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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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Machine LearningOptimizationProbability·Captain: mikedeng1

Graphical Convergence of Subgradients in Nonconvex Optimization and Learning: Uniform Concentration of Empirical Bregman Proximal Points for Weakly Convex RisksResearch Paper

Motivation

A learner who minimizes a regularized population risk

φ(x)=Ez∼P[f(x,z)]+r(x)\varphi(x)=\mathbb E_{z\sim P}[f(x,z)]+r(x)φ(x)=Ez∼P​[f(x,z)]+r(x)

usually has access to PPP only through an i.i.d. sample S=(z1,…,zm)S=(z_1,\dots,z_m)S=(z1​,…,zm​), and so works with the empirical risk φS(x)=1m∑i=1mf(x,zi)+r(x)\varphi_S(x)=\frac1m\sum_{i=1}^m f(x,z_i)+r(x)φS​(x)=m1​∑i=1m​f(x,zi​)+r(x) instead. The question this mission formalizes is how well the first-order behaviour of φS\varphi_SφS​ reflects that of φ\varphiφ when the loss is neither smooth nor convex. This matters because the algorithms used in practice for such problems (stochastic subgradient, proximal point and Gauss–Newton methods) find only approximately stationary points, and a uniform estimate of the gap between empirical and population stationarity tells one when further optimization of the empirical problem stops improving the population one.

For convex losses with strongly convex regularization, Shalev-Shwartz, Shamir, Srebro and Sridharan (COLT 2009) showed that the regularized empirical minimizer is stable and generalizes at a dimension-free rate. For smooth nonconvex losses, Mei, Bai and Montanari (Ann. Statist. 2018) and Foster, Sekhari and Sridharan (NeurIPS 2018) proved uniform convergence of gradients. For nonsmooth nonconvex losses, pointwise convergence of the stationarity measure dist⁡(0,∂φ(x))\operatorname{dist}(0,\partial\varphi(x))dist(0,∂φ(x)) was known, but uniform results were asymptotic and needed extra structure, because x↦dist⁡(0,∂φ(x))x\mapsto\operatorname{dist}(0,\partial\varphi(x))x↦dist(0,∂φ(x)) is highly discontinuous. Davis and Drusvyatskiy (arXiv:1810.07590, Mathematics of Operations Research 2022) replace it by a smoothed measure, the gradient of a Moreau-type envelope, and prove finite-sample uniform bounds for it. The losses covered are the weakly convex ones: phase retrieval, blind deconvolution, robust PCA, censored block models, conditional value-at-risk and sparse dictionary learning all fit (Table 1 of the paper).

Setting

Fix a finite-dimensional real normed space EEE with norm ∥⋅∥\|\cdot\|∥⋅∥ and dual norm ∥⋅∥∗\|\cdot\|_*∥⋅∥∗​. Extended-valued functions g:E→R∪{+∞}g:E\to\mathbb R\cup\{+\infty\}g:E→R∪{+∞} are described by their domain dom⁡g\operatorname{dom} gdomg and their values there.

A Legendre function Φ\PhiΦ is proper, closed and strictly convex, differentiable on the nonempty interior of its domain, and its gradient norm blows up at the boundary of the domain. It induces the Bregman divergence

DΦ(y,x)=Φ(y)−Φ(x)−⟨∇Φ(x),y−x⟩,x∈int⁡(dom⁡Φ),D_\Phi(y,x)=\Phi(y)-\Phi(x)-\langle\nabla\Phi(x),y-x\rangle,\qquad x\in\operatorname{int}(\operatorname{dom}\Phi),DΦ​(y,x)=Φ(y)−Φ(x)−⟨∇Φ(x),y−x⟩,x∈int(domΦ),

and its symmetrization DΦsym(x,y)=DΦ(x,y)+DΦ(y,x)D^{\mathrm{sym}}_\Phi(x,y)=D_\Phi(x,y)+D_\Phi(y,x)DΦsym​(x,y)=DΦ​(x,y)+DΦ​(y,x). For Φ=12∥⋅∥22\Phi=\frac12\|\cdot\|_2^2Φ=21​∥⋅∥22​, DΦ(y,x)=12∥y−x∥22D_\Phi(y,x)=\frac12\|y-x\|_2^2DΦ​(y,x)=21​∥y−x∥22​. A function ggg is ρ\rhoρ-weakly convex relative to Φ\PhiΦ if g+ρΦg+\rho\Phig+ρΦ is convex, and compatible with Φ\PhiΦ if ri⁡(dom⁡g)⊆int⁡(dom⁡Φ)\operatorname{ri}(\operatorname{dom} g)\subseteq\operatorname{int}(\operatorname{dom}\Phi)ri(domg)⊆int(domΦ). For ρˉ>0\bar\rho>0ρˉ​>0 the Φ-proximal map and Φ-envelope are

prox⁡g/ρˉΦ(x)=argmin⁡y{g(y)+ρˉDΦ(y,x)},g1/ρˉΦ(x)=inf⁡y{g(y)+ρˉDΦ(y,x)}.\operatorname{prox}^\Phi_{g/\bar\rho}(x)=\operatorname*{argmin}_y\{g(y)+\bar\rho D_\Phi(y,x)\},\qquad g^\Phi_{1/\bar\rho}(x)=\inf_y\{g(y)+\bar\rho D_\Phi(y,x)\}.proxg/ρˉ​Φ​(x)=yargmin​{g(y)+ρˉ​DΦ​(y,x)},g1/ρˉ​Φ​(x)=yinf​{g(y)+ρˉ​DΦ​(y,x)}.

The standing assumptions are: (A1) Φ\PhiΦ is Legendre, compatible with rrr, and α2∥y−x∥2≤DΦ(x,y)\frac\alpha2\|y-x\|^2\le D_\Phi(x,y)2α​∥y−x∥2≤DΦ​(x,y) on dom⁡r∩int⁡(dom⁡Φ)\operatorname{dom} r\cap\operatorname{int}(\operatorname{dom}\Phi)domr∩int(domΦ); (A2) for a.e. zzz, f(⋅,z)+rf(\cdot,z)+rf(⋅,z)+r is ρ\rhoρ-weakly convex relative to Φ\PhiΦ and bounded below; (A3) ∣f(x,z)−f(y,z)∣≤L(z)DΦsym(x,y)|f(x,z)-f(y,z)|\le L(z)\sqrt{D^{\mathrm{sym}}_\Phi(x,y)}∣f(x,z)−f(y,z)∣≤L(z)DΦsym​(x,y)​ with L≥0L\ge0L≥0 and EL2≤σ\sqrt{\mathbb E L^2}\le\sigmaEL2​≤σ. Finally ψεL(λ)=log⁡E eλεL(z)\psi_{\varepsilon L}(\lambda)=\log\mathbb E\,e^{\lambda\varepsilon L(z)}ψεL​(λ)=logEeλεL(z) for an independent Rademacher sign ε\varepsilonε, and ψεL⋆\psi^\star_{\varepsilon L}ψεL⋆​ is its Fenchel conjugate.

Formalization targets

Goal: Theorem 4.4 (concentration of the stationarity measure)

For every C⊆int⁡(dom⁡Φ)C\subseteq\operatorname{int}(\operatorname{dom}\Phi)C⊆int(domΦ), δ>0\delta>0δ>0, s≥0s\ge0s≥0 and ρˉ>ρ\bar\rho>\rhoρˉ​>ρ, with probability at least 1−N(C,Φ,δ)exp⁡(−m ψεL⋆(s/m))1-\mathcal N(C,\Phi,\delta)\exp(-m\,\psi^\star_{\varepsilon L}(s/\sqrt m))1−N(C,Φ,δ)exp(−mψεL⋆​(s/m​)),

sup⁡y∈C∥prox⁡φS/ρˉΦ(y)−prox⁡φ/ρˉΦ(y)∥≤4(σ+s)2α(ρˉ−ρ)2m+2ρˉδα(ρˉ−ρ),\sup_{y\in C}\big\|\operatorname{prox}^\Phi_{\varphi_S/\bar\rho}(y)-\operatorname{prox}^\Phi_{\varphi/\bar\rho}(y)\big\|\le\sqrt{\frac{4(\sigma+s)^2}{\alpha(\bar\rho-\rho)^2m}}+\frac{2\bar\rho\delta}{\alpha(\bar\rho-\rho)},y∈Csup​​proxφS​/ρˉ​Φ​(y)−proxφ/ρˉ​Φ​(y)​≤α(ρˉ​−ρ)2m4(σ+s)2​​+α(ρˉ​−ρ)2ρˉ​δ​,

where N(C,Φ,δ)\mathcal N(C,\Phi,\delta)N(C,Φ,δ) is the covering number of CCC in the metric ∥∇Φ(x)−∇Φ(y)∥∗\|\nabla\Phi(x)-\nabla\Phi(y)\|_*∥∇Φ(x)−∇Φ(y)∥∗​. If Φ\PhiΦ is twice differentiable, the same probability bounds the event sup⁡y∈C∥∇(φS)1/2ρΦ(y)−∇φ1/2ρΦ(y)∥y∗≤16(σ+s)2/(αm)+8ρδ/α\sup_{y\in C}\|\nabla(\varphi_S)^\Phi_{1/2\rho}(y)-\nabla\varphi^\Phi_{1/2\rho}(y)\|^*_y\le\sqrt{16(\sigma+s)^2/(\alpha m)}+8\rho\delta/\alphasupy∈C​∥∇(φS​)1/2ρΦ​(y)−∇φ1/2ρΦ​(y)∥y∗​≤16(σ+s)2/(αm)​+8ρδ/α in the local dual norm.

Milestones

  1. Theorem 3.1: the Φ-proximal point of a closed, lower-bounded, weakly convex, compatible ggg is unique and interior, and the envelope has gradient 1λ∇2Φ(x)(x−prox⁡λgΦ(x))\frac1\lambda\nabla^2\Phi(x)(x-\operatorname{prox}^\Phi_{\lambda g}(x))λ1​∇2Φ(x)(x−proxλgΦ​(x)).
  2. Theorem 4.1: stability of Bregman-regularized ERM, DΦsym(A(S),A(Si))≤L(zi)+L(zi′)(ρˉ−ρ)m\sqrt{D^{\mathrm{sym}}_\Phi(\mathcal A(S),\mathcal A(S^i))}\le\frac{L(z_i)+L(z_i')}{(\bar\rho-\rho)m}DΦsym​(A(S),A(Si))​≤(ρˉ​−ρ)mL(zi​)+L(zi′​)​, and the expectation bounds (4.2), (4.3).
  3. Theorem 4.2: McDiarmid's inequality with data-dependent differences ωi(zi,zi′)\omega_i(z_i,z_i')ωi​(zi​,zi′​), in log-MGF form (4.7) and tail form (4.8).
  4. Lemma 4.3: prox⁡g/ρˉΦ\operatorname{prox}^\Phi_{g/\bar\rho}proxg/ρˉ​Φ​ is ρˉα(ρˉ−ρ)\frac{\bar\rho}{\alpha(\bar\rho-\rho)}α(ρˉ​−ρ)ρˉ​​-Lipschitz from the metric ∥∇Φ(x)−∇Φ(y)∥∗\|\nabla\Phi(x)-\nabla\Phi(y)\|_*∥∇Φ(x)−∇Φ(y)∥∗​ to ∥⋅∥\|\cdot\|∥⋅∥.

Significance

The result gives a sample size beyond which approximate stationarity of the empirical problem certifies approximate stationarity of the population problem, uniformly over a region, with an explicit dependence on the sample size mmm and on the covering number of the region. Because the graph of the proximal map is linearly isomorphic to the graph of the subdifferential, it also bounds the Hausdorff distance between gph⁡∂φ\operatorname{gph}\partial\varphigph∂φ and gph⁡∂φS\operatorname{gph}\partial\varphi_Sgph∂φS​ (Theorem 4.5 of the paper, not part of this mission). The Bregman setting covers non-Euclidean geometries (an ℓ1\ell_1ℓ1​-setup) and losses that are only locally Lipschitz with polynomial growth. Theorem 4.2 is reusable on its own: it is a McDiarmid inequality for unbounded, light-tailed differences.

The paper's proofs are complete; nothing here is open. None of the statements has been formalized before. Mathlib has the Fréchet derivative, product measures, cumulant generating functions and convexity, but no Legendre functions, Bregman proximal maps or envelopes, and no McDiarmid inequality with data-dependent differences; the platform has McDiarmid only with constant differences.

Difficulty

The naive route, McDiarmid's inequality applied to ∥prox⁡φS/ρˉΦ(y)−prox⁡φ/ρˉΦ(y)∥\|\operatorname{prox}^\Phi_{\varphi_S/\bar\rho}(y)-\operatorname{prox}^\Phi_{\varphi/\bar\rho}(y)\|∥proxφS​/ρˉ​Φ​(y)−proxφ/ρˉ​Φ​(y)∥, needs a bounded difference constant, and the stability estimate (4.1) gives only L(zi)+L(zi′)L(z_i)+L(z_i')L(zi​)+L(zi′​), which is unbounded unless the data are. The concentration step therefore needs a version of McDiarmid's inequality whose differences are random. A second obstacle is that the empirical objects are random sets: proving that the proximal points are single-valued, interior, and measurable in the sample is a step the paper takes for granted. Third, uniformity over CCC comes through Lemma 4.3 in the mirror metric ∥∇Φ(x)−∇Φ(y)∥∗\|\nabla\Phi(x)-\nabla\Phi(y)\|_*∥∇Φ(x)−∇Φ(y)∥∗​, not in the norm of EEE.

Formalization scope

The space is a finite-dimensional real normed space EEE; gradients are Fréchet derivatives, the dual norm is the operator norm, and ∇2Φ(y)\nabla^2\Phi(y)∇2Φ(y) is the second Fréchet derivative, a map E→E∗E\to E^*E→E∗. Extended-valued functions are pairs (domain, real values), so no extended-real arithmetic occurs. Proximal maps are sets of minimizers; envelopes are real infima, used only where Theorem 3.1 guarantees attainment. "With probability 1−p1-p1−p" is an outer-measure bound on the failure set under PmP^mPm. The covering number is replaced by the size of an arbitrary finite δ\deltaδ-net fixed before the sample, and exp⁡(−mψ⋆(t))\exp(-m\psi^\star(t))exp(−mψ⋆(t)) by exp⁡(−m(λt−ψ(λ)))\exp(-m(\lambda t-\psi(\lambda)))exp(−m(λt−ψ(λ))) for an arbitrary λ\lambdaλ with cosh⁡(λL)\cosh(\lambda L)cosh(λL) integrable; both replacements are equivalent to the page. Hypotheses the paper uses without stating are explicit: ρˉ>0\bar\rho>0ρˉ​>0, m≥1m\ge1m≥1, dom⁡r\operatorname{dom} rdomr nonempty and convex, f(x,⋅)f(x,\cdot)f(x,⋅) measurable and integrable, closedness of f(⋅,z)+rf(\cdot,z)+rf(⋅,z)+r and of φ\varphiφ, φ\varphiφ bounded below; the second display of the goal assumes ρ>0\rho>0ρ>0 and an invertible Hessian on CCC. Theorem 4.1 is read, as its proof is, with A∗\mathcal A^*A∗ and A(S)\mathcal A(S)A(S) the proximal points at yyy.

A pointwise version (fixed yyy), a version where the net may depend on the sample, a bound for one fixed λ\lambdaλ, or the Euclidean case Φ=12∥⋅∥22\Phi=\frac12\|\cdot\|_2^2Φ=21​∥⋅∥22​ alone would each be a strictly weaker theorem and does not close the goal.

A complete development needs: Legendre-function theory (coercivity of DΦ(⋅,x)D_\Phi(\cdot,x)DΦ​(⋅,x), interiority of Bregman proximal points), Danskin-type differentiation of the envelope, measurability of argmin maps, the extended McDiarmid inequality, and a covering/union bound. The McDiarmid extension and the Bregman proximal-point lemmas are reusable well beyond this paper. Proofs of the milestones, sanity instances of (A1)–(A3), and intermediate lemmas from the paper's proofs are all welcome.

Selected references

  • D. Davis, D. Drusvyatskiy, Graphical Convergence of Subgradients in Nonconvex Optimization and Learning, Mathematics of Operations Research, 2022. arXiv:1810.07590
  • D. Davis, D. Drusvyatskiy, K. J. MacPhee, Stochastic model-based minimization under high-order growth, 2018. arXiv:1807.00255
  • H. H. Bauschke, M. N. Dao, S. B. Lindstrom, Regularizing with Bregman–Moreau envelopes, SIAM J. Optim., 2018. arXiv:1705.06019
  • S. Shalev-Shwartz, O. Shamir, N. Srebro, K. Sridharan, Stochastic Convex Optimization, COLT, 2009. https://www.cs.mcgill.ca/~colt2009/papers/018.pdf
  • C. McDiarmid, On the method of bounded differences, Surveys in Combinatorics, LMS Lecture Note Ser. 141, 1989. doi:10.1017/CBO9781107359949.008
  • A. Kontorovich, Concentration in unbounded metric spaces and algorithmic stability, ICML, 2014. arXiv:1309.1007
  • S. Mei, Y. Bai, A. Montanari, The landscape of empirical risk for nonconvex losses, Ann. Statist., 2018. arXiv:1607.06534
  • D. J. Foster, A. Sekhari, K. Sridharan, Uniform convergence of gradients for non-convex learning and optimization, NeurIPS, 2018. arXiv:1810.11059
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Control TheoryQuantum InformationQuantum Mechanics·Captain: mikedeng1

How Far do Lindbladians Go?: Single-Qubit Amplitude Damping and Dephasing with Hörmander Unitary Control Make the Closed Channel Class TransitiveResearch Paper

Motivation

The state of a finite-dimensional quantum system is a density: a positive semidefinite matrix of trace one. Under coherent (Hamiltonian) control the evolution is unitary, ρ↦UρU∗\rho\mapsto U\rho U^*ρ↦UρU∗, and preserves the eigenvalues of ρ\rhoρ. Even with full unitary control, a state can therefore only be moved within its unitary orbit. A mixed state cannot be purified, and a pure state cannot be made mixed. Dissipation, modelled by Lindblad generators (Gorini–Kossakowski–Sudarshan 1976, Lindblad 1976), is what breaks these spectral invariants. Engineered dissipation is a standard tool for state preparation (Verstraete–Wolf–Cirac 2009).

This raises a basic control question: how much dissipation must be added to full unitary control before every state can be steered to every other state? Cai, Govindarajan and Junge (arXiv:2504.04883v2) answer it for kkk qubits. One amplitude-damping jump and one dephasing operator, both acting on a single qubit, suffice.

Timeline.

  • Brockett (1972) and Jurdjevic–Sussmann (1972) established the Lie-algebra rank condition for controllability on compact Lie groups. This settled the closed (unitary) case.
  • Altafini (2003) began the controllability analysis of Markovian master equations driven by coherent controls.
  • Dirr, Helmke, Kurniawan and Schulte-Herbrüggen (2009) described Markovian channels through Lie semigroups and Lie wedges.
  • Araiza, Chen, Junge and Wu (2023) studied resource-dependent classes of channels generated by a resource set SSS. The present mission's class Channel(S)‾\overline{\mathrm{Channel}(S)}Channel(S)​ follows that approach.
  • Cai, Govindarajan and Junge (2025) proved Theorem 2.12: Channel(S)‾\overline{\mathrm{Channel}(S)}Channel(S)​ is transitive once SSS contains a single-qubit amplitude-damping jump and a single-qubit dephasing operator. With a convex hull, Theorem 2.8 of the same paper needs only the amplitude-damping jump.

Setting

Let H=C2kH=\mathbb C^{2^k}H=C2k be the space of kkk qubits, with computational basis ∣ω⟩|\omega\rangle∣ω⟩, ω∈{0,1}k\omega\in\{0,1\}^kω∈{0,1}k. A superoperator is a linear map on kkk-qubit matrices. Densities form the set D(H)={ρ:ρ=ρ∗, ρ≥0, tr⁡ρ=1}\mathcal D(H)=\{\rho:\rho=\rho^*,\ \rho\ge0,\ \operatorname{tr}\rho=1\}D(H)={ρ:ρ=ρ∗, ρ≥0, trρ=1}.

For an operator aaa, the Lindblad generator with rate 222 is

La(ρ)=2aρa∗−a∗aρ−ρa∗a.L_a(\rho)=2a\rho a^*-a^*a\rho-\rho a^*a .La​(ρ)=2aρa∗−a∗aρ−ρa∗a.

For every t≥0t\ge0t≥0, etLae^{tL_a}etLa​ is a quantum channel.

Fix a resource set SSS of operators with S=S∗S=S^*S=S∗. The closed class Channel(S)‾\overline{\mathrm{Channel}(S)}Channel(S)​ is the smallest closed set C\mathcal CC of superoperators with three properties:

  • (UN) Ad⁡etX∈C\operatorname{Ad}_{e^{tX}}\in\mathcal CAdetX​∈C, where Ad⁡U(ρ)=UρU∗\operatorname{Ad}_U(\rho)=U\rho U^*AdU​(ρ)=UρU∗, for every anti-Hermitian X=iHX=iHX=iH in the complex span of SSS and every t≥0t\ge0t≥0;
  • (JU) etLa∈Ce^{tL_a}\in\mathcal CetLa​∈C for every a∈Sa\in Sa∈S and every t≥0t\ge0t≥0;
  • (CO) C\mathcal CC is closed under composition.

SSS generates a Hörmander system if the real Lie algebra generated by the anti-Hermitian part of span⁡S\operatorname{span}SspanS contains su(2k)\mathfrak{su}(2^k)su(2k), the traceless anti-Hermitian matrices. A set OOO of superoperators is transitive if for all ρ,σ∈D(H)\rho,\sigma\in\mathcal D(H)ρ,σ∈D(H) some Φ∈O\Phi\in OΦ∈O satisfies Φ(ρ)=σ\Phi(\rho)=\sigmaΦ(ρ)=σ. The range of ρ\rhoρ is DS(ρ)={Φ(ρ):Φ∈Channel(S)‾}D_S(\rho)=\{\Phi(\rho):\Phi\in\overline{\mathrm{Channel}(S)}\}DS​(ρ)={Φ(ρ):Φ∈Channel(S)​}.

On one qubit, Z=diag⁡(1,−1)Z=\operatorname{diag}(1,-1)Z=diag(1,−1), ∣0⟩⟨1∣|0\rangle\langle1|∣0⟩⟨1∣ is the amplitude-damping jump, and E∞E_\inftyE∞​ keeps the diagonal of a 2×22\times22×2 matrix and deletes the rest. The replacer channel is Rσ(ρ)=tr⁡(ρ) σ\mathcal R_\sigma(\rho)=\operatorname{tr}(\rho)\,\sigmaRσ​(ρ)=tr(ρ)σ, and ∣0k⟩=∣0⋯0⟩|0_k\rangle=|0\cdots0\rangle∣0k​⟩=∣0⋯0⟩.

Formalization targets

Goal: Theorem 2.12

If S=S∗S=S^*S=S∗ generates a Hörmander system on C2k\mathbb C^{2^k}C2k and

∣0⟩⟨1∣⊗I⊗(k−1)∈S,Z⊗I⊗(k−1)∈S,|0\rangle\langle1|\otimes I^{\otimes(k-1)}\in S,\qquad Z\otimes I^{\otimes(k-1)}\in S,∣0⟩⟨1∣⊗I⊗(k−1)∈S,Z⊗I⊗(k−1)∈S,

then

∀ ρ,σ∈D(H)∃ Φ∈Channel(S)‾: Φ(ρ)=σ.\forall\,\rho,\sigma\in\mathcal D(H)\quad \exists\,\Phi\in\overline{\mathrm{Channel}(S)}:\ \Phi(\rho)=\sigma .∀ρ,σ∈D(H)∃Φ∈Channel(S)​: Φ(ρ)=σ.

The goal asserts reachability only. It places no bound on time or on the number of compositions.

Milestones

  1. Proposition 2.2(i), as used. Ad⁡U∈Channel(S)‾\operatorname{Ad}_U\in\overline{\mathrm{Channel}(S)}AdU​∈Channel(S)​ for every unitary UUU.
  2. Proposition 2.2(iii). etLuau∗e^{tL_{uau^*}}etLuau∗​ and et∑jLujajuj∗e^{t\sum_jL_{u_ja_ju_j^*}}et∑j​Luj​aj​uj∗​​ lie in the class for a,aj∈Sa,a_j\in Sa,aj​∈S, unitaries u,uju,u_ju,uj​ and t≥0t\ge0t≥0.
  3. Amplitude-damping semigroup ([CW16], p. 8). For a=∣0⟩⟨1∣a=|0\rangle\langle1|a=∣0⟩⟨1∣ on one qubit, etLae^{tL_a}etLa​ has the closed form (ρ00+(1−e−2t)ρ11, e−tρ01; e−tρ10, e−2tρ11)\big(\rho_{00}+(1-e^{-2t})\rho_{11},\ e^{-t}\rho_{01};\ e^{-t}\rho_{10},\ e^{-2t}\rho_{11}\big)(ρ00​+(1−e−2t)ρ11​, e−tρ01​; e−tρ10​, e−2tρ11​).
  4. Dephasing generator (p. 8). On one qubit, LZ=4(E∞−id)L_Z=4(E_\infty-\mathrm{id})LZ​=4(E∞​−id) and etLZ→E∞e^{tL_Z}\to E_\inftyetLZ​→E∞​.
  5. Lemma 2.11(ii). If Z1∈SZ_1\in SZ1​∈S, then E∞⊗idk−1E_\infty\otimes\mathrm{id}^{k-1}E∞​⊗idk−1 and E∞⊗kE_\infty^{\otimes k}E∞⊗k​ lie in the class.
  6. Replacer claim (proof of Theorem 2.12). etLa→R∣0⟩⟨0∣⊗ide^{tL_a}\to\mathcal R_{|0\rangle\langle0|}\otimes\mathrm{id}etLa​→R∣0⟩⟨0∣​⊗id, and both R∣0⟩⟨0∣⊗id\mathcal R_{|0\rangle\langle0|}\otimes\mathrm{id}R∣0⟩⟨0∣​⊗id and R∣0k⟩⟨0k∣\mathcal R_{|0_k\rangle\langle0_k|}R∣0k​⟩⟨0k​∣​ lie in the class.
  7. Lemma 2.11(iii). DS(∣0k⟩⟨0k∣)=D(H)D_S(|0_k\rangle\langle0_k|)=\mathcal D(H)DS​(∣0k​⟩⟨0k​∣)=D(H).

Significance

The result. Full unitary control alone cannot change the spectrum of a state. Theorem 2.12 shows that two dissipative resources acting on one qubit already remove every obstruction. This is close to optimal: Proposition 2.7 of the paper shows that self-adjoint jumps alone produce only unital channels, which fix the maximally mixed state, so at least one non-self-adjoint resource is necessary. The result also needs no convexity. The class contains genuine Markovian semigroups, their compositions and their limits, but no mixtures. The surrounding statements are reusable on their own:

  • every unitary is generated by a Hörmander system (Chow's theorem in the form used here);
  • the pinching and the reset are limits of Lindblad semigroups;
  • the pure state ∣0k⟩|0_k\rangle∣0k​⟩ reaches every density.

Formalizing it. The paper's proof is short, but several steps are stated without detail: "by assumption", "using the conjugation trick and products", and Chow's theorem cited for a semigroup rather than a group. A formal proof fixes exactly what the closure (CL) contributes. It supplies the negative-time unitaries (milestone 1) and the conditional expectations E∞E_\inftyE∞​ and R\mathcal RR (milestones 4–6), none of which is of the form etLe^{tL}etL. No machine-checked proof of these statements is known (a search of the Prove2Me library in October 2026 found none). Mathlib has the matrix exponential, the operator norm on superoperators and Lie subalgebras. It has neither Chow's theorem nor the correspondence between Lie subalgebras and connected subgroups of U(d)U(d)U(d).

Difficulty

The one hard step is milestone 1. (UN) supplies only the forward flows etXe^{tX}etX, t≥0t\ge0t≥0, of the directions in the span of SSS. The Hörmander condition is a statement about the Lie algebra they generate, while the class is a semigroup closed under limits. The naive argument applies the Lie-algebra/Lie-group correspondence directly, but that correspondence speaks about the group generated by the flows etXe^{tX}etX, t∈Rt\in\mathbb Rt∈R. The class contains only nonnegative times and their compositions and limits, so the step from the generated group to the closed semigroup is exactly what has to be supplied.

The remaining milestones are explicit matrix analysis: exponentials of explicit superoperators on one qubit and their limits as t→∞t\to\inftyt→∞, and register swaps. Milestone 7 has two halves. The inclusion ⊇\supseteq⊇ is the construction. The inclusion ⊆\subseteq⊆ requires every element of the closed class, limits included, to be positive and trace-preserving.

Formalization scope

  • Carrier. The basis of C2k\mathbb C^{2^k}C2k is indexed by bit strings Fin k → Bool, with false =∣0⟩=|0\rangle=∣0⟩. Operators are complex matrices on this index set. Superoperators are continuous C\mathbb CC-linear maps with the operator norm over the L2L^2L2-operator norm on matrices. In finite dimension every norm gives the same topology, so closedness and limits do not depend on this choice. Exponentials are NormedSpace.exp on matrices and on superoperators. Milestones 3 and 4 are stated on 2×22\times22×2 matrices indexed by Fin 2, with basis order (∣0⟩,∣1⟩)(|0\rangle,|1\rangle)(∣0⟩,∣1⟩).

  • The class. Channel(S)‾\overline{\mathrm{Channel}(S)}Channel(S)​ is the intersection of all closed sets with (UN), (JU) and (CO). A formalization in which some class with these properties is merely assumed to exist would make the goal trivial (take all superoperators), and is ruled out. Likewise, the Hörmander hypothesis is containment of su(2k)\mathfrak{su}(2^k)su(2k) in the generated real Lie algebra, not in the span of SSS.

  • Conventions committed to.

    • The dissipator has the standard sign 2aρa∗−a∗aρ−ρa∗a2a\rho a^*-a^*a\rho-\rho a^*a2aρa∗−a∗aρ−ρa∗a. The page prints (JU) with the opposite sign, but every computation in the paper uses this one.
    • S=S∗S=S^*S=S∗ means a∈S⇒a∗∈Sa\in S\Rightarrow a^*\in Sa∈S⇒a∗∈S.
    • k≥1k\ge1k≥1 is assumed wherever the first qubit is named; the first qubit is index 000.
    • Proposition 2.2(i) is posed for every unitary UUU, as its proof and its uses read it.
    • The middle term of the page's LZL_ZLZ​ display is a slip; the outer identity LZ=4(E∞−id)L_Z=4(E_\infty-\mathrm{id})LZ​=4(E∞​−id) is posed.
    • In Lemma 2.11(iii), the printed "∣0⟩⟨I∣⊗1k−1|0\rangle\langle I|\otimes 1^{k-1}∣0⟩⟨I∣⊗1k−1" is read as ∣0⟩⟨1∣⊗I⊗(k−1)|0\rangle\langle1|\otimes I^{\otimes(k-1)}∣0⟩⟨1∣⊗I⊗(k−1).
  • Infrastructure needed.

    • Generation of SU(d)SU(d)SU(d) from one-parameter subgroups of a Lie-generating set.
    • Positivity and trace preservation of etLe^{tL}etL for Lindblad LLL, and stability of complete positivity under limits.
    • Exponentials of superoperators that act diagonally on matrix units.
    • Swap and tensor-product manipulations on bit-string indices.

    The first two are reusable well beyond this mission. Proofs of individual milestones, and of general lemmas on Lindblad semigroups, are welcome.

Selected references

  • J. Cai, A. Govindarajan, M. Junge, How Far do Lindbladians Go?, arXiv preprint, v2, 2025. https://arxiv.org/abs/2504.04883
  • 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
  • G. Lindblad, On the generators of quantum dynamical semigroups, Comm. Math. Phys. 48 (1976) 119–130. https://doi.org/10.1007/BF01608499
  • W.-L. Chow, Über Systeme von linearen partiellen Differentialgleichungen erster Ordnung, Math. Ann. 117 (1940) 98–105. https://doi.org/10.1007/BF01450011
  • R. W. Brockett, System theory on group manifolds and coset spaces, SIAM J. Control 10 (1972) 265–284. https://doi.org/10.1137/0310021
  • V. Jurdjevic, H. J. Sussmann, Control systems on Lie groups, J. Differential Equations 12 (1972) 313–329. https://doi.org/10.1016/0022-0396(72)90035-6
  • R. Cleve, C. Wang, Efficient quantum algorithms for simulating Lindblad evolution, arXiv preprint, 2016. https://arxiv.org/abs/1612.09512
  • R. Araiza, Y. Chen, M. Junge, P. Wu, Resource-dependent complexity of quantum channels, arXiv preprint, 2023. https://arxiv.org/abs/2303.11304
  • F. Verstraete, M. M. Wolf, J. I. Cirac, Quantum computation and quantum-state engineering driven by dissipation, Nature Physics 5 (2009) 633–636. https://doi.org/10.1038/nphys1342
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CombinatoricsNumber Theory·Captain: Ethan Cheung Wang

Erdős #195: monotone 444-term APs in permutations of Z\mathbb{Z}ZOpen Problem

Motivation

A permutation of Z\mathbb{Z}Z in the sense of Erdős and Graham is a one-sided arrangement a0,a1,a2,…a_0, a_1, a_2, \ldotsa0​,a1​,a2​,… in which every integer appears exactly once. Erdős Problem 195 (erdosproblems.com/195) asks for the largest kkk such that every such arrangement contains a monotone kkk-term arithmetic progression: indices i1<⋯<iki_1 < \cdots < i_ki1​<⋯<ik​ for which ai1,…,aika_{i_1}, \ldots, a_{i_k}ai1​​,…,aik​​ is an increasing or a decreasing arithmetic progression. The question sits in the Ramsey-type study of how much arithmetic structure an ordering is forced to preserve, alongside its companion Problem 196 for permutations of N\mathbb{N}N.

