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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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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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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.

≤ 19.8899945Formalized record→≤ 14.797074Open frontier
6 provers on it3 of 7 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.
≤ 89Formalized record
3 provers on it3 of 3 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.

≤ 85Formalized record→≤ 5Open frontier
35 provers on it10 of 12 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?

≤ 2.37134Formalized record→≤ 2.371177Open frontier
16 provers on it7 of 8 missions formalized

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Convex OptimizationLinear OptimizationOperations Research+1·Captain: mikedeng1

On Polyhedral Approximations of the Second-Order Cone I: A Compact Polyhedral Approximation of the Lorentz ConeResearch Paper

Motivation

Conic quadratic programs (second-order cone programs) minimize a linear objective subject to linear constraints and constraints of the form ∥Aℓx−bℓ∥2≤cℓTx−dℓ\|A_\ell x-b_\ell\|_2\le c_\ell^Tx-d_\ell∥Aℓ​x−bℓ​∥2​≤cℓT​x−dℓ​. They model robust linear programs with ellipsoidal uncertainty, truss topology design, contact problems with Coulomb friction, and convex quadratically constrained quadratic programs. In theory they are no harder than linear programs of the same size; in practice, linear programming software handles far larger instances than conic quadratic solvers did at the time of writing (Ben-Tal & Nemirovski 2001, pp. 193–195). This raises a question about geometry rather than algorithms: can a second-order cone be replaced by a polyhedral cone of moderate size without losing much accuracy?

The obvious answer — circumscribe the cone by a polyhedral cone with many facets — fails: the number of facets must grow exponentially in the dimension, even for constant accuracy. Ben-Tal and Nemirovski showed that auxiliary variables change the picture completely: a projection of a polyhedral cone can approximate the Lorentz cone with size only O(kln⁡(1/ε))O(k\ln(1/\varepsilon))O(kln(1/ε)). The construction is now standard; it underlies, for instance, the lifted linear-programming branch-and-bound algorithm for mixed-integer conic quadratic programs of Vielma, Ahmed & Nemhauser 2008.

Setting

For y∈Rky\in\mathbb R^ky∈Rk let ∥y∥2=y12+⋯+yk2\|y\|_2=\sqrt{y_1^2+\dots+y_k^2}∥y∥2​=y12​+⋯+yk2​​. The (k+1)(k+1)(k+1)-dimensional Lorentz cone is

Lk={(y,t)∈Rk×R∣t≥∥y∥2}.L^k=\{(y,t)\in\mathbb R^k\times\mathbb R\mid t\ge\|y\|_2\}.Lk={(y,t)∈Rk×R∣t≥∥y∥2​}.

Fix ε>0\varepsilon>0ε>0. A polyhedral ε\varepsilonε-approximation of LkL^kLk is a linear map

Π(y,t,u):Rk×R×Rp→Rq\Pi(y,t,u):\mathbb R^k\times\mathbb R\times\mathbb R^{p}\to\mathbb R^{q}Π(y,t,u):Rk×R×Rp→Rq

such that

  1. if (y,t)∈Lk(y,t)\in L^k(y,t)∈Lk, there is u∈Rpu\in\mathbb R^pu∈Rp with Π(y,t,u)≥0\Pi(y,t,u)\ge0Π(y,t,u)≥0 (componentwise);
  2. if Π(y,t,u)≥0\Pi(y,t,u)\ge0Π(y,t,u)≥0 for some uuu, then ∥y∥2≤(1+ε)t\|y\|_2\le(1+\varepsilon)t∥y∥2​≤(1+ε)t.

Equivalently, the polyhedral cone {(y,t,u)∣Π(y,t,u)≥0}\{(y,t,u)\mid\Pi(y,t,u)\ge0\}{(y,t,u)∣Π(y,t,u)≥0} projects onto a cone lying between LkL^kLk and its (1+ε)(1+\varepsilon)(1+ε)-extension. The size of the approximation is p+qp+qp+q: the number of auxiliary variables plus the number of linear inequalities (an equation counts as two).

The construction in the paper uses a tower of variables: for k=2θk=2^\thetak=2θ, the coordinates y1,…,yky_1,\dots,y_ky1​,…,yk​ form generation 000, each consecutive pair of generation ℓ−1\ell-1ℓ−1 has a successor in generation ℓ\ellℓ (yiℓy_i^\ellyiℓ​ has parents y2i−1ℓ−1,y2iℓ−1y_{2i-1}^{\ell-1},y_{2i}^{\ell-1}y2i−1ℓ−1​,y2iℓ−1​), and the single variable of generation θ\thetaθ is ttt. It also uses an explicit linear system (8) in variables ξj,ηj\xi^j,\eta^jξj,ηj, j=0,…,νj=0,\dots,\nuj=0,…,ν, with trigonometric coefficients cos⁡(π/2j+1)\cos(\pi/2^{j+1})cos(π/2j+1), sin⁡(π/2j+1)\sin(\pi/2^{j+1})sin(π/2j+1), tan⁡(π/2ν+1)\tan(\pi/2^{\nu+1})tan(π/2ν+1), whose accuracy is δ(ν)=1/cos⁡(π/2ν+1)−1\delta(\nu)=1/\cos(\pi/2^{\nu+1})-1δ(ν)=1/cos(π/2ν+1)−1.

Formalization targets

Goal: Theorem 1.1

There is an absolute constant CCC such that for every positive integer kkk and every ε∈(0,1]\varepsilon\in(0,1]ε∈(0,1], LkL^kLk admits a polyhedral ε\varepsilonε-approximation with

pk+qk≤C kln⁡2ε.p_k+q_k\le C\,k\ln\frac{2}{\varepsilon}.pk​+qk​≤Cklnε2​.

The constant is not fixed; the goal asserts only the order of growth, which is what the paper claims.

Milestones

  1. §2, Eq. (5). For k=2θk=2^\thetak=2θ, θ≥1\theta\ge1θ≥1: (y,t)(y,t)(y,t) extends to a tower solving [y2i−1ℓ−1]2+[y2iℓ−1]2≤yiℓ\sqrt{[y_{2i-1}^{\ell-1}]^2+[y_{2i}^{\ell-1}]^2}\le y_i^\ell[y2i−1ℓ−1​]2+[y2iℓ−1​]2​≤yiℓ​ for all i,ℓi,\elli,ℓ if and only if ∥y∥2≤t\|y\|_2\le t∥y∥2​≤t.
  2. §2, Eqs. (6)–(7). Placing polyhedral εℓ\varepsilon_\ellεℓ​-approximations of L2L^2L2 on every level of the tower yields a polyhedral approximation of LkL^kLk with 1+ε=∏ℓ=1θ(1+εℓ)1+\varepsilon=\prod_{\ell=1}^\theta(1+\varepsilon_\ell)1+ε=∏ℓ=1θ​(1+εℓ​).
  3. Proposition 2.1 (i), (ii) and Eq. (9). System (8) is a polyhedral δ(ν)\delta(\nu)δ(ν)-approximation of L2L^2L2, and δ(ν)=O(4−ν)\delta(\nu)=O(4^{-\nu})δ(ν)=O(4−ν).
  4. Proof of Theorem 1.1, system (10), property 3. System (8) with parameter νℓ\nu_\ellνℓ​ on level ℓ\ellℓ of the tower approximates L2θL^{2^\theta}L2θ with quality β=∏ℓ=1θ1/cos⁡(π/2νℓ+1)−1\beta=\prod_{\ell=1}^\theta 1/\cos(\pi/2^{\nu_\ell+1})-1β=∏ℓ=1θ​1/cos(π/2νℓ​+1)−1.
  5. Proof of Theorem 1.1, choice of νℓ\nu_\ellνℓ​. With νℓ=⌊c ℓln⁡(2/ε)⌋\nu_\ell=\lfloor c\,\ell\ln(2/\varepsilon)\rfloorνℓ​=⌊cℓln(2/ε)⌋: β≤ε\beta\le\varepsilonβ≤ε and ∑ℓ2θ−ℓνℓ≤C 2θln⁡(2/ε)\sum_\ell 2^{\theta-\ell}\nu_\ell\le C\,2^\theta\ln(2/\varepsilon)∑ℓ​2θ−ℓνℓ​≤C2θln(2/ε).

Significance

The theorem shows that conic quadratic constraints are, up to a factor logarithmic in the accuracy, no more expensive to express as linear constraints than they are in their native form. Consequences listed in the paper include approximating convex quadratically constrained quadratic programs, robust counterparts of linear programs with ellipsoidal uncertainty, and problems with low-dimensional cones (Coulomb friction, k≤3k\le3k≤3; truss design, k≤2k\le2k≤2) by linear programs of comparable size. Together with the matching lower bound of §3 of the same paper (a separate mission of this series), it pins down the size of the best polyhedral approximation up to constants. The recursive halving of dimensions through the tower of 3-dimensional cones is a reusable device for other rotation-invariant cones.

The result is proved in the paper; as far as is known it has not been machine-checked. This mission produces a formal proof of the construction, including the trigonometric estimate δ(ν)=O(4−ν)\delta(\nu)=O(4^{-\nu})δ(ν)=O(4−ν) and the explicit linear encoding with its size count. Explicit values of the absolute constants are welcome as additional results.

Difficulty

The planar estimate is the core. Part (ii) of Proposition 2.1 must hold for every solution of the inequality system (8), not only for the solution one would write down for a given point of L2L^2L2; an argument that tracks only the intended solution proves part (i) and nothing about part (ii). The accuracy must also come out as 1/cos⁡(π/2ν+1)−11/\cos(\pi/2^{\nu+1})-11/cos(π/2ν+1)−1, geometric in ν\nuν; a bound that decays only polynomially in ν\nuν would give size poly(1/ε)\mathrm{poly}(1/\varepsilon)poly(1/ε) instead of ln⁡(1/ε)\ln(1/\varepsilon)ln(1/ε). The naive idea of approximating LkL^kLk directly by tangent hyperplanes is ruled out by the exponential facet count mentioned above; the auxiliary variables are indispensable. The second difficulty is bookkeeping: packaging k−1k-1k−1 copies of system (8) on a tower of depth θ=log⁡2k\theta=\log_2 kθ=log2​k into a single linear map, counting its variables and inequalities exactly, handling kkk that is not a power of two, and summing the accuracies so that the total size is O(kln⁡(2/ε))O(k\ln(2/\varepsilon))O(kln(2/ε)) rather than O(kln⁡kln⁡(1/ε))O(k\ln k\ln(1/\varepsilon))O(klnkln(1/ε)).

Formalization scope

  • Vectors of Rk\mathbb R^kRk are Fin k → ℝ. The norm ∥y∥2\|y\|_2∥y∥2​ is written out as eucNorm y = Real.sqrt (∑ i, y i ^ 2); the norm Mathlib attaches to Fin k → ℝ is the sup norm, under which the cone would be polyhedral and the theorem trivial.
  • A polyhedral approximation is an R\mathbb RR-linear map (Fin k → ℝ) × ℝ × (Fin p → ℝ) →ₗ[ℝ] (Fin q → ℝ) and ≥0\ge0≥0 is the componentwise order. Linearity is essential: with an arbitrary map, Π(y,t)=t−∥y∥2\Pi(y,t)=t-\|y\|_2Π(y,t)=t−∥y∥2​ would be an exact approximation with p=0p=0p=0, q=1q=1q=1. Affine maps are not allowed either; the paper's approximations are homogeneous.
  • The paper's absolute constants O(1)O(1)O(1) are existential constants quantified before kkk, ε\varepsilonε and θ\thetaθ. The goal requires k≥1k\ge1k≥1 and ε∈(0,1]\varepsilon\in(0,1]ε∈(0,1], as in the paper; ln⁡\lnln is Real.log.
  • System (8) and system (10) are stated as propositions with the absolute values written out; their parameters ν\nuν, νℓ\nu_\ellνℓ​ are required to be positive integers, as in the paper (at ν=0\nu=0ν=0 the coefficient tan⁡(π/2)\tan(\pi/2)tan(π/2) would be evaluated as 000 by Lean).
  • Tower variables are indexed Y ℓ i with 0-based i, so the parents of Y ℓ i are Y (ℓ-1) (2i) and Y (ℓ-1) (2i+1); the milestones on (6)–(7) and (10) are stated on solution sets rather than on an explicit linear map. The size counts of (10) (properties 1–2) are not separate milestones; the arithmetic milestone on νℓ\nu_\ellνℓ​ records the bound on ∑ℓ2θ−ℓνℓ\sum_\ell 2^{\theta-\ell}\nu_\ell∑ℓ​2θ−ℓνℓ​ to which they reduce.
  • δ(ν)=O(1/4ν)\delta(\nu)=O(1/4^\nu)δ(ν)=O(1/4ν) is stated as ∃C>0, ∀ν≥1, δ(ν)≤C/4ν\exists C>0,\ \forall\nu\ge1,\ \delta(\nu)\le C/4^\nu∃C>0, ∀ν≥1, δ(ν)≤C/4ν.

A complete development needs: elementary trigonometry of π/2j\pi/2^{j}π/2j (available in Mathlib), rotations in the plane, finite products and sums over {1,…,θ}\{1,\dots,\theta\}{1,…,θ}, and a way to assemble many small linear systems into one linear map with an exact count of rows and columns. The last piece, and the tower of variables with the reduction from arbitrary kkk to a power of two, are reusable for other lifted polyhedral approximations. Contributions of any milestone, of explicit linear encodings of (8) and (10), and of the extension from k=2θk=2^\thetak=2θ to all kkk are welcome.

Selected references

  • A. Ben-Tal and A. Nemirovski, On Polyhedral Approximations of the Second-Order Cone, Mathematics of Operations Research 26(2):193–205, 2001. https://doi.org/10.1287/moor.26.2.193.10561
  • J. P. Vielma, S. Ahmed and G. L. Nemhauser, A lifted linear programming branch-and-bound algorithm for mixed-integer conic quadratic programs, INFORMS Journal on Computing 20(3):438–450, 2008. https://doi.org/10.1287/ijoc.1070.0256
  • A. Ben-Tal and A. Nemirovski, Robust convex optimization, Mathematics of Operations Research 23(4):769–805, 1998. https://doi.org/10.1287/moor.23.4.769
  • A. Ben-Tal and A. Nemirovski, Lectures on Modern Convex Optimization, SIAM, 2001. https://doi.org/10.1137/1.9780898718829
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🏆Completed
Machine LearningOptimizationProbability+1·Captain: mikedeng1

Simultaneous Analysis of Lasso and Dantzig Selector V: Estimation, Prediction and Sparsity Bounds for the LassoResearch Paper

Motivation

In a linear regression with many more candidate variables than observations, least squares is not defined uniquely and does not estimate anything useful. The Lasso (Tibshirani, 1996) replaces it by an ℓ1\ell_1ℓ1​-penalised least-squares problem, which is convex, can be solved at scale, and returns sparse coefficient vectors. The question that a statistician, a signal-processing engineer or an operations researcher fitting a sparse model must answer before trusting it is quantitative: how far is the Lasso estimate from the true coefficient vector, how well does it predict, and how many variables does it select, as functions of the sample size nnn, the number of variables MMM and the sparsity sss of the truth?

Bickel, Ritov and Tsybakov (arXiv:0801.1095, Ann. Statist. 37(4), 2009) answered this under the restricted eigenvalue (RE) condition, which they introduced, with explicit constants and an explicit failure probability. Their Theorem 7.2, the goal of this mission, is a standard reference result of high-dimensional statistics and a model for the Lasso analyses in the textbooks of Bühlmann and van de Geer (2011) and Wainwright (2019).

Timeline, restricted to what each work proved:

  • 2007: Candès and Tao (arXiv:math/0506081) prove ℓ2\ell_2ℓ2​ bounds for the Dantzig selector under a uniform uncertainty principle.
  • 2007: Bunea, Tsybakov and Wegkamp (doi:10.1214/07-EJS008) prove sparsity oracle inequalities for the Lasso under mutual-coherence conditions; Lemma B.1 of the present paper is essentially their Lemma 1.
  • 2008/2009: Bickel, Ritov and Tsybakov prove Theorem 7.2 under RE(s,3)(s,3)(s,3) and RE(s,m,3)(s,m,3)(s,m,3), conditions weaker than those of the previous works.

Setting

A deterministic design matrix X∈Rn×MX\in\mathbb R^{n\times M}X∈Rn×M with columns x(1),…,x(M)x_{(1)},\dots,x_{(M)}x(1)​,…,x(M)​ is observed together with

y=Xβ∗+w,y=X\beta^*+w,y=Xβ∗+w,

where β∗∈RM\beta^*\in\mathbb R^Mβ∗∈RM is unknown and w=(W1,…,Wn)w=(W_1,\dots,W_n)w=(W1​,…,Wn​) has independent N(0,σ2)\mathcal N(0,\sigma^2)N(0,σ2) entries with σ>0\sigma>0σ>0. Throughout, n≥1n\ge1n≥1, M≥2M\ge2M≥2, and every diagonal entry of the Gram matrix Ψn=X⊤X/n\Psi_n=X^\top X/nΨn​=X⊤X/n equals 111.

For δ∈RM\delta\in\mathbb R^Mδ∈RM write ∣δ∣p=(∑j∣δj∣p)1/p|\delta|_p=(\sum_j|\delta_j|^p)^{1/p}∣δ∣p​=(∑j​∣δj​∣p)1/p, J(δ)={j:δj≠0}J(\delta)=\{j:\delta_j\ne0\}J(δ)={j:δj​=0} for the support, M(δ)=∣J(δ)∣\mathcal M(\delta)=|J(\delta)|M(δ)=∣J(δ)∣ for the sparsity, and δJ\delta_JδJ​ for the vector that agrees with δ\deltaδ on JJJ and vanishes off JJJ. The largest eigenvalue of Ψn\Psi_nΨn​ is ϕmax⁡\phi_{\max}ϕmax​.

The Lasso estimator with tuning parameter r>0r>0r>0 is any minimiser

β^L∈arg⁡min⁡β∈RM{1n∣y−Xβ∣22+2r∣β∣1}.\hat\beta_L\in\arg\min_{\beta\in\mathbb R^M}\Big\{\frac1n|y-X\beta|_2^2+2r|\beta|_1\Big\}.β^​L​∈argβ∈RMmin​{n1​∣y−Xβ∣22​+2r∣β∣1​}.

Minimisers exist but need not be unique.

Assumption RE(s,c0)(s,c_0)(s,c0​) (1≤s≤M1\le s\le M1≤s≤M, c0>0c_0>0c0​>0) asks that

κ(s,c0)=min⁡∣J0∣≤s min⁡δ≠0, ∣δJ0c∣1≤c0∣δJ0∣1∣Xδ∣2n ∣δJ0∣2>0.\kappa(s,c_0)=\min_{|J_0|\le s}\ \min_{\delta\ne0,\ |\delta_{J_0^c}|_1\le c_0|\delta_{J_0}|_1}\frac{|X\delta|_2}{\sqrt n\,|\delta_{J_0}|_2}>0 .κ(s,c0​)=∣J0​∣≤smin​ δ=0, ∣δJ0c​​∣1​≤c0​∣δJ0​​∣1​min​n​∣δJ0​​∣2​∣Xδ∣2​​>0.

Assumption RE(s,m,c0)(s,m,c_0)(s,m,c0​) (1≤s≤M/21\le s\le M/21≤s≤M/2, m≥sm\ge sm≥s, s+m≤Ms+m\le Ms+m≤M) is the same with ∣δJ01∣2|\delta_{J_{01}}|_2∣δJ01​​∣2​ in the denominator, where J01=J0∪J1J_{01}=J_0\cup J_1J01​=J0​∪J1​ and J1J_1J1​ collects the mmm largest in absolute value coordinates of δ\deltaδ outside J0J_0J0​.

Formalization targets

Goal: Theorem 7.2

Let M(β∗)≤s\mathcal M(\beta^*)\le sM(β∗)≤s, let RE(s,3)(s,3)(s,3) hold, and let r=Aσlog⁡M/nr=A\sigma\sqrt{\log M/n}r=AσlogM/n​ with A>22A>2\sqrt2A>22​. With probability at least 1−M1−A2/81-M^{1-A^2/8}1−M1−A2/8, every Lasso solution satisfies

∣β^L−β∗∣1≤16Aκ2(s,3)σslog⁡Mn,∣X(β^L−β∗)∣22≤16A2κ2(s,3)σ2slog⁡M,M(β^L)≤64ϕmax⁡κ2(s,3)s,|\hat\beta_L-\beta^*|_1\le\frac{16A}{\kappa^2(s,3)}\sigma s\sqrt{\frac{\log M}{n}},\qquad |X(\hat\beta_L-\beta^*)|_2^2\le\frac{16A^2}{\kappa^2(s,3)}\sigma^2s\log M,\qquad \mathcal M(\hat\beta_L)\le\frac{64\phi_{\max}}{\kappa^2(s,3)}s,∣β^​L​−β∗∣1​≤κ2(s,3)16A​σsnlogM​​,∣X(β^​L​−β∗)∣22​≤κ2(s,3)16A2​σ2slogM,M(β^​L​)≤κ2(s,3)64ϕmax​​s,

and, if RE(s,m,3)(s,m,3)(s,m,3) holds, on the same event and for all 1<p≤21<p\le21<p≤2,

∣β^L−β∗∣pp≤16{1+3sm}2(p−1)s(Aσκ2(s,m,3)log⁡Mn)p.|\hat\beta_L-\beta^*|_p^p\le16\Big\{1+3\sqrt{\tfrac sm}\Big\}^{2(p-1)}s\Big(\frac{A\sigma}{\kappa^2(s,m,3)}\sqrt{\frac{\log M}{n}}\Big)^p .∣β^​L​−β∗∣pp​≤16{1+3ms​​}2(p−1)s(κ2(s,m,3)Aσ​nlogM​​)p.

Milestones

In the order in which the paper's proof uses them:

  1. (B.4): the noise event A=⋂j{2∣1nx(j)⊤w∣≤r}\mathcal A=\bigcap_j\{2|\tfrac1n x_{(j)}^\top w|\le r\}A=⋂j​{2∣n1​x(j)⊤​w∣≤r} has P(Ac)≤M1−A2/8\mathbb P(\mathcal A^c)\le M^{1-A^2/8}P(Ac)≤M1−A2/8.
  2. (B.6): the optimality conditions of the Lasso.
  3. Lemma B.1 (Section 7 case): the basic inequality (B.1) for all β\betaβ, the residual bound (B.2) and the sparsity bound M(β^L)≤4ϕmax⁡∥fβ^L−f∥n2/r2\mathcal M(\hat\beta_L)\le4\phi_{\max}\|f_{\hat\beta_L}-f\|_n^2/r^2M(β^​L​)≤4ϕmax​∥fβ^​L​​−f∥n2​/r2 (B.3).
  4. Corollary B.2: the error δ=β^L−β\delta=\hat\beta_L-\betaδ=β^​L​−β lies in the cone ∣δJ0c∣1≤3∣δJ0∣1|\delta_{J_0^c}|_1\le3|\delta_{J_0}|_1∣δJ0c​​∣1​≤3∣δJ0​​∣1​.
  5. (B.30)–(B.31): on A\mathcal AA, 1n∣Xδ∣22≤16r2s/κ2\frac1n|X\delta|_2^2\le16r^2s/\kappa^2n1​∣Xδ∣22​≤16r2s/κ2 and ∣δJ0∣2≤4rs/κ2|\delta_{J_0}|_2\le4r\sqrt s/\kappa^2∣δJ0​​∣2​≤4rs​/κ2.
  6. (B.27) and (B.28) with c0=3c_0=3c0​=3: ℓ1\ell_1ℓ1​ and ℓ2\ell_2ℓ2​ norms of a cone vector.
  7. The ℓp\ell_pℓp​ interpolation ∑ajp≤b12−pb2p−1\sum a_j^p\le b_1^{2-p}b_2^{p-1}∑ajp​≤b12−p​b2p−1​.

Significance

The result. Theorem 7.2 gives, for fixed nnn and MMM rather than asymptotically, the rate slog⁡M/ns\log M/nslogM/n for the prediction loss and slog⁡M/ns\sqrt{\log M/n}slogM/n​ for the ℓ1\ell_1ℓ1​ loss of the Lasso, under a condition on the design only (RE), with no assumption on how MMM compares with nnn. The dependence on MMM is only logarithmic, which is what makes the Lasso usable when M≫nM\gg nM≫n. Bound (7.9) shows that the Lasso selects at most a constant multiple of sss variables, and (7.10) covers every ℓp\ell_pℓp​ loss between ℓ1\ell_1ℓ1​ and ℓ2\ell_2ℓ2​. Together with Theorem 7.1 for the Dantzig selector, the result shows that the two estimators have the same rates.

Formalizing it. The theorem is proved on paper. As far as a search of the platform shows, there is no machine-checked proof of a probabilistic Lasso rate. The closest platform statement, HighDimStat.SparseLinear.lasso_l2_error_bound (Wainwright, Theorem 7.13(a)), is deterministic, assumes a lower bound on the regularisation parameter in place of Gaussian noise, uses a restricted eigenvalue condition over the cone of one fixed support, and concludes an ℓ2\ell_2ℓ2​ bound with a different constant. A formal proof of Theorem 7.2 would supply the Gaussian maximal inequality, the Lasso optimality conditions, and the cone and interpolation inequalities as reusable lemmas.

Difficulty

Each step is short on paper, and none of the steps is deep. The main work is in three places. First, the probability: the event on which the deterministic argument runs involves all MMM correlations 1nx(j)⊤w\frac1n x_{(j)}^\top wn1​x(j)⊤​w at once, and its probability must be bounded by exactly M1−A2/8M^{1-A^2/8}M1−A2/8, which requires the law of a linear combination of independent Gaussians and a sharp Gaussian tail estimate, not a generic concentration bound with unspecified constants. Second, the Lasso is defined only through its minimising property, while the sparsity bound (7.9) is a statement about the number of non-zero coordinates of a minimiser of a non-differentiable objective; the characterisation (B.6) of minimisers is not in Mathlib. Third, (7.10) involves two restricted eigenvalue constants, a ranking of coordinates with possible ties, and real exponents, and every constant has to come out exactly.

The obvious idea of proving (7.7)–(7.10) for one fixed minimiser does not suffice: the statement quantifies over every minimiser on a single event.

Formalization scope

The design XXX is a Matrix (Fin n) (Fin M) ℝ; vectors are functions Fin M → ℝ. The noise is a family W : Fin n → Ω → ℝ of independent, measurable random variables with law gaussianReal 0 σ² on a probability space, and y(ω)=Xβ∗+W(ω)y(\omega)=X\beta^*+W(\omega)y(ω)=Xβ∗+W(ω). The probabilistic conclusion is one measurable event EEE with P(E)≥1−M1−A2/8\mathbb P(E)\ge1-M^{1-A^2/8}P(E)≥1−M1−A2/8 on which every minimiser of (7.2) satisfies all bounds; the event does not depend on the minimiser, on mmm or on ppp. log⁡\loglog is the natural logarithm.

RE(s,3)(s,3)(s,3) and RE(s,m,3)(s,m,3)(s,m,3) are stated through witnesses: a predicate "κn∣δJ0∣2≤∣Xδ∣2\kappa\sqrt n|\delta_{J_0}|_2\le|X\delta|_2κn​∣δJ0​​∣2​≤∣Xδ∣2​ for every admissible J0J_0J0​ and δ\deltaδ", and the theorem holds for every witness κ>0\kappa>0κ>0. Because the paper's κ(s,c0)\kappa(s,c_0)κ(s,c0​) is an attained minimum, every witness is at most it and the bounds decrease in κ\kappaκ, so this is equivalent to the printed statement. The assumption quantifies over every J0J_0J0​ with ∣J0∣≤s|J_0|\le s∣J0​∣≤s, as on page 7, not only over the support of β∗\beta^*β∗. ϕmax⁡\phi_{\max}ϕmax​ is the supremum of 1n∣Xx∣22\frac1n|Xx|_2^2n1​∣Xx∣22​ over unit vectors xxx. Lemma B.1 is stated in its Section-7 specialisation (unit column norms, f=Xβ∗f=X\beta^*f=Xβ∗), the form used in the proof of Theorem 7.2; (B.28) is stated for every c0>0c_0>0c0​>0 and (B.27) likewise, since the paper writes them with c0=1c_0=1c0​=1 and invokes them with c0=3c_0=3c0​=3. The printed Theorem 7.2 needs no correction; all four constants were checked against the proof.

A formalization in which the noise is not Gaussian, the Lasso predicate can be vacuous, the RE condition is imposed only on the support of β∗\beta^*β∗, or the probability is that of a non-measurable set, is not this theorem and is ruled out by the statement.

Needed infrastructure: Gaussian tail bounds and the law of a linear combination of independent Gaussians (largely in Mathlib), subdifferential calculus for ℓ1\ell_1ℓ1​-penalised least squares, and elementary finite-sum inequalities. The cone inequalities (B.27)–(B.28), the interpolation inequality and the optimality conditions (B.6) are reusable in other sparse-estimation missions; contributions to any milestone are welcome.

Selected references

  • P. J. Bickel, Y. Ritov, A. B. Tsybakov, Simultaneous analysis of Lasso and Dantzig selector, Ann. Statist. 37(4), 1705–1732, 2009. arXiv:0801.1095v3, https://arxiv.org/abs/0801.1095 ; https://doi.org/10.1214/08-AOS620
  • F. Bunea, A. B. Tsybakov, M. H. Wegkamp, Sparsity oracle inequalities for the Lasso, Electron. J. Statist. 1, 169–194, 2007. https://doi.org/10.1214/07-EJS008
  • E. Candès, T. Tao, The Dantzig selector: statistical estimation when p is much larger than n, Ann. Statist. 35(6), 2313–2351, 2007. https://arxiv.org/abs/math/0506081
  • R. Tibshirani, Regression shrinkage and selection via the lasso, J. R. Statist. Soc. B 58(1), 267–288, 1996. https://doi.org/10.1111/j.2517-6161.1996.tb02080.x
  • M. J. Wainwright, High-Dimensional Statistics: A Non-Asymptotic Viewpoint, Cambridge University Press, 2019, Chapter 7. https://doi.org/10.1017/9781108627771
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Simultaneous Analysis of Lasso and Dantzig Selector IV: Estimation and Prediction Error Bounds for the Dantzig SelectorResearch Paper

Motivation

In high-dimensional linear regression the number of unknown coefficients MMM may be much larger than the number of observations nnn, and the coefficient vector can only be recovered because it is assumed to be sparse: few of its entries are non-zero. Two convex estimators dominate this setting: the Lasso of Tibshirani (1996), an ℓ1\ell_1ℓ1​-penalized least-squares estimator, and the Dantzig selector of Candès and Tao (2007), which minimizes the ℓ1\ell_1ℓ1​ norm subject to a bound on the correlation between the residual and the columns of the design. Both are used routinely in statistics, signal processing and machine learning, and their rates of convergence determine how many observations suffice to estimate a sparse vector.

Bickel, Ritov and Tsybakov (arXiv:0801.1095; Ann. Statist. 37(4), 2009) analysed the two estimators side by side under a single, weak condition on the design, the restricted eigenvalue (RE) assumption. This mission formalizes their rates for the Dantzig selector, Theorem 7.1 of the paper.

Timeline. Candès and Tao (Ann. Statist. 35, 2007) introduced the Dantzig selector and bounded its ℓ2\ell_2ℓ2​ error under a uniform uncertainty principle on the design. Bickel, Ritov and Tsybakov (2009) replaced that condition by the RE assumptions, which are implied by it (their Lemma 4.1), and obtained ℓp\ell_pℓp​ bounds for every 1≤p≤21\le p\le21≤p≤2 and a prediction bound, with explicit constants. Later work (van de Geer and Bühlmann, EJS 2009) compared RE with the compatibility condition and other design conditions.

Setting

Observations follow the linear model

y=Xβ∗+w,y=X\beta^*+w,y=Xβ∗+w,

where X∈Rn×MX\in\mathbb R^{n\times M}X∈Rn×M is a deterministic design matrix, n≥1n\ge1n≥1, M≥2M\ge2M≥2, β∗∈RM\beta^*\in\mathbb R^Mβ∗∈RM is unknown, and w=(W1,…,Wn)w=(W_1,\dots,W_n)w=(W1​,…,Wn​) has independent N(0,σ2)\mathcal N(0,\sigma^2)N(0,σ2) coordinates with σ>0\sigma>0σ>0. The columns are normalized: every diagonal element of the Gram matrix XTX/nX^TX/nXTX/n equals 1.

For β∈RM\beta\in\mathbb R^Mβ∈RM, J(β)={j:βj≠0}J(\beta)=\{j:\beta_j\ne0\}J(β)={j:βj​=0} is its support and M(β)=∣J(β)∣\mathcal M(\beta)=|J(\beta)|M(β)=∣J(β)∣ its sparsity; β∗\beta^*β∗ satisfies M(β∗)≤s\mathcal M(\beta^*)\le sM(β∗)≤s for an integer 1≤s≤M1\le s\le M1≤s≤M. Norms are ∣δ∣p=(∑j∣δj∣p)1/p|\delta|_p=(\sum_j|\delta_j|^p)^{1/p}∣δ∣p​=(∑j​∣δj​∣p)1/p and ∣v∣22=∑ivi2|v|_2^2=\sum_iv_i^2∣v∣22​=∑i​vi2​; for an index set JJJ, δJ\delta_JδJ​ keeps the coordinates of δ\deltaδ in JJJ and sets the others to 0, and JcJ^cJc is the complement of JJJ.

With a tuning level r=Aσlog⁡M/nr=A\sigma\sqrt{\log M/n}r=AσlogM/n​, A>2A>\sqrt2A>2​, the Dantzig selector is any minimizer

β^D∈arg⁡min⁡β∈Λ∣β∣1,Λ={β∈RM: ∣1nXT(y−Xβ)∣∞≤r}.\hat\beta_D\in\arg\min_{\beta\in\Lambda}|\beta|_1,\qquad \Lambda=\Big\{\beta\in\mathbb R^M:\ \Big|\tfrac1nX^T(y-X\beta)\Big|_\infty\le r\Big\}.β^​D​∈argβ∈Λmin​∣β∣1​,Λ={β∈RM: ​n1​XT(y−Xβ)​∞​≤r}.

The cone condition at an index set J0J_0J0​ with constant c0>0c_0>0c0​>0 is ∣δJ0c∣1≤c0∣δJ0∣1|\delta_{J_0^c}|_1\le c_0|\delta_{J_0}|_1∣δJ0c​​∣1​≤c0​∣δJ0​​∣1​. Assumption RE(s,c0)(s,c_0)(s,c0​) asks that

κ(s,c0)=min⁡∣J0∣≤s min⁡δ≠0, ∣δJ0c∣1≤c0∣δJ0∣1∣Xδ∣2n ∣δJ0∣2>0.\kappa(s,c_0)=\min_{|J_0|\le s}\ \min_{\delta\ne0,\ |\delta_{J_0^c}|_1\le c_0|\delta_{J_0}|_1}\frac{|X\delta|_2}{\sqrt n\,|\delta_{J_0}|_2}>0 .κ(s,c0​)=∣J0​∣≤smin​ δ=0, ∣δJ0c​​∣1​≤c0​∣δJ0​​∣1​min​n​∣δJ0​​∣2​∣Xδ∣2​​>0.

Assumption RE(s,m,c0)(s,m,c_0)(s,m,c0​) is the same with ∣δJ01∣2|\delta_{J_{01}}|_2∣δJ01​​∣2​ in the denominator, where J01=J0∪J1J_{01}=J_0\cup J_1J01​=J0​∪J1​ and J1J_1J1​ collects the mmm largest ∣δj∣|\delta_j|∣δj​∣ outside J0J_0J0​; it is used for s≤ms\le ms≤m, s+m≤Ms+m\le Ms+m≤M.

Formalization targets

Goal: Theorem 7.1

With probability at least 1−M1−A2/21-M^{1-A^2/2}1−M1−A2/2, every Dantzig selector satisfies

∣β^D−β∗∣1≤8Aκ2(s,1) σslog⁡Mn,∣X(β^D−β∗)∣22≤16A2κ2(s,1) σ2slog⁡M,|\hat\beta_D-\beta^*|_1\le\frac{8A}{\kappa^2(s,1)}\,\sigma s\sqrt{\frac{\log M}{n}},\qquad |X(\hat\beta_D-\beta^*)|_2^2\le\frac{16A^2}{\kappa^2(s,1)}\,\sigma^2s\log M,∣β^​D​−β∗∣1​≤κ2(s,1)8A​σsnlogM​​,∣X(β^​D​−β∗)∣22​≤κ2(s,1)16A2​σ2slogM,

and, on the same event, if RE(s,m,1)(s,m,1)(s,m,1) holds, simultaneously for all 1<p≤21<p\le21<p≤2,

∣β^D−β∗∣pp≤2p−1 8{1+sm}2(p−1)s(Aσκ2(s,m,1)log⁡Mn)p.|\hat\beta_D-\beta^*|_p^p\le2^{p-1}\,8\Big\{1+\sqrt{\tfrac sm}\Big\}^{2(p-1)}s\Big(\frac{A\sigma}{\kappa^2(s,m,1)}\sqrt{\frac{\log M}{n}}\Big)^p .∣β^​D​−β∗∣pp​≤2p−18{1+ms​​}2(p−1)s(κ2(s,m,1)Aσ​nlogM​​)p.

Milestones

In the order the proof of the paper uses them:

  1. The noise event B=⋂j{∣1n∑iXijWi∣≤r∥fj∥n}\mathcal B=\bigcap_j\{|\frac1n\sum_iX_{ij}W_i|\le r\|f_j\|_n\}B=⋂j​{∣n1​∑i​Xij​Wi​∣≤r∥fj​∥n​} has P{Bc}≤M1−A2/2\mathbb P\{\mathcal B^c\}\le M^{1-A^2/2}P{Bc}≤M1−A2/2 (proof of Lemma B.3).
  2. Lemma B.3, (B.9): for any β\betaβ satisfying the Dantzig constraint, δ=β^D−β\delta=\hat\beta_D-\betaδ=β^​D​−β satisfies the cone condition at J(β)J(\beta)J(β) with c0=1c_0=1c0​=1.
  3. (B.25): on B\mathcal BB, β∗∈Λ\beta^*\in\Lambdaβ∗∈Λ, 1n∣XTXδ∣∞≤2r\frac1n|X^TX\delta|_\infty\le2rn1​∣XTXδ∣∞​≤2r, and 1n∣Xδ∣22≤4rs ∣δJ0∣2\frac1n|X\delta|_2^2\le4r\sqrt s\,|\delta_{J_0}|_2n1​∣Xδ∣22​≤4rs​∣δJ0​​∣2​.
  4. (B.26): under RE(s,1)(s,1)(s,1), 1n∣Xδ∣22≤16r2s/κ2\frac1n|X\delta|_2^2\le16r^2s/\kappa^2n1​∣Xδ∣22​≤16r2s/κ2 and ∣δJ0∣2≤4rs/κ2|\delta_{J_0}|_2\le4r\sqrt s/\kappa^2∣δJ0​​∣2​≤4rs​/κ2.
  5. (B.27): on the cone, ∣δ∣1≤(1+c0)s ∣δJ0∣2|\delta|_1\le(1+c_0)\sqrt s\,|\delta_{J_0}|_2∣δ∣1​≤(1+c0​)s​∣δJ0​​∣2​.
  6. (B.28): on the cone, ∣δ∣2≤(1+c0s/m) ∣δJ01∣2|\delta|_2\le(1+c_0\sqrt{s/m})\,|\delta_{J_{01}}|_2∣δ∣2​≤(1+c0​s/m​)∣δJ01​​∣2​.
  7. (B.29): under RE(s,m,1)(s,m,1)(s,m,1), ∣δ∣22≤16(1+s/m)2(rs/κ2)2|\delta|_2^2\le16(1+\sqrt{s/m})^2(r\sqrt s/\kappa^2)^2∣δ∣22​≤16(1+s/m​)2(rs​/κ2)2.
  8. Interpolation: ∑jaj≤b1\sum_ja_j\le b_1∑j​aj​≤b1​, ∑jaj2≤b2\sum_ja_j^2\le b_2∑j​aj2​≤b2​, aj≥0a_j\ge0aj​≥0 imply ∑jajp≤b12−pb2p−1\sum_ja_j^p\le b_1^{2-p}b_2^{p-1}∑j​ajp​≤b12−p​b2p−1​ for 1<p≤21<p\le21<p≤2.

