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

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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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About Prove2Me

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

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

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
4 provers on it7 of 7 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.

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

Matrix multiplication exponent

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

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

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

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About Prove2Me

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

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Linear algebraProbabilityRandom Matrix Theory·Captain: mikedeng1

User-Friendly Tail Bounds for Sums of Random Matrices I: The Master Tail Bound — the Largest Eigenvalue of an Independent Sum Is Controlled by the Sum of the Matrix Cumulant Generating FunctionsResearch Paper

Motivation

Sums of independent random matrices appear wherever a large matrix is built from random pieces: sample covariance matrices in statistics, random sparsification and sampling in numerical linear algebra, random graphs and their Laplacians, and compressed sensing. The basic question is how far the largest eigenvalue of such a sum can stray above its typical value. For sums of independent real random variables the answer is given by the classical inequalities of Chernoff, Hoeffding and Bernstein, all derived by the Laplace transform method: bound the tail by the moment generating function, and use independence to factor the moment generating function of the sum.

Ahlswede and Winter (2002) showed that a matrix analogue of the Laplace transform method exists, and Oliveira (2010) refined the starting inequality. Tropp's paper (arXiv:1004.4389) replaced the Ahlswede–Winter decoupling step by a consequence of Lieb's concavity theorem (Lieb 1973) and obtained a single master tail bound from which matrix versions of the Gaussian-series, Chernoff, Bernstein and Azuma inequalities follow with sharp variance parameters. This mission formalizes that master bound, the first of five missions covering the paper.

Timeline:

  • 1973: Lieb proves concavity of A↦tr⁡exp⁡(H+log⁡A)A\mapsto \operatorname{tr}\exp(H+\log A)A↦trexp(H+logA) on positive-definite matrices; Epstein gives a second proof (Epstein 1973).
  • 2002: Ahlswede and Winter introduce the matrix Laplace transform method, decoupling summands with the Golden–Thompson inequality.
  • 2010: Oliveira's variant of the matrix Laplace transform bound.
  • 2010–2012: Tropp derives the master bound for independent sums from Lieb's theorem (journal version: Found. Comput. Math. 12 (2012)); in 2011 he also derives Lieb's theorem from the joint convexity of quantum relative entropy (arXiv:1101.1070).

Setting

All matrices are d×dd\times dd×d arrays of complex numbers with d≥1d\ge1d≥1. A matrix AAA is self-adjoint (Hermitian) when A=A∗A=A^*A=A∗; it then has real eigenvalues, and λmax⁡(A)\lambda_{\max}(A)λmax​(A) denotes the largest one. For a function f:R→Rf:\mathbb R\to\mathbb Rf:R→R and a self-adjoint A=QΛQ∗A=Q\Lambda Q^*A=QΛQ∗ with QQQ unitary and Λ\LambdaΛ diagonal, f(A):=Qf(Λ)Q∗f(A):=Qf(\Lambda)Q^*f(A):=Qf(Λ)Q∗. This defines the matrix exponential eAe^{A}eA of every self-adjoint matrix and the matrix logarithm log⁡A\log AlogA of every positive-definite matrix, with log⁡(eA)=A\log(e^A)=Alog(eA)=A. The trace exponential is A↦tr⁡eAA\mapsto\operatorname{tr}e^{A}A↦treA.

A random self-adjoint matrix is a measurable map XXX from a probability space (Ω,F,P)(\Omega,\mathcal F,\mathbb P)(Ω,F,P) to the self-adjoint matrices. Its expectation EX\mathbb E XEX is the matrix of the expectations of its entries. A finite sequence X1,…,XnX_1,\dots,X_nX1​,…,Xn​ is independent when the maps are jointly independent. The matrix moment generating function and matrix cumulant generating function of XXX are

MX(θ):=E eθX,ΞX(θ):=log⁡E eθX,θ∈R,M_X(\theta):=\mathbb E\,e^{\theta X},\qquad \Xi_X(\theta):=\log\mathbb E\,e^{\theta X},\qquad\theta\in\mathbb R,MX​(θ):=EeθX,ΞX​(θ):=logEeθX,θ∈R,

which may fail to exist for some θ\thetaθ. In the Lean development these objects are lambdaMax, mexp, mlog, trExp and mean in the namespace MatrixTail.Master.

Formalization targets

Goal: the master tail bound (Theorem 3.6)

For independent random self-adjoint matrices X1,…,XnX_1,\dots,X_nX1​,…,Xn​ and every t∈Rt\in\mathbb Rt∈R,

P{λmax⁡(∑kXk)≥t}≤inf⁡θ>0{e−θt⋅tr⁡exp⁡(∑klog⁡E eθXk)}.\mathbb P\Bigl\{\lambda_{\max}\Bigl(\sum_k X_k\Bigr)\ge t\Bigr\}\le\inf_{\theta>0}\Bigl\{e^{-\theta t}\cdot\operatorname{tr}\exp\Bigl(\sum_k\log\mathbb E\,e^{\theta X_k}\Bigr)\Bigr\}.P{λmax​(k∑​Xk​)≥t}≤θ>0inf​{e−θt⋅trexp(k∑​logEeθXk​)}.

It contains no constants and no assumption beyond independence: every later inequality of the paper specializes it.

Milestones

  1. Proposition 3.1 (Laplace transform method): P{λmax⁡(Y)≥t}≤inf⁡θ>0{e−θt Etr⁡eθY}\mathbb P\{\lambda_{\max}(Y)\ge t\}\le\inf_{\theta>0}\{e^{-\theta t}\,\mathbb E\operatorname{tr}e^{\theta Y}\}P{λmax​(Y)≥t}≤infθ>0​{e−θtEtreθY}.
  2. Theorem 3.2 (Lieb): for fixed self-adjoint HHH, A↦tr⁡exp⁡(H+log⁡A)A\mapsto\operatorname{tr}\exp(H+\log A)A↦trexp(H+logA) is concave on the positive-definite cone.
  3. Corollary 3.3: Etr⁡exp⁡(H+X)≤tr⁡exp⁡(H+log⁡E eX)\mathbb E\operatorname{tr}\exp(H+X)\le\operatorname{tr}\exp(H+\log\mathbb E\,e^{X})Etrexp(H+X)≤trexp(H+logEeX).
  4. Lemma 3.4 (subadditivity of matrix cgfs): Etr⁡exp⁡(∑kθXk)≤tr⁡exp⁡(∑klog⁡E eθXk)\mathbb E\operatorname{tr}\exp(\sum_k\theta X_k)\le\operatorname{tr}\exp(\sum_k\log\mathbb E\,e^{\theta X_k})Etrexp(∑k​θXk​)≤trexp(∑k​logEeθXk​) for θ∈R\theta\in\mathbb Rθ∈R.

Significance

The master bound reduces every tail estimate for λmax⁡\lambda_{\max}λmax​ of an independent sum to semidefinite bounds on the individual cumulant generating functions. The paper's matrix Gaussian and Rademacher series bound, matrix Chernoff inequality and matrix Bernstein inequality are each one such bound away from it, and the matrix Bernstein inequality in particular is a standard tool in randomized numerical linear algebra, matrix completion and covariance estimation. Missions II–IV of this series take the master bound as their first milestone.

All results here are proved in the literature. What remains is formalization: none of Lieb's concavity theorem, the matrix Laplace transform bound or the subadditivity of matrix cumulant generating functions is in Mathlib, and a machine-checked Lieb theorem would be reusable throughout quantum information theory (strong subadditivity of entropy, joint convexity of relative entropy).

Difficulty

The scalar argument factors Eexp⁡(∑kθXk)=∏kE eθXk\mathbb E\exp(\sum_k\theta X_k)=\prod_k\mathbb E\,e^{\theta X_k}Eexp(∑k​θXk​)=∏k​EeθXk​, which needs ea+b=eaebe^{a+b}=e^ae^bea+b=eaeb. For non-commuting matrices eA+B≠eAeBe^{A+B}\ne e^Ae^BeA+B=eAeB, so this step fails. The Golden–Thompson inequality tr⁡eA+H≤tr⁡(eAeH)\operatorname{tr}e^{A+H}\le\operatorname{tr}(e^Ae^H)treA+H≤tr(eAeH) handles two summands but its three-matrix analogue is false, so it does not iterate. Lieb's concavity theorem is the deep input; it does not follow from elementary properties of the exponential, which is neither operator monotone nor operator convex. On the formal side, the matrix functional calculus of Mathlib carries little of the trace-function theory the statements rely on.

Formalization scope

Matrices are Matrix (Fin d) (Fin d) ℂ with [NeZero d] wherever λmax⁡\lambda_{\max}λmax​ appears; for d=0d=0d=0 the largest eigenvalue would be 000 and the bound would fail at t≤0t\le0t≤0. Exponential and logarithm are Mathlib's continuous functional calculus cfc. Random matrices are measurable maps for the Borel σ-algebra on the entries, independence is iIndepFun, and P is a probability measure. Expectation is entrywise.

The paper's standing assumption that expectations exist is made explicit and only where an expectation is taken: every entry of eθXke^{\theta X_k}eθXk​ is integrable for the θ\thetaθ in question. The infimum over θ>0\theta>0θ>0 is stated as the bound for every θ>0\theta>0θ>0 at which the moment generating functions exist; since an inequality p≤inf⁡θF(θ)p\le\inf_\theta F(\theta)p≤infθ​F(θ) is equivalent to p≤F(θ)p\le F(\theta)p≤F(θ) for every θ\thetaθ, and the paper treats a non-existent moment generating function as +∞+\infty+∞, this is exact. A real-valued infimum over θ\thetaθ, or dropping the integrability hypotheses, would make the statements trivially true through Lean's default values (inf⁡\infinf of an unbounded set and the integral of a non-integrable function are 000); the formalization rules both out.

Useful infrastructure beyond this mission: trace inequalities for cfc on Hermitian matrices, monotonicity of the trace exponential in the semidefinite order, and Lieb's concavity theorem itself. Contributions of any of these as standalone lemmas are welcome.

Selected references

  • J. A. Tropp, User-Friendly Tail Bounds for Sums of Random Matrices, arXiv:1004.4389v7 (2011); Found. Comput. Math. 12 (2012) 389–434. https://arxiv.org/abs/1004.4389, https://doi.org/10.1007/s10208-011-9099-z
  • R. Ahlswede and A. Winter, Strong converse for identification via quantum channels, IEEE Trans. Inform. Theory 48(3) (2002) 569–579. https://arxiv.org/abs/quant-ph/0012127
  • R. I. Oliveira, Sums of random Hermitian matrices and an inequality by Rudelson, Electron. Commun. Probab. 15 (2010) 203–212. https://arxiv.org/abs/1004.3821
  • E. H. Lieb, Convex trace functions and the Wigner–Yanase–Dyson conjecture, Adv. Math. 11 (1973) 267–288. https://doi.org/10.1016/0001-8708(73)90011-X
  • H. Epstein, Remarks on two theorems of E. Lieb, Comm. Math. Phys. 31 (1973) 317–325. https://doi.org/10.1007/BF01646492
  • J. A. Tropp, From joint convexity of quantum relative entropy to a concavity theorem of Lieb, Proc. Amer. Math. Soc. 140 (2012) 1757–1760. https://arxiv.org/abs/1101.1070
6 thms2 active usersReviewed
Numerical AnalysisOptimization·Captain: mikedeng1

Sparsity Constrained Nonlinear Optimization: Optimality Conditions and Algorithms IV: Accumulation Points of the Partial Sparse-Simplex Method Are L2(f)-Stationary PointsResearch Paper

Motivation

Many problems in signal processing, statistics and machine learning ask for a minimizer of a smooth loss among vectors with few nonzero entries: compressed sensing with a nonlinear measurement model, sparse regression with a non-quadratic loss, sparse phase retrieval. The common abstraction is the sparsity constrained problem

(P)min⁡ f(x)s.t.∥x∥0≤s,(\mathrm P)\qquad \min\ f(x)\quad\text{s.t.}\quad \|x\|_0\le s,(P)min f(x)s.t.∥x∥0​≤s,

where fff is continuously differentiable but not necessarily convex. The constraint set is a finite union of linear subspaces, so (P) is nonconvex and in general NP-hard, and its solutions are not characterized by the classical KKT theory.

Beck and Eldar (SIAM J. Optim. 2013, arXiv:1203.4580) introduced a hierarchy of necessary optimality conditions for (P) and matched each condition with an algorithm whose limit points satisfy it. Iterative hard thresholding (Blumensath and Davies 2008) reaches LLL-stationarity for L>L(f)L>L(f)L>L(f); the greedy sparse-simplex method reaches coordinate-wise minimality, but each of its iterations calls up to O(sn)O(sn)O(sn) one-dimensional minimizations. This mission formalizes the paper's compromise between the two: the partial sparse-simplex method, which examines only two candidate moves per saturated iteration, and whose limit points are L2(f)L_2(f)L2​(f)-stationary.

Setting

Vectors live in Rn\mathbb R^nRn with the Euclidean norm; eie_iei​ is the iii-th unit vector. For x∈Rnx\in\mathbb R^nx∈Rn:

  • the ℓ0\ell_0ℓ0​ norm ∥x∥0\|x\|_0∥x∥0​ is the number of nonzero components of xxx;
  • the support is I1(x)={i:xi≠0}I_1(x)=\{i: x_i\ne0\}I1​(x)={i:xi​=0}, and I0(x)={i:xi=0}I_0(x)=\{i: x_i=0\}I0​(x)={i:xi​=0} is its complement;
  • Cs={x:∥x∥0≤s}C_s=\{x:\|x\|_0\le s\}Cs​={x:∥x∥0​≤s} is the feasible set, for an integer 0<s<n0<s<n0<s<n;
  • Ms(x)M_s(x)Ms​(x) is the sss-th largest of ∣x1∣,…,∣xn∣|x_1|,\dots,|x_n|∣x1​∣,…,∣xn​∣, counted with multiplicity; Ms(x)=0M_s(x)=0Ms​(x)=0 exactly when ∥x∥0<s\|x\|_0<s∥x∥0​<s.

The objective fff is continuously differentiable and bounded below (Assumption 1, standing throughout the paper). Assumption 2 asks that ∇f\nabla f∇f be Lipschitz with some constant L(f)L(f)L(f). A constant L2L_2L2​ satisfies the local Lipschitz condition (2.15) if for every pair i≠ji\ne ji=j, every xxx and every ddd supported in {i,j}\{i,j\}{i,j},

∥∇i,jf(x)−∇i,jf(x+d)∥≤L2∥d∥,∇i,jf(x)=(∇if(x),∇jf(x)).\big\|\nabla_{i,j}f(x)-\nabla_{i,j}f(x+d)\big\|\le L_2\|d\|,\qquad \nabla_{i,j}f(x)=(\nabla_if(x),\nabla_jf(x)).​∇i,j​f(x)−∇i,j​f(x+d)​≤L2​∥d∥,∇i,j​f(x)=(∇i​f(x),∇j​f(x)).

The paper's local Lipschitz constant L2(f)=max⁡i≠jLi,j(f)L_2(f)=\max_{i\ne j}L_{i,j}(f)L2​(f)=maxi=j​Li,j​(f) satisfies it, and L2(f)≤L(f)L_2(f)\le L(f)L2​(f)≤L(f).

The projection PCs(y)P_{C_s}(y)PCs​​(y) is the set of points of CsC_sCs​ nearest to yyy. For L>0L>0L>0, a point x∗x^*x∗ is an LLL-stationary point (Definition 2.3) if

x∗∈Csandx∗∈PCs ⁣(x∗−1L∇f(x∗)).[NCL]x^*\in C_s\quad\text{and}\quad x^*\in P_{C_s}\!\Big(x^*-\tfrac1L\nabla f(x^*)\Big).\qquad[\mathrm{NC}_L]x∗∈Cs​andx∗∈PCs​​(x∗−L1​∇f(x∗)).[NCL​]

The partial sparse-simplex method (p. 25) starts at x0∈Csx^0\in C_sx0∈Cs​. If ∥xk∥0<s\|x^k\|_0<s∥xk∥0​<s, it moves to the best point xk+teix^k+te_ixk+tei​ over all iii and ttt if that strictly decreases fff, and stops otherwise. If ∥xk∥0=s\|x^k\|_0=s∥xk∥0​=s, it compares two candidates and takes the better one, preferring the second on ties:

  1. re-optimize one support coordinate: xk+Tk1eik1x^k+T^1_ke_{i^1_k}xk+Tk1​eik1​​, the best point xk+teix^k+te_ixk+tei​ over i∈I1(xk)i\in I_1(x^k)i∈I1​(xk), t∈Rt\in\mathbb Rt∈R;
  2. swap: zero out the support coordinate mkm_kmk​ of smallest absolute value and optimize along the off-support coordinate ik2i^2_kik2​ with the largest ∣∇if(xk)∣|\nabla_if(x^k)|∣∇i​f(xk)∣, giving xk−xmkkemk+Tk2eik2x^k-x^k_{m_k}e_{m_k}+T^2_ke_{i^2_k}xk−xmk​k​emk​​+Tk2​eik2​​.

Formalization targets

Goal: Theorem 3.4

Under Assumption 2, with L2>0L_2>0L2​>0 satisfying (2.15), every accumulation point x∗x^*x∗ of a sequence generated by the partial sparse-simplex method satisfies

x∗∈PCs ⁣(x∗−1L2∇f(x∗)),x^*\in P_{C_s}\!\Big(x^*-\frac1{L_2}\nabla f(x^*)\Big),x∗∈PCs​​(x∗−L2​1​∇f(x∗)),

that is, x∗x^*x∗ is an L2(f)L_2(f)L2​(f)-stationary point.

Milestones

  1. Lemma 2.6 (Local Descent Lemma). For every ddd supported in two coordinates,
f(x+d)≤f(x)+∇f(x)Td+L22∥d∥2.f(x+d)\le f(x)+\nabla f(x)^Td+\frac{L_2}{2}\|d\|^2 .f(x+d)≤f(x)+∇f(x)Td+2L2​​∥d∥2.
  1. (4.10). If ∥xk∥0=s\|x^k\|_0=s∥xk∥0​=s, then f(xk)−f(xk+1)≥12L2max⁡i∈I1(xk)(∇if(xk))2f(x^k)-f(x^{k+1})\ge\frac1{2L_2}\max_{i\in I_1(x^k)}(\nabla_if(x^k))^2f(xk)−f(xk+1)≥2L2​1​maxi∈I1​(xk)​(∇i​f(xk))2.
  2. (4.13). If ∥xk∥0=s\|x^k\|_0=s∥xk∥0​=s, then
f(xk)−f(xk+1)≥Ms(xk)[max⁡i∈I0(xk)∣∇if(xk)∣−L2Ms(xk)]+xmkk∇mkf(xk).f(x^k)-f(x^{k+1})\ge M_s(x^k)\Big[\max_{i\in I_0(x^k)}|\nabla_if(x^k)|-L_2M_s(x^k)\Big]+x^k_{m_k}\nabla_{m_k}f(x^k).f(xk)−f(xk+1)≥Ms​(xk)[i∈I0​(xk)max​∣∇i​f(xk)∣−L2​Ms​(xk)]+xmk​k​∇mk​​f(xk).
  1. Lemma 4.1. f(xk)−f(xk+1)≥12L2max⁡i(∇if(xk))2f(x^k)-f(x^{k+1})\ge\frac1{2L_2}\max_i(\nabla_if(x^k))^2f(xk)−f(xk+1)≥2L2​1​maxi​(∇i​f(xk))2 when ∥xk∥0<s\|x^k\|_0<s∥xk∥0​<s (4.6), and f(xk)−f(xk+1)≥A(xk)f(x^k)-f(x^{k+1})\ge A(x^k)f(xk)−f(xk+1)≥A(xk) when ∥xk∥0=s\|x^k\|_0=s∥xk∥0​=s (4.7), with
A(x)=max⁡{12L2max⁡i∈I1(x)(∇if(x))2, Ms(x)[max⁡i∈I0(x)∣∇if(x)∣−max⁡i∈I1(x)∣∇if(x)∣−L2Ms(x)]}.A(x)=\max\Big\{\frac1{2L_2}\max_{i\in I_1(x)}(\nabla_if(x))^2,\ M_s(x)\Big[\max_{i\in I_0(x)}|\nabla_if(x)|-\max_{i\in I_1(x)}|\nabla_if(x)|-L_2M_s(x)\Big]\Big\}.A(x)=max{2L2​1​i∈I1​(x)max​(∇i​f(x))2, Ms​(x)[i∈I0​(x)max​∣∇i​f(x)∣−i∈I1​(x)max​∣∇i​f(x)∣−L2​Ms​(x)]}.
  1. Lemma 2.2. For L>0L>0L>0, [NCL][\mathrm{NC}_L][NCL​] holds iff ∥x∥0≤s\|x\|_0\le s∥x∥0​≤s, ∣∇if(x)∣≤LMs(x)|\nabla_if(x)|\le LM_s(x)∣∇i​f(x)∣≤LMs​(x) on I0(x)I_0(x)I0​(x) and ∇if(x)=0\nabla_if(x)=0∇i​f(x)=0 on I1(x)I_1(x)I1​(x).

Significance

The theorem shows that a cheap index-selection rule does not cost optimality strength relative to iterative hard thresholding: every limit point satisfies [NCL2(f)][\mathrm{NC}_{L_2(f)}][NCL2​(f)​], and since L2(f)≤L(f)<LL_2(f)\le L(f)<LL2​(f)≤L(f)<L, this is a stronger necessary condition than the [NCL][\mathrm{NC}_L][NCL​] guaranteed by IHT with stepsize 1/L1/L1/L. In the paper's numerical comparison (Example 3.3 contd., Table 3) the method performs much better than IHT and only slightly worse than the greedy method, at a fraction of the greedy method's cost per iteration. The decrease estimates of Lemma 4.1 are the quantitative content: they turn each iteration into a lower bound on the objective decrease in terms of the violation of L2L_2L2​-stationarity.

The results are proved in the paper; to our knowledge none is machine-checked. This mission produces a formal model of the method (with its selection rules as inequality predicates, so every run is covered), the local descent lemma for two-sparse directions, and a checked proof of Theorem 3.4. The printed proof of the case ∥x∗∥0<s\|x^*\|_0<s∥x∗∥0​<s contains two gaps (see Difficulty); a formal proof settles the argument.

Difficulty

The decrease estimates follow from the local descent lemma applied at well-chosen trial points, but passing to the limit is delicate. When ∥x∗∥0=s\|x^*\|_0=s∥x∗∥0​=s, the supports of the subsequence eventually coincide with I1(x∗)I_1(x^*)I1​(x∗) and AAA becomes continuous there; when ∥x∗∥0<s\|x^*\|_0<s∥x∗∥0​<s, the iterates along the subsequence may still have sss nonzeros, and A(xk)→0A(x^k)\to0A(xk)→0 does not by itself force ∇f(x∗)=0\nabla f(x^*)=0∇f(x∗)=0, because Ms(xk)→0M_s(x^k)\to0Ms​(xk)→0 kills the second term of AAA. The swap move optimizes along a single off-support coordinate ik2i^2_kik2​, chosen by the derivative at xkx^kxk and not at the shifted point xk−xmkkemkx^k-x^k_{m_k}e_{m_k}xk−xmk​k​emk​​ where the optimization happens. The printed display (4.19) claims the bound for the maximum over all of I0(xk)I_0(x^k)I0​(xk) at the shifted point, which the argument does not give, and the final display takes a minimum of two bounds that each hold on only one class of indices. Theorem 3.4 itself is not affected, but a complete proof cannot follow those two displays as printed.

Formalization scope

Lean works in EuclideanSpace ℝ (Fin n) (indices 0,…,n−10,\dots,n-10,…,n−1), with fff of class C1C^1C1 and ∇f\nabla f∇f = gradient f. Conventions fixed by the formalization:

  • 0<s<n0<s<n0<s<n, so I1(x)I_1(x)I1​(x) and I0(x)I_0(x)I0​(x) are nonempty whenever ∥x∥0=s\|x\|_0=s∥x∥0​=s.
  • L2L_2L2​ is any constant with 0<L20<L_20<L2​ satisfying (2.15), read with ddd supported in {i,j}\{i,j\}{i,j}; the paper's L2(f)L_2(f)L2​(f) is one such constant. Positivity is required because (4.6), (4.10) and AAA divide by L2L_2L2​.
  • Assumption 1 and Assumption 2 (LipschitzWith Lf (gradient f)) are hypotheses.
  • The method's minimizers and maximizers are inequality predicates, not computed values; the theorem holds for every run. A STOP is modelled by xk+1=xkx^{k+1}=x^kxk+1=xk.
  • Two misprints of the printed box (arXiv v1) are corrected: "for every i∈I1(x∗)i\in I_1(x^*)i∈I1​(x∗)" is read as I1(xk)I_1(x^k)I1​(xk), and "ik1∈argmax⁡{fi}i^1_k\in\operatorname{argmax}\{f_i\}ik1​∈argmax{fi​}" as argmin, as the prose on p. 24 and the proof of (4.10) require. With the literal argmax the goal is not what the paper proves.
  • Maxima over index sets are suprema in R≥0\mathbb R_{\ge0}R≥0​, equal to the maxima on nonempty sets.
  • "Accumulation point" is MapClusterPt xstar atTop x.
  • Theorem numbers and page numbers are those of the arXiv v1 source (arXiv:1203.4580v1), which is the file this mission cites; the published SIAM version is typeset differently.

The run predicate is satisfiable and does not force a STOP: on n=2n=2n=2, s=1s=1s=1, f(x)=(x1−1)2+x22f(x)=(x_1-1)^2+x_2^2f(x)=(x1​−1)2+x22​, the constant sequence at (1,0)(1,0)(1,0) is a run. The conclusion is the projection condition itself, not the coordinate form (2.5), so it cannot be met by an empty or degenerate reading of stationarity.

Reusable parts: the local descent lemma for two-sparse directions, Lemma 2.2 (the coordinate characterization of [NCL][\mathrm{NC}_L][NCL​], shared with the IHT mission of this series), and the order statistic MsM_sMs​. Contributions of proofs for any milestone are welcome, as is the companion result Lemma 3.3 (limit points are BF vectors without Assumption 2).

Selected references

  • A. Beck, Y. C. Eldar, Sparsity Constrained Nonlinear Optimization: Optimality Conditions and Algorithms, SIAM J. Optim. 23(3), 2013. https://doi.org/10.1137/120869778 (source used: arXiv:1203.4580v1, https://arxiv.org/abs/1203.4580v1)
  • T. Blumensath, M. E. Davies, Iterative thresholding for sparse approximations, J. Fourier Anal. Appl. 14(5), 2008. https://doi.org/10.1007/s00041-008-9035-z
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Convex OptimizationMachine LearningOptimization·Captain: mikedeng1

Making Gradient Descent Optimal for Strongly Convex Stochastic Optimization 2: For F Smooth at the Optimum, SGD's Last and Averaged Iterates Attain 2µG²/(λ²T) and 16µG²/(λ²T)Research Paper

Motivation

Stochastic gradient descent (SGD) is the standard method for minimizing an expected loss F(w)=Ez[ℓ(w,z)]F(w) = \mathbb E_z[\ell(w, z)]F(w)=Ez​[ℓ(w,z)] when only noisy gradients are available: in machine learning, www is a predictor, zzz a random example, and each step uses the gradient of the loss on one fresh example. When FFF is strongly convex, as for regularized learning problems such as the SVM, the minimax-optimal error after TTT oracle calls is of order 1/T1/T1/T. Rakhlin, Shamir and Sridharan (arXiv:1109.5647, ICML 2012) asked whether plain SGD attains this rate, or whether the O(log⁡T/T)O(\log T/T)O(logT/T) bound known for averaged SGD is the truth.

Their §3 settles the case where FFF is in addition smooth at its minimizer: both the last iterate and the average of all iterates attain O(1/T)O(1/T)O(1/T), with explicit constants. This mission formalizes that section.

Timeline of the relevant bounds:

  • 2007–2009. Hazan, Agarwal and Kale (doi:10.1007/s10994-007-5016-8) show O(log⁡T)O(\log T)O(logT) regret for online gradient descent on strongly convex losses, which by online-to-batch conversion gives O(log⁡T/T)O(\log T/T)O(logT/T) for the averaged SGD iterate.
  • 2009. Nemirovski, Juditsky, Lan and Shapiro (doi:10.1137/070704277) give an O(1/T)O(1/T)O(1/T) bound for the last iterate when FFF is strongly convex and smooth.
  • 2011. Hazan and Kale (arXiv:1006.2425) obtain O(1/T)O(1/T)O(1/T) for strongly convex, possibly non-smooth FFF with a modified algorithm.
  • 2012. Rakhlin, Shamir and Sridharan prove the O(1/T)O(1/T)O(1/T) bounds of this mission for SGD under smoothness at the optimum only, show the log⁡T\log TlogT is real for averaged SGD on non-smooth problems, and recover O(1/T)O(1/T)O(1/T) with suffix averaging.

Setting

Let W⊆RdW \subseteq \mathbb R^dW⊆Rd be a closed convex set containing 000, let F:Rd→RF : \mathbb R^d \to \mathbb RF:Rd→R, and let DDD be a probability distribution on a measurable space Z\mathcal ZZ.

  • FFF is λ\lambdaλ-strongly convex on WWW, λ>0\lambda > 0λ>0: for all w,w′∈Ww, w' \in Ww,w′∈W and every subgradient ggg of FFF at www, F(w′)≥F(w)+⟨g,w′−w⟩+λ2∥w′−w∥2F(w') \ge F(w) + \langle g, w' - w\rangle + \frac{\lambda}{2}\|w' - w\|^2F(w′)≥F(w)+⟨g,w′−w⟩+2λ​∥w′−w∥2 (equation (1)).
  • FFF attains its minimum over WWW at w∗∈Ww^* \in Ww∗∈W.
  • A stochastic subgradient oracle is a measurable map g:Rd×Z→Rdg : \mathbb R^d \times \mathcal Z \to \mathbb R^dg:Rd×Z→Rd such that, for every w∈Ww \in Ww∈W, the mean Ez∼D[g(w,z)]\mathbb E_{z \sim D}[g(w, z)]Ez∼D​[g(w,z)] is a subgradient of FFF at www relative to WWW, and Ez∼D∥g(w,z)∥2≤G2\mathbb E_{z\sim D}\|g(w,z)\|^2 \le G^2Ez∼D​∥g(w,z)∥2≤G2.
  • FFF is μ\muμ-smooth with respect to w∗w^*w∗ if
F(w)−F(w∗)≤μ2∥w−w∗∥2for all w∈W.(2)F(w) - F(w^*) \le \frac{\mu}{2}\|w - w^*\|^2 \qquad \text{for all } w \in W. \tag{2}F(w)−F(w∗)≤2μ​∥w−w∗∥2for all w∈W.(2)

Projected SGD with step sizes ηt=1/(λt)\eta_t = 1/(\lambda t)ηt​=1/(λt) starts at w1=0w_1 = 0w1​=0, draws z1,z2,⋯∼Dz_1, z_2, \dots \sim Dz1​,z2​,⋯∼D independently and sets

wt+1=ΠW(wt−ηt g(wt,zt)),w_{t+1} = \Pi_W\big(w_t - \eta_t\, g(w_t, z_t)\big),wt+1​=ΠW​(wt​−ηt​g(wt​,zt​)),

where ΠW\Pi_WΠW​ is the Euclidean projection onto WWW. The averaged iterate is wˉT=(w1+⋯+wT)/T\bar w_T = (w_1 + \dots + w_T)/TwˉT​=(w1​+⋯+wT​)/T. In Lean the run is UnderstandingML.sgdStrongIterates lam W g S and the average UnderstandingML.sgdStrongAverage lam W g S, for a sample S : Fin T → Z drawn from UnderstandingML.iidLaw D T.

Formalization targets

Goal: Theorem 2 (averaged iterate)

If FFF is λ\lambdaλ-strongly convex and μ\muμ-smooth with respect to w∗w^*w∗, then for every T≥1T \ge 1T≥1

E[F(wˉT)−F(w∗)]≤16 μG2λ2T.\mathbb E\big[F(\bar w_T) - F(w^*)\big] \le \frac{16\,\mu G^2}{\lambda^2 T}.E[F(wˉT​)−F(w∗)]≤λ2T16μG2​.

Milestones

  1. Lemma 2. If E∥g(w,z)∥2≤G2\mathbb E\|g(w,z)\|^2 \le G^2E∥g(w,z)∥2≤G2 at a point w∈Ww \in Ww∈W, then ∥w−w∗∥2≤4G2/λ2\|w - w^*\|^2 \le 4G^2/\lambda^2∥w−w∗∥2≤4G2/λ2.
  2. Lemma 1. For every T≥1T \ge 1T≥1, E∥wT−w∗∥2≤4G2/(λ2T)\mathbb E\|w_T - w^*\|^2 \le 4G^2/(\lambda^2 T)E∥wT​−w∗∥2≤4G2/(λ2T), without smoothness.
  3. Theorem 1 (last iterate). Under smoothness, E[F(wT)−F(w∗)]≤2μG2/(λ2T)\mathbb E[F(w_T) - F(w^*)] \le 2\mu G^2/(\lambda^2 T)E[F(wT​)−F(w∗)]≤2μG2/(λ2T).
  4. Averaged-iterate distance (App. B.3). For every T≥1T \ge 1T≥1, E∥wˉT−w∗∥2≤32G2/(λ2T)\mathbb E\|\bar w_T - w^*\|^2 \le 32G^2/(\lambda^2 T)E∥wˉT​−w∗∥2≤32G2/(λ2T), without smoothness.

The constants are the paper's. Theorem 1 is a companion of the goal rather than a step of its proof; both rest on Lemma 1.

Significance

The result. Theorem 2 shows that the log⁡T\log TlogT factor in the standard bound for averaged SGD is not needed when FFF grows at most quadratically away from its minimizer. Condition (2) holds for logistic and least-squares regression and, in general, for linear predictors with losses that have Lipschitz-continuous gradients. Together with the paper's Theorem 4, which shows that the log⁡T\log TlogT factor is unavoidable for averaged SGD on some non-smooth problems, it locates where the extra logarithm comes from. Lemma 1 is the paper's key lemma: an O(1/T)O(1/T)O(1/T) bound on the expected squared distance of the last iterate that needs no smoothness, and it is reused in the paper's suffix-averaging analysis.

Formalizing it. All results are proved in the paper; none is formalized. The platform has UnderstandingML.sgd_strongly_convex (Shalev-Shwartz and Ben-David, Theorem 14.11), the classical (ρ2/(2λT))(1+log⁡T)(\rho^2/(2\lambda T))(1 + \log T)(ρ2/(2λT))(1+logT) bound for the same averaged iterate without smoothness. This mission adds the O(1/T)O(1/T)O(1/T) bounds under (2), on the same SGD run, together with a reusable expected-distance bound for the projected iterates.

Difficulty

The obvious route to Theorem 2 is to apply smoothness to each iterate, use Lemma 1, and average: by Jensen, E[F(wˉT)]−F(w∗)≤1T∑t2μG2λ2t\mathbb E[F(\bar w_T)] - F(w^*) \le \frac{1}{T}\sum_t \frac{2\mu G^2}{\lambda^2 t}E[F(wˉT​)]−F(w∗)≤T1​∑t​λ2t2μG2​, which is of order log⁡T/T\log T/TlogT/T. Removing the logarithm requires controlling E∥wˉT−w∗∥2\mathbb E\|\bar w_T - w^*\|^2E∥wˉT​−w∗∥2 directly, where the iterates are dependent and the cross terms E⟨wˉt−w∗,wt+1−w∗⟩\mathbb E\langle \bar w_t - w^*, w_{t+1} - w^*\rangleE⟨wˉt​−w∗,wt+1​−w∗⟩ do not vanish. The resulting recursion is nonlinear in E∥wˉt−w∗∥2\mathbb E\|\bar w_t - w^*\|^2E∥wˉt​−w∗∥2, and an induction with the constant 323232 fails at its first step unless the base case uses the sharper bound of Lemma 2. On the formal side, the expectations are over the product of TTT independent samples, and each one-step argument needs the independence of ztz_tzt​ from wtw_twt​ and the measurability of the projected iterates.

Formalization scope

  • Space. The paper's Hilbert space is specialized to Rd\mathbb R^dRd with the Euclidean norm (UnderstandingML.Vec d).
  • Domain. Convex ℝ W, IsClosed W (so the projection exists; tacit in the paper) and 0 ∈ W (the paper's initialization).
  • Strong convexity is Mathlib's StrongConvexOn W lam F with 0 < lam. Combined with relative subgradients, it gives (1).
  • Oracle. OptimalSGD.Suffix.IsSubgradientOracleOn W F D g (the series' shared oracle predicate): for w∈Ww \in Ww∈W, g w is integrable and its mean is a subgradient of FFF at www relative to WWW. Measurable (Function.uncurry g) and a probability measure DDD are assumed. The second-moment bound holds at every w∈Ww \in Ww∈W, which is the paper's "regardless of how the iterates evolve".
  • Smoothness is (2) exactly (IsSmoothWrt W F μ wstar), with μ≥0\mu \ge 0μ≥0. It is not a Lipschitz-gradient assumption, and FFF need not be differentiable.
  • Indexing. Iterates are indexed from 000. The paper's wTw_TwT​ is sgdStrongIterates lam W g S (T - 1), and wˉT\bar w_TwˉT​ averages indices 0,…,T−10,\dots,T-10,…,T−1. Statements quantify over T≥1T \ge 1T≥1, including T=1T = 1T=1 (wˉ1=w1=0\bar w_1 = w_1 = 0wˉ1​=w1​=0).
  • Expectations. Bounds on ∥⋅∥2\|\cdot\|^2∥⋅∥2 use the lower Lebesgue integral. Bounds on FFF use the Bochner integral, and the integrability of F(wT)F(w_T)F(wT​) or F(wˉT)F(\bar w_T)F(wˉT​) is part of the conclusion.

A statement whose Bochner integral is not shown to be integrable would hold vacuously, because non-integrable functions integrate to 000; the integrability conjuncts rule this out. The run and the average are the published Understanding Machine Learning definitions, so the bounds here apply to the same object as UnderstandingML.sgd_strongly_convex.

Needed infrastructure: measurability of the projected iterates in the sample, independence of ztz_tzt​ from wtw_twt​ under the product measure, conditional unbiasedness of the oracle along the run, non-expansiveness of the projection (available as UnderstandingML.projection_lemma), and an elementary induction on the scalar recursions. Contributions of these as standalone lemmas are welcome, and they are reusable for mission 1 of this series (suffix averaging) and for other projected-SGD analyses.

Selected references

  • A. Rakhlin, O. Shamir, K. Sridharan, Making Gradient Descent Optimal for Strongly Convex Stochastic Optimization, ICML 2012; arXiv:1109.5647v7. https://arxiv.org/abs/1109.5647
  • E. Hazan, A. Agarwal, S. Kale, Logarithmic regret algorithms for online convex optimization, Machine Learning 69, 2007. https://doi.org/10.1007/s10994-007-5016-8
  • A. Nemirovski, A. Juditsky, G. Lan, A. Shapiro, Robust stochastic approximation approach to stochastic programming, SIAM J. Optim. 19(4), 2009. https://doi.org/10.1137/070704277
  • E. Hazan, S. Kale, Beyond the regret minimization barrier: an optimal algorithm for stochastic strongly-convex optimization, COLT 2011; arXiv:1006.2425. https://arxiv.org/abs/1006.2425
  • S. Shalev-Shwartz, S. Ben-David, Understanding Machine Learning: From Theory to Algorithms, Cambridge University Press, 2014, §14.4.4. https://doi.org/10.1017/CBO9781107298019
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Convex OptimizationOperations ResearchOptimization·Captain: mikedeng1

Self-Scaled Barriers and Interior-Point Methods for Convex Programming II: A Long Step of the Conic Karmarkar Method Lowers the Potential by at Least (‖p‖²/|p|²)(1 − ln 2) ≥ 1 − ln 2Research Paper

Motivation

Karmarkar's projective method (1984) was the first interior-point algorithm for linear programming with a polynomial bound that was also fast in practice. Its analysis rests on a potential function that combines the logarithm of the objective gap with a logarithmic barrier: if every iteration lowers the potential by a fixed constant, then the gap shrinks geometrically. Nesterov and Nemirovskii (1994, §4.3) carried the method over to general convex cones with self-concordant barriers, but only with short steps, which move a fraction of the way to the boundary of a ball in the local norm.

Nesterov and Todd (1997) introduced self-scaled barriers, the class behind the cones of linear, second-order cone and semidefinite programming. They used it to allow long steps, which go a large fraction of the way to the boundary of the cone itself. Section 7.1 of that paper analyses the Karmarkar method with long steps on a self-scaled cone. It shows that the potential decrease per iteration is at least the absolute constant 1−ln⁡21-\ln 21−ln2, independent of the barrier parameter, as in the linear-programming case. This mission formalizes that analysis.

Timeline:

  • 1984, Karmarkar: projective method for linear programming, with potential decrease per step bounded below by a constant.
  • 1986, Anstreicher: a strengthened acceptance criterion for approximate projections in Karmarkar's algorithm for standard linear programming, containing the result that Lemma 7.1 of the 1997 paper generalizes (p. 28).
  • 1994, Nesterov–Nemirovskii, Interior-Point Polynomial Algorithms in Convex Programming, §4.3: the extension to self-concordant barriers on general cones, short steps.
  • 1997, Nesterov–Todd: self-scaled barriers and long steps (this paper, Theorem 7.2).

Setting

Let E=RnE=\mathbb R^nE=Rn with inner product ⟨⋅,⋅⟩\langle\cdot,\cdot\rangle⟨⋅,⋅⟩, which identifies the dual space E∗E^*E∗ with EEE. Let K⊆EK\subseteq EK⊆E be a closed convex cone with nonempty interior that contains no line, and let K∗={s:⟨s,x⟩≥0 ∀x∈K}K^*=\{s:\langle s,x\rangle\ge0\ \forall x\in K\}K∗={s:⟨s,x⟩≥0 ∀x∈K} be its dual cone. A ν\nuν-self-scaled barrier F:int⁡K→RF:\operatorname{int}K\to\mathbb RF:intK→R is a self-concordant barrier that is logarithmically homogeneous, F(τx)=F(x)−νln⁡τF(\tau x)=F(x)-\nu\ln\tauF(τx)=F(x)−νlnτ, and satisfies the two scaling conditions of Definition 2.1 of the paper. F′F'F′ and F′′F''F′′ are its gradient and Hessian.

Two measures of a direction p∈Ep\in Ep∈E at x∈int⁡Kx\in\operatorname{int}Kx∈intK are used:

  • the local norm ∥p∥x=⟨F′′(x)p,p⟩1/2\|p\|_x=\langle F''(x)p,p\rangle^{1/2}∥p∥x​=⟨F′′(x)p,p⟩1/2;
  • the σ-measure σx(p)=min⁡{β≥0:βx−p∈K}\sigma_x(p)=\min\{\beta\ge0:\beta x-p\in K\}σx​(p)=min{β≥0:βx−p∈K}, and the uniform norm ∣p∣x=max⁡{σx(p),σx(−p)}|p|_x=\max\{\sigma_x(p),\sigma_x(-p)\}∣p∣x​=max{σx​(p),σx​(−p)}.

The point x−αpx-\alpha px−αp stays in int⁡K\operatorname{int}KintK exactly when α σx(p)<1\alpha\,\sigma_x(p)<1ασx​(p)<1.

