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

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Campaigns (experimental)

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

Block Sensitivity vs. Sensitivity

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

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

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

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

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

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

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

≥ 2.131121719190Formalized record→≥ 2.15Open frontier
9 provers on it18 of 19 missions formalized

Integer Multiplication Below n log n

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

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

For two nnn-bit integers, the target is

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

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

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

3SUM Exponent

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

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

≤ 1.960614Formalized record→≤ 1.9202796Open frontier
4 provers on it7 of 8 missions formalized

All-Pairs Shortest Paths (APSP) Exponent

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

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

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

The irrationality measure of π

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

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

Sharp diagonal Hlawka constant

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

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

References:

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

Odd numbers as sums of primes

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

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

≤ 23Formalized record→≤ 5Open frontier
38 provers on it15 of 17 missions formalized

Matrix multiplication exponent

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

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

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

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

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Algebraic GeometryAnalysisOptimization·Captain: mikedeng1

Exploiting Symmetries in SDP-Relaxations for Polynomial Optimization 1: A G-Linear Functional Is Integration Against a G-Invariant Measure on K iff Its Symmetrized Localizing Forms Are PSDResearch Paper

Motivation

Polynomial optimization asks for the minimum f∗f^*f∗ of a polynomial fff over a set K⊆RnK\subseteq\mathbb R^nK⊆Rn cut out by polynomial inequalities. Lasserre's moment relaxation (Lasserre 2001) replaces the minimization over points by a minimization over probability measures on KKK, and then over linear functionals on polynomials that satisfy semidefinite constraints. The bridge between measures and semidefinite constraints is Putinar's theorem (Putinar 1993): on a compact basic semialgebraic set with an Archimedean description, a linear functional comes from a measure exactly when it is nonnegative on the quadratic module of the constraints.

Many problems of practical size are invariant under a group of linear transformations: permutations of variables, sign changes, rotations of a polygon. Gatermann and Parrilo (2004) showed how such symmetry block-diagonalizes sums-of-squares programs. Riener, Theobald, Jansson Andrén and Lasserre (arXiv:1103.0486, Math. Oper. Res. 2013) carry the reduction to the moment side. Their first step, Theorem 3.2, is a symmetric version of Putinar's theorem: for invariant data it suffices to consider functionals that are themselves invariant, and these are characterized by positivity of symmetrized localizing forms. This mission formalizes that theorem.

Setting

Write R[X]=R[X1,…,Xn]\mathbb R[X]=\mathbb R[X_1,\dots,X_n]R[X]=R[X1​,…,Xn​]. Let GGG be a finite subgroup of GLn(R)\mathrm{GL}_n(\mathbb R)GLn​(R). A matrix σ∈G\sigma\in Gσ∈G acts on points by x↦σxx\mapsto\sigma xx↦σx and on polynomials by

pσ(x):=p(σ−1x),p^\sigma(x):=p(\sigma^{-1}x),pσ(x):=p(σ−1x),

the linear substitution Xi↦∑j(σ−1)ijXjX_i\mapsto\sum_j(\sigma^{-1})_{ij}X_jXi​↦∑j​(σ−1)ij​Xj​. A polynomial is GGG-invariant if pσ=pp^\sigma=ppσ=p for every σ∈G\sigma\in Gσ∈G.

Fix g1,…,gm∈R[X]g_1,\dots,g_m\in\mathbb R[X]g1​,…,gm​∈R[X] and the feasible set

K={x∈Rn: gj(x)≥0, j=1,…,m}.K=\{x\in\mathbb R^n:\ g_j(x)\ge0,\ j=1,\dots,m\}.K={x∈Rn: gj​(x)≥0, j=1,…,m}.

Assumption 2.1 requires KKK to be compact and some polynomial u=u0+∑jujgju=u_0+\sum_j u_jg_ju=u0​+∑j​uj​gj​, with sums of squares u0,…,umu_0,\dots,u_mu0​,…,um​, to have a compact superlevel set {u≥0}\{u\ge0\}{u≥0}. Put g0:=1g_0:=1g0​:=1.

A linear map LG:R[X]→RL^G:\mathbb R[X]\to\mathbb RLG:R[X]→R is GGG-linear if LG(f)=LG(fσ)L^G(f)=L^G(f^\sigma)LG(f)=LG(fσ) for all fff and all σ∈G\sigma\in Gσ∈G. Its symmetrized localizing forms are

LgjG(p,q)=LG(1∣G∣∑σ∈G(p⋅q)σ⋅gj),0≤j≤m.\mathcal L^G_{g_j}(p,q)=L^G\Big(\frac1{|G|}\sum_{\sigma\in G}(p\cdot q)^\sigma\cdot g_j\Big),\qquad 0\le j\le m.Lgj​G​(p,q)=LG(∣G∣1​σ∈G∑​(p⋅q)σ⋅gj​),0≤j≤m.

For a Borel measure μ\muμ on Rn\mathbb R^nRn, μσ(B)=μ(σ−1(B))\mu^\sigma(B)=\mu(\sigma^{-1}(B))μσ(B)=μ(σ−1(B)) is its image under x↦σxx\mapsto\sigma xx↦σx, and μ\muμ is GGG-invariant if μσ=μ\mu^\sigma=\muμσ=μ for all σ∈G\sigma\in Gσ∈G. A measure on KKK is one with μ(Rn∖K)=0\mu(\mathbb R^n\setminus K)=0μ(Rn∖K)=0.

Formalization targets

Goal: Theorem 3.2

If the gjg_jgj​ are GGG-invariant and Assumption 2.1 holds, then for a GGG-linear LGL^GLG: ∃ μ finite, G-invariant, on K:  LG(p)=∫p dμ  ∀p⟺LgjG(p,p)≥0  ∀p∈R[X], ∀ 0≤j≤m.\exists\,\mu\ \text{finite, $G$-invariant, on }K:\ \ L^G(p)=\int p\,d\mu\ \ \forall p \quad\Longleftrightarrow\quad \mathcal L^G_{g_j}(p,p)\ge0\ \ \forall p\in\mathbb R[X],\ \forall\, 0\le j\le m.∃μ finite, G-invariant, on K:  LG(p)=∫pdμ  ∀p⟺Lgj​G​(p,p)≥0  ∀p∈R[X], ∀0≤j≤m.

Milestones

  1. Theorem 2.2 (Putinar). Under Assumption 2.1, a linear LLL is integration against a probability measure on KKK iff L(1)=1L(1)=1L(1)=1 and L(s0+∑jsjgj)≥0L(s_0+\sum_js_jg_j)\ge0L(s0​+∑j​sj​gj​)≥0 for all sums of squares s0,…,sms_0,\dots,s_ms0​,…,sm​.
  2. Averaging identity (p. 10). For GGG-linear LGL^GLG: LG(p)=1∣G∣∑σLG(pσ)=LG(1∣G∣∑σpσ)L^G(p)=\frac1{|G|}\sum_\sigma L^G(p^\sigma)=L^G\big(\frac1{|G|}\sum_\sigma p^\sigma\big)LG(p)=∣G∣1​∑σ​LG(pσ)=LG(∣G∣1​∑σ​pσ).
  3. Only-if computation (p. 11). For a finite GGG-invariant μ\muμ on compact KKK and invariant gjg_jgj​: ∫1∣G∣∑σ(f2)σgj dμ=∫f2gj dμ≥0\int\frac1{|G|}\sum_\sigma(f^2)^\sigma g_j\,d\mu=\int f^2g_j\,d\mu\ge0∫∣G∣1​∑σ​(f2)σgj​dμ=∫f2gj​dμ≥0.
  4. If computation (p. 11). For GGG-linear LGL^GLG and invariant ggg: LgG(h,h)=LG(h2g)\mathcal L^G_g(h,h)=L^G(h^2g)LgG​(h,h)=LG(h2g).
  5. Invariance from moments (p. 11). A finite measure on compact KKK with ∫h dμ=∫hσdμ\int h\,d\mu=\int h^\sigma d\mu∫hdμ=∫hσdμ for every polynomial hhh and every σ∈G\sigma\in Gσ∈G is GGG-invariant.

Significance

The result. Theorem 3.2 turns the moment relaxation of a GGG-invariant problem into one over GGG-linear functionals. Such a functional is determined by its values on the invariant ring R[X]G\mathbb R[X]^GR[X]G, so its moment variables are indexed by a basis of invariants instead of all monomials (Example 3.3 of the paper: five variables instead of fifteen for C4C_4C4​ on R4\mathbb R^4R4 in degree 2). The block-diagonalized relaxations and the convergence result of §3 (Theorems 3.4–3.7) rest on it.

Formalizing it. The theorem is proved in the paper, modulo Putinar's theorem, which is cited. Neither Putinar's theorem nor any Archimedean Positivstellensatz is in Mathlib or on the platform. A complete formalization therefore needs (i) Putinar's theorem itself, in its dual moment form, and (ii) the determinacy of compactly supported finite measures by polynomial moments in several variables. Both are reusable well beyond this paper: every moment-SOS hierarchy result in the literature cites them.

Difficulty

The group-theoretic steps (milestones 2–4) are finite averaging and change of variables. The weight of the theorem sits in two analytic facts. The first is Putinar's theorem: nonnegativity on the quadratic module is an algebraic condition, and producing a measure from it requires the Archimedean hypothesis of Assumption 2.1 in an essential way; without that hypothesis the statement is false in general. The second is that the measure Putinar's theorem returns has to be shown GGG-invariant. Equality of the polynomial moments of μ\muμ and μσ\mu^\sigmaμσ does not by itself identify two measures; it does so here because both are finite and carried by a compact set, where polynomials are dense in the continuous functions. A further detail: Putinar's theorem is stated for normalized functionals, and Theorem 3.2 is not normalized, so the degenerate case LG(1)=0L^G(1)=0LG(1)=0 must be shown to force LG=0L^G=0LG=0.

Formalization scope

Polynomials are MvPolynomial (Fin n) ℝ, points Fin n → ℝ, and GGG a Subgroup (GL (Fin n) ℝ) with a Fintype instance. The action on polynomials is the linear substitution aeval, so GGG is an arbitrary finite matrix group, not only a permutation group. Sums of squares are Mathlib's IsSumSq. "psd" for the symmetric form LgjG\mathcal L^G_{g_j}Lgj​G​ means LgjG(p,p)≥0\mathcal L^G_{g_j}(p,p)\ge0Lgj​G​(p,p)≥0 for every polynomial ppp, with no degree truncation; j=0j=0j=0 (g0=1g_0=1g0​=1) is included. Measures live on the Borel σ-algebra of Rn\mathbb R^nRn, μσ\mu^\sigmaμσ is Measure.map along the continuous (hence measurable) map x↦σxx\mapsto\sigma xx↦σx, and "measure on KKK" is μ(Rn∖K)=0\mu(\mathbb R^n\setminus K)=0μ(Rn∖K)=0.

Committed conventions and disclosed readings:

  • Finite measure. The paper writes "a GGG-invariant measure on KKK". It is formalized as a finite Borel measure; this is the reading that makes ∫p dμ\int p\,d\mu∫pdμ meaningful for every polynomial, and finite measures on a compact set make every polynomial integrable.
  • No normalization. As on the page, Theorem 3.2 has neither LG(1)=1L^G(1)=1LG(1)=1 nor a probability measure; Theorem 2.2 has both.
  • Direction of μσ\mu^\sigmaμσ. With μσ\mu^\sigmaμσ the image of μ\muμ under σ\sigmaσ, one has ∫hσdμ=∫h dμσ−1\int h^\sigma d\mu=\int h\,d\mu^{\sigma^{-1}}∫hσdμ=∫hdμσ−1, where the paper writes ∫h dμσ\int h\,d\mu^\sigma∫hdμσ. Statements quantify over all σ∈G\sigma\in Gσ∈G, so the difference does not change their content.

Trivializing formalizations are ruled out: integrals are taken only against finite measures carried by a compact set, so no statement holds because a Bochner integral of a non-integrable function is 000; positivity is through the forms on all of R[X]\mathbb R[X]R[X], not replaced by pointwise nonnegativity; and the invariance of μ\muμ is a conclusion of milestone 5, never a hypothesis.

Contributions welcome: Putinar's theorem (milestone 1) and multivariate moment determinacy on compact sets are the reusable infrastructure; the averaging milestones are a natural first entry point.

Selected references

  • C. Riener, T. Theobald, L. Jansson Andrén, J. B. Lasserre, Exploiting symmetries in SDP-relaxations for polynomial optimization, Math. Oper. Res. 38(1):122–141, 2013. arXiv:1103.0486v3, doi:10.1287/moor.1120.0558
  • M. Putinar, Positive polynomials on compact semi-algebraic sets, Indiana Univ. Math. J. 42(3):969–984, 1993. doi:10.1512/iumj.1993.42.42045
  • J. B. Lasserre, Global optimization with polynomials and the problem of moments, SIAM J. Optim. 11(3):796–817, 2001. doi:10.1137/S1052623400366802
  • K. Gatermann, P. A. Parrilo, Symmetry groups, semidefinite programs, and sums of squares, J. Pure Appl. Algebra 192:95–128, 2004. doi:10.1016/j.jpaa.2003.12.011
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CombinatoricsDiscrete GeometryGraph Theory·Captain: mikedeng1

Triangle-Free Intersection Graphs of Line Segments with Large Chromatic Number: For Every k ≥ 1 There Is a Triangle-Free Family of Plane Line Segments with Chromatic Number Greater than kResearch Paper

Motivation

A proper coloring of a graph assigns colors to its vertices so that adjacent vertices get different colors; the least number of colors that suffices is the chromatic number χ(G)\chi(G)χ(G). The clique number ω(G)\omega(G)ω(G) is the size of a largest set of pairwise adjacent vertices, and χ(G)≥ω(G)\chi(G)\ge\omega(G)χ(G)≥ω(G) always. A class of graphs is χ\chiχ-bounded if χ\chiχ is bounded by a function of ω\omegaω on the class. Abstract triangle-free graphs (ω≤2\omega\le2ω≤2) of arbitrarily large chromatic number have been known since Zykov (1949) and Mycielski (1955), so the question is which geometric classes are χ\chiχ-bounded.

For geometric intersection graphs (one vertex per set, an edge for each intersecting pair) the history is as follows.

  • 1960: Asplund and Grünbaum prove that families of axis-aligned rectangles in the plane are χ\chiχ-bounded.
  • 1965: Burling constructs triangle-free families of axis-aligned boxes in R3\mathbb R^3R3 with arbitrarily large chromatic number.
  • 1970s: Erdős asks whether families of line segments in the plane are χ\chiχ-bounded (Brass–Moser–Pach, Research Problems in Discrete Geometry, §9.6, Problem 2; Gyárfás 1987, Problem 1.9).
  • 2000–2014: positive special cases. McGuinness (2000) obtains bounds for triangle-free families; Suk (2014) improves them, proving that families of segments meeting a common line, and families of unit-length segments, are χ\chiχ-bounded.
  • 2014: Pawlik, Kozik, Krawczyk, Lasoń, Micek, Trotter and Walczak answer Erdős's question negatively (arXiv:1209.1595).

The same construction disproves Scott's conjecture (1997) that graphs excluding induced subdivisions of a fixed graph are χ\chiχ-bounded, as first observed by Fox and Pach.

Setting

Points of the plane are pairs (x,y)∈R×R(x,y)\in\mathbb R\times\mathbb R(x,y)∈R×R. A line segment is a closed set seg⁡(u,v)={(1−t)u+tv:0≤t≤1}\operatorname{seg}(u,v)=\{(1-t)u+tv: 0\le t\le1\}seg(u,v)={(1−t)u+tv:0≤t≤1} with two distinct endpoints u≠vu\neq vu=v. A family of segments S=(σi)i<N\mathcal S=(\sigma_i)_{i<N}S=(σi​)i<N​ is a finite indexed list of pairwise distinct segments. Its intersection graph has vertex set {0,…,N−1}\{0,\dots,N-1\}{0,…,N−1}, and i≠ji\neq ji=j are adjacent exactly when σi∩σj≠∅\sigma_i\cap\sigma_j\neq\emptysetσi​∩σj​=∅. The family is triangle-free if no three of its segments pairwise intersect, and χ(S)\chi(\mathcal S)χ(S) is the chromatic number of its intersection graph.

The milestones use the paper's auxiliary notions. An axis-aligned rectangle is R=[a,c]×[b,d]R=[a,c]\times[b,d]R=[a,c]×[b,d], with x∈[a,c]x\in[a,c]x∈[a,c] and y∈[b,d]y\in[b,d]y∈[b,d]. For a family S\mathcal SS inside the open interior of RRR, a probe for (S,R)(\mathcal S,R)(S,R) is a rectangle P=[a′,c]×[b′,d′]P=[a',c]\times[b',d']P=[a′,c]×[b′,d′] sharing the right edge line of RRR such that (i) a<a′<ca<a'<ca<a′<c and b<b′<d′<db<b'<d'<db<b′<d′<d; (ii) no segment meets the left edge of PPP; (iii) no segment has an endpoint in the closed rectangle PPP; (iv) the segments meeting PPP are pairwise disjoint. The diagonal DPD_PDP​ runs from the bottom-left corner (a′,b′)(a',b')(a′,b′) to the top-right corner (c,d′)(c,d')(c,d′) of PPP. The sequences sk,pks_k,p_ksk​,pk​ are given by s1=p1=1s_1=p_1=1s1​=p1​=1, sk+1=(pk+1)sk+pk2s_{k+1}=(p_k+1)s_k+p_k^2sk+1​=(pk​+1)sk​+pk2​ and pk+1=2pk2p_{k+1}=2p_k^2pk+1​=2pk2​.

Formalization targets

Goal: Theorem 1 (p. 2)

For every integer k≥1k\ge1k≥1 there is a finite family S\mathcal SS of distinct line segments in the plane with triangle-free intersection graph and

χ(S)>k.\chi(\mathcal S)>k .χ(S)>k.

The goal fixes no size for S\mathcal SS and no particular construction.

Milestones

  1. Base case of Lemma 2 (p. 3): one segment and one probe in any rectangle of positive area.
  2. Diagonal claim (p. 3): for a probe QQQ of a family inside the interior of RRR, a segment meets DQD_QDQ​ if and only if it meets QQQ.
  3. Color-count dichotomy (p. 4): for a proper coloring of an intersection graph and two index sets XXX, YYY each seeing at least kkk colors, if the color sets differ then X∪YX\cup YX∪Y sees at least k+1k+1k+1 colors; if they agree, a member adjacent to all of YYY gets a new color, and XXX together with it sees at least k+1k+1k+1 colors.
  4. Induction step (pp. 3–4): Lemma 2 at kkk for every rectangle gives Lemma 2 at k+1k+1k+1 for every rectangle.
  5. Lemma 2 (p. 3): for k≥1k\ge1k≥1 and a rectangle RRR of positive area there are a triangle-free family Sk\mathcal S_kSk​ of exactly sks_ksk​ segments in the interior of RRR and pkp_kpk​ pairwise disjoint probes for (Sk,R)(\mathcal S_k,R)(Sk​,R) such that every proper coloring of Sk\mathcal S_kSk​ uses at least kkk colors on the segments meeting some probe.
  6. The family S~k\tilde{\mathcal S}_kS~k​ (p. 4): adding the diagonals of all probes to a family with the conclusion of Lemma 2 gives a triangle-free family with χ>k\chi>kχ>k.

Significance

Theorem 1 shows that segment intersection graphs are not χ\chiχ-bounded, and it settles negatively the question for every class containing them: intersection graphs of curves crossing at most once (Kratochvíl–Nešetřil), McGuinness's class of arcwise connected sets with connected pairwise intersections, and string graphs in general. Through the Fox–Pach observation it refutes Scott's conjecture on induced subdivisions, a purely graph-theoretic statement. The counts in Lemma 2 give ∣S~k∣=sk+pk|\tilde{\mathcal S}_k|=s_k+p_k∣S~k​∣=sk​+pk​, so the maximum chromatic number of a triangle-free family of nnn segments is Ω(log⁡log⁡n)\Omega(\log\log n)Ω(loglogn) (§4 of the paper). The family S~k\tilde{\mathcal S}_kS~k​ has the same intersection graph as Burling's boxes.

The theorem is proved on paper; to the best of current knowledge no machine-checked proof exists. The mission produces a Lean 4 statement of the result about actual segments in R2\mathbb R^2R2, a reusable definition of intersection graphs of plane sets, and the paper's probe machinery stated precisely enough to support a full formal proof.

Difficulty

Abstract triangle-free graphs with large chromatic number are easy to build, but almost none of them are intersection graphs of segments, and the standard constructions (Mycielski, Zykov, shift graphs) do not come with a geometric realization. The difficulty is geometric: the construction has to place every new segment so that it meets exactly a prescribed independent set of old segments and nothing else, at every level of a doubly exponential nesting, while keeping finitely many rectangles disjoint and segment endpoints out of them. In a formal development the burden falls on the planar facts the paper treats as evident in one line each: which edges of a rectangle a segment can cross, when two segments must cross, and why the probe conditions survive when families are nested inside one another.

Formalization scope

  • The plane is ℝ × ℝ (first coordinate xxx, second yyy), and segments are Mathlib's closed segment ℝ u v. A family is e : Fin N → (ℝ × ℝ) × (ℝ × ℝ) (endpoint pairs) with seg (e i) the iii-th segment. "A family of line segments" is read as non-degenerate ((e i).1 ≠ (e i).2) and pairwise distinct (Function.Injective (fun i => seg (e i))).
  • interGraph F : SimpleGraph ι is the intersection graph of an indexed family of plane sets: i ≠ j ∧ (F i ∩ F j).Nonempty. Triangle-free is CliqueFree 3; χ\chiχ is Mathlib's chromaticNumber : ℕ∞, and the goal states the literal (k:N∞)<χ(k:\mathbb N_\infty)<\chi(k:N∞​)<χ.
  • Rectangles keep the page's letter order, Rect = ⟨a, c, b, d⟩ for [a,c]×[b,d][a,c]\times[b,d][a,c]×[b,d], with positive area as a separate hypothesis. A probe is stored as (a′,b′,d′)(a',b',d')(a′,b′,d′) and is the closed rectangle [a′,c]×[b′,d′][a',c]\times[b',d'][a′,c]×[b′,d′]; the interior of RRR is open.
  • sSeq k, pSeq k are sk,pks_k,p_ksk​,pk​, 1-based; every statement assumes k≥1k\ge1k≥1 (the value at 000 is junk).
  • Proper colorings take values in an arbitrary type, and "uses at least kkk colors on the segments meeting PPP" is k≤k\lek≤ ncard of the image of those segments.
  • The diagonal claim and the S~k\tilde{\mathcal S}_kS~k​ milestone are stated for any data with the relevant properties, not only for the paper's construction; the hypotheses are exactly those the page's sentences use.
  • The goal is about the intersection graph of the segments the existential provides. A statement about an abstract triangle-free graph with χ>k\chi>kχ>k is a different, much weaker theorem (already available via Mycielski's construction) and does not count.

Needed infrastructure: elementary planar geometry of segments and axis-aligned rectangles (membership, edges, crossing of two segments via the intermediate value theorem), affine images of segment families, and finite coloring counts. The segment and intersection-graph definitions are reusable for other questions on geometric intersection graphs. Contributions are welcome on any milestone, in particular a complete proof of the diagonal claim and of the induction step.

Selected references

  • A. Pawlik, J. Kozik, T. Krawczyk, M. Lasoń, P. Micek, W. T. Trotter, B. Walczak, Triangle-free intersection graphs of line segments with large chromatic number, J. Combin. Theory Ser. B 105 (2014) 6–10; preprint arXiv:1209.1595v5 (2014). https://arxiv.org/abs/1209.1595
  • A. Pawlik, J. Kozik, T. Krawczyk, M. Lasoń, P. Micek, W. T. Trotter, B. Walczak, Triangle-free geometric intersection graphs with large chromatic number, Discrete Comput. Geom. 50(3) (2013) 714–726. https://arxiv.org/abs/1212.2058
  • J. P. Burling, On coloring problems of families of prototypes, PhD thesis, University of Colorado, Boulder, 1965.
  • E. Asplund, B. Grünbaum, On a colouring problem, Math. Scand. 8 (1960) 181–188.
  • P. Brass, W. Moser, J. Pach, Research Problems in Discrete Geometry, Springer, 2005.
  • A. Gyárfás, Problems from the world surrounding perfect graphs, Zastos. Mat. 19 (1987) 413–441.
  • A. Suk, Coloring intersection graphs of x-monotone curves in the plane, Combinatorica 34(4) (2014) 487–505.
  • A. D. Scott, Induced trees in graphs of large chromatic number, J. Graph Theory 24(4) (1997) 297–311.
  • J. Mycielski, Sur le coloriage des graphes, Colloq. Math. 3 (1955) 161–162.
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Machine LearningOptimizationProbability·Captain: mikedeng1

On Nonconvex Optimization for Machine Learning: Gradients, Stochasticity, and Saddle Points 2: Perturbed GD (Variant) Makes Half Its Iterates ε-Second-Order Stationary within Õ(ℓΔ_f/ε²) IterationsResearch Paper

Why saddle points matter for nonconvex learning

Training a model in machine learning usually means minimizing a nonconvex function f:Rd→Rf:\mathbb R^d\to\mathbb Rf:Rd→R with first-order methods. Finding a global minimum of a general nonconvex function is NP-hard, so the classical guarantee for gradient descent (GD), xt+1=xt−η∇f(xt)x_{t+1}=x_t-\eta\nabla f(x_t)xt+1​=xt​−η∇f(xt​), is weaker: with step size η=1/ℓ\eta=1/\ellη=1/ℓ it reaches a point with ∥∇f(x)∥≤ε\|\nabla f(x)\|\le\varepsilon∥∇f(x)∥≤ε within ℓ(f(x0)−f⋆)/ε2\ell(f(x_0)-f^\star)/\varepsilon^2ℓ(f(x0​)−f⋆)/ε2 iterations, independently of the dimension (Nesterov, 1998). Such a point can be a saddle point. For many learning problems (matrix sensing and completion, phase retrieval, dictionary learning, tensor decomposition), every approximate second-order stationary point is an approximate global minimum, so an algorithm that avoids saddle points solves the problem.

Jin, Netrapalli, Ge, Kakade and Jordan (arXiv:1902.04811, J. ACM 2021) show that simple perturbed versions of GD and SGD find approximate second-order stationary points in essentially the number of iterations GD needs for first-order stationarity, up to polylogarithmic factors in the dimension. Their §5 gives a short, self-contained proof for a variant of perturbed GD (Algorithm 4). That proof is the subject of this mission.

Timeline:

  • 2015: Ge, Huang, Jin and Yuan show that noisy SGD escapes strict saddle points in polynomial time.
  • 2017: Jin, Ge, Netrapalli, Kakade and Jordan (ICML) prove that perturbed GD finds an ε\varepsilonε-second-order stationary point in O~(ℓΔf/ε2)\tilde O(\ell\Delta_f/\varepsilon^2)O~(ℓΔf​/ε2) iterations, with a geometric argument on the "stuck region".
  • 2019: arXiv:1902.04811 extends this to SGD and simplifies the deterministic proof through the improve or localize lemma (Lemma 21). §5 of that paper is formalized here.

Setting

Let f:Rd→Rf:\mathbb R^d\to\mathbb Rf:Rd→R, d≥1d\ge1d≥1, with gradient ∇f\nabla f∇f and Hessian ∇2f\nabla^2 f∇2f; ∥⋅∥\|\cdot\|∥⋅∥ is the Euclidean norm on vectors and the spectral norm on matrices. Assumption A: fff is ℓ\ellℓ-gradient Lipschitz, ∥∇f(x1)−∇f(x2)∥≤ℓ∥x1−x2∥\|\nabla f(x_1)-\nabla f(x_2)\|\le\ell\|x_1-x_2\|∥∇f(x1​)−∇f(x2​)∥≤ℓ∥x1​−x2​∥, and ρ\rhoρ-Hessian Lipschitz, ∥∇2f(x1)−∇2f(x2)∥≤ρ∥x1−x2∥\|\nabla^2f(x_1)-\nabla^2f(x_2)\|\le\rho\|x_1-x_2\|∥∇2f(x1​)−∇2f(x2​)∥≤ρ∥x1​−x2​∥. A point xxx is an ε\varepsilonε-second-order stationary point (ε\varepsilonε-SOSP) if

∥∇f(x)∥≤εand∇2f(x)⪰−ρε I.\|\nabla f(x)\|\le\varepsilon\qquad\text{and}\qquad\nabla^2 f(x)\succeq-\sqrt{\rho\varepsilon}\,I .∥∇f(x)∥≤εand∇2f(x)⪰−ρε​I.

Write f⋆=inf⁡ff^\star=\inf ff⋆=inff and Δf=f(x0)−f⋆\Delta_f=f(x_0)-f^\starΔf​=f(x0​)−f⋆.

Algorithm 4 (Perturbed GD, Variant). With step size η\etaη, radius rrr, time interval T\mathscr TT and tolerance ε\varepsilonε, start with tperturb=0t_{\text{perturb}}=0tperturb​=0. At iteration ttt: if ∥∇f(xt)∥≤ε\|\nabla f(x_t)\|\le\varepsilon∥∇f(xt​)∥≤ε and t−tperturb>Tt-t_{\text{perturb}}>\mathscr Tt−tperturb​>T, replace xtx_txt​ by xt−ηξtx_t-\eta\xi_txt​−ηξt​ with ξt∼Uniform(B0(r))\xi_t\sim\mathrm{Uniform}(B_0(r))ξt​∼Uniform(B0​(r)) and set tperturb=tt_{\text{perturb}}=ttperturb​=t; then xt+1=xt−η∇f(xt)x_{t+1}=x_t-\eta\nabla f(x_t)xt+1​=xt​−η∇f(xt​). The parameters are those of Eq. (6):

η=1ℓ,r=ε400ι3,T=ℓρε ι,F=150ι3ε3ρ,S=14ιερ,\eta=\frac1\ell,\quad r=\frac{\varepsilon}{400\iota^3},\quad\mathscr T=\frac{\ell}{\sqrt{\rho\varepsilon}}\,\iota,\quad\mathscr F=\frac{1}{50\iota^3}\sqrt{\frac{\varepsilon^3}{\rho}},\quad\mathscr S=\frac{1}{4\iota}\sqrt{\frac{\varepsilon}{\rho}},η=ℓ1​,r=400ι3ε​,T=ρε​ℓ​ι,F=50ι31​ρε3​​,S=4ι1​ρε​​,

where ι\iotaι is a logarithmic factor, and ω=22−ιℓS\omega=2^{2-\iota}\ell\mathscr Sω=22−ιℓS.

Formalization targets

Goal: Theorem 18

For T=⌈8max⁡{ΔfT/F, Δf/(ηε2)}⌉T=\lceil 8\max\{\Delta_f\mathscr T/\mathscr F,\ \Delta_f/(\eta\varepsilon^2)\}\rceilT=⌈8max{Δf​T/F, Δf​/(ηε2)}⌉ (which equals ⌈400ι4ℓΔf/ε2⌉\lceil400\iota^4\ell\Delta_f/\varepsilon^2\rceil⌈400ι4ℓΔf​/ε2⌉) and every ι≥1\iota\ge1ι≥1 with

Tℓdρε ι228−ι≤δ,\frac{T\ell\sqrt d}{\sqrt{\rho\varepsilon}}\,\iota^2 2^{8-\iota}\le\delta,ρε​Tℓd​​ι228−ι≤δ,

with probability at least 1−δ1-\delta1−δ over the perturbations,

#{t<T: xt is an ε-SOSP} ≥ T/2.\#\{t<T:\ x_t\text{ is an }\varepsilon\text{-SOSP}\}\ \ge\ T/2 .#{t<T: xt​ is an ε-SOSP} ≥ T/2.

The paper writes the count as O~(ℓΔf/ε2)\tilde O(\ell\Delta_f/\varepsilon^2)O~(ℓΔf​/ε2) with ι=clog⁡(dℓΔf/(ρεδ))\iota=c\log(d\ell\Delta_f/(\rho\varepsilon\delta))ι=clog(dℓΔf​/(ρεδ)).

Milestones, in the order the proof uses them

  1. Lemma 19 (descent): f(xt+1)−f(xt)≤−η∥∇f(xt)∥2/2f(x_{t+1})-f(x_t)\le-\eta\|\nabla f(x_t)\|^2/2f(xt+1​)−f(xt​)≤−η∥∇f(xt​)∥2/2 for η≤1/ℓ\eta\le1/\ellη≤1/ℓ.
  2. Lemma 21 (improve or localize): ∥xτ−x0∥≤2ηt(f(x0)−f(xt))\|x_\tau-x_0\|\le\sqrt{2\eta t(f(x_0)-f(x_t))}∥xτ​−x0​∥≤2ηt(f(x0​)−f(xt​))​ for t≥τ>0t\ge\tau>0t≥τ>0.
  3. Lemma 22 (coupling sequence): if λmin⁡(∇2f(x~))≤−ρε\lambda_{\min}(\nabla^2f(\tilde x))\le-\sqrt{\rho\varepsilon}λmin​(∇2f(x~))≤−ρε​ and two GD runs start within ηr\eta rηr of x~\tilde xx~, ηr0\eta r_0ηr0​ apart along the bottom eigenvector with r0>ωr_0>\omegar0​>ω, one of them decreases fff by F\mathscr FF within T\mathscr TT steps.
  4. Volume display (§5, proof of Lemma 20, p. 15): w Vol(B0d−1(a))/Vol(B0d(a))=waπΓ(d/2+1)Γ(d/2+1/2)≤wad/πw\,\mathrm{Vol}(\mathbb B^{d-1}_0(a))/\mathrm{Vol}(\mathbb B^d_0(a))=\frac{w}{a\sqrt\pi}\frac{\Gamma(d/2+1)}{\Gamma(d/2+1/2)}\le\frac wa\sqrt{d/\pi}wVol(B0d−1​(a))/Vol(B0d​(a))=aπ​w​Γ(d/2+1/2)Γ(d/2+1)​≤aw​d/π​.
  5. Lemma 20 (escaping saddle points): at x~\tilde xx~ with ∥∇f(x~)∥≤ε\|\nabla f(\tilde x)\|\le\varepsilon∥∇f(x~)∥≤ε and λmin⁡≤−ρε\lambda_{\min}\le-\sqrt{\rho\varepsilon}λmin​≤−ρε​,
P(f(xT)−f(x~)≤−F/2)≥1−ℓdρε ι228−ιfor x0=x~+ηξ.\mathbb P\bigl(f(x_{\mathscr T})-f(\tilde x)\le-\mathscr F/2\bigr)\ge1-\frac{\ell\sqrt d}{\sqrt{\rho\varepsilon}}\,\iota^22^{8-\iota}\quad\text{for }x_0=\tilde x+\eta\xi .P(f(xT​)−f(x~)≤−F/2)≥1−ρε​ℓd​​ι228−ιfor x0​=x~+ηξ.

Significance

The result. Theorem 18 says that adding occasional small random perturbations to gradient descent costs only a polylogarithmic factor over the first-order rate ℓΔf/ε2\ell\Delta_f/\varepsilon^2ℓΔf​/ε2 and buys second-order stationarity. Combined with the landscape results above, it gives polynomial-time guarantees for gradient methods on those learning problems. Lemma 20, on its own, is a quantitative statement that strict saddle points are unstable under perturbed GD; Lemmas 21 and 22 are reusable tools for any analysis of first-order methods near saddle points.

Formalizing it. The results are proved in the paper; none of them is formalized. A formal development would give machine-checked versions of the descent lemma for Hessian-Lipschitz functions, the improve-or-localize lemma, the coupling argument and the probabilistic escape bound. It would also settle the issue disclosed under Formalization scope.

Difficulty

Lemmas 19 and 21 are short. The difficulty is in Lemma 22 and Lemma 20. The obvious approach, linearizing GD around the saddle and following the unstable eigendirection, fails because the stuck region (starting points that do not escape within T\mathscr TT steps) has no simple shape once fff is not quadratic. The coupling argument controls the difference of two runs instead. It needs an induction in which the non-quadratic error term stays below half of the leading term for all T\mathscr TT steps, with the constants of Eq. (6) used exactly (2ηρST=1/22\eta\rho\mathscr S\mathscr T=1/22ηρST=1/2). Lemma 20 then turns a statement about pairs of points into a measure bound: a set whose every line parallel to e1e_1e1​ meets it in a segment of length at most ηω\eta\omegaηω has volume at most ηω\eta\omegaηω times the (d−1)(d-1)(d−1)-volume of the ball. In Lean this needs Fubini over a rotated coordinate system and measurability of the stuck region. Theorem 18 requires a probabilistic accounting over the whole run, under the product law of the perturbations.

Formalization scope

Rd\mathbb R^dRd is EuclideanSpace ℝ (Fin d) with d≥1d\ge1d≥1. The Hessian is fderiv ℝ (gradient f) x, the derivative of the gradient map, with the operator norm. Statements about λmin⁡\lambda_{\min}λmin​ use the quadratic form: λmin⁡(H)≤−c\lambda_{\min}(H)\le-cλmin​(H)≤−c is "some unit vvv has ⟨Hv,v⟩≤−c\langle Hv,v\rangle\le-c⟨Hv,v⟩≤−c", and H⪰−cIH\succeq-cIH⪰−cI is "⟨Hv,v⟩≥−c∥v∥2\langle Hv,v\rangle\ge-c\|v\|^2⟨Hv,v⟩≥−c∥v∥2 for all vvv". Uniform(B0(r))\mathrm{Uniform}(B_0(r))Uniform(B0​(r)) is normalized Lebesgue measure on the open ball. Algorithm 4 is a deterministic function of the perturbation vectors, which have the product law on (Rd)T(\mathbb R^d)^T(Rd)T. The ttt-th iterate is the point tested at the start of iteration ttt, and "half of its iterations" counts t∈{0,…,T−1}t\in\{0,\dots,T-1\}t∈{0,…,T−1}. Probability statements bound the failure event from above.

The paper's O~(⋅)\tilde O(\cdot)O~(⋅) is instantiated as the proof does:

  • the parameters are exactly Eq. (6), and T=⌈8max⁡{ΔfT/F,Δf/(ηε2)}⌉T=\lceil8\max\{\Delta_f\mathscr T/\mathscr F,\Delta_f/(\eta\varepsilon^2)\}\rceilT=⌈8max{Δf​T/F,Δf​/(ηε2)}⌉ (p. 16);
  • ι\iotaι is any real ≥1\ge1≥1 satisfying the proof's condition (Tℓd/ρε)ι228−ι≤δ(T\ell\sqrt d/\sqrt{\rho\varepsilon})\iota^22^{8-\iota}\le\delta(Tℓd​/ρε​)ι228−ι≤δ, in place of ι=clog⁡(dℓΔf/(ρεδ))\iota=c\log(d\ell\Delta_f/(\rho\varepsilon\delta))ι=clog(dℓΔf​/(ρεδ)). The printed argument of the logarithm changes under rescaling x↦λxx\mapsto\lambda xx↦λx while every quantity in the proof does not, so the printed choice can give ι≤0\iota\le0ι≤0;
  • T\mathscr TT is a natural number equal to ℓι/ρε\ell\iota/\sqrt{\rho\varepsilon}ℓι/ρε​, with no rounding, because the proof uses xTx_{\mathscr T}xT​ and 2ηρST=1/22\eta\rho\mathscr S\mathscr T=1/22ηρST=1/2 exactly;
  • ℓ≥ρε\ell\ge\sqrt{\rho\varepsilon}ℓ≥ρε​ (footnote 1, p. 14), ι≥1\iota\ge1ι≥1, η>0\eta>0η>0 and fff bounded below are the standing assumptions of §5.

A Hessian not tied to fff, an arbitrary unit vector in place of the bottom eigenvector in Lemma 22, a per-realization or existential statement in place of the product-law probability, or a vacuous ι\iotaι would each trivialize the statements; none is used.

Disclosed gap. The proof of Theorem 18 (p. 16) bounds the number of perturbations by applying Lemma 20 at each one. Algorithm 4 also perturbs at points that are already ε\varepsilonε-SOSPs, where Lemma 20 does not apply, and the T\mathscr TT iterations after such a perturbation are not counted. The goal is posed as printed; a solver who finds it false should report this in the discussion. The milestones do not depend on the gap.

Needed infrastructure: second-order Taylor bounds for Hessian-Lipschitz functions, symmetry of the Hessian and existence of a bottom eigenvector, volumes of Euclidean balls (in Mathlib through Γ\GammaΓ), a Fubini-type slicing bound for sets of bounded width along a direction, and measurability of the GD iterates. The volume-ratio and slicing lemmas are reusable beyond this mission. Proofs of any milestone, and alternative proofs, are welcome.