Significance

The result. Theorem 7.1 shows that, up to the factor log⁡M\log MlogM, the Dantzig selector estimates an sss-sparse vector as well as least squares would if the support were known: the prediction error 1n∣X(β^D−β∗)∣22\frac1n|X(\hat\beta_D-\beta^*)|_2^2n1​∣X(β^​D​−β∗)∣22​ is of order σ2slog⁡M/n\sigma^2s\log M/nσ2slogM/n, and the ℓp\ell_pℓp​ errors are of order s1/pσlog⁡M/ns^{1/p}\sigma\sqrt{\log M/n}s1/pσlogM/n​. The bounds hold for any MMM, including M≫nM\gg nM≫n, provided only that RE holds, and every constant is explicit. The paper's Theorem 7.2 gives the same rates for the Lasso; comparing the two is the paper's main message.

Formalizing it. The theorem is proved in the paper; to the best of current knowledge it has not been machine-checked. A complete formal proof would provide: a verified Gaussian maximal inequality for the noise event, the deterministic cone and RE arithmetic that underlies essentially all ℓ1\ell_1ℓ1​-regularized estimation theory, and a reusable ℓ1\ell_1ℓ1​–ℓ2\ell_2ℓ2​ interpolation lemma. Most milestones are deterministic and independent of the probability layer.

Difficulty

The obvious argument — compare β^D\hat\beta_Dβ^​D​ with β∗\beta^*β∗ in Euclidean norm using the smallest eigenvalue of XTX/nX^TX/nXTX/n — fails because that eigenvalue is 0 whenever M>nM>nM>n. The proof must instead show that the error vector lies in a cone on which XXX is injective in a quantitative sense, and this uses the optimality of β^D\hat\beta_Dβ^​D​ (not just feasibility) together with the event B\mathcal BB on which β∗\beta^*β∗ itself is feasible. The ℓp\ell_pℓp​ bound needs a second, stronger condition RE(s,m,1)(s,m,1)(s,m,1) and a control of the tail of the error outside the mmm largest coordinates. On the formal side, handling the non-uniqueness of the minimizer, real powers with exponent p−1p-1p−1 or 2−p2-p2−p, and the union over MMM Gaussian tails with the exact constant M1−A2/2M^{1-A^2/2}M1−A2/2 all need care.

Formalization scope

Vectors are functions Fin M → ℝ, the design is Matrix (Fin n) (Fin M) ℝ; the paper's dictionary of functions enters only through XXX. The unit diagonal of XTX/nX^TX/nXTX/n is a hypothesis, not a normalization performed in the proof. The noise is W : Fin n → Ω → ℝ on a probability space, measurable, mutually independent, each of law N(0,σ2)\mathcal N(0,\sigma^2)N(0,σ2); log⁡\loglog is the natural logarithm. The Dantzig selector is a predicate (feasible and of minimal ℓ1\ell_1ℓ1​ norm among feasible vectors), and every result is stated for every minimizer. RE(s,c0)(s,c_0)(s,c0​) and RE(s,m,c0)(s,m,c_0)(s,m,c0​) are stated through a witness κ\kappaκ (a number with the defining lower-bound property); κ(s,c0)\kappa(s,c_0)κ(s,c0​) is the largest witness and the bounds decrease in κ\kappaκ, so the statements are equivalent to the paper's while avoiding the value of a real infimum over an empty set. Two witnesses are kept apart: κ\kappaκ for RE(s,1)(s,1)(s,1) in (7.4)–(7.5), κ′\kappa'κ′ for RE(s,m,1)(s,m,1)(s,m,1) in (7.6). Ties in the choice of the mmm largest coordinates are handled by quantifying over every admissible J1J_1J1​. The probability statement asserts one measurable event EEE with P(E)≥1−M1−A2/2\mathbb P(E)\ge1-M^{1-A^2/2}P(E)≥1−M1−A2/2 on which all three bounds hold for every minimizer, every admissible mmm, every witness κ′\kappa'κ′ and every ppp.

The event EEE is fixed before the minimizer is quantified, so a formalization in which the event depends on β^D\hat\beta_Dβ^​D​, or in which RE is a hypothesis about the random error vector rather than the design, would be a different (weaker) statement and is not accepted. The deterministic milestones (B.26)–(B.29) take the conclusion of (B.25) as a hypothesis; they are true for every vector satisfying their hypotheses and are not restricted to the event.

A complete development needs Gaussian tail bounds and a union bound (Mathlib's gaussianReal), finite Hölder-type inequalities for real exponents, and elementary sorting arguments for the tail outside J01J_{01}J01​. The cone, RE and interpolation lemmas are reusable for the Lasso (Theorem 7.2, a sister mission) and beyond. Proofs of any milestone are welcome independently.

Selected references

  • P. J. Bickel, Y. Ritov, A. B. Tsybakov, Simultaneous analysis of Lasso and Dantzig selector, Ann. Statist. 37(4), 1705–1732, 2009. arXiv:0801.1095v3: https://arxiv.org/abs/0801.1095
  • E. Candès, T. Tao, The Dantzig selector: statistical estimation when p is much larger than n, Ann. Statist. 35(6), 2313–2351, 2007. https://doi.org/10.1214/009053606000001523
  • R. Tibshirani, Regression shrinkage and selection via the lasso, J. R. Stat. Soc. B 58(1), 267–288, 1996. https://doi.org/10.1111/j.2517-6161.1996.tb02080.x
  • S. van de Geer, P. Bühlmann, On the conditions used to prove oracle results for the Lasso, Electron. J. Statist. 3, 1360–1392, 2009. https://doi.org/10.1214/09-EJS506
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Simultaneous Analysis of Lasso and Dantzig Selector II: Approximate Equivalence of the Lasso and Dantzig Prediction LossesResearch Paper

Motivation

Two estimators dominate sparse high-dimensional regression, where the number MMM of candidate regressors can far exceed the sample size nnn. The Lasso (Tibshirani, 1996) minimises a least-squares criterion plus an ℓ1\ell_1ℓ1​ penalty. The Dantzig selector (Candès and Tao, 2007) minimises the ℓ1\ell_1ℓ1​ norm of the coefficients subject to a bound on the correlation between the residual and the regressors, and is computed by a linear program. They were proposed independently and first analysed under different assumptions: sparsity oracle inequalities for the Lasso (Bunea, Tsybakov and Wegkamp, 2007) and ℓ2\ell_2ℓ2​ bounds for the Dantzig selector under a uniform uncertainty principle (Candès and Tao, 2007). A practitioner choosing between them needs to know whether guarantees for one say anything about the other.

Bickel, Ritov and Tsybakov (arXiv:0801.1095; Ann. Statist. 37(4), 2009, doi:10.1214/08-AOS620) analyse both estimators in parallel under one assumption on the design, the restricted eigenvalue condition. Their main message is that, under sparsity, the two estimators "exhibit similar behavior" (p. 2). Section 5 makes this precise: the prediction losses of the two estimators are close. The result holds in a nonparametric model: the regression function need not be a combination of the regressors. This mission formalizes that comparison, Theorem 5.1 of the paper.

Setting

Let f1,…,fMf_1,\dots,f_Mf1​,…,fM​ be real functions (the dictionary) on a set Z\mathcal ZZ, and Z1,…,Zn∈ZZ_1,\dots,Z_n\in\mathcal ZZ1​,…,Zn​∈Z fixed design points, with n≥1n\ge1n≥1 and M≥2M\ge2M≥2. The design matrix is X=(fj(Zi))∈Rn×MX=(f_j(Z_i))\in\mathbb R^{n\times M}X=(fj​(Zi​))∈Rn×M. Observations are Yi=f(Zi)+WiY_i=f(Z_i)+W_iYi​=f(Zi​)+Wi​, where fff is an unknown function and W1,…,WnW_1,\dots,W_nW1​,…,Wn​ are independent N(0,σ2)\mathcal N(0,\sigma^2)N(0,σ2) with σ>0\sigma>0σ>0. Write y=(Yi)y=(Y_i)y=(Yi​), f=(f(Zi))\boldsymbol f=(f(Z_i))f=(f(Zi​)) and w=(Wi)w=(W_i)w=(Wi​), so y=f+wy=\boldsymbol f+wy=f+w.

The empirical norm of ggg is ∥g∥n=(1n∑ig(Zi)2)1/2\|g\|_n=(\tfrac1n\sum_i g(Z_i)^2)^{1/2}∥g∥n​=(n1​∑i​g(Zi​)2)1/2. Every column has ∥fj∥n≠0\|f_j\|_n\neq0∥fj​∥n​=0, and fmax⁡=max⁡j∥fj∥nf_{\max}=\max_j\|f_j\|_nfmax​=maxj​∥fj​∥n​. For β∈RM\beta\in\mathbb R^Mβ∈RM, fβ=∑jβjfjf_\beta=\sum_j\beta_jf_jfβ​=∑j​βj​fj​ has value vector XβX\betaXβ. The support is J(β)={j:βj≠0}J(\beta)=\{j:\beta_j\ne0\}J(β)={j:βj​=0} and the sparsity is M(β)=∣J(β)∣\mathcal M(\beta)=|J(\beta)|M(β)=∣J(β)∣. For J⊆{1,…,M}J\subseteq\{1,\dots,M\}J⊆{1,…,M}, δJ\delta_JδJ​ agrees with δ\deltaδ on JJJ and vanishes elsewhere.

Fix r>0r>0r>0. The Lasso β^L\hat\beta_Lβ^​L​ is any minimiser of

1n∑i=1n(Yi−fβ(Zi))2+2r∑j=1M∥fj∥n∣βj∣.\frac1n\sum_{i=1}^n\big(Y_i-f_\beta(Z_i)\big)^2+2r\sum_{j=1}^M\|f_j\|_n|\beta_j| .n1​i=1∑n​(Yi​−fβ​(Zi​))2+2rj=1∑M​∥fj​∥n​∣βj​∣.

With D=diag(∥f1∥n2,…,∥fM∥n2)D=\mathrm{diag}(\|f_1\|_n^2,\dots,\|f_M\|_n^2)D=diag(∥f1​∥n2​,…,∥fM​∥n2​), the Dantzig constraint is ∣1nD−1/2X⊤(y−Xβ)∣∞≤r|\tfrac1nD^{-1/2}X^\top(y-X\beta)|_\infty\le r∣n1​D−1/2X⊤(y−Xβ)∣∞​≤r. The Dantzig selector β^D\hat\beta_Dβ^​D​ is any vector of smallest ∣β∣1=∑j∣βj∣|\beta|_1=\sum_j|\beta_j|∣β∣1​=∑j​∣βj​∣ that satisfies it. The estimators are f^L=fβ^L\hat f_L=f_{\hat\beta_L}f^​L​=fβ^​L​​ and f^D=fβ^D\hat f_D=f_{\hat\beta_D}f^​D​=fβ^​D​​.

Assumption RE(s,c0)(s,c_0)(s,c0​) with 1≤s≤M1\le s\le M1≤s≤M, c0>0c_0>0c0​>0 asks that

κ(s,c0)=min⁡∣J0∣≤s min⁡δ≠0, ∣δJ0c∣1≤c0∣δJ0∣1 ∣Xδ∣2n ∣δJ0∣2>0.\kappa(s,c_0)=\min_{|J_0|\le s}\ \min_{\delta\ne0,\ |\delta_{J_0^c}|_1\le c_0|\delta_{J_0}|_1}\ \frac{|X\delta|_2}{\sqrt n\,|\delta_{J_0}|_2}>0 .κ(s,c0​)=∣J0​∣≤smin​ δ=0, ∣δJ0c​​∣1​≤c0​∣δJ0​​∣1​min​ n​∣δJ0​​∣2​∣Xδ∣2​​>0.

Throughout, r=Aσlog⁡M/nr=A\sigma\sqrt{\log M/n}r=AσlogM/n​, where log⁡\loglog is the natural logarithm.

Formalization targets

Goal: Theorem 5.1

Assume RE(s,1)(s,1)(s,1) with 1≤s≤M1\le s\le M1≤s≤M, and let A>22A>2\sqrt2A>22​. With probability at least 1−M1−A2/81-M^{1-A^2/8}1−M1−A2/8, every Lasso solution with M(β^L)≤s\mathcal M(\hat\beta_L)\le sM(β^​L​)≤s and every Dantzig selector satisfy

∣ ∥f^D−f∥n2−∥f^L−f∥n2 ∣≤16A2 M(β^L)σ2n fmax⁡2κ2(s,1) log⁡M.\Big|\,\|\hat f_D-f\|_n^2-\|\hat f_L-f\|_n^2\,\Big|\le16A^2\,\frac{\mathcal M(\hat\beta_L)\sigma^2}{n}\,\frac{f_{\max}^2}{\kappa^2(s,1)}\,\log M .​∥f^​D​−f∥n2​−∥f^​L​−f∥n2​​≤16A2nM(β^​L​)σ2​κ2(s,1)fmax2​​logM.

Milestones

The proof uses one probabilistic event and two one-sided deterministic inequalities.

  1. The Lasso satisfies the Dantzig constraint (2.3).
  2. The noise event A=⋂j{2∣1n∑iXijWi∣≤r∥fj∥n}\mathcal A=\bigcap_j\{2|\tfrac1n\sum_iX_{ij}W_i|\le r\|f_j\|_n\}A=⋂j​{2∣n1​∑i​Xij​Wi​∣≤r∥fj​∥n​} has P(Ac)≤M1−A2/8\mathbb P(\mathcal A^c)\le M^{1-A^2/8}P(Ac)≤M1−A2/8 (B.4).
  3. On A\mathcal AA, ∣1nX⊤(f−Xβ^L)∣∞≤3rfmax⁡/2|\tfrac1nX^\top(\boldsymbol f-X\hat\beta_L)|_\infty\le 3rf_{\max}/2∣n1​X⊤(f−Xβ^​L​)∣∞​≤3rfmax​/2 (Lemma B.1, (B.2)).
  4. The Dantzig error lies in the cone ∣δJ0c∣1≤∣δJ0∣1|\delta_{J_0^c}|_1\le|\delta_{J_0}|_1∣δJ0c​​∣1​≤∣δJ0​​∣1​ (Lemma B.3, (B.9)).
  5. On the larger event B⊇A\mathcal B\supseteq\mathcal AB⊇A, ∣1nX⊤(f−Xβ^D)∣∞≤2rfmax⁡|\tfrac1nX^\top(\boldsymbol f-X\hat\beta_D)|_\infty\le 2rf_{\max}∣n1​X⊤(f−Xβ^​D​)∣∞​≤2rfmax​ (Lemma B.3, (B.10)).
  6. ∥f^D−f∥n2≤∥f^L−f∥n2+16fmax⁡2r2M(β^L)/κ2\|\hat f_D-f\|_n^2\le\|\hat f_L-f\|_n^2+16f_{\max}^2r^2\mathcal M(\hat\beta_L)/\kappa^2∥f^​D​−f∥n2​≤∥f^​L​−f∥n2​+16fmax2​r2M(β^​L​)/κ2 on B\mathcal BB (B.15).
  7. ∥f^L−f∥n2≤∥f^D−f∥n2+9fmax⁡2r2M(β^L)/κ2\|\hat f_L-f\|_n^2\le\|\hat f_D-f\|_n^2+9f_{\max}^2r^2\mathcal M(\hat\beta_L)/\kappa^2∥f^​L​−f∥n2​≤∥f^​D​−f∥n2​+9fmax2​r2M(β^​L​)/κ2 on A\mathcal AA (B.17).

Further result: Theorem 5.2

Assume ∥fj∥n=1\|f_j\|_n=1∥fj​∥n​=1 for all jjj and RE(s,5)(s,5)(s,5). With probability at least 1−M1−A2/81-M^{1-A^2/8}1−M1−A2/8, whenever M(β^D)≤s\mathcal M(\hat\beta_D)\le sM(β^​D​)≤s,

∥f^L−f∥n2≤10∥f^D−f∥n2+81A2 M(β^D)σ2n log⁡Mκ2(s,5).\|\hat f_L-f\|_n^2\le10\|\hat f_D-f\|_n^2+81A^2\,\frac{\mathcal M(\hat\beta_D)\sigma^2}{n}\,\frac{\log M}{\kappa^2(s,5)} .∥f^​L​−f∥n2​≤10∥f^​D​−f∥n2​+81A2nM(β^​D​)σ2​κ2(s,5)logM​.

Significance

The result. Theorem 5.1 bounds the gap between the two prediction losses by the rate M(β^L)σ2log⁡M/n\mathcal M(\hat\beta_L)\sigma^2\log M/nM(β^​L​)σ2logM/n of a sparse regression with M(β^L)\mathcal M(\hat\beta_L)M(β^​L​) parameters. The bound carries a factor fmax⁡2/κ2(s,1)f^2_{\max}/\kappa^2(s,1)fmax2​/κ2(s,1) that measures how ill-conditioned the Gram matrix is on sparse vectors. A prediction bound for one estimator therefore transfers to the other at this cost. The paper uses this transfer in Proposition 6.3, which combines Theorem 5.1 with the Lasso oracle inequality of Section 6 to derive an oracle inequality for the Dantzig selector. The theorem requires no assumption relating fff to the dictionary.

Formalizing it. The result has been proved since 2009, and this mission formalizes that proof. None of the objects involved exists on Prove2Me yet: the weighted Lasso, the Dantzig selector and the Gaussian noise events. The Wainwright series on the platform defines a differently normalised Lasso with an unweighted penalty, a single fixed support and a different restricted eigenvalue condition, so it cannot be reused here. A machine-checked proof would also confirm the paper's constants, 16A216A^216A2 and the thresholds 222\sqrt222​ and M1−A2/8M^{1-A^2/8}M1−A2/8, which appear in all later analyses.

Difficulty

Each estimator is defined only implicitly, as the solution of an optimisation problem, and neither need be unique. Comparing their losses directly gives ±2nδ⊤X⊤(f−Xβ^)\pm\tfrac2n\delta^\top X^\top(\boldsymbol f-X\hat\beta)±n2​δ⊤X⊤(f−Xβ^​) plus 1n∣Xδ∣22\tfrac1n|X\delta|_2^2n1​∣Xδ∣22​ with δ=β^L−β^D\delta=\hat\beta_L-\hat\beta_Dδ=β^​L​−β^​D​. A crude bound on the cross term, ∣δ∣1⋅∣X⊤(⋅)∣∞|\delta|_1\cdot|X^\top(\cdot)|_\infty∣δ∣1​⋅∣X⊤(⋅)∣∞​, yields an error proportional to ∣δ∣1|\delta|_1∣δ∣1​. This does not produce the sparse rate unless ∣δ∣1|\delta|_1∣δ∣1​ is controlled by ∣Xδ∣2|X\delta|_2∣Xδ∣2​. That control needs δ\deltaδ to lie in the restricted eigenvalue cone at the support of the random, data-dependent vector β^L\hat\beta_Lβ^​L​. The restricted eigenvalue condition must therefore hold uniformly over supports of size at most sss; a condition for one fixed support does not suffice. The probabilistic part is a union bound over MMM Gaussian coordinates, and it must be arranged so that a single event serves every minimiser of both programs.

Formalization scope

The dictionary and the design points enter every statement only through XXX and f\boldsymbol ff, so the Lean statements take X : Matrix (Fin n) (Fin M) ℝ and f : Fin n → ℝ directly, and fff is arbitrary. The noise is a family W : Fin n → Ω → ℝ of measurable, mutually independent random variables with law gaussianReal 0 σ², and y=f+W(ω)y=f+W(\omega)y=f+W(ω). The Lasso and the Dantzig selector are predicates (IsLasso, IsDantzig), and every theorem is stated for every solution. The Dantzig constraint is written coordinatewise as ∣1n∑iXij(yi−(Xβ)i)∣≤r∥fj∥n|\tfrac1n\sum_iX_{ij}(y_i-(X\beta)_i)|\le r\|f_j\|_n∣n1​∑i​Xij​(yi​−(Xβ)i​)∣≤r∥fj​∥n​. The Lasso penalty and the Dantzig constraint are weighted by ∥fj∥n\|f_j\|_n∥fj​∥n​, and the Dantzig objective ∣β∣1|\beta|_1∣β∣1​ is unweighted, exactly as in the paper. Theorem 5.1 does not normalise the columns.

RE(s,c0)(s,c_0)(s,c0​) is stated through a witness: a real κ>0\kappa>0κ>0 with κn∣δJ0∣2≤∣Xδ∣2\kappa\sqrt n|\delta_{J_0}|_2\le|X\delta|_2κn​∣δJ0​​∣2​≤∣Xδ∣2​ on the cone, for all ∣J0∣≤s|J_0|\le s∣J0​∣≤s. The paper's κ(s,c0)\kappa(s,c_0)κ(s,c0​) is attained, so it is the largest witness. Every bound decreases in κ\kappaκ, so this reading is equivalent to the paper's and avoids a real infimum over an empty set. "With probability at least ppp" becomes the existence of a measurable event EEE with P(E)≥p\mathbb P(E)\ge pP(E)≥p on which the conclusion holds for every Lasso solution and every Dantzig selector. The condition M(β^L)≤s\mathcal M(\hat\beta_L)\le sM(β^​L​)≤s is imposed inside the event, per realisation. The milestones (B.2), (B.10), (B.15) and (B.17) are stated deterministically, on the noise events A\mathcal AA and B\mathcal BB as predicates on the noise vector; this is how the proof uses them. (B.4) is stated for every A>0A>0A>0, which is stronger than the paper's A>22A>2\sqrt2A>22​ and still true.

The goal cannot be made vacuous. For A>22A>2\sqrt2A>22​ the probability bound 1−M1−A2/81-M^{1-A^2/8}1−M1−A2/8 is positive. Lasso solutions exist because r>0r>0r>0 and every ∥fj∥n>0\|f_j\|_n>0∥fj​∥n​>0, and Dantzig selectors exist because the Lasso is feasible. RE(s,1)(s,1)(s,1) with κ=1\kappa=1κ=1 holds for X=n IX=\sqrt n\,IX=n​I.

A complete development needs:

  • subgradient optimality for the weighted Lasso;
  • a Gaussian tail bound P(∣η∣≥t)≤e−t2/2\mathbb P(|\eta|\ge t)\le e^{-t^2/2}P(∣η∣≥t)≤e−t2/2 together with the law of a weighted sum of independent Gaussians;
  • Cauchy–Schwarz on supports;
  • the quadratic bound bx−x2≤b2/4bx-x^2\le b^2/4bx−x2≤b2/4.

The noise-event lemmas and the Lasso optimality condition can be reused by the companion missions on this paper. Proofs of any milestone are welcome, including proofs that route (B.4) through Mathlib's sub-Gaussian API.

Selected references

  • P. J. Bickel, Y. Ritov, A. B. Tsybakov, Simultaneous analysis of Lasso and Dantzig selector, Ann. Statist. 37(4), 1705–1732, 2009. arXiv:0801.1095v3: https://arxiv.org/abs/0801.1095 ; doi:10.1214/08-AOS620
  • E. Candès, T. Tao, The Dantzig selector: statistical estimation when p is much larger than n, Ann. Statist. 35(6), 2313–2351, 2007. https://doi.org/10.1214/009053606000001523
  • R. Tibshirani, Regression shrinkage and selection via the lasso, J. R. Stat. Soc. B 58(1), 267–288, 1996. https://doi.org/10.1111/j.2517-6161.1996.tb02080.x
  • F. Bunea, A. B. Tsybakov, M. H. Wegkamp, Sparsity oracle inequalities for the Lasso, Electron. J. Stat. 1, 169–194, 2007. https://doi.org/10.1214/07-EJS008
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An Analysis of Several Heuristics for the Traveling Salesman Problem I: Nearest Neighbor Tours Can Be Far from OptimalResearch Paper

Motivation

The traveling salesman problem with the triangle inequality asks for a shortest closed tour through nnn points whose distances form a metric. It is NP-hard, so in practice tours are built by fast construction heuristics, and the natural question is how far such a tour can be from optimal in the worst case. Rosenkrantz, Stearns and Lewis (SIAM J. Comput. 6(3), 1977) gave the first systematic worst-case analysis of the standard heuristics. Their results are reproduced in textbooks on approximation algorithms and combinatorial optimization, and they are the reference point against which later guarantees (Christofides' 3/23/23/2 algorithm, the double-tree 222-approximation) are compared.

The simplest heuristic studied is the nearest neighbor algorithm (Bellmore and Nemhauser, 1968; the "next best method" of Gavett, 1965): from the current node, always move to the closest node not yet visited, and return to the start at the end. The paper shows that this greedy rule is never worse than logarithmic (Theorem 1) and that the logarithm cannot be removed (Theorem 2). This mission is about Theorem 2, the lower bound.

Setting

A traveling salesman graph on nnn nodes is a complete graph with a distance d(a,b)∈Rd(a,b)\in\mathbb Rd(a,b)∈R that is symmetric, d(a,b)=d(b,a)d(a,b)=d(b,a)d(a,b)=d(b,a), nonnegative, d(a,b)≥0d(a,b)\ge 0d(a,b)≥0, and satisfies the triangle inequality d(a,c)≤d(a,b)+d(b,c)d(a,c)\le d(a,b)+d(b,c)d(a,c)≤d(a,b)+d(b,c). A tour lists the nodes in a visiting order τ(0),…,τ(n−1)\tau(0),\dots,\tau(n-1)τ(0),…,τ(n−1) and returns to τ(0)\tau(0)τ(0); its length is the sum of the nnn distances along it. OPTIMAL is the least length of a tour.

The nearest neighbor algorithm starts at an arbitrary node τ(0)\tau(0)τ(0); having reached τ(k)\tau(k)τ(k), it moves to a node τ(k+1)\tau(k+1)τ(k+1) that minimizes d(τ(k),⋅)d(\tau(k),\cdot)d(τ(k),⋅) over the nodes not yet visited, breaking ties arbitrarily; after the last node it returns to τ(0)\tau(0)τ(0). The length of the resulting tour is written NEARNEIBER. Because the start node and the ties are free, one instance has in general several nearest-neighbor tours. A lower bound needs only one of them; an upper bound must hold for all.

The instances of the proof are built from a recursive family of weighted graphs. With li=16(4⋅2i−(−1)i+3)l_i=\frac16(4\cdot 2^i-(-1)^i+3)li​=61​(4⋅2i−(−1)i+3) (so l1,l2,l3,l4=2,3,6,11l_1,l_2,l_3,l_4=2,3,6,11l1​,l2​,l3​,l4​=2,3,6,11), the graph F1F_1F1​ is a triangle with unit weights, and Fi+1F_{i+1}Fi+1​ consists of two copies of FiF_iFi​ joined through one new node by two edges of length 111 and two edges of length lil_ili​. Each FiF_iFi​ has 2i+1−12^{i+1}-12i+1−1 nodes and a path PiP_iPi​ from its start node to its middle node through every node, of length LiL_iLi​ with L1=2L_1=2L1​=2, Li+1=2Li+2liL_{i+1}=2L_i+2l_iLi+1​=2Li​+2li​. The graph GiG_iGi​ adds two closing edges to FiF_iFi​, and Gˉi\bar G_iGˉi​ is the complete graph on the same nodes whose distance is the shortest-path distance of GiG_iGi​.

Formalization targets

Goal: Theorem 2 (p. 566)

For each m>3m>3m>3 there is a traveling salesman graph with n=2m−1n=2^m-1n=2m−1 nodes and a nearest-neighbor tour on it such that

NEARNEIBEROPTIMAL>13lg⁡(n+1)+49.\frac{\mathrm{NEARNEIBER}}{\mathrm{OPTIMAL}}>\frac13\lg(n+1)+\frac49 .OPTIMALNEARNEIBER​>31​lg(n+1)+94​.

The statement is existential in both the instance and the run of the algorithm, exactly as in the paper.

Milestones, in the order the proof uses them

  1. (2.12): the difference equation Li+1=2Li+2liL_{i+1}=2L_i+2l_iLi+1​=2Li​+2li​, L1=2L_1=2L1​=2, has the solution Li=19(6 i 2i+8⋅2i+(−1)i−9)L_i=\frac19(6\,i\,2^i+8\cdot2^i+(-1)^i-9)Li​=91​(6i2i+8⋅2i+(−1)i−9).
  2. Gˉi\bar G_iGˉi​ is a traveling salesman graph: the shortest-path distance of GiG_iGi​ is symmetric, nonnegative and satisfies the triangle inequality.
  3. (2.13)–(2.17): the shortest-path distances in Fi+1F_{i+1}Fi+1​ between the seven named nodes A,…,GA,\dots,GA,…,G of Fig. 1, e.g. AG‾=li+2−2\overline{AG}=l_{i+2}-2AG=li+2​−2.
  4. Property a): every edge of GiG_iGi​ is a shortest path between its endpoints.
  5. Property b): the nearest neighbor algorithm started at the start node of Gˉi\bar G_iGˉi​ can follow PiP_iPi​ and return along the edge of length li−1l_i-1li​−1.
  6. The optimal tour: OPTIMAL(Gˉi)=2i+1−1\mathrm{OPTIMAL}(\bar G_i)=2^{i+1}-1OPTIMAL(Gˉi​)=2i+1−1.
  7. The exact ratio: the tour along PiP_iPi​ has length Li+li−1L_i+l_i-1Li​+li​−1, so its ratio is (Li+li−1)/n(L_i+l_i-1)/n(Li​+li​−1)/n.
  8. The inequality: (Li+li−1)/n>13lg⁡(n+1)+49(L_i+l_i-1)/n>\frac13\lg(n+1)+\frac49(Li​+li​−1)/n>31​lg(n+1)+94​ for i≥3i\ge3i≥3.

The instance for mmm is Gˉm−1\bar G_{m-1}Gˉm−1​.

Significance

Theorem 1 of the same paper shows NEARNEIBER/OPTIMAL≤12⌈lg⁡n⌉+12\mathrm{NEARNEIBER}/\mathrm{OPTIMAL}\le\frac12\lceil\lg n\rceil+\frac12NEARNEIBER/OPTIMAL≤21​⌈lgn⌉+21​ for every nearest-neighbor tour on every traveling salesman graph. Theorem 2 shows that this bound has the right order: no constant-factor guarantee holds for the nearest neighbor rule, and the gap between the two constants (13\frac1331​ against 12\frac1221​) is all that remains. This separates the nearest neighbor rule from the insertion rules analysed later in the same paper, of which nearest and cheapest insertion are within a factor 222 of optimal. It is the standard example of a natural greedy heuristic whose approximation ratio grows with nnn.

The upper bound, Theorem 1, is already on Prove2Me with a machine-checked proof (SupplyChainTheory.nearest_neighbor_bound); its statement notes that the lower-bound instances are not formalized there. This mission supplies them: an explicit recursive family of metric instances, the shortest-path computations that certify it, and the arithmetic of its ratio. The result is proved in the paper; to our knowledge it has not been formalized in any proof assistant. The construction (a recursively defined weighted graph with a closed-form shortest-path table) is also a reusable pattern for other worst-case lower bounds of greedy heuristics.

Difficulty

The arithmetic ((2.12) and the final inequality) is routine. The content is in properties a) and b). A shortest-path distance is an infimum over all walks, and property a) asks that no detour through the recursive structure is shorter than the direct edge, at every level of the recursion. The paper handles this by an induction on (2.13)–(2.17) that tracks only seven nodes per level, and argues that distances inside a copy of FiF_iFi​ are not shortened by embedding it into Fi+1F_{i+1}Fi+1​. Property b) then needs that at each step of PiP_iPi​ the chosen node is at least as close as every unvisited node, including nodes in the other copy and nodes reached through the start or right nodes; ties occur, and the claim is only that some resolution of them follows PiP_iPi​. Checking small cases by computer does not give either property for all iii.

Formalization scope

Nodes of an instance are Fin n, a tour is a permutation of Fin n, the tour length is the sum over consecutive pairs including the closing edge, and OPTIMAL is a minimum over the finite set of permutations. The model is the paper's: symmetric, nonnegative distances with the triangle inequality. The distance structure also carries d(a,a)=0d(a,a)=0d(a,a)=0, a normalization not in the paper; the diagonal never enters a tour length. A nearest-neighbor tour is a permutation in which each step goes to a node at least as close as every unvisited node, from an arbitrary start with arbitrary ties.

Ratios are multiplied out: the goal is (13log⁡2(n+1)+49)⋅OPTIMAL<NEARNEIBER(\frac13\log_2(n+1)+\frac49)\cdot\mathrm{OPTIMAL}<\mathrm{NEARNEIBER}(31​log2​(n+1)+94​)⋅OPTIMAL<NEARNEIBER together with OPTIMAL>0\mathrm{OPTIMAL}>0OPTIMAL>0, the paper's standing assumption (1.1). lg⁡(n+1)\lg(n+1)lg(n+1) is Real.logb 2 of n+1n+1n+1, as printed. Because of the strict inequality and the conjunct OPTIMAL>0\mathrm{OPTIMAL}>0OPTIMAL>0, the all-zero distance does not satisfy the goal, so the statement cannot be met by a degenerate instance.

In the construction the nodes of FiF_iFi​, GiG_iGi​, Gˉi\bar G_iGˉi​ are numbered 0,…,2i+1−20,\dots,2^{i+1}-20,…,2i+1−2 from left to right (start node 000, middle node 2i−12^i-12i−1, right node 2i+1−22^{i+1}-22i+1−2); in Fi+1F_{i+1}Fi+1​ the left copy comes first, then the new node, then the right copy. Graphs are edge lists with real weights and lil_ili​ is defined in R\mathbb RR exactly as in (2.11). The shortest-path distance is the infimum of walk weights over an inductive walk predicate; it would be 000 for two nodes with no connecting walk, a case that does not arise because every GiG_iGi​ and FiF_iFi​ is connected. LiL_iLi​ is defined by its difference equation; its identification with the length of the tour along PiP_iPi​ is milestone 7. All construction statements assume i≥1i\ge1i≥1.

A complete development needs a small library for shortest-path distances of finite weighted edge lists (symmetry, triangle inequality, attainment, behaviour under relabelling and under gluing two graphs at a few nodes); this part is reusable beyond the mission. Contributions welcome: proofs of any milestone, and such general shortest-path lemmas as separate theorems. Theorem 1 is not part of this mission.

Selected references

  • D. J. Rosenkrantz, R. E. Stearns, P. M. Lewis II, An Analysis of Several Heuristics for the Traveling Salesman Problem, SIAM J. Comput. 6(3):563–581, 1977. https://doi.org/10.1137/0206041
  • M. Bellmore, G. L. Nemhauser, The Traveling Salesman Problem: A Survey, Operations Research 16(3):538–558, 1968. https://doi.org/10.1287/opre.16.3.538
  • J. W. Gavett, Three Heuristic Rules for Sequencing Jobs to a Single Production Facility, Management Science 11(8):B166–B176, 1965. https://doi.org/10.1287/mnsc.11.8.B166
  • N. Christofides, Worst-Case Analysis of a New Heuristic for the Travelling Salesman Problem, Report 388, Graduate School of Industrial Administration, Carnegie Mellon University, 1976.
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CombinatoricsOperations ResearchOptimization+1·Captain: mikedeng1

Worst-Case Performance Bounds for Simple One-Dimensional Packing Algorithms 2: First-Fit and Best-Fit with Bounded Item SizesResearch Paper

Motivation

Bin packing asks for the fewest unit-capacity bins that hold a given list of item sizes. It models cutting stock, memory allocation, file placement and the loading of trucks, and it is NP-hard, so in practice lists are packed by simple rules that look at one item at a time. The two most widely used rules are First-Fit and Best-Fit, and the question that Johnson, Demers, Ullman, Garey and Graham answered in 1974 is how far from optimal they can be in the worst case.

Their headline answer is that both rules use at most about 1710\tfrac{17}{10}1017​ times the optimal number of bins, and that 1710\tfrac{17}{10}1017​ is asymptotically attained. The lists that force this ratio use items larger than 12\tfrac1221​. When all items are known to be small, which is typical of memory and storage applications, the guarantee is much better, and this mission is about that refinement: the paper's Theorem 2.3 and its corollary, which determine the asymptotic worst-case ratio of First-Fit and Best-Fit exactly as a function of the largest allowed item size α≤12\alpha\le\tfrac12α≤21​.

Timeline. Ullman (1971) introduced the worst-case analysis of First-Fit with a 1710L∗+3\tfrac{17}{10}L^*+31017​L∗+3 bound. Garey, Graham and Ullman (1972) and Johnson's thesis (MIT, 1973) extended it to Best-Fit and to the decreasing variants. The 1974 SIAM paper collects these results; Theorem 2.3 there is the parametric bound for items of size at most α\alphaα. The additive constants in the unrestricted 1710\tfrac{17}{10}1017​ bound were sharpened over the following four decades, culminating in Dósa and Sgall's proof (2013) that FF(L)≤⌊1710L∗⌋FF(L)\le\lfloor\tfrac{17}{10}L^*\rfloorFF(L)≤⌊1017​L∗⌋.

Setting

A list is a finite sequence L=(a1,…,an)L=(a_1,\dots,a_n)L=(a1​,…,an​) of real numbers in (0,1](0,1](0,1]. Its optimum L∗L^*L∗ is the least number of bins into which the elements of LLL can be placed so that no bin contains numbers whose sum exceeds 111. The level of a bin is the sum of the numbers in it. For a real α>0\alpha>0α>0, write L⊆(0,α]L\subseteq(0,\alpha]L⊆(0,α] when every element of LLL is at most α\alphaα.

First-Fit (FFFFFF) considers bins B1,B2,…B_1,B_2,\dotsB1​,B2​,…, all initially empty, and places a1,a2,…,ana_1,a_2,\dots,a_na1​,a2​,…,an​ in that order: aia_iai​ goes into the bin BjB_jBj​ of least index whose level β\betaβ satisfies β≤1−ai\beta\le 1-a_iβ≤1−ai​. Best-Fit (BFBFBF) is the same except that, among the bins with β≤1−ai\beta\le 1-a_iβ≤1−ai​, it chooses one of largest level β\betaβ (least index among ties). FF(L)FF(L)FF(L) and BF(L)BF(L)BF(L) denote the numbers of nonempty bins at the end.

