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

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Campaigns 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.

Quantum Max-Cut

Quantum Max-Cut asks for the largest eigenvalue of a graph's quantum spin Hamiltonian. For a graph GGG with nonnegative rational edge weights, write

HG=∑i<jwij(I−SWAPij),OPT(G)=λmax⁡(HG).H_G=\sum_{i<j}w_{ij}(I-\mathrm{SWAP}_{ij}),\qquad\mathrm{OPT}(G)=\lambda_{\max}(H_G).HG​=i<j∑​wij​(I−SWAPij​),OPT(G)=λmax​(HG​).

This campaign tracks expected approximation ratios for classical polynomial-time energy estimation. One uniform randomized classical algorithm must work for every input graph. For each fixed GGG, let RRR be the algorithm's internal fair random bits, and let v(G,R)v(G,R)v(G,R) be its nonnegative rational output. A ratio α\alphaα requires

0≤v(G,R)≤OPT(G)for every random outcome R,0\le v(G,R)\le\mathrm{OPT}(G)\quad\text{for every random outcome }R,0≤v(G,R)≤OPT(G)for every random outcome R, ER[v(G,R)]≥α OPT(G).\mathbb E_R[v(G,R)]\ge\alpha\,\mathrm{OPT}(G).ER​[v(G,R)]≥αOPT(G).

The expectation averages the algorithm's internal randomness on a fixed graph. Its running time is bounded by a polynomial on every run. Higher ratios are better.

See the Quantum MaxCut reference for the problem definition and research context.

≥ 0.5Formalized record→≥ 0.526Open frontier
3 provers on it3 of 8 missions formalized

Block Sensitivity vs. Sensitivity

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

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

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

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

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

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

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

≥ 2.13981Formalized record→≥ 2.15Open frontier
11 provers on it22 of 23 missions formalized

Integer Multiplication Below n log n

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

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

For two nnn-bit integers, the target is

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

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

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

3SUM Exponent

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

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

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

All-Pairs Shortest Paths (APSP) Exponent

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

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

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

The irrationality measure of π

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

≤ 2Formalized record
19 provers on it9 of 9 missions formalized

Sharp diagonal Hlawka constant

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

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

References:

  • Wolfram MathWorld, Hlawka's Inequality.
  • Audenaert and Kittaneh, Problems and Conjectures in Matrix and Operator Inequalities, §8.2 (2017).
  • Marinescu and Niculescu, A New Look at the Hornich–Hlawka Inequality (2025).
  • Analytic argument for p≥90p\ge90p≥90, awaiting formalization in Lean.
≤ 4Formalized record→≤ 2Open frontier
8 provers on it17 of 18 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.

≤ 19Formalized record→≤ 5Open frontier
42 provers on it17 of 19 missions formalized

Matrix multiplication exponent

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

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

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

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

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Mathematical Physics·Captain: Lucas

Microstate counting in dS₃: eigenvalue count vs. sphere partition functionResearch Paper

Motivation

Gibbons and Hawking conjectured that the cosmological horizon of a de Sitter static patch carries an entropy, computed semiclassically by the Euclidean gravitational path integral on the sphere. For three-dimensional de Sitter gravity the relevant quantity is log⁡∣ZgravS3∣\log|Z^{S^3}_{\mathrm{grav}}|log∣ZgravS3​∣, whose leading term is the Gibbons–Hawking entropy SGH=πℓdS/(2GN)S_{\mathrm{GH}} = \pi\ell_{\mathrm{dS}}/(2G_N)SGH​=πℓdS​/(2GN​). A microscopic account of this entropy — a count of states in some ordinary quantum or statistical system — is one of the long-standing goals of de Sitter holography.

Collier, Eberhardt and Mühlmann (arXiv:2501.01486) propose that pure dS3_33​ quantum gravity is dual to the double-scaled two-matrix integral of the complex Liouville string (arXiv:2409.17246). In §4.4 they test this by counting the "effective number of eigenvalues" of the matrix model and comparing 2log⁡Neff2\log N_{\mathrm{eff}}2logNeff​ with log⁡∣ZgravS3∣\log|Z^{S^3}_{\mathrm{grav}}|log∣ZgravS3​∣. The comparison reduces to explicit identities between elementary functions of the Liouville parameter bbb; this mission formalizes exactly those identities.

Setting

Fix a complex number bbb with −ib2∈R>0-ib^2 \in \mathbb{R}_{>0}−ib2∈R>0​, i.e. b2=iβb^2 = i\betab2=iβ with β>0\beta>0β>0 (the paper's footnote 2; then the central charge c=1+6(b+b−1)2c = 1+6(b+b^{-1})^2c=1+6(b+b−1)2 lies in 13+iR13+i\mathbb{R}13+iR). Write b−2=(b2)−1b^{-2} = (b^2)^{-1}b−2=(b2)−1 and let S0∈RS_0\in\mathbb{R}S0​∈R be the genus-counting parameter of the matrix model.

  • Eigenvalue density (eq. (C.4)): for real EEE,
ρ0(E)=2π sinh⁡(−iπb2) sin⁡ ⁣(−ib2 arccosh⁡E2).\rho_0(E) = \frac{2}{\pi}\,\sinh(-i\pi b^2)\,\sin\!\Big(-ib^2\,\operatorname{arccosh}\frac{E}{2}\Big).ρ0​(E)=π2​sinh(−iπb2)sin(−ib2arccosh2E​).
  • First zero (§4.4): E0=2cos⁡(πb−2)E_0 = 2\cos(\pi b^{-2})E0​=2cos(πb−2).
  • Effective number of eigenvalues (eq. (4.32)): Neff=∫2E0eS0ρ0(E) dEN_{\mathrm{eff}} = \int_2^{E_0} e^{S_0}\rho_0(E)\,dENeff​=∫2E0​​eS0​ρ0​(E)dE.
  • Microscopic entropy (eq. (4.33)): SdSmicro=2log⁡NeffS^{\mathrm{micro}}_{\mathrm{dS}} = 2\log N_{\mathrm{eff}}SdSmicro​=2logNeff​.
  • ZZ-instanton tension (eq. (4.34)): T^1,1(b)=8b2sin⁡(πb2)sin⁡(πb−2)1−b4\widehat T^{(b)}_{1,1} = \dfrac{8b^2\sin(\pi b^2)\sin(\pi b^{-2})}{1-b^4}T1,1(b)​=1−b48b2sin(πb2)sin(πb−2)​ and T1,1(b)=eS0 T^1,1(b)T^{(b)}_{1,1} = e^{S_0}\,\widehat T^{(b)}_{1,1}T1,1(b)​=eS0​T1,1(b)​.
  • Sphere normalization (eq. (4.4)): CS2(b)=32π4(sin⁡(πb2)sin⁡(πb−2)b2−b−2)2C^{(b)}_{S^2} = 32\pi^4\Big(\dfrac{\sin(\pi b^2)\sin(\pi b^{-2})}{b^2-b^{-2}}\Big)^2CS2(b)​=32π4(b2−b−2sin(πb2)sin(πb−2)​)2.
  • Sphere partition function (eq. (4.5)): ZgravS3∼e2S0 sin⁡(πb2)2sin⁡(πb−2)2(b−2−b2)2Z^{S^3}_{\mathrm{grav}} \sim e^{2S_0}\,\dfrac{\sin(\pi b^2)^2\sin(\pi b^{-2})^2}{(b^{-2}-b^2)^2}ZgravS3​∼e2S0​(b−2−b2)2sin(πb2)2sin(πb−2)2​, where ∼\sim∼ is equality up to a bbb-independent constant.

Formalization targets

Goal (eq. (4.35))

For any function Z(b,S0)Z(b,S_0)Z(b,S0​) whose modulus equals K⋅∣e2S0sin⁡(πb2)2sin⁡(πb−2)2/(b−2−b2)2∣K\cdot\big|e^{2S_0}\sin(\pi b^2)^2\sin(\pi b^{-2})^2/(b^{-2}-b^2)^2\big|K⋅​e2S0​sin(πb2)2sin(πb−2)2/(b−2−b2)2​ for a fixed constant K>0K>0K>0 (the content of (4.5)), there is a real constant ccc, independent of bbb and S0S_0S0​, such that

SdSmicro(b,S0)=log⁡∣Z(b,S0)∣+cfor all admissible b and all S0.S^{\mathrm{micro}}_{\mathrm{dS}}(b,S_0) = \log|Z(b,S_0)| + c \qquad\text{for all admissible } b \text{ and all } S_0.SdSmicro​(b,S0​)=log∣Z(b,S0​)∣+cfor all admissible b and all S0​.

This is the paper's statement that the matrix-model count reproduces the de Sitter entropy "regardless of the specific value of ZgravS3Z^{S^3}_{\mathrm{grav}}ZgravS3​", up to the order-one constants that (4.37) later fixes.

Milestones

  1. E0E_0E0​ is real, E0>2E_0>2E0​>2, ρ0(E0)=0\rho_0(E_0)=0ρ0​(E0​)=0, and ρ0\rho_0ρ0​ is real and positive on (2,E0)(2,E_0)(2,E0​) (§4.4, App. C).
  2. Closed form of NeffN_{\mathrm{eff}}Neff​ (eqs. (4.32)–(4.33)).
  3. The two expressions for SdSmicroS^{\mathrm{micro}}_{\mathrm{dS}}SdSmicro​ in eq. (4.33).
  4. (T^1,1(b))2∼CS2(b)(\widehat T^{(b)}_{1,1})^2 \sim C^{(b)}_{S^2}(T1,1(b)​)2∼CS2(b)​ (eq. (4.36)).

Significance

The identity (4.36) is the step the authors single out as "a genuinely nontrivial check": it holds for the complex Liouville string but, as they note, not for the Virasoro minimal string. The goal packages the argument of §4.4 into one exact statement, valid for every admissible bbb (i.e. exactly in GNG_NGN​), under the single physical input (4.5). The physical assumptions — the choice of cutoff at the first zero, the interpretation of log⁡N2\log N^2logN2 as an entropy, and (4.5) itself — are not formalized; they enter as definitions and as the hypothesis on ZZZ. The mathematical content is a definite-integral evaluation plus trigonometric/hyperbolic identities for complex arguments.

Difficulty

The integral in (4.32) has a complex-looking integrand, a branch of arccosh⁡\operatorname{arccosh}arccosh, and an upper limit given by a complex cosine; one must first show that everything is real in the admissible regime and then evaluate the integral exactly, including the endpoint behaviour at E=2E=2E=2 where arccosh⁡\operatorname{arccosh}arccosh is not differentiable. The entropy statements additionally involve the complex principal logarithm, so one must control the argument (positivity) of NeffN_{\mathrm{eff}}Neff​ and of the tension ratio; identities such as log⁡(eS0x)=S0+log⁡x\log(e^{S_0}x) = S_0+\log xlog(eS0​x)=S0​+logx fail for general complex xxx.

Formalization scope

  • b∈Cb\in\mathbb{C}b∈C with the hypothesis ∃β>0, b2=iβ\exists\beta>0,\ b^2 = i\beta∃β>0, b2=iβ; all objects depend on bbb only through b2b^2b2.
  • ρ0:R→C\rho_0 : \mathbb{R}\to\mathbb{C}ρ0​:R→C uses Mathlib's Real.arcosh (defined as log⁡(x+x2−1)\log(x+\sqrt{x^2-1})log(x+x2−1​)); its values for E<2E<2E<2 never enter.
  • NeffN_{\mathrm{eff}}Neff​ is the oriented interval integral from 222 to Re⁡E0\operatorname{Re}E_0ReE0​; milestone 1 shows E0E_0E0​ is real, so taking the real part loses nothing.
  • log⁡\loglog is the complex principal logarithm (Complex.log), and SdSmicroS^{\mathrm{micro}}_{\mathrm{dS}}SdSmicro​ is complex-valued; the goal forces it to equal a real number.
  • The "∼\sim∼" of (4.5) is encoded as a constant factor K>0K>0K>0 in the modulus; the "∼\sim∼" of (4.36) as a nonzero bbb-independent complex constant.
  • A trivialization is ruled out: the goal quantifies ccc before bbb and S0S_0S0​, and K>0K>0K>0 is required.

Selected references

  • S. Collier, L. Eberhardt, B. Mühlmann, A microscopic realization of dS3_33​, arXiv:2501.01486 (2025). https://arxiv.org/abs/2501.01486
  • S. Collier, L. Eberhardt, B. Mühlmann, V. A. Rodriguez, The complex Liouville string, arXiv:2409.17246 (2024). https://arxiv.org/abs/2409.17246
  • G. W. Gibbons, S. W. Hawking, Cosmological event horizons, thermodynamics, and particle creation, Phys. Rev. D 15 (1977) 2738. https://doi.org/10.1103/PhysRevD.15.2738
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Functional AnalysisMathematical Physics·Captain: Lucas

Uma Breve Introdução à Matemática da Mecânica Quântica I: Princípio da Incerteza de HeisenbergTextbook

Motivation

Heisenberg's uncertainty principle is the first quantitative statement a student meets about the incompatibility of position and momentum measurements in quantum mechanics. In A. O. Lopes' textbook Uma Breve Introdução à Matemática da Mecânica Quântica (31º Colóquio Brasileiro de Matemática, IMPA, 2017), written for mathematics students with no physics background, it is the capstone of Chapter 8 (Princípio da Incerteza e o Pacote de Onda Gaussiano), Teorema 8.2, p. 131. It collects the operator formalism built in Chapters 1, 3 and 4 — position and momentum operators, commutators, expected values — into one inequality. This mission is the first of a series formalizing the capstone results of the book.

Setting

A wave function is a map ψ:Rn→C\psi:\mathbb R^n\to\mathbb Cψ:Rn→C. The book uses the L2L^2L2 inner product ⟨φ,ψ⟩=∫Rnφ(x) ψ(x)‾ dx\langle \varphi,\psi\rangle=\int_{\mathbb R^n}\varphi(x)\,\overline{\psi(x)}\,dx⟨φ,ψ⟩=∫Rn​φ(x)ψ(x)​dx (linear in the first slot) and the norm ∣ψ∣=⟨ψ,ψ⟩1/2|\psi|=\langle\psi,\psi\rangle^{1/2}∣ψ∣=⟨ψ,ψ⟩1/2. A state is a wave function with ∣ψ∣=1|\psi|=1∣ψ∣=1. Fix n≥1n\ge 1n≥1, an index j∈{1,…,n}j\in\{1,\dots,n\}j∈{1,…,n} and the (reduced) Planck constant ℏ>0\hbar>0ℏ>0.

  • The position operator is (Xjψ)(x)=xj ψ(x)(X_j\psi)(x)=x_j\,\psi(x)(Xj​ψ)(x)=xj​ψ(x), with domain D(Xj)={ψ∈L2:xjψ∈L2}D(X_j)=\{\psi\in L^2 : x_j\psi\in L^2\}D(Xj​)={ψ∈L2:xj​ψ∈L2}.
  • The momentum operator is (Pjψ)(x)=−iℏ ∂ψ∂xj(x)(P_j\psi)(x)=-i\hbar\,\dfrac{\partial\psi}{\partial x_j}(x)(Pj​ψ)(x)=−iℏ∂xj​∂ψ​(x) (Definição 1.20), with domain D(Pj)D(P_j)D(Pj​) the C1C^1C1 functions of compact support.
  • The commutator of two operators is [A,B]=AB−BA[A,B]=AB-BA[A,B]=AB−BA (Definição 3.1).
  • The expected value of AAA in ψ\psiψ is Eψ(A)=⟨Aψ,ψ⟩⟨ψ,ψ⟩E_\psi(A)=\dfrac{\langle A\psi,\psi\rangle}{\langle\psi,\psi\rangle}Eψ​(A)=⟨ψ,ψ⟩⟨Aψ,ψ⟩​ (Definição 8.1, p. 125, and p. 128).
  • The dispersion of AAA in ψ\psiψ is Δψ(A)=∣ (A−Eψ(A) I)ψ ∣\Delta_\psi(A)=\big|\,(A-E_\psi(A)\,I)\psi\,\big|Δψ​(A)=​(A−Eψ​(A)I)ψ​ (Definição 8.2).
  • The Gaussian wave packet with parameters a>0a>0a>0, x0,p0∈Rnx_0,p_0\in\mathbb R^nx0​,p0​∈Rn is ψ(x)=(2πa2)−n/4 e−∣x−x0∣2/(4a2) e i⟨p0,x⟩/ℏ\psi(x)=(2\pi a^2)^{-n/4}\,e^{-|x-x_0|^2/(4a^2)}\,e^{\,i\langle p_0,x\rangle/\hbar}ψ(x)=(2πa2)−n/4e−∣x−x0​∣2/(4a2)ei⟨p0​,x⟩/ℏ (Definição 8.3).

Formalization targets

Goal — Teorema 8.2 (Heisenberg)

For every state ψ∈D(Xj)∩D(Pj)\psi\in D(X_j)\cap D(P_j)ψ∈D(Xj​)∩D(Pj​),

Δψ(Xj) Δψ(Pj)  ≥  ℏ2.\Delta_\psi(X_j)\,\Delta_\psi(P_j)\;\ge\;\frac{\hbar}{2}.Δψ​(Xj​)Δψ​(Pj​)≥2ℏ​.

Milestones

  1. Lema 3.2 (canonical commutation relations): [Xk,Xj]=[Pk,Pj]=0[X_k,X_j]=[P_k,P_j]=0[Xk​,Xj​]=[Pk​,Pj​]=0, iℏ[Pj,Xj]=Id\tfrac{i}{\hbar}[P_j,X_j]=\mathrm{Id}ℏi​[Pj​,Xj​]=Id, and iℏ[Pj,Xk]=0\tfrac{i}{\hbar}[P_j,X_k]=0ℏi​[Pj​,Xk​]=0 for j≠kj\ne kj=k.
  2. p. 23 — XjX_jXj​ is symmetric: ⟨Xjψ,φ⟩=⟨ψ,Xjφ⟩\langle X_j\psi,\varphi\rangle=\langle\psi,X_j\varphi\rangle⟨Xj​ψ,φ⟩=⟨ψ,Xj​φ⟩ on D(Xj)D(X_j)D(Xj​).
  3. pp. 26–27 — PjP_jPj​ is symmetric: ⟨Pjψ,φ⟩=⟨ψ,Pjφ⟩\langle P_j\psi,\varphi\rangle=\langle\psi,P_j\varphi\rangle⟨Pj​ψ,φ⟩=⟨ψ,Pj​φ⟩ on D(Pj)D(P_j)D(Pj​).
  4. Proposição 8.1 — Δψ(A)=0\Delta_\psi(A)=0Δψ​(A)=0 if and only if ψ\psiψ is an eigenfunction of AAA.
  5. Definição 8.3 / p. 133 — the Gaussian packet is a state with E(Xj)=(x0)jE(X_j)=(x_0)_jE(Xj​)=(x0​)j​, E(Pj)=(p0)jE(P_j)=(p_0)_jE(Pj​)=(p0​)j​, Δ(Xj)=a\Delta(X_j)=aΔ(Xj​)=a, and it attains equality Δ(Xj) Δ(Pj)=ℏ/2\Delta(X_j)\,\Delta(P_j)=\hbar/2Δ(Xj​)Δ(Pj​)=ℏ/2.

Significance

The inequality is the prototype of all Robertson-type uncertainty relations and is the point where the commutator formalism of the book produces a numerical, physically testable consequence. Milestone 5 shows the constant ℏ/2\hbar/2ℏ/2 cannot be improved. The mathematics is classical and fully proved in the source; what this mission adds is a machine-checked version of the textbook's operator calculus on L2(Rn)L^2(\mathbb R^n)L2(Rn) — integration by parts for compactly supported C1C^1C1 functions, symmetry of XjX_jXj​ and PjP_jPj​, commutation relations, and explicit Gaussian integrals — reusable by later missions of the series (Ehrenfest's theorem, density operators, quantum statistical mechanics).

Difficulty

The algebraic core is a short Cauchy–Schwarz argument, but it silently uses facts about unbounded operators: that ⟨ψ,[Pj,Xj]ψ⟩\langle\psi,[P_j,X_j]\psi\rangle⟨ψ,[Pj​,Xj​]ψ⟩ may be rewritten as ⟨Pjψ,Xjψ⟩−⟨Xjψ,Pjψ⟩\langle P_j\psi,X_j\psi\rangle-\langle X_j\psi,P_j\psi\rangle⟨Pj​ψ,Xj​ψ⟩−⟨Xj​ψ,Pj​ψ⟩ requires integration by parts with vanishing boundary terms, and the reduction to mean-zero observables requires the expected values to be real. Each of these needs integrability bookkeeping that the book leaves implicit. The Gaussian milestone requires evaluating first and second moments of Gaussian integrals in nnn dimensions.

Formalization scope

  • Rn\mathbb R^nRn is EuclideanSpace ℝ (Fin n) with Lebesgue measure; wave functions are plain functions ℝⁿ → ℂ (not L2L^2L2 classes), operators are maps on such functions, and domains are imposed as explicit hypotheses (InPositionDomain, InMomentumDomain).
  • The partial derivative ∂/∂xj\partial/\partial x_j∂/∂xj​ is the Fréchet derivative applied to the jjj-th basis vector.
  • Integrals are Bochner integrals, which return 000 for non-integrable integrands; every statement carries domain hypotheses guaranteeing integrability, so this junk value never enters a meaningful claim.
  • Expected values are complex numbers by definition; for symmetric operators they are real, which is part of what solvers must prove.
  • The goal is not vacuous: D(Pj)D(P_j)D(Pj​) contains nonzero compactly supported C1C^1C1 functions, which can be normalized.

Contributions welcome: integration-by-parts lemmas on Rn\mathbb R^nRn for compactly supported C1C^1C1 functions, Gaussian moment computations, and an abstract Robertson inequality.

Selected references

  • A. O. Lopes, Uma Breve Introdução à Matemática da Mecânica Quântica, 31º Colóquio Brasileiro de Matemática, IMPA, 2017. Extended version: http://mat.ufrgs.br/~alopes/hom/livroquantum.pdf
  • S. Gustafson, I. M. Sigal, Mathematical Concepts of Quantum Mechanics, Springer. https://doi.org/10.1007/978-3-030-59562-3
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CombinatoricsMathematical Logic·Captain: Lucas

Erdős Problem 592: which ω^β are partition ordinals?Open Problem

Motivation

Ramsey's theorem says that every red/blue colouring of the pairs of an infinite set has an infinite monochromatic subset. For well-ordered sets one can ask for more: the monochromatic set should have the same order type as the whole set. Erdős and Rado introduced the partition relation α→(β,c)2\alpha \to (\beta, c)^2α→(β,c)2 to measure exactly this, and asked which countable ordinals α\alphaα satisfy α→(α,3)2\alpha \to (\alpha, 3)^2α→(α,3)2 — every colouring either has a red copy of the whole order or a blue triangle. Such ordinals are called partition ordinals. Every partition ordinal α>1\alpha>1α>1 is a power of ω\omegaω, so the question becomes: for which countable β\betaβ is ωβ\omega^\betaωβ a partition ordinal? This is Erdős Problem 592.

The question is a basic test case for ordinal Ramsey theory: it is the smallest nontrivial "unbalanced" relation (a whole order type against a finite clique), and progress on it has repeatedly required new combinatorial methods.

Timeline (as recorded on erdosproblems.com/592):

  • 1957 — Specker. ω2→(ω2,3)2\omega^2 \to (\omega^2,3)^2ω2→(ω2,3)2, and ωn↛(ωn,3)2\omega^n \not\to (\omega^n,3)^2ωn→(ωn,3)2 for every finite n≥3n \ge 3n≥3.
  • 1972 — Chang. ωω→(ωω,3)2\omega^\omega \to (\omega^\omega,3)^2ωω→(ωω,3)2 (the subject of Erdős Problem 590). Milner extended this to ωω→(ωω,m)2\omega^\omega \to (\omega^\omega,m)^2ωω→(ωω,m)2 for all finite mmm; Larson (1973) gave a short proof.
  • 1974 — Galvin and Larson. If β≥3\beta \ge 3β≥3 and ωβ\omega^\betaωβ is a partition ordinal then β\betaβ is additively indecomposable, so β=ωγ\beta=\omega^\gammaβ=ωγ. They conjectured that every such β≥3\beta\ge3β≥3 works.
  • 2010 — Schipperus. Writing β=ωγ\beta=\omega^\gammaβ=ωγ: the relation holds when γ\gammaγ is a sum of one or two indecomposable ordinals, and fails when γ\gammaγ is a sum of four or more. This refutes the Galvin–Larson conjecture in general.

The case where γ\gammaγ is a sum of exactly three indecomposable ordinals appears to be the remaining open case.

Setting

An ordinal α\alphaα is identified with a well-ordered set XαX_\alphaXα​ of order type α\alphaα. A red/blue colouring of the complete graph KαK_\alphaKα​ on XαX_\alphaXα​ assigns to every pair of distinct vertices exactly one of two colours; equivalently, it is a pair of complementary simple graphs (red, blue) on XαX_\alphaXα​.

For ordinals α,β\alpha,\betaα,β and a cardinal ccc, the partition relation α→(β,c)2\alpha \to (\beta,c)^2α→(β,c)2 holds when every red/blue colouring of KαK_\alphaKα​ has

  • a set S⊆XαS \subseteq X_\alphaS⊆Xα​, all of whose pairs are red, whose order type (with the order inherited from XαX_\alphaXα​) is exactly β\betaβ, or
  • a set T⊆XαT \subseteq X_\alphaT⊆Xα​, all of whose pairs are blue, with ∣T∣=c|T| = c∣T∣=c.

The Lean predicate is Erdos592.OrdinalCardinalRamsey α β c, following the encoding used by the Formal Conjectures project. A partition ordinal is an α\alphaα with α→(α,3)2\alpha \to (\alpha,3)^2α→(α,3)2.

An ordinal is additively indecomposable if it is nonzero and a+b<βa+b<\betaa+b<β for all a,b<βa,b<\betaa,b<β; the additively indecomposable ordinals are exactly the powers ωδ\omega^\deltaωδ. An ordinal γ\gammaγ is the sum of kkk indecomposable ordinals when

γ=ωδ1+⋯+ωδk,δ1≥⋯≥δk,\gamma = \omega^{\delta_1}+\cdots+\omega^{\delta_k}, \qquad \delta_1 \ge \cdots \ge \delta_k,γ=ωδ1​+⋯+ωδk​,δ1​≥⋯≥δk​,

i.e. its Cantor normal form has kkk terms counted with multiplicity. The Lean predicate is Erdos592.IsSumOfIndecomposables k γ.

Formalization targets

Goal: the three-term case

γ countable, γ=ωδ1+ωδ2+ωδ3 (δ1≥δ2≥δ3)  ⟹  ωωγ→(ωωγ,3)2.\gamma \text{ countable},\ \gamma=\omega^{\delta_1}+\omega^{\delta_2}+\omega^{\delta_3}\ (\delta_1\ge\delta_2\ge\delta_3) \;\Longrightarrow\; \omega^{\omega^\gamma} \to \left(\omega^{\omega^\gamma}, 3\right)^2 .γ countable, γ=ωδ1​+ωδ2​+ωδ3​ (δ1​≥δ2​≥δ3​)⟹ωωγ→(ωωγ,3)2.

This is the positive answer in the open case, as predicted by the Galvin–Larson conjecture. Because the truth is unknown, a formal disproof (exhibiting a countable γ\gammaγ with three Cantor-normal-form terms for which the relation fails) is an equally valid resolution of the goal. Together with the milestones below, a proof of the goal gives a complete answer to Problem 592: for countable β\betaβ, ωβ\omega^\betaωβ is a partition ordinal iff β≤2\beta\le2β≤2 or β=ωγ\beta=\omega^\gammaβ=ωγ with γ\gammaγ a sum of at most three indecomposables.

Milestones (known results)

  1. Specker: ω2→(ω2,3)2\omega^2 \to (\omega^2,3)^2ω2→(ω2,3)2.
  2. Specker: ωn↛(ωn,3)2\omega^n \not\to (\omega^n,3)^2ωn→(ωn,3)2 for 3≤n<ω3 \le n < \omega3≤n<ω.
  3. Chang: ωω→(ωω,3)2\omega^\omega \to (\omega^\omega,3)^2ωω→(ωω,3)2.
  4. Galvin–Larson: β≥3\beta \ge 3β≥3 countable and ωβ→(ωβ,3)2\omega^\beta \to (\omega^\beta,3)^2ωβ→(ωβ,3)2 imply that β\betaβ is additively indecomposable.
  5. Schipperus: γ\gammaγ countable and a sum of one or two indecomposables imply ωωγ→(ωωγ,3)2\omega^{\omega^\gamma} \to (\omega^{\omega^\gamma},3)^2ωωγ→(ωωγ,3)2.
  6. Schipperus: γ\gammaγ countable and a sum of k≥4k \ge 4k≥4 indecomposables imply ωωγ↛(ωωγ,3)2\omega^{\omega^\gamma} \not\to (\omega^{\omega^\gamma},3)^2ωωγ→(ωωγ,3)2.

Significance

The result itself. A resolution of the three-term case would, together with the results above, finish the classification of countable partition ordinals of the form ωβ\omega^\betaωβ asked for in Problem 592. Either answer is informative: a positive answer shows the threshold between the positive and negative cases lies between three and four terms, and a negative answer shows it lies between two and three.

Formalizing it. The drafter is not aware of any of the milestone results in Mathlib. The Formal Conjectures entry for Problem 590 links an external Lean formalization of Chang's theorem; the other results (Specker's positive and negative theorems, Galvin–Larson, Schipperus) have, to the best of the drafter's knowledge, no public machine-checked proofs. Formalizing them is a substantial project on its own, independent of the open case, and the goal itself is an open research problem.

Difficulty

The property is not monotone in β\betaβ: it holds for β=2\beta=2β=2, fails for every finite β≥3\beta\ge3β≥3, holds again for β=ω\beta=\omegaβ=ω, and, by Schipperus, both holds and fails for various larger β=ωγ\beta=\omega^\gammaβ=ωγ depending on the number of terms in the Cantor normal form of γ\gammaγ. So no induction on β\betaβ can settle the question, and a naive transfer of the argument for a smaller exponent to a larger one can fail. The known positive and negative results use different arguments, and the three-term case lies exactly on the boundary between the ranges they cover.

Formalization scope

  • Ordinals and cardinals are Mathlib's Ordinal.{u} and Cardinal.{u} in an arbitrary universe u; "countable" is γ.card ≤ ℵ₀.
  • The graph lives on α.ToType, the canonical well-ordered type of order type α; a colouring is a pair of complementary SimpleGraphs (IsCompl red blue). A red KβK_\betaKβ​ is a red clique s with typeLT s = β; a blue K3K_3K3​ is a blue clique of cardinality exactly 3.
  • IsSumOfIndecomposables k γ requires a non-increasing list of exponents of length exactly k; without the ordering requirement, "sum of kkk" would not be well defined, since for instance ω+ω2=ω2\omega+\omega^2=\omega^2ω+ω2=ω2.
  • ω ^ ω ^ γ means ω(ωγ)\omega^{(\omega^\gamma)}ω(ωγ).
  • The Galvin–Larson milestone states additive indecomposability directly as ∀a,b<β, a+b<β\forall a,b<\beta,\ a+b<\beta∀a,b<β, a+b<β (for β≥3\beta \ge 3β≥3 this is equivalent to β=ωγ\beta=\omega^\gammaβ=ωγ).

The goal is not trivially satisfiable: the hypotheses hold, for example, for γ=3\gamma=3γ=3 and γ=ω2+ω+1\gamma=\omega^2+\omega+1γ=ω2+ω+1, and the conclusion is a genuine partition relation on an infinite ordinal.

Useful reusable infrastructure includes Cantor-normal-form combinatorics for countable ordinals, order-type calculations for subsets of ωβ\omega^\betaωβ, and a library of the classical colourings (Specker-type constructions). Contributions formalizing any milestone are welcome.

Selected references

  • T. F. Bloom, Erdős Problem #592, erdosproblems.com. https://www.erdosproblems.com/592 (this page lists the original references [Sp57], [Ch72], [GaLa74], [Sc10] cited below).
  • E. Specker, Teilmengen von Mengen mit Relationen, Comment. Math. Helv., 1957.
  • C. C. Chang, A partition theorem for the complete graph on ωω\omega^\omegaωω, J. Combinatorial Theory Ser. A, 1972.
  • J. A. Larson, A short proof of a partition theorem for the ordinal ωω\omega^\omegaωω, Ann. Math. Logic, 1973/74.
  • F. Galvin and J. Larson, Pinning countable ordinals, Fund. Math., 1974/75.
  • R. Schipperus, Countable partition ordinals, Ann. Pure Appl. Logic, 2010.
  • Formal Conjectures (Google DeepMind), Erdős Problems 590–592. https://github.com/google-deepmind/formal-conjectures
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Group Theory·Captain: dbenbenn

Cannon–Floyd–Parry: Thompson's group T is simpleTextbook

This mission formalizes §5 of J. W. Cannon, W. J. Floyd and W. R. Parry, Introductory notes on Richard Thompson's groups, L'Enseignement Mathématique (2) 42 (1996) 215–256, doi:10.5169/seals-87877: the definition of Thompson's group TTT and Thompson's proof that TTT is simple.

Motivation

Thompson's groups TTT and VVV, introduced in unpublished notes of Richard Thompson in 1965, were the first known examples of infinite, finitely presented, simple groups. Every finitely presented simple group known before them was finite. The notes of Cannon, Floyd and Parry were written in part "to make available Thompson's unpublished proofs … of the simplicity of TTT and VVV" (p. 216), and §5 is that proof for TTT.

TTT is the circle's counterpart of Thompson's group FFF. Earlier missions on this platform formalize FFF and its commutator subgroup (§1 and §4 of the same notes), its tree-diagram normal form (§2), and its two presentations (§3). FFF is not simple: its abelianization is Z2\mathbb{Z}^2Z2. TTT is simple, it has elements of finite order (the generator CCC below has order 333), and it contains FFF as the stabilizer of a point.