Selected references

  • C. Jin, P. Netrapalli, R. Ge, S. M. Kakade, M. I. Jordan, On Nonconvex Optimization for Machine Learning: Gradients, Stochasticity, and Saddle Points, arXiv:1902.04811v2 (2019); J. ACM 68(2), 2021. https://arxiv.org/abs/1902.04811
  • C. Jin, R. Ge, P. Netrapalli, S. M. Kakade, M. I. Jordan, How to Escape Saddle Points Efficiently, ICML 2017. https://arxiv.org/abs/1703.00887
  • R. Ge, F. Huang, C. Jin, Y. Yuan, Escaping From Saddle Points — Online Stochastic Gradient for Tensor Decomposition, COLT 2015. https://arxiv.org/abs/1503.02101
  • Y. Nesterov, Introductory Lectures on Convex Programming, Volume I: Basic Course, 1998; Kluwer, 2004. https://doi.org/10.1007/978-1-4419-8853-9
  • Y. Nesterov, B. T. Polyak, Cubic regularization of Newton method and its global performance, Math. Program. 108 (2006). https://doi.org/10.1007/s10107-006-0706-8
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Operations ResearchOptimal TransportOptimization+1·Captain: mikedeng1

A Short and General Duality Proof for Wasserstein Distributionally Robust Optimization I: Worst-Case Loss = min over λ ≥ 0 of λρ + E[sup f − λc] for All ρ > 0 iff Interchangeability HoldsResearch Paper

Motivation

Wasserstein distributionally robust optimization (DRO) hedges a decision against every probability distribution within a given transport distance of a nominal one, typically the empirical distribution of data. The inner problem, the worst-case loss, is an optimization over an infinite-dimensional set of measures, and every practical use of Wasserstein DRO — tractable reformulations, statistical guarantees, regularization interpretations — rests on a strong duality theorem that replaces it with a one-dimensional minimization over a Lagrange multiplier.

Such duality theorems have been proved under progressively weaker hypotheses:

  • Mohajerin Esfahani and Kuhn (2018) and Zhao and Guan (2018): empirical nominal distributions on subsets of Rd\mathbb R^dRd, via conic duality.
  • Blanchet and Murthy (2019): Polish spaces, lower semi-continuous costs and upper semi-continuous losses, via an approximation argument (arXiv:1604.01446).
  • Gao and Kleywegt (2023): Polish spaces with costs that are powers of a metric and arbitrary measurable losses (arXiv:1604.02199).
  • Zhang, Yang and Gao (2022, v4 2024): an arbitrary measurable space, an arbitrary measurable cost with values in [0,∞][0,\infty][0,∞] and a measurable loss, with duality characterized exactly by an interchangeability principle (arXiv:2205.00362).

This mission formalizes the last of these, Theorem 1 of Zhang–Yang–Gao.

Setting

Let (X,F,P^)(\mathcal X,\mathcal F,\widehat{\mathbb P})(X,F,P) be a probability space, f:X→Rf:\mathcal X\to\mathbb Rf:X→R a measurable loss with EP^[f]>−∞\mathbb E_{\widehat{\mathbb P}}[f]>-\inftyEP​[f]>−∞, and c:X×X→[0,∞]c:\mathcal X\times\mathcal X\to[0,\infty]c:X×X→[0,∞] a measurable transport cost with c(x,x)=0c(x,x)=0c(x,x)=0 (Assumption 1). Expectations take values in Rˉ=[−∞,∞]\bar{\mathbb R}=[-\infty,\infty]Rˉ=[−∞,∞], and the convention 0⋅∞=∞0\cdot\infty=\infty0⋅∞=∞ is used for products λc\lambda cλc.

The Kantorovich transport cost between P^\widehat{\mathbb P}P and a probability measure P\mathbb PP is

Kc(P^,P)=inf⁡γ∈Γ(P^,P)E(X^,X)∼γ[c(X^,X)],\mathcal K_c(\widehat{\mathbb P},\mathbb P)=\inf_{\gamma\in\Gamma(\widehat{\mathbb P},\mathbb P)}\mathbb E_{(\widehat X,X)\sim\gamma}[c(\widehat X,X)],Kc​(P,P)=γ∈Γ(P,P)inf​E(X,X)∼γ​[c(X,X)],

where Γ(P^,P)\Gamma(\widehat{\mathbb P},\mathbb P)Γ(P,P) is the set of couplings with marginals P^\widehat{\mathbb P}P and P\mathbb PP. The worst-case loss is

L(ρ)=sup⁡P{EX∼P[f(X)]:Kc(P^,P)≤ρ},\mathcal L(\rho)=\sup_{\mathbb P}\big\{\mathbb E_{X\sim\mathbb P}[f(X)]:\mathcal K_c(\widehat{\mathbb P},\mathbb P)\le\rho\big\},L(ρ)=Psup​{EX∼P​[f(X)]:Kc​(P,P)≤ρ},

with L(ρ)=−∞\mathcal L(\rho)=-\inftyL(ρ)=−∞ for ρ<0\rho<0ρ<0. For λ≥0\lambda\ge0λ≥0 let ϕλ(x^,x)=f(x)−λc(x^,x)\phi_\lambda(\widehat x,x)=f(x)-\lambda c(\widehat x,x)ϕλ​(x,x)=f(x)−λc(x,x) and

G(λ)=EX^∼P^[sup⁡x∈Xϕλ(X^,x)].\mathcal G(\lambda)=\mathbb E_{\widehat X\sim\widehat{\mathbb P}}\Big[\sup_{x\in\mathcal X}\phi_\lambda(\widehat X,x)\Big].G(λ)=EX∼P​[x∈Xsup​ϕλ​(X,x)].

ΓP^\Gamma_{\widehat{\mathbb P}}ΓP​ is the set of probability measures on X×X\mathcal X\times\mathcal XX×X with first marginal P^\widehat{\mathbb P}P. A measurable ϕ:X×X→R∪{−∞}\phi:\mathcal X\times\mathcal X\to\mathbb R\cup\{-\infty\}ϕ:X×X→R∪{−∞} satisfies the interchangeability principle (IP) if x^↦sup⁡xϕ(x^,x)\widehat x\mapsto\sup_x\phi(\widehat x,x)x↦supx​ϕ(x,x) is P^\widehat{\mathbb P}P-measurable (measurable for the completion of F\mathcal FF) and

EX^∼P^[sup⁡xϕ(X^,x)]=sup⁡γ∈ΓP^E(X^,X)∼γ[ϕ(X^,X)].\mathbb E_{\widehat X\sim\widehat{\mathbb P}}\Big[\sup_{x}\phi(\widehat X,x)\Big]=\sup_{\gamma\in\Gamma_{\widehat{\mathbb P}}}\mathbb E_{(\widehat X,X)\sim\gamma}[\phi(\widehat X,X)].EX∼P​[xsup​ϕ(X,x)]=γ∈ΓP​sup​E(X,X)∼γ​[ϕ(X,X)].

The Legendre transform of h:R→Rˉh:\mathbb R\to\bar{\mathbb R}h:R→Rˉ is h∗(λ)=sup⁡ρ∈R{λρ−h(ρ)}h^*(\lambda)=\sup_{\rho\in\mathbb R}\{\lambda\rho-h(\rho)\}h∗(λ)=supρ∈R​{λρ−h(ρ)}.

Formalization targets

Goal: Theorem 1, (D)

ϕλ\phi_\lambdaϕλ​ satisfies (IP) for every λ>0\lambda>0λ>0 if and only if the supremum functions are P^\widehat{\mathbb P}P-measurable and

L(ρ)=min⁡λ≥0{λρ+EX^∼P^[sup⁡x∈X{f(x)−λc(X^,x)}]}∀ρ>0.\mathcal L(\rho)=\min_{\lambda\ge0}\Big\{\lambda\rho+\mathbb E_{\widehat X\sim\widehat{\mathbb P}}\Big[\sup_{x\in\mathcal X}\{f(x)-\lambda c(\widehat X,x)\}\Big]\Big\}\qquad\forall\rho>0.L(ρ)=λ≥0min​{λρ+EX∼P​[x∈Xsup​{f(x)−λc(X,x)}]}∀ρ>0.

The minimum is attained. Both sides may be +∞+\infty+∞.

Milestones

  1. Lemma 1. L\mathcal LL is bounded below by EP^[f]\mathbb E_{\widehat{\mathbb P}}[f]EP​[f], increasing and concave on [0,∞)[0,\infty)[0,∞).
  2. (P-soft). For λ>0\lambda>0λ>0, (−L)∗(−λ)=sup⁡{EP[f]−λKc(P^,P):Kc<∞}(-\mathcal L)^*(-\lambda)=\sup\{\mathbb E_{\mathbb P}[f]-\lambda\mathcal K_c(\widehat{\mathbb P},\mathbb P):\mathcal K_c<\infty\}(−L)∗(−λ)=sup{EP​[f]−λKc​(P,P):Kc​<∞}.
  3. Theorem 1, first display. (−L)∗(−λ)=sup⁡γ∈ΓP^Eγ[f(X)−λc(X^,X)](-\mathcal L)^*(-\lambda)=\sup_{\gamma\in\Gamma_{\widehat{\mathbb P}}}\mathbb E_\gamma[f(X)-\lambda c(\widehat X,X)](−L)∗(−λ)=supγ∈ΓP​​Eγ​[f(X)−λc(X,X)] for λ>0\lambda>0λ>0.
  4. Lemma 3. Properties of λ↦h∗(−λ)\lambda\mapsto h^*(-\lambda)λ↦h∗(−λ) for a decreasing convex proper hhh that is +∞+\infty+∞ on (−∞,0)(-\infty,0)(−∞,0).
  5. Lemma 2. (−L)∗(−⋅)(-\mathcal L)^*(-\cdot)(−L)∗(−⋅) and G\mathcal GG are bounded below by EP^[f]\mathbb E_{\widehat{\mathbb P}}[f]EP​[f], decreasing, convex and lower semi-continuous on [0,∞)[0,\infty)[0,∞) (two items).
  6. Theorem 1, second display. L(ρ)=min⁡λ≥0{λρ+sup⁡γ∈ΓP^Eγ[f(X)−λc(X^,X)]}\mathcal L(\rho)=\min_{\lambda\ge0}\{\lambda\rho+\sup_{\gamma\in\Gamma_{\widehat{\mathbb P}}}\mathbb E_\gamma[f(X)-\lambda c(\widehat X,X)]\}L(ρ)=minλ≥0​{λρ+supγ∈ΓP​​Eγ​[f(X)−λc(X,X)]} for ρ>0\rho>0ρ>0: duality with no assumption beyond Assumption 1.
  7. Theorem 1, third display. For fixed λ>0\lambda>0λ>0, ϕλ\phi_\lambdaϕλ​ satisfies (IP) iff (−L)∗(−λ)=G(λ)(-\mathcal L)^*(-\lambda)=\mathcal G(\lambda)(−L)∗(−λ)=G(λ).

Significance

The result. Theorem 1 separates Wasserstein DRO duality into two parts. The first, the second display, holds with no regularity at all: the worst-case loss always equals a one-dimensional minimum over λ\lambdaλ of a supremum over couplings with fixed first marginal. The second identifies exactly when that supremum can be moved inside the expectation, which is the form (D) used in applications: (D) holds for all radii if and only if (IP) holds. The question of when Wasserstein DRO has its standard dual becomes a question about measurable selection and measurable projection, which is studied in a companion mission of this series. The duality results of the timeline above become special cases in which (IP) can be verified.

Formalizing it. The results are proved in the paper; none of them has a machine-checked proof. A formalization produces a verified duality theorem at the level of generality of measurable spaces with extended-valued costs, together with a reusable layer: Kantorovich costs with values in [0,∞][0,\infty][0,∞], extended-real expectations, and one-dimensional Legendre transforms of extended-real functions.

Difficulty

The proof is short on paper because it delegates to one-dimensional convex analysis: the involution h∗∗=cl⁡hh^{**}=\operatorname{cl}hh∗∗=clh of the Legendre transform on R\mathbb RR (Rockafellar, Theorem 12.2), applied to −L-\mathcal L−L. The work is in the extended reals. L\mathcal LL can be +∞+\infty+∞ on all of (0,∞)(0,\infty)(0,∞), (−L)∗(-\mathcal L)^*(−L)∗ can be identically +∞+\infty+∞, and the costs and products involve 0⋅∞0\cdot\infty0⋅∞. Concavity of L\mathcal LL on [0,∞)[0,\infty)[0,∞) requires mixing near-optimal distributions and couplings, and lower semi-continuity of G\mathcal GG requires Fatou's lemma for functions bounded below by fff, not by 000. The "only if" direction of the goal has to recover (IP) for every λ>0\lambda>0λ>0 from (D), which goes through biconjugation of G\mathcal GG and the right continuity at λ=0\lambda=0λ=0 of both transforms. A proof that treats every value as finite does not cover the theorem.

Formalization scope

The Lean development lives in the namespace ShortWDRODual.Legendre.

  • X\mathcal XX is a measurable space and P^\widehat{\mathbb P}P a probability measure. The cost is ENNReal-valued and curried, c x̂ x, with the nominal point first. The loss is real-valued and measurable.
  • Kc\mathcal K_cKc​ is the published RWPI.SqrtLasso.transportCost (infimum over probability couplings of the lower Lebesgue integral of ccc, in [0,∞][0,\infty][0,∞]).
  • Expectations are the published ModelRiskOT.Duality.extIntegral, ∫φ+−∫φ−\int\varphi^+-\int\varphi^-∫φ+−∫φ− in EReal. This agrees with the paper whenever one part is finite. It assigns −∞-\infty−∞ to the undefined case ∞−∞\infty-\infty∞−∞, so a law or coupling with an undefined expectation never raises a supremum.
  • The ball constraint Kc≤ρ\mathcal K_c\le\rhoKc​≤ρ is compared in EReal, so that L(ρ)=−∞\mathcal L(\rho)=-\inftyL(ρ)=−∞ for ρ<0\rho<0ρ<0. Reading it as Kc≤max⁡(ρ,0)\mathcal K_c\le\max(\rho,0)Kc​≤max(ρ,0) would make every Legendre transform +∞+\infty+∞.
  • λc\lambda cλc uses the paper's 0⋅∞=∞0\cdot\infty=\infty0⋅∞=∞ (Mathlib's product has 0⋅∞=00\cdot\infty=00⋅∞=0). This matters for λ=0\lambda=0λ=0: the supremum is then over {x:c(x^,x)<∞}\{x:c(\widehat x,x)<\infty\}{x:c(x,x)<∞}.
  • "min" is attainment plus lower bound (IsLeast). Concavity, convexity and monotonicity of extended-real functions are stated as explicit inequalities with real weights. Lower semi-continuity "on [0,∞)[0,\infty)[0,∞)" is relative to [0,∞)[0,\infty)[0,∞).
  • P^\widehat{\mathbb P}P-measurability is NullMeasurable. Disclosed reading: in the goal and in the fixed-λ\lambdaλ milestone, the measurability of the supremum functions is stated explicitly next to the duality formula, because the paper's expectation in (D) presupposes it and (IP) contains it. Lemma 2's statement on G\mathcal GG assumes this measurability for λ>0\lambda>0λ>0, for the same reason.
  • Ruled out: a goal that assumes (IP) and concludes (D) states only one direction. So does a goal that drops attainment, or uses Mathlib's 0⋅∞=00\cdot\infty=00⋅∞=0. All three are weaker theorems.

A complete development needs the one-dimensional Fenchel–Moreau theorem for extended-real functions on R\mathbb RR, gluing and mixing of couplings with a fixed first marginal, and Fatou's lemma for extIntegral. Each is reusable well beyond this mission. Contributions of any of these as separate lemmas are welcome.

Selected references

  • L. Zhang, J. Yang, R. Gao, A Short and General Duality Proof for Wasserstein Distributionally Robust Optimization, arXiv:2205.00362v4, 2024. https://arxiv.org/abs/2205.00362
  • J. Blanchet, K. Murthy, Quantifying Distributional Model Risk via Optimal Transport, Mathematics of Operations Research 44(2):565–600, 2019. https://arxiv.org/abs/1604.01446
  • R. Gao, A. Kleywegt, Distributionally Robust Stochastic Optimization with Wasserstein Distance, Mathematics of Operations Research 48(2):603–655, 2023. https://arxiv.org/abs/1604.02199
  • P. Mohajerin Esfahani, D. Kuhn, Data-driven Distributionally Robust Optimization Using the Wasserstein Metric, Mathematical Programming 171:115–166, 2018. https://arxiv.org/abs/1505.05116
  • R. T. Rockafellar, Convex Analysis, Princeton University Press, 1970. https://doi.org/10.1515/9781400873173
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Convex OptimizationOperations ResearchOptimization+1·Captain: mikedeng1

Distributionally Robust Convex Optimization I: Under the Nesting Condition, a Worst-Case Expectation Constraint over a Standardized Ambiguity Set Is Equivalent to a Finite Conic SystemResearch Paper

Motivation

A constraint E[v(x,z~)]≤w\mathbb E[v(x,\tilde z)] \le wE[v(x,z~)]≤w on a decision xxx requires the distribution of the random vector z~\tilde zz~. In practice that distribution is known only partially: its support, a few moments, or the probability mass of some regions estimated from data. Distributionally robust optimization asks that the constraint hold for every distribution consistent with this information. Wiesemann, Kuhn and Sim (Optimization Online 3757, 2013; Oper. Res. 62(6), 2014) proposed one standardized format for this information. Their format contains, as special cases, many ambiguity sets used earlier: support and moment information (Delage and Ye, 2010), and mean–covariance and directional-deviation information (Goh and Sim, 2010). They then characterized exactly when a worst-case expectation constraint over such a set has a finite conic reformulation. This mission formalizes that characterization: the paper's Theorem 1 and the steps of its proof.

Setting

The uncertain parameters are z~∈RP\tilde z \in \mathbb R^Pz~∈RP, and an auxiliary random vector u~∈RQ\tilde u \in \mathbb R^Qu~∈RQ may be added to describe structure of z~\tilde zz~. A proper cone K\mathcal KK is a closed convex cone with K∩(−K)={0}\mathcal K \cap(-\mathcal K) = \{0\}K∩(−K)={0} and nonempty interior. Write x≼Kyx \preccurlyeq_{\mathcal K} yx≼K​y for y−x∈Ky - x \in \mathcal Ky−x∈K, and K⋆={y:x⊤y≥0 ∀x∈K}\mathcal K^\star = \{y : x^\top y \ge 0\ \forall x \in \mathcal K\}K⋆={y:x⊤y≥0 ∀x∈K} for the dual cone. For indices i∈I={1,…,I}i \in \mathcal I = \{1,\dots,I\}i∈I={1,…,I} the confidence sets are

Ci={(z,u):Ciz+Diu≼Kici},\mathcal C_i = \{(z,u) : C_i z + D_i u \preccurlyeq_{\mathcal K_i} c_i\},Ci​={(z,u):Ci​z+Di​u≼Ki​​ci​},

with matrices Ci,DiC_i, D_iCi​,Di​, vectors cic_ici​ and proper cones Ki\mathcal K_iKi​. The ambiguity set is

P={P:EP[Az~+Bu~]=b,  P[(z~,u~)∈Ci]∈[p‾i,p‾i]  ∀i∈I},\mathcal P = \Big\{\mathbb P : \mathbb E_{\mathbb P}[A\tilde z + B\tilde u] = b,\ \ \mathbb P[(\tilde z,\tilde u) \in \mathcal C_i] \in [\underline p_i,\overline p_i]\ \ \forall i \in \mathcal I\Big\},P={P:EP​[Az~+Bu~]=b,  P[(z~,u~)∈Ci​]∈[p​i​,p​i​]  ∀i∈I},

where 0≤p‾i≤p‾i≤10 \le \underline p_i \le \overline p_i \le 10≤p​i​≤p​i​≤1. The paper imposes three conditions:

  • (C1) CI\mathcal C_ICI​ is bounded and p‾I=p‾I=1\underline p_I = \overline p_I = 1p​I​=p​I​=1;
  • (C2) some P∈P\mathbb P \in \mathcal PP∈P meets every non-degenerate probability bound strictly;
  • (C3) the constraint function is a maximum of finitely many bi-affine pieces,
v(x,z)=max⁡l=1,…,L[(Slz+sl)⊤x+tl⊤z+tl].v(x,z) = \max_{l = 1,\dots,L} \big[(S_l z + s_l)^\top x + \mathbf t_l^\top z + t_l\big].v(x,z)=l=1,…,Lmax​[(Sl​z+sl​)⊤x+tl⊤​z+tl​].

The distributionally robust constraint (3) is EP[v(x,z~)]≤w\mathbb E_{\mathbb P}[v(x,\tilde z)] \le wEP​[v(x,z~)]≤w for all P∈P\mathbb P \in \mathcal PP∈P.

A set AAA is strictly included in BBB, written A⋐BA \Subset BA⋐B, if AAA lies in the interior of BBB. The nesting condition (N) requires that any two distinct confidence sets be strictly nested or disjoint. For each iii, A(i)={i}∪{i′:Ci⋐Ci′}\mathcal A(i) = \{i\} \cup \{i' : \mathcal C_i \Subset \mathcal C_{i'}\}A(i)={i}∪{i′:Ci​⋐Ci′​} indexes the confidence sets containing Ci\mathcal C_iCi​.

Formalization targets

Goal: Theorem 1 (pp. 10–11)

Under (C1)–(C3), (N) and the two regularity conditions (S1)–(S2) described below, the constraint (3) holds if and only if there are β∈RK\beta \in \mathbb R^Kβ∈RK, κ,λ∈R+I\kappa,\lambda \in \mathbb R^I_+κ,λ∈R+I​ and ϕil∈Ki⋆\phi_{il} \in \mathcal K_i^\starϕil​∈Ki⋆​ such that, for all i∈Ii \in \mathcal Ii∈I and lll,

b⊤β+∑i[p‾iκi−p‾iλi]≤w,ci⊤ϕil+sl⊤x+tl≤∑i′∈A(i)[κi′−λi′],b^\top\beta + \sum_{i}\big[\overline p_i\kappa_i - \underline p_i\lambda_i\big] \le w,\qquad c_i^\top\phi_{il} + s_l^\top x + t_l \le \sum_{i' \in \mathcal A(i)}[\kappa_{i'} - \lambda_{i'}],b⊤β+i∑​[p​i​κi​−p​i​λi​]≤w,ci⊤​ϕil​+sl⊤​x+tl​≤i′∈A(i)∑​[κi′​−λi′​], Ci⊤ϕil+A⊤β=Sl⊤x+tl,Di⊤ϕil+B⊤β=0.C_i^\top\phi_{il} + A^\top\beta = S_l^\top x + \mathbf t_l,\qquad D_i^\top\phi_{il} + B^\top\beta = 0.Ci⊤​ϕil​+A⊤β=Sl⊤​x+tl​,Di⊤​ϕil​+B⊤β=0.

Milestones

  1. Theorem 1, sufficiency. The system implies (3), under (C1), (C3) and (N) alone.
  2. Lemma 1 (p. 34). For a strictly feasible conic confidence set, the semi-infinite constraint v(x,z)+f⊤z+g⊤u≤hv(x,z) + f^\top z + g^\top u \le hv(x,z)+f⊤z+g⊤u≤h on the set holds iff multipliers ϕl∈K⋆\phi_l \in \mathcal K^\starϕl​∈K⋆ exist with c⊤ϕl+sl⊤x+tl≤hc^\top\phi_l + s_l^\top x + t_l \le hc⊤ϕl​+sl⊤​x+tl​≤h, C⊤ϕl=Sl⊤x+tl+fC^\top\phi_l = S_l^\top x + \mathbf t_l + fC⊤ϕl​=Sl⊤​x+tl​+f and D⊤ϕl=gD^\top\phi_l = gD⊤ϕl​=g.
  3. The dual of the moment problem (p. 35). Constraint (3) holds iff some β\betaβ, κ,λ≥0\kappa,\lambda \ge 0κ,λ≥0 have objective value ≤w\le w≤w and satisfy [Az+Bu]⊤β+∑i1Ci(z,u)[κi−λi]≥v(x,z)[Az+Bu]^\top\beta + \sum_i \mathbf 1_{\mathcal C_i}(z,u)[\kappa_i - \lambda_i] \ge v(x,z)[Az+Bu]⊤β+∑i​1Ci​​(z,u)[κi​−λi​]≥v(x,z) on CI\mathcal C_ICI​.
  4. The partition step (p. 35). Under (N), the indicator constraint on CI\mathcal C_ICI​ is equivalent to constraints with the constant ∑A(i)\sum_{\mathcal A(i)}∑A(i)​ on the pieces C‾i=Ci∖⋃Ci′⋐CiCi′\overline{\mathcal C}_i = \mathcal C_i \setminus \bigcup_{\mathcal C_{i'} \Subset \mathcal C_i} \mathcal C_{i'}Ci​=Ci​∖⋃Ci′​⋐Ci​​Ci′​.
  5. The boundary step (pp. 35–36). The iii-th constraint holds on C‾i\overline{\mathcal C}_iCi​ iff it holds on all of Ci\mathcal C_iCi​.

Significance

When the Ki\mathcal K_iKi​ are orthants, second-order cones or semidefinite cones, Theorem 1 turns the semi-infinite, measure-valued constraint (3) into a linear, conic-quadratic or semidefinite system of size polynomial in the data. The paper's Theorem 2 shows that when nesting fails, even checking P≠∅\mathcal P \neq \emptysetP=∅ is strongly NP-hard. Theorem 1 is therefore the tractable side of a sharp dividing line. The paper builds its conservative approximation for non-nested sets (Theorem 3) and its lifting results (Section 3) on it.

The result is proved in the paper; nothing here is open. The formalization contributes two things. First, the duality theory for finite moment problems over measures on a compact set, and conic strong duality for strictly feasible sets: neither exists in Mathlib as stated. Second, a corrected statement. As printed, the "only if" direction of Theorem 1 is false, because (C2) does not give the strong duality the proof attributes to it. No machine-checked version of Theorem 1 is known.

Difficulty

The sufficiency half is weak duality: a pointwise inequality on CI\mathcal C_ICI​ integrated against any P∈P\mathbb P \in \mathcal PP∈P. The necessity half needs three facts.

  • Strong duality, with attainment, for an infinite-dimensional linear program over nonnegative measures. Here the obvious reference to a general conic duality theorem needs a constraint qualification on all moment constraints jointly, and (C2) controls only the probability bounds.
  • A geometric step: under (N), a constraint imposed on C‾i\overline{\mathcal C}_iCi​ extends to all of Ci\mathcal C_iCi​. This uses convexity of vvv in (z,u)(z,u)(z,u) together with the compactness of Ci\mathcal C_iCi​ and the strict inclusion of its descendants.
  • Conic duality with dual attainment for each confidence set (Lemma 1), which fails without strict feasibility.

Formalization scope

Vectors are Fin n → ℝ, products are Matrix.mulVec and dotProduct, and the outcome space is (Fin nP → ℝ) × (Fin nQ → ℝ) with its Borel σ\sigmaσ-algebra. The index set is Fin (nI + 1), 0-based, with CI\mathcal C_ICI​ = Fin.last nI. Probabilities are μ.real. Constraint (3) is stated in its "for all P\mathbb PP" form, so no supremum of reals appears. The scalar tlt_ltl​ and the vector tl\mathbf t_ltl​ are separate fields.

Every member of P\mathcal PP is a probability measure with finite first moment, so EP[Az~+Bu~]\mathbb E_{\mathbb P}[A\tilde z + B\tilde u]EP​[Az~+Bu~] is a genuine integral and not Lean's default value 000. The expectation EP[v(x,z~)]\mathbb E_{\mathbb P}[v(x,\tilde z)]EP​[v(x,z~)] is genuine as well, since vvv grows at most linearly. Hypothesis (C2) keeps P\mathcal PP nonempty, so (3) cannot hold vacuously. A sorry-free sanity file exhibits two nested intervals for which all hypotheses of the goal hold at once.

Hypotheses added to the paper's, each needed for a true statement:

  • (S1) moment-problem regularity. Every small common shift of bbb and of each probability interval stays feasible over finite measures on CI\mathcal C_ICI​. It is needed because with C1\mathcal C_1C1​ the unit disk, E[z~1]=1\mathbb E[\tilde z_1] = 1E[z~1​]=1, v=z2v = z_2v=z2​ and w=0w = 0w=0, constraint (3) holds but the system has no solution.
  • (S2) strict feasibility of every confidence set. It is needed because a confidence set that is a single boundary point of a second-order cone constraint admits no dual multipliers in Lemma 1.
  • Ci⊆CI\mathcal C_i \subseteq \mathcal C_ICi​⊆CI​ and P+Q≥1P + Q \ge 1P+Q≥1 in the partition and boundary steps. In dimension zero a set is strictly included in itself and C‾i\overline{\mathcal C}_iCi​ can be empty.

(S1) also excludes some instances the page allows: p‾i=0\overline p_i = 0p​i​=0 or p‾i=1\underline p_i = 1p​i​=1 for i≠Ii \ne Ii=I, and expectation rows that cannot be shifted in every direction by measures on CI\mathcal C_ICI​.

The sufficiency milestone drops (C2) and the standing bounds 0≤p‾i≤p‾i≤10 \le \underline p_i \le \overline p_i \le 10≤p​i​≤p​i​≤1, which only strengthens it.

Needed infrastructure, all reusable: conic duality for closed convex cones, Lagrangian duality for linear programs over finite measures on a compact set, and the extension of a convex inequality from the boundary of a compact set. Contributions of any of these as separate lemmas are welcome.

Selected references

  • W. Wiesemann, D. Kuhn, M. Sim, Distributionally Robust Convex Optimization, Optimization Online preprint 3757, version of September 22, 2013. https://optimization-online.org/wp-content/uploads/2013/02/3757.pdf ; Operations Research 62(6):1358–1376, 2014. https://doi.org/10.1287/opre.2014.1314
  • A. Shapiro, On duality theory of conic linear problems, in Semi-Infinite Programming, chapter 7, Kluwer, 2001 (reference [56] of the paper; the result the proof of Theorem 1 cites as Proposition 3.4).
  • E. Delage, Y. Ye, Distributionally robust optimization under moment uncertainty with application to data-driven problems, Operations Research 58(3):595–612, 2010. https://doi.org/10.1287/opre.1090.0741
  • J. Goh, M. Sim, Distributionally robust optimization and its tractable approximations, Operations Research 58(4):902–917, 2010. https://doi.org/10.1287/opre.1090.0712
  • A. Ben-Tal, A. Nemirovski, Lectures on Modern Convex Optimization, SIAM, 2001. https://doi.org/10.1137/1.9780898718829
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Algebraic GeometryOperations ResearchOptimization·Captain: mikedeng1

Optimality Conditions and Finite Convergence of Lasserre's Hierarchy II: Off a Proper Zariski-Closed Set of Input Data, the Classical Optimality Conditions Hold at Every Local MinimizerResearch Paper

Motivation

Lasserre's hierarchy is a sequence of semidefinite relaxations for minimizing a polynomial over a set defined by polynomial equations and inequalities (Lasserre 2001). Under the archimedean condition its optimal values converge to the true minimum, but only asymptotically in general; in practice the hierarchy is often exact at a small relaxation order. J. Nie's paper (arXiv:1206.0319v2, Math. Program. 146 (2014)) explains this gap in two steps. Its Theorem 1.1 shows that finite convergence follows when the classical optimality conditions of nonlinear programming hold at every global minimizer. Its Theorem 1.2, the subject of this mission, shows that those optimality conditions hold at every local minimizer for all input data outside the zero set of finitely many polynomials in the coefficients. Together the two results give finite convergence of Lasserre's hierarchy for generic archimedean problems.

The genericity statement is also of independent interest in nonlinear programming: it says that degenerate local minimizers (failing constraint qualification, strict complementarity or second order sufficiency) are an algebraically exceptional phenomenon for polynomial data of fixed degrees.

Setting

Fix nnn variables x=(x1,…,xn)x=(x_1,\dots,x_n)x=(x1​,…,xn​) and write R[x]d\mathbb R[x]_dR[x]d​ for the real polynomials of degree at most ddd. Problem (1.1) is

min⁡f(x)s.t.hi(x)=0 (i∈[m1]),gj(x)≥0 (j∈[m2]),\min f(x)\quad\text{s.t.}\quad h_i(x)=0\ (i\in[m_1]),\qquad g_j(x)\ge 0\ (j\in[m_2]),minf(x)s.t.hi​(x)=0 (i∈[m1​]),gj​(x)≥0 (j∈[m2​]),

with feasible set KKK. For u∈Ku\in Ku∈K the active set is J(u)={j:gj(u)=0}J(u)=\{j: g_j(u)=0\}J(u)={j:gj​(u)=0}. At uuu:

  • the constraint qualification condition (CQC) holds if ∇h1(u),…,∇hm1(u),∇gj(u)\nabla h_1(u),\dots,\nabla h_{m_1}(u),\nabla g_j(u)∇h1​(u),…,∇hm1​​(u),∇gj​(u) (j∈J(u)j\in J(u)j∈J(u)) are linearly independent;
  • Lagrange multipliers λ,μ\lambda,\muλ,μ satisfy (1.3) ∇f(u)=∑iλi∇hi(u)+∑jμj∇gj(u)\nabla f(u)=\sum_i\lambda_i\nabla h_i(u)+\sum_j\mu_j\nabla g_j(u)∇f(u)=∑i​λi​∇hi​(u)+∑j​μj​∇gj​(u) and (1.4) μjgj(u)=0\mu_jg_j(u)=0μj​gj​(u)=0, μj≥0\mu_j\ge0μj​≥0;
  • strict complementarity (1.5) is μj+gj(u)>0\mu_j+g_j(u)>0μj​+gj​(u)>0 for all jjj;
  • with L=f−∑iλihi−∑j∈J(u)μjgjL=f-\sum_i\lambda_ih_i-\sum_{j\in J(u)}\mu_jg_jL=f−∑i​λi​hi​−∑j∈J(u)​μj​gj​, the second order sufficiency condition (1.7) is vT∇2L(u)v>0v^T\nabla^2L(u)v>0vT∇2L(u)v>0 for every v≠0v\neq0v=0 orthogonal to all active constraint gradients.

The input data are the coefficient vectors of (f,h,g)∈R[x]d0×∏iR[x]di×∏jR[x]dj′(f,h,g)\in\mathbb R[x]_{d_0}\times\prod_i\mathbb R[x]_{d_i}\times\prod_j\mathbb R[x]_{d'_j}(f,h,g)∈R[x]d0​​×∏i​R[x]di​​×∏j​R[x]dj′​​; a polynomial in the coefficients is a real polynomial evaluated at that vector. The paper's Condition 4.3 lists four families of such polynomials: resultants Res\mathrm{Res}Res and discriminants Δ\DeltaΔ (§2.4) of subsets of the constraints, and the polynomials R\mathscr RR of (4.6) and D\mathscr DD of (4.11), which detect a complex projective solution of the homogenised critical-point systems (4.5) and (4.10). Homogenisation is p~(x~)=x0dp(x/x0)\tilde p(\tilde x)=x_0^{d}p(x/x_0)p~​(x~)=x0d​p(x/x0​) at the nominal degree ddd, with x~=(x0,…,xn)\tilde x=(x_0,\dots,x_n)x~=(x0​,…,xn​).

Formalization targets

Goal: Theorem 1.2

For positive degrees d0,di,dj′d_0,d_i,d'_jd0​,di​,dj′​ there are polynomials ϕ1,…,ϕL\phi_1,\dots,\phi_Lϕ1​,…,ϕL​ in the coefficients such that

∃ (f,h,g) admissible with ∏lϕl≠0,and∏lϕl(f,h,g)≠0 ⟹ CQC, (1.5), (1.7) at every local minimizer of (1.1).\exists\,(f,h,g)\text{ admissible with }\textstyle\prod_l\phi_l\neq0,\qquad\text{and}\qquad \prod_l\phi_l(f,h,g)\neq0\ \Longrightarrow\ \text{CQC, (1.5), (1.7) at every local minimizer of (1.1).}∃(f,h,g) admissible with ∏l​ϕl​=0,and∏l​ϕl​(f,h,g)=0 ⟹ CQC, (1.5), (1.7) at every local minimizer of (1.1).

Milestones

  1. Proposition 4.1: there is R\mathscr RR with R(p0,…,pk;q)=0\mathscr R(p_0,\dots,p_k;q)=0R(p0​,…,pk​;q)=0 iff (4.5) has a solution 0≠x~∈Cn+10\neq\tilde x\in\mathbb C^{n+1}0=x~∈Cn+1; and R≠0\mathscr R\neq0R=0 excludes solutions of (4.4) in Cn\mathbb C^nCn.
  2. Proposition 4.2: there is D\mathscr DD with D(p0,…,pk)=0\mathscr D(p_0,\dots,p_k)=0D(p0​,…,pk​)=0 iff (4.10) has a solution with x~≠0\tilde x\neq0x~=0, y≠0y\neq0y=0; and D≠0\mathscr D\neq0D=0 makes the KKT system (4.2) nonsingular.
  3. Proposition 4.4: at u∈Ku\in Ku∈K with multipliers satisfying (1.3) and μjgj(u)=0\mu_jg_j(u)=0μj​gj​(u)=0, items (a)–(d) of Condition 4.3 give at most n−m1n-m_1n−m1​ active constraints, CQC, λi≠0\lambda_i\neq0λi​=0 and μj≠0\mu_j\neq0μj​=0 on J(u)J(u)J(u), and det⁡H(u)≠0\det H(u)\neq0detH(u)=0 for H(u)=[∇2L(u)G(u)TG(u)0]H(u)=\left[\begin{smallmatrix}\nabla^2L(u)&G(u)^T\\G(u)&0\end{smallmatrix}\right]H(u)=[∇2L(u)G(u)​G(u)T0​].
  4. Lemma 4.6: at a local minimizer where G(u)G(u)G(u) has full rank, (1.7) holds iff det⁡H(u)≠0\det H(u)\neq0detH(u)=0.
  5. Proposition 4.5: Condition 4.3 implies CQC, strict complementarity and SOSC at every local minimizer.
  6. Appendix A: R\mathscr RR and D\mathscr DD do not vanish identically on the input space of given positive degrees.

Significance

The theorem gives the second half of the paper's explanation of finite convergence: combined with Theorem 1.1, Lasserre's hierarchy converges in finitely many steps for all archimedean problems with input outside a proper algebraic subset. Section 5 of the paper derives further consequences, for instance that Marshall's boundary Hessian condition holds on a Zariski open set of data, and that Putinar-type certificates exist generically on the boundary of the cone of nonnegative polynomials. Beyond polynomial optimization, the statement is a precise algebraic form of the folklore that "generic nonlinear programs are nondegenerate".

The result is proved in the paper; no machine-checked version is known. A formalization fixes the exact quantifier structure (the printed statement is vacuous without a nonvanishing clause, and two items of Proposition 4.4 need an extra hypothesis), and builds reusable infrastructure: projective elimination over C\mathbb CC, homogenisation at a nominal degree, and the bordered-Hessian characterization of second order sufficiency.

Difficulty

The local part (Proposition 4.4, Lemma 4.6, Proposition 4.5) is linear algebra plus first and second order necessary conditions. The global part is not. Proposition 4.1 and 4.2 need the main theorem of elimination theory: the set of coefficient vectors for which a homogeneous (or bihomogeneous) system has a nonzero complex solution is Zariski closed, defined by polynomials in the coefficients. Mathlib has the univariate resultant only. Appendix A, which shows these polynomials do not vanish identically, has to control the homogenised systems both at finite points and at points at infinity (x0=0x_0=0x0​=0), where only the leading forms of the data are seen. Reasoning over R\mathbb RR alone does not suffice: the set of data whose real system is solvable is not the zero set of a polynomial.

Formalization scope

Polynomials are MvPolynomial (Fin n) ℝ, points are Fin n → ℝ, and gradients and Hessians are formal partial derivatives. Homogenised polynomials have complex coefficients in n + 1 variables, variable 0 being x0x_0x0​, and homogenisation uses the nominal degree ddd, not the actual degree. CQC is linear independence of an indexed family (repeated gradients count twice). The optimality conditions are bundled: CQC together with one multiplier pair satisfying (1.3), (1.4), (1.5) and (1.7); under CQC the multipliers are unique.

Condition 4.3 is encoded through the defining properties of Res, Δ, R\mathscr RR and D\mathscr DD (unsolvability of the corresponding complex projective systems) rather than through the polynomials themselves; since the goal is existential in the polynomials, this is not a weakening. Coefficient variables exist for monomials of every degree, so the goal's nonvanishing clause is asserted at an admissible input: a formal polynomial that is nonzero but vanishes on all admissible data (such as the variable of a monomial of degree d0+1d_0+1d0​+1) does not satisfy it. Without that clause the printed theorem would be satisfied by ϕ1=0\phi_1=0ϕ1​=0.

Hypotheses added to the page, each disclosed in the statements: m1≤nm_1\le nm1​≤n in Propositions 4.4 and 4.5 (Condition 4.3's standing assumption; Theorem 1.2 is stated for all m1m_1m1​, as printed), the nonvanishing clause in Theorem 1.2, and item (a) of Condition 4.3 in Proposition 4.4 ii)–iv) (with item (b) alone, n=1n=1n=1, g1=x+x2g_1=x+x^2g1​=x+x2, g2=−x+x2g_2=-x+x^2g2​=−x+x2, u=0u=0u=0 violates CQC). Proposition 4.2's nonsingularity is asserted at all complex critical pairs.

A complete development needs projective elimination theory over C\mathbb CC (reusable well beyond this mission), multivariate resultants and discriminants as polynomial functions of coefficients, Euler's identity for forms, and genericity facts about critical points of polynomial programs. Contributions to any of these, and direct proofs of the local milestones, are welcome.

Selected references

  • J. Nie, Optimality conditions and finite convergence of Lasserre's hierarchy, Math. Program. 146 (2014); preprint arXiv:1206.0319v2, 2013. https://arxiv.org/abs/1206.0319v2, https://doi.org/10.1007/s10107-013-0680-x
  • J.B. Lasserre, Global optimization with polynomials and the problem of moments, SIAM J. Optim. 11(3) (2001) 796–817. https://doi.org/10.1137/S1052623400366802
  • R. Hartshorne, Algebraic Geometry, GTM 52, Springer, 1977 (Theorem I.5.7A, elimination). https://doi.org/10.1007/978-1-4757-3849-0
  • I. Gelfand, M. Kapranov, A. Zelevinsky, Discriminants, Resultants, and Multidimensional Determinants, Birkhäuser, 1994. https://doi.org/10.1007/978-0-8176-4771-1
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Harmonic AnalysisNumerical AnalysisProbability·Captain: mikedeng1

Isotropic Gaussian Random Fields on the Sphere: Regularity, Fast Simulation and Stochastic Partial Differential Equations III: Karhunen–Loève Truncation Error ≤ κ^{−β} a.s. for β < (α−2)/2Research Paper

Why approximate a random field on the sphere?