The problem is in Karmarkar form:

(P)min⁡ ⟨c,x⟩s.t.Bx=0,  ⟨d,x⟩=1,  x∈K,(P)\qquad\min\ \langle c,x\rangle\quad\text{s.t.}\quad Bx=0,\ \ \langle d,x\rangle=1,\ \ x\in K,(P)min ⟨c,x⟩s.t.Bx=0,  ⟨d,x⟩=1,  x∈K,

with B:E→RmB:E\to\mathbb R^mB:E→Rm linear and surjective and d∈K∗d\in K^*d∈K∗. Its dual is max⁡{ζ:B∗y+dζ+s=c, s∈K∗}\max\{\zeta: B^*y+d\zeta+s=c,\ s\in K^*\}max{ζ:B∗y+dζ+s=c, s∈K∗}. The standing assumptions are that (P) and the dual have strictly feasible points, and that ⟨c,⋅⟩\langle c,\cdot\rangle⟨c,⋅⟩ is not constant on the feasible set of (P). The optimal value is ζ∗\zeta^*ζ∗. The method decreases the potential

Φ(x;ζ)=νln⁡⟨c−ζd,x⟩+F(x),\Phi(x;\zeta)=\nu\ln\langle c-\zeta d,x\rangle+F(x),Φ(x;ζ)=νln⟨c−ζd,x⟩+F(x),

which is homogeneous of degree 000 in xxx.

One iteration starts from a strictly feasible x^\hat xx^ and a lower bound ζ^≤ζ∗\hat\zeta\le\zeta^*ζ^​≤ζ∗:

  1. Put c^=c+⟨c,x^⟩νF′(x^)\hat c=c+\frac{\langle c,\hat x\rangle}{\nu}F'(\hat x)c^=c+ν⟨c,x^⟩​F′(x^) and d^=d+⟨d,x^⟩νF′(x^)\hat d=d+\frac{\langle d,\hat x\rangle}{\nu}F'(\hat x)d^=d+ν⟨d,x^⟩​F′(x^). Let p(c)p(c)p(c), p(d)p(d)p(d) be their projections into ker⁡B\ker BkerB with respect to F′′(x^)F''(\hat x)F′′(x^): Bp(u)=0Bp(u)=0Bp(u)=0 and B∗y(u)+F′′(x^)p(u)=u^B^*y(u)+F''(\hat x)p(u)=\hat uB∗y(u)+F′′(x^)p(u)=u^ (7.3).
  2. Put x~(ζ)=⟨c−ζd,x^⟩νx^+p(c)−ζp(d)\tilde x(\zeta)=\frac{\langle c-\zeta d,\hat x\rangle}{\nu}\hat x+p(c)-\zeta p(d)x~(ζ)=ν⟨c−ζd,x^⟩​x^+p(c)−ζp(d) (7.4). If x~(ζ^)∉int⁡K\tilde x(\hat\zeta)\notin\operatorname{int}Kx~(ζ^​)∈/intK, keep ζ+=ζ^\zeta^+=\hat\zetaζ+=ζ^​. Otherwise raise the bound to ζ+=ζ^+1/σx~(ζ^)(p(d)+x^/ν)\zeta^+=\hat\zeta+1/\sigma_{\tilde x(\hat\zeta)}(p(d)+\hat x/\nu)ζ+=ζ^​+1/σx~(ζ^​)​(p(d)+x^/ν) (7.6).
  3. Take the direction p=p(c)−ζ+p(d)p=p(c)-\zeta^+p(d)p=p(c)−ζ+p(d) (7.5) and the new point x+=x^−αpx^+=\hat x-\alpha px+=x^−αp.

Formalization targets

Goal: Theorem 7.2 (p. 28)

For a suitable α>0\alpha>0α>0, the point x+=x^−αpx^+=\hat x-\alpha px+=x^−αp lies in {x∈int⁡K:Bx=0}\{x\in\operatorname{int}K:Bx=0\}{x∈intK:Bx=0} and

Φ(x+;ζ+)≤Φ(x^;ζ^)−∥p∥x^2∣p∣x^2(1−ln⁡2)≤Φ(x^;ζ^)−(1−ln⁡2).(7.9)\Phi(x^+;\zeta^+)\le\Phi(\hat x;\hat\zeta)-\frac{\|p\|_{\hat x}^2}{|p|_{\hat x}^2}(1-\ln2)\le\Phi(\hat x;\hat\zeta)-(1-\ln2).\qquad(7.9)Φ(x+;ζ+)≤Φ(x^;ζ^​)−∣p∣x^2​∥p∥x^2​​(1−ln2)≤Φ(x^;ζ^​)−(1−ln2).(7.9)

The goal asserts the existence of the step, not a particular step size, so it does not commit to the step chosen in the proof.

Milestones

  • Lemma 7.1 (p. 27): ζ+≤ζ∗\zeta^+\le\zeta^*ζ+≤ζ∗, and ⟨c,x^⟩−ζ+≤ν σx^(−p)\langle c,\hat x\rangle-\zeta^+\le\nu\,\sigma_{\hat x}(-p)⟨c,x^⟩−ζ+≤νσx^​(−p) (7.7).
  • (7.8) (p. 28): ∥p∥x^2=⟨c−ζ+d,p⟩\|p\|_{\hat x}^2=\langle c-\zeta^+d,p\rangle∥p∥x^2​=⟨c−ζ+d,p⟩.

Companion: Theorem 7.1 (p. 26)

With Kˉ={x∈K:Bx=0, ⟨c,x⟩≤max⁡(⟨c,x0⟩,0)+1, ⟨d,x⟩≤1}\bar K=\{x\in K:Bx=0,\ \langle c,x\rangle\le\max(\langle c,x_0\rangle,0)+1,\ \langle d,x\rangle\le1\}Kˉ={x∈K:Bx=0, ⟨c,x⟩≤max(⟨c,x0​⟩,0)+1, ⟨d,x⟩≤1} and F‾\underline FF​ the minimum of FFF over it: if Φ(x;ζ)≤Φ(x0;ζ0)−Δ\Phi(x;\zeta)\le\Phi(x_0;\zeta_0)-\DeltaΦ(x;ζ)≤Φ(x0​;ζ0​)−Δ with ζ∈[ζ0,ζ∗]\zeta\in[\zeta_0,\zeta^*]ζ∈[ζ0​,ζ∗] and Δ\DeltaΔ large enough, then

⟨c,x⟩−ζ≤(⟨c,x0⟩−ζ0) e(F(x0)−F‾)/ν e−Δ/ν.(7.2)\langle c,x\rangle-\zeta\le(\langle c,x_0\rangle-\zeta_0)\,e^{(F(x_0)-\underline F)/\nu}\,e^{-\Delta/\nu}.\qquad(7.2)⟨c,x⟩−ζ≤(⟨c,x0​⟩−ζ0​)e(F(x0​)−F​)/νe−Δ/ν.(7.2)

Significance

Theorem 7.2 together with Theorem 7.1 gives the O(νln⁡(1/ϵ))O(\nu\ln(1/\epsilon))O(νln(1/ϵ)) iteration bound of the long-step conic Karmarkar method. The decrease constant 1−ln⁡21-\ln21−ln2 does not depend on ν\nuν or on the cone. The finer bound ∥p∥2∣p∣2(1−ln⁡2)\frac{\|p\|^2}{|p|^2}(1-\ln 2)∣p∣2∥p∥2​(1−ln2) can be much larger than 1−ln⁡21-\ln 21−ln2, since ∥p∥x≥∣p∣x\|p\|_x\ge|p|_x∥p∥x​≥∣p∣x​ always holds. This explains why long steps outperform short ones in practice. Lemma 7.1 shows that the lower bound obtained from dual information is valid and tight enough to drive the analysis. The paper presents it as a generalization of a result of Anstreicher (1986) for standard linear programming.

The results are proved in the paper; none of them is formalized anywhere. A formal development checks the interplay of the lower-bound update with the σ-measure and the homogeneity of Φ\PhiΦ, which the paper treats briefly. It also records a correction: on p. 27 the paper prints c^=c−⟨c,x^⟩νF′(x^)\hat c=c-\frac{\langle c,\hat x\rangle}{\nu}F'(\hat x)c^=c−ν⟨c,x^⟩​F′(x^) (and likewise d^\hat dd^). The paper's own surrounding identities, in particular ⟨u^,x^⟩=0\langle\hat u,\hat x\rangle=0⟨u^,x^⟩=0 on p. 28, require the sign "+++", and the formalization uses "+++".

Difficulty

The obvious argument bounds the change of FFF along x−αpx-\alpha px−αp with self-concordance in the local norm. That argument only controls steps with α∥p∥x^<1\alpha\|p\|_{\hat x}<1α∥p∥x^​<1, and it gives a decrease that degrades with the step length. The long step goes up to 1/σx^(p)1/\sigma_{\hat x}(p)1/σx^​(p), which can be much larger. Reaching it requires the long-step barrier bound for self-scaled barriers (Theorem 4.2 of the paper, stated in another mission of this series). That bound controls F(x−αp)F(x-\alpha p)F(x−αp) through σx(p)\sigma_x(p)σx​(p) instead of ∥p∥x\|p\|_x∥p∥x​.

The second obstacle is the linear term. The decrease in νln⁡⟨c−ζ+d,⋅⟩\nu\ln\langle c-\zeta^+d,\cdot\rangleνln⟨c−ζ+d,⋅⟩ must be compared with ∥p∥2\|p\|^2∥p∥2, which needs both the identity (7.8) and the gap bound (7.7). The gap bound is the step at which the lower-bound update is essential: without the update, ⟨c,x^⟩−ζ^\langle c,\hat x\rangle-\hat\zeta⟨c,x^⟩−ζ^​ is not bounded by νσx^(−p)\nu\sigma_{\hat x}(-p)νσx^​(−p).

Formalization scope

The Lean development reuses the published self-scaled setting of the series SelfScaledIPM (IsProperCone, IsSelfScaledBarrier, hess, lnorm, sigma, absn) and ConvexOptimization.dualCone. Conventions:

  • E=E=E= EuclideanSpace ℝ (Fin n), with E∗E^*E∗ identified with EEE.
  • F′′F''F′′ is assumed nondegenerate on int⁡K\operatorname{int}KintK. This follows from the other axioms for a pointed cone.
  • The conjugate barrier is a supremum over int⁡K\operatorname{int}KintK.
  • ν≥1\nu\ge1ν≥1 is a binder. The paper derives it from pointedness on p. 3.
  • ζ∗\zeta^*ζ∗ is a real infimum, made finite by the strict dual feasibility assumption, which every statement carries. Nonconstancy of the objective is stated as the existence of two feasible points with different objective values.
  • The projections p(c)p(c)p(c), p(d)p(d)p(d) are data satisfying (7.3), not chosen by a selection function. The lower-bound update and the direction are definitions computed from them.
  • The goal adds the conjunct ⟨c−ζ+d,x+⟩>0\langle c-\zeta^+d,x^+\rangle>0⟨c−ζ+d,x+⟩>0, so that the logarithm in Φ(x+;ζ+)\Phi(x^+;\zeta^+)Φ(x+;ζ+) is genuine. It does not assert ⟨d,x+⟩=1\langle d,x^+\rangle=1⟨d,x+⟩=1, which the paper notes may fail.
  • Identity (7.8) is stated for every real ζ\zetaζ, which contains the page's ζ=ζ+\zeta=\zeta^+ζ=ζ+.
  • F‾\underline FF​ is an infimum over Kˉ∩int⁡K\bar K\cap\operatorname{int}KKˉ∩intK, where the barrier is finite.
  • c^\hat cc^ and d^\hat dd^ carry the corrected sign "+++".

A statement with ζ+\zeta^+ζ+ an arbitrary real, or with ppp an arbitrary vector, would be false or vacuous. The statements here fix both by the page's construction (7.3)–(7.6), and the logarithm in Φ\PhiΦ is guarded by the positivity conjunct.

A proof needs the long-step barrier inequality (Theorem 4.2), the monotonicity facts of Proposition 4.1, K∗=F′′(v)KK^*=F''(v)KK∗=F′′(v)K (Theorem 3.1 (iii)), and ∥p(u)∥w2=⟨u,p(u)⟩\|p(u)\|^2_w=\langle u,p(u)\rangle∥p(u)∥w2​=⟨u,p(u)⟩ (Proposition 6.2). These are milestones of the other missions of this series, and contributions proving them are reusable here. Elementary facts about σ\sigmaσ (positive homogeneity, the boundary characterization x−αp∈∂Kx-\alpha p\in\partial Kx−αp∈∂K at α=1/σx(p)\alpha=1/\sigma_x(p)α=1/σx​(p)) are useful beyond this mission.

Selected references

  • Yu. E. Nesterov and M. J. Todd, Self-scaled barriers and interior-point methods for convex programming, Mathematics of Operations Research 22(1), 1997, 1–42. https://doi.org/10.1287/moor.22.1.1
  • N. Karmarkar, A new polynomial-time algorithm for linear programming, Combinatorica 4, 1984, 373–395. https://doi.org/10.1007/BF02579150
  • K. M. Anstreicher, A strengthened acceptance criterion for approximate projections in Karmarkar's algorithm, Operations Research Letters 5, 1986, 211–214. https://www.sciencedirect.com/journal/operations-research-letters/vol/5
  • Yu. Nesterov and A. Nemirovskii, Interior-Point Polynomial Algorithms in Convex Programming, SIAM, 1994. https://doi.org/10.1137/1.9781611970791
  • Yu. E. Nesterov and M. J. Todd, Primal-dual interior-point methods for self-scaled cones, SIAM Journal on Optimization 8(2), 1998, 324–364. https://doi.org/10.1137/S1052623495290209
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Self-Scaled Barriers and Interior-Point Methods for Convex Programming III: An Affine Potential-Reduction Step Lowers the Potential by at Least 1 − ln 2, and by (‖p‖²/|p|²)(1 − ln 2) When µ ≥ 2νResearch Paper

Motivation

Potential-reduction methods solve a linear or conic program by driving down a single merit function that combines the objective gap with a barrier for the constraint cone. For linear programming the primal version goes back to Karmarkar (1984) and, without Karmarkar's special problem form, to Gonzaga (1990, Math. Programming 49, 7–21), whose method reduces the potential by a constant at every step while updating a lower bound on the optimal value. Nesterov and Nemirovskii (1994) extended such methods to general convex cones with self-concordant barriers, but their analysis only allows short steps: steps confined to a ball of the local norm, which in practice is a small fraction of the way to the boundary.

Nesterov and Todd (1997) singled out the self-scaled cones (the nonnegative orthant, the second-order cone, the cone of positive semidefinite matrices, and their products) and showed that for them long steps are admissible. This mission formalizes their extension of Gonzaga's method (§7.2 of the paper): a primal potential-reduction step, with a lower-bound update, that decreases the potential by a constant and, when the potential parameter is large enough, by an amount that scales with how far the step can go.

Setting

Let E=RnE = \mathbb R^nE=Rn with its inner product, identified with its dual E∗E^*E∗. Let K⊆EK \subseteq EK⊆E be a closed convex pointed cone with nonempty interior, and FFF a ν\nuν-self-scaled barrier for KKK: a ν\nuν-self-concordant logarithmically homogeneous barrier (F(τx)=F(x)−νln⁡τF(\tau x) = F(x) - \nu\ln\tauF(τx)=F(x)−νlnτ) such that for all w,x∈int⁡Kw, x \in \operatorname{int} Kw,x∈intK the Hessian satisfies F′′(w)x∈int⁡K∗F''(w)x \in \operatorname{int} K^*F′′(w)x∈intK∗ and F∗(F′′(w)x)=F(x)−2F(w)−νF_*(F''(w)x) = F(x) - 2F(w) - \nuF∗​(F′′(w)x)=F(x)−2F(w)−ν, where K∗K^*K∗ is the dual cone and F∗F_*F∗​ the conjugate barrier. Here ν≥1\nu \ge 1ν≥1.

The problem is

(P)min⁡ ⟨c,x⟩s.t.Ax=b, x∈K,(P)\qquad \min\ \langle c, x\rangle \quad\text{s.t.}\quad Ax = b,\ x \in K,(P)min ⟨c,x⟩s.t.Ax=b, x∈K,

with A:E→RmA : E \to \mathbb R^mA:E→Rm linear and surjective, and dual (D)(D)(D): max⁡⟨b,y⟩\max \langle b, y\ranglemax⟨b,y⟩ s.t. A∗y+s=cA^*y + s = cA∗y+s=c, s∈K∗s \in K^*s∈K∗. Both have strictly feasible points: S0(P)={x∈int⁡K:Ax=b}S^0(P) = \{x \in \operatorname{int}K : Ax = b\}S0(P)={x∈intK:Ax=b} and S0(D)S^0(D)S0(D) are nonempty, and the objective is not constant on the feasible region of (P)(P)(P). Let ζ∗\zeta^*ζ∗ be the optimal value.

At x∈int⁡Kx \in \operatorname{int}Kx∈intK the local norm is ∥p∥x=⟨F′′(x)p,p⟩1/2\|p\|_x = \langle F''(x)p, p\rangle^{1/2}∥p∥x​=⟨F′′(x)p,p⟩1/2, its dual is ∥u∥x∗=⟨u,[F′′(x)]−1u⟩1/2\|u\|^*_x = \langle u, [F''(x)]^{-1}u\rangle^{1/2}∥u∥x∗​=⟨u,[F′′(x)]−1u⟩1/2, and σx(p)=min⁡{β≥0:βx−p∈K}\sigma_x(p) = \min\{\beta \ge 0 : \beta x - p \in K\}σx​(p)=min{β≥0:βx−p∈K} measures how far one can move from xxx along −p-p−p: the point x−αpx - \alpha px−αp stays in int⁡K\operatorname{int}KintK for ασx(p)<1\alpha\sigma_x(p) < 1ασx​(p)<1. The uniform norm is ∣p∣x=max⁡{σx(p),σx(−p)}≤∥p∥x|p|_x = \max\{\sigma_x(p), \sigma_x(-p)\} \le \|p\|_x∣p∣x​=max{σx​(p),σx​(−p)}≤∥p∥x​.

For μ>ν\mu > \nuμ>ν and a lower bound ζ≤ζ∗\zeta \le \zeta^*ζ≤ζ∗, the primal potential is

Φ(x;ζ)=μln⁡(⟨c,x⟩−ζ)+F(x).\Phi(x;\zeta) = \mu\ln(\langle c, x\rangle - \zeta) + F(x).Φ(x;ζ)=μln(⟨c,x⟩−ζ)+F(x).

At an iterate x^∈S0(P)\hat x \in S^0(P)x^∈S0(P) with lower bound ζ^\hat\zetaζ^​, let p(c)p(c)p(c) and p(d)p(d)p(d) be the projections of ccc and of d=F′(x^)d = F'(\hat x)d=F′(x^) into ker⁡A\ker AkerA with respect to F′′(x^)F''(\hat x)F′′(x^): Ap(u)=0Ap(u) = 0Ap(u)=0, A∗y(u)+F′′(x^)p(u)=uA^*y(u) + F''(\hat x)p(u) = uA∗y(u)+F′′(x^)p(u)=u. For λ∈R\lambda \in \mathbb Rλ∈R put s~(λ)=F′′(x^)(p(c)+λp(d))−λF′(x^)\tilde s(\lambda) = F''(\hat x)(p(c) + \lambda p(d)) - \lambda F'(\hat x)s~(λ)=F′′(x^)(p(c)+λp(d))−λF′(x^). Whenever s~(λ)∈K∗\tilde s(\lambda) \in K^*s~(λ)∈K∗, the number ⟨c,x^⟩−⟨s~(λ),x^⟩\langle c, \hat x\rangle - \langle \tilde s(\lambda), \hat x\rangle⟨c,x^⟩−⟨s~(λ),x^⟩ is the value of a feasible dual solution, hence a lower bound on ζ∗\zeta^*ζ∗. The updated lower bound ζ+\zeta^+ζ+ is the larger of ζ^\hat\zetaζ^​ and the best such bound. Finally λ+=(⟨c,x^⟩−ζ+)/μ\lambda^+ = (\langle c, \hat x\rangle - \zeta^+)/\muλ+=(⟨c,x^⟩−ζ+)/μ and the search direction is p=p(c)+λ+p(d)p = p(c) + \lambda^+ p(d)p=p(c)+λ+p(d), which is λ+\lambda^+λ+ times the projected gradient of Φ(⋅;ζ+)\Phi(\cdot;\zeta^+)Φ(⋅;ζ+). Write p+=σx^(p)p_+ = \sigma_{\hat x}(p)p+​=σx^​(p).

Formalization targets

Goal: Theorem 7.4 (b), the long step

If μ≥2ν\mu \ge 2\nuμ≥2ν, there is α>0\alpha > 0α>0 with x+=x^−αp∈S0(P)x^+ = \hat x - \alpha p \in S^0(P)x+=x^−αp∈S0(P) and

Φ(x+;ζ+)≤Φ(x^;ζ^)−∥p∥x^2(max⁡{p+,∣p∣x^})2(1−ln⁡2)=Φ(x^;ζ^)−∥p∥x^2∣p∣x^2(1−ln⁡2)≤Φ(x^;ζ^)−(1−ln⁡2).\Phi(x^+;\zeta^+) \le \Phi(\hat x;\hat\zeta) - \frac{\|p\|^2_{\hat x}}{(\max\{p_+, |p|_{\hat x}\})^2}(1-\ln 2) = \Phi(\hat x;\hat\zeta) - \frac{\|p\|^2_{\hat x}}{|p|^2_{\hat x}}(1-\ln 2) \le \Phi(\hat x;\hat\zeta) - (1-\ln 2).Φ(x+;ζ+)≤Φ(x^;ζ^​)−(max{p+​,∣p∣x^​})2∥p∥x^2​​(1−ln2)=Φ(x^;ζ^​)−∣p∣x^2​∥p∥x^2​​(1−ln2)≤Φ(x^;ζ^​)−(1−ln2).

Companion: Theorem 7.4 (a), the short step

If μ≥ν+ν\mu \ge \nu + \sqrt\nuμ≥ν+ν​, there is α>0\alpha > 0α>0 with x+=x^−αp∈S0(P)x^+ = \hat x - \alpha p \in S^0(P)x+=x^−αp∈S0(P) and

Φ(x+;ζ+)≤Φ(x^;ζ^)−∥p∥x^2(max⁡{p+,∥p∥x^})2(1−ln⁡2)=Φ(x^;ζ^)−(1−ln⁡2).\Phi(x^+;\zeta^+) \le \Phi(\hat x;\hat\zeta) - \frac{\|p\|^2_{\hat x}}{(\max\{p_+, \|p\|_{\hat x}\})^2}(1-\ln 2) = \Phi(\hat x;\hat\zeta) - (1-\ln 2).Φ(x+;ζ+)≤Φ(x^;ζ^​)−(max{p+​,∥p∥x^​})2∥p∥x^2​​(1−ln2)=Φ(x^;ζ^​)−(1−ln2).

Milestones

  1. (§7.2, p. 31) The gap ⟨s~(λ),x^⟩=⟨−F′(x^),p(c)⟩+λ((∥F′(x^)∥x^∗)2−∥p(d)∥x^2)\langle\tilde s(\lambda), \hat x\rangle = \langle -F'(\hat x), p(c)\rangle + \lambda\big((\|F'(\hat x)\|^*_{\hat x})^2 - \|p(d)\|^2_{\hat x}\big)⟨s~(λ),x^⟩=⟨−F′(x^),p(c)⟩+λ((∥F′(x^)∥x^∗​)2−∥p(d)∥x^2​) is nondecreasing in λ\lambdaλ.
  2. (Lemma 7.2) If μ≥ν+ν\mu \ge \nu + \sqrt\nuμ≥ν+ν​ then λ+≤∥p∥x^\lambda^+ \le \|p\|_{\hat x}λ+≤∥p∥x^​; if μ≥2ν\mu \ge 2\nuμ≥2ν then λ+≤∣p∣x^\lambda^+ \le |p|_{\hat x}λ+≤∣p∣x^​.

Companion: Theorem 7.3

A total potential decrease Δ>μln⁡(⟨c,x0⟩−ζ0)+F(x0)−F‾\Delta > \mu\ln(\langle c, x_0\rangle - \zeta_0) + F(x_0) - \underline FΔ>μln(⟨c,x0​⟩−ζ0​)+F(x0​)−F​ from the starting pair (x0,ζ0)(x_0, \zeta_0)(x0​,ζ0​) forces ⟨c,x⟩−ζ≤(⟨c,x0⟩−ζ0) e(F(x0)−F‾)/μ e−Δ/μ\langle c, x\rangle - \zeta \le (\langle c, x_0\rangle - \zeta_0)\,e^{(F(x_0) - \underline F)/\mu}\,e^{-\Delta/\mu}⟨c,x⟩−ζ≤(⟨c,x0​⟩−ζ0​)e(F(x0​)−F​)/μe−Δ/μ, where F‾\underline FF​ is the minimum of FFF on a bounded truncation Kˉ\bar KKˉ of the homogenized feasible region.

Significance

Theorem 7.4 together with Theorem 7.3 gives an O(μln⁡(1/ϵ))O(\mu\ln(1/\epsilon))O(μln(1/ϵ))-iteration method for conic programming over self-scaled cones that needs only a primal strictly feasible point and a lower bound, and that, for μ=O(ν)\mu = O(\nu)μ=O(ν), matches the complexity of the short-step theory. Part (b) is the substantive claim: the step α\alphaα may go a large fraction of the way to the boundary of KKK (half way when σx^(p)=σx^(−p)\sigma_{\hat x}(p) = \sigma_{\hat x}(-p)σx^​(p)=σx^​(−p)) and the guaranteed decrease (∥p∥x^2/∣p∣x^2)(1−ln⁡2)(\|p\|^2_{\hat x}/|p|^2_{\hat x})(1 - \ln 2)(∥p∥x^2​/∣p∣x^2​)(1−ln2) is typically much larger than 1−ln⁡21 - \ln 21−ln2. This is the property that distinguishes self-scaled barriers from general self-concordant ones, for which only steps inside the local unit ball are controlled.

The results are proved in the paper. None of them, nor the long-step theory of self-scaled barriers on which they rest, is formalized in any proof assistant as far as is known.

Difficulty

The obvious approach bounds F(x^−αp)−F(x^)F(\hat x - \alpha p) - F(\hat x)F(x^−αp)−F(x^) by the self-concordance inequality, which controls FFF only for α∥p∥x^<1\alpha\|p\|_{\hat x} < 1α∥p∥x^​<1; that is the short-step regime and yields at best part (a). Part (b) requires a bound on FFF along −p-p−p valid all the way to α<1/σx^(p)\alpha < 1/\sigma_{\hat x}(p)α<1/σx^​(p), which holds for self-scaled barriers but not for self-concordant ones. The second difficulty is the interplay with the lower-bound update: the decrease of the barrier term must be paid for by the decrease of μln⁡(⟨c,x⟩−ζ+)\mu\ln(\langle c, x\rangle - \zeta^+)μln(⟨c,x⟩−ζ+), and this needs the scaling factor λ+\lambda^+λ+ of the direction to be at most ∣p∣x^|p|_{\hat x}∣p∣x^​, which in turn depends on how ζ+\zeta^+ζ+ was chosen. With an arbitrary admissible lower bound the claim fails.

Formalization scope

EEE, E∗E^*E∗ are EuclideanSpace ℝ (Fin n) identified through the inner product, and the problem data are A:Rn→LRmA : \mathbb R^n \to_L \mathbb R^mA:Rn→L​Rm surjective, bbb, ccc. The cone, the barrier, the local norms ∥⋅∥x\|\cdot\|_x∥⋅∥x​ (lnorm), ∥⋅∥x∗\|\cdot\|^*_x∥⋅∥x∗​ (dnorm), σx\sigma_xσx​ (sigma) and ∣⋅∣x|\cdot|_x∣⋅∣x​ (absn) are the published definitions of the SelfScaledIPM.ShortStep setting; the paper's starred dual norms map to dnorm at a primal point. Nondegeneracy of F′′F''F′′ is part of that barrier definition, and the conjugate barrier is an sSup over int⁡K\operatorname{int}KintK.

Standing assumptions are hypotheses of every statement: surjectivity of AAA (6.1), strict dual feasibility (6.3) (strict primal feasibility follows from the given iterate), the objective not constant on the feasible region, and ν≥1\nu \ge 1ν≥1. The optimal value ζ∗\zeta^*ζ∗ is the infimum of the objective over the feasible set, finite under these assumptions. The projections (7.12) are given as data satisfying their defining equations. The updated lower bound ζ+\zeta^+ζ+ is defined as max⁡(ζ^,sup⁡G)\max(\hat\zeta, \sup G)max(ζ^​,supG), with GGG the set of dual bounds ⟨c,x^⟩−⟨s~(λ),x^⟩\langle c, \hat x\rangle - \langle\tilde s(\lambda), \hat x\rangle⟨c,x^⟩−⟨s~(λ),x^⟩ over λ\lambdaλ with s~(λ)∈K∗\tilde s(\lambda) \in K^*s~(λ)∈K∗, and ζ+=ζ^\zeta^+ = \hat\zetaζ+=ζ^​ when GGG is empty. Because the gap is nondecreasing in λ\lambdaλ, this equals the paper's value at the minimal admissible λ\lambdaλ. "A suitable value of α\alphaα" is an existential over α>0\alpha > 0α>0, and the conclusion also asserts ⟨c,x+⟩>ζ+\langle c, x^+\rangle > \zeta^+⟨c,x+⟩>ζ+ so that the logarithm in Φ(x+;ζ+)\Phi(x^+;\zeta^+)Φ(x+;ζ+) is genuine. Kˉ\bar KKˉ and F‾\underline FF​ of Theorem 7.3 are defined explicitly, with F‾\underline FF​ the infimum of FFF over Kˉ∩int⁡K\bar K \cap \operatorname{int}KKˉ∩intK.

A statement in which ζ+\zeta^+ζ+ is an arbitrary lower bound above ζ^\hat\zetaζ^​, or ppp an arbitrary vector in ker⁡A\ker AkerA, or α\alphaα arbitrary instead of existentially chosen, would be false; the formalization fixes ζ+\zeta^+ζ+ by (7.17) and ppp by (7.14).

A complete development needs the theory of self-scaled barriers along a line (Theorem 4.2 and Proposition 4.1 of the paper, posed in the sibling mission I of this series), the projection identities (Propositions 6.2–6.3, posed in mission IV), weak conic duality, and the inequalities ⟨−F′(x),p⟩≤ν∥p∥x\langle -F'(x), p\rangle \le \sqrt\nu\|p\|_x⟨−F′(x),p⟩≤ν​∥p∥x​ and ⟨−F′(x),p⟩≤νσx(p)\langle -F'(x), p\rangle \le \nu\sigma_x(p)⟨−F′(x),p⟩≤νσx​(p). These are reusable across self-scaled interior-point methods; proofs of any of them are welcome.

Selected references

  • Yu. E. Nesterov and M. J. Todd, Self-scaled barriers and interior-point methods for convex programming, Mathematics of Operations Research 22(1), 1997, 1–42. https://doi.org/10.1287/moor.22.1.1
  • Yu. E. Nesterov and M. J. Todd, Primal-dual interior-point methods for self-scaled cones, SIAM Journal on Optimization 8(2), 1998, 324–364. https://doi.org/10.1137/S1052623495290209
  • Yu. Nesterov and A. Nemirovskii, Interior-Point Polynomial Algorithms in Convex Programming, SIAM, 1994. https://doi.org/10.1137/1.9781611970791
  • C. C. Gonzaga, Polynomial affine algorithms for linear programming, Mathematical Programming 49, 1990, 7–21 (cited as in the paper's reference list).
  • N. Karmarkar, A new polynomial-time algorithm for linear programming, Combinatorica 4, 1984, 373–395. https://doi.org/10.1007/BF02579150
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Convex OptimizationOperations ResearchOptimization·Captain: mikedeng1

Self-Scaled Barriers and Interior-Point Methods for Convex Programming IV: The Predictor-Corrector Path-Following Scheme Keeps π(τ, x) ≤ 1/4 and Multiplies τ by at Least 1 + 3/(8√ν + 2)Research Paper

Motivation

Interior-point methods solve linear, second-order cone and semidefinite programs by following a smooth curve through the interior of the feasible region. Nesterov and Nemirovskii (1994) showed that the right object to build such methods on is a self-concordant barrier for the cone, and that the number of Newton steps needed by a path-following method is governed by the barrier parameter ν\nuν. For general cones, however, their analysis of Newton's method only controls a small neighbourhood of the path, so the step in the path parameter must be short.

Nesterov and Todd (1997) singled out the cones that admit a self-scaled barrier: the nonnegative orthant, the second-order cone, the cone of positive semidefinite matrices and their products. For these cones the barrier satisfies global, long-range inequalities that general self-concordant barriers do not. Section 9 of the paper uses them to sharpen the classical primal path-following method: Newton's method converges quadratically on the whole region where the proximity measure is below 111 (extending Roos and Vial, 1992), and a predictor-corrector scheme takes a tangent step whose length adapts to the geometry of the cone at the current point.

Setting

Let E=RnE=\mathbb R^nE=Rn with its Euclidean inner product ⟨⋅,⋅⟩\langle\cdot,\cdot\rangle⟨⋅,⋅⟩; the dual space E∗E^*E∗ is identified with EEE. Let K⊂EK\subset EK⊂E be a proper cone: closed, convex, containing no line, with nonempty interior int⁡K\operatorname{int}KintK. A function F:int⁡K→RF:\operatorname{int}K\to\mathbb RF:intK→R is a ν\nuν-self-scaled barrier for KKK if it is a ν\nuν-self-concordant logarithmically homogeneous barrier (F(tx)=F(x)−νln⁡tF(tx)=F(x)-\nu\ln tF(tx)=F(x)−νlnt) and, for all w,x∈int⁡Kw,x\in\operatorname{int}Kw,x∈intK, F′′(w)x∈int⁡K∗F''(w)x\in\operatorname{int}K^*F′′(w)x∈intK∗ and F∗(F′′(w)x)=F(x)−2F(w)−νF_*(F''(w)x)=F(x)-2F(w)-\nuF∗​(F′′(w)x)=F(x)−2F(w)−ν, where F∗F_*F∗​ is the conjugate barrier (Definition 2.1). Then ν≥1\nu\ge1ν≥1.

At a point x∈int⁡Kx\in\operatorname{int}Kx∈intK the paper uses three measures of a vector p∈Ep\in Ep∈E:

  • the local norm ∥p∥x=⟨F′′(x)p,p⟩1/2\|p\|_x=\langle F''(x)p,p\rangle^{1/2}∥p∥x​=⟨F′′(x)p,p⟩1/2, and for q∈E∗q\in E^*q∈E∗ the dual norm ∥q∥x∗=⟨q,[F′′(x)]−1q⟩1/2\|q\|^*_x=\langle q,[F''(x)]^{-1}q\rangle^{1/2}∥q∥x∗​=⟨q,[F′′(x)]−1q⟩1/2;
  • σx(p)=min⁡{β≥0:βx−p∈K}\sigma_x(p)=\min\{\beta\ge0:\beta x-p\in K\}σx​(p)=min{β≥0:βx−p∈K}, the reciprocal of the largest step from xxx along −p-p−p that stays in KKK;
  • the uniform norm ∣p∣x=max⁡{σx(p),σx(−p)}|p|_x=\max\{\sigma_x(p),\sigma_x(-p)\}∣p∣x​=max{σx​(p),σx​(−p)}, which satisfies ∣p∣x≤∥p∥x|p|_x\le\|p\|_x∣p∣x​≤∥p∥x​.

The problem is min⁡{⟨c,x⟩:Ax=b, x∈K}\min\{\langle c,x\rangle: Ax=b,\ x\in K\}min{⟨c,x⟩:Ax=b, x∈K} with A:E→Y=RmA:E\to Y=\mathbb R^mA:E→Y=Rm surjective; S0(P)={x∈int⁡K:Ax=b}S^0(P)=\{x\in\operatorname{int}K:Ax=b\}S0(P)={x∈intK:Ax=b} is the set of strictly feasible points, and the dual problem is assumed strictly feasible. For w∈int⁡Kw\in\operatorname{int}Kw∈intK and u∈E∗u\in E^*u∈E∗ the system

Ap=0,A∗y+F′′(w)p=u(6.4)Ap=0,\qquad A^*y+F''(w)p=u \tag{6.4}Ap=0,A∗y+F′′(w)p=u(6.4)

defines the projection p=p(u)p=p(u)p=p(u) of uuu into ker⁡A\ker AkerA with respect to F′′(w)F''(w)F′′(w).

For τ>0\tau>0τ>0 the penalty function is ψ(τ,x)=τ⟨c,x⟩+F(x)\psi(\tau,x)=\tau\langle c,x\rangle+F(x)ψ(τ,x)=τ⟨c,x⟩+F(x); its minimizers x(τ)x(\tau)x(τ) over S0(P)S^0(P)S0(P) form the central path. The Newton direction p(τ,x)p(\tau,x)p(τ,x) is the projection of τc+F′(x)\tau c+F'(x)τc+F′(x) with respect to F′′(x)F''(x)F′′(x), and the proximity measure is π(τ,x)=∥p(τ,x)∥x\pi(\tau,x)=\|p(\tau,x)\|_xπ(τ,x)=∥p(τ,x)∥x​. The tangent direction v(x)v(x)v(x) is the projection of ccc with respect to F′′(x)F''(x)F′′(x).

One iteration of the path-following scheme (p. 39) from (τ,x)(\tau,x)(τ,x) with π(τ,x)≤1/4\pi(\tau,x)\le1/4π(τ,x)≤1/4 is:

Δτ=38∣v∣x∥v∥x,z=x−Δτ v,τ+=τ+Δτ,x+=z−p(τ+,z),v=v(x).\Delta\tau=\frac{3}{8\sqrt{|v|_x\|v\|_x}},\quad z=x-\Delta\tau\,v,\quad \tau_+=\tau+\Delta\tau,\quad x_+=z-p(\tau_+,z),\qquad v=v(x).Δτ=8∣v∣x​∥v∥x​​3​,z=x−Δτv,τ+​=τ+Δτ,x+​=z−p(τ+​,z),v=v(x).

Formalization targets

Goal: Theorem 9.3

For one iteration of the scheme, with v≠0v\ne0v=0:

z∈int⁡K,x+∈S0(P),π(τ+,x+)≤14,z\in\operatorname{int}K,\qquad x_+\in S^0(P),\qquad \pi(\tau_+,x_+)\le\tfrac14,z∈intK,x+​∈S0(P),π(τ+​,x+​)≤41​, τ+ ≥ (1+38ν+2∥v∥x∣v∣x)τ ≥ (1+38ν+2)τ.\tau_+\ \ge\ \Bigl(1+\frac{3}{8\sqrt\nu+2}\sqrt{\frac{\|v\|_x}{|v|_x}}\Bigr)\tau\ \ge\ \Bigl(1+\frac{3}{8\sqrt\nu+2}\Bigr)\tau .τ+​ ≥ (1+8ν​+23​∣v∣x​∥v∥x​​​)τ ≥ (1+8ν​+23​)τ.

By induction from π(τ0,x0)≤1/4\pi(\tau_0,x_0)\le1/4π(τ0​,x0​)≤1/4, the condition (9.3) holds at every iterate and τk\tau_kτk​ grows geometrically.

Milestones

  • Corollary 3.1: for v,z∈int⁡Kv,z\in\operatorname{int}Kv,z∈intK there is w∈int⁡Kw\in\operatorname{int}Kw∈intK with F′(v)=−F′′(w)zF'(v)=-F''(w)zF′(v)=−F′′(w)z, F′(z)=−F′′(w)vF'(z)=-F''(w)vF′(z)=−F′′(w)v, hence F′(v)−F′(z)=F′′(w)(v−z)F'(v)-F'(z)=F''(w)(v-z)F′(v)−F′(z)=F′′(w)(v−z).
  • Corollary 4.1 (iii): for such www (with F′(v)=−F′′(w)xF'(v)=-F''(w)xF′(v)=−F′′(w)x), σx(v)−1F′′(x)≤F′′(w)≤σv(x)F′′(x)\sigma_x(v)^{-1}F''(x)\le F''(w)\le\sigma_v(x)F''(x)σx​(v)−1F′′(x)≤F′′(w)≤σv​(x)F′′(x).
  • Theorem 4.3: ∥F′(v)−F′(x)−F′′(x)(v−x)∥v∗≤∣v−x∣x ∥v−x∥x\|F'(v)-F'(x)-F''(x)(v-x)\|^*_v\le|v-x|_x\,\|v-x\|_x∥F′(v)−F′(x)−F′′(x)(v−x)∥v∗​≤∣v−x∣x​∥v−x∥x​.
  • Proposition 6.2: ∥p(u)∥w2=⟨u,p(u)⟩\|p(u)\|_w^2=\langle u,p(u)\rangle∥p(u)∥w2​=⟨u,p(u)⟩.
  • Proposition 6.3: ∥p(u)∥w≤∥u−A∗y∥w∗\|p(u)\|_w\le\|u-A^*y\|^*_w∥p(u)∥w​≤∥u−A∗y∥w∗​ for all y∈Yy\in Yy∈Y, with equality only at a minimizer.
  • Theorem 9.2: if π(τ,x)<1\pi(\tau,x)<1π(τ,x)<1, the full Newton step x+=x−p(τ,x)x_+=x-p(\tau,x)x+​=x−p(τ,x) satisfies π(τ,x+)≤∣p∣x π(τ,x)≤π2(τ,x)\pi(\tau,x_+)\le|p|_x\,\pi(\tau,x)\le\pi^2(\tau,x)π(τ,x+​)≤∣p∣x​π(τ,x)≤π2(τ,x).

A companion item, Theorem 9.1, states the decrease of ψ(τ,⋅)\psi(\tau,\cdot)ψ(τ,⋅) along the damped Newton step α=1/(1+σx(p))\alpha=1/(1+\sigma_x(p))α=1/(1+σx​(p)).

Significance

Theorem 9.3 shows that the primal path-following method for self-scaled cones increases the penalty parameter by a factor at least 1+3/(8ν+2)1+3/(8\sqrt\nu+2)1+3/(8ν​+2) per iteration, which yields the O(νln⁡(1/ϵ))O(\sqrt\nu\ln(1/\epsilon))O(ν​ln(1/ϵ)) iteration bound, and that the step can be much longer when the ratio ∥v∥x/∣v∣x\|v\|_x/|v|_x∥v∥x​/∣v∣x​ is large. The paper notes that this ratio is the maximal step α∗\alpha^*α∗ along the normalized tangent direction that keeps x±α∗vˉx\pm\alpha^*\bar vx±α∗vˉ in KKK, so the rule is a "large-step" rule in disguise. Theorem 9.2 removes the restriction of the general self-concordant theory, where quadratic convergence of Newton's method is only shown on a smaller neighbourhood, by allowing any point with π(τ,x)<1\pi(\tau,x)<1π(τ,x)<1.

The milestones are general tools for self-scaled barriers. Theorem 4.3 is a global second-order estimate for the gradient, with no restriction on the distance between the two points; Corollary 3.1 is an exact mean-value identity with a single interior intermediate point; Propositions 6.2 and 6.3 are the basic facts about the projections that every algorithm of the paper computes.

None of these results has a machine-checked proof that we know of. The platform has general self-concordant Newton estimates (the contraction λ+≤(λ/(1−λ))2\lambda_+\le(\lambda/(1-\lambda))^2λ+​≤(λ/(1−λ))2 and the damped Newton decrease λ−ln⁡(1+λ)\lambda-\ln(1+\lambda)λ−ln(1+λ)), which use different measures and do not involve σx\sigma_xσx​, ∣⋅∣x|\cdot|_x∣⋅∣x​ or the constraint Ax=bAx=bAx=b.

Difficulty

The obvious route to Theorem 9.2 is the standard self-concordance argument, which compares F′′F''F′′ at the new point with F′′(x)F''(x)F′′(x) through the local norm ∥p∥x\|p\|_x∥p∥x​ alone. It gives π+≤π2/(1−π)2\pi_+\le\pi^2/(1-\pi)^2π+​≤π2/(1−π)2, which is weaker than the claimed bound and gives nothing near π=1\pi=1π=1. The sharper bound needs estimates that hold only for self-scaled barriers: a second-order remainder for the gradient measured at the new point and controlled by the uniform norm ∣⋅∣x|\cdot|_x∣⋅∣x​ (Theorem 4.3), which in turn requires the intermediate point of Corollary 3.1 and the two-sided Hessian comparison of Corollary 4.1 (iii). These fail for general self-concordant barriers, and they depend on the structure theory of §3 (Theorem 3.2 of the paper).