Setting

The circle S1S^1S1 is [0,1][0,1][0,1] with its endpoints identified, in Lean UnitAddCircle (R/Z\mathbb{R}/\mathbb{Z}R/Z); [x][x][x] denotes the image of x∈Rx \in \mathbb{R}x∈R. Maps compose right to left, (fg)(t)=f(g(t))(fg)(t) = f(g(t))(fg)(t)=f(g(t)), and [x,y]=xyx−1y−1[x, y] = x y x^{-1} y^{-1}[x,y]=xyx−1y−1, the convention of the notes.

The group TTT (pp. 233–234) consists of the piecewise linear homeomorphisms of S1S^1S1 that map images of dyadic rationals to images of dyadic rationals, are differentiable except at finitely many images of dyadic rationals, and have slopes that are powers of 222. In Lean a permutation fff of the circle satisfies IsThompsonCircle f when it has a lift to the line: an order isomorphism LLL of R\mathbb{R}R with L(x+1)=L(x)+1L(x+1) = L(x) + 1L(x+1)=L(x)+1 and f[x]=[L(x)]f[x] = [L(x)]f[x]=[L(x)], mapping dyadic rationals to dyadic rationals, and affine with slope a power of 222 between consecutive integer translates of finitely many dyadic breakpoints. T is the subgroup generated by these maps. That they already form a group is the first milestone.

The elements AAA, BBB, CCC (Example 5.1). AAA and BBB are the generators of FFF from the §1 mission (mapA, mapB), carried to the circle by toCircle, which sends an order isomorphism ggg of [0,1][0,1][0,1] to [x]↦[g(x)][x] \mapsto [g(x)][x]↦[g(x)]. CCC (mapC) is given on [0,1][0,1][0,1] by x/2+3/4x/2 + 3/4x/2+3/4, 2x−12x - 12x−1 and x−1/4x - 1/4x−1/4 on [0,12][0, \tfrac12][0,21​], [12,34][\tfrac12, \tfrac34][21​,43​] and [34,1][\tfrac34, 1][43​,1]. symT sends the formal symbols AAA, BBB, CCC to these three maps.

The presented group T1T_1T1​ (p. 236) is the free group on formal symbols AAA, BBB, CCC modulo six relators:

[AB−1,A−1BA],[AB−1,A−2BA2],C−1B(A−1CB),[AB^{-1}, A^{-1}BA],\quad [AB^{-1}, A^{-2}BA^2],\quad C^{-1}B(A^{-1}CB),[AB−1,A−1BA],[AB−1,A−2BA2],C−1B(A−1CB), ((A−1CB)(A−1BA))−1B(A−2CB2),(CA)−1(A−1CB)2,C3.((A^{-1}CB)(A^{-1}BA))^{-1}B(A^{-2}CB^2),\quad (CA)^{-1}(A^{-1}CB)^2,\quad C^3.((A−1CB)(A−1BA))−1B(A−2CB2),(CA)−1(A−1CB)2,C3.

In T1T_1T1​, X0=AX_0 = AX0​=A and Xn=A−(n−1)BAn−1X_n = A^{-(n-1)}BA^{n-1}Xn​=A−(n−1)BAn−1 (XT1); C0=1C_0 = 1C0​=1 and Cn=A−(n−1)CBn−1C_n = A^{-(n-1)}CB^{n-1}Cn​=A−(n−1)CBn−1 (CT1) for n≥1n \ge 1n≥1. An element is positive (IsPositiveT1) when it is a product of nonnegative powers of the XiX_iXi​.

Target

The goal is the sentence in which the notes state what §5 does, "In §5 we define TTT and give Thompson's proof that TTT is simple" (p. 216):

T is simple.T \text{ is simple.}T is simple.

The route is the section's own. Lemma 5.2 shows that AAA, BBB, CCC generate TTT and satisfy the six relations, so T1T_1T1​ maps onto TTT (Lemma 5.3). Lemmas 5.4–5.6 and a normal form (Theorem 5.7, every g∈T1g \in T_1g∈T1​ is p Cnmq−1p\,C_n^m q^{-1}pCnm​q−1 with ppp, qqq positive and m<n+2m < n + 2m<n+2) lead to Theorem 5.8, T1T_1T1​ is simple, and hence to Corollary 5.9, T1≅TT_1 \cong TT1​≅T. The goal follows.

Significance

The result. The simplicity of TTT is one of the two facts that made Thompson's groups famous: TTT is an infinite, finitely presented, simple group. Corollary 5.9 gives more, an explicit presentation of TTT on three generators and six relators.

Formalizing it. No machine-checked proof that TTT is simple exists on this platform, and Mathlib has nothing on Thompson's groups. The proof in the notes is short and complete. This mission connects the analytic definition of TTT with the combinatorial group T1T_1T1​, reusing the platform's formalization of FFF: the presentation of FFF (Theorem 3.4), its normal form (Corollary 2.7), and the fact that its proper quotients are Abelian (Theorem 4.3).

Difficulty

The algebra of T1T_1T1​ (Lemmas 5.5 and 5.6) is a chain of explicit inductions. The substance lies at two points.

The first is Theorem 5.7. The notes' proof that the set of elements p Cnmq−1p\,C_n^m q^{-1}pCnm​q−1 is closed under multiplication moves q1−1p2q_1^{-1}p_2q1−1​p2​ past CjiC_j^iCji​ and ClkC_l^kClk​ using the normal form of FFF, transported into T1T_1T1​ through Lemma 5.4, and then re-indexes, all inside the abstract group T1T_1T1​ with no geometry to lean on.

The second is the analytic side of Lemma 5.2. Generation reduces an arbitrary f∈Tf \in Tf∈T to an element of FFF by composing with CCC and with an element of FFF that moves f([0])f([0])f([0]) to [34][\tfrac34][43​]. That needs the fact that an element of TTT fixing [0][0][0] comes from FFF, which the notes state in one line. The relations are identities between explicit piecewise linear maps of the circle.

What is left out

  • The remark that TTT is conjugate to a group of C∞C^\inftyC∞ diffeomorphisms (Ghys–Sergiescu, p. 234). It is not used.
  • Tree diagrams for TTT and Figures 11–15. The notes use them only to verify relations 3)–6), and those relations are stated directly in Lemma 5.2.
  • The observation on p. 237 that CnC_nCn​ permutes n+2n + 2n+2 intervals cyclically, given "to gain some insight" and not used afterwards.

Formalization scope

  • TTT is a Subgroup (Equiv.Perm UnitAddCircle) generated by IsThompsonCircle. The lift makes every element an orientation-preserving homeomorphism, so continuity is not stated separately. Unlike for FFF, the condition that dyadics map to dyadics cannot be dropped: an irrational rotation satisfies every other clause.
  • T1T_1T1​ is Mathlib's PresentedGroup on the three-element type FormalABC. Relators are written out as xyx−1y−1xyx^{-1}y^{-1}xyx−1y−1, not with commutator notation.
  • Lemma 5.3 and Corollary 5.9 pin the images of the three symbols, so no isomorphism that ignores the generators can satisfy them. Lemma 5.4 pins the images of AAA and BBB.
  • Reused platform theorems, which solutions may import: Theorem 3.4 (F1≅FF_1 \cong FF1​≅F), Corollary 2.6 (AAA, BBB generate FFF), Lemma 4.2, Corollary 2.7, Lemma 2.8, Theorem 4.3, line (3.2), and Theorem 4.11 (FFF is totally ordered, hence torsion-free).
  • Welcome beyond the milestones: §6's group VVV, whose presentation extends T1T_1T1​.

Selected references

  • J. W. Cannon, W. J. Floyd, W. R. Parry, Introductory notes on Richard Thompson's groups, L'Enseignement Mathématique (2) 42 (1996) 215–256, §5 pp. 233–240. doi:10.5169/seals-87877
  • É. Ghys, V. Sergiescu, Sur un groupe remarquable de difféomorphismes du cercle, Comment. Math. Helv. 62 (1987) 185–239. doi:10.1007/BF02564445
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Differential GeometryMathematical Physics·Captain: Lucas

A No-Nonsense Introduction to General Relativity I: Birkhoff's theorem and the Schwarzschild solutionTextbook

Motivation

General relativity is summed up, in S. M. Carroll's A No-Nonsense Introduction to General Relativity (2001), by two statements: spacetime is a curved pseudo-Riemannian manifold with a metric of signature (−+++)(-+++)(−+++), and the metric obeys Einstein's equation Rμν−12Rgμν=8πGTμνR_{\mu\nu}-\frac12Rg_{\mu\nu}=8\pi GT_{\mu\nu}Rμν​−21​Rgμν​=8πGTμν​. The first exact solution of that equation, and still the most important one, is the Schwarzschild metric: it describes the gravitational field of the Sun outside its surface, the classical tests of GR (perihelion precession, light bending), and non-rotating black holes. Carroll's notes state its key property in one sentence: for a spherically symmetric metric, the vacuum equation has a unique solution, (72) — Birkhoff's theorem. This mission is the first of a series formalizing the capstone results of those notes.

Setting

We work in a single coordinate chart of four-dimensional spacetime. A point is x=(x0,x1,x2,x3)∈R4x=(x^0,x^1,x^2,x^3)\in\mathbb R^4x=(x0,x1,x2,x3)∈R4; a metric is a field x↦gμν(x)x\mapsto g_{\mu\nu}(x)x↦gμν​(x) of real symmetric 4×44\times44×4 matrices of signature (−+++)(-+++)(−+++), i.e. congruent to η=diag(−1,1,1,1)\eta=\mathrm{diag}(-1,1,1,1)η=diag(−1,1,1,1). From ggg and its inverse gμνg^{\mu\nu}gμν one builds, exactly as in Carroll's equations:

  • the Christoffel symbols Γμνσ=12gσρ(∂μgνρ+∂νgρμ−∂ρgμν)\Gamma^\sigma_{\mu\nu}=\frac12g^{\sigma\rho}(\partial_\mu g_{\nu\rho}+\partial_\nu g_{\rho\mu}-\partial_\rho g_{\mu\nu})Γμνσ​=21​gσρ(∂μ​gνρ​+∂ν​gρμ​−∂ρ​gμν​) (36) and the covariant derivative (35);
  • the Riemann tensor Rσμαβ=∂αΓμβσ−∂βΓμασ+ΓαλσΓμβλ−ΓβλσΓμαλR^\sigma{}_{\mu\alpha\beta}=\partial_\alpha\Gamma^\sigma_{\mu\beta}-\partial_\beta\Gamma^\sigma_{\mu\alpha}+\Gamma^\sigma_{\alpha\lambda}\Gamma^\lambda_{\mu\beta}-\Gamma^\sigma_{\beta\lambda}\Gamma^\lambda_{\mu\alpha}Rσμαβ​=∂α​Γμβσ​−∂β​Γμασ​+Γαλσ​Γμβλ​−Γβλσ​Γμαλ​ (44);
  • the Ricci tensor Rαβ=RλαλβR_{\alpha\beta}=R^\lambda{}_{\alpha\lambda\beta}Rαβ​=Rλαλβ​ (45), Ricci scalar R=gμνRμνR=g^{\mu\nu}R_{\mu\nu}R=gμνRμν​ (46) and Einstein tensor Gμν=Rμν−12RgμνG_{\mu\nu}=R_{\mu\nu}-\frac12Rg_{\mu\nu}Gμν​=Rμν​−21​Rgμν​ (50).

In spherical coordinates (t,r,θ,ϕ)=(x0,x1,x2,x3)(t,r,\theta,\phi)=(x^0,x^1,x^2,x^3)(t,r,θ,ϕ)=(x0,x1,x2,x3) the general spherically symmetric metric is (71)

ds2=−A(r,t) dt2+B(r,t) dr2+r2(dθ2+sin⁡2θ dϕ2),ds^2=-A(r,t)\,dt^2+B(r,t)\,dr^2+r^2(d\theta^2+\sin^2\theta\,d\phi^2),ds2=−A(r,t)dt2+B(r,t)dr2+r2(dθ2+sin2θdϕ2),

and the Schwarzschild metric (72) is the case A=1−2Gm/rA=1-2Gm/rA=1−2Gm/r, B=(1−2Gm/r)−1B=(1-2Gm/r)^{-1}B=(1−2Gm/r)−1.

Target

The goal is the uniqueness statement of §6 of the notes, in the form: for A,BA,BA,B smooth and positive on a rectangle (r1,r2)×(t1,t2)(r_1,r_2)\times(t_1,t_2)(r1​,r2​)×(t1​,t2​) with r1≥0r_1\ge0r1​≥0,

Rμν[−A dt2+B dr2+r2dΩ2]=0  ⟺  ∃ m, f>0: A=f(t)(1−2Gmr), B=(1−2Gmr)−1.R_{\mu\nu}\big[-A\,dt^2+B\,dr^2+r^2d\Omega^2\big]=0\iff\exists\,m,\ f>0:\ A=f(t)\Big(1-\frac{2Gm}{r}\Big),\ B=\Big(1-\frac{2Gm}{r}\Big)^{-1}.Rμν​[−Adt2+Bdr2+r2dΩ2]=0⟺∃m, f>0: A=f(t)(1−r2Gm​), B=(1−r2Gm​)−1.

The milestones follow the notes in order:

  1. eqs. (18)–(20): Minkowski space in spherical coordinates;
  2. eq. (25): gμνgμν=4g^{\mu\nu}g_{\mu\nu}=4gμνgμν​=4;
  3. after eq. (36): Γμνσ=Γνμσ\Gamma^\sigma_{\mu\nu}=\Gamma^\sigma_{\nu\mu}Γμνσ​=Γνμσ​;
  4. eq. (37): metric compatibility ∇σgμν=0=∇σgμν\nabla_\sigma g_{\mu\nu}=0=\nabla_\sigma g^{\mu\nu}∇σ​gμν​=0=∇σ​gμν;
  5. eq. (47): the algebraic symmetries of RμνρσR_{\mu\nu\rho\sigma}Rμνρσ​;
  6. eq. (48): Rμν=RνμR_{\mu\nu}=R_{\nu\mu}Rμν​=Rνμ​;
  7. eq. (49): the Bianchi identity ∇[λRμν]ρσ=0\nabla_{[\lambda}R_{\mu\nu]\rho\sigma}=0∇[λ​Rμν]ρσ​=0;
  8. eq. (51): the contracted Bianchi identity ∇μGμν=0\nabla_\mu G^{\mu\nu}=0∇μ​Gμν=0;
  9. eq. (67): −R=8πGT-R=8\pi GT−R=8πGT;
  10. eq. (68): the trace-reversed Einstein equation;
  11. eq. (69): in vacuum, Einstein's equation is Rμν=0R_{\mu\nu}=0Rμν​=0;
  12. eq. (72): the Schwarzschild metric is Ricci-flat for r>0r>0r>0, r≠2Gmr\ne2Gmr=2Gm;
  13. Birkhoff's theorem (the "only if" direction of the goal);
  14. eqs. (73)–(75): Kruskal coordinates, showing r=2Gmr=2Gmr=2Gm is a coordinate singularity.

Significance

The result. Birkhoff's theorem says the exterior field of any spherically symmetric body — static, pulsating or collapsing — is the Schwarzschild field, determined by a single constant mmm. It is why the Schwarzschild solution governs the solar system and spherical collapse, and why spherically symmetric gravitational radiation does not exist. The identities (37), (47)–(51) and (67)–(69) are the working toolkit of every GR computation; (51) is what makes Einstein's equation consistent with local energy–momentum conservation.

Formalizing it. All results here are classical and proved in the textbooks. The value of the mission is a machine-checked, coordinate-level development of the curvature identities in Carroll's exact conventions, and a checked proof of Birkhoff's theorem, which requires solving the vacuum equations as a system of PDEs rather than verifying a given solution. The platform already contains a separate Einstein-field-equations development (built from a Wikipedia-based definition file with a slightly different index placement) in which Ricci-flatness of the Schwarzschild metric is proved; this mission uses its own Carroll-faithful definitions, and that earlier work may help with milestone 12.

Difficulty

Verifying that a given metric is Ricci-flat (milestone 12) is a long but mechanical computation of derivatives of explicit functions. The goal is different in kind: in the "only if" direction one must extract from Rμν=0R_{\mu\nu}=0Rμν​=0 that ∂tB=0\partial_tB=0∂t​B=0 (from Rtr=0R_{tr}=0Rtr​=0), integrate an ODE in rrr to get B=(1−C/r)−1B=(1-C/r)^{-1}B=(1−C/r)−1 with CCC independent of ttt, and then show A/(1−C/r)A/(1-C/r)A/(1−C/r) depends on ttt only — all with the coordinate derivatives of the formal definitions, inside a region where A,BA,BA,B are only known to be smooth and positive. The general identities (47)–(51) need symmetry of second and third derivatives and the derivative of the matrix inverse.

Formalization scope

  • Everything lives in one chart: Coord = Fin 4 → ℝ, a metric is a function Coord → Matrix (Fin 4) (Fin 4) ℝ, partial derivatives are Fréchet derivatives in coordinate directions. All functions are total: non-differentiable points give derivative 000, singular matrices have inverse 000, and a/0=0a/0=0a/0=0. For that reason every statement names the open region (smoothness, signature (−+++)(-+++)(−+++), r>0r>0r>0, r≠2Gmr\ne2Gmr=2Gm, 0<θ<π0<\theta<\pi0<θ<π) on which it is claimed.
  • "Spacetime metric on UUU" means: UUU open, components C∞C^\inftyC∞ on UUU, and g(y)g(y)g(y) congruent to η\etaη for every y∈Uy\in Uy∈U (Carroll's standing assumption that the metric has signature (−+++)(-+++)(−+++)).
  • The goal is stated on a coordinate rectangle (r1,r2)×(t1,t2)(r_1,r_2)\times(t_1,t_2)(r1​,r2​)×(t1​,t2​) with the angular coordinates ranging over 0<θ<π0<\theta<\pi0<θ<π, ϕ∈R\phi\in\mathbb Rϕ∈R. The uniqueness is up to rescaling ttt (the factor f(t)f(t)f(t)); omitting fff would make the statement false.
  • Kruskal "takes the form" is encoded as the change-of-variables identity JTKJ=gSchwJ^{\mathsf T}KJ=g_{\text{Schw}}JTKJ=gSchw​, with the implicit relation (75) as a separate conclusion.
  • Reusable beyond this mission: the definition file CarrollGR_Defs (Christoffel symbols, covariant derivatives, curvature, Einstein tensor in coordinates) is shared by the whole series. Contributions welcome: general lemmas about partialD of products, quotients and matrix inverses, and a tensoriality lemma for the Ricci tensor under changes of coordinates.

Selected references

  • S. M. Carroll, A No-Nonsense Introduction to General Relativity, lecture notes, 2001 (the source; equation numbers above refer to it).
  • S. M. Carroll, Lecture Notes on General Relativity, 1997, arXiv:gr-qc/9712019 (the full notes of which the source is an abridgment).
  • R. M. Wald, General Relativity, University of Chicago Press, 1984.
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Mathematical Physics·Captain: Lucas

String Theory (Tong) I: The Critical Dimension D = 26Textbook

Motivation

The bosonic string can be quantized consistently only in D=26D=26D=26 spacetime dimensions. In lightcone quantization this appears in two ways in David Tong's Cambridge Part III lecture notes. First (Sections 2.2.2–2.3), the normal-ordering constant aaa in the mass formula M2=4α′(N−a)M^2=\frac{4}{\alpha'}(N-a)M2=α′4​(N−a) is identified with a regularized Casimir energy a=D−224a=\frac{D-2}{24}a=24D−2​, using ∑n≥1n\sum_{n\ge1}n∑n≥1​n "===" −112-\frac1{12}−121​; Lorentz invariance then forces the first excited states to be massless, which happens only for D=26D=26D=26. Second (Section 2.4), the commutator [Mi−,Mj−][M^{i-},M^{j-}][Mi−,Mj−] of lightcone Lorentz generators, which must vanish for the quantum theory to be Lorentz invariant, is proportional to a coefficient that vanishes for all oscillator levels nnn exactly when D=26D=26D=26 and a=1a=1a=1 (Goddard–Goldstone–Rebbi–Thorn 1973).

Setting

Let D≥2D\ge2D≥2 be the number of spacetime dimensions, so there are D−2D-2D−2 transverse oscillator directions, and let α′>0\alpha'>0α′>0 be the Regge slope. In lightcone gauge the mass of a closed-string state at level N=N~N=\tilde NN=N~ is (2.25)

M2=4α′(N−a),M^2=\frac{4}{\alpha'}(N-a),M2=α′4​(N−a),

with an undetermined normal-ordering constant aaa. The heuristic evaluation of aaa replaces the divergent zero-point sum D−22∑n≥1n\frac{D-2}2\sum_{n\ge1}n2D−2​∑n≥1​n by its cut-off regularization ∑n≥1ne−ϵn\sum_{n\ge1}ne^{-\epsilon n}∑n≥1​ne−ϵn, or by the Riemann zeta function value ζ(−1)\zeta(-1)ζ(−1), giving a=D−224a=\frac{D-2}{24}a=24D−2​ (2.26). The first excited states α~−1iα−1j∣0;p⟩\tilde\alpha^i_{-1}\alpha^j_{-1}|0;p\rangleα~−1i​α−1j​∣0;p⟩ (2.28) are (D−2)2(D-2)^2(D−2)2 in number and have M2=4α′(1−D−224)M^2=\frac4{\alpha'}\bigl(1-\frac{D-2}{24}\bigr)M2=α′4​(1−24D−2​). In one sector the level-2 states are α−1iα−1j∣0⟩\alpha^i_{-1}\alpha^j_{-1}|0\rangleα−1i​α−1j​∣0⟩ (unordered pairs {i,j}\{i,j\}{i,j}, since the oscillators commute) and α−2i∣0⟩\alpha^i_{-2}|0\rangleα−2i​∣0⟩. Finally, Section 2.4 states that

[Mi−,Mj−]=2(p+)2∑n>0([D−224−1]n+1n[a−D−224])(α−niαnj−α−njαni)+(α↔α~).[M^{i-},M^{j-}]=\frac{2}{(p^+)^2}\sum_{n>0}\left(\Big[\frac{D-2}{24}-1\Big]n+\frac1n\Big[a-\frac{D-2}{24}\Big]\right)\bigl(\alpha^i_{-n}\alpha^j_n-\alpha^j_{-n}\alpha^i_n\bigr)+(\alpha\leftrightarrow\tilde\alpha).[Mi−,Mj−]=(p+)22​n>0∑​([24D−2​−1]n+n1​[a−24D−2​])(α−ni​αnj​−α−nj​αni​)+(α↔α~).

Formalization targets

Goal: the anomaly coefficient vanishes iff D=26D=26D=26, a=1a=1a=1

For D∈ND\in\mathbb ND∈N and a∈Ra\in\mathbb Ra∈R,

(∀n≥1: [D−224−1]n+1n[a−D−224]=0)  ⟺  (D=26 and a=1).\Big(\forall n\ge1:\ \Big[\frac{D-2}{24}-1\Big]n+\frac1n\Big[a-\frac{D-2}{24}\Big]=0\Big)\iff\bigl(D=26\ \text{and}\ a=1\bigr).(∀n≥1: [24D−2​−1]n+n1​[a−24D−2​]=0)⟺(D=26 and a=1).

Milestones (in the order of the notes)

  1. Cut-off regularization: ∑n≥1ne−ϵn=1ϵ2−112+O(ϵ)\sum_{n\ge1}ne^{-\epsilon n}=\frac1{\epsilon^2}-\frac1{12}+O(\epsilon)∑n≥1​ne−ϵn=ϵ21​−121​+O(ϵ) as ϵ→0+\epsilon\to0^+ϵ→0+.
  2. Zeta-function regularization: ζ(−1)=−112\zeta(-1)=-\frac1{12}ζ(−1)=−121​.
  3. First excited states are massless iff D=26D=26D=26.
  4. Level-2 counting: 12(D−2)(D−1)+(D−2)=12D(D−1)−1\frac12(D-2)(D-1)+(D-2)=\frac12D(D-1)-121​(D−2)(D−1)+(D−2)=21​D(D−1)−1, the dimension of the traceless symmetric tensor representation of SO(D−1)SO(D-1)SO(D−1).

Significance

The result. The critical dimension is the single most-quoted prediction of the bosonic string, and the pair (D,a)=(26,1)(D,a)=(26,1)(D,a)=(26,1) fixes the entire lightcone spectrum: the tachyon M2=−4/α′M^2=-4/\alpha'M2=−4/α′, the massless graviton, BBB-field and dilaton, and the massive tower M2=4(N−1)/α′M^2=4(N-1)/\alpha'M2=4(N−1)/α′.

Formalizing it. This mission formalizes the mathematical steps of Tong's lightcone derivation: the two regularizations of ∑n\sum n∑n, the mass-shell and state-counting arithmetic, and the final algebraic step of the Lorentz-algebra argument. It does not formalize the operator computation of [Mi−,Mj−][M^{i-},M^{j-}][Mi−,Mj−] in the lightcone Fock space, which Tong quotes ("After a tedious computation, one finds ...") without derivation; that computation is a natural follow-up mission. The value ζ(−1)=−1/12\zeta(-1)=-1/12ζ(−1)=−1/12 is already available in Mathlib through the Bernoulli-number formula for ζ\zetaζ at negative integers.

Difficulty

The individual statements are elementary once formalized; the difficulty is faithfulness rather than proof. The regularized sum is an asymptotic statement whose leading term diverges, so it has to be stated as an O(ϵ)O(\epsilon)O(ϵ) remainder along ϵ→0+\epsilon\to0^+ϵ→0+ rather than as an equation; and the goal is a statement for all levels n≥1n\ge1n≥1, where a single level (n=1n=1n=1) only forces a=1a=1a=1 and two levels are needed to force D=26D=26D=26.

Formalization scope

The dimension DDD is a natural number and the normal-ordering constant aaa a real number. The regularized sum is Mathlib's tsum of ne−ϵnn e^{-\epsilon n}ne−ϵn over n∈Nn\in\mathbb Nn∈N (the n=0n=0n=0 term vanishes), and the asymptotic claim uses Mathlib's big-O along the right neighbourhood filter of 000. Level-2 states of one sector are counted as unordered pairs with repetition of transverse indices (Mathlib's Sym2 (Fin (D-2))) plus the D−2D-2D−2 states α−2i∣0⟩\alpha^i_{-2}|0\rangleα−2i​∣0⟩; natural-number subtraction and division are safe because D≥2D\ge2D≥2 is assumed and D(D−1)D(D-1)D(D−1) is even. The zeta function is Mathlib's riemannZeta, i.e. the analytic continuation.

Selected references

  • D. Tong, String Theory, Cambridge Part III lecture notes, 2009, Sections 2.2.2–2.4. http://www.damtp.cam.ac.uk/user/tong/string.html (arXiv:0908.0333)
  • P. Goddard, J. Goldstone, C. Rebbi, C. B. Thorn, Quantum dynamics of a massless relativistic string, Nucl. Phys. B 56 (1973) 109. https://doi.org/10.1016/0550-3213(73)90223-X
  • J. Polchinski, String Theory, Vol. 1, Cambridge University Press, 1998, Section 1.3.
  • B. Zwiebach, A First Course in String Theory, 2nd ed., Cambridge University Press, 2009, Chapter 12.
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Termodinâmica de Buracos Negros (Menezes 2021): the first law for Kerr black holesResearch Paper

Motivation

In 1973 Bardeen, Carter and Hawking showed that stationary black holes in general relativity obey four laws with the same structure as the laws of thermodynamics, with the surface gravity κ\kappaκ of the horizon playing the role of temperature and the horizon area AAA the role of entropy (Bardeen–Carter–Hawking 1973). Two years later Hawking showed that quantum fields near a black hole produce thermal radiation at temperature TBH=κ/2πT_{BH}=\kappa/2\piTBH​=κ/2π (Hawking 1975), which turned the analogy into an identification, with entropy SBH=A/4S_{BH}=A/4SBH​=A/4.

The M.Sc. dissertation Termodinâmica de Buracos Negros (F. H. de C. Menezes, UFMG, 2021) presents this construction for the Kerr black hole, the rotating stationary solution of Einstein's vacuum equations. The first law, eq. (3.79), is its central quantitative statement:

δM=κ8π δA+ΩH δJ,\delta M = \frac{\kappa}{8\pi}\,\delta A + \Omega_H\,\delta J,δM=8πκ​δA+ΩH​δJ,

relating first-order changes of mass MMM, horizon area AAA and angular momentum JJJ between neighbouring Kerr black holes, where ΩH\Omega_HΩH​ is the angular velocity of the horizon.

Timeline: Kerr found the rotating solution (1963); Smarr derived the mass formula M=κA/4π+2ΩHJM = \kappa A/4\pi + 2\Omega_H JM=κA/4π+2ΩH​J (1973); Bardeen, Carter and Hawking stated the four laws (1973); Hawking derived the thermal emission (1974–75).

Setting

Units are geometrized, G=c=1G=c=1G=c=1 (and ℏ=kB=1\hbar=k_B=1ℏ=kB​=1 for quantum quantities). A Kerr black hole has mass M>0M>0M>0 and rotation parameter aaa with a2≤M2a^2\le M^2a2≤M2; its angular momentum is J=MaJ=MaJ=Ma. In Boyer–Lindquist coordinates (t,r,θ,φ)(t,r,\theta,\varphi)(t,r,θ,φ) the metric involves

Δ=r2−2Mr+a2,Σ=r2+a2cos⁡2θ,\Delta = r^2-2Mr+a^2,\qquad \Sigma = r^2+a^2\cos^2\theta,Δ=r2−2Mr+a2,Σ=r2+a2cos2θ,

with angular components gθθ=Σg_{\theta\theta}=\Sigmagθθ​=Σ and gφφ=(r2+a2)2−Δa2sin⁡2θΣsin⁡2θg_{\varphi\varphi} = \dfrac{(r^2+a^2)^2-\Delta a^2\sin^2\theta}{\Sigma}\sin^2\thetagφφ​=Σ(r2+a2)2−Δa2sin2θ​sin2θ. The zeros of Δ\DeltaΔ are r±=M±M2−a2r_\pm = M\pm\sqrt{M^2-a^2}r±​=M±M2−a2​; the event horizon is r=r+r=r_+r=r+​.

  • The horizon area AAA is the area of the cross-section t=constt=\text{const}t=const, r=r+r=r_+r=r+​, computed from the induced metric: A=∫0π∫02πgθθgφφ dφ dθA=\int_0^\pi\int_0^{2\pi}\sqrt{g_{\theta\theta}g_{\varphi\varphi}}\,d\varphi\,d\thetaA=∫0π​∫02π​gθθ​gφφ​​dφdθ at r=r+r=r_+r=r+​.
  • The surface gravity is κ=M2−a22M(M+M2−a2)\kappa = \dfrac{\sqrt{M^2-a^2}}{2M(M+\sqrt{M^2-a^2})}κ=2M(M+M2−a2​)M2−a2​​ (eq. (3.3)).
  • The angular velocity of the horizon is ΩH=a2M(M+M2−a2)\Omega_H = \dfrac{a}{2M(M+\sqrt{M^2-a^2})}ΩH​=2M(M+M2−a2​)a​ (eq. (2.42)).

A Kerr black hole is non-extremal when a2<M2a^2<M^2a2<M2, equivalently ∣J∣<M2|J|<M^2∣J∣<M2.

Formalization targets

Goal — the first law (eq. (3.79))

Regard A,κ,ΩHA,\kappa,\Omega_HA,κ,ΩH​ as functions of (M,J)(M,J)(M,J) with a=J/Ma=J/Ma=J/M. For M>0M>0M>0 and J2<M4J^2<M^4J2<M4, the area is differentiable at (M,J)(M,J)(M,J) and, as linear forms in (δM,δJ)(\delta M,\delta J)(δM,δJ),

δM=κ8π δA+ΩH δJ.\delta M = \frac{\kappa}{8\pi}\,\delta A + \Omega_H\,\delta J .δM=8πκ​δA+ΩH​δJ.

Milestones, in the dissertation's order

  1. Eq. (2.42): ΩH=a/(r+2+a2)\Omega_H = a/(r_+^2+a^2)ΩH​=a/(r+2​+a2).
  2. Eq. (3.4): κ=(r+−r−)/(2(r+2+a2))\kappa = (r_+-r_-)/(2(r_+^2+a^2))κ=(r+​−r−​)/(2(r+2​+a2)).
  3. Eq. (3.44): A=8πM(M+M2−a2)A = 8\pi M\left(M+\sqrt{M^2-a^2}\right)A=8πM(M+M2−a2​).
  4. Eq. (3.43), Smarr formula: M=κA/4π+2ΩHJM = \kappa A/4\pi + 2\Omega_H JM=κA/4π+2ΩH​J.
  5. Eq. (3.78), variation of κ\kappaκ: δM=−A4πδκ−2J δΩH\delta M = -\frac{A}{4\pi}\delta\kappa - 2J\,\delta\Omega_HδM=−4πA​δκ−2JδΩH​.
  6. Eq. (3.81) and the following remark: κ=0  ⟺  ∣J∣=M2\kappa=0 \iff |J|=M^2κ=0⟺∣J∣=M2.
  7. Eq. (4.137): M(t)=(M03−t/256π)1/3M(t) = (M_0^3-t/256\pi)^{1/3}M(t)=(M03​−t/256π)1/3 solves M˙=−(768π)−1M−2\dot M = -(768\pi)^{-1}M^{-2}M˙=−(768π)−1M−2, M(0)=M0M(0)=M_0M(0)=M0​.

In the dissertation the first law is the sum of the variation (3.45) of the Smarr formula and the relation (3.78).