An isotropic Gaussian random field is a spatial random quantity whose probability law is unchanged when the sphere is rotated. Such fields model spatially distributed uncertainty when no direction is preferred. The question in this mission is concrete: if a field is simulated by retaining only finitely many spherical harmonic frequencies, how rapidly does the simulation approach the full field? Lang and Schwab study this question while developing regularity, simulation, and stochastic partial differential equation results for isotropic fields on spheres (Lang and Schwab, 2015). Their §5 separates the error in expected spatial energy from the error seen along an individual sample. The latter is the target here.

The field and its finite approximation

Let S2S^2S2 be the unit sphere in R3\mathbb R^3R3 and let σ\sigmaσ be surface area measure, with σ(S2)=4π\sigma(S^2)=4\piσ(S2)=4π. A point yyy has angular coordinates (ϑ,φ)(\vartheta,\varphi)(ϑ,φ), where y=(sin⁡ϑcos⁡φ,sin⁡ϑsin⁡φ,cos⁡ϑ)y=(\sin\vartheta\cos\varphi,\sin\vartheta\sin\varphi,\cos\vartheta)y=(sinϑcosφ,sinϑsinφ,cosϑ). Spherical harmonics YℓmY_{\ell m}Yℓm​ are the normalized complex functions indexed by a degree ℓ≥0\ell\ge0ℓ≥0 and an order −ℓ≤m≤ℓ-\ell\le m\le\ell−ℓ≤m≤ℓ. They form an orthonormal basis of complex L2(S2)L^2(S^2)L2(S2) with this unnormalized surface measure. The real factor Lℓm(ϑ)L_{\ell m}(\vartheta)Lℓm​(ϑ) is the normalized associated Legendre function appearing in Yℓm(ϑ,φ)=Lℓm(ϑ)eimφY_{\ell m}(\vartheta,\varphi)=L_{\ell m}(\vartheta)e^{im\varphi}Yℓm​(ϑ,φ)=Lℓm​(ϑ)eimφ for m≥0m\ge0m≥0 (§2, pp. 4–5).

The angular power spectrum is a nonnegative sequence (Aℓ)ℓ≥0(A_\ell)_{\ell\ge0}(Aℓ​)ℓ≥0​ recording the variance at each harmonic degree. Let Xℓm1X^1_{\ell m}Xℓm1​ and Xℓm2X^2_{\ell m}Xℓm2​ be independent standard normal random variables for the indices that occur below. The centered real field used in §5 is the ordered series

T(y)=∑ℓ=0∞(AℓXℓ01Lℓ0(ϑ)+2Aℓ∑m=1ℓLℓm(ϑ)(Xℓm1cos⁡(mφ)+Xℓm2sin⁡(mφ))).T(y)=\sum_{\ell=0}^{\infty}\left(\sqrt{A_\ell}X^1_{\ell0}L_{\ell0}(\vartheta)+\sqrt{2A_\ell}\sum_{m=1}^{\ell}L_{\ell m}(\vartheta)\bigl(X^1_{\ell m}\cos(m\varphi)+X^2_{\ell m}\sin(m\varphi)\bigr)\right).T(y)=ℓ=0∑∞​(Aℓ​​Xℓ01​Lℓ0​(ϑ)+2Aℓ​​m=1∑ℓ​Lℓm​(ϑ)(Xℓm1​cos(mφ)+Xℓm2​sin(mφ))).

Its Karhunen–Loève truncation TκT^\kappaTκ retains the outer sum through degree κ\kappaκ. These are the approximations analyzed and simulated in the paper (§5, p. 25). The norm ∥f∥L2(S2)\|f\|_{L^2(S^2)}∥f∥L2(S2)​ measures the spatial size of a sample fff, while ∥Z∥Lp(Ω;L2(S2))\|Z\|_{L^p(\Omega;L^2(S^2))}∥Z∥Lp(Ω;L2(S2))​ takes the pppth moment of that spatial norm over randomness. Lemma 5.1 relates this explicit series, in law, to an arbitrary centered isotropic Gaussian field with the same angular power spectrum (pp. 23–24).

Formalization targets

The goal, Corollary 5.4, assumes C>0C>0C>0, α>2\alpha>2α>2, an integer ℓ0≥1\ell_0\ge1ℓ0​≥1, and the tail condition Aℓ≤Cℓ−αA_\ell\le C\ell^{-\alpha}Aℓ​≤Cℓ−α for ℓ>ℓ0\ell>\ell_0ℓ>ℓ0​. It asserts almost-sure convergence in spatial L2L^2L2 and, for each β<(α−2)/2\beta<(\alpha-2)/2β<(α−2)/2, an eventual samplewise bound (p. 28):

∥T−Tκ∥L2(S2)≤κ−βfor all sufficiently large κ,P-almost surely.\|T-T^\kappa\|_{L^2(S^2)}\le\kappa^{-\beta}\qquad\text{for all sufficiently large }\kappa,\quad\mathbb P\text{-almost surely}.∥T−Tκ∥L2(S2)​≤κ−βfor all sufficiently large κ,P-almost surely.

The attack path retains three intermediate statements from §5. The squared mean-square error equals the exact spectral tail ∑ℓ>κ(2ℓ+1)Aℓ\sum_{\ell>\kappa}(2\ell+1)A_\ell∑ℓ>κ​(2ℓ+1)Aℓ​ (the proof of Proposition 5.2, p. 26). Proposition 5.2 establishes convergence in L2(Ω;L2(S2))L^2(\Omega;L^2(S^2))L2(Ω;L2(S2)) and the bound

∥T−Tκ∥L2(Ω;L2(S2))≤C^ κ−(α−2)/2,C^2=C(2α−2+1α−1)\|T-T^\kappa\|_{L^2(\Omega;L^2(S^2))}\le\widehat C\,\kappa^{-(\alpha-2)/2},\qquad \widehat C^2=C\left(\frac2{\alpha-2}+\frac1{\alpha-1}\right)∥T−Tκ∥L2(Ω;L2(S2))​≤Cκ−(α−2)/2,C2=C(α−22​+α−11​)

for κ≥ℓ0\kappa\ge\ell_0κ≥ℓ0​ (p. 25). Theorem 5.3 gives the same exponent for every finite p≥1p\ge1p≥1, with a constant depending only on p,C,αp,C,\alphap,C,α (p. 27). The goal's exponent may approach, but does not include, (α−2)/2(\alpha-2)/2(α−2)/2.

What the result supplies

The mean-square estimate controls average approximation error, but it does not itself say whether one sequence of simulated fields converges along almost every outcome. Corollary 5.4 supplies that pathwise assertion and a quantitative rate for each exponent below the spectral threshold. It identifies the resolution needed to make the spatial error small for almost every sample, rather than only on average. The threshold directly links harmonic spectral decay to numerical truncation quality.

The cited results are already proved in the paper; the remaining task is to formalize their statements and proofs for the explicit KL model. The definition layer provides a reusable real representation of normalized spherical harmonics and mixed norms on S2S^2S2. A completed proof would also make the transition from Gaussian moment estimates to samplewise convergence available as a machine-checked argument in this setting. No claim is made that these results already have machine-checked proofs.

Main difficulty

The spherical harmonics are orthonormal, but an error bound for the full field needs more than termwise estimates. It must control the infinite tail while keeping the harmonic normalization, Gaussian variances, and the surface measure consistent. The passage from an expected error to one bound that eventually holds along almost every sample also requires estimates for arbitrarily high finite moments. A fixed second-moment bound does not yield the full range of exponents in Corollary 5.4. The paper's constant in Proposition 5.2 and the parameter dependence of the constant in Theorem 5.3 therefore matter to the final statement.

Formalization scope

Lean uses EuclideanSpace ℝ (Fin 3) for the sphere. Coordinates 0,1,20,1,20,1,2 represent the paper's y1,y2,y3y_1,y_2,y_3y1​,y2​,y3​. volume.toSphere supplies surface measure of mass 4π4\pi4π. Legendre polynomials use Rodrigues' formula; the associated harmonics use Cartesian coordinates through (y1+iy2)m=sin⁡mϑeimφ(y_1+i y_2)^m=\sin^m\vartheta e^{im\varphi}(y1​+iy2​)m=sinmϑeimφ, so they are defined at the poles without choosing an angle there. The field is the limit of the ordered partial sums TκT^\kappaTκ. A nonconvergent sequence receives Lean's arbitrary limit value, but the theorems concern almost-everywhere convergence and norms, where such exceptional values must be shown irrelevant.

Spatial squared norms and mixed LpL^pLp norms are extended nonnegative integrals. This keeps nonintegrable functions from taking a false zero norm. Lean's natural numbers include zero; ℓ0∈N\ell_0\in\mathbb Nℓ0​∈N in the paper is recorded as ℓ0≥1\ell_0\ge1ℓ0​≥1. Decay is required only above ℓ0\ell_0ℓ0​, exactly where the paper requires it. Coefficients that enter the series are measurable, jointly independent, and standard normal. The unused coordinates Xℓ02X^2_{\ell0}Xℓ02​ are zero, as specified in Lemma 5.1; coefficients at invalid indices are unconstrained. The field is the explicit series of p. 25, with Lemma 5.1 supplying the paper's identification in law with any centered isotropic field. In Theorem 5.3 the constant is chosen before the field and probability space, preventing it from depending on a particular spectrum or cutoff. The almost-sure conclusion is a spatial L2L^2L2 claim, never a pointwise assertion at each sphere point.

The displayed identity on p. 26 omits a square on its left-hand norm, although the neighboring formulas use squared norms. The formal error identity restores the square and the milestone preserves the printed wording. Contributions to the harmonic normalization, exact spectral identity, uniform finite-moment estimates, and the final almost-sure result all fit this mission. The normalizations, the positive cutoff, and the explicit independent Gaussian coefficients rule out vacuous or zero-field encodings.

Selected references

  • A. Lang and Ch. Schwab, Isotropic Gaussian random fields on the sphere: regularity, fast simulation and stochastic partial differential equations, Annals of Applied Probability 25(6), 2015. arXiv:1305.1170v3
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CombinatoricsGraph TheoryMathematical Physics·Captain: mikedeng1

Algorithms for #BIS-Hard Problems on Expander Graphs 2: On Bipartite α-Expanders, the High-Fugacity Hard-Core Partition Function Reduces to Two Kotecký–Preiss Polymer ModelsResearch Paper

Motivation

The hard-core model on a finite graph GGG at fugacity λ>0\lambda > 0λ>0 weights each independent set III of GGG by λ∣I∣\lambda^{|I|}λ∣I∣. Its normalizing constant, the independence polynomial ZG(λ)Z_G(\lambda)ZG​(λ), is a basic object of statistical physics (a lattice gas with hard-core exclusion) and of combinatorics (ZG(1)Z_G(1)ZG​(1) counts independent sets).

The complexity of approximating ZG(λ)Z_G(\lambda)ZG​(λ) on graphs of maximum degree Δ\DeltaΔ is settled for general graphs: below the uniqueness threshold λc(Δ)=(Δ−1)Δ−1/(Δ−2)Δ\lambda_c(\Delta) = (\Delta-1)^{\Delta-1}/(\Delta-2)^{\Delta}λc​(Δ)=(Δ−1)Δ−1/(Δ−2)Δ there is a deterministic approximation scheme (Weitz, STOC 2006, doi:10.1145/1132516.1132538), and above it the problem is NP-hard to approximate. On bipartite graphs the picture is different. Approximately counting independent sets of a bipartite graph defines the class #BIS, whose complexity is a major open problem of approximate counting, and Cai, Galanis, Goldberg, Guo, Jerrum, Štefankovič and Vigoda showed that for Δ≥3\Delta \ge 3Δ≥3 and λ>λc(Δ)\lambda > \lambda_c(\Delta)λ>λc​(Δ) the hard-core model on bipartite graphs of maximum degree Δ\DeltaΔ is #BIS-hard (arXiv:1311.4839).

One route to partial progress is to find natural classes of bipartite graphs on which these #BIS-hard problems become tractable. Helmuth, Perkins and Regts did this for the hard-core model at high fugacity on the torus (Z/nZ)d(\mathbb Z/n\mathbb Z)^d(Z/nZ)d, using Pirogov–Sinai contour models and the cluster expansion (arXiv:1806.11548). Jenssen, Keevash and Perkins extended the method to abstract polymer models and to all bounded-degree bipartite expanders (arXiv:1807.04804; SIAM J. Comput. 49(4), 2020). This mission formalizes the mathematical core of their Theorem 1.

Setting

Let GGG be a finite bipartite graph with vertex classes O\mathcal OO (odd vertices) and E\mathcal EE (even vertices), n=∣O∣+∣E∣n = |\mathcal O| + |\mathcal E|n=∣O∣+∣E∣, and maximum degree at most Δ\DeltaΔ. For a vertex set SSS, the vertex boundary ∂S\partial S∂S is the set of vertices outside SSS with a neighbour in SSS. For α>0\alpha > 0α>0, GGG is a bipartite α\alphaα-expander if

∣∂S∣≥(1+α)∣S∣for all S⊆O, ∣S∣≤∣O∣/2, and all S⊆E, ∣S∣≤∣E∣/2.|\partial S| \ge (1+\alpha)|S| \quad\text{for all } S \subseteq \mathcal O,\ |S| \le |\mathcal O|/2, \text{ and all } S \subseteq \mathcal E,\ |S| \le |\mathcal E|/2.∣∂S∣≥(1+α)∣S∣for all S⊆O, ∣S∣≤∣O∣/2, and all S⊆E, ∣S∣≤∣E∣/2.

A subset of one class is small if it has at most half as many vertices as that class. The hard-core partition function is

ZG(λ)=∑I∈I(G)λ∣I∣,Z_G(\lambda) = \sum_{I \in \mathcal I(G)} \lambda^{|I|},ZG​(λ)=I∈I(G)∑​λ∣I∣,

with I(G)\mathcal I(G)I(G) the independent sets of GGG. A number Z^\hat ZZ^ is an ε\varepsilonε-relative approximation to ZZZ if e−εZ^≤Z≤eεZ^e^{-\varepsilon}\hat Z \le Z \le e^{\varepsilon}\hat Ze−εZ^≤Z≤eεZ^.

G2G^2G2 is the graph on the same vertices in which two distinct vertices are adjacent when their distance in GGG is at most 222; a set is G2G^2G2-connected when it induces a connected subgraph of G2G^2G2. An even polymer is a nonempty, small, G2G^2G2-connected set γ⊆E\gamma \subseteq \mathcal Eγ⊆E; odd polymers are defined in O\mathcal OO. Two polymers are compatible if their distance in GGG exceeds 222. Each polymer has the weight

wγ=λ∣γ∣(1+λ)∣∂γ∣,w_\gamma = \frac{\lambda^{|\gamma|}}{(1+\lambda)^{|\partial\gamma|}},wγ​=(1+λ)∣∂γ∣λ∣γ∣​,

and the polymer partition functions are ΞE(G)=∑Γ∏γ∈Γwγ\Xi^{\mathcal E}(G) = \sum_\Gamma \prod_{\gamma\in\Gamma} w_\gammaΞE(G)=∑Γ​∏γ∈Γ​wγ​, summed over the families Γ\GammaΓ of pairwise compatible even polymers (the empty family included), and ΞO(G)\Xi^{\mathcal O}(G)ΞO(G) likewise. Even polymers describe deviations from the ground state "all odd vertices occupied", and odd polymers from the other ground state.

Formalization targets

Goal: the deterministic core of Theorem 1

For α>0\alpha > 0α>0, Δ≥3\Delta \ge 3Δ≥3, every bipartite α\alphaα-expander GGG of maximum degree at most Δ\DeltaΔ on n≥3n \ge 3n≥3 vertices, and every

λ>max⁡{(2e3Δ4)1/α, e11/α},\lambda > \max\left\{(2e^3\Delta^4)^{1/\alpha},\ e^{11/\alpha}\right\},λ>max{(2e3Δ4)1/α, e11/α},
  1. Z~G(λ)=(1+λ)∣O∣ ΞE(G)+(1+λ)∣E∣ ΞO(G)\tilde Z_G(\lambda) = (1+\lambda)^{|\mathcal O|}\,\Xi^{\mathcal E}(G) + (1+\lambda)^{|\mathcal E|}\,\Xi^{\mathcal O}(G)Z~G​(λ)=(1+λ)∣O∣ΞE(G)+(1+λ)∣E∣ΞO(G) is an e−ne^{-n}e−n-relative approximation to ZG(λ)Z_G(\lambda)ZG​(λ);
  2. both polymer models satisfy the Kotecký–Preiss condition with g(γ)=∣γ∣g(\gamma) = |\gamma|g(γ)=∣γ∣: for every polymer γ\gammaγ,
∑γ′ incompatible with γwγ′ e2∣γ′∣≤∣γ∣.\sum_{\gamma' \text{ incompatible with } \gamma} w_{\gamma'}\, e^{2|\gamma'|} \le |\gamma|.γ′ incompatible with γ∑​wγ′​e2∣γ′∣≤∣γ∣.

Milestones

In the order of the paper's proof: Lemma 18 (every independent set has a small side); the identity Z~G(λ)=ZG(λ)+∑I sparseλ∣I∣\tilde Z_G(\lambda) = Z_G(\lambda) + \sum_{I \text{ sparse}} \lambda^{|I|}Z~G​(λ)=ZG​(λ)+∑I sparse​λ∣I∣; the size bound (2+α)∣I∣≤n(2+\alpha)|I| \le n(2+α)∣I∣≤n for sparse independent sets; Lemma 20 (part 1 of the goal); the weight bound wγ≤(1+λ)−α∣γ∣w_\gamma \le (1+\lambda)^{-\alpha|\gamma|}wγ​≤(1+λ)−α∣γ∣; the count of at most (eΔ2)t(e\Delta^2)^t(eΔ2)t G2G^2G2-connected ttt-sets through a vertex; and inequality (8), ∑γ′∋v(1+λ)−α∣γ′∣e2∣γ′∣≤1/Δ2\sum_{\gamma' \ni v} (1+\lambda)^{-\alpha|\gamma'|} e^{2|\gamma'|} \le 1/\Delta^2∑γ′∋v​(1+λ)−α∣γ′∣e2∣γ′∣≤1/Δ2.

Significance

The two parts of the goal are exactly what Theorem 8 of the paper (adapted from Helmuth, Perkins and Regts) consumes: given a polymer model satisfying the Kotecký–Preiss condition, the truncated cluster expansion of log⁡Ξ\log \XilogΞ yields an FPTAS and, through self-reducibility, a polynomial-time sampler. Together they give a deterministic approximate counting algorithm for a #BIS-hard problem on a natural graph class, at fugacities far above λc(Δ)\lambda_c(\Delta)λc​(Δ), the regime in which the problem is hard on general bipartite graphs. The same template (reduction to polymer models around ground states, then Kotecký–Preiss) underlies the paper's results for the Potts model, for random regular bipartite graphs and for proper colourings, and a large later literature on algorithms at low temperature.

The result is proved in the paper; to our knowledge none of it has been machine-checked. A formalization adds a precise treatment of the degenerate cases (see below), a reusable formal definition of abstract polymer models over vertex sets, and the elementary but intricate bijection between compatible polymer families and sparse sets.

Difficulty

Each step is elementary, and the difficulty lies in the bookkeeping. The reduction needs an exact correspondence between families of pairwise compatible polymers and sparse subsets of a class, and an exact double count over independent sets. The quantitative step of Lemma 20 compares the total weight of sparse independent sets, which have at most n/(2+α)n/(2+\alpha)n/(2+α) vertices, with ZG(λ)≥λn/2Z_G(\lambda) \ge \lambda^{n/2}ZG​(λ)≥λn/2; the printed last inequality, 2nλ−αn/(4+2α)≤e−n2^n\lambda^{-\alpha n/(4+2\alpha)} \le e^{-n}2nλ−αn/(4+2α)≤e−n, follows from λ>e11/α\lambda > e^{11/\alpha}λ>e11/α only for α\alphaα up to about 1.251.251.25, and larger α\alphaα forces both classes to have at most nine vertices, a finite range that needs its own argument. The Kotecký–Preiss half needs the count of connected sets in a bounded-degree graph (Lemma 14 of the paper, from Galvin and Kahn), applied to G2G^2G2, and a geometric series.

Formalization scope

The algorithmic conclusion of Theorem 1 (an FPTAS and a polynomial-time sampling algorithm, with running time (n/ε)O(log⁡Δ)(n/\varepsilon)^{O(\log\Delta)}(n/ε)O(logΔ)) is not formalized: Mathlib has no machine model and the running times carry unspecified constants. The goal is the mathematics the algorithm rests on: the reduction to two polymer models and the Kotecký–Preiss condition for both. The cluster expansion and Theorem 8 are not part of the mission.

Conventions. The graph is a SimpleGraph V on a finite type, with O\mathcal OO a Finset V and E\mathcal EE its complement; bipartiteness is a hypothesis. The fugacity is lam. "∣S∣≤∣O∣/2|S| \le |\mathcal O|/2∣S∣≤∣O∣/2" is 2 * #S ≤ #O in N\mathbb NN. Distances use the extended distance SimpleGraph.edist, so vertices in different components are never close. The Kotecký–Preiss sum ranges over the polymers of the same class incompatible with γ\gammaγ, including γ\gammaγ itself. Polymers are capped at half of their own class, not at n/2n/2n/2; the condition without this cap, or with compatibility in place of incompatibility, would be a different statement.

Two hypotheses differ from the page. Theorem 1 states the threshold as λ>CΔ4/α\lambda > C\Delta^{4/\alpha}λ>CΔ4/α for an absolute constant CCC; the goal uses the threshold its proof uses (§4.3). The hypothesis n≥3n \ge 3n≥3 is added: on the edgeless graph with one vertex in each class the expansion condition is vacuous, no side of the independent set VVV is small, and Lemma 18 and Lemma 20 fail.

A complete development needs: the bijection between compatible families and sparse sets, Lemma 14 for G2G^2G2, and real-power estimates. The polymer-model and graph-power definitions are reusable for the sibling missions of this series. Proofs of individual milestones are welcome independently.

Selected references

  • M. Jenssen, P. Keevash, W. Perkins, Algorithms for #BIS-hard problems on expander graphs, SIAM J. Comput. 49(4) (2020) 681–710. doi:10.1137/19M1286669, arXiv:1807.04804
  • T. Helmuth, W. Perkins, G. Regts, Algorithmic Pirogov–Sinai theory, Probab. Theory Related Fields 176 (2020) 851–895. arXiv:1806.11548
  • R. Kotecký, D. Preiss, Cluster expansion for abstract polymer models, Comm. Math. Phys. 103 (1986) 491–498. doi:10.1007/BF01211762
  • J.-Y. Cai, A. Galanis, L. A. Goldberg, H. Guo, M. Jerrum, D. Štefankovič, E. Vigoda, #BIS-hardness for 2-spin systems on bipartite bounded degree graphs in the tree non-uniqueness region, J. Comput. System Sci. 82 (2016) 690–711. arXiv:1311.4839
  • D. Weitz, Counting independent sets up to the tree threshold, STOC 2006, 140–149. doi:10.1145/1132516.1132538
  • D. Galvin, J. Kahn, On phase transition in the hard-core model on Zd\mathbb Z^dZd, Combin. Probab. Comput. 13 (2004) 137–164. doi:10.1017/S0963548303005947
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Operations ResearchOptimal TransportProbability+1·Captain: mikedeng1

A Stochastic Control Approach to No-Arbitrage Bounds Given Marginals, with an Application to Lookback Options: The Robust Superhedging Bound of g(X*_T) Given the Law of X_T Equals μ^HL(g)Research Paper

Model-free bounds for lookback options

A lookback option pays a function of the running maximum of the underlying asset over the life of the contract. When the prices of European call options of all strikes at the maturity are quoted, the risk-neutral law μ\muμ of the terminal price is known, but the law of the whole path is not. The robust (model-free) superhedging cost of the lookback payoff is the cheapest initial capital that, combined with a static position in the quoted calls and dynamic trading in the underlying, dominates the payoff in every model consistent with μ\muμ.

Hobson (Finance Stoch. 1998) computed this cost for g(x)=xg(x)=xg(x)=x by a pathwise inequality, and identified the extremal model through the Azéma–Yor solution of the Skorokhod embedding problem (Azéma–Yor 1979). Galichon, Henry-Labordère and Touzi (Ann. Appl. Probab. 2014, arXiv:1401.3921) recast model-free bounds as a dual stochastic control problem in which the marginal constraint is penalised by a Lagrange multiplier λ\lambdaλ. Their Theorem 3.1 recovers Hobson's bound for every C1C^1C1 nondecreasing ggg from that dual, with an explicit optimal multiplier and stopping time. The result is one of the founding examples of martingale optimal transport.

Setting

Let BBB be a real Brownian motion with continuous paths and B0=0B_0=0B0​=0, adapted to a filtration (Ft)t≥0(\mathcal F_t)_{t\ge0}(Ft​)t≥0​ with increments independent of the past, and let Xt=X0+BtX_t=X_0+B_tXt​=X0​+Bt​ for a spot X0∈RX_0\in\mathbb RX0​∈R. Write Xτ∗=max⁡t≤τXtX^*_\tau=\max_{t\le\tau}X_tXτ∗​=maxt≤τ​Xt​. Let T∞\mathcal T_\inftyT∞​ be the set of stopping times τ\tauτ for which the stopped process (Xt∧τ)t≥0(X_{t\wedge\tau})_{t\ge0}(Xt∧τ​)t≥0​ is a uniformly integrable martingale.

The marginal is a probability measure μ\muμ on R\mathbb RR with finite first moment and mean ∫x μ(dx)=X0\int x\,\mu(dx)=X_0∫xμ(dx)=X0​. Its call prices are c(x)=∫(y−x)+μ(dy)c(x)=\int(y-x)^+\mu(dy)c(x)=∫(y−x)+μ(dy). The payoff is ξ=g(X∗)\xi=g(X^*)ξ=g(X∗) with g:R→R+g:\mathbb R\to\mathbb R_+g:R→R+​ of class C1C^1C1 and nondecreasing.

For a multiplier λ:R→R\lambda:\mathbb R\to\mathbb Rλ:R→R and τ∈T∞\tau\in\mathcal T_\inftyτ∈T∞​ set J(λ,τ)=E[g(Xτ∗)−λ(Xτ)]J(\lambda,\tau)=\mathbb E[g(X^*_\tau)-\lambda(X_\tau)]J(λ,τ)=E[g(Xτ∗​)−λ(Xτ​)] and uλ(X0,X0)=sup⁡τ∈T∞J(λ,τ)u^\lambda(X_0,X_0)=\sup_{\tau\in\mathcal T_\infty}J(\lambda,\tau)uλ(X0​,X0​)=supτ∈T∞​​J(λ,τ). The admissible multipliers are

Λ0μ={λ∈L1(μ): sup⁡τ∈T∞E[λ(Xτ)−]<∞},\Lambda^\mu_0=\Big\{\lambda\in\mathbb L^1(\mu):\ \sup_{\tau\in\mathcal T_\infty}\mathbb E[\lambda(X_\tau)^-]<\infty\Big\},Λ0μ​={λ∈L1(μ): τ∈T∞​sup​E[λ(Xτ​)−]<∞},

and the reduced superhedging problem (3.7) is

Uμ(ξ)=inf⁡λ∈Λ0μ{∫λ dμ+uλ(X0,X0)}.U^\mu(\xi)=\inf_{\lambda\in\Lambda^\mu_0}\Big\{\int\lambda\,d\mu+u^\lambda(X_0,X_0)\Big\}.Uμ(ξ)=λ∈Λ0μ​inf​{∫λdμ+uλ(X0​,X0​)}.

The barycenter function is b(x)=∫[x,∞)y μ(dy)/μ([x,∞))b(x)=\int_{[x,\infty)}y\,\mu(dy)/\mu([x,\infty))b(x)=∫[x,∞)​yμ(dy)/μ([x,∞)) for μ((x,∞))>0\mu((x,\infty))>0μ((x,∞))>0 and b(x)=xb(x)=xb(x)=x otherwise. The Hardy–Littlewood transform μHL\mu^{HL}μHL is the probability measure with

μHL([y,∞))=inf⁡ξ<yc(ξ)y−ξ.\mu^{HL}([y,\infty))=\inf_{\xi<y}\frac{c(\xi)}{y-\xi}.μHL([y,∞))=ξ<yinf​y−ξc(ξ)​.

The Azéma–Yor stopping time is τ∗=inf⁡{t>0:Xt∗≥b(Xt)}\tau^*=\inf\{t>0:X^*_t\ge b(X_t)\}τ∗=inf{t>0:Xt∗​≥b(Xt​)}, and the candidate multiplier is

λ∗(x)=∫ℓμx ⁣∫ℓμyg′(b(ξ)) b(dξ)b(ξ)−ξ dy,\lambda^*(x)=\int_{\ell^\mu}^{x}\!\int_{\ell^\mu}^{y}g'(b(\xi))\,\frac{b(d\xi)}{b(\xi)-\xi}\,dy ,λ∗(x)=∫ℓμx​∫ℓμy​g′(b(ξ))b(ξ)−ξb(dξ)​dy,

that is, the convex function vanishing below ℓμ\ell^\muℓμ that solves the weak ODE (3.21) with ψ=b−1\psi=b^{-1}ψ=b−1.

Formalization targets

Goal: Theorem 3.1

If sup⁡τ∈T∞E[g(Xτ∗)]<∞\sup_{\tau\in\mathcal T_\infty}\mathbb E[g(X^*_\tau)]<\inftysupτ∈T∞​​E[g(Xτ∗​)]<∞ and μHL(g)=∫g dμHL<∞\mu^{HL}(g)=\int g\,d\mu^{HL}<\inftyμHL(g)=∫gdμHL<∞, then

Uμ(ξ)=μ(λ∗)+J(λ∗,τ∗)=μHL(g).U^\mu(\xi)=\mu(\lambda^*)+J(\lambda^*,\tau^*)=\mu^{HL}(g).Uμ(ξ)=μ(λ∗)+J(λ∗,τ∗)=μHL(g).

The goal is the paper's theorem for the reduced problem (3.7), in its full two-equality form: the value, its attainment by (λ∗,τ∗)(\lambda^*,\tau^*)(λ∗,τ∗), and its closed form.

Milestones

  1. The Neumann condition (3.23) for Peskir's candidate vψv^\psivψ.
  2. Lemma 3.1: uλ≤vψu^\lambda\le v^\psiuλ≤vψ for convex λ∈Λ0μ\lambda\in\Lambda^\mu_0λ∈Λ0μ​ and every relaxed free boundary ψ∈Ψλ\psi\in\Psi^\lambdaψ∈Ψλ.
  3. Step (1) of Lemma 3.2: μ(λ)−λ(X0)=∫(c−c0) dλ′′\mu(\lambda)-\lambda(X_0)=\int(c-c_0)\,d\lambda''μ(λ)−λ(X0​)=∫(c−c0​)dλ′′, with c0(x)=(X0−x)+c_0(x)=(X_0-x)^+c0​(x)=(X0​−x)+.
  4. Lemma 3.2: μ(λ)+uλ(X0,X0)≤g(X0)+∫φ(ψ(m),m)g′(m) dm\mu(\lambda)+u^\lambda(X_0,X_0)\le g(X_0)+\int\varphi(\psi(m),m)g'(m)\,dmμ(λ)+uλ(X0​,X0​)≤g(X0​)+∫φ(ψ(m),m)g′(m)dm.
  5. The pointwise minimizations (3.27) and (3.28).
  6. Steps (2) and (3) of Lemma 3.3: properties of λ∗\lambda^*λ∗, and the integration by parts giving μHL(g)\mu^{HL}(g)μHL(g).
  7. Lemma 3.3, the upper bound Uμ(ξ)≤μHL(g)U^\mu(\xi)\le\mu^{HL}(g)Uμ(ξ)≤μHL(g).
  8. The Azéma–Yor facts: τ∗∈T∞\tau^*\in\mathcal T_\inftyτ∗∈T∞​, Xτ∗∼μX_{\tau^*}\sim\muXτ∗​∼μ, Xτ∗∗∼μHLX^*_{\tau^*}\sim\mu^{HL}Xτ∗∗​∼μHL.
  9. The lower bound Uμ(ξ)≥μHL(g)U^\mu(\xi)\ge\mu^{HL}(g)Uμ(ξ)≥μHL(g) of Section 3.4.

Significance

The theorem identifies the model-free price of a lookback payoff as an explicit functional of the call prices, μHL(g)\mu^{HL}(g)μHL(g), and exhibits the extremal model (Brownian motion stopped at τ∗\tau^*τ∗) and the optimal static hedge (λ∗\lambda^*λ∗). It shows that the dual stochastic control formulation is sharp on a nontrivial path-dependent payoff, which is the template for later work on martingale optimal transport with path-dependent costs.

The result has been proved since 2014 (and Hobson's bound since 1998). It has not been formalized. A complete development would provide machine-checked versions of the Azéma–Yor embedding, the law of the maximum at the embedding, a verification theorem for a reflected optimal stopping problem with a nonsmooth obstacle, and the convex-analytic identities linking call prices to second-derivative measures. Each of these is reusable well beyond this paper.

Difficulty

The upper bound requires a verification argument for an optimal stopping problem of the pair (X,X∗)(X,X^*)(X,X∗) with a reflection at the diagonal, where the candidate vψv^\psivψ is only as regular as the convex multiplier λ\lambdaλ: second derivatives are measures and the free boundary ψ\psiψ solves its ODE only in a relaxed sense. An Itô formula for C2C^2C2 functions does not apply; an Itô–Tanaka (local time) argument for concave functions of XXX, with the reflection term killed by the Neumann condition, is needed, followed by a localisation that uses uniform integrability and the integrability condition in Λ0μ\Lambda^\mu_0Λ0μ​. The lower bound needs the Azéma–Yor embedding and the law of Xτ∗∗X^*_{\tau^*}Xτ∗∗​, neither of which is in Mathlib; the naive appeal to "the embedding exists" does not give the joint law of the stopped value and the maximum.

Formalization scope

The Lean development lives in the namespace LookbackMOT.HL and uses Mathlib's IsBrownianReal, IsStoppingTime, stoppedProcess, stoppedValue, Martingale, UniformIntegrable and HasLaw. Committed conventions:

  • What is formalized. The goal is the reduced problem (3.7), not the superhedging problem (2.6): (2.6) needs stochastic integrals, which Mathlib does not have. The bridge between them (Proposition 2.1, the claim (3.4), Proposition 3.1) is outside this mission. The theorem's hypothesis sup⁡P∈P∞EP[ξ+]<∞\sup_{\mathbb P\in\mathcal P_\infty}\mathbb E^{\mathbb P}[\xi^+]<\inftysupP∈P∞​​EP[ξ+]<∞ is stated through Proposition 3.1 with λ=0\lambda=0λ=0 as sup⁡τ∈T∞E[g(Xτ∗)]<∞\sup_{\tau\in\mathcal T_\infty}\mathbb E[g(X^*_\tau)]<\inftysupτ∈T∞​​E[g(Xτ∗​)]<∞. The horizon TTT disappears: the stopping problem is over T∞\mathcal T_\inftyT∞​ with time in [0,∞)[0,\infty)[0,∞).
  • Standing hypotheses. The Brownian motion lives on an arbitrary filtered probability space with everywhere-continuous paths and B0=0B_0=0B0​=0; the paper's canonical space is one instance. The mean condition and integrability of μ\muμ (p. 7) are assumed throughout. The spot X0X_0X0​ is any real number. μ([0,∞))=1\mu([0,\infty))=1μ([0,∞))=1 is assumed only in (3.27).
  • Added conditions. Every τ∈T∞\tau\in\mathcal T_\inftyτ∈T∞​ is a.s. finite (implied by uniform integrability). Every λ∈Λ0μ\lambda\in\Lambda^\mu_0λ∈Λ0μ​ is measurable.
  • Expectations of payoffs are E[φ+]−E[φ−]\mathbb E[\varphi^+]-\mathbb E[\varphi^-]E[φ+]−E[φ−] in the extended reals, with ∞−∞=−∞\infty-\infty=-\infty∞−∞=−∞; value functions are extended reals.
  • Derivatives. λ′\lambda'λ′ is the right derivative and λ′′\lambda''λ′′ its Stieltjes measure. The weak ODE (3.21) is used both as a change of variables (λ′′\lambda''λ′′ is the image of g′(m)/(m−ψ(m)) dmg'(m)/(m-\psi(m))\,dmg′(m)/(m−ψ(m))dm under ψ\psiψ) and on intervals (λ′(ψ(y2))−λ′(ψ(y1))=∫y1y2g′(m)/(m−ψ(m)) dm\lambda'(\psi(y_2))-\lambda'(\psi(y_1))=\int_{y_1}^{y_2}g'(m)/(m-\psi(m))\,dmλ′(ψ(y2​))−λ′(ψ(y1​))=∫y1​y2​​g′(m)/(m−ψ(m))dm), the two forms the paper's proofs use.
  • The multiplier λ∗\lambda^*λ∗. It is written as λ∗(x)=∫X0<m<rμg′(m)(x−b−1(m))+/(m−b−1(m)) dm\lambda^*(x)=\int_{X_0<m<r^\mu}g'(m)(x-b^{-1}(m))^+/(m-b^{-1}(m))\,dmλ∗(x)=∫X0​<m<rμ​g′(m)(x−b−1(m))+/(m−b−1(m))dm, the change of variables m=b(ξ)m=b(\xi)m=b(ξ) in (3.14) and the solution of (3.21) with ψ=b−1\psi=b^{-1}ψ=b−1 that the proof of Lemma 3.3 uses. It agrees with the b(dξ)b(d\xi)b(dξ) formula when bbb is continuous; at the jumps of bbb (atoms of μ\muμ) the Lebesgue–Stieltjes reading of (3.14) can fail to be μ\muμ-integrable.
  • Measures given by identities. μHL\mu^{HL}μHL and λ′′\lambda''λ′′ enter as measures satisfying their defining identities on intervals; each exists and is unique.
  • Printed slips not copied. (3.12) prints the numerator c(y)c(y)c(y); the formalization uses c(ξ)c(\xi)c(ξ). bbb, μHL\mu^{HL}μHL and λ∗\lambda^*λ∗ are extended from x≥0x\ge0x≥0 to all of R\mathbb RR by the same formulas.

No trivializing reading is available. Payoff expectations are never Bochner integrals (which would be 000 for non-integrable payoffs). τ≡0\tau\equiv0τ≡0 lies in T∞\mathcal T_\inftyT∞​ and λ≡0\lambda\equiv0λ≡0 in Λ0μ\Lambda^\mu_0Λ0μ​, so neither the supremum nor the infimum is over an empty set. The predicates for μHL\mu^{HL}μHL and λ′′\lambda''λ′′ are satisfiable (witnessed for μ=δX0\mu=\delta_{X_0}μ=δX0​​ in a sorry-free check). XτX_\tauXτ​ is only evaluated where τ<∞\tau<\inftyτ<∞ a.s. Every division has a positive denominator on the sets that carry mass.

Contributions welcome: the Azéma–Yor embedding and the law of the maximum; an Itô–Tanaka or local-time calculus sufficient for concave functions of Brownian motion and its maximum; the call-price identities of convex analysis; and the analysis of μHL\mu^{HL}μHL.

Selected references

  • A. Galichon, P. Henry-Labordère, N. Touzi, A stochastic control approach to no-arbitrage bounds given marginals, with an application to lookback options, Ann. Appl. Probab. 24 (2014) 312–336. https://arxiv.org/abs/1401.3921 (v1, the version cited)
  • D. Hobson, Robust hedging of the lookback option, Finance Stoch. 2 (1998) 329–347. https://doi.org/10.1007/s007800050046
  • J. Azéma, M. Yor, Une solution simple au problème de Skorokhod, Séminaire de Probabilités XIII, LNM 721 (1979) 90–115. https://doi.org/10.1007/BFb0070852
  • G. Peskir, Optimal stopping of the maximum process: the maximality principle, Ann. Probab. 26 (1998) 1614–1640. https://doi.org/10.1214/aop/1022855875
  • L. Carraro, N. El Karoui, J. Obłój, On Azéma–Yor processes, their optimal properties and the Bachelier–drawdown equation, Ann. Probab. 40 (2012) 372–400. https://arxiv.org/abs/0902.1328
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Linear OptimizationMachine LearningStatistics·Captain: mikedeng1

Fast Rates for Contextual Linear Optimization 1: Under the Margin Condition, ERM over a Policy Class of Natarajan Dimension η Has Regret O(B(η log(|Z∠|+1) log(n+1)/n)^((1+α)/(2+α)))Research Paper

Motivation

Many operational decisions are linear programs whose cost vector is uncertain but partly predictable: shortest-path routing with uncertain travel times, portfolio choice with uncertain returns, shipment planning with uncertain costs. Before deciding, one observes features XXX (traffic, market signals) correlated with the costs YYY. Contextual linear optimization asks for a policy mapping features to decisions that minimizes the conditional expected cost, learned from past data (X1,Y1),…,(Xn,Yn)(X_1, Y_1), \dots, (X_n, Y_n)(X1​,Y1​),…,(Xn​,Yn​).