In Theorem 9.3 the predictor step is long in the local norm, so no estimate based on ∥v∥x\|v\|_x∥v∥x​ alone keeps the predictor point close enough to the central path for one corrector step to restore π≤1/4\pi\le1/4π≤1/4; the constant 3/83/83/8 in Δτ\Delta\tauΔτ is fixed by the page and leaves little slack.

Formalization scope

The development reuses the published setting of the 1998 Nesterov–Todd series: IsProperCone, IsSelfScaledBarrier, hess, IsPrimalStrict, IsDualStrict, lnorm (∥⋅∥x\|\cdot\|_x∥⋅∥x​), dnorm (∥⋅∥x∗\|\cdot\|^*_x∥⋅∥x∗​), sigma and absn. Its conventions are:

  1. E∗E^*E∗ is identified with E=RnE=\mathbb R^nE=Rn through the Euclidean inner product.
  2. Positive definiteness of F′′F''F′′ on int⁡K\operatorname{int}KintK is part of the barrier definition.
  3. The conjugate is a real supremum over int⁡K\operatorname{int}KintK.
  4. ν≥1\nu\ge1ν≥1 is a hypothesis.

The paper stars dual norms; the 1998 modules do not, so dnorm F x is the paper's ∥⋅∥x∗\|\cdot\|^*_x∥⋅∥x∗​.

New definitions are the projection system (6.4) (IsProjection), the penalty ψ\psiψ, the Newton and tangent systems as predicates on their solutions, and the step size Δτ\Delta\tauΔτ. Solutions of linear systems are always data satisfying these predicates, never chosen by a function. Operator inequalities are written through quadratic forms.

Every theorem of §9 assumes (6.1)–(6.3) (AAA surjective, a strictly feasible dual point), which the paper states on p. 38. Theorems 9.2 and 9.3 are stated for one iteration and state explicitly that the new points are interior, which the scheme presupposes. Theorem 9.3 assumes v(x)≠0v(x)\ne0v(x)=0: when ccc lies in the range of A∗A^*A∗ the objective is constant on the feasible set and Δτ\Delta\tauΔτ is undefined. In Theorem 9.1 the middle bound of (9.1), which divides by σx(p)\sigma_x(p)σx​(p), is stated under σx(p)>0\sigma_x(p)>0σx​(p)>0, and the outer bound in all cases.

A formalization that leaves Δτ\Delta\tauΔτ as a free positive parameter, drops the corrector step, or treats π\piπ as any number at most 1/41/41/4 that is not tied to the Newton system at the new point would state a different, weaker or vacuous theorem. The goal fixes Δτ\Delta\tauΔτ by the formula of p. 39 and bounds ∥p∥x+\|p\|_{x_+}∥p∥x+​​ for every solution of the Newton system at (τ+,x+)(\tau_+,x_+)(τ+​,x+​).

Contributions welcome: proofs of the milestones, the structure results they rest on (existence of the scaling point, Theorem 3.2; the Hessian bounds of Theorem 4.1), and reusable lemmas on σx\sigma_xσx​ and the uniform norm, which also serve the other missions of this series.

Selected references

  • Yu. E. Nesterov and M. J. Todd, Self-scaled barriers and interior-point methods for convex programming, Mathematics of Operations Research 22(1) (1997) 1–42. https://doi.org/10.1287/moor.22.1.1
  • Yu. E. Nesterov and M. J. Todd, Primal-dual interior-point methods for self-scaled cones, SIAM Journal on Optimization 8(2) (1998) 324–364. https://doi.org/10.1137/S1052623495290209
  • Yu. Nesterov and A. Nemirovskii, Interior-Point Polynomial Algorithms in Convex Programming, SIAM, 1994. https://doi.org/10.1137/1.9781611970791
  • C. Roos and J.-Ph. Vial, A polynomial method of approximate centers for linear programming, Mathematical Programming 54 (1992) 295–305.
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Control TheoryDynamical SystemsGraph Theory+1·Captain: mikedeng1

Synchronization and Transient Stability in Power Networks and Nonuniform Kuramoto Oscillators 2: λ₂(L(P_ij cos φ_ij)) > λ_critical Gives Phase Cohesiveness and Exponential Frequency SynchronizationResearch Paper

Motivation

Transient stability of a power grid asks whether the generators of the network return to synchronous operation after a large disturbance such as a fault or a line trip. In the classical network-reduced model the rotor angles obey second-order swing equations, and stability certificates usually come from energy functions evaluated numerically. Dörfler and Bullo (arXiv:0910.5673v4; SIAM J. Control Optim. 50(3), 2012) relate this problem to a first-order system of coupled phase oscillators, the non-uniform Kuramoto model, and derive purely algebraic conditions on the network parameters under which the oscillators synchronize. Such conditions read as "the network connectivity dominates non-uniformity, losses and lack of phase cohesiveness" and are checked from the data alone, without simulation.

The paper gives two such sufficient conditions. This mission formalizes the second, Theorem V.5, which measures connectivity by the algebraic connectivity of the lossless coupling and therefore applies to sparse (connected, not necessarily complete) networks. A companion mission treats Theorem V.3, the condition for complete graphs.

Timeline. For the classical Kuramoto model, Jadbabaie, Motee and Barahona (ACC, 2004) and Chopra and Spong (IEEE TAC, 2009) analysed synchronization with the Lyapunov function ∥Hθ∥22\|H\theta\|_2^2∥Hθ∥22​, and Chopra and Spong proved frequency synchronization under cohesive phases. Dörfler and Bullo (2009–2012) extended the analysis to non-uniform time constants DiD_iDi​, phase shifts φij\varphi_{ij}φij​ and non-complete graphs, using a weighted Lyapunov function.

Setting

There are n≥2n\ge2n≥2 oscillators with phases θi\theta_iθi​, time constants Di>0D_i>0Di​>0, natural frequencies ωi∈R\omega_i\in\mathbb Rωi​∈R, coupling weights Pij≥0P_{ij}\ge0Pij​≥0 and phase shifts φij∈[0,π/2[\varphi_{ij}\in[0,\pi/2[φij​∈[0,π/2[ (i≠ji\ne ji=j), with Pii=φii=0P_{ii}=\varphi_{ii}=0Pii​=φii​=0. The non-uniform Kuramoto model is

Diθ˙i=ωi−∑j=1nPijsin⁡(θi−θj+φij),i=1,…,n.(8)D_i\dot\theta_i=\omega_i-\sum_{j=1}^nP_{ij}\sin(\theta_i-\theta_j+\varphi_{ij}),\qquad i=1,\dots,n. \tag{8}Di​θ˙i​=ωi​−j=1∑n​Pij​sin(θi​−θj​+φij​),i=1,…,n.(8)

In this mission P=PTP=P^TP=PT, and its non-zero entries induce a connected graph.

  • H∈Rn(n−1)/2×nH\in\mathbb R^{n(n-1)/2\times n}H∈Rn(n−1)/2×n is the incidence matrix of the complete graph: Hθ=(θ2−θ1,… )H\theta=(\theta_2-\theta_1,\dots)Hθ=(θ2​−θ1​,…) lists all pairwise differences, and ∥Hθ∥22=∑i<j(θi−θj)2\|H\theta\|_2^2=\sum_{i<j}(\theta_i-\theta_j)^2∥Hθ∥22​=∑i<j​(θi​−θj​)2.
  • Δ(γ)\Delta(\gamma)Δ(γ) is the set of configurations contained in an open arc of length γ\gammaγ, i.e. max⁡i,j∣θi−θj∣<γ\max_{i,j}|\theta_i-\theta_j|<\gammamaxi,j​∣θi​−θj​∣<γ.
  • The Laplacian of a symmetric matrix AAA is L(aij)=diag⁡(∑jaij)−AL(a_{ij})=\operatorname{diag}(\sum_ja_{ij})-AL(aij​)=diag(∑j​aij​)−A and λ2(L(aij))\lambda_2(L(a_{ij}))λ2​(L(aij​)) is its second-smallest eigenvalue, the algebraic connectivity. The lossless coupling is the matrix (Pijcos⁡φij)(P_{ij}\cos\varphi_{ij})(Pij​cosφij​).
  • κ=∑kDk\kappa=\sum_kD_kκ=∑k​Dk​, α=min⁡i≠j{DiDj}/max⁡i≠j{DiDj}\alpha=\sqrt{\min_{i\ne j}\{D_iD_j\}/\max_{i\ne j}\{D_iD_j\}}α=mini=j​{Di​Dj​}/maxi=j​{Di​Dj​}​, φmax⁡=max⁡i,jφij\varphi_{\max}=\max_{i,j}\varphi_{ij}φmax​=maxi,j​φij​, Ω=∑iωi/∑iDi\Omega=\sum_i\omega_i/\sum_iD_iΩ=∑i​ωi​/∑i​Di​.
  • The critical value is
λcritical=∥HD−1ω∥2+n ∥[∑jP1jD1sin⁡φ1j,…,∑jPnjDnsin⁡φnj]∥2cos⁡(φmax⁡)(κ/n)α/max⁡i≠j{DiDj}.(33)\lambda_{\mathrm{critical}}=\frac{\|HD^{-1}\omega\|_2+\sqrt n\,\big\|\big[\sum_j\tfrac{P_{1j}}{D_1}\sin\varphi_{1j},\dots,\sum_j\tfrac{P_{nj}}{D_n}\sin\varphi_{nj}\big]\big\|_2}{\cos(\varphi_{\max})(\kappa/n)\alpha/\max_{i\ne j}\{D_iD_j\}}. \tag{33}λcritical​=cos(φmax​)(κ/n)α/maxi=j​{Di​Dj​}∥HD−1ω∥2​+n​​[∑j​D1​P1j​​sinφ1j​,…,∑j​Dn​Pnj​​sinφnj​]​2​​.(33)
  • The radii γmax⁡∈ ]π/2−φmax⁡,π]\gamma_{\max}\in\,]\pi/2-\varphi_{\max},\pi]γmax​∈]π/2−φmax​,π] and γmin⁡∈[0,π/2−φmax⁡[\gamma_{\min}\in[0,\pi/2-\varphi_{\max}[γmin​∈[0,π/2−φmax​[ solve sinc⁡(γmax⁡)/sinc⁡(π/2−φmax⁡)=sin⁡(γmin⁡)/cos⁡(φmax⁡)=λcritical/λ2(L(Pijcos⁡φij))\operatorname{sinc}(\gamma_{\max})/\operatorname{sinc}(\pi/2-\varphi_{\max})=\sin(\gamma_{\min})/\cos(\varphi_{\max})=\lambda_{\mathrm{critical}}/\lambda_2(L(P_{ij}\cos\varphi_{ij}))sinc(γmax​)/sinc(π/2−φmax​)=sin(γmin​)/cos(φmax​)=λcritical​/λ2​(L(Pij​cosφij​)).

Formalization targets

Goal: Theorem V.5 (Synchronization condition II)

If λ2(L(Pijcos⁡φij))>λcritical\lambda_2(L(P_{ij}\cos\varphi_{ij}))>\lambda_{\mathrm{critical}}λ2​(L(Pij​cosφij​))>λcritical​, then

  1. for every γ∈[γmin⁡,αγmax⁡]\gamma\in[\gamma_{\min},\alpha\gamma_{\max}]γ∈[γmin​,αγmax​] the set {θ∈Δ(π):∥Hθ∥2≤γ}\{\theta\in\Delta(\pi):\|H\theta\|_2\le\gamma\}{θ∈Δ(π):∥Hθ∥2​≤γ} is positively invariant, and every solution with θ(0)∈Δ(π)\theta(0)\in\Delta(\pi)θ(0)∈Δ(π), ∥Hθ(0)∥2<αγmax⁡\|H\theta(0)\|_2<\alpha\gamma_{\max}∥Hθ(0)∥2​<αγmax​ eventually satisfies ∥Hθ(t)∥2≤γ\|H\theta(t)\|_2\le\gamma∥Hθ(t)∥2​≤γ for every γ>γmin⁡\gamma>\gamma_{\min}γ>γmin​;
  2. for every such solution the frequencies converge exponentially to a common θ˙∞∈[θ˙min⁡(0),θ˙max⁡(0)]\dot\theta_\infty\in[\dot\theta_{\min}(0),\dot\theta_{\max}(0)]θ˙∞​∈[θ˙min​(0),θ˙max​(0)]; if φ≡0\varphi\equiv0φ≡0, then θ˙∞=Ω\dot\theta_\infty=\Omegaθ˙∞​=Ω and the rate is no worse than
λfe(γ)=λ2(L(Pij))cos⁡(γ)cos⁡(∠(D1,1))2/Dmax⁡(γ∈ ]γmin⁡,π/2[).\lambda_{\mathrm{fe}}(\gamma)=\lambda_2(L(P_{ij}))\cos(\gamma)\cos(\angle(D\mathbf 1,\mathbf 1))^2/D_{\max}\qquad(\gamma\in\,]\gamma_{\min},\pi/2[).λfe​(γ)=λ2​(L(Pij​))cos(γ)cos(∠(D1,1))2/Dmax​(γ∈]γmin​,π/2[).

Milestones

Lemma V.8 (the identity (36) that replaces HD−1HTHD^{-1}H^THD−1HT by κ\kappaκ), Lemma V.9 (a quadratic-form bound by λ2\lambda_2λ2​), the sinc estimate and the bound X~\tilde XX~ on the lossy coupling (p. 25), the Lyapunov-derivative bound (37), the sandwich bounds (39) on WWW, the existence and uniqueness of γmin⁡,γmax⁡\gamma_{\min},\gamma_{\max}γmin​,γmax​ from the analysis of (41), and the eventual entry of every trajectory into {∥Hθ∥2<π/2−φmax⁡}\{\|H\theta\|_2<\pi/2-\varphi_{\max}\}{∥Hθ∥2​<π/2−φmax​}.

Significance

The condition is checkable from network data: λ2\lambda_2λ2​ of a weighted Laplacian, two vector norms and the extreme time constants. It applies to sparse networks, where the complete-graph condition of Theorem V.3 does not, and specializes for classical Kuramoto oscillators to K>∥Hω∥2K>\|H\omega\|_2K>∥Hω∥2​ (Remark V.7). Through the singular-perturbation argument of Section IV, conditions of this kind certify transient stability of the network-reduced power system.

The result is proved in the paper; no machine-checked version is known. A formalization fixes several points the printed text leaves loose: the norm ∥Hθ∥2\|H\theta\|_2∥Hθ∥2​ is written on p. 23 with a double sum that counts each pair twice; the chain defining X~\tilde XX~ on p. 25 is printed with its inequalities reversed; and "reaches {∥Hθ∥2≤γmin⁡}\{\|H\theta\|_2\le\gamma_{\min}\}{∥Hθ∥2​≤γmin​}" holds only asymptotically. The formal statements make each of these precise.

Difficulty

The obvious Lyapunov function, ∥Hθ∥22\|H\theta\|_2^2∥Hθ∥22​, has a sign-indefinite derivative as soon as the DiD_iDi​ differ, because the coupling Pij/DiP_{ij}/D_iPij​/Di​ is not symmetric. The weighted function W(Hθ)=14∑i,jDiDj∣θi−θj∣2W(H\theta)=\frac14\sum_{i,j}D_iD_j|\theta_i-\theta_j|^2W(Hθ)=41​∑i,j​Di​Dj​∣θi​−θj​∣2 restores a symmetric structure, but only through the non-obvious identity (36). After that, the sinusoidal coupling has to be bounded below by a quadratic form on a set where the phase differences stay below π\piπ, the lossy coupling has to be bounded above uniformly in the state, and the resulting ultimate-boundedness argument has to be run with sublevel sets of WWW, which are ellipsoids rather than balls of ∥Hθ∥2\|H\theta\|_2∥Hθ∥2​ unless all DiD_iDi​ coincide. The constants α\alphaα, γmin⁡\gamma_{\min}γmin​, γmax⁡\gamma_{\max}γmax​ come from this mismatch, and the passage from sublevel sets back to balls is the most delicate step.

Formalization scope

  • Configurations are real lifts θ∈Rn\theta\in\mathbb R^nθ∈Rn; Δ(π)\Delta(\pi)Δ(π) means θi−θj<π\theta_i-\theta_j<\piθi​−θj​<π for all i,ji,ji,j, and ∥Hθ∥2\|H\theta\|_2∥Hθ∥2​ is the pair-sum norm. A solution is a function θ:R→Rn\theta:\mathbb R\to\mathbb R^nθ:R→Rn with right derivative at 000 and derivative at every t>0t>0t>0 equal to the vector field of (8), and statements quantify over every solution. θ˙\dot\thetaθ˙ is the vector field evaluated along the solution.
  • Added hypotheses: n≥2n\ge2n≥2 (needed for λ2\lambda_2λ2​ and the extrema over i≠ji\ne ji=j), and φij=φji\varphi_{ij}=\varphi_{ji}φij​=φji​, which the page uses silently (the lossless coupling must be a symmetric Laplacian) and which holds for power networks. Pij≥0P_{ij}\ge0Pij​≥0 off the diagonal, since §V.B allows zero weights.
  • Corrections: ∥Hθ∥2\|H\theta\|_2∥Hθ∥2​ sums over pairs i<ji<ji<j; the X~\tilde XX~ chain is stated as ∥HX∥2≤X~\|HX\|_2\le\tilde X∥HX∥2​≤X~; the attraction clause of 1) is stated as "eventually below every γ>γmin⁡\gamma>\gamma_{\min}γ>γmin​"; the rate of (19) is taken positive (it is printed with a minus sign), and the "Moreover" rate is stated for every γ∈ ]γmin⁡,π/2[\gamma\in\,]\gamma_{\min},\pi/2[γ∈]γmin​,π/2[ because (19) depends on an arc length the theorem does not name. The page's "Moreover, if γmax⁡=0\gamma_{\max}=0γmax​=0" is read as φmax⁡=0\varphi_{\max}=0φmax​=0, a misprint: γmax⁡>π/2−φmax⁡\gamma_{\max}>\pi/2-\varphi_{\max}γmax​>π/2−φmax​ is never zero.
  • γmin⁡,γmax⁡\gamma_{\min},\gamma_{\max}γmin​,γmax​ are quantified subject to their defining equations, and a milestone proves they exist and are unique, so they are not free parameters. Condition (33) is satisfiable (equal ratios ωi/Di\omega_i/D_iωi​/Di​ and φ≡0\varphi\equiv0φ≡0 give λcritical=0\lambda_{\mathrm{critical}}=0λcritical​=0), so the goal is not vacuous.
  • Source: the arXiv preprint v4 of the SICON article; every page and number refers to that preprint.
  • Infrastructure: weighted graph Laplacians, their second eigenvalue and Courant–Fischer-type bounds, incidence matrices, and ultimate-boundedness arguments for ODEs. The Laplacian and incidence-matrix layer is reusable for consensus and network-dynamics missions; contributions on any milestone are welcome.

Selected references

  • F. Dörfler, F. Bullo, Synchronization and Transient Stability in Power Networks and Nonuniform Kuramoto Oscillators, SIAM J. Control Optim. 50(3), 2012; preprint arXiv:0910.5673v4. https://arxiv.org/abs/0910.5673v4
  • N. Chopra, M. W. Spong, On exponential synchronization of Kuramoto oscillators, IEEE Trans. Automatic Control 54(2), pp. 353–357, 2009 (reference [32] of the source).
  • A. Jadbabaie, N. Motee, M. Barahona, On the stability of the Kuramoto model of coupled nonlinear oscillators, American Control Conference, Boston, 2004, pp. 4296–4301 (reference [33] of the source).
  • H. K. Khalil, Nonlinear Systems, 3rd ed., Prentice Hall, 2002 (ultimate boundedness, Theorem 4.18; reference [51] of the source).
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CombinatoricsOperations ResearchProbability+1·Captain: mikedeng1

Matroid Prophet Inequalities 1: Against Any Online Weight-Adaptive Adversary, the 2-Balanced Threshold Algorithm Earns at Least Half the Expected Max-Weight BasisResearch Paper

Motivation

The prophet inequality of optimal stopping compares a gambler, who sees independent non-negative random values X1,…,XnX_1, \dots, X_nX1​,…,Xn​ one at a time and must accept or reject each on arrival, with a prophet who sees them all in advance. Krengel, Sucheston and Garling showed that the gambler can secure E[Xτ]≥12 E[max⁡iXi]\mathbb E[X_\tau] \ge \tfrac12\,\mathbb E[\max_i X_i]E[Xτ​]≥21​E[maxi​Xi​], and Samuel-Cahn showed that a single threshold suffices. Since Hajiaghayi, Kleinberg and Sandholm (2007) and Chawla, Hartline, Malec and Sivan (2010), prophet inequalities have served as the approximation guarantees of sequential posted-price mechanisms: an online selection rule with a prophet guarantee turns into a truthful mechanism with a revenue guarantee.

The natural multi-choice generalization lets the gambler accept a set of elements, subject to a feasibility constraint. Kleinberg and Weinberg, Matroid Prophet Inequalities (STOC 2012, arXiv:1201.4764), proved that when the feasible sets are the independent sets of a matroid, the factor 12\tfrac1221​ is still achievable, by an explicit threshold rule, and even when the order of arrival is chosen adaptively by an adversary.

Timeline:

  • 1977–78: Krengel and Sucheston, with Garling: the single-choice prophet inequality with factor 12\tfrac1221​, which is tight.
  • 1984: Samuel-Cahn: a single fixed threshold attains 12\tfrac1221​.
  • 2007: Hajiaghayi, Kleinberg, Sandholm: prophet inequalities read as truthful online auctions, with multi-choice prophet inequalities.
  • 2010: Chawla, Hartline, Malec, Sivan: posted-price mechanisms via prophet inequalities, and factor 12\tfrac1221​ for matroids when the algorithm may choose the order of arrival.
  • 2012: Kleinberg–Weinberg: factor 12\tfrac1221​ for every matroid against an online weight-adaptive adversary, and 14p−2\tfrac1{4p-2}4p−21​ for intersections of ppp matroids.

Setting

Let U\mathcal UU be a finite ground set and M=(U,I)\mathcal M = (\mathcal U, \mathcal I)M=(U,I) a matroid; I\mathcal II is its family of independent sets. For each x∈Ux \in \mathcal Ux∈U a distribution FxF_xFx​ on [0,∞)[0,\infty)[0,∞) is given; the weights w(x)w(x)w(x) are independent with w(x)∼Fxw(x) \sim F_xw(x)∼Fx​, and w(A)=∑x∈Aw(x)w(A) = \sum_{x \in A} w(x)w(A)=∑x∈A​w(x). Let OPT(w)=max⁡{w(S):S∈I}\mathrm{OPT}(w) = \max\{w(S) : S \in \mathcal I\}OPT(w)=max{w(S):S∈I} and OPT=E[OPT(w)]\mathrm{OPT} = \mathbb E[\mathrm{OPT}(w)]OPT=E[OPT(w)].

An online weight-adaptive adversary reveals the elements one at a time: it picks xix_ixi​ knowing w(x1),…,w(xi−1)w(x_1), \dots, w(x_{i-1})w(x1​),…,w(xi−1​) but not w(xi)w(x_i)w(xi​). An online algorithm maintains a selected set Ai−1∈IA_{i-1} \in \mathcal IAi−1​∈I and, when xix_ixi​ arrives with its weight, irrevocably accepts or rejects it, keeping AiA_iAi​ independent. A threshold rule offers xix_ixi​ a threshold TiT_iTi​ computed from the revealed prefix (and Ti=∞T_i = \inftyTi​=∞ when Ai−1∪{xi}∉IA_{i-1} \cup \{x_i\} \notin \mathcal IAi−1​∪{xi​}∈/I) and accepts iff w(xi)≥Tiw(x_i) \ge T_iw(xi​)≥Ti​.

The algorithm of the paper uses a ghost sample: an independent copy w′w'w′ of the weights. Let BBB be a w′w'w′-maximum-weight basis. For an independent set AAA, among the partitions B=C⊔RB = C \sqcup RB=C⊔R with R∩A=∅R \cap A = \emptysetR∩A=∅ and A∪RA \cup RA∪R a basis, R(A)R(A)R(A), C(A)C(A)C(A) denote one maximizing w′(R)w'(R)w′(R). The algorithm (9) sets

Ti=12 Ew′[w′(R(Ai−1))−w′(R(Ai−1∪{xi}))].T_i = \tfrac12\,\mathbb E_{w'}\big[w'(R(A_{i-1})) - w'(R(A_{i-1}\cup\{x_i\}))\big].Ti​=21​Ew′​[w′(R(Ai−1​))−w′(R(Ai−1​∪{xi​}))].

Formalization targets

Goal: the matroid prophet inequality

For every matroid on a finite ground set, every family of distributions FxF_xFx​ on [0,∞)[0,\infty)[0,∞) with finite means, and every online weight-adaptive adversary, the set AAA selected by the algorithm (9) satisfies

E[w(A)]  ≥  12 OPT.\mathbb E[w(A)] \;\ge\; \tfrac12\,\mathrm{OPT}.E[w(A)]≥21​OPT.

The goal is stated for the paper's own algorithm, which is stronger than the existence statement of §3.

Milestones

  1. Proposition 1 (with Definition 1): any threshold rule with α\alphaα-balanced thresholds,
∑xi∈ATi≥1α E[w′(C(A))],∑xi∈VTi≤(1−1α) E[w′(R(A))],\sum_{x_i\in A} T_i \ge \tfrac1\alpha\,\mathbb E[w'(C(A))], \qquad \sum_{x_i\in V} T_i \le \big(1-\tfrac1\alpha\big)\,\mathbb E[w'(R(A))],xi​∈A∑​Ti​≥α1​E[w′(C(A))],xi​∈V∑​Ti​≤(1−α1​)E[w′(R(A))],

earns E[w(A)]≥1α OPT\mathbb E[w(A)] \ge \tfrac1\alpha\,\mathrm{OPT}E[w(A)]≥α1​OPT. 2. The identity behind (9) = (10), and the telescoping identity ∑xi∈ATi=12 E[w′(C(A))]\sum_{x_i \in A} T_i = \tfrac12\,\mathbb E[w'(C(A))]∑xi​∈A​Ti​=21​E[w′(C(A))] (Property (2) for α=2\alpha = 2α=2). 3. Lemma 1 (bijective basis exchange, and its weighted form), Lemma 2 (R(A)R(A)R(A) is a maximum-weight basis of the contraction M/A\mathcal M/AM/A), Lemma 3 (S↦w′(R(S))S \mapsto w'(R(S))S↦w′(R(S)) is submodular on subsets of an independent set). 4. Inequalities (11) and (12), and Proposition 2:

∑xi∈V[w′(R(Ai−1))−w′(R(Ai−1∪{xi}))]≤w′(R(A)),\sum_{x_i \in V}\big[w'(R(A_{i-1})) - w'(R(A_{i-1}\cup\{x_i\}))\big] \le w'(R(A)),xi​∈V∑​[w′(R(Ai−1​))−w′(R(Ai−1​∪{xi​}))]≤w′(R(A)),

pointwise in w′≥0w' \ge 0w′≥0; then Property (3) with α=2\alpha = 2α=2 for the thresholds (9).

Significance

The theorem gives the optimal constant: already for a rank-one matroid (choose one element) no online algorithm beats 12\tfrac1221​. It covers every matroid with one algorithm, including uniform, partition, graphic and transversal matroids, which model capacity, unit-demand and spanning-tree constraints. Through the reduction of Chawla et al., the paper derives from it order-oblivious posted-price mechanisms that are 2-approximations to the optimal revenue in single-parameter settings with matroid feasibility and, through the adaptive adversary, in multi-dimensional unit-demand settings (§6 of the paper). The decomposition through α\alphaα-balanced thresholds is reused in the paper for intersections of ppp matroids, with factor 14p−2\tfrac1{4p-2}4p−21​.

The result has been proved since 2012; it has not been formalized. The mission produces a machine-checked development of the model (online adaptive adversaries, threshold rules, the ghost-sample expectations), of the general reduction (Proposition 1), and of the matroid facts the algorithm relies on, notably the bijective exchange lemma (Schrijver, Corollary 39.12a), which is not in Mathlib.

Difficulty

The obvious argument fixes the order of arrival and compares the algorithm with the prophet item by item. It fails here because the order is chosen adaptively from the revealed weights, so the set of elements still to come is random and correlated with the past. The proof must instead compare the algorithm's realized selection with a ghost optimum BBB built from an independent sample, and bound the value the algorithm forgoes by the value the ghost optimum could still add, E[w′(R(A))]\mathbb E[w'(R(A))]E[w′(R(A))]. The step that needs matroid structure is Property (3): the total threshold offered to any set VVV that could still be added must be at most half of E[w′(R(A))]\mathbb E[w'(R(A))]E[w′(R(A))]. The thresholds were computed along the history A0⊆A1⊆…A_0 \subseteq A_1 \subseteq \dotsA0​⊆A1​⊆…, not at the final AAA, so the bound requires the submodularity of S↦w′(R(S))S \mapsto w'(R(S))S↦w′(R(S)) (Lemma 3) and a weight-dominating exchange between VVV and R(A)R(A)R(A) in the contraction M/A\mathcal M/AM/A. Neither holds for general downward-closed families.

Formalization scope

  • The ground set is a Fintype α; the matroid is Mathlib's Matroid α with ground set Set.univ; sets are Finset α; contraction is Matroid.contract.
  • The distributions are F : α → Measure ℝ, probability measures with F x (Set.Iio 0) = 0 (support in [0,∞)[0,\infty)[0,∞)) and Integrable id (F x) (finite means). The weight law is Measure.pi F, and every expectation is a Bochner integral over it. Finite means make OPT(w)\mathrm{OPT}(w)OPT(w), w(A)w(A)w(A) and the integrands of the thresholds integrable, so no expectation is a junk value.
  • OPT(w)\mathrm{OPT}(w)OPT(w) is a maximum over the nonempty finset of independent sets. The maximum-weight basis B(w′)B(w')B(w′) and the maximizer R(A)R(A)R(A) are fixed by choice when weights tie; Lemma 2 shows w′(R(A))w'(R(A))w′(R(A)) does not depend on the choice. R(A)R(A)R(A) is required to be disjoint from AAA, as Lemma 2's placement of R(A)R(A)R(A) in M/A\mathcal M/AM/A needs.
  • A threshold rule is a real-valued function of the current selection, the revealed list, the weights and the arriving element, non-negative, depending on the weights only through revealed ones, measurably; the value ∞\infty∞ on infeasible steps is an independence guard in the acceptance test. "Monotone algorithm" in Proposition 1 means such a rule.
  • An adversary is a deterministic map from the revealed list and the weights to the next unrevealed element, depending only on revealed weights and measurable. Randomized adversaries are mixtures of these.
  • Lemma 1, part 2 is stated for disjoint VVV and RRR: as printed it fails when they overlap, and the paper uses it only for disjoint sets.

The goal fixes the thresholds by (9) through BBB, R(⋅)R(\cdot)R(⋅) and the ghost expectation; a statement in which the thresholds are free parameters assumed to satisfy (2)–(3) would be Proposition 1 and is not the goal.

Contributions are welcome at every level: the measurability of the online run, the exchange lemma for Mathlib matroids, the greedy characterization of maximum-weight bases of a contraction, and the probabilistic core (7) of Proposition 1. The matroid lemmas are reusable beyond this mission, in particular by the matroid-intersection mission of the same paper.

Selected references

  • R. Kleinberg, S. M. Weinberg, Matroid Prophet Inequalities, STOC 2012; arXiv:1201.4764v1. https://arxiv.org/abs/1201.4764 , https://doi.org/10.1145/2213977.2213991
  • U. Krengel, L. Sucheston, Semiamarts and finite values, Bull. Amer. Math. Soc. 83, 745–747, 1977.
  • U. Krengel, L. Sucheston, On semiamarts, amarts, and processes with finite value, Advances in Probability and Related Topics 4, 197–266, 1978.
  • E. Samuel-Cahn, Comparison of threshold stop rules and maximum for independent nonnegative random variables, Annals of Probability 12(4), 1213–1216, 1984.
  • M. T. Hajiaghayi, R. Kleinberg, T. Sandholm, Automated mechanism design and prophet inequalities, AAAI 2007, pp. 58–65.
  • S. Chawla, J. Hartline, D. Malec, B. Sivan, Multi-parameter mechanism design and sequential posted pricing, STOC 2010, pp. 311–320.
  • A. Schrijver, Combinatorial Optimization: Polyhedra and Efficiency, Springer, 2003 (Corollary 39.12a).
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Harmonic AnalysisProbabilityTheoretical Computer Science·Captain: mikedeng1

Optimal Inapproximability Results for MAX-CUT and Other 2-Variable CSPs? 3: Low-Influence Functions Have Level-One Fourier Weight at Most 2/π + CδResearch Paper

Motivation

Fourier analysis of functions on the discrete cube {−1,1}n\{-1,1\}^n{−1,1}n is the main tool behind tight inapproximability results under the Unique Games Conjecture. In the MAX-CUT reduction of Khot, Kindler, Mossel and O'Donnell (SIAM J. Comput. 2007), soundness rests on the Majority Is Stablest theorem: among bounded functions in which no coordinate has large influence, the majority function is asymptotically the most noise stable. That theorem was a conjecture when the paper was written and was proved by Mossel, O'Donnell and Oleszkiewicz (Annals of Math. 2010) using an invariance principle.

Section 6.2 of the paper records special cases of Majority Is Stablest that have short, self-contained proofs. Theorem 6 is the case where the noise parameter ρ\rhoρ tends to 000. There the noise stability is dominated by the Fourier weight at level 1, and the statement says that a bounded function with small influences has level-one weight at most 2/π2/\pi2/π, up to an explicit error linear in the largest influence. Bounds on the level-one weight also appear in Talagrand's work on correlation of monotone sets (Combinatorica 1996), which the paper compares against (its Theorem 18), and the level-one inequality is a standard chapter of the analysis of Boolean functions (O'Donnell 2014).

Setting

Points of the discrete cube {−1,1}n\{-1,1\}^n{−1,1}n are sign vectors x=(x1,…,xn)x=(x_1,\dots,x_n)x=(x1​,…,xn​); following the paper, the bit TRUE is read as −1-1−1 and FALSE as 111. The cube carries the uniform probability measure, so E[g]=2−n∑xg(x)\mathbf E[g]=2^{-n}\sum_x g(x)E[g]=2−n∑x​g(x), and real functions form an inner product space with ⟨f,g⟩=E[fg]\langle f,g\rangle=\mathbf E[fg]⟨f,g⟩=E[fg].

For S⊆[n]S\subseteq[n]S⊆[n] the parity χS(x)=∏i∈Sxi\chi_S(x)=\prod_{i\in S}x_iχS​(x)=∏i∈S​xi​; the parities form an orthonormal basis, and the Fourier coefficient of fff at SSS is f^(S)=⟨f,χS⟩\hat f(S)=\langle f,\chi_S\ranglef^​(S)=⟨f,χS​⟩. The weight of fff at level 1 is

W1(f)=∑∣S∣=1f^(S)2=∑i=1nf^({i})2.W^1(f)=\sum_{|S|=1}\hat f(S)^2=\sum_{i=1}^n\hat f(\{i\})^2 .W1(f)=∣S∣=1∑​f^​(S)2=i=1∑n​f^​({i})2.

The influence of coordinate iii on fff (Definition 2) is

Infi(f)=Ex1,…,xi−1,xi+1,…,xn[Varxi[f]],\mathrm{Inf}_i(f)=\mathop{\mathbf E}_{x_1,\dots,x_{i-1},x_{i+1},\dots,x_n}\big[\mathrm{Var}_{x_i}[f]\big],Infi​(f)=Ex1​,…,xi−1​,xi+1​,…,xn​​[Varxi​​[f]],

the expected variance of fff when all coordinates but xix_ixi​ are fixed at random and xix_ixi​ is a uniform sign. The linear part of fff is ℓ(x)=∑if^({i})xi\ell(x)=\sum_i\hat f(\{i\})x_iℓ(x)=∑i​f^​({i})xi​, and ∥g∥1=E∣g∣\|g\|_1=\mathbf E|g|∥g∥1​=E∣g∣, ∥g∥2=E[g2]\|g\|_2=\sqrt{\mathbf E[g^2]}∥g∥2​=E[g2]​, ∥g∥∞=max⁡x∣g(x)∣\|g\|_\infty=\max_x|g(x)|∥g∥∞​=maxx​∣g(x)∣.

Throughout, C=2(1−2/π)≈0.404C=2\big(1-\sqrt{2/\pi}\big)\approx 0.404C=2(1−2/π​)≈0.404.

Formalization targets

Goal: Theorem 6 (p. 12)

For every nnn, every f:{−1,1}n→[−1,1]f:\{-1,1\}^n\to[-1,1]f:{−1,1}n→[−1,1] and every δ≥0\delta\ge 0δ≥0 with Infi(f)≤δ\mathrm{Inf}_i(f)\le\deltaInfi​(f)≤δ for all iii,

∑∣S∣=1f^(S)2  ≤  2π+Cδ.\sum_{|S|=1}\hat f(S)^2\;\le\;\frac{2}{\pi}+C\delta .∣S∣=1∑​f^​(S)2≤π2​+Cδ.

The constant CCC is explicit, and the goal states it exactly as printed.

Milestones (proof of Theorem 6, p. 25, and Proposition 7.2, p. 16)

  1. For fff with values in [−1,1][-1,1][−1,1]: ∑∣S∣=1f^(S)2=∥ℓ∥22=⟨f,ℓ⟩≤∥f∥∞∥ℓ∥1≤∥ℓ∥1\sum_{|S|=1}\hat f(S)^2=\|\ell\|_2^2=\langle f,\ell\rangle\le\|f\|_\infty\|\ell\|_1\le\|\ell\|_1∑∣S∣=1​f^​(S)2=∥ℓ∥22​=⟨f,ℓ⟩≤∥f∥∞​∥ℓ∥1​≤∥ℓ∥1​.
  2. The König–Schütt–Tomczak-Jaegermann bound: if ∣ai∣≤δ|a_i|\le\delta∣ai​∣≤δ for all iii and ℓ=∑iaixi\ell=\sum_i a_ix_iℓ=∑i​ai​xi​, then
∥ℓ∥1≤2/π ∥ℓ∥2+C2 δ.\|\ell\|_1\le\sqrt{2/\pi}\,\|\ell\|_2+\tfrac C2\,\delta .∥ℓ∥1​≤2/π​∥ℓ∥2​+2C​δ.
  1. The quadratic step: for X,δ≥0X,\delta\ge0X,δ≥0, X2≤2/π X+C2δX^2\le\sqrt{2/\pi}\,X+\tfrac C2\deltaX2≤2/π​X+2C​δ implies X≤1/2π+1/2π+Cδ/2X\le\sqrt{1/2\pi}+\sqrt{1/2\pi+C\delta/2}X≤1/2π​+1/2π+Cδ/2​ and X2≤2/π+CδX^2\le 2/\pi+C\deltaX2≤2/π+Cδ.
  2. Proposition 7.2: Infi(f)=∑S∋if^(S)2\mathrm{Inf}_i(f)=\sum_{S\ni i}\hat f(S)^2Infi​(f)=∑S∋i​f^​(S)2.

Significance

The result. The constant 2/π2/\pi2/π is sharp: majority on nnn variables has influences of order n−1/2n^{-1/2}n−1/2 and level-one weight tending to 2/π2/\pi2/π, which is (E∣Z∣)2(\mathbf E|Z|)^2(E∣Z∣)2 for a standard Gaussian ZZZ. Theorem 6 thus identifies the extremal level-one weight of low-influence bounded functions and gives a rate linear in the maximal influence. It is the ρ→0\rho\to0ρ→0 instance of Majority Is Stablest, obtained without the invariance principle, and level-one bounds of this type are used in hardness reductions and in the study of noise sensitivity.

Formalizing it. The milestones together give a complete formal route from bounded functions to the stated bound, except for one step discussed below. They also produce a reusable layer of Boolean Fourier analysis: Fourier coefficients, level weights, influences in their variance form and the Fourier formula for influences. Mathlib contains no development of influences or level weights on the cube, and the platform has none either; the König–Schütt–Tomczak-Jaegermann inequality, a sharp quantitative central limit bound for Rademacher sums (J. Reine Angew. Math. 1999), has no machine-checked proof.

Status. The published proof's first step, ∣f^({i})∣≤Infi(f)|\hat f(\{i\})|\le\mathrm{Inf}_i(f)∣f^​({i})∣≤Infi​(f), is valid for Boolean-valued fff but not for [−1,1][-1,1][−1,1]-valued fff; for [−1,1][-1,1][−1,1]-valued fff the statement is posed as printed. For f=c x1f=c\,x_1f=cx1​ with 0<c<10<c<10<c<1 one has f^({1})=c>c2=Inf1(f)\hat f(\{1\})=c>c^2=\mathrm{Inf}_1(f)f^​({1})=c>c2=Inf1​(f), and the argument as written then yields only 2/π+Cδ2/\pi+C\sqrt\delta2/π+Cδ​. Numerical search over small cubes has found no function violating the printed bound. A proof of the goal for bounded fff, or a counterexample, is therefore a genuine contribution.

Difficulty

The obvious argument replaces ℓ\ellℓ by a Gaussian with the same variance and uses E∣Z∣=2/π\mathbf E|Z|=\sqrt{2/\pi}E∣Z∣=2/π​. A central limit theorem with an error term is needed, and generic Berry–Esseen bounds give an additive error with a constant far from C/2C/2C/2; the exact constant 1−2/π1-\sqrt{2/\pi}1−2/π​ requires the sharp Rademacher-sum inequality, whose proof is a delicate analysis of E∣∑iaixi∣\mathbf E|\sum_ia_ix_i|E∣∑i​ai​xi​∣ as a function of the coefficients. The second obstacle is the passage from influences to coefficients. For bounded fff only f^({i})2≤Infi(f)\hat f(\{i\})^2\le\mathrm{Inf}_i(f)f^​({i})2≤Infi​(f) holds, so a bound on influences controls coefficients only at scale δ\sqrt\deltaδ​; feeding that into the chain loses the linear dependence on δ\deltaδ. Recovering the printed rate for non-Boolean fff needs an idea beyond the published proof.

Formalization scope

A point of the cube is Fin n → Bool, mapped to a sign by pm with pm true = -1 and pm false = 1. Expectations are normalised finite sums, so no measure theory is involved. A function f:{−1,1}n→[−1,1]f:\{-1,1\}^n\to[-1,1]f:{−1,1}n→[−1,1] is a real function with the hypothesis ∀ x, |f x| ≤ 1. The influence is defined as on the page, as the average over the cube of ((f(xi←1)−f(xi←−1))/2)2\big((f(x^{i\leftarrow1})-f(x^{i\leftarrow-1}))/2\big)^2((f(xi←1)−f(xi←−1))/2)2, which is the variance in xix_ixi​; it is not defined by its Fourier formula, which is a milestone. The level-one weight is ∑if^({i})2\sum_i\hat f(\{i\})^2∑i​f^​({i})2. The constant CCC is written out as 2 * (1 - Real.sqrt (2 / Real.pi)); an existentially quantified constant would be a weaker theorem. The case n=0n=0n=0 is allowed.

Two hypotheses are added and disclosed: δ≥0\delta\ge0δ≥0 in Theorem 6 and in the König–Schütt–Tomczak-Jaegermann bound. For n≥1n\ge1n≥1 each follows from the other hypotheses; for n=0n=0n=0 the influence (resp. coefficient) hypothesis is empty and δ≥0\delta\ge0δ≥0 is what the page assumes.

A trivializing formalization would drop the range hypothesis (then scaled dictators refute the bound and the statement is false), define influence through Fourier coefficients (which makes Proposition 7.2 definitional), or weaken the hypothesis of the goal to a bound on the coefficients ∣f^({i})∣≤δ|\hat f(\{i\})|\le\delta∣f^​({i})∣≤δ; none of these is used here. In particular, the goal is not strengthened to Boolean-valued fff, where the published proof applies verbatim.