Significance

The first law is the identity behind the identification TBH=κ/2πT_{BH}=\kappa/2\piTBH​=κ/2π, SBH=A/4S_{BH}=A/4SBH​=A/4: with these values it becomes δM=TBH δSBH+ΩH δJ\delta M = T_{BH}\,\delta S_{BH} + \Omega_H\,\delta JδM=TBH​δSBH​+ΩH​δJ, the ordinary first law of thermodynamics for a rotating body. The Smarr formula is its integrated (Euler-relation) form, and the vanishing of κ\kappaκ at extremality underlies the dissertation's formulation of the third law.

All results are classical and proved in the literature. The contribution of the mission is a machine-checked version of the explicit Kerr relations, with the horizon area computed from the metric rather than taken as given, and a check of the dissertation's formulas. One such check is already recorded: the coefficient −2πJ-2\pi J−2πJ printed in eq. (3.78) conflicts with the dissertation's own eqs. (3.70) and (3.77), which give −2J-2J−2J, the value required for (3.79); the milestone uses −2J-2J−2J.

Difficulty

The dissertation derives the first law geometrically, from Komar integrals and a perturbation of the horizon Killing field. That route needs Lorentzian geometry, Killing horizons and Stokes' theorem on manifolds, which the Lean library does not provide. The explicit route through the Kerr formulas avoids this, but has its own obstacles: the horizon area is a double integral of a square root of a rational trigonometric expression that simplifies only on the horizon, where Δ(r+)=0\Delta(r_+)=0Δ(r+​)=0; and the differentials involve M2−J2/M2\sqrt{M^2-J^2/M^2}M2−J2/M2​, which is not differentiable at extremality, so the non-extremal hypothesis must be used when differentiating.

Formalization scope

All quantities are real-valued functions of real arguments, defined in one definition file in the namespace KerrBlackHoleThermo. Every theorem restricts to the physical range explicitly (M>0M>0M>0 and a2≤M2a^2\le M^2a2≤M2, or M>0M>0M>0 and J2<M4J^2<M^4J2<M4 for statements involving derivatives), so Lean's conventions for ⋅\sqrt{\cdot}⋅​ of negative numbers and division by zero do not enter the physical content. First-order variations "between two neighbouring Kerr configurations" are formalized as Fréchet derivatives (HasFDerivAt) of the explicit family in the coordinates (M,J)(M,J)(M,J); the first law is an identity of linear forms on R2\mathbb R^2R2. The horizon area is defined as a metric integral, not as the closed form (3.44), so the goal cannot be reduced to a pure algebraic identity by definition.

Out of scope: the general-spacetime versions of the zeroth, second (area theorem) and third laws, which need a theory of Lorentzian manifolds, event horizons and energy conditions, and the quantum field theory derivation of Hawking radiation in Chapter 4. Contributions building that infrastructure are welcome as separate missions.

Selected references

  • F. H. de C. Menezes, Termodinâmica de Buracos Negros, M.Sc. dissertation, Universidade Federal de Minas Gerais, 2021 (the source of this mission).
  • J. M. Bardeen, B. Carter, S. W. Hawking, The four laws of black hole mechanics, Commun. Math. Phys. 31 (1973) 161–170. https://doi.org/10.1007/BF01645742
  • S. W. Hawking, Particle creation by black holes, Commun. Math. Phys. 43 (1975) 199–220. https://doi.org/10.1007/BF02345020
  • L. Smarr, Mass formula for Kerr black holes, Phys. Rev. Lett. 30 (1973) 71–73. https://doi.org/10.1103/PhysRevLett.30.71
  • R. P. Kerr, Gravitational field of a spinning mass as an example of algebraically special metrics, Phys. Rev. Lett. 11 (1963) 237–238. https://doi.org/10.1103/PhysRevLett.11.237
  • R. M. Wald, General Relativity, University of Chicago Press, 1984.
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AlgebraAlgebraic GeometryNumber Theory·Captain: vatsj

Milnor conjecture (Voevodsky 2003), formalizedResearch Paper

Motivation

For a field FFF, two invariants built from very different data turn out to carry the same mod-2 information. One is Milnor K-theory KnM(F)K^M_n(F)KnM​(F), defined by generators and relations from the multiplicative group F×F^\timesF× alone. The other is Galois cohomology Hn(F,Z/2)H^n(F,\mathbb{Z}/2)Hn(F,Z/2), the continuous cohomology of the absolute Galois group of FFF. In 1970 Milnor considered a natural map KnM(F)/2→Hn(F,Z/2)K^M_n(F)/2 \to H^n(F,\mathbb{Z}/2)KnM​(F)/2→Hn(F,Z/2) in all degrees, verified that it is an isomorphism for several classes of fields, and remarked that he knew of no field where it fails (Milnor 1970). The statement that it is always an isomorphism when char⁡F≠2\operatorname{char} F \neq 2charF=2 became known as the Milnor conjecture. Its companion conjecture on quadratic forms was later deduced from it (Orlov–Vishik–Voevodsky 2007). Together they identify the graded Witt ring of quadratic forms, Galois cohomology mod 2, and K∗M(F)/2K^M_*(F)/2K∗M​(F)/2.

Timeline. The attributions below follow the introduction of Voevodsky 2003.

  • 1970: Milnor considers the map KnM(F)/2→Hn(F,Z/2)K^M_n(F)/2 \to H^n(F,\mathbb{Z}/2)KnM​(F)/2→Hn(F,Z/2) in all degrees and gives classes of fields where it is an isomorphism (Milnor 1970).
  • Bass–Tate (published 1973): the Kummer classes satisfy the Steinberg relation, so the Kummer map extends to a ring homomorphism on K∗M(F)K^M_*(F)K∗M​(F) (Bass–Tate 1973).
  • Degrees 0 and 1: the map is an isomorphism, by Kummer theory and Hilbert's Theorem 90.
  • 1981: Merkurjev proves degree 2 with 222 as the coefficient prime.
  • 1982: Merkurjev and Suslin extend degree 2 to every prime ℓ\ellℓ (Merkurjev–Suslin 1982).
  • Degree 3, ℓ=2\ell = 2ℓ=2: proved by Merkurjev–Suslin and, independently, by Rost.
  • 2003: Voevodsky proves all degrees, in every characteristic ≠2\neq 2=2 (Voevodsky 2003, Cor. 7.5), using the motivic Steenrod operations constructed in Voevodsky 2003b. This work was cited for his 2002 Fields Medal.
  • 2011: the analogue for odd primes, the Bloch–Kato conjecture, is proved (Voevodsky 2011); a book-length account is Haesemeyer–Weibel 2019.

Setting

Let FFF be a field with 2≠02 \neq 02=0 in FFF.

Milnor K-theory. For n≥0n \ge 0n≥0, KnM(F)K^M_n(F)KnM​(F) is the quotient of the nnn-fold tensor power (F×)⊗n(F^\times)^{\otimes n}(F×)⊗n, taken over Z\mathbb{Z}Z with F×F^\timesF× written additively, by the subgroup generated by the pure tensors a1⊗⋯⊗ana_1\otimes\cdots\otimes a_na1​⊗⋯⊗an​ in which some adjacent pair satisfies ai+ai+1=1a_i + a_{i+1} = 1ai​+ai+1​=1. This is the degree-nnn part of T(F×)/IT(F^\times)/IT(F×)/I, where III is the two-sided ideal generated by a⊗(1−a)a\otimes(1-a)a⊗(1−a). The class of a1⊗⋯⊗ana_1\otimes\cdots\otimes a_na1​⊗⋯⊗an​ is the symbol {a1,…,an}\{a_1,\dots,a_n\}{a1​,…,an​}. In particular K0M(F)=ZK^M_0(F) = \mathbb{Z}K0M​(F)=Z and K1M(F)=F×K^M_1(F) = F^\timesK1M​(F)=F×. In Lean these are MilnorK F n and symbol a for a : Fin n → Fˣ.

Galois cohomology. Let FsepF^{\mathrm{sep}}Fsep be a separable closure and GF=Gal⁡(Fsep/F)G_F = \operatorname{Gal}(F^{\mathrm{sep}}/F)GF​=Gal(Fsep/F) the absolute Galois group, a profinite group under the Krull topology. Hn(F,Z/2)H^n(F,\mathbb{Z}/2)Hn(F,Z/2) is the continuous cohomology Hctsn(GF,Z/2)H^n_{\mathrm{cts}}(G_F,\mathbb{Z}/2)Hctsn​(GF​,Z/2) with trivial action, computed from GFG_FGF​-invariant continuous homogeneous cochains. In Lean this is H F n, Mathlib's continuousCohomology n of the trivial representation.

The Galois symbol. For a∈F×a \in F^\timesa∈F× fix a∈Fsep\sqrt a \in F^{\mathrm{sep}}a​∈Fsep. The Kummer character χa:GF→Z/2\chi_a : G_F \to \mathbb{Z}/2χa​:GF​→Z/2 is χa(σ)=0\chi_a(\sigma) = 0χa​(σ)=0 if σ(a)=a\sigma(\sqrt a) = \sqrt aσ(a​)=a​ and 111 otherwise. It is a continuous homomorphism representing the Kummer class δa∈H1\delta a \in H^1δa∈H1. The Galois symbol of (a1,…,an)(a_1,\dots,a_n)(a1​,…,an​) is the class of the homogeneous cocycle

(x0,…,xn) ⟼ ∏j=1n(χaj(xj)−χaj(xj−1)),(x_0,\dots,x_n)\ \longmapsto\ \prod_{j=1}^{n}\bigl(\chi_{a_j}(x_j)-\chi_{a_j}(x_{j-1})\bigr),(x0​,…,xn​) ⟼ j=1∏n​(χaj​​(xj​)−χaj​​(xj−1​)),

the homogeneous form of (σ1,…,σn)↦χa1(σ1)⋯χan(σn)(\sigma_1,\dots,\sigma_n) \mapsto \chi_{a_1}(\sigma_1)\cdots\chi_{a_n}(\sigma_n)(σ1​,…,σn​)↦χa1​​(σ1​)⋯χan​​(σn​), i.e. the cup product δa1∪⋯∪δan\delta a_1\cup\cdots\cup\delta a_nδa1​∪⋯∪δan​. In Lean this is galoisSymbol a.

Formalization targets

Goal: the Milnor conjecture (Voevodsky 2003, Corollary 7.5)

For every field FFF with char⁡F≠2\operatorname{char} F \neq 2charF=2 and every n≥0n \ge 0n≥0 there is a homomorphism

φ:KnM(F)→Hn(F,Z/2),φ{a1,…,an}=δa1∪⋯∪δan,\varphi : K^M_n(F) \to H^n(F,\mathbb{Z}/2),\qquad \varphi\{a_1,\dots,a_n\} = \delta a_1\cup\cdots\cup\delta a_n,φ:KnM​(F)→Hn(F,Z/2),φ{a1​,…,an​}=δa1​∪⋯∪δan​,

which is surjective and whose kernel is exactly 2 KnM(F)2\,K^M_n(F)2KnM​(F).

Since symbols generate KnM(F)K^M_n(F)KnM​(F), such a φ\varphiφ is unique; it is the norm residue homomorphism. The statement is therefore equivalent to KnM(F)/2≅Hn(F,Z/2)K^M_n(F)/2 \cong H^n(F,\mathbb{Z}/2)KnM​(F)/2≅Hn(F,Z/2) via the norm residue map. Its existence, i.e. the fact that the Steinberg relations map to zero, is part of the claim.

Significance

The result itself. The theorem gives a presentation of mod-2 Galois cohomology by generators and relations: every class is a sum of cup products of degree-one classes, and every relation among such products comes from Steinberg relations and multiples of 2. With Orlov–Vishik–Voevodsky 2007 it yields Milnor's conjecture on quadratic forms, which classifies quadratic forms up to Witt equivalence by their Galois-cohomological invariants.

Formalizing it. The theorem is proved but not formalized. At the time of writing, Mathlib has neither Milnor K-theory nor cup products in group or continuous cohomology, and has Hilbert 90 only for finite Galois extensions. This mission's definitions provide a sorry-free Galois symbol in Mathlib's continuous cohomology, which already makes the degree 0 and degree 1 cases (Kummer theory) meaningful targets. A complete development would formalize the IHES proof, including motivic cohomology with Z/2\mathbb{Z}/2Z/2 coefficients and the motivic Steenrod algebra. No part of that is currently available in Lean. Related existing work: on this platform, a graded cup product (groupCohomology.exists_isGradedCupProduct) and a Kummer theory and Hilbert 90 for level-constant cocycles have been formalized on top of Mathlib's discrete groupCohomology. The cup product is for discrete groups, and the Kummer and Hilbert 90 results use finite-level hypotheses in place of continuity, so none of them transfers directly to continuousCohomology.

Difficulty

Degrees 0 and 1 follow from Kummer theory and Hilbert 90. Degree 2 is Merkurjev's theorem, whose proof goes through the K-theory of Severi–Brauer varieties. No argument internal to Galois cohomology or K-theory of fields is known in higher degrees. The known proof reformulates the statement as a vanishing theorem for motivic cohomology of fields, the "Hilbert 90" property for weight nnn. It then argues by induction on nnn through geometry over FFF: splitting varieties of symbols (Pfister quadrics), their motives, and cohomology operations on motivic cohomology. Each of these is a substantial theory, none of it exists in Mathlib, and the induction passes through statements about arbitrary smooth varieties, not only fields.

Formalization scope

Scope. The target is the Milnor conjecture, i.e. the prime 222 with coefficients Z/2≅μ2\mathbb{Z}/2 \cong \mu_2Z/2≅μ2​. The Bloch–Kato conjecture for odd primes is out of scope.

Conventions.

  • The field is F : Type, universe 0. Mathlib's continuousCohomology requires the coefficient module to live in the universe of the group. For FFF in a higher universe this forces ULift (ZMod 2), for which the needed Module and ContinuousSMul instances are not available as global instances. Universe polymorphism is not part of this mission. It does not follow by plain transport, since a field in a higher universe need not be isomorphic to any field in Type; one route is a limit argument, using that both sides commute with directed unions of fields and that every field is the directed union of its countable subfields, each isomorphic to a field in Type.
  • The hypothesis char⁡F≠2\operatorname{char} F \neq 2charF=2 is [NeZero (2 : F)].
  • HnH^nHn is Mathlib's continuousCohomology, built from homogeneous cochains, with Z/2\mathbb{Z}/2Z/2 as a trivial representation of GFG_FGF​ with the Krull topology.
  • KnM(F)K^M_n(F)KnM​(F) is defined one degree at a time, not as a graded ring.
  • "Kernel =2KnM= 2K^M_n=2KnM​" means φ(x)=0  ⟺  ∃y, x=2y\varphi(x)=0 \iff \exists y,\ x = 2yφ(x)=0⟺∃y, x=2y.

Ruling out trivializations. The Galois symbol is not a free parameter. It is a fixed, sorry-free definition, and the existence of φ\varphiφ with the prescribed values on symbols is part of the goal. Neither can be chosen to make the statement vacuous.

Route. Reductions should follow Voevodsky 2003 together with Voevodsky 2003b. That route avoids resolution of singularities and works in every characteristic ≠2\neq 2=2. The following rely on resolution of singularities (or on characteristic-0 reductions) and should not be used as inputs:

  • Mazza–Voevodsky–Weibel (MVW 2006), results 16.24, 16.25 and 20.1, and the cdh-topology and compactly-supported-motive material;
  • the original Suslin–Voevodsky paper relating Bloch–Kato to Beilinson–Lichtenbaum (Suslin–Voevodsky 2000); use Haesemeyer–Weibel 2019, Chapter 2, instead;
  • Haesemeyer–Weibel Part II, and their reduction to characteristic 0 (Lemma 1.3);
  • Voevodsky's 1995–96 preprints on the Milnor conjecture.

Infrastructure needed and reusable. A complete development needs:

  • the ring structure on K∗M(F)K^M_*(F)K∗M​(F) (cf. Carlier's KMilnorWitt for Milnor–Witt K-theory);
  • cup products in continuous cohomology;
  • Hilbert 90 for profinite Galois groups;
  • Galois cohomology as étale cohomology of Spec⁡F\operatorname{Spec} FSpecF;
  • the Nisnevich topology;
  • presheaves with transfers, motivic complexes and motivic cohomology;
  • motivic Steenrod operations;
  • motives of Pfister quadrics.

Most of this is reusable well beyond the mission. The homogeneous-cochain construction in the definition files, which turns an invariant continuous cocycle Gn+1→MG^{n+1}\to MGn+1→M into a class in Mathlib's continuousCohomology, applies to any locally compact group with trivial coefficients. Contributions of any of these components, and of the degree 0 and 1 cases, are welcome.

Selected references

  • V. Voevodsky, Motivic cohomology with Z/2\mathbb{Z}/2Z/2-coefficients, Publ. Math. IHÉS 98 (2003), 59–104. https://doi.org/10.1007/s10240-003-0010-6
  • V. Voevodsky, Reduced power operations in motivic cohomology, Publ. Math. IHÉS 98 (2003), 1–57. https://doi.org/10.1007/s10240-003-0009-z
  • J. Milnor, Algebraic K-theory and quadratic forms, Invent. Math. 9 (1970), 318–344. https://doi.org/10.1007/BF01425486
  • H. Bass, J. Tate, The Milnor ring of a global field, in Algebraic K-theory II, Lecture Notes in Math. 342, Springer, 1973. https://doi.org/10.1007/BFb0073733
  • A. S. Merkurjev, A. A. Suslin, K-cohomology of Severi–Brauer varieties and the norm residue homomorphism, Math. USSR Izv. 21 (1983). https://doi.org/10.1070/IM1983v021n02ABEH001793
  • D. Orlov, A. Vishik, V. Voevodsky, An exact sequence for K∗M/2K^M_*/2K∗M​/2 with applications to quadratic forms, Ann. of Math. 165 (2007), 1–13. https://doi.org/10.4007/annals.2007.165.1
  • V. Voevodsky, On motivic cohomology with Z/l\mathbb{Z}/lZ/l-coefficients, Ann. of Math. 174 (2011), 401–438. https://doi.org/10.4007/annals.2011.174.1.11
  • C. Haesemeyer, C. Weibel, The Norm Residue Theorem in Motivic Cohomology, Annals of Math. Studies 200, Princeton, 2019. https://doi.org/10.1515/9780691189635
  • C. Mazza, V. Voevodsky, C. Weibel, Lecture Notes on Motivic Cohomology, Clay Math. Monographs 2, AMS, 2006. https://www.claymath.org/wp-content/uploads/2022/03/Motivic-Cohomology.pdf
  • A. Suslin, V. Voevodsky, Bloch–Kato conjecture and motivic cohomology with finite coefficients, in The Arithmetic and Geometry of Algebraic Cycles, NATO Sci. Ser. C 548, Kluwer, 2000. https://doi.org/10.1007/978-94-011-4098-0_5
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Information TheoryTheoretical Computer Science·Captain: marwahaha

Most Informative Boolean Function ConjectureResearch Paper

One bit of a noisy string

Send a uniformly random string X∈{0,1}nX \in \{0,1\}^nX∈{0,1}n through a memoryless binary symmetric channel with crossover probability ppp: each coordinate is flipped independently with probability ppp, producing Y∈{0,1}nY \in \{0,1\}^nY∈{0,1}n. An observer sees YYY and wants to learn about XXX — but the summary of XXX they are allowed to keep is a single bit f(X)f(X)f(X), computed by a Boolean function fff chosen in advance. Which choice of fff makes that one bit most informative about the noisy observation, in Shannon's sense?

The natural candidate is a dictator, f(x)=xif(x) = x_if(x)=xi​: keep one coordinate and forget the rest. It achieves I(f(X);Y)=I(Xi;Yi)=1−H(p)I(f(X); Y) = I(X_i; Y_i) = 1 - H(p)I(f(X);Y)=I(Xi​;Yi​)=1−H(p), where HHH is the binary entropy function in bits. Majority, parity, and every other symmetric or balanced construction does worse. Courtade and Kumar conjectured in 2014 that nothing does better: no Boolean function of nnn noisy-channel inputs, however many coordinates it reads and however it combines them, beats a single coordinate.

Setting

Fix n∈Nn \in \mathbb{N}n∈N, a crossover probability p∈[0,1]p \in [0,1]p∈[0,1], and a Boolean function f:{0,1}n→{0,1}f : \{0,1\}^n \to \{0,1\}f:{0,1}n→{0,1}. With XXX uniform on the cube and YYY its image under the channel, all the relevant quantities are finite sums: the joint mass of (f(X),Y)(f(X), Y)(f(X),Y) is

Pr⁡[f(X)=b, Y=y]  =  2−n∑x∈{0,1}n1[f(x)=b]∏i=1n((1−p)1[xi=yi]p1[xi≠yi]),\Pr[f(X) = b,\, Y = y] \;=\; 2^{-n}\sum_{x \in \{0,1\}^n} \mathbf{1}[f(x) = b] \prod_{i=1}^{n} \bigl( (1-p)^{\mathbf{1}[x_i = y_i]} p^{\mathbf{1}[x_i \neq y_i]} \bigr),Pr[f(X)=b,Y=y]=2−nx∈{0,1}n∑​1[f(x)=b]i=1∏n​((1−p)1[xi​=yi​]p1[xi​=yi​]),

and mutual information is I(f(X);Y)=H(f(X))+H(Y)−H(f(X),Y)I(f(X); Y) = H(f(X)) + H(Y) - H(f(X), Y)I(f(X);Y)=H(f(X))+H(Y)−H(f(X),Y), all entropies in bits. No measure theory is required, and the endpoints p∈{0,1/2,1}p \in \{0, 1/2, 1\}p∈{0,1/2,1} are included by the conventions 0log⁡0=00 \log 0 = 00log0=0 and log⁡0=0\log 0 = 0log0=0.

Formalization targets

Goal — the general inequality

∀ n∈N, ∀f:{0,1}n→{0,1}, ∀p∈[0,1]:I(f(X);Y)  ≤  1−H(p).\forall\, n \in \mathbb{N},\ \forall f : \{0,1\}^n \to \{0,1\},\ \forall p \in [0,1]: \qquad I\bigl(f(X); Y\bigr) \;\le\; 1 - H(p).∀n∈N, ∀f:{0,1}n→{0,1}, ∀p∈[0,1]:I(f(X);Y)≤1−H(p).

The goal quantifies over every dimension, including n=0n = 0n=0, every Boolean function — balanced or not, monotone or not — and every crossover probability including the three endpoints. Nothing is assumed about fff: no balance condition, no bound on the number of influential coordinates, no restriction to a range of ppp. The bound is tight, attained by any dictator, so the statement is exactly the assertion that dictators are the most informative Boolean functions.

Why the bound matters

The inequality is the sharp, one-bit case of a general question in information theory: how much can a lossy summary of a source tell you about a noisy observation of that source? It is the Boolean-function analogue of a hypercontractivity or "small-set expansion" statement — quantities of the form I(f(X);Y)I(f(X); Y)I(f(X);Y) under a noise operator are precisely what appear in the analysis of Boolean functions, in hardness-of-approximation reductions built on noise stability, and in distributed source-coding and common-information problems, where the bound limits what a single bit of a compressed description can carry. Special cases were known and repeatedly used: balanced functions, functions of few coordinates, and asymptotic or high-noise regimes. The general statement resisted those methods, because the extremal structure is a single coordinate while the space of competitors grows doubly exponentially in nnn.

Why it is hard

Mutual information is neither convex nor concave in fff, and the obvious relaxations are false: the corresponding bound for real-valued or non-Boolean summaries fails, so any argument must use Booleanness. Fourier-analytic approaches control noise stability but lose the constant needed for tightness, and the tightness is the whole content — the inequality is an equality for dictators, leaving no slack to absorb approximation. Induction on nnn requires a statement strong enough to survive restriction, and the known strengthenings become false at the endpoints. The regimes also split: near p=1/2p = 1/2p=1/2 the problem becomes a perturbative curvature computation around the dictator, while for moderate ppp the extremal analysis is a global optimization over a two-parameter family, and the two arguments meet only if their boundaries are matched exactly.

Formalization scope

The goal is stated with the entropy and mutual-information definitions of this mission's definition module: binary entropy via Mathlib's Real.binEntropy divided by log⁡2\log 2log2 (so entropies are in bits), the channel as an explicit product kernel, and the joint and marginal masses as explicit finite sums over the cube. The proposition is a single closed statement — no hypotheses beyond 0≤p≤10 \le p \le 10≤p≤1 — so a solution must establish it for all dimensions uniformly.

A complete machine-checked proof of this statement exists in Lean 4 (Chen–Gohari–Javanmard–Lin–Mirrokni–Nair–Woodruff, 2026): axioms {\{{propext, Classical.choice, Quot.sound}\}}, no sorry and no native_decide, but 45,500 modules and roughly 50 million lines, most of it kernel-checked numerical certificate data. It is therefore not submittable as a single solution, and the mission's supporting structure — the manuscript route's regional statements and its leaf certificate families — will be added as separate theorems as they are transplanted onto the platform.

Selected references

  • T. A. Courtade, G. R. Kumar. Which Boolean functions maximize mutual information on noisy inputs? IEEE Transactions on Information Theory 60(8):4515–4525, 2014. (The conjecture.)
  • Z. Chen, A. Gohari, A. Javanmard, H. Lin, V. Mirrokni, C. Nair, D. P. Woodruff. A Proof of the Most Informative Boolean Function Conjecture. arXiv:2609.24931, 2026.
  • Lean 4 formalization of the above: https://github.com/dpwoodru/general-courtade-kumar-lean
  • R. O'Donnell. Analysis of Boolean Functions. Cambridge University Press, 2014, Chapters 2 and 9 (noise operators, hypercontractivity).
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Mathematical Physics·Captain: Lucas

The International System of Units (SI Brochure, 9th ed.) I: base units from the seven defining constantsTextbook

Motivation

Since 20 May 2019 the International System of Units (SI) is no longer defined through material artefacts or particular experiments. Instead, the 26th General Conference on Weights and Measures fixed the exact numerical values of seven defining constants and declared that the SI is the system of units in which these constants take these values. The reference text is the BIPM's SI Brochure, 9th edition (2019), bipm.org. Every calibration certificate, every value in the CODATA tables and every textbook formula expressed in SI units rests on this definition.

The mathematical content of the new definition is small but exact: from the seven fixed values, the Brochure derives, for each of the seven base units, an explicit formula expressing that unit as a rational multiple of a product of integer powers of the defining constants (Section 2.3.1), and it asserts that any SI unit can be written through products and quotients of the defining constants (Section 2.2). These are statements about a free abelian group of unit monomials together with exact rational coefficients, so they can be checked completely.

Timeline. 1960: the 11th CGPM establishes the SI with six base units (the mole is added in 1971). 1983: the metre is redefined by fixing the speed of light ccc. 2018–2019: the 26th CGPM (Resolution 1) redefines the kilogram, ampere, kelvin and mole by fixing hhh, eee, kkk and NAN_ANA​; the new definitions enter into force on 20 May 2019 and are published in the 9th edition of the SI Brochure.

Setting

A quantity value is written as a number times a unit. In this mission a quantity value is a pair (x,u)(x, u)(x,u), written x ux\,uxu, where x∈Rx\in\mathbb Rx∈R is the numerical value and

u=sa1 ma2 kga3 Aa4 Ka5 mola6 cda7,ai∈Z,u = \mathrm{s}^{a_1}\,\mathrm{m}^{a_2}\,\mathrm{kg}^{a_3}\,\mathrm{A}^{a_4}\,\mathrm{K}^{a_5}\,\mathrm{mol}^{a_6}\,\mathrm{cd}^{a_7},\qquad a_i\in\mathbb Z,u=sa1​ma2​kga3​Aa4​Ka5​mola6​cda7​,ai​∈Z,

is a unit monomial in the seven base units second, metre, kilogram, ampere, kelvin, mole and candela (Table 2 of the Brochure). Products multiply numerical values and add exponents; quotients and integer powers are defined accordingly; a real number rrr acts by r⋅(x u)=(rx) ur\cdot(x\,u) = (rx)\,ur⋅(xu)=(rx)u. Two quantity values are equal exactly when they have the same numerical value and the same seven exponents.

The derived units needed in Section 2.2 are Hz=s−1\mathrm{Hz}=\mathrm s^{-1}Hz=s−1, J=kg m2 s−2\mathrm J=\mathrm{kg\,m^2\,s^{-2}}J=kgm2s−2, C=A s\mathrm C=\mathrm{A\,s}C=As, W=kg m2 s−3\mathrm W=\mathrm{kg\,m^2\,s^{-3}}W=kgm2s−3, sr=m2 m−2\mathrm{sr}=\mathrm{m^2\,m^{-2}}sr=m2m−2 and lm=cd sr\mathrm{lm}=\mathrm{cd\,sr}lm=cdsr. The seven defining constants (Section 2.2, Table 1) are

ΔνCs=9 192 631 770 Hz,c=299 792 458 m s−1,h=6.626 070 15×10−34 J s,\Delta\nu_{\mathrm{Cs}} = 9\,192\,631\,770\ \mathrm{Hz},\quad c = 299\,792\,458\ \mathrm{m\,s^{-1}},\quad h = 6.626\,070\,15\times10^{-34}\ \mathrm{J\,s},ΔνCs​=9192631770 Hz,c=299792458 ms−1,h=6.62607015×10−34 Js, e=1.602 176 634×10−19 C,k=1.380 649×10−23 J K−1,NA=6.022 140 76×1023 mol−1,Kcd=683 lm W−1.e = 1.602\,176\,634\times10^{-19}\ \mathrm C,\quad k = 1.380\,649\times10^{-23}\ \mathrm{J\,K^{-1}},\quad N_A = 6.022\,140\,76\times10^{23}\ \mathrm{mol^{-1}},\quad K_{\mathrm{cd}} = 683\ \mathrm{lm\,W^{-1}}.e=1.602176634×10−19 C,k=1.380649×10−23 JK−1,NA​=6.02214076×1023 mol−1,Kcd​=683 lmW−1.

Formalization targets

Goal (Section 2.2, p. 127)

"The seven constants are chosen in such a way that any unit of the SI can be written either through a defining constant itself or through products or quotients of defining constants." Formally: for every exponent vector u∈Z7u\in\mathbb Z^7u∈Z7 there are a real number aaa and integers n1,…,n7n_1,\dots,n_7n1​,…,n7​ with

su1⋯cdu7  =  a⋅ΔνCs n1 c n2 h n3 e n4 k n5 NA n6 Kcd n7.\mathrm{s}^{u_1}\cdots\mathrm{cd}^{u_7} \;=\; a\cdot \Delta\nu_{\mathrm{Cs}}^{\,n_1}\, c^{\,n_2}\, h^{\,n_3}\, e^{\,n_4}\, k^{\,n_5}\, N_A^{\,n_6}\, K_{\mathrm{cd}}^{\,n_7}.su1​⋯cdu7​=a⋅ΔνCsn1​​cn2​hn3​en4​kn5​NAn6​​Kcdn7​​.

Milestones (Section 2.3.1, pp. 130–135)

The seven exact expressions of the base units in terms of the defining constants, each in both forms displayed by the Brochure:

1 s=9 192 631 770ΔνCs,1 m=9 192 631 770299 792 458 cΔνCs,1 kg=(299 792 458)2(6.626 070 15×10−34)(9 192 631 770) h ΔνCsc2,1\ \mathrm s = \frac{9\,192\,631\,770}{\Delta\nu_{\mathrm{Cs}}},\qquad 1\ \mathrm m = \frac{9\,192\,631\,770}{299\,792\,458}\,\frac{c}{\Delta\nu_{\mathrm{Cs}}},\qquad 1\ \mathrm{kg} = \frac{(299\,792\,458)^2}{(6.626\,070\,15\times10^{-34})(9\,192\,631\,770)}\,\frac{h\,\Delta\nu_{\mathrm{Cs}}}{c^2},1 s=ΔνCs​9192631770​,1 m=2997924589192631770​ΔνCs​c​,1 kg=(6.62607015×10−34)(9192631770)(299792458)2​c2hΔνCs​​, 1 A=ΔνCs e(9 192 631 770)(1.602 176 634×10−19),1 K=1.380 649×10−23(6.626 070 15×10−34)(9 192 631 770) ΔνCs hk,1\ \mathrm A = \frac{\Delta\nu_{\mathrm{Cs}}\,e}{(9\,192\,631\,770)(1.602\,176\,634\times10^{-19})},\quad 1\ \mathrm K = \frac{1.380\,649\times10^{-23}}{(6.626\,070\,15\times10^{-34})(9\,192\,631\,770)}\,\frac{\Delta\nu_{\mathrm{Cs}}\,h}{k},1 A=(9192631770)(1.602176634×10−19)ΔνCs​e​,1 K=(6.62607015×10−34)(9192631770)1.380649×10−23​kΔνCs​h​, 1 mol=6.022 140 76×1023NA,1 cd=(ΔνCs)2 h Kcd(6.626 070 15×10−34)(9 192 631 770)2 683,1\ \mathrm{mol} = \frac{6.022\,140\,76\times10^{23}}{N_A},\qquad 1\ \mathrm{cd} = \frac{(\Delta\nu_{\mathrm{Cs}})^2\,h\,K_{\mathrm{cd}}}{(6.626\,070\,15\times10^{-34})(9\,192\,631\,770)^2\,683},1 mol=NA​6.02214076×1023​,1 cd=(6.62607015×10−34)(9192631770)2683(ΔνCs​)2hKcd​​,

together with the rounded decimal values quoted for the five non-trivial numerical factors (≈30.663 319\approx 30.663\,319≈30.663319, 1.475 5214×10401.475\,5214\times10^{40}1.4755214×1040, 6.789 687×1086.789\,687\times10^{8}6.789687×108, 2.266 66532.266\,66532.2666653, 2.614 830×10102.614\,830\times10^{10}2.614830×1010).