Two families of methods compete. Estimate-then-optimize fits a regression of YYY on XXX and plugs it into the optimizer. Empirical risk minimization (ERM) and its "integrated" variants choose a policy directly to minimize the empirical decision cost. A widespread view holds that the integrated approach should win because it targets the decision cost. Hu, Kallus and Mao (arXiv:2011.03030, Management Science 2022) compare the two through their regret rates. Slow, noise-independent rates of order n−1/2n^{-1/2}n−1/2 do not separate them. The separation appears under a margin (noise) condition controlling how often the problem is nearly dual-degenerate. This mission formalizes the paper's fast rate for ERM, Theorem 6.

Timeline. Margin conditions for classification go back to Mammen–Tsybakov (1999) and Tsybakov (2004); Massart–Nédélec (2006) obtained the corresponding fast rates for ERM over VC classes. El Balghiti, Elmachtoub, Grigas and Tewari (2019) gave slow generalization bounds for decision-focused losses in terms of the Natarajan dimension. Hu, Kallus and Mao (2020, revised 2021) proved the fast rate for ERM over policy classes of finite Natarajan dimension, a matching lower bound, and a faster rate for estimate-then-optimize.

Setting

The decision set is a polytope Z={z∈Rd:Az≤b}\mathcal Z = \{z \in \mathbb R^d : Az \le b\}Z={z∈Rd:Az≤b}, nonempty, with ∥z∥≤B\|z\| \le B∥z∥≤B on Z\mathcal ZZ for some B>0B > 0B>0; Z∠\mathcal Z^\angleZ∠ is its finite set of extreme points. The pair (X,Y)∈Rp×Rd(X, Y) \in \mathbb R^p \times \mathbb R^d(X,Y)∈Rp×Rd has ∥Y∥≤1\|Y\| \le 1∥Y∥≤1, and f∗(x)=E[Y∣X=x]f^*(x) = \mathbb E[Y \mid X = x]f∗(x)=E[Y∣X=x]. The optimal set at xxx is Z∗(x)=arg⁡min⁡z∈Zf∗(x)⊤z\mathcal Z^*(x) = \arg\min_{z \in \mathcal Z} f^*(x)^\top zZ∗(x)=argminz∈Z​f∗(x)⊤z.

A policy is a map π:Rp→Z∠\pi : \mathbb R^p \to \mathcal Z^\angleπ:Rp→Z∠. A data-driven policy π^\hat\piπ^ maps a sample D\mathcal DD of nnn i.i.d. draws to a policy, and its regret is

Regret(π^)=EDEX[f∗(X)⊤π^(X)−min⁡z∈Zf∗(X)⊤z].\mathrm{Regret}(\hat\pi) = \mathbb E_{\mathcal D}\mathbb E_X\bigl[f^*(X)^\top\hat\pi(X) - \min_{z \in \mathcal Z} f^*(X)^\top z\bigr].Regret(π^)=ED​EX​[f∗(X)⊤π^(X)−z∈Zmin​f∗(X)⊤z].

Given a class Π\PiΠ of policies, π^ΠERM\hat\pi^{\mathrm{ERM}}_\Piπ^ΠERM​ returns a member of Π\PiΠ minimizing 1n∑iYi⊤π(Xi)\frac1n\sum_i Y_i^\top\pi(X_i)n1​∑i​Yi⊤​π(Xi​).

The gap Δ(x)\Delta(x)Δ(x) is the difference between the best value over suboptimal extreme points and the optimal value, set to 000 when every point of Z\mathcal ZZ is optimal. Assumption 2 (noise condition) with parameters α,γ≥0\alpha, \gamma \ge 0α,γ≥0 requires

PX(0<Δ(X)≤δ)≤(γδ/B)αfor all δ>0.\mathbb P_X\bigl(0 < \Delta(X) \le \delta\bigr) \le (\gamma\delta/B)^\alpha \qquad \text{for all } \delta > 0.PX​(0<Δ(X)≤δ)≤(γδ/B)αfor all δ>0.

The Natarajan dimension of Π\PiΠ is the largest kkk for which there are points x1,…,xkx_1, \dots, x_kx1​,…,xk​ and labels si≠si′s_i \ne s'_isi​=si′​ such that every pattern of choices between sis_isi​ and si′s'_isi′​ is realized by some π∈Π\pi \in \Piπ∈Π.

Formalization targets

Goal: Theorem 6

If Assumption 2 holds, P(∣Z∗(X)∣>1)=0\mathbb P(|\mathcal Z^*(X)| > 1) = 0P(∣Z∗(X)∣>1)=0, Π\PiΠ has Natarajan dimension at most η\etaη, and Π\PiΠ contains an optimal policy π∗\pi^*π∗, then for a constant C(α,γ)C(\alpha, \gamma)C(α,γ) depending only on α,γ\alpha, \gammaα,γ,

Regret(π^ΠERM)≤C(α,γ) B(ηlog⁡(∣Z∠∣+1)log⁡(n+1)n)1+α2+α.\mathrm{Regret}(\hat\pi^{\mathrm{ERM}}_\Pi) \le C(\alpha, \gamma)\,B\left(\frac{\eta\log(|\mathcal Z^\angle| + 1)\log(n + 1)}{n}\right)^{\frac{1+\alpha}{2+\alpha}}.Regret(π^ΠERM​)≤C(α,γ)B(nηlog(∣Z∠∣+1)log(n+1)​)2+α1+α​.

The constant is existential and uniform over all dimensions, polytopes, distributions, classes, η\etaη and nnn; the goal fixes no numerical value.

Milestones

With d(π,π′)=1BEX[f∗(X)⊤(π′(X)−π(X))]d(\pi, \pi') = \frac1B\mathbb E_X[f^*(X)^\top(\pi'(X) - \pi(X))]d(π,π′)=B1​EX​[f∗(X)⊤(π′(X)−π(X))] and dΔ(π,π′)=PX(π(X)≠π′(X))d_\Delta(\pi, \pi') = \mathbb P_X(\pi(X) \ne \pi'(X))dΔ​(π,π′)=PX​(π(X)=π′(X)):

  1. Lemma 1: d(π∗,π)≤2dΔ(π∗,π)d(\pi^*, \pi) \le 2d_\Delta(\pi^*, \pi)d(π∗,π)≤2dΔ​(π∗,π) and dΔ(π∗,π)≤c1d(π∗,π)α/(α+1)d_\Delta(\pi^*, \pi) \le c_1 d(\pi^*, \pi)^{\alpha/(\alpha+1)}dΔ​(π∗,π)≤c1​d(π∗,π)α/(α+1) with c1=(αγα)−α/(α+1)(α+1)γαc_1 = (\alpha\gamma^\alpha)^{-\alpha/(\alpha+1)}(\alpha+1)\gamma^\alphac1​=(αγα)−α/(α+1)(α+1)γα.
  2. Lemma 2 (Bousquet's inequality): for a countable class bounded by Hˉ\bar HHˉ with second moments at most δ2\delta^2δ2, S−ESS - \mathbb E SS−ES exceeds 2(δ2+4HˉES)t/n+2Hˉt/(3n)\sqrt{2(\delta^2 + 4\bar H\mathbb E S)t/n} + 2\bar Ht/(3n)2(δ2+4HˉES)t/n​+2Hˉt/(3n) with probability at most e−te^{-t}e−t.
  3. Lemma 3: the localized excess-loss process satisfies ED[sup⁡h∈Hδ(Enh−EPh)]≤(1+2)C05ηlog⁡(∣Z∠∣2+1)log⁡(n+1)/n δ\mathbb E_{\mathcal D}[\sup_{h \in \mathcal H_\delta}(\mathbb E_n h - \mathbb E_P h)] \le (1+\sqrt2)C_0\sqrt{5\eta\log(|\mathcal Z^\angle|^2+1)\log(n+1)/n}\,\deltaED​[suph∈Hδ​​(En​h−EP​h)]≤(1+2​)C0​5ηlog(∣Z∠∣2+1)log(n+1)/n​δ for nnn above a threshold.
  4. Tail bound (proof of Theorem 6, p. 27): for t≥1t \ge 1t≥1, P(d(π∗,π^ΠERM)≥Kt(Vˉlog⁡(n+1)/n)(1+α)/(2+α))≤e−t\mathbb P(d(\pi^*, \hat\pi^{\mathrm{ERM}}_\Pi) \ge K t(\bar V\log(n+1)/n)^{(1+\alpha)/(2+\alpha)}) \le e^{-t}P(d(π∗,π^ΠERM​)≥Kt(Vˉlog(n+1)/n)(1+α)/(2+α))≤e−t with Vˉ=5ηlog⁡(∣Z∠∣2+1)\bar V = 5\eta\log(|\mathcal Z^\angle|^2+1)Vˉ=5ηlog(∣Z∠∣2+1) and n≥cVˉlog⁡(n+1)n \ge c\bar V\log(n+1)n≥cVˉlog(n+1).

Significance

Theorem 6 shows that the regret of ERM improves from n−1/2n^{-1/2}n−1/2 to n−(1+α)/(2+α)n^{-(1+\alpha)/(2+\alpha)}n−(1+α)/(2+α) when the instance is rarely near dual degeneracy. With α=1\alpha = 1α=1, the generic case when XXX has a bounded density and f∗f^*f∗ is linear, the rate is n−2/3n^{-2/3}n−2/3. Theorem 7 of the same paper (mission 2 of this series) shows that the exponent is optimal for any method that uses only the policy class. Theorem 8 (mission 3) shows that estimate-then-optimize can reach n−(1+α)/2n^{-(1+\alpha)/2}n−(1+α)/2, which is the paper's case against the conventional preference for integrated methods.

The result is proved in the paper; no machine-checked proof is known. Formalizing it adds a checked fast-rate theorem for a decision-focused learning method, a Lean statement of Bousquet's inequality in the form used throughout statistical learning theory, and a localized empirical-process bound for classes of finite Natarajan dimension.

Difficulty

The slow rate follows from uniform convergence of the empirical cost over Π\PiΠ. This argument cannot give more than n−1/2n^{-1/2}n−1/2: it bounds the deviation of every policy by the same worst-case amount, ignoring that near-optimal policies have small variance. The fast rate needs a variance–mean relation (Lemma 1, which is where the noise condition and the uniqueness assumption P(∣Z∗(X)∣>1)=0\mathbb P(|\mathcal Z^*(X)| > 1) = 0P(∣Z∗(X)∣>1)=0 enter), a concentration inequality that exploits small variance (Lemma 2), and a localized complexity bound (Lemma 3), combined over shells of the class. Lemma 2 is itself a deep result whose known proofs go through the entropy method. Lemma 3 rests on chaining and on bounding the pseudo-dimension of the excess-loss class by the Natarajan dimension, neither of which is in Mathlib.

Formalization scope

All declarations live in the namespace FastCLO.ERM. Conventions:

  • Spaces are EuclideanSpace ℝ (Fin k). The polytope is a structure carrying AAA, bbb, B>0B > 0B>0, nonemptiness and the bound ∥z∥≤B\|z\| \le B∥z∥≤B; ∣Z∠∣|\mathcal Z^\angle|∣Z∠∣ is the cardinality of Set.extremePoints, whose finiteness is a proof obligation, not a hypothesis.
  • The distribution is given by the law μ\muμ of XXX and a Markov kernel κ\kappaκ for YYY given XXX, with ∥Y∥≤1\|Y\| \le 1∥Y∥≤1 κ(x)\kappa(x)κ(x)-almost surely for every xxx; f∗f^*f∗ is the kernel mean; data are Measure.pi of μ⊗κ\mu \otimes \kappaμ⊗κ.
  • Regret is measured against the optimal value; this equals the paper's f∗(X)⊤(π^(X)−π∗(X))f^*(X)^\top(\hat\pi(X) - \pi^*(X))f∗(X)⊤(π^(X)−π∗(X)).
  • ERM is any selection from the empirical argmin over the whole class; the paper's tie-breaking order is not encoded. The ERM rule is assumed jointly measurable in the data and the feature (an added hypothesis, so that the regret is a genuine integral).
  • "π∗∈Π\pi^* \in \Piπ∗∈Π" means some member of Π\PiΠ is optimal at almost every xxx; "Natarajan dimension at most η\etaη" means Π\PiΠ does not shatter η+1\eta + 1η+1 points.
  • Added hypotheses: n≥1n \ge 1n≥1 wherever the paper divides by nnn; Hˉ>0\bar H > 0Hˉ>0 in Lemma 2; measurability of the supremum in Lemma 3; η≥1\eta \ge 1η≥1 in the tail bound (the paper's ϵn>0\epsilon_n > 0ϵn​>0). Constants (CCC, C0C_0C0​, KKK, ccc) are quantified before everything they are uniform over.

A statement in which the regret integrated the empirical cost instead of f∗f^*f∗, or in which ERM minimized over a subset of the class, or in which the constant could depend on the instance, would be a different theorem; the Lean statements rule these out by construction.

Needed infrastructure: Bousquet's (or Talagrand's) inequality, symmetrization and Dudley chaining for empirical processes, packing bounds for classes of finite pseudo-dimension, and the Natarajan-to-pseudo-dimension reduction. These are reusable far beyond this mission; contributions of any of them are welcome.

Selected references

  • Y. Hu, N. Kallus, X. Mao, Fast Rates for Contextual Linear Optimization, Management Science, 2022; arXiv:2011.03030v3, 2021. https://arxiv.org/abs/2011.03030
  • O. Bousquet, A Bennett concentration inequality and its application to suprema of empirical processes, Comptes Rendus Mathématique 334(6), 2002. https://doi.org/10.1016/S1631-073X(02)02292-6
  • P. Massart, É. Nédélec, Risk bounds for statistical learning, Annals of Statistics 34(5), 2006. https://doi.org/10.1214/009053606000000786
  • A. B. Tsybakov, Optimal aggregation of classifiers in statistical learning, Annals of Statistics 32(1), 2004. https://doi.org/10.1214/aos/1079120131
  • O. El Balghiti, A. N. Elmachtoub, P. Grigas, A. Tewari, Generalization Bounds in the Predict-then-Optimize Framework, NeurIPS 2019; arXiv:1905.11488. https://arxiv.org/abs/1905.11488
  • B. K. Natarajan, On learning sets and functions, Machine Learning 4, 1989. https://doi.org/10.1007/BF00114804
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CombinatoricsGraph TheoryMathematical Physics·Captain: mikedeng1

Algorithms for #BIS-Hard Problems on Expander Graphs 1: On α-Expanders of Maximum Degree Δ, the Low-Temperature Potts Partition Function Reduces to a Kotecký–Preiss Polymer ModelResearch Paper

Motivation

The ferromagnetic Potts model assigns a larger weight to a coloring when more adjacent vertices have the same color. Computing its partition function is an approximate counting problem with connections to statistical physics and counting complexity. For three or more colors, Goldberg and Jerrum established #BIS-hardness of approximation on general graphs, and Galanis, Štefankovič, Vigoda, and Yang refined the hardness result for bounded-degree bipartite graphs Goldberg–Jerrum, Galanis et al.. These results make it useful to identify graph classes where the partition sum can still be approximated efficiently.

Jenssen, Keevash, and Perkins proved that edge expansion supplies such a class at sufficiently large inverse temperature. Their Theorem 3 gives an FPTAS and a polynomial-time sampling algorithm for the qqq-color ferromagnetic Potts model on finite α\alphaα-expanders of maximum degree Δ\DeltaΔ, when α>0\alpha>0α>0, Δ≥3\Delta\ge3Δ≥3, q≥2q\ge2q≥2, and β≥(4+2log⁡(qΔ))/α\beta\ge(4+2\log(q\Delta))/\alphaβ≥(4+2log(qΔ))/α Jenssen–Keevash–Perkins. This mission records the mathematical reduction and the polymer convergence condition on which their algorithmic conclusion rests.

Setting

Let G=(V,E)G=(V,E)G=(V,E) be a finite simple graph, let n=∣V∣n=|V|n=∣V∣, and let e(G)=∣E∣e(G)=|E|e(G)=∣E∣. A coloring ω:V→[q]\omega:V\to[q]ω:V→[q] gives each vertex one of qqq colors. Write m(G,ω)m(G,\omega)m(G,ω) for the number of edges whose endpoints receive the same color. The Potts partition function at inverse temperature β\betaβ is

ZG,q(β)=∑ω:V→[q]exp⁡(βm(G,ω)).Z_{G,q}(\beta)=\sum_{\omega:V\to[q]}\exp\bigl(\beta m(G,\omega)\bigr).ZG,q​(β)=ω:V→[q]∑​exp(βm(G,ω)).

For S⊆VS\subseteq VS⊆V, its edge boundary ∂eS\partial_e S∂e​S consists of the edges with exactly one endpoint in SSS. The graph is an α\alphaα-expander if ∣∂eS∣≥α∣S∣|\partial_e S|\ge\alpha|S|∣∂e​S∣≥α∣S∣ whenever 2∣S∣≤n2|S|\le n2∣S∣≤n. The maximum-degree assumption means that each vertex has at most Δ\DeltaΔ neighbors. All logarithms here are natural logarithms.

A color jjj is a strict majority in ω\omegaω when 2∣ω−1(j)∣>n2|\omega^{-1}(j)|>n2∣ω−1(j)∣>n. Let ZGj(β)Z_G^j(\beta)ZGj​(β) be the Potts sum over colorings with that majority, and let ZG∗(β)=∑j∈[q]ZGj(β)Z_G^*(\beta)=\sum_{j\in[q]}Z_G^j(\beta)ZG∗​(β)=∑j∈[q]​ZGj​(β). Because two colors cannot each occupy more than half the vertices, these sectors do not overlap. The monochromatic colorings are the model's ground states at positive β\betaβ.

A polymer γ\gammaγ is a nonempty vertex set for which the induced graph G[γ]G[\gamma]G[γ] is connected and 2∣γ∣≤n2|\gamma|\le n2∣γ∣≤n. Let ∇(γ)\nabla(\gamma)∇(γ) be all edges with at least one endpoint in γ\gammaγ. Two polymers are compatible when the distance between every vertex of one and every vertex of the other exceeds one. In particular, overlapping or adjacent polymers are incompatible. With ZG[γ],q−1(β)Z_{G[\gamma],q-1}(\beta)ZG[γ],q−1​(β) the Potts sum on the induced graph using the other q−1q-1q−1 colors, define

wγ=exp⁡(−β∣∇(γ)∣)ZG[γ],q−1(β),Ξ(G)=∑Γ pairwise compatible∏γ∈Γwγ.w_\gamma=\exp\bigl(-\beta|\nabla(\gamma)|\bigr)Z_{G[\gamma],q-1}(\beta),\qquad \Xi(G)=\sum_{\Gamma\text{ pairwise compatible}}\prod_{\gamma\in\Gamma}w_\gamma.wγ​=exp(−β∣∇(γ)∣)ZG[γ],q−1​(β),Ξ(G)=Γ pairwise compatible∑​γ∈Γ∏​wγ​.

The sum includes the empty family. An ε\varepsilonε-relative approximation Z^\widehat ZZ to ZZZ means e−εZ^≤Z≤eεZ^e^{-\varepsilon}\widehat Z\le Z\le e^\varepsilon\widehat Ze−εZ≤Z≤eεZ Jenssen–Keevash–Perkins, Definitions 10–11.

Formalization targets

The goal is the deterministic core of Theorem 3. For a nonempty α\alphaα-expander with the degree, color, and temperature bounds above, the explicit polymer expression approximates the Potts partition sum:

Z^=qexp⁡(βe(G))Ξ(G),e−2e−nZ^≤ZG,q(β)≤e2e−nZ^.\widehat Z=q\exp\bigl(\beta e(G)\bigr)\Xi(G),\qquad e^{-2e^{-n}}\widehat Z\le Z_{G,q}(\beta)\le e^{2e^{-n}}\widehat Z.Z=qexp(βe(G))Ξ(G),e−2e−nZ≤ZG,q​(β)≤e2e−nZ.

The error 2e−n2e^{-n}2e−n is the composition of the two e−ne^{-n}e−n-relative approximations in Lemmas 12 and 13; the paper does not print it as a separate constant. The same goal also asserts the Kotecký–Preiss condition, with the paper's decay function g(γ)=∣γ∣g(\gamma)=|\gamma|g(γ)=∣γ∣, for every polymer γ\gammaγ:

∑γ′: d(γ′,γ)≤1wγ′e2∣γ′∣≤∣γ∣.\sum_{\gamma':\,d(\gamma',\gamma)\le1}w_{\gamma'}e^{2|\gamma'|}\le|\gamma|.γ′:d(γ′,γ)≤1∑​wγ′​e2∣γ′∣≤∣γ∣.

The milestone list follows the source's stated claims: Lemma 12 bounds the contribution outside the strict-majority sectors; Lemma 13 compares one sector with eβe(G)Ξ(G)e^{\beta e(G)}\Xi(G)eβe(G)Ξ(G); the weight bound controls individual polymers; Lemma 14 counts connected induced subgraphs containing a specified vertex; and displayed inequality (5) bounds the resulting per-vertex sum Jenssen–Keevash–Perkins, pp. 13–16.

Significance

The reduction makes a Potts partition sum on an expanding graph accessible through a finite polymer model whose weights have controlled decay. The Kotecký–Preiss condition is a quantitative convergence criterion for abstract polymer expansions Kotecký–Preiss. In this setting the two statements provide the mathematical hypotheses used with the algorithmic framework cited by the paper Helmuth–Perkins–Regts. Without the approximation, computing the polymer sum would not give a controlled Potts estimate; without the convergence condition, the cited framework would not apply at the stated temperature threshold.

The paper proves the mathematical and algorithmic results. This mission supplies Lean definitions and compile-checked statements, with proofs still to be formalized. A completed development would give reusable formal accounts of finite Potts sums, strict-majority sectors, graph edge expansion, polymer compatibility and weights, and the connected-set counting bound that the paper cites from Galvin and Kahn Galvin–Kahn.

Difficulty

The tempting approximation is to count only monochromatic colorings. That discards all nearby colorings, whose total weight matters even at low temperature. The polymer model retains connected deviations from a monochromatic coloring, but it also admits collections whose union is larger than half the graph. Controlling the weight of these extra configurations is part of the approximation statement. Separately, the convergence criterion sums over every polymer within distance one of a given polymer. A bound on one weight does not control that sum unless the number of connected vertex sets of each size is also bounded. These are the distinct estimates captured by Lemmas 12–14 and inequality (5) Jenssen–Keevash–Perkins, §3.

Formalization scope

The Lean representation uses SimpleGraph V on a finite vertex type. Vertex sets are finite sets, the edge boundary counts each crossing edge once through its orientation from inside to outside, and polymer distance is extended graph distance, so disconnected components are infinitely far apart. Strict-majority colorings use 2∣ω−1(j)∣>n2|\omega^{-1}(j)|>n2∣ω−1(j)∣>n; expansion and polymers use the non-strict bound 2∣S∣≤n2|S|\le n2∣S∣≤n. The polymer weight uses the full incident-edge set ∇(γ)\nabla(\gamma)∇(γ) and the induced Potts sum on q−1q-1q−1 colors. The empty compatible family contributes one to Ξ(G)\Xi(G)Ξ(G).

The vertex set is required to be nonempty in the goal and approximation lemmas: for n=0n=0n=0, the strict-majority sum is zero while the Potts partition sum is one. Lemma 14 states Δ≥1\Delta\ge1Δ≥1 because its printed bound is false for an isolated vertex with Δ=0\Delta=0Δ=0. The weight bound states β≥0\beta\ge0β≥0, which is implied by the goal's threshold. These are the only additional domain pins. The stated goal uses the paper's exact Δ≥3\Delta\ge3Δ≥3, q≥2q\ge2q≥2, and β≥(4+2log⁡(qΔ))/α\beta\ge(4+2\log(q\Delta))/\alphaβ≥(4+2log(qΔ))/α; no free approximation value or freely chosen polymer family can trivialize it.

The algorithm and its running time are out of scope because this Mathlib environment has no machine model for the FPTAS and the paper uses unquantified big-O running times. The goal is the mathematical reduction and Kotecký–Preiss hypothesis consumed by Theorem 8. Contributions that establish the five milestone statements, the color-symmetry identity, or the combination of their bounds are useful; the finite graph and partition-sum definitions are reusable beyond this mission.

Selected references

  • M. Jenssen, P. Keevash, and W. Perkins, Algorithms for #BIS-Hard Problems on Expander Graphs, SIAM Journal on Computing 49(4), 2020. DOI.
  • R. Kotecký and D. Preiss, Cluster Expansion for Abstract Polymer Models, Communications in Mathematical Physics 103, 1986. DOI.
  • D. Galvin and J. Kahn, On Phase Transition in the Hard-Core Model on Zd\mathbb Z^dZd, Combinatorics, Probability and Computing 13(2), 2004. DOI.
  • L. A. Goldberg and M. Jerrum, Approximating the Partition Function of the Ferromagnetic Potts Model, Journal of the ACM 59(5), 2012. arXiv.
  • A. Galanis, D. Štefankovič, E. Vigoda, and L. Yang, Ferromagnetic Potts Model: Refined #BIS-Hardness and Related Results, SIAM Journal on Computing 45(6), 2016. DOI.
  • T. Helmuth, W. Perkins, and G. Regts, Algorithmic Pirogov–Sinai Theory, Probability Theory and Related Fields, 2020. DOI.
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Harmonic AnalysisProbability·Captain: mikedeng1

Isotropic Gaussian Random Fields on the Sphere: Regularity, Fast Simulation and Stochastic Partial Differential Equations II: Σ A_ℓ ℓ^{1+β} < ∞ Gives a Continuous Modification, γ-Hölder for γ < β/2Research Paper

Motivation

A random field on a sphere assigns a random value to every direction. Such fields appear when the underlying data are directional, including spherical models in spatial statistics and geophysics. The covariance of an isotropic field can be recorded by an angular power spectrum: one nonnegative number for each spherical harmonic degree. This changes the sample regularity question into a concrete spectral question. How fast must these numbers decay so that a realization is continuous, and how regular can that realization be? Lang and Schwab, 2015 give a sufficient summability condition and an exact range of Hölder exponents in their Theorem 4.5.

The question matters when a field is evaluated on a mesh or represented by finitely many spherical harmonics. A covariance function can be regular even when the original version of a random field has badly chosen values on null sets. The useful result is therefore the existence of one regular modification: at each fixed sphere point it agrees with the given field almost surely, while its sample paths are regular across the entire sphere. The paper treats this sample path result in §4, separately from its spectral characterization of covariance regularity in §3 and its later simulation and stochastic heat equation results.

Setting

Write S2={x∈R3:∥x∥=1}S^2=\{x\in\mathbb R^3:\|x\|=1\}S2={x∈R3:∥x∥=1} for the unit sphere. Its geodesic distance is d(x,y)=arccos⁡⟨x,y⟩d(x,y)=\arccos\langle x,y\rangled(x,y)=arccos⟨x,y⟩, the length of the shorter great circle arc between xxx and yyy. A random field TTT is a jointly measurable map from a probability space times S2S^2S2 to the real numbers. A field is Gaussian when every finite collection of its values has a joint Gaussian distribution. Isotropy says that rotating all observation points together does not change that joint distribution. These are the conventions of Definition 2.1 in the paper.

For each degree ℓ≥0\ell\ge0ℓ≥0, let PℓP_\ellPℓ​ be the Legendre polynomial normalized by Pℓ(1)=1P_\ell(1)=1Pℓ​(1)=1, and let Aℓ≥0A_\ell\ge0Aℓ​≥0 be its angular power. The field has a constant mean and covariance determined by (Aℓ)(A_\ell)(Aℓ​):

Cov⁡(T(x),T(y))=∑ℓ=0∞Aℓ2ℓ+14πPℓ(⟨x,y⟩).\operatorname{Cov}(T(x),T(y)) =\sum_{\ell=0}^{\infty}A_\ell\frac{2\ell+1}{4\pi}P_\ell(\langle x,y\rangle).Cov(T(x),T(y))=ℓ=0∑∞​Aℓ​4π2ℓ+1​Pℓ​(⟨x,y⟩).

Because ⟨x,y⟩=cos⁡d(x,y)\langle x,y\rangle=\cos d(x,y)⟨x,y⟩=cosd(x,y), the same covariance is expressed by the distance kernel k(r)=∑ℓ≥0Aℓ(2ℓ+1)Pℓ(cos⁡r)/(4π)k(r)=\sum_{\ell\ge0}A_\ell(2\ell+1)P_\ell(\cos r)/(4\pi)k(r)=∑ℓ≥0​Aℓ​(2ℓ+1)Pℓ​(cosr)/(4π) for 0≤r≤π0\le r\le\pi0≤r≤π. A modification T′T'T′ of TTT means T′(x)=T(x)T'(x)=T(x)T′(x)=T(x) almost surely for each fixed xxx; it need not agree on one common full measure set at every xxx. The paper's Assumption 4.1, specialized to S2S^2S2, asks for finiteness of ∑ℓ≥0Aℓℓ1+β\sum_{\ell\ge0}A_\ell\ell^{1+\beta}∑ℓ≥0​Aℓ​ℓ1+β.

Formalization targets

Goal: sample regularity

For 0<β≤20<\beta\le20<β≤2, the target is Theorem 4.5 of Lang and Schwab:

∑ℓ=0∞Aℓℓ1+β<∞⟹∃ T′ modifying T with paths Ho¨lder of every order 0<γ<β/2.\sum_{\ell=0}^{\infty}A_\ell\ell^{1+\beta}<\infty \quad\Longrightarrow\quad \exists\,T'\text{ modifying }T\text{ with paths Hölder of every order }0<\gamma<\beta/2.ℓ=0∑∞​Aℓ​ℓ1+β<∞⟹∃T′ modifying T with paths Ho¨lder of every order 0<γ<β/2.

The same modification serves every eligible exponent. The result leaves the Hölder constant free to depend on the sample and the exponent, as it must.

Supporting targets

The four milestones follow the source's statements and its proof order. The Legendre polynomial bounds on p. 16 lead to Lemma 4.2, ∣k(0)−k(r)∣≤Cβrβ|k(0)-k(r)|\le C_\beta r^\beta∣k(0)−k(r)∣≤Cβ​rβ for r∈[0,π]r\in[0,\pi]r∈[0,π] and β∈[0,2]\beta\in[0,2]β∈[0,2]. Lemma 4.3 transfers this to E∣T(x)−T(y)∣2p≤Cβ,pd(x,y)βp\mathbb E|T(x)-T(y)|^{2p}\le C_{\beta,p}d(x,y)^{\beta p}E∣T(x)−T(y)∣2p≤Cβ,p​d(x,y)βp for every positive integer ppp. Theorem 4.4 is a Kolmogorov–Chentsov theorem for any random field on S2S^2S2: a moment exponent 2+εp2+\varepsilon p2+εp produces a continuous modification with every Hölder exponent below ε\varepsilonε. The Gaussian and isotropic hypotheses belong to Lemma 4.3 and the goal; they are absent from Theorem 4.4.

Significance

The theorem provides a checkable bridge from a harmonic description of a field to sample path behavior. A practitioner can estimate or impose decay of the angular power spectrum, then know that a version of the field admits interpolation on the sphere with any exponent below β/2\beta/2β/2. The endpoint β/2\beta/2β/2 is not asserted. The moment estimate and the spherical modification theorem can also be reused when studying fields produced by other models; in particular, Theorem 4.4 needs no Gaussian assumption.

The result was proved in the 2015 paper; this mission concerns its machine checked formalization. Mathlib supplies Gaussian process and measure theory interfaces, but the paper's sphere distance, Legendre normalization, angular kernel and spherical version of Kolmogorov–Chentsov must be connected. A platform goal for a Kolmogorov–Chentsov theorem on [0,∞)[0,\infty)[0,∞) uses a different index space and hypotheses, so it does not cover the present milestone. The finished development will provide a reusable sphere indexed modification theorem as well as the paper's specific spectral criterion.

Difficulty

A bound on the covariance kernel controls the second moment of field increments, but it does not by itself supply one continuous version with a common pathwise regularity statement. The desired exponent concerns values at uncountably many points, whereas the definition of modification gives an almost sure equality separately at each point. The gap is visible even for simple processes: changing a field at one random location can preserve each fixed point's law while destroying continuity of individual paths. The sphere also carries a two dimensional geodesic metric, so a one dimensional modification theorem indexed by time cannot be substituted without a new argument.

Formalization scope

Lean represents S2S^2S2 as the unit metric sphere in three dimensional Euclidean space. Coordinates have indices 0,1,20,1,20,1,2 for the paper's 1,2,31,2,31,2,3. All regularity statements use d(x,y)=arccos⁡⟨x,y⟩d(x,y)=\arccos\langle x,y\rangled(x,y)=arccos⟨x,y⟩, not the subtype's chord distance. Rodrigues' formula defines PℓP_\ellPℓ​, and the kernel is a real infinite sum with its factor (2ℓ+1)/(4π)(2\ell+1)/(4\pi)(2ℓ+1)/(4π). The spectrum is nonnegative and has ∑(2ℓ+1)Aℓ<∞\sum(2\ell+1)A_\ell<\infty∑(2ℓ+1)Aℓ​<∞ as part of the field model, matching the finite variance convention used in §2. The covariance formulation allows a nonzero constant mean: Theorem 4.5 does not require centering.

The moment inequalities use extended nonnegative integrals, avoiding a default zero for nonintegrable real integrals. The paper's positive integers are expressed with an explicit 1≤p1\le p1≤p because Lean's naturals include zero. Real powers follow the usual convention: the degree zero term of ℓ1+β\ell^{1+\beta}ℓ1+β is zero when β≥0\beta\ge0β≥0. On compact S2S^2S2, local Hölder continuity gives a global constant for each path and exponent. Exceptional sample paths may be redefined, so the formal conclusion states continuity and Hölder regularity for every sample of the chosen modification. The modification retains pointwise almost sure agreement and measurable evaluations; omitting agreement would make the goal trivial.

Contributions can address Legendre inequalities, covariance and Gaussian moment calculations, and a general Kolmogorov–Chentsov theorem for compact manifolds. The latter is reusable beyond this paper. The auxiliary Legendre and kernel definitions are also available to later spherical field missions.

Selected references

  • A. Lang and Ch. Schwab, Isotropic Gaussian random fields on the sphere: regularity, fast simulation and stochastic partial differential equations, Annals of Applied Probability 25(6), 2015, arXiv:1305.1170v3, DOI:10.1214/14-AAP1067.
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Numerical AnalysisPartial Differential EquationsProbability·Captain: mikedeng1

Isotropic Gaussian Random Fields on the Sphere: Regularity, Fast Simulation and Stochastic Partial Differential Equations IV: Heat-Equation Spectral Truncation Error ≤ κ^{−β} a.s. for β < α/2Research Paper

Motivation

Stochastic partial differential equations on the sphere model quantities that live on the surface of the Earth or of the sky and are perturbed by spatially correlated noise: temperature anomalies, geophysical fields, fluctuations of the cosmic microwave background. The simplest such model is the stochastic heat equation on the unit sphere S2\mathbb S^2S2 with additive isotropic noise. Because the noise is isotropic and the Laplace–Beltrami operator is diagonal in the spherical harmonics, the equation decouples into one scalar Ornstein–Uhlenbeck equation per harmonic, and the solution can be simulated exactly in law by truncating its spherical-harmonic expansion at a degree κ\kappaκ. The practical question is how fast this spectral truncation converges, in mean square and along a single simulated path.

A. Lang and Ch. Schwab answer this in §7 of Isotropic Gaussian random fields on the sphere: regularity, fast simulation and stochastic partial differential equations (arXiv:1305.1170v3, Ann. Appl. Probab. 25(6), 2015). Their rates are expressed through the decay of the angular power spectrum of the noise, the same quantity that governs the sample regularity and the Karhunen–Loève truncation of isotropic Gaussian random fields in the earlier sections of the paper.

Setting

Let S2⊂R3\mathbb S^2\subset\mathbb R^3S2⊂R3 be the unit sphere with surface measure σ\sigmaσ (total mass 4π4\pi4π) and L2(S2)L^2(\mathbb S^2)L2(S2) the real square-integrable functions with norm ∥f∥L2(S2)2=∫∣f∣2dσ\|f\|^2_{L^2(\mathbb S^2)}=\int|f|^2d\sigma∥f∥L2(S2)2​=∫∣f∣2dσ. The spherical harmonics YℓmY_{\ell m}Yℓm​, ℓ≥0\ell\ge0ℓ≥0, ∣m∣≤ℓ|m|\le\ell∣m∣≤ℓ, are built from the Legendre polynomials Pℓ(μ)=2−ℓ(ℓ!)−1dℓdμℓ(μ2−1)ℓP_\ell(\mu)=2^{-\ell}(\ell!)^{-1}\frac{d^\ell}{d\mu^\ell}(\mu^2-1)^\ellPℓ​(μ)=2−ℓ(ℓ!)−1dμℓdℓ​(μ2−1)ℓ; the functions Yℓ0Y_{\ell0}Yℓ0​, 2Re⁡Yℓm\sqrt2\operatorname{Re}Y_{\ell m}2​ReYℓm​, 2Im⁡Yℓm\sqrt2\operatorname{Im}Y_{\ell m}2​ImYℓm​ (1≤m≤ℓ1\le m\le\ell1≤m≤ℓ) form a real orthonormal basis of the degree-ℓ\ellℓ harmonics, on which the Laplace–Beltrami operator acts as multiplication by −λℓ-\lambda_\ell−λℓ​, λℓ=ℓ(ℓ+1)\lambda_\ell=\ell(\ell+1)λℓ​=ℓ(ℓ+1).

On a probability space (Ω,A,P)(\Omega,\mathcal A,\mathbb P)(Ω,A,P) let βℓmi\beta^i_{\ell m}βℓmi​ (ℓ≥0\ell\ge0ℓ≥0, 0≤m≤ℓ0\le m\le\ell0≤m≤ℓ, i=1,2i=1,2i=1,2) be independent real Brownian motions, and let (Aℓ)ℓ≥0(A_\ell)_{\ell\ge0}(Aℓ​)ℓ≥0​, Aℓ≥0A_\ell\ge0Aℓ​≥0, be an angular power spectrum. The isotropic QQQ-Wiener process is

W(t)=∑ℓ≥0Aℓ(βℓ01(t)Yℓ0+2∑m=1ℓ(βℓm1(t)Re⁡Yℓm+βℓm2(t)Im⁡Yℓm)).W(t)=\sum_{\ell\ge0}\sqrt{A_\ell}\Big(\beta^1_{\ell0}(t)Y_{\ell0}+\sqrt2\sum_{m=1}^{\ell}\big(\beta^1_{\ell m}(t)\operatorname{Re}Y_{\ell m}+\beta^2_{\ell m}(t)\operatorname{Im}Y_{\ell m}\big)\Big).W(t)=ℓ≥0∑​Aℓ​​(βℓ01​(t)Yℓ0​+2​m=1∑ℓ​(βℓm1​(t)ReYℓm​+βℓm2​(t)ImYℓm​)).

The stochastic heat equation is

dX(t)=ΔS2X(t) dt+dW(t),X(0)=X0∈L2(Ω;L2(S2)).dX(t)=\Delta_{\mathbb S^2}X(t)\,dt+dW(t),\qquad X(0)=X_0\in L^2(\Omega;L^2(\mathbb S^2)).dX(t)=ΔS2​X(t)dt+dW(t),X(0)=X0​∈L2(Ω;L2(S2)).

Its solution is X(t)=∑ℓ≥0Xℓ(t)X(t)=\sum_{\ell\ge0}X_\ell(t)X(t)=∑ℓ≥0​Xℓ​(t) with

Xℓ(t)=e−λℓt∑m=−ℓℓ(X0,Yℓm)Yℓm+Aℓ(∫0te−λℓ(t−s)dβℓ01(s) Yℓ0+2∑m=1ℓ(∫0te−λℓ(t−s)dβℓm1(s)Re⁡Yℓm+∫0te−λℓ(t−s)dβℓm2(s)Im⁡Yℓm)),X_\ell(t)=e^{-\lambda_\ell t}\sum_{m=-\ell}^{\ell}(X_0,Y_{\ell m})Y_{\ell m}+\sqrt{A_\ell}\Big(\int_0^te^{-\lambda_\ell(t-s)}d\beta^1_{\ell0}(s)\,Y_{\ell0}+\sqrt2\sum_{m=1}^{\ell}\Big(\int_0^te^{-\lambda_\ell(t-s)}d\beta^1_{\ell m}(s)\operatorname{Re}Y_{\ell m}+\int_0^te^{-\lambda_\ell(t-s)}d\beta^2_{\ell m}(s)\operatorname{Im}Y_{\ell m}\Big)\Big),Xℓ​(t)=e−λℓ​tm=−ℓ∑ℓ​(X0​,Yℓm​)Yℓm​+Aℓ​​(∫0t​e−λℓ​(t−s)dβℓ01​(s)Yℓ0​+2​m=1∑ℓ​(∫0t​e−λℓ​(t−s)dβℓm1​(s)ReYℓm​+∫0t​e−λℓ​(t−s)dβℓm2​(s)ImYℓm​)),

and the spectral approximation is Xκ(t)=∑ℓ=0κXℓ(t)X^\kappa(t)=\sum_{\ell=0}^{\kappa}X_\ell(t)Xκ(t)=∑ℓ=0κ​Xℓ​(t). The norm ∥Z∥Lp(Ω;L2(S2))=(E∥Z∥L2(S2)p)1/p\|Z\|_{L^p(\Omega;L^2(\mathbb S^2))}=(\mathbb E\|Z\|^p_{L^2(\mathbb S^2)})^{1/p}∥Z∥Lp(Ω;L2(S2))​=(E∥Z∥L2(S2)p​)1/p measures random fields. The standing assumption of §7 is the decay condition

Aℓ≤C ℓ−αfor all ℓ>ℓ0,ℓ0∈{1,2,… }, α>0.A_\ell\le C\,\ell^{-\alpha}\quad\text{for all }\ell>\ell_0,\qquad \ell_0\in\{1,2,\dots\},\ \alpha>0 .Aℓ​≤Cℓ−αfor all ℓ>ℓ0​,ℓ0​∈{1,2,…}, α>0.