Timeline of the known results:

  • 1977. Davis, Entringer, Graham and Simmons (Acta Arith. 34) proved that every permutation of the positive integers contains a monotone 3-term progression, and that the positive integers can be permuted to avoid monotone 5-term progressions. Since the positive entries of a permutation of Z\mathbb{Z}Z form a permutation of the positive integers, every permutation of Z\mathbb{Z}Z contains a monotone 3-term progression.
  • 2019. Geneson (Discrete Math. 342) constructed a permutation of Z\mathbb{Z}Z with no monotone 6-term progression, so the answer is at most 5.
  • 2022–2024. Adenwalla (arXiv:2211.04451, Discrete Math. 347 (2024) 114183) constructed a permutation of Z\mathbb{Z}Z with no monotone 5-term progression, so the answer is at most 4.
  • 2026. Ho (arXiv:2609.12780) constructed a permutation of N\mathbb{N}N with no monotone 4-term progression, settling Problem 196, with a complete Lean 4 proof (github.com/boonsuan/4ap). Geneson (arXiv:2608.12604) proved βZ(4)=1\beta_{\mathbb{Z}}(4)=1βZ​(4)=1: there are sets of integers with lower density arbitrarily close to 111 that can be permuted to avoid monotone 4-term progressions.

The answer to Problem 195 is therefore 333 or 444, and it is 333 exactly when some permutation of Z\mathbb{Z}Z avoids monotone 4-term progressions.

Setting

A permutation of Z\mathbb{Z}Z is a bijection f:N→Zf : \mathbb{N} \to \mathbb{Z}f:N→Z. A list of values is an arithmetic progression of length kkk if it equals a,a+d,…,a+(k−1)da, a+d, \ldots, a+(k-1)da,a+d,…,a+(k−1)d or the same list reversed. The function fff has a monotone kkk-AP if there are indices b1<⋯<bkb_1 < \cdots < b_kb1​<⋯<bk​ such that f(b1),…,f(bk)f(b_1), \ldots, f(b_k)f(b1​),…,f(bk​) is an arithmetic progression of length kkk. For a bijection the common difference is automatically nonzero when k≥2k \ge 2k≥2.

Auxiliary objects used by the milestones:

  1. For ε:N→{true,false}\varepsilon : \mathbb{N} \to \{\mathrm{true},\mathrm{false}\}ε:N→{true,false}, the ε\varepsilonε-order ≺ε\prec_\varepsilon≺ε​ on Z\mathbb{Z}Z: for x≠yx \ne yx=y, let k=ν2(y−x)k = \nu_2(y-x)k=ν2​(y−x) be the lowest binary position at which the two's-complement expansions of xxx and yyy differ; then x≺εyx \prec_\varepsilon yx≺ε​y iff the kkk-th digit of xxx is 111 exactly when ε(k)\varepsilon(k)ε(k) is true. With ε≡true\varepsilon \equiv \mathrm{true}ε≡true this is the extension to Z\mathbb{Z}Z of the order used by Ho.
  2. For a relation RRR and a finite duplicate-free word PPP of integers, the completion C(P)C(P)C(P) lists PPP first, in order, followed by all other integers ordered by RRR. The word PPP is safe if C(P)C(P)C(P) has no monotone 4-term progression.
  3. (No3AP): RRR has no monotone 3-term progression. (Star): aRa+r  ⟺  a+2rRa+3ra \mathrel{R} a+r \iff a+2r \mathrel{R} a+3raRa+r⟺a+2rRa+3r for every aaa and every r≠0r \ne 0r=0.

Formalization targets

Goal

∃f:N≃Z, f has no monotone 4-term arithmetic progression.\exists f : \mathbb{N} \simeq \mathbb{Z},\ f \text{ has no monotone 4-term arithmetic progression.}∃f:N≃Z, f has no monotone 4-term arithmetic progression.

Together with the known bounds this is equivalent to the answer to Problem 195 being 333. A disproof would show that the answer is 444.

Literature milestones

∀f:N≃Z, f has a monotone 3-AP,∃f:N≃Z with no monotone 5-AP,∃f:N≃N with no monotone 4-AP,\forall f : \mathbb{N} \simeq \mathbb{Z},\ f \text{ has a monotone 3-AP}, \qquad \exists f : \mathbb{N}\simeq\mathbb{Z} \text{ with no monotone 5-AP}, \qquad \exists f : \mathbb{N} \simeq \mathbb{N} \text{ with no monotone 4-AP},∀f:N≃Z, f has a monotone 3-AP,∃f:N≃Z with no monotone 5-AP,∃f:N≃N with no monotone 4-AP,

and the reduction: the supremum in the formal-conjectures statement equals 333 iff the goal holds.

Structural milestones

The ε\varepsilonε-orders are strict total orders with no monotone 3-term progression that satisfy (Star). They have no endpoints when ε\varepsilonε is not eventually constant. In every ε\varepsilonε-order, a word listed in reverse order is safe. Conversely, a least element blocks every exhaustive chain of safe words, and the two's-complement order has least element −1-1−1.

Significance

A proof of the goal resolves Problem 195, determines the answer as 333, and completes the classification of monotone progressions in one-sided permutations of N\mathbb{N}N and Z\mathbb{Z}Z. A disproof gives the answer 444 and is the first known statement separating the two problems. The formal-conjectures repository (195.lean) records the problem as open with an unspecified answer. The literature milestones have pen-and-paper proofs. Among them, only Ho's theorem for N\mathbb{N}N has a machine-checked proof, in an external repository, so porting it is part of the work.

Difficulty

The natural first attempt transfers Ho's construction for N\mathbb{N}N to Z\mathbb{Z}Z. Ho's argument builds the permutation as a limit of finite safe words. Each extension step uses that all values are nonnegative: for a progression a,b,c,da, b, c, da,b,c,d with ccc and ddd not yet placed, the bound d=2c−b≤2cd = 2c - b \le 2cd=2c−b≤2c controls which elements are forced. On Z\mathbb{Z}Z this bound is lost. With the two's-complement completion order the obstruction is concrete: −1-1−1 is the least element, and once it is placed no later element can be the maximum or minimum of a safe word, so no chain of safe words can exhaust Z\mathbb{Z}Z. Any approach along these lines must therefore change the completion order between stages, for example through orders without endpoints, or use a different construction entirely.

Formalization scope

Permutations are f : ℕ ≃ ℤ. HasMonotoneAP, ListIsAPOfLength and ListIsAPOfLengthWith copy the formal-conjectures definitions verbatim, so the goal and the reduction milestone use the same objects as Erdos195.erdos_195. Progressions may be listed forwards or backwards, which covers increasing and decreasing ones. A zero common difference never arises because f is injective. Digits are two's-complement digits x / 2^k % 2 with floor division, and ν₂ is padicValInt 2. Safe quantifies over all integers a and all nonzero r of either sign. Everything lives in the namespace Erdos195.

The development needs only Mathlib's integers, lists and ppp-adic valuations. The ε\varepsilonε-order lemmas and the completion lemmas are reusable for related arrangement problems, including Problem 196 and doubly infinite variants. Contributions are welcome on the literature milestones (in particular a port of Ho's Lean proof), on new orders with no endpoints, and on the goal in either direction.

Selected references

  • J. A. Davis, R. C. Entringer, R. L. Graham, G. J. Simmons, On permutations containing no long arithmetic progressions, Acta Arith. 34 (1977), 81–90. https://doi.org/10.4064/aa-34-1-81-90
  • J. Geneson, Forbidden arithmetic progressions in permutations of subsets of the integers, Discrete Math. 342 (2019), 1489–1491. https://doi.org/10.1016/j.disc.2019.02.004
  • S. Adenwalla, Avoiding monotone arithmetic progressions in permutations of integers, Discrete Math. 347 (2024), 114183. https://arxiv.org/abs/2211.04451
  • B. S. Ho, A 4AP-free permutation of the positive integers, arXiv:2609.12780 (2026). https://arxiv.org/abs/2609.12780 ; Lean proof https://github.com/boonsuan/4ap
  • J. Geneson, Density bounds for permutations avoiding monotone arithmetic progressions, arXiv:2608.12604 (2026). https://arxiv.org/abs/2608.12604
  • Erdős Problem 195, https://www.erdosproblems.com/195 ; formal-conjectures ErdosProblems/195.lean.
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Algorithmic Game TheoryBandit AlgorithmsMachine Learning+1·Captain: mikedeng1

V-Learning—A Simple, Efficient, Decentralized Algorithm for Multiagent Reinforcement Learning: Independent V-Learning Finds a Coarse Correlated Equilibrium with Gap O((H²S/K)Ξ(A,K/S,ι) + √(H⁵Sι/K))Research Paper

Motivation

In multi-agent reinforcement learning several agents act in a shared, changing environment, each pursuing its own reward. The standard model is the Markov game (stochastic game), going back to Shapley (1953). When agents learn from experience rather than from a known model, the natural target is an equilibrium of the game, and the natural question is how many episodes of play are needed to find one.

Before V-learning, sample-efficient algorithms for general-sum Markov games were centralized and model-based: they estimated quantities indexed by the joint action, so their sample complexity grew with ∏j=1mAj\prod_{j=1}^m A_j∏j=1m​Aj​, exponentially in the number of players mmm. This is the curse of multiagents. Jin, Liu, Wang and Yu (arXiv:2110.14555, journal version in Mathematics of Operations Research, 2024) introduced V-learning, in which every agent runs its own simple algorithm, sees only its own reward and the states, and never needs the other agents' actions. Theorem 6 of the paper shows that the agents' combined output is an approximate coarse correlated equilibrium (CCE) after a number of episodes polynomial in HHH, SSS and max⁡jAj\max_j A_jmaxj​Aj​ only.

Timeline:

  • 2018: Jin, Allen-Zhu, Bubeck and Jordan analyse optimistic Q-learning with the learning rate αt=(H+1)/(H+t)\alpha_t=(H+1)/(H+t)αt​=(H+1)/(H+t), the rate V-learning reuses (arXiv:1807.03765).
  • 2020: Bai and Jin (arXiv:2002.04017) and Xie et al. give the first sample-efficient algorithms for two-player zero-sum Markov games, based on optimistic value iteration. Bai, Jin and Yu (arXiv:2006.12007, NeurIPS 2020) introduce V-learning, coupled with FTRL, for Nash equilibria of two-player zero-sum games.
  • 2021: Liu, Yu, Bai and Jin (arXiv:2010.01604, ICML 2021) learn Nash, CE and CCE of multi-player general-sum games with a centralized model-based method in O(H4S2∏jAj/ε2)O(H^4S^2\prod_jA_j/\varepsilon^2)O(H4S2∏j​Aj​/ε2) episodes.
  • 2021: the present paper (arXiv v1, 27 October 2021) presents V-learning as a generic class of algorithms with any adversarial bandit subroutine and proves Theorem 6; two concurrent works (references [32] and [47] of the paper) obtain CCE guarantees for V-learning-style algorithms with one more factor of HHH.

Setting

A tabular episodic mmm-player Markov game has SSS states, episodes of HHH steps, and AjA_jAj​ actions for player jjj; A=max⁡jAjA=\max_jA_jA=maxj​Aj​. At step hhh in state sss the players choose actions simultaneously, forming a joint action a\boldsymbol aa; player jjj receives the deterministic reward rj,h(s,a)∈[0,1]r_{j,h}(s,\boldsymbol a)\in[0,1]rj,h​(s,a)∈[0,1], and the next state is drawn from Ph(⋅∣s,a)\mathbb P_h(\cdot\mid s,\boldsymbol a)Ph​(⋅∣s,a). Every episode starts at a fixed state s1s_1s1​.

A joint policy π\piπ may be correlated: the players share a random seed. Vj,1π(s1)V^\pi_{j,1}(s_1)Vj,1π​(s1​) is player jjj's expected total reward. The best response value Vj,1†,π−j(s1)V^{\dagger,\pi_{-j}}_{j,1}(s_1)Vj,1†,π−j​​(s1​) is the largest value player jjj can obtain by switching to a policy of its own, independent of the shared seed, while the others keep playing π−j\pi_{-j}π−j​. A joint policy is an ε\varepsilonε-CCE if max⁡j(Vj,1†,π−j−Vj,1π)(s1)≤ε\max_j\big(V^{\dagger,\pi_{-j}}_{j,1}-V^\pi_{j,1}\big)(s_1)\le\varepsilonmaxj​(Vj,1†,π−j​​−Vj,1π​)(s1​)≤ε.

V-learning (Algorithm 1). Each player keeps, for every state sss and step hhh, a visit count Nh(s)N_h(s)Nh​(s), a value estimate Vj,h(s)V_{j,h}(s)Vj,h​(s) and an adversarial bandit algorithm. After visiting sss at step hhh for the ttt-th time it updates

V~j,h(s)←(1−αt)V~j,h(s)+αt(rj,h+Vj,h+1(sh+1)+βj,t),Vj,h(s)←min⁡{H+1−h,V~j,h(s)},\tilde V_{j,h}(s)\leftarrow(1-\alpha_t)\tilde V_{j,h}(s)+\alpha_t\big(r_{j,h}+V_{j,h+1}(s_{h+1})+\beta_{j,t}\big),\qquad V_{j,h}(s)\leftarrow\min\{H+1-h,\tilde V_{j,h}(s)\},V~j,h​(s)←(1−αt​)V~j,h​(s)+αt​(rj,h​+Vj,h+1​(sh+1​)+βj,t​),Vj,h​(s)←min{H+1−h,V~j,h​(s)},

with αt=(H+1)/(H+t)\alpha_t=(H+1)/(H+t)αt​=(H+1)/(H+t) and a bonus βj,t\beta_{j,t}βj,t​, and feeds the loss (H−rj,h−Vj,h+1(sh+1))/H(H-r_{j,h}-V_{j,h+1}(s_{h+1}))/H(H−rj,h​−Vj,h+1​(sh+1​))/H of its own action to the (s,h)(s,h)(s,h)-th bandit, whose next strategy becomes the policy at (s,h)(s,h)(s,h). The weights αti=αi∏j=i+1t(1−αj)\alpha^i_t=\alpha_i\prod_{j=i+1}^t(1-\alpha_j)αti​=αi​∏j=i+1t​(1−αj​) express V~\tilde VV~ as a weighted average of past updates.

The bandit subroutine must satisfy Assumption 1: against any adaptive adversary with noisy, conditionally unbiased feedback, with probability at least 1−δ1-\delta1−δ the αti\alpha^i_tαti​-weighted regret after ttt rounds is at most ξ(B,t,log⁡(1/δ))\xi(B,t,\log(1/\delta))ξ(B,t,log(1/δ)), where ξ\xiξ is non-decreasing in the number of arms BBB and has a partial-sum upper bound Ξ(B,t,⋅)\Xi(B,t,\cdot)Ξ(B,t,⋅) concave in ttt.

The output policy π^\hat\piπ^ (Algorithm 3) samples an episode index kkk uniformly from [K][K][K]; at each step, in state sss with t=Nhk(s)t=N^k_h(s)t=Nhk​(s) earlier visits in episodes k1<⋯<ktk^1<\dots<k^tk1<⋯<kt, it samples iii with probability αti\alpha^i_tαti​, sets k←kik\leftarrow k^ik←ki, and plays the policies the players held at the beginning of episode kik^iki. For the CCE all players use the same sample iii (shared seed, §5.1).

Formalization targets

Goal: Theorem 6

With ι=log⁡(mHSAK/δ)\iota=\log(mHSAK/\delta)ι=log(mHSAK/δ) and bonuses satisfying ∑i=1tαtiβj,i=Θ(Hξ(Aj,t,ι)+H3ι/t)\sum_{i=1}^t\alpha^i_t\beta_{j,i}=\Theta\big(H\xi(A_j,t,\iota)+\sqrt{H^3\iota/t}\big)∑i=1t​αti​βj,i​=Θ(Hξ(Aj​,t,ι)+H3ι/t​) for t∈[K]t\in[K]t∈[K], with probability at least 1−δ1-\delta1−δ

max⁡j∈[m][Vj,1†,π^−j(s1)−Vj,1π^(s1)]≤O(H2SK Ξ(A,K/S,ι)+H5SιK).\max_{j\in[m]}\Big[V^{\dagger,\hat\pi_{-j}}_{j,1}(s_1)-V^{\hat\pi}_{j,1}(s_1)\Big]\le O\Big(\frac{H^2S}{K}\,\Xi(A,K/S,\iota)+\sqrt{\frac{H^5S\iota}{K}}\Big).j∈[m]max​[Vj,1†,π^−j​​(s1​)−Vj,1π^​(s1​)]≤O(KH2S​Ξ(A,K/S,ι)+KH5Sι​​).

The goal leaves the bandit algorithm abstract: it holds for every subroutine satisfying Assumption 1.

Milestones

  1. Lemma 10: the properties of the weights αti\alpha^i_tαti​.
  2. Lemma 11: V~\tilde VV~ as a weighted sum of past updates.
  3. Lemma 12: Assumption 1 transported to every (s,h,j)(s,h,j)(s,h,j)-bandit of the run, with failure probability δ\deltaδ.
  4. Lemma 13 (optimism): Vj,hk≥Vj,h†,π^−j,hkV^k_{j,h}\ge V^{\dagger,\hat\pi^k_{-j,h}}_{j,h}Vj,hk​≥Vj,h†,π^−j,hk​​.
  5. Lemma 14 (pessimism): V‾j,hk≤Vj,hπ^hk\underline V^k_{j,h}\le V^{\hat\pi^k_h}_{j,h}V​j,hk​≤Vj,hπ^hk​​ for the analysis-only estimate V‾\underline VV​.
  6. The summed gap ∑kmax⁡j[Vj,1k−V‾j,1k](s1)≤O(H2SΞ(A,K/S,ι)+H5SKι)\sum_k\max_j[V^k_{j,1}-\underline V^k_{j,1}](s_1)\le O(H^2S\Xi(A,K/S,\iota)+\sqrt{H^5SK\iota})∑k​maxj​[Vj,1k​−V​j,1k​](s1​)≤O(H2SΞ(A,K/S,ι)+H5SKι​) (p. 24).

Two further steps of the proof of Theorem 6 are included as items without milestone status: the one-step recursion of δhk=max⁡j(Vj,hk−V‾j,hk)(shk)\delta^k_h=\max_j(V^k_{j,h}-\underline V^k_{j,h})(s^k_h)δhk​=maxj​(Vj,hk​−V​j,hk​)(shk​) (p. 23) and the pigeonhole bound on the summed bonus terms (pp. 23–24).

Significance

With the FTRL subroutine of the paper (Corollary 19: Ξ(B,t,log⁡(1/δ))=20HBtlog⁡(B/δ)\Xi(B,t,\log(1/\delta))=20\sqrt{HBt\log(B/\delta)}Ξ(B,t,log(1/δ))=20HBtlog(B/δ)​), Theorem 6 gives an ε\varepsilonε-CCE after O~(H5SA/ε2)\tilde O(H^5SA/\varepsilon^2)O~(H5SA/ε2) episodes, against H4S2∏jAj/ε2H^4S^2\prod_jA_j/\varepsilon^2H4S2∏j​Aj​/ε2 for the earlier centralized method. The same analysis, with a swap-regret subroutine, gives correlated equilibria (Theorem 7) and, specialized to two players with opposite rewards, Nash equilibria of zero-sum games (Theorem 5). The algorithm is decentralized: each agent's computation depends only on the visited states and its own actions and rewards.

The result is proved in the paper; to our knowledge no part of it has been machine-checked. A formalization adds a precise statement of what "independent learning finds a CCE" means for non-Markov, history-dependent output policies, and of the adversary class Assumption 1 must cover for the reduction from the Markov game to the bandits to go through. It also makes explicit the boundary cases the paper leaves implicit (first visits, the last step, the initialization of V~\tilde VV~).

Difficulty

The deterministic steps (Lemmas 10–11, the recursion and the pigeonhole bound) are algebra on weighted sums. The difficulty is probabilistic. Lemma 12 must view each (s,h,j)(s,h,j)(s,h,j)-bandit as playing against an adversary formed by the rest of the run: the other players, the transitions and the player's own other bandits, all adapted to the past. Lemmas 13 and 14 need concentration of αti\alpha^i_tαti​-weighted martingale sums over random visit times, uniformly over all states, steps, episodes and players.

The best response is the other obstacle. The output policy is not Markov: it carries a latent episode index. The opponent of π^−j\hat\pi_{-j}π^−j​ may use the whole history of states and joint actions, and the best response to a non-Markov policy is not given by a Bellman equation. Lemma 13's step (v) handles this; the obvious per-state argument does not apply.

Formalization scope

Everything is finite and real-valued. States, players, actions, steps and episodes are Fin types; steps and episodes are 0-based, so the cap H+1−hH+1-hH+1−h is H - h. The bandit rule is a deterministic function from the feedback history to a probability vector, starting uniform. The adversaries of Assumption 1 range over a finitary class: private randomness in an arbitrary finite type, losses chosen from the past before the learner's action, and conditionally unbiased feedback in [0,1][0,1][0,1]. The training law is a finite product of policy and transition probabilities, and every probability is a finite sum over episode sequences. The best response is a supremum over deterministic history-dependent deviations, taken outside the average over the output policy's initial index. Θ\ThetaΘ and OOO are read with a universal lower constant c0c_0c0​ before every instance and an OOO-constant depending only on the upper constant c1c_1c1​.

Added hypotheses, each disclosed in its item: nonnegative bonuses; K≥1K\ge1K≥1; per-player bandit rules sharing one ξ\xiξ; ξ≥0\xi\ge0ξ≥0 in the pigeonhole step and the summed-gap milestone; mHSAK≥2mHSAK\ge2mHSAK≥2 in milestone 6, whose printed form is false without it. The output policy's convention at a first visit (t=0t=0t=0) keeps the current index and plays the uniform initial policy.

Two formalizations would trivialize the goal and are ruled out: an Assumption 1 that no algorithm satisfies (a sorry-free check shows every valid rule satisfies it with ξ≡1\xi\equiv1ξ≡1), and a best response averaged per latent index or restricted to Markov deviations.

Needed infrastructure: weighted martingale concentration (Azuma–Hoeffding is on the platform), finite-sum manipulation of the training law, and Jensen's inequality for concave functions. Contributions to any milestone are welcome; the deterministic milestones 1, 2 and 6, and the recursion and pigeonhole steps, are independent of the probabilistic ones.

Selected references

  • C. Jin, Q. Liu, Y. Wang, T. Yu, V-Learning—A Simple, Efficient, Decentralized Algorithm for Multiagent RL, arXiv:2110.14555v1, 2021; Mathematics of Operations Research, 2024. https://arxiv.org/abs/2110.14555
  • C. Jin, Z. Allen-Zhu, S. Bubeck, M. I. Jordan, Is Q-learning Provably Efficient?, NeurIPS 2018. https://arxiv.org/abs/1807.03765
  • Y. Bai, C. Jin, Provable Self-Play Algorithms for Competitive Reinforcement Learning, ICML 2020. https://arxiv.org/abs/2002.04017
  • Y. Bai, C. Jin, T. Yu, Near-Optimal Reinforcement Learning with Self-Play, NeurIPS 2020. https://arxiv.org/abs/2006.12007
  • Q. Liu, T. Yu, Y. Bai, C. Jin, A Sharp Analysis of Model-based Reinforcement Learning with Self-Play, ICML 2021. https://arxiv.org/abs/2010.01604
  • L. S. Shapley, Stochastic Games, PNAS 39(10), 1953. https://doi.org/10.1073/pnas.39.10.1095
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Calculus of VariationsMachine LearningOptimization+1·Captain: mikedeng1

Game on Random Environment, Mean-Field Langevin System, and Neural Networks: First-Order Condition for Entropy-Regularized Minimization over Probability Measures with a Fixed MarginalResearch Paper

Motivation

Several problems in machine learning and game theory are optimization problems over probability measures. Training a wide two-layer neural network can be viewed as minimizing a functional F(ν)F(\nu)F(ν) of the distribution ν\nuν of the network's parameters (Mei, Montanari, Nguyen, PNAS 2018; Hu, Ren, Šiška, Szpruch, arXiv:1905.07769). Adding a relative-entropy penalty ηH(ν)\eta H(\nu)ηH(ν) makes the problem strictly convex in the density and connects its minimizers to the invariant measures of Langevin-type diffusions, the mean-field Langevin dynamics. The first-order condition for the unconstrained problem is Hu et al., Proposition 2.4.

Conforti, Kazeykina and Ren (arXiv:2004.02457v2) add a random environment: a variable yyy with a fixed law m\mathsf mm that every player observes, such as the time index in a dynamic game or a shared signal. The strategies are then probability measures on Rd×Y\mathbb R^d\times\mathbb YRd×Y whose Y\mathbb YY-marginal is prescribed. Their Theorem 3.1 extends the first-order condition to this constrained problem. The introduction names it "one of our main contributions": it gives the necessary condition for Nash equilibria of games on a random environment (Corollary 3.3), and it identifies the invariant measure of the mean-field Langevin system studied in the rest of the paper.

Setting

Let Y\mathbb YY be a Polish space with a probability measure m\mathsf mm, and let p≥1p\ge1p≥1. Write Rˉd=Rd×Y\bar{\mathbb R}^d=\mathbb R^d\times\mathbb YRˉd=Rd×Y and xˉ=(x,y)\bar x=(x,y)xˉ=(x,y). The strategy set is

Π={πˉ∈Pp(Rˉd): πˉ(Rd,⋅)=m},\Pi=\{\bar\pi\in\mathcal P_p(\bar{\mathbb R}^d):\ \bar\pi(\mathbb R^d,\cdot)=\mathsf m\},Π={πˉ∈Pp​(Rˉd): πˉ(Rd,⋅)=m},

the probability measures on Rˉd\bar{\mathbb R}^dRˉd with finite ppp-th moment and Y\mathbb YY-marginal m\mathsf mm. By disintegration, πˉ(dxˉ)=π(dx∣y) m(dy)\bar\pi(d\bar x)=\pi(dx|y)\,\mathsf m(dy)πˉ(dxˉ)=π(dx∣y)m(dy).

A function F:Π→RF:\Pi\to\mathbb RF:Π→R has a linear functional derivative δFδπˉ:Π×Rˉd→R\frac{\delta F}{\delta\bar\pi}:\Pi\times\bar{\mathbb R}^d\to\mathbb RδπˉδF​:Π×Rˉd→R if for all ν,ν′∈Π\nu,\nu'\in\Piν,ν′∈Π

F(ν′)−F(ν)=∫01∫RˉdδFδπˉ((1−λ)ν+λν′,xˉ) (ν′−ν)(dxˉ) dλ.(2.1)F(\nu')-F(\nu)=\int_0^1\int_{\bar{\mathbb R}^d}\frac{\delta F}{\delta\bar\pi}\big((1-\lambda)\nu+\lambda\nu',\bar x\big)\,(\nu'-\nu)(d\bar x)\,d\lambda. \tag{2.1}F(ν′)−F(ν)=∫01​∫Rˉd​δπˉδF​((1−λ)ν+λν′,xˉ)(ν′−ν)(dxˉ)dλ.(2.1)

Assumption 2.1 asks that FFF have such a derivative, that FFF and δFδπˉ(⋅,xˉ)\frac{\delta F}{\delta\bar\pi}(\cdot,\bar x)δπˉδF​(⋅,xˉ) be continuous for the ppp-Wasserstein distance Wp\mathcal W_pWp​, that δFδπˉ(πˉ,⋅,y)\frac{\delta F}{\delta\bar\pi}(\bar\pi,\cdot,y)δπˉδF​(πˉ,⋅,y) be continuously differentiable in xxx, and that sup⁡πˉ∈Π∣δFδπˉ(πˉ,xˉ)∣≤C(1+∣xˉ∣p)\sup_{\bar\pi\in\Pi}|\frac{\delta F}{\delta\bar\pi}(\bar\pi,\bar x)|\le C(1+|\bar x|^p)supπˉ∈Π​∣δπˉδF​(πˉ,xˉ)∣≤C(1+∣xˉ∣p).

The regularizer is the relative entropy with respect to Leb×m\mathrm{Leb}\times\mathsf mLeb×m: if πˉ\bar\piπˉ has density π(x∣y)\pi(x|y)π(x∣y) with respect to Leb×m\mathrm{Leb}\times\mathsf mLeb×m, then H(πˉ)=∫ln⁡π(x∣y) πˉ(dxˉ)H(\bar\pi)=\int\ln\pi(x|y)\,\bar\pi(d\bar x)H(πˉ)=∫lnπ(x∣y)πˉ(dxˉ), and H(πˉ)=+∞H(\bar\pi)=+\inftyH(πˉ)=+∞ otherwise. For η>0\eta>0η>0 the objective is

V(πˉ)=F(πˉ)+ηH(πˉ).V(\bar\pi)=F(\bar\pi)+\eta H(\bar\pi).V(πˉ)=F(πˉ)+ηH(πˉ).

Formalization targets

Goal: Theorem 3.1 (p. 4)

If πˉ∗∈argmin⁡πˉ∈ΠV(πˉ)\bar\pi^*\in\operatorname{argmin}_{\bar\pi\in\Pi}V(\bar\pi)πˉ∗∈argminπˉ∈Π​V(πˉ), then πˉ∗\bar\pi^*πˉ∗ has a density π∗(x∣y)\pi^*(x|y)π∗(x∣y) which, for m\mathsf mm-a.e. yyy, is positive with ln⁡π∗(⋅∣y)\ln\pi^*(\cdot|y)lnπ∗(⋅∣y) differentiable and

∇xδFδπˉ(πˉ∗,x,y)+η∇xln⁡π∗(x∣y)=0for all x∈Rd.(3.1)\nabla_x\frac{\delta F}{\delta\bar\pi}(\bar\pi^*,x,y)+\eta\nabla_x\ln\pi^*(x|y)=0\qquad\text{for all }x\in\mathbb R^d. \tag{3.1}∇x​δπˉδF​(πˉ∗,x,y)+η∇x​lnπ∗(x∣y)=0for all x∈Rd.(3.1)

Conversely, if FFF is also convex on Π\PiΠ, every πˉ∗∈Π\bar\pi^*\in\Piπˉ∗∈Π satisfying (3.1) minimizes VVV over Π\PiΠ. The goal states both directions, as printed.

Milestones (proof of Theorem 3.1, §5.1, pp. 9–11)

  1. Step 1 (p. 9): for πˉ,πˉ∗∈Π\bar\pi,\bar\pi^*\in\Piπˉ,πˉ∗∈Π and πˉλ=λπˉ+(1−λ)πˉ∗\bar\pi^\lambda=\lambda\bar\pi+(1-\lambda)\bar\pi^*πˉλ=λπˉ+(1−λ)πˉ∗, 1ε∫0ε∫δFδπˉ(πˉλ,⋅) d(πˉ−πˉ∗) dλ→∫δFδπˉ(πˉ∗,⋅) d(πˉ−πˉ∗)\frac1\varepsilon\int_0^\varepsilon\int\frac{\delta F}{\delta\bar\pi}(\bar\pi^\lambda,\cdot)\,d(\bar\pi-\bar\pi^*)\,d\lambda\to\int\frac{\delta F}{\delta\bar\pi}(\bar\pi^*,\cdot)\,d(\bar\pi-\bar\pi^*)ε1​∫0ε​∫δπˉδF​(πˉλ,⋅)d(πˉ−πˉ∗)dλ→∫δπˉδF​(πˉ∗,⋅)d(πˉ−πˉ∗).
  2. (5.1) (p. 10): for a minimizer πˉ∗\bar\pi^*πˉ∗ and πˉ∈Π\bar\pi\in\Piπˉ∈Π with H(πˉ)<∞H(\bar\pi)<\inftyH(πˉ)<∞, 0≤∫(δFδπˉ(πˉ∗,⋅)+ηln⁡π∗) d(πˉ−πˉ∗)0\le\int\big(\frac{\delta F}{\delta\bar\pi}(\bar\pi^*,\cdot)+\eta\ln\pi^*\big)\,d(\bar\pi-\bar\pi^*)0≤∫(δπˉδF​(πˉ∗,⋅)+ηlnπ∗)d(πˉ−πˉ∗).
  3. (5.2) (p. 10): for a minimizer, Ξy=δFδπˉ(πˉ∗,⋅,y)+ηln⁡π∗(⋅∣y)\Xi_y=\frac{\delta F}{\delta\bar\pi}(\bar\pi^*,\cdot,y)+\eta\ln\pi^*(\cdot|y)Ξy​=δπˉδF​(πˉ∗,⋅,y)+ηlnπ∗(⋅∣y) is π∗(⋅∣y)\pi^*(\cdot|y)π∗(⋅∣y)-a.s. constant for m\mathsf mm-a.e. yyy.
  4. Step 3 (p. 11): a minimizer is equivalent to Leb×m\mathrm{Leb}\times\mathsf mLeb×m.
  5. Sufficiency, FFF-part (p. 11): for convex FFF, F(πˉ)−F(πˉ∗)≥∫δFδπˉ(πˉ∗,⋅) d(πˉ−πˉ∗)F(\bar\pi)-F(\bar\pi^*)\ge\int\frac{\delta F}{\delta\bar\pi}(\bar\pi^*,\cdot)\,d(\bar\pi-\bar\pi^*)F(πˉ)−F(πˉ∗)≥∫δπˉδF​(πˉ∗,⋅)d(πˉ−πˉ∗).
  6. Sufficiency, entropy part (p. 11): under (3.1), H(πˉ)−H(πˉ∗)≥∫ln⁡π∗ d(πˉ−πˉ∗)H(\bar\pi)-H(\bar\pi^*)\ge\int\ln\pi^*\,d(\bar\pi-\bar\pi^*)H(πˉ)−H(πˉ∗)≥∫lnπ∗d(πˉ−πˉ∗).

Significance

Theorem 3.1 says that each fibre of an entropy-regularized minimizer is a Gibbs measure, π∗(x∣y)∝exp⁡(−1ηδFδπˉ(πˉ∗,x,y))\pi^*(x|y)\propto\exp\big(-\frac1\eta\frac{\delta F}{\delta\bar\pi}(\bar\pi^*,x,y)\big)π∗(x∣y)∝exp(−η1​δπˉδF​(πˉ∗,x,y)). In the paper this yields the Nash-equilibrium condition (3.2) for nnn-player games on a random environment, the uniqueness of equilibria under a monotonicity condition (Corollary 3.4), and the identification of the stationary measures of the mean-field Langevin system (2.2) with these equilibria, the basis of the convergence results (Theorems 3.8–3.12). For a one-player problem it is the optimality condition behind gradient-descent training of mean-field neural networks with an environment variable.