Significance

The result itself. The milestones are the operational content of the 2019 redefinition: they say how each base unit is recovered from the fixed constants, and together they show that the matrix of exponents of the seven defining constants with respect to the seven base units is invertible over Z\mathbb ZZ, which is exactly what the goal asserts. Every derived unit is a monomial in base units, so the goal also covers the derived units.

Formalizing it. The platform already has purely numerical checks of these formulas (rational identities of the form "coefficient ×\times× constant values =1=1=1"). This mission adds a model with units as first-class data: equalities are between quantity values, so a wrong exponent or a missing factor of c2c^2c2 is a type-level failure, not a silent numerical coincidence. The definition file is reusable for later missions in this series (derived units, Tables 4–8, prefixes).

Difficulty

The individual milestones are exact finite computations; the only care needed is bookkeeping of exponents and of large decimal constants. The goal requires choosing the integer exponents nin_ini​ as functions of uuu and showing that the unit monomials match componentwise — an argument that the exponent matrix is unimodular, not merely invertible over Q\mathbb QQ. Solving the system over the rationals is not enough.

Formalization scope

  • Numerical values are real numbers; exponents are integers; base units form a seven-element type. Equality of quantity values is equality of the numerical value and of all seven exponents.
  • The steradian is modelled as m2 m−2\mathrm m^2\,\mathrm m^{-2}m2m−2, i.e. the unit of dimension one, as in the Brochure (Table 4); consequently lm=cd\mathrm{lm} = \mathrm{cd}lm=cd in this model.
  • Real division and inversion follow Mathlib's conventions (0−1=00^{-1}=00−1=0); all constants used here are non-zero, so this convention never enters the milestones.
  • The goal allows an arbitrary real coefficient aaa; since unit monomials have numerical value 111, aaa is forced to be non-zero, so the statement cannot be satisfied trivially.
  • Out of scope: the physical realization of units (Section 2.3.2 onward), uncertainties, and the definitions of the non-coherent and non-SI units.

Selected references

  • BIPM, The International System of Units (SI), 9th edition, 2019. ISBN 978-92-822-2272-0. https://www.bipm.org/en/publications/si-brochure
  • CGPM, Resolution 1 of the 26th meeting (2018), On the revision of the International System of Units (SI). https://www.bipm.org/en/committees/cg/cgpm/26-2018/resolution-1
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Mathematical PhysicsQuantum Information·Captain: Lucas

Decoherence in Two-Flavour Neutrino Oscillations (Alves 2020)Research Paper

Motivation

Neutrino oscillations are an interference phenomenon, so they are sensitive to any mechanism that degrades quantum coherence during propagation. The open quantum system description models such effects without specifying their microscopic origin: the neutrino is treated as a subsystem whose reduced density matrix evolves under a Markovian master equation. The dissertation of G. F. S. Alves (Instituto de Física, Universidade de São Paulo, 2020) develops this framework for two and three neutrino generations and uses public IceCube atmospheric data to constrain the new parameters. Its two-generation chapter derives closed-form oscillation probabilities under several choices of the dissipative term; this mission formalizes that chapter's mathematical content.

Setting

A density matrix is a positive semidefinite complex matrix of unit trace. For a two-level system (two neutrino mass eigenstates) the reduced state ρ(t)∈C2×2\rho(t)\in\mathbb C^{2\times2}ρ(t)∈C2×2 obeys the Lindblad equation with constant coefficients,

ρ˙=−i[H,ρ]+D[ρ],D[ρ]=12∑i,j=13aij(2σiρσj−{σjσi,ρ}),\dot\rho=-i[H,\rho]+D[\rho],\qquad D[\rho]=\tfrac12\sum_{i,j=1}^3 a_{ij}\bigl(2\sigma_i\rho\sigma_j-\{\sigma_j\sigma_i,\rho\}\bigr),ρ˙​=−i[H,ρ]+D[ρ],D[ρ]=21​i,j=1∑3​aij​(2σi​ρσj​−{σj​σi​,ρ}),

where σ1,σ2,σ3\sigma_1,\sigma_2,\sigma_3σ1​,σ2​,σ3​ are the Pauli matrices and the 3×33\times33×3 Kossakowski matrix a=(aij)a=(a_{ij})a=(aij​) is Hermitian positive semidefinite (the condition for complete positivity). In the mass basis the vacuum Hamiltonian is H=diag⁡(0,Δm2/2E)H=\operatorname{diag}(0,\Delta m^2/2E)H=diag(0,Δm2/2E), and the mixing matrix with Majorana phase α\alphaα is

U=(cos⁡θeiαsin⁡θ−e−iαsin⁡θcos⁡θ).U=\begin{pmatrix}\cos\theta&e^{i\alpha}\sin\theta\\-e^{-i\alpha}\sin\theta&\cos\theta\end{pmatrix}.U=(cosθ−e−iαsinθ​eiαsinθcosθ​).

The muon neutrino is produced in the state ρμ(0)=U†∣ν1⟩⟨ν1∣U\rho_\mu(0)=U^\dagger|\nu_1\rangle\langle\nu_1|Uρμ​(0)=U†∣ν1​⟩⟨ν1​∣U, and the survival probability after a baseline LLL is Pνμ→νμ=Tr⁡{ρ(L)ρμ(0)}P_{\nu_\mu\to\nu_\mu}=\operatorname{Tr}\{\rho(L)\rho_\mu(0)\}Pνμ​→νμ​​=Tr{ρ(L)ρμ​(0)}. The linear entropy Sl(ρ)=1−Tr⁡ρ2S_l(\rho)=1-\operatorname{Tr}\rho^2Sl​(ρ)=1−Trρ2 and the von Neumann entropy S(ρ)=−Tr⁡ρln⁡ρS(\rho)=-\operatorname{Tr}\rho\ln\rhoS(ρ)=−Trρlnρ measure the loss of purity.

Formalization targets

Goal: decoherent survival probability, eq. (3.24)

For the pure-decoherence Kossakowski matrix a=diag⁡(0,0,γ)a=\operatorname{diag}(0,0,\gamma)a=diag(0,0,γ), γ≥0\gamma\ge0γ≥0, every solution with ρ(0)=ρμ(0)\rho(0)=\rho_\mu(0)ρ(0)=ρμ​(0) satisfies, for all L≥0L\ge0L≥0,

Pνμ→νμ=14(3+cos⁡4θ+2e−2γLcos⁡(Δm22EL)sin⁡22θ).P_{\nu_\mu\to\nu_\mu}=\frac14\Bigl(3+\cos4\theta+2e^{-2\gamma L}\cos\Bigl(\frac{\Delta m^2}{2E}L\Bigr)\sin^22\theta\Bigr).Pνμ​→νμ​​=41​(3+cos4θ+2e−2γLcos(2EΔm2​L)sin22θ).

Milestones

  1. Range of the linear entropy, eq. (2.45), and of the von Neumann entropy, eqs. (2.40)–(2.41).
  2. Non-negativity of the relative entropy, eq. (2.43).
  3. Entropy increase whenever the maximally mixed state is a fixed point of DDD (Appendix B.1, two-level case).
  4. Pauli-basis form of the Dissipator, eq. (3.5).
  5. Average-energy conservation holds iff a=diag⁡(0,0,γ)a=\operatorname{diag}(0,0,\gamma)a=diag(0,0,γ), eqs. (3.19)–(3.22).
  6. The evolved state in case (1), eq. (3.23), and the population in case (4), eq. (3.26).

Significance

The goal is the formula used in the dissertation to show how decoherence damps oscillations: it reduces to the standard vacuum formula at γ=0\gamma=0γ=0, it tends to 14(3+cos⁡4θ)\tfrac14(3+\cos4\theta)41​(3+cos4θ) at large LLL instead of oscillating, and it does not depend on α\alphaα. The milestones connect the formula to the structure of the Lindblad generator (energy conservation singles out this Dissipator) and to entropy growth. A formal development yields a checked two-level Lindblad toolkit (Pauli expansion of dissipators, explicit solutions, entropy bounds) reusable in other open-system missions. The results are proved informally in the source; none is known to be machine-checked.

Difficulty

The ODE part requires a uniqueness argument for a linear matrix ODE on [0,∞)[0,\infty)[0,∞) given only one-sided derivatives at t=0t=0t=0, plus exact trigonometric bookkeeping. The entropy milestones need spectral calculus for Hermitian matrices (Klein's inequality, concavity of −xln⁡x-x\ln x−xlnx) and, for Appendix B.1, the monotonicity of relative entropy under completely positive trace-preserving maps together with complete positivity of Lindblad semigroups, neither of which is expected to be available off the shelf.

Formalization scope

Matrices are Matrix (Fin 2) (Fin 2) ℂ; the Kossakowski matrix is Matrix (Fin 3) (Fin 3) ℂ with indices 0,1,20,1,20,1,2 for the thesis' 1,2,31,2,31,2,3. Solutions are curves R→C2×2\mathbb R\to\mathbb C^{2\times2}R→C2×2 satisfying the Lindblad equation entrywise for t≥0t\ge0t≥0 (derivatives within [0,∞)[0,\infty)[0,∞)); the exponential eLte^{\mathcal Lt}eLt is not used. Entropies use the continuous functional calculus. Two printed formulas are corrected in the drafts: the sign of the ρ0 Im(aij)\rho_0\,\mathrm{Im}(a_{ij})ρ0​Im(aij​) terms in eq. (3.5), and the overall sign of the off-diagonal entries in eq. (3.23); both corrections are explained in the corresponding items. The two-generation cases (4) and (5) survival probabilities, eqs. (3.25) and (3.27), and the three-generation and IceCube analyses are out of scope.

Selected references

  • G. F. S. Alves, Decoherence in Neutrino Oscillations in the IceCube Experiment, MSc dissertation, Instituto de Física, Universidade de São Paulo, 2020.
  • G. Lindblad, On the generators of quantum dynamical semigroups, Commun. Math. Phys. 48 (1976) 119–130, https://doi.org/10.1007/BF01608499
  • V. Gorini, A. Kossakowski, E. C. G. Sudarshan, Completely positive dynamical semigroups of N-level systems, J. Math. Phys. 17 (1976) 821–825, https://doi.org/10.1063/1.522979
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CombinatoricsMathematical Physics·Captain: ShapeZero

The role postulates force exactly seven pointsTextbook

Motivation

The Shape Zero model (Shape Zero LLC, unpublished) reaches the Fano plane — the seven-point, seven-line configuration behind the seven imaginary units of the octonions — by a combinatorial route (C1 Formal Proofs, §3). Points are arranged in Steiner triple systems, and each point of each line is given one of three roles. The model's claim is that the role postulates alone force the number of points to be exactly seven. This mission proves that claim.

What this mission does NOT prove.

  • Not that the system is the Fano plane. It proves the point count is 777. That every Steiner triple system on 777 points is the Fano plane up to relabelling is a classical result, but it is not formalized here.
  • Not the modelling premise. Why lines have three points, and why there are three roles, is an input of the model, not derived here.
  • Not the later steps from the Fano plane to the octonions, and from there to the node size n=3n = 3n=3 and u(3)\mathfrak{u}(3)u(3).

Two corrections to C1 §3 built into this mission.

  • At least one point is required. The empty system — no points, no lines — satisfies every condition vacuously and has 000 points, so C1 Theorem 3.6 as stated is false for it. The goal carries the hypothesis 0<n0 < n0<n. This is proved (in Lean, locally): the empty system is a Steiner triple system with a role colouring, so the statement without 0<n0 < n0<n is false.
  • C1 Theorem 3.3(a) is not used. Its condition "any two lines meet" does not force 777 points: it also holds for a single triple (333 points) and a single point, where there is no pair of lines to fail. This mission uses the role postulates instead.

Setting

Fix a natural number nnn and take the points {0,…,n−1}\{0, \dots, n-1\}{0,…,n−1}. A Steiner triple system is a family of subsets, called lines, such that

  1. every line has exactly 333 points, and
  2. every pair of distinct points lies on exactly one line.

A role colouring assigns to each point xxx and line ℓ\ellℓ a role ρ(x,ℓ)∈{0,1,2}\rho(x, \ell) \in \{0, 1, 2\}ρ(x,ℓ)∈{0,1,2} such that

  1. the three points of a line get three different roles;
  2. completeness: every point takes every role at least once, on some line through it;
  3. minimality: every point takes every role at most once — two different lines through xxx give xxx different roles.

In Lean these are RolesForceSeven.STS n and RolesForceSeven.RoleColouring S role, with points Fin n and lines Finset (Fin n).

Formalization targets

Goal: the role postulates force exactly seven points

n≥1, a Steiner triple system on n points with a role colouring  ⟹  n=7.n \ge 1,\ \text{a Steiner triple system on } n \text{ points with a role colouring} \;\Longrightarrow\; n = 7 .n≥1, a Steiner triple system on n points with a role colouring⟹n=7.

This is RolesForceSeven.roles_force_seven. It asserts the point count only.

Milestones

  1. M1 (replication count). In any Steiner triple system, every point lies on exactly rrr lines with 2r+1=n2r + 1 = n2r+1=n.
  2. M2 (three lines per point). Under a role colouring, every point lies on exactly 333 lines.

Corollaries

  • A — the Fano plane has a role colouring. The Fano plane on {0,…,6}\{0, \dots, 6\}{0,…,6}, with lines {i,i+1,i+3}\{i, i+1, i+3\}{i,i+1,i+3} modulo 777, admits a role colouring. Without this the goal could be vacuously true.
  • B — AG(2, 3) is excluded (C1 Corollary 3.7): no Steiner triple system on 999 points has a role colouring.

Significance

The result itself. It turns the model's role postulates into a precise count: whatever the Steiner triple system, if it carries a role colouring and has a point, it has exactly seven points. Corollary A shows the conditions are satisfiable, and Corollary B rules out the next Steiner triple system, AG(2, 3), explicitly.

Formalizing it. The C1 statement omits the non-emptiness hypothesis and is false for the empty system; the formal statement makes the hypothesis explicit and shows it is needed. The numerical check (Fano plane: 484848 role colourings; AG(2, 3): 000; single triple: 000) is replaced by a proof for every nnn.

Numerical cross-check

systempointslines through each pointrole colourings
Fano plane7348
AG(2, 3)940
single triple310
empty system0—vacuous (all conditions hold)

Difficulty

Moderate. The central step is the replication count: the lines through a point xxx must be shown to cover every other point exactly once, two at a time, which is a double-counting argument over the pairs through xxx. The role postulates then fix the replication number at three. The Fano plane corollary is a finite check.

Formalization scope

  • Points are Fin n; lines are finite sets of points, with no ambient geometry assumed.
  • The role function is total, Fin n → Finset (Fin n) → Fin 3; only its values on pairs x∈ℓx \in \ellx∈ℓ with ℓ\ellℓ a line matter.
  • Completeness and minimality are both hypotheses; the goal uses both.
  • 0<n0 < n0<n is necessary: without it the empty system is a counterexample (proved).
  • The conclusion is the number 777, not an isomorphism with the Fano plane.

Selected references

  • Wikipedia, Steiner system (Steiner triple systems, replication number). https://en.wikipedia.org/wiki/Steiner_system
  • Wikipedia, Fano plane. https://en.wikipedia.org/wiki/Fano_plane
  • Wikipedia, Octonion (Fano plane mnemonic for the multiplication of imaginary units). https://en.wikipedia.org/wiki/Octonion
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CombinatoricsMachine LearningProbability·Captain: naimengye

Understanding Machine Learning XXIV: Compression BoundsTextbook

Motivation

The book has characterized learnability through uniform convergence and through stability; Chapter 30 of Shalev-Shwartz and Ben-David, Understanding Machine Learning: From Theory to Algorithms (doi:10.1017/CBO9781107298019), gives a third sufficient condition, compression: if a learning algorithm's output can be reconstructed from a small subsequence of kkk training examples, then the error on the remaining examples estimates the true error, and the algorithm generalizes with a bound of order klog⁡(m/δ)/mk\log(m/\delta)/mklog(m/δ)/m (Theorem 30.2, Littlestone and Warmuth). The bound is a union bound over the mkm^kmk possible index sequences of a held-out estimate that follows from Bernstein's inequality (Lemma 30.1), and in the consistent case it gives LD≤8klog⁡(m/δ)/mL_D \le 8k\log(m/\delta)/mLD​≤8klog(m/δ)/m (Corollary 30.3). Classes admitting such compression schemes include axis-aligned rectangles (k=2dk = 2dk=2d), homogeneous halfspaces (k=dk = dk=d, through the minimal-norm point of the convex hull and Carathéodory's theorem), separating polynomials by reduction, and any margin-separable data (k≤1/γ2k \le 1/\gamma^2k≤1/γ2, through the Perceptron). Whether every class of finite VC dimension has a compression scheme of size O(d)O(d)O(d) is Warmuth's problem, open when the book was written.

Setting

A sample S=(z1,…,zm)S = (z_1, \dots, z_m)S=(z1​,…,zm​) is drawn i.i.d. from DDD; a selection rule picks (i1,…,ik)∈[m]k(i_1, \dots, i_k) \in [m]^k(i1​,…,ik​)∈[m]k (repetitions allowed), a reconstruction map B:Zk→HB : Z^k \to HB:Zk→H produces A(S)=B(zi1,…,zik)A(S) = B(z_{i_1}, \dots, z_{i_k})A(S)=B(zi1​​,…,zik​​), and VVV is the set of positions not selected, with LVL_VLV​ the average loss over them. The loss takes values in [0,1][0,1][0,1]. A class HHH has a compression scheme of size kkk (Definition 30.4) if for every m≥1m \ge 1m≥1 there are such AAA and BBB with B(SA(S))B(S_{A(S)})B(SA(S)​) correct on every sample labeled by a member of HHH; the unrealizable version (Definition 30.5) asks B(SA(S))B(S_{A(S)})B(SA(S)​) to be an empirical risk minimizer on every sample.

Formalization targets

Goal: Theorem 30.2

For a [0,1][0,1][0,1]-valued loss, k≥1k \ge 1k≥1, m≥2km \ge 2km≥2k, any reconstruction map BBB and any selection rule, with probability at least 1−δ1 - \delta1−δ over S∼DmS \sim D^mS∼Dm,

LD(A(S))≤LV(A(S))+LV(A(S)) 4klog⁡(m/δ)m+8klog⁡(m/δ)m.L_D(A(S)) \le L_V(A(S)) + \sqrt{L_V(A(S))\,\frac{4k\log(m/\delta)}{m}} + \frac{8k\log(m/\delta)}{m}.LD​(A(S))≤LV​(A(S))+LV​(A(S))m4klog(m/δ)​​+m8klog(m/δ)​.

Milestones

Lemma 30.1 (the held-out Bernstein bound); Corollary 30.3 (the consistent case); Lemma 30.6 (realizable schemes give unrealizable schemes); the compression scheme of size 2d2d2d for axis-aligned rectangles (§30.2.1); the separation property of the minimal-norm point of the convex hull (§30.2.2). Further items: the size-ddd scheme for homogeneous halfspaces and the margin scheme of §30.2.4.

Significance

Compression bounds are the cleanest generalization argument in the book: no complexity measure of the class enters, only the number of examples needed to encode the output, and the resulting bound is data-dependent through LVL_VLV​. They explain why support vector machines and the Perceptron generalize in terms of the number of support vectors or updates, and they underlie the sample-compression view of learning that connects to Chapters 9 and 15. Lemma 30.6 shows that compression is robust to label noise in the binary case. The halfspace scheme is a small piece of convex geometry of independent interest, and Warmuth's question about VC classes, settled in the affirmative for finite size by Moran and Yehudayoff after the book appeared, remains open in the form O(d)O(d)O(d).

Difficulty

Lemma 30.1 is Bernstein's inequality for the nnn held-out losses with variance at most LD(hT)L_D(h_T)LD​(hT​), followed by solving the resulting quadratic in LD\sqrt{L_D}LD​​ to move the risk from the right-hand side to LVL_VLV​; the constant 444 comes out of that step (the exact value is about 3.193.193.19). Theorem 30.2 is a union bound over the mkm^kmk index sequences with δ′=mkδ\delta' = m^k\deltaδ′=mkδ, using ∣V∣≥m−k≥m/2|V| \ge m - k \ge m/2∣V∣≥m−k≥m/2 and log⁡(mk/δ′)≤klog⁡(m/δ′)\log(m^k/\delta') \le k\log(m/\delta')log(mk/δ′)≤klog(m/δ′), which needs k≥1k \ge 1k≥1; formally the event for the learner is contained in the union of the events of Lemma 30.1 for each fixed index sequence, so no measurability of the selection rule is needed. Corollary 30.3 is immediate. Lemma 30.6 applies the realizable scheme to the subsample on which an ERM hypothesis is correct. The rectangle scheme is bookkeeping about extremal coordinates. The halfspace scheme needs three facts: the minimal-norm point of the hull separates (a one-line perturbation argument), it lies on a face and hence is a convex combination of ddd sample points (Carathéodory's theorem, in Mathlib, applied to a face), and it is the minimal-norm point of the hull of those ddd points (uniqueness of the projection onto a convex set); the existence of the minimizer uses compactness of the hull. The margin scheme is the Perceptron convergence theorem of Mission VI applied to the batch algorithm, whose output is the sum of the updated examples.

Formalization scope

Samples are Fin m-indexed under Mission I's iidLaw, and probability statements bound the outer measure of the failure event. Lemma 30.1 splits a sample of size k+nk + nk+n into its first kkk and last nnn entries; Theorem 30.2 takes an arbitrary selection rule sel:Zm→[m]k\mathrm{sel} : Z^m \to [m]^ksel:Zm→[m]k and reconstruction map BBB, the held-out set being the positions not in the range of the selection, and requires k≥1k \ge 1k≥1 and m≥1m \ge 1m≥1 in addition to the book's m≥2km \ge 2km≥2k: for k=0k = 0k=0 the bound reads LD≤LVL_D \le L_VLD​≤LV​, which fails, and the book's derivation uses k≥1k \ge 1k≥1 in log⁡(mk/δ′)≤klog⁡(m/δ′)\log(m^k/\delta') \le k\log(m/\delta')log(mk/δ′)≤klog(m/δ′). Compression schemes are defined for every m≥1m \ge 1m≥1, since for m=0m = 0m=0 there is no index to select, with indices allowed to repeat as in [m]k[m]^k[m]k and with BBB's outputs in HHH; the unrealizable version uses Mission XXIII's multiclass 0–1 loss. The halfspace results are stated for strictly separable ±1\pm1±1-labeled samples, yi⟨w⋆,xi⟩>0y_i\langle w^\star, x_i\rangle > 0yi​⟨w⋆,xi​⟩>0, the book's "w.l.o.g. all labels positive" normalization; this avoids the boundary negatives that a realizable sample may contain under the sign⁡(0)\operatorname{sign}(0)sign(0) convention of Mission VI, and it is the setting in which the minimal-norm argument works. The scheme is stated as the existence of ddd indices whose signed examples have a minimal-norm hull point separating the whole sample, which is the content of AAA and BBB without fixing how ties among faces are broken. Rectangles are closed boxes. The margin scheme uses Theorem 9.1's normalization.

Not stated: §30.2.3 (polynomials, a reduction), the bibliographic remarks, and the intermediate Carathéodory step as a separate item.

Selected references

  • S. Shalev-Shwartz, S. Ben-David, Understanding Machine Learning: From Theory to Algorithms, Cambridge University Press, 2014, Chapter 30. doi:10.1017/CBO9781107298019
  • N. Littlestone, M. K. Warmuth, Relating data compression and learnability, technical report, University of California, Santa Cruz, 1986.
  • S. Floyd, M. K. Warmuth, Sample compression, learnability, and the Vapnik-Chervonenkis dimension, Machine Learning 21, 1995. doi:10.1007/BF00993593
  • S. Ben-David, A. Litman, Combinatorial variability of Vapnik-Chervonenkis classes with applications to sample compression schemes, Discrete Applied Mathematics 86, 1998. doi:10.1016/S0166-218X(98)00000-6
  • S. Moran, A. Yehudayoff, Sample compression schemes for VC classes, Journal of the ACM 63(3), 2016. doi:10.1145/2890490
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CombinatoricsMachine LearningProbability·Captain: naimengye

Understanding Machine Learning XXIII: Multiclass LearnabilityTextbook

Motivation

Chapter 17 introduced multiclass prediction; Chapter 29 of Shalev-Shwartz and Ben-David, Understanding Machine Learning: From Theory to Algorithms (doi:10.1017/CBO9781107298019), asks the two questions the fundamental theorem answered for binary classes: which classes of multiclass predictors are PAC learnable with respect to the 0–1 loss, and with what sample complexity. Natarajan's dimension generalizes the VC dimension by shattering with two disagreeing label functions, and the multiclass fundamental theorem (Theorem 29.3) bounds the uniform-convergence, agnostic and realizable sample complexities in terms of it, up to logarithmic factors in the number of labels kkk; the only new ingredient in its proof is Natarajan's lemma, the multiclass substitute for Sauer's lemma. The chapter then computes or bounds the Natarajan dimension of the classes that matter, One-versus-All and general reductions to binary classifiers, and linear multiclass predictors (Theorem 29.7). Its last section is a warning: unlike the binary case, not all ERMs are equal, and with infinitely many labels a class can be learnable by one ERM and not by another, so learnability and uniform convergence come apart (Claim 29.9).

Setting

HHH is a class of functions from XXX to a finite label set YYY with ∣Y∣=k|Y| = k∣Y∣=k. C⊆XC \subseteq XC⊆X is shattered by HHH if there are f0,f1:C→Yf_0, f_1 : C \to Yf0​,f1​:C→Y with f0(x)≠f1(x)f_0(x) \ne f_1(x)f0​(x)=f1​(x) everywhere on CCC such that every B⊆CB \subseteq CB⊆C is realized by some h∈Hh \in Hh∈H agreeing with f0f_0f0​ on BBB and with f1f_1f1​ on C∖BC \setminus BC∖B (Definition 29.1); Ndim⁡(H)\operatorname{Ndim}(H)Ndim(H) is the largest size of a shattered set (Definition 29.2). One-versus-All builds T(hˉ)(x)=argmax⁡ihi(x)T(\bar h)(x) = \operatorname{argmax}_i h_i(x)T(hˉ)(x)=argmaxi​hi​(x) from kkk binary classifiers, the smaller label on ties; a general reduction applies a rule r:{0,1}l→[k]r : \{0,1\}^l \to [k]r:{0,1}l→[k] to lll binary classifiers; the linear class HΨH_\PsiHΨ​ predicts argmax⁡i⟨w,Ψ(x,i)⟩\operatorname{argmax}_i\langle w, \Psi(x, i)\rangleargmaxi​⟨w,Ψ(x,i)⟩ for a class-sensitive feature map Ψ:X×[k]→Rd\Psi : X \times [k] \to \mathbb{R}^dΨ:X×[k]→Rd (29.1). The class of §29.4 has labels Pf(X)∪{∗}P_f(X) \cup \{\ast\}Pf​(X)∪{∗}, the finite and cofinite subsets of XXX plus a special label, and hypotheses hA(x)=Ah_A(x) = AhA​(x)=A if x∈Ax \in Ax∈A and ∗\ast∗ otherwise; AgoodA_{good}Agood​ returns h∅h_\emptyseth∅​ on an all-∗\ast∗ sample and AbadA_{bad}Abad​ returns h{x1,…,xm}ch_{\{x_1, \dots, x_m\}^c}h{x1​,…,xm​}c​.

Formalization targets

Goal: Theorem 29.3

There are absolute constants C1,C2>0C_1, C_2 > 0C1​,C2​>0 such that every class H⊆YXH \subseteq Y^XH⊆YX with Ndim⁡(H)=d\operatorname{Ndim}(H) = dNdim(H)=d satisfies

C1d+log⁡(1/δ)ϵ2≤mHUC(ϵ,δ), mH(ϵ,δ)≤C2dlog⁡k+log⁡(1/δ)ϵ2,C1d+log⁡(1/δ)ϵ≤mHreal(ϵ,δ)≤C2dlog⁡(kd/ϵ)+log⁡(1/δ)ϵ,C_1\frac{d + \log(1/\delta)}{\epsilon^2} \le m^{UC}_H(\epsilon,\delta),\ m_H(\epsilon,\delta) \le C_2\frac{d\log k + \log(1/\delta)}{\epsilon^2}, \qquad C_1\frac{d + \log(1/\delta)}{\epsilon} \le m^{\mathrm{real}}_H(\epsilon,\delta) \le C_2\frac{d\log(kd/\epsilon) + \log(1/\delta)}{\epsilon},C1​ϵ2d+log(1/δ)​≤mHUC​(ϵ,δ), mH​(ϵ,δ)≤C2​ϵ2dlogk+log(1/δ)​,C1​ϵd+log(1/δ)​≤mHreal​(ϵ,δ)≤C2​ϵdlog(kd/ϵ)+log(1/δ)​,

the upper bounds by every ERM learner and the lower bounds for small ϵ,δ\epsilon, \deltaϵ,δ and d≥2d \ge 2d≥2, in the format of Mission IV's Theorem 6.8.

Milestones

Lemma 29.4 (Natarajan: ∣H∣≤∣X∣Ndim⁡(H)k2Ndim⁡(H)|H| \le |X|^{\operatorname{Ndim}(H)}k^{2\operatorname{Ndim}(H)}∣H∣≤∣X∣Ndim(H)k2Ndim(H)); Lemma 29.5 (the Natarajan dimension of One-versus-All is O(kdlog⁡(kd))O(kd\log(kd))O(kdlog(kd))); Theorem 29.7 (Ndim⁡(HΨ)≤d\operatorname{Ndim}(H_\Psi) \le dNdim(HΨ​)≤d); Claim 29.9(1) (AgoodA_{good}Agood​ needs 1ϵlog⁡1δ\frac1\epsilon\log\frac1\deltaϵ1​logδ1​ examples); Claim 29.9(2) (AbadA_{bad}Abad​ fails with constant probability on (∣X∣−1)/(6ϵ)(|X|-1)/(6\epsilon)(∣X∣−1)/(6ϵ) examples). Further items: the equality Ndim⁡=VCdim⁡\operatorname{Ndim} = \operatorname{VCdim}Ndim=VCdim for two classes, and Lemma 29.6 for general reductions.

Significance

Theorem 29.3 is the multiclass fundamental theorem of Natarajan (1989) and Ben-David, Cesa-Bianchi, Haussler and Long (1995): finite Natarajan dimension characterizes multiclass learnability, and the sample complexity is linear in it, with the dependence on kkk confined to logarithms. Natarajan's lemma is the combinatorial core, and the dimension bounds of §29.3 are what make the theorem usable: a One-versus-All scheme over a class of VC dimension ddd costs O~(kd)\tilde O(kd)O~(kd), and a linear multiclass predictor costs at most its number of parameters, so the multivector construction of Chapter 17 is learnable with O~(nk/ϵ2)\tilde O(nk/\epsilon^2)O~(nk/ϵ2) examples. Claim 29.9 is a genuine phenomenon of Daniely, Sabato, Ben-David and Shalev-Shwartz (2011): in multiclass classification the choice of ERM matters, and the equivalence "learnable iff uniform convergence" of the binary theory is false, which is why Conjecture 29.10 about good ERMs is open in the form the chapter states it.

Difficulty

The equality with the VC dimension for two labels is a direct comparison of the two shattering definitions. Natarajan's lemma is a Sauer-type induction on ∣X∣|X|∣X∣, in which a shattered set must be produced from two hypotheses that differ at a point; the exercise-level proof of the book becomes a careful double induction formally. Theorem 29.3's upper bounds follow the binary proof of Chapter 28 with Natarajan's lemma in place of Sauer's, hence Massart's lemma and Theorem 26.5 for the agnostic case and the double-sample argument for the realizable case; the lower bounds reduce to the binary ones by embedding a binary class into a multiclass one on a shattered set. These are long formal developments, and the theorem is stated with unspecified constants for that reason. Lemmas 29.5 and 29.6 are counting: a shattered CCC has 2∣C∣≤∣HC∣≤∣(Hbin)C∣k2^{|C|} \le |H_C| \le |(H_{bin})_C|^k2∣C∣≤∣HC​∣≤∣(Hbin​)C​∣k, Sauer's lemma bounds the right side by (∑i≤d(∣C∣i))k\big(\sum_{i \le d}\binom{|C|}{i}\big)^{k}(∑i≤d​(i∣C∣​))k, and the resulting inequality is solved. For Lemma 29.5's printed 3kdlog⁡(kd)3kd\log(kd)3kdlog(kd) this fails only at (k,d)=(2,1),(3,1)(k, d) = (2, 1), (3, 1)(k,d)=(2,1),(3,1). There a shattered set splits by the label pair {f0(x),f1(x)}\{f_0(x), f_1(x)\}{f0​(x),f1​(x)} into parts shattered by {B∖A:A,B∈Hbin}\{B \setminus A : A, B \in H_{bin}\}{B∖A:A,B∈Hbin​} (pairs {0,b}\{0, b\}{0,b}) or by HbinH_{bin}Hbin​ (other pairs). The first class has at most 313131 traces on 555 points. Theorem 29.7 maps a shattered set into Rd\mathbb{R}^dRd by ρ(x)=Ψ(x,f0(x))−Ψ(x,f1(x))\rho(x) = \Psi(x, f_0(x)) - \Psi(x, f_1(x))ρ(x)=Ψ(x,f0​(x))−Ψ(x,f1​(x)), up to sign, and shows the image is shattered by homogeneous halfspaces; the tie-breaking rule decides which sign and which halfspace convention to use. Claim 29.9(1) is the bound (1−ϵ)m≤δ(1-\epsilon)^m \le \delta(1−ϵ)m≤δ; Claim 29.9(2) needs only that at most (d−1)/2(d-1)/2(d−1)/2 of the d−1d-1d−1 light points appear in the sample, an event of probability at least 1/31/31/3 by Markov's inequality when m≤(d−1)/(6ϵ)m \le (d-1)/(6\epsilon)m≤(d−1)/(6ϵ), which exceeds the claimed e−1/6e^{-1}/6e−1/6.