Formalization targets

Goal: Corollary 7.3 (p. 43)

For every t>0t>0t>0 and every β<α/2\beta<\alpha/2β<α/2, almost surely

∥X(t)−Xκ(t)∥L2(S2)≤κ−βfor all sufficiently large κ.\|X(t)-X^\kappa(t)\|_{L^2(\mathbb S^2)}\le\kappa^{-\beta}\quad\text{for all sufficiently large }\kappa .∥X(t)−Xκ(t)∥L2(S2)​≤κ−βfor all sufficiently large κ.

The goal fixes no constant; only the exponent α/2\alpha/2α/2 enters, so it survives any improvement of the constants below.

Milestones

  1. Display (3), p. 36. For ℓ≥1\ell\ge1ℓ≥1, ∫0te−ℓ(ℓ+1)(t−s)dβ(s)∼N(0,(2ℓ(ℓ+1))−1(1−e−2ℓ(ℓ+1)t))\int_0^te^{-\ell(\ell+1)(t-s)}d\beta(s)\sim\mathcal N\big(0,(2\ell(\ell+1))^{-1}(1-e^{-2\ell(\ell+1)t})\big)∫0t​e−ℓ(ℓ+1)(t−s)dβ(s)∼N(0,(2ℓ(ℓ+1))−1(1−e−2ℓ(ℓ+1)t)).
  2. Lemma 7.1, pp. 39–40, as proved. If the coefficients of X0X_0X0​ are independent of the noise, then for t>0t>0t>0 and κ≥ℓ0\kappa\ge\ell_0κ≥ℓ0​
∥X(t)−Xκ(t)∥L2(Ω;L2(S2))2≤C(2α+1α+1)κ−α+e−2(κ+1)(κ+2)t∥X0∥L2(Ω;L2(S2))2.\|X(t)-X^\kappa(t)\|^2_{L^2(\Omega;L^2(\mathbb S^2))}\le C\Big(\frac2\alpha+\frac1{\alpha+1}\Big)\kappa^{-\alpha}+e^{-2(\kappa+1)(\kappa+2)t}\|X_0\|^2_{L^2(\Omega;L^2(\mathbb S^2))}.∥X(t)−Xκ(t)∥L2(Ω;L2(S2))2​≤C(α2​+α+11​)κ−α+e−2(κ+1)(κ+2)t∥X0​∥L2(Ω;L2(S2))2​.
  1. Lemma 7.2, pp. 41–43, as proved. For each p>0p>0p>0 there is C^p=C^p(p,C,α)\hat C_p=\hat C_p(p,C,\alpha)C^p​=C^p​(p,C,α) with, for t>0t>0t>0 and κ≥ℓ0\kappa\ge\ell_0κ≥ℓ0​,
∥X(t)−Xκ(t)∥Lp(Ω;L2(S2))≤C^pκ−α/2+e−(κ+1)(κ+2)t∥X0∥Lmax⁡(p,2)(Ω;L2(S2)).\|X(t)-X^\kappa(t)\|_{L^p(\Omega;L^2(\mathbb S^2))}\le\hat C_p\kappa^{-\alpha/2}+e^{-(\kappa+1)(\kappa+2)t}\|X_0\|_{L^{\max(p,2)}(\Omega;L^2(\mathbb S^2))}.∥X(t)−Xκ(t)∥Lp(Ω;L2(S2))​≤C^p​κ−α/2+e−(κ+1)(κ+2)t∥X0​∥Lmax(p,2)(Ω;L2(S2))​.

Significance

Corollary 7.3 is the pathwise convergence rate of the spectral method for the stochastic heat equation on the sphere: a single simulated path of the truncated series is within κ−β\kappa^{-\beta}κ−β of the true path in L2(S2)L^2(\mathbb S^2)L2(S2) for all large κ\kappaκ, for any β<α/2\beta<\alpha/2β<α/2. Combined with the exact-in-law recursion on a time grid (pp. 36–38), it says that the only source of error in simulating this SPDE is the spectral truncation, and that the rate is governed by the decay exponent of the noise spectrum alone, with α>0\alpha>0α>0 sufficing (no trace-class condition α>2\alpha>2α>2 is needed, thanks to the smoothing of the heat semigroup). The mean-square and LpL^pLp estimates of Lemmas 7.1 and 7.2 are the quantitative inputs; the LpL^pLp bound for all ppp is what makes a Borel–Cantelli argument possible.

The results are proved in the paper; none of them, nor the stochastic heat equation on the sphere, nor spherical harmonics, has a machine-checked formalization on the platform or in Mathlib. The work here is to formalize the known proof. Two printed statements need correction (see Formalization scope); the milestones state the bounds that the paper's proofs establish.

Difficulty

The obvious argument writes X(t)−Xκ(t)X(t)-X^\kappa(t)X(t)−Xκ(t) as the tail of the series, splits it into the damped initial condition and the noise, and bounds each. The noise part is a Gaussian random field whose angular power spectrum Aℓ(1−e−2λℓt)/(2λℓ)A_\ell(1-e^{-2\lambda_\ell t})/(2\lambda_\ell)Aℓ​(1−e−2λℓ​t)/(2λℓ​) decays like ℓ−(α+2)\ell^{-(\alpha+2)}ℓ−(α+2), so its truncation error is controlled by the corresponding estimates for isotropic Gaussian random fields (Proposition 5.2 and Theorem 5.3 of the paper), which must be re-derived here. Several steps have no current library support: the Wiener integral of a deterministic integrand and its Gaussian law, orthonormality and completeness of the spherical harmonics in L2(S2,σ)L^2(\mathbb S^2,\sigma)L2(S2,σ), moment equivalence for Gaussian vectors in a Hilbert space (to pass from p=2p=2p=2 to all ppp), and the passage between the pointwise series and its L2L^2L2 limit. The initial-condition tail decays like e−(κ+1)(κ+2)te^{-(\kappa+1)(\kappa+2)t}e−(κ+1)(κ+2)t but not uniformly as t↓0t\downarrow0t↓0, which is exactly why the printed "uniformly in time" bounds fail and why every statement takes t>0t>0t>0 fixed.

Formalization scope

  • S2\mathbb S^2S2 is Metric.sphere (0 : EuclideanSpace ℝ (Fin 3)) 1 with coordinates indexed 0,1,20,1,20,1,2 (the paper's y1,y2,y3y_1,y_2,y_3y1​,y2​,y3​); σ\sigmaσ is the measure toSphere of Lebesgue measure, of mass 4π4\pi4π. Spherical harmonics are written in Cartesian form, Pℓm(cos⁡ϑ)eimφ=(−1)mPℓ(m)(y3)(y1+iy2)mP_{\ell m}(\cos\vartheta)e^{im\varphi}=(-1)^mP_\ell^{(m)}(y_3)(y_1+iy_2)^mPℓm​(cosϑ)eimφ=(−1)mPℓ(m)​(y3​)(y1​+iy2​)m, which is the paper's function also at the poles. For real X0X_0X0​ the projection ∑m(X0,Yℓm)Yℓm\sum_m(X_0,Y_{\ell m})Y_{\ell m}∑m​(X0​,Yℓm​)Yℓm​ is written in the real orthonormal basis.
  • Brownian motions are Mathlib's IsBrownianReal processes on R≥0\mathbb R_{\ge0}R≥0​, independent as a family of path-valued random variables. The stochastic convolution ∫0te−r(t−s)db(s)\int_0^te^{-r(t-s)}db(s)∫0t​e−r(t−s)db(s) is defined pathwise as b(t)−r∫0te−r(t−s)b(s) dsb(t)-r\int_0^te^{-r(t-s)}b(s)\,dsb(t)−r∫0t​e−r(t−s)b(s)ds, which equals the Wiener integral almost surely (integration by parts; b(0)=0b(0)=0b(0)=0 a.s.). This is the one place where a stochastic integral is replaced by a pathwise expression.
  • The Laplace–Beltrami operator is not defined: the paper's spectral solution formula of p. 36 is taken as the definition of X(t)X(t)X(t), as a pointwise limit of partial sums in (ω,y)(\omega,y)(ω,y); where they diverge (a P⊗σ\mathbb P\otimes\sigmaP⊗σ-null set for t>0t>0t>0) the value is irrelevant to every norm. All statements take t>0t>0t>0; the paper's time partition with n∈Nn\in\mathbb Nn∈N forces this, and since Xκ(t)X^\kappa(t)Xκ(t) is defined from the solution itself the independence of the time discretization is automatic and the partition is not an argument.
  • Norms are lower Lebesgue integrals in [0,∞][0,\infty][0,∞], so no integrability side condition hides in a default value; X0X_0X0​ is jointly measurable with E∥X0∥L2(S2)2<∞\mathbb E\|X_0\|^2_{L^2(\mathbb S^2)}<\inftyE∥X0​∥L2(S2)2​<∞; Aℓ≥0A_\ell\ge0Aℓ​≥0; ℓ0≥1\ell_0\ge1ℓ0​≥1.
  • Corrections. Lemmas 7.1 and 7.2 claim bounds uniform in time with constants depending only on ∥X0∥\|X_0\|∥X0​∥, CCC, α\alphaα (and ppp). Their proofs bound the initial-condition tail by e−2(κ+1)(κ+2)t∥X0∥2e^{-2(\kappa+1)(\kappa+2)t}\|X_0\|^2e−2(κ+1)(κ+2)t∥X0​∥2 (resp. e−(κ+1)(κ+2)t∥X0∥Lpe^{-(\kappa+1)(\kappa+2)t}\|X_0\|_{L^p}e−(κ+1)(κ+2)t∥X0​∥Lp​) and absorb it into Cκ−αC\kappa^{-\alpha}Cκ−α with a ttt-dependent constant; for nonzero X0X_0X0​ the printed uniform bounds are false (as t↓0t\downarrow0t↓0 the error tends to the L2L^2L2 tail of X0X_0X0​). The milestones state the proofs' bounds with the explicit exponential term; for X0=0X_0=0X0​=0 Lemma 7.1 is the printed statement, uniformly in ttt. Lemma 7.1 additionally assumes that the coefficients of X0X_0X0​ are independent of the noise, which its proof uses to drop a cross term. In Lemma 7.2 the constant C^p\hat C_pC^p​ depends on p,C,αp,C,\alphap,C,α only and is quantified before everything else. Corollary 7.3 is stated for each fixed ttt: "uniformly in time" is not formalized. The constant on p. 42, (2/(α−2)+1/(α−1))(2/(\alpha-2)+1/(\alpha-1))(2/(α−2)+1/(α−1)), should read (2/α+1/(α+1))(2/\alpha+1/(\alpha+1))(2/α+1/(α+1)); it is existential in Lemma 7.2 and has no effect.
  • A trivializing reading is ruled out: the error is measured against the solution defined by the explicit series, not against an arbitrary process satisfying a hypothesis, and no hypothesis pins the conclusion.
  • Reusable infrastructure: real spherical harmonics and their orthonormality on (S2,σ)(\mathbb S^2,\sigma)(S2,σ), the Wiener integral of deterministic functions and the Ornstein–Uhlenbeck law, and LpL^pLp moment equivalence for Gaussian fields. Contributions of any of these, or of the truncation estimates of §5 for the shifted spectrum, are welcome.

Selected references

  • A. Lang, Ch. Schwab, Isotropic Gaussian random fields on the sphere: regularity, fast simulation and stochastic partial differential equations, Ann. Appl. Probab. 25(6), 2015. arXiv:1305.1170
  • A. Jentzen, P. E. Kloeden, Overcoming the order barrier in the numerical approximation of stochastic partial differential equations with additive space–time noise, Proc. R. Soc. A 465, 2009. doi:10.1098/rspa.2008.0325
  • G. Da Prato, J. Zabczyk, Stochastic Equations in Infinite Dimensions, Cambridge University Press, 1992. doi:10.1017/CBO9780511666223
  • D. Marinucci, G. Peccati, Random Fields on the Sphere, Cambridge University Press, 2011. doi:10.1017/CBO9780511751677
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ProbabilityStatisticsStochastic Systems·Captain: mikedeng1

Limit Theorems for Nearly Unstable Hawkes Processes 2: When T(1 − a_T) → λ the Rescaled Intensity Converges in Law to a CIR Process and the Rescaled Hawkes Process to Its IntegralResearch Paper

Motivation

An event stream can raise its own future event rate. A Hawkes process models this feedback by adding to a baseline rate the effects of past arrivals. The parameter measuring total excitation can approach its stability boundary, at which long clusters make a fixed time scale an unreliable guide to the observed count. Jaisson and Rosenbaum identify a regime in which observation time and the distance to that boundary balance, leaving a stochastic limit rather than a deterministic average Jaisson and Rosenbaum, 2015. Their theorem gives a precise bridge from an event count with jumps to a continuous square-root diffusion. The paper notes a practical reason for this bridge: intermediate-scale inference can use diffusion methods to estimate the baseline rate and two aggregate kernel parameters, though it cannot recover the entire excitation kernel Jaisson and Rosenbaum, §2.4, p. 10.

Setting

For each observation horizon TTT, let NtTN^T_tNtT​ count events up to time ttt, with N0T=0N^T_0=0N0T​=0. The process is observed on [0,T][0,T][0,T] and has intensity

λtT=μ+∫0tϕT(t−s) dNsT,ϕT=aTϕ,\lambda^T_t=\mu+\int_0^t\phi^T(t-s)\,dN^T_s, \qquad \phi^T=a_T\phi,λtT​=μ+∫0t​ϕT(t−s)dNsT​,ϕT=aT​ϕ,

where μ>0\mu>0μ>0 is the baseline rate. The integral against NTN^TNT is a sum over its unit jumps. The nonnegative kernel ϕ\phiϕ has total mass one and finite mean m=∫0∞sϕ(s) dsm=\int_0^\infty s\phi(s)\,dsm=∫0∞​sϕ(s)ds; its derivative is bounded and integrable. The coefficients satisfy 0<aT<10<a_T<10<aT​<1 and aT→1a_T\to1aT​→1. Thus aTa_TaT​ is the total mass of ϕT\phi^TϕT, and the model approaches the stability boundary from below. The natural filtration is generated by the observed count. The intensity relation is the identity for conditional expected increments on every interval 0≤a<b≤T0\le a<b\le T0≤a<b≤T and every event observable at time aaa Jaisson and Rosenbaum, §2.1, p. 5.

The resolvent ψT=∑k≥1(ϕT)∗k\psi^T=\sum_{k\ge1}(\phi^T)^{*k}ψT=∑k≥1​(ϕT)∗k collects excitation across repeated generations. Its rescaled density is ρT(x)=TψT(Tx)/∥ψT∥1\rho^T(x)=T\psi^T(Tx)/\|\psi^T\|_1ρT(x)=TψT(Tx)/∥ψT∥1​. The mission uses the paper's additional bound sup⁡T,x≥0∣ρT(x)∣<∞\sup_{T,x\ge0}|\rho^T(x)|<\inftysupT,x≥0​∣ρT(x)∣<∞ and the balance condition T(1−aT)→λ>0T(1-a_T)\to\lambda>0T(1−aT​)→λ>0. Here λ\lambdaλ is a fixed limiting parameter, distinct from the time-dependent intensity λtT\lambda^T_tλtT​. The processes to be compared on a common interval are

CtT=(1−aT)λtTT,VtT=1−aTTNtTT,0≤t≤1.C^T_t=(1-a_T)\lambda^T_{tT},\qquad V^T_t=\frac{1-a_T}{T}N^T_{tT},\qquad 0\le t\le1.CtT​=(1−aT​)λtTT​,VtT​=T1−aT​​NtTT​,0≤t≤1.

Formalization targets

The main target is Theorem 2.2, p. 10: CTC^TCT converges in law in the Skorohod topology on D[0,1]D[0,1]D[0,1] to the unique strong solution, started at zero, of the Cox–Ingersoll–Ross equation

Xt=∫0t(μ−Xs)λm ds+λm∫0tXs dBs.X_t=\int_0^t(\mu-X_s)\frac{\lambda}{m}\,ds +\frac{\sqrt\lambda}{m}\int_0^t\sqrt{X_s}\,dB_s.Xt​=∫0t​(μ−Xs​)mλ​ds+mλ​​∫0t​Xs​​dBs​.

Separately, VTV^TVT converges in law in the same path topology to t↦∫0tXs dst\mapsto\int_0^tX_s\,dst↦∫0t​Xs​ds. These are two convergence claims, each on its own path space law. The statement also asserts that the strong solution exists, so convergence to “every solution” cannot hold merely because there are no solutions.

The supporting targets follow the paper's stated results. Lemma 4.1 and Proposition 2.1 identify the resolvent renewal identity and the intensity's resolvent form; both are supporting theorem items. Lemmas 4.2–4.5 give separation and decay estimates for the plus-sign Fourier transforms of ϕ\phiϕ and ρT\rho^TρT, followed by L2L^2L2 convergence of ρT\rho^TρT to the exponential density (λ/m)e−xλ/m(\lambda/m)e^{-x\lambda/m}(λ/m)e−xλ/m. Lemma 4.9 gives a fourth-moment increment bound for the paper's residual process YTY^TYT, and Proposition 4.1 states that YTY^TYT tends to zero uniformly in probability on [0,1][0,1][0,1]. The latter six are source-stated milestones, with their pages and texts recorded separately.

Significance

The theorem identifies the scale at which a nearly unstable event model retains random dynamics. It also identifies the diffusion coefficients: the drift relaxes toward μ\muμ at rate λ/m\lambda/mλ/m, and the noise has coefficient λ/m\sqrt\lambda/mλ​/m times the square root of the current intensity. The second convergence claim transfers this intensity behavior to accumulated events. Those coefficients make the limit more informative than a statement that merely names a generic continuous process Jaisson and Rosenbaum, Theorem 2.2.

The result is proved in the paper but has no matching published Hawkes formalization in the local Prove2Me index used for this mission. Machine-checked definitions for Brownian motion and strong SDE solutions from the Ethier–Kurtz development are already available and referenced here. The new formal work is the Hawkes model, its path-space convergence, the density estimates, and the limit theorem itself. Formalizing the stated milestones would also leave reusable analytic and probability interfaces for other nearly unstable point-process limits.

Difficulty

Pointwise convergence of an intensity or of finitely many observations does not control its law as a cadlag path. Excitation also couples each event to later events, so a direct independent-increment argument is unavailable. The resolvent has to be controlled at the observation scale, including its high-frequency behavior, while the stochastic remainder has to be controlled uniformly over time. The final limit is a square-root SDE: its coefficient is not globally Lipschitz at zero, and a claim about its law must keep the initial condition and Brownian driver explicit Jaisson and Rosenbaum, §§4.2–4.3.

Formalization scope

The horizon TTT is a positive real sequence tending to infinity, as the paper's footnote specifies; aTa_TaT​ is a sequence in (0,1)(0,1)(0,1) tending to one. Each index may have its own probability space. The count is natural-number valued, nondecreasing, right-continuous, starts at zero, and has unit jumps. Its filtration is generated by evaluations of NTN^TNT. The intensity identity uses extended nonnegative integrals, avoiding an arbitrary real value for an infinite expectation. The right-continuous intensity includes an event at the current time, so CTC^TCT is cadlag. Its predictable left-limit version is available for stochastic integrands. All results use the half-line kernel and ϕT=aTϕ\phi^T=a_T\phiϕT=aT​ϕ; they never replace it by ϕ\phiϕ in the Hawkes process.

Skorohod convergence is represented by a coupling whose cadlag paths approach each other after increasing homeomorphic time changes of [0,1][0,1][0,1]. This is the representation form of weak convergence in D[0,1]D[0,1]D[0,1] with the J1J_1J1​ topology. The limit SDE uses the published global strong-solution predicate, then restricts its paths to [0,1][0,1][0,1]. Its drift is exactly (μ−x)λ/m(\mu-x)\lambda/m(μ−x)λ/m and diffusion exactly (λ/m)x(\sqrt\lambda/m)\sqrt{x}(λ​/m)x​; Real.sqrt on negative arguments does not affect its nonnegative solution. The renewal theorem item additionally makes the unknown fff measurable and locally bounded so its real convolution integral has its stated meaning. Fourier denominators exclude zero explicitly, while the zero-frequency bound is stated separately. The density convergence uses an extended nonnegative squared integral, and uniform probability convergence uses an extended supremum. These choices rule out default-zero values, a vacuous Hawkes class, a free limit process, and finite-dimensional convergence in place of path convergence.

The development needs half-line convolution and summable resolvents, natural filtrations and compensated point processes, Fourier bounds, cadlag path laws, and Itô SDEs. The convolution, path-space, and point-process interfaces are suitable for reuse. Contributions should preserve the exact hypotheses, constants, and two distinct convergence conclusions of the source theorem.

Selected references

  • T. Jaisson and M. Rosenbaum, Limit theorems for nearly unstable Hawkes processes, Annals of Applied Probability 25(2), 2015, arXiv:1310.2033v2. Preprint; DOI.
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A Constant-Factor Approximation Algorithm for the Asymmetric Traveling Salesman Problem: The Asymmetric Held–Karp Relaxation Has Integrality Gap at Most 319Research Paper

Motivation

The asymmetric traveling salesman problem (ATSP) asks for a shortest closed walk through every vertex of a directed graph whose edge weights need not be symmetric. It models routing with one-way streets, scheduling with sequence-dependent setup times, and many other problems in which the cost of going from uuu to vvv differs from the cost of going back. Its standard linear relaxation, the asymmetric Held–Karp relaxation, is the lower bound used both by exact branch-and-cut codes and by approximation algorithms, and the central question about it is how far it can be from the integer optimum.

Timeline of the approximation ratio and of the integrality gap for ATSP:

  • 1982: Frieze, Galbiati and Maffioli give a log⁡2n\log_2 nlog2​n-approximation by repeated cycle covers.
  • 2010: Asadpour, Goemans, Mądry, Oveis Gharan and Saberi reach O(log⁡n/log⁡log⁡n)O(\log n/\log\log n)O(logn/loglogn) via thin trees (SODA 2010).
  • 2015: Anari and Oveis Gharan bound the integrality gap by poly(log⁡log⁡n)\mathrm{poly}(\log\log n)poly(loglogn), non-constructively; Svensson obtains a constant factor for node-weighted digraphs.
  • 2018: Svensson, Tarnawski and Végh obtain the first constant-factor approximation for general ATSP (STOC 2018); the journal version (J. ACM 2020) states the ratio 506506506 and the integrality gap bound 319319319.
  • 2020: Traub and Vygen improve the ratio to 22+ε22+\varepsilon22+ε and the gap to 222222 (STOC 2020).

The lower bound on the integrality gap remains 222 (Charikar, Goemans and Karloff, 2006).

Setting

A digraph G=(V,E)G=(V,E)G=(V,E) has finite vertex and edge sets; each edge has a tail and a head, and parallel edges and loops are allowed. For S⊆VS\subseteq VS⊆V, δ+(S)\delta^+(S)δ+(S) and δ−(S)\delta^-(S)δ−(S) are the edges leaving and entering SSS, and δ(S)=δ+(S)∪δ−(S)\delta(S)=\delta^+(S)\cup\delta^-(S)δ(S)=δ+(S)∪δ−(S). An ATSP input is a strongly connected digraph GGG with a weight function w:E→R≥0w:E\to\mathbb R_{\ge0}w:E→R≥0​.

An edge multiset FFF gives each edge a multiplicity F(e)∈NF(e)\in\mathbb NF(e)∈N; V(F)V(F)V(F) is the set of vertices it touches. FFF is Eulerian if every vertex has as many outgoing as incoming edges of FFF, a subtour if moreover (V(F),F)(V(F),F)(V(F),F) is connected, and a tour if it is a subtour with V(F)=VV(F)=VV(F)=V. Tours are exactly the closed walks visiting every vertex. The weight of FFF is ∑eF(e)w(e)\sum_e F(e)w(e)∑e​F(e)w(e).

The asymmetric Held–Karp relaxation LP(G,w)(G,w)(G,w) is

min⁡∑e∈Ew(e)x(e)s.t.x(δ+(v))=x(δ−(v)) (v∈V),x(δ(S))≥2 (∅≠S⊊V),x≥0,\min\sum_{e\in E}w(e)x(e)\quad\text{s.t.}\quad x(\delta^+(v))=x(\delta^-(v))\ (v\in V),\qquad x(\delta(S))\ge2\ (\emptyset\ne S\subsetneq V),\qquad x\ge0,mine∈E∑​w(e)x(e)s.t.x(δ+(v))=x(δ−(v)) (v∈V),x(δ(S))≥2 (∅=S⊊V),x≥0,

and its optimum is the Held–Karp lower bound.

The mission also uses the paper's intermediate objects: laminarly-weighted instances I=(G,L,x,y)I=(G,\mathcal L,x,y)I=(G,L,x,y), in which L\mathcal LL is a laminar family of sets that are tight for a strictly positive feasible xxx, y≥0y\ge0y≥0 on L\mathcal LL, and the weight of an edge is wI(e)=∑S∈L: e∈δ(S)ySw_I(e)=\sum_{S\in\mathcal L:\,e\in\delta(S)}y_SwI​(e)=∑S∈L:e∈δ(S)​yS​; the value value(I)=2∑S∈LyS\mathrm{value}(I)=2\sum_{S\in\mathcal L}y_Svalue(I)=2∑S∈L​yS​ and the lower bound lbI(U)=∑v∈U2y{v}\mathrm{lb}_I(U)=\sum_{v\in U}2y_{\{v\}}lbI​(U)=∑v∈U​2y{v}​; Subtour Partition Cover and (α,β)(\alpha,\beta)(α,β)-lightness; irreducible instances; vertebrate pairs; and quasi-backbones. Each is defined, with the paper's page reference, in the two definition files of the mission.

Formalization targets

Goal: Theorem 11.1

For every strongly connected digraph GGG with ∣V∣≥2|V|\ge2∣V∣≥2, every w≥0w\ge0w≥0 and every feasible solution xxx of LP(G,w)(G,w)(G,w), there is a tour FFF with

∑e∈EF(e) w(e) ≤ 319∑e∈Ew(e) x(e).\sum_{e\in E}F(e)\,w(e)\ \le\ 319\sum_{e\in E}w(e)\,x(e).e∈E∑​F(e)w(e) ≤ 319e∈E∑​w(e)x(e).

This is the statement that the integrality gap of the asymmetric Held–Karp relaxation is at most 319319319.

Milestones

The milestones are the results the paper's §11 combines, in the order it combines them:

  1. Theorem 4.1: Subtour Partition Cover is (2,0)(2,0)(2,0)-light on singleton instances with B=∅B=\emptysetB=∅.
  2. Theorem 5.1: an (α,β)(\alpha,\beta)(α,β)-light pair (I,B)(I,B)(I,B) has a tour of weight at most 5α lbI(Bˉ)+β+wI(B)5\alpha\,\mathrm{lb}_I(\bar B)+\beta+w_I(B)5αlbI​(Bˉ)+β+wI​(B).
  3. §11: every singleton instance has a tour of weight at most 10 value(I)10\,\mathrm{value}(I)10value(I) (αS′=10\alpha'_S=10αS′​=10).
  4. Theorem 10.1: vertebrate pairs are (4, 2 value(I)+lbI(Bˉ))(4,\,2\,\mathrm{value}(I)+\mathrm{lb}_I(\bar B))(4,2value(I)+lbI​(Bˉ))-light.
  5. §11: a vertebrate pair has a tour of weight at most 2 value(I)+21 lbI(Bˉ)+wI(B)2\,\mathrm{value}(I)+21\,\mathrm{lb}_I(\bar B)+w_I(B)2value(I)+21lbI​(Bˉ)+wI​(B) (η′=1+5⋅4\eta'=1+5\cdot4η′=1+5⋅4).
  6. Lemma 9.3: an irreducible instance has a quasi-backbone of weight at most (αS+3) value(I)(\alpha_S+3)\,\mathrm{value}(I)(αS​+3)value(I).
  7. Theorem 9.4: tours on vertebrate pairs give a ρ\rhoρ-bound on irreducible instances, ρ=κ+η(1−δ)+αS+32δ−1\rho=\frac{\kappa+\eta(1-\delta)+\alpha_S+3}{2\delta-1}ρ=2δ−1κ+η(1−δ)+αS​+3​.
  8. Theorem 8.3: a ρ\rhoρ-bound on irreducible instances gives a 2ρ1−δ\frac{2\rho}{1-\delta}1−δ2ρ​-bound on all laminarly-weighted instances.
  9. Lemma 2.2: DUAL(G,w)(G,w)(G,w) has an optimal solution with laminar support.
  10. Theorem 2.4: a bound α value(I)\alpha\,\mathrm{value}(I)αvalue(I) on all laminarly-weighted instances gives α\alphaα times the Held–Karp bound on all ATSP inputs.

Significance

The result shows that the asymmetric Held–Karp relaxation approximates ATSP within a constant factor, which settled a question open since the 1980s and made the relaxation a certified lower bound with bounded loss. The structural steps (reduction to laminarly-weighted instances, Subtour Partition Cover, irreducibility and vertebrate pairs) are the framework on which the later improvement to 222222 by Traub and Vygen is built.

The theorem is proved; to the best of available knowledge none of it has been formalized in a proof assistant. A complete development would give a machine-checked bound on the integrality gap of a central relaxation in combinatorial optimization, and its intermediate statements are reusable for the improved bounds that follow the same framework.

Difficulty

The obvious approaches do not give a constant. Repeated cycle covers lose a factor at each of logarithmically many rounds. Rounding the LP solution through thin trees needs a spanning tree that is thin in every cut, and only polylogarithmic thinness is known. The paper's route is long: the reduction to laminarly-weighted instances needs an uncrossed dual; the reduction from irreducible to general instances and the one from vertebrate pairs to irreducible instances are recursive, applying the assumed algorithm to instances built by contracting or inducing tight sets, so their hypotheses must hold on all instances and not only on the given one; and the lightness bound for vertebrate pairs (Theorem 10.1) rests on a flow-based construction with careful accounting against the laminar family.

Formalization scope

Vertices and edges are finite types; edges carry tail and head maps, so parallel edges (created by contraction) are distinct edges, and loops are allowed and lie in no cut. Edge multisets are functions E→NE\to\mathbb NE→N. Connectivity of a multiset and its components are defined by the reflexive–transitive closure of undirected adjacency along its edges.

Running times are not formalized. Every algorithmic statement is posed in its existential form, as §11 of the paper itself uses it to derive Theorem 11.1: "there is an algorithm returning a tour within ccc" becomes "every instance has a tour within ccc", and an assumed algorithm becomes a hypothesis quantified over instances on all finite vertex and edge types. The algorithmic constants 9(1+ε)9(1+\varepsilon)9(1+ε), 18+ε18+\varepsilon18+ε, 37+36ε37+36\varepsilon37+36ε and 506506506 are therefore not stated; the non-constructive constants 555, 101010 and 212121 of §11 are.

The Held–Karp lower bound is never defined as an infimum: comparisons with it are stated for every feasible xxx, equivalently because the LP optimum is attained. Likewise dSd_SdS​ and DSD_SDS​ in the definition of irreducibility are expressed through walks, without an infimum.

Added hypotheses, each disclosed in the item's Formalization Note:

  • ∣V∣≥2|V|\ge2∣V∣≥2 in the goal, Theorem 2.4 and every laminarly-weighted instance: on one vertex without a loop no tour exists while LP(G,w)(G,w)(G,w) has value 000.
  • Partition parts in Subtour Partition Cover are nonempty and different from VVV; for B=∅B=\emptysetB=∅ the one-part partition (V)(V)(V) admits no solution.
  • α≥0\alpha\ge0α≥0 in Theorem 5.1, which is false without it.
  • αS\alpha_SαS​ in Lemma 9.3 and Theorem 9.4 is a parameter with the hypothesis that singleton instances have tours within αS value\alpha_S\,\mathrm{value}αS​value, instead of the fixed 18+ε18+\varepsilon18+ε.

These choices rule out trivializing formalizations: no instance class in a hypothesis is empty (a two-vertex singleton instance is valid, irreducible and vertebrate), admissible partitions exist for every instance, and LP(G,w)(G,w)(G,w) is feasible for every strongly connected input. The goal assumes none of the milestones.

Out of scope: the polynomial running times, §5's merge-procedure lemmas, the constructions of §7, and Corollaries 11.2–11.4 on the path version, which rest on external reductions. Contributions are welcome on every milestone, and on infrastructure that a complete development needs: LP duality and uncrossing for cut LPs, Eulerian multigraphs and their decomposition into closed walks, and circulations with lower bounds (Hoffman's theorem). The platform's proved LP strong duality (SmaleNinth.lp_strong_duality) is a natural starting point for Lemma 2.2.

Selected references

  • O. Svensson, J. Tarnawski, L. A. Végh, A constant-factor approximation algorithm for the asymmetric traveling salesman problem, J. ACM 67(6), 2020. https://doi.org/10.1145/3424306 (accepted manuscript: LSE Research Online 106582, https://eprints.lse.ac.uk/106582/)
  • O. Svensson, J. Tarnawski, L. A. Végh, A constant-factor approximation algorithm for the asymmetric traveling salesman problem, STOC 2018. https://doi.org/10.1145/3188745.3188824
  • V. Traub, J. Vygen, An improved approximation algorithm for ATSP, STOC 2020. https://arxiv.org/abs/1912.00670
  • A. Asadpour, M. X. Goemans, A. Mądry, S. Oveis Gharan, A. Saberi, An O(log n/log log n)-approximation algorithm for the asymmetric traveling salesman problem, SODA 2010. https://doi.org/10.1137/1.9781611973075.32
  • A. M. Frieze, G. Galbiati, F. Maffioli, On the worst-case performance of some algorithms for the asymmetric traveling salesman problem, Networks 12(1), 1982. https://doi.org/10.1002/net.3230120103
  • M. Charikar, M. X. Goemans, H. Karloff, On the integrality ratio for the asymmetric traveling salesman problem, Math. Oper. Res. 31(2), 2006. https://doi.org/10.1287/moor.1050.0172
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ProbabilityStatisticsStochastic Systems·Captain: mikedeng1

Limit Theorems for Nearly Unstable Hawkes Processes 1: When T(1 − a_T) → ∞ the Rescaled Hawkes Process Is Asymptotically Deterministic in L²Research Paper

Motivation

A Hawkes process is a model for events that make further events more likely for a time. It is used when event times cluster, including transaction arrivals in financial markets. Jaisson and Rosenbaum study what happens when the feedback approaches the threshold at which the usual stable model ceases to have a finite long-run mean intensity. The behavior depends on how fast the observation horizon grows relative to that approach to instability. Their first regime says that, when the horizon grows sufficiently faster, the observed count still becomes deterministic after normalization. The precise result is Theorem 2.1 of Jaisson and Rosenbaum (2015).

The mission concerns that first regime alone. It isolates an L2L^2L2 statement that controls the whole observed path at once, rather than a count at one fixed time. Later results in the paper use a different balance between the horizon and the feedback parameter and produce stochastic diffusion limits. Those later regimes are separate missions in this series.

Setting

For each horizon T>0T>0T>0, let NtTN^T_tNtT​ count events through time ttt, starting from N0T=0N^T_0=0N0T​=0. It is observed for 0≤t≤T0\le t\le T0≤t≤T on a probability space that may depend on TTT. Its intensity is the nonnegative process

λtT=μ+∫0tϕT(t−s) dNsT,μ>0.\lambda_t^T=\mu+\int_0^t\phi^T(t-s)\,dN_s^T,\qquad \mu>0.λtT​=μ+∫0t​ϕT(t−s)dNsT​,μ>0.

The baseline μ\muμ creates events even before any excitation. At each jump of NTN^TNT, the kernel ϕT\phi^TϕT adds an effect that depends on the elapsed time since that event. The intensity property is specified relative to the natural filtration FtT=σ(NsT:0≤s≤t)\mathcal F_t^T=\sigma(N_s^T:0\le s\le t)FtT​=σ(NsT​:0≤s≤t): for 0≤a<b≤T0\le a<b\le T0≤a<b≤T and A∈FaTA\in\mathcal F_a^TA∈FaT​, the expected number of new events on AAA equals the expected integrated intensity on AAA over (a,b](a,b](a,b]. This is the defining condition used in §2.1 of the paper.

Assumption 1 fixes a nonnegative measurable kernel ϕ\phiϕ of total mass one and finite first moment m=∫0∞sϕ(s) dsm=\int_0^\infty s\phi(s)\,dsm=∫0∞​sϕ(s)ds. Its derivative is bounded and integrable. The horizon-dependent kernel is ϕT=aTϕ\phi^T=a_T\phiϕT=aT​ϕ, with 0<aT<10<a_T<10<aT​<1 and aT→1a_T\to1aT​→1. Thus ∥ϕT∥1=aT\|\phi^T\|_1=a_T∥ϕT∥1​=aT​ approaches the stability boundary. The paper also defines the compensated count MtT=NtT−∫0tλsT dsM_t^T=N_t^T-\int_0^t\lambda_s^T\,dsMtT​=NtT​−∫0t​λsT​ds and the resolvent ψT=∑k≥1(ϕT)∗k\psi^T=\sum_{k\ge1}(\phi^T)^{*k}ψT=∑k≥1​(ϕT)∗k, where each convolution uses nonnegative time. These enter the supporting results.

Formalization targets

The goal is Theorem 2.1, in the regime T(1−aT)→∞T(1-a_T)\to\inftyT(1−aT​)→∞. Its L2L^2L2 assertion is

E ⁣[(sup⁡v∈[0,1]1−aTT∣NTvT−E[NTvT]∣)2]⟶0.\mathbb E\!\left[\left(\sup_{v\in[0,1]}\frac{1-a_T}{T} \left|N^T_{Tv}-\mathbb E[N^T_{Tv}]\right|\right)^2\right]\longrightarrow0.E​(v∈[0,1]sup​T1−aT​​​NTvT​−E[NTvT​]​)2​⟶0.

The supremum is inside the expectation. The time variable vvv runs over the entire unit interval, so this is a statement about the normalized path of the count. The normalizing factor depends on both the horizon and the distance 1−aT1-a_T1−aT​ from the stability boundary.

The milestone list consists of the paper's renewal identity (Lemma 4.1), its two representations of the Hawkes mean and centered count, the exact mass of ψT\psi^TψT, a pathwise fluctuation bound, the Doob L2L^2L2 estimate for MTM^TMT, and the finite-horizon bound with constant 4μ/[T(1−aT)]4\mu/[T(1-a_T)]4μ/[T(1−aT​)]. The final estimate has no asymptotic hypothesis; the goal adds the regime condition and takes its limit. The unnumbered milestones are the displays in §4.1, pp. 14–15, and Lemma 4.1 appears in §4.2, p. 15.

Significance

The result identifies a regime in which near instability does not produce macroscopic random fluctuations at the paper's normalization. It supplies a boundary between the familiar deterministic large-horizon behavior of stable Hawkes processes and the diffusion behavior obtained under the paper's other scaling. The theorem controls the largest fluctuation over the whole observation interval, which is stronger than a statement at each fixed vvv or a bound on the supremum of separate variances.

The mathematical result is proved in the paper; the target here is a machine-checked proof of the same result. A completed development would also provide reusable Lean definitions for a simple counting process, its generated filtration, pathwise jump integration, Hawkes intensity, and nonnegative-time convolution resolvent. It would make explicit the maximal inequality and renewal estimates needed for other Hawkes scaling questions. This mission currently poses these statements as open Lean proof obligations; it does not claim the paper's proof is already formalized.

Difficulty

The near-instability parameter aTa_TaT​ tends to one, so estimates for a Hawkes process with a fixed a<1a<1a<1 cannot simply be used with a uniform constant. The scale of the mean and the size of the fluctuations both change with TTT. There is also a pathwise issue: the theorem places a supremum over all v∈[0,1]v\in[0,1]v∈[0,1] inside an L2L^2L2 expectation. A separate estimate for each vvv does not provide the required control of the path maximum.

The point-process side adds another layer. The compensated count is a continuous-time martingale with jumps, and the intensity depends on its own event history. The result therefore needs the correct relation among the natural filtration, the intensity identity, the resolvent, and the martingale maximum. The book-keeping at a jump matters: the cadlag intensity includes the jump at its time, while stochastic compensator integrals use the same process only up to a set of times of Lebesgue measure zero.

Formalization scope

The Lean development indexes the paper's implicit horizons as a sequence Tn>0T_n>0Tn​>0 tending to infinity; the multipliers an∈(0,1)a_n\in(0,1)an​∈(0,1) tend to one, and Tn(1−an)→∞T_n(1-a_n)\to\inftyTn​(1−an​)→∞. Each NTnN^{T_n}NTn​ may use a different probability space. Time is represented by real numbers, with the counting-process conditions applied on nonnegative time and the Hawkes intensity identity applied only through the observation horizon. The count is natural-number valued, right-continuous, nondecreasing, and has unit jumps. The Hawkes intensity is defined by a finite sum over jumps in (0,t](0,t](0,t], and the conditional intensity identity uses extended nonnegative expectations, so an infinite expectation is not silently assigned zero.