The result is proved in the paper; it is not formalized anywhere known. The mission produces the first machine-checked first-order condition for optimization over probability measures, with or without a marginal constraint, and the supporting objects: the strategy set Π\PiΠ, the linear functional derivative, and relative entropy with respect to the infinite reference measure Leb×m\mathrm{Leb}\times\mathsf mLeb×m. The unconstrained case (Y\mathbb YY a point) is a special case.

Difficulty

The sufficiency direction is two convexity inequalities and a cancellation of the yyy-dependent constants, which uses the common marginal m\mathsf mm. The necessity direction is harder. The first variation of VVV at πˉ∗\bar\pi^*πˉ∗ gives only an inequality (5.1) in the directions πˉ−πˉ∗\bar\pi-\bar\pi^*πˉ−πˉ∗ with H(πˉ)<∞H(\bar\pi)<\inftyH(πˉ)<∞, and the entropy's difference quotient is not dominated where π∗\pi^*π∗ is small, so the limit requires a one-sided Fatou argument. The inequality (5.1) is not yet a pointwise equation. Converting it into "Ξy\Xi_yΞy​ is constant" needs admissible competitors with bounded density relative to πˉ∗\bar\pi^*πˉ∗, built fibre by fibre in yyy, and these only reach the support of πˉ∗\bar\pi^*πˉ∗. Ruling out zeros of π∗\pi^*π∗ (Step 3) needs a separate competitor that charges a set where π∗\pi^*π∗ vanishes. Finally (3.1) concerns a smooth version of the density, which has to be produced from an almost-everywhere identity. The obvious idea of differentiating VVV along πˉ∗+εφ\bar\pi^*+\varepsilon\varphiπˉ∗+εφ for a signed perturbation φ\varphiφ fails: such perturbations leave Π\PiΠ unless they preserve positivity and the Y\mathbb YY-marginal.

Formalization scope

Rd\mathbb R^dRd is EuclideanSpace ℝ (Fin d) with Lebesgue measure; Y\mathbb YY is a complete separable metric space with its Borel σ\sigmaσ-algebra (a Polish space with a fixed compatible metric, needed to state moments and Wp\mathcal W_pWp​); Rˉd\bar{\mathbb R}^dRˉd carries the max product metric, and ∣xˉ∣|\bar x|∣xˉ∣ in the growth bound is the distance to a base point (0,y0)(0,y_0)(0,y0​), with CCC and y0y_0y0​ fixed once for all πˉ∈Π\bar\pi\in\Piπˉ∈Π. Wp\mathcal W_pWp​ is the coupling infimum over this metric, valued in [0,∞][0,\infty][0,∞], and continuity is the ε\varepsilonε–δ\deltaδ notion on Π\PiΠ. FFF and δFδπˉ\frac{\delta F}{\delta\bar\pi}δπˉδF​ are functions on all measures of which only the values on Π\PiΠ matter; δFδπˉ\frac{\delta F}{\delta\bar\pi}δπˉδF​ is part of the data and the theorem holds for every derivative satisfying (2.1). The definition of the derivative makes explicit what (2.1) presupposes: joint measurability in xˉ\bar xxˉ and integrability in λ\lambdaλ. Mixtures are (1−t)ν+tν′(1-t)\nu+t\nu'(1−t)ν+tν′ for t∈[0,1]t\in[0,1]t∈[0,1], and convexity of FFF is along these mixtures. HHH and VVV take values in (−∞,+∞](-\infty,+\infty](−∞,+∞], with H=+∞H=+\inftyH=+∞ off absolute continuity. (3.1) is required of some measurable version of the density, for m\mathsf mm-a.e. yyy and every xxx, together with positivity and differentiability of ln⁡π∗(⋅∣y)\ln\pi^*(\cdot|y)lnπ∗(⋅∣y).

The Lean logarithm satisfies ln⁡0=0\ln 0=0ln0=0, a non-integrable Bochner integral is 000, and the gradient of a non-differentiable function is 000. These would trivialize the statements, so (3.1) demands differentiability, and the milestones that integrate ln⁡π∗\ln\pi^*lnπ∗ assert integrability and that πˉ\bar\piπˉ does not charge {π∗=0}\{\pi^*=0\}{π∗=0}, which is what the paper's convention ln⁡0=−∞\ln0=-\inftyln0=−∞ encodes.

A complete development needs: mixtures and moments of measures in Π\PiΠ; Wp\mathcal W_pWp​-convergence of mixtures; dominated convergence along mixtures; the entropy of a mixture and its one-sided derivative; disintegration with respect to the Y\mathbb YY-marginal; and the passage from an a.e. identity to a smooth version of the density. The mixture, moment and entropy lemmas are reusable for any mean-field optimization problem. Contributions of any of these intermediate results, and of proofs of the milestones in any order, are welcome.

Selected references

  • G. Conforti, A. Kazeykina, Z. Ren, Game on random environment, mean-field Langevin system and neural networks, arXiv:2004.02457v2, 2020; Mathematics of Operations Research, 2023. https://arxiv.org/abs/2004.02457v2
  • K. Hu, Z. Ren, D. Šiška, L. Szpruch, Mean-field Langevin dynamics and energy landscape of neural networks, arXiv:1905.07769, 2019. https://arxiv.org/abs/1905.07769
  • S. Mei, A. Montanari, P.-M. Nguyen, A mean field view of the landscape of two-layer neural networks, PNAS 115 (2018), E7665–E7671. https://doi.org/10.1073/pnas.1806579115
  • P. Cardaliaguet, F. Delarue, J.-M. Lasry, P.-L. Lions, The master equation and the convergence problem in mean field games, arXiv:1509.02505, 2015. https://arxiv.org/abs/1509.02505
  • R. Jordan, D. Kinderlehrer, F. Otto, The variational formulation of the Fokker–Planck equation, SIAM J. Math. Anal. 29 (1998), 1–17. https://doi.org/10.1137/S0036141096303359
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Machine LearningOptimizationReinforcement Learning·Captain: mikedeng1

Neural Temporal-Difference and Q-Learning Provably Converge to Global Optima: Neural TD with Stochastic Semigradients Converges to the Global Optimum of the MSPBE at Rate 1/√TResearch Paper

Why neural temporal-difference learning needs a convergence theory

Temporal-difference (TD) learning estimates the value of a policy in a Markov decision process from sampled transitions, by repeatedly moving a parametrized value function towards a one-step bootstrapped target (Sutton, 1988). With a linear parametrization its behaviour is well understood: TD converges to the fixed point of the projected Bellman equation (Tsitsiklis and Van Roy, 1997), with finite-sample rates for projected and stochastic variants (Bhandari, Russo and Singal, 2018). With a nonlinear parametrization the same update can diverge: Tsitsiklis and Van Roy (1997) give an example, and the TD direction is not the gradient of any objective. Deep reinforcement learning nonetheless runs TD with neural networks as a matter of course.

Cai, Yang, Lee and Wang (arXiv:1905.10027v2, Mathematics of Operations Research, 2024) prove that TD with an overparametrized two-layer ReLU network, projected onto a ball around its random initialization, converges at rate T−1/2T^{-1/2}T−1/2 to the global optimum of the mean-squared projected Bellman error (MSPBE) over a function class that becomes richer as the width grows. This mission formalizes that theorem for the stochastic-semigradient algorithm (Theorem 4.6 of the paper).

Setting

Transitions are tuples (x,r,x′)(x, r, x')(x,r,x′) drawn i.i.d. from a sampling law μ\muμ: x,x′∈Rdx, x' \in \mathbb R^dx,x′∈Rd are feature vectors of the current and next state–action pair, with ∥x∥2=∥x′∥2=1\|x\|_2 = \|x'\|_2 = 1∥x∥2​=∥x′∥2​=1, the reward satisfies ∣r∣≤rˉ|r| \le \bar r∣r∣≤rˉ, and xxx and x′x'x′ have the same distribution (they are drawn from the stationary distribution of the policy). The discount factor is 0≤γ<10 \le \gamma < 10≤γ<1 and d≥3d \ge 3d≥3.

The value function is the two-layer network

Q^(x;W)=1m∑r=1mbr σ(Wr⊤x),σ(y)=max⁡{0,y},\widehat Q(x; W) = \frac{1}{\sqrt m}\sum_{r=1}^m b_r\,\sigma(W_r^\top x), \qquad \sigma(y) = \max\{0, y\},Q​(x;W)=m​1​r=1∑m​br​σ(Wr⊤​x),σ(y)=max{0,y},

of width mmm, with hidden weights W=(W1,…,Wm)∈RmdW = (W_1, \dots, W_m) \in \mathbb R^{md}W=(W1​,…,Wm​)∈Rmd and output weights b∈Rmb \in \mathbb R^mb∈Rm. At initialization br∼Unif{−1,1}b_r \sim \mathrm{Unif}\{-1, 1\}br​∼Unif{−1,1} and Wr(0)∼N(0,Id/d)W_r(0) \sim N(0, I_d/d)Wr​(0)∼N(0,Id​/d), all independent; only WWW is trained. The training set is the ball SB={W:∥W−W(0)∥2≤B}S_B = \{W : \|W - W(0)\|_2 \le B\}SB​={W:∥W−W(0)∥2​≤B}.

Algorithm 1 (neural TD) samples a tuple at each step t=0,…,T−2t = 0, \dots, T-2t=0,…,T−2, forms the Bellman residual δ=Q^(x;W(t))−r−γQ^(x′;W(t))\delta = \widehat Q(x; W(t)) - r - \gamma \widehat Q(x'; W(t))δ=Q​(x;W(t))−r−γQ​(x′;W(t)), takes the semigradient step W(t)−η δ ∇WQ^(x;W(t))W(t) - \eta\,\delta\,\nabla_W \widehat Q(x; W(t))W(t)−ηδ∇W​Q​(x;W(t)), projects it onto SBS_BSB​, and outputs Q^out=Q^(⋅ ;W‾)\widehat Q_{\mathrm{out}} = \widehat Q(\cdot\,; \overline W)Q​out​=Q​(⋅;W) with W‾=1T∑t=0T−1W(t)\overline W = \frac1T \sum_{t=0}^{T-1} W(t)W=T1​∑t=0T−1​W(t).

The linearization of the network at initialization is

Q^0(x;W)=1m∑r=1mbr 1{Wr(0)⊤x>0} Wr⊤x,\widehat Q_0(x; W) = \frac{1}{\sqrt m}\sum_{r=1}^m b_r\,\mathbb 1\{W_r(0)^\top x > 0\}\, W_r^\top x,Q​0​(x;W)=m​1​r=1∑m​br​1{Wr​(0)⊤x>0}Wr⊤​x,

a linear function of WWW with random features. Writing δ0\delta_0δ0​ for the Bellman residual of Q^0\widehat Q_0Q​0​, an approximate stationary point is a W∗∈SBW^* \in S_BW∗∈SB​ with

Eμ[δ0(x,r,x′;W∗) ∇WQ^0(x;W∗)]⊤(W−W∗)≥0for all W∈SB.\mathbb E_\mu\big[\delta_0(x, r, x'; W^*)\,\nabla_W \widehat Q_0(x; W^*)\big]^\top (W - W^*) \ge 0 \quad \text{for all } W \in S_B .Eμ​[δ0​(x,r,x′;W∗)∇W​Q​0​(x;W∗)]⊤(W−W∗)≥0for all W∈SB​.

The function Q^0(⋅ ;W∗)\widehat Q_0(\cdot\,; W^*)Q​0​(⋅;W∗) solves the projected Bellman equation over the class FB,m={Q^0(⋅ ;W):W∈SB}\mathcal F_{B,m} = \{\widehat Q_0(\cdot\,; W) : W \in S_B\}FB,m​={Q​0​(⋅;W):W∈SB​}. The regularity condition (Assumption 4.3) asks for c0>0c_0 > 0c0​>0 with μ(∣w⊤x∣≤τ)≤c0τ\mu(|w^\top x| \le \tau) \le c_0 \tauμ(∣w⊤x∣≤τ)≤c0​τ for every unit vector www and every τ≥0\tau \ge 0τ≥0.

Formalization targets

Goal: Theorem 4.6

With η=min⁡{(1−γ)/8, 1/T}\eta = \min\{(1-\gamma)/8,\ 1/\sqrt T\}η=min{(1−γ)/8, 1/T​} and under Assumption 4.3, there is a constant C=C(c0,d,rˉ,γ)C = C(c_0, d, \bar r, \gamma)C=C(c0​,d,rˉ,γ) such that for all m≥1m \ge 1m≥1, B≥1B \ge 1B≥1, T≥1T \ge 1T≥1 and every approximate stationary point W∗W^*W∗,

Einit,μ[(Q^out(x)−Q^0(x;W∗))2]≤16 (B2+σg2)(1−γ)2T+C(B3m−1/2+B5/2m−1/4),\mathbb E_{\mathrm{init},\mu}\Big[\big(\widehat Q_{\mathrm{out}}(x) - \widehat Q_0(x; W^*)\big)^2\Big] \le \frac{16\,(B^2 + \sigma_g^2)}{(1-\gamma)^2\sqrt T} + C\big(B^3 m^{-1/2} + B^{5/2} m^{-1/4}\big),Einit,μ​[(Q​out​(x)−Q​0​(x;W∗))2]≤(1−γ)2T​16(B2+σg2​)​+C(B3m−1/2+B5/2m−1/4),

where σg2=12+12B2+3rˉ2\sigma_g^2 = 12 + 12B^2 + 3\bar r^2σg2​=12+12B2+3rˉ2 and the expectation is over the initialization, the samples of the run and a fresh x∼μx \sim \mux∼μ.

Milestones

  1. Lemma 4.2: approximate stationary points exist for every initialization; Q^0(⋅ ;W∗)\widehat Q_0(\cdot\,; W^*)Q​0​(⋅;W∗) is unique μ\muμ-a.e. and is the MSPBE optimum over FB,m\mathcal F_{B,m}FB,m​.
  2. Lemmas H.1, H.2: the expected fraction of hidden units whose activation can flip inside SBS_BSB​ is O(Bm−1/2)O(B m^{-1/2})O(Bm−1/2), alone and weighted by Eμ[Q^(x;W(0))2]\mathbb E_\mu[\widehat Q(x; W(0))^2]Eμ​[Q​(x;W(0))2].
  3. Lemmas 5.1, 5.2: the network and its population semigradient stay within O(B3m−1/2)O(B^3 m^{-1/2})O(B3m−1/2) (in mean square) of their linearizations, for every random parameter in SBS_BSB​.
  4. Lemma 4.5: the stochastic semigradient has variance at most σg2\sigma_g^2σg2​.
  5. (C.16): the linearized population semigradient is monotone with modulus 1−γ1-\gamma1−γ in the μ\muμ-norm.
  6. Lemma 5.4: the stochastic descent inequality for E∥W(t)−W∗∥22\mathbb E\|W(t) - W^*\|_2^2E∥W(t)−W∗∥22​.

Significance

The theorem gives a non-asymptotic guarantee for TD with a nonlinear function class, a setting in which the algorithm can diverge without further structure. The limit object Q^0(⋅ ;W∗)\widehat Q_0(\cdot\,; W^*)Q​0​(⋅;W∗) is a projected Bellman fixed point over a class that, as m→∞m \to \inftym→∞, approaches a ball in the reproducing kernel Hilbert space of the neural tangent kernel; the paper uses this to bound the distance to the true value function QπQ^\piQπ (Proposition 4.7) and to analyze neural Q-learning and policy gradient methods (Section 6). The argument is an instance of the "lazy training" or neural-tangent-kernel regime, in which an overparametrized network trained from a random initialization stays close to its linearization.

The result is proved in the paper and, to our knowledge, has no machine-checked proof. A formalization would also produce reusable components: Gaussian anti-concentration of random ReLU activation patterns (Lemmas H.1–H.2), the linearization error of wide two-layer networks (Lemma 5.1), and a projected stochastic-approximation template with averaged iterates. The appendix proofs are short and pass over several measure-theoretic steps (conditioning on the current iterate, independence of the samples from the initialization, Jensen for the averaged iterate), which a formal proof has to supply.

Difficulty

The TD update is not a gradient, so the convergence proof cannot be a descent argument on an objective. The paper's route is to compare the update with that of the linear TD problem defined by Q^0\widehat Q_0Q​0​, whose population semigradient is monotone, and to control the difference by overparametrization. The obvious first approach, linearizing the network in a deterministic neighbourhood of W(0)W(0)W(0), fails: the ReLU activation pattern 1{Wr⊤x>0}\mathbb 1\{W_r^\top x > 0\}1{Wr⊤​x>0} can change for some units whatever mmm is. The comparison holds only in expectation over the random initialization and a fresh input, through Assumption 4.3 and the finiteness of E ∥w∥2−2\mathbb E\,\|w\|_2^{-2}E∥w∥2−2​ for w∼N(0,Id/d)w \sim N(0, I_d/d)w∼N(0,Id​/d), which is where d≥3d \ge 3d≥3 enters. The iterates and W∗W^*W∗ depend on the initialization, so these bounds are needed for random parameters that are correlated with W(0)W(0)W(0) but independent of the evaluation point.

Formalization scope

Lean represents points as EuclideanSpace ℝ (Fin d) and parameters as PiLp 2 over Fin m, so all norms on Rmd\mathbb R^{md}Rmd are ℓ2\ell_2ℓ2​. The MDP, the policy and the feature map are not modelled; the statements see only the sampling law μ\muμ on tuples (x,r,x′)(x, r, x')(x,r,x′) with the properties listed above. The run's samples form an N\mathbb NN-indexed i.i.d. sequence (product measure) independent of the initialization, and the evaluation tuple is a fresh draw. Expectations of nonnegative quantities are lower Lebesgue integrals, so non-integrability cannot make a bound hold vacuously. The ReLU semigradient uses the strict convention 1{Wr⊤x>0}\mathbb 1\{W_r^\top x > 0\}1{Wr⊤​x>0} and keeps the factor m−1/2m^{-1/2}m−1/2 of (3.2).

Conventions and readings fixed by the formalization, all disclosed in the item statements:

  • the paper's "σg2=O(B2)\sigma_g^2 = O(B^2)σg2​=O(B2)" is pinned to the value 12+12B2+3rˉ212 + 12B^2 + 3\bar r^212+12B2+3rˉ2 produced by its proof;
  • the paper's O(B3m−1/2+B5/2m−1/4)O(B^3 m^{-1/2} + B^{5/2} m^{-1/4})O(B3m−1/2+B5/2m−1/4) is a constant CCC depending only on (c0,d,rˉ,γ)(c_0, d, \bar r, \gamma)(c0​,d,rˉ,γ) and chosen before mmm, BBB, TTT, μ\muμ and W∗W^*W∗, with B≥1B \ge 1B≥1 so that lower powers of BBB are absorbed;
  • approximate stationary points are required to lie in SBS_BSB​, as the proof uses;
  • Lemmas 5.1 and 5.2 are posed for every random parameter in SBS_BSB​ (the paper's proofs need nothing else and apply them to W‾\overline WW);
  • Lemma 5.4 carries the coefficient 4ηB4\eta B4ηB, which is what its proof establishes (∥W(t)−W∗∥2≤2B\|W(t) - W^*\|_2 \le 2B∥W(t)−W∗∥2​≤2B), in place of the printed 2ηB2\eta B2ηB.

A formalization in which the comparison point W∗W^*W∗ may lie outside SBS_BSB​, the expectation is a Bochner integral of a possibly non-integrable function, or the constant CCC may depend on mmm, TTT or μ\muμ, would not express the theorem and is excluded. Approximate stationary points are compared through Q^0(⋅ ;W∗)\widehat Q_0(\cdot\,; W^*)Q​0​(⋅;W∗), never through Q^(⋅ ;W∗)\widehat Q(\cdot\,; W^*)Q​(⋅;W∗).

A complete development needs Gaussian measures on Rd\mathbb R^dRd with the integrability of ∥w∥2−2\|w\|_2^{-2}∥w∥2−2​ for d≥3d \ge 3d≥3, product and infinite-product probability measures with conditioning on the past of a sequence, existence of solutions to variational inequalities on compact convex sets, and nonexpansiveness of Euclidean projection onto a ball. Proofs of individual milestones are welcome independently; Lemmas H.1, 5.1 and (C.16) are self-contained.

Selected references

  • Q. Cai, Z. Yang, J. D. Lee, Z. Wang, Neural temporal-difference and Q-learning provably converge to global optima, Mathematics of Operations Research, 2024; arXiv:1905.10027v2. https://arxiv.org/abs/1905.10027
  • R. S. Sutton, Learning to predict by the methods of temporal differences, Machine Learning 3, 1988. https://doi.org/10.1007/BF00115009
  • J. N. Tsitsiklis, B. Van Roy, An analysis of temporal-difference learning with function approximation, IEEE Transactions on Automatic Control 42(5), 1997. https://doi.org/10.1109/9.580874
  • J. Bhandari, D. Russo, R. Singal, A finite time analysis of temporal difference learning with linear function approximation, COLT 2018. https://arxiv.org/abs/1806.02450
  • A. Jacot, F. Gabriel, C. Hongler, Neural tangent kernel: convergence and generalization in neural networks, NeurIPS 2018. https://arxiv.org/abs/1806.07572
10 thms1 active userReviewed
Quantum Information·Captain: Goku

Bounding the energy-constrained quantum and private capacities of phase-insensitive bosonic Gaussian channelsResearch Paper

Motivation

We establish several upper bounds on the energy-constrained quantum and private capacities of all single-mode phase-insensitive bosonic Gaussian channels. The first upper bound, which we call the "data-processing bound," is the simplest and is obtained by decomposing a phase-insensitive channel as a pure-loss channel followed by a quantum-limited amplifier channel. We prove that the data-processing bound can be at most 1.45 bits larger than a known lower bound on these capacities of the phase-insensitive Gaussian channel. We discuss another data-processing upper bound as well. Two other upper bounds, which we call the "ε\varepsilonε-degradable bound" and the "ε\varepsilonε-close-degradable bound," are established using the notion of approximate degradability along with energy constraints. We find a strong limitation on any potential superadditivity of the coherent information of any phase-insensitive Gaussian channel in the low-noise regime, as the data-processing bound is very near to a known lower bound in such cases. We also find improved achievable rates of private communication through bosonic thermal channels, by employing coding schemes that make use of displaced thermal states. We end by proving that an optimal Gaussian input state for the energy-constrained, generalized channel divergence of two particular Gaussian channels is the two-mode squeezed vacuum state that saturates the energy constraint. What remains open for several interesting channel divergences, such as the diamond norm or the Renyi channel divergence, is to determine whether, among all input states, a Gaussian state is optimal.

This mission is the statement-level formalization of Bounding the energy-constrained quantum and private capacities of phase-insensitive bosonic Gaussian channels (arXiv:1708.07257v3). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

5 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Theorem 26: thermal gap bound (Theorem 26, PDF p. 34). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

51 results of the paper are not stated yet, because the library lacks an interface they need:

  • Remark 3: Approximate-degradability implication for state-supremum half-diamond errors on arbitrary separable channel systems, with a certified conversion of the cited full-diamond constants. (hard)
  • Lemma 1: Bit-valued conditional entropy for finite first-system entropy, spectral Gibbs entropy envelope, and the cited energy-constrained half-trace-distance continuity result on separable systems. (hard)
  • Theorem 8: As printed the reference R has no entropy restriction. A product of an infinite-entropy state on R and a vacuum input makes BOTH joint entropies infinite, so their displayed difference is undefined. The proof suggests a telescoping conditional-entropy extension, but the source never defines that extension; adding finite H(R) or changing the conclusion silently would change the theorem. (source-ambiguity)
  • Lemma 2: Common admissible parameter sets, finite real optimization suprema and existing regularized limits for both channels, with the uniform all-positive-n absolute difference bound. (hard)
  • Remark 9: Independently defined constrained and unconstrained operational quantum/private capacities with all-large-positive-blocklength achievability. (hard)
  • Theorem 11: Uniform-energy quantum codes and their capacity, state-supremum half-diamond distance, fixed complement, and output Gibbs entropy envelope. (hard)
  • Theorem 12: Uniform-energy operational Q and optimized coherent information for the actually degradable comparison channel, with all-blocklength receiver-energy bounds. (hard)
  • Theorem 13: Finite-dimensional operational private capacity from normalized POVM private codes and a common environment state, plus an attained entropy maximum and fixed complement. (hard)
  • Theorem 14: Operational private capacity with messagewise energy/security and Gibbs entropy envelope on the identified complementary output. (hard)
  • Theorem 15: Operational private capacity and optimized coherent information for the comparison channel, retaining average ensemble energy. (hard)
  • Remark 17: Unconstrained thermal Q and the supremum/limit of the clipped finite-energy expression, with infinity at eta=1. (hard)
  • Theorem 16: Full Fock thermal CPTP receiver and uniform-energy operational quantum capacity. (hard)
  • Remark 18: Operational thermal quantum capacity positivity and its necessary parameter restriction, including zero energy. (hard)
  • Theorem 19: Actual two-mode purified thermal complement and opposite-phase splitter degrading map (5.20), with arbitrary-reference diamond distance. (hard)
  • Theorem 20: The derivation applies Theorem 11 to TWO environment output modes with total photon budget Wprime=(1-eta)NS+(1+eta)NB, but substitutes the ONE-mode entropy g(Wprime/delta). For the natural sum-number Gibbs observable the maximum entropy is 2g(Wprime/(2delta)), generally larger. The source supplies no alternative Gibbs observable justifying (5.42). Neither silently increasing the correction nor assuming a missing entropy bound states the printed result faithfully. (source-ambiguity)
  • Proposition 21: Actual thermal receiver/degrader, saturating thermal state, and attained optimization over every normalized finite-energy input. (hard)
  • Remark 22: The stated conditions omit Gaussian extremality. Phase-averaging need not preserve Gaussianity. Concavity and local-unitary invariance alone do not single out a thermal maximizer among all states, so no faithful general optimizer theorem follows from the supplied bullet list. (source-ambiguity)
  • Remark 24: High-energy TMS output-fidelity limit for full Fock thermal channels at common 0<=eta<1, and its derived half-diamond lower bound. (hard)
  • Theorem 23: Thermal/pure-loss full Fock CPTP receivers at both transmissivity endpoints and arbitrary-reference normalized-state diamond supremum. (hard)
  • Theorem 25: Operational thermal Q with uniform encoder energy and source close-degradable entropy correction. (hard)
  • Unnumbered asserted gap limit: The fixed-channel equality is false: at NB=0 the thermal channel is pure loss and the two scalar expressions agree for every NS, so Delta is identically zero. The source applies a large-argument entropy expansion to a symplectic occupation that stays bounded. The valid inequality of Theorem 26 is kept at the seed; no false saturation limit is assumed. (source-ambiguity)
  • Remark 28: Unconstrained thermal P and the clipped finite-energy supremum/limit, including the infinite eta=1 endpoint. (hard)
  • Theorem 27: Full Fock thermal receiver and messagewise-energy operational private capacity. (hard)
  • Theorem 29: Theorem 29 inherits the unresolved two-environment-mode Gibbs entropy substitution of Theorem 20: it uses g(Wprime/delta) where the cited general theorem with the sum-number observable gives 2g(Wprime/(2delta)). The intended smaller correction is not justified or specified by the source; retain this theorem as deferred rather than quietly enlarging its bound. (source-ambiguity)
  • Unnumbered displaced-thermal private rate: Displaced-thermal Borel ensemble, trace-norm barycenter, private information with average ensemble energy, and achievable private rates; Dirac displacement at s=NS. (hard)
  • Theorem 30: Operational thermal P with messagewise energy/security and source close-degradable entropy correction. (hard)
  • Theorem 31: Full Weyl-action adapter identifying a centered phase-insensitive CPTP channel and constructed amplifier-then-loss maps, including G=1. (hard)
  • Theorem 32: Noisy-amplifier Fock CPTP receiver and both operational energy-constrained capacities. (hard)
  • Remark 33: Both unconstrained amplifier capacities, scalar high-energy supremum/limit, and complete PLOB-bound comparison. (hard)
  • Remark 34: Operational amplifier Q positivity implication using (G-1)NB<1, without division by NB. (hard)
  • Theorem 36: Fixed purified amplifier complement and environment-port degrading squeezer (9.24), with arbitrary-reference half-diamond distance. (hard)
  • Theorem 37: Printed expression is false at the allowed edge NB=NS=0 and G>1: epsilon=0, zeta occupations are G-1 and 0, so as epsilonPrime decreases to zero its RHS tends to -g(G-1)<0 although capacity is zero. The first output entropy omits spontaneous photons G-1; the complementary photon budget also omits them. In addition the two-mode continuity correction has the unresolved issue of Theorem 20. No single silent transcription fix recovers the claimed formula. (source-ambiguity)
  • Theorem 38: Printed expression is false at the allowed edge NB=NS=0 and G>1: epsilon=0, zeta occupations are G-1 and 0, so as epsilonPrime decreases to zero its RHS tends to -g(G-1)<0 although capacity is zero. The first output entropy omits spontaneous photons G-1; the complementary photon budget also omits them. In addition the two-mode continuity correction has the unresolved issue of Theorem 20. No single silent transcription fix recovers the claimed formula. (source-ambiguity)
  • Theorem 39: Noisy/quantum-limited Fock amplifier CPTP receivers and arbitrary-reference normalized-state diamond distance. (hard)
  • Theorem 40: Operational amplifier Q and corrected common receiver photon budget G NS+(G-1)(NB+1); delta denominator 1+epsilonPrime. (hard)
  • Theorem 41: Operational amplifier P and corrected common receiver photon budget G NS+(G-1)(NB+1); delta denominator 1+epsilonPrime. (hard)
  • Remark 43: Additive-noise CPTP channel, both unconstrained operational capacities, and high-energy supremum/limit. (hard)
  • Remark 45: Operational additive-noise quantum/private capacities and the cited converse (nbar-1)/ln2+log2(1/nbar), including its strict comparison on 0<nbar<1. (hard)
  • Theorem 42: Additive-noise CPTP channel and both energy-constrained capacities, with the finite-energy bound. (hard)
  • Theorem 46: Thermal operational Q/P and physical amplifier-then-loss bottleneck with increased encoder energy G NS+G-1 and clipping. (hard)
  • Remark 47: Thermal operational Q/P positivity implication, including zero capacities in entanglement-breaking cases. (hard)
  • Remark 49: The statement uses unquantified low-noise/low-energy regimes and supplies no analytic boundary. Plots and qualitative comparisons cannot be registered as a universal parameter inequality without inventing a threshold. (source-ambiguity)
  • Remark 50: Additive-noise unconstrained Q/P and the clipped high-energy supremum of Theorem 48 for all 0<nbar<1. (hard)
  • Remark 51: The high-noise regime is not quantified and the printed U4 expression is unclipped, whereas an operational bound must be clipped at zero. Choosing an exact threshold or either version without qualification would assert more than the source specifies. (source-ambiguity)
  • Theorem 48: Additive-noise CPTP channel and both operational energy-constrained capacities with max(0,U4). (hard)
  • Lemma 4: Dimension-compatible generalized divergence on actual trace-class systems with data processing and cq direct sums, and the finite/discrete ensemble group-averaging inequality. (hard)
  • Lemma 5: The text extends the finite-group result “by approximation” while requiring only that D is Borel. Borel measurability permits integration but does not give the semicontinuity/continuous-ensemble direct-sum law needed to pass this inequality to a continuous barycenter. The source neither supplies that law nor specifies a divergence class for which the limiting argument is valid; do not silently replace Borel by lower semicontinuous or assume the desired inequality. (source-ambiguity)
  • Proposition 54: The full statement uses the unresolved continuous-ensemble step of Lemma 5 with only Borel regularity. Additionally the Gaussian-attainment argument on p.56 invokes that only thermal Gaussian states are number-diagonal, but phase averaging a Gaussian state need not stay Gaussian (e.g. coherent-state dephasing is Poisson). No general Gaussian-extremality property of an arbitrary D is supplied. Retain BOTH conclusions as the deferred target; do not replace it by only the diagonal-state reduction or assert an unproved Gaussian optimizer. (source-ambiguity)
  • Unnumbered Gaussian diamond and C-distance optimizers: Explicit main corollaries of the deferred Gaussian-attainment clause of Proposition 54; the source has not supplied the missing Gaussian-extremality/continuous-ensemble argument. Keep both target equalities and do not promote them to unrestricted diamond or C-distance optimizer statements. (source-ambiguity)
  • Unnumbered joint displacement-covariance reduction: Same unresolved Borel-versus-continuous-ensemble issue as Lemma 5. The displaced input is purified afresh, and exact energy is a consequence; it cannot be assumed on the original <=NS optimization domain. (source-ambiguity)
  • Unnumbered joint phase-covariance reduction: This explicitly claimed generalization uses the unresolved continuous-group approximation of Lemma 5. Record the <=NS constraint accurately; without a specified divergence regularity/continuous-ensemble law, the stated generality is not pinned down. (source-ambiguity)

Selected references

  • Bounding the energy-constrained quantum and private capacities of phase-insensitive bosonic Gaussian channels, arXiv:1708.07257v3, https://arxiv.org/abs/1708.07257v3
10 thms1 active userReviewed
Quantum Information·Captain: Goku

Quantum privacy and quantum coherenceResearch Paper

Motivation

We derive a simple relation between a quantum channel's capacity to convey coherent (quantum) information and its usefulness for quantum cryptography.