Contributions welcome: proofs of Parseval-type identities for the linear part, of Proposition 7.2, of the elementary quadratic step, of the König–Schütt–Tomczak-Jaegermann inequality, and of the goal itself. The cube layer is reusable for any later formalization of Boolean function analysis.

Selected references

  • S. Khot, G. Kindler, E. Mossel, R. O'Donnell, Optimal Inapproximability Results for MAX-CUT and Other 2-Variable CSPs?, SIAM J. Comput. 37(1), 2007. https://doi.org/10.1137/S0097539705447372
  • E. Mossel, R. O'Donnell, K. Oleszkiewicz, Noise stability of functions with low influences: invariance and optimality, Annals of Mathematics 171(1), 2010. https://doi.org/10.4007/annals.2010.171.295
  • H. König, C. Schütt, N. Tomczak-Jaegermann, Projection constants of symmetric spaces and variants of Khintchine's inequality, J. Reine Angew. Math. 511, 1999. https://doi.org/10.1515/crll.1999.511.1
  • M. Talagrand, How much are increasing sets positively correlated?, Combinatorica 16(2), 1996. https://doi.org/10.1007/BF01844850
  • R. O'Donnell, Analysis of Boolean Functions, Cambridge University Press, 2014. https://arxiv.org/abs/2105.10386
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Complexity TheoryOperations ResearchTheoretical Computer Science·Captain: mikedeng1

Optimal Inapproximability Results for MAX-CUT and Other 2-Variable CSPs? 1: Assuming the Unique Games Conjecture, (1/2 − ρ/2)- versus ((arccos ρ)/π + ε)-Satisfiable MAX-CUT Is NP-Hard to DistinguishResearch Paper

Motivation

MAX-CUT asks for a partition of the vertices of a graph that cuts as many edges, or as much edge weight, as possible. It is one of Karp's original NP-hard problems and the standard test case for approximation algorithms. A uniformly random partition cuts half of the edges in expectation. Goemans and Williamson (JACM 1995) rounded a semidefinite relaxation with a random hyperplane and obtained the ratio

αGW=min⁡0<θ<πθ/π(1−cos⁡θ)/2≈0.878567.\alpha_{GW}=\min_{0<\theta<\pi}\frac{\theta/\pi}{(1-\cos\theta)/2}\approx 0.878567.αGW​=0<θ<πmin​(1−cosθ)/2θ/π​≈0.878567.

Whether a better ratio can be achieved in polynomial time was a central open question.

Timeline.

  • 1995: Goemans and Williamson give the αGW\alpha_{GW}αGW​-approximation.
  • 2001: Håstad (JACM 2001) shows, via PCPs and gadgets, that approximating MAX-CUT within 16/17+ϵ≈0.94116/17+\epsilon\approx 0.94116/17+ϵ≈0.941 is NP-hard. This remains the best unconditional bound.
  • 2002: Khot (STOC 2002) formulates the Unique Games Conjecture (UGC).
  • 2004–2007: Khot, Kindler, Mossel and O'Donnell (SIAM J. Comput. 2007) show that the UGC implies that αGW\alpha_{GW}αGW​ is optimal. Their reduction rests on the Majority Is Stablest conjecture, which they formulate.
  • 2005–2010: Mossel, O'Donnell and Oleszkiewicz (Annals of Math. 2010, arXiv:math/0503503) prove Majority Is Stablest via the invariance principle.

Setting

A Unique Label Cover instance L(V,W,E,[M],{σv,w})\mathcal L(V,W,E,[M],\{\sigma_{v,w}\})L(V,W,E,[M],{σv,w​}) is a bipartite graph with left vertices VVV, right vertices WWW and edges E⊆V×WE\subseteq V\times WE⊆V×W, together with a bijection σv,w:[M]→[M]\sigma_{v,w}:[M]\to[M]σv,w​:[M]→[M] on each edge. A labeling assigns a label in [M][M][M] to every vertex, and it satisfies (v,w)(v,w)(v,w) if σv,w(label(w))=label(v)\sigma_{v,w}(\mathrm{label}(w))=\mathrm{label}(v)σv,w​(label(w))=label(v). OPT\mathrm{OPT}OPT is the largest fraction of edges satisfied by a labeling. The Unique Games Conjecture says that for all η,γ>0\eta,\gamma>0η,γ>0 there is M=M(η,γ)M=M(\eta,\gamma)M=M(η,γ) such that it is NP-hard to distinguish instances with label set [M][M][M] and OPT≥1−η\mathrm{OPT}\ge 1-\etaOPT≥1−η from those with OPT≤γ\mathrm{OPT}\le\gammaOPT≤γ.

A weighted MAX-CUT instance is a graph with nonnegative edge weights. It is at least ccc-satisfiable if some partition cuts at least a ccc fraction of the total weight, and at most sss-satisfiable if no partition cuts more than an sss fraction.

On the cube {−1,1}n\{-1,1\}^n{−1,1}n, with TRUE =−1=-1=−1 and the uniform measure, the noise stability of f:{−1,1}n→Rf:\{-1,1\}^n\to\mathbb Rf:{−1,1}n→R at ρ∈[−1,1]\rho\in[-1,1]ρ∈[−1,1] is Sρ(f)=E[f(x)f(y)]\mathbb S_\rho(f)=\mathbf E[f(x)f(y)]Sρ​(f)=E[f(x)f(y)]. Here xxx is uniform and yyy is ρ\rhoρ-correlated with xxx: each yiy_iyi​ independently equals xix_ixi​ with probability 12+12ρ\tfrac12+\tfrac12\rho21​+21​ρ. The influence Infi(f)\mathrm{Inf}_i(f)Infi​(f) is the expected variance of fff in the coordinate xix_ixi​, and the low-degree influence is Infi≤k(f)=∑S∋i,∣S∣≤kf^(S)2\mathrm{Inf}_i^{\le k}(f)=\sum_{S\ni i,|S|\le k}\hat f(S)^2Infi≤k​(f)=∑S∋i,∣S∣≤k​f^​(S)2. Majority Is Stablest states: for ρ∈[0,1)\rho\in[0,1)ρ∈[0,1) and ϵ>0\epsilon>0ϵ>0 there is δ>0\delta>0δ>0 such that every f:{−1,1}n→[−1,1]f:\{-1,1\}^n\to[-1,1]f:{−1,1}n→[−1,1] with E[f]=0\mathbf E[f]=0E[f]=0 and all Infi(f)≤δ\mathrm{Inf}_i(f)\le\deltaInfi​(f)≤δ has Sρ(f)≤1−2πarccos⁡ρ+ϵ\mathbb S_\rho(f)\le 1-\tfrac2\pi\arccos\rho+\epsilonSρ​(f)≤1−π2​arccosρ+ϵ.

Formalization targets

Goal: Theorem 1 (p. 11)

Assume the UGC and Majority Is Stablest. For every −1<ρ<0-1<\rho<0−1<ρ<0 and ϵ>0\epsilon>0ϵ>0 it is NP-hard to distinguish MAX-CUT instances that are at least ccc-satisfiable from those that are at most sss-satisfiable, where

c=12−12ρ,s=arccos⁡ρπ+ϵ.c=\tfrac12-\tfrac12\rho,\qquad s=\frac{\arccos\rho}{\pi}+\epsilon.c=21​−21​ρ,s=πarccosρ​+ϵ.

Choosing ρ\rhoρ to minimize s/cs/cs/c gives hardness of approximation within any factor above αGW\alpha_{GW}αGW​; that consequence is not part of the goal.

Milestones

  • The Fourier formulas Sρ(f)=⟨f,Tρf⟩=∑Sρ∣S∣f^(S)2\mathbb S_\rho(f)=\langle f,T_\rho f\rangle=\sum_S\rho^{|S|}\hat f(S)^2Sρ​(f)=⟨f,Tρ​f⟩=∑S​ρ∣S∣f^​(S)2 (Proposition 7.1) and Infi(f)=∑S∋if^(S)2\mathrm{Inf}_i(f)=\sum_{S\ni i}\hat f(S)^2Infi​(f)=∑S∋i​f^​(S)2 (Proposition 7.2).
  • Three variants of Majority Is Stablest:
    • with low-degree influences (Proposition 7.3);
    • in reverse for ρ∈(−1,0]\rho\in(-1,0]ρ∈(−1,0], without E[f]=0\mathbf E[f]=0E[f]=0 (Proposition 7.4);
    • both at once (Proposition 7.5).
  • The completeness of the Long-Code verifier, (1−2η)(12−12ρ)(1-2\eta)(\tfrac12-\tfrac12\rho)(1−2η)(21​−21​ρ) (§8.2).
  • The arithmetization Pr⁡[acc]=12−12Ev[Sρ(gv)]\Pr[\mathrm{acc}]=\tfrac12-\tfrac12\mathbf E_v[\mathbb S_\rho(g_v)]Pr[acc]=21​−21​Ev​[Sρ​(gv​)] (6).
  • The influence-transfer inequality (7).
  • The candidate-set bound ∣Cand[w]∣≤2k/δ|\mathrm{Cand}[w]|\le 2k/\delta∣Cand[w]∣≤2k/δ.
  • The soundness: acceptance ≥(arccos⁡ρ)/π+ϵ\ge(\arccos\rho)/\pi+\epsilon≥(arccosρ)/π+ϵ forces OPT≥γ′(ϵ,ρ)\mathrm{OPT}\ge\gamma'(\epsilon,\rho)OPT≥γ′(ϵ,ρ), independently of MMM (§8.3).

Significance

Under the UGC, Theorem 1 shows that the Goemans–Williamson algorithm is optimal for MAX-CUT. It also shows that the semidefinite relaxation's integrality gap and the hardness threshold coincide. This correspondence was later extended to every constraint satisfaction problem (Raghavendra, STOC 2008). The verifier analysis here is the template for many later UGC-hardness results: dictatorship tests via noise stability, and list-decoding via low-degree influences.

The paper's result is proved, conditional on the UGC; the UGC itself is open. To our knowledge, neither the reduction nor the Majority Is Stablest theorem has a machine-checked proof. This mission produces a checked version of the conditional reduction. Its by-products are reusable: Fourier analysis on the cube (noise stability, influences, the Bonami–Beckner operator), the Long-Code verifier analysis, and a gap-hardness interface on top of a Turing-machine definition of NP.

Difficulty

Completeness is a short calculation. The difficulty is soundness. A proof that the verifier accepts with probability above (arccos⁡ρ)/π+ϵ(\arccos\rho)/\pi+\epsilon(arccosρ)/π+ϵ must be decoded into a labeling that satisfies a fraction γ′\gamma'γ′ of the edges, and γ′\gamma'γ′ must not depend on the label set size MMM. Labeling each www by a coordinate of large influence of fwf_wfw​ is the obvious decoding, but on its own it does not work. The test is passed with high probability by the averaged functions gvg_vgv​, not by the fwf_wfw​ themselves. Ruling out functions with only small influences is exactly the content of Majority Is Stablest. The analysis needs both the reverse form of Majority Is Stablest for negative ρ\rhoρ and low-degree influences, whose sum is bounded by kkk independently of MMM. Turning the PCP into polynomial-time gap-hardness adds further work on top of the analysis:

  • the regularity assumption must be removed;
  • an irrational ρ\rhoρ must be replaced by a nearby rational one, so that the weights are integers;
  • the reduction must be shown polynomial-time on Turing machines.

Formalization scope

  • The cube. {−1,1}n\{-1,1\}^n{−1,1}n is Fin n → Bool, with TRUE ↦−1\mapsto-1↦−1. Expectations are finite averages.
  • No Fourier shortcuts. Noise stability and influence are defined as on pp. 5–6 (a correlated-pair average, an expected coordinate variance), not by their Fourier formulas, which are milestones.
  • Unique Label Cover. Instances have finite V,WV,WV,W, E⊆V×WE\subseteq V\times WE⊆V×W, and a permutation of Fin M\mathrm{Fin}\,MFinM for every pair. OPT\mathrm{OPT}OPT is the maximum over the finitely many labelings, and 000 when there is none.
  • MAX-CUT instances are loopless graphs with natural-number edge weights (edge multiplicities), as §7.1 permits.
  • NP-hardness. "NP-hard to distinguish" is GapNPHard: every NP language of the published CookPvsNP_defs maps by a polynomial-time Turing-machine computable function to Yes-instances or No-instances. Instances are encoded in unary.
  • Hypotheses of the goal. The UGC is a hypothesis of Theorem 1. Majority Is Stablest, which the paper cites from [45] and does not prove, is a second, disclosed hypothesis, of Theorem 1 and of every milestone that uses it.
  • Regularity. The verifier milestones assume the VVV-side regularity of §8.1; Theorem 1 and the UGC do not.
  • No trivial instances. Every Yes- and No-predicate requires a nonempty edge set, so the empty instance cannot carry the hardness. Placeholder (True/False) versions of the UGC or of Majority Is Stablest would trivialize the goal and are excluded.
  • Welcome contributions.
    • The Fourier milestones are self-contained and reusable.
    • A proof of Majority Is Stablest would discharge the second hypothesis.
    • A formal regularization of Unique Label Cover ([38]) would make the reduction self-contained.

Selected references

  • S. Khot, G. Kindler, E. Mossel, R. O'Donnell, Optimal Inapproximability Results for MAX-CUT and Other 2-Variable CSPs?, SIAM J. Comput. 37(1), 2007. https://doi.org/10.1137/S0097539705447372
  • M. X. Goemans, D. P. Williamson, Improved approximation algorithms for maximum cut and satisfiability problems using semidefinite programming, J. ACM 42(6), 1995. https://doi.org/10.1145/227683.227684
  • J. Håstad, Some optimal inapproximability results, J. ACM 48(4), 2001. https://doi.org/10.1145/502090.502098
  • S. Khot, On the power of unique 2-prover 1-round games, STOC 2002. https://doi.org/10.1145/509907.510017
  • E. Mossel, R. O'Donnell, K. Oleszkiewicz, Noise stability of functions with low influences: invariance and optimality, Annals of Math. 171(1), 2010. https://doi.org/10.4007/annals.2010.171.295 (arXiv:math/0503503)
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Operations ResearchOptimizationProbability·Captain: mikedeng1

The Quantity Flexibility Contract and Supplier-Customer Incentives II: With a Perfect Demand Signal the Transfer Price c̄(ψ) Makes the Quantity Flexibility Contract System-EfficientResearch Paper

Motivation

A manufacturer must commit to production before its retail customer knows what the market will demand, while the customer would rather postpone its purchase until better information arrives. Left uncoordinated, each firm protects itself: the customer inflates forecasts it is not bound by, and the manufacturer, discounting those forecasts, builds less than the supply chain as a whole should. Quantity flexibility (QF) contracts, used in practice in the electronics and computer industries (Sun Microsystems, Solectron, Nippon Otis and others are cited in the paper), address this by tying the customer's forecast to a band: the manufacturer guarantees supply up to a percentage above the forecast, and the customer promises to buy at least a percentage below it.

Tsay (1999) gives a two-stage model of such a contract with a demand signal that arrives between production and purchase, shows that a supply chain without commitment underproduces, and characterizes when a QF contract restores efficiency. This mission formalizes the efficiency result for the case in which the signal predicts demand perfectly (Proposition 6(a)), together with the steps of the equilibrium that it rests on.

Setting

A manufacturer (EM) produces at unit cost mmm and sells to a retailer at unit transfer price ccc; the retailer sells at price ppp, unsold units are salvaged at uuu at either site, and each unit of unmet demand costs a goodwill loss sss. The standing assumptions are p>m>0p > m > 0p>m>0, u<mu < mu<m and s≥0s \ge 0s≥0.

Before production, the retailer states a forecast q≥0q \ge 0q≥0. A QF contract {c,(α,ω)}\{c,(\alpha,\omega)\}{c,(α,ω)} with ω∈[0,1]\omega\in[0,1]ω∈[0,1] and α≥−ω\alpha\ge-\omegaα≥−ω obliges the EM to make up to q(1+α)q(1+\alpha)q(1+α) available and the retailer to buy at least q(1−ω)q(1-\omega)q(1−ω). The EM then builds QQQ. A demand signal μ\muμ with distribution function Θ\ThetaΘ is observed, the retailer buys rrr, and market demand is filled from the retailer's stock. In this mission the signal is perfect (σε=0\sigma_\varepsilon = 0σε​=0): market demand equals μ\muμ, so its distribution FFF equals Θ\ThetaΘ.

Given μ\muμ, the retailer's profit from buying rrr is

G(r∣μ)=pmin⁡[μ,r]−c r−s[μ−r]++u[r−μ]+,G(r\mid\mu) = p\min[\mu,r] - c\,r - s[\mu-r]^+ + u[r-\mu]^+,G(r∣μ)=pmin[μ,r]−cr−s[μ−r]++u[r−μ]+,

and it buys rQF∗=μ⊥[q(1−ω),Q]r^*_{QF} = \mu\perp[q(1-\omega),Q]rQF∗​=μ⊥[q(1−ω),Q], the point of the interval closest to μ\muμ. The EM's expected profit (2) is πEM,QF(Q;q)=(c−u)Eμ{rQF∗}−(m−u)Q\pi_{EM,QF}(Q;q) = (c-u)E_\mu\{r^*_{QF}\} - (m-u)QπEM,QF​(Q;q)=(c−u)Eμ​{rQF∗​}−(m−u)Q. The retailer's forecast problem maximizes πR,QF(q)=Eμ{G(rQF∗∣μ)}\pi_{R,QF}(q) = E_\mu\{G(r^*_{QF}\mid\mu)\}πR,QF​(q)=Eμ​{G(rQF∗​∣μ)} with the EM building q(1+α)q(1+\alpha)q(1+α). A central planner earns ΠCC(Q)=Eμ{pmin⁡[μ,Q]−s[μ−Q]++u[Q−μ]+}−mQ\Pi_{CC}(Q) = E_\mu\{p\min[\mu,Q]-s[\mu-Q]^+ + u[Q-\mu]^+\} - mQΠCC​(Q)=Eμ​{pmin[μ,Q]−s[μ−Q]++u[Q−μ]+}−mQ, maximized at

QCC∗=F−1 ⁣(p+s−mp+s−u).Q^*_{CC} = F^{-1}\!\left(\frac{p+s-m}{p+s-u}\right).QCC∗​=F−1(p+s−up+s−m​).

The total flexibility of the contract is ψ=(1+α)/(1−ω)\psi = (1+\alpha)/(1-\omega)ψ=(1+α)/(1−ω).

Formalization targets

Goal: Proposition 6(a)

With σε=0\sigma_\varepsilon = 0σε​=0, the QF contract with flexibility ψ\psiψ and transfer price

cˉ(ψ)=u+m−u1ψF ⁣(1ψF−1 ⁣(p+s−mp+s−u))+m−up+s−u(4)\bar c(\psi) = u + \frac{m-u}{\dfrac1\psi F\!\left(\dfrac1\psi F^{-1}\!\left(\dfrac{p+s-m}{p+s-u}\right)\right) + \dfrac{m-u}{p+s-u}} \tag{4}cˉ(ψ)=u+ψ1​F(ψ1​F−1(p+s−up+s−m​))+p+s−um−u​m−u​(4)

is system-efficient: the retailer's unique optimal forecast is q^=QCC∗/(1+α)\hat q = Q^*_{CC}/(1+\alpha)q^​=QCC∗​/(1+α), the EM's unique optimal production given q^\hat qq^​ is q^(1+α)=QCC∗\hat q(1+\alpha) = Q^*_{CC}q^​(1+α)=QCC∗​, and the resulting expected system profit equals max⁡QΠCC(Q)\max_Q \Pi_{CC}(Q)maxQ​ΠCC​(Q).

Milestones

  1. §4: QCC∗Q^*_{CC}QCC∗​ exists and is the unique maximizer of ΠCC\Pi_{CC}ΠCC​.
  2. §6.1: given μ\muμ, the retailer's unique optimal purchase in [a,b][a,b][a,b] is μ⊥[a,b]\mu\perp[a,b]μ⊥[a,b].
  3. Proposition 3(a): for ω<1\omega<1ω<1, the optimal forecast qQF∗q^*_{QF}qQF∗​ is strictly positive, finite, and the unique solution of the first-order condition (3).
  4. §7: for any forecast q≥0q\ge0q≥0, expected system profit equals ΠCC(q(1+α))\Pi_{CC}(q(1+\alpha))ΠCC​(q(1+α)); hence it is maximal when the production level q(1+α)q(1+\alpha)q(1+α) matches QCC∗Q^*_{CC}QCC∗​.

Significance

The result shows that one contract form, by choosing the transfer price as a function of the flexibility, yields a whole menu of contracts each of which coordinates the supply chain, so that the two firms can trade price against flexibility without losing system profit. Its corollaries in the paper, that any split of expected profit is achievable by some efficient contract and that more flexibility shifts profit to the manufacturer, rest on (4).

The paper prints no proofs ("All proofs are omitted due to space limitations", p. 1341). A machine-checked development supplies them, makes explicit the regularity the argument needs (finite variance, a continuous and strictly increasing Θ\ThetaΘ, a positive efficient quantity), and gives reusable statements about newsvendor objectives with a clipped purchase. To our knowledge none of these results has been formalized before; the platform's quantity-flexibility theorems in other models (no manufacturer production stage, α=0\alpha = 0α=0, retailer side only) do not cover them.

Difficulty

Each firm optimizes its own objective, and the efficient price must work for both at once. Making the retailer's first-order condition hold at q^\hat qq^​ pins down ccc, so nothing is left to adjust for the EM, whose incentive to build more than the contracted q(1+α)q(1+\alpha)q(1+α) has to be ruled out separately at that same price. The retailer's objective is an expectation of a non-smooth function of a clipped purchase, so its derivative must be computed through the distribution of μ\muμ on two moving thresholds q(1+α)q(1+\alpha)q(1+α) and q(1−ω)q(1-\omega)q(1−ω), and strict concavity must come from the strict increase of Θ\ThetaΘ rather than from a density.

Formalization scope

All objects live in the namespace TsayQF.EffQF. The law of μ\muμ is a probability measure ν\nuν on R\mathbb RR with μ∈L2(ν)\mu\in L^2(\nu)μ∈L2(ν), whose distribution function cdf ν is differentiable and strictly increasing on R\mathbb RR (the paper's "differentiable and invertible"). Expectations are Bochner integrals; finite variance makes every integrand integrable. Inverse distribution functions are not used: QCC∗Q^*_{CC}QCC∗​ enters as a real number with the hypothesis F(QCC∗)=κSF(Q^*_{CC}) = \kappa_SF(QCC∗​)=κS​, which determines it uniquely, and (4) is defined in its printed shape. Optimality is IsMaxOn over the decision's natural set: forecasts in [0,∞)[0,\infty)[0,∞), the EM's production in [q(1+α),∞)[q(1+\alpha),\infty)[q(1+α),∞), purchases in [q(1−ω),Q][q(1-\omega),Q][q(1−ω),Q], central production in R\mathbb RR.

Hypotheses made explicit: QCC∗>0Q^*_{CC} > 0QCC∗​>0 in the goal and a positive marginal value of the forecast at q=0q=0q=0 in Proposition 3(a), both standing for the paper's presumption that demand is almost certainly nonnegative; ω<1\omega<1ω<1 (Proposition 3's case). The transfer price is only required to satisfy u<c<p+su<c<p+su<c<p+s rather than m<c<pm<c<pm<c<p, because cˉ(ψ)\bar c(\psi)cˉ(ψ) can exceed ppp when s>0s>0s>0. The milestones are the σε=0\sigma_\varepsilon = 0σε​=0 instances of the paper's general statements.

Two modelling choices are fixed. The retailer's forecast objective takes the EM's production to be q(1+α)q(1+\alpha)q(1+α), as §6.1 does after Proposition 2; the full game in which the retailer anticipates other EM responses is not modelled, and the goal instead verifies that the EM's unique best response at cˉ(ψ)\bar c(\psi)cˉ(ψ) is exactly q(1+α)q(1+\alpha)q(1+α). The efficient price is the explicit formula (4), not "a price that makes QCC∗Q^*_{CC}QCC∗​ optimal", which would make the goal a tautology; likewise system efficiency is stated as an inequality against ΠCC\Pi_{CC}ΠCC​ at every production level, not by definition.

Needed infrastructure: derivatives of expectations of piecewise-linear functions of a clipped variable, and the newsvendor fractile characterization. Both are reusable for other contract models. Proofs of any milestone, and of the goal from the milestones, are welcome.

Selected references

  • A. A. Tsay, The Quantity Flexibility Contract and Supplier-Customer Incentives, Management Science 45(10):1339–1358, 1999. https://doi.org/10.1287/mnsc.45.10.1339
  • G. P. Cachon, Supply Chain Coordination with Contracts, in Handbooks in OR & MS vol. 11, 2003, §6.2.5. https://doi.org/10.1016/S0927-0507(03)11006-7
  • L. V. Snyder and Z.-J. M. Shen, Fundamentals of Supply Chain Theory, Wiley, 2nd ed. 2019, Ch. 14. https://doi.org/10.1002/9781119584445
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Dynamic ProgrammingMarkov ChainOperations Research+1·Captain: mikedeng1

Optimality of (s, S) Policies in Inventory Models with Markovian Demand II: In the Nonstationary Discounted Infinite-Horizon Problem, a State-Dependent (s, S) Policy Is OptimalResearch Paper

Motivation

Periodic-review inventory models with a fixed ordering cost are the setting in which the (s,S)(s,S)(s,S) policy is optimal: when the stock falls below a reorder point sss, order up to a level SSS, otherwise order nothing. Scarf (1960) proved this for independent demands over a finite horizon by introducing KKK-convexity, and Iglehart (1963) extended it to the discounted infinite horizon. In practice the demand distribution changes with an exogenous environment: the economy, the season, the stage of a product's life cycle. Song and Zipkin (Oper. Res. 41(2), 1993) modelled this environment as a Markov chain of demand states in continuous time with Poisson demand.

Sethi and Cheng (Oper. Res. 45(6), 1997) treat the discrete-time version with general demand densities, nonstationary costs and convex surplus costs of linear growth. The companion mission (I) covers their finite-horizon result, Theorem 4.1. This mission covers the nonstationary discounted infinite-horizon result, Theorem 6.2, together with the existence theory (Theorem 6.1, proved in the paper's Appendix) on which it rests.

Setting

Demand states form the finite set I={1,…,L}I = \{1,\dots,L\}I={1,…,L} and follow a Markov chain with transition matrix P=(pij)P = (p_{ij})P=(pij​). In period k=0,1,2,…k = 0,1,2,\dotsk=0,1,2,… the demand ξk≥0\xi_k \ge 0ξk​≥0 has the conditional density φi,k\varphi_{i,k}φi,k​ given ik=ii_k = iik​=i, with mean at most MMM. Orders are placed at the start of a period and delivered at once, and unmet demand is backlogged, so the surplus evolves by xk+1=xk+uk−ξkx_{k+1} = x_k + u_k - \xi_kxk+1​=xk​+uk​−ξk​ (2.4). Ordering u≥0u \ge 0u≥0 costs ck(i,u)=Kki δ(u)+ckiuc_k(i,u) = K^i_k\,\delta(u) + c^i_k uck​(i,u)=Kki​δ(u)+cki​u with Kki,cki≥0K^i_k, c^i_k \ge 0Kki​,cki​≥0 (2.1), where δ(z)=1\delta(z) = 1δ(z)=1 for z>0z > 0z>0 and 000 otherwise. The surplus cost fk(i,⋅)f_k(i,\cdot)fk​(i,⋅) is convex and nonnegative, vanishes at 000, and satisfies fk(i,x)≤C(1+∣x∣)f_k(i,x) \le C(1+|x|)fk​(i,x)≤C(1+∣x∣) (2.2).

An admissible policy UUU chooses each order uk≥0u_k \ge 0uk​≥0 as a measurable function of the past demand states and demands. With a discount factor α\alphaα, the objective from period nnn, state iii and surplus xxx is

Jn(i,x;U)=∑k=n∞αk−n E[ck(ik,uk)+fk(ik,xk)],(6.1)J_n(i,x;U) = \sum_{k=n}^{\infty} \alpha^{k-n}\,E\big[c_k(i_k,u_k) + f_k(i_k,x_k)\big], \tag{6.1}Jn​(i,x;U)=k=n∑∞​αk−nE[ck​(ik​,uk​)+fk​(ik​,xk​)],(6.1)

and the value function is vn(i,x)=inf⁡UJn(i,x;U)v_n(i,x) = \inf_U J_n(i,x;U)vn​(i,x)=infU​Jn​(i,x;U). With Fn+1(b)(i,y)=∑jpij∫0∞b(j,y−z) φi,n(z) dzF_{n+1}(b)(i,y) = \sum_j p_{ij}\int_0^\infty b(j,y-z)\,\varphi_{i,n}(z)\,dzFn+1​(b)(i,y)=∑j​pij​∫0∞​b(j,y−z)φi,n​(z)dz (3.1), the dynamic programming equations are

vn(i,x)=fn(i,x)+inf⁡u≥0{cn(i,u)+αFn+1(vn+1)(i,x+u)},n=0,1,2,…(6.2)v_n(i,x) = f_n(i,x) + \inf_{u\ge0}\big\{c_n(i,u) + \alpha F_{n+1}(v_{n+1})(i,x+u)\big\}, \qquad n = 0,1,2,\dots \tag{6.2}vn​(i,x)=fn​(i,x)+u≥0inf​{cn​(i,u)+αFn+1​(vn+1​)(i,x+u)},n=0,1,2,…(6.2)

The truncations Jn,kJ_{n,k}Jn,k​ keep the first kkk periods of (6.1) (6.3), their values are vn,kv_{n,k}vn,k​ (6.4), and wn=Jn(⋅;0)w_n = J_n(\cdot;\mathbf 0)wn​=Jn​(⋅;0) is the cost of never ordering (6.6). The function classes are B0B_0B0​ (nonnegative pointwise limits of continuous functions), B1B_1B1​ (those of linear growth) and C1C_1C1​ (those also uniformly continuous in xxx). A function ggg is KKK-convex if K+g(z+y)≥g(y)+z (g(y)−g(y−b))/bK + g(z+y) \ge g(y) + z\,(g(y)-g(y-b))/bK+g(z+y)≥g(y)+z(g(y)−g(y−b))/b for all z≥0z \ge 0z≥0, b>0b > 0b>0 (4.3). Assumption (4.1) asks Kni≥∑jpijKn+1j≥0K^i_n \ge \sum_j p_{ij}K^j_{n+1} \ge 0Kni​≥∑j​pij​Kn+1j​≥0, and (4.2) asks cnix+Fn+1(fn+1)(i,x)→+∞c^i_n x + F_{n+1}(f_{n+1})(i,x) \to +\inftycni​x+Fn+1​(fn+1​)(i,x)→+∞ as x→∞x \to \inftyx→∞.

Formalization targets

Goal: Theorem 6.2

Under (2.1), (2.2), (4.1), (4.2) and 0<α<10 < \alpha < 10<α<1, there are sni≤Snis^i_n \le S^i_nsni​≤Sni​ in [−∞,∞)[-\infty,\infty)[−∞,∞) such that

u^n(i,x)=(Sni−x) δ(sni−x)\hat u_n(i,x) = (S^i_n - x)\,\delta(s^i_n - x)u^n​(i,x)=(Sni​−x)δ(sni​−x)

attains the infimum in (6.2) at every (n,i,x)(n,i,x)(n,i,x), and its feedback policy, started at any period nnn and surplus xxx, has cost Jn(i,x;U^)=vn(i,x)J_n(i,x;\hat U) = v_n(i,x)Jn​(i,x;U^)=vn​(i,x): it is optimal among all history-dependent policies.

Milestones

  1. The order-nothing cost wnw_nwn​ is finite, lies in C1C_1C1​, and is the unique C1C_1C1​ solution of wn=fn+αFn+1(wn+1)w_n = f_n + \alpha F_{n+1}(w_{n+1})wn​=fn​+αFn+1​(wn+1​) (6.7).
  2. The truncated values solve the dynamic programming equations (6.5), vn,0=0v_{n,0} = 0vn,0​=0, vn,k∈C1v_{n,k} \in C_1vn,k​∈C1​, and under (4.2) the infimum in (6.4) is attained.
  3. Theorem 6.1, (6.8): 0=vn,0≤vn,1≤⋯≤vn,k≤wn0 = v_{n,0} \le v_{n,1} \le \cdots \le v_{n,k} \le w_n0=vn,0​≤vn,1​≤⋯≤vn,k​≤wn​.
  4. Appendix: ∣vn,k(i,x′)−vn,k(i,x)∣≤C∣x′−x∣/(1−α)|v_{n,k}(i,x') - v_{n,k}(i,x)| \le C|x'-x|/(1-\alpha)∣vn,k​(i,x′)−vn,k​(i,x)∣≤C∣x′−x∣/(1−α), and the same for vn=lim⁡kvn,kv_n = \lim_k v_{n,k}vn​=limk​vn,k​.
  5. Theorem 6.1, (6.9): vn,k↑vnv_{n,k} \uparrow v_nvn,k​↑vn​, a solution of (6.2) in B1B_1B1​.
  6. Theorem 6.1, (6.10): vn∈C1v_n \in C_1vn​∈C1​, a B0B_0B0​ minimizer U^\hat UU^ of (6.2) exists, and every such U^\hat UU^ is optimal: vn(i,x)=min⁡UJn(i,x;U)=Jn(i,x;U^)v_n(i,x) = \min_U J_n(i,x;U) = J_n(i,x;\hat U)vn​(i,x)=minU​Jn​(i,x;U)=Jn​(i,x;U^).
  7. Proof of Theorem 6.2: vn,k(i,⋅)v_{n,k}(i,\cdot)vn,k​(i,⋅) is KniK^i_nKni​-convex.
  8. Proof of Theorem 6.2: vn(i,⋅)v_n(i,\cdot)vn​(i,⋅) is KniK^i_nKni​-convex.

The structural lemma behind the step from KKK-convexity to the (s,S)(s,S)(s,S) form, Proposition 4.2 of the paper (an extension of Bertsekas' lemma to lower semicontinuous functions coercive only at +∞+\infty+∞, with possibly infinite sss, SSS), is posed in the companion finite-horizon mission and is not repeated here.

Significance

Theorem 6.2 says that the classical (s,S)(s,S)(s,S) structure survives two generalizations at once: demand driven by a Markov environment, and nonstationary data over an infinite horizon. The two levels may depend on the period and on the current demand state, so only 2L2L2L numbers per period describe an optimal policy, and with cyclic demand only LLL pairs are needed (Corollary 7.1 of the paper). Theorem 6.1 is a self-contained existence result for a positive-cost, unbounded-state dynamic program: value iteration from zero converges to the value function, which solves the optimality equation, and any measurable minimizer is optimal among history-dependent policies.

The results are proved in the paper, with the finite-horizon existence theory delegated to Beyer, Sethi and Taksar (1998). No machine-checked proof of any of them is known. The platform has KKK-convexity (BertsekasKConvex) and the (s,S)(s,S)(s,S) structure lemma of Bertsekas for continuous functions coercive at both ends; it has no discounted infinite-horizon (s,S)(s,S)(s,S) theorem with Markov-modulated demand. The related posed items SongZipkinFluct.FixedCost.theorem5e_theorem6 and theorem5ab concern the Song–Zipkin model (continuous time, Poisson demand, integer levels, stationary data), a different model.

Difficulty

The obvious argument is "the finite-horizon value functions are KKK-convex, so their limit is, and a minimizer of a KKK-convex optimality equation is (s,S)(s,S)(s,S)". Three steps of it fail as stated.

First, the limit of value iteration need not be the value function, nor solve (6.2), in a positive-cost problem with unbounded actions: exchanging lim⁡k\lim_klimk​ with inf⁡u\inf_uinfu​ requires the minimizers of the truncated problems to stay in a compact set uniformly in kkk, and that bound is where the coercivity assumption (4.2) enters. Second, optimality against history-dependent policies, not only Markov ones, requires a verification argument along histories of states and demands. Third, the functions zn(i,y)=cniy+αFn+1(vn+1)(i,y)z_n(i,y) = c^i_n y + \alpha F_{n+1}(v_{n+1})(i,y)zn​(i,y)=cni​y+αFn+1​(vn+1​)(i,y) may be unbounded below, in which case the reorder level is s=−∞s = -\inftys=−∞ and the order-up-to level does not exist; the goal allows this case.

Formalization scope

The Lean development (namespace SethiChengSS.Infinite) commits to the following.

  • Demand states are Fin L; periods are natural numbers with the paper's base 000.
  • Expectations are sums over state paths of Lebesgue integrals against the product weight ∏tpitit+1φit,t(ξt)\prod_t p_{i_t i_{t+1}}\varphi_{i_t,t}(\xi_t)∏t​pit​it+1​​φit​,t​(ξt​), valued in [0,∞][0,\infty][0,∞]. This builds in the conditional independence of ξk\xi_kξk​ and ik+1i_{k+1}ik+1​ given iki_kik​ that (3.1) uses.
  • A policy is a function of the state history and the past demands; admissible means nonnegative and measurable in the demands. The comparison class is never restricted to Markov policies.
  • JnJ_nJn​ (6.1) is the supremum over kkk of the truncations Jn,kJ_{n,k}Jn,k​ (6.3), which equals the series because all costs are nonnegative.
  • Fn+1F_{n+1}Fn+1​ uses the Bochner integral, which is 000 on non-integrable integrands; the C1C_1C1​ conclusions are what make it genuine.
  • The levels sss, SSS are extended reals with s≤Ss \le Ss≤S, S≠+∞S \ne +\inftyS=+∞, and SSS real whenever sss is (Remark 4.4).

Pins. The paper prints 0<α≤10 < \alpha \le 10<α≤1; the mission assumes 0<α<10 < \alpha < 10<α<1, since wnw_nwn​ is infinite at α=1\alpha = 1α=1 and the Appendix divides by 1−α1-\alpha1−α. Theorem 6.2 is printed without (4.1), which its proof uses through the induction of Section 4; (4.1) is assumed for every period. Theorem 6.1 is printed under (2.1)–(2.2) only, but attainment in (6.2) can fail without coercivity and the Appendix bound (A.3) divides by cnic^i_ncni​; (4.2) is added to (6.9), (6.10) and to the attainment clause of (6.5). "In class C1C_1C1​" for the sequence wnw_nwn​ is read with one growth constant for all periods. The boundary condition "vn+k,0=0v_{n+k,0} = 0vn+k,0​=0" of (6.5) is read as vn,0=0v_{n,0} = 0vn,0​=0, as the next sentence of the paper states.

The goal cannot be met by a degenerate encoding: the value function is the infimum over all admissible history-dependent policies (not the solution of (6.2) by definition), the demand data must be genuine probability densities with bounded mean, and the levels may not be S=+∞S = +\inftyS=+∞.

A complete development needs: monotone convergence for the path-measure costs, measurable selection of minimizers, the KKK-convexity closure properties (Proposition 4.1 of the paper; several are proved on the platform as BertsekasDP.kconvex_*), and Proposition 4.2. The model file and the infinite-horizon verification argument are reusable for other Markov-modulated inventory models. Contributions toward any milestone, or toward general lemmas on positive-cost dynamic programs, are welcome.

Selected references

  • S. P. Sethi and F. Cheng, Optimality of (s, S) policies in inventory models with Markovian demand, Operations Research 45(6), 931–939, 1997. https://doi.org/10.1287/opre.45.6.931
  • J.-S. Song and P. Zipkin, Inventory control in a fluctuating demand environment, Operations Research 41(2), 351–370, 1993. https://doi.org/10.1287/opre.41.2.351
  • H. Scarf, The optimality of (S, s) policies in the dynamic inventory problem, in Mathematical Methods in the Social Sciences, Stanford University Press, 1960.
  • D. L. Iglehart, Optimality of (s, S) policies in the infinite horizon dynamic inventory problem, Management Science 9(2), 259–267, 1963. https://doi.org/10.1287/mnsc.9.2.259
  • D. P. Bertsekas, Dynamic Programming and Stochastic Control, Academic Press, 1976.
  • A. Bensoussan, M. Crouhy and J.-M. Proth, Mathematical Theory of Production Planning, North-Holland, 1983.
  • D. Beyer, S. P. Sethi and M. Taksar, Inventory models with Markovian demands and cost functions of polynomial growth, Journal of Optimization Theory and Applications 98, 1998 (cited by Sethi and Cheng as forthcoming).
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Numerical AnalysisProbabilityStochastic Systems·Captain: mikedeng1

Strong Convergence of an Explicit Numerical Method for SDEs with Nonglobally Lipschitz Continuous Coefficients: The Tamed Euler Scheme Converges to the SDE Solution in Uniform Lp with Order 1/2Research Paper

Motivation

Stochastic differential equations (SDEs) are simulated almost always by time-stepping schemes, and the cheapest and most widely used is the explicit Euler (Euler–Maruyama) scheme. Its strong convergence with order 12\tfrac1221​ is classical when the coefficients are globally Lipschitz. Many models in applications are not: Langevin dynamics with confining potentials, stochastic Ginzburg–Landau equations, and population or volatility models have drifts such as μ(x)=x−x3\mu(x)=x-x^3μ(x)=x−x3 that grow superlinearly.

For such drifts the explicit Euler scheme fails. Hutzenthaler, Jentzen and Kloeden showed in 2011 (Proc. R. Soc. A 467) that its absolute moments diverge to infinity whenever the drift or the diffusion grows superlinearly, so it does not converge in LpL^pLp. Implicit schemes do converge (Higham, Mao and Stuart, SIAM J. Numer. Anal. 40, 2002), but each step requires solving a nonlinear equation.

The paper of this mission (Hutzenthaler, Jentzen and Kloeden, Ann. Appl. Probab. 22(4), 2012) introduces a tamed Euler scheme: an explicit method that costs the same as the Euler scheme, modified by a second-order term in the drift. It proves strong convergence with order 12\tfrac1221​ under a one-sided Lipschitz drift whose derivative grows at most polynomially. The scheme started a line of work on tamed and truncated methods, among them Sabanis's schemes that tame drift and diffusion together for superlinearly growing diffusion coefficients (Ann. Appl. Probab. 26(4), 2016), formalized on this platform in the series "Euler Approximations with Varying Coefficients".

Setting

Fix T∈(0,∞)T\in(0,\infty)T∈(0,∞) and d,m∈N={1,2,… }d,m\in\mathbb N=\{1,2,\dots\}d,m∈N={1,2,…}. Let (Ω,F,P)(\Omega,\mathcal F,\mathbb P)(Ω,F,P) be a probability space with a filtration (Ft)(\mathcal F_t)(Ft​), and let WWW be an mmm-dimensional standard (Ft)(\mathcal F_t)(Ft​)-Brownian motion. On Rk\mathbb R^kRk, ∥v∥\|v\|∥v∥ is the Euclidean norm and ⟨v,w⟩\langle v,w\rangle⟨v,w⟩ the inner product. For a matrix AAA, ∥A∥=sup⁡∥v∥≤1∥Av∥\|A\|=\sup_{\|v\|\le1}\|Av\|∥A∥=sup∥v∥≤1​∥Av∥ is the operator norm.

The initial value ξ:Ω→Rd\xi:\Omega\to\mathbb R^dξ:Ω→Rd is F0\mathcal F_0F0​-measurable with E∥ξ∥p<∞\mathbb E\|\xi\|^p<\inftyE∥ξ∥p<∞ for every p≥1p\ge1p≥1. The drift μ:Rd→Rd\mu:\mathbb R^d\to\mathbb R^dμ:Rd→Rd is continuously differentiable and the diffusion is σ:Rd→Rd×m\sigma:\mathbb R^d\to\mathbb R^{d\times m}σ:Rd→Rd×m. There is one constant c>0c>0c>0 with

∥μ′(x)∥≤c(1+∥x∥c),∥σ(x)−σ(y)∥≤c∥x−y∥,⟨x−y,μ(x)−μ(y)⟩≤c∥x−y∥2\|\mu'(x)\|\le c(1+\|x\|^c),\qquad \|\sigma(x)-\sigma(y)\|\le c\|x-y\|,\qquad \langle x-y,\mu(x)-\mu(y)\rangle\le c\|x-y\|^2∥μ′(x)∥≤c(1+∥x∥c),∥σ(x)−σ(y)∥≤c∥x−y∥,⟨x−y,μ(x)−μ(y)⟩≤c∥x−y∥2

for all x,yx,yx,y. The exact solution XXX is an adapted process with continuous paths and

Xt=ξ+∫0tμ(Xs) ds+∫0tσ(Xs) dWs,t∈[0,T], P-a.s.X_t=\xi+\int_0^t\mu(X_s)\,ds+\int_0^t\sigma(X_s)\,dW_s,\qquad t\in[0,T],\ \mathbb P\text{-a.s.}Xt​=ξ+∫0t​μ(Xs​)ds+∫0t​σ(Xs​)dWs​,t∈[0,T], P-a.s.