The kernel ϕ\phiϕ is measurable and nonnegative on [0,∞)[0,\infty)[0,∞), has total mass one and finite first moment, and has an integrable bounded derivative; differentiability at zero is one-sided. The resolvent starts at the first convolution power, not at an identity term. Its L1L^1L1 mass is taken over positive time. The path supremum and its squared expectation are extended nonnegative quantities. Ordinary real expectations of NTvTN^T_{Tv}NTvT​ are retained because their integrability follows from the Hawkes assumptions; the theorem does not assume it separately.

The Hawkes predicate is the paper's natural-filtration intensity condition for ϕT=aTϕ\phi^T=a_T\phiϕT=aT​ϕ. A vacuous process condition, an intensity built from ϕ\phiϕ instead of ϕT\phi^TϕT, or a supremum taken outside the expectation would change the target. Contributions to the generic counting-process and resolvent definitions, the renewal identity, the finite-horizon martingale estimates, and the goal theorem are all within scope. The source's p. 14 bound omits an absolute value on the centered count; the Lean milestone states the absolute-value form required by its subsequent squared estimate, while its verbatim field preserves the printed form.

Selected references

  • Thibault Jaisson and Mathieu Rosenbaum, Limit theorems for nearly unstable Hawkes processes, Annals of Applied Probability 25(2), 2015, arXiv:1310.2033v2. Pinned preprint; DOI.
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Learning without Concentration: Least-Squares ERM in a Convex Class Is Within 2 max{α_N(γ, δ/4), βN(τQ{F−F}(2τ)/16)} of f* in L₂ under a Small-Ball ConditionResearch Paper

Motivation

Least-squares regression over a class of functions is the basic problem of statistical learning theory: given an i.i.d. sample (Xi,Yi)i=1N(X_i,Y_i)_{i=1}^N(Xi​,Yi​)i=1N​ from an unknown joint law, select a function in a class FFF whose prediction error E(f(X)−Y)2\mathbb E(f(X)-Y)^2E(f(X)−Y)2 is close to the best possible in FFF. The standard analysis of empirical risk minimization (ERM) compares empirical means with true means uniformly over the class, which requires the class and the target to concentrate: bounded functions, or sub-Gaussian tails. Heavy-tailed classes and targets, which arise as soon as the data are not bounded, fall outside that analysis.

S. Mendelson, Learning without Concentration (arXiv:1401.0304, J. ACM 62(3), 2015), showed that concentration is not needed for the lower half of the argument. The only property used for the quadratic part of the loss is a small-ball condition: functions in F−FF-FF−F are not too concentrated near zero. Under that condition, ERM over a closed convex class attains an error governed by two localized complexity parameters, one intrinsic to the class and one measuring its interaction with the noise. The same lower-bound mechanism appears, for random matrices, in Koltchinskii–Mendelson (arXiv:1312.3580); the localized complexity parameters follow Lecué–Mendelson (arXiv:1305.4825).

Setting

Let (Ω,μ)(\Omega,\mu)(Ω,μ) be a probability space and let (X,Y)(X,Y)(X,Y) have joint law ν\nuν on Ω×R\Omega\times\mathbb RΩ×R, with X∼μX\sim\muX∼μ and EY2<∞\mathbb EY^2<\inftyEY2<∞. Let F⊂L2(μ)F\subset L_2(\mu)F⊂L2​(μ) be a closed, convex class of real functions on Ω\OmegaΩ, and let f∗∈Ff^*\in Ff∗∈F minimize E(f(X)−Y)2\mathbb E(f(X)-Y)^2E(f(X)−Y)2 over FFF. The noise is ξ=f∗(X)−Y\xi=f^*(X)-Yξ=f∗(X)−Y. Given an i.i.d. sample (Xi,Yi)i=1N(X_i,Y_i)_{i=1}^N(Xi​,Yi​)i=1N​ from ν\nuν, an empirical minimizer f^\hat ff^​ minimizes 1N∑i=1N(f(Xi)−Yi)2\frac1N\sum_{i=1}^N(f(X_i)-Y_i)^2N1​∑i=1N​(f(Xi​)−Yi​)2 over FFF. Let (εi)i=1N(\varepsilon_i)_{i=1}^N(εi​)i=1N​ be independent random signs, independent of the sample, and write F∩rDf∗={f∈F:∥f−f∗∥L2≤r}F\cap rD_{f^*}=\{f\in F:\|f-f^*\|_{L_2}\le r\}F∩rDf∗​={f∈F:∥f−f∗∥L2​​≤r}.

  • The small-ball function of a class HHH is QH(u)=inf⁡h∈HPr⁡(∣h(X)∣≥u∥h∥L2)Q_H(u)=\inf_{h\in H}\Pr(|h(X)|\ge u\|h\|_{L_2})QH​(u)=infh∈H​Pr(∣h(X)∣≥u∥h∥L2​​); it is applied to F−F={f−h:f,h∈F}F-F=\{f-h:f,h\in F\}F−F={f−h:f,h∈F}.
  • The intrinsic parameter (Definition 2.1) is
βN∗(γ)=inf⁡{r>0:Esup⁡f∈F∩rDf∗∣1N∑iεi(f−f∗)(Xi)∣≤γNr}.\beta^*_N(\gamma)=\inf\Bigl\{r>0:\mathbb E\sup_{f\in F\cap rD_{f^*}}\Bigl|\tfrac1{\sqrt N}\textstyle\sum_{i}\varepsilon_i(f-f^*)(X_i)\Bigr|\le\gamma\sqrt N r\Bigr\}.βN∗​(γ)=inf{r>0:Ef∈F∩rDf∗​sup​​N​1​∑i​εi​(f−f∗)(Xi​)​≤γN​r}.
  • The multiplier process (2.2) is ϕN(s)=sup⁡f∈F∩sDf∗∣1N∑iεiξi(f−f∗)(Xi)∣\phi_N(s)=\sup_{f\in F\cap sD_{f^*}}\bigl|\tfrac1{\sqrt N}\sum_i\varepsilon_i\xi_i(f-f^*)(X_i)\bigr|ϕN​(s)=supf∈F∩sDf∗​​​N​1​∑i​εi​ξi​(f−f∗)(Xi​)​ with ξi=f∗(Xi)−Yi\xi_i=f^*(X_i)-Y_iξi​=f∗(Xi​)−Yi​, and the noise parameter is
αN∗(γ,δ)=inf⁡{s>0:Pr⁡(ϕN(s)≤γs2N)≥1−δ}.\alpha^*_N(\gamma,\delta)=\inf\bigl\{s>0:\Pr(\phi_N(s)\le\gamma s^2\sqrt N)\ge1-\delta\bigr\}.αN∗​(γ,δ)=inf{s>0:Pr(ϕN​(s)≤γs2N​)≥1−δ}.
  • For the proof (§5), βN(H,γ)=inf⁡{r>0:Esup⁡h∈H∩rD∣1N∑iεih(Xi)∣≤γr}\beta_N(H,\gamma)=\inf\{r>0:\mathbb E\sup_{h\in H\cap rD}|\frac1N\sum_i\varepsilon_ih(X_i)|\le\gamma r\}βN​(H,γ)=inf{r>0:Esuph∈H∩rD​∣N1​∑i​εi​h(Xi​)∣≤γr}, with DDD the unit ball of L2(μ)L_2(\mu)L2​(μ), and HHH is star-shaped around 0 if λh∈H\lambda h\in Hλh∈H for all h∈Hh\in Hh∈H, 0<λ≤10<\lambda\le10<λ≤1.

Formalization targets

Goal: Theorem 3.1

Fix τ>0\tau>0τ>0 with QF−F(2τ)>0Q_{F-F}(2\tau)>0QF−F​(2τ)>0 and γ<τ2QF−F(2τ)/16\gamma<\tau^2Q_{F-F}(2\tau)/16γ<τ2QF−F​(2τ)/16. For every 0<δ<10<\delta<10<δ<1, with probability at least 1−δ−exp⁡(−NQF−F2(2τ)/2)1-\delta-\exp(-NQ^2_{F-F}(2\tau)/2)1−δ−exp(−NQF−F2​(2τ)/2), every empirical minimizer satisfies

∥f^−f∗∥L2≤2max⁡{αN∗(γ,δ/4), βN∗(τQF−F(2τ)16)}.\|\hat f-f^*\|_{L_2}\le2\max\Bigl\{\alpha^*_N(\gamma,\delta/4),\ \beta^*_N\Bigl(\frac{\tau Q_{F-F}(2\tau)}{16}\Bigr)\Bigr\}.∥f^​−f∗∥L2​​≤2max{αN∗​(γ,δ/4), βN∗​(16τQF−F​(2τ)​)}.

The joint law, the class and the target are arbitrary subject to the hypotheses above; no boundedness, moment or tail condition beyond L2L_2L2​ is imposed.

Milestones

In attack order:

  1. Localization for a star-shaped class (§5, p. 20): r>βN(H,γ)r>\beta_N(H,\gamma)r>βN​(H,γ) implies Esup⁡h∈H∩rD∣1N∑iεih(Xi)∣≤γr\mathbb E\sup_{h\in H\cap rD}|\frac1N\sum_i\varepsilon_ih(X_i)|\le\gamma rEsuph∈H∩rD​∣N1​∑i​εi​h(Xi​)∣≤γr.
  2. βN∗(γ)=βN(F−f∗,γ)\beta^*_N(\gamma)=\beta_N(F-f^*,\gamma)βN∗​(γ)=βN​(F−f∗,γ) (§5, p. 20).
  3. Theorem 5.4 (p. 21), the uniform empirical small-ball estimate: for HHH in the unit sphere of L2(μ)L_2(\mu)L2​(μ), if Esup⁡h∈H∣1N∑iεih(Xi)∣≤τQH(2τ)/16\mathbb E\sup_{h\in H}|\frac1N\sum_i\varepsilon_ih(X_i)|\le\tau Q_H(2\tau)/16Esuph∈H​∣N1​∑i​εi​h(Xi​)∣≤τQH​(2τ)/16, then with probability at least 1−2exp⁡(−NQH2(2τ)/2)1-2\exp(-NQ_H^2(2\tau)/2)1−2exp(−NQH2​(2τ)/2), inf⁡h∈H∣{i:∣h(Xi)∣≥τ}∣≥NQH(2τ)/4\inf_{h\in H}|\{i:|h(X_i)|\ge\tau\}|\ge NQ_H(2\tau)/4infh∈H​∣{i:∣h(Xi​)∣≥τ}∣≥NQH​(2τ)/4.
  4. Corollary 5.5 (p. 22): the same estimate, ∣{i:∣h(Xi)∣≥τ∥h∥L2}∣≥NQH(2τ)/4|\{i:|h(X_i)|\ge\tau\|h\|_{L_2}\}|\ge NQ_H(2\tau)/4∣{i:∣h(Xi​)∣≥τ∥h∥L2​​}∣≥NQH​(2τ)/4, for every hhh of a star-shaped class with ∥h∥L2≥r>βN(H,τQH(2τ)/16)\|h\|_{L_2}\ge r>\beta_N(H,\tau Q_H(2\tau)/16)∥h∥L2​​≥r>βN​(H,τQH​(2τ)/16).
  5. F−f∗F-f^*F−f∗ is star-shaped when FFF is convex (proof of Theorem 5.3, p. 23).
  6. Theorem 5.3 (p. 21): estimate (5.1) for H=F−f∗H=F-f^*H=F−f∗.
  7. The projection inequality Eξ(f−f∗)(X)≥0\mathbb E\xi(f-f^*)(X)\ge0Eξ(f−f∗)(X)≥0 for f∈Ff\in Ff∈F (§5, p. 23).
  8. Display (5.3) (p. 23): with probability at least 1−2exp⁡(−NQF−F2(2τ)/2)1-2\exp(-NQ^2_{F-F}(2\tau)/2)1−2exp(−NQF−F2​(2τ)/2),
1N∑i=1N(f−f∗)2(Xi)≥τ24QF−F(2τ)∥f−f∗∥L22\frac1N\sum_{i=1}^N(f-f^*)^2(X_i)\ge\frac{\tau^2}4Q_{F-F}(2\tau)\|f-f^*\|^2_{L_2}N1​i=1∑N​(f−f∗)2(Xi​)≥4τ2​QF−F​(2τ)∥f−f∗∥L2​2​

for all f∈Ff\in Ff∈F with ∥f−f∗∥L2≥r\|f-f^*\|_{L_2}\ge r∥f−f∗∥L2​​≥r. 9. Display (5.5) (p. 24): a bound 4γα24\gamma\alpha^24γα2 on ∣PNξ(f−f∗)−Eξ(f−f∗)∣|P_N\xi(f-f^*)-\mathbb E\xi(f-f^*)|∣PN​ξ(f−f∗)−Eξ(f−f∗)∣ on the sphere ∥f−f∗∥L2=α\|f-f^*\|_{L_2}=\alpha∥f−f∗∥L2​​=α extends to 4γ∥f−f∗∥L224\gamma\|f-f^*\|^2_{L_2}4γ∥f−f∗∥L2​2​ outside it (deterministic).

Significance

Theorem 3.1 separates the error of ERM into a "low-noise" term βN∗\beta^*_NβN∗​, which depends on the class only and matches the realizable rate, and a "high-noise" term αN∗\alpha^*_NαN∗​, which depends on how the class correlates with the actual noise. Both are computable for heavy-tailed classes: the paper derives from it sharp rates for linear regression with heavy-tailed design and for the persistence problem in ℓ1n\ell_1^nℓ1n​ (§4). The small-ball lower bound (Theorem 5.4 and (5.3)) is reusable on its own: it gives lower isometry estimates for random matrices with heavy-tailed rows (the setting of Koltchinskii–Mendelson).

The result is proved in the paper. As far as is known, none of it has been machine-checked: there is no formal statement of Theorem 3.1, of the small-ball estimate, or of the localized parameters αN∗,βN∗\alpha^*_N,\beta^*_NαN∗​,βN∗​ in Lean. The mission produces the first formal statements of these objects, and a formal proof would also check the constants of the printed argument.

Difficulty

The obvious approach, a uniform law of large numbers for the squared loss over FFF, fails: without concentration, 1N∑i(f−f∗)2(Xi)\frac1N\sum_i(f-f^*)^2(X_i)N1​∑i​(f−f∗)2(Xi​) need not be close to ∥f−f∗∥L22\|f-f^*\|^2_{L_2}∥f−f∗∥L2​2​ uniformly, and an upper estimate is unavailable. The proof needs only a one-sided lower estimate, and the difficulty is to obtain it uniformly over an infinite, unbounded class from the small-ball condition alone, with a probability that is exponential in NNN. A second difficulty is the multiplier term 1N∑iξi(f−f∗)(Xi)\frac1N\sum_i\xi_i(f-f^*)(X_i)N1​∑i​ξi​(f−f∗)(Xi​), where the noise ξ\xiξ may be heavy-tailed and dependent on XXX; it must be controlled through the random-sign process defining αN∗\alpha^*_NαN∗​, not through a bound on ξ\xiξ. The standard tools involved (bounded differences, symmetrization, contraction for Bernoulli processes) are not in Mathlib.

Formalization scope

All objects live in one definitions file, LearnNoConc.ERM.Setting. The conventions are:

  • The data are a joint law ν on Ω × ℝ; the law of XXX is ν.map Prod.fst. The sample is a point of Fin N → Ω × ℝ under Measure.pi; N≥1N\ge1N≥1 is assumed.
  • ∥⋅∥L2\|\cdot\|_{L_2}∥⋅∥L2​​ is eLpNorm · 2 μ, valued in [0,∞][0,\infty][0,∞]. The expectation over random signs is the average over all 2N2^N2N sign vectors.
  • Suprema and expectations of suprema are taken in [0,∞][0,\infty][0,∞] (⨆, ‖·‖ₑ, lower Lebesgue integral), and αN∗,βN∗,βN\alpha^*_N,\beta^*_N,\beta_NαN∗​,βN∗​,βN​ are [0,∞][0,\infty][0,∞]-valued infima, so an empty set of admissible radii gives +∞+\infty+∞ and a vacuous bound, as on the page. Defining inequalities are compared in the extended reals.
  • "With probability at least 1−p1-p1−p, AAA" is stated as "the outer probability of the complement of AAA is at most ppp".
  • The goal quantifies over every empirical minimizer, and f∗f^*f∗ is any minimizer of the risk over FFF.
  • Added, disclosed hypotheses: EY2<∞\mathbb EY^2<\inftyEY2<∞; every f∈Ff\in Ff∈F measurable; and pointwise separability of FFF (a countable subclass approximating every element pointwise and in L2L_2L2​), which stands in for the measurability of suprema the paper takes for granted. Without it the lower integral of a non-measurable supremum would make βN∗\beta^*_NβN∗​ smaller and the goal stronger than the paper.

A formalization in which an infimum over an empty set is 000, a supremum or an integral of a non-integrable function is truncated to 000, f∗f^*f∗ is an arbitrary element of FFF, or f^\hat ff^​ is one chosen minimizer would trivialize or change the statement; all of these are ruled out above.

A complete development needs McDiarmid's bounded differences inequality, Giné–Zinn symmetrization (in expectation and in probability), the Ledoux–Talagrand contraction inequality for Bernoulli processes, and the measurability theory of suprema over separable classes. These are reusable well beyond this mission, and contributions of any of them are welcome, as are proofs of the milestones independently of the goal.

Selected references

  • S. Mendelson, Learning without Concentration, J. ACM 62(3), Article 21, 2015. Preprint arXiv:1401.0304v2 (the version cited here). https://arxiv.org/abs/1401.0304, https://doi.org/10.1145/2699439
  • V. Koltchinskii, S. Mendelson, Bounding the smallest singular value of a random matrix without concentration, preprint, 2013. https://arxiv.org/abs/1312.3580
  • G. Lecué, S. Mendelson, Learning subgaussian classes: Upper and minimax bounds, preprint, 2013. https://arxiv.org/abs/1305.4825
  • A. W. van der Vaart, J. A. Wellner, Weak Convergence and Empirical Processes, Springer, 1996, §2.3.3 (pointwise separable classes). https://doi.org/10.1007/978-1-4757-2545-2
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AnalysisProbabilityStochastic Systems·Captain: mikedeng1

Affine Volterra Processes 3: Global Solutions with Nonpositive Real Part of the Square-Root Riccati–Volterra EquationResearch Paper

Motivation

The Volterra square-root model describes a nonnegative, time-dependent state whose present value depends on a weighted history. Ordinary square-root diffusions use a constant kernel and have a Markov state; replacing that kernel by a function of elapsed time allows persistent or singular memory. This matters for the transform formulas used to characterize distributions of such processes. Those formulas depend on a deterministic nonlinear integral equation, and require a solution that exists at every finite time. Abi Jaber, Larsson and Pulido isolate that requirement in Lemma 6.3 of Affine Volterra processes, arXiv:1708.08796v3 (2019).

The paper's Section 6 treats processes in the nonnegative orthant and its Section 7 specializes the framework to a Volterra Heston model. The present mission concerns the deterministic equation behind the Section 6 transform. The stochastic existence theorem and the transform identity are separate results in the same paper. Keeping this mission on the integral equation makes its analytic content usable independently of a chosen probability space.

Setting

Fix a finite coordinate set of size ddd. A diagonal kernel consists of real functions Ki(t)K_i(t)Ki​(t) for t≥0t\ge0t≥0, with the iii-th entry of the matrix kernel equal to KiK_iKi​ and all off-diagonal entries zero. A resolvent of the first kind for KiK_iKi​ is a nonnegative measure LiL_iLi​ for which the convolution Ki∗LiK_i*L_iKi​∗Li​ equals one at positive times. The relevant regularity condition, labeled (2.5), requires local square integrability and positive-time translation bounds of order hγih^{\gamma_i}hγi​ for some γi∈(0,2]\gamma_i\in(0,2]γi​∈(0,2]. Condition (3.4) requires a kernel to be nonnegative, nonzero, nonincreasing and continuous at positive times. It also requires its resolvent measure to have decreasing interval masses Li([s,s+t])L_i([s,s+t])Li​([s,s+t]) as sss increases. Each shifted function ΔhKi(t)=Ki(t+h)\Delta_hK_i(t)=K_i(t+h)Δh​Ki​(t)=Ki​(t+h) must satisfy (3.4) for 0≤h≤10\le h\le10≤h≤1, with its own resolvent. These are the assumptions of Theorem 6.1 and hence of its Lemma 6.3 (pp. 6, 14, 28–29).

Let u=(ui)u=(u_i)u=(ui​) be a complex row vector and let f(t)=(fi(t))f(t)=(f_i(t))f(t)=(fi​(t)) be a locally integrable complex row function. Let BBB be a real matrix whose off-diagonal entries are nonnegative, and let σi>0\sigma_i>0σi​>0. The iii-th square-root Riccati–Volterra equation is

ψi(t)=uiKi(t)+∫0tKi(t−s)(fi(s)+∑jψj(s)Bji+σi22ψi(s)2) ds.\psi_i(t)=u_iK_i(t)+\int_0^t K_i(t-s)\left(f_i(s)+\sum_j\psi_j(s)B_{ji}+\frac{\sigma_i^2}{2}\psi_i(s)^2\right)\,ds.ψi​(t)=ui​Ki​(t)+∫0t​Ki​(t−s)(fi​(s)+j∑​ψj​(s)Bji​+2σi2​​ψi​(s)2)ds.

The index BjiB_{ji}Bji​ selects column iii: in the paper's notation B=(b1  ⋯  bd)B=(b^1\;\cdots\;b^d)B=(b1⋯bd) and the coupling is ψ(s)bi\psi(s)b^iψ(s)bi. The kernel acts only on the iii-th equation, while BBB couples the coordinates. The coefficient b0b^0b0 from the stochastic process does not enter this equation (equation (6.3), p. 27).

Formalization targets

The goal is the global existence, uniqueness and sign statement of Lemma 6.3. If Re⁡ui≤0\operatorname{Re}u_i\le0Reui​≤0 and Re⁡fi≤0\operatorname{Re}f_i\le0Refi​≤0, then

∃! ψ∈Lloc2(R+,Cd)solving (6.3) globally, withRe⁡ψi≤0for every i.\exists!\,\psi\in L^2_{\mathrm{loc}}(\mathbb R_+,\mathbb C^d) \quad\text{solving (6.3) globally, with}\quad \operatorname{Re}\psi_i\le0\quad\text{for every }i.∃!ψ∈Lloc2​(R+​,Cd)solving (6.3) globally, withReψi​≤0for every i.

For functions defined only up to null sets, the equation, uniqueness and sign conclusion are understood almost everywhere. The goal has no fixed time horizon and no hard-coded kernel: it covers every diagonal kernel satisfying the paper's conditions. The five milestones record the source's analytic support: the shifted resolvent bounds (3.9)–(3.10), the L2L^2L2 stability lemma C.1, maximal-solution Theorem B.1, global-solution Corollary B.3 and nonnegative-orthant invariance Theorem C.2. Their statements and locations are recorded in the milestone list.

Significance

Global solvability makes the square-root transform equation meaningful at any finite horizon. Uniqueness fixes the transform parameter determined by a kernel and forcing function. The nonpositive real part is the sign property needed in the paper's subsequent exponential-affine transform argument for nonnegative states (Theorem 6.1(ii), pp. 28–29). Without a global solution, that argument would only address a time interval before a possible blow-up.

The result is proved in the cited paper; this mission asks for a machine-checked development of that known theorem and its supporting integral-equation results. Its reusable output includes an L2L^2L2 notion of Volterra solution, the first-kind resolvent hypotheses, maximal lifetime, stability under changes of forcing and kernel, and a comparison statement for diagonal systems. The goal and milestones are presently proof obligations, not claims of existing machine-checked proofs.

Difficulty

Local solvability alone does not control the quadratic term ψi2\psi_i^2ψi2​ for arbitrarily large time. In particular, a generic local fixed-point theorem can yield a maximal solution whose L2L^2L2 norm diverges at a finite horizon. Sign information for the real part is also coupled to the imaginary part through that quadratic term; checking each coordinate independently does not establish invariance of the nonpositive half-plane. The analysis has to preserve the kernel's first-kind resolvent conditions and the off-diagonal sign pattern of BBB across the coupled system. Singular kernels allowed by (2.5) prevent replacing the problem with a standard ordinary differential equation.

Formalization scope

Time is represented by real numbers and every local LpL^pLp condition is restricted to positive bounded intervals. Vectors are functions on Fin d; matrix LpL^pLp membership is componentwise. These finite-dimensional norms are equivalent to the Euclidean and operator norms used in the paper. The kernel regularity estimates are Big-O statements as hhh tends to zero through positive values. A first-kind resolvent is a nonnegative measure supported on nonnegative times, with the convolution identity and interval-mass monotonicity stated directly. The convolution at positive time is an interval integral; the bound at zero in (3.10) uses the integral on [0,0][0,0][0,0], while the source describes a right-continuous extension when available.

Solutions are locally square integrable and satisfy their equations almost everywhere. The integrability of each asserted convolution is part of the solution predicate, so the default zero value of a nonintegrable Lean integral cannot create a spurious solution. A maximal lifetime is extended-nonnegative-real valued, allowing infinity, and a finite lifetime requires an infinite extended L2L^2L2 norm. Sign conditions on locally integrable forcing and on the solution are almost everywhere. Measurable time dependence of the nonlinear drift is made explicit for Theorem B.1 and Corollary B.3, where it is necessary to interpret their integrals. The condition b0≥0b^0\ge0b0≥0 of the square-root process is omitted from the goal because b0b^0b0 is absent from (6.3).

The development needs Mathlib's Bochner integrals, local LpL^pLp predicates, measures, complex arithmetic and asymptotic filters. Proof contributions to the five source milestones and the goal are welcome, including infrastructure for nonconvolution Volterra resolvents where the paper cites earlier literature. The formalization must keep the coefficient σi2/2\sigma_i^2/2σi2​/2, the column index BjiB_{ji}Bji​, and every shift h∈[0,1]h\in[0,1]h∈[0,1].

Selected references

  • E. Abi Jaber, M. Larsson and S. Pulido, Affine Volterra processes, arXiv:1708.08796v3, 2019. Preprint.
  • G. Gripenberg, S.-O. Londen and O. Staffans, Volterra Integral and Functional Equations, Cambridge University Press, 1990. DOI.
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Functional AnalysisMachine LearningProbability+1·Captain: mikedeng1

Generalization Properties of Learning with Random Features: Ridge Regression with c₀√n·log(108κ²√n/δ) Random Features Has Excess Risk at Most c₁·log²(18/δ)/√n with Probability 1 − δResearch Paper

Motivation

Kernel ridge regression is a standard nonparametric estimator with optimal statistical guarantees, but it needs the n×nn\times nn×n kernel matrix of the data: roughly O(n3)O(n^3)O(n3) time and O(n2)O(n^2)O(n2) memory. Random features (Rahimi and Recht, NeurIPS 2007) replace the kernel by an average over MMM randomly sampled feature functions, turning the problem into ridge regression in dimension MMM, at cost O(nM2)O(nM^2)O(nM2) time and O(nM)O(nM)O(nM) memory. The question is how many features are needed before the statistical accuracy of the exact kernel method is lost.

The first statistical analysis of a random-features estimator (Rahimi and Recht, NeurIPS 2009), for Lipschitz losses over a ball of fixed radius, needs O(n)O(n)O(n) features to reach an O(1/n)O(1/\sqrt n)O(1/n​) bound. Rudi and Rosasco (arXiv:1602.04474, NeurIPS 2017) showed that MMM of order nlog⁡n\sqrt n\log nn​logn features already give the O(1/n)O(1/\sqrt n)O(1/n​) excess risk that exact kernel ridge regression attains with regularization λ=n−1/2\lambda=n^{-1/2}λ=n−1/2 (Caponnetto and De Vito 2007), assuming only that the best predictor in the reproducing kernel Hilbert space exists.

Setting

Let XXX be a separable input space and (Ω,π)(\Omega,\pi)(Ω,π) a probability space. A random feature is a function ψ:X×Ω→R\psi:X\times\Omega\to\mathbb Rψ:X×Ω→R, continuous in both variables with ∣ψ(x,ω)∣≤κ|\psi(x,\omega)|\le\kappa∣ψ(x,ω)∣≤κ for some κ≥1\kappa\ge1κ≥1. It defines the kernel

K(x,x′)=∫Ωψ(x,ω)ψ(x′,ω) dπ(ω),K(x,x')=\int_\Omega\psi(x,\omega)\psi(x',\omega)\,d\pi(\omega),K(x,x′)=∫Ω​ψ(x,ω)ψ(x′,ω)dπ(ω),

whose reproducing kernel Hilbert space is H\mathcal HH. Data (x1,y1),…,(xn,yn)(x_1,y_1),\dots,(x_n,y_n)(x1​,y1​),…,(xn​,yn​) are drawn i.i.d. from a probability ρ\rhoρ on X×RX\times\mathbb RX×R with ∣y∣≤b|y|\le b∣y∣≤b almost surely, b>0b>0b>0. The expected risk is E(f)=∫(f(x)−y)2 dρ(x,y)\mathcal E(f)=\int(f(x)-y)^2\,d\rho(x,y)E(f)=∫(f(x)−y)2dρ(x,y), and fH∈Hf_{\mathcal H}\in\mathcal HfH​∈H is a minimizer of E\mathcal EE over H\mathcal HH, assumed to exist.

Given features ω1,…,ωM\omega_1,\dots,\omega_Mω1​,…,ωM​ drawn i.i.d. from π\piπ, independently of the data, the feature map is ϕM(x)=M−1/2(ψ(x,ω1),…,ψ(x,ωM))\phi_M(x)=M^{-1/2}(\psi(x,\omega_1),\dots,\psi(x,\omega_M))ϕM​(x)=M−1/2(ψ(x,ω1​),…,ψ(x,ωM​)). With C^M=1n∑iϕM(xi)ϕM(xi)⊤\widehat C_M=\frac1n\sum_i\phi_M(x_i)\phi_M(x_i)^\topCM​=n1​∑i​ϕM​(xi​)ϕM​(xi​)⊤ and S^M⊤y^=1n∑iyiϕM(xi)\widehat S_M^\top\widehat y=\frac1n\sum_iy_i\phi_M(x_i)SM⊤​y​=n1​∑i​yi​ϕM​(xi​), the random-features ridge estimator with parameter λ>0\lambda>0λ>0 is

f^λ,M(x)=ϕM(x)⊤w^λ,M,w^λ,M=(C^M+λI)−1S^M⊤y^.\widehat f_{\lambda,M}(x)=\phi_M(x)^\top\widehat w_{\lambda,M},\qquad\widehat w_{\lambda,M}=(\widehat C_M+\lambda I)^{-1}\widehat S_M^\top\widehat y .f​λ,M​(x)=ϕM​(x)⊤wλ,M​,wλ,M​=(CM​+λI)−1SM⊤​y​.

In the Lean development these are kernelOf, featureMap, empCov, empCross, rfWeights, rfEstimator and risk in the namespace RFRidge.Basic.

Formalization targets

Goal: Theorem 1

There are constants c0,c1>0c_0,c_1>0c0​,c1​>0, independent of nnn, λ\lambdaλ and δ\deltaδ, and a threshold n0n_0n0​ such that for every δ∈(0,1]\delta\in(0,1]δ∈(0,1] and n≥n0n\ge n_0n≥n0​, with λn=n−1/2\lambda_n=n^{-1/2}λn​=n−1/2 and

Mn=c0n log⁡108κ2nδM_n=c_0\sqrt n\,\log\frac{108\kappa^2\sqrt n}{\delta}Mn​=c0​n​logδ108κ2n​​

features, with probability at least 1−δ1-\delta1−δ over the data and the features,

E(f^λn,Mn)−E(fH)≤c1log⁡218δn.\mathcal E(\widehat f_{\lambda_n,M_n})-\mathcal E(f_{\mathcal H})\le\frac{c_1\log^2\frac{18}{\delta}}{\sqrt n}.E(f​λn​,Mn​​)−E(fH​)≤n​c1​log2δ18​​.

The constants are existential: the paper prints them without values, and the values in its appendix are not established by the printed proof. The goal therefore asserts the shape of the bound, which survives any later improvement of the constants.

Milestones

The proof goes through an analytic decomposition of the excess risk on L2(X,ρX)L^2(X,\rho_X)L2(X,ρX​) followed by concentration. The milestones are the results of that proof that are stated as printed:

  1. Lemma 1: the integral operator LLL of KKK equals ∫ψω⊗ψω dπ(ω)\int\psi_\omega\otimes\psi_\omega\,d\pi(\omega)∫ψω​⊗ψω​dπ(ω).
  2. Lemma 2: the component of the regression function orthogonal to the range of LLL is invisible to every random-features predictor, almost surely.
  3. Proposition 4 (Cordes), Proposition 9 (interpolation ∥XAσ∥≤∥X∥1−σ∥XA∥σ\|XA^\sigma\|\le\|X\|^{1-\sigma}\|XA\|^\sigma∥XAσ∥≤∥X∥1−σ∥XA∥σ) and Proposition 8 (a multiplicative bound between regularized operators).
  4. Lemma 5: the bound on the approximation error under the source condition Pfρ=LrgPf_\rho=L^rgPfρ​=Lrg. Lemmas 3 and 4 remain draft items, but are omitted from the milestone list because the PDF text layer corrupts their displayed equations and the mechanical verbatim checker rejects the exact visual transcription.
  5. Propositions 1 and 2: Bernstein inequalities for real random variables and for random vectors in a Hilbert space.

Significance

Theorem 1 shows that, in the basic setting, random features reduce the cost of kernel ridge regression from O(n3)O(n^3)O(n3) time and O(n2)O(n^2)O(n2) memory to O(n2)O(n^2)O(n2) and O(nn)O(n\sqrt n)O(nn​) without losing the minimax-optimal O(1/n)O(1/\sqrt n)O(1/n​) rate. It is the reference result on the statistical cost of random-features approximations, and the same decomposition yields the paper's faster rates under source and capacity conditions (Theorems 2 and 3) and the analysis of data-dependent feature sampling.

To the best of the mission's knowledge, none of these results has a machine-checked proof. Formalizing them requires real infrastructure: integral operators on L2L^2L2 defined by a kernel with an integral representation, operator inequalities for the continuous functional calculus, and Bernstein inequalities in Hilbert spaces. The Bernstein inequalities and the operator inequalities (Cordes, interpolation, Proposition 8) are reusable well beyond this paper.

Difficulty

The obvious argument controls sup⁡x,x′∣KM(x,x′)−K(x,x′)∣\sup_{x,x'}|K_M(x,x')-K(x,x')|supx,x′​∣KM​(x,x′)−K(x,x′)∣ uniformly and transfers it to the estimator. It needs MMM of order nnn to keep the O(1/n)O(1/\sqrt n)O(1/n​) rate, because a uniform kernel approximation ignores that the estimator only probes KKK through a regularized operator. Getting nlog⁡n\sqrt n\log nn​logn features requires comparing the integral operators LLL and LML_MLM​ relative to L+λIL+\lambda IL+λI, in the operator norm weighted by (L+λI)−1/2(L+\lambda I)^{-1/2}(L+λI)−1/2, and this needs fractional powers of operators, operator monotonicity and concentration of random operators. A second subtlety is that the regression function need not lie in the closure of H\mathcal HH; Lemma 2 shows that the orthogonal component does not affect any random-features estimator.

Formalization scope

All models are posed in Lean 4 with Mathlib. The input space is a separable topological space with its Borel σ-algebra, the feature space Ω\OmegaΩ is the type W, and ψ\psiψ is jointly continuous, jointly measurable for the product σ-algebra (an added hypothesis: without second countability it does not follow from continuity), and bounded by κ≥1\kappa\ge1κ≥1 everywhere. The RKHS is Mathlib's RKHS ℝ H X ℝ, tied to the kernel by RKHS.kernel H x x' 1 = K x x'. Samples and features are indexed from 000; the nnn samples and MnM_nMn​ features have the product law ρ⊗n⊗π⊗Mn\rho^{\otimes n}\otimes\pi^{\otimes M_n}ρ⊗n⊗π⊗Mn​, and MnM_nMn​ is rounded up. "With probability at least 1−δ1-\delta1−δ" is "the failure event has probability at most δ\deltaδ", with δ∈(0,1]\delta\in(0,1]δ∈(0,1] and n≥1n\ge1n≥1.

Operators: the paper's Hilbert spaces are real, but Mathlib's continuous functional calculus for bounded operators, which defines AsA^sAs and (A+λI)−1/2(A+\lambda I)^{-1/2}(A+λI)−1/2, exists only on complex Hilbert spaces. The operator milestones are therefore posed on complex Hilbert spaces, and every inverse or power is the functional calculus of an explicit real function; the real statements follow by complexification. Lemmas 3–5 are stated for abstract positive operators satisfying exactly the relations their proofs use, and add r≤1r\le1r≤1 (the range of Assumption 6), without which Lemma 5 is false. Proposition 8 states β<1\beta<1β<1 as a conclusion. Lemma 3 corrects a sign in the exponent of CM,λC_{M,\lambda}CM,λ​: its display prints −1/2-1/2−1/2 where its proof uses +1/2+1/2+1/2; the printed bound fails for scalar operators.

A trivializing formalization is ruled out: the goal mentions only the estimator, the risk and fHf_{\mathcal H}fH​, never the operators of the proof, and its constants c0,c1c_0,c_1c0​,c1​ are fixed before δ\deltaδ and nnn, so they cannot absorb log⁡2(18/δ)\log^2(18/\delta)log2(18/δ) or n\sqrt nn​.

Not included: Theorem 4 (the analytic decomposition), Propositions 5 and 7 (which need Hilbert–Schmidt norms and traces), Lemmas 6–10 and Theorems 5–7 of Appendix A.3–A.4. Contributions of these intermediate results, of a Lean theory of integral operators of kernels, and of Hilbert-space concentration inequalities are welcome.

Selected references

  • A. Rudi, L. Rosasco, Generalization Properties of Learning with Random Features, NeurIPS 2017; arXiv:1602.04474v5. https://arxiv.org/abs/1602.04474
  • A. Rahimi, B. Recht, Random Features for Large-Scale Kernel Machines, NeurIPS 2007. https://papers.nips.cc/paper/3182-random-features-for-large-scale-kernel-machines
  • A. Caponnetto, E. De Vito, Optimal Rates for the Regularized Least-Squares Algorithm, Foundations of Computational Mathematics 7, 2007. https://doi.org/10.1007/s10208-006-0196-8
  • A. Rahimi, B. Recht, Weighted Sums of Random Kitchen Sinks: Replacing Minimization with Randomization in Learning, NeurIPS 2008 (proceedings 2009). https://papers.nips.cc/paper/3495-weighted-sums-of-random-kitchen-sinks-replacing-minimization-with-randomization-in-learning
  • H. O. Cordes, Spectral Theory of Linear Differential Operators and Comparison Algebras, Cambridge University Press, 1987. https://doi.org/10.1017/CBO9780511662836
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Machine LearningOptimizationProbability·Captain: mikedeng1

Stochastic Model-Based Minimization of Weakly Convex Functions 3: The Projected Stochastic Subgradient Method Is an Approximate Descent Method on the Moreau Envelope for Any StepsizesResearch Paper

Motivation

The projected stochastic subgradient method minimizes an expected loss f(x)=Eξ∼P[f(x,ξ)]f(x) = \mathbb E_{\xi\sim P}[f(x,\xi)]f(x)=Eξ∼P​[f(x,ξ)] over a closed convex set XXX: it samples a data point, steps against a sampled subgradient, and projects back onto XXX. For convex fff its sample complexity has been known for decades, and for smooth nonconvex fff the stochastic gradient method needs O(ε−4)O(\varepsilon^{-4})O(ε−4) samples to reach gradient norm ε\varepsilonε (Ghadimi–Lan 2013). Many problems in statistical learning and signal processing are neither convex nor smooth — robust phase retrieval, nonlinear regression with an ℓ1\ell_1ℓ1​ loss, covariance estimation, conditional value-at-risk with smooth losses — but are weakly convex: they become convex after adding a quadratic ρ2∥x∥2\frac{\rho}{2}\|x\|^22ρ​∥x∥2.

Timeline. Nurminskii (1970s) showed that for weakly convex losses f(⋅,ξ)f(\cdot,\xi)f(⋅,ξ) and no constraint the stochastic subgradient method subsequentially converges to a stationary point almost surely, without a rate. Ghadimi and Lan (2013) proved the O(ε−4)O(\varepsilon^{-4})O(ε−4) rate for smooth fff. Davis and Drusvyatskiy (arXiv:1803.06523, SIAM J. Optim. 2019) proved the first rate for the plain projected stochastic subgradient method on weakly convex problems, measured by the gradient of the Moreau envelope, and for any nonnegative stepsizes. This is Theorem 3.1 of their paper and the goal of this mission.

Setting

Work in Rd\mathbb R^dRd with the Euclidean norm. Let X⊆RdX \subseteq \mathbb R^dX⊆Rd be nonempty, closed and convex, and let f:Rd→Rf : \mathbb R^d \to \mathbb Rf:Rd→R be ρ\rhoρ-weakly convex (ρ>0\rho > 0ρ>0): x↦f(x)+ρ2∥x∥2x \mapsto f(x) + \frac{\rho}{2}\|x\|^2x↦f(x)+2ρ​∥x∥2 is convex. The problem is

min⁡x∈Xf(x),i.e. min⁡xφ(x), φ=f+δX,\min_{x \in X} f(x), \qquad \text{i.e. } \min_x \varphi(x),\ \varphi = f + \delta_X,x∈Xmin​f(x),i.e. xmin​φ(x), φ=f+δX​,

where δX\delta_XδX​ is 000 on XXX and +∞+\infty+∞ off XXX.