This mission is the statement-level formalization of Quantum privacy and quantum coherence (arXiv:quant-ph/9709058v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

3 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Fixed-strategy guaranteed privacy is bounded below by Bob information minus environment Holevo information (Equation (8): fixed-strategy guaranteed privacy lower bound, PDF p. 4). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

3 results of the paper are not stated yet, because the library lacks an interface they need:

  • Main result, equation (12): optimal guaranteed privacy bounds coherent information: An independently specified operational per-use optimal guaranteed privacy over block strategies (source-ambiguity)
  • Equation (9): optimized privacy lower bound by the Holevo difference: An independently specified operational per-use optimal guaranteed privacy over block strategies (source-ambiguity)
  • Unnumbered consequence: positive coherent information permits secure private transmission: An independently specified operational per-use optimal guaranteed privacy over block strategies; also a quantitative meaning of securely (source-ambiguity)

Selected references

  • Quantum privacy and quantum coherence, arXiv:quant-ph/9709058v2, https://arxiv.org/abs/quant-ph/9709058v2
6 thms1 active userReviewed
Quantum Information·Captain: Goku

Strong converse for the classical capacity of optical quantum communication channelsResearch Paper

Motivation

We establish the classical capacity of optical quantum channels as a sharp transition between two regimes---one which is an error-free regime for communication rates below the capacity, and the other in which the probability of correctly decoding a classical message converges exponentially fast to zero if the communication rate exceeds the classical capacity. This result is obtained by proving a strong converse theorem for the classical capacity of all phase-insensitive bosonic Gaussian channels, a well-established model of optical quantum communication channels, such as lossy optical fibers, amplifier and free-space communication. The theorem holds under a particular photon-number occupation constraint, which we describe in detail in the paper. Our result bolsters the understanding of the classical capacity of these channels and opens the path to applications, such as proving the security of noisy quantum storage models of cryptography with optical links.

This mission is the statement-level formalization of Strong converse for the classical capacity of optical quantum communication channels (arXiv:1401.4161v3). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

5 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Operational strong converse above the optical classical-capacity threshold (Introduction and Corollary 1, PDF p. 2). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

1 results of the paper are not stated yet, because the library lacks an interface they need:

  • Abstract: exponential decay: A valid unconditional exponential success-decay conclusion under only a vanishing occupation tail (source-ambiguity)

Selected references

  • Strong converse for the classical capacity of optical quantum communication channels, arXiv:1401.4161v3, https://arxiv.org/abs/1401.4161v3
11 thms1 active userReviewed
Quantum Information·Captain: Goku

A solution of the Gaussian optimizer conjectureResearch Paper

Motivation

The long-standing conjectures of the optimality of Gaussian inputs for Gaussian channel and Gaussian additivity are solved for a broad class of covariant or contravariant Bosonic Gaussian channels (which includes in particular thermal, additive classical noise, and amplifier channels) restricting to the class of states with finite second moments. We show that the vacuum is the input state which minimizes the entropy at the output of such channels. This allows us to show also that the classical capacity of these channels (under the input energy constraint) is additive and is achieved by Gaussian encodings.

This mission is the statement-level formalization of A solution of the Gaussian optimizer conjecture (arXiv:1312.2251v2). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

16 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Main result: vacuum optimizer and unconditional Gaussian minimum-output additivity (Main result: vacuum optimizer and unconditional Gaussian minimum-output additivity, PDF p. 1). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

6 results of the paper are not stated yet, because the library lacks an interface they need:

  • §3: additivity consequences for contravariant channels: General positive quadratic bosonic Hamiltonian and S2-restricted constrained chi capacity with additive block energy, retaining (23) as well as (20)-(21) (hard)
  • §4: additive energy-constrained capacity, Gaussian encoding and finite-dimensional formula: Independent energy-constrained classical block-code capacity on the common coefficient State model, its regularized-chi bridge, and actual Gaussian coherent encoding attainment (hard)
  • §7: thermal-noise entropy minimum and capacity: Independent energy-constrained classical block-code capacity on the common coefficient State model, its regularized-chi bridge, and actual Gaussian coherent encoding attainment (hard)
  • §7: additive classical-noise entropy minimum and capacity: Independent energy-constrained classical block-code capacity on the common coefficient State model, its regularized-chi bridge, and actual Gaussian coherent encoding attainment (hard)
  • §7: noisy-amplifier entropy minimum and capacity: Independent energy-constrained classical block-code capacity on the common coefficient State model, its regularized-chi bridge, and actual Gaussian coherent encoding attainment (hard)
  • §7: claimed extension to all one-mode BGCs via squeezing: Correct domain or infimum/attainment correction for the universal one-mode squeezed-vacuum optimizer claim, including B1 rank-one additive noise (source-ambiguity)

Selected references

  • A solution of the Gaussian optimizer conjecture, arXiv:1312.2251v2, https://arxiv.org/abs/1312.2251v2
21 thms1 active userReviewed
Quantum Information·Captain: Goku

Ultimate communication capacity of quantum optical channels by solving the Gaussian minimum-entropy conjectureResearch Paper

Motivation

Optical channels, such as fibers or free-space links, are ubiquitous in today's telecommunication networks. They rely on the electromagnetic field associated with photons to carry information from one point to another in space. As a result, a complete physical model of these channels must necessarily take quantum effects into account in order to determine their ultimate performances. Specifically, Gaussian photonic (or bosonic) quantum channels have been extensively studied over the past decades given their importance for practical purposes. In spite of this, a longstanding conjecture on the optimality of Gaussian encodings has yet prevented finding their communication capacity. Here, this conjecture is solved by proving that the vacuum state achieves the minimum output entropy of a generic Gaussian bosonic channel. This establishes the ultimate achievable bit rate under an energy constraint, as well as the long awaited proof that the single-letter classical capacity of these channels is additive. Beyond capacities, it also has broad consequences in quantum information sciences.

This mission is the statement-level formalization of Ultimate communication capacity of quantum optical channels by solving the Gaussian minimum-entropy conjecture (arXiv:1312.6225v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

15 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Finite-energy Gaussian minimum output entropy (Eq. (2), PDF p. 2). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Selected references

  • Ultimate communication capacity of quantum optical channels by solving the Gaussian minimum-entropy conjecture, arXiv:1312.6225v1, https://arxiv.org/abs/1312.6225v1
25 thms1 active userReviewed
Differential GeometryLinear algebraOptimization·Captain: mikedeng1

On Geometric Connections of Embedded and Quotient Geometries in Riemannian Fixed-rank Matrix Optimization: Gradient and Hessian Connections for Fixed-rank PSD Matrices via YYᵀResearch Paper

Motivation

Many estimation problems in statistics, signal processing and machine learning ask for a low-rank positive semidefinite matrix: phase retrieval, matrix sensing, PCA-type problems and the Burer–Monteiro approach to semidefinite programs. A standard formulation is

min⁡X∈Sp×p, X⪰0, rank⁡(X)=rf(X),0<r≤p,(1)\min_{X\in\mathbb S^{p\times p},\ X\succeq0,\ \operatorname{rank}(X)=r} f(X),\qquad 0<r\le p, \tag{1}X∈Sp×p, X⪰0, rank(X)=rmin​f(X),0<r≤p,(1)

and Riemannian optimization solves it by treating the feasible set as a smooth manifold. Two geometries are in common use. In the embedded geometry the set of rank-rrr PSD matrices is a submanifold of Rp×p\mathbb R^{p\times p}Rp×p with the Euclidean metric. In the quotient geometry one writes X=YY⊤X=YY^\topX=YY⊤ with a full-column-rank factor YYY and optimizes over equivalence classes [Y]={YO:O orthogonal}[Y]=\{YO:O\text{ orthogonal}\}[Y]={YO:O orthogonal}. Algorithms built on the two geometries behave similarly in experiments, and landscape results (absence of spurious local minima, strict saddles) have been proved separately for each. Luo, Li and Zhang (arXiv:2110.12121, Mathematics of Operations Research 2024) explain this by an explicit dictionary between the Riemannian gradients and Hessians of the two geometries. This mission formalizes their first main result, Theorem 3, for the full-rank factorization of PSD matrices.

Setting

Matrices carry the Frobenius inner product ⟨A,B⟩=tr⁡(A⊤B)\langle A,B\rangle=\operatorname{tr}(A^\top B)⟨A,B⟩=tr(A⊤B). The objective f:Rp×p→Rf:\mathbb R^{p\times p}\to\mathbb Rf:Rp×p→R is twice continuously differentiable and symmetric, f(X)=f(X⊤)f(X)=f(X^\top)f(X)=f(X⊤) (the paper's standing assumptions); ∇f\nabla f∇f and ∇2f\nabla^2f∇2f are its Euclidean gradient and Hessian.

Embedded geometry. Mr+={X∈Sp×p:X⪰0, rank⁡X=r}\mathcal M_{r+}=\{X\in\mathbb S^{p\times p}:X\succeq0,\ \operatorname{rank}X=r\}Mr+​={X∈Sp×p:X⪰0, rankX=r}, viewed as Mr+e⊂Rp×p\mathcal M^e_{r+}\subset\mathbb R^{p\times p}Mr+e​⊂Rp×p. Its tangent space TXMr+eT_X\mathcal M^e_{r+}TX​Mr+e​ is the span of the tangent cone. The Riemannian gradient grad⁡f(X)\operatorname{grad}f(X)gradf(X) is the orthogonal projection of ∇f(X)\nabla f(X)∇f(X) onto TXMr+eT_X\mathcal M^e_{r+}TX​Mr+e​, and the Riemannian Hessian quadratic form Hess⁡f(X)[ξ,ξ]\operatorname{Hess}f(X)[\xi,\xi]Hessf(X)[ξ,ξ] is the derivative ddt⟨grad⁡f(c(t)),ξ⟩\frac{d}{dt}\langle\operatorname{grad}f(c(t)),\xi\rangledtd​⟨gradf(c(t)),ξ⟩ at t=0t=0t=0 along any C1C^1C1 curve ccc in Mr+\mathcal M_{r+}Mr+​ with c(0)=Xc(0)=Xc(0)=X, c′(0)=ξc'(0)=\xic′(0)=ξ.

Quotient geometry. The total space is R∗p×r\mathbb R_*^{p\times r}R∗p×r​, the p×rp\times rp×r matrices of full column rank, with the objective hˉr+(Y)=f(YY⊤)\bar h_{r+}(Y)=f(YY^\top)hˉr+​(Y)=f(YY⊤) (18a). A weight Y↦WYY\mapsto W_YY↦WY​, smooth and symmetric positive definite, defines the metric gˉY(η,θ)=tr⁡(WYη⊤θ)\bar g_Y(\eta,\theta)=\operatorname{tr}(W_Y\eta^\top\theta)gˉ​Y​(η,θ)=tr(WY​η⊤θ). The vertical space VY={YΩ:Ω⊤=−Ω}\mathcal V_Y=\{Y\Omega:\Omega^\top=-\Omega\}VY​={YΩ:Ω⊤=−Ω} is tangent to the orbit [Y][Y][Y], and the horizontal space HY\mathcal H_YHY​ is its gˉY\bar g_Ygˉ​Y​-orthogonal complement. Tangent vectors of the quotient Mr+q1=R∗p×r/Or\mathcal M^{q_1}_{r+}=\mathbb R_*^{p\times r}/\mathbb O_rMr+q1​​=R∗p×r​/Or​ are represented by horizontal vectors: grad⁡hr+([Y])‾\overline{\operatorname{grad}h_{r+}([Y])}gradhr+​([Y])​ is the horizontal part of the total-space gradient ∇hˉr+(Y)WY−1\nabla\bar h_{r+}(Y)W_Y^{-1}∇hˉr+​(Y)WY−1​, and Hess⁡hr+([Y])‾[θ,θ]=gˉY(∇ˉθgrad⁡hˉ,θ)\overline{\operatorname{Hess}h_{r+}([Y])}[\theta,\theta]=\bar g_Y(\bar\nabla_\theta\operatorname{grad}\bar h,\theta)Hesshr+​([Y])​[θ,θ]=gˉ​Y​(∇ˉθ​gradhˉ,θ) for horizontal θ\thetaθ, where ∇ˉ\bar\nabla∇ˉ is the Levi-Civita connection of gˉ\bar ggˉ​ (Koszul formula).

Comparison data. LYr+(θ)=Yθ⊤+θY⊤\mathcal L^{r+}_Y(\theta)=Y\theta^\top+\theta Y^\topLYr+​(θ)=Yθ⊤+θY⊤; U∈St(r,p)U\in\mathrm{St}(r,p)U∈St(r,p) spans the top rrr eigenspace of X=YY⊤X=YY^\topX=YY⊤, P=U⊤YP=U^\top YP=U⊤Y, Y†=(Y⊤Y)−1Y⊤Y^\dagger=(Y^\top Y)^{-1}Y^\topY†=(Y⊤Y)−1Y⊤. For a quadratic form on a ddd-dimensional space with inner product ggg, λk\lambda_kλk​ is its kkk-th largest eigenvalue relative to ggg (1≤k≤d1\le k\le d1≤k≤d). σ1,σr\sigma_1,\sigma_rσ1​,σr​ are the extreme singular values of an r×rr\times rr×r matrix.

Formalization targets

Goal: Theorem 3 (p. 21)

If in addition WY=OWYOO⊤W_Y=OW_{YO}O^\topWY​=OWYO​O⊤ for all orthogonal OOO, then for every Y∈R∗p×rY\in\mathbb R_*^{p\times r}Y∈R∗p×r​ and X=YY⊤X=YY^\topX=YY⊤,

grad⁡f(X)=(grad⁡hr+([Y])‾WYY†+(grad⁡hr+([Y])‾WYY†)⊤(Ip−YY†))/2,grad⁡hr+([Y])‾=2grad⁡f(X)YWY−1,\operatorname{grad}f(X)=\Big(\overline{\operatorname{grad}h_{r+}([Y])}W_YY^\dagger+\big(\overline{\operatorname{grad}h_{r+}([Y])}W_YY^\dagger\big)^\top(I_p-YY^\dagger)\Big)/2,\qquad\overline{\operatorname{grad}h_{r+}([Y])}=2\operatorname{grad}f(X)YW_Y^{-1},gradf(X)=(gradhr+​([Y])​WY​Y†+(gradhr+​([Y])​WY​Y†)⊤(Ip​−YY†))/2,gradhr+​([Y])​=2gradf(X)YWY−1​,

and if [Y][Y][Y] is a Riemannian first-order stationary point of (18a),

Hess⁡hr+([Y])‾[θ,θ]=Hess⁡f(X)[LYr+(θ),LYr+(θ)]∀θ∈HY,\overline{\operatorname{Hess}h_{r+}([Y])}[\theta,\theta]=\operatorname{Hess}f(X)[\mathcal L^{r+}_Y(\theta),\mathcal L^{r+}_Y(\theta)]\quad\forall\theta\in\mathcal H_Y,Hesshr+​([Y])​[θ,θ]=Hessf(X)[LYr+​(θ),LYr+​(θ)]∀θ∈HY​,

both Hessians have d=pr−(r2−r)/2d=pr-(r^2-r)/2d=pr−(r2−r)/2 eigenvalues, and λi(Hess⁡hr+([Y])‾)\lambda_i(\overline{\operatorname{Hess}h_{r+}([Y])})λi​(Hesshr+​([Y])​) lies between 2σr(PWY−1P⊤)λi(Hess⁡f(X))2\sigma_r(PW_Y^{-1}P^\top)\lambda_i(\operatorname{Hess}f(X))2σr​(PWY−1​P⊤)λi​(Hessf(X)) and 4σ1(PWY−1P⊤)λi(Hess⁡f(X))4\sigma_1(PW_Y^{-1}P^\top)\lambda_i(\operatorname{Hess}f(X))4σ1​(PWY−1​P⊤)λi​(Hessf(X)).

Milestones

  1. Lemma 6: Y1Y1⊤=Y2Y2⊤Y_1Y_1^\top=Y_2Y_2^\topY1​Y1⊤​=Y2​Y2⊤​ iff Y2=Y1OY_2=Y_1OY2​=Y1​O; U1B1U1⊤=U2B2U2⊤U_1B_1U_1^\top=U_2B_2U_2^\topU1​B1​U1⊤​=U2​B2​U2⊤​ iff U2=U1OU_2=U_1OU2​=U1​O, B2=O⊤B1OB_2=O^\top B_1OB2​=O⊤B1​O; Mr+={YY⊤}={UBU⊤}\mathcal M_{r+}=\{YY^\top\}=\{UBU^\top\}Mr+​={YY⊤}={UBU⊤}.
  2. Lemma 3: Mr+e\mathcal M^e_{r+}Mr+e​ is a smooth embedded submanifold of dimension pr−r(r−1)/2pr-r(r-1)/2pr−r(r−1)/2, with tangent space in the block form (14).
  3. Lemma 4 (i): explicit VY\mathcal V_YVY​, HY\mathcal H_YHY​ and their dimensions.
  4. Lemma 1 on R∗p×r\mathbb R_*^{p\times r}R∗p×r​: the total-space gradient is already horizontal.
  5. Proposition 1, embedded bullet: the formulas (19) for grad⁡f\operatorname{grad}fgradf and Hess⁡f\operatorname{Hess}fHessf.
  6. Proposition 1, quotient bullet: the formulas (20) for the lifted gradient and Hessian.
  7. Proposition 2: LYr+\mathcal L^{r+}_YLYr+​ is a bijection HY→TXMr+e\mathcal H_Y\to T_X\mathcal M^e_{r+}HY​→TX​Mr+e​.
  8. Proposition 2, (23): 2σr(PWY−1P⊤)gˉY(θ,θ)≤∥LYr+θ∥F2≤4σ1(PWY−1P⊤)gˉY(θ,θ)2\sigma_r(PW_Y^{-1}P^\top)\bar g_Y(\theta,\theta)\le\|\mathcal L^{r+}_Y\theta\|_F^2\le4\sigma_1(PW_Y^{-1}P^\top)\bar g_Y(\theta,\theta)2σr​(PWY−1​P⊤)gˉ​Y​(θ,θ)≤∥LYr+​θ∥F2​≤4σ1​(PWY−1​P⊤)gˉ​Y​(θ,θ).
  9. Theorem 2: the abstract sandwich inequality for spectra of two quadratic forms related by a bijection with bounded metric distortion.

Significance

Theorem 3 says that at stationary points the two geometries see the same second-order landscape: the Hessians are congruent through LYr+\mathcal L^{r+}_YLYr+​, so their eigenvalues have the same signs and comparable magnitudes, with explicit factors depending on WYW_YWY​ and the spectrum of XXX. The paper derives from it (Corollary 1) that first-order stationary points, second-order stationary points and strict saddles correspond between the embedded and quotient formulations, so a landscape result proved in one geometry transfers to the other. The choice of weight WYW_YWY​ (flat IrI_rIr​, right-invariant (Y⊤Y)−1(Y^\top Y)^{-1}(Y⊤Y)−1, or Y⊤YY^\top YY⊤Y) changes the comparison constants, which is how the paper relates the conditioning of the two approaches.

The result is proved in the paper; it is not formalized anywhere. A formal development adds machine-checked Riemannian gradients and Hessians on a concrete embedded submanifold and on a concrete quotient, a checked horizontal-space computation, and a reusable abstract sandwich theorem for max–min eigenvalues. Corollary 1 and the parallel results for the polar factorization and for general rank-rrr matrices (Theorems 4–7) are natural follow-up missions on the same definitions.

Difficulty

The identities (19), (20) and (34) are matrix calculus once the geometric objects are pinned down; the difficulty is that the definitions are intrinsic. The embedded Hessian requires differentiating the tangent projection PTXMr+eP_{T_X\mathcal M^e_{r+}}PTX​Mr+e​​ along the manifold, which produces the curvature term 2⟨∇f(X),U⊥DΣ−1D⊤U⊥⊤⟩2\langle\nabla f(X),U_\perp D\Sigma^{-1}D^\top U_\perp^\top\rangle2⟨∇f(X),U⊥​DΣ−1D⊤U⊥⊤​⟩; the obvious computation that ignores the moving tangent space gives the wrong Hessian. The quotient Hessian involves the derivative of the weight WYW_YWY​ and needs the horizontal-space description of Lemma 4 to see that the projection in (5) can be dropped. Identifying span⁡\operatorname{span}span of the tangent cone with the block form (14) needs an explicit chart of the rank-rrr PSD set. The final sandwich requires a max–min (Courant–Fischer) argument relative to two different inner products, and the order of the bounds flips for negative eigenvalues.

Formalization scope

  • Ra×b\mathbb R^{a\times b}Ra×b is EuclideanSpace ℝ (Fin a × Fin b) (Frobenius inner product) with matrix views toMat/ofMat. The weight WWW takes values in Rr×r\mathbb R^{r\times r}Rr×r in the same form so that DWY\mathrm DW_YDWY​ is defined.
  • The embedded tangent space and Riemannian gradient are the published platform definitions ProjLikeRetr.Retractor.tangentSpace (span of the tangent cone) and ZORiem.RGD.rgrad (projected Euclidean gradient); "smooth embedded submanifold of dimension ddd" is the published coordinate-slice predicate ProjLikeRetr.Retractor.IsSubmanifold k d, for every kkk.
  • The embedded Hessian is a curve-defined predicate on a quadratic form; the quotient Hessian is the Koszul-formula form gˉY(DG[θ],θ)+12Dgˉ(θ,θ)[G]\bar g_Y(\mathrm DG[\theta],\theta)+\tfrac12\mathrm D\bar g(\theta,\theta)[G]gˉ​Y​(DG[θ],θ)+21​Dgˉ​(θ,θ)[G]. Neither is defined by the paper's formulas (19), (20) or (34): those are theorems, and a formalization that defined the Hessians or gradients by them would make the mission trivial.
  • λk\lambda_kλk​ is the max–min value over kkk-dimensional subspaces (the paper's Lemma 13); "sandwiched between aaa and bbb" means min⁡(a,b)≤μ≤max⁡(a,b)\min(a,b)\le\mu\le\max(a,b)min(a,b)≤μ≤max(a,b); σ1,σr\sigma_1,\sigma_rσ1​,σr​ of the symmetric positive definite PWY−1P⊤PW_Y^{-1}P^\topPWY−1​P⊤ are its extreme Rayleigh quotients.
  • Conventions: 0<r≤p0<r\le p0<r≤p; fff is C2C^2C2 and symmetric; WYW_YWY​ is positive definite on R∗p×r\mathbb R_*^{p\times r}R∗p×r​ and WWW is smooth there (the meaning of "Riemannian metric"); "UUU spans the top rrr eigenspace of YY⊤YY^\topYY⊤" is U⊤U=IrU^\top U=I_rU⊤U=Ir​, UU⊤Y=YUU^\top Y=YUU⊤Y=Y; Y†=(Y⊤Y)−1Y⊤Y^\dagger=(Y^\top Y)^{-1}Y^\topY†=(Y⊤Y)−1Y⊤; LYr+\mathcal L^{r+}_YLYr+​ is defined as Yθ⊤+θY⊤Y\theta^\top+\theta Y^\topYθ⊤+θY⊤ rather than by the block formula (22).
  • In Theorem 2 the map L\mathcal LL is assumed linear, as in every application in the paper, and the printed domain HX\mathcal H_XHX​ in (12)–(13) is read as HZ\mathcal H_ZHZ​.
  • Not encoded: the half of Lemma 3 about general rank-rrr matrices, Lemma 4 (ii) (no quotient-manifold structure in Mathlib), the polar factorization geometry and Theorems 4–7, Corollaries 1–2.

Useful contributions include Mathlib-level lemmas on the tangent cone of the rank-rrr PSD set, Courant–Fischer for a form relative to a non-standard inner product, and matrix-calculus lemmas for D(W−1)\mathrm D(W^{-1})D(W−1).

Selected references

  • Y. Luo, X. Li, A. R. Zhang, On Geometric Connections of Embedded and Quotient Geometries in Riemannian Fixed-rank Matrix Optimization, Mathematics of Operations Research, 2024; arXiv:2110.12121v2. https://arxiv.org/abs/2110.12121
  • P.-A. Absil, R. Mahony, R. Sepulchre, Optimization Algorithms on Matrix Manifolds, Princeton University Press, 2008. https://doi.org/10.1515/9781400830244
  • M. Journée, F. Bach, P.-A. Absil, R. Sepulchre, Low-rank optimization on the cone of positive semidefinite matrices, SIAM Journal on Optimization 20(5), 2010. https://doi.org/10.1137/080731359
  • B. Vandereycken, S. Vandewalle, A Riemannian optimization approach for computing low-rank solutions of Lyapunov equations, SIAM J. Matrix Anal. Appl. 31(5), 2010. https://doi.org/10.1137/090764566
  • R. Bhatia, Matrix Analysis, Springer GTM 169, 1997. https://doi.org/10.1007/978-1-4612-0653-8
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AnalysisDynamical SystemsOptimization·Captain: mikedeng1

Examples of Pathological Dynamics of the Subgradient Method for Lipschitz Path-Differentiable Functions: A Bounded Subgradient Sequence That Does Not Converge for a Whitney-Stratifiable KŁ FunctionResearch Paper

Motivation

The small-step subgradient method is the basic algorithm for minimizing a nonsmooth, nonconvex, locally Lipschitz function f:Rn→Rf:\mathbb R^n\to\mathbb Rf:Rn→R. It is also the scheme behind stochastic gradient training of neural networks with nonsmooth activations. From a starting point x0x_0x0​ it iterates

xi+1=xi−εivi,vi∈∂cf(xi),x_{i+1}=x_i-\varepsilon_i v_i,\qquad v_i\in\partial^c f(x_i),xi+1​=xi​−εi​vi​,vi​∈∂cf(xi​),

with step sizes εi→0\varepsilon_i\to0εi​→0 and ∑iεi=+∞\sum_i\varepsilon_i=+\infty∑i​εi​=+∞. The basic question is whether a bounded run converges. For smooth fff, and for continuous-time subgradient flows, convergence follows from a Kurdyka–Łojasiewicz (KŁ) inequality together with tame geometry such as Whitney stratifiability (Bolte, Daniilidis, Lewis, Shiota 2007; Absil, Mahony, Andrews 2005). Whether the same hypotheses suffice for the discrete nonsmooth method was open.

R. Ríos-Zertuche (arXiv:2007.11699, published in Math. Oper. Res. 2022) is a companion to the work of Bolte, Pauwels and Ríos-Zertuche on the long-term dynamics of the subgradient method for path-differentiable functions (arXiv:2006.00098). That work proves positive results, such as slowdown near limit points and convergence of the values under the weak Sard condition. The examples paper shows that these results cannot be improved to convergence of the iterates. Its first example (Section 2) lives on R2\mathbb R^2R2 and is the subject of this mission.

Setting

For a locally Lipschitz f:Rn→Rf:\mathbb R^n\to\mathbb Rf:Rn→R, the Clarke subdifferential ∂cf(x)\partial^c f(x)∂cf(x) is the convex envelope of all limits lim⁡∇f(yk)\lim\nabla f(y_k)lim∇f(yk​) along sequences yk→xy_k\to xyk​→x of points where fff is differentiable. The critical set is crit⁡f={x:0∈∂cf(x)}\operatorname{crit}f=\{x:0\in\partial^c f(x)\}critf={x:0∈∂cf(x)}.

A subgradient sequence (Definition 1) is a sequence obeying the recursion above with positive steps εi→0\varepsilon_i\to0εi​→0, ∑εi=+∞\sum\varepsilon_i=+\infty∑εi​=+∞. The function fff is path-differentiable (Definition 2) if for every Lipschitz curve γ\gammaγ and almost every ttt, (f∘γ)′(t)=v⋅γ′(t)(f\circ\gamma)'(t)=v\cdot\gamma'(t)(f∘γ)′(t)=v⋅γ′(t) for all v∈∂cf(γ(t))v\in\partial^c f(\gamma(t))v∈∂cf(γ(t)). It satisfies the weak Sard condition (Definition 3) if it is constant on each connected component of crit⁡f\operatorname{crit}fcritf. It is Whitney C∞C^\inftyC∞-stratifiable (Definition 5) if its graph in Rn+1\mathbb R^{n+1}Rn+1 is a locally finite union of disjoint connected C∞C^\inftyC∞ submanifolds. These pieces must satisfy the frontier condition and Whitney's condition A: limits of tangent spaces of a stratum contain the tangent spaces of the strata in its boundary.

The example works on R2\mathbb R^2R2. For i≥2i\ge2i≥2 let

ϑi=∑k=2i1klog⁡k,xi=[1+(−1)ii](cos⁡ϑi,sin⁡ϑi),\vartheta_i=\sum_{k=2}^{i}\frac1{k\log k},\qquad x_i=\Bigl[1+\frac{(-1)^i}{i}\Bigr](\cos\vartheta_i,\sin\vartheta_i),ϑi​=k=2∑i​klogk1​,xi​=[1+i(−1)i​](cosϑi​,sinϑi​),

εi=∥xi+1−xi∥\varepsilon_i=\|x_{i+1}-x_i\|εi​=∥xi+1​−xi​∥ and vi=−(xi+1−xi)/εiv_i=-(x_{i+1}-x_i)/\varepsilon_ivi​=−(xi+1​−xi​)/εi​. Let φ(x)=∣1−∥x∥∣\varphi(x)=|1-\|x\||φ(x)=∣1−∥x∥∣ be the distance to the unit circle S1S^1S1. Let ψ\psiψ be a smooth radial bump with values in [0,1][0,1][0,1], equal to 111 on B1(0)B_1(0)B1​(0), vanishing for ∥x∥≥2\|x\|\ge2∥x∥≥2 and non-increasing along rays. Set ψi(x)=ψ(2i(x−xi))\psi_i(x)=\psi(2^i(x-x_i))ψi​(x)=ψ(2i(x−xi​)) and Vi(x)=(x−xi)⋅vi+1/iV_i(x)=(x-x_i)\cdot v_i+1/iVi​(x)=(x−xi​)⋅vi​+1/i. For i0≥2i_0\ge2i0​≥2,

f(x)=(1−∑i≥i0ψi(x))φ(x)+∑i≥i0ψi(x)Vi(x).(4)f(x)=\Bigl(1-\sum_{i\ge i_0}\psi_i(x)\Bigr)\varphi(x)+\sum_{i\ge i_0}\psi_i(x)V_i(x).\tag{4}f(x)=(1−i≥i0​∑​ψi​(x))φ(x)+i≥i0​∑​ψi​(x)Vi​(x).(4)

Formalization targets

Goal

There are f:R2→Rf:\mathbb R^2\to\mathbb Rf:R2→R, steps (εi)(\varepsilon_i)(εi​) and a sequence (xi)(x_i)(xi​) such that (xi)(x_i)(xi​) is a bounded, non-convergent subgradient sequence of fff, and fff has all of the following properties:

  • it is Lipschitz and path-differentiable;
  • it satisfies the weak Sard condition;
  • it is Whitney C∞C^\inftyC∞-stratifiable;
  • it is C∞C^\inftyC∞ on a ball around every xix_ixi​;
  • it satisfies
∥∇f(x)∥≥12for all x∉crit⁡f.\|\nabla f(x)\|\ge\tfrac12\qquad\text{for all }x\notin\operatorname{crit}f.∥∇f(x)∥≥21​for all x∈/critf.

This is the paper's negative answer to its question Q9, combined with its remarks in Q1 and Q12. The witness is left existential.

Milestones

The milestones are the properties of the explicit witness (4):

  • the step-size estimates (εi→0\varepsilon_i\to0εi​→0, ∑εi=∞\sum\varepsilon_i=\infty∑εi​=∞, ∑εi2<∞\sum\varepsilon_i^2<\infty∑εi2​<∞);
  • Lemma 7: viv_ivi​ is close to ±xi/∥xi∥\pm x_i/\|x_i\|±xi​/∥xi​∥, and radial projection is Lipschitz near xix_ixi​;
  • Proposition 6 (i)–(vii): smoothness off S1∪{0}S^1\cup\{0\}S1∪{0}; ∇f=vi\nabla f=v_i∇f=vi​ on B1/2i(xi)B_{1/2^i}(x_i)B1/2i​(xi​), so that (xi)(x_i)(xi​) is a subgradient sequence; ∂cf(p)={ap:a∈[−1,1]}\partial^c f(p)=\{ap:a\in[-1,1]\}∂cf(p)={ap:a∈[−1,1]} on S1S^1S1; crit⁡f=S1∪{0}\operatorname{crit}f=S^1\cup\{0\}critf=S1∪{0}; Lipschitz path-differentiability; Whitney stratifiability; and ∥∇f∥>1/2\|\nabla f\|>1/2∥∇f∥>1/2 off the critical set;
  • the weak Sard condition;
  • acc⁡{xi}=S1\operatorname{acc}\{x_i\}=S^1acc{xi​}=S1, with boundedness and non-convergence.

Significance

The example is a counterexample: the standard toolbox of tame geometry plus a KŁ inequality does not give convergence of the discrete small-step subgradient method, even with a uniform gradient lower bound away from the critical set and the weak Sard condition. In continuous time the same hypotheses give convergence. The gap therefore comes from discretization. Any convergence proof for nonsmooth subgradient methods needs further structure, such as definability in an o-minimal structure or a stronger KŁ inequality near the critical set. Q12 adds that requiring the iterates to stay in the full-measure set of differentiability points does not help.

The result is proved in the paper; to our knowledge none of it is formalized. Formalizing it gives the first machine-checked Clarke-subdifferential, path-differentiability and Whitney-stratification counterexample. It also gives reusable estimates for an explicit sequence spiralling onto a circle.

Difficulty

Most of the steps are explicit estimates, but three of them are delicate.

  • The Clarke subdifferential on S1S^1S1. It must be computed although infinitely many bumps accumulate there. Near each xix_ixi​ the gradient of fff contains the term ∇ψi (Vi−φ)\nabla\psi_i\,(V_i-\varphi)∇ψi​(Vi​−φ), where ∇ψi\nabla\psi_i∇ψi​ is of size 2i2^i2i. Showing that the limiting gradients are still only ±p\pm p±p requires the second-order agreement of ViV_iVi​ and φ\varphiφ on B1/2i−1(xi)B_{1/2^{i-1}}(x_i)B1/2i−1​(xi​), and that rests on the estimate of Lemma 7.
  • Path differentiability. It does not follow from local Lipschitz continuity. A Lipschitz curve may cross the circle at uncountably many times, so the chain rule has to be checked for every element of ∂cf(γ(t))\partial^c f(\gamma(t))∂cf(γ(t)) at almost every such time.
  • Whitney's condition A. It must hold where the two-dimensional strata of the graph meet the circle stratum. That requires control of the tangent planes of the graph along sequences entering the bump regions.