For N∈NN\in\mathbb NN∈N, let ΔWnN=W(n+1)T/N−WnT/N\Delta W^N_n=W_{(n+1)T/N}-W_{nT/N}ΔWnN​=W(n+1)T/N​−WnT/N​. The tamed Euler scheme is Y0N=ξY^N_0=\xiY0N​=ξ and

Yn+1N=YnN+TN μ(YnN)1+TN∥μ(YnN)∥+σ(YnN) ΔWnN,n∈{0,…,N−1}.Y^N_{n+1}=Y^N_n+\frac{\tfrac TN\,\mu(Y^N_n)}{1+\tfrac TN\|\mu(Y^N_n)\|}+\sigma(Y^N_n)\,\Delta W^N_n,\qquad n\in\{0,\dots,N-1\}.Yn+1N​=YnN​+1+NT​∥μ(YnN​)∥NT​μ(YnN​)​+σ(YnN​)ΔWnN​,n∈{0,…,N−1}.

On t∈[nT/N,(n+1)T/N]t\in[nT/N,(n+1)T/N]t∈[nT/N,(n+1)T/N] its interpolation is

YˉtN=YnN+(t−nT/N) μ(YnN)1+TN∥μ(YnN)∥+σ(YnN)(Wt−WnT/N).\bar Y^N_t=Y^N_n+\frac{(t-nT/N)\,\mu(Y^N_n)}{1+\tfrac TN\|\mu(Y^N_n)\|}+\sigma(Y^N_n)(W_t-W_{nT/N}).YˉtN​=YnN​+1+NT​∥μ(YnN​)∥(t−nT/N)μ(YnN​)​+σ(YnN​)(Wt​−WnT/N​).

In Lean, states live in EthierKurtz.SDEState d, σ\sigmaσ takes values in Matrix (Fin d) (Fin m) ℝ, the standing hypotheses are the structures Coefficients and Setting, and the scheme is Y, Ybar, all in the namespace TamedEuler.Convergence.

Formalization targets

Goal: Theorem 1.1

There is a family Cp∈[0,∞)C_p\in[0,\infty)Cp​∈[0,∞), p∈[1,∞)p\in[1,\infty)p∈[1,∞), such that for every solution XXX

(E[sup⁡t∈[0,T]∥Xt−YˉtN∥p])1/p≤Cp N−1/2for all N∈N, p∈[1,∞).\Big(\mathbb E\Big[\sup_{t\in[0,T]}\|X_t-\bar Y^N_t\|^p\Big]\Big)^{1/p}\le C_p\,N^{-1/2}\qquad\text{for all }N\in\mathbb N,\ p\in[1,\infty).(E[t∈[0,T]sup​∥Xt​−YˉtN​∥p])1/p≤Cp​N−1/2for all N∈N, p∈[1,∞).

The constants are left unspecified; only the order 12\tfrac1221​ is asserted.

Milestones: Lemmas 3.1–3.10

These are the ten lemmas the proof rests on, in the paper's order:

  1. the pathwise dominator lemma 1ΩnN∥YnN∥≤DnN\mathbb 1_{\Omega^N_n}\|Y^N_n\|\le D^N_n1ΩnN​​∥YnN​∥≤DnN​ (3.1);
  2. Gaussian and Brownian exponential moments (3.2, 3.3, 3.4);
  3. moments of the dominating processes DnND^N_nDnN​ (3.5);
  4. the decay of P[(ΩNN)c]\mathbb P[(\Omega^N_N)^c]P[(ΩNN​)c] faster than every power of NNN (3.6);
  5. continuous- and discrete-time Burkholder–Davis–Gundy inequalities with constant ppp (3.7, 3.8);
  6. the uniform moment bounds sup⁡Nsup⁡n≤NE∥YnN∥p<∞\sup_N\sup_{n\le N}\mathbb E\|Y^N_n\|^p<\inftysupN​supn≤N​E∥YnN​∥p<∞ (3.9), and the same for μ(YnN)\mu(Y^N_n)μ(YnN​) and σ(YnN)\sigma(Y^N_n)σ(YnN​) (3.10).

Significance

The theorem gives an explicit scheme whose cost per step is the Euler cost and whose strong error is O(N−1/2)O(N^{-1/2})O(N−1/2) in every LpL^pLp, uniformly in time, for the superlinear drifts on which the explicit Euler scheme diverges. Strong error bounds of this kind are what multilevel Monte Carlo (Giles 2008) needs, as the paper notes on p. 3: its complexity analysis requires strong convergence of the coarse and fine levels, and the explicit Euler scheme supplies none for these equations. The moment bound of Lemma 3.9 answers, for the tamed scheme, the open problem Higham, Mao and Stuart formulated in 2002 on when moment bounds hold for explicit methods (quoted on p. 8).

The result is proved in the paper; it has not been formalized. The mission formalizes the statement, its ten lemmas and the scheme. The dominator construction (13)–(14) is a pathwise argument that can be checked independently of the probability. The two Burkholder–Davis–Gundy inequalities with the explicit constant ppp are reusable tools for any numerical analysis of SDEs.

Difficulty

Once the moments of YnNY^N_nYnN​ are bounded uniformly in NNN, the convergence proof follows the globally Lipschitz pattern: an Itô or Gronwall argument on X−YˉNX-\bar Y^NX−YˉN. The difficulty is the moment bound itself. The obvious approach is a Gronwall recursion for E∥Yn+1N∥p\mathbb E\|Y^N_{n+1}\|^pE∥Yn+1N​∥p in terms of E∥YnN∥p\mathbb E\|Y^N_n\|^pE∥YnN​∥p. For superlinear μ\muμ it does not close: the term ∥μ(YnN)∥2(T/N)2\|\mu(Y^N_n)\|^2(T/N)^2∥μ(YnN​)∥2(T/N)2 grows faster than ∥YnN∥2\|Y^N_n\|^2∥YnN​∥2, and for the untamed scheme the moments do in fact diverge. A newcomer's first idea, using the one-sided Lipschitz bound in expectation, fails for the same reason. The paper instead dominates the scheme pathwise on events ΩnN\Omega^N_nΩnN​ and controls the rare complement separately (Lemmas 3.1, 3.5, 3.6).

Formalization scope

The Lean development commits to the following conventions.

  • Normal filtration. Read as a right-continuous filtration (ℱ.IsRightContinuous) together with adaptedness to its P\mathbb PP-completion, which is how the published SabanisEuler.Shared.IsSolution treats completeness.
  • Brownian motion. SabanisEuler.Shared.IsWienerMartingale, defined on [0,∞)[0,\infty)[0,∞) rather than [0,T][0,T][0,T]; this is the usual extension. Time is ℝ≥0.
  • The solution XXX. Any process satisfying the published IsSolution relation, whose stochastic integral is the Ethier–Kurtz Brownian Itô-integral relation. Existence and uniqueness are cited by the paper, not claimed. σ\sigmaσ enters IsSolution entrywise through toDiffusion. Every norm of σ\sigmaσ in a hypothesis or conclusion is the operator norm opNorm.
  • The constant ccc. One real c>0c>0c>0 is both constant and exponent; ∥x∥c\|x\|^c∥x∥c and N1/(2c)N^{1/(2c)}N1/(2c) are real powers.
  • Indices. N={1,2,… }\mathbb N=\{1,2,\dots\}N={1,2,…}: every statement has N≥1N\ge1N≥1 and n≤Nn\le Nn≤N, and d,m≥1d,m\ge1d,m≥1.
  • Interpolation cell. In (10), ttt uses the cell n=min⁡(⌊tN/T⌋,N−1)n=\min(\lfloor tN/T\rfloor,N-1)n=min(⌊tN/T⌋,N−1), so t=Tt=Tt=T uses the last cell.
  • (13) and (14). The supremum over uuu in (13) is a finite maximum. The suprema in (14) are written "for all k<nk<nk<n", so Ω0N=Ω\Omega^N_0=\OmegaΩ0N​=Ω.
  • Moments. Every expectation, LpL^pLp norm and "<∞<\infty<∞" is stated in [0,∞][0,\infty][0,∞] with lintegral or eLpNorm, never as a Bochner integral that could default to 000.
  • Lemma 3.1. Stated pathwise for every ω\omegaω and an arbitrary path WWW.
  • Lemma 3.7. The published Itô relation demands pathwise square-integrability of the integrand. This is stronger than the printed almost-sure condition, and the deviation is disclosed.

A trivializing formalization is ruled out: the scheme is (8) exactly, with only the drift tamed and the step size T/NT/NT/N. The error is taken against the same Brownian path that drives XXX. The setting is satisfiable for the paper's example μ(x)=x−x3\mu(x)=x-x^3μ(x)=x−x3, σ(x)=x\sigma(x)=xσ(x)=x with c=3c=3c=3 (checked in a sorry-free verification file, given any Brownian motion). Replacing the Itô integral by a postulated operator or a pathwise integral is not admitted.

A complete development needs:

  • Gaussian exponential moments;
  • discrete and continuous BDG inequalities with explicit constants for the Ethier–Kurtz Itô integral;
  • an Itô-type or Gronwall argument for X−YˉNX-\bar Y^NX−YˉN.

The BDG inequalities and the Gaussian moment identity are reusable beyond this mission. Contributions to any lemma, or to the stochastic-calculus infrastructure underneath, are welcome.

Selected references

  • M. Hutzenthaler, A. Jentzen, P. E. Kloeden, Strong convergence of an explicit numerical method for SDEs with nonglobally Lipschitz continuous coefficients, Ann. Appl. Probab. 22(4), 1611–1641, 2012. https://arxiv.org/abs/1010.3756 (DOI 10.1214/11-AAP803)
  • M. Hutzenthaler, A. Jentzen, P. E. Kloeden, Strong and weak divergence in finite time of Euler's method for stochastic differential equations with non-globally Lipschitz continuous coefficients, Proc. R. Soc. A 467, 1563–1576, 2011. https://doi.org/10.1098/rspa.2010.0348
  • D. J. Higham, X. Mao, A. M. Stuart, Strong convergence of Euler-type methods for nonlinear stochastic differential equations, SIAM J. Numer. Anal. 40(3), 1041–1063, 2002. https://doi.org/10.1137/S0036142901389530
  • S. Sabanis, Euler approximations with varying coefficients: the case of superlinearly growing diffusion coefficients, Ann. Appl. Probab. 26(4), 2083–2105, 2016. https://arxiv.org/abs/1308.1796
  • X. Mao, Stochastic Differential Equations and Their Applications, Horwood, 1997 (Theorem 2.4.1: existence and uniqueness, cited on p. 2). https://mathscinet.ams.org/mathscinet-getitem?mr=1475218
  • M. B. Giles, Multilevel Monte Carlo path simulation, Oper. Res. 56, 607–617, 2008. https://doi.org/10.1287/opre.1070.0496
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Control TheoryDynamical SystemsGraph Theory·Captain: mikedeng1

Synchronization and Transient Stability in Power Networks and Nonuniform Kuramoto Oscillators 1: Γ_min > Γ_critical Gives Phase Cohesiveness and Exponential Frequency SynchronizationResearch Paper

Motivation

Transient stability asks whether a power grid, after a large disturbance such as a fault or a line trip, returns to synchronous operation in which all generators rotate at a common frequency. The classical approach builds energy functions for the swing equations and estimates regions of attraction numerically; it gives no closed-form test relating synchronization to the network's parameters, and it handles transfer conductances (losses) only when they are "sufficiently small" without saying how small.

Dörfler and Bullo (arXiv:0910.5673v4; SIAM J. Control Optim. 50(3), 2012) observe that, for strongly overdamped generators, the network-reduced swing equations behave like a first-order non-uniform Kuramoto model, and they give purely algebraic conditions under which this model synchronizes. The same model is a generalization of the classical Kuramoto model of coupled oscillators, studied in physics, neuroscience and control, with heterogeneous time constants, asymmetric effective coupling and phase shifts. This mission formalizes the first of the paper's two synchronization conditions, Theorem V.3, which is also statements 1)–2) of the paper's main result, Theorem III.2.

Setting

There are n≥2n \ge 2n≥2 oscillators with phases θ1,…,θn\theta_1, \dots, \theta_nθ1​,…,θn​. Each has a time constant Di>0D_i > 0Di​>0 and a natural frequency ωi∈R\omega_i \in \mathbb Rωi​∈R; each pair has a coupling weight Pij≥0P_{ij} \ge 0Pij​≥0 and a phase shift φij∈[0,π/2[\varphi_{ij} \in [0, \pi/2[φij​∈[0,π/2[, with Pii=φii=0P_{ii} = \varphi_{ii} = 0Pii​=φii​=0. The non-uniform Kuramoto model is

Di θ˙i=ωi−∑j=1nPijsin⁡(θi−θj+φij),i=1,…,n.(8)D_i\,\dot\theta_i = \omega_i - \sum_{j=1}^n P_{ij}\sin(\theta_i - \theta_j + \varphi_{ij}), \qquad i = 1, \dots, n. \tag{8}Di​θ˙i​=ωi​−j=1∑n​Pij​sin(θi​−θj​+φij​),i=1,…,n.(8)

The phases live on the torus. For an arc length γ∈[0,π]\gamma \in [0, \pi]γ∈[0,π], the set Δ(γ)\Delta(\gamma)Δ(γ) consists of configurations whose phases all lie in the interior of some arc of length γ\gammaγ, and Δˉ(γ)\bar\Delta(\gamma)Δˉ(γ) is its closure (with the synchronized configurations). A set is positively invariant if every solution starting in it stays in it. A solution achieves exponential frequency synchronization if all frequencies θ˙i(t)\dot\theta_i(t)θ˙i​(t) converge exponentially fast to a common value θ˙∞\dot\theta_\inftyθ˙∞​.

The condition of the theorem compares two numbers built from the parameters, with φmax⁡=max⁡i,jφij\varphi_{\max} = \max_{i,j}\varphi_{ij}φmax​=maxi,j​φij​:

Γmin⁡:=nmin⁡i≠j{PijDicos⁡φij},Γcritical:=1cos⁡φmax⁡(max⁡i≠j∣ωiDi−ωjDj∣+2max⁡i∑j=1nPijDisin⁡φij).\Gamma_{\min} := n\min_{i\neq j}\Big\{\frac{P_{ij}}{D_i}\cos\varphi_{ij}\Big\},\qquad \Gamma_{\mathrm{critical}} := \frac{1}{\cos\varphi_{\max}}\Big(\max_{i\neq j}\Big|\frac{\omega_i}{D_i}-\frac{\omega_j}{D_j}\Big| + 2\max_i\sum_{j=1}^n\frac{P_{ij}}{D_i}\sin\varphi_{ij}\Big).Γmin​:=ni=jmin​{Di​Pij​​cosφij​},Γcritical​:=cosφmax​1​(i=jmax​​Di​ωi​​−Dj​ωj​​​+2imax​j=1∑n​Di​Pij​​sinφij​).

Γmin⁡\Gamma_{\min}Γmin​ is the weakest lossless coupling of an oscillator to the network; Γcritical\Gamma_{\mathrm{critical}}Γcritical​ measures the spread of natural frequencies and the losses. When Γmin⁡>Γcritical\Gamma_{\min} > \Gamma_{\mathrm{critical}}Γmin​>Γcritical​, put c=cos⁡(φmax⁡)Γcritical/Γmin⁡c = \cos(\varphi_{\max})\Gamma_{\mathrm{critical}}/\Gamma_{\min}c=cos(φmax​)Γcritical​/Γmin​, γmin⁡=arcsin⁡c∈[0,π/2−φmax⁡[\gamma_{\min} = \arcsin c \in [0, \pi/2-\varphi_{\max}[γmin​=arcsinc∈[0,π/2−φmax​[ and γmax⁡=π−arcsin⁡c∈ ]π/2,π]\gamma_{\max} = \pi - \arcsin c \in\, ]\pi/2, \pi]γmax​=π−arcsinc∈]π/2,π].

Formalization targets

Goal: Theorem V.3 (Synchronization condition I), corrected

If P=PTP = P^TP=PT is complete (Pij>0P_{ij} > 0Pij​>0 for i≠ji \ne ji=j) and

Γmin⁡>Γcritical,(26)\Gamma_{\min} > \Gamma_{\mathrm{critical}}, \tag{26}Γmin​>Γcritical​,(26)

then (1) Δˉ(γ)\bar\Delta(\gamma)Δˉ(γ) is positively invariant for every γ∈[γmin⁡,γmax⁡]\gamma \in [\gamma_{\min}, \gamma_{\max}]γ∈[γmin​,γmax​], and every solution starting in Δ(γmax⁡)\Delta(\gamma_{\max})Δ(γmax​) eventually stays in Δˉ(γ)\bar\Delta(\gamma)Δˉ(γ) for each γ∈ ]γmin⁡,γmax⁡]\gamma \in\, ]\gamma_{\min}, \gamma_{\max}]γ∈]γmin​,γmax​]; (2) every solution starting in Δ(γmax⁡)\Delta(\gamma_{\max})Δ(γmax​) achieves exponential frequency synchronization to some θ˙∞\dot\theta_\inftyθ˙∞​, and θ˙∞∈[θ˙min⁡(0),θ˙max⁡(0)]\dot\theta_\infty \in [\dot\theta_{\min}(0), \dot\theta_{\max}(0)]θ˙∞​∈[θ˙min​(0),θ˙max​(0)] when the solution starts in Δ(π/2−φmax⁡)\Delta(\pi/2 - \varphi_{\max})Δ(π/2−φmax​).

Milestones

The milestones follow the paper's proof. Theorem V.1 is a frequency-synchronization theorem for phase-cohesive oscillators under a globally reachable node, with the explicit rate

λfe=λ2(L(Pij))cos⁡(γ)cos⁡(∠(D1,1))2/Dmax⁡\lambda_{fe} = \lambda_2(L(P_{ij}))\cos(\gamma)\cos(\angle(D\mathbf 1, \mathbf 1))^2/D_{\max}λfe​=λ2​(L(Pij​))cos(γ)cos(∠(D1,1))2/Dmax​

when φ≡0\varphi \equiv 0φ≡0 and P=PTP = P^TP=PT. Its supporting steps are the frequency dynamics (20) and a dihedral-angle bound. The phase-cohesiveness argument of Theorem V.3 is split into a trigonometric lower bound, a pointwise bound on the growth rate of the arc containing all phases, the characterization of [γmin⁡,γmax⁡][\gamma_{\min}, \gamma_{\max}][γmin​,γmax​] by inequality (30), positive invariance, and the entry into Δˉ(π/2−φmax⁡)\bar\Delta(\pi/2 - \varphi_{\max})Δˉ(π/2−φmax​).

Significance

The theorem turns synchronization of a heterogeneous, lossy oscillator network into one inequality among explicit parameters. For the classical Kuramoto model it specializes to K>ωmax⁡−ωmin⁡K > \omega_{\max} - \omega_{\min}K>ωmax​−ωmin​ (Remark V.4), which improved the sufficient conditions known at the time. For power networks it gives, through Theorem III.2, a computable sufficient condition for transient stability when generator inertia is small relative to damping.

To our knowledge none of these results has a machine-checked proof. The development needs ODE comparison arguments for a non-smooth Lyapunov function (the arc length) and an exponential convergence theorem for time-varying consensus. Both are general tools that are not in Mathlib and would be reusable for other consensus and synchronization results. The mission also records two clauses of the printed theorem that are false as stated, with counterexamples, and states the corrected theorem.

Difficulty

The arc length V(θ)=max⁡i,j(θi−θj)V(\theta) = \max_{i,j}(\theta_i - \theta_j)V(θ)=maxi,j​(θi​−θj​) is only Lipschitz, so its decrease along solutions must be argued through Dini derivatives and a comparison lemma rather than by differentiation. Positive invariance at the boundary γ=γmin⁡\gamma = \gamma_{\min}γ=γmin​ holds with a non-strict inequality, so a naive "strictly decreasing at the boundary" argument does not apply there. Frequency synchronization rests on a contraction property of linear consensus with time-varying, state-dependent weights. The weights are positive only after the phases have entered Δˉ(π/2−φmax⁡)\bar\Delta(\pi/2 - \varphi_{\max})Δˉ(π/2−φmax​). Before that the frequency range can expand, which is why the range clause of the printed theorem fails for initial arcs longer than π/2−φmax⁡\pi/2 - \varphi_{\max}π/2−φmax​.

Formalization scope

Phases are represented by real lifts θ:Fin n→R\theta : \mathrm{Fin}\,n \to \mathbb Rθ:Finn→R. Δˉ(γ)\bar\Delta(\gamma)Δˉ(γ) means that all pairwise differences of the lift are at most γ\gammaγ, and Δ(γ)\Delta(\gamma)Δ(γ) that they are strictly less than γ\gammaγ. Conclusions are stated for the same continuous lift, which is at least as strong as membership on the torus. A solution is a map θ:R→Rn\theta : \mathbb R \to \mathbb R^nθ:R→Rn with derivative (one-sided at 000) equal to the right-hand side of (8) for all t≥0t \ge 0t≥0. Every statement quantifies over all such solutions. θ˙\dot\thetaθ˙ always denotes the vector field along the solution. Minima and maxima over i≠ji \ne ji=j are over ordered pairs, and n≥2n \ge 2n≥2 is assumed so that they exist. The conventions Pii=φii=0P_{ii} = \varphi_{ii} = 0Pii​=φii​=0 are explicit hypotheses. γmin⁡\gamma_{\min}γmin​ and γmax⁡\gamma_{\max}γmax​ are defined by arcsin⁡\arcsinarcsin, and a milestone certifies that they are the unique solutions in the printed ranges. λ2\lambda_2λ2​ is the second-smallest eigenvalue of the symmetric Laplacian.

The source is the arXiv preprint v4 of the SICON article, cited with its own page and theorem numbers. Three corrections relative to the printed text are made and disclosed in the items:

  • "each trajectory starting in Δ(γmax⁡)\Delta(\gamma_{\max})Δ(γmax​) reaches Δˉ(γmin⁡)\bar\Delta(\gamma_{\min})Δˉ(γmin​)" holds only asymptotically (n=2n = 2n=2, φ≡0\varphi \equiv 0φ≡0, D≡1D \equiv 1D≡1, P12=1P_{12} = 1P12​=1, ω=(1,0)\omega = (1, 0)ω=(1,0): the phase difference tends to the equilibrium π/6=γmin⁡\pi/6 = \gamma_{\min}π/6=γmin​ without reaching it). It is stated for every γ>γmin⁡\gamma > \gamma_{\min}γ>γmin​.
  • the frequency range [θ˙min⁡(0),θ˙max⁡(0)][\dot\theta_{\min}(0), \dot\theta_{\max}(0)][θ˙min​(0),θ˙max​(0)] fails for some initial conditions in Δ(γmax⁡)\Delta(\gamma_{\max})Δ(γmax​) (n=2n = 2n=2, D≡1D \equiv 1D≡1, ω≡0\omega \equiv 0ω≡0, P12=1P_{12} = 1P12​=1, φ12=φ21=1/2\varphi_{12} = \varphi_{21} = 1/2φ12​=φ21​=1/2, θ(0)=(2.4,0)\theta(0) = (2.4, 0)θ(0)=(2.4,0)). It is stated for initial conditions in Δ(π/2−φmax⁡)\Delta(\pi/2 - \varphi_{\max})Δ(π/2−φmax​), while exponential synchronization is stated for all of Δ(γmax⁡)\Delta(\gamma_{\max})Δ(γmax​).
  • the rate (19) is printed with a leading minus sign but is used as a positive decay rate. The positive rate is stated.

No statement is trivially satisfiable. The solution predicate holds for actual solutions (for example the synchronous solution), condition (26) is satisfiable (take ω≡0\omega \equiv 0ω≡0 and φ≡0\varphi \equiv 0φ≡0), the exponential rate is required to be strictly positive, and γmin⁡,γmax⁡\gamma_{\min}, \gamma_{\max}γmin​,γmax​ are specific numbers rather than existential witnesses.

Contributions are welcome on all milestones. The trigonometric bound, the dihedral-angle bound and the γmin⁡/γmax⁡\gamma_{\min}/\gamma_{\max}γmin​/γmax​ characterization are elementary. The comparison lemma for Dini derivatives and the consensus contraction theorem are reusable infrastructure.

Selected references

  • F. Dörfler, F. Bullo, Synchronization and Transient Stability in Power Networks and Nonuniform Kuramoto Oscillators, SIAM J. Control Optim. 50(3), 2012; preprint arXiv:0910.5673v4. https://arxiv.org/abs/0910.5673v4 — DOI: https://doi.org/10.1137/110851584
  • L. Moreau, Stability of continuous-time distributed consensus algorithms, 43rd IEEE CDC, 2004 (the contraction theorem cited as [53, Theorem 1]). https://arxiv.org/abs/math/0409010
  • Y. Kuramoto, Self-entrainment of a population of coupled non-linear oscillators, Int. Symp. on Mathematical Problems in Theoretical Physics, Lecture Notes in Physics 39, 1975. https://doi.org/10.1007/BFb0013365
  • H.-D. Chiang, F. F. Wu, P. P. Varaiya, Foundations of direct methods for power system transient stability analysis, IEEE Trans. Circuits Syst. 34(2), 1987. https://doi.org/10.1109/TCS.1987.1086115
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Graph TheoryLinear algebraProbability+1·Captain: mikedeng1

Spectral Sparsification of Graphs 1: Sampling Each Edge of a High-Conductance Graph with Probability min(1, Υ/min(dᵢ, dⱼ)) Gives a (1+ε)-Spectral Approximation with Few EdgesResearch Paper

Motivation

A spectral sparsifier of a graph is a much sparser weighted graph whose Laplacian quadratic form is within a factor σ\sigmaσ of the original on every vector. Spielman and Teng introduced the notion in Spectral Sparsification of Graphs as a strengthening of the cut sparsifiers of Benczúr and Karger: a spectral sparsifier preserves every cut, and in addition every quantity determined by the Laplacian quadratic form, such as effective resistances, eigenvalues and the behaviour of random walks. Sparsifiers are the reason linear systems in graph Laplacians can be solved in nearly linear time: one preconditions with a sparsifier and solves the sparse system instead (Spielman–Teng, arXiv:cs/0607105).

The construction in the paper has two halves: decompose the graph into pieces of high conductance, then sparsify each piece by random sampling. This mission is the second half, Theorem 6.1 of §6: in a graph whose normalized Laplacian has a spectral gap, keeping each edge independently with probability inversely proportional to the smaller degree of its endpoints, and reweighting kept edges by the inverse probability, produces a (1+ϵ)(1+\epsilon)(1+ϵ)-spectral approximation with few edges, with high probability.

Timeline. Benczúr and Karger (1996) sampled edges with probabilities depending on edge strength and preserved cuts. Achlioptas and McSherry (2001) analysed random sampling of matrices through the random-matrix norm bound of Füredi and Komlós (1981), corrected by Vu (2007). Spielman and Teng (arXiv 2008, SIAM J. Comput. 2011) proved Theorem 6.1 by refining the Füredi–Komlós trace method for downsampling graphs that may already be sparse. Spielman and Srivastava (2008) later replaced conductance-based probabilities by effective resistances.

Setting

Let G=(V,E)G=(V,E)G=(V,E) be an unweighted graph on a finite vertex set VVV, n=∣V∣n=|V|n=∣V∣, with degrees did_idi​, adjacency matrix AAA, diagonal degree matrix DDD and Laplacian LG=D−AL_G=D-ALG​=D−A. Its quadratic form is

xTLGx=∑{u,v}∈E(x(u)−x(v))2,x∈RV.x^TL_Gx=\sum_{\{u,v\}\in E}(x(u)-x(v))^2,\qquad x\in\mathbb R^V .xTLG​x={u,v}∈E∑​(x(u)−x(v))2,x∈RV.

A weighted graph G~\widetilde GG on VVV with weights w(u,v)≥0w(u,v)\ge0w(u,v)≥0 has the form xTLG~x=∑{u,v}w(u,v)(x(u)−x(v))2x^TL_{\widetilde G}x=\sum_{\{u,v\}}w(u,v)(x(u)-x(v))^2xTLG​x=∑{u,v}​w(u,v)(x(u)−x(v))2. G~\widetilde GG is a σ\sigmaσ-approximation of GGG if for all xxx

1σ xTLG~x≤xTLGx≤σ xTLG~x.\tfrac1\sigma\,x^TL_{\widetilde G}x\le x^TL_Gx\le\sigma\,x^TL_{\widetilde G}x .σ1​xTLG​x≤xTLG​x≤σxTLG​x.

When every degree is positive, the normalized Laplacian is LG=D−1/2LGD−1/2\mathcal L_G=D^{-1/2}L_GD^{-1/2}LG​=D−1/2LG​D−1/2; its eigenvalues lie in [0,2][0,2][0,2], and a lower bound λ\lambdaλ on its smallest non-zero eigenvalue measures how well connected each component of GGG is (by Cheeger's inequality it is equivalent to high conductance up to squaring).

Sampling. For a parameter Υ>1\Upsilon>1Υ>1, edge (i,j)(i,j)(i,j) is assigned

pi,j=min⁡(1,Υmin⁡(di,dj)),p_{i,j}=\min\Big(1,\frac{\Upsilon}{\min(d_i,d_j)}\Big),pi,j​=min(1,min(di​,dj​)Υ​),

each edge is kept independently with probability pi,jp_{i,j}pi,j​, and a kept edge gets weight 1/pi,j1/p_{i,j}1/pi,j​. The sampled adjacency matrix A~\widetilde AA then has E[A~]=A\mathbf E[\widetilde A]=AE[A]=A; D~\widetilde DD is the diagonal matrix of weighted degrees of the sampled graph.

The procedure. In Theorem 6.1 sampling is applied only to the edges FFF of an induced subgraph G(S)G(S)G(S), S⊆VS\subseteq VS⊆V; the other edges H=E−FH=E-FH=E−F are kept with weight 1. Sample((S,F),ϵ,p,λ)\mathtt{Sample}((S,F),\epsilon,p,\lambda)Sample((S,F),ϵ,p,λ) sets Υ=(12k/(ϵλ))2\Upsilon=(12k/(\epsilon\lambda))^2Υ=(12k/(ϵλ))2 and uses the degrees did_idi​ of G(S)G(S)G(S); the paper takes k=max⁡(log⁡2(3/p),log⁡2∣S∣)k=\max(\log_2(3/p),\log_2|S|)k=max(log2​(3/p),log2​∣S∣).

Formalization targets

Goal: Theorem 6.1 (p. 8)

For ϵ,p∈(0,1/2)\epsilon,p\in(0,1/2)ϵ,p∈(0,1/2), GGG without isolated vertices whose smallest non-zero normalized Laplacian eigenvalue is at least λ>0\lambda>0λ>0, S⊆VS\subseteq VS⊆V, and an even integer k≥max⁡(log⁡2(3/p),log⁡2∣S∣)k\ge\max(\log_2(3/p),\log_2|S|)k≥max(log2​(3/p),log2​∣S∣): with probability at least 1−p1-p1−p, simultaneously

(S.1)  G~=(V,F~∪H) is a (1+ϵ)-approximation of G,(S.2)  ∣F~∣≤288 k2(ϵλ)2 ∣S∣.\text{(S.1)}\ \ \widetilde G=(V,\widetilde F\cup H)\ \text{is a }(1+\epsilon)\text{-approximation of }G,\qquad \text{(S.2)}\ \ |\widetilde F|\le\frac{288\,k^2}{(\epsilon\lambda)^2}\,|S| .(S.1)  G=(V,F∪H) is a (1+ϵ)-approximation of G,(S.2)  ∣F∣≤(ϵλ)2288k2​∣S∣.

Milestones, in the order the proof uses them

  • Lemma 6.2 (p. 8): if λ2(D−1/2LD−1/2)≥λ\lambda_2(D^{-1/2}LD^{-1/2})\ge\lambdaλ2​(D−1/2LD−1/2)≥λ and ∥D−1/2(L−L~)D−1/2∥≤ϵ<λ\|D^{-1/2}(L-\widetilde L)D^{-1/2}\|\le\epsilon<\lambda∥D−1/2(L−L)D−1/2∥≤ϵ<λ, then G~\widetilde GG is a λ/(λ−ϵ)\lambda/(\lambda-\epsilon)λ/(λ−ϵ)-approximation of a connected GGG.
  • Claim 6.5 (p. 13): ∣Δi,j∣≤1/Υ|\Delta_{i,j}|\le1/\Upsilon∣Δi,j​∣≤1/Υ for Δ=D−1(A~−A)\Delta=D^{-1}(\widetilde A-A)Δ=D−1(A−A), on every outcome of positive probability.
  • Lemma 6.6 (p. 13): E[Δr,tkΔt,rl]≤Υ−(k+l−1)dr−1\mathbf E[\Delta_{r,t}^k\Delta_{t,r}^l]\le\Upsilon^{-(k+l-1)}d_r^{-1}E[Δr,tk​Δt,rl​]≤Υ−(k+l−1)dr−1​ for every edge, k≥1k\ge1k≥1, l≥0l\ge0l≥0.
  • Lemma 6.4 (p. 10): E[Tr⁡(Δk)]≤nkk/Υk/2\mathbf E[\operatorname{Tr}(\Delta^k)]\le nk^k/\Upsilon^{k/2}E[Tr(Δk)]≤nkk/Υk/2 for even kkk.
  • Lemma 6.3 (p. 9): Pr⁡[∥D−1/2(A~−A)D−1/2∥≥2kn1/k/Υ]≤2−k\Pr[\|D^{-1/2}(\widetilde A-A)D^{-1/2}\|\ge 2kn^{1/k}/\sqrt\Upsilon]\le2^{-k}Pr[∥D−1/2(A−A)D−1/2∥≥2kn1/k/Υ​]≤2−k for even k>0k>0k>0.
  • Theorem 6.8 (p. 15, Chernoff bound, cited from Raghavan 1988).
  • Lemma 6.7 (p. 14): Pr⁡[∥D−1/2(D−D~)D−1/2∥≥ϵ]≤2ne−Υϵ2/3\Pr[\|D^{-1/2}(D-\widetilde D)D^{-1/2}\|\ge\epsilon]\le2ne^{-\Upsilon\epsilon^2/3}Pr[∥D−1/2(D−D)D−1/2∥≥ϵ]≤2ne−Υϵ2/3 for 0<ϵ<10<\epsilon<10<ϵ<1.

Significance

Theorem 6.1 is the sampling engine of the first nearly-linear-time spectral sparsification algorithm: combined with a decomposition of an arbitrary graph into high-conductance pieces (§7–§10 of the paper), it yields sparsifiers with O(nlog⁡cn/ϵ2)O(n\log^c n/\epsilon^2)O(nlogcn/ϵ2) edges, which in turn give the nearly-linear-time Laplacian solvers that underlie fast algorithms for electrical flows, maximum flow approximation and graph partitioning. Lemma 6.3 is a self-contained random-matrix result: a norm bound for the normalized deviation of a downsampled graph that does not assume the original graph is dense.

The result is proved in the paper. As far as is known, none of it is formalized in Lean or Mathlib: Mathlib has the graph Laplacian (SimpleGraph.lapMatrix) and the spectral theorem for Hermitian matrices, but no normalized Laplacian, no spectral approximation and no trace-method bounds for random matrices. A complete formalization would be the first machine-checked proof of a spectral sparsification theorem, and the milestones (the trace-method moment bound, Chernoff for weighted two-point sums) are reusable on their own.

Difficulty

The obvious argument — bound each entry of A~−A\widetilde A-AA−A and apply a matrix concentration inequality — needs either a matrix Chernoff bound (not in the paper, and not in Mathlib) or the Füredi–Komlós trace method, which assumes every edge can appear and so fails when the graph is already sparse: a vertex of small degree has no room for its entries to average out. The paper's sampling probabilities keep every edge at a vertex of degree at most Υ\UpsilonΥ, and the trace computation has to exploit exactly this through the moment bound of Lemma 6.6 and a combinatorial count of closed walks. Formally, the obstacles are the walk-counting argument of Lemma 6.4, the passage from a trace bound to an eigenvalue bound for the non-symmetric Δ\DeltaΔ (similar to a symmetric matrix), and Lemma 6.2's restriction to the orthogonal complement of the kernel, which must handle disconnected GGG in the goal.

Formalization scope

  • Vertex sets are finite types V; graphs are SimpleGraph V with decidable adjacency; weighted graphs are weight functions V → V → ℝ (symmetric, nonnegative, loopless). The quadratic form is 12∑u,vw(u,v)(x(u)−x(v))2\frac12\sum_{u,v}w(u,v)(x(u)-x(v))^221​∑u,v​w(u,v)(x(u)−x(v))2; a σ\sigmaσ-approximation keeps both inequalities of (2).
  • The probability space is explicit: an outcome is the set TTT of kept edges, with probability ∏e∈Tpe∏e∉T(1−pe)\prod_{e\in T}p_e\prod_{e\notin T}(1-p_e)∏e∈T​pe​∏e∈/T​(1−pe​); probabilities and expectations are finite sums. The goal is a probability bound over this law, not the existence of a good set of edges, which would be a much weaker statement.
  • Eigenvalue conditions are stated with real eigenpairs: "smallest non-zero eigenvalue ≥λ\ge\lambda≥λ" means every eigenvalue μ≠0\mu\ne0μ=0 satisfies μ≥λ\mu\ge\lambdaμ≥λ; "∥M∥≤t\|M\|\le t∥M∥≤t" ("≥t\ge t≥t") for symmetric MMM means every (some) eigenvalue has absolute value ≤t\le t≤t (≥t\ge t≥t).
  • Hypotheses made explicit (the paper leaves them implicit): in Theorem 6.1, kkk is an even integer with k≥log⁡2(3/p)k\ge\log_2(3/p)k≥log2​(3/p), k≥log⁡2∣S∣k\ge\log_2|S|k≥log2​∣S∣ (the proof applies Lemma 6.3 with Sample's kkk, which the paper defines as a real maximum; the printed statement is the case where that maximum is an even integer), every vertex has degree ≥1\ge1≥1, and λ>0\lambda>0λ>0; in Lemma 6.2, 0≤ϵ<λ0\le\epsilon<\lambda0≤ϵ<λ; in Lemma 6.7, 0<ϵ<10<\epsilon<10<ϵ<1 (without it the printed bound is false for large ϵ\epsilonϵ); in Lemmas 6.3–6.7 and Claim 6.5, positive degrees; in Lemma 6.3, k>0k>0k>0; in Theorem 6.8, β>0\beta>0β>0, ϵ>0\epsilon>0ϵ>0, pi∈[0,1]p_i\in[0,1]pi​∈[0,1]. GGG is not assumed connected in Theorem 6.1.
  • In Theorem 6.1 the probabilities use the degrees of G(S)G(S)G(S) (the input of Sample\mathtt{Sample}Sample), while λ\lambdaλ refers to GGG; nnn in Sample\mathtt{Sample}Sample is ∣S∣|S|∣S∣.
  • Trivializing readings ruled out: a one-sided "approximation", a goal that chooses the kept edges existentially, and a spectral hypothesis with λ≤0\lambda\le0λ≤0 or without positive degrees are all excluded by the statements.
  • Out of scope: running times, the decomposition algorithms of §7–§10, Cheeger's inequality (Theorem 4.1, cited and not used here), the weighted generalization remarked on p. 10, and the use of Theorem 6.1 in Lemma 9.1.
  • Contributions welcome: proofs of any milestone; a Loewner-order formulation equivalence; a general matrix Chernoff or trace-method library from which Lemma 6.3 follows.

Selected references

  • D. A. Spielman, S.-H. Teng, Spectral Sparsification of Graphs, arXiv:0808.4134v3, 2010; SIAM J. Comput. 40(4), 2011. https://arxiv.org/abs/0808.4134
  • A. A. Benczúr, D. R. Karger, Approximating s-t minimum cuts in Õ(n²) time, STOC 1996. https://doi.org/10.1145/237814.237827
  • D. Achlioptas, F. McSherry, Fast computation of low rank matrix approximations, STOC 2001. https://doi.org/10.1145/380752.380858
  • Z. Füredi, J. Komlós, The eigenvalues of random symmetric matrices, Combinatorica 1(3), 1981. https://doi.org/10.1007/BF02579329
  • V. H. Vu, Spectral norm of random matrices, Combinatorica 27(6), 2007. https://doi.org/10.1007/s00493-007-2190-z
  • P. Raghavan, Probabilistic construction of deterministic algorithms: approximating packing integer programs, J. Comput. Syst. Sci. 37(2), 1988. https://doi.org/10.1016/0022-0000(88)90003-7
  • D. A. Spielman, N. Srivastava, Graph sparsification by effective resistances, STOC 2008; arXiv:0803.0929. https://arxiv.org/abs/0803.0929
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AdWords and Generalized On-line Matching I: The Tradeoff Algorithm with ψ_k(i) = Σ_{j≥i} y*_j Is (1 − 1/e)-Competitive as k → ∞ When Bids Are SmallResearch Paper

Motivation

Search engines sell advertising space query by query. Each advertiser states a bid for each keyword and a daily budget; queries arrive one at a time, and each must be assigned to an advertiser immediately, without knowledge of the queries still to come. The revenue-maximizing assignment of the day can only be computed offline. The adwords problem asks how close an online rule can get to it. It generalizes online bipartite matching, for which Karp, Vazirani and Vazirani (KVV 1990) showed that randomized ranking attains ratio 1−1/e1-1/e1−1/e, and bbb-matching, for which Kalyanasundaram and Pruhs (KP 2000) showed that the deterministic BALANCE algorithm attains 1−1/e1-1/e1−1/e as the budget grows.

Mehta, Saberi, Vazirani and Vazirani (J. ACM 2007) gave a deterministic algorithm for arbitrary bids that weighs each bid by a function of the fraction of budget already spent, and proved that it is (1−1/e)(1-1/e)(1−1/e)-competitive when bids are small compared to budgets. The algorithm and its tradeoff function became the reference point for the online budgeted-allocation literature, including the primal-dual analysis of Buchbinder, Jain and Naor (ESA 2007).

Setting

There are NNN bidders, each with budget 111, and a sequence of MMM queries q1,…,qMq_1,\dots,q_Mq1​,…,qM​. Bidder bbb bids cb,t≥0c_{b,t}\ge0cb,t​≥0 for the query at position ttt. An allocation σ\sigmaσ assigns each query to at most one bidder. Bidder bbb's spend before position ttt is min⁡(1,∑s<t, σ(s)=bcb,s)\min(1,\sum_{s<t,\,\sigma(s)=b}c_{b,s})min(1,∑s<t,σ(s)=b​cb,s​), and bbb is alive while its spend is below 111. The revenue of σ\sigmaσ is rev(σ)=∑bmin⁡(1,∑t:σ(t)=bcb,t)\mathrm{rev}(\sigma)=\sum_b\min(1,\sum_{t:\sigma(t)=b}c_{b,t})rev(σ)=∑b​min(1,∑t:σ(t)=b​cb,t​).

Fix an integer kkk and split each budget into kkk equal slabs; a spent fraction s∈((j−1)/k,j/k]s\in((j-1)/k,j/k]s∈((j−1)/k,j/k] lies in slab jjj, and s=0s=0s=0 in slab 111. Given a tradeoff function ψ\psiψ on slabs, the discrete tradeoff algorithm assigns each arriving query to an alive bidder maximizing

cb,t ψ(slab(b)),c_{b,t}\,\psi(\mathrm{slab}(b)),cb,t​ψ(slab(b)),

ties broken arbitrarily. Every allocation produced this way, for any tie-breaking, is a run.