The restricted worst-case ratios are

RFFα(k)=max⁡{FF(L)L∗:L⊆(0,α], L∗=k},RBFα(k)=max⁡{BF(L)L∗:L⊆(0,α], L∗=k}.R^\alpha_{FF}(k)=\max\Big\{\frac{FF(L)}{L^*}: L\subseteq(0,\alpha],\ L^*=k\Big\},\qquad R^\alpha_{BF}(k)=\max\Big\{\frac{BF(L)}{L^*}: L\subseteq(0,\alpha],\ L^*=k\Big\}.RFFα​(k)=max{L∗FF(L)​:L⊆(0,α], L∗=k},RBFα​(k)=max{L∗BF(L)​:L⊆(0,α], L∗=k}.

Throughout, 0<α≤120<\alpha\le\tfrac120<α≤21​ and m=⌊α−1⌋m=\lfloor\alpha^{-1}\rfloorm=⌊α−1⌋, an integer with m≥2m\ge 2m≥2 and 1m+1<α≤1m\tfrac1{m+1}<\alpha\le\tfrac1mm+11​<α≤m1​.

Formalization targets

Goal: the asymptotic ratio (Corollary of Theorem 2.3, p. 308)

lim⁡k→∞RFFα(k)=lim⁡k→∞RBFα(k)=1+1⌊α−1⌋.\lim_{k\to\infty}R^\alpha_{FF}(k)=\lim_{k\to\infty}R^\alpha_{BF}(k)=1+\frac{1}{\lfloor\alpha^{-1}\rfloor}.k→∞lim​RFFα​(k)=k→∞lim​RBFα​(k)=1+⌊α−1⌋1​.

The goal is stated as a limit, which is the stable form of the result: it is unaffected by any improvement of the additive constants below.

Theorem 2.3(i): the lower bound (p. 307)

For each k≥1k\ge1k≥1 there is a list L⊆(0,α]L\subseteq(0,\alpha]L⊆(0,α] with L∗=kL^*=kL∗=k and FF(L)≥m+1mL∗−1mFF(L)\ge\frac{m+1}{m}L^*-\frac1mFF(L)≥mm+1​L∗−m1​; likewise for BFBFBF.

Two steps of the First-Fit upper bound (p. 308)

If no element of LLL exceeds 1m\frac1mm1​, then in the First-Fit packing every bin except possibly the last contains at least mmm elements, and all but at most two bins have level at least mm+1\frac{m}{m+1}m+1m​.

Theorem 2.3(ii): the upper bounds (p. 307)

For every list L⊆(0,α]L\subseteq(0,\alpha]L⊆(0,α],

FF(L)≤m+1mL∗+2,BF(L)≤m+1mL∗+2.FF(L)\le\frac{m+1}{m}L^*+2,\qquad BF(L)\le\frac{m+1}{m}L^*+2.FF(L)≤mm+1​L∗+2,BF(L)≤mm+1​L∗+2.

Significance

The theorem gives an exact, parametric description of how the worst case of the two greedy rules improves as items shrink: the asymptotic ratio is 32\tfrac3223​ when items are at most 12\tfrac1221​, 43\tfrac4334​ when at most 13\tfrac1331​, and tends to 111 as the maximum item size tends to 000. Combined with the 1710\tfrac{17}{10}1017​ bound for unrestricted lists, it shows that the bad behaviour of First-Fit is caused entirely by items larger than 12\tfrac1221​. Such parametric bounds are the standard way bin-packing heuristics are compared in the literature on online and semi-online packing, and the construction in part (i) is a reusable template for lower-bound lists.

The paper proves the First-Fit upper bound and the lower bound (the verification of the lower-bound construction is left to the reader). The Best-Fit upper bound is stated but not proved: the paper says only that "a similar, but slightly more complicated, argument can be used". A formal proof of the goal therefore requires supplying that argument. None of these results is known to have a machine-checked proof; Mathlib contains no bin-packing development.

Difficulty

For First-Fit the upper bound is a counting argument, but it rests on a property of the run, not of the final packing: an item that went into a later bin did not fit into an earlier bin at the moment it was placed. Turning that into a statement about the final levels requires an invariant maintained through the whole sequence of placements.

The Best-Fit upper bound is harder because that property fails: Best-Fit may put a small item into a fuller, later bin while an earlier, lighter bin still has room, so a light early bin and a light later bin can coexist longer than under First-Fit. The paper gives no argument for this case.

The lower bound requires computing the exact behaviour of both algorithms on a specific interleaved list with item sizes perturbed by powers of mmm, and computing L∗L^*L∗ exactly for that list, which needs a matching lower bound on the optimum.

Formalization scope

A list is L : List ℝ with the hypothesis IsList L (every element in (0,1](0,1](0,1]); L⊆(0,α]L\subseteq(0,\alpha]L⊆(0,α] is the additional hypothesis ∀ a ∈ L, a ≤ α. L∗L^*L∗ is optBins L, a sInf in ℕ over numbers of bins admitting a feasible assignment; the hypothesis IsList makes the set nonempty. The runs ffPack L and bfPack L are folds over the list that keep the nonempty bins in the order they were opened, each with its contents; an item that fits nowhere opens a new bin at the end, which is the paper's "least jjj" over infinitely many empty bins. Comparisons are exact (classical decidability on ℝ), and FF(L)FF(L)FF(L), BF(L)BF(L)BF(L) are the lengths of the final bin lists. mmm is Nat.floor α⁻¹, cast before any division.

The ratios RFFα(k)R^\alpha_{FF}(k)RFFα​(k), RBFα(k)R^\alpha_{BF}(k)RBFα​(k) are suprema taken in ℝ≥0∞: an unbounded family would give +∞+\infty+∞, never a default value, and at k=0k=0k=0 the only admissible list is empty and the value is 000. The goal is a Tendsto … atTop (𝓝 (1 + (⌊α⁻¹⌋₊)⁻¹)) statement in ℝ≥0∞. A real-valued sSup would have returned 000 on an unbounded family and made a false bound look provable; that encoding is ruled out. The upper bounds keep the additive constant 222 and the lower bound the subtractive 1m\frac1mm1​ exactly as printed.

The two proof steps are stated under the proof's own hypothesis "no element exceeding 1/m1/m1/m", which is weaker than L⊆(0,α]L\subseteq(0,\alpha]L⊆(0,α].

A complete development needs invariants of the First-Fit and Best-Fit folds, a lower bound L∗≥∑iaiL^*\ge\sum_i a_iL∗≥∑i​ai​, and exact evaluation of both runs on the construction of part (i). Lemmas about the fold encoding of First-Fit and Best-Fit and about L∗L^*L∗ are reusable in the companion missions on the 1710\tfrac{17}{10}1017​, 119\tfrac{11}{9}911​ and 7160\tfrac{71}{60}6071​ bounds of the same paper. Contributions on the Best-Fit upper bound are especially welcome, since the source gives no proof.

Selected references

  • D. S. Johnson, A. Demers, J. D. Ullman, M. R. Garey, R. L. Graham, Worst-Case Performance Bounds for Simple One-Dimensional Packing Algorithms, SIAM Journal on Computing 3(4):299–325, 1974. https://doi.org/10.1137/0203025
  • J. D. Ullman, The Performance of a Memory Allocation Algorithm, Technical Report 100, Princeton University, 1971.
  • M. R. Garey, R. L. Graham, J. D. Ullman, Worst-Case Analysis of Memory Allocation Algorithms, Proc. 4th ACM Symposium on Theory of Computing, 143–150, 1972. https://doi.org/10.1145/800152.804907
  • D. S. Johnson, Near-Optimal Bin Packing Algorithms, PhD thesis, Massachusetts Institute of Technology, 1973. http://hdl.handle.net/1721.1/57819
  • G. Dósa, J. Sgall, First Fit Bin Packing: A Tight Analysis, Proc. 30th STACS, LIPIcs 20:538–549, 2013. https://doi.org/10.4230/LIPIcs.STACS.2013.538
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Bandit AlgorithmsMachine LearningOperations Research+1·Captain: mikedeng1

Stochastic Linear Optimization under Bandit Feedback 1: The Regret Bound of ConfidenceBallResearch Paper

Motivation

In stochastic linear optimization under bandit feedback a learner repeatedly chooses a decision xtx_txt​ from a fixed set D⊆RnD\subseteq\mathbb R^nD⊆Rn and observes only the noisy cost of that one decision, whose expectation is a fixed but unknown linear function μ⊤xt\mu^\top x_tμ⊤xt​. The model covers online routing, ad and product selection with feature vectors, and any sequential decision problem whose decision set is too large to enumerate but whose expected cost is linear in a known representation. The multi-armed bandit is the special case where DDD is the set of standard basis vectors.

Dani, Hayes and Kakade (COLT 2008) analysed the algorithm ConfidenceBall₂, a generalization of Auer's LinRel (JMLR 2002), and proved that its regret is O∗(nT)O^*(n\sqrt T)O∗(nT​) with high probability for an arbitrary compact decision set, and that this is optimal up to logarithmic factors. Their confidence-ellipsoid construction became the template for later linear bandit algorithms (OFUL, LinUCB), and the ellipsoid-plus-potential analysis is the standard argument of the field (Lattimore and Szepesvári, Bandit Algorithms, Chapters 19–20).

Timeline: Auer (2002) introduced LinRel for finite decision sets; Dani, Hayes and Kakade (2008) extended it to arbitrary compact sets with the O∗(nT)O^*(n\sqrt T)O∗(nT​) bound and a matching Ω(nT)\Omega(n\sqrt T)Ω(nT​) lower bound; Rusmevichientong and Tsitsiklis (Math. Oper. Res. 2010) studied linearly parameterized bandits with dimension-dependent regret bounds; Abbasi-Yadkori, Pál and Szepesvári (NeurIPS 2011) sharpened the confidence ellipsoids with self-normalized martingale bounds.

Setting

Fix n≥1n\ge1n≥1 and a compact decision set D⊆RnD\subseteq\mathbb R^nD⊆Rn whose standard basis e1,…,ene_1,\dots,e_ne1​,…,en​ is a barycentric spanner: each ei∈De_i\in Dei​∈D and every x∈Dx\in Dx∈D lies in the cube [−1,1]n[-1,1]^n[−1,1]n. The paper's Section 5 adopts these coordinates without loss of generality. An unknown vector μ∈Rn\mu\in\mathbb R^nμ∈Rn satisfies ∣μ⊤x∣≤1|\mu^\top x|\le1∣μ⊤x∣≤1 for x∈Dx\in Dx∈D, and x∗∈Dx^*\in Dx∗∈D minimises μ⊤x\mu^\top xμ⊤x.

On round t=1,2,…t=1,2,\dotst=1,2,… the learner plays xt∈Dx_t\in Dxt​∈D, measurable with respect to the information Ft\mathcal F_tFt​ before round ttt, and observes a loss ℓt∈[−1,1]\ell_t\in[-1,1]ℓt​∈[−1,1] with E[ℓt∣Ft]=μ⊤xt\mathbb E[\ell_t\mid\mathcal F_t]=\mu^\top x_tE[ℓt​∣Ft​]=μ⊤xt​. The regret after TTT rounds is

RT=∑t=1T(μ⊤xt−μ⊤x∗).R_T=\sum_{t=1}^T\big(\mu^\top x_t-\mu^\top x^*\big).RT​=t=1∑T​(μ⊤xt​−μ⊤x∗).

ConfidenceBall₂(D,δ)(D,\delta)(D,δ) maintains the design matrix At=I+∑τ<txτxτ⊤A_t=I+\sum_{\tau<t}x_\tau x_\tau^\topAt​=I+∑τ<t​xτ​xτ⊤​, the least-squares estimate μ^t=At−1∑τ<tℓτxτ\hat\mu_t=A_t^{-1}\sum_{\tau<t}\ell_\tau x_\tauμ^​t​=At−1​∑τ<t​ℓτ​xτ​, the radius

βt=max⁡(128 nln⁡tln⁡(t2/δ), (83ln⁡(t2/δ))2),\beta_t=\max\Big(128\,n\ln t\ln(t^2/\delta),\ \big(\tfrac83\ln(t^2/\delta)\big)^2\Big),βt​=max(128nlntln(t2/δ), (38​ln(t2/δ))2),

and the confidence ellipsoid Bt2={ν:(ν−μ^t)⊤At(ν−μ^t)≤βt}B^2_t=\{\nu:(\nu-\hat\mu_t)^\top A_t(\nu-\hat\mu_t)\le\beta_t\}Bt2​={ν:(ν−μ^​t​)⊤At​(ν−μ^​t​)≤βt​}. It plays the optimistic decision xt∈argmin⁡x∈Dmin⁡ν∈Bt2ν⊤xx_t\in\operatorname{argmin}_{x\in D}\min_{\nu\in B^2_t}\nu^\top xxt​∈argminx∈D​minν∈Bt2​​ν⊤x. The analysis uses the width wt=xt⊤At−1xtw_t=\sqrt{x_t^\top A_t^{-1}x_t}wt​=xt⊤​At−1​xt​​, the error Zt=(μ^t−μ)⊤At(μ^t−μ)Z_t=(\hat\mu_t-\mu)^\top A_t(\hat\mu_t-\mu)Zt​=(μ^​t​−μ)⊤At​(μ^​t​−μ), and the noise ηt=ℓt−μ⊤xt\eta_t=\ell_t-\mu^\top x_tηt​=ℓt​−μ⊤xt​.

Formalization targets

Goal: Theorem 2, ConfidenceBall₂ bullet (corrected)

For 0<δ<10<\delta<10<δ<1 with n≤β1n\le\beta_1n≤β1​ and noise ∣ηt∣≤1|\eta_t|\le1∣ηt​∣≤1,

Pr⁡(∀T≥1, RT≤8nTβTln⁡(T+1))≥1−δ.\Pr\Big(\forall T\ge1,\ R_T\le\sqrt{8nT\beta_T\ln(T+1)}\Big)\ge1-\delta.Pr(∀T≥1, RT​≤8nTβT​ln(T+1)​)≥1−δ.

A single event covers every horizon, so the bound is anytime.

Milestones

  • Lemma 8. If μ∈Bt2\mu\in B^2_tμ∈Bt2​ then rt≤2min⁡(βtwt,1)r_t\le2\min(\sqrt{\beta_t}w_t,1)rt​≤2min(βt​​wt​,1).
  • Lemma 10. det⁡At+1=∏τ=1t(1+wτ2)\det A_{t+1}=\prod_{\tau=1}^t(1+w_\tau^2)detAt+1​=∏τ=1t​(1+wτ2​).
  • Lemma 9 (corrected). ∑τ=1tmin⁡(wτ2,1)≤2nln⁡(t+1)\sum_{\tau=1}^t\min(w_\tau^2,1)\le2n\ln(t+1)∑τ=1t​min(wτ2​,1)≤2nln(t+1).
  • Theorem 6 (corrected). If μ∈Bt2\mu\in B^2_tμ∈Bt2​ for all t≤Tt\le Tt≤T, then ∑t≤Trt2≤8nβTln⁡(T+1)\sum_{t\le T}r_t^2\le8n\beta_T\ln(T+1)∑t≤T​rt2​≤8nβT​ln(T+1).
  • Theorem 4 (Freedman). Pr⁡(∑Xi≥a, V≤v)≤exp⁡(−a2/(2v+2ab/3))\Pr(\sum X_i\ge a,\ V\le v)\le\exp(-a^2/(2v+2ab/3))Pr(∑Xi​≥a, V≤v)≤exp(−a2/(2v+2ab/3)) for martingale differences bounded above by bbb.
  • Lemma 12. Zt≤n+2∑τ<tητxτ⊤(μ^τ−μ)1+wτ2+∑τ<tητ2wτ21+wτ2Z_t\le n+2\sum_{\tau<t}\eta_\tau\frac{x_\tau^\top(\hat\mu_\tau-\mu)}{1+w_\tau^2}+\sum_{\tau<t}\eta_\tau^2\frac{w_\tau^2}{1+w_\tau^2}Zt​≤n+2∑τ<t​ητ​1+wτ2​xτ⊤​(μ^​τ​−μ)​+∑τ<t​ητ2​1+wτ2​wτ2​​.
  • Lemma 14. Pr⁡(∀t, ∑τ<tMτ≤βt/2)≥1−δ\Pr(\forall t,\ \sum_{\tau<t}M_\tau\le\beta_t/2)\ge1-\deltaPr(∀t, ∑τ<t​Mτ​≤βt​/2)≥1−δ.
  • Theorem 5 (Confidence). Pr⁡(∀t, μ∈Bt2)≥1−δ\Pr(\forall t,\ \mu\in B^2_t)\ge1-\deltaPr(∀t, μ∈Bt2​)≥1−δ.

Significance

The result gives a regret bound for linear bandits over an arbitrary compact decision set that depends on the dimension nnn rather than on ∣D∣|D|∣D∣, holds uniformly over horizons, and requires no gap between the best and second-best decision. With the paper's lower bound it shows that the price of bandit feedback, compared with full information, is a factor Θ∗(n)\Theta^*(\sqrt n)Θ∗(n​). The two components, a confidence theorem for a least-squares ellipsoid under martingale noise and a deterministic potential argument on log⁡det⁡At\log\det A_tlogdetAt​, are reused in the analysis of most optimistic linear and generalized-linear bandit algorithms.

The theorem has a published proof but, to our knowledge, no machine-checked one. The platform already has the elliptical potential lemma (BanditAlgorithm.elliptical_potential_lemma, Lattimore–Szepesvári Lemma 19.4), the matrix determinant lemma and the Woodbury identity, which cover the linear-algebra layer; the LinUCB regret theorem there (BanditAlgorithm.linear_bandit_linucb_regret_bound) is pathwise given confidence, for a different algorithm, so the probabilistic half is new. Formalization also settles the printed constants, three of which need correction (below).

Difficulty

The deterministic half is linear algebra. The difficulty is the confidence theorem. Hoeffding–Azuma applied to ∑τMτ\sum_\tau M_\tau∑τ​Mτ​ would need a deterministic step bound, and the natural one gives only a T3/4T^{3/4}T3/4 regret. The step sizes of MtM_tMt​ are bounded in terms of the random widths wtw_twt​, so the argument must control the conditional variances pathwise and apply Freedman's inequality, whose event {V≤v}\{V\le v\}{V≤v} is random. The escape indicator EtE_tEt​, which switches the martingale off after the first failure of confidence, is what makes the variance bound hold on every path, and the induction that turns Lemma 14 into Theorem 5 must be carried out on a single event for all ttt simultaneously. Freedman's inequality itself is not in Mathlib.

Formalization scope

Vectors are Fin n → ℝ, matrices Matrix (Fin n) (Fin n) ℝ, rounds are indexed t=1,2,…t=1,2,\dotst=1,2,… in ℕ. The spanner is the standard basis, as in Section 5 of the paper (the algorithm is equivariant under the linear change of coordinates). The probability model is a probability space with a general filtration (Ft)(\mathcal F_t)(Ft​); xtx_txt​ is Ft\mathcal F_tFt​-measurable and ℓt\ell_tℓt​ is Ft+1\mathcal F_{t+1}Ft+1​-measurable. The argmin is encoded as a joint minimiser over D×Bt2D\times B^2_tD×Bt2​, which admits every tie-break and is required on every outcome; measurability of xtx_txt​ is a hypothesis, not derived from the selection. The optimum x∗x^*x∗ is a hypothesis (x∗∈Dx^*\in Dx∗∈D, minimising), not an sInf.

Corrections of the printed statements, each labelled in the item's Formalization Note:

  1. ln⁡(T+1)\ln(T+1)ln(T+1) for ln⁡T\ln TlnT in Lemma 9, Theorem 6 and Theorem 2. The printed bounds are false at T=1T=1T=1 (with n=1n=1n=1, D=[−1,1]D=[-1,1]D=[−1,1], μ>0\mu>0μ>0, the tie-break x1=1x_1=1x1​=1 gives R1=2μ>0R_1=2\mu>0R1​=2μ>0 against a bound of 000); the proof of Lemma 9 gives 2ln⁡det⁡At+1≤2nln⁡(t+1)2\ln\det A_{t+1}\le2n\ln(t+1)2lndetAt+1​≤2nln(t+1).
  2. n≤β1=(83ln⁡(1/δ))2n\le\beta_1=(\tfrac83\ln(1/\delta))^2n≤β1​=(38​ln(1/δ))2 is added to Theorems 5 and 2: the proof of Theorem 5 claims Z1≤n<β1Z_1\le n<\beta_1Z1​≤n<β1​, which fails for δ\deltaδ near 111. Theorem 6 takes the proof's "1<β11<\beta_11<β1​" as the hypothesis β1≥1\beta_1\ge1β1​≥1.
  3. ∣ℓt−μ⊤xt∣≤1|\ell_t-\mu^\top x_t|\le1∣ℓt​−μ⊤xt​∣≤1 is added to Lemma 14, Theorems 5 and 2: Section 5.2 uses ∣ηt∣≤1|\eta_t|\le1∣ηt​∣≤1, while the model gives only ∣ηt∣≤2|\eta_t|\le2∣ηt​∣≤2. It holds when costs lie in [0,1][0,1][0,1].
  4. Theorem 5's "δ>0\delta>0δ>0" is stated with 0<δ<10<\delta<10<δ<1; Lemma 10's index typo (wtw_twt​ for wτw_\tauwτ​) and Theorem 4's ∑i=1n\sum_{i=1}^n∑i=1n​ (for TTT) are corrected.

A regret bound for an arbitrary decision sequence under the assumption μ∈Bt2\mu\in B^2_tμ∈Bt2​ for all ttt is Theorem 6, not the goal; the goal carries the ConfidenceBall₂ selection rule, the conditional-mean and measurability hypotheses, and δ\deltaδ as the algorithm's own parameter. The hypotheses are jointly satisfiable, for example by a finite DDD with a fixed tie-break and i.i.d. costs in [0,1][0,1][0,1].

Needed infrastructure: Freedman's inequality for a filtration (reusable across all of bandit theory), the potential lemma (available), and measurability of the algorithm's statistics. Contributions of alternative proofs of Theorem 5, for example via self-normalized bounds, are welcome.

Selected references

  • V. Dani, T. P. Hayes, S. M. Kakade, Stochastic Linear Optimization under Bandit Feedback, COLT 2008. http://colt2008.cs.helsinki.fi/papers/80-Dani.pdf
  • P. Auer, Using Confidence Bounds for Exploitation-Exploration Trade-offs, JMLR 3, 2002. https://www.jmlr.org/papers/v3/auer02a.html
  • D. A. Freedman, On Tail Probabilities for Martingales, Annals of Probability 3(1), 1975. https://doi.org/10.1214/aop/1176996452
  • B. Awerbuch, R. Kleinberg, Adaptive Routing with End-to-End Feedback, STOC 2004. https://doi.org/10.1145/1007352.1007367
  • P. Rusmevichientong, J. N. Tsitsiklis, Linearly Parameterized Bandits, Mathematics of Operations Research 35(2), 2010. https://doi.org/10.1287/moor.1100.0446
  • Y. Abbasi-Yadkori, D. Pál, Cs. Szepesvári, Improved Algorithms for Linear Stochastic Bandits, NeurIPS 2011. https://arxiv.org/abs/1102.2670
  • T. Lattimore, Cs. Szepesvári, Bandit Algorithms, Cambridge University Press, 2020. https://doi.org/10.1017/9781108571401
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Machine LearningOperations ResearchOptimization+1·Captain: mikedeng1

Generalization Bounds in the Predict-then-Optimize Framework I: Natarajan-Dimension Generalization Bound for Polyhedral Feasible RegionsResearch Paper

Motivation

In many operational problems (shortest paths, assignment, planning) the decision solves a linear program whose cost vector is unknown at decision time and is predicted from contextual features. The predict-then-optimize pipeline fits a model fff that maps a feature vector xxx to a predicted cost vector c^=f(x)\hat c=f(x)c^=f(x), and then acts on the decision that is optimal for c^\hat cc^. Elmachtoub and Grigas (Smart "Predict, then Optimize", Management Science 2022) proposed to measure the quality of such a model not by the prediction error but by the SPO loss (Smart Predict-then-Optimize loss): the excess true cost of the decision induced by the prediction over the best decision in hindsight.

The question is whether a small SPO loss on the training sample implies a small SPO loss on new data, uniformly over the models a training procedure may return. The SPO loss is neither convex nor continuous in the prediction, so the standard Lipschitz-based bounds for regression do not apply. El Balghiti, Elmachtoub, Grigas and Tewari (arXiv:1905.11488v3, Mathematics of Operations Research 2023; a preliminary version appeared at NeurIPS 2019) give the first such generalization bounds. This mission formalizes their first one, for polyhedral feasible regions, which treats every vertex of the feasible region as a class label of a multiclass classification problem. The bound has since been used by later work, e.g. Hu, Kallus and Mao (Fast rates for contextual linear optimization, Management Science 2022), who sharpen it by a log⁡n\sqrt{\log n}logn​ factor (as noted on p. 4 of the paper).

Setting

A feasible region S⊆RdS\subseteq\mathbb R^dS⊆Rd is nonempty, compact and convex. For a cost vector c∈Rdc\in\mathbb R^dc∈Rd the nominal problem is min⁡w∈Sc⊤w\min_{w\in S}c^\top wminw∈S​c⊤w. An optimization oracle is a fixed map w∗:Rd→Sw^*:\mathbb R^d\to Sw∗:Rd→S with w∗(c)∈arg⁡min⁡w∈Sc⊤ww^*(c)\in\arg\min_{w\in S}c^\top ww∗(c)∈argminw∈S​c⊤w for every ccc; nothing is assumed about how it breaks ties. The SPO loss of a prediction c^\hat cc^ when the realized cost is ccc is

ℓSPO(c^,c)=c⊤w∗(c^)−c⊤w∗(c) ≥0.\ell_{\rm SPO}(\hat c,c)=c^\top w^*(\hat c)-c^\top w^*(c)\ \ge 0 .ℓSPO​(c^,c)=c⊤w∗(c^)−c⊤w∗(c) ≥0.

The linear optimization gap is ωS(c)=max⁡w∈Sc⊤w−min⁡w∈Sc⊤w\omega_S(c)=\max_{w\in S}c^\top w-\min_{w\in S}c^\top wωS​(c)=maxw∈S​c⊤w−minw∈S​c⊤w, and for a set C\mathcal CC of cost vectors ωS(C)=sup⁡c∈CωS(c)\omega_S(\mathcal C)=\sup_{c\in\mathcal C}\omega_S(c)ωS​(C)=supc∈C​ωS​(c); the SPO loss of a cost in C\mathcal CC lies in [0,ωS(C)][0,\omega_S(\mathcal C)][0,ωS​(C)].

Data are pairs (x,c)(x,c)(x,c) drawn from a distribution D\mathcal DD on X×C\mathcal X\times\mathcal CX×C. A hypothesis class H\mathcal HH is a family of predictors f:X→Rdf:\mathcal X\to\mathbb R^df:X→Rd. The SPO risk is RSPO(f)=ED[ℓSPO(f(x),c)]R_{\rm SPO}(f)=\mathbb E_{\mathcal D}[\ell_{\rm SPO}(f(x),c)]RSPO​(f)=ED​[ℓSPO​(f(x),c)], and on an i.i.d. sample (x1,c1),…,(xn,cn)(x_1,c_1),\dots,(x_n,c_n)(x1​,c1​),…,(xn​,cn​) the empirical SPO risk is R^SPO(f)=1n∑iℓSPO(f(xi),ci)\hat R_{\rm SPO}(f)=\frac1n\sum_i\ell_{\rm SPO}(f(x_i),c_i)R^SPO​(f)=n1​∑i​ℓSPO​(f(xi​),ci​). The empirical Rademacher complexity with respect to the SPO loss is

R^SPOn(H)=Eσ[sup⁡f∈H1n∑i=1nσi ℓSPO(f(xi),ci)]\hat{\mathfrak R}^n_{\rm SPO}(\mathcal H)=\mathbb E_\sigma\Big[\sup_{f\in\mathcal H}\frac1n\sum_{i=1}^n\sigma_i\,\ell_{\rm SPO}(f(x_i),c_i)\Big]R^SPOn​(H)=Eσ​[f∈Hsup​n1​i=1∑n​σi​ℓSPO​(f(xi​),ci​)]

with independent uniform signs σi∈{±1}\sigma_i\in\{\pm1\}σi​∈{±1}, and RSPOn(H)\mathfrak R^n_{\rm SPO}(\mathcal H)RSPOn​(H) is its expectation over the sample.

The decisions induced by H\mathcal HH form the class w∗(H)={x↦w∗(f(x)):f∈H}w^*(\mathcal H)=\{x\mapsto w^*(f(x)):f\in\mathcal H\}w∗(H)={x↦w∗(f(x)):f∈H}. A class F\mathcal FF N-shatters a finite set X⊆X\mathbb X\subseteq\mathcal XX⊆X if there are two labelings g1,g2g_1,g_2g1​,g2​ that differ at every point of X\mathbb XX such that every mixture of them (follow g1g_1g1​ on a subset TTT, g2g_2g2​ on the rest) is realized by some member of F\mathcal FF. The Natarajan dimension dN(F)d_N(\mathcal F)dN​(F) is the largest size of an N-shattered set. When SSS is a polyhedron, S\mathfrak SS denotes its finite set of extreme points.

Formalization targets

Goal: Theorem 2, second display (p. 11)

For a polyhedral SSS and every δ>0\delta>0δ>0, with probability at least 1−δ1-\delta1−δ over an i.i.d. sample of size nnn, every f∈Hf\in\mathcal Hf∈H satisfies

RSPO(f)≤R^SPO(f)+2 ωS(C)2dN(w∗(H))log⁡(n∣S∣2)n+ωS(C)log⁡(1/δ)2n.R_{\rm SPO}(f)\le\hat R_{\rm SPO}(f)+2\,\omega_S(\mathcal C)\sqrt{\frac{2d_N(w^*(\mathcal H))\log(n|\mathfrak S|^2)}{n}}+\omega_S(\mathcal C)\sqrt{\frac{\log(1/\delta)}{2n}} .RSPO​(f)≤R^SPO​(f)+2ωS​(C)n2dN​(w∗(H))log(n∣S∣2)​​+ωS​(C)2nlog(1/δ)​​.

Milestones, in attack order

  1. Theorem 1 (p. 9): with probability 1−δ1-\delta1−δ, RSPO(f)≤R^SPO(f)+2RSPOn(H)+ωS(C)log⁡(1/δ)/(2n)R_{\rm SPO}(f)\le\hat R_{\rm SPO}(f)+2\mathfrak R^n_{\rm SPO}(\mathcal H)+\omega_S(\mathcal C)\sqrt{\log(1/\delta)/(2n)}RSPO​(f)≤R^SPO​(f)+2RSPOn​(H)+ωS​(C)log(1/δ)/(2n)​ for all f∈Hf\in\mathcal Hf∈H.
  2. Massart step (Appendix B.1, p. 31): for a fixed sample with costs in C\mathcal CC, R^SPOn(H)≤ωS(C)2log⁡∣F∣X∣/n\hat{\mathfrak R}^n_{\rm SPO}(\mathcal H)\le\omega_S(\mathcal C)\sqrt{2\log|\mathfrak F_{|\mathbb X}|/n}R^SPOn​(H)≤ωS​(C)2log∣F∣X​∣/n​, where F∣X\mathfrak F_{|\mathbb X}F∣X​ is the set of decision vectors (w∗(f(x1)),…,w∗(f(xn)))(w^*(f(x_1)),\dots,w^*(f(x_n)))(w∗(f(x1​)),…,w∗(f(xn​))).
  3. Natarajan lemma (cited on p. 31; proved on the platform as UnderstandingML.natarajan_lemma): a class from an mmm-point set to kkk labels with Natarajan dimension ddd has at most mdk2dm^d k^{2d}mdk2d members.
  4. Empirical bound (Appendix B.1, p. 31): for a fixed sample, R^SPOn(H)≤ωS(C)2dN(w∗(H))log⁡(n∣S∣2)/n\hat{\mathfrak R}^n_{\rm SPO}(\mathcal H)\le\omega_S(\mathcal C)\sqrt{2d_N(w^*(\mathcal H))\log(n|\mathfrak S|^2)/n}R^SPOn​(H)≤ωS​(C)2dN​(w∗(H))log(n∣S∣2)/n​.
  5. Theorem 2, first display (p. 11): the same bound for the expected complexity RSPOn(H)\mathfrak R^n_{\rm SPO}(\mathcal H)RSPOn​(H).

Significance

The bound controls the out-of-sample decision cost of every predictor in the class, not only of an empirical risk minimizer, so it applies to any training procedure (SPO+ surrogate minimization, decision trees, heuristics) that returns a member of H\mathcal HH. Its dependence on the feasible region is only through ωS(C)\omega_S(\mathcal C)ωS​(C) and log⁡∣S∣\log|\mathfrak S|log∣S∣: the number of vertices of a combinatorial polytope is typically exponential in ddd, and enters only logarithmically. For linear predictors x↦Bxx\mapsto Bxx↦Bx the paper's Corollary 2 bounds dN(w∗(Hlin))d_N(w^*(\mathcal H_{\rm lin}))dN​(w∗(Hlin​)) by dpdpdp, giving a rate of order dplog⁡(n∣S∣)/n\sqrt{dp\log(n|\mathfrak S|)/n}dplog(n∣S∣)/n​.

The results are proved in the paper; this mission formalizes them. No statement about predict-then-optimize or the SPO loss is known to have a machine-checked proof. The platform already has the Natarajan lemma (proved) and several Massart-type lemmas for generic classes; this mission connects that multiclass machinery to decision losses, and its Theorem 1 is a reusable Rademacher generalization bound for a loss with range [0,ω][0,\omega][0,ω].

Difficulty

The obvious route through Lipschitz contraction fails: the SPO loss jumps when the prediction crosses a point where the optimum is not unique, so the Rademacher complexity of the composed class cannot be bounded by that of H\mathcal HH times a Lipschitz constant. Any argument through the finitely many vertices of SSS needs the decisions w∗(f(xi))w^*(f(x_i))w∗(f(xi​)) to take finitely many values on a sample, i.e. the oracle to return vertices; for an oracle that returns a non-vertex optimal point under ties, w∗(H)w^*(\mathcal H)w∗(H) may take infinitely many values on a sample. On the probabilistic side, the passage from the empirical to the expected complexity and the McDiarmid concentration step (Theorem 1) require the suprema over an uncountable class to be measurable, which the paper does not discuss.

Formalization scope

Lean works in Rd\mathbb R^dRd = EuclideanSpace ℝ (Fin d); cost vectors and decisions live in the same space and c⊤wc^\top wc⊤w is the inner product. The standing assumptions of §2 are hypotheses of every theorem: SSS nonempty, compact and convex; w∗w^*w∗ an arbitrary oracle (a hypothesis IsOracle S w, never a specific selection); C\mathcal CC nonempty and bounded, with the cost component of D\mathcal DD in C\mathcal CC almost surely (or, for fixed-sample statements, every ci∈Cc_i\in\mathcal Cci​∈C); n≥1n\ge1n≥1. "Polyhedron" means the solution set of finitely many linear inequalities; with compactness it is a polytope, and ∣S∣|\mathfrak S|∣S∣ is the cardinality of Set.extremePoints ℝ S. The expectation over signs is the exact average over the 2n2^n2n sign vectors; RSPOR_{\rm SPO}RSPO​ and RSPOn\mathfrak R^n_{\rm SPO}RSPOn​ are Bochner integrals. "With probability at least 1−δ1-\delta1−δ" is stated as: the product measure of the set of samples on which some f∈Hf\in\mathcal Hf∈H violates the bound is at most δ\deltaδ.

The formalization commits to the following disclosed additions:

  • In the empirical bound, Theorem 2 and its first display, the oracle returns extreme points of SSS. This is the proof's own "w.l.o.g." (p. 31), made explicit because p. 10 allows non-vertex outputs under ties. The hypothesis is needed: on the unit square, an oracle that returns distinct interior points of an edge under ties can have dN(w∗(H))=1d_N(w^*(\mathcal H))=1dN​(w∗(H))=1 and empirical complexity near 12\frac1221​, which exceeds the printed bound for large nnn.
  • The Natarajan dimension is not defined as a number (a supremum in N\mathbb NN would silently be 000 for unboundedly large shattered sets). Statements carry a natural number kkk bounding the size of every N-shattered set, in place of dN(w∗(H))d_N(w^*(\mathcal H))dN​(w∗(H)). This is equivalent when dNd_NdN​ is finite; the printed bound is vacuous otherwise.
  • Theorem 1 and the goal carry three measurability hypotheses: each loss function z↦ℓSPO(f(z1),z2)z\mapsto\ell_{\rm SPO}(f(z_1),z_2)z↦ℓSPO​(f(z1​),z2​) is measurable; the uniform deviation sup⁡f(RSPO(f)−R^SPO(f))\sup_f(R_{\rm SPO}(f)-\hat R_{\rm SPO}(f))supf​(RSPO​(f)−R^SPO​(f)) and, for each sign vector, the signed supremum sup⁡f1n∑iσiℓSPO(f(xi),ci)\sup_f\frac1n\sum_i\sigma_i\ell_{\rm SPO}(f(x_i),c_i)supf​n1​∑i​σi​ℓSPO​(f(xi​),ci​) are almost-everywhere measurable functions of the sample. Without them the integral defining RSPOn\mathfrak R^n_{\rm SPO}RSPOn​ could default to 000.
  • The Massart step assumes F∣X\mathfrak F_{|\mathbb X}F∣X​ finite, the case in which its printed right-hand side is finite.

A formalization that let dNd_NdN​ be an sSup in N\mathbb NN, or chose a specific tie-breaking oracle inside the definitions, would prove a different and in part trivial statement; both are excluded.

Infrastructure needed: McDiarmid's bounded-differences inequality and symmetrization for the product measure; Massart's finite-class lemma (a proved version is on the platform as RademacherMassart.rad_le_massart, with its own normalization); the Natarajan lemma (proved, UnderstandingML.natarajan_lemma, stated with its own but identical notion of N-shattering over finite types); finiteness and nonemptiness of the extreme points of a nonempty polytope. Theorem 1 and the Massart step do not use polyhedrality and are reusable for any bounded decision loss. Contributions of these infrastructure lemmas are welcome.