Formalization scope

Everything lives in EuclideanSpace ℝ (Fin n). The definitions follow these conventions:

  • ∂cf(x)\partial^c f(x)∂cf(x) is the convex hull of the published ShorNonsmooth.AlmostDiff.almostGradients, which uses cluster points of the gradients rather than limits; the two sets are the same.
  • Path differentiability quantifies over every Lipschitz curve and every element of ∂cf(γ(t))\partial^c f(\gamma(t))∂cf(γ(t)), and also asserts that γ\gammaγ is differentiable at ttt, which holds almost everywhere by Rademacher's theorem.
  • Strata are connected, pairwise disjoint and locally finite at the points of the graph. Each is a CkC^kCk coordinate-slice submanifold (the published ProjLikeRetr.Retractor.IsSubmanifold) for every kkk. Tangent spaces are spans of tangent cones, and Grassmannian convergence is convergence of the subspace gap to 000.
  • The bump is an arbitrary BumpProfile with exactly the properties listed on p. 6, and the series in (4) are tsums. The indices i<2i<2i<2, where 1/0=01/0=01/0=0 and log⁡1=0\log 1=0log1=0 in Lean, are never used.

Four statements are adjusted, and each adjustment is disclosed in its item:

  • Proposition 6 (i) is stated on R2∖(S1∪{0})\mathbb R^2\setminus(S^1\cup\{0\})R2∖(S1∪{0}), as in the paper's proof, because fff has a cone point at 000.
  • The last link "<2/i<2/i<2/i" of the step-size chain is false and is dropped.
  • Proposition 6 (ii), (iv), (vii) and the weak Sard claim hold for i0i_0i0​ beyond a threshold depending on the bump. For small i0i_0i0​ the bump supports overlap.
  • The KŁ clauses also assert differentiability, since Lean's gradient is 000 at non-differentiable points.

The goal cannot be met trivially. Boundedness of the sequence and the conditions εi→0\varepsilon_i\to0εi​→0, ∑εi=∞\sum\varepsilon_i=\infty∑εi​=∞ are part of it, and they rule out an affine fff. Every regularity property is a separate conjunct. Contributions that develop the geometry of Whitney stratifications and path differentiability in Lean are reusable well beyond this example.

Selected references

  • R. Ríos-Zertuche, Examples of pathological dynamics of the subgradient method for Lipschitz path-differentiable functions, arXiv:2007.11699v1, 2020; Math. Oper. Res., 2022. https://arxiv.org/abs/2007.11699
  • J. Bolte, E. Pauwels, R. Ríos-Zertuche, Long term dynamics of the subgradient method for Lipschitz path differentiable functions, arXiv:2006.00098, 2020. https://arxiv.org/abs/2006.00098
  • J. Bolte, A. Daniilidis, A. Lewis, M. Shiota, Clarke subgradients of stratifiable functions, SIAM J. Optim. 18 (2007). https://doi.org/10.1137/060670080
  • D. Davis, D. Drusvyatskiy, S. Kakade, J. D. Lee, Stochastic subgradient method converges on tame functions, Found. Comput. Math. 20 (2020). https://arxiv.org/abs/1804.07795
  • P.-A. Absil, R. Mahony, B. Andrews, Convergence of the iterates of descent methods for analytic cost functions, SIAM J. Optim. 16 (2005). https://doi.org/10.1137/040605266
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Actuarial ScienceOperations ResearchProbability·Captain: mikedeng1

A Theory for Measures of Tail Risk: A Tail Risk Measure Is Coherent, Convex or Monetary if and Only if Its Generator IsResearch Paper

Motivation

Banking and insurance regulation measures capital requirements with risk measures that look only at the tail of a loss distribution. The Basel framework moved from Value-at-Risk (VaR) to Expected Shortfall (ES) for market risk (BCBS, Minimum capital requirements for market risk, 2016), and both VaR and ES at level ppp depend on a loss only through its distribution beyond the ppp-quantile. Liu and Wang (SSRN 2841909; Mathematics of Operations Research 46(3), 2021, doi:10.1287/moor.2020.1072) isolate this feature as a definition. A tail risk measure is any risk measure that depends only on the tail, and every such measure is generated by an ordinary law-invariant risk measure applied to the tail. The paper then asks which of the classical properties of risk measures (Artzner et al. 1999; Föllmer and Schied 2002) survive this construction.

The answer to that question is a practical design rule. A regulator or risk manager who wants a coherent tail risk measure can choose any coherent law-invariant risk measure and apply it to the tail. The theorem guarantees that the result is again coherent, and that nothing is lost by working only with generators.

Setting

Fix an atomless probability space (Ω,F,P)(\Omega,\mathcal F,\mathbb P)(Ω,F,P): every event of positive probability contains an event of strictly smaller positive probability. A random variable X:Ω→RX:\Omega\to\mathbb RX:Ω→R is a loss when positive and a profit when negative. Its distribution function is FX(x)=P(X≤x)F_X(x)=\mathbb P(X\le x)FX​(x)=P(X≤x). The space of risks is X=L∞\mathcal X=L^\inftyX=L∞, the measurable, essentially bounded random variables. A risk measure is a real-valued functional ρ\rhoρ on X\mathcal XX.

For p∈(0,1)p\in(0,1)p∈(0,1), the ppp-tail of XXX is a random variable XpX_pXp​ with distribution function

P(Xp≤x)=(P(X≤x)−p)+1−p,x∈R,(2)\mathbb P(X_p\le x)=\frac{(\mathbb P(X\le x)-p)_+}{1-p},\qquad x\in\mathbb R, \tag{2}P(Xp​≤x)=1−p(P(X≤x)−p)+​​,x∈R,(2)

the conditional law of XXX beyond its ppp-quantile. A risk measure ρ\rhoρ is a ppp-tail risk measure if ρ(X)=ρ(Y)\rho(X)=\rho(Y)ρ(X)=ρ(Y) whenever XpX_pXp​ and YpY_pYp​ have the same law. A pair (ρ,ρ∗)(\rho,\rho^*)(ρ,ρ∗) is a ppp-tail pair if ρ∗\rho^*ρ∗ is law-invariant and

ρ(X)=ρ∗(Xp),X∈X,(3)\rho(X)=\rho^*(X_p),\qquad X\in\mathcal X, \tag{3}ρ(X)=ρ∗(Xp​),X∈X,(3)

in which case ρ∗\rho^*ρ∗ is a ppp-generator of ρ\rhoρ. For example, ESp(X)=E[Xp]\mathrm{ES}_p(X)=\mathbb E[X_p]ESp​(X)=E[Xp​] is generated by the expectation. The mixture X(p)X^{(p)}X(p) has distribution function p 1{x≥ess-inf⁡X}+(1−p)FX(x)p\,\mathbb 1_{\{x\ge\operatorname{ess\text{-}inf}X\}}+(1-p)F_X(x)p1{x≥ess-infX}​+(1−p)FX​(x): it adds mass ppp at the essential infimum of XXX.

The classical properties are those of Appendix A of the paper:

  • (A1) monotonicity: ρ(X)≤ρ(Y)\rho(X)\le\rho(Y)ρ(X)≤ρ(Y) when X≤YX\le YX≤Y a.s.;
  • (A2) translation invariance: ρ(X−m)=ρ(X)−m\rho(X-m)=\rho(X)-mρ(X−m)=ρ(X)−m;
  • (A3) convexity: ρ(λX+(1−λ)Y)≤λρ(X)+(1−λ)ρ(Y)\rho(\lambda X+(1-\lambda)Y)\le\lambda\rho(X)+(1-\lambda)\rho(Y)ρ(λX+(1−λ)Y)≤λρ(X)+(1−λ)ρ(Y) for λ∈[0,1]\lambda\in[0,1]λ∈[0,1];
  • (A4) positive homogeneity: ρ(λX)=λρ(X)\rho(\lambda X)=\lambda\rho(X)ρ(λX)=λρ(X) for λ>0\lambda>0λ>0;
  • (A5) subadditivity;
  • (A6) comonotonic additivity;
  • (A7) ≺cx\prec_{\mathrm{cx}}≺cx​-monotonicity.

A monetary risk measure satisfies (A1)–(A2), a convex one (A1)–(A3), and a coherent one (A1)–(A4) (Definition A.1).

Formalization targets

Goal: Theorem 1 (iii)

For p∈(0,1)p\in(0,1)p∈(0,1) and a ppp-tail pair (ρ,ρ∗)(\rho,\rho^*)(ρ,ρ∗) on L∞L^\inftyL∞,

ρ coherent  ⟺  ρ∗ coherent,ρ convex  ⟺  ρ∗ convex,ρ monetary  ⟺  ρ∗ monetary.\rho\ \text{coherent}\iff\rho^*\ \text{coherent},\qquad \rho\ \text{convex}\iff\rho^*\ \text{convex},\qquad \rho\ \text{monetary}\iff\rho^*\ \text{monetary}.ρ coherent⟺ρ∗ coherent,ρ convex⟺ρ∗ convex,ρ monetary⟺ρ∗ monetary.

All three equivalences are part of the goal. No normalization such as ρ(0)=0\rho(0)=0ρ(0)=0 is assumed.

Milestones

  • Lemma B.1 (p. 19): (X(p))p=dX(X^{(p)})_p\overset{d}{=}X(X(p))p​=dX; the maps X↦XpX\mapsto X_pX↦Xp​ and X↦X(p)X\mapsto X^{(p)}X↦X(p) preserve the stochastic order ≺st\prec_{\mathrm{st}}≺st​; and X≺stXpX\prec_{\mathrm{st}}X_pX≺st​Xp​.
  • Proposition 1 (p. 7): every ppp-tail risk measure has a ppp-generator, which is unique and given by ρ∗(X)=ρ(X(p))\rho^*(X)=\rho(X^{(p)})ρ∗(X)=ρ(X(p)).
  • Eq. (14) (p. 20): for B∼Bern(p)B\sim\mathrm{Bern}(p)B∼Bern(p) independent of ZZZ and t≤ess-inf⁡Zt\le\operatorname{ess\text{-}inf}Zt≤ess-infZ, (tB+Z(1−B))p=d(ess-inf⁡(Z)B+Z(1−B))p=dZ(tB+Z(1-B))_p\overset{d}{=}(\operatorname{ess\text{-}inf}(Z)B+Z(1-B))_p\overset{d}{=}Z(tB+Z(1−B))p​=d(ess-inf(Z)B+Z(1−B))p​=dZ.
  • Theorem 1 (i) (p. 9): monotonicity, translation invariance, positive homogeneity and comonotonic additivity each pass between ρ\rhoρ and ρ∗\rho^*ρ∗ in both directions.
  • Theorem 1 (ii) (p. 9): subadditivity, convexity and ≺cx\prec_{\mathrm{cx}}≺cx​-monotonicity pass from ρ\rhoρ to ρ∗\rho^*ρ∗. The converses fail (Example 1, the tail standard deviation).
  • Theorem 3 (p. 10): for a ppp-tail pair of monotone risk measures and marginals F1,…,FnF_1,\dots,F_nF1​,…,Fn​,
sup⁡{ρ(S):S∈Sn(F1,…,Fn)}=sup⁡{ρ∗(T):T∈Sn(F1[p],…,Fn[p])},\sup\{\rho(S):S\in\mathcal S_n(F_1,\dots,F_n)\}=\sup\{\rho^*(T):T\in\mathcal S_n(F_1^{[p]},\dots,F_n^{[p]})\},sup{ρ(S):S∈Sn​(F1​,…,Fn​)}=sup{ρ∗(T):T∈Sn​(F1[p]​,…,Fn[p]​)},

where Sn\mathcal S_nSn​ is the set of sums Y1+⋯+YnY_1+\dots+Y_nY1​+⋯+Yn​ with Yi∼FiY_i\sim F_iYi​∼Fi​ (resp. Fi[p]F_i^{[p]}Fi[p]​, the law of the ppp-tail).

Significance

The result. Theorem 1 (iii) makes the generator a complete parametrization of coherent and convex tail risk measures. Coherent tail risk measures are exactly ρ∗(Xp)\rho^*(X_p)ρ∗(Xp​) with ρ∗\rho^*ρ∗ coherent and law-invariant, so representation results for law-invariant coherent risk measures (Kusuoka 2001) transfer to tail risk measures. The paper uses this for dual representations (Appendix G) and for the bound ρ≥ESp\rho\ge\mathrm{ES}_pρ≥ESp​ of Theorem 2. Theorem 3 reduces worst-case risk aggregation for a tail risk measure to the same problem for its generator on tail marginals. It contains classical results on worst-case VaR (Bernard et al. 2014, Lemma 4.3) and the subadditivity of ES as special cases.

Formalizing it. The results are proved in the paper; none of them is machine-checked. The mission produces a Lean statement of tail risk measures and their generators that later missions on tail risk can import. It also produces formal versions of the distributional identities (Lemma B.1, eq. (14)) on which the paper's proofs rest, and a statement of worst-case aggregation in extended-real suprema. A complete development would also be the first formal proof that ES-type constructions preserve coherence through a general generator, rather than for one specific measure.

Difficulty

Several directions are routine. Monotonicity, translation invariance and positive homogeneity pass from ρ∗\rho^*ρ∗ to ρ\rhoρ because X↦XpX\mapsto X_pX↦Xp​ commutes with shifts and positive scalings and preserves ≺st\prec_{\mathrm{st}}≺st​. The converse directions go through X(p)X^{(p)}X(p).

Convexity is the obstruction. The obvious argument would compare (λX+(1−λ)Y)p(\lambda X+(1-\lambda)Y)_p(λX+(1−λ)Y)p​ with λXp+(1−λ)Yp\lambda X_p+(1-\lambda)Y_pλXp​+(1−λ)Yp​, but the tail of a sum is not the sum of the tails. The event "beyond the ppp-quantile" for the sum differs from the corresponding events for XXX and YYY, so no pointwise or comonotone coupling identifies them. Example 1 makes this concrete: the tail standard deviation is generated by a convex measure and is not convex. Convexity of ρ\rhoρ therefore needs monotonicity of ρ∗\rho^*ρ∗ together with the worst-case aggregation identity of Theorem 3. That identity is a statement about all dependence structures with given marginals, and it requires constructing, on an atomless space, couplings whose tails dominate a given sum.

Formalization scope

  • Domain. The space of risks is L∞L^\inftyL∞ (TailRiskSharing.TailConv.Linf), as the paper suggests on p. 5. Then X∗=X\mathcal X^*=\mathcal XX∗=X, every risk measure is a real-valued function on Ω→R\Omega\to\mathbb RΩ→R, and every property quantifies over L∞L^\inftyL∞ only. The general cone X⊇L∞\mathcal X\supseteq L^\inftyX⊇L∞ with (−∞,∞](-\infty,\infty](−∞,∞]-valued risk measures is not stated.
  • Atomlessness. The probability space is atomless in the classical sense (TailRiskSharing.VaRConv.IsAtomless), not Mathlib's NoAtoms, which only says that singletons are null.
  • Tails and mixtures are relations on distribution functions: "ZZZ has the law of XpX_pXp​" is the identity (2). The generator relation (3) is required for every Z∈L∞Z\in L^\inftyZ∈L∞ with that law, and no existence of such ZZZ is assumed.
  • Coherence is Definition A.1: monotone, translation-invariant, convex and positively homogeneous. It uses convexity, not subadditivity, and it includes monotonicity.
  • Stochastic orders compare expectations of increasing (resp. convex) test functions. Integrability of f(X)f(X)f(X) and f(Y)f(Y)f(Y) is part of the definition, as in "provided that both expectations exist".
  • Theorem 3. Each marginal FiF_iFi​ is given by a representative in L∞L^\inftyL∞, and the suprema are taken in the extended reals.

A formalization in which ρ∗\rho^*ρ∗ is a fixed Classical.choose of the tail, in which coherence omits monotonicity, or in which atomlessness is replaced by NoAtoms is not this theorem.

A complete development needs the quantile transform on an atomless space, couplings with a prescribed joint law, the elementary identities of Lemma B.1 and eq. (14), and the worst-case aggregation argument of Appendix C. The distributional lemmas, quantile couplings and aggregation sets can be reused in any later mission on law-invariant risk measures. Contributions to any milestone, and to general infrastructure for quantile couplings on atomless spaces, are welcome.

Selected references

  • F. Liu and R. Wang, A Theory for Measures of Tail Risk, SSRN 2841909 (journal accepted version, 2020); Mathematics of Operations Research 46(3), 2021. https://ssrn.com/abstract=2841909, https://doi.org/10.1287/moor.2020.1072
  • P. Artzner, F. Delbaen, J.-M. Eber and D. Heath, Coherent measures of risk, Mathematical Finance 9(3), 1999. https://doi.org/10.1111/1467-9965.00068
  • H. Föllmer and A. Schied, Convex measures of risk and trading constraints, Finance and Stochastics 6(4), 2002. https://doi.org/10.1007/s007800200072
  • S. Kusuoka, On law invariant coherent risk measures, Advances in Mathematical Economics 3, 2001. https://doi.org/10.1007/978-4-431-67891-5_4
  • C. Bernard, X. Jiang and R. Wang, Risk aggregation with dependence uncertainty, Insurance: Mathematics and Economics 54, 2014. https://doi.org/10.1016/j.insmatheco.2013.11.005
  • Basel Committee on Banking Supervision, Minimum capital requirements for market risk, 2016. https://www.bis.org/bcbs/publ/d352.htm
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Machine LearningProbabilityStatistics·Captain: mikedeng1

Data Exploration by Representative Region Selection: Axioms and Convergence: Density Estimates from Arbitrarily Precise Families of RRS Methods Are Consistent in Integrated Absolute ErrorResearch Paper

Motivation

Exploratory data analysis often summarizes a large data set by a small number of representative regions: histogram bins, the leaves of a density estimation tree, balls around cluster centres, or the regions chosen by a covering or kkk-center optimization. Estes, Ball and Lovell (SSRN 3005997; Mathematics of Operations Research, 2021, doi:10.1287/moor.2020.1115) treat all of these as instances of one abstraction, the representative region selection (RRS) method, motivated by summarizing air-traffic ground-delay programs at Newark airport. The first half of their paper proposes axioms for the quality of such summaries. The second half (§6) asks a statistical question: when the data are an i.i.d. sample, do the summaries converge to the population they describe? This mission formalizes that convergence theory, culminating in the consistency of the density estimate that any RRS method induces.

Setting

Let MMM be a set. An RRS method on MMM is a pair (C,f)(\mathcal C, f)(C,f): C⊆2M\mathcal C \subseteq 2^MC⊆2M is a class of allowed regions, and fff maps every finite set S⊆MS \subseteq MS⊆M to a finite set f(S)⊆Cf(S) \subseteq \mathcal Cf(S)⊆C. The coverage region is C(S;f)=⋃A∈f(S)AC(S; f) = \bigcup_{A \in f(S)} AC(S;f)=⋃A∈f(S)​A. The method is sample-covering if S⊆C(S;f)S \subseteq C(S; f)S⊆C(S;f), and sample-intersecting if every A∈f(S)A \in f(S)A∈f(S) contains a point of SSS.

Now let (M,d)(M, d)(M,d) be a metric space with a σ-algebra containing every closed ball, and let X1,X2,…X_1, X_2, \dotsX1​,X2​,… be i.i.d. MMM-valued random variables with law PXP_XPX​. Write Sn={X1,…,Xn}S_n = \{X_1, \dots, X_n\}Sn​={X1​,…,Xn​}, Cn(f)=C(Sn;f)C_n(f) = C(S_n; f)Cn​(f)=C(Sn​;f), and P^X,n(T)\hat P_{X,n}(T)P^X,n​(T) for the fraction of the first nnn observations lying in TTT. The support of PXP_XPX​ is the set of points all of whose closed balls of positive radius have positive probability.

Regularity is imposed on the class, not on the method. A scalable class (C,Θ,R)(\mathcal C, \Theta, R)(C,Θ,R) writes every region as R(θ,λ)R(\theta, \lambda)R(θ,λ) with a shape parameter θ∈Θ\theta \in \Thetaθ∈Θ and a scale λ>0\lambda > 0λ>0, non-decreasing in λ\lambdaλ. It is uniform-scale if increasing the scale by ε\varepsilonε swells every region by a closed ball of a radius δ(ε)\delta(\varepsilon)δ(ε) that does not depend on the region, and uniformly continuous with respect to PXP_XPX​ if changing the scale by δ(ε)\delta(\varepsilon)δ(ε) changes the probability of every region by at most ε\varepsilonε.

A family {(C,fm)}m∈N\{(\mathcal C, f_m)\}_{m \in \mathbb N}{(C,fm​)}m∈N​ is arbitrarily precise if, for every ε>0\varepsilon > 0ε>0, all methods far enough along the family eventually (almost surely, as nnn grows) output regions of diameter at most ε\varepsilonε. A method is uniformly positive with respect to a reference measure μ\muμ if its regions have μ\muμ-measure bounded below, and has asymptotically-bounded cardinality if it eventually outputs at most uuu regions. When PXP_XPX​ has a density gXg_XgX​ with respect to μ\muμ, the RRS density estimate at xxx averages P^X,n(A)/μ(A)\hat P_{X,n}(A)/\mu(A)P^X,n​(A)/μ(A) over the chosen regions AAA that contain xxx:

g^n(x;f)=1∣cn(x;f)∣∑A∈cn(x;f)P^X,n(A)μ(A),cn(x;f)={A∈f(Sn):x∈A},\hat g_n(x; f) = \frac{1}{|c_n(x; f)|} \sum_{A \in c_n(x; f)} \frac{\hat P_{X,n}(A)}{\mu(A)}, \qquad c_n(x; f) = \{A \in f(S_n) : x \in A\},g^​n​(x;f)=∣cn​(x;f)∣1​A∈cn​(x;f)∑​μ(A)P^X,n​(A)​,cn​(x;f)={A∈f(Sn​):x∈A},

and g^n(x;f)=0\hat g_n(x; f) = 0g^​n​(x;f)=0 when no chosen region covers xxx.

Formalization targets

Goal: Theorem 6.5 (p. 28)

If the support KKK of PXP_XPX​ is compact with PX(K)=1P_X(K) = 1PX​(K)=1, gXg_XgX​ is continuous, some closed neighbourhood of KKK has finite μ\muμ-measure, and {fm}\{f_m\}{fm​} is an arbitrarily precise family over a uniform-scale class that is uniformly continuous with respect to PXP_XPX​, with each fmf_mfm​ sample-covering, sample-intersecting, of asymptotically-bounded cardinality and uniformly positive, then almost surely

lim⁡m→∞lim sup⁡n→∞∫M∣gX−g^n(⋅ ;fm)∣ dμ=0.\lim_{m \to \infty} \limsup_{n \to \infty} \int_M \bigl|g_X - \hat g_n(\cdot\,; f_m)\bigr| \, d\mu = 0.m→∞lim​n→∞limsup​∫M​​gX​−g^​n​(⋅;fm​)​dμ=0.

Milestones

  1. Theorem 6.1 (p. 22): such a class is Glivenko–Cantelli, sup⁡A∈C∣P^X,n(A)−PX(A)∣→0\sup_{A \in \mathcal C} |\hat P_{X,n}(A) - P_X(A)| \to 0supA∈C​∣P^X,n​(A)−PX​(A)∣→0 a.s.
  2. Corollary 6.1 (p. 24): the same supremum over the chosen regions A∈f(Sn)A \in f(S_n)A∈f(Sn​).
  3. Lemma 6.1 (p. 24): for a sample-covering method and compact KKK inside the support, sup⁡x∈Kd(x,Cn(f))→0\sup_{x \in K} d(x, C_n(f)) \to 0supx∈K​d(x,Cn​(f))→0 a.s.
  4. Theorem 6.2 (p. 24): with asymptotically-bounded cardinality, PX(K∖Cn(f))→0P_X(K \setminus C_n(f)) \to 0PX​(K∖Cn​(f))→0 a.s.
  5. Corollary 6.2 (p. 25): PX(Cn(f))→1P_X(C_n(f)) \to 1PX​(Cn​(f))→1 a.s.
  6. Theorem 6.4 (p. 26): lim⁡mlim sup⁡nsup⁡x∈Cn(fm)∣gX(x)−g^n(x;fm)∣=0\lim_m \limsup_n \sup_{x \in C_n(f_m)} |g_X(x) - \hat g_n(x; f_m)| = 0limm​limsupn​supx∈Cn​(fm​)​∣gX​(x)−g^​n​(x;fm​)∣=0 a.s.

Significance

The goal shows that one estimator, defined uniformly from any RRS method, is L1L^1L1-consistent under conditions that are checked once for the class of regions and once for the method. Histograms, density estimation trees, and the paper's own minimum-dominating-set and kkk-center summaries (Corollaries 7.1 and 7.2) all become consistent density estimators as soon as they satisfy those conditions. Theorem 6.1 is of independent interest: it is a Glivenko–Cantelli theorem whose hypotheses are geometric and measure-theoretic rather than combinatorial, applying to classes for which no finite VC dimension is known.

The results are proved on paper; none is machine-checked. The mission produces a formal layer for region-based empirical processes (RRS methods, uniform-scale classes, the region-average density estimate) and machine-checked versions of the convergence chain. The formal statements also repair two places where the printed hypotheses are too weak (see Formalization scope), so a completed development certifies corrected theorems, not merely transcribed ones.

Difficulty

The regions an RRS method selects depend on the sample, so the law of large numbers cannot be applied region by region: there are uncountably many candidate regions and no fixed finite family to which the strong law applies. The uniform convergence of Theorem 6.1 must instead come from a finite approximation of the whole class, combining compactness of the support with the uniform-scale and uniform-continuity hypotheses, and the approximation has to work at every scale, including scales smaller than the approximation step. The goal adds a second limit: the error splits into a part on the coverage region, governed by the uniform estimate of Theorem 6.4, and a part on the uncovered portion of the support where the estimate is zero, governed by Corollary 6.2. The two limits (n→∞n \to \inftyn→∞ inside, m→∞m \to \inftym→∞ outside) and the almost-sure quantifier must be interleaved correctly, with countably many null sets collected over mmm.

Formalization scope

All statements live in the namespace RepRegion.Density, with one definitions file RepRegion.Density.Model. MMM is a metric space with an arbitrary σ-algebra in which every closed ball is measurable (no Borel assumption); Ω\OmegaΩ is a probability space; the observations are X : ℕ → Ω → M, measurable, mutually independent (iIndepFun) and identically distributed, indexed from 000. PXP_XPX​ is P.map (X 0). The reference measure μ\muμ is an arbitrary measure on MMM. Regions are Set M, a method is Finset M → Finset (Set M), and the scale map is R : Θ → ℝ → Set M, read only at positive scales.

Committed conventions:

  • the empirical measure counts observations with multiplicity; the paper's ∣T∩Sn∣/n|T \cap S_n|/n∣T∩Sn​∣/n with SnS_nSn​ a set would fail for laws with atoms;
  • the terms R(θ,λ−ε)R(\theta, \lambda - \varepsilon)R(θ,λ−ε) and R(θ,λ−δ)R(\theta, \lambda - \delta)R(θ,λ−δ) of the uniform-scale and uniform-continuity definitions are read as ∅\emptyset∅ when the scale is not positive. In particular, regions of scale at most δ(ε)\delta(\varepsilon)δ(ε) must have probability at most ε\varepsilonε; without this, Theorem 6.1 fails (a counterexample on [0,1][0, 1][0,1] is recorded in its statement);
  • suprema, limits superior and integrals of errors are taken in [0,∞][0, \infty][0,∞]; the integrated error is a lower Lebesgue integral, never a Bochner integral;
  • diameters are stated pairwise (d(x,y)≤Ld(x, y) \le Ld(x,y)≤L), and probabilities of regions are compared with addition rather than truncated subtraction;
  • the regions the methods output have finite μ\muμ-measure, so that g^\hat gg^​ is defined; the paper never states this;
  • the goal's printed conclusion "=ε= \varepsilon=ε" (with ε\varepsilonε unbound) is stated as "=0= 0=0", as its proof and the paper's corollaries establish;
  • the goal assumes gXg_XgX​ continuous on MMM (the paper: on KKK), the hypothesis of Theorem 6.4 that its proof invokes; Theorem 6.4 is stated with gXg_XgX​ uniformly continuous, because with mere continuity it fails for reference measures that do not charge every open set.

A formalization in which the error is a Bochner integral, a supremum is a real sSup, or a diameter is Metric.diam would make the conclusions hold for junk reasons on non-integrable or unbounded inputs; those encodings are ruled out.

A complete development needs the strong law of large numbers for indicators (in Mathlib), finite nets of compact metric sets, and almost-sure hitting arguments for balls of positive probability. The region-based Glivenko–Cantelli theorem and the coverage results are reusable for any later mission on partition-based estimators. Proofs of the individual milestones, alternative arguments, and a version of the goal under continuity of gXg_XgX​ on KKK alone are all welcome.

Selected references

  • A. S. Estes, M. O. Ball, D. J. Lovell, Data Exploration by Representative Region Selection: Axioms and Convergence, Mathematics of Operations Research, 2021. SSRN preprint 3005997: https://ssrn.com/abstract=3005997 ; journal version: https://doi.org/10.1287/moor.2020.1115
  • G. R. Shorack, J. A. Wellner, Empirical Processes with Applications to Statistics, SIAM Classics in Applied Mathematics, 2009. https://doi.org/10.1137/1.9780898719017
  • V. N. Vapnik, A. Ya. Chervonenkis, On the uniform convergence of relative frequencies of events to their probabilities, in Empirical Inference, Springer, 2013 (English translation of the 1968/1971 work). https://doi.org/10.1007/978-3-642-41136-6_3
8 thms1 active userReviewed
AlgebraRepresentation Theory·Captain: mikedeng1

Gradings on Walled Brauer Algebras and Khovanov's Arc Algebra: Mixed Schur–Weyl Duality for gl(m|n) — B_{r,s}(m−n) Maps onto End_g(V^{⊗r}⊗W^{⊗s}), Injectively iff r+s < (m+1)(n+1)Research Paper

Motivation

Schur–Weyl duality says that on the tensor power V⊗NV^{\otimes N}V⊗N of the natural representation of glm(C)\mathfrak{gl}_m(\mathbb C)glm​(C), the symmetric group ΣN\Sigma_NΣN​ acting by place permutations generates the full commutant of glm\mathfrak{gl}_mglm​. It is the bridge between representations of general linear groups and of symmetric groups. Two extensions matter in representation theory and in the theory of tensor categories:

  • Super Schur–Weyl duality. Replacing glm\mathfrak{gl}_mglm​ by the general linear Lie superalgebra glm∣n(C)\mathfrak{gl}_{m|n}(\mathbb C)glm∣n​(C) and inserting Koszul signs, ΣN\Sigma_NΣN​ still generates the commutant of V⊗NV^{\otimes N}V⊗N (Sergeev 1985; Berele and Regev 1987). The kernel is now governed by (m,n)(m,n)(m,n)-hook partitions.
  • Mixed tensor space. On V⊗r⊗W⊗sV^{\otimes r} \otimes W^{\otimes s}V⊗r⊗W⊗s with W=V∗W = V^*W=V∗, the symmetric group must be replaced by the walled Brauer algebra Br,s(δ)B_{r,s}(\delta)Br,s​(δ) of Turaev and Koike, which has diagrams with strands that may turn back.

Brundan and Stroppel (arXiv:1107.0999) prove the combination: mixed Schur–Weyl duality for glm∣n(C)\mathfrak{gl}_{m|n}(\mathbb C)glm∣n​(C). It is the first step towards their main result, a Morita equivalence between Br,s(δ)B_{r,s}(\delta)Br,s​(δ) and an idempotent truncation of Khovanov's generalized arc algebra K(δ)K(\delta)K(δ), from which they derive that Br,s(δ)B_{r,s}(\delta)Br,s​(δ) is Koszul for δ≠0\delta \neq 0δ=0. Comes and Wilson obtained the same duality independently (arXiv:1108.0652); Shader and Moon had a partial result earlier (Commun. Algebra 30, 2002).

Timeline:

  • 1937: Brauer introduces the Brauer algebra for orthogonal and symplectic groups.
  • 1985, 1987: Sergeev, and Berele–Regev, prove super Schur–Weyl duality for glm∣n\mathfrak{gl}_{m|n}glm∣n​ on V⊗NV^{\otimes N}V⊗N.
  • 1989–1994: Turaev and Koike introduce the walled Brauer algebra; Benkart et al. prove mixed duality for glm\mathfrak{gl}_mglm​.
  • 2011: Brundan–Stroppel (Theorem 7.8) and Comes–Wilson prove mixed duality for glm∣n\mathfrak{gl}_{m|n}glm∣n​.

Setting

Fix integers m,n≥0m, n \ge 0m,n≥0 and put δ=m−n\delta = m - nδ=m−n. Let I={1,…,m+n}I = \{1, \dots, m+n\}I={1,…,m+n}, with parity ∣i∣=0|i| = 0∣i∣=0 for i≤mi \le mi≤m and ∣i∣=1|i| = 1∣i∣=1 for i>mi > mi>m. Let VVV have basis v1,…,vm+nv_1, \dots, v_{m+n}v1​,…,vm+n​ with viv_ivi​ of parity ∣i∣|i|∣i∣, and W=V∗W = V^*W=V∗ the dual basis w1,…,wm+nw_1, \dots, w_{m+n}w1​,…,wm+n​. The Lie superalgebra g=glm∣n(C)\mathfrak g = \mathfrak{gl}_{m|n}(\mathbb C)g=glm∣n​(C) is End⁡(V)\operatorname{End}(V)End(V), spanned by matrix units ea,be_{a,b}ea,b​ of parity ∣a∣+∣b∣|a| + |b|∣a∣+∣b∣, acting by

ea,bvk=δb,kva,ea,bwk=−δa,k(−1)(∣a∣+∣b∣)∣a∣wb.e_{a,b} v_k = \delta_{b,k} v_a, \qquad e_{a,b} w_k = -\delta_{a,k} (-1)^{(|a|+|b|)|a|} w_b .ea,b​vk​=δb,k​va​,ea,b​wk​=−δa,k​(−1)(∣a∣+∣b∣)∣a∣wb​.