The analysis uses the factor-revealing LP LLL: maximize ∑i=1k−1k−ikxi\sum_{i=1}^{k-1}\frac{k-i}{k}x_i∑i=1k−1​kk−i​xi​ subject to ∑j=1i(1+i−jk)xj≤ikN\sum_{j=1}^{i}(1+\frac{i-j}{k})x_j\le\frac ikN∑j=1i​(1+ki−j​)xj​≤ki​N and x≥0x\ge0x≥0, written max⁡c⋅x\max c\cdot xmaxc⋅x, Ax≤bAx\le bAx≤b, x≥0x\ge0x≥0, and its dual DDD. Its optimal dual solution is yi∗=1k(1−1k)k−i−1y^*_i=\frac1k(1-\frac1k)^{k-i-1}yi∗​=k1​(1−k1​)k−i−1, and Theorem 8's tradeoff function is

ψk(i)=∑j=ik−1yj∗.\psi_k(i)=\sum_{j=i}^{k-1}y^*_j .ψk​(i)=j=i∑k−1​yj∗​.

Formalization targets

Goal: Theorem 8 (p. 12)

For every δ>0\delta>0δ>0 there is k0k_0k0​ such that for every k≥k0k\ge k_0k≥k0​ there is η>0\eta>0η>0 such that, for every instance with bids in [0,η][0,\eta][0,η], every run σ\sigmaσ of the algorithm with ψk\psi_kψk​, and every allocation τ\tauτ,

rev(σ) ≥ (1−1e−δ)rev(τ).\mathrm{rev}(\sigma)\ \ge\ \Bigl(1-\frac1e-\delta\Bigr)\mathrm{rev}(\tau).rev(σ) ≥ (1−e1​−δ)rev(τ).

The goal fixes no rate in kkk or η\etaη: it asserts only that the ratio tends to 1−1/e1-1/e1−1/e.

Milestones

  1. Proof of Lemma 3 (pp. 8–9): xi∗=Nk(1−1k)i−1x^*_i=\frac Nk(1-\frac1k)^{i-1}xi∗​=kN​(1−k1​)i−1 and y∗y^*y∗ are optimal for LLL and DDD, with value N(1−1/k)kN(1-1/k)^kN(1−1/k)k.
  2. Lemma 3 (p. 8): the value of LLL and DDD tends to N/eN/eN/e.
  3. Lemma 4 (p. 10): for every nonnegative aaa and l=Aal=Aal=Aa, y∗y^*y∗ minimizes l⋅yl\cdot yl⋅y over the constraints of DDD.
  4. Lemma 5 (p. 10): l=b+Δl=b+\Deltal=b+Δ under the relation βi=N/k−(α1+⋯+αi−1)/k\beta_i=N/k-(\alpha_1+\dots+\alpha_{i-1})/kβi​=N/k−(α1​+⋯+αi−1​)/k.
  5. Lemma 6 (p. 11): OPT(q)ψ(type(q))≤ALG(q)ψ(slab(q))\mathrm{OPT}(q)\psi(\mathrm{type}(q))\le\mathrm{ALG}(q)\psi(\mathrm{slab}(q))OPT(q)ψ(type(q))≤ALG(q)ψ(slab(q)) when 1≤type(q)≤k−11\le\mathrm{type}(q)\le k-11≤type(q)≤k−1.
  6. Lemma 7 (p. 11): ∑i=1k−1ψ(i)(αi−βi)≤N/k\sum_{i=1}^{k-1}\psi(i)(\alpha_i-\beta_i)\le N/k∑i=1k−1​ψ(i)(αi​−βi​)≤N/k, for a monotonically decreasing nonnegative ψ\psiψ with ψ(k)=0\psi(k)=0ψ(k)=0 (such as ψk\psi_kψk​).

Significance

Theorem 8 gives an online algorithm for budgeted allocation with arbitrary bids whose revenue is within a factor 1−1/e1-1/e1−1/e of the offline optimum, the best possible ratio even for randomized algorithms (Theorem 9 of the same paper, the second mission of this series). It reduces to BALANCE when all bids are equal, and its tradeoff function 1−ex−11-e^{x-1}1−ex−1 in the limit is the function used in later work on online budgeted allocation and display-ad allocation.

The result is proved in the paper; none of it is formalized. The work here is to formalize the proof in a version that holds for actual runs. The paper's argument makes two simplifications with "negligible error": bidders of type jjj spend exactly j/kj/kj/k of their budget, and the offline optimum exhausts every budget. A formal proof must carry the bid size through the slab boundaries and compare with an arbitrary offline allocation. The LP lemmas (Lemmas 3–5) are self-contained statements about one triangular linear program and are reusable for factor-revealing analyses of BALANCE.

Difficulty

The milestones are short: Lemmas 3–5 are finite linear algebra with geometric sums, Lemma 6 is one application of the assignment rule plus monotonicity of spend, and Lemma 7 regroups finite sums. The difficulty is in Theorem 8. The paper's proof chains Lemmas 4, 5 and 7 through the LP L(π,ψ)L(\pi,\psi)L(π,ψ), whose right-hand side is computed from the numbers αj\alpha_jαj​ of bidders of each type under the assumption that a bidder of type jjj spends exactly j/kj/kj/k. In an actual run this identity fails: a single bid can straddle a slab boundary, and types are intervals, not points. So the chain does not compose literally, and the natural first attempt, instantiating Lemma 5 with the run's quantities, does not apply. The slab-wise inequalities that do hold, with an error of order kηk\etakη, have to replace the equalities, and the comparison with an offline allocation that does not exhaust budgets has to be made through capped revenues.

Formalization scope

Bidders are Fin N and query positions Fin M, zero-based; slabs and LP coordinates keep the paper's 1-based ranges, with vectors as functions N→R\mathbb N\to\mathbb RN→R read on 1≤i≤k−11\le i\le k-11≤i≤k−1. Budgets are 111 (the paper's standing simplification of §2). Bids are real and nonnegative.

A run is a predicate on the whole allocation: at position ttt, if some bidder is alive the query goes to an alive maximizer of bid × ψ(slab)\times\,\psi(\text{slab})×ψ(slab), where spends are computed from earlier positions only; the query is unassigned only when all budgets are exhausted. Every tie-breaking rule gives a run, and the goal holds for all of them. ALG(q)\mathrm{ALG}(q)ALG(q) is the full bid of the chosen bidder; revenue is capped at the budget.

Conventions the statements commit to:

  • ψk\psi_kψk​ is the defining sum of Theorem 8. The closed form printed beside it, 1−(1−1/k)k−i+11-(1-1/k)^{k-i+1}1−(1−1/k)k−i+1, is off by one in the exponent; the sum equals 1−(1−1/k)k−i1-(1-1/k)^{k-i}1−(1−1/k)k−i and vanishes at slab kkk.
  • "As k→∞k\to\inftyk→∞" is ∀δ ∃k0 ∀k≥k0\forall\delta\,\exists k_0\,\forall k\ge k_0∀δ∃k0​∀k≥k0​; "bids small compared to budgets" is a bound η\etaη chosen after kkk, never depending on the instance.
  • The comparator is every allocation τ\tauτ, not an optimum that exhausts all budgets; the paper says the proof extends without that assumption (§4, §6 item 2). Only the lower bound on the ratio is stated.
  • Lemma 4 quantifies over every nonnegative vector aaa, through which alone the instance and ψ\psiψ enter D(π,ψ)D(\pi,\psi)D(π,ψ). Lemma 5 takes the paper's relation for βi\beta_iβi​ as a hypothesis. Lemma 7 defines αi,βi\alpha_i,\beta_iαi​,βi​ as the query sums of its proof, and adds ψ(k)=0\psi(k)=0ψ(k)=0 in place of the paper's bound on the slab-kkk term, which rests on its exact-spend simplification.

Trivializing formalizations are ruled out: a run cannot leave a query unassigned while a bidder has budget, so the empty allocation is not a run; no hypothesis of the form "bidders of type jjj spend exactly j/kj/kj/k" or "the optimum exhausts every budget" is imposed, since either would make the goal vacuous on most instances.

All definitions are local to the namespace AdWordsMSVV.Tradeoff. Related platform items analyse a different algorithm: BJNAdAuctions.Basic.* and OnlinePrimalDual.AdAuctions.* formalize the Buchbinder–Jain–Naor primal-dual algorithm, which updates a covering variable multiplicatively and has ratio (1−1/c)(1−Rmax⁡)(1-1/c)(1-R_{\max})(1−1/c)(1−Rmax​); they are not reused. Proofs of any milestone, and lemmas carrying the bid-size error through slab boundaries, are welcome.

Selected references

  • A. Mehta, A. Saberi, U. Vazirani, V. Vazirani, AdWords and generalized on-line matching, J. ACM 54(5), 2007. https://doi.org/10.1145/1284320.1284321
  • B. Kalyanasundaram, K. Pruhs, An optimal deterministic algorithm for online b-matching, Theoretical Computer Science 233, 2000. https://doi.org/10.1016/S0304-3975(99)00140-1
  • R. M. Karp, U. V. Vazirani, V. V. Vazirani, An optimal algorithm for on-line bipartite matching, STOC 1990. https://doi.org/10.1145/100216.100262
  • N. Buchbinder, K. Jain, J. Naor, Online primal-dual algorithms for maximizing ad-auctions revenue, ESA 2007. https://doi.org/10.1007/978-3-540-75520-3_24
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AdWords and Generalized On-line Matching II: No Randomized Online Algorithm for b-Matching Has Competitive Ratio Better Than 1 − 1/e, for Every Budget bResearch Paper

Motivation

Search engines sell advertising slots query by query. Each advertiser states a bid per keyword and a daily budget; queries arrive one at a time, and the engine must assign each to an advertiser immediately, without knowing which queries will come later. Mehta, Saberi, Vazirani and Vazirani (J. ACM 2007) called this the adwords problem and gave a deterministic online algorithm whose competitive ratio, the worst-case ratio of its revenue to the best offline revenue, tends to 1−1/e1-1/e1−1/e when bids are small compared to budgets. Section 7 of the same paper shows that this ratio cannot be beaten, even by randomized algorithms and even under the small-bids assumption. That lower bound is the subject of this mission.

Timeline of the special cases:

  • 1990. Karp, Vazirani and Vazirani (STOC 1990) proved that no randomized online algorithm for online bipartite matching (unit bids, unit budgets) has competitive ratio better than 1−1/e1-1/e1−1/e, and that their algorithm RANKING attains it.
  • 2000. Kalyanasundaram and Pruhs (Theoret. Comput. Sci. 2000) studied online b-matching: budgets of bbb units and 0/10/10/1 bids. Their deterministic algorithm BALANCE has competitive ratio tending to 1−1/e1-1/e1−1/e as b→∞b\to\inftyb→∞, and they proved that no deterministic algorithm does better. Whether randomization helps for large bbb was left open (Kalyanasundaram–Pruhs 1998).
  • 2007. Mehta, Saberi, Vazirani and Vazirani (Theorem 9) closed that question: no randomized online algorithm beats 1−1/e1-1/e1−1/e for b-matching, for large bbb.

Setting

An instance of online b-matching has NNN bidders and a sequence of queries t=0,1,…,M−1t = 0,1,\dots,M-1t=0,1,…,M−1. Every bidder has the same integer budget B≥1B\ge1B≥1. Each query ttt comes with the set I(t)I(t)I(t) of bidders that bid 111 on it; the others bid 000.

A deterministic online algorithm aaa processes the queries in order. When query ttt arrives it sees the bid sets I(0),…,I(t)I(0),\dots,I(t)I(0),…,I(t) and nothing later, and it either proposes a bidder or leaves the query unallocated. The proposal succeeds if the bidder bids on the query and has won fewer than BBB queries so far; the bidder then pays 111. The algorithm is not required to be greedy. Its revenue ALGa(I)\mathrm{ALG}_a(I)ALGa​(I) is the number of queries won. A randomized online algorithm AAA is a probability distribution over deterministic online algorithms, fixed before the instance is chosen; its expected revenue is EA[ALG(I)]=∑aA(a) ALGa(I)\mathbb E_A[\mathrm{ALG}(I)]=\sum_a A(a)\,\mathrm{ALG}_a(I)EA​[ALG(I)]=∑a​A(a)ALGa​(I).

An offline allocation τ\tauτ assigns each query to a bidder or to nobody, with full knowledge of III. Its revenue is revB(I,τ)=∑rmin⁡{B, ∣{t:τ(t)=r, r∈I(t)}∣}\mathrm{rev}_B(I,\tau)=\sum_r\min\{B,\ |\{t:\tau(t)=r,\ r\in I(t)\}|\}revB​(I,τ)=∑r​min{B, ∣{t:τ(t)=r, r∈I(t)}∣}: each bidder pays for the queries it bids on, up to its budget.

The permuted round instances of the proof are as follows. For a permutation π\piπ of the bidders, the instance IπI_\piIπ​ consists of NNN rounds Q1,…,QNQ_1,\dots,Q_NQ1​,…,QN​ of BBB queries each, and bidders π(i),π(i+1),…,π(N)\pi(i),\pi(i+1),\dots,\pi(N)π(i),π(i+1),…,π(N) bid on the queries of round QiQ_iQi​. The distribution D\mathcal DD is the uniform distribution over these N!N!N! instances, and Eπ\mathbb E_\piEπ​ denotes the average over it. The paper writes this instance with budget 111, bids ϵ\epsilonϵ and 1/ϵ1/\epsilon1/ϵ queries per round; the Lean development uses the same instance scaled by B=1/ϵB=1/\epsilonB=1/ϵ.

Formalization targets

Goal: Theorem 9

For every δ>0\delta>0δ>0 there is N0N_0N0​ such that for all N≥N0N\ge N_0N≥N0​, all B≥1B\ge1B≥1 and every randomized online algorithm AAA for NNN bidders and NBNBNB queries, there are an instance III and an allocation τ\tauτ with

revB(I,τ)=NBandEA[ALG(I)]≤(1−1e+δ)NB.\mathrm{rev}_B(I,\tau)=NB\qquad\text{and}\qquad \mathbb E_A[\mathrm{ALG}(I)]\le\Big(1-\frac1e+\delta\Big)NB.revB​(I,τ)=NBandEA​[ALG(I)]≤(1−e1​+δ)NB.

The constant 1−1/e1-1/e1−1/e is the paper's. The slack δ\deltaδ is not a weakening of the paper's claim: a competitive ratio better than 1−1/e1-1/e1−1/e would mean a ratio 1−1/e+δ′1-1/e+\delta'1−1/e+δ′ for some δ′>0\delta'>0δ′>0 on every instance. The threshold N0N_0N0​ is independent of the budget, which is how "for large bbb" is rendered.

Milestones (proof of Theorem 9, p. 15)

  1. Yao step. If every deterministic algorithm aaa has Eπ[ALGa(Iπ)]≤V\mathbb E_\pi[\mathrm{ALG}_a(I_\pi)]\le VEπ​[ALGa​(Iπ​)]≤V, then every randomized AAA has some π\piπ with EA[ALG(Iπ)]≤V\mathbb E_A[\mathrm{ALG}(I_\pi)]\le VEA​[ALG(Iπ​)]≤V.
  2. The optimum. revB(Iπ,τπ)=NB\mathrm{rev}_B(I_\pi,\tau_\pi)=NBrevB​(Iπ​,τπ​)=NB for the allocation τπ:Qi↦π(i)\tau_\pi:Q_i\mapsto\pi(i)τπ​:Qi​↦π(i), and no allocation earns more.
  3. The display. For a deterministic aaa, with qij(π)q_{ij}(\pi)qij​(π) the fraction of QiQ_iQi​ won by π(j)\pi(j)π(j),
Eπ[qij]≤1N−i+1 (j≥i),Eπ[qij]=0 (j<i).\mathbb E_\pi[q_{ij}]\le\frac1{N-i+1}\ (j\ge i),\qquad \mathbb E_\pi[q_{ij}]=0\ (j<i).Eπ​[qij​]≤N−i+11​ (j≥i),Eπ​[qij​]=0 (j<i).
  1. Per-bidder bound. Eπ[La(π(j))/B]≤min⁡{1,∑i=1j1N−i+1}\mathbb E_\pi\big[L^a(\pi(j))/B\big]\le\min\{1,\sum_{i=1}^{j}\frac1{N-i+1}\}Eπ​[La(π(j))/B]≤min{1,∑i=1j​N−i+11​}, where La(r)L^a(r)La(r) is the number of queries bidder rrr wins.
  2. Summed bound. ∑j=1Nmin⁡{1,∑i=1j1N−i+1}≤(1−1/e+δ)N\sum_{j=1}^{N}\min\{1,\sum_{i=1}^{j}\frac1{N-i+1}\}\le(1-1/e+\delta)N∑j=1N​min{1,∑i=1j​N−i+11​}≤(1−1/e+δ)N for N≥N0(δ)N\ge N_0(\delta)N≥N0​(δ).
  3. Average revenue. Eπ[ALGa(Iπ)]≤(1−1/e+δ)NB\mathbb E_\pi[\mathrm{ALG}_a(I_\pi)]\le(1-1/e+\delta)NBEπ​[ALGa​(Iπ​)]≤(1−1/e+δ)NB for N≥N0(δ)N\ge N_0(\delta)N≥N0​(δ), every B≥1B\ge1B≥1 and every deterministic aaa.

Significance

The result. Theorem 9 shows that the 1−1/e1-1/e1−1/e ratio attained by BALANCE for large budgets, and by the paper's tradeoff algorithm for adwords with small bids, is optimal among all online algorithms, randomized or not. Since b-matching is a special case of adwords with small bids, the same bound applies to adwords. It also answers the question of Kalyanasundaram and Pruhs on whether randomization helps for b-matching. With B=1B=1B=1 it contains the bipartite matching lower bound of Karp, Vazirani and Vazirani.

Formalizing it. The result has been proved since 2007; to our knowledge it has no machine-checked proof. The b = 1 case is posed on the platform as KVVMatching.UpperBound.theorem_2 (Karp–Vazirani–Vazirani), with columns arriving in reverse index order and an analysis of the algorithm RANDOM; this mission poses the budget-uniform statement in its own model. A formalization yields a reusable model of online algorithms with budgets (histories that hide the future, randomized algorithms as mixtures of deterministic rules) and a formal instance of Yao's principle for online problems.

Difficulty

The bound must hold for every deterministic online algorithm, including ones that are not greedy, waste proposals, or base each decision on the entire revealed history. A tempting argument fixes the algorithm's behaviour per round and treats it as oblivious to earlier rounds; that only covers a subclass. The history of the permuted instance reveals, before round iii, exactly which bidders dropped out in earlier rounds, so the information available to the algorithm grows round by round, and the bound on Eπ[qij]\mathbb E_\pi[q_{ij}]Eπ​[qij​] has to hold conditionally on everything revealed. Budgets interact across rounds: whether a proposal in round iii succeeds depends on wins in earlier rounds. Finally, the printed "at most N(1−1/e)N(1-1/e)N(1−1/e)" is false at every finite NNN: the sum in milestone 5 exceeds N(1−1/e)N(1-1/e)N(1−1/e) by a bounded amount (about 0.3160.3160.316 for large NNN), so the analytic step is genuinely asymptotic.

Formalization scope

  • Representation. Bidders are Fin N and query positions Fin M, both zero-based. An instance is Fin M → Finset (Fin N). A history is Fin M → Option (Finset (Fin N)) with unrevealed entries none. A deterministic algorithm is Fin M → History N M → Option (Fin N), a randomized one is a PMF over deterministic algorithms, and expected revenue is a finite sum.
  • Conventions. Budgets are a common integer BBB and bids are 0/10/10/1; the paper's budget-111, bid-ϵ\epsilonϵ instance is the same instance scaled by B=1/ϵB=1/\epsilonB=1/ϵ. A query in position ttt belongs to round ⌊t/B⌋+1\lfloor t/B\rfloor+1⌊t/B⌋+1. Rounds iii and positions jjj in milestones 3–4 are 1-based, as in the paper. "Bidder jjj" in the proof means the bidder π(j)\pi(j)π(j) in position jjj of the permutation. The j<ij<ij<i case of the display is an equality. The comparator in the goal is an explicit allocation of revenue NBNBNB, which is the maximum possible.
  • Ruled out. The algorithm sees only the revealed history, never III or π\piπ, and the randomized algorithm is chosen before the instance. An algorithm that could see the instance would trivially earn NBNBNB, and choosing the instance first would make the goal the averaging statement of milestone 6, not Theorem 9.
  • Infrastructure. Needed: finite sums over permutations, the exchange of the average over π\piπ and over the algorithm, invariance of a run under permutations that fix the revealed information, and estimates of harmonic sums HN−HN−jH_N-H_{N-j}HN​−HN−j​ against log⁡\loglog. The online-algorithm model and the Yao step are reusable for other online lower bounds. Contributions to any milestone are welcome; milestone 5 is pure real analysis and independent of the model.

Selected references

  • A. Mehta, A. Saberi, U. Vazirani, V. Vazirani, AdWords and generalized on-line matching, J. ACM 54(5), 2007. https://doi.org/10.1145/1284320.1284321
  • R. M. Karp, U. V. Vazirani, V. V. Vazirani, An optimal algorithm for on-line bipartite matching, STOC 1990. https://doi.org/10.1145/100216.100262
  • B. Kalyanasundaram, K. R. Pruhs, An optimal deterministic algorithm for online b-matching, Theoret. Comput. Sci. 233, 2000. https://doi.org/10.1016/S0304-3975(99)00140-1
  • A. C.-C. Yao, Probabilistic computations: toward a unified measure of complexity, FOCS 1977. https://doi.org/10.1109/SFCS.1977.24
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AnalysisProbability·Captain: mikedeng1

Optimal Inapproximability Results for MAX-CUT and Other 2-Variable CSPs? 4: The Correlated Gaussian Orthant Probability Satisfies Λρ(μ) ≤ (1 + ρ)·φ(t)/t·N(t√((1 − ρ)/(1 + ρ)))Research Paper

Motivation

Khot, Kindler, Mossel and O'Donnell, Optimal Inapproximability Results for MAX-CUT and Other 2-Variable CSPs? (SIAM J. Comput. 37(1), 2007), prove that, assuming the Unique Games Conjecture, the Goemans–Williamson approximation ratio for MAX-CUT is optimal, and they extend the method to MAX-q-CUT and to Γ-MAX-2LIN(q). For the q-ary problems the key analytic input is the theorem of Mossel, O'Donnell and Oleszkiewicz (arXiv:math/0503503), the MOO theorem. It bounds the noise stability of a low-influence function with mean µ by a Gaussian quantity, the correlated Gaussian orthant probability Λ_ρ(µ): the probability that two ρ-correlated standard Gaussians both exceed the threshold t at which a single one has tail mass µ.

The hardness bounds of the paper for Γ-MAX-2LIN(q) are stated in terms of Λ_ρ(1/q). They are explicit only after Λ_ρ(µ) is estimated. Proposition 6.1 of the paper gives such an estimate in closed form, by slightly improving a bound from the proof of Lemma 11.1 of de Klerk, Pasechnik and Warners (Approximate graph colouring and MAX-k-CUT algorithms based on the theta function, J. Combin. Optim., 2004). The same quantity at µ = 1/2 is Sheppard's orthant probability (Phil. Trans. R. Soc. A 192, 1899), the source of the arccos formulas used throughout the MAX-CUT part of the paper.

This mission formalizes Proposition 6.1 and the steps of its printed proof.

Setting

Let φ be the standard Gaussian density and N the Gaussian tail probability function:

ϕ(x)=12πe−x2/2,N(x)=∫x∞ϕ(s) ds.\phi(x)=\frac{1}{\sqrt{2\pi}}e^{-x^2/2},\qquad N(x)=\int_x^\infty \phi(s)\,ds .ϕ(x)=2π​1​e−x2/2,N(x)=∫x∞​ϕ(s)ds.

So N(x) = Pr[X ≥ x] for a standard Gaussian X. N is strictly decreasing from 1 to 0, and N(0) = 1/2.

Let X and Y be independent standard Gaussian random variables. For ρ ∈ [0, 1] put

X′=ρX+1−ρ2 Y.X'=\rho X+\sqrt{1-\rho^2}\,Y .X′=ρX+1−ρ2​Y.

Then (X, X′) is a centred normal pair with unit variances and covariance ρ, the pair of Definition 8 of the paper. For 0 < µ < 1 let t be the unique real number with Pr[X ≥ t] = µ, and define

Λρ(μ)=Pr⁡[X≥t and X′≥t].\Lambda_\rho(\mu)=\Pr[X\ge t\ \text{and}\ X'\ge t].Λρ​(μ)=Pr[X≥t and X′≥t].

The threshold t is positive exactly when µ < 1/2. Λ_ρ(µ) is the noise stability, in Gaussian space, of the indicator of a half-line of measure µ.

The proof uses two exponents. For u, v ∈ ℝ, with ρ < 1 and t > 0,

g(u,v)=u+v1+ρ+(u−v)2+2(1−ρ)uv2(1−ρ2)t2,h(u,v)=u+v1+ρ+(u−v)22(1−ρ2)t2.g(u,v)=\frac{u+v}{1+\rho}+\frac{(u-v)^2+2(1-\rho)uv}{2(1-\rho^2)t^2},\qquad h(u,v)=\frac{u+v}{1+\rho}+\frac{(u-v)^2}{2(1-\rho^2)t^2}.g(u,v)=1+ρu+v​+2(1−ρ2)t2(u−v)2+2(1−ρ)uv​,h(u,v)=1+ρu+v​+2(1−ρ2)t2(u−v)2​.

In Lean these are phi, tailN, orthantProb ρ t, Lambda ρ μ, gExp ρ t u v and hExp ρ t u v in the namespace OptInapprox.Orthant.

Formalization targets

Goal: Proposition 6.1 (p. 14)

For any 0 ≤ µ < 1/2, let t > 0 be the number with N(t) = µ. Then for all 0 ≤ ρ ≤ 1,

Λρ(μ) ≤ (1+ρ)⋅ϕ(t)t⋅N ⁣(t1−ρ1+ρ).(4)\Lambda_\rho(\mu)\ \le\ (1+\rho)\cdot\frac{\phi(t)}{t}\cdot N\!\Big(t\sqrt{\tfrac{1-\rho}{1+\rho}}\Big).\tag{4}Λρ​(μ) ≤ (1+ρ)⋅tϕ(t)​⋅N(t1+ρ1−ρ​​).(4)

The endpoint ρ = 1 is part of the goal. There X′ = X, Λ₁(µ) = µ, and (4) becomes the classical Mills-ratio inequality N(t) ≤ φ(t)/t.

Milestones (proof of Proposition 6.1, pp. 30–31)

  1. (18). For 0 ≤ ρ < 1, t > 0 and µ = N(t),
Λρ(μ)=12π1−ρ2⋅t2exp⁡(−t21+ρ)∫0∞ ⁣ ⁣∫0∞e−g(u,v) du dv.\Lambda_\rho(\mu)=\frac{1}{2\pi\sqrt{1-\rho^2}\cdot t^2}\exp\Big(-\frac{t^2}{1+\rho}\Big)\int_0^\infty\!\!\int_0^\infty e^{-g(u,v)}\,du\,dv .Λρ​(μ)=2π1−ρ2​⋅t21​exp(−1+ρt2​)∫0∞​∫0∞​e−g(u,v)dudv.
  1. g ≥ h on u, v ≥ 0.
  2. (19)–(20).
∫0∞ ⁣ ⁣∫0∞e−g≤∫0∞ ⁣ ⁣∫0∞e−h=2π(1+ρ)1−ρ2⋅t⋅exp⁡(1−ρ1+ρ⋅t22)⋅N(t1−ρ1+ρ).\int_0^\infty\!\!\int_0^\infty e^{-g}\le\int_0^\infty\!\!\int_0^\infty e^{-h}=\sqrt{2\pi}(1+\rho)\sqrt{1-\rho^2}\cdot t\cdot\exp\Big(\frac{1-\rho}{1+\rho}\cdot\frac{t^2}{2}\Big)\cdot N\Big(t\sqrt{\tfrac{1-\rho}{1+\rho}}\Big).∫0∞​∫0∞​e−g≤∫0∞​∫0∞​e−h=2π​(1+ρ)1−ρ2​⋅t⋅exp(1+ρ1−ρ​⋅2t2​)⋅N(t1+ρ1−ρ​​).
  1. Lower bound (side note in the proof of Corollary 10, p. 31):
μ⋅N(t1−ρ1+ρ)≤Λρ(μ).\mu\cdot N\Big(t\sqrt{\tfrac{1-\rho}{1+\rho}}\Big)\le\Lambda_\rho(\mu).μ⋅N(t1+ρ1−ρ​​)≤Λρ​(μ).

Significance

Proposition 6.1 makes the MOO theorem quantitative for thresholds. With the lower bound of milestone 4 it determines Λ_ρ(µ) up to the factor 1 + ρ, and up to 1 + o(1) as µ → 0, since φ(t)/t ∼ N(t) as t → ∞ (Corollary 10, part 1). Through Corollary 10 it yields the asymptotics of qΛ_ρ(1/q) used in the paper's hardness results for MAX-q-CUT and Γ-MAX-2LIN(q). These quantities also appear in later work on q-ary noise stability and on the approximability of 2-CSPs.

The proposition is proved in the paper; nothing here is open. Mathlib (at the pinned revision) contains no proof of it, of the bivariate-normal integral representation (18), or of the Mills-ratio inequality N(t) ≤ φ(t)/t. On the platform, Mills' inequality appears only as an open statement in the two-sided form Pr[|X| > z] ≤ √(2/π)·e^{−z²/2}/z (KLTNuclear.Lasso.gaussian_tail), and there is no item for orthant probabilities. A complete development provides:

  • the substitution x = t + u/t, y = t + v/t in the bivariate normal density;
  • a closed-form quadrant integral after the rotation r = u + v, s = u − v;
  • the identification of a probability under a product Gaussian measure with an explicit double integral.

Each of these is reusable for Gaussian tail and orthant estimates.

Difficulty

The inequality itself is elementary once (18) and (20) are available. The work lies in the two integral identities and in their measure-theoretic glue.

For (18), the orthant probability is defined as a measure of a set under the product of two one-dimensional Gaussian laws. Writing it as a double integral of the bivariate density is a linear change of variables with Jacobian √(1 − ρ²). The shift and scaling by t then has Jacobian 1/t², and the quadratic form has to be expanded exactly.

For (20), the region u, v ≥ 0 becomes the wedge |s| ≤ r after the rotation, so the inner integral is a truncated Gaussian integral rather than a full one. The closed form appears only after an integration by parts in r, or an equivalent completion of the square.

The endpoint ρ = 1 is not covered by the printed argument, because (18) divides by √(1 − ρ²). It needs Mills' inequality separately. A proof that only treats ρ < 1 does not close the goal.

Formalization scope

  • Gaussian law. Λ_ρ(µ) is a genuine probability. stdGaussPair is the product of two copies of Mathlib's gaussianReal 0 1 on ℝ × ℝ. orthantProb ρ t is the real-valued measure of {X ≥ t, ρX + √(1 − ρ²)Y ≥ t}, which is the representation the paper itself uses on p. 31.
  • Choice of t. Lambda ρ μ chooses a t with Pr[X ≥ t] = µ, where the probability is taken under gaussianReal 0 1. Such a t is unique, so the choice does not matter. For µ ∉ (0, 1) no such t exists and the value is a placeholder 0 that no statement uses.
  • Hypotheses of the statements. Every theorem takes t > 0 and N(t) = µ as hypotheses, as Proposition 6.1 does; the redundant 0 ≤ µ < 1/2 is kept as printed.
  • Functions. φ is written out explicitly and N is the Bochner integral of φ over (x, ∞).
  • Integrals. The double integrals of (18)–(20) are iterated integrals over (0, ∞), inner variable u, as printed. Milestone 3 also asserts that e^{−h} is integrable on the quadrant, so (19) cannot hold through a junk zero integral.
  • Range of ρ. The goal and milestone 4 take 0 ≤ ρ ≤ 1, as on the page. Milestones 1–3 take 0 ≤ ρ < 1, because their constants divide by √(1 − ρ²) or 1 − ρ², and the printed proof uses them only there. This is the only hypothesis added relative to the page.
  • Trivializing formalizations, ruled out.
    • Defining Λ_ρ(µ) by the right-hand side of (18) would make milestone 1 a tautology and the goal a calculus exercise about a formula unrelated to Gaussians. The definition here is a measure of a set.
    • Allowing t = 0 would put the junk value φ(0)/0 = 0 on the right of (4). The statements require t > 0.

The two remarks printed right after Proposition 6.1 (on Λ_ρ(1/2) and on removing the factor 1 + ρ) are not part of this mission.

Contributions are welcome on all four milestones, on the case ρ = 1 of the goal (Mills' inequality), and on general lemmas: N as Pr[X ≥ x], monotonicity and positivity of N, and the law of (X, ρX + √(1 − ρ²)Y) as a bivariate normal.

Selected references

  • S. Khot, G. Kindler, E. Mossel, R. O'Donnell, Optimal Inapproximability Results for MAX-CUT and Other 2-Variable CSPs?, SIAM J. Comput. 37(1), 2007 (authors' version of February 7, 2007). https://doi.org/10.1137/S0097539705447372
  • E. Mossel, R. O'Donnell, K. Oleszkiewicz, Noise stability of functions with low influences: invariance and optimality, FOCS 2005; Annals of Mathematics 171, 2010. https://arxiv.org/abs/math/0503503
  • E. de Klerk, D. Pasechnik, J. Warners, Approximate graph colouring and MAX-k-CUT algorithms based on the theta function, Journal of Combinatorial Optimization 8, 2004 (Lemma 11.1).
  • W. F. Sheppard, On the application of the theory of error to cases of normal distribution and normal correlation, Phil. Trans. R. Soc. London A 192, 101–168, 1899. https://doi.org/10.1098/rsta.1899.0003
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CombinatoricsGraph TheoryTheoretical Computer Science·Captain: mikedeng1

Spectral Sparsification of Graphs 2: Every Graph with m Edges Has a (6 log_{4/3} 2m)⁻¹-Conductance Decomposition Cutting at Most Half of Its EdgesResearch Paper

Motivation

A sparse graph that approximates a dense one, in the sense that both have nearly the same Laplacian quadratic form, can stand in for it in every algorithm that only reads cuts or solves Laplacian linear systems. Spielman and Teng introduced such spectral sparsifiers and built them in nearly linear time; the construction is the sparsification step of their nearly-linear-time Laplacian solver (arXiv:0808.4134, SIAM J. Comput. 40(4), 2011).

Sampling edges at random works well only inside a graph of high conductance, where no vertex set is separated from the rest by few edges. A general graph is therefore first cut into pieces of high conductance, with few edges running between the pieces. Section 7 of the paper proves that such a decomposition always exists. A similar result was obtained independently by Trevisan (2005). The decomposition theorem, together with the sampling theorem of §6, already shows that every graph has a spectral sparsifier with O(nlog⁡7n)O(n\log^7 n)O(nlog7n) edges; the algorithmic decomposition of §8, which the fast algorithm uses, is an approximate version of it, and its analysis rests on the same certificate lemma.

Setting

Let G=(V,E)G=(V,E)G=(V,E) be a finite simple undirected graph with m=∣E∣m=|E|m=∣E∣ edges, and write did_idi​ for the degree of vertex iii. For disjoint S,T⊆VS,T\subseteq VS,T⊆V, E(S,T)E(S,T)E(S,T) is the set of edges with one end in SSS and one in TTT. The volume of S⊆VS\subseteq VS⊆V is Vol⁡(S)=∑i∈Sdi\operatorname{Vol}(S)=\sum_{i\in S}d_iVol(S)=∑i∈S​di​; in particular Vol⁡(V)=2m\operatorname{Vol}(V)=2mVol(V)=2m.

For a vertex set B⊆VB\subseteq VB⊆V and S⊆BS\subseteq BS⊆B, the conductance of SSS inside BBB is

ΦBG(S)=∣E(S,B−S)∣min⁡(Vol⁡(S),Vol⁡(B−S)),ΦBG(∅)=1,\Phi^G_B(S)=\frac{|E(S,B-S)|}{\min\big(\operatorname{Vol}(S),\operatorname{Vol}(B-S)\big)},\qquad \Phi^G_B(\emptyset)=1,ΦBG​(S)=min(Vol(S),Vol(B−S))∣E(S,B−S)∣​,ΦBG​(∅)=1,

and the conductance of BBB is ΦBG=min⁡S⊂BΦBG(S)\Phi^G_B=\min_{S\subset B}\Phi^G_B(S)ΦBG​=minS⊂B​ΦBG​(S) over proper subsets, with ΦBG=1\Phi^G_B=1ΦBG​=1 when ∣B∣=1|B|=1∣B∣=1. Volumes are always measured with the degrees of GGG, never with the degrees inside the induced subgraph G(B)G(B)G(B); consequently ΦBG\Phi^G_BΦBG​ is at most the usual conductance of G(B)G(B)G(B), and lower bounds on ΦBG\Phi^G_BΦBG​ transfer to it.

A decomposition of GGG is a partition (A1,…,Ak)(A_1,\dots,A_k)(A1​,…,Ak​) of VVV. It is a φ\varphiφ-decomposition if ΦAiG≥φ\Phi^G_{A_i}\ge\varphiΦAi​G​≥φ for all iii, and its boundary is the set of edges between different parts,

∂(A1,…,Ak)=E∩⋃i≠j(Ai×Aj).\partial(A_1,\dots,A_k)=E\cap\bigcup_{i\neq j}(A_i\times A_j).∂(A1​,…,Ak​)=E∩i=j⋃​(Ai​×Aj​).

In Lean: vol G S, cutEdges G S T =∣E(S,T)∣=|E(S,T)|=∣E(S,T)∣, condRel G B S =ΦBG(S)=\Phi^G_B(S)=ΦBG​(S), cond G B =ΦBG=\Phi^G_B=ΦBG​, and decompBoundary G P =∂(A1,…,Ak)=\partial(A_1,\dots,A_k)=∂(A1​,…,Ak​) for a Finpartition P of the vertex set, all in the namespace SpectralSparsify.Decomp.

Formalization targets

Goal: Theorem 7.1 (p. 17)

Every graph GGG without isolated vertices has a decomposition (A1,…,Ak)(A_1,\dots,A_k)(A1​,…,Ak​) with

ΦAiG ≥ (6log⁡4/32m)−1for all i,∣∂(A1,…,Ak)∣ ≤ ∣E∣2.\Phi^G_{A_i}\ \ge\ \big(6\log_{4/3}2m\big)^{-1}\quad\text{for all } i,\qquad |\partial(A_1,\dots,A_k)|\ \le\ \frac{|E|}{2}.ΦAi​G​ ≥ (6log4/3​2m)−1for all i,∣∂(A1​,…,Ak​)∣ ≤ 2∣E∣​.

The constants are the paper's. Both conditions must hold for one and the same partition.

Milestones

  1. (12), first inequality (p. 18): for S⊆BS\subseteq BS⊆B, R⊆B−SR\subseteq B-SR⊆B−S, T=R∪ST=R\cup ST=R∪S, ∣E(T,B−T)∣≤∣E(S,B−S)∣+∣E(R,B−S−R)∣|E(T,B-T)|\le|E(S,B-S)|+|E(R,B-S-R)|∣E(T,B−T)∣≤∣E(S,B−S)∣+∣E(R,B−S−R)∣.
  2. The volume bound proving (13) (p. 19): if Vol⁡(R)≤12Vol⁡(B−S)\operatorname{Vol}(R)\le\frac12\operatorname{Vol}(B-S)Vol(R)≤21​Vol(B−S) and Vol⁡(S)=αVol⁡(B)\operatorname{Vol}(S)=\alpha\operatorname{Vol}(B)Vol(S)=αVol(B), then Vol⁡(R∪S)≤1+α2Vol⁡(B)\operatorname{Vol}(R\cup S)\le\frac{1+\alpha}{2}\operatorname{Vol}(B)Vol(R∪S)≤21+α​Vol(B).
  3. Lemma 7.2, Sparsest Cuts as Certificates (p. 18): let φ≤1\varphi\le1φ≤1, and let S⊂BS\subset BS⊂B maximize Vol⁡(S)\operatorname{Vol}(S)Vol(S) subject to (C.1) Vol⁡(S)≤Vol⁡(B)/2\operatorname{Vol}(S)\le\operatorname{Vol}(B)/2Vol(S)≤Vol(B)/2 and (C.2) ΦBG(S)≤φ\Phi^G_B(S)\le\varphiΦBG​(S)≤φ. If Vol⁡(S)=αVol⁡(B)\operatorname{Vol}(S)=\alpha\operatorname{Vol}(B)Vol(S)=αVol(B) with α≤1/3\alpha\le1/3α≤1/3, then
ΦB−SG ≥ φ 1−3α1−α.\Phi^G_{B-S}\ \ge\ \varphi\,\frac{1-3\alpha}{1-\alpha}.ΦB−SG​ ≥ φ1−α1−3α​.
  1. The φ/3\varphi/3φ/3 step (proof of Theorem 7.1, p. 19): under the hypotheses of Lemma 7.2 with Vol⁡(S)≤Vol⁡(B)/4\operatorname{Vol}(S)\le\operatorname{Vol}(B)/4Vol(S)≤Vol(B)/4, ΦB−SG≥φ/3\Phi^G_{B-S}\ge\varphi/3ΦB−SG​≥φ/3.
  2. The per-level cut bound (proof of Theorem 7.1, p. 19): for pairwise disjoint B1,…,BrB_1,\dots,B_rB1​,…,Br​ and Sj⊂BjS_j\subset B_jSj​⊂Bj​ satisfying (C.1) and (C.2) in BjB_jBj​ with φ≥0\varphi\ge0φ≥0, ∑j∣E(Sj,Bj−Sj)∣≤φ∣E∣\sum_j|E(S_j,B_j-S_j)|\le\varphi|E|∑j​∣E(Sj​,Bj​−Sj​)∣≤φ∣E∣.

Significance

The theorem says that every graph is, after removing at most half of its edges, a disjoint union of pieces of conductance Ω(1/log⁡m)\Omega(1/\log m)Ω(1/logm). By Cheeger's inequality each piece then has normalized spectral gap Ω(1/log⁡2m)\Omega(1/\log^2 m)Ω(1/log2m), which is the hypothesis under which the random sampling of §6 produces a spectral approximation; applying the theorem recursively to the removed edges gives the existence of spectral sparsifiers with O(nlog⁡7n)O(n\log^7 n)O(nlog7n) edges (§7.2). Decompositions of this kind, now called expander decompositions, have become a standard tool in graph algorithms.

The theorem is proved in the paper; to the knowledge of this mission it has no machine-checked proof. What the mission produces is a formal proof of the existence statement with the paper's explicit constant, a formal Lemma 7.2 (the certificate lemma that also drives the approximate version, Theorem 8.1), and reusable Lean definitions of volume, relative conductance ΦBG\Phi^G_BΦBG​ and decomposition boundary for finite simple graphs.

Difficulty

The obvious argument, cutting along any sparse set until no sparse set is left, controls the conductance of the final parts but not the number of edges cut: a long sequence of small sparse cuts can remove far more than half of the edges. The difficulty is to show that one well-chosen cut leaves a remainder whose conductance is certified without further search, which is the content of Lemma 7.2. Its hypothesis is a maximality condition over all subsets of BBB, and its conclusion concerns all subsets of B−SB-SB−S, a different set measured with the same ambient degrees, so the two cannot be compared directly. The existence statement then needs a well-founded description of the recursion, a bound on its depth, and an accounting of the cut edges level by level, all against the explicit constant (6log⁡4/32m)−1(6\log_{4/3}2m)^{-1}(6log4/3​2m)−1.

Formalization scope

Graphs are SimpleGraph V on a finite vertex type with decidable adjacency; vertex sets are Finset V; volumes, conductances and the bound on ∣∂∣|\partial|∣∂∣ are real numbers; decompositions are Finpartition (Finset.univ : Finset V); log⁡4/3\log_{4/3}log4/3​ is Real.logb (4/3).