Selected references

  • O. El Balghiti, A. N. Elmachtoub, P. Grigas, A. Tewari, Generalization Bounds in the Predict-then-Optimize Framework, arXiv:1905.11488v3, 2022; Mathematics of Operations Research, 2023. https://arxiv.org/abs/1905.11488
  • A. N. Elmachtoub, P. Grigas, Smart "Predict, then Optimize", Management Science 68(1), 9–26, 2022. https://arxiv.org/abs/1710.08005
  • P. L. Bartlett, S. Mendelson, Rademacher and Gaussian complexities: risk bounds and structural results, Journal of Machine Learning Research 3, 463–482, 2002. https://www.jmlr.org/papers/v3/bartlett02a.html
  • B. K. Natarajan, On learning sets and functions, Machine Learning 4(1), 67–97, 1989. https://doi.org/10.1007/BF00114804
  • S. Shalev-Shwartz, S. Ben-David, Understanding Machine Learning: From Theory to Algorithms, Cambridge University Press, 2014 (Lemma 29.4). https://doi.org/10.1017/CBO9781107298019
  • M. Mohri, A. Rostamizadeh, A. Talwalkar, Foundations of Machine Learning, 2nd ed., MIT Press, 2018 (Theorem 3.3, Corollary 3.8). https://cs.nyu.edu/~mohri/mlbook/
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CombinatoricsOperations ResearchOptimization+1·Captain: mikedeng1

Local Search Heuristics for k-Median and Facility Location Problems III: Add-Drop-Swap Local Search for Uncapacitated Facility Location Has Locality Gap 3Research Paper

Motivation

The uncapacitated facility location (UFL) problem is one of the basic models of location theory and operations research: a firm chooses which warehouses, plants or servers to open, paying a fixed cost for each open site and a service cost for every client according to its distance to the nearest open site. It is also a standard test case for approximation algorithms.

Local search is the simplest of these and the one most used in practice: start from any set of open facilities and repeatedly add, drop or exchange one facility while this lowers the cost. The question is how bad a solution can be when no such move helps. Arya, Garg, Khandekar, Meyerson, Munagala and Pandit (SIAM J. Comput. 33(3), 2004) answered it for UFL with an exact constant.

Timeline. Korupolu, Plaxton and Rajaraman (SODA 1998, J. Algorithms 2000) analysed local search with add, drop and swap moves and proved a locality gap of at most 5; their analysis contains the service cost bound restated here as Lemma 4.1. Charikar and Guha (FOCS 1999) proved a locality gap of 3 for a different local search, in which one facility is added and any number are dropped. Arya et al. (STOC 2001; journal version 2004) proved that the add/drop/swap neighbourhood itself has locality gap at most 3, and gave an instance showing that 3 cannot be improved (§4.3).

Setting

A metric instance consists of a finite set CCC of clients, a finite set FFF of facilities, and a distance ddd on C∪FC \cup FC∪F that is nonnegative, symmetric and satisfies the triangle inequality. The cost of serving client jjj by facility iii is cji=d(j,i)c_{ji} = d(j,i)cji​=d(j,i); the distance cii′c_{ii'}cii′​ between two facilities is also available. Each facility i∈Fi \in Fi∈F has an opening cost fi≥0f_i \ge 0fi​≥0.

A solution is a nonempty set S⊆FS \subseteq FS⊆F of open facilities. Every client is served by its nearest open facility, so

costf(S)=∑i∈Sfi,costs(S)=∑j∈Cmin⁡i∈Scji,cost(S)=costf(S)+costs(S).\mathrm{cost}_f(S) = \sum_{i \in S} f_i, \qquad \mathrm{cost}_s(S) = \sum_{j \in C} \min_{i \in S} c_{ji}, \qquad \mathrm{cost}(S) = \mathrm{cost}_f(S) + \mathrm{cost}_s(S).costf​(S)=i∈S∑​fi​,costs​(S)=j∈C∑​i∈Smin​cji​,cost(S)=costf​(S)+costs​(S).

The neighbourhood of SSS is the set of solutions reachable by adding one facility, dropping one facility, or swapping one open facility for another:

B(S)={S+{s′}}∪{S−{s}∣s∈S}∪{S−{s}+{s′}∣s∈S}.\mathcal B(S) = \{S + \{s'\}\} \cup \{S - \{s\} \mid s \in S\} \cup \{S - \{s\} + \{s'\} \mid s \in S\}.B(S)={S+{s′}}∪{S−{s}∣s∈S}∪{S−{s}+{s′}∣s∈S}.

SSS is locally optimum if cost(S)≤cost(S′)\mathrm{cost}(S) \le \mathrm{cost}(S')cost(S)≤cost(S′) for every S′∈B(S)S' \in \mathcal B(S)S′∈B(S). The locality gap is the supremum, over all instances, of the ratio between the cost of a worst local optimum and the cost of a global optimum.

The proofs use the following notation, which appears in the milestones but not in the goal. Fix a second solution OOO and nearest-facility assignments σS:C→S\sigma_S : C \to SσS​:C→S, σO:C→O\sigma_O : C \to OσO​:C→O; write Sj=cjσS(j)S_j = c_{j\sigma_S(j)}Sj​=cjσS​(j)​, Oj=cjσO(j)O_j = c_{j\sigma_O(j)}Oj​=cjσO​(j)​, NS(s)=σS−1(s)N_S(s) = \sigma_S^{-1}(s)NS​(s)=σS−1​(s), NO(o)=σO−1(o)N_O(o) = \sigma_O^{-1}(o)NO​(o)=σO−1​(o) and Nso=NO(o)∩NS(s)N^o_s = N_O(o) \cap N_S(s)Nso​=NO​(o)∩NS​(s). A facility s∈Ss \in Ss∈S captures o∈Oo \in Oo∈O if ∣Nso∣>12∣NO(o)∣|N^o_s| > \tfrac12 |N_O(o)|∣Nso​∣>21​∣NO​(o)∣; sss is good if it captures no facility of OOO and bad otherwise. The proof of the facility cost bound uses a permutation π\piπ of the clients that maps each NO(o)N_O(o)NO​(o) onto itself, moves every client of a non-capturing block NsoN^o_sNso​ out of that block (Property 3.1), and fixes every client of a capturing block that it would map into the same block.

Formalization targets

Goal: Theorem 4.3

cost(S)≤3⋅cost(O)for every locally optimum S and every solution O.\mathrm{cost}(S) \le 3 \cdot \mathrm{cost}(O) \quad \text{for every locally optimum } S \text{ and every solution } O.cost(S)≤3⋅cost(O)for every locally optimum S and every solution O.

This is the locality gap bound of Theorem 4.3 (p. 557) in its strongest printed form: OOO is any solution, not only an optimal one.

Milestones

  1. Lemma 4.1 (service cost), p. 554: costs(S)≤costf(O)+costs(O)\mathrm{cost}_s(S) \le \mathrm{cost}_f(O) + \mathrm{cost}_s(O)costs​(S)≤costf​(O)+costs​(O).
  2. The refined mapping π\piπ of the proof of Lemma 4.2, p. 555: such a permutation exists for any two assignments.
  3. Inequality (5), p. 555: the drop move for a good facility sss,
−fs+∑j∈NS(s), π(j)≠j(Oj+Oπ(j)+Sπ(j)−Sj)+2∑j∈NS(s), π(j)=jOj≥0.-f_s + \sum_{j \in N_S(s),\ \pi(j) \neq j} (O_j + O_{\pi(j)} + S_{\pi(j)} - S_j) + 2 \sum_{j \in N_S(s),\ \pi(j) = j} O_j \ge 0.−fs​+j∈NS​(s), π(j)=j∑​(Oj​+Oπ(j)​+Sπ(j)​−Sj​)+2j∈NS​(s), π(j)=j∑​Oj​≥0.
  1. Inequality (6), pp. 555–556: the swap of a bad facility sss with the facility ooo it captures that is nearest to it.
  2. Inequality (8), p. 556: for a bad facility sss capturing the set P⊆OP \subseteq OP⊆O, the analogue of (5) with ∑o′∈Pfo′−fs\sum_{o' \in P} f_{o'} - f_s∑o′∈P​fo′​−fs​ in place of −fs-f_s−fs​.
  3. Lemma 4.2 (facility cost), p. 555: costf(S)≤costf(O)+2⋅costs(O)\mathrm{cost}_f(S) \le \mathrm{cost}_f(O) + 2 \cdot \mathrm{cost}_s(O)costf​(S)≤costf​(O)+2⋅costs​(O).

A companion item, not a milestone, states the bound in the proof of Theorem 4.4 with α=2\alpha = \sqrt2α=2​: a local optimum of the instance with facility costs 2fi\sqrt2 f_i2​fi​ costs at most (1+2) cost(O)(1+\sqrt2)\,\mathrm{cost}(O)(1+2​)cost(O) in the original instance.

Significance

The result. Theorem 4.3 shows that the simplest local search for metric UFL is within a factor 3 of optimal at every local optimum, with no LP and no rounding, and the tight example of §4.3 shows the analysis cannot be improved for this neighbourhood. Because Lemmas 4.1 and 4.2 hold against every solution OOO, scaling the facility costs before running local search trades the two bounds against each other and gives the 1+2+ϵ1 + \sqrt2 + \epsilon1+2​+ϵ guarantee of Theorem 4.4. The same capture-and-reassign technique is used for k-median (§3) and capacitated facility location (§5).

Formalizing it. The theorem is proved on paper; no machine-checked proof of it or of any locality gap bound for facility location is known to this mission. A formal development would check the reassignment arguments, which are stated case by case in the paper, and would produce reusable Lean infrastructure for metric facility location instances, nearest-facility costs and neighbourhood-based local optimality.

Difficulty

The service cost bound is routine; the facility cost bound is where the work lies. The natural first idea, closing a facility s∈Ss \in Ss∈S and sending each of its clients to the facility of SSS nearest to that client's optimal facility, fails when sss serves most of the clients of some o∈Oo \in Oo∈O: the nearest facility of SSS to ooo may be sss itself, so the client has nowhere to go. The proof separates good facilities, which can be dropped, from bad ones, which must be swapped with a captured facility, and pays for the clients that cannot be moved through the distance between sss and its nearest captured facility. The combinatorial core is the construction of a permutation within each NO(o)N_O(o)NO​(o) that avoids every non-capturing block and has fixed points only where they are unavoidable.

Formalization scope

Clients and facilities are finite types Cl and Fa. The distance is a real-valued function on Cl ⊕ Fa that is nonnegative, symmetric and satisfies the triangle inequality; d(x,x)=0d(x,x) = 0d(x,x)=0 is not assumed, since the paper neither states nor uses it. Opening costs are a function f : Fa → ℝ with 0 ≤ f i, and demands are unit, as in the paper.

Solutions are nonempty Finsets. The service cost is ∑jmin⁡i∈Scji\sum_j \min_{i \in S} c_{ji}∑j​mini∈S​cji​ (Finset.inf') and is defined only for nonempty sets, so no junk value for ∅\emptyset∅ enters. Accordingly the drop move is considered only when a facility remains open; with at least one client, ∅\emptyset∅ cannot serve anyone and is not a solution. Local optimality is required for all moves of B(S)\mathcal B(S)B(S): every added facility, every dropped facility and every swap, not only the moves used in the proof. The goal is stated as the multiplied-out inequality cost(S)≤3 cost(O)\mathrm{cost}(S) \le 3\,\mathrm{cost}(O)cost(S)≤3cost(O) for every nonempty OOO, never as a ratio, since cost(O)\mathrm{cost}(O)cost(O) may be 000.

In the milestones, the nearest-facility assignments σS\sigma_SσS​, σO\sigma_OσO​ are arbitrary among the nearest ones (ties broken arbitrarily), and the family of bijections π:NO(o)→NO(o)\pi : N_O(o) \to N_O(o)π:NO​(o)→NO​(o) is a single permutation of the clients with σO∘π=σO\sigma_O \circ \pi = \sigma_OσO​∘π=σO​. Inequality (5) assumes at least one client, which the paper assumes implicitly: with no clients and S={s}S = \{s\}S={s} it would read −fs≥0-f_s \ge 0−fs​≥0. The goal and Lemma 4.2 need no such assumption.

A statement that assumes local optimality only for the moves the proof uses, that fixes OOO to be a global optimum defined by hypotheses, or that allows the empty set a zero service cost would be a different theorem; none of these is used.

Needed infrastructure: sums over nearest-facility assignments and their fibers NO(o)N_O(o)NO​(o), the permutation π\piπ, and bookkeeping of the three kinds of moves. The instance, cost and local optimality definitions are reusable for other local search analyses of metric location problems. Proofs of any milestone are welcome, as are alternative proofs of the goal.

Selected references

  • V. Arya, N. Garg, R. Khandekar, A. Meyerson, K. Munagala, V. Pandit, Local Search Heuristics for k-Median and Facility Location Problems, SIAM J. Comput. 33(3):544–562, 2004. https://doi.org/10.1137/S0097539702416402
  • M. R. Korupolu, C. G. Plaxton, R. Rajaraman, Analysis of a Local Search Heuristic for Facility Location Problems, J. Algorithms 37(1):146–188, 2000. https://doi.org/10.1006/jagm.2000.1100
  • M. Charikar, S. Guha, Improved Combinatorial Algorithms for the Facility Location and k-Median Problems, FOCS 1999, 378–388. https://doi.org/10.1109/SFFCS.1999.814609
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Group TheoryMathematical Physics·Captain: Lucas

Siegel's Fields I: SU(2) double cover of SO(3)Textbook

Motivation

Rotations of three-dimensional space are the most frequently used nontrivial Lie group in physics. Quantum mechanics requires more than the rotation group SO(3)SO(3)SO(3) itself: particles of half-integer spin, such as the electron, transform under a group in which a rotation by 2π2\pi2π acts as −1-1−1. That group is SU(2)SU(2)SU(2), the double covering group of SO(3)SO(3)SO(3). W. Siegel's graduate text Fields (arXiv:hep-th/9912205) introduces spin through this covering in Chapter II, Section A ("Two components", pp. 110–116). It encodes a 3-vector as a traceless hermitian 2×22\times22×2 matrix, reads the dot and cross products off the matrix product, and realizes rotations as conjugation by unitary matrices.

This mission is the first in a series formalizing results from Fields. It covers the algebra of §IIA1–IIA3, which ends with the statement that the map SU(2)→SO(3)SU(2)\to SO(3)SU(2)→SO(3) is two-to-one.

Setting

Let M2(C)M_2(\mathbb C)M2​(C) be the complex 2×22\times22×2 matrices, V†V^\daggerV† the conjugate transpose, VTV^TVT the transpose and V∗V^*V∗ the entrywise complex conjugate.

  • A 3-vector is a matrix V∈M2(C)V\in M_2(\mathbb C)V∈M2​(C) with V†=VV^\dagger=VV†=V and tr⁡V=0\operatorname{tr}V=0trV=0. These matrices form a real vector space V\mathcal VV of dimension three.
  • The book's basis: for v=(v1,v2,v3)∈R3v=(v_1,v_2,v_3)\in\mathbb R^3v=(v1​,v2​,v3​)∈R3,
V(v)=12(v1v2−iv3v2+iv3−v1),Ei=V(ei).V(v)=\frac1{\sqrt2}\begin{pmatrix}v_1&v_2-iv_3\\ v_2+iv_3&-v_1\end{pmatrix},\qquad E_i=V(e_i).V(v)=2​1​(v1​v2​+iv3​​v2​−iv3​−v1​​),Ei​=V(ei​).
  • The norm is ∣V∣2=−2det⁡V=tr⁡(V2)|V|^2=-2\det V=\operatorname{tr}(V^2)∣V∣2=−2detV=tr(V2), and the inner product is V⋅W=tr⁡(VW)V\cdot W=\operatorname{tr}(VW)V⋅W=tr(VW).
  • The matrix C=(0−ii0)C=\begin{pmatrix}0&-i\\ i&0\end{pmatrix}C=(0i​−i0​).
  • A rotation acts by V↦UVU†V\mapsto UVU^\daggerV↦UVU† with U∈SU(2)U\in SU(2)U∈SU(2), i.e. U†=U−1U^\dagger=U^{-1}U†=U−1 and det⁡U=1\det U=1detU=1. Its matrix in the basis EiE_iEi​ is
R(U)ij=Re⁡tr⁡(Ei U Ej U†).R(U)_{ij}=\operatorname{Re}\operatorname{tr}\big(E_i\,U\,E_j\,U^\dagger\big).R(U)ij​=Retr(Ei​UEj​U†).

In the Lean development these are SiegelFields.IsThreeVector, vecToMatrix, basisMatrix, matC and rotationOf. Components are indexed by {0,1,2}\{0,1,2\}{0,1,2}.

Formalization targets

Goal: SU(2)SU(2)SU(2) is a double covering of SO(3)SO(3)SO(3)

R: SU(2)→SO(3)  is a surjective homomorphism, and R(U)=R(W)  ⟺  W=±U(U,W∈SU(2)).R:\ SU(2)\to SO(3)\ \text{ is a surjective homomorphism, and } R(U)=R(W)\iff W=\pm U\quad(U,W\in SU(2)).R: SU(2)→SO(3)  is a surjective homomorphism, and R(U)=R(W)⟺W=±U(U,W∈SU(2)).

Concretely: R(U)∈SO(3)R(U)\in SO(3)R(U)∈SO(3) for all U∈SU(2)U\in SU(2)U∈SU(2); R(UW)=R(U)R(W)R(UW)=R(U)R(W)R(UW)=R(U)R(W); every element of SO(3)SO(3)SO(3) is some R(U)R(U)R(U); and R(U)=R(W)R(U)=R(W)R(U)=R(W) exactly when W=UW=UW=U or W=−UW=-UW=−U.

Milestones (in the book's order)

  1. −2det⁡M=tr⁡(M2)−(tr⁡M)2-2\det M=\operatorname{tr}(M^2)-(\operatorname{tr}M)^2−2detM=tr(M2)−(trM)2 (p. 111).
  2. ∣V∣2=−2det⁡V=tr⁡(V2)|V|^2=-2\det V=\operatorname{tr}(V^2)∣V∣2=−2detV=tr(V2) is real, non-negative and vanishes only at V=0V=0V=0 (p. 111).
  3. The 3-vectors are exactly the matrices V(v)V(v)V(v), and vvv is unique (p. 111).
  4. det⁡V(v)=−12∑vi2\det V(v)=-\tfrac12\sum v_i^2detV(v)=−21​∑vi2​ and tr⁡(V(v)2)=∑vi2\operatorname{tr}(V(v)^2)=\sum v_i^2tr(V(v)2)=∑vi2​ (pp. 111–112).
  5. V⋅W=det⁡V+det⁡W−det⁡(V+W)=tr⁡(VW)V\cdot W=\det V+\det W-\det(V+W)=\operatorname{tr}(VW)V⋅W=detV+detW−det(V+W)=tr(VW) and {V,W}=(V⋅W)I\{V,W\}=(V\cdot W)I{V,W}=(V⋅W)I (pp. 111–112).
  6. MCMTC=Idet⁡MMCM^TC=I\det MMCMTC=IdetM, M+CMTC=Itr⁡MM+CM^TC=I\operatorname{tr}MM+CMTC=ItrM, and tr⁡M=0  ⟺  (MC)T=MC\operatorname{tr}M=0\iff(MC)^T=MCtrM=0⟺(MC)T=MC (pp. 111–112).
  7. M2=Mtr⁡M−Idet⁡MM^2=M\operatorname{tr}M-I\det MM2=MtrM−IdetM, hence V2=−Idet⁡V=12∣V∣2IV^2=-I\det V=\tfrac12|V|^2IV2=−IdetV=21​∣V∣2I (p. 112).
  8. [V(v),V(w)]=2 i V(v×w)[V(v),V(w)]=\sqrt2\,i\,V(v\times w)[V(v),V(w)]=2​iV(v×w) (p. 112).
  9. Unitary conjugation preserves 3-vectors and their determinant (p. 114).
  10. Reality conditions V∗=−CVCV^*=-CVCV∗=−CVC and U∗=CUCU^*=CUCU∗=CUC for U∈SU(2)U\in SU(2)U∈SU(2) (pp. 114–115).
  11. cI∈SU(2)  ⟺  c=±1cI\in SU(2)\iff c=\pm1cI∈SU(2)⟺c=±1 (p. 115).
  12. U,W∈SU(2)U,W\in SU(2)U,W∈SU(2) act identically on all 3-vectors iff W=±UW=\pm UW=±U (p. 115).
  13. U V(v) U†=V(R(U)v)U\,V(v)\,U^\dagger=V(R(U)v)UV(v)U†=V(R(U)v) for unitary UUU (p. 114, component form).

Significance

The covering SU(2)→SO(3)SU(2)\to SO(3)SU(2)→SO(3) is the basic reason spinors exist. It gives the spin-12\tfrac1221​ representation, explains why a 2π2\pi2π rotation acts as −1-1−1 on fermions, and is the first instance of the low-dimensional Lie algebra identifications that Siegel lists in §IC5 (such as SO(3,1)=SL(2,C)SO(3,1)=SL(2,\mathbb C)SO(3,1)=SL(2,C) and SO(6)=SU(4)SO(6)=SU(4)SO(6)=SU(4)). Later chapters of Fields build spinor index notation, the Lorentz group and supersymmetry on this material.

The mathematics is classical and fully proved. What this mission adds is a machine-checked version stated in the book's own conventions: its basis, its normalization of the norm (∣V∣2=−2det⁡V|V|^2=-2\det V∣V∣2=−2detV) and its matrix CCC. The result is a dictionary between Siegel's matrix notation and Mathlib's matrix groups that later missions in the series can import.

Difficulty

Most milestones are identities about 2×22\times22×2 matrices and can be checked entrywise. The substantive parts of the goal are surjectivity onto SO(3)SO(3)SO(3) and the kernel computation. Showing that every rotation is some R(U)R(U)R(U) requires constructing UUU from RRR, for example from an axis and an angle or by generating SO(3)SO(3)SO(3) from simpler rotations. It cannot be done by an entrywise identity. Pinning the kernel to {±I}\{\pm I\}{±I} requires showing that a unitary matrix commuting with all of V\mathcal VV is scalar, and then combining this with det⁡U=1\det U=1detU=1. Showing det⁡R(U)=+1\det R(U)=+1detR(U)=+1 rather than ±1\pm1±1 needs either a connectedness argument or an explicit formula.

Formalization scope

  • SU(2)SU(2)SU(2) is Matrix.specialUnitaryGroup (Fin 2) ℂ and SO(3)SO(3)SO(3) is Matrix.specialOrthogonalGroup (Fin 3) ℝ. Unitary matrices are Matrix.unitaryGroup (Fin 2) ℂ.
  • rotationOf U is defined for every matrix UUU and takes the real part of a trace. The statements restrict UUU to the unitary or special unitary group, where that trace is real.
  • The cross product is Mathlib's crossProduct on Fin 3 → ℝ. The book's basis corresponds to the cyclically relabelled Pauli matrices (σ3,σ1,σ2)(\sigma_3,\sigma_1,\sigma_2)(σ3​,σ1​,σ2​), which preserves orientation.
  • Surjectivity appears in the goal because a covering map is onto. The book asserts it through the phrase "double covering" rather than proving it.
  • All statements use the same definition file, and nothing in it is assumed through hypotheses. The goal therefore cannot be satisfied by a vacuous or trivializing choice.

Contributions welcome: proofs of the matrix identities, a proof of surjectivity, and connections to Mathlib's quaternion and unit-sphere API.

Selected references

  • W. Siegel, Fields, arXiv:hep-th/9912205v3, 2005. https://arxiv.org/abs/hep-th/9912205 (Chapter II A, pp. 110–116; Chapter I C5, pp. 107–108)
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Machine LearningProbabilityStatistics·Captain: naimengye

Understanding Machine Learning XXV: PAC-BayesTextbook

Motivation

The MDL and Occam principles of Chapter 7 rank hypotheses by description length and pay for a hypothesis according to its rank. Chapter 31 of Shalev-Shwartz and Ben-David, Understanding Machine Learning: From Theory to Algorithms (doi:10.1017/CBO9781107298019), generalizes this to the PAC-Bayesian approach of McAllester: prior knowledge is a prior distribution PPP over the class, the learner outputs a posterior QQQ, read as the randomized predictor that draws h∼Qh \sim Qh∼Q, and the price of QQQ is its Kullback–Leibler divergence from PPP. The PAC-Bayes theorem (Theorem 31.1) says that with probability 1−δ1 - \delta1−δ, simultaneously for every posterior, the generalization loss exceeds the training loss by at most (D(Q∥P)+ln⁡(m/δ))/(2(m−1))\sqrt{(D(Q\|P) + \ln(m/\delta))/(2(m-1))}(D(Q∥P)+ln(m/δ))/(2(m−1))​. Its proof is a compact and elegant argument: Markov's inequality for an exponential moment, a change of measure from QQQ to PPP by Jensen's inequality, an exchange of expectations that is possible because the prior does not depend on the sample, and a moment bound for the deviation of a single hypothesis. The bound suggests the learning rule of Remark 31.1, minimize LS(Q)L_S(Q)LS​(Q) plus the divergence penalty, which is regularized risk minimization in disguise, and for a finite class with a uniform prior it recovers an Occam-type bound (Exercise 2).

Setting

HHH is a measurable space of hypotheses, ℓ:H×Z→[0,1]\ell : H \times Z \to [0,1]ℓ:H×Z→[0,1] a jointly measurable loss, DDD a distribution over ZZZ, and PPP a prior probability measure on HHH. For a posterior QQQ, ℓ(Q,z)=Eh∼Q[ℓ(h,z)]\ell(Q, z) = \mathbb{E}_{h \sim Q}[\ell(h, z)]ℓ(Q,z)=Eh∼Q​[ℓ(h,z)], LD(Q)=Eh∼Q[LD(h)]L_D(Q) = \mathbb{E}_{h \sim Q}[L_D(h)]LD​(Q)=Eh∼Q​[LD​(h)] and LS(Q)=Eh∼Q[LS(h)]L_S(Q) = \mathbb{E}_{h \sim Q}[L_S(h)]LS​(Q)=Eh∼Q​[LS​(h)], and D(Q∥P)=Eh∼Q[ln⁡(dQ/dP)]D(Q\|P) = \mathbb{E}_{h \sim Q}[\ln(dQ/dP)]D(Q∥P)=Eh∼Q​[ln(dQ/dP)] is the Kullback–Leibler divergence, a real number when Q≪PQ \ll PQ≪P and the log-density is QQQ-integrable.

Formalization targets

Goal: Theorem 31.1

For m≥2m \ge 2m≥2 and δ∈(0,1)\delta \in (0,1)δ∈(0,1), with probability at least 1−δ1 - \delta1−δ over S∼DmS \sim D^mS∼Dm, every probability measure Q≪PQ \ll PQ≪P with finite divergence satisfies

LD(Q)≤LS(Q)+D(Q∥P)+ln⁡(m/δ)2(m−1).L_D(Q) \le L_S(Q) + \sqrt{\frac{D(Q\|P) + \ln(m/\delta)}{2(m-1)}}.LD​(Q)≤LS​(Q)+2(m−1)D(Q∥P)+ln(m/δ)​​.

Milestones

The identity Ez∼D[ℓ(Q,z)]=LD(Q)\mathbb{E}_{z \sim D}[\ell(Q, z)] = L_D(Q)Ez∼D​[ℓ(Q,z)]=LD​(Q) (§31.1); the moment bound ES[e2(m−1)Δ(h)2]≤m\mathbb{E}_S[e^{2(m-1)\Delta(h)^2}] \le mES​[e2(m−1)Δ(h)2]≤m of the proof (p. 417); Exercise 2, the bound for a finite class with the uniform prior.

Significance

PAC-Bayes bounds are among the tightest generalization bounds known in practice, and the reason is visible in Theorem 31.1: the complexity term is not a property of the class but of the posterior actually chosen, measured against a prior, so a learner that stays close to its prior generalizes even in a huge class. The theorem is the ancestor of a large literature (Seeger, Langford, Catoni, Maurer) and of modern nonvacuous bounds for neural networks. Formally it is a pleasant target: the change-of-measure inequality Eh∼Q[f(h)]−D(Q∥P)≤ln⁡Eh∼P[ef(h)]\mathbb{E}_{h \sim Q}[f(h)] - D(Q\|P) \le \ln\mathbb{E}_{h \sim P}[e^{f(h)}]Eh∼Q​[f(h)]−D(Q∥P)≤lnEh∼P​[ef(h)] is the Donsker–Varadhan inequality, of independent value, and the moment bound is a sharp sub-Gaussian fact. On the platform, the mission introduces Gibbs risks and the Kullback–Leibler divergence between measures on a class, ending the book's series with its last learning principle.

Difficulty

The Gibbs risk identity is Fubini for a bounded jointly measurable function. The moment bound is the delicate step: the book derives it from Hoeffding's tail bound through Exercise 1, whose one-sided hypothesis is not enough (a constant negative variable satisfies it with an unbounded moment), and even the two-sided tail integrates only to 2m−12m - 12m−1; the claim ≤m\le m≤m is nevertheless true, for instance by writing eaΔ2=Eg[e2a gΔ]e^{a\Delta^2} = \mathbb{E}_g[e^{\sqrt{2a}\,g\Delta}]eaΔ2=Eg​[e2a​gΔ] for a standard Gaussian ggg and applying Hoeffding's lemma to the sample mean, which gives ES[e2(m−1)Δ2]≤(1−(m−1)/m)−1/2=m\mathbb{E}_S[e^{2(m-1)\Delta^2}] \le (1 - (m-1)/m)^{-1/2} = \sqrt mES​[e2(m−1)Δ2]≤(1−(m−1)/m)−1/2=m​. Theorem 31.1 then follows the book: Markov's inequality on ef(S)e^{f(S)}ef(S) with f(S)=sup⁡Q(2(m−1)Eh∼QΔ(h)2−D(Q∥P))f(S) = \sup_Q(2(m-1)\mathbb{E}_{h \sim Q}\Delta(h)^2 - D(Q\|P))f(S)=supQ​(2(m−1)Eh∼Q​Δ(h)2−D(Q∥P)), the change of measure (31.2) by Jensen's inequality for ln⁡\lnln applied to the density dQ/dPdQ/dPdQ/dP (the Donsker–Varadhan inequality, which needs Q≪PQ \ll PQ≪P and an integrable log-density), the exchange of expectations (31.4) by Fubini, the moment bound, and finally Jensen for x2x^2x2 in (31.6); formally the supremum over all posteriors is handled by proving the bound for each QQQ on the event {S:Eh∼P[e2(m−1)Δ(h)2]≤m/δ}\{S : \mathbb{E}_{h \sim P}[e^{2(m-1)\Delta(h)^2}] \le m/\delta\}{S:Eh∼P​[e2(m−1)Δ(h)2]≤m/δ}, whose complement has probability at most δ\deltaδ by Markov, which sidesteps any measurability question about fff. Exercise 2 is the theorem with Q=δhQ = \delta_hQ=δh​, for which D(Q∥P)=ln⁡∣H∣D(Q\|P) = \ln|H|D(Q∥P)=ln∣H∣.

Formalization scope

The class is an arbitrary measurable space, priors and posteriors are probability measures on it, and Q(h)/P(h)Q(h)/P(h)Q(h)/P(h) is Mathlib's Radon–Nikodym derivative; the divergence is a Bochner integral, so the theorem quantifies over posteriors Q≪PQ \ll PQ≪P whose log-density is QQQ-integrable, exactly the posteriors with a finite divergence, for which the bound has content, and no junk value can make a case false. Posteriors may depend on the sample: the statement bounds the outer measure of the set of samples for which some admissible QQQ violates the bound. The loss is jointly measurable so that h↦LD(h)h \mapsto L_D(h)h↦LD​(h) and (S,h)↦LS(h)(S, h) \mapsto L_S(h)(S,h)↦LS​(h) are measurable and the Gibbs risks are genuine integrals; m≥2m \ge 2m≥2 is forced by the denominator 2(m−1)2(m-1)2(m−1). The moment bound is stated as the claim the proof needs rather than as Exercise 1, whose printed hypothesis is insufficient; the item text records this. Exercise 2 is stated as a simultaneous bound over the finite class, the form in which the theorem delivers it.

Not stated: Remark 31.1 (a learning rule, not a theorem), Exercise 1 as printed, and the second part of Exercise 2.

Selected references

  • S. Shalev-Shwartz, S. Ben-David, Understanding Machine Learning: From Theory to Algorithms, Cambridge University Press, 2014, Chapter 31. doi:10.1017/CBO9781107298019
  • D. A. McAllester, Some PAC-Bayesian theorems, Machine Learning 37, 1999. doi:10.1023/A:1007618624809
  • D. A. McAllester, PAC-Bayesian stochastic model selection, Machine Learning 51, 2003. doi:10.1023/A:1021840411064
  • A. Maurer, A note on the PAC Bayesian theorem, arXiv:cs/0411099, 2004.
  • M. Seeger, PAC-Bayesian generalisation error bounds for Gaussian process classification, Journal of Machine Learning Research 3, 2002.
  • J. Langford, J. Shawe-Taylor, PAC-Bayes and margins, NIPS 2002.
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CombinatoricsMachine LearningOptimization·Captain: naimengye

Understanding Machine Learning XV: Neural NetworksTextbook

Motivation

A feedforward neural network is a directed acyclic graph of neurons, each computing a fixed scalar activation of a weighted sum of its inputs; fixing the graph and the activation and letting the weights vary gives a hypothesis class. Chapter 20 of Shalev-Shwartz and Ben-David, Understanding Machine Learning: From Theory to Algorithms (doi:10.1017/CBO9781107298019), studies these classes through the book's three lenses. Approximation: every Boolean function is implemented by a network of depth 2 (Claim 20.1), but only at exponential size (Theorem 20.2), while a sign neuron implements conjunctions and disjunctions (Lemma 20.4), the bridge to Boolean circuits and hence to everything computable in bounded time. Estimation: the VC dimension of the class of sign networks over a graph with ∣E∣|E|∣E∣ edges is O(∣E∣log⁡∣E∣)O(|E|\log|E|)O(∣E∣log∣E∣) (Theorem 20.6), so the sample complexity is governed by the number of weights. Optimization: training is NP-hard even for tiny networks, and the practical answer is SGD with the gradient computed by backpropagation, whose correctness the chapter derives from the chain rule.

Setting

A layered graph has layers V0,…,VTV_0, \dots, V_TV0​,…,VT​, every edge joining Vt−1V_{t-1}Vt−1​ to VtV_tVt​; V0V_0V0​ holds the nnn inputs and a constant neuron outputting 111. With weights w:E→Rw : E \to \mathbb{R}w:E→R and an activation σ\sigmaσ, the outputs are computed layer by layer, at+1,i=∑j:(vt,j,vt+1,i)∈Ewt,i,j ot,ja_{t+1,i} = \sum_{j : (v_{t,j}, v_{t+1,i}) \in E} w_{t,i,j}\,o_{t,j}at+1,i​=∑j:(vt,j​,vt+1,i​)∈E​wt,i,j​ot,j​ and ot+1,i=σ(at+1,i)o_{t+1,i} = \sigma(a_{t+1,i})ot+1,i​=σ(at+1,i​). The class HV,E,σ={hV,E,σ,w:w:E→R}H_{V,E,\sigma} = \{h_{V,E,\sigma,w} : w : E \to \mathbb{R}\}HV,E,σ​={hV,E,σ,w​:w:E→R} (20.1); for binary classification the output layer is a single neuron and σ\sigmaσ is the sign function, so HV,E,sign⁡H_{V,E,\operatorname{sign}}HV,E,sign​ is a set of {±1}\{\pm1\}{±1}-valued predictors on Rn\mathbb{R}^nRn. The size of the network is ∣V∣|V|∣V∣, its depth TTT. The growth function τH(m)=max⁡∣C∣≤m∣HC∣\tau_H(m) = \max_{|C| \le m}|H_C|τH​(m)=max∣C∣≤m​∣HC​∣ extends to classes with any finite codomain (p. 275), and the proof of Theorem 20.6 uses two of its properties, stated as Exercises 3 and 4: the growth function of a product class is at most the product of the growth functions, and likewise for a composition class. For backpropagation the activation is any differentiable σ\sigmaσ and the loss is 12∥oT−y∥2\frac12\|o_T - y\|^221​∥oT​−y∥2; the backward pass sets δT=oT−y\delta_T = o_T - yδT​=oT​−y and δt=δt+1diag⁡(σ′(at+1))Wt\delta_t = \delta_{t+1}\operatorname{diag}(\sigma'(a_{t+1}))W_tδt​=δt+1​diag(σ′(at+1​))Wt​.

Formalization targets

Goal: Theorem 20.6

The VC dimension of HV,E,sign⁡H_{V,E,\operatorname{sign}}HV,E,sign​ is O(∣E∣log⁡∣E∣)O(|E|\log|E|)O(∣E∣log∣E∣). Explicitly, for a layered graph of depth at least 111 with a single output neuron,

VCdim⁡(HV,E,sign⁡)≤2∣E∣log⁡2(16∣E∣),\operatorname{VCdim}(H_{V,E,\operatorname{sign}}) \le 2|E|\log_2(16|E|),VCdim(HV,E,sign​)≤2∣E∣log2​(16∣E∣),

stated as: every m≤VCdim⁡m \le \operatorname{VCdim}m≤VCdim satisfies this bound (so the VC dimension is finite).

Milestones

Claim 20.1 (the depth-2 graph with ∣V1∣=2n+1|V_1| = 2^n + 1∣V1​∣=2n+1 whose sign class contains every function {±1}n→{±1}\{\pm1\}^n \to \{\pm1\}{±1}n→{±1}); Theorem 20.2 (every sign network implementing all functions {0,1}n→{0,1}\{0,1\}^n \to \{0,1\}{0,1}n→{0,1} has 2n/3≤2∣V∣2^{n/3} \le 2|V|2n/3≤2∣V∣); Lemma 20.4 (conjunction and disjunction as sign neurons); Exercise 4 (growth function of a composition); the correctness of backpropagation (§20.6: the partial derivative for the edge (vt,j,vt+1,i)(v_{t,j}, v_{t+1,i})(vt,j​,vt+1,i​) is δt+1,iσ′(at+1,i)ot,j\delta_{t+1,i}\sigma'(a_{t+1,i})o_{t,j}δt+1,i​σ′(at+1,i​)ot,j​). Further items: Exercise 3 (growth function of a product) and the intermediate bound τH(m)≤(em)∣E∣\tau_H(m) \le (em)^{|E|}τH​(m)≤(em)∣E∣ of the proof of Theorem 20.6.

Significance

Theorem 20.6 is the reason networks are learnable at all in the book's sense: by the fundamental theorem, a class with finite VC dimension is agnostic PAC learnable with sample complexity linear in that dimension, and here the dimension is essentially the number of tunable parameters. The proof technique, due to Kakade and Tewari's lecture notes, is a composition-and-product argument on growth functions that applies to any layered class of threshold units and is reusable well beyond this chapter. Theorem 20.2 is the matching negative fact on expressive power, and it is a corollary of the same bound: a class that shatters 2n2^n2n points needs Ω(2n)\Omega(2^n)Ω(2n) edges. Backpropagation's correctness is the one theorem about training the chapter can offer, given the hardness results, and it is the algorithm every practitioner runs.