Formalization scope

Labels are an arbitrary finite type, shattering and the Natarajan dimension are stated with witnesses f0,f1f_0, f_1f0​,f1​ defined on all of XXX, and the dimension is a supremum in N∪{∞}\mathbb{N} \cup \{\infty\}N∪{∞}. The multiclass 0–1 loss, the ERM property, agnostic PAC learnability and uniform convergence are Mission I's generic notions; the realizable multiclass PAC property is defined here in the shape of Definition 3.1 with D({h≠f})D(\{h \ne f\})D({h=f}) as the error, since Mission I's binary version is {0,1}\{0,1\}{0,1}-specific. Theorem 29.3 is stated exactly as Mission IV states Theorem 6.8, with existential constants, upper bounds for every ERM learner of a nonempty measurable class with the countable-approximation property (the measurability device of Remark 3.1), and lower bounds for ϵ<ϵ0\epsilon < \epsilon_0ϵ<ϵ0​, δ<δ0\delta < \delta_0δ<δ0​, d≥2d \ge 2d≥2. Argmax predictors, both One-versus-All and HΨH_\PsiHΨ​, break ties towards the smallest label; the book states this rule for One-versus-All, and some fixed rule is necessary for Theorem 29.7, since with arbitrary tie-breaking every function is an argmax predictor of the zero mapping. Lemmas 29.5 and 29.6 are stated per shattered set. Lemma 29.5 keeps the printed 3kdlog⁡(kd)3kd\log(kd)3kdlog(kd), which is true although the book's step ∣(Hbin)C∣≤∣C∣d|(H_{bin})_C| \le |C|^d∣(Hbin​)C​∣≤∣C∣d fails for small ∣C∣|C|∣C∣. Lemma 29.6 uses 2ldlog⁡2(2ld)2ld\log_2(2ld)2ldlog2​(2ld), which the counting supports, because the printed 3ldlog⁡(ld)3ld\log(ld)3ldlog(ld) is false at l=d=1l = d = 1l=d=1. Theorem 29.3's uniform-convergence upper bound is stated for d≥1d \ge 1d≥1. At d=0d = 0d=0 the confidence term log⁡(1/δ)\log(1/\delta)log(1/δ) vanishes as δ→1\delta \to 1δ→1, the bound reaches m=1m = 1m=1, and a single example is not representative. The class of §29.4 has labels Option of the subtype of finite-or-cofinite sets, with the discrete σ-algebra, and the two ERMs are predicates fixing the output on all-∗\ast∗ samples; Claim 29.9(1) is stated for countable XXX with measurable singletons and Claim 29.9(2) for finite XXX of size at least 222, with the proof's own distribution, h∅h_\emptyseth∅​ as target, and every ϵ∈(0,1/2)\epsilon \in (0, 1/2)ϵ∈(0,1/2) in place of the book's unspecified constant aaa.

Not stated: Corollary 29.8 (its lower bound (k−1)(n−1)(k-1)(n-1)(k−1)(n−1) is cited, not proved), Conjecture 29.10, the exercises.

Selected references

  • S. Shalev-Shwartz, S. Ben-David, Understanding Machine Learning: From Theory to Algorithms, Cambridge University Press, 2014, Chapter 29. doi:10.1017/CBO9781107298019
  • B. K. Natarajan, On learning sets and functions, Machine Learning 4, 1989. doi:10.1007/BF00114804
  • S. Ben-David, N. Cesa-Bianchi, D. Haussler, P. M. Long, Characterizations of learnability for classes of {0, …, n}-valued functions, Journal of Computer and System Sciences 50(1), 1995. doi:10.1006/jcss.1995.1008
  • D. Haussler, P. M. Long, A generalization of Sauer's lemma, Journal of Combinatorial Theory A 71(2), 1995. doi:10.1016/0097-3165(95)90001-2
  • A. Daniely, S. Sabato, S. Ben-David, S. Shalev-Shwartz, Multiclass learnability and the ERM principle, COLT 2011; Journal of Machine Learning Research 16, 2015.
  • A. Daniely, S. Sabato, S. Shalev-Shwartz, Multiclass learning approaches: a theoretical comparison with implications, NIPS 2012.
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Understanding Machine Learning XXII: Proof of the Fundamental TheoremTextbook

Motivation

Chapter 6 stated the fundamental theorem of statistical learning: a binary class is learnable if and only if its VC dimension is finite, with sample complexity Θ((d+ln⁡(1/δ))/ϵ2)\Theta((d + \ln(1/\delta))/\epsilon^2)Θ((d+ln(1/δ))/ϵ2) in the agnostic case and Θ((dln⁡(1/ϵ)+ln⁡(1/δ))/ϵ)\Theta((d\ln(1/\epsilon) + \ln(1/\delta))/\epsilon)Θ((dln(1/ϵ)+ln(1/δ))/ϵ) in the realizable case. Chapter 28 of Shalev-Shwartz and Ben-David, Understanding Machine Learning: From Theory to Algorithms (doi:10.1017/CBO9781107298019), proves it. The agnostic upper bound is obtained from the Rademacher machinery of Chapter 26 with Sauer's lemma and Massart's lemma, up to a log⁡(d/ϵ)\log(d/\epsilon)log(d/ϵ) factor that only chaining removes (28.1). The agnostic lower bound comes in two parts: a two-point construction giving m≥0.5log⁡(1/(4δ))/ϵ2m \ge 0.5\log(1/(4\delta))/\epsilon^2m≥0.5log(1/(4δ))/ϵ2, and a ddd-point construction giving m≥d/(512ϵ2)m \ge d/(512\epsilon^2)m≥d/(512ϵ2) at confidence 1/81/81/8, whose heart is Lemma 28.1, the optimality of the Maximum-Likelihood rule against the family of noisy distributions DbD_bDb​. The realizable upper bound is proved through ϵ\epsilonϵ-nets: with m≥8ϵ(2dlog⁡(16e/ϵ)+log⁡(2/δ))m \ge \frac8\epsilon(2d\log(16e/\epsilon) + \log(2/\delta))m≥ϵ8​(2dlog(16e/ϵ)+log(2/δ)) examples a random sample hits every set of measure at least ϵ\epsilonϵ in the class (Theorem 28.3), so any hypothesis consistent with the sample has error below ϵ\epsilonϵ. Mission IV states these bounds with unnamed constants; this mission gives the chapter's explicit ones.

Setting

HHH is a class of functions X→{0,1}X \to \{0,1\}X→{0,1} with the 0–1 loss and VCdim⁡(H)=d\operatorname{VCdim}(H) = dVCdim(H)=d. For the upper bound, A={(1[h(xi)≠yi])i:h∈H}A = \{(\mathbb{1}[h(x_i) \ne y_i])_i : h \in H\}A={(1[h(xi​)=yi​])i​:h∈H} is the loss set of a sample and R(A)R(A)R(A) its Rademacher complexity. For the lower bounds, C={c1,…,cd}C = \{c_1, \dots, c_d\}C={c1​,…,cd​} is a set shattered by HHH and, for b∈{±1}db \in \{\pm1\}^db∈{±1}d and ρ∈(0,1)\rho \in (0,1)ρ∈(0,1), DbD_bDb​ draws cic_ici​ uniformly and labels it bib_ibi​ with probability (1+ρ)/2(1+\rho)/2(1+ρ)/2; for d=1d = 1d=1 these are the distributions D±D_\pmD±​ of §28.2.1. The Maximum-Likelihood rule AMLA_{ML}AML​ predicts at each cic_ici​ the majority of the labels seen at cic_ici​. An ϵ\epsilonϵ-net for HHH with respect to DDD is a sample meeting every h∈Hh \in Hh∈H with D(h)≥ϵD(h) \ge \epsilonD(h)≥ϵ (Definition 28.2).

Formalization targets

Goal: Theorem 28.3

Let VCdim⁡(H)=d\operatorname{VCdim}(H) = dVCdim(H)=d, ϵ∈(0,1)\epsilon \in (0,1)ϵ∈(0,1), δ∈(0,1/4)\delta \in (0, 1/4)δ∈(0,1/4) and m≥8ϵ(2dlog⁡16eϵ+log⁡2δ)m \ge \frac8\epsilon\big(2d\log\frac{16e}{\epsilon} + \log\frac2\delta\big)m≥ϵ8​(2dlogϵ16e​+logδ2​). Then with probability at least 1−δ1 - \delta1−δ over S∼DmS \sim D^mS∼Dm, SSS is an ϵ\epsilonϵ-net for HHH.

Milestones

The two-sided deviation bound of §28.1 (∣LD(h)−LS(h)∣≤2(8dlog⁡(em/d)+2log⁡(4/δ))/m|L_D(h) - L_S(h)| \le 2\sqrt{(8d\log(em/d) + 2\log(4/\delta))/m}∣LD​(h)−LS​(h)∣≤2(8dlog(em/d)+2log(4/δ))/m​ uniformly over HHH); the lower bound m(ϵ,δ)≥0.5log⁡(1/(4δ))/ϵ2m(\epsilon,\delta) \ge 0.5\log(1/(4\delta))/\epsilon^2m(ϵ,δ)≥0.5log(1/(4δ))/ϵ2 of §28.2.1; Lemma 28.1; the lower bound m(ϵ,1/8)≥d/(512ϵ2)m(\epsilon, 1/8) \ge d/(512\epsilon^2)m(ϵ,1/8)≥d/(512ϵ2) of §28.2.2; the realizable upper bound of §28.3 (ERM has error at most ϵ\epsilonϵ with probability 1−δ1 - \delta1−δ for the sample size of Theorem 28.3). Further items: the Rademacher bound R(A)≤2dlog⁡(em/d)/mR(A) \le \sqrt{2d\log(em/d)/m}R(A)≤2dlog(em/d)/m​, the explicit uniform-convergence sample complexity of §28.1, and the expectation lower bound ρ/4\rho/4ρ/4 of §28.2.2.

Significance

These are the theorems that make the VC dimension the right measure of learnability, with constants. The upper bounds show what the abstract machinery of Missions II, IV, XX buys when instantiated: Sauer plus Massart plus Theorem 26.5 gives the agnostic rate, and the double-sample symmetrization plus Sauer gives the realizable rate, sharper by a factor 1/ϵ1/\epsilon1/ϵ because ϵ\epsilonϵ-nets need only one-sided control. The lower bounds are the No-Free-Lunch argument refined to quantify ϵ\epsilonϵ and δ\deltaδ: the two-point distribution shows that confidence costs log⁡(1/δ)/ϵ2\log(1/\delta)/\epsilon^2log(1/δ)/ϵ2, and the ddd-point family with Lemma 28.1 shows that the dimension costs d/ϵ2d/\epsilon^2d/ϵ2, through the exact optimality of majority voting and a binomial anti-concentration bound. Theorem 28.3 is also the basic ϵ\epsilonϵ-net theorem of Haussler and Welzl, a result of independent importance in computational geometry.

Difficulty

The Rademacher bound is Sauer's lemma (Mission IV) plus Massart's lemma (Mission XX) with ∥a−aˉ∥≤m\|a - \bar a\| \le \sqrt m∥a−aˉ∥≤m​; the deviation bound is Theorem 26.5 applied to ℓ\ellℓ and −ℓ-\ell−ℓ with a union bound; the explicit sample complexity is Lemma A.2, x≥4alog⁡(2a)+2b⇒x≥alog⁡x+bx \ge 4a\log(2a) + 2b \Rightarrow x \ge a\log x + bx≥4alog(2a)+2b⇒x≥alogx+b, which a formal proof must establish (the tangent inequality for log⁡\loglog at 2a2a2a). The two-point lower bound requires the binomial lower-tail estimate of Lemma B.11 and the algebra 12(1−1−4δ)≥δ\frac12(1 - \sqrt{1 - \sqrt{4\delta}}) \ge \delta21​(1−1−4δ​​)≥δ, valid for δ<1/4\delta < 1/4δ<1/4, the only nonvacuous range. Lemma 28.1 is a conditioning argument: fixing the instance indices and the labels off cic_ici​, the contribution of cic_ici​ is minimized by predicting the more likely bib_ibi​ given the labels at cic_ici​, which is the majority; the formal proof must decompose the product measure DbmD_b^mDbm​ over the positions rrr with xr=cix_r = c_ixr​=ci​. The expectation bound ρ/4\rho/4ρ/4 then needs Lemma B.11 again, 1−e−a≤a1 - e^{-a} \le a1−e−a≤a, Jensen for ⋅\sqrt{\cdot}⋅​ and E[ni]=m/d\mathbb{E}[n_i] = m/dE[ni​]=m/d, and the probability bound 1/81/81/8 follows by Mission III's reverse Markov inequality with ρ=8ϵ\rho = 8\epsilonρ=8ϵ. Theorem 28.3 is the double-sample argument: Claim 1 (P[S∈B]≤2P[(S,T)∈B′]P[S \in B] \le 2P[(S,T) \in B']P[S∈B]≤2P[(S,T)∈B′], via a Chernoff bound that only needs mϵ≥2log⁡2m\epsilon \ge 2\log 2mϵ≥2log2), Claim 2 (symmetrization by a random half, P[(S,T)∈B′]≤e−ϵm/4τH(2m)P[(S,T) \in B'] \le e^{-\epsilon m/4}\tau_H(2m)P[(S,T)∈B′]≤e−ϵm/4τH​(2m)), Sauer's lemma, and Lemma A.2 once more. The realizable upper bound applies Theorem 28.3 to the error sets {x:h(x)≠f(x)}\{x : h(x) \ne f(x)\}{x:h(x)=f(x)}, a class of the same VC dimension.

Formalization scope

All objects are those of the earlier missions: risks, samples and learners from Mission I, vcDim and the countable-approximation property PointwiseSeparable from Mission IV (the measurability device for suprema over HHH, used wherever a symmetrization or Rademacher argument is invoked), condLaw from Mission XIV for the distributions DbD_bDb​, and rademacher, evalSet, lossClass from Mission XX. Probability statements bound the outer measure of the failure event under iidLaw. The Rademacher and deviation items require m>d+1m > d + 1m>d+1, the range in which Mission IV states Sauer's lemma in the form (em/d)d(em/d)^d(em/d)d; the explicit sample complexity of §28.1 implies this range, since its first term 432dlog⁡(64d/ϵ2)/ϵ2432d\log(64d/\epsilon^2)/\epsilon^2432dlog(64d/ϵ2)/ϵ2 dominates the possibly negative 8dlog⁡(e/d)8d\log(e/d)8dlog(e/d), and Lemma A.2 holds for any real bbb, so the book's constants are used verbatim. The lower bounds take a shattered set as an injective c:Fin d→Xc : \mathrm{Fin}\ d \to Xc:Fin d→X with the shattering property written out, use DbD_bDb​ as condLaw of the uniform law on CCC, and state the excess risk against min⁡h∈HLDb(h)\min_{h \in H}L_{D_b}(h)minh∈H​LDb​​(h) as ∃h∈H\exists h \in H∃h∈H with L(h)+ϵ≤L(A(S))L(h) + \epsilon \le L(A(S))L(h)+ϵ≤L(A(S)), or as a real infimum over HHH in the expectation item; no measurability of the learner is needed because DbmD_b^mDbm​ is atomic. Lemma 28.1 compares the sums over bbb of the expected risks, the common term min⁡hLDb\min_h L_{D_b}minh​LDb​​ cancelling, for every majority rule with arbitrary tie-breaking. Theorem 28.3 and the realizable bound are stated for δ∈(0,1/4)\delta \in (0, 1/4)δ∈(0,1/4), the theorem's own range; the realizable bound is the inner clause of Mission I's IsPACWith on that range rather than a sample-complexity function, since the theorem does not cover δ≥1/4\delta \ge 1/4δ≥1/4 with its formula.

Not stated: the realizable lower bound (an exercise), the remark that chaining removes the logarithm in (28.1), and the intermediate claims of the proof of Theorem 28.3 as separate items.

Selected references

  • S. Shalev-Shwartz, S. Ben-David, Understanding Machine Learning: From Theory to Algorithms, Cambridge University Press, 2014, Chapter 28. doi:10.1017/CBO9781107298019
  • 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
  • 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
  • D. Haussler, E. Welzl, ε-nets and simplex range queries, Discrete and Computational Geometry 2, 1987. doi:10.1007/BF02187876
  • M. Anthony, P. L. Bartlett, Neural Network Learning: Theoretical Foundations, Cambridge University Press, 1999. doi:10.1017/CBO9780511624216
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Understanding Machine Learning XX: Rademacher ComplexitiesTextbook

Motivation

Chapter 4 showed that uniform convergence suffices for learnability; Chapter 26 of Shalev-Shwartz and Ben-David, Understanding Machine Learning: From Theory to Algorithms (doi:10.1017/CBO9781107298019), measures its rate. The representativeness of a sample, sup⁡h∈H(LD(h)−LS(h))\sup_{h \in H}(L_D(h) - L_S(h))suph∈H​(LD​(h)−LS​(h)), is the quantity that controls the excess risk of ERM, and the Rademacher complexity R(F∘S)=1mEσsup⁡f∈F∑iσif(zi)R(F \circ S) = \frac1m\mathbb{E}_\sigma\sup_{f \in F}\sum_i\sigma_i f(z_i)R(F∘S)=m1​Eσ​supf∈F​∑i​σi​f(zi​) estimates it from the sample itself: the symmetrization argument gives ERep⁡≤2 ER\mathbb{E}\operatorname{Rep} \le 2\,\mathbb{E}RERep≤2ER (Lemma 26.2), and McDiarmid's bounded-differences inequality turns expectations into high-probability statements, yielding the generalization bounds of Theorem 26.5, including the data-dependent ones in which the complexity is computed on the training set. A small calculus of Rademacher complexities follows, affine images, convex hulls, Massart's lemma for finite sets and the contraction lemma for Lipschitz compositions, and it is applied to linear classes with ℓ2\ell_2ℓ2​ and ℓ1\ell_1ℓ1​ constraints. The chapter's payoff is dimension-free generalization bounds for linear predictors with Lipschitz losses (Theorem 26.12), for hard-SVM (Theorems 26.13–26.14), and for predictors with low ℓ1\ell_1ℓ1​ norm (Theorem 26.15).

Setting

For a loss class F=ℓ∘HF = \ell \circ HF=ℓ∘H and a sample S=(z1,…,zm)S = (z_1, \dots, z_m)S=(z1​,…,zm​), Rep⁡D(F,S)=sup⁡f∈F(LD(f)−LS(f))\operatorname{Rep}_D(F, S) = \sup_{f \in F}(L_D(f) - L_S(f))RepD​(F,S)=supf∈F​(LD​(f)−LS​(f)) (26.1), F∘S={(f(z1),…,f(zm)):f∈F}F \circ S = \{(f(z_1), \dots, f(z_m)) : f \in F\}F∘S={(f(z1​),…,f(zm​)):f∈F}, and for A⊆RmA \subseteq \mathbb{R}^mA⊆Rm, R(A)=1mEσ[sup⁡a∈A∑iσiai]R(A) = \frac1m\mathbb{E}_\sigma[\sup_{a \in A}\sum_i\sigma_i a_i]R(A)=m1​Eσ​[supa∈A​∑i​σi​ai​] with σ\sigmaσ uniform on {±1}m\{\pm1\}^m{±1}m (26.5). The linear classes are H2∘S={(⟨w,xi⟩)i:∥w∥2≤1}H_2 \circ S = \{(\langle w, x_i\rangle)_i : \|w\|_2 \le 1\}H2​∘S={(⟨w,xi​⟩)i​:∥w∥2​≤1} in a Hilbert space and H1∘SH_1 \circ SH1​∘S with ∥w∥1≤1\|w\|_1 \le 1∥w∥1​≤1 in Rn\mathbb{R}^nRn (26.14). Losses of the form ℓ(w,(x,y))=φ(⟨w,x⟩,y)\ell(w, (x, y)) = \varphi(\langle w, x\rangle, y)ℓ(w,(x,y))=φ(⟨w,x⟩,y) with a↦φ(a,y)a \mapsto \varphi(a, y)a↦φ(a,y) ρ\rhoρ-Lipschitz (26.18) cover the hinge and absolute losses.

Formalization targets

Goal: Theorem 26.5

Assume ∣ℓ(h,z)∣≤c|\ell(h, z)| \le c∣ℓ(h,z)∣≤c for all zzz and h∈Hh \in Hh∈H. Then, each with probability at least 1−δ1 - \delta1−δ over S∼DmS \sim D^mS∼Dm:

  1. for all h∈Hh \in Hh∈H, LD(h)−LS(h)≤2 ES′∼DmR(ℓ∘H∘S′)+c2ln⁡(2/δ)/mL_D(h) - L_S(h) \le 2\,\mathbb{E}_{S' \sim D^m}R(\ell \circ H \circ S') + c\sqrt{2\ln(2/\delta)/m}LD​(h)−LS​(h)≤2ES′∼Dm​R(ℓ∘H∘S′)+c2ln(2/δ)/m​;
  2. for all h∈Hh \in Hh∈H, LD(h)−LS(h)≤2R(ℓ∘H∘S)+4c2ln⁡(4/δ)/mL_D(h) - L_S(h) \le 2R(\ell \circ H \circ S) + 4c\sqrt{2\ln(4/\delta)/m}LD​(h)−LS​(h)≤2R(ℓ∘H∘S)+4c2ln(4/δ)/m​;
  3. for any h⋆∈Hh^\star \in Hh⋆∈H, LD(ERMH(S))−LD(h⋆)≤2R(ℓ∘H∘S)+5c2ln⁡(8/δ)/mL_D(\mathrm{ERM}_H(S)) - L_D(h^\star) \le 2R(\ell \circ H \circ S) + 5c\sqrt{2\ln(8/\delta)/m}LD​(ERMH​(S))−LD​(h⋆)≤2R(ℓ∘H∘S)+5c2ln(8/δ)/m​.

Milestones

Lemma 26.2 (symmetrization); Lemma 26.8 (Massart); Lemma 26.9 (contraction); Theorem 26.12 (linear predictors with ℓ2\ell_2ℓ2​ constraints); Theorem 26.13 (hard-SVM). Further items: Theorem 26.3, Lemma 26.4 (McDiarmid), Lemmas 26.6, 26.7, 26.10, 26.11, Theorem 26.14 and Theorem 26.15.

Significance

Rademacher complexity is the modern language of uniform convergence: it is data-dependent, it is dimension-free for linear classes, and it composes with Lipschitz losses, which is why the SVM bounds of this chapter do not depend on the dimension of www and apply verbatim to kernel methods (Remark 26.2). Theorem 26.5 is the template every such bound follows, symmetrization plus McDiarmid, and the two data-dependent parts are the first bounds in the book that use the training set both to learn and to certify. Massart's lemma and the contraction lemma are the two tools that make the calculus work, the first converting finiteness into a logarithmic dependence, the second removing the loss function from the picture. Theorem 26.13 finally justifies the margin-based sample complexity R2∥w⋆∥2/ϵ2R^2\|w^\star\|^2/\epsilon^2R2∥w⋆∥2/ϵ2 of hard-SVM, and Theorem 26.14 gives a bound computable from the output alone.

Difficulty

Lemma 26.2 is the symmetrization argument: a ghost sample, the exchange of zjz_jzj​ and zj′z'_jzj′​ (26.7), the introduction of one Rademacher sign at a time (26.8)–(26.9), and the split of the supremum. Formally it needs Fubini over the product of 2m2m2m copies of DDD and the sign average, and the measurability of the suprema, which the statements assume. McDiarmid's inequality is a martingale argument with Hoeffding's lemma at each step; it is the substantial probabilistic input, and Theorem 26.5 combines it with Lemma 26.2, a union bound and Hoeffding's inequality along the decomposition (26.10). Lemma 26.6 is the symmetry σ↦−σ\sigma \mapsto -\sigmaσ↦−σ; Lemma 26.7 is the fact that a linear functional on the simplex is maximized at a vertex; Massart's lemma is the exponential-moment bound Eeσa≤ea2/2\mathbb{E}e^{\sigma a} \le e^{a^2/2}Eeσa≤ea2/2 with Jensen and an optimized scaling; the contraction lemma is Kakade and Tewari's coordinate-by-coordinate argument (26.12)–(26.13), which in a formal proof must be run as an induction over the coordinates. Lemmas 26.10 and 26.11 are Cauchy–Schwarz and Hölder followed by Jensen, respectively Massart on the 2n2n2n coordinate vectors. Theorem 26.12 chains contraction, Lemma 26.10 and Theorem 26.5 on the almost-sure event ∥x∥≤R\|x\| \le R∥x∥≤R; Theorem 26.13 specializes it to the ramp loss with B=∥w⋆∥B = \|w^\star\|B=∥w⋆∥, where the hard-SVM output has zero empirical ramp loss; Theorem 26.14 is a union bound over the nested classes ∥w∥≤2i\|w\| \le 2^i∥w∥≤2i with δi=δ/(2i2)\delta_i = \delta/(2i^2)δi​=δ/(2i2); Theorem 26.15 repeats Theorem 26.12 with Lemma 26.11.

Formalization scope

The Rademacher complexity is a finite average over the 2m2^m2m sign vectors, so no measure on {±1}m\{\pm1\}^m{±1}m is needed, and the supremum over AAA is the real supremum over the subtype AAA; the theorems assume AAA nonempty and bounded, which every evaluation set of a bounded loss class satisfies. Risks are Mission I's risk and empRisk, samples are Fin m-indexed under iidLaw, and probability statements bound the outer measure of the failure event. Expectations of suprema over uncountable classes are Bochner integrals, so Lemma 26.2, Theorem 26.3 and Theorem 26.5 carry explicit hypotheses that S↦Rep⁡D(F,S)S \mapsto \operatorname{Rep}_D(F, S)S↦RepD​(F,S) and S↦R(F∘S)S \mapsto R(F \circ S)S↦R(F∘S) are measurable, the book's Remark 3.1 made visible; for the linear classes of §26.3–§26.4 these hold automatically when the Hilbert space is separable (the supremum over the ball is a supremum over a countable dense subset), which is why Theorems 26.12–26.14 assume SecondCountableTopology. McDiarmid's inequality is stated for a measurable function on a product of arbitrary probability measures. Theorem 26.13's error is P[y⟨wS,x⟩≤0]P[y\langle w_S, x\rangle \le 0]P[y⟨wS​,x⟩≤0], which dominates P[y≠sign⁡⟨wS,x⟩]P[y \ne \operatorname{sign}\langle w_S, x\rangle]P[y=sign⟨wS​,x⟩] whatever sign⁡(0)\operatorname{sign}(0)sign(0) is, and the hard-SVM learner is any map returning a minimum-norm margin-1 separator on separable samples; measurability of the learner is not needed because the bound is uniform over the ball. Theorem 26.14 is given with the constants of its proof, 4(ln⁡(4log⁡2∥wS∥)+ln⁡(1/δ))/m\sqrt{4(\ln(4\log_2\|w_S\|) + \ln(1/\delta))/m}4(ln(4log2​∥wS​∥)+ln(1/δ))/m​ rather than the printed ln⁡(4log⁡2∥wS∥/δ)/m\sqrt{\ln(4\log_2\|w_S\|/\delta)/m}ln(4log2​∥wS​∥/δ)/m​, and for ∥wS∥≥2\|w_S\| \ge 2∥wS​∥≥2, where i=⌈log⁡2∥wS∥⌉i = \lceil\log_2\|w_S\|\rceili=⌈log2​∥wS​∥⌉ satisfies 1≤i≤2log⁡2∥wS∥1 \le i \le 2\log_2\|w_S\|1≤i≤2log2​∥wS​∥ as the proof requires; the item text records this. Norms on Rn\mathbb{R}^nRn as Fin n → ℝ are sup norms (Lemma 26.11, Theorem 26.15), Euclidean norms are written out (Massart), and inner product spaces carry the Euclidean norm.

Not stated: Definition 26.1 (already Mission II's IsRepresentative), the validation heuristic (26.2)–(26.3), Remark 26.1 (the improved rate under separability, no proof), Remark 26.2.

Selected references

  • S. Shalev-Shwartz, S. Ben-David, Understanding Machine Learning: From Theory to Algorithms, Cambridge University Press, 2014, Chapter 26. doi:10.1017/CBO9781107298019
  • P. L. Bartlett, S. Mendelson, Rademacher and Gaussian complexities: risk bounds and structural results, Journal of Machine Learning Research 3, 2002.
  • V. Koltchinskii, D. Panchenko, Rademacher processes and bounding the risk of function learning, in High Dimensional Probability II, Birkhäuser, 2000. doi:10.1007/978-1-4612-1358-1_29
  • C. McDiarmid, On the method of bounded differences, in Surveys in Combinatorics, Cambridge University Press, 1989. doi:10.1017/CBO9781107359949.008
  • S. M. Kakade, K. Sridharan, A. Tewari, On the complexity of linear prediction: risk bounds, margin bounds, and regularization, NIPS 2008.
  • S. Boucheron, O. Bousquet, G. Lugosi, Theory of classification: a survey of some recent advances, ESAIM: Probability and Statistics 9, 2005. doi:10.1051/ps:2005018
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CombinatoricsMachine LearningOptimization·Captain: naimengye

Understanding Machine Learning XVI: Online LearningTextbook

Motivation

In PAC learning the learner receives a batch of examples, learns, and only then predicts. Online learning has no such separation: on each round the learner receives an instance, predicts its label, and then sees the true label, and the goal is to make few mistakes over the whole sequence, with no statistical assumption whatsoever on how the sequence is generated, adversarially if need be. Chapter 21 of Shalev-Shwartz and Ben-David, Understanding Machine Learning: From Theory to Algorithms (doi:10.1017/CBO9781107298019), develops this model along the same lines as the PAC theory. In the realizable case, mistake bounds replace sample complexity, and a combinatorial dimension due to Littlestone, Ldim⁡(H)\operatorname{Ldim}(H)Ldim(H), characterizes the best achievable bound exactly (Lemmas 21.6 and 21.7), playing the role the VC dimension plays for PAC learning, with VCdim⁡(H)≤Ldim⁡(H)\operatorname{VCdim}(H) \le \operatorname{Ldim}(H)VCdim(H)≤Ldim(H) and an arbitrarily large gap (Theorem 21.9). In the unrealizable case regret replaces excess risk; deterministic learners can be forced to regret T/2T/2T/2 (Cover), but randomized predictions restore sublinear regret through the Weighted-Majority algorithm of Littlestone, Warmuth and Vovk (Theorem 21.11). The chapter closes with online convex optimization, where Online Gradient Descent (Zinkevich) attains regret O(T)O(\sqrt T)O(T​) (Theorem 21.15), and with the online Perceptron, whose mistake bound follows from a round-specific surrogate loss (Theorem 21.16).

Setting

An online algorithm is a deterministic map from the history of past examples and the current instance to a prediction. For a sequence SSS labeled by some h⋆∈Hh^\star \in Hh⋆∈H, MA(S)M_A(S)MA​(S) is the number of mistakes and MA(H)M_A(H)MA​(H) the supremum over all such sequences (Definition 21.1). The Consistent algorithm predicts with any hypothesis of the version space VtV_tVt​ (the hypotheses consistent with the past), Halving with its majority label, and SOA with the label rrr for which {h∈Vt:h(xt)=r}\{h \in V_t : h(x_t) = r\}{h∈Vt​:h(xt​)=r} has the larger Littlestone dimension, ties to 111. An HHH-shattered tree of depth ddd assigns an instance to every node of a complete binary tree so that every labeling (y1,…,yd)(y_1, \dots, y_d)(y1​,…,yd​) is realized by some h∈Hh \in Hh∈H along the path it determines; Ldim⁡(H)\operatorname{Ldim}(H)Ldim(H) is the maximal such depth (Definitions 21.4–21.5). In the unrealizable case predictions are pt∈[0,1]p_t \in [0,1]pt​∈[0,1], the loss is ∣pt−yt∣|p_t - y_t|∣pt​−yt​∣, and the regret against hhh is ∑t∣pt−yt∣−∑t∣h(xt)−yt∣\sum_t |p_t - y_t| - \sum_t |h(x_t) - y_t|∑t​∣pt​−yt​∣−∑t​∣h(xt​)−yt​∣ (21.1). Weighted-Majority maintains wi(t)∝exp⁡(−η∑s<tvs,i)w^{(t)}_i \propto \exp(-\eta\sum_{s<t} v_{s,i})wi(t)​∝exp(−η∑s<t​vs,i​) over ddd experts with costs vt∈[0,1]dv_t \in [0,1]^dvt​∈[0,1]d and pays ⟨w(t),vt⟩\langle w^{(t)}, v_t\rangle⟨w(t),vt​⟩. Online Gradient Descent on a closed convex HHH predicts w(t)w^{(t)}w(t), receives a convex ftf_tft​, takes a subgradient vtv_tvt​ at w(t)w^{(t)}w(t) and projects w(t)−ηvtw^{(t)} - \eta v_tw(t)−ηvt​ back onto HHH; the online Perceptron is the special case w(t+1)=w(t)+ytxtw^{(t+1)} = w^{(t)} + y_t x_tw(t+1)=w(t)+yt​xt​ on rounds with yt⟨w(t),xt⟩≤0y_t\langle w^{(t)}, x_t\rangle \le 0yt​⟨w(t),xt​⟩≤0.

Formalization targets

Goal: Theorem 21.11

For d≥1d \ge 1d≥1 experts, cost vectors vt∈[0,1]dv_t \in [0,1]^dvt​∈[0,1]d, T>2log⁡dT > 2\log dT>2logd and η=2log⁡(d)/T\eta = \sqrt{2\log(d)/T}η=2log(d)/T​,

∑t=1T⟨w(t),vt⟩−min⁡i∈[d]∑t=1Tvt,i≤2log⁡(d) T.\sum_{t=1}^T \langle w^{(t)}, v_t\rangle - \min_{i \in [d]}\sum_{t=1}^T v_{t,i} \le \sqrt{2\log(d)\,T}.t=1∑T​⟨w(t),vt​⟩−i∈[d]min​t=1∑T​vt,i​≤2log(d)T​.

