difficulty is converting this into a statement about quantiles. Quantile values are not linear in the distribution and are discontinuous in the level, so the triangle-inequality argument that bounds the mean-loss gap does not apply. Mass that moves between cells shifts every level of the quantile function, and the up to n−n^(s)n - \hat n(\mathbf s)n−n^(s) samples outside s^\hat{\mathbf s}s^ carry no guarantee at all, so an arbitrary fraction r(s)r(\mathbf s)r(s) of the empirical law is uncontrolled. For the truncated mean this must be done for the whole lower tail up to level β\betaβ, not just at one point, and the atoms of the loss distribution (the second branch of the definition) have to be accounted for exactly.

Formalization scope

  • The Lean namespace is XuMannorRobust.Quantile. Z\mathcal ZZ is a type with a measurable space structure, H\mathcal HH an arbitrary type, a training set a function Fin n → Z, and the i.i.d. law the product measure Measure.pi (fun _ => μ).
  • "With probability at least 1−δ1 - \delta1−δ" is encoded as: the outer measure of the set of training sets on which the claim fails is at most δ\deltaδ. No measurability of s↦As\mathbf s \mapsto \mathcal A_{\mathbf s}s↦As​ is needed.
  • Added measurability. The paper ignores measurability; the formalization requires each l(h,⋅)l(h,\cdot)l(h,⋅) and each cell CiC_iCi​ to be measurable.
  • Corrected Definition 3. The paper prints the second branch of the truncated mean as (β−Pr⁡[X<Q])/Pr⁡[X=Q]⋅Q\big(\beta - \Pr[X < Q]\big)/\Pr[X = Q] \cdot Q(β−Pr[X<Q])/Pr[X=Q]⋅Q. That contradicts its own worked example on p. 399, where the 0.630.630.63-truncated mean of a uniform law on c1<⋯<c10c_1 < \dots < c_{10}c1​<⋯<c10​ is 0.1(∑i≤6ci+0.3c7)0.1(\sum_{i \le 6} c_i + 0.3 c_7)0.1(∑i≤6​ci​+0.3c7​), and its verbal description. The formalization drops the division, as the example requires; with the printed formula Tβ\mathbb T^\betaTβ would not even be monotone in β\betaβ.
  • Qβ\mathbb Q^\betaQβ and Tβ\mathbb T^\betaTβ are defined on the law of the random variable, a measure on R\mathbb RR. Lean returns 000 for the infimum of an empty set or of a set unbounded below, so Q0=0\mathbb Q^0 = 0Q0=0 (the paper's value is −∞-\infty−∞). This never helps: Q(As,β,μ)≥0\mathcal Q(\mathcal A_{\mathbf s}, \beta, \mu) \ge 0Q(As​,β,μ)≥0 and ϵ(s)≥0\epsilon(\mathbf s) \ge 0ϵ(s)≥0, so the goal's inequalities remain meaningful at level 000. The goal keeps every level in [0,1][0,1][0,1] through the paper's side condition, which depends on n^(s)\hat n(\mathbf s)n^(s) and is therefore placed inside the probability event as a premise. The codomain {1,…,n}\{1, \dots, n\}{1,…,n} of n^\hat nn^ is part of the definition: with n^(s)=0\hat n(\mathbf s) = 0n^(s)=0 nothing would constrain ϵ(s)\epsilon(\mathbf s)ϵ(s).
  • The partition is fixed before the training set; the good subset s^\hat{\mathbf s}s^ may depend on s\mathbf ss and is a set of indices. Choosing the partition after s\mathbf ss would make pseudo robustness trivial and is ruled out.
  • Properties 1 and 2 are stated for nonnegative laws and levels in [0,1][0,1][0,1]. The level 111 is admitted only for a variable bounded above (for property 2, the dominating one). For an unbounded variable, Q1\mathbb Q^1Q1 is +∞+\infty+∞ in the paper, where the inequality is trivial, and a junk 000 in Lean. Property 3 of Appendix C (p. 415) is misprinted (with the constraint ∑αi≤β\sum \alpha_i \le \beta∑αi​≤β the minimum is 000) and is not formalized.
  • Needed infrastructure: the Bretagnolle–Huber–Carol inequality for multinomial frequencies (van der Vaart and Wellner 1996, Prop. A.6.6) (or a direct concentration argument), and elementary order properties of lower quantile values and truncated means of laws on R\mathbb RR. Contributions of these as separate lemmas are welcome.

Selected references

  • H. Xu and S. Mannor, Robustness and Generalization, Machine Learning 86(3):391–423, 2012. https://doi.org/10.1007/s10994-011-5268-1
  • R. Koenker and G. Bassett, Regression Quantiles, Econometrica 46(1):33–50, 1978. https://doi.org/10.2307/1913643
  • P. J. Huber, Robust Statistics, Wiley, 1981. https://doi.org/10.1002/0471725250
  • A. W. van der Vaart and J. A. Wellner, Weak Convergence and Empirical Processes, Springer, 1996 (Proposition A.6.6). https://doi.org/10.1007/978-1-4757-2545-2
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