Difficulty

Claim 20.1 and Lemma 20.4 are explicit constructions: the neuron gi(x)=sign⁡(⟨x,ui⟩−n+1)g_i(x) = \operatorname{sign}(\langle x, u_i\rangle - n + 1)gi​(x)=sign(⟨x,ui​⟩−n+1) detects x=uix = u_ix=ui​ because ⟨x,ui⟩≤n−2\langle x, u_i\rangle \le n - 2⟨x,ui​⟩≤n−2 otherwise, and the output neuron takes the disjunction; formally one must build the weight function and evaluate the forward pass on the 2n2^n2n inputs. Exercises 3 and 4 are counting: a restricted product is determined by its two restricted factors, and a restricted composition f2∘f1f_2 \circ f_1f2​∘f1​ on CCC is determined by f1∣Cf_1|_Cf1​∣C​ and f2∣f1(C)f_2|_{f_1(C)}f2​∣f1​(C)​, with ∣f1(C)∣≤∣C∣|f_1(C)| \le |C|∣f1​(C)∣≤∣C∣. Theorem 20.6 then needs: the class of one neuron is the class of homogenous halfspaces on its dt,id_{t,i}dt,i​ incoming coordinates, of VC dimension at most dt,id_{t,i}dt,i​ (Mission VI), Sauer's lemma in the form τ(m)≤(em)d\tau(m) \le (em)^{d}τ(m)≤(em)d for every m≥1m \ge 1m≥1 (Mission IV; for m≤dm \le dm≤d use 2m≤(em)m2^m \le (em)^m2m≤(em)m), the layer class as a product and the network as a composition of layer classes, and finally the arithmetic 2m≤(em)∣E∣⇒m≤2∣E∣log⁡2(16∣E∣)2^m \le (em)^{|E|} \Rightarrow m \le 2|E|\log_2(16|E|)2m≤(em)∣E∣⇒m≤2∣E∣log2​(16∣E∣), which replaces the book's appeal to Lemma A.2 (for m≥8∣E∣m \ge 8|E|m≥8∣E∣ one has ln⁡m≤mln⁡22∣E∣\ln m \le \frac{m\ln 2}{2|E|}lnm≤2∣E∣mln2​). Theorem 20.2 follows from the goal with ∣E∣≤∣V∣2|E| \le |V|^2∣E∣≤∣V∣2. Backpropagation is a chain-rule computation in a single real variable: the loss as a function of one weight is a composition of finitely many differentiable maps, and the derivative unwinds to the backward recursion; the formal effort is in the induction along layers with the natural-number indexing of the model.

Formalization scope

Layers and neurons are indexed by natural numbers: a LayeredGraph records the depth, the layer widths and, for each t<Tt < Tt<T, the finite set of edges (vt,j,vt+1,i)(v_{t,j}, v_{t+1,i})(vt,j​,vt+1,i​) as pairs (i,j)(i, j)(i,j) within the layer widths. Weights are functions on all index triples, and only those on edges are used, so the class is the image of all weight functions, as in (20.1). The forward computation netOutput is a recursion on the layer index; netInput is at+1,ia_{t+1,i}at+1,i​. The sign activation returns ±1\pm1±1 with sign⁡(0)=−1\operatorname{sign}(0) = -1sign(0)=−1, the book's convention elsewhere, and a neuron with no incoming edges outputs σ(0)\sigma(0)σ(0) (p. 270). The binary class signNetClass n G is Bool-valued, true iff the output neuron's input is positive, and is stated for graphs of depth at least 111 (for depth 000 the edges out of the input layer would be used but not counted in ∣E∣|E|∣E∣). Growth functions with finite codomain are growthY, an sSup over restriction sizes, well defined because the codomains are finite; the Bool case is Mission IV's growth, and VC dimension and shattering are Mission IV's. Theorem 20.6 and Theorem 20.2 are given with explicit constants derived from the proof, since O(⋅)O(\cdot)O(⋅) statements have no formal content; the drafter verified max⁡{m:2m≤(em)∣E∣}≤2∣E∣log⁡2(16∣E∣)\max\{m : 2^m \le (em)^{|E|}\} \le 2|E|\log_2(16|E|)max{m:2m≤(em)∣E∣}≤2∣E∣log2​(16∣E∣) numerically for ∣E∣|E|∣E∣ up to 300030003000 and at 104,…,10710^4, \dots, 10^7104,…,107, and 2n≤2∣V∣2log⁡2(16∣V∣2)≤8∣V∣32^n \le 2|V|^2\log_2(16|V|^2) \le 8|V|^32n≤2∣V∣2log2​(16∣V∣2)≤8∣V∣3. Backpropagation is stated for an arbitrary layered graph (phantom edges have weight 000, p. 279), any differentiable activation, and one edge at a time as a HasDerivAt of the loss in that weight; δt\delta_tδt​ is defined by recursion on T−tT - tT−t. The book's layer indices in (20.3) are shifted by one in the statement.

Not stated: Theorem 20.3 (Turing machines), Theorem 20.5 and Exercise 1 (sigmoid approximation, which needs a convention for outputs in [−1,1][-1,1][−1,1] that the chapter leaves open), Theorem 20.7 and Exercise 6 (NP-hardness), Exercise 5 (the Ω(∣E∣2)\Omega(|E|^2)Ω(∣E∣2) sigmoid lower bound, which assumes an exact threshold), the sigmoid half of Theorem 20.2, and the SGD pseudocode of §20.6, which is a heuristic without a stated guarantee.

Selected references

  • S. Shalev-Shwartz, S. Ben-David, Understanding Machine Learning: From Theory to Algorithms, Cambridge University Press, 2014, Chapter 20. doi:10.1017/CBO9781107298019
  • M. Anthony, P. L. Bartlett, Neural Network Learning: Theoretical Foundations, Cambridge University Press, 1999. doi:10.1017/CBO9780511624216
  • D. E. Rumelhart, G. E. Hinton, R. J. Williams, Learning representations by back-propagating errors, Nature 323, 1986. doi:10.1038/323533a0
  • I. Parberry, Circuit Complexity and Neural Networks, MIT Press, 1994.
  • E. B. Baum, D. Haussler, What size net gives valid generalization?, Neural Computation 1(1), 1989. doi:10.1162/neco.1989.1.1.151
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Mathematical PhysicsQuantum Information·Captain: Lucas

Albers–Kiefer–Reginatto 2008: Measurement Analysis and Quantum GravityResearch Paper

Motivation

Whether the gravitational field must be quantized is a long-standing foundational question. A well-known family of arguments tries to settle it by consistency alone: if a classical field were coupled to a quantum system, some basic principle — momentum conservation, the uncertainty relations, or the impossibility of superluminal signalling — would allegedly be violated. The two best-known versions are the gedanken experiment of Eppley and Hannah (1977) and the measurement-theoretic argument of DeWitt (1962).

Albers, Kiefer and Reginatto (Phys. Rev. D 78, 064051 (2008)) re-examine both arguments. Their paper is largely conceptual, but several of its steps are precise, checkable mathematical claims. This mission collects those claims and makes them machine-checkable.

Timeline.

  • 1962 — DeWitt's measurement analysis of the gravitational field, using Peierls brackets and a "universal principle" for apparatus uncertainties.
  • 1977 — Eppley and Hannah's gedanken experiment: a classical gravitational wave scattered off a quantum particle would imply momentum non-conservation, a violation of the uncertainty principle, or superluminal signalling.
  • 2008 — Albers, Kiefer and Reginatto argue that neither gedanken experiment forces quantization, and exhibit a consistent hybrid classical–quantum model.

Setting

Photon pair and detector (Sec. II). Each photon carries a polarization qubit with orthonormal basis ∣↑⟩|\uparrow\rangle∣↑⟩ (horizontal) and ∣↓⟩|\downarrow\rangle∣↓⟩ (vertical). A detector with state space H\mathcal HH (an arbitrary complex inner-product space) is coupled to photon 1. Before the measurement the joint state of photon 1, photon 2 and the detector is

∣Ψ0⟩=12(∣↑⟩1∣↓⟩2−∣↓⟩1∣↑⟩2)∣Φ0⟩,(1)|\Psi_0\rangle = \tfrac{1}{\sqrt2}\bigl(|\uparrow\rangle_1|\downarrow\rangle_2 - |\downarrow\rangle_1|\uparrow\rangle_2\bigr)|\Phi_0\rangle, \qquad (1)∣Ψ0​⟩=2​1​(∣↑⟩1​∣↓⟩2​−∣↓⟩1​∣↑⟩2​)∣Φ0​⟩,(1)

and after the detector has measured photon 1 it is

∣Ψ⟩=12(∣↑⟩1∣↓⟩2∣Φ↑⟩−∣↓⟩1∣↑⟩2∣Φ↓⟩).(2)|\Psi\rangle = \tfrac{1}{\sqrt2}\bigl(|\uparrow\rangle_1|\downarrow\rangle_2|\Phi_\uparrow\rangle - |\downarrow\rangle_1|\uparrow\rangle_2|\Phi_\downarrow\rangle\bigr). \qquad (2)∣Ψ⟩=2​1​(∣↑⟩1​∣↓⟩2​∣Φ↑​⟩−∣↓⟩1​∣↑⟩2​∣Φ↓​⟩).(2)

The reduced density operator of photon 2 is obtained from ∣Ψ⟩⟨Ψ∣|\Psi\rangle\langle\Psi|∣Ψ⟩⟨Ψ∣ by tracing out photon 1 and the detector; the paper asserts that for both states it equals

ρ^=12(∣↑⟩2⟨↑∣2+∣↓⟩2⟨↓∣2).(3)\hat\rho = \tfrac12\bigl(|\uparrow\rangle_2\langle\uparrow|_2 + |\downarrow\rangle_2\langle\downarrow|_2\bigr). \qquad (3)ρ^​=21​(∣↑⟩2​⟨↑∣2​+∣↓⟩2​⟨↓∣2​).(3)

Mass cube and gravitational wave (Sec. III B). The disturbance δT00GW\delta T^{\mathrm{GW}}_{00}δT00GW​ of the averaged energy density of the scattered wave depends on the cube's edge length aaa and speed vvv, with sensitivities Ta=∂ δT00GW/∂aT_a = \partial\,\delta T^{\mathrm{GW}}_{00}/\partial aTa​=∂δT00GW​/∂a and Tv=∂ δT00GW/∂vT_v = \partial\,\delta T^{\mathrm{GW}}_{00}/\partial vTv​=∂δT00GW​/∂v. With Δa≈Δx\Delta a \approx \Delta xΔa≈Δx and Δv≳ℏ/(2mΔx)\Delta v \gtrsim \hbar/(2m\Delta x)Δv≳ℏ/(2mΔx) the uncertainty ΔT00GW=(TaΔa)2+(TvΔv)2\Delta T^{\mathrm{GW}}_{00} = \sqrt{(T_a\Delta a)^2 + (T_v\Delta v)^2}ΔT00GW​=(Ta​Δa)2+(Tv​Δv)2​ has a strictly positive lower bound.

DeWitt's argument (Sec. V). A system observable sss reconstructed from apparatus data has uncertainty Δs2=ΔA2/g2+g2(ΔDΩs)2\Delta s^2 = \Delta A^2/g^2 + g^2(\Delta D_\Omega s)^2Δs2=ΔA2/g2+g2(ΔDΩ​s)2, where ggg is the coupling constant.

Formalization targets

Goal — no signalling through photon 2 (Eq. (3))

For all unit vectors Φ0,Φ↑,Φ↓∈H\Phi_0, \Phi_\uparrow, \Phi_\downarrow \in \mathcal HΦ0​,Φ↑​,Φ↓​∈H,

ρ2(Ψ0)=ρ^andρ2(Ψ)=ρ^.\rho_2(\Psi_0) = \hat\rho \quad\text{and}\quad \rho_2(\Psi) = \hat\rho .ρ2​(Ψ0​)=ρ^​andρ2​(Ψ)=ρ^​.

Milestones

  1. Eq. (1) ⇒ (3): ρ2(Ψ0)=ρ^\rho_2(\Psi_0) = \hat\rhoρ2​(Ψ0​)=ρ^​.
  2. Eq. (2) ⇒ (3): ρ2(Ψ)=ρ^\rho_2(\Psi) = \hat\rhoρ2​(Ψ)=ρ^​.
  3. Sec. III B lower bound: ΔT00GW≥ℏmTvTa\Delta T^{\mathrm{GW}}_{00} \ge \sqrt{\tfrac{\hbar}{m} T_v T_a}ΔT00GW​≥mℏ​Tv​Ta​​ whenever Δx>0\Delta x > 0Δx>0 and Δv≥ℏ/(2mΔx)\Delta v \ge \hbar/(2m\Delta x)Δv≥ℏ/(2mΔx).
  4. Sec. III B optimum: the function Δx↦(TaΔx)2+(Tvℏ/(2mΔx))2\Delta x \mapsto \sqrt{(T_a\Delta x)^2 + (T_v\hbar/(2m\Delta x))^2}Δx↦(Ta​Δx)2+(Tv​ℏ/(2mΔx))2​ attains its minimum over Δx>0\Delta x>0Δx>0 at Δxmin⁡=ℏ2mTvTa\Delta x_{\min} = \sqrt{\tfrac{\hbar}{2m}\tfrac{T_v}{T_a}}Δxmin​=2mℏ​Ta​Tv​​​, with value ℏmTvTa\sqrt{\tfrac{\hbar}{m}T_vT_a}mℏ​Tv​Ta​​.
  5. Eq. (61): min⁡g≠0ΔA2/g2+g2ΔD2=2 ΔA ΔD\min_{g\ne0}\sqrt{\Delta A^2/g^2 + g^2\Delta D^2} = \sqrt{2\,\Delta A\,\Delta D}ming=0​ΔA2/g2+g2ΔD2​=2ΔAΔD​.
  6. Eq. (64): if ΔA ΔC≥ℏ/2\Delta A\,\Delta C \ge \hbar/2ΔAΔC≥ℏ/2 then ℏ ∣Dss∣≤2 ΔA ΔC ∣Dss∣\sqrt{\hbar\,|D_s s|} \le \sqrt{2\,\Delta A\,\Delta C\,|D_s s|}ℏ∣Ds​s∣​≤2ΔAΔC∣Ds​s∣​.

Significance

The goal is the precise content of the paper's rebuttal of the superluminal-signalling branch of the Eppley–Hannah argument: the state of photon 2 accessible to a probe (such as a classical gravitational wave) is the same whether or not photon 1 has been measured, so a probe of photon 2 alone cannot tell whether photon 1 was measured. Milestones 3–6 are the quantitative estimates the paper uses in Sec. III B (a coupling to a test body obeying the uncertainty principle transfers a minimum uncertainty to the classical wave) and Sec. V (DeWitt's limitation on a single observable, Eq. (64)).

The results are elementary once stated; the value of the mission is to pin the paper's claims down exactly, including the hypotheses under which they hold. None of the statements has, to our knowledge, a machine-checked proof on the platform.

Difficulty

The goal and Milestones 1–2 need a workable representation of the partial trace over a factor that is an arbitrary (possibly infinite-dimensional) inner-product space; the cross terms between the two branches vanish because the two branches are orthogonal on photon 1, not because of any property of the detector states. Milestones 3–6 are single-variable optimization statements; the main care is in the side conditions (positivity, excluding g=0g=0g=0 and Δx=0\Delta x = 0Δx=0).

Formalization scope

  • The joint space C2⊗C2⊗H\mathbb C^2\otimes\mathbb C^2\otimes\mathcal HC2⊗C2⊗H is represented by functions {0,1}×{0,1}→H\{0,1\}\times\{0,1\}\to\mathcal H{0,1}×{0,1}→H (component Ψij\Psi_{ij}Ψij​ along ∣i⟩1∣j⟩2|i\rangle_1|j\rangle_2∣i⟩1​∣j⟩2​; index 0=↑0 = \uparrow0=↑, 1=↓1 = \downarrow1=↓). The reduced density matrix of photon 2 has entries ρ2(j,j′)=∑i⟨Ψij′,Ψij⟩H\rho_2(j,j') = \sum_i \langle \Psi_{ij'}, \Psi_{ij}\rangle_{\mathcal H}ρ2​(j,j′)=∑i​⟨Ψij′​,Ψij​⟩H​, and ρ^\hat\rhoρ^​ is a 2×22\times22×2 complex matrix.
  • The detector states are only assumed to be unit vectors. Orthogonality of ∣Φ↑⟩|\Phi_\uparrow\rangle∣Φ↑​⟩ and ∣Φ↓⟩|\Phi_\downarrow\rangle∣Φ↓​⟩ (a physical property of a detector that records the outcome) is not assumed, because Eq. (3) does not depend on it.
  • In Sec. III B the sensitivities Ta,TvT_a, T_vTa​,Tv​, the mass mmm and ℏ\hbarℏ are positive reals; the paper's approximate relations Δa≈Δx\Delta a\approx\Delta xΔa≈Δx and Δp≳ℏ/Δx\Delta p\gtrsim\hbar/\Delta xΔp≳ℏ/Δx are encoded as Δa=Δx\Delta a = \Delta xΔa=Δx and the hypothesis Δv≥ℏ/(2mΔx)\Delta v \ge \hbar/(2m\Delta x)Δv≥ℏ/(2mΔx).
  • In Eq. (61) the coupling constant ranges over all non-zero reals.
  • Sections IV (hybrid classical–quantum ensembles for Nordström gravity) and the appendices are out of scope for this mission.

Selected references

  • M. Albers, C. Kiefer, M. Reginatto, Measurement analysis and quantum gravity, Phys. Rev. D 78, 064051, 2008. https://doi.org/10.1103/PhysRevD.78.064051
  • K. Eppley, E. Hannah, The necessity of quantizing the gravitational field, Found. Phys. 7, 51–68, 1977. https://doi.org/10.1007/BF00715241
  • B. S. DeWitt, Definition of commutators via the uncertainty principle, J. Math. Phys. 3, 619, 1962. https://doi.org/10.1063/1.1724265
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Machine LearningProbability·Captain: Lucas

The Principles of Deep Learning Theory I: Wick's Theorem for Gaussian IntegralsTextbook

Motivation

The book The Principles of Deep Learning Theory by D. A. Roberts and S. Yaida (arXiv:2106.10165) develops a perturbative, physics-style theory of wide deep neural networks. Every later computation in the book, from the statistics of preactivations at initialization to the neural tangent kernel, reduces to Gaussian expectations of polynomials. The single tool that evaluates these expectations is Wick's theorem (eq. 1.45), which the authors ask the reader to "put a box around". This mission formalizes Chapter 1, §1.1 (Gaussian Integrals), culminating in that theorem. It is the first mission of a series formalizing the book, all in the Lean namespace DeepLearningTheory.

Setting

Fix N≥0N \ge 0N≥0 and a symmetric positive-definite real N×NN\times NN×N matrix K=(Kμν)K = (K_{\mu\nu})K=(Kμν​), the covariance. Write Kμν=(K−1)μνK^{\mu\nu} = (K^{-1})_{\mu\nu}Kμν=(K−1)μν​ for its inverse. The zero-mean multivariable Gaussian distribution with covariance KKK (eq. 1.31) has density on RN\mathbb{R}^NRN

p(z)=1∣2πK∣exp⁡(−12∑μ,ν=1NzμKμνzν),∣2πK∣=det⁡(2πK)=(2π)Ndet⁡K,p(z) = \frac{1}{\sqrt{|2\pi K|}} \exp\Big(-\tfrac12 \sum_{\mu,\nu=1}^N z_\mu K^{\mu\nu} z_\nu\Big), \qquad |2\pi K| = \det(2\pi K) = (2\pi)^N \det K,p(z)=∣2πK∣​1​exp(−21​μ,ν=1∑N​zμ​Kμνzν​),∣2πK∣=det(2πK)=(2π)NdetK,

and the expectation of an observable FFF is E[F(z)]=∫dNz p(z)F(z)\mathbb{E}[F(z)] = \int d^N z\, p(z) F(z)E[F(z)]=∫dNzp(z)F(z) (eqs. 1.36, 1.46), an integral against Lebesgue measure. A pairing of the labels 1,…,2m1,\dots,2m1,…,2m is a partition into mmm unordered pairs; equivalently, a fixed-point-free involution σ\sigmaσ of {1,…,2m}\{1,\dots,2m\}{1,…,2m} pairing aaa with σ(a)\sigma(a)σ(a). There are (2m−1)!!(2m-1)!!(2m−1)!! pairings.

Formalization targets

Goal: Wick's theorem (eq. 1.45)

For all indices μ1,…,μ2m∈{1,…,N}\mu_1,\dots,\mu_{2m} \in \{1,\dots,N\}μ1​,…,μ2m​∈{1,…,N} (repetitions allowed),

E[zμ1⋯zμ2m]=∑pairings σ ∏a<σ(a)Kμaμσ(a).\mathbb{E}[z_{\mu_1}\cdots z_{\mu_{2m}}] = \sum_{\text{pairings } \sigma}\ \prod_{a<\sigma(a)} K_{\mu_a \mu_{\sigma(a)}}.E[zμ1​​⋯zμ2m​​]=pairings σ∑​ a<σ(a)∏​Kμa​μσ(a)​​.

Milestones

  1. Eq. (1.30) — the normalization ∫dNz e−12z⊤K−1z=∣2πK∣\int d^N z\, e^{-\frac12 z^\top K^{-1} z} = \sqrt{|2\pi K|}∫dNze−21​z⊤K−1z=∣2πK∣​.
  2. Eq. (1.41) — the generating function ∫dNz e−12z⊤K−1z+J⋅z=∣2πK∣ e12J⊤KJ\int d^N z\, e^{-\frac12 z^\top K^{-1} z + J\cdot z} = \sqrt{|2\pi K|}\, e^{\frac12 J^\top K J}∫dNze−21​z⊤K−1z+J⋅z=∣2πK∣​e21​J⊤KJ for every source J∈RNJ \in \mathbb{R}^NJ∈RN.
  3. Odd moments vanish (p. 22, discussion after eq. 1.42).
  4. Eq. (1.43) — E[zμ1zμ2]=Kμ1μ2\mathbb{E}[z_{\mu_1} z_{\mu_2}] = K_{\mu_1\mu_2}E[zμ1​​zμ2​​]=Kμ1​μ2​​.
  5. Eq. (1.44) — E[zμ1zμ2zμ3zμ4]=Kμ1μ2Kμ3μ4+Kμ1μ3Kμ2μ4+Kμ1μ4Kμ2μ3\mathbb{E}[z_{\mu_1}z_{\mu_2}z_{\mu_3}z_{\mu_4}] = K_{\mu_1\mu_2}K_{\mu_3\mu_4} + K_{\mu_1\mu_3}K_{\mu_2\mu_4} + K_{\mu_1\mu_4}K_{\mu_2\mu_3}E[zμ1​​zμ2​​zμ3​​zμ4​​]=Kμ1​μ2​​Kμ3​μ4​​+Kμ1​μ3​​Kμ2​μ4​​+Kμ1​μ4​​Kμ2​μ3​​.

Significance

Wick's theorem (also known as Isserlis' theorem, 1918) is used throughout the book: the Gaussianity of the first layer (Chapter 4), the four-point correlators of deep linear networks (Chapter 3), and all perturbative expansions around the infinite-width limit are evaluated by Wick contractions. A machine-checked version stated in the book's own density-based conventions gives later missions of this series a dependable foundation. The result is classical; the work remaining is its formalization in exactly this form. A related statement for general (possibly degenerate) Gaussian measures already exists on the platform as FeynmanWick.wick_theorem_gaussian; the present mission keeps the book's formulation via the explicit density and a positive-definite covariance.

Difficulty

The book's derivation differentiates the generating function (1.41) 2m2m2m times at J=0J=0J=0, which requires justifying differentiation under the integral sign and organizing the combinatorics of the product rule into pairings. Both the analytic step (dominated convergence for Gaussian tails, in NNN dimensions) and the combinatorial step (a bijection between surviving terms and pairings, with the 1/(2mm!)1/(2^m m!)1/(2mm!) normalization) are routine on paper but need care in Lean. Computing the normalization (1.30) itself requires diagonalizing KKK and a linear change of variables.

Formalization scope

  • Vectors are functions Fin N → ℝ with Lebesgue measure; KKK is a Matrix (Fin N) (Fin N) ℝ with K.PosDef (which includes symmetry). The inverse is Mathlib's K⁻¹.
  • gaussianDensity K z and gaussExpect K F are exactly the book's p(z)p(z)p(z) and E[F]\mathbb{E}[F]E[F]; gaussQuadForm K z is ∑zμKμνzν\sum z_\mu K^{\mu\nu} z_\nu∑zμ​Kμνzν​.
  • pairings (2m) is the finite set of fixed-point-free involutions of Fin (2m); the product is over labels aaa with a<σ(a)a<\sigma(a)a<σ(a), so each pair contributes once.
  • Positive definiteness is assumed exactly as in the book; no statement is vacuous since, e.g., K=IK = IK=I satisfies every hypothesis.

Selected references

  • D. A. Roberts, S. Yaida (with B. Hanin), The Principles of Deep Learning Theory, Cambridge University Press, 2022. arXiv:2106.10165
  • L. Isserlis, On a formula for the product-moment coefficient of any order of a normal frequency distribution in any number of variables, Biometrika 12 (1918). doi:10.1093/biomet/12.1-2.134
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Mathematical PhysicsPartial Differential Equations·Captain: Lucas

Analytic toroidal 3D MHD equilibria with nested flux surfaces (Landreman 2026)Research Paper

Motivation

A magnetohydrodynamic (MHD) equilibrium is a magnetic field BBB and a scalar pressure ppp on a region of R3\mathbb R^3R3 satisfying

(∇×B)×B=∇p,∇⋅B=0.(\nabla\times B)\times B=\nabla p,\qquad \nabla\cdot B=0 .(∇×B)×B=∇p,∇⋅B=0.

Under the substitution B↦uB\mapsto uB↦u these are exactly the equations of a steady incompressible Euler flow, with ppp replaced by the Bernoulli function, so every statement in this mission is simultaneously a statement about stationary solutions of the 3D Euler equations. Magnetic confinement of a fusion plasma requires equilibria whose pressure surfaces are nested tori, because B⋅∇p=0B\cdot\nabla p=0B⋅∇p=0 forces ppp to be constant on the surfaces swept out by field lines.

Whether such equilibria exist without a continuous symmetry has been open since Grad, who conjectured in 1967 that smooth toroidal equilibria with non-constant pressure do not exist unless the configuration is symmetric (for instance axisymmetric), and restated the claim in 1985 as the assertion that, apart from the symmetric exceptions, there are no families of solutions depending smoothly on a parameter. Modern formulations of the conjecture appear in the work of Constantin–Drivas–Ginsberg (2021), Enciso–Luque–Peralta-Salas (2025) and Cardona–Duignan–Perrella (2025, Conjecture 2.5). Partial results have always relaxed something: Lortz (1970) obtained non-symmetric toroidal equilibria only with mirror symmetry and vanishing rotational transform; Bruno–Laurence (1996) and Enciso–Luque–Peralta-Salas (2025) allow discontinuous pressure and current sheets; Weitzner–Sengupta (2020) work in a topological torus rather than true toroidal geometry; near-axis and high-aspect-ratio expansions (Mercier 1964, Garren–Boozer 1991) give only approximate solutions.

Landreman (2026) exhibits explicit, fully non-axisymmetric, smooth analytic solutions on a genuine solid torus, with exact nested flux surfaces, finite aspect ratio and non-zero rotational transform. This mission formalizes the first of the two families presented there — the family with uniform rotational transform ι=2\iota=2ι=2 — in Lean 4.

Setting

Fix a parameter 0<ϵ<10<\epsilon<10<ϵ<1 and set a=1+ϵa=\sqrt{1+\epsilon}a=1+ϵ​, b=1−ϵb=\sqrt{1-\epsilon}b=1−ϵ​. For a Cartesian point x=(x0,x1,x2)x=(x_0,x_1,x_2)x=(x0​,x1​,x2​) (written (x,y,z)(x,y,z)(x,y,z) in the paper) define

s=x02a2+x12b2,F=1−(1−s)2−4x22,s=\frac{x_0^2}{a^2}+\frac{x_1^2}{b^2},\qquad F=\sqrt{1-(1-s)^2-4x_2^2},s=a2x02​​+b2x12​​,F=1−(1−s)2−4x22​​,

and the vector field

B=(2x2x0−(a/b)Fx1s, 2x2x1+(b/a)Fx0s, 1−s).B=\left(\frac{2x_2x_0-(a/b)Fx_1}{s},\ \frac{2x_2x_1+(b/a)Fx_0}{s},\ 1-s\right).B=(s2x2​x0​−(a/b)Fx1​​, s2x2​x1​+(b/a)Fx0​​, 1−s).

The natural domain is the open set Uϵ={x:1−(1−s)2−4x22>0}U_\epsilon=\{x: 1-(1-s)^2-4x_2^2>0\}Uϵ​={x:1−(1−s)2−4x22​>0}, on which s>0s>0s>0 and all the expressions above are smooth. With

Q=x02+x12+4x222,H=Q+∣B∣22,Q=\frac{x_0^2+x_1^2+4x_2^2}{2},\qquad H=Q+\frac{|B|^2}{2},Q=2x02​+x12​+4x22​​,H=Q+2∣B∣2​,

the flux label and the pressure are

ψ=H−1+ϵ2/22,p=pa−2ψ,\psi=\frac{H-1+\epsilon^2/2}{2},\qquad p=p_a-2\psi ,ψ=2H−1+ϵ2/2​,p=pa​−2ψ,

where pap_apa​ is an arbitrary constant. The level sets of ψ\psiψ are the pressure surfaces. For 0<δ<(1−ϵ)2/40<\delta<(1-\epsilon)^2/40<δ<(1−ϵ)2/4 the region Ωδ={x∈Uϵ:ψ≤δ}\Omega_\delta=\{x\in U_\epsilon:\psi\le\delta\}Ωδ​={x∈Uϵ​:ψ≤δ} is a solid torus bounded by a ψ\psiψ-surface, and this is the plasma domain.

Field lines are described by a second coordinate system. For labels (u,v)(u,v)(u,v) with u2+v2<1/4u^2+v^2<1/4u2+v2<1/4, putting q2=u2+v2q^2=u^2+v^2q2=u2+v2 and L=((1+1−4q2)/2)1/2L=\big((1+\sqrt{1-4q^2})/2\big)^{1/2}L=((1+1−4q2​)/2)1/2, the position map is

r(u,v,ζ)=(a[Lcos⁡ζ+ucos⁡ζ+vsin⁡ζL], b[Lsin⁡ζ+vcos⁡ζ−usin⁡ζL], vcos⁡2ζ−usin⁡2ζ).r(u,v,\zeta)=\Big(a\big[L\cos\zeta+\tfrac{u\cos\zeta+v\sin\zeta}{L}\big],\ b\big[L\sin\zeta+\tfrac{v\cos\zeta-u\sin\zeta}{L}\big],\ v\cos2\zeta-u\sin2\zeta\Big).r(u,v,ζ)=(a[Lcosζ+Lucosζ+vsinζ​], b[Lsinζ+Lvcosζ−usinζ​], vcos2ζ−usin2ζ).

The curve ζ↦r(u,v,ζ)\zeta\mapsto r(u,v,\zeta)ζ↦r(u,v,ζ) is an integral curve of BBB, the pair (u,v)(u,v)(u,v) labels the field line, and ζ\zetaζ acts as a toroidal angle of period 2π2\pi2π. The magnetic axis is the field line u=−ϵ/2u=-\epsilon/2u=−ϵ/2, v=0v=0v=0, on which ψ=0\psi=0ψ=0; it is the non-planar closed curve γ(ζ)=(1−ϵ2cos⁡ζ, 1−ϵ2sin⁡ζ, ϵ2sin⁡2ζ)\gamma(\zeta)=(\sqrt{1-\epsilon^2}\cos\zeta,\ \sqrt{1-\epsilon^2}\sin\zeta,\ \tfrac{\epsilon}{2}\sin 2\zeta)γ(ζ)=(1−ϵ2​cosζ, 1−ϵ2​sinζ, 2ϵ​sin2ζ).

Target

The goal theorem asserts that for every 0<ϵ<10<\epsilon<10<ϵ<1, every 0<δ<(1−ϵ)2/40<\delta<(1-\epsilon)^2/40<δ<(1−ϵ)2/4 and every constant pap_apa​, the pair (B,p)(B,p)(B,p) above is a smooth equilibrium on UϵU_\epsilonUϵ​ that is genuinely three-dimensional:

∇⋅B=0,(∇×B)×B=∇p,B⋅∇p=0on Uϵ,\nabla\cdot B=0,\qquad (\nabla\times B)\times B=\nabla p,\qquad B\cdot\nabla p=0 \quad\text{on } U_\epsilon,∇⋅B=0,(∇×B)×B=∇p,B⋅∇p=0on Uϵ​, ∇p(x)=0  ⟺  ψ(x)=0for x∈Ωδ,\nabla p(x)=0 \iff \psi(x)=0 \quad\text{for } x\in\Omega_\delta ,∇p(x)=0⟺ψ(x)=0for x∈Ωδ​,

together with smoothness of BBB and ppp on UϵU_\epsilonUϵ​ and the failure of axisymmetry: there is a rotation about the zzz axis and a point of Ωδ\Omega_\deltaΩδ​ whose image lies in Ωδ\Omega_\deltaΩδ​ and carries a different pressure.

The milestones are the individual equations of Section 2 of the paper: divergence-freedom, the tension identity (B⋅∇)B=−∇Q(B\cdot\nabla)B=-\nabla Q(B⋅∇)B=−∇Q, force balance, invariance of ψ\psiψ along BBB, the field-line position map and its Jacobian −ab-ab−ab, the expressions H=1+2ϵu+2(u2+v2)H=1+2\epsilon u+2(u^2+v^2)H=1+2ϵu+2(u2+v2) and ψ=(u+ϵ/2)2+v2\psi=(u+\epsilon/2)^2+v^2ψ=(u+ϵ/2)2+v2 in field-line labels, the magnetic axis, the enclosed volume V=2π2ab ψV=2\pi^2ab\,\psiV=2π2abψ, the uniform rotational transform ι=2\iota=2ι=2, and the averages 12π∫02π∣B∣2 dζ=1−ϵ2/2+2ψ\frac{1}{2\pi}\int_0^{2\pi}|B|^2\,d\zeta=1-\epsilon^2/2+2\psi2π1​∫02π​∣B∣2dζ=1−ϵ2/2+2ψ and ⟨∣B∣2⟩V=1−ϵ2/2+δ\langle|B|^2\rangle_V=1-\epsilon^2/2+\delta⟨∣B∣2⟩V​=1−ϵ2/2+δ.

Significance

The solutions contradict the strict formulation of Grad's conjecture used in the recent literature (for example Conjecture 2.5 of Cardona–Duignan–Perrella), since they are smooth, have non-constant pressure, exact nested toroidal flux surfaces, no continuous Euclidean symmetry, finite aspect ratio and non-zero rotational transform, and they form continuous families parameterized by ϵ\epsilonϵ and δ\deltaδ. Because MHD equilibrium is isomorphic to steady Euler flow, the same objects are explicit non-symmetric stationary Euler flows with invariant tori. They also serve as exact benchmarks for numerical equilibrium codes, where analytic three-dimensional solutions with known flux surfaces are otherwise unavailable.

The paper's derivations are elementary but long: they are algebraic identities among square roots and rational functions, verified in the paper by hand and by supporting numerical scripts. A machine-checked development removes the remaining doubt about sign conventions and domains, which is precisely what a counterexample to a conjecture requires. Nothing in this development is currently formalized in Mathlib: there is no curl, no divergence, and no notion of MHD equilibrium, so the mission also produces a small reusable vector-calculus layer on R3\mathbb R^3R3.

Difficulty

Force balance is an identity between derivatives of expressions containing 1−(1−s)2−4z2\sqrt{1-(1-s)^2-4z^2}1−(1−s)2−4z2​ and division by sss; differentiating it directly produces large expressions whose simplification needs the domain hypotheses (s>0s>0s>0 and positive radicand) at every step, so field_simp-style automation must be driven with those side conditions in hand. The statements about field-line coordinates require knowing that the position map is a diffeomorphism onto its image, which the paper establishes by a covering argument rather than by computation. The transform ι=2\iota=2ι=2 is the hardest milestone: it is a winding-number statement about the poloidal displacement of a field line relative to the magnetic axis, and the paper's proof is a continuity-in-ϵ\epsilonϵ argument, which in Lean needs an honest treatment of continuous angle lifts. The volume and average identities need the change of variables theorem with the constant Jacobian −ab-ab−ab over a solid torus.

Formalization scope

Points of space are Fin 3 → ℝ; partial derivatives are fderiv applied to the standard basis vector, and gradient, divergence, curl, cross product, the directional derivative B⋅∇fB\cdot\nabla fB⋅∇f and the tension (B⋅∇)B(B\cdot\nabla)B(B⋅∇)B are defined from it in the first definition file. Squared length is ∑iui2\sum_i u_i^2∑i​ui2​, so the Pi-type norm is never used. All the paper's objects — aaa, bbb, sss, FFF, BBB, UϵU_\epsilonUϵ​, QQQ, HHH, ψ\psiψ, ppp, Ωδ\Omega_\deltaΩδ​, LLL, r(u,v,ζ)r(u,v,\zeta)r(u,v,ζ), γ\gammaγ, rotation about the zzz axis, and the complex poloidal displacement used for the transform — are given in the second definition file, in the same notation as this description. Smoothness is ContDiffOn ℝ ⊤; volumes are the Lebesgue measure on Fin 3 → ℝ; integrals are Bochner integrals.

Everything is stated with the explicit field of Section 2 rather than an abstract existence claim, so no statement can be satisfied by a degenerate or symmetric configuration. The equilibrium conditions are asserted pointwise on UϵU_\epsilonUϵ​, which is open and non-empty for 0<ϵ<10<\epsilon<10<ϵ<1, so no milestone is vacuous. Contributions of the auxiliary calculus lemmas (differentiability of sss, FFF and BBB on UϵU_\epsilonUϵ​, and the product and quotient rules in this partialD formulation) are welcome and reusable by the companion family of Section 3, which is not part of this mission.