Hypotheses made explicit:

  • No isolated vertices (∀ v, 0 < G.degree v) in Theorem 7.1, Lemma 7.2 and the milestones that divide by a volume. The paper leaves it implicit: ΦBG(S)\Phi^G_B(S)ΦBG​(S) is 0/00/00/0 for sets of isolated vertices, and with Lean's 0/0=00/0=00/0=0 Lemma 7.2 would be false (one edge plus two isolated vertices is a counterexample). Under the hypothesis m=0m=0m=0 forces V=∅V=\emptysetV=∅, and Theorem 7.1 is then trivially true.
  • BBB nonempty in Lemma 7.2 and the φ/3\varphi/3φ/3 step, so that α=Vol⁡(S)/Vol⁡(B)\alpha=\operatorname{Vol}(S)/\operatorname{Vol}(B)α=Vol(S)/Vol(B) is determined.
  • φ≥0\varphi\ge0φ≥0 in the per-level bound (the paper's φ\varphiφ is positive).

Conventions: ΦBG\Phi^G_BΦBG​ is the minimum over proper subsets, the empty set contributing 111; ΦBG=1\Phi^G_B=1ΦBG​=1 for ∣B∣≤1|B|\le1∣B∣≤1; ∣E(S,T)∣|E(S,T)|∣E(S,T)∣ counts ordered adjacent pairs in S×TS\times TS×T, which is the edge count for disjoint sets. Neither conclusion of Theorem 7.1 may be dropped: the partition into singletons satisfies the conductance bound and the partition into one part satisfies the boundary bound, so a formalization keeping only one conclusion is trivial.

Not formalized: idealDecomp as an object (step 2 involves a choice, so it is a relation rather than a function; the goal is the existence statement), its termination and depth bound as separate items, the λ-spectral decomposition remark via Cheeger's inequality, the existence sketch for sparsifiers in §7.2, and the algorithmic analogue of §8. Contributions welcome: proofs of the milestones, a formal recursion for idealDecomp, and lemmas on volume and edge-boundary arithmetic that other graph-partitioning missions can reuse.

Selected references

  • D. A. Spielman, S.-H. Teng, Spectral Sparsification of Graphs, arXiv:0808.4134v3, 2010; SIAM J. Comput. 40(4), 2011. https://arxiv.org/abs/0808.4134
  • L. Trevisan, Approximation algorithms for unique games, FOCS 2005, pp. 197–205; journal version Theory of Computing 4 (2008) 111–128. https://doi.org/10.4086/toc.2008.v004a005
  • D. A. Spielman, S.-H. Teng, Nearly-linear time algorithms for graph partitioning, graph sparsification, and solving linear systems, STOC 2004, pp. 81–90. https://doi.org/10.1145/1007352.1007372
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Graph TheoryLinear algebraProbability+2·Captain: mikedeng1

Graph Sparsification by Effective Resistances 1: Sampling O(n log n/ε²) Edges by Effective Resistance Yields a (1±ε) Spectral Sparsifier with Probability 1/2Research Paper

Motivation

Many graph algorithms run in time proportional to the number of edges. A sparsifier of a weighted graph GGG is a graph HHH on the same vertices with far fewer edges that approximates GGG for the purpose at hand, so that the algorithm can be run on HHH instead. Benczúr and Karger (1996) showed that every graph has a sparsifier with O(nlog⁡n/ε2)O(n\log n/\varepsilon^2)O(nlogn/ε2) edges preserving the weight of every cut up to a factor 1±ε1\pm\varepsilon1±ε. Spielman and Teng (2004) introduced the stronger spectral notion, in which the Laplacian quadratic form is preserved for every real vector, not only for cut indicators; their sparsifiers had O(nlog⁡cn)O(n\log^c n)O(nlogcn) edges for a large constant ccc and were the first step of their nearly-linear-time solvers for symmetric diagonally dominant linear systems.

Spielman and Srivastava (arXiv:0803.0929, STOC 2008, SIAM J. Comput. 2011) proved that independent sampling of O(nlog⁡n/ε2)O(n\log n/\varepsilon^2)O(nlogn/ε2) edges, each edge with probability proportional to its weight times its effective resistance, yields a spectral sparsifier. The result improved both earlier bounds, replaced a recursive partitioning construction by a one-line sampling rule, and made effective resistance a standard tool in graph algorithms. Batson, Spielman and Srivastava (arXiv:0808.0163) later obtained O(n/ε2)O(n/\varepsilon^2)O(n/ε2) edges deterministically, by a slower method built on the same matrix Π\PiΠ.

Setting

Let G=(V,E,w)G=(V,E,w)G=(V,E,w) be a connected weighted undirected graph with n=∣V∣n=|V|n=∣V∣ vertices, m=∣E∣m=|E|m=∣E∣ edges and weights we>0w_e>0we​>0. Orient every edge arbitrarily, so that it has a head and a tail (distinct vertices).

  • The incidence matrix B∈Rm×nB\in\mathbb R^{m\times n}B∈Rm×n has B(e,v)=1B(e,v)=1B(e,v)=1 if vvv is the head of eee, −1-1−1 if vvv is its tail, and 000 otherwise; beb_ebe​ denotes its row for eee. WWW is the diagonal m×mm\times mm×m matrix with W(e,e)=weW(e,e)=w_eW(e,e)=we​.
  • The Laplacian is L=BTWBL=B^{\mathsf T}WBL=BTWB, with quadratic form xTLx=∑ewe (x(head e)−x(tail e))2x^{\mathsf T}Lx=\sum_e w_e\,(x(\mathrm{head}\,e)-x(\mathrm{tail}\,e))^2xTLx=∑e​we​(x(heade)−x(taile))2.
  • L+L^{+}L+ is the Moore–Penrose pseudoinverse of LLL: if L=∑i=1n−1λiuiuiTL=\sum_{i=1}^{n-1}\lambda_iu_iu_i^{\mathsf T}L=∑i=1n−1​λi​ui​uiT​ over its nonzero eigenvalues, then L+=∑i=1n−1λi−1uiuiTL^{+}=\sum_{i=1}^{n-1}\lambda_i^{-1}u_iu_i^{\mathsf T}L+=∑i=1n−1​λi−1​ui​uiT​.
  • The effective resistance of the edge eee is Re=beL+beTR_e=b_eL^{+}b_e^{\mathsf T}Re​=be​L+beT​: the potential difference across eee when a unit current enters at one end and leaves at the other, the edges being resistors of conductance wew_ewe​.
  • Π=W1/2BL+BTW1/2\Pi=W^{1/2}BL^{+}B^{\mathsf T}W^{1/2}Π=W1/2BL+BTW1/2 is an m×mm\times mm×m matrix with Π(e,e)=weRe\Pi(e,e)=w_eR_eΠ(e,e)=we​Re​.
  • Sparsify(G,q)(G,q)(G,q) draws qqq edges independently with replacement, the edge eee with probability pe=weRe/∑fwfRfp_e=w_eR_e/\sum_f w_fR_fpe​=we​Re​/∑f​wf​Rf​, and gives eee the weight we/(qpe)w_e/(qp_e)we​/(qpe​) for each time it is drawn. Its output HHH has Laplacian L~=BTW1/2SW1/2B\tilde L=B^{\mathsf T}W^{1/2}SW^{1/2}BL~=BTW1/2SW1/2B, where SSS is the random diagonal matrix with S(e,e)=#{draws of e}/(qpe)S(e,e)=\#\{\text{draws of }e\}/(qp_e)S(e,e)=#{draws of e}/(qpe​).

Formalization targets

Goal: Theorem 1

There are an absolute constant CCC and a threshold N0N_0N0​ such that, for every n≥N0n\ge N_0n≥N0​, every connected weighted graph on nnn vertices and every 1/n<ε≤11/\sqrt n<\varepsilon\le11/n​<ε≤1, with q=⌈9C2nlog⁡n/ε2⌉q=\lceil 9C^2n\log n/\varepsilon^2\rceilq=⌈9C2nlogn/ε2⌉, with probability at least 1/21/21/2

∀x∈Rn:(1−ε) xTLx  ≤  xTL~x  ≤  (1+ε) xTLx.\forall x\in\mathbb R^n:\qquad (1-\varepsilon)\,x^{\mathsf T}Lx\;\le\;x^{\mathsf T}\tilde Lx\;\le\;(1+\varepsilon)\,x^{\mathsf T}Lx .∀x∈Rn:(1−ε)xTLx≤xTL~x≤(1+ε)xTLx.

The constant CCC is left unfixed; the statement asserts the shape q=O(nlog⁡n/ε2)q=O(n\log n/\varepsilon^2)q=O(nlogn/ε2) with the paper's explicit dependence on CCC.

Milestones

  1. Lemma 3 (four parts): Π\PiΠ is an orthogonal projection; im⁡Π=im⁡W1/2B\operatorname{im}\Pi=\operatorname{im}W^{1/2}BimΠ=imW1/2B; the eigenvalues of Π\PiΠ are 111 with multiplicity n−1n-1n−1 and 000 with multiplicity m−n+1m-n+1m−n+1; Π(e,e)=∥Π(⋅,e)∥2\Pi(e,e)=\|\Pi(\cdot,e)\|^2Π(e,e)=∥Π(⋅,e)∥2.
  2. Lemma 4: for a nonnegative diagonal SSS, ∥ΠSΠ−ΠΠ∥2≤ε\|\Pi S\Pi-\Pi\Pi\|_2\le\varepsilon∥ΠSΠ−ΠΠ∥2​≤ε implies (1−ε)xTLx≤xTBTW1/2SW1/2Bx≤(1+ε)xTLx(1-\varepsilon)x^{\mathsf T}Lx\le x^{\mathsf T}B^{\mathsf T}W^{1/2}SW^{1/2}Bx\le(1+\varepsilon)x^{\mathsf T}Lx(1−ε)xTLx≤xTBTW1/2SW1/2Bx≤(1+ε)xTLx for all xxx.
  3. Lemma 5 (Rudelson–Vershynin): for independent samples y1,…,yqy_1,\dots,y_qy1​,…,yq​ of a random vector with ∥y∥2≤M\|y\|_2\le M∥y∥2​≤M and ∥E yyT∥2≤1\|\mathbb E\,yy^{\mathsf T}\|_2\le1∥EyyT∥2​≤1, and q≥2q\ge2q≥2,
E∥1q∑j=1qyjyjT−E yyT∥2≤CMlog⁡qqwhenever the right side is <1.\mathbb E\Big\|\frac1q\sum_{j=1}^q y_jy_j^{\mathsf T}-\mathbb E\,yy^{\mathsf T}\Big\|_2\le CM\sqrt{\frac{\log q}{q}}\quad\text{whenever the right side is }<1.E​q1​j=1∑q​yj​yjT​−EyyT​2​≤CMqlogq​​whenever the right side is <1.

Significance

Theorem 1 says that every weighted graph is spectrally approximated by a reweighted subgraph with O(nlog⁡n/ε2)O(n\log n/\varepsilon^2)O(nlogn/ε2) edges. A spectral approximation preserves cut weights, the eigenvalues of the Laplacian up to 1±ε1\pm\varepsilon1±ε, effective resistances, and the condition number of LLL as a preconditioner, so any algorithm whose output depends on these quantities can run on HHH. Combined with fast approximate computation of effective resistances (the second mission of this series), it gives a nearly-linear-time construction, and it is the sampling step used in Laplacian solvers, in sparsification of sums of rank-one matrices, and in leverage-score sampling for regression, where weRew_eR_ewe​Re​ is exactly the statistical leverage of a row.

The result is proved in the paper; to our knowledge no machine-checked proof exists. This mission formalizes the statement and the paper's proof structure: the linear algebra of Π\PiΠ (Lemma 3), the deterministic reduction from quadratic forms to a spectral-norm bound (Lemma 4), and the matrix concentration inequality (Lemma 5), which is the substantive analytic input and is itself a reusable result about sums of independent rank-one matrices.

Difficulty

The deterministic part is linear algebra over the pseudoinverse. The obstacle is concentration: the expected Laplacian of HHH equals LLL, but bounding the deviation uniformly over all x∈Rnx\in\mathbb R^nx∈Rn is a statement about the spectral norm of a random matrix, and a union bound over a net of directions costs a factor of nnn in the sample count rather than log⁡n\log nlogn. Scalar Chernoff bounds per cut, which suffice for cut sparsifiers, do not give the spectral statement. Lemma 5 is the matrix inequality that removes this loss, and no inequality of this kind (a concentration bound for the spectral norm of a sum of independent random matrices) is in Mathlib.

Formalization scope

All declarations sit in the namespace EffResSparsify.Sampling.

  • Graphs. A structure WGraph V E with orientation maps head, tail : E → V, weights w : E → ℝ, and the fields head e ≠ tail e (no loops) and 0 < w e. Parallel edges are allowed; nothing in §3 uses simplicity. Connectivity is a separate hypothesis on the underlying simple graph and includes V≠∅V\ne\emptysetV=∅. In Theorem 1 the vertex type is Fin n; the edge type is an arbitrary finite type.
  • Pseudoinverse. L+L^{+}L+ is the matrix of the published Moore–Penrose pseudoinverse HarmonicGames.Decomposition.pinv of x↦Lxx\mapsto Lxx↦Lx on Euclidean RV\mathbb R^VRV; it equals the spectral formula above and is the gauge-fixed inverse, never "some solution of Lx=yLx=yLx=y".
  • Sampling. pep_epe​ is defined as weRe/∑fwfRfw_eR_e/\sum_f w_fR_fwe​Re​/∑f​wf​Rf​; the identity ∑fwfRf=n−1\sum_f w_fR_f=n-1∑f​wf​Rf​=n−1 is part of the proof. An outcome of Sparsify is a sequence in EqE^qEq with probability ∏ipsi\prod_i p_{s_i}∏i​psi​​, and probabilities and expectations are finite sums over EqE^qEq, with no measure theory.
  • Norms and logarithms. ∥⋅∥2\|\cdot\|_2∥⋅∥2​ is the ℓ2\ell_2ℓ2​ operator norm on matrices (Matrix.Norms.L2Operator); vector norms in Lemma 5 are Euclidean; log⁡\loglog is natural (the base is absorbed into CCC).
  • Constants. In Theorem 1, ∃C>0, ∃N0, ∀n≥N0\exists C>0,\ \exists N_0,\ \forall n\ge N_0∃C>0, ∃N0​, ∀n≥N0​ precede the graph and ε\varepsilonε; the sample count is ⌈9C2nlog⁡n/ε2⌉\lceil 9C^2n\log n/\varepsilon^2\rceil⌈9C2nlogn/ε2⌉, rounded up because the printed value is not an integer. In Lemma 5, ∃C>0\exists C>0∃C>0 precedes the dimension, the distribution, MMM and qqq.
  • Corrected statement. Lemma 5 as printed, with right side min⁡(CMlog⁡q/q,1)\min(CM\sqrt{\log q/q},1)min(CMlogq/q​,1), is false (at q=1q=1q=1 the bound is 000). The formal milestone is Rudelson and Vershynin's own Theorem 3.1: q≥2q\ge2q≥2, and the bound a=CMlog⁡q/qa=CM\sqrt{\log q/q}a=CMlogq/q​ holds when a<1a<1a<1. It is stated for finitely supported distributions, which is all Theorem 1 uses. Theorem 1 applies it with a≤ε/2a\le\varepsilon/2a≤ε/2, so the correction does not affect the goal.
  • Not a trivialization. Theorem 1 does not take Lemma 5, a bound on E∥ΠSΠ−Π∥2\mathbb E\|\Pi S\Pi-\Pi\|_2E∥ΠSΠ−Π∥2​, or a free sample count as a hypothesis; a statement with any of these, or with "∃q\exists q∃q" in place of ⌈9C2nlog⁡n/ε2⌉\lceil 9C^2n\log n/\varepsilon^2\rceil⌈9C2nlogn/ε2⌉, is a different theorem.

Reusable beyond this mission: the weighted Laplacian with its pseudoinverse and effective resistances, and Lemma 5, which applies to any sampling scheme for sums of rank-one matrices (leverage-score sampling, column subset selection). Contributions toward a matrix Chernoff or Rudelson-type inequality in Mathlib are welcome.

Selected references

  • D. A. Spielman, N. Srivastava, Graph Sparsification by Effective Resistances, arXiv:0803.0929v4, 2009; SIAM J. Comput. 40(6), 2011. https://arxiv.org/abs/0803.0929, https://doi.org/10.1137/080734029
  • M. Rudelson, R. Vershynin, Sampling from large matrices: an approach through geometric functional analysis, J. ACM 54(4), 2007. https://doi.org/10.1145/1255443.1255449
  • M. Rudelson, Random vectors in the isotropic position, J. Funct. Anal. 164(1), 1999. https://doi.org/10.1006/jfan.1998.3384
  • A. A. Benczúr, D. R. Karger, Approximating s-t minimum cuts in Õ(n²) time, STOC 1996. https://doi.org/10.1145/237814.237827
  • D. A. Spielman, S.-H. Teng, Spectral sparsification of graphs, SIAM J. Comput. 40(4), 2011 (arXiv:0808.4134). https://arxiv.org/abs/0808.4134
  • J. Batson, D. A. Spielman, N. Srivastava, Twice-Ramanujan sparsifiers, SIAM J. Comput. 41(6), 2012 (arXiv:0808.0163). https://arxiv.org/abs/0808.0163
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Quantum InformationTheoretical Computer Science·Captain: mikedeng1

Search via Quantum Walk 1: Recursive Amplitude Amplification with Approximate Reflections R(βᵢ), βᵢ = 18γ/(4π³i²), Finds a Marked Element with Probability at Least 1/12 − 3γResearch Paper

Motivation

Grover's algorithm finds a marked element among NNN with O(N)O(\sqrt N)O(N​) queries by alternating two reflections: one about the initial state and one that flips the sign of marked states. In quantum-walk search, the initial state ∣π⟩|\pi\rangle∣π⟩ encodes the stationary distribution of a Markov chain, and the reflection about ∣π⟩|\pi\rangle∣π⟩ is too expensive to implement exactly. Magniez, Nayak, Roland and Santha (arXiv:quant-ph/0608026, SIAM J. Comput. 2011) obtain the reflection approximately, by phase estimation on the quantum walk, and need a search procedure that tolerates the approximation error without paying extra cost to reduce it. Their Section 4 supplies one: a variant of the recursive amplitude amplification (RAA) of Høyer, Mosca and de Wolf (ICALP 2003) in which the reflection about ∣π⟩|\pi\rangle∣π⟩ is replaced, at recursion level iii, by an approximate circuit of precision βi=184π3γ/i2\beta_i=\frac{18}{4\pi^3}\gamma/i^2βi​=4π318​γ/i2. The two lemmas of that section, stated "in full generality for potential further applications" (p. 11), are the exact engine of the paper's headline Theorem 3 (search with cost S+1ε(1δU+C)S+\frac1{\sqrt\varepsilon}(\frac1{\sqrt\delta}U+C)S+ε​1​(δ​1​U+C)).

Timeline: Grover (1996) gives quadratic speedup for unstructured search; Brassard, Høyer, Mosca and Tapp (2002) generalize it to amplitude amplification; Høyer, Mosca and de Wolf (2003) introduce RAA to tolerate a bounded-error marking reflection; Szegedy (2004) defines quantum walks for arbitrary reversible chains with detection guarantees; Magniez, Nayak, Roland and Santha (STOC 2007, SIAM 2011) adapt RAA to an approximate initial-state reflection and obtain search, not only detection, for every reversible ergodic chain.

Setting

Let XXX be a finite set and M⊆XM\subseteq XM⊆X a set of marked elements. The state space is H=CX×X\mathcal H=\mathbb C^{X\times X}H=CX×X. The initial state ∣π⟩∈H|\pi\rangle\in\mathcal H∣π⟩∈H is any unit vector (Lemmas 1 and 2 never use its quantum-walk form), and the marked weight is pM=∥ΠM∣π⟩∥2p_M=\|\Pi_M|\pi\rangle\|^2pM​=∥ΠM​∣π⟩∥2, where ΠM\Pi_MΠM​ projects onto the basis states ∣x⟩∣y⟩|x\rangle|y\rangle∣x⟩∣y⟩ with x∈Mx\in Mx∈M.

For each level i≥1i\ge1i≥1 an extra register KiK_iKi​ (a finite-dimensional space with a basis state ∣0⟩|0\rangle∣0⟩) is given together with a unitary RiR_iRi​ on H⊗Ki\mathcal H\otimes K_iH⊗Ki​, playing the role of R(βi)R(\beta_i)R(βi​):

Ri∣π⟩∣0⟩=∣π⟩∣0⟩,∥(Ri+Id)∣ψ⟩∣0⟩∥≤βi∥ψ∥  whenever ⟨π∣ψ⟩=0.R_i|\pi\rangle|0\rangle=|\pi\rangle|0\rangle,\qquad \|(R_i+\mathrm{Id})|\psi\rangle|0\rangle\|\le\beta_i\|\psi\|\ \text{ whenever }\langle\pi|\psi\rangle=0 .Ri​∣π⟩∣0⟩=∣π⟩∣0⟩,∥(Ri​+Id)∣ψ⟩∣0⟩∥≤βi​∥ψ∥  whenever ⟨π∣ψ⟩=0.

On H⊗K1⊗⋯⊗KT\mathcal H\otimes K_1\otimes\cdots\otimes K_TH⊗K1​⊗⋯⊗KT​ the marked subspace M~\tilde{\mathcal M}M~ consists of states whose first register is marked, and ref(M~⊥)=Id−2ΠM~\mathrm{ref}(\tilde{\mathcal M}^\perp)=\mathrm{Id}-2\Pi_{\tilde M}ref(M~⊥)=Id−2ΠM~​.

Approximate RAA(i,γ)(i,\gamma)(i,γ) is the unitary AiA_iAi​ with A0=IdA_0=\mathrm{Id}A0​=Id and

Ai=Ai−1⋅Oi⋅Ai−1†⋅ref(M~⊥)⋅Ai−1,A_i=A_{i-1}\cdot O_i\cdot A_{i-1}^\dagger\cdot\mathrm{ref}(\tilde{\mathcal M}^\perp)\cdot A_{i-1},Ai​=Ai−1​⋅Oi​⋅Ai−1†​⋅ref(M~⊥)⋅Ai−1​,

where OiO_iOi​ multiplies by −1-1−1 every basis state in which some register KjK_jKj​, j<ij<ij<i, is not ∣0⟩|0\rangle∣0⟩, and otherwise applies RiR_iRi​ to H⊗Ki\mathcal H\otimes K_iH⊗Ki​. Write ∣φi⟩=Ai∣π⟩∣0S⟩|\varphi_i\rangle=A_i|\pi\rangle|0^S\rangle∣φi​⟩=Ai​∣π⟩∣0S⟩ and sin⁡ϕi=∥ΠM~∣φi⟩∥\sin\phi_i=\|\Pi_{\tilde M}|\varphi_i\rangle\|sinϕi​=∥ΠM~​∣φi​⟩∥.

Tolerant RAA(tmax⁡,γ)(t_{\max},\gamma)(tmax​,γ) first samples xxx (succeeding with probability pMp_MpM​); otherwise, for i=1,…,tmax⁡i=1,\dots,t_{\max}i=1,…,tmax​, it applies AiA_iAi​ to the state left over from the previous failed measurement, ∣ψi⟩=Ai∣νi−1⊥⟩|\psi_i\rangle=A_i|\nu^\perp_{i-1}\rangle∣ψi​⟩=Ai​∣νi−1⊥​⟩ with ∣ν0⊥⟩=∣π⟩∣0S⟩|\nu^\perp_0\rangle=|\pi\rangle|0^S\rangle∣ν0⊥​⟩=∣π⟩∣0S⟩, and measures {ΠM~,Id−ΠM~}\{\Pi_{\tilde M},\mathrm{Id}-\Pi_{\tilde M}\}{ΠM~​,Id−ΠM~​}; a failure collapses the state to ∣νi⊥⟩=ΠM~⊥∣ψi⟩/∥ΠM~⊥∣ψi⟩∥|\nu_i^\perp\rangle=\Pi_{\tilde M^\perp}|\psi_i\rangle/\|\Pi_{\tilde M^\perp}|\psi_i\rangle\|∣νi⊥​⟩=ΠM~⊥​∣ψi​⟩/∥ΠM~⊥​∣ψi​⟩∥.

Formalization targets

Goal: Lemma 2 (p. 15)

Let 0<γ≤1/400<\gamma\le1/400<γ≤1/40, let ε>0\varepsilon>0ε>0 satisfy pM≥εp_M\ge\varepsilonpM​≥ε whenever pM>0p_M>0pM​>0, and let tmax⁡t_{\max}tmax​ be the smallest non-negative integer with 3tmax⁡sin⁡−1ε∈[π/4,3π/4]3^{t_{\max}}\sin^{-1}\sqrt\varepsilon\in[\pi/4,3\pi/4]3tmax​sin−1ε​∈[π/4,3π/4]. The probability PsuccP_{\rm succ}Psucc​ that Tolerant RAA(tmax⁡,γ)(t_{\max},\gamma)(tmax​,γ) ends with a marked element satisfies

M=∅⇒Psucc=0,pM>0⇒Psucc≥112−3γ.M=\emptyset\Rightarrow P_{\rm succ}=0,\qquad p_M>0\Rightarrow P_{\rm succ}\ge\frac1{12}-3\gamma .M=∅⇒Psucc​=0,pM​>0⇒Psucc​≥121​−3γ.

Lemma 1 (p. 12)

With ttt the smallest non-negative integer such that 3tsin⁡−1pM∈[π/4,3π/4]3^t\sin^{-1}\sqrt{p_M}\in[\pi/4,3\pi/4]3tsin−1pM​​∈[π/4,3π/4], for every γ>0\gamma>0γ>0,

∥ΠM~At∣π⟩∣0S⟩∥≥12−γ.\|\Pi_{\tilde M}A_t|\pi\rangle|0^S\rangle\|\ge\frac1{\sqrt2}-\gamma .∥ΠM~​At​∣π⟩∣0S⟩∥≥2​1​−γ.

Milestones

In the order of the proofs: Fact 1 (the error operator Ei=Ai−1OiAi−1†−ref(φi−1)E_i=A_{i-1}O_iA_{i-1}^\dagger-\mathrm{ref}(\varphi_{i-1})Ei​=Ai−1​Oi​Ai−1†​−ref(φi−1​) kills ∣φi−1⟩|\varphi_{i-1}\rangle∣φi−1​⟩ and has norm ≤βi\le\beta_i≤βi​ on states with clean registers K≥iK_{\ge i}K≥i​); the one-level bound ∣sin⁡ϕi+1−sin⁡3ϕi∣≤βi+1∣sin⁡2ϕi∣|\sin\phi_{i+1}-\sin3\phi_i|\le\beta_{i+1}|\sin2\phi_i|∣sinϕi+1​−sin3ϕi​∣≤βi+1​∣sin2ϕi​∣; the two trigonometric inequalities on [0,π/4][0,\pi/4][0,π/4]; the surrogate bound e~i≤γϕˉi/π≤γ\tilde e_i\le\gamma\bar\phi_i/\pi\le\gammae~i​≤γϕˉ​i​/π≤γ; Lemma 1; the three terms of the drift recursion (5); and the accumulated drift δt=∥∣ψt⟩−∣φt⟩∥≤π/8+9γ/8\delta_t=\||\psi_t\rangle-|\varphi_t\rangle\|\le\pi/8+9\gamma/8δt​=∥∣ψt​⟩−∣φt​⟩∥≤π/8+9γ/8.

Significance

Lemma 2 turns any family of approximate reflections whose error decays like 1/i21/i^21/i2 into a search procedure that succeeds with constant probability, needs only a lower bound ε\varepsilonε on pMp_MpM​, and costs O(3tmax⁡)=O(1/ε)O(3^{t_{\max}})=O(1/\sqrt\varepsilon)O(3tmax​)=O(1/ε​) calls. Combined with the phase-estimation reflection of the paper's Theorem 6 it yields Theorem 3, the general quantum-walk search theorem that has become the standard tool for walk-based algorithms (element distinctness, triangle finding, group commutativity). Nothing in the lemma refers to Markov chains, so it applies to any setting with an approximate reflection about the initial state.

The results are proved in the paper. None of them is machine-checked: the platform holds a formal Grover search with one marked basis state and exact reflections, but no amplitude amplification with approximate or recursive reflections. A formal proof would also settle the steps the paper passes over quickly, notably that the trigonometric inequalities, claimed for angles in [0,π/4][0,\pi/4][0,π/4], are applied to the actual angles ϕi\phi_iϕi​, which may exceed π/4\pi/4π/4 by O(γ)O(\gamma)O(γ) at the last level.

Difficulty

The ideal analysis (every reflection exact, angle tripled at each level) is a two-dimensional rotation argument. With approximate reflections the state leaves the plane spanned by ∣μ0⟩|\mu_0\rangle∣μ0​⟩ and ∣μ0⊥⟩|\mu_0^\perp\rangle∣μ0⊥​⟩, and each level both triples the error already present and injects a new one; the errors stay bounded only because ∑iβi\sum_i\beta_i∑i​βi​ converges and the injection at level iii is weighted by sin⁡2ϕi\sin2\phi_isin2ϕi​. Fact 1 is not a restatement of the hypothesis on R(β)R(\beta)R(β): it holds only because step 4 flips the phase of states whose earlier registers are dirty, and because Ai−1A_{i-1}Ai−1​ never touches K≥iK_{\ge i}K≥i​. In Lemma 2 the attempts reuse the leftover state, not a fresh ∣π⟩∣0S⟩|\pi\rangle|0^S\rangle∣π⟩∣0S⟩, so the state at the decisive attempt ttt has drifted; bounding the drift needs the normalised unmarked parts ∣μk⊥⟩|\mu_k^\perp\rangle∣μk⊥​⟩ to move little from level to level, which again depends on the error bounds of Lemma 1.

Formalization scope

  • H⊗K1⊗⋯⊗KT\mathcal H\otimes K_1\otimes\cdots\otimes K_TH⊗K1​⊗⋯⊗KT​ is EuclideanSpace ℂ (X × X × ((j : Fin T) → κ (j+1))); operators are complex matrices. Registers are 0-based in Lean (index jjj is Kj+1K_{j+1}Kj+1​).
  • RiR_iRi​ is required only at the precisions βi\beta_iβi​ actually used, which is weaker than the paper's "for any β>0\beta>0β>0". Property 3 is stated in the homogeneous form ≤βi∥ψ∥\le\beta_i\|\psi\|≤βi​∥ψ∥.
  • "Undo" is the conjugate transpose. ttt and tmax⁡t_{\max}tmax​ are explicit naturals with "satisfies the condition and no smaller one does". sin⁡−1\sin^{-1}sin−1 is Real.arcsin; the interval is closed.
  • The success probability of Tolerant RAA is defined from the measurement rule, pM+(1−pM)(1−∏i=1tmax⁡(1−∥ΠM~∣ψi⟩∥2))p_M+(1-p_M)\big(1-\prod_{i=1}^{t_{\max}}(1-\|\Pi_{\tilde M}|\psi_i\rangle\|^2)\big)pM​+(1−pM​)(1−∏i=1tmax​​(1−∥ΠM~​∣ψi​⟩∥2)), with post-measurement states computed from the actual ∣ψi⟩|\psi_i\rangle∣ψi​⟩; registers are not reset. The classical sample succeeds with probability ∥ΠM∣π⟩∥2\|\Pi_M|\pi\rangle\|^2∥ΠM​∣π⟩∥2, which is ∑x∈Mπx\sum_{x\in M}\pi_x∑x∈M​πx​ in the paper's walk setting.
  • "MMM non-empty" in Lemma 2 is read as pM>0p_M>0pM​>0, as in the paper's proof. Edge-case hypotheses: ∥π∥=1\|\pi\|=1∥π∥=1; ϕi≤π/3\phi_i\le\pi/3ϕi​≤π/3 in the one-level bound (so sin⁡3ϕi≥0\sin3\phi_i\ge0sin3ϕi​≥0); pM<1p_M<1pM​<1 in the last drift term; 1≤i<t1\le i<t1≤i<t and T≥tT\ge tT≥t in the drift bounds.
  • Cost is not formalized: property 1 of R(β)R(\beta)R(β), the cost c2c_2c2​ of −ref(M)-\mathrm{ref}(M)−ref(M) and every "incurs a cost of order" clause are out of scope. The data-structure subscript ddd is omitted, as in the paper's own error analysis.
  • A formalization in which step 4 applies an exact reflection about ∣π⟩|\pi\rangle∣π⟩ or ∣φi−1⟩|\varphi_{i-1}\rangle∣φi−1​⟩, or in which the success probability is computed from ideal angles instead of the actual states, would make the lemmas statements about exact RAA; the definitions apply the given RiR_iRi​ and measure the actual states.

Contributions welcome: proofs of the trigonometric milestones and of e~i≤γϕˉi/π\tilde e_i\le\gamma\bar\phi_i/\pie~i​≤γϕˉ​i​/π (pure real analysis), Fact 1 (finite-dimensional linear algebra with a block structure on registers), and the vector inequality ∥u/∥u∥−v/∥v∥∥≤2∥u−v∥/∥v∥\|u/\|u\|-v/\|v\|\|\le2\|u-v\|/\|v\|∥u/∥u∥−v/∥v∥∥≤2∥u−v∥/∥v∥ that the drift bounds share. The register and controlled-unitary infrastructure is reusable for other recursive quantum algorithms.

Selected references

  • F. Magniez, A. Nayak, J. Roland, M. Santha, Search via Quantum Walk, SIAM J. Comput. 40(1), 2011; arXiv:quant-ph/0608026v4. https://arxiv.org/abs/quant-ph/0608026
  • P. Høyer, M. Mosca, R. de Wolf, Quantum search on bounded-error inputs, ICALP 2003. https://arxiv.org/abs/quant-ph/0304052
  • G. Brassard, P. Høyer, M. Mosca, A. Tapp, Quantum amplitude amplification and estimation, Contemp. Math. 305, 2002. https://arxiv.org/abs/quant-ph/0005055
  • L. K. Grover, A fast quantum mechanical algorithm for database search, STOC 1996. https://arxiv.org/abs/quant-ph/9605043
  • M. Szegedy, Quantum speed-up of Markov chain based algorithms, FOCS 2004. https://doi.org/10.1109/FOCS.2004.53
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Stochastic Machine Scheduling with Precedence Constraints 2: LP-Based Graham List Scheduling Is a (2 − 1/m + max{1, (m − 1)Δ/m})-Approximation for P|in-forest|E[Σ w_j C_j]Research Paper

Motivation

Scheduling jobs whose durations are uncertain is the normal situation in project management, manufacturing and computing: a job's processing time becomes known only when the job finishes, but a distribution for it is available in advance. Stochastic machine scheduling models this by random, independent processing times PjP_jPj​ and asks for a scheduling policy, a rule that decides online which jobs to start, using only the information observed so far, that minimizes the expected total weighted completion time E[∑jwjCj]\mathrm E[\sum_j w_jC_j]E[∑j​wj​Cj​]. Optimal policies are known only in a few special cases, and they can depend on the full conditional distributions of the remaining processing times, so the research focus has been on simple policies with provable performance guarantees.

Skutella and Uetz (SIAM J. Comput. 34(4), 2005) gave the first constant-factor guarantees for stochastic parallel-machine scheduling with precedence constraints. Their policies are list scheduling policies whose priority list comes from an optimal solution of a linear program built on the load inequalities of Möhring, Schulz and Uetz (J. ACM 46(6), 1999). This mission formalizes their second main result: for in-forest precedence constraints and no release dates, plain Graham list scheduling in LP order is a (2−1m+max⁡{1,m−1mΔ})(2-\tfrac1m+\max\{1,\tfrac{m-1}{m}\Delta\})(2−m1​+max{1,mm−1​Δ})-approximation.

Timeline.

  • 1966/1969: Graham shows list scheduling is a (2−1/m)(2-1/m)(2−1/m)-approximation for the makespan with precedence constraints, for any list.
  • 1999: Möhring, Schulz and Uetz prove the load inequalities for nonanticipatory policies and obtain constant guarantees for P ∣ rj ∣ E[∑wjCj]P\,|\,r_j\,|\,\mathrm E[\sum w_jC_j]P∣rj​∣E[∑wj​Cj​] without precedence constraints.
  • 2001: Chekuri, Motwani, Natarajan and Stein give, among other results, a 2-approximation for deterministic in-tree scheduling by list scheduling (their Lemma 4.16 contains the deterministic counterpart of Lemma 4.3 below).
  • 2005: Skutella and Uetz extend these ideas to stochastic processing times with precedence constraints (Theorem 4.1, general precedence; Theorem 4.5, in-forests).

Setting

There are a finite set VVV of jobs, m≥1m\ge1m≥1 identical parallel machines, and nonnegative weights wjw_jwj​. Jobs are processed nonpreemptively; each machine handles one job at a time. Precedence constraints form an acyclic digraph (V,A)(V,A)(V,A): an arc (i,j)(i,j)(i,j) means jjj starts only after iii completes. The constraints form an in-forest if each job has at most one successor. There are no release dates.

The processing times Pj≥0P_j\ge0Pj​≥0 are independent random variables. A realization is a vector ppp; a schedule assigns start times SjS_jSj​, with completion times Cj=Sj+pjC_j=S_j+p_jCj​=Sj​+pj​; it is feasible if it respects precedence and at most mmm jobs are in process at any time. A policy Π\PiΠ maps each realization to a feasible schedule, and it is nonanticipatory if what it has started by time ttt depends only on what has been observed by ttt (the processing times of completed jobs and which jobs are still running).

With μj=E[Pj]\mu_j=\mathrm E[P_j]μj​=E[Pj​] and Δ≥0\Delta\ge0Δ≥0 a common bound with Var⁡[Pj]≤Δμj2\operatorname{Var}[P_j]\le\Delta\mu_j^2Var[Pj​]≤Δμj2​ (i.e. CV[Pj]≤Δ\mathrm{CV}[P_j]\le\sqrt\DeltaCV[Pj​]≤Δ​), define

f(W)=12m((∑j∈Wμj)2+∑j∈Wμj2)−(m−1)(Δ−1)2m∑j∈Wμj2.f(W)=\frac1{2m}\Big(\Big(\sum_{j\in W}\mu_j\Big)^2+\sum_{j\in W}\mu_j^2\Big)-\frac{(m-1)(\Delta-1)}{2m}\sum_{j\in W}\mu_j^2 .f(W)=2m1​((j∈W∑​μj​)2+j∈W∑​μj2​)−2m(m−1)(Δ−1)​j∈W∑​μj2​.

The LP-relaxation minimizes ∑jwjCjLP\sum_jw_jC^{\mathrm{LP}}_j∑j​wj​CjLP​ subject to ∑j∈WμjCjLP≥f(W)\sum_{j\in W}\mu_jC^{\mathrm{LP}}_j\ge f(W)∑j∈W​μj​CjLP​≥f(W) for all W⊆VW\subseteq VW⊆V, CjLP≥CiLP+μjC^{\mathrm{LP}}_j\ge C^{\mathrm{LP}}_i+\mu_jCjLP​≥CiLP​+μj​ for arcs (i,j)(i,j)(i,j), and CjLP≥μjC^{\mathrm{LP}}_j\ge\mu_jCjLP​≥μj​. A priority list LLL sorts the jobs by nondecreasing CjLPC^{\mathrm{LP}}_jCjLP​; BjB_jBj​ is the set of jobs up to and including jjj in LLL, and AjA_jAj​ the jobs after jjj.

Graham's list scheduling starts, at every decision time, as many available jobs as possible in the order of LLL. For a schedule, a critical predecessor of jjj is a predecessor that completes last among jjj's predecessors, at a positive time; following critical predecessors backwards gives the critical chain of jjj, whose total processing time is ℓj(p)\ell_j(p)ℓj​(p).

Formalization targets

Goal: Theorem 4.5

For every feasible nonanticipatory policy Π\PiΠ,

E[∑jwjCjGraham(P)] ≤ (2−1m+max⁡{1,m−1mΔ}) E[∑jwjCjΠ(P)].\mathrm E\Big[\sum_jw_jC^{\mathrm{Graham}}_j(P)\Big]\ \le\ \Big(2-\frac1m+\max\Big\{1,\frac{m-1}m\Delta\Big\}\Big)\,\mathrm E\Big[\sum_jw_jC^\Pi_j(P)\Big].E[j∑​wj​CjGraham​(P)] ≤ (2−m1​+max{1,mm−1​Δ})E[j∑​wj​CjΠ​(P)].

Milestones

  • Lemma 4.3: in Graham's schedule for an in-forest, no job of AjA_jAj​ is processed during [rj(p),Sj(p)[[r_j(p),S_j(p)[[rj​(p),Sj​(p)[.
  • Lemma 4.4: E[Cj(P)]≤m−1mE[ℓj(P)]+1m∑i∈BjE[Pi]\mathrm E[C_j(P)]\le\frac{m-1}m\mathrm E[\ell_j(P)]+\frac1m\sum_{i\in B_j}\mathrm E[P_i]E[Cj​(P)]≤mm−1​E[ℓj​(P)]+m1​∑i∈Bj​​E[Pi​], together with its per-realization form.
  • Theorem 3.1: the load inequalities ∑j∈WE[Pj]E[CjΠ(P)]≥f(W)\sum_{j\in W}\mathrm E[P_j]\mathrm E[C^\Pi_j(P)]\ge f(W)∑j∈W​E[Pj​]E[CjΠ​(P)]≥f(W) for every nonanticipatory Π\PiΠ.
  • §3 LP-relaxation: the expected completion times of any policy are LP-feasible.
  • Lemma 3.3: 1m∑k∈Bjμk≤(1+max⁡{1,m−1mΔ})CjLP\frac1m\sum_{k\in B_j}\mu_k\le(1+\max\{1,\frac{m-1}m\Delta\})C^{\mathrm{LP}}_jm1​∑k∈Bj​​μk​≤(1+max{1,mm−1​Δ})CjLP​.
  • Critical-chain lower bound (§4, p. 798): ℓj(p)≤Cj(p)\ell_j(p)\le C_j(p)ℓj​(p)≤Cj​(p) in every feasible schedule.

Significance

The theorem gives a constant performance guarantee for stochastic in-forest scheduling, uniform in the distributions once their coefficients of variation are bounded. For NBUE distributions (exponential, uniform, Erlang, …), where Δ=1\Delta=1Δ=1, the guarantee is 3−1/m3-1/m3−1/m, compared with 3+223+2\sqrt23+22​ for general precedence constraints and release dates with Algorithm CMNS (Table 1, p. 792). The analysis shows that for in-forests, deliberate idle time is unnecessary: Lemma 4.3 replaces it.

The result is proved in the paper, partly by reference: Theorem 3.1 and Lemma 3.3 are cited from Möhring, Schulz and Uetz. To our knowledge none of these results has a machine-checked proof. A complete formalization requires the load inequalities of stochastic scheduling, which are of independent use for every LP-based stochastic scheduling result, and a reusable treatment of list schedules, critical chains and nonanticipatory policies.

Difficulty

Two parts carry the weight. The first is the load inequalities (Theorem 3.1): they hold for nonanticipatory policies only, because a policy's start time of job jjj must be independent of PjP_jPj​; turning the informal "dynamic view" of policies into a statement that yields this independence, and then the variance bookkeeping, is the probabilistic core. The second is Lemma 4.3: the naive argument "a waiting job of high priority blocks lower-priority jobs" fails for general precedence constraints, where Graham's algorithm can be arbitrarily bad; the in-forest structure is used through a counting argument at time rj(p)r_j(p)rj​(p), in which the critical predecessors of the jobs started at that time must be distinct.