The subdifferential ∂f(x)\partial f(x)∂f(x) is the set of vvv with f(y)≥f(x)+⟨v,y−x⟩+o(∥y−x∥)f(y) \ge f(x) + \langle v, y - x\rangle + o(\|y - x\|)f(y)≥f(x)+⟨v,y−x⟩+o(∥y−x∥) as y→xy \to xy→x. For λ>0\lambda > 0λ>0 the Moreau envelope and the proximal point of φ\varphiφ are

φλ(x)=min⁡y∈X{f(y)+12λ∥y−x∥2},prox⁡λφ(x)=argmin⁡y∈X{f(y)+12λ∥y−x∥2}.\varphi_\lambda(x) = \min_{y \in X}\Big\{f(y) + \tfrac{1}{2\lambda}\|y - x\|^2\Big\}, \qquad \operatorname{prox}_{\lambda\varphi}(x) = \operatorname*{argmin}_{y \in X}\Big\{f(y) + \tfrac{1}{2\lambda}\|y - x\|^2\Big\}.φλ​(x)=y∈Xmin​{f(y)+2λ1​∥y−x∥2},proxλφ​(x)=y∈Xargmin​{f(y)+2λ1​∥y−x∥2}.

Assumption A (stochastic subgradient oracle): on a probability space (Ω,F,P)(\Omega, \mathcal F, P)(Ω,F,P) one can draw i.i.d. samples ξ0,ξ1,⋯∼P\xi_0, \xi_1, \dots \sim Pξ0​,ξ1​,⋯∼P (A1); there are an open set U⊇XU \supseteq XU⊇X and a measurable map GGG with Eξ[G(x,ξ)]∈∂f(x)\mathbb E_\xi[G(x,\xi)] \in \partial f(x)Eξ​[G(x,ξ)]∈∂f(x) for all x∈Ux \in Ux∈U (A2); and Eξ∥G(x,ξ)∥2≤L2\mathbb E_\xi\|G(x,\xi)\|^2 \le L^2Eξ​∥G(x,ξ)∥2≤L2 for all x∈Xx \in Xx∈X (A3).

Algorithm 3.1 with r=δXr = \delta_Xr=δX​ starts at x0∈Xx_0 \in Xx0​∈X and, for t=0,…,Tt = 0, \dots, Tt=0,…,T, samples ξt\xi_tξt​ and sets xt+1=proj⁡X(xt−αtG(xt,ξt))x_{t+1} = \operatorname{proj}_X(x_t - \alpha_t G(x_t, \xi_t))xt+1​=projX​(xt​−αt​G(xt​,ξt​)) with stepsizes αt≥0\alpha_t \ge 0αt​≥0. It returns xt∗x_{t^*}xt∗​ with t∗t^*t∗ drawn from {0,…,T}\{0, \dots, T\}{0,…,T} with probability αt/∑iαi\alpha_t / \sum_i \alpha_iαt​/∑i​αi​.

Formalization targets

Goal: Theorem 3.1, (3.4) and (3.5)

For every ρˉ>ρ\bar\rho > \rhoρˉ​>ρ and any stepsizes αt≥0\alpha_t \ge 0αt​≥0 with ∑tαt>0\sum_t \alpha_t > 0∑t​αt​>0,

E[∥∇φ1/ρˉ(xt∗)∥2]≤ρˉρˉ−ρ⋅(φ1/ρˉ(x0)−min⁡φ)+ρˉL22∑t=0Tαt2∑t=0Tαt,\mathbb E\big[\|\nabla\varphi_{1/\bar\rho}(x_{t^*})\|^2\big] \le \frac{\bar\rho}{\bar\rho - \rho}\cdot\frac{\big(\varphi_{1/\bar\rho}(x_0) - \min\varphi\big) + \frac{\bar\rho L^2}{2}\sum_{t=0}^T\alpha_t^2}{\sum_{t=0}^T\alpha_t},E[∥∇φ1/ρˉ​​(xt∗​)∥2]≤ρˉ​−ρρˉ​​⋅∑t=0T​αt​(φ1/ρˉ​​(x0​)−minφ)+2ρˉ​L2​∑t=0T​αt2​​,

and with αt=γ/T+1\alpha_t = \gamma/\sqrt{T+1}αt​=γ/T+1​, γ>0\gamma > 0γ>0,

E[∥∇φ1/(2ρ)(xt∗)∥2]≤2⋅(φ1/(2ρ)(x0)−min⁡φ)+ρL2γ2γT+1.\mathbb E\big[\|\nabla\varphi_{1/(2\rho)}(x_{t^*})\|^2\big] \le 2\cdot\frac{\big(\varphi_{1/(2\rho)}(x_0) - \min\varphi\big) + \rho L^2\gamma^2}{\gamma\sqrt{T+1}}.E[∥∇φ1/(2ρ)​(xt∗​)∥2]≤2⋅γT+1​(φ1/(2ρ)​(x0​)−minφ)+ρL2γ2​.

Milestones

  1. Lemma 2.1 (p. 10): for a closed proper φ\varphiφ, weak convexity, the approximate secant inequality (2.4), the subgradient inequality (2.5) and hypomonotonicity of ∂φ\partial\varphi∂φ are equivalent.
  2. §3.1, display after (3.8) (pp. 13–14; the display starts on p. 13 and ends on p. 14): for x∈Xx \in Xx∈X and x^=prox⁡φ/ρˉ(x)\hat x = \operatorname{prox}_{\varphi/\bar\rho}(x)x^=proxφ/ρˉ​​(x), f(x)−f(x^)−ρ2∥x−x^∥2≥(ρˉ−ρ)∥x−x^∥2=ρˉ−ρρˉ2∥∇φ1/ρˉ(x)∥2f(x) - f(\hat x) - \frac{\rho}{2}\|x - \hat x\|^2 \ge (\bar\rho - \rho)\|x - \hat x\|^2 = \frac{\bar\rho - \rho}{\bar\rho^2}\|\nabla\varphi_{1/\bar\rho}(x)\|^2f(x)−f(x^)−2ρ​∥x−x^∥2≥(ρˉ​−ρ)∥x−x^∥2=ρˉ​2ρˉ​−ρ​∥∇φ1/ρˉ​​(x)∥2.
  3. Lemma 2.2 (p. 11): for λ∈(0,ρ−1)\lambda \in (0, \rho^{-1})λ∈(0,ρ−1) the envelope φλ\varphi_\lambdaφλ​ is C1C^1C1 with ∇φλ(x)=λ−1(x−prox⁡λφ(x))\nabla\varphi_\lambda(x) = \lambda^{-1}(x - \operatorname{prox}_{\lambda\varphi}(x))∇φλ​(x)=λ−1(x−proxλφ​(x)).
  4. Theorem 3.1, (3.3) (p. 13): the one-step estimate
E[φ1/ρˉ(xt+1)]≤E[φ1/ρˉ(xt)]−αt(ρˉ−ρ)ρˉE[∥∇φ1/ρˉ(xt)∥2]+αt2ρˉL22.\mathbb E\big[\varphi_{1/\bar\rho}(x_{t+1})\big] \le \mathbb E\big[\varphi_{1/\bar\rho}(x_t)\big] - \frac{\alpha_t(\bar\rho - \rho)}{\bar\rho}\mathbb E\big[\|\nabla\varphi_{1/\bar\rho}(x_t)\|^2\big] + \frac{\alpha_t^2\bar\rho L^2}{2}.E[φ1/ρˉ​​(xt+1​)]≤E[φ1/ρˉ​​(xt​)]−ρˉ​αt​(ρˉ​−ρ)​E[∥∇φ1/ρˉ​​(xt​)∥2]+2αt2​ρˉ​L2​.

Significance

The result. The gradient of the Moreau envelope is a near-stationarity measure: ∥∇φλ(x)∥\|\nabla\varphi_\lambda(x)\|∥∇φλ​(x)∥ small means that xxx is within λ∥∇φλ(x)∥\lambda\|\nabla\varphi_\lambda(x)\|λ∥∇φλ​(x)∥ of a point x^∈X\hat x \in Xx^∈X with f(x^)≤f(x)f(\hat x) \le f(x)f(x^)≤f(x) and dist⁡(0,∂φ(x^))≤∥∇φλ(x)∥\operatorname{dist}(0, \partial\varphi(\hat x)) \le \|\nabla\varphi_\lambda(x)\|dist(0,∂φ(x^))≤∥∇φλ​(x)∥. Theorem 3.1 therefore gives O(ε−4)O(\varepsilon^{-4})O(ε−4) sample complexity for finding nearly stationary points of nonsmooth nonconvex constrained stochastic problems, matching the smooth case. Estimate (3.3) shows that the Moreau envelope is an approximate Lyapunov function for the method, and it holds for arbitrary nonnegative stepsizes; Theorem 3.4 of the same paper (the proximal extension) needs αt≤1/ρˉ\alpha_t \le 1/\bar\rhoαt​≤1/ρˉ​ and a worse constant.

Formalizing it. The result is proved in the paper; no machine-checked version exists. A formalization requires the Fréchet subdifferential of extended-valued functions, the Moreau envelope and its smoothness under weak convexity (Lemma 2.2, which the paper cites as standard rather than proving), and a measure-theoretic treatment of the iterates of a stochastic algorithm on a product probability space. Lemma 2.1 and Lemma 2.2 are reused by the other missions of this series.

Difficulty

The obvious approach — show that f(xt)f(x_t)f(xt​) decreases in expectation — fails: without smoothness, a subgradient step can increase fff by an amount of order αt\alpha_tαt​, not αt2\alpha_t^2αt2​, and no stepsize repairs that. The argument instead tracks the Moreau envelope, which is smooth even though fff is not; the difficulty moves into (i) Lemma 2.2, the C1C^1C1-smoothness of the envelope of a weakly convex function, which is a nontrivial piece of variational analysis, and (ii) the conditional-expectation bookkeeping that turns a one-sample estimate into (3.3) along the random iterates, including the integrability of φ1/ρˉ(xt)\varphi_{1/\bar\rho}(x_t)φ1/ρˉ​​(xt​) and ∥∇φ1/ρˉ(xt)∥2\|\nabla\varphi_{1/\bar\rho}(x_t)\|^2∥∇φ1/ρˉ​​(xt​)∥2, which the paper does not discuss.

Formalization scope

  • Carrier and encoding. Rd\mathbb R^dRd is EuclideanSpace ℝ (Fin d). An extended-valued function is encoded by its domain and its real values on the domain; φ=f+δX\varphi = f + \delta_Xφ=f+δX​ is the pair (X,f)(X, f)(X,f), and φλ\varphi_\lambdaφλ​ is moreauEnv X f lam, a real infimum over XXX. Lemma 2.2 supplies the attainment and differentiability under which this infimum is the paper's envelope.
  • The projection is a function proj constrained by the published nearest-point predicate SpectralProjGrad.Shared.IsProjOnto X proj. It is not the proximal-point predicate of αtδX\alpha_t\delta_Xαt​δX​, so that αt=0\alpha_t = 0αt​=0 remains meaningful; zero stepsizes are allowed, as in Algorithm 3.1.
  • Randomness. T+1T+1T+1 i.i.d. samples are a point of ΩT+1\Omega^{T+1}ΩT+1 under the product measure; E[⋅(xt∗)]\mathbb E[\cdot(x_{t^*})]E[⋅(xt∗​)] is the α\alphaα-weighted average of E[⋅(xt)]\mathbb E[\cdot(x_t)]E[⋅(xt​)], exactly as the paper's proof identifies it. Every bounded expectation comes with an integrability conclusion, since a Bochner integral of a non-integrable function is 000.
  • Added hypotheses. ρ>0\rho > 0ρ>0 (implicit in φ1/(2ρ)\varphi_{1/(2\rho)}φ1/(2ρ)​ and in λ<ρ−1\lambda < \rho^{-1}λ<ρ−1 of Lemma 2.2); ∑tαt>0\sum_t\alpha_t > 0∑t​αt​>0 in (3.4) (needed for t∗t^*t∗); closedness and properness in Lemmas 2.1–2.2. min⁡φ\min\varphiminφ is any lower bound φ∗\varphi^*φ∗ of fff on XXX. The C2C^2C2 clause of Lemma 2.1 is not stated.
  • Erratum. The rearranged display before "Notice that the left-hand-side is precisely …" (p. 14) has an extra factor ρˉ\bar\rhoρˉ​ in its denominator; the statement (3.4), which the goal formalizes, is what the unfolded recursion gives.
  • Ruled out. A formalization with an unconstrained proj, a stochastic subgradient not tied to ∂f\partial f∂f by (A2), expectations without integrability, or min⁡φ\min\varphiminφ as a junk-valued infimum would be trivial or false; each is excluded by the statements' hypotheses and conclusions.
  • Not included. The complexity remarks (3.9)–(3.10) and the paragraph on improved complexity under convexity.

Proofs of any milestone are welcome; Lemma 2.2 and the product-measure bookkeeping for (3.3) are the reusable parts.

Selected references

  • D. Davis, D. Drusvyatskiy, Stochastic Model-Based Minimization of Weakly Convex Functions, SIAM J. Optim. 29(1), 2019; arXiv:1803.06523v3. https://arxiv.org/abs/1803.06523
  • S. Ghadimi, G. Lan, Stochastic First- and Zeroth-Order Methods for Nonconvex Stochastic Programming, SIAM J. Optim. 23(4), 2013. https://doi.org/10.1137/120880811
  • 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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Dynamic ProgrammingOperations ResearchOptimization·Captain: mikedeng1

Dynamic Type Matching: Under the Modified Monge Condition There Is an Optimal Matching Policy That Respects the Priority Relation ≻MsResearch Paper

Motivation

Many platforms match two sides of a market over time: ride-hailing platforms match riders with drivers, blood banks match donated units with patients, organ allocation matches donors with recipients, and retailers pool inventory across fulfilment centres to serve orders from several regions. Demand and supply arrive in several types (locations, blood groups, quality grades), the reward of a match depends on both types, and whatever is not matched today partly waits for tomorrow. A central operational question is which pairs to match first. Static versions of this question go back to the transportation problem and to Monge sequences: Hoffman (1963) characterized the cost matrices for which a fixed greedy order of the arcs solves a transportation problem.

Hu and Zhou (arXiv:1811.07048, published in Manufacturing & Service Operations Management 24(1), 2022) extend this to a stochastic, multi-period setting. They identify conditions on the rewards, the (weak) modified Monge conditions, under which an optimal dynamic policy matches a dominant pair before the neighbouring pairs it dominates. This mission formalizes their main structural result, Theorem 1, and the chain of results it rests on.

Setting

There are mmm demand types D={1,…,m}\mathcal D=\{1,\dots,m\}D={1,…,m}, nnn supply types S={1,…,n}\mathcal S=\{1,\dots,n\}S={1,…,n}, and TTT periods t=1,…,Tt=1,\dots,Tt=1,…,T. In period ttt the state is a pair of vectors (x,y)∈R+m×R+n(\mathbf x,\mathbf y)\in\mathbb R^m_+\times\mathbb R^n_+(x,y)∈R+m​×R+n​ of available demand and supply. The firm chooses a matching decision Q=(qij)∈Rm×n\mathbf Q=(q_{ij})\in\mathbb R^{m\times n}Q=(qij​)∈Rm×n, collecting the reward

Rt∘Q=∑i=1m∑j=1nrijtqij,\mathbf R^t\circ\mathbf Q=\sum_{i=1}^m\sum_{j=1}^n r^t_{ij}q_{ij},Rt∘Q=i=1∑m​j=1∑n​rijt​qij​,

where the rewards rijtr^t_{ij}rijt​ are arbitrary real numbers. The post-matching levels are ui=xi−∑jqiju_i=x_i-\sum_j q_{ij}ui​=xi​−∑j​qij​ and vj=yj−∑iqijv_j=y_j-\sum_i q_{ij}vj​=yj​−∑i​qij​, and Q\mathbf QQ is feasible if Q≥0\mathbf Q\ge0Q≥0, u≥0\mathbf u\ge0u≥0 and v≥0\mathbf v\ge0v≥0. A fraction α∈[0,1]\alpha\in[0,1]α∈[0,1] of unmatched demand and β∈[0,1]\beta\in[0,1]β∈[0,1] of unmatched supply carries over, and new random quantities (Dt+1,St+1)≥0(\mathbf D^{t+1},\mathbf S^{t+1})\ge0(Dt+1,St+1)≥0 arrive. The value function VtV_tVt​ is defined by the dynamic program

Vt(x,y)=max⁡Q feasibleHt(Q,x,y),Ht(Q,x,y)=Rt∘Q+E Vt+1(αu+Dt+1,βv+St+1),V_t(\mathbf x,\mathbf y)=\max_{\mathbf Q\ \text{feasible}}H_t(\mathbf Q,\mathbf x,\mathbf y),\qquad H_t(\mathbf Q,\mathbf x,\mathbf y)=\mathbf R^t\circ\mathbf Q+\mathbb E\,V_{t+1}(\alpha\mathbf u+\mathbf D^{t+1},\beta\mathbf v+\mathbf S^{t+1}),Vt​(x,y)=Q feasiblemax​Ht​(Q,x,y),Ht​(Q,x,y)=Rt∘Q+EVt+1​(αu+Dt+1,βv+St+1),

with VT+1≡0V_{T+1}\equiv0VT+1​≡0. A matching policy assigns a feasible decision Qt(x,y)\mathbf Q^t(\mathbf x,\mathbf y)Qt(x,y) to every period and state; it is optimal if each of these decisions maximizes HtH_tHt​.

Two neighbouring pairs are compared by the relation ≻M\succ_{\mathcal M}≻M​. For i′≠ii'\ne ii′=i, (i,j)≻M(i′,j)(i,j)\succ_{\mathcal M}(i',j)(i,j)≻M​(i′,j) means rijt>ri′jtr^t_{ij}>r^t_{i'j}rijt​>ri′jt​ for all ttt, and rijt−ri′jt≥α(rij′′t+1−ri′j′′t+1)r^t_{ij}-r^t_{i'j}\ge\alpha(r^{t+1}_{ij''}-r^{t+1}_{i'j''})rijt​−ri′jt​≥α(rij′′t+1​−ri′j′′t+1​) for all t≤T−1t\le T-1t≤T−1 and all j′′j''j′′; the relation (i,j)≻M(i,j′)(i,j)\succ_{\mathcal M}(i,j')(i,j)≻M​(i,j′) is defined symmetrically with β\betaβ. The modified Monge condition requires rijt+ri′j′t≥rij′t+ri′jtr^t_{ij}+r^t_{i'j'}\ge r^t_{ij'}+r^t_{i'j}rijt​+ri′j′t​≥rij′t​+ri′jt​ whenever (i,j)(i,j)(i,j) dominates both (i′,j)(i',j)(i′,j) and (i,j′)(i,j')(i,j′); the paper then writes ≻Ms\succ_{\mathcal M_s}≻Ms​​. For a pair (i,j)(i,j)(i,j), let aia_iai​ be the type-iii demand left after matching iii through all pairs that (i,j)(i,j)(i,j) does not dominate, and bjb_jbj​ the analogous supply residual. A decision respects ≻Ms\succ_{\mathcal M_s}≻Ms​​ if (i,j)≻(i′,j)(i,j)\succ(i',j)(i,j)≻(i′,j) implies qi′j=0q_{i'j}=0qi′j​=0 or ai=0a_i=0ai​=0, and (i,j)≻(i,j′)(i,j)\succ(i,j')(i,j)≻(i,j′) implies qij′=0q_{ij'}=0qij′​=0 or bj=0b_j=0bj​=0.

Formalization targets

Goal: Theorem 1 (p. 12)

Under the modified Monge condition there is a single policy PPP such that, for all 1≤t≤T1\le t\le T1≤t≤T and all x,y≥0\mathbf x,\mathbf y\ge0x,y≥0,

Pt(x,y) is optimalandPt(x,y) respects ≻Ms.P_t(\mathbf x,\mathbf y)\ \text{is optimal}\quad\text{and}\quad P_t(\mathbf x,\mathbf y)\ \text{respects}\ \succ_{\mathcal M_s}.Pt​(x,y) is optimalandPt​(x,y) respects ≻Ms​​.

Milestones

  • Proposition 1 (p. 10): VtV_tVt​ and HtH_tHt​ are continuous and concave, and an optimal policy exists.
  • Lemma A.1 (Online Appendix A, p. 1): shifting ε\varepsilonε units of demand from type iii to type i′i'i′ (or of supply from jjj to j′j'j′) changes VtV_tVt​ by at least −∑τ∑j′λj′τ(rij′τ−ri′j′τ)-\sum_\tau\sum_{j'}\lambda^\tau_{j'}(r^\tau_{ij'}-r^\tau_{i'j'})−∑τ​∑j′​λj′τ​(rij′τ​−ri′j′τ​) for some nonnegative multipliers with ∑τα−(τ−t)∑j′λj′τ≤ε\sum_\tau\alpha^{-(\tau-t)}\sum_{j'}\lambda^\tau_{j'}\le\varepsilon∑τ​α−(τ−t)∑j′​λj′τ​≤ε.
  • Lemma A.2 (p. 3): transferring matching quantity from a dominated pair to a dominant one weakly increases HtH_tHt​.
  • Theorem 2 (p. 28): without the Monge condition, some optimal policy weakly respects ≻M\succ_{\mathcal M}≻M​: qi′j=0q_{i'j}=0qi′j​=0 or ui=0u_i=0ui​=0, and qij′=0q_{ij'}=0qij′​=0 or vj=0v_j=0vj​=0.
  • Monge exchange (proof of Theorem 1, p. 4): the transfer Q+ε(eij+ei′j′−ei′j−eij′)\mathbf Q+\varepsilon(\mathbf e_{ij}+\mathbf e_{i'j'}-\mathbf e_{i'j}-\mathbf e_{ij'})Q+ε(eij​+ei′j′​−ei′j​−eij′​) stays feasible and weakly increases HtH_tHt​.
  • Properties (i)–(iii) imply compatibility (proof of Theorem 1, p. 5).

Significance

Theorem 1 replaces the search over all optimal policies, which are state-dependent and generally complex, by a priority structure: whenever (i,j)(i,j)(i,j) dominates a neighbour, the neighbour is matched only once the residual capacity of (i,j)(i,j)(i,j) is exhausted. The paper derives from it the optimality of greedy matching for "perfect" pairs (Proposition 2), the priority order for horizontal (distance-based) and vertical (quality-based) reward structures, and the match-down-to threshold structure of the optimal policy in those models. These results generalize inventory rationing and capacity allocation with upgrading.

The result is proved in the paper, but not completely: the limit argument in the printed proofs of Theorems 1 and 2 ("the quantity transferred converges to zero") is not justified, and Proposition 1 has no printed proof in this version. A machine-checked development would close these gaps and would provide a reusable finite-horizon model with continuous states, concave value functions and an exchange-argument toolkit. No part of this mission is known to be formalized.

Difficulty

The obvious argument starts from an optimal decision and repeatedly applies the transfers of Lemma A.2 and the Monge exchange. Each transfer preserves optimality, but nothing in the printed argument guarantees that the procedure terminates or that its limit has the required property: transfers of different kinds can undo each other's progress, and with equal rewards they can cycle forever. A complete proof has to select the right optimal decision without relying on such an iteration. Before that, the dynamic program itself needs care: the value function is a supremum of an expectation of the next value function, so continuity, concavity, measurability and integrability have to be established together by backward induction, and attainment of the maximum is needed for any optimal policy to exist. Lemma A.1 is a further backward induction in which the multipliers become random and must be averaged.

Formalization scope

The Lean development lives in the namespace DynTypeMatching.Priority. Types are Fin m and Fin n; states are Fin m → ℝ, Fin n → ℝ; decisions are Fin m → Fin n → ℝ. Periods are natural numbers with the paper's 1-based indexing, and Vt=0V_t=0Vt​=0 for t>Tt>Tt>T. A model Model m n carries TTT, the rewards, α\alphaα, β\betaβ and one arrival law per period on Rm×Rn\mathbb R^m\times\mathbb R^nRm×Rn. The paper permits exogenous correlation between periods; its recursion (1) uses per-period laws and does not specify a joint arrival process. The expectation in HtH_tHt​ is over the law of the arrivals entering period t+1t+1t+1.

Every result assumes Model.WellPosed: each arrival law is a probability measure, supported on the nonnegative orthant and integrable, and 0≤α,β≤10\le\alpha,\beta\le10≤α,β≤1. Integrability is not stated in the paper, but without it the expectation in (1) is undefined. The value function is a real supremum and the expectation a Bochner integral, so outside the nonnegative orthant, or for non-integrable integrands, Lean returns the junk value 0. All statements therefore quantify over nonnegative states and feasible decisions.

The following hypotheses are added relative to the page, and each is disclosed in the item where it occurs:

  • Definition 1(i) is strict, rijt>ri′jtr^t_{ij}>r^t_{i'j}rijt​>ri′jt​, and the neighbours are distinct. With the printed weak inequality, Theorems 1 and 2 are false. Take m=3m=3m=3, n=1n=1n=1, T=1T=1T=1, all rewards equal to 2, x=(0,1,1)\mathbf x=(0,1,1)x=(0,1,1), y=(1)\mathbf y=(1)y=(1). Then types 2 and 3 dominate each other, every optimal decision matches one unit, and no such decision respects the relation.
  • Definition 1(ii) is required only for t+1≤Tt+1\le Tt+1≤T, because rT+1r^{T+1}rT+1 is not part of the model.
  • Lemma A.1 assumes α>0\alpha>0α>0 in part (i) and β>0\beta>0β>0 in part (ii), because α−(τ−t)\alpha^{-(\tau-t)}α−(τ−t) is undefined at α=0\alpha=0α=0.
  • Lemma A.2 assumes that Q\mathbf QQ itself is feasible.

Several printed index slips are corrected: the doubled εeij\varepsilon\mathbf e_{ij}εeij​ in the Monge exchange, the index ranges in Lemma A.1, and "and" for "or" in the compatibility step.

An optimal decision is defined as a feasible maximizer of HtH_tHt​ over feasible decisions, not through the equation Vt=HtV_t=H_tVt​=Ht​. This rules out a trivializing reading of the goal: a decision that respects the relation but is not optimal (for instance Q=0\mathbf Q=0Q=0) does not satisfy it. The goal asserts one policy that is optimal and compatible at the same time.

A complete development needs measurable-function and Bochner-integral calculus on finite-dimensional spaces, concavity and continuity of parametric suprema over polytopes, and compactness arguments for attainment. The model and the exchange lemmas are reusable for later missions on this paper (greedy matching, horizontal and vertical models). Proofs of any milestone are welcome, and so are alternative proofs of the goal.

Selected references

  • Ming Hu, Yun Zhou, Dynamic Type Matching, arXiv:1811.07048v1, 2018; Manufacturing & Service Operations Management 24(1), 2022. https://arxiv.org/abs/1811.07048 · https://doi.org/10.1287/msom.2020.0952
  • Alan J. Hoffman, On simple linear programming problems, Convexity, Proc. Symposia in Pure Mathematics 7, AMS, 1963, 317–327. https://doi.org/10.1090/pspum/007/0157783
  • Rainer E. Burkard, Bettina Klinz, Rüdiger Rudolf, Perspectives of Monge properties in optimization, Discrete Applied Mathematics 70(2), 1996, 95–161. https://doi.org/10.1016/0166-218X(95)00103-X
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Markov ChainProbabilityStatistics·Captain: mikedeng1

Spectral Gaps for a Metropolis–Hastings Algorithm in Infinite Dimensions II: The pCN Algorithm Has a Wasserstein Spectral Gap Uniform in the Dimension When the Potential Is Locally LipschitzResearch Paper

Motivation

Bayesian inverse problems for functions — the initial condition of a PDE, a permeability field, a diffusion coefficient — lead to posterior measures μ\muμ on an infinite-dimensional Hilbert space HHH, given by a density exp⁡(−Φ)\exp(-\Phi)exp(−Φ) with respect to a Gaussian prior γ\gammaγ. In practice μ\muμ is sampled by Markov chain Monte Carlo on an mmm-dimensional discretisation μm\mu_mμm​, and the question that matters is whether the sampler's convergence rate survives the limit m→∞m\to\inftym→∞. For the standard random-walk Metropolis algorithm it does not (mission III of this series). The preconditioned Crank–Nicolson (pCN) algorithm, whose proposal preserves γ\gammaγ, was introduced to avoid this (Beskos, Roberts, Stuart and Voss 2008; Cotter, Roberts, Stuart and White 2013).

Hairer, Stuart and Vollmer (2014) prove that pCN has a Wasserstein spectral gap that is uniform in the dimension. Mission I of this series covers their result for globally Lipschitz potentials Φ\PhiΦ (Theorem 2.12). This mission covers Theorem 2.14, which needs only that Φ\PhiΦ be locally Lipschitz, with a local Lipschitz constant growing slower than any exponential. That class contains potentials of polynomial growth, which arise for nonlinear forward maps.

Setting

HHH is a separable real Hilbert space with a centred Gaussian measure γ\gammaγ, and (ei)i≥0(e_i)_{i\ge0}(ei​)i≥0​ is an orthonormal basis of eigenvectors of the covariance of γ\gammaγ. PmHP_mHPm​H is the span of e0,…,em−1e_0,\dots,e_{m-1}e0​,…,em−1​, and γm\gamma_mγm​ is the image of γ\gammaγ under the orthogonal projection onto PmHP_mHPm​H. For a potential Φ:H→R\Phi:H\to\mathbb RΦ:H→R the targets are

μ(dx)∝e−Φ(x)γ(dx),μm(dx)∝e−Φ(x)γm(dx).\mu(dx)\propto e^{-\Phi(x)}\gamma(dx),\qquad \mu_m(dx)\propto e^{-\Phi(x)}\gamma_m(dx).μ(dx)∝e−Φ(x)γ(dx),μm​(dx)∝e−Φ(x)γm​(dx).

Fix a step size δ∈(0,12]\delta\in(0,\tfrac12]δ∈(0,21​] and put ρ=1−(1−2δ)1/2\rho=1-(1-2\delta)^{1/2}ρ=1−(1−2δ)1/2. One pCN step from xxx draws ξ∼γ\xi\sim\gammaξ∼γ and proposes px=(1−2δ)1/2x+2δ ξp_x=(1-2\delta)^{1/2}x+\sqrt{2\delta}\,\xipx​=(1−2δ)1/2x+2δ​ξ. The proposal is accepted with probability α(x,px)=1∧exp⁡(Φ(x)−Φ(px))\alpha(x,p_x)=1\wedge\exp(\Phi(x)-\Phi(p_x))α(x,px​)=1∧exp(Φ(x)−Φ(px​)); otherwise the chain stays at xxx. Its transition kernel is P\mathcal PP. The kernel Pm\mathcal P_mPm​ is the same algorithm on PmHP_mHPm​H with ξ∼γm\xi\sim\gamma_mξ∼γm​.

Distances between probability measures are Wasserstein lifts of a cost ccc: c(ν1,ν2)=inf⁡π∫c dπc(\nu_1,\nu_2)=\inf_\pi\int c\,d\pic(ν1​,ν2​)=infπ​∫cdπ over couplings π\piπ of ν1,ν2\nu_1,\nu_2ν1​,ν2​. A kernel is ddd-contracting if d(x,y)<1d(x,y)<1d(x,y)<1 implies d(P(x,⋅),P(y,⋅))≤c d(x,y)d(\mathcal P(x,\cdot),\mathcal P(y,\cdot))\le c\,d(x,y)d(P(x,⋅),P(y,⋅))≤cd(x,y) for a fixed c<1c<1c<1. A set SSS is ddd-small if d(P(x,⋅),P(y,⋅))≤s<1d(\mathcal P(x,\cdot),\mathcal P(y,\cdot))\le s<1d(P(x,⋅),P(y,⋅))≤s<1 for all x,y∈Sx,y\in Sx,y∈S.

The distance of this mission is a weighted path length (3.6). For unit-speed C1C^1C1 paths ψ:[0,T]→H\psi:[0,T]\to Hψ:[0,T]→H from xxx to yyy,

dˉ(x,y)=inf⁡T,ψ1ε∫0Teη∥ψ(t)∥ dt,d=1∧dˉ,d~(x,y)=d(x,y) (1+V(x)+V(y)),\bar d(x,y)=\inf_{T,\psi}\frac1\varepsilon\int_0^T e^{\eta\|\psi(t)\|}\,dt,\qquad d=1\wedge\bar d,\qquad \tilde d(x,y)=\sqrt{d(x,y)\,(1+V(x)+V(y))},dˉ(x,y)=T,ψinf​ε1​∫0T​eη∥ψ(t)∥dt,d=1∧dˉ,d~(x,y)=d(x,y)(1+V(x)+V(y))​,

with V(x)=∥x∥iV(x)=\|x\|^iV(x)=∥x∥i (i≥1i\ge1i≥1) or V(x)=ev∥x∥V(x)=e^{v\|x\|}V(x)=ev∥x∥ (v>0v>0v>0).

There are two assumptions. Assumption 2.10 says that for ∥x∥≥R\|x\|\ge R∥x∥≥R every proposal within distance r(∥x∥)r(\|x\|)r(∥x∥) of the proposal mean (1−ρ)x(1-\rho)x(1−ρ)x is accepted with probability at least eαle^{\alpha_l}eαl​, where r(s)≤ρ2sr(s)\le\frac\rho2 sr(s)≤2ρ​s. Assumption 2.13 says that e−Φe^{-\Phi}e−Φ is γ\gammaγ-integrable and that φ(r)=sup⁡x≠y∈Br(0)∣Φ(x)−Φ(y)∣/∥x−y∥≤Mκeκr\varphi(r)=\sup_{x\ne y\in B_r(0)}|\Phi(x)-\Phi(y)|/\|x-y\|\le M_\kappa e^{\kappa r}φ(r)=supx=y∈Br​(0)​∣Φ(x)−Φ(y)∣/∥x−y∥≤Mκ​eκr for every κ>0\kappa>0κ>0.

Formalization targets

Goal: Theorem 2.14

Under Assumption 2.10 with r(s)=rsar(s)=r s^ar(s)=rsa (r>0r>0r>0, a∈(12,1)a\in(\frac12,1)a∈(21​,1)) and Assumption 2.13:

  1. μ\muμ and every μm\mu_mμm​ are the unique invariant probability measures of P\mathcal PP and Pm\mathcal P_mPm​.
  2. For η\etaη small enough and then ε\varepsilonε small enough, there is one n~\tilde nn~ such that for every mmm and all probability measures ν1,ν2\nu_1,\nu_2ν1​,ν2​
d~(ν1Pn~,ν2Pn~)≤12d~(ν1,ν2),d~(ν1Pmn~,ν2Pmn~)≤12d~(ν1,ν2).\tilde d(\nu_1\mathcal P^{\tilde n},\nu_2\mathcal P^{\tilde n})\le\tfrac12\tilde d(\nu_1,\nu_2),\qquad \tilde d(\nu_1\mathcal P_m^{\tilde n},\nu_2\mathcal P_m^{\tilde n})\le\tfrac12\tilde d(\nu_1,\nu_2).d~(ν1​Pn~,ν2​Pn~)≤21​d~(ν1​,ν2​),d~(ν1​Pmn~​,ν2​Pmn~​)≤21​d~(ν1​,ν2​).

The essential point is that n~\tilde nn~ does not depend on mmm.

Milestones

  • Lemma 3.5 (1)–(3): the comparison of dˉ\bar ddˉ with ∥x−y∥eη(∥x∥∨∥y∥)/ε\|x-y\|e^{\eta(\|x\|\vee\|y\|)}/\varepsilon∥x−y∥eη(∥x∥∨∥y∥)/ε, and the contraction of dˉ\bar ddˉ under a common-noise pCN step,
dˉ(px,py)≤(1−2δ)1/2eη[−ρ(∥x∥∨∥y∥)+2δ∥ξ∥+J]dˉ(x,y).\bar d(p_x,p_y)\le(1-2\delta)^{1/2}e^{\eta[-\rho(\|x\|\vee\|y\|)+\sqrt{2\delta}\|\xi\|+J]}\bar d(x,y).dˉ(px​,py​)≤(1−2δ)1/2eη[−ρ(∥x∥∨∥y∥)+2δ​∥ξ∥+J]dˉ(x,y).
  • Lemma 3.6: P\mathcal PP and every Pm\mathcal P_mPm​ are ddd-contracting with one constant.
  • Lemma 3.7: bounded sets are ddd-small for Pn\mathcal P^nPn and every Pmn\mathcal P_m^nPmn​, with nnn and sss independent of mmm.

The paper derives Theorem 2.14 from these, from Lemma 3.2 (Lyapunov functions) and from Proposition 2.6 (the weak Harris theorem of Hairer, Mattingly and Scheutzow 2011). The last two are posed in mission I of this series.

Significance

A Wasserstein spectral gap uniform in mmm means that the number of pCN steps needed to reach a given accuracy does not grow with the discretisation level. In §4 of the paper this yields a strong law of large numbers and a central limit theorem for pCN ergodic averages, and, combined with Theorem 2.15, an Lμ2L^2_\muLμ2​-spectral gap and mean-square error bounds, all uniform in the dimension. The locally Lipschitz case is the one that covers potentials of polynomial growth.

The result is proved in the paper. It has not been formalized. A formalization would produce a reusable weak-Harris toolkit for Markov kernels on Polish spaces, and a machine-checked account of the path-metric construction, which the paper adapts from Hairer and Majda (2010) and Hairer, Mattingly and Scheutzow (2011). It would also check the paper's proof, whose printed Lemma 3.5 (3) contains a typographical slip in the exponent; the formalized bound is the one the proof derives.

Difficulty

With Φ\PhiΦ only locally Lipschitz, no single ε\varepsilonε makes 1∧∥x−y∥/ε1\wedge\|x-y\|/\varepsilon1∧∥x−y∥/ε contracting. The probability that exactly one of two coupled chains accepts is controlled by ∣Φ(x)−Φ(y)∣|\Phi(x)-\Phi(y)|∣Φ(x)−Φ(y)∣, and far from the origin this exceeds any fixed multiple of ∥x−y∥\|x-y\|∥x−y∥. The weighted path distance makes far-out points "close" only when they are very close in norm. But then even the "both accept" move can increase the distance, because the weight eη∥⋅∥e^{\eta\|\cdot\|}eη∥⋅∥ changes along the move. Showing that the shrinkage (1−ρ)(1-\rho)(1−ρ) of the proposal mean beats this, while the Gaussian noise term stays integrable uniformly in mmm, is the content of Lemmas 3.5 and 3.6. The order of the choices (RRR, then η\etaη, then ε\varepsilonε) is essential.

Formalization scope

  • HHH is a real Hilbert space that is complete, separable and Borel. γ\gammaγ is Mathlib's IsGaussian with mean zero. (ei)(e_i)(ei​) is a HilbertBasis ℕ whose vectors are pairwise uncorrelated under the covariance bilinear form.
  • PmHP_mHPm​H is a submodule. γm\gamma_mγm​ is the pushforward under the orthogonal projection. Pm\mathcal P_mPm​ lives on the subtype PmHP_mHPm​H, with Φ\PhiΦ and VVV restricted to it and ddd restricted from HHH.
  • μ\muμ and μm\mu_mμm​ are Mathlib's normalised tilted measures. The goal concludes that they are probability measures.
  • The Metropolis–Hastings kernel is built from Mathlib's Kernel.withDensity. Kernel powers are composition powers, and νPn\nu\mathcal P^nνPn is Measure.bind.
  • Wasserstein lifts and dˉ\bar ddˉ are infima in [0,∞][0,\infty][0,∞], so no junk zero arises from an empty or unbounded set. Unit speed is imposed on (0,T)(0,T)(0,T), so dˉ(x,x)=0\bar d(x,x)=0dˉ(x,x)=0 through the constant path with T=0T=0T=0.
  • Contraction, smallness and Lyapunov constants are explicit arguments. "Uniform in mmm" is "one constant for all mmm".
  • "Small enough" is ∃η0>0 ∀η∈(0,η0] ∃ε0>0 ∀ε∈(0,ε0]\exists\eta_0>0\ \forall\eta\in(0,\eta_0]\ \exists\varepsilon_0>0\ \forall\varepsilon\in(0,\varepsilon_0]∃η0​>0 ∀η∈(0,η0​] ∃ε0​>0 ∀ε∈(0,ε0​].
  • Several readings are disclosed. "r∈Rr\in\mathbb Rr∈R" is read as r>0r>0r>0, i∈Ni\in\mathbb Ni∈N as i≥1i\ge1i≥1, and v>0v>0v>0. Assumption 2.10 is stated for s≥0s\ge0s≥0, the domain of rrr, and requires r(s)>0r(s)>0r(s)>0 for s>0s>0s>0 so that the acceptance balls are nonempty. Its infimum and the supremum φ(r)\varphi(r)φ(r) of Assumption 2.13 are stated pointwise.
  • The general form of Lemma 3.6 has a disclosed radius-floor hypothesis: r(s)r(s)r(s) stays bounded away from zero for large sss. The printed proof needs a uniform positive probability for the proposal ball; this hypothesis supplies it. Theorem 2.14's power-law radius already meets it.
  • The formalization rules out trivialising readings. The tilted measure cannot be the zero measure, because the goal asserts it is a probability measure. Uniqueness is among probability measures. V≡1V\equiv1V≡1 is excluded. A n~\tilde nn~ chosen after mmm would give a per-dimension gap, not this theorem.
  • A complete development needs:
    • the weak Harris theorem (Proposition 2.6, mission I);
    • Gaussian tail bounds of Fernique type, with the dimension-monotonicity of Lemma 3.1 (mission I);
    • the Lyapunov drift Lemma 3.2 (mission I);
    • calculus of C1C^1C1 paths in Hilbert space;
    • synchronous couplings of Metropolis–Hastings kernels.
  • The Harris and coupling layers are reusable well beyond this paper. Contributions to any of them are welcome.