Selected references

  • M. Landreman, Analytic toroidal 3D MHD equilibria and steady Euler flows with invariant surfaces, J. Plasma Phys. (submitted), arXiv:2609.26742 (2026). https://arxiv.org/abs/2609.26742
  • H. Grad, Toroidal containment of a plasma, Phys. Fluids 10 (1967) 137–154. https://doi.org/10.1063/1.1761965
  • R. Cardona, N. Duignan, D. Perrella, Asymmetry of MHD equilibria for generic adapted metrics, Arch. Ration. Mech. Anal. 249 (2025) 1. https://doi.org/10.1007/s00205-024-02072-x
  • A. Enciso, A. Luque, D. Peralta-Salas, MHD equilibria with nonconstant pressure in nondegenerate toroidal domains, J. Eur. Math. Soc. 27 (2025) 2251–2291. https://doi.org/10.4171/JEMS/1328
  • P. Constantin, T. D. Drivas, D. Ginsberg, Flexibility and rigidity in steady fluid motion, Comm. Math. Phys. 385 (2021) 521–563. https://doi.org/10.1007/s00220-021-04048-4
  • O. P. Bruno, P. Laurence, Existence of three-dimensional toroidal MHD equilibria with nonconstant pressure, Comm. Pure Appl. Math. 49 (1996) 717–764. https://doi.org/10.1002/(SICI)1097-0312(199607)49:7<717::AID-CPA3>3.0.CO;2-C
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CombinatoricsMachine LearningProbability+1·Captain: naimengye

An Introduction to Computational Learning Theory III: The Vapnik-Chervonenkis Dimension, ε-Nets and Sample ComplexityTextbook

Motivation

Chapter 3 of Kearns and Vazirani, An Introduction to Computational Learning Theory (MIT Press, 1994, doi:10.7551/mitpress/3897.001.0001), asks how many random examples suffice to learn a concept from an infinite class. The cardinality bound of Occam's Razor is useless there, yet the rectangle game of Chapter 1 shows that some infinite classes are learnable from a finite sample. The answer is the Vapnik–Chervonenkis dimension: the size of the largest set on which the class realizes every labeling. Sauer's lemma says that a class of VC dimension ddd realizes only Φd(m)=∑i≤d(mi)≤(em/d)d\Phi_d(m) = \sum_{i \le d}\binom{m}{i} \le (em/d)^dΦd​(m)=∑i≤d​(im​)≤(em/d)d labelings on any mmm points, polynomially many rather than 2m2^m2m, and the ε-net theorem of Blumer, Ehrenfeucht, Haussler and Warmuth turns this into a sample bound: a consistent hypothesis from a class of VC dimension ddd is probably approximately correct once mmm is of order (1/ϵ)(log⁡(1/δ)+dlog⁡(1/ϵ))(1/\epsilon)(\log(1/\delta) + d\log(1/\epsilon))(1/ϵ)(log(1/δ)+dlog(1/ϵ)). A matching lower bound shows that Ω(d/ϵ)\Omega(d/\epsilon)Ω(d/ϵ) examples are necessary. The chapter thus gives a single combinatorial parameter that characterizes, up to a logarithmic factor, the sample complexity of learning any class in the distribution-free model.

Setting

For a class CCC of concepts X→{0,1}X \to \{0,1\}X→{0,1} and a finite S⊆XS \subseteq XS⊆X, ΠC(S)\Pi_C(S)ΠC​(S) is the set of dichotomies of SSS realized by CCC; SSS is shattered if all 2∣S∣2^{|S|}2∣S∣ are realized; VCD(C)\mathrm{VCD}(C)VCD(C) is the supremum of the sizes of shattered sets, possibly ∞\infty∞; ΠC(m)\Pi_C(m)ΠC​(m) is the largest ∣ΠC(S)∣|\Pi_C(S)|∣ΠC​(S)∣ over ∣S∣=m|S| = m∣S∣=m; and Φd(m)\Phi_d(m)Φd​(m) is defined by Φd(m)=Φd(m−1)+Φd−1(m−1)\Phi_d(m) = \Phi_d(m-1) + \Phi_{d-1}(m-1)Φd​(m)=Φd​(m−1)+Φd−1​(m−1), Φd(0)=Φ0(m)=1\Phi_d(0) = \Phi_0(m) = 1Φd​(0)=Φ0​(m)=1. For a target ccc the error regions are c Δ hc \,\Delta\, hcΔh for hhh in the hypothesis class, and a set of points is an ε-net if it meets every error region of weight at least ϵ\epsilonϵ under the target distribution DDD. Samples, their product law, consistency and the error of a hypothesis are those of Mission I.

Formalization targets

Goal: Theorems 3.3 and 3.4

Let HHH be a class of VC dimension at most ddd, well-behaved for the target ccc (the double-sample event of the proof is null-measurable), and m≥8/ϵm \ge 8/\epsilonm≥8/ϵ. The points of a random sample of mmm examples of a target ccc fail to be an ε-net for the error regions {c Δ h:h∈H}\{c \,\Delta\, h : h \in H\}{cΔh:h∈H} with probability at most

2 Φd(2m) 2−ϵm/2,2\,\Phi_d(2m)\,2^{-\epsilon m/2},2Φd​(2m)2−ϵm/2,

so any algorithm that outputs a hypothesis in HHH consistent with its sample has error greater than ϵ\epsilonϵ with at most that probability; with m≥(4/ϵ)log⁡2(2/δ)m \ge (4/\epsilon)\log_2(2/\delta)m≥(4/ϵ)log2​(2/δ) and m≥(8d/ϵ)log⁡2(13/ϵ)m \ge (8d/\epsilon)\log_2(13/\epsilon)m≥(8d/ϵ)log2​(13/ϵ) the probability is at most δ\deltaδ; and, if HHH is nonempty, every class contained in HHH for whose targets HHH is well-behaved is PAC learnable using HHH.

Milestones

Lemma 3.1 (Sauer's lemma, ΠC(m)≤Φd(m)\Pi_C(m) \le \Phi_d(m)ΠC​(m)≤Φd​(m)); Lemma 3.2 (Φd(m)=∑i≤d(mi)\Phi_d(m) = \sum_{i \le d}\binom{m}{i}Φd​(m)=∑i≤d​(im​)); the polynomial bound Φd(m)≤(em/d)d\Phi_d(m) \le (em/d)^dΦd​(m)≤(em/d)d of p. 57; Theorem 3.5 (the Ω(d/ϵ)\Omega(d/\epsilon)Ω(d/ϵ) lower bound, in the two explicit forms of its proof).

Significance

Theorem 3.3 is the fundamental theorem of PAC learning: it replaces log⁡∣H∣\log|H|log∣H∣ in Occam's Razor by the VC dimension and thereby covers rectangles, halfspaces, polygons, neural networks with a fixed architecture, and every class whose dichotomies grow polynomially. Its proof, the double sample and random partition argument, is the origin of symmetrization in empirical process theory. Sauer's lemma is a cornerstone of extremal combinatorics with independent proofs by Sauer, Shelah and Vapnik–Chervonenkis, and the lower bound of Theorem 3.5 shows that the upper bound is tight to within log⁡(1/ϵ)\log(1/\epsilon)log(1/ϵ), so the VC dimension genuinely characterizes sample complexity. None of these is machine-checked. Formalizing them puts on the platform the VC dimension, the growth function and the ε-net theorem with explicit constants, stated on the same sample law as the rest of this series, and the first information-theoretic lower bound for learning.

Difficulty

Sauer's lemma is a double induction on ddd and mmm through the auxiliary class C′C'C′ of dichotomies whose two extensions to a distinguished point are both realized, which needs care with the identification of dichotomies of SSS and of S∖{x}S \setminus \{x\}S∖{x}. The ε-net theorem needs: the reduction Pr⁡[A]≤2Pr⁡[B]\Pr[A] \le 2\Pr[B]Pr[A]≤2Pr[B] from a failed ε-net on the first half to a region hit at least ϵm/2\epsilon m/2ϵm/2 times by the second half, which is a Chebyshev bound on a binomial variable and is where m≥8/ϵm \ge 8/\epsilonm≥8/ϵ enters; the exchangeability of the 2m2m2m draws with a random partition into two halves; the counting bound (mℓ)/(2mℓ)≤2−ℓ\binom{m}{\ell}/\binom{2m}{\ell} \le 2^{-\ell}(ℓm​)/(ℓ2m​)≤2−ℓ; and Sauer's lemma applied to the error regions, whose growth function equals that of HHH. The explicit constants require the numerical inequality 2(2em/d)d2−ϵm/2≤δ2(2em/d)^d 2^{-\epsilon m/2} \le \delta2(2em/d)d2−ϵm/2≤δ under the two stated conditions. The lower bound is a probabilistic argument with a random target: conditional on the sample, the labels of unseen points are fair coins, so the number of errors on them is binomial and exceeds half its range with probability at least 1/21/21/2; the refined bound scales this construction to a region of weight 16ϵ16\epsilon16ϵ and uses Markov's inequality to bound the number of draws landing in it. Measurability of the failure sets is avoided by stating outer-measure bounds, except for the double-sample event, which the proof integrates: it is assumed null-measurable (the well-behavedness of Blumer et al., without which the theorem is false for a class of VC dimension 111 on ω1\omega_1ω1​). For the lower bound it is avoided by working over a finitely supported distribution on a space with measurable singletons.

Formalization scope

The VC dimension is a supremum in N∪{∞}\mathbb{N} \cup \{\infty\}N∪{∞}, the growth function a supremum in N\mathbb{N}N (bounded by 2m2^m2m), and Φd\Phi_dΦd​ the book's recurrence, with its closed form and polynomial bound stated as separate theorems. The goal is stated for a hypothesis class HHH (Theorem 3.4), Theorem 3.3 being the case C=HC = HC=H; it carries the exact bound of the proof, the explicit constants of Blumer et al. in place of the book's c0c_0c0​, the requirement m≥8/ϵm \ge 8/\epsilonm≥8/ϵ of the proof's Chebyshev step, measurability of the hypotheses and the target, well-behavedness of HHH for the target, and 0<ϵ,δ<10 < \epsilon, \delta < 10<ϵ,δ<1. PAC learnability of the subclasses of HHH needs HHH nonempty, since no algorithm outputs hypotheses in the empty class. The lower bound is stated for every deterministic learning function, on an instance space with measurable singletons, for a class shattering some set of d≥1d \ge 1d≥1 points, with the explicit constants derived in the proof sketch (m≤d/2m \le d/2m≤d/2: error ≥1/8\ge 1/8≥1/8 with probability ≥1/2\ge 1/2≥1/2; ϵ≤1/16\epsilon \le 1/16ϵ≤1/16 and m≤(d−1)/(64ϵ)m \le (d-1)/(64\epsilon)m≤(d−1)/(64ϵ): error >ϵ> \epsilon>ϵ with probability ≥1/4\ge 1/4≥1/4). Running time is not modelled. The composition bound for layered networks (Theorems 3.6 and 3.7) is not stated.

Trivializing readings are excluded: the ε-net event ranges over every hypothesis of HHH, the failure bounds are uniform over all consistent learners, and the lower bound holds for every learning function. Welcome contributions: Sauer's lemma, the closed form and the (em/d)d(em/d)^d(em/d)d bound, the random-partition counting lemma, and the binomial median inequality used in the lower bound.

Selected references

  • M. J. Kearns, U. V. Vazirani, An Introduction to Computational Learning Theory, MIT Press, 1994, Chapter 3. doi:10.7551/mitpress/3897.001.0001
  • A. Blumer, A. Ehrenfeucht, D. Haussler, M. K. Warmuth, Learnability and the Vapnik–Chervonenkis dimension, Journal of the ACM 36(4), 1989. doi:10.1145/76359.76371
  • V. N. Vapnik, A. Ya. Chervonenkis, On the uniform convergence of relative frequencies of events to their probabilities, Theory of Probability and its Applications 16(2), 1971. doi:10.1137/1116025
  • N. Sauer, On the density of families of sets, Journal of Combinatorial Theory, Series A 13(1), 1972. doi:10.1016/0097-3165(72)90019-2
  • A. Ehrenfeucht, D. Haussler, M. Kearns, L. Valiant, A general lower bound on the number of examples needed for learning, Information and Computation 82(3), 1989. doi:10.1016/0890-5401(89)90002-3
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Bandit AlgorithmsOperations ResearchOptimization+1·Captain: naimengye

Multi-armed Bandit Allocation Indices I: The Gittins Index, Optimal Stopping and MonotonicityTextbook

Motivation

A decision-maker has nnn projects, each a Markov reward process, and at every decision time may advance exactly one of them; the others stay frozen. Which project to advance so as to maximize the expected total discounted reward? Posed as a dynamic program the problem has a state space that is the product of the nnn state spaces, and the size of that product defeats every general method. The index theorem of Gittins and Jones (1974) says the dynamic program is solved exactly by an index policy: there is a real number ν(B,x)\nu(B, x)ν(B,x), computable for each bandit process BBB from its own data and its own current state xxx, such that always advancing a process of greatest index is optimal. Chapter 2 of Gittins, Glazebrook and Weber, Multi-armed Bandit Allocation Indices (2nd ed., doi:10.1002/9780470980033), introduces the index, proves the theorem three times, and works out the properties of the index that the rest of the book, from jobs and superprocesses to restless bandits, is built on: which stopping time attains it, how it is computed, how it moves with the discount factor, and when it collapses to the myopic rule.

The index theorem itself is already on the platform, proved, as BanditAlgorithm.gittins_index_theorem in the Bandit Algorithms series (Lattimore and Szepesvári, Theorem 35.9). This mission cites it and formalizes what Chapter 2 establishes around it.

Setting

A bandit process BBB (§2.3–2.4) is a Markov reward process on a countable state space EEE: transition probabilities P(y∣x)P(y \mid x)P(y∣x), a bounded reward r(x)r(x)r(x) received each time the continuation control is applied in state xxx, and a discount factor a∈(0,1)a \in (0, 1)a∈(0,1); the freeze control leaves the state unchanged and yields nothing. The law of the process started at xxx is Px\mathbb{P}_xPx​ and x(t)x(t)x(t) is its state at process time t=0,1,2,…t = 0, 1, 2, \dotst=0,1,2,…. A stopping time τ\tauτ is a past-measurable rule for switching from continuation to freezing, taking values in {1,2,… }∪{∞}\{1, 2, \dots\} \cup \{\infty\}{1,2,…}∪{∞}. For such τ\tauτ, Rτ(B,x)=Ex[∑t<τatr(x(t))]R_\tau(B, x) = \mathbb{E}_x[\sum_{t < \tau} a^t r(x(t))]Rτ​(B,x)=Ex​[∑t<τ​atr(x(t))] is the expected discounted reward and Wτ(B,x)=Ex[∑t<τat]W_\tau(B, x) = \mathbb{E}_x[\sum_{t < \tau} a^t]Wτ​(B,x)=Ex​[∑t<τ​at] the expected discounted time; their ratio ντ(B,x)\nu_\tau(B, x)ντ​(B,x) (2.7) is the equivalent constant reward rate of that portion of BBB. The Gittins index is

ν(B,x)=sup⁡τ>0Rτ(B,x)Wτ(B,x)(2.6)\nu(B, x) = \sup_{\tau > 0} \frac{R_\tau(B, x)}{W_\tau(B, x)} \tag{2.6}ν(B,x)=τ>0sup​Wτ​(B,x)Rτ​(B,x)​(2.6)

and, equivalently, the fair charge (2.5): the greatest rent λ\lambdaλ per period for which continuing BBB for one or more periods, paying λ\lambdaλ each period, can be done without expected loss. A simple family of alternative bandit processes (SFABP) is nnn such processes with a common discount factor, one of which is continued at each decision time; an index policy continues a process of greatest index. In the Lean development the single-arm model is the platform's (GittinsIndex): the chain law is built by the Ionescu–Tulcea construction, stopping times are adapted N∪{∞}\mathbb{N}\cup\{\infty\}N∪{∞}-valued maps on trajectories, and gittinsIndex P r a x is (2.6).

Formalization targets

Goal: Lemma 2.2, the optimal stopping set

The supremum in (2.6) is attained. For the initial state ξ\xiξ, the attaining stopping rule may be taken to be "stop at the first time t≥1t \ge 1t≥1 at which the state lies in Σ0\Sigma_0Σ0​" for any set Σ0\Sigma_0Σ0​ with

{x:ν(B,x)<ν(B,ξ)}⊆Σ0⊆{x:ν(B,x)≤ν(B,ξ)},\{x : \nu(B, x) < \nu(B, \xi)\} \subseteq \Sigma_0 \subseteq \{x : \nu(B, x) \le \nu(B, \xi)\},{x:ν(B,x)<ν(B,ξ)}⊆Σ0​⊆{x:ν(B,x)≤ν(B,ξ)},

and every such rule has ντ(B,ξ)=ν(B,ξ)\nu_\tau(B, \xi) = \nu(B, \xi)ντ​(B,ξ)=ν(B,ξ).

Milestones

Theorem 2.1 as a reference to the proved platform theorem; Eq. (2.5), the fair-charge characterization of the index; the restart-in-state formulation of §2.6.4 as the convergence of the Katehakis–Veinott value iteration; Theorem 2.3, monotonicity in the discount factor; Lemma 2.4, the interchange of two bandit portions; Propositions 2.5–2.8, the monotone-index cases in which the index is the immediate reward, or is attained only after the first step, or only at τ=∞\tau = \inftyτ=∞.

Significance

Lemma 2.2 is the working form of the index: it turns the supremum over all stopping times into a specific rule, the first time the index falls below its starting value, and it is what the interchange proof of §2.7, the modified-forwards-induction policies of §2.6.6, the monotone-index propositions of §2.11 and the treatment of jobs in Chapter 3 all use. The fair-charge form (2.5) is the prevailing-charge proof of the theorem (Weber 1992) and the interpretation that carries over to superprocesses and restless bandits. The restart formulation is how indices are computed in practice (Katehakis and Veinott 1987), and Theorem 2.3 is the first of the comparative statics used throughout Chapters 7 and 8. Lemma 2.4 is the elementary inequality behind the original proof of Gittins and Jones.

Of these, only the index theorem has a machine-checked proof today. Formalizing the rest gives the platform the index as a usable object: a characterization of the optimal stopping rule, a convergent algorithm for it, and the monotonicity facts, all stated against the existing model so that every later mission of this series and every future use of the L&S model can build on them.

Difficulty

The obvious first move for Lemma 2.2, "take the stopping time that achieves the supremum", is what has to be proved: the supremum is over an uncountable family, and attainment comes from the optimal stopping problem with charge λ=ν(B,ξ)\lambda = \nu(B, \xi)λ=ν(B,ξ), whose value function satisfies φ(x)=max⁡{0,r(x)−λ+aE[φ(x(1))∣x(0)=x]}\varphi(x) = \max\{0, r(x) - \lambda + a\mathbb{E}[\varphi(x(1)) \mid x(0) = x]\}φ(x)=max{0,r(x)−λ+aE[φ(x(1))∣x(0)=x]}, together with the fact that its optimal stopping set is characterized by the strict and non-strict inequalities λ>ν(B,x)\lambda > \nu(B, x)λ>ν(B,x) and λ≥ν(B,x)\lambda \ge \nu(B, x)λ≥ν(B,x). That last step is the content: it identifies the local decision "stop or continue" with a comparison of indices, which is why any set between the two level sets works. On the platform's model this requires the dynamic-programming theory of discounted optimal stopping on a countable space (Theorem 2.10 of the book), the identification of fairChargeProfit with that value function, and the strong Markov property of markovChainMeasure at a trajectory stopping time. Theorem 2.3 needs randomized stopping times (a geometric kill) and the fact that they do not enlarge the supremum. The restart iteration is monotone and bounded but its operator is not a contraction in the restart value, so its limit has to be identified with the restart problem's value directly; that value is max⁡(0,ν/(1−a))\max(0, \nu/(1-a))max(0,ν/(1−a)), not ν/(1−a)\nu/(1-a)ν/(1−a), because restarting forever is free.

Formalization scope

The state space is a countable type with measurable singletons, so every subset is measurable; rewards are bounded; a∈(0,1)a \in (0, 1)a∈(0,1). The chain law, stopping times, the discounted stopped sums and the index are the platform's, unchanged. Expectations are Bochner integrals; with bounded rewards they are finite and no total-function default value enters. IsPositiveStoppingTime fixes τ≥1\tau \ge 1τ≥1 everywhere, so Wτ≥1W_\tau \ge 1Wτ​≥1 and the ratio (2.7) is a genuine quotient. The stopping rule of Lemma 2.2 is the hitting time from time 111 of a set, with ∞\infty∞ when the set is never hit. The fair-charge profit is a real supremum over the nonempty bounded family of positive stopping times, and (2.5) is stated with the outer supremum over {λ:profit(λ)≥0}\{\lambda : \text{profit}(\lambda) \ge 0\}{λ:profit(λ)≥0}, a nonempty set bounded above. The restart iteration is stated as a limit, with the value max⁡(0,ν(B,ξ)/(1−a))\max(0, \nu(B, \xi)/(1-a))max(0,ν(B,ξ)/(1−a)): for a nonnegative index this is the book's ν/(1−a)\nu/(1-a)ν/(1−a), and the maximum is forced by a one-state example with negative reward. The propositions' hypotheses are almost-sure events under Px\mathbb{P}_xPx​, written as events of measure one.

Two trivializing readings are excluded: the index is never taken over all N∪{∞}\mathbb{N}\cup\{\infty\}N∪{∞}-valued maps but over adapted stopping times, and the stopping set of the goal is not restricted to the two extreme level sets. Contributions welcome: the optimal-stopping dynamic program on markovChainMeasure (value iteration, the strong Markov property at a stopping time), the equivalence of randomized and non-randomized stopping times for the supremum, and the monotone convergence of the restart iteration.

Selected references

  • J. Gittins, K. Glazebrook, R. Weber, Multi-armed Bandit Allocation Indices, 2nd ed., Wiley, 2011, Chapter 2. doi:10.1002/9780470980033
  • J. C. Gittins, D. M. Jones, A dynamic allocation index for the sequential design of experiments, in Progress in Statistics (Gani, ed.), North-Holland, 1974.
  • R. Weber, On the Gittins index for multiarmed bandits, Annals of Applied Probability 2(4), 1992. doi:10.1214/aoap/1177005588
  • M. N. Katehakis, A. F. Veinott, The multi-armed bandit problem: decomposition and computation, Mathematics of Operations Research 12(2), 1987. doi:10.1287/moor.12.2.262
  • T. Lattimore, C. Szepesvári, Bandit Algorithms, Cambridge University Press, 2020, Chapter 35. doi:10.1017/9781108571401
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Dynamical SystemsMathematical Physics·Captain: Lucas

Dynamics and Relativity I: Kepler's Laws from the Inverse-Square LawTextbook

Motivation

The derivation of Kepler's three laws from Newton's inverse-square law of gravitation is the calculation with which mathematical physics begins. Kepler published the laws in 1609 and 1619 as empirical regularities distilled from Tycho Brahe's naked-eye astrometry: planets travel on ellipses with the Sun at a focus, the Sun–planet segment sweeps equal areas in equal times, and the square of the orbital period scales as the cube of the orbit's size. That an attractive force falling off as 1/r21/r^21/r2 forces exactly these three regularities was established by Newton in the Principia (1687); as David Tong remarks in the source notes, the third law was within reach of several of Newton's contemporaries, but the derivation of the first — that the orbit is a conic section with the centre of attraction at a focus — was Newton's alone.

This mission formalizes that derivation as it is presented in §4 (Central Forces) of David Tong's Dynamics and Relativity, the Cambridge Part IA Mathematical Tripos lecture notes (Lent 2013). It is the first mission in a series covering those notes, and it targets the chapter's capstone, Kepler's first law.

Setting

A point particle of mass m>0m>0m>0 moves in Euclidean 333-space along a trajectory x:R→R3x:\mathbb R\to\mathbb R^3x:R→R3, assumed twice continuously differentiable and never passing through the origin, where the field below is singular. Write r(t)=∥x(t)∥r(t)=\lVert x(t)\rVertr(t)=∥x(t)∥ and r^=x/r\hat r = x/rr^=x/r.

The particle moves in a central force field when it obeys Tong's equation of motion (4.1),

m x¨(t)  =  F(r(t)) r^(t),m\,\ddot x(t) \;=\; F\big(r(t)\big)\,\hat r(t),mx¨(t)=F(r(t))r^(t),

where F:R→RF:\mathbb R\to\mathbb RF:R→R gives the radial component of the force at distance rrr; for a force derived from a central potential V(r)V(r)V(r) one has F=− dV/drF=-\,dV/drF=−dV/dr. The Kepler problem (Tong §4.3.1) is the inverse-square special case, potential (4.12)

V(r)=−k mr,F(r)=−k mr2,V(r) = -\frac{k\,m}{r}, \qquad F(r) = -\frac{k\,m}{r^{2}},V(r)=−rkm​,F(r)=−r2km​,

with k=GM>0k=GM>0k=GM>0 for gravitational attraction by a mass MMM fixed at the origin. (The same equations govern the Coulomb problem, with k=−qQ/4πϵ0mk=-qQ/4\pi\epsilon_0 mk=−qQ/4πϵ0​m, which is repulsive when k<0k<0k<0; this mission fixes k>0k>0k>0.)

Two conserved quantities organize the problem. The angular momentum is the vector

L(t)  =  m x(t)×x˙(t),L(t) \;=\; m\,x(t)\times\dot x(t),L(t)=mx(t)×x˙(t),

and we write l=∥L∥/ml=\lVert L\rVert/ml=∥L∥/m for the angular momentum per unit mass, which in the plane polar coordinates of Tong (4.5) is l=r2θ˙l=r^{2}\dot\thetal=r2θ˙. The total energy of the Kepler problem is

E(t)  =  12m∥x˙(t)∥2  −  k mr(t).E(t) \;=\; \tfrac12 m\lVert \dot x(t)\rVert^{2} \;-\; \frac{k\,m}{r(t)} .E(t)=21​m∥x˙(t)∥2−r(t)km​.

Tong's solution (4.14) of the orbit equation states that the trajectory lies on a conic section with a focus at the origin. Coordinate-free, this says that there is a fixed eccentricity vector A∈R3A\in\mathbb R^3A∈R3, pointing towards the point of closest approach, with

r(t)+⟨A,x(t)⟩  =  r0for all t,r0=l2k,r(t) + \langle A, x(t)\rangle \;=\; r_0 \qquad\text{for all } t, \qquad r_0 = \frac{l^{2}}{k},r(t)+⟨A,x(t)⟩=r0​for all t,r0​=kl2​,

which is Tong's r=r0/(1+ecos⁡θ)r = r_0/(1+e\cos\theta)r=r0​/(1+ecosθ) with e=∥A∥e=\lVert A\rVerte=∥A∥ the eccentricity and θ\thetaθ measured from the direction of AAA, and r0r_0r0​ the semi-latus rectum.

Finally, a set S⊆R3S\subseteq\mathbb R^3S⊆R3 is an ellipse with a focus at the origin when there are a nonzero normal vector nnn, a second focus ccc with ⟨n,c⟩=0\langle n,c\rangle=0⟨n,c⟩=0, and a real number aaa with ∥c∥<2a\lVert c\rVert<2a∥c∥<2a, such that SSS is exactly the set of points yyy of the plane {y:⟨n,y⟩=0}\{y : \langle n,y\rangle = 0\}{y:⟨n,y⟩=0} satisfying the two-foci (string) property

∥y∥+∥y−c∥  =  2a.\lVert y\rVert + \lVert y - c\rVert \;=\; 2a .∥y∥+∥y−c∥=2a.

The inequality ∥c∥<2a\lVert c\rVert<2a∥c∥<2a forces a>0a>0a>0 and rules out the degenerate loci; c=0c=0c=0 gives a circle.

Target

The goal theorem is Kepler's first law, K1 of Tong §4.3.2: each planet moves in an ellipse, with the Sun at one focus. Formally, for a trajectory xxx of the attractive inverse-square problem with nonvanishing angular momentum and negative total energy,

k>0,L≠0,E<0  ⟹  ∃ S an ellipse with a focus at the origin such that x(t)∈S for all t.k>0,\quad L\neq 0,\quad E<0 \;\Longrightarrow\; \exists\,S \text{ an ellipse with a focus at the origin such that } x(t)\in S \text{ for all } t.k>0,L=0,E<0⟹∃S an ellipse with a focus at the origin such that x(t)∈S for all t.

The hypothesis L≠0L\neq0L=0 excludes purely radial free-fall, whose trajectory is a segment rather than an ellipse, and E<0E<0E<0 is the bounded regime, which by Tong (4.16) is exactly e<1e<1e<1.

The milestones follow the source in order: conservation of angular momentum and the resulting planarity of the motion (§4, p. 48); Kepler's second law (K2), which holds for any central force; conservation of energy; the conic orbit (4.14); the identification of a conic of eccentricity e<1e<1e<1 as an ellipse with a focus at the origin (4.15); the energy–eccentricity relation (4.16); and Kepler's third law (K3, p. 62),

T  =  2π R3/2GM,R=12(rmin⁡+rmax⁡).T \;=\; \frac{2\pi\,R^{3/2}}{\sqrt{GM}}, \qquad R = \tfrac12\big(r_{\min}+r_{\max}\big).T=GM​2πR3/2​,R=21​(rmin​+rmax​).

Significance

The result. K1 is the statement that fixes the inverse-square law among all central force laws: K2 holds for every central force, and dimensional analysis alone gives the shape of K3, but closed orbits that are exact ellipses with the attracting centre at a focus are special to the 1/r21/r^21/r2 force (and to the harmonic force, with the centre at the centre of the ellipse). Everything quantitative in classical celestial mechanics — orbit determination, the mass–period relation used to weigh binary stars, and the perturbative treatment of precession that eventually exposed the anomaly in Mercury's orbit — is built on the Kepler solution.

Formalizing it. The mathematics has been settled for three centuries; what this mission produces is a machine-checked treatment of the Newtonian derivation, starting from the differential equation rather than from a prescribed orbit. Mathlib has no central-force or two-body library, so the definitions here — central force motion, angular momentum, conserved energy, swept area, and the two-foci characterization of an ellipse — are new and reusable across the rest of the series and by any later mission in classical mechanics. The existing platform mission Celestial Mechanics I: Binary Star Systems runs the complementary direction, verifying that a prescribed conic orbit satisfies the equations of motion and reducing the two-body problem to a one-body problem; the present mission asks for the converse, which is the harder half and the one Newton is credited with.

Difficulty

The derivation in the source changes the independent variable from time ttt to the polar angle θ\thetaθ, substitutes u=1/ru=1/ru=1/r, and solves the resulting linear oscillator equation (4.11). Each of those steps needs infrastructure that does not exist in Mathlib. There is no polar-angle function attached to a curve in the plane: one has to produce a continuously differentiable angle θ(t)\theta(t)θ(t) lifting the trajectory, show θ˙=l/r2\dot\theta = l/r^{2}θ˙=l/r2 never vanishes so that θ\thetaθ is a legitimate change of variable, and then transport a second-order ODE through that reparametrization. Solving (4.11) then requires a uniqueness theorem for the inhomogeneous harmonic oscillator, and reading the conic back into Cartesian form requires the algebra of (4.15).

Kepler's third law carries an extra burden beyond the formula: the statement quantifies over the least period of the motion, so a solution must establish that a negative-energy orbit is periodic at all, and must identify inf⁡tr(t)\inf_t r(t)inft​r(t) and sup⁡tr(t)\sup_t r(t)supt​r(t) as the periapsis and apoapsis distances r0/(1±e)r_0/(1\pm e)r0​/(1±e).

Formalization scope

Trajectories are maps ℝ → EuclideanSpace ℝ (Fin 3), with ContDiff ℝ 2 smoothness and the standing hypothesis x(t)≠0x(t)\neq0x(t)=0 for all ttt built into the definition of central force motion, together with m>0m>0m>0. Time is all of R\mathbb RR: the trajectories considered are globally defined, so collision orbits are excluded by hypothesis rather than by a maximal-interval argument. Derivatives are Mathlib's deriv, so velocity and acceleration are the first and second derivatives of the trajectory.

Three conventions are worth flagging. First, the force is given by its radial profile FFF rather than by a potential, avoiding any appeal to the junk value of a derivative at 000; the Kepler case is the instance F(r)=−km/r2F(r)=-km/r^{2}F(r)=−km/r2. Second, the swept area of K2 is the integral 12∫∥x×x˙∥ dt\tfrac12\int\lVert x\times\dot x\rVert\,dt21​∫∥x×x˙∥dt, which is the standard area element 12r2 dθ\tfrac12 r^2\,d\theta21​r2dθ of the source written invariantly; the content of K2 is that this integrand is constant in time, so that the area depends on t1−t0t_1-t_0t1​−t0​ alone. Third, K1 asserts that the trajectory is contained in an ellipse; it does not assert that the particle traverses the whole ellipse, which is a separate (true) statement about periodic orbits.

The degenerate readings are ruled out explicitly. The eccentricity vector formulation of the conic is an equation holding at every time, not an existence claim at one time; the ellipse predicate carries ∥c∥<2a\lVert c\rVert<2a∥c∥<2a, so a point or a segment does not qualify; and the hypothesis L≠0L\neq0L=0 in K1 and in the conic milestone is necessary, since a radial trajectory satisfies every other hypothesis but lies on no ellipse.

Contributions of independent interest are welcome: a plane polar coordinate API for curves, uniqueness for the forced harmonic oscillator, and the classification of the loci r+⟨A,x⟩=r0r+\langle A,x\rangle = r_0r+⟨A,x⟩=r0​ into ellipse, parabola and hyperbola according to ∥A∥<1\lVert A\rVert<1∥A∥<1, =1=1=1, >1>1>1 (this mission needs only the first case) would all be reusable well beyond this series.

Selected references

  • David Tong, Dynamics and Relativity, University of Cambridge Part IA Mathematical Tripos lecture notes, Lent 2013, §4 (Central Forces), pp. 48–62. http://www.damtp.cam.ac.uk/user/tong/relativity.html
  • Isaac Newton, Philosophiæ Naturalis Principia Mathematica, 1687, Book I, Propositions XI–XVII.
  • S. Chandrasekhar, Newton's Principia for the Common Reader, Oxford University Press, 1995.
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Dynamical SystemsMathematical PhysicsNumber Theory·Captain: Lucas

Ablowitz–Chakravarty–Halburd: the Chazy–Ramanujan correspondence and the Darboux–Halphen reduction of self-dual Yang–MillsResearch Paper

Motivation

In 1985 R. S. Ward conjectured that "many (and perhaps all?) of the ordinary and partial differential equations that are regarded as being integrable or solvable may be obtained from the self-dual gauge field equations (or its generalizations) by reduction". The self-dual Yang–Mills (SDYM) equations are therefore often called the master integrable system: choosing a gauge algebra and a symmetry group to reduce by produces, on the one hand, the classical soliton equations and the Painlevé transcendents, and on the other — once infinite-dimensional gauge algebras are allowed — a family of third-order equations whose solutions have movable natural barriers and are therefore not of Painlevé type.

This mission formalizes the endpoint of one such reduction chain, as surveyed by Ablowitz, Chakravarty and Halburd, Integrable systems and reductions of the self-dual Yang–Mills equations, J. Math. Phys. 44 (2003) 3147–3173, Section V. Reducing SDYM to functions of a single variable gives the Nahm equations; taking the gauge algebra to be the divergence-free vector fields on S3S^3S3 turns them into a matrix flow which, after diagonalizing the symmetric part, becomes the generalized Darboux–Halphen system. Its trace is governed by the Chazy equation, written down by Chazy in 1909, and — this is the paper's historical observation — the Chazy equation is equivalent to the differential system Ramanujan derived in 1916 for the Eisenstein series P=E2P = E_2P=E2​, Q=E4Q = E_4Q=E4​, R=E6R = E_6R=E6​. Chazy and Ramanujan worked on the same equation at nearly the same time and apparently did not know it.

Setting

Throughout, ttt and qqq are complex variables and all functions are complex-valued; a "solution on sss" means the stated derivative identities hold at every point of a set s⊆Cs \subseteq \mathbb{C}s⊆C.

The classical Chazy equation is the third-order equation

d3ydt3=2y d2ydt2−3(dydt)2.\frac{d^3y}{dt^3} = 2y\,\frac{d^2y}{dt^2} - 3\left(\frac{dy}{dt}\right)^2 .dt3d3y​=2ydt2d2y​−3(dtdy​)2.

The classical Darboux–Halphen system is the first-order system for ω1,ω2,ω3\omega_1,\omega_2,\omega_3ω1​,ω2​,ω3​

ω˙1=ω2ω3−ω1(ω2+ω3),\dot\omega_1 = \omega_2\omega_3 - \omega_1(\omega_2+\omega_3),ω˙1​=ω2​ω3​−ω1​(ω2​+ω3​),

together with its two cyclic images. It arose in Darboux's study of triply orthogonal surfaces and was solved by Halphen. Its generalized form adds a term τ2=τ12+τ22+τ32\tau^2 = \tau_1^2+\tau_2^2+\tau_3^2τ2=τ12​+τ22​+τ32​ to each right-hand side, where τ˙1=−τ1(ω2+ω3)\dot\tau_1 = -\tau_1(\omega_2+\omega_3)τ˙1​=−τ1​(ω2​+ω3​) and cyclically.

Ramanujan's system is

qdPdq=P2−Q12,qdQdq=PQ−R3,qdRdq=PR−Q22,q\frac{dP}{dq} = \frac{P^2-Q}{12},\qquad q\frac{dQ}{dq} = \frac{PQ-R}{3},\qquad q\frac{dR}{dq} = \frac{PR-Q^2}{2},qdqdP​=12P2−Q​,qdqdQ​=3PQ−R​,qdqdR​=2PR−Q2​,

satisfied by P(q)=1−24∑n≥1σ1(n)qnP(q) = 1-24\sum_{n\ge1}\sigma_1(n)q^nP(q)=1−24∑n≥1​σ1​(n)qn, Q(q)=1+240∑n≥1σ3(n)qnQ(q) = 1+240\sum_{n\ge1}\sigma_3(n)q^nQ(q)=1+240∑n≥1​σ3​(n)qn, R(q)=1−504∑n≥1σ5(n)qnR(q) = 1-504\sum_{n\ge1}\sigma_5(n)q^nR(q)=1−504∑n≥1​σ5​(n)qn, where σk(n)=∑d∣ndk\sigma_k(n)=\sum_{d\mid n}d^kσk​(n)=∑d∣n​dk.

Finally, the 3×33\times33×3 matrix flow obtained from the Nahm equations with the diff(S3)\mathrm{diff}(S^3)diff(S3) gauge algebra is

M˙=(Adj⁡M)T+MTM−(Tr⁡M)M,Adj⁡M=(det⁡M)M−1,\dot M = (\operatorname{Adj} M)^{T} + M^{T}M - (\operatorname{Tr} M)M,\qquad \operatorname{Adj}M = (\det M)M^{-1},M˙=(AdjM)T+MTM−(TrM)M,AdjM=(detM)M−1,

and the generalized Chazy equation with parameter nnn is

d3ydt3−2yd2ydt2+3(dydt)2=436−n2(6dydt−y2)2.\frac{d^3y}{dt^3} - 2y\frac{d^2y}{dt^2} + 3\left(\frac{dy}{dt}\right)^2 = \frac{4}{36-n^2}\left(6\frac{dy}{dt}-y^2\right)^2 .dt3d3y​−2ydt2d2y​+3(dtdy​)2=36−n24​(6dtdy​−y2)2.

Formalization targets

Goal — the Chazy–Ramanujan correspondence (eqs. (78) and (71))

If P,Q,RP,Q,RP,Q,R satisfy Ramanujan's system on a region of the punctured qqq-plane, then

y(t):=iπP ⁣(e2πit)y(t) := i\pi P\!\left(e^{2\pi i t}\right)y(t):=iπP(e2πit)

satisfies the classical Chazy equation on the preimage region. In particular y(t)=iπE2(t)y(t)=i\pi E_2(t)y(t)=iπE2​(t) is a solution of the Chazy equation, and knowing the general solution of Chazy gives the general solution of Ramanujan's system.