It acts on V⊗r⊗W⊗sV^{\otimes r} \otimes W^{\otimes s}V⊗r⊗W⊗s, with basis viL⊗wiRv_{\mathbf i^{\mathrm L}} \otimes w_{\mathbf i^{\mathrm R}}viL​⊗wiR​ for i∈Ir+s\mathbf i \in I^{r+s}i∈Ir+s, through Δ(x)=x⊗1+1⊗x\Delta(x) = x \otimes 1 + 1 \otimes xΔ(x)=x⊗1+1⊗x and the sign rule (a⊗b)(c⊗d)=(−1)∣b∣∣c∣ac⊗bd(a \otimes b)(c \otimes d) = (-1)^{|b||c|} ac \otimes bd(a⊗b)(c⊗d)=(−1)∣b∣∣c∣ac⊗bd. The super-commutant End⁡g(V⊗r⊗W⊗s)\operatorname{End}_{\mathfrak g}(V^{\otimes r} \otimes W^{\otimes s})Endg​(V⊗r⊗W⊗s) is the space of all linear maps fff, not necessarily homogeneous, annihilated by the action (xf)(u)=x(f(u))−(−1)∣x∣∣f∣f(xu)(xf)(u) = x(f(u)) - (-1)^{|x||f|} f(xu)(xf)(u)=x(f(u))−(−1)∣x∣∣f∣f(xu) of every x∈gx \in \mathfrak gx∈g.

A walled Brauer diagram pairs the 2(r+s)2(r+s)2(r+s) vertices on the top and bottom edges of a rectangle, with a wall after position rrr: a vertical strand joins vertices on the same side of the wall and a horizontal strand joins vertices on opposite sides. These diagrams are a basis of Br,s(δ)B_{r,s}(\delta)Br,s​(δ); the product στ\sigma\tauστ puts σ\sigmaσ under τ\tauτ and multiplies by δt\delta^tδt for ttt removed circles. Colouring the bottom vertices by i\mathbf ii and the top vertices by j\mathbf jj, the weight wt(iσj)\mathrm{wt}({}_{\mathbf i}\sigma_{\mathbf j})wt(i​σj​) is 000 unless every strand has equally coloured ends, and otherwise (−1)(-1)(−1) raised to the sum of ∣k∣∣l∣|k||l|∣k∣∣l∣ over the crossings of strands of colours k,lk, lk,l plus ∣k∣|k|∣k∣ over the bottom horizontal strands of colour kkk (7.5). The right action

(viL⊗wiR)⋅σ=∑jwt(iσj) vjL⊗wjR(v_{\mathbf i^{\mathrm L}} \otimes w_{\mathbf i^{\mathrm R}}) \cdot \sigma = \sum_{\mathbf j} \mathrm{wt}({}_{\mathbf i}\sigma_{\mathbf j})\, v_{\mathbf j^{\mathrm L}} \otimes w_{\mathbf j^{\mathrm R}}(viL​⊗wiR​)⋅σ=j∑​wt(i​σj​)vjL​⊗wjR​

defines Ψr,sm,n:Br,s(δ)→End⁡g(V⊗r⊗W⊗s)op\Psi^{m,n}_{r,s} : B_{r,s}(\delta) \to \operatorname{End}_{\mathfrak g}(V^{\otimes r} \otimes W^{\otimes s})^{\mathrm{op}}Ψr,sm,n​:Br,s​(δ)→Endg​(V⊗r⊗W⊗s)op (7.12). For s=0s = 0s=0 the permutation diagrams give ΦNm,n:CΣN→End⁡g(V⊗N)op\Phi^{m,n}_{N} : \mathbb C\Sigma_N \to \operatorname{End}_{\mathfrak g}(V^{\otimes N})^{\mathrm{op}}ΦNm,n​:CΣN​→Endg​(V⊗N)op (7.11).

Formalization targets

Goal: Theorem 7.8 (p. 56)

For all m,n,r,s≥0m, n, r, s \ge 0m,n,r,s≥0,

im⁡Ψr,sm,n=End⁡g(V⊗r⊗W⊗s),Ψr,sm,n injective  ⟺  r+s<(m+1)(n+1).\operatorname{im} \Psi^{m,n}_{r,s} = \operatorname{End}_{\mathfrak g}(V^{\otimes r} \otimes W^{\otimes s}), \qquad \Psi^{m,n}_{r,s} \text{ injective} \iff r + s < (m+1)(n+1).imΨr,sm,n​=Endg​(V⊗r⊗W⊗s),Ψr,sm,n​ injective⟺r+s<(m+1)(n+1).

Milestones, in attack order

  • Lemma 7.1: Ω=∑i,j(−1)∣j∣ei,j⊗ej,i\Omega = \sum_{i,j} (-1)^{|j|} e_{i,j} \otimes e_{j,i}Ω=∑i,j​(−1)∣j∣ei,j​⊗ej,i​ on M⊗NM \otimes NM⊗N, M,N∈{V,W}M, N \in \{V, W\}M,N∈{V,W}.
  • Lemma 7.3: (7.6) is a right CΣN\mathbb C\Sigma_NCΣN​-action on V⊗NV^{\otimes N}V⊗N; (a b)(a\ b)(a b) acts as Ωa,b\Omega_{a,b}Ωa,b​; the action lies in End⁡g\operatorname{End}_{\mathfrak g}Endg​.
  • Lemma 7.4: (7.7) is a right Br,s(δ)B_{r,s}(\delta)Br,s​(δ)-action, Ψ(τ)Ψ(σ)=δtΨ(π)\Psi(\tau)\Psi(\sigma) = \delta^t \Psi(\pi)Ψ(τ)Ψ(σ)=δtΨ(π); the signed transpositions act as Ωa,b\Omega_{a,b}Ωa,b​; the action lies in End⁡g\operatorname{End}_{\mathfrak g}Endg​.
  • (2.1)–(2.2): flipr,s\mathrm{flip}_{r,s}flipr,s​ is a bijection from Σr+s\Sigma_{r+s}Σr+s​ to the walled diagrams, so dim⁡Br,s(δ)=(r+s)!\dim B_{r,s}(\delta) = (r+s)!dimBr,s​(δ)=(r+s)!.
  • Theorem 7.5 (Sergeev, Berele–Regev): ΦNm,n\Phi^{m,n}_NΦNm,n​ maps onto End⁡g(V⊗N)\operatorname{End}_{\mathfrak g}(V^{\otimes N})Endg​(V⊗N), injectively iff N<(m+1)(n+1)N < (m+1)(n+1)N<(m+1)(n+1).
  • Lemma 7.6, as its instance (7.16): flipr,s:End⁡(V⊗(r+s))→End⁡(V⊗r⊗W⊗s)\mathrm{flip}_{r,s} : \operatorname{End}(V^{\otimes(r+s)}) \to \operatorname{End}(V^{\otimes r} \otimes W^{\otimes s})flipr,s​:End(V⊗(r+s))→End(V⊗r⊗W⊗s), f⊗g↦f⊗g∗f \otimes g \mapsto f \otimes g^*f⊗g↦f⊗g∗, is a g\mathfrak gg-isomorphism.
  • Lemma 7.7: flipr,s∘Φr+sm,n=Ψr,sm,n∘flipr,s\mathrm{flip}_{r,s} \circ \Phi^{m,n}_{r+s} = \Psi^{m,n}_{r,s} \circ \mathrm{flip}_{r,s}flipr,s​∘Φr+sm,n​=Ψr,sm,n​∘flipr,s​.

Significance

Theorem 7.8 identifies Br,s(m−n)/ker⁡Ψr,sm,nB_{r,s}(m-n)/\ker \Psi^{m,n}_{r,s}Br,s​(m−n)/kerΨr,sm,n​ with the full super-commutant of mixed tensor space. Brundan and Stroppel use this to compare Br,s(δ)B_{r,s}(\delta)Br,s​(δ) with a graded algebra built from Khovanov's arc algebra (Corollary 8.2, Theorem 8.10), which yields a grading on Br,s(δ)B_{r,s}(\delta)Br,s​(δ), its Koszulity for δ≠0\delta \neq 0δ=0, and descriptions of the indecomposable summands of V⊗r⊗W⊗sV^{\otimes r} \otimes W^{\otimes s}V⊗r⊗W⊗s. The injectivity range r+s<(m+1)(n+1)r + s < (m+1)(n+1)r+s<(m+1)(n+1) says exactly when the walled Brauer algebra is faithfully realized on tensor space.

All statements are proved in the literature; none has a machine-checked proof that we are aware of. A complete formalization would need classical and super Schur–Weyl duality (Theorem 7.5 is the deep input, proved in the paper only by citation), the weight calculus of diagrams, and the sign bookkeeping of Lemma 7.7, which the authors call tricky.

Difficulty

Surjectivity onto a commutant is a double-centralizer statement, and the obvious route through semisimplicity fails: for m,n>0m, n > 0m,n>0 the tensor space V⊗NV^{\otimes N}V⊗N is in general not semisimple as a g\mathfrak gg-supermodule. Theorem 7.5 instead rests on Berele and Regev's analysis of hook Young diagrams. Mixed tensor space adds a second obstacle: WWW enters with signs both in its g\mathfrak gg-action and in the dualities W⊗s≅(V⊗s)∗W^{\otimes s} \cong (V^{\otimes s})^*W⊗s≅(V⊗s)∗, and the reduction to V⊗(r+s)V^{\otimes(r+s)}V⊗(r+s) via flipr,s\mathrm{flip}_{r,s}flipr,s​ works only when every sign convention (crossings, bottom caps, the sign rule, the dual map) is matched exactly.

Formalization scope

  • Colours and positions are 0-based: colours are Fin (m + n), odd iff ≥m\ge m≥m. A tensor space is given by a slot pattern Fin N → Bool (true = VVV); operators are complex matrices indexed by Fin N → Fin (m + n), with column = input basis vector.
  • The g\mathfrak gg-action is the explicit iterated coproduct with Koszul signs; End⁡g\operatorname{End}_{\mathfrak g}Endg​ is the joint kernel of the action of all matrix units ea,be_{a,b}ea,b​ on End⁡\operatorname{End}End, with both the even and odd parts and the sign (−1)∣x∣∣f∣(-1)^{|x||f|}(−1)∣x∣∣f∣.
  • Diagrams are fixed-point-free involutions of Fin N ⊕ Fin N (Sum.inl = top), reusing the published WalledBrauer.Blocks.WalledDiagram, its composition comp and its loop count loops. Crossings are counted by interleaving of endpoints along the boundary, which is the crossing set of a reduced drawing; Lemma 7.2 (isotopy invariance) is thereby absorbed.
  • CΣN\mathbb C\Sigma_NCΣN​ and Br,s(δ)B_{r,s}(\delta)Br,s​(δ) enter as vector spaces with their diagram bases; surjectivity and injectivity of (7.11) and (7.12) are properties of these linear maps. δ=m−n∈C\delta = m - n \in \mathbb Cδ=m−n∈C.
  • flipr,s\mathrm{flip}_{r,s}flipr,s​ on endomorphisms is given in coordinates, derived from (7.13), (7.15) and (7.18).
  • No restriction m+n>0m + n > 0m+n>0 or r+s>0r + s > 0r+s>0 is made: for m=n=0m = n = 0m=n=0 and r+s>0r + s > 0r+s>0 the space is zero and Ψ\PsiΨ is not injective, as the criterion predicts.

The following would trivialize or falsify the statement and are ruled out: a commutant of glm⊕gln\mathfrak{gl}_m \oplus \mathfrak{gl}_nglm​⊕gln​ only, or one that drops the odd part or the signs; an unsigned slotwise action; a range statement with only one inclusion; an injectivity statement with only one direction. Not formalized: the paper's general Lemma 7.6 for arbitrary supermodules (no supermodule category in Mathlib), and everything involving K(δ)K(\delta)K(δ). Contributions of a reusable Lie-superalgebra tensor layer and of Berele–Regev's hook-partition theory are welcome.

Selected references

  • J. Brundan, C. Stroppel, Gradings on walled Brauer algebras and Khovanov's arc algebra, Adv. Math. 231 (2012); arXiv:1107.0999v1. https://arxiv.org/abs/1107.0999
  • A. Berele, A. Regev, Hook Young diagrams with applications to combinatorics and to representations of Lie superalgebras, Adv. Math. 64 (1987) 118–175. https://doi.org/10.1016/0001-8708(87)90007-7
  • A. N. Sergeev, The tensor algebra of the identity representation as a module over the Lie superalgebras gl(n,m) and Q(n), Math. USSR Sbornik 51 (1985) 419–427. https://doi.org/10.1070/SM1985v051n02ABEH002867
  • J. Comes, B. Wilson, Deligne's category Rep(GL_δ) and representations of general linear supergroups, Represent. Theory 16 (2012); arXiv:1108.0652. https://arxiv.org/abs/1108.0652
  • G. Benkart, M. Chakrabarti, T. Halverson, R. Leduc, C. Lee, J. Stroomer, Tensor product representations of general linear groups and their connections with Brauer algebras, J. Algebra 166 (1994) 529–567. https://doi.org/10.1006/jabr.1994.1166
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Convex OptimizationOperations ResearchOptimization+1·Captain: Shuze Chen

Robust Optimization XII: Finite-Horizon Robust Bellman RecursionTextbook

Decision making with uncertain transitions

A routing decision can have a known immediate cost while its consequences depend on uncertain weather. A controller observes the current state, chooses an action, and then faces a random next state. A policy optimized for one estimated transition model may perform poorly when those estimates change. Chapter 13 of Ben-Tal, El Ghaoui and Nemirovski, Robust Optimization studies this issue through finite-state control problems and illustrates it with aircraft routing. The mathematical target here is the finite-horizon theorem that evaluates and optimizes policies against admissible changes in transition probabilities.

The uncertainty model matters. Requiring nature to use one fixed transition matrix throughout the horizon couples its choices across time. Allowing each time, state and action to have its own admissible probability row gives a different problem. The latter is the setting of this mission and of the chapter's robust Bellman recursion. No assertion of exact solution of the stationary-uncertainty problem is included.

Finite states, actions, and independent uncertainty rows

Let the state space be a finite nonempty set XXX, and let the action space be a finite nonempty set AAA, available in every state. The decision times are T={0,…,N−1}T=\{0,\ldots,N-1\}T={0,…,N−1}, with terminal time NNN. A deterministic Markov policy uuu assigns an action ut(i)u_t(i)ut​(i) to every time ttt and state iii. The stage cost ct(i,a)c_t(i,a)ct​(i,a) and terminal cost cN(i)c_N(i)cN​(i) are real numbers; they need not be nonnegative. The initial state has a given probability distribution q0q_0q0​.

A transition row ptiap_{ti}^aptia​ gives the probabilities of the next state, conditional on time ttt, current state iii, and action aaa. For fixed policies, distributions evolve according to

qt+1(j)=∑i∈Xqt(i)ptiut(i)(j).q_{t+1}(j)=\sum_{i\in X}q_t(i)p_{ti}^{u_t(i)}(j).qt+1​(j)=i∈X∑​qt​(i)ptiut​(i)​(j).

The expected total cost is defined from these forward distributions:

CN(u,p)=∑t=0N−1∑i∈Xqt(i)ct(i,ut(i))+∑i∈XqN(i)cN(i).C_N(u,p)=\sum_{t=0}^{N-1}\sum_{i\in X}q_t(i)c_t(i,u_t(i))+\sum_{i\in X}q_N(i)c_N(i).CN​(u,p)=t=0∑N−1​i∈X∑​qt​(i)ct​(i,ut​(i))+i∈X∑​qN​(i)cN​(i).

For robust control, every row belongs to a nonempty closed set PtiaP_{ti}^aPtia​ in the probability simplex. Rectangular uncertainty means that nature's admissible policies are the entire product of these sets: choices at different times, states and actions are independent constraints. The sets themselves may depend on time and need not be convex. These are the standing assumptions of Sections 13.2–13.3 of the book.

Formalization targets

The first supporting target is Theorem 13.1.2. For a fixed controller and fixed transition rows, the expected cost equals the attained maximum of the linear program with terminal vector vN=cNv_N=c_NvN​=cN​ and inequalities

vt(i)≤ct(i,ut(i))+∑jptiut(i)(j)vt+1(j),v_t(i)\le c_t(i,u_t(i))+\sum_jp_{ti}^{u_t(i)}(j)v_{t+1}(j),vt​(i)≤ct​(i,ut​(i))+j∑​ptiut​(i)​(j)vt+1​(j),

whose objective is q0Tv0q_0^Tv_0q0T​v0​. The second target, Theorem 13.1.4, is the nominal Bellman theorem: the recursion that minimizes the corresponding one-step expression over actions gives the optimal remaining cost at every time and state, and greedy policies for its values are optimal.

The goal is the full Theorem 13.3.1. With vN=cNv_N=c_NvN​=cN​, define

vt(i)=min⁡a∈A[ct(i,a)+max⁡p∈Ptia∑jp(j)vt+1(j)].v_t(i)=\min_{a\in A}\left[c_t(i,a)+\max_{p\in P_{ti}^a}\sum_jp(j)v_{t+1}(j)\right].vt​(i)=a∈Amin​[ct​(i,a)+p∈Ptia​max​j∑​p(j)vt+1​(j)].

Then vt(i)v_t(i)vt​(i) is the minimum worst-case remaining expected cost starting at state iii at time ttt, and

min⁡umax⁡pCN(u,p)=q0Tv0.\min_u\max_p C_N(u,p)=q_0^Tv_0.umin​pmax​CN​(u,p)=q0T​v0​.

The target includes existence of controller policies choosing the displayed minimizing actions and nature policies choosing maximizing rows. Every such controller is optimal, and corresponding maximizing rows realize its worst cost. For any fixed controller uuu, the separate evaluation recursion

vNu=cN,vtu(i)=ct(i,ut(i))+max⁡p∈Ptiut(i)pTvt+1uv_N^u=c_N,\qquad v_t^u(i)=c_t(i,u_t(i))+\max_{p\in P_{ti}^{u_t(i)}}p^Tv_{t+1}^uvNu​=cN​,vtu​(i)=ct​(i,ut​(i))+p∈Ptiut​(i)​max​pTvt+1u​

must give its attained worst expected remaining cost, including the total value q0Tv0uq_0^Tv_0^uq0T​v0u​.

What the results establish

These statements connect three different objects: a forward stochastic evolution, optimization over complete policies, and backward value calculations. The robust theorem supplies both an optimal decision rule and an evaluation of uncertainty for a prescribed rule. Keeping the initial distribution arbitrary retains the distinction between statewise values and the value of the original control problem.

The results are established mathematics in the source; the work requested is their formal verification. A related proved robust-DP theorem uses time-independent uncertainty sets, nonnegative stage costs and a fixed initial state. This mission preserves the book's different data and attainment conclusions. Its local statements are open proof targets, not completed Lean proofs.

Difficulty

The central issue is relating the independent forward cost to the policy optimization and preserving all attainments. Choosing an individually favorable action does not by itself establish optimality over complete policies. Likewise, replacing a maximum by a real supremum leaves the existence of a maximizing nature policy unresolved. Closedness of the row sets and their probability constraints are substantive assumptions here. The fixed-policy and optimizing recursions must also be distinguished: nature's worst choices for an arbitrary controller need not be the rows selected from the optimal value function.

Formalization scope

States, actions and decision times use finite index types, with nonempty state and action spaces. All costs and probabilities are real. Probability vectors have nonnegative coordinates summing to one. The model retains arbitrary initial distributions, time-dependent uncertainty sets and terminal costs. A zero horizon has no decisions and yields terminal expected cost.

The definition bundle includes forward distributions, expected costs, both Bellman recursions, the independent worst-cost function, and the policy-selection predicates. The theorems compare these independently defined quantities, rather than defining expected cost to be the desired Bellman value. Extrema use attained order predicates, with internal suprema restricted to the admissible nature policies. Full-horizon policies encode suffix policies by ignoring coordinates before the starting time.

Formalization Note Each theorem carries its needed concrete definitions in a separate namespace so it compiles without importing unpublished drafts. The definition item records the common reusable interface. Equation (13.1.3) supplies the forward-distribution definition rather than a tautological milestone. The nominal LP Theorem 13.1.3 is not a dependency in this selected route; its printed index and arbitrary-optimizer issues are recorded locally. No corrected or strengthened variant is posed.

Selected references

  • A. Ben-Tal, L. El Ghaoui and A. Nemirovski, Robust Optimization, Princeton University Press, 2009, Chapter 13, especially Theorems 13.1.2, 13.1.4 and 13.3.1, printed pp. 345–346 and 350. DOI.
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Linear algebraMathematical PhysicsQuantum Information·Captain: mikedeng1

Quantum computation, quantum state engineering, and quantum phase transitions driven by dissipation: The DQC Liouvillian Has a Unique Steady State Encoding the Circuit and a Gap Above 1/T²Research Paper

Motivation

A quantum circuit normally applies a sequence of gates to a prepared state. Verstraete, Wolf and Cirac proposed a different physical route: couple a quantum system to a memoryless environment so that dissipation drives it toward a state recording the circuit's computation. Their dissipative quantum computation construction places a clock beside the computational qubits and makes the circuit history a stationary state of a time independent master equation. A useful process must have a well identified stationary state and a rate of relaxation that does not collapse with the number of qubits or with the chosen gates. The paper argues for these properties in its DQC section and its efficiency appendix (Verstraete, Wolf and Cirac, 2008, pp. 1–2, 4–5).

The printed spectral gap formula and part of its supporting clock block do not describe the slowest decay of the stated generator. Direct finite dimensional calculations reveal a slower coherence sector. This mission therefore targets the stated stationary state and a corrected, explicitly ranged version of the paper's lower bound. The discrepancies and boundary cases are recorded in the formalization scope so that the target is a mathematical claim about the displayed Lindblad operators rather than an unchecked transcription.

Setting

Fix N≥0N\geq 0N≥0 qubits and T≥0T\geq 0T≥0 circuit steps. A computational basis string is a function from the NNN qubit positions to {0,1}\{0,1\}{0,1}. The clock register has basis ∣t⟩|t\rangle∣t⟩ for t=0,…,Tt=0,\ldots,Tt=0,…,T. A family of unitary gates U1,…,UTU_1,\ldots,U_TU1​,…,UT​ acts on the qubit register. Its history vectors are ∣ψ0⟩=∣0⋯0⟩|\psi_0\rangle=|0\cdots0\rangle∣ψ0​⟩=∣0⋯0⟩ and ∣ψt⟩=Ut⋯U1∣0⋯0⟩|\psi_t\rangle=U_t\cdots U_1|0\cdots0\rangle∣ψt​⟩=Ut​⋯U1​∣0⋯0⟩.

A jump operator resets qubit iii only when the clock is at zero: Li=∣0⟩i⟨1∣⊗∣0⟩⟨0∣L_i=|0\rangle_i\langle1|\otimes|0\rangle\langle0|Li​=∣0⟩i​⟨1∣⊗∣0⟩⟨0∣. For each neighboring clock pair, another jump operator moves in both directions, applying the relevant gate on the forward move and its adjoint on the reverse move. The Lindblad generator is the linear map on matrices

L(ρ)=∑k(LkρLk†−12(Lk†Lkρ+ρLk†Lk)).\mathcal L(\rho)=\sum_k\left(L_k\rho L_k^\dagger-\frac12(L_k^\dagger L_k\rho+\rho L_k^\dagger L_k)\right).L(ρ)=k∑​(Lk​ρLk†​−21​(Lk†​Lk​ρ+ρLk†​Lk​)).

There is no Hamiltonian term. The proposed history state is the normalized density matrix

ρ0=1T+1∑t=0T∣ψt⟩⟨ψt∣⊗∣t⟩⟨t∣.\rho_0=\frac1{T+1}\sum_{t=0}^{T}|\psi_t\rangle\langle\psi_t|\otimes|t\rangle\langle t|.ρ0​=T+11​t=0∑T​∣ψt​⟩⟨ψt​∣⊗∣t⟩⟨t∣.

These are equations (1)–(4) of the paper, with the clock step index repaired as described below. The appendix introduces a gate removal unitary WWW, a connected clock path matrix L00L_{00}L00​, and clock blocks with a penalty at time zero. Their spectra lead to the uniqueness and decay claims (paper, pp. 2, 4–5).

Formalization targets

Main goal

For every N≥0N\geq0N≥0, T≥2T\geq2T≥2, and family of unitary gates, prove that L(ρ0)=0\mathcal L(\rho_0)=0L(ρ0​)=0, that ρ0\rho_0ρ0​ is positive semidefinite with trace one, and that the full kernel of L\mathcal LL consists of scalar multiples of ρ0\rho_0ρ0​. For T≥5T\geq5T≥5, prove additionally that every nonzero eigenvalue μ\muμ satisfies

Re⁡(μ)<−1T2.\operatorname{Re}(\mu)<-\frac1{T^2}.Re(μ)<−T21​.

The bound applies uniformly across the number of qubits and the circuit gates. It is the corrected form of the efficiency conclusion on p. 5. The goal does not assert the printed formula Δ=π2/(2T+3)2\Delta=\pi^2/(2T+3)^2Δ=π2/(2T+3)2, which is contradicted by the slowest coherence sector (paper, pp. 2, 5).

Supporting targets

The milestones first establish stationarity and removal of the circuit gates by WWW. They then target the one dimensional fixed space for identity gates, the first nonzero eigenvalue of the connected clock path, the penalized clock blocks, and the full generator's bound for identity gates. This follows the sequence of reductions described in the efficiency appendix while retaining the paper's exact clock constants where they are valid (paper, pp. 4–5).

Significance

The kernel statement identifies every stationary matrix, a stronger assertion than merely finding one stationary density matrix. The eigenvalue bound supplies a uniform spectral scale for the finite dimensional generator, independent of the circuit content. Together these make precise the part of dissipative computation that says the intended history is singled out and spectrally separated from other modes. A convergence time theorem would also have to control Jordan blocks or the operator semigroup and is outside this target; the paper itself notes this separate issue on p. 5 (paper, p. 5).

Formalizing the corrected claim creates a reusable finite matrix representation of a Lindblad generator and a circuit clock, plus independently usable path and boundary penalty spectral statements. The paper result is known in physics prose; these exact Lean statements are open proof goals in this proposal. The correction also prevents later arguments from importing a spectral equality that does not hold for the displayed process.

Difficulty

The gate operators couple the qubit register to the clock, so diagonalizing a clock matrix alone does not describe the generator. Even after the gates are removed, the Liouvillian acts on matrices, including coherences between two qubit states and two clock times. The decay of a one sided coherence at clock zero carries half the penalty of a population term. Reading every nonzero sector as if it had the population penalty produces the printed gap value and misses the slowest mode. The clock path also has to retain the first edge and its endpoint diagonal entries; omitting that edge changes the spectrum.

Formalization scope

Lean uses matrices indexed by NNN bit strings paired with the finite clock {0,…,T}\{0,\ldots,T\}{0,…,T}, and a complex linear endomorphism on those matrices. Gates are quantified as unitary matrices; they may act on all qubits, whereas the paper starts with nearest neighbor gates. The appendix's spectral argument is independent of that locality, so this is a disclosed generalization. The model also permits N=0N=0N=0. Gates use zero based indexing: Lean's U(t)U(t)U(t) is the paper's Ut+1U_{t+1}Ut+1​ and acts on the step t→t+1t\to t+1t→t+1. This repairs equation (3), which otherwise calls for both an undefined U0U_0U0​ and an out of range clock state ∣T+1⟩|T+1\rangle∣T+1⟩.

Uniqueness is restricted to T≥2T\geq2T≥2: at T=1T=1T=1 an additional clock coherence is stationary. The strict 1/T21/T^21/T2 bound is restricted to T≥5T\geq5T≥5: direct diagonalization shows it fails for T=1,2,3,4T=1,2,3,4T=1,2,3,4. The paper's printed corner coefficient −2-2−2 is correct for a population sector, but a one sided coherence has coefficient −3/2-3/2−3/2. A milestone states the valid printed matrix fact and the corrected bound for all clock zero penalties a≥1/2a\geq1/2a≥1/2. The connected path matrix follows the displayed spectral formula rather than the printed tridiagonal sum whose range omits the first edge.

The generator is defined from the jump operators by equation (1). It is not defined from the desired block decomposition or eigenvalues. The spectral assertion quantifies over actual nonzero complex eigenvalues and compares their real parts directly; no default valued infimum defines a gap. Work toward the mission may supply matrix identities, unitary covariance, tridiagonal spectra, or a direct finite dimensional analysis of the generator. The generic finite matrix Lindblad definition can be reused independently of this circuit model.

Selected references

  • Frank Verstraete, Michael M. Wolf, and J. Ignacio Cirac, Quantum computation, quantum state engineering, and quantum phase transitions driven by dissipation, arXiv:0803.1447v2, 2008; later Nature Physics 5, 633–636 (2009). Pinned preprint.
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Differential GeometryTopology·Captain: mikedeng1

A Generalisation of Steenrod's Approximation Theorem: Smoothing a Continuous Section of a Smooth Bundle with Normed-Modelled Fibre near L, Fixed off U, by a Vertical Homotopy Within Any NeighbourhoodResearch Paper

Motivation

Many constructions in differential topology and infinite-dimensional Lie theory start from a continuous object and need a smooth one: a continuous section of a smooth bundle, a continuous map into a manifold, a continuous homotopy between smooth maps. Steenrod's approximation theorem (Steenrod 1951, §6.7) says that, for finite-dimensional bundles, a continuous section can be smoothed by a small homotopy through sections, without changing it where it is already smooth. Hirsch's textbook (Hirsch 1976, Ch. 2) gives the relative version for maps between finite-dimensional manifolds.

Gauge theory and the study of principal bundles whose structure group is an infinite-dimensional Lie group (current groups, diffeomorphism groups, gauge groups) need the same statement when the typical fibre is infinite-dimensional. C. Wockel (arXiv:math/0610252, 2006) proves it for a finite-dimensional base with corners and a fibre that is a manifold modelled on a locally convex space, combining Steenrod's argument with Neeb's approximation results for maps into locally convex spaces (Neeb 2002, App. A.3). The consequences in the paper are that smooth and continuous homotopy classes of sections, and of maps from a finite-dimensional manifold into a locally convex manifold, coincide; this is used in bundle theory for infinite-dimensional structure groups (Müller–Wockel 2006, cited as [MW06] in the paper).

Setting

A manifold with corners MMM is a Hausdorff paracompact space with charts onto open subsets of the quadrant R+d={x∈Rd:xi≥0}\mathbb R^d_+ = \{x \in \mathbb R^d : x_i \ge 0\}R+d​={x∈Rd:xi​≥0} and smooth coordinate changes. A locally convex manifold NNN is a Hausdorff space with charts onto open subsets of a locally convex space and smooth coordinate changes, where smoothness of f:U→Yf : U \to Yf:U→Y means that all iterated directional derivatives exist and are continuous (Definition 0.1 of the paper).

A map π:E→M\pi : E \to Mπ:E→M is a locally trivial smooth bundle with typical fibre NNN if every point of MMM has an open neighbourhood SSS and a diffeomorphism φ:π−1(S)→S×N\varphi : \pi^{-1}(S) \to S \times Nφ:π−1(S)→S×N with pr1∘φ=π\mathrm{pr}_1 \circ \varphi = \pipr1​∘φ=π. A section is a continuous map σ:M→E\sigma : M \to Eσ:M→E with π∘σ=idM\pi \circ \sigma = \mathrm{id}_Mπ∘σ=idM​. A map is smooth on a neighbourhood of a set sss if it is smooth on some open set containing sss.

For spaces X,YX, YX,Y, C(X,Y)c.o.C(X, Y)_{c.o.}C(X,Y)c.o.​ is the space of continuous maps with the compact-open topology, generated by the sets ⌊C,W⌋={f:f(C)⊆W}\lfloor C, W\rfloor = \{f : f(C) \subseteq W\}⌊C,W⌋={f:f(C)⊆W} with CCC compact and WWW open.

Formalization targets

Goal: Theorem 0.11 (Generalised Steenrod Approximation Theorem)

Let MMM be finite-dimensional and connected, π:E→M\pi : E \to Mπ:E→M a locally trivial smooth bundle with typical fibre NNN, σ\sigmaσ a continuous section, L⊆ML \subseteq ML⊆M closed, U⊆MU \subseteq MU⊆M open, and σ\sigmaσ smooth on a neighbourhood of L∖UL \setminus UL∖U. Then for every open O⊇σ(M)O \supseteq \sigma(M)O⊇σ(M) there are a section τ\tauτ and a homotopy HHH with

τ(M)⊆O,τ smooth on a neighbourhood of L,τ∣M∖U=σ∣M∖U,\tau(M) \subseteq O,\quad \tau \text{ smooth on a neighbourhood of } L,\quad \tau|_{M \setminus U} = \sigma|_{M \setminus U},τ(M)⊆O,τ smooth on a neighbourhood of L,τ∣M∖U​=σ∣M∖U​, H:[0,1]×M→O,H(0,⋅)=σ, H(1,⋅)=τ,π∘H(t,⋅)=idM,H(t,x)=σ(x) for x∉U.H : [0,1] \times M \to O,\quad H(0,\cdot) = \sigma,\ H(1, \cdot) = \tau,\quad \pi \circ H(t, \cdot) = \mathrm{id}_M,\quad H(t,x) = \sigma(x) \text{ for } x \notin U.H:[0,1]×M→O,H(0,⋅)=σ, H(1,⋅)=τ,π∘H(t,⋅)=idM​,H(t,x)=σ(x) for x∈/U.

Milestones

  1. Remark 0.4: a connected paracompact finite-dimensional manifold with corners is σ-compact.
  2. Proposition 0.7: C∞(M,Y)C^\infty(M, Y)C∞(M,Y) is dense in C(M,Y)c.o.C(M, Y)_{c.o.}C(M,Y)c.o.​, with support control for compactly supported maps.
  3. Corollary 0.8: C∞(M,V)C^\infty(M, V)C∞(M,V) is dense in C(M,V)c.o.C(M, V)_{c.o.}C(M,V)c.o.​ for V⊆YV \subseteq YV⊆Y open.
  4. Lemma 0.9: relative smoothing of f:M→Wf : M \to Wf:M→W, W⊆YW \subseteq YW⊆Y open convex, within any compact-open neighbourhood, keeping fff off UUU.
  5. Lemma 0.10: the same for maps into a subset W⊆NW \subseteq NW⊆N diffeomorphic to an open convex subset of the model space.
  6. Sections versus fibre maps (proof of Theorem 0.11, p. 5): over a smooth trivialisation φ\varphiφ, a section σ′\sigma'σ′ is smooth near xxx if and only if pr2∘φ∘σ′\mathrm{pr}_2 \circ \varphi \circ \sigma'pr2​∘φ∘σ′ is.