Milestones

Theorem 21.3 (Halving makes at most log⁡2∣H∣\log_2|H|log2​∣H∣ mistakes); Lemma 21.6 (MA(H)≥Ldim⁡(H)M_A(H) \ge \operatorname{Ldim}(H)MA​(H)≥Ldim(H) for every AAA); Lemma 21.7 (MSOA(H)≤Ldim⁡(H)M_{\mathrm{SOA}}(H) \le \operatorname{Ldim}(H)MSOA​(H)≤Ldim(H)); Theorem 21.15 (the three regret bounds of Online Gradient Descent); Theorem 21.16 (the online Perceptron bound ∣M∣≤∑tft(w⋆)+R∥w⋆∥∑tft(w⋆)+R2∥w⋆∥2|M| \le \sum_t f_t(w^\star) + R\|w^\star\|\sqrt{\sum_t f_t(w^\star)} + R^2\|w^\star\|^2∣M∣≤∑t​ft​(w⋆)+R∥w⋆∥∑t​ft​(w⋆)​+R2∥w⋆∥2 and its separable case). Further items: Corollary 21.2, Theorem 21.9, Example 21.4, Cover's impossibility, Corollary 21.12 and the Ldim⁡\operatorname{Ldim}Ldim half of Theorem 21.10.

Significance

Corollary 21.8 is one of the cleanest characterizations in learning theory: the Littlestone dimension is exactly the optimal mistake bound, with SOA attaining it and Lemma 21.6 forbidding anything better. Theorem 21.11 is the engine of the unrealizable case and of a large part of online learning: the multiplicative-weights analysis with the potential log⁡Zt\log Z_tlogZt​ gives regret 2log⁡(d)T\sqrt{2\log(d)T}2log(d)T​ against the best of ddd experts, and with the experts of pp. 298–299 it yields Theorem 21.10, regret 2Ldim⁡(H)log⁡(eT) T\sqrt{2\operatorname{Ldim}(H)\log(eT)\,T}2Ldim(H)log(eT)T​ for any class of finite Littlestone dimension. Theorem 21.15 is the online counterpart of the SGD analysis of Chapter 14, and the derivation of Theorem 21.16 from it shows how a surrogate loss chosen per round turns a regret bound into a mistake bound, the Perceptron bound of Chapter 9 falling out as the separable case. On the platform, these items give the first online-learning model, reusing Mission X's subgradients and projections.

Difficulty

Corollary 21.2 and Theorem 21.3 are counting arguments on the version space, but formally they require tracking the version space along the history and the fact that a mistake by Halving halves it. Lemma 21.6 is the adversary argument: given a shattered tree, feed the instance at the current node and the label opposite to the prediction; the resulting sequence is labeled by some h∈Hh \in Hh∈H by the shattering property, and the algorithm errs on every round. Lemma 21.7 needs the combinatorial core of the chapter: if both restricted version spaces had Littlestone dimension equal to Ldim⁡(Vt)\operatorname{Ldim}(V_t)Ldim(Vt​), their shattered trees could be glued under a new root to a deeper tree. Theorem 21.9 builds a shattered tree with all nodes at depth iii equal to xix_ixi​; Example 21.4 builds the dyadic tree. Theorem 21.11's proof is the book's: e−a≤1−a+a2/2e^{-a} \le 1 - a + a^2/2e−a≤1−a+a2/2 for a≥0a \ge 0a≥0, log⁡(1−b)≤−b\log(1 - b) \le -blog(1−b)≤−b, the telescoping potential log⁡(Zt+1/Zt)\log(Z_{t+1}/Z_t)log(Zt+1​/Zt​), the lower bound log⁡ZT+1≥−ηmin⁡i∑tvt,i\log Z_{T+1} \ge -\eta\min_i\sum_t v_{t,i}logZT+1​≥−ηmini​∑t​vt,i​, and the choice of η\etaη; the hypothesis T>2log⁡dT > 2\log dT>2logd makes η<1\eta < 1η<1. Corollary 21.12 is the reduction of hypotheses to experts, and Theorem 21.10 is the expert construction with the counting bound (21.4) ∑L≤Ldim⁡(TL)≤(eT/Ldim⁡)Ldim⁡\sum_{L \le \operatorname{Ldim}} \binom{T}{L} \le (eT/\operatorname{Ldim})^{\operatorname{Ldim}}∑L≤Ldim​(LT​)≤(eT/Ldim)Ldim (Lemma A.5) and Lemma 21.13, which simulates SOA on the labels of hhh; small horizons are covered by the trivial bound regret≤T\text{regret} \le Tregret≤T. Theorem 21.15 is the telescoping argument of Lemma 14.1 with the projection lemma of Chapter 14 at every step; Theorem 21.16 applies it to ft=1[t∈M][1−yt⟨w,xt⟩]+f_t = \mathbb{1}[t \in M][1 - y_t\langle w, x_t\rangle]_+ft​=1[t∈M][1−yt​⟨w,xt​⟩]+​ with η=∥w⋆∥/(R∣M∣)\eta = \|w^\star\|/(R\sqrt{|M|})η=∥w⋆∥/(R∣M∣​) and solves the quadratic inequality (21.6).

Formalization scope

Online algorithms are deterministic functions List (X × Y) → X → Y; a sequence is Fin T-indexed and the history at round ttt is its first ttt examples. Mistake bounds and the Littlestone dimension are suprema in ℕ∞, so mistakeBound, ldim and their comparisons are meaningful when infinite. Shattered trees are indexed by paths rather than by the book's node numbers it=2t−1+∑j<tyj2t−1−ji_t = 2^{t-1} + \sum_{j<t} y_j 2^{t-1-j}it​=2t−1+∑j<t​yj​2t−1−j, whose binary expansion is exactly the path; the two descriptions are the same tree. Halving and SOA break ties towards 111 as in the book; Consistent is stated as a property of an algorithm. The unrealizable case uses real-valued predictions with the loss ∣pt−yt∣|p_t - y_t|∣pt​−yt​∣ as the book does, and the theorems of that section assert the existence of an algorithm for each horizon TTT, because Weighted-Majority takes TTT as input. Weighted-Majority's distribution is written in unrolled form, wi(t)∝exp⁡(−η∑s<tvs,i)w^{(t)}_i \propto \exp(-\eta\sum_{s<t}v_{s,i})wi(t)​∝exp(−η∑s<t​vs,i​), which is the update rule iterated from w~(1)=(1,…,1)\tilde w^{(1)} = (1, \dots, 1)w~(1)=(1,…,1). Theorem 21.10 is stated for classes with Ldim⁡(H)<∞\operatorname{Ldim}(H) < \inftyLdim(H)<∞ and in its Ldim⁡(H)log⁡(eT)\operatorname{Ldim}(H)\log(eT)Ldim(H)log(eT) form, the log⁡∣H∣\log|H|log∣H∣ form being Corollary 21.12; its lower bound, proved in Ben-David, Pál and Shalev-Shwartz (2009), is not stated. Online Gradient Descent is driven by a subgradient selector gt(w)∈∂ft(w)g_t(w) \in \partial f_t(w)gt​(w)∈∂ft​(w) (Mission X's global subgradients), from w(0)=0w^{(0)} = 0w(0)=0, on a closed convex HHH containing the comparator; the Lipschitz parts take LipschitzWith ρ (f t) and T≥1T \ge 1T≥1. The Perceptron's MMM is the set of update rounds yt⟨w(t),xt⟩≤0y_t\langle w^{(t)}, x_t\rangle \le 0yt​⟨w(t),xt​⟩≤0, which contains every prediction mistake whatever sign⁡(0)\operatorname{sign}(0)sign(0) is and is the set the book's derivation actually uses; RRR is any bound on ∥xt∥\|x_t\|∥xt​∥ for t<Tt < Tt<T. Cover's impossibility is stated for deterministic {0,1}\{0,1\}{0,1}-valued algorithms, the setting in which the book states it.

Not stated: the Doubling Trick (Exercise 4), Exercises 1–3 (specific tight examples), the SOA-based Expert algorithm as a separate definition (it is internal to the proof of Theorem 21.10), Lemma 21.13 and Corollary 21.14 as items, and the lower bound of Theorem 21.10.

Selected references

  • S. Shalev-Shwartz, S. Ben-David, Understanding Machine Learning: From Theory to Algorithms, Cambridge University Press, 2014, Chapter 21. doi:10.1017/CBO9781107298019
  • N. Littlestone, Learning quickly when irrelevant attributes abound: a new linear-threshold algorithm, Machine Learning 2, 1988. doi:10.1007/BF00116827
  • N. Littlestone, M. K. Warmuth, The weighted majority algorithm, Information and Computation 108(2), 1994. doi:10.1006/inco.1994.1009
  • S. Ben-David, D. Pál, S. Shalev-Shwartz, Agnostic online learning, COLT 2009.
  • M. Zinkevich, Online convex programming and generalized infinitesimal gradient ascent, ICML 2003.
  • N. Cesa-Bianchi, G. Lugosi, Prediction, Learning, and Games, Cambridge University Press, 2006. doi:10.1017/CBO9780511546921
  • S. Shalev-Shwartz, Online learning and online convex optimization, Foundations and Trends in Machine Learning 4(2), 2011. doi:10.1561/2200000018
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Mathematical Physics·Captain: Lucas

Dyson 2013: Is a Graviton Detectable?Research Paper

Motivation

Whether the quantization of the gravitational field is observable is a long-standing question at the interface of general relativity and quantum theory. In his 2013 talk Is a Graviton Detectable? (doi:10.1142/S0217751X1330041X), Freeman Dyson examined three families of hypothetical single-graviton detectors and estimated, for each, why it fails: LIGO-type interferometers (Sec. 3), atoms absorbing a graviton by the gravitoelectric effect (Secs. 4–5), and Gertsenshtein photon–graviton conversion in a magnetic field (Secs. 6–7).

Most of the paper consists of order-of-magnitude physical estimates. A part of it, however, consists of precise mathematical statements: exact algebraic consequences of the stated physical relations, and one genuine analytic inequality about the quadrupole factor QQQ that controls the graviton absorption cross-section of a bound particle. This mission collects those statements.

Setting

Sections 3. Let c,G,ℏ>0c, G, \hbar > 0c,G,ℏ>0 be the speed of light, Newton's constant and the reduced Planck constant. The Planck length is Lp=(Gℏ/c3)1/2L_p = (G\hbar/c^3)^{1/2}Lp​=(Gℏ/c3)1/2 (Eq. (5)). A gravitational wave of strain amplitude fff and angular frequency ω\omegaω has energy density E=c232πGω2f2E = \frac{c^2}{32\pi G}\omega^2 f^2E=32πGc2​ω2f2 (Eq. (2)); a single graviton of frequency ω\omegaω has energy density at most Es=ℏω4/c3E_s = \hbar\omega^4/c^3Es​=ℏω4/c3 (Eq. (3)).

Section 4. For an electron bound in a state with zero angular momentum about the zzz-axis, with real wave function f(s,z)f(s,z)f(s,z) in cylindrical coordinates (s>0s>0s>0 the distance from the zzz-axis), let f′=∂f/∂sf' = \partial f/\partial sf′=∂f/∂s and define

Q=∫R∫0∞s3[f′]2 ds dz2∫R∫0∞s f2 ds dz(Eq. (16)).Q = \frac{\int_{\mathbb R}\int_0^\infty s^3 [f']^2\, ds\, dz}{2\int_{\mathbb R}\int_0^\infty s\, f^2\, ds\, dz} \qquad \text{(Eq. (16))}.Q=2∫R​∫0∞​sf2dsdz∫R​∫0∞​s3[f′]2dsdz​(Eq. (16)).

The s-state of Eq. (19) is f=r−ne−r/Rf = r^{-n} e^{-r/R}f=r−ne−r/R with r=s2+z2r = \sqrt{s^2+z^2}r=s2+z2​.

Sections 6–7. For a transverse magnetic field BBB, the mixing length is L=2c2/(G1/2B)L = 2c^2/(G^{1/2}B)L=2c2/(G1/2B) (Eq. (29)) and the photon-to-graviton conversion probability over a distance DDD is P=sin⁡2(D/L)P = \sin^2(D/L)P=sin2(D/L) (Eq. (28)). Vacuum nonlinearity slows the photon by the fraction g=kαB2/(360π2Hc2)g = k\alpha B^2/(360\pi^2 H_c^2)g=kαB2/(360π2Hc2​) (Eq. (36)), where α\alphaα is the fine-structure constant and HcH_cHc​ the critical field, giving the coherence length Lc=c/(gω)L_c = c/(g\omega)Lc​=c/(gω) (Eq. (37)).

Formalization targets

Goal — Eq. (18)

For every nonzero, normalizable axially symmetric wave function with finite ∫s3[f′]2\int s^3 [f']^2∫s3[f′]2,

Q>12.Q > \tfrac12 .Q>21​.

Milestones

  • Eq. (17): ∫ ⁣ ⁣∫s3 [f′+f/s]2 ds dz>0\int\!\!\int s^3\,[f' + f/s]^2\, ds\,dz > 0∫∫s3[f′+f/s]2dsdz>0 (see the note on the sign below).
  • Eq. (20): for the s-state (19), Q=45(1−n6)Q = \frac45\left(1 - \frac n6\right)Q=54​(1−6n​).
  • Eqs. (4), (6): equating (2) and (3) gives f=(32π)1/2Lpω/cf = (32\pi)^{1/2} L_p\omega/cf=(32π)1/2Lp​ω/c, and with D=c/ωD = c/\omegaD=c/ω, δ=fD=(32π)1/2Lp\delta = fD = (32\pi)^{1/2}L_pδ=fD=(32π)1/2Lp​.
  • Eq. (8): free mirrors with Mδ2≥ℏTM\delta^2 \ge \hbar TMδ2≥ℏT, T≥D/cT \ge D/cT≥D/c, δ=Lp\delta = L_pδ=Lp​ satisfy D≤GM/c2D \le GM/c^2D≤GM/c2.
  • Eq. (10): clamped mirrors with δ2≥ℏD/(Ms)\delta^2 \ge \hbar D/(Ms)δ2≥ℏD/(Ms), δ=Lp\delta = L_pδ=Lp​, s<cs < cs<c satisfy GM/c2≥(c/s)D>DGM/c^2 \ge (c/s)D > DGM/c2≥(c/s)D>D.
  • Eqs. (28)–(30): P≤GB2D2/(4c4)P \le GB^2D^2/(4c^4)P≤GB2D2/(4c4), with asymptotic equality as D→0+D \to 0^+D→0+.
  • Eq. (37): for k=4k = 4k=4, Lc=90π2cHc2/(αB2ω)L_c = 90\pi^2 c H_c^2/(\alpha B^2\omega)Lc​=90π2cHc2​/(αB2ω).
  • Eqs. (38)–(39): if D≤LcD \le L_cD≤Lc​ then P≤2025π4GHc4/(α2c2B2ω2)P \le 2025\pi^4 G H_c^4/(\alpha^2 c^2 B^2\omega^2)P≤2025π4GHc4​/(α2c2B2ω2) (the symbolic form of P≤1036/(B2ω2)P \le 10^{36}/(B^2\omega^2)P≤1036/(B2ω2)).

Significance

Eq. (18) is what allows Dyson to conclude that the averaged absorption cross-section 4π2Lp2Q4\pi^2L_p^2 Q4π2Lp2​Q (Eq. (14)) is, for every bound particle, of the order of the Planck area; together with Eq. (20) it shows QQQ is of order unity for tightly bound s-states. The Section 3 bounds are the precise algebraic content of the argument that measuring distances to Planck accuracy forces the apparatus inside its own Schwarzschild radius. The Section 7 bounds are the algebraic content of the argument that vacuum birefringence limits Gertsenshtein conversion.

None of these statements has, to our knowledge, a machine-checked proof. Eq. (18) is a weighted Hardy-type inequality on the half line with sharp constant, applied slice by slice; formalizing it produces reusable one-dimensional weighted Hardy inequalities. Eq. (20) requires explicit Gamma-function integrals in cylindrical coordinates.

Difficulty

For Eq. (18) the difficulty is analytic: the inequality must hold for all admissible fff, including functions that are not compactly supported and may be singular on the zzz-axis, and it is strict although its sharp constant is not attained. Boundary terms of the integration by parts behind Eq. (17) must be controlled using only the integrability assumptions. The printed Eq. (17) has the sign f′−f/sf' - f/sf′−f/s; with that sign the integral is trivially positive and does not imply Eq. (18). The mission uses f′+f/sf' + f/sf′+f/s, the sign under which (17) implies (18). The algebraic milestones are elementary.

Formalization scope

All quantities are real. f:R→R→Rf : \mathbb R \to \mathbb R \to \mathbb Rf:R→R→R is a function of (s,z)(s,z)(s,z); f′f'f′ is deriv in the first variable; integrals are Lebesgue integrals over the half plane {s>0}×R\{s > 0\}\times\mathbb R{s>0}×R. The admissible class for Eqs. (17)–(18) is: f(⋅,z)f(\cdot,z)f(⋅,z) differentiable at every s>0s>0s>0, sf2s f^2sf2 and s3[f′]2s^3[f']^2s3[f′]2 integrable on the half plane, and fff not almost-everywhere zero there. These hypotheses rule out the degenerate reading Q=0/0Q = 0/0Q=0/0 (Lean's division returns 000). Eq. (20) requires R>0R > 0R>0 and n<3/2n < 3/2n<3/2, the range in which the integrals in Eq. (16) converge. Physical constants are arbitrary positive reals; numerical cgs values (e.g. Eqs. (5), (21), (31)) are not formalized. The heuristic parts of the paper (Bohr–Rosenfeld argument, the sum rule (14), astrophysical source estimates, neutrino backgrounds) are out of scope.

Selected references

  • F. Dyson, Is a Graviton Detectable?, Int. J. Mod. Phys. A 28 (2013) 1330041. https://doi.org/10.1142/S0217751X1330041X
  • T. Rothman and S. Boughn, Can gravitons be detected?, Found. Phys. 36 (2006) 1801. https://doi.org/10.1007/s10701-006-9081-9
  • M. E. Gertsenshtein, Wave resonance of light and gravitational waves, Sov. Phys. JETP 14 (1962) 84.
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Understanding Machine Learning XIV: Nearest NeighborTextbook

Motivation

Every learning paradigm of the book so far, ERM, SRM, MDL, RLM, is defined by a hypothesis class: the learner searches a predefined set of functions. Nearest Neighbor is the first method that is not. It memorizes the training set and labels a new point by the labels of its closest neighbors, on the assumption that the features are relevant to the labels in a way that makes close-by points likely to share a label. Chapter 19 of Shalev-Shwartz and Ben-David, Understanding Machine Learning: From Theory to Algorithms (doi:10.1017/CBO9781107298019), makes that assumption precise, a Lipschitz conditional probability, and proves a finite-sample guarantee: the expected error of the 1-NN rule on mmm examples is at most twice the Bayes error plus 4cd m−1/(d+1)4c\sqrt d\, m^{-1/(d+1)}4cd​m−1/(d+1) (Theorem 19.3). The classical results of Cover and Hart (1967) and Stone (1977) are asymptotic; the book insists, as it did in §7.4, on a bound that says what a finite sample buys under an explicit prior assumption. The chapter also proves that the exponential dependence on the dimension is not an artifact (Theorem 19.4, the curse of dimensionality) and, in its exercises, extends the analysis to the kkk-NN rule, whose error converges to (1+8/k)(1 + \sqrt{8/k})(1+8/k​) times the Bayes error (Theorem 19.5).

Setting

The instance domain XXX carries a metric ρ\rhoρ; for the analysis X=[0,1]dX = [0,1]^dX=[0,1]d with the Euclidean distance and Y={0,1}Y = \{0,1\}Y={0,1} with the 0–1 loss. For a sample S=(x1,y1),…,(xm,ym)S = (x_1, y_1), \dots, (x_m, y_m)S=(x1​,y1​),…,(xm​,ym​) and a point xxx, let π1(x),…,πm(x)\pi_1(x), \dots, \pi_m(x)π1​(x),…,πm​(x) reorder the sample by distance to xxx. The kkk-NN rule returns the majority label among yπ1(x),…,yπk(x)y_{\pi_1(x)}, \dots, y_{\pi_k(x)}yπ1​(x)​,…,yπk​(x)​; the 1-NN rule is hS(x)=yπ1(x)h_S(x) = y_{\pi_1(x)}hS​(x)=yπ1​(x)​; in general, for φ:(X×Y)k→Y\varphi : (X \times Y)^k \to Yφ:(X×Y)k→Y, the kkk-NN rule with respect to φ\varphiφ is hS(x)=φ((xπ1(x),yπ1(x)),…,(xπk(x),yπk(x)))h_S(x) = \varphi\big((x_{\pi_1(x)}, y_{\pi_1(x)}), \dots, (x_{\pi_k(x)}, y_{\pi_k(x)})\big)hS​(x)=φ((xπ1​(x)​,yπ1​(x)​),…,(xπk​(x)​,yπk​(x)​)) (19.1).

A distribution DDD over X×YX \times YX×Y has marginal DXD_XDX​ and conditional probability η(x)=P[y=1∣x]\eta(x) = P[y = 1 \mid x]η(x)=P[y=1∣x]; the Bayes optimal rule is h⋆(x)=1[η(x)>1/2]h^\star(x) = \mathbb{1}[\eta(x) > 1/2]h⋆(x)=1[η(x)>1/2], and the standing assumption is that η\etaη is ccc-Lipschitz: ∣η(x)−η(x′)∣≤c∥x−x′∥|\eta(x) - \eta(x')| \le c\|x - x'\|∣η(x)−η(x′)∣≤c∥x−x′∥. In the formalization a distribution with conditional probability η\etaη is written condLaw DX η: draw x∼DXx \sim D_Xx∼DX​, then y∼Bernoulli(η(x))y \sim \mathrm{Bernoulli}(\eta(x))y∼Bernoulli(η(x)). Every distribution with a regression function is of this form, so nothing is lost.

Formalization targets

Goal: Theorem 19.3

For X=[0,1]dX = [0,1]^dX=[0,1]d, Y={0,1}Y = \{0,1\}Y={0,1}, a distribution DDD over X×YX \times YX×Y whose conditional probability η\etaη is ccc-Lipschitz, and hSh_ShS​ the result of the 1-NN rule on S∼DmS \sim D^mS∼Dm,

ES∼Dm[LD(hS)]≤2LD(h⋆)+4cd m−1d+1.\mathbb{E}_{S \sim D^m}[L_D(h_S)] \le 2L_D(h^\star) + 4c\sqrt d\, m^{-\frac{1}{d+1}}.ES∼Dm​[LD​(hS​)]≤2LD​(h⋆)+4cd​m−d+11​.

Milestones

Lemma 19.1 (the Lipschitz reduction: ES[LD(hS)]≤2LD(h⋆)+c ES,x∥x−xπ1(x)∥\mathbb{E}_S[L_D(h_S)] \le 2L_D(h^\star) + c\,\mathbb{E}_{S,x}\|x - x_{\pi_1(x)}\|ES​[LD​(hS​)]≤2LD​(h⋆)+cES,x​∥x−xπ1​(x)​∥); Lemma 19.2 (the expected mass of the sets among C1,…,CrC_1, \dots, C_rC1​,…,Cr​ missed by an i.i.d. sample of size mmm is at most r/(me)r/(me)r/(me)); Theorem 19.4 (for integer c≥2c \ge 2c≥2 and every learning rule there is a distribution with ccc-Lipschitz η\etaη and Bayes error 000 on which the rule's expected error is at least 1/41/41/4 whenever 2m≤(c+1)d2m \le (c+1)^d2m≤(c+1)d); Lemma 19.7 (the majority of k≥10k \ge 10k≥10 independent Bernoulli labels errs, against a label drawn from their mean ppp, at most (1+8/k)(1 + \sqrt{8/k})(1+8/k​) times as often as 1[p>1/2]\mathbb{1}[p > 1/2]1[p>1/2]); Theorem 19.5 (the kkk-NN bound ES[LD(hS)]≤(1+8/k)LD(h⋆)+(6cd+k)m−1/(d+1)\mathbb{E}_S[L_D(h_S)] \le (1 + \sqrt{8/k})L_D(h^\star) + (6c\sqrt d + k)m^{-1/(d+1)}ES​[LD​(hS​)]≤(1+8/k​)LD​(h⋆)+(6cd​+k)m−1/(d+1)). Lemma 19.6, the kkk-fold version of Lemma 19.2 with bound 2rk/m2rk/m2rk/m, is a further item.

Significance

Theorem 19.3 is the book's answer to the question it raised in §7.4: consistency results say that the 1-NN error converges to twice the Bayes error, but not how fast, and the rate necessarily depends on the distribution. The Lipschitz constant ccc and the dimension ddd are exactly the prior knowledge the rule relies on, and Theorem 19.4 shows through the No-Free-Lunch theorem that a sample of size exponential in ddd is genuinely required for some distributions in the class. Theorem 19.5 quantifies what larger kkk buys, the factor 222 improving to 1+8/k1 + \sqrt{8/k}1+8/k​, at the price of the additive term growing linearly in kkk. On the platform, this mission introduces the conditional-probability model of a distribution over X×{0,1}X \times \{0,1\}X×{0,1} and the Bayes rule, which Chapters 24 (generative models) and the nonparametric parts of the book use again, and the box-cover argument of Lemma 19.2, a small combinatorial-probability tool of independent use.

Difficulty

Lemma 19.1 is a computation once the expectation over SSS and (x,y)(x, y)(x,y) is decomposed as the book does: sample the unlabeled points first, find the nearest neighbor, then draw the two labels; the identity P[y≠y′]=2η(x)(1−η(x))+(η(x)−η(x′))(2η(x)−1)P[y \ne y'] = 2\eta(x)(1 - \eta(x)) + (\eta(x) - \eta(x'))(2\eta(x) - 1)P[y=y′]=2η(x)(1−η(x))+(η(x)−η(x′))(2η(x)−1) and LD(h⋆)=Exmin⁡{η,1−η}≥Ex η(1−η)L_D(h^\star) = \mathbb{E}_x\min\{\eta, 1 - \eta\} \ge \mathbb{E}_x\,\eta(1 - \eta)LD​(h⋆)=Ex​min{η,1−η}≥Ex​η(1−η) finish it. Formally the work is in the decomposition itself, which is Fubini for condLaw and the product law, and in the measurability of the rule, which the statement assumes. Lemma 19.2 is E[1[Ci∩S=∅]]=(1−P[Ci])m≤e−P[Ci]m\mathbb{E}[\mathbb{1}[C_i \cap S = \emptyset]] = (1 - P[C_i])^m \le e^{-P[C_i]m}E[1[Ci​∩S=∅]]=(1−P[Ci​])m≤e−P[Ci​]m and max⁡aae−ma≤1/(me)\max_a ae^{-ma} \le 1/(me)maxa​ae−ma≤1/(me). Theorem 19.3 covers the cube by boxes of side ε\varepsilonε, applies Lemma 19.2 to the boxes and sets ε=2m−1/(d+1)\varepsilon = 2m^{-1/(d+1)}ε=2m−1/(d+1); a formal proof must handle 1/ε1/\varepsilon1/ε not being an integer (take T=⌈1/ε⌉T = \lceil 1/\varepsilon \rceilT=⌈1/ε⌉ boxes per side, so r≤(2/ε)dr \le (2/\varepsilon)^dr≤(2/ε)d when ε≤1\varepsilon \le 1ε≤1, which is what the book's 2dε−d2^d\varepsilon^{-d}2dε−d already allows for) and the regime m<2d+1m < 2^{d+1}m<2d+1, where the trivial bound E∥x−xπ1(x)∥≤d\mathbb{E}\|x - x_{\pi_1(x)}\| \le \sqrt dE∥x−xπ1​(x)​∥≤d​ suffices. Theorem 19.4 is the No-Free-Lunch theorem on the grid of spacing 1/c1/c1/c, plus the observation that any {0,1}\{0,1\}{0,1}-valued function on the grid extends to a ccc-Lipschitz [0,1][0,1][0,1]-valued function on the cube (McShane). Lemma 19.6 is Chernoff's bound below the mean; Lemma 19.7 is the delicate one: Chernoff with the function h(a)=(1+a)log⁡(1+a)−ah(a) = (1 + a)\log(1 + a) - ah(a)=(1+a)log(1+a)−a and the inequality (1−2p)e−kp+k2(log⁡(2p)+1)≤8/k p(1 - 2p)e^{-kp + \frac k2(\log(2p) + 1)} \le \sqrt{8/k}\,p(1−2p)e−kp+2k​(log(2p)+1)≤8/k​p for p∈[0,1/2]p \in [0, 1/2]p∈[0,1/2], k≥10k \ge 10k≥10, which the book states without proof. Theorem 19.5 assembles Lemmas 19.6 and 19.7 along the four steps of Exercise 4; to reach the book's constants with an integer number of boxes one takes T=⌈m1/(d+1)/2.07⌉T = \lceil m^{1/(d+1)}/2.07 \rceilT=⌈m1/(d+1)/2.07⌉ boxes per side and Chernoff at δ=1/3\delta = 1/3δ=1/3 in Lemma 19.6, or notes that the bound is trivial unless m1/(d+1)>6cd+km^{1/(d+1)} > 6c\sqrt d + km1/(d+1)>6cd​+k.

Formalization scope

Labels are Bool; bernoulliLaw p is the Bernoulli law on Bool, condLaw DX η the distribution with marginal DX and conditional probability η, and bayesRule η the Bayes rule. The cube is the subtype cube d of EuclideanSpace ℝ (Fin d), so its metric is Euclidean and its Borel structure is inherited; the Lipschitz hypothesis is LipschitzWith c η with c : ℝ≥0, together with η x ∈ [0,1] (a conditional probability). A kkk-NN rule is a learner h with IsKNNRuleWith k φ h: for every sample of size m≥km \ge km≥k and every xxx there is some reordering of the sample by distance to xxx whose first kkk entries feed φ\varphiφ; ties are therefore broken arbitrarily, and the theorems hold for every choice. Majority votes predict 111 iff strictly more than half of the kkk labels are 111, the book's 1[p′>1/2]\mathbb{1}[p' > 1/2]1[p′>1/2] of Lemma 19.7. The nearest-neighbor distance is nnDist S x = ⨅ i, dist x (S i).1. Expectations over S∼DmS \sim D^mS∼Dm are Bochner integrals against iidLaw D m (Mission I), and the expectation statements assume the rule is measurable in (S,x)(S, x)(S,x), the book's Remark 3.1; without it the integrals would be junk. Lemmas 19.2 and 19.6 are stated for arbitrary measurable subsets of an arbitrary measurable space, as in the book, with m≥1m \ge 1m≥1 (for m=0m = 0m=0 the left side is ∑iP[Ci]\sum_i P[C_i]∑i​P[Ci​] while Lean reads r/(0⋅e)r/(0 \cdot e)r/(0⋅e) as 000). Lemma 19.7 uses the product of Bernoulli laws on Fin k → Bool.

Two statements are given as their proofs support them, and the deviations are recorded in the item texts. Theorem 19.4 takes c≥2c \ge 2c≥2 an integer (the grid has spacing 1/c1/c1/c), fixes mmm with 2m≤(c+1)d2m \le (c+1)^d2m≤(c+1)d before choosing the distribution (Theorem 5.1 produces a distribution per mmm), and concludes that the expected true error is at least 1/41/41/4 (Equation (5.2) in the proof of Theorem 5.1; the book's "greater than 1/41/41/4" is what its proof gives for 2m<(c+1)d2m < (c+1)^d2m<(c+1)d only in the form of that expectation). Theorem 19.5 keeps the book's constants; the drafter checked that they are reachable with an integer number of boxes. Not stated: the general weighted-average rules of §19.1 beyond (19.1), the efficient implementation of §19.3, Exercise 3 (a one-line inequality, absorbed into the proof of Theorem 19.5).

Selected references

  • S. Shalev-Shwartz, S. Ben-David, Understanding Machine Learning: From Theory to Algorithms, Cambridge University Press, 2014, Chapter 19. doi:10.1017/CBO9781107298019
  • T. Cover, P. Hart, Nearest neighbor pattern classification, IEEE Transactions on Information Theory 13(1), 1967. doi:10.1109/TIT.1967.1053964
  • C. J. Stone, Consistent nonparametric regression, Annals of Statistics 5(4), 1977. doi:10.1214/aos/1176343886
  • L. Devroye, L. Györfi, G. Lugosi, A Probabilistic Theory of Pattern Recognition, Springer, 1996. doi:10.1007/978-1-4612-0711-5
  • L.-A. Gottlieb, A. Kontorovich, R. Krauthgamer, Efficient classification for metric data, COLT 2010; IEEE Transactions on Information Theory 60(9), 2014. doi:10.1109/TIT.2014.2339840
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Understanding Machine Learning XIII: Multiclass Prediction and RankingTextbook

Motivation

Binary classification is the exception in practice; most prediction tasks have many labels, a structured label space, or ask for a ranking. Chapter 17 of Shalev-Shwartz and Ben-David, Understanding Machine Learning: From Theory to Algorithms (doi:10.1017/CBO9781107298019) extends linear predictors to these settings through one idea: a class-sensitive feature mapping Ψ(x,y)\Psi(x, y)Ψ(x,y) that scores a candidate label, with the prediction hw(x)=argmax⁡y⟨w,Ψ(x,y)⟩h_w(x) = \operatorname{argmax}_y \langle w, \Psi(x, y)\ranglehw​(x)=argmaxy​⟨w,Ψ(x,y)⟩. A cost-sensitive loss Δ(y′,y)\Delta(y', y)Δ(y′,y) replaces the 0–1 loss, and the generalized hinge loss (17.3), max⁡y′(Δ(y′,y)+⟨w,Ψ(x,y′)−Ψ(x,y)⟩)\max_{y'}(\Delta(y', y) + \langle w, \Psi(x, y') - \Psi(x, y)\rangle)maxy′​(Δ(y′,y)+⟨w,Ψ(x,y′)−Ψ(x,y)⟩), is its convex surrogate: it upper bounds Δ(hw(x),y)\Delta(h_w(x), y)Δ(hw​(x),y), is tight under margin, and is convex and Lipschitz in www. Multiclass SVM is then regularized loss minimization for this loss, and Corollaries 17.1 and 17.2 transfer the guarantees of Chapters 13 and 14 with no dependence on the number of labels. The same construction handles ranking: a linear ranking predictor scores each item, the Kendall tau loss has a pairwise hinge surrogate, and the NDCG surrogate reduces to an assignment problem whose linear relaxation is exact by the Birkhoff–von Neumann theorem (Claim 17.3, Lemma 17.4).