Supporting targets

The milestone list covers the reduction chain in both directions: the matrix flow M˙=(Adj⁡M)T+MTM−(Tr⁡M)M\dot M = (\operatorname{Adj}M)^T + M^TM-(\operatorname{Tr}M)MM˙=(AdjM)T+MTM−(TrM)M and its reduction to the Darboux–Halphen system (eqs. (51)–(54)), the first integrals (55), the passage y=−2(ω1+ω2+ω3)y = -2(\omega_1+\omega_2+\omega_3)y=−2(ω1​+ω2​+ω3​) from Darboux–Halphen to Chazy and back through the roots of a cubic, the SL(2)\mathrm{SL}(2)SL(2) symmetry (73) of the Chazy equation, Rankin's fourth-order equation for the discriminant cusp form, the change of variable q=e2iτq=e^{2i\tau}q=e2iτ between the two forms of Ramanujan's system, and the generalized Chazy equation (81).

Significance

The Chazy equation is the bridge between integrable systems and the theory of modular forms. Its particular solution y=iπE2y = i\pi E_2y=iπE2​ makes the quasi-modularity of the second Eisenstein series an ODE statement; via y=12(log⁡Δ)′y = \tfrac12 (\log\Delta)'y=21​(logΔ)′ it turns into Rankin's homogeneous fourth-order equation for the discriminant cusp form Δ\DeltaΔ, whose Fourier coefficients are the Ramanujan τ\tauτ-function. The SL(2,Z)\mathrm{SL}(2,\mathbb{Z})SL(2,Z) action on solutions is exactly the weight-2 quasi-modular transformation law. In the other direction, the general solution of Chazy is a ratio of hypergeometric functions with a movable natural barrier, which is why these reductions are used as the standard counterexample to the identification of integrability with the Painlevé property.

None of this material is currently in Mathlib: there is no Chazy equation, no Darboux–Halphen system, no Ramanujan differential system, and no Eisenstein-series ODE. The mission builds that layer from scratch. Each statement is a closed-form differential identity, so the development is self-contained: it needs no analytic continuation theory, no modular-forms library, and no existence theory for ODEs. What a solver must supply is careful derivative bookkeeping and polynomial algebra.

Status honesty: every statement in this mission is a classical, published result — Darboux, Halphen, Chazy (1909–1911), Ramanujan (1916), Rankin (1956), and Ablowitz–Chakravarty–Halburd (1990s–2003). Nothing here is open mathematics. What is open is the machine-checked proof; to the captain's knowledge no formalization of these identities exists.

Difficulty

The obvious approach — "differentiate three times and call ring" — fails for two reasons. First, the statements are about functions, not about polynomials: each differentiation step requires producing the derivative of a product, a quotient, or a composition from the hypotheses, and only then is the resulting algebraic identity a ring problem. Second, two of the targets go against the flow of the hypotheses. Recovering the Darboux–Halphen system from a Chazy solution means recovering ω˙i\dot\omega_iω˙i​ from the derivatives of the three elementary symmetric functions of the ωi\omega_iωi​: this is a linear system whose matrix is a Vandermonde matrix in ω1,ω2,ω3\omega_1,\omega_2,\omega_3ω1​,ω2​,ω3​, invertible precisely because the roots are assumed distinct — which is why the distinctness hypothesis is not decoration. Similarly, the matrix milestone needs the conjugation-equivariance of M↦(Adj⁡M)T+MTM−(Tr⁡M)MM \mapsto (\operatorname{Adj}M)^T + M^TM - (\operatorname{Tr}M)MM↦(AdjM)T+MTM−(TrM)M, which holds for the transpose only because the conjugating matrix is complex orthogonal.

Formalization scope

Everything is over C\mathbb{C}C, matching the paper. Solutions are represented pointwise on an arbitrary set s⊆Cs \subseteq \mathbb{C}s⊆C rather than on all of C\mathbb{C}C, because the solutions of interest have movable singularities and natural barriers; no openness, holomorphy or connectivity is assumed unless a statement needs it.

Higher derivatives are carried as explicit extra function arguments joined by HasDerivAt hypotheses rather than through iterated deriv. This avoids junk values entirely: a statement never asserts anything about the value of a derivative that does not exist. The same convention is used for the matrix flow, where the derivative is imposed entrywise, so that no norm or normed-space structure on the space of matrices needs to be chosen.

Divisions are arranged so that no denominator can vanish under the stated hypotheses: Ramanujan's system is written in the form q dP/dq=(P2−Q)/12q\,dP/dq = (P^2-Q)/12qdP/dq=(P2−Q)/12, with no division by qqq; the generalized Chazy equation carries the hypothesis n2≠36n^2 \ne 36n2=36; and the first-integral and discriminant statements carry explicit nonvanishing hypotheses.

There is no trivializing formalization available here. Every statement is an implication between two systems of differential equations whose hypotheses are satisfied by the classical explicit solutions (P=E2P=E_2P=E2​, Q=E4Q=E_4Q=E4​, R=E6R=E_6R=E6​ for the Ramanujan system; Halphen's solutions for Darboux–Halphen), so none of them is vacuous, and none is an identity that holds for arbitrary functions.

A complete development needs only Mathlib's derivative calculus (HasDerivAt and its product, quotient and composition rules), Complex.exp, and Matrix.adjugate with the basic adjugate identities. Contributions of reusable pieces are welcome: in particular a clean statement of the derivative of the elementary symmetric functions of a triple of functions, and the Vandermonde inversion step, would both be of use beyond this mission.

Selected references

  • M. J. Ablowitz, S. Chakravarty, R. G. Halburd, Integrable systems and reductions of the self-dual Yang–Mills equations, J. Math. Phys. 44 (2003) 3147–3173. doi:10.1063/1.1586967
  • J. Chazy, Sur les équations différentielles du troisième ordre et d'ordre supérieur dont l'intégrale générale a ses points critiques fixes, Acta Math. 34 (1911) 317–385. doi:10.1007/BF02393131
  • S. Ramanujan, On certain arithmetical functions, Trans. Cambridge Philos. Soc. 22 (1916) 159–184.
  • G. Halphen, Sur un système d'équations différentielles, C. R. Acad. Sci. Paris 92 (1881) 1101–1103.
  • R. A. Rankin, The construction of automorphic forms from the derivatives of a given form, J. Indian Math. Soc. 20 (1956) 103–116.
  • M. J. Ablowitz, S. Chakravarty, R. G. Halburd, The generalized Chazy equation and Schwarzian triangle functions, Asian J. Math. 2 (1998) 619–624. doi:10.4310/AJM.1998.v2.n4.a1
  • R. S. Ward, Integrable and solvable systems, and relations among them, Philos. Trans. R. Soc. London A 315 (1985) 451–457. doi:10.1098/rsta.1985.0051
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High-Dimensional Probability VI: The Hanson-Wright InequalityTextbook

Motivation

Sums of independent random variables are well understood: Bernstein's inequality and its relatives give sharp, non-asymptotic tail bounds for ∑iaiXi\sum_i a_i X_i∑i​ai​Xi​ whenever the XiX_iXi​ are independent and light-tailed. Many quantities that arise in high-dimensional statistics and random matrix theory, however, are not linear but quadratic in an independent sample — the squared norm of a random vector after a linear transformation, a quadratic-form test statistic, the diagonal of a sample covariance matrix, or the number of edges cut by a random partition in a random graph. A quadratic form X⊤AX=∑i,jAijXiXjX^\top A X = \sum_{i,j} A_{ij} X_i X_jX⊤AX=∑i,j​Aij​Xi​Xj​ is a sum with dependent terms: XiXjX_iX_jXi​Xj​ and XiXkX_iX_kXi​Xk​ share the factor XiX_iXi​, so classical sum-of-independent-variables tools do not apply directly.

The Hanson-Wright inequality, first obtained by Hanson and Wright (1971) for sub-gaussian variables and later sharpened and popularized in this form by Rudelson and Vershynin (2013, "Hanson-Wright inequality and sub-gaussian concentration," Electronic Communications in Probability), closes this gap: it gives a concentration inequality for X⊤AXX^\top A XX⊤AX around its mean with the same two-regime (sub-gaussian near the center, sub-exponential in the tail) shape as Bernstein's inequality for linear sums. It is now a standard tool wherever quadratic statistics of independent data are analyzed: covariance estimation, compressed sensing, randomized numerical linear algebra, and the analysis of random matrices more broadly draw on it routinely.

Setting

Fix a probability space and let X=(X1,…,Xn)X = (X_1, \dots, X_n)X=(X1​,…,Xn​) be a random vector whose coordinates X1,…,XnX_1, \dots, X_nX1​,…,Xn​ are independent, mean zero, and sub-gaussian: each XiX_iXi​ has a finite sub-gaussian (Orlicz ψ2\psi_2ψ2​) norm ∥Xi∥ψ2\|X_i\|_{\psi_2}∥Xi​∥ψ2​​, the smallest t>0t > 0t>0 with Eexp⁡(Xi2/t2)≤2\mathbb E \exp(X_i^2/t^2) \le 2Eexp(Xi2​/t2)≤2. Write K=max⁡i∥Xi∥ψ2K = \max_i \|X_i\|_{\psi_2}K=maxi​∥Xi​∥ψ2​​.

Let A=(Aij)i,j=1nA = (A_{ij})_{i,j=1}^nA=(Aij​)i,j=1n​ be an n×nn \times nn×n real matrix, with no constraint on its diagonal, and form the quadratic form

X⊤AX=∑i,j=1nAijXiXj.X^\top A X = \sum_{i,j=1}^n A_{ij} X_i X_j.X⊤AX=i,j=1∑n​Aij​Xi​Xj​.

Two matrix norms measure the size of AAA: the Frobenius norm ∥A∥F=(∑i,jAij2)1/2\|A\|_F = \bigl(\sum_{i,j} A_{ij}^2\bigr)^{1/2}∥A∥F​=(∑i,j​Aij2​)1/2 (the Euclidean norm of AAA's entries) and the operator (spectral) norm ∥A∥=sup⁡∥x∥2=1∥Ax∥2\|A\| = \sup_{\|x\|_2=1} \|Ax\|_2∥A∥=sup∥x∥2​=1​∥Ax∥2​ (the largest singular value of AAA). Always ∥A∥≤∥A∥F≤n ∥A∥\|A\| \le \|A\|_F \le \sqrt{n}\,\|A\|∥A∥≤∥A∥F​≤n​∥A∥, so the two norms can differ by a factor as large as n\sqrt nn​ — the gap between them is exactly what produces the inequality's two regimes below.

Formalization targets

Goal — Theorem 6.2.1 (Hanson-Wright inequality)

P{ ∣X⊤AX−E X⊤AX∣≥t }  ≤  2exp⁡ ⁣[−cmin⁡ ⁣(t2K4∥A∥F2, tK2∥A∥)]for every t≥0,P\bigl\{\, |X^\top A X - \mathbb E\, X^\top A X| \ge t \,\bigr\} \;\le\; 2 \exp\!\left[-c \min\!\left(\frac{t^2}{K^4 \|A\|_F^2},\ \frac{t}{K^2 \|A\|}\right)\right] \qquad \text{for every } t \ge 0,P{∣X⊤AX−EX⊤AX∣≥t}≤2exp[−cmin(K4∥A∥F2​t2​, K2∥A∥t​)]for every t≥0,

where c>0c > 0c>0 is an absolute constant, not depending on nnn, XXX, AAA, or ttt. Stating the constant only as "some absolute ccc" (rather than pinning it to a numeral) is deliberate: the book's own proof does not track a sharp value, and a goal that only asserts the shape of the bound survives any later improvement to ccc.

Significance

The result itself. Hanson-Wright turns a two-dimensional (in i,ji,ji,j) dependency structure into a one-dimensional concentration statement controlled by two scalar quantities, ∥A∥F\|A\|_F∥A∥F​ and ∥A∥\|A\|∥A∥. This is what makes it usable: a practitioner bounding a quadratic statistic need only compute these two norms, not analyze the joint dependency structure of {XiXj}\{X_iX_j\}{Xi​Xj​} directly. It specializes to Bernstein's inequality (Chapter 2 of this book) when AAA is diagonal, and it underlies non-asymptotic guarantees for covariance estimation, the Johnson-Lindenstrauss lemma via a different route, and the concentration of Lipschitz functions of sub-gaussian vectors.

Formalizing it. The published proof of Hanson-Wright is not a single argument but a chain of four steps: a decoupling reduction (Section 6.1), a direct computation for Gaussian chaos (Lemma 6.2.2), a comparison lemma extending the Gaussian bound to general sub-gaussian vectors via a replacement trick (Lemma 6.2.3), and a final assembly that separates the diagonal part (handled by Bernstein's inequality) from the off-diagonal part (handled by decoupling and comparison). This mission formalizes the goal theorem's statement and the first, most reusable link in that chain — the decoupling machinery of Section 6.1, which reduces the analysis of the dependent chaos X⊤AXX^\top A XX⊤AX to the independent-once-conditioned bilinear form X⊤AX′X^\top A X'X⊤AX′ — together with the chapter's separate contraction principle (Section 6.7), a general comparison tool for Rademacher-weighted sums used repeatedly in the book's later chaining chapters. The Gaussian MGF computation and the replacement-trick comparison lemma (Lemmas 6.2.2–6.2.3) are left as future milestones on top of this mission: they require Gaussian rotation invariance and the singular value decomposition of AAA, substantially more machinery than the milestones included here.

Difficulty

The obvious first idea — treat X⊤AX=∑i,jAijXiXjX^\top A X = \sum_{i,j} A_{ij}X_iX_jX⊤AX=∑i,j​Aij​Xi​Xj​ as if it were a sum of independent terms and apply Bernstein's inequality termwise — fails immediately: the terms AijXiXjA_{ij}X_iX_jAij​Xi​Xj​ for fixed iii are not independent across jjj, since they all share the factor XiX_iXi​. Decoupling (Theorem 6.1.1) is the non-obvious fix: it replaces the off-diagonal chaos by a bilinear form X⊤AX′X^\top A X'X⊤AX′ in an independent copy X′X'X′, which genuinely does become a sum of independent terms once one of the two vectors is conditioned on. The price is a universal constant factor of 444 and the restriction to diagonal-free matrices, which is exactly why the full Hanson-Wright proof must separate the diagonal contribution to E X⊤AX\mathbb E\,X^\top A XEX⊤AX (handled directly by Bernstein's inequality, Chapter 2) before decoupling can be applied to what remains.

Formalization scope

Random variables and vectors are real-valued on an explicit probability space (Ω,F,P)(\Omega, \mathcal F, P)(Ω,F,P). The sub-gaussian norm is HighDimProb.Concentration.subgaussianNorm, the Orlicz-ψ2\psi_2ψ2​-norm definition already published for this series (01-concentration), reused here as a reference item rather than redefined. K=max⁡i∥Xi∥ψ2K = \max_i \|X_i\|_{\psi_2}K=maxi​∥Xi​∥ψ2​​ is written as a finite supremum over the coordinate index, ⨆ i, subgaussianNorm P (X i); because the index type is always a Fintype (Fin n), this supremum is well-defined and, at the degenerate index n=0n=0n=0, reduces to a true (if content-free) instance of the inequality rather than a vacuous or false one. The Frobenius and operator norms of AAA are this mission's own frobeniusNorm and opNorm, stated directly from their defining formulas rather than through Mathlib's scoped matrix-norm typeclass instances, which are deliberately not global defaults (to avoid a diamond between the two norms) and so are unsuitable for a statement that needs both simultaneously. Every place the goal or a milestone integrates a quantity, that quantity is required Integrable, guarding against Mathlib's convention of returning 0 for the Bochner integral of a non-integrable function — without these hypotheses, a mean-zero or expectation hypothesis could hold vacuously, or a conclusion could hold trivially, for reasons having nothing to do with the book's mathematics.

The formalization deliberately does not restrict AAA's diagonal in the goal theorem: doing so would collapse Hanson-Wright to a restatement of Bernstein's inequality for the special case of a diagonal matrix, discarding the chapter's actual content, which is handling the off-diagonal, genuinely quadratic dependence between coordinates. The diagonal-free restriction does appear, correctly, in the Decoupling theorem (6.1.1), whose proof needs it.

Reusable beyond this mission: frobeniusNorm and opNorm are needed by any future chapter using matrix norms (Chapter 4's random matrix norms, Chapter 9's matrix deviation inequality); the decoupling theorem and convex decoupling lemma are the standard entry point for any later formalization of chaos concentration; the contraction principle is reused throughout the book's chaining chapters (7 and 8). Welcome contributions include the Gaussian MGF and comparison lemmas (6.2.2–6.2.3) needed to complete a full proof of the goal theorem, and the two-sided version of Bernstein's inequality needed for the diagonal part of that proof.

Selected references

  • R. Vershynin, High-Dimensional Probability: An Introduction with Applications in Data Science, Cambridge University Press, 2018. DOI: 10.1017/9781108231596.
  • D. L. Hanson, F. T. Wright, "A bound on tail probabilities for quadratic forms in independent random variables," Annals of Mathematical Statistics 42 (1971), 1079–1083.
  • M. Rudelson, R. Vershynin, "Hanson-Wright inequality and sub-gaussian concentration," Electronic Communications in Probability 18 (2013), no. 82, 1–9. https://arxiv.org/abs/1306.2872
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High-Dimensional Statistics I: Gaussian Concentration of Lipschitz FunctionsTextbook

Motivation

A recurring question in high-dimensional statistics is how tightly a scalar quantity built from many random inputs concentrates around its mean, even as the number of inputs grows without bound. Two classical answers organize the whole toolkit: martingale methods, which control a sum of dependent increments one conditional step at a time, and Gaussian-specific isoperimetry, which shows that essentially any regular (Lipschitz) function of a high-dimensional Gaussian vector concentrates as tightly as a single Gaussian coordinate, regardless of dimension. This mission formalizes one representative theorem from each line: the general martingale Bernstein bound (Wainwright, High-Dimensional Statistics, 2019, Theorem 2.19) and the Gaussian concentration of Lipschitz functions (Theorem 2.26), following Chapter 2 of the same book.

Setting

A random variable XXX with mean μ=E[X]\mu=\mathbb E[X]μ=E[X] is sub-Gaussian with parameter σ\sigmaσ (Definition 2.2) if E[eλ(X−μ)]≤eσ2λ2/2\mathbb E[e^{\lambda(X-\mu)}]\le e^{\sigma^2\lambda^2/2}E[eλ(X−μ)]≤eσ2λ2/2 for all λ∈R\lambda\in\mathbb Rλ∈R; it is sub-exponential with parameters (ν,α)(\nu,\alpha)(ν,α) (Definition 2.7, a strictly milder condition) if the same bound holds only for ∣λ∣<1/α|\lambda|<1/\alpha∣λ∣<1/α, with the convention 1/0=+∞1/0=+\infty1/0=+∞ so that α=0\alpha=0α=0 recovers the sub-Gaussian case exactly.

A sequence {Dk}k≥1\{D_k\}_{k\ge1}{Dk​}k≥1​, adapted to a filtration {Fk}\{\mathcal F_k\}{Fk​}, is a martingale difference sequence if each DkD_kDk​ is Fk\mathcal F_kFk​-measurable and E[Dk∣Fk−1]=0\mathbb E[D_k\mid\mathcal F_{k-1}]=0E[Dk​∣Fk−1​]=0. Such sequences arise throughout statistics via the Doob martingale construction: given a function fff of independent variables X1,…,XnX_1,\dots,X_nX1​,…,Xn​, setting Dk:=E[f(X)∣X1,…,Xk]−E[f(X)∣X1,…,Xk−1]D_k:=\mathbb E[f(X)\mid X_1,\dots,X_k]-\mathbb E[f(X)\mid X_1,\dots,X_{k-1}]Dk​:=E[f(X)∣X1​,…,Xk​]−E[f(X)∣X1​,…,Xk−1​] telescopes to f(X)−E[f(X)]=∑kDkf(X)-\mathbb E[f(X)]=\sum_k D_kf(X)−E[f(X)]=∑k​Dk​, converting a deviation question about f(X)f(X)f(X) into a martingale concentration question.

A function f:Rn→Rf:\mathbb R^n\to\mathbb Rf:Rn→R is LLL-Lipschitz with respect to the Euclidean norm if ∣f(x)−f(y)∣≤L∥x−y∥2|f(x)-f(y)|\le L\|x-y\|_2∣f(x)−f(y)∣≤L∥x−y∥2​ for all x,yx,yx,y (Eq. (2.38)).

Formalization targets

Goal — Theorem 2.26 (Gaussian concentration of Lipschitz functions)

Let (X1,…,Xn)(X_1,\dots,X_n)(X1​,…,Xn​) be i.i.d. standard Gaussian and fff be LLL-Lipschitz with respect to the Euclidean norm. Then f(X)−E[f(X)]f(X)-\mathbb E[f(X)]f(X)−E[f(X)] is sub-Gaussian with parameter at most LLL, and hence

P[∣f(X)−E[f(X)]∣≥t]  ≤  2e−t2/2L2for all t≥0.\mathbb P[|f(X)-\mathbb E[f(X)]|\ge t] \;\le\; 2e^{-t^2/2L^2} \qquad \text{for all } t\ge 0.P[∣f(X)−E[f(X)]∣≥t]≤2e−t2/2L2for all t≥0.

The bound is dimension-free: it depends on nnn only through fff's Lipschitz constant, not the ambient dimension itself.

Milestone — Lemma 2.27 (Gaussian interpolation identity)

For any differentiable fff and convex φ\varphiφ, E[φ(f(X)−E[f(X)])]≤E[φ(π2⟨∇f(X),Y⟩)]\mathbb E[\varphi(f(X)-\mathbb E[f(X)])] \le \mathbb E[\varphi(\tfrac\pi2\langle\nabla f(X),Y\rangle)]E[φ(f(X)−E[f(X)])]≤E[φ(2π​⟨∇f(X),Y⟩)] for X,Y∼N(0,In)X,Y\sim N(0,I_n)X,Y∼N(0,In​) independent — the interpolation identity Theorem 2.26's proof is built on.

Milestone — Theorem 2.19 (martingale Bernstein bound)

Given a martingale difference sequence with a per-index sub-exponential conditional moment-generating-function bound E[eλDk∣Fk−1]≤eλ2νk2/2\mathbb E[e^{\lambda D_k}\mid\mathcal F_{k-1}]\le e^{\lambda^2\nu_k^2/2}E[eλDk​∣Fk−1​]≤eλ2νk2​/2 for ∣λ∣<1/αk|\lambda|<1/\alpha_k∣λ∣<1/αk​, the sum ∑kDk\sum_k D_k∑k​Dk​ is itself sub-exponential with parameters (∑kνk2, max⁡kαk)\big(\sqrt{\sum_k\nu_k^2},\ \max_k\alpha_k\big)(∑k​νk2​​, maxk​αk​), and satisfies the two-regime concentration inequality of Eq. (2.28): sub-Gaussian for small deviations, sub-exponential for large ones. This is the chapter's central general-purpose martingale concentration tool.

Significance

Theorem 2.19 is the source of two of the most-cited concentration inequalities in the field — the Azuma–Hoeffding inequality (Corollary 2.20) and the bounded-differences/McDiarmid inequality (Corollary 2.21), both already faithfully covered elsewhere on the platform (azuma_hoeffding_two_sided, bounded_diff_martingale_two_sided) and included here as kind: reference milestones rather than redrafted. Theorem 2.26's Gaussian Lipschitz concentration is separately significant: it is the tool behind dimension-free operator-norm bounds for random matrices, concentration of the empirical spectral distribution, and much of the machinery of Chapters 5 and 6 of the same book.

Formalizing it. No faithful prior art exists on the platform for either the martingale Bernstein bound or Lipschitz-Gaussian concentration itself (a fresh search for "martingale Bernstein," "sub-exponential martingale," "Gaussian interpolation," and "Lipschitz concentration" returned no hits; the existing Vershynin-book item HighDimProb.Isoperimetry.lipschitz_concentration_sphere concentrates a Lipschitz function on the sphere, a different underlying space and a different proof from Theorem 2.26's Gaussian vector). Both goal-adjacent theorems and the Gaussian interpolation lemma are drafted here as open goals (:= by sorry); the two Azuma–Hoeffding/bounded-differences corollaries are reused from the platform's existing, already-proved formalizations.

Difficulty

The naive approach to Theorem 2.26 — try to bound f(X)−E[f(X)]f(X)-\mathbb E[f(X)]f(X)−E[f(X)] directly via a Lipschitz-type argument in Rn\mathbb R^nRn — has no obvious route to a dimension-free bound, since a union bound over coordinates (or over an ε\varepsilonε-net of the domain) picks up a factor that grows with nnn. The resolution, Lemma 2.27's interpolation identity, instead exploits a special structural fact about the Gaussian distribution — its rotation invariance — to replace the nonlinear quantity f(X)−E[f(X)]f(X)-\mathbb E[f(X)]f(X)−E[f(X)] with the linear, and hence exactly computable, Gaussian quantity ⟨∇f(X),Y⟩\langle\nabla f(X),Y\rangle⟨∇f(X),Y⟩, at the mild cost of a non-optimal constant. Theorem 2.19's difficulty is bookkeeping rather than a conceptual obstruction: the recursive conditioning step (Eq. (2.29)) must be iterated exactly nnn times while keeping track of the interplay between the two parameters νk,αk\nu_k,\alpha_kνk​,αk​ per difference, and Proposition 2.9's two-regime tail bound (small-deviation sub-Gaussian behavior, large-deviation sub-exponential behavior) must be carried through unchanged into the final statement — dropping either regime understates what the theorem proves.

Formalization scope

Expectations are Bochner integrals against an explicit probability measure, with integrability required as an explicit hypothesis in IsSubGaussian and IsSubExponential (Mathlib's Bochner integral silently returns 000 for a non-integrable function, which this mission's definitions rule out as a trivializing formalization). The sub-exponential condition's domain restriction |λ| < 1/α is realized as the disjunction α = 0 ∨ |λ| < 1/α, since Lean's real division convention 1/0 = 0 is exactly backwards from the book's own stated 1/0 = +\infty convention for the degenerate sub-Gaussian case.

"X,Y∼N(0,In)X,Y\sim N(0,I_n)X,Y∼N(0,In​) independent" (Lemma 2.27, Theorem 2.26) is formalized via Mathlib's HasGaussianLaw predicate together with explicit coordinatewise mean-zero and identity-covariance hypotheses, which together pin down the standard multivariate normal law, plus IndepFun. The inner product ⟨∇f(X),Y⟩\langle\nabla f(X),Y\rangle⟨∇f(X),Y⟩ is realized as fderiv ℝ f (X ω) (Y ω), the Fréchet derivative applied to Y(ω)Y(\omega)Y(ω) — equal to ⟨∇f(X(ω)),Y(ω)⟩\langle\nabla f(X(\omega)),Y(\omega)\rangle⟨∇f(X(ω)),Y(ω)⟩ by the Riesz representation of the gradient on a Hilbert space, avoiding the need to separately construct a gradient vector field.

Theorem 2.19's printed parameter pair for part (a), "(∑kνk2,α∗)(\sum_k\nu_k^2,\alpha_*)(∑k​νk2​,α∗​)," is formalized as (∑kνk2,α∗)(\sqrt{\sum_k\nu_k^2},\alpha_*)(∑k​νk2​​,α∗​): Definition 2.7 parametrizes the sub-exponential MGF bound by ν\nuν (with ν2\nu^2ν2 appearing in the exponent), so a literal transcription of the printed pair's first entry would silently square the effective parameter and make part (a), read literally, inconsistent with part (b)'s own tail-bound formula (which the book derives from part (a) via the general sub-exponential tail bound, Proposition 2.9). The corrected pairing is the one the book's own proof actually establishes; see MODERATION_NOTES.md for the full derivation.

Out of scope for this mission: Proposition 2.5 (plain Hoeffding for a sum of independent sub-Gaussians), used in the book only as background for Theorem 2.26's proof and not redrafted, since the goal theorem's own statement does not depend on it once Lemma 2.27 is in hand.

Selected references

  • M. J. Wainwright, High-Dimensional Statistics: A Non-Asymptotic Viewpoint, Cambridge University Press, 2019. DOI: 10.1017/9781108627771. Chapter 2.
  • K. Azuma, "Weighted sums of certain dependent random variables," Tôhoku Mathematical Journal, 19:357–367, 1967.
  • W. Hoeffding, "Probability inequalities for sums of bounded random variables," Journal of the American Statistical Association, 58:13–30, 1963.
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Machine LearningReinforcement LearningStatistics·Captain: mikedeng1

Foundations of Reinforcement Learning III: Structured Bandits and the Decision-Estimation CoefficientTextbook

Motivation

Every algorithm in the first three chapters of Foster and Rakhlin's Foundations of Reinforcement Learning and Interactive Decision Making — ε-Greedy and UCB for the multi-armed bandit, Inverse Gap Weighting and SquareCB for contextual bandits — is a special case of the same two-step recipe: estimate a model of the world with an online regression oracle, then convert the estimate into a decision that trades exploration against exploitation. Chapter 4 asks whether this recipe can be made generic: given any structured decision-making problem, specified only by a function class FFF and a decision space Π\PiΠ, is there a single quantity that governs the best achievable regret, the way A/γ\sqrt{A/\gamma}A/γ​ governs the multi-armed bandit and d/γ\sqrt{d/\gamma}d/γ​ governs the linear bandit? The chapter's answer is the Decision-Estimation Coefficient (DEC), introduced by Foster, Kakade, Qian, and Rakhlin [40] as a complexity measure that both upper- and lower-bounds achievable regret for a general decision-making protocol, unifying results that were previously proved from scratch, case by case, for each structured setting. This mission formalizes the chapter's central upper bound (Proposition 13) together with the machinery that makes it computable in two concrete cases — the multi-armed bandit (Proposition 14) and the linear bandit (Propositions 16–17).

Setting

Fix a finite decision space Π\PiΠ and a class F⊆RΠF \subseteq \mathbb{R}^\PiF⊆RΠ of candidate mean-reward functions, with a ground-truth f⋆∈Ff^\star \in Ff⋆∈F (realizability). Over TTT rounds, at each round ttt the learner observes an estimate f^t\hat f_tf^​t​ produced by an online regression oracle, plays a decision distribution pt∈Δ(Π)p_t \in \Delta(\Pi)pt​∈Δ(Π) (possibly depending on f^t\hat f_tf^​t​ and the history), and the regret is

Reg:=∑t=1Tf⋆(π⋆)−∑t=1TEπ∼pt[f⋆(π)],\mathrm{Reg} := \sum_{t=1}^T f^\star(\pi^\star) - \sum_{t=1}^T \mathbb{E}_{\pi \sim p_t}[f^\star(\pi)],Reg:=t=1∑T​f⋆(π⋆)−t=1∑T​Eπ∼pt​​[f⋆(π)],

where π⋆=arg⁡max⁡πf⋆(π)\pi^\star = \arg\max_\pi f^\star(\pi)π⋆=argmaxπ​f⋆(π). The oracle's cumulative estimation error is assumed bounded: ∑t=1TEπ∼pt[(f^t(π)−f⋆(π))2]≤EstSq(F,T,δ)\sum_{t=1}^T \mathbb{E}_{\pi \sim p_t}[(\hat f_t(\pi) - f^\star(\pi))^2] \le \mathrm{EstSq}(F,T,\delta)∑t=1T​Eπ∼pt​​[(f^​t​(π)−f⋆(π))2]≤EstSq(F,T,δ) with probability at least 1−δ1-\delta1−δ (Definition 7). Writing πf:=arg⁡max⁡πf(π)\pi_f := \arg\max_\pi f(\pi)πf​:=argmaxπ​f(π), the DEC game value at a reference model f^\hat ff^​ and scale γ>0\gamma > 0γ>0 is the min-max quantity

decγ(F,f^):=min⁡p∈Δ(Π)max⁡f∈F  Eπ∼p[f(πf)−f(π)−γ(f(π)−f^(π))2],\mathrm{dec}_\gamma(F, \hat f) := \min_{p \in \Delta(\Pi)} \max_{f \in F} \; \mathbb{E}_{\pi \sim p}\bigl[f(\pi_f) - f(\pi) - \gamma(f(\pi) - \hat f(\pi))^2\bigr],decγ​(F,f^​):=p∈Δ(Π)min​f∈Fmax​Eπ∼p​[f(πf​)−f(π)−γ(f(π)−f^​(π))2],

and the DEC of FFF itself is decγ(F):=sup⁡f^∈co(F)decγ(F,f^)\mathrm{dec}_\gamma(F) := \sup_{\hat f \in \mathrm{co}(F)} \mathrm{dec}_\gamma(F, \hat f)decγ​(F):=supf^​∈co(F)​decγ​(F,f^​). The Estimation-to-Decisions (E2D) algorithm plays, at each round, a ptp_tpt​ certifying (i.e. attaining or beating) the value of this min-max game at f^t\hat f_tf^​t​.

Formalization targets

Goal — Proposition 13 (E2D regret bound)

Reg≤decγ(F)⋅T+γ⋅EstSq(F,T,δ)\mathrm{Reg} \le \mathrm{dec}_\gamma(F) \cdot T + \gamma \cdot \mathrm{EstSq}(F, T, \delta)Reg≤decγ​(F)⋅T+γ⋅EstSq(F,T,δ)

with probability at least 1−δ1-\delta1−δ, for any exploration parameter γ>0\gamma > 0γ>0. This is the weakest stable statement the chapter proves about E2D: it holds for an arbitrary function class and an arbitrary regression oracle, with no structural assumption on FFF beyond realizability, and the chapter's later sections instantiate it rather than strengthen it.

Milestones

  • Lemma 9 (Decoupling), general form: for any distribution ν\nuν over a finite model class and any fˉ\bar ffˉ​, Ef∼ν[f(πf)−fˉ(πf)]≤A⋅Ef∼νEπ∼p[(f(π)−fˉ(π))2]\mathbb{E}_{f\sim\nu}[f(\pi_f) - \bar f(\pi_f)] \le \sqrt{A \cdot \mathbb{E}_{f\sim\nu}\mathbb{E}_{\pi\sim p}[(f(\pi)-\bar f(\pi))^2]}Ef∼ν​[f(πf​)−fˉ​(πf​)]≤A⋅Ef∼ν​Eπ∼p​[(f(π)−fˉ​(π))2]​ — the estimation-to-decisions bridge the whole chapter's approach rests on, decoupling the model index from the played decision.
  • Proposition 14 (IGW minimizes the DEC): for the multi-armed bandit (Π=[A]\Pi=[A]Π=[A], F=RAF=\mathbb{R}^AF=RA), Inverse Gap Weighting is the exact minimizer of the DEC game, giving decγ(F)=(A−1)/(4γ)\mathrm{dec}_\gamma(F) = (A-1)/(4\gamma)decγ​(F)=(A−1)/(4γ) — the first concrete computation of an abstract quantity, recovering Chapter 3's rate from Proposition 13 alone.
  • Proposition 16 (G-optimal design): existence, for any compact full-dimensional-span set Z⊆RdZ \subseteq \mathbb{R}^dZ⊆Rd, of a distribution ppp with sup⁡z∈Z⟨Σp−1z,z⟩≤d\sup_{z\in Z}\langle \Sigma_p^{-1}z,z\rangle \le dsupz∈Z​⟨Σp−1​z,z⟩≤d — the classical convex-analysis primitive Proposition 17 needs.
  • Proposition 17 (DEC for linear bandits): combining the G-optimal design with inverse gap weighting gives decγ(F)≲d/γ\mathrm{dec}_\gamma(F) \lesssim d/\gammadecγ​(F)≲d/γ for the linear bandit function class, leading via Proposition 13 to a dT\sqrt{dT}dT​ regret bound.

Significance

The Decision-Estimation Coefficient is, in the book's own words, "the main result" of this line of work: Foster, Kakade, Qian, and Rakhlin [40] show it is not merely an upper bound but (in a suitable localized form, developed further in Chapter 6) a tight characterization of the minimax regret for structured bandits and, more generally, for the interactive decision-making protocol the rest of the book studies. Proposition 13 is the mechanism that makes this useful in practice: it reduces regret analysis for a new structured problem to a single, purely convex-analytic computation of decγ(F)\mathrm{dec}_\gamma(F)decγ​(F), in place of a bespoke exploration argument. Propositions 14–17 are the demonstration that this reduction is not vacuous — they recompute, via the DEC alone, the two rates (multi-armed and linear bandit) that earlier chapters of the book derived by direct, setting-specific arguments, and the match is exact. Formalizing this chapter therefore captures the book's unifying abstraction itself, not just one more instance of it. No formalization of the Decision-Estimation Coefficient, in any form, currently exists on the platform (see Formalization scope).

Difficulty

The obvious formalization mistake is to state Proposition 13's conclusion with decγ(F)\mathrm{dec}_\gamma(F)decγ​(F) left as an unconstrained free real-number parameter satisfying only the inequality the theorem asserts — a formalization under which the "theorem" would be a triviality about an arbitrary real number, since nothing about the actual min-max game would ever be checked. The chapter's content is precisely the opposite: that this specific minimax quantity can be computed (Proposition 14) or bounded via a concrete strategy (Proposition 17), and — as Chapter 6 shows for a lower bound outside this chunk's scope — that no smaller quantity would do. A second difficulty is proof-theoretic rather than notational: the book's own proof of Proposition 13 bounds regret by an unconstrained supremum over all reference functions f^:Π→R\hat f : \Pi \to \mathbb{R}f^​:Π→R, and only identifies this with the official, co(F)\mathrm{co}(F)co(F)-restricted decγ(F)\mathrm{dec}_\gamma(F)decγ​(F) of Eq. (4.16) via Proposition 24 — a fact stated on p. 80, outside this chapter's numbered range, whose own proof the book defers to an exercise. A formalization that quietly imports Proposition 24 to close this gap would rest the goal theorem on an unverified fact; this mission instead states the hypothesis the book's own text uses to motivate restricting to co(F)\mathrm{co}(F)co(F) in the first place (online estimation algorithms produce f^t∈co(F)\hat f_t \in \mathrm{co}(F)f^​t​∈co(F)), so the goal is faithful to what is actually established within the chapter's own pages.