Formalization scope

Lean represents jobs by a Fintype V, precedence by a relation A : V → V → Prop with acyclic transitive closure, and in-forests by "at most one outgoing arc". Schedules are start-time vectors in ℝ, with machine capacity by counting jobs in process on half-open intervals. Policies are maps from realizations to start times with an explicit nonanticipation condition. Graham's list scheduling is characterized by rules (feasibility, greedy, list order, decision times); critical chains are taken for every admissible tie-breaking selector. The CV bound includes E[Pj2]<∞\mathrm E[P_j^2]<\inftyE[Pj2​]<∞ and E[Pj]>0\mathrm E[P_j]>0E[Pj​]>0. Zero processing times are allowed.

Standing assumptions and disclosed additions: processing times are independent and nonnegative; the comparator policies have integrable completion times; the completion times and critical-chain lengths of Graham's schedule are assumed almost-everywhere measurable (the paper asserts measurability in §5 without proof); "α\alphaα-approximation" is stated against every comparator policy rather than an optimal one.

A trivializing formalization is ruled out: the comparator ranges over every feasible nonanticipatory policy with integrable completion times, CLPC^{\mathrm{LP}}CLP is optimal over all load inequalities W⊆VW\subseteq VW⊆V, and the Graham family must satisfy the rules for every nonnegative realization.

Welcome contributions: the load inequalities, existence and measurability of Graham schedules, and general lemmas on list schedules.

Selected references

  • M. Skutella and M. Uetz, Stochastic machine scheduling with precedence constraints, SIAM J. Comput. 34(4) (2005) 788–802. https://doi.org/10.1137/S0097539702415007
  • R. H. Möhring, A. S. Schulz and M. Uetz, Approximation in stochastic scheduling: the power of LP-based priority policies, J. ACM 46(6) (1999) 924–942. https://doi.org/10.1145/331524.331530
  • C. Chekuri, R. Motwani, B. Natarajan and C. Stein, Approximation techniques for average completion time scheduling, SIAM J. Comput. 31(1) (2001) 146–166. https://doi.org/10.1137/S0097539797327180
  • R. L. Graham, Bounds on multiprocessing timing anomalies, SIAM J. Appl. Math. 17(2) (1969) 416–429. https://doi.org/10.1137/0117039
  • R. H. Möhring, F. J. Radermacher and G. Weiss, Stochastic scheduling problems I: General strategies, Z. Oper. Res. 28 (1984) 193–260. https://doi.org/10.1007/BF01919323
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Primal and Dual Linear Decision Rules in Stochastic and Robust Optimization 2: With Random Recourse, the SDP (3.14) Conservatively Approximates the Linear Decision Rule Problem, Exactly for l = 1Research Paper

Linear decision rules for stochastic programs with random recourse

In a one-stage stochastic program a decision maker observes a random outcome ξ\xiξ and then picks a decision x(ξ)x(\xi)x(ξ), subject to constraints that depend on ξ\xiξ, so as to minimize expected cost. The optimization variable is a whole function xxx, and computing the optimal value is #P-hard even for a uniform distribution on the unit cube (Dyer and Stougie, 2006, cited in the paper as [16, Theorem 3.2]). A standard tractable approximation, introduced for robust optimization by Ben-Tal, Goryashko, Guslitzer and Nemirovski (2004) and carried to stochastic programming by Shapiro–Nemirovski and Chen–Sim–Sun, restricts decisions to linear decision rules x(ξ)=Xξx(\xi)=X\xix(ξ)=Xξ. This restriction gives an upper bound on the optimal value.

Kuhn, Wiesemann and Georghiou (2009/2011) study these approximations systematically. Their §3 treats the case where the constraint matrix itself depends on ξ\xiξ (random recourse). Linear decisions then produce constraints that are quadratic in ξ\xiξ, and the paper reformulates the resulting semi-infinite problem as a semidefinite program. This mission formalizes that reformulation, the primal half of the paper's Theorem 2.

Setting

Uncertainty is a probability measure P\mathbb PP on Rk\mathbb R^kRk, with outcomes ξ\xiξ. The support Ξ\XiΞ of P\mathbb PP is the smallest closed set of probability one. It is assumed to have the form

Ξ={ξ∈Rk: e1⊤ξ=1,  ξ⊤Wℓξ≥0, ℓ=1,…,l}(3.11)\Xi=\{\xi\in\mathbb R^k:\ e_1^\top\xi=1,\ \ \xi^\top W_\ell\xi\ge0,\ \ell=1,\dots,l\}\qquad(3.11)Ξ={ξ∈Rk: e1⊤​ξ=1,  ξ⊤Wℓ​ξ≥0, ℓ=1,…,l}(3.11)

for symmetric matrices W1,…,WlW_1,\dots,W_lW1​,…,Wl​, where e1e_1e1​ is the first standard basis vector. The first coordinate of every outcome is therefore 111, so linear functions of ξ\xiξ are affine functions of the remaining coordinates. Ξ\XiΞ is assumed nonempty and bounded, and its linear hull is assumed to be Rk\mathbb R^kRk. Let S\mathbb SS denote the symmetric k×kk\times kk×k matrices and M=E(ξξ⊤)M=\mathbb E(\xi\xi^\top)M=E(ξξ⊤) the second-moment matrix.

The data are C∈Rn×kC\in\mathbb R^{n\times k}C∈Rn×k (cost c(ξ)=Cξc(\xi)=C\xic(ξ)=Cξ), B∈Rm×kB\in\mathbb R^{m\times k}B∈Rm×k (right-hand side b(ξ)=Bξb(\xi)=B\xib(ξ)=Bξ, with rows bμ⊤b_\mu^\topbμ⊤​), and A1,…,Am∈Rk×nA_1,\dots,A_m\in\mathbb R^{k\times n}A1​,…,Am​∈Rk×n, where the μ\muμth row of the recourse matrix A(ξ)A(\xi)A(ξ) is ξ⊤Aμ\xi^\top A_\muξ⊤Aμ​. The stochastic program SP\mathcal{SP}SP minimizes E(c(ξ)⊤x(ξ))\mathbb E(c(\xi)^\top x(\xi))E(c(ξ)⊤x(ξ)) over square-integrable xxx subject to A(ξ)x(ξ)≤b(ξ)A(\xi)x(\xi)\le b(\xi)A(ξ)x(ξ)≤b(ξ) almost surely. It is strictly feasible if some square-integrable xˉ,sˉ\bar x,\bar sxˉ,sˉ and some ε>0\varepsilon>0ε>0 satisfy A(ξ)xˉ(ξ)+sˉ(ξ)=b(ξ)A(\xi)\bar x(\xi)+\bar s(\xi)=b(\xi)A(ξ)xˉ(ξ)+sˉ(ξ)=b(ξ) and sˉ(ξ)≥εe\bar s(\xi)\ge\varepsilon esˉ(ξ)≥εe almost surely.

With linear decisions XξX\xiXξ and quadratic slacks ξ⊤Sμξ\xi^\top S_\mu\xiξ⊤Sμ​ξ, Sμ∈SS_\mu\in\mathbb SSμ​∈S, one obtains the primal approximation

SPu:min⁡ Tr⁡(MC⊤X)  s.t.  ξ⊤AμXξ+ξ⊤Sμξ=bμ⊤ξ,  ξ⊤Sμξ≥0  P-a.s., μ=1,…,m,\mathcal{SP}^u:\quad \min\ \operatorname{Tr}(MC^\top X)\ \ \text{s.t.}\ \ \xi^\top A_\mu X\xi+\xi^\top S_\mu\xi=b_\mu^\top\xi,\ \ \xi^\top S_\mu\xi\ge0\ \ \mathbb P\text{-a.s.},\ \mu=1,\dots,m,SPu:min Tr(MC⊤X)  s.t.  ξ⊤Aμ​Xξ+ξ⊤Sμ​ξ=bμ⊤​ξ,  ξ⊤Sμ​ξ≥0  P-a.s., μ=1,…,m,

and the SDP (3.14)

min⁡ Tr⁡(MC⊤X)  s.t.  12(AμX+X⊤Aμ⊤)+Sμ=12(e1bμ⊤+bμe1⊤),  Sμ−∑ℓΛμℓWℓ⪰0,  Λ≥0.\min\ \operatorname{Tr}(MC^\top X)\ \ \text{s.t.}\ \ \tfrac12(A_\mu X+X^\top A_\mu^\top)+S_\mu=\tfrac12(e_1b_\mu^\top+b_\mu e_1^\top),\ \ S_\mu-\textstyle\sum_\ell\Lambda_{\mu\ell}W_\ell\succeq0,\ \ \Lambda\ge0 .min Tr(MC⊤X)  s.t.  21​(Aμ​X+X⊤Aμ⊤​)+Sμ​=21​(e1​bμ⊤​+bμ​e1⊤​),  Sμ​−∑ℓ​Λμℓ​Wℓ​⪰0,  Λ≥0.

Formalization targets

Goal: Theorem 2, primal half (p. 17)

Feas⁡(3.14) projects into Feas⁡SPu,val⁡SPu≤val⁡(3.14),\operatorname{Feas}(3.14)\ \text{projects into}\ \operatorname{Feas}\mathcal{SP}^u,\qquad \operatorname{val}\mathcal{SP}^u\le\operatorname{val}(3.14),Feas(3.14) projects into FeasSPu,valSPu≤val(3.14), l=1 and SP strictly feasible ⟹ val⁡SPu=val⁡(3.14).l=1\ \text{and}\ \mathcal{SP}\ \text{strictly feasible}\ \Longrightarrow\ \operatorname{val}\mathcal{SP}^u=\operatorname{val}(3.14).l=1 and SP strictly feasible ⟹ valSPu=val(3.14).

Milestones

  1. §3.2, (3.13), p. 12. The μ\muμth equality constraint of SPu\mathcal{SP}^uSPu holds almost surely if and only if Hμ:=12(AμX+X⊤Aμ⊤−e1bμ⊤−bμe1⊤)+Sμ=0H_\mu:=\tfrac12(A_\mu X+X^\top A_\mu^\top-e_1b_\mu^\top-b_\mu e_1^\top)+S_\mu=0Hμ​:=21​(Aμ​X+X⊤Aμ⊤​−e1​bμ⊤​−bμ​e1⊤​)+Sμ​=0.
  2. Lemma 1 (S-lemma), p. 12. If ξˉ⊤Wξˉ>0\bar\xi^\top W\bar\xi>0ξˉ​⊤Wξˉ​>0 for some ξˉ\bar\xiξˉ​, then [ξ⊤Wξ≥0⇒ξ⊤Sξ≥0]  ⟺  ∃λ≥0: S⪰λW[\xi^\top W\xi\ge0\Rightarrow\xi^\top S\xi\ge0]\iff\exists\lambda\ge0:\ S\succeq\lambda W[ξ⊤Wξ≥0⇒ξ⊤Sξ≥0]⟺∃λ≥0: S⪰λW. This is linked to the platform's proved S-procedure, of which it is the homogeneous case.
  3. Proposition 6, p. 12. For symmetric SSS: ∃λ≥0\exists\lambda\ge0∃λ≥0 with S−∑ℓλℓWℓ⪰0S-\sum_\ell\lambda_\ell W_\ell\succeq0S−∑ℓ​λℓ​Wℓ​⪰0 implies ξ⊤Sξ≥0\xi^\top S\xi\ge0ξ⊤Sξ≥0 almost surely, and the converse holds when l=1l=1l=1.

Significance

The theorem replaces a problem with infinitely many constraints, one per outcome, by a semidefinite program with O(mk2+ml)O(mk^2+ml)O(mk2+ml) variables. Its value is always an upper bound on SPu\mathcal{SP}^uSPu, and hence on SP\mathcal{SP}SP. When the support is a single ellipsoid in the hyperplane e1⊤ξ=1e_1^\top\xi=1e1⊤​ξ=1 (l=1l=1l=1), the bound loses nothing beyond the restriction to linear decisions. For l>1l>1l>1 the gap is unavoidable in general: an exact tractable reformulation would decide copositivity, which is NP-hard (Remark 7). Random recourse arises whenever technology or yield coefficients are uncertain, for example in production planning and portfolio problems with uncertain returns.

The result is proved in the paper. As far as is known it has no machine-checked proof. A formalization adds a precise statement of the hypotheses. Writing those hypotheses out showed that the unnumbered §3.2 step needs Ξ\XiΞ to have dimension k−1k-1k−1, which spanning alone does not give for nonconvex Ξ\XiΞ (see Formalization scope). The other half of Theorem 2, about the lower-bounding SDP (3.18), is false in this preprint and is not part of the mission.

Difficulty

The semi-infinite constraints hold only P\mathbb PP-almost surely. The first step is to pass from "almost surely" to "for every ξ∈Ξ\xi\in\Xiξ∈Ξ", which uses that Ξ\XiΞ is exactly the support and that the constraint functions are continuous. A bound P(Ξ)=1\mathbb P(\Xi)=1P(Ξ)=1 alone is not enough. For the equality constraints, a quadratic form that vanishes on Ξ\XiΞ must vanish identically. This requires Ξ\XiΞ to be large enough, and the obvious argument from "Ξ\XiΞ spans Rk\mathbb R^kRk" fails when Ξ\XiΞ is a finite set. For the inequality constraints with l=1l=1l=1, the implication ξ⊤W1ξ≥0⇒ξ⊤Sξ≥0\xi^\top W_1\xi\ge0\Rightarrow\xi^\top S\xi\ge0ξ⊤W1​ξ≥0⇒ξ⊤Sξ≥0 must be established on all of Rk\mathbb R^kRk and not only on the slice e1⊤ξ=1e_1^\top\xi=1e1⊤​ξ=1. Doing so needs boundedness of Ξ\XiΞ (no recession directions) and a strictly feasible point for the S-lemma. The S-lemma itself is a nonconvex duality statement. It is available on the platform.

Formalization scope

Outcomes live in Fin k → ℝ, with k≥1k\ge1k≥1 carried in the setting. Indices are 0-based: ξ1\xi_1ξ1​ is coordinate 0, and μ,ℓ\mu,\ellμ,ℓ range over Fin m, Fin l. "Ξ\XiΞ is the support of P\mathbb PP" is stated as: Ξ\XiΞ is closed, P(Ξc)=0\mathbb P(\Xi^{\mathrm c})=0P(Ξc)=0, and every ball centred in Ξ\XiΞ has positive measure. Mathlib has no Measure.support at this revision. The standing assumptions (probability measure, symmetric WℓW_\ellWℓ​, support, nonempty, bounded, spanning) form one predicate assumed by every theorem. Decision rules are Borel measurable square-integrable functions. Optimal values are infima in EReal, +∞+\infty+∞ for an empty feasible set and −∞-\infty−∞ for an unbounded one. "Equivalent" means equal optimal values. Each SμS_\muSμ​ is required symmetric in both problems; ⪰\succeq⪰ is positive semidefiniteness and Λ≥0\Lambda\ge0Λ≥0 is componentwise. Strict feasibility of SP\mathcal{SP}SP in §3 is the paper's condition (2.9) of §2 with AAA replaced by A(ξ)A(\xi)A(ξ). The paper uses the phrase without restating it.

Repairs and narrowings:

  • Only the clauses of Theorem 2 about (3.14) and SPu\mathcal{SP}^uSPu are stated. The clauses about (3.18) and SPl\mathcal{SP}^lSPl are false in this preprint: a strictly feasible instance with l=1l=1l=1 has val⁡(3.18)≈1.170>ln⁡3=val⁡SP\operatorname{val}(3.18)\approx1.170>\ln3=\operatorname{val}\mathcal{SP}val(3.18)≈1.170>ln3=valSP. Propositions 7–9 serve only that half and are not included. "Polynomial size, efficiently solvable" is informal and omitted.
  • The §3.2 milestone carries the extra hypothesis that Ξ\XiΞ contains a relatively open piece of the hyperplane e1⊤ξ=1e_1^\top\xi=1e1⊤​ξ=1 (the paper's "dimension k−1k-1k−1", p. 10). Without it the claim is false for l≥2l\ge2l≥2. For l=1l=1l=1 the hypothesis follows from the standing assumptions, so the goal is unaffected.
  • Strict feasibility is kept in the l=1l=1l=1 clause as printed, although the argument does not use it.

The goal cannot be trivialized through its definitions. Feasibility is quantified P\mathbb PP-almost surely for a measure whose support is Ξ\XiΞ, not over an empty or arbitrary set. Both optimal values are infima of the same real objective over the problems' own feasible sets. The standing assumptions are satisfiable, for instance by k=2k=2k=2, W1=diag⁡(1,−1)W_1=\operatorname{diag}(1,-1)W1​=diag(1,−1), and P\mathbb PP the uniform law on {1}×[−1,1]\{1\}\times[-1,1]{1}×[−1,1].

The definitions (support of a measure, L2\mathcal L^2L2 decision rules, the random-recourse data) are reusable for the other sections of the paper and for related work on decision rules. Proofs of any milestone, Lean lemmas on quadratic forms vanishing on open cones, and an almost-sure-to-support transfer lemma are welcome.

Selected references

  • D. Kuhn, W. Wiesemann, A. Georghiou, Primal and dual linear decision rules in stochastic and robust optimization, Optimization Online 2009/02/2218 (2009); Math. Program. 130 (2011) 177–209. https://optimization-online.org/wp-content/uploads/2009/02/2218.pdf, https://doi.org/10.1007/s10107-009-0331-4
  • A. Ben-Tal, A. Goryashko, E. Guslitzer, A. Nemirovski, Adjustable robust solutions of uncertain linear programs, Math. Program. 99 (2004) 351–376. https://doi.org/10.1007/s10107-003-0454-y
  • S. Boyd, L. El Ghaoui, E. Feron, V. Balakrishnan, Linear Matrix Inequalities in System and Control Theory, SIAM Studies in Applied Mathematics 15, 1994 (the paper's source for Lemma 1). https://doi.org/10.1137/1.9781611970777
  • S. Boyd, L. Vandenberghe, Convex Optimization, Cambridge University Press, 2004, Appendix B (the S-procedure as stated on the platform). https://web.stanford.edu/~boyd/cvxbook/
  • I. Pólik, T. Terlaky, A survey of the S-lemma, SIAM Review 49 (2007) 371–418. https://doi.org/10.1137/S003614450444614X
  • M. Dyer, L. Stougie, Computational complexity of stochastic programming problems, Math. Program. 106 (2006) 423–432. https://doi.org/10.1007/s10107-005-0597-0
7 thms2 active usersReviewed
Linear algebraMarkov Chain·Captain: mikedeng1

Search via Quantum Walk 3: For an Irreducible Chain with Positive Self-Loops the Discriminant diag(π)^{1/2}·P·diag(π)^{−1/2} Has Exactly One Singular Value Equal to 1Research Paper

Motivation

Quantum walks give quadratic speed-ups for a class of search problems that classical algorithms solve by running a Markov chain until it hits a marked state. Ambainis's element-distinctness algorithm (Ambainis 2007) and Szegedy's quantization of reversible Markov chains (Szegedy 2004) are the two starting points. Magniez, Nayak, Roland and Santha (arXiv:quant-ph/0608026v4, SIAM J. Comput. 2011) combined them into one search algorithm whose cost is governed by the eigenvalue gap of a reversible chain PPP.

For a non-reversible chain the relevant spectral quantity is not the eigenvalue gap of PPP. It is the singular value gap of a related matrix, the discriminant D(P)D(P)D(P). In §5 the paper observes that its search algorithm and the proof of its main theorem carry over to non-reversible chains once the eigenvalue gap of PPP is replaced by the singular value gap of D(P)D(P)D(P). Positivity of that gap therefore decides whether the algorithm can be used at all. The paper also notes that irreducibility, and even ergodicity, does not guarantee a positive gap. Its Proposition 3 (p. 17, proved in the appendix on pp. 20–21) gives a simple sufficient condition: every state has a positive probability of staying where it is. This mission formalizes that proposition.

Setting

Let XXX be a finite set of states. A Markov chain on XXX is a real matrix P=(pxy)x,y∈XP=(p_{xy})_{x,y\in X}P=(pxy​)x,y∈X​ with nonnegative entries whose rows sum to one; pxyp_{xy}pxy​ is the probability of moving from xxx to yyy. The graph underlying PPP has an edge x→yx\to yx→y whenever pxy>0p_{xy}>0pxy​>0. The chain is irreducible if this graph is strongly connected, so that every state can be reached from every other state.

A stationary distribution of PPP is a vector π=(πx)x∈X\pi=(\pi_x)_{x\in X}π=(πx​)x∈X​ with

πx>0,∑xπx=1,∑xπxpxy=πy(y∈X).\pi_x>0,\qquad \sum_x \pi_x=1,\qquad \sum_x \pi_x p_{xy}=\pi_y\quad(y\in X).πx​>0,x∑​πx​=1,x∑​πx​pxy​=πy​(y∈X).

Every irreducible chain has exactly one.

The discriminant of PPP is the matrix

D(P)=diag⁡(π)1/2⋅P⋅diag⁡(π)−1/2,D(P)xy=πx pxyπy,D(P)=\operatorname{diag}(\pi)^{1/2}\cdot P\cdot \operatorname{diag}(\pi)^{-1/2},\qquad D(P)_{xy}=\frac{\sqrt{\pi_x}\,p_{xy}}{\sqrt{\pi_y}},D(P)=diag(π)1/2⋅P⋅diag(π)−1/2,D(P)xy​=πy​​πx​​pxy​​,

viewed as an operator on CX\mathbb C^XCX with the inner product ⟨u,w⟩=∑xux‾wx\langle u,w\rangle=\sum_x\overline{u_x}w_x⟨u,w⟩=∑x​ux​​wx​. Its singular values σ0≥σ1≥⋯≥σ∣X∣−1≥0\sigma_0\ge\sigma_1\ge\dots\ge\sigma_{|X|-1}\ge 0σ0​≥σ1​≥⋯≥σ∣X∣−1​≥0 are the square roots of the eigenvalues of D(P)†D(P)D(P)^\dagger D(P)D(P)†D(P), repeated according to multiplicity. The vector v=(πx)x∈Xv=(\sqrt{\pi_x})_{x\in X}v=(πx​​)x∈X​ satisfies D(P)v=vD(P)v=vD(P)v=v and vTD(P)=vTv^{\mathsf T}D(P)=v^{\mathsf T}vTD(P)=vT, so 111 is always a singular value of D(P)D(P)D(P). When PPP is reversible, D(P)D(P)D(P) is symmetric and its singular values are the absolute values of the eigenvalues of PPP. In general the two can differ.

Formalization targets

Goal: Proposition 3

If PPP is an irreducible Markov chain on a finite state space XXX with pxx>0p_{xx}>0pxx​>0 for every xxx, then D(P)D(P)D(P) has exactly one singular value equal to 111:

#{ i<∣X∣: σi(D(P))=1 }=1.\#\{\,i<|X|:\ \sigma_i(D(P))=1\,\}=1 .#{i<∣X∣: σi​(D(P))=1}=1.

Together with the bound below, this says that 1=σ0>σ11=\sigma_0>\sigma_11=σ0​>σ1​, i.e. the singular value gap 1−σ11-\sigma_11−σ1​ is positive. The goal asserts no explicit lower bound on the gap, so it does not depend on any quantitative estimate.

Milestones, in the order the proof uses them

  1. Eq. (9). For unit vectors u,v∈CXu,v\in\mathbb C^Xu,v∈CX,
∣u†D(P)v∣≤(∑x,y∣ux∣2pxy)1/2(∑x,y∣vy∣2πxπypxy)1/2≤1.|u^\dagger D(P)v|\le\Bigl(\sum_{x,y}|u_x|^2p_{xy}\Bigr)^{1/2}\Bigl(\sum_{x,y}|v_y|^2\tfrac{\pi_x}{\pi_y}p_{xy}\Bigr)^{1/2}\le 1 .∣u†D(P)v∣≤(x,y∑​∣ux​∣2pxy​)1/2(x,y∑​∣vy​∣2πy​πx​​pxy​)1/2≤1.
  1. Lemma 3. Every singular value of D(P)D(P)D(P) lies in [0,1][0,1][0,1].
  2. §5, p. 17. v=(πx)v=(\sqrt{\pi_x})v=(πx​​) is a left and right eigenvector of D(P)D(P)D(P) with eigenvalue 111.
  3. Equality case. If u,wu,wu,w are unit vectors with u†D(P)w=1u^\dagger D(P)w=1u†D(P)w=1, then ux=wyπx/πyu_x=w_y\sqrt{\pi_x/\pi_y}ux​=wy​πx​/πy​​ whenever pxy>0p_{xy}>0pxy​>0.
  4. Path chaining. If uy=uxπy/πxu_y=u_x\sqrt{\pi_y/\pi_x}uy​=ux​πy​/πx​​ along every edge x→yx\to yx→y and PPP is irreducible, then uy=ux1πy/πx1u_y=u_{x_1}\sqrt{\pi_y/\pi_{x_1}}uy​=ux1​​πy​/πx1​​​ for all x1,yx_1,yx1​,y.

Significance

The result. Proposition 3 is what makes the search algorithm of the paper usable with non-reversible chains. Theorem 8 of the paper bounds the cost of finding a marked element in terms of the singular value gap of D(P)D(P)D(P), and it needs that gap to be positive. The hypothesis pxx>0p_{xx}>0pxx​>0 costs little: replacing PPP by αI+(1−α)P\alpha I+(1-\alpha)PαI+(1−α)P for any α∈(0,1)\alpha\in(0,1)α∈(0,1) makes every self-loop positive and keeps the stationary distribution. The proposition also connects to the classical study of non-reversible chains: the squared singular values of D(P)D(P)D(P) are the eigenvalues of the multiplicative reversiblization PP∗PP^*PP∗, which Fill (1991) used to bound convergence to stationarity.

Formalizing it. The proposition and its proof are in the paper and are not in dispute. To our knowledge neither is machine-checked anywhere. The work is a formal proof of the known argument. It exercises Mathlib's recently added singular values of linear maps between finite-dimensional inner product spaces and its theory of irreducible nonnegative matrices, in a setting where the matrix is neither symmetric nor normal.

Difficulty

The obvious route goes through eigenvalues. Irreducibility plus self-loops make PPP aperiodic, so by Perron–Frobenius the eigenvalue 111 of PPP is simple and every other eigenvalue has modulus less than 111. This does not settle the question. The singular values of a non-normal matrix are not the moduli of its eigenvalues, and the paper points out ergodic chains whose discriminant has zero singular value gap even though their eigenvalue gap is positive. Simplicity of the eigenvalue 111 of PPP therefore says nothing about the multiplicity of the singular value 111 of D(P)D(P)D(P).

The real content is the equality case of a Cauchy–Schwarz inequality in CX×X\mathbb C^{X\times X}CX×X. It has to be translated into an edge-by-edge relation between the coordinates of the left and right singular vectors, then propagated along directed paths of the chain's graph. The self-loops are what identify the left and right singular vectors with each other. Bookkeeping that is routine on paper costs effort here: passing between the eigenvalue sequence of D(P)†D(P)D(P)^\dagger D(P)D(P)†D(P) and the dimension of its 111-eigenspace, and between paths in Mathlib's quiver of positive entries and chains of equalities.

Formalization scope

  • States and chain. The state space is a Fintype with decidable equality. PPP is a real matrix in Matrix.rowStochastic ℝ X, and irreducibility is Mathlib's Matrix.IsIrreducible (nonnegative entries and a strongly connected quiver with an edge x→yx\to yx→y iff pxy>0p_{xy}>0pxy​>0). For a row-stochastic matrix this agrees with "every state is reachable from every other state".
  • Stationary distribution. It enters as data π\piπ with the three properties above. Positivity is explicit because diag⁡(π)−1/2\operatorname{diag}(\pi)^{-1/2}diag(π)−1/2 needs it. Existence and uniqueness (Perron–Frobenius) are neither needed nor stated.
  • Discriminant. D(P)D(P)D(P) is the complex matrix with entries πxpxy/πy\sqrt{\pi_x}p_{xy}/\sqrt{\pi_y}πx​​pxy​/πy​​, acting on EuclideanSpace ℂ X. Its singular values are Mathlib's LinearMap.singularValues, a sequence indexed by N\mathbb NN that is 000 beyond ∣X∣|X|∣X∣. The goal counts the indices i<∣X∣i<|X|i<∣X∣ with σi=1\sigma_i=1σi​=1. The inner product u†D(P)wu^\dagger D(P)wu†D(P)w is Mathlib's inner ℂ u (D(P) w). Since the equality-case milestone assumes this equals 111 exactly, no phase ambiguity remains.
  • What is not assumed. Reversibility of PPP is not assumed. Neither is aperiodicity, primitivity, or a "lazy" bound pxx≥1/2p_{xx}\ge 1/2pxx​≥1/2: the hypothesis is exactly pxx>0p_{xx}>0pxx​>0 for every xxx.
  • Ruled-out trivializations. "111 is a singular value of D(P)D(P)D(P)" holds for every chain and is not the goal. The goal is that this singular value has multiplicity one. A conclusion such as "some singular value is <1<1<1" would also be too weak.
  • Cost. The paper's search algorithm and its cost bounds (Theorem 8) are out of scope. This mission is purely linear-algebraic.
  • Welcome contributions. Proofs of the milestones. The path-chaining milestone is a reusable fact about functions that are multiplicative along the edges of a strongly connected quiver. A general lemma relating the multiplicity of a singular value to the dimension of an eigenspace of T†TT^\dagger TT†T would be useful well beyond this mission.

Selected references

  • F. Magniez, A. Nayak, J. Roland, M. Santha, Search via Quantum Walk, SIAM J. Comput. 40(1):142–164, 2011; arXiv:quant-ph/0608026v4. https://arxiv.org/abs/quant-ph/0608026 (DOI 10.1137/090745854)
  • M. Szegedy, Quantum speed-up of Markov chain based algorithms, Proc. 45th IEEE FOCS, 32–41, 2004. https://doi.org/10.1109/FOCS.2004.53
  • A. Ambainis, Quantum walk algorithm for element distinctness, SIAM J. Comput. 37(1):210–239, 2007; arXiv:quant-ph/0311001. https://arxiv.org/abs/quant-ph/0311001
  • J. A. Fill, Eigenvalue bounds on convergence to stationarity for nonreversible Markov chains, with an application to the exclusion process, Ann. Appl. Probab. 1(1):62–87, 1991. https://doi.org/10.1214/aoap/1177005981
7 thms2 active usersReviewed
Machine LearningProbabilityRandom Matrix Theory+1·Captain: mikedeng1

Nuclear-Norm Penalization and Optimal Rates for Noisy Low-Rank Matrix Completion 3: Uniform Matrix Completion with |Yᵢ| ≤ η — With Probability ≥ 1 − e^{−t} the Oracle Bound (3.5) Holds for All AResearch Paper

Motivation

Matrix completion asks to recover a large matrix from a small number of its entries. It is the abstraction behind collaborative filtering (recommender systems in which a users × items rating matrix is observed on a sparse set of pairs), sensor localization from partial distance information, and system identification. Without structure the problem is hopeless; the standard structural assumption is that the unknown matrix has low rank, and the standard convex surrogate for rank is the nuclear norm, the sum of singular values.

In the noiseless case, exact recovery by nuclear-norm minimization from about r(m1∨m2) polylogr(m_1\vee m_2)\,\mathrm{polylog}r(m1​∨m2​)polylog uniformly sampled entries was established by Candès and Recht (2009) and refined by Candès and Tao (2010) and Gross (2011). With noisy observations the relevant question is a rate: how fast does an estimator's error decrease with the number nnn of observed entries? Koltchinskii, Lounici and Tsybakov (arXiv:1011.6256, Ann. Statist. 2011) introduced a nuclear-norm penalized estimator that uses the known sampling distribution, showed that in matrix completion it is an explicit soft thresholding of the singular values of a rescaled data matrix, and proved for it sharp oracle inequalities (leading constant 1) whose rates are optimal up to logarithmic factors. This mission formalizes the version of that result for bounded responses: Theorem 4 of the paper, together with the probabilistic lemma and the matrix Bernstein inequality it rests on.

Setting

Fix positive integers n,m1,m2n, m_1, m_2n,m1​,m2​ and write Rm1×m2\mathbb R^{m_1\times m_2}Rm1​×m2​ for the real m1×m2m_1\times m_2m1​×m2​ matrices, with scalar product ⟨A,B⟩=tr⁡(A⊤B)\langle A,B\rangle=\operatorname{tr}(A^\top B)⟨A,B⟩=tr(A⊤B), Frobenius norm ∥A∥2\|A\|_2∥A∥2​, nuclear norm ∥A∥1\|A\|_1∥A∥1​ (sum of singular values) and operator norm ∥A∥∞\|A\|_\infty∥A∥∞​ (largest singular value). Set m=m1+m2m=m_1+m_2m=m1​+m2​ and write m1∧m2=min⁡(m1,m2)m_1\wedge m_2=\min(m_1,m_2)m1​∧m2​=min(m1​,m2​).

The matrix completion basis is

X={ej(m1)ek⊤(m2):1≤j≤m1, 1≤k≤m2},\mathcal X=\{e_j(m_1)e_k^\top(m_2):1\le j\le m_1,\ 1\le k\le m_2\},X={ej​(m1​)ek⊤​(m2​):1≤j≤m1​, 1≤k≤m2​},

where ek(m)e_k(m)ek​(m) are the canonical basis vectors of Rm\mathbb R^mRm. One observes nnn independent random pairs (Xi,Yi)(X_i,Y_i)(Xi​,Yi​), where XiX_iXi​ is uniformly distributed on X\mathcal XX and YiY_iYi​ is real, following the trace regression model

E(Yi∣Xi)=tr⁡(Xi⊤A0),\mathbb E(Y_i\mid X_i)=\operatorname{tr}(X_i^\top A_0),E(Yi​∣Xi​)=tr(Xi⊤​A0​),

for an unknown A0∈Rm1×m2A_0\in\mathbb R^{m_1\times m_2}A0​∈Rm1​×m2​. Thus YiY_iYi​ is a noisy reading of the entry of A0A_0A0​ selected by XiX_iXi​; this is matrix completion under uniform sampling at random (USR), entries possibly sampled more than once.

The estimator is, for a regularization parameter λ>0\lambda>0λ>0,

A^λ=argmin⁡A∈Rm1×m2(1m1m2∥A∥22−⟨2n∑i=1nYiXi,A⟩+λ∥A∥1).\hat A^\lambda=\operatorname*{argmin}_{A\in\mathbb R^{m_1\times m_2}}\Big(\frac1{m_1m_2}\|A\|_2^2-\Big\langle\frac2n\sum_{i=1}^nY_iX_i,A\Big\rangle+\lambda\|A\|_1\Big).A^λ=A∈Rm1​×m2​argmin​(m1​m2​1​∥A∥22​−⟨n2​i=1∑n​Yi​Xi​,A⟩+λ∥A∥1​).

The stochastic error is the random matrix

M=1n∑i=1n(YiXi−E(YiXi)).\mathbf M=\frac1n\sum_{i=1}^n\big(Y_iX_i-\mathbb E(Y_iX_i)\big).M=n1​i=1∑n​(Yi​Xi​−E(Yi​Xi​)).

Formalization targets

Goal: Theorem 4

Assume max⁡i∣Yi∣≤η\max_i|Y_i|\le\etamaxi​∣Yi​∣≤η almost surely. For t>0t>0t>0 and

λ≥4ηmax⁡{t+log⁡m(m1∧m2)n, 2(t+log⁡m)n},\lambda\ge4\eta\max\Big\{\sqrt{\frac{t+\log m}{(m_1\wedge m_2)n}},\ \frac{2(t+\log m)}{n}\Big\},λ≥4ηmax{(m1​∧m2​)nt+logm​​, n2(t+logm)​},

with probability at least 1−e−t1-e^{-t}1−e−t, simultaneously for all A∈Rm1×m2A\in\mathbb R^{m_1\times m_2}A∈Rm1​×m2​,

∥A^λ−A0∥22≤∥A−A0∥22+m1m2min⁡{2λ∥A∥1, (1+22)2m1m2λ2rank⁡(A)}.\|\hat A^\lambda-A_0\|_2^2\le\|A-A_0\|_2^2+m_1m_2\min\Big\{2\lambda\|A\|_1,\ \Big(\frac{1+\sqrt2}2\Big)^2m_1m_2\lambda^2\operatorname{rank}(A)\Big\}.∥A^λ−A0​∥22​≤∥A−A0​∥22​+m1​m2​min{2λ∥A∥1​, (21+2​​)2m1​m2​λ2rank(A)}.

Milestones

  1. (1.4): ∥A∥L2(Π)2=1n∑iE⟨A,Xi⟩2=(m1m2)−1∥A∥22\|A\|_{L_2(\Pi)}^2=\frac1n\sum_i\mathbb E\langle A,X_i\rangle^2=(m_1m_2)^{-1}\|A\|_2^2∥A∥L2​(Π)2​=n1​∑i​E⟨A,Xi​⟩2=(m1​m2​)−1∥A∥22​ for the uniform design.
  2. Theorem 1 for USR matrix completion: at every sample point where λ≥2∥M∥∞\lambda\ge2\|\mathbf M\|_\inftyλ≥2∥M∥∞​, the inequality above holds for all AAA (a deterministic statement).
  3. Proposition 1 (matrix Bernstein): for independent centred m1×m2m_1\times m_2m1​×m2​ random matrices ZiZ_iZi​ with ∥Zi∥≤U\|Z_i\|\le U∥Zi​∥≤U a.s., with probability at least 1−e−t1-e^{-t}1−e−t,
∥Z1+⋯+Znn∥≤2max⁡{σZt+log⁡mn, Ut+log⁡mn}.\Big\|\frac{Z_1+\dots+Z_n}n\Big\|\le2\max\Big\{\sigma_Z\sqrt{\frac{t+\log m}n},\ U\frac{t+\log m}n\Big\}.​nZ1​+⋯+Zn​​​≤2max{σZ​nt+logm​​, Unt+logm​}.
  1. (6.2): for XXX uniform on X\mathcal XX, ∥X∥=1\|X\|=1∥X∥=1, ∥EX∥=(m1m2)−1/2\|\mathbb EX\|=(m_1m_2)^{-1/2}∥EX∥=(m1​m2​)−1/2, σX2=1/(m1∧m2)\sigma_X^2=1/(m_1\wedge m_2)σX2​=1/(m1​∧m2​).
  2. Lemma 1: with probability at least 1−e−t1-e^{-t}1−e−t, ∥M∥≤2ηmax⁡{(t+log⁡m)/((m1∧m2)n), 2(t+log⁡m)/n}\|\mathbf M\|\le2\eta\max\{\sqrt{(t+\log m)/((m_1\wedge m_2)n)},\ 2(t+\log m)/n\}∥M∥≤2ηmax{(t+logm)/((m1​∧m2​)n)​, 2(t+logm)/n}.

Significance

Theorem 4 is a non-asymptotic, sharp oracle inequality: the leading constant in front of ∥A−A0∥22\|A-A_0\|_2^2∥A−A0​∥22​ is 1, so the bound applies to misspecified targets (A0A_0A0​ not low rank) without loss. Taking A=A0A=A_0A=A0​ and ttt of order log⁡m\log mlogm gives a normalized Frobenius error of order η2(m1∨m2)rank⁡(A0)log⁡(m)/n\eta^2(m_1\vee m_2)\operatorname{rank}(A_0)\log(m)/nη2(m1​∨m2​)rank(A0​)log(m)/n, which the paper's minimax lower bounds (§4) show to be optimal up to the logarithm. Because no model is needed for Lemma 1, the same probability bound also drives the paper's statistical-learning reformulation (Theorem 9).

The theorems here are proved in the paper. What is open is their formalization: no matrix Bernstein inequality, and no oracle inequality for nuclear-norm penalized estimators, has a machine-checked proof on this platform. Proposition 1 in particular is a reusable concentration tool well beyond this paper (covariance estimation, random graphs, sketching).

Difficulty

The deterministic part (milestone 2) needs the subdifferential of the nuclear norm, which is not in Mathlib. The probabilistic part is where the obvious argument fails. Bounding ∥M∥∞\|\mathbf M\|_\infty∥M∥∞​ entrywise and summing, or bounding it by the Frobenius norm, loses a factor polynomial in the dimension; a union bound over a net of the unit sphere loses the factor m1∧m2m_1\wedge m_2m1​∧m2​ that makes the rate optimal. The correct rate requires a noncommutative Bernstein inequality, controlling the operator norm of a sum of independent random matrices through the matrix variance σZ2\sigma_Z^2σZ2​ at the price of only a log⁡(m1+m2)\log(m_1+m_2)log(m1​+m2​) factor. The matrix-analytic machinery such inequalities depend on (trace inequalities for matrix exponentials, the passage from rectangular to symmetric matrices) is not currently available in Mathlib.

Formalization scope

All objects are local to the namespace KLTNuclear.Completion, built on the published MatrixCompletion definitions (RealMatrix, nuclearNorm, spectralNorm, frobeniusNormSq, matrixInner, coordinateMatrix). Conventions:

  • The probability space carries IsProbabilityMeasure; n,m1,m2≥1n,m_1,m_2\ge1n,m1​,m2​≥1 are hypotheses. log⁡\loglog is the natural logarithm; m=m1+m2≥2m=m_1+m_2\ge2m=m1​+m2​≥2.
  • The design is encoded by uniform random indices Ii∈[m1]×[m2]I_i\in[m_1]\times[m_2]Ii​∈[m1​]×[m2​] with Xi=ejieki⊤X_i=e_{j_i}e_{k_i}^\topXi​=eji​​eki​⊤​. Mathlib has no σ\sigmaσ-algebra on Matrix, so measurability, independence and conditioning on a random matrix use its entry array with the product σ\sigmaσ-algebra; expectations of matrices are entrywise.
  • The model (1.1) is a conditional expectation given σ(Xi)\sigma(X_i)σ(Xi​). Independence of the pairs (Xi,Yi)(X_i,Y_i)(Xi​,Yi​) is the paper's standing assumption (p. 1) and is assumed in Lemma 1 and Theorem 4, whose proof applies Proposition 1 to Zi=YiXi−E(YiXi)Z_i=Y_iX_i-\mathbb E(Y_iX_i)Zi​=Yi​Xi​−E(Yi​Xi​); the YiY_iYi​ are not assumed identically distributed. λ>0\lambda>0λ>0 is the standing assumption of (1.6). Integrable responses are assumed in milestone 2, bounded measurable responses in Lemma 1 and Theorem 4.
  • A^λ\hat A^\lambdaA^λ is any minimizer of (3.1) at each sample point (it exists and is unique, but neither fact is assumed); the soft-thresholding formula (3.2) is not used as a definition.
  • "With probability at least 1−e−t1-e^{-t}1−e−t" is encoded as an upper bound e−te^{-t}e−t on the outer measure of the failure set; in Theorem 4 the failure set is {ω:∃A, (3.5) fails}\{\omega:\exists A,\ \text{(3.5) fails}\}{ω:∃A, (3.5) fails}, so the bound is uniform in AAA. A formalization that fixes AAA before the probability is weaker and is not the target.
  • No printed slip affects these statements; Corollary 2(ii) of the paper, whose λ\lambdaλ falls below (3.6), is deliberately not included.

The source is the arXiv preprint arXiv:1011.6256v4. Welcome contributions: a general matrix Bernstein inequality (Hermitian and rectangular forms), the nuclear-norm subdifferential, and proofs of the deterministic milestone.

Selected references

  • V. Koltchinskii, K. Lounici, A. B. Tsybakov, Nuclear-norm penalization and optimal rates for noisy low-rank matrix completion, Ann. Statist. 39(5), 2011; preprint arXiv:1011.6256v4. https://arxiv.org/abs/1011.6256
  • J. A. Tropp, User-friendly tail bounds for sums of random matrices, Found. Comput. Math. 12, 2012. https://doi.org/10.1007/s10208-011-9099-z
  • E. J. Candès, B. Recht, Exact matrix completion via convex optimization, Found. Comput. Math. 9, 2009. https://doi.org/10.1007/s10208-009-9045-5
  • E. J. Candès, T. Tao, The power of convex relaxation: near-optimal matrix completion, IEEE Trans. Inform. Theory 56, 2010. https://doi.org/10.1109/TIT.2010.2044061
  • D. Gross, Recovering low-rank matrices from few coefficients in any basis, IEEE Trans. Inform. Theory 57, 2011. https://doi.org/10.1109/TIT.2011.2104999
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