Setting

Labels form a finite nonempty type YYY; the feature mapping takes values in Rd\mathbb{R}^dRd as in Mission VI, and the RLM rule and the SGD of Chapters 13 and 14 are those of Missions IX and X. An argmax predictor for (Ψ,w)(\Psi, w)(Ψ,w) is any hhh with h(x)h(x)h(x) maximizing ⟨w,Ψ(x,y)⟩\langle w, \Psi(x, y)\rangle⟨w,Ψ(x,y)⟩; a canonical one is fixed by choosing among the maximizers, and likewise a canonical maximizer y^\hat yy^​ in the generalized hinge loss, which gives the SGD direction Ψ(x,y^)−Ψ(x,y)\Psi(x, \hat y) - \Psi(x, y)Ψ(x,y^​)−Ψ(x,y). The cost Δ\DeltaΔ is nonnegative with Δ(y,y)=0\Delta(y, y) = 0Δ(y,y)=0. For ranking, an example is a list x1,…,xrx_1, \dots, x_rx1​,…,xr​ of instances with a score vector y∈Rry \in \mathbb{R}^ry∈Rr; the linear predictor is (⟨w,xi⟩)i(\langle w, x_i\rangle)_i(⟨w,xi​⟩)i​, the Kendall tau loss is the fraction of pairs ordered differently, using the three-valued real sign, and permutations of [r][r][r] are Mathlib's permutations of Fin r, with doubly stochastic and permutation matrices from Mathlib.

Formalization targets

Goal: Corollary 17.1

For DDD over X×YX \times YX×Y, ∥Ψ(x,y)∥≤ρ/2\|\Psi(x, y)\| \le \rho/2∥Ψ(x,y)∥≤ρ/2, B>0B > 0B>0, and the Multiclass SVM learner with λ=2ρ2/(B2m)\lambda = \sqrt{2\rho^2/(B^2 m)}λ=2ρ2/(B2m)​: ES[LDΔ(hw)]≤ES[LDg-hinge(w)]\mathbb{E}_S[L^\Delta_D(h_w)] \le \mathbb{E}_S[L^{g\text{-}hinge}_D(w)]ES​[LDΔ​(hw​)]≤ES​[LDg-hinge​(w)], and for every uuu with ∥u∥≤B\|u\| \le B∥u∥≤B, ES[LDg-hinge(w)]≤LDg-hinge(u)+8ρ2B2/m\mathbb{E}_S[L^{g\text{-}hinge}_D(w)] \le L^{g\text{-}hinge}_D(u) + \sqrt{8\rho^2B^2/m}ES​[LDg-hinge​(w)]≤LDg-hinge​(u)+8ρ2B2/m​.

Milestones

Equation (17.3). The generalized hinge loss bounds Δ(hw(x),y)\Delta(h_w(x), y)Δ(hw​(x),y) for every argmax predictor, equals it under the margin condition, and is convex and ρ\rhoρ-Lipschitz in www with ρ=max⁡y′∥Ψ(x,y′)−Ψ(x,y)∥\rho = \max_{y'}\|\Psi(x, y') - \Psi(x, y)\|ρ=maxy′​∥Ψ(x,y′)−Ψ(x,y)∥.

Corollary 17.2. SGD for multiclass learning with T≥B2ρ2/ϵ2T \ge B^2\rho^2/\epsilon^2T≥B2ρ2/ϵ2 examples has E[LDΔ(hwˉ)]≤E[LDg-hinge(wˉ)]≤LDg-hinge(u)+ϵ\mathbb{E}[L^\Delta_D(h_{\bar w})] \le \mathbb{E}[L^{g\text{-}hinge}_D(\bar w)] \le L^{g\text{-}hinge}_D(u) + \epsilonE[LDΔ​(hwˉ​)]≤E[LDg-hinge​(wˉ)]≤LDg-hinge​(u)+ϵ for every ∥u∥≤B\|u\| \le B∥u∥≤B.

Equation (17.7). The permutation induced by sorting yyy maximizes ∑iviyi\sum_i v_i y_i∑i​vi​yi​ over permutation vectors (the rearrangement inequality).

Claim 17.3. The doubly stochastic matrices are the convex hull of the permutation matrices.

Lemma 17.4. The assignment LP over doubly stochastic matrices has an optimal solution that is a permutation matrix.

Further items: Remark 17.2 (the binary case recovers the hinge loss) and the Kendall tau surrogate of §17.4.1 with its convexity and Lipschitz constant.

Significance

The generalized hinge loss is the device that lets the whole convex-learning machinery of Part II run on arbitrary finite label sets and on structured outputs, and Remark 17.3's observation that the bounds of Corollaries 17.1 and 17.2 do not depend on ∣Y∣|Y|∣Y∣ is what makes structured prediction (§17.3) and ranking with exponentially many labelings feasible. The ranking half of the chapter shows the pattern at work: the induced permutation is an argmax over a combinatorial set (17.7), so the NDCG loss admits a generalized hinge surrogate, and its subgradient is an assignment problem, solvable by the Hungarian method or, thanks to Birkhoff–von Neumann, by linear programming.

Nothing here is machine-checked except that Mathlib contains the Birkhoff–von Neumann theorem, which the corresponding item restates in the book's form. The statements are faithful with the clarifications that ties are broken canonically, that the Kendall tau surrogate is stated for tie-free score vectors (the book's rewriting of the pairwise indicator assumes sign⁡(yi−yj)≠0\operatorname{sign}(y_i - y_j) \ne 0sign(yi​−yj​)=0), and that Corollary 17.1 is stated with the measurability conventions of Mission IX.

Difficulty

Remark 17.2 is a two-element maximum and the entry point, and Equation (17.7) is Mathlib's rearrangement inequality for monovarying functions. The properties of the generalized hinge loss are elementary: the bound by choosing y′=hw(x)y' = h_w(x)y′=hw​(x), the equality by showing every term is at most 000 and the term y′=yy' = yy′=y is 000, convexity as a maximum of affine functions, and the Lipschitz bound by Cauchy–Schwarz on each term. Corollary 17.1 is Mission IX's Corollary 13.9 for the generalized hinge loss, which requires verifying convexity, the ρ\rhoρ-Lipschitz property from ∥Ψ∥≤ρ/2\|\Psi\| \le \rho/2∥Ψ∥≤ρ/2, nonnegativity and boundedness at the origin (by max⁡Δ\max\DeltamaxΔ, finite), the measurability of the loss and of the canonical argmax predictor as functions of (w,x)(w, x)(w,x), and the pointwise comparison with the Δ\DeltaΔ-loss; Corollary 17.2 is the same with Mission X's Corollary 14.12 and Claim 14.6 for the subgradient. The Kendall tau surrogate is the pairwise hinge bound under no ties, plus the convexity and Lipschitz constant of an average of hinge terms. Lemma 17.4 follows from Birkhoff–von Neumann by the averaging argument of the book, or directly from the finiteness of the permutation matrices together with the fact that a linear function on a convex hull is minimized at an extreme point.

Formalization scope

The label set is finite, so maxima over YYY are attained and the losses are well defined; maximizers are chosen canonically, and every statement about argmax predictors holds for any choice. The multivector and TF-IDF constructions of §17.2.1, the reductions of §17.1, structured output prediction (§17.3), the NDCG loss and its surrogate (17.8), and bipartite ranking (§17.5) are not stated; the NDCG construction would need the sorting permutation and the discount function and is left for a later revision. Exercises are not stated except 17.4 through Equation (17.7).

Trivializing readings are excluded: the Δ\DeltaΔ-risk in Corollaries 17.1 and 17.2 is that of a genuine argmax predictor, the Lipschitz constants are the book's, and the assignment lemma asserts optimality against every doubly stochastic matrix. Welcome contributions: the Lipschitz constant of a maximum of affine functions, the measurability of a canonical argmax over a finite label set, and the extreme-point argument of Lemma 17.4.

Selected references

  • S. Shalev-Shwartz, S. Ben-David, Understanding Machine Learning: From Theory to Algorithms, Cambridge University Press, 2014, Chapter 17. doi:10.1017/CBO9781107298019
  • K. Crammer, Y. Singer, On the algorithmic implementation of multiclass kernel-based vector machines, Journal of Machine Learning Research 2, 2001.
  • I. Tsochantaridis, T. Joachims, T. Hofmann, Y. Altun, Large margin methods for structured and interdependent output variables, Journal of Machine Learning Research 6, 2005.
  • G. Birkhoff, Tres observaciones sobre el algebra lineal, Universidad Nacional de Tucumán, Revista A 5, 1946.
  • H. W. Kuhn, The Hungarian method for the assignment problem, Naval Research Logistics Quarterly 2, 1955. doi:10.1002/nav.3800020109
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Machine LearningOptimization·Captain: naimengye

Understanding Machine Learning XII: Kernel Methods and the Representer TheoremTextbook

Motivation

Chapter 15 bounded the sample complexity of large-margin halfspaces by the norms of the data and of the separator, independently of the dimension. Chapter 16 of Shalev-Shwartz and Ben-David, Understanding Machine Learning: From Theory to Algorithms (doi:10.1017/CBO9781107298019) removes the remaining obstacle to using halfspaces in very high-dimensional feature spaces: computation. After embedding the data by a feature map ψ\psiψ into a Hilbert space, every SVM-like problem has the form min⁡wf(⟨w,ψ(x1)⟩,…,⟨w,ψ(xm)⟩)+R(∥w∥)\min_w f(\langle w, \psi(x_1)\rangle, \dots, \langle w, \psi(x_m)\rangle) + R(\|w\|)minw​f(⟨w,ψ(x1​)⟩,…,⟨w,ψ(xm​)⟩)+R(∥w∥) (16.2), and the representer theorem (Theorem 16.1) says that an optimal solution lies in the span of the mapped examples. Consequently the problem can be rewritten in terms of the mmm coefficients and the kernel K(x,x′)=⟨ψ(x),ψ(x′)⟩K(x, x') = \langle\psi(x), \psi(x')\rangleK(x,x′)=⟨ψ(x),ψ(x′)⟩ alone (16.3): this is the kernel trick. The chapter exhibits the polynomial and Gaussian kernels (Examples 16.1 and 16.2), characterizes the functions that are kernels as the positive semidefinite ones (Lemma 16.2), and shows that the SGD solver for Soft-SVM of §15.5 can be run entirely on kernel evaluations (Lemma 16.3).

Setting

A feature map ψ:X→F\psi : X \to Fψ:X→F takes values in a real Hilbert space, a complete real inner product space; its kernel is K(x,x′)=⟨ψ(x),ψ(x′)⟩K(x, x') = \langle\psi(x), \psi(x')\rangleK(x,x′)=⟨ψ(x),ψ(x′)⟩, and a function KKK implements an inner product in some Hilbert space if it is the kernel of some feature map into some Hilbert space, quantified existentially in the universe of the domain. The Gram matrix of a sample is Gij=K(xi,xj)G_{ij} = K(x_i, x_j)Gij​=K(xi​,xj​). The general objective (16.2) is f(⟨w,ψ(x1)⟩,…,⟨w,ψ(xm)⟩)+R(∥w∥)f(\langle w, \psi(x_1)\rangle, \dots, \langle w, \psi(x_m)\rangle) + R(\|w\|)f(⟨w,ψ(x1​)⟩,…,⟨w,ψ(xm​)⟩)+R(∥w∥) with fff arbitrary and RRR nondecreasing on [0,∞)[0, \infty)[0,∞). The SGD procedure of §15.5 in the feature space keeps θ(t)\theta^{(t)}θ(t) with w(t)=θ(t)/(λ(t+1))w^{(t)} = \theta^{(t)}/(\lambda(t+1))w(t)=θ(t)/(λ(t+1)) (iterates indexed from 000) and, at each step, for the chosen index iii, adds yiψ(xi)y_i\psi(x_i)yi​ψ(xi​) to θ\thetaθ when yi⟨w(t),ψ(xi)⟩<1y_i\langle w^{(t)}, \psi(x_i)\rangle < 1yi​⟨w(t),ψ(xi​)⟩<1; its kernelized version keeps coefficients β(t)\beta^{(t)}β(t) with α(t)=β(t)/(λ(t+1))\alpha^{(t)} = \beta^{(t)}/(\lambda(t+1))α(t)=β(t)/(λ(t+1)) and tests yi∑jαj(t)K(xj,xi)<1y_i\sum_j\alpha^{(t)}_j K(x_j, x_i) < 1yi​∑j​αj(t)​K(xj​,xi​)<1. Both are driven by the same sequence of chosen indices, which stands for the uniformly random choices of the book.

Formalization targets

Goal: Theorem 16.1 (Representer Theorem)

If RRR is nondecreasing on [0,∞)[0,\infty)[0,∞) and the problem (16.2) has an optimal solution, then there is α∈Rm\alpha \in \mathbb{R}^mα∈Rm such that ∑iαiψ(xi)\sum_i \alpha_i\psi(x_i)∑i​αi​ψ(xi​) is an optimal solution.

Milestones

Equation (16.3). For w=∑jαjψ(xj)w = \sum_j\alpha_j\psi(x_j)w=∑j​αj​ψ(xj​) the objective equals f(∑jαjK(xj,x1),…)+R(∑i,jαiαjK(xj,xi))f\big(\sum_j\alpha_jK(x_j, x_1), \dots\big) + R\big(\sqrt{\sum_{i,j}\alpha_i\alpha_jK(x_j, x_i)}\big)f(∑j​αj​K(xj​,x1​),…)+R(∑i,j​αi​αj​K(xj​,xi​)​).

Example 16.1. The polynomial kernel (1+⟨x,x′⟩)k(1 + \langle x, x'\rangle)^k(1+⟨x,x′⟩)k on Rn\mathbb{R}^nRn is ⟨ψ(x),ψ(x′)⟩\langle\psi(x), \psi(x')\rangle⟨ψ(x),ψ(x′)⟩ for the monomial map into R(n+1)k\mathbb{R}^{(n+1)^k}R(n+1)k.

Example 16.2. On R\mathbb{R}R, the map ψ(x)n=e−x2/2xn/n!\psi(x)_n = e^{-x^2/2}x^n/\sqrt{n!}ψ(x)n​=e−x2/2xn/n!​ into ℓ2\ell^2ℓ2 has ⟨ψ(x),ψ(x′)⟩=e−(x−x′)2/2\langle\psi(x), \psi(x')\rangle = e^{-(x-x')^2/2}⟨ψ(x),ψ(x′)⟩=e−(x−x′)2/2; the Gaussian kernel e−∥x−x′∥2/(2σ)e^{-\|x-x'\|^2/(2\sigma)}e−∥x−x′∥2/(2σ) on Rn\mathbb{R}^nRn is a kernel for every σ>0\sigma > 0σ>0.

Lemma 16.2. A symmetric KKK is a kernel iff all its Gram matrices are positive semidefinite.

Lemma 16.3. The kernelized SGD reproduces the feature-space SGD: θ(t)=∑jβj(t)ψ(xj)\theta^{(t)} = \sum_j\beta^{(t)}_j\psi(x_j)θ(t)=∑j​βj(t)​ψ(xj​) for all ttt, hence the outputs coincide.

Further items: Exercise 16.3 (kernel ridge regression: minimizers of the coefficient objective give minimizers of the ridge objective, and (2λmI+G)α=y(2\lambda mI + G)\alpha = y(2λmI+G)α=y gives one), Exercise 16.4 (min⁡{x,x′}\min\{x, x'\}min{x,x′} is a kernel), Exercise 16.6 (the nearest-class-mean rule is a halfspace).

Significance

The representer theorem is the reason kernel methods exist: it reduces an optimization over an arbitrary Hilbert space to one over Rm\mathbb{R}^mRm, and Lemma 16.2 says the reduction needs nothing but a positive semidefinite similarity function, so one may design the kernel directly, as in the string example of §16.2.1. Lemma 16.3 makes the connection to Chapter 14 concrete: a first-order method never leaves the span of the examples, so it too can be run on the Gram matrix. Together with Chapter 15, the chapter closes the book's treatment of linear predictors: expressive through the embedding, statistically controlled through the margin, and computable through the kernel.

Nothing here is machine-checked. The statements are faithful to the book with two clarifications: the representer theorem assumes the existence of an optimal solution, which the book's proof also assumes, and the kernel-SGD equivalence is stated for a fixed sequence of chosen indices, which is the content of the book's inductive proof.

Difficulty

Equation (16.3) and Exercise 16.6 are inner-product algebra and the entry points. The representer theorem needs the orthogonal decomposition w⋆=∑iαiψ(xi)+uw^\star = \sum_i\alpha_i\psi(x_i) + uw⋆=∑i​αi​ψ(xi​)+u with uuu orthogonal to the span, which is available in Mathlib for the finite-dimensional, hence complete, subspace spanned by the ψ(xi)\psi(x_i)ψ(xi​), together with the Pythagorean identity and the monotonicity of RRR. Example 16.1 is the multinomial expansion of (1+⟨x,x′⟩)k(1 + \langle x, x'\rangle)^k(1+⟨x,x′⟩)k as a sum over index vectors, packaged as an inner product in the Euclidean space indexed by {0,…,n}k\{0, \dots, n\}^k{0,…,n}k. Example 16.2 needs the summability of xn(x′)n/n!x^n(x')^n/n!xn(x′)n/n! and the exponential series, and, for the general Gaussian kernel, either an explicit construction or Lemma 16.2 together with the positive semidefiniteness of the Gaussian Gram matrix. Lemma 16.2 in the nontrivial direction is the construction of the reproducing kernel Hilbert space: the pre-Hilbert space of finite combinations of the functions K(⋅,x)K(\cdot, x)K(⋅,x), the inner product defined through KKK, its well-definedness and positive definiteness from the Gram matrices, and the completion, which Mathlib provides for inner product spaces. Lemma 16.3 is an induction on ttt with the identity ⟨w(t),ψ(xi)⟩=∑jαj(t)K(xj,xi)\langle w^{(t)}, \psi(x_i)\rangle = \sum_j\alpha^{(t)}_jK(x_j, x_i)⟨w(t),ψ(xi​)⟩=∑j​αj(t)​K(xj​,xi​). Exercise 16.3 combines the representer theorem with the identity between the two objectives on the span and the first-order condition for a convex quadratic; Exercise 16.4 needs a feature map such as ψ(x)=(1[1≤j≤x])j\psi(x) = (\mathbb{1}[1 \le j \le x])_jψ(x)=(1[1≤j≤x])j​, or the positive semidefiniteness of the min matrix.

Formalization scope

Hilbert spaces are real, complete inner product spaces; the existential in IsKernel ranges over Hilbert spaces in the universe of the domain, which the reproducing kernel construction respects. The objective (16.2) has real-valued fff, so the hard-SVM instance with f∈{0,∞}f \in \{0, \infty\}f∈{0,∞} is not covered by the representer item as stated. The SGD procedures are deterministic given the index sequence; the random choice of indices is not modelled, exactly as in Lemma 16.3's proof. The string kernel of §16.2.1 and Exercise 16.1, the kernelized Perceptron (Exercise 16.2), Exercise 16.5 and part (2) of Exercise 16.6 are not stated.

Trivializing readings are excluded: the representer theorem asserts optimality against every www, Lemma 16.2 is a biconditional with symmetry assumed as the book does, and the kernels of the examples are exhibited with explicit feature spaces where the book gives them. Welcome contributions: the orthogonal decomposition against a finite span, the multinomial identity of Example 16.1, and the reproducing kernel Hilbert space construction behind Lemma 16.2.

Selected references

  • S. Shalev-Shwartz, S. Ben-David, Understanding Machine Learning: From Theory to Algorithms, Cambridge University Press, 2014, Chapter 16. doi:10.1017/CBO9781107298019
  • B. Schölkopf, R. Herbrich, A. J. Smola, A generalized representer theorem, Proceedings of COLT, 2001. doi:10.1007/3-540-44581-1_27
  • N. Aronszajn, Theory of reproducing kernels, Transactions of the American Mathematical Society 68(3), 1950. doi:10.1090/S0002-9947-1950-0051437-7
  • B. Schölkopf, A. J. Smola, Learning with Kernels, MIT Press, 2002.
  • M. A. Aizerman, E. M. Braverman, L. I. Rozonoer, Theoretical foundations of the potential function method in pattern recognition learning, Automation and Remote Control 25, 1964.
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Machine LearningOptimizationStatistics·Captain: naimengye

Understanding Machine Learning XI: Support Vector Machines and MarginTextbook

Motivation

The sample complexity of learning halfspaces in Rd\mathbb{R}^dRd grows with ddd, which is bad news when features are many or infinite. Chapter 15 of Shalev-Shwartz and Ben-David, Understanding Machine Learning: From Theory to Algorithms (doi:10.1017/CBO9781107298019) introduces the support vector machine, the learning rule that replaces dimension by geometry. Among the halfspaces separating a sample, Hard-SVM picks the one of largest margin, the distance from the hyperplane to the nearest example (Claim 15.1, Lemma 15.2); if the data are separable with margin γ\gammaγ and lie in a ball of radius ρ\rhoρ, the resulting classifier has error O(ρ/(γm))O(\rho/(\gamma\sqrt m))O(ρ/(γm​)) whatever the dimension (Theorem 15.4), and the Perceptron of Chapter 9 makes at most (ρ/γ)2(\rho/\gamma)^2(ρ/γ)2 updates (Remark 15.1). Soft-SVM drops separability by allowing slack variables, and Claim 15.5 identifies it with regularized hinge-loss minimization, so that the stability theory of Chapter 13 applies: the hinge loss is ∥x∥\|x\|∥x∥-Lipschitz (Claim 15.6), and Corollary 15.7 gives an expected-risk bound depending only on the norms of the data and of the comparison halfspace. The chapter closes with the optimality conditions that explain the name: the Hard-SVM solution is a combination of the examples on the margin (Theorem 15.8, via the Fritz John conditions, Lemma 15.9).

Setting

Vectors live in Rd\mathbb{R}^dRd as in Mission VI; labels are real numbers, with y∈{±1}y \in \{\pm 1\}y∈{±1} as a hypothesis wherever the book needs it. A sample is linearly separable if some halfspace (w,b)(w, b)(w,b) has yi(⟨w,xi⟩+b)>0y_i(\langle w, x_i\rangle + b) > 0yi​(⟨w,xi​⟩+b)>0 for all iii, and the margin of (w,b)(w, b)(w,b) on the sample is min⁡iyi(⟨w,xi⟩+b)\min_i y_i(\langle w, x_i\rangle + b)mini​yi​(⟨w,xi​⟩+b). Hard-SVM solutions are minimizers of ∥w∥\|w\|∥w∥ subject to yi(⟨w,xi⟩+b)≥1y_i(\langle w, x_i\rangle + b) \ge 1yi​(⟨w,xi​⟩+b)≥1, formalized as a relation; the minimizer is unique whenever the constraints are feasible, and the homogenous version sets b=0b = 0b=0. A distribution over Rd×{±1}\mathbb{R}^d \times \{\pm 1\}Rd×{±1} is separable with a (γ,ρ)(\gamma, \rho)(γ,ρ)-margin if some unit w⋆w^\starw⋆ (and b⋆b^\starb⋆) has y(⟨w⋆,x⟩+b⋆)≥γy(\langle w^\star, x\rangle + b^\star) \ge \gammay(⟨w⋆,x⟩+b⋆)≥γ and ∥x∥≤ρ\|x\| \le \rho∥x∥≤ρ almost surely. Soft-SVM is the problem λ∥w∥2+1m∑ξi\lambda\|w\|^2 + \frac1m\sum\xi_iλ∥w∥2+m1​∑ξi​ under yi(⟨w,xi⟩+b)≥1−ξiy_i(\langle w, x_i\rangle + b) \ge 1 - \xi_iyi​(⟨w,xi​⟩+b)≥1−ξi​, ξi≥0\xi_i \ge 0ξi​≥0; its homogenous form is the regularized loss minimization rule of Mission IX for the hinge loss max⁡{0,1−y⟨w,x⟩}\max\{0, 1 - y\langle w, x\rangle\}max{0,1−y⟨w,x⟩}, and the 0–1 loss is 1[y⟨w,x⟩≤0]\mathbb{1}[y\langle w, x\rangle \le 0]1[y⟨w,x⟩≤0]. Expectations over samples are integrals against DmD^mDm, with the measurability conventions of Mission IX.

Formalization targets

Goal: Corollary 15.7, last part

For DDD on {∥x∥≤ρ}×{±1}\{\|x\| \le \rho\} \times \{\pm 1\}{∥x∥≤ρ}×{±1} almost surely, B>0B > 0B>0, and the Soft-SVM learner with λ=2ρ2/(B2m)\lambda = \sqrt{2\rho^2/(B^2 m)}λ=2ρ2/(B2m)​: ES[LD0−1(A(S))]≤ES[LDhinge(A(S))]\mathbb{E}_S[L^{0-1}_D(A(S))] \le \mathbb{E}_S[L^{hinge}_D(A(S))]ES​[LD0−1​(A(S))]≤ES​[LDhinge​(A(S))], and for every www with ∥w∥≤B\|w\| \le B∥w∥≤B, ES[LDhinge(A(S))]≤LDhinge(w)+8ρ2B2/m\mathbb{E}_S[L^{hinge}_D(A(S))] \le L^{hinge}_D(w) + \sqrt{8\rho^2 B^2/m}ES​[LDhinge​(A(S))]≤LDhinge​(w)+8ρ2B2/m​.

Milestones

Claim 15.1. The distance from xxx to {v:⟨w,v⟩+b=0}\{v : \langle w, v\rangle + b = 0\}{v:⟨w,v⟩+b=0} with ∥w∥=1\|w\| = 1∥w∥=1 is ∣⟨w,x⟩+b∣|\langle w, x\rangle + b|∣⟨w,x⟩+b∣.

Lemma 15.2. For a sample with both labels present, the normalized Hard-SVM output has unit norm and margin at least that of every unit-norm halfspace.

Theorem 15.4. Under homogenous (γ,ρ)(\gamma, \rho)(γ,ρ)-separability, with probability at least 1−δ1 - \delta1−δ the 0–1 risk of the Hard-SVM output is at most 4(ρ/γ)2/m+2log⁡(2/δ)/m\sqrt{4(\rho/\gamma)^2/m} + \sqrt{2\log(2/\delta)/m}4(ρ/γ)2/m​+2log(2/δ)/m​.

Claim 15.5. Every feasible slack vector has average at least the hinge loss, and the hinge losses are feasible slacks.

Claim 15.6. For y∈{±1}y \in \{\pm 1\}y∈{±1}, w↦max⁡{0,1−y⟨w,x⟩}w \mapsto \max\{0, 1 - y\langle w, x\rangle\}w↦max{0,1−y⟨w,x⟩} is ∥x∥\|x\|∥x∥-Lipschitz.

Corollary 15.7, first parts. For every uuu, ES[LDhinge(A(S))]\mathbb{E}_S[L^{hinge}_D(A(S))]ES​[LDhinge​(A(S))] and ES[LD0−1(A(S))]\mathbb{E}_S[L^{0-1}_D(A(S))]ES​[LD0−1​(A(S))] are at most LDhinge(u)+λ∥u∥2+2ρ2/(λm)L^{hinge}_D(u) + \lambda\|u\|^2 + 2\rho^2/(\lambda m)LDhinge​(u)+λ∥u∥2+2ρ2/(λm).

Theorem 15.8. The homogenous Hard-SVM solution is ∑i∈Iαixi\sum_{i \in I}\alpha_i x_i∑i∈I​αi​xi​ with I={i:∣⟨w0,xi⟩∣=1}I = \{i : |\langle w_0, x_i\rangle| = 1\}I={i:∣⟨w0​,xi​⟩∣=1}.

Lemma 15.9. Fritz John conditions, in the correct form with a multiplier on ∇f\nabla f∇f.

Further items: Exercise 15.1 (the two Hard-SVM formulations agree) and Exercise 15.2 (the Perceptron makes at most (ρ/γ)2(\rho/\gamma)^2(ρ/γ)2 updates).

Significance

SVM is the bridge between the statistical theory of Part I and the kernel methods of Chapter 16: because the bounds of Theorem 15.4 and Corollary 15.7 involve only ρ\rhoρ, γ\gammaγ and BBB, the same algorithm can be run after an embedding into a huge or infinite-dimensional feature space, and Theorem 15.8, that the solution lies in the span of the examples, is what makes the embedding computable. Corollary 15.7 is also the first place where the abstract machinery of Chapter 13 is applied to a specific learning rule.

Nothing here is machine-checked. One correction is built in: the Fritz John lemma is stated with the multiplier α0≥0\alpha_0 \ge 0α0​≥0 on ∇f(w⋆)\nabla f(w^\star)∇f(w⋆) and nonnegative multipliers not all zero, since the printed form, with ∇f(w⋆)\nabla f(w^\star)∇f(w⋆) unweighted and α\alphaα unrestricted, fails already for f(w)=wf(w) = wf(w)=w and g1(w)=w2g_1(w) = w^2g1​(w)=w2 on the line. Theorem 15.8 is unaffected: its constraints are affine, so the multiplier on ∇f\nabla f∇f can be taken to be 111.

Difficulty

Claim 15.6 and Claim 15.5 are short inequalities and the intended entry points, and Exercise 15.2 is Theorem 9.1 of Mission VI with B≤1/γB \le 1/\gammaB≤1/γ and R≤ρR \le \rhoR≤ρ. Claim 15.1 is the book's computation with the foot of the perpendicular v=x−(⟨w,x⟩+b)wv = x - (\langle w, x\rangle + b)wv=x−(⟨w,x⟩+b)w and a Pythagorean inequality for every other point of the hyperplane, packaged as an infimum distance. Lemma 15.2 is the rescaling argument of the book, together with the observation that both labels force w0≠0w_0 \ne 0w0​=0; Exercise 15.1 needs the positivity of the optimal margin on a separable sample. Corollary 15.7 is Corollaries 13.8 and 13.9 of Mission IX for the hinge loss, whose Lipschitz constant is ∥x∥\|x\|∥x∥ only on the support of DDD, so the stability argument must be run with the almost-sure bound; the 0–1 clause is the pointwise inequality ℓ0−1≤ℓhinge\ell_{0-1} \le \ell_{hinge}ℓ0−1​≤ℓhinge​. Theorem 15.4 is the content of §26.3: Rademacher complexity of the class of norm-bounded halfspaces, the contraction lemma for the ramp loss, the observation that the Hard-SVM output has zero ramp loss on the sample and norm at most 1/γ1/\gamma1/γ, and a concentration step, all of which will be items of the Rademacher mission. Theorem 15.8 is the KKT theorem for a strictly convex quadratic with affine constraints (Slater's condition holds), and Lemma 15.9 is the general Fritz John theorem for differentiable data, whose proof goes through a separation or penalty argument; neither is in Mathlib.

Formalization scope

Hard-SVM and Soft-SVM are relations and learners, not programs; the margin is a real infimum over the sample; the ramp loss is defined but its bounds belong to Chapter 26. Theorem 15.4 is stated for any learner that returns the Hard-SVM solution whenever the sample is feasible, which is almost surely the case under the margin assumption, and bounds the failure event in outer measure. Corollary 15.7 carries the measurability conventions of Mission IX. The Fritz John lemma is stated correctly rather than as printed. The duality of §15.4, the SGD implementation of §15.5 (whose guarantee needs the trajectory bound of §14.5.3 rather than Theorem 14.11 as stated in Mission X), Exercises 15.3 and 15.4, and Remark 15.2 are not stated.

Trivializing readings are excluded: both labels must be present for the normalized Hard-SVM output, the margin assumption and the support condition are almost sure with respect to DDD, and the risks are genuine integrals. Welcome contributions: the uniqueness of the Hard-SVM minimizer, the KKT conditions for affine constraints, and the pointwise comparison of the 0–1, ramp and hinge losses.

Selected references

  • S. Shalev-Shwartz, S. Ben-David, Understanding Machine Learning: From Theory to Algorithms, Cambridge University Press, 2014, Chapter 15. doi:10.1017/CBO9781107298019
  • C. Cortes, V. Vapnik, Support-vector networks, Machine Learning 20(3), 1995. doi:10.1007/BF00994018
  • B. E. Boser, I. M. Guyon, V. N. Vapnik, A training algorithm for optimal margin classifiers, Proceedings of COLT, 1992. doi:10.1145/130385.130401
  • F. John, Extremum problems with inequalities as subsidiary conditions, in Studies and Essays Presented to R. Courant, 1948.
  • N. Cristianini, J. Shawe-Taylor, An Introduction to Support Vector Machines, Cambridge University Press, 2000. doi:10.1017/CBO9780511801389
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Machine LearningProbability·Captain: Lucas

The Principles of Deep Learning Theory II: Deep Linear Networks at InitializationTextbook

Motivation

Chapter 3 of The Principles of Deep Learning Theory by D. A. Roberts and S. Yaida (arXiv:2106.10165) is the book's first complete example of its effective-theory method. For deep linear networks at initialization, the two- and four-point correlators of the network outputs can be computed exactly at any width and depth. The resulting formulas exhibit, in the simplest setting, the phenomena that organize the rest of the book: criticality of the weight variance CW=1C_W=1CW​=1, non-Gaussianity that grows with depth, and the depth-to-width ratio ℓ/n\ell/nℓ/n as the parameter controlling deviations from the infinite-width limit. This mission formalizes §§3.1–3.3. It is the second mission in a series formalizing the book (namespace DeepLearningTheory).