Formalization scope

Every item fixes a finite decision space (Fin A, Fin n, or a generic Fintype S) and states the DEC as the literal sInf-of-sSup transcription of the min-max game (Eqs. (4.15)–(4.16)), never as an opaque bound — this is the trivializing formalization the chunk's own reading of the chapter rules out (see Difficulty). piStar : (S → ℝ) → S is a hypothesized global maximizer selector throughout, constrained to be a genuine argmax only on the function class in scope (F or Set.univ), matching how the book treats πf\pi_fπf​ as a fixed but arbitrary tie-breaking choice. The goal theorem (Proposition 13) adds the explicit hypothesis hfhat : ∀ t, fhat t ∈ convexHull ℝ F, replacing an appeal to the out-of-range Proposition 24 (see Difficulty); this is the one place this mission's statement is not a line-by-line transcription of the book's own displayed proof steps, and it is recorded here and in MODERATION_NOTES.md. Proposition 14's and Proposition 17's ≲\lesssim≲ are replaced by the explicit constants the book's own proofs establish ((A−1)/(4γ)(A-1)/(4\gamma)(A−1)/(4γ) exactly, and (4d+1)/(2γ)(4d+1)/(2\gamma)(4d+1)/(2γ) respectively — the latter obtained by summing the three terms the proof of Proposition 17 isolates). Proposition 14's Lean statement splits the book's single equality decγ(F,f^)=(A−1)/(4γ)\mathrm{dec}_\gamma(F,\hat f) = (A-1)/(4\gamma)decγ​(F,f^​)=(A−1)/(4γ) into an upper bound on the literal decGf, a lower bound restricted to full-support distributions, and IGW's own exact game value, because the book's min over the whole simplex is not provable as a literal Lean equality: a distribution with a zero-weight arm makes the inner supremum genuinely unbounded, and Lean's total Real.sSup returns a junk value smaller than (A−1)/(4γ)(A-1)/(4\gamma)(A−1)/(4γ) there (caught in moderation, MODERATION_NOTES.md); the three-conjunct statement recovers exactly the book's real content without asserting that false literal equality. Lemma 9 is restated inside FoundationsRL.Structured rather than imported from the Chapter 2 mission, since draft items across chunks cannot import one another; its source citation still points to its original location (p. 32). Proposition 16 is not drafted: the platform's existing BanditAlgorithm.kiefer_wolfowitz_equivalence (Lattimore & Szepesvári, Theorem 21.1) states the identical existence claim — compact set with full-dimensional span, a design with G-value at most ddd — as one clause of a larger equivalence, and is reused as a reference item rather than redrafted. Proposition 22 (primal/dual DEC equivalence, §4.4) is deliberately excluded: the book states it "under mild regularity conditions" it does not pin down in the statement itself, which is exactly the kind of unquantified hypothesis this series' faithfulness standard excludes from a goal or milestone. Contributions extending this mission with Chapter 6's lower bound (matching decγ(F)\mathrm{dec}_\gamma(F)decγ​(F) from below, establishing tightness) or with a formalization of Proposition 24 itself (removing this mission's hfhat hypothesis) are welcome.

Selected references

  • D. Foster, S. Kakade, J. Qian, and A. Rakhlin, The Statistical Complexity of Interactive Decision Making, arXiv:2112.13487, 2021. https://arxiv.org/abs/2112.13487
  • D. Foster and A. Rakhlin, Foundations of Reinforcement Learning and Interactive Decision Making, arXiv:2312.16730, 2023. https://arxiv.org/abs/2312.16730
  • T. Lattimore and C. Szepesvári, Bandit Algorithms, Cambridge University Press, 2020.
  • J. Kiefer and J. Wolfowitz, The Equivalence of Two Extremum Problems, Canadian Journal of Mathematics, 1960.
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Combinatorics·Captain: Yuxuan Xu

Magic Squares V: The Counting Function of Semi-Magic Squares of Every OrderResearch Paper

Motivation

The magic-square programme already on this platform works at fixed small orders: MacMahon's enumeration of the 3×33\times33×3 squares, both the magic count M3(3e)=2e2+2e+1M_{3}(3e)=2e^{2}+2e+1M3​(3e)=2e2+2e+1 and the semi-magic count H3(t)=3(t+34)+(t+22)H_{3}(t)=3\binom{t+3}{4}+\binom{t+2}{2}H3​(t)=3(4t+3​)+(2t+2​); the classification of the normal 3×33\times33×3 squares; and the counts of the panmagic and symmetric order-three classes. Each of those is a statement about a single order. This mission changes the axis: it asks what the counting function does when the order itself is allowed to vary.

Timeline.

  • 1915 — MacMahon determines H3H_{3}H3​ and M3M_{3}M3​ explicitly [MacMahon 1960].
  • 1966 — Anand, Dumir and Gupta conjecture that Hn(t)H_{n}(t)Hn​(t), as a function of the line sum ttt, is a polynomial of degree (n−1)2(n-1)^{2}(n−1)2 for every order nnn [Anand-Dumir-Gupta 1966].
  • 1973 — the conjecture is proved independently by Ehrhart, from linear Diophantine systems [Ehrhart 1973], and by Stanley, from linear homogeneous Diophantine equations and the magic labelings of graphs [Stanley 1973].
  • 1980 — Spencer gives an elementary proof [Spencer 1980].
  • 2002–2003 — Beck and Pixton compute the Ehrhart polynomial of the Birkhoff polytope at order four [Beck-Pixton 2002]; Beck, Cohen, Cuomo and Gribelyuk extend the structural picture to the magic, symmetric and pan-diagonal counts, which are quasi-polynomials rather than polynomials [BCCG 2003].

That split is the point of the mission, so it is worth naming before anything is proved. A quasi-polynomial of degree ddd and period mmm agrees with a degree-ddd polynomial on each residue class modulo mmm, the polynomials differing between classes; a polynomial is the case m=1m=1m=1. For the magic squares the values do depend on ttt modulo a period — at order three M3(t)M_{3}(t)M3​(t) vanishes unless 3∣t3\mid t3∣t — and the same is true of every other class. For HnH_{n}Hn​ it never happens.

Setting

An n×nn\times nn×n semi-magic square of line sum ttt is an n×nn\times nn×n array of nonnegative integers in which every row and every column sums to ttt. Entries may repeat, and no condition is placed on the diagonals. Write Hn(t)H_{n}(t)Hn​(t) for the number of such arrays.

In Lean the array is a Square n ℕ, that is, a Matrix (Fin n) (Fin n) ℕ; the condition is IsSemiMagic M t, which asks every rowSum and every colSum to equal t; and the counting function is semiMagicCount n t, the cardinality of the finset of all arrays over Fin (t + 1) satisfying IsSemiMagic. Restricting the entries to Fin (t + 1) loses nothing, since an entry of a square of line sum ttt is at most ttt.

Dividing by ttt turns such an array into a doubly stochastic matrix, a nonnegative real matrix whose every row and column sums to 111. So Hn(t)H_{n}(t)Hn​(t) is equally the number of lattice points in the ttt-fold dilation of the Birkhoff polytope BnB_{n}Bn​. Two geometric facts about BnB_{n}Bn​ are what the mission is about. Its dimension is (n−1)2(n-1)^{2}(n−1)2: the n2n^{2}n2 entries satisfy 2n2n2n line equations, exactly one of which is dependent. Its vertices are the n!n!n! permutation matrices, by the Birkhoff–von Neumann theorem, hence integral. The mission states that both facts are visible in the arithmetic of HnH_{n}Hn​.

Formalization targets

Goal — the counting function is a polynomial

∃ p∈Q[X]:deg⁡p=(n−1)2,p(t)=Hn(t)  for all t∈N,\exists\, p\in\mathbb{Q}[X]:\quad \deg p=(n-1)^{2},\qquad p(t)=H_{n}(t)\ \text{ for all }t\in\mathbb{N},∃p∈Q[X]:degp=(n−1)2,p(t)=Hn​(t)  for all t∈N, p(−n−t)=(−1)n−1p(t)  for all t∈Z,p(−1)=p(−2)=⋯=p(−n+1)=0.p(-n-t)=(-1)^{n-1}p(t)\ \text{ for all }t\in\mathbb{Z},\qquad p(-1)=p(-2)=\cdots=p(-n+1)=0 .p(−n−t)=(−1)n−1p(t)  for all t∈Z,p(−1)=p(−2)=⋯=p(−n+1)=0.

This is Theorem 1 of [BCCG 2003], stated there for n≥1n\ge 1n≥1. It is the shape of the truth, not a closed form, so no later improvement of the explicit formulas can invalidate it. The three parts are not independent: the degree is the dimension of BnB_{n}Bn​, and the two identities are the reciprocity law for lattice-point counting, applied to BnB_{n}Bn​.

The intermediate rungs

The goal is far from the easy cases, and the mission is laid out so that each rung is an independently provable statement.

  • Order one. H1(t)=1H_{1}(t)=1H1​(t)=1: a 1×11\times11×1 array of line sum ttt is just [t][t][t].
  • Orders two and three. Already proved on the platform, as MagicSquares.semi_magic_count_two (H2(t)=t+1H_{2}(t)=t+1H2​(t)=t+1) and MagicSquares.semi_magic_count_three (MacMahon's H3(t)=3(t+34)+(t+22)H_{3}(t)=3\binom{t+3}{4}+\binom{t+2}{2}H3​(t)=3(4t+3​)+(2t+2​)). Included as references, not as targets.
  • Order four, with the denominators cleared so that it is an identity between natural numbers:
11340⋅H4(t)=11t9+198t8+1596t7+7560t6+23289t5+48762t4+70234t3+68220t2+40950t+11340.11340\cdot H_{4}(t)=11t^{9}+198t^{8}+1596t^{7}+7560t^{6}+23289t^{5}+48762t^{4}+70234t^{3}+68220t^{2}+40950t+11340 .11340⋅H4​(t)=11t9+198t8+1596t7+7560t6+23289t5+48762t4+70234t3+68220t2+40950t+11340.

Its leading coefficient is 1111340=vol⁡(B4)\tfrac{11}{11340}=\operatorname{vol}(B_{4})1134011​=vol(B4​) and its normalised volume is 352352352.

  • Existence and degree, uniformly in nnn. The polynomial exists, with degree exactly (n−1)2(n-1)^{2}(n−1)2.
  • The reciprocity identity and the vanishing list, for that polynomial.

Significance

The result itself. The theorem makes the semi-magic squares countable in closed form at every order, and it is why the semi-magic count can be tabulated as a polynomial while the magic, symmetric and pandiagonal counts cannot: a polynomial is determined by finitely many values, a quasi-polynomial is not without knowing its period. The reciprocity identities are the same statement seen from the interior of BnB_{n}Bn​, which is why they are what pins an explicit polynomial down once its degree is known. The order-four polynomial above was verified against direct enumeration on seventeen values of ttt; that verification is evidence, not proof, and is recorded because the general statement is what has to be proved.

Formalizing it. The theorem has been known since 1973 and has had an elementary proof since 1980; what does not exist anywhere is a machine-checked proof. Mathlib contains no Ehrhart theory, no quasi-polynomial machinery and no rational-generating-function toolbox — the string "Ehrhart" does not occur in it — so a formalization must construct its own lattice-point-counting argument for this family of polytopes, or find an elementary route that avoids polytopes altogether. Either outcome is reusable: the same absence blocks the quasi-polynomial counts MnM_{n}Mn​, SnS_{n}Sn​ and PnP_{n}Pn​ of BCCG's Theorem 2, which the earlier missions approach only at order three.

Difficulty

The first idea anyone has is to interpolate: compute Hn(t)H_{n}(t)Hn​(t) for enough values of ttt and fit a polynomial. That works, and it is how the order-four rung was produced, but it cannot prove the general statement: the degree is what is being asserted, so the number of values needed is not known in advance, and with nnn itself a variable no finite computation settles it. Interpolation is legitimate as a target at order four; it must not be mistaken for a route to the goal.

The second idea is to import the geometry as a black box: a rational polytope dilated by ttt has a counting function that is a quasi-polynomial of degree equal to its dimension, with period dividing the least common multiple of the vertex denominators. That is Ehrhart's theorem, and it is the textbook route. It is not available here, and reconstructing it in general is a larger project than this mission; the statements the mission asks for are the ones that survive without it.

The part of the goal with no counting interpretation at all is the second line. HnH_{n}Hn​ is defined on N\mathbb{N}N; the assertion that a polynomial agreeing with it there vanishes at −1,…,−(n−1)-1,\dots,-(n-1)−1,…,−(n−1) and satisfies p(−n−t)=(−1)n−1p(t)p(-n-t)=(-1)^{n-1}p(t)p(−n−t)=(−1)n−1p(t) is a statement about the interior of the polytope, and it cannot be read off from the combinatorial definition. A solver who proves only the polynomiality and the degree has not finished the goal.

Formalization scope

The formalization commits to the following conventions.

  • The counting function is semiMagicCount n t, the Finset.card of the arrays over Square n (Fin (t+1)) satisfying IsSemiMagic. Entries are natural numbers, not integers or reals.
  • The polynomial is over ℚ and is quantified existentially. Negative arguments are handled by casting the integer into ℚ and evaluating there; Polynomial.eval₂ is unusable for the reciprocity, since it would need a ring homomorphism Q→Z\mathbb{Q}\to\mathbb{Z}Q→Z, which does not exist.
  • The degree is encoded as p.natDegree = (n - 1) ^ 2, with natural-number subtraction, which makes the n=1n=1n=1 case harmless rather than degenerate.
  • The hypothesis 1 ≤ n is carried explicitly although the statement is meaningful at n=0n=0n=0; it matches the source.
  • A trivializing formalization to avoid: replacing ∀ t by a finite range of values, or replacing semiMagicCount by a smooth surrogate, would make the statement easy and empty. The universal quantifier over ttt and the exact value of natDegree are what give the goal its content.

Reusable beyond this mission: any development of lattice-point counting in the Birkhoff polytope, of dilations of rational polytopes, or of quasi-polynomials. The vocabulary of the programme (MagicSquares, MagicSquaresPandiagonal, MagicSquaresMostPerfect, MagicSquaresTransforms, MagicSquaresNormal3) is shared with the earlier missions and is included as reference items rather than redefined.

Selected references

  • P. A. MacMahon, Combinatory Analysis, Chelsea, New York, 1960.
  • H. Anand, V. C. Dumir and H. Gupta, A combinatorial distribution problem, Duke Math. J. 33 (1966) 757--769.
  • E. Ehrhart, Sur les carrés magiques, C. R. Acad. Sci. Paris Sér. A-B 277 (1973) A651--A654.
  • R. P. Stanley, Linear homogeneous Diophantine equations and magic labelings of graphs, Duke Math. J. 40 (1973) 607--632.
  • J. Spencer, Counting magic squares, Amer. Math. Monthly 87 (1980) 397--399.
  • M. Beck and D. Pixton, The Ehrhart polynomial of the Birkhoff polytope, arXiv:math.CO/0202267 — https://arxiv.org/abs/math/CO/0202267
  • M. Beck, M. Cohen, J. Cuomo and P. Gribelyuk, The number of "magic" squares, cubes and hypercubes, Amer. Math. Monthly 110 (2003) 707--717 — https://arxiv.org/abs/math/0201013
  • G. M. Ziegler, Lectures on Polytopes, Springer-Verlag, New York, 1995.
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AlgebraRepresentation Theory·Captain: lisamegawatts

Clifford Casimir I: Odd-Sector Adjoint Spectrum on Cl(6,0)Research Paper

Motivation

The real Clifford algebra Cl(6,0)\mathrm{Cl}(6,0)Cl(6,0) is the smallest Euclidean Clifford algebra whose full structure carries a nontrivial multiplicity-eight representation-theoretic decomposition, and it has become a recurring object in programs that build internal gauge and family structure from Clifford generators rather than imposing it by hand. Within such programs, the single most basic representation-theoretic question one can ask about the algebra is: how does a distinguished su(2)\mathfrak{su}(2)su(2) subalgebra, acting by the adjoint action, decompose the odd part of the algebra as a representation?

This mission answers that question exactly, for the specific triple of bivectors built on the index set {0,2,5}\{0,2,5\}{0,2,5}. The computation was carried out structurally (by splitting active indices from spectator indices) in the LeanProofs research program in 2026 and recorded with exact multiplicities; no machine-checked proof exists yet. The purpose here is to close that gap: the result is finite-dimensional linear algebra, completely within reach of a Lean 4 + Mathlib development, and every constant in it is explicit.

Setting

Fix R6\mathbb{R}^6R6 with its standard inner product and the associated quadratic form Q60=diag(1,1,1,1,1,1)Q_{60} = \mathrm{diag}(1,1,1,1,1,1)Q60​=diag(1,1,1,1,1,1), and let Cl(6,0)=CliffordAlgebra(Q60)\mathrm{Cl}(6,0) = \mathrm{CliffordAlgebra}(Q_{60})Cl(6,0)=CliffordAlgebra(Q60​) be the real Clifford algebra generated by symbols e0,…,e5e_0,\dots,e_5e0​,…,e5​ with

ei2=1,eiej=−ejei  (i≠j).e_i^2 = 1, \qquad e_i e_j = -e_j e_i \ \ (i \neq j).ei2​=1,ei​ej​=−ej​ei​  (i=j).

The algebra is Z\mathbb{Z}Z-graded in the usual sense: it is the direct sum of its grade-kkk subspaces, spanned by products of kkk distinct generators, of dimension (6k)\binom{6}{k}(k6​). The odd sector is the linear span of the odd grades,

Cl−(6,0)  =  grade1⊕grade3⊕grade5,dim⁡RCl−(6,0)=6+20+6=32.\mathrm{Cl}^-(6,0) \;=\; \mathrm{grade}_1 \oplus \mathrm{grade}_3 \oplus \mathrm{grade}_5, \qquad \dim_{\mathbb{R}} \mathrm{Cl}^-(6,0) = 6 + 20 + 6 = 32.Cl−(6,0)=grade1​⊕grade3​⊕grade5​,dimR​Cl−(6,0)=6+20+6=32.

On it, register three bivectors and their halved adjoint actions:

E1=e0e2,E2=e2e5,E3=e0e5,Ti=12 adEi,E_1 = e_0 e_2, \quad E_2 = e_2 e_5, \quad E_3 = e_0 e_5, \qquad T_i = \tfrac{1}{2}\,\mathrm{ad}_{E_i},E1​=e0​e2​,E2​=e2​e5​,E3​=e0​e5​,Ti​=21​adEi​​,

where adX(Y)=XY−YX\mathrm{ad}_{X}(Y) = XY - YXadX​(Y)=XY−YX. The triple satisfies the su(2)\mathfrak{su}(2)su(2) relations [E1,E2]=2E3[E_1,E_2]=2E_3[E1​,E2​]=2E3​ and cyclic permutations, so the TiT_iTi​ generate a copy of su(2)\mathfrak{su}(2)su(2) with [T1,T2]=T3[T_1,T_2]=T_3[T1​,T2​]=T3​ cyclically. The associated quadratic Casimir is the endomorphism

C  =  −(T12+T22+T32).C \;=\; -(T_1^2 + T_2^2 + T_3^2).C=−(T12​+T22​+T32​).

Because each EiE_iEi​ is even, every TiT_iTi​ preserves the odd sector, and so does CCC.

Formalization targets

Goal — the Casimir spectrum with exact multiplicities

C∣Cl−(6,0) has eigenvalue 2 with multiplicity 24 and eigenvalue 0 with multiplicity 8,C\big|_{\mathrm{Cl}^-(6,0)} \ \text{has eigenvalue } 2 \text{ with multiplicity } 24 \ \text{and eigenvalue } 0 \text{ with multiplicity } 8,C​Cl−(6,0)​ has eigenvalue 2 with multiplicity 24 and eigenvalue 0 with multiplicity 8,

the two eigenspaces spanning the whole odd sector. Equivalently, as a representation of the generated Spin(3)≅SU(2)\mathrm{Spin}(3) \cong \mathrm{SU}(2)Spin(3)≅SU(2),

Cl−(6,0)  ≅  8 Vj=1  ⊕  8 Vj=0,\mathrm{Cl}^-(6,0) \;\cong\; 8\,V_{j=1} \;\oplus\; 8\,V_{j=0},Cl−(6,0)≅8Vj=1​⊕8Vj=0​,

eight copies of the spin-1 module and eight copies of the trivial module. The goal deliberately asserts only the eigenspace dimensions and their spanning property — the decomposition shape — not any particular basis or pairing.

Stronger — the Cartan weight decomposition

T3-weights on Cl−(6,0):0 (multiplicity 16),+1 and −1 (multiplicity 8 each),T_3\text{-weights on } \mathrm{Cl}^-(6,0): \quad 0 \ \text{(multiplicity } 16\text{)}, \qquad +1 \ \text{and} \ -1 \ \text{(multiplicity } 8 \text{ each)},T3​-weights on Cl−(6,0):0 (multiplicity 16),+1 and −1 (multiplicity 8 each),

the three weight spaces spanning the sector. This refines the goal: each j=1j=1j=1 copy contributes weights −1,0,+1-1,0,+1−1,0,+1 and each j=0j=0j=0 copy contributes weight 000.

Significance

The result itself. The spectrum pins down exactly how an su(2)\mathfrak{su}(2)su(2) acting from inside the algebra sees the odd sector: not irreducibly, but as a clean 8⊕88 \oplus 88⊕8 multiplicity split between spin-1 and spin-0. In the LeanProofs program this decomposition is load-bearing for everything downstream that distinguishes "active" indices from "spectator" indices — the multiplicity 888 is the number of spectator degrees of freedom, and its appearance in the spectrum is what makes the split structural rather than coincidental. The weight decomposition further identifies the Cartan grading and is the natural first test case for any technology that must eventually handle larger Clifford algebras or other subalgebras.

Formalizing it. The computation is proved (structurally, by hand, in the research record) but not machine-checked. Everything needed lives in Mathlib: CliffordAlgebra, its Z2\mathbb{Z}_2Z2​ grading CliffordAlgebra.evenOdd, Submodule, LinearMap, Module.finrank. What the mission produces is a fully verified finite spectral computation inside Clifford algebra — a reusable certificate that the platform's Clifford and grading infrastructure supports exact representation-theoretic bookkeeping, not just algebraic identities.

Difficulty

The obstruction is bookkeeping, not ideas. The natural attack — split indices into active {0,2,5}\{0,2,5\}{0,2,5} and spectator {1,3,4}\{1,3,4\}{1,3,4}, decompose Cl(active)⊗Cl(spectator)\mathrm{Cl}(\text{active}) \otimes \mathrm{Cl}(\text{spectator})Cl(active)⊗Cl(spectator) as a tensor product of graded pieces, and read off the 8=238 = 2^38=23 multiplicity from the spectator sector — requires transferring the su(2)\mathfrak{su}(2)su(2) action across such a tensor decomposition, which Mathlib does not provide ready-made for Clifford algebras. A purely computational route (fix the 64-element blade basis, build the 32×3232 \times 3232×32 matrices of the TiT_iTi​ explicitly, compute kernels) is straightforwardly correct but laborious; making it readable is the real work. The statement is stated through arbitrary endomorphisms bound pointwise to the halved adjoint actions precisely so that solvers may choose either route.

Formalization scope

The mission commits to: the quadratic form Q60 as QuadraticMap.weightedSumSquares ℝ (fun _ : Fin 6 => 1); generators e6 i = CliffordAlgebra.ι Q60 (Pi.single i 1); the odd sector as the Mathlib-native CliffordAlgebra.evenOdd Q60 1; and the registered triple as products of two generators. All theorems quantify over endomorphism witnesses bound pointwise to 12 adEi\tfrac12\,\mathrm{ad}_{E_i}21​adEi​​, so no particular matrix realization is privileged. Spectra are stated as eigenspace decompositions with exact Module.finrank multiplicities — never as pointwise eigenvalue claims, which would be false for mixed vectors. No trivializing formalization exists: the multiplicities are hard constants, and the dimension gate (32) rules out statements about degenerate sector choices. The definition file is reusable for any future mission on Cl(6,0)\mathrm{Cl}(6,0)Cl(6,0); the su(2) relations and dimension gate are self-contained milestones. Contributions of either a structural (active/spectator split) or computational (explicit blade basis) proof are equally welcome.

Selected references

  • Lawson & Michelsohn, Spin Geometry, Princeton University Press, 1989 (Clifford algebra grading and structure).
  • MonumentalSystems, LeanProofs research record #2561 (2026): exact full-sector SU(2) decomposition of Cl−(6,0)\mathrm{Cl}^-(6,0)Cl−(6,0) with multiplicities, https://github.com/MonumentalSystems/LeanProofs
  • Mathlib, Mathlib.LinearAlgebra.CliffordAlgebra.Grading (the evenOdd grading used as the odd sector).
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Convex OptimizationOperations ResearchOptimization·Captain: naimengye

Robust Optimization X: Globalized Robust Counterparts of Uncertain Conic Problems (retired)Textbook

Motivation

A robust counterpart draws a hard line. Inside the uncertainty set the constraint must hold; outside it, nothing is promised — and in a real problem the perturbation does sometimes land outside. Chapter 3 answered this for linear problems with the globalized robust counterpart: keep the constraint exactly on the normal range Z\mathcal{Z}Z, and let it degrade at a controlled rate outside, proportionally to the distance from Z\mathcal{Z}Z. That mission published Proposition 3.2.1, which says the GRC of an uncertain linear inequality is equivalent to two ordinary robust counterparts.

Chapter 11 of Ben-Tal, El Ghaoui and Nemirovski, Robust Optimization (Princeton, 2009) does the same for conic constraints, and the move is not routine. The left hand side of a conic constraint is a vector, not a scalar, so "the constraint is violated by at most α dist(ζ,Z)\alpha \,\mathrm{dist}(\zeta, \mathcal{Z})αdist(ζ,Z)" has no direct meaning. What replaces it is the observation that a scalar inequality aTy−b≤0a^Ty - b \le 0aTy−b≤0 is the inclusion aTy−b∈Q≡R−a^Ty - b \in \mathbf{Q} \equiv \mathcal{R}_-aTy−b∈Q≡R−​, and that the violation is the distance from the left hand side to Q\mathbf{Q}Q. In that form the notion lifts verbatim, and the whole chapter follows.

Setting

Definition 11.1.2. Consider an uncertain convex constraint

[P0+∑ℓ=1LζℓPℓ]y−[p0+∑ℓ=1Lζℓpℓ] ∈ Q,(11.1.4)\Bigl[P^0 + \sum_{\ell=1}^L \zeta_\ell P^\ell\Bigr]y - \Bigl[p^0 + \sum_{\ell=1}^L \zeta_\ell p^\ell\Bigr] \ \in\ \mathbf{Q}, \tag{11.1.4}[P0+ℓ=1∑L​ζℓ​Pℓ]y−[p0+ℓ=1∑L​ζℓ​pℓ] ∈ Q,(11.1.4)

with Q⊆Rk\mathbf{Q} \subseteq \mathcal{R}^kQ⊆Rk nonempty, closed and convex. Let the perturbation space split as RL=RL1×⋯×RLS\mathcal{R}^L = \mathcal{R}^{L_1}\times\cdots\times\mathcal{R}^{L_S}RL=RL1​×⋯×RLS​, each factor carrying a normal range Zs\mathcal{Z}^sZs, a closed convex cone Ls\mathcal{L}^sLs and a norm ∥⋅∥s\|\cdot\|_s∥⋅∥s​, and let ∥⋅∥Q\|\cdot\|_{\mathbf{Q}}∥⋅∥Q​ be a norm on Rk\mathcal{R}^kRk. A candidate yyy is robust feasible with global sensitivities αs\alpha_sαs​ if

dist(P(y,ζ),Q) ≤ ∑s=1Sαs dist(ζs,Zs∣Ls)∀ ζ∈Z+L,(11.1.6)\mathrm{dist}\bigl(P(y,\zeta), \mathbf{Q}\bigr) \ \le\ \sum_{s=1}^S \alpha_s\, \mathrm{dist}(\zeta^s, \mathcal{Z}^s|\mathcal{L}^s) \qquad \forall\, \zeta \in \mathcal{Z} + \mathcal{L}, \tag{11.1.6}dist(P(y,ζ),Q) ≤ s=1∑S​αs​dist(ζs,Zs∣Ls)∀ζ∈Z+L,(11.1.6)

where dist(u,Q)=min⁡v∈Q∥u−v∥Q\mathrm{dist}(u,\mathbf{Q}) = \min_{v\in\mathbf{Q}}\|u - v\|_{\mathbf{Q}}dist(u,Q)=minv∈Q​∥u−v∥Q​ and dist(ζs,Zs∣Ls)=min⁡{∥ζs−v∥s:v∈Zs, ζs−v∈Ls}\mathrm{dist}(\zeta^s,\mathcal{Z}^s|\mathcal{L}^s) = \min\{\|\zeta^s - v\|_s : v \in \mathcal{Z}^s,\ \zeta^s - v \in \mathcal{L}^s\}dist(ζs,Zs∣Ls)=min{∥ζs−v∥s​:v∈Zs, ζs−v∈Ls}.

The object that makes the analysis work is the recessive cone of Q\mathbf{Q}Q (Definition 11.3.1): for any xˉ∈Q\bar x \in \mathbf{Q}xˉ∈Q,

Rec(Q)={h:xˉ+th∈Q  ∀t≥0},\mathrm{Rec}(\mathbf{Q}) = \{h : \bar x + th \in \mathbf{Q}\ \ \forall t \ge 0\},Rec(Q)={h:xˉ+th∈Q  ∀t≥0},

which does not depend on xˉ\bar xxˉ and is a nonempty closed convex cone.

Formalization targets

Goal — Proposition 11.3.3, the decomposition of the conic GRC

A candidate yyy is feasible for the GRC (11.1.6) if and only if it satisfies the system

(a)[P0+∑ℓζℓPℓ]y−[p0+∑ℓζℓpℓ]∈Q∀ζ∈Z=Z1×⋯×ZS,\text{(a)}\quad \Bigl[P^0 + \sum_\ell \zeta_\ell P^\ell\Bigr]y - \Bigl[p^0 + \sum_\ell \zeta_\ell p^\ell\Bigr] \in \mathbf{Q} \qquad \forall \zeta \in \mathcal{Z} = \mathcal{Z}^1\times \cdots\times\mathcal{Z}^S,(a)[P0+ℓ∑​ζℓ​Pℓ]y−[p0+ℓ∑​ζℓ​pℓ]∈Q∀ζ∈Z=Z1×⋯×ZS, (bs)dist(∑ℓ[Pℓy−pℓ](Esζs)ℓ, Rec(Q)) ≤ αs∀ζs∈Ls with ∥ζs∥s≤1,s=1,…,S.\text{(b}_s)\quad \mathrm{dist}\Bigl(\sum_{\ell} [P^\ell y - p^\ell](E_s\zeta^s)_\ell,\ \mathrm{Rec}(\mathbf{Q})\Bigr) \ \le\ \alpha_s \qquad \forall \zeta^s \in \mathcal{L}^s \text{ with } \|\zeta^s\|_s \le 1, \quad s = 1,\ldots,S .(bs​)dist(ℓ∑​[Pℓy−pℓ](Es​ζs)ℓ​, Rec(Q)) ≤ αs​∀ζs∈Ls with ∥ζs∥s​≤1,s=1,…,S.

Line (a) is the ordinary robust counterpart over the normal range. Each line (bs_ss​) is a bounded semi-infinite constraint — the perturbation ranges over the unit ball of a cone, not over an unbounded set — measuring the distance to the recessive cone rather than to Q\mathbf{Q}Q itself.

Supporting targets

(Def 11.3.1)Rec(Q) is independent of the base point and is a nonempty closed convex cone,\text{(Def 11.3.1)}\quad \mathrm{Rec}(\mathbf{Q}) \text{ is independent of the base point and is a nonempty closed convex cone},(Def 11.3.1)Rec(Q) is independent of the base point and is a nonempty closed convex cone, (Ex 11.3.2)Q bounded⇒Rec(Q)={0};Q a cone⇒Rec(Q)=Q;Rec{u:Au−b∈K}={h:Ah∈K},\text{(Ex 11.3.2)}\quad \mathbf{Q} \text{ bounded} \Rightarrow \mathrm{Rec}(\mathbf{Q}) = \{0\}; \quad \mathbf{Q} \text{ a cone} \Rightarrow \mathrm{Rec}(\mathbf{Q}) = \mathbf{Q}; \quad \mathrm{Rec}\{u : Au - b \in \mathbf{K}\} = \{h : Ah \in \mathbf{K}\},(Ex 11.3.2)Q bounded⇒Rec(Q)={0};Q a cone⇒Rec(Q)=Q;Rec{u:Au−b∈K}={h:Ah∈K}, (Prop 11.4.1)ΨΞ(M)=ΨΞ∗(M∗),Ψ(M)=max⁡{dist∥⋅∥F(Me,KF):e∈KE, ∥e∥E≤1}.\text{(Prop 11.4.1)}\quad \Psi_\Xi(\mathcal{M}) = \Psi_{\Xi_*}(\mathcal{M}^*), \qquad \Psi(\mathcal{M}) = \max\{\mathrm{dist}_{\|\cdot\|_F}(\mathcal{M}e, \mathbf{K}^F) : e \in \mathbf{K}^E,\ \|e\|_E \le 1\} .(Prop 11.4.1)ΨΞ​(M)=ΨΞ∗​​(M∗),Ψ(M)=max{dist∥⋅∥F​​(Me,KF):e∈KE, ∥e∥E​≤1}.

Significance

The goal is the chapter's structural result and it does exactly what Proposition 3.2.1 did one level down: it converts a single semi-infinite constraint over an unbounded perturbation set into a robust counterpart over the bounded normal range plus finitely many constraints over unit balls. That matters because every tractability result of Chapters 6 to 9 is about bounded uncertainty sets; without the decomposition none of them applies to a GRC.

The two halves of the decomposition are genuinely different objects. Line (a) is familiar. Lines (bs_ss​) are not: they measure the distance from a linear image of a ball to the recessive cone, and that is the function

Ψ(M)=max⁡{dist(Me,KF):e∈KE, ∥e∥E≤1}\Psi(\mathcal{M}) = \max\bigl\{\mathrm{dist}(\mathcal{M}e, \mathbf{K}^F) : e \in \mathbf{K}^E,\ \|e\|_E \le 1\bigr\}Ψ(M)=max{dist(Me,KF):e∈KE, ∥e∥E​≤1}

of §11.4, which is almost a norm on linear maps — nonnegative, positively homogeneous, subadditive, but neither symmetric nor strictly positive. Proposition 11.4.1 says this function is self-dual in the precise sense that Ψ\PsiΨ of a map with respect to a setup equals Ψ\PsiΨ of the adjoint map with respect to the dual setup: dual norms, dual cones, source and destination exchanged. That single identity is what lets every bound on Ψ\PsiΨ be computed on whichever side of the duality is tractable, and it is the engine of §11.4's tractability results.

The recessive cone results are the vocabulary. The one that earns its place is Rec{u:Au−b∈K}={h:Ah∈K}\mathrm{Rec}\{u : Au - b \in \mathbf{K}\} = \{h : Ah \in \mathbf{K}\}Rec{u:Au−b∈K}={h:Ah∈K}: the conic sets of this book are all of that form, so it says the recessive cone of every constraint in sight is computed by deleting the constant term.

Difficulty

The goal is an equivalence and the two directions are asymmetric.

Forward — GRC implies the system — is where the recessive cone is discovered rather than used. Fix ζˉ∈Z\bar\zeta \in \mathcal{Z}ζˉ​∈Z and ζs\zeta^sζs in the unit ball of Ls\mathcal{L}^sLs, and run ζi=ζˉ+i ζs\zeta_i = \bar\zeta + i\,\zeta^sζi​=ζˉ​+iζs out along the cone. The GRC bounds the distance to Q\mathbf{Q}Q by αsi\alpha_s iαs​i, so there are qi∈Qq_i \in \mathbf{Q}qi​∈Q with ∥P(y,ζˉ)+iΦ(y)Esζs−qi∥Q≤αsi\|P(y,\bar\zeta) + i\Phi(y)E_s\zeta^s - q_i\|_{\mathbf{Q}} \le \alpha_s i∥P(y,ζˉ​)+iΦ(y)Es​ζs−qi​∥Q​≤αs​i; the rescaled points qi/iq_i/iqi​/i stay bounded, and a limit point of them lies in Rec(Q)\mathrm{Rec}(\mathbf{Q})Rec(Q) by the limit characterization of the recessive cone. This is a genuine compactness argument, and it is why the recessive cone — not Q\mathbf{Q}Q — is what appears in lines (bs_ss​).

Backward is a decomposition-and-assemble: split each ζs=ζˉs+δs\zeta^s = \bar\zeta^s + \delta^sζs=ζˉ​s+δs with ζˉs∈Zs\bar\zeta^s \in \mathcal{Z}^sζˉ​s∈Zs, δs∈Ls\delta^s \in \mathcal{L}^sδs∈Ls realizing the distance, get a point of Q\mathbf{Q}Q from line (a) and a recession direction from each line (bs_ss​), and add them — using that Q+Rec(Q)⊆Q\mathbf{Q} + \mathrm{Rec}(\mathbf{Q}) \subseteq \mathbf{Q}Q+Rec(Q)⊆Q.

Proposition 11.4.1 is a chain of polarity identities: the polar of X+KX + KX+K is Xo∩(−K∗)X^o \cap (-K_*)Xo∩(−K∗​) for compact convex XXX containing the origin, the polar of a norm ball of radius α\alphaα is the dual-norm ball of radius 1/α1/\alpha1/α, and bipolarity. Each step is standard and the composition is not.

Formalization scope

Built on the module published by the third mission of this series, which carries the linear-case globalized robust counterpart and the dual cone. New here: norms as functions with their defining properties, dual norms, the two distances, the recessive cone, the conic GRC, and the function Ψ\PsiΨ.

Conventions committed to:

  • Norms are functions carrying an explicit predicate, not typeclass instances. Chapter 11 quantifies over arbitrary norms ∥⋅∥Q\|\cdot\|_{\mathbf{Q}}∥⋅∥Q​ and ∥⋅∥s\|\cdot\|_s∥⋅∥s​ on fixed coordinate spaces, and a statement must be able to range over them; a typeclass instance would fix one norm per type. IsNormOn bundles definiteness, absolute homogeneity and the triangle inequality, and nonnegativity follows from them.
  • The dual norm is a predicate, not a construction. ∥f∥∗=sup⁡{fTe:∥e∥≤1}\|f\|^* = \sup\{f^Te : \|e\| \le 1\}∥f∥∗=sup{fTe:∥e∥≤1} is asserted as a least upper bound of the set of values, so no supremum is taken on faith.
  • Distances are infima, not minima. The source writes min⁡\minmin, which is correct because the sets are closed; writing inf⁡\infinf avoids carrying an attainment proof into every statement, and agrees with the minimum whenever the source's own hypotheses hold.
  • The recessive cone is indexed by a base point. Definition 11.3.1 defines it at an arbitrary xˉ∈Q\bar x \in \mathbf{Q}xˉ∈Q and then asserts independence of the choice; that assertion is one of the published items, so the definition cannot presuppose it.
  • The perturbation is carried as a family of blocks, ζ=(ζ1,…,ζS)\zeta = (\zeta^1,\ldots,\zeta^S)ζ=(ζ1,…,ζS) with ζs∈RLs\zeta^s \in \mathcal{R}^{L_s}ζs∈RLs​, rather than as a single vector in RL\mathcal{R}^LRL together with the embeddings EsE_sEs​. This is the same data and removes the index bookkeeping of EsE_sEs​ from every statement.
  • Ψ\PsiΨ is a predicate on a real number, as for the dual norm and for the same reason.
  • §11.2 and §11.5 are out of scope: the definition of a tight safe approximation of a GRC and the worked analysis of nonexpansive dynamical systems. The first is a definition the chapter uses only to phrase §11.4's programme, the second an application.

Selected references

  • A. Ben-Tal, L. El Ghaoui and A. Nemirovski, Robust Optimization, Princeton University Press, 2009. Chapter 11, §§11.1, 11.3-11.4, pp. 281-294; Chapter 3 for the linear case. https://doi.org/10.1515/9781400831050
  • A. Ben-Tal, S. Boyd and A. Nemirovski, Extending scope of robust optimization: comprehensive robust counterparts of uncertain problems, Mathematical Programming 107 (2006), 63-89. https://doi.org/10.1007/s10107-005-0679-z
  • R. T. Rockafellar, Convex Analysis, Princeton University Press, 1970. https://doi.org/10.1515/9781400873173
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