Significance

The result. The theorem turns continuous sections into smooth ones by homotopies that are small (they stay in any prescribed open set OOO around the section) and relative (fixed where nothing needs changing). It yields that C∞(M,N)C^\infty(M, N)C∞(M,N) is dense in C(M,N)C(M, N)C(M,N) for the graph and compact-open topologies (Corollary 0.12), that every continuous section is homotopic to a smooth one and continuously homotopic smooth sections are smoothly homotopic (Proposition 0.13), and that smooth and continuous homotopy classes [M,N][M, N][M,N] agree (Corollary 0.14). These are the statements needed to compare smooth and topological classification of bundles with infinite-dimensional structure groups.

Formalizing it. The theorem is proved in the paper; no machine-checked version exists. Mathlib has smooth partitions of unity on finite-dimensional manifolds with corners and local-to-global smoothing for maps into convex sets, but no density of C∞(M,Y)C^\infty(M, Y)C∞(M,Y) in C(M,Y)C(M, Y)C(M,Y) for the compact-open topology, no relative smoothing lemma, and no smoothing of sections of non-vector bundles. A formalization would supply these as reusable statements about Mathlib's ContMDiff, Bundle.Trivialization and C(M, Y).

Difficulty

The obvious argument glues local smoothings with a partition of unity, as for real-valued functions. This fails for sections of a non-linear bundle: convex combinations of points of EEE, or of NNN, are meaningless, so a partition-of-unity average of local smoothings is not a section, and the smoothing cannot be done in one global step. Any stepwise replacement must keep the section inside the prescribed open set OOO, must not destroy smoothness already achieved near earlier parts of LLL, and must avoid convergence arguments, since infinitely many steps are needed on a non-compact MMM. The homotopy has to be continuous at the end where infinitely many steps accumulate. Finally, an infinite-dimensional NNN is not locally compact, so all compactness must come from MMM; this is why the base is finite-dimensional while the fibre is not.

Formalization scope

  • Normed models. Mathlib's manifolds require a normed model space, so NNN is modelled (without boundary) on a real normed space FFF, not necessarily complete or finite-dimensional, and the total space EEE is a manifold with corners modelled on a real normed space; in Proposition 0.7, Corollary 0.8 and Lemma 0.9 the target YYY is a real normed space. On normed spaces the paper's smoothness coincides with Fréchet C∞C^\inftyC∞, Mathlib's ContMDiff … ∞ (not the analytic ω). This is the one specialisation of the paper; non-normable locally convex fibres are out of scope.
  • The base. MMM carries any finite-dimensional Mathlib model with corners III (which contains the quadrant R+d\mathbb R^d_+R+d​), with [T2Space M], and [ParacompactSpace M] (Theorem 0.11, Remark 0.4, milestone 6) or [SigmaCompactSpace M] (Proposition 0.7, Corollary 0.8, Lemmas 0.9, 0.10), as Definition 0.3 and the statements require; Theorem 0.11 adds [ConnectedSpace M]. NNN is [T2Space N].
  • Conventions. "Smooth on a neighbourhood of sss" is C∞C^\inftyC∞ on an open set containing sss (SmoothNear), not smoothness on sss itself. Spaces C(M,W)C(M, W)C(M,W) for W⊆YW \subseteq YW⊆Y or W⊆NW \subseteq NW⊆N are maps into the subtype with the compact-open topology, so neighbourhoods are taken in C(M,W)C(M, W)C(M,W). A bundle is given by smooth Bundle.Trivializations covering MMM; "WWW diffeomorphic to an open convex subset of FFF" is a partial diffeomorphism N→FN \to FN→F with source WWW and convex target. The homotopy is indexed by unitInterval and runs from σ\sigmaσ at 000 to τ\tauτ at 111. "Support" is the closed support tsupport.
  • No trivial reading. The goal must not be read with smoothness on LLL only (which is weaker for closed LLL), with OOO replaced by all of EEE, or with a trivial bundle or finite-dimensional fibre; a sanity file checks that the hypotheses are satisfiable on the product bundle R×R→R\mathbb R \times \mathbb R \to \mathbb RR×R→R.
  • What a development needs. Smooth partitions of unity on MMM (in Mathlib), local compactness and σ-compactness of MMM, the compact-open topology on C(M,W)C(M, W)C(M,W) and continuity of the operations γ↦λγ+(1−λ)f\gamma \mapsto \lambda\gamma + (1-\lambda)fγ↦λγ+(1−λ)f on it, and the gluing of sections along locally finite covers. Proofs of Proposition 0.7 and Lemma 0.9 are reusable beyond this mission; contributions proving any milestone, or the Mathlib-level density results, are welcome.

Selected references

  • C. Wockel, A Generalisation of Steenrod's Approximation Theorem, preprint arXiv:math/0610252v1, 2006. https://arxiv.org/abs/math/0610252
  • N. Steenrod, The Topology of Fibre Bundles, Princeton University Press, 1951, §6.7. https://doi.org/10.1515/9781400883875
  • M. W. Hirsch, Differential Topology, Graduate Texts in Mathematics 33, Springer, 1976, Ch. 2. https://doi.org/10.1007/978-1-4684-9449-5
  • K.-H. Neeb, Central extensions of infinite-dimensional Lie groups, Ann. Inst. Fourier 52 (2002), App. A.3 (cited as [Ne02]).
  • C. Müller, C. Wockel, Equivalences of smooth and continuous principal bundles with infinite-dimensional structure group, preprint, 2006 (cited as [MW06]).
  • J. Dugundji, Topology, Allyn and Bacon, 1966, Theorems XI.7.2–3.
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AlgebraCombinatoricsRepresentation Theory·Captain: mikedeng1

Rational Semistandard Tableaux and Character Formula for the Lie Superalgebra ĝl∞|∞: A Jacobi–Trudi Determinant Formula for the Characters of A/B-Semistandard TableauxResearch Paper

Motivation

The Lie superalgebra gl^∞∣∞\widehat{\mathfrak{gl}}_{\infty|\infty}gl​∞∣∞​, a central extension of the Lie superalgebra of infinite matrices of finite support, appears in the representation theory of the W1+∞W_{1+\infty}W1+∞​ vertex algebra and in Howe-type dualities with gln\mathfrak{gl}_ngln​ (Kac–Radul; Cheng–Lam). Its irreducible quasi-finite highest weight modules of positive integral level nnn are indexed by generalized partitions λ=(λ1≥⋯≥λn)∈Zn\lambda=(\lambda_1\ge\cdots\ge\lambda_n)\in\mathbb Z^nλ=(λ1​≥⋯≥λn​)∈Zn, and their characters had been computed by Cheng and Lam in terms of hook Schur functions and Littlewood–Richardson coefficients.

J.-H. Kwon (arXiv:math/0605005) gave these characters a tableau model. He introduced A/B-semistandard tableaux, pairs of super-semistandard tableaux attached to a generalized partition, showed that their generating function SλA/BS^{\mathcal A/\mathcal B}_\lambdaSλA/B​ is the character in question (Theorem 5.2), and developed an insertion scheme that yields an RSK correspondence, a Littlewood–Richardson rule, and a Jacobi–Trudi type determinant formula (Theorem 4.5). The paper notes that this determinant formula for the characters of gl^∞∣∞\widehat{\mathfrak{gl}}_{\infty|\infty}gl​∞∣∞​-modules had not been observed before. The combinatorics rests on Stembridge's rational semistandard tableaux (1987), which model the rational representations of gln\mathfrak{gl}_ngln​, and on Berele–Regev's hook Schur functions (1987).

Setting

Let A\mathcal AA and B\mathcal BB be linearly ordered, at most countable sets, each split into even and odd letters, A=A0⊔A1\mathcal A=\mathcal A_0\sqcup\mathcal A_1A=A0​⊔A1​.

A filling TTT of a skew Young diagram with letters of A\mathcal AA is A\mathcal AA-semistandard if its entries weakly increase along rows and down columns, even letters strictly increase down columns, and odd letters strictly increase along rows. The weight of TTT records how many times each letter occurs, and xAT=∏axamax^T_{\mathcal A}=\prod_a x_a^{m_a}xAT​=∏a​xama​​.

A generalized partition of level n≥1n\ge1n≥1 is λ∈Z+n={λ1≥⋯≥λn}\lambda\in\mathbb Z^n_+=\{\lambda_1\ge\cdots\ge\lambda_n\}λ∈Z+n​={λ1​≥⋯≥λn​}. It is drawn against a vertical line: row kkk has λk\lambda_kλk​ boxes to the right of the line if λk≥0\lambda_k\ge0λk​≥0 and ∣λk∣|\lambda_k|∣λk​∣ boxes to the left if λk<0\lambda_k<0λk​<0.

An A/B-semistandard tableau of shape λ\lambdaλ is a pair (T+,T−)(T^+,T^-)(T+,T−) with T+∈SSTA((λ+(dn))/μ)T^+\in SST_{\mathcal A}((\lambda+(d^n))/\mu)T+∈SSTA​((λ+(dn))/μ) and T−∈SSTB((dn)/μ)T^-\in SST_{\mathcal B}((d^n)/\mu)T−∈SSTB​((dn)/μ) for some d≥0d\ge0d≥0 and partition μ⊂(dn)\mu\subset(d^n)μ⊂(dn), μ⊂λ+(dn)\mu\subset\lambda+(d^n)μ⊂λ+(dn). Both tableaux are drawn against the line of λ\lambdaλ, so enlarging ddd by one and μ\muμ by a full column gives the same pair. The character is

SλA/B=∑(T+,T−)∈SSTA/B(λ)xAT+(xBT−)−1∈Z[[xA,xB−1]],S^{\mathcal A/\mathcal B}_\lambda=\sum_{(T^+,T^-)\in SST_{\mathcal A/\mathcal B}(\lambda)}x^{T^+}_{\mathcal A}\big(x^{T^-}_{\mathcal B}\big)^{-1}\in\mathbb Z[[x_{\mathcal A},x_{\mathcal B}^{-1}]],SλA/B​=(T+,T−)∈SSTA/B​(λ)∑​xAT+​(xBT−​)−1∈Z[[xA​,xB−1​]],

a power series in the symbols xax_axa​ and xb−1x_b^{-1}xb−1​. At level one, SkA/BS^{\mathcal A/\mathcal B}_kSkA/B​ is defined for every k∈Zk\in\mathbb Zk∈Z, negative kkk included.

A rational [n][n][n]-semistandard tableau of shape λ\lambdaλ fills the diagram of λ\lambdaλ with 1,…,n1,\dots,n1,…,n right of the line and −n,…,−1-n,\dots,-1−n,…,−1 left of it, rows weakly and columns strictly increasing, subject to Stembridge's compatibility condition between columns 111 and −1-1−1. Its content ν\nuν has νk=mk−m−k\nu_k=m_k-m_{-k}νk​=mk​−m−k​, and KλμK_{\lambda\mu}Kλμ​ counts the tableaux of shape λ\lambdaλ and content μ\muμ.

Formalization targets

Goal: Theorem 4.5

For infinite A\mathcal AA, B\mathcal BB and every λ∈Z+n\lambda\in\mathbb Z^n_+λ∈Z+n​, n≥1n\ge1n≥1,

SλA/B=det⁡(Sλi−i+jA/B)1≤i,j≤n.S^{\mathcal A/\mathcal B}_\lambda=\det\Big(S^{\mathcal A/\mathcal B}_{\lambda_i-i+j}\Big)_{1\le i,j\le n}.SλA/B​=det(Sλi​−i+jA/B​)1≤i,j≤n​.

The entries are level-one A/B-characters, not complete symmetric functions. Unlike hkh_khk​, they do not vanish for k<0k<0k<0.

Milestones

  1. Each coefficient of (3.14) counts finitely many tableaux.
  2. Lemma 3.3: the map σ:SST[n](λ)→SST[n](λ+(1n))\sigma: SST_{[n]}(\lambda)\to SST_{[n]}(\lambda+(1^n))σ:SST[n]​(λ)→SST[n]​(λ+(1n)) is a bijection; it shifts content by (1n)(1^n)(1n).
  3. (4.3): Kλμ=Kλ+(dn) μ+(dn)K_{\lambda\mu}=K_{\lambda+(d^n)\,\mu+(d^n)}Kλμ​=Kλ+(dn)μ+(dn)​, and Kλμ=0K_{\lambda\mu}=0Kλμ​=0 unless λ≥μ\lambda\ge\muλ≥μ lexicographically.
  4. Corollary 4.4: a weight-preserving bijection ∏iSSTA/B(νi)≅⨆μSSTA/B(μ)×SST[n](μ)ν\prod_i SST_{\mathcal A/\mathcal B}(\nu_i)\cong\bigsqcup_\mu SST_{\mathcal A/\mathcal B}(\mu)\times SST_{[n]}(\mu)_\nu∏i​SSTA/B​(νi​)≅⨆μ​SSTA/B​(μ)×SST[n]​(μ)ν​.
  5. The expansion HμA/B=∏iSμiA/B=∑⟨λ⟩=⟨μ⟩KλμSλA/BH^{\mathcal A/\mathcal B}_\mu=\prod_i S^{\mathcal A/\mathcal B}_{\mu_i}=\sum_{\langle\lambda\rangle=\langle\mu\rangle}K_{\lambda\mu}S^{\mathcal A/\mathcal B}_\lambdaHμA/B​=∏i​Sμi​A/B​=∑⟨λ⟩=⟨μ⟩​Kλμ​SλA/B​ (proof of Theorem 4.5).
  6. (4.5): hμ=∑λ≥μKλμsλh_\mu=\sum_{\lambda\ge\mu}K_{\lambda\mu}s_\lambdahμ​=∑λ≥μ​Kλμ​sλ​ and sλ=det⁡(hλi−i+j)s_\lambda=\det(h_{\lambda_i-i+j})sλ​=det(hλi​−i+j​) in nnn variables.
  7. Lemma 3.17: the SλAS^{\mathcal A}_\lambdaSλA​, λ∈PA\lambda\in\mathscr P_{\mathcal A}λ∈PA​, are linearly independent.
  8. Remark 3.19: infinite combinations of Sλ(xA)Sμ(xB−1)S_\lambda(x_{\mathcal A})S_\mu(x_{\mathcal B}^{-1})Sλ​(xA​)Sμ​(xB−1​) converge and have unique coefficients.
  9. Proposition 3.20: Sλ(xA,xB)=∑μ,ν∈Pncμν∗λSμ(xA)Sν(xB−1)S_\lambda(x_{\mathcal A},x_{\mathcal B})=\sum_{\mu,\nu\in\mathscr P_n}c^\lambda_{\mu\nu^*}S_\mu(x_{\mathcal A})S_\nu(x_{\mathcal B}^{-1})Sλ​(xA​,xB​)=∑μ,ν∈Pn​​cμν∗λ​Sμ​(xA​)Sν​(xB−1​).
  10. Corollary 3.23: infinite combinations ∑λaλSλA/B\sum_\lambda a_\lambda S^{\mathcal A/\mathcal B}_\lambda∑λ​aλ​SλA/B​ at a fixed level converge and have unique coefficients.

Significance

The result. Theorem 4.5 is the super, rational analogue of the Jacobi–Trudi identity. Through Theorem 5.2 it becomes a determinant formula for the characters of the irreducible quasi-finite gl^∞∣∞\widehat{\mathfrak{gl}}_{\infty|\infty}gl​∞∣∞​-modules of positive level (Corollary 5.4). Specialising A\mathcal AA and B\mathcal BB recovers formulas for gl^∞\widehat{\mathfrak{gl}}_\inftygl​∞​ and for the (glp∣q,gln)(\mathfrak{gl}_{p|q},\mathfrak{gl}_n)(glp∣q​,gln​) Howe duality. Milestones 2–6 develop the rational Kostka theory along the way: its shift invariance, its triangularity, and its role in an RSK correspondence for A/B-tableaux.

Formalizing it. The theorem is proved in the paper; nothing in it has a machine-checked proof. Mathlib has semistandard Young tableaux and symmetric polynomials, but no Schur polynomials as tableau generating functions, no Kostka numbers, no RSK, and no classical Jacobi–Trudi identity. Milestone 6 is therefore new to formal mathematics in its own right, and it is a prerequisite for the goal's proof.

Difficulty

The obvious attack proves the classical Jacobi–Trudi identity once and then transfers it. That fails here for two reasons. The entries SkA/BS^{\mathcal A/\mathcal B}_kSkA/B​ with k<0k<0k<0 are nonzero, so the classical vanishing hk=0h_k=0hk​=0 that truncates the determinant is unavailable. And the expansion HμA/B=∑KλμSλA/BH^{\mathcal A/\mathcal B}_\mu=\sum K_{\lambda\mu}S^{\mathcal A/\mathcal B}_\lambdaHμA/B​=∑Kλμ​SλA/B​ is an infinite sum over generalized partitions, so the comparison with (4.5) leaves an error term supported on Z+n∖Pn\mathbb Z^n_+\setminus\mathscr P_nZ+n​∖Pn​. Killing it requires both the shift invariance of the rational Kostka numbers and the uniqueness of coefficients in infinite combinations (Corollary 3.23). The combinatorial input, Corollary 4.4, is a weight-preserving insertion bijection for pairs of super tableaux, built from row and column insertion, rectangular complements and Stroomer's theorem. Each of these is substantial to formalize.

Formalization scope

  • Namespace and definitions. Everything is in SuperTableaux.JacobiTrudi, with one definitions item.
  • Letters and grading. Letters are types with LinearOrder and Countable; the grading is a function odd : A → Bool, where true means odd.
  • Characters. Characters live in MvPowerSeries (A ⊕ B) ℤ. The variable Sum.inl a is xax_axa​ and Sum.inr b is the symbol xb−1x_b^{-1}xb−1​, which is literally the ring Z[[xA,xB−1]]\mathbb Z[[x_{\mathcal A},x_{\mathcal B}^{-1}]]Z[[xA​,xB−1​]]. The coefficient at a monomial is Nat.card of the set of tableaux of that weight; milestone 1 proves that set finite.
  • Cut coordinates. A/B-tableaux are stored in cut coordinates: the class of (d,μ)(d,\mu)(d,μ) is the antitone vector c=μ−(dn)c=\mu-(d^n)c=μ−(dn), so each pair of tableaux is counted once.
  • Rows and order. Rows are 000-based. The order on Z+n\mathbb Z^n_+Z+n​ is Mathlib's lexicographic order toLex, which is the paper's "reverse lexicographic ordering" of p. 23.
  • Infinite sums. These are HasSum/Summable in the coefficientwise topology, never tsum.
  • Bijections. Lemma 3.3 is stated for the paper's map σ\sigmaσ, written out as a definition; it also records the content shift of p. 23. Corollary 4.4 asserts a bijection preserving the A/B-weight (the weight clause of Corollary 4.3); the insertion map κA/B\kappa_{\mathcal A/\mathcal B}κA/B​ itself is not written out.

A formalization that defines SλA/BS^{\mathcal A/\mathcal B}_\lambdaSλA/B​ by a determinant or product formula, sums over (d,μ)(d,\mu)(d,μ) without the identification (every coefficient becomes Nat.card of an infinite set, i.e. 000), or drops the parity conditions trivializes the goal; the definitions here are the tableau generating functions of (3.13)–(3.14).

A complete development needs Kostka numbers, Schur polynomials as tableau generating functions, the classical Jacobi–Trudi identity, RSK for super tableaux, and coefficientwise convergence in multivariate power series. All of these are reusable beyond this mission. Contributions are welcome on any milestone, and on intermediate lemmas such as the classical Jacobi–Trudi identity.

Selected references

  • J.-H. Kwon, Rational semistandard tableaux and character formula for the Lie superalgebra gl^∞∣∞\widehat{\mathfrak{gl}}_{\infty|\infty}gl​∞∣∞​, preprint, 2006. https://arxiv.org/abs/math/0605005
  • J. R. Stembridge, Rational tableaux and the tensor algebra of gln\mathfrak{gl}_ngln​, J. Combin. Theory Ser. A 46 (1987) 79–120. https://doi.org/10.1016/0097-3165(87)90077-X
  • A. Berele, A. Regev, Hook Young diagrams with applications to combinatorics and to representations of Lie superalgebras, Adv. Math. 64 (1987) 118–175. https://doi.org/10.1016/0001-8708(87)90007-7
  • S.-J. Cheng, N. Lam, Infinite-dimensional Lie superalgebras and hook Schur functions, Comm. Math. Phys. 238 (2003) 95–118.
  • V. G. Kac, A. Radul, Representation theory of the vertex algebra W1+∞W_{1+\infty}W1+∞​, Transform. Groups 1 (1996) 41–70. https://arxiv.org/abs/hep-th/9512150
  • I. G. Macdonald, Symmetric Functions and Hall Polynomials, 2nd ed., Oxford University Press, 1995.
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Quantum Information·Captain: Goku

Relative tensor products for modules over von Neumann algebrasResearch Paper

Motivation

We give an overview of relative tensor products (RTPs) for von Neumann algebra modules. For background, we start with the categorical definition and go on to examine its algebraic formulation, which is applied to Morita equivalence and index. Then we consider the analytic construction, with particular emphasis on explaining why the RTP is not generally defined for every pair of vectors. We also look at recent work justifying a representation of RTPs as composition of unbounded operators, noting that these ideas work equally well for L^p modules. Finally, we prove some new results characterizing preclosedness of the map (ξ, η) \mapsto ξ\otimes_φη.

This mission is the statement-level formalization of Relative tensor products for modules over von Neumann algebras (arXiv:math/0301061v1). Every numbered result of the paper was scanned. The results stated here are open sorry goals, ready for solvers to prove.

What is formalized

1 statements of the paper are in Lean 4 (Mathlib 0df444a). The goal theorem is Density of the intrinsic bounded-vector domain (§5, bounded-vector density, PDF p. 9). The milestones are the other numbered results, in the paper's order, each quoting the paper.

The paper's own objects are the definition item of this mission. Objects shared across papers come from the prove2quantum library and from earlier papers' missions, listed as references.

Provenance: prove2quantum's pipeline drafted each statement (gpt-6.1-sol on Stanford's Sherlock cluster). A blind read-back, written without seeing the paper, is attached to every item. An independent moderator compared each statement against the paper and passed the whole paper without edits.

Deferred results

23 results of the paper are not stated yet, because the library lacks an interface they need:

  • Theorem 7.1 — preclosedness for two standard modules: Weight-GNS tensor map and trace-density measurable-operator calculus (hard)
  • Proposition2.1: Countable standard row modules, amplification action and bounded intertwiner space (hard)
  • RTPUniqueness: Canonical analytic RTP and enriched countable-sum-compatible module bifunctors (hard)
  • Proposition3.2: Independent analytic Hilbert RTP and actual rectangular amplified standard L2 corner (hard)
  • CorrespondencesAndSectors: Faithful normal correspondence realizations and partial-isometry sector quotient (hard)
  • Proposition3.3: Entrywise normal amplification of a corner embedding and RTP composition (hard)
  • Theorem4.1: Complex-linear Hilbert module categories, concrete RTP functor and unitary categorical equivalence (hard)
  • Lemma4.3: Contragredient bimodule and analytic corner/standard-module identification (hard)
  • Corollary4.4: Morita category, countable spatial amplification and full-support projection corners (hard)
  • RTPAssociativity: Iterated analytic completion with external commuting actions (hard)
  • IndexFactor: Independent factor index and dimension-monoid normalization (source-ambiguity)
  • IndexGeneral: Specified normed linear domain and operator for the index spectral radius (source-ambiguity)
  • BoundedVectorsIntrinsic: Coordinate bounded-strong-sum domain and transport through column-module representations (hard)
  • AnalyticRTPRealizations: Positive tensor Gram form, null quotient completion and independent coordinate realization (hard)
  • WeightIndependence: Analytic RTP for two faithful finite functionals and its natural unitary comparison (hard)
  • OperatorComposition: True domains and closed-product convention for the density-corrected triple operator product (source-ambiguity)
  • LpRTP: Complete canonical general Lp RTP construction, vector domains and topology (source-ambiguity)
  • OperatorRecovery: Precise domain/closure convention for the schematic equation (7.4) (source-ambiguity)
  • FiniteMeasurability: Actual closed affiliated densities, inverses and measurable closed-product algebra (hard)
  • Theorem7.2: Hilbert tensor linearization and normalized atomic trace norm formula (hard)
  • Proposition7.3: Central direct integral of factors and measurable fields of traces and density operators (hard)
  • Proposition7.4: Weight bounded-vector domain, general analytic RTP and inverse-density criterion (hard)
  • FalconeTheorem3.8: Original Falcone continuity and nondegeneracy hypotheses (source-ambiguity)

Selected references

  • Relative tensor products for modules over von Neumann algebras, arXiv:math/0301061v1, https://arxiv.org/abs/math/0301061v1
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🏆Completed
Differential GeometryGeneral RelativityMathematical Physics·Captain: He Wang

Exact Spacetime Atlas IV: Certified Einstein–Maxwell Backgrounds and First VariationsResearch Paper

Motivation

Linearised Einstein–Maxwell equations around charged black-hole backgrounds are the starting point of perturbation theory for the Reissner–Nordström and Kerr–Newman families (Newman et al., 1965; see e.g. Giorgi, arXiv:2002.07228). Every such analysis silently uses two facts: that the backgrounds solve the coupled equations, and that the linearised operator is the derivative of the nonlinear residual. In a proof assistant neither is free. This mission records machine-checked certificates for the two backgrounds and an off-shell theorem identifying explicit linearised operators with true derivatives.

Setting

Coordinates on an open set U⊆R4U\subseteq\mathbb R^4U⊆R4 are x=(x0,x1,x2,x3)x=(x^0,x^1,x^2,x^3)x=(x0,x1,x2,x3). A metric field ggg and an inverse field g−1g^{-1}g−1 are 4×44\times44×4 arrays of real functions with g−1g=1g^{-1}g=1g−1g=1 on UUU; a two-form field FFF is an array FabF_{ab}Fab​. With the coordinate partial derivatives ∂a\partial_a∂a​, Christoffel symbols Γbca\Gamma^a_{bc}Γbca​ and Ricci tensor RabR_{ab}Rab​ built from ggg and the given g−1g^{-1}g−1, the three residuals are

Eab=Rab−12gabR−2Sab,Sab=FacgcdFbd−14gabFcdFcd,E_{ab}=R_{ab}-\tfrac12 g_{ab}R-2S_{ab},\quad S_{ab}=F_{ac}g^{cd}F_{bd}-\tfrac14 g_{ab}F_{cd}F^{cd},Eab​=Rab​−21​gab​R−2Sab​,Sab​=Fac​gcdFbd​−41​gab​Fcd​Fcd, Jb=∂aFab+ΓakaFkb+ΓakbFak,Habc=∂aFbc+∂bFca+∂cFab.J^b=\partial_aF^{ab}+\Gamma^a_{ak}F^{kb}+\Gamma^b_{ak}F^{ak},\qquad H_{abc}=\partial_aF_{bc}+\partial_bF_{ca}+\partial_cF_{ab}.Jb=∂a​Fab+Γaka​Fkb+Γakb​Fak,Habc​=∂a​Fbc​+∂b​Fca​+∂c​Fab​.

An Einstein–Maxwell certificate on UUU records: UUU open and nonempty, ggg symmetric, g−1g^{-1}g−1 a true inverse, all components C∞C^\inftyC∞, FFF antisymmetric, ggg Lorentzian, and E=0E=0E=0, J=0J=0J=0, H=0H=0H=0 on UUU. A family (gε,gε−1,Fε)(g_\varepsilon,g^{-1}_\varepsilon,F_\varepsilon)(gε​,gε−1​,Fε​) on an open W⊆R×R4W\subseteq\mathbb R\times\mathbb R^4W⊆R×R4 is admissible (FamilyData) when (ε,y)↦gε(y),Fε(y)(\varepsilon,y)\mapsto g_\varepsilon(y),F_\varepsilon(y)(ε,y)↦gε​(y),Fε​(y) are jointly C∞C^\inftyC∞ and gε−1gε=1g^{-1}_\varepsilon g_\varepsilon=1gε−1​gε​=1 on WWW; no symmetry, signature, antisymmetry or field equation is assumed. Its tangent (h,f)(h,f)(h,f) is the ε\varepsilonε-derivative at 000.

Formalization targets

Goal

For every admissible family with tangent (h,f)(h,f)(h,f) and every xxx with (0,x)∈W(0,x)\in W(0,x)∈W,

ddε∣0Eab(gε,gε−1,Fε)(x)=LEab(g0,g0−1,F0;h,f)(x),\frac{d}{d\varepsilon}\Big|_0E_{ab}(g_\varepsilon,g^{-1}_\varepsilon,F_\varepsilon)(x)=LE_{ab}(g_0,g^{-1}_0,F_0;h,f)(x),dεd​​0​Eab​(gε​,gε−1​,Fε​)(x)=LEab​(g0​,g0−1​,F0​;h,f)(x),

and likewise ddε∣0Jb=LJb\frac{d}{d\varepsilon}|_0J^b=LJ^bdεd​∣0​Jb=LJb, ddε∣0Habc=LHabc(f)\frac{d}{d\varepsilon}|_0H_{abc}=LH_{abc}(f)dεd​∣0​Habc​=LHabc​(f), where LELELE, LJLJLJ, LHLHLH are explicit finite expressions in the background, hhh, fff and their first and second coordinate derivatives. The statement is off shell.

Milestones

The twelve milestones above: the two background certificates and two parameter specialisations; realisation of arbitrary directions and linearity; covariance and certificate transport; parameter tangents of both families; coordinate and potential gauge directions; and one direction on which LELELE does not vanish.

Significance

The goal makes the linearised operators usable without trusting a hand derivation: any statement about LE,LJ,LHLE,LJ,LHLE,LJ,LH is a statement about true derivatives of the registered residuals. The background certificates cover every real parameter in the stated domains (Kerr–Newman for M>0M>0M>0 and all real a,Qa,Qa,Q), and the parameter-tangent and gauge milestones check the operator against the expected zero directions, while milestone 12 rules out a trivially vanishing operator. The background solutions are classical; what is new here is their machine-checked form and the off-shell derivative theorem in this coordinate setting.

Difficulty

The residuals involve the inverse metric and second derivatives of the metric. Differentiating in ε\varepsilonε requires interchanging ∂ε\partial_\varepsilon∂ε​ with coordinate derivatives and differentiating the inverse family; pointwise differentiability in ε\varepsilonε is not enough, and an operator merely named "derivative" would make the goal vacuous.

Formalization scope

Lean 4 with Mathlib (0df444a3…), autoImplicit off; smoothness is ContDiffOn ℝ ∞ (C∞C^\inftyC∞, not analytic). The pinned Mathlib has no Lorentzian Levi-Civita connection or Ricci tensor, so the coordinate definitions (partial derivative, Christoffel symbols, Ricci tensor, residuals) are a registered local definition layer from the earlier Atlas releases, reused unchanged. The operators LE,LJ,LHLE,LJ,LHLE,LJ,LH are independently specified using finite sums and coordinate derivatives; they are not defined as parameter derivatives of the nonlinear residuals. The goal proves that these expressions equal the genuine parameter derivatives. Not included: nonlinear integrability of tangents, new exact solutions, Newman–Penrose reductions, stability, gauge classification, horizons or global structure. The coordinate family x↦x+εξ(x)x\mapsto x+\varepsilon\xi(x)x↦x+εξ(x) used for the gauge milestone is a local family of coordinate maps, not a flow of ξ\xiξ.

Selected references

  • T. Müller, F. Grave, Catalogue of Spacetimes, arXiv:0904.4184 (v3 used locally). https://arxiv.org/abs/0904.4184
  • E. Giorgi, arXiv:2002.07228 (Kerr–Newman in Boyer–Lindquist form; review-provided, not opened by the executor). https://arxiv.org/abs/2002.07228
  • E. T. Newman, E. Couch, K. Chinnapared, A. Exton, A. Prakash, R. Torrence, Metric of a rotating, charged mass, J. Math. Phys. 6 (1965) 918 (link not re-opened this round).
  • H. Reissner, Ann. Phys. 355 (1916) 106; G. Nordström, Proc. KNAW 20 (1918) 1238 (historical attribution; not transcribed).
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AlgebraRepresentation Theory·Captain: mikedeng1

Walled Brauer Algebras as Idempotent Truncations of Level 2 Cyclotomic Quotients: The Explicit Isomorphism of the Walled Brauer Algebra Br_{r,t}(−δ) with the Truncation f·VBr^cycl_{r,t}·fResearch Paper

Why this algebra comparison matters

The walled Brauer algebra organizes the linear operators that commute with a general linear group acting on a tensor product of vector spaces and their duals. Its diagrams mix crossings and contractions, with a wall distinguishing the two tensor factors. This makes it useful in mixed tensor representation theory, where the ordinary symmetric group algebra no longer records every commuting operator. Sartori and Stroppel compare this diagram algebra with a level-two cyclotomic quotient of a degenerate affine walled Brauer algebra. Their comparison identifies a concrete part of the larger algebra by an explicit change of generators Sartori–Stroppel, Theorem 6.2.

The paper's result is a proved theorem. This mission asks for a machine-checked proof of its algebraic statement. The source builds the cyclotomic quotient using parameters arising from parabolic category O\mathcal OO, but the target here is the resulting algebra isomorphism. The dimension comparison that the authors obtain through category O\mathcal OO is included as a separate milestone, in the exact numerical form used in their injectivity argument Sartori–Stroppel, Theorem 5.2, Corollary 5.8, and Lemma 5.9.

The oriented generators and the cyclotomic quotient

Fix r,t∈Nr,t\in\mathbb Nr,t∈N. An orientation aaa is a word of length r+tr+tr+t containing exactly rrr upward arrows and ttt downward arrows. The walled Brauer algebra Br⁡r,t(d)\operatorname{Br}_{r,t}(d)Brr,t​(d) is a complex algebra with an idempotent 1a1_a1a​ for each orientation. At an adjacent pair of positions k,k+1k,k+1k,k+1, equal arrows admit a crossing sk1as_k1_ask​1a​. Unequal arrows admit a changed-orientation crossing s^k1a\widehat s_k1_ask​1a​, an orientation-preserving contraction ek1ae_k1_aek​1a​, and a changed-orientation contraction e^k1a\widehat e_k1_aek​1a​. The relations (Br1)–(Br6) specify orthogonal idempotents, sources and targets, quadratic and braid relations, and interactions among crossings and contractions Sartori–Stroppel, Definition 2.1.