Selected references

  • M. Hairer, A. M. Stuart and S. J. Vollmer, Spectral gaps for a Metropolis–Hastings algorithm in infinite dimensions, arXiv:1112.1392v4 (2014), published in Ann. Appl. Probab. 24(6) (2014) 2455–2490, https://doi.org/10.1214/13-AAP982. https://arxiv.org/abs/1112.1392v4
  • M. Hairer, J. C. Mattingly and M. Scheutzow, Asymptotic coupling and a general form of Harris' theorem with applications to stochastic delay equations, Probab. Theory Related Fields 149 (2011) 223–259. MR2773030, https://mathscinet.ams.org/mathscinet-getitem?mr=2773030
  • M. Hairer and A. J. Majda, A simple framework to justify linear response theory, Nonlinearity 23 (2010) 909–922. MR2602020, https://mathscinet.ams.org/mathscinet-getitem?mr=2602020
  • A. Beskos, G. O. Roberts, A. M. Stuart and J. Voss, MCMC methods for diffusion bridges, Stoch. Dyn. 8 (2008) 319–350. MR2444507, https://mathscinet.ams.org/mathscinet-getitem?mr=2444507
  • S. L. Cotter, G. O. Roberts, A. M. Stuart and D. White, MCMC methods for functions: modifying old algorithms to make them faster, Statist. Sci. 28 (2013) 424–446. https://doi.org/10.1214/13-STS421
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AnalysisProbabilityStochastic Systems·Captain: mikedeng1

Affine Volterra Processes 2: The Exponential-Affine Transform Formula via the Riccati–Volterra EquationResearch Paper

Motivation

Many stochastic models have a present state that depends on a weighted history of past drift and noise. A stochastic Volterra equation captures this dependence through a kernel KKK: a recent increment and an older increment can enter the current state with different weights. Classical affine diffusions arise from the special constant kernel K=IK=IK=I. For those diffusions, conditional Fourier–Laplace transforms can often be found from finite-dimensional Riccati ordinary differential equations. The paper by Abi Jaber, Larsson and Pulido asks for an analogous transform when the kernel retains memory. Its Theorem 4.3 gives a formula for a continuous affine Volterra process under a stated Riccati–Volterra solution assumption.

The result matters for models in which the history cannot be replaced by the current state alone. The transform characterizes conditional distributions and integrated path functionals in the form used by the paper's later results. The present mission isolates Theorem 4.3 and four of its stated supporting claims. The paper proves these results; the mission seeks machine-checked proofs of their Lean statements.

Setting

Fix a positive integer ddd and a deterministic, matrix-valued kernel K:[0,∞)→Rd×dK:[0,\infty)\to\mathbb R^{d\times d}K:[0,∞)→Rd×d whose entries are locally square integrable. The Volterra convolution of KKK with a vector function vvv is (K∗v)(t)=∫0tK(t−s)v(s) ds(K*v)(t)=\int_0^t K(t-s)v(s)\,ds(K∗v)(t)=∫0t​K(t−s)v(s)ds. Matrix convolutions retain the order of multiplication: (K∗R)(t)=∫0tK(t−s)R(s) ds(K*R)(t)=\int_0^t K(t-s)R(s)\,ds(K∗R)(t)=∫0t​K(t−s)R(s)ds.

Let A0,…,AdA^0,\ldots,A^dA0,…,Ad be real symmetric matrices and b0,…,bdb^0,\ldots,b^db0,…,bd real column vectors. Their affine covariance and drift are a(x)=A0+∑ixiAia(x)=A^0+\sum_i x_iA^ia(x)=A0+∑i​xi​Ai and b(x)=b0+∑ixibib(x)=b^0+\sum_i x_i b^ib(x)=b0+∑i​xi​bi. The matrix B=(b1 ⋯ bd)B=(b^1\ \cdots\ b^d)B=(b1 ⋯ bd) has the bib^ibi as columns. For a complex row uuu, write A(u)=(uA1u⊤,…,uAdu⊤)A(u)=(uA^1u^\top,\ldots,uA^du^\top)A(u)=(uA1u⊤,…,uAdu⊤); the transpose is ordinary, with no complex conjugation.

An affine Volterra process XXX is a continuous solution of

Xt=x0+∫0tK(t−s)b(Xs) ds+∫0tK(t−s)σ(Xs) dWs.X_t=x_0+\int_0^t K(t-s)b(X_s)\,ds+\int_0^t K(t-s)\sigma(X_s)\,dW_s.Xt​=x0​+∫0t​K(t−s)b(Xs​)ds+∫0t​K(t−s)σ(Xs​)dWs​.

Here WWW is a ddd-dimensional Brownian motion on a usual stochastic basis, x0x_0x0​ is deterministic, and XXX stays in a state space EEE. The continuous coefficient σ\sigmaσ obeys σ(x)σ(x)⊤=a(x)\sigma(x)\sigma(x)^\top=a(x)σ(x)σ(x)⊤=a(x) on EEE, where a(x)a(x)a(x) is positive semidefinite. This is Definition 4.1 and the standing setting of Section 4 of the paper.

Formalization targets

The main target is Theorem 4.3. Fix a finite horizon TTT, a complex row uuu, and an integrable complex-row function fff. Suppose a square-integrable function ψ\psiψ solves the Riccati–Volterra equation

ψ=uK+(f+ψB+12A(ψ))∗K.\psi=uK+\bigl(f+\psi B+\tfrac12A(\psi)\bigr)*K.ψ=uK+(f+ψB+21​A(ψ))∗K.

Define YYY by the stochastic integral and drift in equations (4.4)–(4.5). The theorem identifies YtY_tYt​ with a conditional mean plus a quadratic correction:

Yt=E[uXT+(f∗X)T∣Ft]+12∫tTψ(T−s)a(E[Xs∣Ft])ψ(T−s)⊤ ds,0≤t≤T.Y_t=\mathbb E[uX_T+(f*X)_T\mid\mathcal F_t] +\tfrac12\int_t^T\psi(T-s)a(\mathbb E[X_s\mid\mathcal F_t])\psi(T-s)^\top\,ds, \qquad 0\le t\le T.Yt​=E[uXT​+(f∗X)T​∣Ft​]+21​∫tT​ψ(T−s)a(E[Xs​∣Ft​])ψ(T−s)⊤ds,0≤t≤T.

It also states that eYe^{Y}eY is a local martingale on [0,T][0,T][0,T]. If it is a true martingale, then the exponential-affine transform formula is

E ⁣[euXT+(f∗X)T∣Ft]=eYt,t≤T.\mathbb E\!\left[e^{uX_T+(f*X)_T}\mid\mathcal F_t\right]=e^{Y_t},\qquad t\le T.E[euXT​+(f∗X)T​∣Ft​]=eYt​,t≤T.

The milestone list records Lemma 4.2's conditional and unconditional means, the mean Volterra equation stated in the proof of Theorem 4.3, the resolvent commutation claim in the proof of Lemma 4.4, and Lemma 4.4's equivalent Riccati equation. A second-kind resolvent RBR_BRB​ of −KB-KB−KB uses the paper's sign convention H∗RB=RB∗H=H−RBH*R_B=R_B*H=H-R_BH∗RB​=RB​∗H=H−RB​ for H=−KBH=-KBH=−KB; the equivalent equation uses EB=K−RB∗KE_B=K-R_B*KEB​=K−RB​∗K.

Significance

The conditional transform links a path-dependent stochastic equation to a deterministic nonlinear Volterra equation. It supplies a way to describe the law of a future state together with a linear functional of its past. The conditional-mean milestone separately gives a usable formula for E[XT∣Ft]\mathbb E[X_T\mid\mathcal F_t]E[XT​∣Ft​], while the resolvent milestones identify the deterministic kernel relations needed by the transform.

The source provides proofs of these claims. The formalization task is to check their assumptions and equalities against a precise model of Brownian Itô integration, conditional expectation, and matrix convolution. Published Lean definitions for Brownian motion and an Itô integral relation are reused. The affine Volterra process, its Riccati equation, and these theorem statements are drafted here; their proofs remain open.

Difficulty

The conditional payoff involves the entire path before TTT, while XXX generally has no finite-dimensional Markov state. Consequently, the familiar affine-diffusion formula in terms of XtX_tXt​ alone is not the target of Theorem 4.3. Deterministic matrix convolutions are order-sensitive, and the two resolvents of −KB-KB−KB and −BK-BK−BK have different kernels. Stochastic convolutions also have integrands that depend on the terminal time. The passage from fixed-time integral equalities to a continuous local-martingale process requires care about versions and filtration adaptation.

Formalization scope

Processes use nonnegative real time, while deterministic kernels and interval integrals use real time. Finite-dimensional LpL^pLp conditions are checked componentwise. Kernel and resolvent identities between locally integrable functions hold almost everywhere on positive time. Riccati equations hold almost everywhere on [0,T][0,T][0,T]; stochastic and conditional identities hold almost surely at each fixed time. The local-martingale claim uses the real and imaginary parts of the complex exponential, stopped at TTT.

The process definition includes the Section 4 assumptions on symmetry, covariance positivity, continuity of σ\sigmaσ, deterministic x0x_0x0​, and the usual stochastic basis. Brownian Itô terms are constrained by the published integral relation. Deterministic drift convolutions require integrable integrands. The theorem asserts integrability of the payoff and of XsX_sXs​ as conclusions, preventing conditional expectation from defaulting to zero. In (4.6) the conditional means E[Xs∣Ft]\mathbb E[X_s\mid\mathcal F_t]E[Xs​∣Ft​] enter the dsdsds-integral through a jointly measurable version in (s,ω)(s,\omega)(s,ω), so that integral cannot default to zero. The dimension is positive, and the theorem does not specialize the kernel to III or insert a resolvent assumption into its goal.

A complete development will need reusable results on locally integrable matrix kernels and their resolvents, stochastic Fubini interchange, moment bounds for Volterra solutions, and conditional expectation of the resulting integrals. The moment bound is posed as Lemma 3.1 in the companion existence mission. This draft includes the four listed milestones; Lemmas 2.1 and 2.5 from the source are left for a fuller stochastic Fubini and semimartingale encoding. Contributions that preserve their general hypotheses and conclusions are welcome.

Selected references

  • E. Abi Jaber, M. Larsson, and S. Pulido, Affine Volterra processes, arXiv:1708.08796v3, 2019. Preprint
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Convex OptimizationMachine LearningOptimization+1·Captain: mikedeng1

Stochastic Model-Based Minimization of Weakly Convex Functions 4: Under Convexity, Stochastic Model-Based Minimization Reaches Expected Function Gap (½‖x₀−x*‖² + L²γ²)/(γ√(T+1))Research Paper

Motivation

Many problems in statistical learning and signal processing take the form of minimizing an expectation f(x)=Eξ[F(x,ξ)]f(x)=\mathbb E_\xi[F(x,\xi)]f(x)=Eξ​[F(x,ξ)] plus a regularizer or constraint r(x)r(x)r(x), where the only access to fff is through samples ξ∼P\xi\sim Pξ∼P. The classical tool is the stochastic (proximal) subgradient method, which replaces fff at the current point by a random linear function. Two other methods use richer local approximations: the stochastic proximal point method keeps the whole sampled loss F(⋅,ξ)F(\cdot,\xi)F(⋅,ξ), and the stochastic prox-linear method linearizes only the smooth inner part of a composite loss h(c(x,ξ))h(c(x,\xi))h(c(x,ξ)). In experiments the richer models are markedly less sensitive to the choice of step size.

Davis and Drusvyatskiy (arXiv:1803.06523, SIAM J. Optim. 29(1), 2019) treat all three methods as instances of one scheme, stochastic model-based minimization, in which each step minimizes a sampled one-sided model fxt(⋅,ξt)f_{x_t}(\cdot,\xi_t)fxt​​(⋅,ξt​) of fff plus rrr plus a quadratic penalty. Their main theorem (Theorem 4.3) covers weakly convex problems through the Moreau envelope. This mission formalizes the companion result for the convex setting, Theorem 4.1: when the models lower-bound fff in expectation without quadratic error and fx(⋅,ξ)+rf_x(\cdot,\xi)+rfx​(⋅,ξ)+r is convex, the expected function gap at a weighted average of the iterates decays like 1/T1/\sqrt T1/T​. As the paper notes (p. 22), for the stochastic proximal subgradient method this improves earlier bounds (Cruz 2017; Duchi–Singer 2009) because no subgradient norm of rrr enters the estimate.

Setting

Work in Rd\mathbb R^dRd with the Euclidean norm. The problem is

min⁡x∈Rd φ(x):=f(x)+r(x),\min_{x\in\mathbb R^d}\ \varphi(x):=f(x)+r(x),x∈Rdmin​ φ(x):=f(x)+r(x),

where f:Rd→Rf:\mathbb R^d\to\mathbb Rf:Rd→R is locally Lipschitz and r:Rd→R∪{+∞}r:\mathbb R^d\to\mathbb R\cup\{+\infty\}r:Rd→R∪{+∞} is closed (its epigraph is closed) with nonempty domain D=dom⁡rD=\operatorname{dom}rD=domr. A function ψ\psiψ is ρ\rhoρ-weakly convex if x↦ψ(x)+ρ2∥x∥2x\mapsto\psi(x)+\frac\rho2\|x\|^2x↦ψ(x)+2ρ​∥x∥2 is convex; ρ=0\rho=0ρ=0 is ordinary convexity.

Assumption B (p. 18) fixes a probability space (Ω,F,P)(\Omega,\mathcal F,P)(Ω,F,P), an open convex set U⊇DU\supseteq DU⊇D, real constants τ,η,L\tau,\eta,\mathsf Lτ,η,L, a measurable model (x,y,ξ)↦fx(y,ξ)(x,y,\xi)\mapsto f_x(y,\xi)(x,y,ξ)↦fx​(y,ξ) on U×U×ΩU\times U\times\OmegaU×U×Ω and a measurable L:Ω→R+L:\Omega\to\mathbb R_+L:Ω→R+​ such that:

  1. (B1) i.i.d. samples ξ0,ξ1,⋯∼P\xi_0,\xi_1,\dots\sim Pξ0​,ξ1​,⋯∼P can be drawn;
  2. (B2) Eξ[fx(x,ξ)]=f(x)\mathbb E_\xi[f_x(x,\xi)]=f(x)Eξ​[fx​(x,ξ)]=f(x) and Eξ[fx(y,ξ)−f(y)]≤τ2∥y−x∥2\mathbb E_\xi[f_x(y,\xi)-f(y)]\le\frac\tau2\|y-x\|^2Eξ​[fx​(y,ξ)−f(y)]≤2τ​∥y−x∥2 for x,y∈Ux,y\in Ux,y∈U;
  3. (B3) fx(⋅,ξ)+rf_x(\cdot,\xi)+rfx​(⋅,ξ)+r is η\etaη-weakly convex for every x∈Ux\in Ux∈U and almost every ξ\xiξ;
  4. (B4) E[L(ξ)2]≤L\sqrt{\mathbb E[L(\xi)^2]}\le\mathsf LE[L(ξ)2]​≤L and fx(x,ξ)−fx(y,ξ)≤L(ξ)∥x−y∥f_x(x,\xi)-f_x(y,\xi)\le L(\xi)\|x-y\|fx​(x,ξ)−fx​(y,ξ)≤L(ξ)∥x−y∥ for x,y∈Ux,y\in Ux,y∈U and almost every ξ\xiξ.

Algorithm 4.1 (p. 19) starts at x0x_0x0​ and, for t=0,…,Tt=0,\dots,Tt=0,…,T, samples ξt∼P\xi_t\sim Pξt​∼P and sets

xt+1=argmin⁡x{r(x)+fxt(x,ξt)+βt2∥x−xt∥2}.x_{t+1}=\operatorname*{argmin}_{x}\Big\{r(x)+f_{x_t}(x,\xi_t)+\frac{\beta_t}{2}\|x-x_t\|^2\Big\}.xt+1​=xargmin​{r(x)+fxt​​(x,ξt​)+2βt​​∥x−xt​∥2}.

The convex setting is τ=0\tau=0τ=0 and η=0\eta=0η=0. Write αt=βt−1>0\alpha_t=\beta_t^{-1}>0αt​=βt−1​>0 for the step sizes and let x∗x^*x∗ be any minimizer of φ\varphiφ.

Formalization targets

Goal: Theorem 4.1, (4.17) and (4.18)

For every T>0T>0T>0,

E[φ(1∑t=0Tαt∑t=0Tαtxt+1)−φ(x∗)]≤12∥x0−x∗∥2+2L2∑t=0Tαt2∑t=0Tαt,\mathbb E\Big[\varphi\Big(\tfrac{1}{\sum_{t=0}^T\alpha_t}\textstyle\sum_{t=0}^T\alpha_t x_{t+1}\Big)-\varphi(x^*)\Big]\le\frac{\frac12\|x_0-x^*\|^2+2\mathsf L^2\sum_{t=0}^T\alpha_t^2}{\sum_{t=0}^T\alpha_t},E[φ(∑t=0T​αt​1​∑t=0T​αt​xt+1​)−φ(x∗)]≤∑t=0T​αt​21​∥x0​−x∗∥2+2L2∑t=0T​αt2​​,

and with the constant step αt=γ/T+1\alpha_t=\gamma/\sqrt{T+1}αt​=γ/T+1​, γ>0\gamma>0γ>0,

E[φ(1T+1∑t=1T+1xt)−φ(x∗)]≤12∥x0−x∗∥2+2L2γ2γT+1.\mathbb E\Big[\varphi\Big(\tfrac{1}{T+1}\textstyle\sum_{t=1}^{T+1}x_t\Big)-\varphi(x^*)\Big]\le\frac{\frac12\|x_0-x^*\|^2+2\mathsf L^2\gamma^2}{\gamma\sqrt{T+1}}.E[φ(T+11​∑t=1T+1​xt​)−φ(x∗)]≤γT+1​21​∥x0​−x∗∥2+2L2γ2​.

The factor 222 in front of L2\mathsf L^2L2 is the constant the paper's proof establishes; see Formalization scope.

Milestones

  1. Lemma 4.1: φ\varphiφ is (τ+η)(\tau+\eta)(τ+η)-weakly convex and ∣f(x)−f(y)∣≤L∥x−y∥|f(x)-f(y)|\le\mathsf L\|x-y\|∣f(x)−f(y)∣≤L∥x−y∥ on UUU.
  2. Lemma 4.2, (4.8): for every x∈dom⁡rx\in\operatorname{dom}rx∈domr, with xtx_txt​ fixed and Et\mathbb E_tEt​ the expectation over ξt\xi_tξt​,
Et∥xt+1−x∥2≤βt+τβt−η∥xt−x∥2−2βt−ηEt[φ(xt+1)−φ(x)]+4L2βt(βt−η).\mathbb E_t\|x_{t+1}-x\|^2\le\frac{\beta_t+\tau}{\beta_t-\eta}\|x_t-x\|^2-\frac{2}{\beta_t-\eta}\mathbb E_t[\varphi(x_{t+1})-\varphi(x)]+\frac{4\mathsf L^2}{\beta_t(\beta_t-\eta)}.Et​∥xt+1​−x∥2≤βt​−ηβt​+τ​∥xt​−x∥2−βt​−η2​Et​[φ(xt+1​)−φ(x)]+βt​(βt​−η)4L2​.
  1. Proof of Theorem 4.1, first display (p. 23): 2αtE[φ(xt+1)−φ(x∗)]≤E∥xt−x∗∥2−E∥xt+1−x∗∥2+4L2αt22\alpha_t\mathbb E[\varphi(x_{t+1})-\varphi(x^*)]\le\mathbb E\|x_t-x^*\|^2-\mathbb E\|x_{t+1}-x^*\|^2+4\mathsf L^2\alpha_t^22αt​E[φ(xt+1​)−φ(x∗)]≤E∥xt​−x∗∥2−E∥xt+1​−x∗∥2+4L2αt2​.

Significance

Theorem 4.1 is the function-value guarantee of the model-based framework. Theorem 4.3 measures progress by the gradient of the Moreau envelope, which is the right quantity for nonconvex problems but says nothing directly about suboptimality; under convexity, Theorem 4.1 gives the familiar O(1/T)O(1/\sqrt T)O(1/T​) rate for the gap itself. It applies to the stochastic proximal point and prox-linear methods as well as to the proximal subgradient method, and §4.2 of the paper uses it for minimizing an expectation of a pointwise maximum of convex functions, such as the conditional value-at-risk. The estimate (4.8) behind it is also the engine of the strongly convex rate O(1/(μT))O(1/(\mu T))O(1/(μT)) (Theorem 4.2, a separate mission of this series).

The result is proved in the paper; nothing in it is open. To our knowledge none of these statements has a machine-checked proof. The formalization contributes a checked version of the one-step estimate (4.8) with its corrected constant, a reusable Lean encoding of Assumption B and of Algorithm 4.1 with extended-valued rrr, and the passage from conditional one-step bounds to expectations over the product measure of the samples.

Difficulty

The argument is short on paper; the work lies in the measure theory the paper leaves implicit. The iterate xt+1x_{t+1}xt+1​ is an argmin that depends on xtx_txt​ and on the fresh sample ξt\xi_tξt​, and the one-step estimate holds only conditionally, with xtx_txt​ frozen. Turning it into an inequality between unconditional expectations requires measurability of the iterates, independence of ξt\xi_tξt​ from the past, and integrability of φ(xt+1)\varphi(x_{t+1})φ(xt+1​) and ∥xt+1−x∗∥2\|x_{t+1}-x^*\|^2∥xt+1​−x∗∥2, which the paper takes for granted. The convex function φ\varphiφ is extended-valued, so the function gap is meaningful only because every iterate and every average lies in dom⁡r\operatorname{dom}rdomr.

A naive one-step argument that bounds f(xt)−f(xt+1)f(x_t)-f(x_{t+1})f(xt​)−f(xt+1​) and fxt(xt,ξt)−fxt(xt+1,ξt)f_{x_t}(x_t,\xi_t)-f_{x_t}(x_{t+1},\xi_t)fxt​​(xt​,ξt​)−fxt​​(xt+1​,ξt​) separately, each by a Lipschitz constant times ∥xt+1−xt∥\|x_{t+1}-x_t\|∥xt+1​−xt​∥, gives the constant 4L24\mathsf L^24L2 in (4.8) and not the printed 2L22\mathsf L^22L2. The printed constant is false (see below), so the constant cannot be improved simply by tightening that one step.

Formalization scope

  • Space and encoding. Rd\mathbb R^dRd is EuclideanSpace ℝ (Fin d). The extended-valued rrr is a real function together with its domain D; closedness of rrr is closedness of {(x,t):x∈D, r(x)≤t}\{(x,t):x\in D,\ r(x)\le t\}{(x,t):x∈D, r(x)≤t}, and convexity is ConvexOn ℝ D. L\mathsf LL is L and L(ξ)L(\xi)L(ξ) is Lfun.
  • Randomness. The T+1T+1T+1 samples are a point of ΩT+1\Omega^{T+1}ΩT+1 under the product measure P⊗(T+1)P^{\otimes(T+1)}P⊗(T+1); expectations are Bochner integrals. Every theorem that bounds an expectation also concludes integrability of the integrand, so the junk value 000 of a non-integrable integral cannot make a bound hold vacuously. The single-step estimate (4.8) holds xtx_txt​ fixed and integrates over one sample; integrability of r(xt+1)r(x_{t+1})r(xt+1​) is a hypothesis there, and a conclusion in the run-level statements, where the minimizer x∗x^*x∗ supplies the lower bound.
  • Algorithm. The iterates are the run of an update map that always lies in DDD, is jointly measurable, and is a minimizer of the subproblem for almost every sample. An unconstrained update map would make the goal false; this one is pinned to the paper's step. x0∈Ux_0\in Ux0​∈U is assumed, since the model is only defined on UUU. The parameter ρˉ\bar\rhoρˉ​ of Algorithm 4.1 does not affect the iterates, and requiring βt>ρˉ>τ+η=0\beta_t>\bar\rho>\tau+\eta=0βt​>ρˉ​>τ+η=0 over the steps used is the same as αt>0\alpha_t>0αt​>0.
  • Minimizer. x∗∈Dx^*\in Dx∗∈D with φ(x∗)≤φ(y)\varphi(x^*)\le\varphi(y)φ(x∗)≤φ(y) for all y∈Dy\in Dy∈D. A minimizer of fff alone, or an arbitrary point, would trivialize the goal; convexity of φ\varphiφ is not assumed separately, since it follows from Lemma 4.1.
  • Corrected constant (paper typo). The paper prints 2L2/(βt(βt−η))2\mathsf L^2/(\beta_t(\beta_t-\eta))2L2/(βt​(βt​−η)) in (4.8), 2L2αt22\mathsf L^2\alpha_t^22L2αt2​ in the first display of the proof of Theorem 4.1, and L2\mathsf L^2L2 in (4.17)–(4.18). Its own proof of (4.8) (p. 21) bounds the error terms by 2L2/βt2\mathsf L^2/\beta_t2L2/βt​ and divides by (βt−η)/2(\beta_t-\eta)/2(βt​−η)/2, which gives 4L2/(βt(βt−η))4\mathsf L^2/(\beta_t(\beta_t-\eta))4L2/(βt​(βt​−η)). The printed (4.8) and the printed first display fail on a one-dimensional example (r=0r=0r=0, f=∣⋅∣f=|\cdot|f=∣⋅∣, a linear model with slope ±1\pm1±1 at the origin, β=1\beta=1β=1). The Lean statements carry the constants the proof establishes: 4L24\mathsf L^24L2 in (4.8) and the display, 2L22\mathsf L^22L2 in (4.17)–(4.18). Whether the printed (4.17) holds by a sharper argument is not settled here; the milestone texts quote the page verbatim.
  • Needed infrastructure. Product measures and independence of coordinates (Measure.pi), Fubini–Tonelli over Ωt×Ω\Omega^{t}\times\OmegaΩt×Ω, measurability of the run, Jensen's inequality for a convex function on a convex set, and strong convexity of the subproblem. Proofs of any milestone are welcome, as are a general "conditional one-step bound to expectation over the run" lemma reusable by the other missions of this series.

Selected references

  • D. Davis, D. Drusvyatskiy, Stochastic model-based minimization of weakly convex functions, SIAM J. Optim. 29(1):207–239, 2019; arXiv:1803.06523v3. https://arxiv.org/abs/1803.06523
  • J. Duchi, Y. Singer, Efficient online and batch learning using forward backward splitting, J. Mach. Learn. Res. 10:2899–2934, 2009. https://jmlr.org/papers/v10/duchi09a.html
  • J. Cruz, On proximal subgradient splitting method for minimizing the sum of two nonsmooth convex functions, Set-Valued Var. Anal. 25:245–263, 2017. https://doi.org/10.1007/s11228-016-0376-5
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Convex OptimizationMachine LearningOptimization+1·Captain: mikedeng1

Stochastic Model-Based Minimization of Weakly Convex Functions 5: Under μ-Strong Convexity, Model-Based Minimization with β_t = μ(t+1)/2 Reaches Expected Function Gap O(1/(μT))Research Paper

Motivation

Many problems in statistical learning and signal processing minimize an expectation f(x)=Eξ[F(x,ξ)]f(x)=\mathbb E_\xi[F(x,\xi)]f(x)=Eξ​[F(x,ξ)] plus a regularizer or constraint r(x)r(x)r(x), with access to fff only through samples ξ∼P\xi\sim Pξ∼P. The standard tool is the stochastic (proximal) subgradient method, which replaces fff at the current point by a random linear function. Two other methods use richer local approximations: the stochastic proximal point method keeps the whole sampled loss F(⋅,ξ)F(\cdot,\xi)F(⋅,ξ), and the stochastic prox-linear method linearizes only the smooth inner map of a composite loss h(c(x,ξ))h(c(x,\xi))h(c(x,ξ)). The richer models are markedly less sensitive to the step size in practice.

Davis and Drusvyatskiy (arXiv:1803.06523, SIAM J. Optim. 29(1), 2019) treat all three methods as instances of one scheme, stochastic model-based minimization: each step minimizes a sampled one-sided model fxt(⋅,ξt)f_{x_t}(\cdot,\xi_t)fxt​​(⋅,ξt​) of fff, plus rrr, plus a quadratic penalty. Their main theorem (Theorem 4.3) concerns weakly convex problems. This mission formalizes the companion result for the strongly convex setting, Theorem 4.2: when the models lower-bound fff in expectation and fx(⋅,ξ)+rf_x(\cdot,\xi)+rfx​(⋅,ξ)+r is μ\muμ-strongly convex, the expected function gap at a nonuniformly weighted average of the iterates decays like 1/(μT)1/(\mu T)1/(μT). The weighting is the technique of Schmidt, Le Roux and Bach (2012) for the projected stochastic subgradient method; the paper extends it to the fully proximal, model-based setting (p. 23).

Setting

Work in Rd\mathbb R^dRd with the Euclidean norm. The problem is

min⁡x∈Rd φ(x):=f(x)+r(x),\min_{x\in\mathbb R^d}\ \varphi(x):=f(x)+r(x),x∈Rdmin​ φ(x):=f(x)+r(x),

where f:Rd→Rf:\mathbb R^d\to\mathbb Rf:Rd→R is locally Lipschitz and r:Rd→R∪{+∞}r:\mathbb R^d\to\mathbb R\cup\{+\infty\}r:Rd→R∪{+∞} is closed (its epigraph is closed) with nonempty domain D=dom⁡rD=\operatorname{dom}rD=domr. A function ψ\psiψ is ρ\rhoρ-weakly convex if x↦ψ(x)+ρ2∥x∥2x\mapsto\psi(x)+\frac\rho2\|x\|^2x↦ψ(x)+2ρ​∥x∥2 is convex; a negative modulus ρ=−μ\rho=-\muρ=−μ is μ\muμ-strong convexity.

Assumption B (p. 18) fixes a probability space (Ω,F,P)(\Omega,\mathcal F,P)(Ω,F,P), an open convex set U⊇DU\supseteq DU⊇D, real constants τ,η,L\tau,\eta,\mathsf Lτ,η,L, a measurable model (x,y,ξ)↦fx(y,ξ)(x,y,\xi)\mapsto f_x(y,\xi)(x,y,ξ)↦fx​(y,ξ) on U×U×ΩU\times U\times\OmegaU×U×Ω and a measurable L:Ω→R+L:\Omega\to\mathbb R_+L:Ω→R+​ such that:

  1. (B1) i.i.d. samples ξ0,ξ1,⋯∼P\xi_0,\xi_1,\dots\sim Pξ0​,ξ1​,⋯∼P can be drawn;
  2. (B2) Eξ[fx(x,ξ)]=f(x)\mathbb E_\xi[f_x(x,\xi)]=f(x)Eξ​[fx​(x,ξ)]=f(x) and Eξ[fx(y,ξ)−f(y)]≤τ2∥y−x∥2\mathbb E_\xi[f_x(y,\xi)-f(y)]\le\frac\tau2\|y-x\|^2Eξ​[fx​(y,ξ)−f(y)]≤2τ​∥y−x∥2 for x,y∈Ux,y\in Ux,y∈U;
  3. (B3) fx(⋅,ξ)+rf_x(\cdot,\xi)+rfx​(⋅,ξ)+r is η\etaη-weakly convex for every x∈Ux\in Ux∈U and almost every ξ\xiξ;
  4. (B4) E[L(ξ)2]≤L\sqrt{\mathbb E[L(\xi)^2]}\le\mathsf LE[L(ξ)2]​≤L and fx(x,ξ)−fx(y,ξ)≤L(ξ)∥x−y∥f_x(x,\xi)-f_x(y,\xi)\le L(\xi)\|x-y\|fx​(x,ξ)−fx​(y,ξ)≤L(ξ)∥x−y∥ for x,y∈Ux,y\in Ux,y∈U and almost every ξ\xiξ.

Algorithm 4.1 (p. 19) starts at x0x_0x0​ and, for t=0,…,Tt=0,\dots,Tt=0,…,T, samples ξt∼P\xi_t\sim Pξt​∼P and sets

xt+1=argmin⁡x{r(x)+fxt(x,ξt)+βt2∥x−xt∥2}.x_{t+1}=\operatorname*{argmin}_{x}\Big\{r(x)+f_{x_t}(x,\xi_t)+\frac{\beta_t}{2}\|x-x_t\|^2\Big\}.xt+1​=xargmin​{r(x)+fxt​​(x,ξt​)+2βt​​∥x−xt​∥2}.

The strongly convex setting is τ=0\tau=0τ=0 and η=−μ\eta=-\muη=−μ with μ>0\mu>0μ>0, run with βt=μ(t+1)/2\beta_t=\mu(t+1)/2βt​=μ(t+1)/2. Let x∗x^*x∗ be any minimizer of φ\varphiφ.

Formalization targets

Goal: Theorem 4.2

For every integer T>0T>0T>0,

E[φ(2(T+2)(T+3)−2∑t=1T+1(t+1) xt)−φ(x∗)]≤μ∥x0−x∗∥2(T+2)2+16L2μ(T+2),\mathbb E\Big[\varphi\Big(\frac{2}{(T+2)(T+3)-2}\sum_{t=1}^{T+1}(t+1)\,x_t\Big)-\varphi(x^*)\Big]\le\frac{\mu\|x_0-x^*\|^2}{(T+2)^2}+\frac{16\mathsf L^2}{\mu(T+2)},E[φ((T+2)(T+3)−22​t=1∑T+1​(t+1)xt​)−φ(x∗)]≤(T+2)2μ∥x0​−x∗∥2​+μ(T+2)16L2​,

together with integrability of the function inside the expectation. The paper prints 8L28\mathsf L^28L2; see Formalization scope.

Milestones

  1. Lemma 4.1 (p. 18): φ\varphiφ is (τ+η)(\tau+\eta)(τ+η)-weakly convex and ∣f(x)−f(y)∣≤L∥x−y∥|f(x)-f(y)|\le\mathsf L\|x-y\|∣f(x)−f(y)∣≤L∥x−y∥ on UUU.
  2. Lemma 4.2, (4.8) (p. 20): for a fixed current point xtx_txt​ and any x∈dom⁡rx\in\operatorname{dom}rx∈domr,
Et∥xt+1−x∥2≤βt+τβt−η∥xt−x∥2−2βt−ηEt[φ(xt+1)−φ(x)]+4L2βt(βt−η).\mathbb E_t\|x_{t+1}-x\|^2\le\frac{\beta_t+\tau}{\beta_t-\eta}\|x_t-x\|^2-\frac{2}{\beta_t-\eta}\mathbb E_t[\varphi(x_{t+1})-\varphi(x)]+\frac{4\mathsf L^2}{\beta_t(\beta_t-\eta)}.Et​∥xt+1​−x∥2≤βt​−ηβt​+τ​∥xt​−x∥2−βt​−η2​Et​[φ(xt+1​)−φ(x)]+βt​(βt​−η)4L2​.
  1. Proof of Theorem 4.2, first display (p. 23): with Δt=12E∥x∗−xt∥2\Delta_t=\frac12\mathbb E\|x^*-x_t\|^2Δt​=21​E∥x∗−xt​∥2,
E[φ(xt+1)−φ(x∗)]≤βtΔt−(βt+μ)Δt+1+2L2βt.\mathbb E[\varphi(x_{t+1})-\varphi(x^*)]\le\beta_t\Delta_t-(\beta_t+\mu)\Delta_{t+1}+\frac{2\mathsf L^2}{\beta_t}.E[φ(xt+1​)−φ(x∗)]≤βt​Δt​−(βt​+μ)Δt+1​+βt​2L2​.

Significance

The result. Theorem 4.2 is the O(1/(μT))O(1/(\mu T))O(1/(μT)) rate for a whole family of stochastic methods at once: the stochastic proximal point, prox-linear and proximal subgradient methods all satisfy Assumption B (§4.2 of the paper). The rate is in function values at an explicit averaged point, with explicit constants, and needs neither smoothness of fff nor bounded subgradients of rrr: the regularizer enters only through the strong convexity of the subproblems. The 1/(μT)1/(\mu T)1/(μT) order is the one Schmidt, Le Roux and Bach obtained for the projected stochastic subgradient method; Theorem 4.2 extends it to models that are not linear and to a general closed rrr.

Formalizing it. The result is proved in the paper; it is not formalized anywhere to our knowledge. Formalizing it pins down the exact constant (the printed one does not follow from the paper's lemmas; see below), the measure-theoretic content of "iterates generated by Algorithm 4.1" (a measurable selection of the argmin, the product measure of the samples, conditional expectation as an integral over one fresh sample) and the integrability that the expectations presuppose. The one-step estimate (4.8) is shared with mission 4 of this series (Theorem 4.1, convex setting); a proof of it serves both.

Difficulty

The telescoping that turns the one-step bound into the rate is elementary once the weights t+2t+2t+2 are chosen. The work lies in two places. First, (4.8) itself: it combines the strong convexity of the subproblem, the one-sided accuracy (B2) used in expectation, the Lipschitz bound (B4) at the random point xt+1x_{t+1}xt+1​ (so the exceptional null set must not depend on that point), Cauchy–Schwarz, and Lemma 4.1. Second, the passage from one step with xtx_txt​ held fixed to expectations over the whole run: this needs the independence of ξt\xi_tξt​ from ξ0,…,ξt−1\xi_0,\dots,\xi_{t-1}ξ0​,…,ξt−1​ (Fubini on the product measure) and integrability of rrr, ∥xt−x∗∥2\|x_t-x^*\|^2∥xt​−x∗∥2 and φ(xt+1)\varphi(x_{t+1})φ(xt+1​) along the run, none of which is stated on the page. A natural first attempt, bounding φ\varphiφ at the average by the average of φ\varphiφ before checking that the average lies in DDD, is valid only because the weights sum to one and DDD is convex by (B3).

Formalization scope

  • Carrier and extended values. Rd\mathbb R^dRd is EuclideanSpace ℝ (Fin d). The extended-valued rrr is encoded by its domain D and its real values on D; closedness is closedness of {(x,t):x∈D, r(x)≤t}\{(x,t):x\in D,\ r(x)\le t\}{(x,t):x∈D, r(x)≤t}. μ\muμ-strong convexity is (−μ)(-\mu)(−μ)-weak convexity: convexity of ψ−μ2∥⋅∥2\psi-\frac\mu2\|\cdot\|^2ψ−2μ​∥⋅∥2 on D.
  • Randomness. The T+1T+1T+1 samples are a point of ΩT+1\Omega^{T+1}ΩT+1 under Measure.pi; expectations are Bochner integrals, and every bounded expectation comes with an integrability conclusion, so a junk value 000 cannot make a bound hold. Et\mathbb E_tEt​ in (4.8) is the integral over one fresh sample with xtx_txt​ held fixed.
  • Iterates. The update is a jointly measurable map that lies in DDD and is a minimizer of the subproblem for almost every sample; the run is driven by it. Measurability of the update and x0∈Ux_0\in Ux0​∈U are added hypotheses. The parameter ρˉ\bar\rhoρˉ​ of Algorithm 4.1 does not affect the iterates (any ρˉ∈(−μ,μ/2)\bar\rho\in(-\mu,\mu/2)ρˉ​∈(−μ,μ/2) is admissible for all ttt) and does not appear. x∗x^*x∗ is any minimizer of φ=f+r\varphi=f+rφ=f+r over DDD.
  • Constant correction. The proof of (4.8) on p. 21 bounds the δ\deltaδ-terms by 2L2/βt2\mathsf L^2/\beta_t2L2/βt​ and divides by (βt−η)/2(\beta_t-\eta)/2(βt​−η)/2, which gives 4L2/(βt(βt−η))4\mathsf L^2/(\beta_t(\beta_t-\eta))4L2/(βt​(βt​−η)); the display prints 2L2/(βt(βt−η))2\mathsf L^2/(\beta_t(\beta_t-\eta))2L2/(βt​(βt​−η)), which fails on a one-dimensional example. Carried through the proof of Theorem 4.2, the corrected constant gives 2L2/βt2\mathsf L^2/\beta_t2L2/βt​ in the first display (printed L2/βt\mathsf L^2/\beta_tL2/βt​) and 16L2/(μ(T+2))16\mathsf L^2/(\mu(T+2))16L2/(μ(T+2)) in the theorem (printed 8L28\mathsf L^28L2). The Lean states the proof's constants; the milestone texts are quoted as printed. Whether the printed 8L28\mathsf L^28L2 bound holds by a sharper argument is open here.
  • Trivializations ruled out. The stepsize is fixed to βt=μ(t+1)/2\beta_t=\mu(t+1)/2βt​=μ(t+1)/2, the update is constrained to the argmin, x∗x^*x∗ minimizes φ\varphiφ (not fff), and the modulus is −μ-\mu−μ, not μ\muμ (μ\muμ-weak convexity would make the theorem false).
  • Contributions welcome. A proof of (4.8) from Assumption B, the Fubini/independence step for the run, and integrability lemmas for argmin selections are reusable across the series.

Selected references

  • D. Davis, D. Drusvyatskiy, Stochastic model-based minimization of weakly convex functions, SIAM J. Optim. 29(1):207–239, 2019; arXiv:1803.06523v3. https://arxiv.org/abs/1803.06523
  • M. Schmidt, N. Le Roux, F. Bach, A simpler approach to obtaining an O(1/t) convergence rate for the projected stochastic subgradient method, arXiv:1212.2002, 2012 (cited as [62] in the paper). https://arxiv.org/abs/1212.2002
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