Setting

A deep linear network with widths n0,n1,n2,…n_0, n_1, n_2, \dotsn0​,n1​,n2​,… (all positive) and zero biases maps an input x∈Rn0x\in\mathbb{R}^{n_0}x∈Rn0​ to preactivations

zi(0)=xi,zi(ℓ+1)=∑j=1nℓWij(ℓ+1) zj(ℓ)(i=1,…,nℓ+1),z^{(0)}_i = x_i,\qquad z^{(\ell+1)}_i = \sum_{j=1}^{n_\ell} W^{(\ell+1)}_{ij}\, z^{(\ell)}_j \quad (i=1,\dots,n_{\ell+1}),zi(0)​=xi​,zi(ℓ+1)​=j=1∑nℓ​​Wij(ℓ+1)​zj(ℓ)​(i=1,…,nℓ+1​),

(eqs. 3.1–3.2 with b(ℓ)=0b^{(\ell)}=0b(ℓ)=0). At initialization all weights Wij(ℓ)W^{(\ell)}_{ij}Wij(ℓ)​ are independent centered Gaussians with E[Wi1j1(ℓ)Wi2j2(ℓ)]=δi1i2δj1j2 CW/nℓ−1\mathbb{E}[W^{(\ell)}_{i_1j_1}W^{(\ell)}_{i_2j_2}] = \delta_{i_1i_2}\delta_{j_1j_2}\, C_W/n_{\ell-1}E[Wi1​j1​(ℓ)​Wi2​j2​(ℓ)​]=δi1​i2​​δj1​j2​​CW​/nℓ−1​ (eq. 3.4), with a layer-independent CW≥0C_W\ge0CW​≥0. For inputs xα1,xα2x_{\alpha_1}, x_{\alpha_2}xα1​​,xα2​​ let Gα1α2(0)=1n0∑jxj;α1xj;α2G^{(0)}_{\alpha_1\alpha_2} = \frac1{n_0}\sum_j x_{j;\alpha_1}x_{j;\alpha_2}Gα1​α2​(0)​=n0​1​∑j​xj;α1​​xj;α2​​ (eq. 3.9).

Formalization targets

Goal: the exact four-point correlator (eqs. 3.21, 3.25)

For every layer ℓ≥1\ell\ge1ℓ≥1, a single input xxx, and neurons i1,…,i4i_1,\dots,i_4i1​,…,i4​,

E[zi1(ℓ)zi2(ℓ)zi3(ℓ)zi4(ℓ)]=(δi1i2δi3i4+δi1i3δi2i4+δi1i4δi2i3)  CW2ℓ[∏ℓ′=1ℓ−1(1+2nℓ′)](G(0))2.\mathbb{E}\big[z^{(\ell)}_{i_1}z^{(\ell)}_{i_2}z^{(\ell)}_{i_3}z^{(\ell)}_{i_4}\big] = (\delta_{i_1i_2}\delta_{i_3i_4}+\delta_{i_1i_3}\delta_{i_2i_4}+\delta_{i_1i_4}\delta_{i_2i_3})\; C_W^{2\ell}\Big[\prod_{\ell'=1}^{\ell-1}\Big(1+\frac{2}{n_{\ell'}}\Big)\Big]\big(G^{(0)}\big)^2 .E[zi1​(ℓ)​zi2​(ℓ)​zi3​(ℓ)​zi4​(ℓ)​]=(δi1​i2​​δi3​i4​​+δi1​i3​​δi2​i4​​+δi1​i4​​δi2​i3​​)CW2ℓ​[ℓ′=1∏ℓ−1​(1+nℓ′​2​)](G(0))2.

Milestones

  1. Eq. (3.6) — the mean preactivation vanishes.
  2. Eq. (3.10) — first-layer two-point correlator E[zi1;α1(1)zi2;α2(1)]=δi1i2CWGα1α2(0)\mathbb{E}[z^{(1)}_{i_1;\alpha_1}z^{(1)}_{i_2;\alpha_2}] = \delta_{i_1i_2}C_W G^{(0)}_{\alpha_1\alpha_2}E[zi1​;α1​(1)​zi2​;α2​(1)​]=δi1​i2​​CW​Gα1​α2​(0)​.
  3. Eqs. (3.12), (3.15) — two-point correlator in layer ℓ\ellℓ: δi1i2CWℓGα1α2(0)\delta_{i_1i_2}C_W^{\ell}G^{(0)}_{\alpha_1\alpha_2}δi1​i2​​CWℓ​Gα1​α2​(0)​.
  4. Eq. (3.18) — first-layer four-point correlator.
  5. Eq. (3.20) — the layer-to-layer recursion for the four-point correlator.
  6. Eqs. (3.21)–(3.24) — the recursion G4(ℓ+1)=CW2(1+2/nℓ)G4(ℓ)G_4^{(\ell+1)} = C_W^2(1+2/n_\ell)G_4^{(\ell)}G4(ℓ+1)​=CW2​(1+2/nℓ​)G4(ℓ)​ for the coefficient of the Wick tensor structure.
  7. Eq. (3.30) — the connected four-point correlator between two distinct neurons, G4(ℓ)−(G2(ℓ))2G_4^{(\ell)} - (G_2^{(\ell)})^2G4(ℓ)​−(G2(ℓ)​)2.

Significance

The closed forms show that a deep linear network is exactly Gaussian only in the strict infinite-width limit: at criticality CW=1C_W=1CW​=1 the connected four-point correlator (3.29)–(3.30) is [∏(1+2/nℓ′)−1](G(0))2≈2(ℓ−1)n(G(0))2\big[\prod(1+2/n_{\ell'})-1\big](G^{(0)})^2 \approx \frac{2(\ell-1)}{n}(G^{(0)})^2[∏(1+2/nℓ′​)−1](G(0))2≈n2(ℓ−1)​(G(0))2 for equal widths nnn, the first appearance of the depth-to-width ratio as the book's emergent scale. The same recursive method is reused for nonlinear networks in Chapters 4–5. The results are exact computations in the book; this mission formalizes them.

Difficulty

Each correlator is an expectation of a polynomial in exponentially many Gaussian weights. The book's recursion uses that the layer-(ℓ+1)(\ell+1)(ℓ+1) weights are independent of the layer-ℓ\ellℓ preactivations, followed by Wick contraction of the two or four new weights. In Lean this requires independence of a weight family from a measurable function of the earlier layers, integrability of products of Gaussian polynomials, and careful handling of the Kronecker-delta bookkeeping in the sums (3.23).

Formalization scope

  • Widths are n : ℕ → ℕ with n 0 the input dimension; neural indices are 0,…,nℓ−10,\dots,n_\ell-10,…,nℓ​−1. Weights are a random field W : Ω → ℕ → ℕ → ℕ → ℝ on a probability space, only entries Wij(ℓ)W^{(\ell)}_{ij}Wij(ℓ)​ with ℓ≥1\ell\ge1ℓ≥1, i<nℓi<n_\elli<nℓ​, j<nℓ−1j<n_{\ell-1}j<nℓ−1​ are used.
  • IsLinearNetInit P n CW W states mutual independence of all these weights and that each has law gaussianReal 0 (CW / n (ℓ-1)).
  • linearPreact n (W ω) x ℓ i is zi(ℓ)(x)z^{(\ell)}_i(x)zi(ℓ)​(x); inputKernel (n 0) x₁ x₂ is Gα1α2(0)G^{(0)}_{\alpha_1\alpha_2}Gα1​α2​(0)​; kron and wickDelta4 are the Kronecker delta and the three-term tensor structure.
  • Widths are assumed positive where the source's formulas require it (division by nℓn_\ellnℓ​, nonempty hidden layers). Every hypothesis is satisfiable by a product of independent Gaussians.

Selected references

  • D. A. Roberts, S. Yaida (with B. Hanin), The Principles of Deep Learning Theory, Cambridge University Press, 2022, Chapter 3. arXiv:2106.10165
  • B. Hanin, M. Nica, Products of many large random matrices and gradients in deep neural networks, Commun. Math. Phys. 376 (2020). arXiv:1812.05994
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Machine LearningProbability·Captain: Lucas

The Principles of Deep Learning Theory III: Preactivation Statistics in the First Two LayersTextbook

Motivation

Chapter 4 of The Principles of Deep Learning Theory by D. A. Roberts and S. Yaida (arXiv:2106.10165) begins the analysis of general multilayer perceptrons (MLPs) with a nonlinear activation function σ\sigmaσ at initialization. The first layer is exactly Gaussian; the second layer is the first place where non-Gaussianity appears, as a connected four-point correlator suppressed by 1/n11/n_11/n1​ and governed by the four-point vertex V(2)V^{(2)}V(2). This mission formalizes §§4.1–4.2, which are exact at any width. It is the third mission in a series formalizing the book (namespace DeepLearningTheory) and reuses the definitions of Mission II (Deep Linear Networks at Initialization).

Setting

An MLP with widths n0,n1,n2,…n_0,n_1,n_2,\dotsn0​,n1​,n2​,… and activation σ:R→R\sigma:\mathbb{R}\to\mathbb{R}σ:R→R maps inputs xα∈Rn0x_\alpha\in\mathbb{R}^{n_0}xα​∈Rn0​ to preactivations

zi;α(1)=bi(1)+∑j=1n0Wij(1)xj;α,zi;α(ℓ+1)=bi(ℓ+1)+∑j=1nℓWij(ℓ+1) σ(zj;α(ℓ))z^{(1)}_{i;\alpha}=b^{(1)}_i+\sum_{j=1}^{n_0}W^{(1)}_{ij}x_{j;\alpha},\qquad z^{(\ell+1)}_{i;\alpha}=b^{(\ell+1)}_i+\sum_{j=1}^{n_\ell}W^{(\ell+1)}_{ij}\,\sigma\big(z^{(\ell)}_{j;\alpha}\big)zi;α(1)​=bi(1)​+j=1∑n0​​Wij(1)​xj;α​,zi;α(ℓ+1)​=bi(ℓ+1)​+j=1∑nℓ​​Wij(ℓ+1)​σ(zj;α(ℓ)​)

(eqs. 4.2, 4.30). At initialization all biases and weights are independent centered Gaussians with E[bi(ℓ)bj(ℓ)]=δijCb(ℓ)\mathbb{E}[b^{(\ell)}_ib^{(\ell)}_j]=\delta_{ij}C_b^{(\ell)}E[bi(ℓ)​bj(ℓ)​]=δij​Cb(ℓ)​ and E[Wi1j1(ℓ)Wi2j2(ℓ)]=δi1i2δj1j2CW(ℓ)/nℓ−1\mathbb{E}[W^{(\ell)}_{i_1j_1}W^{(\ell)}_{i_2j_2}]=\delta_{i_1i_2}\delta_{j_1j_2}C_W^{(\ell)}/n_{\ell-1}E[Wi1​j1​(ℓ)​Wi2​j2​(ℓ)​]=δi1​i2​​δj1​j2​​CW(ℓ)​/nℓ−1​ (eqs. 4.3–4.4). The first-layer metric is Gα1α2(1)=Cb(1)+CW(1)1n0∑jxj;α1xj;α2G^{(1)}_{\alpha_1\alpha_2}=C_b^{(1)}+C_W^{(1)}\frac1{n_0}\sum_jx_{j;\alpha_1}x_{j;\alpha_2}Gα1​α2​(1)​=Cb(1)​+CW(1)​n0​1​∑j​xj;α1​​xj;α2​​ (eq. 4.8), and ⟨F(zα1,…,zαm)⟩g\langle F(z_{\alpha_1},\dots,z_{\alpha_m})\rangle_{g}⟨F(zα1​​,…,zαm​​)⟩g​ denotes the expectation over a centered Gaussian vector (zα)(z_\alpha)(zα​) with covariance ggg (eq. 4.25), with σα≡σ(zα)\sigma_\alpha\equiv\sigma(z_\alpha)σα​≡σ(zα​).

Formalization targets

Goal: second-layer connected four-point correlator (eq. 4.43)

E[zi1;α1(2)zi2;α2(2)zi3;α3(2)zi4;α4(2)]∣connected=1n1[δi1i2δi3i4V(α1α2)(α3α4)(2)+δi1i3δi2i4V(α1α3)(α2α4)(2)+δi1i4δi2i3V(α1α4)(α2α3)(2)]\mathbb{E}\big[z^{(2)}_{i_1;\alpha_1}z^{(2)}_{i_2;\alpha_2}z^{(2)}_{i_3;\alpha_3}z^{(2)}_{i_4;\alpha_4}\big]\Big|_{\text{connected}}=\frac{1}{n_1}\Big[\delta_{i_1i_2}\delta_{i_3i_4}V^{(2)}_{(\alpha_1\alpha_2)(\alpha_3\alpha_4)}+\delta_{i_1i_3}\delta_{i_2i_4}V^{(2)}_{(\alpha_1\alpha_3)(\alpha_2\alpha_4)}+\delta_{i_1i_4}\delta_{i_2i_3}V^{(2)}_{(\alpha_1\alpha_4)(\alpha_2\alpha_3)}\Big]E[zi1​;α1​(2)​zi2​;α2​(2)​zi3​;α3​(2)​zi4​;α4​(2)​]​connected​=n1​1​[δi1​i2​​δi3​i4​​V(α1​α2​)(α3​α4​)(2)​+δi1​i3​​δi2​i4​​V(α1​α3​)(α2​α4​)(2)​+δi1​i4​​δi2​i3​​V(α1​α4​)(α2​α3​)(2)​]

with the four-point vertex V(α1α2)(α3α4)(2)=(CW(2))2[⟨σα1σα2σα3σα4⟩G(1)−⟨σα1σα2⟩G(1)⟨σα3σα4⟩G(1)]V^{(2)}_{(\alpha_1\alpha_2)(\alpha_3\alpha_4)}=\big(C_W^{(2)}\big)^2\big[\langle\sigma_{\alpha_1}\sigma_{\alpha_2}\sigma_{\alpha_3}\sigma_{\alpha_4}\rangle_{G^{(1)}}-\langle\sigma_{\alpha_1}\sigma_{\alpha_2}\rangle_{G^{(1)}}\langle\sigma_{\alpha_3}\sigma_{\alpha_4}\rangle_{G^{(1)}}\big]V(α1​α2​)(α3​α4​)(2)​=(CW(2)​)2[⟨σα1​​σα2​​σα3​​σα4​​⟩G(1)​−⟨σα1​​σα2​​⟩G(1)​⟨σα3​​σα4​​⟩G(1)​] (eq. 4.40).

Milestones

  1. Eq. (4.6) — first-layer mean vanishes.
  2. Eqs. (4.7)–(4.8) — first-layer two-point correlator δi1i2Gα1α2(1)\delta_{i_1i_2}G^{(1)}_{\alpha_1\alpha_2}δi1​i2​​Gα1​α2​(1)​.
  3. Eq. (4.9) — first-layer four-point correlator is the Wick value.
  4. Eq. (4.23) — the first-layer preactivations are exactly Gaussian with covariance δi1i2Gα1α2(1)\delta_{i_1i_2}G^{(1)}_{\alpha_1\alpha_2}δi1​i2​​Gα1​α2​(1)​.
  5. Eqs. (4.27), (4.28), (4.29) — activation correlators in the first layer as Gaussian expectations.
  6. Eq. (4.40) — two-point correlator of the second-layer metric fluctuation.
  7. Eq. (4.41) — second-layer two-point correlator.

Significance

These identities are the base case of the book's recursion (Chapter 4.3 onward) for the kernel and four-point vertex in deeper layers, and they show concretely that a finite-width network is not a Gaussian process: the 1/n11/n_11/n1​ connected correlator is generically nonzero for nonlinear σ\sigmaσ. The results are exact computations in the book; this mission formalizes them.

Difficulty

The second layer is a Gaussian conditional on the first layer, with a random covariance (the stochastic metric, eq. 4.36). Turning this into unconditional correlators requires conditioning on the first-layer preactivations, independence of different first-layer neurons, and the identification of first-layer activation correlators with Gaussian expectations over the metric G(1)G^{(1)}G(1), which may be degenerate (e.g. repeated inputs). Integrability of σ\sigmaσ against Gaussians must be controlled.

Formalization scope

  • Definitions from Mission II are reused: kron, inputKernel, WeightIndex. New definitions: mlpPreact (zi(ℓ)(x)z^{(\ell)}_i(x)zi(ℓ)​(x)), IsMLPInit (independent Gaussian biases and weights with layer-dependent Cb(ℓ),CW(ℓ)C_b^{(\ell)},C_W^{(\ell)}Cb(ℓ)​,CW(ℓ)​), firstLayerMetric (G(1)G^{(1)}G(1) on finitely many inputs), gaussAvg (⟨⋅⟩g\langle\cdot\rangle_g⟨⋅⟩g​, via Mathlib's multivariateGaussian, which handles singular positive-semidefinite ggg), and HasPolyGrowth.
  • Statements about activations assume σ\sigmaσ measurable with polynomial growth, the standing convention guaranteeing that all Gaussian averages are finite; this covers ReLU, tanh, sigmoid, GELU, SWISH and the perceptron step function.
  • The sample set is Fin D (for the specific statements, D=2D=2D=2 or 444 inputs, possibly repeated). n1>0n_1>0n1​>0 is assumed where the formulas divide by n1n_1n1​.

Selected references

  • D. A. Roberts, S. Yaida (with B. Hanin), The Principles of Deep Learning Theory, Cambridge University Press, 2022, Chapter 4. arXiv:2106.10165
  • R. M. Neal, Bayesian Learning for Neural Networks, Springer, 1996. doi:10.1007/978-1-4612-0745-0
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Machine LearningOptimizationProbability·Captain: naimengye

Understanding Machine Learning X: Gradient Descent, Subgradients and Stochastic Gradient DescentTextbook

Motivation

Chapter 13 showed that convex-Lipschitz-bounded and convex-smooth-bounded problems are learnable by regularized loss minimization; Chapter 14 of Shalev-Shwartz and Ben-David, Understanding Machine Learning: From Theory to Algorithms (doi:10.1017/CBO9781107298019) shows how to learn them with the simplest possible algorithm. Gradient descent moves against the gradient with a fixed step size and outputs the average of its iterates; its analysis (Lemma 14.1) is a single telescoping identity that bounds ∑t⟨w(t)−w⋆,vt⟩\sum_t \langle w^{(t)} - w^\star, v_t\rangle∑t​⟨w(t)−w⋆,vt​⟩ for any sequence of directions vtv_tvt​, and this generality is the whole point. It gives the rate Bρ/TB\rho/\sqrt TBρ/T​ for convex Lipschitz functions (Corollary 14.2), extends to nondifferentiable functions through subgradients (Definition 14.4, Lemmas 14.3 and 14.7), and, because it never used that the directions were gradients, extends to stochastic gradient descent, in which each direction is random with a subgradient as its conditional expectation (Theorem 14.8). Applied to the risk LD(w)L_D(w)LD​(w) with a fresh example at each step, SGD is a learning algorithm whose sample complexity is the iteration count: B2ρ2/ϵ2B^2\rho^2/\epsilon^2B2ρ2/ϵ2 examples for convex-Lipschitz-bounded problems (Corollary 14.12) and 12B2β/ϵ212B^2\beta/\epsilon^212B2β/ϵ2 for convex-smooth-bounded ones (Theorem 14.13, Corollary 14.14). A projected, decreasing-step variant for strongly convex objectives has rate (ρ2/(2λT))(1+log⁡T)(\rho^2/(2\lambda T))(1 + \log T)(ρ2/(2λT))(1+logT) (Theorem 14.11).

Setting

Hypotheses are vectors in Rd\mathbb{R}^dRd; convex, Lipschitz and smooth losses, convex-Lipschitz-bounded and convex-smooth-bounded problems, and strong convexity are those of Mission IX. A vector vvv is a subgradient of fff at www if f(u)≥f(w)+⟨u−w,v⟩f(u) \ge f(w) + \langle u - w, v\ranglef(u)≥f(w)+⟨u−w,v⟩ for all uuu. The iterates of an update rule w(1)=0w^{(1)} = 0w(1)=0, w(t+1)=w(t)−ηvtw^{(t+1)} = w^{(t)} - \eta v_tw(t+1)=w(t)−ηvt​ are indexed from 000, and the output after TTT steps is wˉ=1T∑t<Tw(t)\bar w = \frac1T\sum_{t < T} w^{(t)}wˉ=T1​∑t<T​w(t). The randomness of SGD is modelled as the chapter uses it in §14.5: a sample z0,…,zT−1z_0, \dots, z_{T-1}z0​,…,zT−1​ drawn i.i.d. from DDD and an oracle ggg with vt=g(w(t),zt)v_t = g(w^{(t)}, z_t)vt​=g(w(t),zt​), where ggg is a stochastic subgradient oracle for fff if Ez∼D g(w,z)∈∂f(w)\mathbb{E}_{z \sim D}\, g(w, z) \in \partial f(w)Ez∼D​g(w,z)∈∂f(w) for every www. This is the book's condition E[vt∣w(t)]∈∂f(w(t))\mathbb{E}[v_t \mid w^{(t)}] \in \partial f(w^{(t)})E[vt​∣w(t)]∈∂f(w(t)) in the case where the direction depends on the past only through w(t)w^{(t)}w(t) and on fresh randomness, which is what every application in the book does; the expectation E[f(wˉ)]\mathbb{E}[f(\bar w)]E[f(wˉ)] is then an integral over DTD^TDT. For learning, g(w,z)g(w, z)g(w,z) is a subgradient of ℓ(⋅,z)\ell(\cdot, z)ℓ(⋅,z) at www, so that Ezg(w,z)\mathbb{E}_z g(w,z)Ez​g(w,z) is a subgradient of LDL_DLD​ at www (14.13). The projection of www onto a convex set HHH is a nearest point of HHH, and the strongly convex variant projects after each step with step size 1/(λt)1/(\lambda t)1/(λt).

Formalization targets

Goal: Theorem 14.8

For a convex fff, B,ρ>0B, \rho > 0B,ρ>0, a measurable oracle ggg with Ezg(w,z)∈∂f(w)\mathbb{E}_z g(w, z) \in \partial f(w)Ez​g(w,z)∈∂f(w) and ∥g(w,z)∥≤ρ\|g(w, z)\| \le \rho∥g(w,z)∥≤ρ, any w⋆w^\starw⋆ with ∥w⋆∥≤B\|w^\star\| \le B∥w⋆∥≤B, T≥1T \ge 1T≥1 and η=B/(ρT)\eta = B/(\rho\sqrt T)η=B/(ρT​): E[f(wˉ)]−f(w⋆)≤Bρ/T\mathbb{E}[f(\bar w)] - f(w^\star) \le B\rho/\sqrt TE[f(wˉ)]−f(w⋆)≤Bρ/T​; and for every ϵ>0\epsilon > 0ϵ>0, T≥B2ρ2/ϵ2T \ge B^2\rho^2/\epsilon^2T≥B2ρ2/ϵ2 gives E[f(wˉ)]−f(w⋆)≤ϵ\mathbb{E}[f(\bar w)] - f(w^\star) \le \epsilonE[f(wˉ)]−f(w⋆)≤ϵ.

Milestones

Lemma 14.1. For any directions, ∑t<T⟨w(t)−w⋆,vt⟩≤∥w⋆∥2/(2η)+(η/2)∑t<T∥vt∥2\sum_{t<T}\langle w^{(t)} - w^\star, v_t\rangle \le \|w^\star\|^2/(2\eta) + (\eta/2)\sum_{t<T}\|v_t\|^2∑t<T​⟨w(t)−w⋆,vt​⟩≤∥w⋆∥2/(2η)+(η/2)∑t<T​∥vt​∥2; with ∥vt∥≤ρ\|v_t\| \le \rho∥vt​∥≤ρ, ∥w⋆∥≤B\|w^\star\| \le B∥w⋆∥≤B and η=B/(ρT)\eta = B/(\rho\sqrt T)η=B/(ρT​) the average is at most Bρ/TB\rho/\sqrt TBρ/T​.

Corollary 14.2. Subgradient descent on a convex ρ\rhoρ-Lipschitz fff with η=B/(ρT)\eta = B/(\rho\sqrt T)η=B/(ρT​) has f(wˉ)−f(w⋆)≤Bρ/Tf(\bar w) - f(w^\star) \le B\rho/\sqrt Tf(wˉ)−f(w⋆)≤Bρ/T​ for every ∥w⋆∥≤B\|w^\star\| \le B∥w⋆∥≤B, and T≥B2ρ2/ϵ2T \ge B^2\rho^2/\epsilon^2T≥B2ρ2/ϵ2 gives ϵ\epsilonϵ.

Lemma 14.7. A convex fff on Rd\mathbb{R}^dRd is ρ\rhoρ-Lipschitz iff all its subgradients have norm at most ρ\rhoρ.

Lemma 14.9. For the projection vvv of www onto a convex HHH and u∈Hu \in Hu∈H, ∥w−u∥2≥∥v−u∥2\|w - u\|^2 \ge \|v - u\|^2∥w−u∥2≥∥v−u∥2.

Theorem 14.11. For λ\lambdaλ-strongly convex fff, a closed convex HHH, an oracle with Ez∥g(w,z)∥2≤ρ2\mathbb{E}_z\|g(w,z)\|^2 \le \rho^2Ez​∥g(w,z)∥2≤ρ2 and any w⋆∈Hw^\star \in Hw⋆∈H, the projected variant with ηt=1/(λt)\eta_t = 1/(\lambda t)ηt​=1/(λt) has E[f(wˉ)]−f(w⋆)≤(ρ2/(2λT))(1+log⁡T)\mathbb{E}[f(\bar w)] - f(w^\star) \le (\rho^2/(2\lambda T))(1 + \log T)E[f(wˉ)]−f(w⋆)≤(ρ2/(2λT))(1+logT).

Corollary 14.12. SGD on the risk of a convex-Lipschitz-bounded problem with T≥B2ρ2/ϵ2T \ge B^2\rho^2/\epsilon^2T≥B2ρ2/ϵ2 examples has E[LD(wˉ)]≤LD(w)+ϵ\mathbb{E}[L_D(\bar w)] \le L_D(w) + \epsilonE[LD​(wˉ)]≤LD​(w)+ϵ for every w∈Hw \in Hw∈H.

Theorem 14.13. For convex, β\betaβ-smooth, nonnegative losses and ηβ<1\eta\beta < 1ηβ<1, SGD with gradient directions has E[LD(wˉ)]≤11−ηβ(LD(w⋆)+∥w⋆∥2/(2ηT))\mathbb{E}[L_D(\bar w)] \le \frac{1}{1-\eta\beta}(L_D(w^\star) + \|w^\star\|^2/(2\eta T))E[LD​(wˉ)]≤1−ηβ1​(LD​(w⋆)+∥w⋆∥2/(2ηT)).

Corollary 14.14. For a convex-smooth-bounded problem with ℓ(0,z)≤1\ell(0,z) \le 1ℓ(0,z)≤1 and any ϵ>0\epsilon > 0ϵ>0, SGD with η=1/(β(1+3/ϵ))\eta = 1/(\beta(1 + 3/\epsilon))η=1/(β(1+3/ϵ)) and T≥12B2β/ϵ2T \ge 12B^2\beta/\epsilon^2T≥12B2β/ϵ2 has E[LD(wˉ)]≤LD(w)+ϵ\mathbb{E}[L_D(\bar w)] \le L_D(w) + \epsilonE[LD​(wˉ)]≤LD​(w)+ϵ for every w∈Hw \in Hw∈H.

Further items: Lemma 14.3, Claims 14.5, 14.6 and 14.10, and the hinge-loss subgradient of Example 14.2.

Significance

SGD is the algorithm behind most of modern machine learning, and Theorem 14.8 is its basic guarantee: dimension-free, independent of the form of fff beyond convexity, and with a sample complexity matching the regularization bound of Chapter 13 up to a constant. Lemma 14.1 isolates the deterministic identity that makes both gradient descent and its stochastic version work, and Lemma 14.7 is the bridge between the Lipschitz assumption of Chapter 12 and the bounded directions the analysis needs. The learning corollaries make the point that runs through Part II of the book: for convex problems, optimization and learning are the same activity, and one pass over the data suffices.

Nothing here is machine-checked. The chapter's statements are essentially correct, and the formalization records the reading choices rather than corrections: the i.i.d.-oracle model of the randomness, the subgradient form of gradient descent, the bound at every point of the ball rather than at a minimizer, and, in Corollary 14.14, the assumptions ϵ≤1\epsilon \le 1ϵ≤1 and 0∈H0 \in H0∈H under which the derivation from Theorem 14.13 goes through.

Difficulty

Lemma 14.1 is a completed square and a telescoping sum and is the intended entry point; the Bρ/TB\rho/\sqrt TBρ/T​ clause is the substitution of η\etaη. Corollary 14.2 is Lemma 14.1 with Jensen's inequality for the average and the subgradient inequality at each iterate, plus Lemma 14.7 to bound the directions. The subgradient facts need convex analysis: Lemma 14.3 in the direction "convex implies subgradients exist" is the supporting hyperplane theorem on Rd\mathbb{R}^dRd, which Mathlib does not offer directly; Claim 14.5 uses the first-order characterization of convexity for differentiable functions; Lemma 14.7's "Lipschitz implies bounded subgradients" is the book's one-line argument along u=w+ϵv/∥v∥u = w + \epsilon v/\|v\|u=w+ϵv/∥v∥. Theorem 14.8 is Lemma 14.1 plus the conditioning argument of the book, which in the i.i.d.-oracle model is Fubini on the product DTD^TDT: the iterate w(t)w^{(t)}w(t) is a measurable function of z0,…,zt−1z_0, \dots, z_{t-1}z0​,…,zt−1​, and integrating ⟨w(t)−w⋆,g(w(t),zt)⟩\langle w^{(t)} - w^\star, g(w^{(t)}, z_t)\rangle⟨w(t)−w⋆,g(w(t),zt​)⟩ over ztz_tzt​ first gives ⟨w(t)−w⋆,Ezg(w(t),z)⟩≥f(w(t))−f(w⋆)\langle w^{(t)} - w^\star, \mathbb{E}_z g(w^{(t)}, z)\rangle \ge f(w^{(t)}) - f(w^\star)⟨w(t)−w⋆,Ez​g(w(t),z)⟩≥f(w(t))−f(w⋆). Theorem 14.11 adds the projection lemma, the strong-convexity inequality of Claim 14.10, the telescoping of λt2(at−at+1)−λ2at\frac{\lambda t}{2}(a_t - a_{t+1}) - \frac\lambda2 a_t2λt​(at​−at+1​)−2λ​at​ and the harmonic sum ∑t≤T1/t≤1+log⁡T\sum_{t \le T} 1/t \le 1 + \log T∑t≤T​1/t≤1+logT; the second-moment hypothesis makes E∥w(t)−w⋆∥2\mathbb{E}\|w^{(t)} - w^\star\|^2E∥w(t)−w⋆∥2 finite inductively. Corollary 14.12 is Theorem 14.8 for f=LDf = L_Df=LD​ with the oracle of (14.13), which requires exchanging a subgradient inequality with the integral over zzz. Theorem 14.13 replaces the Lipschitz bound by self-boundedness, ∥∇ℓ∥2≤2βℓ\|\nabla\ell\|^2 \le 2\beta\ell∥∇ℓ∥2≤2βℓ, and rearranges; Corollary 14.14 is its arithmetic under the added assumptions. In all expectation statements the measurability of the iterates in the sample, from the measurability of the oracle, is a routine but necessary lemma.

Formalization scope

Iterates are defined by structural recursion, so no argmin is chosen; the sample-driven SGD stops after TTT updates; the projection onto HHH is a chosen nearest point, unique for closed convex HHH. Bounds are stated for every w⋆w^\starw⋆ in the ball (or in HHH) rather than for a minimizer, which is what the proofs give and is stronger. The oracle bound ∥g(w,z)∥≤ρ\|g(w,z)\| \le \rho∥g(w,z)∥≤ρ is required surely (the book: with probability 111); the almost-sure version is a routine extension. The second-moment hypothesis of Theorem 14.11 is a lower Lebesgue integral, so that a non-integrable oracle cannot satisfy it vacuously. The learning corollaries assume a measurable loss, nonnegative and bounded at the origin, so that the risks are genuine integrals, and a measurable selector of subgradients. Variable step sizes (§14.4.2), other averaging schemes (§14.4.3), SGD for regularized loss minimization (§14.5.3) and the exercises are not stated.

Trivializing readings are excluded: the expectations are over the product law of the examples with measurable integrands, the subgradient conditions are pointwise inequalities, and the iteration counts are the book's. Welcome contributions: Lemma 14.1 as a reusable telescoping lemma, the measurability of the SGD iterates, and the Fubini step that turns an oracle condition into the inequality (14.10).

Selected references

  • S. Shalev-Shwartz, S. Ben-David, Understanding Machine Learning: From Theory to Algorithms, Cambridge University Press, 2014, Chapter 14. doi:10.1017/CBO9781107298019
  • H. Robbins, S. Monro, A stochastic approximation method, Annals of Mathematical Statistics 22(3), 1951. doi:10.1214/aoms/1177729586
  • M. Zinkevich, Online convex programming and generalized infinitesimal gradient ascent, Proceedings of ICML, 2003.
  • A. Nemirovski, A. Juditsky, G. Lan, A. Shapiro, Robust stochastic approximation approach to stochastic programming, SIAM Journal on Optimization 19(4), 2009. doi:10.1137/070704277
  • S. Shalev-Shwartz, Online learning and online convex optimization, Foundations and Trends in Machine Learning 4(2), 2012. doi:10.1561/2200000018
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