The degenerate affine walled Brauer algebra adds commuting elements y1,…,yr+ty_1,\ldots,y_{r+t}y1​,…,yr+t​ and their relations with the oriented generators. Its level-two cyclotomic quotient imposes a quadratic relation on y1y_1y1​ in each first-arrow component Sartori–Stroppel, Definitions 2.5 and 2.8. Write this quotient as AAA. It uses positive integers m,nm,nm,n and an integer δ\deltaδ, with

β1↑=−δ+(m+n)/2,β2↑=(n−m)/2,β1↓=(m+n)/2,β2↓=δ+(m−n)/2,ω0=m+n,ω1=−δm+(m+n)2/2.\begin{aligned} \beta_1^\uparrow&=-\delta+(m+n)/2,&\beta_2^\uparrow&=(n-m)/2,\\ \beta_1^\downarrow&=(m+n)/2,&\beta_2^\downarrow&=\delta+(m-n)/2,\\ \omega_0&=m+n,&\omega_1&=-\delta m+(m+n)^2/2. \end{aligned}β1↑​β1↓​ω0​​=−δ+(m+n)/2,=(m+n)/2,=m+n,​β2↑​β2↓​ω1​​=(n−m)/2,=δ+(m−n)/2,=−δm+(m+n)2/2.​

The later ωj\omega_jωj​ follow the quadratic recurrence determined by the upward cyclotomic polynomial; they are fixed by these parameters. These are the paper's parameters (5.4), with values in C\mathbb CC Sartori–Stroppel, Definition 5.1 and Lemma 2.9.

For each position kkk and orientation aaa, let ηk1a\eta_k1_aηk​1a​ project away from the generalized eigenspace of yk1ay_k1_ayk​1a​ with eigenvalue β1ak\beta_1^{a_k}β1ak​​. The spectral truncation is f1a=η1⋯ηr+t1af1_a=\eta_1\cdots\eta_{r+t}1_af1a​=η1​⋯ηr+t​1a​, with f=∑af1af=\sum_a f1_af=∑a​f1a​. The intermediate products are fk1a=η1⋯ηk1af_k1_a=\eta_1\cdots\eta_k1_afk​1a​=η1​⋯ηk​1a​ and f0=1f_0=1f0​=1. This gives the corner algebra fAffAffAf Sartori–Stroppel, Definition 5.6. The elements bk,ckb_k,c_kbk​,ck​, polynomial square roots, and resulting images σk,σ^k,τk,τ^k\sigma_k,\widehat\sigma_k,\tau_k,\widehat\tau_kσk​,σk​,τk​,τk​ are defined by (6.1)–(6.4) Sartori–Stroppel, Definition 6.1.

Formalization targets

The goal is the full form of the paper's isomorphism theorem:

Φ:Br⁡r,t(−δ)→ ∼ fAf,(1a,sk1a,s^k1a,ek1a,e^k1a)↦(f1a,σk1a,σ^k1a,τk1a,τ^k1a).\Phi:\operatorname{Br}_{r,t}(-\delta)\xrightarrow{\ \sim\ }fAf, \qquad (1_a,s_k1_a,\widehat s_k1_a,e_k1_a,\widehat e_k1_a) \mapsto(f1_a,\sigma_k1_a,\widehat\sigma_k1_a,\tau_k1_a,\widehat\tau_k1_a).Φ:Brr,t​(−δ) ∼ ​fAf,(1a​,sk​1a​,sk​1a​,ek​1a​,ek​1a​)↦(f1a​,σk​1a​,σk​1a​,τk​1a​,τk​1a​).

Here m,n>0m,n>0m,n>0, m,n≥r+tm,n\ge r+tm,n≥r+t, and δ∈Z\delta\in\mathbb Zδ∈Z satisfy Assumption 5.5: ∣β2↑∣+r+t<β1↑|\beta_2^\uparrow|+r+t<\beta_1^\uparrow∣β2↑​∣+r+t<β1↑​ and ∣β2↓∣+r+t<β1↓|\beta_2^\downarrow|+r+t<\beta_1^\downarrow∣β2↓​∣+r+t<β1↓​. The inequalities separate the relevant eigenvalues. The explicit m,n≥r+tm,n\ge r+tm,n≥r+t condition is needed for Theorem 5.2 in the paper's dimension argument; Assumption 5.5 alone does not imply it Sartori–Stroppel, Assumption 5.5 and Theorem 5.2.

The milestone list records the finite-dimensional inverse and square-root result (Proposition 4.2), the inverse sandwich identity (Lemma 8.7), the changed contraction parameter (Lemma 8.4), the equal-orientation involution (Lemma 8.5), the Jucys–Murphy image identity (Lemma 6.6), and the dimension of the spectral corner (Corollary 5.8 with Lemma 5.9). The last two are stated in algebraic forms that avoid taking the sought map or category O\mathcal OO as extra hypotheses.

What the result supplies

The theorem gives an explicit dictionary between diagram generators and operators in a cyclotomic quotient, including the change from the quotient's loop parameter ω0=m+n\omega_0=m+nω0​=m+n to the source parameter −δ-\delta−δ Sartori–Stroppel, Remark 6.3. It also identifies the whole corner, rather than merely producing a homomorphism into it. This lets properties of the larger algebra be transported to the diagram algebra when their hypotheses are met. The paper discusses graded cellular and Koszul consequences, and an oriented-category extension, separately Sartori–Stroppel, Remarks 6.4–6.5.

A formal development must establish that the presentations do not collapse, that every required oriented relation survives the generator assignment, and that the image fills precisely fAffAffAf. The milestone statements isolate several of the authors' central identities, while the final theorem retains injectivity and surjectivity. A proof would also create reusable infrastructure for quotient presentations with source and target idempotents and for inverses in idempotent corners.

The central difficulty

The formulas for the images involve inverses and square roots after a spectral truncation, and the quotient need not be semisimple. Substituting a scalar directly into a formal power-series identity does not justify the key contraction identity in that setting; the authors explicitly point out this obstruction Sartori–Stroppel, Remark 6.3. The oriented relations also contain dotted symbols that stand for several local choices, so a single equation between global sums does not fully state every relation. Finally, proving that the map exists is only one part of the theorem: its image and kernel require separate control.

Formalization scope

Lean represents both algebras as quotients of free complex algebras by the paper's generators and relations. An orientation is a Boolean sequence with exactly rrr true entries; true denotes an upward arrow. Positions start at zero in Lean, so a paper index kkk corresponds to Lean index k−1k-1k−1. Relations involving dotted generators are imposed for every composable choice with the same source and target. Invalid orientation choices are zero. The affine quotient uses ek2=ω0eke_k^2=\omega_0e_kek2​=ω0​ek​; the source of the theorem uses ek2=−δeke_k^2=-\delta e_kek2​=−δek​. The recurrence fixes every ωj\omega_jωj​ rather than leaving later parameters free.

The ηk\eta_kηk​, intermediate fkf_kfk​, and fff are defined from the polynomial spectral-idempotent characterization, rather than supplied as arbitrary hypotheses. An inverse of xuxuxu is selected by its two inverse equations in the corner uAuuAuuAu. Square roots are not unique in the source, so each theorem holds for every family RkR_kRk​ of polynomial square roots satisfying Rk2=bkfR_k^2=b_kfRk2​=bk​f; the factorized form Qk=Rk+1Rk−1Q_k=R_{k+1}R_k^{-1}Qk​=Rk+1​Rk−1​ is used. A vacuous hypothesis, a collapsed or under-related presentation, a freely chosen fff, or a merely linear map does not express this target. The conclusion requires multiplication, the specified generator values, injectivity, and range exactly fAffAffAf.

The category O\mathcal OO construction and the paper's later applications are outside this mission. The needed reusable pieces are the finite-dimensional algebra lemma, oriented presentation machinery, polynomial spectral idempotents, and corner algebra operations. Contributions that strengthen the supporting algebraic library or close any of the stated milestones are within scope.

Selected references

  • Antonio Sartori and Catharina Stroppel, Walled Brauer algebras as idempotent truncations of level 2 cyclotomic quotients, arXiv preprint, 2015. arXiv:1411.2771v2.
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AlgebraRepresentation Theory·Captain: mikedeng1

The Representation Theory of Cyclotomic BMW Algebras: Semisimplicity Criterion for the Cyclotomic Birman–Wenzl Algebra B_{r,n} over a FieldResearch Paper

Motivation

The Birman–Murakami–Wenzl (BMW) algebras were introduced by Birman and Wenzl and by Murakami to study the Kauffman link polynomial; they are deformations of the Brauer algebras and act as centralizer algebras of quantum groups of orthogonal and symplectic type on tensor powers of the natural module. Their cyclotomic generalization was introduced by Häring-Oldenburg (J. Pure Appl. Algebra 161 (2001)) as the BMW analogue of the Ariki–Koike algebras, the cyclotomic Hecke algebras of type G(r,1,n)G(r,1,n)G(r,1,n). Representation theorists care about when such an algebra is semisimple: in the semisimple case its representation theory is governed by a combinatorial index set (multipartitions with extra data), and outside it one needs decomposition numbers.

For the Ariki–Koike algebra the answer is Ariki's criterion (J. Algebra 169 (1994)). For the ordinary BMW algebra (r=1r = 1r=1) it is due to Rui and Si (J. Reine Angew. Math., [17] in the paper). Rui and Xu proved that the cyclotomic BMW algebra is free and cellular for odd rrr under their u-admissibility conditions (arXiv:0801.0465), and Goodman and Hauschild Mosley (arXiv:math/0612064) and Yu (PhD thesis, Sydney, 2007) obtained freeness by other routes. Rui and Si (arXiv:0807.4149, 2008) extended cellularity to even rrr and, by computing Gram determinants of cell modules, gave a semisimplicity criterion for all r≥2r \ge 2r≥2. That criterion is the goal of this mission.

Setting

Let FFF be a field and r,nr, nr,n positive integers. Fix non-zero q,u1,…,ur∈Fq, u_1, \dots, u_r \in Fq,u1​,…,ur​∈F with δ=q−q−1≠0\delta = q - q^{-1} \ne 0δ=q−q−1=0 and the uiu_iui​ pairwise distinct, and a sign ε∈{1,−1}\varepsilon \in \{1, -1\}ε∈{1,−1}. Put α=ε\alpha = \varepsilonα=ε if rrr is odd and α=εq−ε\alpha = \varepsilon q^{-\varepsilon}α=εq−ε if rrr is even, ϱ−1=α∏ℓuℓ\varrho^{-1} = \alpha\prod_\ell u_\ellϱ−1=α∏ℓ​uℓ​, γr(x)=1\gamma_r(x) = 1γr​(x)=1 (rrr odd), −x-x−x (rrr even), and

γi=(γr(ui)+δ−1ϱ(ui2−1)∏j≠iuj)∏j≠iuiuj−1ui−uj,ωa=∑j=1rujaγj(a∈Z).\gamma_i = \Big(\gamma_r(u_i) + \delta^{-1}\varrho(u_i^2-1)\prod_{j \ne i}u_j\Big)\prod_{j\ne i}\frac{u_iu_j - 1}{u_i - u_j},\qquad \omega_a = \sum_{j=1}^r u_j^a\gamma_j\quad(a\in\mathbb Z).γi​=(γr​(ui​)+δ−1ϱ(ui2​−1)j=i∏​uj​)j=i∏​ui​−uj​ui​uj​−1​,ωa​=j=1∑r​uja​γj​(a∈Z).

These are the u-admissible parameters of Assumption 2.2. The cyclotomic Birman–Wenzl algebra Br,n\mathscr B_{r,n}Br,n​ is the unital associative FFF-algebra generated by Ti,EiT_i, E_iTi​,Ei​ (1≤i<n1 \le i < n1≤i<n) and Xj±1X_j^{\pm1}Xj±1​ (1≤j≤n1 \le j \le n1≤j≤n) subject to the relations a)–k) of Definition 2.1: among them the Kauffman skein relation Ti2−δTi+δϱEi=1T_i^2 - \delta T_i + \delta\varrho E_i = 1Ti2​−δTi​+δϱEi​=1, the braid relations, Ei2=ω0EiE_i^2 = \omega_0E_iEi2​=ω0​Ei​, the skein relations between TiT_iTi​ and Xi,Xi+1X_i, X_{i+1}Xi​,Xi+1​, the unwrapping relations E1X1aE1=ωaE1E_1X_1^aE_1 = \omega_aE_1E1​X1a​E1​=ωa​E1​ for all a∈Za \in \mathbb Za∈Z, the tangle and untwisting relations, EiXiXi+1=Ei=XiXi+1EiE_iX_iX_{i+1} = E_i = X_iX_{i+1}E_iEi​Xi​Xi+1​=Ei​=Xi​Xi+1​Ei​, and the cyclotomic relation (X1−u1)⋯(X1−ur)=0(X_1 - u_1)\cdots(X_1 - u_r) = 0(X1​−u1​)⋯(X1​−ur​)=0. The Ariki–Koike algebra Hr,n\mathscr H_{r,n}Hr,n​ is generated by g1,…,gn−1,y1,…,yng_1, \dots, g_{n-1}, y_1, \dots, y_ng1​,…,gn−1​,y1​,…,yn​ with (gi−q)(gi+q−1)=0(g_i - q)(g_i + q^{-1}) = 0(gi​−q)(gi​+q−1)=0, the braid relations, yi+1=giyigiy_{i+1} = g_iy_ig_iyi+1​=gi​yi​gi​, commuting yjy_jyj​ and (y1−u1)⋯(y1−ur)=0(y_1 - u_1)\cdots(y_1 - u_r) = 0(y1​−u1​)⋯(y1​−ur​)=0.

Write o(q2)>no(q^2) > no(q2)>n for "q2k≠1q^{2k} \ne 1q2k=1 for 1≤k≤n1 \le k \le n1≤k≤n", and set

Qr,ϱ={{−εq,εq−1},2∤r,{−qε,qε},2∣r,Sr,ϱ={⋃k=3n{±q3−k,±qk−3,εq3−2k,−εq2k−3},2∤r,⋃k=3n{±q3−k,±qk−3,±q(2k−3)ε},2∣r.Q_{r,\varrho} = \begin{cases}\{-\varepsilon q, \varepsilon q^{-1}\}, & 2 \nmid r,\\ \{-q^\varepsilon, q^\varepsilon\}, & 2 \mid r,\end{cases}\qquad S_{r,\varrho} = \begin{cases}\bigcup_{k=3}^n\{\pm q^{3-k}, \pm q^{k-3}, \varepsilon q^{3-2k}, -\varepsilon q^{2k-3}\}, & 2 \nmid r,\\ \bigcup_{k=3}^n\{\pm q^{3-k}, \pm q^{k-3}, \pm q^{(2k-3)\varepsilon}\}, & 2 \mid r.\end{cases}Qr,ϱ​={{−εq,εq−1},{−qε,qε},​2∤r,2∣r,​Sr,ϱ​={⋃k=3n​{±q3−k,±qk−3,εq3−2k,−εq2k−3},⋃k=3n​{±q3−k,±qk−3,±q(2k−3)ε},​2∤r,2∣r.​

Formalization targets

Goal: Theorem 6.8

For n≥2n \ge 2n≥2 and r≥2r \ge 2r≥2:

(a) if uiuj=1u_iu_j = 1ui​uj​=1 for some i≠ji \ne ji=j, or ui∈Qr,ϱu_i \in Q_{r,\varrho}ui​∈Qr,ϱ​ for some iii, then Br,n\mathscr B_{r,n}Br,n​ is not semisimple;

(b) if uiuj≠1u_iu_j \ne 1ui​uj​=1 for all i≠ji \ne ji=j and no uiu_iui​ lies in Qr,ϱQ_{r,\varrho}Qr,ϱ​, then

Br,2 semisimple  ⟺  o(q2)>2 and (uiuj−1=q2d, i<j⇒∣d∣≥2),\mathscr B_{r,2}\ \text{semisimple} \iff o(q^2) > 2 \ \text{and}\ \big(u_iu_j^{-1} = q^{2d},\ i<j \Rightarrow |d| \ge 2\big),Br,2​ semisimple⟺o(q2)>2 and (ui​uj−1​=q2d, i<j⇒∣d∣≥2),

and for n≥4n \ge 4n≥4, Br,n\mathscr B_{r,n}Br,n​ is semisimple if and only if (a) o(q2)>no(q^2) > no(q2)>n; (b) ∣d∣≥n|d| \ge n∣d∣≥n whenever uiuj−1=q2du_iu_j^{-1} = q^{2d}ui​uj−1​=q2d, i<ji < ji<j; (c) ui∉Sr,ϱu_i \notin S_{r,\varrho}ui​∈/Sr,ϱ​ for all iii; (d) uiuj∉⋃k=3n{q4−2k,q2k−4}u_iu_j \notin \bigcup_{k=3}^n\{q^{4-2k}, q^{2k-4}\}ui​uj​∈/⋃k=3n​{q4−2k,q2k−4} for all i≠ji \ne ji=j. For n=3n = 3n=3 the goal states that semisimplicity implies (a)–(d).

The page states (b)(2) as an equivalence for all n≥3n \ge 3n≥3. The goal keeps only necessity at n=3n = 3n=3: Proposition 6.2 and Lemma 6.3 describe the same cell module of Br,3\mathscr B_{r,3}Br,3​ and list different exclusions (εq\varepsilon qεq against −εq−1-\varepsilon q^{-1}−εq−1 for odd rrr), and Sr,ϱS_{r,\varrho}Sr,ϱ​ at n=3n = 3n=3 contains neither.

Milestones

The rank dim⁡FBr,n=rn(2n−1)!!\dim_F\mathscr B_{r,n} = r^n(2n-1)!!dimF​Br,n​=rn(2n−1)!! (Theorem 2.14); the corner identities En−1Br,nEn−1=En−1Br,n−2E_{n-1}\mathscr B_{r,n}E_{n-1} = E_{n-1}\mathscr B_{r,n-2}En−1​Br,n​En−1​=En−1​Br,n−2​ (Lemma 3.1) and Ef,nBr,nEf,n=Br,n−2fEf,nE_{f,n}\mathscr B_{r,n}E_{f,n} = \mathscr B_{r,n-2f}E_{f,n}Ef,n​Br,n​Ef,n​=Br,n−2f​Ef,n​ (Corollary 3.2), corrected at the two-strand boundary by requiring some ωa≠0\omega_a\ne0ωa​=0; Proposition 6.1, which says that det⁡G1,∅=det⁡(ωa+b)a,b∈Nr\det G_{1,\emptyset} = \det(\omega_{a+b})_{a,b\in N_r}detG1,∅​=det(ωa+b​)a,b∈Nr​​ is non-zero exactly when uiuj≠1u_iu_j \ne 1ui​uj​=1 (i≠ji \ne ji=j) and no uiu_iui​ lies in Qr,ϱQ_{r,\varrho}Qr,ϱ​; Proposition 6.5(b), non-semisimplicity when that determinant vanishes; and the reduction "Hr,n\mathscr H_{r,n}Hr,n​ not semisimple ⇒Br,n\Rightarrow \mathscr B_{r,n}⇒Br,n​ not semisimple" from the proof of Theorem 6.8.

Significance

The criterion gives a closed list of parameter values at which the cyclotomic BMW algebra fails to be semisimple, and so, by Graham–Lehrer theory, the parameters at which all cell modules are simple and pairwise non-isomorphic. Outside that list the algebra's simple modules, their dimensions and the decomposition of tensor-type modules are given by the combinatorics of up-down tableaux; inside it, the list says which Gram determinants vanish and where decomposition numbers begin. For r=1r = 1r=1 it specializes to the semisimplicity criterion for BMW algebras, and its conditions (a)–(b) are Ariki's conditions for Hr,n\mathscr H_{r,n}Hr,n​.

As far as is known, none of this is machine-checked: Mathlib has no BMW, Brauer, Ariki–Koike or Iwahori–Hecke algebras and no cellular algebras. The mission formalizes the statements of the paper on a presentation of Br,n\mathscr B_{r,n}Br,n​ by generators and relations; a solver must supply a basis (or at least a dimension count), the cellular structure and the Gram-determinant computations. The paper leaves several of its proofs to the reader ("by arguments in the proof of [19, 5.41]"), so the formal proofs would also close gaps in the published argument.

Difficulty

Non-semisimplicity in part (a) needs only one degenerate bilinear form on a non-zero cell module, but showing that the module is non-zero, or that Br,n\mathscr B_{r,n}Br,n​ does not collapse, already needs a lower bound on the dimension of a presented algebra, which no rewriting argument provides: the rank rn(2n−1)!!r^n(2n-1)!!rn(2n−1)!! is proved in the literature through seminormal representations. Sufficiency in part (b) requires the Gram determinants of all cell modules Δ(f,λ)\Delta(f,\lambda)Δ(f,λ), which the paper obtains by a recursion over up-down tableaux; vanishing of a single factor must be traced through branching and Morita-type functors between levels n−2n-2n−2, n−1n-1n−1 and nnn. Ariki's criterion for Hr,n\mathscr H_{r,n}Hr,n​ is itself an external input.

Formalization scope

Br,n\mathscr B_{r,n}Br,n​ and Hr,n\mathscr H_{r,n}Hr,n​ are RingQuot quotients of FreeAlgebra F on finite generator types; indices are 0-based (the Lean T i is the paper's Ti+1T_{i+1}Ti+1​), and Xj−1X_j^{-1}Xj−1​ is a separate generator tied to XjX_jXj​ by relation a). The sign ε∈Z×\varepsilon \in \mathbb Z^\timesε∈Z× is the free parameter and α,ϱ,γi,ωa\alpha, \varrho, \gamma_i, \omega_aα,ϱ,γi​,ωa​ are computed from (q,u,ε)(q, u, \varepsilon)(q,u,ε), so the parameters are u-admissible by construction. The uiu_iui​ are pairwise distinct (Assumption 2.2(1) divides by ui−uju_i - u_jui​−uj​; the paper extends 2.2 to coincident uiu_iui​ through [19, 3.11]). "Semisimple" is Mathlib's IsSemisimpleRing. The condition o(q2)>no(q^2) > no(q2)>n is written as q2k≠1q^{2k} \ne 1q2k=1 for 1≤k≤n1 \le k \le n1≤k≤n, not through orderOf, which is 000 for elements of infinite order. Relations d) and g) both use ω0=∑jγj\omega_0 = \sum_j\gamma_jω0​=∑j​γj​, which equals the paper's 1−δ−1(ϱ−ϱ−1)1 - \delta^{-1}(\varrho - \varrho^{-1})1−δ−1(ϱ−ϱ−1) for these parameters; were they different, the presentation would collapse. The corrected corner milestones require n≥3n\ge3n≥3 or some ωa≠0\omega_a\ne0ωa​=0 in Lemma 3.1, and 2f<n2f<n2f<n or some ωa≠0\omega_a\ne0ωa​=0 in Corollary 3.2. At n=2n=2n=2, r=2r=2r=2, q=3q=3q=3, u=(2,12)u=(2,\tfrac12)u=(2,21​), and ε=1\varepsilon=1ε=1, every ωa\omega_aωa​ vanishes, exposing the missing condition. det⁡G1,∅\det G_{1,\emptyset}detG1,∅​ is expressed as the Hankel determinant of the ωa\omega_aωa​, and Br,m⊆Br,n\mathscr B_{r,m} \subseteq \mathscr B_{r,n}Br,m​⊆Br,n​ is the subalgebra generated by the first generators.

A presentation that collapses to the zero algebra would make the goal false in part (a) but trivially true elsewhere; the rank milestone rules this out. Replacing semisimplicity by non-vanishing of Gram determinants would turn the goal into a different theorem and is not acceptable.

A complete development needs a basis theorem for Br,n\mathscr B_{r,n}Br,n​, cellular algebras and Graham–Lehrer's semisimplicity criterion, the Ariki–Koike algebra and Ariki's criterion, and Gram-determinant computations. The cellular-algebra layer and the Ariki–Koike algebra are reusable beyond this mission; contributions of any of these, or of the milestones on their own, are welcome.

Selected references

  • H. Rui and M. Si, The representation theory of cyclotomic BMW algebras (printed title The representations of cyclotomic BMW algebras, II), preprint, 2008. https://arxiv.org/abs/0807.4149
  • H. Rui and J. Xu, The representations of cyclotomic BMW algebras, preprint, 2007. https://arxiv.org/abs/0801.0465
  • R. Häring-Oldenburg, Cyclotomic Birman–Murakami–Wenzl algebras, J. Pure Appl. Algebra 161 (2001), 113–144. https://doi.org/10.1016/S0022-4049(00)00100-6
  • S. Ariki, On the semi-simplicity of the Hecke algebra of (Z/rZ)≀Sn(\mathbb Z/r\mathbb Z)\wr\mathfrak S_n(Z/rZ)≀Sn​, J. Algebra 169 (1994), 216–225. https://doi.org/10.1006/jabr.1994.1280
  • J. J. Graham and G. I. Lehrer, Cellular algebras, Invent. Math. 123 (1996), 1–34. https://doi.org/10.1007/BF01232365
  • J. S. Birman and H. Wenzl, Braids, link polynomials and a new algebra, Trans. Amer. Math. Soc. 313 (1989), 249–273. https://doi.org/10.1090/S0002-9947-1989-0992598-X
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Information TheoryLinear algebraQuantum Information·Captain: mikedeng1

Classical capacity of fermionic product channels: An Explicit Formula for the Gaussian Capacity, Which Equals the One-Shot Capacity for n ≤ 2Research Paper

Motivation

Sending classical messages through a quantum device requires choosing input states that remain distinguishable after noise. The one-shot classical capacity measures the best information rate when each channel use is signaled with a separate input state. For many channels the optimization is difficult because it ranges over all ensembles of quantum states. Fermionic systems provide a finite-dimensional setting in which the noise has a direct description on elementary operators, but the optimal signaling states still need not be obvious. Bravyi's 2005 paper isolates a family of fermionic product channels, computes the best rate from Gaussian input states for any number of qubits, and proves that this restricted rate is the full one-shot rate for one or two qubits.

Setting

The system has nnn qubits, with computational basis indexed by bit strings x∈{0,1}nx\in\{0,1\}^nx∈{0,1}n. The Jordan–Wigner Majorana operators c1,…,c2nc_1,\ldots,c_{2n}c1​,…,c2n​ are tensor products of Pauli matrices: c2j−1c_{2j-1}c2j−1​ has ZZZ on qubits before jjj, XXX on qubit jjj, and identity afterwards; c2jc_{2j}c2j​ replaces XXX with YYY. Their ordered monomials c(x)=c1x1⋯c2nx2nc(x)=c_1^{x_1}\cdots c_{2n}^{x_{2n}}c(x)=c1x1​​⋯c2nx2n​​, x∈{0,1}2nx\in\{0,1\}^{2n}x∈{0,1}2n, form a basis of all operators on the qubits. The paper gives these operators and their monomials in Eq. (3).

A fermionic product channel Φb\Phi_bΦb​ is determined by attenuation coefficients bp∈[0,1]b_p\in[0,1]bp​∈[0,1]. On each monomial it acts by Φb(c(x))=(∏p:xp=1bp)c(x)\Phi_b(c(x))=(\prod_{p:x_p=1}b_p)c(x)Φb​(c(x))=(∏p:xp​=1​bp​)c(x), and linearity defines it on every operator. A state is a positive semidefinite matrix of trace one. For a finite ensemble of output states {(pa,ρa)}\{(p_a,\rho_a)\}{(pa​,ρa​)}, with nonnegative weights summing to one, its Holevo quantity in bits is

χ=S ⁣(∑apaρa)−∑apaS(ρa),S(ρ)=−Tr⁡(ρlog⁡2ρ).\chi= S\!\left(\sum_a p_a\rho_a\right)-\sum_a p_aS(\rho_a), \qquad S(\rho)=-\operatorname{Tr}(\rho\log_2\rho).χ=S(a∑​pa​ρa​)−a∑​pa​S(ρa​),S(ρ)=−Tr(ρlog2​ρ).

The supremum of χ\chiχ over all finite ensembles of outputs of Φb\Phi_bΦb​ is C1(Φb)C_1(\Phi_b)C1​(Φb​). A Gaussian state has the specific form UρλU†U\rho_\lambda U^\daggerUρλ​U† of Definition 1: ρλ=2−n∏j(I+λjZj)\rho_\lambda=2^{-n}\prod_j(I+\lambda_j Z_j)ρλ​=2−n∏j​(I+λj​Zj​), each λj∈[−1,1]\lambda_j\in[-1,1]λj​∈[−1,1], and U=exp⁡(iH2+iH1)U=\exp(iH_2+iH_1)U=exp(iH2​+iH1​) for Hermitian quadratic and linear combinations of Majorana operators. Requiring Gaussian input states gives C1g(Φb)C_1^g(\Phi_b)C1g​(Φb​). Setting H1=0H_1=0H1​=0 gives an even Gaussian state. These are separate classes; the even class supplies an intermediate entropy minimum. Definition 1 and Eq. (13) are on page 4.

Formalization targets

Gaussian capacity

Write b1↓≥⋯≥b2n↓b_1^\downarrow\ge\cdots\ge b_{2n}^\downarrowb1↓​≥⋯≥b2n↓​ for the coefficients in decreasing order, and let H(t)=−tlog⁡2t−(1−t)log⁡2(1−t)H(t)=-t\log_2t-(1-t)\log_2(1-t)H(t)=−tlog2​t−(1−t)log2​(1−t). The main formula, Theorem 1 and Eq. (6), is

C1g(Φb)=n−H ⁣(1+b1↓2)−∑j=1n−1H ⁣(1+b2j↓b2j+1↓2).C_1^g(\Phi_b)=n-H\!\left(\frac{1+b_1^\downarrow}{2}\right) -\sum_{j=1}^{n-1}H\!\left(\frac{1+b_{2j}^\downarrow b_{2j+1}^\downarrow}{2}\right).C1g​(Φb​)=n−H(21+b1↓​​)−j=1∑n−1​H(21+b2j↓​b2j+1↓​​).

It holds for every n≥1n\ge1n≥1 and every unsorted b∈[0,1]2nb\in[0,1]^{2n}b∈[0,1]2n. The milestones identify the covariance and Gaussian-preservation facts, the exact even and general Gaussian minimum-output entropies, and an ensemble attaining the capacity.

Full one-shot capacity for at most two qubits

The second clause of Theorem 1 states

C1(Φb)=C1g(Φb)(n≤2).C_1(\Phi_b)=C_1^g(\Phi_b)\qquad(n\le2).C1​(Φb​)=C1g​(Φb​)(n≤2).

Thus restricting the input ensemble to Gaussian states loses no one-shot capacity in these dimensions. The paper does not prove this equality for arbitrary nnn.

Significance

The formula replaces an optimization over arbitrary finite Gaussian ensembles with binary entropies of sorted attenuation coefficients. In the one- and two-qubit cases it also settles the unrestricted one-shot optimization for this channel family. The intermediate result C1=n−Smin⁡C_1=n-S_{\min}C1​=n−Smin​ relates signaling directly to minimum output entropy; the even-Gaussian and Gaussian minima make the distinction between the two state classes explicit. These relationships are established in Sections II–IV of the paper.

The mathematical results are proved in the 2005 paper. This mission asks for machine-checked proofs of their exact finite-dimensional statements. The definitions of bit-valued von Neumann entropy, finite output ensembles, ordered Majorana monomials, Gaussian-state predicates, and covariance matrices can support later work on fermionic channels. The submitted goal and milestones are presently proof obligations rather than claims of existing Lean proofs.

Difficulty

The channel is simple on each Majorana monomial, but the entropy of a general output state is not determined by its one- and two-point correlations. Even within the Gaussian class, optimizing only the even Gaussian states gives a different formula from optimizing all Gaussian states: linear Majorana terms change the optimum. A direct search over density matrices therefore does not expose the closed expression in Theorem 1. For the unrestricted two-qubit clause, one must also relate arbitrary states to the Gaussian class; the paper invokes a three-qubit parity result for that step. The distinctions and parity result appear in Sections III–IV.

Formalization scope

Lean represents qubit basis vectors by Fin n → Fin 2 and operators by complex matrices on that finite type. Majorana indices start at zero in Lean, so the paper's c2j−1,c2jc_{2j-1},c_{2j}c2j−1​,c2j​ correspond to consecutive indices 2j−2,2j−12j-2,2j-12j−2,2j−1. The Jordan–Wigner tensor factor at coordinate jjj acts on qubit jjj; the monomial product follows increasing Majorana index. The channel is defined on all matrices by the trace-orthogonal monomial expansion of Eq. (4), not merely on covariance matrices. Attenuations may equal zero or one. Entropies use logarithms to base two, with 0log⁡20=00\log_2 0=00log2​0=0.

Every capacity uses a real supremum over all finite normalized ensembles, with arbitrary ensemble size. The inputs are density matrices, and their channel outputs must be density matrices. The Gaussian capacity requires every input to satisfy Definition 1; Lemma 2 ensures these outputs are Gaussian too. The minimum-output quantities are real infima over their stated input classes, and the corresponding milestone theorems assert attainment. For the actual channels the relevant sets are nonempty and bounded: the maximally mixed state supplies an output state, while every Holevo quantity lies between zero and nnn. This representation rules out restricting the Gaussian ensemble to the displayed optimizing family, assuming the goal's coefficients are initially sorted, or replacing bit entropy with natural-log entropy.

The development needs finite-matrix functional calculus, positivity, matrix exponentials, permutation and singular-value reasoning, and finite ensemble entropy bounds. Contributions to those reusable layers and to the paper's covariance, Gaussian-preservation, and minimum-output results are within scope. Lemma 3 is stated in its even-Gaussian form, which its proof establishes; the displayed lemma says only “Gaussian.”

Selected references

  • Sergey Bravyi, Classical capacity of fermionic product channels, arXiv preprint quant-ph/0507282v1, 2005. arXiv
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